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We show that if a flavour-less vector meson remains bound after deconfinement, and if its limiting velocity in the quark-gluon plasma is subluminal, then this meson produces a distinct peak in the spectrum of thermal photons emitted by the plasma.
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C. Hoyos-Badajoz, K. Landsteiner and S. Montero, JHEP 0704
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An alternative possibility (not realised in plasmas with a gravity dual) would be that meson states with k k above some upper bound cease to exist. In any event, our conclusions will rely on meson states existing (with a sufficiently narrow width) only up to some moderate k k for which ω ( k ) ∼ k \omega(k)\sim k
Cited in the paper.
We assume that the meson is flavour-less and we neglect the thermal mass of the photon
Cited in the paper.
In the vacuum, only the decay into a virtual photon would be allowed by kinematics
Cited in the paper.
Specific examples of this transition in so-called Dp/Dq systems were originally seen in dpdq . More recently similar transitions for Dp/Dq/D q ¯ \bar{\mbox{q}} systems SS have been found in dpdqdqbar
Cited in the paper.
In the Dp/Dq systems this is because the bare quark mass increases; in the Dp/Dq/D q ¯ \bar{\mbox{q}} systems this is because the chiral symmetry-breaking scale increases. In Dp/Dq systems at finite baryon density the branes always fall through the horizon, but for large quark masses the physics is essentially the same as at zero density finite
Cited in the paper.
2008
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