Choos- ingt≥Γ −1 log(1/ϵ) implies that etL(ρ0)− T EPU 1 ≤ ϵ

Then, we show in Appendix E that etL(ρ0)− T EPU 1 ≤e −tΓ ||∆ρ0||1 ≤2e −tΓ,(18) where Γ := min E{γE, λE}and||∆ρ 0||1 ≤2 · 2024

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quant-ph · 2026-04-10 · unverdicted · novelty 6.0

Invariance under energy-preserving unitaries forces large-N reduced states to be close to thermal mixtures, with vanishing error bounds.

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Symmetry-driven thermalization via finite de Finetti theorems quant-ph · 2026-04-10 · unverdicted · none · ref 1
Invariance under energy-preserving unitaries forces large-N reduced states to be close to thermal mixtures, with vanishing error bounds.