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NASA Scientific and Technical Aerospace Reports

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distribution of ions) with given initial conditions will undergo chaotic motion.<br />

NTIS<br />

Ions; Magnetic Field Configurations<br />

20040111127 Princeton Univ., NJ<br />

L<strong>and</strong>au Damping <strong>and</strong> Anomalous Skin Effect in Low Pressure Gas Discharges: Self-Consistent Treatment of<br />

Collisionless Heating<br />

Kaganovich, I. D.; Polomarov, O. V.; Theodosiou, C. E.; Jan. 2004; 42 pp.; In English<br />

Report No.(s): DE2004-821522; PPPL-3922; No Copyright; Avail: Department of Energy Information Bridge<br />

In low-pressure discharges, where the electron mean free path is larger or comparable with the discharge length, the<br />

electron dynamics is essentially nonlocal. Moreover, the electron energy distribution function (EEDF) deviates considerably<br />

from a Maxwellian. Therefore, an accurate kinetic description of the low-pressure discharges requires knowledge of the<br />

nonlocal conductivity operator <strong>and</strong> calculation of the non-Maxwellian EEDF. The previous treatments made use of simplifying<br />

assumptions: a uniform density pro.le <strong>and</strong> a Maxwellian EEDF. In the present study a self-consistent system of equations for<br />

the kinetic description of nonlocal, nonuniform, nearly collisionless plasmas of low-pressure discharges is reported. It consists<br />

of the nonlocal conductivity operator <strong>and</strong> the averaged kinetic equation for calculation of the non-Maxwellian EEDF. This<br />

system was applied to the calculation of collisionless heating in capacitively <strong>and</strong> inductively coupled plasmas. In particular,<br />

the importance of accounting for the nonuniform plasma density pro.le for computing the current density pro.le <strong>and</strong> the EEDF<br />

is demonstrated. The enhancement of collisionless heating due to the bounce resonance between the electron motion in the<br />

potential well <strong>and</strong> the external rf electric .eld is investigated. It is shown that a nonlinear <strong>and</strong> self-consistent treatment is<br />

necessary for the correct description of collisionless heating.<br />

NTIS<br />

Collisionless Plasmas; Gas Heating; Kinetic Equations; L<strong>and</strong>au Damping<br />

20040111128 California Univ., Lawrence Berkeley National Lab., Berkeley, CA, USA, Deutsches Elektronen-Synchrotron,<br />

Hamburg, Germany<br />

Damping Ring Designs <strong>and</strong> Issues<br />

Wolski, A.; Decking, W.; 2004; 10 pp.; In English<br />

Report No.(s): DE2004-822803; LBNL-52580; No Copyright; Avail: Department of Energy Information Bridge<br />

The luminosity performance of a future linear collider (LC) will depend critically on the performance of the damping<br />

rings. The design luminosities of the current LC proposals require rings with very short damping times, large acceptance, low<br />

equilibrium emittance <strong>and</strong> high beam intensity. We discuss the design strategies for lattices achieving the goals of dynamical<br />

stability, examine the challenges for alignment <strong>and</strong> coupling correction, <strong>and</strong> consider a variety of collective effects that<br />

threaten to limit beam quality. We put the design goals in context by referring to the experience of operating facilities, <strong>and</strong><br />

outline the further research <strong>and</strong> development that is needed.<br />

NTIS<br />

Damping; Accelerators; Stability<br />

20040111129 Lawrence Livermore National Lab., Livermore, CA<br />

Beam-Target Interaction Experiments for Multipulse Bremsstrahlung Converters Applications<br />

Sampayan, S.; Buckles, R.; Caporaso, G.; Chambers, F. C.; Chen, Y. J.; 2004; In English<br />

Report No.(s): DE2003-15005533; No Copyright; Avail: National <strong>Technical</strong> Information Service (NTIS)<br />

As part of the Dual Axis Radiography Hydrotest Facility, Phase II (DARHT II) multipulse Bremsstrahlung target, we have<br />

been performing an investigation of (1) the possible adverse effects of backstreaming ion emission from the Bremsstrahlung<br />

converter target <strong>and</strong> (2) maintaining sufficient target density to ensure dose in latter pulses. Theory predictions show that the<br />

first effect would primarily be manifested in the static focusing system as a rapidly varying x-ray spot. From experiments<br />

performed on ETA-II, we have shown that the first effect is not strongly present when the beam initially interacts with the<br />

target. Electron beam pulses delivered to the target after formation of a plasma are strongly affected, however. Secondly, we<br />

have performed studies of the effect of the time varying target density on dose <strong>and</strong> seek to demonstrate various techniques for<br />

maintaining that density. Measurements are presented of the target density as a function of time <strong>and</strong> are compared with our<br />

hydrodynamic models.<br />

NTIS<br />

Accelerators; Bremsstrahlung; Radiography; X Rays<br />

273

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