The Team:Marcin Borucki (ERASMUS, 4 th year MSc) Gillis Carlsson (postdoc) Jacek Dobaczewski (project leader) Jenni Kotila (Jouni Suhonen group) Markus.

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.

Valence shell excitations in even-even spherical nuclei within microscopic model Ch. Stoyanov Institute for Nuclear Research and Nuclear Energy Sofia,

EkEk ∆ δ A I of rigid Gap parameters from moments of Inertia.

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.

Mean-field calculation based on proton-neutron mixed energy density functionals Koichi Sato (RIKEN Nishina Center) Collaborators: Jacek Dobaczewski (Univ.

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

The Collective Model Aard Keimpema.

Gamow-Teller Transitions for Light Nuclei by the Deformed Quasi-particle RPA(DQRPA) Soongsil University, Korea Eun Ja HA and Myung-Ki CHEOUN HNP.

John Daoutidis October 5 th 2009 Technical University Munich Title Continuum Relativistic Random Phase Approximation in Spherical Nuclei.

Double beta decay nuclear matrix elements in deformed nuclei O. Moreno, R. Álvarez-Rodríguez, P. Sarriguren, E. Moya de Guerra F. Šimkovic, A. Faessler.

Detecting Giant Monopole Resonances Peter Nguyen Advisors: Dr. Youngblood, Dr. Lui Texas A&M University Energy Loss Identifying The Particles Discovered.

Single Particle Energies

Nuclear Reactions Emissions, Balancing, and predicting decays of Nuclear Reactions.

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

Detecting Giant Monopole Resonances Peter Nguyen Advisors: Dr. Youngblood, Dr. Lui Texas A&M University.

Classical Model of Rigid Rotor

Motion near an equilibrium position can be approximated by SHM

02/03/2014PHY 712 Spring Lecture 81 PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 8: Start reading Chapter 4 Multipole moment.

Multi-physics coupling Application on TRIGA reactor Student Romain Henry Supervisors: Prof. Dr. IZTOK TISELJ Dr. LUKA SNOJ PhD Topic presentation 27/03/2012.

Unit 2: Properties of Matter. The Goals… Define Matter Define Matter Calculate and understand density Calculate and understand density Describe viscosity.

Isospin effect in asymmetric nuclear matter (with QHD II model) Kie sang JEONG.

DPG Tagung, Breathing mode in an improved transport model T. Gaitanos, A.B. Larionov, H. Lenske, U. Mosel Introduction Improved relativistic transport.

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.

Cluster Structure in Nuclei Big Question: What nuclei have a cluster structure? ◦Clusters predicted in excited states close to decay thresholds ◦Signs.

Bohr Models and Lewis Dot Structures. Atoms ** Basic unit of matter Consists of: Electrons, Protons, & Neutrons.

Bound States 1. A quick review on the chapters 2 to Quiz Topics in Bound States:  The Schrödinger equation.  Stationary States.  Physical.

Specific Heat of Solids Quantum Size Effect on the Specific Heat Electrical and Thermal Conductivities of Solids Thermoelectricity Classical Size Effect.

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

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.

A conservative FE-discretisation of the Navier-Stokes equation JASS 2005, St. Petersburg Thomas Satzger.

Collective Model. Nuclei Z N Character j Q obs. Q sp. Qobs/Qsp 17 O 8 9 doubly magic+1n 5/ K doubly magic -1p 3/

Quantum Atom. Louis deBroglie Suggested if energy has particle nature then particles should have a wave nature Particle wavelength given by λ = h/ mv.

An Electron Trapped in A Potential Well Probability densities for an infinite well Solve Schrödinger equation outside the well.

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

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.

Lecture 16: Beta Decay Spectrum 29/10/2003 (and related processes...) Goals: understand the shape of the energy spectrum total decay rate sheds.

1 Proton-neutron pairing by G-matrix in the deformed BCS Soongsil University, Korea Eun Ja Ha Myung-Ki Cheoun.

Scattering of particles - topic 1 - june 2007 Particle Scattering: –Differential cross section –Trajectories and currents –Mean free path Quantal Scattering:

The Nuclear Energy Density Functional: What do we really know? Aurel Bulgac University of Washington, Seattle Collaborators: Michael McNeil Forbes - Washington.

Physics 3210 Week 14 clicker questions. When expanding the potential energy about a minimum (at the origin), we have What can we say about the coefficients.

Surrey Mini-School Lecture 2 R. F. Casten. Outline Introduction, survey of data – what nuclei do Independent particle model and residual interactions.

Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology KITPC, Beijing.

Nuclear Chemistry Chapter 23 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. PowerPoint Lecture Presentation.

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

Lecture 23: Applications of the Shell Model 27/11/ Generic pattern of single particle states solved in a Woods-Saxon (rounded square well)

Shell Model with residual interactions – mostly 2-particle systems Simple forces, simple physical interpretation Lecture 2.

DIRECT AND SEMIDIRECT NEUTRON RADIATIVE CAPTURE BY MEDIUM-HEAVY MASS NUCLEI: A NEW VERSION OF THE SEMIMICROSCOPIC DESCRIPTION B.A. Tulupov 1, M.H. Urin.

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)

And Mesons in Strange Hadronic Medium at Finite Temperature and Density Rahul Chhabra (Ph.D student) Department Of Physics NIT Jalandhar India In cooperation.

Quantum Chemistry: Our Agenda Postulates in quantum mechanics (Ch. 3) Schrödinger equation (Ch. 2) Simple examples of V(r) Particle in a box (Ch. 4-5)

Quantum phase transitions and structural evolution in nuclei.

PhD student at the International PhD Studies Institute of Nuclear Physics PAN Institute of Nuclear Physics PAN Department of Theory of Structure of Matter.

The Team: Ab initio DFT OSU (Drut, Furnstahl, Platter) MSU (Bogner, Gebremariam) DFT applications UTK (Nazarewicz, Pei, Schunck, Sheikh, Stoitsov) UW Seattle.

Continuum quasiparticle linear response theory using the Skyrme functional for exotic nuclei University of Jyväskylä Kazuhito Mizuyama, Niigata University,

Schrodinger wave equation

Nuclear Structure Tools for Continuum Spectroscopy

Regularized delta interactions for nuclear structure calculations

Structure and dynamics from the time-dependent Hartree-Fock model

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

Local Density Functional Theory for Superfluid Fermionic Systems

Lecture 9 The Hydrogen Atom

Kinetic Theory.

Kinetic Theory.

Alex Brown PAN July 26, 2018.

Presentation transcript:

The Team:Marcin Borucki (ERASMUS, 4 th year MSc) Gillis Carlsson (postdoc) Jacek Dobaczewski (project leader) Jenni Kotila (Jouni Suhonen group) Markus Kortelainen (postdoc) Kazuhito Mizuyama (postdoc) Francesco Raimondi (1 st year PhD) Rayner Rodriguez-Guzman (assistant) Jussi Toivanen (assistant) Pekka Toivanen (1 st year PhD) The FIDIPRO project at JYFL

The FIDIPRO topics Effective-operator methods to perform infinite summations of the harmonic oscillator-matrix elements of the kinetic energy in mean-field models Project leader: JussiStatus: on hold Extension of energy density functionals by a dependence of all coupling constants on the isoscalar and isovector densities Project leader: MarkusStatus: near completion Stability conditions in function of saturation density and momentum in infinite asymmetric nuclear matter Project leader: KazuhitoStatus: advanced, now on hold Spherical HO code for energy density functionals extended to N3LO terms with derivatives of densities up to sixth order Project leader: GillisStatus: in the initial phase

The FIDIPRO topics Nuclear and neutron matter properties for energy density functionals extended to N3LO terms with derivatives of densities up to sixth order Project leader: MarcinStatus: just initialized Adjustments of parameters in energy density functionals extended to N3LO terms with derivatives of densities up to sixth order Project leader: ?Status: planned Solution of the QRPA equations by the mean-filed plus Lanczos methods (I) proof of principle – spherical nuclei, HO basis, multipole modes Project leaders: Rayner&KazuhitoStatus: advanced Solution of the QRPA equations by the mean-filed plus Lanczos methods (II) axial nuclei, HO and/or spline basis,  -decay rates Project leader: ?Status: planned

The FIDIPRO topics Polarization effects exerted by odd particles in open-shell semi-magic nuclei along the Z=50 and N=50 lines Project leader: GillisStatus: on hold