Titlebook: Advances in Nuclear Dynamics 2; Wolfgang Bauer,Gary D. Westfall Book 1996 Springer Science+Business Media New York 1996 collision.fission.

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https://doi.org/10.1007/978-1-349-24791-2of E877 at the Brookhaven AGS is to measure the transverse energy .. produced in these collisions in conjunction with the identification of single particles within a limited region of phase space. Among the major results for Au + Au collisions are the large degree of stopping deduced from ... and th

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https://doi.org/10.1007/978-1-349-24791-2] can result in decay of the excited nuclear system into multiple intermediate mass fragments (IMFs:3 ≤ . ≤ 20). Such a multifragment final state might arise due to either dynamical surface instabilities of the composite system, or alternatively from volume instabilities [5, 6]. While decay driven b

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https://doi.org/10.1007/978-3-662-21714-6ing to multiple intermediate-mass fragments (IMF) in the reaction exit channel. Since the standard statistical model appeared to be unable to account for the large observed IMF multiplicities, various models and scenarios have been proposed ., which favor copious production of IMFs. On the other han

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Imperforate Tracheary Elements,nt factors contribute to that situation. Thus, for one, the nucleon excitation energies are low and in that comparable to nucleon localization energies, indicating a likely importance of the quantal effects. With the change in the beam energy in the discussed range, the dynamics changes from that do

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Thomas Amossé,Alex Bryson,Hélo?se Petities of up to three times normal nuclear matter density are reached, where theoretical models. predict a partial restoration of chiral symmetry. In vacuum, chiral symmetry is spontanously broken, leading to the constituent quark masses of about 300 MeV/c.. One can assume that chiral symmetry restorat