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NSR database version of April 27, 2024.

Search: Author = J.R.Tesmer

Found 14 matches.

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2007DE31      Nucl.Instrum.Methods Phys.Res. B261, 405 (2007)

D.J.DeSimone, C.Haertling, J.R.Tesmer, Y.Q.Wang

Measurement of the D(p, p)D cross section at laboratory backward angles of 151 degrees and 167 degrees

NUCLEAR REACTIONS 2H(p, p), E=1.9-3.0 MeV; measured elastic scattering σ at backward angles.

doi: 10.1016/j.nimb.2007.03.027
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1574.


2002VE02      Nucl.Instrum.Methods Phys.Res. B187, 383 (2002)

R.D.Verda, J.R.Tesmer, M.Nastasi, R.W.Bower

An Energy Spread Correction for Depth Profiling by Elastic Recoil Detection Analysis

doi: 10.1016/S0168-583X(01)01138-7
Citations: PlumX Metrics


1993FO09      Nucl.Instrum.Methods Phys.Res. B 79, 454 (1993)

L.A.Foster, J.R.Tesmer, T.R.Jervis, M.Nastasi

Non-Rutherford backscattering analysis of nitrogen content in titanium substrates

NUCLEAR REACTIONS 14N(α, α), E=8.6-8.9 MeV; measured products, 14N; deduced σ(θ). Data were imported from EXFOR entry C1364.

doi: 10.1016/0168-583X(93)95386-J
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1364.


1988MA59      App.Phys.Lett. 52, 2177 (1988)

J.A.Martin, M.Nastasi, J.R.Tesmer, C.J.Maggiore

High-Energy Elastic Backscattering of Helium Ions for Compositional Analysis of High-Temperature Superconductor Thin Films

NUCLEAR REACTIONS 16O, Ba(α, α), E=8.2-9.1 MeV; Y, Cu, Ba(α, α), E=2-9 MeV; measured relative σ(θ=166°).

doi: 10.1063/1.99761
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0760.


1979PE08      Phys.Rev.Lett. 43, 675 (1979)

J.C.Peng, N.Stein, J.W.Sunier, D.M.Drake, J.D.Moses, J.A.Cizewski, J.R.Tesmer

Study of the Reactions 46,48Ti(14C, 16O)44,46Ca and 50,52Cr(14C, 16O)48,50Ti at 51 MeV

NUCLEAR REACTIONS 46,48Ti, 50,52Cr(14C, 16O), E=51 MeV; measured σ(θ). 44,46Ca levels deduced configuration, S, reaction mechanism. Finite range DWBA calculations.

doi: 10.1103/PhysRevLett.43.675
Citations: PlumX Metrics


1974GR07      Nucl.Phys. A229, 346 (1974)

J.A.Grau, F.A.Rickey, G.J.Smith, P.C.Simms, J.R.Tesmer

The Collective Excitation of 103Pd Following (Heavy Ion, xn) Reactions

NUCLEAR REACTIONS 100Ru(α, nγ), E=16-24 MeV; 94Zr(12C, 3nγ), E=44-54 MeV; measured σ(Eα, Eγ), σ(E(12C), Eγ), σ(Eγ, θ), γγ-coin, pγ. 103Pd deduced levels, J, π, T1/2, γ-multipolarity.

doi: 10.1016/0375-9474(74)90792-1
Citations: PlumX Metrics


1974SI02      Phys.Rev. C9, 684 (1974)

P.C.Simms, G.J.Smith, F.A.Rickey, J.A.Grau, J.R.Tesmer, R.M.Steffen

Collective Excitation of 101Pd Following (Heavy Ion, xn) Reactions

NUCLEAR REACTIONS 99Ru(α, 2nγ), E=16-24 MeV; 92Zr(12C, 3nγ), E=45-56 MeV; 88Sr(16O, 3nγ), E=56-64 MeV; measured σ(E)γ, γ-γcoin, σ(θ)γ, linear p; 101Pd deduced levels, J, π.

doi: 10.1103/PhysRevC.9.684
Citations: PlumX Metrics


1973SI07      Phys.Rev.Lett. 30, 710 (1973)

P.C.Simms, F.A.Rickey, J.R.Tesmer

Evidence for Well-Developed Band Structure in 101Pd

NUCLEAR REACTIONS 99Ru(α, 2nγ), 92Zr(12C, 3nγ), 88Sr(16O, 3nγ), E(16O)=56 MeV; measured σ(E), Eγ, Iγ, γ(θ), γγ-coin. 101Pd deduced levels, J, π, ±.

doi: 10.1103/PhysRevLett.30.710
Citations: PlumX Metrics


1973SI09      Phys.Rev. C7, 1631 (1973)

P.C.Simms, R.Anderson, F.A.Rickey, G.Smith, R.M.Steffen, J.R.Tesmer

Level Structure of 102Pd Investigated by (α, xn;γ) Reactions

NUCLEAR REACTIONS 99Ru(α, nγ), E=16-20 MeV; measured Eγ, Iγ, γγ-coin, Iγ(θ). 102Pd deduced levels, J, π.

doi: 10.1103/PhysRevC.7.1631
Citations: PlumX Metrics


1972TE01      Phys.Rev. C5, 864 (1972)

J.R.Tesmer, F.H.Schmidt

Substate Excitation of 2+ States Produced by Inelastic Scattering of Protons on 12C, 54Fe, and 58Ni

NUCLEAR REACTIONS 12C, 54Fe, 58Ni(p, p'), E=20, 19.6, 20 MeV; measured p'γ(θ), σ(θ(p')); deduced substate excitation probabilities.

doi: 10.1103/PhysRevC.5.864
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0079.


1971RU03      Phys.Rev. C3, 1595 (1971)

P.A.Russo, R.Vandenbosch, M.Mehta, J.R.Tesmer, K.L.Wolf

Spin Isomers of the Shape Isomer 237mPu

RADIOACTIVITY, Fission 237mPu(SF); measured T1/2; deduced shape isomerism.

doi: 10.1103/PhysRevC.3.1595
Citations: PlumX Metrics


1971TE03      Phys.Rev.Lett. 26, 857 (1971)

J.R.Tesmer, F.H.Schmidt

Spin Dependence in the Excitation of the First 2+ State of 54Fe

NUCLEAR REACTIONS 54Fe(p, p'γ), E=19.6 MeV; measured nothing; analyzed p'γ(θ) data; deduced J-dependence of excitation of first 2+ state. 54Fe deduced deformation parameters.

doi: 10.1103/PhysRevLett.26.857
Citations: PlumX Metrics


1969KO07      Phys.Rev. 180, 1006 (1969)

W.A.Kolasinski, J.Eenmaa, F.H.Schmidt, H.Sherif, J.R.Tesmer

Spin Flip in the Inelastic Scattering of Protons

NUCLEAR REACTIONS 12C, 58,60,64Ni(p, p), (p, p'), E=9-20 MeV; measured σ(E;Ep', θ); deduced spin-flip probability(θ).

doi: 10.1103/PhysRev.180.1006
Citations: PlumX Metrics


1968EE01      Phys.Letters 28B, 321(1968)

J.Eenmaa, F.H.Schmidt, J.R.Tesmer

Proton Spin Flip in the Reaction 58Ni(p, p'γ)58Ni*(1.45 Mev) at 20 MeV

NUCLEAR REACTIONS 58Ni(p, p'γ), E=20 MeV; measured σ(Ep', θ); deduced proton spin flip probability. 58Ni deduced levels.

doi: 10.1016/0370-2693(68)90121-4
Citations: PlumX Metrics


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