Quantum Monte Carlo Simulation of Bipolaron Superconductivity in Extended Hubbard–Holstein models on Face‐Centered‐Cubic and Body‐Centered‐Cubic Lattices

ABSTRACT We investigate superlight pairing of bipolarons driven by electron‐phonon interactions (EPIs) in face‐center‐cubic (FCC) and body‐center‐cubic (BCC) lattices using a continuous‐time path‐integral quantum Monte Carlo (QMC) algorithm. The EPIs are of the Holstein and extended Holstein types, and a Hubbard interaction is also included. Effects of adiabaticity are calculated. The number of phonons associated with the bipolaron, inverse mass, and radius are calculated and used to construct a phase diagram for bipolaron pairing (identifying the regions of pairing into intersite bipolarons and onsite bipolarons). From the inverse mass we determine that for the extended interaction, there is a region of light pairing associated with intersite bipolarons formed in both BCC and FCC lattices. Intersite bipolarons in the extended model at intermediate phonon frequency and large Coulomb repulsion become superlight due to first order hopping effects. We estimate the transition temperature, determining that intersite bipolarons are associated with regions of high transition temperatures.

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Publication Details

Journal
Annalen der Physik
Published
2025-12-14
DOI
https://doi.org/10.1002/andp.202500343
Primary Topic
Physics of Superconductivity and Magnetism
Type
article
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article

Quantum Monte Carlo Simulation of Bipolaron Superconductivity in Extended Hubbard–Holstein models on Face‐Centered‐Cubic and Body‐Centered‐Cubic Lattices

P. E. Kornilovitch, J. P. Hague, Ganiyu D. Adebanjo
Annalen der Physik
Physics of Superconductivity and Magnetism
article

Quantum Monte Carlo Simulation of Bipolaron Superconductivity in Extended Hubbard–Holstein models on Face‐Centered‐Cubic and Body‐Centered‐Cubic Lattices

P. E. Kornilovitch, J. P. Hague, Ganiyu D. Adebanjo
article en

Abstract

ABSTRACT We investigate superlight pairing of bipolarons driven by electron‐phonon interactions (EPIs) in face‐center‐cubic (FCC) and body‐center‐cubic (BCC) lattices using a continuous‐time path‐integral quantum Monte Carlo (QMC) algorithm. The EPIs are of the Holstein and extended Holstein types, and a Hubbard interaction is also included. Effects of adiabaticity are calculated. The number of phonons associated with the bipolaron, inverse mass, and radius are calculated and used to construct a phase diagram for bipolaron pairing (identifying the regions of pairing into intersite bipolarons and onsite bipolarons). From the inverse mass we determine that for the extended interaction, there is a region of light pairing associated with intersite bipolarons formed in both BCC and FCC lattices. Intersite bipolarons in the extended model at intermediate phonon frequency and large Coulomb repulsion become superlight due to first order hopping effects. We estimate the transition temperature, determining that intersite bipolarons are associated with regions of high transition temperatures.

Annalen der PhysikVol. 538(1)
Oregon State University (US), The Open University (GB)
Openalex Percentile: Top 74%
Physics of Superconductivity and Magnetism
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Quantum Monte Carlo Simulation of Bipolaron Superconductivity in Extended Hubbard–Holstein models on Face‐Centered‐Cubic and Body‐Centered‐Cubic Lattices — P. E. Kornilovitch, J. P. Hague, et al. · Annalen der Physik (2025) | TGRS Research Map | TGRS