NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = M.Staniou Found 8 matches. 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
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
2018FE05 Phys.Lett. B 779, 124 (2018) B.Fernandez-Dominguez, B.Pietras, W.N.Catford, N.A.Orr, M.Petri, M.Chartier, S.Paschalis, N.Patterson, J.S.Thomas, M.Caamano, T.Otsuka, A.Poves, N.Tsunoda, N.L.Achouri, J.-C.Angelique, N.I.Ashwood, A.Banu, B.Bastin, R.Borcea, J.Brown, F.Delaunay, S.Franchoo, M.Freer, L.Gaudefroy, S.Heil, M.Labiche, B.Laurent, R.C.Lemmon, A.O.Macchiavelli, F.Negoita, E.S.Paul, C.Rodriguez-Tajes, P.Roussel-Chomaz, M.Staniou, M.J.Taylor, L.Trache, G.L.Wilson Re-examining the transition into the N = 20 island of inversion: Structure of 30Mg NUCLEAR REACTIONS C(31Mg, n)30Mg, E=55.1 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, single-particle σ, spectroscopic factors. Comparison with shell model calculations.
doi: 10.1016/j.physletb.2018.02.002
2011PE20 Phys.Lett. B 703, 552 (2011) D.Perez-Loureiro, J.Benlliure, 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 Production of neutron-rich nuclei in fragmentation reactions of 132Sn projectiles at relativistic energies NUCLEAR REACTIONS Pb(238U, X)132Sn, E=950 MeV/nucleon; Be(132Sn, X), E not given; measured reaction products; deduced σ. Comparison with code COFRA results.
doi: 10.1016/j.physletb.2011.08.037
2010BE24 Nucl.Phys. A834, 467c (2010) J.Benlliure, D.Dragosavac, D.Perez-Loureiro, H.Alvarez-Pol, B.Blank, E.Casarejos, V.Fohr, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, S.Lukic, F.Montes, L.Pienkowski, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska, M.Veselsky Investigating the radial distributions of medium-mass nuclei NUCLEAR REACTIONS 9Be(111Sn, X), (112Sn, X), (113Sn, X), (114Sn, X), (115Sn, X), (117Sn, X), (118Sn, X), (119Sn, X), (120Sn, X), (121Sn, X), (123Sn, X), (124Sn, X), (125Sn, X), (126Sn, X), (127Sn, X), (128Sn, X), (129Sn, X), (130Sn, X), (131Sn, X), (132Sn, X), (133Sn, X), (134Sn, X), (135Sn, X), E not given; measured total σ; analyzed σ, radii dependence, halo nuclei, neutron skin. Calculations using Glauber model optical limit and "black disk". Transmission method with FRS at GSI.
doi: 10.1016/j.nuclphysa.2010.01.066
2009PE12 Acta Phys.Pol. B40, 863 (2009) D.Perez-Loureiro, H.Alvarez-Pol, J.Benlliure, B.Blank, E.Casarejos, D.Dragosavac, V.Fohr, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, A.Kelic, S.Lukic, F.Montes, L.Pienkowski, K.-H.Schmidt, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska Production of Medium-Mass Neutron Rich Nuclei from Fragmentation of Fission Residues Around Sn
2003GI13 Nucl.Phys. A722, 434c (2003) J.Giovinazzo, B.Blank, C.Borcea, B.A.Brown, M.Chartier, S.Czajkowski, A.Fleury, R.Grzywacz, M.Lewitowicz, M.J.Lopez Jimenez, V.Maslov, F.de Oliveira-Santos, M.Pfutzner, M.S.Pravikoff, M.Staniou, J.-C.Thomas Two-proton decay of 48Fe: a new type of radioactivity RADIOACTIVITY 45Fe(2p) [from Ni(58Ni, X)]; measured Ep, T1/2, Q-value. Mass separator. NUCLEAR REACTIONS Ni(58Ni, X), E=75 MeV/nucleon; measured fragment yields.
doi: 10.1016/S0375-9474(03)01403-9
2001CA60 Eur.Phys.J. A 12, 377 (2001) G.Canchel, L.Achouri, J.Aysto, R.Beraud, B.Blank, E.Chabanat, S.Czajkowski, P.Dendooven, A.Emsallem, J.Giovinazzo, J.Honkanen, A.Jokinen, M.Lewitowicz, C.Longour, F.de Oliveira-Santos, K.Perajarvi, M.Staniou, J.C.Thomas The β-Delayed One- and Two-Proton Emission of 27S RADIOACTIVITY 27S(β+), (β+p), (β+2p) [from C(36Ar, X)]; measured Eγ, Ep, T1/2, branching ratios. Mass separator. NUCLEAR REACTIONS C(36Ar, X)27S/26P/25Si/24Al/23Mg, E=95 MeV/nucleon; measured relative yields. Mass separator.
doi: 10.1007/s10050-001-8659-z
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