Summary
This paper employs neural quantum states, in particular hidden fermion determinant states (HFDS), to perform a scalable variational study of the three-band Emery model for CuO2/NiO2 planes in cuprates and nickelates. The authors first benchmark against matrix product states on width-two geometries and then simulate fully two-dimensional systems up to 10×10 unit cells (300 sites), characterizing the momentum-space distribution of dopants and finding an electron-hole dichotomy similar to that observed in cuprate experiments. The study further downfolds the three-band model to an effective single-band description by constructing interacting Wannier functions, with parameters covering the cuprate charge-transfer regime, the nickelate Hubbard-Mott regime, and scans of the charge-transfer gap. The results show that the effective model deviates significantly from the usual Fermi-Hubbard model: U/t is enhanced, some parameters exhibit pronounced doping dependence, and important terms beyond the conventional Hubbard model emerge, most notably the density-assisted hopping tn; moreover, tn makes the largest contribution to particle-hole asymmetry, rather than next-nearest-neighbor hopping. The effective parameters depend sensitively on the charge-transfer energy, doping, and interaction ratio. The conclusion is that HFDS is an efficient tool for studying the two-dimensional Emery model, and that a single-band description may need to include new interaction terms generated by the underlying multiband model.
Materials
- cuprates
- infinite-layer nickelates
- copper-oxide layers
- nickel-oxide layers
- CuO2 planes
Methods
- Neural quantum states (NQS)
- Hidden Fermion Determinant States (HFDS)
- Matrix product states (MPS)
- Density-matrix renormalization group (DMRG)
- Convolutional neural networks (CNNs)
- Interacting Wannier functions
- Downfolding
- Variational optimization
- Symmetry-averaging
Keywords
- high temperature superconductivity
- three band emery model
- single band fermi hubbard model
- electron hole asymmetry
- nodal antinodal dichotomy
- charge transfer gap
- density assisted hopping
- particle hole asymmetry
- charge transfer regime
- hubbard mott regime
- superconducting critical temperature
- zhang rice singlets
- momentum space distribution of dopants
- fermi arc
Highlights
- To our knowledge, this is the first time that NQS are employed for a three-band study.
- Despite the apparent increase in complexity, the number of simulated fermions is not increased by a factor of three; instead, the dimension of the determinant remains of the same order as in single-band models, rendering its evaluation computationally comparable to that of the corresponding single-band ansätze.
- Our NQS provide competitive energies with a substantially smaller number of variational parameters while extending naturally to geometries beyond the quasi-one-dimensional regime.
- The data for different system sizes are nearly indistinguishable, indicating that finite-size effects are small.
- Including Vpd in the downfolding significantly enhances tn and moreover generates additional equal-spin density terms that are not present for Vpd=0.
- The electron-hole asymmetry is captured by tn, rather than by assigning different signs to t'.
- This procedure follows Ref. [32], but we extend the analysis to systematic Emery parameter and doping scans.
Conclusions
- HFDS provide an efficient variational description of the copper- and nickel-oxide layers of cuprate and nickelate superconductors that goes beyond the usually considered single-band Fermi-Hubbard model: the three-band Emery model.
- The favorable scaling of HFDS enables accurate calculations on square lattices of up to 10×10 unit cells, establishing NQS as a practical route to studying the ground state of the Emery model on large two-dimensional systems.
- The simulations reveal a clear asymmetry between electron and hole doping in momentum space, which is qualitatively consistent with ARPES experiments in cuprates.
- The systematic downfolding of the correlated three-band ground state to an effective single-band description finds sizable contributions beyond the bare Fermi-Hubbard model.
- The effective model significantly deviates from the usual Fermi-Hubbard model: the typical ratio U/t is enhanced, some parameters experience a significant doping dependence, and sizable terms beyond the conventional Hubbard model are present, most notably a density-assisted hopping tn.
- In all effective models, tn has the largest contribution to particle-hole asymmetry, rather than next-nearest-neighbor hopping contributions.
- The effective parameters sensitively depend on the charge-transfer energy, doping, and interaction ratios.
- The charge-transfer energy has a particularly strong impact on the spatial extent of the interacting Wannier orbitals and, consequently, on the effective hopping and interaction strengths.
- Single-band descriptions can require interaction terms generated by the underlying multi-band models.
Main claims
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Workflow
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