Holographic meson melting

By C. Hoyos, K. Landsteiner, S. Montero. 2006

163 citations recorded by the source corpus.

The plasma phase at high temperatures of a strongly coupled gauge theory can be holographically modelled by an AdS black hole. Matter in the fundamental representation and in the quenched approximation is introduced through embedding D7-branes in the AdS-Schwarzschild background. Low spin mesons correspond to the fluctuations of the D7-brane world volume. As is well known by now, there are two different kinds of embeddings, either reaching down to the black hole horizon or staying outside of it. In the latter case the fluctuations of the D7-brane world volume represent stable low spin mesons. In the plasma phase we do not expect mesons to be stable but to melt at sufficiently high temperature. We model the late stages of this meson melting by the quasinormal modes of D7-brane fluctuations for the embeddings that do reach down to the horizon. The inverse of the imaginary part of the quasinormal frequency gives the typical relaxation time back to equilibrium of the meson perturbation in the hot plasma. We briefly comment on the possible application of our model to quarkonium suppression.

Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Statistical and Nonlinear Physics

View Paper: https://www.semanticscholar.org/paper/daa3a5c33de831fb847f1bdf21309be024f5ee32

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In Astronomy and Astrophysics

  1. R. Myers
  2. D. Mateos
  3. V. Hubeny
  4. M. Rangamani
  5. R. Thomson
  6. Johanna Erdmenger
  7. S. Hartnoll
  8. Diego Trancanelli

In Nuclear and High Energy Physics

  1. R. Myers
  2. D. Mateos
  3. V. Hubeny
  4. S. Hartnoll
  5. Johanna Erdmenger
  6. M. Rangamani
  7. R. Thomson
  8. M. Ammon

In Statistical and Nonlinear Physics

  1. R. Myers
  2. D. Mateos
  3. R. Thomson
  4. Hong Liu
  5. M. Kaminski
  6. V. Hubeny
  7. K. Landsteiner
  8. Johanna Erdmenger

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