NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.M.Boillos Found 4 matches. 2022BO01 Phys.Rev. C 105, 014611 (2022) J.M.Boillos, for the R3B Collaboration Isotopic cross sections of fragmentation residues produced by light projectiles on carbon near 400A MeV NUCLEAR REACTIONS C(12C, X)7Li/8Li/7Be/9Be/10Be/8B/10B/11B/11C, E=100-600, 450 MeV/nucleon; C(14N, X)7Be/9Be/10Be/11Be/8B/10B/11B/12B/10C/11C/12C/13C/14C/12N/13N, E=450 MeV/nucleon; C(13O, X)7Be/9Be/8B/10B/11B/9C/10C/11C/12C/12N, E=397 MeV/nucleon; C(14O, X)7Be/9Be/10Be/8B/10B/11B/9C/10C/11C/12C/11N/12N/13N, E=349 MeV/nucleon; C(15O, X)7Be/9Be/10Be/10B/11B/9C/10C/11C/12C/13C/12N/13N/14N/13O/14O, E=308 MeV/nucleon; C(16O, X)9Be/10Be/10B/11B/13B/10C/11C/12C/13C/14C/12N/14N/15N/14O/15O, E=450 MeV/nucleon; C(20O, X)10Be/11Be/12Be/10B/11B/12B/13B/14B/12C/13C/14C/15C/16C/13N/14N/15N/16N/17N/18N/19N/15O/16O/17O/18O/19O, E=415 MeV/nucleon; C(22O, X)9Be/10Be/11Be/11B/12B/13B/14B/15B/12C/13C/14C/15C/16C/17C/18C/19C/14N/15N/16N/17N/18N/19N/20N/21N/16O/17O/18O/19O/20O/21O, E=414 MeV/nucleon, [secondary beams produced in 9Be(40Ar, X), E=500 MeV/nucleon, using the FRS fragment separator at the UNILAC and SIS18 accelerators of GSI]; measured reaction products identified in mass and charge using the energy loss and time-of-flight methods, production σ(E), charged reaction fragments analyzed by a large-acceptance dipole magnet (ALADIN) and R3B/LAND setup at GSI. Comparison with different theoretical model calculations: ABRABLA07, INCL+Fermi breakup, and INCL+ABLA07, with their benchmarking. Comparison with available previous experimental results.
doi: 10.1103/PhysRevC.105.014611
2020SY01 Phys.Lett. B 809, 135748 (2020) I.Syndikus, M.Petri, A.O.Macchiavelli, S.Paschalis, C.A.Bertulani, T.Aumann, H.Alvarez-Pol, L.Atar, S.Beceiro Novo, J.Benlliure, J.M.Boillos, K.Boretzky, M.J.G.Borge, B.A.Brown, M.Caamano, C.Caesar, E.Casarejos, W.Catford, J.Cederkall, S.Chakraborty, L.V.Chulkov, D.Cortina-Gil, E.Cravo, R.Crespo, U.Datta Pramanik, I.Dillmann, P.Diaz Fernandez, Z.Elekes, J.Enders, F.Farinon, L.M.Fraile, D.Galaviz, H.Geissel, R.Gernhauser, P.Golubev, K.Gobel, M.Heil, M.Heine, A.Heinz, A.Henriques, M.Holl, H.T.Johansson, B.Jonson, N.Kalantar-Nayestanaki, R.Kanungo, A.Kelic-Heil, T.Kroll, N.Kurz, C.Langer, T.Le Bleis, J.Machado, J.Marganiec-Galazka, E.Nacher, T.Nilsson, C.Nociforo, V.Panin, A.Perea, S.B.Pietri, R.Plag, A.Rahaman, R.Reifarth, A.Revel, G.Ribeiro, C.Rigollet, D.M.Rossi, D.Savran, H.Scheit, H.Simon, O.Sorlin, O.Tengblad, Y.Togano, M.Vandebrouck, V.Volkov, F.Wamers, C.Wheldon, G.L.Wilson, J.S.Winfield, H.Weick, P.Woods, D.Yakorev, M.Zhukov, A.Zilges, K.Zuber Probing the Z=6 spin-orbit shell gap with (p, 2p) quasi-free scattering reactions NUCLEAR REACTIONS C, H(17N, X)16C, E=438 MeV/nucleon; C, H(19N, X)18C, E=430 MeV/nucleon; C, H(21N, X)20C, E=422 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced σ, spectroscopic factors, proton component of spin-orbit splitting.
doi: 10.1016/j.physletb.2020.135748
2019HO08 Phys.Lett. B 795, 682 (2019) M.Holl, V.Panin, H.Alvarez-Pol, L.Atar, T.Aumann, S.Beceiro Novo, J.Benlliure, C.A.Bertulani, J.M.Boillos, K.Boretzky, M.Caamano, C.Caesar, E.Casarejos, W.Catford, J.Cederkall, L.Chulkov, D.Cortina-Gil, E.Cravo, I.Dillmann, P.Diaz Fernandez, Z.Elekes, J.Enders, L.M.Fraile, D.Galaviz-Redondo, R.Gernhauser, P.Golubev, T.Heftrich, M.Heil, M.Heine, A.Heinz, A.Henriques, H.T.Johansson, B.Jonson, N.Kalantar-Nayestanaki, R.Kanungo, A.Kelic-Heil, T.Kroll, N.Kurz, C.Langer, T.Le Bleis, S.Lindberg, J.Machado, E.Nacher, M.A.Najafi, T.Nilsson, C.Nociforo, S.Paschalis, M.Petri, R.Reifarth, G.Ribeiro, C.Rigollet, D.M.Rossi, D.Savran, H.Scheit, H.Simon, O.Sorlin, I.Syndikus, O.Tengblad, Y.Togano, M.Vandebrouck, P.Velho, F.Wamers, H.Weick, C.Wheldon, G.L.Wilson, J.S.Winfield, P.Woods, M.Zhukov, K.Zuber Quasi-free neutron and proton knockout reactions from light nuclei in a wide neutron-to-proton asymmetry range NUCLEAR REACTIONS 1H(11C, 2p), (10C, np), (11C, np), (12C, np), E=300-400 MeV/nucleon; measured reaction products, Ep, Ip, En, In; deduced σ and momentum distributions. Comparison with DWIA calculations.
doi: 10.1016/j.physletb.2019.06.069
2015BO01 Phys.Rev. C 91, 034311 (2015) Effects of deformation on the β-decay patterns of light even-even and odd-mass Hg and Pt isotopes NUCLEAR STRUCTURE 176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192Hg, 172,173,174,175,176,177,178,179,180,181,182,183,184,185,186Pt; calculated deformation energy curves as function of β, quadrupole deformation parameter, rms radii, Gamow-Teller strength distributions; deduced signatures of nuclear deformation. Self-consistent Skyrme-Hartree-Fock calculations with pairing and QRPA correlations. RADIOACTIVITY 176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192Hg, 172,173,174,175,176,177,178,179,180,181,182,183,184,185,186Pt(EC), (β+); calculated half-lives, Gamow-Teller strength distributions. Self-consistent Skyrme-Hartree-Fock calculations with pairing and QRPA correlations. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.034311
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