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Title: Weak-strong instability as a diffusion process

Abstract

The phenomenological analysis of the weak-strong instability for an electron storage ring is developed. The vertical size of the weak beam is found to depend on two machine parameters: {radical}{eta}, which is proportional to {Delta}Q, and b, which depends on the aspect ratio of the strong beam. The model also contains one fitting parameter. Experimental consequences of such dependence are discussed. 5 refs., 7 figs.

Authors:
Publication Date:
Research Org.:
Stanford Linear Accelerator Center, Menlo Park, CA (USA)
OSTI Identifier:
5788430
Report Number(s):
SLAC-PEP-NOTE-278; SLAC-PUB-2252; CONF-790327-161
ON: DE89006310; TRN: 89-006181
DOE Contract Number:  
AC03-76SF00515
Resource Type:
Conference
Resource Relation:
Conference: IEEE particle accelerator conference, San Francisco, CA (United States), 12-14 Mar 1979
Country of Publication:
United States
Language:
English
Subject:
43 PARTICLE ACCELERATORS; STORAGE RINGS; BEAM-BEAM INTERACTIONS; BEAM BUNCHING; BETATRON OSCILLATIONS; DIFFUSION; DISTRIBUTION FUNCTIONS; FOKKER-PLANCK EQUATION; INSTABILITY; BEAM DYNAMICS; DIFFERENTIAL EQUATIONS; EQUATIONS; FUNCTIONS; OSCILLATIONS; PARTIAL DIFFERENTIAL EQUATIONS; 430400* - Particle Accelerators- Storage Rings; 430200 - Particle Accelerators- Beam Dynamics, Field Calculations, & Ion Optics

Citation Formats

Kheifets, S.A. Weak-strong instability as a diffusion process. United States: N. p., 1979. Web.
Kheifets, S.A. Weak-strong instability as a diffusion process. United States.
Kheifets, S.A. Thu . "Weak-strong instability as a diffusion process". United States. https://www.osti.gov/servlets/purl/5788430.
@article{osti_5788430,
title = {Weak-strong instability as a diffusion process},
author = {Kheifets, S.A.},
abstractNote = {The phenomenological analysis of the weak-strong instability for an electron storage ring is developed. The vertical size of the weak beam is found to depend on two machine parameters: {radical}{eta}, which is proportional to {Delta}Q, and b, which depends on the aspect ratio of the strong beam. The model also contains one fitting parameter. Experimental consequences of such dependence are discussed. 5 refs., 7 figs.},
doi = {},
journal = {},
number = ,
volume = ,
place = {United States},
year = {1979},
month = {2}
}

Conference:
Other availability
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