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4. Rotation about a tilted axis and reflection asymmetry
How do nuclei rotate? 4. Rotation about a tilted axis and reflection asymmetry
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discrete symmetries for
reflection symmetric shapes
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Small E Triaxial rotor Classical motion of J Uniform rotation only about the principal axes! Large E
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inertial ellipsoid molecule nucleus
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The nucleus is not a simple piece of matter, but more like a clockwork of gyroscopes. 5/23
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Tilted bands contain all spins (no signature selection rule).
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Rotational bands in 1 1’ 2 3 4 7
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Vacuum drives moderately toward 90
2 3 1’ 4 1 4 4
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Vacuum drives strongly toward 90
3 1’ 2 7 1 4 7 4 7 4
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Fixed K-approximation in CSM
Simplifying assumptions: Comparison with calculations like for PAC. Nice, simple, and very popular. 10/23
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New possibility For triaxial nuclei. Principal Axis Cranking
PAC solutions Tilted Axis Cranking TAC or planar tilted solutions Chiral or aplanar solutions Doubling of states New possibility For triaxial nuclei.
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Chirality It is impossible to transform one configuration
into the other by rotation. mirror
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mirror mass-less particles
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Time reversal not reflection!
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Examples for chiral sister bands
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Left-right tunneling Breaking of chiral symmetry is not very strong.
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Dynamical (Particle Rotor) calculation
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Reflection asymmetric shapes, two reflection planes
Simplex quantum number Parity doubling 20/23
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Summary The different discrete symmetries of the m.f. are manifest by different level sequences in the rotational bands. For reflection symmetric shapes, a band has fixed parity and one has: Rotation about a principal axis (signature selects every second I) Rotation about an axis in a principal plane (all I) Rotation about an axis not in a principal plane (all I, for each I a pair of states – chiral doubling) For reflection asymmetric shapes, a band contains both parities. If the rotational axis is normal to one of two reflection planes the bands contain all I and the levels have alternating parity. For reflection asymmetric shapes exists 16 different symmetry types.
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