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NSR database version of May 24, 2024.

Search: Author = A.Kelic-Heil

Found 43 matches.

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2023RO03      Phys.Rev.Lett. 130, 132501 (2023)

J.L.Rodriguez-Sanchez, J.Cugnon, J.-C.David, J.Hirtz, A.Kelic-Heil, I.Vidana

Constraint of the Nuclear Dissipation Coefficient in Fission of Hypernuclei

NUCLEAR REACTIONS 209Bi, 238U(p, F), E=1-2.4 GeV/nucleon; calculated hypernuclear fission σ. Comparison with experimental data.

doi: 10.1103/PhysRevLett.130.132501
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2022CH38      Phys.Rev. C 106, 024618 (2022)

A.Chatillon, J.Taieb, A.Heinz, H.Alvarez-Pol, L.Audouin, Y.Ayyad, G.Belier, J.Benlliure, G.Boutoux, M.Caamano, E.Casarejos, D.Cortina-Gil, A.Ebran, F.Farget, B.Fernandez-Dominguez, T.Gorbinet, L.Grente, H.T.Johansson, B.Jurado, A.Kelic-Heil, N.Kurz, B.Laurent, J.-F.Martin, C.Nociforo, C.Paradela, E.Pellereau, S.Pietri, A.Prochazka, J.L.Rodriguez-Sanchez, D.Rossi, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Influence of proton and neutron deformed shells on the asymmetric fission of thorium isotopes

NUCLEAR REACTIONS 222,223,225,226,229,230Th, 228,229,231,232Pa, 234,235,238U, 238Np(γ, F), E=13-14 MeV; 219,223,227Ac(γ, F), E ≈ 16 MeV; analyzed elemental, isotonic, and isobaric experimental fission fragment yields in Coulex experiments obtained at R3B/SOFIA setups (2019CH20); deduced average value of the atomic number of the light and heavy fission fragments, centroid positions of the light and heavy peaks of the isotonic yields, average total prompt-neutron multiplicity. Discussed the influence of deformed neutron and proton shells on the fission process.

doi: 10.1103/PhysRevC.106.024618
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2022RO02      Phys.Rev. C 105, 014623 (2022)

J.L.Rodriguez-Sanchez, J.Cugnon, J.-C.David, J.Hirtz, A.Kelic-Heil, S.Leray

Hypernuclei formation in spallation reactions by coupling the Liege intranuclear cascade model to the deexcitation code ABLA

NUCLEAR REACTIONS 209Bi(p, X), E=10 GeV; 12C(Mg, X), E=1 GeV/nucleon; calculated separation energy of the Λ hyperon and S(2n) for 208Pb hypernuclei as a function of the hypernucleus mass number. 1H(136Xe, X), (208Pb, X), (238U, X), E=1000 MeV/nucleon; calculated production σ for Z=10-90 nuclei using INCL+ABLA07, INCL+ABLA, and INCL+SMM model calculations, probability of nuclear fission and evaporation residues surviving to the emission of light particles using ABLA and SMM models for 209Bi and 238U compound nuclei and hypernuclei, hypernuclear production cross sections as a function of the target mass number. 1H(238U, X), E=1.5, 3, 6 GeV/nucleon; calculated Λ-hypernuclei probability as a function of the hypernuclei mass number, isotopic production cross sections of Λ hypernuclei. Liege intranuclear cascade model coupled with a new version of the ablation (ABLA) model for the evaporation of Λ particles from hot hyperremnants during the intranuclear cascade stage. Comparison with available experimental data.

doi: 10.1103/PhysRevC.105.014623
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2022RO11      Phys.Rev. C 106, 014618 (2022)

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

Systematic study of Δ(1232) resonance excitations using single isobaric charge-exchange reactions induced by medium-mass projectiles of Sn

NUCLEAR REACTIONS 1H, 12C, Cu, Pb(112Sn, 112In), (112Sn, 112Sb), 1H, C(124Sn, 124Sb), E=1 GeV/nucleon; measured reaction products; deduced total σ, quasielastic and inelastic σ; missing energy spectra. Observed energy shift for the Δ-resonance peak of about 63 ± 5 MeV and quenching of the quasielastic component. Comparison to theoretical predictions using random phase approximation (RPA) with Giessen energy density functional (GiEDF). FRS spectrometer with SIS-18 synchrotron beam (GSI).

doi: 10.1103/PhysRevC.106.014618
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2021MA68      Phys.Rev. C 104, 044602 (2021)

J.-F.Martin, J.Taieb, G.Boutoux, A.Chatillon, T.Gorbinet, E.Pellereau, L.Audouin, A.Heinz, H.Alvarez-Pol, Y.Ayyad, G.Belier, J.Benlliure, M.Caamano, E.Casarejos, D.Cortina-Gil, A.Ebran, F.Farget, B.Fernandez-Dominguez, L.Grente, H.T.Johansson, B.Jurado, A.Kelic-Heil, N.Kurz, B.Laurent, C.Nociforo, C.Paradela, S.Pietri, A.Prochazka, J.L.Rodriguez-Sanchez, D.Rossi, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Fission-fragment yields and prompt-neutron multiplicity for Coulomb-induced fission of 234, 235U and 237, 238Np

NUCLEAR REACTIONS 238U(234U, F), (235U, F), (237Np, F), (238Np, F), E=555 MeV/nucleon in the center of the target, [secondary 234,235U, 237,238Np beams from 9Be(238U, X), E=1 GeV/nucleon primary reaction, followed by separation of reaction products using FRS separator at GSI facility]; measured fission fragments, (fragment)(fragment)-coin, Coulomb excitation induced fission σ(A, Z), electromagnetic-induced fission yields, mass and charge distribution of fission fragments, isotonic, isobaric, and isotopic fission yields produced for Coulomb-induced fission using the Reactions with Relativistic Radioactive Beams/Studies On FIssion with Aladin (R3B/SOFIA) apparatus at GSI facility. 234,235,238U, 237,238Np(γ, F), virtual photons from Coulomb excitation; deduced yields Y(A, Z), σ(A, Z), prompt-neutron and total neutron multiplicities ν(A, Z) for A=77-157, Z=28-64, and N=45-97 fragments: 77,78,79,80,81,82,83,84Ge, 78,79,80,81,82,83,84,85,86,87As, 80,81,82,83,84,85,86,87,88,89Se, 83,84,85,86,87,88,89,90,91Br, 85,86,87,88,89,90,91,92,93Kr, 87,88,89,90,91,92,93,94,95,96Rb, 90,91,92,93,94,95,96,97,98Sr, 92,93,94,95,96,97,98,99,100,101Y, 95,96,97,98,99,100,101,102,103Zr, 97,98,99,100,101,102,103,104,105,106Nb, 100,101,102,103,104,105,106,107,108Mo, 103,104,105,106,107,108,109,110,111Tc, 102,103,104,105,106,107,108,109,110,111,112,113,114Ru, 108,109,110,111,112,113,114,115,116,117Rh, 110,111,112,113,114,115,116,117,118,119,120Pd, 113,114,115,116,117,118,119,120,121,122Ag, 115,116,117,118,119,120,121,122,123,124,125,126Cd, 118,119,120,121,122,123,124,125,126,127,128,129In, 121,122,123,124,125,126,127,128,129,130,131,132,133Sn, 124,125,126,127,128,129,130,131,132,133,134,135Sb, 127,128,129,130,131,132,133,134,135,136,137Te, 130,131,132,133,134,135,136,137,138,139,140I, 132,133,134,135,136,137,138,139,140,141,142Xe, 135,136,137,138,139,140,141,142,143,144Cs, 137,138,139,140,141,142,143,144,145,146,147Ba, 139,140,141,142,143,144,145,146,147,148,149,150La, 142,143,144,145,146,147,148,149,150,151,152Ce, 144,145,146,147,148,149,150,151,152,153,154Pr, 146,147,148,149,150,151,152,153,154,155,156,157Nd, 151,152,153,154,155,156, and 157Pm, average values of atomic, neutron, and mass numbers for the light and heavy fission fragments, proton even-odd staggering, neutron excess of pre-neutron-evaporation fission fragments produced for Coulomb-induced fission. Comparison with previous measurements using (γ, F) and thermal-neutron induced fission. Comparison with theoretical reaction model calculations using GEF-2019V1.1 code, unchanged charge density (UCD) approach, and by fission treated as an adiabatic process in a Fermi gas (FA). Numerical values of yields, cross sections and neutron multiplicities are listed in the Supplemental Material of this work.

doi: 10.1103/PhysRevC.104.044602
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2020CH18      Phys.Rev.Lett. 124, 202502 (2020)

A.Chatillon, J.Taieb, H.Alvarez-Pol, L.Audouin, Y.Ayyad, G.Belier, J.Benlliure, G.Boutoux, M.Caamano, E.Casarejos, D.Cortina-Gil, A.Ebran, F.Farget, B.Fernandez-Dominguez, T.Gorbinet, L.Grente, A.Heinz, H.T.Johansson, B.Jurado, A.Kelic-Heil, N.Kurz, B.Laurent, J.-F.Martin, C.Nociforo, C.Paradela, E.Pellereau, S.Pietri, A.Prochazka, J.L.Rodriguez-Sanchez, D.Rossi, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Evidence for a New Compact Symmetric Fission Mode in Light Thorium Isotopes

NUCLEAR REACTIONS 222,226,230Th(γ, F)1NN, E not given; measured reaction products, En, In; deduced prompt-neutron emission probability, σ(E), yields.

doi: 10.1103/PhysRevLett.124.202502
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0076.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD8031.


2020RO12      Phys.Lett. B 807, 135565 (2020)

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

Study of Δ excitations in medium-mass nuclei with peripheral heavy ion charge-exchange reactions

NUCLEAR REACTIONS C(112Sn, 112In), E=1 GeV/nucleon; analyzed available data; deduced missing spectra, change in the relative magnitude between the contribution of the excitation of the resonance in the target and in the projectile.

doi: 10.1016/j.physletb.2020.135565
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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.


2019CH20      Phys.Rev. C 99, 054628 (2019)

A.Chatillon, J.Taieb, H.Alvarez-Pol, L.Audouin, Y.Ayyad, G.Belier, J.Benlliure, G.Boutoux, M.Caamano, E.Casarejos, D.Cortina-Gil, A.Ebran, F.Farget, B.Fernandez-Dominguez, T.Gorbinet, L.Grente, A.Heinz, H.T.Johansson, B.Jurado, A.Kelic-Heil, N.Kurz, B.Laurent, J.-F.Martin, C.Nociforo, C.Paradela, E.Pellereau, S.Pietri, A.Prochazka, J.L.Rodriguez-Sanchez, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Experimental study of nuclear fission along the thorium isotopic chain: From asymmetric to symmetric fission

NUCLEAR REACTIONS 208Pb, 238U(219Ac, F), (220Ac, F), (223Ac, F), (227Ac, F), (221Th, F), (222Th, F), (223Th, F), (225Th, F), (226Th, F), (229Th, F), (230Th, F), (228Pa, F), (229Pa, F), (219Ac, F), (220Ac, F), (223Ac, F), (227Ac, F), (221Th, F), (222Th, F), (223Th, F), (225Th, F), (226Th, F), (229Th, F), (230Th, F), (228Pa, F), (229Pa, F), E=551.7-568.9 MeV/nucleon, [secondary Ac and Th beams from 9Be(238U, X), E=1 GeV/nucleon primary reaction, and using FRS separator at GSI facility for separation of reaction products]; measured fission fragments, (fragment)(fragment)-coin, Coulomb excitation induced fission σ, differential Coulomb excitation σ(θ), electromagnetic-induced fission yields, mass and charge distribution of fission fragments, isotonic and isobaric fission yields using the Reactions with Relativistic Radioactive Beams/Studies On FIssion with Aladin (R3B/SOFIA) apparatus at GSI accelerator facility. Comparison with local even-odd staggering, previous measurements using either the same reaction mechanism and/or thermal-neutron induced fission.

doi: 10.1103/PhysRevC.99.054628
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0074.


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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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0955.


2017PA10      Phys.Rev. C 95, 044606 (2017)

C.Paradela, L.Tassan-Got, J.Benlliure, J.L.Rodriguez-Sanchez, L.Audouin, A.Boudard, E.Casarejos, T.Enqvist, J.E.Ducret, F.Farget, B.Fernandez-Dominguez, M.Fernandez-Ordonez, L.Giot, A.Heinz, V.Henzl, D.Henzlova, A.Kelic-Heil, A.Lafriaskh, S.Leray, P.Napolitani, J.Pereira, D.Perez-Loureiro, M.V.Ricciardi, C.Stephan, K.-H.Schmidt, C.Schmitt, C.Villagrasa, C.Volant, O.Yordanov

Isotopic production cross sections of residual nuclei in the spallation reaction 136Xe (200A MeV) + p

NUCLEAR REACTIONS 1H(136Xe, X)115Cd/116Cd/115In/116In/117In/118In/119In/120In/115Sn/116Sn/117Sn/118Sn/119Sn/120Sn/121Sn/122Sn/123Sn/115Sb/116Sb/117Sb/118Sb/119Sb/120Sb/121Sb/122Sb/123Sb/124Sb/125Sb/126Sb/127Sb/128Sb/117Te/118Te/119Te/120Te/121Te/122Te/123Te/124Te/125Te/126Te/127Te/128Te/129Te/130Te/131Te/132Te/119I/120I/121I/122I/123I/124I/125I/126I/127I/128I/129I/130I/131I/132I/133I/134I/135I/120Xe/121Xe/122Xe/123Xe/124Xe/125Xe/126Xe/127Xe/128Xe/129Xe/130Xe/131Xe/132Xe/133Xe/134Xe/135Xe/121Cs/122Cs/123Cs/124Cs/125Cs/126Cs/127Cs/128Cs/129Cs/130Cs/131Cs/132Cs/133Cs/134Cs/135Cs/136Cs, E=200 MeV/nucleon; measured charge distribution, energy loss and isotopic σ(A, Z) and isobaric σ(A) of the fragments using the FRS separator and multisampling ionization chambers (MUSICs) at GSI; deduced correlation plot between atomic number (Z) and mass-over-charge ratio (A/Z), identification plot, correlation between the mass identification in the two FRS sections, momentum distribution of the 125Xe. Comparison with theoretical predictions using INCL4.6 and ISABEL codes coupled to the deexcitation code ABLA07.

doi: 10.1103/PhysRevC.95.044606
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2017PE08      Phys.Rev. C 95, 054603 (2017)

E.Pellereau, J.Taieb, A.Chatillon, H.Alvarez-Pol, L.Audouin, Y.Ayyad, G.Belier, J.Benlliure, G.Boutoux, M.Caamano, E.Casarejos, D.Cortina-Gil, A.Ebran, F.Farget, B.Fernandez-Dominguez, T.Gorbinet, L.Grente, A.Heinz, H.Johansson, B.Jurado, A.Kelic-Heil, N.Kurz, B.Laurent, J.-F.Martin, C.Nociforo, C.Paradela, S.Pietri, J.L.Rodriguez-Sanchez, K.-H.Schmidt, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Accurate isotopic fission yields of electromagnetically induced fission of 238U measured in inverse kinematics at relativistic energies

NUCLEAR REACTIONS 238U(238U, F), E=650 MeV/nucleon; measured mass and charge coincidences, elemental, isobaric and isotopic yields and mass distribution of fission fragments of Z=29-62, N=43-95, A=71-156 in 238U(γ, F) using the SOFIA experimental setup and around the ALADIN magnet at GSI. Comparison with the GEF model calculations, and with 238U(n, F) data in ENDF-BVII.1 and JEFF.3.1.

doi: 10.1103/PhysRevC.95.054603
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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
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2017TU01      Phys.Rev. C 95, 014610 (2017)

X.L.Tu, A.Kelic-Heil, Yu.A.Litvinov, Zs.Podolyak, Y.H.Zhang, W.J.Huang, H.S.Xu, K.Blaum, F.Bosch, R.J.Chen, X.C.Chen, C.Y.Fu, B.S.Gao, Z.Ge, Z.G.Hu, D.W.Liu, S.A.Litvinov, X.W.Ma, R.S.Mao, B.Mei, P.Shuai, B.H.Sun, Y.Sun, Z.Y.Sun, P.M.Walker, M.Wang, N.Winckler, J.W.Xia, G.Q.Xiao, Y.M.Xing, X.Xu, T.Yamaguchi, X.L.Yan, J.C.Yang, Y.J.Yuan, Q.Zeng, W.Zhang, H.W.Zhao, T.C.Zhao, X.H.Zhou

Application of isochronous mass spectrometry for the study of angular momentum population in projectile fragmentation reactions

NUCLEAR REACTIONS 9Be(78Kr, X)53Fe/53mFe/53Co/53mCo, E=479.4 MeV/nucleon; measured revolution time spectra of the isomeric and ground states of 53Co and 53Fe using isochronous mass spectrometry (IMS) technique at HIRFL-CSR-Lanzhou facility; deduced isomeric ratios for the 19/2 state, and compared with the predictions of theoretical calculations using ABRABLA07 code. 53Fe; calculated production probability of 53Fe versus spin using ABRABLA07 code for the 58Ni, 78Kr, 84Kr, and 112Sn projectiles.

doi: 10.1103/PhysRevC.95.014610
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2016ME15      Phys.Rev. C 94, 044615 (2016)

B.Mei, H.S.Xu, Y.H.Zhang, M.Wang, X.L.Tu, K.-H.Schmidt, Yu.A.Litvinov, Z.Y.Sun, X.H.Zhou, Y.J.Yuan, K.Blaum, M.V.Ricciardi, A.Kelic-Heil, R.S.Mao, Z.G.Hu, P.Shuai, Y.D.Zang, X.W.Ma, X.Y.Zhang, J.W.Xia, G.Q.Xiao, Z.Y.Guo, J.C.Yang, X.H.Zhang, X.Xu, X.L.Yan, W.Zhang, W.L.Zhan

Odd-even staggering in yields of neutron-deficient nuclei produced by projectile fragmentation

NUCLEAR REACTIONS 9Be(58Ni, X), E=463 MeV/nucleon; measured neutron-deficient fragment, revolution-time spectrum, fragment yields and particle-emission threshold energy (PETE) of Tz=-3/2 and -1 nuclei using fragment separator RIBLL2 and experimental Cooler Storage Ring (CSRe) at HIRFL-Lanzhou facility; deduced odd-even staggering (OES) of fragment yields.

doi: 10.1103/PhysRevC.94.044615
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2016PA02      Phys.Lett. B 753, 204 (2016)

V.Panin, J.T.Taylor, S.Paschalis, F.Wamers, Y.Aksyutina, H.Alvarez-Pol, T.Aumann, C.A.Bertulani, K.Boretzky, C.Caesar, M.Chartier, L.V.Chulkov, D.Cortina-Gil, J.Enders, O.Ershova, H.Geissel, R.Gernhauser, M.Heil, H.T.Johansson, B.Jonson, A.Kelic-Heil, C.Langer, T.Le Bleis, R.Lemmon, T.Nilsson, M.Petri, R.Plag, R.Reifarth, D.Rossi, H.Scheit, H.Simon, H.Weick, C.Wimmer

Exclusive measurements of quasi-free proton scattering reactions in inverse and complete kinematics

NUCLEAR REACTIONS C, 1H(12C, 2p)10B/11B, E=400 MeV/nucleon; measured reaction products, Ep, Ip; deduced σ(θ), σ(E), σ and corresponding spectroscopic factors. Comparison with theoretical calculations employing the eikonal formalism.

doi: 10.1016/j.physletb.2015.11.082
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2016RO20      Phys.Rev. C 94, 034605 (2016)

J.L.Rodriguez-Sanchez, J.Benlliure, C.Paradela, Y.Ayyad, E.Casarejos, H.Alvarez-Pol, L.Audouin, G.Belier, G.Boutoux, A.Chatillon, D.Cortina-Gil, T.Gorbinet, A.Heinz, A.Kelic-Heil, B.Laurent, J.-F.Martin, E.Pellereau, B.Pietras, D.Ramos, C.Rodriguez-Tajes, D.M.Rossi, H.Simon, J.Taieb, J.Vargas, B.Voss

Light charged particles emitted in fission reactions induced by protons on 208Pb

NUCLEAR REACTIONS 1H(208Pb, F), E=370, 500, 650 MeV/nucleon; 27Al(208Pb, F), E=500 MeV/nucleon; measured light charged particles, fission fragments, (light charged particles)(fission fragments)-coin using SOFIA detection system at GSI facility; deduced multiplicity distribution of particles with Z=1, width of the atomic-number distribution of the fission fragments as function of the atomic number of the light charged particle, transient time and dissipative effects. Comparison with model calculations.

doi: 10.1103/PhysRevC.94.034605
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2016RO29      Phys.Rev. C 94, 061601 (2016)

J.L.Rodriguez-Sanchez, J.Benlliure, J.Taieb, H.Alvarez-Pol, L.Audouin, Y.Ayyad, G.Belier, G.Boutoux, E.Casarejos, A.Chatillon, D.Cortina-Gil, T.Gorbinet, A.Heinz, A.Kelic-Heil, B.Laurent, J.-F.Martin, C.Paradela, E.Pellereau, B.Pietras, D.Ramos, C.Rodriguez-Tajes, D.M.Rossi, H.Simon, J.Vargas, B.Voss

Presaddle and postsaddle dissipative effects in fission using complete kinematics measurements

NUCLEAR REACTIONS 1H(208Pb, F), E=500 MeV/nucleon; measured fission fragments, fission cross sections, prescission neutron multiplicities and average neutron excess of the final fission fragments as function of atomic number of fissioning nuclei by magnetic rigidity and time-of-flight techniques at GSI facility. Kinematics of the two fission fragments used for the first time to investigate fission dynamics at small and large deformations. Comparison of measured cross sections with model calculations using INCL4.6+ABLA07 codes.

doi: 10.1103/PhysRevC.94.061601
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2015AL19      Phys.Rev. C 92, 024607 (2015)

J.Alcantara-Nunez, J.Benlliure, C.Paradela, C.Perez-Loureiro, J.L.Rodriguez-Sanchez, L.Audouin, A.Boudard, E.Casarejos, T.Enqvist, F.Farget, M.Fernandez-Ordonez, A.Heinz, V.Henzl, D.Henzlova, A.Kelic-Heil, A.Lafriaskh, S.Leray, P.Napolitani, J.Pereira, M.V.Ricciardi, C.Stephan, K.-H.Schmidt, C.Schmitt, L.Tassan-Got, C.Villagrasa, C.Volant, O.Yordanov

Isotopic yields of spallation residues produced in 136Xe-induced reactions on deuterium at 500 A MeV

NUCLEAR REACTIONS 2H(136Xe, X)37Ar/38Ar/39Ar/40Ar/41Ar/42Ar/38K/39K/40K/41K/42K/43K/44K/45K/40Ca/41Ca/42Ca/43Ca/44Ca/45Ca/46Ca/47Ca/42Sc/43Sc/44Sc/45Sc/46Sc/47Sc/48Sc/49Sc/50Sc/44Ti/45Ti/46Ti/47Ti/48Ti/49Ti/50Ti/51Ti/52Ti/46V/47V/48V/49V/50V/51V/52V/53V/54V/55V/56V/48Cr/49Cr/50Cr/51Cr/52Cr/53Cr/54Cr/55Cr/56Cr/57Cr/58Cr/50Mn/51Mn/52Mn/53Mn/54Mn/55Mn/56Mn/57Mn/58Mn/59Mn/60Mn/61Mn/52Fe/53Fe/54Fe/55Fe/56Fe/57Fe/58Fe/59Fe/60Fe/61Fe/62Fe/63Fe/54Co/55Co/56Co/57Co/58Co/59Co/60Co/61Co/62Co/63Co/64Co/65Co/56Ni/57Ni/58Ni/59Ni/60Ni/61Ni/62Ni/63Ni/64Ni/65Ni/66Ni/67Ni/68Ni/59Cu/60Cu/61Cu/62Cu/63Cu/64Cu/65Cu/66Cu/67Cu/68Cu/69Cu/70Cu/61Zn/62Zn/63Zn/64Zn/65Zn/66Zn/67Zn/68Zn/69Zn/70Zn/71Zn/72Zn/73Zn/63Ga/64Ga/65Ga/66Ga/67Ga/68Ga/69Ga/70Ga/71Ga/72Ga/73Ga/74Ga/75Ga/65Ge/66Ge/67Ge/68Ge/69Ge/70Ge/71Ge/72Ge/73Ge/74Ge/75Ge/76Ge/77Ge/78Ge/67As/68As/69As/70As/71As/72As/73As/74As/75As/76As/77As/78As/79As/80As/69Se/70Se/71Se/72Se/73Se/74Se/75Se/76Se/77Se/78Se/79Se/80Se/81Se/82Se/83Se/71Br/72Br/73Br/74Br/75Br/76Br/77Br/78Br/79Br/80Br/81Br/82Br/83Br/84Br/85Br/86Br/73Kr/74Kr/75Kr/76Kr/77Kr/78Kr/79Kr/80Kr/81Kr/82Kr/83Kr/84Kr/85Kr/86Kr/87Kr/88Kr/76Rb/77Rb/78Rb/79Rb/80Rb/81Rb/82Rb/83Rb/84Rb/85Rb/86Rb/87Rb/88Rb/89Rb/90Rb/78Sr/79Sr/80Sr/81Sr/82Sr/83Sr/84Sr/85Sr/86Sr/87Sr/88Sr/89Sr/90Sr/91Sr/92Sr/93Sr/94Sr, E=500 MeV/nucleon; measured yields and cross sections of spallation reaction residue products using the FRS magnetic spectrometer and multisampling ionization chambers at GSI facility. 2H(136Xe, X)79Y/80Y/81Y/82Y/83Y/84Y/85Y/86Y/87Y/88Y/89Y/90Y/91Y/92Y/93Y/94Y/95Y/96Y/97Y/81Zr/82Zr/83Zr/84Zr/85Zr/86Zr/87Zr/88Zr/89Zr/90Zr/91Zr/92Zr/93Zr/94Zr/95Zr/96Zr/97Zr/98Zr/99Zr/83Nb/84Nb/85Nb/86Nb/87Nb/88Nb/89Nb/90Nb/91Nb/92Nb/93Nb/94Nb/95Nb/96Nb/97Nb/98Nb/99Nb/100Nb/101Nb/102Nb/85Mo/86Mo/87Mo/88Mo/89Mo/90Mo/91Mo/92Mo/93Mo/94Mo/95Mo/96Mo/97Mo/98Mo/99Mo/100Mo/101Mo/102Mo/102Mo/104Mo/105Mo/88Tc/89Tc/90Tc/91Tc/92Tc/93Tc/94Tc/95Tc/96Tc/97Tc/98Tc/99Tc/100Tc/101Tc/102Tc/103Tc/104Tc/105Tc/106Tc/107Tc/108Tc/90Ru/91Ru/92Ru/93Ru/94Ru/95Ru/96Ru/97Ru/98Ru/99Ru/100Ru/101Ru/102Ru/103Ru/104Ru/105Ru/106Ru/107Ru/108Ru/109Ru/110Ru/111Ru/112Ru/92Rh/93Rh/94Rh/95Rh/96Rh/97Rh/98Rh/99Rh/100Rh/101Rh/102Rh/103Rh/104Rh/105Rh/106Rh/107Rh/108Rh/109Rh/110Rh/111Rh/112Rh/113Rh/114Rh/115Rh/116Rh/94Pd/95Pd/96Pd/97Pd/98Pd/99Pd/100Pd/101Pd/102Pd/103Pd/104Pd/105Pd/106Pd/107Pd/108Pd/109Pd/110Pd/111Pd/112Pd/113Pd/114Pd/115Pd/116Pd/117Pd/118Pd/119Pd/120Pd/98Ag/99Ag/100Ag/101Ag/102Ag/103Ag/104Ag/105Ag/106Ag/107Ag/108Ag/109Ag/110Ag/111Ag/112Ag/113Ag/114Ag/115Ag/116Ag/117Ag/118Ag/119Ag/120Ag/121Ag/122Ag/123Ag/100Cd/101Cd/102Cd/103Cd/104Cd/105Cd/106Cd/107Cd/108Cd/109Cd/110Cd/111Cd/112Cd/113Cd/114Cd/115Cd/116Cd/117Cd/118Cd/119Cd/120Cd/121Cd/122Cd/123Cd/124Cd/125Cd/126Cd, E=500 MeV/nucleon; measured yields and cross sections of spallation reaction residue products using the FRS magnetic spectrometer and multisampling ionization chambers at GSI facility. 2H(136Xe, X)102In/103In/104In/105In/106In/107In/108In/109In/110In/111In/112In/113In/114In/115In/116In/117In/118In/119In/120In/121In/122In/123In/124In/125In/126In/127In/128In/129In/105Sn/106Sn/107Sn/108Sn/109Sn/110Sn/111Sn/112Sn/113Sn/114Sn/115Sn/116Sn/117Sn/118Sn/119Sn/120Sn/121Sn/122Sn/123Sn/124Sn/125Sn/126Sn/127Sn/128Sn/129Sn/130Sn/131Sn/132Sn/107Sb/108Sb/109Sb/110Sb/111Sb/112Sb/113Sb/114Sb/115Sb/116Sb/117Sb/118Sb/119Sb/120Sb/121Sb/122Sb/123Sb/124Sb/125Sb/126Sb/127Sb/128Sb/129Sb/130Sb/131Sb/132Sb/133Sb/134Sb/110Te/111Te/112Te/113Te/114Te/115Te/116Te/117Te/118Te/119Te/120Te/121Te/122Te/123Te/124Te/125Te/126Te/127Te/128Te/129Te/130Te/131Te/132Te/133Te/134Te/135Te/112I/113I/114I/115I/116I/117I/118I/119I/120I/121I/122I/123I/124I/125I/126I/127I/128I/129I/130I/131I/132I/133I/134I/135I/136I/116Xe/117Xe/118Xe/119Xe/120Xe/121Xe/122Xe/123Xe/124Xe/125Xe/126Xe/127Xe/128Xe/129Xe/130Xe/131Xe/132Xe/133Xe/134Xe/135Xe/119Cs/120Cs/121Cs/122Cs/123Cs/124Cs/125Cs/126Cs/127Cs/128Cs/129Cs/130Cs/131Cs/132Cs/133Cs/134Cs/135Cs/136Cs/123Ba/124Ba/125Ba/126Ba/127Ba/128Ba/129Ba/130Ba/131Ba/132Ba/133Ba/134Ba/135Ba, E=500 MeV/nucleon; measured yields and cross sections of spallation reaction residue products using the FRS magnetic spectrometer and multisampling ionization chambers at GSI facility. Benchmarked reference model calculations describing spallation reactions. Comparison with the measured production yields in 1H(136Xe, X), E=500, 1000 MeV/nucleon.

doi: 10.1103/PhysRevC.92.024607
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1889.


2015AY01      Phys.Rev. C 91, 034601 (2015)

Y.Ayyad, J.Benlliure, J.L.Rodriguez-Sanchez, A.Bacquias, A.Boudard, E.Casarejos, T.Enqvist, M.Fernandez, V.Henzl, V.Henzlova, B.Jurado, A.Kelic-Heil, T.Kurtukian, S.Lukic, P.Nadtochy, D.Perez-Loureiro, R.Pleskac, F.Farget, M.V.Ricciardi, K.-H.Schmidt, C.Schmitt, N.N.Son

Dissipative effects in spallation-induced fission of 208Pb at high excitation energies

NUCLEAR REACTIONS 1,2H(208Pb, F), E=500 MeV/nucleon; measured particle spectra, energy loss of the fission fragments, sum spectrum of fission fragments nuclear charge Z1+Z2, fission fragment charge distributions as function of mass number, partial fission and normalized cross sections as a function of the charge, distribution of the excitation energy of all the prefragments, width of the fission fragment charge distribution. Comparisons with model calculations using INCL and ISABEL codes coupled to ABLA.

doi: 10.1103/PhysRevC.91.034601
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2015MA70      Eur.Phys.J. A 51, 174 (2015)

J.-F.Martin, J.Taieb, A.Chatillon, G.Belier, G.Boutoux, A.Ebran, T.Gorbinet, L.Grente, B.Laurent, E.Pellereau, H.Alvarez-Pol, L.Audouin, T.Aumann, Y.Ayyad, J.Benlliure, E.Casarejos, D.Cortina Gil, M.Caamano, F.Farget, B.Fernandez-Dominguez, A.Heinz, B.Jurado, A.Kelic-Heil, N.Kurz, C.Nociforo, C.Paradela, S.Pietri, D.Ramos, J.-L.Rodriguez-Sanchez, C.Rodriguez-Tajes, D.Rossi, K.-H.Schmidt, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Studies on fission with ALADIN - Precise and simultaneous measurement of fission yields, total kinetic energy and total prompt neutron multiplicity at GSI

doi: 10.1140/epja/i2015-15174-0
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2015ME07      Phys.Rev. C 92, 035803 (2015)

B.Mei, T.Aumann, S.Bishop, K.Blaum, K.Boretzky, F.Bosch, C.Brandau, H.Brauning, T.Davinson, I.Dillmann, C.Dimopoulou, O.Ershova, Z.Fulop, H.Geissel, J.Glorius, G.Gyurky, M.Heil, F.Kappeler, A.Kelic-Heil, C.Kozhuharov, C.Langer, T.Le Bleis, Y.Litvinov, G.Lotay, J.Marganiec, G.Munzenberg, F.Nolden, N.Petridis, R.Plag, U.Popp, G.Rastrepina, R.Reifarth, B.Riese, C.Rigollet, C.Scheidenberger, H.Simon, K.Sonnabend, M.Steck, T.Stohlker, T.Szucs, K.Summerer, G.Weber, H.Weick, D.Winters, N.Winters, P.Woods, Q.Zhong

First measurement of the 96Ru(p, γ)97Rh cross section for the p process with a storage ring

NUCLEAR REACTIONS 1H(96Ru, γ)97Rh, E=9, 10, 11 MeV/nucleon; measured particle spectra in different charge states, x-ray and γ spectra, σ(E) using stored heavy ions in storage ring ESR at GSI; deduced astrophysical S factors and stellar reaction rates over a range of T9=0.5-19. Comparison with predictions from standard NON-SMOKER code and TALYS-1.4 code using different γ-ray strength functions from HFB, Brink-Axel Lorentzian (BAL), and Kopecky-Uhl, and different density models of constant temperature (CT), BSFG, generalized superfluid (GS), and Hartree-Fock-Bogolyubov (HFB). Recommended REACLIB parameters for the reactivity of 96Ru(p, γ)97Rh, and 97Rh(γ, p)96Ru reactions. Relevance to p-process network calculations.

doi: 10.1103/PhysRevC.92.035803
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2272.


2015RO11      Phys.Rev. C 91, 064616 (2015)

J.L.Rodriguez-Sanchez, J.Benlliure, J.Taieb, H.Alvarez-Pol, L.Audouin, Y.Ayyad, G.Belier, G.Boutoux, E.Casarejos, A.Chatillon, D.Cortina-Gil, T.Gorbinet, A.Heinz, A.Kelic-Heil, B.Laurent, J.-F.Martin, C.Paradela, E.Pellereau, B.Pietras, D.Ramos, C.Rodriguez-Tajes, D.M.Rossi, H.Simon, J.Vargas, B.Voss

Complete characterization of the fission fragments produced in reactions induced by 208Pb projectiles on proton at 500A MeV

NUCLEAR REACTIONS 1H(208Pb, F), E=500 MeV/nucleon; measured fission fragments, (fragment)(fragment)-coin, σ and mean velocities of fission fragments using SIS18 synchrotron and MUSIC detector system at GSI facility; deduced role of charge polarization and excitation energy gained by the fragments from analysis of correlations between the two fragments, parametrize the distance between two fission fragments at scission as function of the size of the fissioning system from analysis of the average velocities of the fission fragments, final neutron excess of the fission fragments. 58,59,60,61,62,63,64,65Co, 60,61,62,63,64,65,66,67,68Ni, 63,64,65,66,67,68,69,70Cu, 64,65,66,67,68,69,70,71,72,73,74Zn, 66,67,68,69,70,71,72,73,74,75,76,77Ga, 69,70,71,72,73,74,75,76,77,78,79Ge, 72,73,74,75,76,77,78,79,80,81As, 74,75,76,77,78,79,80,81,82,83Se, 78,79,80,81,82,83,84,85,86,87,88,89Kr, 80,81,82,83,84,85,86,87,88,89,90,91,92Rb, 82,83,84,85,86,87,88,89,90,91,92,93,94Sr, 84,85,86,87,88,89,90,91,92,93,94,95,96,97Y, 86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101Zr, 88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103Nb, 89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105Mo, 93,94,95,96,97,98,99,100,101,102,103,104,105,106,107Tc, 95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110Ru, 97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112Rh, 100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115Pd, 104,105,106,107,108,109,110,111,112,113,114,115,116,117Ag, 106,107,108,109,110,111,112,113,114,115,116,117,118Cd, 109,110,111,112,113,114,115,116,117,118,119,120,121In, 112,113,114,115,116,117,118,119,120,121Sn, 114,115,116,117,118,119,120,121,122,123,124,125Sb, 116,117,118,119,120,121,122,123,124,125,126,127,128Te; deduced isotopic cross sections of the fission fragments with associated statistical and systematical uncertainties. Comparison with state-of-the-art model calculations using NCL4.6+ABLA07 codes.

doi: 10.1103/PhysRevC.91.064616
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2267.


2015RO18      Phys.Rev. C 92, 044612 (2015)

J.L.Rodriguez-Sanchez, J.Benlliure, H.Alvarez-Pol, L.Audouin, Y.Ayyad, G.Belier, G.Boutoux, E.Casarejos, A.Chatillon, D.Cortina-Gil, T.Gorbinet, A.Heinz, A.Kelic-Heil, B.Laurent, J.-F.Martin, C.Paradela, E.Pellereau, B.Pietras, D.Ramos, C.Rodriguez-Tajes, D.M.Rossi, H.Simon, J.Taieb, J.Vargas, B.Voss

Constraining the level density using fission of lead projectiles

NUCLEAR REACTIONS 1H, 27Al(208Pb, F), E=370, 500, 650 MeV/nucleon; measured spallation and fragmentation-induced fission fragments, fission σ(E), atomic-number distribution of final fission fragments using double multisampling ionization chamber (twin MUSIC) at GSI; deduced fission decay widths, and level densities at ground-state and at saddle-point deformations. Comparison with several theoretical model calculations, and benchmarking of data.

doi: 10.1103/PhysRevC.92.044612
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2014AY03      Phys.Rev. C 89, 054610 (2014)

Y.Ayyad, J.Benlliure, E.Casarejos, H.Alvarez-Pol, A.Bacquias, A.Boudard, M.Caamano, T.Enqvist, V.Fohr, A.Kelic-Heil, K.Kezzar, S.Leray, D.Mancusi, C.Paradela, D.Perez-Loureiro, R.Pleskac, J.L.Rodriguez-Sanchez, D.Tarrio

Proton-induced fission of 181Ta at high excitation energies

NUCLEAR REACTIONS 1H(181Ta, F), E=300, 500, 800, 1000 MeV/nucleon; measured energy losses of the tantalum beam particles, and fission products at GSI facility; deduced proton-induced total fission σ(E), Mass, charge, and excitation energy distributions of prefragments, average fission lifetime, temperature dependence of dissipative and transient effects at small deformation. Comparison with previous experimental data, and model calculations using INCL+ABLA, ISABEL+ABLA, and INCL+GEMINI++ statistical model codes. Benchmarking state-of-the-art reaction codes

doi: 10.1103/PhysRevC.89.054610
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1888.


2014BE30      Nucl.Data Sheets 119, 277 (2014)

J.Benlliure, Y.Ayyad, A.Boudard, E.Casarejos, T.Enqvist, F.Farget, A.Bacquias, M.Fernandez, L.Giot, V.Henzl, D.Henzlova, A.Kelic-Heil, T.Kurtukian, S.Leray, S.Lukic, N.N.Son, P.Nadtochy, D.Perez, R.Pleskak, K.-H.Schmidt, C.Schmitt

Fission in Lead on Proton and Deuteron Reactions at 500 A MeV

NUCLEAR REACTIONS 1,2H(208Pb, F), E=500, 1000 MeV/nucleon; measured fission fragments energy, angle, atomic number; deduced fission fragment charge distribution, total fusion σ. Compared with data.

doi: 10.1016/j.nds.2014.08.076
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2294.


2014LA09      Phys.Rev. C 89, 035806 (2014)

C.Langer, O.Lepyoshkina, Y.Aksyutina, T.Aumann, S.Beceiro Novo, J.Benlliure, K.Boretzky, M.Chartier, D.Cortina, U.Datta Pramanik, O.Ershova, H.Geissel, R.Gernhauser, M.Heil, G.Ickert, H.T.Johansson, B.Jonson, A.Kelic-Heil, A.Klimkiewicz, J.V.Kratz, R.Krucken, R.Kulessa, K.Larsson, T.Le Bleis, R.Lemmon, K.Mahata, J.Marganiec, T.Nilsson, V.Panin, R.Plag, W.Prokopowicz, R.Reifarth, V.Ricciardi, D.M.Rossi, S.Schwertel, H.Simon, K.Summerer, B.Streicher, J.Taylor, J.R.Vignote, F.Wamers, C.Wimmer, P.Z.Wu

Thermonuclear reaction 30S(p, γ)31Cl studied via Coulomb breakup of 31Cl

NUCLEAR REACTIONS Pb(31Cl, p), [31Cl secondary beam from 9Be(36Ar, X), E=825 MeV/nucleon primary reaction], E=650 MeV/nucleon; measured reaction products, fragment spectra, Eγ, Iγ at R3B-LAND-GSI facility. 31Cl; deduced levels, resonances, J, π, width, comparison with levels predicted in shell-model calculations. 30S(p, γ), T=0.08-2.00 GK; deduced thermonuclear reaction rates. Relevance to rp process in typical Type I x-ray burst conditions.

doi: 10.1103/PhysRevC.89.035806
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Data from this article have been entered in the XUNDL database. For more information, click here.


2014ME05      Phys.Rev. C 89, 054612 (2014)

B.Mei, H.S.Xu, X.L.Tu, Y.H.Zhang, Yu.A.Litvinov, K.-H.Schmidt, M.Wang, Z.Y.Sun, X.H.Zhou, Y.J.Yuan, M.V.Ricciardi, A.Kelic-Heil, R.Reifarth, K.Blaum, R.S.Mao, Z.G.Hu, P.Shuai, Y.D.Zang, X.W.Ma, X.Y.Zhang, J.W.Xia, G.Q.Xiao, Z.Y.Guo, J.C.Yang, X.H.Zhang, X.Xu, X.L.Yan, W.Zhang, W.L.Zhan

Origin of odd-even staggering in fragment yields: Impact of nuclear pairing and shell structure on the particle-emission threshold energy

NUCLEAR REACTIONS 9Be(78Kr, X), E=482.9 MeV/nucleon; measured reaction products, fragment yields, particle-emission threshold energies of Tz=-1/2 and +1/2, Z=8-31 nuclei using in-flight fragment separator and a storage ring facility at CSRe-HIRFL-Lanzhou; deduced odd-even staggering (OES) effect on yields of fragments, and impact of pairing and shell structure.

doi: 10.1103/PhysRevC.89.054612
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2014RO28      Phys.Rev. C 90, 064606 (2014)

J.L.Rodriguez-Sanchez, J.Benlliure, J.Taieb, A.Chatillon, C.Paradela, Y.Ayyad, G.Belier, G.Boutoux, E.Casarejos, T.Gorbinet, B.Laurent, J.-F.Martin, E.Pellereau, H.Alvarez-Pol, L.Audouin, D.Cortina-Gil, A.Heinz, A.Kelic-Heil, B.Pietras, D.Ramos, C.Rodriguez-Tajes, D.Rossi, H.Simon, L.Tassan-Got, J.Vargas, B.Voss

Proton-induced fission cross sections on 208Pb at high kinetic energies

NUCLEAR REACTIONS 1H(208Pb, X), E=370, 500, 650 MeV/nucleon; measured fission fragment distributions, fission yields and fission σ(E) at GSI facility. Comparison with previous experimental data at E=50-1000 MeV/nucleon, and with Prokofiev's systematics. Benchmarking of model calculations using the intranuclear cascade code INCL4.6 coupled to the deexcitation code ABLA07. 208Pb(n, X), E=20-1000 MeV; analyzed fission σ(E).

doi: 10.1103/PhysRevC.90.064606
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2179.


2014SC28      Phys.Rev. C 90, 064605 (2014), Erratum Phys.Rev. C 94, 039901 (2016)

C.Schmitt, K.-H.Schmidt, A.Kelic-Heil

SPACS: A semi-empirical parameterization for isotopic spallation cross sections

NUCLEAR REACTIONS 1H(208Pb, X), E=500, 1000 MeV/nucleon; 1H(197Au, X), E=800 MeV/nucleon; 1H(136Xe, X), E=200, 500, 1000 MeV/nucleon; 1H(56Fe, X), E=300, 500, 750, 1000, 1500 MeV/nucleon; 1H(40Ca, X), E=763 MeV/nucleon; 1H(22Ne, X), E=894 MeV/nucleon; 28Si(p, X)22Ne, E=30-1500 MeV; 56Fe(p, X)42K, E=100-3000 MeV; 93Nb(p, X)54Mn/73Se/74As, E=150-3000 MeV; 181Ta(p, X)110Sn/172Lu, E=100-3000 MeV; 197Au(p, X)196Au, E=200-5000 MeV; 209Bi(p, X)206Bi, E=150-10000 MeV; calculated residue-production σ(E, Z, N) for Z=12-83, N=10-120 in spallation reactions using the prescription named SPACS, and benchmarked with experimental data from GSI and other laboratories.

doi: 10.1103/PhysRevC.90.064605
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2013GI02      Nucl.Phys. A899, 116 (2013)

L.Giot, J.A.Alcantara-Nunez, J.Benlliure, D.Perez-Loureiro, L.Audouin, A.Boudard, E.Casarejos, T.Enqvist, J.E.Ducret, B.Fernandez-Dominguez, M.Fernandez-Ordonez, F.Farget, A.Heinz, V.Henzl, D.Henzlova, A.Kelic-Heil, A.Lafriaskh, S.Leray, P.Napolitani, C.Paradela, J.Pereira, M.V.Ricciardi, C.Stephan, K.-H.Schmidt, C.Schmitt, L.Tassan-Got, C.Villagrasa, C.Volant, O.Yordanov

Isotopic production cross sections of the residual nuclei in spallation reactions induced by 136Xe projectiles on proton at 500 A MeV

NUCLEAR REACTIONS 1H(136Xe, X), E=500 MeV/nucleon; measured spallation products mass, charge distribution using FRS magnetic spectrometer; deduced fragment isotopes yields, production σ, longitudinal momentum distributions. Compared with published data at 1000 MeV/nucleon.

doi: 10.1016/j.nuclphysa.2012.12.119
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2143.


2013RO33      Phys.Rev.Lett. 111, 242503 (2013)

D.M.Rossi, P.Adrich, F.Aksouh, H.Alvarez-Pol, T.Aumann, J.Benlliure, M.Bohmer, K.Boretzky, E.Casarejos, M.Chartier, A.Chatillon, D.Cortina-Gil, U.Datta Pramanik, H.Emling, O.Ershova, B.Fernandez-Dominguez, H.Geissel, M.Gorska, M.Heil, H.T.Johansson, A.Junghans, A.Kelic-Heil, O.Kiselev, A.Klimkiewicz, J.V.Kratz, R.Krucken, N.Kurz, M.Labiche, T.Le Bleis, R.Lemmon, Yu.A.Litvinov, K.Mahata, P.Maierbeck, A.Movsesyan, T.Nilsson, C.Nociforo, R.Palit, S.Paschalis, R.Plag, R.Reifarth, D.Savran, H.Scheit, H.Simon, K.Summerer, A.Wagner, W.Walus, H.Weick, M.Winkler

Measurement of the Dipole Polarizability of the Unstable Neutron-Rich Nucleus 68Ni

NUCLEAR REACTIONS Pb(68Ni, 68Ni'), (68Ni, X), E=502.7 MeV/nucleon; measured reaction products, Eγ, Iγ, En, In. 68Ni; deduced σ(E), giant and pygmy dipole resonance parameters, E1 strength, neutron skin thickness. Comparison with available data.

doi: 10.1103/PhysRevLett.111.242503
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2013SC07      Phys.Rev. C 87, 034601 (2013)

K.-H.Schmidt, B.Jurado, R.Pleskac, M.V.Ricciardi, J.Benlliure, A.Boudard, E.Casarejos, T.Enqvist, F.Farget, A.Bacquias, M.Fernandez, L.Giot, V.Henzl, D.Henzlova, A.Kelic-Heil, T.Kurtukian, S.Leray, S.Lukic, N.N.Son, P.Nadtochy, D.Perez, C.Schmitt

High-precision measurement of total fission cross sections in spallation reactions of 208Pb and 238U

NUCLEAR REACTIONS 1,2H(208Pb, F), (238U, F), E=500-1000 MeV/nucleon; measured beam particle and fission fragment spectra in coincidence, energy-loss, time of flight, total fission σ(E) at GSI facility. Spallation reactions in inverse kinematics. Comparisons with Prokofiev's systematics, and previous measurements.

doi: 10.1103/PhysRevC.87.034601
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2141.


2012BA09      Phys.Rev. C 85, 024904 (2012)

A.Bacquias, V.Fohr, D.Henzlova, A.Kelic-Heil, M.V.Ricciardi, K.-H.Schmidt

Dispersion of longitudinal momentum distributions induced in fragmentation reactions

doi: 10.1103/PhysRevC.85.024904
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2012KU26      Phys.Lett. B 717, 371 (2012)

J.Kurcewicz, F.Farinon, H.Geissel, S.Pietri, C.Nociforo, A.Prochazka, H.Weick, J.S.Winfield, A.Estrade, P.R.P.Allegro, A.Bail, G.Belier, J.Benlliure, G.Benzoni, M.Bunce, M.Bowry, R.Caballero-Folch, I.Dillmann, A.Evdokimov, J.Gerl, A.Gottardo, E.Gregor, R.Janik, A.Kelic-Heil, R.Knobel, T.Kubo, Yu.A.Litvinov, E.Merchan, I.Mukha, F.Naqvi, M.Pfutzner, M.Pomorski, Zs.Podolyak, P.H.Regan, B.Riese, M.V.Ricciardi, C.Scheidenberger, B.Sitar, P.Spiller, J.Stadlmann, P.Strmen, B.Sun, I.Szarka, J.Taieb, S.Terashima, J.J.Valiente-Dobon, M.Winkler, Ph.Woods

Discovery and cross-section measurement of neutron-rich isotopes in the element range from neodymium to platinum with the FRS

NUCLEAR REACTIONS 9B(238U, X)157Nd/158Nd/159Nd/160Nd/161Nd/160Pm/161Pm/162Pm/163Pm/163Sm/164Sm/165Sm/167Eu/168Eu/167Gd/168Gd/169Gd/170Gd/169Tb/170Tb/171Tb/172Tb/171Dy/172Dy/173Dy/174Dy/173Ho/174Ho/175Ho/176Ho/176Er/177Er/178Er/178Tm/179Tm/180Tm/181Tm/181Yb/182Yb/183Yb/184Yb/185Yb/185Lu/186Lu/187Lu/188Lu/190Hf/193Ta/194Ta/195W/196W/197W/198Re/199Re/202Os/203Os/205Ir/206Pt/207Pt/208Pt, E=1 GeV/nucleon; measured time-of-flight, energy loss, fragment σ using FRS at GSI facility; discovered 60 new isotopes. Comparison of σ(A, Z) distributions with ABRABLA, COFRA and EPAX-3 model calculations.

doi: 10.1016/j.physletb.2012.09.021
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2068.


2011CU05      J.Phys.:Conf.Ser. 312, 082019 (2011)

J.Cugnon, A.Boudard, J.-C.David, A.Kelic-Heil, S.Leray, D.Mancusi, M.V.Ricciardi

Production of heavy clusters (up to A=10) by coalescence during the intranuclear cascade phase of spallation reactions

NUCLEAR REACTIONS 197Au(p, 6Li), (p, 7Be), E=1200 MeV; calculated spallation σ(θ, E) using Liege Intra-Nuclear Cascade model INCL4.5 plus ABLA07. Compared with data and older models. Also other energies between 1.2 and 2.5 GeV, targets from Al to Th and other clusters calculated, but their results not presented within the paper.

doi: 10.1088/1742-6596/312/4/082019
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2011FO17      Phys.Rev. C 84, 054605 (2011)

V.Fohr, A.Bacquias, E.Casarejos, T.Enqvist, A.R.Junghans, A.Kelic-Heil, T.Kurtukian, S.Lukic, D.Perez-Loureiro, R.Pleskac, M.V.Ricciardi, K.-H.Schmidt, J.Taieb

Experimental study of fragmentation products in the reactions 112Sn+112Sn and 124Sn+124Sn at 1A GeV

doi: 10.1103/PhysRevC.84.054605
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0908.


2011MA60      J.Korean Phys.Soc. 59, 943s (2011)

D.Mancusi, J.Cugnon, A.Boudard, J.-C.David, S.Leray, R.J.Charity, A.Kelic-heil, M.V.Ricciardi

Multifragmentation in Reactions of 1-GeV Protons with Iron Nuclei

NUCLEAR REACTIONS 56Fe(p, X), E=1 GeV; calculated multifragmentation IMF residue yields, σ, charge distributions, 7Li, 10B longitudinal velocity distributions, neutron multiplicity, α multiplicity. GEMINI++, SPALADIN, ABLA07 codes with and without multifragmentation. Comparison to data.

doi: 10.3938/jkps.59.943
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1956.


2010PA41      Astron.Astrophys. 513, A61 (2010)

I.V.Panov, I.Yu.Korneev, T.Rauscher, G.Martínez-Pinedo, A.Kelic-Heil, N.T.Zinner, F.-K.Thielemann

Neutron-induced astrophysical reaction rates for translead nuclei

NUCLEAR REACTIONS 235,236,238U, 237Np, 238,239,240,241,242Pu(n, F), (n, γ), E<1 MeV; calculated astrophysical reaction rates. Comparison with JENDL-3.3 library.

doi: 10.1051/0004-6361/200911967
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2010TH06      J.Phys.:Conf.Ser. 202, 012006 (2010)

F.-K.Thielemann, I.Dillmann, K.Farouqi, T.Fischer, C.Frohlich, A.Kelic-Heil, I.Korneev, K.-L.Kratz, K.Langanke, M.Liebendorfer, I.V.Panov, G.Martinez-Pinedo, T.Rauscher

The r-, p-, and νp-Process

NUCLEAR REACTIONS 252Cf(n, F), E=0.002-20 MeV; calculated fission σ using different barrier predicions. Compared with data and JENDL-3.3. A≈220-260(n, F), E not given; calculated fission σ using different barrier predictions. Compared with data.

doi: 10.1088/1742-6596/202/1/012006
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