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NSR database version of May 24, 2024.

Search: Author = J.M.Boillos

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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2523. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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2015BO01      Phys.Rev. C 91, 034311 (2015)

J.M.Boillos, P.Sarriguren

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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