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NSR database version of May 20, 2024.

Search: Author = G.W.Newton

Found 18 matches.

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1990EN01      J.Phys.(London) G16, 105 (1990)

J.G.England, I.S.Grant, J.A.R.Griffith, D.E.Evans, D.A.Eastham, G.W.A.Newton, P.M.Walker

Isotope Shifts and Hyperfine Splittings in 144-154Sm I

RADIOACTIVITY 145,151,153,146Sm; measured isotope shifts, hfs; deduced hfs constants, rms radii differences, μ, Q. Other data input.

NUCLEAR MOMENTS 144,147,148,149,150,152,154Sm; measured isotope shifts, hfs; deduced hfs constants, rms radii differences, μ, Q. Other data input.

NUCLEAR STRUCTURE 145,147,149,151,153Sm; calculated μ, quadrupole moment.

doi: 10.1088/0954-3899/16/1/014
Citations: PlumX Metrics


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, T1/2. 171Ta deduced transitions, T1/2. 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 T1/2. 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, T1/2. 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 T1/2, γ transitions, abundances. 172Re deduced T1/2. 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, T1/2. 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.


1984EA02      J.Phys.(London) G10, L271 (1984)

D.A.Eastham, J.G.England, D.E.Evans, M.J.Fawcett, I.S.Grant, J.A.R.Griffith, G.W.A.Newton, P.M.Walker

Optical Isotope Shift and Hyperfine Structure of 153Sm

RADIOACTIVITY 153Sm(β-) [from 152Sm neutron irradiation]; measured optical isotope shift, hfs. 146,147,148,149,150,151,152,153,154Sm deduced rms charge radii relative to 144Sm.

doi: 10.1088/0305-4616/10/12/002
Citations: PlumX Metrics


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.


1981AU10      J.Inorg.Nucl.Chem. 43, 2611 (1981)

L.T.Auler, A.G.Da Silva, G.W.A.Newton

Excitation Functions and Isomer Ratios in 93Nb(3He, xn) Reactions with X = 2 and 3

NUCLEAR REACTIONS 93Nb(3He, xn), E=14-36 MeV; measured σ(E) for x=2, 3; deduced preequilibrium process role. 93,94Tc deduced isomer production ratios. Activation technique. Hybrid, exciton models.

doi: 10.1016/0022-1902(81)80585-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1338.


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,105Ag, 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 120,124,126,128Sb, 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.


1977ES01      Phys.Rev. C15, 319 (1977)

R.A.Esterlund, D.Molzahn, R.Brandt, P.Patzelt, P.Vater, A.H.Boos, M.R.Chandratillake, I.S.Grant, J.D.Hemingway, G.W.A.Newton

Search for Long-Lived Superheavy Elements in the Reaction System 238U + 9.6-MeV/Nucleon 63,65Cu

NUCLEAR REACTIONS 238U(63Cu, X), (65Cu, X), E=9.6 MeV/nucleon; measured σ for production of superheavy elements, 254Cf.

doi: 10.1103/PhysRevC.15.319
Citations: PlumX Metrics


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, 146,148,151,153Gd, 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.


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