Abstract
It is shown possible to define the temperature of Lorentz-squeezed hadrons in terms of their speed. Within the framework of the covariant harmonic oscillator formalism which is the simplest scientific language for Lorentz-squeezed hadrons, the hadronic temperature is measured through ( v c ) 2 = exp( - h ̵ ω kT ) . As the temperature rises, the hadron goes through a transition from the confinement phase to a plasma phase.
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