The dynamics of long-wavelength dispersive Alfven wave trains propagating p
arallel to an ambient field in a magnetized plasma is investigated by means
of a three-dimensional extension of the derivative nonlinear Schrodinger e
quation that includes the mean effect of the longitudinal magneto-sonic wav
es. In the strongly dispersive regime, quasi-monochromatic right-hand polar
ized plane waves perturbed by a broad-spectrum noise develop a transverse c
ollapse leading to the formation of strong magnetic filaments parallel to t
he ambient field, as asymptotically predicted by the nonlinear Schrodinger
equation for the wave envelope. In contrast, for left-hand polarized waves
filamentation only takes place when the noise is confined to Fourier modes
with wavenumbers close enough to that of the pump. In the regime where disp
ersion and nonlinearity are comparable, the amplitude growth is strongly in
hibited but intense gradients are still formed, associated with the creatio
n of pancake-like magnetic structures. The transverse focusing of weakly no
nlinear dispersive waves still takes place when the spectrum of the initial
conditions is broadened, in spite of the fragmentation of the magnetic fil
aments into chains of magnetic bubbles and ultimately into randomly distrib
uted three-dimensional structures. (C) 2001 Elsevier Science B.V. All right
s reserved.