An error-cancellation matrix-product ansatz constructs exact zero-energy many-body scar eigenstates in non-frustration-free 1D and 2D spin Hamiltonians.
Title resolution pending
4 Pith papers cite this work. Polarity classification is still indexing.
citation-role summary
citation-polarity summary
roles
background 1polarities
unclear 1representative citing papers
Granovskii-Zhedanov scar states in XYZ models are described via spectrum-generating algebra with perturbative and optimized constructions, and lattice-independent versions exist only on specific uniform and non-uniform higher-dimensional lattices.
Non-Hermitian spin relaxation stabilizes Granovskii-Zhedanov scar states in the perturbed XYZ chain, producing a nonequilibrium steady state with finite fidelity to the scar.
Transverse spin helices in XXZ chains with single-ion anisotropy decay slowly for chosen wave numbers and can be stabilized by easy-axis exchange anisotropy, per iTEBD simulations and spin-wave estimates.
citing papers explorer
-
Exact Quantum Many-Body Scars by a generalized Matrix-Product Ansatz
An error-cancellation matrix-product ansatz constructs exact zero-energy many-body scar eigenstates in non-frustration-free 1D and 2D spin Hamiltonians.
-
Granovskii-Zhedanov Scars of XYZ Models: Modern Algebraic Perspectives and Realization in Higher Dimensional Lattices
Granovskii-Zhedanov scar states in XYZ models are described via spectrum-generating algebra with perturbative and optimized constructions, and lattice-independent versions exist only on specific uniform and non-uniform higher-dimensional lattices.
-
Stabilization of Granovskii-Zhedanov scars of the XYZ quantum spin chain via non-Hermitian spin relaxation
Non-Hermitian spin relaxation stabilizes Granovskii-Zhedanov scar states in the perturbed XYZ chain, producing a nonequilibrium steady state with finite fidelity to the scar.
-
Decay of spin helices in XXZ quantum spin chains with single-ion anisotropy
Transverse spin helices in XXZ chains with single-ion anisotropy decay slowly for chosen wave numbers and can be stabilized by easy-axis exchange anisotropy, per iTEBD simulations and spin-wave estimates.