Time variation of space-charge forces in a beam-transport channel will lead to a time-averaged emittance growth of the beam. The Kapchinskii-Vladimirskii (K-V) equations have been used to follow the envelope of a round beam with effective beam current fluctuation i through a transport channel. The area of the ellipse that encloses the varying ellipses at the end has been used as the criterion for emittance growth. Simple formulae give the relation between i, initial emittance epilson, allowable fractional emittance growth ..delta.. eta, effective average current I, average beam radius R, and transport length. For example, for a long transport channel a nominally compensated beam must have i < (..beta gamma.. epsilon/sup 2/I/sub 0//R/sup 2/)..delta.. eta, where I/sub 0/ = 4..pi..epsilon/sub 0/Mc/sup 3//e, and ..beta gamma.. is the usual relativistic factor. Results for other conditions are presented. A comparison with a numerical calculation from the TRACE code for transport of a 100-keV, 100-mA beam is made. 6 refs., 3 figs.
No takes yet. Share an insight, caveat, or question.
Paul Allison (1985) studied this question.
Synapse has enriched 3 closely related papers on similar clinical questions. Consider them for comparative context: