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Reversal of orbital angular momentum arising from an extreme Doppler shift

The linear Doppler shift is familiar as the rise and fall in pitch of a siren as it passes by. Less well known is the rotational Doppler shift, proportional to the rotation rate between source and receiver, multiplied by the angular momentum carried by the beam. In extreme cases the Doppler shift ca...

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Autores principales: Gibson, Graham M., Toninelli, Ermes, Horsley, Simon A. R., Spalding, Gabriel C., Hendry, Euan, Phillips, David B., Padgett, Miles J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: National Academy of Sciences 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5899465/
https://www.ncbi.nlm.nih.gov/pubmed/29581257
http://dx.doi.org/10.1073/pnas.1720776115
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author Gibson, Graham M.
Toninelli, Ermes
Horsley, Simon A. R.
Spalding, Gabriel C.
Hendry, Euan
Phillips, David B.
Padgett, Miles J.
author_facet Gibson, Graham M.
Toninelli, Ermes
Horsley, Simon A. R.
Spalding, Gabriel C.
Hendry, Euan
Phillips, David B.
Padgett, Miles J.
author_sort Gibson, Graham M.
collection PubMed
description The linear Doppler shift is familiar as the rise and fall in pitch of a siren as it passes by. Less well known is the rotational Doppler shift, proportional to the rotation rate between source and receiver, multiplied by the angular momentum carried by the beam. In extreme cases the Doppler shift can be larger than the rest-frame frequency and for a red shift, the observed frequency then becomes “negative.” In the linear case, this effect is associated with the time reversal of the received signal, but it can be observed only with supersonic relative motion between the source and receiver. However, the rotational case is different; if the radius of rotation is smaller than the wavelength, then the velocities required to observe negative frequencies are subsonic. Using an acoustic source at [Formula: see text] 100 Hz we create a rotational Doppler shift larger than the laboratory-frame frequency. We observe that once the red-shifted wave passes into the “negative frequency” regime, the angular momentum associated with the sound is reversed in sign compared with that of the laboratory frame. These low-velocity laboratory realizations of extreme Doppler shifts have relevance to superoscillatory fields and offer unique opportunities to probe interactions with rotating bodies and aspects of pseudorelativistic frame translation.
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spelling pubmed-58994652018-04-17 Reversal of orbital angular momentum arising from an extreme Doppler shift Gibson, Graham M. Toninelli, Ermes Horsley, Simon A. R. Spalding, Gabriel C. Hendry, Euan Phillips, David B. Padgett, Miles J. Proc Natl Acad Sci U S A Physical Sciences The linear Doppler shift is familiar as the rise and fall in pitch of a siren as it passes by. Less well known is the rotational Doppler shift, proportional to the rotation rate between source and receiver, multiplied by the angular momentum carried by the beam. In extreme cases the Doppler shift can be larger than the rest-frame frequency and for a red shift, the observed frequency then becomes “negative.” In the linear case, this effect is associated with the time reversal of the received signal, but it can be observed only with supersonic relative motion between the source and receiver. However, the rotational case is different; if the radius of rotation is smaller than the wavelength, then the velocities required to observe negative frequencies are subsonic. Using an acoustic source at [Formula: see text] 100 Hz we create a rotational Doppler shift larger than the laboratory-frame frequency. We observe that once the red-shifted wave passes into the “negative frequency” regime, the angular momentum associated with the sound is reversed in sign compared with that of the laboratory frame. These low-velocity laboratory realizations of extreme Doppler shifts have relevance to superoscillatory fields and offer unique opportunities to probe interactions with rotating bodies and aspects of pseudorelativistic frame translation. National Academy of Sciences 2018-04-10 2018-03-26 /pmc/articles/PMC5899465/ /pubmed/29581257 http://dx.doi.org/10.1073/pnas.1720776115 Text en Copyright © 2018 the Author(s). Published by PNAS. https://creativecommons.org/licenses/by-nc-nd/4.0/ This open access article is distributed under Creative Commons Attribution-NonCommercial-NoDerivatives License 4.0 (CC BY-NC-ND) (https://creativecommons.org/licenses/by-nc-nd/4.0/) .
spellingShingle Physical Sciences
Gibson, Graham M.
Toninelli, Ermes
Horsley, Simon A. R.
Spalding, Gabriel C.
Hendry, Euan
Phillips, David B.
Padgett, Miles J.
Reversal of orbital angular momentum arising from an extreme Doppler shift
title Reversal of orbital angular momentum arising from an extreme Doppler shift
title_full Reversal of orbital angular momentum arising from an extreme Doppler shift
title_fullStr Reversal of orbital angular momentum arising from an extreme Doppler shift
title_full_unstemmed Reversal of orbital angular momentum arising from an extreme Doppler shift
title_short Reversal of orbital angular momentum arising from an extreme Doppler shift
title_sort reversal of orbital angular momentum arising from an extreme doppler shift
topic Physical Sciences
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5899465/
https://www.ncbi.nlm.nih.gov/pubmed/29581257
http://dx.doi.org/10.1073/pnas.1720776115
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