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Yu Zhang(张宇), Feng Pan(潘峰)
Nucleon shape phase transition at the nucleon level within SD-pair shell model Yanan Luo(罗延安), Lei Li(李磊) School of Physics, Nankai University, Tianjin Yu Zhang(张宇), Feng Pan(潘峰) Department of Physics, Liaoning Normal University, Dalian J. P. Draayer Department of Physics and Astronomy, LSU, BTR Lanzhou, Sept.6, 2015
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Outline I. Nuclear Shapes and Shape Phase Transition
II. Status of the Research on the nuclear shape Phase Transition III. SD-pair shell model(SDPSM) IV. Nuclear shapes in SD-pair shell model V. Nucear shape phase transition in SD- pair shell model VI. Summary
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I. Nuclear Shape-Phases and Shape-Phase Transition
Modes of nuclear collective motion and the symmetries Shape of Nucleus Sphere Deforemation quadrupole octupole hexadecupole Modes of Nuclear Collective Motion vibration axial rotation ( prolate, oblate) -soft rotation triaxial rotation ••• ••• ••• ••• From Prof. Yuxin Liu
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Correspondence between collective motion and symmetry
Vibration U(5) Axial Rotation SU(3) ( SU*(3)) γ-soft rotation O(6) Shape Phase Transition and the States at the Critical Points of the Phase Transitions Vibration – γ-soft Rotation E(5) Vibration – Prolate Axial Rotation X(5) Prolate – Oblate Axial Rotations Y(5)
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Iachello, PRL 91, (’03)
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The shape-phase transition in the U(5)-SU(3) transitional region
X(5) SU(3) Harmonic Vibrator Soft Liquid-drop Rigid Rotor
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II. Status of the research on nuclear shape phase transition
System: Even-even nuclei, Odd-even nuclei, Odd-odd nuclei Theoretical method: IBM, IBFM, IBFFM Geometric Collective models Fermionic approaches FDSM, shell model, HFB ••••••••••••
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The most useful observables
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Two neutron seperation energies
E0 transition Isotopes shifts Two neutron transfer cross sections ……………….
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III. SD-pair shell model(SDPSM)
Because of the success of the IBM, the full space was truncated into SD-pair subspace, r=0, 2 The Hamiltonian can be diagonolized directly in the Fermion space!
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All one and two-body matrix elements
can be expressed in terms of overlap For eg.
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The overlap between two N-pair basis
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The new pair structure coefficient
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The hierarchy of various nuclear model
SDPSM NPSM
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IV. Nuclear shape phases in SDPSM
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Rotational spectrum
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V. Nuclear shape phase transition in SDPSM
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Vibration to rotational transitional pattern
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Liu YX, et. al., Phys. Lett. B688,298(2010)
Boson Mapping (Dyson) It is found that the nuclear shape phase transitional pattern can be Produced by changing the interactional strength! Problem: is it true without Bosonization approximation?
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The Hamiltonian used in the SD-pair shell model
Toy case: N=9 oscillator shell
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The effect of monopole pairing interaction
Quadrupolel-quadrupole interactional strength kappa
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The effect of quadrupole-quadrupole interaction
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Summary The nuclear shape phases can be produced very well in the SDPSM The nulcear shape phase transitional pattern as in the IBM can be produced in the SDPSM The properties of the critical symmetry can be produced in the SDPSM
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Thanks !
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Spectrum of E(5) Spectrum of X(5) Spectrum of Y(5) Symmetry Symmetry Symmetry
( Iachello, PRL 85, 3580 (2000) ) ( Iachello, PRL 87, (2001)) ( Iachello, PRL 91, (2003)) 134Ba, 108Pd, 130Xe, ··· Sm, 154Gd, 156Dy, 150Nd, ··· Er, 168Er, ··· ( Casten, PRL 85, 3584 (2000); ( Casten, PRL 87, (2001); (PRC 68 , (2003); … Ginocchio, PRL 90, (2003) ; Capirio, PRC 66, (2002); Liu, PRC 65, (2002), … ) Tonev, PRC 69, (2004); …)
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Characteristic of Evolution of Energy Spectrum for the
Transition from U(5) to SU(3) Through X(5) SU(3) (Rotation) X(5) U(5) (Vibration) ( Pan, Draayer, et. al., PLB 576, 297 (2003) )
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Summary for the shape-phase transition in the U(5)-SU(3) transitional region
Harmonic Vibrator Soft Liquid-drop Rigid Rotor
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Extension: Unified description of the shape phase structure and
phase transition of odd-A nuclei F. Iachello, Phys. Rev. Lett. 95, (2005); Result of U(6,4) model 135Ba, E(5/4) Symmetry, M.S. Fetea, et al., Phys. Rev. C 73, (2005)
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Nuclear shape-phase and phase transition in IBM-2
M. A. Caprio and F. Iachello,Phys. Rev. Lett. 93, (2004)
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