1992
DOI: 10.1103/physrevlett.69.1600
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Polaronic anharmonicity in the Holstein-Hubbard model

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Cited by 96 publications
(83 citation statements)
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“…The on-site phonon is usually interpreted as a vibration of the apical oxygen above a given Cu site [428]. However, it is also possible to interpret the electronic band as an 'effective Cu atom', incorporating the coupling to a symmetric superposition of the wave function on the four neighboring O's (a Zhang-Rice singlet [351]).…”
Section: Appendix B: τ (Xc) In the One Band Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…The on-site phonon is usually interpreted as a vibration of the apical oxygen above a given Cu site [428]. However, it is also possible to interpret the electronic band as an 'effective Cu atom', incorporating the coupling to a symmetric superposition of the wave function on the four neighboring O's (a Zhang-Rice singlet [351]).…”
Section: Appendix B: τ (Xc) In the One Band Modelmentioning
confidence: 99%
“…This means that the coupling can be analyzed in terms of conventional polaronic effects [150]. In fact, the Holstein and Holstein-Hubbard models can also play a role [427][428][429][430]237,51,405], since the associated Umklapp scattering can also split the VHS degeneracy. Note that, while these modes are not condensed in the macroscopic LTO or LTT phases, they could play a role in a dynamic JT or local polaronic picture.…”
Section: Tilt-stretch Mode Couplingmentioning
confidence: 99%
“…From this point of view it is of interest to carry out exact diagonalizations of the HtJM on small clusters. Along this line, a number of ED studies have been performed treating the phonons in the static limit, i.e., classically, in the so-called adiabatic or frozen phonon approximation [42,31,43,44]. The stability of the ground state against static lattice distortions was investigated and the phase diagram of the 2D HtJM has been explored in the one-and two-hole sectors [31], as well as for the quarter-filled band case [44], where a polaronic superlattice was found to occur above a critical EP coupling strength.…”
Section: The Holstein T-j Modelmentioning
confidence: 99%
“…In the weak-coupling (adiabatic) limit, one expects (from scaling arguments) a quasi-free electron behaviour for D > 1, while in a 1D system the carrier state becomes polaronic at arbitrary small λ ("large" polaron). Previous exact diagonalization (ED) work has concentrated on the 1D case [8][9][10][11][12]21,[13][14][15][16][17], where, however, the calculations were limited to either very small clusters, rather weak EP coupling (λ < 1) or to the adiabatic limit (ω o = 0). On the other hand, the most interesting effects will be expected if the characteristic electronic and phononic energy scales are not well separated (λ ∼ 1; α ∼ 1).…”
Section: Introductionmentioning
confidence: 99%