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NASA Scientific and Technical Aerospace Reports

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Tevatron. We report here preliminary results on key elements to the measurement including B(sub s) event reconstruction,<br />

proper time resolution <strong>and</strong> initial B flavor tagging. The prospects on B(sub s) mixing with the upgraded CDF <strong>and</strong> D0 detectors<br />

are also discussed.<br />

NTIS<br />

Hadrons; Particle Accelerators<br />

20040120906 S<strong>and</strong>ia National Labs., Albuquerque, NM<br />

Developing a Multifidelity Modeling Algorithm for System-Level Engineering Analysis<br />

Gardner, D. R.; Hennigan, G. L.; Feb. 2003; In English<br />

Report No.(s): DE2004-820880; SAND2003-0399; No Copyright; Avail: National <strong>Technical</strong> Information Service (NTIS)<br />

Multifidelity modeling, in which one component of a system is modeled at a significantly different level of fidelity than<br />

another, has several potential advantages. For example, a higher-fidelity component model can be evaluated in the context of<br />

a lower-fidelity full system model that provides more realistic boundary conditions <strong>and</strong> yet can be executed quickly enough<br />

for rapid design changes or design optimization. Developing such multifidelity models presents challenges in several areas,<br />

including coupling models with differing spatial dimensionalities. In this report we describe a multifidelity algorithm for<br />

thermal radiation problems in which a three-dimensional, finite-element model of a system component is embedded in a<br />

system of zero-dimensional (lumped-parameter) components. We tested the algorithm on a prototype system with three<br />

problems: heating to a constant temperature, cooling to a constant temperature, <strong>and</strong> a simulated fire environment.<br />

NTIS<br />

Heat Transfer; Cooling Systems; Systems Analysis<br />

20040120916 Lawrence Livermore National Lab., Livermore, CA<br />

Deployment, Commissioning <strong>and</strong> Operation of Plasma Electrode Pockels Cells in the National Ignition Facility<br />

Arnold, P. A.; Ollis, C. W.; Hinz, A.; Robb, C.; Dec. 01, 2003; 18 pp.; In English<br />

Report No.(s): DE2004-15007263; UCRL-CONF-155436; No Copyright; Avail: Department of Energy Information Bridge<br />

Large aperture Plasma Electrode Pockels Cells (PEPCs) are an enabling technology in the National Ignition Facility (NIF)<br />

at the Lawrence Livermore National Laboratory. The Pockels cells allow the NIF laser to take advantage of multipass main<br />

amplifier architecture, thus reducing costs <strong>and</strong> physical size of the facility. Each Pockels cell comprises four 40-cm x 40-cm<br />

apertures arranged in a4x1array. The combination of the Pockels cell <strong>and</strong> a thin-film polarizer, also configured in a4x1<br />

array, forms an optical switch that is key to achieving the required multi-pass operation.<br />

NTIS<br />

Amplifiers; Plasma Electrodes<br />

20040120917 Academy of Sciences (USSR), Novosibirsk, USSR, Kentucky Univ., Lexington, KY, USA, Stanford Linear<br />

Accelerator Center, Stanford, CA, USA<br />

Radiative Decays, Nonet Symmetry <strong>and</strong> SU(3) Breaking<br />

Benayoun, M.; DelBuono, L.; Eidelman, S.; Ivanchenko, V. N.; 2004; 42 pp.; In English<br />

Report No.(s): DE2004-10196; UK/TP 99-01; LPNHE 99-01,SLAC-PUB-8048; No Copyright; Avail: Department of Energy<br />

Information Bridge<br />

We re-examine the problem of simultaneously describing in a consistent way all radiative <strong>and</strong> leptonic decays of light<br />

mesons (V(yields) P(gamma), P(yields) V(gamma), P(yields)(gamma)(gamma), V(yields) e(sup+)e(sup -)). For this purpose,<br />

we rely on the Hidden Local Symmetry model in both its anomalous <strong>and</strong> non-anomalous sectors. We show that the SU(3)<br />

symmetry breaking scheme proposed by B<strong>and</strong>o, Kugo <strong>and</strong> Yamawaki, supplemented with nonet symmetry breaking in the<br />

pseudoscalar sector, allows one to reach a nice agreement with all data, except for the K*(sup(+-)) radiative decay. An<br />

extension of this breaking pattern allows one to account for this particular decay mode too. Considered together, the whole<br />

set of radiative decays provides a pseudoscalar mixing angle(theta)(sub P)(approx-equal) <strong>and</strong> a value for(theta)(sub V) which<br />

is(approx-equal) 3(sup o) from that of ideal mixing. We also show that it is impossible, in a practical sense, to disentangle the<br />

effects of nonet symmetry breaking <strong>and</strong> those of glue inside the(eta)(prime), using only light meson decays.<br />

NTIS<br />

Broken Symmetry; Particle Decay<br />

284

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