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Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


1

Beamlines  

NLE Websites -- All DOE Office Websites (Extended Search)

Beamlines Beamlines Beamlines Print Beamlines Directory List of ALS beamlines, techniques, energy ranges, beamline scientists' contact information, and individual beamline schedules. The ALS Beamclock and links to the ALS Energy-Related Beamlines poster and beamclock are also available. Beam Status Current status of the ALS accelerator, updated every minute. Instructions on how to get beam status updates via Twitter @ALSRingStatus or text messages, and request form for beam history information. Research Techniques Research techniques and the corresponding beamlines where they are available (under construction). Schedules Weekly user schedule, current and upcoming long-term operating schedules; individual beamline long-term schedules can be found on the ALS Beamlines Directory.

2

Beamline  

NLE Websites -- All DOE Office Websites (Extended Search)

about how nif works Beamline Every NIF beam starts at the master oscillator. The low-energy beam is amplified in the preamplifier module and then in the power amplifier, the main...

3

Beamline 12.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

Beamline 12.2.2 Beamline 12.2.2 Beamline 12.2.2 Print Tuesday, 20 October 2009 09:31 High-Pressure (California High-Pressure Science Observatory: Calipso) Endstations: Medium pressure High pressure laser heating GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Superbend magnet, 1.9GeV, 5.29Tesla, 500mA Monochromator Si(111) or Multilayer Energy range 6-40 keV for Si(111), 14-28 keV for Multilayer Resolving power (E/ΔE) Si(111) = 7000, Multilayer =100 Beam size (HxV) Focused: 10 x 10 micron Unfocused: 90 x 100 micron Scientific applications High-pressure science Scientific disciplines Earth sciences, materials science, construction materials, chemistry, energy. Endstations Medium pressure

4

Beamline 7.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and Materials Science, Spectromicroscopy Scientific disciplines: Correlated electron system, materials science Endstations: nanoARPES (nARPES) Electronic Structure Factory (ESF) Advanced x-ray inelastic scattering (AXIS) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range See endstation tables Monochromator See endstation tables Scientific disciplines Correlated electron system, materials science Website Beamline 7: http://www-bl7.lbl.gov/ ENDSTATION INFORMATION Endstation name nanoARPES Operational This instrument is currently under development. Expected user operation in 2012. For consideration, speak to the beamline scientist before applying for beamtime.

5

Beamline 1.4.3  

NLE Websites -- All DOE Office Websites (Extended Search)

Beamline 1.4.3 Print Beamline 1.4.3 Print FTIR spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.2 eV Frequency range 650 - 10,000 cm-1 Interferometer resolution Up to 0.125 cm-1 Endstations Nicolet Magna 760 FTIR, Nic-Plan IR Microscope (N2 purged) Characteristics Motorized sample stage, 0.1-micron resolution, reflection, transmission, and grazing-incidence reflection modes Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy Detectors MCT-A (mercury cadmium telluride) Spot size at sample

6

Beamline 7.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and Materials Science, Spectromicroscopy Scientific disciplines: Correlated electron system, materials science Endstations: nanoARPES (nARPES) Electronic Structure Factory (ESF) Advanced x-ray inelastic scattering (AXIS) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range See endstation tables Monochromator See endstation tables Scientific disciplines Correlated electron system, materials science Website Beamline 7: http://www-bl7.lbl.gov/ ENDSTATION INFORMATION Endstation name nanoARPES Operational This instrument is currently under development. Expected user operation in 2012. For consideration, speak to the beamline scientist before applying for beamtime.

7

Beamline 7.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and Materials Science, Spectromicroscopy Scientific disciplines: Correlated electron system, materials science Endstations: nanoARPES (nARPES) Electronic Structure Factory (ESF) Advanced x-ray inelastic scattering (AXIS) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range See endstation tables Monochromator See endstation tables Scientific disciplines Correlated electron system, materials science Website Beamline 7: http://www-bl7.lbl.gov/ ENDSTATION INFORMATION Endstation name nanoARPES Operational This instrument is currently under development. Expected user operation in 2012. For consideration, speak to the beamline scientist before applying for beamtime.

8

Beamline 1.4.3  

NLE Websites -- All DOE Office Websites (Extended Search)

Beamline 1.4.3 Print Beamline 1.4.3 Print FTIR spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.2 eV Frequency range 650 - 10,000 cm-1 Interferometer resolution Up to 0.125 cm-1 Endstations Nicolet Magna 760 FTIR, Nic-Plan IR Microscope (N2 purged) Characteristics Motorized sample stage, 0.1-micron resolution, reflection, transmission, and grazing-incidence reflection modes Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy Detectors MCT-A (mercury cadmium telluride) Spot size at sample

9

Beamline 7.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and Materials Science, Spectromicroscopy Scientific disciplines: Correlated electron system, materials science Endstations: nanoARPES (nARPES) Electronic Structure Factory (ESF) Advanced x-ray inelastic scattering (AXIS) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range See endstation tables Monochromator See endstation tables Scientific disciplines Correlated electron system, materials science Website Beamline 7: http://www-bl7.lbl.gov/ ENDSTATION INFORMATION Endstation name nanoARPES Operational This instrument is currently under development. Expected user operation in 2012. For consideration, speak to the beamline scientist before applying for beamtime.

10

Beamline 10.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 0.1 Beamline 10.0.1 Print Tuesday, 20 October 2009 09:08 Photoemission of Highly Correlated Materials; High-Resolution Atomic, Molecular, and Optical Physics Scientific disciplines: AMO, correlated electron systems Endstations: High energy resolution spectrometer (HERS) High-resolution atomic and molecular electron spectrometer (HiRAMES) HRAMO-Ion-photon beamline (IPB) Velocity map imaging spectrometer Electron spin polarization (ESP) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 10-cm period undulator (U10) (first and third harmonics) Energy range 17-350 eV Monochromator SGM (gratings: 380, 925, 2100 lines/mm) Calculated and measured flux (1.9 GeV, 400 mA) Up to 1013 photons/s/0.01% BW at 30 eV

11

Beamline 1.4.3  

NLE Websites -- All DOE Office Websites (Extended Search)

Beamline 1.4.3 Print Beamline 1.4.3 Print FTIR spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.2 eV Frequency range 650 - 10,000 cm-1 Interferometer resolution Up to 0.125 cm-1 Endstations Nicolet Magna 760 FTIR, Nic-Plan IR Microscope (N2 purged) Characteristics Motorized sample stage, 0.1-micron resolution, reflection, transmission, and grazing-incidence reflection modes Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy Detectors MCT-A (mercury cadmium telluride) Spot size at sample

12

Beamline 7.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

7.0.1 Print 7.0.1 Print Surface and Materials Science, Spectromicroscopy Scientific disciplines: Correlated electron system, materials science Endstations: nanoARPES (nARPES) Electronic Structure Factory (ESF) Advanced x-ray inelastic scattering (AXIS) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range See endstation tables Monochromator See endstation tables Scientific disciplines Correlated electron system, materials science Website Beamline 7: http://www-bl7.lbl.gov/ ENDSTATION INFORMATION Endstation name nanoARPES Operational This instrument is currently under development. Expected user operation in 2012. For consideration, speak to the beamline scientist before applying for beamtime.

13

Beamline 7.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and Materials Science, Spectromicroscopy Scientific disciplines: Correlated electron system, materials science Endstations: nanoARPES (nARPES) Electronic Structure Factory (ESF) Advanced x-ray inelastic scattering (AXIS) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range See endstation tables Monochromator See endstation tables Scientific disciplines Correlated electron system, materials science Website Beamline 7: http://www-bl7.lbl.gov/ ENDSTATION INFORMATION Endstation name nanoARPES Operational This instrument is currently under development. Expected user operation in 2012. For consideration, speak to the beamline scientist before applying for beamtime.

14

Beamline 10.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 0.1 Beamline 10.0.1 Print Tuesday, 20 October 2009 09:08 Photoemission of Highly Correlated Materials; High-Resolution Atomic, Molecular, and Optical Physics Scientific disciplines: AMO, correlated electron systems Endstations: High energy resolution spectrometer (HERS) High-resolution atomic and molecular electron spectrometer (HiRAMES) HRAMO-Ion-photon beamline (IPB) Velocity map imaging spectrometer Electron spin polarization (ESP) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 10-cm period undulator (U10) (first and third harmonics) Energy range 17-350 eV Monochromator SGM (gratings: 380, 925, 2100 lines/mm) Calculated and measured flux (1.9 GeV, 400 mA) Up to 1013 photons/s/0.01% BW at 30 eV

15

Beamline 7.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and Materials Science, Spectromicroscopy Scientific disciplines: Correlated electron system, materials science Endstations: nanoARPES (nARPES) Electronic Structure Factory (ESF) Advanced x-ray inelastic scattering (AXIS) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range See endstation tables Monochromator See endstation tables Scientific disciplines Correlated electron system, materials science Website Beamline 7: http://www-bl7.lbl.gov/ ENDSTATION INFORMATION Endstation name nanoARPES Operational This instrument is currently under development. Expected user operation in 2012. For consideration, speak to the beamline scientist before applying for beamtime.

16

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 0.1 Beamline 8.0.1 Print Tuesday, 20 October 2009 08:51 Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE)

17

Beamline 10.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Photoemission of Highly Correlated Materials; High-Resolution Atomic, Molecular, and Optical Physics Scientific disciplines: AMO, correlated electron systems Endstations: High energy resolution spectrometer (HERS) High-resolution atomic and molecular electron spectrometer (HiRAMES) HRAMO-Ion-photon beamline (IPB) Velocity map imaging spectrometer Electron spin polarization (ESP) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 10-cm period undulator (U10) (first and third harmonics) Energy range 17-350 eV Monochromator SGM (gratings: 380, 925, 2100 lines/mm) Calculated and measured flux (1.9 GeV, 400 mA) Up to 1013 photons/s/0.01% BW at 30 eV Resolving power (E/ΔE)

18

Beamline 10.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Photoemission of Highly Correlated Materials; High-Resolution Atomic, Molecular, and Optical Physics Scientific disciplines: AMO, correlated electron systems Endstations: High energy resolution spectrometer (HERS) High-resolution atomic and molecular electron spectrometer (HiRAMES) HRAMO-Ion-photon beamline (IPB) Velocity map imaging spectrometer Electron spin polarization (ESP) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 10-cm period undulator (U10) (first and third harmonics) Energy range 17-350 eV Monochromator SGM (gratings: 380, 925, 2100 lines/mm) Calculated and measured flux (1.9 GeV, 400 mA) Up to 1013 photons/s/0.01% BW at 30 eV Resolving power (E/ΔE)

19

Beamline 10.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Photoemission of Highly Correlated Materials; High-Resolution Atomic, Molecular, and Optical Physics Scientific disciplines: AMO, correlated electron systems Endstations: High energy resolution spectrometer (HERS) High-resolution atomic and molecular electron spectrometer (HiRAMES) HRAMO-Ion-photon beamline (IPB) Velocity map imaging spectrometer Electron spin polarization (ESP) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 10-cm period undulator (U10) (first and third harmonics) Energy range 17-350 eV Monochromator SGM (gratings: 380, 925, 2100 lines/mm) Calculated and measured flux (1.9 GeV, 400 mA) Up to 1013 photons/s/0.01% BW at 30 eV Resolving power (E/ΔE)

20

Beamline 12.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2.2 2.2 Beamline 12.2.2 Print Tuesday, 20 October 2009 09:31 High-Pressure (California High-Pressure Science Observatory: Calipso) Endstations: Medium pressure High pressure laser heating GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Superbend magnet, 1.9GeV, 5.29Tesla, 500mA Monochromator Si(111) or Multilayer Energy range 6-40 keV for Si(111), 14-28 keV for Multilayer Resolving power (E/ΔE) Si(111) = 7000, Multilayer =100 Beam size (HxV) Focused: 10 x 10 micron Unfocused: 90 x 100 micron Scientific applications High-pressure science Scientific disciplines Earth sciences, materials science, construction materials, chemistry, energy. Endstations Medium pressure High pressure laser heating

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


21

Beamline 12.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

2.0.1 Print 2.0.1 Print EUV optics testing and interferometry, angle- and spin-resolved photoemission Scientific discipline: Applied science, correlated electron systems Endstations: Angle- and spin-resolved photoemission (12.0.1.1) Berkeley Dose Calibration Tool (DCT)(12.0.1.2) SEMATECH Berkeley Microfield Exposure Tool (MET) (12.0.1.3) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 8-cm-period undulator (U8) Energy range See endstation tables Monochromator See endstation tables Endstations Angle- and spin-resolved photoemission (12.0.1.1) SEMATECH Berkeley Microfield Exposure Tool (MET) (12.0.1.2) Berkeley Dose Calibration Tool (DCT)(12.0.1.3) Beamline phone numbers (510) 495-2121 (12.0.1.1)

22

Beamline 12.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

2.0.1 Print 2.0.1 Print EUV optics testing and interferometry, angle- and spin-resolved photoemission Scientific discipline: Applied science, correlated electron systems Endstations: Angle- and spin-resolved photoemission (12.0.1.1) Berkeley Dose Calibration Tool (DCT)(12.0.1.2) SEMATECH Berkeley Microfield Exposure Tool (MET) (12.0.1.3) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 8-cm-period undulator (U8) Energy range See endstation tables Monochromator See endstation tables Endstations Angle- and spin-resolved photoemission (12.0.1.1) SEMATECH Berkeley Microfield Exposure Tool (MET) (12.0.1.2) Berkeley Dose Calibration Tool (DCT)(12.0.1.3) Beamline phone numbers (510) 495-2121 (12.0.1.1)

23

Beamline 10.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Photoemission of Highly Correlated Materials; High-Resolution Atomic, Molecular, and Optical Physics Scientific disciplines: AMO, correlated electron systems Endstations: High energy resolution spectrometer (HERS) High-resolution atomic and molecular electron spectrometer (HiRAMES) HRAMO-Ion-photon beamline (IPB) Velocity map imaging spectrometer Electron spin polarization (ESP) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 10-cm period undulator (U10) (first and third harmonics) Energy range 17-350 eV Monochromator SGM (gratings: 380, 925, 2100 lines/mm) Calculated and measured flux (1.9 GeV, 400 mA) Up to 1013 photons/s/0.01% BW at 30 eV Resolving power (E/ΔE)

24

Beamline 10.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Photoemission of Highly Correlated Materials; High-Resolution Atomic, Molecular, and Optical Physics Scientific disciplines: AMO, correlated electron systems Endstations: High energy resolution spectrometer (HERS) High-resolution atomic and molecular electron spectrometer (HiRAMES) HRAMO-Ion-photon beamline (IPB) Velocity map imaging spectrometer Electron spin polarization (ESP) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 10-cm period undulator (U10) (first and third harmonics) Energy range 17-350 eV Monochromator SGM (gratings: 380, 925, 2100 lines/mm) Calculated and measured flux (1.9 GeV, 400 mA) Up to 1013 photons/s/0.01% BW at 30 eV Resolving power (E/ΔE)

25

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 0.1 Beamline 8.0.1 Print Tuesday, 20 October 2009 08:51 Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE)

26

Beamline 10.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Photoemission of Highly Correlated Materials; High-Resolution Atomic, Molecular, and Optical Physics Scientific disciplines: AMO, correlated electron systems Endstations: High energy resolution spectrometer (HERS) High-resolution atomic and molecular electron spectrometer (HiRAMES) HRAMO-Ion-photon beamline (IPB) Velocity map imaging spectrometer Electron spin polarization (ESP) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 10-cm period undulator (U10) (first and third harmonics) Energy range 17-350 eV Monochromator SGM (gratings: 380, 925, 2100 lines/mm) Calculated and measured flux (1.9 GeV, 400 mA) Up to 1013 photons/s/0.01% BW at 30 eV Resolving power (E/ΔE)

27

Beamline 10.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Photoemission of Highly Correlated Materials; High-Resolution Atomic, Molecular, and Optical Physics Scientific disciplines: AMO, correlated electron systems Endstations: High energy resolution spectrometer (HERS) High-resolution atomic and molecular electron spectrometer (HiRAMES) HRAMO-Ion-photon beamline (IPB) Velocity map imaging spectrometer Electron spin polarization (ESP) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 10-cm period undulator (U10) (first and third harmonics) Energy range 17-350 eV Monochromator SGM (gratings: 380, 925, 2100 lines/mm) Calculated and measured flux (1.9 GeV, 400 mA) Up to 1013 photons/s/0.01% BW at 30 eV Resolving power (E/ΔE)

28

Beamline 12.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

2.0.1 Print 2.0.1 Print EUV optics testing and interferometry, angle- and spin-resolved photoemission Scientific discipline: Applied science, correlated electron systems Endstations: Angle- and spin-resolved photoemission (12.0.1.1) Berkeley Dose Calibration Tool (DCT)(12.0.1.2) SEMATECH Berkeley Microfield Exposure Tool (MET) (12.0.1.3) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 8-cm-period undulator (U8) Energy range See endstation tables Monochromator See endstation tables Endstations Angle- and spin-resolved photoemission (12.0.1.1) SEMATECH Berkeley Microfield Exposure Tool (MET) (12.0.1.2) Berkeley Dose Calibration Tool (DCT)(12.0.1.3) Beamline phone numbers (510) 495-2121 (12.0.1.1)

29

Beamline 10.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Photoemission of Highly Correlated Materials; High-Resolution Atomic, Molecular, and Optical Physics Scientific disciplines: AMO, correlated electron systems Endstations: High energy resolution spectrometer (HERS) High-resolution atomic and molecular electron spectrometer (HiRAMES) HRAMO-Ion-photon beamline (IPB) Velocity map imaging spectrometer Electron spin polarization (ESP) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 10-cm period undulator (U10) (first and third harmonics) Energy range 17-350 eV Monochromator SGM (gratings: 380, 925, 2100 lines/mm) Calculated and measured flux (1.9 GeV, 400 mA) Up to 1013 photons/s/0.01% BW at 30 eV Resolving power (E/ΔE)

30

Beamline 12.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

2.0.1 Print 2.0.1 Print EUV optics testing and interferometry, angle- and spin-resolved photoemission Scientific discipline: Applied science, correlated electron systems Endstations: Angle- and spin-resolved photoemission (12.0.1.1) Berkeley Dose Calibration Tool (DCT)(12.0.1.2) SEMATECH Berkeley Microfield Exposure Tool (MET) (12.0.1.3) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 8-cm-period undulator (U8) Energy range See endstation tables Monochromator See endstation tables Endstations Angle- and spin-resolved photoemission (12.0.1.1) SEMATECH Berkeley Microfield Exposure Tool (MET) (12.0.1.2) Berkeley Dose Calibration Tool (DCT)(12.0.1.3) Beamline phone numbers (510) 495-2121 (12.0.1.1)

31

Beamline 9.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

9.3.2 9.3.2 Beamline 9.3.2 Print Tuesday, 20 October 2009 09:06 Chemical and Materials Scientific disciplines: Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry Endstations: Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)* Ambient pressure photoemission GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 30-850 eV Monochromator SGM (gratings: 100, 600 lines/mm) Calculated flux (1.9 GeV, 400 mA) up to 1.5 x 1011 photons/sec, energy dependent Resolving power (E/ΔE) <10,000 Scientific disciplines Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry. Endstations Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)*

32

Beamline 12.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

2.0.1 Print 2.0.1 Print EUV optics testing and interferometry, angle- and spin-resolved photoemission Scientific discipline: Applied science, correlated electron systems Endstations: Angle- and spin-resolved photoemission (12.0.1.1) Berkeley Dose Calibration Tool (DCT)(12.0.1.2) SEMATECH Berkeley Microfield Exposure Tool (MET) (12.0.1.3) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 8-cm-period undulator (U8) Energy range See endstation tables Monochromator See endstation tables Endstations Angle- and spin-resolved photoemission (12.0.1.1) SEMATECH Berkeley Microfield Exposure Tool (MET) (12.0.1.2) Berkeley Dose Calibration Tool (DCT)(12.0.1.3) Beamline phone numbers (510) 495-2121 (12.0.1.1)

33

Beamline 12.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Coherent science Scientific disciplines: Applied science, magnetism, materials science Endstations: 12.0.2.1: Coherent optics 12.0.2.2: Coherent x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Third harmonic of 8-cm-period undulator (U8) Energy range 300-1500 eV Monochromator VLS-PGM, with two gratings (600 and 1200 lines/mm) Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 500 eV Resolving power (E/DE) 1,000 Beam size Focused: 70 x 10 µm Unfocused: 200 x 200 µm Endstations 12.0.2.1: Coherent optics 12.0.2.2: Coherent scattering Detectors DetectorsCCD, photodiode, scintillator Scientific applications Branchlines designed for spatially coherent soft x-ray experiments

34

Beamline 12.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Coherent science Scientific disciplines: Applied science, magnetism, materials science Endstations: 12.0.2.1: Coherent optics 12.0.2.2: Coherent x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Third harmonic of 8-cm-period undulator (U8) Energy range 300-1500 eV Monochromator VLS-PGM, with two gratings (600 and 1200 lines/mm) Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 500 eV Resolving power (E/DE) 1,000 Beam size Focused: 70 x 10 µm Unfocused: 200 x 200 µm Endstations 12.0.2.1: Coherent optics 12.0.2.2: Coherent scattering Detectors DetectorsCCD, photodiode, scintillator Scientific applications Branchlines designed for spatially coherent soft x-ray experiments

35

Beamline 11.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print PEEM3, Soft X-Ray Scattering Scientific disciplines: Magnetism, materials, surface science, polymers Endstations: 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 150-2000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 800 eV Resolving power (E/ΔE) 4,000 at 800 eV Endstations 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization

36

Beamline 9.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Chemical and Materials Scientific disciplines: Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry Endstations: Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)* Ambient pressure photoemission GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 30-850 eV Monochromator SGM (gratings: 100, 600 lines/mm) Calculated flux (1.9 GeV, 400 mA) up to 1.5 x 1011 photons/sec, energy dependent Resolving power (E/ΔE) <10,000 Scientific disciplines Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry. Endstations Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)*

37

Beamline 1.4.4  

NLE Websites -- All DOE Office Websites (Extended Search)

4 Print 4 Print Infrared spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.5 eV Frequency range 800 - 10,000 cm-1 Interferometer resolution up to 0.125 cm-1 Endstations Thermo Nicolet Nexus 870 FTIR, Continuum XL IR microscope (N2 purged) Characteristics Computerized sample stage, 0.1-micron resolution; reflection, transmission, and attenuated total reflectance (ATR) modes; differential interference contrast (DIC), polarizing and UV fluorescence optics Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy

38

Beamline 9.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Chemical and Materials Scientific disciplines: Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry Endstations: Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)* Ambient pressure photoemission GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 30-850 eV Monochromator SGM (gratings: 100, 600 lines/mm) Calculated flux (1.9 GeV, 400 mA) up to 1.5 x 1011 photons/sec, energy dependent Resolving power (E/ΔE) <10,000 Scientific disciplines Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry. Endstations Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)*

39

Beamline 1.4.3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 Print 3 Print FTIR spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.2 eV Frequency range 650 - 10,000 cm-1 Interferometer resolution Up to 0.125 cm-1 Endstations Nicolet Magna 760 FTIR, Nic-Plan IR Microscope (N2 purged) Characteristics Motorized sample stage, 0.1-micron resolution, reflection, transmission, and grazing-incidence reflection modes Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy Detectors MCT-A (mercury cadmium telluride) Spot size at sample 2-10 µm (diffraction-limited)

40

Beamline 12.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

0.2 Print 0.2 Print Coherent science Scientific disciplines: Applied science, magnetism, materials science Endstations: 12.0.2.1: Coherent optics 12.0.2.2: Coherent x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Third harmonic of 8-cm-period undulator (U8) Energy range 300-1500 eV Monochromator VLS-PGM, with two gratings (600 and 1200 lines/mm) Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 500 eV Resolving power (E/DE) 1,000 Beam size Focused: 70 x 10 µm Unfocused: 200 x 200 µm Endstations 12.0.2.1: Coherent optics 12.0.2.2: Coherent scattering Detectors DetectorsCCD, photodiode, scintillator Scientific applications Branchlines designed for spatially coherent soft x-ray experiments

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


41

Beamline 9.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Chemical and Materials Scientific disciplines: Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry Endstations: Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)* Ambient pressure photoemission GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 30-850 eV Monochromator SGM (gratings: 100, 600 lines/mm) Calculated flux (1.9 GeV, 400 mA) up to 1.5 x 1011 photons/sec, energy dependent Resolving power (E/ΔE) <10,000 Scientific disciplines Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry. Endstations Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)*

42

Beamline 12.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2.2 Print 2.2 Print High-Pressure (California High-Pressure Science Observatory: Calipso) Endstations: Medium pressure High pressure laser heating GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Superbend magnet, 1.9GeV, 5.29Tesla, 500mA Monochromator Si(111) or Multilayer Energy range 6-40 keV for Si(111), 14-28 keV for Multilayer Resolving power (E/ΔE) Si(111) = 7000, Multilayer =100 Beam size (HxV) Focused: 10 x 10 micron Unfocused: 90 x 100 micron Scientific applications High-pressure science Scientific disciplines Earth sciences, materials science, construction materials, chemistry, energy. Endstations Medium pressure High pressure laser heating Experimental techniques High pressure, diffraction, x-ray imaging, XAS, laser heating

43

Beamline 12.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Coherent science Scientific disciplines: Applied science, magnetism, materials science Endstations: 12.0.2.1: Coherent optics 12.0.2.2: Coherent x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Third harmonic of 8-cm-period undulator (U8) Energy range 300-1500 eV Monochromator VLS-PGM, with two gratings (600 and 1200 lines/mm) Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 500 eV Resolving power (E/DE) 1,000 Beam size Focused: 70 x 10 µm Unfocused: 200 x 200 µm Endstations 12.0.2.1: Coherent optics 12.0.2.2: Coherent scattering Detectors DetectorsCCD, photodiode, scintillator Scientific applications Branchlines designed for spatially coherent soft x-ray experiments

44

Beamline 11.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print PEEM3, Soft X-Ray Scattering Scientific disciplines: Magnetism, materials, surface science, polymers Endstations: 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 150-2000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 800 eV Resolving power (E/ΔE) 4,000 at 800 eV Endstations 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization

45

Beamline 9.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

3.2 Print 3.2 Print Chemical and Materials Scientific disciplines: Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry Endstations: Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)* Ambient pressure photoemission GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 30-850 eV Monochromator SGM (gratings: 100, 600 lines/mm) Calculated flux (1.9 GeV, 400 mA) up to 1.5 x 1011 photons/sec, energy dependent Resolving power (E/ΔE) <10,000 Scientific disciplines Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry. Endstations Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)*

46

Beamline 1.4.3  

NLE Websites -- All DOE Office Websites (Extended Search)

1.4.3 Print 1.4.3 Print FTIR spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.2 eV Frequency range 650 - 10,000 cm-1 Interferometer resolution Up to 0.125 cm-1 Endstations Nicolet Magna 760 FTIR, Nic-Plan IR Microscope (N2 purged) Characteristics Motorized sample stage, 0.1-micron resolution, reflection, transmission, and grazing-incidence reflection modes Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy Detectors MCT-A (mercury cadmium telluride) Spot size at sample

47

Beamline 11.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print PEEM3, Soft X-Ray Scattering Scientific disciplines: Magnetism, materials, surface science, polymers Endstations: 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 150-2000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 800 eV Resolving power (E/ΔE) 4,000 at 800 eV Endstations 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization

48

Beamline 11.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print PEEM3, Soft X-Ray Scattering Scientific disciplines: Magnetism, materials, surface science, polymers Endstations: 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 150-2000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 800 eV Resolving power (E/ΔE) 4,000 at 800 eV Endstations 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization

49

Beamline 12.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Coherent science Scientific disciplines: Applied science, magnetism, materials science Endstations: 12.0.2.1: Coherent optics 12.0.2.2: Coherent x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Third harmonic of 8-cm-period undulator (U8) Energy range 300-1500 eV Monochromator VLS-PGM, with two gratings (600 and 1200 lines/mm) Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 500 eV Resolving power (E/DE) 1,000 Beam size Focused: 70 x 10 µm Unfocused: 200 x 200 µm Endstations 12.0.2.1: Coherent optics 12.0.2.2: Coherent scattering Detectors DetectorsCCD, photodiode, scintillator Scientific applications Branchlines designed for spatially coherent soft x-ray experiments

50

Beamline 1.4.3  

NLE Websites -- All DOE Office Websites (Extended Search)

1.4.3 Print 1.4.3 Print FTIR spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.2 eV Frequency range 650 - 10,000 cm-1 Interferometer resolution Up to 0.125 cm-1 Endstations Nicolet Magna 760 FTIR, Nic-Plan IR Microscope (N2 purged) Characteristics Motorized sample stage, 0.1-micron resolution, reflection, transmission, and grazing-incidence reflection modes Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy Detectors MCT-A (mercury cadmium telluride) Spot size at sample

51

Beamline 1.4.4  

NLE Websites -- All DOE Office Websites (Extended Search)

4 Print 4 Print Infrared spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.5 eV Frequency range 800 - 10,000 cm-1 Interferometer resolution up to 0.125 cm-1 Endstations Thermo Nicolet Nexus 870 FTIR, Continuum XL IR microscope (N2 purged) Characteristics Computerized sample stage, 0.1-micron resolution; reflection, transmission, and attenuated total reflectance (ATR) modes; differential interference contrast (DIC), polarizing and UV fluorescence optics Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy

52

Beamline 12.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2.2 Print 2.2 Print High-Pressure (California High-Pressure Science Observatory: Calipso) Endstations: Medium pressure High pressure laser heating GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Superbend magnet, 1.9GeV, 5.29Tesla, 500mA Monochromator Si(111) or Multilayer Energy range 6-40 keV for Si(111), 14-28 keV for Multilayer Resolving power (E/ΔE) Si(111) = 7000, Multilayer =100 Beam size (HxV) Focused: 10 x 10 micron Unfocused: 90 x 100 micron Scientific applications High-pressure science Scientific disciplines Earth sciences, materials science, construction materials, chemistry, energy. Endstations Medium pressure High pressure laser heating Experimental techniques High pressure, diffraction, x-ray imaging, XAS, laser heating

53

Beamline 1.4.3  

NLE Websites -- All DOE Office Websites (Extended Search)

1.4.3 Print 1.4.3 Print FTIR spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.2 eV Frequency range 650 - 10,000 cm-1 Interferometer resolution Up to 0.125 cm-1 Endstations Nicolet Magna 760 FTIR, Nic-Plan IR Microscope (N2 purged) Characteristics Motorized sample stage, 0.1-micron resolution, reflection, transmission, and grazing-incidence reflection modes Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy Detectors MCT-A (mercury cadmium telluride) Spot size at sample

54

Beamline 11.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print PEEM3, Soft X-Ray Scattering Scientific disciplines: Magnetism, materials, surface science, polymers Endstations: 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 150-2000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 800 eV Resolving power (E/ΔE) 4,000 at 800 eV Endstations 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization

55

Beamline 9.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

3.2 Print 3.2 Print Chemical and Materials Scientific disciplines: Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry Endstations: Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)* Ambient pressure photoemission GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 30-850 eV Monochromator SGM (gratings: 100, 600 lines/mm) Calculated flux (1.9 GeV, 400 mA) up to 1.5 x 1011 photons/sec, energy dependent Resolving power (E/ΔE) <10,000 Scientific disciplines Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry. Endstations Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)*

56

Beamline 11.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print PEEM3, Soft X-Ray Scattering Scientific disciplines: Magnetism, materials, surface science, polymers Endstations: 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 150-2000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 800 eV Resolving power (E/ΔE) 4,000 at 800 eV Endstations 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization

57

Beamline 11.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print PEEM3, Soft X-Ray Scattering Scientific disciplines: Magnetism, materials, surface science, polymers Endstations: 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 150-2000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 800 eV Resolving power (E/ΔE) 4,000 at 800 eV Endstations 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization

58

Beamline 12.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2.2 Print 2.2 Print High-Pressure (California High-Pressure Science Observatory: Calipso) Endstations: Medium pressure High pressure laser heating GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Superbend magnet, 1.9GeV, 5.29Tesla, 500mA Monochromator Si(111) or Multilayer Energy range 6-40 keV for Si(111), 14-28 keV for Multilayer Resolving power (E/ΔE) Si(111) = 7000, Multilayer =100 Beam size (HxV) Focused: 10 x 10 micron Unfocused: 90 x 100 micron Scientific applications High-pressure science Scientific disciplines Earth sciences, materials science, construction materials, chemistry, energy. Endstations Medium pressure High pressure laser heating Experimental techniques High pressure, diffraction, x-ray imaging, XAS, laser heating

59

Beamline 1.4.3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 Print 3 Print FTIR spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.2 eV Frequency range 650 - 10,000 cm-1 Interferometer resolution Up to 0.125 cm-1 Endstations Nicolet Magna 760 FTIR, Nic-Plan IR Microscope (N2 purged) Characteristics Motorized sample stage, 0.1-micron resolution, reflection, transmission, and grazing-incidence reflection modes Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy Detectors MCT-A (mercury cadmium telluride) Spot size at sample 2-10 µm (diffraction-limited)

60

Beamline 11.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print PEEM3, Soft X-Ray Scattering Scientific disciplines: Magnetism, materials, surface science, polymers Endstations: 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 150-2000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 800 eV Resolving power (E/ΔE) 4,000 at 800 eV Endstations 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


61

Beamline 12.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2.2 Print 2.2 Print High-Pressure (California High-Pressure Science Observatory: Calipso) Endstations: Medium pressure High pressure laser heating GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Superbend magnet, 1.9GeV, 5.29Tesla, 500mA Monochromator Si(111) or Multilayer Energy range 6-40 keV for Si(111), 14-28 keV for Multilayer Resolving power (E/ΔE) Si(111) = 7000, Multilayer =100 Beam size (HxV) Focused: 10 x 10 micron Unfocused: 90 x 100 micron Scientific applications High-pressure science Scientific disciplines Earth sciences, materials science, construction materials, chemistry, energy. Endstations Medium pressure High pressure laser heating Experimental techniques High pressure, diffraction, x-ray imaging, XAS, laser heating

62

Beamline 9.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

3.2 Print 3.2 Print Chemical and Materials Scientific disciplines: Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry Endstations: Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)* Ambient pressure photoemission GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 30-850 eV Monochromator SGM (gratings: 100, 600 lines/mm) Calculated flux (1.9 GeV, 400 mA) up to 1.5 x 1011 photons/sec, energy dependent Resolving power (E/ΔE) <10,000 Scientific disciplines Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry. Endstations Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)*

63

Beamline 12.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2.2 Print 2.2 Print High-Pressure (California High-Pressure Science Observatory: Calipso) Endstations: Medium pressure High pressure laser heating GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Superbend magnet, 1.9GeV, 5.29Tesla, 500mA Monochromator Si(111) or Multilayer Energy range 6-40 keV for Si(111), 14-28 keV for Multilayer Resolving power (E/ΔE) Si(111) = 7000, Multilayer =100 Beam size (HxV) Focused: 10 x 10 micron Unfocused: 90 x 100 micron Scientific applications High-pressure science Scientific disciplines Earth sciences, materials science, construction materials, chemistry, energy. Endstations Medium pressure High pressure laser heating Experimental techniques High pressure, diffraction, x-ray imaging, XAS, laser heating

64

Beamline 1.4.3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 Print 3 Print FTIR spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.2 eV Frequency range 650 - 10,000 cm-1 Interferometer resolution Up to 0.125 cm-1 Endstations Nicolet Magna 760 FTIR, Nic-Plan IR Microscope (N2 purged) Characteristics Motorized sample stage, 0.1-micron resolution, reflection, transmission, and grazing-incidence reflection modes Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy Detectors MCT-A (mercury cadmium telluride) Spot size at sample 2-10 µm (diffraction-limited)

65

Beamline 12.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2.2 Print 2.2 Print High-Pressure (California High-Pressure Science Observatory: Calipso) Endstations: Medium pressure High pressure laser heating GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Superbend magnet, 1.9GeV, 5.29Tesla, 500mA Monochromator Si(111) or Multilayer Energy range 6-40 keV for Si(111), 14-28 keV for Multilayer Resolving power (E/ΔE) Si(111) = 7000, Multilayer =100 Beam size (HxV) Focused: 10 x 10 micron Unfocused: 90 x 100 micron Scientific applications High-pressure science Scientific disciplines Earth sciences, materials science, construction materials, chemistry, energy. Endstations Medium pressure High pressure laser heating Experimental techniques High pressure, diffraction, x-ray imaging, XAS, laser heating

66

Beamline 9.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

3.2 Print 3.2 Print Chemical and Materials Scientific disciplines: Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry Endstations: Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)* Ambient pressure photoemission GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 30-850 eV Monochromator SGM (gratings: 100, 600 lines/mm) Calculated flux (1.9 GeV, 400 mA) up to 1.5 x 1011 photons/sec, energy dependent Resolving power (E/ΔE) <10,000 Scientific disciplines Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry. Endstations Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)*

67

Beamline 1.4.3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 Print 3 Print FTIR spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.2 eV Frequency range 650 - 10,000 cm-1 Interferometer resolution Up to 0.125 cm-1 Endstations Nicolet Magna 760 FTIR, Nic-Plan IR Microscope (N2 purged) Characteristics Motorized sample stage, 0.1-micron resolution, reflection, transmission, and grazing-incidence reflection modes Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy Detectors MCT-A (mercury cadmium telluride) Spot size at sample 2-10 µm (diffraction-limited)

68

Beamline 1.4.3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 Print 3 Print FTIR spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.2 eV Frequency range 650 - 10,000 cm-1 Interferometer resolution Up to 0.125 cm-1 Endstations Nicolet Magna 760 FTIR, Nic-Plan IR Microscope (N2 purged) Characteristics Motorized sample stage, 0.1-micron resolution, reflection, transmission, and grazing-incidence reflection modes Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy Detectors MCT-A (mercury cadmium telluride) Spot size at sample 2-10 µm (diffraction-limited)

69

Beamline 9.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Chemical and Materials Scientific disciplines: Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry Endstations: Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)* Ambient pressure photoemission GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 30-850 eV Monochromator SGM (gratings: 100, 600 lines/mm) Calculated flux (1.9 GeV, 400 mA) up to 1.5 x 1011 photons/sec, energy dependent Resolving power (E/ΔE) <10,000 Scientific disciplines Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry. Endstations Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)*

70

Beamline 12.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2.2 Print 2.2 Print High-Pressure (California High-Pressure Science Observatory: Calipso) Endstations: Medium pressure High pressure laser heating GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Superbend magnet, 1.9GeV, 5.29Tesla, 500mA Monochromator Si(111) or Multilayer Energy range 6-40 keV for Si(111), 14-28 keV for Multilayer Resolving power (E/ΔE) Si(111) = 7000, Multilayer =100 Beam size (HxV) Focused: 10 x 10 micron Unfocused: 90 x 100 micron Scientific applications High-pressure science Scientific disciplines Earth sciences, materials science, construction materials, chemistry, energy. Endstations Medium pressure High pressure laser heating Experimental techniques High pressure, diffraction, x-ray imaging, XAS, laser heating

71

Beamline 11.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print PEEM3, Soft X-Ray Scattering Scientific disciplines: Magnetism, materials, surface science, polymers Endstations: 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 150-2000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 800 eV Resolving power (E/ΔE) 4,000 at 800 eV Endstations 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization

72

Beamline 1.4.3  

NLE Websites -- All DOE Office Websites (Extended Search)

1.4.3 Print 1.4.3 Print FTIR spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.2 eV Frequency range 650 - 10,000 cm-1 Interferometer resolution Up to 0.125 cm-1 Endstations Nicolet Magna 760 FTIR, Nic-Plan IR Microscope (N2 purged) Characteristics Motorized sample stage, 0.1-micron resolution, reflection, transmission, and grazing-incidence reflection modes Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy Detectors MCT-A (mercury cadmium telluride) Spot size at sample

73

Beamline 1.4.4  

NLE Websites -- All DOE Office Websites (Extended Search)

4 Print 4 Print Infrared spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.5 eV Frequency range 800 - 10,000 cm-1 Interferometer resolution up to 0.125 cm-1 Endstations Thermo Nicolet Nexus 870 FTIR, Continuum XL IR microscope (N2 purged) Characteristics Computerized sample stage, 0.1-micron resolution; reflection, transmission, and attenuated total reflectance (ATR) modes; differential interference contrast (DIC), polarizing and UV fluorescence optics Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy

74

Beamline 9.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Chemical and Materials Scientific disciplines: Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry Endstations: Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)* Ambient pressure photoemission GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 30-850 eV Monochromator SGM (gratings: 100, 600 lines/mm) Calculated flux (1.9 GeV, 400 mA) up to 1.5 x 1011 photons/sec, energy dependent Resolving power (E/ΔE) <10,000 Scientific disciplines Surfaces, interfaces, catalysis, environmental science, material science, electrochemistry. Endstations Ambient pressure X-ray Photoelectron Spectroscopy (APXPS)*

75

Beamline 1.4.3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 Print 3 Print FTIR spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.2 eV Frequency range 650 - 10,000 cm-1 Interferometer resolution Up to 0.125 cm-1 Endstations Nicolet Magna 760 FTIR, Nic-Plan IR Microscope (N2 purged) Characteristics Motorized sample stage, 0.1-micron resolution, reflection, transmission, and grazing-incidence reflection modes Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy Detectors MCT-A (mercury cadmium telluride) Spot size at sample 2-10 µm (diffraction-limited)

76

Beamline 11.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print PEEM3, Soft X-Ray Scattering Scientific disciplines: Magnetism, materials, surface science, polymers Endstations: 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 150-2000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 800 eV Resolving power (E/ΔE) 4,000 at 800 eV Endstations 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization

77

Beamline 12.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2.2 Print 2.2 Print High-Pressure (California High-Pressure Science Observatory: Calipso) Endstations: Medium pressure High pressure laser heating GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Superbend magnet, 1.9GeV, 5.29Tesla, 500mA Monochromator Si(111) or Multilayer Energy range 6-40 keV for Si(111), 14-28 keV for Multilayer Resolving power (E/ΔE) Si(111) = 7000, Multilayer =100 Beam size (HxV) Focused: 10 x 10 micron Unfocused: 90 x 100 micron Scientific applications High-pressure science Scientific disciplines Earth sciences, materials science, construction materials, chemistry, energy. Endstations Medium pressure High pressure laser heating Experimental techniques High pressure, diffraction, x-ray imaging, XAS, laser heating

78

Beamline 12.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Coherent science Scientific disciplines: Applied science, magnetism, materials science Endstations: 12.0.2.1: Coherent optics 12.0.2.2: Coherent x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Third harmonic of 8-cm-period undulator (U8) Energy range 300-1500 eV Monochromator VLS-PGM, with two gratings (600 and 1200 lines/mm) Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 500 eV Resolving power (E/DE) 1,000 Beam size Focused: 70 x 10 µm Unfocused: 200 x 200 µm Endstations 12.0.2.1: Coherent optics 12.0.2.2: Coherent scattering Detectors DetectorsCCD, photodiode, scintillator Scientific applications Branchlines designed for spatially coherent soft x-ray experiments

79

Beamline 12.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Coherent science Scientific disciplines: Applied science, magnetism, materials science Endstations: 12.0.2.1: Coherent optics 12.0.2.2: Coherent x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Third harmonic of 8-cm-period undulator (U8) Energy range 300-1500 eV Monochromator VLS-PGM, with two gratings (600 and 1200 lines/mm) Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 500 eV Resolving power (E/DE) 1,000 Beam size Focused: 70 x 10 µm Unfocused: 200 x 200 µm Endstations 12.0.2.1: Coherent optics 12.0.2.2: Coherent scattering Detectors DetectorsCCD, photodiode, scintillator Scientific applications Branchlines designed for spatially coherent soft x-ray experiments

80

Beamline 11.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print PEEM3, Soft X-Ray Scattering Scientific disciplines: Magnetism, materials, surface science, polymers Endstations: 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 150-2000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 800 eV Resolving power (E/ΔE) 4,000 at 800 eV Endstations 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
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they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


81

Beamline 1.4.4  

NLE Websites -- All DOE Office Websites (Extended Search)

4 Print 4 Print Infrared spectromicroscopy Scientific disciplines: Biology, correlated electron systems, environmental science, geology, chemistry, polymers, soft materials GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Bend magnet Energy range 0.05-1.5 eV Frequency range 800 - 10,000 cm-1 Interferometer resolution up to 0.125 cm-1 Endstations Thermo Nicolet Nexus 870 FTIR, Continuum XL IR microscope (N2 purged) Characteristics Computerized sample stage, 0.1-micron resolution; reflection, transmission, and attenuated total reflectance (ATR) modes; differential interference contrast (DIC), polarizing and UV fluorescence optics Spatial resolution Diffraction-limited (~wavelength); x-y stage with 0.1 micron accuracy

82

Beamline 12.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2.0.2 Print 2.0.2 Print Coherent science Scientific disciplines: Applied science, magnetism, materials science Endstations: 12.0.2.1: Coherent optics 12.0.2.2: Coherent x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Third harmonic of 8-cm-period undulator (U8) Energy range 300-1500 eV Monochromator VLS-PGM, with two gratings (600 and 1200 lines/mm) Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 500 eV Resolving power (E/DE) 1,000 Beam size Focused: 70 x 10 µm Unfocused: 200 x 200 µm Endstations 12.0.2.1: Coherent optics 12.0.2.2: Coherent scattering Detectors DetectorsCCD, photodiode, scintillator Scientific applications Branchlines designed for spatially coherent soft x-ray experiments

83

Beamline 12.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

0.2 0.2 Beamline 12.0.2 Print Tuesday, 20 October 2009 09:30 Coherent science Scientific disciplines: Applied science, magnetism, materials science Endstations: 12.0.2.1: Coherent optics 12.0.2.2: Coherent x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics Third harmonic of 8-cm-period undulator (U8) Energy range 300-1500 eV Monochromator VLS-PGM, with two gratings (600 and 1200 lines/mm) Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 500 eV Resolving power (E/DE) 1,000 Beam size Focused: 70 x 10 µm Unfocused: 200 x 200 µm Endstations 12.0.2.1: Coherent optics 12.0.2.2: Coherent scattering Detectors DetectorsCCD, photodiode, scintillator Scientific applications Branchlines designed for spatially coherent soft x-ray experiments

84

Beamline 11.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 1 Beamline 11.0.1 Print Tuesday, 20 October 2009 09:16 PEEM3, Soft X-Ray Scattering Scientific disciplines: Magnetism, materials, surface science, polymers Endstations: 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 150-2000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1013 photons/s/0.1%BW at 800 eV Resolving power (E/ΔE) 4,000 at 800 eV Endstations 11.0.1.1: Photoemission electron microscope (PEEM3) 11.0.1.2: Soft x-ray scattering Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization

85

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE) 7000 Scientific disciplines Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system.

86

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

8.0.1 Print 8.0.1 Print Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE) 7000 Scientific disciplines Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system.

87

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE) 7000 Scientific disciplines Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system.

88

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE) 7000 Scientific disciplines Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system.

89

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

8.0.1 Print 8.0.1 Print Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE) 7000 Scientific disciplines Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system.

90

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE) 7000 Scientific disciplines Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system.

91

Beamline 4.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Magnetic spectroscopy Scientific disciplines: Magnetism, materials science Endstations: Eight-pole electromagnet XMCD chamber (6T, 2K) L-edge chamber with superconducting spectrometer GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 100-2000 eV Monochromator Variable-included-angle PGM Calculated flux (1.9 GeV, 400 mA) 1 x 1013 photons/s/0.1%BW at 800 eV [Value reported is the merit function, flux = total flux x (degree of circular polarization)2.] Resolving power (E/ΔE) 5,000-10,000 (at source-size limit; energy-dependent) >25,000 (64 eV, 10-mm entrance/exit slits) Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization.

92

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE) 7000 Scientific disciplines Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system.

93

Beamline 4.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Magnetic spectroscopy Scientific disciplines: Magnetism, materials science Endstations: Eight-pole electromagnet XMCD chamber (6T, 2K) L-edge chamber with superconducting spectrometer GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 100-2000 eV Monochromator Variable-included-angle PGM Calculated flux (1.9 GeV, 400 mA) 1 x 1013 photons/s/0.1%BW at 800 eV [Value reported is the merit function, flux = total flux x (degree of circular polarization)2.] Resolving power (E/ΔE) 5,000-10,000 (at source-size limit; energy-dependent) >25,000 (64 eV, 10-mm entrance/exit slits) Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization.

94

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE) 7000 Scientific disciplines Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system.

95

Beamline 4.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Magnetic spectroscopy Scientific disciplines: Magnetism, materials science Endstations: Eight-pole electromagnet XMCD chamber (6T, 2K) L-edge chamber with superconducting spectrometer GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 100-2000 eV Monochromator Variable-included-angle PGM Calculated flux (1.9 GeV, 400 mA) 1 x 1013 photons/s/0.1%BW at 800 eV [Value reported is the merit function, flux = total flux x (degree of circular polarization)2.] Resolving power (E/ΔE) 5,000-10,000 (at source-size limit; energy-dependent) >25,000 (64 eV, 10-mm entrance/exit slits) Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization.

96

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE) 7000 Scientific disciplines Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system.

97

Beamline 4.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Magnetic spectroscopy Scientific disciplines: Magnetism, materials science Endstations: Eight-pole electromagnet XMCD chamber (6T, 2K) L-edge chamber with superconducting spectrometer GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 100-2000 eV Monochromator Variable-included-angle PGM Calculated flux (1.9 GeV, 400 mA) 1 x 1013 photons/s/0.1%BW at 800 eV [Value reported is the merit function, flux = total flux x (degree of circular polarization)2.] Resolving power (E/ΔE) 5,000-10,000 (at source-size limit; energy-dependent) >25,000 (64 eV, 10-mm entrance/exit slits) Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization.

98

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE) 7000 Scientific disciplines Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system.

99

Beamline 4.0.2  

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4.0.2 Print 4.0.2 Print Magnetic spectroscopy Scientific disciplines: Magnetism, materials science Endstations: Eight-pole electromagnet XMCD chamber (6T, 2K) L-edge chamber with superconducting spectrometer GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 100-2000 eV Monochromator Variable-included-angle PGM Calculated flux (1.9 GeV, 400 mA) 1 x 1013 photons/s/0.1%BW at 800 eV [Value reported is the merit function, flux = total flux x (degree of circular polarization)2.] Resolving power (E/ΔE) 5,000-10,000 (at source-size limit; energy-dependent) >25,000 (64 eV, 10-mm entrance/exit slits) Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization.

100

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE) 7000 Scientific disciplines Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system.

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


101

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

8.0.1 Print 8.0.1 Print Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE) 7000 Scientific disciplines Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system.

102

Beamline 4.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Magnetic spectroscopy Scientific disciplines: Magnetism, materials science Endstations: Eight-pole electromagnet XMCD chamber (6T, 2K) L-edge chamber with superconducting spectrometer GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 100-2000 eV Monochromator Variable-included-angle PGM Calculated flux (1.9 GeV, 400 mA) 1 x 1013 photons/s/0.1%BW at 800 eV [Value reported is the merit function, flux = total flux x (degree of circular polarization)2.] Resolving power (E/ΔE) 5,000-10,000 (at source-size limit; energy-dependent) >25,000 (64 eV, 10-mm entrance/exit slits) Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization.

103

Beamline 8.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

0.1 Print 0.1 Print Surface and materials science, soft x-ray fluorescence (SXF), open port Scientific disciplines: Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system Endstations: 8.0.1.1: Soft x-ray fluorescence (SXF) spectrometer 8.0.1.2: Open port 8.0.1.3: Wet-RIXS 8.0.1.4: Nano-NEXAFS 8.0.1.5: Bio-NEXAFS GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5-cm period undulator (U5) (first, third, and fifth harmonics) Energy range 80-1250 eV Monochromator SGM (gratings: 150, 380, 925 lines/mm) Flux (1.9 GeV, 400 mA) 1011 to 6 x 1015 photons/s (resolution and energy dependent) Resolving power (E/ΔE) 7000 Scientific disciplines Green energy sciences, material sciences, nanosciences, surfaces sciences, correlated electron system.

104

Beamline 4.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Magnetic spectroscopy Scientific disciplines: Magnetism, materials science Endstations: Eight-pole electromagnet XMCD chamber (6T, 2K) L-edge chamber with superconducting spectrometer GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for General Sciences Beamlines (6-month cycle) Source characteristics 5.0-cm period elliptical polarization undulator (EPU5) Energy range 100-2000 eV Monochromator Variable-included-angle PGM Calculated flux (1.9 GeV, 400 mA) 1 x 1013 photons/s/0.1%BW at 800 eV [Value reported is the merit function, flux = total flux x (degree of circular polarization)2.] Resolving power (E/ΔE) 5,000-10,000 (at source-size limit; energy-dependent) >25,000 (64 eV, 10-mm entrance/exit slits) Special notes Polarization is user selectable; linear polarization continuously variable from horizontal to vertical; left and right elliptical (or circular) polarization.

105

ALS Beamlines Directory  

NLE Websites -- All DOE Office Websites (Extended Search)

Beamlines Directory Beamlines Directory ALS Beamlines Directory Print Beamlines, Parameters, Contact Information, and Schedules Download a high-resolution version of the ALS Beamclock. See Beamclock to view the ALS energy-related beamlines beamclock. Beamline Parameters Beamline and endstation technical information is available through the links below. Unless otherwise noted, all beamlines are currently operational. Individual beamline schedules are posted when available. Please contact the responsible beamline scientist for additional schedule information. When calling from off-site, all beamline (BL) phone numbers that begin with a "2" are preceded by 495- (i.e., 495-2014); all others are preceded by 486-. Beamline Number Source Technique/ Group Name Energy Range Beamline Contact Schedule/BL Phone

106

BNL | ATF Beamline Descriptions  

NLE Websites -- All DOE Office Websites (Extended Search)

Beamline Simulation Data and Control Panel Displays Beamline Simulation Data and Control Panel Displays Beamline 0 Beamline 1 Beamline 2 Beamline 0 is directly downstream of the linac and serves to transport the beam from the linac to any one of the three experimental beamlines. Beamline 0 is modeled using MAD. Shown below is a summary of the MAD simulation results. Beamline control system panel (PDF) Transport line control system panel (PDF) MAD input deck Raw output beamline 0 This beam line currently serves the Plasma Acceleration, Current Filamentation Instability and Compton scattering experiments. A summary of the MAD simulation results is shown below. MAD input deck | Output of optical functions | Beamline control system panel (PDF) beamline 1 output ATF beamline 2 previously served the IFEL experiment, the SASE experiment

107

ALS Beamlines Directory  

NLE Websites -- All DOE Office Websites (Extended Search)

Beamlines Directory Print Beamlines Directory Print Beamlines, Parameters, Contact Information, and Schedules Download a high-resolution version of the ALS Beamclock. See Beamclock to view the ALS energy-related beamlines beamclock. Beamline Parameters Beamline and endstation technical information is available through the links below. Unless otherwise noted, all beamlines are currently operational. Individual beamline schedules are posted when available. Please contact the responsible beamline scientist for additional schedule information. When calling from off-site, all beamline (BL) phone numbers that begin with a "2" are preceded by 495- (i.e., 495-2014); all others are preceded by 486-. Beamline Number Source Technique/ Group Name Energy Range Beamline Contact Schedule/BL Phone

108

ALS Beamlines Directory  

NLE Websites -- All DOE Office Websites (Extended Search)

ALS Beamlines Directory Print ALS Beamlines Directory Print Beamlines, Parameters, Contact Information, and Schedules Download a high-resolution version of the ALS Beamclock. See Beamclock to view the ALS energy-related beamlines beamclock. Beamline Parameters Beamline and endstation technical information is available through the links below. Unless otherwise noted, all beamlines are currently operational. Individual beamline schedules are posted when available. Please contact the responsible beamline scientist for additional schedule information. When calling from off-site, all beamline (BL) phone numbers that begin with a "2" are preceded by 495- (i.e., 495-2014); all others are preceded by 486-. Beamline Number Source Technique/ Group Name Energy Range Beamline Contact Schedule/BL Phone

109

ALS Beamlines Directory  

NLE Websites -- All DOE Office Websites (Extended Search)

ALS Beamlines Directory Print ALS Beamlines Directory Print Beamlines, Parameters, Contact Information, and Schedules Download a high-resolution version of the ALS Beamclock. See Beamclock to view the ALS energy-related beamlines beamclock. Beamline Parameters Beamline and endstation technical information is available through the links below. Unless otherwise noted, all beamlines are currently operational. Individual beamline schedules are posted when available. Please contact the responsible beamline scientist for additional schedule information. When calling from off-site, all beamline (BL) phone numbers that begin with a "2" are preceded by 495- (i.e., 495-2014); all others are preceded by 486-. Beamline Number Source Technique/ Group Name Energy Range Beamline Contact Schedule/BL Phone

110

ALS Beamlines Directory  

NLE Websites -- All DOE Office Websites (Extended Search)

Beamlines Directory Print Beamlines Directory Print Beamlines, Parameters, Contact Information, and Schedules Download a high-resolution version of the ALS Beamclock. See Beamclock to view the ALS energy-related beamlines beamclock. Beamline Parameters Beamline and endstation technical information is available through the links below. Unless otherwise noted, all beamlines are currently operational. Individual beamline schedules are posted when available. Please contact the responsible beamline scientist for additional schedule information. When calling from off-site, all beamline (BL) phone numbers that begin with a "2" are preceded by 495- (i.e., 495-2014); all others are preceded by 486-. Beamline Number Source Technique/ Group Name Energy Range Beamline Contact Schedule/BL Phone

111

Beamline 12.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 1 Beamline 12.3.1 Print Tuesday, 20 October 2009 09:33 Structurally Integrated Biology for Life Sciences (SIBYLS) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend Energy range 5-17 keV (1% max flux) Frequency range 2.5-0.73 Angstrom wavelength Beam size 100 µm round beam default 10 µm and 30 µm collimators available for small samples with flux reduced to 1% and 12%, respectively. 120 µm x 120 µm Gaussian uncollimated beam shape at sample. Scientific discipline Structural biology Monochromator #1 Si(111) Double crystal Calculated flux (1.9 GeV, 400 mA) 2.5 x 1011 photons/sec at 11 keV Resolving power (E/ΔE) 7000 Monochromator #2

112

Beamline 5.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 1 Beamline 5.0.1 Print Tuesday, 20 October 2009 08:32 Berkeley Center for Structural Biology (BCSB) Monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm-period wiggler (W11) Energy range 12.7 keV (fixed) Monochromator Si(220) Asymmetric cut single crystal Measured flux 1.50 x 1011 photons/s at 400-mA ring current, with 1.5-mrad divergence and 100-µm pinhole collimator Resolving power (E/ΔE) ~10,000 Divergence at sample 3.0 (h) x 0.4 (v) mrad (user selectable) Spot size 100 µm Endstations Standard hutch Detectors 3 x 3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules

113

Beamline 12.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

3.1 3.1 Beamline 12.3.1 Print Tuesday, 20 October 2009 09:33 Structurally Integrated Biology for Life Sciences (SIBYLS) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend Energy range 5-17 keV (1% max flux) Frequency range 2.5-0.73 Angstrom wavelength Beam size 100 µm round beam default 10 µm and 30 µm collimators available for small samples with flux reduced to 1% and 12%, respectively. 120 µm x 120 µm Gaussian uncollimated beam shape at sample. Scientific discipline Structural biology Monochromator #1 Si(111) Double crystal Calculated flux (1.9 GeV, 400 mA) 2.5 x 1011 photons/sec at 11 keV Resolving power (E/ΔE) 7000

114

Beamline 12.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

2.3.1 2.3.1 Beamline 12.3.1 Print Tuesday, 20 October 2009 09:33 Structurally Integrated Biology for Life Sciences (SIBYLS) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend Energy range 5-17 keV (1% max flux) Frequency range 2.5-0.73 Angstrom wavelength Beam size 100 µm round beam default 10 µm and 30 µm collimators available for small samples with flux reduced to 1% and 12%, respectively. 120 µm x 120 µm Gaussian uncollimated beam shape at sample. Scientific discipline Structural biology Monochromator #1 Si(111) Double crystal Calculated flux (1.9 GeV, 400 mA) 2.5 x 1011 photons/sec at 11 keV Resolving power (E/ΔE) 7000

115

Beamline 5.0.3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 3 Beamline 5.0.3 Print Tuesday, 20 October 2009 08:36 Berkeley Center for Structural Biology (BCSB) Monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm-period wiggler (W11) Energy range 12,700 eV(fixed) Monochromator Asymmetric cut single crystal Si(220) Measured flux 2.4 x 1011 photons/s at 400-mA ring current, with 1.5-mrad divergence and 100-µm pinhole collimator Divergence at sample 3.0 (h) x 0.4 (v) mrad (user selectable) Spot size 100 µm Endstations Standard hutch Detectors 3 x 3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available; automated sample mounting system

116

Beamline 5.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

5.0.2 5.0.2 Beamline 5.0.2 Print Tuesday, 20 October 2009 08:35 Berkeley Center for Structural Biology (BCSB) Multiple-wavelength anomalous diffraction (MAD) and monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm period wiggler (W11) Energy range 5-16 keV Monochromator Double-crystal, Si(111) liquid N2 cooled Measured flux at 12.4 keV 8.0 x 1011 photons/s at 400-mA ring current, with 1.5-mrad convergence and 100-µm pinhole collimator Resolving power (E/ΔE) 7,000 Divergence at sample 3.0(h) x 0.4 (v) mrad (user selectable) Spot size 25-125 µm (user selectable) Endstations Standard hutch Characteristics

117

Beamline 5.0.3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 3 Beamline 5.0.3 Print Tuesday, 20 October 2009 08:36 Berkeley Center for Structural Biology (BCSB) Monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm-period wiggler (W11) Energy range 12,700 eV(fixed) Monochromator Asymmetric cut single crystal Si(220) Measured flux 2.4 x 1011 photons/s at 400-mA ring current, with 1.5-mrad divergence and 100-µm pinhole collimator Divergence at sample 3.0 (h) x 0.4 (v) mrad (user selectable) Spot size 100 µm Endstations Standard hutch Detectors 3 x 3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available; automated sample mounting system

118

Beamline Temperatures  

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Temperatures Temperatures Energy: 3.0000 GeV Current: 493.2242 mA Date: 11-Jan-2014 21:40:00 Beamline Temperatures Energy 3.0000 GeV Current 493.2 mA 11-Jan-2014 21:40:00 LN:MainTankLevel 124.4 in LN:MainTankPress 56.9 psi SPEAR-BL:B120HeFlow 15.4 l/min SPEAR-BL:B131HeFlow 22.2 l/min BL 4 BL02:LCW 0.0 ℃ BL02:M0_LCW 31.5 ℃ BL 4-1 BL04-1:BasePlate -14.0 ℃ BL04-1:Bottom1 46.0 ℃ BL04-1:Bottom2 47.0 ℃ BL04-1:Lower 32.0 ℃ BL04-1:Moly 46.0 ℃ BL04-1:ChinGuard1 31.0 ℃ BL04-1:ChinGuard2 31.0 ℃ BL04-1:FirstXtalA -167.0 ℃ BL04-1:FirstXtalB -172.0 ℃ BL04-1:Pad1 31.0 ℃ BL04-1:Pad2 31.0 ℃ BL04-1:SecondXtalA -177.0 ℃ BL04-1:SecondXtalB -175.0 ℃ BL 4-2 BL04-2:BasePlate -14.0 ℃ BL04-2:Bottom1 24.0 ℃ BL04-2:Bottom2 25.0 ℃

119

Final Beamline Design Report  

NLE Websites -- All DOE Office Websites (Extended Search)

Final Beamline Design Report Final Beamline Design Report Guidelines and Review Criteria (SCD 1.20.95) 6.0 Final Beamline Design Report (FDR) Overview The Final Beamline Design Report is part of the Advanced Photon Source (APS) beamline review process and should be planned for when approximately 90% of the total beamline design has been completed. Fifteen copies of the FDR are to be submitted to the APS Users Office. Approval of the Collaborative Access Team's (CAT) designs described in the report is required prior to installation of beamline components in the APS Experiment Hall. Components that have a long lead time for design or procurement can be reviewed separately from the remainder of the beamline, but enough information must be provided so that the reviewer can understand the

120

Beamline 12.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Structurally Integrated Biology for Life Sciences (SIBYLS) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend Energy range 5-17 keV (1% max flux) Frequency range 2.5-0.73 Angstrom wavelength Beam size 100 µm round beam default 10 µm and 30 µm collimators available for small samples with flux reduced to 1% and 12%, respectively. 120 µm x 120 µm Gaussian uncollimated beam shape at sample. Scientific discipline Structural biology Monochromator #1 Si(111) Double crystal Calculated flux (1.9 GeV, 400 mA) 2.5 x 1011 photons/sec at 11 keV Resolving power (E/ΔE) 7000 Monochromator #2 0.6% bandpass multilayers Calculated flux (1.9 GeV, 400 mA)

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


121

Beamline 5.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Berkeley Center for Structural Biology (BCSB) Monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm-period wiggler (W11) Energy range 12.7 keV (fixed) Monochromator Si(220) Asymmetric cut single crystal Measured flux 1.50 x 1011 photons/s at 400-mA ring current, with 1.5-mrad divergence and 100-µm pinhole collimator Resolving power (E/ΔE) ~10,000 Divergence at sample 3.0 (h) x 0.4 (v) mrad (user selectable) Spot size 100 µm Endstations Standard hutch Detectors 3 x 3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available

122

Beamline 8.2.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Berkeley Center for Structural Biology (BCSB) Multiple-Wavelength Anomalous Diffraction (MAD) and Macromolecular Crystallography (MX) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend magnet (5.0 T, single pole) Energy range 5-16 keV Monochromator Double crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 3.0 x 1011 photons/sec Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0 (h) x 0.5 (v) mrad Measured spot size (FWHM) 100 µm Endstations Minihutch Detectors 3x3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available Sample environment Ambient or ~100 K

123

Beamline 5.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Berkeley Center for Structural Biology (BCSB) Multiple-wavelength anomalous diffraction (MAD) and monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm period wiggler (W11) Energy range 5-16 keV Monochromator Double-crystal, Si(111) liquid N2 cooled Measured flux at 12.4 keV 8.0 x 1011 photons/s at 400-mA ring current, with 1.5-mrad convergence and 100-µm pinhole collimator Resolving power (E/ΔE) 7,000 Divergence at sample 3.0(h) x 0.4 (v) mrad (user selectable) Spot size 25-125 µm (user selectable) Endstations Standard hutch Characteristics Single axis, air bearing goniometer; CCD detector, low-temperature system

124

Beamline 8.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Berkeley Center for Structural Biology (BCSB) Multiple-Wavelength Anomalous Diffraction (MAD) and Macromolecular Crystallography (MX) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend (5.0 T, single pole) Energy range 5-16 keV Monochromator Double crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 3.0 x 1011 photons/sec Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0(h) x 0.5(v) mrad Measured spot size at sample (FWHM) 100 µm Endstations Minihutch Detectors 3x3 CCD array (ADSC Q315) Sample format Single crystals of biological molecules Sample preparation Support labs available Sample environment Ambient or ~100 K Special notes Computers for data processing and analysis are available

125

Beamline 5.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Berkeley Center for Structural Biology (BCSB) Multiple-wavelength anomalous diffraction (MAD) and monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm period wiggler (W11) Energy range 5-16 keV Monochromator Double-crystal, Si(111) liquid N2 cooled Measured flux at 12.4 keV 8.0 x 1011 photons/s at 400-mA ring current, with 1.5-mrad convergence and 100-µm pinhole collimator Resolving power (E/ΔE) 7,000 Divergence at sample 3.0(h) x 0.4 (v) mrad (user selectable) Spot size 25-125 µm (user selectable) Endstations Standard hutch Characteristics Single axis, air bearing goniometer; CCD detector, low-temperature system

126

Beamline 5.0.3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 Print 3 Print Berkeley Center for Structural Biology (BCSB) Monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm-period wiggler (W11) Energy range 12,700 eV(fixed) Monochromator Asymmetric cut single crystal Si(220) Measured flux 2.4 x 1011 photons/s at 400-mA ring current, with 1.5-mrad divergence and 100-µm pinhole collimator Divergence at sample 3.0 (h) x 0.4 (v) mrad (user selectable) Spot size 100 µm Endstations Standard hutch Detectors 3 x 3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available; automated sample mounting system

127

Beamline 5.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Berkeley Center for Structural Biology (BCSB) Multiple-wavelength anomalous diffraction (MAD) and monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm period wiggler (W11) Energy range 5-16 keV Monochromator Double-crystal, Si(111) liquid N2 cooled Measured flux at 12.4 keV 8.0 x 1011 photons/s at 400-mA ring current, with 1.5-mrad convergence and 100-µm pinhole collimator Resolving power (E/ΔE) 7,000 Divergence at sample 3.0(h) x 0.4 (v) mrad (user selectable) Spot size 25-125 µm (user selectable) Endstations Standard hutch Characteristics Single axis, air bearing goniometer; CCD detector, low-temperature system

128

Beamline 8.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Berkeley Center for Structural Biology (BCSB) Multiple-Wavelength Anomalous Diffraction (MAD) and Macromolecular Crystallography (MX) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend (5.0 T, single pole) Energy range 5-16 keV Monochromator Double crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 3.0 x 1011 photons/sec Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0(h) x 0.5(v) mrad Measured spot size at sample (FWHM) 100 µm Endstations Minihutch Detectors 3x3 CCD array (ADSC Q315) Sample format Single crystals of biological molecules Sample preparation Support labs available Sample environment Ambient or ~100 K Special notes Computers for data processing and analysis are available

129

Beamline 8.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Berkeley Center for Structural Biology (BCSB) Multiple-Wavelength Anomalous Diffraction (MAD) and Macromolecular Crystallography (MX) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend (5.0 T, single pole) Energy range 5-16 keV Monochromator Double crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 3.0 x 1011 photons/sec Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0(h) x 0.5(v) mrad Measured spot size at sample (FWHM) 100 µm Endstations Minihutch Detectors 3x3 CCD array (ADSC Q315) Sample format Single crystals of biological molecules Sample preparation Support labs available Sample environment Ambient or ~100 K Special notes Computers for data processing and analysis are available

130

Beamline 8.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Berkeley Center for Structural Biology (BCSB) Multiple-Wavelength Anomalous Diffraction (MAD) and Macromolecular Crystallography (MX) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend (5.0 T, single pole) Energy range 5-16 keV Monochromator Double crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 3.0 x 1011 photons/sec Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0(h) x 0.5(v) mrad Measured spot size at sample (FWHM) 100 µm Endstations Minihutch Detectors 3x3 CCD array (ADSC Q315) Sample format Single crystals of biological molecules Sample preparation Support labs available Sample environment Ambient or ~100 K Special notes Computers for data processing and analysis are available

131

Beamline 5.0.3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 Print 3 Print Berkeley Center for Structural Biology (BCSB) Monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm-period wiggler (W11) Energy range 12,700 eV(fixed) Monochromator Asymmetric cut single crystal Si(220) Measured flux 2.4 x 1011 photons/s at 400-mA ring current, with 1.5-mrad divergence and 100-µm pinhole collimator Divergence at sample 3.0 (h) x 0.4 (v) mrad (user selectable) Spot size 100 µm Endstations Standard hutch Detectors 3 x 3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available; automated sample mounting system

132

Beamline 5.0.3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 Print 3 Print Berkeley Center for Structural Biology (BCSB) Monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm-period wiggler (W11) Energy range 12,700 eV(fixed) Monochromator Asymmetric cut single crystal Si(220) Measured flux 2.4 x 1011 photons/s at 400-mA ring current, with 1.5-mrad divergence and 100-µm pinhole collimator Divergence at sample 3.0 (h) x 0.4 (v) mrad (user selectable) Spot size 100 µm Endstations Standard hutch Detectors 3 x 3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available; automated sample mounting system

133

Beamline 5.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Berkeley Center for Structural Biology (BCSB) Monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm-period wiggler (W11) Energy range 12.7 keV (fixed) Monochromator Si(220) Asymmetric cut single crystal Measured flux 1.50 x 1011 photons/s at 400-mA ring current, with 1.5-mrad divergence and 100-µm pinhole collimator Resolving power (E/ΔE) ~10,000 Divergence at sample 3.0 (h) x 0.4 (v) mrad (user selectable) Spot size 100 µm Endstations Standard hutch Detectors 3 x 3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available

134

Beamline 5.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Berkeley Center for Structural Biology (BCSB) Monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm-period wiggler (W11) Energy range 12.7 keV (fixed) Monochromator Si(220) Asymmetric cut single crystal Measured flux 1.50 x 1011 photons/s at 400-mA ring current, with 1.5-mrad divergence and 100-µm pinhole collimator Resolving power (E/ΔE) ~10,000 Divergence at sample 3.0 (h) x 0.4 (v) mrad (user selectable) Spot size 100 µm Endstations Standard hutch Detectors 3 x 3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available

135

Beamline 8.2.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Berkeley Center for Structural Biology (BCSB) Multiple-Wavelength Anomalous Diffraction (MAD) and Macromolecular Crystallography (MX) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend magnet (5.0 T, single pole) Energy range 5-16 keV Monochromator Double crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 3.0 x 1011 photons/sec Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0 (h) x 0.5 (v) mrad Measured spot size (FWHM) 100 µm Endstations Minihutch Detectors 3x3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available Sample environment Ambient or ~100 K

136

Beamline 8.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Multiple-wavelength anomalous diffraction (MAD) and macromolecular crystallography (MX) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend magnet (5.0 tesla, single pole) Energy range 5-17 keV (1% max flux) Monochromator Double flat crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 2.5 x 1011 at 11 keV Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0 (h) x 0.35 (v) mrad Endstations Minihutch Detectors 3 x 3 CCD array (ADSC Q315r) Measured spot size at sample (FWHM) 0.120 (h) x 0.108 (v) mm Sample format Single crystals of biological molecules. Crystallization tray goniometer available with prior arrangement.

137

Beamline 5.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Berkeley Center for Structural Biology (BCSB) Monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm-period wiggler (W11) Energy range 12.7 keV (fixed) Monochromator Si(220) Asymmetric cut single crystal Measured flux 1.50 x 1011 photons/s at 400-mA ring current, with 1.5-mrad divergence and 100-µm pinhole collimator Resolving power (E/ΔE) ~10,000 Divergence at sample 3.0 (h) x 0.4 (v) mrad (user selectable) Spot size 100 µm Endstations Standard hutch Detectors 3 x 3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available

138

Beamline 8.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Berkeley Center for Structural Biology (BCSB) Multiple-Wavelength Anomalous Diffraction (MAD) and Macromolecular Crystallography (MX) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend (5.0 T, single pole) Energy range 5-16 keV Monochromator Double crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 3.0 x 1011 photons/sec Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0(h) x 0.5(v) mrad Measured spot size at sample (FWHM) 100 µm Endstations Minihutch Detectors 3x3 CCD array (ADSC Q315) Sample format Single crystals of biological molecules Sample preparation Support labs available Sample environment Ambient or ~100 K Special notes Computers for data processing and analysis are available

139

Beamline 8.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Multiple-wavelength anomalous diffraction (MAD) and macromolecular crystallography (MX) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend magnet (5.0 tesla, single pole) Energy range 5-17 keV (1% max flux) Monochromator Double flat crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 2.5 x 1011 at 11 keV Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0 (h) x 0.35 (v) mrad Endstations Minihutch Detectors 3 x 3 CCD array (ADSC Q315r) Measured spot size at sample (FWHM) 0.120 (h) x 0.108 (v) mm Sample format Single crystals of biological molecules. Crystallization tray goniometer available with prior arrangement.

140

Beamline 8.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Berkeley Center for Structural Biology (BCSB) Multiple-Wavelength Anomalous Diffraction (MAD) and Macromolecular Crystallography (MX) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend (5.0 T, single pole) Energy range 5-16 keV Monochromator Double crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 3.0 x 1011 photons/sec Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0(h) x 0.5(v) mrad Measured spot size at sample (FWHM) 100 µm Endstations Minihutch Detectors 3x3 CCD array (ADSC Q315) Sample format Single crystals of biological molecules Sample preparation Support labs available Sample environment Ambient or ~100 K Special notes Computers for data processing and analysis are available

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


141

Beamline 5.0.3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 Print 3 Print Berkeley Center for Structural Biology (BCSB) Monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm-period wiggler (W11) Energy range 12,700 eV(fixed) Monochromator Asymmetric cut single crystal Si(220) Measured flux 2.4 x 1011 photons/s at 400-mA ring current, with 1.5-mrad divergence and 100-µm pinhole collimator Divergence at sample 3.0 (h) x 0.4 (v) mrad (user selectable) Spot size 100 µm Endstations Standard hutch Detectors 3 x 3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available; automated sample mounting system

142

Beamline 8.2.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Berkeley Center for Structural Biology (BCSB) Multiple-Wavelength Anomalous Diffraction (MAD) and Macromolecular Crystallography (MX) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend magnet (5.0 T, single pole) Energy range 5-16 keV Monochromator Double crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 3.0 x 1011 photons/sec Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0 (h) x 0.5 (v) mrad Measured spot size (FWHM) 100 µm Endstations Minihutch Detectors 3x3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available Sample environment Ambient or ~100 K

143

Beamline 8.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Multiple-wavelength anomalous diffraction (MAD) and macromolecular crystallography (MX) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend magnet (5.0 tesla, single pole) Energy range 5-17 keV (1% max flux) Monochromator Double flat crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 2.5 x 1011 at 11 keV Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0 (h) x 0.35 (v) mrad Endstations Minihutch Detectors 3 x 3 CCD array (ADSC Q315r) Measured spot size at sample (FWHM) 0.120 (h) x 0.108 (v) mm Sample format Single crystals of biological molecules. Crystallization tray goniometer available with prior arrangement.

144

Beamline 8.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Berkeley Center for Structural Biology (BCSB) Multiple-Wavelength Anomalous Diffraction (MAD) and Macromolecular Crystallography (MX) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend (5.0 T, single pole) Energy range 5-16 keV Monochromator Double crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 3.0 x 1011 photons/sec Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0(h) x 0.5(v) mrad Measured spot size at sample (FWHM) 100 µm Endstations Minihutch Detectors 3x3 CCD array (ADSC Q315) Sample format Single crystals of biological molecules Sample preparation Support labs available Sample environment Ambient or ~100 K Special notes Computers for data processing and analysis are available

145

Beamline 5.0.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Berkeley Center for Structural Biology (BCSB) Monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm-period wiggler (W11) Energy range 12.7 keV (fixed) Monochromator Si(220) Asymmetric cut single crystal Measured flux 1.50 x 1011 photons/s at 400-mA ring current, with 1.5-mrad divergence and 100-µm pinhole collimator Resolving power (E/ΔE) ~10,000 Divergence at sample 3.0 (h) x 0.4 (v) mrad (user selectable) Spot size 100 µm Endstations Standard hutch Detectors 3 x 3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available

146

Beamline 12.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Structurally Integrated Biology for Life Sciences (SIBYLS) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend Energy range 5-17 keV (1% max flux) Frequency range 2.5-0.73 Angstrom wavelength Beam size 100 µm round beam default 10 µm and 30 µm collimators available for small samples with flux reduced to 1% and 12%, respectively. 120 µm x 120 µm Gaussian uncollimated beam shape at sample. Scientific discipline Structural biology Monochromator #1 Si(111) Double crystal Calculated flux (1.9 GeV, 400 mA) 2.5 x 1011 photons/sec at 11 keV Resolving power (E/ΔE) 7000 Monochromator #2 0.6% bandpass multilayers Calculated flux (1.9 GeV, 400 mA)

147

Beamline 12.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Structurally Integrated Biology for Life Sciences (SIBYLS) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend Energy range 5-17 keV (1% max flux) Frequency range 2.5-0.73 Angstrom wavelength Beam size 100 µm round beam default 10 µm and 30 µm collimators available for small samples with flux reduced to 1% and 12%, respectively. 120 µm x 120 µm Gaussian uncollimated beam shape at sample. Scientific discipline Structural biology Monochromator #1 Si(111) Double crystal Calculated flux (1.9 GeV, 400 mA) 2.5 x 1011 photons/sec at 11 keV Resolving power (E/ΔE) 7000 Monochromator #2 0.6% bandpass multilayers Calculated flux (1.9 GeV, 400 mA)

148

Beamline 8.2.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Berkeley Center for Structural Biology (BCSB) Multiple-Wavelength Anomalous Diffraction (MAD) and Macromolecular Crystallography (MX) GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend (5.0 T, single pole) Energy range 5-16 keV Monochromator Double crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 3.0 x 1011 photons/sec Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0(h) x 0.5(v) mrad Measured spot size at sample (FWHM) 100 µm Endstations Minihutch Detectors 3x3 CCD array (ADSC Q315) Sample format Single crystals of biological molecules Sample preparation Support labs available Sample environment Ambient or ~100 K Special notes Computers for data processing and analysis are available

149

Beamline 5.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Berkeley Center for Structural Biology (BCSB) Multiple-wavelength anomalous diffraction (MAD) and monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm period wiggler (W11) Energy range 5-16 keV Monochromator Double-crystal, Si(111) liquid N2 cooled Measured flux at 12.4 keV 8.0 x 1011 photons/s at 400-mA ring current, with 1.5-mrad convergence and 100-µm pinhole collimator Resolving power (E/ΔE) 7,000 Divergence at sample 3.0(h) x 0.4 (v) mrad (user selectable) Spot size 25-125 µm (user selectable) Endstations Standard hutch Characteristics Single axis, air bearing goniometer; CCD detector, low-temperature system

150

Beamline 5.0.3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 Print 3 Print Berkeley Center for Structural Biology (BCSB) Monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm-period wiggler (W11) Energy range 12,700 eV(fixed) Monochromator Asymmetric cut single crystal Si(220) Measured flux 2.4 x 1011 photons/s at 400-mA ring current, with 1.5-mrad divergence and 100-µm pinhole collimator Divergence at sample 3.0 (h) x 0.4 (v) mrad (user selectable) Spot size 100 µm Endstations Standard hutch Detectors 3 x 3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available; automated sample mounting system

151

Beamline 8.2.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Berkeley Center for Structural Biology (BCSB) Multiple-Wavelength Anomalous Diffraction (MAD) and Macromolecular Crystallography (MX) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend magnet (5.0 T, single pole) Energy range 5-16 keV Monochromator Double crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 3.0 x 1011 photons/sec Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0 (h) x 0.5 (v) mrad Measured spot size (FWHM) 100 µm Endstations Minihutch Detectors 3x3 CCD array (ADSC Q315R) Sample format Single crystals of biological molecules Sample preparation Support labs available Sample environment Ambient or ~100 K

152

Beamline 8.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

3.1 Print 3.1 Print Multiple-wavelength anomalous diffraction (MAD) and macromolecular crystallography (MX) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend magnet (5.0 tesla, single pole) Energy range 5-17 keV (1% max flux) Monochromator Double flat crystal, Si(111) Measured flux (1.9 GeV, 400 mA) 2.5 x 1011 at 11 keV Resolving power (E/ΔE) 7,000 Divergence (max at sample) 3.0 (h) x 0.35 (v) mrad Endstations Minihutch Detectors 3 x 3 CCD array (ADSC Q315r) Measured spot size at sample (FWHM) 0.120 (h) x 0.108 (v) mm Sample format Single crystals of biological molecules. Crystallization tray goniometer available with prior arrangement.

153

Beamline 12.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

12.3.1 Print 12.3.1 Print Structurally Integrated Biology for Life Sciences (SIBYLS) Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics Superbend Energy range 5-17 keV (1% max flux) Frequency range 2.5-0.73 Angstrom wavelength Beam size 100 µm round beam default 10 µm and 30 µm collimators available for small samples with flux reduced to 1% and 12%, respectively. 120 µm x 120 µm Gaussian uncollimated beam shape at sample. Scientific discipline Structural biology Monochromator #1 Si(111) Double crystal Calculated flux (1.9 GeV, 400 mA) 2.5 x 1011 photons/sec at 11 keV Resolving power (E/ΔE) 7000 Monochromator #2 0.6% bandpass multilayers Calculated flux (1.9 GeV, 400 mA)

154

Beamline 5.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Berkeley Center for Structural Biology (BCSB) Multiple-wavelength anomalous diffraction (MAD) and monochromatic protein crystallography Scientific discipline: Structural biology GENERAL BEAMLINE INFORMATION Operational Yes Proposal cycle Proposals for Structural Biology Beamlines (2-month cycle) Source characteristics 11.4-cm period wiggler (W11) Energy range 5-16 keV Monochromator Double-crystal, Si(111) liquid N2 cooled Measured flux at 12.4 keV 8.0 x 1011 photons/s at 400-mA ring current, with 1.5-mrad convergence and 100-µm pinhole collimator Resolving power (E/ΔE) 7,000 Divergence at sample 3.0(h) x 0.4 (v) mrad (user selectable) Spot size 25-125 µm (user selectable) Endstations Standard hutch Characteristics Single axis, air bearing goniometer; CCD detector, low-temperature system

155

Hutch for CSX Beamlines  

ScienceCinema (OSTI)

NSLS-II will produce x-rays 10,000 times brighter than NSLS. To keep people safe from intense x-rays in the new facility, special enclosures, called hutches, will surround particular sections of beamlines.

Ed Haas

2013-07-17T23:59:59.000Z

156

ROTIGOTINE TRANSDERMAL PATCH IS EFFECTIVE IN THE TREATMENT OF IDIOPATHIC RLS: RESULTS OF A 6-MONTH,  

E-Print Network (OSTI)

ROTIGOTINE TRANSDERMAL PATCH IS EFFECTIVE IN THE TREATMENT OF IDIOPATHIC RLS: RESULTS OF A 6-MONTH of the SP792 study group Objective: To evaluate efficacy and safety of rotigotine transdermal patch. Conclusion: Therapy with rotigotine transdermal patch in doses of 2 and 3 mg/24h over a period of 6 months

Lichtarge, Olivier

157

APS 7-BM Beamline: Beamline Controls and Data Handling  

NLE Websites -- All DOE Office Websites (Extended Search)

Beamline Controls and Data Acquisition Beamline Controls and Data Acquisition Beamline controls operate through EPICS, with the standard MEDM graphical interface. When needed, Python is used for scripting, based on the PyEpics implementation written by CARS. The beamline workstation has access to the Enthought Python Distribution, which includes many common Python packages, such as numpy, scipy, h5py, and others. Data formats Time resolved data collected at the beamline are typically stored in a locally-defined binary data file. For distribution to users, these files are converted to HDF5, a widely used, hierarchical binary data format that can be accessed using tools in a wide variety of programming languages. Other formats can potentially be accommodated upon request; please contact beamline staff prior to your beamtime if a different format is needed.

158

Beamline 7.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Diagnostic beamline GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range Port 1: ~17 keV transmission though Mo filters Port 2: IR-visible from large-angle synchrotron radiation; UV-x-ray for beam position monitor (BPM) Endstations Port 1: Hard x-ray to visible converter (phosphor) Port 2: None (available for temporary experiments) Both ports are inside the ALS shielding. Characteristics Port 1: Pinhole-based x-ray system for transverse measurements Port 2: IR/visible port available for temporary experiments; x-ray BPM based on electron secondary emission induced in metallic blades by synchrotron radiation Spatial resolution Port 1: <25 µm transverse Port 2: ~1 µm position; <1 µrad angle (x-ray BPM)

159

BNL | ATF Beamline Parameters  

NLE Websites -- All DOE Office Websites (Extended Search)

Beamline Parameters Beamline Parameters Electron beam energy: 25 to 76 MeV Temporal structure: Macropulse length: 3 microseconds Macropulse repetition rate from under 1 PPS to 3 PPS. Micropulse repetition period 12.25 ns or 24.5 ns. Micropulse length variable from about 1 ps FWHM to 10 ps FWHM. Electron beam charge: continuously variable. Single micropulse charge from zero to a few nanoculombs. Bunch train charge up to about 10 nanoculombs. Emittance: depends on various conditions, e.g. peak current, gun field, microbunch length etc. At 1 nC we have measured the emittance at 2.6 mm mrad (rms normalized) at a bunch length of 10 ps FWHM. The local emittance (Slice Emittance) is smaller, measured 1.4 mm mrad for a slice out of the 1 nC bunch. Stability: (approx.) 1 ps in short term phase, 1% of beam diameter

160

Beamline 7.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Diagnostic beamline GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range Port 1: ~17 keV transmission though Mo filters Port 2: IR-visible from large-angle synchrotron radiation; UV-x-ray for beam position monitor (BPM) Endstations Port 1: Hard x-ray to visible converter (phosphor) Port 2: None (available for temporary experiments) Both ports are inside the ALS shielding. Characteristics Port 1: Pinhole-based x-ray system for transverse measurements Port 2: IR/visible port available for temporary experiments; x-ray BPM based on electron secondary emission induced in metallic blades by synchrotron radiation Spatial resolution Port 1: <25 µm transverse Port 2: ~1 µm position; <1 µrad angle (x-ray BPM)

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


161

Beamline 7.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Diagnostic beamline GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range Port 1: ~17 keV transmission though Mo filters Port 2: IR-visible from large-angle synchrotron radiation; UV-x-ray for beam position monitor (BPM) Endstations Port 1: Hard x-ray to visible converter (phosphor) Port 2: None (available for temporary experiments) Both ports are inside the ALS shielding. Characteristics Port 1: Pinhole-based x-ray system for transverse measurements Port 2: IR/visible port available for temporary experiments; x-ray BPM based on electron secondary emission induced in metallic blades by synchrotron radiation Spatial resolution Port 1: <25 µm transverse Port 2: ~1 µm position; <1 µrad angle (x-ray BPM)

162

Beamline 7.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Diagnostic beamline GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range Port 1: ~17 keV transmission though Mo filters Port 2: IR-visible from large-angle synchrotron radiation; UV-x-ray for beam position monitor (BPM) Endstations Port 1: Hard x-ray to visible converter (phosphor) Port 2: None (available for temporary experiments) Both ports are inside the ALS shielding. Characteristics Port 1: Pinhole-based x-ray system for transverse measurements Port 2: IR/visible port available for temporary experiments; x-ray BPM based on electron secondary emission induced in metallic blades by synchrotron radiation Spatial resolution Port 1: <25 µm transverse Port 2: ~1 µm position; <1 µrad angle (x-ray BPM)

163

APS Safety Guidelines for Beamlines  

NLE Websites -- All DOE Office Websites (Extended Search)

Safety Guidelines for Beamlines Accident Investigations LOM Shop Usage User Shop Access - Policies and Procedures User Shop Orientation User Shop Authorization Certification Form...

164

Beamline 9.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print Atomic, molecular, and materials science Endstations: X-ray absorption endstation Polarized-x-ray emission spectrometer GENERAL BEAMLINE INFORMATION Operational Yes Source...

165

Find a Beamline | Advanced Photon Source  

NLE Websites -- All DOE Office Websites (Extended Search)

Find a Beamline Find a Beamline The Advanced Photon Source consists of 34 sectors; each sector contains one or more beamlines. There are several resources available to help you find information about APS sectors and beamlines. Maps: Interactive Map Clicking on the link above or the picture below will take you to a page where you can see which APS beamlines are operational and relevant to your scientific interests. sectors map thumb Beamlines Map Clicking on the link above or the picture below will take you to a detailed bird's eye view of every beamline at the APS. beamline map thumb Directories: Beamlines Directory The complete listing of all APS beamlines' contacts, specifications, and status. Techniques Directory An explanation of the various research techniques in use at the APS, and a

166

Photon Sciences | NSLS-II Beamlines  

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NSLS-II Beamlines NSLS-II Beamlines beamlines Current NSLS-II Beamline Diagram The National Synchrotron Light Source II will accommodate more than 60 beamlines using 27 straight sections for insertion-device sources and 31 bending-magnet or three-pole-wiggler sources, with additional beamlines possible through canted insertion devices and multiple branches. Six beamlines were selected in 2008 and are now funded within the NSLS-II project. These project beamlines encompass research programs in inelastic x-ray scattering, hard x-ray nanoprobe, coherent hard x-ray scattering, coherent soft x-ray scattering and polarization, submicron resolution x-ray spectroscopy, and x-ray powder diffraction. For each beamline, a beamline advisory team, or BAT, has been established to represent the broader scientific community in a specific area of

167

Beamline 29-ID  

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IEX Milestones(4/29/2013) IEX Milestones(4/29/2013) • Spring 2012 ✓ Completion of the IEX EM-VPU insertion device (photos) ✓ Installation of EM-VPU in the storage ring (photo1, photo2) ✓ Installation of high heat-load mirrors M0/M1 (photo) • Summer 2012 ✓ Testing of various polarization mode of EM-VPU with stored beam ✓ Installation of vacuum transport, support tables and diagnostic component; implementation of beamline controls and safety systems (cleanroom, FOE progress, FOE progress2) • Fall 2012 ✓ FDR approval (October 15) ✓ Installation of first optical enclosure components (photo) ✓ First light and testing of white/pink beam components (photo1, photo2) • Winter/Spring 2013 - White beam commissioning ✓ Alignment of mirrors with synchrotron beam ✓ Installation and alignment of support tables (photo)

168

The BEAR Beamline at Elettra  

SciTech Connect

The BEAR (Bending Magnet for Emission Absorption and Reflectivity) beamline is installed at the right exit of the 8.1 bending magnet at ELETTRA. The beamline - in operation since January 2003 - delivers linear and circularly polarized radiation in the 5 - 1600 eV energy range. The experimental station is composed of a UHV chamber for reflectivity, absorption, fluorescence and angle resolved photoemission measurements and a UHV chamber for in-situ sample preparation.

Nannarone, S.; Pasquali, L.; Selvaggi, G. [UdR-INFM Modena, Universita di Modena and Reggio Emilia, Via Vignolese 905, 41100 Modena (Italy); Borgatti, F.; DeLuisa, A.; Doyle, B.P.; Gazzadi, G.C.; Giglia, A.; Finetti, P.; Pedio, M. [TASC-INFM, MM building in Area Science Park, s.s.14 km 163.5, 34012 Basovizza, Trieste (Italy); Mahne, N. [TASC-INFM, Universita di Trieste, Trieste (Italy); Naletto, G.; Pelizzo, M.G.; Tondello, G. [LUXOR-INFM, Universita di Padova, Padua (Italy)

2004-05-12T23:59:59.000Z

169

APS Preliminary Beamline Design Report Guide  

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PRELIMINARY BEAMLINE DESIGN REPORT PRELIMINARY BEAMLINE DESIGN REPORT December 5, 1994 5.1 Preliminary Beamline Design: General Guidelines The Preliminary Design of the beamline represents an approximately 30% design level of each of the beamline components. This level of design permits the CAT to develop cost estimates for the construction of the beamline, as well as a realistic timeline for completion of the construction tasks. A committee from the APS has been charged with reviewing the Preliminary Design Reports and has established the evaluation criteria described below. The Preliminary Beamline Report is expected to expand upon the Conceptual Design Report in the following areas: Beamline Layout Component Design Work Breakdown Structure Cost and Schedule Additional Operational Requirements

170

Instrumentation upgrades for the Macromolecular Crystallography beamlines  

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Instrumentation upgrades for the Macromolecular Crystallography beamlines Instrumentation upgrades for the Macromolecular Crystallography beamlines of the Swiss Light Source Monday, October 29, 2012 - 2:00am SSRL, Bldg. 137, Rm. 322 Martin Fuchs, MX Group, Swiss Light Source; Paul Scherrer Institute (Villigen, Switzerland) A new unified diffractometer - the D3 - has been developed for the three MX beamlines. The first of the instruments is in general user operation at beamline X10SA since April 2012. The varied demands from both challenging academic research projects as well as high throughput industrial applications on today's macromolecular crystallography beamlines drive developments to both endstations and beamline optics. Recent instrumentation upgrades to the macromolecular crystallography (MX) beamlines of the Swiss Light Source therefore aimed to

171

Beamline 4.0.3  

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3 Print 3 Print High-resolution spectroscopy of complex materials (MERLIN) Endstations: MERIXS: High-resolution inelastic scattering ARPES: Angle-resolved photoemission spectroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics 9.0-cm-period quasiperiodic elliptical polarization undulator (EPU9) Energy range 9eV-120eV with current gratings Monochromator Variable-included-angle spherical grating monochromator (SGM) Calculated flux (1.9 GeV, 400 mA) 1012 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) High flux 1200 lines/mm; ~1/25,000 Endstations High-resolution inelastic scattering (MERIXS) and ARPES Characteristics Milli-Electron-volt Resolution beamLINe (MERLIN): Ultrahigh-resolution inelastic scattering and angle-resolved photoemission

172

Beamline 5.4.1  

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5.4.1 5.4.1 Beamline 5.4.1 Print Infrared spectromicroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics Bend magnet Energy range 0.07-1.25 eV Frequency range 600 - 10,000 cm-1 Interferometer resolution 0.125 cm-1 Endstations FTIR bench and IR microscope (N2 purged) Characteristics Computerized sample stage, 0.1-micron resolution; reflection, transmission, and attenuated total reflectance (ATR) modes; polarizing and UV fluorescence optics Spatial resolution Diffraction limited (~wavelength) Detectors Probably MCT-A*, MCT-B (mercury cadmium telluride) Spot size at sample 2-10 µm (diffraction-limited) Sample preparation Biological preparation equipment available including incubator, biohoods, prep table, and more TBD. Sample environment N2 purged, minimal clean area (no particle specification), microcryostat/heater stages available for 4.2-730 K

173

Beamline 4.0.3  

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3 Print 3 Print High-resolution spectroscopy of complex materials (MERLIN) Endstations: MERIXS: High-resolution inelastic scattering ARPES: Angle-resolved photoemission spectroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics 9.0-cm-period quasiperiodic elliptical polarization undulator (EPU9) Energy range 9eV-120eV with current gratings Monochromator Variable-included-angle spherical grating monochromator (SGM) Calculated flux (1.9 GeV, 400 mA) 1012 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) High flux 1200 lines/mm; ~1/25,000 Endstations High-resolution inelastic scattering (MERIXS) and ARPES Characteristics Milli-Electron-volt Resolution beamLINe (MERLIN): Ultrahigh-resolution inelastic scattering and angle-resolved photoemission

174

Beamline 4.0.3  

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3 Print 3 Print High-resolution spectroscopy of complex materials (MERLIN) Endstations: MERIXS: High-resolution inelastic scattering ARPES: Angle-resolved photoemission spectroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics 9.0-cm-period quasiperiodic elliptical polarization undulator (EPU9) Energy range 9eV-120eV with current gratings Monochromator Variable-included-angle spherical grating monochromator (SGM) Calculated flux (1.9 GeV, 400 mA) 1012 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) High flux 1200 lines/mm; ~1/25,000 Endstations High-resolution inelastic scattering (MERIXS) and ARPES Characteristics Milli-Electron-volt Resolution beamLINe (MERLIN): Ultrahigh-resolution inelastic scattering and angle-resolved photoemission

175

Beamline 9.0.2  

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9.0.2 9.0.2 Beamline 9.0.2 Print Tuesday, 20 October 2009 08:59 Chemical Dynamics Scientific disciplines: Chemical dynamics, aerosol chemistry, imaging mass spectrometry, chemical kinetics, laser ablation and clusters, combustion and flames. Endstations: Molecular-beam photoelectron/photoion imaging and spectroscopy Flame chamber Ablation chamber Aerosol chamber Kinetics chamber GENERAL BEAMLINE INFORMATION Operational Yes Source characteristics 10-cm period undulator (U10) (fundamental) Energy range 7.4-30 eV Undulator beam White beam (straight undulator beam) Calculated flux (1.9 GeV, 400 mA) 1016 photons/s, 2.5%BW Spot size at sample 170 (h) x 50 (v) µm Monochromator #1 3-m Off-plane Eagle Calculated flux (1.9 GeV, 400 mA) 1014 photons/s, 0.1%BW Spot size at sample 400 (h) x 350 (v) µm

176

Beamlines Directory | Advanced Photon Source  

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Beamlines Directory Beamlines Directory Filter by: L bracket Discipline: All Atomic Physics Chemistry Environmental Science GeoScience Life Sciences Materials Science Physics Polymer Science Technique: All Anomalous and resonant scattering (hard x-ray) Anomalous and resonant scattering (soft x-ray) Biohazards at the BSL2/3 level Coherent x-ray scattering Diffraction anomalous fine structure Diffuse x-ray scattering Energy dispersive X-ray diffraction Fiber diffraction Fluorescence spectroscopy General diffraction Grazing incidence diffraction Grazing incidence small-angle scattering High-energy x-ray diffraction High-pressure diamond anvil cell High-pressure multi-anvil press Inelastic x-ray scattering Inelastic x-ray scattering (1 eV resolution) Intensity fluctuation spectroscopy Large unit cell crystallography Laue

177

Beamline 4.0.3  

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3 Print 3 Print High-resolution spectroscopy of complex materials (MERLIN) Endstations: MERIXS: High-resolution inelastic scattering ARPES: Angle-resolved photoemission spectroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics 9.0-cm-period quasiperiodic elliptical polarization undulator (EPU9) Energy range 9eV-120eV with current gratings Monochromator Variable-included-angle spherical grating monochromator (SGM) Calculated flux (1.9 GeV, 400 mA) 1012 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) High flux 1200 lines/mm; ~1/25,000 Endstations High-resolution inelastic scattering (MERIXS) and ARPES Characteristics Milli-Electron-volt Resolution beamLINe (MERLIN): Ultrahigh-resolution inelastic scattering and angle-resolved photoemission

178

Beamline 7.3.1  

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7.3.1 Print 7.3.1 Print Photoemission electron microscope PEEM2 Scientific disciplines: Magnetism, materials, surface science, polymers Note: This beamline is NOT open to general users. GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 180-1500 eV Monochromator SGM Calculated flux (1.9 GeV, 400 mA) 3 x 1012 photons/s/0.1%BW at 800 eV (linearly polarized) Resolving power (E/ΔE) 1,000 Endstations Photoemission electron microscope (PEEM2) Characteristics X-ray absorption spectromicroscopy Spatial resolution Below 100 nm Detectors Slow scan CCD Spot size at sample 30 x 30 µm Sample format UHV-compatible flat, conductive samples up to 1 cm2 in area Sample preparation Sputter-cleaning, heating, e-beam and sputter evaporation, LEED, transfer capability, magnet (1 kOe)

179

Beamline 7.3.1  

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7.3.1 Print 7.3.1 Print Photoemission electron microscope PEEM2 Scientific disciplines: Magnetism, materials, surface science, polymers Note: This beamline is NOT open to general users. GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 180-1500 eV Monochromator SGM Calculated flux (1.9 GeV, 400 mA) 3 x 1012 photons/s/0.1%BW at 800 eV (linearly polarized) Resolving power (E/ΔE) 1,000 Endstations Photoemission electron microscope (PEEM2) Characteristics X-ray absorption spectromicroscopy Spatial resolution Below 100 nm Detectors Slow scan CCD Spot size at sample 30 x 30 µm Sample format UHV-compatible flat, conductive samples up to 1 cm2 in area Sample preparation Sputter-cleaning, heating, e-beam and sputter evaporation, LEED, transfer capability, magnet (1 kOe)

180

Beamline 4.0.3  

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3 Print 3 Print High-resolution spectroscopy of complex materials (MERLIN) Endstations: MERIXS: High-resolution inelastic scattering ARPES: Angle-resolved photoemission spectroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics 9.0-cm-period quasiperiodic elliptical polarization undulator (EPU9) Energy range 9eV-120eV with current gratings Monochromator Variable-included-angle spherical grating monochromator (SGM) Calculated flux (1.9 GeV, 400 mA) 1012 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) High flux 1200 lines/mm; ~1/25,000 Endstations High-resolution inelastic scattering (MERIXS) and ARPES Characteristics Milli-Electron-volt Resolution beamLINe (MERLIN): Ultrahigh-resolution inelastic scattering and angle-resolved photoemission

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


181

Beamline 10.3.1  

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0.3.1 0.3.1 Beamline 10.3.1 Print Tuesday, 20 October 2009 09:14 X-ray fluorescence microprobe Scientific disciplines: Environmental science, detector development, low-dose radiation effects in cells GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 3-20 keV Monochromator White light, multilayer mirrors in Kirkpatrick-Baez configuration Calculated flux (1.9 GeV, 400 mA) 3 x 1010 photons/s at 12.5 keV Resolving power (E/ΔE) White light to 30 at 12 keV Endstations Large hutch with optical table Characteristics X-ray fluorescence analysis of samples with high elemental sensitivity and high spatial resolution Spatial resolution 10 x 10 µm Detectors Silicon drift detector Spot size at sample 1.0 x 1.2 µm Sample format

182

Beamline 4.0.3  

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3 Print 3 Print High-resolution spectroscopy of complex materials (MERLIN) Endstations: MERIXS: High-resolution inelastic scattering ARPES: Angle-resolved photoemission spectroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics 9.0-cm-period quasiperiodic elliptical polarization undulator (EPU9) Energy range 9eV-120eV with current gratings Monochromator Variable-included-angle spherical grating monochromator (SGM) Calculated flux (1.9 GeV, 400 mA) 1012 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) High flux 1200 lines/mm; ~1/25,000 Endstations High-resolution inelastic scattering (MERIXS) and ARPES Characteristics Milli-Electron-volt Resolution beamLINe (MERLIN): Ultrahigh-resolution inelastic scattering and angle-resolved photoemission

183

Beamline 4.0.3  

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3 Print 3 Print High-resolution spectroscopy of complex materials (MERLIN) Endstations: MERIXS: High-resolution inelastic scattering ARPES: Angle-resolved photoemission spectroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics 9.0-cm-period quasiperiodic elliptical polarization undulator (EPU9) Energy range 9eV-120eV with current gratings Monochromator Variable-included-angle spherical grating monochromator (SGM) Calculated flux (1.9 GeV, 400 mA) 1012 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) High flux 1200 lines/mm; ~1/25,000 Endstations High-resolution inelastic scattering (MERIXS) and ARPES Characteristics Milli-Electron-volt Resolution beamLINe (MERLIN): Ultrahigh-resolution inelastic scattering and angle-resolved photoemission

184

Beamline 4.0.3  

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3 Print 3 Print High-resolution spectroscopy of complex materials (MERLIN) Endstations: MERIXS: High-resolution inelastic scattering ARPES: Angle-resolved photoemission spectroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics 9.0-cm-period quasiperiodic elliptical polarization undulator (EPU9) Energy range 9eV-120eV with current gratings Monochromator Variable-included-angle spherical grating monochromator (SGM) Calculated flux (1.9 GeV, 400 mA) 1012 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) High flux 1200 lines/mm; ~1/25,000 Endstations High-resolution inelastic scattering (MERIXS) and ARPES Characteristics Milli-Electron-volt Resolution beamLINe (MERLIN): Ultrahigh-resolution inelastic scattering and angle-resolved photoemission

185

Design of the LBNE Beamline  

E-Print Network (OSTI)

The Long Baseline Neutrino Experiment (LBNE) will utilize a beamline facility located at Fermilab to carry out a compelling research program in neutrino physics. The facility will aim a wide band beam of neutrinos toward a detector placed at the Sanford Underground Research Facility in South Dakota, about 1,300 km away. The main elements of the facility are a primary proton beamline and a neutrino beamline. The primary proton beam (60 -120 GeV) will be extracted from the MI-10 section of Fermilab's Main Injector. Neutrinos are produced after the protons hit a solid target and produce mesons which are sign selected and subsequently focused by a set of magnetic horns into a 204 m long decay pipe where they decay mostly into muons and neutrinos. The parameters of the facility were determined taking into account the physics goals, spacial and radiological constraints and the experience gained by operating the NuMI facility at Fermilab. The initial beam power is expected to be ~1.2 MW, however the facility is desi...

Papadimitriou, V; Hylen, J; Kobilarcik, T; Marchionni, A; Moore, C D; Schlabach, P; Tariq, S

2015-01-01T23:59:59.000Z

186

APS Beamline 6-ID-B,C  

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B,C Home B,C Home Recent Publications Beamline Info Optics Instrumentation Software User Info Beamline 6-ID-B,C Beamline 6-ID-B,C is operated by the Magnetic Materials Group in the X-ray Science Division (XSD) of the Advanced Photon Source. Research on this beamline centers on general x-ray scattering studies of materials. The beamline has 2 end-stations: 6-ID-B: Psi -Diffractomter & In-Field Studies 6-ID-C: UHV in-situ growth Recent Research Highlights LSMO pictures Searching for Next-Generation Electronic Materials December 14, 2009 A new class of layered oxide materials discovered thanks to research at the beamline 6-ID-B offers scientists unprecedented opportunities for creating the next generation of electronic devices. Local Contact: Phil Ryan Local Contacts: Philip Ryan (Surface Diffraction) 630.252.0252 ryan@aps.anl.gov

187

Transportation Beamline at the Advanced Photon Source | Argonne...  

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Transportation Beamline at the Advanced Photon Source Argonne's dedicated transportation research beamline at Argonne's Advanced Photon Source (APS) allows researchers to use the...

188

APS 7-BM Beamline: Techniques  

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Motivation Motivation The major thrust of the 7-BM beamline is the application of synchrotron radiation tools to examine complex fluid flowfields. Two major techniques are applied: radiography and x-ray fluorescence spectroscopy. While optical techniques are often ideally suited to the study of fluid flowfields, there are certain flowfields for which optical diagnostics have significant challenges. These include: Multiphase flows: Visible light interacts strongly with phase boundaries. This leads to strong refraction, scattering, and attenuation of light. These effects hinder quantitative measurements of dense multiphase flowfields. Opaque media. Flows with strong refractive effects. Luminous flames: The strong light emission from sooting flames can hinder certain optical diagnostics.

189

Diamond Beamline I16 (Materials and Magnetism)  

SciTech Connect

We describe the key features and performance specifications of a facility for high-resolution single-crystal x-ray diffraction at Diamond Light Source. The scientific emphasis of the beamline is materials- and x-ray-physics, including resonant and magnetic scattering. We highlight some of the more novel aspects of the beamline design.

Collins, S. P.; Bombardi, A.; Marshall, A. R.; Williams, J. H.; Barlow, G.; Day, A. G.; Pearson, M. R.; Woolliscroft, R. J.; Walton, R. D.; Beutier, G.; Nisbet, G. [Diamond Light Source Ltd, Diamond House, Harwell Science and Innovation Campus, Didcot, Oxfordshire, OX11 0DE (United Kingdom)

2010-06-23T23:59:59.000Z

190

Photon Sciences Directorate | 2010 Annual Report | FY10 Beamline Guide  

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FY10 Beamline Guide FY10 Beamline Guide beamline status chart Click on the image to download a high-resolution version. Beamline Status In 2010, 49 X-Ray and 11 Vacuum Ultraviolet-Infrared operational beamlines were available for a wide range of experiments using a variety of techniques. There are two types of beamlines at NSLS: facility beamlines, of which there were 21; and participating research team (PRT) beamlines, of which there were 39. Facility beamlines are operated by Photon Sciences staff members and reserve a minimum of 50 percent of their beam time for general users. PRT beamlines are run by user groups with similar interests and reserve 25 percent of their beam time for general users, although they can grant additional time at their own discretion. The following pages provide details on NSLS operational beamlines,

191

APS Beamline 6-ID-D  

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MM-Group Home MM-Group Home MMG Advisory Committees 6-ID-D Home Recent Publications Beamline Info Optics Instrumentation Software User Info Beamline 6-ID-D Beamline 6-ID-D is operated by the Magnetic Materials Group in the X-ray Science Division (XSD) of the Advanced Photon Source. This is a high energy (50 - 130 keV) beamline used for structural studies primarily on single crystal materials. Recent Research Highlights LuFeO Unlikely route to ferroelectricity May 16, 2012 A new type of ferroelectric, LuO2Fe4, has been investigated at the APS by a research team from Julich research center. XAS & XMCD studies on beamline 4-ID-C determined the Fe magnetism and valence, while single crystal x-ray scattering measurements at 6-ID-B & 6-ID-D probed the associated structural and charge ordering.

192

APS Beamline 6-ID-D  

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D Home D Home Recent Publications Beamline Info Optics Instrumentation Software User Info Beamline 6-ID-D Beamline 6-ID-D is operated by the Magnetic Materials Group in the X-ray Science Division (XSD) of the Advanced Photon Source. This is a high energy (50 - 130 keV) beamline used for structural studies primarily on single crystal materials. Recent Research Highlights A New Family of Quasicrystals A New Family of Quasicrystals June 24, 2013 Scientists from the U.S. Department of Energy's Ames Laboratory and Iowa State University have used the high energy x-rays available on beamline 6-ID-D, to confirm the structure of the only known magnetic rare earth icosahedral binary quasicrystals. Contacts: Alan Goldman & Paul Canfield - Iowa State Univ. & Ames Lab Local Contacts:

193

APS 7-BM Beamline: 7-BM Home  

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Overview of the 7-BM beamline Overview of the 7-BM beamline The 7-BM beamline is dedicated to time-resolved measurements of complex fluid flowfields using x-ray radiography and fluorescence spectroscopy. Funding for the final commissioning of 7-BM was provided by the DOE Office of Energy Efficiency and Renewable Energy. Commissioning was completed at the end of FY2012. The beamline is currently operated by the X-Ray Science Division of the APS. Major Areas of Research Fuel sprays from automotive fuel injectors, both diesel and gasoline. See more on the X-Ray Fuel Spray web page from Argonne's Energy Systems Division. Sprays for air-breathing propulsion. Fuel injection for rocket injectors. Gas-phase fuel injection and mixing. Beamline Performance Total flux: 4 x 1011 ph/s at 8 keV Energy range: 5.5 - 11 keV, 1.4% ΔE/E

194

Overview of the SPring-8 Diagnostics Beamlines  

SciTech Connect

We present an overview of the two SPring-8 diagnostics beamlines, the beamline I (dipole magnet source) and II (insertion device source). At the beamline I, synchrotron radiation (SR) in both the X-ray and the visible bands is exploited for characterizations of the electron beam. At the beamline II, by observing the spectral, spatial, and temporal characteristics of X-ray SR of the insertion device (ID), new techniques for accelerator diagnostics are investigated. Irradiation experiments with the ID to develop accelerator components such as photon absorbers, and production of intensive 10 MeV {gamma}-rays by backward Compton scattering of external far infrared (FIR) laser photons are being prepared at the beamline II.

Takano, S.; Masaki, M.; Tamura, K.; Mochihashi, A.; Nakamura, T.; Suzuki, S.; Oishi, M.; Shoji, M.; Taniuchi, Y.; Okayasu, Y.; Ohkuma, H. [Japan Synchrotron Radiation Research Institute, SPring-8, Sayo, Hyogo, 679-5198 (Japan); Okajima, S. [Center of Advanced Metrology, Chubu University, Kasugai, Aichi, 487-8501 (Japan)

2010-06-23T23:59:59.000Z

195

APS Beamline Questionnaire Form | Advanced Photon Source  

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APS Beamline Motor Drive Questionnaire Form APS Beamline Motor Drive Questionnaire Form * indicates required field Please send a separate email to Thomas Barkalow with an attached beamline drawing or sketch showing where the groups are located and the distances they are apart. First Name*: Middle Initial/Name: Last Name*: Beamline Designation*: What is the total number of driver units with makes and models?: How are driver units grouped together and each group's location within the beamline?: What number of driver units are in use simultaneously for each group?: What is the maximum amperage setting actually used for each unit?: What is the number of groups in use simultaneously and which groups are they?: Verification: We need to make sure you are a human. Please solve the challenge below, and click the I'm a Human button to get a confirmation code. To make this

196

Diagnostic X-Multi-Axis Beamline  

SciTech Connect

Tomographic reconstruction of explosive events require time resolved multipal lines of sight. Considered here is a four (or eight) line of sight beam layout for a nominal 20 MeV 2000 Ampere 2 microsecond electron beam for generation of x-rays 0.9 to 5 meters from a given point, the ''firing point''. The requirement of a millimeter spatial x-ray source requires that the electron beam be delivered to the converter targets with sub-millimeter precision independent of small variations in beam energy and initial conditions. The 2 usec electron beam pulse allows for four bursts in each line, separated in time by about 500 microseconds. Each burst is divided by a electro-magnetic kicker into four (or eight) pulses, one for each beamline. The arrival time of the four (or eight) beam pulses at the x-ray target can be adjusted by the kicker timing and the sequence that the beams of each burst are switched into the different beamlines. There exists a simple conceptual path from a four beamline to a eight beamline upgrade. The eight line beamline is built up from seven unique types of sub-systems or ''blocks''. The beamline consists of 22 of these functional blocks and contains a total of 455 individual magnets, figure 1. The 22 blocks are inter-connected by a total of 30 straight line inter-block sections (IBS). Beamlines 1-4 are built from 12 blocks with conceptual layout structure shown in figure 2. Beamlines 5-8 are built with an additional 10 blocks with conceptual layout structure shown in figure 3. This beamline can be thought of as looking like a lollipop consisting of a 42 meter long stick leading to a 60 by 70 meter rectangular candy blob consisting of the eight lines of sight. The accelerator providing the electron beam is at the end of the stick and the firing point is at the center of the blob. The design allows for a two stage implementation. Beamlines 1-3 can be installed to provide a tomographic azimuthal resolution of 45 degrees. An upgrade can later be made by adding beamlines 5-8 azimuthally indexed so as to provide an azimuthal resolution of 22.5 degrees. All eight beamlines point down by 10 degrees (pitch). The x-ray converter target can be located along each beamline anywhere between 0 to 5 meters from the firing point. An example of inter-facing the Diagnostic X facility with the Darht II accelerator located at LANL will be given.

Paul, A C

2000-04-05T23:59:59.000Z

197

Beamlines  

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Two Beryllium windows, 100 m and 120 m. Distance source point - mask plane 10.35 meter. DEX 02 scanner, from Jenoptik GmbH. Micromachining II (XRLM2), Port 2B, 10 mrad...

198

Beamline 3.2.1  

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2.1 Print 2.1 Print Commercial deep-etch x-ray lithography (LIGA) GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 3-12 keV Monochromator None Endstations Hutch with automated scanner Calculated spot size at sample 100 x 10 mm Sample format 3- and 4-in. wafer format; x-ray mask and LIGA substrate Sample environment Ambient, air Scientific disciplines Applied science Scientific applications Deep-etch x-ray lithography (LIGA) Spokesperson This e-mail address is being protected from spambots. You need JavaScript enabled to view it Advanced Light Source, Berkeley Lab Phone: (510) 486-5527 Fax: (510) 486-4102 This e-mail address is being protected from spambots. You need JavaScript enabled to view it AXSUN Technology

199

Beamline 9.0.2  

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9.0.2 Print 9.0.2 Print Chemical Dynamics Scientific disciplines: Chemical dynamics, aerosol chemistry, imaging mass spectrometry, chemical kinetics, laser ablation and clusters, combustion and flames. Endstations: Molecular-beam photoelectron/photoion imaging and spectroscopy Flame chamber Ablation chamber Aerosol chamber Kinetics chamber GENERAL BEAMLINE INFORMATION Operational Yes Source characteristics 10-cm period undulator (U10) (fundamental) Energy range 7.4-30 eV Undulator beam White beam (straight undulator beam) Calculated flux (1.9 GeV, 400 mA) 1016 photons/s, 2.5%BW Spot size at sample 170 (h) x 50 (v) µm Monochromator #1 3-m Off-plane Eagle Calculated flux (1.9 GeV, 400 mA) 1014 photons/s, 0.1%BW Spot size at sample 400 (h) x 350 (v) µm Monochromator #2 3-m Off-plane Eagle

200

Beamline 10.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print X-ray fluorescence microprobe Scientific disciplines: Environmental science, detector development, low-dose radiation effects in cells GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 3-20 keV Monochromator White light, multilayer mirrors in Kirkpatrick-Baez configuration Calculated flux (1.9 GeV, 400 mA) 3 x 1010 photons/s at 12.5 keV Resolving power (E/ΔE) White light to 30 at 12 keV Endstations Large hutch with optical table Characteristics X-ray fluorescence analysis of samples with high elemental sensitivity and high spatial resolution Spatial resolution 10 x 10 µm Detectors Silicon drift detector Spot size at sample 1.0 x 1.2 µm Sample format Sample size flexible up to 30 cm x 1 meter depending on configuration.

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


201

Beamline 10.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print X-ray fluorescence microprobe Scientific disciplines: Environmental science, detector development, low-dose radiation effects in cells GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 3-20 keV Monochromator White light, multilayer mirrors in Kirkpatrick-Baez configuration Calculated flux (1.9 GeV, 400 mA) 3 x 1010 photons/s at 12.5 keV Resolving power (E/ΔE) White light to 30 at 12 keV Endstations Large hutch with optical table Characteristics X-ray fluorescence analysis of samples with high elemental sensitivity and high spatial resolution Spatial resolution 10 x 10 µm Detectors Silicon drift detector Spot size at sample 1.0 x 1.2 µm Sample format Sample size flexible up to 30 cm x 1 meter depending on configuration.

202

Beamline 9.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Chemical Dynamics Scientific disciplines: Chemical dynamics, aerosol chemistry, imaging mass spectrometry, chemical kinetics, laser ablation and clusters, combustion and flames. Endstations: Molecular-beam photoelectron/photoion imaging and spectroscopy Flame chamber Ablation chamber Aerosol chamber Kinetics chamber GENERAL BEAMLINE INFORMATION Operational Yes Source characteristics 10-cm period undulator (U10) (fundamental) Energy range 7.4-30 eV Undulator beam White beam (straight undulator beam) Calculated flux (1.9 GeV, 400 mA) 1016 photons/s, 2.5%BW Spot size at sample 170 (h) x 50 (v) µm Monochromator #1 3-m Off-plane Eagle Calculated flux (1.9 GeV, 400 mA) 1014 photons/s, 0.1%BW Spot size at sample 400 (h) x 350 (v) µm Monochromator #2 3-m Off-plane Eagle

203

Beamline 3.2.1  

NLE Websites -- All DOE Office Websites (Extended Search)

2.1 Print 2.1 Print Commercial deep-etch x-ray lithography (LIGA) GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 3-12 keV Monochromator None Endstations Hutch with automated scanner Calculated spot size at sample 100 x 10 mm Sample format 3- and 4-in. wafer format; x-ray mask and LIGA substrate Sample environment Ambient, air Scientific disciplines Applied science Scientific applications Deep-etch x-ray lithography (LIGA) Spokesperson This e-mail address is being protected from spambots. You need JavaScript enabled to view it Advanced Light Source, Berkeley Lab Phone: (510) 486-5527 Fax: (510) 486-4102 This e-mail address is being protected from spambots. You need JavaScript enabled to view it AXSUN Technology

204

Beamline 5.4.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Infrared spectromicroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics Bend magnet Energy range 0.07-1.25 eV Frequency range 600 - 10,000 cm-1 Interferometer resolution 0.125 cm-1 Endstations FTIR bench and IR microscope (N2 purged) Characteristics Computerized sample stage, 0.1-micron resolution; reflection, transmission, and attenuated total reflectance (ATR) modes; polarizing and UV fluorescence optics Spatial resolution Diffraction limited (~wavelength) Detectors Probably MCT-A*, MCT-B (mercury cadmium telluride) Spot size at sample 2-10 µm (diffraction-limited) Sample preparation Biological preparation equipment available including incubator, biohoods, prep table, and more TBD. Sample environment N2 purged, minimal clean area (no particle specification), microcryostat/heater stages available for 4.2-730 K

205

Beamline 9.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Atomic, molecular, and materials science Endstations: X-ray absorption endstation Polarized-x-ray emission spectrometer Magnetic mass spectrometer Liquid cell endstation GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 2320eV-5600eV Monochromator Double Si(111) crystal Measured flux (1.9 GeV, 300 mA) 1011 photons/s Resolving power (E/ΔE) 3000-8000 Beam size Adjustable with 2nd mirror Focused: 1.0 mm x 0.7 mm (~0.5 mm square at 2800 eV) Unfocused: 10 mm x 10 mm or larger Endstations X-ray absorption endstation Polarized-x-ray emission spectrometer Magnetic mass spectrometer Liquid cell endstation Local contact Wayne Stolte Advanced Light Source, Berkeley Lab Phone: (510) 486-5804 Fax: (510) 495-2111

206

Beamline 9.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

9.0.2 Print 9.0.2 Print Chemical Dynamics Scientific disciplines: Chemical dynamics, aerosol chemistry, imaging mass spectrometry, chemical kinetics, laser ablation and clusters, combustion and flames. Endstations: Molecular-beam photoelectron/photoion imaging and spectroscopy Flame chamber Ablation chamber Aerosol chamber Kinetics chamber GENERAL BEAMLINE INFORMATION Operational Yes Source characteristics 10-cm period undulator (U10) (fundamental) Energy range 7.4-30 eV Undulator beam White beam (straight undulator beam) Calculated flux (1.9 GeV, 400 mA) 1016 photons/s, 2.5%BW Spot size at sample 170 (h) x 50 (v) µm Monochromator #1 3-m Off-plane Eagle Calculated flux (1.9 GeV, 400 mA) 1014 photons/s, 0.1%BW Spot size at sample 400 (h) x 350 (v) µm Monochromator #2 3-m Off-plane Eagle

207

Beamline 5.4.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Infrared spectromicroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics Bend magnet Energy range 0.07-1.25 eV Frequency range 600 - 10,000 cm-1 Interferometer resolution 0.125 cm-1 Endstations FTIR bench and IR microscope (N2 purged) Characteristics Computerized sample stage, 0.1-micron resolution; reflection, transmission, and attenuated total reflectance (ATR) modes; polarizing and UV fluorescence optics Spatial resolution Diffraction limited (~wavelength) Detectors Probably MCT-A*, MCT-B (mercury cadmium telluride) Spot size at sample 2-10 µm (diffraction-limited) Sample preparation Biological preparation equipment available including incubator, biohoods, prep table, and more TBD. Sample environment N2 purged, minimal clean area (no particle specification), microcryostat/heater stages available for 4.2-730 K

208

Beamline 9.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Atomic, molecular, and materials science Endstations: X-ray absorption endstation Polarized-x-ray emission spectrometer Magnetic mass spectrometer Liquid cell endstation GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 2320eV-5600eV Monochromator Double Si(111) crystal Measured flux (1.9 GeV, 300 mA) 1011 photons/s Resolving power (E/ΔE) 3000-8000 Beam size Adjustable with 2nd mirror Focused: 1.0 mm x 0.7 mm (~0.5 mm square at 2800 eV) Unfocused: 10 mm x 10 mm or larger Endstations X-ray absorption endstation Polarized-x-ray emission spectrometer Magnetic mass spectrometer Liquid cell endstation Local contact Wayne Stolte Advanced Light Source, Berkeley Lab Phone: (510) 486-5804 Fax: (510) 495-2111

209

Beamline 9.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 Print 2 Print Chemical Dynamics Scientific disciplines: Chemical dynamics, aerosol chemistry, imaging mass spectrometry, chemical kinetics, laser ablation and clusters, combustion and flames. Endstations: Molecular-beam photoelectron/photoion imaging and spectroscopy Flame chamber Ablation chamber Aerosol chamber Kinetics chamber GENERAL BEAMLINE INFORMATION Operational Yes Source characteristics 10-cm period undulator (U10) (fundamental) Energy range 7.4-30 eV Undulator beam White beam (straight undulator beam) Calculated flux (1.9 GeV, 400 mA) 1016 photons/s, 2.5%BW Spot size at sample 170 (h) x 50 (v) µm Monochromator #1 3-m Off-plane Eagle Calculated flux (1.9 GeV, 400 mA) 1014 photons/s, 0.1%BW Spot size at sample 400 (h) x 350 (v) µm Monochromator #2 3-m Off-plane Eagle

210

Beamline 9.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Atomic, molecular, and materials science Endstations: X-ray absorption endstation Polarized-x-ray emission spectrometer Magnetic mass spectrometer Liquid cell endstation GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 2320eV-5600eV Monochromator Double Si(111) crystal Measured flux (1.9 GeV, 300 mA) 1011 photons/s Resolving power (E/ΔE) 3000-8000 Beam size Adjustable with 2nd mirror Focused: 1.0 mm x 0.7 mm (~0.5 mm square at 2800 eV) Unfocused: 10 mm x 10 mm or larger Endstations X-ray absorption endstation Polarized-x-ray emission spectrometer Magnetic mass spectrometer Liquid cell endstation Local contact Wayne Stolte Advanced Light Source, Berkeley Lab Phone: (510) 486-5804 Fax: (510) 495-2111

211

Beamline 10.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print X-ray fluorescence microprobe Scientific disciplines: Environmental science, detector development, low-dose radiation effects in cells GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 3-20 keV Monochromator White light, multilayer mirrors in Kirkpatrick-Baez configuration Calculated flux (1.9 GeV, 400 mA) 3 x 1010 photons/s at 12.5 keV Resolving power (E/ΔE) White light to 30 at 12 keV Endstations Large hutch with optical table Characteristics X-ray fluorescence analysis of samples with high elemental sensitivity and high spatial resolution Spatial resolution 10 x 10 µm Detectors Silicon drift detector Spot size at sample 1.0 x 1.2 µm Sample format Sample size flexible up to 30 cm x 1 meter depending on configuration.

212

Beamline 3.2.1  

NLE Websites -- All DOE Office Websites (Extended Search)

2.1 Print 2.1 Print Commercial deep-etch x-ray lithography (LIGA) GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 3-12 keV Monochromator None Endstations Hutch with automated scanner Calculated spot size at sample 100 x 10 mm Sample format 3- and 4-in. wafer format; x-ray mask and LIGA substrate Sample environment Ambient, air Scientific disciplines Applied science Scientific applications Deep-etch x-ray lithography (LIGA) Spokesperson This e-mail address is being protected from spambots. You need JavaScript enabled to view it Advanced Light Source, Berkeley Lab Phone: (510) 486-5527 Fax: (510) 486-4102 This e-mail address is being protected from spambots. You need JavaScript enabled to view it AXSUN Technology

213

Beamline 5.4.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Infrared spectromicroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics Bend magnet Energy range 0.07-1.25 eV Frequency range 600 - 10,000 cm-1 Interferometer resolution 0.125 cm-1 Endstations FTIR bench and IR microscope (N2 purged) Characteristics Computerized sample stage, 0.1-micron resolution; reflection, transmission, and attenuated total reflectance (ATR) modes; polarizing and UV fluorescence optics Spatial resolution Diffraction limited (~wavelength) Detectors Probably MCT-A*, MCT-B (mercury cadmium telluride) Spot size at sample 2-10 µm (diffraction-limited) Sample preparation Biological preparation equipment available including incubator, biohoods, prep table, and more TBD. Sample environment N2 purged, minimal clean area (no particle specification), microcryostat/heater stages available for 4.2-730 K

214

Beamline 10.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print X-ray fluorescence microprobe Scientific disciplines: Environmental science, detector development, low-dose radiation effects in cells GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 3-20 keV Monochromator White light, multilayer mirrors in Kirkpatrick-Baez configuration Calculated flux (1.9 GeV, 400 mA) 3 x 1010 photons/s at 12.5 keV Resolving power (E/ΔE) White light to 30 at 12 keV Endstations Large hutch with optical table Characteristics X-ray fluorescence analysis of samples with high elemental sensitivity and high spatial resolution Spatial resolution 10 x 10 µm Detectors Silicon drift detector Spot size at sample 1.0 x 1.2 µm Sample format Sample size flexible up to 30 cm x 1 meter depending on configuration.

215

Beamline 9.3.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Atomic, molecular, and materials science Endstations: X-ray absorption endstation Polarized-x-ray emission spectrometer Magnetic mass spectrometer Liquid cell endstation GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 2320eV-5600eV Monochromator Double Si(111) crystal Measured flux (1.9 GeV, 300 mA) 1011 photons/s Resolving power (E/ΔE) 3000-8000 Beam size Adjustable with 2nd mirror Focused: 1.0 mm x 0.7 mm (~0.5 mm square at 2800 eV) Unfocused: 10 mm x 10 mm or larger Endstations X-ray absorption endstation Polarized-x-ray emission spectrometer Magnetic mass spectrometer Liquid cell endstation Local contact Wayne Stolte Advanced Light Source, Berkeley Lab Phone: (510) 486-5804 Fax: (510) 495-2111

216

Beamline 3.2.1  

NLE Websites -- All DOE Office Websites (Extended Search)

2.1 Print 2.1 Print Commercial deep-etch x-ray lithography (LIGA) GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 3-12 keV Monochromator None Endstations Hutch with automated scanner Calculated spot size at sample 100 x 10 mm Sample format 3- and 4-in. wafer format; x-ray mask and LIGA substrate Sample environment Ambient, air Scientific disciplines Applied science Scientific applications Deep-etch x-ray lithography (LIGA) Spokesperson This e-mail address is being protected from spambots. You need JavaScript enabled to view it Advanced Light Source, Berkeley Lab Phone: (510) 486-5527 Fax: (510) 486-4102 This e-mail address is being protected from spambots. You need JavaScript enabled to view it AXSUN Technology

217

Beamline 9.0.2  

NLE Websites -- All DOE Office Websites (Extended Search)

9.0.2 Print 9.0.2 Print Chemical Dynamics Scientific disciplines: Chemical dynamics, aerosol chemistry, imaging mass spectrometry, chemical kinetics, laser ablation and clusters, combustion and flames. Endstations: Molecular-beam photoelectron/photoion imaging and spectroscopy Flame chamber Ablation chamber Aerosol chamber Kinetics chamber GENERAL BEAMLINE INFORMATION Operational Yes Source characteristics 10-cm period undulator (U10) (fundamental) Energy range 7.4-30 eV Undulator beam White beam (straight undulator beam) Calculated flux (1.9 GeV, 400 mA) 1016 photons/s, 2.5%BW Spot size at sample 170 (h) x 50 (v) µm Monochromator #1 3-m Off-plane Eagle Calculated flux (1.9 GeV, 400 mA) 1014 photons/s, 0.1%BW Spot size at sample 400 (h) x 350 (v) µm Monochromator #2 3-m Off-plane Eagle

218

Beamline 5.4.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Infrared spectromicroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics Bend magnet Energy range 0.07-1.25 eV Frequency range 600 - 10,000 cm-1 Interferometer resolution 0.125 cm-1 Endstations FTIR bench and IR microscope (N2 purged) Characteristics Computerized sample stage, 0.1-micron resolution; reflection, transmission, and attenuated total reflectance (ATR) modes; polarizing and UV fluorescence optics Spatial resolution Diffraction limited (~wavelength) Detectors Probably MCT-A*, MCT-B (mercury cadmium telluride) Spot size at sample 2-10 µm (diffraction-limited) Sample preparation Biological preparation equipment available including incubator, biohoods, prep table, and more TBD. Sample environment N2 purged, minimal clean area (no particle specification), microcryostat/heater stages available for 4.2-730 K

219

Beamline 5.4.1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Print 1 Print Infrared spectromicroscopy GENERAL BEAMLINE INFORMATION Operational 2011 Source characteristics Bend magnet Energy range 0.07-1.25 eV Frequency range 600 - 10,000 cm-1 Interferometer resolution 0.125 cm-1 Endstations FTIR bench and IR microscope (N2 purged) Characteristics Computerized sample stage, 0.1-micron resolution; reflection, transmission, and attenuated total reflectance (ATR) modes; polarizing and UV fluorescence optics Spatial resolution Diffraction limited (~wavelength) Detectors Probably MCT-A*, MCT-B (mercury cadmium telluride) Spot size at sample 2-10 µm (diffraction-limited) Sample preparation Biological preparation equipment available including incubator, biohoods, prep table, and more TBD. Sample environment N2 purged, minimal clean area (no particle specification), microcryostat/heater stages available for 4.2-730 K

220

Beamline 3.2.1  

NLE Websites -- All DOE Office Websites (Extended Search)

2.1 Print 2.1 Print Commercial deep-etch x-ray lithography (LIGA) GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 3-12 keV Monochromator None Endstations Hutch with automated scanner Calculated spot size at sample 100 x 10 mm Sample format 3- and 4-in. wafer format; x-ray mask and LIGA substrate Sample environment Ambient, air Scientific disciplines Applied science Scientific applications Deep-etch x-ray lithography (LIGA) Spokesperson This e-mail address is being protected from spambots. You need JavaScript enabled to view it Advanced Light Source, Berkeley Lab Phone: (510) 486-5527 Fax: (510) 486-4102 This e-mail address is being protected from spambots. You need JavaScript enabled to view it AXSUN Technology

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


221

A Test Beamline on Diamond Light Source  

SciTech Connect

A Test beamline B16 has been built on the 3 GeV Diamond synchrotron radiation source. The beamline covers a wide photon energy range from 2 to 25 keV. The beamline is highly flexible and versatile in terms of the available beam size (a micron to 100 mm) and the range of energy resolution and photon flux; by virtue of its several operational modes, and the different inter-changeable instruments available in the experiments hutch. Diverse experimental configurations can be flexibly configured using a five-circle diffractometer, a versatile optics test bench, and a suite of detectors. Several experimental techniques including reflectivity, diffraction and imaging are routinely available. Details of the beamline and its measured performance are presented.

Sawhney, K. J. S.; Dolbnya, I. P.; Tiwari, M. K.; Alianelli, L.; Scott, S. M.; Preece, G. M.; Pedersen, U. K.; Walton, R. D. [Diamond Light Source Ltd, Harwell Science and Innovation Campus, Didcot, Oxfordshire-OX11 0DE (United Kingdom)

2010-06-23T23:59:59.000Z

222

Beamline 11.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

1.3.2 Print 1.3.2 Print Inspection of EUV lithography masks GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 50-1000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1011 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) 7000 Endstations The SEMATECH Berkeley Actinic Inspection Tool Detector 2048 x 2048 EUV CCD Characteristics 900-1000x zoneplate microscope Spot size at sample 1-5 microns Spatial resolution 60 nm Sample format EUV Photolithography masks: 6" glass plate, multilayer coated for normal incidence reflectivity at 13.4 nm Sample preparation Cleanroom handling Sample environment 2.0 x 10-7 Torr base pressure Scientific applications EUV lithography Local contacts/ Spokespersons This e-mail address is being protected from spambots. You need JavaScript enabled to view it

223

Beamline 11.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

1.3.2 Print 1.3.2 Print Inspection of EUV lithography masks GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 50-1000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1011 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) 7000 Endstations The SEMATECH Berkeley Actinic Inspection Tool Detector 2048 x 2048 EUV CCD Characteristics 900-1000x zoneplate microscope Spot size at sample 1-5 microns Spatial resolution 60 nm Sample format EUV Photolithography masks: 6" glass plate, multilayer coated for normal incidence reflectivity at 13.4 nm Sample preparation Cleanroom handling Sample environment 2.0 x 10-7 Torr base pressure Scientific applications EUV lithography Local contacts/ Spokespersons This e-mail address is being protected from spambots. You need JavaScript enabled to view it

224

Beamline 11.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

1.3.2 Print 1.3.2 Print Inspection of EUV lithography masks GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 50-1000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1011 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) 7000 Endstations The SEMATECH Berkeley Actinic Inspection Tool Detector 2048 x 2048 EUV CCD Characteristics 900-1000x zoneplate microscope Spot size at sample 1-5 microns Spatial resolution 60 nm Sample format EUV Photolithography masks: 6" glass plate, multilayer coated for normal incidence reflectivity at 13.4 nm Sample preparation Cleanroom handling Sample environment 2.0 x 10-7 Torr base pressure Scientific applications EUV lithography Local contacts/ Spokespersons This e-mail address is being protected from spambots. You need JavaScript enabled to view it

225

Beamline 11.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

1.3.2 Print 1.3.2 Print Inspection of EUV lithography masks GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 50-1000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1011 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) 7000 Endstations The SEMATECH Berkeley Actinic Inspection Tool Detector 2048 x 2048 EUV CCD Characteristics 900-1000x zoneplate microscope Spot size at sample 1-5 microns Spatial resolution 60 nm Sample format EUV Photolithography masks: 6" glass plate, multilayer coated for normal incidence reflectivity at 13.4 nm Sample preparation Cleanroom handling Sample environment 2.0 x 10-7 Torr base pressure Scientific applications EUV lithography Local contacts/ Spokespersons This e-mail address is being protected from spambots. You need JavaScript enabled to view it

226

Beamline 11.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

1.3.2 Print 1.3.2 Print Inspection of EUV lithography masks GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 50-1000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1011 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) 7000 Endstations The SEMATECH Berkeley Actinic Inspection Tool Detector 2048 x 2048 EUV CCD Characteristics 900-1000x zoneplate microscope Spot size at sample 1-5 microns Spatial resolution 60 nm Sample format EUV Photolithography masks: 6" glass plate, multilayer coated for normal incidence reflectivity at 13.4 nm Sample preparation Cleanroom handling Sample environment 2.0 x 10-7 Torr base pressure Scientific applications EUV lithography Local contacts/ Spokespersons This e-mail address is being protected from spambots. You need JavaScript enabled to view it

227

Beamline 11.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

1.3.2 Print 1.3.2 Print Inspection of EUV lithography masks GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 50-1000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1011 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) 7000 Endstations The SEMATECH Berkeley Actinic Inspection Tool Detector 2048 x 2048 EUV CCD Characteristics 900-1000x zoneplate microscope Spot size at sample 1-5 microns Spatial resolution 60 nm Sample format EUV Photolithography masks: 6" glass plate, multilayer coated for normal incidence reflectivity at 13.4 nm Sample preparation Cleanroom handling Sample environment 2.0 x 10-7 Torr base pressure Scientific applications EUV lithography Local contacts/ Spokespersons This e-mail address is being protected from spambots. You need JavaScript enabled to view it

228

Beamline 11.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

1.3.2 Print 1.3.2 Print Inspection of EUV lithography masks GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 50-1000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1011 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) 7000 Endstations The SEMATECH Berkeley Actinic Inspection Tool Detector 2048 x 2048 EUV CCD Characteristics 900-1000x zoneplate microscope Spot size at sample 1-5 microns Spatial resolution 60 nm Sample format EUV Photolithography masks: 6" glass plate, multilayer coated for normal incidence reflectivity at 13.4 nm Sample preparation Cleanroom handling Sample environment 2.0 x 10-7 Torr base pressure Scientific applications EUV lithography Local contacts/ Spokespersons This e-mail address is being protected from spambots. You need JavaScript enabled to view it

229

Beamline 11.3.2  

NLE Websites -- All DOE Office Websites (Extended Search)

1.3.2 Print 1.3.2 Print Inspection of EUV lithography masks GENERAL BEAMLINE INFORMATION Operational Yes, but not open to users Source characteristics Bend magnet Energy range 50-1000 eV Monochromator VLS-PGM Calculated flux (1.9 GeV, 400 mA) 1011 photons/s/0.01%BW at 100 eV Resolving power (E/ΔE) 7000 Endstations The SEMATECH Berkeley Actinic Inspection Tool Detector 2048 x 2048 EUV CCD Characteristics 900-1000x zoneplate microscope Spot size at sample 1-5 microns Spatial resolution 60 nm Sample format EUV Photolithography masks: 6" glass plate, multilayer coated for normal incidence reflectivity at 13.4 nm Sample preparation Cleanroom handling Sample environment 2.0 x 10-7 Torr base pressure Scientific applications EUV lithography Local contacts/ Spokespersons This e-mail address is being protected from spambots. You need JavaScript enabled to view it

230

National synchrotron light source user's manual: Guide to the VUV and x-ray beamlines: Third edition  

SciTech Connect

This report contains information on the following topics: A Word on the Writing of Beamline Descriptions; Beamline Equipment Utilization for General Users; the Vacuum Ultraviolet (VUV) Storage Ring and Beamlines; VUV Beamline Descriptions--An Explanation; VUV Beamline Descriptions; X-Ray Storage Ring and Beamlines; X-Ray Beamline Descriptions--An Explanation; and X-Ray Beamline Descriptions.

Gmuer, N.F.; Thomlinson, W.; White-DePace, S.

1989-01-01T23:59:59.000Z

231

BeamLine Operations and Safety Awareness (BLOSA) Checklist Beamline X8A All users must be instructed in operating the beamline safely. Leave checkbox blank if not applicable. Training valid 2 years. Visitors use Visitor/Escort forms.  

E-Print Network (OSTI)

BeamLine Operations and Safety Awareness (BLOSA) Checklist Beamline X8A All users must procedure for removal of solder wasteSolder B CLOSE OUT Secure the beamline and disable shutter/beam before for this beamline:I understand the instructions given to me on beamline operations and safety awareness. Date UAdm

Ohta, Shigemi

232

LENGTH OF BEAMLINES AND WIDTH OF THE LS-37  

NLE Websites -- All DOE Office Websites (Extended Search)

LENGTH OF BEAMLINES AND WIDTH OF THE LENGTH OF BEAMLINES AND WIDTH OF THE LS-37 November 10, 1985 G. K. Shenoy G. S. Knapp EXPERIMENTAL HALL AT A 6-GeV SYNCHROTRON FACILITY The width of the experimental hall at a 6-GeV facility is closely related to the length of the beamlines. This note addresses this aspect in some de tail. In general, no two beamlines will have identical lengths or the placement of various optical elements. Hence fixing the beamline lengths prior to their assignment to specific experiments is difficult. In spite of this fact, a few general conclusions are made. 1. At least 25m of all the beamlines will be behind the shielding wall. Within this length many beamline components can be accommodated as shown in Fig. 1. 2. For most beamlines on bending magnets (BM), the first optical element will

233

Beamline Safety Design Review Steering Committee Charter  

NLE Websites -- All DOE Office Websites (Extended Search)

Meeting Minutes internal link Meeting Minutes internal link Reviews internal link Beamline Safety Design Review Steering Committee (BSDRSC) 1. Purpose The Beamline Safety Design Review Steering Committee (BSDRSC) oversees the review of all safety aspects related to beamline and critical component design, regardless of who generated the design, and includes facility operational issues when reviewing non-APS generated designs. 2. Membership Members appointed by the APS Division Directors will be comprised of a pre-selected standing committee with membership chosen by function. The following functions will be included: AES User Technical Interface (Committee Chair) AES Technical Operations Specialist APS Electrical / Electronics Technical Representative AES QA Engineering Specialist APS Radiation Safety Shielding Committee Chair

234

1-ID: Sector 1, Insertion Device Beamline  

NLE Websites -- All DOE Office Websites (Extended Search)

1-ID beamline schematic 1-ID beamline schematic ID on-axis brilliance values 1-ID - Sector 1, Insertion Device Beamline Responsible Scientists Jon Almer, phone: (630) 252-1049, e-mail: almer@aps.anl.gov Sarvjit Shastri, phone: (630) 252-0129, e-mail: shastri@aps.anl.gov John Okasinski, phone: (630) 252-0162, e-mail: okasinski@aps.anl.gov Peter Kenesei, phone: (630) 252-0133, e-mail: kenesei@aps.anl.gov Scientific Programs Coupled high-energy SAXS/WAXS studies (HE-SAXS/WAXS) High-energy diffraction microscopy (HEDM) Single-grain studies Stress/strain/texture studies Pair-distribution function (PDF) measurements High-energy fluorescence Source Characteristics Upstream insertion device: APS Undulator A No. of Poles 72 Undulator Period 3.3 cm Device Length 2.4 m Minimum Gap 11 mm Downstream insertion device

235

The Phase I MX Beamlines at Diamond Light Source  

SciTech Connect

Three beamlines dedicated to macromolecular crystallography, I02, I03 and I04 at Diamond Light Source are presented. These beamlines formed the life science component of Phase 1 of Diamond Light Source. The article provides details of the design and the current status of the beamlines.

Duke, E. M. H.; Evans, G.; Flaig, R.; Hall, D. R.; Latchem, M.; McAuley, K. E.; Sandy, D. J.; Sorensen, T. L-M.; Waterman, D.; Johnson, L. N. [Diamond Light Source, Harwell Science and Innovation Campus, Didcot, Oxon. OX11 0DE (United Kingdom)

2010-06-23T23:59:59.000Z

236

Beamline Phone Numbers| Advanced Photon Source  

NLE Websites -- All DOE Office Websites (Extended Search)

Interactive Map Interactive Map Beamlines Map Beamlines Directory Techniques Directory Sectors Directory Beamline Phone Numbers Status and Schedule Beamline Phone Numbers From on-site, dial 2, then a number listed below. From off-site, dial 630-252 and a number listed below. Sector 1 1-BM-A: 1701 1-BM-C: 5468 1-ID: 1801 Sector 2 2-BM: 1702 2-ID-B: 1628 2-ID-D: 1802 2-ID-E: 3711 Sector 3 3-ID: 1803 Sector 4 4-ID-C: 1704 4-ID-D: 1804 Sector 5 5-BM: 1705 5-ID: 1805 Sector 6 6-ID-B: 1806 6-ID-C: 1406 6-ID-D: 1606 Sector 7 7-ID-B: 1607 7-ID-C: 1707 7-ID-D: 1807 7-ID-E: 1207 Sector 8 8-ID-E: 1908 8-ID-I: 1808 Sector 9 9-BM-B: 1709 9-ID-B: 0349 9-ID-C: 1809 Column 95: 4705 Sector 10 10-BM-B: 6792 10-ID-B: 1710 Sector 11 11-BM-B: 5877 11-ID-B: 1711 11-ID-C: 1711 11-ID-D: 2162 Laser lab: 0379 Sector 12 12-BM-B: 0378 12-ID-B,C: 1712

237

On Line Beamline Commissioning Activity Approval Form  

NLE Websites -- All DOE Office Websites (Extended Search)

Commissioning Activity Approval Form Commissioning Activity Approval Form This form is to be filled by the Commissioning Activity Team Leader. No beamline commissioning activities will be allowed to run without a properly completed, approved, and posting of this commissioning approval form. You will be notified by e-mail upon approval. Sector Beamline Expected Start Date Expected Duration 01 02 03 04 05 06 07 08 09 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 BM ID ( Give a Unit) Activity Description( Give only a brief description) Commissioning Team Members First and Last Name Affiliation Phone Number 1. 2. 3. 4. 5. 6. Special Safety Concerns Commissioning Activity Team Leader Name E-Mail Address Submit Commissioning Activity Approval Form Clear all Fields and start All over again!!!

238

Performance measurements at the SLS SIM beamline  

SciTech Connect

The Surface/Interface: Microscopy beamline of the Swiss Light Source started operation in 2001. In 2007 the beamline has been significantly upgraded with a second refocusing section and a blazed grating optimized for high photon flux. Two Apple II type undulators with a plane grating monochromator using the collimated light scheme deliver photons with an energy from 90eV to about 2keV with variable polarization for the photoemission electron microscope (PEEM) as the primary user station. We measured a focus of (45x60) {mu}m({nu}xh) and a photon flux > 10{sup 12} photon/s for all gratings. Polarization switching within a few seconds is realized with the small bandpass of the monochromator and a slight detuning of the undulator.

Flechsig, U.; Nolting, F.; Fraile Rodriguez, A.; Krempasky, J.; Quitmann, C.; Schmidt, T.; Spielmann, S.; Zimoch, D. [Paul Scherrer Institut, Swiss Light Source, 5232 Villigen PSI (Switzerland)

2010-06-23T23:59:59.000Z

239

1993 CAT workshop on beamline optical designs  

SciTech Connect

An Advanced Photon Source (APS) Collaborative Access Team (CAT) Workshop on Beamline Optical Designs was held at Argonne National Laboratory on July 26--27, 1993. The goal of this workshop was to bring together experts from various synchrotron sources to provide status reports on crystal, reflecting, and polarizing optics as a baseline for discussions of issues facing optical designers for CAT beamlines at the APS. Speakers from the European Synchrotron Radiation Facility (ESRF), the University of Chicago, the National Synchrotron Light Source, and the University of Manchester (England) described single- and double-crystal monochromators, mirrors, glass capillaries, and polarizing optics. Following these presentations, the 90 participants divided into three working groups: Crystal Optics Design, Reflecting Optics, and Optics for Polarization Studies. This volume contains copies of the presentation materials from all speakers, summaries of the three working groups, and a ``catalog`` of various monochromator designs.

Not Available

1993-11-01T23:59:59.000Z

240

Macromolecular crystallography beamline X25 at the NSLS  

Science Journals Connector (OSTI)

A description of the upgraded beamline X25 at the NSLS, operated by the PXRR and the Photon Sciences Directorate serving the Macromolecular Crystallography community, is presented.

H?roux, A.

2014-04-08T23:59:59.000Z

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


241

The New Materials Science Beamline HARWI-II at DESY  

SciTech Connect

In autumn 2005, the GKSS-Research Center Geesthacht in cooperation with Deutsches Elektronen-Synchrotron DESY, Hamburg, started operation of the new synchrotron radiation beamline HARWI-II. The beamline is specialized for performing materials science experiments using hard X-rays. First experiments were successfully performed studying the residual strain in a VPPA welded Al alloy plate, the texture of cold extruded Al90-Cu10 composites, and the 3 dimensional material flow of friction steer welds by micro tomography. At the new beamline HARWI-II, the GKSS now has direct access for using synchrotron radiation for materials science experiments.

Beckmann, Felix; Dose, Thomas; Lippmann, Thomas; Lottermoser, Lars; Martins, Rene-V.; Schreyer, Andreas [GKSS-Research Center Geesthacht, Max-Planck-Strasse 1, 21502 Geesthacht (Germany)

2007-01-19T23:59:59.000Z

242

The New Materials Science Beamline HARWI?II at DESY  

Science Journals Connector (OSTI)

In autumn 2005 the GKSS?Research Center Geesthacht in cooperation with Deutsches Elektronen?Synchrotron DESY Hamburg started operation of the new synchrotron radiation beamline HARWI?II. The beamline is specialized for performing materials science experiments using hard X?rays. First experiments were successfully performed studying the residual strain in a VPPA welded Al alloy plate the texture of cold extruded Al90?Cu10 composites and the 3 dimensional material flow of friction steer welds by micro tomography. At the new beamline HARWI?II the GKSS now has direct access for using synchrotron radiation for materials science experiments.

Felix Beckmann; Thomas Dose; Thomas Lippmann; Lars Lottermoser; Rene?V. Martins; Andreas Schreyer

2007-01-01T23:59:59.000Z

243

BeamLine Operations and Safety Awareness (BLOSA) Checklist Beamline X20A All users must be instructed in operating the beamline safely. Leave checkbox blank if not applicable. Training valid 2 years. Visitors use Visitor/Escort forms.  

E-Print Network (OSTI)

BeamLine Operations and Safety Awareness (BLOSA) Checklist Beamline X20A All users must A Review procedure and location for temporary SAA (for soldering or other wastes)SAA - Solder B CLOSE OUT to me on beamline operations and safety awareness. Date UAdmTrainer's Signature J. Jordan-Sweet C

Ohta, Shigemi

244

BeamLine Operations and Safety Awareness (BLOSA) Checklist Beamline X20C All users must be instructed in operating the beamline safely. Leave checkbox blank if not applicable. Training valid 2 years. Visitors use Visitor/Escort forms.  

E-Print Network (OSTI)

BeamLine Operations and Safety Awareness (BLOSA) Checklist Beamline X20C All users must containerDisposal - Sharps A Review procedure and location for temporary SAA (for soldering or other wastes)SAA - Solder B CLOSE OUT Secure the beamline and disable shutter/beam before you leaveDisabling Beam A Review

Ohta, Shigemi

245

Efficacy of memantine in the treatment of fibromyalgia: A double-blind, randomised, controlled trial with 6-month follow-up  

Science Journals Connector (OSTI)

Abstract Fibromyalgia (FM) is a prevalent and disabling chronic disease. Recent studies have found elevated levels of glutamate in several brain regions, leading to hypotheses about the usefulness of glutamate-blocking drugs such as memantine in the treatment of FM. The aim of this study was to evaluate the efficacy of memantine in the treatment of pain and other clinical variables (global function, clinical impression, depression, anxiety, quality of life) in FM patients. A double-blind, parallel randomised controlled trial was developed. A total of 63 patients diagnosed with FM were recruited from primary health care centres in Zaragoza, Spain. Memantine was administered at doses of 20mg/d after 1month of titration. Assessments were carried out at baseline, posttreatment, and 3- and 6-month follow-up. Compared with a placebo group, memantine significantly decreased ratings on a pain visual analogue scale (Cohens d=1.43 at 6months) and pain measured with a sphygmomanometer (d=1.05). All other secondary outcomes except anxiety also improved, with moderate-to-large effect sizes at 6months. Compared with placebo, the absolute risk reduction obtained with memantine was 16.13% (95% confidence interval=2.0% to 32.6%), and the number needed to treat was 6.2 (95% confidence interval=3 to 47). Tolerance was good, with dizziness (8 patients) and headache (4 patients) being the most frequent side effects of memantine. Although additional studies with larger sample sizes and longer follow-up times are needed, this study provides preliminary evidence of the utility of memantine for the treatment of FM.

Brbara Olivan-Blzquez; Paola Herrera-Mercadal; Marta Puebla-Guedea; Mari-Cruz Prez-Yus; Eva Andrs; Nicolas Fayed; Yolanda Lpez-Del-Hoyo; Rosa Magallon; Miquel Roca; Javier Garcia-Campayo

2014-01-01T23:59:59.000Z

246

NSLS II: The Future National Synchrotron Light Source | 2010 Beamline  

NLE Websites -- All DOE Office Websites (Extended Search)

2010 Beamline Development Proposals - Approved Proposals 2010 Beamline Development Proposals - Approved Proposals Proposal Results Announcement Acronym Title Spokesperson Type Information 4DE 4-Dimensional Studies in Extreme Environments Donald J. Weidner, Stony Brook University 1 Slide ABS A Highly Automated Instrument for Static X-ray Scattering Measurements of Biological Molecules in Solution Lin Yang, BNL 1 Slide AIM Advanced Infrared Microspectroscopy Lisa Miller, BNL 1 Slide AMX Flexible Access Macromolecular Crystallography at an Undulator Beamline Dieter Schneider, BNL 1 Slide | Proposal BMM Hard X-ray Absorption Spectroscopy and Diffraction - Beamline for Materials Measurements Daniel Fischer, NIST 2 Slide | Proposal CDI Coherent X-ray Diffraction Ian Robinson, University College London 1 Slide | Proposal

247

Status of the LBNE Neutrino Beamline  

SciTech Connect

The Long Baseline Neutrino Experiment (LBNE) will utilize a neutrino beamline facility located at Fermilab to carry out a compelling research program in neutrino physics. The facility will aim a beam of neutrinos toward a detector placed at the Homestake Mine in South Dakota. The neutrinos are produced in a three-step process. First, protons from the Main Injector (60-120 GeV) hit a solid target and produce mesons. Then, the charged mesons are focused by a set of focusing horns into the decay pipe, towards the far detector. Finally, the mesons that enter the decay pipe decay into neutrinos. The parameters of the facility were determined taking into account several factors including the physics goals, the Monte Carlo modeling of the facility, spacial and radiological constraints and the experience gained by operating the NuMI facility at Fermilab. The initial beam power is expected to be {approx}700 kW, however some of the parameters were chosen to be able to deal with a beam power of 2.3 MW. We discuss here the status of the conceptual design and the associated challenges.

Papadimitriou, Vaia; /Fermilab

2011-12-01T23:59:59.000Z

248

Metrology and Tests beamline at SOLEIL Design and first results  

SciTech Connect

The objectives of this project is install at the 2.75 GeV SOLEIL synchrotron radiation source a calibration and metrology test facility for the R and D of optical components and detectors. We have build, on a bending magnet, two branches to cover an energy range from few eV to 28 keV and give access to white beam. This installation will first address the needs of the SOLEIL experimental groups(Optics and Detectors)and will be used by a large community. This beamline will also be valuable as a general-purpose beamline to prepare, test and set up a wide range of experiments in the field of Astrophysics, laser plasma etc...A complementary important aspect of this installation is the realization of primary standard: the metrology beamline of SOLEIL could become the national primary standard source in collaboration with the Laboratoire National d'Essais(LNE)and help in the design and characterization of several diagnostics for the Megajoule Laser in Bordeaux in collaboration with the CEA DIF. The beamline has been designed to provide great flexibility. In this paper, we describe the beamline design, the end station instrumentation and give also some preliminary results.

Idir, Mourad; Mercere, Pascal; Moreno, Thierry; Delmotte, Aurelien; Dasilva, Paulo; Modi, Mohammed H. [Synchrotron SOLEIL, L'Orme des Merisiers, Saint-Aubin-BP 48 91192 GIF-sur-YVETTE CEDEX (France)

2010-06-23T23:59:59.000Z

249

Temperature and TimeResolved XRay Powder Diffraction X14A EERE sponsored PRT beamline  

E-Print Network (OSTI)

Temperature and TimeResolved XRay Powder Diffraction X14A EERE sponsored PRT beamline Objective, in ambience or with gas flow Capabilities: X14A, EERE-sponsored PRT beamline · High photon flux: typically 9x

Ohta, Shigemi

250

E-Print Network 3.0 - absorption beamline x-11 Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

of beamline: 9... open Checkpoints on the X9 side of beamline: 2. Bremsstrahlung shield (BS 1) in place and banded... photo 11. Mirror windows (3) covered in lead as per photo...

251

Photon Sciences | Beamlines | HXN: Hard X-ray Nanoprobe  

NLE Websites -- All DOE Office Websites (Extended Search)

HXN: Hard X-ray Nanoprobe HXN: Hard X-ray Nanoprobe Poster | Fact Sheet | Preliminary Design Report Scientific Scope The Hard X-ray Nanoprobe beamline and endstation instruments (HXN) will be designed and constructed to explore new frontiers of hard x-ray microscopy applications with the highest achievable spatial resolution. Currently the available spatial resolution for scientific applications, provided by scanning x-ray microscopes in the hard x-ray regime, is limited to ~50nm, which is still insufficient for probing the nanoscale interfacial structures critical in determining properties and functionalities of material and biological systems. The HXN beamline aims to enable x-ray experiments at spatial resolutions ranging from 10 to 30 nm with an ultimate goal of ~1 nm. Beamline Description

252

U2B Beamline | Photon Sciences | Brookhaven National Laboratory  

NLE Websites -- All DOE Office Websites (Extended Search)

BNL People BNL People Photon SciencesInfrared Programs PS Home Infrared Home Beamlines U2A U2B U4IR U10A U10B U12IR Publications User Info Useful Sites Beamline U2B Home Publications Equipment Schedule Beamtime Instrument Spectrometer endstation: Thermo Nicolet Magna 860 Step-Scan FTIR and Continuum IR microscope Frequency Range (cm-1): 500 - 4000 Spectral resolution (cm-1): 4.0 Spatial resolution: diffraction-limit (i.e. ~ 3 to 10 microns) Brightness (compared to a black body): 100x to 1000x Smallest practical targeting aperture size: 3 microns square Beamline angular acceptance: (milliradians): 40H x 40V (100% vertical collection down to 240 cm-1) Optical Configuration A two-mirror system (M1 and M2) collects and re-images the synchrotron infrared source at a point just outside of the storage ring's UHV. M1 is a

253

APS beamline standard components handbook, Version 1. 3  

SciTech Connect

This Handbook in its current version (1.3) contains descriptions, specifications, and preliminary engineering design drawings for many of the standard components. The design status and schedules have been provided wherever possible. In the near future, the APS plans to update engineering drawings of identified standard beamline components and complete the Handbook. The completed version of this Handbook will become available to both the CATs and potential vendors. Use of standard components should result in major cost reductions for CATs in the areas of beamline design and construction.

Hahn, U.; Shu, D.; Kuzay, T.M.

1993-02-01T23:59:59.000Z

254

A New Beamline For Time Resolved And Extreme Conditions X-Ray Absorption Spectroscopy  

SciTech Connect

The ESRF has recently started an ambitious project spread over 10 years aimed at an upgrade of the accelerator, beamlines and infrastructure. Through this upgrade, we are proposing a refurbishment of the scanning EXAFS beamline BM29 and of the Energy Dispersive XAS (EDXAS) beamline ID24.

Mathon, Olivier; Mairs, Trevor; Pascarelli, Sakura [ESRF, BP220, 38043 Grenoble Cedex (France)

2010-06-23T23:59:59.000Z

255

Beamline standard component designs for the Advanced Photon Source  

SciTech Connect

The Advanced Photon Source (APS) has initiated a design standardization and modularization activity for the APS synchrotron radiation beamline components. These standard components are included in components library, sub-components library and experimental station library. This paper briefly describes these standard components using both technical specifications and side view drawings.

Shu, D.; Barraza, J.; Brite, C.; Chang, J.; Sanchez, T.; Tcheskidov, V.; Kuzay, T.M.

1994-12-01T23:59:59.000Z

256

Physics Potential of the Fermilab NuMI beamline  

E-Print Network (OSTI)

We explore the physics potential of the NuMI beamline with a detector located 10 km off-axis at a distant site (810 km). We study the sensitivity to $\\sin^2 2 \\theta_{13}$ and to the CP-violating parameter $\\sin \\delta$ as well as the determination of the neutrino mass hierarchy by exploiting the $\

Olga Mena; Stephen Parke

2005-07-25T23:59:59.000Z

257

Beamline Control and Instrumentation System using Industrial Interface Techniques  

SciTech Connect

How should a beamline be designed, which satisfies the needs and requirements of scientists and is easy to build and operate? Today, most control and instrumentation systems for beamlines are based on scientific requirements. Scientific details of the beamline, e.g. vacuum and beam physics details; are usually extensively described. However, control system specifications are often reduced to few requirements, e.g. which beam-related device to use. Lots of these systems work perfectly from the physicist's point of view, but are hard to bring into service and operate and difficult to extend with additional equipment. To overcome this, the engineering company ENZ has developed components using industrial standard interfaces to guarantee high flexibility for equipment extension. Using special interface boards and galvanic isolation offers increased stability of motion control axes. This saves resources during commissioning and service. A control system was developed and installed at a Soft-X-ray beamline at ASP Melbourne. It is operated under EPICs on distributed embedded IOC's based on PC-hardware. Motion and vacuum systems, measurement devices, e.g. a Low-Current Monitor (LoCuM) for beam position monitoring, and parts of the equipment protection system were developed and most of them tested in cooperation with DELTA at the Technical University of Dortmund.

Enz, F. [ENZ Engineering company for environmental electronic and automation, F.-Woehler-Str. 2, 12489 Berlin (Germany)

2010-06-23T23:59:59.000Z

258

The Project for the High Energy Materials Science Beamline at Petra III  

SciTech Connect

The high energy materials science beamline will be among the first fourteen beamlines planned to be operational in 2009 at the new third generation synchrotron light source Petra III at DESY, Germany. The operation and funding of this beamline is assured by GKSS. 70% of the beamline will be dedicated to materials science. The remaining 30% are reserved for physics and are covered by DESY. The materials science activities will be concentrating on three intersecting topics which are industrial, applied, and fundamental research. The beamline will combine three main features: Firstly, the high flux, fast data acquisition systems, and the beamline infrastructure will allow carrying out complex and highly dynamic in-situ experiments. Secondly, a high flexibility in beam shaping will be available, fully exploiting the high brilliance of the source. Thirdly, the beamline will provide the possibility to merge in one experiment different analytical techniques such as diffraction and tomography.

Martins, R. V.; Lippmann, T.; Beckmann, F.; Schreyer, A. [GKSS-Research Centre Geesthacht GmbH, Max-Planck-Strasse, 21502 Geesthacht (Germany)

2007-01-19T23:59:59.000Z

259

Instrumentation and Experimental Developments for the Beamlines at the Synchrotron SOLEIL  

SciTech Connect

This paper presents an overview of the instrumentation and experiments developed for the beamlines at Synchrotron SOLEIL in France. Currently fourteen beamlines are opened to users out of the twenty six scheduled. About half of the beamlines cover the soft x-rays region using spectroscopy and imagery techniques. The second half covers the hard x-rays field studying diffraction of matter. Some sample environments carried out for beamlines, for biology, chemistry and surface sciences are described. For the soft x-rays beamlines, carbon contamination of optics is a crucial issue. Different experiments are currently under study in order to reduce or even avoid this effect. Other studies relate to the improvement of metrological methods for beamline optics, to the reduction of vibrational effects for the microbeams and development of computer control for diffractometers. The various types of instruments and experiments will be presented both with an overview of the status of the beamlines in operation and under construction.

Prigent, P.; Bac, S.; Blanchandin, S.; Cauchon, G.; David, G.; Fernandez Varela, P.; Kubsky, S.; Picca, F. [Synchrotron SOLEIL, Division Experiences-L'Orme des merisiers-Saint-Aubin-BP 48-91192 GIF S/YVETTE Cedex (France)

2010-06-23T23:59:59.000Z

260

BeamLine Operations and Safety Awareness (BLOSA) Checklist Beamline U3C All users must be instructed in operating the beamline safely. Leave checkbox blank if not applicable. Training valid 2 years. Visitors use Visitor/Escort forms.  

E-Print Network (OSTI)

BeamLine Operations and Safety Awareness (BLOSA) Checklist Beamline U3C All users mustVent System A Avoid skin contact with soldering iron to prevent burns to the skinBurns B Use caution when and safety awareness. Date UAdmTrainer's Signature Bin Dong LU-BLOSA-U3C R = NSLS Content A = Applicable

Ohta, Shigemi

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


261

Investigation of pin-post monochromators for a wiggler beamline  

SciTech Connect

Three water-cooled pin-post monochromators, to be used on a wiggler beamline at the Advanced Photon Source (APS), were built with the heat exchanger engineered to provide very high heat transfer. The geometry of the heat exchanger as well as calculated data on the heat transfer will be presented. Before using the monochromators on the beamline, they were checked by x-ray diffraction topography. Reflections (333) and (220) in Bragg case were utilized. In all crystals, similar patterns of strain in the diffracting silicon layers were revealed, which can be attributed to the geometry of the heat exchangers, the bonding technology, and the thickness of the top layer. Conclusions about construction of future pin-post monochromators have been drawn.

Krasnicki, S.; Maj, J. [Argonne National Lab., IL (United States); Schildkamp, W. [Univ. of Chicago, IL (United States); Tonnessen, T. [Boeing North American, Albuquerque, NM (United States). Albuquerque Operations

1998-12-31T23:59:59.000Z

262

Performance of Saga-University Beamline with Planer Undulator  

SciTech Connect

A planer undulator consisted of 24 periods of an 85-mm length has been installed in a 2.7-m straight section of the SAGA-LS, in order to provide brilliant soft x-rays for advanced researches on nano-surfaces and interfaces at the Saga-university beamline BL13. The photon flux of 2x10{sup 11} photons/100 mA was obtained at 133 eV, and the available photon energy was beyond 800 eV using higher harmonics. The achieved resolving power of the varied-line-spacing (VLS) monochromator system was 8,670 at 130 eV with slits of 15 um. This agrees very well with the value of 8,790 expected from the ray-tracing calculation. The details in the performance tests will be reported, indicating the high performance of the beamline BL13 for photoelectron spectroscopy in the soft x-ray region.

Azuma, J.; Takahashi, K.; Kamada, M. [Synchrotron Light Application Center, Saga University, Saga 840-8502 (Japan); Ohkuma, H. [Japan Synchrotron Radiation Research Institute, Sayo-gun, Hyogo 679-5198 (Japan); Yamamoto, S. [High Energy Accelerator Research Organization (KEK), Oho, Tsukuba, Ibaraki 305-0801 (Japan)

2010-06-23T23:59:59.000Z

263

10 Questions for a Beamline Scientist: Apurva Mehta | Department of Energy  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

10 Questions for a Beamline Scientist: Apurva Mehta 10 Questions for a Beamline Scientist: Apurva Mehta 10 Questions for a Beamline Scientist: Apurva Mehta November 4, 2011 - 1:02pm Addthis Apurva Mehta | Image courtesy of SLAC Apurva Mehta | Image courtesy of SLAC Niketa Kumar Niketa Kumar Public Affairs Specialist, Office of Public Affairs "It was exhilarating when we found a novel solution and the instrument evolved." Apurva Mehta, Beamline Scientist Fifteen years ago, SLAC National Accelerator Laboratory (SLAC) scientist Apurva Mehta volunteered to help a friend build beamline parts at the Stanford Synchrotron Radiation Lightsource (SSRL). Today, he's "still mucking around with beamlines."
 
In the latest 10 Questions, Dr. Mehta shares how he landed at SLAC and his adventures in a wide range of projects, from advanced semiconductors to

264

Photon Sciences Directorate | 2010 Annual Report | Beamline & Optics R&D:  

NLE Websites -- All DOE Office Websites (Extended Search)

Beamline & Optics R&D: Enhancing Tools at NSLS, NSLS-II Beamline & Optics R&D: Enhancing Tools at NSLS, NSLS-II Qun Shen "Synchrotron sources have quickly become an essential tool for a wide spectrum of research. All the action takes place at beamlines, each one consisting of a suite of sophisticated scientific instruments. The robust beamlines at NSLS produce remarkable science, and we made excellent progress on developing NSLS-II beamlines and associated science programs." - Qun Shen Director, Photon Division While keeping the existing ring and beamline mechanical systems running, Photon Sciences staff completed a number of R&D projects this year that will improve the tools of researchers at NSLS and, in the near future, NSLS-II. One of the major accomplishments was the installation and commissioning of

265

Biological soft X-ray tomography on beamline 2.1 at the Advanced Light Source  

Science Journals Connector (OSTI)

Beamline 2.1, a transmission soft X-ray microscope at the Advanced Light Source of Lawrence Berkeley National Laboratory, is described.

Le Gros, M.A.

2014-10-01T23:59:59.000Z

266

E-Print Network 3.0 - als infrared beamlines Sample Search Results  

NLE Websites -- All DOE Office Websites (Extended Search)

2002 Advances in Bioengineering RADIATIVE PROPERTIES OF POLAR BEAR HAIR Summary: synchroton infrared spectromicroscopy beamline was utilized to provide a continuous spectrum of...

267

The Nanofocus Endstation of the MINAXS Beamline of PETRA III  

SciTech Connect

The Micro- and Nanofocus X-ray Scattering Beamline (MINAXS) of the new 3rd generation source PETRA III is equipped with two endstations, out of which the farthest from the high beta undulator source is designed to provide a high flux, monochromatic X-ray beam focused to a size in the order of 100 nmx100 nm routinely used for microdiffraction experiments (nanofocus endstation). This contribution presents an overview on the current status of the nanofocus endstation and outlines the to-be-used experimental setup.

Krywka, C. A. [IEAP, Christian-Albrechts-Universitaet zu Kiel, Leibnizstrasse 19, D-24098 Kiel (Germany); Doehrmann, R.; Roth, S. V. [DESY, Notkestrasse 85, D-22063 Hamburg (Germany); Mueller, M. [GKSS Forschungszentrum Geesthacht, Max-Planck-Strasse 1, D-21502 Geesthacht (Germany)

2010-06-23T23:59:59.000Z

268

The holography endstation of beamline P10 at PETRA III  

SciTech Connect

We present the design and instrumentation of a novel holography endstation for the P10 coherence beamline at PETRA III at DESY. The experimental imaging scheme is based on a highly coherent and divergent (cone) beam illumination, achieved by fixed curvature focusing mirrors with additional spatial and coherence filtering by x-ray waveguides. The optical elements along the beam path and the instrument under construction are described. Preliminary results obtained in a similar setting under comparable parameters are given as a benchmark, and first simulations of one of the two mirrors are presented to study the effect of imperfections on the field distribution in the focal plane.

Kalbfleisch, S.; Osterhoff, M.; Giewekemeyer, K.; Neubauer, H.; Krueger, S. P.; Hartmann, B.; Bartels, M.; Salditt, T. [Institut fuer Roentgenphysik, Universitaet Goettingen, Friedrich-Hund-Platz 1, 37077 Goettingen (Germany); Sprung, M.; Leupold, O. [HASYLAB at DESY, Notkestr. 85, 22607 Hamburg (Germany); Siewert, F. [Helmholtz Zentrum Berlin, BESSY-II, Albert-Einstein-Str. 15, 12489 Berlin (Germany)

2010-06-23T23:59:59.000Z

269

Automation of the EMBL Hamburg protein crystallography beamline BW7B  

Science Journals Connector (OSTI)

The automation of the EMBL Hamburg wiggler beamline BW7B for protein crystallography is described. The beamline features an automated end-station, a robotic sample changer, semi-automated sample centering based on UV fluorescence and new control software including intuitive graphical user interfaces.

Pohl, E.

2004-08-17T23:59:59.000Z

270

A Beamline for Fast Polarization Switching at NSLS-II  

SciTech Connect

The first XUV beamline (200-2000 eV) at NSLS-II will have two branches, one optimized for photon hungry experiments requiring high coherent flux and one optimized for studies of polarization sensitive materials and interfaces based on fast polarization switching. We describe here the branch designed for fast polarization switching with frequencies up to 1 kHz, high photon flux, and good energy resolution. The beamline will be served by two canted undulators and is based on the focusing variable line spacing grating monochromator. The two beams will be focused at the same spot of approximately 80x10 {mu}m (hor.xver.). The expected circular polarized flux at the sample from each device up to 1.4 keV will be higher than 10{sup 12} photons/s at a resolving power better than 10{sup 4}. An additional KB focusing system will deliver the two beams to a spot in the {mu}m range.

Reininger, R.; Sanchez-Hanke, C.; Hulbert, S. L. [NSLS and NSLS-II, Brookhaven National Laboratory, Upton, New York 11973 (United States)

2010-06-23T23:59:59.000Z

271

The Diamond Beamline I13L for Imaging and Coherence  

SciTech Connect

I13L is the first long beamline at Diamond dedicated to imaging and coherence. Two independent branches will operate in the energy range of 6-30 keV with spatial resolution on the micro- to nano-lengthscale. The Imaging branch is dedicated to imaging and tomography with In-line phase contrast and full-field microscopy on the micron to nano-length scale. Ultimate resolution will be achieved on the Coherence branch at I13L with imaging techniques in the reciprocal space. The experimental stations will be located about 250 m from the source, taking advantage of the coherence properties of the source. The beamline has some outstanding features such as the mini-beta layout of the storage ring's straight section. The optical layout is optimized for beam stability and high optical quality to preserve the coherent radiation. In the experimental stations several methods will be available, starting for the first user with in-line phase contrast imaging on the imaging branch and Coherent X-ray Diffraction (CXRD) on the coherence branch.

Rau, C. [Diamond Light Source Ltd., Chilton, Oxfordshire (United Kingdom); Feinberg School of Medicine, Northwestern University, Chicago, Illinois (United States); Wagner, U.; Peach, A.; Singh, B.; Wilkin, G.; Jones, C. [Diamond Light Source Ltd., Chilton, Oxfordshire (United Kingdom); Robinson, I. K. [Diamond Light Source Ltd., Chilton, Oxfordshire (United Kingdom); Laboratory for Nanomaterials, University College London, London, London (United Kingdom)

2010-06-23T23:59:59.000Z

272

Photon Sciences | Beamlines | IXS: Inelastic X-ray Scattering  

NLE Websites -- All DOE Office Websites (Extended Search)

IXS: Inelastic X-ray Scattering IXS: Inelastic X-ray Scattering Poster | Fact Sheet | Preliminary Design Report Scientific Scope Many hot topics related to the high frequency dynamics of condensed matter require both a narrower and steeper resolution function and access to a broader dynamic range than what are currently available. This represents a sort of "no man's land" that falls right in the dynamic gap lying between the high frequency spectroscopies, such as inelastic x-ray scattering (IXS), and the low frequency ones. New IXS spectrometers with improved energy and momentum resolutions would be required to fill this gap. To achieve this goal, a new x-ray optics concept for both the monochromatization and energy analysis of x-rays will be implemented at the NSLS-II Inelastic X-ray Scattering beamline. This solution exploits the

273

FRONTIER SYNCHROTRON INFRARED SPECTROSCOPY BEAMLINE UNDER EXTREME CONDITIONS (FIS)  

NLE Websites -- All DOE Office Websites (Extended Search)

FRONTIER SYNCHROTRON INFRARED SPECTROSCOPY FRONTIER SYNCHROTRON INFRARED SPECTROSCOPY BEAMLINE UNDER EXTREME CONDITIONS (FIS) Proposal Team: L. Carr 1 , D. Dolan 2 , R. Hemley 3 , S. Jacobson 4 , S. Karato 5 , Z. Liu 3 , W. Panero 6 , M. Pravica 7 , and T. Zhou 8 1 Brookhaven National Laboratory, 2 Sandia National Laboratories, 3 Carnegie Institution of Washington, 4 Northwestern University, 5 Yale University, 6 Ohio State University, 7 University of Nevada, 8 New Jersey Institute of Technology TECHNIQUES AND CAPABILITIES APPLICATIONS SPECIFIC PROJECTS / ADDITIONAL INFORMATION * TECHNIQUE(S): Fourier transform infrared spectroscopy; Raman and visible spectroscopy; Diamond anvil cell techniques for static high pressure; Gas-gun launchers for dynamic compression; Cryogenic techniques combined with DACs;

274

Measuring The Source Brilliance at An Undulator Beamline  

SciTech Connect

Third-generation X-ray synchrotrons like the European Synchrotron Radiation Facility (ESRF) are optimized to produce intense undulator radiation. Insertion devices, such as undulators, ensure the highest possible brilliance--the key parameter for the success of e.g. coherent scattering, which is one of the main techniques employed at ESRF's TROIKA beamline. Nowadays, the constant efforts to reduce the emittance and improve the stability of the electron beam allow using small-gap insertion devices and increase the brilliance. Obviously, it is important to have an experimental technique for evaluating the performance of the undulator source. Here we present a method based on measuring the diffuse scattering from a light amorphous material by a photon counting detector. The measured spectral intensities show a very good agreement with the simulated spectra, demonstrating the high brilliance (above 10{sup 20} ph/s/0.1%bw/mrad{sup 2}/mm{sup 2}) achieved at modern facilities.

Zontone, Federico; Madsen, Anders; Konovalov, Oleg [European Synchrotron Radiation Facility, BP220, F-38043 Grenoble Cedex (France)

2010-06-23T23:59:59.000Z

275

Photon Sciences | Beamlines | SRX: Submicron Resolution X-ray Spectroscopy  

NLE Websites -- All DOE Office Websites (Extended Search)

SRX: Submicron Resolution X-ray Spectroscopy SRX: Submicron Resolution X-ray Spectroscopy Poster | Fact Sheet | Preliminary Design Report Scientific Scope Scientific communities such as environmental sciences, life sciences, and material sciences have identified the need to develop analytical resources to advance the understanding of complex natural and engineered systems that are heterogeneous on the micron to nanometer scale. These needs for high intensity x-ray nanoprobes resulted in the commitment of the NSLS-II Project to build the Submicron Resolution X-ray (SRX) Spectroscopy beamline showing a unique combination of high spectral resolution over a very broad energy range and very high beam intensity in a sub-micrometer spot. NSLS-II will provide one of the best sources in the world for such an instrument.

276

ANL/APS/TB-21 Radiation Shielding of Insertion Device Beamlines  

NLE Websites -- All DOE Office Websites (Extended Search)

1 1 Radiation Shielding of Insertion Device Beamlines Using a Mirror as the First Optical Element W. Yun, B. Lai, K. J. Randall, S. Davey, D. R. Haeffner, P. K. Job, and D. Shu February 1995 Abstract The radiation shielding for an Advanced Photon Source (APS) insertion device beamline using a mirror as the first optical component is discussed. The beamline layout for a specific Synchrotron Radiation Instrumentation Collaborative Access Team beamline (sector 2 of SRI CAT) is described, and the methodology used to determine the radiation shielding is presented. Results indicate that, by using a x-ray mirror with a critical energy of 32 keV for total reflection, an undulator beam containing nearly all x-rays in the 0 - 32 keV spectral range can be delivered

277

E-Print Network 3.0 - aps beamline front Sample Search Results  

NLE Websites -- All DOE Office Websites (Extended Search)

Page 1 of 11 Policy& Procedure : 3.1.37 Summary: The beamline front end provides the UHV transition from the APS storage ring through the ratchet wall... to the portions of the...

278

Time Resolved Detectors and Measurements for Accelerators and Beamlines at the Australian Synchrotron  

SciTech Connect

Time resolved experiments require precision timing equipment and careful configuration of the machine and the beamline. The Australian Synchrotron has a state of the art timing system that allows flexible, real-time control of the machine and beamline timing parameters to target specific electron bunches. Results from a proof-of-principle measurement with a pulsed laser and a streak camera on the optical diagnostic beamline will be presented. The timing system was also used to fast trigger the PILATUS detector on an x-ray beamline to measure the fill pattern dependent effects of the detector. PILATUS was able to coarsely measure the fill pattern in the storage ring which implies that fill pattern intensity variations need to be corrected for when using the detector in this mode.

Boland, M. J. [Australian Synchrotron, Clayton, Victoria 3168 (Australia); School of Physics, University of Melbourne, Parkville, Victoria 3010 (Australia); Rassool, R. P.; Peake, D. J.; Sobott, B. A.; Lee, V.; Schubert, A. [School of Physics, University of Melbourne, Parkville, Victoria 3010 (Australia); LeBlanc, G. S.; Kirby, N. [Australian Synchrotron, Clayton, Victoria 3168 (Australia)

2010-06-23T23:59:59.000Z

279

New Soft X-ray Beamline (BL10) at the SAGA Light Source  

SciTech Connect

A new soft X-ray beamline (BL10) at the SAGA Light Source (SAGA-LS) was constructed at the end of 2008. Commissioning of this new beamline started at the beginning of 2009. Synchrotron radiation from a variably polarizing undulator (APPLE-II) can be used in this beamline. The obtained light is monochromatized by a varied-line-spacing plane grating monochromator with the variable included angle mechanism. Its designed resolving power and photon flux are 3,000-10,000 and 10{sup 12}-10{sup 9} photons/s at 300 mA, respectively. The performance test results were generally satisfactory. An overview of the optical design of the beamline and the current status of commissioning are reported.

Yoshimura, D.; Setoyama, H.; Okajima, T. [Beamline group, SAGA Light Source, 8-7 Yayoigaoka, Tosu, Saga 841-0005 (Japan)

2010-06-23T23:59:59.000Z

280

Development of soft X-ray polarized light beamline on Indus-2 synchrotron radiation source  

SciTech Connect

This article describes the development of a soft x-ray beamline on a bending magnet source of Indus-2 storage ring (2.5 GeV) and some preliminary results of x-ray absorption spectroscopy (XAS) measurements using the same. The beamline layout is based on a spherical grating monochromator. The beamline is able to accept synchrotron radiation from the bending magnet port BL-1 of the Indus-2 ring with a wide solid angle. The large horizontal and vertical angular acceptance contributes to high photon flux and selective polarization respectively. The complete beamline is tested for ultrahigh vacuum (UHV) ? 10{sup ?10} mbar. First absorption spectrum was obtained on HOPG graphite foil. Our performance test indicates that modest resolving power has been achieved with adequate photon flux to carry out various absorption experiments.

Phase, D. M., E-mail: mgupta@csr.res.in; Gupta, Mukul, E-mail: mgupta@csr.res.in; Potdar, S., E-mail: mgupta@csr.res.in; Behera, L., E-mail: mgupta@csr.res.in; Sah, R., E-mail: mgupta@csr.res.in; Gupta, Ajay, E-mail: mgupta@csr.res.in [UGC-DAE Consortium for Scientific Research, University Campus, Khandwa Road, Indore, 452001 (India)

2014-04-24T23:59:59.000Z

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


281

E-Print Network 3.0 - aps wiggler beamline Sample Search Results  

NLE Websites -- All DOE Office Websites (Extended Search)

SPX BEAMLINES The crab cavity scheme (sections 3.5 and 6... .1), offers a unique tunable high average flux source of 1ps x-rays. We propose to develop two ... Source:...

282

ANL/APS/TB-14 APS Beamline Design and Construction Requirements:  

NLE Websites -- All DOE Office Websites (Extended Search)

14 14 APS Beamline Design and Construction Requirements: A Reference Manual for Designers and Builders Version 1.0 May 1994 iii TABLE OF CONTENTS SECTION I DEFINITIONS, GUIDELINES, AND REVIEW CRITERIA ............................1 1. Introduction (July 21, 1998) ...............................................................................................1 1.1 About the Advanced Photon Source ...........................................................................1 1.2 About this Manual.......................................................................................................1 2. Beamline Definitions and Responsibilities (July 21, 1998) .................................................2 2.1 Definitions...................................................................................................................2

283

Fundamental Neutron Physics Beamline at the Spallation Neutron Source at ORNL  

E-Print Network (OSTI)

We describe the Fundamental Neutron Physics Beamline (FnPB) facility located at the Spallation Neutron Source at Oak Ridge National Laboratory. The FnPB was designed for the conduct of experiments that investigate scientific issues in nuclear physics, particle physics, astrophysics and cosmology using a pulsed slow neutron beam. We present a detailed description of the design philosophy, beamline components, and measured fluxes of the polychromatic and monochromatic beams.

N. Fomin; G. L. Greene; R. Allen; V. Cianciolo; C. Crawford; T. Ito; P. R. Huffman; E. B. Iverson; R. Mahurin; W. M. Snow

2014-08-04T23:59:59.000Z

284

Automatic sample Dewar for MX beam-line  

SciTech Connect

It is very common for crystals of large biological macromolecules to show considerable variation in quality of their diffraction. In order to increase the number of samples that are tested for diffraction quality before any full data collections at the ESRF*, an automatic sample Dewar has been implemented. Conception and performances of the Dewar are reported in this paper. The automatic sample Dewar has 240 samples capability with automatic loading/unloading ports. The storing Dewar is capable to work with robots and it can be integrated in a full automatic MX** beam-line. The samples are positioned in the front of the loading/unloading ports with and automatic rotating plate. A view port has been implemented for data matrix camera reading on each sample loaded in the Dewar. At last, the Dewar is insulated with polyurethane foam that keeps the liquid nitrogen consumption below 1.6 L/h. At last, the static insulation also makes vacuum equipment and maintenance unnecessary. This Dewar will be useful for increasing the number of samples tested in synchrotrons.

Charignon, T.; Tanchon, J.; Trollier, T.; Ravex, A. [Absolut-System, Meylan, 38240 (France); Theveneau, P. [European Synchrotron Radiation Facility, Grenoble, 38000 (France)

2014-01-29T23:59:59.000Z

285

Design of a High Flux Vacuum-Ultraviolet Beamline for Circular Dichroism Experiments  

SciTech Connect

A vacuum-ultraviolet bending-magnet beamline for circular dichroism (CD) experiments has been designed. To maximize the photon flux and minimize the focused beam size, a cylindrical mirror and a cylindrical grating with independent optical functions are utilized. The beamline can collect a 30 mrad horizontal by 7 mrad vertical solid angle of synchrotron radiation. By using a 600 grooves/mm grating, the calculated photon flux is greater than 1x10{sup 13} photons/sec and the focused beam size is 0.4 mmx0.65 mm for the spectral range from 130 nm to 330 nm with the energy resolving power set at 1000. The linear polarization degree is better than 75% and can be increased to 90% by reducing the vertical acceptance angle down to 2 mrad. In addition to the high flux mode described above, this beamline can also be operated in a high resolution mode. By using a 1200 grooves/mm grating, a resolving power greater than 10,000 can be achieved for the spectral range from 180 to 330 nm. This beamline can provide photon flux as high as the best synchrotron CD beamlines in the world while offers simultaneously a smaller focused beam size.

Fu, H. W.; Fung, H. S.; Chung, S. C.; Huang, L. J.; Chen, C. T. [National Synchrotron Radiation Research Center, Hsinchu 30076, Taiwan (China)

2010-06-23T23:59:59.000Z

286

Application of Partially coherent Wavefront Propagation Calculations for Design of Coherence-Preserving Synchrotron Radiation Beamlines  

SciTech Connect

Ultra-low emittance third-generation synchrotron radiation (SR) sources, such as NSLS-II and MAX-IV, will offer excellent opportunities for further development of experimental techniques exploiting X-ray coherence. However, even in these new SR sources, the radiation produced by relativistic electrons (in undulators, wigglers and bending magnets) will remain only partially coherent in the X-ray spectral range. 'Extraction' of 'coherent portion' of the radiation flux and its transport to sample without loss of coherence must be performed by dedicated SR beamlines, optimized for particular types of experiments. Detailed quantitative prediction of partially coherent X-ray beam properties at propagation through optical elements, which is required for the optimization of such beamlines, can only be obtained from accurate and efficient physical-optics based numerical simulations. Examples of such simulations, made for NSLS-II beamlines, using 'Synchrotron Radiation Workshop' (SRW) computer code, are presented. Special attention is paid to the numerical analysis of the basic properties of partially coherent undulator radiation beam and its distinctions from the Gaussian beam. Performance characteristics of importance for particular beamlines, such as radiation spot size and flux at sample vs size of secondary source aperture for high-resolution microscopy beamlines, are predicted by the simulations.

O Chubar; Y Chu; K Kaznatcheev; h Yan

2011-12-31T23:59:59.000Z

287

CAT Guide and Beamline Directory. A key to APS Collaborative Access Teams  

SciTech Connect

The Advanced Photon Source (APS), a national user facility for synchrotrons radiation research, is located at Argonne National Laboratory, approximately 25 miles southwest of Chicago, Illinois. The APS is considered a third-generation synchrotrons radiation facility (specifically designed to accommodate insertion devices to serve as radiation sources) and is one of three such facilities in the world. Currently, it is the most brilliant source in the United States for research in such diverse fields as biology, medicine, materials science, chemistry, geology, agriculture and soil science, physics, and manufacturing technology. Researchers use the APS either as members of Collaborative Access Teams (CATS) or as Independent Investigators (IIs). CATS are responsible for designing, building, and operating beamlines in one or more sectors, each sector consisting of an insertion-device (ID) beamline and a bending-magnet (BM) beamline. Each beamline is designed to accommodate a specific type of research program(s) and is optimized accordingly. CAT members are entitled to use 75% of the available beam time to pursue CAT research goals. The remaining 25% of the available beam time must be made available to IIs. This document was written to help prospective IIs determine which beamlines are suitable for their specific experiments.

NONE

1999-07-08T23:59:59.000Z

288

Photon Sciences | Beamlines | CSX: Coherent Soft X-ray Scattering and  

NLE Websites -- All DOE Office Websites (Extended Search)

CSX: Coherent Soft X-ray Scattering and polarization CSX: Coherent Soft X-ray Scattering and polarization X-Ray 1 Poster | X-Ray 2 Poster | Fact Sheet | Preliminary Design Report Scientific Scope The Coherent Soft X-ray Scattering and Polarization (CSX) beamline design (source and optics) has been optimized to the NSLS-II parameters to provide the highest possible flux for experiments requiring either high coherence or full control of the polarization. Beamline Description The CSX beamline will be served by two identical EPU49 sources. Both EPUs are planned to operate in a canted geometry with opposite circular polarization for fast polarization switching experiments at the full polarization control (PC) branch. The EPUs will also be able to operate "phased" as a single device for high coherent flux experiments at the

289

Development and Application of the STARS-based Beamline Control System at the Photon Factory  

SciTech Connect

STARS{sup [1-2]}(Simple Transmission and Retrieval System) is a message transferring software for small-scale control systems with TCP/IP sockets, originally developed at the Photon Factory (PF). Because it has a server-client architecture using TCP/IP sockets and can work on various types of operating systems, the design and application are quite flexible. We have developed a common low-level beamline control system based on the STARS technology. Many kinds of useful STARS clients (device drivers, data acquisitions, user interfaces etc.) are available now, and so far, the system has been installed at 22 PF beamlines. We will describe the development and generalize of the STARS-based beamline control system at the PF.

Kosuge, Takashi; Nigorikawa, Kazuyuki; Nagatani, Yasuko; Saito, Yuuki [Photon Factory, 1-1 Oho Tsukuba-shi Ibaraki-ken 305-0801 (Japan)

2010-06-23T23:59:59.000Z

290

Optical Design of VLS-PGM Soft X-Ray Beamline on Indus-2  

SciTech Connect

The optical design of a soft x-ray beamline on the bending magnet of Indus-2 synchrotron source is presented. A Varied Line Spacing Plane Grating Monochromator (VLS-PGM) was adopted with Hettrick type optics. The VLS-PGM consists of a spherical mirror and three interchangeable gratings of line densities 1200 l/mm, 400 l/mm and 150 l/mm to efficiently cover the energy region 50-1500 eV. The VLS groove parameters were obtained by minimizing defocus aberration, coma and spherical aberration. The overall performance of the beamline was estimated by detailed raytracing calculations. The beamline design, results of the raytracing calculations and the expected performances are presented.

Prasad, T. T.; Modi, M. H.; Lodha, G. S. [X-ray Optics Section, Indus Synchrotrons Ultilization Division, Raja Ramanna Centre for Advanced Technology, Indore (India)

2010-06-23T23:59:59.000Z

291

The Design of Superconducting Wiggler Beamline BL7 at SAGA-LS  

SciTech Connect

A new hard X-ray beamline has been designed at Saga Light Source. The beamline, named BL7, uses a newly developed 4-Tesla superconducting wiggler as a light source in order to cover a wide energy range to 30 keV. This beamline has a simple optics: a double-crystal monochromator and a Rh-coated bent-cylindrical mirror and can supply a focused beam with a photon flux about 1x10{sup 10} photons/s and a sub-millimeter size. Several experiments will be performed in the experimental station: e.g. protein crystallography; X-ray micro computed tomography; X-ray absorption fine structure measurement.

Kawamoto, M.; Sumitani, K.; Okajima, T. [Beamline Group, Kyushu Synchrotron Light Research Center, Tosu, Saga 841-0005 (Japan)

2010-06-23T23:59:59.000Z

292

Analysis of the optical design of the NSLS-II Coherent Hard X-ray beamline  

SciTech Connect

Ultra-low emittance third-generation synchrotron radiation sources such as the NSLS-II offer excellent opportunities for the development of experimental techniques exploiting x-ray coherence. Coherent light scattered by a heterogeneous sample produces a speckle pattern characteristic for the specific arrangement of the scatterers. This may vary over time, and the resultant intensity fluctuations can be measured and analyzed to provide information about the sample dynamics. X-ray photon correlation spectroscopy (XPCS) extends the capability of dynamic light scattering to opaque and turbid samples and extends the measurements of time evolution to nanometer length scales. As a consequence XPCS became crucial in the study of dynamics in systems including, but not being limited to, colloids, polymers, complex fluids, surfaces and interfaces, phase ordering alloys, etc. In this paper we present the conceptual optical design and the theoretical performance of the Coherent Hard X-ray (CHX) beamline at NSLS-II, dedicated to XPCS and other coherent scattering techniques. For the optical design of this beamline, there is a tradeoff between the coherence needed to distinguish individual speckles and the phase acceptance (high intensity) required to measure fast dynamics with an adequate signal-to-noise level. As XPCS is a 'photon hungry' technique, the beamline optimization requires maximizing the signal-to-noise ratio of the measured intensity-intensity autocorrelation function. The degree of coherence, as measured by a two-slit (Young) experiment, is used to characterize the speckle pattern visibilities. The beamline optimization strategy consists of maximization of the on-sample intensity while keeping the degree of coherence within the 0.1-0.5 range. The resulted design deviates substantially from an ad-hoc modification of a hard x-ray beamline for XPCS measurements. The CHX beamline will permit studies of complex systems and measurements of bulk dynamics down to the microsecond time scales. In general, the 10-fold increase in brightness of the NSLS-II, compared to other sources, will allow for measurements of dynamics on time-scales that are two orders of magnitude faster than what is currently possible. We also conclude that the common approximations used in evaluating the transverse coherence length would not be sufficiently accurate for the calculation of the coherent properties of an undulator-based beamline, and a thorough beamline optimization at a low-emittance source such as the NSLS-II requires a realistic wave-front propagation analysis.

Fluerasu A.; Chubar, O.; Kaznatcheev, K.; Baltser, J.; Wiegart, Lutz; Evans-Lutterodt, K.; Carlucci-Dayton, M.; Berman, L.

2011-08-21T23:59:59.000Z

293

Data acquisition and control software for XRD beamline at Indus?2  

Science Journals Connector (OSTI)

X?ray diffraction (XRD) beamline is under commissioning on Indus?2 synchrotron radiation facility. The experimental setup of XRD beamline consists of a six?circle diffractometer and various detector systems such as scintillation detector ionization chamber and image plate. The diffractometer can be controlled via EIA232 serial interface or Ethernet. Standard data acquisition software with a graphical user interface has been developed using LabVIEW. A firm safety and error handling scheme is implemented for failsafe operation of the experimental station. This paper describes in detail the data acquisition and control software for the experimental station.

Sanjeev R. Kane; C. K. Garg; A. K. Sinha

2010-01-01T23:59:59.000Z

294

APS beamline standard components handbook, Version 1.3. Revision 1  

SciTech Connect

This Handbook in its current version (1.3) contains descriptions, specifications, and preliminary engineering design drawings for many of the standard components. The design status and schedules have been provided wherever possible. In the near future, the APS plans to update engineering drawings of identified standard beamline components and complete the Handbook. The completed version of this Handbook will become available to both the CATs and potential vendors. Use of standard components should result in major cost reductions for CATs in the areas of beamline design and construction.

Hahn, U.; Shu, D.; Kuzay, T.M.

1993-02-01T23:59:59.000Z

295

The New Structural Materials Science Beamlines BL8A and 8B at Photon Factory  

SciTech Connect

BL8A and 8B are new beamlines for structural materials science at Photon Factory. The primary characteristics of both beamlines are similar. The incident beam is monochromatized by the Si(111) double-flat crystal monochromator and focused at the sample position by a Rh-coated bent cylindrical quartz mirror. The Weissenberg-camera-type imaging-plate (IP) diffractometers were installed. The X-ray diffraction experiments for structural studies of strongly correlated materials, such as transition metals, molecular conductors, endohedral fullerenes, nano-materials, etc, are conducted at these stations.

Nakao, A.; Sugiyama, H.; Koyama, A.; Watanabe, K. [Insttitute of Materials Science, High Energy Accelerator Research Organization, 1-1 Oho, Tsukuba, Ibaraki 305-0801 (Japan)

2010-06-23T23:59:59.000Z

296

Design of the First Infrared Beamline at the Siam Photon Laboratory  

SciTech Connect

This report presents the optical design and optical simulations for the first infrared beamline at the Siam Photon Laboratory. The beamline collects the edge radiation and bending magnet radiation, producing from the BM4 bending magnet of the 1.2 GeV storage ring of the Siam Photon Source. The optical design is optimized for the far- to mid-infrared spectral range (4000-100 cm{sup -1}) for microspectroscopic applications. The optical performance has been examined by computer simulations.

Pattanasiriwisawa, W. [Synchrotron Light Research Institute, P.O. Box 93, Muang, Nakhon Ratchasima 30000 (Thailand); Songsiriritthigul, P. [Synchrotron Light Research Institute, P.O. Box 93, Muang, Nakhon Ratchasima 30000 (Thailand); School of Physics, Suranaree University of Technology, Muang, Nakhon Ratchasima 30000 (Thailand); Dumas, P. [SOLEIL Synchrotron, L'Orme des Merisiers, BP48, F-91192 Gif sur Yvette Cedex (France)

2010-06-23T23:59:59.000Z

297

The X-ray microscopy beamline UE46-PGM2 at BESSY  

SciTech Connect

The Max Planck Institute for Metal Physics in Stuttgart and the Helmholtz Center Berlin operate a soft X-ray microscopy beamline at the storage ring BESSY II. A collimated PGM serves as monochromator for a scanning X-ray microscope and a full field X-ray microscope at the helical undulator UE46. The selection between both instruments is accomplished via two switchable focusing mirrors. The scanning microscope (SM) is based on the ALS STXM microscope and fabricated by the ACCEL company. The full field microscope (FFM) is currently in operation at the U41-SGM beamline and will be relocated to its final location this year.

Follath, R.; Schmidt, J. S. [Helmholtz-Center Berlin, Albert-Einstein-Strasse 15, 12489 Berlin (Germany); Weigand, M. [Max Planck Institute for Metals Research, Heisenbergstrasse 3, 70569 Stuttgart (Germany); Fauth, K. [University Erlangen, Experimental Physics 4, Am Hubland, 97074 Wuerzburg (Germany)

2010-06-23T23:59:59.000Z

298

Correlated single-crystal electronic absorption spectroscopy and X-ray crystallography at NSLS beamline X26-C  

SciTech Connect

The research philosophy and new capabilities installed at NSLS beamline X26-C to support electronic absorption and Raman spectroscopies coupled with X-ray diffraction are reviewed. This beamline is dedicated full time to multidisciplinary studies with goals that include revealing the relationship between the electronic and atomic structures in macromolecules. The beamline instrumentation has been fully integrated such that optical absorption spectra and X-ray diffraction images are interlaced. Therefore, optical changes induced by X-ray exposure can be correlated with X-ray diffraction data collection. The installation of Raman spectroscopy into the beamline is also briefly reviewed. Data are now routinely generated almost simultaneously from three complementary types of experiments from the same sample. The beamline is available now to the NSLS general user population.

Orville, A.M.; Buono, R.; Cowan, M.; Heroux, A.; Shea-McCarthy, G.; Schneider, D. K.; Skinner, J. M.; Skinner, M. J.; Stoner-Ma, D.; Sweet, R. M.

2011-05-01T23:59:59.000Z

299

Correlated Single-Crystal Electronic Absorption Spectroscopy and X-ray Crystallography at NSLS Beamline X26-C  

SciTech Connect

The research philosophy and new capabilities installed at NSLS beamline X26-C to support electronic absorption and Raman spectroscopies coupled with X-ray diffraction are reviewed. This beamline is dedicated full time to multidisciplinary studies with goals that include revealing the relationship between the electronic and atomic structures in macromolecules. The beamline instrumentation has been fully integrated such that optical absorption spectra and X-ray diffraction images are interlaced. Therefore, optical changes induced by X-ray exposure can be correlated with X-ray diffraction data collection. The installation of Raman spectroscopy into the beamline is also briefly reviewed. Data are now routinely generated almost simultaneously from three complementary types of experiments from the same sample. The beamline is available now to the NSLS general user population.

A Orville; R Buono; M Cowan; A Heroux; G Shea-McCarthy; D Schneider; J Skinner; M Skinner; D Stoner-Ma; R Sweet

2011-12-31T23:59:59.000Z

300

Performance of new infrared beamline U12IR at the National Synchrotron Light Source  

E-Print Network (OSTI)

frequency limit of 2 cm 1 i.e., 60 GHz or a photon energy of 250 eV . The infrared light from infrared beamline at the NSLS and, with increasing demand for measurement time, has been followed by a series of new infrared ports presently under construction and com- missioning. This also allowed for some

Tanner, David B.

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


301

7-GeV advanced photon source beamline initiative: Conceptual design report  

SciTech Connect

The DOE is building a new generation 6-7 GeV Synchrotron Radiation Source known as the Advanced Photon Source (APS) at Argonne National Laboratory. This facility, to be completed in FY 1996, can provide 70 x-ray sources of unprecedented brightness to meet the research needs of virtually all scientific disciplines and numerous technologies. The technological research capability of the APS in the areas of energy, communications and health will enable a new partnership between the DOE and US industry. Current funding for the APS will complete the current phase of construction so that scientists can begin their applications in FY 1996. Comprehensive utilization of the unique properties of APS beams will enable cutting-edge research not currently possible. It is now appropriate to plan to construct additional radiation sources and beamline standard components to meet the excess demands of the APS users. In this APS Beamline Initiative, 2.5-m-long insertion-device x-ray sources will be built on four straight sections of the APS storage ring, and an additional four bending-magnet sources will also be put in use. The front ends for these eight x-ray sources will be built to contain and safeguard access to these bright x-ray beams. In addition, funds will be provided to build standard beamline components to meet scientific and technological research demands of the Collaborative Access Teams. The Conceptual Design Report (CDR) for the APS Beamline Initiative describes the scope of all the above technical and conventional construction and provides a detailed cost and schedule for these activities. The document also describes the preconstruction R&D plans for the Beamline Initiative activities and provides the cost estimates for the required R&D.

Not Available

1993-05-01T23:59:59.000Z

302

National Synchrotron Light Source user`s manual: Guide to the VUV and x-ray beamlines. Fifth edition  

SciTech Connect

The success of the National Synchrotron Light Source is based, in large part, on the size of the user community and the diversity of the scientific and technical disciplines represented by these users. As evidence of this success, the VUV Ring has just celebrated its 10th anniversary and the X-ray Ring will do the same in 1995. In order to enhance this success, the NSLS User`s Manual: Guide to the VUV and X-Ray Beamlines - Fifth Edition, is being published. This Manual presents to the scientific community-at-large the current and projected architecture, capabilities and research programs of the various VUV and X-ray beamlines. Also detailed is the research and computer equipment a General User can expect to find and use at each beamline when working at the NSLS. The Manual is updated periodically in order to keep pace with the constant changes on these beamlines.

Gmuer, N.F. [ed.

1993-04-01T23:59:59.000Z

303

Optical design and performance of the inelastic scattering beamline at the National Synchrotron Light Source  

SciTech Connect

Phase I of the X21 beamline at the National Synchrotron Light Source was commissioned during 1993. The research program at the X21 beamline is focused on the study of electronic excitations in condensed matter with total energy resolution of 0.1 eV to 1.0 eV. The source is a 27 pole hybrid wiggler. A water-cooled horizontal focusing Si(220) monochromator and a spherically bent Si(444) analyzer were installed and commissioned. At 8 keV the energy resolution of the monochromator is about 0.7 eV, and the energy resolution of the analyzer is about 0.1 eV. Results from several selected experiments are also discussed.

Kao, C.C.; Siddons, D.P.; Oversluizen, T.; Hastings, J.B. [Brookhaven National Lab., Upton, NY (United States); Hamalainen, K. [Helsinki Univ. (Finland). Dept. of Physics; Krisch, M. [European Synchrotron Radiation Facility, 38 - Grenoble (France)

1994-12-31T23:59:59.000Z

304

ANL/APS/TB-24 Diamond Monochromators for APS Undulator-A Beamlines  

NLE Websites -- All DOE Office Websites (Extended Search)

4 4 Diamond Monochromators for APS Undulator-A Beamlines R.C. Blasdell, L. A. Assoufid, and D. M. Mills TABLE OF CONTENTS 1. INTRODUCTION .................................................................................1 2. PHYSICAL PROPERTIES OF DIAMONDS ..................................................5 2.1 Varieties of Diamonds ....................................................................5 2.2 The Lattice Parameter .....................................................................5 2.3 Bulk Thermal and Mechanical Properties ...............................................6 2.4 Typical Surface and Lattice Plane Morphology ......................................8 2.5 The Liquid-GaIn/Diamond Interface ...................................................10 3. DIFFRACTION PROPERTIES OF DIAMOND

305

Beamline Front-End for Minipole Undulator at the Photon Factory Storage Ring  

SciTech Connect

The straight-section upgrade project of the Photon Factory created four new short straight sections capable of housing in-vacuum minipole undulators. The first to third minipole undulators SGU no. 17, SGU no. 03 and SGU no. 01 were installed at the 2.5-GeV Photon Factory storage ring in 2005, 2006 and 2009, respectively. The beamline front ends for SGU0 no. 3 and SGU0 no. 1 are described in this paper.

Miyauchi, Hiroshi; Tahara, Toshihiro; Asaoka, Seiji [Photon Factory, High Energy Accelerator Research Organization, KEK Oho, Tsukuba, Ibakaki 305-0801 (Japan)

2010-06-23T23:59:59.000Z

306

Design of the angiography beamline for the Argonne Advanced Photon Source  

Science Journals Connector (OSTI)

The angiography beamline planned for the Argonne Advanced Photon Source (APS) is a very special beamline dedicated to medical imaging. It is especially designed to enhance the art of digital subtraction angiography. It is different from the angiography beamlines presently in operation that scan the X-ray picture line by line, in that it will take both the high and low energy angiography X-ray pixtures simultaneously as full frame pictures. Pictures with 0.25 mm resolution and good signal to noise will be possible with 2 ms exposure times. This is possible because of the increase in flux that is available at the APS. The source of the 33 keV photons is a special high intensity wiggler. The photon beam is separated into two parts, spread out in the vertical direction, and monochro- matized with two convex bent crystals. These two crystals are bent in a non-uniform way that allows one to both make the photon flux uniform over the 15 cm 15 cm examining area and stabilize the shape of the surface of the diffraction crystal against distortion caused by the heat load on the crystal. Most of the energy of the photon beam is absorbed by a fast shutter placed in front of the crystals. The two images at the two different energies are recorded in two large position-sensitive detectors.

Robert K. Smither; Edwin M. Westbrook

1988-01-01T23:59:59.000Z

307

Photostimulated phosphor based image plate detection system for HRVUV beamline at Indus-1 synchrotron radiation source  

E-Print Network (OSTI)

A high resolution vacuum ultraviolet (HRVUV) beamline based on a 6.65 meter off-plane Eagle spectrometer is in operation at the Indus-1 synchrotron radiation source, RRCAT, Indore, India. To facilitate position sensitive detection and fast spectral recording, a new BaFBr:Eu2+ phosphor based image plate (IP) detection system interchangeable with the existing photomultiplier (PMT) scanning system has been installed on this beamline. VUV photoabsorption studies on Xe, O2, N2O and SO2 are carried out to evaluate the performance of the IP detection system. An FWHM of ~ 0.5 {\\AA} is achieved for the Xe atomic line at 1469.6 {\\AA}. Reproducibility of spectra is found to be within the experimental resolution. Compared to the PMT scanning system, the IP shows several advantages in terms of sensitivity, recording time and S/N ratio, which are highlighted in the paper. This is the first report of incorporation of an IP detection system in a VUV beamline using synchrotron radiation. Commissioning of the new detection sys...

Haris, K; Shastri, Aparna; K., Sunanda; K., Babita; Rao, S V N Bhaskara; Ahmad, Shabbir; Tauheed, A

2014-01-01T23:59:59.000Z

308

Time-Resolved Research at the Advanced Photon Source Beamline 7-ID  

SciTech Connect

The Sector 7 undulator beamline (7-ID) of the Advanced Photon Source (APS) is dedicated to time-resolved x-ray research and is capable of ultrafast measurements on the order of 100 ps. Beamline 7-ID has a laser laboratory featuring a Ti:Sapphire system (average power of 2.5W, pulse duration <50 fs, repetition rate 1-5 kHz) that can be synchronized to the bunch pattern of the storage ring. The laser is deliverable to x-ray enclosures, which contain diffractometers, as well as motorized optical tables for table-top experiments. Beamline 7-ID has a single APS Undulator A and uses a diamond (111) double-crystal monochromator, providing good energy resolution over a range of 6-24 keV. Available optics include Kirkpatrick-Baez (KB) mirrors to microfocus the x-ray beam. A variety of time-resolved diffraction and spectroscopy research is available at 7-ID, with experiments being done in the atomic, molecular, optical, chemistry, and solid state (bulk and surface) fields.

Dufresne, Eric M.; Adams, Bernhard; Arms, Dohn A.; Chollet, Matthieu; Landahl, Eric C.; Li, Yuelin; Walko, Donald A.; Wang, Jin

2010-08-02T23:59:59.000Z

309

Optical Design in Phase-Space for the I13L X-Ray Imaging and Coherence Beamline at Diamond using XPHASY  

SciTech Connect

I13L is a 250 m long beamline for imaging and coherent diffraction currently under construction at the Diamond Light Source. For modeling the beamline optics the phase-space based ray-tracing code XPHASY was developed, as general ray-tracing codes for x-rays do not easily allow studying the propagation of coherence along the beamline. In contrast to computational intensive wave-front propagation codes, which fully describe the propagation of a photon-beam along a beamline but obscure the impact of individual optical components onto the beamline performance, this code allows to quickly calculate the photon-beam propagation along the beamline and estimate the impact of individual components.In this paper we will discuss the optical design of the I13L coherence branch from the perspective of phase-space by using XPHASY. We will demonstrate how the phase-space representation of a photon-beam allows estimating the coherence length at any given position along the beamline. The impact of optical components on the coherence length and the effect of vibrations on the beamline performance will be discussed. The paper will demonstrate how the phase-space representation of photon-beams allows a more detailed insight into the optical performance of a coherence beamline than ray-tracing in real space.

Wagner, Ulrich H. [Science, Diamond Light Source Ltd., Didcot, Oxon OX11 0DE (United Kingdom); Rau, Christoph [Science, Diamond Light Source Ltd., Didcot, Oxon OX11 0DE (United Kingdom); Northwestern University, Chicago (United States)

2010-06-23T23:59:59.000Z

310

Cycle cover with short cycles Nicole Immorlica  

E-Print Network (OSTI)

Introduction Given a graph and a subset of marked elements (nodes, edges, or some combination thereof), a cycleCycle cover with short cycles Nicole Immorlica£ Mohammad Mahdian£ Vahab S. Mirrokni£ Abstract Cycle for variants of cycle covering problems which bound the size and/or length of the covering cycles

Immorlica, Nicole

311

100-J level amplifier concepts for HiLASE and ELI-Beamlines  

Science Journals Connector (OSTI)

We present comparison of two alternative layouts of a 100 J cryogenically cooled Yb:YAG multi-slab laser system operating at 10 Hz for HiLASE and ELI Beamlines projects. In the first approach the 100 J slab amplifier consists of a preamplifier and power amplifier while in the second approach it uses single power amplifier with two amplifier heads. These two concepts are compared with respect to output power B-integral accumulated B-integral and peak fluence. Results are obtained by simulating beam propagation in MIR code and calculating stored energy in the amplifier by homemade ray-tracing MATLAB code for amplified spontaneous emission evaluation.

2012-01-01T23:59:59.000Z

312

SYNCH: A program for design and analysis of synchrotrons and beamlines -- user`s guide  

SciTech Connect

SYNCH is a computer program for use in the design and analysis of synchrotrons, storage rings, and beamlines. It has a large repertoire of commands that can be accessed in a flexible way. The input statements and the results of the calculations they invoke are saved in an internal database so that this information may be shared by other statements. SYNCH is the first accelerator program to organize its input in the form of a language. The statements, which resemble sentences, provide a natural way of describing lattices and invoking relevant calculations. The organization of the program is modular, so that it has been possible to expand its capabilities progressively.

Garren, A.A.; Kenney, A.S.; Courant, E.D.; Russell, A.D.; Syphers, M.J.

1993-12-31T23:59:59.000Z

313

The New X-Ray Lithography Beamline BL1 At DELTA  

SciTech Connect

Lithography using synchrotron radiation in the x-ray regime provides a powerful method to produce mechanical components of sub-millimeter size with a very good quality for microtechnological applications. In recent years the demand for x-ray lithography beamtime for industrial production of microparts increased rapidly resulting in the development of new experimental endstations at synchrotron radiation sources dedicated for the production of micromechanical devices. We present in this work the layout of the new x-ray lithography beamline BL1 at the synchrotron radiation source DELTA in Dortmund and discuss first results of exposure tests.

Lietz, D.; Paulus, M.; Sternemann, C.; Berges, U.; Hippert, B.; Tolan, M. [Fakultaet Physik / DELTA, TU Dortmund, Maria-Goeppert-Mayer-Str. 2, 44227 Dortmund (Germany)

2010-06-23T23:59:59.000Z

314

X-ray Experiments for Students at the SLS Optics Beamline  

SciTech Connect

We present a X-ray training course for students. The course covers fundamental properties of synchrotron radiation and basic techniques like scattering and absorption. We prepared ten experiments together with a tutorial. The whole course takes about a week. A first student group from the University of Copenhagen passed the course in June 2009. The experiments were performed at the optics beamline of the Swiss Light Source which can be part-time allocated for training purposes. Two experiments are described in more detail: scattering from a hanging drop of water turning into ice and measurement of the power of a pink synchrotron beam using a simple calorimeter.

Flechsig, U.; Jaggi, A.; Krempasky, J.; Oberta, P.; Spielmann, S.; Veen, J. F. van der [Paul Scherrer Institut, Swiss Light Source, 5232 Villigen PSI (Switzerland); Als-Nielsen, J. [University of Copenhagen, Universitetsparken 5, DK 2100 Copenhagen (Denmark)

2010-06-23T23:59:59.000Z

315

Achieving Vibration Stability of the NSLS-II Hard X-ray Nanoprobe Beamline  

SciTech Connect

The hard x-ray nanoprobe (HXN) beamline of the National Synchrotron Light Source II (NSLS-II) requires high levels of stability in order to achieve the desired instrument resolution. To ensure that the design of the endstation helps meet the stringent criteria and that natural and cultural vibration is mitigated both passively and actively, a comprehensive study complimentary to the design process has been undertaken. Vibration sources that have the potential to disrupt sensitive experiments such as wind, traffic, and NSLS II operating systems have been studied using state-of-the-art simulations and an array of field data. Further, final stage vibration isolation principles have been explored.

Simos, N.; Chu, Y. S.; Broadbent, A.; Nazaretski, E.; Margulies, L.; Dyling, O.; Shen, Q.; Fallier, M. [National Synchrotron Light Source II, Brookhaven National Laboratory, Upton, NY 11973 (United States)

2011-09-09T23:59:59.000Z

316

Parallel-beam imaging at the ESRF beamline ID19: current status and plans for the future  

SciTech Connect

The ESRF synchrotron beamline ID19, dedicated to full-field parallel-beam imaging techniques such as phase-contrast and absorption microtomography and X-ray topography, is one of the most versatile instruments of its kind. This paper presents key characteristics of ID19 in its present form, names examples for research and development performed on the beamline, and outlines the plans for an upgrade on the beamline in coming years, to adapt to the growing needs of the user community. The technical goals envisioned include an increase in available beam size and maximum photon energy, and a substantial increase in flux density for applications using beams of small and intermediate size.

Weitkamp, T.; Tafforeau, P.; Boller, E.; Cloetens, P.; Valade, J.-P.; Bernard, P.; Baruchel, J. [European Synchrotron Radiation Facility (ESRF), BP 220, 38043 Grenoble (France); Peyrin, F. [European Synchrotron Radiation Facility (ESRF), BP 220, 38043 Grenoble (France); Creatis / INSA Lyon (France); Ludwig, W. [European Synchrotron Radiation Facility (ESRF), BP 220, 38043 Grenoble (France); INSA Lyon (France); Helfen, L. [European Synchrotron Radiation Facility (ESRF), BP 220, 38043 Grenoble (France); ISS / ANKA Light Source, Forschungszentrum Karlsruhe / KIT, Karlsruhe (Germany)

2010-06-23T23:59:59.000Z

317

X-ray micro-diffraction studies on biological samples at the BioCAT Beamline 18-ID at the Advanced Photon Source  

Science Journals Connector (OSTI)

Advances in synchrotron beamlines bring opportunities with accompanying challenges for the study of soft condensed (biological) matter. This article describes improvements to the BioCAT beamline that include micro-focus, scanning and cryo-cooling of soft connective tissues yielding X-ray data from whole rat-tail tendons to better than 4 ?.

Barrea, R.A.

2014-08-08T23:59:59.000Z

318

Design and characterization of an undulator beamline optimized for small-angle coherent X-ray scattering at the Advanced Photon Source  

Science Journals Connector (OSTI)

The design of an undulator beamline at the Advanced Photon Source optimized for performing coherent small-angle X-ray scattering is described. The beamline has been characterized by measuring and analysing static speckle patterns from isotropically disordered samples. The measured speckle widths and amplitudes are compared with a theory described herein and found to be in good agreement with its predictions.

Sandy, A.R.

1999-11-01T23:59:59.000Z

319

Carbon Cycle  

NLE Websites -- All DOE Office Websites (Extended Search)

Carbon Cycle Carbon Cycle Latest Global Carbon Budget Estimates Including CDIAC Estimates Terrestrial Carbon Management Data Sets and Analyses Carbon Dioxide Emissions from Fossil-Fuel Consumption and Cement Manufacture, (2011) Annual Fossil-Fuel CO2 Emissions: Mass of Emissions Gridded by One Degree Latitude by One Degree Longitude (2012) Monthly Fossil-Fuel CO2 Emissions: Mass of Emissions Gridded by One Degree Latitude by One Degree Longitude (2012) Annual Fossil-Fuel CO2 Emissions: Global Stable Carbon Isotopic Signature (2012) Monthly Fossil-Fuel CO2 Emissions: Isomass (δ 13C) of Emissions Gridded by One Degree Latitude by One Degree Longitude (2012) AmeriFlux - Terrestrial Carbon Dioxide, Water Vapor, and Energy Balance Measurements Estimates of Monthly CO2 Emissions and Associated 13C/12C Values

320

Full-Automatic XAFS Measurement System of the Engineering Science Research II beamline BL14B2 at SPring-8  

SciTech Connect

The Engineering Science Research II beamline BL14B2 at SPring-8 is a hard X-ray bending magnet beamline covering the wide energy range from 3.8 to 72 keV, and has been open to XAFS users since September 2007. The gas distribution and exhaust gas treatment systems have been installed for the in-situ XAFS measurements. Recent improvements in the speed of XAFS measurements have increased the demand for automated measurements. We have developed such a system, in which the adjustment of X-ray optics and the XAFS measurement in transmission mode can be performed automatically.

Honma, Tetsuo; Takagaki, Masashi [Japan Synchrotron Radiation Research Institute, 1-1-1, kouto, Sayo, Hyogo 679-5198 (Japan); Oji, Hiroshi; Hirayama, Sayaka; Taniguchi, Yosuke; Ofuchi, Hironori [Japan Synchrotron Radiation Research Institute, 1-1-1, kouto, Sayo, Hyogo 679-5198 (Japan); SPring-8 Service Co., Ltd., 2-23-1 Kouto, Kamigori, Hyogo 678-1205 (Japan)

2010-06-23T23:59:59.000Z

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


321

Full?Automatic XAFS Measurement System of the Engineering Science Research II beamline BL14B2 at SPring?8  

Science Journals Connector (OSTI)

The Engineering Science Research II beamline BL14B2 at SPring?8 is a hard X?ray bending magnet beamline covering the wide energy range from 3.8 to 72 keV and has been open to XAFS users since September 2007. The gas distribution and exhaust gas treatment systems have been installed for the in?situ XAFS measurements. Recent improvements in the speed of XAFS measurements have increased the demand for automated measurements. We have developed such a system in which the adjustment of X?ray optics and the XAFS measurement in transmission mode can be performed automatically.

Tetsuo Honma; Hiroshi Oji; Sayaka Hirayama; Yosuke Taniguchi; Hironori Ofuchi; Masashi Takagaki

2010-01-01T23:59:59.000Z

322

Application of Goubau Surface Wave Transmission Line for Improved Bench Testing of Diagnostic Beamline Elements  

SciTech Connect

In-air test fixtures for beamline elements typically utilize an X-Y positioning stage, and a wire antenna excited by an RF source. In most cases, the antenna contains a standing wave, and is useful only for coarse alignment measurements in CW mode. A surface-wave (SW) based transmission line permits RF energy to be launched on the wire, travel through the beamline component, and then be absorbed in a load. Since SW transmission lines employ travelling waves, the RF energy can be made to resemble the electron beam, limited only by ohmic losses and dispersion. Although lossy coaxial systems are also a consideration, the diameter of the coax introduces large uncertainties in centroid location. A SW wire is easily constructed out of 200 micron magnet wire, which more accurately approximates the physical profile of the electron beam. Benefits of this test fixture include accurate field mapping, absolute calibration for given beam currents, Z-axis independence, and temporal response measurements of sub-nanosecond pulse structures. Descriptions of the surface wave launching technique, transmission line, and instrumentation are presented, along with measurement data.

John Musson, Keith Cole, Sheldon Rubin

2009-05-01T23:59:59.000Z

323

XRLM Beamlines  

NLE Websites -- All DOE Office Websites (Extended Search)

steel ring Substrate: standard 4" wafer and any dimension not larger than 4.75" Photon BPM A photon BPM is installed in the front end section and provides actual information of...

324

A New Tomography Beamline at a Wiggler Port at the Center for Advanced Microstructures and Devices (CAMD) Storage Ring  

Science Journals Connector (OSTI)

A new tomography beamline has been built and commissioned at the 7 T wiggler of the CAMD storage ring. This beamline is equipped with two monochromators that can be used interchangeably for X?ray absorption spectroscopy or high resolution X?ray tomography at best 23 ?m pixel size. The high?flux double multilayer?mirror monochromator (W?B4C multilayers) can be used in the energy range from 6 to 35 keV with a resolution (?E/E ) between 0.010.03. The second is a channel?cut Si(311)?crystal monochromator with a range of 15 to 36 keV and resolution of ca. 10?4 this is not yet tested. Tomography has the potential for high?throughput materials analysis; however there are some significant obstacles to be overcome in the areas of data acquisition reconstruction visualization and analysis. Data acquisition is facilitated by the multilayer monochromator as this provides high photon flux thus reducing measurement time. At the beamline Matlab routines provide simple x y z fly?throughs of the sample. Off?beamline processing with Amira can yield more sophisticated inspection of the sample. Standard data acquisition based on fixed angle increments is not optimal however new patterns based on Greek golden ratio angle increments offer faster convergence to a high signal?to?noise?ratio image. The image reconstruction has traditionally been done by back?projection reconstruction. In this presentation we will show first results from samples studied at the new beamline.

Kyungmin Ham; Heath A. Barnett; Leslie G. Butler; Clinton S. Willson; Kevin J. Morris; Roland C. Tittsworth; John D. Scott

2007-01-01T23:59:59.000Z

325

ANL/APS/TB-5 Functional Description of APS Beamline Front Ends  

NLE Websites -- All DOE Office Websites (Extended Search)

Functional Description of APS Beamline Front Ends by Tuncer Kuzay February 1993 Advanced Photon Source & Argonne National Laboratory, Argonne, Illinois 60439 o operated by The University of Chicago for the United States Department of Energy under Contract W-31-1 09-Eng-38 Argonne National Laboratory, with facilties in the states of Ilinois and Idaho, is owned by the United States government, and operated by The University of Chicago under the provisions of a contract with the Deparment of Energy. DISCLAIMER This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any waranty, express or implied, or assumes any legal liability or responsibility for the accuracy,

326

HARWI-II, The New High-Energy Beamline for Materials Science at HASYLAB/DESY  

SciTech Connect

The GKSS Forschungszentrum Geesthacht, Germany, will setup a new high-energy beamline specialized for texture, strain and imaging measurements for materials science at the Hamburger Synchrotronstrahlungslabor HASYLAB of the Deutsches Elektronen-Synchrotron DESY. Four different experiments will be installed at the new wiggler HARWI-II. The high pressure cell will be run by the GFZ Potsdam, Germany, the high-energy diffractometer together with a microtomography camera will be run by the GKSS. A further station will allow space for the diffraction enhanced imaging setup. The optics will provide for a small white beam (0.5 mm x 0.5 mm) and a large monochromatic X-ray beam (50 mm x 10 mm) with an energy range of 20 to 250 keV.

Beckmann, Felix; Lippmann, Thomas; Metge, Joachim; Dose, Thomas; Donath, Tilman; Schreyer, Andreas [GKSS Forschungszentrum, Max-Planck-Strasse, 21502 Geesthacht (Germany); Tischer, Markus [HASYLAB at Deutsches Elektronen-Synchrotron DESY, Notkestrasse 85, 22607 Hamburg (Germany); Liss, Klaus Dieter [Technische Universitaet, Hamburg-Harburg, 21071 Hamburg (Germany)

2004-05-12T23:59:59.000Z

327

Advanced photoelectric effect experiment beamline at Elettra: A surface science laboratory coupled with Synchrotron Radiation  

SciTech Connect

We report the main characteristics of the advanced photoelectric effect experiments beamline, operational at Elettra storage ring, featuring a fully independent double branch scheme obtained by the use of chicane undulators and able to keep polarization control in both linear and circular mode. The paper describes the novel technical solutions adopted, namely, (a) the design of a quasiperiodic undulator resulting in optimized suppression of higher harmonics over a large photon energy range (10-100 eV), (b) the thermal stability of optics under high heat load via cryocoolers, and (c) the end station interconnected setup allowing full access to off-beam and on-beam facilities and, at the same time, the integration of users' specialized sample growth chambers or modules.

Panaccione, G.; Vobornik, I.; Fujii, J.; Krizmancic, D.; Annese, E.; Giovanelli, L.; Maccherozzi, F.; Salvador, F.; De Luisa, A.; Benedetti, D.; Gruden, A.; Bertoch, P.; Rossi, G. [TASC Laboratory, INFM-CNR, S.S. 14-Km 163.5 in AREA Science Park, I-34012 Basovizza (Trieste) (Italy); Polack, F. [Synchrotron SOLEIL, B.P. 48, 91192 Gif-sur-Yvette (France); Cocco, D.; Sostero, G.; Diviacco, B. [Sincrotrone Trieste S.C.p.A., S.S. 14 Km 163.5, Area Science Park, 34012 Trieste (Italy); Hochstrasser, M.; Maier, U.; Pescia, D. [Laboratorium fuer Festkoerperphysik, ETH Hoenggerberg, CH-8093 Zuerich (Switzerland); and others

2009-04-15T23:59:59.000Z

328

Characterizations and Applications of the Insertion Device of the SPring-8 Diagnostics Beamline II  

SciTech Connect

An insertion device (ID05) of the SPring-8 diagnostics beamline II (BL05SS) was characterized from the aspects of both the magnetic field performance and the spectral performance as a high K wiggler, which was confirmed to have the field performance with the rms phase error less than 2 degree. Meanwhile, the spectral performance of ID05 as an undulator with small K was also investigated by the energy spectrum measurements. The rms phase error less than 2degree leads us to apply the wiggler radiation on the higher harmonics to the beam diagnostics. We successfully demonstrated an application to the energy-spread diagnostics of electron beam using the 19th harmonics.

Masaki, Mitsuhiro; Takano, Shiro; Tamura, Kazuhiro; Mochihashi, Akira; Oishi, Masaya; Shoji, Masazumi; Fujita, Takahiro; Takashima, Takeo; Ohkuma, Haruo [Japan Synchrotron Radiation Research Institute (JASRI/SPring-8), 1-1-1 Kouto, Sayo, Hyogo (Japan); Yamamoto, Shigeru [High Energy Accelerator Research Organization (KEK)/Institute of Materials Structure Science, 1-1 Oho, Tsukuba, Ibaraki (Japan)

2010-06-23T23:59:59.000Z

329

HARWI?II, The New High?Energy Beamline for Materials Science at HASYLAB/DESY  

Science Journals Connector (OSTI)

The GKSS Forschungszentrum Geesthacht Germany will setup a new high?energy beamline specialized for texture strain and imaging measurements for materials science at the Hamburger Synchrotronstrahlungslabor HASYLAB of the Deutsches Elektronen?Synchrotron DESY. Four different experiments will be installed at the new wiggler HARWI?II. The high pressure cell will be run by the GFZ Potsdam Germany the high?energy diffractometer together with a microtomography camera will be run by the GKSS. A further station will allow space for the diffraction enhanced imaging setup. The optics will provide for a small white beam (0.5 mm 0.5 mm) and a large monochromatic X?ray beam (50 mm 10 mm) with an energy range of 20 to 250 keV.

Felix Beckmann; Thomas Lippmann; Joachim Metge; Thomas Dose; Tilman Donath; Markus Tischer; Klaus Dieter Liss

2004-01-01T23:59:59.000Z

330

Achieving Vibration Stability of the NSLS-II Hard X-ray Nanoprobe Beamline  

SciTech Connect

The Hard X-ray Nanoprobe (HXN) Beamline of National Synchrotron Light Source II (NSLS-lI) requires high levels of stability in order to achieve the desired instrument resolution. To ensure that the design of the endstation helps meet the stringent criteria and that natural and cultural vibration is mitigated both passively and actively, a comprehensive study complimentary to the design process has been undertaken. Vibration sources that have the potential to disrupt sensitive experiments such as wind, traffic and NSLS II operating systems have been studied using state of the art simulations and an array of field data. Further, final stage vibration isolation principles have been explored in order to be utilized in supporting endstation instruments. This paper presents results of the various study aspects and their influence on the HXN design optimization.

Simos, N.; Chu, Y. N.; Broadbent, A.; Nazaretski, E.; Margulies, L.; Dyling, O.; Shen, Q.; Fallier, M.

2010-08-30T23:59:59.000Z

331

Annular Vortex Generation for Inertial Fusion Energy Beam-Line Protection  

SciTech Connect

The use of swirling annular vortex flow inside beam entrance tubes can protect beam-line structural materials in chambers for heavy-ion inertial fusion energy (IFE) applications. An annular wall jet, or vortex tube, is generated by injecting liquid tangent to the inner surface of a tube wall with both axially and azimuthally directed velocity components. A layer of liquid then lines the beam tube wall, which may improve the effectiveness of neutron shielding, and condenses and removes vaporized coolant that may enter the beam tubes. Vortex tubes have been constructed and tested with a thickness of three-tenths the pipe radius. Analysis of the flow is given, along with experimental examples of vortex tube fluid mechanics and an estimate of the layer thickness, based on simple mass conservation considerations.

Pemberton, Steven J.; Abbott, Ryan P.; Peterson, Per F. [University of California (United States)

2003-05-15T23:59:59.000Z

332

X-ray multilayer characterization using reflectivity beamline at Indus-1  

SciTech Connect

Poor knowledge of optical constants of various materials in the soft x-ray region requires to test the soft x-ray optical devices at actual wavelengths. For such purposes a soft x-ray/vacuum ultraviolet reflectivity beamline has been setup on Indus-1 synchrotron.X-ray multilayer structures are also being developed at RRCAT. Silicon based different multilayer optics fabricated in house for 100-200A ring wavelength region show a very high reflectivity performance. A new multilayer combination comprised of NbC/Si is proposed for achieving good thermal stability high reflectivity in the Si L-edge region. A high reflectivity of 63% in near normal incidence region is obtained with a sputter deposited Mo/Si combination. Results prospects of growing NbC/Si multilayer are presented.

Modi, Mohammed H.; Prasad, T. T.; Nayak, M.; Pothana, N.; Jaiswal, A.; Rai, S. K.; Lodha, G. S. [X-ray Optics Section Raja Ramanna Centre for Advanced Technology (RRCAT) Indore 452013 (India)

2010-06-23T23:59:59.000Z

333

The Current Performance of the Wide Range (90-2500 eV) Soft X-ray Beamline at the Australian Synchrotron  

SciTech Connect

The Soft X-ray beamline at the Australian synchrotron has been constructed around a collimated light Plane Grating Monochromator taking light from an Elliptically Polarized Undulator (EPU). The beamline covers a wide photon energy range between 90 to 2500 eV, using two gratings of 250 l/mm and 1200 l/mm. At present the output from the monochromator is directed into one branchline with a dedicated UHV endstation. The measured performance of the beamline in flux and resolution is shown to be very close to that of theoretical calculations.

Cowie, B. C. C.; Tadich, A.; Thomsen, L. [Australian Synchrotron, 800 Blackburn Road, Clayton, Victoria (Australia)

2010-06-23T23:59:59.000Z

334

Commissioning of a Soft X-ray Beamline PF-BL-16A with a Variable-Included-Angle Varied-Line-Spacing Grating Monochromator  

SciTech Connect

The design and commissioning of a new soft X-ray beamline, BL-16A, at the Photon Factory is presented. The beamline consists of a pre-focusing mirror, an entrance slit, a variable-included-angle varied-line-spacing plane grating monochromator, and a post-focusing system as usual, and provides circularly and linearly polarized soft X rays in the energy range 200-1500 eV with an APPLE-II type undulator. The commissioning procedure for the beamline optics is described in detail, especially the check of the focal position for the zero-th order and diffracted X rays.

Amemiya, Kenta; Toyoshima, Akio; Kikuchi, Takashi; Kosuge, Takashi; Nigorikawa, Kazuyuki; Sumii, Ryohei; Ito, Kenji [Institute of Materials Structure Science, High Energy Accelerator Research Organization, 1-1 Oho, Tsukuba, Ibaraki 305-0801 (Japan)

2010-06-23T23:59:59.000Z

335

Innovations in the design of mechanical components for a beamline -- The SRl`95 Workshop 2 summary  

SciTech Connect

The Synchrotron Radiation Instrumentation 1995 Conference (SRI`95) was hosted by the Advanced Photon Source (APS) at Argonne National Laboratory (ANL). Of the many workshops within the conference, the SRI`95 Workshop 2 was ``Innovations in the Design of Mechanical Components of a Beamline``. The workshop was attended well with over 140 registrants. The following topics were discussed. Industry`s perspective on the status and future was provided by Huber Diffrationtechnik, Oxford Instruments, and Kohzu Seiko Ltd. on goniometers/diffractometers, advanced manufacturing technique of high heat load components, such as the APS photon shutter, and the specialties of monochromators provided to the third-generation synchrotrons, respectively. This was followed by a description of the engineering of a dual function monochromator design for water-cooled diamond or cryogenically cooled silicon monochromators by CMC CAT/APS. Another category was the nagging problem of sensitivity of the photon beam position monitors (XBPM) to bending magnet radiation (``BM contamination``) and the undulator magnet gap changes. Problem descriptions and suggested solutions were provided by both the Advanced Light Source (ALS) and the APS. Other innovative ideas were the cooling schemes (enhanced cooling of beamline components using metallic porous meshes including cryo-cooled applications); Glidcop photon shutter design using microchannels at the ALS; and window/filter design, manufacture and operational experiences at CHESS and PETRA/HASYLAB. Additional discussions were held on designing for micromotions and precision in the optical support systems and smart user filter schemes. This is a summary of the presentations at the Workshop. 5 refs., 5 figs.

Kuzay, T.M. [Argonne National Lab., IL (United States); Warwick, T. [Lawrence Berkeley Lab., CA (United States)

1995-12-31T23:59:59.000Z

336

(Research at and operation of the material science x-ray absorption beamline (X-11) at the National Synchrotron Light Source)  

SciTech Connect

This report discusses three projects at the Material Science X-Ray Absorption Beamline. Topics discussed include: XAFS study of some titanium silicon and germanium compounds; initial XAS results of zirconium/silicon reactions; and low angle electron yield detector.

Not Available

1992-01-01T23:59:59.000Z

337

[Research at and operation of the material science x-ray absorption beamline (X-11) at the National Synchrotron Light Source]. Progress report  

SciTech Connect

This report discusses three projects at the Material Science X-Ray Absorption Beamline. Topics discussed include: XAFS study of some titanium silicon and germanium compounds; initial XAS results of zirconium/silicon reactions; and low angle electron yield detector.

Not Available

1992-08-01T23:59:59.000Z

338

An automated system to mount cryo-cooled protein crystals on a synchrotron beamline, using compact sample cassettes and a small-scale robot  

Science Journals Connector (OSTI)

A system, implemented at SSRL, for automatically mounting and dismounting pre-frozen crystals at a synchrotron beamline is described. The system is based on a small industrial robot and compact cylindrical sample cassettes.

Cohen, A.E.

2002-11-13T23:59:59.000Z

339

Previously, DC Magnets located at Neutron-Scattering Beamlines were commercially-manufactured superconducting magnets and limited to 17 T. A  

E-Print Network (OSTI)

Previously, DC Magnets located at Neutron-Scattering Beamlines were commercially, this was the first designed specifically for neutron scattering and the first to include resistive suitable for neutron scattering, diffraction and spectroscopy experiments with the neutron beam passing

Weston, Ken

340

Cycle Track Lessons Learned  

E-Print Network (OSTI)

Cycle Track Lessons Learned #12;Presentation Overview · Bicycling trends · Cycle track lessons learned · What is a "Cycle track"? · Essential design elements of cycle tracks Separation Width Crossing driveways & low-volume streets Signalized intersections #12;Trend in kilometers cycled per year

Bertini, Robert L.

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
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to obtain the most current and comprehensive results.


341

Photovoltaics Life Cycle Analysis  

E-Print Network (OSTI)

Metrics of Life-Cycle Performance Energy Payback Times (EPBT) Greenhouse Gas Emissions (GHG) Toxic Gases #12;6 Life Cycle GHG Emissions ­EuropeLife Cycle GHG Emissions ­Europe Insolation: 1700 kwh/m2-yr 0 10 #12;7 Life Cycle GHG Emissions ­Comparison with Conventional Technologies Life Cycle GHG Emissions

342

The BioCAT undulator beamline 18ID: A facility for biological non-crystalline diffraction and x-ray absorption spectroscopy at the APS  

SciTech Connect

The 18ID undulator beamline of the Biophysics Collaborative Access Team at the Advanced Photon Source, Argonne, IL, USA, is a high-performance instrument designed for, and dedicated to, the study of partially ordered and disordered biological materials using the techniques of small-angle X-ray scattering, fiber diffraction, and X-ray absorption spectroscopy. The beamline and associated instrumentation are described in detail and examples of the representative experimental results are presented.

Fischetti, R.; Stepanov, S.; Rosenbaum, G.; Barrea, R.; Black, E.; Gore, D.; Heurich, R.; Kondrashkina, E.; Kropf, A.J.; Wang, S.; Zhang, K.; Irving, T.C.; Bunker, G.B. (IIT); (Georgia)

2008-07-02T23:59:59.000Z

343

From Protein Structure to Function: Ring Cycle for Dilating and  

NLE Websites -- All DOE Office Websites (Extended Search)

From Protein Structure to Function: Ring Cycle for Dilating and Constricting the Nuclear Pore Print From Protein Structure to Function: Ring Cycle for Dilating and Constricting the Nuclear Pore Print Nuclear pore complexes (NPCs) act as the central gatekeepers for selective transport between the cytoplasm and the nucleus. They allow the exchange of selected proteins and ribonucleoproteins, while preventing the transport of material not meant to cross the nuclear envelope. The NPC transport channel is the largest and most complex transport conduit in the eukaryotic kingdom and it is likely composed of only 3 out of 30 nuclear pore complex proteins (nups). Researchers from the Howard Hughes Medical Institute at the Rockefeller University have determined crystal structures of interacting domains of these centrally located channel nups, Nup54, Nup58, and Nup62, using data collected at ALS Beamline 8.2.1. These structures allowed them to elucidate the molecular mechanism that underlies large-scale diameter changes of NPCs and propose a 'ring cycle' for dilating and constricting NPCs from 10-50 nm. The ring cycle would provide a method to adjust transport activities to cellular demands with a rapid response time.

344

From Protein Structure to Function: Ring Cycle for Dilating and  

NLE Websites -- All DOE Office Websites (Extended Search)

From Protein Structure to From Protein Structure to Function: Ring Cycle for Dilating and Constricting the Nuclear Pore From Protein Structure to Function: Ring Cycle for Dilating and Constricting the Nuclear Pore Print Wednesday, 28 August 2013 00:00 Nuclear pore complexes (NPCs) act as the central gatekeepers for selective transport between the cytoplasm and the nucleus. They allow the exchange of selected proteins and ribonucleoproteins, while preventing the transport of material not meant to cross the nuclear envelope. The NPC transport channel is the largest and most complex transport conduit in the eukaryotic kingdom and it is likely composed of only 3 out of 30 nuclear pore complex proteins (nups). Researchers from the Howard Hughes Medical Institute at the Rockefeller University have determined crystal structures of interacting domains of these centrally located channel nups, Nup54, Nup58, and Nup62, using data collected at ALS Beamline 8.2.1. These structures allowed them to elucidate the molecular mechanism that underlies large-scale diameter changes of NPCs and propose a 'ring cycle' for dilating and constricting NPCs from 10-50 nm. The ring cycle would provide a method to adjust transport activities to cellular demands with a rapid response time.

345

From Protein Structure to Function: Ring Cycle for Dilating and  

NLE Websites -- All DOE Office Websites (Extended Search)

From Protein Structure to Function: Ring Cycle for Dilating and Constricting the Nuclear Pore Print From Protein Structure to Function: Ring Cycle for Dilating and Constricting the Nuclear Pore Print Nuclear pore complexes (NPCs) act as the central gatekeepers for selective transport between the cytoplasm and the nucleus. They allow the exchange of selected proteins and ribonucleoproteins, while preventing the transport of material not meant to cross the nuclear envelope. The NPC transport channel is the largest and most complex transport conduit in the eukaryotic kingdom and it is likely composed of only 3 out of 30 nuclear pore complex proteins (nups). Researchers from the Howard Hughes Medical Institute at the Rockefeller University have determined crystal structures of interacting domains of these centrally located channel nups, Nup54, Nup58, and Nup62, using data collected at ALS Beamline 8.2.1. These structures allowed them to elucidate the molecular mechanism that underlies large-scale diameter changes of NPCs and propose a 'ring cycle' for dilating and constricting NPCs from 10-50 nm. The ring cycle would provide a method to adjust transport activities to cellular demands with a rapid response time.

346

The UHV Experimental Chamber For Optical Measurements (Reflectivity and Absorption) and Angle Resolved Photoemission of the BEAR Beamline at ELETTRA  

SciTech Connect

The experimental station of the BEAR (Bending magnet for Emission, Absorption and Reflectivity) beamline at ELETTRA (Trieste, Italy) is an UHV chamber conceived to fully exploit the spectroscopic possibilities offered by the light spot produced by the beamline. Spectroscopies include reflectivity ({theta}-2{theta} and diffuse), optical absorption, fluorescence and angle resolved photoemission. The chamber can be rotated around the beam axis to select the s (TE) or p (TM) incidence conditions and/or the position of the ellipse of polarization with respect to the sample. Photon detectors (e.g. photodiodes) and electron detector (hemispherical analyzer - 1 deg. angular resolution, 20 meV energy resolution) cover about completely the full 2{pi} solid angle above the sample surface in any light incidence condition.

Pasquali, L.; Nannarone, S. [UdR-INFM Modena, Universita di Modena and Reggio Emilia, Via Vignolese 905, 41100 Modena (Italy); Dipartimento di Ingegneria dei Materiali e dell'Ambiente, Universita di Modena and Reggio Emilia, Via Vignolese 905, 41100 Modena (Italy); De Luisa, A. [TASC-INFM, MM building in Area Science Park, s.s.14 km 163.5, 34012 Basovizza, Trieste (Italy)

2004-05-12T23:59:59.000Z

347

Redesign and Reconstruction of the Equipment Protection Systems for the Upgrading Front Ends and Beamlines at BSRF  

SciTech Connect

The BEPC(Beijing Electron-Positron Collider) is upgraded to be BEPCII, a two-ring Electron-Positron collider. Due to the construction of the BEPCII and upgrade of the existing front ends and beamlines, all the existing EPSs(Equipment Protection Systems) have to be redesigned and reconstructed at BSRF. All the redesigned EPSs for the upgrading front ends and beamlines are a PLC- and SCADA-based equipment protection and control and monitoring system. The EPSs are used to protect BEPCII two storage rings vacuum against vacuum failures in a beamline, as well as to protect the front-end and beamline components from being damaged by synchrotron radiation. For the high-power wiggler beam lines, a fast movable mask is used to protect the blade of a fast-closing valve from damage when the fast-closing valve is triggered to close, which does not need to dump the electron beam running in BEPCII outer ring. In addition, all redesigned PLC- based EPSs are used to communicate with the same centralized monitoring computer to monitor a variety of parameters from all PLC- based EPS systems. The monitoring computer runs the SCADA (Supervisory Control And Data Acquisition) software with its own web server. Graphical HMI interfaces are used to display a few overall views of all front-end equipment operation status and the further detailed information for each EPS in a different pop-up window. On the web services, the SCADA-based centralized monitoring system provides a web browse function, etc. The design of the reconstructed systems is described in this paper.

Xiong Shenshou; Tan Yinglei; Wu Xuehui [Beijing Synchrotron Radiation Laboratory, Institute of High Energy Physics, P. O. Box 918, Branch 2-7, Beijing 100049 (China)

2007-01-19T23:59:59.000Z

348

Long-Working-Distance Kirkpatrick-Baez Mirrors for Hard X-ray Beamlines at SPring-8  

SciTech Connect

We designed and installed two types of long-working-distance Kirkpatrick-Baez (KB) mirrors and mirror manipulators, which were customized into each experiment for hard x-ray undulator beamlines at SPring-8. For the BL32XU RIKEN Targeted Proteins beamline, 400-mm-long KB focusing mirrors for a beam size of 1 {mu}m with a 730-mm-long working distance were designed for carrying out the structural analysis of protein microcrystals. We realized a focusing beam size of 0.9x0.9 {mu}m{sup 2}(FWHM) and a focusing intensity of 6x10{sup 10} (photons/s) at an x-ray energy of 12.4 keV. For the BL19LXU RIKEN SR Physics beamline, we developed KB mirrors for 100-nm focusing with a 100-mm-working distance for the purpose of nano-focus x-ray diffraction. A focusing beam size of 100x100 nm{sup 2}(FWHM) and a high focusing intensity of 3.7x10{sup 10} (photons/s) at an x-ray energy of 12.4 keV were realized.

Yumoto, H.; Koyama, T. [Japan Synchrotron Radiation Research Institute (JASRI)/SPring-8, 1-1-1, Kouto, Sayo-cho, Sayo-gun, Hyogo 679-5198 (Japan); Hirata, K.; Kawano, Y.; Ueno, G.; Nisawa, A.; Hikima, T.; Takeshita, S.; Ito, K.; Tanaka, Y.; Arima, T.; Yamamoto, M. [RIKEN/SPring-8, 1-1-1 Kouto, Sayo-cho, Sayo-gun, Hyogo 679-5148 (Japan); Ohsumi, H.; Ohashi, H.; Goto, S. [Japan Synchrotron Radiation Research Institute (JASRI)/SPring-8, 1-1-1, Kouto, Sayo-cho, Sayo-gun, Hyogo 679-5198 (Japan); RIKEN/SPring-8, 1-1-1 Kouto, Sayo-cho, Sayo-gun, Hyogo 679-5148 (Japan)

2011-09-09T23:59:59.000Z

349

Offshore Rankine Cycles.  

E-Print Network (OSTI)

?? The title of the thesis - "Offshore Rankine Cycles" - is very general and cover a large range of engineering fields, e.g. thermodynamic cycles (more)

Brandsar, Jo

2012-01-01T23:59:59.000Z

350

The Organic Rankine Cycle  

Science Journals Connector (OSTI)

Chap. 3 is dedicated to Rankine cycles with organic fluids: the so-called organic Rankine cycles (ORC), which in recent years have ... of the use of...

Costante Mario Invernizzi

2013-01-01T23:59:59.000Z

351

Optimization of Air Conditioning Cycling  

E-Print Network (OSTI)

Benchmark Long Cycle .............................................................................................. 95 5.46 System Pressures and Temperatures Valve Part Cycle Vs Benchmark Long Cycle...

Seshadri, Swarooph

2012-10-19T23:59:59.000Z

352

Integration of an Atomic Force Microscope in a Beamline Sample Environment  

SciTech Connect

We developed and optimised an optics-free Atomic Force Microscope (AFM) that can be directly installed on most of the synchrotron radiation end-stations. The combination of Scanning Probe Microscopies with X-ray microbeams adds new possibilities to the variety of synchrotron radiation techniques. The instrument can be used for atomic force imaging of the investigated sample or to locally measure the X-ray absorption or diffraction, or it can also be used to mechanically interact with the sample while simultaneously taking spectroscopy or diffraction measurements. The local character of these measurements is intrinsically linked with the use of the Atomic Force Microscope tip. It is the sharpness of the tip that gives the opportunity to measure the photons flux impinging on it giving beam position monitor features, or allows to locally measure the absorption coefficient or the shape of the diffraction pattern. As an example of the possibilities opened by the instrument we will show diffraction measurements performed on a Ge/Si island while being indented with the AFM tip providing local measure of the Young coefficient. Three ESRF beamlines are going to be equipped with this new instrument.

Rodrigues, M. S.; Hrouzek, M.; Dhez, O.; Comin, F. [ESRF, 6 rue Horowitz 38042 Grenoble Cedex (France); Chevrier, J. [Institut Neel-CNRS and Universite Joseph Fourier, 38042 Grenoble (France)

2010-06-23T23:59:59.000Z

353

Combined sampler robot and high-performance liquid chromatography: a fully automated system for biological small-angle X-ray scattering experiments at the Synchrotron SOLEIL SWING beamline  

Science Journals Connector (OSTI)

A prototype was developed to perform online purification and automatic loading of protein solutions at a small-angle X-ray scattering beamline.

David, G.

2009-09-08T23:59:59.000Z

354

Multiple Rankine topping cycles  

SciTech Connect

The efficiency of a Rankine cycle is primarily determined by the temperatures of heat addition and rejection. However, no working fluid has been identified which will operate in a Rankine cycle over an extremely wide temperature range. Multiple Rankine topping cycles offer a technique for achieving high thermal efficiencies in power plants by allowing the use of several working fluids. This paper gives a history of Rankine topping cycles, presents an analysis for the calculation of the overall efficiency of a three-module multiple Rankine cycle, and presents results from a case study for a sodium-mercury-water cycle.

McWhirter, J.D. [Argonne National Lab., Idaho Falls, ID (United States). Engineering Div.]|[Idaho State Univ., Pocatello, ID (United States). Coll. of Engineering

1995-07-01T23:59:59.000Z

355

Optimization of a coherent soft x-ray beamline for coherent scattering experiments at NSLS-II  

SciTech Connect

The coherent soft x-ray and full polarization control (CSX) beamline at the National Synchrotron Light Source - II (NSLS-II) will deliver 1013 coherent photons per second in the energy range of 0.2-2 keV with a resolving power of 2000. The source, a dual elliptically polarizing undulator (EPU), and beamline optics should be optimized to deliver the highest possible coherent flux in a 10-30 {micro}m spot for use in coherent scattering experiments. Using the computer code Synchrotron Radiation Workshop (SRW), we simulate the photon source and focusing optics in order to investigate the conditions which provide the highest usable coherent intensity on the sample. In particular, we find that an intermediate phasing magnet is needed to correct for the relative phase between the two EPUs and that the optimum phase setting produces a spectrum in which the desired wavelength is slightly red-shifted thus requiring a larger aperture than originally anticipated. This setting is distinct from that which produces an on-axis spectrum similar to a single long undulator. Furthermore, partial coherence calculations, utilizing a multiple electron approach, indicate that a high degree of spatial coherence is still obtained at the sample location when such an aperture is used. The aperture size which maximizes the signal-to-noise ratio of a double-slit experiment is explored. This combination of high coherence and intensity is ideally suited for x-ray ptychography experiments which reconstruct the scattering density from micro-diffraction patterns. This technique is briefly reviewed and the effects on the image quality of proximity to the beamline focus are explored.

Shapiro D.; Chubar, O.; Kaznatcheev, K.; Reininger, R.; Sanchez-Hanke, C.; Wang, S.

2011-08-21T23:59:59.000Z

356

Quantifying Carbon Cycle Feedbacks  

Science Journals Connector (OSTI)

Perturbations to the carbon cycle could constitute large feedbacks on future changes in atmospheric CO2 concentration and climate. This paper demonstrates how carbon cycle feedback can be expressed in formally similar ways to climate feedback, ...

J. M. Gregory; C. D. Jones; P. Cadule; P. Friedlingstein

2009-10-01T23:59:59.000Z

357

Edgeworth cycles revisited  

E-Print Network (OSTI)

Some gasoline markets exhibit remarkable price cycles, where price spikes are followed by a series of small price declines: a pattern consistent with a model of Edgeworth cycles described by Maskin and Tirole. We extend ...

Doyle, Joseph J.

358

The combined cycle  

Science Journals Connector (OSTI)

Any combination of at least two cyclic processes converting thermal energy (heat) to work forms a combined cycle. In principle, the potential number of ... number of options reduces to a variety of cycles consi...

R. U. Pitt

1995-01-01T23:59:59.000Z

359

Water Cycle Pilot Study  

NLE Websites -- All DOE Office Websites (Extended Search)

1 Water Cycle Pilot Study To learn more about Earth's water cycle, the U.S. Department of Energy (DOE) has established a multi-laboratory science team representing five DOE...

360

mathematics single cycle  

E-Print Network (OSTI)

47 mathematics education single cycle master's study programme #12;48 single cycle master's study program in Mathematics Education #12;49 single cycle master's study program in Mathematics Education MATHEMATICS EDUCATION The program is in tune with the principles of the Bologna Declaration. · Academic title

?umer, Slobodan

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


361

Cycle to Cycle Manufacturing Process Control  

E-Print Network (OSTI)

Most manufacturing processes produce parts that can only be correctly measured after the process cycle has been completed. Even if in-process measurement and control is possible, it is often too expensive or complex to ...

Hardt, David E.

362

T-R Cycle Characterization and Imaging: Advanced Diagnostic Methodology for Petroleum Reservoir and Trap Detection and Delineation  

SciTech Connect

The principal research effort for Year 2 of the project is on stratigraphic model assessment and development. The research focus for the first six (6) months of Year 2 is on T-R cycle model development. The emphasis for the remainder of the year is on assessing the depositional model and developing and testing a sequence stratigraphy model. The development and testing of the sequence stratigraphy model has been accomplished through integrated outcrop, well log and seismic studies of Mesozoic strata in the Gulf of Mexico, North Atlantic and Rocky Mountain areas.

Ernest A. Mancini; William C. Parcell; Bruce S. Hart

2005-09-19T23:59:59.000Z

363

Set-up of an XAFS beamline for measurements between 2.4-8 keV at DORIS III  

SciTech Connect

In this paper results from the commissioning phase and from first user experiments of a new EXAFS beamline at the DORIS III storage ring are presented. The bending magnet EXAFS beamline A1 underwent a complete rebuild and now covers the energy range 2.4-8 keV. A Ni-coated toroidal mirror, placed in a 2:1 focusing position and a plane mirror with one Ni coated stripe and one uncoated (SiO{sub 2}) stripe are used for effective higher harmonics suppression and focusing. The UHV-compatible fixed-exit Double Crystal Monochromator (DCM) is equipped with two Si(111) crystal pairs. The second crystal of one of the two crystal pairs is tilted by 90 deg. around the surface normal to shift the position of glitches. It allows Bragg angles between 5 deg. and 55.5 deg. and continuous scans in quick-EXAFS mode. Test measurements during the commissioning phase proved the excellent performance of the monochromator and a high quality of the XAFS spectra over the entire working range.

Welter, Edmund [Deutsches Elektronen-Synchrotron A Research Centre of the Helmholtz Association, Notkestrasse 85, D-22607 Hamburg (Germany)

2010-06-23T23:59:59.000Z

364

Experimental results with cryogenically cooled, thin, silicon crystal x-ray monochromators on high-heat-flux beamlines  

SciTech Connect

A novel, silicon crystal monochromator has been designed and tested for use on undulator and focused wiggler beamlines at third-generation synchrotron sources. The crystal utilizes a thin, partially transmitting diffracting element fabricated within a liquid-nitrogen cooled, monolithic block of silicon. This report summarizes the results from performance tests conducted at the European Synchrotron Radiation Facility (ESRF) using a focused wiggler beam and at the Advanced Photon Source (APS) on an undulator beamline. These experiments indicate that a cryogenic crystal can handle the very high power and power density x-ray beams of modem synchrotrons with sub-arcsec thermal broadening of the rocking curve. The peak power density absorbed on the surface of the crystal at the ESRF exceeded go W/mm{sup 2} with an absorbed power of 166 W, this takes into account the spreading of the beam due to the Bragg angle of 11.4{degrees}. At the APS, the peak heat flux incident on the crystal was 1.5 W/mA/mm{sup 2} with a power of 6.1 W/mA for a 2.0 H x 2.5 V mm{sup 2} beam at an undulator gap of 11.1 mm and stored current up to 96 mA.

Rogers, C.S.; Mills, D.M.; Lee, W.K.; Fernandez, P.B.; Graber, T.

1996-08-01T23:59:59.000Z

365

ANL/APS/TB-44, Guidelines for Beamline and Front-End Radiation Shielding Design at the Advanced Photon Source  

NLE Websites -- All DOE Office Websites (Extended Search)

APS/TB-44 Rev. 4 APS/TB-44 Rev. 4 Guidelines for Beamline and Front-End Radiation Shielding Design at the Advanced Photon Source Revision 4 Advanced Photon Source About Argonne National Laboratory Argonne is a U.S. Department of Energy laboratory managed by UChicago Argonne, LLC under contract DE-AC02-06CH11357. The Laboratory's main facility is outside Chicago, at 9700 South Cass Avenue, Argonne, Illinois 60439. For information about Argonne and its pioneering science and technology programs, see www.anl.gov. Availability of This Report This report is available, at no cost, at http://www.osti.gov/bridge. It is also available on paper to the U.S. Department of Energy and its contractors, for a processing fee, from: U.S. Department of Energy Office of Scientific and Technical Information

366

ANL/APS/TB-54, Dose Calculations using MARS for Bremsstrahlung Beam Stops and Collimators in APS Beamline Stations  

NLE Websites -- All DOE Office Websites (Extended Search)

4 4 DOSE CALCULATIONS USING MARS FOR BREMSSTRAHLUNG BEAM STOPS AND COLLIMATORS IN APS BEAMLINE STATIONS Jeffrey C. Dooling Accelerator Systems Division Advanced Photon Source August 2010 This work is sponsored by the US Department of Energy Office of Science The submitted manuscript has been created by UChicago Argonne, LLC, Operator of Argonne National Laboratory ("Argonne"). Argonne, a U.S. Department of Energy Office of Science laboratory, is operated under Contract No. DE-AC02-06CH11357. The U.S. Government retains for itself, and others acting on its behalf, a paid-up nonexclusive, irrevocable worldwide license in said article to reproduce, prepare derivative works, distribute copies to the public, and perform publicly and display

367

Higher Order Suppressor (HOS) for the PolLux Microspectroscope Beamline at the Swiss Light Source SLS  

SciTech Connect

The mechanical design and performance of a device to suppress higher orders of a spherical grating monochromator at a constant deviation angle is described. The higher order suppressor (HOS) is used for a scanning transmission x-ray microspectroscope beamline (PolLux) at a bending magnet of the Swiss Light Source (SLS). The instruments allow microspectroscopy in polymer science, of biological samples in the water window as well as the study of magnetic materials with circular or linear polarized light in a photon energy range of 200 eV to 1400 eV. The HOS uses three mirrors acting as a low pass filter for soft x-rays to improve the absorption spectroscopy of carbon, oxygen and nitrogen 1s core levels. The successful installation and operation of the HOS located after the monochromator is reported. First results obtained using samples from materials research and environmental sciences exemplify the improved spectroscopy capabilities of the instrument.

Frommherz, U.; Stefani, R.; Ellenberger, U. [Paul Scherrer Institut, Division of Mechanical Engineering Sciences, 5232 Villigen PSI (Switzerland); Raabe, J.; Watts, B. [Paul Scherrer Institut, Swiss Light Source, 5232 Villigen PSI (Switzerland)

2010-06-23T23:59:59.000Z

368

Power Plant Cycling Costs  

SciTech Connect

This report provides a detailed review of the most up to date data available on power plant cycling costs. The primary objective of this report is to increase awareness of power plant cycling cost, the use of these costs in renewable integration studies and to stimulate debate between policymakers, system dispatchers, plant personnel and power utilities.

Kumar, N.; Besuner, P.; Lefton, S.; Agan, D.; Hilleman, D.

2012-07-01T23:59:59.000Z

369

Life Cycle Cost Estimate  

Directives, Delegations, and Requirements

Life-cycle costs (LCCs) are all the anticipated costs associated with a project or program alternative throughout its life. This includes costs from pre-operations through operations or to the end of the alternative.This chapter discusses life cycle costs and the role they play in planning.

1997-03-28T23:59:59.000Z

370

The Carbon Cycle  

NLE Websites -- All DOE Office Websites (Extended Search)

The Carbon Cycle The Carbon Cycle The global carbon cycle involves the carbon in and exchanging between the earth's atmosphere, fossil fuels, the oceans, and the vegetation and soils of the earth's terrestrial ecosystems. image Each year, the world's terrestrial ecosystems withdraw carbon from the atmosphere through photosynthesis and add it again through respiration and decay. A more detailed look at the global carbon cycle for the 1990s is shown below. The main annual fluxes in GtC yr-1 are: pre-industrial "natural" fluxes in black and "anthropogenic" fluxes in red (modified from Sarmiento and Gruber, 2006, with changes in pool sizes from Sabine et al., 2004a). The net terrestrial loss of -39 GtC is inferred from cumulative fossil fuel emissions minus atmospheric increase minus ocean storage. The loss of

371

Wetland (peat) Carbon Cycle  

NLE Websites -- All DOE Office Websites (Extended Search)

Wetland (peat) Carbon Cycle Methane (CH4) is an important greenhouse gas, twenty times more potent than CO2, but atmospheric concentrations of CH4 under future climate change are...

372

IFR fuel cycle  

SciTech Connect

The next major milestone of the IFR program is engineering-scale demonstration of the pyroprocess fuel cycle. The EBR-II Fuel Cycle Facility has just entered a startup phase, which includes completion of facility modifications and installation and cold checkout of process equipment. This paper reviews the development of the electrorefining pyroprocess, the design and construction of the facility for the hot demonstration, the design and fabrication of the equipment, and the schedule and initial plan for its operation.

Battles, J.E.; Miller, W.E. [Argonne National Lab., IL (United States); Lineberry, M.J.; Phipps, R.D. [Argonne National Lab., Idaho Falls, ID (United States)

1992-04-01T23:59:59.000Z

373

Malone cycle refrigerator development  

SciTech Connect

This paper describes the progress made in demonstrating a Malone Cycle Refrigerator/Freezer. The Malone cycle is similar to the Stirling cycle but uses a supercritical fluid in place of real gas. In the approach, solid-metal diaphragms are used to seal and sweep the working volumes against the high working fluid pressures required in Malone cycle machines. This feature eliminates the friction and leakage that accounted for nearly half the losses in the best piston-defined Malone cycle machines built to date. The authors successfully built a Malone cycle refrigerator that: (1) used CO{sub 2} as the working fluid, (2) operated at pressures up to 19.3 Mpa (2,800 psi), (3) achieved a cold end metal temperatures of {minus}29 C ({minus}20 F), and (4) produced over 400 Watts of cooling at near ambient temperatures. The critical diaphragm components operated flawlessly throughout characterization and performance testing, supporting the conclusion of high reliability based on analysis of fatigue date and actual strain measurements.

Shimko, M.A.; Crowley, C.J.

1999-07-01T23:59:59.000Z

374

Photodiode-Based X-Ray Beam-Position Monitor With High Spatial-Resolution for the NSLS-II Beamlines  

SciTech Connect

We developed a photodiode-based monochromatic X-ray beam-position monitor (X-BPM) with high spatial resolution for the project beamlines of the NSLS-II. A ring array of 32 Si PIN-junction photodiodes were designed for use as a position sensor, and a low-noise HERMES4 ASIC chip was integrated into the electronic readout system. A series of precision measurements to characterize electrically the Si-photodiode sensor and the ASIC chip demonstrated that the inherent noise is sufficiently below tolerance levels. Following up modeling of detector's performance, including geometrical optimization using a Gaussian beam, we fabricated and assembled a first prototype. In this paper, we describe the development of this new state-of-the-art X-ray BPM along the beamline, in particular, downstream from the monochromator.

Yoon, P.S.; Siddons, D. P.

2009-05-25T23:59:59.000Z

375

A highly modular beamline electrostatic levitation facility, optimized for in situ high-energy x-ray scattering studies of equilibrium and supercooled liquids  

SciTech Connect

High-energy x-ray diffraction studies of metallic liquids provide valuable information about structural evolution on the atomic length scale, leading to insights into the origin of the nucleation barrier and the processes of supercooling and glass formation. The containerless processing of the beamline electrostatic levitation (BESL) facility allows coordinated thermophysical and structural studies of equilibrium and supercooled liquids to be made in a contamination-free, high-vacuum ({approx}10{sup -8} Torr) environment. To date, the incorporation of electrostatic levitation facilities into synchrotron beamlines has been difficult due to the large footprint of the apparatus and the difficulties associated with its transportation and implementation. Here, we describe a modular levitation facility that is optimized for diffraction studies of high-temperature liquids at high-energy synchrotron beamlines. The modular approach used in the apparatus design allows it to be easily transported and quickly setup. Unlike most previous electrostatic levitation facilities, BESL can be operated by a single user instead of a user team.

Mauro, N.A.; Kelton, K.F. (WU)

2011-10-27T23:59:59.000Z

376

High energy resolution five-crystal spectrometer for high quality fluorescence and absorption measurements on an x-ray absorption spectroscopy beamline  

SciTech Connect

Fluorescence detection is classically achieved with a solid state detector (SSD) on x-ray absorption spectroscopy (XAS) beamlines. This kind of detection however presents some limitations related to the limited energy resolution and saturation. Crystal analyzer spectrometers (CAS) based on a Johann-type geometry have been developed to overcome these limitations. We have tested and installed such a system on the BM30B/CRG-FAME XAS beamline at the ESRF dedicated to the structural investigation of very dilute systems in environmental, material and biological sciences. The spectrometer has been designed to be a mobile device for easy integration in multi-purpose hard x-ray synchrotron beamlines or even with a laboratory x-ray source. The CAS allows to collect x-ray photons from a large solid angle with five spherically bent crystals. It will cover a large energy range allowing to probe fluorescence lines characteristic of all the elements from Ca (Z = 20) to U (Z = 92). It provides an energy resolution of 1-2 eV. XAS spectroscopy is the main application of this device even if other spectroscopic techniques (RIXS, XES, XRS, etc.) can be also achieved with it. The performances of the CAS are illustrated by two experiments that are difficult or impossible to perform with SSD and the complementarity of the CAS vs SSD detectors is discussed.

Llorens, Isabelle [CEA/DSM/INAC/SP2M/NRS, F-38054 Grenoble cedex 9 (France); Synchrotron SOLEIL - MARS beamline, L'Orme des Merisiers, F-91192 Gif sur Yvette (France); Lahera, Eric; Delnet, William; Proux, Olivier [Observatoire des Sciences de l'Univers de Grenoble, UMS 832 CNRS Universite Joseph Fourier, F-38041 Grenoble cedex 9 (France); BM30B/FAME beamline, ESRF, F-38043 Grenoble cedex 9 (France); Braillard, Aurelien; Hazemann, Jean-Louis; Prat, Alain; Testemale, Denis [BM30B/FAME beamline, ESRF, F-38043 Grenoble cedex 9 (France); Institut Neel, UPR 2940 CNRS, F-38042 Grenoble cedex 9 (France); Dermigny, Quentin; Gelebart, Frederic; Morand, Marc; Shukla, Abhay [Institut de Mineralogie et de Physique des Milieux Condenses, UMR 7590, 4 place Jussieu, F-75005 Paris (France); Bardou, Nathalie [Laboratoire de Photonique et de Nanostructures, UPR 20 CNRS, Route de Nozay, F-91460 Marcoussis (France); Ulrich, Olivier [CEA/DSM/INAC/SP2M/NRS, F-38054 Grenoble cedex 9 (France); BM32/IF beamline, ESRF, F-38043 Grenoble cedex 9 (France); Arnaud, Stephan; Berar, Jean-Francois; Boudet, Nathalie; Caillot, Bernard [Institut Neel, UPR 2940 CNRS, F-38042 Grenoble cedex 9 (France); BM02/D2AM beamline, ESRF, F-38043 Grenoble cedex 9 (France); Chaurand, Perrine; Rose, Jerome [Centre Europeen de Recherche et d'Enseignement des Geosciences de l'Environnement, UMR 7730, F-13545 Aix en Provence (France); and others

2012-06-15T23:59:59.000Z

377

Helium process cycle  

DOE Patents (OSTI)

A unique process cycle and apparatus design separates the consumer (cryogenic) load return flow from most of the recycle return flow of a refrigerator and/or liquefier process cycle. The refrigerator and/or liquefier process recycle return flow is recompressed by a multi-stage compressor set and the consumer load return flow is recompressed by an independent consumer load compressor set that maintains a desirable constant suction pressure using a consumer load bypass control valve and the consumer load return pressure control valve that controls the consumer load compressor's suction pressure. The discharge pressure of this consumer load compressor is thereby allowed to float at the intermediate pressure in between the first and second stage recycle compressor sets. Utilizing the unique gas management valve regulation, the unique process cycle and apparatus design in which the consumer load return flow is separate from the recycle return flow, the pressure ratios of each recycle compressor stage and all main pressures associated with the recycle return flow are allowed to vary naturally, thus providing a naturally regulated and balanced floating pressure process cycle that maintains optimal efficiency at design and off-design process cycle capacity and conditions automatically.

Ganni, Venkatarao (Yorktown, VA)

2008-08-12T23:59:59.000Z

378

Helium process cycle  

DOE Patents (OSTI)

A unique process cycle and apparatus design separates the consumer (cryogenic) load return flow from most of the recycle return flow of a refrigerator and/or liquefier process cycle. The refrigerator and/or liquefier process recycle return flow is recompressed by a multi-stage compressor set and the consumer load return flow is recompressed by an independent consumer load compressor set that maintains a desirable constant suction pressure using a consumer load bypass control valve and the consumer load return pressure control valve that controls the consumer load compressor's suction pressure. The discharge pressure of this consumer load compressor is thereby allowed to float at the intermediate pressure in between the first and second stage recycle compressor sets. Utilizing the unique gas management valve regulation, the unique process cycle and apparatus design in which the consumer load return flow is separate from the recycle return flow, the pressure ratios of each recycle compressor stage and all main pressures associated with the recycle return flow are allowed to vary naturally, thus providing a naturally regulated and balanced floating pressure process cycle that maintains optimal efficiency at design and off-design process cycle capacity and conditions automatically.

Ganni, Venkatarao (Yorktown, VA)

2007-10-09T23:59:59.000Z

379

Power Plant Cycling Costs  

NLE Websites -- All DOE Office Websites (Extended Search)

Power Plant Cycling Costs Power Plant Cycling Costs April 2012 N. Kumar, P. Besuner, S. Lefton, D. Agan, and D. Hilleman Intertek APTECH Sunnyvale, California NREL Technical Monitor: Debra Lew Subcontract Report NREL/SR-5500-55433 July 2012 NREL is a national laboratory of the U.S. Department of Energy, Office of Energy Efficiency & Renewable Energy, operated by the Alliance for Sustainable Energy, LLC. National Renewable Energy Laboratory 15013 Denver West Parkway Golden, Colorado 80401 303-275-3000 * www.nrel.gov Contract No. DE-AC36-08GO28308 Power Plant Cycling Costs April 2012 N. Kumar, P. Besuner, S. Lefton, D. Agan, and D. Hilleman Intertek APTECH Sunnyvale, California NREL Technical Monitor: Debra Lew Prepared under Subcontract No. NFT-1-11325-01

380

AR-NE3A, a New Macromolecular Crystallography Beamline for Pharmaceutical Applications at the Photon Factory  

SciTech Connect

Recent advances in high-throughput techniques for macromolecular crystallography have highlighted the importance of structure-based drug design (SBDD), and the demand for synchrotron use by pharmaceutical researchers has increased. Thus, in collaboration with Astellas Pharma Inc., we have constructed a new high-throughput macromolecular crystallography beamline, AR-NE3A, which is dedicated to SBDD. At AR-NE3A, a photon flux up to three times higher than those at existing high-throughput beams at the Photon Factory, AR-NW12A and BL-5A, can be realized at the same sample positions. Installed in the experimental hutch are a high-precision diffractometer, fast-readout, high-gain CCD detector, and sample exchange robot capable of handling more than two hundred cryo-cooled samples stored in a Dewar. To facilitate high-throughput data collection required for pharmaceutical research, fully automated data collection and processing systems have been developed. Thus, sample exchange, centering, data collection, and data processing are automatically carried out based on the user's pre-defined schedule. Although Astellas Pharma Inc. has a priority access to AR-NE3A, the remaining beam time is allocated to general academic and other industrial users.

Yamada, Yusuke; Hiraki, Masahiko; Sasajima, Kumiko; Matsugaki, Naohiro; Igarashi, Noriyuki; Kikuchi, Takashi; Mori, Takeharu; Toyoshima, Akio; Kishimoto, Shunji; Wakatsuki, Soichi [Photon Factory, Institute of Materials Structure Science, High Energy Accelerator Research Organization, 1-1 Oho, Tsukuba, Ibaraki, 305-0801 (Japan); Amano, Yasushi; Warizaya, Masaichi; Sakashita, Hitoshi [Drug Discovery Research, Astellas Pharma Inc., 21, Miyukigaoka, Tukuba, Ibaraki, 300-8585 (Japan)

2010-06-23T23:59:59.000Z

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


381

mathematical Study program cycle  

E-Print Network (OSTI)

TSW ECTS TSW Fundamentals of statistics 2 2 0 5 150 0 0 0 0 0 5 150 Probability 4 3 0 10 300 0 0 0 0 0127 mathematical statistics Master's study programms #12;128 #12;· Study program cycle: Second Statistics. In Slovenian: magister matematicne statistike (masculine), magistrica matematicne statistike

?umer, Slobodan

382

CLASS DESCRIPTIONS CYCLING SERIES  

E-Print Network (OSTI)

will utilize concepts from the 50-minute cycling class while going the distance to optimal health. Whether you're an avid cyclist, triathlete, or desire a longer class for a greater challenge, join us for this 75-minute AN URBANATHLETE Are you registered to compete in an adventure race like the Men's Health Urbanathlon, Warrior Dash

Pittendrigh, Barry

383

D-Cycle - 4-Differential -Stroke Cycle | Department of Energy  

Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

-Stroke Cycle The D-Cycle offers the opportunity to use less fuel and gain more power while being able to be retrofit to an OEM and aftermarket engines deer09conti.pdf...

384

BNL | Carbon Cycle Science  

NLE Websites -- All DOE Office Websites (Extended Search)

The Carbon Cycle Science & Technology Group aims to increase understanding The Carbon Cycle Science & Technology Group aims to increase understanding of the impacts of global change on managed and unmanaged ecosystems and improve knowledge of possible global change mitigation approaches. The group has three main focus areas. FACE Climate Change Experimental Facility Design and Management The CCS&T group is an internationally recognized leader in the development of Free Air CO2 Enrichment (FACE) research facilities. We are interested in the design and management of manipulative experiments that examine the effects of carbon dioxide, ozone, other atmospheric pollutants, temperature and precipitation on natural and managed ecosystems. FACE Plant Physiology and High Throughput Biochemical Phenotyping At FACE facilities we have studied the mechanisms that underlie the

385

Fuel Cycle Subcommittee  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Report to NEAC Report to NEAC Fuel Cycle Subcommittee Meeting of April 23, 2013 Washington D.C. June 13, 2013 Burton Richter (Chair), Margaret Chu, Darleane Hoffman, Raymond Juzaitis, Sekazi K Mtingwa, Ronald P Omberg, Joy L Rempe, Dominique Warin 2 I Introduction and Summary The Fuel Cycle Subcommittee of NEAC met in Washington on April 23, 2013. The meeting focused on issues relating to the NE advanced reactor program (sections II, III, and IV), and on storage and transportation issues (section V) related to a possible interim storage program that is the first step in moving toward a new permanent repository as recommended by the Blue Ribbon Commission (BRC) and discussed in the recent response by DOE to Congress on the BRC report 1 . The agenda is given in

386

CANDU fuel cycle flexibility  

SciTech Connect

High neutron economy, on-power refuelling, and a simple bundle design provide a high degree of flexibility that enables CANDU (CANada Deuterium Uranium; registered trademark) reactors to be fuelled with a wide variety of fuel types. Near-term applications include the use of slightly enriched uranium (SEU), and recovered uranium (RU) from reprocessed spent Light Water Reactor (LWR) fuel. Plutonium and other actinides arising from various sources, including spent LWR fuel, can be accommodated, and weapons-origin plutonium could be destroyed by burning in CANDU. In the DUPIC fuel cycle, a dry processing method would convert spent Pressurized Water Reactor (PWR) fuel to CANDU fuel. The thorium cycle remains of strategic interest in CANDU to ensure long-term resource availability, and would be of specific interest to those countries possessing large thorium reserves, but limited uranium resources.

Torgerson, D.F.; Boczar, P.G. [Chalk River Lab., Ontario (Canada); Dastur, A.R. [AECL CANDU, Mississauga, Ontario (Canada)

1994-12-31T23:59:59.000Z

387

USCEA fuel cycle '93  

SciTech Connect

The US Council for Energy Awareness sponsored the Fuel Cycle '93 conference in Dallas, Texas, on March 21-24, 1993. Over 250 participants attended, numerous papers were presented, and several panel discussions were held. The focus of most industry participants remains the formation of USEC and the pending US-Russian HEU agreement. Following are brief summaries of two key papers and the Fuel Market Issues panel discussion.

Not Available

1993-04-01T23:59:59.000Z

388

American business cycles and innovation  

E-Print Network (OSTI)

introduces the concepts of innovation and invention. The second section discusses the business cycles and highlights general causes of business cycles. The final section details the history of the iron, steel, aluminum, and pharmaceutical industries...

Hood, Michael

2013-02-22T23:59:59.000Z

389

Edinburgh Research Explorer Money Cycles  

E-Print Network (OSTI)

Edinburgh Research Explorer Money Cycles Citation for published version: Clausen, A & Strub, C 2014 'Money Cycles' Edinburgh School of Economics Discussion Paper Series. Link: Link to publication record date: 11. Dec. 2014 #12;Edinburgh School of Economics Discussion Paper Series Number 249 Money Cycles

Millar, Andrew J.

390

HEURISTIC SEARCH FOR HAMILTON CYCLES  

E-Print Network (OSTI)

by combining it with the remaining cycles. The following is the description of the main part of the algorithmHEURISTIC SEARCH FOR HAMILTON CYCLES IN CUBIC GRAPHS Janez ALES, Bojan MOHAR and Tomaz PISANSKI. A successful heuristic algorithm for nding Hamilton cycles in cubic graphs is described. Several graphs from

Mohar, Bojan

391

MULTIPARAMETER OPTIMIZATION STUDIES ON GEOTHERMAL ENERGY CYCLES  

E-Print Network (OSTI)

of Practical Cycles for Geothermal Power Plants." GeneralDesign and Optimize Geothermal Power Cycles." Presented atof Practical Cycles for Geothermal Power Plants." General

Pope, W.L.

2011-01-01T23:59:59.000Z

392

THE TRANSPOSED CRITICAL TEMPERATURE RANKINE THERMODYNAMIC CYCLE  

E-Print Network (OSTI)

Process Program for Geothermal Power Plant Cycles,'*for a Rankine Cycle Geothermal Power Plant," Proceedings,Design and Optimize Geothermal Power Cycles," presented at

Pope, William L.

2012-01-01T23:59:59.000Z

393

n-step cycle inequalities - Optimization Online  

E-Print Network (OSTI)

also introduced the so-called cycle inequalities (called 1-step cycle inequalities in this ...... combination of the cycle detection strategy of Tarjan [16] and the...

2014-07-02T23:59:59.000Z

394

Life-cycle Assessment of Semiconductors  

E-Print Network (OSTI)

life-cycle energy requirements (e total ) and global warmingtotal life-cycle global warming impacts. Chapter 3 Life-cycle Energy and Global

Boyd, Sarah B.

2009-01-01T23:59:59.000Z

395

Quantum thermodynamic cooling cycle  

E-Print Network (OSTI)

The quantum-mechanical and thermodynamic properties of a 3-level molecular cooling cycle are derived. An inadequacy of earlier models is rectified in accounting for the spontaneous emission and absorption associated with the coupling to the coherent driving field via an environmental reservoir. This additional coupling need not be dissipative, and can provide a thermal driving force - the quantum analog of classical absorption chillers. The dependence of the maximum attainable cooling rate on temperature, at ultra-low temperatures, is determined and shown to respect the recently-established fundamental bound based on the second and third laws of thermodynamics.

Palao, J P; Gordon, J M; Palao, Jose P.; Kosloff, Ronnie; Gordon, Jeffrey M.

2001-01-01T23:59:59.000Z

396

Quantum thermodynamic cooling cycle  

E-Print Network (OSTI)

The quantum-mechanical and thermodynamic properties of a 3-level molecular cooling cycle are derived. An inadequacy of earlier models is rectified in accounting for the spontaneous emission and absorption associated with the coupling to the coherent driving field via an environmental reservoir. This additional coupling need not be dissipative, and can provide a thermal driving force - the quantum analog of classical absorption chillers. The dependence of the maximum attainable cooling rate on temperature, at ultra-low temperatures, is determined and shown to respect the recently-established fundamental bound based on the second and third laws of thermodynamics.

Jose P. Palao; Ronnie Kosloff; Jeffrey M. Gordon

2001-06-08T23:59:59.000Z

397

Geothermal Life Cycle Calculator  

SciTech Connect

This calculator is a handy tool for interested parties to estimate two key life cycle metrics, fossil energy consumption (Etot) and greenhouse gas emission (ghgtot) ratios, for geothermal electric power production. It is based solely on data developed by Argonne National Laboratory for DOEs Geothermal Technologies office. The calculator permits the user to explore the impact of a range of key geothermal power production parameters, including plant capacity, lifetime, capacity factor, geothermal technology, well numbers and depths, field exploration, and others on the two metrics just mentioned. Estimates of variations in the results are also available to the user.

Sullivan, John

2014-03-11T23:59:59.000Z

398

Open cycle thermoacoustics  

SciTech Connect

A new type of thermodynamic device combining a thermodynamic cycle with the externally applied steady flow of an open thermodynamic process is discussed and experimentally demonstrated. The gas flowing through this device can be heated or cooled in a series of semi-open cyclic steps. The combination of open and cyclic flows makes possible the elimination of some or all of the heat exchangers (with their associated irreversibility). Heat is directly exchanged with the process fluid as it flows through the device when operating as a refrigerator, producing a staging effect that tends to increase First Law thermodynamic efficiency. An open-flow thermoacoustic refrigerator was built to demonstrate this concept. Several approaches are presented that describe the physical characteristics of this device. Tests have been conducted on this refrigerator with good agreement with a proposed theory.

Reid, Robert Stowers

2000-01-01T23:59:59.000Z

399

Advanced regenerative absorption refrigeration cycles  

DOE Patents (OSTI)

Multi-effect regenerative absorption cycles which provide a high coefficient of performance (COP) at relatively high input temperatures. An absorber-coupled double-effect regenerative cycle (ADR cycle) (10) is provided having a single-effect absorption cycle (SEA cycle) (11) as a topping subcycle and a single-effect regenerative absorption cycle (1R cycle) (12) as a bottoming subcycle. The SEA cycle (11) includes a boiler (13), a condenser (21), an expansion device (28), an evaporator (31), and an absorber (40), all operatively connected together. The 1R cycle (12) includes a multistage boiler (48), a multi-stage resorber (51), a multisection regenerator (49) and also uses the condenser (21), expansion device (28) and evaporator (31) of the SEA topping subcycle (11), all operatively connected together. External heat is applied to the SEA boiler (13) for operation up to about 500 degrees F., with most of the high pressure vapor going to the condenser (21) and evaporator (31) being generated by the regenerator (49). The substantially adiabatic and isothermal functioning of the SER subcycle (12) provides a high COP. For higher input temperatures of up to 700 degrees F., another SEA cycle (111) is used as a topping subcycle, with the absorber (140) of the topping subcycle being heat coupled to the boiler (13) of an ADR cycle (10). The 1R cycle (12) itself is an improvement in that all resorber stages (50b-f) have a portion of their output pumped to boiling conduits (71a-f) through the regenerator (49), which conduits are connected to and at the same pressure as the highest pressure stage (48a) of the 1R multistage boiler (48).

Dao, Kim (14 Nace Ave., Piedmont, CA 94611)

1990-01-01T23:59:59.000Z

400

Carbon Cycle 2.0  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Carbon Cycle 2.0 Carbon Cycle 2.0 Pioneering science for sustainable energy solutions Artificial Photosynthesis Energy Storage Combustion Carbon Capture & Storage Developing World Efficiency Photovoltaics Biofuels Energy Analysis Climate Modeling Carbon Cycle 2.0 is... 1. A vision for * a global energy system integrated with the Earth's natural carbon cycles * an interactive Berkeley Lab environment with a shared sense of purpose 2. A program development plan that will allow us to deepen our capabilities and provide more opportunities to have impact 3. An attempt to integrate our basic research with applications using models of technology deployment constraints 4. Set of internal activities aimed at priming the effort

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


401

Building Life Cycle Cost Programs  

Energy.gov (U.S. Department of Energy (DOE))

The National Institute of Standards and Technology (NIST) developed the Building Life Cycle Cost (BLCC) Program to provide computational support for the analysis of capital investments in buildings.

402

Minimize Boiler Short Cycling Losses  

Energy.gov (U.S. Department of Energy (DOE))

This tip sheet on minimizing boiler short cycling losses provides how-to advice for improving industrial steam systems using low-cost, proven practices and technologies.

403

BEAMLINE 4-1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 1 CURRENT STATUS: Open SUPPORTED TECHNIQUES: X-ray Absorption Spectroscopy MAIN SCIENTIFIC DISCIPLINES: Environmental / Materials / Chemistry / Biology % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: 20-pole, 2.0-Tesla Wiggler, 0.75 mrad, side station BEAM LINE SPECIFICATIONS: energy range grating type resolution DE/E spot size flux angular acceptance unfocused 5,500-38,000eV 10-4 4x18mm 0.75 mrad OPTICS: M0 mirror: Flat, bent vertically collimating, 1 m, Si, Rh-coated, cutoff 9-23 keV, LN2-cooled monochromator. Energies over 22keV are run with the mirror out. MONOCHROMATOR: Si(220) f=0° or Si(220) f=90° double-crystal, non-fixed exit slit Monochromator Crystal Glitch Library

404

BEAMLINE 2-2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 2 CURRENT STATUS: Open with limited support SUPPORTED TECHNIQUES: White light station MAIN SCIENTIFIC DISCIPLINES: X-ray optics characterization and development % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: Bend Magnet Side Station BEAM LINE SPECIFICATIONS: energy range resolution DE/E spot size flux angular acceptance unfocused 1000-40000 eV NA 4.0 x 8.0 mm NA 0.4 mrad OPTICS: None MONOCHROMATOR: None (white beam) ABSORPTION: 673 microns Be, 12.4 meters He, 15.2 microns C INSTRUMENTATION: X-Y stages, ion chambers, PMT DATA ACQUISITION AND ANALYSIS: SPEC For questions and issues related to SPEC, contact beam line staff or send an email to M$SPEC@ssrl.slac.stanford.edu SUPER

405

BEAMLINE 8-1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 1 CURRENT STATUS: Open SUPPORTED TECHNIQUES: Photoemission spectroscopy MAIN SCIENTIFIC DISCIPLINES: BL8-1a: Materials / Surface Chemistry BL8-1b: Materials % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: Bending magnet station (vacuum ultraviolet) BEAM LINE SPECIFICATIONS: energy range grating type resolution DE/E spot size (FWHM) flux angular acceptance focused 15 - 185 eV ~1 x 10-3 0.1 mm2 8.0 mrad OPTICS: M0 mirror: Cylindrical, SiC M1 mirror: Spherical, Fused Silica MONOCHROMATOR: 6m toroidal grating monochromator (TGM) Grating Monochromator References Monochromator Crystal Glitch Library Crystal changes need to be scheduled and coordinated in advance with BL support staff.

406

BEAMLINE 4-2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 2 CURRENT STATUS: Open SUPPORTED TECHNIQUES: Biological Small Angle X-ray Scattering/Diffraction Macromolecular solution x-ray scattering Lipid membrane diffraction Fiber diffraction Time-resolved x-ray scattering/diffraction Small-angle single crystal diffraction Ultra small-angle x-ray scattering (under development) MAIN SCIENTIFIC DISCIPLINES: Biology % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: 20-pole, 2.0-Tesla Wiggler ID End Station BEAM LINE SPECIFICATIONS: energy range grating type resolution DE/E spot size flux angular acceptance focused (crystal) 6000-18000 eV ~5 x 10-4 ~0.2 x 1.0mm < 1.0 mrad focused (multilayers) 8000-12000 eV ~3 x 10-2 ~0.2 x 1.0mm < 1.0 mrad

407

BEAMLINE 9-3  

NLE Websites -- All DOE Office Websites (Extended Search)

9-3 9-3 CURRENT STATUS: Closed (Down-pending mirror repair) SUPPORTED TECHNIQUES: X-ray absorption spectroscopy Single crystal x-ray absorption spectroscopy MAIN SCIENTIFIC DISCIPLINES: Structural Biology % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: 16-pole, 2-Tesla wiggler, 2 mrad beam BEAM LINE SPECIFICATIONS: energy range resolution DE/E spot size (fwhm) flux* angular acceptance focused 5000-30000 eV 1 x 10-4 0.4 x 3 mm2 ~2 x 1012 2.0 mrad *ph/sec @100 mA / 9 keV w 1x4 mm aperture OPTICS: M0 mirror: Flat, bent, vertically collimating, 1 m, Si, Rh-coated, LN2-cooled monochromator M1 mirror: Bent, cylindrical, 1.2 m, Zerodur, Rh-coated MONOCHROMATOR: Si(220) phi=0°, Si(220) phi=90° double-crystal,

408

BEAMLINE 1-4  

NLE Websites -- All DOE Office Websites (Extended Search)

-4 -4 CURRENT STATUS: Open SUPPORTED TECHNIQUES: Small angle x-ray scattering MAIN SCIENTIFIC DISCIPLINES: Materials % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: Bend magnet BEAM LINE SPECIFICATIONS: energy range resolution DE/E spot size flux angular acceptance focused 7100-9000 eV 4.0 x 10-3 0.25 x 1.0 mm ~1010 2.0 mrad OPTICS: MONOCHROMATOR: Bent crystal; Si ABSORPTION: NA INSTRUMENTATION: Small/Low Angle X-ray Scattering Camera System w/CCD Detector DATA ACQUISITION AND ANALYSIS: SPEC For questions and issues related to SPEC, contact beam line staff or send an email to M$SPEC@ssrl.slac.stanford.edu RESPONSIBLE STAFF: Chris Tassone, 650-926-3124 BEAM LINE PHONE NUMBER: 650-926-5214

409

BEAMLINE 13-2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 2 CURRENT STATUS Open RESPONSIBLE STAFF: Dan Brehmer Hirohito Ogasawara EXPERIMENTS: Photoemission; NEXAFS (see also: Spectroscopic Techniques) SCHEDULING: BL13 Schedules Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: Elliptically polarized undulator OPTICS: M0 vertical deflecting spherical, water-cooled M2 horizontal deflecting spherical M3 vertical deflecting elliptical MONOCHROMATOR: Spherical Grating Monochromator (SGM) SLITS : 0-1000 µm. Entrance slit cooled and movable ± 200 mm along optical axis GRATINGS : 3 water-cooled interchangeable HORIZONTAL ANGULAR ACCEPTANCE : 0.25 mrad ENERGY RANGE : 300 l/mm: 150 - 400 E/DE 10000 600 l/mm: 250 - 700 E/DE 10000 1100 l/mm: 500 - 1200 E/DE 10000 SPOT SIZE : 0.01 x 0.075 mm2

410

BEAMLINE 8-2  

NLE Websites -- All DOE Office Websites (Extended Search)

2 2 CURRENT STATUS: Open SUPPORTED TECHNIQUES: X-ray absorption spectroscopy, near edge Photoemission spectroscopy MAIN SCIENTIFIC DISCIPLINES: Materials % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: Bending magnet station (soft x-ray) BEAM LINE SPECIFICATIONS: energy range grating type resolution DE/E spot size (FWHM) flux angular acceptance focused 100 - 1300 eV ~4 x 10-4 >0.1 mm2 4.0 mrad OPTICS: M0 mirror: toroidal SiC MONOCHROMATOR: 6m spherical grating monochromator (TGM) Grating Monochromator References ABSORPTION: NA INSTRUMENTATION: User Chambers on VUV Lines DATA ACQUISITION AND ANALYSIS: SPEC For questions and issues related to SPEC, contact beam line staff or send

411

BEAMLINE 5-4  

NLE Websites -- All DOE Office Websites (Extended Search)

5-4 5-4 CURRENT STATUS: Open SUPPORTED TECHNIQUES: Very High Energy Resolution; Photoemission Angle-Resolved Photoelectron Spectroscopy MAIN SCIENTIFIC DISCIPLINES: Materials % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: 10-period undulator, maximum field 0.61 T BEAM LINE SPECIFICATIONS: energy range grating type resolution DE/E spot size flux angular acceptance focused 7-40 eV 1700 l/mm: 7-18 eV, E/DE > 10000 2800 l/mm: 16-32 eV, E/DE> 10000 3600 l/mm: 20-40 eV, E/DE> 10000 ≥1 x 10-4 0.5 x 0.6 mm2 ~1011 >1.5 mrad OPTICS: M0: horizontal deflecting, flat, water-cooled M1: vertical focusing 10:1, elliptically cylinder M3: horizontal refocusing 1:1, cylinder M4: vertical refocusing 1:1, cylinder

412

BEAMLINE 2-1  

NLE Websites -- All DOE Office Websites (Extended Search)

1 1 CURRENT STATUS: Open SUPPORTED TECHNIQUES: Powder diffraction Thin film diffraction MAIN SCIENTIFIC DISCIPLINES: Materials / Environmental % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: 1.3 Tesla Bend Magnet BEAM LINE SPECIFICATIONS: energy range resolution DE/E spot size flux angular acceptance focused 4000-14500 eV ~5 x 10-4 .20 x 0.45 mm 1.5 mrad OPTICS: Bent cylinder, single-crystal Si, Rh-coated mirror Radii: 2900 m (adjustable) x 52 mm Mean angle of incidence: 4.2 milliradians Cut off energy: 14.5 keV, Magnification: 1.1 MONOCHROMATOR: Si(111), Si(220) Si(400), upward reflecting, double-crystal Monochromator Crystal Glitch Library Crystal changes need to be scheduled and coordinated in advance with BL

413

BEAMLINE 7-3  

NLE Websites -- All DOE Office Websites (Extended Search)

3 3 CURRENT STATUS: Open SUPPORTED TECHNIQUES: X-ray absorption spectroscopy MAIN SCIENTIFIC DISCIPLINES: Structural Biology % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: 20-pole, 2-Tesla wiggler, 0.8 mrad beam, side station BEAM LINE SPECIFICATIONS: energy range resolution DE/E spot size (fwhm) flux* angular acceptance unfocused 4600-37000 eV 1 x 10-4 2 x 15 mm2 ~1 x 1012 0.8 mrad *ph/sec @100 mA / 9 keV w 2x15 mm aperture OPTICS: M0 mirror: Flat, bent, vertically collimating, 1 m, Si, Rh-coated, LN2-cooled monochromator MONOCHROMATOR: Si(220) phi=0°, Si(220) phi=90° double-crystal, non-fixed exit slit Monochromator Crystal Glitch Library Crystal changes need to be scheduled and coordinated in advance with BL

414

BEAMLINE 13-3  

NLE Websites -- All DOE Office Websites (Extended Search)

EXPERIMENTAL STATION 13-3 EXPERIMENTAL STATION 13-3 CURRENT STATUS Open RESPONSIBLE STAFF Bart Johnson EXPERIMENTS Soft X-ray Coherent Scattering: Resonant, Polarization-dependent; Lensless Imaging: X-ray Holography, MAD phasing; X-ray Photon Correlation Spectroscopy SCHEDULING Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE EPU, Linear and Circular Polarization MONOCHROMATOR SGM, Rowland Circle Spherical Grating 300l/mm 600l/mm 1100l/mm Energy Range 150-400eV 350-750eV 600-1200eV Entrance Slit: 5-20 microns (typical), movable along beam path Exit Slit: 30-100 microns (typical) FOCUSING OPTICS 1313M1 Spherical Mirror, Horizontal Demag. 3:1 133M2 Spherical Mirror, Vertical Demag. 3:2 Spot Size on Sample (min) 24 microns (vertical) x 240 microns (horizontal)

415

BEAMLINE 7-2  

NLE Websites -- All DOE Office Websites (Extended Search)

7-2 7-2 CURRENT STATUS: Open SUPPORTED TECHNIQUES: X-ray scattering X-ray diffraction MAIN SCIENTIFIC DISCIPLINES: Materials / Environmental % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: 20-pole, 2-Tesla Wiggler ID End Station BEAM LINE SPECIFICATIONS: energy range resolution DE/E spot size flux angular acceptance focused 4600 - 16500 eV 0.12 x 0.50 mm 0.4 mrad OPTICS: Bent cylinder, single crystal Si, Rh-coated M0 mirror Radii: 2945 m (adjustable) x 56.1 mm Mean angle of incidence: 3.81 mrad Cut off energy: 17.7 keV Magnification: 1.0 MONOCHROMATOR: LN2-cooled, sagitally focusing, double crystal Si(111) Upward reflecting Monochromator Crystal Glitch Library Crystal changes need to be scheduled and coordinated in advance with BL

416

BEAMLINE 10-2  

NLE Websites -- All DOE Office Websites (Extended Search)

0-2 0-2 CURRENT STATUS: Open SUPPORTED TECHNIQUES: 10-2a: X-ray absorption spectroscopy; XAS imaging 10-2b: X-ray scattering MAIN SCIENTIFIC DISCIPLINES: Biology / Materials / Environmental % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: 30-pole, 1.45-Tesla Wiggler ID End Station BEAM LINE SPECIFICATIONS: energy range resolution DE/E spot size flux angular acceptance focused 4500 - 30000 eV 0.2 x .43 mm 1.5 mrad unfocused 4500 - 45000 eV 2.0 x 20.0 mm 1.5 mrad OPTICS: Bent cylinder, Rh-coated, single crystal Si, M0 mirror Radii: 1500 m (adjustable) x 32.9 mm Cut off energy: 22 keV, Mean angle of incidence: 2.7 mrad MONOCHROMATOR: Si(111) f=90° or Si(220) f=90° Liquid nitrogen-cooled,

417

BEAMLINE 6-2  

NLE Websites -- All DOE Office Websites (Extended Search)

6-2 6-2 CURRENT STATUS: Open SUPPORTED TECHNIQUES: BL6-2a: Rapid-scanning xRF imaging Advanced x-ray spectroscopy (XES, XRS, RIXS) XES: Resonant and non-resonant x-ray emission spectroscopy XRS: Non-resonant x-ray Raman scattering BL6-2b: Rapid-scanning xRF imaging Advanced x-ray spectroscopy (XES, XRS, RIXS) XES: Resonant and non-resonant x-ray emission spectroscopy XRS: Non-resonant x-ray Raman scattering BL6-2c: Transmission X-ray Microscopy MAIN SCIENTIFIC DISCIPLINES: Biology / Materials / Environmental % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: 56-pole, 0.9-Tesla Wiggler ID End Station BEAM LINE SPECIFICATIONS: energy range resolution DE/E spot size flux angular acceptance

418

BEAMLINE 4-3  

NLE Websites -- All DOE Office Websites (Extended Search)

4-3 4-3 CURRENT STATUS: Open SUPPORTED TECHNIQUES: X-ray Absorption Spectroscopy MAIN SCIENTIFIC DISCIPLINES: Environmental / Materials / Biology % TIME GENERAL USE: 100% SCHEDULING: Proposal Submittal and Scheduling Procedures Current SPEAR and Beam Line Schedules SOURCE: 20-pole, 2.0-Tesla wiggler, 0.75 mrad, side station BEAM LINE SPECIFICATIONS: energy range resolution DE/E spot size flux angular acceptance unfocused 2400-14000 eV 10-4 3 x 16 mm 0.75 mrad OPTICS: M0 mirror: Flat, bent vertically collimating, 1 m, Si, Rh-coated, cutoff 4-14 keV, LN2-cooled monochromator MONOCHROMATOR: Si(111) f=0° or Si(111) f=90° double-crystal, non-fixed exit slit Monochromator Crystal Glitch Library Crystal changes need to be scheduled and coordinated in advance with BL

419

BEAMLINE 10-1  

NLE Websites -- All DOE Office Websites (Extended Search)

in advance with BL support staff. ABSORPTION: NA INSTRUMENTATION: Facility or user UHV chambers User Chambers on VUV Lines DATA ACQUISITION AND ANALYSIS: Data acquisition:...

420

BEAMLINE 13-1  

NLE Websites -- All DOE Office Websites (Extended Search)

studies 10-50 ps time resolution based on SSRL operating mode Sample environment: UHV, Spectroscopy: T 25-450K, magnetic fields up to 0.25 Tesla Microscopy: Room...

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


421

The SLS optics beamline  

E-Print Network (OSTI)

brazing the window is fully UHV compatible and bakable up touses a newly developed UHV compatible, 100 m thick, brazed

2006-01-01T23:59:59.000Z

422

NYSBC MICRODIFFRACTION BEAMLINE  

NLE Websites -- All DOE Office Websites (Extended Search)

f or m acromolecular complexes a nd m embrane p roteins. * X---ray e nergy c overage f rom 3 .5---17.5 k eV. C apable o f a nomalous d iffracPon experiments f rom u ranium M V (...

423

Beamline Advisory Committees  

NLE Websites -- All DOE Office Websites (Extended Search)

Prof. Dr. Thomas Brckel (Institute of Solid State Research, Forschungszentrum Jlich, Germany ) Dr. Carsten Detlefs (European Synhrotron Radiation Facility) Prof. Bruce Gaulin...

424

Virtuous Cycle Cycles of activity and software projects  

E-Print Network (OSTI)

Inspection #12;Programming Cycle - single bug Selected Bug Shared Code Fix Bug Continuous Integration ~8 cycle cvscheck compilation style checking testing javadocs documentation jumble quality of unit testing #12;NetValue Development cvscheck - Source Code Control and Build Shared Centralized Automatic

Pfahringer, Bernhard

425

Life Cycle Asset Management  

Directives, Delegations, and Requirements

(The following directives are deleted or consolidated into this Order and shall be phased out as noted in Paragraph 2: DOE 1332.1A; DOE 4010.1A; DOE 4300.1C; DOE 4320.1B; DOE 4320.2A; DOE 4330.4B; DOE 4330.5; DOE 4540.1C; DOE 4700.1). This Order supersedes specific project management provisions within DOE O 430.1A, LIFE CYCLE ASSET MANAGEMENT. The specific paragraphs canceled by this Order are 6e(7); 7a(3); 7b(11) and (14); 7c(4),(6),(7),(11), and (16); 7d(4) and (8); 7e(3),(10), and (17); Attachment 1, Definitions (item 30 - Line Item Project, item 42 - Project, item 48 - Strategic System); and Attachment 2, Contractor Requirements Document (paragraph 1d regarding a project management system). The remainder of DOE O 430.1A remains in effect. Cancels DOE O 430.1. Canceled by DOE O 413.3.

1998-10-14T23:59:59.000Z

426

Natural Gas Combined Cycle  

E-Print Network (OSTI)

The Coal Ash Corrosion Resistant Materials Testing Program is being conducted by B&W at Reliant Energys Niles plant in Niles, Ohio. The total estimated cost of $1,864,603 is co-funded by DOE contributing 37.5%, OCDO providing 33.3 % and B&W providing 17%. The remaining 12 % is in-kind contributions by Reliant Energy and tubing suppliers. Materials development is important to the power industry, and to the use of coal. Figure 1 compares the cost of electricity for subcritical and supercritical coal-fired plants with a natural gas combined cycle (NGCC) plant based on an 85 % capacity factor. This shows that at $1.20/MBtu for fuel, coal is competitive with NGCC when gas is at $3.40/MBtu or higher. An 85 % capacity factor is realistic for a coal-fired plant, but NGCC plants are currently only achieving about 60%. This gives coal an advantage if compared on the basis of cost per kW generated per year. When subcritical and supercritical plants are compared,

Dennis K. Mcdonald; Subcritical Coal Plant; Supercritical Coal Plant

427

Biomass Gasification Combined Cycle  

SciTech Connect

Gasification combined cycle continues to represent an important defining technology area for the forest products industry. The ''Forest Products Gasification Initiative'', organized under the Industry's Agenda 2020 technology vision and supported by the DOE ''Industries of the Future'' program, is well positioned to guide these technologies to commercial success within a five-to ten-year timeframe given supportive federal budgets and public policy. Commercial success will result in significant environmental and renewable energy goals that are shared by the Industry and the Nation. The Battelle/FERCO LIVG technology, which is the technology of choice for the application reported here, remains of high interest due to characteristics that make it well suited for integration with the infrastructure of a pulp production facility. The capital cost, operating economics and long-term demonstration of this technology area key input to future economically sustainable projects and must be verified by the 200 BDT/day demonstration facility currently operating in Burlington, Vermont. The New Bern application that was the initial objective of this project is not currently economically viable and will not be implemented at this time due to several changes at and around the mill which have occurred since the inception of the project in 1995. The analysis shows that for this technology, and likely other gasification technologies as well, the first few installations will require unique circumstances, or supportive public policies, or both to attract host sites and investors.

Judith A. Kieffer

2000-07-01T23:59:59.000Z

428

Nuclear fuel cycle information workshop  

SciTech Connect

This overview of the nuclear fuel cycle is divided into three parts. First, is a brief discussion of the basic principles of how nuclear reactors work; second, is a look at the major types of nuclear reactors being used and world-wide nuclear capacity; and third, is an overview of the nuclear fuel cycle and the present industrial capability in the US.

Not Available

1983-01-01T23:59:59.000Z

429

Working fluid for Rankine cycle  

SciTech Connect

A Rankine cycle working fluid is disclosed containing a mixture of 2,2,3,3tetrafluoropropanol and water, which is low toxic, incombustible, nonexplosive, noncorrosive and stable, and also has a high critical temperature and forms azeotropic-like composition. It is suited for use in a rankine cycle using heat source of low temperature.

Aomi, H.; Enjo, N.

1980-11-11T23:59:59.000Z

430

Extreme Financial cycles$ B. Candelonb,  

E-Print Network (OSTI)

Extreme Financial cycles$ B. Candelonb, , G. Gauliera , C. Hurlinb aUniversity Maastricht proposes a new approach to date extreme financial cycles. Elabo- rating on recent methods in extreme value theory, it elaborates an extension of the famous calculus rule to detect extreme peaks and troughs

Paris-Sud XI, Université de

431

Reading Comprehension - The Water Cycle  

NLE Websites -- All DOE Office Websites (Extended Search)

The Water Cycle The Water Cycle Evaporation, Condensation and Precipitation The _________ moon sun water clouds evaporates _________ fish oceans rain water from lakes and oceans. As the air rises, it cools. The water vapor condenses into tiny droplets of _________ evaporation clouds water sunshine . The droplets crowd together and form a _________ cloud lake storm precipitation . Wind blows the _________ rain sun droplet cloud towards the land. The tiny droplets join together and fall as precipitation to the _________ river lake ground cloud . The water soaks into the ground and collects in _________ rivers and lakes oceans and clouds jars and cups plants and animals . The _________ storm cycle river house that never ends has started again! A water cycle diagram. Use the diagram to identify the different parts of the water cycle:

432

CMVRTC: Heavy Truck Duty Cycle  

NLE Websites -- All DOE Office Websites (Extended Search)

heavy truck duty cycle (HTDC) project heavy truck duty cycle (HTDC) project OVERVIEW The Heavy Truck Duty Cycle (HTDC) Project was initiated in 2004 and is sponsored by the US Department of Energy's (DOE's) Office of FreedomCar and Vehicle Technologies Program. ORNL designed the research program to generate real-world-based duty cycle data from trucks operating in long-haul operations and was designed to be conducted in three phases: identification of parameters to be collected, instrumentation and pilot testing, identification of a real-world fleet, design of the data collection suite and fleet instrumentation, and data collection, analysis, and development of a duty cycle generation tool (DCGT). ANL logo dana logo michelin logo Schrader logo This type of data will be useful for supporting energy efficiency

433

Fuel cycle cost uncertainty from nuclear fuel cycle comparison  

SciTech Connect

This paper examined the uncertainty in fuel cycle cost (FCC) calculation by considering both model and parameter uncertainty. Four different fuel cycle options were compared in the analysis including the once-through cycle (OT), the DUPIC cycle, the MOX cycle and a closed fuel cycle with fast reactors (FR). The model uncertainty was addressed by using three different FCC modeling approaches with and without the time value of money consideration. The relative ratios of FCC in comparison to OT did not change much by using different modeling approaches. This observation was consistent with the results of the sensitivity study for the discount rate. Two different sets of data with uncertainty range of unit costs were used to address the parameter uncertainty of the FCC calculation. The sensitivity study showed that the dominating contributor to the total variance of FCC is the uranium price. In general, the FCC of OT was found to be the lowest followed by FR, MOX, and DUPIC. But depending on the uranium price, the FR cycle was found to have lower FCC over OT. The reprocessing cost was also found to have a major impact on FCC.

Li, J.; McNelis, D. [Institute for the Environment, University of North Carolina, Chapel Hill (United States); Yim, M.S. [Department of Nuclear and Quantum Engineering, Korea Advanced Institute of Science and Technology (Korea, Republic of)

2013-07-01T23:59:59.000Z

434

CMVRTC: Medium Truck Duty Cycle  

NLE Websites -- All DOE Office Websites (Extended Search)

medium truck duty cycle (MTdc) project medium truck duty cycle (MTdc) project OVERVIEW The Medium Truck Duty Cycle (MTDC) project involves efforts to collect, analyze and archive data related to medium-truck operations in real-world driving environments. Such data and information will be useful to support technology evaluation efforts and to provide a means of accounting for real-world driving performance within medium-class truck analyses. The project involves private industry partners from various truck vocations. The MTDC project is unique in that there currently does not exist a national database of characteristic duty cycles for medium trucks. This project involves the collection of data from multiple vocations (four vocations) and multiple vehicles within these vocations (three vehicles per

435

Minimize Boiler Short Cycling Losses  

SciTech Connect

This revised ITP tip sheet on minimizing boiler short cycling losses provides how-to advice for improving industrial steam systems using low-cost, proven practices and technologies.

Not Available

2006-01-01T23:59:59.000Z

436

THE TRANSPOSED CRITICAL TEMPERATURE RANKINE THERMODYNAMIC CYCLE  

E-Print Network (OSTI)

Combined Diesel-Organic Rankine Cycle Power Plant", in25OoC) closed simple organic Rankine cycle geothermal powerthe simple closed organic Rankine cycle for a given set of

Pope, William L.

2012-01-01T23:59:59.000Z

437

Sustainability Features of Nuclear Fuel Cycle Options  

E-Print Network (OSTI)

The nuclear fuel cycle is the series of stages that nuclear fuel materials go through in a cradle to grave framework. The Once Through Cycle (OTC) is the current fuel cycle implemented in the United States; in which an ...

Passerini, Stefano

438

146 CALIFORNIA AGRICULTURE VOLUME 59, NUMBER 3 Over the past 6 months I've been  

E-Print Network (OSTI)

, elected officials, environ- mental advocates -- who rely on the University for research findings, new though I had worked with UC for 25 years as a Cooperative Extension forestry specialist, I hadn't fully's Agricultural Experiment Station (AES) and Cooperative Extension (UCCE). Our campus- and county

Standiford, Richard B.

439

FedEx Gasoline Hybrid Electric Delivery Truck Evaluation: 6-Month...  

NLE Websites -- All DOE Office Websites (Extended Search)

each of these systems. These systems and specific components of interest include: * Vehicle Systems o Engine o Hybrid propulsion system o Brakes * Vehicle Components o Brake...

440

FedEx Gasoline Hybrid Electric Delivery Truck Evaluation: 6-Month...  

NLE Websites -- All DOE Office Websites (Extended Search)

ignition CO Carbon monoxide DOE U.S. Department of Energy DPF Diesel particulate filter gHEV Gasoline hybrid electric vehicle GVWR Gross vehicle weight rating HP...

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


441

Exergy Analysis of Stirling Cycle Cryogenerator  

Science Journals Connector (OSTI)

Exergy or the available work energy function is ... various systems. This paper attempts to present exergy analysis for Stirling cycle cryogenerator. The cycle...

K. G. Narayankhedkar

1998-01-01T23:59:59.000Z

442

Life Cycle Analysis: Integrated Gasification Combined Cycle (IGCC) Power Plant  

NLE Websites -- All DOE Office Websites (Extended Search)

Life Cycle Analysis: Integrated Life Cycle Analysis: Integrated Gasification Combined Cycle (IGCC) Power Plant Revision 2, March 2012 DOE/NETL-2012/1551 Disclaimer This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference therein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise does not necessarily constitute or

443

The behavioral manipulation hypothesis Life cycle of  

E-Print Network (OSTI)

1 The behavioral manipulation hypothesis · No one knows how the parasite causes these Life cycle eat mostly hares · Linked cycles? Predator-Prey Cycles? · Think and then discuss: · Under the hypothesis that predators cause this cycle, what would you expect for the following when hare populations

Mitchell, Randall J.

444

SNMR pulse sequence phase cycling  

DOE Patents (OSTI)

Technologies applicable to SNMR pulse sequence phase cycling are disclosed, including SNMR acquisition apparatus and methods, SNMR processing apparatus and methods, and combinations thereof. SNMR acquisition may include transmitting two or more SNMR pulse sequences and applying a phase shift to a pulse in at least one of the pulse sequences, according to any of a variety cycling techniques. SNMR processing may include combining SNMR from a plurality of pulse sequences comprising pulses of different phases, so that desired signals are preserved and indesired signals are canceled.

Walsh, David O; Grunewald, Elliot D

2013-11-12T23:59:59.000Z

445

Simple ocean carbon cycle models  

SciTech Connect

Simple ocean carbon cycle models can be used to calculate the rate at which the oceans are likely to absorb CO{sub 2} from the atmosphere. For problems involving steady-state ocean circulation, well calibrated ocean models produce results that are very similar to results obtained using general circulation models. Hence, simple ocean carbon cycle models may be appropriate for use in studies in which the time or expense of running large scale general circulation models would be prohibitive. Simple ocean models have the advantage of being based on a small number of explicit assumptions. The simplicity of these ocean models facilitates the understanding of model results.

Caldeira, K. [Lawrence Livermore National Lab., CA (United States); Hoffert, M.I. [New York Univ., NY (United States). Dept. of Earth System Sciences; Siegenthaler, U. [Bern Univ. (Switzerland). Inst. fuer Physik

1994-02-01T23:59:59.000Z

446

Closed cycle liquid helium refrigerators  

Science Journals Connector (OSTI)

We have developed closed cycle liquid helium refrigerators using a Joule Thomson circuit precooled by commercially available two staged Gifford Mac Mahon cryocoolers. The Joule Thomson counterflow heat exchangers are modular and have been thermo-hydraulically characterized. Fully automatic cool down and operation are achieved by two pneumatically driven by pass and expansion valves. Several apparatus have been built or are under assembly with cooling power ranging from 100 mW up to 5 Watt, for temperature ranging from 2.8 K up to 4.5 K. A trouble free operation with several warm up and cool down cycles has been proven over 7000 hours.

G. Claudet; R. Lagnier; A. Ravex

1992-01-01T23:59:59.000Z

447

GAX absorption cycle design process  

SciTech Connect

This paper presents an absorption system design process that relies on computer simulations that are validated by experimental findings. An ammonia-water absorption heat pump cycle at 3 refrigeration tons (RT) and chillers at 3.3 RT and 5 RT (10.5 kW, 11.6 kW, and 17.6 kW) were initially modeled and then built and tested. The experimental results were used to calibrate both the cycle simulation and the component simulations, yielding computer design routines that could accurately predict component and cycle performance. Each system was a generator-absorber heat exchange (GAX) cycle, and all were sized for residential and light commercial use, where very little absorption equipment is currently used. The specific findings of the 5 RT (17.6 kW) chiller are presented. Modeling incorporated a heat loss from the gas-fired generator and pressure drops in both the evaporator and absorber. Simulation results and experimental findings agreed closely and validated the modeling method and simulation software.

Priedeman, D.K.; Christensen, R.N.

1999-07-01T23:59:59.000Z

448

Fluorescence-type Monochromatic X-ray Beam-position Monitor with High-spatial Resolution for the NSLS-II Beamlines  

SciTech Connect

We developed a fluorescence-type monochromatic X-ray beam-position monitor (X-BPM) with high-spatial resolution for end-station experiments at the initial project beamlines of the NSLS-II. We designed a ring array of multi-segmented Si PIN-junction photodiodes to use as a position sensor. Further, we integrated a low-noise charge-preamplification HERMES4 ASIC chip into an electronic readout system for photon-counting application. A series of precision measurements to characterize electronically the Si-photodiode sensor and the ASIC chip demonstrated that the inherent noise from the detector system is sufficiently low to meet our stringent requirements. Using a Gaussian beam, we parametrically modeled the optimum working distance to ensure the detector's best performance. Based upon the results from the parametric modeling, prototypes of the next versions of the X-BPM are being developed. In this paper, we describe the methodology for developing the new compact monochromatic X-ray BPM, including its instrumentation, detector modeling, and future plan.

Yoon, Phil S. [Experimental Facility Division, NSLS-II, Brookhaven National Laboratory, Upton, NY 11973 (United States); Siddons, D. Peter [Experimental Systems, NSLS, Brookhaven National Laboratory, Upton, NY 11973 (United States)

2010-06-23T23:59:59.000Z

449

Rankine and Brayton Cycle Cogeneration for Glass Melting  

E-Print Network (OSTI)

Rankine cycle, b) an organic Rankine cycle, c) an indirectly heated positive pressure Brayton cycle and d) a directly heated subatmospheric Brayton cycle. For the specified flue gas temperatures considered, the organic Rankine cycle produced the most...

Hnat, J. G.; Patten, J. S.; Sheth, P. R.

1981-01-01T23:59:59.000Z

450

Definition: Rankine cycle | Open Energy Information  

Open Energy Info (EERE)

Rankine cycle Rankine cycle Jump to: navigation, search Dictionary.png Rankine cycle Sometimes referred to as the steam cycle. Fuel is used to heat a liquid to produce a high pressure gas that expands and produces work, such as turning a turbine; when the turbine is connected to a generator, it produces electricity. Usually water is the liquid used in the Rankine cycle (to produce steam), but other liquids can also be used. The exhaust vapor expelled from the turbine condenses and the liquid is pumped back to the boiler to repeat the cycle.[1][2] View on Wikipedia Wikipedia Definition The Rankine cycle is a mathematical model that is used to predict the performance of steam engines. The Rankine cycle is an idealised thermodynamic cycle of a heat engine that converts heat into mechanical

451

Kalina combined cycle performance and operability  

SciTech Connect

Gas turbine combined cycles using Rankine bottoming cycles have gained broad market acceptance. The favorable plant economics derive from their high efficiency, short construction cycles and excellent environmental performance. The responsive operating characteristics of combined cycles is another key advantage for customers. Duty cycles cover the spectrum from daily start stop (DSS) to base load. Performance and economics of combined cycles have progressed with advances in gas turbine technology as well as the introduction of increasingly efficient multi-pressure Rankine bottoming cycles. Further advances in gas turbine technology and Rankine bottoming cycle performance are becoming incrementally more difficult and costly to achieve. The availability of the Kalina cycle presents a clear path toward improved combined-cycle system performance and reduced cost of electricity. This paper presents detailed performance and operating characteristics of a STAG 207FA combined cycle employing the Kalina bottoming cycle. These characteristics are compared to a conventional three-pressure reheat Rankine bottoming cycle. The Kalina cycle is shown to have performance and operability advantages throughout the range of site conditions and operating regimes, such as base load, load following, DSS duty, wet and dry cooling tower applications and unattended operation. These advantages derive from a single-pressure once-through heat recovery system, above atmospheric working fluid pressure throughout the system, above atmospheric working fluid pressure throughout the system, very high thermal efficiency ({approximately}2.0 to 2.5 percentage points better than the best Rankine), and compatibility with sub-freezing ambient conditions.

Smith, R.W.; Ranasinghe, J.; Stats, D.; Dykas, S.

1996-12-31T23:59:59.000Z

452

VISION - Verifiable Fuel Cycle Simulation of Nuclear Fuel Cycle Dynamics  

SciTech Connect

The U.S. DOE Advanced Fuel Cycle Initiatives (AFCI) fundamental objective is to provide technology options that - if implemented - would enable long-term growth of nuclear power while improving sustainability and energy security. The AFCI organization structure consists of four areas; Systems Analysis, Fuels, Separations and Transmutations. The Systems Analysis Working Group is tasked with bridging the program technical areas and providing the models, tools, and analyses required to assess the feasibility of design and deployment options and inform key decision makers. An integral part of the Systems Analysis tool set is the development of a system level model that can be used to examine the implications of the different mixes of reactors, implications of fuel reprocessing, impact of deployment technologies, as well as potential "exit" or "off ramp" approaches to phase out technologies, waste management issues and long-term repository needs. The Verifiable Fuel Cycle Simulation Model (VISION) is a computer-based simulation model that allows performing dynamic simulations of fuel cycles to quantify infrastructure requirements and identify key trade-offs between alternatives. It is based on the current AFCI system analysis tool "DYMOND-US" functionalities in addition to economics, isotopic decay, and other new functionalities. VISION is intended to serve as a broad systems analysis and study tool applicable to work conducted as part of the AFCI and Generation IV reactor development studies.

Steven J. Piet; A. M. Yacout; J. J. Jacobson; C. Laws; G. E. Matthern; D. E. Shropshire

2006-02-01T23:59:59.000Z

453

Rankine cycle leak detection via continuous monitoring  

SciTech Connect

Rankine cycle power plants operate on a closed cycle in which heat is transferred from a high temperature reservoir to a low temperature sink while performing useful work. leaks in this cycle cause the loss of working fluid and/or corrosion of the power plant. Both of these constitute a loss of capital assets. A severe leak can reduce the efficiency of the cycle to the extent of creating an operating loss. PNL is undertaking the development of continuous monitoring techniques to protect rankine cycle plants from such losses. The location of these continuous monitors on an organic rankine cycle is described and shown schematically.

Kindle, Cecil H.

1982-10-08T23:59:59.000Z

454

Low-Cycle-Fatigue Behavior of Copper Materials and Their Use  

Office of Scientific and Technical Information (OSTI)

facilities such as the 7-GeV Advanced Photon Source Project ( A P S ) generate x-ray beams with very high heat loads and heat flux levels. The front-end and beamline components...

455

NREL: U.S. Life Cycle Inventory Database - Life Cycle Assessments  

NLE Websites -- All DOE Office Websites (Extended Search)

Life Cycle Assessments A life cycle assessment (LCA) is a systematic, cradle-to-grave process that evaluates the environmental impacts of products, processes, and services. Its...

456

Medium Truck Duty Cycle (MTDC)  

NLE Websites -- All DOE Office Websites (Extended Search)

Routes Data Acquisition System Setup Routes Data Acquisition System Setup Medium Truck Duty Cycle (MTDC) Objective This Department of Energy project focuses on the collection and analysis medium truck (Class-6 and -7) duty cycle data from real-world operations. Analysis of this data will provide information pertaining to the fuel efficiencies and performance of medium trucks in several vocations. Outcomes Rich source of data and information that can contribute to the development of new tools Sound basis upon which DOE can make technology investment decisions A national archive of real-world-based medium-truck operational data that will support medium-duty vehicle energy efficiency research Collected Data Speed & Acceleration Fuel Consumption GPS Location Road Grade

457

The Life Cycle Analysis Toolbox  

SciTech Connect

The life cycle analysis toolbox is a valuable integration of decision-making tools and supporting materials developed by Oak Ridge National Laboratory (ORNL) to help Department of Energy managers improve environmental quality, reduce costs, and minimize risk. The toolbox provides decision-makers access to a wide variety of proven tools for pollution prevention (P2) and waste minimization (WMin), as well as ORNL expertise to select from this toolbox exactly the right tool to solve any given P2/WMin problem. The central element of the toolbox is a multiple criteria approach to life cycle analysis developed specifically to aid P2/WMin decision-making. ORNL has developed numerous tools that support this life cycle analysis approach. Tools are available to help model P2/WMin processes, estimate human health risks, estimate costs, and represent and manipulate uncertainties. Tools are available to help document P2/WMin decision-making and implement programs. Tools are also available to help track potential future environmental regulations that could impact P2/WMin programs and current regulations that must be followed. An Internet-site will provide broad access to the tools.

Bishop, L.; Tonn, B.E.; Williams, K.A.; Yerace, P.; Yuracko, K.L.

1999-02-28T23:59:59.000Z

458

The Quebec Life Cycle Inventory Database Project  

Science Journals Connector (OSTI)

Life cycle assessment (LCA) in Quebec (Canada) is increasingly important. Yet, ... life cycle inventory (LCI) data. The Quebec government invested in the creation of a Quebec LCI database. The approach is to work...

Pascal Lesage; Rjean Samson

2013-05-01T23:59:59.000Z

459

Profit cycle dynamics by Kawika Pierson.  

E-Print Network (OSTI)

My thesis consists of three essays investigating the existence, causes, and mitigation of profit cycles at an industry level. The first essay examines profit cycles by proposing that the industry-specific features of how ...

Pierson, Kawika (Kawika Paul)

2011-01-01T23:59:59.000Z

460

Rethinking the light water reactor fuel cycle  

E-Print Network (OSTI)

The once through nuclear fuel cycle adopted by the majority of countries with operating commercial power reactors imposes a number of concerns. The radioactive waste created in the once through nuclear fuel cycle has to ...

Shwageraus, Evgeni, 1973-

2004-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


461

Viable combined cycle design for automotive applications  

Science Journals Connector (OSTI)

A relatively new approach for improving fuel economy and automotive engine performance involves the use of automotive combined cycle generation technologies. The combined cycle generation, a process widely used i...

K. -B. Kim; K. -W. Choi; K. -H. Lee

2012-04-01T23:59:59.000Z

462

Coal-Fuelled Combined Cycle Power Plants  

Science Journals Connector (OSTI)

Combined cycle power plant, when used as a generic ... which converts heat into mechanical energy in a combined gas and steam turbine process. Combined cycle processes with coal gasification or coal combustion .....

Dr. Hartmut Spliethoff

2010-01-01T23:59:59.000Z

463

Toward single-cycle optical pulses  

E-Print Network (OSTI)

Single-cycle optical pulses, the never-before-achieved regime, have a great potential for attosecond science and phase-sensitive nonlinear optics. To achieve single-cycle optical pulses by active synchronization, three ...

Kim, Jung-Won, 1976-

2004-01-01T23:59:59.000Z

464

Development Plan for the Fuel Cycle Simulator  

SciTech Connect

The Fuel Cycle Simulator (FCS) project was initiated late in FY-10 as the activity to develop a next generation fuel cycle dynamic analysis tool for achieving the Systems Analysis Campaign 'Grand Challenge.' This challenge, as documented in the Campaign Implementation Plan, is to: 'Develop a fuel cycle simulator as part of a suite of tools to support decision-making, communication, and education, that synthesizes and visually explains the multiple attributes of potential fuel cycles.'

Brent Dixon

2011-09-01T23:59:59.000Z

465

Using Cycles and Scaling Parallel Algorithms  

E-Print Network (OSTI)

graph by finding a max­ imal set of edge­disjoint cycles. We give a parallel algorithm to find the first efficient parallel algorithm for finding an approximation to a min­ imum cycle cover. Our algorithm finds a cycle cover whose size is within a factor of O(1 + n log n m+n ) of the minimum sized

Yang, Junfeng

466

How Minds Work The IDA Cognitive Cycle  

E-Print Network (OSTI)

1 How Minds Work The IDA Cognitive Cycle Stan Franklin Computer Science Division & Institute for Intelligent Systems The University of Memphis #12;HMW: The IDA Cognitive Cycle 2 Memory Systems #12;HMW: The IDA Cognitive Cycle 3 Global Workspace Theory I · The nervous system is a distributed parallel

Memphis, University of

467

SPACETELESCOPESCIENCEINSTITUTE WFPC2 Cycle 14 Calibration  

E-Print Network (OSTI)

/chip combinations used for science in Cycle 14 + Close Out ~10% reserve 2 Placeholder for unexpected items. TOTALSPACETELESCOPESCIENCEINSTITUTE WFPC2 Cycle 14 Calibration Director's Review 8 August 2005 John Biretta 1 Cycle 14 WFPC2 Calibration Plan Overall Goals: · Monitor & maintain WFPC2 health & safety

Sirianni, Marco

468

Building Life Cycle Cost Programs | Department of Energy  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Building Life Cycle Cost Programs Building Life Cycle Cost Programs The National Institute of Standards and Technology (NIST) developed the Building Life Cycle Cost (BLCC) Program...

469

Life Cycle Assessment Comparing the Use of Jatropha Biodiesel...  

NLE Websites -- All DOE Office Websites (Extended Search)

on Climate Change IR Indian Railways Jatropha Jatropha curcas L. KCl potassium chloride LCA life cycle assessment LCI life cycle inventory LCIA life cycle impact assessment MSRTH...

470

Working fluid design for organic rankine cycle systems (ORC):.  

E-Print Network (OSTI)

??The Organic Rankine Cycle is an energy conversion cycle similar to the conventional Rankine cycle which runs on a working fluid other than water. The (more)

Hattiangadi, A.

2013-01-01T23:59:59.000Z

471

Working Fluid Design for Organic Rankine Cycle (ORC) Systems:.  

E-Print Network (OSTI)

??The Organic Rankine Cycle is an energy conversion cycle similar to the conventional Rankine cycle which runs on a working fluid other than water. The (more)

Hattiangadi, A.

2013-01-01T23:59:59.000Z

472

Advanced Fuel Cycle Economic Sensitivity Analysis  

SciTech Connect

A fuel cycle economic analysis was performed on four fuel cycles to provide a baseline for initial cost comparison using the Gen IV Economic Modeling Work Group G4 ECON spreadsheet model, Decision Programming Language software, the 2006 Advanced Fuel Cycle Cost Basis report, industry cost data, international papers, the nuclear power related cost study from MIT, Harvard, and the University of Chicago. The analysis developed and compared the fuel cycle cost component of the total cost of energy for a wide range of fuel cycles including: once through, thermal with fast recycle, continuous fast recycle, and thermal recycle.

David Shropshire; Kent Williams; J.D. Smith; Brent Boore

2006-12-01T23:59:59.000Z

473

MHD Integrated Topping Cycle Project  

SciTech Connect

This eighteenth quarterly technical progress report of the MHD Integrated Topping cycle Project presents the accomplishments during the period November 1, 1991 to January 31, 1992. The precombustor is fully assembled. Manufacturing of all slagging stage components has been completed. All cooling panels were welded in place and the panel/shell gap was filled with RTV. Final combustor assembly is in progress. The low pressure cooling subsystem (LPCS) was delivered to the CDIF. Second stage brazing issues were resolved. The construction of the two anode power cabinets was completed.

Not Available

1992-07-01T23:59:59.000Z

474

Working fluids for rankine cycle  

SciTech Connect

This patent describes a method for converting thermal energy into mechanical energy through the utilization of a cycle consisting of: (1) vaporizing, with heating, a mixture selected from the group of (a) 60 to 95% by weight of chlorodifluoromethane and 5 to 40% by weight of difluoroethane; and (b) 3 to 40% by weight of chlorodifluoromethane and 60 to 97% by weight of dichlorotetrafluoroethane; (2) expanding the vapor in an expansion device to produce mechanical energy; and (3) compressing the vapor by a pump and cooling the vapor to condense the vapor.

Enjo, N.; Aomi, H.; Noguchi, M.; Ide, S.

1986-01-07T23:59:59.000Z

475

Rankine cycle system and method  

DOE Patents (OSTI)

A Rankine cycle waste heat recovery system uses a receiver with a maximum liquid working fluid level lower than the minimum liquid working fluid level of a sub-cooler of the waste heat recovery system. The receiver may have a position that is physically lower than the sub-cooler's position. A valve controls transfer of fluid between several of the components in the waste heat recovery system, especially from the receiver to the sub-cooler. The system may also have an associated control module.

Ernst, Timothy C.; Nelson, Christopher R.

2014-09-09T23:59:59.000Z

476

An introduction to the Kalina cycle  

SciTech Connect

This paper is intended as a primer on the Kalina cycle--a novel, efficient power cycle that uses an ammonia-water mixture as the working fluid. The reader needs no more than a basic understanding of conventional water based Rankine cycle power plants to comprehend the basic thermodynamics, principles and arrangements of Kalina cycle power plants presented in this paper. The Kalina cycle is principally a modified Rankine cycle. The transformation starts with an important process change to the Rankine cycle--changing the working fluid in the cycle from a pure component (typically water) to a mixture of ammonia and water. The modifications that complete the transformation of the cycle from Rankine to Kalina consist of proprietary system designs that specifically exploit the virtues of the ammonia-water working fluid. These special designs, either applied individually or integrated together in a number of different combinations, comprise a family of unique Kalina cycle systems. This is somewhat analogous to the Rankine cycle which, in fact, has many design options such as reheat, regenerative heating, supercritical pressure, dual pressure, etc. all of which can be applied in a number of different combinations in a particular plant.

Micak, H.A.

1996-12-31T23:59:59.000Z

477

Fuel Cycle CrossCut Group  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

CrossCut Group CrossCut Group 1 NERAC Briefing: Assessment of Dose of Closed vs Open Gen-IV Fuel Cycles David Wade NERAC Meeting September 30, 2002 Fuel Cycle CrossCut Group 2 Public Dose and Worker Dose Comparison of Open vs Closed Fuel Cycles * Gen-IV fuel cycle options are meant to address all stated Gen-IV Goals - Dose to workers and to the public is one of the numerous elements to be evaluated by Gen-IV R&D - The Fuel Cycle Crosscut Group was assigned to take an early look at dose implication tradeoffs of open and closed fuel cycles * FCCG Interpretation of Assignment: - Collect already-existing evaluations and prepare a briefing on what is currently known Fuel Cycle CrossCut Group 3 Approach * Look at Actual Historical Doses Based on Operational Experience - Data compiled by the United Nations Scientific Committee on the Effects of Atomic

478

VISION: Verifiable Fuel Cycle Simulation Model  

SciTech Connect

The nuclear fuel cycle is a very complex system that includes considerable dynamic complexity as well as detail complexity. In the nuclear power realm, there are experts and considerable research and development in nuclear fuel development, separations technology, reactor physics and waste management. What is lacking is an overall understanding of the entire nuclear fuel cycle and how the deployment of new fuel cycle technologies affects the overall performance of the fuel cycle. The Advanced Fuel Cycle Initiatives systems analysis group is developing a dynamic simulation model, VISION, to capture the relationships, timing and delays in and among the fuel cycle components to help develop an understanding of how the overall fuel cycle works and can transition as technologies are changed. This paper is an overview of the philosophy and development strategy behind VISION. The paper includes some descriptions of the model and some examples of how to use VISION.

Jacob J. Jacobson; Abdellatif M. Yacout; Gretchen E. Matthern; Steven J. Piet; David E. Shropshire

2009-04-01T23:59:59.000Z

479

Definition: Brayton cycle | Open Energy Information  

Open Energy Info (EERE)

form form View source History View New Pages Recent Changes All Special Pages Semantic Search/Querying Get Involved Help Apps Datasets Community Login | Sign Up Search Definition Edit with form History Facebook icon Twitter icon » Definition: Brayton cycle Jump to: navigation, search Dictionary.png Brayton cycle A thermodynamic cycle using constant pressure, heat addition and rejection. Fuel and a compressor are used to heat and increase the pressure of a gas; the gas expands and spins the blades of a turbine, which, when connected to a generator, generates electricity.[1][2] View on Wikipedia Wikipedia Definition The Brayton cycle is a thermodynamic cycle that describes the workings of a constant pressure heat engine. Gas turbine engines and airbreathing jet engines use the Brayton Cycle. Although the Brayton cycle

480

Fuel Cycle Research and Development Program  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Development Program Presentation to Office of Environmental Management Tank Waste Corporate Board James C. Bresee, ScD, JD Advisory Board Member Office of Nuclear Energy July 29, 2009 July 29, 2009 Fuel Cycle Research and Development DM 195665 2 Outline Fuel Cycle R&D Mission Changes from the Former Advanced Fuel Cycle Initiative The Science-Based Approach Key Collaborators Budget History Program Elements Summary July 29, 2009 Fuel Cycle Research and Development DM 195665 3 Fuel Cycle R&D Mission The mission of Fuel Cycle Research and Development is to develop options to current fuel cycle management strategy to enable the safe, secure, economic, and sustainable expansion of nuclear energy while reducing proliferation risks by conducting

Note: This page contains sample records for the topic "beamlines 6-month cycle" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


481

MHD Integrated Topping Cycle Project  

SciTech Connect

The overall objective of the project is to design and construct prototypical hardware for an integrated MHD topping cycle, and conduct long duration proof-of-concept tests of integrated system at the US DOE Component Development and Integration Facility in Butte, Montana. The results of the long duration tests will augment the existing engineering design data base on MHD power train reliability, availability, maintainability, and performance, and will serve as a basis for scaling up the topping cycle design to the next level of development, an early commercial scale power plant retrofit. The components of the MHD power train to be designed, fabricated, and tested include: A slagging coal combustor with a rated capacity of 50 MW thermal input, capable of operation with an Eastern (Illinois {number sign}6) or Western (Montana Rosebud) coal, a segmented supersonic nozzle, a supersonic MHD channel capable of generating at least 1.5 MW of electrical power, a segmented supersonic diffuser section to interface the channel with existing facility quench and exhaust systems, a complete set of current control circuits for local diagonal current control along the channel, and a set of current consolidation circuits to interface the channel with the existing facility inverter.

Not Available

1992-01-01T23:59:59.000Z

482

MHD Integrated Topping Cycle Project  

SciTech Connect

The Magnetohydrodynamics (MHD) Integrated Topping Cycle (ITC) Project represents the culmination of the proof-of-concept (POC) development stage in the US Department of Energy (DOE) program to advance MHD technology to early commercial development stage utility power applications. The project is a joint effort, combining the skills of three topping cycle component developers: TRW, Avco/TDS, and Westinghouse. TRW, the prime contractor and system integrator, is responsible for the 50 thermal megawatt (50 MW{sub t}) slagging coal combustion subsystem. Avco/TDS is responsible for the MHD channel subsystem (nozzle, channel, diffuser, and power conditioning circuits), and Westinghouse is responsible for the current consolidation subsystem. The ITC Project will advance the state-of-the-art in MHD power systems with the design, construction, and integrated testing of 50 MW{sub t} power train components which are prototypical of the equipment that will be used in an early commercial scale MHD utility retrofit. Long duration testing of the integrated power train at the Component Development and Integration Facility (CDIF) in Butte, Montana will be performed, so that by the early 1990's, an engineering data base on the reliability, availability, maintainability and performance of the system will be available to allow scaleup of the prototypical designs to the next development level. This Sixteenth Quarterly Technical Progress Report covers the period May 1, 1991 to July 31, 1991.

Not Available

1992-03-01T23:59:59.000Z

483

The Seasonal Cycle over the United States and Mexico  

Science Journals Connector (OSTI)

The annual cycle occupies a unique position in the spectra of meteorological time series. This cycle and its first three harmonics are extracted from the series as a seasonal cycle. The distributions of the annual and seasonal cycles are studied ...

Vernon E. Kousky; S. Srivatsangam

1983-01-01T23:59:59.000Z

484

MHD Integrated Topping Cycle Project  

SciTech Connect

This seventeenth quarterly technical progress report of the MHD Integrated Topping Cycle Project presents the accomplishments during the period August 1, 1991 to October 31, 1991. Manufacturing of the prototypical combustor pressure shell has been completed including leak, proof, and assembly fit checking. Manufacturing of forty-five cooling panels was also completed including leak, proof, and flow testing. All precombustor internal components (combustion can baffle and swirl box) were received and checked, and integration of the components was initiated. A decision was made regarding the primary and backup designs for the 1A4 channel. The assembly of the channel related prototypical hardware continued. The cathode wall electrical wiring is now complete. The mechanical design of the diffuser has been completed.

Not Available

1992-07-01T23:59:59.000Z

485

Efficiency combined cycle power plant  

SciTech Connect

This patent describes a method of operating a combined cycle power plant. It comprises: flowing exhaust gas from a combustion turbine through a heat recovery steam generator (HRSG); flowing feed water through an economizer section of the HRSG at a flow rate and providing heated feed water; flowing a first portion of the heated feed water through an evaporator section of the HRSG and producing saturated steam at a production rate, the flow rate of the feed water through the economizer section being greater than required to sustain the production rate of steam in the evaporator section; flowing fuel for the turbine through a heat exchanger; and, flowing a second portion of the heated feed water provided by the economizer section through the heat exchanger then to an inlet of the economizer section, thereby heating the fuel flowing through the heat exchanger.

Pavel, J.; Meyers, G.A.; Baldwin, T.S.

1990-06-12T23:59:59.000Z

486

2D representation of life cycle greenhouse gas emission and life cycle cost of energy conversion for various energy resources  

Science Journals Connector (OSTI)

We suggest a 2D-plot representation combined with life cycle greenhouse gas (GHG) emissions and life cycle cost for various energy conversion technologies. In general, life cycle ... use life cycle GHG emissions ...

Heetae Kim; Claudio Tenreiro; Tae Kyu Ahn

2013-10-01T23:59:59.000Z

487

Nuclear Fuel Cycle | Department of Energy  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Cycle Cycle Nuclear Fuel Cycle This is an illustration of a nuclear fuel cycle that shows the required steps to process natural uranium from ore for preparation for fuel to be loaded in nuclear reactors. This is an illustration of a nuclear fuel cycle that shows the required steps to process natural uranium from ore for preparation for fuel to be loaded in nuclear reactors. The mission of NE-54 is primarily focused on activities related to the front end of the nuclear fuel cycle which includes mining, milling, conversion, and enrichment. Uranium Mining Both "conventional" open pit, underground mining, and in situ techniques are used to recover uranium ore. In general, open pit mining is used where deposits are close to the surface and underground mining is used

488

NREL: Energy Analysis - Life Cycle Assessment Harmonization  

NLE Websites -- All DOE Office Websites (Extended Search)

Life Cycle Assessment Harmonization Life Cycle Assessment Harmonization Life Cycle Greenhouse Gas Emissions from Electricity Generation (Fact Sheet) Cover of the Life Cycle Greenhouse Gas Emissions from Electricity Generation factsheet Download the Fact Sheet The U.S. Department of Energy enlisted NREL to review and "harmonize" life cycle assessments (LCA) of electricity generation technologies. Hundreds of assessments have been published, often with considerable variability in results. These variations in approach, while usually legitimate, hamper comparison across studies and pooling of published results. Learn more about life cycle assessments of energy technologies. By harmonizing this data, NREL seeks to reduce the uncertainty around estimates for environmental impacts of renewables and increase the value of

489

Definition: Thermodynamic cycle | Open Energy Information  

Open Energy Info (EERE)

Thermodynamic cycle Thermodynamic cycle Jump to: navigation, search Dictionary.png Thermodynamic cycle A process in which a fluid (water, air, ammonia, etc) successively changes state (from a liquid to a gas and back to a liquid) for the purpose of producing or transferring energy.[1] View on Wikipedia Wikipedia Definition A thermodynamic