Ensemble Steering, Weak Self-Duality, and the Structure of Probabilistic Theories
In any probabilistic theory, we say that a bipartite state ω on a composite system AB steers its marginal state ω B if, for any decomposition of ω B as a mixture ω B =∑ i p i β i of states β i on B , there exists an observable { a i } on A such that the conditional states are exactly the states β i...
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Veröffentlicht in: | Foundations of physics 2013-12, Vol.43 (12), p.1411-1427 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | In any probabilistic theory, we say that a bipartite state
ω
on a composite system
AB
steers
its marginal state
ω
B
if, for any decomposition of
ω
B
as a mixture
ω
B
=∑
i
p
i
β
i
of states
β
i
on
B
, there exists an observable {
a
i
} on
A
such that the conditional states
are exactly the states
β
i
. This is always so for pure bipartite states in quantum mechanics, a fact first observed by Schrödinger in 1935. Here, we show that, for
weakly
self-dual state spaces (those isomorphic, but perhaps not canonically isomorphic, to their dual spaces), the assumption that every state of a system
A
is steered by some bipartite state of a composite
AA
consisting of two copies of
A
, amounts to the homogeneity of the state cone. If the state space is actually self-dual, and not just weakly so, this implies (via the Koecher-Vinberg Theorem) that it is the self-adjoint part of a formally real Jordan algebra, and hence, quite close to being quantum mechanical. |
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ISSN: | 0015-9018 1572-9516 |
DOI: | 10.1007/s10701-013-9752-2 |