Only the time-independent part ofpsurvives, p(k,∞) =e −iθk cos(∆θk), whileq(k,∞) = 0

Stationary state via dephasing At long timest→ ∞, the oscillating termscos(2ε kt) andsin(2ε kt)inp(k, t)andq(k, t)average to zero due to dephasing across modes with different group

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Non-Local Magic Resources for Fermionic Gaussian States

quant-ph · 2026-04-29 · unverdicted · novelty 6.0

Closed-form formula computes non-local magic for fermionic Gaussian states from two-point correlations in polynomial time.

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Non-Local Magic Resources for Fermionic Gaussian States quant-ph · 2026-04-29 · unverdicted · none · ref 2
Closed-form formula computes non-local magic for fermionic Gaussian states from two-point correlations in polynomial time.

Only the time-independent part ofpsurvives, p(k,∞) =e −iθk cos(∆θk), whileq(k,∞) = 0

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