Abstract

The hot and dense medium formed in high energy heavy ion collisions may modify some hadronic properties. In particular, if hadron masses are shifted in-medium, it was demonstrated that this could lead to back-to-back squeezed correlations (BBC) of particle-antiparticle pairs. Although well-established theoretically, the squeezed correlations have not yet been discovered experimentally. A method has been suggested for the empirical search of this effect, which was previously illustrated for $\ensuremath{\phi}\ensuremath{\phi}$ pairs. We apply here the formalism and the suggested method to the case of ${K}^{+}{K}^{\ensuremath{-}}$ pairs, since they may be easier to identify experimentally. The time distribution of the emission process plays a crucial role in the survival of the BBC's. We analyze the cases where the emission is supposed to occur suddenly or via a Lorentzian distribution, and compare with the case of a L\'evy distribution in time. Effects of squeezing on the correlation function of identical particles are also analyzed.

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