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NSR database version of April 11, 2024.

Search: Author = S.M.Tang

Found 16 matches.

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1994LI45      Nucl.Instrum.Methods Phys.Res. B85, 621 (1994)

S.C.Liew, K.K.Loh, S.M.Tang

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
Citations: PlumX Metrics


1994OR06      At.Data Nucl.Data Tables 56, 159 (1994)

I.Orlic, C.H.Sow, S.M.Tang

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1967HS01      Nucl.Phys. A94, 146 (1967)

S.T.Hsue, M.U.Kim, S.M.Tang

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1966HS03      Bull.Am.Phys.Soc. 11, 808 AD8 (1966)

S.T.Hsue, M.U.Kim, S.M.Tang

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
Citations: PlumX Metrics


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