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NSR database version of April 27, 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, T_1/2, 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
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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
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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
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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 ^{106,110,112,116}Cd(¹⁴C, ¹⁴C), (¹⁴C, ¹⁶O), E=60 MeV; measured σ(θ); deduced optical model parameters. ^{104,108,110,114}Pd levels deduced relative S.

doi: 10.1007/BF01412085
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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 ^{100,102,104,106,108,110,112,114,116}Pd; calculated levels, B(E2). Interacting boson model.

NUCLEAR REACTIONS ^{96,100,102,104}Ru(¹⁴C, ¹⁶O), ^{98,102,104,106}Ru(d, ⁶Li), ^96,100Mo(p, t), ^92,96,98,100Mo(t, p), E not given; analyzed data; ^{94,98,100,102}Mo levels deduced ground state σ, ratios. ^104,106,108Ru, ^{104,108,110,114}Pd 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 ^{96,100,102,104}Ru, ^106,108,110Pd(¹⁴C, ¹⁶O), E=60 MeV; measured σ(θ). ^{94,98,100,102}Mo, ^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
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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
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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
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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
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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
Citations: PlumX Metrics

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
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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
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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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