“…This could proceed either directly, through the unstable wave-beam interaction (Malkin & Fisch 2002), or indirectly, through an instability-induced increased plasma resistivity (Sentoku et al 2003). In contrast to past studies, which mostly focused on electrostatic beam-aligned instabilities, recent FIS-related theoretical works have considered the whole unstable k-spectrum (Bret et al 2004, Califano et al 2006, Bret et al 2006, Cottrill et al 2008, Karmakar et al 2009, Bret, Gremillet & Bénisti 2010, Bret, Gremillet & Dieckmann 2010, paying particular attention to the quasi-magnetic filamentation modes developing normal to the beam direction (Pegoraro et al 1996, Califano et al 1998, Sentoku et al 2000, Honda & Meyer-ter-Vehn 2000, Taguchi et al 2001, Silva et al 2002, Hill et al 2005, Kato 2005, Adam et al 2006, Schaefer-Rolffs et al 2006, Mart'yanov et al 2008, Karmakar, Kumar, Shvets, Polomarov & Pukhov 2008, Khudik et al 2012. Being all the stronger when the beam and plasma densities are comparable , the collisionless instabilities are most likely to disrupt the early propagation of the beam into the "low"-density regions of the target.…”