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Abstract
In the case of k=l, √s ≥√s0 =l.847x108x (l ± 0.397)Gev and at the constant temperature and volume, the overage particle number in each fire-ball n and the rapidity y can be related to the following equation 1/n.dn/dy=1/ch2y. (3)/F(Mc2/kBT).exp(-Mc2/kBT.chy)1+ Mc2/kBT.chy+1/2(Mc2/kBT.chy)2 and in the inelastic case where √s ≥√s0 , the cross section σin ~ constant.
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Cite this article:
WANG Zhengzhi. ONE FIRE-BALL[J]. Chin. Phys. Lett., 1989, 6(4): 153-156.
WANG Zhengzhi. ONE FIRE-BALL[J]. Chin. Phys. Lett., 1989, 6(4): 153-156.
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WANG Zhengzhi. ONE FIRE-BALL[J]. Chin. Phys. Lett., 1989, 6(4): 153-156.
WANG Zhengzhi. ONE FIRE-BALL[J]. Chin. Phys. Lett., 1989, 6(4): 153-156.
|