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NSR database version of April 27, 2024.

Search: Author = T.Petrovic

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2024PE03      Appl.Radiat.Isot. 205, 111182 (2024)

T.Petrovic, M.Korun, B.Vodenik, B.Zorko

Calculation of the detection limits with the least-squares method in gamma-ray spectrometry: A simple procedure

doi: 10.1016/j.apradiso.2024.111182
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2017LI33      Phys.Lett. B 773, 553 (2017)

M.Lipoglavsek, S.Markelj, M.Mihovilovic, T.Petrovic, S.Stajner, M.Vencelj, J.Vesic

Observation of electron emission in the nuclear reaction between protons and deuterons

NUCLEAR REACTIONS ²H(p, X)³He, E=260 keV; measured reaction products, Eβ, Iβ, X-rays; deduced electron yields.

doi: 10.1016/j.physletb.2017.09.004
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2015CV01      Appl.Radiat.Isot. 104, 160 (2015)

A.Cvetinovic, A.Likar, M.Lipoglavsek, A.Mihelic, T.Petrovic, J.Vesic, B.Vodenik

Precise measurement of the half-life of ⁶¹Cu

RADIOACTIVITY ⁶¹Cu(β⁺), (EC) [from ⁶⁰Ni(p, γ)]; measured decay products, Eγ, Iγ; deduced T_1/2, level energies, J, π. Comparison with theoretical calculations.

doi: 10.1016/j.apradiso.2015.07.005
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Data from this article have been entered in the XUNDL database. For more information, click here.

2015VE03      Acta Phys.Pol. B46, 467 (2015)

J.Vesic, A.Cvetinovic, T.Petrovic, M.Lipoglavsek

Effect of Electron Screening on Nuclear Reaction Rates

NUCLEAR REACTIONS ²H(p, γ), E=0.24-0.44 MeV; measured reaction products, Eγ, Iγ; deduced σ, lack of sensitivity for the value of the electron screening potential.

doi: 10.5506/APhysPolB.46.467
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2014VE03      Eur.Phys.J. A 50, 153 (2014)

J.Vesic, A.Cvetinovic, M.Lipoglavsek, T.Petrovic

Influence of electronic environment on nuclear reaction rates

NUCLEAR REACTIONS ¹H(⁷Li, α), E=0.34-2.07 MeV; measured reaction products for hydrogen-implanted Ni, Zn, Pt, Pd targets; deduced screening potential, astrophysical S-factor. ⁵⁵Mn(p, n), (p, γ), E=1500-1595 keV; measured reaction products; deduced thick target γ yield ratio for Mn and MnO targets, neutron number near 1.54 MeV resonance. ¹¹⁵Cd(p, n), E=1560-2600 keV; measured Eγ, Iγ, nγ-coin for Cd and CdO; deduced neutron number per 299 keV γ transition. ⁵¹V(p, γ)(p, n), E=700-1600 keV; measured thick target Eγ, Iγ, nγ-coin for V and VO2 targets; deduced ratio of 1434 keV γ yields. ¹¹⁵In(p, n), E=1750-2500 keV; measured neutrons, X-ray, nX-coin for In and In2O3 targets; deduced neutron number per 24 keV X-ray.

doi: 10.1140/epja/i2014-14153-3
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2013GA25      Eur.Phys.J. A 49, 70 (2013)

J.Gajevic, A.Cvetinovic, A.Likar, M.Lipoglavsek, P.Pelicon, T.Petrovic, A.Sanchez Ortiz

Electron screening in nickel

ATOMIC PHYSICS Ni(p, γ), (p, X), E=0.86-3.08 MeV; measured thick target Eγ, Iγ using HPGe, backscattered protons, X-rays from PIXE using SiLi from metallic Ni and NiO; deduced isotope yields, levels, γ transitions, branching ratios, electron screening potential, electron density vs intranuclear distance.

doi: 10.1140/epja/i2013-13070-3
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