Abstract

We study two-state discrimination in chaotic quantum systems. Assuming that one of two N-qubit pure states has been randomly selected, the probability to correctly identify the selected state from an optimally chosen experiment involving a subset of qubits is given by the trace-distance of the states, with N B qubits partially traced out. In the thermodynamic limit , the average subsystem trace-distance for random pure states makes a sharp, first order transition from unity to zero at , as the fraction of unmeasured qubits is increased. We analytically calculate the corresponding crossover for finite numbers N of qubits, study how it is affected by the presence of local conservation laws, and test our predictions against exact diagonalization of models for many-body chaos.

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