Phys. Rev. ST Accel. Beams 7, 083501 (2004) [29 pages]

Design and characterization of a neutralized-transport experiment for heavy-ion fusion

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Enrique Henestroza, Shmuel Eylon, Prabir K. Roy, Simon S. Yu, André Anders, Frank M. Bieniosek, Wayne G. Greenway, B. Grant Logan, Robert A. MacGill, Derek B. Shuman, David L. Vanecek, and William L. Waldron
Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA

William M. Sharp and Timothy L. Houck
Lawrence Livermore National Laboratory, Livermore, California 94551, USA

Ronald C. Davidson, Philip C. Efthimion, Erik P. Gilson, and Adam B. Sefkow
Princeton Plasma Physics Laboratory, Princeton, New Jersey 08543, USA

Dale R. Welch and David V. Rose
Mission Research Corporation, Albuquerque, New Mexico 87110, USA

Craig L. Olson
Sandia National Laboratory, Albuquerque, New Mexico 87107, USA

Received 29 September 2003; published 9 August 2004

In heavy-ion inertial-confinement fusion systems, intense beams of ions must be transported from the exit of the final-focus magnet system through the fusion chamber to hit spots on the target with radii of about 2 mm. For the heavy-ion-fusion power-plant scenarios presently favored in the U.S., a substantial fraction of the ion-beam space charge must be neutralized during this final transport. The most effective neutralization technique found in numerical simulations is to pass each beam through a low-density plasma after the final focusing. To provide quantitative comparisons of these theoretical predictions with experiment, the Virtual National Laboratory for Heavy Ion Fusion has completed the construction and has begun experimentation with the neutralized-transport experiment. The experiment consists of three main sections, each with its own physics issues. The injector is designed to generate a very high-brightness, space-charge-dominated potassium beam, while still allowing variable perveance by a beam aperturing technique. The magnetic-focusing section, consisting of four pulsed quadrupoles, permits the study of magnet tuning, as well as the effects of phase-space dilution due to higher-order nonlinear fields. In the final section, the converging ion beam exiting the magnetic section is transported through a drift region with plasma sources for beam neutralization, and the final spot size is measured under various conditions of neutralization. In this paper, we discuss the design and characterization of the three sections in detail and present initial results from the experiment.


©2004 The American Physical Society

URL: http://link.aps.org/abstract/PRSTAB/v7/e083501
DOI: 10.1103/PhysRevSTAB.7.083501
PACS: 52.58.Hm, 41.85.–p, 52.59.Sa, 52.70.Nc

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