Holographic zero sound at finite temperature in the Sakai-Sugimoto model
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Abstract
In this paper, we study the fate of the holographic zero sound mode at finite
temperature and non-zero baryon density in the deconfined phase of the Sakai-Sugimoto
model of holographic QCD. We establish the existence of such a mode for a wide range
of temperatures and investigate the dispersion relation, quasi-normal modes, and spectral
functions of the collective excitations in four different regimes, namely, the collisionless
quantum, collisionless thermal, and two distinct hydrodynamic regimes. For sufficiently
high temperatures, the zero sound completely disappears, and the low energy physics is
dominated by an emergent diffusive mode. We compare our findings to Landau-Fermi
liquid theory and to other holographic models
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DiNunno, B.S., Ihl, M., Jokela, N. et al. Holographic zero sound at finite temperature in the Sakai-Sugimoto model. J. High Energ. Phys. 2014, 149 (2014). https://doi.org/10.1007/JHEP04(2014)149
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https://doi.org/10.1007/JHEP04(2014)149Sponsors
The
work of B.D and J.P is partially supported by the National Science Foundation under grant
Grant No. PHY-1316033 and by the Texas Cosmology Center. M.I. is funded by the FCT
fellowship SFRH/BI/52188/2013. The Centro de F´ısica do Porto is partially funded by
FCT through the projects PTDC/FIS/099293/2008 and CERN/FP/116358/2010. N.J. is
funded by the Spanish grant FPA2011-22594, by the Consolider-Ingenio 2010 Programme
CPAN (CSD2007-00042), by Xunta de Galicia (GRC2013-024), and by FEDER. N.J. is
also supported by the Juan de la Cierva program
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© 2014 The Authors. This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (https://creativecommons.org/licenses/by/4.0), which permits use, duplication, adaptation, distribution, and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made



