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Quantum U-statistics

Abstract

The notion of a UU-statistic for an nn-tuple of identical quantum systems is introduced in analogy to the classical (commutative) case: given a selfadjoint `kernel' KK acting on (Cd)r(\mathbb{C}^{d})^{\otimes r} with r<nr<n, we define the symmetric operator Un=(nr)βK(β)U_{n}= {n \choose r} \sum_{\beta}K^{(\beta)} with K(β)K^{(\beta)} being the kernel acting on the subset β\beta of {1,,n}\{1,\dots ,n\}. If the systems are prepared in the i.i.d state ρn\rho^{\otimes n} it is shown that the sequence of properly normalised UU-statistics converges in moments to a linear combination of Hermite polynomials in canonical variables of a CCR algebra defined through the Quantum Central Limit Theorem. In the special cases of non-degenerate kernels and kernels of order 22 it is shown that the convergence holds in the stronger distribution sense. Two types of applications in quantum statistics are described: testing beyond the two simple hypotheses scenario, and quantum metrology with interacting hamiltonians.Comment: 30 pages, added section on quantum metrolog

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