NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = O.Artun Found 15 matches. 2022AR01 Nucl.Instrum.Methods Phys.Res. B512, 12 (2022) The investigation of the production of Ac-227, Ra-228, Th-228, and U-232 in thorium by particle accelerators for use in radioisotope power systems and nuclear batteries NUCLEAR REACTIONS 232Th(p, X), (d, X), (t, X), (3He, X), (α, X)227Ac/228Ra/228Th/232U, E<350 MeV; calculated σ, integral yields. Comparison with the EXFOR database, TALYS calculations.
doi: 10.1016/j.nimb.2021.12.004
2022AR05 Appl.Radiat.Isot. 185, 110222 (2022) A new production route of Gadolinium-148 for use in Radioisotope Thermoelectric Generators NUCLEAR REACTIONS Sm, Eu(α, X), (3He, X), (d, X), (t, X)148Gd, E<100 MeV; calculated production yields, σ using TALYS nuclear model code. Comparison with available data.
doi: 10.1016/j.apradiso.2022.110222
2021AR13 Phys.Atomic Nuclei 84, 837 (2021) Neutron Structure Properties of Titanium in a Supernova NUCLEAR STRUCTURE 44Ti; calculated average neutron-proton interactions, neutron skin thickness, bubble structure, single-particle energy levels, charge form factor using the Skyrme-Hartree-Fock approach.
doi: 10.1134/S106377882106003X
2020AR06 Turk.J.Phys. 44, 256 (2020) Investigation of some nuclear structure properties of 213Bi, 201Tl, 188Re, 186Re, 133Xe, 131I, 125I, 123I, 111In, 94Tc, 90Y, 67Ga, 67Cu, 62Cu, 61Cu, 55Co, and 48V nuclei used in SPECT in axial deformation NUCLEAR STRUCTURE 213Bi, 201Tl, 188Re, 186Re, 133Xe, 131I, 125,123I, 111In, 94Tc, 90Y, 67Ga, 67,62,61Cu, 55Co, 48V; analyzed available data; calculated neutron skin thicknesses, the proton, neutron quadrupole moments, quadrupole deformation parameter, the proton and neutron pairing energies using Skyrme and Gogny interactions.
doi: 10.3906/fiz-2001-3
2020AR12 Int.J.Mod.Phys. E29, 2050059 (2020) Production calculation of medical 67Ga, 111In, 117mSn, 131, 125, 123I, 133Xe, 153Sm, 159Gd, 188Re and 201Tl nuclei used for cancer diagnostics in single photon emission computed tomography via theoretical models NUCLEAR REACTIONS 67Zn(p, n), 66Zn, 122Te(d, n), 65Cu(α, 2n), 112Sn(n, X)111In, 111Cd, 123Te(p, n), 118Sn(n, 2n), 114Cd(α, n), 116Cd(α, 3n), 123Sb(α, 4n), 125Te(p, n), 123Sb(α, 2n), 131Xe(n, p), 133Cs(d, 2p), 160Gd(n, 2n), 162Dy(n, α), 188Os(n, p), 187Re(d, p), 186W(α, X)188Re, E<100 MeV; calculated σ, yields. Comparison with available data.
doi: 10.1142/S0218301320500597
2020AR14 Appl.Radiat.Isot. 166, 109337 (2020) Production of energetic 232U, 236, 238Pu, 242Cm, 248Bk, 250, 252Cf and 252Es radioisotopes for use as nuclear battery in thin targets via particle accelerators NUCLEAR REACTIONS 231Pa(p, γ), (d, n), (t, 2n), (3He, X), (α, X), 233U(α, n), 235U(3He, 2n), (α, 3n), 237Np(p, 2n), (d, 3n), (t, 4n), (3He, X), (α, X), 238U(3He, 7n), (t, 3n), (p, n), (d, 2n), (3He, X), (α, X), 239Pu(α, n), 241Am(p, γ), (d, n), (t, 2n), (3He, X), (α, X), 245Cm(α, p), 246Cm(α, d), (3He, p), (t, n), 247Cm(p, γ), (d, n), (t, 2n), (3He, d), (α, t), 248Cm(p, n), (d, 2n), (t, 3n), (3He, t), (α, X), 248Cm(p, n), (d, 2n), (t, 3n), (3He, t), (α, X), 250Cm(p, 3n), (d, 4n), (t, 5n), (3He, X), (α, X), 247Bk(d, p), (t, d), (α, X), 249Bk(p, d), (d, t), (t, X), (3He, X), (α, X), 249Cf(d, α), 250Cf(p, 3He), (d, α), (t, X), (p, X), (d, X), 252Cf(p, X), (d, X), (t, X)248Bk, E=15-61 MeV; measured reaction products. 232U, 236,238Pu, 238Np, 242Cm, 248Bk, 250,252Cf, 252Es; deduced yields, σ. Comparison with calculations, EXFOR library.
doi: 10.1016/j.apradiso.2020.109337
2020AR17 Int.J.Mod.Phys. E29, 2050079 (2020) Nuclear structure properties in neutron stars NUCLEAR STRUCTURE N=88-184; calculated charge, proton and neutron density distributions along with nuclear properties using Hartree-Fock approach with Skyrme force interaction. Comparison with available data.
doi: 10.1142/S0218301320500792
2019AR01 Appl.Radiat.Isot. 144, 64 (2019) Calculation of productions of medical 201Pb, 198Au, 186Re, 111Ag, 103Pd, 90Y, 89Sr, 77Kr, 77As, 67Cu, 64Cu, 47Sc and 32P nuclei used in cancer therapy via phenomenological and microscopic level density models NUCLEAR REACTIONS 32S(n, p), 48Ti(p, 2p), 64Ni(d, 2n), (p, n), 64Zn(n, p), 68Zn(p, 2p), 70Zn(p, α), 67Zn(n, p), 80Se(p, α), 79Br(p, 3n), 89Y(n, p), 90Zr(n, p), 103Rh(d, 2n), (p, n), 110Pd(d, n), 186W(d, 2n), 186W(p, n), 198Pt(d, 2n), (p, n), 203Tl(p, 3n), E<100 MeV; calculated yields, σ using TALYS 1.9 and EMPIRE 3.2 nuclear model codes. Comparison with experimental data.
doi: 10.1016/j.apradiso.2018.11.011
2019AR10 Int.J.Mod.Phys. E28, 1950057 (2019) The (n, γ) reaction productions of 35S, 42Ar, 45Ca, 63Ni, 85Kr, 89Sr, 113mCd, 121m, 123Sn, 147Pm, 151Sm, 152, 154, 155Eu, 170, 171Tm, 185, 188W, 194Os, 204Tl, 210Po, 227Ac, 242, 244Cm radioisotopes for using in nuclear battery via phenomenological and microscopic level density models NUCLEAR REACTIONS 34S, 40Ar, 44Ca, 62Ni, 84Kr, 88Sr, 112Cd, 120,122Sn, 146Nd, 150Sm, 151,153Eu, 154Sm, 169Tm, 170Er, 184,186W, 192Os, 203Tl, 209Bi, 226Ra, 243Cm(n, γ), E<1 MeV; calculated σ.
doi: 10.1142/S0218301319500575
2018AR04 Int.J.Mod.Phys. E27, 1850070 (2018) A study of nuclear structure properties of even and odd 103-140Sb, 105-143Te, 107-145I, 109-148Xe and 112-151Cs nuclei in the axial deformation NUCLEAR STRUCTURE 103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140Sb, 105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143Te, 107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145I, 109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148Xe, 112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151Cs; calculated binding energies, charge, proton, and neutron density radii, one-neutron and two-neutron separation energies, quadrupole deformation parameter and moment, neutron skin thickness, pairing gap energy. Comparison with available data.
doi: 10.1142/S0218301318500702
2017AR08 Appl.Radiat.Isot. 127, 166 (2017) Estimation of the production of medical Ac-225 on thorium material via proton accelerator NUCLEAR REACTIONS 232Th(p, X)229Pa/225Ra/229Th/225Ac, E<1 GeV; calculated production σ, simulated activities of reactions as a function of irradiation time using Fermi-gas model with constant temperature (CTM) by choosing the best input parameters. Comparison with available data.
doi: 10.1016/j.apradiso.2017.06.006
2017AR15 Turk.J.Phys. 41, 295 (2017) Investigation of excitation functions of proton-induced reactions on 94, 96, 98, 100Mo targets for production of radioisotopes 94m, 94g, 96m, 96g, 96, 99mTc NUCLEAR REACTIONS 94,96,98,100Mo(p, X)94Tc/96Tc/99Tc, E<50 MeV; calculated σ. TALYS nuclear model code, comparison with experimental data.
doi: 10.3906/fiz-1612-2
2015AR03 Nucl.Instrum.Methods Phys.Res. B345, 1 (2015) Calculation of excitation functions of proton, alpha and deuteron induced reactions for production of medical radioisotopes 122-125I NUCLEAR REACTIONS 123Te(p, 2n), (d, 2n), (p, n), (d, n), 122Te(p, n), (d, 2n), 125Te(p, 4n), (p, 3n), (p, 2n), 126Te(p, 4n), (p, 3n), (p, 2n), 121Sb(α, 2n), (α, n), 123Sb(α, 4n), (α, 3n), (α, 2n), 124Te(d, 3n), (p, 2n), (d, 2n), (p, n), (d, n), E<70 MeV; calculated σ. TALYS 1.6 nuclear model code, comparison with experimental data.
doi: 10.1016/j.nimb.2014.12.029
2013AY06 J.Radioanal.Nucl.Chem. 298, 95 (2013) Cross-section calculations of proton induced (p, n) and (p, 2n) reactions for production of diagnostic 67Ga, 81Rb, 111In, 123, 124I, 123Cs and 123Xe radioisotopes NUCLEAR REACTIONS 67Zn, 111Cd, 123,124Te(p, n), 68Zn, 82Kr, 112Cd, 124Te, 124Xe(p, 2n), E<40 MeV; calculated σ. ALICE/ASH and TALYS nuclear model codes, comparison with available data.
doi: 10.1007/s10967-013-2478-y
1975AR17 Phys.Rev.Lett. 35, 773 (1975) O.Artun, Y.Cassagnou, R.Legrain, N.Lisbona, L.Roussel, J.P.Alard, A.Baldit, J.P.Costilhes, J.Fargeix, G.Roche, J.C.Tamain Multinucleon Removal Induced by High-Energy Protons NUCLEAR REACTIONS N, O, P, S, V(p, X), E=230 MeV; Al, Si, Ca, Fe(p, X), E < 1 GeV; measured σ(fragment mass).
doi: 10.1103/PhysRevLett.35.773
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