blob: d081a9436d4606f935afd2116e08968d2fe18948 (
plain)
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
|
<html>
<head></head>
<body>
<br id="br1"/>
<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"/>
</body>
</html>
|
