Adding XX interactions to a non-Hermitian Floquet Ising chain shifts its time-crystal phase boundaries and, above K_c ≈ 0.085, stabilizes a new x-ferromagnetic phase at R=1.
Similarly, for the NFM2 phase, C(y) ∼ y−α 2 cos (a2y)
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Effects of non-integrability in a non-Hermitian time crystal
Adding XX interactions to a non-Hermitian Floquet Ising chain shifts its time-crystal phase boundaries and, above K_c ≈ 0.085, stabilizes a new x-ferromagnetic phase at R=1.