Abstract
In the course of the past few years, the nuclear Boltzmann-Langevin (BL) model has emerged as a promising microscopic model for nuclear dynamics at intermediate energies1,2. The BL model goes beyond the much employed Boltzmann-Uehling-Uhlenbeck (BUU) model3, and hence it provides a basis for describing dynamics of density fluctuations and addressing processes exhibiting spontaneous symmetry breaking and catastrophic transformations in nuclear collisions, such as induced fission and mult ifragmentation4,5,6.
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Ayik, S. (1996). Dynamics of Density Fluctuations in a Non-Markovian Boltzmann-Langevin Model. In: Bauer, W., Westfall, G.D. (eds) Advances in Nuclear Dynamics 2. Springer, Boston, MA. https://doi.org/10.1007/978-1-4757-9086-3_7
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DOI: https://doi.org/10.1007/978-1-4757-9086-3_7
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