Spin alignment conjecture for entropy minimization

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Let nn be a positive integer, let σ\sigma be a density operator, and let McM^c denote the complement of MM in {1,2,⋯ ,n}\{1,2,\cdots,n\}. For a subset MM, write σ⊗Mc\sigma^{\otimes M^c} for the tensor product of copies of σ\sigma on the tensor factors indexed by McM^c, and similarly interpret ∣ek0⟩⟨ek0∣⊗M\lvert e_{k_0}\rangle\langle e_{k_0}\rvert^{\otimes M}. Let {xM}M⊆{1,2,⋯ ,n}\{x_M\}_{M\subseteq \{1,2,\cdots,n\}} be a fixed probability distribution, and let ∣ek0⟩\lvert e_{k_0}\rangle be an eigenvector corresponding to the maximal eigenvalue of σ\sigma. Spin alignment conjecture. The entropy minimization problem in the stated spin-alignment setting is achieved at the state

κ=∑M⊆{1,2,⋯ ,n}xM∣ek0⟩⟨ek0∣⊗M⊗σ⊗Mc.\kappa=\sum_{M\subseteq \{1,2,\cdots,n\}}x_M\lvert e_{k_0}\rangle\langle e_{k_0}\rvert^{\otimes M}\otimes\sigma^{\otimes M^c}.

This conjecture identifies the entropy-minimizing state by aligning every tensor factor indexed by MM with a maximal-eigenvalue eigenvector of σ\sigma, while retaining σ\sigma on the complementary factors. Its resolution is not established by the supplied material.

References

Primary source

Peixue Wu and Yunkai Wang, “Quantum capacity amplification via privacy”, arXiv:2510.04527 (2025).

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