NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = B.Jurado Found 78 matches. 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
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
2021SC10 Nucl.Data Sheets 173, 54 (2021) K.-H.Schmidt, M.Estienne, M.Fallot, S.Cormon, A.Cucoanes, T.Shiba, B.Jurado, K.Kern, Ch.Schmitt Extensive Study of the Quality of Fission Yields from Experiment, Evaluation and GEF for Antineutrino Studies and Applications NUCLEAR REACTIONS 241Pu(n, F), E thermal; analyzed available data; calculated fission yields using GEF code. Comparison with JEFF-3.3 library.
doi: 10.1016/j.nds.2021.04.004
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
2020KR12 Phys.Rev. A 102, 042825 (2020) F.M.Kroger, G.Weber, M.O.Herdrich, J.Glorius, C.Langer, Z.Slavkovska, L.Bott, C.Brandau, B.Bruckner, K.Blaum, X.Chen, S.Dababneh, T.Davinson, P.Erbacher, S.Fiebiger, T.Gassner, K.Gobel, M.Groothuis, A.Gumberidze, Gy.Gyurky, S.Hagmann, C.Hahn, M.Heil, R.Hess, R.Hensch, P.Hillmann, P.-M.Hillenbrand, O.Hinrichs, B.Jurado, T.Kausch, A.Khodaparast, T.Kisselbach, N.Klapper, C.Kozhuharov, D.Kurtulgil, G.Lane, C.Lederer-Woods, M.Lestinsky, S.Litvinov, Yu.A.Litvinov, B.Loher, F.Nolden, N.Petridis, U.Popp, M.Reed, R.Reifarth, M.S.Sanjari, H.Simon, U.Spillmann, M.Steck, J.Stumm, T.Szucs, T.T.Nguyen, A.Taremi Zadeh, B.Thomas, S.Yu.Torilov, H.Tornqvist, C.Trageser, S.Trotsenko, M.Volknandt, M.Weigand, C.Wolf, P.J.Woods, V.P.Shevelko, I.Yu.Tolstikhina, Th.Stohlker Electron capture of Xe54+ in collisions with H2 molecules in the energy range between 5.5 and 30.9 MeV/u NUCLEAR REACTIONS H(Xe, X), E=5.5-30.9 MeV/nucleon; measured reaction products, X-rays; deduced X-ray spectra, electron-capture σ. Comparison with available data.
doi: 10.1103/PhysRevA.102.042825
2020PE08 Phys.Rev.Lett. 125, 122502 (2020) R.Perez Sanchez, B.Jurado, V.Meot, O.Roig, M.Dupuis, O.Bouland, D.Denis-Petit, P.Marini, L.Mathieu, I.Tsekhanovich, M.Aiche, L.Audouin, C.Cannes, S.Czajkowski, S.Delpech, A.Gorgen, M.Guttormsen, A.Henriques, G.Kessedjian, K.Nishio, D.Ramos, S.Siem, F.Zeiser Simultaneous Determination of Neutron-Induced Fission and Radiative Capture Cross Sections from Decay Probabilities Obtained with a Surrogate Reaction NUCLEAR REACTIONS 240Pu(α, α'), (α, F), E=30 MeV; 239Pu(n, F), (n, γ), E<2 MeV; measured reaction products, Eγ, Iγ, Eα, Iα, α-fission fragment-γ ray triple coin.; deduced 239Pu σ as a function of energy. Comparison with ENDF/B-VIII.0, JENDL 4.0. JEFF 3.3 libraries.
doi: 10.1103/PhysRevLett.125.122502
2020RA05 Phys.Rev. C 101, 034609 (2020) D.Ramos, M.Caamano, A.Lemasson, M.Rejmund, H.Alvarez-Pol, L.Audouin, J.D.Frankland, B.Fernandez-Dominguez, E.Galiana-Baldo, J.Piot, C.Schmitt, D.Ackermann, S.Biswas, E.Clement, D.Durand, F.Farget, M.O.Fregeau, D.Galaviz, A.Heinz, A.Henriques, B.Jacquot, B.Jurado, Y.H.Kim, P.Morfouace, D.Ralet, T.Roger, P.Teubig, I.Tsekhanovich Scission configuration of 239U from yields and kinetic information of fission fragments NUCLEAR REACTIONS 9Be(238U, 239U)8Be, E=5.88 MeV/nucleon; measured fission fragments of 239U, α-α coin using a double-sided segmented silicon telescope SPIDER, mass and charge distribution of fission fragments, yields of fission fragment using VAMOS++ spectrometer at GANIL; deduced fragment velocity and kinetic energy, fragment neutron excess and multiplicity, average total kinetic energy of fission fragments, total excitation energy and elongation at scission. Comparison with evaluated data in ENDF/B-VIII.0, with predictions of GEF code, and with similar observables from the fission of 240Pu.
doi: 10.1103/PhysRevC.101.034609
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
2019GL01 Phys.Rev.Lett. 122, 092701 (2019) J.Glorius, C.Langer, Z.Slavkovska, L.Bott, C.Brandau, B.Bruckner, K.Blaum, X.Chen, S.Dababneh, T.Davinson, P.Erbacher, S.Fiebiger, T.Gassner, K.Gobel, M.Groothuis, A.Gumberidze, G.Gyurky, M.Heil, R.Hess, R.Hensch, P.Hillmann, P.-M.Hillenbrand, O.Hinrichs, B.Jurado, T.Kausch, A.Khodaparast, T.Kisselbach, N.Klapper, C.Kozhuharov, D.Kurtulgil, G.Lane, C.Lederer-Woods, M.Lestinsky, S.Litvinov, Y.A.Litvinov, B.Loher, F.Nolden, N.Petridis, U.Popp, T.Rauscher, M.Reed, R.Reifarth, M.S.Sanjari, D.Savran, H.Simon, U.Spillmann, M.Steck, T.Stohlker, J.Stumm, A.Surzhykov, T.Szucs, T.T.Nguyen, A.Taremi Zadeh, B.Thomas, S.Yu.Torilov, H.Tornqvist, M.Trager, C.Trageser, S.Trotsenko, L.Varga, M.Volknandt, H.Weick, M.Weigand, C.Wolf, P.J.Woods, Y.M.Xing Approaching the Gamow Window with Stored Ions: Direct Measurement of 124Xe(p, γ) in the ESR Storage Ring NUCLEAR REACTIONS 124Xe(p, γ), E=5.5-8 MeV/nucleon; measured reaction products, X-rays; deduced σ, σ(θ).
doi: 10.1103/PhysRevLett.122.092701
2019RA23 Phys.Rev.Lett. 123, 092503 (2019) D.Ramos, M.Caamano, A.Lemasson, M.Rejmund, L.Audouin, H.Alvarez-Pol, J.D.Frankland, B.Fernandez-Dominguez, E.Galiana-Baldo, J.Piot, D.Ackermann, S.Biswas, E.Clement, D.Durand, F.Farget, M.O.Fregeau, D.Galaviz, A.Heinz, A.I.Henriques, B.Jacquot, B.Jurado, Y.H.Kim, P.Morfouace, D.Ralet, T.Roger, C.Schmitt, P.Teubig, I.Tsekhanovich First Direct Measurement of Isotopic Fission-Fragment Yields of 239U NUCLEAR REACTIONS 9Be(238U, 8Be)239U, E=5.88 MeV/nucleon; measured fission products, Eα, Iα; deduced isotopic fission yields of 239U.
doi: 10.1103/PhysRevLett.123.092503
2018SC10 Phys.Rev. C 98, 044605 (2018) C.Schmitt, K.-H.Schmidt, B.Jurado Benchmark of the GEF code for fission-fragment yields over an enlarged range in fissioning nucleus mass, excitation energy, and angular momentum NUCLEAR REACTIONS 238U(n, F), E=2, 5.5, 10.05, 13, 20, 50 MeV; 12C(238U, X)239Np*, E*=7.5 MeV; 12C(238U, X)240Pu*, E*=10.7 MeV; 12C(238U, X)244Cm*, E*=23 MeV; 12C(238U, X)250Cf*, E*=45 MeV; 12C(238U, X)238U*, E*=14.7 MeV; 16O(232Th, X)231Th*/232Th*/233Th*/234Th*/232Pa*/233Pa*/234Pa*/235Pa*/236Pa*/234U*/235U*/236U*/237U*/238U*, E*=5, 15, 25, 35, 45, 55 MeV; 235U, 239Pu(n, F)95Zr/97Zr/105Ru/127Sb/132Te/140Ba/147Nd, E=0-15 MeV; calculated fission fragment postneutron and pre-neutron mass yield distributions, fissioning system mass, charge, excitation energy, angular momentum, and neutron to proton ratio using GEneral description of Fission observables (GEF) code. Comparison with experimental data.
doi: 10.1103/PhysRevC.98.044605
2017MA74 Phys.Rev. C 96, 054604 (2017) P.Marini, L.Mathieu, M.Aiche, G.Belier, S.Czajkowski, Q.Ducasse, B.Jurado, G.Kessedjian, J.Matarranz, A.Plompen, P.Salvador-Castineira, J.Taieb, I.Tsekhanovich 242Pu neutron-induced fission cross-section measurement from 1 to 2 MeV neutron energy NUCLEAR REACTIONS 242Pu(n, F), E=1.1, 1.4, 2.0 MeV; measured neutron flux, and fission fragments, σ(E) relative to that for 1H(n, p) elastic scattering cross section at the Van de Graaff accelerator of CEA-DIF, France. Comparison with previous experimental results, and with evaluated data in ENDF/B-VII.1 and JEFF3.2.
doi: 10.1103/PhysRevC.96.054604
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
2016DU18 Phys.Rev. C 94, 024614 (2016) Q.Ducasse, B.Jurado, M.Aiche, P.Marini, L.Mathieu, A.Gorgen, M.Guttormsen, A.C.Larsen, T.Tornyi, J.N.Wilson, G.Barreau, G.Boutoux, S.Czajkowski, F.Giacoppo, F.Gunsing, T.W.Hagen, M.Lebois, J.Lei, V.Meot, B.Morillon, A.M.Moro, T.Renstrom, O.Roig, S.J.Rose, O.Serot, S.Siem, I.Tsekhanovich, G.M.Tveten, M.Wiedeking Investigation of the 238U (d, p) surrogate reaction via the simultaneous measurement of γ-decay and fission probabilities NUCLEAR REACTIONS 238U(d, p)239U*, E=15 MeV; measured particle spectra Eγ, Iγ, (proton)γ- and (proton)(fission events)-coin using ΔE/E silicon telescope SiRi for particles and CACTUS array for γ rays at Oslo Cyclotron Laboratory; corrected data using continuum-discretized coupled channels calculations for elastic breakup, and DWBA for inelastic breakup; deduced excitation energy of 239U versus detected γ-ray energy, ratio between the γ-coincidence and the singles spectra, average angular momentum, γ-decay and fission probabilities as function of excitation energy and compared with JENDL 4.0, ENDF-B/VII.1 and JEFF 3.2 evaluated libraries, and corresponding neutron-induced data; calculated contributions to the total deuteron breakup process (TB) as a function of the excitation energy of 239U. Statistical model calculations for decay probabilities and average angular momentum.
doi: 10.1103/PhysRevC.94.024614
2016SC02 Nucl.Data Sheets 131, 107 (2016) K.-H.Schmidt, B.Jurado, C.Amouroux, C.Schmitt General Description of Fission Observables: GEF Model Code
doi: 10.1016/j.nds.2015.12.009
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
2015CA21 Phys.Rev. C 92, 034606 (2015) M.Caamano, F.Farget, O.Delaune, K.-H.Schmidt, C.Schmitt, L.Audouin, C.-O.Bacri, J.Benlliure, E.Casarejos, X.Derkx, B.Fernandez-Dominguez, L.Gaudefroy, C.Golabek, B.Jurado, A.Lemasson, D.Ramos, C.Rodriguez-Tajes, T.Roger, A.Shrivastava Characterization of the scission point from fission-fragment velocities RADIOACTIVITY 240Pu(SF)[from 12C(238U, 10Be), E=6.1 MeV/nucleon]; 250Cf(SF)[from 12C(238U, X)250Cf*, E=6.1 MeV/nucleon]; measured fragment spectra using VAMOS spectrometer at GANIL; deduced velocity of fission fragments with Z=34-62 as a function of the neutron number of the fragment (N=45-100), average fragment velocity, average neutron excess of fragments, neutron multiplicity and total neutron evaporation multiplicity, total kinetic energy of fission fragments, total excitation energy at scission, post-neutron evaporation normalized yields, average difference between the ground states of the fissioning system and the fragments, and minimum energy released in neutron evaporation as functions of the fragment atomic number. Modeling of the fission process through correlated observables.
doi: 10.1103/PhysRevC.92.034606
2015FA14 Eur.Phys.J. A 51, 175 (2015) F.Farget, M.Caamano, D.Ramos, C.Rodriguez-Tajes, K.-H.Schmidt, L.Audouin, J.Benlliure, E.Casarejos, E.Clement, D.Cortina, O.Delaune, X.Derkx, A.Dijon, D.Dore, B.Fernandez-Dominguez, L.Gaudefroy, C.Golabek, A.Heinz, B.Jurado, A.Lemasson, C.Paradela, T.Roger, M.D.Salsac, C.Schmitt Transfer-induced fission in inverse kinematics: Impact on experimental and evaluated nuclear data bases
doi: 10.1140/epja/i2015-15175-y
2015GU27 Eur.Phys.J. A 51, 170 (2015) M.Guttormsen, M.Aiche, F.L.Bello Garrote, L.A.Bernstein, D.L.Bleuel, Y.Byun, Q.Ducasse, T.K.Eriksen, F.Giacoppo, A.Gorgen, F.Gunsing, T.W.Hagen, B.Jurado, M.Klintefjord, A.C.Larsen, L.Lebois, B.Leniau, H.T.Nyhus, T.Renstrom, S.J.Rose, E.Sahin, S.Siem, T.G.Tornyi, G.M.Tveten, A.Voinov, M.Wiedeking, J.Wilson Experimental level densities of atomic nuclei
doi: 10.1140/epja/i2015-15170-4
2015JU01 J.Phys.(London) G42, 055101 (2015) Influence of complete energy sorting on the characteristics of the odd-even effect in fission-fragment element distributions NUCLEAR REACTIONS 229,230Th, 234,236U, 239Np, 240Pu, 243Am, 246Cm, 250Cf(n, F), E<10 MeV; calculated fission fragments. Comparison with experimental data.
doi: 10.1088/0954-3899/42/5/055101
2015KE02 Phys.Rev. C 91, 044607 (2015) G.Kessedjian, B.Jurado, G.Barreau, P.Marini, L.Mathieu, I.Tsekhanovich, M.Aiche, G.Boutoux, S.Czajkowski, Q.Ducasse Fission probabilities of 242Am, 243Cm, and 244Cm induced by transfer reactions NUCLEAR REACTIONS 243Am(3He, αF), (3He, tF), (3He, dF), E=24 MeV; measured particle and fission fragment spectra in singles and coincidences, angular distribution of fission fragments using ΔE-E detectors at IPN, Orsay Tandem accelerator facility; deduced fission probabilities of the 242Am, 243,244Cm as a function of excitation energy, fission-barrier parameters. Detailed covariance analysis. Comparison with statistical-model calculations.
doi: 10.1103/PhysRevC.91.044607
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
2015SC23 Eur.Phys.J. A 51, 176 (2015) Revealing hidden regularities with a general approach to fission
doi: 10.1140/epja/i2015-15176-x
2014DU11 Nucl.Data Sheets 119, 233 (2014) Q.Ducasse, B.Jurado, M.Aiche, L.Mathieu, T.Tornyi, A.Gorgen, J.N.Wilson, G.Barreau, I.Companis, S.Czajkowski, F.Giacoppo, F.Gunsing, M.Guttormsen, A.C.Larsen, M.Lebois, J.Matarranz, T.Renstrom, S.Rose, S.Siem, I.Tsekhanovich, G.M.Tveten, T.W.Hagen, M.Wiedeking, O.Serot, G.Boutoux, P.Chau, V.Meot, O.Roig Neutron-induced Cross Sections of Actinides via the Surrogate-reaction Method NUCLEAR REACTIONS 238U(d, p), E=15 MeV;238U(3He, t), (3He, α), E=24 MeV; measured ejectiles, fission fragments, coincidences using SiRi detector and PPAC fission detectors, Eγ, Iγ using NaI CACTUS detectors. 238U(n, F), E*=5.55-7.25 MeV; deduced fission probability. 238U(n, γ), E*=4.65-5.9 MeV; deduced γ-decay probability using surrogate method. 238U(n, F), E*=4.8-7.25 MeV; calculated fission probability using TALYS. Preliminary. Fission probability compared with results of Cramer and Britt. Further analysis in progress.
doi: 10.1016/j.nds.2014.08.064
2014GU04 Phys.Rev. C 89, 014302 (2014) M.Guttormsen, L.A.Bernstein, A.Gorgen, B.Jurado, S.Siem, M.Aiche, Q.Ducasse, F.Giacoppo, F.Gunsing, T.W.Hagen, A.C.Larsen, M.Lebois, B.Leniau, T.Renstrom, S.J.Rose, T.G.Tornyi, G.M.Tveten, M.Wiedeking, J.N.Wilson Scissors resonance in the quasicontinuum of Th, Pa, and U isotopes NUCLEAR REACTIONS 232Th(d, d'), (d, p), E=12 MeV; 232Th(3He, 3He'), (3He, d), (3He, t), (3He, α), E=24 MeV; 238U(d, d'), (d, p), (d, t), E=15 MeV; measured Eγ, Iγ, particle spectra, (particle)γ-coin using SiRi particle telescope and CACTUS γ-detector array at Oslo cyclotron facility. 231,232,233Th, 232,233Pa, 237,238,239U; deduced γ strength functions in the quasicontinuum, low-energy M1 scissors resonance (SR), level densities using Oslo method Comparison with previous (γ, γ') experimental results, and with theoretical model calculations.
doi: 10.1103/PhysRevC.89.014302
2014KU02 Phys.Rev. C 89, 024616 (2014) T.Kurtukian-Nieto, J.Benlliure, K.-H.Schmidt, L.Audouin, F.Becker, B.Blank, E.Casarejos, F.Farget, M.Fernandez-Ordonez, J.Giovinazzo, D.Henzlova, B.Jurado, J.Pereira, O.Yordanov Production cross sections of heavy neutron-rich nuclei approaching the nucleosynthesis r-process path around A=195 NUCLEAR REACTIONS 9Be(208Pb, X), E=1 GeV/nucleon; measured reaction products, production σ for 190 heavy neutron-rich nuclei, including 26 nuclides produced for the first time, using FRS, SEETRAM, MUSIC1 and MUSIC2 at UNILAC-SIS facility at GSI. In-flight fragmentation. 181,182Yb, 185,186Lu, 189,190Hf, 191,192,193Ta, 193,194,195W, 195,196,197,198Re, 198,199,200,201Os, 200,201,202,203Ir, 203,204Pt; measured production σ for new nuclides. Z=70, A=170-182; Z=71, A=170-186; Z=72, A=174, 175, 177-190; Z=73, A=176-193; Z=74, A=178-195; Z=75, A=182-184, 186-198; Z=76, A=183-201; Z=77, A=186-203; Z=78, A=188-190, 192-204; Z=79, A=191-205; Z=80, A=197-202, 204-206; Z=81, A=200-204, 206, 207; Z=82, A=204-207; Z=83, A=205-208; measured production σ. Comparison with EPAX, COFRA, and ABRABLA nuclear fragmentation cross-section models. Relevance to r-process waiting point nuclei at A=195.
doi: 10.1103/PhysRevC.89.024616
2014KU23 Eur.Phys.J. A 50, 135 (2014) T.Kurtukian-Nieto, J.Benlliure, K.-H.Schmidt, L.Audouin, F.Becker, B.Blank, I.N.Borzov, E.Casarejos, F.Farget, M.Fernandez-Ordonez, J.Giovinazzo, D.Henzlova, B.Jurado, K.Langanke, G.Martinez-Pinedo, J.Pereira, O.Yordanov Beta-decay half-lives of new neutron-rich isotopes of Re, Os and Ir approaching the r-process path near N = 126
doi: 10.1140/epja/i2014-14135-5
2014LE24 Nucl.Data Sheets 119, 353 (2014) X.Ledoux, M.Aiche, M.Avrigeanu, V.Avrigeanu, L.Audouin, E.Balanzat, B.Ban-detat, G.Ban, G.Barreau, E.Bauge, G.Belier, P.Bem, V.Blideanu, C.Borcea, S.Bouffard, T.Caillaud, A.Chatillon, S.Czajkowski, P.Dessagne, D.Dore, M.Fallot, F.Farget, U.Fischer, L.Giot, T.Granier, S.Guillous, F.Gunsing, C.Gustavsson, B.Jacquot, K.Jansson, B.Jurado, M.Kerveno, A.Klix, O.Landoas, F.R.Lecolley, J.L.Lecouey, M.Majerle, N.Marie, T.Materna, J.Mrazek, F.Negoita, J.Novak, S.Oberstedt, A.Oberstedt, S.Panebianco, L.Perrot, A.J.M.Plompen, S.Pomp, J.M.Ramillon, D.Ridikas, B.Rosse, G.Rudolf, O.Serot, S.P.Simakov, E.Simeckova, A.G.Smith, J.C.Sublet, J.Taieb, L.Tassan-Got, D.Tarrio, A.Takibayev, I.Thfoin, I.Tsekhanovich, C.Varignon The Neutrons for Science Facility at SPIRAL-2
doi: 10.1016/j.nds.2014.08.097
2014MA63 Nucl.Data Sheets 119, 368 (2014) L.Mathieu, I.Companis, M.Aiche, P.Schillebeeckx, J.Heyse, G.Barreau, G.Boutoux, S.Czajkowski, F.Gunsing, B.Jurado, G.Kessedjian, A.J.M.Plompen, I.Tsekhanovitch Development of Ionisation Chambers for the Simultaneous Measurement of the Neutron-induced Capture and Fission Cross Section of 233U
doi: 10.1016/j.nds.2014.08.101
2014PL06 Nucl.Data Sheets 119, 201 (2014) A.J.M.Plompen, F.-J.Hambsch, S.Kopecky, M.Nyman, C.Rouki, P.Salvador-Castineira, P.Schillebeeckx, F.Belloni, E.Berthoumieux, F.Gunsing, C.Lampoudis, M.Calviani, C.Guerrero, D.Cano-Ott, E.Gonzalez-Romero, M.Aiche, B.Jurado, L.Mathieu, X.Derckx, F.Farget, C.Rodrigues Tajes, A.Bacquias, Ph.Dessagne, M.Kerveno, C.Borcea, A.Negret, N.Colonna, I.Goncalves, H.Penttila, S.Rinta-Antila, V.S.Kolhinen, A.Jokinen ANDES Measurements for Advanced Reactor Systems
doi: 10.1016/j.nds.2014.08.056
2014RO05 Phys.Rev. C 89, 024614 (2014) C.Rodriguez-Tajes, F.Farget, X.Derkx, M.Caamano, O.Delaune, K.-H.Schmidt, E.Clement, A.Dijon, A.Heinz, T.Roger, L.Audouin, J.Benlliure, E.Casarejos, D.Cortina, D.Dore, B.Fernandez-Dominguez, B.Jacquot, B.Jurado, A.Navin, C.Paradela, D.Ramos, P.Romain, M.D.Salsac, C.Schmitt Transfer reactions in inverse kinematics: An experimental approach for fission investigations NUCLEAR REACTIONS 12C(238U, 238U), (238U, 238U'), (238U, 237U)13C, (238U, 236U)14C, (238U, 239Np)11B, (238U, 240Pu)10Be, (238U, 241Pu)9Be, (238U, 242Pu)8Be, (238U, 243Am)7Li, (238U, 244Cm)6He, (238U, 246Cm)4He, E=6.14 MeV/nucleon; measured particle spectra, (particle)(fission fragment)-coin and (particle)(fission fragment)-anticoin, integral σ, σ(θ), total excitation-energy distributions, optimal Q values, Eγ, Iγ, (particle)γ-coin using VAMOS spectrometer, SPIDER array for particle detection, and EXOGAM array for γ rays at GANIL CSS1 cyclotron facility; deduced transfer induced fission probabilities for 238U, 239Np, 240,241,242Pu, 244Cm by surrogate-reaction technique. 12C, 11B, 10Be; deduced first excited level, probabilities of γ-ray emission from the first excited state. Comparison with other experimental data, and with TALYS calculations of neutron-induced fission probabilities.
doi: 10.1103/PhysRevC.89.024614
2013CA16 Phys.Rev. C 88, 024605 (2013); Erratum Phys.Rev. C 89, 069903 (2014) M.Caamano, O.Delaune, F.Farget, X.Derkx, K.-H.Schmidt, L.Audouin, C.-O.Bacri, G.Barreau, J.Benlliure, E.Casarejos, A.Chbihi, B.Fernandez-Dominguez, L.Gaudefroy, C.Golabek, B.Jurado, A.Lemasson, A.Navin, M.Rejmund, T.Roger, A.Shrivastava, C.Schmitt Isotopic yield distributions of transfer- and fusion-induced fission from 238U+12C reactions in inverse kinematics NUCLEAR REACTIONS 12C(238U, F)240Pu/241Pu/250Cf*, E=6.1 MeV/nucleon; measured particle and γ spectra, (fragment)γ-coin, energy loss, time-of-flight, yields and angular distributions of fragments of Z=30-64, A=80-160 from fission of 250Cf, 240,241Pu using SPIDER, VAMOS, and EXOGAM detector systems at GANIL facility. Inverse kinematics and multi-nucleon transfer-induced fission. 110Ru, 144Ce; deduced levels from (fragment)γ coin spectra. Z=30, A=70-82, 85; Z=31, A=70-85; Z=32, A=71-87; Z=33, A=73-89; Z=34, A=73, 75-90; Z=35, A=79-93; Z=36, A=81-96; Z=37, A=83-99; Z=38, A=86-102; Z=39, A=88-105; Z=40, A=90-107; Z=41, A=93-110; Z=42, A=95-113; Z=43, A=97-115; Z=44, A=100-118; Z=45, A=102-120; Z=46, A=104-122; Z=47, A=107-126; Z=48, A=109-127; Z=49, A=112-131; Z=50, A=114-133; Z=51, A=116-135; Z=52, A=118-138; Z=53, A=122-141; Z=54, A=123-143; Z=55, A=126-146; Z=56, A=130-148; Z=57, A=131-150; Z=58, A=134-152; Z=59, A=137-153; Z=60, A=139-156; Z=61, A=142-158; Z=62, A=144-159; Z=63, A=149-160; Z=64, A=151-159; measured yields from fission of compound nucleus 250Cf. Z=34, A=82-88; Z=35, A=85-92; Z=36, A=85-94; Z=37, A=87-97; Z=38, A=90-101; Z=39, A=91-102; Z=40, A=94-106; Z=41, A=95-109; Z=42, A=98-111; Z=43, A=101-112; Z=44, A=104-114; Z=45, A=105-114; Z=46, A=110-116; Z=47, A=114-119; Z=48, A=115, 118-122; Z=49, A=122-130; Z=50, A=125-134, 136; Z=51, A=125-137; Z=52, A=129-139; Z=53, A=128-140; Z=54, A=130-144; Z=55, A=133-145; Z=56, A=134-145; Z=57, A=138-149; Z=58, A=142-151; Z=59, A=145-152; Z=60, A=148-154; measured yields from fission of multi-nucleon transfer induced nuclei 240,241Pu.
doi: 10.1103/PhysRevC.88.024605
2013GU27 Phys.Rev. C 88, 024307 (2013) M.Guttormsen, B.Jurado, J.N.Wilson, M.Aiche, L.A.Bernstein, Q.Ducasse, F.Giacoppo, A.Gorgen, F.Gunsing, T.W.Hagen, A.C.Larsen, M.Lebois, B.Leniau, T.Renstrom, S.J.Rose, S.Siem, T.Tornyi, G.M.Tveten, M.Wiedeking Constant-temperature level densities in the quasicontinuum of Th and U isotopes NUCLEAR REACTIONS 232Th(d, p), (d, d'), (d, t), E=12 MeV; 232Th(3He, 3He'), (3He, α), E=24 MeV; 238U(d, p), (d, d'), (d, t), E=15 MeV; measured (particle)γ-coin in the quasicontinuum region using SiRi particle detector array and CACTUS-γ detector system at Oslo cyclotron laboratory; deduced excitation energy vs Eγ distributions. 231,232,233Th, 237,238,239U; deduced level densities using the Oslo method, increase in level density for odd-A isotopes as compared to even-even isotopes, similar temperatures in the quasicontinuum. 237,238,239U; deduced entropy, excess of entropy for odd-A isotopes as compared to even-even neighbor, microcanonical temperature, heat capacity. Evidence for continuous melting of Cooper pairs from constant temperature behavior.
doi: 10.1103/PhysRevC.88.024307
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
2012BE38 J.Phys.:Conf.Ser. 337, 012070 (2012) J.Benlliure, H.Alvarez-Pol, T.Kurtukian-Nieto, A.I.Morales, L.Audouin, F.Becker, B.Blank, I.Borzov, E.Casarejos, D.Cortina-Gil, B.Fernandez, J.Giovinazzo, D.Henzlova, B.Jurado, L.Langanke, G.Martinez-Pinedo, P.Napolitani, J.Pereira, F.Rejmund, K.-H.Schmidt, O.Yordanov, for the RISING Collaboration Approaching r-process nuclei at N = 126 RADIOACTIVITY 194,195,196Re, 199,200Os, 198,201,202Ir, 203,204Pt, 204Au(β-); measured Iβ(t) using DSSSD; deduced T1/2; calculated T1/2 using Gross theory, FR droplet model and energy-density functional.
doi: 10.1088/1742-6596/337/1/012070
2012BO08 Phys.Lett. B 712, 319 (2012) G.Boutoux, B.Jurado, V.Meot, O.Roig, L.Mathieu, M.Aiche, G.Barreau, N.Capellan, I.Companis, S.Czajkowski, K.-H.Schmidt, J.T.Burke, A.Bail, J.M.Daugas, T.Faul, P.Morel, N.Pillet, C.Theroine, X.Derkx, O.Serot, I.Matea, L.Tassan-Got Study of the surrogate-reaction method applied to neutron-induced capture cross sections NUCLEAR REACTIONS 174Yb(3He, αγ), (3He, pγ), E=24 MeV; measured reaction products, Eγ, Iγ; deduced σ, J, π. TALYS nuclear reaction model code calculations, comparison with available data.
doi: 10.1016/j.physletb.2012.05.012
2012KE04 Phys.Rev. C 85, 044613 (2012) G.Kessedjian, G.Barreau, M.Aiche, B.Jurado, A.Bidaud, S.Czajkowski, D.Dassie, B.Haas, L.Mathieu, L.Tassan-Got, J.N.Wilson, F.-J.Hambsch, S.Oberstedt, I.AlMahamid, J.Floyd, W.Lukens, D.Shuh 243Am neutron-induced fission cross section in the fast neutron energy range NUCLEAR REACTIONS 243Am(n, F), E=1-8 MeV; measured fission fragment spectra, σ(E). Measurements with reference to 235,238U(n, F), and 1H(n, p). Variance-covariance analysis and interpretation by principal components. Comparison with previous studies and evaluated data libraries.
doi: 10.1103/PhysRevC.85.044613
2012SC15 Phys.Rev. C 86, 044322 (2012) Inconsistencies in the description of pairing effects in nuclear level densities
doi: 10.1103/PhysRevC.86.044322
2011BO30 J.Korean Phys.Soc. 59, 1924s (2011) G.Boutoux, B.Jurado, V.Meot, M.Aiche, A.Bail, G.Barreau, E.Bauge, J.T.Burke, N.Capellan, I.Companis, S.Czajkowski, J.M.Daugas, D.Dassie, X.Derkx, T.Faul, B.Haas, L.Gaudefroy, F.Gunsing, I.Matea, L.Mathieu, P.Morel, N.Pillet, M.G.Porquet, O.Roig, P.Romain, O.Serot, J.Taieb, L.Tassan-Got, C.Theroine Neutron-Induced Capture Cross Sections via the Surrogate Reaction Method NUCLEAR REACTIONS 174Yb(3He, pγ), E=24 MeV; measured Ep, Ip(θ) using Si(Li), Eγ, Iγ using C6D6, pγ-coin, γγ-coin. 176Lu deduced γ emission probability, 175Lu(n, γ) σ using surrogate reaction; calculated 176Lu γ emission probability, 175Lu(n, γ) σ using TALYS.
doi: 10.3938/jkps.59.1924
2011BU11 J.Korean Phys.Soc. 59, 1892s (2011) J.T.Burke, J.J.Ressler, J.E.Escher, N.D.Scielzo, I.J.Thompson, R.Henderson, J.Gostic, L.Bernstein, D.Bluel, M.Weideking, V.Meot, O.Roig, L.W.Phair, R.Hatarik, J.Munson, C.Angell, B.Goldblum, C.W.Beausang, T.Ross, R.Hughes, M.Aiche, G.Barreau, N.Cappelan, S.Czajkowski, B.Hass, B.Jurado, L.Mathieu, I.Companis Experimental Approaches to Studying the Fission Process Using the Surrogate Reaction Technique NUCLEAR REACTIONS 235,236U, 239Pu(α, α'), E=55 MeV; measured E(charged particle), I(charged particle), Eγ, Iγ(θ), γγ-coin, fission products using STARS (Silicon Telescope Array for Reaction Studies), LIBERACE, HYDRA; deduced σ 238Pu(n, F) below 20 MeV using surrogate reactions. Comparison with other data.
doi: 10.3938/jkps.59.1892
2011SC02 Phys.Rev. C 83, 014607 (2011) Thermodynamics of nuclei in thermal contact NUCLEAR STRUCTURE 172Yb; calculated transport of excitation energy by nucleon exchange; deduced thermal averaging of fluctuations in measured level densities, dependence of excitation energy division on the level densities. Heat exchange between nascent fragments using statistical mechanics. Energy sorting mechanism. Schematic dynamical microscopic model for Fermi-Dirac gases in contact. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.014607
2011SC16 Phys.Rev. C 83, 061601 (2011); Erratum Phys.Rev. C 84, 059906 (2011) Final excitation energy of fission fragments
doi: 10.1103/PhysRevC.83.061601
2010AL24 Phys.Rev. C 82, 041602 (2010) H.Alvarez-Pol, J.Benlliure, E.Casarejos, L.Audouin, D.Cortina-Gil, T.Enqvist, B.Fernandez-Dominguez, A.R.Junghans, B.Jurado, P.Napolitani, J.Pereira, F.Rejmund, K.-H.Schmidt, O.Yordanov Production of new neutron-rich isotopes of heavy elements in fragmentation reactions of 238U projectiles at 1A GeV NUCLEAR REACTIONS 9Be(238U, X), E=1 GeV/nucleon; measured fragment residues using a high resolution magnetic spectrometer Fragment Separator, σ, yields. 203,204,205Pt, 207,208,209,210Au, 210,211,212,213,214,215,216Hg, 210,211,212,213,214,215,216,217Tl, 214,215,216,217,218,219,220Pb, 217,218,219,220,221,222,223,224Bi, 220,221,222,223,224,225,226,227Po, 222,223,224,225,226,227,228,229At, 225,226,227,228,229,230,231Rn, 228,229,230,232,232,233Fr; deduced yields, production σ. Comparisons of σ with the predictions obtained using the computer codes COFRA and EPAX.
doi: 10.1103/PhysRevC.82.041602
2010KE05 Phys.Lett. B 692, 297 (2010) G.Kessedjian, B.Jurado, M.Aiche, G.Barreau, A.Bidaud, S.Czajkowski, D.Dassie, B.Haas, L.Mathieu, L.Audouin, N.Capellan, L.Tassan-Got, J.N.Wilson, E.Berthoumieux, F.Gunsing, Ch.Theisen, O.Serot, E.Bauge, I.Ahmad, J.P.Greene, R.V.F.Janssens Neutron-induced fission cross sections of short-lived actinides with the surrogate reaction method NUCLEAR REACTIONS 243Am(3He, d), (3He, t), (3He, α), E=24, 30 MeV; 242,243Cm, 241Am(n, F), E<10 MeV; measured surrogate reaction products; deduced fission σ. Comparison with experimental data, JENDL-3.3, ENDF/B-VII.0 and JEFF-3.1 libraries.
doi: 10.1016/j.physletb.2010.07.048
2010SC09 Phys.Rev.Lett. 104, 212501 (2010) Entropy Driven Excitation Energy Sorting in Superfluid Fission Dynamics NUCLEAR REACTIONS 237Np(n, F), E=0.8, 5.55 MeV; analyzed average number of prompt neutrons as a function of the primary fragment mass; deduced neutron yields for light and heavy fragments, peculiar state of thermal equilibrium at scission, energy-sorting mechanism.
doi: 10.1103/PhysRevLett.104.212501
2010SC14 Phys.Rev. C 81, 064602 (2010) C.Schmitt, K.-H.Schmidt, A.Kelic, A.Heinz, B.Jurado, P.N.Nadtochy Fragmentation of spherical radioactive heavy nuclei as a novel probe of transient effects in fission NUCLEAR REACTIONS Pb(205At, X), (206At, X), (207Rn, X), (209Rn, X), (212Fr, X), (217Fr, X), (218Fr, X), (211Ra, X), (212Ra, X), (213Ra, X), (214Ra, X), (215Ra, X), (216Ra, X), (217Ra, X), (218Ra, X), (219Ra, X), (220Ra, X), (221Ra, X), (222Ra, X), (223Ra, X), (215Ac, X), (216Ac, X), (217Ac, X), (218Ac, X), (219Ac, X), (220Ac, X), (221Ac, X), (222Ac, X), (223Ac, X), (224Ac, X), (225Ac, X), (226Ac, X), (221Th, X), (222Th, X), (224Th, X), [secondary radioactive beams from primary reaction Be(238U, X), E=1000 MeV/nucleon], E=420 MeV/nucleon; measured σ, charge correlations of two fragments, deformation parameter, transient time as a function of ΔZ. Comparison with model calculations and Kramer-type calculations.
doi: 10.1103/PhysRevC.81.064602
2009AL32 Eur.Phys.J. A 42, 485 (2009) H.Alvarez-Pol, J.Benlliure, E.Casarejos, L.Audouin, D.Cortina-Gil, T.Enqvist, B.Fernandez, A.R.Junghans, B.Jurado, P.Napolitani, J.Pereira, F.Rejmund, K.-H.Schmidt, O.Yordanov Production cross-sections of neutron-rich Pb and Bi isotopes in the fragmentation of 238U NUCLEAR REACTIONS 9Be(238U, X)196Pb/197Pb/198Pb/199Pb/200Pb/201Pb/202Pb/203Pb/204Pb/205Pb/206Pb/207Pb/208Pb/209Pb/210Pb/214Pb/215Pb/216Pb/217Pb/218Pb/219Pb/199Bi/200Bi/201Bi/202Bi/203Bi/204Bi/205Bi/206Bi/207Bi/208Bi/209Bi/210Bi/211Bi/212Bi/213Bi/214Bi/218Bi/219Bi/220Bi/221Bi/222Bi/223Bi, E=1 GeV/nucleon; measured production σ. Comparison with other data.
doi: 10.1140/epja/i2009-10856-8
2009KU28 Nucl.Phys. A827, 587c (2009) T.Kurtukian-Nieto, J.Benlliure, K.-H.Schmidt, L.Audouin, F.Becker, B.Blank, I.N.Borzov, E.Casarejos, M.Fernandez-Ordonez, J.Giovinazzo, D.Henzlova, B.Jurado, K.Langanke, G.Martinez-Pinedo, J.Pereira, F.Rejmund, O.Yordanov Recent progress in measuring β half-lives of nuclei approaching the r-process waiting point A = 195 RADIOACTIVITY 194,195,196Re, 199,200Os, 198,199,200Ir(β-) [from Be(208Pb, X), E=1 GeV/nucleon]; measured T1/2. Comparison with two QRPA models.
doi: 10.1016/j.nuclphysa.2009.05.129
2009SC26 Int.J.Mod.Phys. E18, 2150 (2009) C.Schmitt, A.Kelic, K.-H.Schmidt, A.Heinz, B.Jurado, P.N.Nadtochy Fragmentation of radioactive beams for tailoring fission transients
doi: 10.1142/S0218301309014469
2009SH42 Phys.Rev. C 80, 051305 (2009) A.Shrivastava, M.Caamano, M.Rejmund, A.Navin, F.Rejmund, K.-H.Schmidt, A.Lemasson, C.Schmitt, L.Gaudefroy, K.Sieja, L.Audouin, C.O.Bacri, G.Barreau, J.Benlliure, E.Casarejos, X.Derkx, B.Fernandez-Dominguez, C.Golabek, B.Jurado, T.Roger, J.Taieb Prompt γ-ray spectroscopy of isotopically identified fission fragments NUCLEAR REACTIONS 12C(238U, X), E=1.45 GeV; measured Eγ, Iγ using EXOGAM array, fission fragments using VAMOS detector. 134Xe; deduced levels, J, π. 100Zr, 106,107,108,109Ru, 133Xe, 138Xe; measured Eγ. Comparison with shell model calculations for Z>49, N<83 nuclei.
doi: 10.1103/PhysRevC.80.051305
2009TA20 Int.J.Mod.Phys. E18, 767 (2009) J.Taieb, G.Belier, A.Chatillon, T.Granier, A.Kelic, V.Ricciardi, K.-H.Schmidt, B.Voss, M.Coste-Delclaux, C.Diop, C.Jouanne, C.Schmitt, M.Aiche, S.Czajkowski, B.Jurado, L.Audouin, J.Peyre, P.Rosier, L.Tassan-got, E.Bertoumieux, D.Dore, E.Dupont, A.Letourneau, S.Panebianco ELISe: A new facility for unprecedented experimental nuclear fission studies
doi: 10.1142/S0218301309012859
2008CA22 Phys.Rev. C 78, 044001 (2008) M.Caamano, D.Cortina-Gil, W.Mittig, H.Savajols, M.Chartier, C.E.Demonchy, B.Fernandez, M.B.Gomez Hornillos, A.Gillibert, B.Jurado, O.Kiselev, R.Lemmon, A.Obertelli, F.Rejmund, M.Rejmund, P.Roussel-Chomaz, R.Wolski Experimental study of resonance states in 7H and 6H NUCLEAR REACTIONS 12C(8He, 6H), (8He, 7H), E=15.4 MeV/nucleon; measured particle spectra. 5,6,7H; deduced excitation energies, resonances, widths. Comparison with phase space calculations.
doi: 10.1103/PhysRevC.78.044001
2008HE13 Phys.Rev. C 78, 044616 (2008) D.Henzlova, K.-H.Schmidt, M.V.Ricciardi, A.Kelic, V.Henzl, P.Napolitani, L.Audouin, J.Benlliure, A.Boudard, E.Casarejos, J.E.Ducret, T.Enqvist, A.Heinz, A.Junghans, B.Jurado, A.Krasa, T.Kurtukian, S.Leray, M.F.Ordonez, J.Pereira, R.Pleskac, F.Rejmund, C.Schmitt, C.Stephan, L.Tassan-Got, C.Villagrasa, C.Volant, A.Wagner, O.Yordanov Experimental investigation of the residues produced in the 136Xe + Pb and 124Xe + Pb fragmentation reactions at 1A GeV NUCLEAR REACTIONS Pb(124Xe, X), (136Xe, X)Z=3-56, E=1 GeV/nucleon; measured σ. Production cross sections for over 1100 individual nuclides measured.
doi: 10.1103/PhysRevC.78.044616
2007BO37 Eur.Phys.J. A 33, 47 (2007) D.Boilley, A.Marchix, B.Jurado, K.-H.Schmidt A new formula for the saddle-to-scission time
doi: 10.1140/epja/i2007-10415-5
2007CA28 Phys.Rev.Lett. 99, 062502 (2007) M.Caamano, D.Cortina-Gil, W.Mittig, H.Savajols, M.Chartier, C.E.Demonchy, B.Fernandez, M.B.Gomez Hornillos, A.Gillibert, B.Jurado, O.Kiselev, R.Lemmon, A.Obertelli, F.Rejmund, M.Rejmund, P.Roussel-Chomaz, R.Wolski Resonance State in 7H NUCLEAR REACTIONS 12C(8He, p), E=15.4 MeV/nucleon; measured particle energies and excitation energy distributions. 7H deduced resonance energies.
doi: 10.1103/PhysRevLett.99.062502
2007CA47 Eur.Phys.J. Special Topics 150, 9 (2007) M.Caamano, D.Cortina-Gil, W.Mittig, H.Savajols, M.Chartier, C.E.Demonchy, B.Fernandez, A.Gillibert, M.B.Gomez Hornillos, B.Jurado, O.Kiselev, R.Lemmon, A.Obertelli, F.Rejmund, M.Rejmund, P.Roussel-Chomaz, R.Wolski The search for 7H NUCLEAR REACTIONS 12C(8He, 7H), E=15.4 MeV/nucleon; measured production σ(θ). 7H; deduced resonance parameters.
doi: 10.1140/epjst/e2007-00252-2
2007GI08 Nucl.Phys. A787, 423c (2007) A.Gillibert, N.Alamanos, M.Alvarez, F.Auger, D.Beaumel, E.Becheva, Y.Blumenfeld, R.Dayras, F.Delaunay, A.Drouart, G.de France, L.Giot, B.Jurado, N.Keeley, K.W.Kemper, V.Lapoux, W.Mittig, X.Mougeot, L.Nalpas, A.Obertelli, N.Patronis, A.Pakou, E.C.Pollacco, R.Raabe, P.Roussel-Chomaz, F.Rejmund, M.Rejmund, H.Savajols, J.A.Scarpaci, J.L.Sida, F.Skaza, S.Stepantsov, Ch.Theisen, R.Wolski Structure of exotic nuclei from direct reactions NUCLEAR REACTIONS 1H(8He, 8He), (8He, d), (8He, t), E=15.7, 61.3 MeV/nucleon; analyzed σ(θ). Coupled reaction channel calculations, DWBA analysis. 2H(26Ne, p), E=9.7 MeV/nucleon; measured fragment yield, Eγ, Iγ, (particle)γ-coin. 27Ne deduced levels, J, π. Exogam array, Vamos spectrometer.
doi: 10.1016/j.nuclphysa.2006.12.064
2007GI17 Eur.Phys.J. Special Topics 150, 161 (2007) A.Gillibert, A.Obertelli, N.Alamanos, M.Alvarez, F.Auger, R.Dayras, A.Drouart, G.de France, B.Jurado, N.Keeley, V.Lapoux, W.Mittig, X.Mougeot, L.Nalpas, A.Pakou, N.Patronis, E.Pollacco, F.Rejmund, M.Rejmund, P.Roussel-Chomaz, H.Savajols, F.Skaza, Ch.Theisen Study of N = 16 for Ne isotopes NUCLEAR REACTIONS 2H(26Ne, p), E=9.7 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin. 27Ne; deduced levels, cross sections, and spectroscopic factors.
doi: 10.1140/epjst/e2007-00293-5
2007JU03 Phys.Lett. B 649, 43 (2007) B.Jurado, H.Savjols, W.Mittig, N.A.Orr, P.Roussel-Chomaz, D.Baiborodin, W.N.Catford, M.Chartier, C.E.Demonchy, Z.Dlouhy, A.Gillibert, L.Giot, A.Khouaja, A.Lepine-Szily, S.Lukyanov, J.Mrazek, Y.E.Penionzhkevich, S.Pita, M.Rousseau, A.C.Villari Mass measurements of neutron-rich nuclei near the N = 20 and 28 shell closures ATOMIC MASSES 23N, 23,24O, 25,26,27F, 27,28,29,30,31Ne, 31,32,33Na, 34,35,36Mg, 34,35,36,37,38,39Al, 36,37,38,39,40,41,42Si, 40,41,42,43,44P, 40,43,44,45S, 43,45,46,47Cl; measured masses; analysed neutron separation energy. Cyclotron-based mass spectrometry.
doi: 10.1016/j.physletb.2007.04.006
2007SC28 Phys.Rev.Lett. 99, 042701 (2007) C.Schmitt, P.N.Nadtochy, A.Heinz, B.Jurado, A.Kelic, K.-H.Schmidt First Experiment on Fission Transients in Highly Fissile Spherical Nuclei Produced by Fragmentation of Radioactive Beams NUCLEAR REACTIONS 208Pb(205At, X), (207Rn, X), (208Fr, X), (211Ra, X), (215Ra, X), (215Ac, X), (219Ac, X), (221Th, X), (222Th, X), (223Ac, X), E=530 MeV/nucleon; measured widths of fission fragment nuclear-charge distributions.
doi: 10.1103/PhysRevLett.99.042701
2007VI06 Phys.Rev. C 75, 044603 (2007) C.Villagrasa-Canton, A.Boudard, J.-E.Ducret, B.Fernandez, S.Leray, C.Volant, P.Armbruster, T.Enqvist, F.Hammache, K.Helariutta, B.Jurado, M.-V.Ricciardi, K.-H.Schmidt, K.Summerer, F.Vives, O.Yordanov, L.Audouin, C.-O.Bacri, L.Ferrant, P.Napolitani, F.Rejmund, C.Stephan, L.Tassan-Got, J.Benlliure, E.Casarejos, M.Fernandez-Ordonez, J.Pereira, S.Czajkowski, D.Karamanis, M.Pravikoff, J.S.George, R.A.Mewaldt, N.Yanasak, M.Wiedenbeck, J.J.Connell, T.Faestermann, A.Heinz, A.Junghans Spallation residues in the reaction 56Fe+p at 0.3A, 0.5A, 0.75A, 1.0A, and 1.5A GeV NUCLEAR REACTIONS 1H(56Fe, X), E=0.3, 0.5, 0.75, 1.0, 1.5 GeV/nucleon; measured spallation products isotopic yields, excitation functions.
doi: 10.1103/PhysRevC.75.044603
2006AU01 Nucl.Phys. A768, 1 (2006) L.Audouin, L.Tassan-Got, P.Armbruster, J.Benlliure, M.Bernas, A.Boudard, E.Casarejos, S.Czajkowski, T.Enqvist, B.Fernandez-Dominguez, B.Jurado, R.Legrain, S.Leray, B.Mustapha, J.Pereira, M.Pravikoff, F.Rejmund, M.-V.Ricciardi, K.-H.Schmidt, C.Stephan, J.Taieb, C.Volant, W.Wlazlo Evaporation residues produced in spallation of 208Pb by protons at 500 A MeV NUCLEAR REACTIONS 1H(208Pb, X), E=500 MeV/nucleon; measured spallation fragments isotopic production σ, momentum transfer distributions; deduced reaction mechanism features. Comparisons with model predictions and results from higher-energy reactions.
doi: 10.1016/j.nuclphysa.2006.01.006
2006OB01 Phys.Lett. B 633, 33 (2006) A.Obertelli, A.Gillibert, N.Alamanos, M.Alvarez, F.Auger, R.Dayras, A.Drouart, G.de France, B.Jurado, N.Keeley, V.Lapoux, W.Mittig, X.Mougeot, L.Nalpas, A.Pakou, N.Patronis, E.C.Pollacco, F.Rejmund, M.Rejmund, P.Roussel-Chomaz, H.Savajols, F.Skaza, Ch.Theisen Shell gap reduction in neutron-rich N=17 nuclei NUCLEAR REACTIONS 2H(26Ne, p), E=9.7 MeV/nucleon; measured Eγ, Iγ, (charged-particle)γ-coin, σ(E). 27Ne deduced levels, J, π, spectroscopic factor.
doi: 10.1016/j.physletb.2005.11.033
2006OB05 Phys.Rev.C 74, 064305 (2006) A.Obertelli, A.Gillibert, N.Alamanos, M.A.G.Alvarez, F.Auger, R.Dayras, A.Drouart, N.Keeley, V.Lapoux, X.Mougeot, L.Nalpas, E.Pollacco, F.Skaza, Ch.Theisen, G.de France, B.Jurado, W.Mittig, F.Rejmund, M.Rejmund, P.Roussel-Chomaz, H.Savajols, A.Pakou, N.Patronis γ spectroscopy of 25, 27Ne and 26, 27Na NUCLEAR REACTIONS 2H(26Ne, 26Ne'), (26Ne, 25Ne), (26Ne, 27Ne), (26Ne, 26Na), (26Ne, 27Na), E=9.7 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin. 25,26,27Ne, 26,27Na deduced levels, J, π. Exogam array, Vamos spectrometer, comparison with previous results and model predictions.
doi: 10.1103/PhysRevC.74.064305
2005DE49 J.Phys.(London) G31, S1831 (2005) C.E.Demonchy, W.Mittig, H.Savajols, M.Caamano, M.Chartier, D.Cortina-Gil, A.Fomichev, A.Gillibert, L.Giot, M.S.Golovkov, B.Jurado, A.Obertelli, E.Pollacco, P.Roussel-chomaz, A.Rodin, S.Stepantsov, G.Ter-Akopian, H.Wang First results of the new active target MAYA NUCLEAR REACTIONS H, C(8He, pX), (8He, dX), (8He, tX), E=3.5 MeV/nucleon; measured particle spectra, relative yields. Isobutane target.
doi: 10.1088/0954-3899/31/10/082
2005FE02 Nucl.Phys. A747, 227 (2005) B.Fernandez-Dominguez, P.Armbruster, L.Audouin, J.Benlliure, M.Bernas, A.Boudard, E.Casarejos, S.Czajkowski, J.E.Ducret, T.Enqvist, B.Jurado, R.Legrain, S.Leray, B.Mustapha, J.Pereira, M.Pravikoff, F.Rejmund, M.V.Ricciardi, K.-H.Schmidt, C.Stephan, J.Taieb, L.Tassan-Got, C.Volant, W.Wlazlo Nuclide cross-sections of fission fragments in the reaction 208Pb + p at 500 A MeV NUCLEAR REACTIONS 1H(208Pb, X), E=500 MeV/nucleon; measured spallation fragments isotopic production σ, kinetic energy distributions; deduced reaction mechanism features. Comparisons with model predictions and results from higher-energy reactions.
doi: 10.1016/j.nuclphysa.2004.10.013
2005GO36 J.Phys.(London) G31, S1869 (2005) M.B.Gomez Hornillos, M.Chartier, W.Mittig, B.Blank, F.Chautard, C.E.Demonchy, A.Gillibert, B.Jacquot, B.Jurado, N.Lecesne, A.Lepine-Szily, N.A.Orr, P.Roussel-Chomaz, H.Savajols, A.C.C.Villari Mass measurements with the CIME cyclotron at GANIL ATOMIC MASSES 12C, 16O, 20Ne, 32S, 36,40Ar; measured masses. Cyclotron-based mass spectrometry.
doi: 10.1088/0954-3899/31/10/090
2005HE07 Nucl.Phys. A749, 110c (2005) D.Henzlova, L.Audouin, J.Benlliure, A.S.Botvina, A.Boudard, E.Casarejos, J.E.Ducret, T.Enqvist, L.T.Got, A.Heinz, V.Henzl, A.Junghans, B.Jurado, A.Kelic, A.Krasa, T.Kurtukian, S.Leray, P.Napolitani, M.F.Ordonez, J.Pereira, R.Pleskac, F.Rejmund, M.V.Ricciardi, K.-H.Schmidt, Ch.Schmitt, C.Stephan, C.Villagrasa, C.Volant, A.Wagner, O.Yordanov Isotopically resolved residues from the fragmentation of projectiles with largely different N/Z - the isospin-thermometer method NUCLEAR REACTIONS Pb(124Xe, X), (136Xe, X), E=1 GeV/nucleon; measured fragments charge and mass distributions; deduced freeze-out temperature.
doi: 10.1016/j.nuclphysa.2004.12.016
2005JU01 Nucl.Phys. A747, 14 (2005) B.Jurado, C.Schmitt, K.-H.Schmidt, J.Benlliure, A.R.Junghans A critical analysis of the modelling of dissipation in fission NUCLEAR STRUCTURE 248Cm; calculated time-dependent fission decay rate, dissipation effects. Langevin equation, Fokker-Planck equation, analytical approximation.
doi: 10.1016/j.nuclphysa.2004.09.123
2005JU09 Nucl.Phys. A757, 329 (2005) B.Jurado, C.Schmitt, K.-H.Schmidt, J.Benlliure, A.R.Junghans Conditions for the manifestation of transient effects in fission NUCLEAR REACTIONS U, Au(238U, F), E=1 GeV/nucleon; analyzed fission σ; deduced role of transient effects.
doi: 10.1016/j.nuclphysa.2005.04.020
2005MI31 Eur.Phys.J. A 25, Supplement 1, 263 (2005) W.Mittig, C.E.Demonchy, H.Wang, P.Roussel-Chomaz, B.Jurado, M.Gelin, H.Savajols, A.Fomichev, A.Rodin, A.Gillibert, A.Obertelli, M.D.Cortina-Gil, M.Caamano, M.Chartier, R.Wolski Reactions induced beyond the dripline at low energy by secondary beams NUCLEAR REACTIONS H, C(8He, pX), (8He, dX), (8He, tX), E=2-3.5 MeV/nucleon; measured particle spectra, relative yields; 7He deduced production σ and spectroscopic factor. Isobutane target.
doi: 10.1140/epjad/i2005-06-138-5
2005SA61 Eur.Phys.J. A 25, Supplement 1, 23 (2005) H.Savajols, B.Jurado, W.Mittig, D.Baiborodin, W.Catford, M.Chartier, C.E.Demonchy, Z.Dlouhy, A.Gillibert, L.Giot, A.Khouaja, A.Lepine-Szily, S.Lukyanov, J.Mrazek, N.Orr, Y.Penionzhkevich, S.Pita, M.Rousseau, P.Roussel-Chomaz, A.C.C.Villari New mass measurements at the neutron drip-line NUCLEAR STRUCTURE Z=8-20; analyzed data; deduced two-neutron separation energies and shell correction energies.
doi: 10.1140/epjad/i2005-06-189-6
2004JU05 Phys.Rev.Lett. 93, 072501 (2004) B.Jurado, C.Schmitt, K.-H.Schmidt, J.Benlliure, T.Enqvist, A.R.Junghans, A.Kelic, F.Rejmund Transient Effects in Fission from New Experimental Signatures NUCLEAR REACTIONS H, C, Pb(238U, X), E=1 GeV/nucleon; measured projectile fission σ, fragment charge distributions; deduced transient effects, damping of collective motion. Abrasion-ablation model analysis.
doi: 10.1103/PhysRevLett.93.072501
2004SC09 Int.J.Mod.Phys. E13, 97 (2004) C.Schmitt, B.Jurado, A.R.Junghans, K.-H.Schmidt, J.Benlliure Modelling of dissipation in nuclear fission NUCLEAR REACTIONS 208Pb(232Th, X), E=0.6 GeV; calculated partial fission σ, fragment charge distribution widths, dissipation effects.
doi: 10.1142/S0218301304001783
2003JU01 Phys.Lett. B 553, 186 (2003) B.Jurado, K.-H.Schmidt, J.Benlliure Time evolution of the fission-decay width under the influence of dissipation NUCLEAR REACTIONS Pb(238U, X), E=1 GeV/nucleon; calculated induced fission σ, time-dependent width, dissipation effects. Fokker-Planck equation, comparison with data.
doi: 10.1016/S0370-2693(02)03234-3
2002RE36 Acta Phys.Hung.N.S. 16, 85 (2002) F.Rejmund, A.Bethenod, P.Napolitani, J.Taieb, C.Villagrasa, L.Audouin, P.Armbruster, C.O.Bacri, J.Benlliure, M.Bernas, B.Berthier, A.Boudard, E.Casajeros, S.Czajkowski, J.J.Connell, T.Enqvist, T.Faestermann, J.S.George, A.Junghans, B.Jurado, F.Hammache, S.Leray, R.Legrain, R.A.Mewaldt, J.Pereira, M.V.Ricciardi, K.-H.Schmidt, C.Stephan, K.Summerer, L.Tassan-Got, C.Volant, M.E.Wiedenbeck, W.Wlazlo, N.E.Yanasak Disappearance of Shell Effects and Persistence of an Even-Odd Staggering in the Fragment Production in Nuclear Reactions at Relativistic Energies NUCLEAR REACTIONS 1H(U, X), (Fe, X), E=1 GeV/nucleon; measured fragments isotopic yields; deduced shell and pairing effects.
doi: 10.1556/APH.16.2002.1-4.10
2002SC54 J.Nucl.Radiochem.Sci. 3, No 1, 51 (2002) K.-H.Schmidt, P.Armbruster, J.Benlliure, C.Bockstiegel, A.Botvina, H.-G.Clerc, T.Enqvist, A.Grewe, A.Heinz, A.R.Junghans, B.Jurado, J.Muller, M.V.Ricciardi, F.Rejmund, S.Steinhauser, B.Voss Experiments on Fission Dynamics with Relativistic Heavy-ion Beams
2000JU06 Acta Phys.Pol. B31, 367 (2000) B.Jurado, K.-H.Schmidt, F.Farget, T.Enqvist, F.Ameil, P.Armbruster, J.Benlliure, M.Bernas, B.Mustapha, L.Tassan-Got, C.Stephan, A.Boudard, S.Leray, R.Legrain, C.Volant, S.Czajkowski, M.Pravikoff Projectile Fragmentation at Relativistic Energies: A possibility to determine the viscosity of nuclear matter NUCLEAR REACTIONS Pb(238U, X), E=1 GeV/nucleon; measured partial fission σ vs fragment charge; deduced dissipation coefficient.
Back to query form |