NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = D.H.Templeton Found 18 matches. 1963HA07 Phys.Rev. 129, 1601 (1963) J.N.Haag, D.A.Shirley, D.H.Templeton Nuclear Alignment of Ce137m, Ce137, Ce139, Ce141, and Ce143 NUCLEAR STRUCTURE 143Ce, 139Ce, 137Ce, 141Ce; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.129.1601
1963SH01 Bull.Am.Phys.Soc. 8, No.1, 74, VA5 (1963) D.A.Shirley, D.H.Templeton, J.N.Haag Nuclear Alignment of Ce137m, Ce137, Ce139, Ce141, and Ce143 NUCLEAR STRUCTURE 143Ce, 139Ce, 137Ce, 141Ce; measured not abstracted; deduced nuclear properties.
1961HA05 Phys.Rev. 121, 591 (1961) J.N.Haag, C.E.Johnson, D.A.Shirley, D.H.Templeton Nuclear Moment of Ce137m by Nuclear Alignment NUCLEAR STRUCTURE 137Ce; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.121.591
1954MI01 Phys.Rev. 93, 1422 (1954) Mass Assignments by Isotope Separation NUCLEAR REACTIONS Au(α, xn), E=40 MeV; measured 198Tl, 166,169Yb, 161,160Er, 166,165,167Tm isotope masses. Tof isotope separator. RADIOACTIVITY 198m,198Tl(EC), (β+) [from Au(α, xn), E=40 MeV]; 169,166Yb, 160Er, 167Tm(EC); 165,166Tm, 161Er(EC), (β+); measured T1/2. Tof isotope separator mass assignment.
doi: 10.1103/PhysRev.93.1422
1954MI16 Phys.Rev. 93, 1422 (1954) Mass Assignments by Isotope Separation
doi: 10.1103/PhysRev.93.1422
1952CA39 Phys.Rev. 88, 1126 (1952) Some Neutron Deficient Strontium Isotopes
doi: 10.1103/PhysRev.88.1126
1951KA03 Phys.Rev. 81, 510 (1951) Polonium Isotopes Produced with High Energy Particles
doi: 10.1103/PhysRev.81.510
1951KA37 Phys.Rev. 83, 390 (1951) D.G.Karraker, A.Ghiorso, D.H.Templeton Alpha-Decay Energies of Polonium Isotopes RADIOACTIVITY 200,201Po(α), (EC), 206,207,208,209Po(α), 226Ra(α) [from 209Bi(p, X), E=100 MeV]; measured decay products, Eα, Iα; deduced α-particles energies, T1/2. Comparison with available data. Berkeley 184-inch and 60-inch cyclotrons.
doi: 10.1103/PhysRev.83.390
1950FI11 J.Am.Chem.Soc. 72, 2818 (1950) Radioactive Isotopes of Barium
doi: 10.1021/ja01162a558
1950FI16 Phys.Rev. 77, 614 (1950) R.W.Fink, F.L.Reynolds, D.H.Templeton Neutron-Deficient Cesium Isotopes
doi: 10.1103/PhysRev.77.614
1950KA62 Phys.Rev. 80, 646 (1950) Radioactive Isotopes of Rubidium
doi: 10.1103/PhysRev.80.646
1950TE03 Phys.Rev. 78, 312 (1950) The Half-Life of Po208
doi: 10.1103/PhysRev.78.312
1949OR01 Phys.Rev. 75, 1100 (1949) D.A.Orth, L.Marquez, W.J.Heiman, D.H.Templeton Radioactive Thallium Isotopes Produced from Gold
doi: 10.1103/PhysRev.75.1100
1949RE19 Phys.Rev. 75, 313 (1949) F.L.Reynolds, D.G.Karraker, D.H.Templeton Mass Spectrographic Assignment of Rubidium Isotopes RADIOACTIVITY 81,82Rb(EC), (β+) [Br(α, X), E=20, 100 MeV]; measured decay products, Eβ, Iβ; deduced T1/2, decay radiations. The Berkeley 60-inch and 184-inch cyclotrons.
doi: 10.1103/PhysRev.75.313
1948TE01 Phys.Rev. 73, 1211 (1948) Artificial Alpha-Active Bismuth Isotopes
doi: 10.1103/PhysRev.73.1211
1947HO06 Phys.Rev. 71, 552 (1947) J.J.Howland, D.H.Templeton, I.Perlman Artificial Radioactive Isotopes of Polonium, Bismuth and Lead RADIOACTIVITY 206,207Po(α), (EC), 208Po(α), 204Bi(EC) [from Pb(α, X), E=40 MeV; Pb(d, 2n), E=20 MeV]; 206Bi, 203Pb(EC), 204Pb(IT); measured decay products. 208Bi; deduced T1/2.
doi: 10.1103/PhysRev.71.552
1947TE01 Phys.Rev. 72, 758 (1947) D.H.Templeton, J.J.Howland, I.Perlman Artificial Radioactive Isotopes of Polonium
doi: 10.1103/PhysRev.72.758
1947TE03 Phys.Rev. 72, 766 (1947) D.H.Templeton, J.J.Howland, I.Perlman Artificial Radioactive Isotopes of Bismuth and Lead
doi: 10.1103/PhysRev.72.766
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