3RD-ORDER RESONANT OPTICAL NONLINEARITY FROM TRANS-CIS PHOTOISOMERIZATION OF AN AZO-DYE IN A RIGID MATRIX
Citation
C. Egami et al., 3RD-ORDER RESONANT OPTICAL NONLINEARITY FROM TRANS-CIS PHOTOISOMERIZATION OF AN AZO-DYE IN A RIGID MATRIX, Applied physics. B, Lasers and optics, 64(4), 1997, pp. 471-478
Categorie Soggetti
Physics, Applied",Optics
SICI code
0946-2171(1997)64:4<471:3RONFT>2.0.ZU;2-5
Abstract
We investigated the trans-cis photoisomerization of an azo dye in a ri
gid matrix and the resulting third-order resonant optical nonlinearity
by means of the simple theoretical prediction of a two-energy-level s
ystem, thin-layer chromatography and H-NMR studies. A methylorange (MO
), a methylred (MR), congored (CR) or a Disperse Red 1 (DR1) doped pol
yvinyl alcohol (PVA) or silica film was used as nonlinear optical mate
rial. The existence of equi-absorbing points, or isosbestic points in
the absorbance spectrum change and the remarkable stationary transmitt
ance to be independent of the action beam intensity enabled us to conf
irm the photoisomerization even in a rigid matrix. Then, we measured t
he third-order resonant optical nonlinearity of dichroism through the
polarization absorbance spectrum measurement and determined the charac
teristic optical parameters of the photoisomerization in the film such
as the quantum yields phi(T), phi(C), the thermal reaction constant K
and the photoisomerization time constant by fitting the theoretical c
urve of the two-energy-level system to the observed temporal transmitt
ance change after the action beam exposure of the MO/PVA film. The qua
ntum yields were <(phi(T))over bar> = 0.36 and <(phi(C))over bar> = 0.
38, respectively. The photoisomerization time constant of MO embedded
in the PVA film was a few seconds. The thermal reaction constant K dep
ended on the excitation beam intensity.