NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = F.Dietrich Found 108 matches. Showing 1 to 100. [Next]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
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
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
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
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
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
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
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
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
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
2010ES02 Phys.Rev. C 81, 024612 (2010) 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
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
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
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
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
2008DI18 Nucl.Data Sheets 109, 2774 (2008) 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
2007DI12 Nucl.Phys. A787, 237c (2007) 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
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
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
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
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
2006ES03 Phys.Rev. C 74, 054601 (2006) 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
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
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
2005ES07 Nucl.Phys. A758, 86c (2005) J.Escher, L.Ahle, L.Bernstein, J.A.Church, F.Dietrich, C.Forssen, R.Hoffman Surrogate Nuclear Reactions and the origin of the heavy elements
doi: 10.1016/j.nuclphysa.2005.05.167
2005ES08 J.Phys.(London) G31, S1687 (2005) J.Escher, L.Ahle, L.Bernstein, J.Burke, J.A.Church, F.Dietrich, C.Forssen, V.Gueorguiev, R.Hoffman Surrogate nuclear reactions: an indirect method for determining reaction cross sections
doi: 10.1088/0954-3899/31/10/054
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
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
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
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
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
1998CO19 J.Phys.(London) G24, 1547 (1998) M.D.Cortina-Gil, A.Pakou, N.Alamanos, W.Mittig, P.Roussel-Chomaz, F.Auger, J.Barrette, Y.Blumenfeld, J.M.Casandjian, M.Chartier, F.Dietrich, V.Fekou-Youmbi, B.Fernandez, N.Frascaria, A.Gillibert, H.Laurent, A.Lepine-Szily, N.Orr, V.Pascalon, J.A.Scarpaci, J.L.Sida, T.Suomijarvi Charge-Exchange Reaction with Light Neutron-Rich Beams NUCLEAR REACTIONS 1H(6He, 6Li), E=41.6 MeV/nucleon; measured σ(θ); deduced no halo effect on transition strength. Optical model analysis.
doi: 10.1088/0954-3899/24/8/032
1998CO28 Nucl.Phys. A641, 263 (1998) M.D.Cortina-Gil, A.Pakou, N.Alamanos, W.Mittig, P.Roussel-Chomaz, F.Auger, J.Barrette, Y.Blumenfeld, J.M.Casandjian, M.Chartier, F.Dietrich, V.Fekou-Youmbi, B.Fernandez, N.Frascaria, A.Gillibert, H.Laurent, A.Lepine-Szily, N.Orr, V.Pascalon, J.A.Scarpaci, J.L.Sida, T.Suomijarvi Charge-Exchange Reaction Induced by 6He and Nuclear Densities NUCLEAR REACTIONS 1H(6He, 6Li), E=41.6 MeV/nucleon; measured σ(θ) for transition to ground state, IAS; deduced dependence on interaction potential. 6He deduced density distribution.
doi: 10.1016/S0375-9474(98)00470-9
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 σn/σp 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
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
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
1996AR02 Phys.Rev. C53, 2248 (1996) J.Arrington, P.Anthony, R.G.Arnold, E.J.Beise, J.E.Belz, P.E.Bosted, H.-J.Bulten, M.S.Chapman, K.P.Coulter, F.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.R.Kinney, S.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, K.van Bibber, J.F.J.van den Brand, J.L.White, D.Winter, B.Zeidman Inclusive Electron Scattering from Nuclei at x ≈ 1 NUCLEAR REACTIONS 2H, C, Fe, 197Au(e, e'X), E=2.02-5.12 GeV; measured inclusive σ; deduced scaling behavior.
doi: 10.1103/PhysRevC.53.2248
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
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
1995BE08 Phys.Rev.Lett. 74, 646 (1995) J.E.Belz, D.H.Potterveld, P.Anthony, R.G.Arnold, J.Arrington, D.Beck, E.J.Beise, P.E.Bosted, H.-J.Bulten, M.S.Chapman, K.P.Coulter, F.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.R.Kinney, S.Kuhn, K.Lee, W.Lorenzon, A.Lung, N.C.R.Makins, D.J.Margaziotis, R.D.McKeown, Z.E.Meziani, R.G.Milner, B.Mueller, J.Napolitano, J.Nelson, T.G.O'Neill, V.Papavassiliou, G.G.Petratos, S.E.Rock, R.E.Segel, M.Spengos, Z.M.Szalata, L.H.Tao, K.van Bibber, J.F.L.van den Brand, J.L.White, B.Zeidman Two-Body Photodisintegration of the Deuteron up to 2.8 GeV NUCLEAR REACTIONS 2H(γ, p), E=1.6-2.8 GeV; measured σ(θ) vs E; deduced agreement with constituent counting rules.
doi: 10.1103/PhysRevLett.74.646
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
1995ON02 Phys.Lett. 351B, 87 (1995) T.G.O'Neill, W.Lorenzon, P.Anthony, R.G.Arnold, J.Arrington, E.J.Beise, J.E.Belz, P.E.Bosted, H.-J.Bulten, M.S.Chapman, K.P.Coulter, F.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.R.Kinney, S.Kuhn, K.Lee, A.Lung, N.C.R.Makins, D.J.Margaziotis, R.D.McKeown, R.G.Milner, B.Mueller, J.Napolitano, J.Nelson, V.Papavassiliou, G.G.Petratos, D.H.Potterveld, S.E.Rock, M.Spengos, Z.M.Szalata, L.H.Tao, K.van Bibber, J.F.J.van den Brand, J.L.White, B.Zeidman A-Dependence of Nuclear Transparency in Quasielastic A(e, e'p) at High Q2 NUCLEAR REACTIONS 2H, C, Fe, 197Au(e, e'p), E=2-5.12 GeV; measured transparency vs target mass; deduced no color transparency evidence.
doi: 10.1016/0370-2693(95)00362-O
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
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
1994DA34 Phys.Rev. D49, 5641 (1994) S.Dasu, P.de Barbaro, A.Bodek, H.Harada, M.W.Krasny, K.Lang, E.M.Riordan, L.Andivahis, R.Arnold, D.Benton, P.Bosted, G.deChambrier, A.Lung, S.E.Rock, Z.M.Szalata, R.C.Walker, B.W.Filippone, J.Jourdan, R.Milner, R.McKeown, D.Potterveld, A.Para, F.Dietrich, K.Van Bibber, J.Button-Shafer, B.Debebe, R.S.Hicks, R.Gearhart, L.W.Whitlow, J.Alster Measurement of Kinematic and Nuclear Dependence of R = σ(L)/σ(T) in Deep Inelastic Electron Scattering NUCLEAR REACTIONS 1,2H, Fe, 197Au(e, e'X), E=high; measured σ(longitudinal)/σ(transverse), deep inelastic scattering; deduced nuclear, nucleon higher twist effects role comparison.
doi: 10.1103/PhysRevD.49.5641
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
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
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
1994WA32 Phys.Rev. D49, 5671 (1994) R.C.Walker, B.W.Filippone, J.Jourdan, R.Milner, R.McKeown, D.Potterveld, L.Andivahis, R.Arnold, D.Benton, P.Bosted, G.deChambrier, A.Lung, S.E.Rock, Z.M.Szalata, A.Para, F.Dietrich, K.Van Bibber, J.Button-Shafer, B.Debebe, R.S.Hicks, S.Dasu, P.De Barbaro, A.Bodek, H.Harada, M.W.Krasny, K.Lang, E.M.Riordan, R.Gearhart, L.W.Whitlow, J.Alster Measurements of the Proton Elastic Form Factors for 1 ≤ Q2 ≤ 3 (GeV/c)2 at SLAC NUCLEAR REACTIONS 1H(e, e), E=0.5-9 GeV; measured σ(θ). 1H deduced form factors G(p)(E), G(p)(M).
doi: 10.1103/PhysRevD.49.5671
1993AN04 Nucl.Phys. A553, 713c (1993) L.Andivahis, P.Bosted, A.Lung, L.Stuart, J.Alster, R.Arnold, C.Chang, F.Dietrich, W.Dodge, R.Gearhart, J.Gomez, K.Griffioen, R.Hicks, C.Hyde-Wright, C.Keppel, S.Kuhn, J.Lichtenstadt, R.Miskimen, G.Peterson, G.Petratos, S.Rock, S.Rokni, W.Sakumoto, M.Spengos, K.Swartz, Z.Szalata, L.Tao Measurements of the Nucleon Form Factors at Large Momentum Transfers NUCLEAR REACTIONS 2,1H(e, e), E=1.5-9.8 GeV; measured σ(θ, E). 1H, 1n deduced form factors.
doi: 10.1016/0375-9474(93)90686-R
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
1993FR05 Phys.Rev. C47, 1599 (1993) M.Frodyma, R.G.Arnold, D.Benton, P.E.Bosted, L.Clogher, G.Dechambrier, A.T.Katramatou, J.Lambert, A.Lung, G.G.Petratos, A.Rahbar, S.E.Rock, Z.M.Szalata, B.Debebe, R.S.Hicks, A.Hotta, G.A.Peterson, R.A.Gearhart, J.Alster, J.Lichtenstadt, F.Dietrich, K.van Bibber Measurements of Transverse Electron Scattering from the Deuteron in the Threshold Region at High Momentum Transfers NUCLEAR REACTIONS 2H(e, e'X), E=0.734-1.279 GeV; measured σ(θ, E(np)); deduced inelastic structure function ratio. Model comparison.
doi: 10.1103/PhysRevC.47.1599
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
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
1991BO21 Nucl.Phys. A527, 339c (1991) P.E.Bosted, L.Clogher, A.Lung, L.Stuart, J.Alster, R.G.Arnold, C.C.Chang, F.Dietrich, W.R.Dodge, R.Gearhart, J.Gomez, K.Griffioen, R.Hicks, C.Hyde-Wright, C.Keppel, S.Kuhn, J.Lichtenstadt, R.Miskimen, G.G.Petratos, G.A.Peterson, S.E.Rock, S.H.Rokni, W.K.Sakumoto, K.Swartz, Z.N.Szalata, L.H.Tao New Measurements of the Electric and Magnetic Elastic Form Factors of the Proton and Neutron at High Momentum Transfers NUCLEAR REACTIONS 1H(e, e'), E=1.4-10 GeV; measured electron spectra. 1H deduced magnetic form factor.
doi: 10.1016/0375-9474(91)90123-N
1990AR09 Phys.Rev. C42, R1 (1990) R.G.Arnold, D.Benton, P.E.Bosted, L.Clogher, G.deChambrier, A.T.Katramatou, J.Lambert, A.Lung, G.G.Petratos, A.Rahbar, S.E.Rock, Z.M.Szalata, B.Debebe, M.B.Frodyma, R.S.Hicks, A.Hotta, G.A.Peterson, R.A.Gearhart, J.Alster, J.Lichtenstadt, F.Dietrich, K.van Bibber Transverse Electrodisintegration of the Deuteron in the Threshold Region at High Q2 NUCLEAR REACTIONS 2H(e, np), E=0.73-1.3 GeV; measured σ(θ) vs E(np), θ=180°; deduced non-nucleonic degrees of freedom role.
doi: 10.1103/PhysRevC.42.R1
1990BO18 Phys.Rev. C42, 38 (1990) P.E.Bosted, A.T.Katramatou, R.G.Arnold, D.Benton, L.Clogher, G.DeChambrier, J.Lambert, A.Lung, G.G.Petratos, A.Rahbar, S.E.Rock, Z.M.Szalata, B.Debebe, M.Frodyma, R.S.Hicks, A.Hotta, G.A.Peterson, R.A.Gearhart, J.Alster, J.Lichtenstadt, F.Dietrich, K.van Bibber Measurements of the Deuteron and Proton Magnetic Form Factors at Large Momentum Transfers NUCLEAR REACTIONS 2H(e, e'), E=0.5-1.3 GeV; measured ed-, ep-coin, form factors. 2H deduced magnetic structure function.
doi: 10.1103/PhysRevC.42.38
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
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
1988AR14 Phys.Rev.Lett. 61, 806 (1988) R.G.Arnold, D.Benton, P.Bosted, L.Clogher, G.DeChambrier, A.T.Katramatou, J.Lambert, A.Lung, G.G.Petratos, A.Rahbar, S.E.Rock, Z.M.Szalata, B.Debebe, M.Frodyma, R.S.Hicks, A.Hotta, G.A.Peterson, R.A.Gearhart, J.Alster, J.Lichtenstadt, F.Dietrich, K.van Bibber Measurements of Transverse Quasielastic Electron Scattering from the Deuteron at High Momentum Transfers NUCLEAR REACTIONS 2H(e, e'), E=0.843-1.281 GeV; measured σ(θ, E(e')); deduced scaling function.
doi: 10.1103/PhysRevLett.61.806
1988DA06 Nucl.Phys. A478, 391c (1988) S.Dasu, P.de Barbaro, R.C.Walker, L.W.Whitlow, J.Alster, R.Arnold, P.Bosted, D.Benton, A.Bodek, J.Button-Shafer, G.de Chambrier, L.Clogher, B.Debebe, F.Dietrich, B.Filippone, R.Gearhart, H.Harada, R.Hicks, J.Jourdan, M.W.Krasny, K.Lang, A.Lung, R.Milner, R.McKeown, A.Para, D.Potterveld, E.M.Riordan, S.E.Rock, Z.M.Szalata, K.Van Bibber A Study of the Nuclear and Kinematic Dependence of R = σ(L)/σ(T) in Deep Inelastic Electron Scattering NUCLEAR REACTIONS 2H, Fe, 197Au(e, e'), E not given; measured longitudinal to transverse σ ratio.
doi: 10.1016/0375-9474(88)90869-X
1988DA10 Phys.Rev.Lett. 60, 2591 (1988) S.Dau, P.de Barbaro, A.Bodek, H.Harada, M.W.Krasny, K.Lang, E.M.Riordan, R.Arnold, D.Benton, P.Bosted, L.Clogher, G.deChambrier, A.Lung, S.E.Rock, Z.M.Szalata, R.C.Walker, B.W.Filippone, J.Jourdan, R.Milner, R.McKeown, D.Potterveld, A.Para, F.Dietrich, K.Van Bibber, J.Button-Shafer, B.Debebe, R.S.Hicks, R.Gearhart, L.W.Whitlow, J.Alster Measurement of the Difference in R = σ(L)/σ(T) and of σ(A)/σ(D) in Deep-Inelastic e-D, e-Fe, and e-Au Scattering NUCLEAR REACTIONS 2H, Fe, 197Au(e, e), E=high; measured longitudinal to transverse σ(ratio), σ relative to 2H.
doi: 10.1103/PhysRevLett.60.2591
1987AR09 Phys.Rev.Lett. 58, 1723 (1987) R.G.Arnold, D.Benton, P.Bosted, L.Clogher, G.DeChambrier, A.T.Katramatou, J.Lambert, A.Lung, G.G.Petratos, A.Rahbar, S.E.Rock, Z.M.Szalata, R.A.Gearhart, B.Debebe, M.Frodyma, R.S.Hicks, A.Hotta, G.A.Peterson, J.Alster, J.Lichtenstadt, F.Dietrich, K.van Bibber Deuteron Magnetic Form Factor Measurements of High Momentum Transfer NUCLEAR REACTIONS 2H(e, e), E at 0.41-0.54 GeV/c; measured σ(θ). 2H deduced structure function, magnetic form factor. Liquid deuterium, multi-wire proportional chambers.
doi: 10.1103/PhysRevLett.58.1723
1987DE06 Phys.Rev. C35, 942 (1987) 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
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
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
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
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
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
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
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
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
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
1984HA50 Phys.Rev. C30, 1795 (1984) G.Haouat, Ch.Lagrange, R.de Swiniarski, F.Dietrich, J.P.Delaroche, Y.Patin Nuclear Deformations of 24Mg, 28Si, and 32S from Fast Neutron Scattering NUCLEAR REACTIONS 24Mg, 28Si, 32S(n, n), (n, n'), E=9.76, 14.83 MeV; measured σ(En), σ(θ); deduced optical model parameters. 24Mg, 28Si, 32S deduced deformation parameters β2, β4, deformation lengths. Compound nucleus, coupled-channels model analyses.
doi: 10.1103/PhysRevC.30.1795
1984MA67 Astrophys.J. 287, 969 (1984) 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
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
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
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
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
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
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
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
1979DI06 Phys.Rev.Lett. 43, 114 (1979) 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
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
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
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
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
1974BR38 Phys.Rev. C10, 2545 (1974) 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
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
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
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
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
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
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
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
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
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
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
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
1965DI03 Nucl.Phys. 69, 49 (1965) 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
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