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Reversal of orbital angular momentum arising from an extreme Doppler shift.


ABSTRACT: 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.

SUBMITTER: Gibson GM 

PROVIDER: S-EPMC5899465 | biostudies-literature | 2018 Apr

REPOSITORIES: biostudies-literature

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Reversal of orbital angular momentum arising from an extreme Doppler shift.

Gibson Graham M GM   Toninelli Ermes E   Horsley Simon A R SAR   Spalding Gabriel C GC   Hendry Euan E   Phillips David B DB   Padgett Miles J MJ  

Proceedings of the National Academy of Sciences of the United States of America 20180326 15


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 sign  ...[more]

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