2015
DOI: 10.1016/j.aop.2015.08.012
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Gouy phase and visibility in the double-slit experiment

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Cited by 10 publications
(5 citation statements)
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“…The indices R and I stand for the real and imaginary part of the complex numbers that appear in the solutions. As discussed in [23], µ et (t, τ ) and θ et (t, τ ) are phases that do not depend of the transverse position x, i.e., they are axial phases. Different from the Gouy phase µ et (t, τ ) (App.…”
Section: Resultsmentioning
confidence: 99%
“…The indices R and I stand for the real and imaginary part of the complex numbers that appear in the solutions. As discussed in [23], µ et (t, τ ) and θ et (t, τ ) are phases that do not depend of the transverse position x, i.e., they are axial phases. Different from the Gouy phase µ et (t, τ ) (App.…”
Section: Resultsmentioning
confidence: 99%
“…The state at the detector is represented by a density matrix. We consider the paraxial propagation, i.e., p x p z and the classical movement in the z-direction such that z = v z t. Thus, the quantum effects are observed only in the x-direction [20,21]. This is illustrated in fig.…”
Section: Double-slit Experiments With Loss Of Coherence -mentioning
confidence: 99%
“…For instance, line-focusing a cylindrical wave propagating from to yields a Gouy phase of , while point-focusing a spherical wave in the same interval yields a Gouy phase of 11 . Gaussian matter wave packets diffracting through small apertures generate a Gouy phase of 12 . Experiments were performed with acoustic and water waves 13 – 15 , surface plasmon-polaritons with non-Gaussian spatial properties 16 , focused cylindrical phonon-polariton wave packets in LiTaO 3 crystals, and for Bose-Einstein condensates and electron waves 17 20 .…”
Section: Introductionmentioning
confidence: 99%