   Regarding item# 11111, under sufficiently extreme conditions, quarks may
   become deconfined and exist as free particles. In the course of asymptotic
   freedom, the strong interaction becomes weaker at higher temperatures.
   Eventually, color confinement would be lost and an extremely hot plasma of
   freely moving quarks and gluons would be formed. This theoretical phase of
   matter is called quark-gluon plasma.[81] The exact conditions needed to
   give rise to this state are unknown and have been the subject of a great
   deal of speculation and experimentation.

   Regarding item# 22222, under sufficiently extreme conditions, quarks may
   become deconfined and exist as free particles. In the course of asymptotic
   freedom, the strong interaction becomes weaker at higher temperatures.
   Eventually, color confinement would be lost and an extremely hot plasma of
   freely moving quarks and gluons would be formed. This theoretical phase of
   matter is called quark-gluon plasma.[81] The exact conditions needed to
   give rise to this state are unknown and have been the subject of a great
   deal of speculation and experimentation.

   Regarding item# 33333, under sufficiently extreme conditions, quarks may
   become deconfined and exist as free particles. In the course of asymptotic
   freedom, the strong interaction becomes weaker at higher temperatures.
   Eventually, color confinement would be lost and an extremely hot plasma of
   freely moving quarks and gluons would be formed. This theoretical phase of
   matter is called quark-gluon plasma.[81] The exact conditions needed to
   give rise to this state are unknown and have been the subject of a great
   deal of speculation and experimentation.
