NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.Anderson Found 21 matches. 2020AN11 Phys.Rev. C 102, 014002 (2020) M.R.Anderson, for the SNO+ Collaboration Measurement of neutron-proton capture in the SNO+ water phase NUCLEAR REACTIONS 1H(n, γ), E=thermal, [neutrons from Am-Be calibration source]; measured Eγ, Iγ, and γγ-coin from calibration source and neutron captures using the SNO+ water Cherenkov detectors; deduced neutron detection efficiency, neutron capture time constant and thermal neutron-proton capture cross section.
doi: 10.1103/PhysRevC.102.014002
2014MY01 Phys.Rev. C 89, 035202 (2014) L.S.Myers, K.Shoniyozov, M.F.Preston, M.D.Anderson, J.R.M.Annand, M.Boselli, W.J.Briscoe, J.Brudvik, J.I.Capone, G.Feldman, K.G.Fissum, K.Hansen, S.S.Henshaw, L.Isaksson, R.Jebali, M.A.Kovash, K.Lewis, M.Lundin, I.J.D.MacGregor, D.G.Middleton, D.E.Mittelberger, M.Murray, A.M.Nathan, S.Nutbeam, G.V.O'Rielly, B.Schroder, B.Seitz, S.C.Stave, H.R.Weller, for the COMPTON @ MAX-lab Collaboration Compton scattering from 12C using tagged photons in the energy range 65-115 MeV NUCLEAR REACTIONS 12C(γ, γ), E=65-115 MeV; measured photon spectra, σ(E, θ) at Tagged-Photon Facility of the MAX IV-Lund Laboratory; deduced bound-nucleon polarizabilities. GEANT4 lineshape analysis of Compton-scattered photon spectrum. Phenomenological model. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.89.035202
2002PI05 Nucl.Phys. A698, 495c (2002) C.Pinkenburg, N.N.Ajitanand, J.M.Alexander, M.Anderson, D.Best, F.P.Brady, T.Case, W.Caskey, D.Cebra, J.L.Chance, P.Chung, B.Cole, K.Crowe, A.C.Das, J.E.Draper, M.L.Gilkes, S.Gushue, M.Heffner, A.S.Hirsch, E.L.Hjort, L.Huo, M.Justice, M.Kaplan, D.Keane, J.C.Kintner, J.Klay, D.Krofcheck, R.A.Lacey, C.Law, J.Lauret, M.A.Lisa, H.Liu, Y.M.Liu, R.L.McGrath, Z.Milosevich, G.Odyniec, D.L.Olson, S.Panitkin, N.T.Porile, G.Rai, H.G.Ritter, J.L.Romero, R.Scharenberg, L.S.Schroeder, B.Srivastava, N.T.B.Stone, T.J.M.Symons, S.Wang, J.Whitfield, R.Witt, L.Wood, W.N.Zhang Production and Collective Behavior of Strange Particles in Au + Au Collisions at 2-8A GeV NUCLEAR REACTIONS 197Au(197Au, X), E=2-8 GeV/nucleon; measured hyperon and kaon yields, sideward flow.
doi: 10.1016/S0375-9474(01)01412-9
2001CH09 J.Phys.(London) G27, 293 (2001) P.Chung, J.M.Alexander, N.N.Ajitanand, M.Anderson, D.Best, E.P.Brady, T.Case, W.Caskey, D.Cebra, J.L.Chance, B.Cole, K.Crowe, A.C.Das, J.E.Draper, M.L.Gilkes, S.Gushue, M.Heffner, A.S.Hirsch, E.L.Hjort, L.Huo, M.Justice, M.Kaplan, D.Keane, J.C.Kintner, J.Klay, D.Krofcheck, R.A.Lacey, C.Law, J.Lauret, M.A.Lisa, H.Liu, Y.M.Liu, R.McGrath, Z.Milosevich, G.Odyniec, D.L.Olson, S.Panitkin, C.Pinkenburg, N.T.Porile, G.Rai, H.G.Ritter, J.L.Romero, R.Scharenberg, L.Schroeder, B.Srivastava, N.T.B.Stone, T.J.M.Symons, J.Whitfield, R.Witt, L.Wood, W.N.Zhang Λ Flow and Λ-P Correlation in Au + Au Collisions at AGS Energies NUCLEAR REACTIONS 197Au(197Au, X), E=2, 4, 6 GeV/nucleon; measured hyperon transverse and radial flow, hyperon-proton correlations. Comparison with model predictions.
doi: 10.1088/0954-3899/27/3/306
1996LE22 Nucl.Instrum.Methods Phys.Res. A374, 299 (1996) M.J.Leitch, M.E.Anderson, J.Kapustinsky, T.K.Li, C.S.Mishra, J.C.Peng, J.E.Simmons, S.A.Dytman, J.G.Hardie, K.F.Von Reden, C.Smith Performance of a BGO-NaI η Spectrometer NUCLEAR REACTIONS 1H(π-, X), E at 200, 698 MeV/c; measured missing mass, invariant mass spectra for π0, η production. Performance of two-arm spectrometer with BGO actiuve converters discussed.
doi: 10.1016/0168-9002(96)00181-7
1994AN31 Chem.Phys.Lett. 224, 381 (1994) Metal Hyperfine Structure in Magnesium Chloride. The Millimeter-Wave Spectrum of 25MgCl and 26MgCl NUCLEAR MOMENTS 26Mg, 25Mg; measured NMR in MgCl(X2Σ+); deduced Fermi contact term average value, electron density at Mg nucleus.
doi: 10.1016/0009-2614(94)00532-X
1983AN11 Nucl.Phys. A405, 170 (1983) M.R.Anderson, L.W.Mitchell, M.E.Sevior, D.G.Sargood 25Mg(α, n)28Si and 26Mg(α, n)29Si as Neutron Sources in Explosive Neon Burning NUCLEAR REACTIONS, ICPND 25Mg(α, n), (α, nγ), E=1.8-6.3 MeV; 26Mg(α, n), E=1.8-6 MeV; measured neutron, γ-ray yields; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched targets.
doi: 10.1016/0375-9474(83)90330-5
1983SE19 Aust.J.Phys. 36, 463 (1983); Corrigendum Aust.J.Phys. 37, 709 (1984) M.E.Sevior, L.W.Mitchell, M.R.Anderson, C.I.W.Tingwell, D.G.Sargood Absolute Cross Sections of Proton Induced Reactions on 65Cu, 64Ni and 63Cu NUCLEAR REACTIONS, ICPND 65Cu(p, γ), E=1.05-3.25 MeV; 63Cu(p, γ), E=1.05-4.7 MeV; 64Ni(p, γ), E=1-3.45 MeV; 63Cu(p, p'), E=1.05-4 MeV; 65Cu(p, n), E=threshold-3.25 MeV; 64Ni(p, n), E=threshold-3.8 MeV; 63Cu(p, n), E=threshold-4.86 MeV; measured absolute σ(E). Global statistical model calculations.
doi: 10.1071/PH830463
1982AN01 Nucl.Phys. A373, 326 (1982) M.R.Anderson, L.W.Mitchell, M.E.Sevior, S.R.Kennett, D.G.Sargood Resonance Strength Measurements and Thermonuclear Reaction Rates for 25Mg(p, γ)26Al (II) NUCLEAR REACTIONS, ICPND 25Mg(p, γ), E=600-1730 keV; measured σ(E). 26Al deduced resonance strengths, thermonuclear reaction rates. Statistical-model analysis. Enriched target.
doi: 10.1016/0375-9474(82)90154-3
1982MI06 Nucl.Phys. A380, 318 (1982) L.W.Mitchell, M.R.Anderson, S.R.Kennett, D.G.Sargood Cross Sections and Thermonuclear Reaction Rates for 42Ca(p, γ)43Sc, 44Ca(p, γ)45Sc, 44Ca(p, n)44Sc and 45Sc(p, n)45Ti NUCLEAR REACTIONS, ICPND 42Ca(p, γ), (p, p'γ), E=0.63-3.01 MeV; 44Ca(p, γ), (p, p'γ), (p, n), E=0.775-5.05 MeV; 45Sc(p, n), E=2.9-4 MeV; measured γ-ray, neutron yields, residual activities; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched Ca, natural Sc targets.
doi: 10.1016/0375-9474(82)90108-7
1982SE02 Nucl.Phys. A378, 349 (1982) M.E.Sevior, M.R.Anderson, L.W.Mitchell, S.R.Kennett, D.G.Sargood Thermonuclear Reaction Rates for Proton Induced Reactions on 41K and Neutron Induced Reactions on 41Ca NUCLEAR REACTIONS, ICPND 41K(p, γ), (p, n), (p, α), E=0.68-2.48 MeV; measured γ, neutron yields; deduced σ(E), thermonuclear reaction rates for these and inverse reactions. Statistical model analysis. Natural target.
doi: 10.1016/0375-9474(82)90598-X
1981AN23 Aust.J.Phys. 34, 105 (1981) M.R.Anderson, S.R.Kennett, M.E.Sevior, D.G.Sargood 45Sc(p, p')45Sc* and the Attainment of a Thermal Distribution of States in an Astrophysical Environment NUCLEAR REACTIONS 45Sc(p, p'), E=1.2-2.5 MeV; measured σ(E). Activation technique. Statistical model. NUCLEAR STRUCTURE 45Sc; calculated thermal state distribution. Astrophysical enviroment, statistical model, reaction data input, explosive silicon burning.
doi: 10.1071/PH810105
1981GA38 Aust.J.Phys. 34, 25 (1981) H.J.Gardner, L.W.Mitchell, S.R.Kennett, M.R.Anderson, D.G.Sargood Cross Section Measurements for the Reactions 54Cr(p, γ)54Mn, 53Cr(p, n)53Mn and 53Cr(p, p')53Cr NUCLEAR REACTIONS 53Cr(p, γ), (p, n), (p, p'), E=0.88-2.4 MeV; measured σ(E). 54Mn deduced IAS. Ge(Li), BF3 neutron detectors. Statistical, global optical model analyses.
doi: 10.1071/PH810025
1981KE06 Nucl.Phys. A363, 233 (1981) S.R.Kennett, L.W.Mitchell, M.R.Anderson, D.G.Sargood Cross-Section Measurements and Thermonuclear Reaction Rates for 52Cr(p, α)53Mn and 54Fe(p, γ)55Co NUCLEAR REACTIONS 52Cr(p, γ), (p, p'γ), E=0.84-4 MeV; 54Fe(p, γ), (p, p'γ), E=1.05-3.69 MeV; measured γ-ray yields; deduced σ(E), thermonuclear reaction rates. Statistical model analysis. Enriched targets.
doi: 10.1016/0375-9474(81)90463-2
1981KE09 Nucl.Phys. A368, 337 (1981) S.R.Kennett, L.W.Mitchell, M.R.Anderson, D.G.Sargood Cross-Section Measurements and Thermonuclear Reactions Rates for 46Ti(p, γ)47V, 47Ti(p, γ)48V, 47Ti(p, n)47V and 48Ti(p, γ)49V NUCLEAR REACTIONS 46Ti(p, γ), (p, p'γ), E=0.72-3 MeV; 47Ti(p, p'γ), (p, n), E=0.74-3.5 MeV; 48Ti(p, γ), (p, p'γ), E=0.72-4.4 MeV; measured γ, neutron yields; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched targets.
doi: 10.1016/0375-9474(81)90689-8
1980AN25 Nucl.Phys. A349, 154 (1980) M.R.Anderson, S.R.Kennett, L.W.Mitchell, D.G.Sargood Resonance Strength Measurements and Thermonuclear Reaction Rates for 25Mg(p, γ)26Al NUCLEAR REACTIONS 25Mg(p, γ), E=317-591 keV; measured σ(Ep). 26Al deduced resonance strengths, thermonuclear reaction rates. Statistical model. Enriched target.
doi: 10.1016/0375-9474(80)90450-9
1980KE09 Nucl.Phys. A344, 351 (1980) S.R.Kennett, M.R.Anderson, Z.E.Switkowski, D.G.Sargood Cross-Section Measurements and Thermonuclear Reaction Rates for 49Ti(p, γ)50V and 49Ti(p, n)49V NUCLEAR REACTIONS 49Ti(p, γ), (p, n), E=0.74-3.25 MeV; measured σ(Eγ), σ(En); deduced σ(E), thermonuclear reaction rates. Statistical model. Enriched target.
doi: 10.1016/0375-9474(80)90683-1
1980KE11 Nucl.Phys. A346, 523 (1980) S.R.Kennett, M.R.Anderson, L.W.Mitchell, Z.E.Switkowski, D.G.Sargood Cross-Section Measurements and Thermonuclear Reaction Rates for 50Ti(p, γ)51V and 50Ti(p, n)50V NUCLEAR REACTIONS 50Ti(p, γ), (p, p'), (p, n), E=0.73-4.39 MeV; measured σ(Eγ), σ(En); deduced σ(E), thermonuclear reaction rates. Enriched target. Statistical model analysis.
doi: 10.1016/0375-9474(80)90484-4
1979AN04 Nucl.Phys. A318, 471 (1979) M.R.Anderson, S.R.Kennett, Z.E.Switkowski, D.G.Sargood The 56Fe(α, γ)60Ni Reaction Cross Section NUCLEAR REACTIONS 56Fe(α, γ), (α, nγ), (α, α'γ), E=4.2-7.1 MeV; measured γ-ray yields; deduced σ(E). Statistical model analysis. Enriched target.
doi: 10.1016/0375-9474(79)90661-4
1977AN13 Nucl.Sci.Eng. 62, 511 (1977) The Half-Life of Cobalt-56 RADIOACTIVITY 56Co; measured T1/2.
doi: 10.13182/NSE77-A26988
1972AN31 Nucl.Instrum.Methods 99, 231 (1972) Neutron energy spectra of different size 239Pu-Be (α, n) Sources NUCLEAR REACTIONS 9Be(α, n), E=5.15 MeV; measured reaction products, En, In; deduced relative σ(E).
doi: 10.1016/0029-554X(72)90781-1
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