RELAXATION PROCESSES YIELDING NONLINEAR EXCITATIONS IN THE EXTENDED PEIERLS-HUBBARD MODEL FOR PHOTOEXCITED MX CHAINS

Authors
Citation
K. Iwano, RELAXATION PROCESSES YIELDING NONLINEAR EXCITATIONS IN THE EXTENDED PEIERLS-HUBBARD MODEL FOR PHOTOEXCITED MX CHAINS, Journal of the Physical Society of Japan, 66(4), 1997, pp. 1088-1096
Citations number
19
Categorie Soggetti
Physics
ISSN journal
00319015
Volume
66
Issue
4
Year of publication
1997
Pages
1088 - 1096
Database
ISI
SICI code
0031-9015(1997)66:4<1088:RPYNEI>2.0.ZU;2-8
Abstract
The relaxations occurring after photoexcitation in the MX chains are i nvestigated, using a one-dimensional extended Peierls-Hubbard model. T he special emphasis is placed on the processes in which the nonlinear excitations such as solitons and polarons are created in the backgroun d of the charge-density wave (CDW). The way of relaxations changes its nature, depending mainly on the relative strengths of the on-site and nearest-neighbor Coulombic repulsions U and V, respectively, to the o n-site electron-lattice interaction S. When U or both L and V dominate over S, soliton-pair states are unstable compared with the self-trapp ed exciton (STE) in the localized Limit of the model. However, the neu tral-soliton pair can be the lowest structural excitation in intermedi ate-transfer cases. stabilized by the effect of itineracy. As for the adiabatic potential surfaces, the uniform CDW is connected to the neut ral-soliton pair, while the STE to the charged-soliton pair. It is exp ected that the STE will make a transition to the neutral-soliton pair nonadiabatically. When S dominates over U and V, on the other hand! th e charged-soliton pair is the lowest structural excitation even in the localized limit. In those cases, the uniform CDW is connected to the charged-soliton pair, while the STE to the neutral-soliton pair on the same potential surfaces. Following these considerations, the calculat ion of the photoinduced absorption is also performed assuming that the former case is realistic. The obtained spectrum in the presence of a neutral soliton is compared with the experimental result.