NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = D.R.Tilley Found 123 matches. Showing 1 to 100. [Next]2004PR09 Phys.Rev. C 70, 055801 (2004) R.M.Prior, M.C.Spraker, A.M.Amthor, K.J.Keeter, S.O.Nelson, A.Sabourov, K.Sabourov, A.Tonchev, M.Ahmed, J.H.Kelley, D.R.Tilley, H.R.Weller, H.M.Hofmann Energy dependence of the astrophysical S factor for the 6Li(p, γ)7Be reaction NUCLEAR REACTIONS 6Li(polarized p, γ), E=80, 95, 110, 120, 130 keV; measured Eγ, Iγ, analyzing power; deduced energy dependence of astrophysical S-factor.
doi: 10.1103/PhysRevC.70.055801
2004TI06 Nucl.Phys. A745, 155 (2004) D.R.Tilley, J.H.Kelley, J.L.Godwin, D.J.Millener, J.E.Purcell, C.G.Sheu, H.R.Weller Energy levels of light nuclei A = 8, 9, 10 COMPILATION 8,10n, 8,9,10He, 8,9,10Li, 8,9,10Be, 8,9,10B, 8,9,10C, 9,10N, 10O, 10F, 10Ne; compiled, evaluated structure data.
doi: 10.1016/j.nuclphysa.2004.09.059
2002CA18 Phys.Rev. C65, 044008 (2002) R.S.Canon, S.O.Nelson, K.Sabourov, E.Wulf, H.R.Weller, R.M.Prior, M.Spraker, J.H.Kelley, D.R.Tilley 3H(p(pol), γ)4He Reaction below Ep = 80 keV NUCLEAR REACTIONS 3H(polarized p, γ), E=40, 80 keV; measured σ(θ), Ay(θ); deduced astrophysical S-factors.
doi: 10.1103/PhysRevC.65.044008
2002TI10 Nucl.Phys. A708, 3 (2002) D.R.Tilley, C.M.Cheves, J.L.Godwin, G.M.Hale, H.M.Hofmann, J.H.Kelley, C.G.Sheu, H.R.Weller Energy Levels of Light Nuclei A = 5, 6, 7 COMPILATION 5,6n, 5,6,7H, 5,6,7He, 5,6,7Li, 5,6,7Be, 6,7B, 6C; compiled, evaluated structure data.
doi: 10.1016/S0375-9474(02)00597-3
2001NE15 Phys.Rev. C64, 065804 (2001) C.D.Nesaraja, C.R.Brune, B.T.Crowley, J.H.Kelley, S.O.Nelson, R.M.Prior, K.Sabourov, D.R.Tilley, A.Tonchev, H.R.Weller Ratio of S Factors for (p, γ) Reactions on 12C and 13C at Astrophysically Relevant Energies NUCLEAR REACTIONS 12,13C(p, γ), E < 160 keV; measured σ; deduced S-factor ratio. Comparison with model predictions.
doi: 10.1103/PhysRevC.64.065804
2000KE10 Phys.Rev. C62, 025803 (2000) J.H.Kelley, R.S.Canon, S.J.Gaff, R.M.Prior, B.J.Rice, E.C.Schreiber, M.Spraker, D.R.Tilley, E.A.Wulf, H.R.Weller The 11B(p(pol), γ)12C Reaction below 100 keV NUCLEAR REACTIONS 11B(polarized p, γ), E < 100 keV; measured Eγ, Iγ, σ, Ay(θ=90°); deduced astrophysical S factor, influence of low-lying resonances.
doi: 10.1103/PhysRevC.62.025803
2000SP01 Phys.Rev. C61, 015802 (2000) M.Spraker, R.M.Prior, M.A.Godwin, B.J.Rice, E.A.Wulf, J.H.Kelley, D.R.Tilley, H.R.Weller Slope of the Astrophysical S Factor for the 7Li(p, γ)8Be Reaction NUCLEAR REACTIONS 7Li(polarized p, γ), E=40-100 keV; measured yields, analyzing power; deduced slope of astrophysical S factor, role of subthreshold resonance.
doi: 10.1103/PhysRevC.61.015802
2000WU02 Phys.Rev. C61, 021601 (2000) E.A.Wulf, R.S.Canon, S.J.Gaff, J.H.Kelley, R.M.Prior, E.C.Schreiber, M.Spraker, D.R.Tilley, H.R.Weller, M.Viviani, A.Kievsky, S.Rosati, R.Schiavilla New Photodisintegration Threshold Observable in 3He NUCLEAR REACTIONS 2H(polarized p, γ), 1H(polarized d, γ), E=0-80 keV; measured σ(θ), vector and tensor analyzing powers, γ-ray polarization. 3He deduced matrix elements, sum rule features.
doi: 10.1103/PhysRevC.61.021601
1999GA21 Phys.Rev. C59, 3425 (1999) S.J.Gaff, R.S.Canon, J.H.Kelley, S.O.Nelson, K.Sabourov, E.C.Schreiber, D.R.Tilley, H.R.Weller, E.A.Wulf Spin Parity of the 7.478 MeV State of 10B and the S Factor of the 9Be(p(pol), γ0)10B Reaction NUCLEAR REACTIONS 9Be(polarized p, γ), E=280 keV; measured Ay(θ); deduced ground-state capture S-factor. 10B level deduced J, π.
doi: 10.1103/PhysRevC.59.3425
1998TI06 Nucl.Phys. A636, 249 (1998) D.R.Tilley, C.M.Cheves, J.H.Kelley, S.Raman, H.R.Weller Energy Levels of Light Nuclei, A = 20 COMPILATION 20N, 20O, 20F, 20Ne, 20Na, 20Mg; compiled, evaluated structure data.
doi: 10.1016/S0375-9474(98)00129-8
1998WU05 Phys.Rev. C58, 517 (1998) E.A.Wulf, M.A.Godwin, J.F.Guillemette, C.M.Laymon, R.M.Prior, B.J.Rice, M.Spraker, D.R.Tilley, H.R.Weller Astrophysical S Factors for the 9Be(p(pol), γ)10B Reaction NUCLEAR REACTIONS 9Be(polarized p, γ), E=100 keV; measured Eγ, Iγ, A(y)(θ); deduced astrophysical S-factors. HPGe detector. Direct capture plus resonance calculation.
doi: 10.1103/PhysRevC.58.517
1997GO13 Phys.Rev. C56, 1605 (1997) M.A.Godwin, C.M.Laymon, R.M.Prior, D.R.Tilley, H.R.Weller 7Li(p(pol), γ)8Be Reaction at E(p) = 80-0 keV NUCLEAR REACTIONS, ICPND 7Li(polarized p, γ), E=0-80 keV; measured σ(θ)/A0, A(y)(θ) for capture to ground, first-, third-excited states, total σ, astrophysical S-factor for capture to third-excited state; deduced M1 resonance capture role, implications to M1 capture in 7Be(p, γ) reaction. Direct capture model, other reactions discussed.
doi: 10.1103/PhysRevC.56.1605
1997RI15 Phys.Rev. C56, R2917 (1997) B.J.Rice, E.A.Wulf, R.S.Canon, J.H.Kelley, R.M.Prior, M.Spraker, D.R.Tilley, H.R.Weller Direct Determination of the Doublet and Quartet M1 Cross Sections in p-d Radiative Capture at Near-Thermal Energies NUCLEAR REACTIONS 1H(polarized d, γ), E=80 keV; measured T11(θ); analyzed σ(θ), T20(θ); 2H(polarized p, γ), E=40 keV; analyzed A(y); 2H(p, γ), E=80 keV; analyzed γ-polarization; deduced M1 radiative capture σ, meson exchange currents role.
doi: 10.1103/PhysRevC.56.R2917
1997SC31 Phys.Rev. C56, 2565 (1997) G.J.Schmid, B.J.Rice, R.M.Chasteler, M.A.Godwin, G.C.Kiang, L.L.Kiang, C.M.Laymon, R.M.Prior, D.R.Tilley, H.R.Weller The 2H(p(pol), γ)3He and 1H(d(pol), γ)3He Reactions Below 80 keV NUCLEAR REACTIONS 2H(p, γ), (polarized p, γ), 1H(d, γ), (polarized d, γ), E=10-80 keV; measured Eγ, Iγ, σ(E, θ), vector, tensor analyzing power, astrophysical S-factor, γ polarization; deduced meson exchange current, Δ-isobar effects, astrophysical implications. 3He deduced asymptotic D- to S-state ratio. Three-body calculations. Ice targets.
doi: 10.1103/PhysRevC.56.2565
1996GO01 Phys.Rev. C53, R1 (1996) M.A.Godwin, R.M.Chasteler, C.M.Laymon, R.M.Prior, D.R.Tilley, H.R.Weller Search for p Waves in Low-Energy Proton Capture Reactions Relevant to the Solar Neutrino Problem NUCLEAR REACTIONS, ICPND 7Li(polarized p, γ), E=0-80 keV; measured αγ-coin, A(y)(θ), σ(θ)/A0; deduced p-wave strength, astrophysical implications.
doi: 10.1103/PhysRevC.53.R1
1996LA10 Phys.Rev. C53, 1977 (1996) C.M.Laymon, R.M.Prior, D.R.Tilley, H.R.Weller Low-Energy Polarized-Proton Capture on 6Li NUCLEAR REACTIONS, ICPND 6Li(polarized p, γ), E ≤ 80 keV; measured Eγ, Iγ, thick target yield, analyzing power vs θ; deduced s-, p-wave relative contributions, astrophysical S-factor.
doi: 10.1103/PhysRevC.53.1977
1996SC01 Phys.Rev. C53, 35 (1996) G.J.Schmid, R.M.Chasteler, H.R.Weller, D.R.Tilley, A.C.Fonseca, D.R.Lehman T20 Measurements for 1H(d(pol), γ)3He and the P-Wave Component of the Nucleon-Nucleon Force NUCLEAR REACTIONS 1H(polarized d, γ), E=12.7-19.8 MeV; measured T20(θ); deduced sensitivity to P-wave component of NN-force. Compared measurements to 3-body calculations.
doi: 10.1103/PhysRevC.53.35
1996SC14 Phys.Rev.Lett. 76, 3088 (1996) G.J.Schmid, M.Viviani, B.J.Rice, R.M.Chasteler, M.A.Godwin, G.C.Kiang, L.L.Kiang, A.Kievsky, C.M.Laymon, R.M.Prior, R.Schiavilla, D.R.Tilley, H.R.Weller Effects of Non-Nucleonic Degrees of Freedom in the D(p(pol), γ)3He and p(d(pol), γ)3He Reactions NUCLEAR REACTIONS, ICPND 2H(polarized p, γ), 1H(polarized d, γ), E=80 keV; analyzed σ(θ), polarization observables, astrophysical S-factor data.
doi: 10.1103/PhysRevLett.76.3088
1996SC26 Nucl.Phys. A607, 139 (1996) G.J.Schmid, R.M.Chasteler, C.M.Laymon, H.R.Weller, E.F.Moore, C.R.Bybee, J.M.Drake, D.R.Tilley, G.Vavrina, P.M.Wallace Correction Factors for γ-Ray Relative Intensities in the 66Ga Radioisotope RADIOACTIVITY 66Ga(β+), (EC); measured γ spectra; deduced relative Iγ, detector efficiency, implications to 2H(p, γ) reaction astrophysical S-factor data.
doi: 10.1016/0375-9474(96)00214-X
1995SC40 Phys.Rev. C52, R1732 (1995) G.J.Schmid, R.M.Chasteler, C.M.Laymon, H.R.Weller, R.M.Prior, D.R.Tilley Polarized Proton Capture by Deuterium and the 2H(p, γ)3He Astrophysical S Factor NUCLEAR REACTIONS, ICPND 2H(polarized p, γ), E=0-80 keV; measured Eγ, Iγ, σ(θ), analyzing power vs E; deduced astrophysical S-factor vs E.
doi: 10.1103/PhysRevC.52.R1732
1995TI07 Nucl.Phys. A595, 1 (1995) D.R.Tilley, H.R.Weller, C.M.Cheves, R.M.Chasteler Energy Levels of Light Nuclei A = 18-19 COMPILATION 18Be, 18,19B, 18,19C, 18,19N, 18,19O, 18,19F, 18,19Ne, 18,19Na; compiled, evaluated structure data.
doi: 10.1016/0375-9474(95)00338-1
1994BA02 Phys.Rev. C49, 912 (1994) M.J.Balbes, J.C.Riley, G.Feldman, H.R.Weller, D.R.Tilley Polarized Deuteron Capture by 3He and 3H at and above the Fusion Resonance Region NUCLEAR REACTIONS 3He, 3H(polarized d, γ), E=0.4-8.6 MeV; measured Eγ, Iγ, σ(θ), vector, tensor analyzing power vs θ; deduced transition matrix elements, reaction mechanism. Resonating group model.
doi: 10.1103/PhysRevC.49.912
1994CH23 Phys.Rev.Lett. 72, 3949 (1994) R.M.Chasteler, H.R.Weller, D.R.Tilley, R.M.Prior Observation of Substantial p-Wave Capture Strength in the 7Li(p(pol), γ)8Be Reaction for E(p) = 80-0 keV and Implications for Astrophysical S Factors NUCLEAR REACTIONS, ICPND 7Li(polarized p, γ), E ≤ 80 keV; measured σ(θ), analyzing power vs θ; deduced implications for astrophysical S-factor.
doi: 10.1103/PhysRevLett.72.3949
1994WI08 Nucl.Phys. A577, 653 (1994) J.Z.Williams, G.Feldman, H.R.Weller, D.R.Tilley Radiative Capture of Polarized Deuterons by 6Li and the D-State of 8Be NUCLEAR REACTIONS 6Li(polarized d, γ), E=2-14 MeV; measured σ(E) vs θ, vector, tensor analyzing power vs θ, E; deduced transition matrix elements phases. 8Be deduced D-state probability. Direct capture, multi-channel resonating group model.
doi: 10.1016/0375-9474(94)90938-5
1993KR06 Phys.Lett. 304B, 208 (1993) L.H.Kramer, R.M.Chasteler, E.Hayward, R.M.Prior, D.R.Tilley, H.R.Weller Observation of p-Wave Capture Strength in the 2H(d(pol), γ)4He Reaction at E(d) = 80-0 KeV NUCLEAR REACTIONS 2H(polarized d, γ), E=80 keV; measured σ(θ), vector, tensor analyzing power vs θ; deduced p-wave capture dominance. Model comparison.
doi: 10.1016/0370-2693(93)90284-O
1993SC19 Phys.Rev. C48, 441 (1993) G.J.Schmid, R.M.Chasteler, H.R.Weller, D.R.Tilley Radiative Capture of Polarized Deuterons on 7Li NUCLEAR REACTIONS 7Li(polarized d, γ), E=6 MeV; measured σ(θ), vector, tensor analyzing power vs θ; deduced angle integrated σ.
doi: 10.1103/PhysRevC.48.441
1993TI07 Nucl.Phys. A564, 1 (1993) D.R.Tilley, H.R.Weller, C.M.Cheves Energy Levels of Light Nuclei A = 16-17 COMPILATION 16He, 17,16Be, 17,16B, 17,16C, 17,16N, 17,16O, 17,16F, 17,16Ne, 17Na; compiled, evaluated structure data.
doi: 10.1016/0375-9474(93)90073-7
1992BA04 Phys.Rev. C45, R487 (1992) M.J.Balbes, G.Feldman, H.R.Weller, D.R.Tilley Polarized d + 3He Capture Into the (3/2)+ Fusion Resonance of 5Li and the Role of the Tensor Force NUCLEAR REACTIONS 3He(polarized d, γ), E=0.8 MeV; measured absolute σ(θ), vector, tensor analyzing power vs θ; deduced tensor force role. 5Li level deduced E1 transition matrix elements. Resonanting group model.
doi: 10.1103/PhysRevC.45.R487
1992TI02 Nucl.Phys. A541, 1 (1992) D.R.Tilley, H.R.Weller, G.M.Hale Energy Levels of Light Nuclei A = 4 COMPILATION 4H, 4He, 4Li; compiled, evaluated structure data.
doi: 10.1016/0375-9474(92)90635-W
1991BA02 Phys.Rev. C43, 343 (1991) M.J.Balbes, G.Feldman, L.H.Kramer, H.R.Weller, D.R.Tilley Ground-State Widths of 5He and 5Li Determined in the 3H(d, γ)5He and the 3He(d, γ)5Li Reactions NUCLEAR REACTIONS 3H, 3He(d, γ), E=8.6 MeV; measured Eγ, Iγ. 5Li, 5He level deduced Γ, nucleon decay widths.
doi: 10.1103/PhysRevC.43.343
1991WI04 Phys.Rev. C43, 1363 (1991) V.Wijekumar, J.Z.Williams, G.Feldman, H.R.Weller, D.R.Tilley Resolution of the Twofold Ambiguity in the E1 Capture Amplitudes for the 13C(p(pol), γ)14N Reaction NUCLEAR REACTIONS 13C(polarized p, γ), E=3-4.2 MeV; measured Eγ, Iγ, σ(θ), analyzing power; deduced E1 capture mechanism.
doi: 10.1103/PhysRevC.43.1363
1991WI19 Phys.Lett. 273B, 216 (1991) J.Z.Williams, G.Feldman, H.R.Weller, D.R.Tilley The 6Li(d(pol), γ)8Be Reaction at E(d) = 9.0 MeV and the D-State of 8Be NUCLEAR REACTIONS 6Li(polarized d, γ), E=90 MeV; measured Eγ, Iγ, σ(θ), vector, tensor analyzing power vs θ. 8Be deduced d+6Li D-state probability.
doi: 10.1016/0370-2693(91)91674-K
1990FE06 Phys.Rev. C42, R1167 (1990) G.Feldman, M.J.Balbes, L.H.Kramer, J.Z.Williams, H.R.Weller, D.R.Tilley 3H(p, γ)4He Reaction and the (γ, p)/(γ, n) Ratio in 4He NUCLEAR REACTIONS, ICPND 3H(p, γ), E=2-15 MeV; measured σ(E, θ=90°); deduced σ(E) for (γ, p), σ(γ, p)/σ(γ, n). 4He deduced no charge symmetry violation evidence.
doi: 10.1103/PhysRevC.42.R1167
1990LA16 Phys.Rev. C42, 1214 (1990) J.L.Langenbrunner, H.R.Weller, D.R.Tilley Two-Deuteron Radiative Capture: Polarization observables at E(d) ≤ 15 MeV NUCLEAR REACTIONS 2H(polarized d, γ), E=0-14.7 MeV; measured σ(θ, E), analyzing power vs θ, E; deduced T-matrix elements. 4He deduced D-state probability. Multi-channel resonating group model.
doi: 10.1103/PhysRevC.42.1214
1989RI04 Phys.Rev. C40, 1517 (1989) J.C.Riley, H.R.Weller, D.R.Tilley Radiative Capture of Tensor and Vector Polarized Deuterons by 3H at 400 keV NUCLEAR REACTIONS 3H(polarized d, γ), E=400 keV; measured σ(θ), analyzing power vs θ; deduced transition multipolarity. Transition matrix element analysis.
doi: 10.1103/PhysRevC.40.1517
1989WA03 Phys.Rev. C39, 352 (1989) D.J.Wagenaar, N.R.Roberson, H.R.Weller, D.R.Tilley Evidence for M1 Strength in the 3H(p(pol), γ)4He Reaction NUCLEAR REACTIONS 3H(polarized p, γ), E=2, 5, 9 MeV; measured σ(θ), analyzing power vs θ; deduced E1, E2, M1 T-matrix elements. Direct capture calculation.
doi: 10.1103/PhysRevC.39.352
1988LA14 Phys.Rev. C38, 565 (1988) J.L.Langenbrunner, G.Feldman, H.R.Weller, D.R.Tilley, B.Wachter, T.Mertelmeier, H.M.Hofmann 2H(d(pol), γ)4He Reaction at E(d) = 1.2 MeV NUCLEAR REACTIONS 2H(polarized d, γ), E=1.2 MeV; measured σ(θ), analyzing power vs θ; deduced γ-multipolarity, relative transition strengths. Microscopic multi-channel resonating group model.
doi: 10.1103/PhysRevC.38.565
1988WE15 Phys.Lett. 213B, 413 (1988) H.R.Weller, R.M.Whitton, J.Langenbrunner, E.Hayward, W.R.Dodge, S.Kuhn, D.R.Tilley The Energy Dependence of Polarization Observables in the 2H(d, γ)4He Reaction NUCLEAR REACTIONS 2H(polarized d, γ), E=0.3-50 MeV; measured γ-spectra, tensor, vector analyzing power vs E.
doi: 10.1016/0370-2693(88)91283-X
1987AU02 Phys.Rev. C35, 393 (1987) R.A.August, H.R.Weller, D.R.Tilley Measurement of the 12C(n, γ0)13C Cross Section in the Giant Dipole Resonance Region NUCLEAR REACTIONS 12C(n, γ), E=6.5-18.5 MeV; measured σ(E, θ), θ=90°. Graphite target. Direct-semidirect calculations.
doi: 10.1103/PhysRevC.35.393
1987TI07 Nucl.Phys. A474, 1 (1987) D.R.Tilley, H.R.Weller, H.H.Hasan Energy Levels of Light Nuclei A = 3 COMPILATION 3H, 3He, 3n; compiled, evaluated structure data.
doi: 10.1016/0375-9474(87)90193-X
1986MI17 Phys.Rev. C34, 389 (1986) G.Mitev, P.Colby, N.R.Roberson, H.R.Weller, D.R.Tilley Radiative Neutron Capture by Deuterium NUCLEAR REACTIONS 2H(n, γ), (polarized n, γ), E=9-14 MeV; measured σ(θ), A(θ); deduced capture σ, E1, E2, amplitudes, phases, σ(3H(γ, n))/σ(3He(γ, n)). Direct capture models.
doi: 10.1103/PhysRevC.34.389
1986WE07 Phys.Rev. C34, 32 (1986) H.R.Weller, P.Colby, J.Langenbrunner, Z.D.Huang, D.R.Tilley, F.D.Santos, A.Arriaga, A.M.Eiro 4He D-State Effects in the 2H(d, γ)4He Reaction at Low Energies NUCLEAR REACTIONS, ICPND 2H(d, γ), E=0.7-14.9 MeV; measured Eγ, Iγ, γ(θ), σ(E). 4He deduced asymptotic D-to-S state ratio.
doi: 10.1103/PhysRevC.34.32
1985AU10 Phys.Rev. C32, 1420 (1985) R.A.August, H.R.Weller, D.R.Tilley Radiative Deuteron Capture into the Secondary Doorway State of 13C NUCLEAR REACTIONS 11B(polarized d, γ), E=1.6-4 MeV; measured σ(E, θ), A(E, θ), T20(E, θ). 13C deduced doorway state parameters. Enriched targets. Seconday doorway state formalism.
doi: 10.1103/PhysRevC.32.1420
1985WA12 Nucl.Instrum.Methods 234, 109 (1985) D.J.Wagenaar, N.R.Roberson, H.R.Weller, D.R.Tilley A Bismuth Germanate Gamma-Ray Spectrometer with a Plastic Anticoincidence Shield NUCLEAR REACTIONS 12C(p, γ), E=14.26 MeV; 13C(p, γ), E=3.11 MeV; 3H(p, γ), E=1.6 MeV; 40Ca(n, γ), E=10 MeV; measured Eγ, Iγ. Bismuth Germanate X-ray spectrometer, plastic anticoincidence shield.
doi: 10.1016/0168-9002(85)90814-9
1985WA28 Phys.Rev. C32, 2155 (1985) D.J.Wagenaar, N.R.Roberson, H.R.Weller, D.R.Tilley 3He(p(pol), γ)4He Reaction at E(p) = 9.0 MeV NUCLEAR REACTIONS 3H(polarized p, γ), E=9 MeV; measured σ(θ), A(θ), Eγ, Iγ; deduced 1P1, 3P1, 1D2, 3D2 transition matrix amplitudes.
doi: 10.1103/PhysRevC.32.2155
1985WR01 Phys.Rev. C31, 1125 (1985) M.C.Wright, H.Kitazawa, N.R.Roberson, H.R.Weller, M.Jensen, D.R.Tilley Polarized Neutron Capture on 13C NUCLEAR REACTIONS 13C(polarized n, γ), E=5.6-17 MeV; measured σ(θ=90°) vs E, Eγ, Iγ, analyzing power vs E. 14C deduced narrow M1 resonances. Direct-semidirect model, isovector dipole, isoscalar electric quadrupole components.
doi: 10.1103/PhysRevC.31.1125
1984KI06 Phys.Rev. C30, 21 (1984) S.E.King, N.R.Roberson, H.R.Weller, D.R.Tilley Polarized and Unpolarized Proton Capture on Deuterium NUCLEAR REACTIONS 2H(p, γ), (polarized p, γ), E=6.5-15.94 MeV; measured σ(θ), analyzing power vs θ; deduced T-matrix amplitudes. 3He deduced E1, E2 admixture. Legendre polynominal analysis, channel spin representation.
doi: 10.1103/PhysRevC.30.21
1984KI14 Phys.Rev. C30, 1335 (1984) S.King, N.R.Roberson, H.R.Weller, D.R.Tilley, H.P.Engelbert, H.Berg, E.Huttel, G.Clausnitzer Vector Analyzing Power of 1H(d, γ) and 2H(p, γ) Reactions at E(x) = 6 MeV NUCLEAR REACTIONS 2H(polarized p, γ), E=0.77 MeV; 1H(polarized d, γ), E=1.62 MeV; measured vector analyzing power vs θ. 3He deduced M1 capture strength, channel spin 3/2 contribution.
doi: 10.1103/PhysRevC.30.1335
1984WE14 Phys.Rev.Lett. 53, 1325 (1984) H.R.Weller, P.Colby, N.R.Roberson, D.R.Tilley Tensor-Polarized-Deuteron Capture on Deuterium and the D State of 4He NUCLEAR REACTIONS 2H(polarized d, γ), E=9.7 MeV; measured Eγ, Iγ, σ(θ), T20(θ). 4He deduced D-state admixture in d-cluster configuration. Direct capture model.
doi: 10.1103/PhysRevLett.53.1325
1984WO05 Phys.Rev. C29, 1186 (1984) J.G.Woodworth, R.A.August, N.R.Roberson, D.R.Tilley, H.R.Weller, J.W.Jury Polarized Neutron Capture into 13C: Evidence for a secondary doorway state effect NUCLEAR REACTIONS 12C(n, γ), (polarized n, γ), E=12-18.8 MeV; measured σ(θ), analyzing power. 13C deduced secondary doorway state. Other data input, Legendre polynomial analysis.
doi: 10.1103/PhysRevC.29.1186
1983KI11 Phys.Rev.Lett. 51, 877 (1983) S.E.King, N.R.Roberson, H.R.Weller, D.R.Tilley Effects of the 3He D State in the Reaction 2H(p, γ)3He NUCLEAR REACTIONS 2H(p, γ), E=6.5-16 MeV; measured σ(θγ); deduced three-body D-state role.
doi: 10.1103/PhysRevLett.51.877
1982KI05 Nucl.Phys. A384, 129 (1982) S.E.King, M.Potokar, N.R.Roberson, H.R.Weller, D.R.Tilley Neutron Capture in the Giant Resonance Region of 209Pb NUCLEAR REACTIONS 208Pb(n, γ), E=7-13 MeV; measured σ(θ). 209Pb levels deduced dipole EWSR in GDR region. Direct-semidirect, pure resonance model calculations.
doi: 10.1016/0375-9474(82)90309-8
1982MC03 Phys.Rev. C25, 1644 (1982) R.C.McBroom, H.R.Weller, N.R.Roberson, D.R.Tilley 3H(p, γ)4He Reaction below E(p) = 30 MeV NUCLEAR REACTIONS 3H(p, γ), E=8-30 MeV; measured σ(E, θ). Legendre polynomial analysis.
doi: 10.1103/PhysRevC.25.1644
1982WE01 Phys.Rev. C25, 89 (1982) S.A.Wender, H.R.Weller, N.R.Roberson, D.R.Tilley, R.G.Seyler Neutron Capture in the Giant Resonance Region of 15N NUCLEAR REACTIONS 14N(n, γ), E=5.6-13 MeV; measured σ(θ, E), γ(θ). Direct semi-direct model.
doi: 10.1103/PhysRevC.25.89
1982WE05 Phys.Rev. C25, 2111 (1982) H.R.Weller, N.R.Roberson, G.Mitev, L.Ward, D.R.Tilley Polarized Neutron Capture on 3He at E(n) = 9.0 MeV NUCLEAR REACTIONS 3He(polarized n, γ), E=9 MeV; measured σ(θ), A(θ). Legendre polynomial analysis.
doi: 10.1103/PhysRevC.25.2111
1982WR01 Phys.Rev. C25, 2823 (1982) M.C.Wright, N.R.Roberson, H.R.Weller, D.R.Tilley, D.Halderson Proton Capture in the 19 MeV Region of 12C NUCLEAR REACTIONS 11B(p, γ), E=2.9-4.6 MeV; measured Eγ, Iγ, σ(θ) vs E. 12C transition deduced M1 quenching. Continuum shell model comparison.
doi: 10.1103/PhysRevC.25.2823
1981MA33 Phys.Rev. C24, 2378 (1981) S.Manglos, N.R.Roberson, H.R.Weller, D.R.Tilley Search for a Giant Resonance Built on the 16.6-MeV State in 8Be NUCLEAR REACTIONS 7Li(p, γ), E=11.5-30 MeV; measured Eγ, Iγ; deduced σ(E, θ); 7Li(p, γ), E=4-30 MeV; measured σ(E). 8Be deduced possible GDR. Natural target. Direct capture model.
doi: 10.1103/PhysRevC.24.2378
1981WA18 Phys.Rev. C24, 317 (1981) L.Ward, D.R.Tilley, D.M.Skopik, N.R.Roberson, H.R.Weller Confirmation of the Photoneutron Cross Section for 4He below 33 MeV NUCLEAR REACTIONS 3He(n, γ), E=6-17 MeV; measured σ(θ, E); deduced σ(γ, p)/σ(γ, n) vs E. Detailed balance.
doi: 10.1103/PhysRevC.24.317
1980CA16 Phys.Rev. C22, 397 (1980) C.P.Cameron, R.D.Ledford, M.Potokar, D.G.Rickel, N.R.Roberson, H.R.Weller, D.R.Tilley Polarized Proton Capture on 30Si NUCLEAR REACTIONS 30Si(polarized p, γ), E=6.4-15 MeV; measured σ(θ), analyzing power vs θ; 30Si(p, γ), E=5-28 MeV; measured σ(θ). 31P deduced E1, E2 transition matrix elements in GDR region, EWSR for E2 transition. Direct-semidirect model.
doi: 10.1103/PhysRevC.22.397
1980MC06 Phys.Rev.Lett. 45, 243 (1980) R.C.McBroom, H.R.Weller, S.Manglos, N.R.Roberson, S.A.Wender, D.R.Tilley, D.M.Skopik, L.G.Arnold, R.G.Seyler Evidence for a 2+ Resonance in 4He at 40 MeV NUCLEAR REACTIONS 3H(p, γ), E=17-31 MeV; measured σ(θ, E), asymmetry vs E. 4He(e, t), E not given; measured asymmetry vs E. 4He deduced resonance, J, π, Γ.
doi: 10.1103/PhysRevLett.45.243
1980TU01 Phys.Rev. C21, 525 (1980) J.D.Turner, N.R.Roberson, S.A.Wender, H.R.Weller, D.R.Tilley Polarized Proton Capture on 13C NUCLEAR REACTIONS 13C(polarized p, γ), E=8.05-15.5 MeV; measured σ(θ), A(θ). 13C(p, γ), E=6.24-17.0 MeV; measured σ(90°). 14N deduced E1, E2 amplitudes, phases. direct-semidirect model.
doi: 10.1103/PhysRevC.21.525
1979JE03 Z.Phys. A291, 609 (1979) M.Jensen, D.R.Tilley, H.R.Weller, N.R.Roberson, S.A.Wender, T.B.Clegg Polarized-Neutron Capture in the Giant-Resonance Region of 41Ca NUCLEAR REACTIONS 40Ca(polarized n, γ), E=10 MeV; measured σ(θ), A(θ). 41Ca deduced E2 contribution in giant dipole region. Legendre polynomial analysis.
1979JE05 Phys.Rev.Lett. 43, 609 (1979) M.Jensen, D.R.Tilley, H.R.Weller, N.R.Robertson, S.A.Wender, T.B.Clegg Polarized-Neutron Capture In The Giant-Resonance Region Of 41Ca NUCLEAR REACTIONS 40Ca(n, γ), E=10 MeV; measured products, Eγ, Iγ; deduced σ(θ), polarization data. Data were imported from EXFOR entry 12708.
doi: 10.1103/PhysRevLett.43.609
1979SK04 Phys.Rev. C20, 409 (1979) D.M.Skopik, J.J.Murphy II, H.R.Weller, R.A.Blue, N.R.Roberson, S.A.Wender, D.R.Tilley Reactions 15N(γ, d0)13C and 13C(d, γ0)15N in the Giant Resonance Region NUCLEAR REACTIONS 15N(e, e'd), E not given; measured σ(θ); deduced σ(γ, d). 13C(polarized d, γ), E=6.74 MeV; measured σ(θ), A(θ). 15N deduced E1 matrix elements, T-character, phases around 22-MeV excitation.
doi: 10.1103/PhysRevC.20.409
1979WE08 Phys.Rev. C20, 1589 (1979) H.R.Weller, S.Manglos, S.A.Wender, N.R.Roberson, M.Potokar, D.R.Tilley Inelastic α Cross Sections in the Region of the Giant Quadrupole Resonance for Nuclei Near Mass 60 NUCLEAR REACTIONS 52Cr, 54,58Fe, 60Ni(α, α'), E=8-18 MeV; measured σ(Eα, θ).
doi: 10.1103/PhysRevC.20.1589
1978TU02 Phys.Rev. C17, 1853 (1978) J.D.Turner, C.P.Cameron, N.R.Roberson, H.R.Weller, D.R.Tilley Polarized Proton Capture on 59Co NUCLEAR REACTIONS 59Co(polarized p, γ), E=6.8-12.8 MeV; measured σ(θ), A(θ). 59Co(p, γ), E=5.8-16.5 MeV; measured σ(E); deduced T-matrix amplitudes, phases.
doi: 10.1103/PhysRevC.17.1853
1978WE02 Phys.Rev. C17, 1260 (1978) H.R.Weller, R.A.Blue, P.L.Von Behren, N.R.Roberson, C.R.Gould, D.R.Tilley, S.A.Wender Angular Distribution Measurements for Radiative Capture of Fast Neutrons by 40Ca NUCLEAR REACTIONS 40Ca(n, γ), E=8.0, 12.0 MeV; measured σ(θ). DSD calculations.
doi: 10.1103/PhysRevC.17.1260
1978WE03 Phys.Rev. C17, 1365 (1978) S.A.Wender, C.R.Gould, D.R.Tilley, D.G.Rickel, R.W.Zurmuhle Confirmation of 8+ Assignment to the 11.86 MeV Level in 24Mg NUCLEAR REACTIONS 12C(16O, αγ), E=42 MeV; measured linear polarization, αγ-coin. 24Mg level deduced J, π.
doi: 10.1103/PhysRevC.17.1365
1978WE11 Phys.Rev.Lett. 41, 1217 (1978) S.A.Wender, N.R.Roberson, M.Potokar, H.R.Weller, D.R.Tilley Quadrupole Radiation in Fast-Neutron Capture on 40Ca NUCLEAR REACTIONS 40Ca(n, γ), E=6-13 MeV; measured σ(E). DSD calculations.
doi: 10.1103/PhysRevLett.41.1217
1976CA22 Phys.Rev. C14, 553 (1976) C.P.Cameron, N.R.Roberson, D.G.Rickel, R.D.Ledford, H.R.Weller, R.A.Blue, D.R.Tilley Giant Dipole Resonances in 55,57,59Co Using Polarized Proton Capture NUCLEAR REACTIONS 54,56,58Fe(polarized p, γ), E=8-15 MeV; measured σ(E, θ), A(E, θ). 58Fe(p, γ), E=5-16 MeV; measured σ. 55,57,59Co GDR deduced isospin splitting.
doi: 10.1103/PhysRevC.14.553
1976NE04 Nucl.Phys. A261, 427 (1976) R.O.Nelson, J.R.Williams, D.R.Tilley, D.G.Rickel, N.R.Roberson, S.Maripuu, C.P.Camerson, R.D.Ledford Mean Lifetimes of Levels in 55Co NUCLEAR REACTIONS 54Fe(3He, dγ), E=12 MeV; measured Eγ(θ), Doppler-shift attenuation. 55Co deduced levels, J, π, T1/2. Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(76)90156-1
1976RI01 Nucl.Phys. A256, 152 (1976) D.G.Rickel, N.R.Roberson, C.P.Cameron, R.D.Ledford, S.G.Buccino, D.R.Tilley Measurement of γ-Ray Angular Distributions and Linear Polarizations for 48V NUCLEAR REACTIONS 48Ti(p, nγ), E=5.5, 6.0, 6.4, 7.0 MeV; 34S(16O, pnγ), E=34 MeV; measured Eγ, γ(θ), pγ(θ). 48V levels deduced J, π, γ-mmixing.
doi: 10.1016/0375-9474(76)90100-7
1976RI05 Phys.Rev. C13, 2077 (1976) D.G.Rickel, N.R.Roberson, J.D.Turner, H.R.Weller, D.R.Tilley Assignment of 0- to the 2.99-MeV Level in 38K via the 40Ca(d, α)38K Reaction NUCLEAR REACTIONS 40Ca(polarized d, α), E=5.9-6.8 MeV; measured σ(E). 38K level deduced J, π.
doi: 10.1103/PhysRevC.13.2077
1976RI08 Phys.Rev. C14, 338 (1976) D.G.Rickel, C.P.Cameron, R.D.Ledford, N.R.Roberson, H.R.Weller, D.R.Tilley Giant Dipole Resonance in 56Fe Observed via (p, γ) and (α, γ) Reactions NUCLEAR REACTIONS 52Cr(α, γ), E=7-14 MeV; 55Mn(p, γ), E=4-11.7 MeV; measured σ(E, Eγ). 56Fe deduced GDR, strength.
doi: 10.1103/PhysRevC.14.338
1976WE07 Phys.Rev. C13, 922 (1976) H.R.Weller, R.A.Blue, N.R.Roberson, D.G.Rickel, S.Maripuu, C.P.Cameron, R.D.Ledford, D.R.Tilley Giant Resonance Region of 15N Studied by Polarized and Unpolarized Proton Capture Measurements NUCLEAR REACTIONS 14C(polarized p, γ), E=4.0-16.2 MeV; measured σ(E, Eγ, θ), A(E, θ). 15N deduced E1, E2 strength, T-matrix amplitudes, phases.
doi: 10.1103/PhysRevC.13.922
1976WE23 Phys.Rev. C14, 1179 (1976) S.A.Wender, C.R.Gould, D.R.Tilley, D.G.Rickel, J.D.Turner, N.R.Roberson g Factor of the 738 keV State in 43K NUCLEAR REACTIONS 40Ar(α, p), E=15 MeV; measured γγ(θ, H, t). 43K level deduced T1/2, g.
doi: 10.1103/PhysRevC.14.1179
1975WI05 Phys.Rev. C11, 1111 (1975) J.R.Williams, R.O.Nelson, C.R.Gould, D.R.Tilley Gamma Ray Linear Polarization Measurements for 29Al NUCLEAR REACTIONS 26Mg(α, p), E=11.26 MeV; measured linear polarization, pγ-coin. 29Al levels deduced J, π. Enriched target.
doi: 10.1103/PhysRevC.11.1111
1975WI28 Nucl.Phys. A253, 365 (1975) J.R.Williams, C.R.Gould, R.O.Nelson, D.R.Tilley, D.G.Rickel, N.R.Roberson A Study of the Low-Lying Levels in 61Ni NUCLEAR REACTIONS 58Fe(α, nγ), E=8 MeV; measured nγ-coin, γγ(θ), DSA, linear polarization. 60Ni(d, pγ), E=6 MeV; measured pγ-coin. 61Ni levels deduced J, π, δ, γ-branching, 3He. Enriched targets.
doi: 10.1016/0375-9474(75)90487-X
1974KE09 Nucl.Phys. A223, 253 (1974) W.Kessel, R.Bass, E.C.Hagen, N.R.Roberson, C.R.Gould, D.R.Tilley Study of Excited States of 39Ca and 39K NUCLEAR REACTIONS 36Ar(α, nγ), 36Ar(α, pγ), E=15.8, 17.0 MeV; measured Doppler-shift attenuation. 39Ca, 39K levels, deduced T1/2. Enriched 36Ar target.
doi: 10.1016/0375-9474(74)90413-8
1974NE08 Phys.Rev. C9, 2193 (1974) R.O.Nelson, C.R.Gould, D.R.Tilley, N.R.Robinson Mean Lifetimes of Levels in 59Cu NUCLEAR REACTIONS 58Ni(3He, dγ), E=11.6 MeV; measured Eγ, Iγ, dγ-coin, DSA. 59Cu deduced levels, T1/2, γ-branching, J, π.
doi: 10.1103/PhysRevC.9.2193
1974RI13 Nucl.Phys. A232, 200 (1974) D.G.Rickel, N.R.Roberson, R.O.Nelson, J.R.Williams, D.R.Tilley Measurement of Mean Lifetimes, γ-Ray Angular Distributions and Linear Polarizations for Low-Lying Levels of 50V NUCLEAR REACTIONS 50Ti(p, nγ), E=4.50, 4.62, 4.80 MeV; measured Eγ, Iγ, nγ-coin, γ(θ), pγ(θ), DSA. 50V levels deduced J, π, T1/2, γ-mixing, γ-branching ratios.
doi: 10.1016/0375-9474(74)90653-8
1974WE07 Phys.Rev.Lett. 33, 657 (1974) H.R.Weller, N.R.Roberson, D.Rickel, D.R.Tilley Giant-Dipole-Resonance Region of 15N Observed via 14C(p, p)14C Cross Section and Polarization Measurements NUCLEAR REACTIONS 14C(p, p), (polarized p, p), E=7.5-12.45 MeV; measured σ(θ), P(θ). 15N deduced giant dipole resonance, level-width, p-width, J, π.
doi: 10.1103/PhysRevLett.33.657
1973GO02 Phys.Rev.Lett. 30, 298 (1973) C.R.Gould, R.O.Nelson, J.R.Williams, D.R.Tilley, J.D.Hutton, N.R.Robertson, C.E.Busch, T.B.Clegg Application of Polarized Deuterons in (d, pγ) Angular Correlation Measurements NUCLEAR REACTIONS 12C, 30Si(d, pγ), E=4.15 MeV; measured pγ(θ). 13C, 31Si transitions deduced γ-mixing.
doi: 10.1103/PhysRevLett.30.298
1973GO10 Phys.Rev. C7, 1068 (1973); Erratum Phys.Rev. C8, 423 (1973) C.R.Gould, D.R.Tilley, N.R.Roberson Mean Lifetimes of Levels in 26Al NUCLEAR REACTIONS 24Mg(3He, pγ), E=6 MeV; measured σ(Ep, Eγ), Doppler shift attenuation. 26Al levels deduced T1/2.
doi: 10.1103/PhysRevC.7.1068
1973HU03 Nucl.Phys. A206, 403 (1973) J.D.Hutton, N.R.Roberson, C.R.Gould, D.R.Tilley A Study of Low-Lying Levels in 59Ni NUCLEAR REACTIONS 56Fe(α, nγ), E=8.5, 10.5 MeV; measured Doppler-shift attenuation, recoil distance, σ(Eα, Eγ, θ(αγ)). 59Ni levels deduced J, π, T1/2, γ-branching, γ-mixing. Enriched target.
doi: 10.1016/0375-9474(73)90543-5
1973NE18 Nucl.Phys. A215, 541 (1973) R.O.Nelson, C.R.Gould, D.R.Tilley, N.R.Roberson Study of Low-Lying Levels of 53Fe NUCLEAR REACTIONS 54Fe(p, d), E=29 MeV; measured σ(θ(d)). 50Cr(α, nγ), E=7.45, 8.7, 10.5; measured σ(θ(γ)), Doppler-shift attenuation. 53Fe deduced levels, L, S, T1/2, J, γ-mixing, B(M1), B(E2). Enriched targets.
doi: 10.1016/0375-9474(73)90487-9
1972GO02 Phys.Rev. C5, 281 (1972) C.R.Gould, N.R.Roberson, G.E.Mitchell, D.R.Tilley Properties of the 2.443- and 3.003-MeV Levels in 57Ni NUCLEAR REACTIONS 54Fe(α, n), E=9.2, 10.5 MeV; measured σ(θ(γ)), Doppler shift attenuation. 57Ni levels deduced J, π, T1/2.
doi: 10.1103/PhysRevC.5.281
1972HA22 Particles Nucl. 3, 92 (1972) E.C.Hagen, C.R.Gould, N.R.Roberson, D.R.Tilley Lifetime Measurements in 27Si NUCLEAR REACTIONS 24Mg(α, nγ), E=10.8, 12.61, 15.0 MeV; measured DSA, σ(En, Eγ). 27Si levels deduced T1/2, transition strengths.
1971RA03 Phys.Rev. C3, 1152 (1971) C.E.Ragan III, C.R.Gould, N.R.Roberson, G.E.Mitchell, D.R.Tilley Study of Low-Lying Levels of 37Ar NUCLEAR REACTIONS 34S(α, nγ), E=7.6-8.8 MeV; measured σ(E, Eγ, θ(γ)), Doppler shift attenuation. 37Ar deduced levels, T1/2, J, π.
doi: 10.1103/PhysRevC.3.1152
1971RA05 Phys.Rev. C3, 2076 (1971); Erratum Phys.Rev. C4, 2294 (1971) C.E.Ragan III, G.E.Mitchell, D.R.Tilley, C.R.Gould, N.R.Roberson Mean Lifetime of the 1.61 MeV Level in 37Ar NUCLEAR REACTIONS 34S(α, nγ), E=8.1 MeV; measured recoil distance. 37Ar level deduced T1/2.
doi: 10.1103/PhysRevC.3.2076
1970GO18 Phys.Rev.Lett. 25, 463 (1970) C.R.Gould, E.C.Hagen, R.V.Poore, N.R.Roberson, G.E.Mitchell, D.R.Tilley Lifetimes of Low-Lying Levels in 57Ni NUCLEAR REACTIONS 54Fe(α, nγ), E=8.7, 9.2, 10.5 MeV; measured σ(E;En, Eγ), Doppler shift attenuation. 57Ni deduced levels, T1/2, B(λ).
doi: 10.1103/PhysRevLett.25.463
1970HA02 Nucl.Phys. A140, 333 (1970) L.C.Haun, N.R.Roberson, D.R.Tilley A Study of the Low-Lying States of 23Mg NUCLEAR REACTIONS 24Mg(3He, αγ), E=6.37, 8.05 MeV; measured σ(Eα, Eγ, θ(αγ)). 23Mg levels deduced J, π, γ-branching, γ-mixing. Enriched target.
doi: 10.1016/0375-9474(70)90330-1
1970LA17 Nucl.Phys. A158, 43 (1970) G.P.Lamaze, C.R.Gould, C.E.Moss, N.R.Roberson, D.R.Tilley An Angular Correlation Study of the Low-Lying Levels of 29P NUCLEAR REACTIONS 32S(p, αγ), E=12.12, 12.89 MeV; measured σ(Eα, Eγ, θ(αγ)). 29P deduced levels, J, π, γ-branching ratios, γ-mixing ratios. Natural targets.
doi: 10.1016/0375-9474(70)90048-5
1970MO09 Nucl.Phys. A144, 577 (1970) C.E.Moss, R.V.Poore, N.R.Roberson, D.R.Tilley Spins of Levels in 32P and 34S NUCLEAR REACTIONS 29Si, 31P(α, pγ), E=7.65, 8.00 MeV; measured Eγ, σ(Ep, Eγ, θ(pγ)). 32P, 34S deduced levels, J, γ-branching ratios, γ-mixing ratios. Enriched, natural targets.
doi: 10.1016/0375-9474(70)90346-5
1970MO13 Nucl.Phys. A148, 480 (1970) G.L.Morgan, D.R.Tilley, G.E.Mitchell, R.A.Hilko, N.R.Roberson Study of 18O Through 14C + α Reactions NUCLEAR REACTIONS 14C(α, α), E=3.5-16.5 MeV; measured σ(E, θ). 14C(α, n), E=4.9-8.5 MeV; measured σ(E). 18O deduced resonances J, π, level-width. Enriched target.
doi: 10.1016/0375-9474(70)90641-X
1970MO17 Phys.Lett. 32B, 353 (1970) G.L.Morgan, D.R.Tilley, G.E.Mitchell, R.A.Hilko, N.R.Roberson States in 18O Excited by the 14C(7Li, t) Reaction NUCLEAR REACTIONS 14C(7Li, t), E=20.4 MeV; measured σ(Et, θ). 18O deduced levels, rotational bands.
doi: 10.1016/0370-2693(70)90494-6
1970RA17 Phys.Rev. C1, 2012 (1970) C.E.Ragan III, R.V.Poore, N.R.Roberson, G.E.Mitchell, D.R.Tilley Mean Lifetimes of Low-Lying Levels of 34S NUCLEAR REACTIONS 31P(α, pγ), E=5.0-7.3 MeV; measured Doppler shift attenuation. 34S levels deduced T1/2.
doi: 10.1103/PhysRevC.1.2012
1970RA24 Phys.Rev. C2, 557 (1970) C.E.Ragan III, C.E.Moss, C.R.Gould, N.R.Roberson, G.E.Mitchell, D.R.Tilley Mean Lifetime of the 2.94-MeV Level in 33S NUCLEAR REACTIONS 30Si(α, nγ), E=7.8-8.4 MeV; measured σ(E, Eγ), recoil distance. 33S level deduced T1/2.
doi: 10.1103/PhysRevC.2.557
1969RA29 Phys.Rev. 188, 1806 (1969); Erratum Phys.Rev. C2, 1581 (1970) C.E.Ragan III, C.E.Moss, R.V.Poore, N.R.Roberson, G.E.Mitchell, D.R.Tilley Mean Lifetimes and Branching Ratios of Low-Lying Levels in 33S NUCLEAR REACTIONS 30Si(α, nγ), E=5.5-9.0 MeV; measured σ(E, Eγ), Doppler shift attenuation. 33S deduced levels, T1/2, branching ratios, γ-mixing.
doi: 10.1103/PhysRev.188.1806
1968LE06 Phys.Rev. 168, 1205 (1968) M.B.Lewis, N.R.Roberson, D.R.Tilley Nuclear-Structure Studies of the Low-Lying Levels of Ca39 NUCLEAR STRUCTURE 39Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.168.1205
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