Liquid-fog and liquid-gas phase transitions in hot nuclei
Thermal multifragmentation of hot nuclei is interpreted as the nuclear liquid-fog phase transition inside the spinodal region. The exclusive data for p(8.1 GeV) + Au collisions are analyzed within the framework of the statistical model SMM. It is found that the partition of hot nuclei is specified a...
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Veröffentlicht in: | Physics of atomic nuclei 2006-07, Vol.69 (7), p.1142-1148 |
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container_title | Physics of atomic nuclei |
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creator | Karnaukhov, V. A. Oeschler, H. Budzanowski, A. Avdeyev, S. P. Kirakosyan, V. V. Rodionov, V. K. Rukoyatkin, P. A. Simonenko, A. V. Karcz, W. Skwirczyńska, I. Kuzmin, E. A. Norbeck, E. Botvina, A. S. |
description | Thermal multifragmentation of hot nuclei is interpreted as the nuclear liquid-fog phase transition inside the spinodal region. The exclusive data for p(8.1 GeV) + Au collisions are analyzed within the framework of the statistical model SMM. It is found that the partition of hot nuclei is specified after expansion to a volume equal to Vt = (2.6 ± 0.3)V0. The freeze-out volume is found to be twice as large: Vf = (5 ± 1)V0. The similarity between multifragmentation and ordinary fission is discussed. |
doi_str_mv | 10.1134/S1063778806070076 |
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A. ; Oeschler, H. ; Budzanowski, A. ; Avdeyev, S. P. ; Kirakosyan, V. V. ; Rodionov, V. K. ; Rukoyatkin, P. A. ; Simonenko, A. V. ; Karcz, W. ; Skwirczyńska, I. ; Kuzmin, E. A. ; Norbeck, E. ; Botvina, A. S.</creator><creatorcontrib>Karnaukhov, V. A. ; Oeschler, H. ; Budzanowski, A. ; Avdeyev, S. P. ; Kirakosyan, V. V. ; Rodionov, V. K. ; Rukoyatkin, P. A. ; Simonenko, A. V. ; Karcz, W. ; Skwirczyńska, I. ; Kuzmin, E. A. ; Norbeck, E. ; Botvina, A. S.</creatorcontrib><description>Thermal multifragmentation of hot nuclei is interpreted as the nuclear liquid-fog phase transition inside the spinodal region. The exclusive data for p(8.1 GeV) + Au collisions are analyzed within the framework of the statistical model SMM. It is found that the partition of hot nuclei is specified after expansion to a volume equal to Vt = (2.6 ± 0.3)V0. The freeze-out volume is found to be twice as large: Vf = (5 ± 1)V0. 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title | Liquid-fog and liquid-gas phase transitions in hot nuclei |
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