NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = M.Krcmar Found 18 matches. 2001KR21 Phys.Rev. D64, 115016 (2001) M.Krcmar, Z.Krecak, A.Ljubicic, M.Stipcevic, D.A.Bradley Search for Solar Axions using 7Li
doi: 10.1103/PhysRevD.64.115016
2001KR26 Fizika(Zagreb) B10, 247 (2001) Z.Krecak, M.Krcmar, S.Kaucic, A.Ljubicic Experimental Arrangement for Investigation of β+-Decay End-Point Energies RADIOACTIVITY 58Co(β+); measured Eβ, βγ-coin; deduced end-point energy.
1998KR24 Phys.Lett. 442B, 38 (1998) M.Krcmar, Z.Krecak, M.Stipcevic, A.Ljubicic, D.A.Bradley Search for Solar Axions using 57Fe NUCLEAR REACTIONS 57Fe(X, γ), E ≈ 14.4 keV; measured γ spectrum; deduced hadronic axion mass upper limit. Solar axions from thermally excited 57Fe.
doi: 10.1016/S0370-2693(98)01231-3
1997TU01 Appl.Radiat.Isot. 48, 45 (1997) T.Tustonic, M.Krcmar, A.Ljubicic, M.Bistrovic Photoactivation of Isomeric Level in 115In NUCLEAR REACTIONS 115In(γ, γ'), E=radioactive source; analyzed isomeric level excitation data; deduced nonresonant contribution to σ.
doi: 10.1016/S0969-8043(96)00059-0
1995KR18 Appl.Radiat.Isot. 46, 477 (1995) M.Krcmar, Z.Krecak, A.Ljubicic, B.A.Logan, D.B.Isabelle, J.Vernois Efficiency of the Channel Electron Multiplier for Low Energy 205Pb Ions RADIOACTIVITY 209Po(α) [from 209Bi(p, n), E=9 MeV]; 205Pb(EC) [from 209Po(α)-decay]; measured α(ce)-coin; deduced channel electron multiplier efficiency vs 205Pb ion energy.
doi: 10.1016/0969-8043(95)00058-5
1995KR19 Appl.Radiat.Isot. 46, 547 (1995) Z.Krecak, M.Krcmar, A.Ljubicic, B.A.Logan, D.B.Isabelle, J.Vernois Experimental Estimation of the Population of the First Excited Level in 205Pb Accompanying α Decay of 209Po RADIOACTIVITY 209Po(α); measured 205Pb level population probability per α-decay.
doi: 10.1016/0969-8043(95)00084-4
1994KR11 Phys.Rev. C50, 1319 (1994) Z.Krecak, M.Krcmar, A.Ljubicic, B.A.Logan, D.B.Isabelle, J.Vernois Measurement of the Half-Life of the First Excited States of 205Pb RADIOACTIVITY 209Po(α); measured α-decay; deduced 205Tl(ν, e)205Pb implications. 205Pb levels deduced structure characteristics, decay T1/2.
doi: 10.1103/PhysRevC.50.1319
1993KR02 Phys.Rev. C47, 906 (1993) M.Krcmar, A.Ljubicic, B.A.Logan, M.Bistrovic Reply to ' Comment on ' Resonant and Nonresonant Contributions to the Photoactivation of 111Cd ' ' NUCLEAR REACTIONS 111Cd(γ, γ'), E=radioactive source; analyzed data; deduced isomeric level excitation, reaction mechanism. Photoactivation using 60Co source.
doi: 10.1103/PhysRevC.47.906
1990KR01 Phys.Rev. C41, 771 (1990) M.Krcmar, S.Kaucic, T.Tustonic, A.Ljubicic, B.A.Logan, M.Bistrovic Resonant and Nonresonant Contributions to the Photoactivation of 111Cd NUCLEAR REACTIONS 111Cd(γ, γ'), E=396 keV; measured isomer excitation probability; deduced nonresonant contributions. Photoactivation, 60Co source.
doi: 10.1103/PhysRevC.41.771
1989BL05 Z.Phys. A333, 321 (1989) S.Blagus, M.Bogovac, D.Hodko, M.Krcmar, D.Miljanic, P.Tomas, M.Vajic, M.Vukovic Search for Neutron Production During Heavy Water Electrolysis on Palladium Electrodes NUCLEAR REACTIONS 2H(d, n), E=low; measured neutron yield upper limit. Comparison with 252Cf source spectra, Pd electrodes, heavy water electrolysis.
1989TO08 Fizika(Zagreb) 21, 209 (1989) P.Tomas, S.Blagus, M.Bogovac, D.Hodko, M.Krcmar, D.Miljanic, V.Pravdic, D.Rendic, M.Vajic, M.Vukovic Deuterium Nuclear Fusion in Metals at Room Temperature NUCLEAR REACTIONS 2H(d, n), E=low; measured no significant neutron excess above background. Heavy water electrolysis, PdD nuclear fusion.
1987KR05 Nucl.Instrum.Methods Phys.Res. A255, 99 (1987) M.Krcmar, A.Ljubicic, B.A.Logan, M.Bistrovic Photoactivation Investigations with 113In and 87Sr NUCLEAR REACTIONS 113In, 87Sr(γ, γ'), E=radioactive source; measured photoactivation σ. 113In, 87Sr deduced isomer excitation mechanism. Ge(Li) detector, 60Co source.
doi: 10.1016/0168-9002(87)91082-5
1986KR01 Phys.Rev. C33, 293 (1986) M.Krcmar, A.Ljubicic, B.A.Logan, M.Bistrovic Photoactivation of Isomeric Levels in 113In and 87Sr NUCLEAR REACTIONS 87Sr, 113In(γ, γ'), E ≈ resonance; measured Eγ, Iγ, photoactivation σ; deduced isomer level production mechanism. Intense 60Co source.
doi: 10.1103/PhysRevC.33.293
1986KR11 Fizika(Zagreb) 18, 171 (1986) M.Krcmar, A.Ljubicic, K.Pisk, B.A.Logan, M.Bistrovic Secondary Photon-Atom Contributions to Nonresonant Excitation of 115In Isomeric Level NUCLEAR REACTIONS 115In(γ, γ'), E=radioactive source; measured isomer nonresonant excitation number per unit time; deduced photon-atom interaction contribution. Various mechanism calculations. Ge(Li) detector, 60Co source.
1985PI06 Phys.Rev. C32, 83 (1985) K.Pisk, M.Krcmar, A.Ljubicic, B.A.Logan Nonradiative versus Radiative Nuclear Excitation in the Positron-K-Electron Annihilation NUCLEAR REACTIONS 115In(γ, γ), E=positron spectrum; calculated radiative to nonradiative level excitation probabilities.
doi: 10.1103/PhysRevC.32.83
1983PI02 Phys.Rev. C27, 1260 (1983) Autoionization Accompanying Emission of Internal Bremsstrahlung in K Capture RADIOACTIVITY 37Ar(EC); 55Fe(EC); calculated simultaneous inner bremsstrahlung, autoionization probability. Feynman diagrams.
doi: 10.1103/PhysRevC.27.1260
1982KR06 Phys.Rev. C25, 2097 (1982) M.Krcmar, A.Ljubicic, K.Pisk, B.A.Logan, M.Vrtar Photoactivation of 111Cd NUCLEAR REACTIONS 111Cd(γ, γ'), E ≈ resonance; measured Eγ, Iγ, σ(E); deduced nonresonant process dominance, isomer excitation probability. 111Cd level deduced Γ. Photoactivation, 60Co source.
doi: 10.1103/PhysRevC.25.2097
1975PA24 Fizika 7, 91 (1975) G.Paic, M.Antic, M.Krcmar, S.Blagus Kα/Kβ Ratio for Cu Measured by Different Modes of Excitation ATOMIC PHYSICS Cu; measured Kα/Kβ.
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