  We give a new expression for the law of the eigenvalues of the discrete
Anderson model on the finite interval $[0,N]$, in terms of two random processes
starting at both ends of the interval. Using this formula, we deduce that the
tail of the eigenvectors behaves approximatelylike $\exp(\sigma
B\_{|n-k|}-\gamma\frac{|n-k|}{4})$ where $B\_{s}$ is the Brownian motion and
$k$ is uniformly chosen in $[0,N]$ independentlyof $B\_{s}$. A similar result
has recently been shown by B. Rifkind and B. Virag in the critical case, that
is, when the random potential is multiplied by a factor $\frac{1}{\sqrt{N}}$
