NSR Query Results
Output year order : Descending NSR database version of May 9, 2024. Search: Author = Y.Skakun Found 7 matches. 2022CH11 Nucl.Instrum.Methods Phys.Res. B517, 1 (2022) A.Chekhovska, Ye.Skakun, I.Semisalov, V.Kasilov Intensities of the γ-ray emissions following the 111Sn decay determined via photonuclear reaction yield measurements RADIOACTIVITY 111Sn(EC) [112Sn(γ, n), E<30 MeV]; measured decay products, Eγ, Iγ; deduced γ-ray energies and intensities, yields. Comparison with available data. Electron LINear ACcelerator (LINAC) located at National Science Center "Kharkiv Institute of Physics and Technology" (NSC KIPT).
doi: 10.1016/j.nimb.2022.02.004
2021SE15 Appl.Radiat.Isot. 176, 109843 (2021) I.Semisalov, A.Chekhovska, Ye.Skakun, S.Karpus, V.Kasilov Intensities of the strongest γ-ray transitions originating from the In decay determined via photoactivation yield measurements RADIOACTIVITY 112In(IT), (EC), (β+) [from 113In(γ, n), E=9.44, 15 MeV]; measured decay products, Eγ, Iγ; deduced γ-ray energies and intensities. Comparison with ENSDF library.
doi: 10.1016/j.apradiso.2021.109843
2011SK07 J.Korean Phys.Soc. 59, 1487s (2011) Ye.Skakun, S.N.Utenkov, A.N.Dovbnya, S.M.Qaim, H.H.Coenen Half-Lives of the Isomeric States 102m, gRh NUCLEAR REACTIONS 103Rh(γ, n), E=0-22 MeV; measured 102Rh discrete Eγ, Iγ(t) using bremsstrahlung γ. 102,102mRh deduced T1/2. Compared with Shibata's data.
doi: 10.3938/jkps.59.1487
2008SK01 Appl.Radiat.Isot. 66, 653 (2008) Measurement of excitation functions of helion-induced reactions on enriched Ru targets for production of medically important 103Pd and 101mRh and some other radionuclides NUCLEAR REACTIONS 100Ru(α, n), 101Ru(α, 2n), 101Ru(3He, n), 102Ru(3He.2n), 101Ru(3He, X)101Rh, 102Ru(3He, X)101Rh, 101Ru(3He, X)102Rh, 102Ru(3He, X)102Rh, 101Ru(3He, X)101gRh, 102Ru(3He, X)101gRh, 101Ru(3He, 3n), 102Ru(3He, 4n), 101Ru(3He, 4n), 101Ru(3He, X)100Rh, E<34 MeV; measured Eγ, Iγ, x-ray spectra, excitation functions, σ. X-ray and γ-ray spectrometry, enriched targets, comparison with calculations.
doi: 10.1016/j.apradiso.2007.11.013
2005TA38 Radiochim.Acta 93, 561 (2005) F.Tarkanyi, S.Takacs, A.Hermanne, P.Van den Winkel, R.van der Zwart, Ye.A.Skakun, Yu.N.Shubin, S.F.Kovalev Investigation of the production of the therapeutic radioisotope 114mIn through proton and deuteron induced nuclear reactions on cadmium NUCLEAR REACTIONS 114Cd(p, X)115mIn/114mIn/113mIn/111In/111Ag/110Ag, E ≈ 3-36 MeV; 114Cd(d, X)115mIn/114mIn/113mIn/115Cd/112Ag/111Ag, E ≈ 2-21 MeV; measured σ; deduced thick-target yields.
doi: 10.1524/ract.2005.93.9-10.561
2004SK01 Appl.Radiat.Isot. 60, 33 (2004) Excitation function of the 64Ni(α, p)67Cu reaction for production of 67Cu NUCLEAR REACTIONS 64Ni(α, p), E=6-24 MeV; measured σ; deduced integral yield. Stacked-foil activation, comparison with previous results.
doi: 10.1016/j.apradiso.2003.09.003
2003HI18 Appl.Radiat.Isot. 59, 343 (2003) K.Hilgers, T.Stoll, Y.Skakun, H.H.Coenen, S.M.Qaim Cross-section measurements of the nuclear reactions natZn(d, x)64Cu, 66Zn(d, α)64Cu and 68Zn(p, αn)64Cu for production of 64Cu and technical developments for small-scale production of 67Cu via the 70Zn(p, α)67Cu process NUCLEAR REACTIONS Zn(d, X)64Cu, E=9-13 MeV; 66Zn(d, α), E=5-14 MeV; 68Zn(p, nα), E=8-45 MeV; measured σ; deduced thick-target yields. Stacked-foil activation, radiochemical separation.
doi: 10.1016/S0969-8043(03)00199-4
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