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NSR database version of April 11, 2024.

Search: Author = A.J.Koning

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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2631.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2702.


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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2615.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2640.


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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2614.


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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23255.


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
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2015KO01      Nucl.Data Sheets 123, 207 (2015)

A.J.Koning

Bayesian Monte Carlo Method for Nuclear Data Evaluation

doi: 10.1016/j.nds.2014.12.036
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2015KO22      Eur.Phys.J. A 51, 184 (2015)

A.J.Koning

Bayesian Monte Carlo method for nuclear data evaluation

doi: 10.1140/epja/i2015-15184-x
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23292. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2478.


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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2472.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22991.


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0713.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23204.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2433.


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
Citations: PlumX Metrics


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2385.


2012KO42      Nucl.Data Sheets 113, 2841 (2012)

A.J.Koning, D.Rochman

Modern Nuclear Data Evaluation with the TALYS Code System

doi: 10.1016/j.nds.2012.11.002
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2012RO02      Nucl.Sci.Eng. 274, 265 (2012)

D.Rochman, A.J.Koning

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
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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
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2011DU27      J.Korean Phys.Soc. 59, 1333s (2011)

E.Dupont, A.J.Koning, N.Otuka

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
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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
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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
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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
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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
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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
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2011KO38      J.Korean Phys.Soc. 59, 773s (2011)

A.J.Koning, D.Rochman

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
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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
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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
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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
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2011RO24      Nucl.Sci.Eng. 169, 68 (2011)

D.Rochman, A.J.Koning

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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0653.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2363.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32219.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2179.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2295.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22655.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22680.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14236.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2164.


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
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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
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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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2008MI01      Nucl.Phys. A799, 1 (2008)

L.C.Mihailescu, C.Borcea, A.J.Koning, A.Pavlik, A.J.M.Plompen

High resolution measurement of neutron inelastic scattering and (n, 2n) cross-sections for 209Bi

NUCLEAR REACTIONS 209Bi(n, n'γ), (n, 2nγ), E=threshold - 20 MeV; measured, Eγ, Iγ, En, In, σ, σ(θ). 209Bi deduced level energies, branching ratios. Comparison with existing data and TALYS calculations.

doi: 10.1016/j.nuclphysa.2007.11.007
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22741.


2008MI16      Nucl.Phys. A811, 1 (2008)

L.C.Mihailescu, C.Borcea, P.Baumann, Ph.Dessagne, E.Jericha, H.Karam, M.Kerveno, A.J.Koning, N.Leveque, A.Pavlik, A.J.M.Plompen, C.Quetel, G.Rudolf, I.Tresl

A measurement of (n, xnα) cross sections for 208Pb from threshold up to 20 MeV

NUCLEAR REACTIONS 208Pb(n, n'γ), (n, 2nγ), (n, 3nγ), E=threshold-20 MeV; measured Eγ, Iγ, σ, σ(θ). 208Pb deduced level branching ratios. Comparison with TALYS calculations and other data.

doi: 10.1016/j.nuclphysa.2008.07.016
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23039.


2008RO07      Nucl.Instrum.Methods Phys.Res. A589, 85 (2008)

D.Rochman, A.J.Koning

Pb and Bi neutron data libraries with full covariance evaluation and improved integral tests

NUCLEAR REACTIONS 204,206,207,208Pb, 209Bi(n, γ), (n, n'), E=thermal-200 MeV; analyzed σ. Updated JEFF-3.1 evaluated data files.

doi: 10.1016/j.nima.2008.02.003
Citations: PlumX Metrics


2008UT02      Phys.Rev.Lett. 100, 162502 (2008)

H.Utsunomiya, S.Goriely, T.Kondo, T.Kaihori, A.Makinaga, S.Goko, H.Akimune, T.Yamagata, H.Toyokawa, T.Matsumoto, H.Harano, S.Hohara, Y.-W.Liu, S.Hilaire, S.Peru, A.J.Koning

M1 γ Strength for Zirconium Nuclei in the Photoneuton Channel

NUCLEAR REACTIONS 91,92,94Zr(γ, n), E not given; measured En, In, cross sections. Compared results to model calculations.

doi: 10.1103/PhysRevLett.100.162502
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2115.


2007KO41      Nucl.Sci.Eng. 156, 357 (2007)

A.J.Koning, M.C.Duijvestijn, S.C.van der Marck, R.Klein Meulekamp, A.Hogenbirk

New Nuclear Data Libraries for Lead and Bismuth and Their Impact on Accelerator-Driven Systems Design

NUCLEAR REACTIONS 204,206,207,208Pb, 209Bi(n, X), (p, X), E=0=200 MeV; evaluated and compiled ENDF-6 formatted data libraries.

doi: 10.13182/NSE156-357
Citations: PlumX Metrics


2007MI07      Nucl.Phys. A786, 1 (2007)

L.C.Mihailescu, C.Borcea, A.J.Koning, A.J.M.Plompen

High resolution measurement of neutron inelastic scattering and (n, 2n) cross-sections for 52Cr

NUCLEAR REACTIONS 52Cr(n, n'), (n, 2n), E ≈ 3-18 MeV; measured Eγ, Iγ, σ. Comparison with model predictions.

doi: 10.1016/j.nuclphysa.2007.01.004
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22870.


2006AV01      Nucl.Phys. A765, 1 (2006)

V.Avrigeanu, S.V.Chuvaev, R.Eichin, A.A.Filatenkov, R.A.Forrest, H.Freiesleben, M.Herman, A.J.Koning, K.Seidel

Pre-equilibrium reactions on the stable tungsten isotopes at low energy

NUCLEAR REACTIONS 180,186W(n, 2n), 182,183,184,186W(n, p), (n, α), 186W(n, n'α), E=13.4-14.9 MeV; measured Eγ, Iγ, activation σ. 181Ta(p, n), E=0-50 MeV; 180,182,183,184,186W, 181Ta(n, γ), E=0-3 MeV; analyzed σ. Comparison with model predictions.

doi: 10.1016/j.nuclphysa.2005.10.003
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset41469.


2006GO17      Phys.Rev.Lett. 96, 192501 (2006)

S.Goko, H.Utsunomiya, S.Goriely, A.Makinaga, T.Kaihori, S.Hohara, H.Akimune, T.Yamagata, Y.-W.Lui, H.Toyokawa, A.J.Koning, S.Hilaire

Partial Photoneutron Cross Sections for the Isomeric State 180Tam

NUCLEAR REACTIONS 181Ta(γ, n), E=9.2-12.3 MeV; measured total photoneutron and ground-state σ; deduced partial σ for isomeric state production. Astrophysical implications discussed.

doi: 10.1103/PhysRevLett.96.192501
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0690.


2006KO22      Nucl.Instrum.Methods Phys.Res. B248, 197 (2006)

A.J.Koning, M.C.Duijvestijn

New nuclear data evaluations for Ge isotopes

NUCLEAR REACTIONS 70,72,74,76Ge(n, γ), (n, p), (n, n'), (n, 2n), (n, α), E ≈ 0-20 MeV; compiled, evaluated σ.

doi: 10.1016/j.nimb.2006.04.008
Citations: PlumX Metrics


2006TI04      Phys.Rev. C 73, 034611 (2006)

U.Tippawan, S.Pomp, A.Atac, B.Bergenwall, J.Blomgren, S.Dangtip, A.Hildebrand, C.Johansson, J.Klug, P.Mermod, L.Nilsson, M.Osterlund, N.Olsson, A.V.Prokofiev, P.Nadel-Turonski, V.Corcalciuc, A.J.Koning

Light-ion production in the interaction of 96 MeV neutrons with oxygen

NUCLEAR REACTIONS 16O(n, pX), (n, dX), (n, tX), (n, 3HeX), (n, αX), E=96 MeV; measured particle spectra, σ(E, θ). Comparison with model predictions.

doi: 10.1103/PhysRevC.73.034611
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22923.


2005DE47      Phys.Rev. C 72, 034607 (2005)

P.Demetriou, Ch.Dufauquez, Y.El Masri, A.J.Koning

Light charged-particle production from proton- and α-induced reactions on natSi at energies from 25 to 65 MeV: A theoretical analysis

NUCLEAR REACTIONS Si(p, pX), (p, dX), (p, tX), (p, 3HeX), (p, αX), (α, pX), (α, dX), (α, tX), (α, 3HeX), (α, αX), E=25-65 MeV; measured light charged particle spectra, σ(E, θ); deduced reaction mechanism features. Comparison with model predictions.

doi: 10.1103/PhysRevC.72.034607
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1296.


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