NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = R.E.Pywell Found 41 matches. 2022LI18 Phys.Rev.Lett. 128, 132502 (2022) X.Li, M.W.Ahmed, A.Banu, C.Bartram, B.Crowe, E.J.Downie, M.Emamian, G.Feldman, H.Gao, D.Godagama, H.W.Griesshammer, C.R.Howell, H.J.Karwowski, D.P.Kendellen, M.A.Kovash, K.K.H.Leung, D.M.Markoff, J.A.McGovern, S.Mikhailov, R.E.Pywell, M.H.Sikora, J.A.Silano, R.S.Sosa, M.C.Spraker, G.Swift, P.Wallace, H.R.Weller, C.S.Whisnant, Y.K.Wu, Z.W.Zhao Proton Compton Scattering from Linearly Polarized Gamma Rays NUCLEAR REACTIONS 1H(polarized γ, γ'), E=83.4 MeV; measured reaction products, Eγ, Iγ; deduced σ(θ), electromagnetic dipole polarizabilities of the proton. The High Intensity Gamma-Ray Source facility at the Triangle Universities Nuclear Laboratory.
doi: 10.1103/PhysRevLett.128.132502
2020LI10 Phys.Rev. C 101, 034618 (2020) X.Li, M.W.Ahmed, A.Banu, C.Bartram, B.Crowe, E.J.Downie, M.Emamian, G.Feldman, H.Gao, D.Godagama, H.W.Griesshammer, C.R.Howell, H.J.Karwowski, D.P.Kendellen, M.A.Kovash, K.K.H.Leung, D.Markoff, S.Mikhailov, R.E.Pywell, M.H.Sikora, J.A.Silano, R.S.Sosa, M.C.Spraker, G.Swift, P.Wallace, H.R.Weller, C.S.Whisnant, Y.K.Wu, Z.W.Zhao Compton scattering from 4He at the TUNL HIγS facility NUCLEAR REACTIONS 4He(polarized γ, γ), E=81.3 MeV, 100% circularly and linearly polarized γ-ray beam via Compton backscattering from HiγS at TUNL; measured Compton scattered photons at different angles, time-of-flight spectra using an array of large NaI(Tl) detectors; deduced differential σ(θ). Comparison with previous experimental data from Lund at Eγ=87 MeV.
doi: 10.1103/PhysRevC.101.034618
2017SI26 Phys.Rev. C 96, 055209 (2017) M.H.Sikora, M.W.Ahmed, A.Banu, C.Bartram, B.Crowe, E.J.Downie, G.Feldman, H.Gao, H.W.Griesshammer, H.Hao, C.R.Howell, H.J.Karwowski, D.P.Kendellen, M.A.Kovash, X.Li, D.M.Markoff, S.Mikhailov, V.Popov, R.E.Pywell, J.A.Silano, M.C.Spraker, P.Wallace, H.R.Weller, C.S.Whisnant, Y.K.Wu, W.Xiong, X.Yan, Z.W.Zhao Compton scattering from 4He at 61 MeV NUCLEAR REACTIONS 4He(γ, γ'), E=61 MeV; measured Eγ, Iγ, Compton scattering differential σ(θ) using NaI(Tl) detectors and liquid 4He target at HIγS facility at TUNL. Data interpreted using phenomenological model sensitive to the dipole isoscalar electromagnetic polarizabilities of the nucleon. Comparison with previous experimental data. Benchmarks for future calculations from effective field theories and lattice quantum chromodynamics.
doi: 10.1103/PhysRevC.96.055209
2015WU05 Phys.Rev. C 92, 044603 (2015) W.A.Wurtz, R.E.Pywell, B.E.Norum, S.Kucuker, B.D.Sawatzky, H.R.Weller, S.Stave, M.W.Ahmed Photodisintegration of 7Li with progeny nuclei in excited states NUCLEAR REACTIONS 7Li(polarized γ, n)6Li, Eγ=13, 15 MeV, E(6Li) at 2.19, 3.56 MeV; 7Li(polarized γ, d)5He, Eγ=12, 13, 15 MeV, E(5He) at 1.27 MeV decays to n+α; measured neutron kinetic energy spectra, absolute cross sections and angular dependences using the Blowfish Neutron Detector Array. Photon beams from High Intensity Gamma-Ray Source (HIGS) at Duke University.
doi: 10.1103/PhysRevC.92.044603
2014WU05 Phys.Rev. C 90, 014613 (2014) W.A.Wurtz, R.E.Pywell, B.E.Norum, S.Kucuker, B.D.Sawatzky, H.R.Weller, S.Stave, M.W.Ahmed Photodisintegration of 6Li NUCLEAR REACTIONS 6Li(polarized γ, p), (polarized γ, n), E=8, 9, 10, 11, 12, 13, 15, 15.6 MeV linearly polarized photons, and E=20, 25, 30, 35 MeV circularly polarized photons; measured En, In, time of flight spectra, σ(E) for (γ, n0), (γ, n1), (γ, n2), (γ, n3), (γ, p1), (γ, p2) and (γ, p3) reaction channels using HIγS facility at TUNL. Legendre function parametrizations, and GEANT4 simulation. Comparison with predictions of Lorentz integral transform calculation using AV4, MN, and MTI-III models.
doi: 10.1103/PhysRevC.90.014613
2011WU06 Phys.Rev. C 84, 044601 (2011) W.A.Wurtz, R.E.Pywell, B.E.Norum, S.Kucuker, B.D.Sawatzky, H.R.Weller, M.W.Ahmed, S.Stave Measurement of the absolute and differential cross sections for 7Li(γ, n0)6Li NUCLEAR REACTIONS 7Li(γ, n), E=10, 11, 12, 13, 15, 20, 25, 30, 35 MeV; 7Li(polarized γ, n), E=10-15 MeV; measured E(n), I(n), TOF spectra using High Intensity Gamma-Ray Source (HIGS); deduced absolute and differential cross sections, yields, associated Legendre polynomial expansion coefficients for 7Li(γ, n)6Li(g.s.) reaction channel.
doi: 10.1103/PhysRevC.84.044601
2008BA24 Phys.Rev. C 77, 064601 (2008) M.G.Barnett, R.Igarashi, R.E.Pywell, J.C.Bergstrom Near threshold (γ, π0) reactions for 4He and 12C NUCLEAR REACTIONS 4He(γ, π0), E=141-159 MeV; measured σ, angular distributions; deduced reduced isovector amplitudes. 12C(γ, π0); analyzed σ, deduced reduced isovector amplitudes.
doi: 10.1103/PhysRevC.77.064601
2008BL14 Phys.Rev. C 78, 034003 (2008); Publishers Note Phys.Rev. C 78, 069905 (2008) M.A.Blackston, M.A.Ahmed, B.A.Perdue, H.R.Weller, B.Bewer, R.E.Pywell, W.A.Wurtz, R.Igarashi, S.Kucuker, B.Norum, K.Wang, J.Li, S.F.Mikhailov, V.G.Popov, Y.K.Wu, B.D.Sawatzky First observation of the splittings of the E1 p-wave amplitudes in low energy deuteron photodisintegration and its implications for the Gerasimov-Drell-Hearn Sum Rule integrand NUCLEAR REACTIONS 2H(polarized γ, n), E=14, 16 MeV; measured σ, σ(θ), linear analyzing power, phase shifts.
doi: 10.1103/PhysRevC.78.034003
2001GA65 Phys.Rev. C64, 064602 (2001) K.R.Garrow, F.Adimi, N.R.Kolb, J.Lu, R.E.Pywell, D.M.Skopik, J.M.Vogt, J.W.Jury, A.Kuzin, M.N.Thompson, J.Ryckebusch High Resolution Measurement of the 18O(γ, pn)14N0, 1, 2, ... Reaction NUCLEAR REACTIONS 16O(γ, np), E=98.5-141.0 MeV; measured Ep, En, np-coin, angular correlations, σ(E, θ); deduced reaction mechanism features. Comparison with model predictions.
doi: 10.1103/PhysRevC.64.064602
2001WA24 Phys.Rev. C64, 014603 (2001) B.J.Warkentin, D.L.Hornidge, R.Igarashi, J.C.Bergstrom, E.L.Hallin, N.R.Kolb, R.E.Pywell, D.M.Skopik, J.M.Vogt, G.Feldman Nuclear Compton Scattering from 12C and Bound-Nucleon Polarizabilities NUCLEAR REACTIONS 12C(γ, γ), (γ, γ'), E=84-105 MeV; measured Eγ, Iγ, σ(θ); deduced approximate bound nucleon polarizabilities. Tagged photon beam.
doi: 10.1103/PhysRevC.64.014603
2000HO02 Phys.Rev.Lett. 84, 2334 (2000) D.L.Hornidge, B.J.Warkentin, R.Igarashi, J.C.Bergstrom, E.L.Hallin, N.R.Kolb, R.E.Pywell, D.M.Skopik, J.M.Vogt, G.Feldman Elastic Compton Scattering from the Deuteron and Nucleon Polarizabilities NUCLEAR REACTIONS 2H(γ, γ), E=84-105 MeV; measured Eγ, Iγ, σ(θ). 1n, 1H deduced polarizabilities. Tagged photons, large-volume NaI spectrometer.
doi: 10.1103/PhysRevLett.84.2334
2000KO36 Phys.Rev.Lett. 85, 1388 (2000) N.R.Kolb, A.W.Rauf, R.Igarashi, D.L.Hornidge, R.E.Pywell, B.J.Warkentin, E.Korkmaz, G.Feldman, G.V.O'Rielly Quasifree Compton Scattering from the Deuteron and Nucleon Polarizabilities NUCLEAR REACTIONS 2H(γ, nγ), E=236-260 MeV bremsstrahlung; measured Eγ, Iγ, σ(θ). 1H, 1n deduced polarizabilities in deuteron bound state.
doi: 10.1103/PhysRevLett.85.1388
2000RI10 Phys.Rev. C61, 064612 (2000) B.J.Rice, R.S.Canon, E.A.Wulf, H.R.Weller, K.Keeter, N.R.Kolb, C.Mueller, R.E.Pywell, G.A.Retzlaff, D.M.Skopik, G.Feldman Two-Deuteron Photodisintegration of 4He at Eγ = 150-250 MeV NUCLEAR REACTIONS 4He(γ, d), E=150-250 MeV; measured deuteron spectra, σ(θ), σ, dd-coin; deduced reaction mechanism features. Transition matrix element analysis, direct capture calculation.
doi: 10.1103/PhysRevC.61.064612
2000SA09 Phys.Rev. C61, 034604 (2000) J.C.Sanabria, B.L.Berman, C.Cetina, P.L.Cole, G.Feldman, N.R.Kolb, R.E.Pywell, J.M.Vogt, V.G.Nedorezov, A.S.Sudov, Ya.Kezerashvili Photofission of Actinide Nuclei in the Quasideuteron and Lower Part of the Δ Energy Region NUCLEAR REACTIONS 232Th, 233,235,238U, 237Np(γ, F), E=68-264 MeV; measured photofission σ. 232Th, 233,235,238U, 237Np deduced relative fissility. Tagged photons, comparisons with previous results.
doi: 10.1103/PhysRevC.61.034604
1999BE79 Nucl.Phys. (Supplement) A654, 837c (1999) B.L.Berman, C.Cetina, P.L.Cole, W.R.Dodge, G.Feldman, J.C.Sanabria, N.Kolb, R.E.Pywell, J.Vogt, V.Nedorezov, A.Sudov, G.Ya.Kezerashvili Photofission of Actinide and Pre-Actinide Nuclei in the Quasideuteron and Delta Energy Regions NUCLEAR REACTIONS Pb, 197Au(γ, F), E=122-222 MeV; measured fission σ. 232Th, 233,235,238U, 237Np(γ, F), E=64-264 MeV; measured fission σ; deduced relative fissilities. Tagged photon beams.
doi: 10.1016/S0375-9474(00)88557-7
1999KO43 Phys.Rev.Lett. 83, 3609 (1999) E.Korkmaz, N.R.Kolb, D.A.Hutcheon, G.V.O'Rielly, J.C.Bergstrom, G.Feldman, D.Jordan, A.K.Opper, R.E.Pywell, B.Sawatzky, D.M.Skopik Measurement of thr γp → π+n Reaction Near Threshold NUCLEAR REACTIONS 1H(γ, π+), E=152-154 MeV; measured σ(θ), neutron yields; deduced electric dipole amplitude. Comparison with chiral perturbation theory.
doi: 10.1103/PhysRevLett.83.3609
1998BE22 Phys.Rev. C57, 3203 (1998) J.C.Bergstrom, R.Igarashi, J.M.Vogt, N.Kolb, R.E.Pywell, D.M.Skopik, E.Korkmaz Measurement of the 2H(γ, π0) Reaction Near Threshold NUCLEAR REACTIONS 2H(γ, π0), E ≈ threshold; measured σ(E), σ(E, θ); deduced nuclear S-wave, P-wave amplitudes.
doi: 10.1103/PhysRevC.57.3203
1998QU01 Phys.Rev. C57, 2118 (1998) M.A.Quraan, E.D.Hackett, E.Korkmaz, W.J.McDonald, A.K.Opper, N.L.Rodning, G.Feldman, N.R.Kolb, G.V.O'Rielly, R.E.Pywell, D.M.Skopik Final State Interactions in 2H(γ, ppπ-) Near the Δ(1232) Resonance NUCLEAR REACTIONS 2H(γ, 2pπ-), E=220-280 MeV; measured σ(φ(π)), σ(θ(π)), σ(Eγ), σ(θ(Δ)); deduced final state interactions, Δ-resonance role.
doi: 10.1103/PhysRevC.57.2118
1996FE07 Phys.Rev. C54, R2124 (1996) G.Feldman, K.E.Mellendorf, R.A.Eisenstein, F.J.Federspiel, G.Garino, R.Igarashi, N.R.Kolb, M.A.Lucas, B.E.MacGibbon, W.K.Mize, A.M.Nathan, R.E.Pywell, D.P.Wells Compton Scattering, Meson Exchange, and the Polarizabilities of Bound Nucleons NUCLEAR REACTIONS 16O(γ, γ), E=27-108 MeV; measured Eγ, Iγ, σ(θ) vs E; deduced bound-nucleon polarizability, meson-exchange contribution.
doi: 10.1103/PhysRevC.54.R2124
1996HA03 Phys.Rev. C53, R1047 (1996) E.D.Hackett, W.J.McDonald, A.K.Opper, M.A.Quraan, N.L.Rodning, F.M.Rozon, G.Feldman, N.R.Kolb, R.E.Pywell, D.M.Skopik, D.E.Tiller, J.M.Vogt, E.Korkmaz, G.V.O'Rielly Reaction Mechanisms in 12C(γ, pp) Near 200 MeV NUCLEAR REACTIONS 12C(γ, 2pX), E=187-227 MeV; measured inclusive differential σ. Monte Carlo intranuclear cascade calculation.
doi: 10.1103/PhysRevC.53.R1047
1996KO45 Phys.Rev. C54, 2175 (1996) N.R.Kolb, G.Feldman, G.V.O'Rielly, R.E.Pywell, D.M.Skopik, E.D.Hackett, M.A.Quraan, N.L.Rodning 3He(γ, pp)n Cross Sections with Tagged Photons Below the Δ Resonance Energy NUCLEAR REACTIONS 3He(γ, 2p), E=161-208 MeV; measured absolute σ(θ(pp), φ(pp)). Tagged photons. Model comparison.
doi: 10.1103/PhysRevC.54.2175
1994KO11 Phys.Rev. C49, 2586 (1994) N.R.Kolb, E.B.Cairns, E.D.Hackett, E.Korkmaz, T.Nakano, A.K.Opper, M.A.Quraan, N.L.Rodning, F.M.Rozon, J.Asai, G.Feldman, E.Hallin, G.V.O'Rielly, R.E.Pywell, D.M.Skopik 3He(γ, pd) Cross Sections with Tagged Photons Below the Δ Resonance NUCLEAR REACTIONS 3He(γ, pd), E=166-213 MeV; measured σ(θ). Tagged photons.
doi: 10.1103/PhysRevC.49.2586
1993SA03 Phys.Rev. C47, 459 (1993) A.J.Sarty, K.G.R.Doss, G.Feldman, E.L.Hallin, R.E.Pywell, G.A.Retzlaff, D.M.Skopik, H.R.Weller, W.R.Dodge, J.W.Lightbody, Jr., J.S.O'Connell, C.C.Chang Measurement of the Reaction 3He(γ, pp)n and Its Relation to Three-Body Forces NUCLEAR REACTIONS 3He(γ, 2p), E=90-250 MeV bremsstrahlung; measured σ(θn, θp) vs neutron momentum; deduced two-pion-exchange, three-body absorption mechanisms role.
doi: 10.1103/PhysRevC.47.459
1992CA30 Nucl.Instrum.Methods Phys.Res. A321, 109 (1992) E.B.Cairns, J.Cameron, C.Choi, H.W.Fielding, P.W.Green, L.G.Greeniaus, E.D.Hackett, L.Holm, N.R.Kolb, E.Korkmaz, P.P.Langill, W.J.McDonald, D.Mack, W.C.Olsen, B.A.Peterson, N.L.Rodning, J.Soukup, J.Zhu, D.Hutcheon, H.S.Caplan, R.E.Pywell, D.M.Skopik, J.M.Vogt, I.J.van Heerden The Saskatchewan-Alberta Large Acceptance Detector for Photonuclear Physics NUCLEAR REACTIONS 1H(p, p), E=220 MeV; measured σ(θ). 4π large acceptance detector.
doi: 10.1016/0168-9002(92)90380-M
1992ZU01 Phys.Rev. C45, 174 (1992); Erratum Phys.Rev. C46, 1147 (1992) D.Zubanov, M.N.Thompson, B.L.Berman, J.W.Jury, R.E.Pywell, K.G.McNeill Giant Dipole Resonance in 17O Observed with the (γ, p) Reaction NUCLEAR REACTIONS, ICPND 17O(γ, p), (γ, X), E=13.5-43.15 MeV; measured reaction yields; deduced σ(γ, p), σ. 17O deduced resonances, J, π, Γ, GDR. Activation technique.
doi: 10.1103/PhysRevC.45.174
1991MC01 Phys.Rev. C43, 489 (1991) K.G.McNeill, J.W.Jury, M.N.Thompson, B.L.Berman, R.E.Pywell 18O(γ, pn+np) Cross Section NUCLEAR REACTIONS 18O(γ, xnyp), E=19-43 MeV; measured two-nucleon production σ(E); deduced channel effect on total photoabsorption σ. Enriched target.
doi: 10.1103/PhysRevC.43.489
1987BE37 Phys.Rev. C36, 1286 (1987) B.L.Berman, R.E.Pywell, S.S.Dietrich, M.N.Thompson, K.G.McNeill, J.W.Jury Absolute Photoneutron Cross Sections for Zr, I, Pr, Au, and Pb NUCLEAR REACTIONS Zr, 127I, 141Pr, 197Au, Pb(γ, n), E ≈ 12-17 MeV; Zr, 127I, 141Pr, 197Au, Pb(γ, 2n), E=threshold-17 MeV; measured absolute photonucleon σ(E).
doi: 10.1103/PhysRevC.36.1286
1987MC04 Phys.Rev. C36, 1621 (1987) K.G.McNeill, R.E.Pywell, B.L.Berman, J.G.Woodworth, M.N.Thompson, J.W.Jury Photoneutron Cross Section for 29Si NUCLEAR REACTIONS 29Si(γ, n), E=9.4-18.3 MeV; measured σ(E).
doi: 10.1103/PhysRevC.36.1621
1987OK04 Nucl.Phys. A469, 239 (1987) G.J.O'Keefe, M.N.Thompson, Y.I.Assafiri, R.E.Pywell, K.Shoda The Photonuclear Cross Sections of 48Ca NUCLEAR REACTIONS 48Ca(γ, np), E=12-26 MeV bremsstrahlung; measured neutron + proton yield. Activation technique. Natural target. 48Ca(e, p), E=15-29 MeV; measured proton yield; deduced particle σ(γ, p). 48Ca deduced GDR isospin splitting. Enriched target.
doi: 10.1016/0375-9474(87)90108-4
1985PY01 Phys.Rev. C32, 384 (1985) R.E.Pywell, B.L.Berman, J.G.Woodworth, J.W.Jury, K.G.McNeill, M.N.Thompson Photoneutron Cross Sections for 14C NUCLEAR REACTIONS 14C(γ, n), (γ, 2n), E=8.2-36 MeV; measured neutron yields, integrated σ. 14C deduced GDR, decay characteristics.
doi: 10.1103/PhysRevC.32.384
1983BE01 Phys.Rev. C27, 1 (1983) B.L.Berman, J.W.Jury, J.G.Woodworth, R.E.Pywell, K.G.McNeill, M.N.Thompson Photoneutron Cross Section for 16O NUCLEAR REACTIONS 16O(γ, n), E=17-33 MeV bremsstrahlung; measured σ(photoproduction) vs E; deduced (γ, n0) dominance. Monoenergetic beam.
doi: 10.1103/PhysRevC.27.1
1983GR03 Lett.Nuovo Cim. 36, 221 (1983) L.H.Greenberg, D.Y.Kim, S.I.H.Naqvi, R.E.Pywell Evidence for the Existence of a Low-Mass Pseudoscalar Meson NUCLEAR REACTIONS 24Mg(e, e'), E=11.5 MeV; measured phion production σ. Activation technique.
doi: 10.1007/BF02719454
1983PY01 Phys.Rev. C27, 960 (1983) R.E.Pywell, B.L.Berman, J.W.Jury, J.G.Woodworth, K.G.McNeill, M.N.Thompson Photoneutron Cross Sections for the Silicon Isotopes NUCLEAR REACTIONS 28,29Si(γ, n), 30Si(γ, n), (γ, 2n), E=13.4-33.1 MeV; measured σ(E). 28,29,30Si deduced GDR fragmentation characteristics.
doi: 10.1103/PhysRevC.27.960
1983SK01 Phys.Rev. C28, 52 (1983) D.M.Skopik, J.Asai, D.H.Beck, T.P.Dielschneider, R.E.Pywell, G.A.Retzlaff 3He(e, d)e'p Isochromats and Angular Distribution Measurements NUCLEAR REACTIONS 3He(e, e'd), E ≈ 15-60 MeV; measured σ(θd, Ed, E); deduced σ(Ed, E), relative E1, E2 contribution to deuteron photoproduction σ. Virtual photon spectrum analysis.
doi: 10.1103/PhysRevC.28.52
1982JU03 Phys.Rev. C26, 777 (1982) J.W.Jury, B.L.Berman, J.G.Woodworth, M.N.Thompson, R.E.Pywell, K.G.McNeill Photoneutron Cross Sections for 15N NUCLEAR REACTIONS 15N(γ, n), (γ, 2n), E=10.8-38 MeV; measured σ(E), total σ(photoproduction). 15N deduced resonances, decay characteristics.
doi: 10.1103/PhysRevC.26.777
1982OD01 Nucl.Phys. A388, 445 (1982) G.Odgers, B.L.Berman, R.E.Pywell, M.N.Thompson Photoneutron Cross Section for 30Si NUCLEAR REACTIONS 30Si(γ, xn), E ≈ 10-28 MeV bremsstrahlung; measured neutron yield; deduced σ(E). 30Si deduced GDR fragmentation.
doi: 10.1016/0375-9474(82)90470-5
1981PY01 Nucl.Phys. A369, 141 (1981) R.E.Pywell, B.L.Berman, P.Kean, M.N.Thompson Photoneutron Cross Section of 29Si NUCLEAR REACTIONS 29Si(γ, xn), E ≈ 8-28 MeV bremsstrahlung; measured neutron yield; deduced σ(E). 29Si deduced GDR, pygmy resonance. Enriched target, 4π counter.
doi: 10.1016/0375-9474(81)90011-7
1980PY01 Nucl.Instrum.Methods 178, 149 (1980) R.E.Pywell, M.N.Thompson, B.L.Berman A Measurement of the 18O Photonuclear Cross Sections as a Test of a Bremsstrahlung Unfolding Technique NUCLEAR REACTIONS 18O(γ, n), (γ, 2n), (γ, p), E=8-28 MeV bremsstrahlung; measured σ(E). Enriched target, variable bin Penfold-Leiss bremmsstrahlung yield curve unfolding technique, BF3 neutron detectors, pulsed X-ray photon source.
doi: 10.1016/0029-554X(80)90869-1
1980PY02 Aust.J.Phys. 33, 685 (1980) R.E.Pywell, M.N.Thompson, K.Shoda, M.Sugawara, T.Saito, H.Tsubota, H.Miyase, J.Uegaki, T.Tamae, H.Ohashi, T.Urano Charged Particle Photoemission from 42Ca NUCLEAR REACTIONS 42Ca(γ, p), (γ, α), E=16-28 MeV; measured σ(θ, E). 42Ca deduced T=2, GDR.
doi: 10.1071/PH800685
1979PY02 Nucl.Phys. A318, 461 (1979) Isospin Splitting in the Giant Dipole Resonance in 46Ti NUCLEAR REACTIONS 46Ti(γ, n), E=12-25 MeV; measured σ. 46Ti deduced possibility of deformation splitting of GDR.
doi: 10.1016/0375-9474(79)90660-2
1979PY03 Nucl.Phys. A325, 116 (1979) R.E.Pywell, M.N.Thompson, R.A.Hicks A Measurement of the 50Ti(γ, n) and 50Ti(γ, n0) Cross Sections NUCLEAR REACTIONS 50Ti(γ, n), E=threshold-28 MeV bremsstrahlung; measured yield curves; 50Ti(γ, n0), E=15.5-26 MeV bremsstrahlung; measured neutron spectra; deduced σ. Stilbene detector. Enriched target.
doi: 10.1016/0375-9474(79)90156-8
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