Abstract
Measurement and fluctuations are closely related to each other in quantum mechanics. This fact is explicitly demonstrated in the case of a quantum non-demolition photodetector which is composed of a double quantum-wire electron interferometer.
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Reference [18] assumed that the coherence length in reservoirs, ℓ res c , is short, whereas Refs. [16] assumed that ℓ res c is long (which was implicitly assumed by assuming the perfect Fermi distribution in reservoirs.) The noise formula in the general case, which interpolates between the two limiting cases, was given in Eq. (21) of Ref. [17], which shows that finite ℓ res c induces an “emission noise” in addition to the “granularity noise” derived in [16]. However, conserning the fundamental limits of quantum interference devices, which were derived in [18], the limits depend only on the granularity noise, hence apply to any case irrespective of the length of ℓ res c . To break the limits, one must resort to well-designed many-body correlations among electrons, as discussed in [13].
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Shimizu, A. (1994). Quantum Measurement and Fluctuations in Nanostructures. In: Nanostructures and Quantum Effects. Springer Series in Materials Science , vol 31. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-79232-8_5
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DOI: https://doi.org/10.1007/978-3-642-79232-8_5
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