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Search: Author = M.J.Smithson

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1216.


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0542.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1750.


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