NSR Query Results
Output year order : Descending NSR database version of April 23, 2024. Search: Author = H.Faust Found 78 matches. 2021CH64 Eur.Phys.J. A 57, 335 (2021) A.Chebboubi, G.Kessedjian, O.Serot, H.Faust, U.Koster, O.Litaize, C.Sage, A.Blanc, D.Bernard, A.Letourneau, T.Materna, O.Meplan, P.Mutti, M.Rapala, M.Ramdhane Measurements of 233U(nth, f) fission product mass yields with the LOHENGRIN recoil mass spectrometer NUCLEAR REACTIONS 233U(n, F), E thermal; measured reaction products; deduced fission product mass yields, mean and total kinetic energies. Comparison with ENDF/B-VIII.0 and JEFF-3.3 libraries. The LOHENGRIN recoil mass spectrometer of the ILL.
doi: 10.1140/epja/s10050-021-00645-y
2018AL14 Phys.Rev. C 97, 034327 (2018) P.Alexa, M.Ramdhane, G.Thiamova, G.S.Simpson, H.R.Faust, J.Genevey, U.Koster, T.Materna, R.Orlandi, J.A.Pinston, A.Scherillo, Z.Hons Quasiparticle phonon model description of low-energy states in 152Pr RADIOACTIVITY 152Pr(IT)[from 241Am(n, F), E=thermal, followed by mass separation of A=152 fission fragments using Lohengrin separator at ILL-Grenoble]; measured Eγ, Iγ, ce, x rays, (A=152 ions)γ-coin, (A=152 ions)ce-coin, half-life of the isomer by (A=152 ions)γ(t), conversion coefficients. 152Pr; deduced levels, J, π, multipolarities, configurations. Comparison with quasiparticle phonon model (QPM), combined with the particle-rotor model to include octupole correlations and Coriolis mixing. 152Nd; calculated energies of the first two 3- levels in connection with β- decay of 152Pr g.s. to 152Nd.
doi: 10.1103/PhysRevC.97.034327
2018LO18 Phys.Rev. C 98, 024323 (2018) R.Lozeva, E.A.Stefanova, H.Naidja, F.Nowacki, T.Rzaca-Urban, J.Wisniewski, W.Urban, I.Ahmad, A.Blanc, G.De France, F.Didierjean, G.Duchene, H.Faust, J.P.Greene, U.Koster, P.Mutti, G.Simpson, A.G.Smith, T.Soldner, C.A.Ur New yrast and non-yrast states in 136I and medium-spin structure of 136I and 136Xe : Roles of the proton d5/2 and the neutron h9/2 orbitals beyond 132Sn NUCLEAR REACTIONS 235U, 241Pu(n, F)136I, E=thermal; measured Eγ, Iγ, γγ-coin, γγ(θ), γγ(linear pol) using the EXILL-FATIMA system, EXOGAM and EUROGAM clover HPGe detectors at ILL, Grenoble. 136I; deduced yrast and non-yrast levels, J, π, conversion coefficients, multipolarities, mixing ratios, configurations. Comparison with large scale shell-model calculations. RADIOACTIVITY 248Cm, 252Cf(SF); 136Te, 136I(β-)[136Te from 235U(n, F), E=thermal followed by separation of 136Te using Lohengrin fission-fragment separator at Grenoble, and 136I from 136Te decay]; measured Eγ, Iγ, γγ-coin, γγ(θ), γγ(lin pol). 136I, 136Xe; deduced levels, J, π, conversion coefficients, multipolarities, mixing ratios, configurations, Gamow-Teller strengths. Comparison with large scale shell-model calculations.
doi: 10.1103/PhysRevC.98.024323
2018RZ01 Phys.Rev. C 98, 064315 (2018) T.Rzaca-Urban, W.Urban, M.Czerwinski, J.Wisniewski, A.Blanc, H.Faust, M.Jentschel, P.Mutti, U.Koster, T.Soldner, G.de France, G.S.Simpson, C.A.Ur Low-spin excitations in 97Zr NUCLEAR REACTIONS 96Zr(n, γ), E=cold or thermal; measured Eγ, Iγ, γγ-coin, γγ(θ) using the EXILL HPGe array at the PF1B cold-neutron facility of ILL, Grenoble. 97Zr; deduced levels, J, π, multipolarities, mixing ratios, S(n), configurations. Comparison with previous experimental values. 27Al, 35Cl, 91Zr(n, γ), E=cold or thermal; measured Eγ, Iγ, data used for calibration purpose. 28Al, 92,97Zr; deduced S(n) and compared with literature values. RADIOACTIVITY 97,97mY(β-)[from 235U(n, F) using Lohengrin fission-fragment separator of the ILL]; measured Eγ, Iγ, γγ-coin, γγ(θ), γγ(linear polarization) using the EXILL Ge array. 97Zr; deduced levels, J, π, multipolarities, mixing ratios. 97Sr, 88Br(IT); measured isomer half-lives of 830-keV isomer in 97Sr, and 270-keV isomer in 88Br by γ(t).
doi: 10.1103/PhysRevC.98.064315
2017CH51 Phys.Lett. B 775, 190 (2017) A.Chebboubi, G.Kessedjian, O.Litaize, O.Serot, H.Faust, D.Bernard, A.Blanc, U.Koster, O.Meplan, P.Mutti, C.Sage Kinetic energy dependence of fission fragment isomeric ratios for spherical nuclei 132Sn NUCLEAR REACTIONS 235U(n, F)132Sn/132Te, E thermal; measured fission products, Eγ, Iγ; deduced γ-ray energies, isomeric ratios. Comparison with FIFRELIN code calculations.
doi: 10.1016/j.physletb.2017.10.067
2017GU18 Phys.Rev. C 96, 014608 (2017) Y.K.Gupta, D.C.Biswas, O.Serot, D.Bernard, O.Litaize, S.Julien-Laferriere, A.Chebboubi, G.Kessedjian, C.Sage, A.Blanc, H.Faust, U.Koster, A.Ebran, L.Mathieu, A.Letourneau, T.Materna, S.Panebianco Fission fragment yield distribution in the heavy-mass region from the 239Pu (nth, f) reaction NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured fission fragments in A=126 to 150 range using the Lohengrin recoil-mass spectrometer at ILL-Grenoble high-flux reactor facility; deduced distributions of kinetic energies and ionic charge, relative mass yields in three independent experiments. Comparison with JEFF-3.1.1 fission yield evaluation, and with predictions of Monte Carlo nuclear fission models using GEF and FIFRELIN codes.
doi: 10.1103/PhysRevC.96.014608
2017UR03 Phys.Rev. C 96, 044333 (2017) W.Urban, M.Czerwinski, J.Kurpeta, T.Rzaca-Urban, J.Wisniewski, T.Materna, L.W.Iskra, A.G.Smith, I.Ahmad, A.Blanc, H.Faust, U.Koster, M.Jentschel, P.Mutti, T.Soldner, G.S.Simpson, J.A.Pinston, G.de France, C.A.Ur, V.-V.Elomaa, T.Eronen, J.Hakala, A.Jokinen, A.Kankainen, I.D.Moore, J.Rissanen, A.Saastamoinen, J.Szerypo, C.Weber, J.Aysto Shape coexistence in the odd-odd nucleus 98Y: The role of the g9/2 neutron extruder NUCLEAR REACTIONS 235U(n, F), E=cold neutrons from PF1B facility at ILL Grenoble; measured Eγ, Iγ, γγ-coin, delayed γγ-coin, half-lives of several isomers in 98Y using the EXILL array at Grenoble. 98Y; deduced levels, isomers, J, π, bands, configurations, deformed and spherical isomers. RADIOACTIVITY 248Cm, 252Cf(SF); measured Eγ, Iγ, γγ-coin, γγ(θ), γγ-coin with γ rays from fission partner 147La in 248Cm SF decay using Eurogam2 array at Grenoble and Gammasphere array at Argonne. 98Y; deduced levels, J, π, multipolarities. 98Sr, 98,98mY(β-)[from 235U(n, F), E=cold neutrons and using Lohengrin fission-fragment separator]; measured Eγ, Iγ, γγ-coin, γγ(θ), γγ(linear pol), half-lives of decays of 98Sr, 98Y and 98Y isomer, excitation energy of the 2.36-s isomer in 98Y by using JYFLTRAP Penning trap at Jyvaskyla accelerator facility, . 98Y, 98Zr; deduced levels, J, π, multipolarities, mixing ratios, β feedings, logft, configurations. Comparison of negative-parity levels in 98Y with Interacting Boson Fermion Fermion Model (IBFFM) and Quasi-Particle Rotor Model (QPRM) calculations.
doi: 10.1103/PhysRevC.96.044333
2015MA51 Phys.Rev. C 92, 034305 (2015) T.Materna, W.Urban, K.Sieja, U.Koster, H.Faust, M.Czerwinski, T.Rzaca-Urban, C.Bernards, C.Fransen, J.Jolie, J.-M.Regis, T.Thomas, N.Warr Low spin structure of 86Se: Confirmation of γ collectivity at N=52 RADIOACTIVITY 86As(β-)[from 235U(n, F), E=thermal followed by mass separation using Lohengrin separator at ILL-Grenoble]; measured Eγ, Iγ, Eβ, βγ-, γγ-coin, γγ(θ). 86Se; deduced levels, J, π, γ collectivity. Comparison with systematics of neighboring nuclides, and with shell-model calculations. 94,96Y, 99Zr; observed γ rays. NUCLEAR STRUCTURE 86Se; calculated levels, J, π, B(M1), B(E2) using shell model. 84Ge, 86Se, 88Kr, 90Sr, 92Zr; calculated energies of second 2+ and 4+, and first 3+ states. Comparison with experimental values.
doi: 10.1103/PhysRevC.92.034305
2014MA61 Nucl.Data Sheets 119, 328 (2014) F.Martin, C.Sage, G.Kessedjian, O.Serot, C.Amouroux, C.O.Bacri, A.Bidaud, A.Billebaud, N.Capellan, S.Chabod, X.Doligez, H.Faust, U.Koster, A.Letourneau, T.Materna, L.Mathieu, O.Meplan, S.Panebianco Measurements of the Mass and Isotopic Yields of the 233U(nth, f) Reaction by the Lohengrin Spectrometer NUCLEAR REACTIONS 233U(n, F), E=thermal; measured reaction products; deduced fission mass yields, isotopic yields. Mass yields compared with JEFF-3.1.1, ENDF/B-VII.0, isotopic production with JEFF-3.1.1. and Piksaykin data. Isotopic production preliminary.
doi: 10.1016/j.nds.2014.08.090
2014SE17 Nucl.Data Sheets 119, 320 (2014) O.Serot, C.Amouroux, A.Bidaud, N.Capellan, S.Chabod, A.Ebran, H.Faust, G.Kessedjian, U.Koester, A.Letourneau, O.Litaize, F.Martin, T.Materna, L.Mathieu, S.Panebianco, J.-M.Regis, M.Rudigier, C.Sage, W.Urban Recent Results from Lohengrin on Fission Yields and Related Decay Properties NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured fission products; deduced fission yields.
doi: 10.1016/j.nds.2014.08.088
2012KU06 Phys.Rev. C 85, 027302 (2012) J.Kurpeta, W.Urban, T.Materna, H.Faust, U.Koster, J.Rissanen, T.Rzaca-Urban, C.Mazzocchi, A.G.Smith, J.F.Smith, J.P.Greene, I.Ahmad Low-spin structure of 85Se and the βn branching of 85As RADIOACTIVITY 85As(β-)[from 235U(n, F)]; measured Eγ, Iγ, βγ-, γγ-coin. 85Se; deduced levels, J, π, configuration. 85As(β-n); discussed delayed neutron decay branch. RADIOACTIVITY 248Cm, 252Cf(SF); measured Eγ, Iγ, γγ-coin for prompt γ rays. 85Se; deduced levels, J, π. Eurogam2 and Gammasphere arrays.
doi: 10.1103/PhysRevC.85.027302
2012MA63 J.Instrum. 7, P08029 (2012) L.Mathieu, O.Serot, T.Materna, A.Bail, U.Koster, H.Faust, O.Litaize, E.Dupont, C.Jouanne, A.Letourneau, S.Panebianco New neutron long-counter for delayed neutron investigations with the LOHENGRIN fission fragment separator RADIOACTIVITY 99Y, 136Te(β-n); measured %Pn using LOENIE neutron counter at LOHENGRIN separator facility. Discussed general aspects of beta-delayed neutron emission, and the measurement methods. COMPILATION Z=28-61, A=73-161; compiled and compared delayed neutron emission probabilities %Pn quoted in different compilations and libraries: NNDC chart of nuclides, ENDF/B-VII.0 (2009), JENDL/FPD-2000 (2001), JEFF-3.1.1 (2009), Audi (2003Au02), Pfeiffer (2002Pf04), Table of Isotopes (1996FiZX) and Rudstam (1993Ru01).
doi: 10.1088/1748-0221/7/08/P08029
2011BA33 Phys.Rev. C 84, 034605 (2011) A.Bail, O.Serot, L.Mathieu, O.Litaize, T.Materna, U.Koster, H.Faust, A.Letourneau, S.Panebianco Isotopic yield measurement in the heavy mass region for 239Pu thermal neutron induced fission NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured reaction products, Eγ, Iγ. 93Kr, 93,94,95Rb, 93,94,95,96,98,99Sr, 94,95,96,98,99Y, 99Zr, 99Nb, 133,134Sb, 133,134,136Te, 134,136,137,138,139,140I, 137,138,139,140Xe, 138,139,140,141,142Cs, 141,142,143,144,145,146Ba, 142,143,144,145,146,147,148La, 145,146,147,148Ce, 151,152Pr, 151,152Nd; deduced fission yields, isomeric to g.s. ratios, activation method. Comparison with previous experimental data and with evaluated files JEFF-3.1.1, ENDF/B-VII.0 and JENDL-4.0.
doi: 10.1103/PhysRevC.84.034605
2011FA11 J.Korean Phys.Soc. 59, 879s (2011) H.Faust, U.Koster, T.Materna, W.Urban Population Characteristics for Spin and Excitation Energy of Fragments in Thermal Neutron Induced Fission NUCLEAR REACTIONS 233U(n, f), E=thermal; calculated fission fragment kinetic energies, mean fragment spin of 136I. Simple statistical model.
doi: 10.3938/jkps.59.879
2010SI03 Phys.Rev. C 81, 024313 (2010) G.S.Simpson, W.Urban, J.A.Pinston, J.C.Angelique, I.Deloncle, H.R.Faust, J.Genevey, U.Koster, T.Materna, R.Orlandi, A.Scherillo, A.G.Smith, J.F.Smith, T.Rzaca-Urban, I.Ahmad, J.P.Greene Near-yrast structure of N=93 neutron-rich lanthanide nuclei NUCLEAR REACTIONS 239Pu(n, F), 241Am(n, F), E=thermal; measured Eγ, Iγ, ce, γγ-, (x ray)γ-, (ce)γ-, (fragment)γ-coin, delayed γ, and half-lives. 153Nd, 155Sm; deduced levels, J, π, conversion coefficients, multipolarities, bands, Nilsson configurations. Comparison with quasiparticle-rotor-model (QPRM) calculations. RADIOACTIVITY 248Cm, 252Cf(SF); measured Eγ, Iγ, γγ-coin, and half-lives using Gammasphere and Eurogam-II arrays. 151Ce, 153Nd; deduced levels, J, π, bands, and configurations. Comparison with quasiparticle-rotor-model (QPRM) calculations. 151Ce, 153Nd, 155Sm, 157Gd, 159Dy; systematics of bandheads.
doi: 10.1103/PhysRevC.81.024313
2010SI17 Phys.Rev. C 82, 024302 (2010) G.S.Simpson, W.Urban, K.Sieja, J.A.Dare, J.Jolie, A.Linneman, R.Orlandi, A.Scherillo, A.G.Smith, T.Soldner, I.Tsekhanovich, B.J.Varley, A.Zlomaniec, J.L.Durell, J.F.Smith, T.Rzaca-Urban, H.Faust, I.Ahmad, J.P.Greene Near-yrast, medium-spin, excited states of 91Rb, 93Rb, and 95Rb NUCLEAR REACTIONS 235U(n, F)93Rb/95Rb; measured Eγ, Iγ, γγ-, (fragment)γ-coin, and half-lives using FIFI fragment identification system and Ge detector array. 93,95Rb; deduced levels, J, π, isomers, transition probabilities, and configurations. Comparison with shell-model calculations. RADIOACTIVITY 248Cm, 252Cf(SF); measured Eγ, Iγ, γγ-coin, γγ(θ), and half-lives using EUROGAM-II and Gammasphere arrays. 91,93,95Rb; deduced levels, J, π, isomers, transition probabilities, and configurations. Comparison with shell-model calculations. Systematics of low-lying levels in 89,91,93,95Rb. 93Rb, 95Y; comparison of experimental and calculated spectra.
doi: 10.1103/PhysRevC.82.024302
2009RZ02 Phys.Rev. C 80, 064317 (2009) T.Rzaca-Urban, J.Genevey, T.Materna, W.Urban, A.G.Smith, J.A.Pinston, G.S.Simpson, M.P.Sadowski, U.Koster, H.Faust, A.Bail, L.Mathieu, O.Serot, F.Michel-Sendis, I.Ahmad Near-yrast structure of 142Cs and 144Cs RADIOACTIVITY 248Cm, 252Cf(SF); measured Eγ, Iγ, γγ-coin, γγ(θ), γ(t), and isomer half-lives using EUROGAM2 array. 142,144Cs; deduced levels, J, π, bands, isomers and configurations. Comparison with quasiparticle rotor model (QPRM) calculations. NUCLEAR REACTIONS 235U, 242Am(n, F)137Te/142Cs/144Cs, E=thermal; measured ionic charge distribution of fragments, Eγ, Iγ, ce, γ(ce)-, delayed γ(fragments)-, delayed (ce)(fragments)-coin using LOHENGRIN fragment separator. 142,144Cs; deduced levels and isomer half-lives.
doi: 10.1103/PhysRevC.80.064317
2009UR01 Phys.Rev. C 79, 037304 (2009) W.Urban, A.Zlomaniec, G.S.Simpson, H.Faust, T.Rzaca-Urban, M.Jentschel New information on medium-spin structure of 133Sb NUCLEAR REACTIONS 235U(n, X)133Sb, E=thermal; measured Eγ, Iγ, γγ-coin, γ(t), half-lives. 133Sb; deduced levels, J, π, configurations.
doi: 10.1103/PhysRevC.79.037304
2009UR02 Phys.Rev. C 79, 044304 (2009) W.Urban, K.Sieja, G.S.Simpson, H.Faust, T.Rzaca-Urban, A.Zlomaniec, M.Lukasiewicz, A.G.Smith, J.L.Durell, J.F.Smith, B.J.Varley, F.Nowacki, I.Ahmad New isomers and medium-spin structure of the 95Y nucleus RADIOACTIVITY 248Cm, 252Cf(SF); measured Eγ, Iγ, γγ-coin, γγ(θ), half-lives. 95Y; deduced levels, J, π, isomers, configurations. Comparisons with shell-model calculations. NUCLEAR REACTIONS 238U(n, F), E=thermal; measured Eγ, Iγ, γγ-coin, half-lives. 95Y; deduced levels, J, π, isomers.
doi: 10.1103/PhysRevC.79.044304
2007RZ01 Phys.Rev. C 75, 054319 (2007) T.Rzaca-Urban, K.Pagowska, W.Urban, A.Zlomaniec, J.Genevey, J.A.Pinston, G.S.Simpson, M.S.Sarkar, S.Sarkar, H.Faust, A.Scherillo, I.Tsekhanovich, R.Orlandi, J.L.Durell, A.G.Smith, I.Ahmad First observation of excited states in the 138I nucleus RADIOACTIVITY 138I [from 248Cm(SF)]; measured prompt and delayed Eγ, Iγ. Deduced level energies, J, π.
doi: 10.1103/PhysRevC.75.054319
2006MA01 Nucl.Instrum.Methods Phys.Res. A556, 547 (2006) F.Marie, A.Letourneau, G.Fioni, O.Deruelle, Ch.Veyssiere, H.Faust, P.Mutti, I.Al Mahamid, B.Muhammad Thermal neutron capture cross-section measurements of 243Am and 242Pu using the new mini-INCA α- and γ-spectroscopy station NUCLEAR REACTIONS 243Am, 242Pu(n, γ), E=thermal; measured delayed Eγ, Eα; deduced σ. Comparison with previous results.
doi: 10.1016/j.nima.2005.10.125
2005PI13 Phys.Rev. C 71, 064327 (2005) J.A.Pinston, J.Genevey, R.Orlandi, A.Scherillo, G.S.Simpson, I.Tsekhanovich, W.Urban, H.Faust, N.Warr Shape coexistence in the very neutron-rich odd-odd 96Rb NUCLEAR REACTIONS 241Pu(n, F)96Rb, E=thermal; measured delayed Eγ, Iγ, E(ce), I(ce), γγ-, (ce)γ-coin, X-ray spectra. 96Rb deduced levels, J, π, configurations, deformation, isomer T1/2. Mass separator, comparisons with neighboring nuclides.
doi: 10.1103/PhysRevC.71.064327
2005ZL01 Phys.Rev. C 72, 067302 (2005) A.Zlomaniec, H.Faust, J.Genevey, J.A.Pinston, T.Rzaca-Urban, G.S.Simpson, I.Tsekhanovich, W.Urban Half-life of the 830.2 keV isomer in 97Sr NUCLEAR REACTIONS 239Pu(n, F)97Sr, E=thermal; measured prompt and delayed Eγ, Iγ, γγ-coin. 97Sr deduced isomer T1/2, configuration. Fission fragment separator.
doi: 10.1103/PhysRevC.72.067302
2004FA05 Int.J.Mod.Phys. E13, 321 (2004) Fragment excitation, kinetic energy distributions and neutron evaporation in nuclear fission calculated from a random excitation model RADIOACTIVITY 252Cf(SF); calculated fission fragments excitation energy and kinetic energy distributions, neutron evaporation probabilities. Comparison with data.
doi: 10.1142/S0218301304002120
2004FA10 Nucl.Phys. A736, 55 (2004) Higher moments in the kinetic energy distribution of fission products NUCLEAR REACTIONS 233U(n, F), E=thermal; measured fission fragments kinetic energy and mass distributions; deduced neutron evaporation probabilities. Comparison with random excitation model predictions.
doi: 10.1016/j.nuclphysa.2004.03.001
2004SC42 Phys.Rev. C 70, 054318 (2004) A.Scherillo, J.Genevey, J.A.Pinston, A.Covello, H.Faust, A.Gargano, R.Orlandi, G.S.Simpson, I.Tsekhanovich, N.Warr Neutron-rich In and Cd isotopes close to the doubly magic 132Sn NUCLEAR REACTIONS 239,240,241Pu(n, F), E=thermal; measured delayed Eγ, Iγ, (fission fragment)γ-coin. 123,125,126,127,128,129,130In, 126,128Cd deduced levels, isomeric states T1/2, B(M2), B(E3). Comparison with model predictions.
doi: 10.1103/PhysRevC.70.054318
2003GE04 Phys.Rev. C 67, 054312 (2003) J.Genevey, J.A.Pinston, H.R.Faust, R.Orlandi, A.Scherillo, G.S.Simpson, I.S.Tsekhanovich, A.Covello, A.Gargano, W.Urban High-spin microsecond isomers in 129In and 129Sb NUCLEAR REACTIONS 241Pu(n, F), E=thermal; measured Eγ, Iγ, E(ce), I(ce), (fragment)γ-coin following fission. 129In, 129Sb deduced levels, J, π, ICC, configurations, high-spin isomers T1/2. Fragment separator. Comparison with shell model predictions. RADIOACTIVITY 129In, 129Sb(IT) [from 241Pu(n, F)]; measured Eγ, Iγ, E(ce), I(ce), T1/2. 129In, 129Sb deduced levels, J, π, ICC, configurations. Comparison with shell model predictions.
doi: 10.1103/PhysRevC.67.054312
2002FA09 Eur.Phys.J. A 14, 459 (2002) A model for fragment excitation and kinetic energy in nuclear fission NUCLEAR REACTIONS 229Th, 239Pu, 249Cf(n, F), E=thermal; 237Np(2n, F), E=thermal; calculated fission fragments excitation and kinetic energies, neutron multiplicities. Comparisons with data. RADIOACTIVITY 248Fm, 252Cf(SF); calculated fission fragments excitation and kinetic energies, neutron multiplicities. Comparisons with data.
doi: 10.1140/epja/i2002-10028-6
2002GE07 Phys.Rev. C65, 034322 (2002) J.Genevey, J.A.Pinston, C.Foin, M.Rejmund, H.Faust, B.Weiss High Spin Isomers in 129Sn and 130Sb NUCLEAR REACTIONS 239,241Pu(n, F)129Sn/130Sb, E=thermal; measured delayed Eγ, Iγ, E(ce), I(ce), (fragment)γ-coin. 129Sn, 130Sb deduced levels, J, π, B(E2), isomers T1/2. Mass separator.
doi: 10.1103/PhysRevC.65.034322
2002RE20 Nucl.Phys. A701, 209c (2002) P.Reiter, J.Eberth, H.Faust, S.Franchoo, J.Gerl, C.Gund, D.Habs, M.Huyse, A.Jungclaus, K.P.Lieb, H.Scheit, D.Schwalm, H.G.Thomas, P.van Duppen, D.Weisshaar The MINIBALL Array
doi: 10.1016/S0375-9474(01)01576-7
2002RO37 Nucl.Phys. A710, 3 (2002) D.Rochman, H.Faust, I.Tsekhanovich, F.Gonnenwein, F.Storrer, S.Oberstedt, V.Sokolov Isotopic yields from the reaction 245Cm(nth, f) at the Lohengrin mass separator NUCLEAR REACTIONS 245Cm(n, F), E=thermal; measured fission product isotopic yields, kinetic energy spectra; deduced global odd-even effect, related features. Mass separator.
doi: 10.1016/S0375-9474(02)01026-6
2001FI15 Nucl.Phys. A693, 546 (2001) G.Fioni, M.Cribier, F.Marie, M.Aubert, S.Ayrault, T.Bolognese, J.-M.Cavedon, F.Chartier, O.Deruelle, F.Doneddu, H.Faust, A.Gaudry, F.Gunsing, Ph.Leconte, F.Lelievre, J.Martino, R.Oliver, A.Pluquet, S.Rottger, M.Spiro, C.Veyssiere Incineration of 241Am Induced by Thermal Neutrons NUCLEAR REACTIONS 241,242,242mAm(n, γ), E=thermal; measured capture σ. Application to nuclear waste transmutation discussed.
doi: 10.1016/S0375-9474(01)00920-4
2001GE07 Phys.Rev. C63, 054315 (2001) J.Genevey, J.A.Pinston, C.Foin, M.Rejmund, R.F.Casten, H.Faust, S.Oberstedt Conversion Electron Measurements of Isomeric Transitions in 130, 132Te and 134Xe NUCLEAR REACTIONS 239,241Pu(n, F), E=thermal; measured delayed Eγ, Iγ, E(ce), I(ce), (fragment)γ-, γγ-, (ce)γ-coin. 130,132Te, 134Xe deduced levels, J, π, isomers T1/2, B(E2). Systematics in neighboring nuclides discussed. RADIOACTIVITY 130,132Te, 134Xe(IT) [from239,241Pu(n, F), E=thermal]; measured Eγ, Iγ, E(ce), I(ce), γγ-, (ce)γ-coin, T1/2. 130,132Te, 134Xe deduced levels, J, π, B(E2). Systematics in neighboring nuclides discussed.
doi: 10.1103/PhysRevC.63.054315
2001TS05 Nucl.Phys. A688, 633 (2001) I.Tsekhanovich, H.-O.Denschlag, M.Davi, Z.Buyukmumcu, F.Gonnenwein, S.Oberstedt, H.R.Faust Mass and Charge Distributions in the Very Asymmetric Mass Region of the Neutron Induced Fission of 238Np NUCLEAR REACTIONS 237Np(2n, F), E=thermal; measured fission fragment yields, charge distributions; deduced odd-even effect. Mass separation.
doi: 10.1016/S0375-9474(00)00586-8
2000GE08 Eur.Phys.J. A 7, 463 (2000) J.Genevey, J.A.Pinston, H.Faust, C.Foin, S.Oberstedt, B.Weiss On the Nature of the 17 μs Isomer of the 133Sb Valence Nucleus RADIOACTIVITY 133Sb(IT) [from 241Pu(n, F)]; measured Eγ, Iγ(t), E(ce), I(ce), (ce)γ-coin, T1/2. 133Sb deduced levels, J, π, B(E2), ICC, configurations.
doi: 10.1007/s100500050418
2000GE18 Eur.Phys.J. A 9, 191 (2000) J.Genevey, J.A.Pinston, H.Faust, C.Foin, S.Oberstedt, M.Rejmund New High-Spin Microsecond Isomers in 131Sb NUCLEAR REACTIONS 241Pu(n, F), E=thermal; measured Eγ, Iγ(t), (fragment)γ-, (fragment)(X-ray)-coin following fission. 131Sb deduced levels, J, π, configurations, high-spin isomers T1/2, B(E2). Mass separator.
doi: 10.1007/s100500070036
2000PI03 Phys.Rev. C61, 024312 (2000) J.A.Pinston, C.Foin, J.Genevey, R.Beraud, E.Chabanat, H.Faust, S.Oberstedt, B.Weiss Microsecond Isomers in 125, 127, 129Sn NUCLEAR REACTIONS 233U, 239Pu(n, F), E=thermal; measured Eγ, Iγ(t), E(ce), I(ce), γγ-, (ce)γ-, (fission fragment)γ-coin. 123,125,127,129Sn deduced levels, J, π, isomers T1/2, B(E2). 127,129In deduced possible high-spin β isomers.
doi: 10.1103/PhysRevC.61.024312
1999BO08 Acta Phys.Slovaca 49, 1 (1999) T.Bolognese, G.Fioni, M.Cribier, F.Marie, M.Aubert, S.Ayrault, J.-M.Cavedon, F.Chartier, F.Doneddu, H.Faust, A.Gaudry, F.Gunsing, Ph.Leconte, F.Lelievre, J.Martino, R.Oliver, A.Pluquet, M.Spiro, C.Veyssiere Preliminary Results on 241Am Transmutation in a High Thermal Flux NUCLEAR REACTIONS 242Am(n, γ), E=thermal; measured capture σ. Mass spectrometry techniques. Implications for waste transmutation discussed. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22696. 1999GE01 Phys.Rev. C59, 82 (1999) J.Genevey, F.Ibrahim, J.A.Pinston, H.Faust, T.Friedrichs, M.Gross, S.Oberstedt Identification of μs Isomers in the Fission Products of 241Pu(nth, f) RADIOACTIVITY 88mBr, 96mRb, 97mSr, 94m,98m,99mY, 99mZr, 100m,106mNb, 104mTc, 107mMo, 109mRu, 109mRh(IT) [from 241Pu(n, F), E=thermal]; measured Eγ, Iγ(t), E(ce), I(ce), γγ-, (ce)γ-coin, T1/2. 88Br, 94Y, 96Rb, 97Sr, 100,106Nb deduced levels, J, π. NUCLEAR REACTIONS 241Pu(n, F), E=thermal; measured Eγ, Iγ(t), E(ce), I(ce), γγ-, (ce)γ-coin; deduced isomer yields.
doi: 10.1103/PhysRevC.59.82
1999KO26 Nucl.Phys. A652, 371 (1999) U.Koster, H.Faust, G.Fioni, T.Friedrichs, M.Gross, S.Oberstedt Ternary Fission Yields of 241Pu(nth, f) NUCLEAR REACTIONS 241Pu(n, F), E=thermal; measured fission fragments isotopic yields; deduced evidence for 11Li, 14Be, 19C. Recoil separator.
doi: 10.1016/S0375-9474(99)00115-3
1999TS07 Nucl.Phys. A658, 217 (1999) I.Tsekhanovich, H.O.Denschlag, M.Davi, Z.Buyukmumcu, M.Wostheinrich, F.Gonnenwein, S.Oberstedt, H.R.Faust Mass and Charge Distributions in the Very Asymmetric Thermal Neutron Induced Fission of the Odd-Z Nucleus 242mAm NUCLEAR REACTIONS 242mAm(n, F), E=thermal; measured fission fragment isotopic yields, mass and charge distributions; deduced odd-even effects.
doi: 10.1016/S0375-9474(99)00338-3
1999WO03 Acta Phys.Slovaca 49, 117 (1999) M.Wostheinrich, R.Pfister, F.Gonnenwein, H.O.Denschlag, H.Faust, S.Oberstedt Yields of Ternary Particles from the Reactions 229Th(nth, f), 233U(nth, f) and 239Pu(nth, f) NUCLEAR REACTIONS 229Th, 233U, 239Pu(n, F), E=thermal; measured ternary fission fragments yields, energy distributions. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22734. 1997GO36 Nuovo Cim. 110A, 1089 (1997) F.Gonnenwein, A.Moller, M.Croni, M.Hesse, M.Wostheinrich, H.Faust, G.Fioni, S.Oberstedt Cold Binary and Ternary Fission RADIOACTIVITY 252Cf(SF); measured fragments yields, kinetic energy distributions; deduced 132Sn-associated cluster mode. NUCLEAR REACTIONS 242Am(n, F), E=thermal; measured ternary fission yields; deduced fission process features. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23807. 1997HA12 Nucl.Phys. A616, 39c (1997) D.Habs, O.Kester, P.Thirolf, K.E.G.Lobner, H.J.Maier, D.Rudolph, K.Rudolph, U.Schramm, T.Faestermann, G.Hinderer, P.Kienle, U.Koster, H.-J.Korner, E.Steichele, A.Ulrich, T.von Egidy, H.Faust, M.Gross The Munich Fission Fragment Accelerator
doi: 10.1016/S0375-9474(97)00072-9
1994BE24 Phys.Lett. 331B, 19 (1994) M.Bernas, S.Czajkowski, P.Armbruster, H.Geissel, Ph.Dessagne, C.Donzaud, H.-R.Faust, E.Hanelt, A.Heinz, M.Hesse, C.Kozhuharov, Ch.Miehe, G.Munzenberg, M.Pfutzner, C.Rohl, K.-H.Schmidt, W.Schwab, C.Stephan, K.Summerer, L.Tassan-Got, B.Voss Projectile Fission at Relativistic Velocities: A novel and powerful source of neutron-rich isotopes well suited for in-flight isotopic separation NUCLEAR REACTIONS Pb(238U, F)86Ge/88As/89As/90Se/96Kr/103Y/104Y/105Y/106Zr/107Zr/108Nb/109Nb/110Nb/111Mo/112Mo/113Mo/114Tc/115Tc/116Ru/118Ru/118Rh/119Rh/120Rh/121Rh/121Pd/122Pd/123Pd/125Ag/126Ag/135Sn/136Sn/137Sn/137Sb/138Sb/139Sb/139Te/140Te/141Te/142Te/143I/144I/147Xe/151Ba/151La/152La/153La/153Ce/154Ce/155Ce, E at 750 MeV/nucleon; measured reaction products; deduced projectile fission fragment yields, production σ. Fragment separator, energy-loss, tof techniques.
doi: 10.1016/0370-2693(94)90937-7
1994HE10 Nucl.Phys. A571, 427 (1994) R.Hentzschel, H.R.Faust, H.O.Denschlag, B.D.Wilkins, J.Gindler Mass, Charge and Energy Distributions in the Very Asymmetric Fission of 249Cf Induced by Thermal Neutrons NUCLEAR REACTIONS 249Cf(n, F), E=thermal; measured fission product yields (A=69-87) at various kinetic energies of the fission fragments; deduced nuclear charge, kinetic energy distributions, odd-even factors.
doi: 10.1016/0375-9474(94)90220-8
1994SC30 Nucl.Phys. A577, 674 (1994) W.Schwab, H.-G.Clerc, M.Mutterer, J.P.Theobald, H.Faust Cold Fission of 233U(n(th), f) NUCLEAR REACTIONS 233U(n, F), E=thermal; measured light fission fragment nuclide yields at high kinetic energies; deduced yields at constant total excitation energy, ground-state yields, influence of level densities and scission barrier pentrabilities.
doi: 10.1016/0375-9474(94)90939-3
1993DE47 Radiochim.Acta 62, 177 (1993) H.O.Denschlag, O.Alhassanieh, M.Weis, W.Faubel, H.R.Faust On the Absolute γ-Ray Line Intensities in the Decay of 99Nb and the Branching Ratio in the Decay of 99Zr to 99mNb and 99gNb RADIOACTIVITY 99Zr(β-) [from 235U(n, F), E=thermal]; measured Eγ, Iγ. 99Nb levels deduced branching ratio, transitions absolute Iγ. NUCLEAR REACTIONS 235U(n, F), E=thermal; measured Eγ, Iγ; deduced fractional independent fission yields. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23596. 1992GR06 Nucl.Instrum.Methods Phys.Res. A311, 512 (1992) M.Gross, P.Jurgens, U.Keyser, S.Kluge, M.Mehrtens, S.Muller, F.Munnich, J.Wulff, H.R.Faust Determination of High Q(β)-Values by Beta-Gamma-Coincidence Measurements with a Plastic Scintillator Telescope RADIOACTIVITY 92Kr(β-); 139I(β-); 139Xe(β-) [from 139I-decay]; measured β-spectra endpoint energies, βγ-coin; deduced Qβ. Plastic scintillator telescope.
doi: 10.1016/0168-9002(92)90649-O
1991BE33 Phys.Rev.Lett. 67, 3661 (1991) M.Bernas, P.Armbruster, S.Czajkowski, H.Faust, J.P.Bocquet, R.Brissot Discovery of Neutron-Rich Co and Fe Isotopes in 239Pu(n(th), f): Yields and half-lives NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured fission fragment mass, isotopic yields, (fragment)β(t). 69,68Co, 68Fe deduced T1/2.
doi: 10.1103/PhysRevLett.67.3661
1991BO35 Nucl.Phys. A534, 255 (1991) H.G.Borner, R.F.Casten, I.Forster, D.Lieberz, P.von Brentano, S.J.Robinson, T.von Egidy, G.Hlawatsch, H.Lindner, P.Geltenbort, F.Hoyler, H.Faust, G.Colvin, W.R.Kane, M.MacPhail Level Structure of 191Os: Coexisting oblate and prolate configurations NUCLEAR REACTIONS 190Os(n, γ), (n, e), E=thermal, resonance; measured Eγ, Iγ, γγ-coin, I(ce). 190Os(d, t), E=20 MeV; measured σ(Et). 191Os deduced levels, J, π, ICC, γ multipolarity.
doi: 10.1016/0375-9474(91)90498-U
1990BE13 Z.Phys. A336, 41 (1990) M.Bernas, P.Armbruster, J.P.Bocquet, R.Brissot, H.Faust, Ch.Kozhuharov, J.L.Sida Beta-Decay Half-Lives of Neutron Rich Cu and Ni Isotopes Produced by Thermal Fission of 235U and 239Pu NUCLEAR REACTIONS 235U, 239Pu(n, F), E=thermal; measured fission fragment elemental distributions; deduced evidence for 74,75Cu, 71,72,73Ni. Magnetic, electrostatic analysis. RADIOACTIVITY 74,75Cu, 71,72,73Ni [from 235U, 239Pu(n, F), E=thermal]; measured β-decay T1/2. Model comparison. Planar Si detectors.
1990BO05 Z.Phys. A335, 41 (1990) J.P.Bocquet, R.Brissot, H.R.Faust, M.Fowler, J.Wilhelmy, M.Asghar, M.Djebara Characteristics of Mass and Nuclear Charge Distributions of 229Th(n(th), F). Implications for Fission Dynamics NUCLEAR REACTIONS 229Th(n, F), E=thermal; measured fission fragment yield vs mass, charge; deduced proton odd-even effect role in fission. Other data analyzed. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22143. 1990GR10 Z.Phys. A336, 247 (1990) M.Graefenstedt, P.Jurgens, U.Keyser, F.Munnich, F.Schreiber, K.Balog, T.Winkelmann, H.R.Faust, B.Pfeiffer Beta Decay Energies and Nuclear Masses of 148Ba, 148La and 151Pr RADIOACTIVITY 148Ba, 148La, 151Pr(β-); measured Eβ, Iβ, Eγ, Iγ, βγ-coin; deduced Qβ, Ba, La, Ce, Pr isotope mass differences.
1990MA49 Nucl.Phys. A515, 433 (1990) G.Martinez, G.Barreau, A.Sicre, T.P.Doan, P.Audouard, B.Leroux, W.Arafa, R.Brissot, J.P.Bocquet, H.Faust, P.Koczon, M.Mutterer, F.Gonnenwein, M.Asghar, U.Quade, K.Rudolph, D.Engelhardt, E.Piasecki Mass and Nuclear Charge Yields for 237Np(2n(th), f) at Different Fission Fragment Kinetic Energies NUCLEAR REACTIONS 239Np(n, F), E=thermal; measured light fission product mass versus kinetic energies; deduced fractional independent fission yields, odd-even effects of elements, isotones. Double neutron capture on 237Np target.
doi: 10.1016/0375-9474(90)90593-B
1989GR23 Z.Phys. A334, 239 (1989) M.Graefenstedt, P.Jurgens, U.Keyser, F.Munnich, F.Schreiber, K.Balog, T.Winkelmann, H.R.Faust Experimental Beta-Decay Energies of Very Neutron-Rich Fission Products with 107 ≤ A ≤ 109 RADIOACTIVITY 107Mo, 108,109,107Tc, 107,108,109Ru, 108Rh(β-n); measured βγ-coin, β-endpoint energies; deduced Qβ, mass excess, two-neutron separation energies.
1989SI22 Nucl.Phys. A502, 233c (1989) J.L.Sida, P.Armbruster, M.Bernas, J.P.Bocquet, R.Brissot, H.R.Faust Mass, Charge, and Energy Distributions in Very Asymmetric Thermal Fission of 235U NUCLEAR REACTIONS 235U(n, F), E=thermal; measured fission fragment mass, charge, energy distributions; deduced fission features.
doi: 10.1016/0375-9474(89)90664-7
1987AR21 Europhys.Lett. 4, 793 (1987) P.Armbruster, M.Bernas, J.P.Bocquet, R.Brissot, H.R.Faust, P.Roussel Identification of the New Neutron-Rich Isotopes 70-74Ni and 74-77Cu in Thermal Neutron Fission of 235U NUCLEAR REACTIONS 235U(n, F)70Ni/71Ni/72Ni/73Ni/74Ni/74Cu/75Cu/76Cu/77Cu, E=thermal; measured fission fragment yields. Recoil separator, ΔE-E detection.
doi: 10.1209/0295-5075/4/7/006
1987GR18 Z.Phys. A327, 383 (1987) M.Graefenstedt, U.Keyser, F.Munnich, F.Schreiber, H.R.Faust, H.Weikard Nuclear Structure Effects in the Mass Region Around A = 100, Derived from Experimental Q(β)-Values RADIOACTIVITY 101,102,103Zr, 101,102,103,104,105Nb, 103,104,105,106Mo, 104,105,106Tc(β-); measured β-endpoint energies, Q(β). 101,102,103Zr, 101,102,103,104,105Nb, 103,104,105,106Mo, 104,105,106Tc deduced two-neutron, two-proton separation energies, mass excesses. Mass separator, plastic scintillator telescope, Ge(Li) detector.
1987GR39 Verh.Deut.Phys.Ges. 22, IV, PG-81 (1987) M.Graefenstedt, U.Keyser, F.Munnich, F.Schreiber, H.R.Faust, U.Stohlker Measurement of the Qβ-values of 87-90Br and 87Se
1986KE10 Radiat.Eff. 94, 39 (1986) U.Keyser, F.Munnich, B.Pahlmann, M.Graefenstedt, H.Faust, H.Weikard Experimental Beta-Decay Energies of very Neutron-Rich Light Fission Products RADIOACTIVITY 90Br, 101,102,103Zr, 101,102,103,104,105Nb, 103,104,105,106Mo, 104,105,106Tc(β-); measured βγ-coin; deduced Qβ.
doi: 10.1080/00337578608208350
1986WE11 Nucl.Instrum.Methods Phys.Res. A248, 506 (1986) E.Weissenberger, P.Geltenbort, A.Oed, F.Gonnenwein, H.Faust Energy Calibration of Surface Barrier Detectors for Fission Fragments RADIOACTIVITY 252Cf(SF); measured fission fragment total kinetic energies. Surface barrier detectors. NUCLEAR REACTIONS 233,235U, 239Pu(n, F), E=thermal; measured fission fragment total kinetic energies. Surface barrier detectors.
doi: 10.1016/0168-9002(86)91041-7
1985TO10 Nucl.Phys. A439, 427 (1985) Y.Tokunaga, H.Seyfarth, R.A.Meyer, O.W.B.Schult, H.G.Borner, G.Barreau, H.R.Faust, K.Schreckenbach, S.Brant, V.Paar, M.Vouk, D.Vretenar Low-Lying Levels of 77Se Studied by Thermal Neutron Capture and Evidence for a New Term in the E2 Operator of TQM(IBM) NUCLEAR REACTIONS 76Se(n, γ), E=thermal; measured Iγ, Eγ, I(ce); deduced Q, neutron separation energy. 77Se deduced levels J, π, population probability. Enriched target, crystal-, β-, pair-spectrometers. Statistical, particle-vibration model analyses.
doi: 10.1016/0375-9474(85)90420-8
1984MH01 Nucl.Phys. A412, 113 (1984) A.Mheemeed, K.Schreckenbach, G.Barreau, H.R.Faust, H.G.Borner, R.Brissot, P.Hungerford, H.H.Schmidt, H.J.Scheerer, T.Von Egidy, K.Heyde, J.L.Wood, P.Van Isacker, M.Waroquier, G.Wenes, M.L.Stelts The Level Structure of 114Cd from (n, γ) and (d, p) Studies NUCLEAR REACTIONS 113Cd(n, γ), E=thermal, 2 keV, 24 keV; 113Cd(n, e-), E=thermal; 113Cd(d, p), E=10 MeV; measured Eγ, Iγ, I(ce), E(p), σ(E(p)). 114Cd deduced levels, J, π, ICC, γ-branching, E0 branches. Curved crystal spectrometers, Ge(Li) pair spectrometers, magnetic conversion electron spectrometer, magnetic spectrograph, enriched targets. Comparison with proton 2p-2h coupling, interacting boson model configuration mixing calculations.
doi: 10.1016/0375-9474(84)90388-9
1984SC38 Nucl.Phys. A430, 21 (1984) C.Schmitt, A.Guessous, J.P.Bocquet, H.-G.Clerc, R.Brissot, D.Engelhardt, H.R.Faust, F.Gonnenwein, M.Mutterer, H.Nifenecker, J.Pannicke, Ch.Ristori, J.P.Theobald Fission Yields at Different Fission-Product Kinetic Energies for Thermal-Neutron-Induced Fission of 239Pu NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured fission fragment mass, charge distribution; deduced fragment fractional yields, odd-even effects, isobar average kinetic energies.
doi: 10.1016/0375-9474(84)90191-X
1984TO11 Nucl.Phys. A430, 269 (1984) Y.Tokunaga, H.Seyfarth, O.W.B.Schult, S.Brant, V.Paar, D.Vretenar, H.G.Borner, G.Barreau, H.Faust, Ch.Hofmeyr, K.Schreckenbach, R.A.Meyer A Study of 75Se by Neutron Capture and the SU(3)-SU(5) Transition in the Quadrupole-Phonon Representation NUCLEAR REACTIONS 74Se(n, γ), E=thermal; measured Iγ, Eγ, I(ce); deduced Q. 75Se, 75As deduced levels, J, π. Enriched target, crystal, pair β-spectrometers.
doi: 10.1016/0375-9474(84)90041-1
1983BL14 J.Phys.(London) B16, 4565 (1983) S.J.Blakeway, W.Gelletly, H.R.Faust, K.Schreckenbach, J.Byrne Measurements of the Transverse Polarization of K-Shell Photoelectron Produced by Unpolarised 334 and 439 keV Photons in Thorium ATOMIC PHYSICS Th(γ, e), E=339, 439 keV; measured transverse photoelectron polarization; deduced nonzero correlation coefficient.
doi: 10.1088/0022-3700/16/24/013
1983FA11 Nucl.Instrum.Methods 213, 277 (1983) H.R.Faust, H.Klewe-Nebenius, H.Rebel, K.Wisshak Determination of the Multipolarity of Prompt Electromagnetic Transitions from Angular Distributions of Conversion Electrons Part II: Spectrometer and Measurements NUCLEAR REACTIONS 169Tm, 192Os(d, 5n), E=52 MeV; measured I(ce), ce(θ). 166Yb, 189Ir deduced rotational band transition angular distribution coefficients. Mini-orange spectrometer, magnetic filter system.
doi: 10.1016/0167-5087(83)90420-9
1983FA15 Z.Phys. A313, 351 (1983) On the Octupole Excitation in 236U NUCLEAR REACTIONS 236U(n, e-), E=thermal; measured I(ce). 236U deduced subshell ICC. Electron penetration formalism.
doi: 10.1007/BF01439489
1982KA28 Phys.Lett. 117B, 15 (1982) W.R.Kane, R.F.Casten, D.D.Warner, K.Schreckenbach, H.R.Faust, S.Blakeway Strengths of E0 Transitions in 188Os and 196Pt and the Structure of IBA Wavefunctions in the Os-Pt Transition Region NUCLEAR REACTIONS 187Os, 195Pt(n, γ), E=thermal; measured I(ce), Eγ, Iγ. 188Os, 196Pt deduced levels, B(E0)/B(E2), E0 transition strength. Interacting boson model, O(6) limit.
doi: 10.1016/0370-2693(82)90864-4
1982SC09 Phys.Lett. 110B, 364 (1982) K.Schreckenbach, A.Mheemeed, G.Barreau, T.von Egidy, H.R.Faust, H.G.Borner, R.Brissot, M.L.Stelts, K.Heyde, P.van Isacker, M.Waroquier, G.Wenes The Importance of Intruder States in 114Cd NUCLEAR REACTIONS 113Cd(n, γ), (n, e-), E=thermal; 113Cd(n, γ), E=2, 24 keV; measured Eγ, Iγ, I(ce). 114Cd deduced levels, γ-branching ratio, J, π, T1/2, B(E0), B(E2). Two-particle, two-hole core coupling calculations.
doi: 10.1016/0370-2693(82)91273-4
1981SU12 Fizika(Zagreb) 13, Suppl.No.2, 39 (1981) P.A.Sushkov, I.A.Kondurov, M.Bogdanovic, T.Mitsunari, T.D.Mac Mahon, H.A.Baader, D.Breitig, R.Koch, H.Seyfarth, O.W.B.Schult, H.Borner, R.Brissot, G.Barreau, H.Faust, K.Schreckenbach The Level Scheme of 110Ag from the (n, γ) Reaction NUCLEAR REACTIONS 109Ag(n, γ), E not given; measured Eγ, Iγ, I(ce), γγ-coin. 110Ag deduced levels, configuration.
1978FA03 J.Phys.(London) G4, 247 (1978) H.Faust, A.Hanser, H.Klewe-Nebenius, H.Rebel, J.Buschmann, H.J.Gils Experimental Studies of Hexadecapole Motion in Spherical Nuclei RADIOACTIVITY 60Co, 140La; measured γ-spectrum. 60Ni, 140Ce deduced E4 transitions. NUCLEAR REACTIONS 60Ni, 140Ce(α, α'γ), E=104 MeV; measured γ-spectrum, σ(Eα'). 60Ni, 140Ce levels deduced L, B(E4), β.
doi: 10.1088/0305-4616/4/2/014
1977KR01 Z.Phys. A280, 61 (1977) J.Kropp, H.Klewe-Nebenius, H.Faust, J.Buschmann, H.Rebel, H.J.Gils, K.Wisshak Excitation Functions of 191+193Ir, 197Au(6Li, xn+yp) Compound Nuclear Reactions at E = 48-156 MeV NUCLEAR REACTIONS 191,193Ir, 197Au(6Li, xnyp), X=3-13, y=0-2, E=48-156 MeV; measured σ(E).
doi: 10.1007/BF01438110
1976WI09 Z.Phys. A277, 129 (1976) K.Wisshak, A.Hanser, H.Klewe-Nebenius, J.Buschmann, H.Rebel, H.Faust Experimental Studies of the Level Scheme of 143Eu and a Generalized Decoupling Model Description RADIOACTIVITY 143mGd; measured Eγ, Iγ, γγ-coin, T1/2; deduced log ft, ICC. 143Eu deduced levels, J, π, λ. NUCLEAR REACTIONS 144Sm(α, 4npγ), E=75-120 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), γ(t). 143Eu deduced levels, J, π, T1/2, γ-branching.
doi: 10.1007/BF01433704
1975KL02 Nucl.Phys. A240, 137 (1975) H.Klewe-Nebenius, D.Habs, K.Wisshak, H.Faust, G.Nowicki, S.Goring, H.Rebel, G.Schatz, M.Schwall The Level Scheme of 137Pr; Evidence for Prolate Nuclear Shape RADIOACTIVITY 137Nd[from 141Pr(α, 7np)]; measured Eγ, Iγ, γγ-coin, E(ce), I(ce); deduced ICC. 137Pr deduced levels, J, π. Mass separated sources. NUCLEAR REACTIONS 139La(α, 6nγ), E=70-104 MeV; measured σ(E, Eγ, θ), E(ce), I(ce), γ(t); deduced ICC. 137Pr deduced levels, J, π, T1/2. Natural target. Ge(Li), Si(Li) detectors with magnetic filter.
doi: 10.1016/0375-9474(75)90442-X
1975NO08 Nucl.Phys. A249, 76 (1975) G.P.Nowicki, J.Buschmann, A.Hanser, H.Rebel, H.Faust, D.Habs, H.Klewe-Nebenius, K.Wisshak The Level Scheme of 137Nd from (α, xn) Reactions and from β-Decay of The 11/2- Isomer of 137Pm RADIOACTIVITY 137Pm [from 141Pr(α, 8n)]; measured Eγ, Iγ, γγ-coin, E(ce), I(ce); deduced ICC. 137Nd deduced levels, J, π. Natural target, mass-separated sources, Ge(Li) detectors, Si(Li) detector with magnetic filter. NUCLEAR REACTIONS 140Ce(α, 7n), E=80-104 MeV; measured σ(E, Eγ, θ), γγcoin, E(ce), I(ce)(θ). 137Nd deduced levels, J, π. Natural target, Ge(Li) detectors, Si(Li) detector with magnetic filter.
doi: 10.1016/0375-9474(75)90092-5
1975WI11 Nucl.Phys. A247, 59 (1975) K.Wisshak, H.Klewe-Nebenius, D.Habs, H.Faust, G.Nowicki, H.Rebel The Level Scheme of 135Pr: Prolate Deformation of the 11/2- Isomer RADIOACTIVITY 135Nd [from 138Ce(α, 7n), 136Ce(α, 5n)]; measured Eγ, Iγ, γγ-coin, I(ce), E(ce); deduced ICC, K/L. 135Pr deduced levels, J, π. Enriched targets, mass separated sources, Ge(Li) detectors, Si(Li) detector with magnetic filter for background suppression. NUCLEAR REACTIONS 139La(α, 8n), E=80-104 MeV; measured σ(E, Eγ, θ), γγ-coin. 135Pr deduced levels, J, π. Natural target, Ge(Li) detectors.
doi: 10.1016/0375-9474(75)90277-8
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