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Eta-Pairing in Hubbard Models: From Spectrum Generating Algebras to Quantum Many-Body Scars

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arxiv 2004.13727 v2 pith:BOHI7RHX submitted 2020-04-28 cond-mat.str-el cond-mat.stat-mechquant-ph

Eta-Pairing in Hubbard Models: From Spectrum Generating Algebras to Quantum Many-Body Scars

classification cond-mat.str-el cond-mat.stat-mechquant-ph
keywords modelsscarsspectrumquantumeigenstatesequallygeneratingmany-body
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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abstract

We revisit the $\eta$-pairing states in Hubbard models and explore their connections to quantum many-body scars to discover a universal scars mechanism. $\eta$-pairing occurs due to an algebraic structure known as a Spectrum Generating Algebra (SGA), giving rise to equally spaced towers of eigenstates in the spectrum. We generalize the original $\eta$-pairing construction and show that several Hubbard-like models on arbitrary graphs exhibit SGAs, including ones with disorder and spin-orbit coupling. We further define a Restricted Spectrum Generating Algebra (RSGA) and give examples of perturbations to the Hubbard-like models that preserve an equally spaced tower of the original model as eigenstates. The states of the surviving tower exhibit a sub-thermal entanglement entropy, and we analytically obtain parameter regimes for which they lie in the bulk of the spectrum, showing that they are exact quantum many-body scars. The RSGA framework also explains the equally spaced towers of eigenstates in several well-known models of quantum scars, including the AKLT model.

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  1. The $S=\frac{1}{2}$ XY and XYZ models on the two or higher dimensional hypercubic lattice do not possess nontrivial local conserved quantities

    cond-mat.stat-mech 2024-12 unverdicted novelty 6.0

    The S=1/2 XY and XYZ models on d≥2 hypercubic lattices possess no nontrivial local conserved quantities.