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+<div>
+ <p id="first">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.</p>
+ <p id="second">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.</p>
+ <p id="third">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.</p>
+ <br id="br2"></br></div> \ No newline at end of file