NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.J.Smithson Found 23 matches. 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
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
1990SE11 Phys.Rev. C42, 1929 (1990) P.A.Seidl, M.A.Bryan, M.Burlein, G.R.Burleson, K.S.Dhuga, H.T.Fortune, R.Gilman, S.J.Greene, M.A.Machuca, C.F.Moore, S.Mordechai, C.L.Morris, D.S.Oakley, M.A.Plum, G.Rai, M.J.Smithson, Z.F.Wang, D.L.Watson, J.D.Zumbro Pion Double Charge Exchange on T = 2 Nuclei in the Δ(3/2, 3/2) Resonance Region NUCLEAR REACTIONS 12C, 16O, 44Ca, 56Fe(π+, π-), E=100-300 MeV; measured σ(θ) vs E.
doi: 10.1103/PhysRevC.42.1929
1990SM03 Nucl.Phys. A517, 193 (1990) M.J.Smithson, J.S.Lilley, M.A.Nagarajan, P.V.Drumm, R.A.Cunningham, B.R.Fulton, I.J.Thompson The Threshold Anomaly in Inelastic Scattering NUCLEAR REACTIONS 208Pb(16O, 16O), (16O, 16O'), E=70-94 MeV; measured σ(θ); deduced model parameters. 208Pb deduced deformation lengths, quadrupole moment. DWBA analysis.
doi: 10.1016/0375-9474(90)90268-Q
1989TH06 Nucl.Phys. A505, 84 (1989) I.J.Thompson, M.A.Nagarajan, J.S.Lilley, M.J.Smithson The Threshold Anomaly in 16O + 208Pb Scattering NUCLEAR REACTIONS, ICPND 208Pb(16O, 16O), E=78-102 MeV; calculated σ(θ), reaction σ vs E. Coupled reaction channels model.
doi: 10.1016/0375-9474(89)90417-X
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
1988MO01 Phys.Rev.Lett. 60, 408 (1988) S.Mordechai, N.Auerbach, G.R.Burleson, K.S.Dhuga, M.Dwyer, J.A.Faucett, H.T.Fortune, R.Gilman, S.J.Greene, C.Laymon, C.F.Moore, C.L.Morris, D.S.Oakley, M.A.Plum, S.J.Seestrom-Morris, P.A.Seidl, M.J.Smithson, Z.F.Wang, J.D.Zumbro Giant Dipole Resonances Built on Isobaric Analog States in Pion Double Charge Exchange NUCLEAR REACTIONS 56Fe, 80Se, 208Pb(π+, π-), E at 292 MeV/c; measured σ(E(π-), θ(π-)), σ(θ(π-)). 56Ni, 80Kr, 208Po deduced giant dipole resonance parameters. Coupled-channel impulse approximation calculations.
doi: 10.1103/PhysRevLett.60.408
1988OA01 Phys.Rev. C37, 866 (1988) D.S.Oakley, M.J.Smithson, S.Mordechai, C.F.Moore, P.A.Seidl, C.L.Morris, S.J.Seestrom-Morris, R.Gilman, J.D.Zumbro, H.T.Fortune, K.S.Dhuga Pion Inelastic Scattering from 48,50Ti, 52Cr, and 54,56Fe: Higher-lying states NUCLEAR REACTIONS 48,50Ti, 52Cr, 54,56Fe(π+, π+), (π+, π+'), E=180 MeV; measured σ(θ). 48,50Ti, 52Cr, 54,56Fe levels deduced neutron, proton matrix elements.
doi: 10.1103/PhysRevC.37.866
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
1988SM01 Phys.Rev. C37, 1036 (1988) M.J.Smithson, D.L.Watson, H.T.Fortune 13C(6Li, p)18O Reaction at E(6Li) = 28 MeV NUCLEAR REACTIONS, ICPND 13C(6Li, p), E=28 MeV; measured σ(Ep), σ(θ); deduced model parameters, σ(E). 18O deduced levels, J, π.
doi: 10.1103/PhysRevC.37.1036
1987FO06 Phys.Rev. C35, 1603 (1987) H.T.Fortune, C.Ogilvie, R.Gilman, J.D.Zumbro, D.L.Watson, M.J.Smithson, M.D.Cohler, A.Ghazarian, R.Wadsworth, J.O'Donnell No Two-Proton Strength to 72Ge (02+) NUCLEAR REACTIONS 70Zn(16O, 14C), E=110 MeV; measured σ(E(14C)). 72Ge level deduced no two-proton strength.
doi: 10.1103/PhysRevC.35.1603
1987FO21 J.Phys.(London) G13, 1531 (1987) P.B.Foot, D.Barker, C.O.Blyth, J.B.A.England, O.Karban, M.C.Mannion, J.M.Nelson, C.A.Ogilvie, C.Pinder, L.Potvin, S.Roman, G.G.Shute, L.Zybert, R.Zybert, J.M.O'Donnell, M.J.Smithson, N.M.Clarke, K.I.Pearce, P.Simmonds, B.M.Spicer The 12C(t, α)11B Reaction at 33 MeV NUCLEAR REACTIONS, MECPD 12C(t, α), E=33 MeV; measured σ(Eα), σ(θ); deduced model parameters. DWBA, coupled-reaction channel analyses.
doi: 10.1088/0305-4616/13/12/011
1987MO18 Phys.Rev. C36, 710 (1987) S.Mordechai, M.J.Smithson, M.Lynker, D.S.Oakley, C.F.Moore, D.L.Watson, R.Gilman, J.D.Zumbro, P.Kutt, H.T.Fortune, C.L.Morris, K.S.Dhuga Neutron and Proton Matrix Elements for Transitions in 39K from Pion Inelastic Scattering NUCLEAR REACTIONS 39K(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured missing mass spectra, σ(θ); deduced neutron, proton octupole matrix elements. 39K level deduced E2 transition probe sensitivity. DWIA analyses.
doi: 10.1103/PhysRevC.36.710
1987OA01 Phys.Rev. C35, 1392 (1987) D.S.Oakley, M.J.Smithson, S.Mordechai, C.F.Moore, C.L.Morris, G.C.Idzorek, Z.F.Wang, R.Gilman, J.D.Zumbro, H.T.Fortune, S.J.Seestrom-Morris, K.S.Dhuga, D.L.Watson Pion Elastic and Inelastic Scattering from 48,50Ti, 52Cr, and 54,56Fe at 180 MeV: Determination of neutron and proton multipole matrix elements NUCLEAR REACTIONS 48,50Ti, 52Cr, 54,56Fe(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured σ(E(π)), σ(θ). 48,50Ti, 52Cr, 54,56Fe deduced levels, neutron, proton multipole matrix elements, ground state density distribution parameters.
doi: 10.1103/PhysRevC.35.1392
1987OA02 Phys.Rev. C36, 1074 (1987) D.S.Oakley, M.A.Machuca, M.J.Smithson, S.Mordechai, C.F.Moore, P.A.Seidl, C.L.Morris, Z.F.Wang, R.Gilman, J.D.Zumbro, H.T.Fortune, S.J.Seestrom-Morris, K.S.Dhuga, D.L.Watson Pion Elastic and Inelastic Scattering from 51V at 180 MeV NUCLEAR REACTIONS 51V(π+, π+), (π+, π+'), E=180 MeV; measured σ(θ). 51V deduced levels, J, π, B(λ), proton, neutron matrix elements.
doi: 10.1103/PhysRevC.36.1074
1987ZU03 Phys.Rev. C36, 1479 (1987) J.D.Zumbro, H.T.Fortune, M.Burlein, C.L.Morris, Z.-F.Wang, R.Gilman, K.S.Dhuga, G.R.Burleson, M.W.Rawool, R.W.Garnett, M.J.Smithson, D.S.Oakley, S.Mordechai, C.F.Moore, M.A.Machuca, D.L.Watson, N.Auerbach Double Charge Exchange to the Double Isobaric Analog State at T(π) ≈ 292 MeV NUCLEAR REACTIONS 30Si, 34S, 44Ca, 50Ti, 51V, 52Cr, 58Ni(π+, π-), E ≈ 292 MeV; measured σ(θ), σ(π). 44Ti, 51Mn, 52Fe, 50Cr levels deduced ground state, double IAS excitation σ.
doi: 10.1103/PhysRevC.36.1479
1986SM01 Phys.Rev. C33, 509 (1986) M.J.Smithson, D.L.Watson, H.T.Fortune Selectivity in 13C(6Li, p)18O NUCLEAR REACTIONS, ICPND 13C(6Li, p), E=28 MeV; measured σ(θ); deduced σ, correlation with 12C(7Li, p) data.
doi: 10.1103/PhysRevC.33.509
1986SM10 J.Phys.(London) G12, 985 (1986) M.J.Smithson, D.L.Watson, H.T.Fortune A Study of the 12C(6Li, p)17O Reaction at E = 28 MeV NUCLEAR REACTIONS, ICPND 12C(6Li, p), E=28 MeV; measured σ(θ); deduced σ, model parameters. 17O deduced levels, J, π, T. Enriched target, multiangle spectrograph. Hauser-Feshbach, DWBA analyses.
doi: 10.1088/0305-4616/12/10/010
1985CO22 Z.Phys. A322, 491 (1985) M.D.Cohler, R.Wadsworth, S.M.Lane, D.L.Watson, M.J.Smithson, R.E.Brown, D.M.Drake, N.Stein, J.-C.Peng, J.W.Sunier Investigation of a Possible Abrupt Change in Structure at N = 58-60 using Two-Proton Transfer NUCLEAR REACTIONS 106,110,112,116Cd(14C, 14C), (14C, 16O), E=60 MeV; measured σ(θ); deduced optical model parameters. 104,108,110,114Pd levels deduced relative S.
doi: 10.1007/BF01412085
1985WA21 J.Phys.(London) G11, 1045 (1985) R.Wadsworth, M.D.Cohler, S.M.Lane, M.J.Smithson, D.L.Watson A Comparison of Two-Proton Pick-Up Strengths with IBA 2 Predictions in the Mass A = 100 Region NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116Pd; calculated levels, B(E2). Interacting boson model. NUCLEAR REACTIONS 96,100,102,104Ru(14C, 16O), 98,102,104,106Ru(d, 6Li), 96,100Mo(p, t), 92,96,98,100Mo(t, p), E not given; analyzed data; 94,98,100,102Mo levels deduced ground state σ, ratios. 104,106,108Ru, 104,108,110,114Pd deduced relative ground state transition strengths, σ. Interacting boson model form factors.
doi: 10.1088/0305-4616/11/9/013
1984CO19 Z.Phys. A319, 107 (1984) M.D.Cohler, D.L.Watson, R.Wadsworth, S.M.Lane, M.J.Smithson, R.E.Brown, J.-C.Peng, N.Stein, J.W.Sunier, D.M.Drake Measurement of the Mass of 110Pd and 114Pd using the (14C, 16O) Reaction NUCLEAR REACTIONS 112,114Cd(14C, 16O), E=60 MeV; measured σ(E(16O)). 110,114Pd deduced mass. Enriched target. Mass model comparison.
doi: 10.1007/BF01429774
1984WA05 J.Phys.(London) G10, L79 (1984) R.Wadsworth, M.D.Cohler, S.M.Lane, M.J.Smithson, D.L.Watson, R.E.Brown, D.M.Drake, J.-C.Peng, N.Stein, J.W.Sunier A Study of the (14C, 16O) Reaction in the Mass-100 Region NUCLEAR REACTIONS 96,100,102,104Ru, 106,108,110Pd(14C, 16O), E=60 MeV; measured σ(θ). 94,98,100,102Mo, 104,106,108Ru levels deduced relative spectroscopic factors. 96,102,104Ru, 106,108,110Pd(14C, 14C), E=60 MeV; 100Mo(16O, 16O), E=65 MeV; measured σ(θ); deduced optical model parameters. Exact finite-range DWBA analysis.
doi: 10.1088/0305-4616/10/4/003
1983WA19 J.Phys.(London) G9, 1237 (1983) R.Wadsworth, M.D.Cohler, M.J.Smithson, D.L.Watson, F.Jundt, L.Kraus, I.Linck, J.C.Sens A Study of the (6Li, 7Be) Reaction in the Mass-90 Region at 60 MeV NUCLEAR REACTIONS 90Zr, 89Y(6Li, 7Be), (6Li, 6Li), 89Y(7Li, 7Li), E=60 MeV; 90Zr(6Li, 6Li), E=30 MeV; measured σ(θ); deduced optical model parameters. 88Sr, 89Y levels deduced C2S. Finite-range DWBA analysis.
doi: 10.1088/0305-4616/9/10/011
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