Beam experiments in the extreme space-charge limit on the University of Maryland Electron Ring
Phys. Plasmas 11, 2907 (2004); doi:10.1063/1.1668288
Published 23 April 2004
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The University of Maryland Electron Ring (UMER), designed for transport studies of space-charge dominated beams in a strong focusing lattice, is nearing completion. UMER models, for example, the recirculator accelerator envisioned as a possible driver for heavy-ion inertial fusion. The UMER lattice will consist of 36 alternating-focusing (FODO) periods over an 11.5 m circumference. The main diagnostics are phosphor screens and capacitive beam position monitors placed at the center of each 20° bending section. In addition, pepper-pot and slit-wire emittance meters are in operation. We present experimental results for three cases of strong space-charge dominated transport (7.2, 24, and 85 mA, at 10 keV) and contrast them with one case in the emittance-dominated regime (0.6 mA at 10 keV). With focusing given by
0 = 76°, the zero-current betatron phase advance per period, the range of currents corresponds to a space-charge tune depression of 0.2 to 0.8. This range is unprecedented for a circular machine. The beam physics over three transport distances is considered: at or near the source, over the length of the matching section (about 1 m), and single turn (10 m). Issues associated with beam characterization, scaling of various parameters, alignment, and envelope matching are discussed. ©2004 American Institute of Physics.
0 = 76°, the zero-current betatron phase advance per period, the range of currents corresponds to a space-charge tune depression of 0.2 to 0.8. This range is unprecedented for a circular machine. The beam physics over three transport distances is considered: at or near the source, over the length of the matching section (about 1 m), and single turn (10 m). Issues associated with beam characterization, scaling of various parameters, alignment, and envelope matching are discussed. ©2004 American Institute of Physics.
| History: | Received 30 October 2003; accepted 16 January 2004; published 23 April 2004 |
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http://link.aip.org/link/?PHPAEN/11/2907/1 |
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1070-664X (print)
1089-7674 (online)
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b, is defined in this reference [see Eqs. (8) and (16) of the reference]; it is related to our intensity
by
b =
/(1
). The two parameters are identical only in the zero-current, or high-temperature limit.






