Nonclassical Paths in Quantum Interference Experiments

Aug 8, 2013
5 pages
Published in:
  • Phys.Rev.Lett. 113 (2014) 12, 120406
  • Published: Sep 19, 2014
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Abstract: (APS)
In a double slit interference experiment, the wave function at the screen with both slits open is not exactly equal to the sum of the wave functions with the slits individually open one at a time. The three scenarios represent three different boundary conditions and as such, the superposition principle should not be applicable. However, most well-known text books in quantum mechanics implicitly and/or explicitly use this assumption that is only approximately true. In our present study, we have used the Feynman path integral formalism to quantify contributions from nonclassical paths in quantum interference experiments that provide a measurable deviation from a naive application of the superposition principle. A direct experimental demonstration for the existence of these nonclassical paths is difficult to present. We find that contributions from such paths can be significant and we propose simple three-slit interference experiments to directly confirm their existence.
Note:
  • v2: 5 pages + 3 pages supplementary, title changed, version to appear in Physical Review Letters
  • 03.65.Ta
  • 31.15.xk
  • wave function
  • interference
  • path integral
  • boundary condition
  • quantum mechanics
  • [1]
    Classical Theory of Fields (Pergammon Press, Oxford, Fourth revised English Edition,)
    • L.D. Landau
      ,
    • E.M. Lifshitz
  • [2]
    Principles of Optics (Cambridge University Press, Seventh expanded edition,)
    • M. Born
      ,
    • E. Wolf
  • [3]
    Sunil
    • Kumar P. B.
      ,
    • Ranganath G. S.
      • Pramana 3 (1991) 6
  • [4]
    The Feynman Lectures on Physics Vol. 3 ey, Reading Mass,)
    • Feynman
      ,
    • R. R. P. Leighton
      ,
    • M. Sands
  • [5]
    Quantum Mechanics I CH, 2nd edition,)
    • Cohen-Tannoudji
      ,
    • B. C. Diu
      ,
    • F. Laloe
  • [6]
    Principles of Quantum Mechanics 2nd edition,)
    • R. Shankar
  • [7]
    Strictly Speaking, in equation S19 one should excise the region where |r1 - r2| ∼ λ (the diagonal of the Ω × Ω integration). This integral is already accounted for in KΩ 1. However this does not affect any of the terms in the expression (S22)
    • [10]
      Quantum Mechanics and Path Integrals New York, 3rd. ed.)
      • R.P. Feynman
        ,
      • A.R. Hibbs