4.6 Article

Superconductivity, charge density waves, and bipolarons in the Holstein model

Journal

PHYSICAL REVIEW B
Volume 103, Issue 23, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.103.235156

Keywords

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Funding

  1. U.S. Department of Energy, Office of Basic Energy Sciences, Division of Materials Sciences and Engineering [DE-AC02-76SF00515]
  2. NSF at Stanford [DMR-1608055]
  3. Harvard Quantum Initiative Postdoctoral Fellowship in Science and Engineering
  4. Gordon and Betty Moore Foundation EPiQS Initiative [GBMF 4305, GBMF 8691]
  5. Scientific Discovery through Advanced Computing (SciDAC) program - U.S. Department of Energy, Office of Science, Advanced Scientific Computing Research and Basic Energy Sciences, Division of Materials Sciences and Engineering

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A study on the two-dimensional electron-phonon coupling in the Holstein model explores CDW correlations, competition between superconducting and CDW orders, and polaron formation. It was found that superconductivity is optimized at intermediate e-ph coupling strength and intermediate electron density.
The electron-phonon (e-ph) interaction remains of great interest in condensed matter physics and plays a vital role in realizing superconductors, charge density waves (CDW), and polarons. We study the two-dimensional Holstein model for e-ph coupling using determinant quantum Monte Carlo across a wide range of its phase diagram as a function of temperature, electron density, dimensionless e-ph coupling strength, and the adiabatic ratio of the phonon frequency to the Fermi energy. We describe the behavior of the CDW correlations, the competition between superconducting and CDW orders and polaron formation, the optimal conditions for superconductivity, and the transition from the weak-coupling regime to the strong-coupling regime. Superconductivity is optimized at intermediate e-ph coupling strength and intermediate electron density, and the superconducting correlations increase monotonically with phonon frequency. The global maximum for superconductivity in the Holstein model occurs at large phonon frequency, the limit where an attractive Hubbard model effectively describes the physics.

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