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.

Slides:



Advertisements
Similar presentations
QMD and Low Energy Neutron Development Koi, Tatsumi SLAC National Accelerator Laboratory Geant4 Collaboration Workshop
Advertisements

Spectroscopy at the Particle Threshold H. Lenske 1.
Be BeTe BeO Gamma-ray spectroscopy of cluster hypernuclei : 9  Be K. Shirotori for the Hyperball collaboration, Tohoku Univ. 8 Be is known as the  -
Nuclear “Pasta” in Compact Stars Hidetaka Sonoda University of Tokyo Theoretical Astrophysics Group Collaborators (G. Watanabe, K. Sato, K. Yasuoka, T.
Toshiki Maruyama (JAEA) Nobutoshi Yasutake (Chiba Inst. of Tech.) Minoru Okamoto (Univ. of Tsukuba & JAEA ) Toshitaka Tatsumi (Kyoto Univ.) Structures.
Solution of the Deuteron using Perturbation Theory (ongoing work with R. S. Azevedo and Prof. Bira van Kolck) University of Arizona Undergraduate Symposium.
Introduction to Molecular Orbitals
Dineutron formation and breaking in 8 He th Sep. The 22nd European Conference on Few-Body Problems in Physics 1 Department of Physics, Kyoto University.
Isospin effect in the projectile fragmentation of calcium isotopes and a possible experimental observable? Chun-Wang Ma Department of Physics, Henan Normal.
On the formulation of a functional theory for pairing with particle number restoration Guillaume Hupin GANIL, Caen FRANCE Collaborators : M. Bender (CENBG)
Finite Nuclei and Nuclear Matter in Relativistic Hartree-Fock Approach Long Wenhui 1,2, Nguyen Van Giai 2, Meng Jie 1 1 School of Physics, Peking University,
Kazimierz What is the best way to synthesize the element Z=120 ? K. Siwek-Wilczyńska, J. Wilczyński, T. Cap.
Forces for extensions of mean-field PhD Thesis Marlène Assié Denis Lacroix (LPC Caen), Jean-Antoine Scarpaci (IPN Orsay)  Extensions of mean-field ? 
Neutron Number N Proton Number Z a sym =30-42 MeV for infinite NM Inclusion of surface terms in symmetry.
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)
Coupled-Channel analyses of three-body and four-body breakup reactions Takuma Matsumoto (RIKEN Nishina Center) T. Egami 1, K. Ogata 1, Y. Iseri 2, M. Yahiro.
 What are the appropriate degrees of freedom for describing fission of heavy nuclei (171 ≤ A ≤ 330)?  Fission barrier heights for 5239 nuclides between.
Nucleon Optical Potential in Brueckner Theory Wasi Haider Department of Physics, AMU, Aligarh, India. E Mail:
Equation of State of Neutron-Rich Matter in the Relativistic Mean-Field Approach Farrukh J. Fattoyev My TAMUC collaborators: B.-A. Li, W. G. Newton My.
M. Girod, F.Chappert, CEA Bruyères-le-Châtel Neutron Matter and Binding Energies with a New Gogny Force.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
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)
モンテカルロ殻模型による ベリリウム同位体の密度分布 T. Yoshida (a), N. Shimizu (a), T. Abe (b) and T. Otsuka (a, b) Center for Nuclear Study (a) and Department of Physics (b),
J.B. Natowitz. Correlations – Cluster Formation Bose Condensates Efimov States Superfluidity Perfect Liquid? Perfect Gas ? Few Body Syst.Suppl. 14 (2003)
Mary Beard University of Notre Dame Reaction Rates Calculations in Dense Stellar Matter Frontiers 2005 Aim: To establish a general reaction.
Yu-Gang Ma 18th Few Body Conference, 2006, Santos, Brazil Nucleon-Nucleon momentum correlation functions induced by the radioactive beams Yu-Gang Ma Shanghai.
XII Nuclear Physics Workshop Maria and Pierre Curie: Nuclear Structure Physics and Low-Energy Reactions, Sept , Kazimierz Dolny, Poland Self-Consistent.
Effects of self-consistence violations in HF based RPA calculations for giant resonances Shalom Shlomo Texas A&M University.
Alex Brown UNEDF Feb Strategies for extracting optimal effective Hamiltonians for CI and Skyrme EDF applications.
Nicolas Michel CEA / IRFU / SPhN Shell Model approach for two-proton radioactivity Nicolas Michel (CEA / IRFU / SPhN) Marek Ploszajczak (GANIL) Jimmy Rotureau.
MEM analysis of the QCD sum rule and its Application to the Nucleon spectrum Tokyo Institute of Technology Keisuke Ohtani Collaborators : Philipp Gubler,
Nuclear deformation in deep inelastic collisions of U + U.
J. Su( 苏军 ) and F.S. Zhang( 张丰收 ) College of Nuclear Science and Technology Beijing Normal University, Beijing, China Tel: ,
Pavel Stránský Complexity and multidiscipline: new approaches to health 18 April 2012 I NTERPLAY BETWEEN REGULARITY AND CHAOS IN SIMPLE PHYSICAL SYSTEMS.
Microscopic Modeling of Supernova Matter Igor Mishustin FIAS, J. W. Goethe University, Frankfurt am Main, Germany and National Research Center “Kurchatov.
Hadronic Physics II Geant4 Users’ Tutorial CERN February 2010 Gunter Folger.
Neutron enrichment of the neck-originated intermediate mass fragments in predictions of the QMD model I. Skwira-Chalot, T. Cap, K. Siwek-Wilczyńska, J.
Probing the symmetry energy with isospin ratio from nucleons to fragments Yingxun Zhang( 张英逊 ) China Institute of Atomic Energy The 11 th International.
Auxiliary Field Diffusion Monte Carlo study of symmetric nuclear matter S. Gandolfi Dipartimento di Fisica and INFN, Università di Trento I Povo,
Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology KITPC, Beijing.
NEUTRON SKIN AND GIANT RESONANCES Shalom Shlomo Cyclotron Institute Texas A&M University.
The 13th National Nuclear Structure Conference of China, Chifeng Fragments cross section distributions of even Ca at intermediate energy 马春旺
Three-body force effect on the properties of asymmetric nuclear matter Wei Zuo Institute of Modern Physics, Lanzhou, China.
Study on Sub-barrier Fusion Reactions and Synthesis of Superheavy Elements Based on Transport Theory Zhao-Qing Feng Institute of Modern Physics, CAS.
How do you build a good Hamiltonian for CEID? Andrew Horsfield, Lorenzo Stella, Andrew Fisher.
Tailoring new interactions in the nuclear many-body problem for beyond- mean-field models Marcella Grasso Tribute to Daniel Gogny.
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)
Inha Nuclear Physics Group Quantum Opacity and Refractivity in HBT Puzzle Jin-Hee Yoon Dept. of Physics, Inha University, Korea John G. Cramer,
Nuclear density functional theory with a semi-contact 3-body interaction Denis Lacroix IPN Orsay Outline Infinite matter Results Energy density function.
PhD student at the International PhD Studies Institute of Nuclear Physics PAN Institute of Nuclear Physics PAN Department of Theory of Structure of Matter.
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.
1 Z.Q. Feng( 冯兆庆 ) 1 G.M. Jin( 靳根明 ) 2 F.S. Zhang ( 张丰收 ) 1 Institute of Modern Physics, CAS 2 Institute of Low Energy Nuclear Physics Beijing NormalUniversity.
Few-Body Models of Light Nuclei The 8th APCTP-BLTP JINR Joint Workshop June 29 – July 4, 2014, Jeju, Korea S. N. Ershov.
Improvements of microscopic transport models stimulated by spallation data for incident energies from 113 to MeV Umm Al-Qura University and King.
HIRG 重离子反应组 Heavy Ion Reaction Group GDR as a Probe of Alpha Cluster in Light Nuclei Wan-Bing He ( 何万兵 ) SINAP-CUSTIPEN Collaborators : Yu-Gang.
Transverse and elliptic flows and stopping
Tensor optimized shell model and role of pion in finite nuclei
Regularized delta interactions for nuclear structure calculations
The Isovector Giant Quadrupole Resonance & Nuclear Matter
Structure and dynamics from the time-dependent Hartree-Fock model
Content Heavy ion reactions started fragmenting nuclei in the 1980’s. Its study taught us that nuclear matter has liquid and gaseous phases, phase.
Quantify correlations between the neutron skin and other quantities characterizing finite nuclei and infinite nuclear matter. How will additional data.
Impurity effects in p-sd shell and neutron-rich L hypernuclei
Department of Physics, Fudan University, Shanghai, China
Variational Calculation for the Equation of State
Samara State University, Samara, Russia
V.V. Sargsyan, G.G. Adamian, N.V.Antonenko
Nicolas Michel (ESNT/SPhN/CEA) Kenichi Matsuyanagi (Kyoto University)
Presentation transcript:

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 energy 3.Comparision with the data 4.Conclusions Z. Sosin

in form given by expansion can not be solved analitycally

=>

How new EOS describes some theoretical predictions

N. Wang et al., Phys. Rev. C 69 (2004)

~

=> ~

Positions (r(k)) and sigmas (σ(k)) of the Gaussian packets can be found by applying minimization procedure to the Hamiltonian:

12 C 72 Kr r (fm) ρ(nucleons/fm 3 )

Conclusions: ρ 0 = nuc/fm 3 e 0 = MeV K 0 = 350 MeV μ = /fm 2 Z=N Z= , evet-event nuclei New form of EOS permits analiticaly integrate the hamiltonian density given as the sum of the Gaussian packets Proposed surface term properly describes nuclear matter density on the surface With more extensive calculations for, neutron skins and binding energies of nuclei in the ground states, parameters of EOS can be more constrained One can used this new form of EOS in the QMD type calculation