Title: Exotic Nuclear Shapes
1Exotic Nuclear Shapes
I 0 T 0
I gtgt 1 T gt 0
- Nicolas Schunck
- Departamento de Fisica Teorica,
- Universidad Autonoma de Madrid
- Cantoblanco 28049, Madrid, Spain
2Standard Nuclear Shapes
- Types of nuclear shapes
- Spherical
- Prolate
- Oblate
- Tri-axial
- Pear-shape
3Point Symmetries in the Microscopic World
- Synthetic inorganic-organic compound with ZnO4
tetrahedral clusters linked by C6H4-C-O2 struts
(Li, Nature, 1999). - 1.29 nm spacing between centers of adjacent
clusters.
4Point Symmetries and Nuclear Stability
- Shell Gaps ? Stable configurations
- In nuclei Higher degeneracies ? Larger
shell gaps
Degeneracies are a direct consequence of the
underlying point symmetry of the shape
5Point Groups and Level Degeneracy
Survey of the properties of a few point groups
6Symmetry Groups Td and Oh
- Parameterization of the shape symmetries
- Tetrahedral a32 ? 0
- Octahedral a40, a44 ? 0
- Other possibilities involving higher order
multipoles a?µ
7Tetrahedral Shell Gaps
8Tetrahedral Shell Effects
9Neutron-rich Zr Isotopes
10Tetrahedral Magic Numbers
- From a WS potential
- 20, 32, 40, 56-58, 64, 70, 90, 100, 112,
- Existence of Td magic numbers independent of the
realization of the mean-field
Universality
Yb isotopes
Zr isotopes
Best candidates proton-rich or neutron-rich
nuclei
11Experimental signatures (1/2)
- Stable tetrahedral minimum Shape isomer
- Low-spin physics dont expect I gt 10 h
- Possibly high excitation energy
- Static octupole moment Q3
- No dipole moment
12Experimental signatures (2/2)
- Weak collective rotation
- Yrast traps with parity doublet ? (because of
parity-breaking) - Bunch of quasi-particle excitations (because of
the 4-fold degeneracy of s.p. levels) - Investigations under way
- RPA (Strasbourg)
- GCM (Warsaw)
- Spectroscopy with point symmetries (Lublin)
13Summary (for Part I)
- Mean-field Theories predict tetrahedral
configurations in islands of nuclei throughout
the nuclear chart - Low-lying states (by opposition to cluster
states) - New types of shape coexistence prolate, oblate,
spherical, tetrahedral, octahedral, pear-shaped,
etc. - The best candidates will be found away from the
valley of stability
The nuclear tetrahedral symmetry reflects the
quantal nature of the nucleus (always competing
with the macroscopic, liquid-drop aspects)
14Deformed nuclei in motion
Consequence of the breaking of the rotational
invariance deformed nuclei can rotate
Example of a super-deformed rotational band
Jacobi Shape transition
15The Jacobi Shape Transition
Example of the Jacobi shape transition in 152Dy
16The various forms of the Jacobi transition
Instability of the Jacobi transition leading to
fission
17Jacobi transition and Hyper-deformation
Liquid drop High-temperature Limit
18Hyper-deformed configurations
- Neat Jacobi Transition a prerequisite for
populating SD and HD states - Mean-field at the limits
- Single-particle structure
- Effective interaction
- Jacobi Shapes and many-body problem
19Summary (Part II)
- Hyper-deformation (and Jacobi shapes) can be
observed only at very high angular momentum - Short spin-window in-between the Jacobi
transition and fission - Mass A 100 among the best candidates
The Jacobi shape transition reflects the
macroscopic, liquid-drop nature of the nucleus
(always competing with the quantal aspects)
20Collaboration Network
- IReS-ULP, Strasbourg, France
- Institute of Theoretical Physics, Warsaw
University, Poland - University Marie Curie-Sklodowska, Lublin, Poland
- University of Notre Dame, USA
- Université Libre de Bruxelles, Bruxelles, Belgium
- University of Surrey, Guildford, UK
- Niels Bohr Institute, Copenhagen, Denmark
- Henrik Niewodniczanski Institute of Nuclear
Physics, Kraków, Poland
21Bibliography
- X. Li, J. Dudek, Phys. Rev. C49 (1994) 1250(R)
- S. Takami , K. Yabana, M. Matsuo, Phys. Lett.
B431 (1998) 242-248 - M. Yamagami, K. Matsuyanagi, M. Matsuo, Nucl.
Phys. A693 (2001) 579-602 - J. Dudek, A. Gózdz, N. Schunck and M. Miskiewicz,
Phys. Rev. Lett. 88 (2002) 252502 - J. Dudek, A. Gózdz and N. Schunck, Act. Phys.
Pol. B34 2491 (2003) - N. Schunck, J. Dudek, A. Gózdz, P. Regan, Phys.
Rev. C69 (2004) 061305(R)