NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = A.Koning Found 137 matches. Showing 1 to 100. [Next]2024SC02 Nucl.Data Sheets 193, 1 (2024) G.Schnabel, D.L.Aldama, T.Bohm, U.Fischer, S.Kunieda, A.Trkov, C.Konno, R.Capote, A.J.Koning, S.Breidokaite, T.Eade, M.Fabbri, D.Flammini, L.Isolan, I.Kodeli, M.Kostal, S.Kwon, D.Laghi, D.Leichtle, S.Nakayama, M.Ohta, L.W.Packer, Y.Qiu, S.Sato, M.Sawan, M.Schulc, G.Stankunas, M.Sumini, A.Valentine, R.Villari, A.Zohar FENDL: A library for fusion research and applications NUCLEAR REACTIONS 1,2,3H, 3,4He, 6,7Li, 9Be, 10,11B, 12,13C, 14,15N, 16,17,18O, 19F, 20,21,22Ne, 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34S, 36S, 35,37Cl, 36,38,40Ar, 39,40,41K, 40Ca, 42,43,44Ca, 46,48Ca, 45Sc, 46,47,48,49,50Ti, 50,51V, 50Cr, 52,53,54Cr, 55Mn, 54Fe, 56,57,58Fe, 59Co, 58Ni, 60,61,62Ni, 64Ni, 63,65Cu, 64Zn, 66,67,68Zn, 70Zn, 69,71Ga, 70Ge, 72,73,74Ge, 76Ge, 79,81Br, 89Y, 90,91,92,93,94Zr, 96Zr, 93Nb, 92Mo, 94,95,96,97,98Mo, 100Mo, 103Rh, 107,109Ag, 106,108,110Cd, 111,112,113,114Cd, 116Cd, 112Sn, 114,115,116,117,118,119,120Sn, 122,124Sn, 121,123Sb, 127I, 133Cs, 130,132,134Ba, 135,136,137,138Ba, 138,139La, 136,138,140,142Ce, 144Sm, 147,148,149,150Sm, 154Sm, 152Gd, 154,155,156,157,158Gd, 160Gd, 162,164,166,168,170Er, 167Er, 175,176Lu, 174,176,178,180Hf, 177,179Hf, 180,181Ta, 182,184,186W, 183W, 185,187Re, 190,192,194,196,198Pt, 195Pt, 197Au, 204,206,208Pb, 207Pb, 209Bi, 232Th, 234,235U, 238U(n, X), 1,2,3H, 3He, 6,7Li, 9Be, 10,11B, 12,13C, 14,15N, 16,17,18O, 19F, 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34S, 36S, 35,37Cl, 36,38,40Ar, 39,40,41K, 40Ca, 42,43,44Ca, 46,48Ca, 45Sc, 46,47,48,49,50Ti, 50,51V, 50Cr, 52,53,54Cr, 55Mn, 54Fe, 58Fe, 59Co, 58Ni, 60,61,62Ni, 64Ni, 63,65Cu, 64Zn, 66,67,68Zn, 70Zn, 69,71Ga, 70Ge, 72,73,74Ge, 76Ge, 79,81Br, 89Y, 90,91,92,93,94Zr, 96Zr, 93Nb, 92Mo, 94,95,96,97,98Mo, 100Mo, 103Rh, 107,109Ag, 106,108Cd, 110,111,112,113,114Cd, 116Cd, 112Sn, 114,115,116,117,118,119,120Sn, 122,124Sn, 121,123Sb, 127I, 133Cs, 130,132,134,136,138Ba, 135,137Ba, 138,139La, 136,138,140,142Ce, 152,153,154,155,156,157,158,159,160Gd, 155,157Gd, 162,164,166,168,170Er, 167Er, 175,176Lu, 174,176,178,180Hf, 177,178,179Hf, 181Ta, 180,182,184,186W, 183W, 185,187Re, 190,192,194,196,198Pt, 195Pt, 197Au, 204,206,208Pb, 207Pb, 209Bi, 232Th, 235U, 238U(p, X), E<3000 MeV; analyzed ENDF/B-VII.0, ENDF/B-VII.1, ENDF/B-VIII.0, INDEN-1.0, JENDL-4, JENDL/HE-2007, JEFF-3.1.1, FENDL-3.2 , TENDL-2010, TENDL-2011, TENDL-2014, TENDL-2015, TENDL-2019 libraries data; deduced recommended σ data coordinated by the International Atomic Energy Agency (IAEA) Nuclear Data Section (NDS).
doi: 10.1016/j.nds.2024.01.001
2023AL11 Appl.Radiat.Isot. 198, 110832 (2023) E.Alhassan, D.Rochman, A.Vasiliev, A.J.Koning, H.Ferroukhi TENDL-based evaluation and adjustment of p+111Cd between 1 and 100 MeV NUCLEAR REACTIONS 111Cd(p, n), (p, 2n), (p, 3n), (p, 4n), E=1-100 MeV; calculated σ using TALYS. Comparison with available data.
doi: 10.1016/j.apradiso.2023.110832
2023CA21 Eur.Phys.J. A 59, 295 (2023) S.Cannarozzo, S.Pomp, A.Solders, A.Al-Adili, A.Gook, A.Koning Global comparison between experimentally measured isomeric yield ratios and nuclear model calculations
doi: 10.1140/epja/s10050-023-01202-5
2023FU03 Eur.Phys.J. A 59, 178 (2023) K.Fujio, A.Al-Adili, F.Nordstrom, J.-F.Lemaitre, S.Okumura, S.Chiba, A.Koning TALYS calculations of prompt fission observables and independent fission product yields for the neutron-induced fission of 235U NUCLEAR REACTIONS 235U(n, F), E<20 MeV; calculated prompt neutron and γ-ray multiplicities, PFNS, independent fission product yields. Comparison with available data.
doi: 10.1140/epja/s10050-023-01095-4
2023KO14 Eur.Phys.J. A 59, 131 (2023), Erratum Eur.Phys.J. A 59, 146 (2023) A.Koning, S.Hilaire, S.Goriely TALYS: modeling of nuclear reactions
doi: 10.1140/epja/s10050-023-01034-3
2023NE10 Eur.Phys.J. N 9, 35 (2023) D.Neudecker, A.M.Lewis, E.F.Matthews, J.Vanhoy, R.C.Haight, D.L.Smith, P.Talou, S.Croft, A.D.Carlson, B.Pierson, A.Wallner, A.Al-Adili, L.Bernstein, R.Capote, M.Devlin, M.Drosg, D.L.Duke, S.Finch, M.W.Herman, K.J.Kelly, A.Koning, A.E.Lovell, P.Marini, K.Montoya, G.P.A.Nobre, M.Paris, B.Pritychenko, H.Sjostrand, L.Snyder, V.Sobes, A.Solders, J.Taieb Templates of Expected Measurement Uncertainties: a CSEWG Effort NUCLEAR REACTIONS 235U(n, F), E<20 MeV; analyzed available data; deduced nubar mean values and uncertainties.
doi: 10.1051/epjn/2023014
2023RO07 At.Data Nucl.Data Tables 153, 101583 (2023) A.Rodrigo, N.Otuka, S.Takacs, A.J.Koning Compilation of isomeric ratios of light particle induced nuclear reactions COMPILATION Z=36-94; compiled experimental isomeric ratios of light (A<4) particle-induced nuclear reactions for the product nuclides having metastable states with half-lives longer than 0.1 s using the EXFOR library. Comparison with the isomeric ratios predicted by the reaction model code TALYS-1.96.
doi: 10.1016/j.adt.2023.101583
2023VA11 Eur.Phys.J. N 9, 31 (2023) J.R.Vanhoy, R.C.Haight, S.F.Hicks, M.Devlin, D.Neudecker, M.Herman, A.Koning, K.J.Kelly, I.Thompson Templates of expected measurement uncertainties for (n, xn) cross sections NUCLEAR REACTIONS 56Fe, 23Na(n, n'), 9Be(n, X), E=3.5, 6 MeV; analyzed available data; deduced a template for evaluating experimental uncertainties for neutron elastic and inelastic scattering σ and γ-ray production σ from (n, xn) measurements at laboratories with monoenergetic or white neutron sources.
doi: 10.1051/epjn/2023019
2022AV01 Eur.Phys.J. A 58, 3 (2022) M.Avrigeanu, D.Rochman, A.J.Koning, U.Fischer, D.Leichtle, C.Costache, V.Avrigeanu Advanced breakup-nucleon enhancement of deuteron-induced reaction cross sections NUCLEAR REACTIONS 58Ni, 96Zr, 231Pa(d, X), (d, 2n), (d, 2p), E<200 MeV; calculated σ using TALYS-1.95 nuclear model code. Comparison with available data.
doi: 10.1140/epja/s10050-021-00659-6
2021FO05 Phys.Rev. C 103, 034601 (2021) M.B.Fox, A.S.Voyles, J.T.Morrell, L.A.Bernstein, A.M.Lewis, A.J.Koning, J.C.Batchelder, E.R.Birnbaum, C.S.Cutler, D.G.Medvedev, F.M.Nortier, E.M.O'Brien, C.Vermeulen Investigating high-energy proton-induced reactions on spherical nuclei: Implications for the preequilibrium exciton model NUCLEAR REACTIONS 93Nb(p, X)72Se/73As/74As/75Se/81Rb/82mRb/83Rb/83Sr/84Rb/85mY/86Rb/86Y/86Zr/87Y/87mY/88Y/88Zr/89Zr/90Nb/90Mo/91mNb/92mNb/93mNb, E=192.38, 177.11, 163.31, 148.66, 133.87, 119.8, 104.2, 91.21, 79.32, 72.52, 67.14, 63.06, 60.08, 57.47, 55.58, 53.62, 51.61 MeV; 93Nb(p, 4n)90Mo, (p, 3np)90Nb, (p, nα)89Zr, (p, 3n2p)89Zr, (p, 3npα)86Y, (p, 2α)88Zr, (p, n)93mMo, (p, np)92mNb, (p, 3nα)87Zr, (p, npα)88Y, (p, 4nα)86Zr, (p, 4np)89Nb, (p, 2npα)87Y, (p, np2α)84Rb, E=25-200 MeV; 139La(p, 5n)135Ce, (p, 6n)134Ce, (p, 4np)135La, (p, 7n)133mCe, (p, 3nα)133Ba/133mBa, (p, 3n)137Ce/137mCe, (p, n)139Ce, (p, 8n)132Ce, (p, 6np)133La, (p, 3npα)132Cs, (p, 5nα)131Ba, E=20-100 MeV; measured Eγ, Iγ, σ(E) by activation method in a Tri-lab collaboration among the Lawrence Berkeley, Los Alamos, and Brookhaven National Laboratories. Comparison with literature data, and with calculations of the nuclear model codes: TALYS, CoH, EMPIRE, and ALICE; deduced best parametrization for the preequilibrium two-component exciton model.
doi: 10.1103/PhysRevC.103.034601
2021FO13 Phys.Rev. C 104, 064615 (2021) M.B.Fox, A.S.Voyles, J.T.Morrell, L.A.Bernstein, J.C.Batchelder, E.R.Birnbaum, C.S.Cutler, A.J.Koning, A.M.Lewis, D.G.Medvedev, F.M.Nortier, E.M.O'Brien, Ch.Vermeulen Measurement and modeling of proton-induced reactions on arsenic from 35 to 200 MeV NUCLEAR REACTIONS 75As(p, X)56Co/57Co/58Co/60Co/65Zn/69mZn/66Ga/67Ga/68Ga/72Ga/66Ge/68Ge/69Ge/70As/71As/72As/73As/74As/72Se/73Se/75Se, E=35-200 MeV; Cu(p, X)44mSc/46Sc/47Sc/48V/48Cr/49Cr/51Cr/52Mn/54Mn/56Mn/55Co/56Co/57Co/60Co/56Ni/57Ni/59Fe/60Cu/61Cu/64Cu/62Zn/63Zn/65Zn, E=35-200 MeV; Ti(p, X)42K/43K/43Sc/44Sc/44mSc/46Sc/47Sc/48Sc/44Ti/47Ca/48V, E=35-200 MeV; measured production σ(E) using stacked-target technique, and off-line γ-ray spectrometry, Eγ, Iγ at the LBNL 88-Inch Cyclotron for E(p)<55 MeV, at LANL, IPF for E(p)=50-100 MeV, and at BNL, BLIP for E(p)=100-200 MeV. 75As(p, 4n)72Se, (p, 3n)73Se, (p, 3np)72As, (p, X)56Co/57Co/58Co/60Co/65Zn/69mZn/66Ga/67Ga/68Ga/72Ga/66Ge/68Ge/69Ge/70As/71As/73As/74As/75Se, E=25-200 MeV; Ti(p, X)44Sc/44mSc, E=10-200 MeV; Ti(p, X)42K/43K/43Sc/44Sc/44mSc/46Sc/47Sc/48Sc/47Ca/44Ti/48V, E=25-200 MeV; Cu(p, X)44mSc/46Sc/47Sc/48V/48Cr/49Cr/51Cr/52Mn/54Mn/56Mn/55Co/56Co/57Co/60Co/56Ni/57Ni/59Fe/60Cu/61Cu/64Cu/62Zn/63Zn/65Zn, E=25-200 MeV; comparison of measured s(E) in the present work and previous experiments with theoretical cross sections using ALICE-20, CoH-3.5.3, EMPIRE-3.2.3, TALYS-1.95 and TENDL-2019. 75As(p, n)75Se, (p, np)74As, E<200 MeV; 75As(p, 3n)73Se, (p, 2np)73As, (p, 4n)72Se, (p, X)71As/69Ge/68Ga/67Ga, E=25-200; TALYS default and adjusted σ(E) calculations for residual products. 75As(p, 3np)72As, (p, X)72Ga/70As/65Zn/69mZn/68Ge/66Ge/66Ga/56Co/57Co/58Co/60Co, E=25-200 MeV; TALYS default and adjusted calculations extended to residual products not used in the parameter adjustment sensitivity studies. 68,71,73As, 72,73Se, 69Ge, 67,69Ga; adjusted level density scalings in global fitting procedure for residual products. Relevance to production cross sections for positron emission tomography (PET) generator system of 72Se/72As and 68Ge/68Ga.
doi: 10.1103/PhysRevC.104.064615
2021SC11 Nucl.Data Sheets 173, 239 (2021) G.Schnabel, H.Sjostrand, J.Hansson, D.Rochman, A.Koning, R.Capote Conception and Software Implementation of a Nuclear Data Evaluation Pipeline NUCLEAR REACTIONS 56Fe(n, X), E<20 MeV; analyzed available EXFOR library data; calculated σ; deduced TALYS library parameters.
doi: 10.1016/j.nds.2021.04.007
2020PL02 Eur.Phys.J. A 56, 181 (2020) A.J.M.Plompen, O.Cabellos, C.De Saint Jean, M.Fleming, A.Algora, M.Angelone, P.Archier, E.Bauge, O.Bersillon, A.Blokhin, F.Cantargi, A.Chebboubi, C.Diez, H.Duarte, E.Dupont, J.Dyrda, B.Erasmus, L.Fiorito, U.Fischer, D.Flammini, D.Foligno, M.R.Gilbert, J.R.Granada, W.Haeck, F.-J.Hambsch, P.Helgesson, S.Hilaire, I.Hill, M.Hursin, R.Ichou, R.Jacqmin, B.Jansky, C.Jouanne, M.A.Kellett, D.H.Kim, H.I.Kim, I.Kodeli, A.J.Koning, A.Yu.Konobeyev, S.Kopecky, B.Kos, A.Krasa, L.C.Leal, N.Leclaire, P.Leconte, Y.O.Lee, H.Leeb, O.Litaize, M.Majerle, J.I.Marquez Damian, F.Michel-Sendis, R.W.Mills, B.Morillon, G.Noguere, M.Pecchia, S.Pelloni, P.Pereslavtsev, R.J.Perry, D.Rochman, A.Rohrmoser, P.Romain, P.Romojaro, D.Roubtsov, P.Sauvan, P.Schillebeeckx, K.H.Schmidt, O.Serot, S.Simakov, I.Sirakov, H.Sjostrand, A.Stankovskiy, J.C.Sublet, P.Tamagno, A.Trkov, S.van der Marck, F.Alvarez-Velarde, R.Villari, T.C.Ware, K.Yokoyama, G.Zerovnik The joint evaluated fission and fusion nuclear data library, JEFF-3.3
doi: 10.1140/epja/s10050-020-00141-9
2020RO03 Nucl.Data Sheets 163, 163 (2020) D.Rochman, A.J.Koning, J.-Ch.Sublet A Statistical Analysis of Evaluated Neutron Resonances with TARES for JEFF-3.3, JENDL-4.0, ENDF/B-VIII.0 and TENDL-2019
doi: 10.1016/j.nds.2019.12.003
2019BE41 Ann.Rev.Nucl.Part.Sci. 69, 109 (2019) L.A.Bernstein, D.A.Brown, A.J.Koning, B.T.Rearden, C.E.Romano, A.A.Sonzogni, A.S.Voyles, W.Younes Our Future Nuclear Data Needs
doi: 10.1146/annurev-nucl-101918-023708
2019CH01 Phys.Rev. C 99, 014305 (2019) E.V.Chimanski, B.V.Carlson, R.Capote, A.J.Koning Quasiparticle nature of excited states in random-phase approximation NUCLEAR STRUCTURE 56Ni; calculated level energy deviation, state strength function and width as function of excitation energy, contributions to the RPA transition matrix from collective, two-noncollective, and 3- states, response functions for low-energy 3-, and high energy particle-hole configurations of 3- states, single-particle contribution to the response function, width of the Breit-Wigner distribution for 3- and 4+ states, energy level spacing with local widths of particle-hole pair configurations. 16O, 56Ni, 90Zr, 120Sn; calculated spreading width of Breit Wigner distributions. Random phase approximation (RPA) on the basis of particle-hole configurations of excited states. Relevance to multistep direct (MSD) nuclear reactions.
doi: 10.1103/PhysRevC.99.014305
2019KO01 Nucl.Data Sheets 155, 1 (2019) A.J.Koning, D.Rochman, J.-Ch.Sublet, N.Dzysiuk, M.Fleming, S.van der Marck TENDL: Complete Nuclear Data Library for Innovative Nuclear Science and Technology
doi: 10.1016/j.nds.2019.01.002
2019UT01 Phys.Rev. C 99, 024609 (2019) H.Utsunomiya, T.Renstrom, G.M.Tveten, S.Goriely, T.Ari-izumi, D.Filipescu, J.Kaur, Y.-W.Lui, W.Luo, S.Miyamoto, A.C.Larsen, S.Hilaire, S.Peru, A.J.Koning γ-ray strength function for thallium isotopes relevant to the 205Pb - 205Tl chronometry NUCLEAR REACTIONS 203,205Tl(γ, n), E=7.9-13.0 MeV; measured E(n), I(n), σ(E) using 4π 3He proportional counter array for neutron detection at NewSUBARU synchrotronic radiation facility; deduced GDR parameters and γ-ray strength function (γSF), the latter on the basis of the Hartree-Fock-Bogolyubov plus quasiparticle random-phase approximation using the Gogny D1M interaction for E1 and M1 components with the zero-limit correction (QRPA+D1M+0lim). 203,205Tl(n, γ), Eγ=0.001-4 MeV; calculated σ(E) with the D1M+QRPA+0lim, and compared with available experimental results. 204Tl(n, γ), T=0-1 GK; calculated Maxwellian averaged σ(E) (MACS) with the D1M+QRPA+0lim strength function, and compared with experimental results, and recommended σ in compilations by Bao et al.
doi: 10.1103/PhysRevC.99.024609
2019UT02 Phys.Rev. C 100, 034605 (2019) H.Utsunomiya, T.Renstrom, G.M.Tveten, S.Goriely, T.Ari-izumi, V.W.Ingeberg, B.V.Kheswa, Y.-W.Lui, S.Miyamoto, S.Hilaire, S.Peru, A.J.Koning γ-ray strength function for barium isotopes NUCLEAR REACTIONS 137Ba(γ, n)136Ba, E=7-13 MeV; 138Ba(γ, n)137Ba, E=8.75-13 MeV from laser Compton scattering at the NewSUBARU synchrotron radiation facility at the University of Hyogo; measured En, In; deduced σ(E), E1 and M1 γ-strength functions; σ(E) compared to TALYS calculations. The photoneutron data used to constrain the γ strength function on the basis of the Hartree-Fock-Bogolyubov plus quasiparticle random phase approximation using the Gogny D1M interaction. Comparison with previous experimental data. 131,133Ba(n, γ), kT=30 keV; estimated Maxwellian-averaged cross sections.
doi: 10.1103/PhysRevC.100.034605
2018BA02 Acta Phys.Pol. B49, 27 (2018) A.Bajpeyi, A.Shukla, A.J.Koning Systematic Nuclear Structure and Nuclear Reaction Studies Relevant to p-process NUCLEAR REACTIONS 102Pd, 120Te, 124,126Xe, 130,132Ba(p, γ), (α, γ), E<15 MeV; calculated σ using TALYS nuclear model code. Comparison with available data.
doi: 10.5506/aphyspolb.49.27
2018BR05 Nucl.Data Sheets 148, 1 (2018) D.A.Brown, M.B.Chadwick, R.Capote, A.C.Kahler, A.Trkov, M.W.Herman, A.A.Sonzogni, Y.Danon, A.D.Carlson, M.Dunn, D.L.Smith, G.M.Hale, G.Arbanas, R.Arcilla, C.R.Bates, B.Beck, B.Becker, F.Brown, R.J.Casperson, J.Conlin, D.E.Cullen, M.-A.Descalle, R.Firestone, T.Gaines, K.H.Guber, A.I.Hawari, J.Holmes, T.D.Johnson, T.Kawano, B.C.Kiedrowski, A.J.Koning, S.Kopecky, L.Leal, J.P.Lestone, C.Lubitz, J.I.Marquez Damian, C.M.Mattoon, E.A.McCutchan, S.Mughabghab, P.Navratil, D.Neudecker, G.P.A.Nobre, G.Noguere, M.Paris, M.T.Pigni, A.J.Plompen, B.Pritychenko, V.G.Pronyaev, D.Roubtsov, D.Rochman, P.Romano, P.Schillebeeckx, S.Simakov, M.Sin, I.Sirakov, B.Sleaford, V.Sobes, E.S.Soukhovitskii, I.Stetcu, P.Talou, I.Thompson, S.van der Marck, L.Welser-Sherrill, D.Wiarda, M.White, J.L.Wormald, R.Q.Wright, M.Zerkle, G.Zerovnik, Y.Zhu ENDF/B-VIII.0: The 8 th Major Release of the Nuclear Reaction Data Library with CIELO-project Cross Sections, New Standards and Thermal Scattering Data COMPILATION Z=1-118; compiled, analyzed decay data, Maxwellian averaged neutron capture σ, neutron-induced fission σ. NUCLEAR REACTIONS 1,2H, 3He, 6,7Li, 9Be, 10,11B, 12,13C, 14,15N, 16,17,18O, 19F, 20,21,22Ne, 22,23Na, 24,25,26Mg, 26,27Al, 28,29,30,31,32Si, 31P, 32,33,34,35,36S, 35,36,37Cl, 36,37,38,39,40,41Ar, 39,40,41K, 40,41,42,43,44,45,46,47,48Ca, 45Sc, 46,47,48,49,50Ti, 49,50,51V, 50,51,52,53,54Cr, 54,55Mn, 54,55,56,57,58Fe, 58,59Co, 58,59,60,61,62,63,64Ni, 63,64,65Cu, 64,65,66,67,68,69,70Zn, 69,70,71Ga, 70,71,72,73,74,75,76Ge, 73,74,75As, 74,75,76,77,78,79,80,81,82Se, 79,80,81Br, 78,79,80,81,82,83,84,85,86Kr, 85,86,87Rb, 84,85,86,87,88,89,90Sr, 89,90,91Y, 90,91,92,93,94,95,96Zr, 93,94,95Nb, 92,93,94,95,96,97,98,99,100Mo, 98,99Tc, 96,97,98,99,100,101,102,103,104,105,106Ru, 103,104,105Rh, 102,103,104,105,106,107,108,109,110Pd, 107,108,109,110,111,112,113,114,115,116,117,118Ag, 106,107,108,109,110,111,112,113,114,115,116Cd, 113,114,115In, 112,113,114,115,116,117,118,119,120,121,122,123,124,125,126Sn, 121,122,123,124,125,126Sb, 120,121,122,123,124,125,126,127,128,129,130,121,132Te, 127,128,129,130,131,132,133,134,135I, 123,124,125,126,127,128,129,130,131,132,133,134,135,136Xe, 133,134,135,136,137Cs, 130,131,132,133,134,135,136,137,138,139,140Ba, 138,139,140La, 136,137,138,139,140,141,142,143,144Ce, 141,142,143Pr, 142,143,144,145,146,147,148,149,150Nd, 143,144,145,146,147,148,149,151Pm, 144,145,146,147,148,149,150,151,152,153,154Sm, 151,152,153,154,155,156,157Eu, 152,153,154,155,156,157,158,159,160Gd, 158,159,160,161Tb, 154,155,156,157,158,159,160,161,162,163,164Dy, 165,166Ho, 162,163,164,165,166,167,168,170,170Er, 168,169,170,171Tm, 168,169,170,171,172,173,174,175,176Yb, 175,176Lu, 174,175,176,177,178,179,180,181,182Hf, 180,181,182Ta, 180,181,182,183,184,185,186W, 185,186,187Re, 184,185,186,187,188,189,190,191,192Os, 191,192,193Ir, 190,191,192,193,194,195,196,197,198Pt, 197Au, 196,197,198,199,200,201,202,203,204Hg, 203,204,205Tl, 204,205,206,207,208,209,210Pb, 209,210Bi, 208,209,210Po, 223,224,225,226Ra, 225,226,227Ac, 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,245,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,248,249,250Bk, 246,247,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), E=30 keV; calculated Maxwellian-averaged σ using ENDF/B-VIII.0 evaluated neutron library. Comparison with ENDF/B-VII.1 and KADONIS values. NUCLEAR REACTIONS 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,245,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,248,249,250Bk, 246,247,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), (n, F), E=thermal; calculated thermal σ. Comparison with ENDF/B-VII.1, JENDL-4.0u+ and Atlas of Neutron Resonances values.
doi: 10.1016/j.nds.2018.02.001
2018CH12 Nucl.Data Sheets 148, 189 (2018) M.B.Chadwick, R.Capote, A.Trkov, M.W.Herman, D.A.Brown, G.M.Hale, A.C.Kahler, P.Talou, A.J.Plompen, P.Schillebeeckx, M.T.Pigni, L.Leal, Y.Danon, A.D.Carlson, P.Romain, B.Morillon, E.Bauge, F.-J.Hambsch, S.Kopecky, G.Giorginis, T.Kawano, J.Lestone, D.Neudecker, M.Rising, M.Paris, G.P.A.Nobre, R.Arcilla, O.Cabellos, I.Hill, E.Dupont, A.J.Koning, D.Cano-Ott, E.Mendoza, J.Balibrea, C.Paradela, I.Duran, J.Qian, Z.Ge, T.Liu, L.Hanlin, X.Ruan, W.Haicheng, M.Sin, G.Noguere, D.Bernard, R.Jacqmin, O.Bouland, C.De Saint Jean, V.G.Pronyaev, A.V.Ignatyuk, K.Yokoyama, M.Ishikawa, T.Fukahori, N.Iwamoto, O.Iwamoto, S.Kunieda, C.R.Lubitz, M.Salvatores, G.Palmiotti, I.Kodeli, B.Kiedrowski, D.Roubtsov, I.Thompson, S.Quaglioni, H.I.Kim, Y.O.Lee, U.Fischer, S.Simakov, M.Dunn, K.Guber, J.I.Marquez Damian, F.Cantargi, I.Sirakov, N.Otuka, A.Daskalakis, B.J.McDermott, S.C.van der Marck CIELO Collaboration Summary Results: International Evaluations of Neutron Reactions on Uranium, Plutonium, Iron, Oxygen and Hydrogen NUCLEAR REACTIONS 1H, 16O, 56Fe, 235,238U, 239Pu(n, X), E<20 MeV; analyzed available data; calculated σ, σ(θ), σ(θ, E).
doi: 10.1016/j.nds.2018.02.003
2018UT03 Phys.Rev. C 98, 054619 (2018) H.Utsunomiya, T.Renstrom, G.M.Tveten, S.Goriely, S.Katayama, T.Ari-izumi, D.Takenaka, D.Symochko, B.V.Kheswa, V.W.Ingeberg, T.Glodariu, Y.-W.Lui, S.Miyamoto, A.C.Larsen, J.E.Midtbo, A.Gorgen, S.Siem, L.Crespo Campo, M.Guttormsen, S.Hilaire, S.Peru, A.J.Koning Photoneutron cross sections for Ni isotopes: Toward understanding (n, γ) cross sections relevant to weak s-process nucleosynthesis NUCLEAR REACTIONS 58,60,61,64Ni(γ, n), E=8.00-22.02 MeV; measured E(n), I(n), σ(E) using 3He proportional counters for neutrons and LaBr3(Ce) detector for γ-flux at NewSUBARU synchrotron radiation facility; deduced γ-ray strength functions (γSF); compared σ(E) with previous experimental data, and with TALYS predictions. 58,60,63,64(n, γ), E=0.01-10 MeV; calculated radiative σ(E) and Maxwellian averaged σ (MACS) in terms of the experimentally constrained γ-ray strength functions from the Hartree-Fock-Bogolyubov plus quasiparticle-random-phase approximation (HFB+QRPA) based on the Gogny D1M interaction for E1 and M1 components, supplemented with the M1 upbend. Relevance to the s-process nucleosynthesis, and radioactive nuclei at the s-process branching points.
doi: 10.1103/PhysRevC.98.054619
2017BA23 Phys.Atomic Nuclei 80, 402 (2017) A.Bajpeyi, A.Shukla, A.J.Koning, S.Aberg Study of the (p, γ) and (α, γ) reactions for 96, 98, 104Ru and 112, 114, 116Sn at astrophysically relevant energies
doi: 10.1134/S1063778817030024
2017RO18 Phys.Lett. B 764, 109 (2017) D.Rochman, S.Goriely, A.J.Koning, H.Ferroukhi Radiative neutron capture: Hauser Feshbach vs. statistical resonances NUCLEAR REACTIONS 24Mg, 27Al, 28Si, 32S, 110,112,115,118,120,122,124,128,138,148,158Sn, 187Re(n, γ), E<200 KeV; calculated Maxwellian-averaged σ using statistical Hauser Feshbach reaction model and High Fidelity Resonance method. Comparison with available data.
doi: 10.1016/j.physletb.2016.11.018
2016RO09 Ann.Nucl.Energy 94, 612 (2016) D.Rochman, O.Leray, G.Perret, A.Vasiliev, H.Ferroukhi, A.J.Koning Re-evaluation of the thermal neutron capture cross section of 147Nd NUCLEAR REACTIONS 147Nd(n, γ), E thermal; analyzed available data; deduced a need for σ reevaluation.
doi: 10.1016/j.anucene.2016.03.024
2015BA56 Eur.Phys.J. A 51, 157 (2015) A.Bajpeyi, A.J.Koning, A.Shukla, S.Aberg Systematic study of proton capture rates for Mo and Cd isotopes
doi: 10.1140/epja/i2015-15157-1
2015DZ01 Nucl.Phys. A936, 6 (2015) N.Dzysiuk, I.Kadenko, V.Gressier, A.J.Koning Cross section measurement of the 159Tb(n, γ)Tb160 nuclear reaction NUCLEAR REACTIONS 159Tb(n, γ), E=3.7, 4.3, 5.4, 7.0 MeV; measured activation Eγ, Iγ; deduced σ; calculated σ using TALYS-1.2 with different level density models. Compared with TENDL 2011, ENDF/B-VII and EXFOR data.
doi: 10.1016/j.nuclphysa.2015.01.003
2015HE02 Nucl.Data Sheets 123, 214 (2015) P.Helgesson, H.Sjostrand, A.J.Koning, D.Rochman, E.Alhassan, S.Pomp Incorporating Experimental Information in the Total Monte Carlo Methodology Using File Weights
doi: 10.1016/j.nds.2014.12.037
2015KO01 Nucl.Data Sheets 123, 207 (2015) Bayesian Monte Carlo Method for Nuclear Data Evaluation
doi: 10.1016/j.nds.2014.12.036
2015KO22 Eur.Phys.J. A 51, 184 (2015) Bayesian Monte Carlo method for nuclear data evaluation
doi: 10.1140/epja/i2015-15184-x
2015NE11 Phys.Rev. C 91, 064618 (2015) A.Negret, L.C.Mihailescu, C.Borcea, Ph.Dessagne, K.H.Guber, M.Kerveno, A.J.Koning, A.Olacel, A.J.M.Plompen, C.Rouki, G.Rudolf Cross section measurements for neutron inelastic scattering and the (n, 2nγ) reaction on 206Pb NUCLEAR REACTIONS 206Pb(n, n'), (n, 2n), E=0.8-18 MeV; measured Eγ, Iγ at GELINA neutron time-of-flight facility of the EC-JRC-IRMM. 206Pb; deduced levels, J, π, γ-branching ratios, integral γ-ray production σ(E). 205Pb; deduced integral γ-ray production σ(E) for 703.4- and 987.7-keV γ rays in 205Pb. Comparison with TALYS reaction code calculations, evaluated data, and previous experimental values.
doi: 10.1103/PhysRevC.91.064618
2015NY01 Phys.Rev. C 91, 015808 (2015) H.-T.Nyhus, T.Renstrom, H.Utsunomiya, S.Goriely, D.M.Filipescu, I.Gheorghe, O.Tesileanu, T.Glodariu, T.Shima, K.Takahisa, S.Miyamoto, Y.-W.Lui, S.Hilaire, S.Peru, M.Martini, L.Siess, A.J.Koning Photoneutron cross sections for neodymium isotopes: Toward a unified understanding of (γ, n) and (n, γ) reactions in the rare earth region NUCLEAR REACTIONS 143,144,145,146,148Nd(γ, n), E=7.55-13.00 MeV laser Compton scattered (LCS) rays; measured neutron spectra, σ(E) at GACKO (Gamma Collaboration Hutch of Konan University) using SUBARU synchrotron radiation facility; deduced σ(E) for 147Nd(n, γ) by combining present (γ, n) data with existing (n, γ) data for 142,143,144,145,146,148Nd(n, γ), and using γ-SF method. Comparison of σ(E) for 147Nd(n, γ) with JENDL-4.0, ENDF/B-VII.1, and ROSFOND-2010 evaluated libraries. Comparison with predictions of Skyrme-Fock-Bogoliubov (HFB) plus quasiparticle random phase approximation (QRPA) model, and axially symmetric-deformed Gogny HFB plus QRPA model of E1 γ-ray strength using TALYS code. Comparison with previous experimental data.
doi: 10.1103/PhysRevC.91.015808
2015PO02 Nucl.Data Sheets 123, 220 (2015) S.Pomp, A.Al-Adili, E.Alhassan, C.Gustavsson, P.Helgesson, C.Hellesen, A.J.Koning, M.Lantz, M.Osterlund, D.Rochman, V.Simutkin, H.Sjostrand, A.Solders Experiments and Theoretical Data for Studying the Impact of Fission Yield Uncertainties on the Nuclear Fuel Cycle with TALYS/GEF and the Total Monte Carlo Method
doi: 10.1016/j.nds.2014.12.038
2015RO29 Eur.Phys.J. A 51, 182 (2015) D.Rochman, A.J.Koning, S.C.van der Marck Improving neutronics simulations and uncertainties via a selection of nuclear data
doi: 10.1140/epja/i2015-15182-0
2014AL26 Nucl.Data Sheets 118, 542 (2014) E.Alhassan, H.Sjostrand, J.Duan, C.Gustavsson, A.J.Koning, S.Pomp, D.Rochman, M.Osterlund Combining Total Monte Carlo and Benchmarks for Nuclear Data Uncertainty Propagation on a Lead Fast Reactor's Safety Parameters
doi: 10.1016/j.nds.2014.04.129
2014BA22 Nucl.Data Sheets 118, 32 (2014) E.Bauge, M.Dupuis, S.Hilaire, S.Peru, A.J.Koning, D.Rochman, S.Goriely Connecting the Dots, or Nuclear Data in the Age of Supercomputing NUCLEAR REACTIONS 238U(n, xn), E=14.1 MeV; calculated σ(En, θ=300, σ(En, θ=900 using TMC )TALYS/TEFAL/NJOY) code system. Compared to data. NUCLEAR STRUCTURE N=4-170; calculated binding energy, Q using beyond-the-mean-field level using different interactions.
doi: 10.1016/j.nds.2014.04.004
2014BA34 Nucl.Data Sheets 119, 186 (2014) A.Bacquias, Ph.Dessagne, M.Kerveno, G.Rudolf, A.J.M.Plompen, J.C.Drohe, C.Rouki, N.Nankov, M.Nyman, C.Borcea, A.Negret, P.Archier, C.De Saint Jean, G.Noguere, C.Vaglio-Gaudard, A.Koning, A.Domula, K.Zuber, L.C.Leal Neutron Inelastic Scattering Measurements for Na, Ge, Zr, Mo and U NUCLEAR REACTIONS 238U(n, n'γ), (n, 2nγ), E=0-22 MeV; measured Eγ, Iγ; deduced γ transitions, σ; calculated σ using TALYS-1.2 and EMPIRE. Compared with other data. 92Mo(n, n'γ), 95Mo(n, n'γ), 96Mo(n, n'γ), 98Mo(n, n'γ), E=50-18000 keV; measured Eγ, Iγ; deduced γ transitions, yields. Measurements for some other targets sent for publications but not given here.
doi: 10.1016/j.nds.2014.08.052
2014CH24 Nucl.Data Sheets 118, 1 (2014) M.B.Chadwick, E.Dupont, E.Bauge, A.Blokhin, O.Bouland, D.A.Brown, R.Capote, A.Carlson, Y.Danon, C.De Saint Jean, M.Dunn, U.Fischer, R.A.Forrest, S.C.Frankle, T.Fukahori, Z.Ge, S.M.Grimes, G.M.Hale, M.Herman, A.Ignatyuk, M.Ishikawa, N.Iwamoto, O.Iwamoto, M.Jandel, R.Jacqmin, T.Kawano, S.Kunieda, A.Kahler, B.Kiedrowski, I.Kodeli, A.J.Koning, L.Leal, Y.O.Lee, J.P.Lestone, C.Lubitz, M.MacInnes, D.McNabb, R.McKnight, M.Moxon, S.Mughabghab, G.Noguere, G.Palmiotti, A.Plompen, B.Pritychenko, V.Pronyaev, D.Rochman, P.Romain, D.Roubtsov, P.Schillebeeckx, M.Salvatores, S.Simakov, E.Sh.Soukhovitskii, J.C.Sublet, P.Talou, I.Thompson, A.Trkov, R.Vogt, S.van der Marck The CIELO Collaboration: Neutron Reactions on 1H, 16O, 56Fe, 235, 238U, and 239Pu COMPILATION 1H, 16O, 56Fe, 235,238U, 239Pu(n, x), E≈0-20 MeV; analyzed available data on σ, neutron multiplicity, criticality using ENDF/B-VII.1, JENDL-4.0, JEFF-3.1, ROSFOND 2010, CENDL-3.1, EAF-2010 evaluated nuclear libraries, Atlas of Neutron Resonances, Neutron Cross Section Standards evaluations; deduced recommendations for CIELO library, parameters, Maxwellian-averaged, thermal, californium σ, Westcott factors, resonance integrals. Compared with available data.
doi: 10.1016/j.nds.2014.04.002
2014DA05 Nucl.Technology 185, 174 (2014) D.F.Da Cruz, D.Rochman, A.J.Koning Uncertainty Analysis on Reactivity and Discharged Inventory Due to 235, 238U, 239, 240, 241Pu, and Fission Products: Application to a Pressurized Water Reactor Fuel Assembly NUCLEAR REACTIONS 235,238U, 239,240,241Pu(n, F), E thermal; analyzed uncertainties for keff, fission yield and products. Comparison with available data.
doi: 10.13182/NT12-154
2014DA12 Nucl.Data Sheets 118, 531 (2014) D.F.da Cruz, D.Rochman, A.J.Koning Quantification of Uncertainties due to 235, 238U, 239, 240, 241Pu and Fission Products Nuclear Data Uncertainties for a PWR Fuel Assembly
doi: 10.1016/j.nds.2014.04.126
2014DU07 Nucl.Data Sheets 118, 346 (2014) J.Duan, S.Pomp, H.Sjostrand, E.Alhassan, C.Gustavsson, M.Osterlund, A.Koning, D.Rochman Uncertainty Study of Nuclear Model Parameters for the n+56Fe Reactions in the Fast Neutron Region below 20 MeV
doi: 10.1016/j.nds.2014.04.076
2014DU08 Nucl.Data Sheets 120, 264 (2014) E.Dupont, M.B.Chadwick, Y.Danon, C.De Saint Jean, M.Dunn, U.Fischer, R.A.Forrest, T.Fukahori, Z.Ge, H.Harada, M.Herman, M.Igashira, A.Ignatyuk, M.Ishikawa, O.Iwamoto, R.Jacqmin, A.C.Kahler, T.Kawano, A.J.Koning, L.Leal, Y.O.Lee, R.McKnight, D.McNabb, R.W.Mills, G.Palmiotti, A.Plompen, M.Salvatores, P.Schillebeeckx Working Party on International Nuclear Data Evaluation Cooperation (WPEC)
doi: 10.1016/j.nds.2014.07.063
2014FI12 Nucl.Data Sheets 120, 226 (2014) U.Fischer, M.Avrigeanu, V.Avrigeanu, O.Cabellos, I.Kodeli, A.Koning, A.Yu.Konobeyev, H.Leeb, D.Rochman, P.Pereslavtsev, P.Sauvan, J.-C.Sublet, A.Trkov, E.Dupont, D.Leichtle, J.Izquierdo The Activities of the European Consortium on Nuclear Data Development and Analysis for Fusion
doi: 10.1016/j.nds.2014.07.053
2014FI17 Phys.Rev. C 90, 064616 (2014) D.M.Filipescu, I.Gheorghe, H.Utsunomiya, S.Goriely, T.Renstrom, H.-T.Nyhus, O.Tesileanu, T.Glodariu, T.Shima, K.Takahisa, S.Miyamoto, Y.-W.Lui, S.Hilaire, S.Peru, M.Martini, A.J.Koning Photoneutron cross sections for samarium isotopes: Toward a unified understanding of (γ, n) and (n, γ) reactions in the rare earth region NUCLEAR REACTIONS 144,147,148,149,150,152,154Sm(γ, n), E=6-17 MeV; measured E(n), I(n), monochromatic and nonmonochromatic σ(E). Comparison with previous experimental results, and predictions from Skyrme HFB+QRPA using BSk7 interaction, and axially deformed Gogny HFB+QRPA models using D1M interaction. 147,148,149,150,151,152Sm(n, γ), E=0.001-1 MeV; analyzed measured σ(E) with a TALYS calculation using D1M+QRPA calculation for the E1 strength function. 153Sm(n, γ), E=0.001-1 MeV; predicted σ(E) from TALYS calculations using γ-strength function (γSF) approach. Comparison with evaluated libraries JENDL-4.0, ENDF/B-VII.1, ROSFOND-2010.
doi: 10.1103/PhysRevC.90.064616
2014KE06 Eur.Phys.J. A 50, 162 (2014) M.Kerveno, R.Nolte, P.Baumann, Ph.Dessagne, E.Jericha, S.Jokic, A.J.Koning, S.Lukic, J.P.Meulders, A.Nachab, A.Pavlik, M.Reginatto, G.Rudolf Measurement of 232Th(n, 5n γ) cross sections from 29 MeV to 42 MeV NUCLEAR REACTIONS 232Th(n, 5n), E=29-42 MeV; measured Eγ, Iγ(θ) using HPGe; deduced σ(θ) to specified states, γ-ray spectrum, σ; calculated σ to specific γ-transitions using TALYS-1.4, fission σ. Compared with ENDF/B-VII.1, JEFF-3.1, JENDL-4.0 and EXFOR data.
doi: 10.1140/epja/i2014-14162-2
2014KO19 Nucl.Data Sheets 118, 187 (2014) A.J.Koning, D.Rochman, S.C.van der Marck Extension of TALYS to 1 GeV NUCLEAR REACTIONS 27Al, 93Nb, 197Au(n, x), (p, x), E=0-1000 MeV; calculated neutron total σ, proton non-elastic σ. Fe(d, x)52Mn, E=1-1000 MeV;Fe(p, x)32P, E=100-1000 MeV;Fe(p, x)51Cr, E=1-1000 MeV;Pb(p, x)198Pb, E=10-1000 MeV;Pb(p, x)203Bi, E=1-1000 MeV;Pb(p, x)202Tl, E=10=1000 MeV;208Pb(p, x)202Tl, E=10=1000 MeV; calculated σ. TALYS code.
doi: 10.1016/j.nds.2014.04.033
2014KO31 Nucl.Data Sheets 119, 310 (2014) T.Kondo, H.Utsunomiya, S.Goriely, C.Iwamoto, H.Akimune, T.Yamagata, H.Toyokawa, H.Harada, F.Kitatani, Y.-W.Lui, S.Hilaire, A.J.Koning Partial Photoneutron Cross Sections for 207, 208Pb NUCLEAR REACTIONS 207,208Pb(polarized γ, n), E=6.5-12.5 MeV; measured En, In; deduced σ, partial σ(E1), σ(M1), B(E1), B(M1), pygmy dipole resonance near the neutron threshold, relative contribution of M1 γ-decay strength to total photoneutron σ; calculated partial E1 σ using HFB plus QRPA and paramaterized PDR. Compared with Harvey data (renormalized by a factor of 1.22).
doi: 10.1016/j.nds.2014.08.085
2014MA38 Nucl.Data Sheets 118, 273 (2014) M.Martini, S.Hilaire, S.Goriely, A.J.Koning, S.Peru Improved Nuclear Inputs for Nuclear Model Codes Based on the Gogny Interaction NUCLEAR STRUCTURE 238U; calculated positive parity level density, temperature (and level density for T=0) below 100 MeV. NUCLEAR REACTIONS 174Yb, 180Hf, 238U(γ, x), E=5-25 MeV; calculated photoabsorption σ using QRPA with broadening. Sn(n, x), E≈90 keV; calculated Maxwell-averaged neutron capture rate for isotopes between 115 and 160 using GLO and QRPA.
doi: 10.1016/j.nds.2014.04.056
2014QA01 Appl.Radiat.Isot. 85, 101 (2014) S.M.Qaim, S.Sudar, B.Scholten, A.J.Koning, H.H.Coenen Evaluation of excitation functions of 100Mo(p, d+pn)99Mo and 100Mo (p, 2n)99mTc reactions: Estimation of long-lived Tc-impurity and its implication on the specific activity of cyclotron-produced 99mTc NUCLEAR REACTIONS 98,100Mo(p, γ), 100Mo(p, α), (p, nα), (p, 2nα), (p, npd), (p, n), (p, 2n), 100Mo(p, xn)100Tc/99Tc/98Tc/97Tc/96Tc, E<70 MeV; calculated σ. TALYS, STARPE nuclear model code calculations, comparison with experimental data. NUCLEAR REACTIONS Mo(p, X)96Tc, E<70 MeV; analyzed available data; deduced σ.
doi: 10.1016/j.apradiso.2013.10.004
2014RO10 Nucl.Data Sheets 118, 367 (2014) D.Rochman, S.C.van der Marck, A.J.Koning, H.Sjostrand, W.Zwermann Uncertainty Propagation with Fast Monte Carlo Techniques
doi: 10.1016/j.nds.2014.04.082
2014RO16 Ann.Nucl.Energy 73, 7 (2014) D.Rochman, A.J.Koning, E.Bauge, A.J.M.Plompen From flatness to steepness: Updating TALYS covariances with experimental information NUCLEAR REACTIONS 56Fe(n, X), E<20 MeV; calculated σ. EXFOR library, TALYS nuclear reaction model code.
doi: 10.1016/j.anucene.2014.06.016
2014SJ01 Nucl.Data Sheets 118, 527 (2014) H.Sjostrand, E.Alhassan, J.Duan, C.Gustavsson, A.J.Koning, S.Pomp, D.Rochman, M.Osterlund Propagation of Nuclear Data Uncertainties for ELECTRA Burn-up Calculations
doi: 10.1016/j.nds.2014.04.125
2014SU15 Nucl.Data Sheets 118, 418 (2014) J.-Ch.Sublet, A.Koning, D.Rochman TENDL-2012 Processing, Verification and Validation Steps
doi: 10.1016/j.nds.2014.04.095
2014VA09 Nucl.Data Sheets 118, 446 (2014) S.C.van der Marck, A.J.Koning, D.A.Rochman Benchmarking TENDL-2012
doi: 10.1016/j.nds.2014.04.102
2014XU09 Phys.Rev. C 90, 024604 (2014) Y.Xu, S.Goriely, A.J.Koning, S.Hilaire Systematic study of neutron capture including the compound, pre-equilibrium, and direct mechanisms NUCLEAR REACTIONS 16,18O, 22Ne, 26Mg, 27Al, 37Cl, 48Ca, 61Ni, 97Mo, 112Sn, 176Lu, 208Pb, 232Th(n, γ), E=0.001-10 MeV; calculated total capture σ(E) for three processes of compound-nucleus capture (CNC), pre-equilibrium capture (PEC), and direct capture (DIC) using Hauser-Feshbach model, the exciton model, and potential model, respectively, and Compared with experimental data. Z=8-100, N=10-180; calculated total neutron-capture cross sections and astrophysical reaction rates using TALYS code for about 8000 nuclei. Impact of the newly determined reaction rates on the r process abundances.
doi: 10.1103/PhysRevC.90.024604
2014ZE01 Nucl.Data Sheets 120, 277 (2014) O.Zeydina, A.J.Koning, N.Soppera, D.Raffanel, M.Bossant, E.Dupont, B.Beauzamy Cross-checking of Large Evaluated and Experimental Nuclear Reaction Databases NUCLEAR REACTIONS 72Ge(n, p), E<30 MeV; analyzed available data.; deduced EXFOR data deficiencies. Comparison with JEFF and TENDL libraries.
doi: 10.1016/j.nds.2014.07.066
2013AV05 Phys.Rev. C 88, 014612 (2013) M.Avrigeanu, V.Avrigeanu, P.Bem, U.Fischer, M.Honusek, A.J.Koning, J.Mrazek, E.Simeckova, M.Stefanik, L.Zavorka Low-energy deuteron-induced reactions on 93Nb NUCLEAR REACTIONS 93Nb(d, p)94mNb; 93Nb(d, 2n)93mMo; 93Nb(d, X)92mNb; 93Nb(d, 2nα)89Zr; 93Nb(d, pα)90mY, E=1-20 MeV; measured Eγ, Iγ, σ(E) by activation method and stacked-foil technique. Comparison with previous experimental data. 93Nb(d, d), E=11.8, 15, 34.4, 52 MeV; analyzed σ(θ, E) data; deduced optical model parameters. 93,94,95Mo; comparison of previously measured and calculated E1 strength functions. Comparisons with calculations which included deuteron breakup effects, one-nucleon transfer (DR), pre-equilibrium (PE) and compound nucleus mechanisms, spin distribution of nuclear level densities and radiative strength functions using FRESCO and STAPRE-H computer codes. Comparison with calculations using TALYS-1.4 computer code, and with TENDL-2012 evaluated data.
doi: 10.1103/PhysRevC.88.014612
2013RO31 Phys.Rev. C 88, 054613 (2013) C.Rouki, A.R.Domula, J.C.Drohe, A.J.Koning, A.J.M.Plompen, K.Zuber γ production and neutron inelastic scattering cross sections for 76Ge NUCLEAR REACTIONS 76Ge(n, n'), E=white spectrum; measured Eγ, Iγ using GAINS array at GELINA-IRMM facility. 76Ge; deduced levels, γ branching ratios; production σ of 2040.7-keV γ ray from 3951.9-keV level in connection with its relevance to GERDA experiments for double-beta decay. 76Ge(n, n'), E<2.3 MeV; measured angle-integrated σ(E) for several γ rays, comparison with previous experimental results and TALYS model code calculations using DWBA for first few levels. Discussed implications for 0νββ experimental studies.
doi: 10.1103/PhysRevC.88.054613
2013UT02 Phys.Rev. C 88, 015805 (2013) H.Utsunomiya, S.Goriely, T.Kondo, C.Iwamoto, H.Akimune, T.Yamagata, H.Toyokawa, H.Harada, F.Kitatani, Y.-W.Lui, A.C.Larsen, M.Guttormsen, P.E.Koehler, S.Hilaire, S.Peru, M.Martini, A.J.Koning Photoneutron cross sections for Mo isotopes: A step toward a unified understanding of (γ, n) and (n, γ) reactions NUCLEAR REACTIONS 94,95,96,97,98,100Mo(γ, n), E=7.55-13.00 MeV laser Compton scattered (LCS) γ rays; measured neutron spectra, σ(E). Comparison with previous experimental measurements, and with predictions of Skyrme Hartree-Fock-Bogoliubov (HFB) plus quasiparticle random phase approximation (QRPA) model, and axially symmetric-deformed Gogny HFB plus QRPA model of E1 γ-ray strength. 94,95,96,97(n, γ); analyzed σ(E) data by combining data from (γ, n), (γ, γ'), (3He, αγ) and (3He, 3He'γ) experiments. 93,99Mo(n, γ); predicted TALYS σ using (γ, γ') and (3He, 3He'γ) data. Comparison with JENDL-4.0, ENDF/B-VII.1, and ROSFOND-2010 evaluated reaction data files.
doi: 10.1103/PhysRevC.88.015805
2012AV02 Phys.Rev. C 85, 034603 (2012) M.Avrigeanu, V.Avrigeanu, A.J.Koning Investigation of deuteron breakup and deuteron-induced fission on actinide nuclei at low incident energies NUCLEAR REACTIONS 231Pa(d, 3n)230U, E=10-20 MeV; analyzed deuteron breakup cross section as function of energy, excitation function, neutron- and proton-emission cross sections. Investigated dominance of the deuteron breakup mechanism. Comparison with Evaluated data.
doi: 10.1103/PhysRevC.85.034603
2012GO12 J.Phys.:Conf.Ser. 337, 012026 (2012) S.Goriely, S.Hilaire, A.J.Koning, M.Girod Nuclear ingredients for cross section calculation of exotic nuclei
doi: 10.1088/1742-6596/337/1/012026
2012HI11 Phys.Rev. C 86, 064317 (2012) S.Hilaire, M.Girod, S.Goriely, A.J.Koning Temperature-dependent combinatorial level densities with the D1M Gogny force NUCLEAR STRUCTURE 54Cr, 100Ru, 130Xe, 180Hf, 208Pb, 238U; calculated excitation energies, quadrupole deformations, moments of inertia as function of nuclear temperature. A=20-250; deduced ratio of HFB plus combinatorial densities to experimental s-wave neutron resonance spacings as function of temperature. 40Ca, 42K, 50,51V, 56,57Fe, 58Ni, 60Co, 68Zn, 90Zr, 90,94Nb, 93,94,95,96,97,98Mo, 107Cd, 127Te, 132Xe, 148,149Sm, 155Eu, 160,161,162Dy, 166,167,168Er, 171,172Yb, 178Hf, 194Ir, 208Pb, 210Bi, 237U, 238U, 238Np, 239Pu, 242Am; calculated combinatorial nuclear level densities (NLD) using temperature-dependent D1M Gogny interaction. Comparison with experimental data. Z=50, N=50-120; deduced ratio of Maxwellian-averaged (n, γ) rates for T9=1 obtained with current NLDs and those in previous calculations.
doi: 10.1103/PhysRevC.86.064317
2012KO26 Phys.Rev. C 86, 014316 (2012) T.Kondo, H.Utsunomiya, S.Goriely, I.Daoutidis, C.Iwamoto, H.Akimune, A.Okamoto, T.Yamagata, M.Kamata, O.Itoh, H.Toyokawa, Y.-W.Lui, H.Harada, F.Kitatani, S.Hilaire, A.J.Koning Total and partial photoneutron cross sections for Pb isotopes NUCLEAR REACTIONS 206,207,208Pb(polarized γ, n), E=7.0-13.5 MeV; measured En, In, angular distribution of neutrons using 4π neutron detector, total photoneutron σ(E), partial E1 and M1 photoneutron σ(E) for 207,208Pb using quasimonochromatic laser-Compton scattering (LCS) γ rays. Comparison with previous experimental studies, and with theoretical calculations using Hartree-Fock-Bogoliubov with quasiparticle random phase approximation.
doi: 10.1103/PhysRevC.86.014316
2012KO42 Nucl.Data Sheets 113, 2841 (2012) Modern Nuclear Data Evaluation with the TALYS Code System
doi: 10.1016/j.nds.2012.11.002
2012RO02 Nucl.Sci.Eng. 274, 265 (2012) Evaluation and Adjustment of the Neutron-Induced Reactions of 63, 65Cu 63,65Cu(n, n), (n, n'), (n, γ), (n, 2n), E < 200 MeV ; calculated σ, resonance integrals, uncertainties and correlation matrix. TALYS nuclear model code calculations.
doi: 10.13182/NSE11-37
2012RO20 Nucl.Technology 179, 323 (2012) D.Rochman, A.J.Koning, D.F.Da Cruz Propagation of 235, 236, 238U and 239Pu Nuclear Data Uncertainties for a Typical PWR Fuel Element
doi: 10.13182/NT11-61
2011DU27 J.Korean Phys.Soc. 59, 1333s (2011) Exploratory Data Analysis of the EXFOR Database COMPILATION 96Zr(n, γ), E≈2 keV;40Ca(n, t), E≈14-15 MeV;169Tm(n, γ), E=0.001-10 MeV; re-analyzed σ. Old EXFOR entries corrected.
doi: 10.3938/jkps.59.1333
2011DZ01 Nucl.Phys. A858, 1 (2011) N.Dzysiuk, I.Kadenko, A.J.Koning Cross sections for (d-t) neutron interaction with germanium isotopes NUCLEAR REACTIONS 70Ge(n, p), 74Ge(n, α), 70,72,76Ge(n, 2n), E≈14 MeV; measured Eγ, Iγ using activation method; deduced σ, IT-decay σ; calculated σ using TALYS. 70Ge(n, p), E=4-15.5 MeV compared with data and calculations; 72Ge(n, 2n) with JENDL-3.3.
doi: 10.1016/j.nuclphysa.2011.03.011
2011GO05 Phys.Rev. C 83, 034601 (2011) S.Goriely, S.Hilaire, A.J.Koning, R.Capote Towards an improved evaluation of neutron-induced fission cross sections on actinides NUCLEAR REACTIONS 232,233,234,235,236,237,238U(n, F), E=0-30 MeV; 233,234,235,236,238U(n, γ), E=0-20 MeV; 233,235,238U(n, 2n), E=0-20 MeV; 233,234,235,236U(γ, F), E=0-30 MeV; calculated σ using microscopic mean-field calculations, and included in the TALYS reaction analysis code. Comparison with experimental data from EXFOR library; and with evaluated reaction libraries for 233U(n, 2n) and 234U(n, γ) reactions.
doi: 10.1103/PhysRevC.83.034601
2011GO28 J.Korean Phys.Soc. 59, 979s (2011) S.Goriely, S.Hilaire, A.J.Koning, R.Capote Towards Improved Evaluation of Neutron-Induced Fission Cross Section NUCLEAR REACTIONS 232,233,234,235,236,237,238U, 237Np, 238,239,240,241,242Pu(n, f), E=0.01-30 MeV;233,235,236,238U(n, γ), E=0.001-30 MeV;235,236U(γ, f), E=5-30 MeV; calculated σ using microscopic HFB fission paths and HFB plus combinatorial level density, TALYS code. Comparison with EXFOR data.
doi: 10.3938/jkps.59.979
2011HE16 J.Korean Phys.Soc. 59, 1028s (2011) M.Herman, J.Katakura, A.J.Koning, C.Nordborg International Cooperation in Nuclear Data Evaluation
doi: 10.3938/jkps.59.1028
2011HI12 J.Korean Phys.Soc. 59, 767s (2011) S.Hilaire, A.J.Koning, S.Goriely Towards Nuclear Data Evaluations Based on Many Body Theory NUCLEAR REACTIONS 181Ta(γ, n), E=7.5-14 MeV; 89Y(n, n'), (n, 2n), E=0-30 MeV; calculated σ, isomeric state σ; deduced E1 γ-strength function. 235,236U, 237Np, 238,240,241Pu(n, f), E=0.01-25 MeV; calculated σ. TALYS code. Comparison with data.
doi: 10.3938/jkps.59.767
2011KO38 J.Korean Phys.Soc. 59, 773s (2011) Modern Nuclear Data Evaluation: Straight from Nuclear Physics to Applications NUCLEAR REACTIONS 232,233,234,235,236,237,238U(n, f), E=0.1-20 MeV;238,241Pu, 244,245Cm(n, f), E≈0.05-10 MeV; calculated σ, covariances. TALYS code, TMC (Total Monte Carlo) approach. Comparison with data, JEFF-3.1.
doi: 10.3938/jkps.59.773
2011KO40 J.Korean Phys.Soc. 59, 927s (2011) A.Yu.Konobeyev, U.Fischer, A.J.Koning, H.Leeb, S.Leray, Y.Yariv What Can We Expect from the Use of Nuclear Models Implemented in MCNPX at Projectile Energies below 150 MeV? Detailed Comparison with Experimental Data
doi: 10.3938/jkps.59.927
2011KO41 J.Korean Phys.Soc. 59, 935s (2011) A.Yu.Konobeyev, U.Fischer, P.E.Pereslavtsev, A.J.Koning, M.Blann Implementation of the Geometry Dependent Hybrid Model in TALYS NUCLEAR REACTIONS 56Fe(n, n'), E=14.1 MeV;90Zr(p, n), E=160 MeV; calculated σ(En); 56Fe(n, p), E=14.8 MeV; calculated σ(Ep); 58Ni(p, n), (p, p'), (p, d), E=90 MeV; calculated σ(En), σ(Ep), σ(E(deuteron)); 27Al(p, d), (p, α)E=61.7 MeV; calculated σ(Eα), σ(E(deuteron)); 209Bi(p, α), E=90 MeV; calculated σ(Eα). GDH (Geometry-Dependent Hybrid Model) implemented into TALYS code. Comparison with data, ALICE and ALICE/ASH codes.
doi: 10.3938/jkps.59.935
2011KO42 J.Korean Phys.Soc. 59, 1057s (2011) A.J.Koning, E.Bauge, C.J.Dean, E.Dupont, U.Fischer, R.A.Forrest, R.Jacqmin, H.Leeb, M.A.Kellett, R.W.Mills, C.Nordborg, M.Pescarini, Y.Rugama, P.Rullhusen Status of the JEFF Nuclear Data Library COMPILATION Z=1-100(n, X), E=1.E-5 eV-20 MeV; compiled, evaluated activation σ. Z=90, 92-96(n, f), E not given;242,244Cm, 252Cf(SF); compiled, evaluated fission yields, σ. Z=0-111; compiled, evaluated decay data. TALYS code. Also proton data for 26 unspecified isotopes.
doi: 10.3938/jkps.59.1057
2011OH05 J.Korean Phys.Soc. 59, 1817s (2011) A.Ohrn, C.Gustavsson, M.Blann, V.Blideanu, J.Blomgren, S.Chiba, H.Duarte, F.Haddad, C.Kalbach, J.Klug, A.Koning, C.Le brun, C.Lebrun, F.R.Lecolley, X.Ledoux, N.Marie-noury, P.Mermod, L.Nilsson, M.Osterlund, S.Pomp, A.Prokofiev, U.Tippawan, Y.Watanabe Measurements of Inelastic Neutron Scattering at 96 MeV from Carbon, Iron, Yttrium and Lead NUCLEAR REACTIONS 12C, 56Fe, 89Y, 208Pb(n, n'x), E=96 MeV; measured En, In(θ) using SCANDAL (SCAttered Nucleon Detection AssembLy); deduced σ(E, θ), σ(θ); calculated σ(E, θ), σ(θ) using TALYS, QMD, PRECO. Compared with UCLA data at 65 MeV.
doi: 10.3938/jkps.59.1817
2011RO24 Nucl.Sci.Eng. 169, 68 (2011) How to Randomly Evaluate Nuclear Data: A New Data Adjustment Method Applied to 239Pu NUCLEAR REACTIONS 239Pu(n, n), (n, n'), (n, 2n), (n, F), E<20 MeV; calculated σ, fission neutron spectrum, nubar. TALYS calculations, comparison with benchmarks and ENDF/B-VII.0, JEFF-3.1 and JENDL-3.3 evaluated nuclear reaction libraries.
doi: 10.13182/NSE10-66
2011RO44 J.Korean Phys.Soc. 59, 1191s (2011) D.Rochman, A.J.Koning, D.F.Dacruz, S.C.van der Marck Nuclear Data Uncertainty Propagation for a Sodium Fast Reactor NUCLEAR REACTIONS 238U(n, γ), E=0.1-20 MeV;238U(n, n'), 239,240Pu(n, F), E=0-20 MeV; calculated σ using TALYS.
doi: 10.3938/jkps.59.1191
2011RO45 J.Korean Phys.Soc. 59, 1236s (2011) D.Rochman, A.J.Koning, S.C.van der Marck, A.Hogenbirk, D.van Veen Nuclear Data Uncertainty Propagation: Total Monte Carlo vs. Covariances
doi: 10.3938/jkps.59.1236
2011RO46 J.Korean Phys.Soc. 59, 1386s (2011) D.Rochman, A.J.Koning, S.C.van der Marck Exact Nuclear Data Uncertainty Propagation for Fusion Design
doi: 10.3938/jkps.59.1386
2011SA56 J.Korean Phys.Soc. 59, 1195s (2011) P.Sauvan, A.Mayoral, J.Sanz, F.Ogando, M.Garcia, D.Lopez, A.J.Koning, A.Ibarra Computational Tools and Nuclear Data for Radioprotection Studies in Low Energy Light Ions Accelerators NUCLEAR REACTIONS Cu(d, n), E=10, 15, 16, 33 MeV; calculated neutron thick target yields, σ(En, θ=00), σ(θ) using MCUNED (Modified MCNPX) with TENDL-2009 library. Comparison with data.
doi: 10.3938/jkps.59.1195
2011SI17 Phys.Rev. C 84, 014605 (2011) E.Simeckova, P.Bem, M.Honusek, M.Stefanik, U.Fischer, S.P.Simakov, R.A.Forrest, A.J.Koning, J.-C.Sublet, M.Avrigeanu, F.L.Roman, V.Avrigeanu Low and medium energy deuteron-induced reactions on 63, 65Cu nuclei NUCLEAR REACTIONS Cu(d, X)64Cu, E=1.5-19.88 MeV; 63Cu(d, 2n)63Zn, E=4.56-19.49 MeV; 63Cu(d, 3n)62Zn, E=16.44-19.88 MeV; 65Cu(d, p)66Cu, E=4.56-19.49 MeV; 65Cu(d, 2n)65Zn, E=4.25-19.88 MeV; 65Cu(d, 2p)65Ni, E=11.36-19.88 MeV; measured Eγ, Iγ, σ(E), activation method. Comparison with previous experimental data, and with evaluated data files. Cu(d, d), E=11.8, 15, 21.6 MeV; 63,65Cu(d, d), E=12, 34.4 MeV; analyzed σ(θ) data; Cu(d, d), 63,65Cu(d, d), E<60 MeV; analyzed σ(E) data; deduced optical potential model parameters for reaction cross sections. Deuteron breakup mechanism, and direct reaction stripping discussed.
doi: 10.1103/PhysRevC.84.014605
2011TH04 J.Korean Phys.Soc. 59, 1880s (2011) J.C.Thiry, C.Borcea, P.Dessagne, J.C.Drohe, E.Jericha, H.Karam, M.Kerveno, A.J.Koning, A.Negret, A.Pavlik, A.Plompen, C.Rouki, G.Rudolf, M.Stanoiu Measurement of (n, xnγ) Reactions of Interest for the New Nuclear Reactors NUCLEAR REACTIONS 232Th(n, n'), 235U(n, xn), E=0-20 MeV; measured En, In, Eγ, Iγ(θ) using ToF technique at GELINA; deduced σ(Eγ) to specified transitions; calculated σ(Eγ) using TALYS.
doi: 10.3938/jkps.59.1880
2011UT02 Phys.Rev. C 84, 055805 (2011) H.Utsunomiya, S.Goriely, M.Kamata, H.Akimune, T.Kondo, O.Itoh, C.Iwamoto, T.Yamagata, H.Toyokawa, Y.-W.Lui, H.Harada, F.Kitatani, S.Goko, S.Hilaire, A.J.Koning Photoneutron cross sections for 118-124Sn and the γ-ray strength function method NUCLEAR REACTIONS 118,119,120,122,124Sn(γ, n), E=6.78-13 MeV;measured E(n), I(n), σ(E); analyzed γ-strength functions on the basis of the HFB+QRPA model of E1 strength including pygmy dipole resonance. Laser-Compton scattered γ rays.Comparison with previous experimental data, and with evaluated data libraries ENDF/B-VII, JEFF-3.1 and JENDL-4.0.
doi: 10.1103/PhysRevC.84.055805
2010DZ01 Phys.Rev. C 81, 014610 (2010) N.Dzysiuk, I.Kadenko, A.J.Koning, R.Yermolenko Cross sections for fast-neutron interaction with Lu, Tb, and Ta isotopes NUCLEAR REACTIONS 175Lu(n, 2n), (n, p), (n, α), E=13.5-14.6 MeV; 176Lu(n, α)E=13.5-14.6 MeV; 159Tb(n, p), (n, α), (n, n'α), (n, 2n), E=13.5-14.6 MeV; 181Ta(n, γ), E=0.0019, 0.0587, 0.1445, 2.850, 14.340 MeV; measured Eγ, Iγ, σ by activation technique, and isomeric ratios. Natural Lu, Tb and Ta targets. Comparison with values from TALYS-1.0 code.
doi: 10.1103/PhysRevC.81.014610
2010RO01 Nucl.Instrum.Methods Phys.Res. A612, 374 (2010) D.Rochman, A.J.Koning, D.F.da Cruz, P.Archier, J.Tommasi On the evaluation of 23Na neutron-induced reactions and validations COMPILATION 23Na; compiled evaluated nuclear reaction data.
doi: 10.1016/j.nima.2009.10.147
2010TI06 Radiat.Meas. 45, 1134 (2010) U.Tippawan, S.Pomp, J.Blomgren, S.Dangtip, C.Gustavsson, J.Klug, P.Nadel-Turonski, M.Osterlund, L.Nilsson, N.Olsson, O.Jonsson, A.V.Prokofiev, V.Corcalciuc, A.J.Koning, Y.Watanabe Double-differential cross sections and kerma coefficients for light-charged particles produced by 96 MeV neutrons on carbon NUCLEAR REACTIONS C(n, pX), (n, dX), (n, tX), (n, 3HeX), (n, αX)1H/2H/3H/3He/4He, E=96 MeV; measured neutron time of flight, reaction products; deduced σ(θ, E), σ(E), σ. Comparison with GNASH and TALYS calculations.
doi: 10.1016/j.radmeas.2010.06.030
2010UT01 Phys.Rev. C 81, 035801 (2010) H.Utsunomiya, S.Goriely, H.Akimune, H.Harada, F.Kitatani, S.Goko, H.Toyokawa, K.Yamada, T.Kondo, O.Itoh, M.Kamata, T.Yamagata, Y.-W.Lui, S.Hilaire, A.J.Koning Photoneutron cross sections for 96Zr: A systematic experimental study of photoneutron and radiative neutron capture cross sections for zirconium isotopes NUCLEAR REACTIONS 96Zr(γ, n), E=8.1-14 MeV; measured Eγ, Iγ, En, In, σ. Laser Compton-scattered (LCS) beam. Comparisons with previous data and with QRPA and Lorentzian model calculation. 90,91,92,93,94,95,96Zr(n, γ), E=1 keV to 1 MeV; comparison of previous experimental cross sections with calculated values from Hartree-Fock-Bogoliubov (HFB) and quasiparticle random-phase approximation (QRPA).
doi: 10.1103/PhysRevC.81.035801
2010UT02 Phys.Rev. C 82, 064610 (2010) H.Utsunomiya, S.Goriely, H.Akimune, H.Harada, F.Kitatani, S.Goko, H.Toyokawa, K.Yamada, T.Kondo, O.Itoh, M.Kamata, T.Yamagata, Y.-W.Lui, I.Daoutidis, D.P.Arteaga, S.Hilaire, A.J.Koning γ-ray strength function method and its application to 107Pd NUCLEAR REACTIONS 105,106,108Pd(γ, n), E=7.25-15.0 MeV; σ(E) by γ-ray strength function method, Laser-Compton-scattering γ-ray beams. Comparison with evaluated data and several theoretical calculations. 104,105,107Pd(n, γ), E=0-1 MeV; analyzed σ data and comparison with theoretical calculations. Hybrid model and deformed RRPA calculation for γ-strength functions and Hauser-Feshbach (HF) model calculation to provide radiative neutron capture cross for 107Pd(n, γ) reaction.
doi: 10.1103/PhysRevC.82.064610
2009CA27 Nucl.Data Sheets 110, 3107 (2009) R.Capote, M.Herman, P.Oblozinsky, P.G.Young, S.Goriely, T.Belgya, A.V.Ignatyuk, A.J.Koning, S.Hilaire, V.A.Plujko, M.Avrigeanu, O.Bersillon, M.B.Chadwick, T.Fukahori, Z.Ge, Y.Han, S.Kailas, J.Kopecky, V.M.Maslov, G.Reffo, M.Sin, E.Sh.Soukhovitskii, P.Talou RIPL - Reference Input Parameter Library for Calculation of Nuclear Reactions and Nuclear Data Evaluations
doi: 10.1016/j.nds.2009.10.004
2009GO05 Phys.Rev. C 79, 024612 (2009) S.Goriely, S.Hilaire, A.J.Koning, M.Sin, R.Capote Towards a prediction of fission cross sections on the basis of microscopic nuclear inputs NUCLEAR REACTIONS 232Th, 235,236,238U, 238,239,240,241,242Pu, 237Np(n, F), E=0.01-30 MeV; calculated fission σ using global renormalization of barrier heights within the HFB fission path and microscopic nuclear level densities at saddle points. Comparison with experimental data. 234,235,236,237,238,239U, 238,239,240,241,242,243Pu; calculated fission path total energy.
doi: 10.1103/PhysRevC.79.024612
2009RE01 Nucl.Phys. A815, 1 (2009) P.Reimer, A.J.Koning, A.J.M.Plompen, S.M.Qaim, S.Sudar Neutron induced reaction cross sections for the radioactive target nucleus 99Tc NUCLEAR REACTIONS 99Tc(n, n'γ), (n, p), (n, α), E=threshold-20.6 MeV; measured σ using the activation method. Comparison with TALYS and STAPRE calculations.
doi: 10.1016/j.nuclphysa.2008.10.014
2009SE10 Phys.Rev. C 80, 024610 (2009) V.Semkova, P.Reimer, T.Altzitzoglou, A.J.M.Plompen, C.Quetel, S.Sudar, J.Vogl, A.J.Koning, S.M.Qaim, D.L.Smith Neutron activation cross sections on lead isotopes NUCLEAR REACTIONS 204Pb(n, n'γ), (n, 2n), (n, 3n)202mPb/203Pb/203mPb/204mPb, E=14-21 MeV; 206Pb(n, 3n), (n, α)203Hg/204mPb, E=14-21 MeV; 208Pb(n, p)208Tl, E=14-21 MeV; measured Eγ, Iγ and σ. Comparison with TALYS and STAPRE model calculations.
doi: 10.1103/PhysRevC.80.024610
2009TI05 Phys.Rev. C 79, 064611 (2009) U.Tippawan, S.Pomp, J.Blomgren, S.Dangtip, C.Gustavsson, J.Klug, P.Nadel-Turonski, L.Nilsson, M.Osterlund, N.Olsson, O.Jonsson, A.V.Prokofiev, P.-U.Renberg, V.Corcalciuc, Y.Watanabe, A.J.Koning Light-ion production in the interaction of 96 MeV neutrons with carbon NUCLEAR REACTIONS C(n, X)p/d/t/3He/4He, E=96 MeV; measured particle spectra, σ, double differential σ, σ(θ). Comparison with GNASH I calculations.
doi: 10.1103/PhysRevC.79.064611
2009UT01 Phys.Rev. C 80, 055806 (2009) H.Utsunomiya, S.Goriely, M.Kamata, T.Kondo, O.Itoh, H.Akimune, T.Yamagata, H.Toyokawa, Y.-W.Lui, S.Hilaire, A.J.Koning γ-ray strength function for 116, 117Sn with the pygmy dipole resonance balanced in the photoneutron and neutron capture channels NUCLEAR REACTIONS 116,117Sn(γ, n), E=6.80-13.5 MeV; measured neutron spectra and σ using incident beam of laser Compton-scattered (LCS) photons. Comparisons of E1 γ-ray strength functions with previous experimental results and calculations using Hartree-Fock-Bogoliubov plus quasiparticle random-phase approximation (HFB+QRPA) models.
doi: 10.1103/PhysRevC.80.055806
2008AV03 Nucl.Phys. A806, 15 (2008) M.Avrigeanu, S.V.Chuvaev, A.A.Filatenkov, R.A.Forrest, M.Herman, A.J.Koning, A.J.M.Plompen, F.L.Roman, V.Avrigeanu Fast-neutron induced pre-equilibrium reactions on 55Mn and 63, 65Cu at energies up to 40 MeV NUCLEAR REACTIONS 55Mn, 63,65Cu(n, X), (n, γ), E=0.001?50 MeV; 52,53,54Cr, 55Mn, 54,56,57,58Fe, 59Co, 58,60,61,62,64Ni, 63,65Cu, 64,66,68Zn(p, X), (p, n), (p, γ), E=1?20 MeV; analyzed total, activation and capture σ and particle emission spectra using an optical model with emphasis on pre-equilibrium emission. Comparison with all available data.
doi: 10.1016/j.nuclphysa.2008.03.010
2008GO29 Phys.Rev. C 78, 064307 (2008) S.Goriely, S.Hilaire, A.J.Koning Improved microscopic nuclear level densities within the Hartree-Fock-Bogoliubov plus combinatorial method NUCLEAR STRUCTURE A=24-250; calculated nuclear level densities. Hartree-Fock-Bogoliubov model.
doi: 10.1103/PhysRevC.78.064307
2008KO19 Nucl.Phys. A810, 13 (2008) A.J.Koning, S.Hilaire, S.Goriely Global and local level density models NUCLEAR REACTIONS 92Zr(n, γ), (n, 2n), (n, α), E=0-40 MeV; calculated σ. 93Nb(n, xn), E=14 MeV; 197Au(p, xn), E=11 MeV; calculated σ(E'). Comparison of TALYS results with four level density models. NUCLEAR STRUCTURE Z=9-100; A=16-256; calculated/analyzed level densities using four models.
doi: 10.1016/j.nuclphysa.2008.06.005
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