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Transient particle distribution for linearly coupled motion in an electron storage ring

Technical Report ·
OSTI ID:6955591

The stationary distribution function for an electron bunch in a storage ring has been studied in the presence of radiation damping, quantum excitation and linear coupling between the transverse modes of oscillation, x and y, and energy collision, delta. This distribution, /psi//sub s/, has been found to be given in a form exp (/Sigma Sigma/ A/sub ij/ x/sub i/x/sub j/) with x/sub i/ denoting the coordinates (x, p/sub x/, y, p/sub y/, delta, p/sup delta/) and A/sub ij/'s some constants. This distribution function can be obtained by finding the time-independent solution of the Fokker-Planck equation. Under certain conditions, e.g., during injection or the presence of perturbations, the particle distribution function, /psi/, is nonstationary and is different from /psi//sub s/. After injection is terminated or the perturbations are removed, /psi/ leaves its initial form /psi//sub o/, and migrates toward its final form, /psi//sub s/. This transient behavior of /psi/ can be obtained by solving the time-dependent Fokker-Planck equation which satisfies the boundary condition /psi/ = /psi//sub o/ at t = 0. It will be shown in this report that the time-dependent particle distribution function can be expressed in a similar form as /psi//sub s/ except that the A/sub ij/'s are functions of time. A solution for A/sub ij/(t) will be described, and an example will be presented as an illustration. The result could be applied to find the quantum loss rate due to an aperture limit. Smooth approximation will be used in the analysis. 7 refs.

Research Organization:
Stanford Linear Accelerator Center, Menlo Park, CA (USA)
DOE Contract Number:
AC03-76SF00515
OSTI ID:
6955591
Report Number(s):
SLAC-PEP-NOTE-189; PEP-131; ON: DE88014834
Country of Publication:
United States
Language:
English