The nuclear lattice model of proton-induced multi-fragmentation reactions☆
References (33)
- et al.
Phys. Lett.
(1982)et al.Phys. Rev.
(1984) - et al.
Phys. Rev.
(1984)et al.Nucl. Phys.
(1984)et al.Nucl. Phys.
(1985)et al.Nucl. Phys.
(1985) - et al.
Phys. Rev.
(1983)et al.Phys. Rev.
(1983) - et al.
Z. Phys.
(1984) - et al.
Nucl. Phys.
(1981)et al.Phys. Lett.
(1982)et al.Nucl. Phys.
(1982)et al.Nucl. Phys.
(1983) Physica
(1979)- et al.
Phys. Rev. Lett.
(1979)et al.Z. Phys.
(1981) Physics
(1967)- et al.
J. of Phys.
(1982)
Nucl. Phys.
(1976)
et al.Phys. Rev.
(1983)
et al.Phys. Rev.
(1984)
Cited by (133)
The percolation phase transition and statistical multifragmentation in finite systems
2020, Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy PhysicsSystem size effect on the critical behavior in nuclear multifragmentation
2011, Nuclear Physics AFragmentation and the Nuclear Equation of State
2007, Nuclear Physics AGeometrical aspects of isoscaling
2007, Physica A: Statistical Mechanics and its ApplicationsCitation Excerpt :In order to explore the behavior of isoscaling we use a three-dimensional bond percolation model. This model was first applied in nuclear multifragmentation by Bauer et al. [13] and used by many groups [14–17] ever since. In the usual bond percolation model, a fragmenting nucleus is represented by a three-dimensional cubic lattice, and individual “nucleons” by nodes on the lattice.
Light-ion-induced multifragmentation: The ISiS project
2006, Physics ReportsAnalysis of the characteristics of nucleus-nucleus collisions depending on the centrality
2004, Nuclear Physics A
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Work supported by BMFT and GSI Darmstadt.
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