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NSR database version of May 1, 2024.

Search: Author = V.J.Robinson

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1994BE52      Radiochim.Acta 64, 11 (1994)

L.F.Bellido, V.J.Robinson, H.E.Sims

Production of ²³⁵Np and ²³⁶Pu for Environmental Applications

NUCLEAR REACTIONS, ICPND ²³⁸U(p, n), (p, 3n), (p, 4n), E=13-56 MeV; measured σ(E); deduced ²³⁵Np, ²³⁶Pu production best route.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0426.

1993BE64      Radiochim.Acta 62, 123 (1993)

L.F.Bellido, V.J.Robinson, H.E.Sims

Excitation Functions for the ^235,238U(d, xn)^237,240(-x)Np Reactions

NUCLEAR REACTIONS, ICPND ^235,238U(d, xn)²³⁵Np/²³⁶Np/^236mNp, E=20-32 MeV; measured production σ(E).

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1064.

1987SZ03      Radiochim.Acta 41, 5 (1987)

A.Szymanski, G.W.A.Newton, V.J.Robinson, H.E.Sims

Gamma Ray Abundances of Re and W Isotopes, Part V, A = 171

RADIOACTIVITY ¹⁷¹Re [from ¹⁶⁵Ho(¹⁶O, 10n), E=110-183 MeV]; ¹⁷¹W(β⁺), (EC) [from ¹⁶⁵Ho(¹⁴N, 8n), E=140.3 MeV]; measured γ-abundances, T_1/2. ¹⁷¹Ta deduced transitions, T_1/2. ¹⁷¹Hf deduced transitions.

NUCLEAR REACTIONS ¹⁶⁵Ho(¹⁶O, 10n), E=110-183 MeV; ¹⁶⁵Ho(¹⁴N, 8n), E=140.3 MeV; measured residuals γ-ray abundances. Helium jet recoil transportation system.

1986SZ05      Radiochim.Acta 40, 61 (1986)

A.Szymanski, G.W.A.Newton, V.J.Robinson, H.E.Sims

Absolute Gamma Ray Abundances of Rhenium and Tungsten Isotopes: Part III, A = 173

NUCLEAR REACTIONS ¹⁶⁵Ho(¹⁴N, 6n), E=117.4 MeV; ¹⁶⁵Ho(¹⁴N, 5np), E=118.2 MeV; ¹⁶⁵Ho(¹⁶O, 8n), E=151.2 MeV; measured Eγ, Iγ. ¹⁷³Ta, ¹⁷³W, ¹⁷³Re deduced T_1/2. ¹⁷³W, ¹⁷³Ta, ¹⁷³Hf deduced transitions, absolute γ abundances.

RADIOACTIVITY ¹⁷³Ta, ¹⁷³W(EC), (β⁺); ¹⁷³Re(EC) [from ¹⁶⁵Ho(¹⁴N, 6n), (¹⁴N, p5n), (¹⁶O, 8n)]; measured Eγ, Iγ, T_1/2. ¹⁷³W, ¹⁷³Ta, ¹⁷³Hf deduced transitions, absolute γ abundances.

1986SZ06      Radiochim.Acta 40, 67 (1986)

A.Szymanski, G.W.A.Newton, V.J.Robinson, H.E.Sims

Absolute Gamma Ray Abundances of Re and W Isotopes: Part IV, A = 172

NUCLEAR REACTIONS ¹⁶⁵Ho(¹⁴N, 7n), E=89-147 MeV; ¹⁶⁵Ho(¹⁶O, 9n), E=110-183 MeV; measured Eγ, Iγ, σ(Eγ, E). ¹⁷²W deduced T_1/2, γ transitions, abundances. ¹⁷²Re deduced T_1/2. ¹⁷²Ta deduced γ transitions, abundances. Ge(Li) detector, He-jet recoil system.

RADIOACTIVITY ¹⁷²W, ¹⁷²Re(β⁺), (EC) [from ¹⁶⁵Ho(¹⁴N, 7n), (¹⁶O, 9n)]; measured Eγ, Iγ, T_1/2. Ge(Li) detector, He-jet recoil system.

1985SZ03      Radiochim.Acta 38, 113 (1985)

A.Szymanski, G.W.A.Newton, V.J.Robinson, H.E.Sims

Absolute Gamma Ray Abundances of Re and W Isotopes: Part II, A = 174

RADIOACTIVITY ¹⁷⁴Re(β⁺), (EC) [from ¹⁶⁵Ho(¹⁶O, 7n)]; ¹⁷⁴W(EC) [from ¹⁶⁵Ho(¹⁴N, 5n)]; measured Eγ, Iγ. ¹⁷⁴W, ¹⁷⁴Re deduced absolute γ-abundances.

1984NE06      J.Radioanal.Nucl.Chem. 84, 149 (1984)

G.W.A.Newton, V.J.Robinson, E.M.Shaw, R.J.Smith, H.E.Sims

Single Neutron Transfer Reactions in the Systems: ¹³⁹La + ¹⁶O, ⁹³Nb + ¹²C, ¹⁴N, ¹⁶O and ²⁰Ne

NUCLEAR REACTIONS, ICPND ¹³⁹La(¹⁶O, ¹⁵O), E=105.8-153.1 MeV; ⁹³Nb(¹²C, ¹³C), E=88.7-171.2 MeV; ⁹³Nb(¹⁴N, ¹⁵N), E=89.4-145.6 MeV; ⁹³Nb(¹⁶O, ¹⁷O), E=117.3-183.6 MeV; ⁹³Nb(²⁰Ne, ²¹Ne), E=112.2-191.4 MeV; measured σ(E), residuals yields, isomer production σ; deduced reaction mechanism.

doi: 10.1007/BF02038191
Citations: PlumX Metrics

1984SZ07      Radiochim.Acta 37, 121 (1984)

A.Szymanski, G.W.A.Newton, V.J.Robinson, S.M.A.Hoffmann, H.E.Sims

Absolute Gamma Ray Abundances of Re and W Isotopes: Part I, A = 175

RADIOACTIVITY ¹⁷⁵W(EC), (β⁺) [from ¹⁶⁵Ho(¹⁴N, 4n)]; ¹⁷⁵Re(EC), (β⁺) [from ¹⁶⁵Ho(¹⁶O, 6n)]; measured Eγ, Iγ. ¹⁷⁵W, ¹⁷⁵Re deduced absolute γ-abundances.

1981NE05      J.Inorg.Nucl.Chem. 43, 1739 (1981)

G.W.A.Newton, V.J.Robinson, E.M.Shaw

Recoil Ranges of Tc Activities from ⁹³Nb(⁴He, xn) Reactions

NUCLEAR REACTIONS ⁹³Nb(α, xn), E=38.4, 56.8 MeV; measured σ for x=2, 3, 4, 5, recoil momenta of Tc isotopes; deduced reaction mechanism.

doi: 10.1016/0022-1902(81)80375-2
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1339.

1981NE07      J.Inorg.Nucl.Chem. 43, 2227 (1981)

G.W.A.Newton, V.J.Robinson, E.M.Shaw

¹⁰³Rh(α, xn)(107-x)Ag Reactions

NUCLEAR REACTIONS ¹⁰³Rh(α, xn), E=16-82 MeV; measured production σ(E) for ^{102m,102,104,104m,106,106m,105}Ag, isomer ratios; deduced reaction mechanism.

doi: 10.1016/0022-1902(81)80237-0
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0327.

1980CU02      J.Phys.(London) G6, 127 (1980)

J.G.Cuninghame, J.A.B.Goodall, J.E.Freeman, G.W.A.Newton, V.J.Robinson, J.L.Durell, G.S.Foote, I.S.Grant, M.Rathle

Isomer Ratios in Fission Fragments at High Excitation

NUCLEAR REACTIONS ²⁰⁹Bi(¹²C, X), E=75-112 MeV; ¹⁹⁶Pt(¹²C, X), E=79-105 MeV; ²⁰⁴Pb(α, X), E=49-79 MeV; measured isomer yield ratios for ^{120,124,126,128}Sb, ⁸⁴Br. Evaporation model.

doi: 10.1088/0305-4616/6/1/018
Citations: PlumX Metrics

1979BR11      J.Inorg.Nucl.Chem. 41, 617 (1979)

C.L.Branquinho, S.M.A.Hoffmann, G.W.A.Newton, V.J.Robinson, H.-Y.Wang, I.S.Grant, J.A.B.Goodall

Excitation Functions and Isomer Ratios in the Reactions ⁹³Nb(α, xn)(X = 1-4)

NUCLEAR REACTIONS ⁹³Nb(α, n), E=15-25 MeV; ⁹³Nb(α, 2n), E=15-50 MeV; ⁹³Nb(α, 3n), E=40-70 MeV; measured σ(E), isomeric ratio; deduced reaction mechanisms.

doi: 10.1016/0022-1902(79)80343-7
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0140.

1979BR16      J.Inorg.Nucl.Chem. 41, 791 (1979)

C.L.Branquinho, S.M.A.Hoffmann, G.W.A.Newton, V.J.Robinson, I.S.Grant, J.A.B.Goodall

Spallation Cross Sections in the System ⁹³Nb + ⁴He

NUCLEAR REACTIONS ⁹²Nb(α, 5n), (α, 3np), (α, 2p), (α, α'n), (α, α'xn), E=15-72 MeV; measured production σ(E) for ⁹²Tc, ^93mMo, ^95m,95Nb, ^90m,90Nb, ^89m,89Nb. Compound nucleus model with pre-equilibrium nucleon emission.

doi: 10.1016/0022-1902(79)80267-5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1328.

1977BR13      J.Inorg.Nucl.Chem. 39, 921 (1977)

C.L.Branquinho, V.J.Robinson

Charge Distribution of Fission Products in the Reaction ²⁰⁹Bi(¹²C, Fission)

NUCLEAR REACTIONS ²⁰⁹Bi(¹²C, F), E=40, 53, 66 MeV; measured σ(A, Z).

doi: 10.1016/0022-1902(77)80235-2
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0153.

1976AL17      Radiochem.Radioanal.Lett. 25, 345 (1976)

M.A.A.Al-Janabi, G.W.A.Newton, V.J.Robinson

Photofission of Uranium by High Energy Bremsstrahlung

NUCLEAR REACTIONS U(γ, F), E=3.5 GeV bremsstrahlung; measured σ(A, Z).

1976FR06      J.Inorg.Nucl.Chem. 38, 941 (1976)

J.E.Freeman, A.K.A.R.Ahmed, G.W.A.Newton, V.J.Robinson, K.Gregory, I.S.Grant

Radiochemical Studies of Charge Distribution and Dispersion in the ¹²C-Induced Fission of ²⁰⁹Bi

NUCLEAR REACTIONS ²⁰⁹Bi(¹²C, F), E ≤ 115 MeV; measured radiochemical yields of Sb, Y, Cd, Nb.

doi: 10.1016/0022-1902(76)80002-4
Citations: PlumX Metrics

1973NE06      J.Inorg.Nucl.Chem. 35, 1435 (1973)

G.W.A.Newton, V.J.Robinson, M.Skarestad, J.D.Hemingway

Rare Earth Yields from Bombardment of Tungsten Targets with 24 GeV Protons

NUCLEAR REACTIONS W(p, X), E=24 GeV; measured σ. ^143,144Pm, ¹⁵⁴Sm, ^148,149Eu, ^{146,148,151,153}Gd, ¹⁵⁹Dy, ¹⁶⁸Tm, ¹⁶⁹Yb deduced chain yield.

doi: 10.1016/0022-1902(73)80229-5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0670.

1964BU02      J.Inorg.Nucl.Chem. 26, 1 (1964)

F.D.S.Butement, V.J.Robinson

New Isotopes of Emanation Em²²³ and Em²²⁴

NUCLEAR STRUCTURE ²²⁴Rn, ²²³Rn; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0022-1902(64)80224-4
Citations: PlumX Metrics

1964BU05      J.Inorg.Nucl.Chem. 26, 491 (1964)

F.D.S.Butement, V.J.Robinson, S.M.Qaim

A New Isotope of Lead: ²¹³Pb

NUCLEAR STRUCTURE ²¹³Pb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0022-1902(64)80279-7
Citations: PlumX Metrics