Experimental characterization of CANDELA photo-injector

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

Volumn 393, Issue 1-3, 1997, Pages 451-454

  Travier, C ^a   Devanz, G ^a   Leblond, B ^a   Mouton, B ^a  

^a UNIVERSITÉ PARIS SUD   (France)

Author keywords

[No Author keywords available]

Indexed keywords

ELECTRIC POWER MEASUREMENT; ELECTRON SOURCES; LASER PULSES; PHOTOCATHODES; SOLID STATE LASERS;

BUNCH LENGTH MEASUREMENT; PHOTOINJECTORS;

INJECTION LASERS;

EID: 0031192193     PISSN: 01689002     EISSN: None     Source Type: Journal    
DOI: 10.1016/S0168-9002(97)00544-5     Document Type: Article

References (14)

1. C. Travier, AIP Proc. 335 (1995) 57.
2. C. Travier, J. Gao, LAL (Orsay) RF Gun Project, in: Proc. European Particle Accelerator Conf., Nice, 1990, pp. 706.
3. C. Travier, J. Gao, H. Liu, LAL (Orsay) RF Gun Simulations and Model Cavity Design, in: Proc. Linear Accelerator Conf., Albuquerque, NM, 1990, pp. 602.
4. J. Gao et al., CANDELA Photoinjector Status Report, in: Proc. European Particle Accelerator Conf., Berlin, 1992, pp. 1020.
5. B. Leblond, Nucl. Instr. and Meth. A 317 (1992) 365.
6. P. Georges et al., CANDELA photo-injector drive laser, in: Proc. Particle Accelerator Conf., Washington, 1993, pp. 3053.
7. C. Travier et al., First operation of a femtosecond laser driven photo-injector, in: Proc. European Particle Accelerator Conf., London, 1994, pp. 1462.
8. C. Travier et al., CANDELA photo-injector experimental results with a dispenser photocathode, in: Proc. Particle Accelerator Conf., Dallas, TX, 1995, pp. 945.
9. Original Version from K. Crandall, L. Young (LANL). Version used at Orsay modified by B. Mouton, The PARMELA Program, LAL/SERA 93-455, 1993.
10. C. Travier et al., Nucl. Instr. and Meth. B 89 (1994) 27.
11. ARP, Centre de Transfert de technologies, Route de Hausbergen, F67088 Strasbourg, France.
12. G. Devanz et al., Bunch length measurement on CANDELA photo-injector, in: Proc. Linear Accelerator Conf., Geneva, 1996, p. 761.
13. 12 is the phase of the field in the second cell when the phase of the field in the first cell is 0. With this definition 180° would correspond to π-mode.
14. D.H. Dowell et al., Nucl. Instr. and Meth. A 375 (1996) 104.