ELECTRONIC DEPHASING AND ELECTRON-PHONON COUPLING OF ALUMINUM PHTHALOCYANINE TETRASULFONATE IN HYPERQUENCHED AND ANNEALED GLASSY FILMS OF ETHANOL AND METHANOL OVER A BROAD TEMPERATURE-RANGE
T. Reinot et al., ELECTRONIC DEPHASING AND ELECTRON-PHONON COUPLING OF ALUMINUM PHTHALOCYANINE TETRASULFONATE IN HYPERQUENCHED AND ANNEALED GLASSY FILMS OF ETHANOL AND METHANOL OVER A BROAD TEMPERATURE-RANGE, The Journal of chemical physics, 106(2), 1997, pp. 457-466
The electronic dephasing (spectral dynamics) and electron-phonon coupl
ing of aluminum phthalocyanine tetrasulphonate (APT) in glassy films o
f ethanol and methanol were investigated by nonphotochemical hole burn
ing over a broad temperature range, similar to 5-100 K. Films formed b
y hyperquenching (similar to 10(6) K s(-1)) at 4.7 K were studied as w
ell as films that were subsequently annealed at temperatures up to sim
ilar to 170 K. Results are compared against those for APT in glassy wa
ter [Kim et al., J. Phys. Chem. 99, 7300 (1995); Reinot et al., J. Che
m. Phys. 104, 793 (1996)]. As in the case of water, the linear couplin
g is weak with a Huang-Rhys factor S similar to 0.4 but:the mean phono
n frequencies for ethanol and methanol of 26 and 17 cm(-1) are conside
rably lower than the 38 cm(-1) value for water. These modes are assign
ed as pseudolocalized with significant amplitude (libration) localized
an APT. Below about 8 K, the electronic dephasing/spectral diffusion
is dominated by coupling to the tunneling intrinsic two-level systems
of the glass. At higher temperatures the electronic dephasing is domin
ated by the exchange coupling mechanism, which derives from diagonal q
uadratic electron-phonon coupling. Here, for both ethanol and water, a
pseudolocalized model(s) at similar to 50 cm(-1) is operative. This f
requency corresponds to a peak in the spectral density of the liquids
which for water is due to the transverse acoustic mode. The results sh
ow that the modes responsible for linear and quadratic coupling are di
stinctly different. Implications of this for optical coherence loss in
liquids are considered. Novel results from annealing experiments are
reported and discussed in terms of the complex phase diagrams of ethan
ol and methanol. Formation of the glass from the supercooled liquid ju
st above the melting point of a crystalline phase leads to a marked re
duction (similar to 10X) in the homogeneous width of the zero-phonon h
ole at 4.7 K. This is interpreted in terms of a reduction in the densi
ty of intrinsic two-level systems due to reduced structural disorder o
f the glass formed from the supercooled liquid. As in the case of wate
r, the highly efficient hole burning in glassy ethanol and methanol is
observed to become highly inefficient upon formation of a crystalline
phase as predicted by the Shu-Small mechanism for nonphotochemical ho
le burning. The close connection between this mechanism and Onsager's
inverse snowball effect for solvent dynamics around an instantaneously
created point charge or dipole in a liquid is emphasized. (C) 1997 Am
erican Institute of Physics.