NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = E.G.Adelberger Found 99 matches. 2011AD03 Rev.Mod.Phys. 83, 195 (2011) E.G.Adelberger, A.Garcia, R.G.H.Robertson, K.A.Snover, A.B.Balantekin, K.Heeger, M.J.Ramsey-Musolf, A.B.Balantekin, K.Heeger, M.J.Ramsey-Musolf, D.Bemmerer, A.Junghans, D.Bemmerer, A.Junghans, C.A.Bertulani, K.-W.Chen, H.Costantini, P.Prati, M.Couder, E.Uberseder, M.Wiescher, R.Cyburt, B.Davids, S.J.Freedman, M.Gai, D.Gazit, L.Gialanella, G.Imbriani, U.Greife, M.Hass, W.C.Haxton, T.Itahashi, K.Kubodera, K.Langanke, D.Leitner, M.Leitner, P.Vetter, L.Winslow, L.E.Marcucci, T.Motobayashi, A.Mukhamedzhanov, R.E.Tribble, F.M.Nunes, T.-S.Park, R.Schiavilla, E.C.Simpson, C.Spitaleri, F.Strieder, H.-P.Trautvetter, K.Suemmerer, S.Typel Solar fusion cross sections. II. The pp chain and CNO cycles NUCLEAR REACTIONS 2H(p, γ), 3He(3He, 2p), (α, γ), (p, e), 7Be, 12C, 14N, 15N, 17O(p, γ), 15N, 16,17,18O(p, α), E<3 MeV; analyzed and evaluated experimental data; deduced recommended values and uncertainties.
doi: 10.1103/RevModPhys.83.195
2010JU01 Phys.Rev. C 81, 012801 (2010) A.R.Junghans, K.A.Snover, E.C.Mohrmann, E.G.Adelberger, L.Buchmann Updated S factors for the 7Be(p, γ)8B reaction NUCLEAR REACTIONS 7Be(p, γ)8B, E(cm)=0-2500 keV; analyzed previous data for σ using detailed target analysis and improved stopping powers; deduced updated astrophysical S-factors.
doi: 10.1103/PhysRevC.81.012801
2008BH08 Phys.Rev. C 77, 065503 (2008) M.Bhattacharya, D.Melconian, A.Komives, S.Triambak, A.Garcia, E.G.Adelberger, B.A.Brown, M.W.Cooper, T.Glasmacher, V.Guimaraes, P.F.Mantica, A.M.Oros-Peusquens, J.I.Prisciandaro, M.Steiner, H.E.Swanson, S.L.Tabor, M.Wiedeking ft value of the 0+ → 0+ β+ decay of 32Ar: A measurement of isospin symmetry breaking in a superallowed decay RADIOACTIVITY 32Ar(β+) [from 9Be(36Ar, X), E=100 MeV/nucleon]; measured Eγ, Iγ, Ep, Ip, pγ-coin. 32Ar; deduced superallowed decay branching ratio, ft value, isospin symmetry breaking correction. 32Cl; deduced levels, J, π. 31S; deduced levels, π. Comparison with theoretical data. ATOMIC MASSES 32Cl; measured masses. Q-value method.
doi: 10.1103/PhysRevC.77.065503
2006BH03 Phys.Rev. C 73, 055802 (2006) M.Bhattacharya, E.G.Adelberger, H.E.Swanson Precise study of the final-state continua in 8Li and 8B decays RADIOACTIVITY 8Li(β-α) [from 7Li(d, p)]; 8B(β+α) [from 6Li(3He, n)]; measured β-delayed Eα; deduced final-state continuum shapes. R-matrix analysis, comparison with previous results.
doi: 10.1103/PhysRevC.73.055802
2006TR03 Phys.Rev. C 73, 054313 (2006) S.Triambak, A.Garcia, E.G.Adelberger, G.J.P.Hodges, D.Melconian, H.E.Swanson, S.A.Hoedl, S.K.L.Sjue, A.L.Sallaska, H.Iwamoto Mass of the lowest T = 2 state in 32S: A test of the isobaric multiplet mass equation NUCLEAR REACTIONS 31P(p, γ), E=3.285 MeV; measured Eγ, Iγ. 32S deduced excited states energies. ATOMIC MASSES 32Si, 32P, 32S, 32Cl, 32Ar; analyzed mass excesses for T=2 quintet. Isospin-multiplet mass equation.
doi: 10.1103/PhysRevC.73.054313
2005JU03 Nucl.Phys. B(Proc.Supp.) S138, 112 (2005) A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.R.Buchmann, A.Laird, S.Park, A.Y.Zyuzin The new Seattle-TRIUMF 7Be(p, γ)8B S-factor determination NUCLEAR REACTIONS 7Be(p, γ), E(cm)=116-2460 MeV; measured σ; deduced astrophysical S-factors. Comparison with previous results.
doi: 10.1016/j.nuclphysbps.2004.11.028
2005SN03 Nucl.Phys. A758, 685c (2005) K.A.Snover, A.R.Junghans, E.C.Mohrmann, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.Buchmann, S.H.Park, A.Zyuzin, A.M.Laird The 7Be(p, γ)8B astrophysical S-factor
doi: 10.1016/j.nuclphysa.2005.05.122
2004JU08 Nucl.Phys. A746, 210c (2004) A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.R.Buchmann, A.M.Laird, S.Park, A.Y.Zyuzin New determination of the 7Be(p, γ)8B S-factor NUCLEAR REACTIONS 7Be(p, γ), E(cm)=116-2460 MeV; measured σ; deduced astrophysical S-factors. Comparison with previous results.
doi: 10.1016/j.nuclphysa.2004.09.035
2003JU04 Phys.Rev. C 68, 065803 (2003) A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.Buchmann, S.H.Park, A.Zyuzin, A.M.Laird Precise measurement of the 7Be(p, γ)8B S factor NUCLEAR REACTIONS 7Be(p, γ), E(cm)=116-2460; measured σ; deduced astrophysical S-factors. Comparison with previous results.
doi: 10.1103/PhysRevC.68.065803
2003PA33 Nucl.Phys. A718, 113c (2003) S.H.Park, A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.Buchmann, A.Zyuzin, A.Laird A new measurement of 7Be(p, γ)8B cross section and its astrophysical meaning NUCLEAR REACTIONS 7Be(p, γ), E=221, 1379 keV; measured σ; deduced astrophysical S-factor.
doi: 10.1016/S0375-9474(03)00687-0
2002BH03 Phys.Rev. C65, 055502 (2002) M.Bhattacharya, E.G.Adelberger Reanalysis of α + α Scattering and the β-Delayed α Spectra from 8Li and 8B Decays RADIOACTIVITY 8Li(β-); 8B(EC); analyzed β-delayed Eα. 8Be deduced R-matrix parameters. NUCLEAR REACTIONS 4He(α, α), E ≈ 0.4-33 MeV; analyzed phase shifts. 8Be deduced R-matrix parameters.
doi: 10.1103/PhysRevC.65.055502
2002JU01 Phys.Rev.Lett. 88, 041101 (2002) A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.Buchmann, S.H.Park, A.Zyuzin 7Be(p, γ)8B Astrophysical S Factor from Precision Cross Section Measurements NUCLEAR REACTIONS 7Be(p, γ), E(cm)=186-1200 keV; measured σ; deduced astrophysical S-factor.
doi: 10.1103/PhysRevLett.88.041101
2000GA61 Hyperfine Interactions 129, 237 (2000) A.Garcia, E.G.Adelberger, C.Ortiz, H.E.Swanson, M.Beck, O.Tengblad, M.J.G.Borge, I.Martel, H.Bichsel, and the ISOLDE Collaboration Positron-neutrino correlations in 32Ar and 33Ar decays: Probes of scalar weak currents and nuclear isospin mixing RADIOACTIVITY 32,33Ar(β+); measured delayed proton spectra, pβ-coin; deduced positron-neutrino correlation, constraints on scalar weak interactions.
doi: 10.1023/A:1012605731737
1999AD10 Phys.Rev.Lett. 83, 1299 (1999); Erratum Phys.Rev.Lett. 83, 3101 (1999) E.G.Adelberger, C.Ortiz, A.Garcia, H.E.Swanson, M.Beck, O.Tengblad, M.J.G.Borge, I.Martel, H.Bichsel, and the ISOLDE Collaboration Positron-Neutrino Correlation in the 0+ → 0+ Decay of 32Ar RADIOACTIVITY 32Ar(β+); measured delayed proton spectra, pβ-coin; deduced positron-neutrino correlation, constraints on scalar weak interactions.
doi: 10.1103/PhysRevLett.83.1299
1998AD12 Rev.Mod.Phys. 70, 1265 (1998) E.G.Adelberger, S.M.Austin, J.B.Bahcall, A.B.Balantekin, G.Bogaert, L.S.Brown, L.Buchmann, F.E.Cecil, A.E.Champagne, L.de Braeckeleer, C.A.Duba, S.R.Elliott, S.J.Freedom, M.Gai, G.Goldring, C.R.Gould, A.Gruzinov, W.C.Haxton, K.M.Heeger, E.Henley, C.W.Johnson, M.Kamionkowski, R.W.Kavanagh, S.E.Koonin, K.Kubodera, K.Langanke, T.Motobayashi, V.Pandharipande, P.Parker, R.G.H.Robertson, C.Rolfs, R.F.Sawyer, N.Shaviv, T.D.Shoppa, K.A.Snover, E.Swanson, R.E.Tribble, S.Turck-Chieze, J.F.Wilkerson Solar Fusion Cross Sections NUCLEAR REACTIONS 7Be, 12,13C, 15N, 16,17,18O(p, γ), 14,15N, 17,18O(p, α), 7Li(d, p), 3He(p, e+), (α, γ), (3He, 2p), 1H(p, e+), E=low; compiled, analyzed S-factor data, calculations; deduced implications for solar neutrino flux calculations.
doi: 10.1103/RevModPhys.70.1265
1998BH12 Phys.Rev. C58, 3677 (1998) M.Bhattacharya, A.Garcia, N.I.Kaloskamis, E.G.Adelberger, H.E.Swanson, R.Anne, M.Lewitowicz, M.G.Saint-Laurent, W.Trinder, C.Donzaud, D.Guillemaud-Mueller, S.Leenhardt, A.C.Mueller, F.Pougheon, O.Sorlin Neutrino Absorption Efficiency of an 40Ar Detector from the β Decay of 40Ti RADIOACTIVITY 40,41Ti, 37Ca(β+) [from 50Cr fragmentation]; measured β-delayed Ep, Ip, Eγ, Iγ, T1/2, branching ratios; deduced decay branches reduced transition strengths. 40Sc deduced Gamow-Teller strength distribution. 40Ar deduced neutrino capture σ. Implications for neutrino detector efficiency discussed.
doi: 10.1103/PhysRevC.58.3677
1998LE45 Nuovo Cim. 111A, 835 (1998) M.Lewitowicz, W.Trinder, M.Bhattacharya, E.G.Adelberger, J.C.Angelique, R.Anne, J.Aysto, C.Borcea, J.M.Daugas, C.Donzaud, A.Garcia, S.Grevy, R.Grzywacz, D.Guillemaud-Mueller, A.Jokinen, N.I.Kaloskamis, S.Leenhardt, M.J.Lopez, A.C.Mueller, F.de Oliveira, A.Ostrowski, F.Pougheon, M.G.Saint-Laurent, T.Siiskonen, O.Sorlin, H.E.Swanson Beta-Decay of Light Nuclei Close to the Proton Drip-Line: 40Ti and 35Ca RADIOACTIVITY 40Ti, 35Ca(β+) [from Ni(50Cr, X), (40Ca, X)]; measured β-delayed proton spectra, Eγ, T1/2, B(F), B(GT). 35K deduced IAS. Implications for solar neutrino detector efficiency discussed.
1997KA10 Phys.Rev. C55, 640 (1997) N.I.Kaloskamis, A.Garcia, S.E.Darden, E.Miller, W.Haeberli, P.A.Quin, B.P.Schwartz, E.Yacoub, E.G.Adelberger Isospin Mixing in 37K and Spin Decomposition of Gamow-Teller Strength in 37Ca Decay NUCLEAR REACTIONS 36Ar(polarized p, p), E=3.22-5.98 MeV; measured σ(θ), analyzing power vs θ vs E. 37K deduced resonances, J, π, Γ, Γp, isospin-mixing matrix elements. RADIOACTIVITY 37Ca(β+); analyzed data; deduced Gamow-Teller transition strength related features.
doi: 10.1103/PhysRevC.55.640
1997TR05 Nucl.Phys. A620, 191 (1997) W.Trinder, E.G.Adelberger, B.A.Brown, Z.Janas, H.Keller, K.Krumbholz, V.Kunze, P.Magnus, F.Meissner, A.Piechaczek, M.Pfutzner, E.Roeckl, K.Rykaczewski, W.-D.Schmidt-Ott, M.Weber Study of the β Decays of 37Ca and 36Ca RADIOACTIVITY 37,36Ca(β+p) [from 9Be(40Ca, X), E=300 MeV/nucleon]; measured β-delayed Ep, Ip, Eγ, Iγ, βγ-, βγp-coin, T1/2. 37K deduced levels isospin mixing. 36K levels deduced J, π assignment nonvalidity. Ge, Si detectors. sd-shell model.
doi: 10.1016/S0375-9474(97)00163-2
1997TR11 Phys.Lett. 415B, 211 (1997) W.Trinder, R.Anne, M.Lewitowicz, M.G.Saint-Laurent, C.Donzaud, D.Guillemaud-Mueller, S.Leenhardt, A.C.Mueller, F.Pougheon, O.Sorlin, M.Bhattacharya, A.Garcia, N.I.Kaloskamis, E.G.Adelberger, H.E.Swanson 40Ti β Decay and the Neutrino Capture Cross Section of 40Ar RADIOACTIVITY 40Ti(β+p) [from Ni(50Cr, X), E=82.6 MeV/nucleon]; measured β-delayed Ep, Ip, Eγ, Iγ; deduced Gamow-Teller strengths. 40Ar deduced isobaric analog ν capture σ. 40,41Ti(β+p); measured T1/2.
doi: 10.1016/S0370-2693(97)01243-4
1996HA26 Phys.Rev. C54, 1999 (1996) K.I.Hahn, A.Garcia, E.G.Adelberger, P.V.Magnus, A.D.Bacher, N.Bateman, G.P.A.Berg, J.C.Blackmon, A.E.Champagne, B.Davis, A.J.Howard, J.Liu, B.Lund, Z.Q.Mao, D.M.Markoff, P.D.Parker, M.S.Smith, E.J.Stephenson, K.B.Swartz, S.Utku, R.B.Vogelaar, K.Yildiz Structure of 18Ne and the Breakout from the Hot CNO Cycle NUCLEAR REACTIONS, ICPND 12C(12C, 6He), E=80 MeV; 16O(3He, n), E=10.9-14.5 MeV; 20Ne(p, t), E=44, 88 MeV; measured σ(θ). 18Ne deduced levels, Γ, J, π. 14O(α, p), E(cm) ≤ 2.5 MeV; calculated astrophysical S-factor vs E, astrophysical reaction rate vs temperature.
doi: 10.1103/PhysRevC.54.1999
1995DE18 Phys.Rev. C51, 2778 (1995); Erratum Phys.Rev. C52, 3509 (1995) L.De Braeckeleer, E.G.Adelberger, J.H.Gundlach, M.Kaplan, D.Markoff, A.M.Nathan, W.Schieff, K.A.Snover, D.W.Storm, K.B.Swartz, D.Wright, B.A.Brown Radiative Decays of the 16.6 and 16.9 MeV States in 8Be and Tests of the Conservation of the Vector Current in the A = 8 Multiplet NUCLEAR REACTIONS, ICPND 4He(α, γ), E=33-34.7 MeV; measured γ yield vs E, Iγ(θ). 8Be deduced doublet decay features, δ(E2/M1), Γγ, B(λ). Other A=8 nuclei data included in analysis, vector current conservation features discussed.
doi: 10.1103/PhysRevC.51.2778
1995GA03 Phys.Rev. C51, R439 (1995) A.Garcia, E.G.Adelberger, P.V.Magnus, H.E.Swanson, D.P.Wells, F.E.Wietfeldt, O.Tengblad, and the ISOLDE Collaboration β-Delayed γ-Ray Emission in 37Ca Decay RADIOACTIVITY 37Ca(β+); measured βγ-coin. 37K levels deduced B(GT). Implications to 37Cl(p, n) data discussed.
doi: 10.1103/PhysRevC.51.R439
1995GA16 Phys.Rev. C51, 3487 (1995) A.Garcia, E.G.Adelberger, P.V.Magnus, H.E.Swanson, F.E.Wietfeldt, O.Tengblad, and the Isolde Collaboration 36Ca β Decay and the Isobaric Multiplet Mass Equation RADIOACTIVITY 36Ca(β+p); measured β-delayed Ep, Ip. 36K deduced T=2 states mass. Precise test of the isobaric multiplet mass equation.
doi: 10.1103/PhysRevC.51.3487
1995MA36 Phys.Rev. C51, 2806 (1995) P.V.Magnus, E.G.Adelberger, N.Cabot γ Decays of Proton Unbound Levels in 37K NUCLEAR REACTIONS 40Ca(p, αX), E=18 MeV; measured Eα, α(fragment)-coin. 37K deduced levels, Γγ/Γp.
doi: 10.1103/PhysRevC.51.2806
1995TR02 Phys.Lett. 348B, 331 (1995) W.Trinder, E.G.Adelberger, B.A.Brown, Z.Janas, H.Keller, K.Krumbholz, V.Kunze, P.Magnus, F.Meissner, A.Piechaczek, M.Pfutzner, E.Roeckl, K.Rykaczewski, W.-D.Schmidt-Ott, M.Weber Gamow-Teller Strength in the β-Decay of 36Ca RADIOACTIVITY 36Ca(β+p); measured βγ-coin, β+-delayed proton spectra, T1/2; deduced log ft, Gamow-Teller transition strength.
doi: 10.1016/0370-2693(95)00130-D
1995TR03 Phys.Lett. 349B, 267 (1995) W.Trinder, E.G.Adelberger, Z.Janas, H.Keller, K.Krumbholz, V.Kunze, P.Magnus, F.Meissner, A.Piechaczek, M.Pfutzner, E.Roeckl, K.Rykaczewski, W.-D.Schmidt-Ott, M.Weber β-Decay of 37Ca RADIOACTIVITY 37Ca(β+p); measured βγ-coin, T1/2; deduced Gamow-Teller transition strength. 37K levels deduced Γγ/Γp. Comparison with other data.
doi: 10.1016/0370-2693(95)00282-P
1995ZE01 Phys.Rev. C51, 1494 (1995) V.J.Zeps, E.G.Adelberger, A.Garcia, C.A.Gossett, H.E.Swanson, W.Haeberli, P.A.Quin, J.Sromicki Parity Mixing of the 0+-0- I = 1 Doublet in 14N NUCLEAR REACTIONS, ICPND 13C(polarized p, p), E=1.1-2.2 MeV; 13C(p, γ), E=0.45-3 MeV; measured σ(E). 14N levels deduced ΔI=0 parity-mixing matrix element, levels parameters. Enriched targets. S-matrix analysis.
doi: 10.1103/PhysRevC.51.1494
1994MA14 Phys.Rev. C49, R1755 (1994) P.V.Magnus, E.G.Adelberger, A.Garcia The ' Hot CNO Cycle ' 13N(p, γ) Resonance Energy and the 18Ne Mass NUCLEAR REACTIONS 16O, 12C, 11B(3He, n), E=7.31 MeV; measured neutron tof spectra; deduced 13N(p, γ) reaction rate implications. 14O, 18Ne levels deduced mass excess.
doi: 10.1103/PhysRevC.49.R1755
1993AD02 Phys.Rev.Lett. 70, 2856 (1993) Improved Limits on Scalar Weak Couplings RADIOACTIVITY 32,33Ar(β+p); analyzed β-delayed proton decay data; deduced limits on scalar weak couplings.
doi: 10.1103/PhysRevLett.70.2856
1993AD09 Phys.Lett. 314B, 185 (1993) E.G.Adelberger, L.De Braeckeleer, W.C.Haxton, K.A.Snover Accelerator Calibration of Solar Neutrino Detectors NUCLEAR REACTIONS 12C(p, n), E not given; calculated neutrino flux from 12N source.
doi: 10.1016/0370-2693(93)90447-P
1993SM04 Phys.Rev. C47, 2740 (1993) M.S.Smith, P.V.Magnus, K.I.Hahn, R.M.Curley, P.D.Parker, T.F.Wang, K.E.Rehm, P.B.Fernandez, S.J.Sanders, A.Garcia, E.G.Adelberger Gamma Width of 14O(*)(5.17 MeV) and the Stellar 13N(p, γ)14O Reaction Rate NUCLEAR REACTIONS 14N(p, n), E(cm)=11.67 MeV; measured σ(θ). 1H(14N, 14O), E=175 MeV; measured 14O momentum spectra; deduced 13N(p, γ)14O stellar reaction rate. 14O level deduced Γγ/Γ.
doi: 10.1103/PhysRevC.47.2740
1992WE09 Phys.Rev.Lett. 69, 2446 (1992) D.P.Wells, E.G.Adelberger, P.V.Magnus, A.Garcia Wells et al. Reply: NUCLEAR STRUCTURE A=37; analyzed data, β-decay, (p, n) reaction probes; deduced need for new studies.
doi: 10.1103/PhysRevLett.69.2446
1991AD07 Phys.Rev.Lett. 67, 3658 (1991) E.G.Adelberger, A.Garcia, P.V.Magnus, D.P.Wells Is the Weak Axial-Vector Current Renormalized in Nuclei ( Question ) RADIOACTIVITY 37Cl(β+p); analyzed Gamow-Teller transition strength along with that from 37Cl(p, n) data; deduced weak axial-vector current renormalization features. NUCLEAR REACTIONS 37Cl(p, n), E not given; analyzed Gamow-Teller transition strength along with that from 37Cl(β+-decay) data; deduced weak axial-vector current renormalization features.
doi: 10.1103/PhysRevLett.67.3658
1991GA03 Phys.Rev. C43, 2012 (1991) A.Garcia, E.G.Adelberger, P.V.Magnus, D.M.Markoff, K.B.Swartz, M.S.Smith, K.I.Hahn, N.Bateman, P.D.Parker The ' Missing ' 3+ State of 18Ne and Explosive 17F(p, γ) Burning NUCLEAR REACTIONS, ICPND 16O(3He, n), E=10.9 MeV; measured σ(θ) vs excitation energy. 18Ne deduced level, J, π. 17F(p, γ), E(cm) ≈ 100-800 MeV; calculated astrophysical S-factor vs E, reaction rate. Input from 16O(3He, n) data.
doi: 10.1103/PhysRevC.43.2012
1991GA23 Phys.Rev.Lett. 67, 3654 (1991) A.Garcia, E.G.Adelberger, P.V.Magnus, H.E.Swanson, O.Tengblad, D.M.Moltz, and the ISOLDE Collaboration β+ Decays of 37Ca: Implications for the efficiency of the 37Cl solar ν detector RADIOACTIVITY 37Ca(β+p); measured β-delay pγ-coin; deduced Gamow-Teller transition strengths, solar ν cross section.
doi: 10.1103/PhysRevLett.67.3654
1991SC18 Z.Phys. A339, 305 (1991) T-Violation Experiments Using Mossbauer Transitions
1990GA02 Phys.Rev. C41, 775 (1990) A.Garcia, E.G.Adelberger, A.Charlop, S.Gil, J.H.Gundlach, S.Kailas Low Lying States in 127Xe: Implications for the efficiency of an 127I solar ν detector RADIOACTIVITY 127Cs(β+); measured γγ(θ), γγ-coin. 127Xe deduced levels, possible J, π, δ, γ-branching ratio.
doi: 10.1103/PhysRevC.41.775
1990GA17 Phys.Rev. C42, 765 (1990) A.Garcia, E.G.Adelberger, H.E.Swanson, T.F.Lang, D.M.Moltz 37Ca β+ Decay and the Efficiency of the 37Cl Detector for High Energy Neutrinos RADIOACTIVITY 37Ca(β+p) [from Ca(3He, X), E=60 MeV]; 25Si(β+) [from 24Mg(3He, 2n)]; measured β-delayed Ep, Ip, Eγ, Iγ, γγ-, pγ-coin; deduced log ft. 36Ar level deduced branching.
doi: 10.1103/PhysRevC.42.765
1989FE06 Phys.Rev. C40, 1887 (1989) P.B.Fernandez, E.G.Adelberger, A.Garcia γ Width of the Unbound 5.17 MeV Level of 14O and the ' Hot ' CNO Cycle NUCLEAR REACTIONS, ICPND 13C(3He, nγ), E=9.35 MeV; measured nγ-coin. 14O level deduced Γγ/Γ. 13N(p, γ), E ≈ astrophysical region; calculated σ; deduced astrophysical S-factor vs E.
doi: 10.1103/PhysRevC.40.1887
1988HI14 Phys.Rev. C38, 1370 (1988) M.M.Hindi, E.G.Adelberger, S.E.Kellogg, T.Murakami Search for the l-Forbidden Beta Decay 207Tl → 207Pb(*)(570 keV) RADIOACTIVITY 207Tl(β-) [from 223Ra decay chain]; measured I(β), E(γ), I(γ). 211Pb(β-) [from 223Ra decay chain]; measured E(γ), I(γ). 207Pb levels deduced ICC, γ-branching, B(M1). Ge(Li), NaI detectors.
doi: 10.1103/PhysRevC.38.1370
1987AD05 Phys.Rev. C36, 879 (1987) 37Cl Solar Neutrino Capture Cross Section RADIOACTIVITY 37Ca(β+p); calculated β-delayed p-emission effects; deduced 37Cl solar neutrino detector consequences. 37K levels deduced β-delayed proton branching ratios, Gamow-Teller transition strength.
doi: 10.1103/PhysRevC.36.879
1986AD01 Phys.Rev. C33, 1840 (1986) E.G.Adelberger, P.Hoodbhoy, B.A.Brown Reply to ' Parity Violating Asymmetries in the Scattering of Transversely Polarized Protons ' NUCLEAR REACTIONS 13C(polarized p, p), E=1.12-1.18 MeV; measured analyzing power vs E. 14N deduced levels, Γ, parity mixing effects.
doi: 10.1103/PhysRevC.33.1840
1985AD10 Phys.Rev.Lett. 55, 2129 (1985) E.G.Adelberger, P.B.Fernandez, C.A.Gossett, J.L.Osborne, V.J.Zeps Does the Cabibbo Angle Vanish in Fermi Matrix Elements of High-J States ( Question ) RADIOACTIVITY 24Al(β+) [from 24Mg(p, n), E=18 MeV]; measured Eγ, Iγ, T1/2; deduced ft, vector coupling constant, no evidence for Cabibbo angle vanishing in high spin states. 24Mg levels deduced absolute β+-branching ratios.
doi: 10.1103/PhysRevLett.55.2129
1984AD01 Nucl.Phys. A417, 269 (1984) E.G.Adelberger, J.L.Osborne, H.E.Swanson, B.A.Brown The l-Forbidden Gamow-Teller Decay of 39Ca RADIOACTIVITY 35Ar, 39Ca(β+); measured Iγ, Eγ; deduced ft, empirical single-particle operator normalizations. 35Cl levels deduced Iβ, γ-branching ratios, Gamow-Teller transition strengths. 39K levels deduced Iβ, Gamow-Teller transition strengths. Shell model.
doi: 10.1016/0375-9474(84)90508-6
1984AD04 Phys.Rev. C30, 456 (1984) E.G.Adelberger, P.Hoodbhoy, B.A.Brown Parity Mixing of Elastic Scattering Resonances: General theory and application to 14N NUCLEAR REACTIONS 13C(p, p), (polarized p, p), E=1-1.8 MeV; calculated σ(θ), analyzing power vs E. 14N resonances deduced parity mixing effects. S-matrix formalism.
doi: 10.1103/PhysRevC.30.456
1984BI03 Nucl.Phys. A413, 503 (1984) J.Billowes, E.G.Adelberger, O.Avila, N.A.Jelley, W.R.Kolbl The g-Factor and Lifetime of the 3- (298 keV) States in 16N NUCLEAR REACTIONS 2H(15N, p), E=25 MeV; measured γ(θ), DSA, γ(θ, t). 16N levels deduced g, T1/2, μ, B(M1). Ge(Li) detector, deuterium target. Shell model calculations.
doi: 10.1016/0375-9474(84)90424-X
1983AD03 Phys.Rev. C27, 2833 (1983) E.G.Adelberger, M.M.Hindi, C.D.Hoyle, H.E.Swanson, R.D.Von Lintig, W.C.Haxton Beta Decays of 18Ne and 19Ne and Their Relation to Parity Mixing in 18F and 19F NUCLEAR STRUCTURE 18,19F, 19,21Ne, 21Na; calculated B(λ). 18,19Ne, 21Na; calculated Gamow-Teller transition strengths. Shell model. RADIOACTIVITY 18Ne(β+) [from O(3He, xn), E=12 MeV]; 19Ne(β+) [from 19F(p, n), E=6.4 MeV]; measured Eγ, Iγ; deduced ft. 18,19F levels deduced β-branching ratios, relative Iγ, parity mixing effects. Shell model. Natural O2, SF6 gas targets.
doi: 10.1103/PhysRevC.27.2833
1983EA01 Nucl.Phys. A396, 221c (1983) E.D.Earle, A.B.McDonald, E.G.Adelberger, K.A.Snover, H.E.Swanson, R.von Lintig, H.B.Mak, C.A.Barnes Parity Mixing in 21Ne; Evidence for weak neutral currents in nuclei NUCLEAR STRUCTURE 18,19F, 21Ne; analyzed data; deduced isoscalar, isovector weak nucleon-nucleon coupling constants. NUCLEAR REACTIONS 21Ne(p, p'γ), E=4.08 MeV; measured Eγ, Iγ, γ CP; deduced isoscalar, isovector weak nucleon-nucleon coupling constants. 21Ne levels deduced parity mixing matrix element. Parity mixing input from 19,18F data.
doi: 10.1016/0375-9474(83)90021-0
1983HO05 Phys.Rev. C27, 1244 (1983) C.D.Hoyle, E.G.Adelberger, J.S.Blair, K.A.Snover, H.E.Swanson, R.D.Von Lintig Isospin Mixing in 24Mg RADIOACTIVITY 24Al(β+) [from 24Mg(p, n)]; measured βγ CP asymmetry, Eγ, Iγ; deduced isospin forbidden transition matrix element. 24Mg levels deduced isospin mixing.
doi: 10.1103/PhysRevC.27.1244
1983SN03 Phys.Rev. C27, 1837 (1983) K.A.Snover, E.G.Adelberger, P.G.Ikossi, B.A.Brown Proton Capture to Excited States of 16O: M1, E1, and Gamow-Teller transitions and shell model calculations NUCLEAR STRUCTURE 16N; calculated levels, B(M1); deduced IAS. 16O, 16C; calculated M1, E1, Gamow-Teller, (p, n) transition rates. 15C, 17,18N; calculated Gamow-Teller transition rates. Shell model. NUCLEAR REACTIONS 15N(p, γ), (p, p'γ), (p, αγ), (polarized p, γ), (polarized p, p'γ), (polarized p, αγ), E=2.5-9.5 MeV; measured capture σ(Eγ), σ(θγ), Eγ, Iγ, analyzing power vs θ. 16O deduced resonances, J, π, T, Γ, ΓpΓγ/Γ, B(M1) ratios, Γp/Γ, M1, E1 transition strengths. Shell model.
doi: 10.1103/PhysRevC.27.1837
1981AD01 Phys.Rev.Lett. 46, 695 (1981) E.G.Adelberger, C.D.Hoyle, H.E.Swanson, R.D.Von Lintig O+ → O- β+ Decay of 18Ne and the Determination of F(π) RADIOACTIVITY 18Ne [from O(3He, xn), E=12 MeV]; measured β-delayed Eγ, Iγ; 18F levels deduced β-branching, strength of parity-nonconserving effects. Pion exchange, parity-mixing operator in nucleon-nucleon interaction.
doi: 10.1103/PhysRevLett.46.695
1981AD05 Phys.Rev. C24, 313 (1981) E.G.Adelberger, M.M.Hindi, C.D.Hoyle, H.E.Swanson, R.D.Von Lintig (1/2)+ → (1/2)- Beta Decay of 19Ne and the Parity Nonconserving NN Force RADIOACTIVITY 19Ne [from 19F(p, n), E=6.4 MeV]; measured γγγ-coin; deduced Iβ, log ft. 19F deduced parity mixing effect smaller than shell model predictions.
doi: 10.1103/PhysRevC.24.313
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
1980SN01 Phys.Rev.Lett. 44, 927 (1980) K.A.Snover, P.G.Ikossi, E.G.Adelberger, K.T.Lesko Unique Determination of the Amplitude and Phase for the Population of The Giant-Dipole Resonance in the Reaction 12C(p(pol), γ0)13N NUCLEAR REACTIONS 12C(polarized p, γ), E=5-30 MeV; measured σ(E). 13N deduced GDR, T=3/2 M1(E2) interference.
doi: 10.1103/PhysRevLett.44.927
1979AD01 Phys.Rev. C19, 1 (1979) E.G.Adelberger, R.E.Marrs, K.A.Snover Isospin Nonconserving Proton Decays of 13N(T = 3/2) to Negative Parity States of 12C NUCLEAR REACTIONS 11B(3He, np), E=7 MeV; measured np-coin. 12C levels deduced isospin-forbidden excitation by proton decay from lowest T=3/2 level in 13N.
doi: 10.1103/PhysRevC.19.1
1979FR04 Phys.Rev. C19, 1907 (1979) S.J.Freedman, C.A.Gagliardi, M.A.Oothoudt, A.V.Nero, R.G.H.Robertson, F.J.Zutavern, E.G.Adelberger, A.B.McDonald Decays of the Lowest T = 2 States in A = 4N Nuclei from 8Be to 44Ti NUCLEAR REACTIONS 10Be, 14C, 18O, 26Mg, 30Si, 34S, 38Ar, 42Ca, 46Ti(p, t), E=42, 46 MeV; measured t-charged particle-coin, tnγ-coin. 8Be, 12C, 16O, 24Mg, 28Si, 32S, 36Ar, 40Ca, 44Ti deduced lowest J=0, T=2 positive parity level, systematics of isospin forbidden decay widths.
doi: 10.1103/PhysRevC.19.1907
1979IK02 Nucl.Phys. A319, 109 (1979) P.G.Ikossi, K.A.Snover, J.L.Osborne, E.G.Adelberger, A.B.McDonald The α-Width of the Lowest T = 2 State in 28Si NUCLEAR REACTIONS 24Mg(α, α), E=5.9-6.25 MeV; measured σ(Eα, θ). 28Si deduced resonances, L, J, π, Γ, Γα, T. Enriched target.
doi: 10.1016/0375-9474(79)90174-X
1978BA08 Phys.Rev.Lett. 40, 840 (1978) C.A.Barnes, M.M.Lowry, J.M.Davidson, R.E.Marrs, F.B.Morinigo, B.Chang, E.G.Adelberger, H.E.Swanson Search for Neutral-Weak-Current Effects in the Nucleus 18F NUCLEAR REACTIONS 16O(3He, pγ), E=4 MeV. 18F measured CP for transitions.
doi: 10.1103/PhysRevLett.40.840
1978DI05 Nucl.Phys. A303, 442 (1978) P.A.Dickey, J.E.Bussoletti, E.G.Adelberger Isospin-Forbidden β-Decay of 28Mg RADIOACTIVITY 28Mg [from 28Mg(18O, 16O)]; measured βγ-coin; deduced branching ratio to 28Al (0.972), log ft, isospin-mixing matrix element.
doi: 10.1016/0375-9474(78)90370-6
1978DI08 Phys.Rev. C18, 1973 (1978) P.A.Dickey, P.L.Dyer, K.A.Snover, E.G.Adelberger Gamma Decays of the First T = 3/2 States in 9Be and 9B NUCLEAR REACTIONS 7Li(3He, pγ), E=7.5 MeV; 7Li(3He, nγ), E=13 MeV; measured pγ-, nγ-coin. 9Be, 9B levels deduced γ-branching, Γ.
doi: 10.1103/PhysRevC.18.1973
1978FR10 Phys.Rev. C17, 2071 (1978) S.J.Freedman, C.A.Gagliardi, M.A.Oothoudt, A.V.Nero, R.G.H.Robertson, F.J.Zutavern, E.G.Adelberger, A.B.McDonald Decays of the Lowest T = 2 State in 44Ti NUCLEAR REACTIONS 46Ti(p, t), E=42 MeV; measured tγ-coin, tα-coin. 44Ti levels deduced Γγ/Γ, Γα/Γ.
doi: 10.1103/PhysRevC.17.2071
1978MC04 Phys.Rev.Lett. 40, 1692 (1978) Schematic Model for Isospin Mixing in Light Nuclei NUCLEAR STRUCTURE 36Ar, 32S, 28Si, 24Mg, 20Ne, 16O, 12C, 8Be, 4He; calculated isospin mixing matrix elements.
doi: 10.1103/PhysRevLett.40.1692
1978OS04 Nucl.Phys. A305, 144 (1978) J.L.Osborne, E.G.Adelberger, K.A.Snover Total Width of the Lowest T = 2 State in 24Mg NUCLEAR REACTIONS 23Na(p, γ), E=3906 keV; 27Al(p, γ), E=3671 keV; measured σγ(Ep, θ=90°). 24Mg T=2 resonance, 28Si resonance deduced Γ(cm). Natural targets.
doi: 10.1016/0375-9474(78)90168-9
1978RO08 Phys.Rev. C17, 1535 (1978) R.G.H.Robertson, T.L.Khoo, G.M.Crawley, A.B.McDonald, E.G.Adelberger, S.J.Freedman Mass of Lowest T = 2 State of 12C NUCLEAR REACTIONS 14C(p, t), E ≈ 45 MeV; measured σ; deduced Q. 12C deduced level, T, Γ. 12C(p, t), E=45 MeV; measured σ; deduced Q. 10C deduced level.
doi: 10.1103/PhysRevC.17.1535
1978SN01 Phys.Rev.Lett. 41, 145 (1978) K.A.Snover, R.von Lintig, E.G.Adelberger, H.E.Swanson, T.A.Trainor, A.B.McDonald, E.D.Earle, C.A.Barnes Upper Limit on Parity Mixing in 21Ne NUCLEAR REACTIONS 21Ne(p, p'), E=4.08 MeV; measured parity nonconserving γ-CP. 21Ne levels deduced parity-mixing matrix element.
doi: 10.1103/PhysRevLett.41.145
1977AD02 Phys.Rev. C15, 484 (1977) E.G.Adelberger, R.E.Marrs, K.A.Snover, J.E.Bussoletti Radiative Transitions and Isospin Mixing in 12C NUCLEAR REACTIONS 10B(3He, pγ), E=4.1 MeV; measured pγ-coin. 11B(p, γ), E=163 keV; measured σ(Eγ). 12C resonances deduced Γγ, isospin mixing.
doi: 10.1103/PhysRevC.15.484
1977BA50 Phys.Rev. C16, 928 (1977) Electromagnetic Decays of T = 2 States in T(z) = 1 Nuclei NUCLEAR REACTIONS 18O, 26Mg, 30Si, 54Fe, 58Ni(3He, pγ), E=11-15 MeV; measured pγ-coin. 20F, 28Al, 32P, 56Co, 60Cu T=2 0+ levels deduced γ-branching.
doi: 10.1103/PhysRevC.16.928
1977MA07 Nucl.Phys. A277, 429 (1977) R.E.Marrs, E.G.Adelberger, K.A.Snover Gamma Decays of Some T = 0, T = 1 and T = 2 States Above E(x) = 9.5 MeV in 20Ne NUCLEAR REACTIONS 19F(3He, dγ), E=15.0 MeV; measured dγ-coin. 16O(α, γ), (α, α'γ), E=6.93, 9.2-9.7 MeV; measured σ(E, θ). 20Ne deduced levels, J, π, T, γ-branching, Γ, Γγ, Γα. NaI spectrometer.
doi: 10.1016/0375-9474(77)90711-4
1977MA16 Phys.Rev. C16, 61 (1977) R.E.Marrs, E.G.Adelberger, K.A.Snover Electromagnetic Transitions in 13C and 13N NUCLEAR REACTIONS 12C(p, γ), E ≈ 14.25 MeV; measured thick target yield. 11B(3He, pγ), E=5.3 MeV; 11B(3He, nγ), E=7.0 MeV; measured particle γ-coin. 13C, 13N levels deduced partial, total Γ, B(λ).
doi: 10.1103/PhysRevC.16.61
1976AD03 Phys.Lett. 62B, 29 (1976) E.G.Adelberger, R.E.Marrs, K.A.Snover, J.E.Bussoletti Isospin Mixing in 12C NUCLEAR REACTIONS 10B(3He, pγ), E=4.1 MeV; measured γγ-coin. 11B(p, γ); measured resonance γ. 12C levels deduced γ-branching.
doi: 10.1016/0370-2693(76)90039-3
1976MA01 Nucl.Phys. A256, 1 (1976) R.E.Marrs, E.G.Adelberger, K.A.Snover, M.D.Cooper Upper Limits for Isospin-Forbidden γ-Decays of T=2 States in 20Ne NUCLEAR REACTIONS 19F(p, γ), E ≈ 4.09, 5.88 MeV; measured σ(E, Eγ). 20Ne deduced isospin-forbidden transition strengths, T=2 levels.
doi: 10.1016/0375-9474(76)90090-7
1976MC10 Nucl.Phys. A273, 451 (1976) A.B.McDonald, T.K.Alexander, O.Hausser, D.Disdier, E.G.Adelberger, H.B.Mak, A.P.Shukla, A.V.Nero Isospin-Forbidden Particle Decays in Light Nuclei (I). T = 3/2 Levels of 9Be, 9B NUCLEAR REACTIONS 7Li(3He, n), (3He, p), E=8.25 11 MeV; measured np-, pn-coin. 9Be deduced Γn/Γ. 9B deduced Γp/Γ. Enriched target.
doi: 10.1016/0375-9474(76)90603-5
1975AD01 Phys.Rev.Lett. 34, 402 (1975) E.G.Adelberger, H.E.Swanson, M.D.Cooper, J.W.Tape, T.A.Trainor Parity Mixing in 19F NUCLEAR REACTIONS 22Ne(polarized p, αγ), E=4.93 MeV; measured Eγ, CP. 19F level deduced parity nonconserving asymmetry.
doi: 10.1103/PhysRevLett.34.402
1975MA21 Phys.Rev.Lett. 35, 202 (1975) R.E.Marrs, E.G.Adelberger, K.A.Snover, M.D.Cooper Mirror γ Decays in 13C and 13N NUCLEAR REACTIONS 12C(p, γ), E=14.2-14.3 MeV; measured resonance γ-yield. 11B(3He, pγ), (3He, nγ); measured pγ-, nγ-coin. 13N level deduced γ-mixing, B(λ).
doi: 10.1103/PhysRevLett.35.202
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
1974SN02 Phys.Rev.Lett. 32, 1061 (1974) K.A.Snover, E.G.Adelberger, D.R.Brown Isoscalar Electric Quadrupole Strength in 16O NUCLEAR REACTIONS 12C(α, γ), E=7-27.5 MeV; measured σ(E). 16O deduced giant E2 resonance.
doi: 10.1103/PhysRevLett.32.1061
1973AD02 Phys.Rev. C7, 889 (1973) E.G.Adelberger, A.B.McDonald, C.L.Cocke, C.N.Davids, A.P.Shukla, H.B.Mak, D.Ashery Isospin-Forbidden Particle Decay of T = 3/2 Levels in Mirror Nuclei NUCLEAR REACTIONS 11B(3He, np), E=7.0 MeV; measured σ(Ep, En, θ(n), θ(p)), αn-, pn-coin. 13N deduced level-width(γ), level-width(p), level-width(α). 11B(3He, np), E=7.5, 6.6 MeV; measured σ(En, Ep, θ(n), θ(p)), np-coin. 13C deduced level-width(γ), level-width(n). 15N(3He, np), E=8.25, 8.44 MeV; measured σ(En, Ep, θ(n), θ(p)), np-coin. 17F deduced level-width(p). 15N(3He, np), E=9.6 MeV; measured σ(En, Ep, θ(n), θ(p)), np-coin. 17O deduced level-width(n). 18O(3He, nα), E=12 MeV; measured σ(En, Eα, θ(α), θ(n))nα-coin. 17O deduced level-width(n).
doi: 10.1103/PhysRevC.7.889
1973MA24 Phys.Rev. C8, 427 (1973) R.E.Marrs, D.Bodansky, E.G.Adelberger Accelerator Production of 8B Neutrinos NUCLEAR REACTIONS 6Li(3He, nγ), E=8.9-26.5 MeV; measured σ(E). 8B deduced production.
doi: 10.1103/PhysRevC.8.427
1972AD10 Phys.Rev.Lett. 29, 883 (1972) E.G.Adelberger, P.T.Debevec, G.T.Garvey, R.Ohanian Failure of the Coexistence Model to Account for Observed Two-Neutron Pickup Cross Sections NUCLEAR REACTIONS 18O, 42Ca(p, t), E=41.7 MeV; measured σ(θ); deduced pickup amplitudes, failure of coexistence model.
doi: 10.1103/PhysRevLett.29.883
1972BU18 Phys.Lett. 40B, 357 (1972) D.Burch, P.Russo, H.Swanson, E.G.Adelberger Lifetime of the First Excited State in 96Zr NUCLEAR REACTIONS 90,96Zr, 98Mo(p, p'γ), E=8.16, 12.25 MeV; measured pce-delay. 98Mo, 90,96Zr levels deduced T1/2.
doi: 10.1016/0370-2693(72)90819-2
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
1972KU24 Nucl.Phys. A193, 497 (1972) H.M.Kuan, G.L.Latshaw, W.J.O'Connell, D.W.Heikkinen, E.G.Adelberger, A.V.Nero, S.S.Hanna Observation of the Second T = 2 State of 20Ne as a Compound Resonance in the 19F + p Reactions NUCLEAR REACTIONS 19F(p, p), (p, n), (p, α), (p, γ), Ep=5.65-6.20 MeV; measured σ(E, θ). 20Ne second T=2 resonance deduced levels, J, π, T, level-width.
doi: 10.1016/0375-9474(72)90336-3
1972NE10 Phys.Rev. C6, 679 (1972) A.V.Nero, R.E.Pixley, E.G.Adelberger Some Properties of the Lowest T = 2 States in 16O NUCLEAR REACTIONS 14N(d, p), (d, α), E=2.25-2.35 MeV; 12C(α, p), (α, α'), E=20.70-20.80 MeV; measured σ(E). 16O deduced resonances, level-width, J, π.
doi: 10.1103/PhysRevC.6.679
1972TA18 Phys.Rev.Lett. 29, 878 (1972) J.W.Tape, E.G.Adelberger, D.Burch, L.Zamick Lifetime of the 0+2 State of 206Pb and the State Dependence of the Monopole Effective Charge NUCLEAR REACTIONS 206Pb(p, p'γ), E=12.25 MeV; measured E(ce), I(ce), p'ce-delay. 206Pb level deduced T1/2.
doi: 10.1103/PhysRevLett.29.878
1971AD06 Phys.Rev.Lett. 27, 1597 (1971) Electromagnetic Decays of the Lowest T = 2 State in 32P NUCLEAR REACTIONS 30Si(3He, pγ), E=10 MeV; measured σ(Ep, Eγ). 32P deduced lowest T=2 state, γ-branching.
doi: 10.1103/PhysRevLett.27.1597
1970AD01 Nucl.Phys. A143, 97 (1970) E.G.Adelberger, A.V.Nero, A.B.McDonald Low-Lying T = 2 States of 16O NUCLEAR REACTIONS 12C, 14C(3He, n), E=11.3-18.0 MeV; measured σ(E;En, θ). 14O, 16O deduced levels, T, level-width, J, π, L. Enriched target.
doi: 10.1016/0375-9474(70)90682-2
1970AD02 Nucl.Phys. A145, 497 (1970) A Study of the 16O(3He, n) and 12C(3He, n) Stripping Reactions and a Comparison of Analogous (3He, n), (3He, p) and (t, p) Transitions NUCLEAR REACTIONS 16O, 12C(3He, n), E=9.0-13.5 MeV; measured σ(E;En, θ). 18Ne, 14O deduced levels, J, π. Compared with (3He, p), (t, p) reactions. Natural targets.
doi: 10.1016/0375-9474(70)90438-0
1970GO04 Phys.Rev. C1, 123 (1970) D.R.Goosman, E.G.Adelberger, K.A.Snover T = 3/2 Levels in 11B from the 10Be(p, γ0)11B Reaction NUCLEAR REACTIONS 10Be(p, γ), E=0.6-6.3 MeV; measured σ(E;Eγ, θ(γ)). 11B deduced isobaric analog resonances, J, π, level-width.
doi: 10.1103/PhysRevC.1.123
1970MC02 Phys.Lett. 31B, 119 (1970) A.B.McDonald, E.G.Adelberger, H.B.Mak, D.Ashery, A.P.Shukla, C.L.Cocke, C.N.Davids Isospin-Nonconserving Particle Decays of the Lowest T = 3/2 Levels in 17F and 17O NUCLEAR REACTIONS 15N(3He, n), E=8.44 MeV; 18O(3He, α), E=12 MeV; measured σ(En, Ep), σ(Eα, En). 17F, 17O T=3/2 levels deduced level-width, branching ratios.
doi: 10.1016/0370-2693(70)90126-7
1970MC06 Nucl.Phys. A144, 593 (1970) A Study of 22Mg by the 20Ne(3He, n) Reaction NUCLEAR REACTIONS 20Ne(3He, n), E=3.4-9.4 MeV; measured σ(E;En, θ), Q. 22Mg deduced levels, J, π. Enriched target.
doi: 10.1016/0375-9474(70)90347-7
1969AD01 Phys.Rev.Letters 22, 352(1969) E.G.Adelberger, C.L.Cocke, C.N.Davids, A.B.McDonald Isospin-Nonconserving Decays in Mirror Nuclei NUCLEAR REACTIONS 11B(3He, pn), (3He, np), E=7 MeV; measured σ(En, Ep). 13C, 13N levels deduced n-, p-decay branching, form of isospin impurity.
doi: 10.1103/PhysRevLett.22.352
1969AD02 Nucl.Phys. A124, 49(1969) E.G.Adelberger, A.B.McDonald, C.A.Barnes A Study of Low-Lying T = 3/2 and T = 2 States in Some Light Nuclei (I) NUCLEAR REACTIONS 11B, 15N, 18O, 19F, 22Ne(3He, n), E=4.2-13.5 MeV; measured σ(En, θ). 13N, 17F, 20Ne, 21Na, 24Mg deduced levels, T, level-width, J, π, L. Enriched targets.
doi: 10.1016/0375-9474(69)90520-X
1969AD03 Nucl.Phys. A131, 430 (1969) A.Adams, M.H.Shapiro, W.M.Denny, E.G.Adelberger, C.A.Barnes The 18O(α, γ)22Ne Reaction NUCLEAR REACTIONS 18O(α, γ), E=2.15-3.70 MeV; measured σ(Eα;θ). Enriched target.
doi: 10.1016/0375-9474(69)90546-6
1968MC03 Phys.Letters 26B, 380 (1968) T = 3/2 Levels in 21Na NUCLEAR STRUCTURE 21Na, 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90619-9
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
1967BA59 Intern.Nucl.Phys.Conf., Gatlinburg, Tenn.(1966), R.L.Becker, C.D.Goodman, P.H.Stelson, A.Zucker, Eds., Academic Press, New York, p.261(1967) C.A.Barnes, E.G.Adelberger, D.C.Hensley, A.B.MacDonald The Nuclear Masses of C9 and the Corresponding Analog State of B9 NUCLEAR STRUCTURE 9C; measured not abstracted; deduced nuclear properties.
1967MC15 Bull.Am.Phys.Soc. 12, No.8, 1145, FB14 (1967) Study of the 20Ne(3He, N)22Mg reaction NUCLEAR STRUCTURE 22Mg; measured not abstracted; deduced nuclear properties.
1966AD07 Phys.Letters 23, 474 (1966) T=3/2 Levels in 17F NUCLEAR STRUCTURE 15N, 17F; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90780-3
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