Rotation and alignment of high-j orbitls in transfermium nuclei

Slides:



Advertisements
Similar presentations
1 Effects of high-order deformation on high-spin structure in the heaviest nuclei accessible by spectroscopy experiments
Advertisements

Γ spectroscopy of neutron-rich 95,96 Rb nuclei by the incomplete fusion reaction of 94 Kr on 7 Li Simone Bottoni University of Milan Mini Workshop 1°-
Nuclear structure in the A~50 region Roberto V. Ribas Instituto de Física – USP XXVII RTFNB – Santos, 2004.
Projected-shell-model study for the structure of transfermium nuclei Yang Sun Shanghai Jiao Tong University Beijing, June 9, 2009.
High spin states in 136,137 La, 148 Ce and 105 Mo.
I. Bentley and S. Frauendorf Department of Physics University of Notre Dame, USA Calculation of the Wigner Term in the Binding Energies by Diagonalization.
Nuclear models. Models we will consider… Independent particle shell model Look at data that motivates the model Construct a model Make and test predictions.
The Shell Model of the Nucleus 5. Nuclear moments
Structure of Be hyper-isotopes Masahiro ISAKA (RIKEN) Collaborators: H. Homma and M. Kimura (Hokkaido University)
The stability of triaxial superdeformed shape in odd-odd Lu isotopes Tu Ya.
5. Exotic modes of nuclear rotation Tilted Axis Cranking -TAC.
Structures of Exotic 131,133 Sn Isotopes for r-process nucleosynthesis Shisheng Zhang 1,2 ( 张时声 ) 1. School of Physics and Nuclear Energy Engineering,
Shell Model based deformation analysis of light Cadmium isotopes T. Schmidt 1, A. Blazhev 1, K. Heyde 2, J. Jolie 1 1 Institut für Kernphysik, Universität.
Rotation and alignment of high-j orbitls in transfermium nuclei Dr. Xiao-tao He College of Material Science and Technology, Nanjing University of Aeronautics.
4. The rotating mean field. The mean field concept A nucleon moves in the mean field generated by all nucleons. The mean field is a functional of the.
High-spin structures in the 159 Lu nucleus Jilin University, China Institute of Atomic Energy 李聪博 The 13th National Nuclear Structure Conference of China.
1 In-Beam Observables Rauno Julin Department of Physics University of Jyväskylä JYFL Finland.
Structure of neutron-rich A~60 nuclei: A theoretical perspective Yang Sun Shanghai Jiao Tong University, China KAVLI-Beijing, June 26, 2012.
Isospin and mixed symmetry structure in 26 Mg DONG Hong-Fei, BAI Hong-Bo LÜ Li-Jun, Department of Physics, Chifeng university.
The excitation and decay of nuclear isomers Phil Walker CERN and University of Surrey, UK 3. Isomers at the limits of stability ● p decay ● n decay ● α.
POPULATION OF GROUND-STATE ROTATIONAL BANDS OF SUPERHEAVY NUCLEI PRODUCED IN COMPLETE FUSION REACTIONS A.S. Zubov, V.V. Sargsyan, G.G. Adamian, N.V.Antonenko.
The Highs and Lows of the A~100 Region Paddy Regan Dept. of Physics, University of Surrey, UK and WNSL, Yale University, New Haven, CT
Coupling of (deformed) core and weakly bound neutron M. Kimura (Hokkaido Univ.)
Spontaneous symmetry breaking and rotational bands S. Frauendorf Department of Physics University of Notre Dame.
Erosion of N=28 Shell Gap and Triple Shape Coexistence in the vicinity of 44 S M. KIMURA (HOKKAIDO UNIV.) Y. TANIGUCHI (RIKEN), Y. KANADA-EN’YO(KYOTO UNIV.)
Symmetries and collective Nuclear excitations PRESENT AND FUTURE EXOTICS IN NUCLEAR PHYSICS In honor of Geirr Sletten at his 70 th birthday Stefan Frauendorf,
ShuangQuan Zhang School of Physics, Peking University Static chirality and chiral vibration of atomic nucleus in particle rotor model.
Saclay, 30 January 2007 Rauno Julin Department of Physics University of Jyväskylä FinlandJYFL In-beam Spectroscopy of In-beam Spectroscopy of Transfermium.
July 29-30, 2010, Dresden 1 Forbidden Beta Transitions in Neutrinoless Double Beta Decay Kazuo Muto Department of Physics, Tokyo Institute of Technology.
Furong Xu Rotations of multi-quasiparticle high-K states 北京大学 Peking University Outline I.Introduction II.Rotations built on excited configurations Deformation-pairing.
Some (more) High(ish)-Spin Nuclear Structure Paddy Regan Department of Physics Univesity of Surrey Guildford, UK Lecture 2 Low-energy.
Shape evolution of highly deformed 75 Kr and projected shell model description Yang Yingchun Shanghai Jiao Tong University Shanghai, August 24, 2009.
Symmetries of the Cranked Mean Field S. Frauendorf Department of Physics University of Notre Dame USA IKH, Forschungszentrum Rossendorf, Dresden Germany.
The i 13/2 Proton and j 15/2 Neutron Orbital and the SD Band in A~190 Region Xiao-tao He En-guang Zhao En-guang Zhao Institute of Theoretical Physics,
Congresso del Dipartimento di Fisica Highlights in Physics –14 October 2005, Dipartimento di Fisica, Università di Milano Contribution to nuclear.
How do nuclei rotate? 3. The rotating mean field.
Production mechanism of neutron-rich nuclei in 238 U+ 238 U at near-barrier energy Kai Zhao (China Institute of Atomic Energy) Collaborators: Zhuxia Li,
Nordita Workshop on chiral bands /04/2015 Multiple chiral bands associated with the same strongly asymmetric many- particle nucleon configuration.
超重原子核的结构 孙 扬 上海交通大学 合作者:清华大学 龙桂鲁, F. Al-Khudair 中国原子能研究院 陈永寿,高早春 济南,山东大学, 2008 年 9 月 20 日.
A microscopic investigation on magnetic and antimagnetic rotations in 110 Cd Jing Peng Beijing Normal University Collaborators:P.W.Zhao, Jie Meng, and.
1 Jeff Tostevin, Department of Physics Faculty of Engineering and Physical Sciences University of Surrey, United Kingdom Sensitivity of two-nucleon knockout.
Determining Reduced Transition Probabilities for 152 ≤ A ≤ 248 Nuclei using Interacting Boson Approximation (IBA-1) Model By Dr. Sardool Singh Ghumman.
The role of isospin symmetry in medium-mass N ~ Z nuclei
Content of the talk Exotic clustering in neutron-rich nuclei
Shape parameterization
Tutor: Prof. Yang Sun (孙扬 教授)
Nuclear structure of lowest 229Th states
Structure and dynamics from the time-dependent Hartree-Fock model
Evolution of octupole collectivity in 221Th
Emmanuel Clément IN2P3/GANIL – Caen France
Isospin Symmetry test on the semimagic 44Cr
Nuclear masses of neutron-rich nuclei and symmetry energy
Deformed relativistic Hartree Bogoliubov model in a Woods-Saxon basis
Hiroshi MASUI Kitami Institute of Technology
Isomers and shape transitions in the n-rich A~190 region:
Nuclear Chemistry CHEM 396 Chapter 4, Part B Dr. Ahmad Hamaed
Lecture 5-6 xxxxxxx.
Introduction Calculations for the N=7 isotones Summary
(Lawrence Berkeley National Laboratory)
a non-adiabatic microscopic description
Symmetry energy coefficients and shell gaps from nuclear masses
High spin physics- achievements and perspectives
Nuclei at the Extremes of Spin: The Superdeformed Bands in 131,132Ce
Kazuo MUTO Tokyo Institute of Technology
第十四届核结构会议,2012年4月11-16,湖州师范学院
An improved nuclear mass formula
Shape-coexistence enhanced by multi-quasiparticle excitations in A~190 mass region 石跃 北京大学 导师:许甫荣教授
V.V. Sargsyan, G.G. Adamian, N.V.Antonenko
Department of Physics, Sichuan University
Probing correlations by use of two-nucleon removal
Presentation transcript:

Rotation and alignment of high-j orbitls in transfermium nuclei Dr. Xiao-tao He College of Material Science and Technology, Nanjing University of Aeronautics and Astronautics Huzhou • China,2012,04,12-16

Motivation Exploration of the island of stability with high mass and charge, i.e. the region of superheavy elements (SHE) has been one of the fundamental questions in nature science !

α-decays: life time, spin, parity … … Motivation How to get structure information about superheavy elements (SHE) ? α-decays: life time, spin, parity … … Spectroscopy of collective rotation: spin, parity, configurations, deformations, single-particle orbiting … … ! Difficulty: The extremely low production cross-sections. It can rarely reveal the detailed spectroscopic information of SHE in the experiments. Tansfermium nuclei (Z > 100) are the heaviest system accessible in present in-beam experiment.

Motivation The study of these deformed transfermium nuclei may provide an indirect way to access the single particle states of the next closed spherical shells. ε2=0.30 100 102 ε2=0.25

Some experimental results Even-even nuclei: 254No β2=0.27±2 P. Reiter, et al., PRL82 (1999) 509.

252No β2=0.28±2 Even-even nuclei: Rotational Band R.-D. Herzberg, et al., PRC, 65 (2001) 014303

250Fm β2=0.28±2 Even-even nuclei: Rotational Band J. E. Bastin, et al., PRC 73 (2006) 024308.

253No Odd-neutron nuclei: Rotational Band R.-D. Herzberg, et al., Eur. Phys. J. A 15, 205 (2002) P. Reiter, et al., PRL 95, 032501 (2005). R.-D. Herzberg, et al., Eur. Phys. J. A 42, 333 (2009).

251Md Odd-proton nuclei: This band: 1/2[521] Rotational Band Odd-proton nuclei: 251Md This band: 1/2[521] Ground state band: 7/2[514] A. Chatillon, et al., PRL 98, 132503 (2007).

Rotational Band Odd-proton nuclei: 255Lr The structures are tentatively assigned to be based on the 1/2[521] and 7/2[514] Nilsson states, respectively. S. Ketelhut, et al., PRL 102, 212501 (2007).

High-K structure R.D. Herzberg et al., Nature 442 (2006) 896

250Fm High-K structure B. Sulignano, et al., EPJA 33 (2007) 327. P. T. Greenlees, et al., PRC 78 (2008) 021303

the ground-state configuration in 257Rf is 1/2+[620]. High-K structure 11/2−[725] the ground-state configuration in 257Rf is 1/2+[620]. H. B. Jeppesen,et al., PRC 79, 031303(R) (2009). J. Qian, et.al., PRC 79, 064319 (2009).

High-K structure Odd-proton nuclei: 255Lr Assuming the quadrupole deformation of the band to be β2 = 0.3 (typical for nuclei in this region). the lowest observed sequence is built upon the [624]9/2+ Nilsson state. H. B. Jeppesen, et al., PRC 80, 034324 (2009).

Theoretical study Cranked Shell Model single particle part : H0 with Particle number conserving method treatment for the pairing correlation: Hp

Theoretical study In rotating frame: HCSM is diagonalized in the Cranked Many-Particle Configuration (CMPC) space, we get the solution of CSM Hamiltonian: Di:Real

The angular momentum alignment in : Theoretical study The angular momentum alignment in : Kinematic MoI: Dynamic MoI:

Parameters The Nilsson parameters (κ,μ) are taken from: Theoretical study Parameters The Nilsson parameters (κ,μ) are taken from: S.G. Nilsson, et al., Nucl. Phys. A131 (1969) 1. * The deformation parameters ε2 =0.29 , ε4=0.02 for 252,253,254No and 250Fm, ε2 =0.30 , ε4=0.02 for 251Md. The effective pairing interaction strengths (in unite of MeV), G0p=0.45, G0n=0.35, G2p=0.02, G2n=0.02 * Proton: Ecut : 0.60 ω0 CMCP space ~ 1000 Neutron: Ecut : 0.50 ω0 CMCP space ~ 1000 通过拟合Z=96-103(A=240-255)的30多个原子核的带头能量以及转动惯量,确定了一组主量子数,轨道角动量量子数依赖的(κ,μ) Zhen-Hua Zhang et al., Phys. Rev. C 85, 014324 (2012); 83, 011304 (2011).

Theoretical results Even-even nuclei: Experimental and theoretical J(1) of the bands in 250Fm, 252No and 254No.

Odd-proton nuclei 251Md Theoretical results ε2=0.30

Theoretical results

The cranked proton Nilsson orbitals near the Fermi surface in 251Md Theoretical results The cranked proton Nilsson orbitals near the Fermi surface in 251Md

Odd-neutron nuclei 253No: Theoretical results

Summary * The observed bands are reproduced very well by the theoretical results. * Exploration of behaviors of these bands at high spin shows that there is backbending taking place at hω ≈ 0.275 MeV in bands of 252,253,254No. * α = −1/2 band in 251Md is predicted. It is very encouraged to find that there is a backbending occurring at very low frequency, hω ≈ 0.15 MeV,which might be during the possible observed frequency. * The neutron 2h11/2 (1/2[761]) and proton 1j15/2 (1/2[770]) orbitals play a very important role in the rotational properties of transfermium nuclei.

Thank you ! Thank you !

Welcome to Nanjing !

Thank you !

Thank you !

Theoretical results The total angular momentum alignment <Jx>, and the separate contributions to <Jx> from neutron and proton in 251Md.

Theoretical results The contributions to <Jx> from the particle in each proton cranked orbitalμ, jx(μ) and the interference term jx(μν) between cranked orbitals μ and ν for the 7/2+[624] band in 253No, which are simply denoted by μ and μν, respectively.

Theoretical results Nilsson S G et al., NPA, 131 (1969) 1.

Theoretical results Nilsson S G et al., NPA, 131 (1969) 1.

Theoretical results Nilsson S G et al., NPA, 131 (1969) 1.

Theoretical results Nilsson S G et al., NPA, 131 (1969) 1.

Theoretical results Nilsson S G et al., NPA, 131 (1969) 1.

Theoretical results Nilsson S G et al., NPA, 131 (1969) 1.

Theoretical results

Theoretical results T. Bengtsson, I. Ragnarsson, NPA436 (1985) 14-82

Theoretical results T. Bengtsson, I. Ragnarsson, NPA436 (1985) 14-82

rotation and alignment of high-j orbitls in transfermium nuclei Dr. Xiao-tao He College of Material Science and Technology, Nanjing University of Aeronautics and Astronautics Prof. Zhong-zhou Ren Department of Physics, Nanjing University Prof. En-guang Zhao Institute of Theoretical Physics, Chinese of Academy of Sciences. Prof. Shu-xin Liu & Jin-yan Zeng School of Physics, Peking University Chifeng • China,2010,07,25-31

Theoretical study Odd-mass transfermium nuclei are seldom studied; Cranked shell model are seldom used. We used the cranked shell model to calculate the collective rotation of SHE. Collective rotational bands provide important testing ground to check the extrapolations of current models to SHE region!