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NSR database version of May 30, 2024.

Search: Author = H.Faust

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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23784.


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2004FA05      Int.J.Mod.Phys. E13, 321 (2004)

H.R.Faust

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
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2004FA10      Nucl.Phys. A736, 55 (2004)

H.R.Faust, Z.Bao

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
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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
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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
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2002FA09      Eur.Phys.J. A 14, 459 (2002)

H.R.Faust

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
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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
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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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23098.


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
Citations: PlumX Metrics

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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
Citations: PlumX Metrics


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22296.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22257.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22233.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22179.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22151.


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
Citations: PlumX Metrics

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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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21928.


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
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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
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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
Citations: PlumX Metrics


1983FA15      Z.Phys. A313, 351 (1983)

H.R.Faust

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
Citations: PlumX Metrics


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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0120.


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
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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
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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
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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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Note: The following list of authors and aliases matches the search parameter H.Faust: , H.R.FAUST