Exact strong zero modes arise generically in integrable anisotropic spin models from quasi-periodicity of R-matrices and tracelessness of K-matrices, unifying known cases and predicting new ones.
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Symmetric superpositions of antipodal triplet states produce exact zero-energy eigenstates in non-integrable spin Hamiltonians that are scars with tunable entanglement from volume to area law.
A dissipative protocol with nonreciprocal auxiliary atoms stabilizes arbitrary correlated states across the many-body spectrum in Rydberg arrays.
Coherently synchronized oscillations appear in mirror-symmetric MBL systems and undergo a synchronization transition that maps to a paramagnetic-ferromagnetic Ising transition in an effective model built from local integrals of motion.
citing papers explorer
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Exact strong zero modes are generic in integrable spin systems with large anisotropy
Exact strong zero modes arise generically in integrable anisotropic spin models from quasi-periodicity of R-matrices and tracelessness of K-matrices, unifying known cases and predicting new ones.
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Symmetric tensor scars with tunable entanglement from volume to area law
Symmetric superpositions of antipodal triplet states produce exact zero-energy eigenstates in non-integrable spin Hamiltonians that are scars with tunable entanglement from volume to area law.
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Dissipative Preparation of Correlated Quantum States in Dipolar Rydberg Arrays
A dissipative protocol with nonreciprocal auxiliary atoms stabilizes arbitrary correlated states across the many-body spectrum in Rydberg arrays.
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Coherently synchronized oscillations in many-body localization
Coherently synchronized oscillations appear in mirror-symmetric MBL systems and undergo a synchronization transition that maps to a paramagnetic-ferromagnetic Ising transition in an effective model built from local integrals of motion.