Abstract
In this note we explore the conditions under which synchrotron radiation can be used to trigger a photocathode gun. We show that such a solution offers in principle the possibility of operating with a pulsed electron beam filling all the buckets of the accelerating radio frequency. Some comments on the e-beam characteristics are also presented.
Similar content being viewed by others
References
J.S. Fraser, R.L. Sheffield: IEEE QE-23, 1489 (1987)
J. Fisher, T. Srinivasan Rao: In Proc. ECPA Workshop, New Developments in Particle Accelerators Techniques, ed. by S. Turner (CER 87–11 1987) p. 506
D.W. Feldmann et al.: IEEE QE-27, 2636 (1991)
K.J. Kim: Nucl. Instrum. Methods A275, 201 (1989)
L. Serafini, M. Ferrario, C. Pagani, R. Rivolta: INFN/TC-91/07 (June 1991)
L. Serafini et al.: INFN/TC-90/10 (1990)
R. Barbini, F. Ciocci, G. Dattoli, L. Giannessi: La rivista del Nuovo Cimento 6 (1990)
A.H. Sommer: Photoemissive Materials (Wiley, New York 1968) p. 70
S. Krinsky, M.L. Perlmann, R.E. Watson: Synchrotron Radiation, Vol 1 (North-Holland, Amsterdam 1983)
G. Dattoli, C. Mari, A. Torre: Submitted to Phys. Rev. A
R. Barbini, F. Ciocci, G. Dattoli, A. Dipace, L. Giannessi, G. Maino, C. Mari, A. Marino, C. Ronsvialle, E. Sabia, A. Torre: ENEA RT/INN/90/35 (1990)
Usually the factor of proportionality between laser and electron power is given to be 1/(2N u), more recent analysis have shown that it is 1/(4N u), for more specific details see: G. Dattoli, L. Giannessi, S. Cabrini: Phys. Rev. A, 44, 8433 (1991)
K.J. Kim, Ming Xie: Nucl. Instrum. Methods A304, 146 (1991)