By M.A. Hooshyar, Irwin Reichstein, F. Bary Malik

It is the 1st program to nuclear-physics from energy-density useful process, for which Professor Walter Kohn got the Nobel Prize in Chemistry. The e-book provides a entire extension of the Bohr-Wheeler thought with the current wisdom of nuclear density distribution function.

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**Nuclear Fission And Cluster Radioactivity An Energy Density Functional Approach**

It's the first software to nuclear-physics from energy-density useful strategy, for which Professor Walter Kohn bought the Nobel Prize in Chemistry. The e-book offers a entire extension of the Bohr-Wheeler concept with the current wisdom of nuclear density distribution functionality.

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Phys. Rev. 141, 1146 (1966). 85. E. Johansson. Nucl. Phys. 60, 387 (1964). 86. F. L. W. Schmitt. Phys. Rev. C 6, 1023 (1972). 87. G. H. Gamel and L. Rosen. Los Alamos Report LA-1670 (1954) and L. Cranberg and N. Nereson, Los Alamos Report, LA-1916 (1955). 88. D. J. Swiatecki. Nucl. Phys. 81, 1 (1966). 89. S. Green. Phys. Rev. 95, 1006 (1954). 90. C. Wahl. J. Inorganic Nucl. Chem. 6, 262 (1953). 91. C. L. R. E. Troutner and K. Wolfsberg. Phys. Rev. 126, 1112 (1962). 92. W. Wapstra and G. Audi. Nucl.

Brenner, T. B. Malik (Springer Verlag, 1993) p. 273. 22 1 A Summary of Observed Data and Pre-Amble 79. M. F. Le-Du, D. Trubert, R. Bonetti, A. P. L. N. A. Ponomarenko. Pis’ma Zh. Eksp. Teor. Fiz. 62, 685 (1995). 80. A Oglobin, R. A. Denisov, A. G. Itkis, C. L. T. A. Pik-Pichak, G. M. M. A. K. P. Tretyakova. Phys. Rev. C 61, 034301 (2000). 81. E. Holden, 50 Years with Nuclear Fission eds. J. W. D. Carlson (American Nuclear Society, La Grange Park, IL 60525, 1989) 465. 82. J. B. Schwartz. Neutron Cross Sections, Supp.

It includes only the nuclear part of the matrix elements of the potential. 6) is also valid for Fmnα = Amn fnα (R). 9) one obtains the following expression for ﬁssion amplitude: Fmα (θ, ϕ) = Σn Amn fnα (θ, ϕ) . 10) The ﬁssion diﬀerential cross section for a parent nucleus in state, m, to a 2 is given by daughter pair in state, n, with asymptotic kinetic energy knα 2 Amn fnα (θ, ϕ) . 11) n In case, there is only one single dominant channel n, one may consider only one term in the summation and hence, the ﬁssion probability from a parent in state m to a daughter pair in state, n, is given by 2 |Amn fnα (θ, ϕ)| .