Nonlinear Langevin dynamics via holography

Abstract In this work, we consider non-linear corrections to the Langevin effective theory of a heavy quark moving through a strongly coupled CFT plasma. In AdS/CFT, this system can be identified with that of a string stretched between the boundary and the horizon of an asymptotically AdS black bran...

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Main Authors: Bidisha Chakrabarty, Joydeep Chakravarty, Soumyadeep Chaudhuri, Chandan Jana, R. Loganayagam, Akhil Sivakumar
Format: Article
Language:English
Published: SpringerOpen 2020-01-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP01(2020)165
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spelling doaj-24a7147893724ba3877d63f6e95c9d122021-01-31T12:11:33ZengSpringerOpenJournal of High Energy Physics1029-84792020-01-012020114010.1007/JHEP01(2020)165Nonlinear Langevin dynamics via holographyBidisha Chakrabarty0Joydeep Chakravarty1Soumyadeep Chaudhuri2Chandan Jana3R. Loganayagam4Akhil Sivakumar5International Centre for Theoretical Sciences (ICTS-TIFR), Tata Institute of Fundamental ResearchInternational Centre for Theoretical Sciences (ICTS-TIFR), Tata Institute of Fundamental ResearchInternational Centre for Theoretical Sciences (ICTS-TIFR), Tata Institute of Fundamental ResearchInternational Centre for Theoretical Sciences (ICTS-TIFR), Tata Institute of Fundamental ResearchInternational Centre for Theoretical Sciences (ICTS-TIFR), Tata Institute of Fundamental ResearchInternational Centre for Theoretical Sciences (ICTS-TIFR), Tata Institute of Fundamental ResearchAbstract In this work, we consider non-linear corrections to the Langevin effective theory of a heavy quark moving through a strongly coupled CFT plasma. In AdS/CFT, this system can be identified with that of a string stretched between the boundary and the horizon of an asymptotically AdS black brane solution. We compute the Feynman-Vernon influence phase for the heavy quark by evaluating the Nambu-Goto action on a doubled string configuration. This configuration is the linearised solution of the string motion in the doubled black brane geometry which has been proposed as the holographic dual of a thermal Schwinger-Keldysh contour of the CFT. Our expression for the influence phase passes non-trivial consistency conditions arising from the underlying unitarity and thermality of the bath. The local effective theory obeys the recently proposed non-linear fluctuation dissipation theorem relating the non-Gaussianity of thermal noise to the thermal jitter in the damping constant. This furnishes a non-trivial check for the validity of these relations derived in the weak coupling regime.https://doi.org/10.1007/JHEP01(2020)165Holography and quark-gluon plasmasQuantum Dissipative SystemsAdS- CFT Correspondence
collection DOAJ
language English
format Article
sources DOAJ
author Bidisha Chakrabarty
Joydeep Chakravarty
Soumyadeep Chaudhuri
Chandan Jana
R. Loganayagam
Akhil Sivakumar
spellingShingle Bidisha Chakrabarty
Joydeep Chakravarty
Soumyadeep Chaudhuri
Chandan Jana
R. Loganayagam
Akhil Sivakumar
Nonlinear Langevin dynamics via holography
Journal of High Energy Physics
Holography and quark-gluon plasmas
Quantum Dissipative Systems
AdS- CFT Correspondence
author_facet Bidisha Chakrabarty
Joydeep Chakravarty
Soumyadeep Chaudhuri
Chandan Jana
R. Loganayagam
Akhil Sivakumar
author_sort Bidisha Chakrabarty
title Nonlinear Langevin dynamics via holography
title_short Nonlinear Langevin dynamics via holography
title_full Nonlinear Langevin dynamics via holography
title_fullStr Nonlinear Langevin dynamics via holography
title_full_unstemmed Nonlinear Langevin dynamics via holography
title_sort nonlinear langevin dynamics via holography
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2020-01-01
description Abstract In this work, we consider non-linear corrections to the Langevin effective theory of a heavy quark moving through a strongly coupled CFT plasma. In AdS/CFT, this system can be identified with that of a string stretched between the boundary and the horizon of an asymptotically AdS black brane solution. We compute the Feynman-Vernon influence phase for the heavy quark by evaluating the Nambu-Goto action on a doubled string configuration. This configuration is the linearised solution of the string motion in the doubled black brane geometry which has been proposed as the holographic dual of a thermal Schwinger-Keldysh contour of the CFT. Our expression for the influence phase passes non-trivial consistency conditions arising from the underlying unitarity and thermality of the bath. The local effective theory obeys the recently proposed non-linear fluctuation dissipation theorem relating the non-Gaussianity of thermal noise to the thermal jitter in the damping constant. This furnishes a non-trivial check for the validity of these relations derived in the weak coupling regime.
topic Holography and quark-gluon plasmas
Quantum Dissipative Systems
AdS- CFT Correspondence
url https://doi.org/10.1007/JHEP01(2020)165
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AT chandanjana nonlinearlangevindynamicsviaholography
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