Breaking rotations without violating the KSS viscosity bound
A bstract We revisit the computation of the shear viscosity to entropy ratio in a holographic p-wave superfluid model, focusing on the role of rotational symmetry breaking. We study the interplay between explicit and spontaneous symmetry breaking and derive a simple horizon formula for η/s , which i...
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Published in | The journal of high energy physics Vol. 2023; no. 7; pp. 16 - 33 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
Published |
Berlin/Heidelberg
Springer Berlin Heidelberg
03.07.2023
Springer Nature B.V SpringerOpen |
Subjects | |
Online Access | Get full text |
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Summary: | A
bstract
We revisit the computation of the shear viscosity to entropy ratio in a holographic p-wave superfluid model, focusing on the role of rotational symmetry breaking. We study the interplay between explicit and spontaneous symmetry breaking and derive a simple horizon formula for
η/s
, which is valid also in the presence of explicit breaking of rotations and is in perfect agreement with the numerical data. We observe that a source which explicitly breaks rotational invariance suppresses the value of
η/s
in the broken phase, competing against the effects of spontaneous symmetry breaking. However,
η/s
always reaches a constant value in the limit of zero temperature, which is never smaller than the Kovtun-Son-Starinets (KSS) bound, 1
/
4
π
. This behavior appears to be in contrast with previous holographic anisotropic models which found a power-law vanishing of
η/s
at small temperature. This difference is shown to arise from the properties of the near-horizon geometry in the extremal limit. Thus, our construction shows that the breaking of rotations itself does not necessarily imply a violation of the KSS bound. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP07(2023)016 |