  The initial value problem of an integrable system, such as the Nonlinear
Schr\" odinger equation, is solved by subjecting the linear eigenvalue problem
arising from its Lax pair to inverse scattering, and, thus, transforming it to
a matrix Riemann-Hilbert problem (RHP) in the spectral variable. In the
semiclassical limit, the method of nonlinear steepest descent, supplemented by
the $g$-function mechanism, is applied to this RHP to produce explicit
asymptotic solution formulae for the integrable system. These formule are based
on a hyperelliptic Riemann surface $\Rscr=\Rscr(x,t)$ in the spectral variable,
where the space-time variables $(x,t)$ play the role of external parameters.
The curves in the $x,t$ plane, separating regions of different genuses of
$\Rscr(x,t)$, are called breaking curves or nonlinear caustics. The genus of
$\Rscr(x,t)$ is related to the number of oscillatory phases in the asymptotic
solution of the integrable system at the point $x,t$.
  In this paper we prove that in the case of a regular break, the nonlinear
steepest descent asymptotics can be "automatically" continued through the
breaking curve (however, the expressions for the asymptotic solution will be
different on the different sides of the curve). Although the results are stated
and proven for the focusing NLS equation, it is clear that they can be
reformulated for AKNS systems, as well as for the nonlinear steepest descend
method in a more general setting.
