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arXiv:0906.2000 · Physical Review A

Local and global statistical distances are equivalent on pure states

Scott M. Cohen

Published Sep 22, 2009• 0 citations
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Abstract

The statistical distance between pure quantum states is obtained by finding a measurement that is optimal in a sense defined by Wootters. As such, one may expect that the statistical distance will turn out to be different if the set of possible measurements is restricted in some way. It nonetheless turns out that if the restriction is to local operations and classical communication on any multipartite system, then the statistical distance is the same as it is without restriction, being equal to the angle between the states in Hilbert space.

DOI
10.1103/physreva.80.032323

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The statistical distance between pure quantum states is obtained by finding a measurement that is optimal in a sense defined by Wootters. As such, one may expect that the statistical distance will turn out to be different if the set of possible measurements is restricted in some way. It nonetheless turns out that if the restriction is to local operations and classical communication on any multipartite system, then the statistical distance is the same as it is without restriction, being equal to the angle between the states in Hilbert space.
We consider an infinite class of unambiguous quantum state discrimination problems on multipartite systems, described by Hilbert space H\mathcal{H}H, of any number of parties. Restricting consideration to measurements that act only on H\mathcal{H}H, we find the optimal global measurement for each element of this class, achieving the maximum possible success probability of 1/21/21/2 in all cases. This measurement turns out to be both separable and unique, and by our recently discovered necessary condition for local quantum operations and classical communication (LOCC) it is easily shown to be impossible by any finite-round LOCC protocol. We also show that, quite generally, if the input state is restricted to lie in H\mathcal{H}H, then any LOCC measurement on an enlarged Hilbert space is effectively identical to an LOCC measurement on H\mathcal{H}H. Therefore, our necessary condition for LOCC demonstrates directly that a higher success probability is attainable for each of these problems using general separable measurements as compared to that which is possible with any finite-round LOCC protocol.
We study measures of quantum information when the space spanned by the set of accessible observables is not closed under products, i.e., we consider systems where an observer may be able to measure the expectation values of two operators, ⟨O1⟩⟨{O}_{1}⟩⟨O1​⟩ and ⟨O2⟩⟨{O}_{2}⟩⟨O2​⟩, but may not have access to ⟨O1O2⟩⟨{O}_{1}{O}_{2}⟩⟨O1​O2​⟩. This problem is relevant for the study of localized quantum information in gravity since the set of approximately local operators in a region may not be closed under arbitrary products. While we cannot naturally associate a density matrix with a state in this setting, it is still possible to define a modular operator for a state, and distinguish between two states using a relative modular operator. These operators are defined on a ``little Hilbert space,'' which parametrizes small deformations of the system away from its original state, and they do not depend on the structure of the full Hilbert space of the theory. We extract a class of relative-entropy-like quantities from the spectrum of these operators that measure the distance between states, are monotonic under contractions of the set of available observables, and vanish only when the states are equal. Consequently, these distance measures can be used to define measures of bipartite and multipartite entanglement. We describe applications of our measures to ``coarse-grained'' and ``fine-grained'' subregion dualities in AdS/CFT\mathrm{AdS}/\mathrm{CFT}AdS/CFT and provide a few sample calculations to illustrate our formalism.
The restricted numerical range W R ( A ) of an operator A acting on a D -dimensional Hilbert space is defined as a set of all possible expectation values of this operator among pure states which belong to a certain subset R of the set of pure quantum states of dimension D . One considers for instance the set of real states, or in the case of composite spaces, the set of product states and the set of maximally entangled states. Combining the operator theory with a probabilistic approach we introduce the restricted numerical shadow of A —a normalized probability distribution on the complex plane supported in W R ( A ). Its value at point is equal to the probability that the expectation value 〈ψ| A |ψ〉 is equal to z , where |ψ〉 represents a random quantum state in subset R distributed according to the natural measure on this set, induced by the unitarily invariant Fubini–Study measure. Studying restricted shadows of operators of a fixed size D = N A N B we analyse the geometry of sets of separable and maximally entangled states of the N A × N B composite quantum system. Investigating trajectories formed by evolving quantum states projected into the plane of the shadow, we study the dynamics of quantum entanglement. A similar analysis extended for operators on D = 2 3 -dimensional Hilbert space allows us to investigate the structure of the orbits of GHZ and W quantum states of a three-qubit system.