Quantized lattice dynamic effects on the Peierls transition of the extended Hubbard-Peierls model
The density matrix renormalization group method is used to investigate the Peierls transition for the extended Hubbard model coupled to quantized phonons. Following our earlier work on spin-Peierls systems, we use a phonon spectrum that interpolates between a gapped, dispersionless (Einstein) limit...
| Autores principales: | , , |
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| Formato: | Journal article |
| Lenguaje: | English |
| Publicado: |
2011
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| _version_ | 1826257897046147072 |
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| author | Pearson, C Barford, W Bursill, R |
| author_facet | Pearson, C Barford, W Bursill, R |
| author_sort | Pearson, C |
| collection | OXFORD |
| description | The density matrix renormalization group method is used to investigate the Peierls transition for the extended Hubbard model coupled to quantized phonons. Following our earlier work on spin-Peierls systems, we use a phonon spectrum that interpolates between a gapped, dispersionless (Einstein) limit and a gapless, dispersive (Debye) limit to investigate the entire frequency range. A variety of theoretical probes are used to determine the quantum phase transition, including energy gap crossing, a finite-size scaling analysis, and bipartite quantum entanglement. All these probes indicate that a transition of Berezinskii-Kosterlitz-Thouless type is observed at a nonzero electron-phonon coupling gc for a nonvanishing electron-electron interaction. An extrapolation from the Einstein limit to the Debye limit is accompanied by an increase in gc for a fixed optical (q=π) phonon gap. We therefore conclude that the dimerized ground state is more unstable with respect to Debye phonons, with the introduction of phonon dispersion renormalizing the effective electron-lattice coupling for the Peierls-active mode. By varying the Coulomb interaction U, we observe a generalized Peierls transition, intermediate between the uncorrelated (U=0) and spin-Peierls (U→) limits, where U is the Hubbard Coulomb parameter. Using the extended Hubbard model with Debye phonons, we investigate the Peierls transition in trans-polyacetylene and show that the transition is close to the critical regime. © 2011 American Physical Society. |
| first_indexed | 2024-03-06T18:25:26Z |
| format | Journal article |
| id | oxford-uuid:07c9d6a7-3c85-44b5-8de8-0a5e8f120da6 |
| institution | University of Oxford |
| language | English |
| last_indexed | 2024-03-06T18:25:26Z |
| publishDate | 2011 |
| record_format | dspace |
| spelling | oxford-uuid:07c9d6a7-3c85-44b5-8de8-0a5e8f120da62022-03-26T09:09:28ZQuantized lattice dynamic effects on the Peierls transition of the extended Hubbard-Peierls modelJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:07c9d6a7-3c85-44b5-8de8-0a5e8f120da6EnglishSymplectic Elements at Oxford2011Pearson, CBarford, WBursill, RThe density matrix renormalization group method is used to investigate the Peierls transition for the extended Hubbard model coupled to quantized phonons. Following our earlier work on spin-Peierls systems, we use a phonon spectrum that interpolates between a gapped, dispersionless (Einstein) limit and a gapless, dispersive (Debye) limit to investigate the entire frequency range. A variety of theoretical probes are used to determine the quantum phase transition, including energy gap crossing, a finite-size scaling analysis, and bipartite quantum entanglement. All these probes indicate that a transition of Berezinskii-Kosterlitz-Thouless type is observed at a nonzero electron-phonon coupling gc for a nonvanishing electron-electron interaction. An extrapolation from the Einstein limit to the Debye limit is accompanied by an increase in gc for a fixed optical (q=π) phonon gap. We therefore conclude that the dimerized ground state is more unstable with respect to Debye phonons, with the introduction of phonon dispersion renormalizing the effective electron-lattice coupling for the Peierls-active mode. By varying the Coulomb interaction U, we observe a generalized Peierls transition, intermediate between the uncorrelated (U=0) and spin-Peierls (U→) limits, where U is the Hubbard Coulomb parameter. Using the extended Hubbard model with Debye phonons, we investigate the Peierls transition in trans-polyacetylene and show that the transition is close to the critical regime. © 2011 American Physical Society. |
| spellingShingle | Pearson, C Barford, W Bursill, R Quantized lattice dynamic effects on the Peierls transition of the extended Hubbard-Peierls model |
| title | Quantized lattice dynamic effects on the Peierls transition of the extended Hubbard-Peierls model |
| title_full | Quantized lattice dynamic effects on the Peierls transition of the extended Hubbard-Peierls model |
| title_fullStr | Quantized lattice dynamic effects on the Peierls transition of the extended Hubbard-Peierls model |
| title_full_unstemmed | Quantized lattice dynamic effects on the Peierls transition of the extended Hubbard-Peierls model |
| title_short | Quantized lattice dynamic effects on the Peierls transition of the extended Hubbard-Peierls model |
| title_sort | quantized lattice dynamic effects on the peierls transition of the extended hubbard peierls model |
| work_keys_str_mv | AT pearsonc quantizedlatticedynamiceffectsonthepeierlstransitionoftheextendedhubbardpeierlsmodel AT barfordw quantizedlatticedynamiceffectsonthepeierlstransitionoftheextendedhubbardpeierlsmodel AT bursillr quantizedlatticedynamiceffectsonthepeierlstransitionoftheextendedhubbardpeierlsmodel |