A graph-theoretic method systematically constructs quantum many-body scars in frustrated Rydberg lattices via type-I and type-II mechanisms, with numerical demonstration of an exponential family of scarred trajectories on the hexagonal lattice.
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A flow equation for the resonance density exponent θ(w) derived in the SJA predicts resonance proliferation driving delocalization, with θ(w)>0 for localized phases and instability signaling thermalization, matching numerics in Anderson and MBL models.
A protocol using emergent Hamiltonians enables storage of Bell-product and GHZ entangled states by making them exact eigenstates of a local Hamiltonian.
In the long-range Haldane-Shastry model, pristine Poisson level statistics emerge only with combined position disorder and random magnetic fields, with an approximate scaling collapse governed by the product αδ when SU(2) symmetry is broken.
Kibble-Zurek defect scaling does not generally correspond to quantum criticality in representative quasi-1D Fermi models.
citing papers explorer
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Systematic construction of quantum many-body scars in frustrated Rydberg arrays
A graph-theoretic method systematically constructs quantum many-body scars in frustrated Rydberg lattices via type-I and type-II mechanisms, with numerical demonstration of an exponential family of scarred trajectories on the hexagonal lattice.
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Resonance Proliferation Across Localization Transitions
A flow equation for the resonance density exponent θ(w) derived in the SJA predicts resonance proliferation driving delocalization, with θ(w)>0 for localized phases and instability signaling thermalization, matching numerics in Anderson and MBL models.
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From Bell Products to Greenberger-Horne-Zeilinger states: Quantum Memories via emergent Hamiltonians
A protocol using emergent Hamiltonians enables storage of Bell-product and GHZ entangled states by making them exact eigenstates of a local Hamiltonian.
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Level statistics of the disordered Haldane-Shastry model with $1/r^\alpha$ interaction
In the long-range Haldane-Shastry model, pristine Poisson level statistics emerge only with combined position disorder and random magnetic fields, with an approximate scaling collapse governed by the product αδ when SU(2) symmetry is broken.
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Separation of the Kibble-Zurek Mechanism from Quantum Criticality
Kibble-Zurek defect scaling does not generally correspond to quantum criticality in representative quasi-1D Fermi models.