Acoustic ghost diffraction

An attempt is made to implement acoustic ghost diffraction in the space-momentum domain using ultrasound. The Hanbury Brown—Twiss effect helps ghost diffraction—interference fringes hidden in a large backdrop of first-order fringes to materialize only after making the two emitters mutually incoherent in a post-selective manner, which is leveraged by programmed decoherence. Cross correlation of phononic coherent states is taken in a reciprocal two-slit diffraction geometry so that nontrivial fringes due to virtual one-phonon diffraction—interference fringes emulated by two phonons emerge on the side of the transmitter as opposed to the receiver.

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Institutions

Publication Details

Journal
Applied Physics Letters
Published
2025-07-14
DOI
https://doi.org/10.1063/5.0268818
Citations
1
Primary Topic
Random lasers and scattering media
Type
article
Field-Weighted Citation Impact
1.30

Funders

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article

Acoustic ghost diffraction

S. Fukatsu, Ryota Keyaki, Hiroka Otomo
1 citations
Applied Physics Letters
Random lasers and scattering media
1.30
article

Acoustic ghost diffraction

S. Fukatsu, Ryota Keyaki, Hiroka Otomo
article en
1 citations

Abstract

An attempt is made to implement acoustic ghost diffraction in the space-momentum domain using ultrasound. The Hanbury Brown—Twiss effect helps ghost diffraction—interference fringes hidden in a large backdrop of first-order fringes to materialize only after making the two emitters mutually incoherent in a post-selective manner, which is leveraged by programmed decoherence. Cross correlation of phononic coherent states is taken in a reciprocal two-slit diffraction geometry so that nontrivial fringes due to virtual one-phonon diffraction—interference fringes emulated by two phonons emerge on the side of the transmitter as opposed to the receiver.

Applied Physics LettersVol. 127(2)
Tokyo University of the Arts (JP), The University of Tokyo (JP)
Japan Society for the Promotion of Science
Openalex Percentile: Top 20%
Random lasers and scattering media
1.30
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