Ab. Borisov et al., STABILITY ANALYSIS OF RELATIVISTIC AND CHARGE-DISPLACEMENT SELF-CHANNELING OF INTENSE LASER-PULSES IN UNDERDENSE PLASMAS, Plasma physics and controlled fusion, 37(5), 1995, pp. 569-597
The stability against small azimuthal perturbations of confined modes
of propagation of intense short-pulse radiation governed by relativist
ic and charge-displacement nonlinearities in underdense plasmas is exa
mined theoretically. In the plane of the dimensionless parameters rho(
0) = tau(0) omega(p,0)/c and eta = P-0/P-cr, defined by the critical p
ower (P-cr) and the initial conditions represented by the focal radius
(tau(0)) of the incident radiation, the unperturbed plasma frequency
(omega(p,0)), and the peak incident power (P-0), zones corresponding t
o stable (single-channel) and unstable (strong filamentation) regimes
of propagation are established. The general finding is that large regi
ons of stable propagation exist. The results show that for values of r
ho(0) sufficiently close to the dimensionless radius of the zeroth eig
enmode rho(e,0), the self-channelling is stable for all values of eta
> 1, a condition of exceptional robustness. It is also found that for
the region 1 < eta less than or similar to 10, the propagation is stab
le for a very wide range of values of rho(0). In addition, the locatio
n of the boundary separating the stable and unstable zones is largely
independent of the curvature of the phase front of the incident wave a
nd weakly influenced both by the magnitudes of the azimuthal perturbat
ions and the detailed radial profile of the incident radiation. Since
self-focusing generated solely by relativistic mechanisms tends strong
ly to unstable behaviour in the eta >> 1 regime, these results demonst
rate the crucial role of the ponderomotively driven charge displacemen
t in stabilizing the propagation. Physically, the ponderomotive radial
displacement of the electrons and the contrasting inertial confinemen
t of the ions simultaneously produce the two chief characteristics of
the channels. They are the refractive self-focusing of the propagating
energy arising from the displaced electrons and the spatial stability
of the channels produced by the immobile electrostatic spine formed b
y the ions.