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arXiv:math/0702544 · Proceedings - Mathematical Sciences

Extreme points of the convex set of joint probability distributions with fixed marginals

Kalyanapuram Rangachari Parthasarathy

Published Nov 1, 2007• 4 citations
arXivHTMLPDF
DOI
10.1007/s12044-007-0042-9

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Extremal Marginal States of Maximal Rank in (d,d+m)(d, d+m)(d,d+m)
We study the extreme points of the convex set C(ρ1,ρ2)\mathcal{C}(ρ_1,ρ_2)C(ρ1​,ρ2​) of bipartite quantum states with fixed marginals ρ1ρ_1ρ1​ and ρ2ρ_2ρ2​. We construct extreme points in (d, d+m)(d,\,d+m)(d,d+m) dimension, of rank d+md+md+m, matching the highest possible value, for all d≥3d\geq 3d≥3, m>d2−2d−22m > \frac{d^2-2d-2}{2}m>2d2−2d−2​ (when d=2d=2d=2, m≥1m\geq 1m≥1). This proves the existence of extremal states with relatively large rank and also covers all the known examples. We further show that, in order to analyze the extreme points of C(ρ1,ρ2)\mathcal{C}(ρ_1,ρ_2)C(ρ1​,ρ2​), it is sufficient to study the special case C(D1,D2)\mathcal{C}(\mathcal{D}_1,\mathcal{D}_2)C(D1​,D2​), where the marginals are diagonal. Additionally, we observe that it is sufficient to consider d1≤d2d_1\leq d_2d1​≤d2​. Thus, our results show that apart from possibly a few finite cases, for each d1d_1d1​, the maximal rank is achieved almost all times.
Many problems of quantum information theory rely on the set of quantum marginals. A precise knowledge of the faces of this convex set is necessary, for example, in the reconstruction of states from their marginals or in the evaluation of complexity measures of many-body systems. Yet, even the two-body marginals of just three qubits were only described in part. Here, we propose an experimental method to search for the coatoms in the lattice of exposed faces of the convex set of quantum marginals. The method is based on sampling from the extreme points of the dual spectrahedron. We provide an algebraic certificate of correctness, employing ground projectors of local Hamiltonians. Using this method, we present an explicit family of coatoms of rank five in the lattice of ground projectors of two-local three-qubit Hamiltonians (the rank is always six for bits). This family describes a family of coatoms in the lattice of exposed faces of the convex set of two-body marginals of three qubits. Besides introducing the experimental method, we show that the support sets of probability distributions that factor are the ground projectors of frustration-free Hamiltonians in the commutative setting. We also discuss nonexposed points of the set of marginals.
We will consider completely positive maps defined on tensor products of von Neumann algebras and taking values in the algebra of bounded operators on a Hilbert space and particularly certain convex subsets of the set of such maps. We show that when one of the marginal maps of such a map is an extreme point, then the marginals uniquely determine the map. We will further prove that when both of the marginals are extreme, then the whole map is extreme. We show that this general result is the common source of several well-known results dealing with, e.g., jointly measurable observables. We also obtain new insight especially in the realm of quantum instruments and their marginal observables and channels.