13–19 Jun 2015
University of Alberta
America/Edmonton timezone
Welcome to the 2015 CAP Congress! / Bienvenue au congrès de l'ACP 2015!

Session

M1-7 Advances in Nuclear Physics and Particle Physics Theory (DNP-PPD-DTP) / Progrès en physique nucléaire et en physique des particules théoriques (DPN-PPD-DPT)

M1-7
15 Jun 2015, 13:45
University of Alberta

University of Alberta

Edmonton, AB

Conveners

M1-7 Advances in Nuclear Physics and Particle Physics Theory (DNP-PPD-DTP) / Progrès en physique nucléaire et en physique des particules théoriques (DPN-PPD-DPT)

  • Pierre Ouimet (University of Regina)

Presentation materials

There are no materials yet.

  1. Petr Navratil (TRIUMF)
    15/06/2015, 13:45
    Nuclear Physics / Physique nucléaire (DNP-DPN)
    Invited Speaker / Conférencier invité
    The description of nuclei starting from the constituent nucleons and the realistic interactions among them has been a long-standing goal in nuclear physics. In recent years, a significant progress has been made in developing ab initio many-body approaches capable of describing both bound and scattering states in light and medium mass nuclei based on input from QCD employing Hamiltonians...
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  2. Dr Juris P. Svenne (University of Manitoba, Dept. of Physics and Astronomy)
    15/06/2015, 14:15
    Nuclear Physics / Physique nucléaire (DNP-DPN)
    Oral (Non-Student) / orale (non-étudiant)
    The Multi-Channel Algebraic-Scattering (MCAS) method, developed in 2003 for the analysis of low-energy nuclear spectra and of resonant scattering, continues to be effectively used for nuclear-structure studies. The MCAS approach allows the construction of the nucleon-core model Hamiltonian which can be defined in detail (coupling to the collective modes, rotational or vibrational, diverse...
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  3. Mr Gaëtan Landry (Dalhousie University)
    15/06/2015, 14:30
    Industrial and Applied Physics / Physique industrielle et appliquée (DIAP-DPIA)
    Oral (Non-Student) / orale (non-étudiant)
    The bouncing of sports balls is often characterized in terms of the coefficient of restitution, which represents the ratio of the after-impact velocity to the before-impact velocity. While the behaviour of the coefficient of restitution as a function of the internal pressure of the ball has been studied, no theoretical justification has been given for any parametric curve fitted to the data....
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