For the SPARC photoinjector commissioning the emittance compensation process has been studied experimentally under different beam conditions (variation of charge, spot size, beam shape....) by a novel device called “emittance-meter”, consisting in a movable emittance measurement system based on the 1D pepper pot method scanning a region 1.2 m long downstream the RF-gun. The results of a detailed comparison between the measurements and beam dynamics simulations performed by the codes (PARMELA,HOMDYN,TREDI) employed for SPARC design are presented and discussed here
COMPARISON BETWEEN SPARC E-METER MEASUREMENTS AND SIMULATIONS / Ronsivalle, C.; Giannessi, L.; Quattromini, M.; Bacci, A.; Rossi, A. R.; Serafini, L.; Boscolo, M.; Chiadroni, E.; Ferrario, M.; Filippetto, D.; Fusco, V.; Gatti, G.; Migliorati, Mauro; Mostacci, Andrea; Vaccarezza, C.; Vicario, C.; Cianchi, A.; Petrarca, Massimo. - STAMPA. - (2007), pp. 3185-3187. (Intervento presentato al convegno IEEE Particle Accelerator Conference tenutosi a Albuquerque, New Mexico, USA nel June 2007).
COMPARISON BETWEEN SPARC E-METER MEASUREMENTS AND SIMULATIONS
E. Chiadroni;MIGLIORATI, Mauro;MOSTACCI, Andrea;PETRARCA, MASSIMO
2007
Abstract
For the SPARC photoinjector commissioning the emittance compensation process has been studied experimentally under different beam conditions (variation of charge, spot size, beam shape....) by a novel device called “emittance-meter”, consisting in a movable emittance measurement system based on the 1D pepper pot method scanning a region 1.2 m long downstream the RF-gun. The results of a detailed comparison between the measurements and beam dynamics simulations performed by the codes (PARMELA,HOMDYN,TREDI) employed for SPARC design are presented and discussed hereI documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.
