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NSR database version of April 27, 2024.

Search: Author = J.Diaz-Cortes

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2020DI05      Phys.Lett. B 811, 135962 (2020)

J.Diaz-Cortes, J.Benlliure, J.L.Rodriguez-Sanchez, H.Alvarez-Pol, T.Aumann, C.A.Bertulani, B.Blank, E.Casarejos, D.Cortina-Gil, D.Dragosavac, V.Fohr, A.Gargano, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, A.Kelic-Heil, S.Lukic, F.Montes, D.Perez-Loureiro, L.Pienkowski, K.-H.Schmidt, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska

Systematic reduction of the proton-removal cross section in neutron-rich medium-mass nuclei

NUCLEAR REACTIONS ⁹Be(²³⁸U, X)¹³²Sn/¹³¹Sn/¹³¹In/¹²⁸Sn/¹³⁰Sn/¹³⁶Sn, E=950 MeV/nucleon; ⁹Be(¹³²Xe, X)¹¹⁹Sn/¹²⁴Sn/¹²⁶Sn, E=1200 MeV/nucleon; ⁹Be(¹¹⁹Sn, X), (¹²⁴Sn, X), (¹²⁶Sn, X), (¹³⁰Sn, X), (¹³¹Sn, X), (¹³²Sn, X), (¹²⁸Sn, X), (¹³⁶Sn, X), (¹³¹Sn, X), E ∼ 1000 MeV/nucleon; measured reaction products, TOF; deduced single neutron and single proton removal σ. Comparison with the advanced Liege intra-nuclear cascade (INCL) model calculations.

doi: 10.1016/j.physletb.2020.135962
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD8031.

2019PE09      Phys.Rev. C 99, 054606 (2019)

D.Perez-Loureiro, J.Benlliure, J.Diaz-Cortes, J.L.Rodriguez-Sanchez, H.Alvarez-Pol, B.Blank, E.Casarejos, D.Dragosavac, V.Fohr, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, A.Kelic-Heil, S.Lukic, F.Montes, L.Pienkowski, K-H.Schmidt, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska

Neutron-rich fragments produced by in-flight fission of ²³⁸U

NUCLEAR REACTIONS ²⁰⁸Pb(²³⁸U, F)⁹⁰Kr/⁹¹Kr/⁹⁴Rb/⁹⁵Rb/⁹⁶Rb/⁹⁷Rb/⁹⁸Rb/⁹⁹Rb/¹⁰⁰Rb/⁹⁶Sr/⁹⁷Sr/⁹⁸Sr/⁹⁹Sr/¹⁰⁰Sr/¹⁰¹Sr/¹⁰²Sr/¹⁰³Sr/⁹⁹Y/¹⁰⁰Y/¹⁰¹Y/¹⁰²Y/¹⁰³Y/¹⁰⁴Y/¹⁰⁵Y/¹⁰⁶Y/¹⁰²Zr/¹⁰³Zr/¹⁰⁴Zr/¹⁰⁵Zr/¹⁰⁶Zr/¹⁰⁷Zr/¹⁰⁸Zr/¹⁰⁹Zr/¹⁰⁴Nb/¹⁰⁵Nb/¹⁰⁶Nb/¹⁰⁷Nb/¹⁰⁸Nb/¹⁰⁹Nb/¹¹⁰Nb/¹¹¹Nb/¹⁰⁷Mo/¹⁰⁸Mo/¹⁰⁹Mo/¹¹⁰Mo/¹¹¹Mo/¹¹²Mo/¹¹³Mo/¹¹⁰Tc/¹¹¹Tc/¹¹²Tc/¹¹³Tc/¹¹⁴Tc/¹¹⁵Tc/¹¹⁶Tc/¹¹⁷Tc/¹¹²Ru/¹¹³Ru/¹¹⁴Ru/¹¹⁵Ru/¹¹⁶Ru/¹¹⁷Ru/¹¹⁸Ru/¹¹⁹Ru/¹¹⁵Rh/¹¹⁶Rh/¹¹⁷Rh/¹¹⁸Rh/¹¹⁹Rh/¹²⁰Rh/¹²¹Rh/¹²²Rh/¹¹⁸Pd/¹¹⁹Pd/¹²⁰Pd/¹²¹Pd/¹²²Pd/¹²³Pd/¹²⁴Pd/¹²⁵Pd/¹²⁰Ag/¹²¹Ag/¹²²Ag/¹²³Ag/¹²⁴Ag/¹²⁵Ag/¹²⁶Ag/¹²⁷Ag/¹²⁸Ag/¹²³Cd/¹²⁴Cd/¹²⁵Cd/¹²⁶Cd/¹²⁷Cd/¹²⁸Cd/¹²⁹Cd/¹³⁰Cd/¹³¹Cd/¹²⁶In/¹²⁷In/¹²⁸In/¹²⁹In/¹³⁰In/¹³¹In/¹³²In/¹³³In/¹³⁴In/¹³⁵In/¹²⁸Sn/¹²⁹Sn/¹³⁰Sn/¹³¹Sn/¹³²Sn/¹³³Sn/¹³⁴Sn/¹³⁵Sn/¹³⁶Sn/¹³⁷Sn/¹³²Sb/¹³³Sb/¹³⁴Sb/¹³⁵Sb/¹³⁶Sb/¹³⁷Sb/¹³⁸Sb/¹³⁹Sb/¹³⁵Te/¹³⁶Te/¹³⁷Te/¹³⁸Te/¹³⁹Te/¹⁴⁰Te/¹⁴¹Te/¹⁴²Te/¹³⁷I/¹³⁸I/¹³⁹I/¹⁴⁰I/¹⁴¹I/¹⁴²I/¹⁴³I/¹⁴⁴I/¹⁴¹Xe/¹⁴²Xe/¹⁴³Xe/¹⁴⁴Xe/¹⁴⁵Xe/¹⁴⁶Xe/¹⁴⁷Xe/¹⁴⁴Cs/¹⁴⁵Cs/¹⁴⁶Cs/¹⁴⁷Cs/¹⁴⁸Cs/¹⁴⁹Cs/¹⁴⁵Ba/¹⁴⁶Ba/¹⁴⁷Ba/¹⁴⁸Ba/¹⁴⁹Ba/¹⁵⁰Ba/¹⁵¹Ba/¹⁴⁸La/¹⁴⁹La/¹⁵⁰La/¹⁵¹La/¹⁵²La/¹⁵³La/¹⁵¹Ce/¹⁵²Ce/¹⁵³Ce/¹⁵⁴Ce/¹⁵²Pr/¹⁵³Pr/¹⁵⁵Pr/¹⁵⁵Nd/¹⁵⁶Nd, E=950 MeV/nucleon; ⁹Be(²³⁸U, F)⁸⁰Ga/⁸⁴Ga/⁷⁹Ge/⁸⁰Ge/⁸²Ge/⁸³Ge/⁸⁴Ge/⁸¹As/⁸²As/⁸³As/⁸⁵As/⁸⁶As/⁸⁷As/⁸⁸As/⁸⁴Se/⁸⁵Se/⁸⁷Se/⁸⁸Se/⁸⁹Se/⁹⁰Se/⁸⁶Br/⁸⁷Br/⁸⁸Br/⁸⁹Br/⁹¹Br/⁹²Br/⁹³Br/⁹⁴Br/⁸⁹Kr/⁹⁰Kr/⁹¹Kr/⁹²Kr/⁹³Kr/⁹⁴Kr/⁹⁵Kr/⁹⁶Kr/⁹⁷Kr/⁹²Rb/⁹³Rb/⁹⁴Rb/⁹⁵Rb/⁹⁶Rb/⁹⁷Rb/⁹⁸Rb/⁹⁹Rb/¹⁰⁰Rb/¹⁰¹Rb/⁹⁴Sr/⁹⁵Sr/⁹⁶Sr/⁹⁷Sr/⁹⁸Sr/⁹⁹Sr/¹⁰⁰Sr/¹⁰¹Sr/¹⁰²Sr/¹⁰³Sr/⁹⁹Zr/¹⁰⁰Zr/¹⁰¹Zr/¹⁰²Zr/¹⁰³Zr/¹⁰⁴Zr/¹⁰⁵Zr/¹⁰⁶Zr/¹⁰⁷Zr/¹⁰⁸Zr/¹⁰⁹Zr/¹⁰²Nb/¹⁰³Nb/¹⁰⁴Nb/¹⁰⁵Nb/¹⁰⁶Nb/¹⁰⁷Nb/¹⁰⁸Nb/¹⁰⁹Nb/¹¹⁰Nb/¹¹¹Nb/¹¹²Nb/¹⁰⁵Mo/¹⁰⁶Mo/¹⁰⁷Mo/¹⁰⁸Mo/¹⁰⁹Mo/¹¹⁰Mo/¹¹¹Mo/¹¹²Mo/¹¹³Mo/¹¹⁴Mo/¹¹⁵Mo/¹⁰⁷Tc/¹⁰⁸Tc/¹⁰⁹Tc/¹¹⁰Tc/¹¹¹Tc/¹¹²Tc/¹¹³Tc/¹¹⁴Tc/¹¹⁵Tc/¹¹⁶Tc/¹¹⁷Tc/¹¹⁸Tc/¹¹⁰Ru/¹¹¹Ru/¹¹²Ru/¹¹³Ru/¹¹⁴Ru/¹¹⁵Ru/¹¹⁶Ru/¹¹⁷Ru/¹¹⁸Ru/¹¹⁹Ru/¹²⁰Ru/¹¹³Rh/¹¹⁴Rh/¹¹⁷Pd/¹¹⁸Pd/¹¹⁹Pd/¹²⁰Pd/¹²¹Pd/¹²²Pd/¹²³Pd/¹²⁴Pd/¹²⁵Pd/¹¹⁸Ag/¹¹⁹Ag/¹²⁰Ag/¹²¹Ag/¹²²Ag/¹²³Ag/¹²⁴Ag/¹²⁵Ag/¹²⁶Ag/¹²⁷Ag/¹²⁸Ag/¹²¹Cd/¹²²Cd/¹²³Cd/¹²⁴Cd/¹²⁵Cd/¹²⁶Cd/¹²⁷Cd/¹²⁸Cd/¹²⁹Cd/¹³⁰Cd/¹³¹Cd/¹³²Cd/¹²³In/¹²⁴In/¹²⁵In/¹²⁶In/¹²⁷In/¹²⁸In/¹²⁹In/¹³⁰In/¹³¹In/¹³²In/¹³³In/¹³⁴In/¹²⁶Sn/¹²⁷Sn/¹²⁸Sn/¹²⁹Sn/¹³⁰Sn/¹³¹Sn/¹³²Sn/¹³³Sn/¹³⁴Sn/¹³⁵Sn/¹³⁶Sn/¹³⁷Sn/¹²⁹Sb/¹³³Te/¹³⁴Te/¹³⁵Te/¹³⁶Te/¹³⁷Te/¹³⁸Te/¹³⁹Te/¹⁴⁰Te/¹⁴¹Te/¹⁴²Te/¹⁴³Te/¹³⁵I/¹³⁶I/¹³⁷I/¹³⁸I/¹³⁹I/¹⁴⁰I/¹⁴¹I/¹⁴²I/¹⁴³I/¹⁴⁴I/¹⁴⁵I/¹³⁷Xe/¹³⁸Xe/¹³⁹Xe/¹⁴⁰Xe/¹⁴¹Xe/¹⁴²Xe/¹⁴³Xe/¹⁴⁴Xe/¹⁴⁵Xe/¹⁴⁶Xe/¹⁴⁷Xe/¹⁴⁰Cs/¹⁴¹Cs/¹⁴²Cs/¹⁴³Cs/¹⁴⁴Cs/¹⁴⁵Cs/¹⁴⁶Cs/¹⁴⁷Cs/¹⁴⁸Cs/¹⁴⁹Cs/¹⁴³Ba/¹⁴⁴Ba/¹⁴⁵Ba/¹⁴⁶Ba/¹⁴⁷Ba/¹⁴⁸Ba/¹⁴⁹Ba/¹⁵⁰Ba/¹⁵¹Ba/¹⁵²Ba/¹⁴⁶La/¹⁴⁷La/¹⁴⁸La/¹⁴⁹La, E=950 MeV/nucleon; measured fission fragments, isotopic distributions of the fission fragments, production σ and yields using zero-degree magnetic spectrometer Fragment Separator at GSI accelerator facilities; deduced mean neutron-to-proton ratio of fission fragments, role of Coulomb and nuclear excitation mechanisms in the neutron excess of the final fragments.

doi: 10.1103/PhysRevC.99.054606
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0955.

2017RO22      Phys.Rev. C 96, 034303 (2017)

J.L.Rodriguez-Sanchez, J.Benlliure, C.A.Bertulani, J.Vargas, Y.Ayyad, H.Alvarez-Pol, J.Atkinson, T.Aumann, S.Beceiro Novo, K.Boretzky, M.Caamano, E.Casarejos, D.Cortina-Gil, J.Diaz-Cortes, P.Diaz Fernandez, A.Estrade, H.Geissel, A.Kelic-Heil, Yu.A.Litvinov, M.Mostazo, C.Paradela, D.Perez-Loureiro, S.Pietri, A.Prochazka, M.Takechi, H.Weick, J.S.Winfield

Knockout and fragmentation reactions using a broad range of tin isotopes

NUCLEAR REACTIONS C(¹¹²Sn, X)¹⁰³Rh/¹⁰⁴Rh/¹⁰⁵Rh/¹⁰⁶Rh/¹⁰⁷Rh/¹⁰⁵Pd/¹⁰⁶Pd/¹⁰⁷Pd/¹⁰⁸Pd/¹⁰⁷Ag/¹⁰⁸Ag/¹⁰⁹Ag/¹¹⁰Ag/¹⁰⁹Cd/¹¹⁰Cd/¹¹¹Cd, E=1 GeV/nucleon; measured production cross sections of the most neutron-rich residues in the fragmentation of ¹¹²Sn beam at GSI. C(¹²⁴Sn, ¹²³Sn), (¹²⁴Sn, ¹²³In), (¹²⁰Sn, ¹¹⁹Sn), (¹²⁰Sn, ¹¹⁹In), (¹²⁰Sn, ¹¹⁸Cd), (¹¹²Sn, ¹¹¹Sn), (¹¹²Sn, ¹¹¹In), (¹¹⁰Sn, ¹⁰⁹Sn), (¹¹⁰Sn, ¹⁰⁹In), (¹¹⁰Sn, ¹⁰⁸Cd), E=1 GeV/nucleon; measured One- and two-nucleon-removal cross sections. Comparison with previous experimental data and with Glauber model calculations.

doi: 10.1103/PhysRevC.96.034303
Citations: PlumX Metrics