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What can we learn from a second phi meson peak in ultrarelativistic nuclear collisions

Journal Article · · Physical Review, C (Nuclear Physics); (United States)
;  [1]
  1. Cyclotron Institute and Physics Department, Texas A M University, College Station, Texas 77843 (United States) Theory Divison, CERN, CH-1211 Geneva 23 (Switzerland)
The decay width of a phi meson is reduced from its vacuum value as its mass decreases in hot hadronic matter as a result of the partial restoration of chiral symmetry. This reduction is, however, cancelled by collisional broadening through the reactions [phi][pi][r arrow][ital KK][sup *], [phi][ital K][r arrow][phi][ital K], [phi][rho][r arrow][ital KK], and [phi][phi][r arrow][ital KK]. The resulting phi meson width in hot hadronic matter is found to be less than about 10 MeV for temperatures below 200 MeV. If hadronic matter has a strong first-order phase transtion, this narrow phi meson with reduced mass will appear as a second peak in the dilepton spectrum in ultrarelativistic heavy-ion collisions. We discuss use of this second phi peak to determine the transition temperature and the lifetime of the two-phase coexistence region in the case of a strong first-order phase transition. We also discuss using the peak to determine the range of temperatures over which the transition occurs in the case of a smooth but fast change in the entropy density.
OSTI ID:
5093058
Journal Information:
Physical Review, C (Nuclear Physics); (United States), Journal Name: Physical Review, C (Nuclear Physics); (United States) Vol. 49:4; ISSN 0556-2813; ISSN PRVCAN
Country of Publication:
United States
Language:
English