Localization of Large Polarons in the Disordered Holstein Model

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, $\hslash \omega /4t_0={\omega }^{\prime }<1$, and the `large' polaron regime, $\lambda <1$, are applicable to most conjugated polymers. We show that as a consequence of the polaron effective mass diverging in the adiabatic limit (defined as ${\omega }^{\prime }\to 0$ subject to fixed $\lambda$) 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 (${\omega }^{\prime }$, $\lambda$) parameter space, however, self-localized Born-Oppenheimer solutions are not expected. If ${\omega }^{\prime }$ is not small enough and $\lambda$ 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 ($\lambda \ll 1$) the disorder-induced localization length is always smaller than the classical polaron size, $2/\lambda$, so that disorder always dominates. We comment on the implication of our results on the electronic properties of conjugated polymers.

References in corpus (4)

• Trapping of three-dimensional Holstein polarons by various impurities
• Trapping of lattice polarons by impurities
• Stochastic Green's function approach to disordered systems
• A perturbational study of the lifetime of a Holstein polaron in the presence of weak disorder

Cited by in corpus (3)

• Charge-density-wave melting in the one-dimensional Holstein model
• Thermally Driven Polaron Transport in Conjugated Polymers
• Disorder Suppression of Charge Density Waves in the Honeycomb Holstein Model