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NSR database version of April 11, 2024.

Search: Author = E.G.Adelberger

Found 99 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1004.


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1448. Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1004.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1004.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1479.


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1004.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0162.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1144.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0213.


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
Citations: PlumX Metrics


1993AD02      Phys.Rev.Lett. 70, 2856 (1993)

E.G.Adelberger

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1190.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0114.


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
Citations: PlumX Metrics


1991SC18      Z.Phys. A339, 305 (1991)

A.Schafer, E.G.Adelberger

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
Citations: PlumX Metrics


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
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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
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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
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1987AD05      Phys.Rev. C36, 879 (1987)

E.G.Adelberger, W.C.Haxton

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1981NE09      Phys.Rev. C24, 1864 (1981)

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

Structure of 18Ne

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

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

doi: 10.1103/PhysRevC.24.1864
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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
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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
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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
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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
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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
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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
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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
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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
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1978MC04      Phys.Rev.Lett. 40, 1692 (1978)

A.B.McDonald, E.G.Adelberger

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
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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
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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
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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
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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
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1977BA50      Phys.Rev. C16, 928 (1977)

D.P.Balamuth, E.G.Adelberger

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1971AD06      Phys.Rev.Lett. 27, 1597 (1971)

E.G.Adelberger, D.P.Balamuth

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
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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
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1970AD02      Nucl.Phys. A145, 497 (1970)

E.G.Adelberger, A.B.McDonald

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
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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
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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
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1970MC06      Nucl.Phys. A144, 593 (1970)

A.B.McDonald, E.G.Adelberger

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1268.


1968MC03      Phys.Letters 26B, 380 (1968)

A.B.McDonald, E.G.Adelberger

T = 3/2 Levels in 21Na

NUCLEAR STRUCTURE 21Na, 19F; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90619-9
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1967AD05      Phys.Letters 25B, 595 (1967)

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

A Lower Limit on the Mass of 5Be

doi: 10.1016/0370-2693(67)90125-6
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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)

A.B.McDonald, E.G.Adelberger

Study of the 20Ne(3He, N)22Mg reaction

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


1966AD07      Phys.Letters 23, 474 (1966)

E.G.Adelberger, C.A.Barnes

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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