no code implementations • 6 Jan 2021 • V. Girard-Alcindor, I. Stefan, F. de Oliveira Santos, O. Sorlin, D. Ackermann, P. Adsley, J. C. Angelique, M. Assie, M. Assuncao, D. Beaumel, E. Berthoumieux, R. Borcea, L. Caceres, I. Celikovic, M. Ciemala, V. Chudoba, G. D Agata, F. de Grancey, G. Dumitru, F. Flavigny, C. Fougeres, S. Franchoo, A. Georgiadou, S. Grevy, J. Guillot, V. Guimaraes, F. Hammache, O. Kamalou, J. Kiener, S. Koyama, L. Lalanne, V. Lapoux, I. Matea, A. Matta, A. Meyer, P. Morfouace, J. Mrazek, F. Negoita, M. Niikura, D. Pantelica, L. Perrot, C. Petrone, J. Piot, C. Portail, T. Roger, F. Rotaru, A. M. Sanchez Benitez, N. de Sereville, M. Stanoiu, C. Stodel, K. Subotic, D. Suzuki, V. Tatischeff, J. C. Thomas, P. Ujic, D. Verney
The strength of the $nucleon-nucleon$ effective interaction involving the loosely bound proton in the $s_{1/2}$ orbit is significantly modified with respect to their mirror nuclei $^{16}$N and $^{15}$C.
Nuclear Experiment
no code implementations • 17 Dec 2020 • L. Maunoury, O. Kamalou, J. F. Cam, S. Damoy, P. Delahaye, M. Dubois, R. Frigot, S. Hormigos, C. Vandamme
Hence, it has been decided to focus our effort on that procedure as to get control of the 1+ beam optics leading to high charge breeding efficiencies whatever the 1+ mass, energy and Target Ion Source System (TISS) used.
Accelerator Physics
