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3 Simulations The experimental results were compared with the code POSINST developed by M. Furman and M. Pivi at LBNL . POSINST calculations at the center of a long field-free section were compared to RFA 6. 5 to account for the transmission attenuation in the experiment (Fig. 1 was assumed for an unconditioned Al surface. Figure 2a shows the comparison between the modeled and measured electron wall current for ten positron bunches as a function of bunch spacing. The model reproduced the broad peak centered at a 7-λ bunch spacing; however, the sharp, resonant peak at 7 λ is not reproduced.
Furman, M. Pivi, in Proc. of Mini-Workshop on Electron-Cloud Simulations for Positron and Proton Beams, CERN Yellow Report No. CERN-2002-001, 69 (2002). L. Kustom, in Proc. fr/Accelerators/Conferences/ID_Workshop/). U. Irizo, in Proc. ch/icfaecloud04/ ). 5 Measurement of electron cloud effects in KEKB H. 1 Introduction A large number of electrons called "an electron cloud" can be generated in positively charged beam. Main sources of the electrons in positron storage rings are photoelectrons generated by the synchrotron radiation and secondary electrons.
Ng, and D. Wildman, in Proc. , Chicago, 688 (IEEE, Piscataway, NJ, 2001). H. Fukuma, in Proc. of Mini-Workshop on Electron-Cloud Simulations for Positron and Proton Beams, CERN Yellow Report No. ch/collective/ecloud02/ ) (2002). M. A. Furman and M. T. F. Pivi, PRST-AB 5, 124404 (2002). K. C. Harkay and R. A. Rosenberg, in Proc. , New York, 1641 (IEEE, Piscataway, NJ, 1999). R. Kirby and F. King, Nucl. Instrum. Methods A469 (1), 1 (2001); also SLAC Report No. SLAC-PUB-8212 (Oct. 2000). 52 11. V.
Beam Dynamics Newsletter 33