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NSR database version of April 11, 2024.

Search: Author = F.S.Dietrich

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2015NO01      Phys.Rev. C 91, 024618 (2015)

G.P.A.Nobre, A.Palumbo, M.Herman, D.Brown, S.Hoblit, F.S.Dietrich

Derivation of an optical potential for statically deformed rare-earth nuclei from a global spherical potential

NUCLEAR REACTIONS 165Ho, 182,184,186W(n, X), E=0.003-200 MeV; calculated total σ(E). 158,160Gd(n, n), (n, n'), E=2.5, 4.1 MeV; Gd(n, n), E=0.334-0.919 MeV; Gd(n, n'), E=4.51-8.41 MeV; 165Ho(n, n), E=0.350, 0.60, 0.79, 0.93 MeV; 165Ho(n, n'), E=1.20, 4.51, 9.99, 11 MeV; 182,184W(n, n), (n, n')E=1.5-6.0 MeV; calculated σ(θ, E). Coupled-channel calculations with optical potential for statically deformed rare-earth nuclei using rotational excited states of the g.s. band. Comparison with experimental data.

doi: 10.1103/PhysRevC.91.024618
Citations: PlumX Metrics


2014NO06      Nucl.Data Sheets 118, 266 (2014)

G.P.A.Nobre, A.Palumbo, D.Brown, M.Herman, S.Hoblit, F.S.Dietrich

Towards a Coupled-channel Optical Potential for Rare-earth Nuclei

NUCLEAR REACTIONS 152Sm, 156Gd, 162,166Dy, 180Hf(n, x), E=0.002-20 MeV;184W(n, x), E=0.05-20 MeV; calculated total σ. 184W(n, γ), E=0.003-40 MeV; calculated σ. 184W(n, n), E=1.5-6.0 MeV;184W(n, n'), E=1.5-3.5 MeV;calculated σ(θ) using optical model, coupled channels with quadrupole- and hexadecupole deformed potential and other corrections. Compared to EXFOR data.

doi: 10.1016/j.nds.2014.04.054
Citations: PlumX Metrics


2012DI07      Phys.Rev. C 85, 044611 (2012)

F.S.Dietrich, I.J.Thompson, T.Kawano

Target-state dependence of cross sections for reactions on statically deformed nuclei

NUCLEAR REACTIONS 233,235,238U, 239Pu, 165Ho, 169Tm, 170Yb, 20Ne(n, X), E<20 MeV; calculated compound nucleus formation cross section for ground and excited states of different K quantum numbers, cross section ratios for adiabatic to nonadiabatic approximations. Coupled-channels calculations. Application to transmission coefficients in Hauser-Feshbach calculations.

doi: 10.1103/PhysRevC.85.044611
Citations: PlumX Metrics


2012ES03      Rev.Mod.Phys. 84, 353 (2012)

J.E.Escher, J.T.Burke, F.S.Dietrich, N.D.Scielzo, I.J.Thompson, W.Younes

Compound-nuclear reaction cross sections from surrogate measurements

doi: 10.1103/RevModPhys.84.353
Citations: PlumX Metrics


2012GO06      Phys.Rev. C 85, 054616 (2012)

B.L.Goldblum, M.Wiedeking, T.Reed, K.Alfonso, J.M.Allmond, L.A.Bernstein, D.L.Bleuel, F.S.Dietrich, R.Hatarik, P.T.Lake, I.-Y.Lee, S.R.Lesher, S.Paschalis, M.Petri, L.Phair, N.D.Scielzo, R.Vial, J.Vujic

Indirect determination of neutron capture cross sections on spherical and near-spherical nuclei using the surrogate method

NUCLEAR REACTIONS 92,94Mo(d, p), E=11 MeV; measured particle spectrum, Eγ, Iγ, (particle)γ-coin using STARS-LIBERACE array. DWBA analysis. 92Mo(n, γ), E=80-890 keV; deduced capture cross section using the absolute surrogate and surrogate ratio methods (SRM) relative to 94Mo(n, γ) cross section. Gamma decay tagging techniques. Dicebox statistical model analysis for gamma cascades. Comparison with ENDF/B-VII.0 evaluation.

doi: 10.1103/PhysRevC.85.054616
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14338.


2012SC10      Phys.Rev. C 85, 054619 (2012)

N.D.Scielzo, J.E.Escher, J.M.Allmond, M.S.Basunia, C.W.Beausang, L.A.Bernstein, D.L.Bleuel, J.T.Burke, R.M.Clark, F.S.Dietrich, P.Fallon, J.Gibelin, B.L.Goldblum, S.R.Lesher, M.A.McMahan, E.B.Norman, L.Phair, E.Rodriguez-Vieitez, S.A.Sheets, I.J.Thompson, M.Wiedeking

Statistical γ rays in the analysis of surrogate nuclear reactions

NUCLEAR REACTIONS 154,155,156,158Gd(p, p'), E=21.7 MeV; measured Ep, Ip, Eγ, Iγ, pγ-coin using STARS-LiBerACE at LBNL cyclotron facility; deduced γ-ray emission probability. 155,157Gd(n, γ), E<3.5 MeV; deduced cross section ratios by surrogate analyses using statistical and discrete γ-rays. Comparison with reaction theory. Surrogate nuclear reaction technique.

doi: 10.1103/PhysRevC.85.054619
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14339.


2011ES04      J.Korean Phys.Soc. 59, 815s (2011)

J.E.Escher, F.S.Dietrich, N.D.Scielzo

Surrogate Approaches for Neutron Capture

NUCLEAR STRUCTURE 92Zr, 156Gd, 236U; calculated γ decay probabilities for excited nuclei.

NUCLEAR REACTIONS 91Zr, 155Gd, 235U(n, γ), E=0.02-5 MeV; analyzed σ from simulated surrogate experiments using different spin-parity distributions.

doi: 10.3938/jkps.59.815
Citations: PlumX Metrics


2011NO17      Phys.Rev. C 84, 064609 (2011)

G.P.A.Nobre, F.S.Dietrich, J.E.Escher, I.J.Thompson, M.Dupuis, J.Terasaki, J.Engel

Toward a microscopic reaction description based on energy-density-functional structure models

NUCLEAR REACTIONS 90Zr(n, X), E=10, 20, 30 MeV; 58Ni(n, X), E=20, 30 MeV; 58Ni(p, X), E=10-70 MeV; 48Ca(p, X), E=10-50 MeV; 40,48Ca, 58Ni, 144Sm(n, X), (p, X), E=30 MeV; 90Zr(p, X), E=20-70 MeV; calculated reaction cross section. 90Zr(p, p), E=40, 65 MeV; calculated σ(θ). Random-phase, Hartree-Fock-Bogoliubov (HFB) framework and Skyrme density functional with coupling to all RPA and QRPA inelastic channels including deuteron formation. Assessed effects of couplings between inelastic resonances from higher-order channels. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.064609
Citations: PlumX Metrics


2011NO18      J.Phys.:Conf.Ser. 312, 082033 (2011)

G.P.A.Nobre, I.J.Thompson, J.E.Escher, F.S.Dietrich

Reaction cross-section predictions for nucleon induced reactions

NUCLEAR REACTIONS 58Ni(n, X), E=20, 30 MeV;90Zr(n, X), E=10, 20, 40 MeV;144Sm(n, X), E=30 MeV;40,48Ca, 58Ni(p, X), E=10, 20, 30, 40 MeV;90Zr(p, X), E=10, 20, 30, 40, 50, 60, 70 MeV;144Sm(p, X), E=30 MeV; calculated reaction σ using optical model with QRPA target excitations and coupling to inelastic and transfer channels. Proton reactions compared to data.

doi: 10.1088/1742-6596/312/4/082033
Citations: PlumX Metrics


2011PI01      Phys.Rev. C 83, 024601 (2011)

M.T.Pigni, M.Herman, P.Oblozinsky, F.S.Dietrich

Sensitivity analysis of neutron total and absorption cross sections within the optical model

NUCLEAR REACTIONS 56Fe(n, X), E=0.001-200 MeV; calculated total neutron cross section and compared to experimental data ENDF/B-VII.0 evaluation, sensitivity of the total and absorption cross sections to perturbations of the potential strengths, radii, and diffuseness parameters. A=20-200; calculated fractional uncertainties for neutron total and absorption across sections on 75 target nuclei obtained for three different global spherical optical potentials (Koning-Delaroche, Walter-Guss, Becchetti-Greenlees) for E(n)=0.001-200 MeV. Comparisons with Ramsauer model for neutron energies above 4 MeV. Optical model parametrization and applicability.

doi: 10.1103/PhysRevC.83.024601
Citations: PlumX Metrics


2010ES02      Phys.Rev. C 81, 024612 (2010)

J.E.Escher, F.S.Dietrich

Cross sections for neutron capture from surrogate measurements: An examination of Weisskopf-Ewing and ratio approximations

NUCLEAR REACTIONS 235U, 235mU(n, γ), E=0.01-4.5 MeV; 235U(n, f), E=0-20 MeV; analyzed yields of γ rays in the ground-state band of 236U to the total production of 236U, σ from experiments and ENSDF/B-VII, Weisskopf-Ewing estimates from surrogate experiments, external and internal surrogate ratio estimates from simulated surrogate experiments. 233U(n, γ), E=0-3.5 MeV; 155,157Gd(n, γ), E=0-4.5 MeV; analyzed Weisskopf-Ewing estimates from surrogate experiments. Discussed validity and limitations of Weisskopf-Ewing and ratio approximations for surrogate reactions.

NUCLEAR STRUCTURE 156,158Gd, 236U; calculated Jπ distributions, γ-decay probabilities of compound nuclei as function of spin-parity distributions and excitation energy.

doi: 10.1103/PhysRevC.81.024612
Citations: PlumX Metrics


2010NO06      Phys.Rev.Lett. 105, 202502 (2010)

G.P.A.Nobre, F.S.Dietrich, J.E.Escher, I.J.Thompson, M.Dupuis, J.Terasaki, J.Engel

Coupled-Channel Calculation of Nonelastic Cross Sections Using a Density-Functional Structure Model

NUCLEAR REACTIONS 40,48Ca, 58Ni, 90Zr, 144Sm(p, X), (n, X), E<40 MeV; calculated total reaction σ. Complete microscopic calculation, comparison with experimental data.

doi: 10.1103/PhysRevLett.105.202502
Citations: PlumX Metrics


2010SC06      Phys.Rev. C 81, 034608 (2010)

N.D.Scielzo, J.E.Escher, J.M.Allmond, M.S.Basunia, C.W.Beausang, L.A.Bernstein, D.L.Bleuel, J.T.Burke, R.M.Clark, F.S.Dietrich, P.Fallon, J.Gibelin, B.L.Goldblum, S.R.Lesher, M.A.McMahan, E.B.Norman, L.Phair, E.Rodriquez-Vieitez, S.A.Sheets, I.J.Thompson, M.Wiedeking

Measurement of γ-emission branching ratios for 154, 156, 158Gd compound nuclei: Tests of surrogate nuclear reaction approximations for (n, γ) cross sections

NUCLEAR REACTIONS 154,156,158Gd(p, p'γ), E=22 MeV; measured Eγ, Iγ, proton spectra, γ-ray emission probabilities using STARS/LiBerACE array. 155,157Gd(n, γ), E=0.01-4 MeV; deduced σ by surrogate reaction method using Weisskopf-Ewing and ratio approximations.

doi: 10.1103/PhysRevC.81.034608
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14268.


2009BA23      Nucl.Instrum.Methods Phys.Res. B267, 1899 (2009)

M.S.Basunia, R.M.Clark, B.L.Goldblum, L.A.Bernstein, L.Phair, J.T.Burke, C.W.Beausang, D.L.Bleuel, B.Darakchieva, F.S.Dietrich, M.Evtimova, P.Fallon, J.Gibelin, R.Hatarik, C.C.Jewett, S.R.Lesher, M.A.McMahan, E.Rodriguez-Vieitez, M.Wiedeking

The (3He, tf) as a surrogate reaction to determine (n, f) cross sections in the 10-20 MeV energy range

NUCLEAR REACTIONS 238U(3He, tf), E=10-20 MeV; Measured surrogate σ;237Np(n, f); Deduced σ. Compared results with ENDF/B-VII.0, JENDL-3.3 libraries.

doi: 10.1016/j.nimb.2009.04.006
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31673.


2009LE11      Phys.Rev. C 79, 044609 (2009)

S.R.Lesher, J.T.Burke, L.A.Bernstein, H.Ai, C.W.Beausang, D.L.Bleuel, R.M.Clark, F.S.Dietrich, J.E.Escher, P.Fallon, J.Gibelin, B.L.Goldblum, I.Y.Lee, A.O.Macchiavelli, M.A.McMahan, K.J.Moody, E.B.Norman, L.Phair, E.Rodriguez-Vieitez, N.D.Scielzo, M.Wiedeking

Surrogate ratio method in the actinide region using the (α, α'f) reaction

NUCLEAR REACTIONS 234,236U(α, α'f), E=55 MeV; measured fission spectra, α(fission)-coin, in-plane and out-of-plane fission ratios; deduced direct-reaction-induced fission probability ratio. 233,235U(n, f); compared cross sections. Comparison between fission probability ratio and ratio of cross sections. Surrogate ratio method (SRM). Application of SRM as a method of calculating unknown cross sections.

doi: 10.1103/PhysRevC.79.044609
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14250.


2008DI18      Nucl.Data Sheets 109, 2774 (2008)

F.S.Dietrich

Uncertainties in Measurements and Calculations of Nonelastic Cross Sections

NUCLEAR REACTIONS 238U(n, X), E < 20 MeV; 54,56Fe(n, X), E < 20 MeV; analyzed cross sections.

doi: 10.1016/j.nds.2008.11.008
Citations: PlumX Metrics


2007DI12      Nucl.Phys. A787, 237c (2007)

F.S.Dietrich, J.E.Escher

Compound-nuclear reaction cross sections via surrogate reactions

NUCLEAR REACTIONS 233,235U(n, F), E=0-20 MeV; calculated fission σ. Hauser-Feshbach model with Weisskopf-Ewing treatment.

doi: 10.1016/j.nuclphysa.2006.12.038
Citations: PlumX Metrics


2007ES03      Nucl.Instrum.Methods Phys.Res. B261, 1075 (2007)

J.E.Escher, F.S.Dietrich, C.Forssen

Surrogate nuclear reaction methods for astrophysics

NUCLEAR REACTIONS 235U(n, X), E < 7 MeV; calculated fission probability and cross section using the surrogate technique.

doi: 10.1016/j.nimb.2007.04.223
Citations: PlumX Metrics


2007FO04      Phys.Rev. C 75, 055807 (2007)

C.Forssen, F.S.Dietrich, J.Escher, R.D.Hoffman, K.Kelley

Determining neutron capture cross sections via the surrogate reaction technique

NUCLEAR REACTIONS Zr(n, γ), E< 5 MeV; calculated cross sections and neutron tranmission coefficients using the surrogate method. Discussed astrophysical implications.

doi: 10.1103/PhysRevC.75.055807
Citations: PlumX Metrics


2007LY04      Phys.Rev. C 76, 014606 (2007); Erratum Phys.Rev. C 76, 019905 (2007)

B.F.Lyles, L.A.Bernstein, J.T.Burke, F.S.Dietrich, J.Escher, I.Thompson, D.L.Bleuel, R.M.Clark, P.Fallon, J.Gibelin, A.O.Macchiavelli, M.A.McMahan, L.Phair, E.Rodriguez-Vieitez, M.Wiedeking, C.W.Beausang, S.R.Lesher, B.Darakchieva, M.Evtimova

Absolute and relative surrogate measurements of the 236U(n, f) cross section as a probe of angular momentum effects

NUCLEAR REACTIONS 235,238U(3He, αf), E=42 MeV; measured fission fragment spectra in coincidence with α-particles. 236U(n, f), E< 20 MeV; deduced cross sections using the surrogate technique.

doi: 10.1103/PhysRevC.76.014606
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14146.


2006BU06      Phys.Rev. C 73, 054604 (2006)

J.T.Burke, L.A.Bernstein, J.Escher, L.Ahle, J.A.Church, F.S.Dietrich, K.J.Moody, E.B.Norman, L.Phair, P.Fallon, R.M.Clark, M.A.Deleplanque, M.Descovich, M.Cromaz, I.Y.Lee, A.O.Macchiavelli, M.A.McMahan, L.G.Moretto, E.Rodriguez-Vieitez, F.S.Stephens, H.Ai, C.Plettner, C.Beausang, B.Crider

Deducing the 237U(n, f) cross section using the surrogate ratio method

NUCLEAR REACTIONS 236,238U(α, α'F), E=55 MeV; measured Eα, fission fragment spectra; deduced relative fission yields. 237U(n, F), E=0-20 MeV; deduced fission σ. Surrogate ratio method.

doi: 10.1103/PhysRevC.73.054604
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14094.


2006ES03      Phys.Rev. C 74, 054601 (2006)

J.E.Escher, F.S.Dietrich

Determining (n, f) cross sections for actinide nuclei indirectly: Examination of the surrogate ratio method

NUCLEAR REACTIONS 233,235,235mU(n, F), E ≈ 0-20 MeV; analyzed fission σ, pre-equilibrium effects, branching ratios. Validity of surrogate ratio method discussed.

doi: 10.1103/PhysRevC.74.054601
Citations: PlumX Metrics


2006MC01      Nucl.Sci.Eng. 152, 15 (2006)

D.P.McNabb, J.D.Anderson, R.W.Bauer, F.S.Dietrich, S.M.Grimes, C.A.Hagmann

Comparison of Ramsauer and Optical Model Neutron Angular Distributions

NUCLEAR REACTIONS 208Pb(n, n), E < 60 MeV; analyzed σ(θ). Comparison of Ramsauer and optical model approaches, role of angular bin dispersion discussed.

doi: 10.13182/NSE06-A2558
Citations: PlumX Metrics


2005CH53      Nucl.Phys. A758, 126c (2005)

J.A.Church, L.Ahle, L.A.Bernstein, J.Cooper, F.S.Dietrich, J.Escher, C.Forssen, H.Ai, H.Amro, M.Babilon, C.Beausang, J.Caggiano, A.Heinz, R.Hughes, E.McCutchan, D.Meyer, C.Plettner, J.Ressler, V.Zamfir

Determining neutron capture cross sections with the Surrogate Reaction Technique: Measuring decay probabilities with STARS

NUCLEAR REACTIONS 92Zr(α, α'), (α, 3HeX), (α, tX), (α, dX), (α, pX), E=51 MeV; measured particle spectra. 92Zr(α, α'), (α, xnα), E=51 MeV; measured Eγ, Iγ, αγ-coin. 90,91,92Zr deduced transitions. Surrogate reaction technique.

doi: 10.1016/j.nuclphysa.2005.05.169
Citations: PlumX Metrics


2005FO11      Nucl.Phys. A758, 130c (2005)

C.Forssen, L.Ahle, L.A.Bernstein, J.A.Church, F.S.Dietrich, J.Escher, R.D.Hoffman

Theoretical challenges of determining low-energy neutron-capture cross sections via the Surrogate Technique

doi: 10.1016/j.nuclphysa.2005.05.026
Citations: PlumX Metrics


2003DI03      Phys.Rev. C 67, 044606 (2003)

F.S.Dietrich, J.D.Anderson, R.W.Bauer, S.M.Grimes, R.W.Finlay, W.P.Abfalterer, F.B.Bateman, R.C.Haight, G.L.Morgan, E.Bauge, J.-P.Delaroche, P.Romain

Importance of isovector effects in reproducing neutron total cross section differences in the W isotopes

NUCLEAR REACTIONS 182,184,186W(n, X), E=5-560 MeV; measured total σ. Comparison with model predictions.

doi: 10.1103/PhysRevC.67.044606
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13887.


2003DI13      Phys.Rev. C 68, 064608 (2003)

F.S.Dietrich, J.D.Anderson, R.W.Bauer, S.M.Grimes

Wick's limit and new method for estimating neutron reaction cross sections

NUCLEAR REACTIONS 28Si, 40Ca, 59Co, 89Y, 140Ce, 208Pb(n, X), E ≈ 1-200 MeV; calculated reaction σ, deviation from Wick's limit. Analytic model.

doi: 10.1103/PhysRevC.68.064608
Citations: PlumX Metrics


2001AB14      Phys.Rev. C63, 044608 (2001)

W.P.Abfalterer, F.B.Bateman, F.S.Dietrich, R.W.Finlay, R.C.Haight, G.L.Morgan

Measurement of Neutron Total Cross Sections up to 560 MeV

NUCLEAR REACTIONS H, Li, 6,7Li, B, 10,11B, C, 13C, F, Mg, S, P, K, Ca, Ti, V, Cr, Mn, Fe, Ni, Co, Y, Mo, In, W, 197Au, Hg, Pb, Th, 238U(n, X), E < 600 MeV; measured transmission neutron spectra; deduced total σ. Comparisons with model predictions, previous results.

doi: 10.1103/PhysRevC.63.044608
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13753.


1998AB21      Phys.Rev.Lett. 81, 57 (1998)

W.P.Abfalterer, F.B.Bateman, F.S.Dietrich, Ch.Elster, R.W.Finlay, W.Glockle, J.Golak, R.C.Haight, D.Huber, G.L.Morgan, H.W.Witala

Inadequacies of the Nonrelativistic 3N Hamiltonian in Describing the n + d Total Cross Section

NUCLEAR REACTIONS 1,2H(n, X), E=7-600 MeV; measured σ; deduced possible relativistic effects. Fadeev calculations.

doi: 10.1103/PhysRevLett.81.57
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13889.


1998ST17      Phys.Rev. D58, 032003 (1998)

L.M.Stuart, P.E.Bosted, L.Andivahis, A.Lung, J.Alster, R.G.Arnold, C.C.Chang, F.S.Dietrich, W.R.Dodge, R.Gearhart, J.Gomez, K.A.Griffioen, R.S.Hicks, C.E.Hyde-Wright, C.Keppel, S.E.Kuhn, J.Lichtenstadt, R.A.Miskimen, G.A.Peterson, G.G.Petratos, S.E.Rock, S.H.Rokni, W.K.Sakumoto, M.Spengos, K.Swartz, Z.Szalata, L.H.Tao

Measurements of the Δ(1232) Transition Form Factor and the Ratio σnp from Inelastic Electron-Proton and Electron-Deuteron Scattering

NUCLEAR REACTIONS 1,2H(e, e'), E=9.8 GeV; measured σ(E', θ); deduced transition form factors, Δ production σ(n)/σ(p).

doi: 10.1103/PhysRevD.58.032003
Citations: PlumX Metrics


1997CO11      Phys.Lett. 401B, 9 (1997)

M.D.Cortina-Gil, P.Roussel-Chomaz, N.Alamanos, J.Barrette, W.Mittig, F.S.Dietrich, F.Auger, Y.Blumenfeld, J.M.Casandjian, M.Chartier, V.Fekou-Youmbi, B.Fernandez, N.Frascaria, A.Gillibert, H.Laurent, A.Lepine-Szily, N.A.Orr, J.A.Scarpaci, J.L.Sida, T.Suomijarvi

Proton Elastic Scattering on Light Neutron-Rich Nuclei

NUCLEAR REACTIONS 1H(7Li, 7Li), E=68 MeV/nucleon; 1H(6He, 6He), E=41.6 MeV/nucleon; 1H(10Be, 10Be), E=59.3 MeV/nucleon; 1H(11Be, 11Be), E=49.3 MeV/nucleon; measured σ(θ); 1H(8He, 8He), E=72 MeV/nucleon; 1H(9Li, 9Li), E=60 MeV/nucleon; 1H(11Li, 11Li), E=62 MeV/nucleon; analyzed σ(θ); deduced break-up channels role, optical potential related features. Phenomenological, microscopic optical models.

doi: 10.1016/S0370-2693(97)00321-3
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0246.


1996AB02      Phys.Rev.Lett. 76, 587 (1996)

K.Abe, T.Akagi, P.L.Anthony, R.Antonov, R.G.Arnold, T.Averett, H.R.Band, J.M.Bauer, H.Borel, P.E.Bosted, V.Breton, J.Button-Shafer, J.P.Chen, T.E.Chupp, J.Clendenin, C.Comptour, K.P.Coulter, G.Court, D.Crabb, M.Daoudi, D.Day, F.S.Dietrich, J.Dunne, H.Dutz, R.Erbacher, J.Fellbaum, A.Feltham, H.Fonvieille, E.Frlez, D.Garvey, R.Gearhart, J.Gomez, P.Grenier, K.A.Griffioen, S.Hoibraten, E.W.Hughes, C.Hyde-Wright, J.R.Johnson, D.Kawall, A.Klein, S.E.Kuhn, M.Kuriki, R.Lindgren, T.J.Liu, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, X.K.Maruyama, J.McCarthy, W.Meyer, Z.-E.Meziani, R.Minehart, J.Mitchell, J.Morgenstern, G.G.Petratos, R.Pitthan, D.Pocanic, C.Prescott, R.Prepost, P.Raines, B.Raue, D.Reyna, A.Rijllart, Y.Roblin, L.S.Rochester, S.E.Rock, O.A.Rondon, I.Sick, L.C.Smith, T.B.Smith, M.Spengos, F.Staley, P.Steiner, S.St.Lorant, L.M.Stuart, F.Suekane, Z.M.Szalata, H.Tang, Y.Terrien, T.Usher, D.Walz, J.L.White, K.Witte, C.C.Young, B.Youngman, H.Yuta, G.Zapalac, B.Zihlmann, D.Zimmermann, and the E143 Collaboration

Measurements of the Proton and Deuteron Spin Structure Function g2 and Asymmetry A2

NUCLEAR STRUCTURE 1,2H; analyzed data; deduced spin structure function, asymmetry data. Polarized ammonia targets, (polarized e, e') reaction.

NUCLEAR REACTIONS 1,2H(polarized e, e'), E=29.1 GeV; measured spin asymmetries. 1,2H deduced spin structure functions. Polarized ammonia targets.

doi: 10.1103/PhysRevLett.76.587
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1995AB02      Phys.Rev.Lett. 74, 346 (1995)

K.Abe, T.Akagi, P.L.Anthony, R.Antonov, R.G.Arnold, T.Averett, H.R.Band, J.M.Bauer, H.Borel, P.E.Bosted, V.Breton, J.Button-Shafer, J.P.Chen, T.E.Chupp, J.Clendenin, C.Comptour, K.P.Coulter, G.Court, D.Crabb, M.Daoudi, D.Day, F.S.Dietrich, J.Dunne, H.Dutz, R.Erbacher, J.Fellbaum, A.Feltham, H.Fonvieille, E.Frlez, D.Garvey, R.Gearhart, J.Gomez, P.Grenier, K.A.Griffioen, S.Hoibraten, E.W.Hughes, C.Hyde-Wright, J.R.Johnson, D.Kawall, A.Klein, S.E.Kuhn, M.Kuriki, R.Lindgren, T.J.Liu, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, X.K.Maruyama, J.McCarthy, W.Meyer, Z.-E.Meziani, R.Minehart, J.Mitchell, J.Morgenstern, G.G.Petratos, R.Pitthan, D.Pocanic, C.Prescott, R.Prepost, P.Raines, B.Raue, D.Reyna, A.Rijllart, Y.Roblin, L.S.Rochester, S.E.Rock, O.A.Rondon, I.Sick, L.C.Smith, T.B.Smith, M.Spengos, F.Staley, P.Steiner, S.St.Lorant, L.M.Stuart, F.Suekane, Z.M.Szalata, H.Tang, Y.Terrien, T.Usher, D.Walz, J.L.White, K.Witte, C.C.Young, B.Youngman, H.Yuta, G.Zapalac, B.Zihlmann, D.Zimmermann, and the E143 Collaboration

Precision Measurement of the Proton Spin Structure Function g1(p)

NUCLEAR REACTIONS 1H(polarized e, e'), E=9.7-29.1 GeV; measured asymmetry. 1H deduced spin structure function g1(p). Polarized 15NH3 target.

doi: 10.1103/PhysRevLett.74.346
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1995AR06      Phys.Rev. C51, R1078 (1995)

G.Arbanas, M.B.Chadwick, F.S.Dietrich, A.K.Kerman

Linking of Direct and Compound Chains in Multistep Nuclear Reactions

NUCLEAR REACTIONS 93Nb(n, n'), E=14 MeV; analyzed angle integrated σ data; deduced direct, compound chains linking role on emisssion probabilities. Modified DWBA, multi-step reactions.

doi: 10.1103/PhysRevC.51.R1078
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1995BU28      Phys.Rev.Lett. 74, 4775 (1995)

H.J.Bulten, P.L.Anthony, R.G.Arnold, J.Arrington, E.J.Beise, J.E.Belz, K.van Bibber, P.E.Bosted, J.F.J.van den Brand, M.S.Chapman, K.P.Coulter, F.S.Dietrich, R.Ent, M.Epstein, B.W.Filippone, H.Gao, R.A.Gearhart, D.F.Geesaman, J.-O.Hansen, R.J.Holt, H.E.Jackson, C.E.Jones, C.E.Keppel, E.Kinney, S.E.Kuhn, K.Lee, W.Lorenzon, A.Lung, N.C.R.Makins, D.J.Margaziotis, R.D.McKeown, R.G.Milner, B.Mueller, J.Napolitano, J.Nelson, T.G.O'Neill, V.Papavassiliou, G.G.Petratos, D.H.Potterveld, S.E.Rock, M.Spengos, Z.M.Szalata, L.H.Tao, J.L.White, B.Zeidman

Exclusive Electron Scattering from Deuterium at High Momentum Transfer

NUCLEAR REACTIONS 2H(e, e'p), E=2-5.1 GeV; measured σ(θ(e), θp, E(e)), asymmetry A(φ). Nonrelativistic, relativistic framework analyses.

doi: 10.1103/PhysRevLett.74.4775
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1995PA24      Phys.Rev. C52, 252 (1995)

W.E.Parker, M.B.Chadwick, F.S.Dietrich, J.E.Kammeraad, S.J.Luke, K.E.Sale, R.M.Chasteler, M.A.Godwin, L.H.Kramer, G.J.Schmid, H.R.Weller, A.K.Kerman

Fluctuation Effects in Radiative Capture to Unstable Final States: A test via the 89Y(p(pol), γ) reaction at E(p) = 19.6 MeV

NUCLEAR REACTIONS 89Y(polarized p, γ), E=19.6 MeV; measured σ(θ), analyzing power(θ) vs Eγ. Direct-semdirect Hauser-Feshbach analyses. NaI(T1) detector.

doi: 10.1103/PhysRevC.52.252
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1994AN34      Phys.Rev. D50, 5491 (1994)

L.Andivahis, P.E.Bosted, A.Lung, L.M.Stuart, J.Alster, R.G.Arnold, C.C.Chang, F.S.Dietrich, W.Dodge, R.Gearhart, J.Gomez, K.A.Griffioen, R.S.Hicks, C.E.Hyde-Wright, C.Keppel, S.E.Kuhn, J.Lichtenstadt, R.A.Miskimen, G.A.Peterson, G.G.Petratos, S.E.Rock, S.Rokni, W.K.Sakumoto, M.Spengos, K.Swartz, Z.Szalata, L.H.Tao

Measurements of the Electric and Magnetic Form Factors of the Proton from Q2 = 1.75 to 8.83 (GeV/c)2

NUCLEAR REACTIONS 1H(e, e), E ≈ 9.8 GeV; measured σ(θ). 1H deduced electric, magnetic form factors. Model comparison.

doi: 10.1103/PhysRevD.50.5491
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1994DE17      Phys.Rev. C50, R541 (1994)

P.V.Degtyarenko, J.Button-Shafer, L.Elouadrhiri, R.A.Miskimen, G.A.Peterson, K.Wang, V.B.Gavrilov, M.V.Kossov, G.A.Leksin, S.M.Shuvalov, F.S.Dietrich, S.O.Melnikoff, J.D.Molitoris, K.Van Bibber

Multiple Hadron Production by 14.5 GeV Electron and Positron Scattering from Nuclear Targets

NUCLEAR REACTIONS 12C, 16O, 40Ar(e, e'2p), E=14.5 GeV; measured secondary protons, pions differential multiplicities; deduced spectra phenomenological parameters, their dependence on ν, Q2. Deep inelastic nuclear reactions.

doi: 10.1103/PhysRevC.50.R541
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1994EL13      Phys.Rev. C50, R2266 (1994)

L.Elouadrhiri, R.A.Miskimen, J.Button-Shafer, P.Degtyarenko, G.A.Peterson, S.Shuvalov, K.Wang, V.Gavrilov, F.S.Dietrich, S.O.Melnikoff, J.D.Molitoris, K.Van Bibber

Measurements of the (e, e'pπ-) Reaction on Nuclei in the Nucleon Resonance Region

NUCLEAR REACTIONS 2H, C, O, Ar, Xe(e, e'pπ-), E=14.5 GeV; measured missing transverse momentum distribution, other aspects; deduced resonance beyond Δ(1232). DWIA analysis.

doi: 10.1103/PhysRevC.50.R2266
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1994MA23      Phys.Rev.Lett. 72, 1986 (1994)

N.C.R.Makins, R.Ent, M.S.Chapman, J.-O.Hansen, K.Lee, R.G.Milner, J.Nelson, R.G.Arnold, P.E.Bosted, C.E.Keppel, A.Lung, S.E.Rock, M.Spengos, Z.M.Szalata, L.H.Tao, J.L.White, K.P.Coulter, D.F.Geesaman, R.J.Holt, H.E.Jackson, V.Papavassiliou, D.H.Potterveld, B.Zeidman, J.Arrington, E.J.Beise, J.E.Belz, B.W.Filippone, H.Gao, W.Lorenzon, B.Mueller, R.D.McKeown, T.G.O'Neill, M.Epstein, D.J.Margaziotis, J.Napolitano, E.Kinney, P.L.Anthony, K.van Bibber, F.S.Dietrich, R.A.Gearhart, G.G.Petratos, S.E.Kuhn, J.F.J.van den Brand, H.-J.Bulten, C.E.Jones

Momentum Transfer Dependence of Nuclear Transparency from the Quasielastic 12C(e, e'p) Reaction

NUCLEAR REACTIONS 12C(e, e'p), E not given; measured missing energy distributions; deduced nuclear transparency vs momentum transfer.

doi: 10.1103/PhysRevLett.72.1986
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1993AN12      Phys.Rev.Lett. 71, 959 (1993)

P.L.Anthony, R.G.Arnold, H.R.Band, H.Borel, P.E.Bosted, V.Breton, G.D.Cates, T.E.Chupp, F.S.Dietrich, J.Dunne, R.Erbacher, J.Fellbaum, H.Fonvieille, R.Gearhart, R.Holmes, E.W.Hughes, J.R.Johnson, D.Kawall, C.Keppel, S.E.Kuhn, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, W.Meyer, Z.-E.Meziani, H.Middleton, J.Morgenstern, N.R.Newbury, G.G.Petratos, R.Pitthan, R.Prepost, Y.Roblin, S.E.Rock, S.H.Rokni, G.Shapiro, T.Smith, P.A.Souder, M.Spengos, F.Staley, L.M.Stuart, Z.M.Szalata, Y.Terrien, A.K.Thompson, J.L.White, M.Woods, J.Xu, C.C.Young, G.Zapalac, and the E142 Collaboration

Determination of the Neutron Spin Structure Function

NUCLEAR REACTIONS 3He(polarized e, e'), E=19-26 GeV; measured neutron asymmetry. 1n deduced spin structure function. Polarized target.

doi: 10.1103/PhysRevLett.71.959
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1993PE13      Nucl.Phys. A563, 387 (1993)

F.Petrovich, S.K.Yoon, M.J.Threapleton, R.J.Philpott, J.A.Carr, F.S.Dietrich, L.F.Hansen

Consistent Folding Model Description of Nucleon Elastic, Inelastic, and Charge-Exchange Scattering from 6,7Li at 25-50 MeV

NUCLEAR REACTIONS 6Li(p, p), E=24.4-49.75 MeV; analyzed σ(θ). 7Li(polarized p, p), (polarized p, p'), E=24.4, 49.75, 200 MeV; analyzed σ(θ), analyzing power vs θ. Folding model.

doi: 10.1016/0375-9474(93)90120-M
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1992BO34      Phys.Rev. C46, 2505 (1992)

P.E.Bosted, A.Lung, L.Andivahis, L.M.Stuart, J.Alster, R.G.Arnold, C.C.Chang, F.S.Dietrich, W.Dodge, R.Gearhart, J.Gomez, K.A.Griffioen, R.S.Hicks, C.E.Hyde-Wright, C.Keppel, S.E.Kuhn, J.Lichtenstadt, R.A.Miskimen, G.A.Peterson, G.G.Petratos, S.E.Rock, S.Rokni, W.K.Sakumoto, M.Spengos, K.Swartz, Z.Szalata, L.H.Tao

Measurements of (ν)W2 and R = σ(L)/σ(T) from Inelastic Electron-Aluminum Scattering Near x = 1

NUCLEAR REACTIONS 27Al(e, e'X), E=1.5-5.5 GeV; measured inclusive σ per nucleon, ratio to 2H; deduced σ(L)/σ(T) vs Q2.

doi: 10.1103/PhysRevC.46.2505
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1989CA08      Phys.Rev. C39, 1725 (1989)

H.S.Camarda, F.S.Dietrich, T.W.Phillips

Microscopic Optical-Model Calculations of Neutron Total Cross Sections and Cross Section Differences

NUCLEAR REACTIONS 142,140Ce, 139La, 141Pr, 40,44Ca(n, X), E=6-60 MeV; calculated σ(E). Microscopic optical model.

doi: 10.1103/PhysRevC.39.1725
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1989FI02      Phys.Rev. C39, 804 (1989)

R.W.Finlay, J.Wierzbicki, R.K.Das, F.S.Dietrich

Phenomenological Analysis of Dispersion Corrections for Neutron and Proton Scattering from 208Pb

NUCLEAR REACTIONS 208Pb(polarized p, p), E=9-61 MeV; 208Pb(polarized n, n), E=4-40 MeV; analyzed σ(θ), A(θ); deduced optical model parameters, dispersion correction.

doi: 10.1103/PhysRevC.39.804
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1987DE06      Phys.Rev. C35, 942 (1987)

J.P.Delaroche, F.S.Dietrich

Coupled-Channel Description of Inelastic Scattering from Soft Nuclei

NUCLEAR REACTIONS 196Pt(polarized p, p), (polarized p, p'), E=35 MeV; calculated σ(θ), analyzing power vs θ. Many-body collective wave functions, coupled-channels description.

doi: 10.1103/PhysRevC.35.942
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1987ME10      Phys.Rev. C36, 577 (1987)

S.Mellema, J.S.Petler, R.W.Finlay, F.S.Dietrich, J.A.Carr, F.Petrovich

Microscopic Distorted-Wave Approximation Study of Low-Energy Nucleon Scattering from 89Y

NUCLEAR REACTIONS 89Y(n, n), (n, n'), E=11 MeV; measured σ(θ). 89Y levels deduced B(λ), transition densities. Tof. Optical model. Microscopic distorted wave calculations.

doi: 10.1103/PhysRevC.36.577
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1987OL03      Nucl.Phys. A472, 237 (1987)

N.Olsson, B.Trostell, E.Ramstrom, B.Holmqvist, F.S.Dietrich

Microscopic and Conventional Optical Model Analysis of Neutron Elastic Scattering at 21.6 MeV over a Wide Mass Range

NUCLEAR REACTIONS Mg, 27Al, Si, S, Ca, Cr, Fe, 59Co, Ni, 89Y, Ce, Pb, 209Bi(n, n), E=21.6 MeV; measured σ(θ); deduced spherical optical model parameters. Microscopic analyses. Radiogenic Pb target.

doi: 10.1016/0375-9474(87)90209-0
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1986BE17      Nucl.Phys. A456, 426 (1986)

I.Bergqvist, D.M.Drake, D.K.McDaniels, S.A.Wender, A.Lindholm, L.Nilsson, N.Olsson, R.Zorro, F.S.Dietrich

The 12C(n, γ0)13C Reaction in the Giant Resonance Region

NUCLEAR REACTIONS 12C(n, γ), E=7-19.5 MeV; measured σ(E, θ=90°). 13C deduced giant, pygmy resonances. DSD model, 12,13C(n, γ) data input.

doi: 10.1016/0375-9474(86)90403-3
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1986ME01      Phys.Rev. C33, 481 (1986)

S.Mellema, R.W.Finlay, F.S.Dietrich

Neutron Inelastic Scattering from 54,56Fe

NUCLEAR REACTIONS 56,54Fe(n, n'), E=11, 26 MeV; measured σ(θ); deduced optical model parameters. 54,56Fe levels deduced β. DWBA, coupled-channels analyses.

doi: 10.1103/PhysRevC.33.481
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1985AN15      Nucl.Phys. A443, 249 (1985)

J.R.M.Annand, R.W.Finlay, F.S.Dietrich

A Low-Energy Optical-Model Analysis of 208Pb and 209Bi

NUCLEAR REACTIONS 208Pb, 209Bi(n, n), (n, n'), E=4-7 MeV; measured σ(E, θ); deduced optical model parameters. Statistical model analysis, DWBA, coupled-channel calculations.

doi: 10.1016/0375-9474(85)90263-5
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1985FI02      Phys.Lett. 155B, 313 (1985)

R.W.Finlay, J.R.M.Annand, J.S.Petler, F.S.Dietrich

Anomalous Behavior of the n + 208Pb Potential near the Fermi Energy

NUCLEAR REACTIONS 208Pb, 209Bi(n, n), (n, n'), E=4-7 MeV; measured σ(θ); deduced potential parameters, Fermi surface anomaly.

doi: 10.1016/0370-2693(85)91577-1
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1985HA02      Phys.Rev. C31, 111 (1985)

L.F.Hansen, F.S.Dietrich, B.A.Pohl, C.H.Poppe, C.Wong

Test of Microscopic Optical Model Potentials for Neutron Elastic Scattering at 14.6 MeV over a Wide Mass Range

NUCLEAR REACTIONS 9Be, C, 27Al, Fe, 59Co, 93Nb, 89Y, In, 140Ce, 181Ta, 197Au, 208Pb, 209Bi(n, n), E=14.6 MeV; measured σ(θ). Local microscopic potentials, optical model analysis.

doi: 10.1103/PhysRevC.31.111
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1985PE10      Phys.Rev. C32, 673 (1985)

J.S.Petler, M.S.Islam, R.W.Finlay, F.S.Dietrich

Microscopic Optical Model Analysis of Nucleon Scattering from Light Nuclei

NUCLEAR REACTIONS 13C(n, n), E=24 MeV; 14N(n, n), E=20, 25 MeV; 16O, 27Al(n, n), E=18-26 MeV; measured σ(θ) vs E; 12C(n, n), E=20-40 MeV; 12C(p, p), E=35-46 MeV; 14N(p, p), E=35.2 MeV; 16O(p, p), E=24.5, 30.1, 39.7 MeV; analyzed σ(θ). Micropscopic optical model.

doi: 10.1103/PhysRevC.32.673
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1984FI12      Phys.Rev. C30, 796 (1984)

R.W.Finlay, J.R.M.Annand, T.S.Cheema, J.Rapaport, F.S.Dietrich

Energy Dependence of Neutron Scattering from 208Pb in the Energy Range 7-50 MeV

NUCLEAR REACTIONS 208Pb(n, n), E=7, 20, 22, 24 MeV; 208Pb(n, n'), E=7, 20, 22 MeV; measured σ(E, θ); deduced optical model parameters. 208Pb level deduced octupole deformation parameter.

doi: 10.1103/PhysRevC.30.796
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1984MA67      Astrophys.J. 287, 969 (1984)

G.J.Mathews, F.S.Dietrich

The 13N(p, γ)14O Thermonuclear Reaction Rate and the Hot CNO Cycle

NUCLEAR REACTIONS, ICPND 13N(p, γ), E=resonance; calculated thermonuclear capture σ, reaction rate. 14O level deduced Γ. Semi-direct radiative capture model.

doi: 10.1086/162754
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1984ME07      Phys.Rev. C29, 2385 (1984)

S.Mellema, R.W.Finlay, F.S.Dietrich, F.Petrovich

Isovector Effects in Nucleon Inelastic Scattering in a Density-Dependent Folding Model

NUCLEAR REACTIONS 56,54Fe(p, p'), (n, n'), E=11-26 MeV; analyzed σ(θ); deduced isovector effects. 54,56Fe levels deduced neutron, proton transition matrix element ratio. Microscopic DWBA, folding model potentials from density-dependent interactions.

doi: 10.1103/PhysRevC.29.2385
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1983DI11      Phys.Rev.Lett. 51, 1629 (1983)

F.S.Dietrich, R.W.Finlay, S.Mellema, G.Randers-Pehrson, F.Petrovich

Isospin Dependence of the Microscopic Optical Model for Nucleon Scattering

NUCLEAR REACTIONS 208Pb(n, n), E=7-24 MeV; measured σ(θ). 208Pb(p, p), E=21-61.4 MeV; analyzed σ(θ); deduced optical model isospin dependence. Microscopic folding model study.

doi: 10.1103/PhysRevLett.51.1629
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1983ME21      Phys.Rev. C28, 2267 (1983)

S.Mellema, R.W.Finlay, F.S.Dietrich, F.Petrovich

Microscopic and Conventional Optical Model Analysis of Fast Neutron Scattering from 54,56Fe

NUCLEAR REACTIONS 54Fe(n, n), E=20, 22, 24, 26 MeV; 56Fe(n, n), E=20, 26 MeV; measured σ(θ); deduced optical model parameters. Phenomenological, microscopic models.

doi: 10.1103/PhysRevC.28.2267
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1982BL19      Phys.Rev. C26, 1471 (1982)

M.Blann, D.Akers, T.A.Komoto, F.S.Dietrich, L.F.Hansen, J.G.Woodworth, W.Scobel, J.Bisplinghoff, B.Sikora, F.Plasil, R.L.Ferguson

Saturation Analysis as a Test of Statistical Fission in Heavy Ion Reactions

NUCLEAR REACTIONS 120,122Sn(56Fe, X), E=330-456 MeV; measured σ(evaporation residue θ), σ(fragment θ) vs mass; deduced statistical fission decay yield limit. 176Os deduced fission barrier vs J.

doi: 10.1103/PhysRevC.26.1471
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1981NE09      Phys.Rev. C24, 1864 (1981)

A.V.Nero, E.G.Adelberger, F.S.Dietrich

Structure of 18Ne

NUCLEAR STRUCTURE 18O, 18F, 18Ne; calculated levels T=1 Coulomb shifts.

NUCLEAR REACTIONS 16O(3He, n), E=10-22 MeV; measured σ(En, θ). 20Ne(p, t), E=41.8 MeV; measured σ(Et, θ). 18Ne deduced levels, J, π. Gas targets. DWBA analysis.

doi: 10.1103/PhysRevC.24.1864
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1980HO06      Phys.Rev. C21, 1153 (1980)

R.H.Howell, F.S.Dietrich, D.W.Heikkinen, F.Petrovich

(p, p'γ) Spin-Flip Measurement for 1+ States in 12C at E = 23.5-27 MeV

NUCLEAR REACTIONS 12C(p, p'γ), E=22-27 MeV; measured out-of-plane p'γ(θ), p'γ-coin, σ(Ep', θ). 12C levels deduced M1 spin-flip probability vs θ. Microscopic DWBA, realistic G-matrix interaction.

doi: 10.1103/PhysRevC.21.1153
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1980HO07      Phys.Rev. C21, 1158 (1980)

R.H.Howell, F.S.Dietrich, F.Petrovich

Effect of the Tensor Force on Gamma-Ray de-Excitation Angular Distributions from Dipole States Populated in the 12C(p, p') Reaction

NUCLEAR REACTIONS 12C(p, p'γ), E=22-27 MeV; measured γ(θ), Eγ, Iγ. 12C dipole transitions deduced tensor-force effects. Microscopic distorted-wave analysis, realistic G-matrix interaction.

doi: 10.1103/PhysRevC.21.1158
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1979DI06      Phys.Rev.Lett. 43, 114 (1979)

F.S.Dietrich, A.K.Kerman

Pure-Resonance Model for Radiative Capture of Fast Nucleons

NUCLEAR REACTIONS 208Pb(n, γ), E=6-16 MeV; calculated σ(E). Direct semidirect model giant resonance projected from continuum space.

doi: 10.1103/PhysRevLett.43.114
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1978HA33      Phys.Rev. C18, 1582 (1978)

L.F.Hansen, F.S.Dietrich, R.P.Koopman

Identification of the Lowest 3- Collective Level in 116Cd

NUCLEAR REACTIONS 116Cd(p, p'γ), E=5-20 MeV; measured σ(E, Eγ). 116Cd deduced levels, J, π.

doi: 10.1103/PhysRevC.18.1582
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1977DI01      Phys.Rev.Lett. 38, 156 (1977)

F.S.Dietrich, D.W.Heikkinen, K.A.Snover, K.Ebisawa

Investigation of E2 and E3 Radiation Above the Giant Dipole Resonance in 89Y(p, γ0)90Zr

NUCLEAR REACTIONS 89Y(p, γ), E=14-27 MeV; measured σ(E, Eγ, θ). 90Zr deduced resonances, λ.

doi: 10.1103/PhysRevLett.38.156
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1976DI04      Nucl.Phys. A259, 75 (1976)

F.S.Dietrich, S.D.Bloom, D.W.Heikkinen

Gamma Decay of Analog States in 49Sc: Jπ = 5/2- and 9/2+

NUCLEAR REACTIONS 48Ca(p, γ), E=6.00-6.17 MeV; measured σ(E, Eγ, θ). 49Sc deduced isobaric analog resonances, Γ, Γγ. Enriched target, NaI detector.

doi: 10.1016/0375-9474(76)90496-6
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1976DI13      Nucl.Sci.Eng. 61, 267 (1976)

F.S.Dietrich, L.F.Hansen, R.P.Koopman

Cross Section for the 9Be(n, t1)7Li Reaction between 13.3 and 15 MeV

NUCLEAR REACTIONS 9Be(n, t), E=13.3-15 MeV; measured σ(E).

doi: 10.13182/NSE76-A27361
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1974BR38      Phys.Rev. C10, 2545 (1974)

J.C.Browne, F.S.Dietrich

Hauser-Feshbach Calculation of the 252Cf Spontaneous-Fission Neutron Spectrum

RADIOACTIVITY, Fission 252Cf(SF); calculated neutron spectrum; Hauser-Feshbach calculation.

doi: 10.1103/PhysRevC.10.2545
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1974DI04      Phys.Rev. C9, 973 (1974)

F.S.Dietrich, M.C.Gregory, J.D.Anderson

Gamma Production Cross Sections from 14-MeV Neutron Bombardment of 89Y

NUCLEAR REACTIONS 89Y(n, n'γ), (n, 2nγ), E=14.1 MeV; measured σ(Eγ). 88Y deduced levels, J, π; 89Y deduced transitions.

doi: 10.1103/PhysRevC.9.973
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1974DI10      Phys.Rev. C10, 795 (1974)

F.S.Dietrich, J.C.Browne, W.J.O'Connell, M.J.Kay

Spectrum of γ Rays in the 8- to 20-MeV Range from 252Cf Spontaneous Fission

RADIOACTIVITY, Fission 252Cf(SF); measured Eγ, Iγ, γ(t). Statistical calculation of high-energy γ-ray spectrum.

doi: 10.1103/PhysRevC.10.795
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14642.


1974DI14      Phys.Rev. C10, 1587 (1974)

F.S.Dietrich, L.F.Hansen, R.P.Koopman

Lifetimes of the First Two Excited States of 66Ga

NUCLEAR REACTIONS 66Zn(p, nγ), E=7.5-10 MeV; measured Eγ, γ(t). 66Ga levels deduced T1/2. Enriched target.

doi: 10.1103/PhysRevC.10.1587
Citations: PlumX Metrics


1974HA42      Phys.Rev. C10, 1111 (1974)

L.F.Hansen, J.C.Davis, F.S.Dietrich, M.C.Gregory, R.P.Koopman

Levels of 64Ga via the 64Zn(p, n) and 64Zn(p, nγ) Reactions

NUCLEAR REACTIONS 64Zn(p, n), E=10, 10.5 MeV; measured σ(En, θ). 64Zn(p, nγ), E=8.0-10.5 MeV; measured σ(E, Eγ), γ(t); deduced Q. 64Ga deduced levels, T1/2, J, π.

doi: 10.1103/PhysRevC.10.1111
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0477.


1974NE04      Phys.Rev.Lett. 32, 623 (1974)

A.V.Nero, E.G.Adelberger, F.S.Dietrich, G.E.Walker

Where Is the (2s1/2)2 T = 1 Strength in Mass 18

NUCLEAR REACTIONS 16O(3He, n), E=10-20 MeV; 20Ne(p, t), E=41.8 MeV; measured σ(Et, θ), σ(En, θ). 18Ne deduced levels, J, π, L.

doi: 10.1103/PhysRevLett.32.623
Citations: PlumX Metrics


1972DI05      Nucl.Phys. A184, 449 (1972)

F.S.Dietrich, E.G.Adelberger, W.E.Meyerhof

Study of the 2H(d, n)3He Reaction between 12 and 19 MeV

NUCLEAR REACTIONS 2H(d, n), E=12, 14, 16, 18 MeV; measured σ(θ), σ(En, θ0); deduced Legendre coeff.

doi: 10.1016/0375-9474(72)90420-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1074.


1970DI11      Nucl.Phys. A155, 209 (1970)

F.S.Dietrich, B.Herskind, R.A.Naumann, R.G.Stokstad

Hole-Vibration Coupling in 115In

NUCLEAR REACTIONS 115In(d, d'), E=12 MeV; measured σ(Ed', θ). 115In(16O, 16O'γ), E=41-55 MeV; measured σ(E;E(16O'), Eγ). 115In deduced levels, J, π, B(E2), branching ratios. Natural targets.

doi: 10.1016/0375-9474(70)90087-4
Citations: PlumX Metrics


1970WH05      Nucl.Phys. A157, 529 (1970)

S.Whineray, F.S.Dietrich, R.G.Stokstad

A Study of Isobaric Analogue Resonances in the Yb Isotopes

NUCLEAR REACTIONS 168,170,172,174,176Yb(p, p), E=10.0-13.0 MeV; measured σ(Ep;θ). 169,171,173,175,177Lu deduced isobaric analog resonances, p-width, level-width. Lu-Yb deduced Coulomb displacement energies. 174Yb(d, p), E=12.0 MeV; measured σ(90°). 175Yb deduced levels, J, π, S. Enriched targets.

doi: 10.1016/0375-9474(70)90231-9
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1968DI04      Phys.Rev. 168, 1169 (1968)

F.S.Dietrich, M.Suffert, A.V.Nero, S.S.Hanna

Gamma Decay of the Lowest T = 3/2 State of 13N

NUCLEAR STRUCTURE 12C, 13N; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.168.1169
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1967AD05      Phys.Letters 25B, 595 (1967)

E.G.Adelberger, A.B.McDonald, T.A.Tombrello, F.S.Dietrich, A.V.Nero

A Lower Limit on the Mass of 5Be

doi: 10.1016/0370-2693(67)90125-6
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1966ZA01      Nucl.Phys. 77, 81(1966); Erratum Nucl.Phys. 89, 706(1966)

C.D.Zafiratos, F.Ajzenberg-Selove, F.S.Dietrich

The 10B(3He, N)12N Reaction

ATOMIC MASSES 12N; measured.

NUCLEAR REACTIONS 10B(3He, n), E = 2.6, 3.0, 4.0, 5.8 MeV; measured σ(En, θ), Q. 12N deduced levels, level-width.

doi: 10.1016/0029-5582(66)90678-X
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0406.


1965DI03      Nucl.Phys. 69, 49 (1965)

F.S.Dietrich

A Study of the Li7(He3, n)B9 Reaction by Time-of-Flight Techniques

NUCLEAR REACTIONS 7Li(3He, n), E = 5.2 to 12.5 MeV; measured σ(En, θ), Q, level-width. 9B; deduced levels, isobaric spin.

doi: 10.1016/0029-5582(65)90501-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1421.


1965ZA01      Phys.Rev. 137, B1479 (1965)

C.D.Zafiratos, F.Ajzenberg-Selove, F.S.Dietrich

N14(He3, n)F16 Reaction

NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.137.B1479
Citations: PlumX Metrics


1964ZA01      Bull.Am.Phys.Soc. 9, No.1, 56, FA9 (1964)

C.D.Zafiratos, F.Ajzenberg-Selove, F.S.Dietrich

B10(He3, n)N12 Reaction

NUCLEAR STRUCTURE 10B; measured not abstracted; deduced nuclear properties.


1964ZA05      Bull.Am.Phys.Soc. 9, No.7, 705, B12 (1964)

C.D.Zafiratos, F.Ajzenberg-Selove, F.S.Dietrich

N14(He3, n)F16 Reaction

NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.


1963DI02      Bull.Am.Phys.Soc. 8, No.2, 120, M5 (1963)

F.S.Dietrich, J.L.Honsaker, J.W.Davies

Neutron Time-of-Flight Investigation of Levels in B8 and B9

NUCLEAR STRUCTURE 6Li; measured not abstracted; deduced nuclear properties.


1963DI19      Bull.Am.Phys.Soc. 8, No.8, 598, F6 (1963)

F.S.Dietrich, J.W.Davies

B9 Levels from the Li7(He3, n) Reaction

NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.


1961AJ03      Phys.Rev. 124, 1548 (1961)

F.Ajzenberg-Selove, L.Cranberg, F.S.Dietrich

Energy Levels of Na21 and Mg22

NUCLEAR STRUCTURE 22Mg, 20Ne, 21Na, 23Na; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.124.1548
Citations: PlumX Metrics


1960AJ05      Bull.Am.Phys.Soc. 5, No.7, 493, C2 (1960)

F.Ajzenberg-Selove, L.Cranberg, F.S.Dietrich

Energy Levels of Na21 and Mg22

NUCLEAR STRUCTURE 22Mg, 21Na; measured not abstracted; deduced nuclear properties.


1960DI02      Bull.Am.Phys.Soc. 5, No.7, 493, C1 (1960)

F.S.Dietrich, L.Cranberg

Level Structure of Be8 from Li7(d, n)Be8

NUCLEAR STRUCTURE 8Be; measured not abstracted; deduced nuclear properties.


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