“…The dispersive section is either a three-or foursection chicane where the electrons experience modulation without resonant interaction. Without resonant interaction in the dispersive section, the small changes in the electron velocity lead to phase modulation and this leads to enhanced emission of radiation in the second section of the undulator, called the radiator (Dattoli & Bucci, 2000a,b;Dattoli et al, 1993;Gehlot & Mishra, 2010;Elleaume, 1986;Kong, 1996). There have been several studies on the optical klystron undulator that explain the modelling of the dispersive section (Boscolo & Colson, 1985;Colson & Fredman, 1983;Gallardo & Pellegrini, 1990a,b;Thomas et al, 2002;Elleaume, 1983;Vinokurov & Skrinsky, 1977;Vinokurov, 1977;Artamonov et al, 1980).…”