NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of April 11, 2024.

Search: Author = H.R.Faust

Found 27 matches.

Back to query form



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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22849.


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23179.


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

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23580.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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


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
Citations: PlumX Metrics


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
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

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23586.


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
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
Citations: PlumX Metrics


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.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


Back to query form