NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.R.Faust Found 27 matches. 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
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
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
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
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
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
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
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
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.
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
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
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
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