Recent progress in matter-wave interferometry aims to directly probe the quantum properties of matter on ever increasing scales. However, in order to perform interferometric experiments with massive mesoscopic objects, taking into account the constraints on the experimental setups, the pointlike-particle approximation needs to be cast aside. In this work, we consider near-field interferometry based on the Talbot effects with a single optical grating for large spherical particles beyond the point-particle approximation. We account for the suppression of the coherent grating effect and, at the same time, the enhancement of the decoherence effects due to scattering and absorption of grating photons.

Belenchia A., Gasbarri G., Kaltenbaek R., Ulbricht H., Paternostro M. (2019). Talbot-Lau effect beyond the point-particle approximation. PHYSICAL REVIEW A, 100(3) [10.1103/PhysRevA.100.033813].

Talbot-Lau effect beyond the point-particle approximation

Paternostro M.
Ultimo
Conceptualization
2019-09-11

Abstract

Recent progress in matter-wave interferometry aims to directly probe the quantum properties of matter on ever increasing scales. However, in order to perform interferometric experiments with massive mesoscopic objects, taking into account the constraints on the experimental setups, the pointlike-particle approximation needs to be cast aside. In this work, we consider near-field interferometry based on the Talbot effects with a single optical grating for large spherical particles beyond the point-particle approximation. We account for the suppression of the coherent grating effect and, at the same time, the enhancement of the decoherence effects due to scattering and absorption of grating photons.
11-set-2019
Belenchia A., Gasbarri G., Kaltenbaek R., Ulbricht H., Paternostro M. (2019). Talbot-Lau effect beyond the point-particle approximation. PHYSICAL REVIEW A, 100(3) [10.1103/PhysRevA.100.033813].
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/10447/629294
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