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Divergence in intense ion beams caused by incomplete charge neutralization

Conference ·
OSTI ID:7113166
Space charge neutralization for light ion fusion (LIF) ion beam transport is usually assumed to be perfect in the charge-neutral'' region of the diode and in the gas transport cell. However, small charge clumps in the beam will not be totally charge-neutralized, and the residual net space charge may contribute to the beam microdivergence {theta} {sub {mu}}. If the net potential of the clump is limited only by electron trapping, the minimum potential will be e{phi} {approximately} 1/2 m{sub e}v{sub i}{sup 2} where m{sub e} is the electron mass and v{sub i} is the ion velocity. For proton beams this leads to {theta}{sub {mu}} {approximately} (m {sub e}/M{sub p}){sup 1/2} {approximately} 23 mrad, where M{sub p} is the proton rest mass. For non-protonic beams, different results occur. The mechanism predicts no dependence of {theta} {sub {mu}} on diode voltage, non-protonic {theta} {sub {mu}} greater than proton {theta} {sub {mu}} for proton-contaminated beams, and axial energy spread {Delta}{var epsilon}{sub {parallel}}/{var epsilon}{sub {parallel}} {approximately} {plus minus} 2 {theta} {sub {mu}}, which are all consistent with present data. Results of analytic studies and computer simulations of this mechanism are presented. Plasma shielding reduces the effects of this mechanism but collisions and magnetic fields reduce the plasma shielding effects. 2-D PIC MAGIC simulations show that this mechanism contributes to {theta} {sub {mu}} both in the charge-neutral'' region and in the gas transport region. It is concluded that this mechanism is especially important in the charge-neutral'' region.
Research Organization:
Sandia National Labs., Albuquerque, NM (United States)
Sponsoring Organization:
DOE; USDOE, Washington, DC (United States)
DOE Contract Number:
AC04-76DP00789
OSTI ID:
7113166
Report Number(s):
SAND-91-2744C; CONF-920515--27; ON: DE92016891
Country of Publication:
United States
Language:
English