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By A. C. Mueller, M. Mirea, L. Tassan-Got

This booklet covers new experimental and theoretical reviews that target the fashionable advancements of nuclear fission, aiming at a number of functions in a variety of fields and bringing jointly scientists operating in numerous fields relating to nuclear fission. the subsequent issues are handled: radioactive beam amenities in keeping with nuclear fission; nuclear waste transmutations and the longer term accelerator-driven process; fission and spallation nuclear information and modeling: experimental and theoretical advances within the research of nuclear fission; fusion reactions and rot modes of superheavy nuclei; balance opposed to fission and many-body structures; superasymmetric and multicluster fission.

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Additional resources for Proceedings of the International Workshop on the New Applications Of Nuclear Fission: Bucharest, Romania, 7-12 September 2003

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For realistic calculations of fission dynamics, we employ a multi-dimensional Langevin equation which is equivalent to Kramers equation and easy to solve numerically 10,11 . dpi dV 1 d -^- = - g - ~ 2 a r ( — = (m lij )ijPj, m ! _x )ikPjPk ~ Uj (m )jkPk + 9ijRj (t), (2) T = gikQjk, where repeated indices are assumed to sum up. V(q) is the potential energy, which is calculated as the sum of a generalized surface energy, a Coulomb energy for diffused surface and a centrifugal potential. The tensors rriij and jij denote the inertia mass and the friction tensors, respectively.

J. , Ann. Phys. (NY) 113 330 (1978). 14. Y. Abe, Proc. 3rd IN2P3-RIKEN symp. on Heavy Ion Collisions, Tokyo, Oct. 1994 (World Scientific, 1995) p. 127. 15. P. Paul and M. Thoennessen, Ann. Rev. Nucl. Part. Sci. 44 65 (1994). 16. D. N. Nadtocky, Physics of Atomic Nuclei 66 618 (2003). 17. M. , Nucl. Phys. A630 200 (1998). 18. J. Swiatecki, Physica Scripta 24 113 (1981). 19. E. Gross and H. Kalinowski, Phys. Reports C45 175 (1978). 20. K. , Z. Phys. A288 383 (1978). 21. D. Bao, D. Boilley and Y. Abe, to be published.

The resulting spectrum obtained after the background subtraction is shown in Fig. 3. The energy region around 3368 keV now has a clear zero. In 45 1 20 37 15 -_4 :! ; 2 Z\ . rir ~* A riT' . , i . 3100 . • . n. iU^-U-jJl'dt J;;j ! I i i -,iA':'' '' 1 ! j i : ' ! x • ^ • " , ... bP ! r M": fi U Hirr^-rf-i": rn 4 '4 1 1 1 1 1 1 I 3200 3300 . V i L_i I_I . ^Ti' • • 1—i i t ,,.. i q- ; ' i 1 i J 1 1 1 1 1 1 11 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 Figure 2: Histogram drawn with a dotted line shows the spectrum of y rays coinciding with Be LCPs.

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