Abstract
The two-dimensional extended Holstein-Hubbard model is investigated in the strong correlation regime to study the nature of self-trapping transition and the polaron phase diagram in the absence of superconductivity. Using a series of canonical transformations followed by zero-phonon averaging the extended Holstein-Hubbard model is converted into an effective extended Hubbard model which is subsequently transformed into an effective t-J model in the strong correlation limit. This effective t-J model is finally solved using the mean-field Hartree-Fock approximation to show that the self-trapping transition is continuous in the anti-adiabatic limit while it is discontinuous in the adiabatic limit. The phase diagrams for the localization-delocalization transition, namely the phase line and the phase surface separating the small polaron and large polaron states are also shown.
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Sankar, I.V., Chatterjee, A. Self-trapping phase diagram for the strongly correlated extended Holstein-Hubbard model in two-dimensions. Eur. Phys. J. B 87, 154 (2014). https://doi.org/10.1140/epjb/e2014-50146-9
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DOI: https://doi.org/10.1140/epjb/e2014-50146-9