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NASA Scientific and Technical Aerospace Reports

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20040047242 Lawrence Livermore National Lab., Livermore, CA<br />

Investigation of Vacuum Insulator Surface Dielectric Strength with Nanosecond Pulses<br />

Nummally, W. C.; Krogh, M.; Williams, C.; Trimble, D.; Sampayan, S.; Jun. 03, 2003; 10 pp.; In English<br />

Report No.(s): DE2004-15005840; UCRL-JC-151647; No Copyright; Avail: Department of Energy Information Bridge<br />

The maximum vacuum insulator surface dielectric strength determines the acceleration electric field gradient possible in<br />

a short pulse accelerator. Previous work has indicated that higher electric field strengths along the insulator-vacuum interface<br />

might be obtained as the pulse duration is decreased. In this work, a 250 kV, single ns wide impulse source was applied to<br />

small diameter, segmented insulators samples in a vacuum to evaluate the multi-layer surface dielectric strength of the sample<br />

construction. Resonances in the low inductance test geometry were used to obtain unipolar, pulsed electric fields in excess of<br />

100 MV/m on the insulator surface. The sample construction, experimental arrangement <strong>and</strong> experimental results are<br />

presented for the initial data in this work. Modeling of the multi-layer structure is discussed <strong>and</strong> methods of improving<br />

insulator surface dielectric strength in a vacuum are proposed.<br />

NTIS<br />

Electric Fields; Field Strength; Pulse Duration; Dielectrics<br />

20040047243 Lawrence Livermore National Lab., Livermore, CA<br />

Tables of Neutron-induced Fission Cross Sections for Various Pu, U, <strong>and</strong> Th Isotopes, Deduced from Measured Fission<br />

Probabilities<br />

Younes, W.; Britt, H. C.; Mar. 31, 2003; 18 pp.; In English<br />

Report No.(s): DE2004-15005842; UCRL-ID-152906; No Copyright; Avail: Department of Energy Information Bridge<br />

Cross sections for neutron-induced fission of (sup 231, 233)Th, (sup 234,235,236,237,239)U, <strong>and</strong> (sup 240,241, 243)Pu<br />

are presented in tabular form for incident neutron energies of 0.1(le) E(sub n)(MeV)(le) 2.5. The cross sections were obtained<br />

by converting measured fission probabilities from (t,pf) reactions on mass-A targets to (n,f) cross sections on mass-A+ 1<br />

neutron targets, by using modeling to compensate for the differences in the reaction mechanisms.<br />

NTIS<br />

Neutrons; Neutron Cross Sections; Plutonium Isotopes; Thorium Isotopes; Uranium Isotopes<br />

20040047244 Lawrence Livermore National Lab., Livermore, CA<br />

POINT 2003: A Temperature Dependent ENDF/B-VI, Release 8 Cross Section Library<br />

Cullen, D. E.; May 22, 2003; 20 pp.; In English<br />

Report No.(s): DE2004-15005843; UCRL-ID-127776-R2; No Copyright; Avail: Department of Energy Information Bridge<br />

The ENDF/B data library has recently been updated <strong>and</strong> is now freely available through the National Nuclear Data Center<br />

(NNDC), Brookhaven National Laboratory. This most recent library is identified as ENDF/B-VI, Release 8. Release 8<br />

completely supersedes all preceding releases. Release 8 will be the last release of ENDF/B-VI; the next release of ENDF/B<br />

data will be for the new ENDF/B-VII library. As distributed the ENDF/B-VI, Release 8 data includes cross sections<br />

represented in the form of a combination of resonance parameters <strong>and</strong>/or tabulated energy dependent cross sections, nominally<br />

at 0 Kelvin temperature.<br />

NTIS<br />

Cross Sections; Temperature Dependence<br />

20040047253 Lawrence Livermore National Lab., Livermore, CA<br />

Superconducting Detector Endstation for High-Resolution Energy-Dispersive SR-XRF<br />

Friedrich, S.; Drury, O.; Niedermayr, T.; Cunningham, M. F.; van den Berg, M. L.; Sep. 15, 2000; 18 pp.; In English<br />

Report No.(s): DE2004-15005851; UCRL-JC-138005; No Copyright; Avail: Department of Energy Information Bridge<br />

We have built a two-stage adiabatic demagnetization refrigerator (ADR) to operate cryogenic high-resolution x-ray<br />

detectors in synchrotron-based fluorescence applications. The detector is held at the end of a 40 cm cold finger that extends<br />

into a UHV sample chamber. The ADR attains a base temperature below 100 mK with about 24 hours hold time below 400<br />

mK, <strong>and</strong> does not require pumping on the liquid He bath. We will discuss cryostat design <strong>and</strong> performance.<br />

NTIS<br />

Superconductivity; X Ray Detectors; Magnetic Fields; Magnetic Cooling<br />

20040047254 Lawrence Livermore National Lab., Livermore, CA<br />

Position Resolution Studies with MSU 32-Fold Segmented HPGe Detector<br />

Lehner, C. E.; Vetter, K.; Kunh, A.; Schmid, G. J.; Beckedahl, D. A.; Oct. 25, 2001; 12 pp.; In English<br />

Report No.(s): DE2004-15005670; UCRL-JC-143745; No Copyright; Avail: Department of Energy Information Bridge<br />

173

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