NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = Z.Kovacs Found 49 matches. 2017SZ02 Appl.Radiat.Isot. 119, 94 (2017) F.Szelecsenyi, Z.Kovacs, K.Nagatsu, M.-R.Zhang, K.Suzuki Production cross sections of radioisotopes from 3He-particle induced nuclear reactions on natural titanium NUCLEAR REACTIONS Ti(3He, X)44Sc/46Sc/47Sc/48Sc/48V/48Cr, E<70 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with available data, predictions from TENDL-2015 library.
doi: 10.1016/j.apradiso.2016.10.016
2016SZ01 J.Radioanal.Nucl.Chem. 307, 1877 (2016) F.Szelecsenyi, Z.Kovacs, K.Nagatsu, M.-R.Zhang, K.Suzuki Investigation of deuteron-induced reactions on natGd up to 30 MeV: possibility of production of medically relevant 155Tb and 161Tb radioisotopes NUCLEAR REACTIONS Gd(d, X)155Tb/156Tb/160Tb/161Tb, E<30 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with available data, TALYS nuclear model code calculations.
doi: 10.1007/s10967-015-4528-0
2015SZ04 Nucl.Instrum.Methods Phys.Res. B343, 173 (2015); Erratum Nucl.Instrum.Methods Phys.Res. B447, 113 (2019) F.Szelecsenyi, G.F.Steyn, Z.Kovacs, C.Vermeulen, K.Nagatsu, M.-R.Zhang, K.Suzuki Excitation functions of natZr + p nuclear processes up to 70 MeV: New measurements and compilation NUCLEAR REACTIONS Zr(p, X)89Nb/90Nb/91Nb/92Nb/95Nb/96Nb/86Zr/87Zr/88Zr/89Zr/95Zr/85Y/86Y/87Y/88Y/90Y/91Y/85Sr, E<70 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with TALYS nuclear model code calculations.
doi: 10.1016/j.nimb.2014.11.081
2014ST01 Nucl.Instrum.Methods Phys.Res. B319, 128 (2014) G.F.Steyn, C.Vermeulen, F.Szelecsenyi, Z.Kovacs, A.Hohn, N.P.van der Meulen, R.Schibli, T.N.van der Walt Cross sections of proton-induced reactions on 152Gd, 155Gd and 159Tb with emphasis on the production of selected Tb radionuclides NUCLEAR REACTIONS Cu(p, xn)62Zn, Tb(p, X)153Dy/155Dy/157Dy/159Dy, 152,155Gd(p, 4n), 159Tb(p, 5n), (p, 3n), Tb(p, X)153Tb/154Tb/155Tb/156Tb/151Gd/153Gd, E<70 MeV; measured reaction products, Eγ, Iγ; deduced σ, integral yields. Comparison with ALICE/ASH and TENDL 2012 calculations.
doi: 10.1016/j.nimb.2013.11.013
2014SZ02 Radiochim.Acta 102, 465 (2014) F.Szelecsenyi, Z.Kovacs, K.Nagatsu, M.-R.Zhang, K.Suzuki Excitation function of (p, α) nuclear reaction on enriched 67Zn: possibility of production of 64Cu at low energy cyclotron NUCLEAR REACTIONS 67Zn(p, α), E<30 MeV; measured reaction products, Eγ, Iγ; deduced σ, integral yields. TALYS nuclear model code calculations, comparison with available data.
doi: 10.1515/ract-2013-2145
2012SZ01 Radiochim.Acta 100, 5 (2012) F.Szelecsenyi, Z.Kovacs, K.Nagatsu, K.Fukumura, K.Suzuki, K.Mukai Investigation of direct production of 68Ga with low energy multiparticle accelerator NUCLEAR REACTIONS Cu(α, xn)66Ga/67Ga/68Ga, E<36 MeV; 68Zn(p, xn)67Ga/68Ga, E<20 MeV; measured reaction products, Eγ, Iγ; deduced σ, excitation functions. Comparison with theoretical calculations. NUCLEAR REACTIONS 68Zn(p, n), E, 20 MeV; calculated yields, 66,67Ga contamination.
doi: 10.1524/ract.2011.1896
2012VE02 Nucl.Instrum.Methods Phys.Res. B275, 24 (2012) C.Vermeulen, G.F.Steyn, F.Szelecsenyi, Z.Kovacs, K.Suzuki, K.Nagatsu, T.Fukumura, A.Hohn, T.N.van der Walt Cross sections of proton-induced reactions on natGd with special emphasis on the production possibilities of 152Tb and 155Tb NUCLEAR REACTIONS Gd(p, X)151Tb/152Tb/153Tb/154Tb/155Tb/156Tb/160Tb, E<66 MeV; measured reaction products, Eγ, Iγ; deduced σ, yields. Comparison with ALICE/ASH nuclear model calculations.
doi: 10.1016/j.nimb.2011.12.064
2011SP02 J.Korean Phys.Soc. 59, 1983s (2011) I.Sphan, M.M.Shehata, S.Spellerberg, B.Scholten, H.H.Coenen, S.Q.Qaim, G.F.Steyn, C.Vermeulen, Z.Kovacs, F.Szelecsenyi Investigation of Production Possibilities of Radiobromines for Diagnostic and Therapeutic Applications NUCLEAR REACTIONS 77Se(p, n), (p, 2n), 78Se(p, 2n), (p, 3n)E=21-66 MeV;80Se(p, n)80mBr, E=2.5-18 MeV;80Se(p, 4n), (p, 5n), E=21-85 MeV; measured induced Eγ, Iγ using stacked-foil; deduced σ, 75,76,77,80mBr integral yields. Considered radioisotopic purity of produced medical isotopes.
doi: 10.3938/jkps.59.1983
2011ST26 J.Korean Phys.Soc. 59, 1991s (2011) G.F.Steyn, C.Vermeulen, F.Szelecsenyi, Z.Kovacs, K.Suzuki, T.Fukumura, K.Nagatsu Excitation Functions of Proton Induced Reactions on 89Y and 93Nb with Emphasis on the Production of Selected Radio-Zirconiums NUCLEAR REACTIONS 89Y(p, n), (p, 2n), E=0-70 MeV;93Nb(p, αn), (p, 3n2p), (p, α2n), (p, 4n2p), E=0-70 MeV;93Nb(p, 2np), (p, 3np), E=0-70 MeV; measured off-line Eγ, Iγ using stacked foil; deduced σ. Compared with other data. 89Y(p, n), (p, 2n), 93Nb(p, α2n), (p, 2np), E=10-70 MeV; measured thick target yields.
doi: 10.3938/jkps.59.1991
2010SP05 Radiochim.Acta 98, 749 (2010) I.Spahn, G.F.Steyn, C.Vermeulen, Z.Kovacs, F.Szelecsenyi, M.M.Shehata, S.Spellerberg, B.Scholten, H.H.Coenen, S.M.Qaim New cross section measurements for the production of the Auger electron emitters 77Br and 80mBr NUCLEAR REACTIONS 77,78,80Se(p, n), (p, 2n), (p, 4n)77Br, 80Se(p, n), E=21-85 MeV; measured Eγ, Iγ; deduced σ and their uncertainties, integral yields.
doi: 10.1524/ract.2010.1781
2010SZ03 Nucl.Instrum.Methods Phys.Res. B268, 3306 (2010) F.Szelecsenyi, C.Vermeulen, G.F.Steyn, Z.Kovacs, K.Aardaneh, T.N.van der Walt Excitation functions of 186, 187, 188, 189, 190, 192Ir formed in proton-induced reactions on highly enriched 192Os up to 66 MeV NUCLEAR REACTIONS 192Os(p, n), (p, 3n), (p, 4n), (p, 5n), (p, 6n), Cu(p, n)65Zn, Al(p, X)24Na, Cu(p, X)62Zn E < 66 MeV; measured reaction products, Eγ, Iγ; deduced σ, integral yields. Comparison with model code ALICE/ASH.
doi: 10.1016/j.nimb.2010.07.010
2009EL02 Radiochim.Acta 97, 71 (2009) K.M.El-Azony, K.Suzuki, T.Fukumura, F.Szelecsenyi, Z.Kovacs Excitation functions of proton induced reactions on natural selenium up to 62 MeV NUCLEAR REACTIONS Se(p, X)75Br/76Br/77Br/80Br/82Br/73Se/75Se/71As/72As/76As/77As, E <62 MeV; measured Eγ, Iγ, excitation functions.
doi: 10.1524/ract.2009.1580
2009SP01 Radiochim.Acta 465, 535 (2009) I.Spahn, G.F.Steyn, C.Vermeulen, Z.Kovacs, F.Szelecsenyi, H.H.Coenen, S.M.Qaim New cross section measurements for production of the positron emitters 75Br and 76Br via intermediate energy proton induced reactions NUCLEAR REACTIONS 77,78,80Se(p, xn)75Br/76Br, E<85 MeV; measured Eγ, Iγ; deduced σ, yields. Comparison with ALICE-IPPE code.
doi: 10.1524/ract.2009.1636
2009SZ01 Nucl.Instrum.Methods Phys.Res. B267, 1877 (2009) F.Szelecsenyi, G.F.Steyn, S.G.Dolley, Z.Kovacs, C.Vermeulen, T.N.van der Walt Investigation of the 68Zn(p, 2p)67Cu nuclear reaction: New measurements up to 40 MeV and compilation up to 100 MeV NUCLEAR REACTIONS 68Zn(p, 2p), E=19.2-39.7 MeV; Measured σ; compiled and evaluated earlier measurements.
doi: 10.1016/j.nimb.2009.03.097
2009SZ03 J.Radioanal.Nucl.Chem. 282, 261 (2009) F.Szelecsenyi, G.F.Steyn, Z.Kovacs, K.Aardaneh, C.Vermeulen, T.N.van der Walt Production possibility of 186Re via the 192Os(p, α3n)186Re NUCLEAR REACTIONS 192Os(p, α3n), 186W(p, n), (d, 2n), Cu(p, X)65Zn, Al(p, X)24Na, E<66.7 MeV; measured reaction products, Eγ, Iγ; deduced σ, uncertainties.
doi: 10.1007/s10967-009-0147-y
2009VA05 Appl.Radiat.Isot. 67, 1320 (2009) N.P.van der Meulen, T.N.van der Walt, G.F.Steyn, F.Szelecsenyi, Z.Kovacs, C.M.Perrang, H.G.Raubenheimer The production of 88Y in the proton bombardment of natSr: New excitation and separation studies NUCLEAR REACTIONS 88Sr(p, n), Cu(p, x), E=5-20 MeV; 65Zn; Measured σ. SrCl2 target. Ion exchange chromatographic methods.
doi: 10.1016/j.apradiso.2009.02.058
2008NA03 Nucl.Instrum.Methods Phys.Res. B266, 709 (2008) K.Nagatsu, T.Fukumura, M.Takei, F.Szelecsenyi, Z.Kovacs, K.Suzuki Measurement of thick target yields of the natS(α, x)34mCl nuclear reaction and estimation of its excitation function up to 70 MeV NUCLEAR REACTIONS S(α, X)34Cl, E=14.2-69.5 MeV; measured Eγ, Iγ, thick target saturation yield. S(α, X)34Cl, E=14.2-69.5 MeV; Deduced excitation function.
doi: 10.1016/j.nimb.2008.01.019
2007VE02 Nucl.Instrum.Methods Phys.Res. B255, 331 (2007) C.Vermeulen, G.F.Steyn, F.M.Nortier, F.Szelecsenyi, Z.Kovacs, S.M.Qaim Production of 139Ce by proton-induced reactions on 141Pr and natLa NUCLEAR REACTIONS 141Pr(p, X)132Ce/133mCe/135Ce/137mCe/139Ce, E ≈ 21-97 MeV; La(p, X)139Ce, E ≈ 4-11 MeV; measured production σ; deduced thick-target yields.
doi: 10.1016/j.nimb.2006.12.145
2006KI15 J.Radioanal.Nucl.Chem. 270, 369 (2006) B.Kiraly, F.Tarkanyi, S.Takacs, Z.Kovacs Excitation functions of proton induced nuclear reactions on natural tellurium up to 18 MeV for validation of isotopic cross sections NUCLEAR REACTIONS Te(p, xn)121I/123I/124I/126I/128I/130I, E=2-18 MeV; Te(p, X)121Te, E=13-18 MeV; measured production σ. Stacked foil activation technique.
doi: 10.1007/s10967-006-0359-3
2006ST20 Nucl.Instrum.Methods Phys.Res. B252, 149 (2006) G.F.Steyn, C.Vermeulen, F.M.Nortier, F.Szelecsenyi, Z.Kovacs, S.M.Qaim Production of no-carrier-added 139Pr via precursor decay in the proton bombardment of natPr NUCLEAR REACTIONS Pr(p, X)135Nd/136Nd/137Nd/138Nd/139Nd/139mNd/141Nd/136Pr/137Pr/138mPr, E ≈ 7-97 MeV; measured production σ. Stacked-foil activation technique.
doi: 10.1016/j.nimb.2006.08.012
2006SZ03 Appl.Radiat.Isot. 64, 789 (2006) F.Szelecsenyi, G.F.Steyn, Z.Kovacs, T.N.van der Walt, K.Suzuki Comments on the feasibility of 61Cu production by proton irradiation of natZn on a medical cyclotron NUCLEAR REACTIONS Zn(p, X)60Cu/61Cu/64Cu, E=7-30 MeV; analyzed σ. Feasibility of large-scale production discussed.
doi: 10.1016/j.apradiso.2006.01.011
2005SZ02 Nucl.Instrum.Methods Phys.Res. B234, 375 (2005) F.Szelecsenyi, G.F.Steyn, Z.Kovacs, T.N.van der Walt, K.Suzuki, K.Okada, K.Mukai New cross-section data for the 66Zn(p, n)66Ga, 68Zn(p, 3n)66Ga, natZn(p, x)66Ga, 68Zn(p, 2n)67Ga and natZn(p, x)67Ga nuclear reactions up to 100 Mev NUCLEAR REACTIONS 66Zn(p, n), 68Zn(p, 2n), (p, 3n), E ≈ 5-100 MeV; Zn(p, X)66Ga/67Ga, E ≈ 5-100 MeV; measured production σ. Stacked-foil activation, comparison with previous results.
doi: 10.1016/j.nimb.2005.02.011
2005SZ04 Nucl.Instrum.Methods Phys.Res. B240, 625 (2005) F.Szelecsenyi, G.F.Steyn, Z.Kovacs, C.Vermeulen, N.P.van der Meulen, S.G.Dolley, T.N.van der Walt, K.Suzuki, K.Mukai Investigation of the 66Zn(p, 2pn)64Cu and 68Zn(p, x)64Cu nuclear processes up to 100 MeV: Production of 64Cu NUCLEAR REACTIONS Zn, 68Zn(p, X)64Cu, E ≈ 18-100 MeV; 66Zn(p, n2p), E ≈ 35-100 MeV; measured production σ. Stacked-foil activation technique.
doi: 10.1016/j.nimb.2005.05.057
2004SZ06 Nucl.Instrum.Methods Phys.Res. B222, 364 (2004) F.Szelecsenyi, Z.Kovacs, K.Suzuki, K.Okada, T.Fukumura, K.Mukai Formation of 60Cu and 61Cu via Co + 3He reactions up to 70 MeV: production possibility of 60Cu for PET studies NUCLEAR REACTIONS 59Co(3He, n), (3He, 2n), E=4-70 MeV; measured excitation functions. Stacked-foil activation, comparison with previous results.
doi: 10.1016/j.nimb.2004.03.013
2003KO72 Radiochim.Acta 91, 185 (2003) Z.Kovacs, B.Scholten, F.Tarkanyi, H.H.Coenen, S.M.Qaim Cross section measurements using gas and solid targets for production of the positron-emitting radionuclide O-14 NUCLEAR REACTIONS 14N(p, n), (p, α), (p, d), E ≈ 6-19 MeV; measured excitation functions; deduced integral yields.
doi: 10.1524/ract.91.4.185.19970
2003SZ01 Appl.Radiat.Isot. 58, 377 (2003) F.Szelecsenyi, Z.Kovacs, T.N.van der Walt, G.F.Steyn, K.Suzuki, K.Okada Investigation of the natZn(p, x)62Zn nuclear process up to 70MeV: a new 62Zn/62Cu generator NUCLEAR REACTIONS Zn(p, X)62Zn/66Ga, E ≈ 24-70 MeV; 66Zn(p, n), (p, 4np), E ≈ 35-67 MeV; measured production σ; deduced thick-target yields. Stacked-foil activation technique.
doi: 10.1016/S0969-8043(02)00345-7
2002SZ01 Nucl.Instrum.Methods Phys.Res. B187, 153 (2002) F.Szelecsenyi, K.Suzuki, Z.Kovacs, M.Takei, K.Okada Production Possibility of 60, 61, 62Cu Radioisotopes by Alpha Induced Reactions on Cobalt for PET Studies NUCLEAR REACTIONS 59Co(α, n), (α, 2n), (α, 3n), E=18-58 MeV; measured production σ; deduced thick target yields. Stacked-foil activation technique, comparison with previous results and model predictions.
doi: 10.1016/S0168-583X(01)00923-5
2001SZ06 Nucl.Instrum.Methods Phys.Res. B184, 589 (2001) F.Szelecsenyi, K.Suzuki, Z.Kovacs, M.Takei, K.Okada Alpha Beam Monitoring via natCu + Alpha Processes in the Energy Range from 40 to 60 MeV NUCLEAR REACTIONS Cu(α, X)61Cu/66Ga/67Ga, E=16-60 MeV; measured production σ. Stacked-foil activation technique, comparison with previous results.
doi: 10.1016/S0168-583X(01)00793-5
1999TA04 Appl.Radiat.Isot. 50, 535 (1999) S.Takacs, A.Azzam, M.Sonck, F.Szelecsenyi, Z.Kovacs, A.Hermanne, F.Tarkanyi Excitation Function of 122Te(d, n)123I Nuclear Reaction: Production of 123I at a low energy cyclotron NUCLEAR REACTIONS 122Te(d, n), E=4.7-21.1 MeV; measured σ; deduced excitation function, integral yield. Stacked-foil activation.
doi: 10.1016/S0969-8043(98)00059-1
1997SC02 Appl.Radiat.Isot. 48, 267 (1997) B.Scholten, S.Takacs, Z.Kovacs, F.Tarkanyi, S.M.Qaim Excitation Functions of Deuteron Induced Reactions on 123Te: Relevance to the production of 123I and 124I at low and medium sized cyclotrons NUCLEAR REACTIONS, ICPND 123Te(d, n), (d, 2n), E=threshold 12.5 MeV; measured residuals production σ(E); deduced yields. Stacked-foil technique.
doi: 10.1016/S0969-8043(96)00149-2
1996TA32 Nucl.Instrum.Methods Phys.Res. B 113, 424 (1996) S.Takacs, F.Tarkanyi, Z.Kovacs Excitation function of alpha-particle induced nuclear reactions on natural nickel NUCLEAR REACTIONS Ni(α, x), E=2.3-24.4 MeV; measured products, 62Zn, 61Cu, 67Cu, 57Ni, 57Co, 65Zn, 63Zn, 60Cu; deduced σ, σ(E). Data were imported from EXFOR entry D4050.
doi: 10.1016/0168-583X(95)01349-0
1995SC19 Appl.Radiat.Isot. 46, 255 (1995) B.Scholten, Z.Kovacs, F.Tarkanyi, S.M.Qaim Excitation Functions of 124Te(p, xn)124,123I Reactions from 6 to 31 MeV with Special Reference to the Production of 124I at a Small Cyclotron NUCLEAR REACTIONS, ICPND 124Te(p, 2n), (p, n), E=6-31 MeV; measured residuals production σ(E). Stacked foils, activation technique.
doi: 10.1016/0969-8043(94)00145-P
1993TA15 Appl.Radiat.Isot. 44, 1105 (1993) F.Tarkanyi, Z.Kovacs, S.M.Qaim Excitation Functions of Proton Induced Nuclear Reactions on Highly Enriched 78Kr: Relevance to the Production of 75Br and 77Br at a Small Cyclotron NUCLEAR REACTIONS, ICPND 78Kr(p, np), (p, α), (p, 2p), E=threshold-19.62 MeV; measured residual production σ(E), thick target yields. Activation technique.
doi: 10.1016/0969-8043(93)90114-P
1992TA07 Appl.Radiat.Isot. 43, 503 (1992) F.Tarkanyi, Z.Kovacs, S.M.Qaim, G.Stocklin Production of 38K via the 38Ar(p, n)-Process at a Small Cyclotron NUCLEAR REACTIONS, ICPND 38Ar(p, n), E ≈ 7-18 MeV; measured σ(E). Calculated differential, integral yields. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4006. 1991KO06 Appl.Radiat.Isot. 42, 329 (1991) Z.Kovacs, F.Tarkanyi, S.M.Qaim, G.Stocklin Excitation Functions for the Formation of Some Radioisotopes of Rubidium in Proton Induced Nuclear Reactions on (nat)Kr, 82Kr and 83Kr with Special Reference to the Production of 81Rb(81mKr) Generator Radionuclide NUCLEAR REACTIONS, ICPND Kr(p, xn)82Rb/82mRb/81Rb/83Rb/84Rb, E=5-30 MeV; 84,82,83Kr(p, n), 83,84,82Kr(p, 2n), 83,84,86Kr(p, 3n), E=5-30 MeV; measured residuals production σ(E). Stacked gas cell technique. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0489. 1991KO24 Appl.Radiat.Isot. 42, 831 (1991) Z.Kovacs, F.Tarkanyi, S.M.Qaim, G.Stocklin Production of 6.5h 82mRb via the 82Kr(p, n)-Process at a Low-Energy Cyclotron - a Potential Substitute for 82Rb NUCLEAR REACTIONS, ICPND 82Kr(p, n)82Rb/82mRb, 82Kr(p, 2n), (p, 3n), (p, xn), E=threshold-30 MeV; calculated differential, integral thick target yields. Radiation dose calculations. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4009. 1991SZ04 J.Labelled Compd.Radiopharm. 30, 98 (1991) F.Szelecsenyi, Z.Kovacs, F.Tarkanyi, Gy.Toth Production of 110In for PET Investigation via Cd(3He, xn)110Sn-110In Reaction with Low Energy Cyclotron NUCLEAR REACTIONS, ICPND Cd(3He, xn)110Sn, E ≈ 16-27 MeV; measured residual production σ(E). Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4010. 1991TA24 Radiochim.Acta 54, 165 (1991) F.Tarkanyi, Z.Kovacs, I.Mahunka, O.Solin, J.Bergman Excitation Function of the 35Cl(α, n)38K Reaction Using Gas Targets NUCLEAR REACTIONS, ICPND 35Cl(α, n), E ≈ 8-16 MeV; measured σ(E). Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4007. 1990AL06 Phys.Lett. 237B, 29 (1990) N.P.Aleshin, S.L.Belostotsky, Yu.V.Dotsenko, O.G.Grebenyuk, L.M.Kochenda, L.G.Kudin, N.P.Kuropatkin, S.I.Manayenkov, O.V.Miklukho, V.N.Nikulin, O.E.Prokofev, A.Yu.Tsaregorotsev, S.S.Volkov, J.Ero, J.Kecskemeti, P.Koncz, Zs.Kovacs, Z.Seres Study of the Proton-Deuteron Break-Up Reaction in Complete Kinematics at 1 GeV NUCLEAR REACTIONS 2H(p, np), E=1 GeV; measured σ(θp, θp1) vs proton momentum, recoil proton polarization. Kinematically complete experiment. Impulse approximation.
doi: 10.1016/0370-2693(90)90455-F
1990BU23 Nucl.Phys. A515, 541 (1990) R.Buchle, J.Franz, P.Koncz, M.Marx, E.Rossle, C.Sauerwein, H.Schmitt, K.Schmoll, J.Ero, Z.Fodor, J.Kecskemeti, Zs.Kovacs, Z.Seres Neutron-Induced Pion Production on Carbon, Copper and Bismuth at Intermediate Energies NUCLEAR REACTIONS C, Cu, 209Bi(n, π), E=300-580 MeV; measured pion production σ(E, θ) vs particle energy.
doi: 10.1016/0375-9474(90)90272-N
1990FR05 Nucl.Phys. A510, 774 (1990) J.Franz, P.Koncz, E.Rossle, C.Sauerwein, H.Schmitt, K.Schmoll, J.Ero, Z.Fodor, J.Kecskemeti, Zs.Kovacs, Z.Seres Neutron-Induced Production of Protons, Deuterons and Tritons on Copper and Bismuth NUCLEAR REACTIONS Cu, 209Bi(n, p), (n, d), (n, t), E=300-580 MeV; measured light-particle production σ(E, θ) versus particle energy.
doi: 10.1016/0375-9474(90)90360-X
1990TA20 Radiochim.Acta 50, 19 (1990) F.Tarkanyi, F.Szelecsenyi, Z.Kovacs, S.Sudar Excitation Functions of Proton Induced Nuclear Reactions on Enriched 66Zn, 67Zn and 68Zn Production of 67Ga and 66Ga NUCLEAR REACTIONS, ICPND 66,67,68Zn(p, n), 67,68Zn(p, 2n), 66Zn(p, n), E=6-22 MeV; measured residuals production σ(E); calculated thick target yields. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4004. 1989TA18 Radiochim.Acta 47, 25 (1989) F.Tarkanyi, Z.Kovacs, S.M.Qaim, G.Stocklin Differential Production Yields of 123I in Proton and Deuteron Induced Reactions on Natural Xenon NUCLEAR REACTIONS, ICPND Xe(p, xn), (p, xnp), (p, xnα)123I, E=17-43 MeV; Xe(d, xn), (d, xnp), (d, xnα)123I, E=22-53 MeV; measured product differential yields vs E. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4035. 1988BU16 Phys.Lett. 213B, 125 (1988) R.Buchle, J.Franz, P.Koncz, M.Marx, E.Rossle, C.Sauerwein, H.Schmitt, J.Ero, Z.Fodor, J.Kecskemeti, Zs.Kovacs, Z.Seres Pion Production on Carbon by Medium Energy Neutrons NUCLEAR REACTIONS C(n, π+), (n, π-), E=300-580 MeV; measured pion production σ(θ) vs E.
doi: 10.1016/0370-2693(88)91011-8
1987FR16 Nucl.Phys. A472, 733 (1987) J.Franz, E.Rossle, C.Sauerwein, H.Schmitt, H.L.Woolverton, J.Ero, Z.Fodor, J.Kecskemeti, P.Koncz, Zs.Kovacs, Z.Seres Production of Protons, Deuterons and Tritons on Carbon by Intermediate Energy Neutrons NUCLEAR REACTIONS C(n, p), (n, d), (n, t), E=300-580 MeV; measured light particle production σ(E, θ) vs particle energy.
doi: 10.1016/0375-9474(87)90053-4
1986ER02 Acta Phys.Acad.Sci.Hung. 59, 401 (1986) J.Ero, Z.Fodor, J.Kecskemeti, P.Koncz, Zs.Kovacs, Z.Seres, S.L.Belostotsky, V.N.Nikulin Inclusive Backward Proton and Deuteron Production from 40,44,48Ca Isotopes by 1 GeV Protons NUCLEAR REACTIONS 40,44,48Ca(p, pX), (p, dX), E=1 GeV; measured inclusive σ(θp, Ep), σ(θd, Ed); deduced target dependence.
1986KO26 J.Phys.(London) G12, 1355 (1986) Hadron and Fragment Emission in Cluster-Excitation Processes at Medium Energies NUCLEAR REACTIONS 12C(n, π), (n, p), (n, d), (n, t), E=545 MeV; calculated decay probability distributions, σ(E(π+), θ), σ(Ep, θ), σ(Et, θ), σ(Ed, θ). Cluster excitation model.
doi: 10.1088/0305-4616/12/12/014
1985FR07 Phys.Lett. 153B, 382 (1985) J.Franz, E.Rossle, C.Sauerwein, H.Schmitt, H.L.Woolverton, J.Ero, Z.Fodor, J.Kecskemeti, P.Koncz, Zs.Kovacs, Z.Seres Charged Particle Production on 12C By Intermediate Energy Neutrons NUCLEAR REACTIONS 12C(n, p), (n, d), (n, t), E=545 MeV; measured σ(θ, Ep), σ(θ, Ed), σ(θ, Et).
doi: 10.1016/0370-2693(85)90477-0
1985KO25 Int.J.Appl.Radiat.Isotop. 36, 635 (1985) Z.Kovacs, G.Blessing, S.M.Qaim, G.Stocklin Production of 75Br via the 76Se(p, 2n)75Br Reaction at a Compact Cyclotron NUCLEAR REACTIONS, ICPND 76Se(p, n), E ≈ 7-40 MeV; 76Se(p, 2n), E ≈ 15.5-40 MeV; 76Se(p, 3n), E ≈ 32-40 MeV; 76Se(p, α), E=10-40 MeV; 76Se(p, nα), E=20-40 MeV; 76Se(p, 2nα), E=30-40 MeV; 76Se(p, np), E=13-40 MeV; measured reaction σ(E). 76Se(p, 3He), (p, n2p), (p, pd), E ≈ 29-40 MeV; measured summed reaction σ(E). 76Se(p, xn)76Br/75Br/74mBr, E=threshold-40 MeV; calculated cumulative thick target yield vs E. Activation technique.
doi: 10.1016/0020-708X(85)90004-3
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