EPJ Web of Conferences (Jan 2023)
Fission studies in inverse kinematics with the R3B setup
- Graña-González A.,
- Rodríguez-Sánchez J.L.,
- Benlliure J.,
- García-Jiménez G.,
- Alvarez-Pol H.,
- Cortina-Gil D.,
- Atar L.,
- Audouin L.,
- Authelet G.,
- Besteiro A.,
- Blanchon G.,
- Boretzky K.,
- Borge M.J.G.,
- Cabanelas P.,
- Casarejos E.,
- Cederkall J.,
- Chatillon A.,
- Corsi A.,
- Feijoo M.,
- De Filippo E.,
- Galaviz D.,
- Gasparic I.,
- Geraci E.,
- Gernhäuser R.,
- Gnoffo B.,
- Heil M.,
- Heinz A.,
- Hensel T.,
- Holl M.,
- Jelavic Malenica D.,
- Jenegger T.,
- Ji L.,
- Johansson H.,
- Kiselev O.A.,
- Klenze P.,
- Knyazev A.,
- Körper D.,
- Kröll T.,
- Lihtar I.,
- Litvinov Y.,
- Löher B.,
- Martorana N.S.,
- Morfouace P.,
- Mücher D.,
- Murillo Morales S.,
- Obertelli A.,
- Panin V.,
- Park J.,
- Paschalis S.,
- Perea A.,
- Petri M.,
- Pirrone S.,
- Ponnath L.,
- Revel A.,
- Rhee H.-B.,
- Rose L.,
- Rossi D.M.,
- Russotto P.,
- Simon H.,
- Stott A.,
- Sun Y.,
- Sürder C.,
- Taïeb J.,
- Taniuchi R.,
- Tengblad O.,
- Törnqvist H.T.,
- Trimarchi M.,
- Velardita S.,
- Vesic J.,
- Voss B.
Affiliations
- Graña-González A.
- IGFAE, University of Santiago de Compostela
- Rodríguez-Sánchez J.L.
- IGFAE, University of Santiago de Compostela
- Benlliure J.
- IGFAE, University of Santiago de Compostela
- García-Jiménez G.
- IGFAE, University of Santiago de Compostela
- Alvarez-Pol H.
- IGFAE, University of Santiago de Compostela
- Cortina-Gil D.
- IGFAE, University of Santiago de Compostela
- Atar L.
- Technische Universität Darmstadt, Fachbereich Physik, Institut für Kernphysik
- Audouin L.
- IPN Orsay
- Authelet G.
- CEA Saclay, IRFU/DPhN, Centre de Saclay
- Besteiro A.
- CINTECX, Universidade de Vigo, DSN
- Blanchon G.
- CEA, DAM, DIF
- Boretzky K.
- GSI Helmholtzzentrum für Schwerionenforschung
- Borge M.J.G.
- Instituto de Estructura de la Materia, CSIC
- Cabanelas P.
- IGFAE, University of Santiago de Compostela
- Casarejos E.
- CINTECX, Universidade de Vigo, DSN
- Cederkall J.
- Department of Physics, Lund University
- Chatillon A.
- CEA, DAM, DIF
- Corsi A.
- CEA Saclay, IRFU/DPhN, Centre de Saclay
- Feijoo M.
- IGFAE, University of Santiago de Compostela
- De Filippo E.
- IGFAE, University of Santiago de Compostela
- Galaviz D.
- LIP and Faculty os Sciences, University of Lisbon
- Gasparic I.
- RBI Zagreb
- Geraci E.
- INFN Laboratori Nazionali del Sud
- Gernhäuser R.
- Technische Universität München
- Gnoffo B.
- INFN Laboratori Nazionali del Sud
- Heil M.
- GSI Helmholtzzentrum für Schwerionenforschung
- Heinz A.
- Institutionen för Fysik, Chalmers Tekniska Högskola
- Hensel T.
- Institut für Kern-und Teilchenphysik, Technische Universität Dresden
- Holl M.
- Institutionen för Fysik, Chalmers Tekniska Högskola
- Jelavic Malenica D.
- RBI Zagreb
- Jenegger T.
- Technische Universität München
- Ji L.
- Technische Universität Darmstadt, Fachbereich Physik, Institut für Kernphysik
- Johansson H.
- Institutionen för Fysik, Chalmers Tekniska Högskola
- Kiselev O.A.
- GSI Helmholtzzentrum für Schwerionenforschung
- Klenze P.
- Technische Universität München
- Knyazev A.
- Department of Physics, Lund University
- Körper D.
- GSI Helmholtzzentrum für Schwerionenforschung
- Kröll T.
- Technische Universität Darmstadt, Fachbereich Physik, Institut für Kernphysik
- Lihtar I.
- RBI Zagreb
- Litvinov Y.
- GSI Helmholtzzentrum für Schwerionenforschung
- Löher B.
- GSI Helmholtzzentrum für Schwerionenforschung
- Martorana N.S.
- INFN Laboratori Nazionali del Sud
- Morfouace P.
- CEA, DAM, DIF
- Mücher D.
- University of Guelph
- Murillo Morales S.
- School of Physics, Engineering and Technology, University of York
- Obertelli A.
- Technische Universität Darmstadt, Fachbereich Physik, Institut für Kernphysik
- Panin V.
- GSI Helmholtzzentrum für Schwerionenforschung
- Park J.
- Institute for Basic Science, Center for Exotic Nuclear Studies
- Paschalis S.
- School of Physics, Engineering and Technology, University of York
- Perea A.
- Instituto de Estructura de la Materia, CSIC
- Petri M.
- School of Physics, Engineering and Technology, University of York
- Pirrone S.
- INFN Laboratori Nazionali del Sud
- Ponnath L.
- Technische Universität München
- Revel A.
- CEA Saclay, IRFU/DPhN, Centre de Saclay
- Rhee H.-B.
- Technische Universität Darmstadt, Fachbereich Physik, Institut für Kernphysik
- Rose L.
- School of Physics, Engineering and Technology, University of York
- Rossi D.M.
- Technische Universität Darmstadt, Fachbereich Physik, Institut für Kernphysik
- Russotto P.
- INFN Laboratori Nazionali del Sud
- Simon H.
- GSI Helmholtzzentrum für Schwerionenforschung
- Stott A.
- School of Physics, Engineering and Technology, University of York
- Sun Y.
- Technische Universität Darmstadt, Fachbereich Physik, Institut für Kernphysik
- Sürder C.
- Technische Universität Darmstadt, Fachbereich Physik, Institut für Kernphysik
- Taïeb J.
- CEA, DAM, DIF
- Taniuchi R.
- School of Physics, Engineering and Technology, University of York
- Tengblad O.
- Instituto de Estructura de la Materia, CSIC
- Törnqvist H.T.
- Technische Universität Darmstadt, Fachbereich Physik, Institut für Kernphysik
- Trimarchi M.
- INFN Laboratori Nazionali del Sud
- Velardita S.
- Technische Universität Darmstadt, Fachbereich Physik, Institut für Kernphysik
- Vesic J.
- Jozef Stefan Institute
- Voss B.
- GSI Helmholtzzentrum für Schwerionenforschung
- DOI
- https://doi.org/10.1051/epjconf/202329002015
- Journal volume & issue
-
Vol. 290
p. 02015
Abstract
Nuclear fission is a complex dynamical process, whose description involves the coupling between intrinsic and collective degrees of freedom, as well as different quantum-mechanical phenomena. For this reason, to this day it still lacks a satisfactory and complete microscopic description. In addition to the importance of describing fission itself, studies of the r-process in astrophysics depend on fission observables to constrain the theoretical models that explain the isotopic abundances in the Universe. To improve on the existing data, fission reactions of heavy nuclei in inverse kinematics are produced in quasi-free (p,2p) scattering reactions, which induce fission through particle-hole excitations that can range from few to tens of MeV. In order to study the evolution of the fission yields with temperature, the excitation energy of the fissioning system must be reconstructed, which is possible by measuring the four-momenta of the two outgoing protons. Performing this kind of experiment requires a complex experimental setup, providing full isotopic identification of both fission fragments and an accurate measurement of the momenta of the two outgoing protons. This was realized recently at the GSI/FAIR facility and some of the results obtained for the charge distributions are presented in this work.
