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Triaxiality in nuclei: Theoretical aspects S. Frauendorf Department of Physics University of Notre Dame, USA IKH, Forschungszentrum Rossendorf Dresden, Germany
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In collaboration with D. Almehed, UMIST V. Dimitrov, FZR, ND F. Doenau, FZR Ying-ye Zhang, UT
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Triaxial shell gaps
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A normal def. A large def. 165 190 134 105 80
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Phenomena in triaxial nuclei Wobbling Chiral vibrations Static chirality Tidal waves
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Wobbler types
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Collective Wobbler large
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Aligned Wobbler 1 3 High-j particle Increases with spin
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Tilted Wobbler High-j hole
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High-j particle, Irrotational flow MoI realignment with 2-axis
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Irrotational exchanged Cranking moments of inertia
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Matsuzaki, Shimizu, Matsuyanagi, PRC 65, 041303(R) (2002) RPA
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Wobbling (A=164) No collective wobbler Transition probablities Aligned wobbler Energies Tilted wobbler TAC in between Constant moment of inertia ?? Lower I in other mass regions (A=105,134,190) chirality__
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Chirality
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Dynamical (Particle Rotor) calculation Chiral vibration
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chiral vibration chiral rotation
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Chiral vibrator
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[8] K. Starosta et al., Physical Review Letters 86, 971 (2001)
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Transition probabilities
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out in out in yrast yrare
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yrast yrare out in
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Microscopic TAC calculations
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Consequence of chirality: Two identical rotational bands. (Static approximation)
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Chiral sister bands Representative nucleus observed13 0.21 14 13 0.21 40 13 0.21 14 predicted 45 0.32 26 observed 23 0.20 29 observed13 0.18 26 31/37
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Composite chiral bands
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Types of chirality
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Status of breaking of chiral symmetry Chiral mean field solutions do exist Chiral sister bands are seen Transition from chiral vibrations to rotations Transition matrix elements needed Sensitive to details Microscopic approach to dynamics needed
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“I call any geometrical figure, or group of points, chiral, and say it has chirality, if its image in a plane mirror, ideally realized, cannot brought to coincide with itself.” Kelvin, 1904, Baltimore lectures on Molecular Dynamics and Wave Theory of Light
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Chirality of molecules mirror The two enantiomers of 2-iodubutene
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carvon
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mirror Chirality of mass-less particles z
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Chirality “I call a physical object, chiral, and say it has chirality, if its image, generated by space inversion or time reversal, cannot brought to coincide with itself by a rotation.” 11/37
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Tidal wave
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High-spin waves Combination of Angular momentum reorientation Triaxial deformation
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yrast D. Cullen et. al
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25 26 27 28 29 30 Line distance: 20keV TAC
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Line distance: 200 keV
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Tidal wave Less favored vibrations Mixed with p-h excitations
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s ot i m K=25 i (130 ns) s o t m K=0 0 8 14 21 24 P. Chowdhury et al NPA 484, 136 (1988)
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First example of a triaxial tilted Tidal Wave 10 Phonons! Softness in shows up in isomer decay Large order amplitude phonons First phase transition
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Rotating mean field: Cranking model Seek a mean field solution carrying finite angular momentum. Use the variational principle with the auxillary condition The state |> is the stationary mean field solution in the frame that rotates uniformly with the angular velocity w about the z axis. In the laboratory frame it corresponds to a uniformly rotating mean field state
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Can calculate molecule Very different from
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p n
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