SearcharxivSearch

arXiv subjects

Lepsa Vuskovic

Publications and source records attributed to Lepsa Vuskovic.

2 recordsLinked to original sources

An asymmetric double-slit interferometer for small and large quantum particles

Quantum theory of interference phenomena does not take the diameter of the particle into account, since particles were much smaller than the width of the slits in early observations. In recent experiments with large molecules, the diameter of the particle has approached the width of the slits. Therefore, analytical description of these cases should include a finite particle size. The generic quantum interference setup is an asymmetric double slit interferometer. We evaluate the wave function of the particle transverse motion using two forms of the solution of Schrodinger's equation in an asymmetric interferometer: the Fresnel-Kirchhoff form and the form derived from the transverse wave function in the momentum representation. The transverse momentum distribution is independent of the distance from the slits, while the space distribution strongly depends on this distance. Based on the transverse momentum distribution we determined the space distribution of particles behind the slits. We will present two cases: a) when the diameter of the particle may be neglected with respect to the width of both slits, and b) when the diameter of the particle is larger than the width of the smaller slit.

quant-ph

Non-classical behavior of atoms in an interferometer

We have studied the properties of the non-classical behavior of atoms in a double-slit interferometer. An indication of this behavior for metastable helium was reported by Kurtsiefer, Pfau and Mlynek [Nature 386, 150 (1997)] showing distinctive negative values of the Wigner function, which was reconstructed from the measured diffraction data. Our approach to explain this non-classical behavior is based on the de Broglie-Bohm-Vigier-Selleri understanding of the wave-particle duality and compatible statistical interpretation of the atomic wave function. It follows from the results that the atomic motion is non-classical because it does not obey the laws of classical mechanics. However, there is no evidence that this atomic behavior violates the classical probability law of the addition of probabilities.

quant-ph