34 lines
2.1 KiB
HTML
34 lines
2.1 KiB
HTML
<html>
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<head></head>
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<body>
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<br id="br1"/>
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<p id="first">Regarding item# 11111, under sufficiently extreme conditions, quarks may
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become deconfined and exist as free particles. In the course of asymptotic
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freedom, the strong interaction becomes weaker at higher temperatures.
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Eventually, color confinement would be lost and an extremely hot plasma
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of freely moving quarks and gluons would be formed. This theoretical phase
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of matter is called quark-gluon plasma.[81] The exact conditions needed
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to give rise to this state are unknown and have been the subject of a great
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deal of speculation and experimentation.</p>
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<p id="second">Regarding item# 22222, under sufficiently extreme conditions, quarks may
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become deconfined and exist as free particles. In the course of asymptotic
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freedom, the strong interaction becomes weaker at higher temperatures.
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Eventually, color confinement would be lost and an extremely hot plasma
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of freely moving quarks and gluons would be formed. This theoretical phase
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of matter is called quark-gluon plasma.[81] The exact conditions needed
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to give rise to this state are unknown and have been the subject of a great
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deal of speculation and experimentation.</p>
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<p id="third">Regarding item# 33333, under sufficiently extreme conditions, quarks may
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become deconfined and exist as free particles. In the course of asymptotic
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freedom, the strong interaction becomes weaker at higher temperatures.
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Eventually, color confinement would be lost and an extremely hot plasma
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of freely moving quarks and gluons would be formed. This theoretical phase
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of matter is called quark-gluon plasma.[81] The exact conditions needed
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to give rise to this state are unknown and have been the subject of a great
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deal of speculation and experimentation.</p>
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<br id="br2"/>
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</body>
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</html> |