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Large Classes of Quantum Scarred Hamiltonians from Matrix Product States

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arxiv 2002.11725 v2 pith:I2GJFYU6 submitted 2020-02-26 cond-mat.str-el cond-mat.stat-mechquant-ph

classification cond-mat.str-elcond-mat.stat-mechquant-ph
keywords exacthamiltoniansquantumakltchainderiveeigenstatesscars
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abstract

Motivated by the existence of exact many-body quantum scars in the AKLT chain, we explore the connection between Matrix Product State (MPS) wavefunctions and many-body quantum scarred Hamiltonians. We provide a method to systematically search for and construct parent Hamiltonians with towers of exact eigenstates composed of quasiparticles on top of an MPS wavefunction. These exact eigenstates have low entanglement in spite of being in the middle of the spectrum, thus violating the strong Eigenstate Thermalization Hypothesis (ETH). Using our approach, we recover the AKLT chain starting from the MPS of its ground state, and we derive the most general nearest-neighbor Hamiltonian that shares the AKLT quasiparticle tower of exact eigenstates. We further apply this formalism to other simple MPS wavefunctions, and derive new families of Hamiltonians that exhibit AKLT-like quantum scars. As a consequence, we also construct a scar-preserving deformation that connects the AKLT chain to the integrable spin-1 pure biquadratic model. Finally, we also derive other families of Hamiltonians that exhibit new types of exact quantum scars, including a $U(1)$-invariant perturbed Potts model.

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  1. The "not-A", RSPT and Potts phases in an $S_3$-invariant chain

    cond-mat.stat-mech 2019-08 accept novelty 8.0 of 10

    A two-parameter S3-invariant spin chain has four gapped phases, including a new 'not-A' phase and a representation symmetry-protected topological phase, with all transitions in the three-state Potts universality class.

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