A frequency-domain description of the second-harmonic generation by us
ing laser pulses is presented. The influences of the pulse spectrum an
d of the crystal dispersion are taken into account which, for high int
ensities at perfect phase-matching can produce stretching and eventual
ly breaking of the pulse. A double autocorrelator has bern constructed
tu monitor the pulse breaking during perfectly-matched second harmoni
c generation in a type I KDP crystal. A double passage inside the crys
tal was necessary to measure the nonlinear phase that the fundamental
beam experiences during the first generation. (C) 1998 Elsevier Scienc
e B.V.