“…A nonlinear medium is susceptible to filamentation instability, which is characterized by growing electron density and irradiance fluctuations, transverse to the direction of propagation of the beam. There are two complementary approaches to the study of the filamentation instability in a plasma, as discussed by In the first usual approach (Askaryan,1962;Talanov, 1966;Hora, 1967;Palmer, 1971;Kaw et al, 1973;Max et al, 1974;Drake et al, 1974;Mannheimer and Ott, 1974;Perkins and Valeo, 1974;Yu et al, 1974;Chen, 1974;Sodha et al, 1976a;Sodha et al, 1976b;Bingham and Lashmore, 1976;Sodha and Tripathi, 1977;Gurevich, 1978;Perkins and Goldman, 1981;Kruer et al, 1985;Epperlein, 1990;Berger et al, 1993;Ghanshyam and Tripathi, 1993;Wilks et al, 1994;Kaiser et al, 1994;Vidal and Johnston, 1996;Lal et al, 1997;Guzdar et al, 1998;Bendib et al, 2006;Keskinen and Basu, 2003;Gondarenko et al, 2005), one considers an refer to the components of the wave number k of the instability parallel and perpendicular to the direction of propagation viz., z axis. The instability grows or not, as the beam propagates, depending on whether k || is imaginary or real.…”