NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = L.W.Mitchell Found 27 matches. 1996VO07 Phys.Rev. C53, 1945 (1996) R.B.Vogelaar, L.W.Mitchell, R.W.Kavanagh, A.E.Champagne, P.V.Magnus, M.S.Smith, A.J.Howard, P.D.Parker, H.A.O'Brien Constraining 26Al + p Resonances using 26Al(3He, d)27Si NUCLEAR REACTIONS 26Al(3He, d), E=20 MeV; measured σ(Ed), σ(θ); deduced implications for 26Al(p, γ) stellar reaction rate, model parameters. 27Si deduced levels, resonance, spectroscopic factors.
doi: 10.1103/PhysRevC.53.1945
1995MA90 Nucl.Instrum.Methods Phys.Res. A359, 506 (1995) Ion Transport in Xenon Gas Applications to Double Beta Decay RADIOACTIVITY 212Pb(β-); 212Bi(α) [from 212Pb(β-decay)]; measured 208Tl ions yield vs Xe pressure at given electric field, also vs drift field at fixed pressure; deduced applications to 2β-decay of 136Xe. Ion transport in Xe gas.
doi: 10.1016/0168-9002(95)00178-6
1993VU02 Phys.Rev. D48, 1009 (1993) J.-C.Vuilleumier, J.Busto, J.Farine, V.Jorgens, L.W.Mitchell, M.Treichel, J.-L.Vuilleumier, H.T.Wong, F.Boehm, P.Fisher, H.E.Henrikson, D.A.Imel, M.Z.Iqbal, B.M.O'Callaghan-Hay, J.Thomas, K.Gabathuler Search for Neutrinoless Double-β Decay in 136Xe with a Time Projection Chamber RADIOACTIVITY 136Xe(2β); measured 0ν-, 2ν-accompanied 2β-decay T1/2 lower limits. Xenon time projection chamber, underground measurement.
doi: 10.1103/PhysRevD.48.1009
1992RE03 Phys.Rev. D45, 2548 (1992) D.Reusser, M.Treichel, F.Boehm, P.Fisher, K.Gabathuler, H.E.Henrikson, V.Jorgens, L.W.Mitchell, C.Nussbaum, J.-L.Vuilleumier Final Report on the Search for Neutrinoless Double-β Decay of 76Ge from the Gotthard Underground Experiment RADIOACTIVITY 76Ge(2β); measured T1/2 lower limit; deduced neutrino Majorana mass upper limit. Gotthard underground laboratory, high purity natual Ge crystal array.
doi: 10.1103/PhysRevD.45.2548
1991TR07 J.Phys.(London) G17, S193 (1991) M.Treichel, F.Boehm, C.Broggini, D.Reusser, P.Fisher, L.Fluri, K.Gabathuler, H.Henrikson, V.Jorgens, L.W.Mitchell, C.Nussbaum, J.-L.Vuilleumier Double Beta Decay and Dark Matter in the Gotthard Germanium Experiment RADIOACTIVITY 76Ge(2β); measured 0ν-accompanied 2β-decay T1/2 lower limit. High purity Ge crystal detector, Gotthard road tunnel.
doi: 10.1088/0954-3899/17/S/020
1991WO03 Phys.Rev.Lett. 67, 1218 (1991) H.T.Wong, F.Boehm, P.Fisher, K.Gabathuler, H.E.Henrikson, D.A.Imel, M.Z.Iqbal, V.Jorgens, L.W.Mitchell, B.M.O'Callaghan-Hay, J.Thomas, M.Treichel, J.-C.Vuilleumier, J.-L.Vuilleumier New Limit on Neutrinoless Double β Decay in 136Xe with a Time Projection Chamber RADIOACTIVITY 136Xe(2β); measured neutrinoless double β-decay T1/2 lower limit; deduced Majorana neutrino mass parameter upper limit. Xenon time projection chamber.
doi: 10.1103/PhysRevLett.67.1218
1991WO06 J.Phys.(London) G17, S165 (1991) H.T.Wong, F.Boehm, P.Fisher, K.Gabathuler, H.E.Henrikson, D.A.Imel, M.Z.Iqbal, V.Jorgens, L.W.Mitchell, B.M.O'Callaghan-Hay, J.Thomas, M.Treichel, J.-C.Vuilleumier, J.-L.Vuilleumier First 0ν Half-Life Limit from the Gotthard Xenon Time Projection Chamber RADIOACTIVITY 136Xe(2β); measured 0ν-mode 2β-decay T1/2 lower limit. Xenon time projection chamber, Gotthard Tunnel underground laboratory.
doi: 10.1088/0954-3899/17/S/017
1988KR06 Phys.Rev.Lett. 60, 1475 (1988) R.M.Kremer, C.A.Barnes, K.H.Chang, H.C.Evans, B.W.Filippone, K.H.Hahn, L.W.Mitchell Coincidence Measurement of the 12C(α, γ)16O Cross Section at Low Energies NUCLEAR REACTIONS, ICPND 12C(α, γ), E(cm)=1.29-3 MeV; measured γ-spectra, γ(recoil)-coin; deduced γ yields, dipole capture σ(E), S-factor vs E.
doi: 10.1103/PhysRevLett.60.1475
1988MI13 Phys.Rev. C38, 895 (1988) Rare Decays of Cadmium and Tellurium RADIOACTIVITY 106,114,116Cd, 128,130Te(2β); 113Cd(β-); measured T1/2 lower limits. Low background shield, CdTe detector.
doi: 10.1103/PhysRevC.38.895
1988WI12 Nucl.Instrum.Methods Phys.Res. A267, 242 (1988) M.Wiescher, J.Gorres, K.L.Kratz, B.Leist, K.H.Chang, B.W.Filippone, L.W.Mitchell, M.J.Savage, R.B.Vogelaar The Fabrication and Properties of a 22Na Target NUCLEAR REACTIONS 23Na(p, γ), E ≈ 310-340 keV; 19F(p, α), E ≈ 600-900 keV; measured thick target yield. 30Si(p, γ), E=620 keV; measured Eγ, Iγ. 24Mg(d, α), E not given; measured Eγ, Iγ; deduced 22Na target feasibility.
doi: 10.1016/0168-9002(88)90471-8
1987IQ01 Nucl.Instrum.Methods Phys.Res. A259, 459 (1987) M.Z.Iqbal, H.E.Henrikson, L.W.Mitchell, B.M.G.O'Callaghan, J.Thomas, H.T.-k.Wong Design and Construction of a High Pressure Xenon Time Projection Chamber RADIOACTIVITY 136Xe(2β); measured double beta decay, T1/2. High pressure time projection chamber.
doi: 10.1016/0168-9002(87)90827-8
1986KA34 Phys.Rev. C34, 1477 (1986) R.W.Kavanagh, L.W.Mitchell, D.G.Sargood Branching Ratio of the Second Excited State of 30P NUCLEAR REACTIONS 27Al(α, n), E=4.2 MeV; measured Eγ, Iγ. 30P levels deduced decay charateristics, M1 transition width, M1 matrix element spin, orbital ratio, γ-branching.
doi: 10.1103/PhysRevC.34.1477
1986SE02 Nucl.Phys. A454, 128 (1986) M.E.Sevior, L.W.Mitchell, C.I.W.Tingwell, D.G.Sargood Cross Sections for Proton Induced Reactions on 41K and for the Reaction 62Ni(α, p)65Cu NUCLEAR REACTIONS, ICPND 41K(p, α), (p, γ), (p, n), (p, αγ), (p, nγ), (p, p'γ), E=0.6-4 MeV; 62Ni(α, p), E=6.5-9 MeV; measured α-particle, γ-ray, neutron, proton yields; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched targets.
doi: 10.1016/0375-9474(86)90151-X
1985MI17 Nucl.Phys. A443, 487 (1985) L.W.Mitchell, R.W.Kavanagh, M.E.Sevior, C.I.W.Tingwell, D.G.Sargood The 42Ca(α, γ)46Ti and 42Ca(α, p)45Sc Cross Sections and the Mass-45 Bottleneck NUCLEAR REACTIONS, ICPND 42Ca(α, γ), E=3.42-5.62 MeV; 42Ca(α, pγ), E=4.06-5.92 MeV; 42Ca(α, p), E=4.78-5.92 MeV; measured γ-ray, proton yields; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched targets.
doi: 10.1016/0375-9474(85)90414-2
1985TI04 Nucl.Phys. A439, 371 (1985) C.I.W.Tingwell, L.W.Mitchell, M.E.Sevior, D.G.Sargood The Thermonuclear Reaction Rate of 58Ni(p, γ)59Cu NUCLEAR REACTIONS, ICPND 58Ni(p, γ), (p, p'γ), E=1.18-4.2 MeV; measured γ-ray yields; deduced σ(E), thermonuclear reaction rates. 59Cu deduced resonances, strengths. Statistical-model analysis. Enriched targets.
doi: 10.1016/0375-9474(85)90437-3
1985WE07 Nucl.Phys. A439, 176 (1985) R.O.Weber, C.I.W.Tingwell, L.W.Mitchell, M.E.Sevior, D.G.Sargood Cross Sections and Thermonuclear Reaction Rates of Proton-Induced Reactions on 37Cl NUCLEAR REACTIONS, ICPND 37Cl(p, γ), (p, αγ), (p, n), E=0.65-2.5 MeV; measured γ-ray, neutron yields; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched target.
doi: 10.1016/0375-9474(85)90212-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
1983MI05 Aust.J.Phys. 36, 1 (1983) The 55Mn(p, γ)56Fe and 55Mn(p, n)55Fe Cross Sections NUCLEAR REACTIONS, ICPND 55Mn(p, γ), E=0.8-2.04 MeV; 55Mn(p, n), E=threshold-2.04 MeV; measured σ(E); deduced thermonuclear reaction rates.
doi: 10.1071/PH830001
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
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
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
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