Localization of Large Polarons in the Disordered Holstein Model
arXiv:1403.6749 · doi:10.1103/PhysRevB.89.155434
Abstract
We solve the disordered Holstein model via the DMRG method to investigate the combined roles of electron-phonon coupling and disorder on the localization of a single charge or exciton. The parameter regimes chosen, namely the adiabatic regime, , and the `large' polaron regime, , are applicable to most conjugated polymers. We show that as a consequence of the polaron effective mass diverging in the adiabatic limit (defined as subject to fixed ) self-localized, symmetry breaking solutions are predicted by the quantum Holstein model for infinitesimal disorder -- in complete agreement with the predictions of the Born-Oppenheimer Holstein model. For other parts of the (, ) parameter space, however, self-localized Born-Oppenheimer solutions are not expected. If is not small enough and is not large enough, then the polaron is predominately localized by Anderson disorder, albeit more than for a free particle, because of the enhanced effective mass. Alternatively, for very small electron-nuclear coupling () the disorder-induced localization length is always smaller than the classical polaron size, , so that disorder always dominates. We comment on the implication of our results on the electronic properties of conjugated polymers.
References in corpus (4)
Cited by in corpus (6)
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- Thermally Driven Polaron Transport in Conjugated Polymers
- Disorder Suppression of Charge Density Waves in the Honeycomb Holstein Model