Abstract

We consider the problem of testing multiple quantum hypotheses {ρ1⊗n,…,ρr⊗n}\{ρ_1^{\otimes n},\ldots,ρ_r^{\otimes n}\}, where an arbitrary prior distribution is given and each of the rr hypotheses is nn copies of a quantum state. It is known that the average error probability PeP_e decays exponentially to zero, that is, Pe=exp⁡{−ξn+o(n)}P_e=\exp\{-ξn+o(n)\}. However, this error exponent ξξ is generally unknown, except for the case that r=2r=2. In this paper, we solve the long-standing open problem of identifying the above error exponent, by proving Nussbaum and Szkoła's conjecture that ξ=min⁡i≠jC(ρi,ρj)ξ=\min_{i\neq j}C(ρ_i,ρ_j). The right-hand side of this equality is called the multiple quantum Chernoff distance, and C(ρi,ρj):=max⁡0≤s≤1{−log⁡Tr⁡ρisρj1−s}C(ρ_i,ρ_j):=\max_{0\leq s\leq 1}\{-\log\operatorname{Tr}ρ_i^sρ_j^{1-s}\} has been previously identified as the optimal error exponent for testing two hypotheses, ρi⊗nρ_i^{\otimes n} versus ρj⊗nρ_j^{\otimes n}. The main ingredient of our proof is a new upper bound for the average error probability, for testing an ensemble of finite-dimensional, but otherwise general, quantum states. This upper bound, up to a states-dependent factor, matches the multiple-state generalization of Nussbaum and Szkoła's lower bound. Specialized to the case r=2r=2, we give an alternative proof to the achievability of the binary-hypothesis Chernoff distance, which was originally proved by Audenaert et al.

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