By A. A. Raduta, V. Baran, A. C. Gheorghe, I. Ursu
This quantity comprises the invited contributions that have been awarded on the Predeal foreign summer season tuition in Nuclear Physics 2006. It covers the new achievements within the fields of nuclear constitution, double beta decay, nuclear multifragmentation, kaon and dilepton construction in heavy ion collisions, and the quark-gluon plasma. The therapy is either theoretical and experimental, with emphasis at the collective facets and comparable section transitions. The papers are authored through many best researchers within the box.
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Extra info for Collective Motion and Phase Transitions in Nuclear Systems: Proceedings of the Predeal International Summer School Innuclear Physics, Predeal, Romania, 28 August-9 September 2006
Rev. 102,p. 788 (1956). P. Bizzeti and A. Bizzeti-Sona, in Nuclear Theory 05, ed. S . Dimitrova (Heron Press, Sofia, 2005). F. Iachello, Phys. Rev. Lett. 87, p. 052502 (2001). P. Bizzeti and A. Bizzeti-Sona, Phys. Rev. C 66,p. R031301 (2002). P. Lipas, Nucl. Phys. 40,p. 629 (1963). A. Tsvenkov, 3. Kvasil and R. Nazmitdinov, J. Phys. G 28, p. 2187 (2002). P. Bizzeti and A. Bizzeti-Sona, in Symmetries and low-energy phase transition in nuclear-structure physics, eds. G. L. Bianco and D. Balabanski (University of Camerino, Italy, 2005).
48 We denote with F1, F2, F3, F4, the corresponding integrands one needs to write the Euler-Lagrange equation: F3 = p2 ; F4 = p2F (7) The derivatives are easily obtained According to the calculus of variations the function p ( z ) minimizing the energy with two constraints should satisfy the Euler-Lagrange equation leading to - pI2 - (A1 + X2lzl + 6XVs)p(1 + p'2)3/2 - 1 = 0 pp" (13) if we choose F = IzI (hence f = lzl) and express 3&pe/(5n) as 6X because the Coulomb and surface energy of a spherical nucleus within LDM are given by EE = ( 3 Z 2 e 2 ) / ( 5 & ) and E: = 47rR37,respectively.
11 for 172Yb,where relevant data are available . In Fig. 12 the dynamic moment of inertia is plotted vs. the angular momentum. From this figure one notices that the results corresponding to even and those corresponding to odd angular momenta are lying on separate smooth curves as if these sets of states belonged to two distinct bands. The remark is valid for both the positive and negative parity bands. In order to see whether there are signatures of octupole deformation in 38 80 V I 1*, Th.