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NSR database version of March 21, 2024.

Search: Author = M.Staniou

Found 8 matches.

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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.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0931. Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1956.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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