1998
DOI: 10.1103/physreve.57.4713
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Stability of anisotropic beams with space charge

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Cited by 133 publications
(150 citation statements)
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“…This contribution is most significant for low-order resonances [24,25]. For a round beam near a half-integer resonance (m 2), when the horizontal and vertical tunes are close to each other, C 2 1͞2 for the symmetric mode, and C 2 3͞4 for the antisymmetric mode.…”
Section: Effective Space-charge Tune Shiftmentioning
confidence: 99%
“…This contribution is most significant for low-order resonances [24,25]. For a round beam near a half-integer resonance (m 2), when the horizontal and vertical tunes are close to each other, C 2 1͞2 for the symmetric mode, and C 2 3͞4 for the antisymmetric mode.…”
Section: Effective Space-charge Tune Shiftmentioning
confidence: 99%
“…On the other hand, an approach based on solving the Vlasov-Poisson equations is more general and, in some cases (in the smooth approximation and for beam distributions entailing purely linear space charge forces), the calculation can be carried out analytically. A 1D model of a beam in a uniform focusing was studied using this method by Sacherer [6]; the extension to 2D for an isotropic Kapchinskij-Vladimirskij (KV) [8] beam was carried out by Gluckstern [7], and a further generalization to an unisotropic KV beam (i.e., with unequal emittances and depressed tunes in the horizontal and vertical planes) has recently been presented by Hofmann [9]. This is the method that we will employ in this paper.…”
Section: Introductionmentioning
confidence: 99%
“…Hence, we predict the number of survival real particles per a spill as 6×10 6 particles/(macro particle)/(turn)×1000 (macro particles) ×20(turns)×injection Figures 7 and 8 reveal structures of the phase space. This is believed to be higher-order resonances caused by tune shifts in the presence of space charge effect [9] but it requires more study.…”
Section: Optimization Of the Bump Magnet Parametersmentioning
confidence: 99%