THE SHAPE TRANSITION IN ROTATING NUCLEI F. Ivanyuk 1, K. Pomorski 2 and J.Bartel 3 1 Institut for Nuclear Research, Kiev, Ukraine 2 Theoretical Physics Division, UMCS, Lublin, Poland 3 Institute Pluridisciplinaire Hubert Curien, Strasbourg University, Strasbourg, France Introduction The Strutinsky‘s procedure for the shape of fissioning nuclei The shape transition in axially symmetric rotating charged liquid drop The shape of triaxial rotating drop Summary and outlook
Strutinsky‘s optimal shapes V.M.Strutinsky et al, Nucl. Phys. 46, 659 (1963)
Optimal shapes of fissioning drop
The deformation energy F. Ivanyuk, Int. J. Mod. Phys. E18 (2009) 130
The shape of axially symmetric rotating drop J. Bartel, F. Ivanyuk and K.Pomorski, Int. Jour. Mod. Phys. E19 (2010) 601
The energy and shape transition in axially symmetric rotating drop
The deformation energy of rotating drop
The energy and shape transition in axially symmetric rotating drop
The shape transition in rotating drop
The energy and shape transition in axially symmetric rotating drop
The critical rotational velocities
The non-axial rotating drops K. Pomorski, F. Ivanyuk and J. Bartel, Acta Phys. Polon. B42 (2011) 455 A. May, K. Mazurek, J. Dudec, M. Kmiecik and D. Rouvel, Int. J. Mod. Phys. E19 (2010) 532
The equations for
The shape of axially non-symmetric rotating drop
The energy of axially non-symmetric rotating drop
The comparison with ellipsoidal shapes
The effective ellipsoids
The effective ellipsoids, the energy
The limiting values of rotational velocity
Summary and outlook Within a liqiud drop model we have developed a method for the calculation of optimal shape of the surface within a broad region of rotational velocitiy and fissility parameter We have found out that sharp Jacobi transition from oblate to triaxiall ellipsoides is the result of limitation imposed by the assumption of the ellipsoidal shape For the more flexible shape parmeterisation the Jacobi transition gets smoothed For the drops with the fissility parameter x LD >0.612 the fission takes place before the Jacobi transition The investigation of Poincare instability will be the subject of future studies
Thank you for attention
The barrier heights, topographical theorem W. D.Myers and W. J. Swiatecki, Nucl. Phys. A601, 141 (1996): the “barrier will be determined by a path that avoids positive shell effects and has no use for negative shell effects. Hence the saddle point energy will be close to what it would have been in the absence of shell effects, i.e., close to the value given by the macroscopic theory!” F.A.Ivanyuk and K.Pomorski, Phys: Rev. C 79, (2009)