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NSR database version of May 1, 2024.

Search: Author = J.Desimoni

Found 9 matches.

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1991RE09      J.Phys.Condens.Matter 3, 3625 (1991)

M.Renteria, A.G.Bibiloni, M.S.Moreno, J.Desimoni, R.C.Mercader, A.Bartos, M.Uhrmacher, K.P.Lieb

Hyperfine Interactions of ¹¹¹In-Implanted Tin Oxide Thin Films

RADIOACTIVITY ¹¹¹In; measured γγ(θ, H); deduced ¹¹¹In hyperfine interaction in tin oxides. Conversion electron Mossbauer spectroscopy.

doi: 10.1088/0953-8984/3/20/023
Citations: PlumX Metrics

1990DE08      Phys.Rev. B41, 1443 (1990)

J.Desimoni, A.G.Bibiloni, C.P.Massolo, M.Renteria

Hyperfine Interactions in the Cubic Semiconductor CdO

RADIOACTIVITY ¹¹¹In(EC); measured γγ(θ, H, t); deduced hyperfine interaction in cubic CdO.

doi: 10.1103/PhysRevB.41.1443
Citations: PlumX Metrics

1988BI04      Phys.Rev. B38, 20 (1988)

A.G.Bibiloni, J.Desimoni, C.P.Massolo, M.Renteria

Hyperfine Interaction between Indium Atoms and Oxygen Vacancies in Stannic Oxide

RADIOACTIVITY ¹¹¹In(EC); measured γγ(θ, H, t); deduced static quadrupole interaction parameters.

doi: 10.1103/PhysRevB.38.20
Citations: PlumX Metrics

1987DE25      Hyperfine Interactions 34, 271 (1987)

J.Desimoni, A.G.Bibiloni, L.A.Mendoza-Zelis, L.C.Damonte, F.H.Sanchez, A.Lopez-Garcia

TDPAC Studies in the Semiconductors SnO₂ and Cu₂O

RADIOACTIVITY ¹¹¹In(EC); measured γγ(θ, H, t).

doi: 10.1007/BF02072719
Citations: PlumX Metrics

1986DA07      Hyperfine Interactions 30, 57 (1986)

L.C.Damonte, L.A.Mendoza-Zelis, A.G.Bibiloni, J.Desimoni, C.P.Massolo, A.R.Lopez-Garcia

Electron-Capture Aftereffects: The case of CdCl₂

RADIOACTIVITY ¹¹¹In(EC); measured γγ(θ, H, t); deduced EC-capture after effects in CdCl₂.

doi: 10.1007/BF02400101
Citations: PlumX Metrics

1986MA14      Hyperfine Interactions 30, 1 (1986)

C.P.Massolo, J.Desimoni, A.G.Bibiloni, L.A.Mendoza-Zelis, F.H.Sanchez, A.F.Pasquevich, A.R.Lopez-Garcia

TDPAC Studies of After-Effects in In₂O₃ Precipitates in a Silver Matrix

RADIOACTIVITY ¹¹¹In(EC) [from ¹⁰⁹Ag(α, 2n), E=56 MeV]; measured γγ(θ, H, t); deduced atomic recovery probability for Cd impurities in In₂O₃.

NUCLEAR REACTIONS ¹⁰⁹Ag(α, 2n), E=56 MeV; measured γγ(θ, H, t); deduced atomic recovery probability for Cd impurities in In₂O₃.

doi: 10.1007/BF02400095
Citations: PlumX Metrics

1986ME09      Phys.Rev. B34, 2982 (1986)

L.A.Mendoza-Zelis, L.C.Damonte, A.G.Bibiloni, J.Desimoni, A.R.Lopez-Garcia

Time-Differential Perturbed-Angular-Correlation Study of the Electric Field Gradient in Amorphous Zr₆₈Hf₂Cu₃₀

RADIOACTIVITY ¹⁸¹Hf(β^-) [from ¹⁸⁰Hf(n, γ), E=thermal]; measured γγ(θ, H, t); deduced electric field gradient at Zr sites. Amorphous, crystalline Zr₆₈Hf₂Cu₃₀ alloys.

doi: 10.1103/PhysRevB.34.2982
Citations: PlumX Metrics

1984BI01      Phys.Rev. B29, 1109 (1984)

A.G.Bibiloni, J.Desimoni, C.P.Massolo, L.Mendoza-Zelis, A.F.Pasquevich, F.H.Sanchez, A.Lopez-Garcia

Temperature Dependence of Electron-Capture After Effects in the Semiconductor In₂O₃

RADIOACTIVITY ¹¹¹In(EC); measured γγ(θ, H, t); deduced electron capture after effects.

doi: 10.1103/PhysRevB.29.1109
Citations: PlumX Metrics

1984SA25      Hyperfine Interactions 20, 195 (1984)

F.H.Sanchez, C.P.Massolo, A.G.Bibiloni, J.Desimoni, A.R.Lopez Garcia

A Simple Model to Analyze TDPAC Measurements of Electric Field Gradients Due to Repulsive Impurities in a Cubic Lattice. Its Application to the AgIn System

RADIOACTIVITY ¹¹¹In(EC) [from ¹⁰⁹Ag(α, 2n), E=56 MeV]; measured γγ(θ, H, t); deduced ¹¹¹Cd probe electric field gradient at AgIn alloys.