Ruskai–Audenaert decomposition conjecture for quantum channels

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Let P∈Herm⁡(Cd1⊗Cd2)P\in \operatorname{Herm}(\mathbb{C}^{d_1}\otimes \mathbb{C}^{d_2}) be the Choi matrix of a completely positive trace-preserving map T:Cd1×d1→Cd2×d2T:\mathbb{C}^{d_1\times d_1}\rightarrow \mathbb{C}^{d_2\times d_2}. There are n=d2n=d_2 positive operators PiP_i of rank at most r=d1r=d_1 such that

P=∑i=1nPiP=\sum_{i=1}^n P_i

and either tr2[Pi]∝\1{\rm tr}_2[P_i]\propto\1 for all ii, or tr2[Pi]=tr2[Pj]{\rm tr}_2[P_i]={\rm tr}_2[P_j] for all i,ji,j. Ruskai–Audenaert conjecture. Every quantum channel admits such a decomposition; the first alternative is the weak conjecture, while the second is the strong conjecture. The weak form is equivalent to a convex decomposition into d2d_2 generalized extreme points, and the strong form additionally requires equal weights, hence a barycentric decomposition. These are open equipartition and convex-decomposition problems for completely positive trace-preserving maps.

References

Primary source

Niranjan Kumar and Michael M. Wolf, “The Ruskai-Audenaert conjecture & equipartitions of positive operators”, arXiv:2607.23066 (2026).

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