2010/11/08 by T. M. Partanen, J. A. Niskanen, J.A. Niskanen · 4 citations
Physics and Astronomy · #Atomic and Molecular Physics #Atomic physics #Deuterium #Excitation #Hamiltonian (control theory) #Isobar #Neutron #Nuclear physics #Nuclear physics research studies #Nucleon #Parity (physics) #Particle physics #Photodisintegration #Photon #Physics #Quantum Chromodynamics and Particle Interactions #Quantum mechanics #nucl-th
paper · pdf · doi:10.1140/epja/i2011-11053-0
published in The European Physical Journal A 47(4) (Springer Science+Business Media) · 14 pages, 13 figures (18 eps files), LaTeX2e
arxiv created 2010/11/08 · openalex publication_date 2011/04/01 · arxiv updated 2011/05/09 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We calculate the asymmetries in parity nonconserving deuteron photodisintegration due to circularly polarized photons gamma+d to n+p with the photon laboratory energy ranging from the threshold up to 10 MeV and the radiative capture of thermal polarized neutrons by protons n+p to gamma+d. We use the leading order electromagnetic Hamiltonian neglecting the smaller nuclear exchange currents. Comparative calculations are done by using the Reid93 and Argonne v18 potentials for the strong interaction and the DDH and FCDH "best" values for the weak couplings in a weak one-meson exchange potential. A weak NDelta transition potential is used to incorporate also the Delta(1232)-isobar excitation in the coupled-channels formalism.