pith. sign in

( B.1), b3 = −ie iπ 2ω (F + G) so that the saddles occur at x∗ 3 ∝ ei(2m+1)π(ω+1)e− iπ(ω+1) 2ω and Eq

= eiΘ1cτ ω + 1 cτ ω (ω + 1)2 sin( π 2ω )G ω (B

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Kink-kink correlations in nonlinear quenches across a quantum critical point

cond-mat.stat-mech · 2026-05-06 · accept · novelty 5.0

For algebraic quenches in the 1D TFIM, the longitudinal kink-kink correlator depends only on the KZ length for superlinear cases and otherwise needs a dephasing length, decaying as a compressed exponential with exponent varying continuously with the quench exponent.

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  • Kink-kink correlations in nonlinear quenches across a quantum critical point cond-mat.stat-mech · 2026-05-06 · accept · none · ref 3

    For algebraic quenches in the 1D TFIM, the longitudinal kink-kink correlator depends only on the KZ length for superlinear cases and otherwise needs a dephasing length, decaying as a compressed exponential with exponent varying continuously with the quench exponent.