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For the ferromagnetic model, the quasisymmetry is SO(3), generated by usual spin gener- ators: ˆq± = ˆs±, ˆqz = ˆsz

Energy dispersion, variance In the following, we always consider the degenerate limit by setting h = 0

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Quasi-Nambu-Goldstone modes in many-body scar models

cond-mat.str-el · 2024-05-01 · unverdicted · novelty 7.0

Quasi-Nambu-Goldstone modes exist universally in many-body scar models in the degenerate limit, with properties determined by the quasisymmetry of the scar tower.

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  • Quasi-Nambu-Goldstone modes in many-body scar models cond-mat.str-el · 2024-05-01 · unverdicted · none · ref 6

    Quasi-Nambu-Goldstone modes exist universally in many-body scar models in the degenerate limit, with properties determined by the quasisymmetry of the scar tower.