EXOTIC NUCLEAR STRUCTURE PHENOMENA the complex EXCITED VAMPIR approach

Slides:



Advertisements
Similar presentations
A brief introduction D S Judson. Kinetic Energy Interactions between of nucleons i th and j th nucleons The wavefunction of a nucleus composed of A nucleons.
Advertisements

Coulomb excitation with radioactive ion beams
HL-3 May 2006Kernfysica: quarks, nucleonen en kernen1 Outline lecture (HL-3) Structure of nuclei NN potential exchange force Terra incognita in nuclear.
Electromagnetic Properties of
How do nuclei rotate? 5. Appearance of bands. Deformed mean field solutions This is clearly the case for a well deformed nucleus. Deformed nuclei show.
II. Spontaneous symmetry breaking. II.1 Weinberg’s chair Hamiltonian rotational invariant Why do we see the chair shape? States of different IM are so.
Structure of odd-odd nuclei in the interacting boson fermion-fermion model 3.
NPSC-2003Gabriela Popa Microscopic interpretation of the excited K  = 0 +, 2 + bands of deformed nuclei Gabriela Popa Rochester Institute of Technology.
Nuclear Low-lying Spectrum and Quantum Phase Transition Zhipan Li School of Physical Science and Technology Southwest University 17th Nuclear Physics Workshop,
NUCLEAR STRUCTURE PHENOMENOLOGICAL MODELS
Introduction to Nuclear Physics
5. Exotic modes of nuclear rotation Tilted Axis Cranking -TAC.
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.
Lecture 20: More on the deuteron 18/11/ Analysis so far: (N.B., see Krane, Chapter 4) Quantum numbers: (J , T) = (1 +, 0) favor a 3 S 1 configuration.
Chirality of Nuclear Rotation S. Frauendorf Department of Physics University of Notre Dame, USA IKH, Forschungszentrum Rossendorf Dresden, Germany.
Hypernuclear Production with Hadronic and Electromagnetic Probes Radhey Shyam Saha Institute of Nuclear Physics, Kolkata, India Z.Zt. Institut f. Theo.
Nuclear Structure and dynamics within the Energy Density Functional theory Denis Lacroix IPN Orsay Coll: G. Scamps, D. Gambacurta, G. Hupin M. Bender and.
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.
ESNT Saclay February 2, Structure properties of even-even actinides at normal- and super-deformed shapes J.P. Delaroche, M. Girod, H. Goutte, J.
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.)
Application of the Adiabatic Self-Consistent Collective Coordinate (ASCC) Method to Shape Coexistence/ Mixing Phenomena Application of the Adiabatic Self-Consistent.
Quantum Phase Transitions (QPT) in Finite Nuclei R. F. Casten June 21, 2010, CERN/ISOLDE.
Modification of nucleon spectral function in the nuclear medium from QCD sum rules Collaborators: Philipp Gubler(ECT*), Makoto Oka Tokyo Institute of Technology.
E. Sahin, G. de Angelis Breaking of the Isospin Symmetry and CED in the A  70 mass region: the T z =-1 70 Kr.
Nuclear Isovector Equation-of-State (EOS) and Astrophysics Hermann Wolter Dep. f. Physik, LMU Topics: 1.Phase diagram of strongly interacting matter and.
Héloïse Goutte CERN Summer student program 2009 Introduction to Nuclear physics; The nucleus a complex system Héloïse Goutte CEA, DAM, DIF
Variational approach to isospin symmetry breaking in medium mass nuclei A. PETROVICI Institute for Physics and Nuclear Engineering, Bucharest, Romania.
第十四届全国核结构大会暨第十次全国核结构专题讨论会
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.
How do nuclei rotate? 3. The rotating mean field.
Nordita Workshop on chiral bands /04/2015 Multiple chiral bands associated with the same strongly asymmetric many- particle nucleon configuration.
Nuclear Low-lying Spectrum and Quantum Phase Transition 李志攀 西南大学物理科学与技术学院.
Rotational energy term in the empirical formula for the yrast energies in even-even nuclei Eunja Ha and S. W. Hong Department of Physics, Sungkyunkwan.
Pairing Correlation in neutron-rich nuclei
Determining Reduced Transition Probabilities for 152 ≤ A ≤ 248 Nuclei using Interacting Boson Approximation (IBA-1) Model By Dr. Sardool Singh Ghumman.
Workshop Spiral II - Caen 4-6th October 2005
The role of isospin symmetry in medium-mass N ~ Z nuclei
Content of the talk Exotic clustering in neutron-rich nuclei
Shape parameterization
Nuclear structure far from stability
Université de Caen Basse-Normandie
Probing Nuclear Skins through Density Form Factors
Bubble structures in exotic nuclei
Nuclear structure of lowest 229Th states
Zao-Chun Gao(高早春) China Institute of Atomic Energy Mihai Horoi
Structure and dynamics from the time-dependent Hartree-Fock model
mesons as probes to explore the chiral symmetry in nuclear matter
Low energy nuclear collective modes and excitations
Evolution of octupole collectivity in 221Th
Emmanuel Clément IN2P3/GANIL – Caen France
Exotic nuclei beyond 132Sn: where do we stand?
Introduction to Nuclear physics; The nucleus a complex system
Systematic study of Z = 83 nuclei: 193,194,195Bi
Isospin Symmetry test on the semimagic 44Cr
Nuclear Chemistry CHEM 396 Chapter 4, Part B Dr. Ahmad Hamaed
Introduction Calculations for the N=7 isotones Summary
Kernfysica: quarks, nucleonen en kernen
Nuclear excitations in relativistic nuclear models
Nuclear Forces - Lecture 2 -
Daisuke ABE Department of Physics, University of Tokyo
Single particle states
UWC Beyond mean-field: present and future
Cluster and Density wave --- cluster structures in 28Si and 12C---
Nuclear shapes for the critical point
Di-nucleon correlations and soft dipole excitations in exotic nuclei
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
How do nuclei rotate? 5. Appearance of bands.
II. Spontaneous symmetry breaking
Presentation transcript:

EXOTIC NUCLEAR STRUCTURE PHENOMENA the complex EXCITED VAMPIR approach IN MEDIUM MASS NUCLEI O. RADU1, A. PETROVICI1,2, K.W. SCHMID2, A. FAESSLER2 1 Horia Hulubei National Institute for Physics and Nuclear Engineering, Bucharest,Romania 2 Institut für Theoretische Physik, Universität Tübingen, Germany within the complex EXCITED VAMPIR approach

Variational approaches to the nuclear many-body problem using symmetry-projected Hartree-Fock-Bogoliubov configurations General theoretical tools the model space is defined by a finite set of spherical single particle states the effective many-body Hamiltonian is represented as a sum of one- and two-body terms the basic building blocks are HFB vacua, only restricted by time-reversal and axial symmetry the HFB transformations are essentially complex and allow proton-neutron and parity mixing the broken symmetries are restored by projection techniques (s = N, Z, I, ) O.Radu – NNPSS, Tallahassee 2007

O.Radu – NNPSS, Tallahassee 2007

O.Radu – NNPSS, Tallahassee 2007

O.Radu – NNPSS, Tallahassee 2007

Variational procedures complex Vampir approach O.Radu – NNPSS, Tallahassee 2007

complex Excited Vampir approach O.Radu – NNPSS, Tallahassee 2007

A= 50 – 90 mass region O.Radu – NNPSS, Tallahassee 2007

Shape coexistence effects in 78Kr Nucl. Phys. A770 (2006) 107 J. Phys. G: Nucl.Part.Phys.32(2006) 583 Shape coexistence effects in 78Kr O.Radu – NNPSS, Tallahassee 2007

O.Radu – NNPSS, Tallahassee 2007

O.Radu – NNPSS, Tallahassee 2007

O.Radu – NNPSS, Tallahassee 2007 xp Q(2+1)= -61(3) efm2 Q(2+2)= +44(6) efm2 O.Radu – NNPSS, Tallahassee 2007

O.Radu – NNPSS, Tallahassee 2007

O.Radu – NNPSS, Tallahassee 2007 Exp. g(2+1)=0.43(3) g(2+2)=0.54(10) g(4+1)=0.46(7) small effective g-factors at spins 8+, 10+, 12+ O.Radu – NNPSS, Tallahassee 2007

2exp(E0;0+2 0+1)=0.047(13) ; 2EXV(E0;0+3 0+1)=0.017 O.Radu – NNPSS, Tallahassee 2007

Magnetic bands in 82Rb O.Radu – NNPSS, Tallahassee 2007 Eur. Phys. J. A28 (2006) 19 Magnetic bands in 82Rb O.Radu – NNPSS, Tallahassee 2007

O.Radu – NNPSS, Tallahassee 2007

O.Radu – NNPSS, Tallahassee 2007

O.Radu – NNPSS, Tallahassee 2007

O.Radu – NNPSS, Tallahassee 2007

Summary and outlook the shape coexistence and the variable oblate-prolate mixing with increasing spin and excitation energy could explain the irregularities observed at low, intermediate and high spins the forking observed at the highest identified spins is determined by a high density of strongly mixed configurations the calculated electromagnetic properties agree with the available data an alternative mechanism to the shears bands able to describe microscopically the phenomenon in the A~80 mass region is provided the experimental trend is produced by an increased mixing of differently deformed states at the highest calculated spins the description of the exotic phenomena in medium mass nuclei requires very large many-nucleon model spaces considerable effort has to be devoted deriving improved effective interaction O.Radu – NNPSS, Tallahassee 2007