Fission Barriers in Skyrme-HFB Approach LORW group 14 th Nuclear Physics Workshop "Marie & Pierre Curie" Kazimierz 2007.

Slides:

Advertisements

Similar presentations

PRESPEC & The (Time- Dependent) Mean Field Dr Paul D Stevenson University of Surrey.

Advertisements

電気的に励起された岩田順敬 ( 東大理 ) Cedric Simenel (CEA/Saclay) 原子核の時間発展 Thanks to: 大塚孝治 ( 東大理、東大 CNS 、理研 ) Michael Bender (CEA/Saclay)

University of Liverpool

Testing isospin-symmetry breaking and mapping the proton drip-line with Lanzhou facilities Yang Sun Shanghai Jiao Tong University, China SIAP, Jan.10,

Generalized pairing models, Saclay, June 2005 Generalized models of pairing in non-degenerate orbits J. Dukelsky, IEM, Madrid, Spain D.D. Warner, Daresbury,

12 June, 2006Istanbul, part I1 Mean Field Methods for Nuclear Structure Part 1: Ground State Properties: Hartree-Fock and Hartree-Fock- Bogoliubov Approaches.

Lawrence Livermore National Laboratory UCRL-XXXX Lawrence Livermore National Laboratory, P. O. Box 808, Livermore, CA This work performed under.

On the formulation of a functional theory for pairing with particle number restoration Guillaume Hupin GANIL, Caen FRANCE Collaborators : M. Bender (CENBG)

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.

Towards a Universal Energy Density Functional Towards a Universal Energy Density Functional Study of Odd-Mass Nuclei in EDF Theory N. Schunck University.

Continuum QRPA calculation with the Skyrme effective force Niigata University Kazuhito Mizuyama Masayuki Matsuo & Yasuyoshi Serizawa.

Secondary Minima and Non-axial Saddles in Superheavy (Z around 120) Introduction Method ot the analysis Deformation space Results Summary P. Jachimowicz,

Nuclear equation of state in form suitable for quantum molecular dynamics model 1.Brief indroduction of the EOS prescription 2.New form for bullk and surface.

Single Particle Energies

9/28/ :01 (00) PAIRING PROPERTIES OF SUPERHEAVY NUCLEI A. Staszczak, J. Dobaczewski and W. Nazarewicz (KFT UMCS) (IFT UW) (ORNL & UT)

Fission potential energy surfaces in ten-dimensional deformation space. Vitaly Pashkevich Joint Institute for Nuclear Research. Dubna, Russia Yuri Pyatkov.

:12 (00) Below-barrier paths: multimodal fission & doughnut nuclei A. Staszczak (UMCS, Lublin) FIDIPRO-UNEDF collaboration meeting on nuclear.

Application of DFT to the Spectroscopy of Odd Mass Nuclei N. Schunck Department of Physics  Astronomy, University of Tennessee, Knoxville, TN-37996, USA.

Systematics of the First 2 + Excitation in Spherical Nuclei with Skyrme-QRPA J. Terasaki Univ. North Carolina at Chapel Hill 1.Introduction 2.Procedure.

Relative kinetic energy correction to fission barriers 1. Motivation 2. Results for A= systems 3. A cluster model perspective 4. Prescription based.

1 Symmetries of the local densities S.G.Rohoziński, J. Dobaczewski, W. Nazarewicz University of Warsaw, University of Jyväskylä The University of Tennessee,

Terminating states as a unique laboratory for testing nuclear energy density functional Maciej Zalewski, UW under supervision of W. Satuła Kazimierz Dolny,

Fission fragment properties at scission:

NUCLEAR STRUCTURE PHENOMENOLOGICAL MODELS

 What are the appropriate degrees of freedom for describing fission of heavy nuclei (171 ≤ A ≤ 330)?  Fission barrier heights for 5239 nuclides between.

CEA Bruyères-le-ChâtelESNT 2007 Fission fragment properties at scission: An analysis with the Gogny force J.F. Berger J.P. Delaroche N. Dubray CEA Bruyères-le-Châtel.

M. Girod, F.Chappert, CEA Bruyères-le-Châtel Neutron Matter and Binding Energies with a New Gogny Force.

Relativistic chiral mean field model for nuclear physics (II) Hiroshi Toki Research Center for Nuclear Physics Osaka University.

NSDD Workshop, Trieste, February 2006 Nuclear Structure (II) Collective models P. Van Isacker, GANIL, France.

Tomohiro Oishi 1,2, Markus Kortelainen 2,1, Nobuo Hinohara 3,4 1 Helsinki Institute of Phys., Univ. of Helsinki 2 Dept. of Phys., Univ. of Jyvaskyla 3.

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.

XII Nuclear Physics Workshop Maria and Pierre Curie: Nuclear Structure Physics and Low-Energy Reactions, Sept , Kazimierz Dolny, Poland Self-Consistent.

1 New formulation of the Interacting Boson Model and the structure of exotic nuclei 10 th International Spring Seminar on Nuclear Physics Vietri sul Mare,

Effects of self-consistence violations in HF based RPA calculations for giant resonances Shalom Shlomo Texas A&M University.

Symmetries in Nuclei, Tokyo, 2008 Symmetries in Nuclei Symmetry and its mathematical description The role of symmetry in physics Symmetries of the nuclear.

Nuclear Structure and dynamics within the Energy Density Functional theory Denis Lacroix IPN Orsay Coll: G. Scamps, D. Gambacurta, G. Hupin M. Bender and.

Ning Wang 1, Min Liu 1, Xi-Zhen Wu 2, Jie Meng 3 Isospin effect in Weizsaecker-Skyrme mass formula ISPUN14, , Ho Chi Minh City 1 Guangxi Normal.

Mean-Field Description of Heavy Neutron-Rich Nuclei P. D. Stevenson University of Surrey NUSTAR Neutron-Rich Minischool Surrey, 2005.

The calculation of Fermi transitions allows a microscopic estimation (Fig. 3) of the isospin mixing amount in the parent ground state, defined as the probability.

Nuclear deformation in deep inelastic collisions of U + U.

Isospin mixing and parity- violating electron scattering O. Moreno, P. Sarriguren, E. Moya de Guerra and J. M. Udías (IEM-CSIC Madrid and UCM Madrid) T.

A new statistical scission-point model fed with microscopic ingredients Sophie Heinrich CEA/DAM-Dif/DPTA/Service de Physique Nucléaire CEA/DAM-Dif/DPTA/Service.

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.)

IAEA Workshop on NSDD, Trieste, November 2003 The interacting boson model P. Van Isacker, GANIL, France Dynamical symmetries of the IBM Neutrons, protons.

Spectroscopy of Odd-Mass Nuclei in Energy Density Functional Theory Impact of Terascale Computing N. Schunck University of Tennessee, 401 Nielsen Physics,

Fission Collective Dynamics in a Microscopic Framework Kazimierz Sept 2005 H. Goutte, J.F. Berger, D. Gogny CEA Bruyères-le-Châtel Fission dynamics with.

ShuangQuan Zhang School of Physics, Peking University Static chirality and chiral vibration of atomic nucleus in particle rotor model.

Ning Wang An improved nuclear mass formula Guangxi Normal University, Guilin, China KITPC , Beijing.

1 Technology to calculate observables Global properties Spectroscopy DFT Solvers Functional form Functional optimization Estimation of theoretical errors.

Application of the Adiabatic Self-Consistent Collective Coordinate (ASCC) Method to Shape Coexistence/ Mixing Phenomena Application of the Adiabatic Self-Consistent.

July 29-30, 2010, Dresden 1 Forbidden Beta Transitions in Neutrinoless Double Beta Decay Kazuo Muto Department of Physics, Tokyo Institute of Technology.

DFT with Continuum Junchen Pei (Peking U) With Collaborators: US : W. Nazarewicz, G. Fann, Yue Shi, R.Harrison, S. Thornton Europe: M. Kortelainen, P.

Tailoring new interactions in the nuclear many-body problem for beyond- mean-field models Marcella Grasso Tribute to Daniel Gogny.

Symmetries of the Cranked Mean Field S. Frauendorf Department of Physics University of Notre Dame USA IKH, Forschungszentrum Rossendorf, Dresden Germany.

F. C HAPPERT N. P ILLET, M. G IROD AND J.-F. B ERGER CEA, DAM, DIF THE D2 GOGNY INTERACTION F. C HAPPERT ET AL., P HYS. R EV. C 91, (2015)

Nuclear density functional theory with a semi-contact 3-body interaction Denis Lacroix IPN Orsay Outline Infinite matter Results Energy density function.

Global fitting of pairing density functional; the isoscalar-density dependence revisited Masayuki YAMAGAMI (University of Aizu) Motivation Construction.

Exotic Nuclear Shapes Probing the limits of nuclear stability

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.

Gogny-TDHFB calculation of nonlinear vibrations in 44,52 Ti Yukio Hashimoto Graduate school of pure and applied sciences, University of Tsukuba 1.Introduction.

How do nuclei rotate? 3. The rotating mean field.

性別平等教育尊重彼此的不同學會善解別人瑞田國小. 你喜歡看那一種卡通？小妹妹一定是背著洋娃娃嗎？

Few-Body Models of Light Nuclei The 8th APCTP-BLTP JINR Joint Workshop June 29 – July 4, 2014, Jeju, Korea S. N. Ershov.

The role of isospin symmetry in medium-mass N ~ Z nuclei

Solving Quadratic Equations by the Complete the Square Method

The Isovector Giant Quadrupole Resonance & Nuclear Matter

Microscopic studies of the fission process

Quantify correlations between the neutron skin and other quantities characterizing finite nuclei and infinite nuclear matter. How will additional data.

Superheavy nuclei: relativistic mean field outlook

Presentation transcript:

Fission Barriers in Skyrme-HFB Approach LORW group 14 th Nuclear Physics Workshop "Marie & Pierre Curie" Kazimierz 2007

Seniority pairing: J. Dudek, et al., J. Phys. G6 (1980)447.  pairing force: R. R. Chasman, Phys. Rev. C 14 (1976)1935. G. F. Bertsch and H. Esbensen, Ann. Phys. (N.Y.) 209 (1991)327. In the pairing (BCS) window  n/p  N (or Z) s. p. states are taken, and parameters are chosen to reproduce  n/p for 252 Fm.

SLy4

LORW group: A. Baran, A. S. (Lublin) W. Nazarewicz (Oak Ridge) J. Dobaczewski (Warszawa )

KONIEC

The constrained HF procedure  The constraints act as the external fields capable to deform the nucleus in different ways  The collective coordinates can be defined in a natural way by measuring the deformations generated by the various constraints The constrained mean field theory defines the deformed states (BCS- or HFB-type) that solve the variational equation: with the constraint conditions quadratic multipole constraints The multipole constraints prescribe different kinds of deformation characterized by the set of parameters

is the many-body nuclear (non-relativistic) Hamiltonian center-of-mass “projection” term (in the VAP technique), to eliminate spurious mode associated with the broken translational symmetry nuclear effective interaction term (Skyrme, Gogne type forces) To describe the fission process most “important” are the low-multipolarity mass moments, i.e., “nuclear stretching” “reflection-asymmetry” “necking”

The spectral (average) gap: