Partial majorization and Schur concave functions on the sets of quantum and classical states

M. E. Shirokov

#2250 of 2593 · Quantum Physics
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1298±39
10501750
28%
Win Rate
9
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23
Losses
32
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Rating
5.8/ 10
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Abstract

We construct for a Schur concave function ff on the set of quantum states a tight upper bound on the difference f(ρ)f(σ)f(ρ)-f(σ) for a quantum state ρρ with finite f(ρ)f(ρ) and any quantum state σσ mm-partially majorized by the state ρρ in the sense described in [1]. We also obtain a tight upper bound on this difference under the additional condition 12ρσ1ε\frac{1}{2}\|ρ-σ\|_1\leq\varepsilon and find simple sufficient conditions for vanishing this bound with min{ε,1/m}0\,\min\{\varepsilon,1/m\}\to0\,. The obtained results are applied to the von Neumann entropy. The concept of ε\varepsilon-sufficient majorization rank of a quantum state with finite entropy is introduced and a tight upper bound on this quantity is derived and applied to the Gibbs states of a quantum oscillator. We also show how the obtained results can be reformulated for Schur concave functions on the set of probability distributions with a finite or countable set of outcomes.

AI Impact Assessments

(3 models)

Scientific Impact Assessment

Core Contribution

This paper develops a general framework for bounding the difference f(ρ)f(σ)f(\rho) - f(\sigma) for Schur concave functions ff when a quantum state σ\sigma is only *partially* majorized by ρ\rho (i.e., the majorization inequalities hold only for the first mm partial sums of eigenvalues). The central result (Theorem 1) provides a tight upper bound on this difference, parameterized by both the partial majorization rank mm and the trace-norm distance ε\varepsilon between the states. The paper introduces the state transformation ρρm,ε\rho \mapsto \rho_{m,\varepsilon}, which serves as an extremal state achieving the bound, and proves that ρm,ε\rho_{m,\varepsilon} majorizes all states in the intersection of the mm-partial majorization set and the ε\varepsilon-ball around ρ\rho.

The key conceptual advance is bridging partial majorization (a finitely verifiable condition) with full majorization-based inequalities (which require infinitely many checks for infinite-rank states), quantifying exactly how much Schur concavity can be "violated" under partial majorization.

Methodological Rigor

The mathematical approach is rigorous and well-structured. The proof strategy proceeds in clear stages:

1. Lemma 1 establishes that for any state σ\sigma that is mm-partially majorized by ρ\rho, there exists an auxiliary state σ\sigma^* in a structured set Tm(ρ)T_m(\rho) that majorizes σ\sigma while being no farther from ρ\rho in trace norm. This leverages prior results (Lemmas 2A and 2B from [1]) combined with the Mirsky inequality.

2. Lemma 2 shows the constructed extremal state ρm,ε\rho_{m,\varepsilon} majorizes all states in Tm(ρ)Uε(ρ)T_m(\rho) \cap U_\varepsilon(\rho), completing the optimization.

3. Theorem 1 combines these to yield the tight bound, with explicit sufficient conditions for convergence to zero.

The tightness of the bounds is demonstrated by constructing explicit states achieving equality, which is a strong methodological feature. The three-case definition of ρm,ε\rho_{m,\varepsilon} (equations 16–18) covers all regimes cleanly, though the piecewise construction adds complexity. The paper carefully handles both finite and infinite rank cases throughout.

One minor concern is that some arguments rely on constructions from [1] (particularly Lemmas 2A and 2B), making this paper somewhat dependent on the companion paper. However, the logical chain is self-contained enough for verification.

Potential Impact

Quantum information theory: The results apply broadly to any Schur concave (or convex) function, covering von Neumann, Rényi, and Tsallis entropies. The explicit bounds for the Rényi entropy (Example 1) and von Neumann entropy (Section 5) are directly useful. The concept of ε\varepsilon-sufficient majorization rank (Section 5.2) is a novel and potentially useful characteristic of quantum states, quantifying how quickly the spectrum decays. The application to Gibbs states of a quantum oscillator provides concrete, physically meaningful estimates.

Classical probability theory: Section 6 translates all results to probability distributions with finite or countable outcomes, broadening applicability to classical information theory, statistics, and analysis of discrete random variables.

Continuity bounds: The framework generalizes and extends the continuity bound methodology of Hanson-Datta [13], providing tools that could be applied to other optimization problems involving majorization constraints.

The practical significance lies in situations where verifying full majorization is infeasible (infinite-rank states) but partial majorization can be checked. This is a realistic scenario in quantum information processing with infinite-dimensional systems (e.g., bosonic channels, continuous-variable quantum information).

Timeliness & Relevance

The paper addresses a genuine gap in the theory of majorization for infinite-dimensional quantum systems. While majorization theory is classical and well-developed for finite dimensions, infinite-dimensional extensions remain an active area. The paper builds directly on the author's recent companion work [1] (arXiv:2504.08098), suggesting this is part of an active and evolving research program. Continuity bounds for entropic quantities in infinite dimensions have been an important topic in quantum information theory, with practical implications for channel capacities and entanglement measures.

Strengths

1. Universality: The technique applies to any Schur concave function, not just the von Neumann entropy, making it a broadly applicable tool.

2. Tightness: All major bounds are proven to be optimal, with explicit constructions achieving equality.

3. Clean sufficient conditions: The conditions for convergence (lower semicontinuity of ff, which holds for standard entropies) are simple and easily verified.

4. Concrete applications: The worked examples (Rényi entropy, Gibbs states of quantum oscillator) demonstrate practical usability. The plots in Figures 1–3 provide useful visual intuition.

5. Dual formulation: Theorem 2 provides the complementary infimum version without requiring finiteness of f(ρ)f(\rho).

Limitations

1. Incremental nature: This work extends [1] and generalizes [13], and while the generalization is substantial, the core technical ideas (Mirsky inequality, spectral rearrangement arguments) are not fundamentally new.

2. Limited physical applications: The paper remains largely in the mathematical framework. Connections to specific quantum information protocols (e.g., entanglement distillation, channel coding) where partial majorization naturally arises are not explored.

3. Accessibility: The three-case definition of ρm,ε\rho_{m,\varepsilon} and the associated notation are somewhat heavy, which may limit adoption.

4. Dependence on companion paper: Key lemmas from [1] are invoked without reproduction, requiring readers to consult both papers.

5. No computational complexity analysis: For practical applications, understanding the computational cost of evaluating the bounds would be valuable.

Overall Assessment

This is a technically solid paper that provides a useful generalization of majorization-based inequalities for Schur concave functions. The results are tight, general, and cleanly presented. The impact is primarily within mathematical quantum information theory and majorization theory, with potential applications in infinite-dimensional quantum systems. While not groundbreaking in terms of new conceptual insights, it fills a meaningful theoretical gap with rigorous and optimal results.

Rating:5.8/ 10
Significance 5.5Rigor 8.5Novelty 5Clarity 7

Generated Apr 15, 2026

Comparison History (32)

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