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Testing nuclear forces by polarization transfer coefficients in d(p,p)d and d(p,d)p reactions at E=22.7 MeV

Authors :
M. Smoluchowski Institute of Physics, Jagiellonian University, PL-30059 Kraków, Poland
Institut für Theoretische Physik II, Ruhr-Universität Bochum, D-44780 Bochum, Germany
Institut für Kernphysik, Forschungszentrum Jülich, D-52425 Jülich, Germany
Jefferson Laboratory, Theory Division, Newport News, Virginia 23606, USA
Department of Physics, Faculty of Engineering, Kyushu Institute of Technology, 1-1 Sensuicho, Tobata, Kitakyushu 804-8550, Japan
Istituto Nazionale di Fisica Nucleare, Via Buonarroti 2, I-56100 Pisa, Italy
Witala, H
Golak, J
Skibinski, R
Glockle, W
Nogga, A
Epelbaum, E
Kamada, Hiroyuki
Kievsky, A
Viviani, M
M. Smoluchowski Institute of Physics, Jagiellonian University, PL-30059 Kraków, Poland
Institut für Theoretische Physik II, Ruhr-Universität Bochum, D-44780 Bochum, Germany
Institut für Kernphysik, Forschungszentrum Jülich, D-52425 Jülich, Germany
Jefferson Laboratory, Theory Division, Newport News, Virginia 23606, USA
Department of Physics, Faculty of Engineering, Kyushu Institute of Technology, 1-1 Sensuicho, Tobata, Kitakyushu 804-8550, Japan
Istituto Nazionale di Fisica Nucleare, Via Buonarroti 2, I-56100 Pisa, Italy
Witala, H
Golak, J
Skibinski, R
Glockle, W
Nogga, A
Epelbaum, E
Kamada, Hiroyuki
Kievsky, A
Viviani, M
Publication Year :
2017

Abstract

type:Journal Article<br />The proton to proton polarization transfer coefficients K,K, and K, and the proton to deuteron polarization transfer coefficients K,K,K, K,K,K,K, and K were measured in d(p,p)d and d(p,d)p reactions, respectively, at E=22.7 MeV. The data were compared to predictions of modern nuclear forces obtained by solving the three-nucleon Faddeev equations in momentum space. Realistic (semi)phenomenological nucleon-nucleon potentials combined with model three-nucleon forces and modern chiral nuclear forces were used. The AV18, CD Bonn, and Nijm I and II nucleon-nucleon interactions were applied alone or combined with the Tucson-Melbourne 99 three-nucleon force, adjusted separately for each potential to reproduce the triton binding energy. For the AV18 potential, the Urbana IX three-nucleon force was also used. In addition, chiral NN potentials in the next-to-leading order and chiral two- and three-nucleon forces in the next-to-next-to-leading order were applied. Only when three-nucleon forces are included does a satisfactory description of all data result. For the chiral approach, the restriction to the forces in the next-to-leading order is insufficient. Only when going over to the next-to-next-to-leading order does one get a satisfactory description of the data, similar to the one obtained with the (semi)phenomenological forces.<br />source:http://link.aps.org/abstract/PRC/v73/e044004<br />source:http://www.aps.org

Details

Database :
OAIster
Notes :
English
Publication Type :
Electronic Resource
Accession number :
edsoai.on1389680182
Document Type :
Electronic Resource