Abstract

In quantum chromodynamics (QCD), the role which topologically non-trivial configurations play in splitting the singlet pseudo-Goldstone meson, the η′η^\prime, from the octet is familiar. In addition, such configurations contribute to other processes which violate the axial U(1)AU(1)_A symmetry. While the nature of topological fluctuations in the confined phase is still unsettled, at temperatures well above that for the chiral phase transition, they can be described by a dilute gas of instantons. We show that instantons of arbitrary topological charge QQ generate anomalous interactions between 2Nf∣Q∣2 N_f |Q| quarks, which for Q=1Q = 1 make the η′η^\prime heavy. For two flavors we compute an anomalous quartic meson coupling and discuss its implications for the phenomenology of the chiral phase transition. A dilute instanton gas suggests that for cold, dense quarks, instantons do not evaporate until very high densities, when the baryon chemical potential is ≳2\gtrsim 2 GeV.

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