NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = S.M.Tang Found 16 matches. 1994LI45 Nucl.Instrum.Methods Phys.Res. B85, 621 (1994) Application of an Iterative Maximum-Likelihood Algorithm in PIXE Depth Profiling of Trace Elements NUCLEAR REACTIONS 31P(p, X), E=0.6-2 MeV; calculated K X-ray yields; deduced application to trace elements depth profiling. Iterative maximum likelihood algorithm method. ATOMIC PHYSICS 31P(p, X), E=0.6-2 MeV; calculated K X-ray yields; deduced application to trace elements depth profiling. Interative maximum likelihood algorithm method.
doi: 10.1016/0168-583X(94)95894-7
1994OR06 At.Data Nucl.Data Tables 56, 159 (1994) Experimental L-Shell X-Ray Production and Ionization Cross Sections for Proton Impact COMPILATION Z=14-92; compiled proton induced L X-ray production, L-shell ionization σ data.
doi: 10.1006/adnd.1994.1005
1994OS06 Nucl.Instrum.Methods Phys.Res. B85, 499 (1994) T.Osipowicz, S.C.Liew, K.K.Loh, I.Orlic, S.M.Tang, Th.Weber Reconstruction of Ar Depth Profiles from PIXE Measurements NUCLEAR REACTIONS Ar(α, X), E=1.5, 1.3 MeV; measured X-ray yields, Ar implantation on Al samples; deduced Ar depth profiles reconstruction.
doi: 10.1016/0168-583X(94)95871-8
1994SO11 Nucl.Instrum.Methods Phys.Res. B85, 133 (1994) C.H.Sow, I.Orlic, T.Osipowicz, S.M.Tang L X-Ray Production Cross Sections of Medium Z Elements for 0.4 to 2.0 MeV Protons NUCLEAR REACTIONS Ce, La, Ba, Te, Sb, Sn, In, Ag(p, X), E=0.4-2 MeV; measured partial L X-ray production σ. Model comparison. ATOMIC PHYSICS Ce, La, Ba, Te, Sb, Sn, In, Ag(p, X), E=0.4-2 MeV; measured partial L X-ray production σ. Model comparison.
doi: 10.1016/0168-583X(94)95800-9
1987PE05 Phys.Rev.Lett. 58, 2027 (1987) J.C.Peng, J.Kapustinsky, C.Lee, M.J.Leitch, T.K.Li, C.Liu, J.M.Moss, J.E.Simmons, S.M.Tang, C.Smith, R.R.Whitney Observation of Eta-Meson Production in the Reaction π- + 3He → Eta + t NUCLEAR REACTIONS 3He(π-, t), E at 680 MeV/c; measured triton spectra; deduced eta-meson production σ. Large acceptance spectrometer.
doi: 10.1103/PhysRevLett.58.2027
1984LA02 J.Phys.(London) G10, 247 (1984) V.Lakshminarayana, T.T.Neo, S.M.Tang, A.Rajaratnam Internal Conversion Studies in the Decay of 84mRb RADIOACTIVITY 84mRb(IT) [from Rb(n, 2n), E=14 MeV]; measured Eγ, Iγ, X-ray(γ)-, γγ-coin. 84Rb levels deduced J, π, total, K-shell, ICC, γ-transition probabilities, enhancements.
doi: 10.1088/0305-4616/10/2/015
1983LA26 Nuovo Cim. 78A, 444 (1983) V.Lakshminarayana, T.T.Neo, S.M.Tang, A.Rajaratnam Total-Conversion Coefficients of High Multipole Transitions in the Decay of 197mPt RADIOACTIVITY 197mPt(β-), (IT) [from Pt(n, 2n), E=fast]; measured Eγ, Iγ. 197Pt deduced transition ICC. 197Au deduced relative Iγ, ICC. High resolution hyperpure Ge system.
doi: 10.1007/BF02962239
1969GE05 Nucl.Phys. A134, 141(1969) D.A.Gedcke, S.T.Lam, S.M.Tang, G.M.Stinson, J.T.Sample, T.B.Grandy, W.J.McDonald, W.K.Dawson, G.C.Neilson The 40Ca(d, n)41Sc Reaction; Neutron Polarization and Angular Distribution Measurements NUCLEAR REACTIONS 40Ca(d, n), E = 5.0, 6.0, 6.5 MeV; measured P(θ), σ(θ). 41Sc deduced levels, L, S, Q. Natural target.
doi: 10.1016/0375-9474(69)90689-7
1969TA02 Nucl.Phys. A125, 289(1969) S.M.Tang, B.D.Sowerby, D.M.Sheppard Study of Levels in 24Mg by the 23Na(d, n)24Mg Reaction NUCLEAR REACTIONS 23Na(d, n), E=5.5 MeV; measured σ(En, θ). 24Mg deduced levels, L(p), π, J, T, S. 24Na levels deduced J, π. Natural targets.
doi: 10.1016/0375-9474(69)91074-4
1968LA15 Nucl.Phys. A119, 146 (1968) S.T.Lam, D.A.Gedcke, G.M.Stinson, S.M.Tang, J.T.Sample Polarization of Neutrons from the Reaction 28Si(d, n)29P at E = 5.0 MeV NUCLEAR REACTIONS 28Si(d, n), E=4.64-5.50 MeV; measured σ(E;En, θ), polarization P(n)(En, θ). 29P levels deduced J. Natural target.
doi: 10.1016/0375-9474(68)90811-7
1968LA25 Nucl.Instr.Methods 62, 1 (1968) S.T.Lam, D.A.Gedcke, G.M.Stinson, S.M.Tang, J.T.Sample A Liquid Helium Polarimeter for Fast Neutrons, I. Instrumentation NUCLEAR REACTIONS 28Si(d, n), 40Ca(d, n)E=5.2 MeV; measured P(n).
doi: 10.1016/0029-554X(68)90608-3
1967HS01 Nucl.Phys. A94, 146 (1967) End Point of the RaE Beta Spectrum RADIOACTIVITY 210Bi [RaE from decay of RaD]; measured Eβ, Qβ.
doi: 10.1016/0375-9474(67)90814-7
1966HS01 Nucl.Phys. 80, 657 (1966) S.T.Hsue, L.M.Langer, E.H.Spejewski, S.M.Tang Search for Post-End-Point Electrons and for Evidence of Neutrino Degeneracy RADIOACTIVITY 147Pm, 63Ni; measured Eβ; deduced upper limit Fermi energy of neutrino sea.
doi: 10.1016/0029-5582(66)90072-1
1966HS02 Nucl.Phys. 86, 47 (1966) S.T.Hsue, L.M.Langer, S.M.Tang Precise Determination of the Shape of the Twice Forbidden Beta Spectrum of 137Cs RADIOACTIVITY 137Cs; measured Eβ, Iβ, I(ce), Q; deduced shape factor. 137Ba deduced ICC.
doi: 10.1016/0029-5582(66)90289-6
1966HS03 Bull.Am.Phys.Soc. 11, 808 AD8 (1966) End Point of the RaE Beta Spectrum RADIOACTIVITY 210Bi(β-); measured decay products, Eβ, Iβ; deduced Q-value.
1965HS02 Nucl.Phys. 73, 379 (1965) S.T.Hsue, L.M.Langer, S.M.Tang, D.A.Zollman 124Sb Spectrum Shape RADIOACTIVITY 124Sb [from 123Sb(n, γ)]; measured Eβ (spectrum shape), Qβ.
doi: 10.1016/0029-5582(65)90683-8
Back to query form |