4.5 Article

Downfolding the Su-Schrieffer-Heeger model

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SCIPOST PHYSICS
卷 11, 期 4, 页码 -

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SCIPOST FOUNDATION
DOI: 10.21468/SciPostPhys.11.4.079

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  1. Deutsche Forschungsgemeinschaft (DFG) through the Research Training Group Quantum Mechanical Materials Modelling [RTG 2247]
  2. Central Research Development Fund of the University of Bremen
  3. Deutsche Forschungsgemeinschaft (DFG) through Germany's Excellence Strategy (University Allowance) [EXC 2077]

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Charge-density waves cause symmetry-breaking displacements of atoms and changes in electronic structure. Linear response theories offer a way to study these effects based on a single ab initio calculation. Downfolding approaches reduce the electronic system to a smaller number of bands, incorporating additional correlation and environmental effects, but the limitations of this approach are not always clear.
Charge-density waves are responsible for symmetry-breaking displacements of atoms and concomitant changes in the electronic structure. Linear response theories, in particular density-functional perturbation theory, provide a way to study the effect of displacements on both the total energy and the electronic structure based on a single ab initio calculation. In downfolding approaches, the electronic system is reduced to a smaller number of bands, allowing for the incorporation of additional correlation and environmental effects on these bands. However, the physical contents of this downfolded model and its potential limitations are not always obvious. Here, we study the potential-energy landscape and electronic structure of the Su-Schrieffer-Heeger (SSH) model, where all relevant quantities can be evaluated analytically. We compare the exact results at arbitrary displacement with diagrammatic perturbation theory both in the full model and in a downfolded effective single-band model, which gives an instructive insight into the properties of downfolding. An exact reconstruction of the potential-energy landscape is possible in a downfolded model, which requires a dynamical electron-biphonon inter-action. The dispersion of the bands upon atomic displacement is also found correctly, where the downfolded model by construction only captures spectral weight in the target space. In the SSH model, the electron-phonon coupling mechanism involves exclusively hybridization between the low- and high-energy bands and this limits the computational efficiency gain of downfolded models.

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