By A. A. Raduta, V. Baran, A. C. Gheorghe, I. Ursu
This quantity includes the invited contributions that have been awarded on the Predeal overseas summer season university in Nuclear Physics 2006. It covers the hot 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 elements and similar section transitions. The papers are authored by means of many major researchers within the box.
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Additional 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
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). W. Nazarewicz and P. Olanders, Nucl. Phys. A 441,p. 420 (1985). http://www. rice. edu/software/ARPA CK/.
7h. 218 Ra - - '81 w. Th 220 Ra 226 Ra (see Fig. 4. Experimental and calculated energies for the g* bands in 218,220,226Ra Ref. 173). energies is different from the J(J+l) pattern. The quality of the agreement between the theoretical results and the experimental energies can be best judged by plotting the dynamic moment of inertia which is a very sensitive function of the rotational frequency. Such a plot is shown in Fig. 6 for the pairs of bands g*, b+,y*. This graph indicates 226Raas the best candidate for a static octupole deformation in all three bands.
However, in many cases the excitation energies deviate drastically from the J ( J 1) law. If energies depend quadratically on J ( J l),the vanishing of the second order energy displacement function indicates that the second order derivative for energy with respect to J ( J 1) is the same for the two parity partner bands. 4 04 00 . r . 2 . 3 , . @*'* 0 F thrband 0 th f p band A ex @and A 20- el 0 0 00 z70- - f 40- 0 . 6 a. -- oo oo 00 e@ef) @ @ .. 4 ,ifw[Mevl T * , is plotted Fig. 6. The dynamic moment of inertia characterizing the bands g*, /I*, as function of the rotational frequency.
Collective Motion and Phase Transitions in Nuclear Systems: Proceedings of the Predeal International Summer School Innuclear Physics, Predeal, Romania, 28 August-9 September 2006 by A. A. Raduta, V. Baran, A. C. Gheorghe, I. Ursu