SciPost Phys. 15, 081 (2023) ·
published 6 September 2023
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We derive BM-like continuum models for the bands of superlattice heterostructures formed out of Fe-chalcogenide monolayers: (I) a single monolayer experiencing an external periodic potential, and (II) twisted bilayers with long-range moire tunneling. A symmetry derivation for the inter-layer moire tunnelling is provided for both the $\Gamma$ and $M$ high-symmetry points. In this paper, we focus on moire bands formed from hole-band maxima centered on $\Gamma$, and show the possibility of moire bands with $C=0$ or ±1 topological quantum numbers without breaking time-reversal symmetry. In the $C=0$ region for $\theta→0$ (and similarly in the limit of large superlattice period for I), the system becomes a square lattice of 2D harmonic oscillators. We fit our model to FeSe and argue that it is a viable platform for the simulation of the square Hubbard model with tunable interaction strength.
SciPost Phys. 3, 043 (2017) ·
published 26 December 2017
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We compute exactly the von Neumann entanglement entropy of the eta-pairing
states - a large set of exact excited eigenstates of the Hubbard Hamiltonian.
For the singlet eta-pairing states the entropy scales with the logarithm of the
spatial dimension of the (smaller) partition. For the eta-pairing states with
finite spin magnetization density, the leading term can scale as the volume or
as the area-times-log, depending on the momentum space occupation of the
Fermions with flipped spins. We also compute the corrections to the leading
scaling. In order to study the eigenstate thermalization hypothesis (ETH), we
also compute the entanglement Renyi entropies of such states and compare them
with the corresponding entropies of thermal density matrix in various
ensembles. Such states, which we find violate strong ETH, may provide a useful
platform for a detailed study of the time-dependence of the onset of
thermalization due to perturbations which violate the total pseudospin
conservation.
