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Sharp quantum conditional-entropy continuity bound

6 years old · traced to

Let ρAB\rho_{AB} and σAB\sigma_{AB} be quantum states, let d=dim⁡A≥2d=\dim A\geq 2, and suppose that T(ρAB,σAB)≤δ≤1T(\rho_{AB},\sigma_{AB})\leq\delta\leq 1, where TT is the trace distance. Then

∣H(A∣B)ρ−H(A∣B)σ∣≤{h2(δ)+δlog⁡(d2−1),0≤δ≤1−d−2,2log⁡d,1−d−2≤δ≤1.\left\lvert H(A|B)_{\rho}-H(A|B)_{\sigma}\right\rvert\leq \begin{cases} h_{2}(\delta)+\delta\log(d^{2}-1),&0\leq\delta\leq 1-d^{-2},\\ 2\log d,&1-d^{-2}\leq\delta\leq 1. \end{cases}

If dim⁡B≥d\dim B\geq d, the right-hand side is optimal for every δ∈[0,1]\delta\in[0,1].

References

Progress summary

Refreshed
Open · solution reported

A July 2026 paper proves the best possible dimension-only continuity bound for quantum conditional entropy, settling the unrestricted case.

The problem asks for the optimal uniform bound on changes in H(A∣B)H(A|B) controlled by trace distance and d=dim⁡Ad=\dim A. The unrestricted fully quantum case had remained open after classical, quantum-classical, and equal-BB-marginal cases were settled.

Known results

  • Alicki and Fannes established an earlier dimension-dependent continuity estimate; Winter strengthened it.
  • Alhejji and Smith determined the sharp classical modulus in 2020.
  • Wilde proved the quantum-classical result and conjectured the fully quantum expression.
  • Berta, Lami, and Tomamichel, and independently Audenaert, Datta, Jabbour, Capel, and Gondolf, proved the equal-BB-marginal case.

July 2026 sharp-bound theorem

Theorem 1.1 gives, for T(ρAB,σAB)≤δT(\rho_{AB},\sigma_{AB})\leq\delta and d=dim⁡A≥2d=\dim A\geq2, the optimal bound h2(δ)+δlog⁡(d2−1)h_2(\delta)+\delta\log(d^2-1) up to δ=1−d−2\delta=1-d^{-2}, followed by 2log⁡d2\log d. It is attained for every δ∈[0,1]\delta\in[0,1] when dim⁡B≥d\dim B\geq d, via maximally entangled/Weyl-sector examples. The proof idea was developed with assistance from ChatGPT 5.6 Sol.

Current status (as of July 2026): the unrestricted sharp bound and its optimality are settled by the arXiv theorem; no part of the stated problem remains open.

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