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NSR database version of April 11, 2024.

Search: Author = M.D.Cohler

Found 21 matches.

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1997BE45      Phys.Rev. C56, 1960 (1997)

M.B.Becha, C.O.Blyth, C.N.Pinder, N.M.Clarke, R.P.Ward, P.R.Hayes, K.I.Pearce, D.L.Watson, A.Ghazarian, M.D.Cohler, I.J.Thompson, M.A.Nagarajan

The 40Ca(t, p)42Ca Reaction at Triton Energies Near 10 MeV per Nucleon

NUCLEAR REACTIONS 40Ca(t, p), E=28, 33, 37.3 MeV; measured proton spectra, σ(E, θ); deduced model parameters, reaction mechanism features. 48Ca(t, p), (t, d), E=37.3 MeV; measured σ(θ). 49Ca level deduced J, π. Shell model calculations, DWBA analysis.

doi: 10.1103/PhysRevC.56.1960
Citations: PlumX Metrics

1988MU22      J.Phys.(London) G14, 1373 (1988)

S.M.Mullins, M.D.Cohler, A.Ghazarian, J.R.Hughes, R.Wadsworth, D.L.Watson, P.J.Bishop, A.J.Kirwan, P.J.Nolan, R.J.Poynter, D.J.G.Love, J.Heese

Collective Bands and Lifetime Measurements in 137Pm

NUCLEAR REACTIONS 122Te(19F, 4n), E=83 MeV; 108Pd(32S, 2np), E=152 MeV; measured Eγ, Iγ, γγ-coin, recoil distance. 137Pm deduced levels J, π, T1/2, deformation parameter, B(E2). Ge detectors, BGO escape suppression shields, BGO multiplicity filter, enriched targets. Cranked shell model.

NUCLEAR STRUCTURE 137Pm; calculated levels, deformation parameter. Cranked shell model.

doi: 10.1088/0305-4616/14/11/009
Citations: PlumX Metrics

1987EN06      Nucl.Phys. A475, 422 (1987)

J.B.A.England, L.Zybert, G.T.A.Squier, O.Karban, R.Zybert, J.M.Nelson, D.Barker, B.R.Fulton, M.C.Mannion, C.A.Ogilvie, L.Potvin, C.Pinder, C.O.Blyth, G.C.Morrison, G.J.Pyle, S.Roman, N.M.Clarke, K.I.Pearce, P.J.Simmonds, R.J.Griffiths, D.L.Watson, M.D.Cohler, R.Wadsworth, J.O'Donnell, M.Smithson

Elastic Scattering of 33 MeV Tritons and Isospin Dependence of Mass-3 Optical Potential

NUCLEAR REACTIONS 12C, 16O, 19F, 24Mg, 40,48Ca, 51V, 58Ni, 89Y, 208Pb, 232Th(t, t), E=33 MeV; measured σ(θ); deduced optical-model parameters, isospin dependence.

doi: 10.1016/0375-9474(87)90072-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0072.

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
Citations: PlumX Metrics

1987KA40      Nucl.Phys. A472, 189 (1987)

O.Karban, J.B.A.England, D.Barker, M.Mannion, J.M.Nelson, C.A.Ogilvie, L.Potvin, L.Zybert, R.Zybert, N.M.Clarke, K.I.Pearce, D.L.Watson, M.D.Cohler

A Study of 52V with the 51V(t, d) Reaction

NUCLEAR REACTIONS, MECPD 51V(t, d), E=33 MeV; measured σ(Ed), σ(θ). 52V deduced levels, j-transfer, spectroscopic factors.

doi: 10.1016/0375-9474(87)90206-5
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0087.

1986BU16      Phys.Rev. C34, 1592 (1986)

M.Burlein, H.T.Fortune, D.L.Watson, M.D.Cohler

80Se from the 78Se(t, p) Reaction

NUCLEAR REACTIONS 78Se(t, p), E=17 MeV; measured σ(θ); deduced model parameters. 80Se deduced levels, J, π, L.

doi: 10.1103/PhysRevC.34.1592
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1306.

1986FO01      J.Phys.(London) G12, L37 (1986)

H.T.Fortune, M.Carchidi, D.L.Watson, M.D.Cohler

A Dependence of GS Se(t, p) Cross Sections

NUCLEAR REACTIONS 76,78,80,82Se(t, p), E=17 MeV; measured σ(Ep), σ(θ); deduced σ mass dependence. 78,80,82,84Se levels deduced configuration, absolute σ. DWBA analysis.

doi: 10.1088/0305-4616/12/1/007
Citations: PlumX Metrics

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

1984WA13      Phys.Rev. C30, 826 (1984)

D.L.Watson, M.D.Cohler, H.T.Fortune

82Se from the 80Se(t, p)82Se Reaction

NUCLEAR REACTIONS 80Se(t, p), E=15 MeV; measured σ(Ep), σ(θ). 82Se levels deduced L, J, π.

doi: 10.1103/PhysRevC.30.826
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0025.

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
Citations: PlumX Metrics

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

1980ST06      J.Phys.(London) G6, 501 (1980)

M.F.Steeden, J.Coopersmith, S.J.Cartwright, M.D.Cohler, N.M.Clarke, R.J.Griffiths

Phenomenological and Microscopic Optical Potentials for 88 MeV 7Li Scattering

NUCLEAR REACTIONS 24,26Mg, 40,48Ca(7Li, 7Li), E=88 MeV; measured σ(θ); deduced energy dependence of optical potentials. Phenomenological, double-folding microscopic potentials.

doi: 10.1088/0305-4616/6/4/018
Citations: PlumX Metrics

1979BA12      J.Phys.(London) G5, L69 (1979)

J.Barnwell, M.D.Cohler, N.M.Clarke, R.J.Griffiths, J.S.Hanspal, O.Karban, S.Roman

Ambiguities in the 3He Spin-Orbit Potential for 32S

NUCLEAR REACTIONS 32S(polarized 3He, 3He), E=33 MeV; measured P(θ); deduced parameters of 3He spin-orbit potential. Optical-model analysis.

doi: 10.1088/0305-4616/5/4/005
Citations: PlumX Metrics

1979CL08      J.Phys.(London) G5, 1233 (1979); see 79Cl09

N.M.Clarke, M.D.Cohler, R.J.Griffiths

Effects of Coupled Reaction Channels on Polarisation in 3He Scattering

doi: 10.1088/0305-4616/5/9/008
Citations: PlumX Metrics

1979CL09      J.Phys.(London) G5, 1233 (1979)

N.M.Clarke, M.D.Cohler, R.J.Griffiths

Effects of Coupled Reaction Channels on Polarisation in 3He Scattering

NUCLEAR REACTIONS 26Mg(t, t), E=33 MeV; 26Mg(3He, 3He), (3He, 3He'), E=33.7 MeV; 26Mg(α, α), (α, α'), E=42.6 MeV; 24Mg(3He, α), E not given; calculated σ(θ), P(θ), A(θ); deduced influence of reaction channels on polarization. Coupled channels method.

doi: 10.1088/0305-4616/5/9/008
Citations: PlumX Metrics

1979CO04      J.Phys.(London) G5, L43 (1979)

M.D.Cohler, R.J.Griffiths, N.M.Clarke, J.S.Hanspal

The Microscopic Spin-Orbit Potential for Light Ions

NUCLEAR REACTIONS 24Mg(p, p), E=50 MeV; 26Mg(3He, 3He), E=30 MeV; calculated P(θ). Microscopic spin-orbit potential including incomplete spin saturation for valence nucleons.

doi: 10.1088/0305-4616/5/3/001
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1978SA06      Nucl.Phys. A298, 313 (1978)

G.R.Satchler, M.L.Halbert, N.M.Clarke, E.E.Gross, C.B.Fulmer, A.Scott, D.Martin, M.D.Cohler, D.C.Hensley, C.A.Ludemann, J.G.Cramer, M.S.Zisman, R.M.DeVries

Heavy-Ion Elastic Scattering (II). 142 MeV 16O on 28Si, 59Co and 60Ni

NUCLEAR REACTIONS 28Si, 59Co, 60Ni(16O, 16O); 28Si, 60Ni(16O, 16O'), E=141.9 MeV; measured σ(θ); deduced optical potentials.

doi: 10.1016/0375-9474(78)90259-2
Citations: PlumX Metrics

1977GR09      J.Phys.(London) G3, L-129 (1977)

R.J.Griffiths, N.M.Clarke, M.D.Cohler, J.M.Barnwell

Microscopic Potentials for the (3He, 4He) Reaction

NUCLEAR REACTIONS 56Fe(3He, α), E=83 MeV; 56Fe(α, α), E=86 MeV; calculated σ(θ).

doi: 10.1088/0305-4616/3/6/004
Citations: PlumX Metrics

1976CO21      Phys.Lett. 63B, 377 (1976)

M.D.Cohler, B.C.Sinha, R.J.Griffiths, N.M.Clarke

Pauli Exchange Effects in 3He and 4He Interaction Potentials

NUCLEAR REACTIONS 56Fe(α, α), E=18 MeV; 26Mg(3He, 3He), E=33.7 MeV; calculated interaction potential, σ(θ).

doi: 10.1016/0370-2693(76)90373-7
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