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Physics Letters A

Quantum Zeno effect with neutron spin

Saverio Pascazio, Mikio Namiki, G. Badurek, Helmut Rauch

Published Aug 1, 1993• 72 citations
Publisher
DOI
10.1016/0375-9601(93)91131-n

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arXiv:quant-ph/0301068•Physical Review A•Jul 22, 2003•9 citations
The dynamics of a quantum system undergoing frequent ``measurements,'' leading to the so-called quantum Zeno effect, is examined on the basis of a neutron-spin experiment recently proposed for its demonstration. Unlike in all previous studies, the spatial degrees of freedom of the neutron are duly taken into account. Their inclusion in the analysis is important for two reasons: first, neutron-reflection effects are shown to be very important; second, the evolution may turn out to be totally different from the ideal case. Our results can be interpreted in terms of a rigorous theorem due to Misra and Sudarshan: indeed we clarify that, in contrast with a widespread belief, a quantum Zeno effect does not halt the evolution of a quantum system; it rather modifies it, by forcing the system to remain in a certain subspace, defined by the very measurement performed.
A neutron-spin experimental test of the quantum Zeno effect (QZE) is discussed from a practical point of view, where the nonideal efficiency of the magnetic mirrors, used for filtering the spin state, is taken into account. In the idealized case, the number N of (ideal) mirrors can be indefinitely increased, yielding an increasingly better QZE. In contrast, in a practical situation with imperfect mirrors, there is an optimal number of mirrors, Nopt,{N}_{\mathrm{opt}},Nopt​, at which the QZE becomes maximum: more frequent measurements would deteriorate the performance. However, a quantitative analysis shows that a good experimental test of the QZE is still feasible. These conclusions are of general validity: in a realistic experiment, the presence of losses and imperfections leads to an optimal frequency Nopt,{N}_{\mathrm{opt}},Nopt​, which is in general finite. One should not increase N beyond Nopt.{N}_{\mathrm{opt}}.Nopt​. A convenient formula for Nopt,{N}_{\mathrm{opt}},Nopt​, valid in a broad framework, is derived as a function of the parameters characterizing the experimental setup.