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Origin of quantum-mechanical complementarity probed by a ‘which-way’ experiment in an atom interferometer

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Abstract

The principle of complementarity refers to the ability of quantum-mechanical entities to behave as particles or waves under different experimental conditions. For example, in the famous double-slit experiment, a single electron can apparently pass through both apertures simultaneously, forming an interference pattern. But if a ‘which-way’ detector is employed to determine the particle's path, the interference pattern is destroyed. This is usually explained in terms of Heisenberg's uncertainty principle, in which the acquisition of spatial information increases the uncertainty in the particle's momentum, thus destroying the interference. Here we report a which-way experiment in an atom interferometer in which the ‘back action’ of path detection on the atom's momentum is too small to explain the disappearance of the interference pattern. We attribute it instead to correlations between the which-way detector and the atomic motion, rather than to the uncertainty principle.

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Figure 1: Scheme of the atom interferometer.
Figure 2: Spatial fringe pattern in the far field of the interferometer.
Figure 3: Storage of which-way information.
Figure 4: Same as Fig. 2a, but with which-way information stored in the internal atomic state.

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Acknowledgements

We thank S. Kunze for discussions. This work was supported by the Deutsche Forschungsgemeinschaft.

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Correspondence to G. Rempe.

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Dürr, S., Nonn, T. & Rempe, G. Origin of quantum-mechanical complementarity probed by a ‘which-way’ experiment in an atom interferometer. Nature 395, 33–37 (1998). https://doi.org/10.1038/25653

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