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1

b144.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

00) 00) 3/2 + I (J P ) = 1 2 ( 3 2 + ) Status: ∗∗∗ The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. N(1900) BREIT-WIGNER MASS N(1900) BREIT-WIGNER MASS N(1900) BREIT-WIGNER MASS N(1900) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 1900 OUR ESTIMATE ≈ 1900 OUR ESTIMATE ≈ 1900 OUR ESTIMATE ≈ 1900 OUR ESTIMATE 1905± 30 ANISOVICH 12A DPWA Multichannel 1915± 60 NIKONOV 08 DPWA Multichannel * * * We do not use the following data for averages, fits, limits, etc. * * * 1900± 8 SHRESTHA 12A DPWA Multichannel 1951± 53 PENNER 02C DPWA Multichannel 1879± 17 MANLEY 92 IPWA π N → π N & N π π N(1900) BREIT-WIGNER WIDTH N(1900) BREIT-WIGNER WIDTH N(1900) BREIT-WIGNER WIDTH N(1900) BREIT-WIGNER WIDTH VALUE (MeV) DOCUMENT ID TECN COMMENT ∼ 250 OUR ESTIMATE ∼ 250 OUR ESTIMATE ∼ 250 OUR ESTIMATE ∼ 250 OUR ESTIMATE 250 + 120 - 50 ANISOVICH 12A DPWA Multichannel

2

b087.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

80) 80) 1/2 + I (J P ) = 1 2 ( 1 2 + ) Status: ∗∗ OMITTED FROM SUMMARY TABLE N(1880) BREIT-WIGNER MASS N(1880) BREIT-WIGNER MASS N(1880) BREIT-WIGNER MASS N(1880) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1870± 35 ANISOVICH 12A DPWA Multichannel * * * We do not use the following data for averages, fits, limits, etc. * * * 1900± 36 SHRESTHA 12A DPWA Multichannel 1885± 30 MANLEY 92 IPWA π N → π N & N π π N(1880) BREIT-WIGNER WIDTH N(1880) BREIT-WIGNER WIDTH N(1880) BREIT-WIGNER WIDTH N(1880) BREIT-WIGNER WIDTH VALUE (MeV) DOCUMENT ID TECN COMMENT 235± 65 ANISOVICH 12A DPWA Multichannel * * * We do not use the following data for averages, fits, limits, etc. * * * 485± 142 SHRESTHA 12A DPWA Multichannel 113± 44 MANLEY 92 IPWA π N → π N & N π π N(1880) POLE POSITION N(1880) POLE POSITION N(1880) POLE POSITION N(1880) POLE POSITION REAL PART REAL PART REAL PART REAL PART

3

b087.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

7 7 N(1880) 1/2 + I (J P ) = 1 2 ( 1 2 + ) Status: ∗∗ OMITTED FROM SUMMARY TABLE N(1880) BREIT-WIGNER MASS N(1880) BREIT-WIGNER MASS N(1880) BREIT-WIGNER MASS N(1880) BREIT-WIGNER MASS NODE=B087M NODE=B087M VALUE (MeV) DOCUMENT ID TECN COMMENT 1870 ± 35 ANISOVICH 12A DPWA Multichannel * * * We do not use the following data for averages, fits, limits, etc. * * * 1900 ± 36 SHRESTHA 12A DPWA Multichannel 1885 ± 30 MANLEY 92 IPWA π N → π N & N π π N(1880) BREIT-WIGNER WIDTH N(1880) BREIT-WIGNER WIDTH N(1880) BREIT-WIGNER WIDTH N(1880) BREIT-WIGNER WIDTH NODE=B087W NODE=B087W VALUE (MeV) DOCUMENT ID TECN COMMENT 235 ± 65 ANISOVICH 12A DPWA Multichannel * * * We do not use the following data for averages, fits, limits, etc. * * * 485 ± 142 SHRESTHA 12A DPWA Multichannel 113 ± 44 MANLEY 92 IPWA π N → π N & N π π N(1880) POLE POSITION N(1880) POLE POSITION N(1880) POLE POSITION N(1880)

4

b005.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

60) 60) 5/2 - I (J P ) = 1 2 ( 5 2 - ) Status: ∗∗ OMITTED FROM SUMMARY TABLE Before our 2012 Review, this state appeared in our Listings as the N(2200). The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. N(2060) BREIT-WIGNER MASS N(2060) BREIT-WIGNER MASS N(2060) BREIT-WIGNER MASS N(2060) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 2060 OUR ESTIMATE ≈ 2060 OUR ESTIMATE ≈ 2060 OUR ESTIMATE ≈ 2060 OUR ESTIMATE 2060± 15 ANISOVICH 12A DPWA Multichannel 1900 BELL 83 DPWA π - p → Λ K 0 2180± 80 CUTKOSKY 80 IPWA π N → π N 1920 SAXON 80 DPWA π - p → Λ K 0 2228± 30 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 2116± 21 SHRESTHA 12A DPWA Multichannel 2217± 27 BATINIC 10 DPWA π N → N π, N η N(2060) BREIT-WIGNER WIDTH N(2060) BREIT-WIGNER WIDTH N(2060) BREIT-WIGNER WIDTH N(2060) BREIT-WIGNER WIDTH VALUE

5

b066.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

650) 650) 1/2 - I (J P ) = 1 2 ( 1 2 - ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(1650) BREIT-WIGNER MASS N(1650) BREIT-WIGNER MASS N(1650) BREIT-WIGNER MASS N(1650) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1645 to 1670 (≈ 1655) OUR ESTIMATE 1645 to 1670 (≈ 1655) OUR ESTIMATE 1645 to 1670 (≈ 1655) OUR ESTIMATE 1645 to 1670 (≈ 1655) OUR ESTIMATE 1651 ± 6 ANISOVICH 12A DPWA Multichannel 1634.7± 1.1 ARNDT 06 DPWA π N → π N, η N 1650 ± 30 CUTKOSKY 80 IPWA π N → π N 1670 ± 8 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1664 ± 2 SHRESTHA 12A DPWA Multichannel 1680 ± 40 ANISOVICH 10 DPWA Multichannel

6

b064.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

75) 75) 5/2 - I (J P ) = 1 2 ( 5 2 - ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(1675) BREIT-WIGNER MASS N(1675) BREIT-WIGNER MASS N(1675) BREIT-WIGNER MASS N(1675) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1670 to 1680 (≈ 1675) OUR ESTIMATE 1670 to 1680 (≈ 1675) OUR ESTIMATE 1670 to 1680 (≈ 1675) OUR ESTIMATE 1670 to 1680 (≈ 1675) OUR ESTIMATE 1664 ± 5 ANISOVICH 12A DPWA Multichannel 1674.1± 0.2 ARNDT 06 DPWA π N → π N, η N 1675 ± 10 CUTKOSKY 80 IPWA π N → π N 1679 ± 8 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1679 ± 1 SHRESTHA 12A DPWA Multichannel 1678 ± 5 ANISOVICH 10 DPWA Multichannel

7

b061.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

440) 440) 1/2 + I (J P ) = 1 2 ( 1 2 + ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(1440) BREIT-WIGNER MASS N(1440) BREIT-WIGNER MASS N(1440) BREIT-WIGNER MASS N(1440) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1420 to 1470 (≈ 1440) OUR ESTIMATE 1420 to 1470 (≈ 1440) OUR ESTIMATE 1420 to 1470 (≈ 1440) OUR ESTIMATE 1420 to 1470 (≈ 1440) OUR ESTIMATE 1430 ± 8 ANISOVICH 12A DPWA Multichannel 1485.0± 1.2 ARNDT 06 DPWA π N → π N, η N 1440 ± 30 CUTKOSKY 80 IPWA π N → π N 1410 ± 12 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1412 ± 2 SHRESTHA 12A DPWA Multichannel 1440 ± 12 ANISOVICH 10 DPWA Multichannel

8

b063.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

535) 535) 1/2 - I (J P ) = 1 2 ( 1 2 - ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(1535) BREIT-WIGNER MASS N(1535) BREIT-WIGNER MASS N(1535) BREIT-WIGNER MASS N(1535) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1525 to 1545 (≈ 1535) OUR ESTIMATE 1525 to 1545 (≈ 1535) OUR ESTIMATE 1525 to 1545 (≈ 1535) OUR ESTIMATE 1525 to 1545 (≈ 1535) OUR ESTIMATE 1519 ± 5 ANISOVICH 12A DPWA Multichannel 1547.0± 0.7 ARNDT 06 DPWA π N → π N, η N 1550 ± 40 CUTKOSKY 80 IPWA π N → π N 1526 ± 7 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1538 ± 1 SHRESTHA 12A DPWA Multichannel 1535 ± 20 ANISOVICH 10 DPWA Multichannel

9

Multi-channel polarized thermal emitter  

DOE Patents [OSTI]

A multi-channel polarized thermal emitter (PTE) is presented. The multi-channel PTE can emit polarized thermal radiation without using a polarizer at normal emergence. The multi-channel PTE consists of two layers of metallic gratings on a monolithic and homogeneous metallic plate. It can be fabricated by a low-cost soft lithography technique called two-polymer microtransfer molding. The spectral positions of the mid-infrared (MIR) radiation peaks can be tuned by changing the periodicity of the gratings and the spectral separation between peaks are tuned by changing the mutual angle between the orientations of the two gratings.

Lee, Jae-Hwang; Ho, Kai-Ming; Constant, Kristen P

2013-07-16T23:59:59.000Z

10

Spectroscopy with Multichannel Correlation Radiometers  

E-Print Network [OSTI]

Correlation radiometers make true differential measurements in power with high accuracy and small systematic errors. This receiver architecture has been used in radio astronomy for measurements of continuum radiation for over 50 years; this article examines spectroscopy over broad bandwidths using correlation techniques. After general discussions of correlation and the choice of hybrid phase, experimental results from tests with a simple laboratory multi-channel correlation radiometer are shown. Analysis of the effect of the input hybrid's phase shows that a 90 degree hybrid is likely to be the best general choice for radio astronomy, depending on its amplitude match and phase flatness with frequency. The laboratory results verify that the combination of the correlation architecture and an analog lag correlator is an excellent method for spectroscopy over very wide bandwidths.

A. I. Harris

2005-04-20T23:59:59.000Z

11

b015.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

20) 20) 3/2 + I (J P ) = 1 2 ( 3 2 + ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(1720) BREIT-WIGNER MASS N(1720) BREIT-WIGNER MASS N(1720) BREIT-WIGNER MASS N(1720) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1700 to 1750 (≈ 1720) OUR ESTIMATE 1700 to 1750 (≈ 1720) OUR ESTIMATE 1700 to 1750 (≈ 1720) OUR ESTIMATE 1700 to 1750 (≈ 1720) OUR ESTIMATE 1690 + 70 - 35 ANISOVICH 12A DPWA Multichannel 1763.8± 4.6 ARNDT 06 DPWA π N → π N, η N 1700 ± 50 CUTKOSKY 80 IPWA π N → π N 1710 ± 20 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1720 ± 5 SHRESTHA 12A DPWA Multichannel 1770 ± 100 ANISOVICH 10 DPWA

12

b012.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

10) 10) 1/2 + I (J P ) = 3 2 ( 1 2 + ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). ∆(1910) BREIT-WIGNER MASS ∆(1910) BREIT-WIGNER MASS ∆(1910) BREIT-WIGNER MASS ∆(1910) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1860 to 1910 (≈ 1890) OUR ESTIMATE 1860 to 1910 (≈ 1890) OUR ESTIMATE 1860 to 1910 (≈ 1890) OUR ESTIMATE 1860 to 1910 (≈ 1890) OUR ESTIMATE 1860 ± 40 ANISOVICH 12A DPWA Multichannel 2067.9± 1.7 ARNDT 06 DPWA π N → π N, η N 1910 ± 40 CUTKOSKY 80 IPWA π N → π N 1888 ± 20 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1934 ± 5 SHRESTHA 12A DPWA Multichannel 1995 ± 12 VRANA 00 DPWA

13

Multi-channel coded-aperture photography  

E-Print Network [OSTI]

This thesis describes the multi-channel coded-aperture photography, a modified camera system that can extract an all-focus image of the scene along with a depth estimate over the scene. The modification consists of inserting ...

Baek, Jongmin

2008-01-01T23:59:59.000Z

14

Multichannel framework for singular quantum mechanics  

SciTech Connect (OSTI)

A multichannel S-matrix framework for singular quantum mechanics (SQM) subsumes the renormalization and self-adjoint extension methods and resolves its boundary-condition ambiguities. In addition to the standard channel accessible to a distant (asymptotic) observer, one supplementary channel opens up at each coordinate singularity, where local outgoing and ingoing singularity waves coexist. The channels are linked by a fully unitary S-matrix, which governs all possible scenarios, including cases with an apparent nonunitary behavior as viewed from asymptotic distances. -- Highlights: A multichannel framework is proposed for singular quantum mechanics and analogues. The framework unifies several established approaches for singular potentials. Singular points are treated as new scattering channels. Nonunitary asymptotic behavior is subsumed in a unitary multichannel S-matrix. Conformal quantum mechanics and the inverse quartic potential are highlighted.

Camblong, Horacio E., E-mail: camblong@usfca.edu [Department of Physics and Astronomy, University of San Francisco, San Francisco, CA 94117-1080 (United States); Epele, Luis N., E-mail: epele@fisica.unlp.edu.ar [Laboratorio de Fsica Terica, Departamento de Fsica, IFLP, CONICET, Facultad de Ciencias Exactas, Universidad Nacional de La Plata, C.C. 671900 La Plata (Argentina); Fanchiotti, Huner, E-mail: huner@fisica.unlp.edu.ar [Laboratorio de Fsica Terica, Departamento de Fsica, IFLP, CONICET, Facultad de Ciencias Exactas, Universidad Nacional de La Plata, C.C. 671900 La Plata (Argentina)] [Laboratorio de Fsica Terica, Departamento de Fsica, IFLP, CONICET, Facultad de Ciencias Exactas, Universidad Nacional de La Plata, C.C. 671900 La Plata (Argentina); Garca Canal, Carlos A., E-mail: garcia@fisica.unlp.edu.ar [Laboratorio de Fsica Terica, Departamento de Fsica, IFLP, CONICET, Facultad de Ciencias Exactas, Universidad Nacional de La Plata, C.C. 671900 La Plata (Argentina); Ordez, Carlos R., E-mail: ordonez@uh.edu [Department of Physics, University of Houston, Houston, TX 77204-5506 (United States)

2014-01-15T23:59:59.000Z

15

Multichannel photodiode detector for ultrafast optical spectroscopy  

E-Print Network [OSTI]

Construction and characterization of a multichannel photodiode detector based on commercially available components with high signal to noise of $\\sim10^{6}$ and a rapid frame rate, suitable for time resolved femtosecond spectroscopy with high repetition femtosecond sources, is presented.

Mertelj, T; Borzda, T; Vaskivskyi, I; Pogrebna, A; Mihailovic, D

2014-01-01T23:59:59.000Z

16

b139.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

9 9 ∆(2000) 5/2 + I (J P ) = 3 2 ( 5 2 + ) Status: ∗∗ OMITTED FROM SUMMARY TABLE The latest GWU analysis (ARNDT 06) finds no evidence for this NODE=B139 resonance. ∆(2000) BREIT-WIGNER MASS ∆(2000) BREIT-WIGNER MASS ∆(2000) BREIT-WIGNER MASS ∆(2000) BREIT-WIGNER MASS NODE=B139M NODE=B139M VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 2000 OUR ESTIMATE ≈ 2000 OUR ESTIMATE ≈ 2000 OUR ESTIMATE ≈ 2000 OUR ESTIMATE → UNCHECKED ← 1724 ± 61 VRANA 00 DPWA Multichannel OCCUR=2 2200 ± 125 CUTKOSKY 80 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 2015 ± 24 SHRESTHA 12A DPWA Multichannel 1752 ± 32 MANLEY 92 IPWA π N → π N & N π π ∆(2000) BREIT-WIGNER WIDTH ∆(2000) BREIT-WIGNER WIDTH ∆(2000) BREIT-WIGNER WIDTH ∆(2000) BREIT-WIGNER WIDTH NODE=B139W NODE=B139W VALUE (MeV) DOCUMENT ID TECN COMMENT 138 ± 68 VRANA 00 DPWA Multichannel

17

b009.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

60) 60) 5/2 + I (J P ) = 1 2 ( 5 2 + ) Status: ∗∗ OMITTED FROM SUMMARY TABLE Before the 2012 Review, all the evidence for a J P = 5/2 + state with a mass above 1800 MeV was filed under a two-star N(2000). There is now some evidence from ANISOVICH 12A for two 5/2 + states in this region, so we have split the older data (according to mass) between two two-star 5/2 + states, an N(1860) and an N(2000). N(1860) BREIT-WIGNER MASS N(1860) BREIT-WIGNER MASS N(1860) BREIT-WIGNER MASS N(1860) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1820 to 1960 (≈ 1860) OUR ESTIMATE 1820 to 1960 (≈ 1860) OUR ESTIMATE 1820 to 1960 (≈ 1860) OUR ESTIMATE 1820 to 1960 (≈ 1860) OUR ESTIMATE 1860 + 120 - 60 ANISOVICH 12A DPWA Multichannel 1817.7 ARNDT 06 DPWA π N → π N, η N 1882 ± 10 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1900 ± 7 SHRESTHA 12A DPWA Multichannel

18

b113.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

50) 50) 9/2 - I (J P ) = 1 2 ( 9 2 - ) Status: ∗∗∗∗ Some obsolete results published before 1980 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(2250) BREIT-WIGNER MASS N(2250) BREIT-WIGNER MASS N(2250) BREIT-WIGNER MASS N(2250) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 2200 to 2350 (≈ 2275) OUR ESTIMATE 2200 to 2350 (≈ 2275) OUR ESTIMATE 2200 to 2350 (≈ 2275) OUR ESTIMATE 2200 to 2350 (≈ 2275) OUR ESTIMATE 2280± 40 ANISOVICH 12A DPWA Multichannel 2302± 6 ARNDT 06 DPWA π N → π N, η N 2250± 80 CUTKOSKY 80 IPWA π N → π N 2268± 15 HOEHLER 79 IPWA π N → π N 2200± 100 HENDRY 78 MPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 2376± 43 ARNDT 04 DPWA π N → π N, η N 2291 ARNDT 95 DPWA π N → N π N(2250) BREIT-WIGNER WIDTH N(2250) BREIT-WIGNER WIDTH N(2250) BREIT-WIGNER WIDTH N(2250) BREIT-WIGNER

19

b113.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

3 3 N(2250) 9/2 - I (J P ) = 1 2 ( 9 2 - ) Status: ∗∗∗∗ Some obsolete results published before 1980 were last included in NODE=B113 our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(2250) BREIT-WIGNER MASS N(2250) BREIT-WIGNER MASS N(2250) BREIT-WIGNER MASS N(2250) BREIT-WIGNER MASS NODE=B113M NODE=B113M VALUE (MeV) DOCUMENT ID TECN COMMENT 2200 to 2350 (≈ 2275) OUR ESTIMATE 2200 to 2350 (≈ 2275) OUR ESTIMATE 2200 to 2350 (≈ 2275) OUR ESTIMATE 2200 to 2350 (≈ 2275) OUR ESTIMATE → UNCHECKED ← 2280 ± 40 ANISOVICH 12A DPWA Multichannel 2302 ± 6 ARNDT 06 DPWA π N → π N, η N 2250 ± 80 CUTKOSKY 80 IPWA π N → π N 2268 ± 15 HOEHLER 79 IPWA π N → π N 2200 ± 100 HENDRY 78 MPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 2376 ± 43 ARNDT 04 DPWA π N → π N, η N 2291 ARNDT 95 DPWA π N → N π N(2250) BREIT-WIGNER WIDTH N(2250) BREIT-WIGNER

20

Multichannel Scheduling and Its Connection to Queueing Network Control Problem  

E-Print Network [OSTI]

Multichannel Scheduling and Its Connection to Queueing Network Control Problem Pouya Tehrani , Qing scheduling problem and a closed queueing network control problem which is known to be EXP-complete, we obtain {potehrani,qzhao}@ucdavis.edu Abstract--We consider the multichannel scheduling problem where the data rate

Islam, M. Saif

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

b011.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

5) 5) 5/2 + I (J P ) = 3 2 ( 5 2 + ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). ∆(1905) BREIT-WIGNER MASS ∆(1905) BREIT-WIGNER MASS ∆(1905) BREIT-WIGNER MASS ∆(1905) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1855 to 1910 (≈ 1880) OUR ESTIMATE 1855 to 1910 (≈ 1880) OUR ESTIMATE 1855 to 1910 (≈ 1880) OUR ESTIMATE 1855 to 1910 (≈ 1880) OUR ESTIMATE 1861 ± 6 ANISOVICH 12A DPWA Multichannel 1857.8± 1.6 ARNDT 06 DPWA π N → π N, η N 1910 ± 30 CUTKOSKY 80 IPWA π N → π N 1905 ± 20 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1818 ± 8 SHRESTHA 12A DPWA Multichannel 1890 ± 25 1 ANISOVICH 10

22

b071.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

90) 90) 7/2 - I (J P ) = 1 2 ( 7 2 - ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(2190) BREIT-WIGNER MASS N(2190) BREIT-WIGNER MASS N(2190) BREIT-WIGNER MASS N(2190) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 2100 to 2200 (≈ 2190) OUR ESTIMATE 2100 to 2200 (≈ 2190) OUR ESTIMATE 2100 to 2200 (≈ 2190) OUR ESTIMATE 2100 to 2200 (≈ 2190) OUR ESTIMATE 2180 ± 20 ANISOVICH 12A DPWA Multichannel 2152.4± 1.4 ARNDT 06 DPWA π N → π N, η N 2200 ± 70 CUTKOSKY 80 IPWA π N → π N 2140 ± 12 HOEHLER 79 IPWA π N → π N 2140 ± 40 HENDRY 78 MPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 2150 ± 26 SHRESTHA 12A DPWA Multichannel

23

Multichannel image regularization using anisotropic geodesic filtering  

SciTech Connect (OSTI)

This paper extends a recent image-dependent regularization approach introduced in aiming at edge-preserving smoothing. For that purpose, geodesic distances equipped with a Riemannian metric need to be estimated in local neighbourhoods. By deriving an appropriate metric from the gradient structure tensor, the associated geodesic paths are constrained to follow salient features in images. Following, we design a generalized anisotropic geodesic filter; incorporating not only a measure of the edge strength, like in the original method, but also further directional information about the image structures. The proposed filter is particularly efficient at smoothing heterogeneous areas while preserving relevant structures in multichannel images.

Grazzini, Jacopo A [Los Alamos National Laboratory

2010-01-01T23:59:59.000Z

24

b040.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

70) 70) 1/2 - I (J P ) = 0( 1 2 - ) Status: ∗∗∗∗ The measurements of the mass, width, and elasticity published be- fore 1974 are now obsolete and have been omitted. They were last listed in our 1982 edition Physics Letters 111B 111B 111B 111B 1 (1982). Λ(1670) MASS Λ(1670) MASS Λ(1670) MASS Λ(1670) MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1660 to 1680 (≈ 1670) OUR ESTIMATE 1660 to 1680 (≈ 1670) OUR ESTIMATE 1660 to 1680 (≈ 1670) OUR ESTIMATE 1660 to 1680 (≈ 1670) OUR ESTIMATE 1677.5± 0.8 1 GARCIA-REC...03 DPWA K N multichannel 1673 ± 2 MANLEY 02 DPWA K N multichannel 1670.8± 1.7 KOISO 85 DPWA K - p → Σ π 1667 ± 5 GOPAL 80 DPWA K N → K N 1671 ± 3 ALSTON-... 78 DPWA K N → K N 1670 ± 5 GOPAL 77 DPWA K N multichannel 1675 ± 2 HEPP 76B DPWA K - N → Σ π 1679 ± 1 KANE 74 DPWA K - p → Σ π 1665 ± 5 PREVOST 74 DPWA K - N → Σ (1385) π * * * We do not use the following data for averages, fits, limits, etc.

25

b040.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

0 0 Λ(1670) 1/2 - I (J P ) = 0( 1 2 - ) Status: ∗∗∗∗ The measurements of the mass, width, and elasticity published be- NODE=B040 fore 1974 are now obsolete and have been omitted. They were last listed in our 1982 edition Physics Letters 111B 111B 111B 111B 1 (1982). Λ(1670) MASS Λ(1670) MASS Λ(1670) MASS Λ(1670) MASS NODE=B040M NODE=B040M VALUE (MeV) DOCUMENT ID TECN COMMENT 1660 to 1680 (≈ 1670) OUR ESTIMATE 1660 to 1680 (≈ 1670) OUR ESTIMATE 1660 to 1680 (≈ 1670) OUR ESTIMATE 1660 to 1680 (≈ 1670) OUR ESTIMATE → UNCHECKED ← 1677.5 ± 0.8 1 GARCIA-REC...03 DPWA K N multichannel 1673 ± 2 MANLEY 02 DPWA K N multichannel 1670.8 ± 1.7 KOISO 85 DPWA K - p → Σ π 1667 ± 5 GOPAL 80 DPWA K N → K N 1671 ± 3 ALSTON-... 78 DPWA K N → K N 1670 ± 5 GOPAL 77 DPWA K N multichannel 1675 ± 2 HEPP 76B DPWA K - N → Σ π 1679 ± 1 KANE 74 DPWA K - p → Σ π 1665 ± 5 PREVOST 74 DPWA K - N → Σ (1385) π * * * We do

26

The role of the mobile medium in multichannel CRM communication  

Science Journals Connector (OSTI)

Research concerning the multichannel environment in different industries and contexts is increasing. However, the majority of studies fail to acknowledge the different characteristics of each individual channel. Therefore, this study takes a closer look at the mobile medium within the multichannel environment in CRM. More specifically, the purpose of this study is to examine the role of the mobile medium among other channels within multichannel CRM communication. Based on the purpose of the study, this research builds on an empirical single-case study in the airline industry. The findings of the study indicate that the mobile medium has an important, albeit complementary, role within multichannel CRM communication. The role is enhanced when the company takes into account the phase of the customer relationship and, moreover, the customers' travelling process.

Jaakko Sinisalo

2011-01-01T23:59:59.000Z

27

Multi-channel blind system identification for central hemodynamic monitoring  

E-Print Network [OSTI]

Multi-channel Blind System Identification (MBSI) is a technique for estimating both an unknown input and unknown channel dynamics from simultaneous output measurements at different channels through which the input signal ...

Zhang, Yi, 1973-

2002-01-01T23:59:59.000Z

28

Multichannel Audio Coding for Multimedia Services in Intelligent Environments  

E-Print Network [OSTI]

5 Multichannel Audio Coding for Multimedia Services in Intelligent Environments Athanasios Summary. Audio is an integral component of multimedia services in intelligent environments. Use of multiple channels in audio capturing and rendering offers the advantage of recreating arbitrary acoustic

Tsakalides, Panagiotis

29

b067.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

880) 880) 1/2 + I (J P ) = 1( 1 2 + ) Status: ∗∗ OMITTED FROM SUMMARY TABLE A P 11 resonance is suggested by several partial-wave analyses, but with wide variations in the mass and other parameters. We list here all claims which lie well above the P 11 Σ (1770). Σ (1880) MASS Σ (1880) MASS Σ (1880) MASS Σ (1880) MASS VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 1880 OUR ESTIMATE ≈ 1880 OUR ESTIMATE ≈ 1880 OUR ESTIMATE ≈ 1880 OUR ESTIMATE 1826± 20 GOPAL 80 DPWA K N → K N 1870± 10 CAMERON 78B DPWA K - p → N K ∗ 1847 or 1863 1 MARTIN 77 DPWA K N multichannel 1960± 30 2 BAILLON 75 IPWA K N → Λ π 1985± 50 VANHORN 75 DPWA K - p → Λ π 0 1898 3 LEA 73 DPWA Multichannel K-matrix ∼ 1850 ARMENTEROS70 IPWA K N → K N 1950± 50 BARBARO-... 70 DPWA K - N → Λ π 1920± 30 LITCHFIELD 70 DPWA K - N → Λ π 1850 BAILEY 69 DPWA K N → K N 1882± 40 SMART 68 DPWA K - N → Λ π Σ (1880) WIDTH Σ (1880) WIDTH Σ (1880) WIDTH Σ (1880)

30

b067.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

7 7 Σ (1880) 1/2 + I (J P ) = 1( 1 2 + ) Status: ∗∗ OMITTED FROM SUMMARY TABLE A P 11 resonance is suggested by several partial-wave analyses, but NODE=B067 with wide variations in the mass and other parameters. We list here all claims which lie well above the P 11 Σ (1770). Σ (1880) MASS Σ (1880) MASS Σ (1880) MASS Σ (1880) MASS NODE=B067M NODE=B067M VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 1880 OUR ESTIMATE ≈ 1880 OUR ESTIMATE ≈ 1880 OUR ESTIMATE ≈ 1880 OUR ESTIMATE → UNCHECKED ← 1826 ± 20 GOPAL 80 DPWA K N → K N 1870 ± 10 CAMERON 78B DPWA K - p → N K ∗ 1847 or 1863 1 MARTIN 77 DPWA K N multichannel 1960 ± 30 2 BAILLON 75 IPWA K N → Λ π 1985 ± 50 VANHORN 75 DPWA K - p → Λ π 0 1898 3 LEA 73 DPWA Multichannel K-matrix ∼ 1850 ARMENTEROS70 IPWA K N → K N 1950 ± 50 BARBARO-... 70 DPWA K - N → Λ π 1920 ± 30 LITCHFIELD 70 DPWA K - N → Λ π 1850 BAILEY 69 DPWA K N → K N 1882 ± 40 SMART 68 DPWA K - N → Λ

31

b016.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

16 16 N(1875) 3/2 - I (J P ) = 1 2 ( 3 2 - ) Status: ∗∗∗ Before the 2012 Review, all the evidence for a J P = 3/2 - state NODE=B016 with a mass above 1800 MeV was filed under a two-star N(2080). There is now evidence from ANISOVICH 12A for two 3/2 - states in this region, so we have split the older data (according to mass) between a three-star N(1875) and a two-star N(2120). The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. N(1875) BREIT-WIGNER MASS N(1875) BREIT-WIGNER MASS N(1875) BREIT-WIGNER MASS N(1875) BREIT-WIGNER MASS NODE=B016M NODE=B016M VALUE (MeV) DOCUMENT ID TECN COMMENT 1820 to 1920 (≈ 1875) OUR ESTIMATE 1820 to 1920 (≈ 1875) OUR ESTIMATE 1820 to 1920 (≈ 1875) OUR ESTIMATE 1820 to 1920 (≈ 1875) OUR ESTIMATE → UNCHECKED ← 1880 ± 20 ANISOVICH 12A DPWA Multichannel 1920 BELL 83 DPWA π - p → Λ K 0 1880 ± 100 1 CUTKOSKY 80 IPWA π N → π N 1900 SAXON 80 DPWA π

32

b016.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

75) 75) 3/2 - I (J P ) = 1 2 ( 3 2 - ) Status: ∗∗∗ Before the 2012 Review, all the evidence for a J P = 3/2 - state with a mass above 1800 MeV was filed under a two-star N(2080). There is now evidence from ANISOVICH 12A for two 3/2 - states in this region, so we have split the older data (according to mass) between a three-star N(1875) and a two-star N(2120). The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. N(1875) BREIT-WIGNER MASS N(1875) BREIT-WIGNER MASS N(1875) BREIT-WIGNER MASS N(1875) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1820 to 1920 (≈ 1875) OUR ESTIMATE 1820 to 1920 (≈ 1875) OUR ESTIMATE 1820 to 1920 (≈ 1875) OUR ESTIMATE 1820 to 1920 (≈ 1875) OUR ESTIMATE 1880± 20 ANISOVICH 12A DPWA Multichannel 1920 BELL 83 DPWA π - p → Λ K 0 1880± 100 1 CUTKOSKY 80 IPWA π N → π N 1900 SAXON 80 DPWA π - p → Λ K 0 * * * We do not use the following data for averages,

33

A Joint Transmission Grant Scheduling and Wavelength Assignment in Multichannel SG-EPON  

Science Journals Connector (OSTI)

In this paper, we investigate the problem of transmission grant scheduling in multichannel optical access networks using a scheduling theoretic ...

Meng, Lehan; El-Najjar, Jad; Alazemi, Hamed; Assi, Chadi

2009-01-01T23:59:59.000Z

34

b036.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

6 6 Λ(1800) 1/2 - I (J P ) = 0( 1 2 - ) Status: ∗∗∗ This is the second resonance in the S 01 wave, the first being the NODE=B036 Λ(1670). Λ(1800) MASS Λ(1800) MASS Λ(1800) MASS Λ(1800) MASS NODE=B036M NODE=B036M VALUE (MeV) DOCUMENT ID TECN COMMENT 1720 to 1850 (≈ 1800) OUR ESTIMATE 1720 to 1850 (≈ 1800) OUR ESTIMATE 1720 to 1850 (≈ 1800) OUR ESTIMATE 1720 to 1850 (≈ 1800) OUR ESTIMATE → UNCHECKED ← 1845 ± 10 MANLEY 02 DPWA K N multichannel 1841 ± 10 GOPAL 80 DPWA K N → K N 1725 ± 20 ALSTON-... 78 DPWA K N → K N 1825 ± 20 GOPAL 77 DPWA K N multichannel 1830 ± 20 LANGBEIN 72 IPWA K N multichannel * * * We do not use the following data for averages, fits, limits, etc. * * * 1767 or 1842 1 MARTIN 77 DPWA K N multichannel 1780 KIM 71 DPWA K-matrix analysis 1872 ± 10 BRICMAN 70B DPWA K N → K N Λ(1800) WIDTH Λ(1800) WIDTH Λ(1800) WIDTH Λ(1800) WIDTH NODE=B036W NODE=B036W VALUE (MeV) DOCUMENT

35

b036.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

00) 00) 1/2 - I (J P ) = 0( 1 2 - ) Status: ∗∗∗ This is the second resonance in the S 01 wave, the first being the Λ(1670). Λ(1800) MASS Λ(1800) MASS Λ(1800) MASS Λ(1800) MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1720 to 1850 (≈ 1800) OUR ESTIMATE 1720 to 1850 (≈ 1800) OUR ESTIMATE 1720 to 1850 (≈ 1800) OUR ESTIMATE 1720 to 1850 (≈ 1800) OUR ESTIMATE 1845± 10 MANLEY 02 DPWA K N multichannel 1841± 10 GOPAL 80 DPWA K N → K N 1725± 20 ALSTON-... 78 DPWA K N → K N 1825± 20 GOPAL 77 DPWA K N multichannel 1830± 20 LANGBEIN 72 IPWA K N multichannel * * * We do not use the following data for averages, fits, limits, etc. * * * 1767 or 1842 1 MARTIN 77 DPWA K N multichannel 1780 KIM 71 DPWA K-matrix analysis 1872± 10 BRICMAN 70B DPWA K N → K N Λ(1800) WIDTH Λ(1800) WIDTH Λ(1800) WIDTH Λ(1800) WIDTH VALUE (MeV) DOCUMENT ID TECN COMMENT 200 to 400 (≈ 300) OUR ESTIMATE 200 to 400 (≈ 300) OUR ESTIMATE 200

36

PECVD Silicon Carbide Waveguides for Multichannel G. Pandraud  

E-Print Network [OSTI]

PECVD Silicon Carbide Waveguides for Multichannel Sensors G. Pandraud Kavli Institute of Nano Deposition (PECVD) Silicon Carbide (SiC) waveguides. Thin SiC films have been deposited onto Si substrates with a SiO2 film acting as a cladding layer around the carbide core. In the sensor, the evanescent tale

Technische Universiteit Delft

37

Analysis of multichannel patch clamp recordings by Hidden Markov Models  

E-Print Network [OSTI]

Analysis of multichannel patch clamp recordings by Hidden Markov Models Stefan Klein Jens Timmer Conventional methods of analysis do not allow the kinetics of patch clamped ion channels to be completely determined if more than one chan­ nel is present in the patch. This hinders investigations on small ion chan

Timmer, Jens

38

INTELLIGENT SYSTEMS FOR MIXING MULTICHANNEL AUDIO Joshua D. Reiss  

E-Print Network [OSTI]

in the engineering tasks and requirements that must be addressed during the audio production process. Although't have the time, expertise or inclination to perform all the audio engineering required. Similarly, [2INTELLIGENT SYSTEMS FOR MIXING MULTICHANNEL AUDIO Joshua D. Reiss Centre for Digital Music, Queen

Reiss, Josh

39

b055.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

90) 90) 3/2 - I (J P ) = 0( 3 2 - ) Status: ∗∗∗∗ The measurements of the mass, width, and elasticity published be- fore 1974 are now obsolete and have been omitted. They were last listed in our 1982 edition Physics Letters 111B 111B 111B 111B 1 (1982). Λ(1690) MASS Λ(1690) MASS Λ(1690) MASS Λ(1690) MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1685 to 1695 (≈ 1690) OUR ESTIMATE 1685 to 1695 (≈ 1690) OUR ESTIMATE 1685 to 1695 (≈ 1690) OUR ESTIMATE 1685 to 1695 (≈ 1690) OUR ESTIMATE 1695.7± 2.6 KOISO 85 DPWA K - p → Σ π 1690 ± 5 GOPAL 80 DPWA K N → K N 1692 ± 5 ALSTON-... 78 DPWA K N → K N 1690 ± 5 GOPAL 77 DPWA K N multichannel 1690 ± 3 HEPP 76B DPWA K - N → Σ π 1689 ± 1 KANE 74 DPWA K - p → Σ π * * * We do not use the following data for averages, fits, limits, etc. * * * 1687 or 1689 1 MARTIN 77 DPWA K N multichannel 1692 ± 4 CARROLL 76 DPWA Isospin-0 total σ Λ(1690) WIDTH Λ(1690) WIDTH Λ(1690) WIDTH

40

b055.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

5 5 Λ(1690) 3/2 - I (J P ) = 0( 3 2 - ) Status: ∗∗∗∗ The measurements of the mass, width, and elasticity published be- NODE=B055 fore 1974 are now obsolete and have been omitted. They were last listed in our 1982 edition Physics Letters 111B 111B 111B 111B 1 (1982). Λ(1690) MASS Λ(1690) MASS Λ(1690) MASS Λ(1690) MASS NODE=B055M NODE=B055M VALUE (MeV) DOCUMENT ID TECN COMMENT 1685 to 1695 (≈ 1690) OUR ESTIMATE 1685 to 1695 (≈ 1690) OUR ESTIMATE 1685 to 1695 (≈ 1690) OUR ESTIMATE 1685 to 1695 (≈ 1690) OUR ESTIMATE → UNCHECKED ← 1695.7 ± 2.6 KOISO 85 DPWA K - p → Σ π 1690 ± 5 GOPAL 80 DPWA K N → K N 1692 ± 5 ALSTON-... 78 DPWA K N → K N 1690 ± 5 GOPAL 77 DPWA K N multichannel 1690 ± 3 HEPP 76B DPWA K - N → Σ π 1689 ± 1 KANE 74 DPWA K - p → Σ π * * * We do not use the following data for averages, fits, limits, etc. * * * 1687 or 1689 1 MARTIN 77 DPWA K N multichannel 1692 ± 4 CARROLL 76 DPWA Isospin-0

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41

b024.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

20) 20) 3/2 - I (J P ) = 1 2 ( 3 2 - ) Status: ∗∗ OMITTED FROM SUMMARY TABLE Before the 2012 Review, all the evidence for a J P = 3/2 - state with a mass above 1800 MeV was filed under a two-star N(2080). There is now evidence from ANISOVICH 12A for two 3/2 - states in this region, so we have split the older data (according to mass) between a three-star N(1875) and a two-star N(2120). N(2120) BREIT-WIGNER MASS N(2120) BREIT-WIGNER MASS N(2120) BREIT-WIGNER MASS N(2120) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 2120 OUR ESTIMATE 2120 OUR ESTIMATE 2120 OUR ESTIMATE 2120 OUR ESTIMATE 2150± 60 ANISOVICH 12A DPWA Multichannel 2060± 80 1 CUTKOSKY 80 IPWA π N → π N 2081± 20 HOEHLER 79 IPWA π N → π N N(2120) BREIT-WIGNER WIDTH N(2120) BREIT-WIGNER WIDTH N(2120) BREIT-WIGNER WIDTH N(2120) BREIT-WIGNER WIDTH VALUE (MeV) DOCUMENT ID TECN COMMENT 330± 45 ANISOVICH 12A DPWA Multichannel 300±

42

b014.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

10) 10) 1/2 + I (J P ) = 1 2 ( 1 2 + ) Status: ∗∗∗ Most of the results published before 1975 were last included in our 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. N(1710) BREIT-WIGNER MASS N(1710) BREIT-WIGNER MASS N(1710) BREIT-WIGNER MASS N(1710) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1680 to 1740 (≈ 1710) OUR ESTIMATE 1680 to 1740 (≈ 1710) OUR ESTIMATE 1680 to 1740 (≈ 1710) OUR ESTIMATE 1680 to 1740 (≈ 1710) OUR ESTIMATE 1710± 20 ANISOVICH 12A DPWA Multichannel 1700± 50 CUTKOSKY 80 IPWA π N → π N 1723± 9 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1662± 7 SHRESTHA 12A DPWA Multichannel 1725±

43

b117.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

20) 20) 3/2 + I (J P ) = 3 2 ( 3 2 + ) Status: ∗∗∗ Most of the results published before 1975 were last included in our 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. ∆(1920) BREIT-WIGNER MASS ∆(1920) BREIT-WIGNER MASS ∆(1920) BREIT-WIGNER MASS ∆(1920) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1900 to 1970 (≈ 1920) OUR ESTIMATE 1900 to 1970 (≈ 1920) OUR ESTIMATE 1900 to 1970 (≈ 1920) OUR ESTIMATE 1900 to 1970 (≈ 1920) OUR ESTIMATE 1900 ± 30 ANISOVICH 12A DPWA Multichannel 1920 ± 80 CUTKOSKY 80 IPWA π N → π N 1868 ± 10 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 2146 ± 32 SHRESTHA 12A DPWA Multichannel

44

Receiver Antenna Array for a Multichannel Sense-and-Avoid Radar for Small UAVs  

E-Print Network [OSTI]

Receiver Antenna Array for a Multichannel Sense-and-Avoid Radar for Small UAVs Jose Francisco for use in a sense-and-avoid radar for use in the Cessna C-172 and small Unmanned Aerial Vehicles (UAVs. . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . ..10 1.1.1 Multichannel Sense-and-Avoid Radar for UAVs. . . . . . . . . . . . . . . . . . . . . . ...10

Kansas, University of

45

Single ultrafast diffusive conduction based optoelectronic switch for multi-channel operation  

E-Print Network [OSTI]

Single ultrafast diffusive conduction based optoelectronic switch for multi-channel operation Fatih to multi-channel operation, including Green's function diffusive conduction solution and crosstalk conduction based optoelectronic switches that accommodate >100 optical channels (with 2,000mm-2 channel

Miller, David A. B.

46

Computational Science Technical Note CSTN-071 Clusters in Hyper-cubic Multi-Channel Satellite Imagery  

E-Print Network [OSTI]

0 Computational Science Technical Note CSTN-071 Clusters in Hyper-cubic Multi-Channel Satellite Imagery K. A. Hawick 2011 Multi-spectral remotely-sensed data such as satellite imagery can yield excellent insights into complex phenomena such as weather systems. Analysing the multi-channel space

Hawick, Ken

47

Simultaneous Greedy Analysis Pursuit for Compressive Sensing of Multi-Channel ECG Signals  

E-Print Network [OSTI]

Simultaneous Greedy Analysis Pursuit for Compressive Sensing of Multi-Channel ECG Signals Yurrit sensing for multi- channel ECG signals. In contrast to the traditional sparse approach where the signal of compressive sensing for ECG signals. Moreover, to efficiently recover multi-channel ECG signals, clas- sical

48

Development of multichannel low-energy neutron spectrometer  

SciTech Connect (OSTI)

A multichannel low-energy neutron spectrometer for down-scattered neutron (DSN) measurements in inertial confinement fusion (ICF) experiments has been developed. Our compact-size 256-channel lithium-glass-scintillator-based spectrometer has been implemented and tested in ICF experiments with the GEKKO XII laser. We have performed time calibration of the 256-channel analog-to-digital convertor system used for DSN measurements via X-ray pulse signals. We have clearly observed the DD-primary fusion neutron signal and have successfully studied the detector's impulse response. Our detector is soon to be implemented in future ICF experiments.

Arikawa, Y., E-mail: arikawa-y@ile.osaka-u.ac.jp; Nagai, T.; Abe, Y.; Kojima, S.; Sakata, S.; Inoue, H.; Utsugi, M.; Iwasa, Y.; Sarukura, N.; Nakai, M.; Shiraga, H.; Fujioka, S.; Azechi, H. [Institute of Laser Engineering, Osaka University, 2-6 Yamada-oka, Suita, Osaka (Japan); Murata, T. [Kumamoto University, 2-40-1 Kurokami, Kumamoto 860-8555 (Japan)

2014-11-15T23:59:59.000Z

49

PCA-multiport, a universal computer-based multichannel analyzer  

SciTech Connect (OSTI)

Nearly a decade has passed since Tennelec/Nucleus introduced the first personal-computer-based multichannel analyzer (MCA). These new MCA architectures, including plug-in cards, nuclear instrumentation module (NIM), and non-NIM versions, have revolutionized spectroscopy measurements and virtually replaced conventional one-box MCAs. The Tennelec personal computer analyzer (PCA)-Multiport is a third-generation system capable of interfacing with virtually any computer. It is designed to be used for most energy and timing measurements commonly encountered in nuclear spectroscopy.

Seymour, R.; Bedwell, M.; Stockton, S.; Beal, T.; Ahsan, Z.

1991-11-01T23:59:59.000Z

50

b044.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

3/2 3/2 - I (J P ) = 1( 3 2 - ) Status: ∗∗∗∗ For most results published before 1974 (they are now obsolete), see our 1982 edition Physics Letters 111B 111B 111B 111B 1 (1982). Results from production experiments are listed separately in the next entry. Σ (1670) MASS Σ (1670) MASS Σ (1670) MASS Σ (1670) MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1665 to 1685 (≈ 1670) OUR ESTIMATE 1665 to 1685 (≈ 1670) OUR ESTIMATE 1665 to 1685 (≈ 1670) OUR ESTIMATE 1665 to 1685 (≈ 1670) OUR ESTIMATE 1673 ± 1 GAO 12 DPWA K N → Λ π 1665.1± 4.1 KOISO 85 DPWA K - p → Σ π 1682 ± 5 GOPAL 80 DPWA K N → K N 1679 ± 10 ALSTON-... 78 DPWA K N → K N 1670 ± 5 GOPAL 77 DPWA K N multichannel 1670 ± 6 HEPP 76B DPWA K - N → Σ π 1685 ± 20 BAILLON 75 IPWA K N → Λ π 1659 + 12 - 5 VANHORN 75 DPWA K - p → Λ π 0 1670 ± 2 KANE 74 DPWA K - p → Σ π * * * We do not use the following data for averages, fits, limits, etc. * * * 1667 or 1668 1 MARTIN 77

51

Multichannel Quantum Defect Theory of Strontium Rydberg Series  

E-Print Network [OSTI]

Using the reactance matrix approach, we systematically develop new multichannel quantum defect theory models for the singlet and triplet S, P, D and F states of strontium based on improved energy level measurements. The new models reveal additional insights into the character of doubly excited perturber states, and the improved energy level measurements for certain series allow fine structure to be resolved for those series' perturbers. Comparison between the predictions of the new models and those of previous empirical and \\emph{ab initio} studies reveals good agreement with most series, however some discrepancies are highlighted. Using the multichannel quantum defect theory wave functions derived from our models we calculate other observables such as Land\\'e $g_J$-factors and radiative lifetimes. The analysis reveals the impact of perturbers on the Rydberg state properties of divalent atoms, highlighting the importance of including two-electron effects in the calculations of these properties. The work enables future investigations of properties such as Stark maps and long-range interactions of Rydberg states of strontium.

C L Vaillant; M P A Jones; R M Potvliege

2014-02-24T23:59:59.000Z

52

Deep-towed High Resolution multichannel seismic imaging  

Science Journals Connector (OSTI)

Abstract High Resolution (2201050Hz) seismic acquisition performed in deep water using deep-towed systems provides unrivalled lateral resolution when compared to conventional surface seismic. The lateral resolution of these acquisitions is controlled by the width of the first Fresnel zone, taking advantage of their positions close to the sea bottom. No current existing deep towed equipment can benefit from seismic imaging processing techniques to improve this resolution as a consequence of positioning inaccuracies. The technological developments of a digital deep-towed multichannel streamer are presented with a particular attention to positioning: each hydrophone incorporates a pitch, roll and heading sensor in order to monitor the constant deformation of the streamer in operation. The sea trials took place in July 2013 in the Mediterranean Sea. Pre-stack depth migration applied to the deep-towed multichannel data illustrates the potential of this emerging methodology in terms of penetration (12dB improvement in Signal/Noise) and lateral resolution (mean signal wavelength: 3m) when compared with deep-towed single-channel acquisition.

B. Marsset; E. Menut; S. Ker; Y. Thomas; J.-P. Regnault; P. Leon; H. Martinossi; L. Artzner; D. Chenot; S. Dentrecolas; B. Spychalski; G. Mellier; N. Sultan

2014-01-01T23:59:59.000Z

53

b145.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

5 5 ∆(1750) 1/2 + I (J P ) = 3 2 ( 1 2 + ) Status: ∗ OMITTED FROM SUMMARY TABLE Neither ARNDT 06 nor ANISOVICH 12A finds any evidence for this NODE=B145 resonance. ∆(1750) BREIT-WIGNER MASS ∆(1750) BREIT-WIGNER MASS ∆(1750) BREIT-WIGNER MASS ∆(1750) BREIT-WIGNER MASS NODE=B145M NODE=B145M VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 1750 OUR ESTIMATE ≈ 1750 OUR ESTIMATE ≈ 1750 OUR ESTIMATE ≈ 1750 OUR ESTIMATE → UNCHECKED ← * * * We do not use the following data for averages, fits, limits, etc. * * * 1712 ± 1 PENNER 02C DPWA Multichannel 1721 ± 61 VRANA 00 DPWA Multichannel 1744 ± 36 MANLEY 92 IPWA π N → π N & N π π 1715.2 ± 21.0 1 CHEW 80 BPWA π + p → π + p OCCUR=2 1778.4 ± 9.0 1 CHEW 80 BPWA π + p → π + p ∆(1750) BREIT-WIGNER WIDTH ∆(1750) BREIT-WIGNER WIDTH ∆(1750) BREIT-WIGNER WIDTH ∆(1750) BREIT-WIGNER WIDTH NODE=B145W NODE=B145W VALUE (MeV) DOCUMENT ID TECN

54

Cluster expansion, multichannel scattering, and the optical potential  

Science Journals Connector (OSTI)

This paper investigates approximate solutions for the few-body multichannel reaction problem. In the context of the three-body scattering problem, we extend the cluster expansion formalism that is based on the Karlsson-Zeiger integral equations. The decoupling scheme developed by Boll and Kuzmichev is modified to extract the elastic channel optical potential. The utility and rate of convergence of the cluster expansion is tested in a model three-boson problem. The interactions for the model problem are chosen to include elastic, inelastic, and rearrangement channels. It is found that only a few terms of the cluster expansion are needed to reproduce the exact three-body solutions and that cusp singularity effects which appear in the phase shift at channel thresholds are accounted for accurately.NUCLEAR REACTIONS Three-body problem. Cluster representations. Optical potential. Threshold singularities. Approximation methods.

D. Eyre; T. A. Osborn; J. P. Svenne

1981-12-01T23:59:59.000Z

55

A multichannel sensor for parameters of layered media with one detective element  

Science Journals Connector (OSTI)

We propose detective element structures for a multichannel sensor based on a distributed long line with kinks distributed along its length. We find generalized relations between the eigenvalues of a resonator with an arbitrary number of kinks and the ...

B. V. Lunkin

2012-10-01T23:59:59.000Z

56

1166 IEEE TRANSACTIONS ON INSTRUMENTATION AND MEASUREMENT, VOL. 48, NO. 6, DECEMBER 1999 A Multichannel Photon Counting System for  

E-Print Network [OSTI]

of which are in the fields of medical electronics (confocal microscopy) and bio-electronics, air pollution. Index Terms-- Air pollution, laser gas sensor, multichannel gas monitoring, optoelectronic measurement a multichannel photon- counting system for the in situ quantitative monitoring of up to five air pollutants

Athens, University of

57

b064.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

49 49 Page 1 NODE=B064 N(1675) 5/2 - I (J P ) = 1 2 ( 5 2 - ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our NODE=B064 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(1675) POLE POSITION N(1675) POLE POSITION N(1675) POLE POSITION N(1675) POLE POSITION NODE=B064215 REAL PART REAL PART REAL PART REAL PART NODE=B064RE NODE=B064RE VALUE (MeV) DOCUMENT ID TECN COMMENT 1655 to 1665 (≈ 1660) OUR ESTIMATE 1655 to 1665 (≈ 1660) OUR ESTIMATE 1655 to 1665 (≈ 1660) OUR ESTIMATE 1655 to 1665 (≈ 1660) OUR ESTIMATE → UNCHECKED ← 1654 ± 4 ANISOVICH 12A DPWA Multichannel 1657 ARNDT 06 DPWA π N → π N, η N 1656 1 HOEHLER 93 ARGD π N → π N 1660 ± 10 CUTKOSKY 80 IPWA π N → π N * * * We do not use the following data for averages,

58

b063.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

7 7 Page 1 NODE=B063 N(1535) 1/2 - I (J P ) = 1 2 ( 1 2 - ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our NODE=B063 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(1535) BREIT-WIGNER MASS N(1535) BREIT-WIGNER MASS N(1535) BREIT-WIGNER MASS N(1535) BREIT-WIGNER MASS NODE=B063M NODE=B063M VALUE (MeV) DOCUMENT ID TECN COMMENT 1525 to 1545 (≈ 1535) OUR ESTIMATE 1525 to 1545 (≈ 1535) OUR ESTIMATE 1525 to 1545 (≈ 1535) OUR ESTIMATE 1525 to 1545 (≈ 1535) OUR ESTIMATE → UNCHECKED ← 1519 ± 5 ANISOVICH 12A DPWA Multichannel 1547.0 ± 0.7 ARNDT 06 DPWA π N → π N, η N 1550 ± 40 CUTKOSKY 80 IPWA π N → π N 1526 ± 7 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. *

59

b012.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

2 2 ∆(1910) 1/2 + I (J P ) = 3 2 ( 1 2 + ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our NODE=B012 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). ∆(1910) BREIT-WIGNER MASS ∆(1910) BREIT-WIGNER MASS ∆(1910) BREIT-WIGNER MASS ∆(1910) BREIT-WIGNER MASS NODE=B012M NODE=B012M VALUE (MeV) DOCUMENT ID TECN COMMENT 1860 to 1910 (≈ 1890) OUR ESTIMATE 1860 to 1910 (≈ 1890) OUR ESTIMATE 1860 to 1910 (≈ 1890) OUR ESTIMATE 1860 to 1910 (≈ 1890) OUR ESTIMATE → UNCHECKED ← 1860 ± 40 ANISOVICH 12A DPWA Multichannel 2067.9 ± 1.7 ARNDT 06 DPWA π N → π N, η N 1910 ± 40 CUTKOSKY 80 IPWA π N → π N 1888 ± 20 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * *

60

b062.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

2 2 N(1520) 3/2 - I (J P ) = 1 2 ( 3 2 - ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our NODE=B062 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(1520) BREIT-WIGNER MASS N(1520) BREIT-WIGNER MASS N(1520) BREIT-WIGNER MASS N(1520) BREIT-WIGNER MASS NODE=B062M NODE=B062M VALUE (MeV) DOCUMENT ID TECN COMMENT 1510 to 1520 (≈ 1515) OUR ESTIMATE 1510 to 1520 (≈ 1515) OUR ESTIMATE 1510 to 1520 (≈ 1515) OUR ESTIMATE 1510 to 1520 (≈ 1515) OUR ESTIMATE NEW;→ UNCHECKED ← [1515 to 1525 (≈ 1520) MeV OUR 2013 ESTIMATE] 1517 ± 3 ANISOVICH 12A DPWA Multichannel 1514.5 ± 0.2 ARNDT 06 DPWA π N → π N, η N 1525 ± 10 CUTKOSKY 80 IPWA π N → π N 1519 ± 4 HOEHLER 79 IPWA π N → π N * * * We do not use the following data

Note: This page contains sample records for the topic "12a dpwa multichannel" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
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We encourage you to perform a real-time search of NLEBeta
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61

b071.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

71 71 N(2190) 7/2 - I (J P ) = 1 2 ( 7 2 - ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our NODE=B071 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(2190) BREIT-WIGNER MASS N(2190) BREIT-WIGNER MASS N(2190) BREIT-WIGNER MASS N(2190) BREIT-WIGNER MASS NODE=B071M NODE=B071M VALUE (MeV) DOCUMENT ID TECN COMMENT 2100 to 2200 (≈ 2190) OUR ESTIMATE 2100 to 2200 (≈ 2190) OUR ESTIMATE 2100 to 2200 (≈ 2190) OUR ESTIMATE 2100 to 2200 (≈ 2190) OUR ESTIMATE → UNCHECKED ← 2180 ± 20 ANISOVICH 12A DPWA Multichannel 2152.4 ± 1.4 ARNDT 06 DPWA π N → π N, η N 2200 ± 70 CUTKOSKY 80 IPWA π N → π N 2140 ± 12 HOEHLER 79 IPWA π N → π N 2140 ± 40 HENDRY 78 MPWA π N → π N * * * We do not use the following data for averages,

62

b010.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

8 8 Page 1 NODE=B010 ∆(1700) 3/2 - I (J P ) = 3 2 ( 3 2 - ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our NODE=B010 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). ∆(1700) BREIT-WIGNER MASS ∆(1700) BREIT-WIGNER MASS ∆(1700) BREIT-WIGNER MASS ∆(1700) BREIT-WIGNER MASS NODE=B010M NODE=B010M VALUE (MeV) DOCUMENT ID TECN COMMENT 1670 to 1750 (≈ 1700) OUR ESTIMATE 1670 to 1750 (≈ 1700) OUR ESTIMATE 1670 to 1750 (≈ 1700) OUR ESTIMATE 1670 to 1750 (≈ 1700) OUR ESTIMATE → UNCHECKED ← 1715 + 30 - 15 ANISOVICH 12A DPWA Multichannel 1695.0 ± 1.3 ARNDT 06 DPWA π N → π N, η N 1710 ± 30 CUTKOSKY 80 IPWA π N → π N 1680 ± 70 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits,

63

b065.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

53 53 Page 1 NODE=B065 N(1680) 5/2 + I (J P ) = 1 2 ( 5 2 + ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our NODE=B065 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(1680) POLE POSITION N(1680) POLE POSITION N(1680) POLE POSITION N(1680) POLE POSITION NODE=B065215 REAL PART REAL PART REAL PART REAL PART NODE=B065RE NODE=B065RE VALUE (MeV) DOCUMENT ID TECN COMMENT 1665 to 1680 (≈ 1675) OUR ESTIMATE 1665 to 1680 (≈ 1675) OUR ESTIMATE 1665 to 1680 (≈ 1675) OUR ESTIMATE 1665 to 1680 (≈ 1675) OUR ESTIMATE → UNCHECKED ← 1676 ± 6 ANISOVICH 12A DPWA Multichannel 1674 ARNDT 06 DPWA π N → π N, η N 1673 1 HOEHLER 93 ARGD π N → π N 1667 ± 5 CUTKOSKY 80 IPWA π N → π N * * * We do not use the following data for averages,

64

b011.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

1 1 ∆(1905) 5/2 + I (J P ) = 3 2 ( 5 2 + ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our NODE=B011 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). ∆(1905) BREIT-WIGNER MASS ∆(1905) BREIT-WIGNER MASS ∆(1905) BREIT-WIGNER MASS ∆(1905) BREIT-WIGNER MASS NODE=B011M NODE=B011M VALUE (MeV) DOCUMENT ID TECN COMMENT 1855 to 1910 (≈ 1880) OUR ESTIMATE 1855 to 1910 (≈ 1880) OUR ESTIMATE 1855 to 1910 (≈ 1880) OUR ESTIMATE 1855 to 1910 (≈ 1880) OUR ESTIMATE → UNCHECKED ← 1861 ± 6 ANISOVICH 12A DPWA Multichannel 1857.8 ± 1.6 ARNDT 06 DPWA π N → π N, η N 1910 ± 30 CUTKOSKY 80 IPWA π N → π N 1905 ± 20 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1818

65

b013.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

3 3 ∆(1930) 5/2 - I (J P ) = 3 2 ( 5 2 - ) Status: ∗∗∗ Most of the results published before 1975 were last included in our NODE=B013 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). ∆(1930) BREIT-WIGNER MASS ∆(1930) BREIT-WIGNER MASS ∆(1930) BREIT-WIGNER MASS ∆(1930) BREIT-WIGNER MASS NODE=B013M NODE=B013M VALUE (MeV) DOCUMENT ID TECN COMMENT 1900 to 2000 (≈ 1950) OUR ESTIMATE 1900 to 2000 (≈ 1950) OUR ESTIMATE 1900 to 2000 (≈ 1950) OUR ESTIMATE 1900 to 2000 (≈ 1950) OUR ESTIMATE → UNCHECKED ← 2233 ± 53 ARNDT 06 DPWA π N → π N, η N 1940 ± 30 CUTKOSKY 80 IPWA π N → π N 1901 ± 15 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1930 ± 12 SHRESTHA 12A DPWA Multichannel 2046 ± 45

66

b061.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

1 1 N(1440) 1/2 + I (J P ) = 1 2 ( 1 2 + ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our NODE=B061 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(1440) BREIT-WIGNER MASS N(1440) BREIT-WIGNER MASS N(1440) BREIT-WIGNER MASS N(1440) BREIT-WIGNER MASS NODE=B061M NODE=B061M VALUE (MeV) DOCUMENT ID TECN COMMENT 1410 to 1450 (≈ 1430) OUR ESTIMATE 1410 to 1450 (≈ 1430) OUR ESTIMATE 1410 to 1450 (≈ 1430) OUR ESTIMATE 1410 to 1450 (≈ 1430) OUR ESTIMATE NEW;→ UNCHECKED ← [1420 to 1470 (≈ 1440) MeV OUR 2013 ESTIMATE] 1430 ± 8 ANISOVICH 12A DPWA Multichannel 1485.0 ± 1.2 ARNDT 06 DPWA π N → π N, η N 1440 ± 30 CUTKOSKY 80 IPWA π N → π N 1410 ± 12 HOEHLER 79 IPWA π N → π N * * * We do not use the following data

67

b015.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

5 5 N(1720) 3/2 + I (J P ) = 1 2 ( 3 2 + ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our NODE=B015 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(1720) BREIT-WIGNER MASS N(1720) BREIT-WIGNER MASS N(1720) BREIT-WIGNER MASS N(1720) BREIT-WIGNER MASS NODE=B015M NODE=B015M VALUE (MeV) DOCUMENT ID TECN COMMENT 1700 to 1750 (≈ 1720) OUR ESTIMATE 1700 to 1750 (≈ 1720) OUR ESTIMATE 1700 to 1750 (≈ 1720) OUR ESTIMATE 1700 to 1750 (≈ 1720) OUR ESTIMATE → UNCHECKED ← 1690 + 70 - 35 ANISOVICH 12A DPWA Multichannel 1763.8 ± 4.6 ARNDT 06 DPWA π N → π N, η N 1700 ± 50 CUTKOSKY 80 IPWA π N → π N 1710 ± 20 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1720 ± 5 SHRESTHA

68

b033.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

33 33 ∆(1232) 3/2 + I (J P ) = 3 2 ( 3 2 + ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our NODE=B033 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). ∆(1232) BREIT-WIGNER MASSES ∆(1232) BREIT-WIGNER MASSES ∆(1232) BREIT-WIGNER MASSES ∆(1232) BREIT-WIGNER MASSES NODE=B033205 MIXED CHARGES MIXED CHARGES MIXED CHARGES MIXED CHARGES NODE=B033M NODE=B033M VALUE (MeV) DOCUMENT ID TECN COMMENT 1230 to 1234 (≈ 1232) OUR ESTIMATE 1230 to 1234 (≈ 1232) OUR ESTIMATE 1230 to 1234 (≈ 1232) OUR ESTIMATE 1230 to 1234 (≈ 1232) OUR ESTIMATE → UNCHECKED ← 1228 ± 2 ANISOVICH 12A DPWA Multichannel 1233.4 ± 0.4 ARNDT 06 DPWA π N → π N, η N 1232 ± 3 CUTKOSKY 80 IPWA π N → π N 1233 ± 2 HOEHLER 79 IPWA π N

69

b066.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

6 6 N(1650) 1/2 - I (J P ) = 1 2 ( 1 2 - ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our NODE=B066 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(1650) BREIT-WIGNER MASS N(1650) BREIT-WIGNER MASS N(1650) BREIT-WIGNER MASS N(1650) BREIT-WIGNER MASS NODE=B066M NODE=B066M VALUE (MeV) DOCUMENT ID TECN COMMENT 1645 to 1670 (≈ 1655) OUR ESTIMATE 1645 to 1670 (≈ 1655) OUR ESTIMATE 1645 to 1670 (≈ 1655) OUR ESTIMATE 1645 to 1670 (≈ 1655) OUR ESTIMATE → UNCHECKED ← 1651 ± 6 ANISOVICH 12A DPWA Multichannel 1634.7 ± 1.1 ARNDT 06 DPWA π N → π N, η N 1650 ± 30 CUTKOSKY 80 IPWA π N → π N 1670 ± 8 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1664 ± 2 SHRESTHA

70

A service re-design methodology for multi-channel adaptation  

Science Journals Connector (OSTI)

Many available services have been designed for a single-channel world, Web and Internet typically. In a real world scenario, an ever-growing number of users take advantage of different kinds of communication channels and devices. In this paper, we propose ... Keywords: context of use, location awareness, methodology, multi-channel application, qualities of services, service re-design

M. Comerio; F. De Paoli; S. Grega; C. Batini; C. Di Francesco; A. Di Pasquale

2004-11-01T23:59:59.000Z

71

A Specific Multi-channel Photon-Counting Unit for Air-Pollution Measurement  

E-Print Network [OSTI]

A Specific Multi-channel Photon-Counting Unit for Air-Pollution Measurement Papageorgas P.1.g. confocal microscopy), air pollution optical measurements, laser sounding of the atmosphere for the in situ quantitative monitoring of up to five air pollutants simultaneously and one calibration channel

Athens, University of

72

SYSTEM IDENTIFICATION FOR MULTI-CHANNEL LISTENING-ROOM COMPENSATION USING AN ACOUSTIC ECHO CANCELLER  

E-Print Network [OSTI]

SYSTEM IDENTIFICATION FOR MULTI-CHANNEL LISTENING-ROOM COMPENSATION USING AN ACOUSTIC ECHO hands-free telecommunication devices jointly apply several subsystems, e.g. for noise reduction (NR), acoustic echo cancella- tion (AEC) and listening-room compensation (LRC). In this contri- bution

Lübeck, Universität zu

73

Clusters in Hyper-Cubic Multi-Channel Satellite Imagery K.A. Hawick  

E-Print Network [OSTI]

satellites. Weather prediction it- self remains a challenging problem, not least due to the chaotic, but previously very successful GMS5 Japanese weather satellite[6]. Regularly sampled full-disk Earth image dataClusters in Hyper-Cubic Multi-Channel Satellite Imagery K.A. Hawick Computer Science, Massey

Hawick, Ken

74

New plasma measurements with a multichannel millimeter-wave fluctuation diagnostic system in the DIII-D tokamak  

E-Print Network [OSTI]

A novel multichannel, tunable Doppler backscattering (DBS)/reflectometry system has recently been developed and applied to a variety of DIII-D plasmas. Either DBS or reflectometry can be easily configured for use in a wide ...

Hillesheim, J. C.

75

b060.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

60 60 Λ(1890) 3/2 + I (J P ) = 0( 3 2 + ) Status: ∗∗∗∗ For results published before 1974 (they are now obsolete), see our NODE=B060 1982 edition Physics Letters 111B 111B 111B 111B 1 (1982). The J P = 3/2 + assignment is consistent with all available data (including polarization) and recent partial-wave analyses. The dom- inant inelastic modes remain unknown. Λ(1890) MASS Λ(1890) MASS Λ(1890) MASS Λ(1890) MASS NODE=B060M NODE=B060M VALUE (MeV) DOCUMENT ID TECN COMMENT 1850 to 1910 (≈ 1890) OUR ESTIMATE 1850 to 1910 (≈ 1890) OUR ESTIMATE 1850 to 1910 (≈ 1890) OUR ESTIMATE 1850 to 1910 (≈ 1890) OUR ESTIMATE → UNCHECKED ← 1897 ± 5 GOPAL 80 DPWA K N → K N 1908 ± 10 ALSTON-... 78 DPWA K N → K N 1900 ± 5 GOPAL 77 DPWA K N multichannel 1894 ± 10 HEMINGWAY 75 DPWA K - p → K N * * * We do not use the following data for averages, fits, limits, etc. * * * 1856 or 1868 1 MARTIN 77 DPWA K N multichannel

76

Calibrating spectral estimation for the LISA Technology Package with multichannel synthetic noise generation  

SciTech Connect (OSTI)

The scientific objectives of the LISA Technology Package experiment on board of the LISA Pathfinder mission demand accurate calibration and validation of the data analysis tools in advance of the mission launch. The level of confidence required in the mission outcomes can be reached only by intensively testing the tools on synthetically generated data. A flexible procedure allowing the generation of a cross-correlated stationary noise time series was set up. A multichannel time series with the desired cross-correlation behavior can be generated once a model for a multichannel cross-spectral matrix is provided. The core of the procedure comprises a noise coloring, multichannel filter designed via a frequency-by-frequency eigendecomposition of the model cross-spectral matrix and a subsequent fit in the Z domain. The common problem of initial transients in a filtered time series is solved with a proper initialization of the filter recursion equations. The noise generator performance was tested in a two-dimensional case study of the closed-loop LISA Technology Package dynamics along the two principal degrees of freedom.

Ferraioli, Luigi; Hueller, Mauro; Vitale, Stefano; Heinzel, Gerhard; Hewitson, Martin; Monsky, Anneke; Nofrarias, Miquel [University of Trento and INFN, via Sommarive 14, 38123 Povo (Trento) (Italy); Albert-Einstein-Institut, Max-Planck-Institut fuer, Gravitationsphysik und Universitaet Hannover, Callinstrasse 38, 30167 Hannover (Germany)

2010-08-15T23:59:59.000Z

77

Effects, determination, and correction of count rate nonlinearity in multi-channel analog electron detectors  

SciTech Connect (OSTI)

Detector counting rate nonlinearity, though a known problem, is commonly ignored in the analysis of angle resolved photoemission spectroscopy where modern multichannel electron detection schemes using analog intensity scales are used. We focus on a nearly ubiquitous inverse saturation nonlinearity that makes the spectra falsely sharp and beautiful. These artificially enhanced spectra limit accurate quantitative analysis of the data, leading to mistaken spectral weights, Fermi energies, and peak widths. We present a method to rapidly detect and correct for this nonlinearity. This algorithm could be applicable for a wide range of nonlinear systems, beyond photoemission spectroscopy.

Reber, T. J.; Plumb, N. C.; Waugh, J. A.; Dessau, D. S. [Department of Physics, University of Colorado, Boulder, Colorado 80309-0390 (United States)] [Department of Physics, University of Colorado, Boulder, Colorado 80309-0390 (United States)

2014-04-15T23:59:59.000Z

78

A Closer Look at Salt, Faults, and Gas in the Northwestern Gulf of Mexico with 2-D Multichannel Seismic Data  

E-Print Network [OSTI]

The sedimentary wedge of the northern Gulf of Mexico is extensively deformed and faulted by salt tectonics. Industry 2-D multichannel seismic data covering a large area (33,800 km2) of the lower Texas continental slope [96 degrees 40'- 93 degrees 40...

Nemazi, Leslie A.

2010-07-14T23:59:59.000Z

79

Hydrogen production in Multi-Channel Membrane Reactor via Steam Methane Reforming and Methane Catalytic Combustion  

Science Journals Connector (OSTI)

Abstract A novel Multi-Channel Membrane Reactor (MCMR) was designed and built for the small-scale production of hydrogen via Steam Methane Reforming (SMR). The prototype alternates an SMR gas channel to produce hydrogen catalytically, with a Methane Catalytic Combustion (MCC) gas channel to provide the heat of reaction needed by the endothermic reforming. A palladiumsilver membrane inside the reforming gas channel shifts the reaction equilibrium, allowing lower operating temperatures, and producing pure hydrogen in a single vessel. Using an innovative air-spray coating technique, channels were coated with RuMgOLa2O3/?-Al2O3 and Pd/?-Al2O3 catalyst particles for the SMR and MCC reactions, respectively. Results for the proof-of-concept MCMR showed that methane conversion in the reformer of 91% and a hydrogen purity in excess of 99.99% were possible with the reformer operating at 570C and 15bar.

Alexandre Vigneault; John R. Grace

2014-01-01T23:59:59.000Z

80

Device for modular input high-speed multi-channel digitizing of electrical data  

DOE Patents [OSTI]

A multi-channel high-speed digitizer module converts a plurality of analog signals to digital signals (digitizing) and stores the signals in a memory device. The analog input channels are digitized simultaneously at high speed with a relatively large number of on-board memory data points per channel. The module provides an automated calibration based upon a single voltage reference source. Low signal noise at such a high density and sample rate is accomplished by ensuring the A/D converters are clocked at the same point in the noise cycle each time so that synchronous noise sampling occurs. This sampling process, in conjunction with an automated calibration, yields signal noise levels well below the noise level present on the analog reference voltages. 1 fig.

VanDeusen, A.L.; Crist, C.E.

1995-09-26T23:59:59.000Z

Note: This page contains sample records for the topic "12a dpwa multichannel" 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.


81

A multichannel design for QoS aware energy efficient clustering and routing in WMSN  

Science Journals Connector (OSTI)

Wireless Multimedia Sensor Networks (WMSNs) are used in video surveillance applications for disaster management inside buildings. There is unavailability of electricity in a building during a disastrous situation. To have an energy efficient and real-time data delivery, a Quality of Service (QoS) aware energy efficient routing technique is proposed in this paper. It tries to find a route that meets the real-time data delivery deadlines by minimising the energy consumption. Also, WMSNs usually employ single channel design approach whereas at a given instant several video or image streams should be delivered. Based on the channel conditions, a game theory based distributed multichannel allocation mechanism is proposed which improves the network performance parameters in varying channel conditions. These network design mechanisms are investigated using NS-2 simulator for a test case application. It is shown that the combined approach leads to further reduction in the energy consumption by meeting the data reporting deadlines.

Zeeshan Ali Khan; Michel Auguin

2013-01-01T23:59:59.000Z

82

Two-particle multichannel systems in a finite volume with arbitrary spin  

SciTech Connect (OSTI)

The quantization condition for two-particle systems with arbitrary number of two-body open coupled channels, spin and masses in a finite cubic volume with either periodic or twisted boundary conditions is presented. The condition presented is in agreement with all previous studies of two-body systems in a finite volume. The result is relativistic, holds for all momenta below the three- and four-particle thresholds, and is exact up to exponential volume corrections that are governed by L/r, where L is the spatial extent of the volume and r is the range of the interactions between the particles. For hadronic systems the range of the interaction is set by the inverse of the pion mass, m?, and as a result the formalism presented is suitable for m?L>>1. Implications of the formalism for the studies of multichannel baryon-baryon systems are discussed.

Briceno, Raul A. [JLAB

2014-04-01T23:59:59.000Z

83

Non-cross talk multi-channel photomultiplier using guided electron multipliers  

DOE Patents [OSTI]

An improved multi-channel electron multiplier is provided that exhibits zero cross-talk and high rate operation. Resistive material input and output masks are employed to control divergence of electrons. Electron multiplication takes place in closed channels. Several embodiments are provided for these channels including a continuous resistive emissive multiplier and a discrete resistive multiplier with discrete dynode chains interspaced with resistive layers-masks. Both basic embodiments provide high gain multiplication of electrons without accumulating surface charges while containing electrons to their proper channels to eliminate cross-talk. The invention can be for example applied to improve the performance of ion mass spectrometers, positron emission tomography devices, in DNA sequencing and other beta radiography applications and in many applications in particle physics. 28 figs.

Gomez, J.; Majewski, S.; Weisenberger, A.G.

1995-09-26T23:59:59.000Z

84

Non cross talk multi-channel photomultiplier using guided electron multipliers  

DOE Patents [OSTI]

An improved multi-channel electron multiplier is provided that exhibits zero cross-talk and high rate operation. Resistive material input and output masks are employed to control divergence of electrons. Electron multiplication takes place in closed channels. Several embodiments are provided for these channels including a continuous resistive emissive multiplier and a discrete resistive multiplier with discrete dynode chains interspaced with resistive layers-masks. Both basic embodiments provide high gain multiplication of electrons without accumulating surface charges while containing electrons to their proper channels to eliminate cross-talk. The invention can be for example applied to improve the performance of ion mass spectrometers, positron emission tomography devices, in DNA sequencing and other beta radiography applications and in many applications in particle physics.

Gomez, Javier (Newport News, VA); Majewski, Stanislaw (Grafton, VA); Weisenberger, Andrew G. (Grafton, VA)

1995-01-01T23:59:59.000Z

85

Mk12A/W78 ground test project (u)  

SciTech Connect (OSTI)

The slides present the scope, objectives and status of the Mk12A1W78 Ground Test Project for the purpose of updating the ICBM Project Officers Group. In addition, project constraints and risks are discussed.

Stokes, Kyle R [Los Alamos National Laboratory

2010-12-01T23:59:59.000Z

86

Salt Tectonics and Its Effect on Sediment Structure and Gas Hydrate Occurrence in the Northwestern Gulf of Mexico from 2-D Multichannel Seismic Data  

E-Print Network [OSTI]

This study was undertaken to investigate mobile salt and its effect on fault structures and gas hydrate occurrence in the northwestern Gulf of Mexico. Industry 2-D multichannel seismic data were used to investigate the effects of the salt within...

Lewis, Dan'L 1986-

2012-10-04T23:59:59.000Z

87

b100.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

0 0 Σ (1770) 1/2 + I (J P ) = 1( 1 2 + ) Status: ∗ OMITTED FROM SUMMARY TABLE Evidence for this state now rests solely on solution 1 of BAILLON 75, NODE=B100 (see the footnotes) but the Λ π partial-wave amplitudes of this solu- tion are in disagreement with amplitudes from most other Λ π anal- yses. Σ (1770) MASS Σ (1770) MASS Σ (1770) MASS Σ (1770) MASS NODE=B100M NODE=B100M VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 1770 OUR ESTIMATE ≈ 1770 OUR ESTIMATE ≈ 1770 OUR ESTIMATE ≈ 1770 OUR ESTIMATE → UNCHECKED ← 1738 ± 10 1 GOPAL 77 DPWA K N multichannel 1770 ± 20 2 BAILLON 75 IPWA K N → Λ π 1772 3 KANE 72 DPWA K - p → Σ π Σ (1770) WIDTH Σ (1770) WIDTH Σ (1770) WIDTH Σ (1770) WIDTH NODE=B100W NODE=B100W VALUE (MeV) DOCUMENT ID TECN COMMENT 72 ± 10 1 GOPAL 77 DPWA K N multichannel 80 ± 30 2 BAILLON 75 IPWA K N → Λ π 80 3 KANE 72 DPWA K - p → Σ π Σ (1770) DECAY MODES Σ (1770) DECAY MODES Σ (1770)

88

Multichannel, time-resolved picosecond laser ultrasound imaging and spectroscopy with custom complementary metal-oxide-semiconductor detector  

SciTech Connect (OSTI)

This paper presents a multichannel, time-resolved picosecond laser ultrasound system that uses a custom complementary metal-oxide-semiconductor linear array detector. This novel sensor allows parallel phase-sensitive detection of very low contrast modulated signals with performance in each channel comparable to that of a discrete photodiode and a lock-in amplifier. Application of the instrument is demonstrated by parallelizing spatial measurements to produce two-dimensional thickness maps on a layered sample, and spectroscopic parallelization is demonstrated by presenting the measured Brillouin oscillations from a gallium arsenide wafer. This paper demonstrates the significant advantages of our approach to pump probe systems, especially picosecond ultrasonics.

Smith, Richard J.; Light, Roger A.; Johnston, Nicholas S.; Pitter, Mark C.; Somekh, Mike G. [Institute of Biophysics, Imaging and Optical Science, University of Nottingham, Nottinghamshire NG7 2RD (United Kingdom); Sharples, Steve D. [Applied Optics Group, Electrical Systems and Optics Research Division, University of Nottingham, Nottinghamshire NG7 2RD (United Kingdom)

2010-02-15T23:59:59.000Z

89

b006.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

6 6 N(2000) 5/2 + I (J P ) = 1 2 ( 5 2 + ) Status: ∗∗ OMITTED FROM SUMMARY TABLE Before the 2012 Review, all the evidence for a J P = 5/2 + state with NODE=B006 a mass above 1800 MeV was filed under a two-star N(2000). There is now some evidence from ANISOVICH 12A for two 5/2 + states in this region, so we have split the older data (according to mass) between two two-star 5/2 + states, an N(1860) and an N(2000). N(2000) BREIT-WIGNER MASS N(2000) BREIT-WIGNER MASS N(2000) BREIT-WIGNER MASS N(2000) BREIT-WIGNER MASS NODE=B006M NODE=B006M VALUE (MeV) DOCUMENT ID TECN COMMENT 1950 to 2150 (≈ 2050) OUR ESTIMATE 1950 to 2150 (≈ 2050) OUR ESTIMATE 1950 to 2150 (≈ 2050) OUR ESTIMATE 1950 to 2150 (≈ 2050) OUR ESTIMATE → UNCHECKED ← 2090 ± 120 ANISOVICH 12A DPWA Multichannel 2025 AYED 76 IPWA π N → π N 1970 1 LANGBEIN 73 IPWA π N → Σ K (sol. 2) 2175 ALMEHED 72 IPWA π N → π N 1930 DEANS 72 MPWA γ p →

90

b024.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

4 4 N(2120) 3/2 - I (J P ) = 1 2 ( 3 2 - ) Status: ∗∗ OMITTED FROM SUMMARY TABLE Before the 2012 Review, all the evidence for a J P = 3/2 - state NODE=B024 with a mass above 1800 MeV was filed under a two-star N(2080). There is now evidence from ANISOVICH 12A for two 3/2 - states in this region, so we have split the older data (according to mass) between a three-star N(1875) and a two-star N(2120). N(2120) BREIT-WIGNER MASS N(2120) BREIT-WIGNER MASS N(2120) BREIT-WIGNER MASS N(2120) BREIT-WIGNER MASS NODE=B024M NODE=B024M VALUE (MeV) DOCUMENT ID TECN COMMENT 2120 OUR ESTIMATE 2120 OUR ESTIMATE 2120 OUR ESTIMATE 2120 OUR ESTIMATE → UNCHECKED ← 2150 ± 60 ANISOVICH 12A DPWA Multichannel 2060 ± 80 1 CUTKOSKY 80 IPWA π N → π N 2081 ± 20 HOEHLER 79 IPWA π N → π N N(2120) BREIT-WIGNER WIDTH N(2120) BREIT-WIGNER WIDTH N(2120) BREIT-WIGNER WIDTH N(2120) BREIT-WIGNER WIDTH NODE=B024W NODE=B024W

91

b019.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

00) 00) 3/2 + I (J P ) = 3 2 ( 3 2 + ) Status: ∗∗∗ Most of the results published before 1975 are now obsolete and have been omitted. They may be found in our 1982 edition, Physics Let- ters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). The various analyses are not in good agreement. ∆(1600) BREIT-WIGNER MASS ∆(1600) BREIT-WIGNER MASS ∆(1600) BREIT-WIGNER MASS ∆(1600) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1500 to 1700 (≈ 1600) OUR ESTIMATE 1500 to 1700 (≈ 1600) OUR ESTIMATE 1500 to 1700 (≈ 1600) OUR ESTIMATE 1500 to 1700 (≈ 1600) OUR ESTIMATE 1510± 20 ANISOVICH 12A DPWA Multichannel 1600± 50 CUTKOSKY 80 IPWA π N → π N 1522± 13 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1626± 8 SHRESTHA 12A

92

b032.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

2 2 Σ (1620) 1/2 - I (J P ) = 1( 1 2 - ) Status: ∗ OMITTED FROM SUMMARY TABLE The S 11 state at 1697 MeV reported by VANHORN 75 is tentatively NODE=B032 listed under the Σ (1750). CARROLL 76 sees two bumps in the isospin-1 total cross section near this mass. GAO 12 sees no evidence for this resonance. Production experiments are listed separately in the next entry. Σ (1620) MASS Σ (1620) MASS Σ (1620) MASS Σ (1620) MASS NODE=B032M NODE=B032M VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 1620 OUR ESTIMATE ≈ 1620 OUR ESTIMATE ≈ 1620 OUR ESTIMATE ≈ 1620 OUR ESTIMATE → UNCHECKED ← 1600 ± 6 1 MORRIS 78 DPWA K - n → Λ π - 1608 ± 5 2 CARROLL 76 DPWA Isospin-1 total σ OCCUR=2 1633 ± 10 3 CARROLL 76 DPWA Isospin-1 total σ 1630 ± 10 LANGBEIN 72 IPWA K N multichannel 1620 KIM 71 DPWA K-matrix analysis Σ (1620) WIDTH Σ (1620) WIDTH Σ (1620) WIDTH Σ (1620) WIDTH NODE=B032W NODE=B032W VALUE (MeV) DOCUMENT

93

1266 IEEE JOURNAL OF SOLID-STATE CIRCUITS, VOL. 38, NO. 7, JULY 2003 A Multichannel Pipeline Analog-to-Digital Converter  

E-Print Network [OSTI]

1266 IEEE JOURNAL OF SOLID-STATE CIRCUITS, VOL. 38, NO. 7, JULY 2003 A Multichannel Pipeline Analog-channel 10-bit pipeline analog-to-digital con- verter, designed for use in an integrated three-interleaved pipeline paths, each operating at 80 MHz. The two parallel pipelines are subsequently multiplexed

Khuri-Yakub, Butrus T. "Pierre"

94

A modular architecture for multi-channel external cavity quantum cascade laser-based chemical sensors: a systems approach  

SciTech Connect (OSTI)

A multi-channel laser-based chemical sensor platform is presented, in which a modular architecture allows the exchange of complete sensor channels without disruption to overall operation. Each sensor channel contains custom optical and electronics packages, which can be selected to access laser wavelengths, interaction path lengths and modulation techniques optimal for a given application or mission. Although intended primarily to accommodate mid-infrared (MIR) external cavity quantum cascade lasers (ECQCLs)and astigmatic Herriott cells, channels using visible or near infrared (NIR) lasers or other gas cell architectures can also be used, making this a truly versatile platform. Analog and digital resources have been carefully chosen to facilitate small footprint, rapid spectral scanning, ow-noise signal recovery, failsafe autonomous operation, and in-situ chemometric data analysis, storage and transmission. Results from the demonstration of a two-channel version of this platform are also presented.

Taubman, Matthew S.; Myers, Tanya L.; Bernacki, Bruce E.; Stahl, Robert D.; Cannon, Bret D.; Schiffern, John T.; Phillips, Mark C.

2012-04-01T23:59:59.000Z

95

b014.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

4 4 N(1710) 1/2 + I (J P ) = 1 2 ( 1 2 + ) Status: ∗∗∗ Most of the results published before 1975 were last included in our NODE=B014 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. N(1710) BREIT-WIGNER MASS N(1710) BREIT-WIGNER MASS N(1710) BREIT-WIGNER MASS N(1710) BREIT-WIGNER MASS NODE=B014M NODE=B014M VALUE (MeV) DOCUMENT ID TECN COMMENT 1680 to 1740 (≈ 1710) OUR ESTIMATE 1680 to 1740 (≈ 1710) OUR ESTIMATE 1680 to 1740 (≈ 1710) OUR ESTIMATE 1680 to 1740 (≈ 1710) OUR ESTIMATE → UNCHECKED ← 1710 ± 20 ANISOVICH 12A DPWA Multichannel 1700 ± 50 CUTKOSKY 80 IPWA π N → π N 1723 ± 9 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits,

96

b030.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

0 0 ∆(1900) 1/2 - I (J P ) = 3 2 ( 1 2 - ) Status: ∗∗ OMITTED FROM SUMMARY TABLE Some obsolete results published before 1980 were last included in NODE=B030 our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. ∆(1900) BREIT-WIGNER MASS ∆(1900) BREIT-WIGNER MASS ∆(1900) BREIT-WIGNER MASS ∆(1900) BREIT-WIGNER MASS NODE=B030M NODE=B030M VALUE (MeV) DOCUMENT ID TECN COMMENT 1840 to 1920 (≈ 1860) OUR ESTIMATE 1840 to 1920 (≈ 1860) OUR ESTIMATE 1840 to 1920 (≈ 1860) OUR ESTIMATE 1840 to 1920 (≈ 1860) OUR ESTIMATE → UNCHECKED ← 1840 ± 30 ANISOVICH 12A DPWA Multichannel 1890 ± 50 CUTKOSKY 80 IPWA π N → π N 1908 ± 30 HOEHLER 79 IPWA π N → π N * * * We do not use the following

97

b030.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

0) 0) 1/2 - I (J P ) = 3 2 ( 1 2 - ) Status: ∗∗ OMITTED FROM SUMMARY TABLE Some obsolete results published before 1980 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. ∆(1900) BREIT-WIGNER MASS ∆(1900) BREIT-WIGNER MASS ∆(1900) BREIT-WIGNER MASS ∆(1900) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1840 to 1920 (≈ 1860) OUR ESTIMATE 1840 to 1920 (≈ 1860) OUR ESTIMATE 1840 to 1920 (≈ 1860) OUR ESTIMATE 1840 to 1920 (≈ 1860) OUR ESTIMATE 1840 ± 30 ANISOVICH 12A DPWA Multichannel 1890 ± 50 CUTKOSKY 80 IPWA π N → π N 1908 ± 30 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1868 ± 12 SHRESTHA

98

b117.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

7 7 ∆(1920) 3/2 + I (J P ) = 3 2 ( 3 2 + ) Status: ∗∗∗ Most of the results published before 1975 were last included in our NODE=B117 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. ∆(1920) BREIT-WIGNER MASS ∆(1920) BREIT-WIGNER MASS ∆(1920) BREIT-WIGNER MASS ∆(1920) BREIT-WIGNER MASS NODE=B117M NODE=B117M VALUE (MeV) DOCUMENT ID TECN COMMENT 1900 to 1970 (≈ 1920) OUR ESTIMATE 1900 to 1970 (≈ 1920) OUR ESTIMATE 1900 to 1970 (≈ 1920) OUR ESTIMATE 1900 to 1970 (≈ 1920) OUR ESTIMATE → UNCHECKED ← 1900 ± 30 ANISOVICH 12A DPWA Multichannel 1920 ± 80 CUTKOSKY 80 IPWA π N → π N 1868 ± 10 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages,

99

b018.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

00) 00) 3/2 - I (J P ) = 1 2 ( 3 2 - ) Status: ∗∗∗ Most of the results published before 1975 are now obsolete and have been omitted. They may be found in our 1982 edition, Physics Let- ters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). The various partial-wave analyses do not agree very well. The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. N(1700) BREIT-WIGNER MASS N(1700) BREIT-WIGNER MASS N(1700) BREIT-WIGNER MASS N(1700) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1650 to 1750 (≈ 1700) OUR ESTIMATE 1650 to 1750 (≈ 1700) OUR ESTIMATE 1650 to 1750 (≈ 1700) OUR ESTIMATE 1650 to 1750 (≈ 1700) OUR ESTIMATE 1790± 40 ANISOVICH 12A DPWA Multichannel 1675± 25 CUTKOSKY 80 IPWA π N → π N 1731± 15 HOEHLER 79 IPWA π N → π N * * * We do not use the

100

b017.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

7 7 N(1990) 7/2 + I (J P ) = 1 2 ( 7 2 + ) Status: ∗∗ OMITTED FROM SUMMARY TABLE Most of the results published before 1975 are now obsolete and have NODE=B017 been omitted. They may be found in our 1982 edition, Physics Let- ters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1984 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). The various analyses do not agree very well with one another. The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. N(1990) BREIT-WIGNER MASS N(1990) BREIT-WIGNER MASS N(1990) BREIT-WIGNER MASS N(1990) BREIT-WIGNER MASS NODE=B017M NODE=B017M VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 1990 OUR ESTIMATE ≈ 1990 OUR ESTIMATE ≈ 1990 OUR ESTIMATE ≈ 1990 OUR ESTIMATE → UNCHECKED ← 2060 ± 65 ANISOVICH 12A DPWA Multichannel 1970 ± 50 CUTKOSKY 80 IPWA π N → π N 2005 ± 150 HOEHLER 79 IPWA

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101

Fundamental studies on initiation and evolution of multi-channel discharges and their application to next generation pulsed power machines.  

SciTech Connect (OSTI)

Future pulsed power systems may rely on linear transformer driver (LTD) technology. The LTD's will be the building blocks for a driver that can deliver higher current than the Z-Machine. The LTD's would require tens of thousands of low inductance ( < 85nH), high voltage (200 kV DC) switches with high reliability and long lifetime ( 10 4 shots). Sandia's Z-Machine employs 36 megavolt class switches that are laser triggered by a single channel discharge. This is feasible for tens of switches but the high inductance and short switch life- time associated with the single channel discharge are undesirable for future machines. Thus the fundamental problem is how to lower inductance and losses while increasing switch life- time and reliability. These goals can be achieved by increasing the number of current-carrying channels. The rail gap switch is ideal for this purpose. Although those switches have been extensively studied during the past decades, each effort has only characterized a particular switch. There is no comprehensive understanding of the underlying physics that would allow predictive capability for arbitrary switch geometry. We have studied rail gap switches via an extensive suite of advanced diagnostics in synergy with theoretical physics and advanced modeling capability. Design and topology of multichannel switches as they relate to discharge dynamics are investigated. This involves electrically and optically triggered rail gaps, as well as discrete multi-site switch concepts.

Schwarz, Jens; Savage, Mark E.; Lucero, Diego Jose; Jaramillo, Deanna M.; Seals, Kelly Gene; Pitts, Todd; Hautzenroeder, Brenna M.; Laine, Mark Richard; Karelitz, David B.; Porter, John L.

2014-09-01T23:59:59.000Z

102

The Use of a Multichannel Analyzer to Investigate Effects of Experimental Factors on Gross-Counting Gamma and Neutron Detectors  

SciTech Connect (OSTI)

Radiation detection technology is invaluable to many fields of study in identifying nuclear materials. However, many detectors use gross-counting methods that give only a relative count rate. Without a spectrum (information on counts over time vs energy), it can be more difficult to discern if an alarm is false, innocent, or real. In particular, we would like to understand better the effect of experimental factors (i.e., external conditions and equipment parameters) on detector data, with possible implications for false alarms. To more thoroughly characterize detector technology, a multichannel analyzer (MCA) was used to record spectra from neutron (helium-3 tubes) and gamma (photomultiplier tubes) gross-counting detectors. Several factors could affect the signal-to-noise ratio of sources. For example, we examined the effects of neutron detector high voltage setting on the appearance of a californium-252 spectrum, the effect of discriminator values on integrated counts in neutron detection, and the effect of gain changes on the gamma spectra from several sources. Possible implications of ambient temperature of the experiment on the data collected will be discussed. The input impedance of the MCA must be considered to ensure that data are not affected by the measurement itself. Moreover, a calibration on the MCA was performed to verify the conversion of a MCA channel number to a voltage. In summary, the series of source spectra collected on an MCA with a variety of experimental conditions allow us to understand factors that affect data better, and assure us that gross-counting neutron and gamma detectors will have minimal false alarms.

Volz, Heather M. [Los Alamos National Laboratory; Rennie, John A. [Los Alamos National Laboratory; Lovejoy, Christopher M. [Los Alamos National Laboratory; Martinez, Diana E. R [Los Alamos National Laboratory; Dempsey, Michael A. [Los Alamos National Laboratory; Livesay, Jake [ORNL; Lousteau, Angela [ORNL

2012-07-12T23:59:59.000Z

103

Extended Coulomb approximation for multichannel-quantum-defect-theory computations of dipole moments:?Method of calculation and application to H2  

Science Journals Connector (OSTI)

A method for calculating dipole transition moments in effective one-electron systems when some channels are closed is investigated within the framework of multichannel quantum-defect theory (MQDT). A treatment of the energy dependence is also given. This method is useful when electronic channel interactions occur and MQDT is combined with frame transformations. Our calculations are made in the Coulomb approximation and include provisions for core transitions. They are tested by comparing transitions between bound states of molecular hydrogen with ab initio computations.

A. Matzkin; Ch. Jungen; S. C. Ross

1998-12-01T23:59:59.000Z

104

Multichannel response analysis on 2D projection views for detection of clustered microcalcifications in digital breast tomosynthesis  

SciTech Connect (OSTI)

Purpose: To investigate the feasibility of a new two-dimensional (2D) multichannel response (MCR) analysis approach for the detection of clustered microcalcifications (MCs) in digital breast tomosynthesis (DBT). Methods: With IRB approval and informed consent, a data set of two-view DBTs from 42 breasts containing biopsy-proven MC clusters was collected in this study. The authors developed a 2D approach for MC detection using projection view (PV) images rather than the reconstructed three-dimensional (3D) DBT volume. Signal-to-noise ratio (SNR) enhancement processing was first applied to each PV to enhance the potential MCs. The locations of MC candidates were then identified with iterative thresholding. The individual MCs were decomposed with HermiteGaussian (HG) and LaguerreGaussian (LG) basis functions and the channelized Hotelling model was trained to produce the MCRs for each MC on the 2D images. The MCRs from the PVs were fused in 3D by a coincidence counting method that backprojects the MC candidates on the PVs and traces the coincidence of their ray paths in 3D. The 3D MCR was used to differentiate the true MCs from false positives (FPs). Finally a dynamic clustering method was used to identify the potential MC clusters in the DBT volume based on the fact that true MCs of clinical significance appear in clusters. Using two-fold cross validation, the performance of the 3D MCR for classification of true and false MCs was estimated by the area under the receiver operating characteristic (ROC) curve and the overall performance of the MCR approach for detection of clustered MCs was assessed by free response receiver operating characteristic (FROC) analysis. Results: When the HG basis function was used for MCR analysis, the detection of MC cluster achieved case-based test sensitivities of 80% and 90% at the average FP rates of 0.65 and 1.55 FPs per DBT volume, respectively. With LG basis function, the average FP rates were 0.62 and 1.57 per DBT volume at the same sensitivity levels. The difference in the two sets of basis functions for detection of MCs did not show statistical significance. Conclusions: The authors' experimental results indicate that the MCR approach is promising for the detection of MCs on PV images. The HG or LG basis functions are both effective in characterizing the signal response of MCs using the channelized Hotelling model. The coincidence counting method for fusion of the 2D MCR in 3D is an important step for FP reduction. Further study is underway to improve the MCR approach for microcalcification detection in DBT.

Wei, Jun, E-mail: jvwei@umich.edu; Chan, Heang-Ping; Hadjiiski, Lubomir M.; Helvie, Mark A.; Lu, Yao; Zhou, Chuan; Samala, Ravi [Department of Radiology, University of Michigan, Ann Arbor, Michigan 48109-5842 (United States)] [Department of Radiology, University of Michigan, Ann Arbor, Michigan 48109-5842 (United States)

2014-04-15T23:59:59.000Z

105

b041.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

00) 00) 7/2 - I (J P ) = 0( 7 2 - ) Status: ∗∗∗∗ Discovered by COOL 66 and by WOHL 66. Most of the results published before 1973 are now obsolete and have been omitted. They may be found in our 1982 edition Physics Letters 111B 111B 111B 111B 1 (1982). This entry only includes results from partial-wave analyses. Param- eters of peaks seen in cross sections and in invariant-mass distribu- tions around 2100 MeV used to be listed in a separate entry immedi- ately following. It may be found in our 1986 edition Physics Letters 170B 170B 170B 170B 1 (1986). Λ(2100) MASS Λ(2100) MASS Λ(2100) MASS Λ(2100) MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 2090 to 2110 (≈ 2100) OUR ESTIMATE 2090 to 2110 (≈ 2100) OUR ESTIMATE 2090 to 2110 (≈ 2100) OUR ESTIMATE 2090 to 2110 (≈ 2100) OUR ESTIMATE 2104± 10 GOPAL 80 DPWA K N → K N 2106± 30 DEBELLEFON 78 DPWA K N → K N 2110± 10 GOPAL 77 DPWA K N multichannel 2105±

106

b046.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

15) 15) 5/2 + I (J P ) = 1( 5 2 + ) Status: ∗∗∗∗ Discovered by COOL 66. For results published before 1974 (they are now obsolete), see our 1982 edition Physics Letters 111B 111B 111B 111B 1 (1982). This entry only includes results from partial-wave analyses. Parame- ters of peaks seen in cross sections and invariant-mass distributions in this region used to be listed in in a separate entry immediately following. They may be found in our 1986 edition Physics Letters 170B 170B 170B 170B 1 (1986). Σ (1915) MASS Σ (1915) MASS Σ (1915) MASS Σ (1915) MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1900 to 1935 (≈ 1915) OUR ESTIMATE 1900 to 1935 (≈ 1915) OUR ESTIMATE 1900 to 1935 (≈ 1915) OUR ESTIMATE 1900 to 1935 (≈ 1915) OUR ESTIMATE 1937± 20 ALSTON-... 78 DPWA K N → K N 1894± 5 1 CORDEN 77C K - n → Σ π 1909± 5 1 CORDEN 77C K - n → Σ π 1920± 10 GOPAL 77 DPWA K N multichannel 1900± 4 2 CORDEN 76 DPWA

107

b047.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

7 7 Σ (2030) 7/2 + I (J P ) = 1( 7 2 + ) Status: ∗∗∗∗ Discovered by COOL 66 and by WOHL 66. For most results pub- NODE=B047 lished before 1974 (they are now obsolete), see our 1982 edition Physics Letters 111B 111B 111B 111B 1 (1982). This entry only includes results from partial-wave analyses. Parame- ters of peaks seen in cross sections and invariant-mass distributions around 2030 MeV may be found in our 1984 edition, Reviews of Modern Physics 56 56 56 56 S1 (1984). Σ (2030) MASS Σ (2030) MASS Σ (2030) MASS Σ (2030) MASS NODE=B047M NODE=B047M VALUE (MeV) DOCUMENT ID TECN COMMENT 2025 to 2040 (≈ 2030) OUR ESTIMATE 2025 to 2040 (≈ 2030) OUR ESTIMATE 2025 to 2040 (≈ 2030) OUR ESTIMATE 2025 to 2040 (≈ 2030) OUR ESTIMATE → UNCHECKED ← 2036 ± 5 GOPAL 80 DPWA K N → K N 2038 ± 10 CORDEN 77B K - N → N K ∗ 2040 ± 5 GOPAL 77 DPWA K N multichannel 2030 ± 3 1 CORDEN 76 DPWA K - n → Λ π - 2035 ± 15 BAILLON

108

Masked multichannel analyzer  

DOE Patents [OSTI]

An analytical instrument and particularly a time-of-flight-mass spectrometer for processing a large number of analog signals irregularly spaced over a spectrum, with programmable masking of portions of the spectrum where signals are unlikely in order to reduce memory requirements and/or with a signal capturing assembly having a plurality of signal capturing devices fewer in number than the analog signals for use in repeated cycles within the data processing time period.

Winiecki, Alan L. (Downers Grove, IL); Kroop, David C. (Columbia, MD); McGee, Marilyn K. (Colorado Springs, CO); Lenkszus, Frank R. (Woodridge, IL)

1986-01-01T23:59:59.000Z

109

Essays on multichannel marketing  

E-Print Network [OSTI]

Results?????????????????????.. 98 3.3 Predictive Validity for Catalog Only Customer-Channel Segment???... 100 3.4 Predictive Validity for Store Only Customer-Channel Segment???....... 102 3.5 Predictive Validity for Web Only Customer...?????????????????????? 97 3.7 Profitability Decomposition???????????????????. 108 1 CHAPTER I INTRODUCTION There?s not a customer who wants to shop just by catalog or just by store. Everybody has different needs and those needs may even differ depending...

Kushwaha, Tarun Lalbahadur

2009-05-15T23:59:59.000Z

110

Multichannel homodyne receiver  

DOE Patents [OSTI]

A homodyne radar transmitter/receiver device which produces a single combined output which contains modulated backscatter information for all phase conditions of both modulated and unmodulated backscatter signals. The device utilizes taps along coaxial transmission lines, strip transmission line, and waveguides which are spaced by 1/8 wavelength or 1/6 wavelength, etc. This greatly reduces costs by eliminating separate transmission and reception antennas and an expensive arrangement of power splitters and mixers utilized in the prior art.

Landt, Jeremy A. (Los Alamos, NM)

1982-01-01T23:59:59.000Z

111

CEWEP -Confederation of European Waste-to-Energy Plants Boulevard Clovis 12A  

E-Print Network [OSTI]

CEWEP - Confederation of European Waste-to- Energy Plants Boulevard Clovis 12A B-1000 Brussels Tel. : +32 (0)2 770 63 11 Fax : +32 (0)2 770 68 14 info@cewep.eu www.cewep.eu 1 Waste-to-Energy: towards recovery CEWEP welcomes that `energy recovery' should cover the use of waste for generating energy through

Columbia University

112

Genome Sequence of Pseudomonas putida S12, a Potential Platform Strain for Industrial Production of Valuable Chemicals  

Science Journals Connector (OSTI)

...S12, a Potential Platform Strain for Industrial...Production of Valuable Chemicals Fei Tao a Yaling...is considered a platform strain for the production of many chemicals. Here, we present...S12, a potential platform strain for industrial...production of valuable chemicals. | Pseudomonas...

Fei Tao; Yaling Shen; Ziqi Fan; Hongzhi Tang; Ping Xu

2012-11-01T23:59:59.000Z

113

Pion correlations for 1.2A GeV lanthanum on lanthanum  

Science Journals Connector (OSTI)

Results are presented for pion interferometry measurements of 1.2A GeV La+La at the Lawrence Berkeley Laboratory Heavy Ion Spectrometer System. The experiments acceptance is at forward angles in the center-of-mass system. The fit parameters R, ?, ?, R?, and R? are presented. The extracted shape of the pion source is oblate. The correlation between the extracted size of the pion source and the centrality of the collision is investigated as well as the dependence of the source size on the mean momentum of the pion pairs. We conclude that the fitted radius parameters scale with mass for symmetric systems. We observe a dependence of the fitted size of the pion source on the mean momentum of the pion pairs. Comparisons are made with previous results.

W. B. Christie; D. L. Olson; C. E. Tull; F. P. Brady; G. P. Grim; J. H. Osborne; M. L. Partlan; J. L. Romero; J. Chang; S. Y. Fung; J. Kang; S. Zhang; D. Keane; D. Beavis; Y. Dardenne

1993-02-01T23:59:59.000Z

114

PREGO ELETRNICO N 11/2012 =SRP VALIDADE 26/06/12 a 25/06/13  

E-Print Network [OSTI]

PREG?O ELETR?NICO Nº 11/2012 =SRP VALIDADE 26/06/12 a 25/06/13 AQUISI??O DE CARTUCHO DE TONER e

Paraná, Universidade Federal do

115

Magnetic properties of MoS2: Existence of ferromagnetism Sefaattin Tongay,1,2,a),b)  

E-Print Network [OSTI]

Magnetic properties of MoS2: Existence of ferromagnetism Sefaattin Tongay,1,2,a),b) Sima S 4 September 2012; published online 18 September 2012) We report on the magnetic properties of MoS2 measured from room temperature down to 10K and magnetic fields up to 5 T. We find that single crystals

Wu, Junqiao

116

Fire and Emergency Management Group SLAC-I-730-0A12A-001-R000  

E-Print Network [OSTI]

Fire and Emergency Management Group SLAC-I-730-0A12A-001-R000 Fire Protection System Impairment NFPA National Fire Protection Association SLAC Stanford Linear Accelerator Center SSO DOE Stanford Site000 iii #12;#12;1 Introduction This document describes the fire protection system impairment program

Wechsler, Risa H.

117

Doping-induced metal-insulator transition in aluminum-doped 4H silicon P. Achatz,1,2,a  

E-Print Network [OSTI]

Doping-induced metal-insulator transition in aluminum-doped 4H silicon carbide P. Achatz,1,2,a J an experimental determination of the doping-induced metal-insulator transition in aluminum-doped 4H silicon concentration lying between 6.4 and 8.7 1020 cm-3 for the metal-insulator transition in these epilayers grown

Paris-Sud XI, Université de

118

Data:244cda0a-21fd-4059-889a-12a0147a129b | Open Energy Information  

Open Energy Info (EERE)

a-21fd-4059-889a-12a0147a129b a-21fd-4059-889a-12a0147a129b No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Monroe, North Carolina (Utility Company) Effective date: 2013/06/01 End date if known: Rate name: Schedule TS - Traffic Signal Service Sector: Lighting Description: Source or reference: http://www.monroenc.org/services.php?cat=150 Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous

119

Data:1844e12d-12a3-4722-a554-be3c170bffaa | Open Energy Information  

Open Energy Info (EERE)

e12d-12a3-4722-a554-be3c170bffaa e12d-12a3-4722-a554-be3c170bffaa No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Tell City, Indiana (Utility Company) Effective date: 2008/07/01 End date if known: Rate name: Tariff A1: Single Phase Residential, Greater Than 200 Amps and Less Than 400 Amps Sector: Residential Description: The charges derived in the Tariff A1 rate are subject to adjustment for: Purchased Power Adjustment Tracking Factor. Source or reference: Rates Binder 1, Illinois State University Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months):

120

Data:33d1657d-8616-4475-94a0-e6ed12a79571 | Open Energy Information  

Open Energy Info (EERE)

d1657d-8616-4475-94a0-e6ed12a79571 d1657d-8616-4475-94a0-e6ed12a79571 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Village of Belmont, Wisconsin (Utility Company) Effective date: 2005/01/21 End date if known: Rate name: Rg-1 Residential Service Single Phase Sector: Residential Description: This rate will be applied to residential single phase customers for ordinary household purposes. Single-Phase motors may not exceed 5 horsepower individual-rated capacity without utility permission. Fixed Monthly Charge includes Commitment to Community Rider: $1.00 per customer per month Source or reference: http://psc.wi.gov/apps40/tariffs/viewfile.aspx?type=electric&id=440

Note: This page contains sample records for the topic "12a dpwa multichannel" from the National Library of EnergyBeta (NLEBeta).
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121

b132.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

00) 00) 1/2 + I (J P ) = 1 2 ( 1 2 + ) Status: ∗ OMITTED FROM SUMMARY TABLE The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. N(2100) BREIT-WIGNER MASS N(2100) BREIT-WIGNER MASS N(2100) BREIT-WIGNER MASS N(2100) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 2100 OUR ESTIMATE ≈ 2100 OUR ESTIMATE ≈ 2100 OUR ESTIMATE ≈ 2100 OUR ESTIMATE 2125± 75 CUTKOSKY 80 IPWA π N → π N 2050± 20 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 2157± 42 BATINIC 10 DPWA π N → N π, N η 2068± 3 + 15 - 40 ABLIKIM 06K BES2 J/ψ → (p π - ) n 2084± 93 VRANA 00 DPWA Multichannel 1986± 26 + 10 - 30 PLOETZKE 98 SPEC γ p → p η ' (958) N(2100) BREIT-WIGNER WIDTH N(2100) BREIT-WIGNER WIDTH N(2100) BREIT-WIGNER WIDTH N(2100) BREIT-WIGNER WIDTH VALUE (MeV) DOCUMENT ID TECN COMMENT 260± 100 CUTKOSKY 80 IPWA π N → π N 200± 30 HOEHLER

122

Determination of the binding energies of the np Rydberg states of H{sub 2}, HD, and D{sub 2} from high-resolution spectroscopic data by multichannel quantum-defect theory  

SciTech Connect (OSTI)

Multichannel quantum-defect theory (MQDT) is used to calculate the electron binding energies of np Rydberg states of H{sub 2}, HD, and D{sub 2} around n = 60 at an accuracy of better than 0.5?MHz. The theory includes the effects of rovibronic channel interactions and the hyperfine structure, and has been extended to the calculation of the asymmetric hyperfine structure of Rydberg states of a heteronuclear diatomic molecule (HD). Starting values for the eigenquantum-defect parameters of MQDT were extracted from ab initio potential-energy functions for the low-lying p Rydberg states of molecular hydrogen and subsequently refined in a global weighted fit to available experimental data on the singlet and triplet Rydberg states of H{sub 2} and D{sub 2}. The electron binding energies of high-np Rydberg states derived in this work represent important quantities for future determinations of the adiabatic ionization energies of H{sub 2}, HD, and D{sub 2} at sub-MHz accuracy.

Sprecher, Daniel; Merkt, Frdric, E-mail: frederic.merkt@phys.chem.ethz.ch [Laboratorium fr Physikalische Chemie, ETH-Zrich, 8093 Zrich (Switzerland)] [Laboratorium fr Physikalische Chemie, ETH-Zrich, 8093 Zrich (Switzerland); Jungen, Christian [Laboratoire Aim Cotton du CNRS, Universit de Paris-Sud, 91405 Orsay (France)] [Laboratoire Aim Cotton du CNRS, Universit de Paris-Sud, 91405 Orsay (France)

2014-03-14T23:59:59.000Z

123

Ultrafast terahertz-induced response of GeSbTe phase-change materials Michael J. Shu,1,2,a)  

E-Print Network [OSTI]

Ultrafast terahertz-induced response of GeSbTe phase-change materials Michael J. Shu,1,2,a) Peter-optically, pumping with single-cycle terahertz pulses as a means of biasing phase-change materials on a sub of these materials is important for predicting the field-driven heating and phase-change behavior. However

124

Data:B04aa56c-12a5-43dc-86dd-3355e2a5cd72 | Open Energy Information  

Open Energy Info (EERE)

6c-12a5-43dc-86dd-3355e2a5cd72 6c-12a5-43dc-86dd-3355e2a5cd72 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Wild Rice Electric Coop, Inc Effective date: 2012/03/18 End date if known: Rate name: FARM AND HOME SERVICE - Up to 15 KVA transformer Sector: Residential Description: Source or reference: http://www.wildriceelectric.com/b-rate.html Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous

125

Data:7e12a3cc-a6ed-40c3-acfc-dffb0212ba16 | Open Energy Information  

Open Energy Info (EERE)

7e12a3cc-a6ed-40c3-acfc-dffb0212ba16 7e12a3cc-a6ed-40c3-acfc-dffb0212ba16 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Moorhead, Minnesota (Utility Company) Effective date: End date if known: Rate name: Small General Service/General Service: Dual-Fuel Sector: Commercial Description: Available to Small General Service and General Service customers in conformance with Moorhead Public Service' Source or reference: http://www.mpsutility.com/images/stories/rates/2013/Electric%20Rates.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh)

126

Data:B04adc72-6615-4040-901d-e4a8b12a0385 | Open Energy Information  

Open Energy Info (EERE)

2-6615-4040-901d-e4a8b12a0385 2-6615-4040-901d-e4a8b12a0385 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Johnson City, Tennessee (Utility Company) Effective date: 2012/08/01 End date if known: Rate name: STREET LIGHTING Sector: Lighting Description: Source or reference: http://www.jcpb.com/yourBusiness/meters/rates.asp#rateSheet Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous

127

Data:D5afa075-e887-4728-97a1-2a2bc811845d | Open Energy Information  

Open Energy Info (EERE)

afa075-e887-4728-97a1-2a2bc811845d afa075-e887-4728-97a1-2a2bc811845d No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Rochester Public Utilities Effective date: 2009/01/01 End date if known: Rate name: SECURITY LIGHTING(250 Watt HPS) Sector: Lighting Description: At all locations whenever the service can be provided with overhead wiring on an existing RPU owned pole. Source or reference: http://www.rpu.org/documents/2012_rate_schedule.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage

128

Data:Ad262f27-c738-4d12-a3a0-0c0b5f53221a | Open Energy Information  

Open Energy Info (EERE)

62f27-c738-4d12-a3a0-0c0b5f53221a 62f27-c738-4d12-a3a0-0c0b5f53221a No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Singing River Elec Pwr Assn (Mississippi) Effective date: 2009/12/04 End date if known: Rate name: Security Lighting MV 175 W Post Top (Includes Pole) Sector: Lighting Description: *Subject to power cost adjustment, tax expense adjustment, and an environmental compliance charge. Source or reference: http://www.singingriver.com/Files/R-18.pdf Source Parent: Comments Energy Adjustment is Power Cost Adjustment plus Environmental Clause plus Regulatory Adjustment Applicability Demand (kW)

129

Data:F1983099-90dc-4b12-a937-bc3c29638f2d | Open Energy Information  

Open Energy Info (EERE)

99-90dc-4b12-a937-bc3c29638f2d 99-90dc-4b12-a937-bc3c29638f2d No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Mt Carmel Public Utility Co Effective date: End date if known: Rate name: Residential Sector: Residential Description: AVAILABILITY Available for any customer for Company's standard service for residential purposes. Where a residence and business are combined in one premise, the service classification shall be determined by the predominant electric use at the premise. Source or reference: http://www.mtcpu.com/includes/tariff_electric.htm?t=Residential_Electric_Service Source Parent:

130

Data:Dd3d2c12-a21e-43ef-a56f-eec753ee1976 | Open Energy Information  

Open Energy Info (EERE)

c12-a21e-43ef-a56f-eec753ee1976 c12-a21e-43ef-a56f-eec753ee1976 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Choctaw Electric Coop Inc Effective date: 2008/10/21 End date if known: Rate name: Choctaw Nation Senior Citizens Center Sector: Commercial Description: * Available to the Choctaw Nation for multi-building complexes having electric space heating where more than one building is served from a single transformer. Electric service shall be billed to and paid by the Choctaw Nation on one monthly bill. Subject to Tax Adjustment. Source or reference: Rate binder # 4 Source Parent: Comments

131

Data:1eed3a36-f12a-4353-b92b-d5c5c0281e45 | Open Energy Information  

Open Energy Info (EERE)

eed3a36-f12a-4353-b92b-d5c5c0281e45 eed3a36-f12a-4353-b92b-d5c5c0281e45 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Three Notch Elec Member Corp Effective date: 2012/03/01 End date if known: Rate name: 175 Mercury vapor with Underground Wiring- (Type - 'MV-Open', Fiberglass Pole) Sector: Lighting Description: Applicable only for dusk to dawn lighting by means of photo-electric controlled, ballast operated vapor lamp luminaries and poles conforming to the Cooperative's specifications. Service will be rendered only at locations that, solely in the opinion of the Cooperative, are readily accessible for installation and maintenance.

132

Interferometric Multichannel Analysis of Surface Waves (IMASW)  

Science Journals Connector (OSTI)

...Number 08HQGR0068 and by the Department of Energy (DOE) under award number DE-EE0002758 with the disclaimer http://apps1.eere.energy.gov/buildings/tools_directory/disclaimer.cfm (last accessed June 2011). References Abrahamson, N...

Daniel R. H. OConnell; James P. Turner

133

Digitally Assisted Multi-Channel Receivers  

E-Print Network [OSTI]

-channel charge sampling receivers with sinc filter banks together with a complete system calibration and synchronization algorithm for the receiver. A unified model has been defined for the receiver containing all first order mismatches, offsets... and imperfections and a technique based on least mean squares algorithm is employed to track these errors. The performance of this technique under noisy channel conditions has been verified. The sinc filter bank is compared with the conventional analog filter...

Pentakota, Krishna Anand Santosh Spikanth

2011-10-21T23:59:59.000Z

134

Study I: Effectiveness of Multichannel Online Advertising  

Science Journals Connector (OSTI)

Chapter 2 shows that consumers increasingly use the Internet to purchase goods and services. To benefit from this growth, firms increasingly invest in digital advertising, and budgets have climbed steadily over t...

Sebastian Klapdor

2013-01-01T23:59:59.000Z

135

Multichannel chiral approach for kaonic hydrogen  

E-Print Network [OSTI]

We present an exact solution to the $K^{-}$-proton bound state problem formulated in the momentum space. The 1s level characteristics of the kaonic hydrogen are described together with the available low energy $\\bar{K}N$ data.

A. Cieply; J. Smejkal

2007-10-22T23:59:59.000Z

136

Investigation of the ultrasonic wave influence on magnetic ordering in a 20 x [Fe(20 A)/Cr(12 A)]/MgO layered structure  

SciTech Connect (OSTI)

A 20 x [Fe(20 A)/Cr (12 A)]/MgO structure excited by an ultrasonic wave was investigated by polarized neutron reflectometry. It was found that magnetic domains oscillate and their effective size decreases in weak magnetic fields. In close-to-saturation fields, a magnetic lattice is formed in the layered structure; the interplanar spacings in this lattice change with an increase in the field strength and as a result of the excitation of the structure by an ultrasonic wave.

Aksenov, V. L.; Nikitenko, Yu. V.; Proglyado, V. V.; Khaidukov, Yu. N., E-mail: khaiduk@nf.jinr.ru [Joint Institute for Nuclear Research (Russian Federation); Gavrilov, V. N.; Raitman, E. [Institute of Physical Energetics (Latvia); Bottyan, L.; Nagy, D. L. [Research Institute for Particle and Nuclear Physics (Hungary)

2008-09-15T23:59:59.000Z

137

c12a.xls  

Gasoline and Diesel Fuel Update (EIA)

1,522 3,228 1,772 18,031 33,384 20,243 84.4 96.7 87.6 Building Floorspace (Square Feet) 1,001 to 5,000 ................................. 193 300 193 2,168 2,904 1,850 89.0 103.2 104.2 5,001 to 10,000 ............................... 134 263 165 2,032 3,217 1,784 66.0 81.9 92.5 10,001 to 25,000 ............................. 241 432 226 3,273 5,679 3,707 73.6 76.1 60.9 25,001 to 50,000 ............................. 181 370 191 2,517 4,518 2,347 71.8 81.8 81.5 50,001 to 100,000 ............................ 156 473 285 2,095 4,763 3,433 74.3 99.3 82.9 100,001 to 200,000 .......................... 219 523 323 2,161 4,706 3,350 101.1 111.1 96.5 200,001 to 500,000 .......................... 221 371 160 2,179 3,623 1,692 101.4 102.3 94.3 Over 500,000 ................................... 179 497 Q 1,606 3,974 2,080 111.2 125.0 Q Principal Building Activity

138

Data:Bb1cc354-27f0-4e38-a12a-449df422b2f6 | Open Energy Information  

Open Energy Info (EERE)

cc354-27f0-4e38-a12a-449df422b2f6 cc354-27f0-4e38-a12a-449df422b2f6 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Miami-Cass County Rural E M C Effective date: 2011/10/01 End date if known: Rate name: Security Lights Metered 250 watt high pressure sodium Sector: Lighting Description: The Miami-Cass County Rural Electric Membership Corporation (REMC) shall charge and collect for security lighting service on the following bases of availability, character of service, monthly rate, and tax adjustment. AVAILABILITY: Available to any member of the REMC for continuous year round service for outdoor lighting where 120 volt service exists ahead of the meter loop.

139

Data:37cfd1b4-12a3-480f-ba5b-79db36229eec | Open Energy Information  

Open Energy Info (EERE)

cfd1b4-12a3-480f-ba5b-79db36229eec cfd1b4-12a3-480f-ba5b-79db36229eec No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Groton, South Dakota (Utility Company) Effective date: End date if known: Rate name: Schedule C - HEAT METER Geothermal/Heat Pump Rates Sector: Residential Description: #2 Heat Meter - All kwh at $.08 per kwh Minimum 10 kw resistance backup. Source or reference: http://city.grotonsd.gov/electric.html Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V):

140

Data:0c7149ef-adf6-42a7-963d-4b12a98d024d | Open Energy Information  

Open Energy Info (EERE)

ef-adf6-42a7-963d-4b12a98d024d ef-adf6-42a7-963d-4b12a98d024d No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Duke Energy Ohio Inc Effective date: 2013/05/06 End date if known: Rate name: Rate OL - Outdoor Lighting Service - MV 400 Watts Sector: Lighting Description: Applicable for outdoor lighting services on private property with Company owned fixtures in the Company's entire service area where secondary distribution lines are adjacent to the premises to be served. Not applicable for lighting public roadways which are dedicated, or anticipated to be dedicated, except to meet the occasional singular need of a customer who has obtained written approval from the proper governmental authority.

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

Data:638bc389-fb01-4b31-96a5-0c12a8e0261b | Open Energy Information  

Open Energy Info (EERE)

bc389-fb01-4b31-96a5-0c12a8e0261b bc389-fb01-4b31-96a5-0c12a8e0261b No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Nevada Power Co Effective date: 2013/01/01 End date if known: Rate name: OLGS-1-TOU (Large General Service Time-Of-Use) Sector: Commercial Description: Optional for non-Domestic Service where consumption of energy exceeds 3,500 kWh in any one month, where the Billing Demand is equal to or less than 299 kW in any one month and where time-of-use pricing is requested by the Customer. All service will be supplied at one Point of Delivery and measured through one kilowatthour Meter. Not applicable to standby, resale, temporary, shared, or mixed class of service. Not applicable to supplemental service unless the Customer is a Qualifying Facility under Title 18, Code of Federal Regulations, Section 292.201 through 292.207. This schedule is limited to the addition of 1,000 new Customers per month on all optional time-of-use schedules.

142

Data:Eac1dd3a-0268-4e5c-b1d1-ed9feeb2a12a | Open Energy Information  

Open Energy Info (EERE)

dd3a-0268-4e5c-b1d1-ed9feeb2a12a dd3a-0268-4e5c-b1d1-ed9feeb2a12a No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Ameren Illinois Company Effective date: 2010/11/19 End date if known: Rate name: DS-2 and BGS-2 Zone 2 - Bundled Small General Delivery Service 600V or Less Sector: Commercial Description: AVAILABILITY Service under this Rate is available for any eligible Non-Residential Customer within the territory served by Company that meets the following criteria: Customers served under this Rate shall have a maximum monthly Demand of less than 150 kilowatts (kW) as qualified in the Delivery Service Rate Reassignment section. A Customer without a demand meter installed, but with an average usage of less than 1,200 kWh per day during each monthly billing period will be normally assumed to have a maximum monthly Demand of less than 150 kW. Where Customer's average daily usage is 1,200 kWh per day or more in any monthly billing period, Company may install a demand meter at Company's expense to determine if Customer remains eligible for service under this Rate.

143

Data:4bb12a66-235d-4b62-8af0-1e344385ee34 | Open Energy Information  

Open Energy Info (EERE)

4bb12a66-235d-4b62-8af0-1e344385ee34 4bb12a66-235d-4b62-8af0-1e344385ee34 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Electric Coop, Inc (Florida) Effective date: End date if known: Rate name: Outdoor Lighting MHF 400 W Sector: Lighting Description: Source or reference: http://www.tcec.com/myBusiness/resSinglePhase.aspx Source Parent: http://www.tcec.com/ Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous

144

Data:8100a82f-3ccb-4ce5-b6dc-12a267a595c1 | Open Energy Information  

Open Energy Info (EERE)

0a82f-3ccb-4ce5-b6dc-12a267a595c1 0a82f-3ccb-4ce5-b6dc-12a267a595c1 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Wahoo, Nebraska (Utility Company) Effective date: 2012/02/01 End date if known: Rate name: Industrial Large General Service (Three Phase) Sector: Industrial Description: Source or reference: http://www.wahoo.ne.us/content_subcat.asp?SubCategoryID=88&CategoryID=125&ContentID=68 Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V):

145

Data:5820ba98-12a4-4dd7-a83b-c3350ad462a2 | Open Energy Information  

Open Energy Info (EERE)

ba98-12a4-4dd7-a83b-c3350ad462a2 ba98-12a4-4dd7-a83b-c3350ad462a2 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Orange & Rockland Utils Inc Effective date: 2012/04/01 End date if known: Rate name: SC16 Street Lighting Induction Overhead and Underground 70w (Customer owned, retail service, multiple bills) Sector: Description: APPLICABLE TO USE OF SERVICE FOR: Sales and delivery of electric power supply provided by the Company or delivery of electric power supply provided by an Energy Service Company under the Company's Retail Access Program for outdoor lighting of areas, beyond the limits of public streets, highways or roadways, for use of individuals and private or public organizations where existing distribution facilities are suitable for the service requested.

146

Data:420fb714-7054-49c9-8b1f-f07dac56b12a | Open Energy Information  

Open Energy Info (EERE)

14-7054-49c9-8b1f-f07dac56b12a 14-7054-49c9-8b1f-f07dac56b12a No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: KEM Electric Coop Inc Effective date: End date if known: Rate name: Electric Heat Service -7 M Sector: Residential Description: Available to all members under SE-1, where electric heat is the primary source of heating. Service shall be to a single point of service Type of Service Single Phase, 60 cycle, at secondary voltages. The Cooperative will provide meter, meter socket, and C.T. equipment necessary to measure electric usage. Source or reference: http://www.kemelectric.com/Customer_Service/Rate_Schedules/Schedule%20EH-7M/index.html

147

Data:De12a8fe-13b5-4491-9139-ea729b96ec3d | Open Energy Information  

Open Energy Info (EERE)

De12a8fe-13b5-4491-9139-ea729b96ec3d De12a8fe-13b5-4491-9139-ea729b96ec3d No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Seattle, Washington (Utility Company) Effective date: 2012/01/01 End date if known: Rate name: Schedule LGB-Large Standard General Service:Burien(First Avenue South 1 Undergrounding Charge) Sector: Commercial Description: SCHEDULE LGS is for standard general service provided to Burien customers whose maximum monthly demand is equal to or greater than 1,000 kW but less than 10,000 kW. Minimum Charge: $34.21 per meter per day. First Avenue South 1 Undergrounding Charge: All kWh at 0.37 cent per kWh

148

Data:Eabd2142-fc95-40fa-b50c-1ac0c9a2d12a | Open Energy Information  

Open Energy Info (EERE)

Eabd2142-fc95-40fa-b50c-1ac0c9a2d12a Eabd2142-fc95-40fa-b50c-1ac0c9a2d12a No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Painesville, Ohio (Utility Company) Effective date: 1990/07/01 End date if known: Rate name: Intersection flasher light-Within Corporate Limits Sector: Lighting Description: For the purpose of paying the expenses of conducting and managing the Electric Division, Utilities Department, of the City, the City Manager is hereby authorized and directed to charge the following rates, for all utility bills issued on and after the dates indicated below. These rates are applicable to service calls, unmetered services, standby power and miscellaneous installations which do not fall under the normal rate schedules, which rates are hereby adopted for all utility bills issued on and after July 1, 1990

149

Data:4f82f0e5-12a3-453d-9fbf-d3583d8e7236 | Open Energy Information  

Open Energy Info (EERE)

2f0e5-12a3-453d-9fbf-d3583d8e7236 2f0e5-12a3-453d-9fbf-d3583d8e7236 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Provo City Corp (Utility Company) Effective date: 2012/06/01 End date if known: Rate name: Private Outdoor Security (Closed Rate) - 250 W MV - Wood Pole Sector: Lighting Description: Source or reference: http://www.provo.org/util.rates_summary.html Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring:

150

Data:6f693279-9c83-43fc-8432-a0927c12a5f9 | Open Energy Information  

Open Energy Info (EERE)

9-9c83-43fc-8432-a0927c12a5f9 9-9c83-43fc-8432-a0927c12a5f9 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Kiel, Wisconsin (Utility Company) Effective date: 2011/05/06 End date if known: Rate name: Cp-3 Industrial Power Time-of-Day Service above 600kW Demand 8am-10pm Sector: Industrial Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0754 per kilowatt-hour.

151

Data:7fb75ac1-2a7e-4b4a-b21e-c51764137a9e | Open Energy Information  

Open Energy Info (EERE)

7fb75ac1-2a7e-4b4a-b21e-c51764137a9e 7fb75ac1-2a7e-4b4a-b21e-c51764137a9e No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: New York Power Authority Effective date: 2013/07/01 End date if known: Rate name: SC 68 Conventional (Westchester Customers) Sector: Commercial Description: Source or reference: http://www.nypa.gov/about/documents.htm Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >>

152

Data:28b54f08-c941-4fd0-93d1-2a577e3dd598 | Open Energy Information  

Open Energy Info (EERE)

8-c941-4fd0-93d1-2a577e3dd598 8-c941-4fd0-93d1-2a577e3dd598 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Puget Sound Energy Inc Effective date: 2013/07/01 End date if known: Rate name: Company Street Lights-120 watt Sector: Lighting Description: Source or reference: http://pse.com/aboutpse/Rates/Documents/elec_sch_053.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >>

153

Data:19280696-9d1c-44f3-a80a-12a25ad40f31 | Open Energy Information  

Open Energy Info (EERE)

696-9d1c-44f3-a80a-12a25ad40f31 696-9d1c-44f3-a80a-12a25ad40f31 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Orange & Rockland Utils Inc Effective date: 2012/04/01 End date if known: Rate name: SC16 Street Lighting Induction Overhead and Underground 150w (Customer owned, full service, single bill) Sector: Description: APPLICABLE TO USE OF SERVICE FOR: Sales and delivery of electric power supply provided by the Company or delivery of electric power supply provided by an Energy Service Company under the Company's Retail Access Program for outdoor lighting of areas, beyond the limits of public streets, highways or roadways, for use of individuals and private or public organizations where existing distribution facilities are suitable for the service requested.

154

Data:Cb684dd4-12a1-4e54-928a-bf6281e7b00e | Open Energy Information  

Open Energy Info (EERE)

Data Data Edit with form History Facebook icon Twitter icon » Data:Cb684dd4-12a1-4e54-928a-bf6281e7b00e No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Sulphur Springs Valley E C Inc Effective date: 2013/03/18 End date if known: Rate name: Street Lighting: 250 Watt MV - Double/Wood Sector: Lighting Description: Customer provided Facilities and Cooperative Owned and Maintained Lighting Service. Source or reference: http://www.ssvec.org/wp-content/uploads/downloads/2013/03/SSVEC-Rates-03.18.13.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW):

155

Pion correlations in 1.8A GeV Ar on KCl and La and 1.2A GeV Xe on La  

Science Journals Connector (OSTI)

Results are presented for pion interferometry measurements of 1.8A GeV Ar+KCl and Ar+La, and 1.2A GeV Xe + La at the Lawrence Berkeley Laboratory Heavy Ion Spectrometer System. The parameters R, ?, ?, R?, and R? are presented for all three projectile-target combinations. The correlation between the extracted size of the pion source and the centrality of the collision is investigated as well as the freeze-out densities and the dependence of the source size on the mean momentum of the pion pairs. The experimental setup and analysis are discussed and comparisons made with the results of others. The phase space covered is at forward angles in the center-of-mass system.

W. B. Christie; W. F. J. Mueller; D. L. Olson; T. J. M. Symons; H. H. Wieman; D. Beavis; F. P. Brady; J. L. Romero; C. E. Tull; T. Abbott; S. Y. Fung; D. Keane; Y. Liu

1992-06-01T23:59:59.000Z

156

Data:E72ee42e-a63e-4795-9893-3ef12a88bed0 | Open Energy Information  

Open Energy Info (EERE)

ee42e-a63e-4795-9893-3ef12a88bed0 ee42e-a63e-4795-9893-3ef12a88bed0 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Idaho Power Co Effective date: 2008/03/01 End date if known: Rate name: Schedule 62 - Green energy Purchase Program Rider Sector: Description: PURPOSE The Green Energy Purchase Program is an optional, voluntary program designed to provide customers and non-customer participants an opportunity to participate in the purchase of new environmentally friendly "green" energy. Funds collected in this program will be wholly distributed to the purchase of green energy products. APPLICABILITY Service under this schedule is applicable to all Customers and non-customer participants who choose to participate in this Program. MONTHLY GREEN ENERGY PURCHASE CONTRIBUTION Customers designate their level of participation by choosing a fixed dollar per month amount. The monthly Green Energy Purchase Program contribution is in addition to all other charges included in the service schedule under which the Customer receives electrical service and will be added to the Customer's monthly electric bill. Non-Customer participants will be issued a monthly invoice that reflects their designated fixed dollar per month amount. The Program funds will wholly be used to purchase green energy or cover the green energy price premium. PROGRAM CONSIDERATIONS No electric service disconnections will result in the event of non-payment of Program commitments.

157

Data:E2d97b12-a1ba-4919-b041-0ce6b9bc25dd | Open Energy Information  

Open Energy Info (EERE)

7b12-a1ba-4919-b041-0ce6b9bc25dd 7b12-a1ba-4919-b041-0ce6b9bc25dd No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Northern States Power Co - Wisconsin Effective date: 2012/01/15 End date if known: Rate name: Experimental Advanced Renewable Energy Purchase Service Solar Energy Systems 10 kW (at more than 200 amps) Sector: Description: Effective In All territories served by the Company. Definition: Distributed generation facilities are electricity generators owned by the customer, located R close to the point of energy consumption, and small in scale, usually no more than the existing load of the customer. Availability The advanced renewable energy tariff is available to retail customers who own small distributed generation facilities that are powered by a renewable resource and placed in initial service after January 1, 2012, or who executed an advanced renewable energy contract prior to January 1, 2012. aximum size project per customer is: Solar: 10 kW Technology Limit The solar technology category will be fully subscribed when 300 kW of capacity has been subscribed. Community-based Limits The Community-based Project Category is only applicable to the Biomass/Biogas and Wind technology categories and will be fully subscribed when 5 MW of capacity has been subscribed. In addition, the Community-based Category is applicable only to projects owned by local units of government (Village, City, Town or County), or to projects majority-owned by existing retail customers that choose to join together to develop a joint project. The customer will receive a $1.50/watt capital incentive payment up to a total of $15,000 per facility.

158

Thermally stable compositions including 2,4,8,10-tetranitro-5H-pyrido[3',2':4,5][1,2,3]triazolo[1,2-a]benzotriazo- l-6-ium, inner salt  

DOE Patents [OSTI]

An explosive formulation including 2,4,8,10-tetranitro-5H-pyrido[3',2':4,5][1,2,3]triazolo[1,2-a]benzotriazo- l-6-ium, inner salt and a high temperature binder is disclosed together with a process of preparing 2,4,8,10-tetranitro-5H-pyrido[3',2':4,5][1,2,3]triazolo[1,2-a]benzotriazo- l-6-ium, inner salt.

Hiskey, Michael A. (Los Alamos, NM); Huynh, My Hang (Los Alamos, NM)

2010-01-26T23:59:59.000Z

159

Parity meter for charge qubits: An efficient quantum entangler B. Trauzettel,1,2 A. N. Jordan,3,4 C. W. J. Beenakker,1 and M. Bttiker3  

E-Print Network [OSTI]

Parity meter for charge qubits: An efficient quantum entangler B. Trauzettel,1,2 A. N. Jordan,3,4 C parity meter based on two double quantum dots alongside a quantum point contact. Such a device off the parity meter. Two applications of the parity meter are discussed: the measurement of Bell

160

b134.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

50) 50) 5/2 - I (J P ) = 3 2 ( 5 2 - ) Status: ∗ OMITTED FROM SUMMARY TABLE The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. ∆(2350) BREIT-WIGNER MASS ∆(2350) BREIT-WIGNER MASS ∆(2350) BREIT-WIGNER MASS ∆(2350) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 2350 OUR ESTIMATE ≈ 2350 OUR ESTIMATE ≈ 2350 OUR ESTIMATE ≈ 2350 OUR ESTIMATE 2400± 125 CUTKOSKY 80 IPWA π N → π N 2305± 26 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 2459± 100 VRANA 00 DPWA Multichannel 2171± 18 MANLEY 92 IPWA π N → π N & N π π ∆(2350) BREIT-WIGNER WIDTH ∆(2350) BREIT-WIGNER WIDTH ∆(2350) BREIT-WIGNER WIDTH ∆(2350) BREIT-WIGNER WIDTH VALUE (MeV) DOCUMENT ID TECN COMMENT 400± 150 CUTKOSKY 80 IPWA π N → π N 300± 70 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits,

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161

b134.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

4 4 ∆(2350) 5/2 - I (J P ) = 3 2 ( 5 2 - ) Status: ∗ OMITTED FROM SUMMARY TABLE The latest GWU analysis (ARNDT 06) finds no evidence for this NODE=B134 resonance. ∆(2350) BREIT-WIGNER MASS ∆(2350) BREIT-WIGNER MASS ∆(2350) BREIT-WIGNER MASS ∆(2350) BREIT-WIGNER MASS NODE=B134M NODE=B134M VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 2350 OUR ESTIMATE ≈ 2350 OUR ESTIMATE ≈ 2350 OUR ESTIMATE ≈ 2350 OUR ESTIMATE → UNCHECKED ← 2400 ± 125 CUTKOSKY 80 IPWA π N → π N 2305 ± 26 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 2459 ± 100 VRANA 00 DPWA Multichannel 2171 ± 18 MANLEY 92 IPWA π N → π N & N π π ∆(2350) BREIT-WIGNER WIDTH ∆(2350) BREIT-WIGNER WIDTH ∆(2350) BREIT-WIGNER WIDTH ∆(2350) BREIT-WIGNER WIDTH NODE=B134W NODE=B134W VALUE (MeV) DOCUMENT ID TECN COMMENT 400 ± 150 CUTKOSKY 80 IPWA π N → π N 300 ±

162

Problems #3, Math 204, Dr. M. Bohner. Sep 10, 2003. Due Sep 15, 11 am. 12. A tank has ten gallons of water in which two pounds of salt has been dissolved. Brine with  

E-Print Network [OSTI]

Problems #3, Math 204, Dr. M. Bohner. Sep 10, 2003. Due Sep 15, 11 am. 12. A tank has ten gallons through the supplementary homework problems for Chapters 1­2: 1, 3 of Section 1.1; 1 of Section 1.2; 1-8, 14, 15, 17, 19, 21, 25, 26 of Section 1.3; 1, 3, 4, 13­17, 21, 26, 29 of Section 2.1; 1, 4­8, 9, 11

Bohner, Martin

163

CONTROL OF HAZARDOUS ENERGY 12.A GENERAL  

E-Print Network [OSTI]

on or near any system that produces, uses, or stores hazardous energy, a hazardous energy control program by the contractor-managed HECP (e.g., QA's on construction sites, etc.), they shall comply with the contractor and implementation of these activities. Each shall inform the other of their HECPs and Hazardous Energy Control (HEC

US Army Corps of Engineers

164

CONTROL OF HAZARDOUS ENERGY 12.A GENERAL  

E-Print Network [OSTI]

as all requirements of 1910.147, ANSI Z244.1, and ANSI A10.44. c. When contractor work involving.147, ANSI Z244.1, and ANSI A10.44. When a site is controlled by a contractor and USACE employees

US Army Corps of Engineers

165

Data:Ea6a12a3-4a11-4d01-8ca1-0be1b3e38aeb | Open Energy Information  

Open Energy Info (EERE)

a12a3-4a11-4d01-8ca1-0be1b3e38aeb a12a3-4a11-4d01-8ca1-0be1b3e38aeb No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Northern Plains Electric Coop Effective date: 2012/02/01 End date if known: Rate name: SMALL RENEWABLE ENERGY PURCHASE RATE Sector: Description: Availability This rate is applicable for a member-owned renewable energy generating facility with a capacity less than 150 KW which is properly interconnected to the Northern Plains Electric Cooperative electrical system (Qualifying Facility) and which the generated power is sold to Northern Plains. Type of Service Single or three phase, 60 hertz, at available primary or secondary voltages.

166

Data:04c64d7f-c7c7-43f6-aca1-2a7ab06dd02d | Open Energy Information  

Open Energy Info (EERE)

4d7f-c7c7-43f6-aca1-2a7ab06dd02d 4d7f-c7c7-43f6-aca1-2a7ab06dd02d No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Delta Montrose Electric Assn Effective date: 2012/01/01 End date if known: Rate name: LARGE COMMERCIAL NET METERING Sector: Commercial Description: Source or reference: http://www.dmea.com/index.php?option=com_content&view=article&id=95&Itemid=72 Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category:

167

Scanning multichannel microwave radiometer snow water equivalent assimilation  

E-Print Network [OSTI]

(AMSR-E) observing system. Many investi- gators have carefully evaluated the accuracy of remotely sensed

Walker, Jeff

168

Multichannel heterodyning for wideband interferometry, correlation and signal processing  

DOE Patents [OSTI]

A method of signal processing a high bandwidth signal by coherently subdividing it into many narrow bandwidth channels which are individually processed at lower frequencies in a parallel manner. Autocorrelation and correlations can be performed using reference frequencies which may drift slowly with time, reducing cost of device. Coordinated adjustment of channel phases alters temporal and spectral behavior of net signal process more precisely than a channel used individually. This is a method of implementing precision long coherent delays, interferometers, and filters for high bandwidth optical or microwave signals using low bandwidth electronics. High bandwidth signals can be recorded, mathematically manipulated, and synthesized.

Erskine, David J. (Oakland, CA)

1999-01-01T23:59:59.000Z

169

A Multichannel, Variable?Threshold, Time?Sequence Recorder  

Science Journals Connector (OSTI)

The analysis and design of a ten?channel variable?threshold time?sequence recorder that uses TTL is presented. Channel?to?channel time resolution is ? 250 nsec and risetime is ? 6 usec for a 2?V p?p signal. Although the recorder is designed to examine the flux?jump phenomenon in large superconducting magnets it has application wherever variable?threshold time?sequencing is required.

Mark L. McKinstry

1973-01-01T23:59:59.000Z

170

Original articles: Intelligent multichannel sensors for pulse wave analysis  

Science Journals Connector (OSTI)

Aortic pulse wave velocity is an independent predictive indicator for all cause mortality and cardiovascular morbidity. Unfortunately it is only invasively accessible and thus the A. carotis-A. femoralis pulse wave velocity (cfPWV) is recommended as ... Keywords: Arterial stiffness, BP, Cardiovascular risk, ECG, Electrocardiography, FIR, ICA, INA, Idxao, Idxo, Idxs, LED, PTT, PW, PWV, Pulse transit time, Pulse wave velocity, SD, cfPWV, dBP, p'(Idxo), p'(Idxs), p(Idxo), p(Idxs), sBP

S. Rosenkranz; C. Mayer; J. Kropf; S. Wassertheurer

2011-11-01T23:59:59.000Z

171

A Survey on Multichannel Assignment Protocols in Wireless Sensor Networks  

E-Print Network [OSTI]

device equipped with a single radio transceiver such as the CC2420 so it can only use one channel: The hidden node problem occurs when the node misses an RTS/CTS exchanged on one channel while listening of visited nodes. · low duty cycling device support: To save energy, nodes resort to low duty cycles

Paris-Sud XI, Université de

172

A compact, multichannel, and low noise arbitrary waveform generator  

SciTech Connect (OSTI)

A new type of high functionality, fast, compact, and easy programmable arbitrary waveform generator for low noise physical measurements is presented. The generator provides 7 fast differential waveform channels with a maximum bandwidth up to 200 MHz frequency. There are 6 fast pulse generators on the generator board with 78 ps time resolution in both duration and delay, 3 of them with amplitude control. The arbitrary waveform generator is additionally equipped with two auxiliary slow 16 bit analog-to-digital converters and four 16 bit digital-to-analog converters for low frequency applications. Electromagnetic shields are introduced to the power supply, digital, and analog compartments and with a proper filter design perform more than 110 dB digital noise isolation to the output signals. All the output channels of the board have 50 ? SubMiniature version A termination. The generator board is suitable for use as a part of a high sensitive physical equipment, e.g., fast read out and manipulation of nuclear magnetic resonance or superconducting quantum systems and any other application, which requires electromagnetic interference free fast pulse and arbitrary waveform generation.

Govorkov, S. [Sema Systems, 302-5553 16th ave., Delta, British Columbia V4M 2H7 (Canada)] [Sema Systems, 302-5553 16th ave., Delta, British Columbia V4M 2H7 (Canada); Ivanov, B. I. [Leibniz-Institute of Photonic Technology, PO Box 100239, D-07702 Jena (Germany) [Leibniz-Institute of Photonic Technology, PO Box 100239, D-07702 Jena (Germany); Novosibirsk State Technical University, K.Marx-Ave. 20, Novosibirsk 630092 (Russian Federation); Il'ichev, E.; Meyer, H.-G. [Leibniz-Institute of Photonic Technology, PO Box 100239, D-07702 Jena (Germany)] [Leibniz-Institute of Photonic Technology, PO Box 100239, D-07702 Jena (Germany)

2014-05-15T23:59:59.000Z

173

Combining Multichannel ERP Data for Early Diagnosis of Alzheimer's Disease  

E-Print Network [OSTI]

. A neurodegenerative disorder, AD is caused by neuronal death due two misfolded proteins, -amyloid and describe an ensemble of classifiers based ap- proach that combines decision and data fusion techniques

Polikar, Robi

174

Multichannel analog-digital converter in VEKTOR-CAMAC systemsystems  

SciTech Connect (OSTI)

This paper describes a four-channel analog-digital converter (ADC) that is implemented by large-scale integrated circuits. Resdundancy of signal conversion in intermediate cycles ensures a more accurate conversion result from cycle to cycle. The ADC is fully compatible with the Vektor system and, with slight modifications, is CAMAC compatible. The conversion time of the ADC for one channel is 5 used, the output code is 14-bit binary, the maximum integral nonlinearity is not more than 0.05% of the dynamic range of + or -10V, and the size of the random access memeory is 1024 14-bit words.

Borodyanskii, M.E.

1986-09-01T23:59:59.000Z

175

Multichannel Simultaneous Determination of Activities of Lactate Dehydrogenase  

SciTech Connect (OSTI)

It is very important to find the best conditions for some enzymes to do the best catalysis in current pharmaceutical industries. Based on the results above, we could say that this set-up could be widely used in finding the optimal condition for best enzyme activity of a certain enzyme. Instead of looking for the best condition for enzyme activity by doing many similar reactions repeatedly, we can complete this assignment with just one run if we could apply enough conditions.

Ma, L.

2000-09-12T23:59:59.000Z

176

ElectronVibration Interaction in Multichannel Single-Molecule Junctions  

Science Journals Connector (OSTI)

The electron-vibration coupling gives rise to small drops in the conductance at voltages corresponding to energies of some of the vibrational modes. ... where only the apex atoms are allowed to vibrate. ... We explore a full range of parameters going from weak to strong electron-vibration coupling, from tunneling to contact, and from 1-vibration description to the need of including all vibrations for a correct description of inelastic effects in transport. ...

Regev Ben-Zvi; Ran Vardimon; Tamar Yelin; Oren Tal

2013-11-19T23:59:59.000Z

177

Multichannel heterodyning for wideband interferometry, correlation and signal processing  

DOE Patents [OSTI]

A method is disclosed of signal processing a high bandwidth signal by coherently subdividing it into many narrow bandwidth channels which are individually processed at lower frequencies in a parallel manner. Autocorrelation and correlations can be performed using reference frequencies which may drift slowly with time, reducing cost of device. Coordinated adjustment of channel phases alters temporal and spectral behavior of net signal process more precisely than a channel used individually. This is a method of implementing precision long coherent delays, interferometers, and filters for high bandwidth optical or microwave signals using low bandwidth electronics. High bandwidth signals can be recorded, mathematically manipulated, and synthesized. 50 figs.

Erskine, D.J.

1999-08-24T23:59:59.000Z

178

Experimental investigations and three-dimensional transmission line matrix simulation of Ca 5 ? x A x B 2 Ti O 12 ( A = Mg , Zn, Ni, and Co; B = Nb and Ta) ceramic resonators  

Science Journals Connector (OSTI)

Temperature-stable low-loss Ca 5 ? x A x B 2 Ti O 12 ( A = Mg Zn Ni and Co; B = Nb and Ta)dielectrics suitable for microwave telecommunication applications were prepared by the conventional solid-state ceramic route. Investigations were made on the structure and microstructure of the ceramics employing x-ray and scanning electron microscopic techniques. The dielectric properties were measured in the 3.5 7 GHz frequency range. The time domain simulation of electromagnetic wave interaction with dielectric materials using three-dimensional transmission line matrix modeling methods is presented. Excellent agreement between experimental and simulated values of microwavedielectric properties was observed. The materials are potential candidates for applications in filters oscillators and high efficiency low-loss dielectric antennas working especially at millimeter wave region.

Pazhoor Varghese Bijumon; Mailadil Thomas Sebastian; Pezholil Mohanan

2005-01-01T23:59:59.000Z

179

Data:F157faf1-12a5-4c9e-84de-b1ea0d72e277 | Open Energy Information  

Open Energy Info (EERE)

F157faf1-12a5-4c9e-84de-b1ea0d72e277 F157faf1-12a5-4c9e-84de-b1ea0d72e277 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: South Central Indiana REMC Effective date: 2010/06/01 End date if known: Rate name: Residential & Farm Rate - RS - HP Sector: Residential Description: Availability Available as an optional rate to any residential or farm consumer of the Corporation for singlephase electric service at a single delivery point who has an air source heat pump with natural gas or LP gas backup. The air source heat pump system must not have any auxiliary emergency resistance heat installed. A representative of the Corporation must certify the air source heat pump as meeting the requirements of this rate schedule. A Demand Response Unit (DRU) must be installed that allows for control of the air conditioning load during peak periods as determined by the Corporation. The rated capacity of any motor served under this schedule in excess of ten (10) horsepower shall be subject to the approval of the Corporation. A consumer choosing this optional rate must remain on the rate for a minimum of six months. Consumers opting to change to a different rate schedule after the six month minimum period must wait a minimum of six months before returning to this optional rate.

180

b048.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

250) 250) I (J P ) = 1(? ? ) Status: ∗∗∗ Results from partial-wave analyses are too weak to warrant sep- arating them from the production and cross-section experiments. LASINSKI 71 in K N using a Pomeron + resonances model, and DEBELLEFON 76, DEBELLEFON 77, and DEBELLEFON 78 in energy-dependent partial-wave analyses of K N → Λ π, Σ π, and N K , respectively, suggest two resonances around this mass. Σ (2250) MASS Σ (2250) MASS Σ (2250) MASS Σ (2250) MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 2210 to 2280 (≈ 2250) OUR ESTIMATE 2210 to 2280 (≈ 2250) OUR ESTIMATE 2210 to 2280 (≈ 2250) OUR ESTIMATE 2210 to 2280 (≈ 2250) OUR ESTIMATE 2270± 50 DEBELLEFON 78 DPWA D 5 wave 2210± 30 DEBELLEFON 78 DPWA G 9 wave 2275± 20 DEBELLEFON 77 DPWA D 5 wave 2215± 20 DEBELLEFON 77 DPWA G 9 wave 2300± 30 1 DEBELLEFON 75B HBC K - p → Ξ ∗0 K 0 2251 + 30 - 20 VANHORN 75 DPWA K - p → Λ π 0 , F 5 wave 2280± 14 AGUILAR-...

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181

Citation: D.E. Groom  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

N(1535) N(1535) S 11 I (J P ) = 1 2 ( 1 2 - ) Status: ∗∗∗∗ Most of the results published before 1975 are now obsolete and have been omitted. They may be found in our 1982 edition, Physics Letters 111B 111B 111B 111B (1982). N(1535) BREIT-WIGNER MASS N(1535) BREIT-WIGNER MASS N(1535) BREIT-WIGNER MASS N(1535) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 1520 to 1555 (≈ 1535) OUR ESTIMATE 1520 to 1555 (≈ 1535) OUR ESTIMATE 1520 to 1555 (≈ 1535) OUR ESTIMATE 1520 to 1555 (≈ 1535) OUR ESTIMATE 1534± 7 MANLEY 92 IPWA π N → π N & N π π 1550±40 CUTKOSKY 80 IPWA π N → π N 1526± 7 HOEHLER 79 IPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 1532± 5 ARMSTRONG 99B DPWA γ ∗ p → p η 1549± 2 ABAEV 96 DPWA π - p → η n 1525±10 ARNDT 96 IPWA γ N → π N 1535 ARNDT 95 DPWA π N → N π 1542± 6 BATINIC 95 DPWA π N → N π, N η 1537 BATINIC 95B DPWA π N →

182

trinity-aa-use-case-v1.2a  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Trinity Trinity Use Case Scenarios ( SAND 2 013---2941 P U nclassified, U nlimited R elease) Page 1 of 9 Trinity / N ERSC---8 U se C ase S cenarios April 5 , 2 013 This d ocument p rovides a dditional v iews o f a nticipated u sage s cenarios f or t wo o f the a dvanced a rchitecture f eatures o f T rinity, t he b urst b uffer a nd p ower/energy measurement a nd c ontrol. T his d ocument m ay c hange as our understanding of needs a nd t echnologies e volves. T hese scenarios are not intended to include all intended u ses o f t hese t echnologies. Format: E mbedded i n t he p rimary s cenario d escriptions a re n umbered t ags r eferring t o requirements ( listed f ollowing e ach s cenario) t hat a re i nferred b y t he s cenario. T he r eader should r ead t he s pecific r equirement, s pecified b y n umber, a t t he t ime i t i s e ncountered

183

rough ut Maximaization in Multi-channel I reless esh Access etworkcs  

E-Print Network [OSTI]

regulation entities and hence non-cooperative. The long- term behavior and corresponding pertormance and Yuguang Fang Department of Electrical and Computer Engineering University of Florida Gainesville, Florida of wireless mesh access networks is addressed. For the case ot cooperative access points, we present

Latchman, Haniph A.

184

Multi-Channel FIR HCN Laser Interferometer on HT-7 Tokamak  

Science Journals Connector (OSTI)

A Five-channel far-infrared (FIR) hydrogen cyanide (HCN) laser interferometer was developed to measure plasma electron density profile on the HT-7 superconducting tokamak. The structure of the five-channel FIR .....

Y. X. Jie; X. Gao; Y. F. Cheng; K. Yang

2000-09-01T23:59:59.000Z

185

Combination of multichannel detection and fast time response in a multichord spectrometer  

E-Print Network [OSTI]

deflectometry for temperature analysis of filamentary non-thermal atmospheric pressure plasma Rev. Sci. Instrum diagnostics with electric probe measurements of inductively coupled Ar/O2/Ar-O2 plasmas Phys. Plasmas 19, 113502 (2012) Fourier transform infrared absorption spectroscopy characterization of gaseous atmospheric

186

The addition of multichannel analog-to-digital conversion capability to a minicomputer facility  

E-Print Network [OSTI]

output with small 60 ma lamps. Figure 11 shows the circuit diagram of the buffers and the display lamp drivers. The inverting buffers are TTL 7400 NAND gates [17]. The input channel number is also displayed with a 7-segment display lamp. The 7... buffer exchanges. The input/output requests perform status checking of the standard I/O devices, data recording on the magnetic tape re- corder (MT) unit, and message printing on the teletype (TTY). Hewlett-Packard Software Interface The HP computers...

Malek-Shahmirzadi, Homayoun

2012-06-07T23:59:59.000Z

187

An Autonomous, Broadband, Multi-channel Neural Recording System for Freely Behaving Primates  

E-Print Network [OSTI]

. features, 2) their battery life or storage capacity is limited to a few hours or less for broadband behaving primates. In this paper we present a dual- channel, battery powered, neural recording system of advances, particularly in the field of neural prosthetics. However, current state of the art experimental

Shenoy, Krishna V.

188

XPS: A multi-channel preamplifier shaper IC for X-ray spectroscopy  

SciTech Connect (OSTI)

An integrated circuit featuring 48 channels of charge-sensitive preamplifiers followed by variable-gain pulse shaping amplifiers is being developed as part of an x-ray spectrometer with a highly segmented detector to handle high fluxes in synchrotron experiments. Such detector systems can provide excellent energy resolution combined with one-dimensional spatial information. The IC combines many basic spectroscopy amplifier functions with a low-noise preamplifier section to produce a unique circuit capable of driving conventional ADC modules directly. An important feature of the design is the novel CR-RC{sup 2} pulse shaper. In this section, high-linearity transconductor circuits are required in order to provide a broad range of continuously variable peaking times while still maintaining the linearity and noise performance necessary for x-ray spectroscopy. Reported here are first measurements made on the performance of a 16-channel prototype integrated circuit. At present, the preamplifier-shaper circuit achieves an equivalent input noise of 26 electrons rms at 2 {micro}s peaking time with a 0.2 pF external capacitor, which is similar to the capacitance of a single detector element. The design was fabricated in standard 1.2 {micro}m CMOS technology.

Krieger, B.; Kipnis, I.; Ludewigt, B.A.

1997-11-01T23:59:59.000Z

189

Traffic-Aware Multi-Channel Multi-Stage Spectrum Sensing Protocols for Dynamic Spectrum Access  

E-Print Network [OSTI]

radios search for licensed spectral vacancies by performing spectrumspectrum sensing protocol, a DSA radio has to period- ically scan the licensedspectrum scarcity. All usable radio frequencies are already licensed

Gabran, Wesam Ramy I. F.

2012-01-01T23:59:59.000Z

190

Blind deconvolution of multichannel recordings by linearized inversion in the spectral domain  

Science Journals Connector (OSTI)

...the crust and lithosphere: Advances in Geophysics, 46 , , doi: http://dx.doi.org/10.1016/S0065-2687(03)46002-0 .ADGOAR. Ruigrok, E. , Campman, X., Draganov, D., and Wapenaar, K., 2010, High-resolution lithospheric imaging...

Michael Behm; Bharath Shekar

191

Suppressing Multi-Channel Ultra-Low-Field MRI Measurement Noise Using Data Consistency and Image  

E-Print Network [OSTI]

SQUID sensors demonstrate the effectiveness of this data consistency constraint and sparsity prior-mail: fhlin@ntu.edu.tw Introduction MRI has become an indispensible resource in clinical medicine because

192

Characterization of Woody and Herbaceous Biomasses Lignin Composition with 1064 nm Dispersive Multichannel Raman Spectroscopy  

Science Journals Connector (OSTI)

Biomass representing different classes of bioenergy feedstocks, including woody and herbaceous species, was measured with 1064 nm Raman spectroscopy. Pine, oak, poplar, kenaf,...

Lupoi, Jason S; Smith, Emily A

2012-01-01T23:59:59.000Z

193

Development of the analog ASIC for multi-channel readout X-ray CCD camera  

E-Print Network [OSTI]

We report on the performance of an analog application-specific integrated circuit (ASIC) developed aiming for the front-end electronics of the X-ray CCDcamera system onboard the next X-ray astronomical satellite, ASTRO-H. It has four identical channels that simultaneously process the CCD signals. Distinctive capability of analog-to-digital conversion enables us to construct a CCD camera body that outputs only digital signals. As the result of the front-end electronics test, it works properly with low input noise of =range of 720 mV covers the effective energy range of the typical X-ray photon counting CCD (up to 20 keV). The integrated non-linearity is 0.2% that is similar as those of the conventional CCDs in orbit. We also performed a radiation tolerance test against the total ionizing dose (TID) effect and the single event effect. The irradiation test using 60Co and proton beam showed ...

Nakajima, Hiroshi; Idehara, Toshihiro; Anabuki, Naohisa; Tsunemi, Hiroshi; Doty, John P; Ikeda, Hirokazu; Katayama, Haruyoshi; Kitamura, Hisashi; Uchihori, Yukio; 10.1016/j.nima.2010.12.174

2011-01-01T23:59:59.000Z

194

Joint synchronization and calibration of multi-channel transform-domain charge sampling receivers  

E-Print Network [OSTI]

, the expansion coe?cients become the Fourier series coe?cients, hence, the receiver is referred to as the Frequency domain (FD) receiver. In each channel, the input signal is mixed with the basis signal and integrated in a window of duration Tc seconds... that cover the entire signal block provide a total of MN coe?cients R(m;n)jM?1m=0jN?1n=0 given by, Rm;n = Z mTs+Tc mTs x(t)'?n(t)dt; (1.1) where Ts = Tc ? Tov, x(t) is the received signal, m = 0 to M ? 1 indicates the mth segment in each channel and n = 0...

Kotte Prakasam, Pradeep

2010-07-14T23:59:59.000Z

195

Multichannel calculations for frequency shift and line broadening cross sections in collisions of cold hydrogen atoms  

E-Print Network [OSTI]

Zygelman,B. Jamieson,M.J. Stancil,P.C. Dalgarno,A. Workshop on Collisions of Cold Trapped Atoms at Joint Institute for Laboratory Astrophysics, Boulder, CO, U.S.A.

Zygelman, B.; Jamieson, M.J.

196

High-speed, multi-channel detector readout electronics for fast radiation detectors  

SciTech Connect (OSTI)

In this project, we are developing a high speed digital spectrometer that a) captures detector waveforms at rates up to 500 MSPS b) has upgraded event data acquisition with additional data buffers for zero dead time operation c) moves energy calculations to the FPGA to increase spectrometer throughput in fast scintillator applications d) uses a streamlined architecture and high speed data interface for even faster readout to the host PC These features are in addition to the standard functions in our existing spectrometers such as digitization, programmable trigger and energy filters, pileup inspection, data acquisition with energy and time stamps, MCA histograms, and run statistics. In Phase I, we upgraded one of our existing spectrometer designs to demonstrate the key principle of fast waveform capture using a 500 MSPS, 12 bit ADC and a Xilinx Virtex-4 FPGA. This upgraded spectrometer, named P500, performed well in initial tests of energy resolution, pulse shape analysis, and timing measurements, thus achieving item (a) above. In Phase II, we are revising the P500 to build a commercial prototype with the improvements listed in items (b)-(d). As described in the previous report, two devices were built to pursue this goal, named the Pixie-500 and the Pixie-500 Express. The Pixie-500 has only minor improvements from the Phase I prototype and is intended as an early commercial product (its production and part of its development were funded outside the SBIR). It also allows testing of the ADC performance in real applications.The Pixie-500 Express (or Pixie-500e) includes all of the improvements (b)-(d). At the end of Phase II of the project, we have tested and debugged the hardware, firmware and software of the Pixie-500 Express prototype boards delivered 12/3/2010. This proved substantially more complex than anticipated. At the time of writing, all hardware bugs have been fixed, the PCI Express interface is working, the SDRAM has been successfully tested and the SHARC DSP has been booted with preliminary code. All new ICs and circuitry on the prototype are working properly, however some of the planned firmware and software functions have not yet been completely implemented and debugged. Overall, due to the unanticipated complexity of the PCI Express interface, some aspects of the project could not be completed with the time and funds available in Phase II. These aspects will be completed in self-funded Phase III.

Hennig, Wolfgang

2012-06-22T23:59:59.000Z

197

Designing a Multichannel Sense-and-Avoid Radar for Small UASs  

E-Print Network [OSTI]

, then the transmitted signals bandwidth will be 15 MHz and not 500 kHz. Pulse compression is also used in FMCW radars (as its name implies) because the bandwidth of the transmit signal doesnt correspond to the SRP (i.e., the duration of each pulse... also determine what the bandwidth and SRP of the signal are. Equation 1.12 shows how the Doppler shift can be calculated based on radial velocity, and the signals wavelength ( ). (1.11) (1...

Zakharov, Mikhail

2014-05-31T23:59:59.000Z

198

Recording Uterine Contraction Patterns in Pregnant Women: Application of the Strain Gage in a Multichannel Tokodynamometer  

Science Journals Connector (OSTI)

...The recording unit now in use was made to our specifications by the Electro Physical Laboratories, New York...sample, while the lampblack pro-vided excellent thermal insulation. The assembly shown was placed inside a closed...

S. R. M. REYNOLDS; O. O. HEARD; PAUL BRUNS

1947-10-31T23:59:59.000Z

199

Multichannel Virtual Access Points for Seamless Handoffs in IEEE 802.11 Wireless Networks  

E-Print Network [OSTI]

to extend wired networks due to their rapid deployment and easy configuration. These characteristics of such networks are university campuses, convention centers, airports, and corpo- ration intranets. Because APs

Paris-Sud XI, Université de

200

Low-energy neutron-12C analyzing powers: Results from a multichannel algebraic scattering theory  

E-Print Network [OSTI]

Analyzing powers in low-energy neutron scattering from 12C are calculated in an algebraic momentum-space coupled-channel formalism (MCAS). The results are compared with recently obtained experimental data. The channel-coupling potentials have been defined previously to reproduce the total cross section and sub-threshold bound states of the compound system. Without further adjustment, good agreement with data for the analyzing powers is obtained.

J. P. Svenne; K. Amos; S. Karataglidis; D. van der Knijff; L. Canton; G. Pisent

2005-10-29T23:59:59.000Z

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

Multi-channel blind system identification using the Laguerre expansion for characterization of circulatory hemodynamics  

E-Print Network [OSTI]

A new tool for real-time characterization of both systemic and local circulatory hemodynamics has been developed. Given two peripheral circulatory waveform measurements this new signal-processing algorithm generates two ...

McCombie, Devin Barnett, 1972-

2004-01-01T23:59:59.000Z

202

Multi-channel conduction in redox-based resistive switch modelled using quantum point contact theory  

SciTech Connect (OSTI)

A simple analytic model for the electron transport through filamentary-type structures in Si-rich silica (SiO{sub x})-based resistive switches is proposed. The model is based on a mesoscopic description and is able to account for the linear and nonlinear components of conductance that arise from both fully and partially formed conductive channels spanning the dielectric film. Channels are represented by arrays of identical scatterers whose number and quantum transmission properties determine the current magnitude in the low and high resistance states. We show that the proposed model not only reproduces the experimental current-voltage (I-V) characteristics but also the normalized differential conductance (dln(I)/dln(V)-V) curves of devices under test.

Miranda, E., E-mail: enrique.miranda@uab.cat; Su, J. [Departament d'Enginyeria Electrnica, Universitat Autnoma de Barcelona, 08193 Cerdanyola del Valls, Barcelona (Spain)] [Departament d'Enginyeria Electrnica, Universitat Autnoma de Barcelona, 08193 Cerdanyola del Valls, Barcelona (Spain); Mehonic, A.; Kenyon, A. J. [Department of Electronic and Electrical Engineering, University College London, Torrington Place, London WC1E 7JE (United Kingdom)] [Department of Electronic and Electrical Engineering, University College London, Torrington Place, London WC1E 7JE (United Kingdom)

2013-11-25T23:59:59.000Z

203

Design and implementation of a multichannel millimeter wave interferometer for the Compact Toroidal Hybrid experiment  

SciTech Connect (OSTI)

A three-channel 1 mm wave interferometer has been designed, assembled, and installed on the Compact Toroidal Hybrid torsatron (CTH). The interferometer design makes novel use of a subharmonic mixer for detection, which simplifies alignment. It employs a single electronically tunable source that is repetitively chirped using a sawtooth waveform of frequency up to 1 MHz. The 15.25 GHz drive oscillator is multiplied in two stages to 122 GHz before a final doubler stage brings it to 244 GHz. Local oscillator (LO) power at 122 GHz is directed through waveguide to the LO input of the subharmonic mixer of each viewing chord, simplifying alignment. Phase detection is performed by directly digitizing the amplified mixer outputs at 50 MHz and processing them with a software algorithm. Initial measurements made with the central chord of the new interferometer agree with those from the existing 4 mm system at low densities. The 1 mm system performs well in current-driven discharges reaching densities over 10{sup 19} m{sup -3}, whereas the lower frequency interferometer is found to be less reliable due to loss of fringes. This is a critical improvement for experiments studying the onset, avoidance, and vacuum magnetic transform dependence of disruptions in the CTH device.

Miller, M. C.; Hanson, J. D.; Hartwell, G. J.; Knowlton, S. F.; Maurer, D. A.; Stevenson, B. A. [Physics Department, Auburn University, Auburn, Alabama 36849 (United States)

2012-10-15T23:59:59.000Z

204

Adaptive Beamforming Technique for Accurate Vertical Wind Measurements with Multichannel MST Radar  

E-Print Network [OSTI]

Center, Tachikawa, Japan TAKUJI NAKAMURA National Institute of Polar Research, Tokyo, Japan TORU SATO Research, Tachikawa, Tokyo 1908518, Japan. E-mail: knish@ieee.org DECEMBER 2012 N I S H I M U R A E T A L

Sato, Toru

205

Multichannel ECG and Noise Modeling: Application to Maternal and Fetal ECG Signals  

E-Print Network [OSTI]

A three-dimensional dynamic model of the electrical activity of the heart is presented. The model is based on the single dipole model of the heart and is later related to the body surface potentials through a linear model ...

Clifford, Gari D.

206

b088.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

8 8 Σ (2080) 3/2 + I (J P ) = 1( 3 2 + ) Status: ∗∗ OMITTED FROM SUMMARY TABLE Suggested by some but not all partial-wave analyses across this re- NODE=B088 gion. Σ (2080) MASS Σ (2080) MASS Σ (2080) MASS Σ (2080) MASS NODE=B088M NODE=B088M VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 2080 OUR ESTIMATE ≈ 2080 OUR ESTIMATE ≈ 2080 OUR ESTIMATE ≈ 2080 OUR ESTIMATE → UNCHECKED ← 2091 ± 7 1 CORDEN 76 DPWA K - n → Λ π - 2070 to 2120 DEBELLEFON 76 IPWA K - p → Λ π 0 2120 ± 40 BAILLON 75 IPWA K N → Λ π (sol. 1) OCCUR=2 2140 ± 40 BAILLON 75 IPWA K N → Λ π (sol. 2) 2082 ± 4 COX 70 DPWA See CORDEN 76 2070 ± 30 LITCHFIELD 70 DPWA K - N → Λ π Σ (2080) WIDTH Σ (2080) WIDTH Σ (2080) WIDTH Σ (2080) WIDTH NODE=B088W NODE=B088W VALUE (MeV) DOCUMENT ID TECN COMMENT 186 ± 48 1 CORDEN 76 DPWA K - n → Λ π - 100 DEBELLEFON 76 IPWA K - p → Λ π 0 240 ± 50 BAILLON 75 IPWA K N → Λ π (sol. 1) OCCUR=2 200 ± 50 BAILLON 75

207

b000.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

80) 80) 3/2 - I (J P ) = 1( 3 2 - ) Status: ∗ OMITTED FROM SUMMARY TABLE Seen in the isospin-1 K N cross section at BNL (LI 73, CARROLL 76) and in a partial-wave analysis of K - p → Λ π 0 for c.m. energies 1560-1600 MeV by LITCHFIELD 74. LITCHFIELD 74 finds J P = 3/2 - . Not seen by ENGLER 78 or by CAMERON 78C (with larger statistics in K 0 L p → Λ π + and Σ 0 π + ). Neither OLMSTED 04 (in K - p → Λ π 0 ) nor PRAKHOV 04 (in K - p → Λ π 0 π 0 ) see any evidence for this state. Σ (1580) MASS Σ (1580) MASS Σ (1580) MASS Σ (1580) MASS VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 1580 OUR ESTIMATE ≈ 1580 OUR ESTIMATE ≈ 1580 OUR ESTIMATE ≈ 1580 OUR ESTIMATE 1583± 4 1 CARROLL 76 DPWA Isospin-1 total σ 1582± 4 2 LITCHFIELD 74 DPWA K - p → Λ π 0 Σ (1580) WIDTH Σ (1580) WIDTH Σ (1580) WIDTH Σ (1580) WIDTH VALUE (MeV) DOCUMENT ID TECN COMMENT 15 1 CARROLL 76 DPWA Isospin-1 total σ 11± 4 2 LITCHFIELD 74 DPWA K - p → Λ π 0 Σ (1580)

208

58 IEEE TRANSACTIONS ON INSTRUMENTATION AND MEASUREMENT, VOL. 53, NO. 1, FEBRUARY 2004 Multichannel Raman Gas Analyzer: The Data  

E-Print Network [OSTI]

with the green laser source previously used and reported in a related article. Index Terms--Air-pollution, data Raman Gas Analyzer: The Data Acquisition and Control System. Measurement Improvement With Blue Laser Albrecht, and Nikiforos G. Theofanous Abstract--In this paper, the data acquisition and control system

Athens, University of

209

1128 IEEE TRANSACTIONS ON WIRELESS COMMUNICATIONS, VOL. 9, NO. 3, MARCH 2010 Optimal Multi-Channel Cooperative Sensing in  

E-Print Network [OSTI]

--Cognitive radio, spectrum sensing, throughput maximization. I. INTRODUCTION DUE to the rapid growth of wireless-utilization of licensed spectrum at a time or a location has been observed by measurements of wireless spectrum usage [1 (secondary) users can utilize the spectrum when and where the licensed (primary) users are not using it

Jiang, Hai

210

We present a patient-specific seizure detection algorithm conveying structural information from the multichannel EEG using a novel ma-  

E-Print Network [OSTI]

. Meth- ods: The proposed training algorithm uses nuclear norm regularization to convey structural. The performances of the detectors are demonstrated on a pub- licly available dataset containing 131 seizures in the liter- ature using the same dataset. Conclusion: The strength of our method lies within conveying

211

Constrained Parameterization of the Multichannel Analysis of Surface Waves Approach with Application at Yuma Proving Ground, Arizona  

E-Print Network [OSTI]

.................................................................................................................. 50 5.3. VP-TOMOGRAPHY (JARS) .......................................................................................................... 55 6. CONSTRAINED-PARAMETERIZATION MASW DISCUSSION .......................................................... 60... 6.1. VS-JARS AND MASW ............................................................................................................... 60 6.2. RMS ERROR...

Schwenk, Jacob Tyler

2013-08-31T23:59:59.000Z

212

Dual-Band Multi-Channel Airborne Radar for Mapping the Internal and Basal Layers of Polar Ice Sheets  

E-Print Network [OSTI]

Engineering lowpass filter acts as an anti-imaging filter. The lowpass filters have a 1.7 dB cut-o? frequency at 55 MHz. Since the maximum usable baseband signal is only 48 MHz (due to sinc frequency roll-o? e?ect, section 3.2) there is an alternate design...;#19;#0;#3;#0;#16;#0;#20;#0;#26;#0;#19;#0;#3;#0;0#0;+#0;] #0;,#0;/#0;#3;#0; #0;#3;#0;#22;#0;#3;#0;G#0;% #0;5#0;)#0;#3;#0;2#0;X#0;W #0;$#0;Q#0;D#0;O#0;R#0;J#0;#3;#0;'#0;H#0;Y#0;L#0;F#0;H#0;V #0;$#0;'#0;*#0;#28;#0;#19;#0;#20;#0;#3;#0;#16;#0;$#0;E#0;V#0;R...

Marathe, Kiran Chidambara

2008-03-06T23:59:59.000Z

213

Load balancing and adaptive scheduling for data intensive prioritised traffic in multi-radio multi-channel wireless mesh networks  

Science Journals Connector (OSTI)

In recent times, wireless technology has emerged as a key technology for many data intensive applications such as Video on Demand (VoD), Voice over IP (VoIP), high speed internet access, video conferencing, etc. All these applications require high data rate so that data can be transmitted to the end users in a prioritised manner. The underlying system that suits these applications better is the Wireless Mesh Network (WMN), because it is a special type of network which is cost effective, resilient and adaptive. To preserve the Quality of Service (QoS) for all these applications, in this paper, we propose a Load Balancing and Adaptive Scheduling (LBAS) algorithm for data intensive prioritised traffic in WMNs. To schedule the incoming traffic, the Available Capacity (AC) and Load Index (LI) of each link is calculated. A new Cost Evaluation Function (CEF) is defined based upon the values of AC and LI. Each traffic flow is also associated with Rate Index (RI) and Delay Estimation (DE). Each link has lower and upper bounds on AC, and as soon as the load on a particular link crosses these bounds, the load is transferred to another link dynamically at run time. Higher priority traffic will be assigned to the link having high value of AC to minimise DE, and simultaneously, a matrix for LI is also constructed. This matrix is used to keep track of the system load at run time, so that scheduling can be done for the incoming traffic in a prioritised manner based upon the values of AC and LI. The performance of the proposed algorithm is evaluated using simulations on ns-2 with respect to various metrics. The results obtained show that the proposed algorithm is quite effective for balancing the load of multiclass traffic flows.

Neeraj Kumar; Naveen Chilamkurti; Jong Hyouk Park; Doo Soon Park

2013-01-01T23:59:59.000Z

214

Design of multi-channel radio-frequency front-end for 200mhz parallel magnetic resonance imaging  

E-Print Network [OSTI]

increases to 64 or even 128, the traditional method of stacking the same number of radio-frequency (RF) receivers with very low level of integration becomes expensive and cumbersome. However, the cost, size, power consumption of the Parallel MRI receivers...

Liu, Xiaoqun

2009-05-15T23:59:59.000Z

215

3-D multichannel seismic reflection study of variable-flux hydrocarbon seeps, continental slope, northern Gulf of Mexico  

E-Print Network [OSTI]

. The reprocessed 3D seismic data were used to map in greater detail near seafloor features and amplitude anomalies. Using remote sensing geophysical data, we were effectively able to map sub-surface features such as salt topography, seep-related faults...

Thomas, Ryan Douglas

2004-11-15T23:59:59.000Z

216

Fast, multi-channel real-time processing of signals with microsecond latency using graphics processing units  

SciTech Connect (OSTI)

Fast, digital signal processing (DSP) has many applications. Typical hardware options for performing DSP are field-programmable gate arrays (FPGAs), application-specific integrated DSP chips, or general purpose personal computer systems. This paper presents a novel DSP platform that has been developed for feedback control on the HBT-EP tokamak device. The system runs all signal processing exclusively on a Graphics Processing Unit (GPU) to achieve real-time performance with latencies below 8 ?s. Signals are transferred into and out of the GPU using PCI Express peer-to-peer direct-memory-access transfers without involvement of the central processing unit or host memory. Tests were performed on the feedback control system of the HBT-EP tokamak using forty 16-bit floating point inputs and outputs each and a sampling rate of up to 250 kHz. Signals were digitized by a D-TACQ ACQ196 module, processing done on an NVIDIA GTX 580 GPU programmed in CUDA, and analog output was generated by D-TACQ AO32CPCI modules.

Rath, N., E-mail: Nikolaus@rath.org; Levesque, J. P.; Mauel, M. E.; Navratil, G. A.; Peng, Q. [Department of Applied Physics and Applied Mathematics, Columbia University, 500 W 120th St, New York, New York 10027 (United States)] [Department of Applied Physics and Applied Mathematics, Columbia University, 500 W 120th St, New York, New York 10027 (United States); Kato, S. [Department of Information Engineering, Nagoya University, Nagoya (Japan)] [Department of Information Engineering, Nagoya University, Nagoya (Japan)

2014-04-15T23:59:59.000Z

217

Multi-Channel Auto-Dilution System for Remote Continuous Monitoring of High Soil-CO2 Fluxes  

SciTech Connect (OSTI)

Geological sequestration has the potential capacity and longevity to significantly decrease the amount of anthropogenic CO2 introduced into the atmosphere by combustion of fossil fuels such as coal. Effective sequestration, however, requires the ability to verify the integrity of the reservoir and ensure that potential leakage rates are kept to a minimum. Moreover, understanding the pathways by which CO2 migrates to the surface is critical to assessing the risks and developing remediation approaches. Field experiments, such as those conducted at the Zero Emissions Research and Technology (ZERT) project test site in Bozeman, Montana, require a flexible CO2 monitoring system that can accurately and continuously measure soil-surface CO2 fluxes for multiple sampling points at concentrations ranging from background levels to several tens of percent. To meet this need, PNNL is developing a multi-port battery-operated system capable of both spatial and temporal monitoring of CO2 at concentrations from ambient to at least 150,000 ppmv. This report describes the system components (sampling chambers, measurement and control system, and power supply) and the results of a field test at the ZERT site during the late summer and fall of 2008. While the system performed well overall during the field test, several improvements to the system are suggested for implementation in FY2009.

Amonette, James E.; Barr, Jonathan L.

2009-04-23T23:59:59.000Z

218

Energy loss spectra of xenon and krypton and their analysis by energy-dependent multichannel quantum defect theory  

Science Journals Connector (OSTI)

Oscillator strengths of xenon and krypton for transitions from the ground state to the optically allowed states forming the five resonance series were measured by means of high energy electron spectroscopy (HE...

J. Geiger

1977-01-01T23:59:59.000Z

219

A truthful auction mechanism for channel allocation in multi-radio, multi-channel non-cooperative wireless networks  

Science Journals Connector (OSTI)

Due to users' fast-growing demands, wireless spectrum is becoming a more and more scarce resource. However, the state of spectrum usage shows that while large chunks of spectrum are left idle at many places, many emerging wireless applications cannot ... Keywords: Channel allocation, Game theory, Mechanism design, Wireless network

Zuying Wei, Tianrong Zhang, Fan Wu, Xiaofeng Gao, Guihai Chen, Ping Yi

2014-04-01T23:59:59.000Z

220

Submitted Phys. Rev. A 2002 Multichannel study of spin-exchange and hyper ne induced frequency shift and line  

E-Print Network [OSTI]

to the temperature range, 10 mK for Ultra-Cold Atoms, Cambridge MA 02139 USA ; Electronic address: bernard@physics.unlv. edu y Electronic

Stancil, Phillip C.

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

Studies of multichannel rotational predissociation of ArH2 van der Waals molecule by the complexcoordinate coupledchannel formalism  

E-Print Network [OSTI]

van der Waals molecules. Calculations are performed using several realistic anisotropic potentials obtained recently by experiments, including Lennard?Jones (LJ), BuckinghamCorner (BC) type potentials, as well as the semiempirical potential of Tang...

Chu, Shih-I; Datta, Krishna K.

1982-01-01T23:59:59.000Z

222

Monolithic multichannel ultraviolet detector arrays and continuous phase evolution in MgxZn1xO composition spreads  

E-Print Network [OSTI]

American Institute of Physics. DOI: 10.1063/1.1623923 I. INTRODUCTION ZnO is a wide band gap semiconductor whose potential device applications include UV lasers,1,2 transparent con- ducting films for solar cells simultaneously is central in today's photonics tech- nology. In order to detect signals at discrete wavelengths

Rubloff, Gary W.

223

Real Time Streaming of Multi-channel Audio Data over Internet 5120 (I -3) Aoxiang Xu and Jeremy Cooperstock,  

E-Print Network [OSTI]

and remittance to the Audio Engineering Society, 60 East 42nd St., New York, New York 10165-2520, USA. All rights from the Journal of the Audio Engineering Society. AN AUDIO ENGINEERING SOCIETY PREPRINT #12;XU sufficient for a society of musicians and professional audio engineers [l], to whom high

Cooperstock, Jeremy R.

224

Subduction dynamics at the middle America trench : new constraints from swath bathymetry, multichannel seismic data, and ?Be  

E-Print Network [OSTI]

The cosmogenic radionuclide ?Be is a unique tracer of shallow sediment subduction in volcanic arcs. The range in ?Be enrichment in the Central American Volcanic Arc between Guatemala and Costa Rica is not controlled by ...

Kelly, Robyn K

2003-01-01T23:59:59.000Z

225

Dynamic communities in multichannel data: An application to the foreign exchange market during the 20072008 credit crisis  

E-Print Network [OSTI]

, HSBC Bank, 8 Canada Square, London E14 5HQ, United Kingdom 5 Department of Physics, University of Miami

Porter, Mason A.

226

Table HC1-12a. Housing Unit Characteristics by West Census Region,  

U.S. Energy Information Administration (EIA) Indexed Site

2a. Housing Unit Characteristics by West Census Region, 2a. Housing Unit Characteristics by West Census Region, Million U.S. Households, 2001 Housing Unit Characteristics RSE Column Factor: Total U.S. West Census Region RSE Row Factors Total Census Division Mountain Pacific 0.5 1.0 1.7 1.1 Total .............................................................. 107.0 23.3 6.7 16.6 NE Census Region and Division Northeast ..................................................... 20.3 -- -- -- NF New England ............................................. 5.4 -- -- -- NF Middle Atlantic ........................................... 14.8 -- -- -- NF Midwest ....................................................... 24.5 -- -- -- NF East North Central ..................................... 17.1 -- -- -- NF West North Central ....................................

227

CEC'99 Amor & Anumba Page 1 of 12 A SURVEY AND ANALYSIS OF INTEGRATED  

E-Print Network [OSTI]

such as the application area, development environment, modelling approaches used, reusability, hardware and software and Dr C. J. Anumba2 ABSTRACT This paper is concerned with the development of an integrated project approaches to its development. A detailed survey and analysis of recent UK projects that have sought

Amor, Robert

228

Acoustic Performance Analysis of Bionic Coupling Multi-layer Structure Yonghua Wang1,2,a  

E-Print Network [OSTI]

coefficients and analyze the influences of different parameters of each layer on absorption coefficients. Laboratory of Tribology and System Dynamics, Ecole Centrale de Lyon, Ecully 69134, France 3. Laboratory bionic method to develop a new sound absorption structure. Inspired by the coupling absorption structure

Boyer, Edmond

229

Notes 12. (a) Annular pressure (damper) seals, and (b) Hydrostatic journal bearings  

E-Print Network [OSTI]

Bearings ? Learn more See http://phn.tamu.edu/TRIBGroup Publications For complete list of computational model predictions and comparisons to test data (over 30 journal papers and 10+ technical progress reports to NASA, USAF, P&W, Rocketdyne, Snecma... Bearings for Oil-Free Turbomachinery,? Journal of Engineering for Gas Turbines and Power, (2007), 129(4), pp. 1020-1027. NOTES 12(b): HYDROSTATIC JOURNAL BEARINGS ? ? Dr. Luis San Andr?s (2009) 18 San Andr?s, L., S. Phillips and D. Childs, Static...

San Andres, Luis

2009-01-01T23:59:59.000Z

230

CEWEP -Confederation of European Waste-to-Energy Plants Boulevard Clovis 12A  

E-Print Network [OSTI]

Recovered Fuel) as a fuel in both cement kilns and power plants, dedicated Biomass Energy Plants (BEP; BEP ­ Biomass Energy Plants; LFG ­ Landfill Gas; WtE ­ Waste-to-Energy 1 Excluding agricultural is considered biomass, thus a renewable energy source. Summary of the overall development of Renewable Energy

231

Titania nanostructure arrays from lithographically defined templates Deying Xia,1,2,a  

E-Print Network [OSTI]

and Engineering, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge, Massachusetts 02139,9 dye-sensitized solar cells,10 lithium-ion batteries,11 and superhydrophobic/ superhydrophilic

New Mexico, University of

232

Page 1 Vol. 18 No. 12 A Rutgers Cooperative Extension Publication  

E-Print Network [OSTI]

of crops where silicon nutrition helped to control powdery mildew disease in field trials and/or green as a liming material. For example, calcium silicate slag, a product produced during the manufacture of steel research has demonstrated that calcium silicate slag is an effec- tive liming material that it can

Goodman, Robert M.

233

3.12 A WILDLAND FIRE DYNAMIC DATA-DRIVEN APPLICATION SYSTEM Janice L. Coen  

E-Print Network [OSTI]

University of Colorado at Denver and Health Sciences Center, Denver, CO 3 University of Kentucky, Lexington- range forecast of wildfire behavior using a coupled atmosphere-fire model injected with real disparate data sources. The DDDAS is built upon a previously existing coupled atmosphere-wildfire model

Douglas, Craig C.

234

Anisotropic electrical resistivity during annealing of oriented columnar titanium films Nicolas MARTIN, 1,2 a)  

E-Print Network [OSTI]

1 Anisotropic electrical resistivity during annealing of oriented columnar titanium films Nicolas of anisotropic electrical resistivity versus temperature of titanium thin films. An oriented titanium film (1 µm. The average DC electrical resistivity changes from 6.03?10-6 to more than 2.40?10-1 m with the increasing

Paris-Sud XI, Université de

235

What is the fate of runaway positrons in tokamaks? Hong Qin,1,2,a)  

E-Print Network [OSTI]

positrons have been generated in accelerators for scien- tific research, in nuclear reactors or on the first wall of the vacuum chamber? Because the annihilation probability dependents on the path and veloc to runaway velocity by the loop voltage. In the toroidal direction, the runaway positrons are accelerated

236

Table HC1-2a. Housing Unit Characteristics by Year of Construction,  

U.S. Energy Information Administration (EIA) Indexed Site

2a. Housing Unit Characteristics by Year of Construction, 2a. Housing Unit Characteristics by Year of Construction, Million U.S. Households, 2001 Housing Unit Characteristics RSE Column Factor: Total Year of Construction RSE Row Factors 1990 to 2001 1 1980 to 1989 1970 to 1979 1960 to 1969 1950 to 1959 1949 or Before 0.5 1.6 1.2 1.0 1.1 1.1 0.8 Total ............................................... 107.0 15.5 18.2 18.8 13.8 14.2 26.6 4.3 Census Region and Division Northeast ...................................... 20.3 1.5 2.4 2.1 2.8 3.0 8.5 8.8 New England .............................. 5.4 0.4 0.7 0.4 0.8 0.9 2.3 11.3 Middle Atlantic ............................ 14.8 1.1 1.7 1.7 2.0 2.2 6.2 11.2 Midwest ......................................... 24.5 2.8 3.7 3.6 2.9 3.5 8.1 10.2 East North Central ...................... 17.1 2.0 2.5 2.5 2.0 2.6 5.5 11.9

237

b112.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

25) 25) 3/2 - I (J P ) = 0( 3 2 - ) Status: ∗ OMITTED FROM SUMMARY TABLE BACCARI 77 finds this state with either J P = 3/2 - or 3/2 + in a energy-dependent partial-wave analyses of K - p → Λ ω from 2070 to 2436 MeV. A subsequent semi-energy-independent analysis from threshold to 2436 MeV selects 3/2 - . DEBELLEFON 78 (same group) also sees this state in an energy-dependent partial-wave anal- ysis of K - p → K N data, and finds J P = 3/2 - or 3/2 + . They again prefer J P = 3/2 - , but only on the basis of model-dependent considerations. Λ(2325) MASS Λ(2325) MASS Λ(2325) MASS Λ(2325) MASS VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 2325 OUR ESTIMATE ≈ 2325 OUR ESTIMATE ≈ 2325 OUR ESTIMATE ≈ 2325 OUR ESTIMATE 2342± 30 DEBELLEFON 78 DPWA K N → K N 2327± 20 BACCARI 77 DPWA K - p → Λ ω Λ(2325) WIDTH Λ(2325) WIDTH Λ(2325) WIDTH Λ(2325) WIDTH VALUE (MeV) DOCUMENT ID TECN COMMENT 177± 40 DEBELLEFON 78 DPWA

238

b090.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

20) 20) 9/2 + I (J P ) = 1 2 ( 9 2 + ) Status: ∗∗∗∗ Most of the results published before 1975 were last included in our 1982 edition, Physics Letters 111B 111B 111B 111B 1 (1982). Some further obsolete results published before 1980 were last included in our 2006 edition, Journal of Physics, G 33 33 33 33 1 (2006). N(2220) BREIT-WIGNER MASS N(2220) BREIT-WIGNER MASS N(2220) BREIT-WIGNER MASS N(2220) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT 2200 to 2300 (≈ 2250) OUR ESTIMATE 2200 to 2300 (≈ 2250) OUR ESTIMATE 2200 to 2300 (≈ 2250) OUR ESTIMATE 2200 to 2300 (≈ 2250) OUR ESTIMATE 2316.3± 2.9 ARNDT 06 DPWA π N → π N, η N 2230 ± 80 CUTKOSKY 80 IPWA π N → π N 2205 ± 10 HOEHLER 79 IPWA π N → π N 2300 ± 100 HENDRY 78 MPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 2270 ± 11 ARNDT 04 DPWA π N → π N, η N 2258 ARNDT 95 DPWA π N → N π N(2220) BREIT-WIGNER

239
240

Journal of The Electrochemical Society, 158 (12) A1461-A1477 (2011) A1461 0013-4651/2011/158(12)/A1461/17/$28.00 The Electrochemical Society  

E-Print Network [OSTI]

Reformulation and Simulation of Electrochemical-Thermal Behavior of Lithium-Ion Battery Stacks Paul W. C-isothermal lithium-ion pseudo 2-D battery model. The transformed model is then conveniently discretized using operation of an 8-cell battery stack subject to varying heat transfer coefficients as well as specified

Subramanian, Venkat

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

file://C:\Documents%20and%20Settings\VM3\My%20Documents\hc6-12a  

U.S. Energy Information Administration (EIA) Indexed Site

2a. Usage Indicators by West Census Region, 2a. Usage Indicators by West Census Region, Million U.S. Households, 2001 ____________________________________________________________________________________________ | | | | | West Census Region | | |___________________________________| | | | | | | | Census Division | | | |_______________________|

242

Data:12a700f2-b169-42ae-bcdf-25646587ea4b | Open Energy Information  

Open Energy Info (EERE)

-b169-42ae-bcdf-25646587ea4b -b169-42ae-bcdf-25646587ea4b No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Loup River Public Power Dist Effective date: 2013/01/15 End date if known: Rate name: District Owned Lighting EMH 11000 Sector: Commercial Description: Source or reference: http://www.loup.com/customersvc/rates.asp Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >>

243

Data:12a45141-7972-4ec8-a2dc-37fedc8133d3 | Open Energy Information  

Open Energy Info (EERE)

5141-7972-4ec8-a2dc-37fedc8133d3 5141-7972-4ec8-a2dc-37fedc8133d3 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Ameren Illinois Company Effective date: 2010/11/19 End date if known: Rate name: DS-2 Zone 2 - Small General Delivery Service 600V to 15kV Sector: Commercial Description: AVAILABILITY Service under this Rate is available for any eligible Non-Residential Customer within the territory served by Company that meets the following criteria: Customers served under this Rate shall have a maximum monthly Demand of less than 150 kilowatts (kW) as qualified in the Delivery Service Rate Reassignment section. A Customer without a demand meter installed, but with an average usage of less than 1,200 kWh per day during each monthly billing period will be normally assumed to have a maximum monthly Demand of less than 150 kW. Where Customer's average daily usage is 1,200 kWh per day or more in any monthly billing period, Company may install a demand meter at Company's expense to determine if Customer remains eligible for service under this Rate.

244

Structure and stoichiometry of ,,0001... 4HSiC/oxide interface Xingguang Zhu,1,2,a  

E-Print Network [OSTI]

polytype of silicon carbide SiC is a promising candidate for high temperature and high power metal that hampers SiC device applications. The nature of the transition region stoichiometry and structure need beneath the SiC/SiO2 interface, setting limits on the previously predicted nonstoichiometric transition

Garfunkel, Eric

245

b000.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

0 0 Σ (1580) 3/2 - I (J P ) = 1( 3 2 - ) Status: ∗ OMITTED FROM SUMMARY TABLE Seen in the isospin-1 K N cross section at BNL (LI 73, CARROLL 76) NODE=B000 and in a partial-wave analysis of K - p → Λ π 0 for c.m. energies 1560-1600 MeV by LITCHFIELD 74. LITCHFIELD 74 finds J P = 3/2 - . Not seen by ENGLER 78 or by CAMERON 78C (with larger statistics in K 0 L p → Λ π + and Σ 0 π + ). Neither OLMSTED 04 (in K - p → Λ π 0 ) nor PRAKHOV 04 (in K - p → Λ π 0 π 0 ) see any evidence for this state. Σ (1580) MASS Σ (1580) MASS Σ (1580) MASS Σ (1580) MASS NODE=B000M NODE=B000M VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 1580 OUR ESTIMATE ≈ 1580 OUR ESTIMATE ≈ 1580 OUR ESTIMATE ≈ 1580 OUR ESTIMATE → UNCHECKED ← 1583 ± 4 1 CARROLL 76 DPWA Isospin-1 total σ 1582 ± 4 2 LITCHFIELD 74 DPWA K - p → Λ π 0 Σ (1580) WIDTH Σ (1580) WIDTH Σ (1580) WIDTH Σ (1580) WIDTH NODE=B000W NODE=B000W VALUE (MeV) DOCUMENT ID TECN COMMENT

246

b112.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

2 2 Λ(2325) 3/2 - I (J P ) = 0( 3 2 - ) Status: ∗ OMITTED FROM SUMMARY TABLE BACCARI 77 finds this state with either J P = 3/2 - or 3/2 + in a NODE=B112 energy-dependent partial-wave analyses of K - p → Λ ω from 2070 to 2436 MeV. A subsequent semi-energy-independent analysis from threshold to 2436 MeV selects 3/2 - . DEBELLEFON 78 (same group) also sees this state in an energy-dependent partial-wave anal- ysis of K - p → K N data, and finds J P = 3/2 - or 3/2 + . They again prefer J P = 3/2 - , but only on the basis of model-dependent considerations. Λ(2325) MASS Λ(2325) MASS Λ(2325) MASS Λ(2325) MASS NODE=B112M NODE=B112M VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 2325 OUR ESTIMATE ≈ 2325 OUR ESTIMATE ≈ 2325 OUR ESTIMATE ≈ 2325 OUR ESTIMATE → UNCHECKED ← 2342 ± 30 DEBELLEFON 78 DPWA K N → K N 2327 ± 20 BACCARI 77 DPWA K - p → Λ ω Λ(2325) WIDTH Λ(2325) WIDTH Λ(2325) WIDTH Λ(2325) WIDTH NODE=B112W

247

Efficient Scheduling and Grant Sizing Methods for WDM PONs  

Science Journals Connector (OSTI)

Bandwidth allocation and transmission grant scheduling are problems of particular interest to multichannel passive optical networks (PONs). While ...

Kiaei, Mohammad S; Meng, Lehan; Assi, Chadi; Maier, Martin

2010-01-01T23:59:59.000Z

248

Data:12a99515-0eda-4991-8ebe-b838e14266e0 | Open Energy Information  

Open Energy Info (EERE)

15-0eda-4991-8ebe-b838e14266e0 15-0eda-4991-8ebe-b838e14266e0 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Columbus Southern Power Co Effective date: 2012/03/09 End date if known: Rate name: Residential Storage Water Heating Energy Charge Sector: Residential Description: Storage Water Heating Provision: Availability of this provision is limited to those customers served under this provision as of December 31,2000.If the customer installs a Company approved storage water heating system which consumes electrical energy only during off-peak hours as specified by the Company and stores hot water for use during on-peak hours, the following shall apply: (a) For minimum capacity of 80 gallons, the last 300 KWH of use in any month shall be billed at the storage water heating energy charge. (Schedule Code 016)

249

Data:D12a4ee9-489c-4929-96b2-6324a0b8e925 | Open Energy Information  

Open Energy Info (EERE)

ee9-489c-4929-96b2-6324a0b8e925 ee9-489c-4929-96b2-6324a0b8e925 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Raton Public Service Company Effective date: End date if known: Rate name: Security Lights 3- Prompt Payment Discount Sector: Lighting Description: Security lights are available to all (except as noted) residential, commercial and industrial customers served by the Raton Public Service Company for outside lighting purposes at the voltage and phase of the company's distribution system. RPS owns fixture and pole, power is furnished by customer. RPS furnishes parts & service.

250

Data:65a49a12-a982-4cf5-8447-6f7ea00191e7 | Open Energy Information  

Open Energy Info (EERE)

a982-4cf5-8447-6f7ea00191e7 a982-4cf5-8447-6f7ea00191e7 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Anoka, Minnesota (Utility Company) Effective date: 2012/04/01 End date if known: Rate name: Parallel Generation Rate Time of Day Purchase Rate Industrial Sector: Industrial Description: Less than 40KW Source or reference: Rate Binder Kelly 3 ISU Documentation Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category:

251

Data:6e12a440-93b5-4896-a479-0a2a32a05d2a | Open Energy Information  

Open Energy Info (EERE)

2a440-93b5-4896-a479-0a2a32a05d2a 2a440-93b5-4896-a479-0a2a32a05d2a No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Intermountain Rural Elec Assn Effective date: End date if known: 2013/02/01 Rate name: Residential Time of Use (A-TOU) Sector: Residential Description: Residential Time of Use rate. Assumes all adjustments are included. Source or reference: Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous

252

Data:12a72f65-3385-4f7c-ab20-1355dd6f6a6b | Open Energy Information  

Open Energy Info (EERE)

-3385-4f7c-ab20-1355dd6f6a6b -3385-4f7c-ab20-1355dd6f6a6b No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tri-County Elec Member Corp Effective date: 2008/10/01 End date if known: Rate name: Outdoor Lighting HPS Underground Flood 400 W Sector: Lighting Description: Assuming Existing Pole Source or reference: http://www.tri-countyemc.com/skins/userfiles/file/Outdoor_lighting_1_2_3.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service

253

Data:0b12a8f0-ce39-41bc-b6cf-16606647c57c | Open Energy Information  

Open Energy Info (EERE)

a8f0-ce39-41bc-b6cf-16606647c57c a8f0-ce39-41bc-b6cf-16606647c57c No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Cuba City, Wisconsin (Utility Company) Effective date: 2009/10/14 End date if known: Rate name: Gs-1 General Service Three Phase Sector: Commercial Description: Power Cost Adjustment Clause - All metered rates shall be subject to a positive or negative power cost adjustment charge equivalent to the amount by which the current cost of power (per kilowatt-hour of sales) is greater or lesser than the base cost of power purchased (per kilowatt-hour of sales). The base cost of power (U) is $0.0765 per kilowatt-hour.

254

Data:F4d71c12-a075-4e42-ab03-ab9047022664 | Open Energy Information  

Open Energy Info (EERE)

a075-4e42-ab03-ab9047022664 a075-4e42-ab03-ab9047022664 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Borough of Kutztown, Pennsylvania (Utility Company) Effective date: End date if known: Rate name: INSTITIONAL SERVICE RATE120000 Sector: Commercial Description: Source or reference: http://www.kutztownboro.org/kutztown/uploads/ElectricRatesJanuary2012.pdf Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring:

255

Data:B12a96b8-e5dc-4002-a47e-f82fe67c5828 | Open Energy Information  

Open Energy Info (EERE)

b8-e5dc-4002-a47e-f82fe67c5828 b8-e5dc-4002-a47e-f82fe67c5828 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Mille Lacs Energy Cooperative Effective date: End date if known: Rate name: General Service Sector: Residential Description: Availability Available for all non-commercial service Source or reference: Rate Binder A Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service Voltage Category: Phase Wiring: << Previous 1 2 3 Next >>

256

Data:424a30a1-d12a-4cb7-b0f4-9285e6014872 | Open Energy Information  

Open Energy Info (EERE)

2a-4cb7-b0f4-9285e6014872 2a-4cb7-b0f4-9285e6014872 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Kit Carson Electric Coop, Inc Effective date: 2011/09/22 End date if known: Rate name: Market Based Rate Schedule Sector: Industrial Description: Available to all consumers within the Utility's service area who have entered into a contract, with a term of at least one year, for demand of 1,000 kW or more. Service shall be supplied through a point of delivery and measured through primary metering. Source or reference: www.kitcarson.com Source Parent: Comments Applicability Demand (kW)

257

Data:12a1bed7-432b-4810-83de-351ba5b1d371 | Open Energy Information  

Open Energy Info (EERE)

-432b-4810-83de-351ba5b1d371 -432b-4810-83de-351ba5b1d371 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Tipton Municipal Electric Util Effective date: 2004/08/13 End date if known: Rate name: Rate E- Outdoor Lighting Service: 400 Watt Metal Halide Sector: Lighting Description: Add $1.15 per month, if pole installation is required. Source or reference: Rates Binder 1, Illinois State University Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh) Minimum (kWh): Maximum (kWh): History (months): Service Voltage Minimum (V): Maximum (V): Character of Service

258

Data:175de12a-c7bb-4312-8cd7-5013d702e8e6 | Open Energy Information  

Open Energy Info (EERE)

2a-c7bb-4312-8cd7-5013d702e8e6 2a-c7bb-4312-8cd7-5013d702e8e6 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: City of Shelby, Ohio (Utility Company) Effective date: End date if known: Rate name: Schedule B- Three Phase Sector: Description: Delivery Voltages: $0.15/kVA Source or reference: http://www.amlegal.com/nxt/gateway.dll/Ohio/shelby_oh/parttenstreetsutilitiesandpublicservices/titlefour-utilities/chapter1050electricity?f=templates$fn=default.htm$3.0$vid=amlegal:shelby_oh$anc=JD_1050.02 Source Parent: Comments Applicability Demand (kW) Minimum (kW): Maximum (kW): History (months): Energy (kWh)

259

Data:7f77674c-c12a-4eca-85a1-474a5732a091 | Open Energy Information  

Open Energy Info (EERE)

Southeastern Power Admin Effective date: 20140516 End date if known: Rate name: Wholesale Power Rate Schedule NC-1-B Sector: Commercial Description: Availability: This rate...

260

Rough order of magnitude cost estimate for immobilization of 50MT of plutonium using new faciliites at the Savannah River site: alternative 12A  

SciTech Connect (OSTI)

The purpose of this Cost Estimate Report is to identify preliminary capital and operating costs for a facility to immobilize 50 metric tons of plutonium using ceramic in a new facility at Savannah River Site (SRS).

DiSabatino, A., LLNL

1998-06-01T23:59:59.000Z

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

ZPR-3 Assembly 12 : A cylindrical assembly of highly enriched uranium, depleted uranium and graphite with an average {sup 235}U enrichment of 21 atom %.  

SciTech Connect (OSTI)

Over a period of 30 years, more than a hundred Zero Power Reactor (ZPR) critical assemblies were constructed at Argonne National Laboratory. The ZPR facilities, ZPR-3, ZPR-6, ZPR-9 and ZPPR, were all fast critical assembly facilities. The ZPR critical assemblies were constructed to support fast reactor development, but data from some of these assemblies are also well suited for nuclear data validation and to form the basis for criticality safety benchmarks. A number of the Argonne ZPR/ZPPR critical assemblies have been evaluated as ICSBEP and IRPhEP benchmarks. Of the three classes of ZPR assemblies, engineering mockups, engineering benchmarks and physics benchmarks, the last group tends to be most useful for criticality safety. Because physics benchmarks were designed to test fast reactor physics data and methods, they were as simple as possible in geometry and composition. The principal fissile species was {sup 235}U or {sup 239}Pu. Fuel enrichments ranged from 9% to 95%. Often there were only one or two main core diluent materials, such as aluminum, graphite, iron, sodium or stainless steel. The cores were reflected (and insulated from room return effects) by one or two layers of materials such as depleted uranium, lead or stainless steel. Despite their more complex nature, a small number of assemblies from the other two classes would make useful criticality safety benchmarks because they have features related to criticality safety issues, such as reflection by soil-like material. ZPR-3 Assembly 12 (ZPR-3/12) was designed as a fast reactor physics benchmark experiment with an average core {sup 235}U enrichment of approximately 21 at.%. Approximately 68.9% of the total fissions in this assembly occur above 100 keV, approximately 31.1% occur below 100 keV, and essentially none below 0.625 eV - thus the classification as a 'fast' assembly. This assembly is Fast Reactor Benchmark No. 9 in the Cross Section Evaluation Working Group (CSEWG) Benchmark Specifications and has historically been used as a data validation benchmark assembly. Loading of ZPR-3 Assembly 12 began in late Jan. 1958, and the Assembly 12 program ended in Feb. 1958. The core consisted of highly enriched uranium (HEU) plates, depleted uranium plates and graphite plates loaded into stainless steel drawers which were inserted into the central square stainless steel tubes of a 31 x 31 matrix on a split table machine. The core unit cell consisted of two columns of 0.125 in.-wide (3.175 mm) HEU plates, seven columns of 0.125 in.-wide depleted uranium plates and seven columns of 0.125 in.-wide graphite plates. The length of each column was 9 in. (228.6 mm) in each half of the core. The graphite plates were included to produce a softer neutron spectrum that would be more characteristic of a large power reactor. The axial blanket consisted of 12 in. (304.8 mm) of depleted uranium behind the core. The thickness of the radial blanket was approximately 12 in. and the length of the radial blanket in each half of the matrix was 21 in. (533.4 mm). The assembly geometry approximated a right circular cylinder as closely as the square matrix tubes allowed. According to the logbook and loading records for ZPR-3/12, the reference critical configuration was loading 10 which was critical on Feb. 5, 1958. The subsequent loadings were very similar but less clean for criticality because there were modifications made to accommodate reactor physics measurements other than criticality. Accordingly, ZPR-3/12 loading 10 was selected as the only configuration for this benchmark. As documented below, it was determined to be acceptable as a criticality safety benchmark experiment. An accurate transformation to a simplified model is needed to make any ZPR assembly a practical criticality-safety benchmark. There is simply too much geometric detail in an exact (as-built) model of a ZPR assembly, even a clean core such as ZPR-3/12 loading 10. The transformation must reduce the detail to a practical level without masking any of the important features of the critical experiment. And it must d

Lell, R. M.; McKnight, R. D.; Perel, R. L.; Wagschal, J. J.; Nuclear Engineering Division; Racah Inst. of Physics

2010-09-30T23:59:59.000Z

262

Data:Da12a36f-ae00-4cb4-a9dd-ed19ceba5550 | Open Energy Information  

Open Energy Info (EERE)

reference: http:www.xcelenergy.comstaticfilesxeRegulatoryRegulatory%20PDFsratesMIMieSection4.pdf Source Parent: http:www.xcelenergy.comAboutUsRates&Regulations...

263

CMP 12A, Exam 1, 10/24/2003 Name: Login: 1 This is a 60 minute, CLOSED notes, books, etc. exam.  

E-Print Network [OSTI]

if anything is not clear. WORK INDIVIDUALLY. CHEATERS WILL BE REALLY SORRY. Strategy: Scan the entire exam side1, side2, side3; boolean vs12, vs13, vs21, vs23, vs31, vs32; vs12 = (side1 > side2); vs13 = (side1 > side3); vs21 = (side2 > side1); vs23 = (side2 > side3); vs31 = (side3 > side1); vs32 = (side3 > side2

Pang, Alex

264

Data:E4cc5a03-1850-4ec9-b817-5d679a29f12a | Open Energy Information  

Open Energy Info (EERE)

Medium General Service Sector: Commercial Description: Min. 11 kW - Max. 25 kW, Transformer Max. 50 kVA (MGS) Motors 10 HP (single phase), 50 HP (three phase) Additional kVA...

265

Zones of T-wave excitation in the NE Indian ocean mapped using variations in backazimuth over time obtained from multi-channel correlation of IMS hydrophone triplet data  

Science Journals Connector (OSTI)

......detection is coded in grey shades (light grey 0 to black 1). The...bathymetric features such as Christmas Island more than 3 south of...wave is also observed from the Christmas Island area. The corresponding...reflections from Java, from Christmas Island and from a seamount......

Frank M. Graeber; Pierre-Franck Piserchia

2004-07-01T23:59:59.000Z

266

Structural and Morphologic Study of Shatsky Rise Oceanic Plateau in the Northwest Pacific Ocean from 2D Multichannel Seismic Reflection and Bathymetry Data and Implications for Oceanic Plateau Evolution  

E-Print Network [OSTI]

Shatsky Rise is one of the largest oceanic plateaus, a class of volcanic features whose formation is poorly understood. It is also a plateau that was formed near spreading ridges, but the connection is unclear. The geologic structure and morphology...

Zhang, Jinchang

2014-04-10T23:59:59.000Z

267

PDF file  

E-Print Network [OSTI]

additive noise, and f ? Rn2 be an observation which satisfies the relationship ...... and its multichannel variant, which are suitable for impulsive noise removal.

2009-11-18T23:59:59.000Z

268

Enhanced thermal and gas flow performance in a three-way catalytic converter through use of insulation within the ceramic monolith  

Broader source: Energy.gov [DOE]

Emissions performance comparison of conventional catalytic converter with multi-channel catalytic converter (ceramic fiber insulation layers introduced into ceramic monolith of three-way catalytic converter)

269

E-Print Network 3.0 - abdelkader hameurlain rosine Sample Search...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Wales, Cardiff Collection: Computer Technologies and Information Sciences 14 Service Oriented Architecture in Multichannel e-Services Advanced Transactions for Electronic Summary:...

270

High-speed  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

system was operated as ei- ther a multi-channel interferometer or a polarimeter diagnos- tic, separately. To reconstruct the equilibrium current and magnetic field profiles and to...

271

E-Print Network 3.0 - absorption spectrometric detection Sample...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

is achieved using two... microbalance QCM , multichannel spectro- scopic ellipsometry,2,3 atomic absorption spectroscopy AAS , electron Source: Rubloff, Gary W. - Institute for...

272

A Journey from UCSB physics to Audrey Nelson  

E-Print Network [OSTI]

Target Gas Patented Waveguide Incandescent Infrared Source Microprocessor Diffusion Membranes Dual Beam integrated electronics Incandescent IR source and multi-channel thermopile detector Current gases applicable

Akhmedov, Azer

273

Proc. of the 9th Int. Conference on Digital Audio Effects (DAFX'06), Montreal, Canada, September 18-20, 2006 PARAMETRIC CODING OF STEREO AUDIO  

E-Print Network [OSTI]

Proc. of the 9th Int. Conference on Digital Audio Effects (DAFX'06), Montreal, Canada, September 18-20, 2006 DAFX-1 PARAMETRIC CODING OF STEREO AUDIO BASED ON PRINCIPAL COMPONENT ANALYSIS Manuel Briand parametric coding of multichannel audio is mainly based on Binaural Cue Coding (BCC). Another multichannel

Paris-Sud XI, Université de

274

Insulating state of granular superconductors in a strong-coupling regime I. S. Beloborodov,1 Ya. V. Fominov,1,2 A. V. Lopatin,1 and V. M. Vinokur1  

E-Print Network [OSTI]

Insulating state of granular superconductors in a strong-coupling regime I. S. Beloborodov,1 Ya. V-field-induced insulating state in a two-dimensional granular superconductor with relatively strong intergranular coupling the superconductor-insulator transi- tion, and a reentrant drop upon further increase of magnetic field. The magnetic

Fominov, Yakov

275

Data:Adb12a6c-76a5-4ff7-9db1-8e5b113c0667 | Open Energy Information  

Open Energy Info (EERE)

2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: Northern States Power Co - Wisconsin Effective date: 20120101 End date if known: Rate name:...

276

RCRA Facility investigation report for Waste Area Grouping 6 at Oak Ridge National Laboratory, Oak Ridge, Tennessee. Volume 5, Technical Memorandums 06-09A, 06-10A, and 06-12A: Environmental Restoration Program  

SciTech Connect (OSTI)

This report provides a detailed summary of the activities carried out to sample groundwater at Waste Area Grouping (WAG) 6. The analytical results for samples collected during Phase 1, Activity 2 of the WAG 6 Resource Conservation and Recovery Act Facility Investigation (RFI) are also presented. In addition, analytical results for Phase 1, activity sampling events for which data were not previously reported are included in this TM. A summary of the groundwater sampling activities of WAG 6, to date, are given in the Introduction. The Methodology section describes the sampling procedures and analytical parameters. Six attachments are included. Attachments 1 and 2 provide analytical results for selected RFI groundwater samples and ORNL sampling event. Attachment 3 provides a summary of the contaminants detected in each well sampled for all sampling events conducted at WAG 6. Bechtel National Inc. (BNI)/IT Corporation Contract Laboratory (IT) RFI analytical methods and detection limits are given in Attachment 4. Attachment 5 provides the Oak Ridge National Laboratory (ORNL)/Analytical Chemistry Division (ACD) analytical methods and detection limits and Resource Conservation and Recovery Act (RCRA) quarterly compliance monitoring (1988--1989). Attachment 6 provides ORNL/ACD groundwater analytical methods and detection limits (for the 1990 RCRA semi-annual compliance monitoring).

Not Available

1991-09-01T23:59:59.000Z

277

9/24/12 A cosmic whodunit: the case of the Higgs boson 1/5www.statesman.com/opinion/insight/a-cosmic-whodunit-the-case-of-the-higgs-2465209.html?viewAs...  

E-Print Network [OSTI]

with mass, and why do the media (but only a few scientists) call the Higgs the "God particle"? To understand and blogs around the world. Scientists using two separate and enormous particle accelerators -- the Tevatron

Toback, David

278

Electronic structure and ionicity of actinide oxides from first principles L. Petit,1,2,* A. Svane,1 Z. Szotek,2 W. M. Temmerman,2 and G. M. Stocks3  

E-Print Network [OSTI]

isotopes through irradiation, thus taking part in the fuel cycle and reducing the long-term nuclear-waste, and Cf. In original, "once through" reactors, the highly radioactive waste that was produced re- sulted in very troublesome long-time storage requirements; particularly of Pu. However, it was soon realized

Svane, Axel Torstein

279

3a-Phenyl-2,3,3a,4-tetrahydro-1H-benzo[d]pyrrolo[1,2-a]imidazol-1-one, a potential plant-growth regulator  

Science Journals Connector (OSTI)

Molecules of the title compound are linked into chains by intermolecular C=OH-N hydrogen bonds and the chains are weakly interconnected by - stacking interactions. A comparison of the geometric parameters of the title molecule and several related benzimidazoles and pyrrolidones is presented.

Grinev, V.S.

2013-07-09T23:59:59.000Z

280

Multiplet effects in the electronic structure of light rare-earth metals S. Lebgue,1,2 A. Svane,3 M. I. Katsnelson,4 A. I. Lichtenstein,5 and O. Eriksson1  

E-Print Network [OSTI]

radioactive element promethium is excluded from our study, since experimental information is more scarce. Also

Svane, Axel Torstein

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

Data:3c12a91f-c90f-4e1e-9d1e-7f1372e6b177 | Open Energy Information  

Open Energy Info (EERE)

1f-c90f-4e1e-9d1e-7f1372e6b177 1f-c90f-4e1e-9d1e-7f1372e6b177 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information Utility name: CenterPoint Energy Effective date: 2013/01/25 End date if known: Rate name: Secondary Service - Greater than 10 kVa, IDR Metered, greater than 2000 kVa (TC-LOS-A) - Muni Discount Rate Sector: Commercial Description: Delivery Service will be single-phase, 60 hertz, at a standard secondary voltage. Delivery Service will be metered using Company's standard watt-hour Meter provided for this type of Delivery Service. Any other metering option(s) will be provided at an additional charge and/or will be provided by a Meter Owner other than the Company pursuant to Applicable Legal Authorities. Where Delivery Service of the type desired is not available at the Point of Delivery, additional charges and special contract arrangements may be required prior to Delivery Service being furnished, pursuant to Section 6.1.2.2, Construction Services, in this Tariff.

282

CANDAC 16*16M Revision 1.  

E-Print Network [OSTI]

multi-channel functional generator. User can store in on-board memory up to 8 files, which describes changing output voltages in time by using a linear interpolation method. A start of file procession may

Kozak, Victor R.

283

1-apr-2011. Embedded software version 4.  

E-Print Network [OSTI]

or a single multi-channel functional generator. User can store in on-board memory a file, which describes changing output voltages in time by using a linear interpolation method. A start of file procession may

Kozak, Victor R.

284

Helicity amplitudes for photoexcitation of nucleon resonances off neutrons  

SciTech Connect (OSTI)

The helicity amplitudes $A^{1/2}_n$ and $A^{3/2}_n$ for the photoexcitation of nucleon resonances off neutrons are determined in a multi-channel partial-wave analysis.

Anisovich, A. V. [Bonn; Burkert, Volker D. [JLAB; Klempt, Eberhard [Bonn; Nikonov, A. V. [Bonn, PNPI Gatchina; Sarantsev, A. V. [Bonn, PNPI Gatchina; Thoma, Ulrike [Bonn

2013-06-01T23:59:59.000Z

285

How Sales Taxes Affect Customer and Firm Behavior: The Role of Search on the Internet  

E-Print Network [OSTI]

When a multichannel retailer opens its first retail store in a state, the firm is obligated to collect sales taxes on all Internet and catalog orders shipped to that state. This article assesses how opening a store affects ...

Anderson, Eric T.

286

Application of the 2-D Continuous Wavelet Transforms for Characterization of Geological and Geophysical Data  

E-Print Network [OSTI]

multi-channel seismic (MCS) data were collected over Shatsky Rise to image its upper crustal structure. These data have the potential to improve understanding of the processes of basaltic volcanism and the formation and evolution of oceanic plateaus...

Vuong, Au K

2014-05-05T23:59:59.000Z

287

Two-phase xenon emission detector with electron multiplier and optical readout by multipixel avalanche Geiger photodiodes  

E-Print Network [OSTI]

A successful operation of a new optical readout system (THGEM + WLS + MGPDs (multichannel array of multipixel avalanche Geiger photodiodes) in a two-phase liquid xenon detector was demonstrated.

Akimov, D Yu; Alexandrov, I S; Belov, V A; Bolozdynya, A I; Burenkov, A A; Buzulutskov, A F; Danilov, M V; Efremenko, Yu V; Kirsanov, M A; Kovalenko, A G; Stekhanov, V N

2013-01-01T23:59:59.000Z

288

Generalized quantum defect methods in quantum chemistry  

E-Print Network [OSTI]

The reaction matrix of multichannel quantum defect theory, K, gives a complete picture of the electronic structure and the electron - nuclear dynamics for a molecule. The reaction matrix can be used to examine both bound ...

Altunata, Serhan

2006-01-01T23:59:59.000Z

289

Alamos National Laboratory  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Economic development in Northern New Mexico focus of new podcast from Los Alamos National Laboratory November 25, 2013 Podcast part of Lab's new multi-channel effort to better...

290

Experimental and numerical characterization of ion-cyclotron heated protons on the Alcator C-Mod tokamak .  

E-Print Network [OSTI]

??Energetic minority protons with -100 keV effective temperature are routinely created in Alcator C-Mod plasmas with the application of ICRF. A new multi-channel Compact Neutral (more)

Tang, Vincent, 1978-

2006-01-01T23:59:59.000Z

291

Optimal Channel Probing and Transmission Scheduling for Opportunistic Spectrum Access  

E-Print Network [OSTI]

In this study, we consider optimal opportunistic spectrum access (OSA) policies for a transmitter in a multichannel wireless system, where a channel can be in one of multiple states. In such systems, the transmitter typically ...

Chang, Nicholas B.

292

Nested potassium hydroxide etching and protective coatings for silicon-based microreactors  

E-Print Network [OSTI]

We have developed a multilayer, multichannel silicon-based microreactor that uses elemental fluorine as a reagent and generates hydrogen fluoride as a byproduct. Nested potassium hydroxide etching (using silicon nitride ...

de Mas, Nuria

293

Time-resolved spectra in the 80340- wavelength region from Princeton Large Torus tokamak plasmas  

Science Journals Connector (OSTI)

High-resolution spectra from the Princeton Large Torus plasma have been recorded by a 2-m SchwobFraenkel soft-x-ray multichannel spectrometer. Spectra covering a wavelength range of...

Wouters, A; Dav, J H; Feldman, U; Seely, J F; Suckewer, S; Hinnov, E; Schwob, J L

1987-01-01T23:59:59.000Z

294

Emission in the 5080- region from highly ionized silver in Princeton Large Torus tokamak plasmas  

Science Journals Connector (OSTI)

The spectrum of silver emitted by Princeton Large Torus tokamak plasmas has been recorded in the 25150- region by a multichannel time-resolving grazing-incidence spectrometer. Silver...

Schwob, J L; Finkenthal, M; Wouters, A; Suckewer, S; Cohen, S A

1986-01-01T23:59:59.000Z

295

Mapping of volcanic apron and the upper crust between Gran Canaria and Tenerife (Canary Islands) with seismic reflection profiling  

Science Journals Connector (OSTI)

During the Volcanic Island Clastic Apron Project (VICAP), south of the Canary Islands, a total of 700 line-km multichannel seismic profiles were acquired. Two prominent reflectors (A and C) were observed alter...

A. Geisslinger; H. B. Hirschleber; M. Schnaubelt; J. J. Daobeitia

1996-01-01T23:59:59.000Z

296

One-Channel Audio Source Separation of Convolutive Mixture  

Science Journals Connector (OSTI)

Methods based on one-channel audio source separation are more practical than multi-channel ones in the real world applications. In this paper we proposed a new method to separate audio signals from single conv...

Jalal Taghia; Jalil Taghia

2008-01-01T23:59:59.000Z

297

b123.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

3 3 ∆(2300) 9/2 + I (J P ) = 3 2 ( 9 2 + ) Status: ∗∗ OMITTED FROM SUMMARY TABLE The latest GWU analysis (ARNDT 06) finds no evidence for this NODE=B123 resonance. ∆(2300) BREIT-WIGNER MASS ∆(2300) BREIT-WIGNER MASS ∆(2300) BREIT-WIGNER MASS ∆(2300) BREIT-WIGNER MASS NODE=B123M NODE=B123M VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 2300 OUR ESTIMATE ≈ 2300 OUR ESTIMATE ≈ 2300 OUR ESTIMATE ≈ 2300 OUR ESTIMATE → UNCHECKED ← 2204.5 ± 3.4 CHEW 80 BPWA π + p → π + p 2400 ± 125 CUTKOSKY 80 IPWA π N → π N 2217 ± 80 HOEHLER 79 IPWA π N → π N 2450 ± 100 HENDRY 78 MPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 2400 CANDLIN 84 DPWA π + p → Σ + K + ∆(2300) BREIT-WIGNER WIDTH ∆(2300) BREIT-WIGNER WIDTH ∆(2300) BREIT-WIGNER WIDTH ∆(2300) BREIT-WIGNER WIDTH NODE=B123W NODE=B123W VALUE (MeV) DOCUMENT ID TECN COMMENT 32.3 ± 1.0 CHEW

298

b051.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

1 1 Σ (1670) Bumps I (J P ) = 1(? ? ) OMITTED FROM SUMMARY TABLE Formation experiments are listed separately in the preceding entry. NODE=B051 Probably there are two states at the same mass with the same quan- tum numbers, one decaying to Σ π and Λ π, the other to Λ(1405) π. See the note in front of the preceding entry. Σ (1670) MASS Σ (1670) MASS Σ (1670) MASS Σ (1670) MASS NODE=B051M (PRODUCTION EXPERIMENTS) (PRODUCTION EXPERIMENTS) (PRODUCTION EXPERIMENTS) (PRODUCTION EXPERIMENTS) NODE=B051M VALUE (MeV) EVTS DOCUMENT ID TECN CHG COMMENT ≈ 1670 OUR ESTIMATE ≈ 1670 OUR ESTIMATE ≈ 1670 OUR ESTIMATE ≈ 1670 OUR ESTIMATE → UNCHECKED ← 1670 ± 4 1 CARROLL 76 DPWA Isospin-1 total σ 1675 ± 10 2 HEPP 76 DBC - K - N 1.6-1.75 GeV/c 1665 ± 1 APSELL 74 HBC K - p 2.87 GeV/c 1688 ± 2 or 1683 ± 5 1.2k BERTHON 74 HBC 0 Quasi-2-body σ 1670 ± 6 AGUILAR-... 70B HBC K - p → Σ π π 4 GeV OCCUR=2 1668 ±

299

b135.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

200) 200) 7/2 - I (J P ) = 3 2 ( 7 2 - ) Status: ∗ OMITTED FROM SUMMARY TABLE The various analyses are not in good agreement. The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. ∆(2200) BREIT-WIGNER MASS ∆(2200) BREIT-WIGNER MASS ∆(2200) BREIT-WIGNER MASS ∆(2200) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 2200 OUR ESTIMATE ≈ 2200 OUR ESTIMATE ≈ 2200 OUR ESTIMATE ≈ 2200 OUR ESTIMATE 2200± 80 CUTKOSKY 80 IPWA π N → π N 2215± 60 HOEHLER 79 IPWA π N → π N 2280± 80 HENDRY 78 MPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 2280± 40 CANDLIN 84 DPWA π + p → Σ + K + ∆(2200) BREIT-WIGNER WIDTH ∆(2200) BREIT-WIGNER WIDTH ∆(2200) BREIT-WIGNER WIDTH ∆(2200) BREIT-WIGNER WIDTH VALUE (MeV) DOCUMENT ID TECN COMMENT 450± 100 CUTKOSKY 80 IPWA π N → π N 400± 100 HOEHLER 79 IPWA π N → π N 400± 150 HENDRY

300

b051.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Bumps Bumps I (J P ) = 1(? ? ) OMITTED FROM SUMMARY TABLE Formation experiments are listed separately in the preceding entry. Probably there are two states at the same mass with the same quan- tum numbers, one decaying to Σ π and Λ π, the other to Λ(1405) π. See the note in front of the preceding entry. Σ (1670) MASS Σ (1670) MASS Σ (1670) MASS Σ (1670) MASS (PRODUCTION EXPERIMENTS) (PRODUCTION EXPERIMENTS) (PRODUCTION EXPERIMENTS) (PRODUCTION EXPERIMENTS) VALUE (MeV) EVTS DOCUMENT ID TECN CHG COMMENT ≈ 1670 OUR ESTIMATE ≈ 1670 OUR ESTIMATE ≈ 1670 OUR ESTIMATE ≈ 1670 OUR ESTIMATE 1670± 4 1 CARROLL 76 DPWA Isospin-1 total σ 1675± 10 2 HEPP 76 DBC - K - N 1.6-1.75 GeV/c 1665± 1 APSELL 74 HBC K - p 2.87 GeV/c 1688± 2 or 1683 ± 5 1.2k BERTHON 74 HBC 0 Quasi-2-body σ 1670± 6 AGUILAR-... 70B HBC K - p → Σ π π 4 GeV 1668± 10 AGUILAR-... 70B HBC K - p → Σ 3π 4 GeV 1660± 10 ALVAREZ 63 HBC + K - p 1.51

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

b041.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

1 1 Λ(2100) 7/2 - I (J P ) = 0( 7 2 - ) Status: ∗∗∗∗ Discovered by COOL 66 and by WOHL 66. Most of the results NODE=B041 published before 1973 are now obsolete and have been omitted. They may be found in our 1982 edition Physics Letters 111B 111B 111B 111B 1 (1982). This entry only includes results from partial-wave analyses. Param- eters of peaks seen in cross sections and in invariant-mass distribu- tions around 2100 MeV used to be listed in a separate entry immedi- ately following. It may be found in our 1986 edition Physics Letters 170B 170B 170B 170B 1 (1986). Λ(2100) MASS Λ(2100) MASS Λ(2100) MASS Λ(2100) MASS NODE=B041M NODE=B041M VALUE (MeV) DOCUMENT ID TECN COMMENT 2090 to 2110 (≈ 2100) OUR ESTIMATE 2090 to 2110 (≈ 2100) OUR ESTIMATE 2090 to 2110 (≈ 2100) OUR ESTIMATE 2090 to 2110 (≈ 2100) OUR ESTIMATE → UNCHECKED ← 2104 ± 10 GOPAL 80 DPWA K N → K N 2106 ± 30 DEBELLEFON

302

b123.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

300) 300) 9/2 + I (J P ) = 3 2 ( 9 2 + ) Status: ∗∗ OMITTED FROM SUMMARY TABLE The latest GWU analysis (ARNDT 06) finds no evidence for this resonance. ∆(2300) BREIT-WIGNER MASS ∆(2300) BREIT-WIGNER MASS ∆(2300) BREIT-WIGNER MASS ∆(2300) BREIT-WIGNER MASS VALUE (MeV) DOCUMENT ID TECN COMMENT ≈ 2300 OUR ESTIMATE ≈ 2300 OUR ESTIMATE ≈ 2300 OUR ESTIMATE ≈ 2300 OUR ESTIMATE 2204.5± 3.4 CHEW 80 BPWA π + p → π + p 2400 ± 125 CUTKOSKY 80 IPWA π N → π N 2217 ± 80 HOEHLER 79 IPWA π N → π N 2450 ± 100 HENDRY 78 MPWA π N → π N * * * We do not use the following data for averages, fits, limits, etc. * * * 2400 CANDLIN 84 DPWA π + p → Σ + K + ∆(2300) BREIT-WIGNER WIDTH ∆(2300) BREIT-WIGNER WIDTH ∆(2300) BREIT-WIGNER WIDTH ∆(2300) BREIT-WIGNER WIDTH VALUE (MeV) DOCUMENT ID TECN COMMENT 32.3± 1.0 CHEW 80 BPWA π + p → π + p 425 ± 150 CUTKOSKY 80 IPWA π N → π N 300 ± 100 HOEHLER 79 IPWA

303

Observation of the 2p 3=2 !2s 1=2 intrashell transition in Helike M. Trassinelli 1;2 (a) , A. Kumar 2;3 , H.F. Beyer 2 , P. Indelicato 4 , R. Martin 2;5 , R. Reuschl 1;2 ,  

E-Print Network [OSTI]

epl draft Observation of the 2p 3=2 !2s 1=2 intra­shell transition in He­like uranium M observation of the 1s2p 3 P2 ! 1s2s 3 S1 transition in He­like uranium. The experiment was performed and a germanium solid state detector. Using the 1s 2 2p 2 P 3=2 ! 1s 2 2s 2 S 1=2 transition in Li­like uranium

Recanati, Catherine

304

A.12a (Pre-SAS 115) Letter to communicate significant deficiencies and/or material weaknesses in internal control over financial reporting noted in an audit of financial statements of a nonpublic entity, excluding FDICIA engagements (Rev. 1/08)  

Broader source: Energy.gov (indexed) [DOE]

I325 8 I325 8 (8-89) EFG (07-90) United States Government Department of Energy Memorandum DATE: December 22,2009 REPLY TO A I T N OF: IG-322 (A09FN006) SUBJECT: Management Letter on the Audit of the Department of Energy's Consolidated Financial Statements for Fiscal Year 2009 TO: Chief Financial Officer, CF- 1 Attached is the subject letter prepared by KPMG LLP, our contract auditors. The letter contains 21 new findings (see letter, Exhibit A) and 5 repeat findings (see letter, Exhibit B) that were issued during the course of the Fiscal Year 2009 audit of the Department of Energy's (Department) Consolidated Financial Statements. Management generally concurred with and provided planned corrective actions for most of the recommendations listed in the Management Letter and management's comments are

305

ARM - Publications: Science Team Meeting Documents: The life stage of deep  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

The life stage of deep convection defined by the MSG multi-channel data and The life stage of deep convection defined by the MSG multi-channel data and rainfall type observed by PR/TRMM Inoue, Toshiro MRI/JMA The life cycle of deep convection is characterized as the cumulus/cumulonimbus type cloud classified by the method is dominant at the earlier stage and cirrus type cloud (anvil) is dominant at the decaying stage for no-split/no-merge case. We also know that convective rain is dominant at developing and mature stage, and stratiform rain is dominant at decaying stage. We studied the life cycle of deep convection in terms of cloud type using MSG ( Meteosat Second Generation) data taken every 15 minutes. The multi-channel data of MSG are use for cloud type classification. Cloud types are first classified by the split window method

306

Neural Networks 23 (2010) 685697 Contents lists available at ScienceDirect  

E-Print Network [OSTI]

Neural Networks 23 (2010) 685­697 Contents lists available at ScienceDirect Neural Networks journal Received in revised form 29 March 2010 Accepted 5 May 2010 Keywords: Micro-electrode array Cell culture Batch processing Connectivity a b s t r a c t Multi-channel acquisition from neuronal networks, either

Arleo, Angelo

307

Model-driven development of context-aware Web applications  

Science Journals Connector (OSTI)

Context-aware, multi-channel Web applications are more and more gaining consensus among both content providers and consumers, but very few proposals exist for their conceptual modeling. This article illustrates a conceptual framework that provides modeling ... Keywords: Context, WebML, adaptive hypertext, conceptual modeling, context-aware Web applications, context-awareness

Stefano Ceri; Florian Daniel; Maristella Matera; Federico M. Facca

2007-02-01T23:59:59.000Z

308

The synthesis of sound figures  

Science Journals Connector (OSTI)

In this paper we discuss a novel technique to control the spatial distribution of sound level within a synthesized sound field. The problem is formulated by separating the sound field into regions with high acoustic level, so-called bright regions, and ... Keywords: Multichannel sound reproduction, Quiet zones, Sound field synthesis, Sound figures

Karim Helwani; Sascha Spors; Herbert Buchner

2014-04-01T23:59:59.000Z

309

Episodic Rifting of Phanerozoic Rocks in the Victoria Land Basin, Western Ross Sea, Antarctica  

Science Journals Connector (OSTI)

...Geological Survey multichannel seismic-reflection tracklines, and location of seismic line 407 (Fig. 2). 1085 the axis tow art iions of naginatic rocks. The faultsap-pear to cut sedimentary rocks near the seafloor and to show an increasing dis-Olacement...

ALAN K. COOPER; F. J. DAVEY

1985-09-13T23:59:59.000Z

310

Cooperative Spectrum Sensing Using Q-Learning with Experimental Validation  

E-Print Network [OSTI]

approach is effective. This work is a part of the efforts toward building a cognitive radio network testbed-learning [9], [10] is one of the algorithms in the reinforcement learning family of machine learning selection without negotiations among secondary users for multi-user and multi-channel CR systems. Both

Qiu, Robert Caiming

311

THE PROTOTYPE OF RECORDING SYSTEM FOR SHOCK AND DETONATION WAVE INVESTIGATION WITH APPLICATION OF  

E-Print Network [OSTI]

THE PROTOTYPE OF RECORDING SYSTEM FOR SHOCK AND DETONATION WAVE INVESTIGATION WITH APPLICATION of the prototype of multichannel recording system for shock-wave and detonation processes investigations (first of all, shock-wave and detonation ones) [1, 2]. A prototype of recording system [3], providing

Fedotov, Mikhail G.

312

Impact of Secondary MAC Cooperation on Spectrum Sharing in Cognitive Radio Networks  

E-Print Network [OSTI]

Impact of Secondary MAC Cooperation on Spectrum Sharing in Cognitive Radio Networks Tariq Elkourdi and opportunistic spectrum access, and more generally cognitive radio, were introduced as possible solutions (see, e of secondary MAC coop- eration on the sum-throughput of multichannel cognitive radio networks is studied

Simeone, Osvaldo

313

THE DIGITAL SYSTEM ARTEMIS FOR REAL-TIME PROCESSING OF RADIO TRANSIENT EMISSIONS IN THE SOLAR CORONA  

E-Print Network [OSTI]

THE DIGITAL SYSTEM ARTEMIS FOR REAL-TIME PROCESSING OF RADIO TRANSIENT EMISSIONS IN THE SOLAR); it is used to process and record the 120 channels of a multichannel solar radiospectrograph in the frequency 30-80 MHz and a two-dimensional multicor- relator interferometer at 75.5 MHz. The large quantity

Athens, University of

314

Organisation Mndliche Prfung nach Vereinbarung  

E-Print Network [OSTI]

Modellbildung Verbrennungsmotor Benchmark Data Set Diesel Engine 10 Diesel Engine indicated torque boost pressure EGR rate start of injection rail pressure engine speed HC measured NOx measured Diesel series;2 Benchmark Data Sets 2.1 Diesel Engine 11 Experiment Space Multichannel s

Wichmann, Felix

315

Quantitative multiplex detection of pathogen biomarkers  

DOE Patents [OSTI]

The present invention addresses the simultaneous detection and quantitative measurement of multiple biomolecules, e.g., pathogen biomarkers through either a sandwich assay approach or a lipid insertion approach. The invention can further employ a multichannel, structure with multi-sensor elements per channel.

Mukundan, Harshini; Xie, Hongzhi; Swanson, Basil I; Martinez, Jennifer; Grace, Wynne K

2014-10-14T23:59:59.000Z

316

Design for scalability in enterprise SSDs  

Science Journals Connector (OSTI)

Solid State Drives (SSDs) have recently emerged as a high speed random access alternative to classical magnetic disks. To date, SSD designs have been largely based on multi-channel bus architecture that confronts serious scalability problems in high-end ... Keywords: i/o interface, interconnection network, nand flash memory, solid state drive

Arash Tavakkol, Mohammad Arjomand, Hamid Sarbazi-Azad

2014-08-01T23:59:59.000Z

317

Geological investigation of a lineated massif at the Kane Transform Fault: implications for oceanic core complexes  

Science Journals Connector (OSTI)

...al. 1998; Blackman et al. 1998) and marine multichannel seismic data (White et al...or as striations formed by abrasional wear along a fault surface (Cann et al. 1997...they are not the products of abrasional wear on frictional fault zones, they need not...

1999-01-01T23:59:59.000Z

318

Study of excited nucleons and their structure  

SciTech Connect (OSTI)

Recent advances in the study of excited nucleons are discussed. Much of the progress has been achieved due to the availability of high precision meson production data in the photoproduction and electroproduction sectors, the development of multi-channel partial wave analysis techniques, and advances in Lattice QCD with predictions of the full excitation spectrum.

Burkert, Volker D. [JLAB, Newport News, VA (United States)

2014-01-01T23:59:59.000Z

319

Pion- and photo-induced transition amplitudes to $?K$, $? K$, and $N?$  

E-Print Network [OSTI]

Pion and photo-induced inelastic reactions off protons are studied in a multichannel partial-wave analysis. Properties of nucleon and $\\Delta$ resonances are derived and compared to previous analyses. Amplitudes are shown for transitions to $N\\eta$, $\\Lambda K$, and $\\Sigma K$ final states.

A. V. Anisovich; R. Beck; E. Klempt; V. A. Nikonov; A. V. Sarantsev; U. Thoma

2012-05-10T23:59:59.000Z

320

Experimental multi-photon-resolving detector using a single avalanche photodiode  

E-Print Network [OSTI]

A multichannel detector has been constructed using a single avalanche photodiode and a fiber-loop delay line. Detection probabilities of the channels can be set using a variable-ratio coupler. The performance of the detector is demonstrated on its capability to distinguish multi-photon states (containing two or more photons) from the one-photon state and the vacuum state.

Ondrej Haderka; Martin Hamar; Jan Perina, Jr.

2003-02-20T23:59:59.000Z

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

Studies on the structure and dynamics of the human telomeric G quadruplex by single-molecule fluorescence resonance energy transfer  

Science Journals Connector (OSTI)

...multichannel scalar cards (MCS-plus, EG & G, ORTEC, Oak Ridge, TN). Sample solutions of 50 pM were used to achieve single-molecule detection...in equilibrium is consistent with the results of other workers. A switching between parallel and antiparallel quadruplexes...

Liming Ying; Jeremy J. Green; Haitao Li; David Klenerman; Shankar Balasubramanian

2003-01-01T23:59:59.000Z

322

The accident site portable integrated video system  

SciTech Connect (OSTI)

This paper presents a high bandwidth fiber-optic communication system intended for post accident recovery of weapons. The system provides bi-directional multichannel, and multi-media communications. Two smaller systems that were developed as direct spin-offs of the larger system are also briefly discussed.

Jones, D.P.; Shirey, D.L.; Amai, W.A.

1995-12-31T23:59:59.000Z

323

A Seismic Refraction and Reflexion Study of the Continent--Ocean Transition beneath the North Biscay Margin  

Science Journals Connector (OSTI)

5 May 1982 research-article A Seismic Refraction and Reflexion Study of the...post-rift sediments of Aptian to Recent age. Seismic refraction profiles were occupied on the...expanding spread multichannel (48-trace) seismic reflexion profiles and 30 km fixed offset...

1982-01-01T23:59:59.000Z

324

http://stir.ac.uk/4x Why study Retail Marketing?  

E-Print Network [OSTI]

http://stir.ac.uk/4x BA(Hons) Retail Marketing #12;Why study Retail Marketing? Retailers lead marketing: Retailers have taken over marketing leadership from manufacturers. Retailers lead innovation and change: Sophisticated customer relationship programmes, multi-channel promotional and marketing

Little, Tony

325

Realization of a 5-bit NMR Quantum Computer Using a New Molecular Architecture  

E-Print Network [OSTI]

We demonstrate a five-bit nuclear-magnetic-resonance quantum computer that distinguishes among various functions on four bits, making use of quantum parallelism. Its construction draws on the recognition of the sufficiency of linear coupling along a chain of nuclear spins, the synthesis of a suitably coupled molecule, and the use of a multi-channel spectrometer.

R. Marx; A. F. Fahmy; J. M. Myers; W. Bermel; S. J. Glaser

1999-05-25T23:59:59.000Z

326

Measurement of the half-life of (198)Au in a nonmetal: High-precision measurement shows no host-material dependence  

E-Print Network [OSTI]

://www.ortec-online.com/Solutions/multichannel-analyzers. aspx]. [8] R. Jenkins, R. W. Gould, and D. Gedcke, Quantitative X-ray Spectrometry (Dekker, New York, 1981), p. 266. [9] D. Radford (private communication) [http://radware.phy. ornl.gov/main.html]. [10] R. Brun and F. Rademakers, Nucl. Instrum...

Goodwin, J. R.; Nica, N.; Iacob, V. E.; Dibidad, A.; Hardy, John C.

2010-01-01T23:59:59.000Z

327

Developments in enzyme immobilization and near-infrared Raman spectroscopy with downstream renewable energy applications  

SciTech Connect (OSTI)

This dissertation focuses on techniques for (1) increasing ethanol yields from saccharification and fermentation of cellulose using immobilized cellulase, and (2) the characterization and classification of lignocellulosic feedstocks, and quantification of useful parameters such as the syringyl/guaiacyl (S/G) lignin monomer content using 1064 nm dispersive multichannel Raman spectroscopy and chemometrics.

Lupoi, Jason [Ames Laboratory

2012-08-27T23:59:59.000Z

328

Motors Motor controllers  

E-Print Network [OSTI]

Aluminium frame Motors Motor controllers Ultrasonic multi-channel acquisition PC Tank Tank 400 600 800 1000 0 50 2 4 6 8 x 10 -3 r/r 0 Range (mm) Depth(mm) 25 /t Tand / or #12;Shallow water

329

Electron, Photon, and Positron Scattering Dynamics of Complex Molecular Targets  

E-Print Network [OSTI]

from ground state Cl2 and Pt in the 1S and 3D states in the multichannel configuration-interaction (MCCI) approximation originally developed for photoionization for scattering up to 10 eV. Photoionization cross sections and angular distributions...

Carey, Ralph

2012-07-16T23:59:59.000Z

330

Patch-based Segmentation of Brain Tissues Nicolas Cordier1  

E-Print Network [OSTI]

Patch-based Segmentation of Brain Tissues Nicolas Cordier1 , Bjoern Menze1,2 , Herv´e Delingette1-channel patches. After patches are extracted from several MR channels for a test case, similar patches are found to these developed for human brain labelling in [1]. A database of multi-channel patches is first built from a set

Paris-Sud XI, Université de

331

ETH Zurich Distributed Computing Group Stephan HolzerETH Zurich Distributed Computing www.disco.ethz.ch Stephan Holzer -ETH Zrich  

E-Print Network [OSTI]

ETH Zurich ­ Distributed Computing Group Stephan HolzerETH Zurich ­ Distributed Computing ­ www Wattenhofer - ETH Zürich Deterministic Multi-Channel Information Exchange #12;ETH Zurich ­ Distributed Problem: n:= # nodes k:= # information Have information Disseminate to all! ? #12;ETH Zurich ­ Distributed

332

High resolution bragg focusing optics for synchrotron monochromators and analyzers  

SciTech Connect (OSTI)

A number of different applications for high resolution Bragg Focusing Optics are reviewed. Applications include Sagittal Focusing, Energy Dispersive optics for x-ray absorption and diffraction, a curved analyzer-multichannel detector method for efficient acquisition of powder and small angle scattering data, the use of Backscattering Analyzers for very high resolution inelastic scattering, and curved crystals for high energy applications.

Knapp, G.S.; Beno, M.A.; Gofron, K.J.

1997-07-01T23:59:59.000Z

333

IEEE TRANSACTIONS ON SIGNAL PROCESSING, VOL. 57, NO. 4, APRIL 2009 1469 Finite Word Length Effects on Transmission Rate in  

E-Print Network [OSTI]

, vectoring. I. INTRODUCTION DSL systems are capable of delivering high data rates over copper lines. A major on Transmission Rate in Zero Forcing Linear Precoding for Multichannel DSL Eitan Sayag, Amir Leshem, Senior Member factor in trans- mission over copper lines. Crosstalk cancellation techniques show greatpotential

Langendoen, Koen

334

Audio Engineering Society Convention Paper  

E-Print Network [OSTI]

Audio Engineering Society Convention Paper Presented at the 120th Convention 2006 May 20­23 Paris. Additional papers may be obtained by sending request and remittance to Audio Engineering Society, 60 East 42 of the Audio Engineering Society. Parametric Representation of Multichannel Audio Based on Principal Component

Paris-Sud XI, Université de

335

Tensor-based Detection of T Wave Alternans in Multilead ECG Signals G Goovaerts1,2  

E-Print Network [OSTI]

Tensor-based Detection of T Wave Alternans in Multilead ECG Signals G Goovaerts1,2 , C Varon1,2 , B for the detection of T wave alternans in multichannel ECG signals is introduced. The use of tensors robust. To construct a 3D tensor from a 2D ECG signal, the T wave is first roughly segmented

336

What ICA Provides for ECG Processing: Application to Noninvasive Fetal ECG Extraction  

E-Print Network [OSTI]

What ICA Provides for ECG Processing: Application to Noninvasive Fetal ECG Extraction Reza Sameni1 (ICA) has been used for the analysis of multi-channel ECG recordings. However most of these works have of the heart and the ECG dimensionality are studied from the source separation viewpoint. Based on this study

Paris-Sud XI, Université de

337

ROBUST 3-WAY TENSOR DECOMPOSITION AND EXTENDED STATE KALMAN FILTERING TO EXTRACT FETAL ECG  

E-Print Network [OSTI]

ROBUST 3-WAY TENSOR DECOMPOSITION AND EXTENDED STATE KALMAN FILTERING TO EXTRACT FETAL ECG Mohammad ABSTRACT This paper addresses the problem of fetal electrocardiogram (ECG) extraction from multichannel that are robust to outliers are proposed and used to better track weak traces of the fetal ECG. Then, the state

Boyer, Edmond

338

The Cyclin-Dependent Kinase Inhibitor KRP6 Induces Mitosis and Impairs Cytokinesis in Giant Cells Induced by Plant-Parasitic Nematodes in Arabidopsis  

Science Journals Connector (OSTI)

...that the irregular-sized nuclei and nuclear fusion observed in cell cultures with ectopic...multichannel setting with 488- and 543-nm laser source for GFP and RFP excitation, respectively...GFP was excited with a 488-nm argon laser, and fluorescence was captured in lambda...

Paulo Vieira; Annelies De Clercq; Hilde Stals; Jelle Van Leene; Eveline Van De Slijke; Gert Van Isterdael; Dominique Eeckhout; Geert Persiau; Daniël Van Damme; Aurine Verkest; José Dijair Antonino de Souza; Júnior; Nathalie Glab; Pierre Abad; Gilbert Engler; Dirk Inzé; Lieven De Veylder; Geert De Jaeger; Janice de Almeida Engler

2014-06-24T23:59:59.000Z

339

Kadygrov-EN  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Investigation of the Atmospheric Boundary Layer Investigation of the Atmospheric Boundary Layer Thermodynamics on the Base of Microwave Remote Sensing E. N. Kadygrov, V. E. Kadygrov, A. D. Lykov, E. A. Miller, and A. V. Troitsky Central Aerological Observatory Russia Introduction Temperature profiles through the atmospheric boundary layer (ABL) are important in studying the energy balance near the ground surface and in validating satellite remote sensing retrievals. For continuous measurement of atmospheric temperature during the last several years different microwave remote sensing instruments were used: multichannel (Westwater 1993; Ware and Solheim 2000) and single-channel scanning radiometers (Troitsky et al. 1993; Westwater et al. 1999). Multi-channel instruments can measure temperature profiles up to about 7 - 10 km in contrast with the single-channel

340

System and method for assaying a radionuclide  

DOE Patents [OSTI]

A system for assaying a radionuclide includes a liquid scintillation detector, an analyzer connected to the liquid scintillation detector, and a delay circuit connected to the analyzer. A gamma detector and a multi-channel analyzer are connected to the delay circuit and the gamma detector. The multi-channel analyzer produces a signal reflective of the radionuclide in the sample. A method for assaying a radionuclide includes selecting a sample, detecting alpha or beta emissions from the sample with a liquid scintillation detector, producing a first signal reflective of the alpha or beta emissions, and delaying the first signal a predetermined time. The method further includes detecting gamma emissions from the sample, producing a second signal reflective of the gamma emissions, and combining the delayed first signal with the second signal to produce a third signal reflective of the radionuclide.

Cadieux, James R; King, III, George S; Fugate, Glenn A

2014-12-23T23:59:59.000Z

Note: This page contains sample records for the topic "12a dpwa multichannel" 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.


341

Angular momentum reduction for physical amplitudes in the three-body problem  

Science Journals Connector (OSTI)

We give here an approach to the angular momentum reduction that is tailed to be appropriate for the multichannel structure of the three-body problem. Wherever possible we work directly with the physical scattering amplitudes. We obtain concrete partial-wave expansions of elastic, rearrangement, and breakup amplitudes. For these amplitudes we obtain a coupled two-variable integral equation. The effects of parity, time reversal, and rotational invariance are fully discussed. Finally, we provide expressions for the multichannel partial-wave cross sections, asymptotic coordinate-space wave functions, off-shell unitarity, and the partial-wave version of the optical theorem as well as phase-shift parametrizations of the amplitudes.

D. Boll and T. A. Osborn

1974-02-01T23:59:59.000Z

342

Mass spectrometer calibration of Cosmic Dust Analyzer Thomas J. Ahrens, Satish C. Gupta,1  

E-Print Network [OSTI]

. Using aluminum alloy as a test sample, each pulse produces a charge of $4.6 pC (mostly Al+1 ), whereas of the instrument. Particles impact a Rh target plate at velocities of 1-100 km/s and produce some 10?8 to 10?5 in the CDA geometry. Employing a multichannel plate detector in this MS yields for Al-Mg-Cu alloy

Stewart, Sarah T.

343

Rate Coefficients and Kinetic Isotope Effect for the C2H Reactions with NH3 and ND3 in the 104?294 K Temperature Range  

Science Journals Connector (OSTI)

Departments of Chemistry and Physics and Lawrence Berkeley National Laboratory, University of California, Berkeley, California 94720 ... The chemiluminescence signal is detected using a photomultiplier tube with a 430 nm band-pass filter (10 nm band-pass) and recorded using a multichannel scaler in a photon counting regime. ... Using the NO + O ? NO2* chemiluminescence as a calibration std., CH* formation rates were derived from the measured I(CH*), and the values of the rate coeff. ...

Boris Nizamov; Stephen R. Leone

2004-03-31T23:59:59.000Z

344

Highly excited {Sigma}{sup -} states of molecular hydrogen  

SciTech Connect (OSTI)

We report calculations of H{sub 2} {Sigma}{sup -} states using a variational R-matrix approach combined with multichannel quantum defect theory. Several Rydberg series converging to the 2p{pi} state of the H{sub 2}{sup +} ion core are established and their mutual channel interactions characterized. The influence of the external electron on the chemical bond is found to be particularly strong in these electronically and chemically weakly bound states.

Argoubi, F.; Bezzaouia, S.; Oueslati, H. [LSAMA Department of Physics, Faculty of Science of Tunis, University of Tunis El Manar, 2092 Tunis (Tunisia); Telmini, M. [LSAMA Department of Physics, Faculty of Science of Tunis, University of Tunis El Manar, 2092 Tunis (Tunisia); National Centre for Nuclear Science and Technology, Sidi Thabet Technopark 2020 (Tunisia); Jungen, Ch. [Laboratoire Aime Cotton du CNRS, Universite de Paris-Sud, F-91405 Orsay (France)

2011-05-15T23:59:59.000Z

345

The Seismic Stratigraphy and Sedimentation along the Ninetyeast Ridge  

E-Print Network [OSTI]

examines the stratigraphy and sediment thickness on the ridge using new seismic data to describe the sedimentary history of NER. More than 3700 km of 2D multichannel seismic reflection profiles were collected along NER at seven sites between 5.5? N............................................................................ 28 Figure 2 Seismic Survey Map of KNOX06RR Site 758 .................................. 29 Figure 3 Total Sediment Thickness Isopach Map of KNOX06RR Site 758 .... 30 Figure 4 Seismic Reflection Profile from KNOX06RR Site 758 .................... 31...

Eisin, Amy Elizabeth

2010-10-12T23:59:59.000Z

346

Raman activity in synchronously dividing bacteria  

SciTech Connect (OSTI)

Using a spectrometer equipped with an optical-multichannel analyzer as the detector (OMA), we have observed the Stokes laser-Raman spectra of metabolically active Escherichia coli and Bacillus megaterium from 100 - 2100 cm/sup -1/. After lengthy investigation, no Raman lines attributable to the metabolic process nor the cells themselves were found. Previous Raman spectra of active bacteria cannot be used to support nonlinear theories in biology. 34 refs., 9 figs.

Layne, S.P.

1985-01-01T23:59:59.000Z

347

A simple technique for gamma ray and cosmic ray spectroscopy using plastic scintillator  

E-Print Network [OSTI]

A new and simple technique has been developed using plastic scintillator detectors for gamma ray and cosmic ray spectroscopy without single channel analyzer (SCA) or multichannel analyzer (MCA). In these experiments only a leading edge discriminator (LED) and NIM scalers have been used. Energy calibration of gamma spectra in plastic scintillators has been done using Co$^{60}$ and Cs$^{137}$ sources. The details experimental technique, analysis procedure and experimental results has been presented in this article.

Akhilesh P. Nandan; Sharmili Rudra; Himangshu Neog; S. Biswas; S. Mahapatra; B. Mohanty; P. K. Samal

2014-12-30T23:59:59.000Z

348

Methods for characterizing, classifying, and identifying unknowns in samples  

DOE Patents [OSTI]

Disclosed is a method for taking the data generated from an array of responses from a multichannel instrument, and determining the characteristics of a chemical in the sample without the necessity of calibrating or training the instrument with known samples containing the same chemical. The characteristics determined by the method are then used to classify and identify the chemical in the sample. The method can also be used to quantify the concentration of the chemical in the sample.

Grate, Jay W [West Richland, WA; Wise, Barry M [Manson, WA

2002-01-01T23:59:59.000Z

349

Gray disks in perturbative Reggeon calculus  

Science Journals Connector (OSTI)

We discuss the connection between the opacity of a gray disk and its diffraction-dissociation cross section in the multichannel eikonal model which is formulated in such a way as to take account of continuum intermediate states of the projectile. The model is equivalent to Reggeon calculated to a finite order in the triple-Pomeron coupling and where the bare-Pomeron intercept exceeds unity.

G. A. Winbow

1977-07-15T23:59:59.000Z

350

Developing a Methodology for Characterizing the Effects of Building Materials Natural Radiation Background on a Radiation Portal Monitoring System  

E-Print Network [OSTI]

the sponsors of this research, Oak Ridge National Laboratory (ORNL). vi NOMENCLATURE EW Energy Windowing FWHM Full-Width at Half Maximum HEU Highly Enriched Uranium HPGe High-Purity Germanium ISOCS In-Situ Object Counting System MCA Multichannel... Naturally Occurring Radioactive Material ? Diameter ORNL Oak Ridge National Laboratory PMT Photomultiplier Tube PNNL Pacific Northwest National Laboratory PVT Polyvinyl Toluene RDD Radiological Dispersal Device vii RPM Radiation Portal Monitor...

Fitzmaurice, Matthew Blake 1988-

2012-11-06T23:59:59.000Z

351

Two-phase interfacial area and flow regime modeling in FLOWTRAN-TF code  

SciTech Connect (OSTI)

FLOWTRAN-TF is a new two-component, two-phase thermal-hydraulics code to capture the detailed assembly behavior associated with loss-of-coolant accident analyses in multichannel assemblies of the SRS reactors. The local interfacial area of the two-phase mixture is computed by summing the interfacial areas contributed by each of three flow regimes. For smooth flow regime transitions, the code uses an interpolation technique in terms of component void fraction for each basic flow regime.

Smith, F.G. III; Lee, S.Y.; Flach, G.P.; Hamm, L.L.

1992-12-31T23:59:59.000Z

352

Two-phase interfacial area and flow regime modeling in FLOWTRAN-TF code  

SciTech Connect (OSTI)

FLOWTRAN-TF is a new two-component, two-phase thermal-hydraulics code to capture the detailed assembly behavior associated with loss-of-coolant accident analyses in multichannel assemblies of the SRS reactors. The local interfacial area of the two-phase mixture is computed by summing the interfacial areas contributed by each of three flow regimes. For smooth flow regime transitions, the code uses an interpolation technique in terms of component void fraction for each basic flow regime.

Smith, F.G. III; Lee, S.Y.; Flach, G.P.; Hamm, L.L.

1992-01-01T23:59:59.000Z

353

Feshbach resonances in ultracold atom-diatom scattering  

Science Journals Connector (OSTI)

Quantum-mechanical scattering calculations of Feshbach resonances arising from van der Waals molecule formation are used to determine vibrational and rotational predissociation lifetimes. A multichannel effective range theory is used to establish the relationship between predissociation and the zero-temperature limit of collisional quenching for resonances lying close to the thresholds for dissociation. The elastic scattering Feshbach resonances may be measurable in ultracold atom-molecule experiments.

R. C. Forrey; N. Balakrishnan; V. Kharchenko; A. Dalgarno

1998-10-01T23:59:59.000Z

354

The effect of a constant magnetic field on spontaneous activity of the subesophageal ganglion of the cockroach, Periplaneta americana  

E-Print Network [OSTI]

of the Investigation Historical Background, CHAPTER II - APPARATUS AND PROCEDURES Apparatus for Collecting Bioelectrical Data Electrically shielded flow system . Electrode assembly Movable e le c trode car riage Permanent magnet Ganglion Pre-amplifier. Audio... oscillator ~ Stereo tape recorder, oscilloscope, and audio amplifier Apparatus for Analyzing Bioelectrical Data. Tape recorder, audio amplifier, and pre-amplifier ~ Pulse converter and oscilloscope Multi-channel analyzer and electric typewriter ~ 9...

Russell, Dennis Reginald

2012-06-07T23:59:59.000Z

355

High-resolution seismic stratigraphic analysis of the Late Quaternary upper slope and shelf edge: Main Pass-Viosca Knoll area, Gulf of Mexico  

SciTech Connect (OSTI)

High-resolution (800 Hz) sparker data from the Main Pass-Viosca Knoll area, offshore Louisiana, show shelf-edge deltas with oblique progradational clinoforms, parallel, and channel-fill reflections in the near-surface, latest Quaternary section of the upper slope. Sequence boundaries are indicated by onlap of slope facies onto older outershelf deltas and shelf margins, erosional truncation, and minor channel erosion on the top of progradational units and on the slope. The authors tentatively identify these sequence boundaries as Type I. Each depositional sequence consists of two seismic units: (1) a lower unit consisting of parallel, seaward-dipping reflections; (2) an upper unit consisting of parallel reflections and progradational clinoforms that converge or downlap downslope on top of the lower parallel unit. Precise correlation to absolute time and sea level awaits analysis and integration of shallow cores taken in the area by an industry consortium. Facies and isochron mapping of each sequence indicates an overall back-stepping of the shelf-edge deltas and shelf margins during the latest Quaternary. The Quaternary shelf edges are an area of isochron thicks and thins resulting from erosion and redeposition. Major channels commonly cross salt diapirs and may occupy the same site during successive lowstands. Comparison with multichannel seismic profiles shows that each shelf-edge delta seen on the high resolution profiles is represented by a single reflection on multichannel data. Steep clinoforms, downlap surfaces, and individual sequences are not seen on the multichannel data.

McMillen, K.J. (Marathon Oil Co., Houston, TX (United States)); Winn, R.D. Jr. (Marathon Oil Co., Littleton, CO (United States)); Damuth, J.E. (Mobile Oil Co., Dallas, TX (United States)); Weimer, P. (Univ. of Colorado, Boulder (United States))

1991-03-01T23:59:59.000Z

356

What is Geovisualization? Why is the work needed?  

E-Print Network [OSTI]

#12;Research Frontiers... Geocomputation and Database Semantics #12;Research Frontiers... Uncertainty History ILM 1982 #12;A Brief History ILM 1983 #12;A Brief History JPL 1987 #12;A Brief History Terra

Wright, Dawn Jeannine

357

Gene finding with Hidden Markov  

E-Print Network [OSTI]

Initial distribution: A B PAB PBA PBB PAA #12;A simple HMM Initial distribution: A B PAB PBA PBB PAA #12;A

Pachter, Lior

358

Ultrahigh heat flux plasma-facing components for magnetic fusion energy  

SciTech Connect (OSTI)

Sandia and Ultramet partnered to design and test refractory metal plasma-facing components and heat exchangers for advanced, high-temperature power conversion systems. These devices consisted of high-temperature helium-to-helium and lithium-to-helium heat exchangers that operate with high efficiency due to the porous foam inserts used in the gas stream, which promote turbulence and provide extended surface area for enhanced convection. Single- and multi-channel helium panels and the Li-He heat exchanger were fabricated from either pure molybdenum, TZM, or tungsten. The design was carried out through an Ultramet subcontractor. The flow path was carefully tailored to minimize the pressure drop while maximizing the heat transfer. The single- and multi-channel helium panels were tested at Sandia's PMTF using an electron beam system and the closed helium flow loop. In 2006, a single-channel tungsten tube was successfully tested to an average heat flux of 14 MW/m{sup 2} with a localized peak of 22 MW/m{sup 2} along the axial centerline at the outer radius. Under this CRADA, multiple square-channel molybdenum components were successfully tested to heat flux levels approaching 8.5 MW/m{sup 2}. The three multi-channel prototypes experienced mechanical failure due to issues related to the design of the large unsupported span of the heated faceplates in combination with prototype material and braze selection. The Li-He heat exchanger was both designed and partially tested at the PMTF for helium and lithium flow.

Youchison, D. L.

2012-03-01T23:59:59.000Z

359

COMMUNITY CHOICE AGGREGATION PILOT PROJECT  

E-Print Network [OSTI]

........................................................................................11 3. Energy Efficiency Impacts..........................................................................................11 III. Organizational Structure........................................................................................................12 A. Organizational Overview

360

High-Throughput Methodology for Discovery of Metal-Organic Frameworks with a High  

E-Print Network [OSTI]

of California, Berkeley Lily Ackerman and Thomas R. Boussie Symyx Technologies, Inc. #12;A Tetrazolate

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

THE HEBREW UNIVERSITY OF JERUSALEM: FOR THE WORLD THE PRESIDENT'S REPORT 2005/2006  

E-Print Network [OSTI]

COSTA RICA KAZAKHSTAN CAMEROON SURINAME ECUADOR CYPRUS BURKINA FASO #12;A NOBEL FOR JERUSALEM PROFESSOR

Anat, Maril,

362

Proceedings of the Conference on  

E-Print Network [OSTI]

Education 146 David Stricker, University of Minnesota #12;A GLIMPSE OF THE FUTURE Theodore Lewis Professor

363

Microsoft Word - cimini-d.doc  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Microwave Radiative Models Study Microwave Radiative Models Study Based on Ground-Based Multichannel Radiometer Observations in the 20-60 GHz Band C. Cimini, F. S. Marzano, and P. Ciotti Center of Excellence CETEMPS Universita' dell'Aquila L'Aquila, Italy D. Cimini Science and Technology Corporation Hampton, Virginia E. R. Westwater Cooperative Institute for Research in Environmental Sciences University of Colorado National Oceanic and Atmospheric Administration Environmental Technology Laboratory Boulder, Colorado Y. Han National Oceanic and Atmospheric Administration National Environmental Satellite, Data, and Information Service Office of Research and Application Camp Springs, Maryland S. J. Keihm National Aeronautics and Space Administration Jet Propulsion Laboratory

364

NETL: Oil & Natural Gas Technologies Reference Shelf - Presentation on a  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

a Unified Imaging Procedure for 2-D Land Multichannel Seismic Data a Unified Imaging Procedure for 2-D Land Multichannel Seismic Data Towards a Unified Imaging Procedure for 2-D Land Multichannel Seismic Data Authors: Jaiswal, Priyank, Zelt, C.A., Rice University, and Dasgupta, R., Oil India Limited Venue: 70th EAGE Conference and Exhibition, Rome, Italy, June 11-14, 2008 (http://www.eage.org/events/index.php?eventid=57&Opendivs=s2 [external site). Abstract: This project demonstrates that imaging of 2-D multichannel seismic data can be effectively accomplished by a combination of travel-time inversion and pre-stack depth migration (PSDM); this combined method is referred to as unified imaging. Unified imaging begins with inversion of direct arrivals for estimating a velocity model that is used in static corrections and stacking velocity analysis. The interval velocity model (from stacking velocities) is used for PSDM. The stacked data and the PSDM image are interpreted for common horizons and the corresponding wide-aperture reflections are identified in the shot gathers. Using the interval velocity model the stack interpretations are inverted as zero-offset reflections for constraining the corresponding interfaces in depth; the interval velocity model is maintained stationary. A coefficient of congruence, j, is defined which measures the discrepancy between the horizons from the PSDM image and their counterparts from the zero-offset inversion. A value of unity for j implies that the interpreted and inverted horizons are consistent to within the interpretational uncertainties and the unified imaging is said to have converged at this point. For j greater than unity, the interval velocity model and the horizon depths are updated by jointly inverting the direct arrivals with the zero-offset and the wide-aperture reflections. The updated interval velocity model is used again for both PSDM and zero-offset inversion. Interpretations of the new PSDM image are the updated horizons depths. The unified imaging is applied to seismic data from the Naga Thrust and Fold Belt, India. Wide-aperture and zero-offset data from three geologically significant horizons are used. Three runs of joint inversion and PSDM are required in a cyclic manner for j to converge to unity. A joint interpretation of the final velocity model and the final depth image reveal the presence of a triangle zone that appears to be promising for exploration.

365

Eigenchannel treatment of R-matrix theory  

Science Journals Connector (OSTI)

We here present an alternatve way to perform R-matrix calculations in which the eigenchannel parameters of multichannel quantum defect theory are calculated directly. Merits of our R-matrix calculations are twofold: (1) an analytical treatment of perturbed discrete Rydberg states, autoionizing states, and their adjacent continuum to avoid numerical calculations outside the R-matrix box; (2) clear assignment of overlapped resonances, e.g., to analyze the lithium inner-shell photoionization cross section, which has been of considerable interest in recent experimental measurements.

Jia-Ming Li; Lan Vo Ky; Yi-Zhi Qu; Jun Yan; Pei-Hong Zhang; Hsiao-Ling Zhou; Paul Faucher

1997-04-01T23:59:59.000Z

366

Hardware and Software Developments for the Accurate Time-Linked Data Acquisition System  

SciTech Connect (OSTI)

Wind-energy researchers at Sandia National Laboratories have developed a new, light-weight, modular data acquisition system capable of acquiring long-term, continuous, multi-channel time-series data from operating wind-turbines. New hardware features have been added to this system to make it more flexible and permit programming via telemetry. User-friendly Windows-based software has been developed for programming the hardware and acquiring, storing, analyzing, and archiving the data. This paper briefly reviews the major components of the system, summarizes the recent hardware enhancements and operating experiences, and discusses the features and capabilities of the software programs that have been developed.

BERG,DALE E.; RUMSEY,MARK A.; ZAYAS,JOSE R.

1999-11-09T23:59:59.000Z

367

Magneto-transport properties of InAs nanowires laterally-grown by selective area molecular beam epitaxy on GaAs (110) masked substrates  

SciTech Connect (OSTI)

We prepared InAs nanowires (NWs) by lateral growth on GaAs (110) masked substrates in molecular beam epitaxy. We measured magneto-transport properties of the InAs NWs. In spite of parallel-NW multi-channels, we observed fluctuating magneto-conductance. From the fluctuation, we evaluated phase coherence length as a function of measurement temperature, and found decrease in the length with increase in the temperature. We also evaluate phase coherence length as a function of gate voltage.

Akabori, M.; Yamada, S. [Center for Nano-Materials and Technology, Japan Advanced Institute of Science and Technology, 1-1, Asahidai, Nomi, Ishikawa 923-1292 (Japan)

2013-12-04T23:59:59.000Z

368

Time-Distance Seismology of the Solar Corona with CoMP  

E-Print Network [OSTI]

We employ a sequence of Doppler images obtained with the Coronal Multi-channel Polarimeter (CoMP) instrument to perform time-distance seismology of the solar corona. We construct the first k-omega diagrams of the region. These allow us to separate outward and inward propagating waves and estimate the spatial variation of the plane-of-sky projected phase speed, and the relative amount of outward and inward directed wave power. The disparity between outward and inward wave power and the slope of the observed power law spectrum indicate that low-frequency Alfvenic motions suffer significant attenuation as they propagate, consistent with isotropic MHD turbulence.

Tomczyk, Steven

2009-01-01T23:59:59.000Z

369

Development of a process control sensor for the glass industry. Phase 2: Prototype design, development and demonstration  

SciTech Connect (OSTI)

This report describes an advanced multichannel, on-line optical system for the non-contact measurement of forehearth glass melt temperatures at depth. The analyzer employs multiple narrow infrared (IR) band measurements of glass radiation to reconstruct the glass temperature profiles at depth. The TAS replaces expensive Tri-plex thermocouples, which frequently have service lives as short as 6 months to 1 years. By using passive non-contact sensor heads and fiber optic cables, temperature sensitive electronic components can be located at a safe distance from the hostile process environment. This provides significantly better reliability of the vulnerable electro-optic components and ready access for maintenance.

Gardner, M.; Candee, A.; Koppang, R.

1994-06-01T23:59:59.000Z

370

Laser-Beam-Scattering Measurement of Ion Temperature in a ?-Pinch Plasma and Evidence for Thermonuclear Reactions  

Science Journals Connector (OSTI)

Results are reported on an experiment to measure the ion temperature in a 100-kJ ?-pinch deuterium plasma. A ruby laser was used for scattering observations at 5 and 90 using multichannel spectrum analyzers and gave n=1.051017 cm-3 and Ti=300 eV. An independent measurement of the density was made by means of Rayleigh scattering. The neutron yield from the plasma was measured to be 8108 sec-1. The observed neutron emission was compared with that expected from a plasma with an ion temperature of 300 eV and was found to be of thermonuclear origin.

P. K. John

1972-08-01T23:59:59.000Z

371

VUV studies of molecular photofragmentation dynamics  

SciTech Connect (OSTI)

State-resolved, photoion and photoelectron methods are used to study the neutral fragmentation and ionization dynamics of small molecules relevant to atmospheric and combustion chemistry. Photodissociation and ionization are initiated by coherent VUV radiation and the fragmentation dynamics are extracted from measurements of product rovibronic state distributions, kinetic energies and angular distributions. The general aim of these studies is to investigate the multichannel interactions between the electronic and nuclear motions which determine the evolution of the photoexcited {open_quotes}complex{close_quotes} into the observed asymptotic channels.

White, M.G. [Brookhaven National Laboratory, Upton, NY (United States)

1993-12-01T23:59:59.000Z

372

Cimel Sunphotometer (CSPHOT) Handbook  

SciTech Connect (OSTI)

The Cimel sunphotometer (CSPHOT) is a multi-channel, automatic sun-and-sky scanning radiometer that measures the direct solar irradiance and sky radiance at the Earths surface. Measurements are taken at pre-determined discrete wavelengths in the visible and near-IR parts of the spectrum to determine atmospheric transmission and scattering properties. This instrument is weather-proof and requires little maintenance during periods of adverse weather conditions. It takes measurements only during daylight hours (sun above horizon).

Gregory, L

2011-01-17T23:59:59.000Z

373

Integrative studies of thermoregulation in ectothermic vertebrates in aquatic habitats. Annual progress report, 1 October 1980-30 September 1981  

SciTech Connect (OSTI)

Field experiments are underway to determine the behavioral mechanisms by which largemouth bass, Micropterus salmoides, respond to rapid temperature changes in their natural environment. Laboratory experiments are clarifying the relationship between basking behavior of the turtle, Pseudemys scripta and its nutritional state. Important progress has been made in the development and miniaturization of a multichannel, temperature sensing, radio transmitter for fish. Theoretical analysis and mathematical modeling have defined the realized and fundamental climate space of P. scripta and allows the prediction of the behavior of this turtle.

Spotila, J R

1981-05-01T23:59:59.000Z

374

Long distance transmission of 15 Gb/s digital using subcarrier multiplexing and external modulation  

SciTech Connect (OSTI)

This paper provides an overview of a high-speed link design using subcarrier multiplexing techniques with external modulators. Although we have few experimental results to data, we feel the techniques and technology described in this paper will enable the simultaneous transmission of multi-channel analog video and up to 15 Gb/s of digital data on a single wavelength. Furthermore, we show preliminary modeling that would indicate that at least four channels of 2.5 Gb/s can be sent over distances exceeding 500 km using a new dispersion technique that takes advantage of subcarrier multiplexing.

Hugenberg, K.; Lowry, M.; Beckedahl, D. [Lawrence Livermore National Lab., CA (United States); Blair, J. [EG and G Idaho, Inc., Idaho Falls, ID (United States)

1994-03-01T23:59:59.000Z

375

Method of pedestal and common-mode noise correction for switched-capacitor analog memories  

DOE Patents [OSTI]

A method and apparatus are disclosed for correcting common-mode noise and pedestal noise in a multichannel array of switched-capacitor analog memories wherein each analog memory is connected to an associated analog-to-digital converter. The apparatus comprises a single differential element in two different embodiments. In a first embodiment, the differential element is a reference analog memory connected to a buffer. In the second embodiment, the differential element is a reference analog memory connected to a reference analog-to-digital connected to an array of digital summing circuits. 4 figs.

Britton, C.L.

1996-12-31T23:59:59.000Z

376

p-wave optical Feshbach resonances in {sup 171}Yb  

SciTech Connect (OSTI)

We study the use of an optical Feshbach resonance to modify the p-wave interaction between ultracold polarized {sup 171}Yb spin-1/2 fermions. A laser exciting two colliding atoms to the {sup 1}S{sub 0}+{sup 3}P{sub 1} channel can be detuned near a purely-long-range excited molecular bound state. Such an exotic molecule has an inner turning point far from the chemical binding region, and thus, three-body recombination in the Feshbach resonance will be highly suppressed in contrast to that typically seen in a ground-state p-wave magnetic Feshbach resonance. We calculate the excited molecular bound-state spectrum using a multichannel integration of the Schroedinger equation, including an external perturbation by a magnetic field. From the multichannel wave functions, we calculate the Feshbach resonance properties, including the modification of the elastic p-wave scattering volume and inelastic spontaneous scattering rate. The use of magnetic fields and selection rules for polarized light yields a highly controllable system. We apply this control to propose a toy model for three-color superfluidity in an optical lattice for spin-polarized {sup 171}Yb, where the three colors correspond to the three spatial orbitals of the first excited p band. We calculate the conditions under which tunneling and on-site interactions are comparable, at which point quantum critical behavior is possible.

Goyal, Krittika; Deutsch, Ivan [Center for Quantum Information and Control, University of New Mexico, Albuquerque, New Mexico 87131 (United States); Department of Physics and Astronomy, University of New Mexico, Albuquerque, New Mexico 87131 (United States); Reichenbach, Iris [Max Planck Institute for the Physics of Complex Systems, Noethnitzer Strasse 38, D-01187 Dresden (Germany)

2010-12-15T23:59:59.000Z

377

Combustion kinetics and reaction pathways  

SciTech Connect (OSTI)

This project is focused on the fundamental chemistry of combustion. The overall objectives are to determine rate constants for elementary reactions and to elucidate the pathways of multichannel reactions. A multitechnique approach that features three independent experiments provides unique capabilities in performing reliable kinetic measurements over an exceptionally wide range in temperature, 300 to 2500 K. Recent kinetic work has focused on experimental studies and theoretical calculations of the methane dissociation system (CH{sub 4} + Ar {yields} CH{sub 3} + H + Ar and H + CH{sub 4} {yields} CH{sub 3} + H{sub 2}). Additionally, a discharge flow-photoionization mass spectrometer (DF-PIMS) experiment is used to determine branching fractions for multichannel reactions and to measure ionization thresholds of free radicals. Thus, these photoionization experiments generate data that are relevant to both reaction pathways studies (reaction dynamics) and fundamental thermochemical research. Two distinct advantages of performing PIMS with high intensity, tunable vacuum ultraviolet light at the National Synchrotron Light Source are high detection sensitivity and exceptional selectivity in monitoring radical species.

Klemm, R.B.; Sutherland, J.W. [Brookhaven National Laboratory, Upton, NY (United States)

1993-12-01T23:59:59.000Z

378

Electronic spin-flipping collisions of hydrogen atoms  

SciTech Connect (OSTI)

We present a unified multichannel approach to calculate electron spin-exchange and spin-flipping transition cross sections for collisions of H with H, H with T, and T with T. We use the theory to calculate the hyperfine quenching cross sections for collision energies that range from 1 mK to thermal temperatures. We show that spin-flipping transitions are induced by the splitting of the b {sup 3{Sigma}}{sub u} Born-Oppenheimer potential via the long-range magnetic interactions among electrons. We find that the spin-flipping cross sections in the tritium dimer are about a magnitude larger than that predicted by mass scaling the H-H cross sections. For the former, we show that the spin-exchange cross sections are several magnitudes larger, at cold temperatures, than that of the hydrogen system. We compare the results of the multichannel approach with those obtained using approximate methods such as the degenerate internal-state, the elastic, and Born approximations and discuss their respective range of validity.

Zygelman, B. [Department of Physics and Astronomy, University of Nevada, Las Vegas, Las Vegas, Nevada 89154 (United States)

2010-03-15T23:59:59.000Z

379

CSP patches: an ensemble of optimized spatial filters. An evaluation study  

Science Journals Connector (OSTI)

Laplacian filters are widely used in neuroscience. In the context of braincomputer interfacing, they might be preferred to data-driven approaches such as common spatial patterns (CSP) in a variety of scenarios such as, e.g., when no or few user data are available or a calibration session with a multi-channel recording is not possible, which is the case in various applications. In this paper we propose the use of an ensemble of local CSP patches (CSPP) which can be considered as a compromise between Laplacian filters and CSP. Our CSPP only needs a very small number of trials to be optimized and significantly outperforms Laplacian filters in all settings studied. Additionally, CSPP also outperforms multi-channel CSP and a regularized version of CSP even when only very few calibration data are available, acting as a CSP regularizer without the need of additional hyperparameters and at a very low cost: 25 min of data recording, i.e. ten times less than CSP.

Claudia Sannelli; Carmen Vidaurre; Klaus-Robert Mller; Benjamin Blankertz

2011-01-01T23:59:59.000Z

380

Neotectonics of the Panama region. II. Deformation of the southern Colobian Basin  

SciTech Connect (OSTI)

The southern Colombian Basin is currently undergoing deformation as a result of convergence between Panama and the Caribbean plate. The structural expression of this convergence north of Panama is the Panama Deformed Belt (PDB), a marginal wedge of highly deformed sediments. The authors interpretation of UTIG multichannel data suggest that deformation of the PDB initiated during the Miocene and that the deformation front is migrating northward with respect to the Caribbean plate. Earthquake activity along the PDB is concentrated toward the east where the Mono Rise is underthrusting the PDB. The hypo-central distribution of these events indicate the presence of a seismic zone which has shallow dip to the southwest. Multichannel data also indicate that the style of deformation within the PDB changes from east to west. The authors propose that the observed variations in seismicity and deformation of the PDB are dependent on two factors: 1. The difference in Panama-Caribbean plate convergence along the PDB and 2. The fluctuation in oceanic crustal thickness of the Colombian Basin.

Adamek, S.H.

1985-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

E-Print Network 3.0 - ao benomyl por Sample Search Results  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

FINEP e IBM BRASIL, por seu apoio ao... , especialmente ao Romildo, 12;a K atia e ao Luiz Velho. 12;A toda minha fam lia, por seus ininterruptos apoios... e ... Source:...

382

E-Print Network 3.0 - ao entalhe por Sample Search Results  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

FINEP e IBM BRASIL, por seu apoio ao... , especialmente ao Romildo, 12;a K atia e ao Luiz Velho. 12;A toda minha fam lia, por seus ininterruptos apoios... e ... Source:...

383

E-Print Network 3.0 - ao parasitismo por Sample Search Results  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

FINEP e IBM BRASIL, por seu apoio ao... , especialmente ao Romildo, 12;a K atia e ao Luiz Velho. 12;A toda minha fam lia, por seus ininterruptos apoios... e ... Source:...

384

E-Print Network 3.0 - ao glifosato por Sample Search Results  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

FINEP e IBM BRASIL, por seu apoio ao... , especialmente ao Romildo, 12;a K atia e ao Luiz Velho. 12;A toda minha fam lia, por seus ininterruptos apoios... e ... Source:...

385

DOI: 10.1126/science.1150646 , 64 (2008);319Science  

E-Print Network [OSTI]

(2006). 11. E. Bauer, A. Ganopolski, Paleoceanography 19, PA3014 (2004). 12. A. P. Wiersma, H. Renssen

Wang, Yan Mei

386

Towards automatic cell identi cation in DIC microscopy , C.A. Glasbey2y  

E-Print Network [OSTI]

1998. Journal of Microscopy, 192, 186-193. #12;a b c Figure 1: DIC microscope images: a Chlorella algal

Stone, J. V.

387

Academic Resources The Florida State University  

E-Print Network [OSTI]

Westcott Building Tallahassee, Florida 32306-1410 http://www.gradschool.fsu.edu #12;A MESSAGE FROM THE DEAN

388

Modeling Electric Vehicle Benefits Connected to Smart Grids  

E-Print Network [OSTI]

Vehicle Benefits Connected to Smart Grids M. Stadler 1,2,a ,Electric Vehicle Benefits Connected to Smart Grids Michael

Stadler, Michael

2012-01-01T23:59:59.000Z

389

D E S I G N A N D F E A S I B I L I T Y O F P E E R -TO -P E E R M O B I L E  

E-Print Network [OSTI]

. #12;A B S T R A C T Digital payment methods are becoming increasingly popular. The advent of Bitcoin

Vellekoop, Michel

390

technology  

National Nuclear Security Administration (NNSA)

1%2A en ICF Reports http:nnsa.energy.govaboutusourprogramsdefenseprogramsstockpilestewardshipinertialconfinementfusionicfreports

391

warhead protection  

National Nuclear Security Administration (NNSA)

1%2A en Office of Nuclear Warhead Protection http:nnsa.energy.govaboutusourprogramsnonproliferationprogramofficesinternationalmaterialprotectionandcooperation-0

392

A Timing Requirements-Aware Scratchpad Memory Allocation Scheme for a Precision Timed Architecture  

E-Print Network [OSTI]

, and the following companies: Agilent, Bosch, HSBC, Lockheed-Martin, National Instruments, and Toyota. #12;A Timing

393

Unfolding and Finite Pre x for Nets with Read Arcs Walter Vogler  

E-Print Network [OSTI]

`Halbordnungstesten'). y Partially supported by EPSRC (projects HADES and TIMBRE, GR/K70175/L28098) 1 #12;(a) (b

Newcastle upon Tyne, University of

394

Molecular Foundry  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

See the Foundry's full equipment list See the Foundry's full equipment list Nanofabrication Capabilities & Tools Major Capabilities: Instruments and Labs Zeiss Crossbeam 1540 EsB The Molecular Foundry Zeiss Cross-beam is one of the most versatile lithographic and inspection tools allowing fabrication of complex prototypes for nanoelectronics, nano-optical antenna, modifying scanning probe tips, rapid electrical contacting and many other applications. The 1500XB Cross Beam combines the Gemini field emission column (FESEM) with the Orsay Physics focused ion beam (FIB). In addition, the instrument offers a multi-channel gas injection system to allow ion and electron beam induced deposition (IBID and EBID) and chemically assisted ion beam etching (CAIBE). The tool can be used for lithographic patterning of materials or

395

Internal Structure Of Puna Ridge- Evolution Of The Submarine East Rift Zone  

Open Energy Info (EERE)

Internal Structure Of Puna Ridge- Evolution Of The Submarine East Rift Zone Internal Structure Of Puna Ridge- Evolution Of The Submarine East Rift Zone Of Kilauea Volcano, Hawaii Jump to: navigation, search GEOTHERMAL ENERGYGeothermal Home Journal Article: Internal Structure Of Puna Ridge- Evolution Of The Submarine East Rift Zone Of Kilauea Volcano, Hawaii Details Activities (3) Areas (1) Regions (0) Abstract: Multichannel seismic reflection, sonobuoy, gravity and magnetics data collected over the submarine length of the 75 km long Puna Ridge, Hawaii, resolve the internal structure of the active rift zone. Laterally continuous reflections are imaged deep beneath the axis of the East Rift Zone (ERZ) of Kilauea Volcano. We interpret these reflections as a layer of abyssal sediments lying beneath the volcanic edifice of Kilauea. Early

396

ARM - Facility News Article  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Sunphotometer Re-installed at North Slope of Alaska Sunphotometer Re-installed at North Slope of Alaska Bookmark and Share The CIMEL sunphotometer takes sky radiance measurements during daylight hours, when the sun is above horizon. The CIMEL sunphotometer takes sky radiance measurements during daylight hours, when the sun is above horizon. In early May, a CIMEL sunphotometer owned by the National Aeronautics and Space Administration (NASA) was re-installed at Barrow, Alaska, one of two research sites that make up the ARM Climate Research Facility's North Slope of Alaska (NSA) locale. The CIMEL is a multi-channel, automatic sun-and-sky scanning radiometer that takes daytime measurements of direct solar radiance and sky radiance at the Earth's surface. Measurements are taken at discrete wavelengths in visible and near-infrared regions of the solar

397

EQ-SANS: the Extended Q-Range Small-Angle Neutron Scattering Diffractometer  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

The Extended Q-Range Small-Angle Neutron Scattering Diffractometer at SNS The Extended Q-Range Small-Angle Neutron Scattering Diffractometer at SNS Extended Q-Range Small Angle Diffractometer EQ-SANS detector array The EQ-SANS Diffractometer is designed to study non-crystalline, nano-sized materials in solid, liquid, or gas forms such as polymers, micelles, proteins, and other large biological molecular complexes in solution. It offers high neutron flux, high wavelength resolution (precision), and wide Q-coverage. EQSANS is located on beam line 6, viewing the top-downstream, coupled supercritical hydrogen moderator. It has a curved multichannel beam bender to avoid the direct line of sight of the moderator, which cleans out the background from the prompt neutron pulse quite effectively. The cutoff wavelength of the optics is ~1.5 Å. Above this minimum wavelength, the

398

Section 37  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

' ' T(J,csza) T " ' T%"a sph T/(1&"a sph ) Session Papers 161 (1) (2) Cloud Optical Properties Obtained from the Multi-Filter Rotating Shadowband Radiometer Instrument: Methodology and Analysis of Data Obtained in Fairbanks, Alaska E. Leontieva and K. Stamnes Geophysical Institute University of Alaska Fairbanks, Alaska Introduction A retrieval technique is presented to infer the cloud optical depth from data obtained by a ground-based, multi-channel radiometer operating in the solar and near-infrared (IR) range. An approach is introduced that uses observed and model-simulated transmittances rather than irradiances. Cloud optical depth retrievals are most meaningful under com- pletely overcast cloud conditions. The observed atmospheric transmittances under fractional cloud cover are of interest by

399

Deep Trek Re-configurable Processor for Data Acquisition (RPDA)  

SciTech Connect (OSTI)

This report summarizes technical progress achieved during the cooperative research agreement between Honeywell and U.S. Department of Energy to develop a high-temperature Re-configurable Processor for Data Acquisition (RPDA). The RPDA development has incorporated multiple high-temperature (225C) electronic components within a compact co-fired ceramic Multi-Chip-Module (MCM) package. This assembly is suitable for use in down-hole oil and gas applications. The RPDA module is programmable to support a wide range of functionality. Specifically this project has demonstrated functional integrity of the RPDA package and internal components, as well as functional integrity of the RPDA configured to operate as a Multi-Channel Data Acquisition Controller. This report reviews the design considerations, electrical hardware design, MCM package design, considerations for manufacturing assembly, test and screening, and results from prototype assembly and characterization testing.

Bruce Ohme; Michael Johnson

2009-06-30T23:59:59.000Z

400

Shape resonances in low-energy-electron collisions with halopyrimidines  

SciTech Connect (OSTI)

We report calculated cross sections for elastic collisions of low-energy electrons with halopyrimidines, namely, 2-chloro, 2-bromo, and 5-bromopyrimidine. We employed the Schwinger multichannel method with pseudopotentials to compute the cross sections in the static-exchange and static-exchange plus polarization levels of approximation for energies up to 10 eV. We found four shape resonances for each molecule: three of ?* nature localized on the ring and one of ?* nature localized along the carbonhalogen bond. We compared the calculated positions of the resonances with the electron transmission spectroscopy data measured by Modelli et al. [J. Phys. Chem. A 115, 10775 (2011)]. In general the agreement between theory and experiment is good. In particular, our results show the existence of a ?* temporary anion state of A{sub 2} symmetry for all three halopyrimidines, in agreement with the dissociative electron attachment spectra also reported by Modelli et al. [J. Phys. Chem. A 115, 10775 (2011)].

Barbosa, Alessandra Souza; Bettega, Mrcio H. F., E-mail: bettega@fisica.ufpr.br [Departamento de Fsica, Universidade Federal do Paran, Caixa Postal 19044, 81531-990 Curitiba, Paran (Brazil)] [Departamento de Fsica, Universidade Federal do Paran, Caixa Postal 19044, 81531-990 Curitiba, Paran (Brazil)

2013-12-07T23:59:59.000Z

Note: This page contains sample records for the topic "12a dpwa multichannel" from the National Library of EnergyBeta (NLEBeta).
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401

Communicating potential risks of uncontrolled site development at a Fusrap site  

SciTech Connect (OSTI)

This paper describes a particular risk communication challenge at the FUSRAP Maywood Superfund Site (the Site) in Maywood, New Jersey, USA. That challenge is communicating the potential human exposure risks of uncontrolled site development to landowners, tenants, private contractors and public works entities that may engage in construction activities at or adjacent to Site properties. This is of special concern because the Site does not have the authority to establish physical control over most of the properties where contamination is known or suspected to exist. Consequently, a range of communications techniques have been employed to alert property owners and others to the risks of uncontrolled site development. Each technique has its particular limitations, but collectively this multi-channel communication strategy has proved successful in delivering the risk message. (authors)

Roos, A.D. [U.S. Army Corps of Engineers, New York District, New York, NY (United States); Kollar, W. [Shaw Environmental, Inc., Maywood, NJ (United States)

2008-07-01T23:59:59.000Z

402

Final Technical Report on DOE Junior Faculty Development Award  

SciTech Connect (OSTI)

Over the course of this project we developed and contstructed the Colorado FRC facility, which included a custom vacuum vessel, high voltage and firing circuitry, two plasma gun electrodes, and pumping system, and several diagnostics. Density measurements were made with a multichannel CO{sub 2} (10.6 ?m) laser interferometer. We also developed and a high-resolution magnetic probe array for 3-axis measurements of magnetic fluctuations. We constructed and implemented a triple Langmuir probe for making time-resolved measurements of plasma density, potential, and temperature. By calculating the time history of the gun eigenvalue, we observed indications that the Taylor formation paradigm applies. To estimate the spectral characteristics of fluctuations in an FRC, we developed a technique to extract the relevant spectral information using data from the high-resolution multi-point magnetic probe.

Munsat, Tobin

2014-08-21T23:59:59.000Z

403

Faraday-effect polarimeter-interferometer system for current density measurement on EAST  

SciTech Connect (OSTI)

A multichannel far-infrared laser-based POlarimeter-INTerferometer (POINT) system utilizing the three-wave technique is under development for current density and electron density profile measurements in the EAST tokamak. Novel molybdenum retro-reflectors are mounted in the inside wall for the double-pass optical arrangement. A Digital Phase Detector with 250 kHz bandwidth, which will provide real-time Faraday rotation angle and density phase shift output, have been developed for use on the POINT system. Initial calibration indicates the electron line-integrated density resolution is less than 5 10{sup 16} m{sup ?2} (?2), and the Faraday rotation angle rms phase noise is <0.1.

Liu, H. Q.; Jie, Y. X., E-mail: yx-jie@ipp.ac.cn; Zou, Z. Y.; Li, W. M.; Wang, Z. X.; Qian, J. P.; Yang, Y.; Zeng, L.; Wei, X. C.; Hu, L. Q.; Wan, B. N. [Institute of Plasma Physics, Chinese Academy of Sciences, Hefei, Anhui 230031 (China); Ding, W. X.; Brower, D. L. [Department of Physics and Astronomy, University of California Los Angeles, Los Angeles, California 90095 (United States); Lan, T.; Li, G. S. [Institute of Plasma Physics, Chinese Academy of Sciences, Hefei, Anhui 230031 (China); University of Science and Technology of China, Hefei, Anhui 230026 (China)

2014-11-15T23:59:59.000Z

404

Polarization effects in autoionization processes: The 5d5g states in barium  

Science Journals Connector (OSTI)

Accurate measurements of the autoionization widths of 5d5g levels of barium coupled to theoretical calculations, based on the eigenchannel R-matrix method and the multichannel quantum-defect theory, permit an investigation of the quadrupolar autoionization mechanism. The direct polarization of the inner electron by the outer one is an important correction to the Coulomb repulsion that causes autoionization. Also, the dielectronic polarization interaction significantly influences the autoionization widths. The occurrence of these polarization effects in the 5d5g doubly excited states with nonoverlapping valence electrons results in a significant narrowing of their widths and explains the failure of the single-configuration model for high-l Rydberg levels.

E. Luc-Koenig; M. Aymar; R. Van Leeuwen; W. Ubachs; W. Hogervorst

1995-07-01T23:59:59.000Z

405

Observing, modeling and predicting the effects of solar radio bursts on radio communications  

Science Journals Connector (OSTI)

The Sun is a source of broadband radio noise which can reach significantly high levels during outbursts associated with the time evolution of the activity cycle. The statistics point out that the maximum occurrence frequency and intensity of solar radio bursts (SRBs) are observed in the proximity of the activity maximum but relevant phenomena can occur also in the raising and declining phases of the cycle. Both theoretical estimations based on extensive statistical analyses carried out in recent years and direct observations performed in the past solar activity cycle indicate that solar radio bursts can interfere wireless communications as well as Global Navigation Satellite Systems (GNSS). In this work we briefly review the theoretical basis and the experimental evidences to date and we show the effectiveness of fast multichannel solar radiopolarimeters like the Trieste Solar Radio System in monitoring and predicting solar radio noise increase in the framework of Space Weather applications.

Mauro Messerotti

2008-01-01T23:59:59.000Z

406

Competing decay-channel fluorescence, dissociation, and ionization in superexcited levels of H{sub 2}  

SciTech Connect (OSTI)

The absolute cross sections for the competing decay-channel fluorescence, dissociation, and ionization of photoexcited long-lived superexcited H{sub 2} molecular levels have been measured from the ionization threshold of H{sub 2} up to the H(1s) + H(n=3) dissociation limit. The total and partial natural widths of these levels have been determined. Good agreement is found with first principles calculations carried out with the multichannel quantum defect theory for excited levels of {sup 1{Pi}}{sub u}{sup -} symmetry, which represent 70% of the levels studied experimentally. The calculations reproduce the balance between the competing decay processes as well as its substantial evolution from level to level.

Glass-Maujean, M. [Laboratoire de Physique Moleculaire pour l'Atmosphere et l'Astrophysique, Universite Pierre et Marie Curie, 4 place Jussieu, F-75252 Paris Cedex 5 (France); Jungen, Ch. [Laboratoire Aime Cotton, Centre National de la Recherche Scientifique, Batiment 505, Universite de Paris-Sud, F-91405 Orsay (France); Department of Physics and Astronomy, University College London, London WC1E 6BT (United Kingdom); Reichardt, G.; Balzer, A. [BESSY II, Albert-Einstein-Strasse 15, D-12489 Berlin (Germany); Schmoranzer, H. [Fachbereich Physik, Technische Universitaet Kaiserslautern, D-67653 Kaiserslautern (Germany); Ehresmann, A.; Haar, I.; Reiss, P. [Institute of Physics and Interdisciplinary Nanostructure Science and Technology, Heinrich-Plett-Strasse 40, Universitaet Kassel, D-34132 Kassel (Germany)

2010-12-15T23:59:59.000Z

407

Evaluation of the Antioxidant Capacity of Limonin, Nomilin, and Limonin Glucoside  

Science Journals Connector (OSTI)

The antioxidant capacity (AOC) of three representative citrus limonoids, limonin, nomilin, and limonin glucoside, was examined by the oxygen radical absorbance capacity (ORAC), Trolox equivalent antioxidant capacity (TEAC), ?-carotene?linoleic acid bleaching, and 1,1-diphenyl-2-picryl hydrazyl (DPPH) radical scavenging assays. ... Briefly, in a glass 96-well reaction plate, samples, along with positive (BHT, ascorbic acid) and negative (cinnamic acid) controls (50 ?L) prepared in methanol (0.001?1 mg/mL), were combined in triplicate with 155 ?M methanolic DPPH (200 ?L). ... After incubation (37 C, 15 min), AAPH (60 ?L, 37 C) was added rapidly using a multichannel pipet, and the microplate was immediately placed in a Molecular Devices Gemini-EM (Sunnyvale, CA) fluorescence plate reader. ...

Andrew P. Breksa; III; Gary D. Manners

2006-05-03T23:59:59.000Z

408

Systems and Methods for Integrated Emissivity and Temperature Measurement of a Surface  

DOE Patents [OSTI]

A multi-channel spectrometer and a light source are used to measure both the emitted and the reflected light from a surface which is at an elevated temperature relative to its environment. In a first method, the temperature of the surface and emissivity in each wavelength is calculated from a knowledge of the spectrum and the measurement of the incident and reflected light. In the second method, the reflected light is measured from a reference surface having a known reflectivity and the same geometry as the surface of interest and the emitted and the reflected light are measured for the surface of interest. These measurements permit the computation of the emissivity in each channel of the spectrometer and the temperature of the surface of interest.

Poulsen, Peter

2005-11-08T23:59:59.000Z

409

Significance of decay mechanism into continuum in dynamical Wannier-Stark ladder  

SciTech Connect (OSTI)

We examine the resonance structure of photodressed electron states of laser-driven Wannier-Stark ladder, namely, dynamic Wannier-Stark ladder, in terms of the excess density of states (DOS) closely related to a lifetime of the state of concern. It is revealed that the resonance structure in the strong laser-field region shows clear dependence on the ratio, ?, of a Bloch-frequency to a laser frequency. As the laser strength increases, for ? = 1, the excess DOS becomes involved with a lot of newly-growing resonance peaks. This result would be understood from the viewpoint of a Fano-like decay-mechanism caused by a multichannel continuum effect, in marked contrast to the cases of larger ?s; for ? = 3, the excess DOS just is found to show a pronounced red-shift of a single dominant peak caused by a single-channel continuum effect.

Nemoto, Yuya [Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, 305-8573 (Japan); Maeshima, Nobuya; Hino, Ken-ichi [Faculty of Pure and Applied Sciences, University of Tsukuba, Tsukuba 305-8573, Japan and Center for computational Sciences, University of Tsukuba, Tsukuba 305-8577 (Japan)

2013-12-04T23:59:59.000Z

410

Real-time MSE measurements for current profile control on KSTAR  

SciTech Connect (OSTI)

To step up from current day fusion experiments to power producing fusion reactors, it is necessary to control long pulse, burning plasmas. Stability and confinement properties of tokamak fusion reactors are determined by the current or q profile. In order to control the q profile, it is necessary to measure it in real-time. A real-time motional Stark effect diagnostic is being developed at Korean Superconducting Tokamak for Advanced Research for this purpose. This paper focuses on 3 topics important for real-time measurements: minimize the use of ad hoc parameters, minimize external influences and a robust and fast analysis algorithm. Specifically, we have looked into extracting the retardance of the photo-elastic modulators from the signal itself, minimizing the influence of overlapping beam spectra by optimizing the optical filter design and a multi-channel, multiharmonic phase locking algorithm.

De Bock, M. F. M.; Aussems, D.; Huijgen, R.; Scheffer, M. [Eindhoven University of Technology, Eindhoven (Netherlands); Chung, J. [National Fusion Research Institute, Daejeon (Korea, Republic of)

2012-10-15T23:59:59.000Z

411

Verification of the Astrometric Performance of the Korean VLBI Network, using comparative SFPR studies with the VLBA at 14/7 mm  

E-Print Network [OSTI]

The Korean VLBI Network (KVN) is a new mm-VLBI dedicated array with capability for simultaneous observations at multiple frequencies, up to 129 GHz. The innovative multi-channel receivers present significant benefits for astrometric measurements in the frequency domain. The aim of this work is to verify the astrometric performance of the KVN using a comparative study with the VLBA, a well established instrument. For that purpose, we carried out nearly contemporaneous observations with the KVN and the VLBA, at 14/7 mm, in April 2013. The KVN observations consisted of simultaneous dual frequency observations, while the VLBA used fast frequency switching observations. We used the Source Frequency Phase Referencing technique for the observational and analysis strategy. We find that having simultaneous observations results in a superior performance for compensation of all atmospheric terms in the observables, in addition to offering other significant benefits for astrometric analysis. We have compared the KVN astr...

Rioja, Mar\\'\\ia J; Jung, TaeHyun; Sohn, Bong Won; Byun, Do-Young; Agudo, Ivn; Cho, Se-Hyung; Lee, Sang-Sung; Kim, Jongsoo; Kim, Kee-Tae; Oh, Chung Sik; Han, Seog-Tae; Je, Do-Heung; Chung, Moon-Hee; Wi, Seog-Oh; Kang, Jiman; Lee, Jung-Won; Chung, Hyunsoo; Kim, Hyo Ryoung; Kim, Hyun-Goo; Lee, Chang-Hoon; Roh, Duk-Gyoo; Oh, Se-Jin; Yeom, Jae-Hwan; Song, Min-Gyu; Kang, Yong-Woo

2014-01-01T23:59:59.000Z

412

Measurement of quasi-isentropic compressibility of helium and deuterium at pressures of 1500-2000 GPa  

SciTech Connect (OSTI)

The quasi-isentropic compressibility of helium and deuterium plasmas at pressures of up to 1500-2000 GPa has been measured using devices with spherical geometry and an X-ray diagnostic complex comprising three betatrons and a multichannel imaging system with electro-optic gamma detectors. A deuterium density of 4.5 g/cm{sup 3} and a helium density of 3.8 g/cm{sup 3} have been obtained at pressures of 2210 and 1580 GPa, respectively. The internal energy of a deuterium plasma at the indicated pressure is about 1 MJ/cm{sup 3}, which is about 100 times greater than the specific energy of condensed chemical explosives. Analysis of the obtained data shows that the degree of helium ionization under the achieved plasma compression parameters is about 0.9.

Mochalov, M. A., E-mail: postmaster@ifv.vniief.ru; Il'kaev, R. I. [Russian Federal Nuclear Center, All-Russia Institute of Experimental Physics (Russian Federation); Fortov, V. E. [Russian Academy of Sciences, Joint Institute for High Temperatures (Russian Federation); Mikhailov, A. L.; Makarov, Yu. M.; Arinin, V. A.; Blikov, A. O.; Baurin, A. Yu.; Komrakov, V. A.; Ogorodnikov, V. A.; Ryzhkov, A. V.; Pronin, E. A.; Yukhimchuk, A. A. [Russian Federal Nuclear Center, All-Russia Institute of Experimental Physics (Russian Federation)

2012-10-15T23:59:59.000Z

413

Subbarrier fusion reactions and many-particle quantum tunneling  

E-Print Network [OSTI]

Low energy heavy-ion fusion reactions are governed by quantum tunneling through the Coulomb barrier formed by a strong cancellation of the repulsive Coulomb force with the attractive nuclear interaction between the colliding nuclei. Extensive experimental as well as theoretical studies have revealed that fusion reactions are strongly influenced by couplings of the relative motion of the colliding nuclei to several nuclear intrinsic motions. Heavy-ion subbarrier fusion reactions thus provide a good opportunity to address a general problem on quantum tunneling in the presence of couplings, which has been a popular subject in the past decades in many branches of physics and chemistry. Here we review theoretical aspects of heavy-ion subbarrier fusion reactions from the view point of quantum tunneling in systems with many degrees of freedom. Particular emphases are put on the coupled-channels approach to fusion reactions, and the barrier distribution representation for multi-channel penetrability. We also discuss ...

Hagino, K

2012-01-01T23:59:59.000Z

414

Operation and upgrade of diagnostic neutral beam injector RUDI at TEXTOR tokamak  

SciTech Connect (OSTI)

The status and the executing modernization of RUssian Diagnostic Injector (RUDI) are described. The ion source consists of arc plasma emitter and multiaperture four-electrode ion optical system. The present ion optical system with round beamlets is to be replaced by new slit apertures system for the reducing beam angular divergence in one direction. Due to enlarged dimensions and transparency of new ion optical system the extracted ion beam current will be by 50% increased. For the extension of beam pulse duration from 4 s to 8-10 s an optimized metal-ceramic arc-discharge channel is introduced. In the paper, the optical measurements results of beam parameters, including the profile of species distribution, scanned by custom-built multichannel spectroscope, are also presented.

Listopad, A. A. [Trilateral Euregio Cluster, Institut fuer Energieforschung-Plasmaphysik, Forschungszentrum Juelich GmbH, Association EURATOM-FZJ, 52425 Juelich (Germany); Budker Institute of Nuclear Physics, 630090 Novosibirsk (Russian Federation); Coenen, J. W.; Schalt, W.; Schweer, B.; Uhlemann, R. [Trilateral Euregio Cluster, Institut fuer Energieforschung-Plasmaphysik, Forschungszentrum Juelich GmbH, Association EURATOM-FZJ, 52425 Juelich (Germany); Davydenko, V. I.; Deichuli, P. P.; Ivanov, A. A.; Mishagin, V. V.; Savkin, V. Ya.; Shulzhenko, G. I.; Stupishin, N. V. [Budker Institute of Nuclear Physics, 630090 Novosibirsk (Russian Federation)

2010-02-15T23:59:59.000Z

415

Response Time Measurements of the NIF DANTE XRD-31 X-Ray Diodes (Pre-print)  

SciTech Connect (OSTI)

The XRD-31 is a fast, windowless X-ray vacuum photodiode developed by EG&G. It is currently the primary fast X-ray detector used to diagnose the X-rays on NIF and OMEGA on the multichannel DANTE spectrometer. The XRD-31 has a dynamic range of less than 1e-12 amps to more than 10 amps. A technique is described to measure the impulse response of the diodes to a 150 fs pulse of 200 nm laser light and a method to calculate the risetime for a square pulse and compare it with the computed electron transit time from the photocathode to the anode. Measured response time for 5 XRD-31s assembled in early 2004 was 149.7 ps +-2.75 ps.

Don Pellinen and Michael Griffin

2009-01-23T23:59:59.000Z

416

Retrofit SCADA installation combines SCADA and process control functions  

SciTech Connect (OSTI)

When Gulf States Utilities Company`s (now part of Entergy Operations, Inc.) River Bend Nuclear Plant, decided to add a closed cooling water system for the plant service water, a new SCADA system was required. Previously the normal service water system shared common cooling towers and flume with the plant`s circulating water system. Closing the system required a new cooling tower with pumps and heat exchangers to be constructed in a remote location. Existing equipment in the area was controlled via a multichannel tone SCADA system that did not have sufficient spare capacity for control of the new components. This paper will discuss how a new SCADA system was designed and installed, that also included process control. It will also address the operational experience to date.

Moffitt, T.O. [Entergy Operations, Inc., St. Francisville, LA (United States)

1995-09-01T23:59:59.000Z

417

Testing the plutonium isotopic analysis code FRAM with various CdTe detectors.  

SciTech Connect (OSTI)

The isotopic analysis code Fixed-energy Response-function Analysis with Multiple efficiency (FRAM)1,2 has been proven to successfully analyze plutonium spectra taken with a portable CdTe detector with Peltier cooling, the first results of this kind for a noncryogenic detector.3 These are the first wide-range plutonium gamma-ray isotopics analysis results obtained with other than Ge spectrometers. The CdTe spectrometer measured small plutonium reference samples in reasonable count times, covering the range from low to high burnup. This paper describes further testing of FRAM with two CdTe detectors of different sizes and resolutions using different analog and digital, portable multichannel analyzers (MCAs).

Vo, Duc T.; Russo, P. A. (Phyllis A.)

2002-01-01T23:59:59.000Z

418

Silicon detector for high rate EXAFS applications  

SciTech Connect (OSTI)

A multichannel silicon pad detector for EXAFS (Extended X-ray Absorption Fine Structure) applications has been designed and built. The X-ray spectroscopic measurements demonstrate that an adequate energy resolution of 230 eV FWHM (corresponding to 27 rms electrons in silicon) can be achieved reliably at {minus}35 C. A resolution of 190 eV FWHM (corresponding to 22 rms electrons) has been obtained from individual pads at {minus}35 C. At room temperature (25 C) an average energy resolution of 380 eV FWHM is achieved and a resolution of 350 eV FWHM (41 rms electrons) is the best performance. A simple cooling system constituted of Peltier cells is sufficient to reduce the reverse currents of the pads and their related shot noise contribution, in order to achieve resolutions better than 300 eV FWHM which is adequate for the EXAFS applications.

Kraner, H.W.; Siddons, D.P.; Furenlid, L.R. [Brookhaven National Lab., Upton, NY (United States); Bertuccio, G. [Politecnico di Milano (Italy). Dipt. di Elettronica e Informazione

1995-08-01T23:59:59.000Z

419

Polarization effects on low-energy electron collisions with propane  

Science Journals Connector (OSTI)

We employed the Schwinger multichannel method to compute elastic cross sections for low-energy electron collisions with propane (C3H8). The calculations are carried out within the static-exchange and static-exchange plus polarization approximations and covered the energy range from 0 to 15 eV. The computed differential cross sections show good agreement with the experiment, and the computed integral cross sections present the same shape as the measured total cross sections. We found a broad structure in the integral cross section around 8.5 eV and also a Ramsauer-Townsend minimum around 0.1 eV. These results are in agreement with the experimental observations.

Mrcio H. F. Bettega; Romarly F. da Costa; Marco A. P. Lima

2008-05-08T23:59:59.000Z

420

Radio-nuclide mixture identification using medium energy resolution detectors  

DOE Patents [OSTI]

According to one embodiment, a method for identifying radio-nuclides includes receiving spectral data, extracting a feature set from the spectral data comparable to a plurality of templates in a template library, and using a branch and bound method to determine a probable template match based on the feature set and templates in the template library. In another embodiment, a device for identifying unknown radio-nuclides includes a processor, a multi-channel analyzer, and a memory operatively coupled to the processor, the memory having computer readable code stored thereon. The computer readable code is configured, when executed by the processor, to receive spectral data, to extract a feature set from the spectral data comparable to a plurality of templates in a template library, and to use a branch and bound method to determine a probable template match based on the feature set and templates in the template library.

Nelson, Karl Einar

2013-09-17T23:59:59.000Z

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

An MS-DOS-based program for analyzing plutonium gamma-ray spectra  

SciTech Connect (OSTI)

A plutonium gamma-ray analysis system that operates on MS-DOS-based computers has been developed for the International Atomic Energy Agency (IAEA) to perform in-field analysis of plutonium gamma-ray spectra for plutonium isotopics. The program titled IAEAPU consists of three separate applications: a data-transfer application for transferring spectral data from a CICERO multichannel analyzer to a binary data file, a data-analysis application to analyze plutonium gamma-ray spectra, for plutonium isotopic ratios and weight percents of total plutonium, and a data-quality assurance application to check spectral data for proper data-acquisition setup and performance. Volume 3 contains the software listings for these applications.

Ruhter, W.D.; Buckley, W.M.

1989-09-07T23:59:59.000Z

422

Large rank Wilson loops in N=2 superconformal QCD at strong coupling  

E-Print Network [OSTI]

We compute the expectation values of circular Wilson loops in large representations at strong coupling, in the large-N limit of the N=2 superconformal theory with SU(N) gauge group and 2N hypermultiplets. Employing Pestun's matrix integral, we focus attention on symmetric and antisymmetric representations with ranks of order N. We find that large rank antisymmetric loops are independent of the coupling at strong 't Hooft coupling while symmetric Wilson loops grow exponentially with it. Symmetric loops display a non-analyticity as a function of the rank, characterized by the splitting of a single matrix model eigenvalue from the continuum, bearing close resemblance to Bose-Einstein condensation in an ideal gas. We discuss implications of these for a putative large-N string dual. The method of calculation we adopt makes explicit the connection to Fermi and Bose gas descriptions and also suggests a tantalizing connection of the above system to a multichannel Kondo model.

Benedict Fraser; S. Prem Kumar

2012-02-28T23:59:59.000Z

423

Crystal Structure and Spectroscopic Characterization of a Luminescent Europium Chelate  

Science Journals Connector (OSTI)

This ligation removes the last water bound to the primary coordination sphere of europium, resulting in no waters bound to the lanthanide. ... 6,11-13 Their utility arises because of the lanthanide's unusual spectroscopic emission characteristics, which include millisecond lifetime, spiked emission peaks (150 nm), potentially high quantum yields (?1), and excellent solubility. ... A pulsed nitrogen laser (337 nm, 5 ns pulse-width, 40 Hz repetition rate; Laser Photonics) excited the Eu-DTPA-cs124 sample, and emission was passed through a double-monochromator (SPEX 1680B, blaze = 500 nm, f/4) and detected by a gallium arsenide photomultiplier tube operating in photon-counting mode (Hamamatsu R943-02) with associated electronics (MITEQ 500 MHz preamplifier; Ortec 854 gated discriminator; Canberra FMS multichannel scalar with 2 ?s time resolution). ...

Paul R. Selvin; Jaru Jancarik; Min Li; Li-Wei Hung

1996-01-31T23:59:59.000Z

424

Integrated Emissivity And Temperature Measurement  

DOE Patents [OSTI]

A multi-channel spectrometer and a light source are used to measure both the emitted and the reflected light from a surface which is at an elevated temperature relative to its environment. In a first method, the temperature of the surface and emissivity in each wavelength is calculated from a knowledge of the spectrum and the measurement of the incident and reflected light. In the second method, the reflected light is measured from a reference surface having a known reflectivity and the same geometry as the surface of interest and the emitted and the reflected light are measured for the surface of interest. These measurements permit the computation of the emissivity in each channel of the spectrometer and the temperature of the surface of interest.

Poulsen, Peter (Livermore, CA)

2005-11-08T23:59:59.000Z

425

Phase analysis of vibrational wave packets in the ground and excited states in polydiacetylene  

Science Journals Connector (OSTI)

Molecular vibration of several modes in blue-phase polydiacetylene-3-butoxycarbonylmethylurethane (PDA-3BCMU) was real-time observed by 5-fs pump-probe measurement. The contribution of the vibrational wave packets in the ground state and in the excited state in the signal were separated by multichannel measurement. The C?C stretching mode in the ground state starts to oscillate ?-out-of-phase with the C?C stretching mode. The structure of PDA-3BCMU in the geometrically relaxed state is not pure butatriene type but more like acetylene type. The frequencies of C?C and C?C stretching modes there were determined by singular value decomposition method to be 14726cm?1 and 20926cm?1, respectively. The double and triple bond stretching frequencies in the ground state are 14636cm?1 and 20836cm?1, respectively.

Mitsuhiro Ikuta; Yoshiharu Yuasa; Tatsumi Kimura; Hiroo Matsuda; Takayoshi Kobayashi

2004-12-02T23:59:59.000Z

426

NETL: Methane Hydrates - DOE/NETL Projects - Structural and Stratigraphic  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Structural and Stratigraphic Controls on Methane Hydrate Occurrence and Distribution: Gulf of Mexico, Walker Ridge 313 and Green Canyon 955 Last Reviewed 12/24/2013 Structural and Stratigraphic Controls on Methane Hydrate Occurrence and Distribution: Gulf of Mexico, Walker Ridge 313 and Green Canyon 955 Last Reviewed 12/24/2013 DE-FE0009904 Goal The goal of this project is to determine structural and stratigraphic controls on hydrate occurrence and distribution in Green Canyon (GC) 955 and Walker Ridge (WR) 313 blocks with special emphasis on hydrate-bearing sand reservoirs. Structural and stratigraphic controls on hydrate distribution are examined by jointly analyzing surface-towed, multichannel seismic (MCS) and Ocean Bottom Seismometer (OBS) data and well logs through a combination of pre-stack depth migration (PSDM), traveltime and full-waveform inversion (FWI), and rock physics modeling methods. Performers Oklahoma State University, Stillwater, OK 74078-1026

427

ARM - Employment Opportunities Article  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Postdoctoral Position at University of Miami Postdoctoral Position at University of Miami Bookmark and Share The Rosenstiel School of Marine and Atmospheric Sciences (RSMAS), University of Miami invites applications for a postdoctoral position. We are seeking a highly motivated postdoctoral research associate who will team with scientists to conduct research to try to infer the sensitivities of atmospheric convection to ambient humidity, using field observations from the DYNAMO campaign (held in 2011-12 in the equatorial Indian Ocean). Key observations will be humidity data, including time-height profiles needed to retrieve or deduce from multi-channel passive microwave remote sensing, as well as data on convective cloud systems, such as Doppler radar-derived wind divergence profiles. Candidates should be familiar with

428

E-Print Network 3.0 - adiabatic shock capturing Sample Search...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Department of Applied Mathematics, University of Waterloo Collection: Plasma Physics and Fusion 12 A bow shock flow containing (almost) all types of (exotic') MHD discontinuities...

429

E-Print Network 3.0 - als-provoking enzyme sod1 Sample Search...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

It is also possible that such protective effect of blocking copper delivery to mutant enzymes... - oxide toxicity1,2. A variety of studies, including ... Source: Blackshaw, Seth -...

430

E-Print Network 3.0 - ax tank farm Sample Search Results  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

In collaboration with The Dow Chemical Company 12;A tank farm is a set of storage tanks that hold finished product... product Dedicated Tanks Without available storage ......

431

E-Print Network 3.0 - anestesia espinal tratamiento Sample Search...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

SOCIAL 3 CURSO DE LA DIPLOMATURA EN TRABAJO SOCIAL Summary: o tratamiento. -Enorme carga cultural. -- Difcil aplicacin en discap. sensoriales 12;a) Clasificacin...

432

Michael C. Bond, MD, FACEP, FAAEM Assistant Professor  

E-Print Network [OSTI]

. 75% E. 100% #12;A. Ben Stiller B. Johnny Depp C. Leonardo DiCaprio D. Tom Hanks Ben Stiller Johnny

Weber, David J.

433

E-Print Network 3.0 - arteriellen verschlusserkrankung der Sample...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

of Physiology, McGill University Collection: Biology and Medicine 12 A precursor in waterhammer analysis rediscovering Johannes Arris S Tijsseling Alexander Anderson Summary: )....

434

E-Print Network 3.0 - ayuda para dejar Sample Search Results  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

pulsando sobre l. 12;Pulsamos sobre el botn subir para posicionarlo en primer lugar. 12;A partir de... Explorer, para conseguir un correcto funcionamiento de esta...

435

1 Introduction 1 1.1 Department Staffs . . . . . . . . . . . . . . . . . . . . . . . . . .*  

E-Print Network [OSTI]

Contents 1 Introduction 1 1.1 Department Staffs . . . . . . . . . . . . . . . . . . . . . . . . . .* * . . . . . . . . 1 1.2 A Brief History of the Department . . . . . . . . . . . . . . . . . . * *. . . . . . . 2 2

Imai, Hiroshi

436

E-Print Network 3.0 - asynchronous event-driven particle Sample...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Princeton University Collection: Computer Technologies and Information Sciences 12 A Comparison of Two Methods for Advancing Time In Parallel Discrete Event Simulation...

437

E-Print Network 3.0 - ancestor aegilops tauschii Sample Search...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Medicine 12 A SINE family widely distributed in the plant kingdom and its evolutionary history Summary: by database sear- ches. Group Family Species Monocots Gramineae Aegilops...

438

Graphene and its Hybrid Nanostructures for Nanoelectronics and Energy Applications  

E-Print Network [OSTI]

improve the PCE of photovoltaic cells. Figure 1.12 (a) Ramantransparent electrode in photovoltaic cell. Novel synthesiswith ITO-based photovoltaic cell. And two approaches of

LIN, JIAN

2011-01-01T23:59:59.000Z

439

E-Print Network 3.0 - adventitious rooting process1 Sample Search...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

12 A rapid regeneration protocol from 7-day-old hypocotyls from mature embryos of green ash (Fraxinus pennsylvanica) was developed. The best hypocotyl regeneration medium...

440

Health & Safety Plan Last Updated  

E-Print Network [OSTI]

Health & Safety Plan Last Updated March 2008 1 #12;A. SCOPE AND RESPONSIBILITY....................................................................................................................................... 3 2. Safety and Health Policy...................................................................................................................... 3 4. Safety Coordinator

Anderson, Richard

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

E-Print Network 3.0 - activity-based travel demand Sample Search...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Approach to Household Travel Choice by Kara... Fall 1998 12;A Utility-Theory-Consistent System-of-Demand-Equations Approach to Household Travel... the...

442

Effects of Spectral Error in Efficiency Measurements of GaInAs...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

with respect to reference spectral irradiance distributions, which are tables of solar irradiance and light wavelength pairs 1,2. A reference spectrum is one element of...

443

Riso-M-1937 Research Establishment Riso  

E-Print Network [OSTI]

.N.Singh, and P.Barlow May 1977 University of S U I H X , Brighton, and AERE Harwell, Didcot, England #12;A. E

444

mac  

National Nuclear Security Administration (NNSA)

1%2A en Military Academic Collaborations http:nnsa.energy.govaboutusourprogramsdefenseprogramsmilitaryacademiccollaborations

445

planning for emergencies  

National Nuclear Security Administration (NNSA)

1%2A en Planning for Emergencies http:nnsa.energy.govaboutusourprogramsemergencyoperationscounterterrorismplanningforemergencies

446

operations center  

National Nuclear Security Administration (NNSA)

1%2A en Operations Center http:nnsa.energy.govaboutusourprogramsemergencyoperationscounterterrorismoperationscenter

...

447

Rensselaer  

E-Print Network [OSTI]

problems were derived by Sun et al. [133, 134]. Their algorithm ...... SDPLIB 1.2, a library of semidefinite programming test problems. Optimization. Methods and...

2009-05-11T23:59:59.000Z

448

A New Years Trip A New Years Trip  

E-Print Network [OSTI]

A New Years Trip A New Years Trip December 26, 2003 - January 3, 2004 By Saul Wilson #12;A New Years Trip 7 INTRODUCTION #12;A New Years Trip 8 rom December 26, 2003 to January 3, 2004 my dad and I

Wilson, W. Stephen

449

Jnosi Imre Krmn Krnyezeti ramlsok Hallgati Laboratrium,  

E-Print Network [OSTI]

Szolitonok a laboratóriumban #12;A 2004 december 26.-i esemény Kenji Satake, 2005 DigitalGlobe, 2005 #12;A 2004 december 26.-i esemény #12;#12;Cunami elfordulások #12;Cunami elfordulások #12;Hullámtörés S

Jánosi, Imre M.

450

SPARTANS ABROAD 2011 entries  

E-Print Network [OSTI]

Lines Madrid - Spain Architecture #12;Showboat Opera House Sydney - Australia Architecture #12;Our Architecture #12;A Land Down Under Sydney ­ Australia Architecture #12;A Sydney Sunset Sydney - Australia Architecture #12;Capturing Big Ben from Trafalgar Square London - England Architecture #12;Sydney Sydney

451

Quantum Computation with the Jaynes-Cummings Model  

Science Journals Connector (OSTI)

......2 a1|0 a2 - |0 a1|2 a2) NS1,NS2 - - 1 2 (|2 a1|0 a2 - |0 a1|2 a2...to utilize the quantum error correcting codes. The quantum error correction and the...if we use the Calderbank-Shor-Steane code, which maps one qubit into seven qubits......

Hiroo Azuma

2011-09-01T23:59:59.000Z

452

a parent handbook for Talking with  

E-Print Network [OSTI]

a parent handbook for Talking with College Students About Alcohol Rob Turrisi, Ph.D., Prevention Research Center, The Pennsylvania State University #12;a parent handbook for Talking with College Students the author. A Parent Handbook for Talking with College Students About Alcohol2 #12;A Parent Handbook

Wisconsin at Madison, University of

453

IDS Business Support, Communications and  

E-Print Network [OSTI]

to space to achieve thermal control and maintain components at acceptable temperatures. An Active Thermal a constant coolant supply to equipment, payloads and avionics to maintain proper temperature. The U Thermal Control System (ATCS) Overview EEATCS (5A-12A.1)/EATCS (12A.1+) Active Thermal Control System

454

b038.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

520) 520) 3/2 - I (J P ) = 0( 3 2 - ) Status: ∗∗∗∗ Discovered by FERRO-LUZZI 62; the elaboration in WATSON 63 is the classic paper on the Breit-Wigner analysis of a multichannel resonance. The measurements of the mass, width, and elasticity published be- fore 1975 are now obsolete and have been omitted. They were last listed in our 1982 edition Physics Letters 111B 111B 111B 111B 1 (1982). Production and formation experiments agree quite well, so they are listed together here. Λ(1520) MASS Λ(1520) MASS Λ(1520) MASS Λ(1520) MASS VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 1519.5 ± 1.0 OUR ESTIMATE 1519.5 ± 1.0 OUR ESTIMATE 1519.5 ± 1.0 OUR ESTIMATE 1519.5 ± 1.0 OUR ESTIMATE 1519.53± 0.19 OUR AVERAGE 1519.53± 0.19 OUR AVERAGE 1519.53± 0.19 OUR AVERAGE 1519.53± 0.19 OUR AVERAGE 1520.4 ± 0.6 ± 1.5 1 QIANG 10 SPEC e p → e ' K + X (fit to X ) 1517.3 ± 1.5 300 BARBER 80D SPEC γ p → Λ(1520)

455

b023.dvi  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

480) 480) Bumps I (J P ) = 1(? ? ) Status: ∗ OMITTED FROM SUMMARY TABLE These are peaks seen in Λ π and Σ π spectra in the reaction π + p → ( Y π ) K + at 1.7 GeV/c. Also, the Y polarization oscillates in the same region. MILLER 70 suggests a possible alternate explanation in terms of a reflection of N(1675) → Λ K decay. However, such an explanation for the ( Σ + π 0 ) K + channel in terms of ∆(1650) → Σ K decay seems unlikely (see PAN 70). In addition such reflections would also have to account for the oscillation of the Y polarization in the 1480 MeV region. HANSON 71, with less data than PAN 70, can neither confirm nor deny the existence of this state. MAST 75 sees no structure in this region in K - p → Λ π 0 . ENGELEN 80 performs a multichannel analysis of K - p → p K 0 π - at 4.2 GeV/c. They observe a 3.5 standard-deviation signal at 1480 MeV in p K 0 which cannot be explained as a reflection of any com- peting

456

Design of far-infrared three-wave polarimeter-interferometer system for the J-TEXT tokamak  

SciTech Connect (OSTI)

A multichannel three-wave far-infrared polarimeter-interferometer will be constructed on the J-TEXT tokamak (R=1.05 m, a=0.27 m, B{sub T}{<=}3 T, and I{sub P}{<=}350 kA) for current density profile and electron density profile measurements. The system will adopt the three-wave polarimeter configuration which was first introduced on RTP. Three 432.5 {mu}m HCOOH lasers pumped by three CO{sub 2} lasers separately will be adopted, which could generate high output power, nearly 50 mW at each cavity. Two of them will be counter-rotating circularly polarized to probe the Faraday angle, while the third laser will be used as a local oscillator to get the phase shift caused by electron density. Excellent port access (600x76 mm{sup 2}) and high laser power would promise a profile measurement across the whole plasma section with good signal quality. A high-speed digital phase comparator with a few ({approx}2) {mu}s temporal resolution will be developed, so that fast changes of current or density profile could be measured. Six channels will be installed in the first stage.

Chen, J.; Gao, L.; Zhuang, G.; Wang, Z. J. [Institute of Nuclear Fusion and Plasma Physics, College of Electrical and Electronic Engineering, Huazhong University of Science and Technology, Wuhan 430074, China and Key Laboratory of Fusion and Advanced Electromagnetic Technology, Ministry of Education, Wuhan 430074 (China); Gentle, K. W. [Institute of Fusion Studies, University of Texas at Austin, Texas 78712 (United States)

2010-10-15T23:59:59.000Z

457

FPGA design and implementation for EIT data acquisition  

Science Journals Connector (OSTI)

OXBACT-5 was designed to meet the challenges involved in working in the intensive care hospital environment focussed particularly on thoracic imaging of patients with respiratory distress and chronic heart failure (CHF). The FPGA-based wireless LAN linked multi-channel EIT data acquisition system (DAS) providing 16 programmable excitation current channels and 64 voltage measurement channels is presented. It contains function modules of a PCI bus interface, direct digital synthesizers, dual-port memory blocks, digital demodulation and all the command and control logic in the FPGA. The whole EIT data acquisition system is fully programmable and reconfigurable from the host PC. The excitation frequency, excitation patterns, the measuring sequence and the gain of each measurement channel can be set from the host PC before each measurement. The demodulation is implemented in the FPGA chip to reduce the data rate between the DAS and the host PC. In addition, measurement process management is achieved in this FPGA chip. Complemented by analogue devices such as ADCs, DACs, analogue buffers and analogue multiplexers, the new FPGA-based EIT DAS system is implemented in a very compact way for bedside use in intensive care units of hospitals. It is intended for applications such as continuous respiration monitoring with data collection at 25 frames per second. Image reconstruction times depend on the choice of 2D or 3D imaging algorithms and the available processing power.

Xicai Yue; Chris McLeod

2008-01-01T23:59:59.000Z

458

Fusion of product and process data: Batch-mode and real-time streaming  

SciTech Connect (OSTI)

In today's DP product realization enterprise it is imperative to reduce the design-to-fabrication cycle time and cost while improving the quality of DP parts (reducing defects). Much of this challenge resides in the inherent gap between the product and process worlds. The lack of seamless, bi-directional flow of information prevents true concurrency in the product realization world. This report addresses a framework for product-process data fusion to help achieve next generation product realization. A fundamental objective is to create an open environment for multichannel observation of process date, and subsequent mapping of that data onto product geometry. In addition to the sensor-based observation of manufacturing processes, model-based process data provides an important complement to empirically acquired data. Two basic groups of manufacturing models are process physics, and machine kinematics and dynamics. Process physics addresses analytical models that describe the physical phenomena of the process itself. Machine kinematic and dynamic models address the mechanical behavior of the processing equipment. As a secondary objective, an attempt has been made in this report to address part of the model-based realm through the development of an open object-oriented library and toolkit for machine kinematics and dynamics. Ultimately, it is desirable to integrate design definition, with all types of process data; both sensor-based and model-based. Collectively, the goal is to allow all disciplines within the product realization enterprise to have a centralized medium for the fusion of product and process data.

Vincent De Sapio; Spike Leonard

1999-12-01T23:59:59.000Z

459

Ambient temperature cadmium zinc telluride radiation detector and amplifier circuit  

DOE Patents [OSTI]

A low noise, low power consumption, compact, ambient temperature signal amplifier for a Cadmium Zinc Telluride (CZT) radiation detector. The amplifier can be used within a larger system (e.g., including a multi-channel analyzer) to allow isotopic analysis of radionuclides in the field. In one embodiment, the circuit stages of the low power, low noise amplifier are constructed using integrated circuit (IC) amplifiers , rather than discrete components, and include a very low noise, high gain, high bandwidth dual part preamplification stage, an amplification stage, and an filter stage. The low noise, low power consumption, compact, ambient temperature amplifier enables the CZT detector to achieve both the efficiency required to determine the presence of radio nuclides and the resolution necessary to perform isotopic analysis to perform nuclear material identification. The present low noise, low power, compact, ambient temperature amplifier enables a CZT detector to achieve resolution of less than 3% full width at half maximum at 122 keV for a Cobalt-57 isotope source. By using IC circuits and using only a single 12 volt supply and ground, the novel amplifier provides significant power savings and is well suited for prolonged portable in-field use and does not require heavy, bulky power supply components.

McQuaid, James H. (Livermore, CA); Lavietes, Anthony D. (Hayward, CA)

1998-05-29T23:59:59.000Z

460

Development and experimental study on organic Rankine cycle system with single-screw expander for waste heat recovery from exhaust of diesel engine  

Science Journals Connector (OSTI)

Abstract A single-screw expander with 155mm diameter screw has been developed. A spiral-tube type evaporator and an aluminum multi-channel parallel type condenser have also been developed with weight of 147kg and 78kg, respectively. Based on the development of above components, an ORC (organic Rankine cycle) system prototype was assembled and tested for waste heat recovery from diesel engine exhaust. An experimental system was built for this ORC system, and experiments were conducted for different expander torque and diesel engine loads. Influences of expander torque and diesel engine loads on the performances of ORC system were studied. The results indicated that the maximum of the power output is 10.38kW and the biggest ORC efficiency and overall system efficiency are respectively 6.48% and 43.8%, which are achieved at 250kW of diesel engine output. Meanwhile the biggest improvement of overall system efficiency is 1.53%. The maximums of volume efficiency, adiabatic efficiency and total efficiency of single-screw expander are 90.73%, 73.25% and 57.88%, respectively.

Ye-Qiang Zhang; Yu-Ting Wu; Guo-Dong Xia; Chong-Fang Ma; Wei-Ning Ji; Shan-Wei Liu; Kai Yang; Fu-Bin Yang

2014-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "12a dpwa multichannel" 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

Hadamard multimode optical imaging transceiver  

DOE Patents [OSTI]

Disclosed is a method and system for simultaneously acquiring and producing results for multiple image modes using a common sensor without optical filtering, scanning, or other moving parts. The system and method utilize the Walsh-Hadamard correlation detection process (e.g., functions/matrix) to provide an all-binary structure that permits seamless bridging between analog and digital domains. An embodiment may capture an incoming optical signal at an optical aperture, convert the optical signal to an electrical signal, pass the electrical signal through a Low-Noise Amplifier (LNA) to create an LNA signal, pass the LNA signal through one or more correlators where each correlator has a corresponding Walsh-Hadamard (WH) binary basis function, calculate a correlation output coefficient for each correlator as a function of the corresponding WH binary basis function in accordance with Walsh-Hadamard mathematical principles, digitize each of the correlation output coefficient by passing each correlation output coefficient through an Analog-to-Digital Converter (ADC), and performing image mode processing on the digitized correlation output coefficients as desired to produce one or more image modes. Some, but not all, potential image modes include: multi-channel access, temporal, range, three-dimensional, and synthetic aperture.

Cooke, Bradly J; Guenther, David C; Tiee, Joe J; Kellum, Mervyn J; Olivas, Nicholas L; Weisse-Bernstein, Nina R; Judd, Stephen L; Braun, Thomas R

2012-10-30T23:59:59.000Z

462

Subbarrier fusion reactions and many-particle quantum tunneling  

E-Print Network [OSTI]

Low energy heavy-ion fusion reactions are governed by quantum tunneling through the Coulomb barrier formed by a strong cancellation of the repulsive Coulomb force with the attractive nuclear interaction between the colliding nuclei. Extensive experimental as well as theoretical studies have revealed that fusion reactions are strongly influenced by couplings of the relative motion of the colliding nuclei to several nuclear intrinsic motions. Heavy-ion subbarrier fusion reactions thus provide a good opportunity to address a general problem on quantum tunneling in the presence of couplings, which has been a popular subject in the past decades in many branches of physics and chemistry. Here we review theoretical aspects of heavy-ion subbarrier fusion reactions from the view point of quantum tunneling in systems with many degrees of freedom. Particular emphases are put on the coupled-channels approach to fusion reactions, and the barrier distribution representation for multi-channel penetrability. We also discuss an application of the barrier distribution method to elucidation of the mechanism of dissociative adsorption of H$_2$ melecules in surface science.

K. Hagino; N. Takigawa

2012-09-28T23:59:59.000Z

463

A pepper-pot emittance meter for low-energy heavy-ion beams  

SciTech Connect (OSTI)

A novel emittance meter has been developed to measure the four-dimensional, transverse phase-space distribution of a low-energy ion beam using the pepper-pot technique. A characteristic feature of this instrument is that the pepper-pot plate, which has a linear array of holes in the vertical direction, is scanned horizontally through the ion beam. This has the advantage that the emittance can also be measured at locations along the beam line where the beam has a large horizontal divergence. A set of multi-channel plates, scintillation screen, and ccd camera is used as a position-sensitive ion detector allowing a large range of beam intensities that can be handled. This paper describes the design, construction, and operation of the instrument as well as the data analysis used to reconstruct the four-dimensional phase-space distribution of an ion beam. Measurements on a 15 keV He{sup +} beam are used as an example.

Kremers, H. R.; Beijers, J. P. M.; Brandenburg, S. [Kernfysisch Versneller Instituut, University of Groningen, Zernikelaan 25, 9747 AA Groningen (Netherlands)

2013-02-15T23:59:59.000Z

464

On the Determination of Elastic and Inelastic Nuclear Observables from Lattice QCD  

E-Print Network [OSTI]

One of the overarching goals of nuclear physics is to rigorously compute properties of hadronic systems directly from the fundamental theory of the strong interaction, Quantum Chromodynamics (QCD). Currently, lattice QCD (LQCD) provides the only reliable option for performing calculations of low-energy hadronic observables. LQCD calculations are necessarily performed in a finite Euclidean spacetime. As a result, it is necessary to construct formalism that maps the finite-volume observables determined via LQCD to the infinite-volume quantities of interest. This methodology is commonly referred to as the Luscher method, as it was Martin Luscher who first developed such formalism for scalar bosons with zero total momentum below inelastic thresholds. In this work, we review recent progress on the generalization of this formalism. We present a detailed derivation of the extension of Luscher's seminal work for multi-channel two-body scalar systems, two-nucleon non-relativistic systems, and three-body non-relativistic scalar systems. For all of these scenarios we allow for the total momenta of the systems of interest to be nonzero. We also present steps towards being able to study weak processes involving two-nucleon systems, in particular we show how to determine the transition amplitude for proton-proton fusion (pp->e^+ + nu_e) directly from LQCD.

Raul A. Briceno

2013-11-23T23:59:59.000Z

465

Quench dynamics in SRF cavities: can we locate the quench origin with 2nd sound?  

SciTech Connect (OSTI)

A newly developed method of locating quenches in SRF cavities by detecting second-sound waves has been gaining popularity in SRF laboratories. The technique is based on measurements of time delays between the quench as determined by the RF system and arrival of the second-sound wave to the multiple detectors placed around the cavity in superfluid helium. Unlike multi-channel temperature mapping, this approach requires only a few sensors and simple readout electronics; it can be used with SRF cavities of almost arbitrary shape. One of its drawbacks is that being an indirect method it requires one to solve an inverse problem to find the location of a quench. We tried to solve this inverse problem by using a parametric forward model. By analyzing the data we found that the approximation where the second-sound emitter is a near-singular source does not describe the physical system well enough. A time-dependent analysis of the quench process can help us to put forward a more adequate model. We present here our current algorithm to solve the inverse problem and discuss the experimental results.

Maximenko, Yulia; /Moscow, MIPT; Segatskov, Dmitri A.; /Fermilab

2011-03-01T23:59:59.000Z

466

OBSERVATIONAL EVIDENCE OF RESONANTLY DAMPED PROPAGATING KINK WAVES IN THE SOLAR CORONA  

SciTech Connect (OSTI)

In this Letter, we establish clear evidence for the resonant absorption damping mechanism by analyzing observational data from the novel Coronal Multi-Channel Polarimeter. This instrument has established that in the solar corona there are ubiquitous propagating low-amplitude ({approx}1 km s{sup -1}) Alfvenic waves with a wide range of frequencies. Realistically interpreting these waves as the kink mode from magnetohydrodynamic wave theory, they should exhibit a frequency-dependent damping length due to resonant absorption, governed by the Terradas-Goossens-Verth relation showing that transverse plasma inhomogeneity in coronal magnetic flux tubes causes them to act as natural low-pass filters. It is found that the observed frequency dependence on damping length (up to about 8 mHz) can be explained by the kink wave interpretation; and furthermore, the spatially averaged equilibrium parameter describing the length scale of transverse plasma density inhomogeneity over a system of coronal loops is consistent with the range of values estimated from Transition Region and Coronal Explorer observations of standing kink modes.

Verth, G.; Goossens, M. [Centrum voor Plasma Astrofysica and Leuven Mathematical Modeling and Computational Science Centre, KU Leuven, Celestijnenlaan 200B, 3001 Heverlee (Belgium); Terradas, J., E-mail: gary.verth@wis.kuleuven.b, E-mail: marcel.goossens@wis.kuleuven.b, E-mail: jaume.terradas@uib.e [Departament de Fisica, Universitat de les Illes Balears, E-07122 Palma de Mallorca (Spain)

2010-08-01T23:59:59.000Z

467

Neutron-scattering study of the magnon energies and intensities in iron  

Science Journals Connector (OSTI)

The magnetic inelastic neutron scattering at low temperatures has been measured from a large single crystal of Fe54(12 at.% Si) up to energy transfers of 100 meV using the constant-Q spectrometer at the Los Alamos pulsed neutron source. The spin-wave energies and intensities were obtained from the data by using a multichannel maximum-entropy technique, and we show that much more detailed information can be obtained from the maximum-entropy analysis. The observed spin-wave dispersion relations obtained in the present experiment are in excellent agreement with earlier data, and we observe a sharp falloff of the (001) magnon intensity at approximately 80 meV, which is in accord with previous experimental measurements and multiband theoretical calculations of the dynamic susceptibility of iron. We also compare the data rate obtained with the constant-Q spectrometer to a triple-axis instrument and find that the spectrometer is competitive for this type of measurement.

M. Yethiraj; R. A. Robinson; D. S. Sivia; J. W. Lynn; H. A. Mook

1991-02-01T23:59:59.000Z

468

New underwater acoustic tank facility at Georgia Tech  

Science Journals Connector (OSTI)

A large underwater acoustic tank facility located in the Woodruff School of Mechanical Engineering at Georgia Tech has recently been completed. The facility includes a rectangular concrete water tank 25 feet deep 25 feet wide and 34 feet long containing around 160 000 gallons of water. There are three computer?controlled positioners: an x?y?z?? positioner and a z?? positioner mounted on carriages and a bottom mounted rotator. The facility has a large rectangular nearfield array which can be used either as a receiver or a transmitter. A single vertical nearfield line array can be translated by the x?y positioner to synthesize a cylindrical nearfield receiving array. The rectangular nearfield transmitting array and the synthesized cylindrical receiving array were designed to be used with the bottom mounted rotator to measure the true farfield bistatic target strength of any target up to one meter in length as a function of the target aspect angle. Such measurements can be done from 2 kHz to over 10 kHz. The tank is being used for transducer development materials and flow noise studies in addition to structural acoustics. Several available multichannel data acquisition systems will be described. [Work supported in part by a DURIP grant from ONR.

2002-01-01T23:59:59.000Z

469

Ambient temperature cadmium zinc telluride radiation detector and amplifier circuit  

DOE Patents [OSTI]

A low noise, low power consumption, compact, ambient temperature signal amplifier for a Cadmium Zinc Telluride (CZT) radiation detector is disclosed. The amplifier can be used within a larger system (e.g., including a multi-channel analyzer) to allow isotopic analysis of radionuclides in the field. In one embodiment, the circuit stages of the low power, low noise amplifier are constructed using integrated circuit (IC) amplifiers , rather than discrete components, and include a very low noise, high gain, high bandwidth dual part preamplification stage, an amplification stage, and an filter stage. The low noise, low power consumption, compact, ambient temperature amplifier enables the CZT detector to achieve both the efficiency required to determine the presence of radionuclides and the resolution necessary to perform isotopic analysis to perform nuclear material identification. The present low noise, low power, compact, ambient temperature amplifier enables a CZT detector to achieve resolution of less than 3% full width at half maximum at 122 keV for a Cobalt-57 isotope source. By using IC circuits and using only a single 12 volt supply and ground, the novel amplifier provides significant power savings and is well suited for prolonged portable in-field use and does not require heavy, bulky power supply components. 9 figs.

McQuaid, J.H.; Lavietes, A.D.

1998-05-26T23:59:59.000Z

470

Absolute spectral characterization of silicon barrier diode: Application to soft X-ray fusion diagnostics at Tore Supra  

SciTech Connect (OSTI)

This paper presents an experimental protocol for absolute calibration of photo-detectors. Spectral characterization is achieved by a methodology that unlike the usual line emissions-based method, hinges on the Bremsstrahlung radiation of a Soft X-Ray (SXR) tube only. Although the proposed methodology can be applied virtually to any detector, the application presented in this paper is based on Tore Supra's SXR diagnostics, which uses Silicon Surface Barrier Diodes. The spectral response of these n-p junctions had previously been estimated on a purely empirical basis. This time, a series of second-order effects, like the spatial distribution of the source radiated power or multi-channel analyser non linearity, are taken into account to achieve accurate measurements. Consequently, a parameterised physical model is fitted to experimental results and the existence of an unexpected dead layer (at least 5 {mu}m thick) is evidenced. This contribution also echoes a more general on-going effort in favour of long-term quality of passive radiation measurements on Tokamaks.

Vezinet, D.; Mazon, D.; Malard, P. [CEA, IRFM, F-13108 Saint-Paul-lez-Durance (France)

2013-07-14T23:59:59.000Z

471

RAMONA-4B a computer code with three-dimensional neutron kinetics for BWR and SBWR system transient - user`s manual  

SciTech Connect (OSTI)

This document is the User`s Manual for the Boiling Water Reactor (BWR), and Simplified Boiling Water Reactor (SBWR) systems transient code RAMONA-4B. The code uses a three-dimensional neutron-kinetics model coupled with a multichannel, nonequilibrium, drift-flux, phase-flow model of the thermal hydraulics of the reactor vessel. The code is designed to analyze a wide spectrum of BWR core and system transients. Chapter 1 gives an overview of the code`s capabilities and limitations; Chapter 2 describes the code`s structure, lists major subroutines, and discusses the computer requirements. Chapter 3 is on code, auxillary codes, and instructions for running RAMONA-4B on Sun SPARC and IBM Workstations. Chapter 4 contains component descriptions and detailed card-by-card input instructions. Chapter 5 provides samples of the tabulated output for the steady-state and transient calculations and discusses the plotting procedures for the steady-state and transient calculations. Three appendices contain important user and programmer information: lists of plot variables (Appendix A) listings of input deck for sample problem (Appendix B), and a description of the plotting program PAD (Appendix C). 24 refs., 18 figs., 11 tabs.

Rohatgi, U.S.; Cheng, H.S.; Khan, H.J.; Mallen, A.N.; Neymotin, L.Y.

1998-03-01T23:59:59.000Z

472

Technical Note: Removing the stem effect when performing Ir-192 HDR brachytherapy in vivo dosimetry using plastic scintillation detectors: A relevant and necessary step  

SciTech Connect (OSTI)

Purpose: The purpose of this study was to investigate whether or not a stem effect removal technique is necessary when performing Ir-192 HDR brachytherapy in vivo dosimetry using a scintillation detector. Methods: A red-green-blue photodiode connected to a multichannel electrometer was used to detect the light emitted from a plastic scintillation detector (PSD) during irradiation with an Ir-192 HDR brachytherapy source. Accuracy in dose measurement was compared with and without the use of stem effect removal techniques. Monochromatic and polychromatic filtration techniques were studied. An in-house template was built for accurate positioning of catheters in which the source and the PSD were inserted. Dose distribution was measured up to 5 cm from source to detector in the radial and longitudinal directions. Results: The authors found the stem effect to be particularly important when the source was close to the optical fiber guide and far from the scintillation component of the detector. It can account for up to (72{+-}3)% of the signal under clinically relevant conditions. The polychromatic filtration outperformed the monochromatic filtration as well as the absence of filtration in regard to dose measurement accuracy. Conclusions: It is necessary to implement a stem effect removal technique when building a PSD for in vivo dosimetry during Ir-192 HDR brachytherapy. The PSD that the authors have developed for this study would be suitable for such an application.

Therriault-Proulx, Francois; Beddar, Sam; Briere, Tina M.; Archambault, Louis; Beaulieu, Luc [Department of Radiation Physics, University of Texas MD Anderson Cancer Center, 1515 Holcombe Boulevard, Unit 94, Houston, Texas 77030 (United States) and Departement de Physique, de Genie Physique et d'Optique, Universite Laval, Quebec, Quebec G1K 7P4 (Canada); Department of Radiation Physics, University of Texas MD Anderson Cancer Center, 1515 Holcombe Boulevard, Unit 94, Houston, Texas 77030 (United States); Departement de Physique, de Genie Physique et d'Optique, Universite Laval, Quebec, Quebec G1K 7P4 (Canada) and Departement de Radio-Oncologie, Ho circumflex tel-Dieu de Quebec, Centre Hospitalier Universitaire de Quebec, Quebec, Quebec G1R 2J6 (Canada)

2011-04-15T23:59:59.000Z

473

Integrated intra-subassembly treatment in the SASSYS-1 LMR systems analysis code  

SciTech Connect (OSTI)

This report discusses a hot channel treatment which has been added to the SASSYS-1 LMR systems analysis code by providing for a multiple pin treatment of each of one or more subassemblies. This is an explicit calculation of intra-subassembly effects, not a hot-channel adjustment to a calculated average channel. Thus, the code can account for effects such as transient flow redistribution, both within a subassembly and among subassemblies. The code now provides a total integrated thermal hydraulic treatment including a multiple pin treatment within subassemblies, a multi-channel treatment of the whole core, and models for the primary coolant loops, the intermediate coolant loops, the steam generators, and the balance of plant. Currently the multiple-pin option is only implemented for single-phase calculations. It is not applicable after the onset of boiling or pin disruption. The new multiple pin treatment is being verified with detailed temperature data from instrumented subassemblies in EBR-II, both steady-state and transient, with special emphasis on passive safety tests such as SHRT-45. For the SHRT-45 test, excellent agreement is obtained between code predictions and experimental measurements of coolant temperatures.

Dunn, F.

1992-09-01T23:59:59.000Z

474

Integrated intra-subassembly treatment in the SASSYS-1 LMR systems analysis code  

SciTech Connect (OSTI)

This report discusses a hot channel treatment which has been added to the SASSYS-1 LMR systems analysis code by providing for a multiple pin treatment of each of one or more subassemblies. This is an explicit calculation of intra-subassembly effects, not a hot-channel adjustment to a calculated average channel. Thus, the code can account for effects such as transient flow redistribution, both within a subassembly and among subassemblies. The code now provides a total integrated thermal hydraulic treatment including a multiple pin treatment within subassemblies, a multi-channel treatment of the whole core, and models for the primary coolant loops, the intermediate coolant loops, the steam generators, and the balance of plant. Currently the multiple-pin option is only implemented for single-phase calculations. It is not applicable after the onset of boiling or pin disruption. The new multiple pin treatment is being verified with detailed temperature data from instrumented subassemblies in EBR-II, both steady-state and transient, with special emphasis on passive safety tests such as SHRT-45. For the SHRT-45 test, excellent agreement is obtained between code predictions and experimental measurements of coolant temperatures.

Dunn, F.

1992-01-01T23:59:59.000Z

475

Energy performance evaluation of fishing vessels by fuel mass flow measuring system  

Science Journals Connector (OSTI)

A new fuel consumption monitoring system was set up for research purpose in order to evaluate the energy performance of fishing vessels under different operating conditions. The system has been tested on two semi-pelagic pair trawlers in the Adriatic Sea with an engine power of around 900kW, and with length overall of around 30m. Both vessels work with a gear of similar design and size, the differences between the two vessels are in the propeller design and the hull material: the first with a controllable pitch propeller (CPP) and a metal hull, the second with a fixed pitch propeller (FPP) and a wooden hull. The fuel monitoring system conceived at CNR-ISMAR Ancona (Italy) consists of two mass flow sensors, one multichannel recorder and one GPS data logger. The working time duration, the vessel speed, the total fuel consumption and the instant fuel rate were logged by the system. A typical commercial round trip for a semi-pelagic trawler consists of several fishing operations (steaming, trawling sailing, etc.). Fuel consumption rate and vessel speed data were used to identify energy performance under different vessel-operating conditions. The highest fuel demands were during the trawling (130l/h at 4.4kn) and the steaming (100130l/h at 11kn) phases. Fuel savings of up to 15% could be obtained by reducing the navigation speed of half a knot.

Antonello Sala; Francesco De Carlo; Gabriele Buglioni; Alessandro Lucchetti

2011-01-01T23:59:59.000Z

476

Statistical Evidence for the Existence of Alfv\\'enic Turbulence in Solar Coronal Loops  

E-Print Network [OSTI]

Recent observations have demonstrated that waves which are capable of carrying large amounts of energy are ubiquitous throughout the solar corona. However, the question of how this wave energy is dissipated (on which time and length scales) and released into the plasma remains largely unanswered. Both analytic and numerical models have previously shown that Alfv\\'enic turbulence may play a key role not only in the generation of the fast solar wind, but in the heating of coronal loops. In an effort to bridge the gap between theory and observations, we expand on a recent study [De Moortel et al., ApJL, 782:L34, 2014] by analyzing thirty-seven clearly isolated coronal loops using data from the Coronal Multi-channel Polarimeter (CoMP) instrument. We observe Alfv\\'enic perturbations with phase speeds which range from 250-750 km/s and periods from 140-270 s for the chosen loops. While excesses of high frequency wave-power are observed near the apex of some loops (tentatively supporting the onset of Alfv\\'enic turbu...

Liu, Jiajia; De Moortel, Ineke; Threlfall, James; Bethge, Christian

2014-01-01T23:59:59.000Z

477

Role of alkyl alcohol on viscosity of silica-based chemical gels for decontamination of highly radioactive nuclear facilities  

SciTech Connect (OSTI)

Silica-based chemical gel for the decontamination of nuclear facilities was prepared by using fumed silica as a viscosifier, a 0.5 M Ce (IV) solution dissolved in concentrated nitric acid as a chemical decontamination agent, and tripropylene glycol butyl ether (TPGBE) as a co-viscosifier. A new effective strategy for the preparation of the chemical gel was investigated by introducing the alkyl alcohols as organic solvents to effectively dissolve the co-viscosifier. The mixture solution of the co-viscosifier and alkyl alcohols was more effective in the control of viscosity than that of the co-viscosifier only in gel. Here, the alkyl alcohols played a key role as an effective dissolution solvent for the co-viscosifier in the preparation of the chemical gel, resulting in a reducing of the amount of the co-viscosifier and gel time compared with that of the chemical gel prepared without the alkyl alcohols. It was considered that the alkyl alcohols contributed to the effective dissolution of the co-viscosifier as well as the homogeneous mixing in the formation of the gel, while the co-viscosifier in an aqueous media of the chemical decontamination agent solution showed a lower solubility. The decontamination efficiency of the chemical gels prepared in this work using a multi-channel analyzer (MCA) showed a high decontamination efficiency of over ca. 94% and ca. 92% for Co-60 and Cs-137 contaminated on surface of the stainless steel 304, respectively. (authors)

Choi, B. S.; Yoon, S. B.; Jung, C. H.; Lee, K. W.; Moon, J. K. [Div. of Decontamination and Decommissioning Technology Development, Korea Atomic Energy Research Inst., Daedeok-daero 989-111, Yuseong-gu, Daejeon, 305-353 (Korea, Republic of)

2012-07-01T23:59:59.000Z

478

Evidence for natural gas hydrate occurrences in Colombia Basin  

SciTech Connect (OSTI)

Multichannel and selected single-channel seismic lines of the continental margin sediments of the Colombia basin display compelling evidence for large accumulations of natural gas hydrate. Seismic bottom simulating reflectors (BSRs), interpreted to mark the base of the hydrate stability zone, are pronounced and very widespread along the entire Panama-Colombia lower continental slope. BSRs have also been identified at two locations on the abyssal plain. Water depths for these suspected hydrate occurrences range from 900 to 4000 m. Although no gas hydrate samples have been recovered from this area, biogenic methane is abundant in Pliocene turbidites underlying the abyssal plain. More deeply buried rocks beneath the abyssal plain are thermally mature. Thermogenic gas from these rocks may migrate upward along structural pathways into the hydrate stability zone and form hydrate. Impermeable hydrate layers may form caps over large accumulations of free gas, accounting for the very well-defined BSRs in the area. The abyssal plain and the deformed continental margin hold the highest potential for major economic accumulations of gas hydrate in the basin. The extensive continuity of BSRs, relatively shallow water depths, and promixity to onshore production facilities render the marginal deformed belt sediments the most favorable target for future economic development of the gas hydrate resource within the Colombia basin. The widespread evidence of gas hydrates in the Colombia basin suggests a high potential for conventional hydrocarbon deposits offshore of Panama and Colombia.

Finley, P.D.; Krason, J.; Dominic, K.

1987-05-01T23:59:59.000Z

479

K-Shell Photoabsorption of Magnesium Ions  

E-Print Network [OSTI]

X-ray photoabsorption cross sections have been computed for all magnesium ions using the R-matrix method. A comparison with the other available data for Mg II- Mg X shows good qualitative agreement in general. However, for the lower ionization stages, and for singly-ionized Mg II in particular, the previous R-matrix results (Witthoeft et al. 2009; Witthoeft et al. 2011) overestimate the K-edge position due to the absence of important orbital relaxation effects in those earlier calculations, and a global shift downward in photon energy of those cross sections is therefore warranted. The resultant resonance shapes are found to be quite similar between the two R-matrix results, on the other hand. The cross sections for Mg I and Mg II are further complicated by the M-shell (n=3) occupancy. As a result, the treatment of spectator Auger decay of 1s-> np resonances using the multichannel quantum defect, optical potential method becomes problematic, and it was necessary to implement an alternative, approximate treatm...

Hasoglu, M F; Gorczyca, T W

2013-01-01T23:59:59.000Z

480

Low-energy electron scattering from methanol and ethanol  

Science Journals Connector (OSTI)

Measured and calculated differential cross sections for elastic (rotationally unresolved) electron scattering from two primary alcohols, methanol (CH3OH) and ethanol (C2H5OH), are reported. The measurements are obtained using the relative flow method with helium as the standard gas and a thin aperture as the collimating target gas source. The relative flow method is applied without the restriction imposed by the relative flow pressure conditions on helium and the unknown gas. The experimental data were taken at incident electron energies of 1, 2, 5, 10, 15, 20, 30, 50, and 100eV and for scattering angles of 5130. There are no previous reports of experimental electron scattering differential cross sections for CH3OH and C2H5OH in the literature. The calculated differential cross sections are obtained using two different implementations of the Schwinger multichannel method, one that takes all electrons into account and is adapted for parallel computers, and another that uses pseudopotentials and considers only the valence electrons. Comparison between theory and experiment shows that theory is able to describe low-energy electron scattering from these polyatomic targets quite well.

M. A. Khakoo, J. Blumer, K. Keane, C. Campbell, H. Silva, M. C. A. Lopes, C. Winstead, V. McKoy, R. F. da Costa, L. G. Ferreira, M. A. P. Lima, and M. H. F. Bettega

2008-04-09T23:59:59.000Z

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481

Concentration and temperature measurements in a laser-induced high explosive ignition zone. Part I: LIF spectroscopy measurements  

Science Journals Connector (OSTI)

This paper describes a method that combines a laser ignition technique with laser-induced fluorescence (LIF) spectroscopy for studying the gas-phase products in a laser-induced subignition zone and the reactions that lead to a self-sustained ignition. The experiment comprises a tunable 180 W CO2-laser as ignition source, an excimer pumped dye-laser for inducing the fluorescence, and a spectrometer equipped with an optical multichannel analyzer. This technique was used for measurements of relative NO and CN concentrations in the subignition zone of RDX (1,3,5-Trinitrohexahydro-s-triazine) in pseudo-real time (time resolution better than 1 ?s). By using LIF technique for measuring the relative population of different vibrational levels, we were able to calculate the vibrational temperature in the gas phase reaction zone in front of the sample at subignition to approximately 3100 K. The measurements show clearly that the chemical reactions and the diffusion in the subignition zone play an important part long before a self-sustained reaction occurs, and thus influence the sensitivity of an explosive. By using LIF imaging technique, two-dimensional images of the NO concentration were registered at different times in the ignition pulse, and the wavelength dependence of the ignition source was also studied. The results correspond to a model for fast radiative ignition where Lambert-Beer absorption is the main energy interaction mechanism between the energetic material and the laser beam.

H. stmark; M. Carlson; K. Ekvall

1996-01-01T23:59:59.000Z

482

Pulse generators based on air-insulated linear-transformer-driver stages  

Science Journals Connector (OSTI)

In this paper we present the design and test results of pulse generators based on air-insulated linear-transformer-driver stages that drive a vacuum transmission line. A custom designed unit, referred to as a capacitor block, was developed for use as a main structural element of the transformer stages. It incorporates two capacitors GA 35426 (40nF, 100kV) and a multichannel multigap gas switch. Two types of stages were developed: (1)stage LTD-20 with four modules in parallel and five capacitor blocks in each module (in tests of this stage current amplitude up to 850kA with ?140??ns rise time was obtained on a 0.05???? load at 100kV charging voltage); (2)stage LTD-4 with two modules in parallel and two capacitor blocks in each module. Several installations were built on the base of these stages, including a linear transformer, consisting of two identical LTD-20 stages in series, and a high power electron accelerator on the base of LTD-4 stages. The design, tests results, and main problems are presented and discussed in this paper for these installations.

B. M. Kovalchuk; A. V. Kharlov; E. V. Kumpyak; A. A. Zherlitsyn

2013-05-16T23:59:59.000Z

483

Use of delayed gamma rays for active non-destructive assay of 235U irradiated by pulsed neutron source (plasma focus)  

Science Journals Connector (OSTI)

Abstract A pulsed neutron source based on plasma focus device has been used for active interrogation and assay of 235U by monitoring its delayed high energy ?-rays. The method involves irradiation of fissile material by thermal neutrons obtained after moderation of a burst of neutrons emitted upon fusion of deuterium in plasma focus (PF) device. The delayed gamma rays emitted from the fissile material as a consequence of induced fission were detected by a large volume sodium iodide (NaI(Tl)) detector. The detector is coupled to a data acquisition system of 2k input size with 2k ADC conversion gain. Counting was carried out in pulse height analysis mode for time integrated counts up to 100s while the temporal profile of delayed gamma has been obtained by counting in multichannel scaling mode with dwell time of 50ms. To avoid the effect of passive (natural) and active (from surrounding materials) backgrounds, counts have been acquired for gamma energy between 3 and 10MeV. The lower limit of detection of 235U in the oxide samples with this set-up is estimated to be 14mg.

Sanjay Andola; Ram Niranjan; T.C. Kaushik; R.K. Rout; Ashwani Kumar; D.B. Paranjape; Pradeep Kumar; B.S. Tomar; K.L. Ramakumar; S.C. Gupta

2014-01-01T23:59:59.000Z

484

High-resolution laser spectroscopy between 0.9 and 14.3 THz in a supersonic beam: Rydberg-Rydberg transitions of atomic Xe at intermediate n values  

SciTech Connect (OSTI)

A laser-based, pulsed, narrow-band source of submillimeter-wave radiation has been developed that is continuously tunable from 0.1 THz to 14.3 THz. The source is based on difference-frequency mixing in the nonlinear crystal trans-4{sup Prime }-(dimethylamino)-N-methyl-4-stilbazolium tosylate. By varying the pulse length, the bandwidth of the submillimeter-wave radiation can be adjusted between 85 MHz and 2.8 MHz. This new radiation source has been integrated in a vacuum-ultraviolet-submillimeter-ware double-resonance spectrometer, with which low-frequency transitions of atoms and molecules in supersonic beams can be detected mass-selectively by photoionization and time-of-flight mass spectrometry. The properties of the radiation source and spectrometer are demonstrated in a study of 33f Leftwards-Arrow nd Rydberg-Rydberg transitions in Xe with n in the range 16-31. The frequency calibration of the submillimeter-wave radiation was performed with an accuracy of 2.8 MHz. The narrowest lines observed experimentally have a full-width at half-maximum of {approx}3 MHz, which is sufficient to fully resolve the hyperfine structure of the Rydberg-Rydberg transitions of {sup 129}Xe and {sup 131}Xe. A total of 72 transitions were measured in the range between 0.937 THz and 14.245 THz and their frequencies are compared with frequencies calculated by multichannel quantum defect theory.

Haase, Christa; Agner, Josef A.; Merkt, Frederic [Laboratorium fuer Physikalische Chemie, ETH Zuerich, 8093 Zuerich (Switzerland)

2013-06-28T23:59:59.000Z

485

Speech feature encoding through an electrotactile speech processor Robert  

Science Journals Connector (OSTI)

Efficiency of speech feature encoding by the University of Melbourne multichannel electrotactile speech processor was assessed through performance of eight subjects on a closed?set tactual test battery. The battery consisted of 12 subtests each assessing discrimination of a particular speech feature in an ABX paradigm. All subjects scored significantly above chance on suprasegmental features such as syllable number stress and vowel length. Discrimination of vowelformant contrasts was significantly above chance for seven subjects. Discrimination of consonant manner varied across specific subtest contrasts with better encoding of the high?frequency fricatives and affricates. Discrimination of initial voicing contrasts suggested that tactual encoding of this feature could be improved. Comparison of these results with test battery scores from five different subjects with five commercially available tactile devices showed superior encoding of vowelformant and manner contrasts by the Tickle Talker. Subsequent consonant confusion studies with two hearing?impaired adults one using tactual input in combination with lipreading and one in combination with aided residual hearing and lipreading confirmed that added tactual information reduced the proportion of manner confusions and to a lesser extent voicing confusions.

S. C. Cowan; Peter J. Blamey; Joseph I. Alcantara; Lesley A. Whitford; Graeme Clark; Geoff Plant

1989-01-01T23:59:59.000Z

486

Continuation of studies on thermoregulation of fish and turtles in thermally stressed habitats. Summary progress report, 1 October 1977-30 September 1980  

SciTech Connect (OSTI)

Biophysical-behavioral-ecological models have been completed to explain the behavioral thermoregulation of largemouth bass (Micropterus salmoides) and turtles (Chrysemys scripta). Steady state and time dependent mathematical models accurately predict the body temperatures of largemouth bass. Field experiments using multichannel radio transmitters have provided temperatures of several body compartments of free ranging bass in their natural habitat. Initial studies have been completed to describe the behavioral thermoregulation of bass in a reactor cooling reservoir. Energy budgets, fundamental climate spaces, and realized climate spaces have been completed for the turtle, C. scripta. We have described the behavioral thermoregulation of C. scripta in Par Pond, S.C. and have measured its movements, home ranges and population levels in heated and unheated arms of the reservoir. Operative environmental temperature is a good predictor of the basking behavior of this turtle. A new synthesis explained the evolution of thermoregulatory strategies among animals. Laboratory experiments clarified the effects of movement, diving and temperature on the blood flow of alligators. Other experiments defined the role of boundary layers in controlling the evaporation of water from the surfaces of turtles and alligators in still and moving air. Nutritional status may be an important factor affecting the thermoregulatory behavior of turtles.

Spotila, J.R.

1980-05-01T23:59:59.000Z

487

Density fluctuation measurements by far-forward collective scattering in the MST reversed-field pinch  

SciTech Connect (OSTI)

The multichannel polarimeter-interferometer system on the MST reversed-field pinch can be utilized to measure far-forward collective scattering from electron density fluctuations. The collective scattering system has 11 viewing chords with {approx}8 cm spacing. The source is a 432 {mu}m (694 GHz) far infrared laser and the scattered power is measured using a heterodyne detection scheme. Collective scattering provides a line-integrated measurement of fluctuations within the divergence of the probe beam covering wavenumber range: k{sub Up-Tack} < 1.3 cm{sup -1}, corresponding k{sub Up-Tack }{rho}{sub s} < 1.3 ({rho}{sub s} is the ion-sound Larmor radius), the region of primary interest for turbulent fluctuation-induced transport. The perpendicular wavenumber consists of toroidal, poloidal, and radial contributions, which vary with chord position. Coherent modes associated with tearing instabilities and neutral-beam driven fast particles are observed along with broadband turbulence at frequencies up to 500 kHz. Changes in frequency are consistent with a Doppler shift due to parallel plasma flow.

Ding, W. X.; Lin, L.; Brower, D. L. [Department of Physics and Astronomy, University of California Los Angeles, Los Angeles, California 90095 (United States); Duff, J. R.; Sarff, J. S. [Department of Physics, University of Wisconsin-Madison, Madison, Wisconsin 53706 (United States)

2012-10-15T23:59:59.000Z

488

Microchannel Reactor System for Catalytic Hydrogenation  

SciTech Connect (OSTI)

We successfully demonstrated a novel process intensification concept enabled by the development of microchannel reactors, for energy efficient catalytic hydrogenation reactions at moderate temperature, and pressure, and low solvent levels. We designed, fabricated, evaluated, and optimized a laboratory-scale microchannel reactor system for hydrogenation of onitroanisole and a proprietary BMS molecule. In the second phase of the program, as a prelude to full-scale commercialization, we designed and developed a fully-automated skid-mounted multichannel microreactor pilot plant system for multiphase reactions. The system is capable of processing 1 10 kg/h of liquid substrate, and an industrially relevant immiscible liquid-liquid was successfully demonstrated on the system. Our microreactor-based pilot plant is one-of-akind. We anticipate that this process intensification concept, if successfully demonstrated, will provide a paradigm-changing basis for replacing existing energy inefficient, cost ineffective, environmentally detrimental slurry semi-batch reactor-based manufacturing practiced in the pharmaceutical and fine chemicals industries.

Adeniyi Lawal; Woo Lee; Ron Besser; Donald Kientzler; Luke Achenie

2010-12-22T23:59:59.000Z

489

High-resolution Bent-crystal Spectrometer for the Ultra-soft X-ray Region  

DOE R&D Accomplishments [OSTI]

A multichannel vacuum Brag-crystal spectrometer has been developed for high-resolution measurements of the line emission from tokamak plasmas in the wavelength region between 4 and 25 angstrom. The spectrometer employs a bent crystal in Johann geometry and a microchannel-plate intensified photodiode array. The instrument is capable of measuring high-resolution spectra (lambda/..delta..lambda approx. 3000) with fast time resolution (4 msec per spectrum) and good spatial resolution (3 cm). The spectral bandwidth is ..delta..lambda/lambda{sub 0} = 8 angstrom. A simple tilt mechanism allows access to different wavelength intervals. In order to illustrate the utility of the new spectrometer, time- and space-resolved measurements of the n = 3 to n = 2 spectrum of selenium from the Princeton Large Torus tokamak plasmas are presented. The data are used to determine the plasma transport parameters and to infer the radial distribution of fluorinelike, neonlike, and sodiumlike ions of selenium in the plasma. The new ultra-soft x-ray spectrometer has thus enabled us to demonstrate the utility of high-resolution L-shell spectroscopy of neonlike ions as a fusion diagnostic.

Beiersdorfer, P.; von Goeler, S.; Bitter, M.; Hill, K. W.; Hulse, R. A.; Walling, R. S.

1988-10-00T23:59:59.000Z

490

Laser for high frequency modulated interferometry  

DOE Patents [OSTI]

A Stark-tuned laser operating in the 119 micron line of CH[sub 3]OH has an output power of several tens of milliwatts at 30 Watts of pump power while exhibiting a doublet splitting of about ten MHz with the application of a Stark field on the order of 500 volts/cm. This output power allows for use of the laser in a multi-channel interferometer, while its high operating frequency permits the interferometer to measure rapid electron density changes in a pellet injected or otherwise fueled plasma such as encountered in magnetic fusion devices. The laser includes a long far-infrared (FIR) pyrex resonator tube disposed within a cylindrical water jacket and incorporating charged electrodes for applying the Stark field to a gas confined therein. With the electrodes located within the resonator tube, the resonator tube walls are cooled by a flowing coolant without electrical breakdown in the coolant liquid during application of the Stark field. Wall cooling allows for substantially increased FIR output powers. Provision is made for introducing a buffer gas into the resonator tube for increasing laser output power and its operating bandwidth. 10 figures.

Mansfield, D.K.; Vocaturo, M.; Guttadora, L.J.

1991-07-23T23:59:59.000Z

491

Extractor configurations for a heavy ion fusion volume source  

SciTech Connect (OSTI)

In order for volume sources to deliver the current (e.g., 0.8 A of Ar{sup +} per module) and brightness necessary for heavy ion fusion (HIF), they must operate at high current density. Conventional extractor designs for 1 to 2 MeV run into voltage breakdown limitations and cannot easily produce the required current rise time (about one microsecond). We discuss two systems that can overcome these volume-extraction problems. Each uses multichannel preaccelerators followed by a single channel main accelerator. Fast beam switching is done in the low energy beamlet stages. A new design, utilizing concentric ring preaccelerators, was recently described for another application [2]. A more conventional design uses a large number of small round beamlets. In either case, the merging beamlets are angled toward the axis, a feature that dominates other focusing. By suitable adjustment of the individual angles, beam aberrations are reduced. Because of the high current density, the overall structure is compact. Emittance growth from merging of beamlets is calculated and scaling is discussed.

Anderson, O.A.

2004-08-30T23:59:59.000Z

492

Synchronisation of the LHC Betatron Coupling and Phase Advance Measurement System  

E-Print Network [OSTI]

The new LHC Diode ORbit and OScillation (DOROS) system will provide beam position readings with submicrometre resolution and at the same time will be able to perform measurements of local betatron coupling and beam phase advance with micrometre beam excitation. The oscillation sub-system employs gain-controlled RF amplifiers, shared with the orbit system, and followed by dedicated diode detectors to demodulate the beam oscillation signals into the kHz frequency range, subsequently digitized by multi-channel 24-bit ADCs. The digital signals are processed in each front-end with an FPGA and the results of reduced throughput are sent using an Ethernet protocol to a common concentrator, together with the orbit data. The phase advance calculation between multiple Beam Position Monitors (BPMs) requires that all DOROS front-ends have a common phase reference. This paper presents methods used to generate such a reference and to maintain a stable synchronous sampling on all system front-ends. The performance of the DOR...

Gasior, M

2014-01-01T23:59:59.000Z

493

Laser for high frequency modulated interferometry  

DOE Patents [OSTI]

A Stark-tuned laser operating in the 119 micron line of CH.sub.3 OH has an output power of several tens of milliwatts at 30 Watts of pump power while exhibiting a doublet splitting of about ten MHz with the application of a Stark field on the order of 500 volts/cm. This output power allows for use of the laser in a multi-channel interferometer, while its high operating frequency permits the interferometer to measure rapid electron density changes in a pellet injected or otherwise fueled plasma such as encountered in magnetic fusion devices. The laser includes a long far-infrared (FIR) pyrex resonator tube disposed within a cylindrical water jacket and incorporating charged electrodes for applying the Stark field to a gas confined therein. With the electrodes located within the resonator tube, the resonator tube walls are cooled by a flowing coolant without electrical breakdown in the coolant liquid during application of the Stark field. Wall cooling allows for substantially increased FIR output powers. Provision is made for introducing a buffer gas into the resonator tube for increasing laser output power and its operating bandwidth.

Mansfield, Dennis K. (E. Windsor, NJ); Vocaturo, Michael (Columbus, NJ); Guttadora, Lawrence J. (Iselin, NJ)

1991-01-01T23:59:59.000Z

494

Evidence for O+ and 1- Levels in U234 Populated in the One-Minute Beta Decay of Pa234  

Science Journals Connector (OSTI)

A directional correlation measurement has been performed on the 250-kev vs (751+795)-kev composite cascade in U234 following the 24-day beta decay of Th234 and the subsequent one-minute beta decay of Pa234. The "770"-kev (751+795 kev) composite photopeak spectrum coincident with the 250-kev gamma ray was displayed on a multichannel pulse-height analyzer for different positions of the scintillation counters. From these spectra the directional correlations between the 250-kev gamma ray and the lower and upper sides of the 770-kev composite line were measured. The results together with other measurements are consistent with assignments of multipolarity E1 to the 250-, 751-, and 795-kev gamma rays and spin and parity assignments 0+-1--2+ and 0+-1--0+ to the levels involved in the 250-751 kev and 250-795 kev gamma-gamma cascades, respectively. Thus new levels are proposed at 795 and 1046 kev with spin and parity 1- and 0+, respectively.

G. T. Wood

1960-09-15T23:59:59.000Z

495

Updated user`s guide for SAMMY: multilevel R-matrix fits to neutron data using Bayes` equation  

SciTech Connect (OSTI)

In 1980 the multilevel multichannel R-matrix code SAMMY was released for use in analysis of neutron data at the Oak Ridge Electron Linear Accelerator. Since that time, SAMMY has undergone significant modifications: (1) User-friendly options have been incorporated to streamline common operations and to protect a run from common user errors, (2) The Reich-Moore formalism has been extended to include an optional logarithmic parameterization of the external R-matrix, for which any or all parameters may be varied, (3) the ability to vary sample thickness, effective temperature, matching radius, and/or resolution-broadening parameters has been incorporated, (4) to avoid loss of information (i.e. computer round-off errors) between runs, the ``covariance file`` now includes precise values for al variables, (5) Unused but correlated variables may be included in the analysis. Because of these and earlier changes, the 1980 SAMMY manual is now hopelessly obsolete. This report is intended to be complete documentation for the current version of SAMMY. Its publication in looseleaf form will permit updates to the manual to be made concurrently with updates to the code itself, thus eliminating most of the time lag between update and documentation.

Larson, N.M.

1996-10-01T23:59:59.000Z

496

Density effect on newly identified high-n Rydberg series of krypton by a resonantly enhanced multiphoton ionization method  

Science Journals Connector (OSTI)

Four even-parity atomic series corresponding to transitions from the 5s[1/2]10 level to the (2P3/20)np,nf levels of krypton have been observed, using a resonant multistep two-color photoionization method. The energies of 7p[3/2]1, 7p[1/2]1, 7p[3/2]2, 7p[1/2]0, np[1/2]1, np[3/2]2, np[1/2]0, and nf[3/2]1,2 levels are determined and the principal quantum numbers are calculated for n up to 45, 32, 49, and 44, respectively. Strong spectral irregularities in intensity and position are analyzed with the help of Lu-Fano diagrams and multichannel quantum defect theory in the case of the most intense 5s[1/2]10?np[1/2]0 series. Density shift rates have the constant value of -7.4(2)10-19 cm-1/cm-3 for the s?p high-n series members, outside regions where irregularities are observed, in agreement with existing doped krypton data. A close agreement with the Fermi model is obtained for these high-n members of regular series. Departure from this agreement is found for members whose excited levels are mixed with 7p states. A clear relationship between the p?p admixture and shift rate decrease, in regions of irregularities, is demonstrated.

E. Audouard; P. Laporte; J.-L. Subtil; N. Damany; M. Pellarin

1990-06-01T23:59:59.000Z

497

RELAP5 Prediction of Transient Tests in the RD-14 Test Facility  

SciTech Connect (OSTI)

Although the RELAP5 computer code has been developed for best-estimate transient simulation of a pressurized water reactor and its associated systems, it could not assess the thermal-hydraulic behavior of a Canada deuterium uranium (CANDU) reactor adequately. However, some studies have been initiated to explore the applicability for simulating a large-break loss-of-coolant accident in CANDU reactors. In the present study, the small-reactor inlet header break test and the steam generator secondary-side depressurization test conducted in the RD-14 test facility were simulated with the RELAP5/MOD3.2.2 code to examine its extended capability for all the postulated transients and accidents in CANDU reactors. The results were compared with experimental data and those of the CATHENA code performed by Atomic Energy of Canada Limited.In the RELAP5 analyses, the heated sections in the facility were simulated as a multichannel with five pipe models, which have identical flow areas and hydraulic elevations, as well as a single-pipe model.The results of the small-reactor inlet header break and the steam generator secondary-side depressurization simulations predicted experimental data reasonably well. However, some discrepancies in the depressurization of the primary heat transport system after the header break and consequent time delay of the major phenomena were observed in the simulation of the small-reactor inlet header break test.

Lee, Sukho [Korea Institute of Nuclear Safety (Korea, Republic of); Kim, Manwoong [Korea Institute of Nuclear Safety (Korea, Republic of); Kim, Hho-Jung [Korea Institute of Nuclear Safety (Korea, Republic of); Lee, John C. [University of Michigan (United States)

2005-09-15T23:59:59.000Z

498

Is This the End of the Automobile Era?  

E-Print Network [OSTI]

Asian 53% 27% 47% #12;A Changing Workforce 50% 52% 54% 56% 58% 60% 62% 64% 66% 68% 70% '60 '70 '80 '90 Planning Today Planning Horizon All of these unknowns warrant a shift from prediction to preparation #12

Minnesota, University of

499

851 S.W. Sixth Avenue, Suite 1100 Steve Crow 503-222-5161 Portland, Oregon 97204-1348 Executive Director 800-452-5161  

E-Print Network [OSTI]

to Section 4(h)(12)(A) of the Northwest Power Act. The Council's bylaws, which include its organizational............................................................................................................. 9 Proving new energy-efficiency technologies.......................................................................... 9 Television energy efficiency

500

SUMMAR OF DISCUSSIONS OF USES OF THE ADVANCED LIGHT SOURCE (ALS) FOR EARTH SCIENCES RESEARCH: WORKSHOP REPORT OF THE ALS USERS' ASSOCIATION ANNUAL MEETING, LAWRENCE BERKELEY LABORATORY, BERKELEY,CA, JUNE 2-3, 1988  

E-Print Network [OSTI]

in the Earth Sciences: Argonne National Workshop Report",V. Smith and M. H. Manghnani, Argonne National Laboratories,of a workshop held at Argonne National Laboratory (12). A

Dillard, J.; Wallenberg, H.; Perry, D.

2008-01-01T23:59:59.000Z