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The holographic dual of a finite-temperature gauge theory with a small number of flavours typically contains D-brane probes in a black hole background. At low temperature the branes sit outside the black hole and the meson spectrum is discrete and possesses a mass gap. As the temperature increases the branes approach a critical solution. Eventually they fall into the horizon and a phase transition occurs. In the new phase the meson spectrum is continuous and gapless. At large N and large 't Hooft coupling, this phase transition is always of first order, and in confining theories with heavy quarks it occurs at a temperature higher than the deconfinement temperature for the glue.
6 pages, 7 figures, RevTeX4; v2: minor changes, reference added
High Energy Physics - Theory, Field theory (Physics), Teoria de camps (Física), FOS: Physical sciences, String and superstring theories; other extended objects (e.g., branes) in quantum field theory, Partícules (Física nuclear), Cromodinàmica quàntica, High Energy Physics - Phenomenology, High Energy Physics - Phenomenology (hep-ph), High Energy Physics - Theory (hep-th), Quantum chromodynamics, Particles (Nuclear physics)
High Energy Physics - Theory, Field theory (Physics), Teoria de camps (Física), FOS: Physical sciences, String and superstring theories; other extended objects (e.g., branes) in quantum field theory, Partícules (Física nuclear), Cromodinàmica quàntica, High Energy Physics - Phenomenology, High Energy Physics - Phenomenology (hep-ph), High Energy Physics - Theory (hep-th), Quantum chromodynamics, Particles (Nuclear physics)
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