NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = G.W.Newton Found 18 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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