pith. sign in

(S.67) to vanish, which then yields A1 → √π 4 ⇒f 1(x) = π 2 e−x2 .(S.68) We thus obtain the universal coefficient as expected

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Universal dynamics from a single-particle dark state

cond-mat.quant-gas · 2026-05-15 · unverdicted · novelty 7.0

A single-particle dark state in a dissipating spin chain induces universal long-time many-body dynamics with momentum distribution scaling as k sqrt(t) and density decaying as 1/(sqrt(t) log t).

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  • Universal dynamics from a single-particle dark state cond-mat.quant-gas · 2026-05-15 · unverdicted · none · ref 66

    A single-particle dark state in a dissipating spin chain induces universal long-time many-body dynamics with momentum distribution scaling as k sqrt(t) and density decaying as 1/(sqrt(t) log t).