A new method for the measurement of the phase shift between second-har
monic light generated by a bulk glass and the injected second-harmonic
seed is presented. A linearly polarized pump and a second-harmonic se
ed with noncollinear polarizations were used for preparation of cerium
-doped lead-silica glass. Independence of the phase shift from the ang
le between the polarizations of the recording waves is demonstrated, a
nd a phase shift value close to 90-degrees is observed, i.e., the chi(
2) grating was in phase with the real [E(EE)].