Nuclear Science References (NSR)

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NSR database version of May 3, 2024.

Search: Author = B.H.Armitage

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1970GU08 Nucl.Phys. A153, 390 (1970)

K.Gul, B.H.Armitage, B.W.Hooton

The ¹⁸O(³He, n)²⁰Ne and ⁷Li(³He, n)⁹B Reactions

NUCLEAR REACTIONS ¹⁸O(³He, n), E=3.1 MeV; ⁷Li(³He, n), E=2.3-3.2 MeV; measured σ(En, θ), σ(E;En, θ). ²⁰Ne, ⁹B deduced levels, J, π. Enriched ¹⁸O target, natural Li target.

doi: 10.1016/0375-9474(70)90777-3
Citations: PlumX Metrics

1970JO07 Nucl.Phys. A146, 514 (1970)

R.K.Jolly, B.H.Armitage, A.K.Sen Gupta

Inelastic Deuteron Scattering from ⁵⁶Fe and ⁵⁸Fe

NUCLEAR REACTIONS ^56,58Fe(d, d'), E=11.5 MeV, 11.8 MeV; measured σ(Ed', θ). ^56,58Fe deduced levels, J, π, deformation parameters β(L). Enriched targets.

doi: 10.1016/0375-9474(70)90743-8
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1767.

1969AR04 Nucl.Phys. A133, 241(1969)

B.H.Armitage, A.T.G.Ferguson, G.C.Neilson, W.D.N.Pritchard

Energy Levels of ⁵⁶Fe: The ⁵⁶Fe(n, n'γ)⁵⁶Fe Reaction and the γ-Spectrum of ⁵⁶Co

RADIOACTIVITY ⁵⁶Co [from ⁵⁶Fe(p, n)]; measured Eγ, Iγ. ⁵⁶Fe deduced levels, J, π. Natural target. Ge(Li) detector.

NUCLEAR REACTIONS ⁵⁶Fe(n, n'γ), E=4.3, 5.3 MeV; measured σ(Eγ), Eγ. ⁵⁶Fe deduced levels, J, π.

doi: 10.1016/0375-9474(69)90628-9
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20466.

1968AR10 AERE-PR/NP-14, p.32 (1968)

B.H.Armitage, A.T.G.Ferguson, G.C.Neilson, W.D.N.Pritchard

Energy Levels of ⁵⁶Fe: The Fe(n, n'γ)⁵⁶Fe Reaction and the Gamma Spectrum of ⁵⁶Co

RADIOACTIVITY ⁵⁶Co; measured Eγ, Iγ.

NUCLEAR REACTIONS ⁵⁶Fe(n, n'γ), E=5.3 MeV; measured Eγ, Iγ. ⁵⁶Fe deduced levels. Ge(Li) detector.

1968GU07 Nucl.Phys. A122, 81(1968)

K.Gul, B.H.Armitage, B.W.Hooton

The Energy Levels of ¹⁹F and ¹⁹Ne

NUCLEAR REACTIONS ¹⁹F(p, p')¹⁹F, E=9 MeV; measured σ(Ep'). ¹⁸O(d, n)¹⁹F, ¹⁷O(³He, n)¹⁹Ne, E=3 MeV; measured σ(En, θ). ¹⁹F, ¹⁹Ne deduced levels, J, π. Enriched targets.

doi: 10.1016/0375-9474(68)90704-5
Citations: PlumX Metrics

1965AL11 Nucl.Phys. 66, 481 (1965)

D.L.Allan, B.H.Armitage, B.A.Doran

Energy Levels in Even Tin Isotopes from 11 MeV Proton Inelastic Scattering

NUCLEAR REACTIONS ^{116,118,120,122,124}Sn(p, p'), E = 11 MeV; measured σ(Ep', θ). ^{116,118,120,122,124}Sn deduced levels.

doi: 10.1016/0029-5582(65)90779-0
Citations: PlumX Metrics

1964AR04 Phys. Letters 8, 346 (1964)

B.H.Armitage, R.E.Meads

Levels in B¹⁰ Above 5.16 MeV Observed by Proton and Deuteron Inelastic Scattering

NUCLEAR STRUCTURE ¹⁰B; measured not abstracted; deduced nuclear properties.

doi: 10.1016/S0031-9163(64)80028-7
Citations: PlumX Metrics

1964MA46 Nucl.Phys. 59, 583(1964)

F.Manero, B.H.Armitage, J.M.Freeman, J.H.Montague

Total Neutron Cross Sections of C, Ca and Fe Between 8 and 14 MeV

NUCLEAR REACTIONS C(n, X), En=7.0-14.3 MeV; Ca, Fe(n, X), En=8.3-14.3 MeV; measured σ(nT). ¹³C deduced resonances, ⁴¹Ca, ⁵⁷Fe, no resonances.

doi: 10.1016/0029-5582(64)90035-5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21044.

1963AR10 Phys.Letters 7, 274 (1963)

B.H.Armitage, J.H.Montague, A.K.M.Siddiq, R.E.Meads

Levels in Al²⁷ below 2.21 MeV

NUCLEAR STRUCTURE ²⁷Al, ²⁷Mg; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(63)90330-5
Citations: PlumX Metrics

1962AR01 Phys.Letters 1, 284 (1962)

B.H.Armitage, R.E.Meads

The 5.18 MeV State in B¹⁰

NUCLEAR STRUCTURE ¹⁰B; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(62)91385-9
Citations: PlumX Metrics

1962AR02 Nuclear Phys. 33, 494 (1962)

B.H.Armitage, R.E.Meads