Statistical multifragmentation of nuclei

Bondorf, J.P.; Donangelo, R.; Mishustin, I. N.; Pethick, C. J.; Schulz, H.; Sneppen, Kim

doi:10.1016/0375-9474(85)90266-0

Cited by 462 publications

(319 citation statements)

References 24 publications

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“…We assume, as usual, that the break up into different composites occurs at a radius R c which is greater than normal radius R 0 . Considering this as a process in which a uniform dilute charge distribution within radius R c collapses successively into denser blobs of proper radius R i,j we write the Coulomb energy [126] as…”

Section: Generalisation To a More Realistic Modelmentioning

confidence: 99%

Liquid-Gas Phase Transition in Nuclear Multifragmentation

Gupta

Mekjian

Tsang

2001

Advances in the Physics of Particles and Nuclei

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The equation of state of nuclear matter suggests that at suitable beam energies the disassembling hot system formed in heavy ion collisions will pass through a liquid-gas coexistence region. Searching for the signatures of the phase transition has been a very important focal point of experimental endeavours in heavy-ion collisions, in the last fifteen years. Simultaneously theoretical models have been developed to provide information about the equation of state and reaction mechanisms consistent with the experimental observables.

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Section: Generalisation To a More Realistic Modelmentioning

confidence: 99%

Liquid-Gas Phase Transition in Nuclear Multifragmentation

Gupta

Mekjian

Tsang

2001

Advances in the Physics of Particles and Nuclei

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“…Indeed from 32 to 52 A · MeV the proportions of 1 and 2-IMF events decrease slightly whereas the other partitions increase. This rise of the IMF yield with energy is predicted by statistical models [5,7]. However owing to the total charge conservation, the IMF charge falls as the IMF multiplicity goes up.…”

Section: General Trendsmentioning

confidence: 63%

“…Some theoretical calculations support this new interpretation and predict an initial compression phase of the nuclear matter followed by an expansion phase during which the fragments are created [3,4]. Moreover a liquid-gaz phase transition could be associated with this multifragmentation process [5]. The new generation of 4π detector such as INDRA should give some reliable answers to these open questions in the next years.…”

Section: Introductionmentioning

confidence: 85%

Evolution of Fragment Distributions and Reaction Mechanisms for the 36Ar + 58Ni System From 32 to 95 A.Mev

Nalpas

Charvet

Dayras

et al. 1996

Advances in Nuclear Dynamics

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Within the framework of flow and multifragmentation study, the 36 Ar+ 58 Ni experiment has been performed at seven incident energies from 32 to 95 A · MeV with the INDRA detector at GANIL. After a brief description of the experimental set-up, the main trends as well as the evolution of fragment distributions will be presented. Some results about reaction mechanisms for particular classes of events will conclude this report.

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“…Similar expressions can be deIjved for the canonical and grand canonical partition functions, eqs .. (9)(10). In particular, the canonical partition function (9) takes precisely the form (15) with (IS) while the grand-canonical partition function (10) …”

mentioning

confidence: 76%

“…In particular, the canonical partition function (9) takes precisely the form (15) with (IS) while the grand-canonical partition function (10) …”

mentioning

confidence: 99%