INT October 28, 2004Mihai Horoi - Central Michigan Univ1 New Approaches for Spin- and Parity-Dependent Shell Model Nuclear Level Density Mihai Horoi, Department.

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

Spectroscopy at the Particle Threshold H. Lenske 1.
Delta-hole effects on the shell evolution of neutron-rich exotic nuclei Takaharu Otsuka University of Tokyo / RIKEN / MSU Chiral07 Osaka November 12 -
Constrained-Path Quantum Monte-Carlo Approach for the Nuclear Shell Model Jérémy Bonnard 1,2, Olivier Juillet 2 1 INFN, section of Padova 2 University.
Testing shell model on nuclei
K. Kaneko Kyushu Sangyo University, Fukuoka, Japan Particle-number conservation for pairing transition in finite systems A. Schiller Michigan State University,
Spin polarization of 23 Ne produced in heavy ion reactions M. Mihara 1, K. Matsuta 1, R. Matsumiya 1, T. Nagatomo 1*, M. Fukuda 1,T. Minamisono 2, S.
W A RICHTER UNIVERSITY OF THE WESTERN CAPE Shell-model studies of the rp reaction 25 Al(p,γ) 26 Si.
Beta decay and Structure of Exotic Nuclei near 78 Ni Alexander Lisetskiy NSCL,JINA,MSU.
Nucleon knockout reactions with heavy nuclei Edward Simpson University of Surrey Brighton PRESPEC Meeting 12 th January 2011.
Determination of freeze-out temperatures Excellent consistency with thermal equilibrium for central collisions near the multi-fragmentation threshold Deduced.
EURISOL workshop, ECT* Trento, Jan Two-component (neutron/proton) statistical description of low-energy heavy-ion reactions E. Běták & M.
INT Seattle 3/14/2002M Horoi - Central Michigan University 1 Central Michigan Shell Model Code (CMichSM): Present and Future Applications  Mihai Horoi,
Nucleon Optical Potential in Brueckner Theory Wasi Haider Department of Physics, AMU, Aligarh, India. E Mail:
Role of mass asymmetry in fusion of super-heavy nuclei
Outline  Simple comments on regularities of many-body systems under random interactions  Number of spin I states for single-j configuration  J-pairing.
Shell-model CI codes and applications Calvin Johnson (1) Plamen Krastev (1,2) * Erich Ormand (2) 1 San Diego State University 2 Lawrence Livermore National.
横田 朗A 、 肥山 詠美子B 、 岡 眞A 東工大理工A、理研仁科セB
Structure of Be hyper-isotopes Masahiro ISAKA (RIKEN) Collaborators: H. Homma and M. Kimura (Hokkaido University)
Stephane Grévy : October 8, 2012 Unveiling the intruder deformed state in 34 Si 20 and few words about N=28 IFIN - Bucharest F. Rotaru.
Statistical properties of nuclei: beyond the mean field Yoram Alhassid (Yale University) Introduction Beyond the mean field: correlations via fluctuations.
Aim  to compare our model predictions with the measured (Dubna and GSI) evaporation cross sections for the 48 Ca Pb reactions. Calculations.
D.Bucurescu, T. von Egidy, Level density, spin distribution-Ohio, July Nuclear Level Densities and Spin Distributions Dorel Bucurescu National Institute.
Nuclear Level Densities Edwards Accelerator Laboratory Steven M. Grimes Ohio University Athens, Ohio.
The structure of giant resonances in calcium and titanium isotopes. N.G.Goncharova, Iu.A.Skorodumina Skobelzyn Institute of Nuclear Physics, Moscow State.
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.
XII Nuclear Physics Workshop Maria and Pierre Curie: Nuclear Structure Physics and Low-Energy Reactions, Sept , Kazimierz Dolny, Poland Self-Consistent.
Alex Brown PREX Aug Neutron Radii and the Neutron Equation of State.
Alex Brown UNEDF Feb Strategies for extracting optimal effective Hamiltonians for CI and Skyrme EDF applications.
Nuclear Level Density 1.What we know, what we do not know, and what we want to know 2.Experimental techniques to study level densities, what has been done.
On microscopic description of the gamma-ray strength functions S. Kamerdzhiev, D. Voitenkov Institute of Physics and Power Engineering, Obninsk, Russia.
Cluster-shell Competition in Light Nuclei N. Itagaki, University of Tokyo S. Aoyama, Kitami Institute of Technology K. Ikeda, RIKEN S. Okabe, Hokkaido.
Coupling of (deformed) core and weakly bound neutron M. Kimura (Hokkaido Univ.)
Relativistic mean field and RPA with negative energy states for finite nuclei Akihiro Haga, Hiroshi Toki, Setsuo Tamenaga, Yoko Ogawa, Research Center.
Hiroshi MASUI Kitami Institute of Technology Collaborators:K. KatoHokkaido Univ. K. IkedaRIKEN Aug. 2011, APFB2011, Sungkyunkwan Univ., Seoul, Korea.
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.)
ISOVECTOR EXCITATIONS OF sd-SHELL NUCLEI IN THE PARTICLE-CORE COUPLING VERSION OF SHELL MODEL N.G. Goncharova Skobelzyn Institute of Nuclear Physics, Moscow.
Shell Model with residual interactions – mostly 2-particle systems Start with 2-particle system, that is a nucleus „doubly magic + 2“ Consider two identical.
N. Itagaki Yukawa Institute for Theoretical Physics, Kyoto University.
What can we learn from nuclear level density? Magne Guttormsen Department of Physics and SAFE University of Oslo.
Numerical accuracy of mean-field calculations The case of the 3-dimensional mesh scheme The Lagrange implementation P. Bonche, J. Dobaczewski, H. Flocard.
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 (许甫荣) Many-body calculations with realistic and phenomenological nuclear forces Outline I. Nuclear forces II. N 3 LO (LQCD): MBPT, BHF, GSM (resonance.
Effective interactions in shell-model calculations M. Honma (Univ. of Aizu) T. Mizusaki (Senshu Univ.) T. Otsuka (Univ. of Tokyo/RIKEN) B. A. Brown (MSU)
Variational approach to isospin symmetry breaking in medium mass nuclei A. PETROVICI Institute for Physics and Nuclear Engineering, Bucharest, Romania.
MICROSCOPIC CALCULATION OF SYMMETRY PROJECTED NUCLEAR LEVEL DENSITIES Kris Van Houcke Ghent University In collaboration with S. Rombouts, K. Heyde, Y.
Reaction cross sections of carbon isotopes incident on proton and 12 C International Nuclear Physics Conference, Tokyo, Japan June 3-8, 2007 W. Horiuchi.
Nuclear density functional theory with a semi-contact 3-body interaction Denis Lacroix IPN Orsay Outline Infinite matter Results Energy density function.
11 Tensor optimized shell model with bare interaction for light nuclei In collaboration with Hiroshi TOKI RCNP, Osaka Univ. Kiyomi IKEDA RIKEN 19th International.
Satoru Sugimoto Kyoto University 1. Introduction 2. Charge- and parity-projected Hartree-Fock method (a mean field type model) and its application to sub-closed.
Time dependent GCM+GOA method applied to the fission process ESNT janvier / 316 H. Goutte, J.-F. Berger, D. Gogny CEA/DAM Ile de France.
g-ray spectroscopy of the sd-shell hypernuclei
Computational Nuclear Structure SNP Moment (and Fermi gas) methods for modeling nuclear state densities Calvin W. Johnson (PI) Edgar Teran (former.
Lecture 4 1.The role of orientation angles of the colliding nuclei relative to the beam energy in fusion-fission and quasifission reactions. 2.The effect.
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.
1 Jeff Tostevin, Department of Physics Faculty of Engineering and Physical Sciences University of Surrey, United Kingdom Sensitivity of two-nucleon knockout.
Shell-model calculations for the IoI —a review from a personal point of view Yutaka Utsuno Advanced Science Research Center, Japan Atomic Energy Agency.
Large-scale shell-model study of E1 strength function and level density Yutaka Utsuno Advanced Science Research Center, Japan Atomic Energy Agency Center.
Zao-Chun Gao(高早春) China Institute of Atomic Energy Mihai Horoi
Structure and dynamics from the time-dependent Hartree-Fock model
Zeeman effect HFS and isotope shift
Diproton correlation in a proton-rich Borromean nucleus 17Ne
Role of Pions in Nuclei and Experimental Characteristics
Grigory Nigmatkulov National Research Nuclear University MEPhI
Daisuke ABE Department of Physics, University of Tokyo
Cluster and Density wave --- cluster structures in 28Si and 12C---
Content of the talk Exotic clustering in neutron-rich nuclei
for BCS quasiparticles
Probing correlations by use of two-nucleon removal
Presentation transcript:

INT October 28, 2004Mihai Horoi - Central Michigan Univ1 New Approaches for Spin- and Parity-Dependent Shell Model Nuclear Level Density Mihai Horoi, Department of Physics, Central Michigan University, Mount Pleasant, Michigan 48859, USA  Support from NSF grant PHY is acknowledged

INT October 28, 2004Mihai Horoi - Central Michigan Univ2 Plan of the Talk Part I: Methods for Shell Model NLD –Motivation –Sum on partitions vs moments of the whole density –Exponential Convergence Method –Fixed-J Configuration Centroids and Widths –Energy-Dependent Cutoff Description –PRC 67, (2003), PRC 69, (2004) Part II: Methods of Removal of the Center-of-Mass Spurious Contribution

INT October 28, 2004Mihai Horoi - Central Michigan Univ3 Hauser and Feshbach, Phys. Rev 87, 366 (1952)

INT October 28, 2004Mihai Horoi - Central Michigan Univ4 The Back-Shifted Fermi Gas Model for Nuclear Level Density

INT October 28, 2004Mihai Horoi - Central Michigan Univ5 A.Adams, G.Mitchell, J.F. Shriner Phys.Lett, B422, 13(1998) 26 Al sd-shell model, USD interaction

INT October 28, 2004Mihai Horoi - Central Michigan Univ6 Data: Table of Isotopes Theory: sd-shell model + USD interaction 28 Si: positive parity

INT October 28, 2004Mihai Horoi - Central Michigan Univ7 p ’s sd ’s pf ’s pf 5/2 -g 9/ Example: 76 Sr PRL 92, pf 5/2 -g 9/2 dimension 11,090,052,440 CMichSM code - m-scheme dimension 250,000,000 on one-processor machine Lanczos iterations/week

INT October 28, 2004Mihai Horoi - Central Michigan Univ8 12 particles in sd model space

INT October 28, 2004Mihai Horoi - Central Michigan Univ9 Nuclear Shell Model d = 2 (2 j + 1)

INT October 28, 2004Mihai Horoi - Central Michigan Univ10 Sum on Partitions vs Moments of the Whole Distribution 6 particles in pf 5/2 -g 9/2 New interaction A. Lisetskiy et al. PRC 2004

INT October 28, 2004Mihai Horoi - Central Michigan Univ11 12 particles in sd model space

INT October 28, 2004Mihai Horoi - Central Michigan Univ12 12 particles in sd model space

INT October 28, 2004Mihai Horoi - Central Michigan Univ13 6 particles in p-sd model space

INT October 28, 2004Mihai Horoi - Central Michigan Univ14 Exponential Convergence Method

INT October 28, 2004Mihai Horoi - Central Michigan Univ15 Exponential Convergence Method for fp-nuclei

INT October 28, 2004Mihai Horoi - Central Michigan Univ16 Exponential Convergence Method for fp-nuclei Central Michigan Shell Model (CMichSM) code Exact: MeV

INT October 28, 2004Mihai Horoi - Central Michigan Univ17 r,s,.. – orbits, not states

INT October 28, 2004Mihai Horoi - Central Michigan Univ18 Fixed J Configura tion Centroids and Widths C. Jacquemin, Z. Phys. A 303, 135 (1981)

INT October 28, 2004Mihai Horoi - Central Michigan Univ19 Shell Model vs Fixed-J Centroids and Widths Density of States 28 Si: 12 particles in sd, Tz=0

INT October 28, 2004Mihai Horoi - Central Michigan Univ20 Shell Model vs Fixed-J Centroids and Widths Density of States 28 Si: 12 particles in sd, Tz=0

INT October 28, 2004Mihai Horoi - Central Michigan Univ21 Spin Cutoff Factor Zeroth-Order: S.S.M. Wong, Nuclear Spectroscopy, Oxford 1986, p. 45, Si: 12 particles in sd, Tz=0

INT October 28, 2004Mihai Horoi - Central Michigan Univ22 Shell Model 28 Si: 12 particles in sd, Tz=0

INT October 28, 2004Mihai Horoi - Central Michigan Univ23 Shell Model 28 Si: 12 particles in sd, Tz=0

INT October 28, 2004Mihai Horoi - Central Michigan Univ24 Zeroth-Order 28 Si: 12 particles in sd, Tz=0

INT October 28, 2004Mihai Horoi - Central Michigan Univ25 Zeroth-Order 28 Si: 12 particles in sd, Tz=0

INT October 28, 2004Mihai Horoi - Central Michigan Univ26 Summary of Part I Shell Model NLD look very promising, at least up to the particle emission threshold. More comparison with experimental data necessary. J-dependent SM NLD are very accurately described by a sum of finite range Gaussians with fixed-J centroids and widths, if one knows with good precision the energy of g.s. and yrast states. We derived explicit expression to calculate fixed-J centroids and widths. Exponential Convergence Method (ECM) proves to be a very powerful tool for finding yrast and non-yrast energies, by doing shell model calculations in truncated model spaces. J-dependent SM NLD are reasonably well described by spin cutoff formula with exact cutoff factor, except for higher J’s, but not very well described by spin cutoff formula with zeroth-order cutoff factor. Improvement in estimating cutoff factor requires knowledge of higher order moments.

INT October 28, 2004Mihai Horoi - Central Michigan Univ27 The Center-of-Mass Problem nucl-th/

INT October 28, 2004Mihai Horoi - Central Michigan Univ28 Nuclear Shell Model N

INT October 28, 2004Mihai Horoi - Central Michigan Univ29 The Center-of-Mass Problem

INT October 28, 2004Mihai Horoi - Central Michigan Univ30 No E (MeV) Ex (MeV) J T No E (MeV) Ex (MeV) J T p-sd s-p-sd 2 particles 6 particles N = 1

INT October 28, 2004Mihai Horoi - Central Michigan Univ31 Dimensions of Nonspurious Spaces Example: s-p-sd, 6 particles J N=1(K=1) N=0 0 4 = = = = =1 0 Total 26

INT October 28, 2004Mihai Horoi - Central Michigan Univ32

INT October 28, 2004Mihai Horoi - Central Michigan Univ33 C. Jacquemin, Z. Phys. A 303, 135 (1981) Fixed J Restricted Configura tion Widths

INT October 28, 2004Mihai Horoi - Central Michigan Univ34

INT October 28, 2004Mihai Horoi - Central Michigan Univ35 N   Nonspurious Level Density

INT October 28, 2004Mihai Horoi - Central Michigan Univ36 20 Ne: 20 particles in s-p-sd-pf shell model space

INT October 28, 2004Mihai Horoi - Central Michigan Univ37 20 Ne: 20 particles in s-p-sd-pf shell model space

INT October 28, 2004Mihai Horoi - Central Michigan Univ38 20 Ne: 20 particles in s-p-sd-pf shell model space

INT October 28, 2004Mihai Horoi - Central Michigan Univ39 Nonspurious Level Density: (0+2)  

INT October 28, 2004Mihai Horoi - Central Michigan Univ40 10 B: 10 particles in s-p-sd-pf shell model space

INT October 28, 2004Mihai Horoi - Central Michigan Univ41 10 B: 10 particles in s-p-sd-pf shell model space

INT October 28, 2004Mihai Horoi - Central Michigan Univ42 Nonspurious Level Density: General

INT October 28, 2004Mihai Horoi - Central Michigan Univ43 Summary We derived explicit expressions to calculate fixed- J centroids and widths for restricted set of configurations, such N   configurations We found recursive formulae to calculate the dimensions of nospurious spaces We found recursive formulae for calculating exactly the nonspurious level density when one knows the level density for a restricted set of configurations, such N   configurations Using our method of calculating the level density for restricted set of configurations we can calculate very accurately the nonspurious level density