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1

b002.dvi  

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

15 GOPAL 80 DPWA K N K N 1955 15 GOPAL 77 DPWA K N multichannel 1755 or 1834 1 MARTIN 77 DPWA K N multichannel 2004 40 VANHORN 75 DPWA K - p 0 (2000) WIDTH...

2

MULTICHANNEL ANALYZER  

DOE Patents (OSTI)

A multichannel pulse analyzer having several window amplifiers, each amplifier serving one group of channels, with a single fast pulse-lengthener and a single novel interrogation circuit serving all channels is described. A pulse followed too closely timewise by another pulse is disregarded by the interrogation circuit to prevent errors due to pulse pileup. The window amplifiers are connected to the pulse lengthener output, rather than the linear amplifier output, so need not have the fast response characteristic formerly required.

Kelley, G.G.

1959-11-10T23:59:59.000Z

3

b079.dvi  

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

78 DPWA K N K N 1676 15 GOPAL 77 DPWA K N multichannel 1668 25 VANHORN 75 DPWA K - p 0 1670 20 KANE 74 DPWA K - p * * * We do not use the...

4

b144.dvi  

NLE Websites -- All DOE Office Websites (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

5

Essays on multichannel marketing  

E-Print Network (OSTI)

Multichannel marketing is the practice of simultaneously offering information, goods, services, and support to customers through two or more synchronized channels. In this dissertation, I develop an integrated framework of multichannel marketing and develop models to assist managers in their marketing resource allocation decisions. In the first essay of the dissertation, I investigate the factors that drive customers multichannel shopping behavior and identify its consequences for retailers. In the second essay, I build on this work and develop a model that enables firms to optimize their allocation of marketing resources across different customer-channel segments. In the first essay, I develop a framework comprising the factors that drive consumers channel choice, the consequences of channel choice, and their implications for managing channel equity. The results show that customer-channel choice is driven in a nonlinear fashion by a customer demographic variable such as age and is also influenced by consumer shopping traits such as number of categories bought and the duration of relationship with a retailer. I show that by controlling for the moderating effects of channel-category associations, the influence of customers demographics and shopping traits on their channel choices can vary significantly across product categories. Importantly, the results show that multichannel shoppers buy more often, buy more items, and spend considerably more than single channel shoppers. The channel equity of multichannel customers is nearly twice that of the closest single channel customers (online or offline). In the second essay, I propose a model for optimal allocation of marketing efforts across multiple customer-channel segments. I first develop a set of models for consumer response to marketing efforts for each channel-customer segment. This set comprises four models, the first for purchase frequency, the second for purchase quantity, the third for product return behavior, and the fourth for contribution margin of purchase. The results show that customers responses to firm marketing efforts vary significantly across the customer-channel segments. They also suggest that marketing efforts influence purchase frequency, purchase quantity and monetary value in different ways. The resource allocation results show that profits can be substantially improved by reallocating marketing efforts across the different customer-channel segments.

Kushwaha, Tarun Lalbahadur

2007-08-01T23:59:59.000Z

6

Fractional channel multichannel analyzer  

DOE Patents (OSTI)

A multichannel analyzer incorporating the features of the present invention obtains the effect of fractional channels thus greatly reducing the number of actual channels necessary to record complex line spectra. This is accomplished by using an analog-to-digital converter in the asynchronous mode, i.e., the gate pulse from the pulse height-to-pulse width converter is not synchronized with the signal from a clock oscillator. This saves power and reduces the number of components required on the board to achieve the effect of radically expanding the number of channels without changing the circuit board. 9 figs.

Brackenbush, L.W.; Anderson, G.A.

1994-08-23T23:59:59.000Z

7

Multichannel optical sensing device  

DOE Patents (OSTI)

A multichannel optical sensing device is disclosed, for measuring the outr sky luminance or illuminance or the luminance or illuminance distribution in a room, comprising a plurality of light receptors, an optical shutter matrix including a plurality of liquid crystal optical shutter elements operable by electrical control signals between light transmitting and light stopping conditions, fiber optic elements connected between the receptors and the shutter elements, a microprocessor based programmable control unit for selectively supplying control signals to the optical shutter elements in a programmable sequence, a photodetector including an optical integrating spherical chamber having an input port for receiving the light from the shutter matrix and at least one detector element in the spherical chamber for producing output signals corresponding to the light, and output units for utilizing the output signals including a storage unit having a control connection to the microprocessor based programmable control unit for storing the output signals under the sequence control of the programmable control unit.

Selkowitz, Stephen E. (Piedmont, CA)

1990-01-01T23:59:59.000Z

8

b087.dvi  

NLE Websites -- All DOE Office Websites (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

9

b087.dvi  

NLE Websites -- All DOE Office Websites (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)

10

b005.dvi  

NLE Websites -- All DOE Office Websites (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

11

b063.dvi  

NLE Websites -- All DOE Office Websites (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

12

b066.dvi  

NLE Websites -- All DOE Office Websites (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

13

b064.dvi  

NLE Websites -- All DOE Office Websites (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

14

b061.dvi  

NLE Websites -- All DOE Office Websites (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

15

Consumer behaviour at multi-channel retailers  

E-Print Network (OSTI)

Consumer behaviour at pure Internet players has been analysed thoroughly in earlier work. When it comes to retailers with multiple distribution channels, however, new behaviour patterns can be observed. Given the fact that multi-channel retailing is much more common than Internet-only, the analysis of consumer behaviour in a multi-channel context constitutes a challenge for the deeper understanding of e-business. The contribution of this research is threefold: first, this study provides an overview of how the 50 largest e-retailers presently coordinate the interaction between sales on their web sites and in physical stores. Second, we present findings from a consumer survey suggesting what consumers like about multi-channel services on retail sites. Finally, user behaviour is empirically evaluated based on transaction and web log data from a large multi-channel retailer. The results indicate a strong demand for multi-channel services and suggest that retailers should expand their multi-channel service spectrum.

Maximilian Teltzrow; Bettina Berendt; Oliver Gnther

2003-01-01T23:59:59.000Z

16

b001.dvi  

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

ESTIMATE 1840 OUR ESTIMATE 1840 OUR ESTIMATE UNCHECKED 1798 or 1802 1 MARTIN 77 DPWA K N multichannel 1720 30 2 BAILLON 75 IPWA K N 1925 200...

17

b015.dvi  

NLE Websites -- All DOE Office Websites (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

18

b012.dvi  

NLE Websites -- All DOE Office Websites (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

19

Multichannel baseband processor for wideband CDMA  

Science Conference Proceedings (OSTI)

The system architecture of the cellular base station modem engine (CBME) is described. The CBME is a single-chip multichannel transceiver capable of processing and demodulating signals from multiple users simultaneously. It is optimized to process different ... Keywords: CDMA, RAKE, chip-rate processing, micro-DSP, multipath, symbol-rate processing

Louay M. A. Jalloul; Jim Lin

2005-01-01T23:59:59.000Z

20

Multi-channel neutral analyzer-system  

DOE Green Energy (OSTI)

Design and calibration of a 15 channel multi-channel analyzer for analysis of energetic neutral particles escaping a hot plasma are discussed. Features of the analyzer include a frequency response from DC to 50 kHz, spatial resolution, mass resolution, and data acquisition and processing for 15 points on the energy distribution that are simultaneously recorded. Another feature of the system is the ability to radially scan the plasma. An rf ion source is used to provide ions and neutrals used for calibration of a reference single channel analyzer. This analyzer is, in turn, used to calibrate the multi-channel analyzer over the energy range 500 eV to 40 keV. A brief description of the data processing system is included. (RME)

Nexsen, Jr., W. E.; Turner, W. C.; Cummins, W. F.

1977-09-14T23:59:59.000Z

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.


21

An efficient multi-channel wireless switching system  

E-Print Network (OSTI)

the scheduling operation in wireless switching systems. Thefor the local operation between a wireless switch port andoperations in interference-rich multi-channel wireless

Shim, Jaewook

2010-01-01T23:59:59.000Z

22

A theoretical framework to characterize multichannel interaction in electronic commerce  

Science Conference Proceedings (OSTI)

This paper presents an initial study of multichannel interactions within the framework of the E-Marketing. A analysis and prediction theoretical framework, based on the one hand on concepts resulting from psycholinguistics, and the other hand on information ... Keywords: E-marketing, interaction, media richness theory, multichannel, psycholinguistics

Vincent Chevrin; Alain Derycke; Jos Rouillard

2003-11-01T23:59:59.000Z

23

b139.dvi  

NLE Websites -- All DOE Office Websites (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

24

b009.dvi  

NLE Websites -- All DOE Office Websites (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

25

b113.dvi  

NLE Websites -- All DOE Office Websites (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

26

b113.dvi  

NLE Websites -- All DOE Office Websites (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

27

b071.dvi  

NLE Websites -- All DOE Office Websites (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

28

b011.dvi  

NLE Websites -- All DOE Office Websites (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

29

The Multi-Channel Infrared Sea Truth Radiometric Calibrator (MISTRC)  

Science Conference Proceedings (OSTI)

A new multichannel infrared sea truth radiometer has been designed and built to improve validation of satellite-determined sea surface temperature. Horizontal grid polarized filters installed on the shortwave channels are very effective in ...

M. J. Suarez; W. J. Emery; G. A. Wick

1997-04-01T23:59:59.000Z

30

b040.dvi  

NLE Websites -- All DOE Office Websites (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.

31

b040.dvi  

NLE Websites -- All DOE Office Websites (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

32

On optimal feedback allocation in multichannel wireless downlinks  

Science Conference Proceedings (OSTI)

This paper studies feedback resource allocation in the downlink of a Frequency Division Duplex (FDD) multichannel wireless system. We consider a downlink network with a single base station, L shared channels and N mobile users. Throughput ... Keywords: downlink scheduling, limited feedback, throughput optimality

Ming Ouyang; Lei Ying

2010-09-01T23:59:59.000Z

33

Recent advances in Multi-Channel Algebraic Scattering  

SciTech Connect

For coupled-channel descriptions of low-energy nucleon-induced interactions involving nuclei with particle-unstable exited states, it is necessary to include the widths of the target states. How those widths may affect the elastic scattering cross sections is examined within the framework of the Multi-Channel Algebraic Scattering (MCAS) method.

Karataglidis, S. [Department of Physics, University of Johannesburg, P.O. Box 524, Auckland Park, 2006 (South Africa); Fraser, P. R. [Instituto de Ciencias Nucleares, Universidad Nacional Autonoma de Mexico, 04150, Mexico, D.F. (Mexico); Amos, K. [School of Physics, University of Melbourne, Victoria, 3010 (Australia); Canton, L.; Pisent, G. [Istituto Nazionale di Fisica Nucleare, Sezione di Padova, I-35131 (Italy); Svenne, J. P. [Department of Physics and Astronomy, University of Manitoba, Winnipeg, Manitoba, R3T 2N2 (Canada); Knijff, D. van der [Advanced Research Computing, Information Division, University of Melbourne, Victoria, 3010 (Australia)

2011-10-28T23:59:59.000Z

34

Scanning multichannel microwave radiometer snow water equivalent assimilation  

E-Print Network (OSTI)

climatic driver through the surface albedo's role in energy and water budgets [e.g., Yeh et al., 1983Scanning multichannel microwave radiometer snow water equivalent assimilation Jiarui Dong,1 due to complicating effects, including distance to open water, presence of wet snow, and presence

Houser, Paul R.

35

b067.dvi  

NLE Websites -- All DOE Office Websites (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

36

b067.dvi  

NLE Websites -- All DOE Office Websites (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)

37

b016.dvi  

NLE Websites -- All DOE Office Websites (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

38

b016.dvi  

NLE Websites -- All DOE Office Websites (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,

39

b001.dvi  

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

1840 OUR ESTIMATE 1840 OUR ESTIMATE 1840 OUR ESTIMATE 1798 or 1802 1 MARTIN 77 DPWA K N multichannel 1720 30 2 BAILLON 75 IPWA K N 1925 200 VANHORN...

40

b036.dvi  

NLE Websites -- All DOE Office Websites (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

Note: This page contains sample records for the topic "12a dpwa multichannel" from the National Library of EnergyBeta (NLEBeta).
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41

b036.dvi  

NLE Websites -- All DOE Office Websites (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

42

b055.dvi  

NLE Websites -- All DOE Office Websites (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

43

b055.dvi  

NLE Websites -- All DOE Office Websites (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

44

b024.dvi  

NLE Websites -- All DOE Office Websites (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±

45

An Efficient Multi-Channel MAC Protocol for Mobile Ad Hoc Networks  

Science Conference Proceedings (OSTI)

This paper proposes a novel multi-channel MAC protocol for mobile ad hoc networks that enables the nodes to transmit packets in distributed channels. In our protocol, the ATIM window is divided into two windows. The first window is called deciding channel ... Keywords: Ad hoc network, media access control (MAC), multi-channel

Wen-Hwa Liao; Wen-Chin Chung

2009-01-01T23:59:59.000Z

46

AOCS Official Method Ca 12a-02  

Science Conference Proceedings (OSTI)

Colorimetric Determination of Phosphorus Content in Fats and Oils AOCS Official Method Ca 12a-02 Methods Methods and Analyses Analytical Chemistry Methods Downloads Methods Downloads DEFINITION The test portion

47

b117.dvi  

NLE Websites -- All DOE Office Websites (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

48

b014.dvi  

NLE Websites -- All DOE Office Websites (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±

49

Multi-channel gas electron multiplier with metallic electrodes  

E-Print Network (OSTI)

The design of multi-channel gas electron multiplier (MGEM) with metallic electrodes is proposed, produced and tested. The electrodes of MGEM are produced from the brass plates with thickness of 1 mm, round openings of 1 mm in diameter and 1.5 mm steps between them. The gap between the electrodes is equal to 3 mm, while the total working area has a diameter of 20 mm. The neon gas fillings of the MWGEM chamber with micro admixtures of N_2 and H_2O have been tested. The total maximal coefficient of proportional multiplication of electrons in neon with admixture of (H_2O+N_2)<100 ppm of 30000 is obtained.

B. M. Ovchinnikov; V. V. Parusov; Yu. B. Ovchinnikov

2010-06-15T23:59:59.000Z

50

A scalable, fast and multichannel arbitrary waveform generator  

E-Print Network (OSTI)

This article reports on development of a multichannel arbitrary waveform generator (MAWG), which simultaneously generates arbitrary voltage waveforms on 24 independent channels with a dynamic update rate of up to 25 Msps. A real-time execution of a single waveform and/or sequence of multiple waveforms in succession, with a user programmable arbitrary sequence order is provided under the control of a stand-alone sequencer circuit implemented using an FPGA. The device is operated using an internal clock and can be synced to other devices by means of the TTL pulses. The device can be used for output voltages in the range of up to +-9 V with a drift rate below +-10 uV/min and a maximum deviation less than +- 300 uVpp over a period of two hours.

Baig, Muhammad Tanveer; Wiese, Andreas; Heidbrink, Stefan; Ziolkowski, Michael; Wunderlich, Christof

2013-01-01T23:59:59.000Z

51

A scalable, fast and multichannel arbitrary waveform generator  

E-Print Network (OSTI)

This article reports on development of a multichannel arbitrary waveform generator (MAWG), which simultaneously generates arbitrary voltage waveforms on 24 independent channels with a dynamic update rate of up to 25 Msps. A real-time execution of a single waveform and/or sequence of multiple waveforms in succession, with a user programmable arbitrary sequence order is provided under the control of a stand-alone sequencer circuit implemented using an FPGA. The device is operated using an internal clock and can be synced to other devices by means of the TTL pulses. The device can be used for output voltages in the range of up to +-9 V with a drift rate below +-10 uV/min and a maximum deviation less than +-300 uVpp over a period of two hours.

Muhammad Tanveer Baig; Michael Johanning; Andreas Wiese; Stefan Heidbrink; Michael Ziolkowski; Christof Wunderlich

2013-07-22T23:59:59.000Z

52

Nonlinear Multichannel Algorithms for Estimating Sea Surface Temperature with AVHRR Satellite Data  

Science Conference Proceedings (OSTI)

The familiar linear multichannel sea surface temperature algorithms (MCSST) for estimating sea surface temperature with AVHRR satellite data describe the solution in terms of a constant gamma parameter multiplied by the measured brightness ...

Charles C. Walton

1988-02-01T23:59:59.000Z

53

A Multichannel Cloud Pyranometer System for Airborne Measurement of Solar Spectral Reflectance by Clouds  

Science Conference Proceedings (OSTI)

The design and performance of a spectral radiometer system are described for airborne measurements of solar flux reflectance by clouds. The system consists of a pair of identical multichannel pyranometers: one installed on the top and the other ...

Shoji Asano; Masataka Shiobara; Yuji Nakanishi; Yukiharu Miyake

1995-06-01T23:59:59.000Z

54

Correlations between Nimbus-7 Scanning Multichannel Microwave Radiometer Data and an Antecedent Precipitation Index  

Science Conference Proceedings (OSTI)

Passive microwave brightness temperatures from the Nimbus-7 Scanning Multichannel Microwave Radiometer (SMMR) can be used to infer the soil moisture content over agricultural areas such as the southern Great Plains of the United States. A linear ...

Gregory D. Wilke; Marshall J. McFarland

1986-02-01T23:59:59.000Z

55

b044.dvi  

NLE Websites -- All DOE Office Websites (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

56

b145.dvi  

NLE Websites -- All DOE Office Websites (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

57

Multichannel Sampling of Pulse Streams at the Rate of Innovation  

E-Print Network (OSTI)

We consider minimal-rate sampling schemes for streams of delayed and weighted versions of a known pulse shape. Such signals belong to the class of finite rate of innovation (FRI) models. The minimal sampling rate for these parametric signals, is the number of degrees of freedom per unit of time, referred to as the rate of innovation. Although sampling of pulse streams was treated in previous works, either the rate of innovation was not achieved, or the pulse shape was limited to diracs and the method was instable for high rates of innovation. In this work we propose a multichannel framework for pulse streams with arbitrary shape, operating at the rate of innovation. Our approach is based on modulating the input signal with a set of properly chosen waveforms, followed by a bank of integrators. We show that the pulse stream can be recovered from the proposed minimal-rate samples using standard tools taken from spectral estimation in a stable way even at high rates of innovation. In addition, we address practica...

Gedalyahu, Kfir; Eldar, Yonina C

2010-01-01T23:59:59.000Z

58

Determination of total ozone from DMSP multichannel filter radiometer measurements  

Science Conference Proceedings (OSTI)

The multichannel filter radiometer (MFR) infrared sensor was first flown in 1977 on a Defense Meteorological Satellite Program (DMSP) Block 5D series satellite operated by the US Air Force. The first four satellites in this series carried MFR sensors from which total atmospheric column ozone amounts may be derived. The last MFR sensor ceased operating on February 16, 1980. The series of four sensors spans a data period of nearly three years. The MFR sensor measures infrared radiances for 16 channels. Total ozone amounts are determined from sets of radiance measurements using an empirical relationship that is developed using linear regression analysis. Total ozone is modeled as a linear combination of terms involving functions of the MFR radiances for four channels (1, 3, 7 and 16) and the secant of the zenith angle. The ozone retrieval methodology is described schematically. The ozone retrieval model is developed through regression analysis using sets of simulated MFR radiances derived from detailed radiative transfer calculations. The MFR total ozone data are compared with independent ground-based Dobson measurements in order to evaluate the ozone retrieval methodology. Many Dobson observatories have been providing their daily measurements of total ozone which are taken close in time to DMSP overpass times. MFR total ozone data are compared with Dobson measurements taken between January 1 and February 15, 1979, and the results are summarized. Comparisons were made where the MFR and Dobson measurements are within 300 km and 300 minutes of each other. Percentages are computed with respect to the Dobson values. The MFR data were processed using a preliminary methodology, and the data will be reprocessed in the near future.

Luther, F.M.; Weichel, R.L.

1980-09-01T23:59:59.000Z

59

Resolution Enhancement of Multichannel Microwave Imagery from the Nimbus-7 SMMR for Maritime Rainfall Analysis  

Science Conference Proceedings (OSTI)

A restoration of the 37, 21, 18, 10.7 and 6.6 GHz satellite imagery from the Scanning Multichannel Microwave Radiometer (SMMR) aboard Nimbus-7 to 22.2 km resolution is attempted using a deconvolution method based upon nonlinear programming. The ...

William S. Olson; Chia-Lung Yeh; James A. Weinman; Roland T. Chin

1986-09-01T23:59:59.000Z

60

Optimal monitoring in multi-channel multi-radio wireless mesh networks  

Science Conference Proceedings (OSTI)

Wireless mesh networks (WMN) are finding increasing usage in city-wide deployments for providing network connectivity. Mesh routers in WMNs typically use multiple wireless channels to enhance the spatial-reuse of frequency bands, often with multiple ... Keywords: approximation algorithm, lp rounding, multi-channel multi-radio wireless networks, security monitoring, wireless mesh networks

Dong-Hoon Shin; Saurabh Bagchi

2009-05-01T23:59:59.000Z

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While these samples are representative of the content of NLEBeta,
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61

Handling Triple Hidden Terminal Problems for Multi-Channel MAC in Long-Delay Underwater  

E-Print Network (OSTI)

1 Handling Triple Hidden Terminal Problems for Multi-Channel MAC in Long-Delay Underwater Sensor-channel MAC problem in underwater acoustic sensor networks. To reduce hardware cost, only one acoustic transceiver is often preferred on every node. In a single-transceiver multi- channel long-delay underwater

Cui, Jun-Hong

62

Channel Selection in Multi-channel Opportunistic Spectrum Access Networks with  

E-Print Network (OSTI)

Channel Selection in Multi-channel Opportunistic Spectrum Access Networks with Perfect Sensing Xin and utilized by primary users (PU). In dynamic spectrum access networks, the protection of PU's is vital, since no PU would accommo- date SU access to its own detriment. Therefore the objective of the problem we

Liu, Xin

63

A low-power, multichannel gated oscillator-based CDR for short-haul applications  

Science Conference Proceedings (OSTI)

A gated current-controlled oscillator (GCCO) based topology is used to implement a low-power multi-channel clock and data recovery (CDR) system in a 0.18um digital CMOS technology. A systematic approach is presented to design a reliable and low-power ...

Armin Tajalli; Paul Muller; Mojtaba Atarodi; Yusuf Leblebici

2005-08-01T23:59:59.000Z

64

b065.dvi  

NLE Websites -- All DOE Office Websites (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,

65

b011.dvi  

NLE Websites -- All DOE Office Websites (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

66

b013.dvi  

NLE Websites -- All DOE Office Websites (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

67

b061.dvi  

NLE Websites -- All DOE Office Websites (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

68

b015.dvi  

NLE Websites -- All DOE Office Websites (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

69

b033.dvi  

NLE Websites -- All DOE Office Websites (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

70

b066.dvi  

NLE Websites -- All DOE Office Websites (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

71

b064.dvi  

NLE Websites -- All DOE Office Websites (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,

72

b063.dvi  

NLE Websites -- All DOE Office Websites (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. *

73

b012.dvi  

NLE Websites -- All DOE Office Websites (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. * * *

74

b062.dvi  

NLE Websites -- All DOE Office Websites (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

75

b071.dvi  

NLE Websites -- All DOE Office Websites (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,

76

b010.dvi  

NLE Websites -- All DOE Office Websites (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,

77

Calibration of a Multichannel Water Vapor Raman Lidar through Noncollocated Operational Soundings: Optimization and Characterization of Accuracy and Variability  

Science Conference Proceedings (OSTI)

This paper presents a parametric automatic procedure to calibrate the multichannel RayleighMieRaman lidar at the Institute for Atmospheric Science and Climate of the Italian National Research Council (ISAC-CNR) in Tor Vergata, Rome, Italy, ...

Davide Dionisi; Fernando Congeduti; Gian Luigi Liberti; Francesco Cardillo

2010-01-01T23:59:59.000Z

78

Toward the Quantum Design of Multichannel Systems (The Inverse Problem Approach)  

E-Print Network (OSTI)

The multichannel generalization of the theory of spectral, scattering and decay control is presented. New universal algorithms of construction of complex quantum systems with given properties are suggested. Particularly, transformations of interaction matrices leading to the concentration of waves in a chosen partial channel and spatial localization are shown. The limiting instructive cases illustrating different phenomena which occur with the combination of 'incompatible' properties are considered. For example, the scattering solutions with different resonance widths at the same energy for the same interaction are revealed. Analogously, a 'paradoxical' coexistence of both strong reflection and absolute transparency is explained. The case of the violation of 'natural' asymptotic behavior of partial wave function is demonstrated : it has a greater damping decrement for the channel with a lower threshold. Peculiarities of the multichannel periodic structures, bound states embedded into continuum, resonance tunneling and degeneracy of states are described.

V. M. Chabanov; B. N. Zakhariev; I. V. Amirkhanov

2001-03-30T23:59:59.000Z

79

Toward the Quantum Design of Multichannel Systems (The Inverse Problem Approach)  

E-Print Network (OSTI)

The multichannel generalization of the theory of spectral, scattering and decay control is presented. New universal algorithms of construction of complex quantum systems with given properties are suggested. Particularly, transformations of interaction matrices leading to the concentration of waves in a chosen partial channel and spatial localization are shown. The limiting instructive cases illustrating different phenomena which occur with the combination of 'incompatible' properties are considered. For example, the scattering solutions with different resonance widths at the same energy for the same interaction are revealed. Analogously, a 'paradoxical' coexistence of both strong reflection and absolute transparency is explained. The case of the violation of 'natural' asymptotic behavior of partial wave function is demonstrated : it has a greater damping decrement for the channel with a lower threshold. Peculiarities of the multichannel periodic structures, bound states embedded into continuum, resonance tunn...

Chabanov, V M; Amirkhanov, I V

2000-01-01T23:59:59.000Z

80

Multi-channel scattering problems: Analytical approach for exact solution using Green's functions  

E-Print Network (OSTI)

We have proposed an analytical approach for exact solution of multi-channel scattering problems, in presence of Dirac Delta function couplings. Our solution is quite general and is valid for any set of potentials, if the Green's functions of the uncoupled potentials are known at the crossing point. Using our model, it is possible to express N-channel problem by N independent `single' channel problems and hence one can have a realistic solution of multi-channel scattering problem. In this paper we have shown that transition probability from first diabatic potential to any other potential can be easily evaluated using a very simple analytical formula - which only require value of eigenfunction of first uncoupled potential and value of Green's function of other uncoupled potential, at the crossing.

Diwaker; Aniruddha Chakraborty

2013-08-04T23:59:59.000Z

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

Development of refined MCNPX-PARET multi-channel model for transient analysis in research reactors  

SciTech Connect

Reactivity insertion transients are often analyzed (RELAP, PARET) using a two-channel model, representing the hot assembly with specified power distribution and an average assembly representing the remainder of the core. For the analysis of protected by the reactor safety system transients and zero reactivity feedback coefficients this approximation proves to give adequate results. However, a more refined multi-channel model representing the various assemblies, coupled through the reactivity feedback effects to the whole reactor core is needed for the analysis of unprotected transients with excluded over power and period trips. In the present paper a detailed multi-channel PARET model has been developed which describes the reactor core in different clusters representing typical BR2 fuel assemblies. The distribution of power and reactivity feedback in each cluster of the reactor core is obtained from a best-estimate MCNPX calculation using the whole core geometry model of the BR2 reactor. The sensitivity of the reactor response to power, temperature and energy distributions is studied for protected and unprotected reactivity insertion transients, with zero and non-zero reactivity feedback coefficients. The detailed multi-channel model is compared vs. simplified fewer-channel models. The sensitivities of transient characteristics derived from the different models are tested on a few reactivity insertion transients with reactivity feedback from coolant temperature and density change. (authors)

Kalcheva, S.; Koonen, E. [SCK-CEN, BR2 Reactor Dept., Boeretang 200, 2400 Mol (Belgium); Olson, A. P. [RERTR Program, Nuclear Engineering Div., Argonne National Laboratory, Cass Avenue, Argonne, IL 60439 (United States)

2012-07-01T23:59:59.000Z

82

Development of a multichannel analysis code for the MITR-III safety analysis  

SciTech Connect

This paper describes the development of a MULti-CHannel analysis (MULCH-II) code to be used for the safety analysis of the Massachusetts Institute of Technology Research Reactor (MITR). The code models the primary and the secondary coolant systems with special emphasis on analysis of detailed thermal-hydraulic conditions in the core region. The hot channel is modeled in parallel with the average channels to predict conditions in the core during a flow excursion instability. Fuel and cladding temperatures are calculated under all conditions so that the margin to fuel failure is given in addition to the thermal-hydraulic conditions.

Hu, Lin-Wen; Bernard, J.A. [Massachusetts Inst. of Technology, Cambridge, MA (United States)

1996-12-31T23:59:59.000Z

83

Support vector machine in novelty detection for multi-channel combustion data  

E-Print Network (OSTI)

Abstract. Multi-channel combustion data, consisting of gas pressure and two combustion chamber luminosity measurements, are investigated in the prediction of combustion instability. Wavelet analysis is used for feature extraction. A SVM approach is applied for novelty detection and the construction of a model of normal system operation. Novelty scores generated by classifiers from different channels are combined to give a final decision of data novelty. Comparisons between the proposed SVM method and a GMM approach show that earlier identification of combustion instability, and greater distinction between stable and unstable data classes, are achieved with the proposed SVM approach. 1

Lei A. Clifton; Hujun Yin; Yang Zhang

2006-01-01T23:59:59.000Z

84

Direct experimental measurement of SRS-induced spectral tilt in multichannel multispan communication systems  

SciTech Connect

Nonlinear SRS-induced tilt of the spectrum of a multichannel DWDM signal is studied experimentally in standard singlemode fibreoptic communication lines. It is found that at a fixed spectral bandwidth and total power the nonlinear SRS tilt is independent of the number of channels, radiation source type, and the initial tilt (positive or negative). In a multispan line consisting of identical spans the total nonlinear tilt of the spectrum (in dB) is proportional to the number of spans, spectral width and total power. (optical fibres, lasers and amplifiers. properties and applications)

Kapin, Yu A; Nanii, Oleg E; Novikov, A G; Pavlov, V N; Plotskii, A Yu; Treshchikov, V N

2012-09-30T23:59:59.000Z

85

b060.dvi  

NLE Websites -- All DOE Office Websites (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

86

Multichannel transition emissions of Dy{sup 3+} in fiber-adaptive germanium tellurite glasses  

SciTech Connect

Multichannel transition visible and near-infrared (NIR) fluorescences have been captured in Dy{sup 3+}-doped fiber-adaptive Na{sub 2}O-ZnO-PbO-GeO{sub 2}-TeO{sub 2} glasses. The maximum stimulated emission cross-sections {sigma}{sub em-max} were derived to be 0.33 Multiplication-Sign 10{sup -21}, 3.66 Multiplication-Sign 10{sup -21}, and 0.67 Multiplication-Sign 10{sup -21} cm{sup 2} for conventional visible emissions assigned to {sup 4}F{sub 9/2}{yields}{sup 6}H{sub J} (J = 15/2, 13/2, and 11/2) transitions, respectively. Infrequent multi-peak NIR emissions were recorded in the spectral range of 900-1500 nm, among which the values of {sigma}{sub em-max} were solved to be 1.05 Multiplication-Sign 10{sup -22} and 1.56 Multiplication-Sign 10{sup -22} cm{sup 2} for {approx}1.02 and {approx}1.18 {mu}m emission bands. Internal quantum efficiency for the {sup 4}F{sub 9/2} level and external quantum yield for visible emissions of Dy{sup 3+} were determined to be 88.44% and 12.38%, severally. Effective multichannel radiative emissions reveal a potential in developing fiber-lighting sources, tunable lasers, and NIR optical amplifiers.

Li, Y. H.; Chen, B. J.; Lin, H. [School of Textile and Material Engineering, Dalian Polytechnic University, Dalian 116034 (China); Department of Electronic Engineering, City University of Hong Kong, Tat Chee Avenue, Kowloon, Hong Kong (China); Pun, E. Y. B. [Department of Electronic Engineering, City University of Hong Kong, Tat Chee Avenue, Kowloon, Hong Kong (China)

2013-03-28T23:59:59.000Z

87

Multi-Channel Transfer Function with Dimensionality Han Suk Kima, c, Jurgen P. Schulzeb, Angela C. Conec,  

E-Print Network (OSTI)

compromising visualization accuracy. In this publication we report on the impact of the dimensionality, Transfer Function, Multi-Channel Volume, Light Microscopy Imaging, Dimen- sionality Reduction 1 ABSTRACT The design of transfer functions for volume rendering is a difficult task. This is particularly

Schulze, Jürgen P.

88

Rate-adaption channel assignment and routing algorithm for multi-channel wirelessMAN mesh networks  

Science Conference Proceedings (OSTI)

Wireless mesh networks provide an easy deployed and extensible solution to access Internet or communicate with each other for both enterprises and individuals. With the help of multi-channel and multi-radio, wireless mesh network can support more traffic ... Keywords: IEEE 802.16, channel assignment, rate-adaption, routing, wireless mesh network

Eric Hsiao-Kuang Wu; Wei-Li Chang; Hsuan-Hao Chan

2007-07-01T23:59:59.000Z

89

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

90

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.

VanDeusen, Alan L. (Lee' s Summit, MO); Crist, Charles E. (Waxahachie, TX)

1995-09-26T23:59:59.000Z

91

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

92

Impact of elliptical cross-section on the propagation delay of multi-channel gate-all-around MOSFET based inverters  

Science Conference Proceedings (OSTI)

Multi-channel (MC) gate-all-around (GAA) metal-oxide-semiconductor field-effect transistor (MOSFET) is one of the promising candidates for the next-generation high performance devices. However, due to fabrication imperfections the cross-section of GAA ... Keywords: Effective diameter, Gate-all-around (GAA), Metal-oxide-semiconductor field-effect transistor (MOSFET), Multi-channel, Propagation delay, Scaling

Subindu Kumar, Shankaranand Jha

2013-09-01T23:59:59.000Z

93

Multi-channel transmission with efficient delivery of routing information in maritime WiMAX mesh networks  

Science Conference Proceedings (OSTI)

There is a lack of broadband wireless network in sea to meet the increasing needs of modern maritime users and we have envisaged WiMAX mesh networks for high-speed and low-cost ship-to-ship/shore communications. In such a maritime WiMAX mesh network, ... Keywords: IEEE Std 802.16-2004, broadband wireless access, maritime communications, mesh network, multi-channel transmission

Ming-Tuo Zhou; Hiroshi Harada; Peng-Yong Kong; Chee-Wei Ang; Yu Ge; J. S. Pathmasuntharam

2009-06-01T23:59:59.000Z

94

diff -ruN oommf12a4pre-20100719/app/mmdisp/scripts ...  

Science Conference Proceedings (OSTI)

diff -ruN oommf12a4pre-20100719/app/mmdisp/scripts/mmdisp.tcl oommf12a4pre-20100719bis/app/mmdisp/scripts/mmdisp.tcl --- oommf12a4pre ...

2011-10-16T23:59:59.000Z

95

b100.dvi  

NLE Websites -- All DOE Office Websites (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)

96

Global distributions of total ozone during January and February 1979 as determined from DMSP multichannel filter radiometer measurements  

Science Conference Proceedings (OSTI)

The multichannel filter radiometer instrument (MFR) was first flown on a Defense Meteorological Satellite Program (DMSP) Block 5D series satellite in 1977. Daily analyses of the global distribution of retrieved total ozone are presented for January and February 1979. The temporal and spatial averages and variability of ozone during this period are discussed. Retrieved total column ozone data derived from the MFR measurements for January 1979 are compared with preliminary SBUV measurements and with distributions of total ozone measured between 1958 and 1967.

Luther, F.M.; Ellis, J.S.; Lovill, J.E.; Sullivan, T.J.; Weichel, R.L.

1980-09-01T23:59:59.000Z

97

b024.dvi  

NLE Websites -- All DOE Office Websites (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

98

b019.dvi  

NLE Websites -- All DOE Office Websites (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

99

b006.dvi  

NLE Websites -- All DOE Office Websites (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 →

100

Table HC4-12a. Air Conditioning by West Census Region, Million U.S ...  

U.S. Energy Information Administration (EIA)

Table HC4-12a. Air Conditioning by West Census Region, Million U.S. Households, 2001 Air Conditioning Characteristics RSE Column Factor: Total U.S.

Note: This page contains sample records for the topic "12a dpwa multichannel" from the National Library of EnergyBeta (NLEBeta).
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they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
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101

12 a ficha de exerccios de Mecanica Geometrica 27 de Maio de 2002  

E-Print Network (OSTI)

12 a ficha de exerc??�cios de Mec??anica Geom??etrica 27 de Maio de 2002 1. Seja (M,#) uma variedade

Natário, José

102

b032.dvi  

NLE Websites -- All DOE Office Websites (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

103

b017.dvi  

NLE Websites -- All DOE Office Websites (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

104

b014.dvi  

NLE Websites -- All DOE Office Websites (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,

105

b030.dvi  

NLE Websites -- All DOE Office Websites (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

106

b030.dvi  

NLE Websites -- All DOE Office Websites (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

107

b117.dvi  

NLE Websites -- All DOE Office Websites (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,

108

b018.dvi  

NLE Websites -- All DOE Office Websites (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

109

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'W; 27 degrees 10N - 26 degrees N] were examined to evaluate the interplay of salt, faults and gas. Seismic interpretation revealed the study area has two different styles of faulting and two different types of salt bodies that vary east to west. The eastern region of the study area has a thin sedimentary section and a massive, nearly continuous salt sheet characterized by minibasins and local salt highs. Faulting in this area appears to be the result of salt tectonism. The western region of the study area has a thick sedimentary wedge, and a few isolated salt diapirs. Long, linear faults are parallel to slope and imply some degree of gravitation sliding. The difference in faulting styles and salt bodies can be attributed to different depositional environments, different styles and amounts of sediment loading and different amounts of salt initially deposited. While there is a widespread occurrence of gas throughout the study area, little evidence of continuous bottom simulating reflectors (BSRs), a widely accepted geophysical indicator of gas hydrate, has been found. The gas hydrate stability zone (GHSZ) was modeled to provide information on the thickness and variability of the stability zone, and provide a baseline in a search for BSRs. The dataset was analyzed for multiple seismic expressions of BSRs, however only a few small and isolated examples were found. Potential fluid escape structures were seen in the seismic data. Despite the great number of potential features found in the seismic data only seven active seeps were found in a seep study by I. R. MacDonald. Seeps were seen in far less abundance than the number of seeps found offshore Louisiana. This may imply a lack of source offshore Texas.

Nemazi, Leslie A.

2010-05-01T23:59:59.000Z

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 is described. 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, J.A.

1981-01-19T23:59:59.000Z

111

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

112

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

113

Application and development of the Schwinger multichannel scattering theory and the partial differential equation theory of electron-molecule scattering. Final report  

Science Conference Proceedings (OSTI)

One version of the multichannel theory for electron-target scattering based on the Schwinger variational principle, the SMC method, requires the introduction of a projection parameter. The role of the projection parameter a is investigated and it is shown that the principal-value operator in the SMC equation is Hermitian regardless of the value of a as long as it is real and nonzero. In a basis that is properly orthonormalizable, the matrix representation of this operator is also Hermitian. The use of such basis is consistent with the Schwinger variational principle because the Lippmann-Schwinger equation automatically builds in the correct boundary conditions. Otherwise, an auxiliary condition needs to be introduced, and Takatsuka and McKoy's original value of a is one of the three possible ways to achieve Hermiticity. In all cases but one, a can be uncoupled from the Hermiticity condition and becomes a free parameter. An equation for a based on the variational stability of the scattering amplitude is derived; its solution has an interesting property that the scattering amplitude from a converged SMC calculation is independent of the choice of a even though the SMC operator itself is a-dependent. This property provides a sensitive test of the convergence of the calculation. For a static-exchange calculation, the convergence requirement only depends on the completeness of the one-electron basis, but for a general multichannel case, the a-invariance in the scattering amplitude requires both the one-electron basis and the N plus 1-electron basis to be complete. The role of a in the SMC equation and the convergence property are illustrated using two examples: e-CO elastic scattering in the static-exchange approximation, and a two-state treatment of the e-H2 Chi[sup 1]Sigma[sub g](+) yields b[sup 3]Sigma[sub u](+) excitation.

Weatherford, C.A.

1993-12-01T23:59:59.000Z

114

Influence of Alloy Microstructure on Oxide Growth in HCM12A in Supercritical Water Jeremy Bischoff1  

E-Print Network (OSTI)

corrosion resistance. Because of their radiation and stress corrosion cracking resistance, ferritic to oxidation appears to enhance the corrosion resistance of the alloy [2]. In the present study, HCM12A samples on the corrosion resistance but these results are not shown in this article. The oxide layers formed on HCM12A

Motta, Arthur T.

115

b041.dvi  

NLE Websites -- All DOE Office Websites (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±

116

b046.dvi  

NLE Websites -- All DOE Office Websites (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

117

b047.dvi  

NLE Websites -- All DOE Office Websites (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

118

EFTEM and EELS analysis of the oxide layer formed on HCM12A exposed to SCW Jeremy Bischoff  

E-Print Network (OSTI)

and stress corrosion cracking, ferritic­martensitic steels, such as HCM12A, are candidate materials the corrosion resistance of these alloys. ? 2012 Elsevier B.V. All rights reserved. 1. Introduction 1

Motta, Arthur T.

119

Flaxseed in Human Nutrition, 2nd EditionChapter 12 a-Linolenic Acid and Heart Disease  

Science Conference Proceedings (OSTI)

Flaxseed in Human Nutrition, 2nd Edition Chapter 12 a-Linolenic Acid and Heart Disease Food Science Health Nutrition Biochemistry eChapters Food Science & Technology Health - Nutrition - Biochemistry Press Downloadable

120

Application of the Schwinger multichannel formulation to electron-impact excitation of the b sup 3. Sigma. sup + state of CO  

Science Conference Proceedings (OSTI)

We report integral and differential cross sections for the electron-impact excitation of the {ital b} {sup 3}{Sigma}{sup +} state of CO using the Schwinger multichannel formulation. The calculations were carried out using a two-state approximation, with the incident electron energies in the range from 10.66 to 20 eV. We find four peaks in the inelastic cross section, centered at approximately 10.87, 11.6, 13.4, and 16.2 eV. The origins of the peak structures are discussed in terms of a partial-wave analysis, and comparison is made with experiment and theory where appropriate. We attribute the two sharp, low-energy (10.87 and 11.6 eV) peaks to the decay of {sup 2}{Sigma}{sup +} core-excited Rydberg resonance states of CO{sup {minus}}. The two higher-energy peaks are broad and less well defined. The 13.4-eV peak is not clearly identifiable as a resonance, whereas the 16.2-eV peak in the inelastic cross section occurs as a result of a {sup 2}{Sigma}{sup +} shape resonance in the elastic channel of the {ital b}{sup 3}{Sigma}{sup +} state. The magnitudes of the cross sections indicate that the {sup 2}{Sigma}{sup +} symmetry is dominant for all four peaks. In all the resonances, we find more than one partial wave contributing at energies slightly shifted with respect to each other. The present calculation represents the first {ital ab} {ital initio} study of core-excited Rydberg resonances in electron-molecule scattering.

Weatherford, C.A. (Department of Physics and Institute for Molecular Computations, Florida A M University, Tallahassee, Florida 32307 (USA)); Huo, W.M. (NASA Ames Research Center, Mail Stop 230-3, Moffett Field, California 94035 (USA))

1990-01-01T23:59:59.000Z

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

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

122

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

123

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):

124

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 an area of 7,577 mi^2 (19,825 km^2) on the Texas continental slope in the northwestern Gulf of Mexico. The western half of the study area is characterized by a thick sedimentary wedge and isolated salt diapirs whereas the eastern half is characterized by a massive and nearly continuous salt sheet topped by a thin sedimentary section. This difference in salt characteristics marks the edge of the continuous salt sheets of the central Gulf of Mexico and is likely a result of westward decline of original salt volume. Beneath the sedimentary wedge in the western part of the survey, an anomalous sedimentary package was found, that is described here as the diapiric, gassy sediment package (DGSP). The DGSP is highly folded at the top and is marked by tall, diapiric features. It may be either deformed shale or the toe of a complex thrust zone detaching the sedimentary wedge from deeper layers. The dataset was searched for the occurrence of bottom simulating reflectors (BSRs), as they are widely accepted as a geophysical indicator of gas trapped beneath gas hydrate deposits, which are known to occur farther east in the Gulf. Although, many seismic signatures were found that suggest widespread occurrence of gas within the upper sediment column, few BSRs were found. Even considering non-traditional definitions of BSRs, only a few occurrences of patchy and isolated BSRs features were identified. The lack of traditional BSRs is likely the result of geologic conditions that make it difficult to recognize gas hydrate deposits. These factors include: (1) unfavorable layer geometries, (2) flow of warm brines from depth, (3) elevated geotherms due to the thermogenic properties of salt and its varying thickness, and (4) widespread low porosity and permeability sediments within the gas hydrate stability zone.

Lewis, Dan'L 1986-

2012-12-01T23:59:59.000Z

125

Multi-channel infrared thermometer  

DOE Patents (OSTI)

A device for measuring the two-dimensional temperature profile of a surface comprises imaging optics for generating an image of the light radiating from the surface; an infrared detector array having a plurality of detectors; and a light pipe array positioned between the imaging optics and the detector array for sampling, transmitting, and distributing the image over the detector surfaces. The light pipe array includes one light pipe for each detector in the detector array.

Ulrickson, Michael A. (East Windsor, NJ)

1986-01-01T23:59:59.000Z

126

MULTICHANNEL PULSE-HEIGHT ANALYZER  

DOE Patents (OSTI)

This patent deals with electronic computing circuits and more particularly to pulse-height analyzers used for classifying variable amplitude pulses into groups of different amplitudes. The device accomplishes this pulse allocation by by converting the pulses into frequencies corresponding to the amplitudes of the pulses, which frequencies are filtered in channels individually pretuned to a particular frequency and then detected and recorded in the responsive channel. This circuit substantially overcomes the disadvantages of prior annlyzers incorporating discriminators pre-set to respond to certain voltage levels, since small variation in component values is not as critical to satisfactory circuit operation.

Russell, J.T.; Lefevre, H.W.

1958-01-21T23:59:59.000Z

127

b132.dvi  

NLE Websites -- All DOE Office Websites (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

128

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

129

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)

130

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:

131

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

132

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.

133

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

134

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)

135

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

136

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

137

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 >>

138

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.

139

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.

140

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):

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: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.

142

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.

143

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.

144

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

145

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):

146

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.

147

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

148

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

149

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

150

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:

151

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.

152

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 >>

153

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):

154

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.

155

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.

156

A compact multichannel spectrometer for Thomson scattering  

Science Conference Proceedings (OSTI)

The availability of high-efficiency volume phase holographic (VPH) gratings and intensified CCD (ICCD) cameras have motivated a simplified, compact spectrometer for Thomson scattering detection. Measurements of T{sub e} 100 eV by a 2072 l/mm VPH grating. The spectrometer uses a fast-gated ({approx}2 ns) ICCD camera for detection. A Gen III image intensifier provides {approx}45% quantum efficiency in the visible region. The total read noise of the image is reduced by on-chip binning of the CCD to match the 8 spatial channels and the 10 spectral bins on the camera. Three spectrometers provide a minimum of 12 spatial channels and 12 channels for background subtraction.

Schoenbeck, N. L.; Schlossberg, D. J.; Dowd, A. S.; Fonck, R. J.; Winz, G. R. [Department of Engineering Physics, University of Wisconsin, Madison, Wisconsin 53706 (United States)

2012-10-15T23:59:59.000Z

157

Multi-channel medical imaging system  

Science Conference Proceedings (OSTI)

A medical imaging system provides simultaneous rendering of visible light and fluorescent images. The system may employ dyes in a small-molecule form that remain in the subject's blood stream for several minutes, allowing real-time imaging of the subject's circulatory system superimposed upon a conventional, visible light image of the subject. The system may provide an excitation light source to excite the fluorescent substance and a visible light source for general illumination within the same optical guide used to capture images. The system may be configured for use in open surgical procedures by providing an operating area that is closed to ambient light. The systems described herein provide two or more diagnostic imaging channels for capture of multiple, concurrent diagnostic images and may be used where a visible light image may be usefully supplemented by two or more images that are independently marked for functional interest.

Frangioni, John V

2013-12-31T23:59:59.000Z

158

Multi-channel medical imaging system  

DOE Patents (OSTI)

A medical imaging system provides simultaneous rendering of visible light and fluorescent images. The system may employ dyes in a small-molecule form that remain in the subject's blood stream for several minutes, allowing real-time imaging of the subject's circulatory system superimposed upon a conventional, visible light image of the subject. The system may provide an excitation light source to excite the fluorescent substance and a visible light source for general illumination within the same optical guide used to capture images. The system may be configured for use in open surgical procedures by providing an operating area that is closed to ambient light. The systems described herein provide two or more diagnostic imaging channels for capture of multiple, concurrent diagnostic images and may be used where a visible light image may be usefully supplemented by two or more images that are independently marked for functional interest.

Frangioni, John V

2013-12-31T23:59:59.000Z

159

Low power, scalable multichannel high voltage controller  

DOE Patents (OSTI)

A low voltage control circuit is provided for individually controlling high voltage power provided over bus lines to a multitude of interconnected loads. An example of a load is a drive for capillary channels in a microfluidic system. Control is distributed from a central high voltage circuit, rather than using a number of large expensive central high voltage circuits to enable reducing circuit size and cost. Voltage is distributed to each individual load and controlled using a number of high voltage controller channel switches connected to high voltage bus lines. The channel switches each include complementary pull up and pull down photo isolator relays with photo isolator switching controlled from the central high voltage circuit to provide a desired bus line voltage. Switching of the photo isolator relays is further controlled in each channel switch using feedback from a resistor divider circuit to maintain the bus voltage swing within desired limits. Current sensing is provided using a switched resistive load in each channel switch, with switching of the resistive loads controlled from the central high voltage circuit.

Stamps, James Frederick (Livermore, CA); Crocker, Robert Ward (Fremont, CA); Yee, Daniel Dadwa (Dublin, CA); Dils, David Wright (Fort Worth, TX)

2006-03-14T23:59:59.000Z

160

Low power, scalable multichannel high voltage controller  

DOE Patents (OSTI)

A low voltage control circuit is provided for individually controlling high voltage power provided over bus lines to a multitude of interconnected loads. An example of a load is a drive for capillary channels in a microfluidic system. Control is distributed from a central high voltage circuit, rather than using a number of large expensive central high voltage circuits to enable reducing circuit size and cost. Voltage is distributed to each individual load and controlled using a number of high voltage controller channel switches connected to high voltage bus lines. The channel switches each include complementary pull up and pull down photo isolator relays with photo isolator switching controlled from the central high voltage circuit to provide a desired bus line voltage. Switching of the photo isolator relays is further controlled in each channel switch using feedback from a resistor divider circuit to maintain the bus voltage swing within desired limits. Current sensing is provided using a switched resistive load in each channel switch, with switching of the resistive loads controlled from the central high voltage circuit.

Stamps, James Frederick (Livermore, CA); Crocker, Robert Ward (Fremont, CA); Yee, Daniel Dadwa (Dublin, CA); Dils, David Wright (Fort Worth, TX)

2008-03-25T23:59:59.000Z

Note: This page contains sample records for the topic "12a dpwa multichannel" from the National Library of EnergyBeta (NLEBeta).
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161

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

2007-10-18T23:59:59.000Z

162

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

163

LANGMUIR TURBULENCE AND SOLAR RADIO BURSTS F. B. RIZZATO1,2, A. C.-L. CHIAN2,3, M. V. ALVES3, R. ERICHSEN1, S. R. LOPES4,  

E-Print Network (OSTI)

weather and monitoring the space environment. For example, type-III solar radio bursts are producedLANGMUIR TURBULENCE AND SOLAR RADIO BURSTS F. B. RIZZATO1,2, A. C.-L. CHIAN2,3, M. V. ALVES3, R beam-plasma instability play a fundamental role in the generation of solar radio bursts. We report

164

OOMMF 1.2a3 Patches  

Science Conference Proceedings (OSTI)

... (Thanks to RP Boardman for reporting this.) Solution: Apply this patch, and if you haven't already, also the the patch at item 3, and rerun pimake. ...

2011-07-01T23:59:59.000Z

165

NEPA Determination: LM-12a-12  

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

Additional Considerations Amendment to LM #12-12, Routine and Non-Routine Activities at the Grand Junction, Colorado, Office Site

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

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.

168

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.

169

b134.dvi  

NLE Websites -- All DOE Office Websites (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,

170

b134.dvi  

NLE Websites -- All DOE Office Websites (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 ±

171

An efficient multi-channel wireless switching system  

E-Print Network (OSTI)

of half-and full-duplex fdd in future multi-hop mobile radioassignment in half-duplex fdd relaying cellular networks,frequency division duplex (FDD), which is commonly used in

Shim, Jaewook

2010-01-01T23:59:59.000Z

172

Multichannel generalization of eigen-phase preserving supersymmetric transformations  

E-Print Network (OSTI)

We generalize eigen-phase preserving (EPP) supersymmetric (SUSY) transformations to $N>2$ channel Schr\\"odinger equation with equal thresholds. It is established that EPP SUSY transformations exist only in the case of even number of channels, $N=2M$. A single EPP SUSY transformation provides an $M(M-1)+2$ parametric deformation of the matrix Hamiltonian without affecting eigen-phase shifts of the scattering matrix.

Andrey M. Pupasov-Maksimov

2013-01-17T23:59:59.000Z

173

Multichannel blind separation and deconvolution of images for document analysis  

Science Conference Proceedings (OSTI)

In this paper, we apply Bayesian blind source separation (BSS) from noisy convolutive mixtures to jointly separate and restore source images degraded through unknown blur operators, and then linearly mixed. We found that this problem arises in several ... Keywords: Markov random fields (MRFs), blind image deconvolution, blind source separation, document image processing, parameter learning

Anna Tonazzini; Ivan Gerace; Francesca Martinelli

2010-04-01T23:59:59.000Z

174

Multi-channel CSMA/CA based smart utility networks  

Science Conference Proceedings (OSTI)

IEEE 802.15.4g is a recent standard for Smart Utility Networks (SUN). SUN is a house-to-house level subordinate network in the Smart Grid network. IEEE 802.15.4g uses a Carrier Sense Multiple Access/Collision Avoidance (CSMA/CA) algorithm for channel ...

Jiyoung Cha; Hu Jin; Dan Keun Sung

2011-08-01T23:59:59.000Z

175

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

176

Information Acquisition and Exploitation in Multichannel Wireless Networks  

E-Print Network (OSTI)

A wireless system with multiple channels is considered, where each channel has several transmission states. A user learns about the instantaneous state of an available channel by transmitting a control packet in it. Since probing all channels consumes significant energy and time, a user needs to determine what and how much information it needs to acquire about the instantaneous states of the available channels so that it can maximize its transmission rate. This motivates the study of the trade-off between the cost of information acquisition and its value towards improving the transmission rate. A simple model is presented for studying this information acquisition and exploitation trade-off when the channels are multi-state, with different distributions and information acquisition costs. The objective is to maximize a utility function which depends on both the cost and value of information. Solution techniques are presented for computing near-optimal policies with succinct representation in polynomial time. Th...

Guha, Sudipto; Sarkar, Saswati

2008-01-01T23:59:59.000Z

177

Original articles: Intelligent multichannel sensors for pulse wave analysis  

Science Conference Proceedings (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

178

Multichannel Satellite Retrieval of Cloud Parameter Probability Distribution Functions  

Science Conference Proceedings (OSTI)

A retrieval method has been developed to directly retrieve statistics of cloud parameters from Geostationary Operational Environmental Satellite (GOES) visible and infrared imager data. This method retrieves cloud parameter probability density ...

Darren McKague; K. Franklin Evans

2002-04-01T23:59:59.000Z

179

Sparse Multichannel Estimation Algorithm for Cooperative Underwater Acoustic Communication Networks  

E-Print Network (OSTI)

Introduction: Cooperative Underwater Acoustic Communicationsgain for wireless and underwater network in interference-

Richard, Nick; Mitra, Urbasi

2007-01-01T23:59:59.000Z

180

trinity-aa-use-case-v1.2a  

NLE Websites -- All DOE Office Websites (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

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.


181

OOMMF 1.2a4pre snapshots  

Science Conference Proceedings (OSTI)

... This code requires Tcl/Tk. We recommend the latest stable (ie, not alpha or beta) release of Tcl and Tk concurrent with the snapshot. ...

2011-10-16T23:59:59.000Z

182

Citation: D.E. Groom  

NLE Websites -- All DOE Office Websites (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 →

183

b048.dvi  

NLE Websites -- All DOE Office Websites (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-...

184

Multichannel Microwave Radiometric Observations at Saipan during the 1990 Tropical Cyclone Motion Experiment  

Science Conference Proceedings (OSTI)

To estimate mesoscale variations in integrated water vapor, cloud liquid water, and temperature in a tropical region, multiwavelength microwave radiometric observations were carried out over a seven-week period on the island of Saipan during the ...

Yong Han; Dennis W. Thomson

1994-02-01T23:59:59.000Z

185

Energy Efficient Reduced Complexity Multi-Service, Multi-Channel Scheduling Techniques.  

E-Print Network (OSTI)

??The need for energy efficient communications is essential in current and next-generation wireless communications systems. A large component of energy expenditure in mobile devices is (more)

Dechene, Dan J

2011-01-01T23:59:59.000Z

186

Multichannel blind signal separation in semiconductor-based GAS sensor arrays  

Science Conference Proceedings (OSTI)

Traditional approaches to gas sensing are usually related with gas identification and classification, i.e., recognition of aromas. In this work we propose an innovative approach to determine the concentration of the single species in a gas mixture by ...

Guillermo Bedoya; Sergi Bermejo; Joan Cabestany

2005-06-01T23:59:59.000Z

187

Multi-channel video-based parallel fire detection acceleration method using multi-cores  

Science Conference Proceedings (OSTI)

This paper presents a novel fire detection algorithm which uses several temporal and spatial features to recognize fire in video. It also proposes an acceleration strategy for parallel detection. We explore the parallelization from both coarse-grained ... Keywords: CPU acceleration, Fourier transform, fire detection, parallelization, wavelet transform

Di Xie; Ruofeng Tong; Hongsen Wu

2009-11-01T23:59:59.000Z

188

A multichannel electronic monitor of acoustic behaviors, and software to parse individual channels  

E-Print Network (OSTI)

circuit that produced a TTL-level high whenever a soundcomparator that produces a TTL-high whenever a sound in thesimultaneously with the TTL output of the channel monitoring

Hedrick, Ann V; Mulloney, B

2004-01-01T23:59:59.000Z

189

Multi-channel ultra-low-power receiver architecture for body area networks  

E-Print Network (OSTI)

In recently published integrated medical monitoring systems, a common thread is the high power consumption of the radio compared to the other system components. This observation is indicative of a natural place to attempt ...

Nadeau, Phillip Michel

2011-01-01T23:59:59.000Z

190

Equatorial Long Waves in Geostationary Satellite Observations and in a Multichannel Sea Surface Temperature Analysis  

Science Conference Proceedings (OSTI)

Geostationary satellite observations of a zonally oriented sea surface temperature front in the eastern equatorial Pacific were made between 1975 and 1981. Long waves appeared along the front mainly during the summer and fall, except during 1976, ...

Richard Legeckis; William Pichel; George Nesterczuk

1983-02-01T23:59:59.000Z

191

System for remote multichannel real-time monitoring of mouse ECG via the Internet  

E-Print Network (OSTI)

A hardware/software system was developed to allow real-time monitoring of multiple physiological signals simultaneously via the Internet. The hardware is specifically designed for measuring ECG signals from mice, while the ...

Oefinger, Matthew Blake, 1976-

2003-01-01T23:59:59.000Z

192

MULTICHANNEL SIGNAL SEPARATION FOR COCKTAIL PARTY SPEECH RECOGNITION: A DYNAMIC RECURRENT NETWORK  

E-Print Network (OSTI)

and some nonsingular di­ agonal matrix \\Lambda. Theorem 1 (Skitovich­Darmois) Let fs1 ; s2 ; : : : ; sng

Choi, Seungjin

193

Moving target indication via RADARSAT-2 multichannel synthetic aperture radar processing  

Science Conference Proceedings (OSTI)

With the recent launches of the German TerraSAR-X and the Canadian RADARSAT-2, both equipped with phased array antennas and multiple receiver channels, synthetic aperture radar, ground moving target indication (SAR-GMTI) data are now routinely being ...

S. Chiu; M. V. Dragoevi?

2010-01-01T23:59:59.000Z

194

Bridging the resolution gap : superimposition of multiple multi-channel volumes  

E-Print Network (OSTI)

4.4 Pixel Shader . . . . . . . . . . . . . . . . . . . . . .4.4.1 Shader Program . . . . . . . . . . . . . . . . .4.5A Flexible Multi-Volume Shader Framework for Arbitrarily

Liang, Chih K.

2008-01-01T23:59:59.000Z

195

MULTI-CHANNEL SEARCH FOR SUPERGRAVITY AT THE LARGE HADRON COLLIDER  

E-Print Network (OSTI)

The potential of seeing supersymmetry (SUSY) at the CERN Large Hadron Collider (LHC) was studied by looking at 3 types of signals: dilepton events from slepton pair productions, trilepton events from chargino/neutralino productions and missing energy plus multi-jet events from gluino/squark productions. I described my results by mapping out reachable areas in the supergravity parameter space. Areas explorable at LEP II were also mapped out for comparison.

Chih-Hao Chen

1995-03-09T23:59:59.000Z

196

Estimating VDT mental fatigue using multichannel linear descriptors and KPCA-HMM  

Science Conference Proceedings (OSTI)

The impacts of prolonged visual display terminal (VDT) work on central nervous system and autonomic nervous system are observed and analyzed based on electroencephalogram (EEG) and heart rate variability (HRV). Power spectral indices of HRV, the P300 ...

Chong Zhang; Chongxun Zheng; Xiaolin Yu; Yi Ouyang

2008-01-01T23:59:59.000Z

197

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.

198

CALIOP: a multichannel design code for gas-cooled fast reactors. Code description and user's guide  

Science Conference Proceedings (OSTI)

CALIOP is a design code for fluid-cooled reactors composed of parallel fuel tubes in hexagonal or cylindrical ducts. It may be used with gaseous or liquid coolants. It has been used chiefly for design of a helium-cooled fast breeder reactor and has built-in cross section information to permit calculations of fuel loading, breeding ratio, and doubling time. Optional cross-section input allows the code to be used with moderated cores and with other fuels.

Thompson, W.I.

1980-10-01T23:59:59.000Z

199

TARGET: A multi-channel digitizer chip for very-high-energy gamma-ray telescopes  

SciTech Connect

The next-generation very-high-energy (VHE) gamma-ray observatory, the Cherenkov Telescope Array, will feature dozens of imaging atmospheric Cherenkov telescopes (IACTs), each with thousands of pixels of photosensors. To be affordable and reliable, reading out such a mega-channel array requires event recording technology that is highly integrated and modular, with a low cost per channel. We present the design and performance of a chip targeted to this application: the TeV Array Readout with GSa/s sampling and Event Trigger (TARGET). This application-specific integrated circuit (ASIC) has 16 parallel input channels, a 4096-sample buffer for each channel, adjustable input termination, self-trigger functionality, and tight window-selected readout. We report the performance of TARGET in terms of sampling frequency, power consumption, dynamic range, current-mode gain, analog bandwidth, and cross talk. The large number of channels per chip allows a low cost per channel ($10 to $20 including front-end and back-end electronics but not including photosensors) to be achieved with a TARGET-based IACT readout system. In addition to basic performance parameters of the TARGET chip itself, we present a camera module prototype as well as a second-generation chip (TARGET 2), both of which have been produced.

Bechtol, K.; Funk, S.; /Stanford U., HEPL /KIPAC, Menlo Park; Okumura, A.; /JAXA, Sagamihara /Stanford U., HEPL /KIPAC, Menlo Park; Ruckman, L.; /Hawaii U.; Simons, A.; Tajima, H.; Vandenbroucke, J.; /Stanford U., HEPL /KIPAC, Menlo Park; Varner, G.; /Hawaii U.

2011-08-11T23:59:59.000Z

200

Heavy Thunderstorms Observed Over Land by the Nimbus 7 Scanning Multichannel Microwave Radiometer  

Science Conference Proceedings (OSTI)

In an examination of microwave data from the Nimbus 7 satellite, brightness temperatures were found that were much lower than those expected for the radiation emanating from rain-producing clouds. Every case of very cold brightness temperature ...

R. W. Spencer; W. S. Olson; Wu Rongzhang; D. W. Martin; J. A. Weinman; D. A. Santek

1983-06-01T23:59:59.000Z

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.


201

PIP: A multichannel, TDMA-based MAC for efficient and scalable bulk transfer in sensor networks  

Science Conference Proceedings (OSTI)

In this article, we consider the goal of achieving high throughput in a wireless sensor network. Our work is set in the context of those wireless sensor network applications which collect and transfer bulk data. We present PIP (Packets in Pipe), a MAC ... Keywords: Bulk data transfer, MAC, TDMA, pipelining, throughput optimization, wireless sensor network applications

Vijay Gabale; Kameswari Chebrolu; Bhaskaran Raman; Sagar Bijwe

2012-09-01T23:59:59.000Z

202

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

SciTech Connect

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

203

Laboratory Calibration in Distilled Water and Seawater of an Oceanographic Multichannel Interferometer-Refractometer  

Science Conference Proceedings (OSTI)

This paper begins by presenting the history and relevance of the index of refraction as a parameter in physical oceanography, the principle of operation and construction of a Russian interferometer-refractometer, the prior results of the use of ...

G. A. Seaver; V. L. Vlasov; A. G. Kostianoy

1997-04-01T23:59:59.000Z

204

b088.dvi  

NLE Websites -- All DOE Office Websites (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

205

b000.dvi  

NLE Websites -- All DOE Office Websites (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)

206

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

207

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 ....................................

208

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

E-Print Network (OSTI)

The mechanism of centering stiffness in seals. Force coefficients for short-length pressure seals. Design of annular seals: swirl brakes, impact on rotordynamics. Hydrostatic bearings in modern applications. The principle of hydrostatic lubrication. Effects of recess volume-fluid compressibility on force coefficients for operation at low and high frequencies. Applications of hydrostatic bearings

San Andres, Luis

2009-01-01T23:59:59.000Z

209

diff -crN oommf-1.2a2/CHANGES oommf/CHANGES  

Science Conference Proceedings (OSTI)

... renamed the port.h header file to ocport.h. + - support for Tcl/Tk up through release 8.4.1. +. ... support for Tcl/Tk up through release 8.4.1. +. ...

210

diff -crN oommf-1.2a0/CHANGES oommf/CHANGES  

Science Conference Proceedings (OSTI)

... 31,37 ****. with pre-compiled executables compatible with Tcl/Tk 8.3.x. Type. ... tclsh83 oommf.tcl pimake upgrade. tclsh83 oommf.tcl. ...

211

Table 8.12a Electric Noncoincident Peak Load and Capacity ...  

U.S. Energy Information Administration (EIA)

7 East Central Area Reliability Coordination Agreement (ECAR). 20 United States excluding Alaska and Hawaii. 8 ECAR, MAAC, and MAIN dissolved at the ...

212

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

E-Print Network (OSTI)

follow at a distance, are energy from Landfill Gas (LFG) extraction, co-incineration of SRF (Solid; BEP ­ Biomass Energy Plants; LFG ­ Landfill Gas; WtE ­ Waste-to-Energy 1 Excluding agricultural policy would be even more ambitious, replacing landfilling). Both the supply of renewable electricity

213

J12: A Modified Pidgeon Process for Energy Savings and Low ...  

Science Conference Proceedings (OSTI)

A18: Effect of Local Alendronate Delivery on In Vivo Osteogenesis From PCL ... A7: On-the-fly System Design for High Precision/Ultra Fast/Wide Area Fabrication .... C19: Dissolution Behavior of Cu Under Bump Metallization in Ball Grid Array ... High Volume and Fast Turnaround Automated Inline TEM Sample Preparation.

214

1642 IEEE TRANSACTIONS ON IMAGE PROCESSING, VOL. 12, NO. 12, DECEMBER 2003 Bayesian Multichannel Image Restoration Using  

E-Print Network (OSTI)

. [30] A. Tonazzini, L. Bedini, and E. Salerno, "A Markov model for blind image separation by a mean

Granada, Universidad de

215

Architecture for ultra-low power multi-channel transmitters for Body Area Networks using RF resonators  

E-Print Network (OSTI)

Body Area Networks (BANs) are gaining prominence for their use in medical and sports monitoring. This thesis develops the specifications of a ultra-low power 2.4GHz transmitter for use in a Body Area Networks, taking ...

Paidimarri, Arun

2011-01-01T23:59:59.000Z

216

On a joint temporal-spatial multi-channel assignment and routing scheme in resource-constrained wireless mesh networks  

Science Conference Proceedings (OSTI)

Use of multiple orthogonal channels can significantly improve network throughput of multi-hop wireless mesh networks (WMNs). In these WMNs where multiple channels are available, channel assignment is done either in a centralized manner, which unfortunately ... Keywords: Channel assignment, Linear programming (LP), Routing, Spatial, Temporal, Throughput, Wireless mesh networks (WMNs)

Yan Jin; Weiping Wang; Yingtao Jiang; Mei Yang

2012-05-01T23:59:59.000Z

217

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

218

Multi-channel reliability and spectrum usage in real homes: empirical studies for home-area sensor networks  

Science Conference Proceedings (OSTI)

Home area networks (HANs) consisting of wireless sensors have emerged as the enabling technology for important applications such as smart energy. These applications impose unique QoS constraints, requiring low data rates but high network reliability ...

Mo Sha; Gregory Hackmann; Chenyang Lu

2011-06-01T23:59:59.000Z

219

New Plasma Measurements With a Multichannel Milllimeter-wave Fluctuation Diagnostic System in the DIII-D Tokamak (A26734)  

E-Print Network (OSTI)

Proc. 18th Topical Conf. On High Temperature Plasma Diagnostics, May 16-20, 2010, Wildwood, New Jersey And To Be Published In Rev. Sci18th Topical Conference on High Temperature Plasma Diagnostics Wildwood New Jersey, US, 2010999617350

Hillesheim, J.C.

2010-06-10T23:59:59.000Z

220

Adaptation of a cubic smoothing spline algortihm for multi-channel data stitching at the National Ignition Facility  

SciTech Connect

Some diagnostics at the National Ignition Facility (NIF), including the Gamma Reaction History (GRH) diagnostic, require multiple channels of data to achieve the required dynamic range. These channels need to be stitched together into a single time series, and they may have non-uniform and redundant time samples. We chose to apply the popular cubic smoothing spline technique to our stitching problem because we needed a general non-parametric method. We adapted one of the algorithms in the literature, by Hutchinson and deHoog, to our needs. The modified algorithm and the resulting code perform a cubic smoothing spline fit to multiple data channels with redundant time samples and missing data points. The data channels can have different, time-varying, zero-mean white noise characteristics. The method we employ automatically determines an optimal smoothing level by minimizing the Generalized Cross Validation (GCV) score. In order to automatically validate the smoothing level selection, the Weighted Sum-Squared Residual (WSSR) and zero-mean tests are performed on the residuals. Further, confidence intervals, both analytical and Monte Carlo, are also calculated. In this paper, we describe the derivation of our cubic smoothing spline algorithm. We outline the algorithm and test it with simulated and experimental data.

Brown, C; Adcock, A; Azevedo, S; Liebman, J; Bond, E

2010-12-28T23:59:59.000Z

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.


221

Remotely Sensed Measurements of Stratocumulus Properties during FIRE Using the C130 Aircraft Multi-channel Radiometer  

Science Conference Proceedings (OSTI)

This paper gives a description of a narrow-hand near-infrared radiometer that was operated during the marine stratocumulus intensive field observation program of FIRE in 1987 from the United Kingdom Meteorological Office C130 aircraft. All data ...

F. Rawlins; J. S. Foot

1990-11-01T23:59:59.000Z

222

Multichannel Generalization of Kitaevs Majorana End States and a Practical Route to Realize Them in Thin Films  

E-Print Network (OSTI)

The ends of one-dimensional p+ip superconductors have long been predicted to possess localized Majorana fermion modes [A. Kitaev, arXiv:cond-mat/0010440]. We show that Majorana end states are robust beyond the strict 1D ...

Potter, Andrew Cole

223

PIP: a connection-oriented, multi-hop, multi-channel TDMA-based MAC for high throughput bulk transfer  

Science Conference Proceedings (OSTI)

In this paper, we consider the goal of achieving high throughput in a wireless sensor network. Our work is set in the context of those wireless sensor network applications which collect and transfer bulk data. We present PIP (Packets in Pipe), a MAC ... Keywords: MAC, TDMA, bulk data transfer, pipelining, throughput optimization, wireless sensor network applications

Bhaskaran Raman; Kameswari Chebrolu; Sagar Bijwe; Vijay Gabale

2010-11-01T23:59:59.000Z

224

Cenozoic gravity tectonics in the northern Gulf of Mexico induced by crustal extension. A new interpretation of multichannel seismic data  

E-Print Network (OSTI)

Cenozoic gravity tectonics in the northern Gulf of Mexico induced by crustal extension. A new HUSSON3 Key-words. ­ Gravity tectonics, Cenozoic rifting, Gulf of Mexico, Texas, Northeast Mexico. Abstract. ­ The Gulf of Mexico margin in Texas is one of the most impressive examples of starved passive

Husson, Laurent

225

b090.dvi  

NLE Websites -- All DOE Office Websites (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

226

b112.dvi  

NLE Websites -- All DOE Office Websites (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

227

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 | | | |_______________________|

228

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 >>

229

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.

230

Generalized redundancies for time series analysis Dean Prichard 1;2a and James Theiler 2;3  

E-Print Network (OSTI)

, Nonproliferation and International Security Division, Los Alamos National Laboratory, Los Alamos, NM 87545 3 Santa

Theiler, James

231

diff -crN oommf12a3/app/mmdisp/scripts/avf2ovf.tcl oommf ...  

Science Conference Proceedings (OSTI)

... REAL8m>(step_count); Happ.push_back(((1-t)*h0) + (t*h1)); } + if(step_count> 0) Happ.push_back(h1); + } + vector::iterator it = Happ ...

2011-06-03T23:59:59.000Z

232

Parametrization of a reactive force field for aluminum hydride J. G. O. Ojwang,1,2,a  

E-Print Network (OSTI)

the total energy of atomic hydro- gen instead of that of molecular hydrogen. Therefore, in Table VIII we of hydro- gen desorption in the two instances are similar. In Fig. 5 ii there is a slight rise in energy is the development of solid-state hydrogen storage media for vehicles. The United States' Department of Energy Do

Goddard III, William A.

233

Algorithms using inter-band cross-correlation for pixel registration and jitter reconstruction in multi-channel push-broom imagers  

SciTech Connect

We present two algorithms for determining sensor motion of a multi-spectral push-broom imager for use in subsequent image registration. The first algorithm, termed the {open_quotes}pairwise{close_quotes} method, performs cross-correlations between individual pairs of channels. The offsets of maximum correlation are formulated into a system of linear equations whose solution gives an estimate of the jitter function. The second algorithm performs cross-correlations between channels and a reference image called the {open_quotes}baseline{close_quotes} which is constructed by averaging together all the channels in the image cube. An estimated jitter time series is computed for each channel, all of which are overlapped and averaged to obtain a best estimate of the jitter function. The pairwise method is more general in that it can handle a wider range of jitter scenarios. The baseline method, although more restricted, is very simple to implement, and its accuracy can be improved substantially through iteration. In this paper, we describe both methods in detail and present results of simulations performed on thermal-infrared data cubes.

Theiler, J.; Henderson, B.G.; Smith, B.W.

1997-11-01T23:59:59.000Z

234

A Multichannel, Multiangle Method for the Determination of Infrared Optical Depth of Semitransparent High Cloud from an Orbiting Satellite. Part I: Formulation and Simulation  

Science Conference Proceedings (OSTI)

A method is presented for determining the infrared optical depth of semitransparent clouds from satellite measurements. The technique employs cloud measurements at two infrared wavelengths and two angles. Using a simple but accurate model it is ...

A. J. Prata; I. J. Barton

1993-10-01T23:59:59.000Z

235

Study of the possibility of developing a multichannel-diode-pumped multikilowatt solid-state laser based on optically dense active media  

SciTech Connect

Optimal conditions are determined for the development of efficient diode-pumped 1-{mu}m solid-state lasers with output powers up to a few tens of kilowatts. The thermal operating conditions are analysed for various Yb{sup 3+}- or Nd{sup 3+}-doped active media used in high-power laser systems. The advantages and disadvantages of these active ions and various crystal matrices are discussed. The theoretical analysis and experimental simulations allow one to determine the application fields of various laser crystals. A new concept of a multibeam (multipoint) pumping of active media is proposed. (special issue devoted to the 25th anniversary of the a.m. prokhorov general physics institute)

Garnov, S V; Mikhailov, V A; Serov, R V; Smirnov, V A; Tsvetkov, V B; Shcherbakov, I A [A.M. Prokhorov General Physics Institute, Russian Academy of Sciences, Moscow (Russian Federation)

2007-10-31T23:59:59.000Z

236

Components of an algebraic solution of the multichannel problem of low-energy n-${}^{12}$C scattering plus sub-threshold (${}^{13}$C) states  

E-Print Network (OSTI)

The effects of components in an assumed model interaction potential, as well as of the order to which its deformation is taken, upon resonances in the low-energy cross sections and upon sub-threshold bound states of the compound nucleus (${}^{13}$C) are discussed.

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

2004-03-22T23:59:59.000Z

237

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)

238

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)

239

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.

240

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:

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

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

242

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

243

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.

244

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:

245

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 >>

246

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)

247

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

248

Data:466ba082-9e49-4eac-a12a-24da3651e616 | Open Energy Information  

Open Energy Info (EERE)

WIND MACHINE SERVICE RATE SCHEDULE E-40 Sector: Commercial Description: AVAILABILITY This rate schedule is available in all territory served by the Company at all...

249

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 %.  

Science Conference Proceedings (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

250

Pages that link to "Data:De12a8fe-13b5-4491-9139-ea729b96ec3d...  

Open Energy Info (EERE)

91-9139-ea729b96ec3d: View (previous 50 | next 50) (20 | 50 | 100 | 250 | 500) City of Seattle, Washington (Utility Company) ( links) View (previous 50 | next 50) (20 | 50 |...

251

Data:72b22d28-179d-417f-83f5-80f86e12a95a | Open Energy Information  

Open Energy Info (EERE)

Sector: Lighting Description: Applicable for dusk to dawn lighting service by means of ballast operated lamp fixtures on a suitable wood pole. The service includes all electrical...

252

Experimental investigations of photochemically-generated organic aerosols and applications to early Earth and Mars  

E-Print Network (OSTI)

laser line filter to ensure measurement of elastic scattering. A multichannel scaler/averager (MSA, Stanford Research Systemslaser line filter to ensure measurement of elastic scattering. A multichannel scaler/averager (MSA, Stanford Research Systems:

Chu, Emily Faye

2013-01-01T23:59:59.000Z

253

Kommunikations-und Betriebssysteme (KBS, Hei) Komplexe und Verteilte IT-Systeme (CIT, Kao)  

E-Print Network (OSTI)

Bee Adoption. Smartgrid TMCNET. [6] Choong, Leslie, "Multi-Channel IEEE 802.15.4 Packet Capture Using Software

Wichmann, Felix

254

b112.dvi  

NLE Websites -- All DOE Office Websites (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

255

b000.dvi  

NLE Websites -- All DOE Office Websites (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

256

X-Ray Microdiffraction for VLSI  

Science Conference Proceedings (OSTI)

Energy windows, with resolutions Ehkl(2 )/Ehkl(2 )=0.03, were then opened in the multichannel analyzer (MCA), and the scattered intensities Ihkl were...

257

Internal Structure Of Puna Ridge- Evolution Of The Submarine...  

Open Energy Info (EERE)

(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,...

258

China Energy Primer  

E-Print Network (OSTI)

program Oil and natural gas supply Geopolitics such asa multi-channel natural gas (LNG) supply strategy since theof Malacca Strait Supply of oil, natural gas, and coal

Ni, Chun Chun

2010-01-01T23:59:59.000Z

259

Chemical Rearrangement under Hydrothermal Conditions: Formation of Polymeric Chains (CuX)2(dpiz) and (CuX)3(dpiz) (X ) Cl, Br; dpiz ) Dipyrido[1,2-a:2,3-d]imidazole) and Crystal Structures of  

E-Print Network (OSTI)

due to their excellent redox catalytic abilities.10 In this Communication, we report the synthesisL acid digestion bombs at 170 °C afforded orange crystals of 1 [(CuCl)2(C10H7N3)] (I) and 1 [(CuBr)3(C crystallographically independent copper sites in this common motif. Cu(1), the Cu atom in the tetrahedral site

Li, Jing

260

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.

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

Data:E6782d3f-9dca-4fb8-88c1-2a34a6a548d8 | Open Energy Information  

Open Energy Info (EERE)

in the fall of 2008. Source or reference: UtilityRateAPCo-WPCo-July-2008-Tariff-Book.pdf Assume net metering (buy sell): Flat rate buy (kWh): Flat rate sell (kWh):...

262

The SignCom system for data-driven animation of interactive virtual signers: Methodology and Evaluation  

Science Conference Proceedings (OSTI)

In this article we present a multichannel animation system for producing utterances signed in French Sign Language (LSF) by a virtual character. The main challenges of such a system are simultaneously capturing data for the entire body, including the ... Keywords: Communicative gestures, data-driven animation, multichannel animation, multimedia generation, multimodal corpora, signed language gestures

Sylvie Gibet; Nicolas Courty; Kyle Duarte; Thibaut Le Naour

2011-10-01T23:59:59.000Z

263

Copr. 1949-1998 Hewlett-Packard Co.On-Line Data Reduction for Nuclear Analyzers  

E-Print Network (OSTI)

Sniffing out minute amounts of radioactivity in our environment is just one of the talents of the versatile multichannel analyzer. Here are four multichannel analyzer systems two of them from new that include on-line computing devices capable of anything from straight number crunching to completely automating the analysis.

R. Cross; James A. Doub; John M. Stedman

1971-01-01T23:59:59.000Z

264

Overmodulation in subcarrier multiplexed video FM broad-band optical networks  

Science Conference Proceedings (OSTI)

The probability of an SCM (subcarrier multiplexed) signal falling outside the linear region of a laser diode is calculated in order to determine the overmodulation that may be practically employed for multichannel video distribution in single-octave ...

F. V.C. Mendis; B. T. Tan

2006-09-01T23:59:59.000Z

265

Remote Sensing of Precipitable Water over the Oceans from Nimbus 7 Microwave Measurements  

Science Conference Proceedings (OSTI)

Nimbus 7 Scanning Multichannel Microwave Radiometer (SMMR) brightness temperature measurements in the 21 and 18 GHz channels are used to sense the precipitable water in the atmosphere over oceans. The difference in the brightness temperature (T21 ...

C. Prabhakara; H. D. Chang; A. T. C. Chang

1982-01-01T23:59:59.000Z

266

An Integrated Approach toward Retrieving Physically Consistent Profiles of Temperature, Humidity, and Cloud Liquid Water  

Science Conference Proceedings (OSTI)

A method is presented for deriving physically consistent profiles of temperature, humidity, and cloud liquid water content. This approach combines a ground-based multichannel microwave radiometer, a cloud radar, a lidar-ceilometer, the nearest ...

Ulrich Lhnert; Susanne Crewell; Clemens Simmer

2004-09-01T23:59:59.000Z

267

Daylight Spectra of Individual Lightning Flashes in the 370690 nm Region  

Science Conference Proceedings (OSTI)

An optical multichannel analyzer slit spectrometer coupled to a minicomputer was used to record lightning spectra. This is the first successful application of a slit spectrometer to the study of individual lightning flashes and it was ...

Richard E. Orville

1980-04-01T23:59:59.000Z

268

Microstructure Profiles of Laser-induced Chlorophyll Fluorescence Spectra: Evaluation of Backscatter and Forward-Scatter Fiber-Optic Sensors  

Science Conference Proceedings (OSTI)

The implementation and characterization of backscatter and forward-scatter fiber-optic fluorescence sensors attached to a microstructure profiling instrument are described. By using an optical multichannel array detector to record emission ...

Russell A. Desiderio; Timothy J. Cowles; James N. Moum; Michael Myrick

1993-04-01T23:59:59.000Z

269

Merging Conventional (191592) and Passive Microwave (19782002) Estimates of Snow Extent and Water Equivalent over Central North America  

Science Conference Proceedings (OSTI)

A detailed evaluation of snow water equivalent (SWE) and snow cover extent (SCE) derived using the combined Scanning Multichannel Microwave Radiometer (SMMR) and Special Sensor Microwave Imager (SSM/I) brightness temperature records for the 1978...

C. Derksen; R. Brown; A. Walker

2004-10-01T23:59:59.000Z

270

Spectroradiometric Sun Photometry  

Science Conference Proceedings (OSTI)

This paper presents a method for calculating atmospheric transmittance from direct-beam solar spectral irradiance measurements under cloudless skies by treating spectral irradiance as a multichannel sun photometer. Computing the ratio of the ...

C. R. Osterwald; K. A. Emery

2000-09-01T23:59:59.000Z

271

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.

272

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

273

A Satellite Passive 37-GHz Scattering-based Method for Measuring Oceanic Rain Rates  

Science Conference Proceedings (OSTI)

A combination of theory and measurement is used to develop a scattering-based method for quantitatively measuring rainfall over the ocean from Nimbus-7 Scanning Multichannel Microwave Radiometer (SMMR) 37-GHz observations. This technique takes ...

Roy W. Spencer

1986-06-01T23:59:59.000Z

274

Satellite Passive Microwave Rain Rate Measurement over Croplands during Spring, Summer and Fall  

Science Conference Proceedings (OSTI)

Rain rate algorithms for spring, summer and fall that have been developed from comparisons between the brightness temperatures measured by the Nimbus-7 Scanning Multichannel Microwave Radiometer (SMMR) and rain rates derived from operational WSR-...

Roy W. Spencer

1984-11-01T23:59:59.000Z

275

A Passive Microwave Technique for Estimating Rainfall and Vertical Structure Information from Space. Part I: Algorithm Description  

Science Conference Proceedings (OSTI)

This paper describes a multichannel physical approach for retrieving rainfall and vertical structure information from satellite-based passive microwave observations. The algorithm makes use of statistical inversion techniques based upon ...

Christian Kummerow; Louis Giglio

1994-01-01T23:59:59.000Z

276

An ENSO Signal in Soybean Futures Prices  

Science Conference Proceedings (OSTI)

An example of socioeconomic repercussions of the El Nio-Southern Oscillation (ENSO) is examined. Multichannel singular spectrum analysis, a variant of principal component analysis useful in isolating the spatial and temporal variability ...

Christian L. Keppenne

1995-06-01T23:59:59.000Z

277

Impact of the Vertical Variation of Cloud Droplet Size on the Estimation of Cloud Liquid Water Path and Rain Detection  

Science Conference Proceedings (OSTI)

Cloud droplet effective radius (DER) and liquid water path (LWP) are two key parameters for the quantitative assessment of cloud effects on the exchange of energy and water. Chang and Li presented an algorithm using multichannel measurements made ...

Ruiyue Chen; Fu-Lung Chang; Zhanqing Li; Ralph Ferraro; Fuzhong Weng

2007-11-01T23:59:59.000Z

278

Modes of Interannual and Interdecadal Variability of Pacific SST  

Science Conference Proceedings (OSTI)

The multichannel singular spectrum analysis has been used to characterize the spatiotemporal structures of interdecadal and interannual variability of SST over the Pacific Ocean from 20S to 58N. Using the Comprehensive OceanAtmosphere Data ...

Xuebin Zhang; Jian Sheng; Amir Shabbar

1998-10-01T23:59:59.000Z

279

Comparison of Nimbus-7 SMMR and GOES-1 VISSR Atmospheric Liquid Water Content  

Science Conference Proceedings (OSTI)

Vertically integrated atmospheric liquid water content derived from Nimbus-7 Scanning Multichannel Microwave Radiometer (SMMR) brightness temperatures and from GOES-1 Visible and Infrared Spin-Scan Radiometer (VISSR) radiances in the visible are ...

Jean-Yves Lojou; Robert Frouin; Ren Bernard

1991-02-01T23:59:59.000Z

280

On Sub-ENSO Variability  

Science Conference Proceedings (OSTI)

Multichannel singular spectrum analysis (MSSA) of surface zonal wind, sea surface temperature (SST), 20 isotherm depth, and surface zonal current observations (between 1990 and 2004) identifies three coupled oceanatmosphere modes of variability ...

Noel S. Keenlyside; Mojib Latif; Anke Drkop

2007-07-01T23:59:59.000Z

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.


281

Inference of Marine Atmospheric Boundary Layer Moisture and Temperature Structure Using Airborne Lidar and Infrared Radiometer Data  

Science Conference Proceedings (OSTI)

A new technique for retrieving near-surface moisture and profiles of mixing ratio and potential temperature through the depth of the marine atmospheric boundary layer (MABL) using airborne lidar and multichannel infrared radiometer data is ...

Stephen P. Palm; Denise Hagan; Geary Schwemmer; S. H. Melfi

1998-03-01T23:59:59.000Z

282

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 Particle Analyzer is used to make measurements ...

Tang, Vincent, 1978-

2006-01-01T23:59:59.000Z

283

Design and implementation of A truecolor wide dimming single-pin LED driver  

E-Print Network (OSTI)

This thesis develops a single-pin LED driver used in wide screen displays. With the increasing size of the displays, a more compact multi-channel driver solution is needed for the increasing number of back light LEDs. This ...

Li, Zhen, M. Eng. Massachusetts Institute of Technology

2010-01-01T23:59:59.000Z

284

A Bayesian Approach to Microwave Precipitation Profile Retrieval  

Science Conference Proceedings (OSTI)

A multichannel passive microwave precipitation retrieval algorithm is developed. Bayes theorem is used to combine statistical information from numerical cloud models with forward radiative transfer modeling. Amultivariate lognormal prior ...

K. Franklin Evans; Joseph Turk; Takmeng Wong; Graeme L. Stephens

1995-01-01T23:59:59.000Z

285

Design and Performance Analysis of an Automated 10-Channel Solar Radiometer Instrument  

Science Conference Proceedings (OSTI)

An automated multichannel solar radiometer has been designed and fabricated by the Atmospheric Remote Sensing Laboratory at The University of Arizona. The automated radiometer has 10 separate silicon-photodiode-based channels that allow near-...

A. R. Ehsani; J. A. Reagan; W. H. Erxleben

1998-06-01T23:59:59.000Z

286

Snow Cover Distribution, Variability, and Response to Climate Change in Western China  

Science Conference Proceedings (OSTI)

A study is presented of the geographical distribution and spatial and temporal variabilities of the western China snow cover in the past 47 yr between 1951 and 1997. The data used consist of Scanning Multichannel Microwave Radiometer (SMMR) 6-day ...

Qin Dahe; Liu Shiyin; Li Peiji

2006-05-01T23:59:59.000Z

287

Estimation of Cloud Physical Parameters from Airborne Solar Spectral Reflectance Measurements for Stratocumulus Clouds  

Science Conference Proceedings (OSTI)

A new method is proposed to retrieve various cloud physical parameters of water clouds from the solar-flux reflectances at four wavelengths measured by using the airborne Multi-channel Cloud Pyranometer (MCP) system. The MCP system was designed ...

Shoji Asano; Masataka Shiobara; Akihiro Uchiyama

1995-10-01T23:59:59.000Z

288

Absolute Spectral Irradiance Measurements of Lightning from 375 to 880 nm  

Science Conference Proceedings (OSTI)

A spectrometer-detector optical multichannel analyzer system capable of absolute spectral irradiance measurements has been used to record the time-integrated emissions (150 or 300 ms) from cloud-to-ground lightning. Two detectors, one operating ...

Richard E. Orville; Ronald W. Henderson

1984-11-01T23:59:59.000Z

289

Rainfall Estimation over Oceans from SMMR and SSM/I Microwave Data  

Science Conference Proceedings (OSTI)

Passive microwave measurements made by the Scanning Multichannel Microwave Radiometer (SMMR) and the Special Sensor Microwave/Imager (SSM/I) reveal information about rain and precipitation-sized ice in the field of view (FOV) of the instruments. ...

C. Prabhakara; G. Dalu; G. L. Liberti; J. J. Nucciarone; R. Suhasini

1992-06-01T23:59:59.000Z

290

Global Soil Moisture from Satellite Observations, Land Surface Models, and Ground Data: Implications for Data Assimilation  

Science Conference Proceedings (OSTI)

Three independent surface soil moisture datasets for the period 197987 are compared: 1) global retrievals from the Scanning Multichannel Microwave Radiometer (SMMR), 2) global soil moisture derived from observed meteorological forcing using the ...

Rolf H. Reichle; Randal D. Koster; Jiarui Dong; Aaron A. Berg

2004-06-01T23:59:59.000Z

291

Remote Sensing of Cloud Optical Properties from Ground-Based Measurements of Transmittance: A Feasibility Study  

Science Conference Proceedings (OSTI)

The authors present a retrieval technique for the inference of cloud optical depth from data obtained by a ground-based multichannel radiometer for use in climate-related studies. The basic steps of the analysis procedure are considered, ...

E. Leontieva; K. Stamnes

1996-11-01T23:59:59.000Z

292

Constraining Microwave Brightness Temperatures by Radar Brightband Observations  

Science Conference Proceedings (OSTI)

Multichannel microwave sensors make it possible to construct physically based rainfall retrieval algorithms. In these schemes, errors arising from the inaccuracy of the physical modeling of the cloud system under observation have to be accounted ...

A. Battaglia; C. Kummerow; Dong-Bin Shin; C. Williams

2003-06-01T23:59:59.000Z

293

Nimbus-7 37 GHz Radiances Correlated with Radar Rain Rates over the Gulf of Mexico  

Science Conference Proceedings (OSTI)

In a comparison between 37 GHz brightness temperatures from the Nimbus 7 Scanning Multichannel Microwave Radiometer and rain rates derived from the WSR-57 radars at Galveston, Texas and Apalachicola, Florida, it was found that the brightness ...

Roy W. Spencer; Barry B. Hinton; William S. Olson

1983-12-01T23:59:59.000Z

294

Alamos National Laboratory  

NLE Websites -- All DOE Office Websites (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...

295

Three Years of Rainfall over the Indian Ocean  

Science Conference Proceedings (OSTI)

Monthly rain failing on the Indian Ocean is mapped for the period 1979 through 1981 by means of observations of the Nimbus-7 Scanning Multichannel Microwave Radiometer. Both stationary and mobile parts were found in the pattern of rain. The ...

David W. Martin; Barry B. Hinton; Brian A. Auvine

1993-04-01T23:59:59.000Z

296

b051.dvi  

NLE Websites -- All DOE Office Websites (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

297

b041.dvi  

NLE Websites -- All DOE Office Websites (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

298

b123.dvi  

NLE Websites -- All DOE Office Websites (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

299

b123.dvi  

NLE Websites -- All DOE Office Websites (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

300

b051.dvi  

NLE Websites -- All DOE Office Websites (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 ±

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

b135.dvi  

NLE Websites -- All DOE Office Websites (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

302

Influence of induced axial magnetic field on plasma dynamics and radiative characteristics of Z pinches  

SciTech Connect

The influence of an induced axial magnetic field on plasma dynamics and radiative characteristics of Z pinches is investigated. An axial magnetic field was induced in a novel Z-pinch load: a double planar wire array with skewed wires (DPWAsk), which represents a planar wire array in an open magnetic configuration. The induced axial magnetic field suppressed magneto-Rayleigh-Taylor (MRT) instabilities (with m = 0 and m = 1 instability modes) in the Z-pinch plasma. The influence of the initial axial magnetic field on the structure of the plasma column at stagnation was manifested through the formation of a more uniform plasma column compared to a standard double planar wire array (DPWA) load [V. L. Kantsyrev et al., Phys. Plasmas 15, 030704 (2008)]. The DPWAsk load is characterized by suppression of MRT instabilities and by the formation of the sub-keV radiation pulse that occurs before the main x-ray peak. Gradients in plasma parameters along the cathode-anode gap were observed and analyzed for DPWAsk loads made from low atomic number Z (Al) and mid-Z (brass) wires.

Kantsyrev, V. L.; Esaulov, A. A.; Safronova, A. S.; Osborne, G. C.; Shrestha, I.; Weller, M. E.; Stafford, A.; Shlyaptseva, V. V. [Physics Department, University of Nevada, Reno, Nevada 89557 (United States); Velikovich, A. L. [Plasma Physics Division, Naval Research Laboratory, Washington, D.C. 20375 (United States); Rudakov, L. I. [Icarus Research Inc., Bethesda, Maryland 20824 (United States); Williamson, K. M. [Physics Department, University of Nevada, Reno, Nevada 89557 (United States); Plasma Engineering Research Laboratory, Texas A and M University, Corpus Christi, TX 78412 (United States)

2011-10-15T23:59:59.000Z

303

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)  

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

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

304

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

NLE Websites -- All DOE Office Websites (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

305

Scanning angle Raman spectroscopy: Investigation of Raman scatter enhancement techniques for chemical analysis  

SciTech Connect

This thesis outlines advancements in Raman scatter enhancement techniques by applying evanescent fields, standing-waves (waveguides) and surface enhancements to increase the generated mean square electric field, which is directly related to the intensity of Raman scattering. These techniques are accomplished by employing scanning angle Raman spectroscopy and surface enhanced Raman spectroscopy. A 1064 nm multichannel Raman spectrometer is discussed for chemical analysis of lignin. Extending dispersive multichannel Raman spectroscopy to 1064 nm reduces the fluorescence interference that can mask the weaker Raman scattering. Overall, these techniques help address the major obstacles in Raman spectroscopy for chemical analysis, which include the inherently weak Raman cross section and susceptibility to fluorescence interference.

Meyer, Matthew W. [Ames Laboratory

2013-03-14T23:59:59.000Z

306

Results of Nucleon Resonance Extraction via Dynamical Coupled-Channels Analysis from #11;Collaboration @ EBAC  

SciTech Connect

We review a global analysis of meson production reactions off the nucleons by a collaboration at Excited Baryon Analysis Center of Jefferson Lab. The analysis is pursued with a dynamical coupled-channels approach, within which the dynamics of multi-channel reaction processes are taken into account in a fully consistent way with the two-body as well as three-body unitarity of the S-matrix. With this approach, new features of nucleon excitations are revealed as resonant particles originating from the non-trivial multi-channel reaction dynamics, which cannot be addressed by static hadron models where the nucleon excitations are treated as stable particles.

Hiroyuki Kamano

2012-04-01T23:59:59.000Z

307

Transmission Model and Ground-Truth Investigation of Satellite-Derived Sea Surface Temperatures  

Science Conference Proceedings (OSTI)

A band model of atmospheric transmission is used to investigate some of the multichannel sea surface temperature (MCSST) algorithms that are currently in use. The model is used with a set of atmospheric data to derive algorithms for the AVHRR and ...

I. J. Barton

1985-06-01T23:59:59.000Z

308

Inference of Cloud Temperature and Thickness by Microwave Radiometry from Space  

Science Conference Proceedings (OSTI)

The Scanning Multichannel Microwave Radiometer (SMMR) on the Seasat and Nimbus-7 satellite measured microwave radiation at 6.6, 10.69, 18.0, 21.0 and 37.0 GHz with both horizontal and vertical polarizations. Numerical simulations have been ...

P. C. Pandey; E. G. Njoku; J. W. Waters

1983-11-01T23:59:59.000Z

309

Dependent component analysis for cosmology: a case study  

Science Conference Proceedings (OSTI)

In this paper, we discuss various dependent component analysis approaches available in the literature and study their performances on the problem of separation of dependent cosmological sources from multichannel microwave radiation maps of the sky. Realisticaly ... Keywords: cosmic microwave background radiation, cosmological source separation, dependent component analysis

Ercan E. Kuruoglu

2010-09-01T23:59:59.000Z

310

Adaptive langevin sampler for separation of t-distribution modelled astrophysical maps  

Science Conference Proceedings (OSTI)

We propose to model the image differentials of astrophysical source maps by Student's t-distribution and to use them in the Bayesian source separation method as priors. We introduce an efficient Markov Chain Monte Carlo (MCMC) sampling scheme ... Keywords: astrophysical images, bayesian source separation, langevin stochastic equation, markov chain monte carlo (MCMC), metropolis-hastings, multichannel denoising, student's t-distribution

Koray Kayabol; Ercan E. Kuruo?lu; Jos Luis Sanz; Blent Sankur; Emanuele Salerno; Diego Herranz

2010-09-01T23:59:59.000Z

311

HUMAN BRAIN IMAGING AT 9.4 TESLA USING A COMBINATION OF TRAVELING WAVE EXCITATION WITH A 15-CHANNEL RECEIVE-ONLY ARRAY  

E-Print Network (OSTI)

HUMAN BRAIN IMAGING AT 9.4 TESLA USING A COMBINATION OF TRAVELING WAVE EXCITATION WITH A 15-CHANNEL is a successful setup for routine human brain imaging at 7 Tesla. For reception, the use of multiple surface coils multichannel transmit coils. At 9.4 Tesla, however, the even shorter RF wavelength in tissue causes the B1

312

Skylab Near-Infrared Observations of Clouds Indicating Supercooled Liquid Water Droplets  

Science Conference Proceedings (OSTI)

Orographically-induced lee-wave clouds were observed over New Mexico by a multichannel scanning radiometer on Skylab during December 1973. Channels centered at 0.83, 1.61 and 2.125 ?m were used to determine the cloud optical thickness, ...

Robert J. Curran; Man-Li C. Wu

1982-03-01T23:59:59.000Z

313

Dialog system for automatic data input/output and processing with two BESM-6 computers  

Science Conference Proceedings (OSTI)

This paper presents a system for conducting experiments with fully automatic processing of data from multichannel recorders in the dialog mode. The system acquires data at a rate of 2.5 . 10/sup 3/ readings/sec, processes in real time, and outputs digital and graphical material in a multitasking environment.

Belyaev, Y.N.; Gorlov, Y.P.; Makarychev, S.V.; Monakov, A.A.; Shcherbakov, S.A.

1985-09-01T23:59:59.000Z

314

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

DOE Green Energy (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

315

A min-max optimization framework for designing ?? learners: theory and hardware  

Science Conference Proceedings (OSTI)

In this paper, we present a framework for constructing ?? learning algorithms and hardware that can identify and track low-dimensional manifolds embedded in a high-dimensional analog signal space. At the core of the proposed approach is a min-max ... Keywords: ?? conversion, analog-to-digital conversion (ADC), high-dimensional signal processing, manifold learning, multichannel ADC, signal decorrelation

Amit Gore; Shantanu Chakrabartty

2010-03-01T23:59:59.000Z

316

Theory and Applications of Biotelemetry  

Science Conference Proceedings (OSTI)

In this study, biotelemetry and its evolution is explained in detail. Bioelectric and physiological variables could be measured by biotelemetry systems. The development of a biotelemetry system and its principal operation are presented. The components ... Keywords: biotelemetry, data gathering, implantable device, modulation, remote monitoring, single channel and multichannel biotelemetry, telemetry types

Nihal Fatma Gler; Elif Derya beyli

2002-04-01T23:59:59.000Z

317

A Model for Saharan Dust Transport  

Science Conference Proceedings (OSTI)

In this paper the source strength and the deposition rate of the dust emerging from the Sahara are assessed. For this purpose a multichannel sunphotometer has been developed and a turbidity network covering 11 stations has been set up in the ...

Guillaume A. d'Almeida

1986-07-01T23:59:59.000Z

318

Citizens and Service Channels: Channel Choice and Channel Management Implications  

Science Conference Proceedings (OSTI)

The arrival of electronic channels in the 1990s has had a huge impact on governmental service delivery. The new channels have led to many new opportunities to improve public service delivery, not only in terms of citizen satisfaction, but also in cost ... Keywords: Channel Behavior, Channel Choice, Channel Usage, Multi-Channel Management, Public Service Delivery, Service Channels, e-Government

Willem Pieterson

2010-04-01T23:59:59.000Z

319

Aircraft Microwave Observations and Simulations of Deep Convection from 18 to 183 GHz. Part II: Model Results  

Science Conference Proceedings (OSTI)

In Part II of the 29 June 1986 case study, a radiative transfer model is used to simulate the aircraft multichannel microwave brightness temperatures presented in Part I and to study the convective storm structure. Ground-based radar data are ...

Hwa-Young M. Yeh; N. Prasad; Robert A. Mack; Robert F. Adler

1990-06-01T23:59:59.000Z

320

IEEE TRANSACTIONS ON PLASMA SCIENCE. VOL. 17, NO. 1, FEBRUARY 1989 17 Experimental Study of CF4Conical Theta Pinch  

E-Print Network (OSTI)

) Optical multichannel analyzer, C ) Photodiode, H) Langmuir probe, and I) Oil diffusion vacuum pump. netically driven puff valve [lo] that delivered CF4 gas. The vacuum pump was an oil diffusion type with DOW Corning 704 pump oil. The conical theta pinch coil was IO-cm long, had a small ID of 12 cm, a large ID

Pedrow, Patrick D.

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

Substation Integrated Automation System Based on DSP  

Science Conference Proceedings (OSTI)

This Paper introduces the application of digital signal processor (DSP) at Substation Integrated Automation System. Using the powerful digital signal processing capability of DSP, high-speed multi-channel data acquisition function, and excellent data ... Keywords: Substation, Digital Signal Processor, Integrated Automation System

Yanzhe Li; Duowang Fan; Xuwei Dong

2009-08-01T23:59:59.000Z

322

Bayesian inference for multiband image segmentation via model-based cluster trees  

Science Conference Proceedings (OSTI)

We consider the problem of multiband image clustering and segmentation. We propose a new methodology for doing this, called model-based cluster trees. This is grounded in model-based clustering, which bases inference on finite mixture models estimated ... Keywords: Bayesian model, Clustering, Hyperspectral, Information criterion, Information fusion, Ising, Markov model, Multiband, Multichannel, Multispectral, Potts, Quantization, Segmentation

Fionn Murtagh; Adrian E. Raftery; Jean-Luc Starck

2005-06-01T23:59:59.000Z

323

Based on Two Swarm Optimized Algorithm of Neural Network to Prediction the Switch's Traffic of Coal  

Science Conference Proceedings (OSTI)

Coal accurately predict multi-channel network traffic monitoring network for transmission to enhance and improve the QoS is very important, the characteristics of coalmine monitoring network, the first neural network model was constructed, followed by ... Keywords: Coal, network traffic, ant colony algorithm, Particle swarm optimization

Xiao-qiang Shao

2011-07-01T23:59:59.000Z

324

Toward Applications of EMG and Preliminary Study in the Next Design of Compact Integrated Bio-Signal Recording System  

Science Conference Proceedings (OSTI)

Electromygraph or EMG is a device used to measure and record muscle signal. The developments of microelectronics allow the design and realization of such a device with current off-shelf components. The authors developed system consists of multi-channel ... Keywords: Electromyography, Hand-Held, Microcontroller, Multi Channels, Portable

Kastam Astami; Arga Aridarma

2010-07-01T23:59:59.000Z

325

Measurement system for metal-oxide gas sensors  

Science Conference Proceedings (OSTI)

A study on smell sensing and classification has been developed for a long time by many ways. Most of these have been focused on bad smells, when factors of bad smells were known chemically. Many gas sensors have been developed to detect specific chemicals. ... Keywords: Metal-oxide gas sensor, Multi-channel sensors, Smell measurement

Hideo Araki; Sigeru Omatu

2013-02-01T23:59:59.000Z

326

987 Orrington Road (847) 555-3700 Evanston, IL 60208 b-cats@baxter.org  

E-Print Network (OSTI)

from 82% to 99.7% through enhanced queue design, work flow analysis, phone skills training, and call Results-oriented leader with extensive experience in general management, multi-channel marketing Creation New Market and Product Development General Management, Finance, Operations B-to-B and B

Shull, Kenneth R.

327

Nanotechnology-Based Systems for Nuclear Radiation and Chemicl Detection  

SciTech Connect

This main objectives of this effort are the development and prototyping of a small. sensitive, and low-cost multi-channel nanoparticle scintillation microdevice with integrated waveguides for alpha, beta, gamma, and neutron detection. This research effort has integrated experiments and simulation to determine the combination of process-specific materials for the achievement optimum detection conditions.

Kody Varahramyan; Pedro Derosa; Chester Wilson

2006-10-11T23:59:59.000Z

328

Development and Validation of a Perceptual Instrument to Measure E-Commerce Performance  

Science Conference Proceedings (OSTI)

This paper develops and validates an attitudinal scale that can measure the performance of e-commerce operations both in "pure play" Internet firms and in on-line components of multichannel firms. The measurement instrument is grounded in a resource-based ... Keywords: E-Commerce, Organizational Performance, Reliability, Resource-Based View, Scale Development, Validity

Michael R. Wade; Saggi Nevo

2006-01-01T23:59:59.000Z

329

Real Time Optics of the Growth of Textured Silicon Films in Photovoltaics: Final Technical Report, 1 August 1999--12 August 2002  

DOE Green Energy (OSTI)

Novel optical instruments, including single and dual rotating-compensator multichannel ellipsometers, have been designed and developed to probe the evolution of the microstructure, spectroscopic optical properties, and other materials characteristics during the fabrication and processing of individual thin films and thin-film structures used in photovoltaic devices. These instruments provide a foundation for next-generation process design/control and metrology in existing and future photovoltaics technologies. In this project, the materials system studied in the greatest detail was thin-film silicon, fabricated at low temperatures by plasma-enhanced chemical vapor deposition. Real-time measurements of such thin films by multichannel ellipsometry have established deposition phase diagrams that provide guiding principles for multistep fabrication of high-performance amorphous (a-Si:H) and microcrystalline (mc-Si:H) solar cells. Such phase diagrams have also served to disprove conventional wisdom in the fabrication of thin-film solar cell structures, thus avoiding future unproductive research efforts.

Collins, R. W.; Wronski, C. R.

2003-10-01T23:59:59.000Z

330

Analysis of long-lived radionuclidic impurities in short-lived radiopharmaceutical waste using gamma spectrometry  

Science Conference Proceedings (OSTI)

Large hospitals and biomedical research centers utilize decay-in-storage programs to minimize the volume of their low level radioactive waste. However, some medically useful radionuclides often contain small amounts of long-lived radionuclidic impurities which may complicate simple waste management procedures. We have evaluated the extent of this problem in low level radioactive waste involving {sup 67}Cu and {sup 111}In over a 6-mo cycle of decay-in-storage by identifying the residual radionuclides in our dry waste using a multichannel analyzer. The multichannel analyzer was also used to quantify the radionuclide constituents of our liquid waste at the beginning of a decay-in-storage cycle. Radionuclides were identified by the presence of characteristic photopeaks of each isotope in the gamma spectrum and quantified by region of interest analysis. Gamma spectrometry can be used to aid waste segregation and final management decisions on low level radioactive waste. 10 refs., 1 fig., 2 tabs.

Salako, Q.; DeNardo, S.J. [Univ. of California, Sacramento, CA (United States)

1997-01-01T23:59:59.000Z

331

Kadygrov-EN  

NLE Websites -- All DOE Office Websites (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

332

Pulser injection with subsequent removal for gamma-ray spectrometry  

DOE Patents (OSTI)

An improved system for gamma-ray spectroscopy characterized by an interface module that controls the injection of electronic pulses as well as separation logic that enables storage of pulser events in a region of the spectrum of a multichannel analyzer distinct from the region reserved for storage of gamma-ray events. The module accomplishes this by tagging pulser events (high or low) injected into the amplification circuitry, adding an offset to the events so identified at the time the events are at the output of the analog to digital converter, and storing such events in the upper portion of the spectrum stored in the multichannel analyzer. The module can be adapted for use with existing gamma-ray spectroscopy equipment to provide for automatic analyses of radioisotopes. 7 figs.

Hartwell, J.K.; Goodwin, S.G.; Johnson, L.O.; Killian, E.W.

1989-02-01T23:59:59.000Z

333

Ultrarelativistic laser systems based on coherent beam combining  

Science Conference Proceedings (OSTI)

Conceptual design for femtosecond laser system of exawatt class, based on multi-channel amplifier and coherent field combining of petawatt amplifier channels with phase-frequency controlled radiation by optical clock are discussed. The scheme of start petawatt level few-cycle laser system with stable phase-frequency parameters determinated by the accuracy of the optical standard based on parametric amplification in big-size LBO crystals pumped by picosecond pulses is analyzed.

Bagayev, S. N.; Trunov, V. I.; Pestryakov, E. V.; Frolov, S. A.; Leschenko, V. E.; Kirpichnikov, A. V.; Kokh, A. E.; Petrov, V. V.; Vasiliev, V. A. [Institute of Laser Physics SB RAS, Ac. Lavrentyev's prosp., 13/3, Novosibirsk (Russian Federation); Institute of Geology and Mineralogy SB RAS, Ac. Koptug's prosp., 3, Novosibirsk (Russian Federation); Institute of Laser Physics SB RAS, Ac. Lavrentyev's prosp., 13/3, Novosibirsk (Russian Federation)

2012-07-11T23:59:59.000Z

334

Mercuric iodide research and development in support of DOE Historically Black Colleges and University Program. Semiannual technical progress report  

Science Conference Proceedings (OSTI)

This report describes the progress achieved during the first six months of the program. The different subjects studied were: zone refining experiments of mercuric iodide to establish optimum refining parameters and produce purified material; development of surface reflection spectroscopy as a method to measure crystal surface temperatures, with emphasis on investigation the potential of using optical multichannel analysis; optical methods for measuring iodine vapor during physical vapor transport of HgI{sub 2}; and atomic force microscopy studies.

George, M.A.; Zheng, Y.; Salary, L.; Chen, K.T.; Burger, A.

1994-10-31T23:59:59.000Z

335

Direct observation of dynamic surface acoustic wave controlled carrier injection into single quantum posts using phase-resolved optical spectroscopy  

E-Print Network (OSTI)

A versatile stroboscopic technique based on active phase-locking of a surface acoustic wave to picosecond laser pulses is used to monitor dynamic acoustoelectric effects. Time-integrated multi-channel detection is applied to probe the modulation of the emission of a quantum well for different frequencies of the surface acoustic wave. For quantum posts we resolve dynamically controlled generation of neutral and charged excitons and preferential injection of holes into localized states within the nanostructure.

Vlk, S; Schlein, F J R; Truong, T A; Kim, H; Petroff, P M; Wixforth, A; Krenner, H J

2010-01-01T23:59:59.000Z

336

Direct observation of dynamic surface acoustic wave controlled carrier injection into single quantum posts using phase-resolved optical spectroscopy  

E-Print Network (OSTI)

A versatile stroboscopic technique based on active phase-locking of a surface acoustic wave to picosecond laser pulses is used to monitor dynamic acoustoelectric effects. Time-integrated multi-channel detection is applied to probe the modulation of the emission of a quantum well for different frequencies of the surface acoustic wave. For quantum posts we resolve dynamically controlled generation of neutral and charged excitons and preferential injection of holes into localized states within the nanostructure.

S. Vlk; F. Knall; F. J. R. Schlein; T. A. Truong; H. Kim; P. M. Petroff; A. Wixforth; H. J. Krenner

2010-11-08T23:59:59.000Z

337

Raman activity in synchronously dividing bacteria  

SciTech Connect

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

338

Exploratory Research on MEMS Technology for Air-Conditioning and Heat-Pumps  

Science Conference Proceedings (OSTI)

Multiple refrigerant channels are essential for improving system efficiency in refrigeration and air-conditioning systems. A study was conducted to study the use of micro-electrical-mechanical- systems (MEMS) and micro device technologies to improve current vapor compression refrigeration cycles. The first step toward realizing this goal, and the focus of this report, is to determine how to better control multi-channel evaporators by reducing refrigerant maldistribution among channels.

1998-12-14T23:59:59.000Z

339

Data acquisition system of Moeller polarimeter Hall A Jefferson Lab (in Russian)  

SciTech Connect

The structure, parameters and test results of a new data acquisition system for Moller polarimeter based on flash-ADC are presented. Flash-ADC is electronic module in VME format that consists of high-speed multichannel ADC piped type and FPGA unit on board. The use of flash-ADC has a lot of advantages: reduce of cable interconnections, events registration with higher rate, considerable decreases of system deadtime and, as result, the accuracy of polarization measurements is increases.

Roman Pomatsalyuk

2012-11-01T23:59:59.000Z

340

Readout electronics of silicon detectors used in space cosmic-ray charges measurement  

E-Print Network (OSTI)

A readout electronics used in space cosmic-ray charges measurement for multi-channel silicon detector and its performance test results are introduced in this paper. A 64-channel charge sensitive ASIC (VA140) from IDEAS company is adopt in this method. With its features of low power consumption, low noise, large dynamic range and high integration, it can be used in future particle detecting experiments base on silicon detector.

Zhang Fei; Fan Rui-Rui; Peng Wen-Xi; Dong Yi-Fan; Gong Ke; Liang Xiao-Hua; Liu Ya-Qing; Wang Huan-Yu

2013-07-11T23:59:59.000Z

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

AZURE: An R-matrix code for nuclear astrophysics  

Science Conference Proceedings (OSTI)

The paper describes a multilevel, multichannel R-matrix code, AZURE, for applications in nuclear astrophysics. The code allows simultaneous analysis and extrapolation of low-energy particle scattering, capture, and reaction cross sections of relevance to stellar hydrogen, helium, and carbon burning. The paper presents a summary of R-matrix theory, code description, and a number of applications to demonstrate the applicability and versatility of AZURE.

Azuma, R. E. [Department of Physics, University of Toronto, Toronto, Ontario M5S 1A7 (Canada); University of Notre Dame, Department of Physics, Notre Dame, Indiana 46556 (United States); Uberseder, E.; Boer, R. J. de; Goerres, J.; LeBlanc, P. J.; Ugalde, C.; Wiescher, M. [University of Notre Dame, Department of Physics, Notre Dame, Indiana 46556 (United States); Simpson, E. C. [University of Notre Dame, Department of Physics, Notre Dame, Indiana 46556 (United States); Department of Physics, Faculty of Engineering and Physical Sciences, University of Surrey, Guildford, Surrey GU2 7XH (United Kingdom); Brune, C. R. [Department of Physics and Astronomy, Ohio University, Ohio 45701 (United States); Costantini, H. [University of Notre Dame, Department of Physics, Notre Dame, Indiana 46556 (United States); Istituto Nazionale Fisica Nucleare (INFN), Genova (Italy); Heil, M. [GSI Darmstadt, Planckstr. 1, 64291 Darmstadt (Germany)

2010-04-15T23:59:59.000Z

342

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

343

Noninstrusive Appliance Load Monitoring System (NIALMS): Beta-Test Results  

Science Conference Proceedings (OSTI)

Traditional methods for gathering appliance-specific load data require installation of individual recording meters on each appliance or multi-channel recording meters with remote sensors on individual appliances. This is a highly intrusive approach that is expensive and cumbersome in terms of capital, labor, and customer goodwill. A newly developed non-intrusive appliance load monitoring system (NIALMS) promises to minimize many of the costs of traditional end-use metering approaches.

1997-11-04T23:59:59.000Z

344

Ultrahigh heat flux plasma-facing components for magnetic fusion energy  

Science Conference Proceedings (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

345

Design Strategy for a Formally Veri ed Reliable Computing Platform  

E-Print Network (OSTI)

. Pecht, Ed., Product Reliability, Maintainability, and Supportability Hdbk: CRC Press, 1995. [12] A

Butler, Ricky W.

346

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

NLE Websites -- All DOE Office Websites (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.

347

Microsoft Word - cimini-d.doc  

NLE Websites -- All DOE Office Websites (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

348

Experimental confirmation of photon-induced spin-flip transitions in helium via triplet metastable yield spectra  

SciTech Connect

Doubly excited states below the N=2 ionization threshold are populated by exciting helium atoms in a supersonic beam with monochromatized synchrotron radiation. The fluorescence decay of these states triggers a radiative cascade back to the ground state with large probability to populate long lived singlet and triplet helium metastable states. The yield of metastables is measured using a multichannel plate detector after the beam has passed a singlet-quenching discharge lamp. The variation of the yield observed with the lamp switched on or off is related to the triplet-singlet mixing of the doubly excited states.

Rubensson, Jan-Erik [Department of Physics and Astronomy, Box 530, S-75121 Uppsala (Sweden); Moise, Angelica; Richter, Robert [Sincrotrone Trieste, in Area Science Park, I-34149 Basovizza, Trieste (Italy); Mihelic, Andrej; Bucar, Klemen; Zitnik, Matjaz [Jozef Stefan Institute, Jamova cesta 39, SI-1000 Ljubljana (Slovenia)

2010-06-15T23:59:59.000Z

349

Numerical integration method for FIBWR2  

Science Conference Proceedings (OSTI)

FIBWR2 is a computer code for the detailed analysis of transient flow distribution in boiling water reactor (BWR) cores. It is a successor of the well-known steady-state FIBWR code developed for Yankee Atomic Electric Company and the Electric Power Research Institute in 1981. In the 8 yr since the original development of FIBWR, BWR fuel designs have become more complex, and computer speed and memory have greatly increased. In mid-1988, several utilities formed a support group to extend FIBWR's capabilities. The new transient version of FIBWR, referred to as FIBWR2, can model new fuel designs and perform multichannel core thermal-hydraulic transient analysis.

Andersen, P.S. (Andersen Associates, Washington, DC (USA)); Gitnick, B.J. (ENSA, Inc., Rockville, MD (USA))

1989-11-01T23:59:59.000Z

350

Initial Results from the Lost Alpha Diagnostics on Joint European Torus  

DOE Green Energy (OSTI)

Two devices have been installed in the Joint European Torus (JET) vacuum vessel near the plasma boundary to investigate the loss of energetic ions and fusion products in general and alpha particles in particular during the upcoming JET experiments. These devices are (i) a set of multichannel thin foil Faraday collectors, and (ii) a well collimated scintillator which is optically connected to a charge-coupled device. Initial results, including the radial energy and poloidal dependence of lost ions from hydrogen and deuterium plasmas during the 200506 JET restart campaign, will be presented.

Darrow, Doug; Cecil, Ed; Ellis, Bob; Fullard, Keith; Hill, Ken; Horton, Alan; Kiptily, Vasily; Pedrick, Les; Reich, Matthias

2007-07-25T23:59:59.000Z

351

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

SciTech Connect

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

352

Coupled-Channel Evaluations of Cross Sections for Scattering Involving Particle-Unstable Resonances  

Science Conference Proceedings (OSTI)

How does the scattering cross section change when the colliding bound-state fragments are allowed particle-emitting resonances? This question is explored in the framework of a multichannel algebraic scattering method of determining nucleon-nucleus cross sections at low energies. Two cases are examined, the first being a gedanken investigation in which n+{sup 12}C scattering is studied with the target states assigned artificial widths. The second is a study of neutron scattering from {sup 8}Be, a nucleus that is particle unstable. Resonance character of the target states markedly varies evaluated cross sections from those obtained assuming stability in the target spectrum.

Fraser, P.; Amos, K. [School of Physics, University of Melbourne, Victoria 3010 (Australia); Canton, L.; Pisent, G. [Istituto Nazionale di Fisica Nucleare, Sezione di Padova, I-35131 (Italy); Karataglidis, S. [Department of Physics and Electronics, Rhodes University, Grahamstown 6140 (South Africa); Svenne, J. P. [Department of Physics and Astronomy, University of Manitoba, Winnipeg, Manitoba, R3T 2N2 (Canada); Knijff, D. van der [Advanced Research Computing, Information Division, University of Melbourne, Victoria 3010 (Australia)

2008-12-12T23:59:59.000Z

353

The Cold Dark Matter Search test stand warm electronics card  

SciTech Connect

A card which does the signal processing for four SQUID amplifiers and two charge sensitive channels is described. The card performs the same functions as is presently done with two custom 9U x 280mm Eurocard modules, a commercial multi-channel VME digitizer, a PCI to GPIB interface, a PCI to VME interface and a custom built linear power supply. By integrating these functions onto a single card and using the power over Ethernet standard, the infrastructure requirements for instrumenting a Cold Dark Matter Search (CDMS) detector test stand are significantly reduced.

Hines, Bruce; /Colorado U., Denver; Hansen, Sten; /Fermilab; Huber, Martin; /Colorado U., Denver; Kiper, Terry; /Fermilab; Rau, Wolfgang; /Queen's U., Kingston; Saab, Tarek; /Florida U.; Seitz, Dennis; Sundqvist, Kyle; /UC, Berkeley; Mandic, Vuk; /Minnesota U.

2010-11-01T23:59:59.000Z

354

LARGE-SCALE FLOWS IN PROMINENCE CAVITIES  

Science Conference Proceedings (OSTI)

Regions of rarefied density often form cavities above quiescent prominences. We observed two different cavities with the Coronal Multichannel Polarimeter on 2005 April 21 and with Hinode/EIS on 2008 November 8. Inside both of these cavities, we find coherent velocity structures based on spectral Doppler shifts. These flows have speeds of 5-10 km s{sup -1}, occur over length scales of tens of megameters, and persist for at least 1 hr. Flows in cavities are an example of the nonstatic nature of quiescent structures in the solar atmosphere.

Schmit, D. J. [Department of Astrophysical and Planetary Sciences, University of Colorado-Boulder, UCB 391, Boulder, CO 80309 (United States); Gibson, S. E.; Tomczyk, S. [High Altitude Observatory, National Center for Atmospheric Research, P.O. Box 3000, Boulder, CO 80307 (United States); Reeves, K. K. [Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, MS 58, Cambridge, MA 02138 (United States); Sterling, Alphonse C. [NASA Marshall Space Flight Center, Space Science Office, VP62, Huntsville, AL 35805 (United States); Brooks, D. H. [Space Science Division, Naval Research Laboratory, Washington, DC 20375 (United States); Williams, D. R. [Mullard Space Science Laboratory, University College London, Holmbury St. Mary, Dorking, Surrey RH5 6NT (United Kingdom); Tripathi, D. [Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Wilberforce Road, Cambridge CB3 0WA (United Kingdom)

2009-08-01T23:59:59.000Z

355

Three-dimensional geometry of fluvial reservoir sands: steam-drive case study  

Science Conference Proceedings (OSTI)

The three-dimensional geometry of fluvial sands in South Belridge heavy oil field was investigated as part of an Enhanced Oil Recovery study. It was shown that only close-spaced well data are sufficient to define the sand-body geometries and heterogeneities of multichannelled fluvial systems. Reservoir flow-unit patterns cannot necessarily be correctly delineated by isolated vertical sequence analysis. Wireline logs from 19 wells and conventional cores from seven wells in a 10-ac (660 ft x 660 ft) pattern were correlated in detail, using additional input from sedimentology, steam-flow patterns, and reservoir flow-unit continuity.

McPherson, J.G.; Miller, D.D.

1989-03-01T23:59:59.000Z

356

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

DOE Green Energy (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

357

Recent progress of the HCN interferometer on J-TEXT tokamak  

Science Conference Proceedings (OSTI)

A multichannel far-infrared HCN laser interferometer has been developed to measure plasma electron density for the J-TEXT tokamak. Initial operation of a seven chords system with 7 cm spacing and a 0.1 ms temporal resolution is described. Density modulation experiments in J-TEXT show that it is possible to obtain information on particle transport by precise measurement of the density perturbation amplitude and phase spatial variation. An optical configuration upgrade has been implemented in order to improve phase resolution.

Gao, L.; Zhuang, G.; Wang Zhijiang; Chen, W.; Chen, J.; Li, Q.; Liu, Y. [State Key Laboratory of Advanced Electromagnetic Engineering and Technology, Huazhong University of Science and Technology, Wuhan 430074 (China)

2012-10-15T23:59:59.000Z

358

Cimel Sunphotometer (CSPHOT) Handbook  

Science Conference Proceedings (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

359

Methods for improved forewarning of critical events across multiple data channels  

DOE Patents (OSTI)

This disclosed invention concerns improvements in forewarning of critical events via phase-space dissimilarity analysis of data from mechanical devices, electrical devices, biomedical data, and other physical processes. First, a single channel of process-indicative data is selected that can be used in place of multiple data channels without sacrificing consistent forewarning of critical events. Second, the method discards data of inadequate quality via statistical analysis of the raw data, because the analysis of poor quality data always yields inferior results. Third, two separate filtering operations are used in sequence to remove both high-frequency and low-frequency artifacts using a zero-phase quadratic filter. Fourth, the method constructs phase-space dissimilarity measures (PSDM) by combining of multi-channel time-serial data into a multi-channel time-delay phase-space reconstruction. Fifth, the method uses a composite measure of dissimilarity (C.sub.i) to provide a forewarning of failure and an indicator of failure onset.

Hively, Lee M [Philadelphia, TN

2007-04-24T23:59:59.000Z

360

Noise Reduction with Microphone Arrays for Speaker Identification  

SciTech Connect

Reducing acoustic noise in audio recordings is an ongoing problem that plagues many applications. This noise is hard to reduce because of interfering sources and non-stationary behavior of the overall background noise. Many single channel noise reduction algorithms exist but are limited in that the more the noise is reduced; the more the signal of interest is distorted due to the fact that the signal and noise overlap in frequency. Specifically acoustic background noise causes problems in the area of speaker identification. Recording a speaker in the presence of acoustic noise ultimately limits the performance and confidence of speaker identification algorithms. In situations where it is impossible to control the environment where the speech sample is taken, noise reduction filtering algorithms need to be developed to clean the recorded speech of background noise. Because single channel noise reduction algorithms would distort the speech signal, the overall challenge of this project was to see if spatial information provided by microphone arrays could be exploited to aid in speaker identification. The goals are: (1) Test the feasibility of using microphone arrays to reduce background noise in speech recordings; (2) Characterize and compare different multichannel noise reduction algorithms; (3) Provide recommendations for using these multichannel algorithms; and (4) Ultimately answer the question - Can the use of microphone arrays aid in speaker identification?

Cohen, Z

2011-12-22T23:59:59.000Z

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361

An analysis of the proposed MITR-III core to establish thermal-hydraulic limits at 10 MW. Final report  

Science Conference Proceedings (OSTI)

The 5 MW Massachusetts Institute of Technology Research Reactor (MITR-II) is expected to operate under a new license beginning in 1999. Among the options being considered is an upgrade in the heat removal system to allow operation at 10 MW. The purpose of this study is to predict the Limiting Safety System Settings and Safety Limits for the upgraded reactor (MITR-III). The MITR Multi-Channel Analysis Code was written to analyze the response of the MITR system to a series of anticipated transients in order to determine the Limiting Safety System Settings and Safety Limits under various operating conditions. The MIT Multi-Channel Analysis Code models the primary and secondary systems, with special emphasis placed on analyzing the thermal-hydraulic conditions in the core. The code models each MITR fuel element explicitly in order to predict the behavior of the system during flow instabilities. The results of the code are compared to experimental data from MITR-II and other sources. New definitions are suggested for the Limiting Safety System Settings and Safety Limits. MITR Limit Diagrams are included for three different heat removal system configurations. It is concluded that safe, year-round operating at 10 MW is possible, given that the primary and secondary flow rates are both increased by approximately 40%.

Harling, O.K.; Lanning, D.D.; Bernard, J.A.; Meyer, J.E.; Henry, A.F.

1997-06-01T23:59:59.000Z

362

Development of a fuel-powered compact SMA (Shape Memory Alloy) actuator system  

E-Print Network (OSTI)

The work presents investigations into the development of a fuel-powered compact SMA actuator system. For the final SMA actuator, the K-alloy SMA strip (0.9 mm x 2.5 mm), actuated by a forced convection heat transfer mechanism, was embedded in a rectangular channel. In this channel, a rectangular piston, with a slot to accommodate the SMA strip, ran along the strip and was utilized to prevent mixing between the hot and the cold fluid in order to increase the energy density of the system. The fuel, such as propane, was utilized as main energy source in order to achieve high energy and power densities of the SMA actuator system. Numerical analysis was carried out to determine optimal channel geometry and to estimate maximum available force, strain and actuation frequency. Multi-channel combustor/heat exchanger and micro-tube heat exchanger were designed and tested to achieve high heat transfer rate and high compactness. The final SMA actuator system was composed of pumps, valves, bellows, multi-channel combustor/heat exchanger, micro-tube heat exchanger and control unit. The experimental tests of the final system resulted in 250 N force with 2 mm displacement and 1.0 Hz actuation frequency in closed-loop operation, in which the hot and the cold fluid were re-circulated by pumps.

Jun, Hyoung Yoll

2003-12-01T23:59:59.000Z

363

A method for extracting the resonance parameters from experimental cross section  

E-Print Network (OSTI)

The matrix elements of the multi-channel Jost matrices are written in such a way that their dependencies on all possible odd powers of channel momenta are factorized explicitly. As a result the branching of the Riemann energy surface at all the channel thresholds is represented in them via exact analytic expressions. The remaining single-valued functions of the energy are expanded in the Taylor series near an arbitrary point on the real axis. Using the thus obtained Jost matrices, the $S$-matrix is constructed and then the scattering cross section is calculated, which therefore depends on the Taylor expansion coefficients. These coefficients are considered as the adjustable parameters that are optimized to fit a given set of experimental data. After finding the coefficients, the resonances are located as zeros of the Jost matrix determinant at complex energies. Within this approach the $S$-matrix has proper analytic structure. This enables us not only to locate multi-channel resonances but also to reproduce their partial widths as well as the scattering cross section in the channels for which the data are not available.

S. A. Rakityansky; N. Elander

2012-10-22T23:59:59.000Z

364

A Brief History of the Chemistry Department -Part II  

E-Print Network (OSTI)

geniuses during the great #12;A brief history, continued porn poge I the world, among them -Barcelona

Kounaves, Samuel P.

365

Microwave Graphene Electronics Laboratoire Pierre Aigrain Ecole Normale Suprieure  

E-Print Network (OSTI)

et al. RMP 2011, etc...... #12;A graphene capacitor thin oxide Thick metallic gate Vdc+Vrf CQ Cgeo r

Plaçais, Bernard

366

Annual Energy Review - Energy Information Administration  

U.S. Energy Information Administration (EIA)

Comprehensive data summaries, comparisons, analysis, ... 8.12a Electric Noncoincident Peak Load and Capacity Margin: Summer Peak Period, 1986

367

Metroflux: a high performance system for analysing flow at very fine-grain  

E-Print Network (OSTI)

available on the market to perform traffic capture (for example, products from Endace, Solera #12;(a) all

Gonçalves, Paulo

368

Section 37  

NLE Websites -- All DOE Office Websites (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

369

Portable active interrogation system.  

SciTech Connect

The system consists of a pulsed DT neutron generator (5 x 10{sup 7} n/s) and a portable but high intrinsic efficiency, custom-designed, polyethylene-moderated {sup 3}He neutron detector. A multichannel scaler card in a ruggedized laptop computer acquires the data. A user-friendly LabVIEW program analyzes and displays the data. The program displays a warning message when highly enriched uranium or any other fissionable materials is detected at a specified number of sigmas above background in the delayed region between pulses. This report describes the system and gives examples of the response of the system to highly enriched uranium and some other fissionable materials, at several distances and with various shielding materials.

Moss, C. E. (Calvin E.); Brener, M. W. (Mathieu W.); Hollas, C. L. (Charles L.); Myers, W. L. (William L.)

2004-01-01T23:59:59.000Z

370

Plutonium isotopic analysis of highly enriched mixed oxides  

SciTech Connect

We investigated the analysis method used by the International Atomic Energy Agency (IAEA) to determine the plutonium isotopic composition of highly enriched mixed oxides (MOX). The IAEA currently uses the Cicero multichannel analyzer and the IAEAPU algorithm for its analysis. In our investigation the plutonium isotopic measurements were found to be good for PuO/sub 2/ powder or low-enriched MOX, but acceptable for highly enriched MOX in IAEA special nuclear material (SNM) accountability applications. The gamma-ray interferences from /sup 235/U resulted in underestimation of the isotopic composition of /sup 239/Pu and overestimation of all other plutonium isotopes. Samples with high /sup 240/Pu content were found to have significantly higher error in plutonium isotopic analyses of highly enriched MOX. Code modifications or use of calibration curves are necessary for plutonium isotopic analyses of highly enriched MOX in IAEA SNM accountability applications.

Clement, S.D.; Augustson, R.H.

1986-08-01T23:59:59.000Z

371

Response Time Measurements of the NIF DANTE XRD-31 X-Ray Diodes (Pre-print)  

SciTech Connect

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

372

NETL: Methane Hydrates - DOE/NETL Projects - Structural and Stratigraphic  

NLE Websites -- All DOE Office Websites (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

373

ARM - Employment Opportunities Article  

NLE Websites -- All DOE Office Websites (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

374

Molecular Foundry  

NLE Websites -- All DOE Office Websites (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

375

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

376

ARM - Facility News Article  

NLE Websites -- All DOE Office Websites (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

377

EQ-SANS: the Extended Q-Range Small-Angle Neutron Scattering Diffractometer  

NLE Websites -- All DOE Office Websites (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

378

Self-modulation oscillation regimes in fibre lasers with microoptomechanical resonance structures  

Science Conference Proceedings (OSTI)

Self-modulation oscillation regimes are studied in erbium fibre lasers with intracavity microoptomechanical structures (microoscillators) of different types, namely, based on silicon structures and consisting of special waveguide segments. Optical excitation of acoustomechanical vibrations of microoscillators is accomplished using photothermal effect or light pressure. Under the conditions of resonance interaction, i.e., when the eigenfrequencies of microoscillators coincide with the frequencies of relaxation oscillations or with those of intermode beats, the dependences of self-oscillation characteristics on the system parameters are found and the stability of the self-modulation frequency within 10{sup -4} - 10{sup -6} is obtained at relatively low (40 - 300) Q-factors of microoscillators. The possibility to construct multivariate (multichannel) fibreoptical sensors of physical quantities with frequency division of measurement channels is demonstrated. (optical fibres, lasers and amplifiers. properties and applications)

Egorov, F A; Potapov, V T [V.A.Kotel'nikov Institute of Radio Engineering and Electronics, Fryazino Branch, Russian Academy of Sciences, Fryazino, Moscow Region (Russian Federation)

2012-09-30T23:59:59.000Z

379

Notes on parafermionic QFT's with boundary interaction  

E-Print Network (OSTI)

The main result of these notes is an analytical expression for the partition function of the circular brane model for arbitrary values of the topological angle. The model has important applications in condensed matter physics. It is related to the dissipative rotator (Ambegaokar-Eckern-Schon) model and describes a ``weakly blocked'' quantum dot with an infinite number of tunneling channels under a finite gate voltage bias. A numerical check of the analytical solution by means of Monte Carlo simulations has been performed recently. To derive the main result we study the so-called boundary parafermionic sine-Gordon model. The latter is of certain interest to condensed matter applications, namely as a toy model for a point junction in the multichannel quantum wire.

S. L. Lukyanov

2006-06-16T23:59:59.000Z

380

A Novel Charge Recycling Approach to Low-Power  

SciTech Connect

A novel charge-recycling scheme has been designed and implemented to demonstrate the feasibility of operating digital circuits using the charge scavenged from the leakage and dynamic load currents inherent to digital logic. The proposed scheme uses capacitors to efficiently recover the ground-bound charge and to subsequently boost the capacitor voltage to power up the source circuit. This recycling methodology has been implemented on a 12-bit Gray-code counter within a 12-bit multichannel Wilkinson ADC. The circuit has been designed in 0.5 m BiCMOS and in 90nm CMOS processes. SPICE simulation results reveal a 46 53% average reduction in the energy consumption of the counter. The total energy savings including the control generation aggregates to an average of 26 34%.

Ulaganathan, Chandradevi [University of Tennessee, Knoxville (UTK); Britton Jr, Charles L [ORNL; Holleman, Jeremy [University of Tennessee, Knoxville (UTK); Blalock, Benjamin [University of Tennessee, Knoxville (UTK)

2012-01-01T23:59:59.000Z

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

Stark spectroscopy of a probe lithium beam excited with two dye lasers as a technique to study a high-power ion-beam diode  

SciTech Connect

A non-disturbing measurement of electric field distributions is a subject of special interest in plasma physics and high-voltage devices. In this paper we describe a diagnostic technique for remote sensing of electric fields via injection of a probe beam of lithium atoms and cascade excitation of resonance fluorescence with two broadband dye lasers. The fluorescence spectrum was recorded using a monochromator equipped with an optical multi-channel analyser. The magnitude of the local electric field was retrieved from the Stark-shifted components of the 3d-2plithium spectral line. The technique was applied to measurements of the electric field in the applied-B-field high-voltage diode of the 1 TW KALIF ion-beam accelerator.

Knyazev, B. A. [Budker Institute of Nuclear Physics SB RAS, 630090 Novosibirsk (Russian Federation); An, W.; Bluhm, H. [Karlsruhe Institute of Technology (KIT), Institute for Pulsed Power and Microwave Technology (IHM), D-76131 Karlsruhe (Germany)

2012-03-15T23:59:59.000Z

382

Open Source Scanning Probe Microscopy Control Software package GXSM  

SciTech Connect

GXSM is a full featured and modern scanning probe microscopy (SPM) software. It can be used for powerful multidimensional image/data processing, analysis, and visualization. Connected to an instrument, it is operating many different flavors of SPM, e.g., scanning tunneling microscopy and atomic force microscopy or, in general, two-dimensional multichannel data acquisition instruments. The GXSM core can handle different data types, e.g., integer and floating point numbers. An easily extendable plug-in architecture provides many image analysis and manipulation functions. A digital signal processor subsystem runs the feedback loop, generates the scanning signals, and acquires the data during SPM measurements. The programmable GXSM vector probe engine performs virtually any thinkable spectroscopy and manipulation task, such as scanning tunneling spectroscopy or tip formation. The GXSM software is released under the GNU general public license and can be obtained via the internet.

Zahl, P.; Wagner, T.; Moller, R.; Klust, A.

2010-05-01T23:59:59.000Z

383

Dense ceramic membranes for converting methane to syngas  

DOE Green Energy (OSTI)

Dense mixed-oxide ceramics capable of conducting both electrons and oxygen ions are promising materials for partial oxygenation of methane to syngas. We are particularly interested in an oxide based on the Sr-Fe-Co-O system. Dense ceramic membrane tubes have been fabricated by a plastic extrusion technique. The sintered tubes were then used to selectively transport oxygen from air through the membrane to make syngas without the use of external electrodes. The sintered tubes have operated for >1000 h, and methane conversion efficiencies of >98% have been observed. Mechanical properties, structural integrity of the tubes during reactor operation, results of methane conversion, selectivity of methane conversion products, oxygen permeation, and fabrication of multichannel configurations for large-scale production of syngas will be presented.

Balachandran, U.; Dusek, J.T.; Picciolo, J.J.; Ma, B.; Maiya, P.S.; Mieville, R.L. [Argonne National Lab., IL (United States); Kleefisch, M.S.; Udovich, C.A. [Amoco Exploration/Production, Naperville, IL (United States)

1995-07-01T23:59:59.000Z

384

Studies of electron collisions with polyatomic molecules using distributed-memory parallel computers  

SciTech Connect

Elastic electron scattering cross sections from 5--30 eV are reported for the molecules C{sub 2}H{sub 4}, C{sub 2}H{sub 6}, C{sub 3}H{sub 8}, Si{sub 2}H{sub 6}, and GeH{sub 4}, obtained using an implementation of the Schwinger multichannel method for distributed-memory parallel computer architectures. These results, obtained within the static-exchange approximation, are in generally good agreement with the available experimental data. These calculations demonstrate the potential of highly parallel computation in the study of collisions between low-energy electrons and polyatomic gases. The computational methodology discussed is also directly applicable to the calculation of elastic cross sections at higher levels of approximation (target polarization) and of electronic excitation cross sections.

Winstead, C.; Hipes, P.G.; Lima, M.A.P.; McKoy, V. (A. A. Noyes Laboratory of Chemical Physics, California Institute of Technology, Pasadena, California 91125 (US))

1991-04-15T23:59:59.000Z

385

Energy-dependent target widths in a coupled-channel scattering study  

Science Conference Proceedings (OSTI)

The question of how the scattering cross section changes when the spectra of the colliding nuclei have low-excitation particle-emitting resonances is explored using a multichannel algebraic scattering method. As a test case, the particle-unstable nucleus {sup 8}Be has been considered as a target. Nucleon-nucleus scattering cross sections, as well as the spectra of the compound nuclei formed, have been determined from calculations that consider, as well as those that disregard, particle-emission widths of the target nuclear states. The resonant character of the unstable excited states introduces a problem because the low-energy tails of these resonances can intrude into the subthreshold, bound-state region. This unphysical behavior needs to be corrected by modifying, in an energy-dependent way, the shape of the target resonances from the usual Lorentzian form. The resonance function must smoothly reach zero at the elastic threshold. We explore herein a way of achieving this condition.

Canton, L. [Istituto Nazionale di Fisica Nucleare, Sezione di Padova, I-35131 Padova (Italy); Fraser, P. R. [Instituto de Ciencias Nucleares, Universidad Nacional Autonoma de Mexico, 04510 Mexico Distrito Federal (Mexico); School of Physics, University of Melbourne, Victoria 3010 (Australia); Svenne, J. P. [Department of Physics and Astronomy, University of Manitoba, Winnipeg, Manitoba, R3T 2N2 (Canada); Amos, K.; Knijff, D. van der [School of Physics, University of Melbourne, Victoria 3010 (Australia); Karataglidis, S. [Department of Physics, University of Johannesburg, Auckland Park 2006 (South Africa)

2011-04-15T23:59:59.000Z

386

Body composition to climate change studies - the many facets of neutron induced prompt gamma-ray analysis  

Science Conference Proceedings (OSTI)

In-vivo body composition analysis of humans and animals and in-situ analysis of soil using fast neutron inelastic scattering and thermal neutron capture induced prompt-gamma rays have been described. By measuring carbon (C), nitrogen (N) and oxygen (O), protein, fat and water are determined. C determination in soil has become important for understanding below ground carbon sequestration process in the light of climate change studies. Various neutron sources ranging from radio isotopic to compact 14 MeV neutron generators employing the associated particle neutron time-of-flight technique or micro-second pulsing were implemented. Gamma spectroscopy using recently developed digital multi-channel analyzers has also been described.

Mitra,S.

2008-11-17T23:59:59.000Z

387

Thick-film technology for ultra high vacuum interfaces of micro-structured traps  

E-Print Network (OSTI)

We adopt thick-film technology to produce ultra high vacuum compatible interfaces for electrical signals. These interfaces permit voltages of hundreds of Volts and currents of several Amperes and allow for very compact vacuum setups, useful in quantum optics in general, and especially for quantum information and quantum simulations using miniaturized traps for ions or neutral atoms. Such printed circuits can also be useful as pure in-vacuum devices. We demonstrate a specific interface, which provides eleven current feedthroughs, more than 70 dc feedthroughs and a feedthrough for radio frequencies. We achieve a pressure in the low 1e-11mbar range and demonstrate the full functionality of the interface by trapping chains of cold ytterbium ions, which requires all of the signals mentioned above being present. In addition, a versatile multi-channel device for supplying precise time-dependent voltages has been developed.

Delia Kaufmann; Thomas Collath; M. Tanveer Baig; Peter Kaufmann; Eman Asenwar; Michael Johanning; Christof Wunderlich

2011-07-20T23:59:59.000Z

388

An automated neutron monitor maintenance system  

Science Conference Proceedings (OSTI)

Neutron detectors are commonly used by the nuclear materials processing industry to monitor fissile materials in process vessels and tanks. The proper functioning of these neutron monitors must be periodically evaluated. We have developed and placed in routine use a PC-based multichannel analyzer (MCA) system for on-line BF3 and He-3 gas-filled detector function testing. The automated system: 1) acquires spectral data from the monitor system, 2) analyzes the spectrum to determine the detector`s functionality, 3) makes suggestions for maintenance or repair, as required, and 4) saves the spectrum and results to disk for review. The operator interface has been designed to be user-friendly and to minimize the training requirements of the user. The system may also be easily customized for various applications

Moore, F.S.; Griffin, J.C.; Odell, D.M.C.

1996-09-01T23:59:59.000Z

389

Simulation of the tropical Pacific climate with a coupled ocean - atmosphere general circulation model. Part II: Interannual variability  

Science Conference Proceedings (OSTI)

Two multiyear simulations with a coupled ocean-atmosphere general circulation model (GCM)-totaling 45 years-are used to investigate interannual variability at the equator. The model consists of the UCLA global atmospheric GCM coupled to the GFDL oceanic GCM, dynamically active over the tropical Pacific. Multichannel singular spectrum analysis along the equator identifies ENSO-like quasi-biennial (QB) and quasi-quadrennial (QQ) modes. Both consist of predominantly standing oscillations in sea surface temperature and zonal wind stress that peak in the central or east Pacific, accompanied by an oscillation in equatorial thermocline depth that is characterized by a phase shift of about 90{degrees} across the basin, with west leading east. Simulated interannual variability is weaker than observed in both simulations. One of these is dominated by the QB, the other by the QQ mode, although the two differ only in details of the surface-layer parameterizations. 42 refs., 19 figs., 2 tabs.

Robertson, A.W.; Ma, C.C.; Ghil, M. [Univ. of California, Los Angeles, CA (United States)] [and others

1995-05-01T23:59:59.000Z

390

Constructing a coherent long-term global total ozone climatology from the BUV, MFR, and SBUV/TOMS data sets  

Science Conference Proceedings (OSTI)

The backscatter ultraviolet spectrometer (BUV) aboard the NIMBUS 4 satellite provided global ozone data until mid-1977. The Total Ozone Mapping Spectrometer (TOMS) and Solar Backscattered Ultraviolet (SBUV) instrument aboard the NIMBUS 7 satellite began providing global ozone in November 1978. The only satellite derived global total ozone data available between the termination of the BUV data and the startup of the SBUV/TOMS data is that from the Multichannel Filter Radiometer (MFR) instrument aboard the Defense Meteorological Satellite Program (DMSP) series of satellites. The MFR and the SBUV/TOMS data are compared during the data overlap period in order to determine how well the MFR data might be used to represent the SBUV/TOMS and BUV data during the data gap period. 5 refs., 3 figs., 3 tabs.

Ellis, J.S.; Luther, F.M.

1986-02-01T23:59:59.000Z

391

LLE review, volume 73. Quarterly report, October 1997--December 1997  

SciTech Connect

This progress report contains discussion on the following topics: A high-bandwidth electrical-waveform generator based on aperture-coupled striplines for OMEGA pulse-shaping applications; sweep deflection circuit development using computer-aided circuit design for the OMEGA multichannel streak camera; D-{sup 3}He protons as a diagnostic for target {rho}R; growth rates of the ablative Rayleigh-Taylor instability in inertial confinement fusion; three-dimensional analysis of the power transfer between crossed laser beams; characterization of freestanding polymer films for application in 351-nm, high-peak-power laser systems; subsurface damage in microgrinding optical glasses; bound-abrasive polishers for optical glass; and color gamut of cholesteric liquid crystal films and flakes by standard colorimetry.

NONE

1998-04-01T23:59:59.000Z

392

Description, field test and data analysis of a controlled-source EM system (EM-60). [Leach Hot Springs, Grass Valley  

DOE Green Energy (OSTI)

The three sections describe the transmitter, the receiver, and data interpretations and indicate the advances made toward the development of a large moment electromagnetic (EM) system employing a magnetic dipole source. A brief description is given of the EM-60 transmitter, its general design, and the consideration involved in the selection of a practical coil size and weight for routine field operations. A programmable, multichannel, multi-frequency, phase-sensitive receiver is described. A field test of the EM-60, the data analysis and interpretation procedures, and a comparison between the survey results and the results obtained using other electrical techniques are presented. The Leach Hot Springs area in Grass Valley, Pershing County, Nevada, was chosen for the first field site at which the entire system would be tested. The field tests showed the system capable of obtaining well-defined sounding curves (amplitude and phase of magnetic fields) from 1 kHz down to 0.1 Hz. (MHR)

Morrison, H.F.; Goldstein, N.E.; Hoversten, M.; Oppliger, G.; Riveros, C.

1978-10-01T23:59:59.000Z

393

Large scale integration based, signal processor-its application and possible evolution  

Science Conference Proceedings (OSTI)

The micro-vector processor (MVP) is designed for applications ranging from expendable single-processor weapons and buoys to large multiprocessor federated systems. Multiple applications, easy reprogrammability, and low-power operation were achieved with an architecture that provides high throughput at moderate clock rates and maximum use of lsi circuts. The MVP software design includes support for both application programming in high-level language and implementation of signal-processing algorithms in a symbolic microprogramming language. These two programmability levels reduce software costs for new applications and for changing requirements. Two examples are used to illustrate MVP applications: cruise missile guidance and a multichannel acoustic beamformer. The MVP architecture, or some close derivative, is considered suitable for reimplementation in very large-scale integration. 2 references.

Harland, W.L.; Carvell, R. Jr.

1981-01-01T23:59:59.000Z

394

The first photon shutter development for APS insertion device beamline front ends  

Science Conference Proceedings (OSTI)

One of the most critical components on the Advanced Photon Source (APS) insertion device (ID) beamline front ends is the first photon shutter. It operates in two modes to fully intercept the high total power and high-heat flux ID photon beam in seconds (normal mode) or in less than 100 ms (emergency fast mode). It is designed to operate in ultra high vacuum (UHV). The design incorporates a multi-channel rectangular bar, bent in a ``hockey stick`` configuration, with two-point suspension. The flanged end is an articulated bellows with rolling hinges. The actuation end is a spring-assisted, pneumatic fail-safe flexural pivot type. The coolant (water) channels incorporate brazed copper foam to enhance the heat transfer, a tube technology particular to the APS. The design development, and material aspects, as well as the extensive thermal and vibrational analyses in support of the design, are presented in this paper.

Shu, Deming; Nian, H.L.T.; Wang, Zhibi; Collins, J.T.; Ryding, D.G.; Kuzay, T.M.

1992-09-01T23:59:59.000Z

395

The first photon shutter development for APS insertion device beamline front ends  

Science Conference Proceedings (OSTI)

One of the most critical components on the Advanced Photon Source (APS) insertion device (ID) beamline front ends is the first photon shutter. It operates in two modes to fully intercept the high total power and high-heat flux ID photon beam in seconds (normal mode) or in less than 100 ms (emergency fast mode). It is designed to operate in ultra high vacuum (UHV). The design incorporates a multi-channel rectangular bar, bent in a hockey stick'' configuration, with two-point suspension. The flanged end is an articulated bellows with rolling hinges. The actuation end is a spring-assisted, pneumatic fail-safe flexural pivot type. The coolant (water) channels incorporate brazed copper foam to enhance the heat transfer, a tube technology particular to the APS. The design development, and material aspects, as well as the extensive thermal and vibrational analyses in support of the design, are presented in this paper.

Shu, Deming; Nian, H.L.T.; Wang, Zhibi; Collins, J.T.; Ryding, D.G.; Kuzay, T.M.

1992-01-01T23:59:59.000Z

396

E parallel B canted detector neutral-particle spectrometer  

DOE Green Energy (OSTI)

A multichannel, mass-discriminating, neutral-particle spectrometer using parallel E and B analyzer fields has been operational on the Doublet III tokamak. The device records 60 energy channels each of hydrogen and deuterium, simultaneously, during a shot with a dynamic range in energy of greater than 20. Its unique feature is a microchannel plate detector plane set at an angle to the exit face of the magnet. This angled detector plane linearizes the columns of each mass which simplifies the detector design, and permits the magnet gap to be very small. The narrow gap minimizes figure field effects on particle trajectories and simplifies power supply and cooling design. Details are given on the design, calibration, and instrumentation of the device, as well as on its operation and experimental results.

Armentrout, C.J.; Bramson, G.; Evanko, R.

1985-11-01T23:59:59.000Z

397

SPARSE FARADAY ROTATION MEASURE SYNTHESIS  

Science Conference Proceedings (OSTI)

Faraday rotation measure synthesis is a method for analyzing multichannel polarized radio emissions, and it has emerged as an important tool in the study of Galactic and extragalactic magnetic fields. The method requires the recovery of the Faraday dispersion function from measurements restricted to limited wavelength ranges, which is an ill-conditioned deconvolution problem. Here, we discuss a recovery method that assumes a sparse approximation of the Faraday dispersion function in an overcomplete dictionary of functions. We discuss the general case when both thin and thick components are included in the model, and we present the implementation of a greedy deconvolution algorithm. We illustrate the method with several numerical simulations that emphasize the effect of the covered range and sampling resolution in the Faraday depth space, and the effect of noise on the observed data.

Andrecut, M.; Stil, J. M.; Taylor, A. R. [Institute for Space Imaging Science, Department of Physics and Astronomy, University of Calgary, Calgary, Alberta T2N 1N4 (Canada)

2012-02-15T23:59:59.000Z

398

COMSOL-based Multiphysics Simulations to Support HFIR s Conversion to LEU Fuel  

Science Conference Proceedings (OSTI)

In this paper, development of at least one form of the COMSOL-based modeling framework for the HFIR is presented, key simulation steps are identified and several milestones achieved towards a coupled multi-physics capability are highlighted. COMSOL-based multi-physics simulation capability is able to answer the need for predictive 3D simulations of HFIR s involute plate and channels. Step-by-step development and analyses of the COMSOL models for the single and multi-channels will lead towards the desired full-core simulation capability for the HFIR. With very few experiments planned to support the conversion process, these 3D simulations will become the basis for the nuclear safety analysis of the HFIR s LEU fuel core.

Jain, Prashant K [ORNL; Freels, James D [ORNL; Cook, David Howard [ORNL

2011-01-01T23:59:59.000Z

399

Real-time MSE measurements for current profile control on KSTAR  

SciTech Connect

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

400

'Optical' soft x-ray arrays for fluctuation diagnostics in magnetic fusion energy experiments  

Science Conference Proceedings (OSTI)

We are developing large pixel count, fast ({>=}100 kHz) and continuously sampling soft x-ray (SXR) array for the diagnosis of magnetohydrodynamics (MHD) and turbulent fluctuations in magnetic fusion energy plasmas. The arrays are based on efficient scintillators, high thoughput multiclad fiber optics, and multichannel light amplification and integration. Compared to conventional x-ray diode arrays, such systems can provide vastly increased spatial coverage, and access to difficult locations with small neutron noise and damage. An eight-channel array has been built using columnar CsI:Tl as an SXR converter and a multianode photomultiplier tube as photoamplifier. The overall system efficiency is measured using laboratory SXR sources, while the time response and signal-to-noise performance have been evaluated by recording MHD activity from the spherical tori (ST) Current Drive Experiment-Upgrade and National Spherical Torus Experiment, both at Princeton Plasma Physics Laboratory.

Delgado-Aparicio, L.F.; Stutman, D.; Tritz, K.; Finkenthal, M.; Kaita, R.; Roquemore, L.; Johnson, D.; Majeski, R. [Johns Hopkins University, Department of Physics and Astronomy, Plasma Spectroscopy Group, Bloomberg Center 3400 N. Charles Street, Baltimore, Maryland 21218 (United States); Princeton University Plasma Physics Laboratory, P. O. Box 451, Princeton, New Jersey 08543 (United States)

2004-10-01T23:59:59.000Z

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.


401

Geographic Information Systems Applications on an ATM-Based Distributed High Performance Computing System  

E-Print Network (OSTI)

. We present a distributed geographic information system (DGIS) built on a distributed high performance computing environment using a number of software infrastructural building blocks and computational resources interconnected by an ATM-based broadband network. Archiving, access and processing of scientific data are discussed in the context of geographic and environmental applications with special emphasis on the potential for local-area weather, agriculture, soil and land management products. Software technologies such as tiling and caching techniques can be used to optimise storage requirements and response time for applications requiring very large data sets such as multi-channel satellite data. Distributed High Performance Computing hardware technology underpins our proposed system. In particular, we discuss the capabilities of a distributed hardware environment incorporating: high bandwidth communications networks such as Telstra's Experimental Broadband Network (EBN); large capa...

November Hawick

1997-01-01T23:59:59.000Z

402

Optimization of plasma diagnostics using Bayesian probability theory  

SciTech Connect

The diagnostic set-up for Wendelstein 7-X, a magnetic fusion device presently under construction, is currently in the design process to optimize the outcome under given technical constraints. Compared to traditional design approaches, Bayesian Experimental Design (BED) allows to optimize with respect to physical motivated design criterions. It aims to find the optimal design by maximizing an expected utility function that quantifies the goals of the experiment. The expectation marginalizes over the uncertain physical parameters and the possible values of future data. The approach presented here bases on maximization of an information measure (Kullback-Leibler entropy). As an example, the optimization of an infrared multichannel interferometer is shown in detail. Design aspects like the impact of technical restrictions are discussed.

Dreier, H.; Dinklage, A.; Hirsch, M.; Kornejew, P. [Max-Planck-Institut fuer Plasmaphysik, EURATOM-Association, Wendelsteinstr. 1, 17491 Greifswald (Germany); Fischer, R. [Boltzmannstr. 2, 85748 Garching (Germany)

2006-11-29T23:59:59.000Z

403

Frequency Scanned Interferometry for ILC Tracker Alignment  

E-Print Network (OSTI)

In this paper, we report high-precision absolute distance and vibration measurements performed with frequency scanned interferometry. Absolute distance was determined by counting the interference fringes produced while scanning the laser frequency. High-finesse Fabry-Perot interferometers were used to determine frequency changes during scanning. A dual-laser scanning technique was used to cancel drift errors to improve the absolute distance measurement precision. A new dual-channel FSI demonstration system is also presented which is an interim stage toward practical application of multi-channel distance measurement. Under realistic conditions, a precision of 0.3 microns was achieved for an absolute distance of 0.57 meters. A possible optical alignment system for a silicon tracker is also presented.

Hai-Jun Yang; Tianxiang Chen; Keith Riles

2011-09-12T23:59:59.000Z

404

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

405

Deep Trek Re-configurable Processor for Data Acquisition (RPDA)  

Science Conference Proceedings (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

406

Quasifree Kaon Photoproduction on Nuclei  

E-Print Network (OSTI)

Investigations of the quasifree reaction A$(\\gamma, K Y)$B are presented in the distorted wave impulse approximation (DWIA). For this purpose, we present a revised tree-level model of elementary kaon photoproduction that incorporates hadronic form factors consistent with gauge invariance, uses SU(3) values for the Born couplings and uses resonances consistent with multi-channel analyses. The potential of exclusive quasifree kaon photoproduction on nuclei to reveal details of the hyperon-nucleus interaction is examined. Detailed predictions for the coincidence cross section, the photon asymmetry, and the hyperon polarization and their sensitivities to the ingredients of the model are obtained for all six production channels. Under selected kinematics these observables are found to be sensitive to the hyperon-nucleus final state interaction. Some polarization observables are found to be insensitive to distortion effects, making them ideal tools to search for possible medium modifications of the elementary amplitude.

F. X. Lee; T. Mart; C. Bennhold; H. Haberzettl; L. E. Wright

1999-07-30T23:59:59.000Z

407

An Alternative View of the Dynamical Origin of the P11 Nucleon Resonances: Results from the Excited Baryon Analysis Center  

Science Conference Proceedings (OSTI)

We present an alternative interpretation for the dynamical origin of the P{sub 11} nucleon resonances, which results from the dynamical coupled-channels analysis at Excited Baryon Analysis Center of Jefferson Lab. The results indicate the crucial role of the multichannel reaction dynamics in determining the N* spectrum. An understanding of the spectrum and structure of the excited nucleon (N*) states is a fundamental challenge in the hadron physics. The N* states, however, couple strongly to the meson-baryon continuum states and appear only as resonance states in the {gamma}N and {pi}N reactions. One can expect from such strong couplings that the (multichannel) reaction dynamics will affect significantly the N* states and cannot be neglected in extracting the N* parameters from the data and giving physical interpretations. It is thus well recognized nowadays that a comprehensive study of all relevant meson production reactions with {pi}N,{eta}N,{pi}{pi}N,KY, {hor_ellipsis} final states is necessary for a reliable extraction of the N* parameters. To address this challenging issue, the Excited Baryon Analysis Center (EBAC) of Jefferson Lab has been conducting the comprehensive analysis of the world data of {gamma}N,{pi}N {yields} {pi}N,{eta}N,{pi}{pi}N,KY, {hor_ellipsis} reactions systematically, covering the wide energy and kinematic regions. The analysis is pursued with a dynamical coupled-channels (DCC) model, the EBAC-DCC model, within which the unitarity among relevant meson-baryon channels, including the three-body {pi}{pi}N channel, is fully taken into account.

Hiroyuki Kamano

2012-04-01T23:59:59.000Z

408

EIA - Electricity Data - Energy Information Administration  

U.S. Energy Information Administration (EIA)

Energy Information Administration - EIA ... Table 1.12.A. Net Generation from Nuclear Energy: by State, by Sector, August 2013 and 2012 (Thousand Megawatthours)

409

TAC Entity Linking by Performing Full-document Entity ...  

Science Conference Proceedings (OSTI)

... few major global economies that will see respectable GDP growth this ... entities per topic: 12 ... a request by the International Atomic Energy Agency to ...

2012-02-27T23:59:59.000Z

410

Annual Energy Review - U.S. Energy Information Administration ...  

U.S. Energy Information Administration (EIA)

Crude oil, gasoline, heating oil, diesel, propane, ... 8.12a Electric Noncoincident Peak Load and Capacity Margin: Summer Peak Period, 1986 PDF XLS ...

411

Annual Energy Review - U.S. Energy Information Administration ...  

U.S. Energy Information Administration (EIA)

1.10 Cooling Degree-Days by Census Division, 1949 PDF XLS ... 8.12a Electric Noncoincident Peak Load and Capacity Margin: Summer Peak Period, 1986

412

Annual Energy Review - Energy Information Administration  

U.S. Energy Information Administration (EIA)

1.10 Cooling Degree-Days by Census Division, 1949 PDF XLS ... 8.12a Electric Noncoincident Peak Load and Capacity Margin: Summer Peak Period, 1986

413

Marginalized Monitoring: Adaptively Managing Urban Stormwater  

E-Print Network (OSTI)

A Case Study from Racine, Wisconsin, USA 12 A QUATIC Eand harbor - Milwaukee, Wisconsin. E. coli , Enterococcus,water in Racine, Wisconsin. Human-specific Bacteroides , E.

Scanlan, Melissa K; Tai, Stephanie

2013-01-01T23:59:59.000Z

414

596.ps - Optimization Online  

E-Print Network (OSTI)

Department of Mathematics, National University of Singapore, 2 Science ...... [6] B . Borchers, SDPLIB 1.2, a library of semide nite programming test problems,.

415

A First Order Method for Finding Minimal Norm-Like Solutions of ...  

E-Print Network (OSTI)

Introductory Lectures on Convex Optimization. Kluwer, Boston, 2004. [12] A. N. Tikhonov and V. Y. Arsenin. Solution of Ill-Posed Problems. Washington, DC:.

416

A Lithium Experiment in the Program of Solar Neutrino Research  

E-Print Network (OSTI)

The experiments sensitive to pp-neutrinos from the Sun are very perspective for the precise measurement of a mixing angle $\\theta_{12}$. A $\

A. Kopylov; I. Orekhov; V. Petukhov; A. Solomatin

2006-01-12T23:59:59.000Z

417

No Slide Title  

Science Conference Proceedings (OSTI)

... A. Borgschulte et al. Journal of Catalysis 239 (2006) 263271 Page 12. ... A. Borgschulte et al. Journal of Catalysis 239 (2006) 263271 ...

2012-10-04T23:59:59.000Z

418

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

419

Diverse Firewall Design Alex X. Liu Mohamed G. Gouda  

E-Print Network (OSTI)

and Privacy, pages 17­31, 1999. [12] A. Condor and G. Hinton. Fault tolerant and fail-safe de- sign of candu

Liu, Alex X.

420

Mechanochemical Behavior of BaNd 2 Ti 4 O 12 Powder in Ball ...  

Science Conference Proceedings (OSTI)

When ball milling BaNd2Ti4O12, a high slurry viscosity reduces the capability of the grinding media to shear, and...

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

Reaction Kinetics Between Fiber and Matrix Components in Metal ...  

Science Conference Proceedings (OSTI)

parabolic rate constants for the total growth of the reaction zone and the component of the reaction zone which displaces the fiber (12). (a). (b). Figure 4 - Cross-...

422

Precision Measurement of Neutrino Oscillation Parameters with KamLAND  

E-Print Network (OSTI)

Likelihood profile projection onto the sin 2 ? 13Likelihood profile projections onto the ?m 221 - and ? 12 -A.3 Likelihood profile projection onto the sin 2 ? 13 axis

O'Donnell, Thomas

2013-01-01T23:59:59.000Z

423

Fusion systems and biset functors via ghost algebras  

E-Print Network (OSTI)

2.2 Fusion Preserving1 Background 1.1 Fusion System Basics . . . . . . 1.2A. Craven. The theory of fusion systems. Vol. 131. Cambridge

O'Hare, Shawn Michael

2013-01-01T23:59:59.000Z

424

Modeling Electric Vehicle Benefits Connected to Smart Grids  

E-Print Network (OSTI)

Benefits Connected to Smart Grids M. Stadler 1,2,a , C.Benefits Connected to Smart Grids Michael Stadler , Chris

Stadler, Michael

2012-01-01T23:59:59.000Z

425

A lifestyle-based scenario, Energy Policy A lifestyle-based scenario for U.S. buildings  

E-Print Network (OSTI)

A lifestyle-based scenario, Energy Policy A lifestyle-based scenario for U.S. buildings the speculative nature of the #12;A lifestyle-based scenario, Energy Policy exercise, the rationale was to broaden implications of these changes, and how might we create energy policies to 2 #12;A lifestyle-based scenario

Diamond, Richard

426

October 2007 BWXTymes  

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

7 J a w s o f l i f e a t Y- 12 , p g . 4 , * A l p h a b e t s o u p , p g . 6 * Y- 12 a w a r d w i n n e r s , p g . 8 Y-12: a good environmental steward The Y-12 National...

427

The Third Claude E. Shannon Memorial Lecture  

E-Print Network (OSTI)

(Physics) · Aperture · Frequency · Power · Shannon (Mathematics) · Error-Correction · Data Compression #12 It Worth the Effort? #12;"Frequently the messages have meaning" #12;A Tour of the Solar System. #12;A Tour of the Solar System. UCSD April 29, 2005 Ludwig van Beethoven, Moonlight Sonata Daniel Barenboim, pianist #12

Adolphs, Ralph

428

Detection of bacterial endospores by means of ultrafast coherent raman spectroscopy  

E-Print Network (OSTI)

This work is devoted to formulation and development of a laser spectroscopic technique for rapid detection of biohazards, such as Bacillus anthracis spores. Coherent anti-Stokes Raman scattering (CARS) is used as an underlying process for active retrieval of species-specific characteristics of an analyte. Vibrational modes of constituent molecules are Raman-excited by a pair of ultrashort, femtosecond laser pulses, and then probed through inelastic scattering of a third, time-delayed laser field. We first employ the already known time-resolved CARS technique. We apply it to the spectroscopy of easy-to-handle methanol-water mixtures, and then continue building our expertise on solutions of dipicolinic acid (DPA) and its salts, which happen to be marker molecules for bacterial spores. Various acquisition schemes are evaluated, and the preference is given to multi-channel frequency-resolved detection, when the whole CARS spectrum is recorded as a function of the probe pulse delay. We demonstrate a simple detection algorithm that manages to differentiate DPA solution from common interferents. We investigate experimentally the advantages and disadvantages of near-resonant probing of the excited molecular coherence, and finally observe the indicative backscattered CARS signal from DPA and NaDPA powders. The possibility of selective Raman excitation via pulse shaping of the preparation pulses is also demonstrated. The analysis of time-resolved CARS experiments on powders and B. subtilis spores, a harmless surrogate for B. anthracis, facilitates the formulation of a new approach, where we take full advantage of the multi-channel frequency-resolved acquisition and spectrally discriminate the Raman-resonant CARS signal from the background due to other instantaneous four-wave mixing (FWM) processes. Using narrowband probing, we decrease the magnitude of the nonresonant FWM, which is further suppressed by the timing of the laser pulses. The devised technique, referred to as hybrid CARS, leads to a single-shot detection of as few as 104 bacterial spores, bringing CARS spectroscopy to the forefront of potential candidates for real-time biohazard detection. It also gives promise to many other applications of CARS, hindered so far by the presence of the overwhelming nonresonant FWM background, mentioned above.

Pestov, Dmitry Sergeyevich

2008-05-01T23:59:59.000Z

429

A New Measurement of the $?^0$ Radiative Decay Width  

E-Print Network (OSTI)

High precision measurements of the differential cross sections for $\\pi^0$ photoproduction at forward angles for two nuclei, $^{12}$C and $^{208}$Pb, have been performed for incident photon energies of 4.9 - 5.5 GeV to extract the ${\\pi^0 \\to \\gamma\\gamma}$ decay width. The experiment was done at Jefferson Lab using the Hall B photon tagger and a high-resolution multichannel calorimeter. The ${\\pi^0 \\to \\gamma\\gamma}$ decay width was extracted by fitting the measured cross sections using recently updated theoretical models for the process. The resulting value for the decay width is $\\Gamma{(\\pi^0 \\to \\gamma\\gamma)} = 7.82 \\pm 0.14 ~({\\rm stat.}) \\pm 0.17 ~({\\rm syst.}) ~{\\rm eV}$. With the 2.8% total uncertainty, this result is a factor of 2.5 more precise than the current PDG average of this fundamental quantity and it is consistent with current theoretical predictions.

I. Larin; D. McNulty; E. Clinton; P. Ambrozewicz; D. Lawrence; I. Nakagawa; Y. Prok; A. Teymurazyan; A. Ahmidouch; A. Asratyan; K. Baker; L. Benton; A. M. Bernstein; V. Burkert; P. Cole; P. Collins; D. Dale; S. Danagoulian; G. Davidenko; R. Demirchyan; A. Deur; A. Dolgolenko; G. Dzyubenko; R. Ent; A. Evdokimov; J. Feng; M. Gabrielyan; L. Gan; A. Gasparian; S. Gevorkyan; A. Glamazdin; V. Goryachev; V. Gyurjyan; K. Hardy; J. He; M. Ito; L. Jiang; D. Kashy; M. Khandaker; P. Kingsberry; A. Kolarkar; M. Konchatnyi; A. Korchin; W. Korsch; S. Kowalski; M. Kubantsev; V. Kubarovsky; X. Li; P. Martel; V. Matveev; B. Mecking; B. Milbrath; R. Minehart; R. Miskimen; V. Mochalov; S. Mtingwa; S. Overby; E. Pasyuk; M. Payen; R. Pedroni; B. Ritchie; T. E. Rodrigues; C. Salgado; A. Shahinyan; A. Sitnikov; D. Sober; S. Stepanyan; W. Stephens; J. Underwood; A. Vasiliev; V. Vishnyakov; M. Wood; S. Zhou

2010-09-09T23:59:59.000Z

430

Pulsed, Photonuclear-induced, Neutron Measurements of Nuclear Materials with Composite Shielding  

SciTech Connect

Active measurements were performed using a 10-MeV electron accelerator with inspection objects containing various nuclear and nonnuclear materials available at the Idaho National Laboratorys Zero Power Physics Reactor (ZPPR) facility. The inspection objects were assembled from ZPPR reactor plate materials to evaluate the measurement technologies for the characterization of plutonium, depleted uranium or highly enriched uranium shielded by both nuclear and non-nuclear materials. A series of pulsed photonuclear, time-correlated measurements were performed with unshielded calibration materials and then compared with the more complex composite shield configurations. The measurements used multiple 3He detectors that are designed to detect fission neutrons between pulses of an electron linear accelerator. The accelerator produced 10-MeV bremsstrahlung X-rays at a repetition rate of 125 Hz (8 ms between pulses) with a 4-us pulse width. All inspected objects were positioned on beam centerline and 100 cm from the X-ray source. The time-correlated data was collected in parallel using both a Los Alamos National Laboratory-designed list-mode acquisition system and a commercial multichannel scaler analyzer. A combination of different measurement configurations and data analysis methods enabled the identification of each object. This paper describes the experimental configuration, the ZPPR inspection objects used, and the various measurement and analysis results for each inspected object.

James Jones; Kevin Haskell; Rich Waston; William Geist; Jonathan Thron; Corey Freeman; Martyn Swinhoe; Seth McConchie; Eric Sword; Lee Montierth; John Zabriskie

2011-07-01T23:59:59.000Z

431

The Evolving Magnetic Scales of the Outer Solar Atmosphere and Their Potential Impact on Heliospheric Turbulence  

E-Print Network (OSTI)

The presence of turbulent phenomena in the outer solar atmosphere is a given. However, because we are reduced to remotely sensing the atmosphere of a star with instruments of limited spatial and/or spectral resolution, we can only infer the physical progression from macroscopic to microscopic phenomena. Even so, we know that many, if not all, of the turbulent phenomena that pervade interplanetary space have physical origins at the Sun and so in this brief article we consider some recent measurements which point to sustained potential source(s) of heliospheric turbulence in the magnetic and thermal domains. In particular, we look at the scales of magnetism that are imprinted on the outer solar atmosphere by the relentless magneto-convection of the solar interior and combine state-of-the-art observations from the Solar Dynamics Observatory (SDO) and the Coronal Multi-channel Polarimeter (CoMP) which are beginning to hint at the origins of the wave/plasma interplay prevalent closer to the Earth. While linking th...

McIntosh, Scott W; Threlfall, James; De Moortel, Ineke; Leamon, Robert J; Tian, Hui

2013-01-01T23:59:59.000Z

432

Side-by-Side Testing of Commercial Office Lighting Systems: Two-lamp Fluorescent Fixtures  

E-Print Network (OSTI)

Lighting systems in commercial office buildings are primary determinants of building energy use. In warmer climates, lighting energy use has important implications for building cooling loads as well as those directly associated with illumination tasks. To research the comparative performance of conventional and advanced office lighting systems, Florida Solar Energy Center (FSEC) set up the Lighting Flexible Test Facility (LFTF) which allows side-by-side comparison of lighting options in two otherwise identical 2.7 m x 3.7 m (9' x 12') south facing offices. The ceiling of the LFTF contains 0.61 m x 1.2 m (2' x 4') recessed fluorescent fixtures designed to be easily changed. Differing lighting systems were comparatively tested against each other over weeklong periods. Data on power consumption (watts), power quality (power factor), work-plane interior lighting levels (lux), bulb-wall, fixture and plenum temperatures were recorded every 15 minutes on a multi-channel data logger. This data allows realistic analysis of comparative lighting system performance including interactions with daylighting.

Parker, D. S.; Schrum, L.; Sonne, J. K.; Stedman, T. C.

1996-01-01T23:59:59.000Z

433

Efficiency Calibration Using HEU Standards of 2-Inch by 2-Inch NaI Detector  

SciTech Connect

The Analytical Development Section of SRTC was requested by the Facilities Disposition Division (FDD) to determine the holdup of highly enriched uranium (HEU) in the 321-M facility as part of an overall deactivation project of the facility. The 321-M facility was used to fabricate enriched uranium fuel assemblies, lithium-aluminum target tubes, neptunium assemblies, and miscellaneous components for the production reactors. The facility also includes the 324-M storage building and the passageway connecting it to 321-M. The results of the holdup assays are essential for determining compliance with the solid waste Waste Acceptance Criteria, Material Control and Accountability, and to meet criticality safety controls. Two measurement systems will be used to determine HEU holdup: One is a portable EG and G Dart system that contains Gamma-Vision software to support a Multichannel Analyzer (MCA) card, high voltage power, and space to store and manipulate multiple 4096-channel gamma-ray spect ra. The other is a 2-inch x 2-inch NaI crystal with an MCA that uses a portable computer with a Canberra NaI plus card installed. This card converts the PC to a full function MCA and contains the ancillary electronics, high voltage power supply and amplifier, required for data acquisition. This report will discuss the calibration of the 2-inch x 2-inch NaI detector.

Dewberry, R. A.

2000-10-24T23:59:59.000Z

434

High-magnetic-field MHD-generator program. Quarterly report, January 1, 1981-March 31, 1981  

DOE Green Energy (OSTI)

Progress in an experimental and theoretical program designed to investigate MHD channel phenomena which are important at high magnetic fields is reported. The areas of research include nonuniformity effects, boundary layers, Hall field breakdown, the effects of electrode configuration and current concentrations, and studies of steady-state combustion disk and linear channels in an existing 6 Tesla magnet of small dimensions. In the study of the effects of nonuniformities, experiments have been performed to test a multi-channel, fiber optics diagnostic system that yields time-resolved temperature profiles in an MHD channel. For the study of magneto-acoustic fluctuation phenomena, a one-dimensional model has been developed to describe the performance of a non-ideal MHD generator with a generalized electrical configuration. The installation of the hardware for the data acquisition and reduction of the laser Doppler velocimeter data, to be used in the study of turbulence suppression in a magnetic field, has been nearly completed. A two-dimensional MHD computer code has been developed which predicts the dependence on electrode and insulator dimensions of the onset of interelectrode Hall field breakdown. Calculations have been performed of the effects of nonuniformities on the flow and electrical behavior of baseload-sized disk generators.

None

1981-04-01T23:59:59.000Z

435

High-magnetic-field MHD-generator program. Quarterly report, April 1, 1981-June 30, 1981  

DOE Green Energy (OSTI)

Progress in an experimental and theoretical program designed to investigate MHD channel phenomena which are important at high magnetic fields is described. The areas of research include nonuniformity effects, boundary layers, Hall field breakdown, the effects of electrode configuration and current concentrations, and studies of steady-state combustion disk and linear channels in an existing 6 Tesla magnet of small dimensions. In the study of the effects of nonuniformities, experiments have been performed to test a multi-channel, fiber optics diagnostic system that yields time-resolved temperature profiles in an MHD channel. For the study of magneto-acoustic fluctuation phenomena, a one-dimensional model has been developed to describe the performance of a non-ideal MHD generator with a generalized electrical configuration. The installation of the hardware for the data acquisition and reduction of the laser Doppler velocimeter data, to be used in the study of turbulence suppression in a magnetic field, has been nearly completed and preliminary software has been written. A two-dimensional MHD computer code has been developed which predicts the dependence on electrode and insulator dimensions of the onset of interelectrode Hall field breakdown, as initiated either by breakdown in the insulator or in the plasma. There is good agreement between calculation and measurements. Calculations have been performed of the effects of nonuniformities on the flow and electrical behavior of baseload-sized disk generators. Also, predictions of the performance of baseload inflow disk generators have been calculated and compared with linear generators.

Kruger, C.H.; Eustis, R.H.; Mitchner, M.; Self, S.A.; Koester, J.K.; Nakamura, T.

1981-07-01T23:59:59.000Z

436

First performances of the GOLF-NG instrumental prototype observing the Sun in Tenerife  

E-Print Network (OSTI)

The primary challenge of GOLF-NG (Global Oscillations at Low Frequency New Generation) is the detection of the low-frequency solar gravity and acoustic modes, as well as the possibility to measure the high-frequency chromospheric modes. On June 8th 2008, the first sunlight observations with the multichannel resonant GOLF-NG prototype spectrometer were obtained at the Observatorio del Teide (Tenerife). The instrument performs integrated (Sun-as-a-star), Doppler velocity measurements, simultaneously at eight different heights in the D1 sodium line profile, corresponding to photospheric and chromospheric layers of the solar atmosphere. In order to study its performances, to validate the conceived strategy, and to estimate the necessary improvements, this prototype has been running on a daily basis over the whole summer of 2008 at the Observatorio del Teide. We present here the results of the first GOLF-NG observations, clearly showing the characteristics of the 5-minute oscillatory signal at different heights in the solar atmosphere. We compare these signals with simultaneous observations from GOLF/SOHO and from the Mark-I instrument -- a node of the BiSON network, operating at the same site.

D. Salabert; S. Turck-Chieze; J. C. Barriere; P. H. Carton; P. Daniel-Thomas; A. Delbart; R. A. Garcia; R. Granelli; S. J. Jimenez-Reyes; C. Lahonde-Hamdoun; D. Loiseau; S. Mathur; F. Nunio; P. L. Palle; Y. Piret; J. M. Robillot; R. Simoniello

2008-10-19T23:59:59.000Z

437

Next Generation Trusted Radiation Identification System (NG-TRIS).  

SciTech Connect

The original Trusted Radiation Identification System (TRIS) was developed from 1999-2001, featuring information barrier technology to collect gamma radiation template measurements useful for arms control regime operations. The first TRIS design relied upon a multichannel analyzer (MCA) that was external to the protected volume of the system enclosure, undesirable from a system security perspective. An internal complex programmable logic device (CPLD) contained data which was not subject to software authentication. Physical authentication of the TRIS instrument case was performed by a sensitive but slow eddy-current inspection method. This paper describes progress to date for the Next Generation TRIS (NG-TRIS), which improves the TRIS design. We have incorporated the MCA internal to the trusted system volume, achieved full authentication of CPLD data, and have devised rapid methods to authenticate the system enclosure and weld seals of the NG-TRIS enclosure. For a complete discussion of the TRIS system and components upon which NG-TRIS is based, the reader is directed to the comprehensive user's manual and system reference of Seager, et al.

Flynn, Adam J.; Amai, Wendy A.; Merkle, Peter Benedict; Anderson, Lawrence Frederick; Strother, Jerry D.; Weber, Thomas M.; Etzkin, Joshua L.

2010-05-01T23:59:59.000Z

438

b038.dvi  

NLE Websites -- All DOE Office Websites (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)

439

b023.dvi  

NLE Websites -- All DOE Office Websites (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

440

Hadamard multimode optical imaging transceiver  

SciTech Connect

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

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

A Low-Power 9-bit Pipelined CMOS ADC with Amplifier and Comparator Sharing Technique  

E-Print Network (OSTI)

This paper describes a pipelined analog-to-digital converter (ADC) employing a power and area efficient architecture. The adjacent stages of a pipeline share operational amplifiers. In order to keep accuracy of the amplifiers in the first stages, they use a partially sharing technique. The feature of the proposed scheme is that it also shares the comparators. The capacitors of the first stages of a pipeline are scaled down along a pipeline for a further reducing the chip area and its power consumption. A 9-bit 20-MSamples/s ADC, intended for use in multi-channel mixed-signal chips, has been fabricated via Europractice in a 180-nm CMOS process from UMC. The prototype ADC shows a spurious-free dynamic range of 58.5 dB at a sample rate of 20 MSamples/s, when a 400 kHz input signal with a swing of 1 dB below full scale is applied. The effective number of bits is 8.0 at the same conditions. ADC occupies an active area of 0.4 mm2 and dissipates 8.6 mW at a 1.8 V supply.

Bocharov, Yuri; Osipov, Dmitry

2012-01-01T23:59:59.000Z

442

Probabilistic DCS: An RFID reader-toreader anti-collision protocol  

E-Print Network (OSTI)

The wide adoption of Radio Frequency Identification (RFID) for applications requiring a large number of tags and readers makes critical the reader-to-reader collision problem. Various anticollision protocols have been proposed, but the majority require considerable additional resources and costs. Distributed Color System (DCS) is a state-of-the-art protocol based on time division, without noteworthy additional requirements. This paper presents the Probabilistic DCS (PDCS) reader-to-reader anticollision protocol which employs probabilistic collision resolution. Differently from previous time division protocols, PDCS allows multichannel transmissions, according to international RFID regulations. A theoretical analysis is provided in order to clearly identify the behavior of the additional parameter representing the probability. The proposed protocol maintains the features of DCS, achieving more efficiency. Theoretical analysis demonstrates that the number of reader-to-reader collisions after a slot change is decreased by over 30%. The simulation analysis validates the theoretical results, and shows that PDCS reaches better performance than state-of-the-art reader-to-reader anticollision protocols. Key words: RFID, reader-to-reader collision 1.

Renato Ferrero; Bartolomeo Montrucchio; Maurizio Rebaudengo

2010-01-01T23:59:59.000Z

443

Stainless Steel 18-10 CO2 Laser Welding And Plasma Diagnostics  

Science Conference Proceedings (OSTI)

The welding of materials by CO2 laser took significant considerations in industry, for the reason of the quality of the carried out weldings, and for other many advantages, but the automation of the welding operation requires a control system in real time. The operation of welding is an operation of interaction between the radiation (laser), and the matter (welded part), which is characterized by the vaporization of the matter, formation of the keyhole in material, and appearance of plasma over the material. This study relates to the relation between the welding (molten material) and the plasma which is formed on material. The light emitted by plasma during laser welding was recorded by an OMA detector (Optical Multichannel Analyzer) over a wavelength width of 450 A ring . The analysis of this light allows to determine the composition of this plasma, its dimensions, and the state of its energy according to the laser parameters. The welded material is the stainless steel 18-10, it was found that the intensity of the light emitted by plasma depends on laser power, the welding speed, the flow rate of assist gas. The relation between the plasma and the state of the bead were analyzed for on-line monitoring welding.

Amar, Taibi [Department of Mechanical Engineering, University of M'sila (Algeria); Laboratory of Industrial Physics, Thermal centre of INSA of Lyon, CETHIL (France); Michel, Laurent [Laboratory of Industrial Physics, Thermal centre of INSA of Lyon, CETHIL (France)

2008-09-23T23:59:59.000Z

444

Global warming and global dioxide emission: An empirical study  

Science Conference Proceedings (OSTI)

In this paper, the dynamic relationship between global surface temperature (global warming) and global carbon dioxide emission (CO{sub 2}) is modelled and analyzed by causality and spectral analysis in the time domain and frequency domain, respectively. Historical data of global CO{sub 2} emission and global surface temperature anomalies over 129 years from 1860-1988 are used in this study. The causal relationship between the two phenomena is first examined using the Sim and Granger causality test in the time domain after the data series are filtered by ARIMA models. The Granger causal relationship is further scrutinized and confirmed by cross-spectral and multichannel spectral analysis in the frequency domain. The evidence found from both analyses proves that there is a positive causal relationship between the two variables. The time domain analysis suggests that Granger causality exists between global surface temperature and global CO{sub 2} emission. Further, CO{sub 2} emission causes the change in temperature. The conclusions are further confirmed by the frequency domain analysis, which indicates that the increase in CO{sub 2} emission causes climate warming because a high coherence exists between the two variables. Furthermore, it is proved that climate changes happen after an increase in CO{sub 2} emission, which confirms that the increase in CO{sub 2} emission does cause global warming. 27 refs., 10 figs., 5 tabs.

Linyan Sun [Xian Jiaotong Univ., Shaanxi (China); Wang, M. [Saint Mary`s Univ., Halifax, Nova Scotia (Canada)

1996-04-01T23:59:59.000Z

445

RAMONA-4B a computer code with three-dimensional neutron kinetics for BWR and SBWR system transient - user`s manual  

Science Conference Proceedings (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

446

Characterizing Exoplanets in the Visible and Infrared: A Spectrometer Concept for the EChO Space Mission  

E-Print Network (OSTI)

Transit-spectroscopy of exoplanets is one of the key observational techniques to characterize the extrasolar planet and its atmosphere. The observational challenges of these measurements require dedicated instrumentation and only the space environment allows an undisturbed access to earth-like atmospheric features such as water or carbon-dioxide. Therefore, several exoplanet-specific space missions are currently being studied. One of them is EChO, the Exoplanet Characterization Observatory, which is part of ESA's Cosmic Vision 2015-2025 program, and which is one of four candidates for the M3 launch slot in 2024. In this paper we present the results of our assessment study of the EChO spectrometer, the only science instrument onboard this spacecraft. The instrument is a multi-channel all-reflective dispersive spectrometer, covering the wavelength range from 400 nm to 16 microns simultaneously with a moderately low spectral resolution. We illustrate how the key technical challenge of the EChO mission - the high...

Glauser, A M; Krause, O; Henning, Th; Benneke, B; Bouwman, J; Cubillos, P E; Crossfield, I J M; Detre, H; Ebert, M; Grzinger, U; Gdel, M; Harrington, J; Justtanont, K; Klaas, U; Lenzen, R; Madhusudhan, N; Meyer, M R; Mordasini, C; Mller, F; Ottensamer, R; Plesseria, J -Y; Quanz, S P; Reiners, A; Renotte, E; Rohloff, R -R; Scheithauer, S; Schmid, H M; Schrader, J -R; Seemann, U; Stam, D; Vandenbussche, B; Wehmeier, U

2013-01-01T23:59:59.000Z

447

Validation of the MULCH-II code for thermal-hydraulic safety analysis of the MIT research reactor conversion to LEU  

SciTech Connect

An in-house thermal hydraulics code was developed for the steady-state and loss of primary flow analysis of the MIT Research Reactor (MITR). This code is designated as MULti-CHannel-II or MULCH-II. The MULCH-II code is being used for the MITR LEU conversion design study. Features of the MULCH-II code include a multi-channel analysis, the capability to model the transition from forced to natural convection during a loss of primary flow transient, and the ability to calculate safety limits and limiting safety system settings for licensing applications. This paper describes the validation of the code against PLTEMP/ANL 3.0 for steady-state analysis, and against RELAP5-3D for loss of primary coolant transient analysis. Coolant temperature measurements obtained from loss of primary flow transients as part of the MITR-II startup testing were also used for validating this code. The agreement between MULCH-II and the other computer codes is satisfactory. (author)

Ko, Y.-C. [Nuclear Science and Engineering Department, MIT, Cambridge, MA 02139 (United States); Hu, L.-W. [Nuclear Reactor Laboratory, MIT, Cambridge, MA 02139 (United States)], E-mail: lwhu@mit.edu; Olson, Arne P.; Dunn, Floyd E. [RERTR Program, Argonne National Laboratory, Argonne, IL 60439 (United States)

2008-07-15T23:59:59.000Z

448

Validation of the MULCH-II code for thermal-hydraulic safety analysis of the MIT research reactor conversion to LEU.  

SciTech Connect

An in-house thermal hydraulics code was developed for the steady-state and loss of primary flow analysis of the MIT Research Reactor (MITR). This code is designated as MULti-CHannel-II or MULCH-II. The MULCH-II code is being used for the MITR LEU conversion design study. Features of the MULCH-II code include a multi-channel analysis, the capability to model the transition from forced to natural convection during a loss of primary flow transient, and the ability to calculate safety limits and limiting safety system settings for licensing applications. This paper describes the validation of the code against PLTEMP/ANL 3.0 for steady-state analysis, and against RELAP5-3D for loss of primary coolant transient analysis. Coolant temperature measurements obtained from loss of primary flow transients as part of the MITR-II startup testing were also used for validating this code. The agreement between MULCH-II and the other computer codes is satisfactory.

Ko, Y. C.; Hu, L. W.; Olson, A. P.; Dunn, F. E.; Nuclear Engineering Division; MIT

2007-01-01T23:59:59.000Z

449

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

450

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

451

The CLAS Excited Baryon Program at Jlab  

DOE Green Energy (OSTI)

Nucleons are complex systems of confined quarks and exhibit characteristic spectra of excited states. Highly excited nucleon states are sensitive to details of quark confinement which is poorly understood within Quantum Chromodynamics (QCD), the fundamental theory of strong interactions. Thus, measurements of excited states and the corresponding determination of their properties are needed to come to a better understanding of how confinement works in nucleons. However, the excited states of the nucleon cannot simply be inferred from cleanly separated spectral lines. Quite the contrary, a spectral analysis in nucleon resonance physics is challenging because of the fact that the resonances are broadly overlapping states which decay into a multitude of final states involving mesons and baryons. To provide a consistent and complete picture of an individual nucleon resonance, the various possible production and decay channels must be treated in a multichannel framework that permits separating resonance from background contributions. Very often, resonances reveal themselves more clearly through interference with dominant amplitudes. These interference terms can be isolated via polarization observables. The current CLAS effort is to utilize highly-polarized hydrogen and deuterium targets as well as polarized photon beams toward a complete measurement of a large number of reaction channels.

Volker Crede

2007-10-01T23:59:59.000Z

452

Inelastic shadowing effects in multiple scattering  

SciTech Connect

The projectile--nucleon scattering amplitudes used as input into multiple scattering theories of projectile--nucleus scattering naturally include the effects of coupling to inelastic (i.e., production) channels. We employ a multichannel separable potential to describe the projectile--nucleon interaction and show that within the fixed nucleon framework we can obtain the nuclear elastic scattering amplitude. This includes terms outside the conventional formalisms, corresponding to intermediate propagation in the inelastic channels both above and below inelastic threshold. We refer to this as inelastic shadowing. In a two-channel approximation, we show that knowledge of the projectile--nucleon elastic scattering phase shifts plus specification of the inelastic threshold energy are sufficient to determine the off-shell coupled- channel transition matrix, implying that the nuclear amplitude can be calculated within this model without any detailed information about the inelastic channels. We study this solution quantitatively for some model problems and for pion scattering, with the general result that inelastic shadowing can be significant whenever the elementary interaction has important channel coupling. For pion scattering in the energy regime characterized by strongly absorptive resonance, we find, for example, that the effect of inelastic shadowing is much more important than that due to two-nucleon correlations. (AIP)

Londergan, J.T.; Moniz, E.J.

1975-09-19T23:59:59.000Z

453

MCP Upgrade: Transmission Line and Pore Importance  

E-Print Network (OSTI)

In order to take advantage of all of the benefits of Multi-Channel Plate Photo-Multiplier Tubes (MCPs) a fast and efficient readout scheme must be implemented. One scheme that appears very promising is that of a transmission line coupled to a digital sampling readout. Transmission line readout allows for 2D position reconstruction, as well as an extremely fast response time, allowing for an exceptional timing resolution. I will be discussing the development of a method to connect the transmission line readout to the anode of the MCP, as well as testing the resultant MCP-transmission line readout system. This testing occurred at Argonnes laser lab, which featured a tunable fast rise time laser as well as a data acquisition system with a low noise level. A study to determine the importance of the pore size of the MCP was also carried out at Argonnes laser lab. In this study two MCPs which differed only in pore size (25m and 10m) were tested and their timing resolutions were compared. The objective of the following discussion is to quantify the effectiveness of the transmission line readout, learn more about the nature of the MCP and its signals, and look for ways in which to improve upon the present readout technique. 2 Tyler Natoli 1

Tyler Natoli; Advisor Henry Frisch

2009-01-01T23:59:59.000Z

454

High-resolution bent-crystal spectrometer for the ultra-soft x-ray region  

SciTech Connect

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. 43 refs., 23 figs.

Beiersdorfer, P.; von Goeler, S.; Bitter, M.; Hill, K.W.; Hulse, R.A.; Walling, R.S.

1988-10-01T23:59:59.000Z

455

Mathematical Formulation of Multi-Layer Networks  

E-Print Network (OSTI)

A network representation is useful for describing the structure of a large variety of complex systems. However, most real and engineered systems have multiple subsystems and layers of connectivity, and the data produced by such systems is very rich. Achieving a deep understanding of such systems necessitates generalizing "traditional" network theory, and the newfound deluge of data now makes it possible to test increasingly general frameworks for the study of networks. In particular, although adjacency matrices are useful to describe traditional single-layer networks, such a representation is insufficient for the analysis and description of multiplex and time-dependent networks. One must therefore develop a more general mathematical framework to cope with the challenges posed by multi-layer complex systems. In this paper, we introduce a tensorial framework to study multi-layer networks, and we discuss the generalization of several important network descriptors and dynamical processes --including degree centrality, clustering coefficients, eigenvector centrality, modularity, Von Neumann entropy, and diffusion-- for this framework. We examine the impact of different choices in constructing these generalizations, and we illustrate how to obtain known results for the special cases of single-layer and multiplex networks. Our tensorial approach will be helpful for tackling pressing problems in multi-layer complex systems, such as inferring who is influencing whom (and by which media) in multichannel social networks and developing routing techniques for multimodal transportation systems.

Manlio De Domenico; Albert Sol-Ribalta; Emanuele Cozzo; Mikko Kivel; Yamir Moreno; Mason A. Porter; Sergio Gmez; Alex Arenas

2013-07-18T23:59:59.000Z

456

Analytical Chemistry Laboratory (ACL) procedure compendium. Volume 3, Inorganic instrumental methods  

Science Conference Proceedings (OSTI)

The methods cover: C in solutions, F (electrode), elements by atomic emission spectrometry, inorganic anions by ion chromatography, Hg in water/solids/sludges, As, Se, Bi, Pb, data calculations for SST (single shell tank?) samples, Sb, Tl, Ag, Pu, O/M ratio, ignition weight loss, pH value, ammonia (N), Cr(VI), alkalinity, U, C sepn. from soil/sediment/sludge, Pu purif., total N, water, C and S, surface Cl/F, leachable Cl/F, outgassing of Ge detector dewars, gas mixing, gas isotopic analysis, XRF of metals/alloys/compounds, H in Zircaloy, H/O in metals, inpurity extraction, reduced/total Fe in glass, free acid in U/Pu solns, density of solns, Kr/Xe isotopes in FFTF cover gas, H by combustion, MS of Li and Cs isotopes, MS of lanthanide isotopes, GC operation, total Na on filters, XRF spectroscopy QC, multichannel analyzer operation, total cyanide in water/solid/sludge, free cyanide in water/leachate, hydrazine conc., ICP-MS, {sup 99}Tc, U conc./isotopes, microprobe analysis of solids, gas analysis, total cyanide, H/N{sub 2}O in air, and pH in soil.

Not Available

1993-08-01T23:59:59.000Z

457

E-Smart System for In-Situ Detection of Environmental Contaminants  

SciTech Connect

A team of industrial, academic, and government organizations participated in the development of the Environmental Systems Management, Analysis and Reporting Network (E-SMART). E-SMART integrates diverse monitoring and control technologies by means of a modular, ''building block'' design approach to allow for flexible system configuration. The E-SMART network treats each smart device-whether a sensor, sampler, or actuator- as a black box that obeys the standard communication protocols and electrical interfaces for the network. This approach allows multiple vendors to produce different sensors which meet the same functional specification and which can be interchanged on the network without affecting operation. The project further developed and advanced the E-SMART standardized network protocol to include new sensors, sampling systems, and graphical user interfaces. Specifically, the E-SMART team developed the following three system elements: (1) Base technology for a new class of smart , highly sensitive, chemically-specific, in-situ, multichannel microsensors utilizing integrated optical interferometry technology, (2) A set of additional E-SMART-compatible sensors adapted from commercial off-the-shelf technologies, and (3) A Data Management and Analysis System (DMAS), including network management components and the user-friendly graphical user interface (GUI) for data evaluation and visualization.

S. Leffler

2000-03-01T23:59:59.000Z

458

RAMONA-4B a computer code with three-dimensional neutron kinetics for BWR and SBWR system transient - models and correlations  

Science Conference Proceedings (OSTI)

This document describes the major modifications and improvements made to the modeling of the RAMONA-3B/MOD0 code since 1981, when the code description and assessment report was completed. The new version of the code is RAMONA-4B. RAMONA-4B is a systems transient code for application to different versions of Boiling Water Reactors (BWR) such as the current BWR, the Advanced Boiling Water Reactor (ABWR), and the Simplified Boiling Water Reactor (SBWR). This code uses a three-dimensional neutron kinetics model coupled with a multichannel, non-equilibrium, drift-flux, two-phase flow formulation of the thermal hydraulics of the reactor vessel. The code is designed to analyze a wide spectrum of BWR core and system transients and instability issues. Chapter 1 is an overview of the code`s capabilities and limitations; Chapter 2 discusses the neutron kinetics modeling and the implementation of reactivity edits. Chapter 3 is an overview of the heat conduction calculations. Chapter 4 presents modifications to the thermal-hydraulics model of the vessel, recirculation loop, steam separators, boron transport, and SBWR specific components. Chapter 5 describes modeling of the plant control and safety systems. Chapter 6 presents and modeling of Balance of Plant (BOP). Chapter 7 describes the mechanistic containment model in the code. The content of this report is complementary to the RAMONA-3B code description and assessment document. 53 refs., 81 figs., 13 tabs.

Rohatgi, U.S.; Cheng, H.S.; Khan, H.J.; Mallen, A.N.; Neymotin, L.Y.

1998-03-01T23:59:59.000Z

459

Recent MCAS applications on hypernuclei and radiative capture  

E-Print Network (OSTI)

In recent years, we have developed a Multi-Channel Algebraic Scattering (MCAS) approach to study low-energy nucleon-nucleus scattering, resonance phenomena, and sub-threshold spectra for medium-light nuclei. We have considered compound nuclei that are stable, or weakly bound, and have also extended the analysis to very unstable systems that are unbound with respect to proton emission, namely, that are beyond the proton drip line. More recent developments concerned the application of the MCAS approach to the analysis of the spectra of two hypernuclear systems, 9 Be and 13 C. We have studied the splitting of the two odd-parity excited levels ( 1 2 ? and 3 2 ?) at 11 MeV excitation in 13 C, finding that it is driven mainly by the weak -nucleus spin-orbit force. Conversely, the splittings of the 3 2 + and 5 2 + levels in both 9 Be and 13 C originate from couplings to the collective 2+ states of the core nuclei. In both hypernuclei, our MCAS-based calculations suggest that there are additional low-lying resona...

Canton, L; Karataglidis, S; Svenne, J P

2010-01-01T23:59:59.000Z

460

Geologic evolution and aspects of the petroleum geology of the northern East China Sea shelf basin  

Science Conference Proceedings (OSTI)

Analysis of multichannel seismic reflection profiles reveals that the northern East China Sea shelf basin experienced two phases of rifting, followed by regional subsidence. The initial rifting in the Late Cretaceous created a series of grabens and half grabens, filled by alluvial and fluviolacustrine deposits. Regional uplift and folding (Yuquan movement) in the late Eocene-early Oligocene terminated the initial rifting. Rifting resumed in the early Oligocene, while alluvial and fluviolacustrine deposition continued to prevail. A second phase of uplift in the early Miocene terminated the rifting, marking the transition to the postrift phase. The early postrift phase (early Miocene-late Miocene) is characterized by regional subsidence and westward and northwestward marine transgression. Inversion (Longjing movement) in the late Miocene interrupted the postrift subsidence, resulting in an extensive thrust-fold belt in the eastern part of the area. The entire area entered a stage of regional subsidence again and has become a broad continental shelf. Source rocks include synrift lacustrine facies, fluvial shales, and coal beds. Synrift fluvial, lacustrine, and deltaic deposits, postrift littoral and/or shallow-marine sandstones, and fractured basement have the potential to provide reservoirs. Various types of hydrocarbon traps (e.g., faulted anticlines, overthrusts, rollover anticlines, faults, unconformity traps, combination structural-stratigraphic traps, weathered basement, and stratigraphic traps) are recognized, but many of these traps have not been tested.

Lee, G.H.; Kim, B.Y.; Shin, K.S.; Sunwoo, D. [Pukyong National University, Pusan (Republic of Korea). Dept. of Environmental Exploration Engineering

2006-02-15T23:59:59.000Z

Note: This page contains sample records for the topic "12a dpwa multichannel" from the National Library of EnergyBeta (NLEBeta).
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461

Portable NDA equipment for enrichment measurements for the HEU transparency program  

SciTech Connect

In October 1996, the Department of Energy (DOE) and MINATOM agreed to use portable non-destructive assay (NDA) equipment to measure the {sup 235}U enrichment of material subject to the HEU Transparency agreement. A system based on the ''enrichment meter'' method and high-purity germanium (HPGe) detectors had been previously developed for this application. Instead, sodium iodide (NaI) detectors were chosen to measure {sup 235}U enrichment because HPGe systems might reveal sensitive information. Although the accuracy of the NaI systems is less than an HPGe system, it still satisfies the transparency requirements. The equipment consists of a collimated NaI detector, a Canberra Inspector Multi-channel Analyzer, and a laptop computer. The units have been used to confirm the enrichment of material at Russian facilities since January 1997. This paper compares the performance of the NaI systems with the HPGe system and discusses some significant differences.

Decman, D J; Glaser, J; Hernandez, J M; Luke, S J

1999-07-20T23:59:59.000Z

462

RELAP5 Prediction of Transient Tests in the RD-14 Test Facility  

Science Conference Proceedings (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

463

Extraction of ionization spectra from correlated wave functions: a comparison between different methods  

E-Print Network (OSTI)

We compare three techniques to extract partial photoelectron spectra from the wave packet resulting from the integration on a finite-element discrete variable representation basis of the time-dependent Schr\\"odinger equation for an helium atom subject to an ultra-short XUV pulse. These techniques are: projection on products of hydrogenic bound and continuum states, projection onto multi-channel scattering states computed in a B-spline close-coupling basis, and a technique based on exterior complex scaling (ECS) [Palacios \\emph{et al}, Phys. Rev. A {\\bf 76}, 043420 (2007)] implemented in the same basis used for the time propagation. These methods allow to monitor the population of continuum states in wave packets created with ultrashort pulses in different regimes. The first method works well at the energies where the ionization continuum is unstructured while it becomes inefficient close to threshold openings due to the presence of long-lived metastable states or of vanishingly slow photofragments. The agreem...

Argenti, Luca; Feist, Johannes; Nagele, Stefan; Liertzer, Matthias; Persson, Emil; Burgdrfer, Joachim; Lindroth, Eva

2013-01-01T23:59:59.000Z

464

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

465

Near-field characterization of hydrogen and helium operation on the TFTR (Tokamak Fusion Test Reactor) diagnostic neutral beam  

DOE Green Energy (OSTI)

An Optical Multichannel Analyzer has been used to measure beam divergence and composition. This measurement is usually performed near the center of the neutralizer or beyond the magnet. In the past, these locations suffered difficult beam composition analysis and low light intensity, respectively. It has been determined that the light emission is relatively independent of neutralizer line density in the near field, allowing near-field measurements to overcome both difficulties. At optimum perveance, but under conditions of high gas throughput, the helium 1/e-divergence angle was measured to be 1.5{degree}. Further investigation found that the divergence decreased with gas throughput down to 1.25{degree}. Mimimum divergences for the full-, half-, and third-energy hydrogen components were 1.1{degree}, 1.2{degree}, and 1.4{degree}, respectively. Relative neutral hydrogen particle fluxes available for injection into TFTR are a function of perveance. At maximum perveance, the full-, half-, and third-energy atom fractions were 0.25 {plus minus} 0.04, 0.5 {plus minus} 0.04, and 0.25 {plus minus} 0.05, respectively. 10 refs., 5 figs.

Kamperschroer, J.H.; Schilling, G.; Roquemore, A.L.

1990-07-01T23:59:59.000Z

466

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 device. 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, D.K.; Vocatura, M.; Guttadora, L.J.

1989-12-05T23:59:59.000Z

467

Near-field characterization of hydrogen and helium operation on the TFTR diagnostic neutral beam  

DOE Green Energy (OSTI)

An optical multichannel analyzer has been used to measure beam divergence and composition. This measurement is usually performed near the center of the neutralizer or beyond the magnet. In the past, these locations suffered difficult beam composition analysis and low light intensity, respectively. It has been determined that the light emission is relatively independent of neutralizer line density in the near field, allowing near-field measurements to overcome both difficulties. At optimum perveance, but under conditions of high gas throughput, the helium 1/{ital e} divergence angle was measured to be 1.5{degree}. Further investigation found that the divergence decreased with gas throughput down to 1.25{degree}. Minimum divergences for the full-, half-, and third-energy hydrogen components were 1.1{degree}, 1.2{degree}, and 1.4{degree}, respectively. Relative neutral hydrogen particle fluxes available for injection into TFTR are a function of perveance. At maximum perveance, the full-, half-, and third-energy atom fractions were 0.25{plus minus}0.04, 0.5{plus minus}0.04, and 0.25{plus minus}0.05, respectively.

Kamperschroer, J.H.; Schilling, G.; Roquemore, A.L. (Princeton Plasma Physics Laboratory, Princeton University, Princeton, NJ (USA))

1990-10-01T23:59:59.000Z

468

DEVELOPMENT OF NEXT-GENERATION DETECTORS AND INSTRUMENTATION FOR PHOTOELECTRON SPECTROSCOPY, DIFFRACTION AND HOLOGRAPHY  

SciTech Connect

We have developed a new multichannel detector for use in photoelectron spectroscopy (as well as other types of high-count-rate spectroscopy) that will operate at rates of up to 1 GHz. Such detectors are crucial to the full utilization of the high-brightness radiation generated by third-generation synchrotron radiation sources. In addition, new software and hardware has been developed to permit rapidly and accurately scanning photoelectron spectra that will be accumulated in as little as a 200 micros. A versatile next-generation sample goniometer permitting equally rapid scanning of specimen angles or photon energies for angle-resolved photoemission studies, photoelectron diffraction, and photoelectron holography measurements, and cooling to below 10K has also been designed and constructed. These capabilities have been incorporated into a unique photoelectron spectrometer/diffractometer at the Advanced Light Source of the Lawrence Berkeley National Laboratory; this experimental system includes ultrahigh energy resolution, in situ rotation, variable polarization, and optional spin detection. This overall system is now being used in studies of a variety of problems including magnetic metals and oxides; metal/metal, metal/metal oxide, and metal-oxide/metal-oxide multilayers; and systems exhibiting giant and colossal magnetoresistance.

Charles S. Fadley, Principal Investigator

2005-10-16T23:59:59.000Z

469

Updated User's Guide for Sammy: Multilevel R-Matrix Fits to Neutron Data Using Bayes' Equations  

SciTech Connect

In 1980 the multilevel multichannel R-matrix code SAMMY was released for use in analysis of neutron-induced cross section data at the Oak Ridge Electron Linear Accelerator. Since that time, SAMMY has evolved to the point where it is now in use around the world for analysis of many different types of data. SAMMY is not limited to incident neutrons but can also be used for incident protons, alpha particles, or other charged particles; likewise, Coulomb exit hannels can be included. Corrections for a wide variety of experimental conditions are available in the code: Doppler and resolution broadening, multiple-scattering corrections for capture or reaction yields, normalizations and backgrounds, to name but a few. The fitting procedure is Bayes' method, and data and parameter covariance matrices are properly treated within the code. Pre- and post-processing capabilities are also available, including (but not limited to) connections with the Evaluated Nuclear Data Files. Though originally designed for use in the resolved resonance region, SAMMY also includes a treatment for data analysis in the unresolved resonance region.

Larson, Nancy M [ORNL

2008-10-01T23:59:59.000Z

470

Doppler-shift proton fraction measurement on a CW proton injector  

Science Conference Proceedings (OSTI)

A spectrometer/Optical Multi-channel Analyzer has been used to measure the proton fraction of the cw proton injector developed for the Accelerator Production of Tritium (APT) and the Low Energy Demonstration Accelerator (LEDA) at Los Alamos. This technique, pioneered by the Lawrence Berkeley National Laboratory (LBNL), was subsequently adopted by the international fusion community as the standard for determining the extracted ion fractions of neutral beam injectors. Proton fractions up to 95 {+-} 3% have been measured on the LEDA injector. These values are in good agreement with results obtained by magnetically sweeping the ion beam, collimated by a slit, across a Faraday cup. Since the velocity distribution of each beam species is measured, it also can be used to determine beam divergence. While divergence has not yet been ascertained due to the wide slit widths in use, non-Gaussian distributions have been observed during operation above the design-matched perveance. An additional feature is that the presence of extracted water ions can be observed. During ion source conditioning at 75 kV, an extracted water fraction > 30% was briefly observed.

Kamperschroer, J.H. [General Atomics, San Diego, CA (United States); Sherman, J.D.; Zaugg, T.J. [Los Alamos National Lab., NM (United States); Arvin, A.H.; Bolt, A.S.; Richards, M.C. [Savannah River Site, Aiken, SC (United States)

1998-12-31T23:59:59.000Z

471

Comparison of CdTe and CdZnTe Detectors for Field Determination of Uranium Isotopic Enrichments  

DOE Green Energy (OSTI)

A performance comparison of a CdTe and a CdZnTe detector when exposed to uranium samples of various isotopic enrichments has been performed. These high-resolution detectors can assist in the rapid determination of uranium isotopic content of illicit material. Spectra were recorded from these room temperature semiconductor detectors with a portable multi-channel analyzer, both in the laboratory and in a field environment. Both detectors were operated below ambient temperature using the vendor supplied thermoelectric coolers. Both detectors had nominally the same active volume (18 mm3 for the CdZnTe and 25 mm3 for the CdTe detector) and resolution. Spectra of samples of known isotopic content were recorded at fixed geometries. An evaluation of potential signature g rays for the detection of enriched uranium was completed. Operational advantages and disadvantages of each detector are discussed. There is a need to improve the detection sensitivity during the interdiction of special nuclear materials (SNM) for increased homeland protection. It is essential to provide additional tools to first responders and law enforcement personnel for assessing nuclear and radiological threats.

Hofstetter, KJ

2004-01-23T23:59:59.000Z

472

Field implementation of geophysical diffraction tomography  

SciTech Connect

Geophysical diffraction tomography is a new technique that shows promise as a tool for quantitative subsurface (below-ground) imaging. The approach being used is based upon the filtered backpropagation algorithm, which is a mathematical extension of the reconstruction software used in conventional X-ray CAT scanners. The difference between this method and existing methods is that the new algorithm rigorously accounts for diffraction effects through an exact inversion of the wave equation. This refinement is necessary in that it admits the use of acoustic and long-wavelength electromagnetic waves, allowing tomography to be taken from the laboratory to the field. ORNL's effort in geophysical diffraction tomography involves reducing the filtered backpropagation algorithm to practice. This requires the design and construction of field instrumentation as well as the development of an improved algorithm. The original algorithm requires the imaged region to be illuminated by plane waves. This requirement simplifies the algorithm but complicates its field implementation in that plane waves are difficult to generate. Consequently, ORNL has been working to generalize the filtered backpropagation algorithm to allow a broader range of incoming wave fields which can more easily be realized in the field. The instrumentation aspects involve the selection of appropriate sonic sources and receivers along with the development of a state-of-art, portable, computer-controlled, multichannel data acquisition system. 5 references, 6 figures.

Witten, A.J.; Stevens, S.S.

1984-01-01T23:59:59.000Z

473

Rayleigh temperature profiles in a hydrogen diffusion flame  

DOE Green Energy (OSTI)

Rayleigh scattering from a hydrogen-air laminar jet diffusion flame in combination with a numerical model of the flame has been used to determine temperature profiles. The model predictions of species concentration are used to calculate a mean Rayleigh cross-section which is used to relate the Rayleigh scattered intensity to temperature. Using an argon ion laser producing 7.5 watts at 488 nm and an optical multichannel analyzer (OMA), the scattered light was imaged into a spectrometer. The OMA was rotated 90 degrees to its normal orientation, allowing scans to be taken along the spectrometer exit slit. This resulted in a spatially resolved Rayleigh signal along the laser beam through the entire flame. Spatial resolution of 0.18 mm on each of the 500 detector elements with good signal-to-noise ratios was achieved even with integration times of only 0.03 second. Since the entire profile is made simultaneously, particulate perturbed profiles are easily recognized and discarded. Transverse profiles are presented to show flame structure. Axial profiles are compared to radiation corrected thermocouple measurements.

Smith, J.R.

1978-09-01T23:59:59.000Z

474

Events trigger generator for resonant spherical detectors of gravitational waves  

E-Print Network (OSTI)

We have set up and tested a pipeline for processing the data from a spherical gravitational wave detector with six transducers. The algorithm exploits the multichannel capability of the system and provides a list of candidate events with their arrival direction. The analysis starts with the conversion of the six detector outputs into the scalar and the five quadrupolar modes of the sphere, which are proportional to the corresponding gravitational wave spherical components. Event triggers are then generated by an adaptation of the WaveBurst algorithm. Event validation and direction reconstruction are made by cross-checking two methods of different inspiration: geometrical (lowest eigenvalue) and probabilistic (maximum likelihood). The combination of the two methods is able to keep substantially unaltered the efficiency and can reduce drastically the detections of fake events (to less than ten per cent). We show a quantitative test of these ideas by simulating the operation of the resonant spherical detector miniGRAIL, whose planned sensitivity in its frequency band (few hundred Hertz's around 3 kHz) is comparable with the present LIGO one.

Stefano Foffa; Riccardo Sturani

2008-05-06T23:59:59.000Z

475

PULSE HEIGHT ANALYZER  

DOE Patents (OSTI)

An anticoincidence device is described for a pair of adjacent channels of a multi-channel pulse height analyzer for preventing the lower channel from generating a count pulse in response to an input pulse when the input pulse has sufficient magnitude to reach the upper level channel. The anticoincidence circuit comprises a window amplifier, upper and lower level discriminators, and a biased-off amplifier. The output of the window amplifier is coupled to the inputs of the discriminators, the output of the upper level discriminator is connected to the resistance end of a series R-C network, the output of the lower level discriminator is coupled to the capacitance end of the R-C network, and the grid of the biased-off amplifier is coupled to the junction of the R-C network. In operation each discriminator produces a negative pulse output when the input pulse traverses its voltage setting. As a result of the connections to the R-C network, a trigger pulse will be sent to the biased-off amplifier when the incoming pulse level is sufficient to trigger only the lower level discriminator.

Johnstone, C.W.

1958-01-21T23:59:59.000Z

476

Quantum probabilities of composite events in quantum measurements with multimode states  

E-Print Network (OSTI)

The problem of defining quantum probabilities of composite events is considered. This problem is of high importance for the theory of quantum measurements and for quantum decision theory that is a part of measurement theory. We show that the Luders probability of consecutive measurements is a transition probability between two quantum states and that this probability cannot be treated as a quantum extension of the classical conditional probability. The Wigner distribution is shown to be a weighted transition probability that cannot be accepted as a quantum extension of the classical joint probability. We suggest the definition of quantum joint probabilities by introducing composite events in multichannel measurements. The notion of measurements under uncertainty is defined. We demonstrate that the necessary condition for the mode interference is the entanglement of the composite prospect together with the entanglement of the composite statistical state. As an illustration, we consider an example of a quantum game. A special attention is payed to the application of the approach to systems with multimode states, such as atoms, molecules, quantum dots, or trapped Bose-condensed atoms with several coherent modes.

V. I. Yukalov; D. Sornette

2013-08-26T23:59:59.000Z

477

Microchannel Reactor System for Catalytic Hydrogenation  

Science Conference Proceedings (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

478

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

479

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

480

wyang98@stanford.edu; phone 1 650 723-6213; fax 1 650 725-9755; http://eil.stanford.edu/WiMMS/  

E-Print Network (OSTI)

In this study, a new wireless sensing unit for operation within an automated Structural Health Monitoring (SHM) system is proposed, designed and validated. The design of the wireless sensing unit emphasizes minimization of its power consumption characteristics to ensure it is suited for long-term field deployment in civil structures. The wireless modem integrated with the unit has a long communication range that permits wireless sensors to be spaced over 100m apart. A multi-channel high-resolution analog-to-digital converter is included within each sensing unit to provide flexibility for high-fidelity data collection. A key feature of the wireless sensing unit design is the inclusion of a sophisticated computing core that is capable of locally executing engineering algorithms in real-time. As part of the embedded software, a novel communication protocol is written that can accomplish low-latency communications for accurate time synchronization between spatially distributed wireless sensors. To illustrate the capabilities of the wireless monitoring platform, including the execution of extensive computational tasks, a prototype system is fabricated and tested in the laboratory and field. As part of validating the system performance in the field, the vertical acceleration response of the Geumdang Bridge under traffic loading is measured by 14 wireless sensing unit prototypes.

Design Of Low-Power; Wang Yang; Jerome P. Lynch; B Kincho H. Law

2005-01-01T23:59:59.000Z

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481

Method and apparatus for stabilizing pulsed microwave amplifiers  

DOE Patents (OSTI)

Phase and amplitude variations at the output of a high power pulsed microwave amplifier arising from instabilities of the driving electron beam are suppressed with a feed-forward system that can stabilize pulses which are too brief for regulation by conventional feedback techniques. Such variations tend to be similar during successive pulses. The variations are detected during each pulse by comparing the amplifier output with the low power input signal to obtain phase and amplitude error signals. This enables storage of phase and amplitude correction signals which are used to make compensating changes in the low power input signal during the following amplifier output pulse which suppress the variations. In the preferred form of the invention, successive increments of the correction signals for each pulse are stored in separate channels of a multi-channel storage. Sequential readout of the increments during the next pulse provides variable control voltages to a voltage controlled phase shifter and voltage controlled amplitude modulator in the amplifier input signal path.

Hopkins, Donald B. (Sacramento, CA)

1993-01-01T23:59:59.000Z

482

TOD Version 2.0: Dreams and Realities  

E-Print Network (OSTI)

transit planning and good community development planning... #12;A new frame for considering TOD · AB 32 perspective, local funding Cost effective mobility enhancement Multi-modal access and mobility; co

Bertini, Robert L.

483

Non-rigid Registration and Restoration of Double-sided Historical Manuscripts Jie Wang and Chew Lim Tan  

E-Print Network (OSTI)

-sided document images. In IEEE WACV, 2000. [11] A. Tonazzini, L. Bedini, and E. Salerno. Independent com- ponent analysis for document restoration. IJDAR, 7(1):17­ 27, 2004. [12] A. Tonazzini, E. Salerno, and L. Bedini

Tan, Chew Lim

484

Representing Website Design Copyright 2003 David K. Farkas.  

E-Print Network (OSTI)

Make Me Think. Que, 2000. #12;A web page with a simple, straightforward visual hierarchy #12;Visual are part of other things. In other words, each page should have a clear visual hierarchy." Steve Krug, Don't

485

Energy Information Administration - Commercial Energy Consumption...  

Gasoline and Diesel Fuel Update (EIA)

Released: Dec 2006 Next CBECS will be conducted in 2007 Table C12A. Consumption and Gross Energy Intensity by Year Constructed for Sum of Major Fuels for All Buildings, 2003 Sum of...

486

1360.ps  

E-Print Network (OSTI)

a Service d'architecture BSC (PC 12A7), Nortel GSM Access R&D, Parc d' activits ... Nortel GSM Access R&D Technical Report PE/BSC/INF/016550 V01/ EN,...

487

1365.ps  

E-Print Network (OSTI)

a Service d'architecture BSC (PC 12A7), Nortel GSM Access R&D, Parc ... Technical report Nortel GSM Access R&D PE/BSC/INF/017912 V01/EN, to appear.

488