Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:cond-mat/0505687 · The European Physical Journal B

Analytical approach to the quantum-phase transition in the one-dimensional spinless Holstein model

Steffen Sykora, A. Hübsch, K. W. Becker

Published May 1, 2006• 13 citations
arXivHTMLPDF
DOI
10.1140/epjb/e2006-00211-1

Related papers

Quantum phase transition in a one-dimensional Holstein-Hubbard model at half-filling in the thermodynamic limit: A quantum entanglement approach

I. V. Sankar, Ashok Chatterjee

Physica B Condensed Matter•Feb 20, 2016•10 citations

Nature of the self-trapping transition in a one-dimensional Holstein–Hubbard model

R.P. Murali Krishna, Soma Mukhopadhyay, Ashok Chatterjee

Physics Letters A•May 8, 2004•9 citations

A semi-exact analytical study of the phase diagram of the two dimensional extended Holstein-Hubbard model

Debika Debnath, Kuntal Bhattacharyya, Ashok Chatterjee

Physica B Condensed Matter•Nov 27, 2023•0 citations

Nature of the self-trapping transition in a one-dimensional Holstein?Hubbard model

R MURALIKRISHNA

Physics Letters A•May 1, 2004•0 citations

Phase diagram and optical conductivity of the one-dimensional spinless Holstein model

Q. Wang, H. Zheng, M. Avignon

The effects of quantum lattice fluctuations on the Peierls transition and the optical conductivity in the one-dimensional Holstein model of spinless fermions have been studied by developing an analytical approach based on the unitary transformation method. We show that when the electron-phonon coupling constant decreases to a finite critical value, the Peierls dimerization is destroyed by the quantum lattice fluctuations. The dimerization gap is much more reduced by the quantum lattice fluctuations than the phonon order parameter. The calculated optical conductivity does not have the inverse-square-root singularity, but it has a peak above the gap edge, and there exists a significant tail below the peak. The peak of optical-conductivity spectrum is not directly corresponding to the dimerized gap. Our results of the phase diagram and the spectral-weight function agree with those of the density-matrix renormalization group and the exact diagonalization methods.

arXiv:cond-mat/0105003•Physical review. B, Condensed matter•Dec 12, 2000•14 citations

Phase diagram for the one-dimensional Hubbard-Holstein model

Masaki Tezuka, Ryotaro Arita, Hideo Aoki

•Jul 21, 2007•0 citations
The effects of quantum lattice fluctuations on the Peierls transition and the optical conductivity in the one-dimensional Holstein model of spinless fermions have been studied by developing an analytical approach based on the unitary transformation method. We show that when the electron-phonon coupling constant decreases to a finite critical value, the Peierls dimerization is destroyed by the quantum lattice fluctuations. The dimerization gap is much more reduced by the quantum lattice fluctuations than the phonon order parameter. The calculated optical conductivity does not have the inverse-square-root singularity, but it has a peak above the gap edge, and there exists a significant tail below the peak. The peak of optical-conductivity spectrum is not directly corresponding to the dimerized gap. Our results of the phase diagram and the spectral-weight function agree with those of the density-matrix renormalization group and the exact diagonalization methods.