NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = R.G.Robertson Found 60 matches. 2023BY02 Phys.Rev.Lett. 131, 082502 (2023) W.Byron, H.Harrington, R.J.Taylor, W.DeGraw, N.Buzinsky, B.Dodson, M.Fertl, A.Garcia, G.Garvey, B.Graner, M.Guigue, L.Hayen, X.Huyan, K.S.Khaw, K.Knutsen, D.McClain, D.Melconian, P.Muller, E.Novitski, N.S.Oblath, R.G.H.Robertson, G.Rybka, G.Savard, E.Smith, D.D.Stancil, M.Sternberg, D.W.Storm, H.E.Swanson, J.R.Tedeschi, B.A.VanDevender, F.E.Wietfeldt, A.R.Young, X.Zhu, for the He6-CRES Collaboration First Observation of Cyclotron Radiation from MeV-Scale e± following Nuclear β Decay RADIOACTIVITY 6He(β-), 19Ne(β+) [7Li(d, 3He), E=17.8 MeV; 19F(p, n), E=12 MeV]; measured decay products, Eβ, Iβ; deduced β spectra, first direct observation of cyclotron radiation from individual highly relativistic β in a waveguide. The cyclotron radiation emission spectroscopy (CRES) technique, FN-tandem accelerator at the University of Washington.
doi: 10.1103/PhysRevLett.131.082502
2023DE11 Phys.Rev. C 107, L042501 (2023) Shake-up and shake-off effects in neutrinoless double-β decay RADIOACTIVITY 76Ge, 136Xe(2β-); analyzed information on shake-up and shake-off effects in neutrinoless double-β decay; deduced the reduction of Q values due to atomic excitation in the final-state. Showed that change of Q value due to atomic effects for 0νββ-decay is negligible comparing to the resolution of current and planned experiments. of the initial and final state atoms
doi: 10.1103/PhysRevC.107.L042501
2022BA17 Phys.Rev.Lett. 128, 232501 (2022) V.V.Barinov, B.T.Cleveland, S.N.Danshin, H.Ejiri, S.R.Elliott, D.Frekers, V.N.Gavrin, V.V.Gorbachev, D.S.Gorbunov, W.C.Haxton, T.V.Ibragimova, I.Kim, Y.P.Kozlova, L.V.Kravchuk, V.V.Kuzminov, B.K.Lubsandorzhiev, Y.M.Malyshkin, R.Massarczyk, V.A.Matveev, I.N.Mirmov, J.S.Nico, A.L.Petelin, R.G.H.Robertson, D.Sinclair, A.A.Shikhin, V.A.Tarasov, G.V.Trubnikov, E.P.Veretenkin, J.F.Wilkerson, A.I.Zvir Results from the Baksan Experiment on Sterile Transitions (BEST) NUCLEAR REACTIONS 71Ga(ν, e-), E<1 MeV; measured reaction products, Eβ, Iβ; deduced the deficit of electron neutrinos observed in gallium-based radiochemical measurements with high-intensity neutrino sources, commonly referred to as the gallium anomaly. The Baksan Experiment on Sterile Transitions (BEST).
doi: 10.1103/PhysRevLett.128.232501
2022BA21 Phys.Rev. C 105, 065502 (2022) V.V.Barinov, S.N.Danshin, V.N.Gavrin, V.V.Gorbachev, D.S.Gorbunov, T.V.Ibragimova, Yu.P.Kozlova, L.V.Kravchuk, V.V.Kuzminov, B.K.Lubsandorzhiev, Yu.M.Malyshkin, I.N.Mirmov, A.A.Shikhin, E.P.Veretenkin, B.T.Cleveland, H.Ejiri, S.R.Elliott, I.Kim, R.Massarczyk, D.Frekers, W.C.Haxton, V.A.Matveev, G.V.Trubnikov, J.S.Nico, A.L.Petelin, V.A.Tarasov, A.I.Zvir, R.G.H.Robertson, D.Sinclair, J.F.Wilkerson Search for electron-neutrino transitions to sterile states in the BEST experiment NUCLEAR REACTIONS 71Ga(ν, e-), E<1 MeV; measured reaction products, Eb, Iβ; deduced 71Ge yields, deficit of electron neutrinos observed in gallium-based radiochemical measurements with high-intensity neutrino sources, commonly referred as "the gallium anomaly". The Baksan Experiment on Sterile Transitions (BEST). Neutrinos from decay of the 51Cr decay. RADIOACTIVITY 51Cr(EC); measured Eγ, Iγ, calorimetric heat; deduced T1/2.
doi: 10.1103/PhysRevC.105.065502
2021AS07 Phys.Rev. C 103, 065501 (2021) A.Ashtari Esfahani, M.Betancourt, Z.Bogorad, S.Boser, N.Buzinsky, R.Cervantes, C.Claessens, L.de Viveiros, M.Fertl, J.A.Formaggio, L.Gladstone, M.Grando, M.Guigue, J.Hartse, K.M.Heeger, X.Huyan, J.Johnston, A.M.Jones, K.Kazkaz, B.H.LaRoque, A.Lindman, R.Mohiuddin, B.Monreal, J.A.Nikkel, E.Novitski, N.S.Oblath, M.Ottiger, W.Pettus, R.G.H.Robertson, G.Rybka, L.Saldana, M.Schram, V.Sibille, P.L.Slocum, Y.-H.Sun, P.T.Surukuchi, J.R.Tedeschi, A.B.Telles, M.Thomas, T.Thummler, L.Tvrznikova, B.A.VanDevender, T.E.Weiss, T.Wendler, E.Zayas, A.Ziegler Bayesian analysis of a future β decay experiment's sensitivity to neutrino mass scale and ordering RADIOACTIVITY 3H(β-); analyzed sensitivity to the neutrino mass scale and ordering by Bayesian approach for a planned experiment 'Project-8 Collaboration' which aims to measure the neutrino mass to a sensitivity 40 meV by analyzing a spectrum produced in β- decay of atomic tritium through the technique of Cyclotron Radiation Emission Spectroscopy (CRES) for obtaining a high-precision β- spectrum by measuring the cyclotron frequencies of electrons in a magnetic field, followed by a computation of corresponding electron energies.
doi: 10.1103/PhysRevC.103.065501
2021FO07 Phys.Rep. 914, 1 (2021) J.A.Formaggio, A.L.C.de Gouvea, R.G.H.Robertson Direct measurements of neutrino mass RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 130Te, 136Xe, 150Nd(2β-); analyzed available data; deduced Majorana neutrino mass limit.
doi: 10.1016/j.physrep.2021.02.002
2020LI16 Phys.Rev.Lett. 124, 222502 (2020) Y.-T.Lin, T.H.Burritt, C.Claessens, G.Holman, M.Kallander, E.Machado, L.I.Minter, R.Ostertag, D.S.Parno, J.Pedersen, D.A.Peterson, R.G.H.Robertson, E.B.Smith, T.D.Van Wechel, A.P.Vizcaya Hernandez, for the TRIMS Collaboration Beta Decay of Molecular Tritium RADIOACTIVITY 3H(β-); measured decay products, Eβ, Iβ; deduced branching ratios and uncertainties to specific ionization states.
doi: 10.1103/PhysRevLett.124.222502
2020RO14 Phys.Rev. C 102, 035502 (2020) R.G.H.Robertson, V.Venkatapathy Shakeup and shakeoff satellite structure in the electron spectrum of 83Krm ATOMIC PHYSICS 83mKr; calculated shakeup and shakeoff spectrum, a satellite spectrum of the K-conversion line from the decay of 83Kr isomer, Kr 1s ionization cross sections and double excitation cross sections, Levinger distributions for 1s, 2s, and 2p shakeoff, Lorentzian and Levinger distributions for the shakeup and shakeoff spectrum of the 32-keV K line, correlation matrix for the fitted spectrum parameters from experimental data and theoretical calculations. Relevance to calibration standard for planned tritium beta decay neutrino mass experiments, such as Project 8 and, possibly, KATRIN.
doi: 10.1103/PhysRevC.102.035502
2017AS02 J.Phys.(London) G44, 054004 (2017) A.Ashtari Esfahani, D.M.Asner, S.Boser, R.Cervantes, C.Claessens, L.de Viveiros, P.J.Doe, S.Doeleman, J.L.Fernandes, M.Fertl, E.C.Finn, J.A.Formaggio, D.Furse, M.Guigue, K.M.Heeger, A.M.Jones, K.Kazkaz, J.A.Kofron, C.Lamb, B.H.LaRoque, E.Machado, E.L.McBride, M.L.Miller, B.Monreal, P.Mohanmurthy, J.A.Nikkel, N.S.Oblath, W.C.Pettus, R.G.H.Robertson, L.J.Rosenberg, G.Rybka, D.Rysewyk, L.Saldana, P.L.Slocum, M.G.Sternberg, J.R.Tedeschi, T.Thummler, B.A.VanDevender, L.E.Vertatschitsch, M.Wachtendonk, J.Weintroub, N.L.Woods, A.Young and E.M.Zayas Determining the neutrino mass with cyclotron radiation emission spectroscopy-Project 8
doi: 10.1088/1361-6471/aa5b4f
2015BO02 Phys.Rev. C 91, 035505 (2015) L.I.Bodine, D.S.Parno, R.G.H.Robertson Assessment of molecular effects on neutrino mass measurements from tritium β decay RADIOACTIVITY 3H(β-); analyzed and assessed molecular effects on neutrino mass measurements from β decay of tritium, schematic calculations of the recoil-fragment energy spectra following dissociation, role of molecular excitations in modifying the shape of the observed β spectrum in the vicinity of the end point. Relevance to upcoming Karlsruhe Tritium Neutrino (KATRIN) experiment of high statistical sensitivity and excellent resolution in the last 20 eV of the β spectrum.
doi: 10.1103/PhysRevC.91.035505
2015RO03 Phys.Rev. C 91, 035504 (2015) Examination of the calorimetric spectrum to determine the neutrino mass in low-energy electron capture decay RADIOACTIVITY 163Ho(EC); calculated atomic two-hole states in 163Dy with Carlson-Nestor photoionization model, visible (calorimetric) energy spectrum; deduced effect on neutrino mass measurement with calorimeters.
doi: 10.1103/PhysRevC.91.035504
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
2007BA75 Phys.Rev. C 76, 055806 (2007) M.K.Bacrania, N.M.Boyd, R.G.H.Robertson, D.W.Storm Search for the second forbidden β decay of 8B to the ground state of 8Be RADIOACTIVITY 8B(β+) [from 3He(6Li, n), E=15.5 MeV]; measured delayed α particles, branching ratio to the ground state of 8Be.
doi: 10.1103/PhysRevC.76.055806
2005NO02 Nucl.Phys. B(Proc.Supp.) S138, 221 (2005) M.Nomachi, P.Doe, H.Ejiri, S.R.Elliott, J.Engel, M.Finger, J.A.Formaggio, K.Fushimi, V.Gehman, A.Gorin, M.Greenfield, R.Hazama, K.Ichihara, Y.Ikegami, H.Ishii, T.Itahashi, P.Kavitov, V.Kekelidze, K.Kuroda, V.Kutsalo, I.Manouilov, K.Matsuoka, H.Nakamura, T.Ogama, A.Para, K.Rielage, A.Rjazantsev, R.G.H.Robertson, Y.Shichijo, T.Shima, Y.Shimada, G.Shirkov, A.Sissakian, Y.Sugaya, A.Titov, V.Vatulin, O.E.Vilches, V.Voronov, J.F.Wilkerson, D.I.Will, S.Yoshida MOON (Mo Observatory Of Neutrinos) for double beta decay
doi: 10.1016/j.nuclphysbps.2004.11.053
2004BB06 Nucl.Phys. A746, 463c (2004) M.K.Bacrania, D.W.Storm, R.G.H.Robertson Search for the 8B(2+) → 8Be(0+) ground-state transition RADIOACTIVITY 8B(β+) [from 6Li(3He, n)]; measured β-delayed Eα, βγ-coin; deduced upper limit for ground-state transition branching ratio.
doi: 10.1016/j.nuclphysa.2004.09.073
2004ST01 Phys.Rev. C 69, 015801 (2004) L.C.Stonehill, J.A.Formaggio, R.G.H.Robertson Solar neutrinos from CNO electron capture NUCLEAR REACTIONS 13N, 15O, 17F(e, ν), E=low; calculated solar neutrino flux from electron capture.
doi: 10.1103/PhysRevC.69.015801
2003CH10 Phys.Rev. C 67, 025801 (2003) J.-W.Chen, K.M.Heeger, R.G.H.Robertson Constraining the leading weak axial two-body current by recent solar neutrino flux data
doi: 10.1103/PhysRevC.67.025801
2003DO13 Nucl.Phys. A721, 517c (2003) P.Doe, H.Ejiri, S.R.Elliott, J.Engel, M.Finger, K.Fushimi, V.Gehman, A.Gorine, M.Greenfield, R.Hazama, K.Ichihara, T.Itahashi, P.Kavitov, V.Kekelidze, K.Kuroda, V.Kutsalo, K.Matsuoka, I.Manouilov, M.Nomachi, A.Para, A.Rjazantsev, R.G.H.Robertson, Y.Shichijo, L.C.Stonehill, T.Shima, G.Shirkov, A.Sissakian, Y.Sugaya, A.Titov, V.Vatulin, V.Voronov, O.E.Vilches, J.F.Wilkerson, D.I.Will, S.Yoshida Neutrino Studies in 100Mo and MOON - Mo Observatory of Neutrinos -
doi: 10.1016/S0375-9474(03)01113-8
2002EJ05 Nucl.Phys. B(Proc.Supp.) S110, 375 (2002) H.Ejiri, J.Engel, K.Fushimi, K.Hayashi, R.Hazama, T.Kishimoto, P.Krastev, N.Kudomi, K.Kume, H.Kuramoto, K.Matsuoka, R.G.H.Robertson, K.Takahisa, S.Yoshida Double Beta Decays of 100Mo and Molybdenum Observatory of Neutrinos RADIOACTIVITY 100Mo(2β-); measured β-spectra, 2ν-accompanied 2β-decay T1/2, 0ν-accompanied 2β-decay T1/2 lower limit.
doi: 10.1016/S0920-5632(02)01514-1
2000EJ01 Phys.Rev.Lett. 85, 2917 (2000) H.Ejiri, J.Engel, R.Hazama, P.Krastev, N.Kudomi, R.G.H.Robertson Spectroscopy of Double-Beta and Inverse-Beta Decays from 100Mo for Neutrinos RADIOACTIVITY 100Mo(2β-); calculated 0ν-, 2ν-accompanied 2β decay spectra, correlation features. Detector design, solar neutrino detection discussed.
doi: 10.1103/PhysRevLett.85.2917
2000JO03 Nucl.Instrum.Methods Phys.Res. A440, 648 (2000) G.L.Jones, J.M.Adams, J.M.Anaya, T.J.Bowles, T.E.Chupp, K.P.Coulter, M.S.Dewey, S.J.Freedman, B.K.Fujikawa, A.Garcia, G.L.Greene, S.-R.Hwang, L.J.Lising, H.P.Mumm, J.S.Nico, R.G.H.Robertson, T.D.Steiger, W.A.Teasdale, A.K.Thompson, E.G.Wasserman, F.E.Wietfeldt, J.F.Wilkerson Time Reversal in Polarized Neutron Decay: The emiT experiment RADIOACTIVITY 1n(β-); measured proton-electron correlations following polarized neutron decay.
doi: 10.1016/S0168-9002(99)01056-6
2000LI42 Phys.Rev. C62, 055501 (2000) L.J.Lising, S.R.Hwang, J.M.Adams, T.J.Bowles, M.C.Browne, T.E.Chupp, K.P.Coulter, M.S.Dewey, S.J.Freedman, B.K.Fujikawa, A.Garcia, G.L.Greene, G.L.Jones, H.P.Mumm, J.S.Nico, J.M.Richardson, R.G.H.Robertson, T.D.Steiger, W.A.Teasdale, A.K.Thompson, E.G.Wasserman, F.E.Wietfeldt, R.C.Welsh, J.F.Wilkerson, and the emiT Collaboration New Limit on the D Coefficient in Polarized Neutron Decay RADIOACTIVITY 1n(β-); measured pβ-coin following polarized neutron decay; deduced limits on time-reversal invariance coefficient.
doi: 10.1103/PhysRevC.62.055501
2000PO21 Nucl.Instrum.Methods Phys.Res. A452, 115 (2000) A.W.P.Poon, R.J.Komar, C.E.Waltham, M.C.Browne, R.G.H.Robertson, N.P.Kherani, H.B.Mak A Compact 3H(p, γ)4He 19.8-MeV Gamma-Ray Source for Energy Calibration at the Sudbury Neutrino Observatory NUCLEAR REACTIONS 3H(p, γ), (p, X), E=29 keV; measured Eγ, Iγ, neutron yields. Calibration source for neutrino observatory.
doi: 10.1016/S0168-9002(00)00424-1
1999HA01 Phys.Rev. C59, 515 (1999) Solar Neutrino Interactions with 18O in the SuperKamiokande Water Cerenkov Detector
doi: 10.1103/PhysRevC.59.515
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
1998RO33 Prog.Part.Nucl.Phys. 40, 113 (1998) R.G.H.Robertson, for the Sudbury Neutrino Observatory Collaboration Neutral-Current Detection via 3He(n, p)3H in the Sudbury Neutrino Observatory NUCLEAR REACTIONS 3He(n, p), E=thermal; analyzed data; deduced neutron capture rate for solar neutrino detection.
doi: 10.1016/S0146-6410(98)00015-5
1991RO07 Phys.Rev.Lett. 67, 957 (1991) R.G.H.Robertson, T.J.Bowles, G.J.Stephenson, Jr., D.L.Wark, J.F.Wilkerson, D.A.Knapp Limit on (ν-bar(e)) Mass from Observation of the β Decay of Molecular Tritium RADIOACTIVITY 3H; measured β-decay spectrum shape; deduced electron antineutrino mass upper limit. Molecular tritium.
doi: 10.1103/PhysRevLett.67.957
1989RE04 Phys.Rev. C40, 368 (1989) Binding of Hydrogen and Helium in Silicon, the Mass Difference between 3H and 3He, and the Mass of ν(e) RADIOACTIVITY 3H(β-); calculated chemical correction to β endpoint energy; deduced m(ν). 3H, 3He deduced mass difference. ATOMIC MASSES 3H, 3He; calculated chemical correction to β-endpoint energy; deduced mass, m(ν).
doi: 10.1103/PhysRevC.40.368
1989ST05 Phys.Rev. C39, 1503 (1989) S.T.Staggs, R.G.H.Robertson, D.L.Wark, P.P.Nguyen, J.F.Wilkerson, T.J.Bowles Energy of the 32-keV Transition of 83mKr and the Atomic Mass Difference between 3H and 3He RADIOACTIVITY 83mKr(IT); 3H(β-); measured E(γ), I(γ). 83Kr deduced transition energy. 3H, 3He deduced atomic mass difference.
doi: 10.1103/PhysRevC.39.1503
1988RO21 Ann.Rev.Nucl.Part.Sci. 38, 185 (1988) Direct Measurements of Neutrino Mass
doi: 10.1146/annurev.ns.38.120188.001153
1988WI07 Nucl.Phys. A478, 439c (1988) J.F.Wilkerson, T.J.Bowles, D.A.Knapp, M.P.Maley, R.G.H.Robertson, D.L.Wark Limit on ν(bar)(e) Mass from Free Molecular Tritium Beta Decay RADIOACTIVITY 3H(β-); measured β-spectra; deduced neutrino mass upper limit. Free molecular tritium source.
doi: 10.1016/0375-9474(88)90878-0
1987WI07 Phys.Rev.Lett. 58, 2023 (1987) J.F.Wilkerson, T.J.Bowles, M.P.Maley, R.G.H.Robertson, J.S.Cohen, R.L.Martin, D.A.Knapp, J.A.Helffrich Limit on (ν-bar(e)) Mass from Free-Molecular-Tritium Beta Decay RADIOACTIVITY 3H(β-); measured molecular beta spectrum; deduced electron-antineutrino mass limit. Si detector, beta spectrometer.
doi: 10.1103/PhysRevLett.58.2023
1984RO04 Phys.Rev. C29, 755 (1984) R.G.H.Robertson, P.Dyer, R.C.Melin, T.J.Bowles, A.B.McDonald, G.C.Ball, W.G.Davies, E.D.Earle Upper Limit on the Isovector Parity-Violating Decay Width of the 0+ T = 1 State of 6Li NUCLEAR REACTIONS, ICPND 2H(α, γ), E=6.24 MeV; measured capture σ. 6Li level deduced isovector parity violating decay Γ upper limit.
doi: 10.1103/PhysRevC.29.755
1983GA03 Phys.Rev. C27, 1353 (1983) C.A.Gagliardi, G.T.Garvey, N.Jarmie, R.G.H.Robertson 0+ → 0- Beta Decay of 16C RADIOACTIVITY 16C(β-), (β-n) [from 14C(t, p), E=6 MeV]; measured β(t), γ(t), βγ-coin; deduced log ft. 16N levels deduced β-branching ratio.
doi: 10.1103/PhysRevC.27.1353
1983RO12 Phys.Rev. C28, 443 (1983) Estimate of the Parity-Violating α-Decay Width of the 0+, T = 1 State of 6Li NUCLEAR STRUCTURE 6Li; calculated parity violating α-decay width; deduced pion exchange contribution. Shell model.
doi: 10.1103/PhysRevC.28.443
1981MC14 Phys.Rev.Lett. 47, 1720 (1981) A.B.McDonald, E.D.Earle, J.J.Simpson, R.G.H.Robertson, H.B.Mak Measurement of Pair Emission from the 2.8-MeV Parity-Mixed Doublet of 21Ne RADIOACTIVITY 21Ne [from 18O(α, n), E=4.48, 4.85, 4.95 MeV]; measured pair emission relative branching ratios. 21Ne transition deduced γ-multipolarity, δ lower limit.
doi: 10.1103/PhysRevLett.47.1720
1981RO02 Phys.Rev. C23, 973 (1981) R.G.H.Robertson, J.A.Nolen, Jr., T.Chapuran, R.Vodhanel Mass of 6Li and the Excitation Energy of its 3.56-MeV State NUCLEAR REACTIONS 6Li(γ, γ'), E=7 MeV bremsstrahlung; measured Eγ. 6Li level deduced energy. Ge(Li) detector. 6Li(p, α), E=10.5 MeV; measured Q. 6Li deduced mass excess. Magnetic spectrograph.
doi: 10.1103/PhysRevC.23.973
1981RO12 Phys.Rev.Lett. 47, 1867 (1981); Erratum Phys.Rev.Lett. 75, 4334 (1995) R.G.H.Robertson, P.Dyer, R.A.Warner, R.C.Melin, T.J.Bowles, A.B.McDonald, G.C.Ball, W.G.Davies, E.D.Earle Observation of the Capture Reaction 2H(α, γ)6Li and Its Role in Production of 6Li in the Big Bang NUCLEAR REACTIONS 2H(α, γ), E(cm)=1, 1.33, 1.63, 2.08, 2.33, 3.01 MeV; measured σ(capture) vs E; deduced 6Li production role in big bang. Recoil 6Li ion detection, magnetic analysis.
doi: 10.1103/PhysRevLett.47.1867
1980LE18 Phys.Rev. C22, 1723 (1980) A.G.Ledebuhr, L.H.Harwood, R.G.H.Robertson, T.J.Bowles Test of the Isobaric Multiplet Mass Equation from β-Delayed Proton Decay of 24Si RADIOACTIVITY 24Si [from 24Mg(3He, 3n)]; measured T1/2, β-delayed Ep. Isobaric multiplet mass equation.
doi: 10.1103/PhysRevC.22.1723
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
1979ZW01 Nucl.Phys. A315, 124 (1979) B.Zwieglinski, W.Benenson, R.G.H.Robertson, W.R.Coker Study of the 10Be(d, p)11Be Reaction at 25 MeV NUCLEAR REACTIONS 10Be(d, p), E=25 MeV; measured σ(θ). 11Be levels deduced S, DWBA analysis. Comparison with shell model. Reactor-produced 10Be target.
doi: 10.1016/0375-9474(79)90637-7
1978BE26 Phys.Rev. C17, 1939 (1978) W.Benenson, E.Kashy, A.G.Ledebuhr, R.C.Pardo, R.G.H.Robertson, L.W.Robinson T = 3/2 Levels in 15F and 15O NUCLEAR REACTIONS 20Ne(3He, 8Li), E=74.5 MeV; 17O(p, t), E=45 MeV; measured σ; deduced Q. 15F deduced mass excess, levels, Γ. 15O deduced analog level, Γ, proton branching.
doi: 10.1103/PhysRevC.17.1939
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
1978RO01 Phys.Rev. C17, 4 (1978) R.G.H.Robertson, E.Kashy, W.Benenson, A.Ledebuhr Mass of 6He NUCLEAR REACTIONS 7Li, 19F(d, 3He), E=20.8 MeV; measured σ; deduced Q. 6He deduced mass excess.
doi: 10.1103/PhysRevC.17.4
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
1977KO14 Nucl.Phys. A286, 253 (1977) R.Kouzes, J.Lind, W.H.Moore, R.G.H.Robertson, R.Sherr Investigation of the (3He, 8He) Reaction on 58Ni and 64Ni NUCLEAR REACTIONS 58,64Ni(3He, 8He), E=75.3 MeV; measured σ.
doi: 10.1016/0375-9474(77)90406-7
1977RO05 Phys.Rev. C15, 1072 (1977) R.G.H.Robertson, R.A.Warner, S.M.Austin Measurement of the Internal Pair Emission Branch of the 7.654-MeV State of 12C, and the Rate of the Stellar Triple-α Reaction NUCLEAR REACTIONS 12C(p, p'), E=10.5 MeV; measured p' pair-coin. 12C level deduced Γπ/Γ. Stellar helium burning.
doi: 10.1103/PhysRevC.15.1072
1976KH03 Phys.Rev.Lett. 37, 823 (1976) T.L.Khoo, F.M.Bernthal, R.G.H.Robertson, R.A.Warner High-Spin Multiquasiparticle Yrast Traps in 176Hf NUCLEAR REACTIONS 176Yb(α, 4nγ), E=48 MeV; measured I(ce), γγ(t), γ(t), σ(Eγ, θ). 176Hf deduced levels, K, J, π, λ, g.
doi: 10.1103/PhysRevLett.37.823
1976RO04 Phys.Rev. C13, 1018 (1976) R.G.H.Robertson, W.Benenson, E.Kashy, D.Mueller Measurement of the Mass of 8C by the 14N(3He, 9Li) Reaction NUCLEAR REACTIONS 14N(3He, 9Li), E=76 MeV; measured σ(θ), Q. 8C deduced mass excess, Γ.
doi: 10.1103/PhysRevC.13.1018
1975KA18 Phys.Rev. C11, 1959 (1975) E.Kashy, W.Benenson, D.Mueller, R.G.H.Robertson, D.R.Goosman Mass of 9Li NUCLEAR REACTIONS 10Be(d, 3He), E=23.92 MeV; measured σ(E(3He)). 9Li deduced mass excess.
doi: 10.1103/PhysRevC.11.1959
1975RO01 Phys.Rev.Lett. 34, 33 (1975) R.G.H.Robertson, W.S.Chien, D.R.Goosman Complete Isobaric Quintet NUCLEAR REACTIONS 11B(3He, 6He), E=72 MeV; measured σ(E(6He), θ); 10B(p, t), (p, 3He), E=45 MeV; measured σ(Et, θ), σ(E(3He), θ); deduced Q. 8B, 8Li, 8Be deduced T=2 levels, completed isobaric quintet.
doi: 10.1103/PhysRevLett.34.33
1974RO16 Phys.Rev. C9, 1801 (1974) Neutron-Deficient Isotopes 64Ge and 65Ge NUCLEAR REACTIONS 64Zn(p, nγ), E=7.8-9.5 MeV; measured σ(E, Eγ); 64Zn(3He, t), E=37.6 MeV; measured Q, σ(Et); 64Zn(3He, 2n), (3He, 3n), (3He, p2n), E=20-70 MeV; measured σ(E). 64Ga deduced levels. RADIOACTIVITY 64,65Ge; measured T1/2, Eγ, Iγ, deduced log ft. 64,65Ga deduced levels, J, π.
doi: 10.1103/PhysRevC.9.1801
1974RO17 Phys.Rev.Lett. 32, 1207 (1974) R.G.H.Robertson, S.Martin, W.R.Falk, D.Ingham, A.Djaloeis Highly Proton-Rich T(z) = -2 Nuclides: 8C and 20Mg NUCLEAR REACTIONS C, 24Mg(α, 8He), E=156 MeV; measured Q, σ. 8C, 20Mg deduced mass excess.
doi: 10.1103/PhysRevLett.32.1207
1973RO08 Phys.Rev. C7, 543 (1973) Proton Capture by 7Be and the Solar Neutrino Problem NUCLEAR REACTIONS 7Be(p, γ), E < 1.5 MeV; analyzed σ(E).
doi: 10.1103/PhysRevC.7.543
1973RO22 Phys.Rev. C8, 241 (1973) R.G.H.Robertson, B.H.Wildenthal Shell-Model Study of 24Ne NUCLEAR STRUCTURE 24Mg; calculated binding energy. 24Ne; calculated levels, J, π, log ft, T1/2, B(M1), B(M2). 24Si; calculated mass log ft, T1/2. NUCLEAR REACTIONS 20Ne(t, p); measured nothing, calculated pair transfer amplitude.
doi: 10.1103/PhysRevC.8.241
1972RO13 Phys.Rev.Lett. 29, 130 (1972) Germanium-64 RADIOACTIVITY 64Ge[from 64Zn(3He, 3n)]; measured T1/2, Eγ, Iγ; deduced log ft. 64Ga deduced levels, J, π.
doi: 10.1103/PhysRevLett.29.130
1971RO08 Can.J.Phys. 49, 1186 (1971) R.G.H.Robertson, R.G.Summers-Gill Low-Lying Levels of 58Co NUCLEAR REACTIONS 59Co(d, t), E=15, 16.5 MeV; measured σ(Et, θ). 55Mn(α, nγ), E=10 MeV; measured Eγ, Iγ, γγ-coin, γγ-delay. 58Co deduced levels, J, π, T1/2, S, γ-branching.
doi: 10.1139/p71-143
1971RO21 Can.J.Phys. 49, 2227 (1971) R.G.H.Robertson, Sung Ho Choh, R.G.Summers-Gill, C.V.Stager Spin and Magnetic Moment of 151Sm NUCLEAR MOMENTS 151Sm; measured J, μ. EPR.
doi: 10.1139/p71-270
1968RO08 Priv.Comm. (1968) NUCLEAR STRUCTURE 60Co; measured not abstracted; deduced nuclear properties.
1968RO16 Can.J.Phys. 46, 2499 (1968) R.G.H.Robertson, J.C.Waddington, R.G.Summers-Gill Hyperfine Interactions in the J = 5 States of 147Sm and 149Sm NUCLEAR STRUCTURE 147Sm, 149Sm; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p68-610
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