Beam induced RF cavity transient voltage

Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment

Volumn 423, Issue 2-3, 1999, Pages 260-264

  Kramer, S L ^a   Wang, Jiunn Ming ^a  

^a BROOKHAVEN NATIONAL LABORATORY   (United States)

Author keywords

29.27; 61.16.B; 61.80.F; Beam loading; RF superconducting cavity; Transient voltage

Indexed keywords

ELECTRIC CURRENTS; ELECTRIC POTENTIAL; MATHEMATICAL MODELS; PARTICLE ACCELERATORS; PARTICLE BEAM INJECTION; SUPERCONDUCTING DEVICES;

RADIATION INDUCED TRANSIENT VOLTAGE; RADIO FREQUENCY SUPERCONDUCTING CAVITIES;

RADIATION EFFECTS;

EID: 0033098515     PISSN: 01689002     EISSN: None     Source Type: Journal    
DOI: 10.1016/S0168-9002(98)01369-2     Document Type: Article

References (7)

1. Murphy J.B., Krinsky S. Nuc. Instr. and Meth. A. 346:1994;571.
2. K. Bane, P. Wilson, T. Weiland, AIP Conf. Proc. 127 (1985).
3. P. Wilson, AIP Conf. Proc. 87 (1981) 452. For an elegant and intuitive treatment of this theorem, see Boussard's paper on beam loading cited below.
4. D. Boussard, Proc. CERN Accel. School, CERN 87-03, p. 626. The discrepancy between Boussard's Eq. (8) and our Eq. (22) is due to the fact that Boussard's expression describes the voltage seen by the beam (τ = 0) , while our expression is for τ > 0 . Boussard's expression can be obtained easily from ours by using the fundamental theorem of beam loading.
5. J.M. Wang, C. Pellegrini, BNL-51236, 1979.
6. Towne N., Wang J.M. Phys. Rev. E. 57:1998;3461.
7. Biscardi R. et al. Rev. Sci. Instrum. 66:1995;1856.