Chiral drag force
We provide a holographic evaluation of novel contributions to the drag force acting on a heavy quark moving through strongly interacting plasma. The new contributions are chiral in the sense that they act in opposite directions in plasmas containing an excess of left- or right-handed quarks. The new...
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Springer Berlin Heidelberg
2016
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Online Access: | http://hdl.handle.net/1721.1/103803 https://orcid.org/0000-0001-9679-2409 https://orcid.org/0000-0001-5812-8718 |
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author | Rajagopal, Krishna Sadofyev, Andrey |
author2 | Massachusetts Institute of Technology. Center for Theoretical Physics |
author_facet | Massachusetts Institute of Technology. Center for Theoretical Physics Rajagopal, Krishna Sadofyev, Andrey |
author_sort | Rajagopal, Krishna |
collection | MIT |
description | We provide a holographic evaluation of novel contributions to the drag force acting on a heavy quark moving through strongly interacting plasma. The new contributions are chiral in the sense that they act in opposite directions in plasmas containing an excess of left- or right-handed quarks. The new contributions are proportional to the coefficient of the axial anomaly, and in this sense also are chiral. These new contributions to the drag force act either parallel to or antiparallel to an external magnetic field or to the vorticity of the fluid plasma. In all these respects, these contributions to the drag force felt by a heavy quark are analogous to the chiral magnetic effect (CME) on light quarks. However, the new contribution to the drag force is independent of the electric charge of the heavy quark and is the same for heavy quarks and antiquarks, meaning that these novel effects do not in fact contribute to the CME current. We show that although the chiral drag force can be non-vanishing for heavy quarks that are at rest in the local fluid rest frame, it does vanish for heavy quarks that are at rest in a suitably chosen frame. In this frame, the heavy quark at rest sees counterpropagating momentum and charge currents, both proportional to the axial anomaly coefficient, but feels no drag force. This provides strong concrete evidence for the absence of dissipation in chiral transport, something that has been predicted previously via consideration of symmetries. Along the way to our principal results, we provide a general calculation of the corrections to the drag force due to the presence of gradients in the flowing fluid in the presence of a nonzero chemical potential. We close with a consequence of our result that is at least in principle observable in heavy ion collisions, namely an anticorrelation between the direction of the CME current for light quarks in a given event and the direction of the kick given to the momentum of all the heavy quarks and antiquarks in that event. |
first_indexed | 2024-09-23T11:30:44Z |
format | Article |
id | mit-1721.1/103803 |
institution | Massachusetts Institute of Technology |
language | English |
last_indexed | 2024-09-23T11:30:44Z |
publishDate | 2016 |
publisher | Springer Berlin Heidelberg |
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spelling | mit-1721.1/1038032022-10-01T04:07:18Z Chiral drag force Rajagopal, Krishna Sadofyev, Andrey Massachusetts Institute of Technology. Center for Theoretical Physics Massachusetts Institute of Technology. Department of Physics Rajagopal, Krishna Sadofyev, Andrey We provide a holographic evaluation of novel contributions to the drag force acting on a heavy quark moving through strongly interacting plasma. The new contributions are chiral in the sense that they act in opposite directions in plasmas containing an excess of left- or right-handed quarks. The new contributions are proportional to the coefficient of the axial anomaly, and in this sense also are chiral. These new contributions to the drag force act either parallel to or antiparallel to an external magnetic field or to the vorticity of the fluid plasma. In all these respects, these contributions to the drag force felt by a heavy quark are analogous to the chiral magnetic effect (CME) on light quarks. However, the new contribution to the drag force is independent of the electric charge of the heavy quark and is the same for heavy quarks and antiquarks, meaning that these novel effects do not in fact contribute to the CME current. We show that although the chiral drag force can be non-vanishing for heavy quarks that are at rest in the local fluid rest frame, it does vanish for heavy quarks that are at rest in a suitably chosen frame. In this frame, the heavy quark at rest sees counterpropagating momentum and charge currents, both proportional to the axial anomaly coefficient, but feels no drag force. This provides strong concrete evidence for the absence of dissipation in chiral transport, something that has been predicted previously via consideration of symmetries. Along the way to our principal results, we provide a general calculation of the corrections to the drag force due to the presence of gradients in the flowing fluid in the presence of a nonzero chemical potential. We close with a consequence of our result that is at least in principle observable in heavy ion collisions, namely an anticorrelation between the direction of the CME current for light quarks in a given event and the direction of the kick given to the momentum of all the heavy quarks and antiquarks in that event. United States. Department of Energy (Contract Number DE-SC0011090) Russian Foundation for Basic Research (grant 14-02-01185A) 2016-07-29T17:09:07Z 2016-07-29T17:09:07Z 2015-10 2015-07 2016-05-23T09:37:27Z Article http://purl.org/eprint/type/JournalArticle 1029-8479 http://hdl.handle.net/1721.1/103803 Rajagopal, Krishna, and Andrey V. Sadofyev. “Chiral Drag Force.” Journal of High Energy Physics 2015.10 (2015): n. pag. https://orcid.org/0000-0001-9679-2409 https://orcid.org/0000-0001-5812-8718 en http://dx.doi.org/10.1007/JHEP10(2015)018 Journal of High Energy Physics Creative Commons Attribution http://creativecommons.org/licenses/by/4.0/ The Author(s) application/pdf Springer Berlin Heidelberg Springer Berlin Heidelberg |
spellingShingle | Rajagopal, Krishna Sadofyev, Andrey Chiral drag force |
title | Chiral drag force |
title_full | Chiral drag force |
title_fullStr | Chiral drag force |
title_full_unstemmed | Chiral drag force |
title_short | Chiral drag force |
title_sort | chiral drag force |
url | http://hdl.handle.net/1721.1/103803 https://orcid.org/0000-0001-9679-2409 https://orcid.org/0000-0001-5812-8718 |
work_keys_str_mv | AT rajagopalkrishna chiraldragforce AT sadofyevandrey chiraldragforce |