NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.McDonald Found 43 matches. 2007FR11 Phys.Rev. C 75, 065802 (2007) R.H.France III, E.L.Wilds, J.E.McDonald, M.Gai Further measurement of the β-delayed α-particle emission of 16N RADIOACTIVITY 16N(β-); measured delayed α spectrum. Compared results to existing data.
doi: 10.1103/PhysRevC.75.065802
2007WI09 Phys.Rev. C 76, 018501 (2007) E.L.Wilds, Jr., R.H.France III, J.E.McDonald, Z.Zhao, M.Gai Upper limits on the first-forbidden rank-one β decay of 20F RADIOACTIVITY 20F(β-); measured Eβ, Eγ, Eα. Deduced first forbidden decay branching ratios.
doi: 10.1103/PhysRevC.76.018501
2003FR22 Nucl.Phys. A718, 398c (2003) R.H.France III, L.T.Baby, C.Bordeanu, Th.Delbar, J.A.Dooley, M.Gai, M.Hass, J.E.McDonald, A.Ninane, C.M.Przybycien Destruction of 7Li and 7Be in astrophysical environments NUCLEAR REACTIONS 7Li(3He, α), (3He, d), E=390-1130 keV; measured Eα, σ, σ(θ).
doi: 10.1016/S0375-9474(03)00813-3
2002MC09 Nucl.Phys. B(Proc.Supp.) S112, 226 (2002) K.S.McFarland, G.P.Zeller, T.Adams, A.Alton, S.Avvakumov, L.de Barbaro, P.de Barbaro, R.H.Bernstein, A.Bodek, T.Bolton, J.Brau, D.Buchholz, H.Budd, L.Bugel, J.Conrad, R.B.Drucker, B.T.Fleming, R.Frey, J.A.Formaggio, J.Goldman, M.Goncharov, D.A.Harris, R.A.Johnson, J.H.Kim, S.Koutsoliotas, M.J.Lamm, W.Marsh, D.Mason, J.McDonald, C.McNulty, D.Naples, P.Nienaber, V.Radescu, A.Romosan, W.K.Sakumoto, H.Schellman, M.H.Shaevitz, P.Spentzouris, E.G.Stern, N.Suwonjandee, M.Tzanov, M.Vakili, A.Vaitaitis, U.K.Yang, J.Yu, E.D.Zimmerman Nuclear Effects and the NuTeV sin2θw Measurement NUCLEAR REACTIONS Fe(ν, X), (ν-bar, X), E not given; measured ratio of neutral to charged-current σ; deduced electroweak parameter, possible nuclear effects on parton distribution functions. Comparison with model predictions.
doi: 10.1016/S0920-5632(02)01777-2
2002ZE02 Phys.Rev.Lett. 88, 091802 (2002); Erratum Phys.Rev.Lett. 90, 239902(2003) G.P.Zeller, K.S.McFarland, T.Adams, A.Alton, S.Avvakumov, L.de Barbaro, P.de Barbaro, R.H.Bernstein, A.Bodek, T.Bolton, J.Brau, D.Buchholz, H.Budd, L.Bugel, J.Conrad, R.B.Drucker, B.T.Fleming, R.Frey, J.A.Formaggio, J.Goldman, M.Goncharov, D.A.Harris, R.A.Johnson, J.H.Kim, S.Koutsoliotas, M.J.Lamm, W.Marsh, D.Mason, J.McDonald, C.McNulty, D.Naples, P.Nienaber, A.Romosan, W.K.Sakumoto, H.Schellman, M.H.Shaevitz, P.Spentzouris, E.G.Stern, N.Suwonjandee, M.Tzanov, M.Vakili, A.Vaitaitis, U.K.Yang, J.Yu.E.D.Zimmerman Precise Determination of Electroweak Parameters in Neutrino-Nucleon Scattering NUCLEAR REACTIONS 1H(ν, ν'), (ν-bar, ν-bar'), E not given; measured ratio of neutral to charged current σ; deduced electroweak parameter. Comparison with model prediction.
doi: 10.1103/PhysRevLett.88.091802
2002ZE05 Phys.Rev. D65, 111103 (2002) G.P.Zeller, K.S.McFarland, T.Adams, A.Alton, S.Avvakumov, L.de Barbaro, P.de Barbaro, R.H.Bernstein, A.Bodek, T.Bolton, J.Brau, D.Buchholz, H.Budd, L.Bugel, J.Conrad, R.B.Drucker, B.T.Fleming, R.Frey, J.A.Formaggio, J.Goldman, M.Goncharov, D.A.Harris, R.A.Johnson, J.H.Kim, S.Koutsoliotas, M.J.Lamm, W.Marsh, D.Mason, J.McDonald, C.McNulty, D.Naples, P.Nienaber, A.Romosan, W.K.Sakumoto, H.Schellman, M.H.Shaevitz, P.Spentzouris, E.G.Stern, N.Suwonjandee, M.Tzanov, M.Vakili, A.Vaitaitis, U.K.Yang, J.Yu, E.D.Zimmerman Effect of Asymmetric Strange Seas and Isospin-Violating Parton Distribution Functions on sin2θW Measured in the NuTeV Experiment
doi: 10.1103/PhysRevD.65.111103
2001AL24 Phys.Rev. D64, 012002 (2001) A.Alton, T.Adams, T.Bolton, J.Goldman, M.Goncharov, R.A.Johnson, N.Suwonjandee, M.Vakili, J.Conrad, B.T.Fleming, J.Formaggio, J.H.Kim, S.Koutsoliotas, C.McNulty, A.Romosan, M.H.Shaevitz, P.Spentzouris, E.G.Stern, A.Vaitaitis, E.D.Zimmerman, R.H.Bernstein, L.Bugel, M.J.Lamm, W.Marsh, P.Nienaber, J.Yu, L.de Barbaro, D.Buchholz, H.Schellman, G.P.Zeller, J.Brau, R.B.Drucker, R.Frey, D.Mason, J.McDonald, D.Naples, S.Avvakumov, P.de Barbaro, A.Bodek, H.Budd, D.A.Harris, K.S.McFarland, W.K.Sakumoto, U.K.Yang Observation of Neutral Current Charm Production in νμ Fe Scattering at the Fermilab Tevatron NUCLEAR REACTIONS Fe(ν, X), E ≈ 154 GeV; 1n, 1H(p, X), E(cm)=38.8 GeV; measured charm production σ.
doi: 10.1103/PhysRevD.64.012002
2001GO43 Phys.Rev. D64, 112006 (2001) M.Goncharov, T.Adams, A.Alton, T.Bolton, J.Goldman, P.Spentzouris, J.Conrad, B.T.Fleming, J.Formaggio, S.Koutsoliotas, J.H.Kim, C.McNulty, A.Romosan, M.H.Shaevitz, E.G.Stern, A.Vaitaitis, E.D.Zimmerman, R.A.Johnson, M.Vakili, N.Suwonjandee, R.H.Bernstein, L.Bugel, M.J.Lamm, W.Marsh, P.Nienaber, J.Yu, L.de Barbaro, D.Buchholz, H.Schellman, G.P.Zeller, J.Brau, R.B.Drucker, R.Frey, D.Mason, J.E.McDonald, D.Naples, M.Tzanov, S.Avvakumov, P.de Barbaro, A.Bodek, H.Budd, D.A.Harris, K.S.McFarland, W.K.Sakumoto, U.K.Yang Precise Measurement of Dimuon Production Cross Sections in νμFe and (ν-bar)mFe Deep Inelastic Scattering at the Fermilab Tevatron NUCLEAR REACTIONS Fe(ν, μ+μ-X), (ν-bar, μ+μ-X), E ≈ 80-270 GeV; measured dimuon production σ. Comparison with previous results.
doi: 10.1103/PhysRevD.64.112006
1997FR12 Nucl.Phys. A621, 165c (1997) R.H.France III, E.L.Wildes, N.B.Jevtic, J.E.McDonald, M.Gai Further Measurement of the Beta-Delayed Alpha-Particle Emission of 16N RADIOACTIVITY 16N(β-) [from 2H(15N, X), E=70 MeV]; measured β-delayed α spectra. Other data, theory compared.
doi: 10.1016/S0375-9474(97)00231-5
1996BR37 Phys.Rev. A53, 2194 (1996) J.-P.Briand, B.d'Etat-Ban, D.Schneider, M.A.Briere, V.Decaux, J.W.McDonald, S.Bardin Time for the Empty L Shell of a Hollow Atom to be Filled
doi: 10.1103/PhysRevA.53.2194
1992HI01 Phys.Rev. C45, 601 (1992) N.M.Hintz, X.H.Yang, M.Gazzaly, S.J.Seestrom-Morris, C.L.Morris, D.C.Cook, A.M.Mack, J.W.McDonald, S.Mordechai, D.S.Oakley, C.F.Moore, M.Lynker, J.D.Zumbro Determination of Neutron and Proton Multipole Matrix Elements in 208Pb from π- and π+ Scattering at 180 MeV NUCLEAR REACTIONS 208Pb(π+, π+), (π+, π+'), (π-, π-'), (π-, π-), E=180 MeV; measured σ(θ). 208Pb levels deduced neutron, proton multipole matrix elements.
doi: 10.1103/PhysRevC.45.601
1992JO03 Phys.Rev. C46, 52 (1992) M.K.Jones, D.Dehnhard, S.K.Nanda, S.M.Sterbenz, C.L.Morris, M.Plum, J.D.Zumbro, A.H.Hussein, D.S.Oakley, M.J.Smithson, A.L.Williams, J.McDonald, M.A.Bryan, A.H.Fuentes, M.Lynker, D.Crockett, M.A.Machuca, S.Mordechai, C.F.Moore 4He(π, π'p)3H Reaction Near the P33 π-Nucleon Resonance NUCLEAR REACTIONS 4He(π+, π+'p), (π-, π-'p), E=140, 180 MeV; measured σ(θ(π'), σ(p)) vs excitation energy; deduced reaction mechanisms.
doi: 10.1103/PhysRevC.46.52
1991MO15 Phys.Rev. C44, 2209 (1991) C.F.Moore, K.Johnson, G.P.Kahrimanis, J.McDonald, M.Snell, H.J.Ward, S.H.Yoo, C.L.Morris, S.Mordechai, M.Burlein, N.Claytor, H.T.Fortune, R.Ivie, G.B.Liu, J.M.O'Donnell, D.Smith, N.Auerbach, D.Robson Angular Distributions for the Double Isobaric Analog and a T (<) State at High Excitation in Pion Double Charge Exchange on 93Nb NUCLEAR REACTIONS 93Nb(π+, π-), E=295 MeV; measured σ(θ(π), E(π)), σ(θ). 93Tc deduced large probability for T< excitation.
doi: 10.1103/PhysRevC.44.2209
1991OA01 Phys.Rev. C44, 2058 (1991) D.S.Oakley, R.J.Peterson, S.J.Seestrom, C.L.Morris, M.A.Plum, J.D.Zumbro, A.L.Williams, M.A.Bryan, J.W.McDonald, C.F.Moore Energy Dependence of Pion Inelastic Scattering from 208Pb NUCLEAR REACTIONS 208Pb(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=120, 250 MeV; calculated σ(θ). 208Pb levels deduced proton, neutron matrix elements ratio. Different structure models.
doi: 10.1103/PhysRevC.44.2058
1991WA04 Phys.Rev. C43, 1318 (1991) D.L.Watson, R.Gilman, C.L.Morris, J.D.Zumbro, S.Mordechai, M.Burlein, J.M.O'Donnell, H.T.Fortune, A.Kotwal, J.Puttz, J.D.Silk, J.S.McDonald, C.F.Moore, A.L.Williams, S.Y.Yoo Pion-Induced Double Charge Exchange on 12C, 24Mg, 32S, and 40Ca NUCLEAR REACTIONS 12C, 24Mg, 32S, 40Ca(π+, π-), E=164 MeV; measured σ(θ). Isobar-nucleon interaction mechanism.
doi: 10.1103/PhysRevC.43.1318
1990JO04 Phys.Rev. C42, R807 (1990) M.K.Jones, D.Dehnhard, S.K.Nanda, S.M.Sterbenz, C.L.Morris, M.Plum, J.D.Zumbro, A.Hussein, D.S.Oakley, M.J.Smithson, A.L.Williams, J.McDonald, M.A.Bryan, A.H.Fuentes, M.Lynker, D.Crockett, M.A.Machuca, S.Mordechai, C.F.Moore 4He(π, π'p)3H Reaction: Quasifree and resonance scattering NUCLEAR REACTIONS 4He(π+, π+'p), (π-, π-'p), E=180 MeV; measured σ(θ(π), θp); deduced σ(π+)/σ(π-). DWIA calculation.
doi: 10.1103/PhysRevC.42.R807
1988AS04 Phys.Lett. 215B, 41 (1988) D.Ashery, J.Lichtenstadt, E.Piasetzky, C.L.Morris, J.D.Zumbro, R.Gilman, M.W.Rawool, S.Mordechai, B.Boyer, A.Fuentes, K.Johnson, J.W.McDonald, M.J.Smithson, A.Williams, S.H.Yoo, C.F.Moore A Search for πNN Bound Systems NUCLEAR REACTIONS 2H(π+, π-), (π-, π+), E=260 MeV; measured possible (πNN) system mass; deduced σ upper limit.
doi: 10.1016/0370-2693(88)91066-0
1988OA03 Phys.Rev. C38, 2978 (1988) D.S.Oakley, R.J.Peterson, D.J.Rilett, C.L.Morris, S.J.Greene, B.Boyer, K.Johnson, A.H.Fuentes, J.W.McDonald, M.J.Smithson, A.L.Williams, S.H.Yoo, C.F.Moore Energy Dependence of Pion Inelastic Scattering to the 1+ States in 12C NUCLEAR REACTIONS 12C(π-, π-'), (π+, π+'), E=80-295 MeV; measured σ(θ); deduced isobar excitation role. 12C levels deduced σ ratio.
doi: 10.1103/PhysRevC.38.2978
1987DH01 Phys.Rev. C35, 1148 (1987) K.S.Dhuga, G.R.Burleson, J.A.Faucett, R.L.Boudrie, W.B.Cottingame, S.J.Greene, C.L.Morris, Z.F.Wang, J.W.McDonald, C.F.Moore, S.Mordechai, A.L.Williams, P.A.Seidl, M.A.Bryan, S.Nanda, S.J.Seestrom-Morris, J.D.Zumbro Sensitivity of Large-Angle Pion Elastic Scattering to Medium Modifications NUCLEAR REACTIONS 12C, 16O(π+, π+), E=100-240 MeV; measured σ(θ); deduced model parameter modifications. Optical model.
doi: 10.1103/PhysRevC.35.1148
1976FO10 Nucl.Phys. A267, 317 (1976) B.Fogelberg, Y.Kawase, J.McDonald, A.Backlin Levels in 117Cd Studied in the Decays of 117Ag and 117mAg RADIOACTIVITY 117Ag [from 235U(n, F)]; measured T1/2, Eγ, Iγ, I(ce), γγ-coin, γγ-delay; deduced ICC, log ft. 117Cd deduced levels, J, π, T1/2, γ-multipolarity, B(E1), B(E2), B(M1). Mass separated fission product. Ge(Li), Si(Li), NaI, plastic detectors.
doi: 10.1016/0375-9474(76)90663-1
1976MC06 Atomkernenergie 27, 112 (1976) Measurement of Thermal Neutron Cross Sections for Charged Particle Reactions in Ni59 and Ni61 NUCLEAR REACTIONS 59,61Ni(n, α), 59Ni(n, p), E=thermal; measured σ. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20433. 1975BR07 Phys.Rev. C11, 1122 (1975) B.A.Brown, D.B.Fossan, J.M.McDonald, K.A.Snover Recoil-Distance Lifetime Measurements of 48V Levels NUCLEAR REACTIONS 45Sc(α, nγ), E=9.5 MeV; measured nγ-coin, recoil distance. 48V deduced levels, π, T1/2, B(λ).
doi: 10.1103/PhysRevC.11.1122
1975KA09 Nucl.Phys. A241, 237 (1975) Y.Kawase, B.Fogelberg, J.McDonald, A.Backlin States in 119Cd Studied in the Decay of 119Ag RADIOACTIVITY 119Ag [from 235U(n, F)]; measured T1/2, Eγ, Iγ, I(ce), γγ-coin, γγ-delay; deduced ICC, log ft. 119Cd deduced levels, J, π, T1/2, γ-multipolarity, B(E1), B(E2), B(M1). Mass separated fission product. Ge(Li), Si(Li), NaI, plastic detectors.
doi: 10.1016/0375-9474(75)90315-2
1974BR04 Phys.Rev. C9, 1033 (1974) B.A.Brown, D.B.Fossan, J.M.McDonald, K.A.Snover Lifetime Measurements and E2 Effective Charges for Nuclei in the 1f7/2 Shell NUCLEAR REACTIONS 39K(α, n), E=10.4 MeV; 16O, 40Ca(3He, p), E=10.5 MeV; 40Ca, 41K(α, p), E=14.0 MeV; 45Sc(α, p), E=10.0 MeV; 46Ti(α, p), E=11.0 MeV; 40Ca(16O, 2pα), E=47 MeV; 49Ti(α, n), E=14.5 MeV; 40Ca(16O, 3p), E=47 MeV; 40Ca(16O, 2p), E=47 MeV; measured recoil distance. 18F, 42,43Sc, 44Ca, 48Ti, 49V, 50,52Cr, 51,53Mn levels deduced T1/2, B(E2). Deduced 40 < A < 56 effective charges. Natural, enriched targets, Ge(Li) detector.
doi: 10.1103/PhysRevC.9.1033
1974MC09 Nucl.Phys. A224, 13 (1974); Erratum Nucl.Phys. A239, 530 (1975) J.McDonald, B.Fogelberg, A.Backlin, Y.Kawase The Decays of 2.6 min 119gCd and 1.9 min 119mCd to 119In RADIOACTIVITY 119gCd, 119mCd [from 235U(n, F)]; measured T1/2, Eγ, Iγ, E(ce), I(ce), γγ coin, βγ, γγ delay, deduced multipolarities. 119In deduced levels, J, π, B(E1), B(E2). Isotopically separated 119Cd sources. Ge(Li), Si(Li), NaI(Tl), plastic detectors. Ge(Li)-Ge(Li) coin.
doi: 10.1016/0375-9474(74)90159-6
1973KE21 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1822 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.9, 28 (1974) 130Te Levels Excited in the β Decay of 130Sb (T1/2 = 40 min) RADIOACTIVITY 130Sb [from 235U(n, F), isotope separator]; measured Eγ, Iγ, γγ(t). 130Te deduced levels, J, π, T1/2, B(λ).
1973KE23 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1617 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.8, 48 (1974) A.Kerek, G.B.Holm, P.Carle, J.McDonald 132Sb States of the Proton-Neutron Hole Type Populated in the Decay of The Doubly Magic Nucleus 132Sn RADIOACTIVITY 132Sn; measured Eβ, βγ(t), deduced log ft. 132Sb deduced levels, T1/2, J, π. On-line mass separator.
1973KE25 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1622 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.8, 53 (1974) A.Kerek, P.Carle, S.Borg, J.McDonald The 132Sb → 132Te Decay with T1/2 = 3.4 and 4.9 min RADIOACTIVITY 132Sb; measured βγ(t). Eγ, Iγ, γγ-coin, T1/2, I(ce). 132Te deduced levels T1/2, J, π. On-line mass separator.
1973MC09 Nucl.Phys. A206, 417 (1973) Transition Probability Measurements in 132Te; The Systematics of E2 Transition Rates in Neutron-Rich Even Te Nuclei RADIOACTIVITY 132Sb [from 235U fission]; measured βγ-, γγ-delay, Eγ, ICC, Iγ. 132Te deduced T1/2, ICC, B(E2). Isotopically separated source. Ge(Li), Si(Li), NaI(Tl), plastic detectors.
doi: 10.1016/0375-9474(73)90544-7
1972KE20 Nucl.Phys. A195, 159 (1972) A.Kerek, G.B.Holm, P.Carle, J.McDonald Proton-Neutron-Hole States in 132Sb Populated in the β-Decay of the Doubly Closed Shell Nucleus 132Sn RADIOACTIVITY 132Sn[from 235U fission]; measured T1/2, Eγ, Iγ, E(ce), I(ce), Eβ, βγ-coin, γγ-coin, βγ-delay; deduced log ft, Q. 132Sb deduced levels, J, π, T1/2, ICC, B(M1), B(E2), γ-multipolarity. Isotopically separated source;Ge(Li), Si(Li), NaI(Tl), plastic, anthracene detectors, Ge(Li)-Ge(Li) coin.
doi: 10.1016/0375-9474(72)90728-2
1972KE28 Nucl.Phys. A198, 466 (1972) Properties of 130Te as Observed in the 40 min β-Decay of 130Sb RADIOACTIVITY 130Sb[from 235U fission]; measured Eγ, Iγ, E(ce), I(ce), Eβ-, γγ-coin, βγ-, γγ-delay; deduced Q. 130Te deduced levels, J, π, ICC, T1/2, B(E2). Isotopically separated source, Ge(Li), Si(Li), NaI(Tl), plastic, anthracene detectors, Ge(Li)-Ge(Li) coin.
doi: 10.1016/0375-9474(72)90702-6
1972MA67 Phys.Rev. C6, 2109 (1972) M.Marmor, J.M.McDonald, D.B.Fossan Lifetime of the 2+ 1759-keV State in 26Al via the 23Na(α, nγ)26Al Reaction NUCLEAR REACTIONS 23Na(α, nγ), E=9.5 MeV; measured recoil distance. 26Al level deduced T1/2.
doi: 10.1103/PhysRevC.6.2109
1972MC04 Priv.Comm. (January 1972)
1972MC09 Phys.Rev.Lett. 28, 1057 (1972) J.M.McDonald, P.M.S.Lesser, D.B.Fossan Time-Differential Quadrupole Interactions Following Recoil Implantation NUCLEAR REACTIONS 111Cd(16O, 16O'γ), E=40 MeV; measured (16O')(γ)(θ, t) in Cd metal; deduced quadrupole interaction frequencies.
doi: 10.1103/PhysRevLett.28.1057
1971CO08 Phys.Rev. C3, 1352 (1971) S.Cochavi, J.M.McDonald, D.B.Fossan Experimental Study of Electromagnetic Matrix Elements in 92Mo RADIOACTIVITY 92mTc; measured γγ-delay. 92Mo level deduced T1/2. 90Zr(α, 2nγ), E=20-24 MeV; measured σ(E;Eγ), αγ-delay, αγ(θ, H, t). 92Mo(p, p'γ), E=6-9 MeV; measured σ(E;Ep', Eγ), p'γ-delay. 92Mo levels deduced T1/2, μ.
doi: 10.1103/PhysRevC.3.1352
1971LE24 Nucl.Phys. A170, 663 (1971) K.W.D.Ledingham, J.Y.Gourlay, J.L.Campbell, M.L.Fitzpatrick, J.G.Lynch, J.McDonald The Ratio of K-Capture to Positon Emission in the Decay of 30P RADIOACTIVITY 30P[from 31P(γ, n)]; measured K/β+ ratio.
doi: 10.1016/0375-9474(71)90244-2
1971MC02 Nucl.Phys. A162, 365 (1971) J.McDonald, A.Backlin, S.G.Malmskog Transition Probabilities in 99Tc RADIOACTIVITY 99Mo[from 98Mo(n, γ)]; measured I(ce), γce-, cece-delay. 99Tc deduced T1/2, ICC, Iγ, mixing ratios, B(E2), B(M1). Enriched target.
doi: 10.1016/0375-9474(71)90991-2
1971MC10 Nucl.Phys. A176, 526 (1971); Priv. Comm. Levels in 128Te
doi: 10.1016/0375-9474(71)90934-1
1971SN01 Phys.Rev. C4, 398 (1971) K.A.Snover, J.M.McDonald, D.B.Fossan, E.K.Warburton Gamma-Ray Decay of the Low-Lying Levels of Cl34 NUCLEAR REACTIONS 32S(3He, pγ), E=6.8 MeV; measured Eγ, Iγ, Doppler shift attenuation. 31P(α, nγ), E=8-11 MeV; measured recoil distance. 34Cl deduced levels, T1/2, γ-branching.
doi: 10.1103/PhysRevC.4.398
1970CO28 Phys.Lett. 33B, 297 (1970) S.Cochavi, J.M.McDonald, D.B.Fossan The Magnetic Moment of the 2761 keV 8+ State in 92Mo NUCLEAR REACTIONS 90Zr(α, 2nγ), E=24 MeV; measured nγ(θ, H, t). 92Mo level deduced g.
doi: 10.1016/0370-2693(70)90274-1
1970MA07 Nucl.Phys. A142, 263 (1970) The 93.54 keV Level in 91Sr RADIOACTIVITY 91Rb[from 235U fission]; measured Eγ, Iγ, I(ce), βce-delay. 91Sr deduced levels, T1/2, J, π, ICC, γ-multipolarities, γ-mixing. Isotopically separated source, Ge(Li) singles, electron lens coin spectrometer.
doi: 10.1016/0375-9474(70)90528-2
1968MC04 Nucl.Phys. A109, 529 (1968) Excited States in 111Cd RADIOACTIVITY 111Ag [from 110Pd(n, γ)]; measured βγ-delay, Eγ. 111Cd level deduced T1/2. Enriched target, Ge(Li) detector. 111Cd(α, α'γ), E=8 MeV; measured σ(Eγ). 111Cd deduced levels, B(E2), T1/2. Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(68)90025-0
1967MC13 Nucl.Phys. A104, 177 (1967) J.McDonald, D.Porter, D.T.Stewart Excited States in 115In RADIOACTIVITY 115Cd [from 114Cd(n, γ)]; measured Iγ, I(X-ray), βγ-, γγ-delay, ICC. 115In deduced T1/2, multipolarity. Enriched target, Si(Li) detector. 115In(α, α'γ), E=8 MeV; 115In(16O, 16O'γ), E=35 MeV; measured σ(Eγ). 115In deduced level, B(E2). Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(67)90762-2
Back to query form Note: The following list of authors and aliases matches the search parameter J.McDonald: , J.E.MCDONALD, J.L.MCDONALD, J.M.MCDONALD, J.S.MCDONALD, J.W.MCDONALD |