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NSR database version of April 29, 2024.

Search: Author = N.E.Sanderson

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1985WO01      Phys.Lett. 150B, 79 (1985)

P.J.Woods, R.Chapman, J.L.Durell, J.N.Mo, N.E.Sanderson, R.A.Cunningham, B.R.Fulton

The Mass of ²¹O from the Reactions ^{61, 64}Ni(¹⁸O, ²¹O)^{58, 61}Ni

NUCLEAR REACTIONS ^61,64Ni(¹⁸O, ²¹O), E=150 MeV; measured σ(E(²¹O)). ²¹O deduced mass excess, levels.

doi: 10.1016/0370-2693(85)90142-X
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1985WO07      Z.Phys. A321, 119 (1985)

P.J.Woods, R.Chapman, J.L.Durell, J.N.Mo, R.J.Smith, N.E.Sanderson, B.R.Fulton, R.A.Cunningham

Use of the ⁶⁴Ni(³⁶S, ³⁴Si)⁶⁶Zn Reaction to Measure the Mass of ³⁴Si

NUCLEAR REACTIONS ⁶⁴Ni(³⁶S, ³⁴Si), E=198 MeV; measured ³⁴Si ion momentum spectra. ³⁴Si deduced mass. Mass, shell models comparison.

doi: 10.1007/BF01411955
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1984DA07      Phys.Lett. 139B, 150 (1984)

T.Davinson, V.Rapp, A.C.Shotter, D.Branford, M.A.Nagarajan, I.J.Thompson, N.E.Sanderson

Coulomb and Nuclear Contribution to the Excitation of ⁷Li Incident on Heavy Nuclei

NUCLEAR REACTIONS ²⁰⁸Pb(⁷Li, ⁷Li), (⁷Li, ⁷Li'), E=68 MeV; measured σ(θ); deduced Coulomb, nuclear contribution relative importance. Coupled-channels, adiabatic model calculations.

doi: 10.1016/0370-2693(84)91233-4
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1984SH17      Phys.Rev.Lett. 53, 1539 (1984)

A.C.Shotter, V.Rapp, T.Davinson, D.Branford, N.E.Sanderson, M.A.Nagarajan

Direct Coulomb Breakup of ⁷Li

NUCLEAR REACTIONS ¹²⁰Sn(⁷Li, tα), E=70 MeV; measured σ(Eα); deduced projectile breakup mechanism.

doi: 10.1103/PhysRevLett.53.1539
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1983DR06      Phys.Lett. 126B, 155 (1983)

P.V.Drumm, J.B.A.England, O.Karban, J.M.Nelson, J.M.Barnwell, N.E.Sanderson

Break-Up of Polarized ³He at 33 MeV

NUCLEAR REACTIONS ¹²C, ²⁷Al, ⁵⁸Ni(polarized ³He, pd), E=33 MeV; measured σ(θd, θp, Ed), analyzing power vs θd, σ(θd, θp); deduced breakup yield on ³He spin orientation. Kinematically complete experiment.

doi: 10.1016/0370-2693(83)90581-6
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1981BH02      Nucl.Phys. A363, 516 (1981)

R.K.Bhowmik, E.C.Pollacco, J.B.A.England, G.C.Morrison, N.E.Sanderson

Emission of α-Particles in Deep Inelastic Reactions Induced by 148 MeV ¹⁴N

NUCLEAR REACTIONS ¹²C, ²⁷Al, ⁵⁸Ni(¹⁴N, X), E=148 MeV; measured σ(fragment E, θ), fragment mass = 2-8; ¹²C, ²⁷Al, ⁵⁸Ni(¹⁴N, αX), E=148 MeV; measured absolute σ(E(X), θ(X), Eα, θα), αX-coin; deduced reaction mechanisms. Enriched ⁵⁸Ni target.

doi: 10.1016/0375-9474(81)90271-2
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1980DU10      Phys.Lett. B94, 335 (1980)

J.L.Durell, W.R.Phillips, B.R.Fulton, J.S.Lilley, N.E.Sanderson

Comparison of Heavy Ion Transfer and Electron Scattering Measurements of the 1g_9/2 Neutron Distribution in ⁸⁷Sr

NUCLEAR REACTIONS ⁸⁶Sr(¹⁸O, ¹⁷O), E=45, 46 MeV; measured σ(E(¹⁷O), θ). ⁸⁷Sr level deduced 1g_9/2 neutron rms radius.

doi: 10.1016/0370-2693(80)90891-6
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1980MO28      J.Phys.(Paris), Colloq.C-10, 243 (1980)

G.C.Morrison, R.K.Bhowmik, E.C.Pollacco, J.B.A.England, N.E.Sanderson

Alpha Emission with 10 MeV/A ¹⁴N Projectiles

NUCLEAR REACTIONS ⁵⁸Ni, ²⁷Al, ¹²C(¹⁴N, αX), E=148 MeV; measured σ(fragment E, θ), σ(θα, Eα), σ(Eα, θα, fragment E, θ), αX-coin, αX(θ); deduced direct mechanism for α-decay followed by deep inelastic collision.

1979BH06      Phys.Rev.Lett. 43, 619 (1979)

R.K.Bhowmik, E.C.Pollacco, N.E.Sanderson, J.B.A.England, G.C.Morrison

Pre-Emission of α Particles in Deep-Inelastic Reactions

NUCLEAR REACTIONS ⁵⁸Ni(¹⁴N, 2α), (¹⁴N, αX), E=148 MeV; measured σ(Eα, E(HI), θ) for X=Li, Be, B, C, N; deduced reaction mechanism. Thick target.

doi: 10.1103/PhysRevLett.43.619
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1979FU01      Nucl.Phys. A315, 477 (1979)

B.R.Fulton, N.E.Sanderson, R.Ost, B.A.England, G.C.Morrison

Transfer Reactions and Scattering Induced by ¹³C on ⁵²Cr

NUCLEAR REACTIONS ⁵²Cr(¹³C, ¹³C'), (¹³C, ¹²B), (¹³C, ¹⁴C), (¹³C, ¹⁴N), E=105 MeV; measured σ(θ). ⁵¹V, ⁵¹Cr, ⁵³Mn levels deduced S. Optical model, DWBA analyses. Enriched target.

doi: 10.1016/0375-9474(79)90624-9
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1978BH03      Phys.Lett. 80B, 41 (1978)

R.K.Bhowmik, E.C.Pollacco, N.E.Sanderson, J.B.A.England, G.C.Morrison

A Study of Heavy-Ion-Alpha Correlations with ¹¹B Projectiles

NUCLEAR REACTIONS ¹²C(¹¹B, αX), ⁵⁸Ni(¹¹B, αX), E=116 MeV; measured X-α(θ), differential α-multiplicities.

doi: 10.1016/0370-2693(78)90301-5
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1977RO17      Nucl.Phys. A289, 269 (1977)

S.Roman, A.K.Basak, J.B.A.England, J.M.Nelson, N.E.Sanderson, F.D.Santos, A.M.Eiro

³He D-State Effects in (d, ³He) Reactions

NUCLEAR REACTIONS ²⁷Al(polarized d, ³He), E=12.4 MeV; measured iT₁₁, T₂₀, T₂₂(θ); deduced ³He d-state contribution. Natural target.

doi: 10.1016/0375-9474(77)90032-X
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1976OS04      Nucl.Phys. A265, 142 (1976)

R.Ost, N.E.Sanderson, S.Mordechai, J.B.A.England, B.R.Fulton, J.M.Nelson, G.C.Morrison

Do Many-Particle Reactions Contribute to 'Deep-Inelastic' Peaks (Question)

NUCLEAR REACTIONS ⁶⁰Ni(¹³C, X), E=105 MeV; measured σ(E(Z), θ), Z=3-8. ^58,64Ni(¹³C, X), E=105 MeV; measured σ(E(Z), θ), Z=3-8, light particle coin for Li, B, Be, α, p; deduced reaction mechanism. Enriched targets.

doi: 10.1016/0375-9474(76)90120-2
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1976SA07      Nucl.Phys. A261, 93 (1976)

N.E.Sanderson, R.G.Summers-Gill

Spectroscopy of ⁷⁵Se Studied with the ⁷²Ge(α, nγ) Reaction

NUCLEAR REACTIONS ⁷²Ge(α, nγ), E=8.1, 10.0, 13.0 MeV; measured σ(Eγ, θ), γγ-coin. ⁷⁵Se deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(76)90043-9
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1976SA14      Nucl.Phys. A266, 215 (1976)

N.E.Sanderson, M.Ivanovich

Evidence for Inelastic Processes in the ²⁴Mg(¹³C, ¹²C)²⁵Mg Reaction at E(lab) = 30 MeV

NUCLEAR REACTIONS ²⁴Mg(¹³C, ¹³C), (¹³C, ¹²C), E=30 MeV; measured σ(θ). ²⁵Mg levels deduced S. DWBA analysis. Enriched targets.

doi: 10.1016/0375-9474(76)90291-8
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1976SA26      Phys.Rev.Lett. 37, 1672 (1976)

N.E.Sanderson, A.K.Basak, J.B.A.England, J.M.Nelson, S.Roman

Investigation of d₅/₂-d₃/₂ Admixing in the Pickup Strength to the First Excited States of ²²Ne and ²⁶Mg

NUCLEAR REACTIONS ²³Na, ²⁷Al(polarized d, ³He), E=12.4 MeV; measured vector analyzing power iT₁₁; deduced admixing in pickup strength to levels in ²²Ne, ²⁶Mg.

doi: 10.1103/PhysRevLett.37.1672
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1974HU03      Nucl.Phys. A219, 407 (1974)

S.G.Hussein, N.E.Sanderson, R.G.Summers-Gill

Low-Lying Levels of ¹⁴⁰Pr

NUCLEAR REACTIONS ¹⁴¹Pr(d, t), E=16 MeV; measured σ(Et, θ). ¹⁴⁰Ce(p, nγ), E=4.78 MeV; measured σ(Eγ, θ). ¹⁴⁰Pr deduced levels, L(n), J, π, spectroscopic strengths. Natural, enriched targets.

doi: 10.1016/0375-9474(74)90075-X
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1974SA32      J.Phys.(London) A7, 1156 (1974)

N.E.Sanderson, J.C.Lisle, J.C.Willmott

The Level Structure of ⁷⁸Kr

RADIOACTIVITY ⁷⁸Rb; measured Eγ, Iγ, γγ-coin, γ(t), γγ(θ). ⁷⁸Kr deduced levels, J, π, T_1/2.

NUCLEAR REACTIONS ⁶⁸Zn(¹²C, 2nγ), E=32-48 MeV; measured σ(E, Eγ, θ). ⁶⁴Ni(¹⁶O, 2nγ), E=42 MeV; measured γγ-coin. ⁷⁸Kr deduced levels, J, π.

doi: 10.1088/0305-4470/7/10/008
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1973SA39      Nucl.Phys. A216, 173 (1973)

N.E.Sanderson

The ⁷⁶Se(d, t) Reaction and a Coriolis Coupling Theory of Anomalous States in 1g₉/₂ Nuclei

NUCLEAR REACTIONS ⁷⁶Se(d, t), E=18, 19 MeV; measured σ(Et, θ). ⁷⁵Se deduced levels, J, π, L, S. Enriched target.

doi: 10.1016/0375-9474(73)90526-5
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1971MU14      Nucl.Phys. A171, 435 (1971)

G.Murray, N.E.Sanderson, J.C.Willmott

Low-Lying Positive-Parity States in ⁷¹Ge

RADIOACTIVITY ^71mGe, ⁷¹As[from ⁷⁰Ge(d, p), ⁷⁰Ge(d, n)]; measured T_1/2, Eγ, Iγ, γγ-coin; deduced log ft. ⁷¹Ge deduced levels, J, π. Enriched target, Ge(Li) detector.

doi: 10.1016/0375-9474(71)90033-9
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