Tw. Hagler et Aj. Heeger, QUANTUM-LATTICE FLUCTUATIONS AND THE LINEAR AND NONLINEAR-OPTICAL SUSCEPTIBILITY OF DEGENERATE GROUND-STATE CONJUGATED POLYMERS, Progress of theoretical physics. Supplement, (113), 1993, pp. 65-81
The contributions of soliton-antisoliton (SSBAR) configurations to the
linear and third-order nonlinear optical response are investigated fo
r conjugated polymers having a degenerate ground state.1),2) We treat
the direct photoproduction of charged solitons as a nonlinear Franck-C
ondon problem and obtain analytical expressions for the linear optical
susceptibility, chi(1)(omega). With the help of the oscillator streng
th sum rule, we decompose the pi-pi oscillator strength into two part
s; a contribution where the final states are SSBAR pairs and a contrib
ution where the final states are free electron-hole pairs (as in the n
oninteracting rigid-lattice). The linear optical coefficients calculat
ed from chi(1)(omega) are in general agreement with optical data obtai
ned from trans-polyacetylene. The results imply that approximately 25%
of the integrated oscillator strength of trans-polyacetylene arises f
rom the direct photoproduction of solitons. A parallel treatment of th
e generalized third-order nonlinear optical susceptibility, chi(3)(ome
ga), is presented, demonstrating that, for any third-order process, co
ntributions arising from neutral SSBAR pair configurations as intermed
iate states are one to two orders of magnitude larger than the corresp
onding rigid-lattice contribution. This mechanism for chi(3) is enable
d by nonlinear zero-point motion which provides a finite Franck-Condon
overlap between the ground and Sg excited state lattice wavefunctions
. The large contribution to chi(3) from the SSBAR intermediate states
results from the large transition dipole moment between the free elect
ron-hole pair excited states of B(u) symmetry and the A(g) symmetric n
eutral SSBAR excited state. This enhanced transition dipole moment is
a consequence of the large virtual shifts of oscillator strength assoc
iated with the localized Sg electron-lattice configuration. The third-
harmonic conversion efficiency chi(3)(3omega) is further enhanced by a
condition unique to degenerate ground state systems, simultaneous two
and three-photon resonance.