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NSR database version of May 24, 2024.

Search: Author = G.Arbanas

Found 27 matches.

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2023FR01      Ann.Nucl.Energy 181, 109475 (2023)

D.Fritz, Y.Danon, M.Rapp, T.H.Trumbull, M.Zerkle, J.Holmes, C.W.Chapman, G.Arbanas, J.M.Brown, K.Ramic, X.Hu, S.Singh, A.Ney, P.Brain, K.Cook, B.Wang

Total thermal neutron cross section measurements of yttrium hydride from 0.0005 - 3 eV

NUCLEAR REACTIONS 89Y, H(n, X), E=0.0005 - 3 eV; measured reaction products, En, In; deduced total σ and uncertainties. Comparison with ENDF/B-VIII.0library. The RPI LINAC facility.

doi: 10.1016/j.anucene.2022.109475
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2021NO03      Nucl.Data Sheets 173, 1 (2021)

G.P.A.Nobre, M.T.Pigni, D.A.Brown, R.Capote, A.Trkov, K.H.Guber, R.Arcilla, J.Gutierrez, A.Cuadra, G.Arbanas, B.Kos, D.Bernard, P.Leconte

Newly Evaluated Neutron Reaction Data on Chromium Isotopes

NUCLEAR REACTIONS 50,52,53Cr(n, n), (n, γ), (n, X), E<20 MeV; analyzed available data; deduced recommended σ using EMPIRE code within the Hauser-Feshbach framework.

doi: 10.1016/j.nds.2021.04.002
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2019AH05      Phys.Rev. C 100, 044613 (2019)

S.Ahn, D.W.Bardayan, K.L.Jones, A.S.Adekola, G.Arbanas, J.C.Blackmon, K.Y.Chae, K.A.Chipps, J.A.Cizewski, S.Hardy, M.E.Howard, R.L.Kozub, B.Manning, M.Matos, C.D.Nesaraja, P.D.O'Malley, S.D.Pain, W.A.Peters, S.T.Pittman, B.C.Rasco, M.S.Smith, I.Spassova

Direct neutron capture cross section on 80Ge and probing shape coexistence in neutron-rich nuclei

NUCLEAR REACTIONS 2H(80Ge, p), (80Ge, d), E=310 MeV; measured energies and angles of light-ion ejectiles, Ep, Ip, E(d), I(d), (80Ge)p- and (80Ge)d-coin, angular distributions of ejected proton using various silicon detectors at the Holifield Radioactive Ion Beam Facility at ORNL. Proton angular distributions analyzed using adiabatic wave approximation including finite range effects (ADWAFR) using FRESCO code, and by DWBA. 81Ge; deduced levels, J, π, spectroscopic factors, configurations, region of shape coexistence around N≈50. Systematics of low-lying levels in N=49 isotones 81Ge, 83Se, 85Kr and 87Sr. Discussed implications for the magic nature of 78Ni. 80Ge(n, γ), E=0.01-3 MeV; calculated σ(E) for r-process simulations using direct-semidirect (DSD) model and the CUPIDO code.

doi: 10.1103/PhysRevC.100.044613
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2441. Data from this article have been entered in the XUNDL database. For more information, click here.


2019MA26      Phys.Rev. C 99, 041302 (2019); Erratum Phys.Rev. C 99, 069901 (2019)

B.Manning, G.Arbanas, J.A.Cizewski, R.L.Kozub, S.Ahn, J.M.Allmond, D.W.Bardayan, K.Y.Chae, K.A.Chipps, M.E.Howard, K.L.Jones, J.F.Liang, M.Matos, C.D.Nesaraja, F.M.Nunes, P.D.O'Malley, S.D.Pain, W.A.Peters, S.T.Pittman, A.Ratkiewicz, K.T.Schmitt, D.Shapira, M.S.Smith, L.Titus

Informing direct neutron capture on tin isotopes near the N=82 shell closure

NUCLEAR REACTIONS 2H(124Sn, p), (126Sn, p), (128Sn, p), E=630 MeV; measured Ep, Ip, (recoils)p-coin, Q-value spectra, differential σ(θ) using Super Oak Ridge Rutgers University Barrel Array (SuperORRUBA) for light charged particle detection and ionization chamber for detection of beam intensity and recoils at Oak Ridge National Laboratory. 125,127,129Sn; deduced levels, Jπ, L-transfers, spectroscopic factors. 2H(130Sn, p), (132Sn, p); reanalyzed previous experimental data. Angular distribution data compared with Finite Range Adiabatic Wave Approximation. 124,126,128,130,132Sn(n, γ), E=30 keV; calculated direct-semidirect σ(n, γ) from spectroscopic information, and compared with various theoretical predictions. Relevance to r-process abundance calculations.

doi: 10.1103/PhysRevC.99.041302
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14557. Data from this article have been entered in the XUNDL database. For more information, click here.


2019TH03      Eur.Phys.J. A 55, 92 (2019)

I.J.Thompson, R.J.deBoer, P.Dimitriou, S.Kunieda, M.T.Pigni, G.Arbanas, H.Leeb, T.Srdinko, G.Hale, P.Tamagno, P.Archier

Verification of R-matrix calculations for charged-particle reactions in the resolved resonance region for the 7Be system

NUCLEAR REACTIONS 4He(3He, 3He)4He; 6Li(p, α0)3He; 6Li(p, p0)6Li, E* below 8 MeV; calculated σ using different R-code algorithms; compared results and possibilities both for total σ and for the individual l-waves.

doi: 10.1140/epja/i2019-12753-y
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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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2018RA28      Ann.Nucl.Energy 120, 778 (2018)

K.Ramic, C.Wendorff, Y.Cheng, A.I.Kolesnikov, D.L.Abernathy, L.Daemen, G.Arbanas, L.Leal, Y.Danon, L.Liu

Thermal scattering law of (C2H4)n: Integrating experimental data with DFT calculations

NUCLEAR REACTIONS C, H(n, n), E thermal; measured reaction products, En, In; deduced σ(θ, E). Comparison with ENDF/B-VII.1 library.

doi: 10.1016/j.anucene.2018.06.029
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14508.


2015AR02      Nucl.Data Sheets 123, 51 (2015)

G.Arbanas, M.L.Williams, L.C.Leal, M.E.Dunn, B.A.Khuwaileh, C.Wang, H.Abdel-Khalik

Advancing Inverse Sensitivity/Uncertainty Methods for Nuclear Fuel Cycle Applications

doi: 10.1016/j.nds.2014.12.009
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2015ZH13      Phys.Rev. C 91, 045802 (2015)

S.-S.Zhang, J.-P.Peng, M.S.Smith, G.Arbanas, R.L.Kozub

Exploration of direct neutron capture with covariant density functional theory inputs

NUCLEAR REACTIONS 16O, 36S, 48Ca, 132Sn(n, γ), E<3 MeV; calculated σ(E) using nuclear structure information obtained from a covariant density functional theory as input for the FRESCO coupled reaction channels code; investigated impact of pairing, spectroscopic factors, and optical potentials on direct capture cross sections. Comparison with experimental data. Predictions for neutron capture cross sections for unstable nuclei such as 132Sn.

doi: 10.1103/PhysRevC.91.045802
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2014AR06      Nucl.Data Sheets 118, 374 (2014)

G.Arbanas, M.E.Dunn, M.L.Williams

Inverse Sensitivity/Uncertainty Methods Development for Nuclear Fuel Cycle Applications

doi: 10.1016/j.nds.2014.04.084
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2014ES03      Phys.Rev. C 89, 054605 (2014)

J.E.Escher, I.J.Thompson, G.Arbanas, Ch.Elster, V.Eremenko, L.Hlophe, F.M.Nunes

Reexamining surface-integral formulations for one-nucleon transfers to bound and resonance states

NUCLEAR REACTIONS 90Zr(d, p), E=11 MeV; 48Ca(d, p), E=13, 19.3, 56 MeV; 20O(d, p), E=21 MeV; calculated σ(θ, E), interior, surface, and exterior contributions to the transfer reaction for bound states and resonances. Improvements to surface-integral approach. R-matrix theory, and finite range distorted-wave Born approximation (DWBA) calculations using reaction code FRESCO. Comparison with experimental data.

doi: 10.1103/PhysRevC.89.054605
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2014HL01      Phys.Rev. C 90, 061602 (2014)

L.Hlophe, V.Eremenko, Ch.Elster, F.M.Nunes, G.Arbanas, J.E.Escher, I.J.Thompson, for the TORUS Collaboration

Separable representation of proton-nucleus optical potentials

NUCLEAR REACTIONS 12C, 48Ca(p, p), E=38 MeV; 208Pb(p, p), E=45 MeV; calculated S-matrix elements and σ(θ); deduced effects of the short-range Coulomb potential on the proton-nucleus form factor. Comparison with coordinate space calculations. Generalization of the Ernst-Shakin-Thaler (EST) scheme.

doi: 10.1103/PhysRevC.90.061602
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2014TH05      Nucl.Data Sheets 118, 292 (2014)

I.J.Thompson, J.E.Escher, G.Arbanas

Coupled-Channel Models of Direct-Semidirect Capture via Giant-Dipole Resonances

NUCLEAR REACTIONS 208Pb(n, γ), E=1-20 MeV; calculated capture σ using second-order DWBA implemented in FRESSCO and in CUPIDO codes. Compared with data. 130Sn(n, γ), E=0.01-6 MeV; calculated direct-semidirect σ using CUPIDO code with phenomenological optical model potential. Compared with other calculations.

doi: 10.1016/j.nds.2014.04.061
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2014TH06      Nucl.Data Sheets 118, 298 (2014)

I.J.Thompson, G.Arbanas

Coupled-channel Treatment of Isobaric Analog Resonances in (p, p') Capture Processes

NUCLEAR REACTIONS 208Pb(p, p'γ), E=12-20 MeV; calculated proton inelastic σ to specified state, IAR neutron bound state using CC code FRESCO.

doi: 10.1016/j.nds.2014.04.063
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2014UP02      Phys.Rev. C 90, 014615 (2014)

N.J.Upadhyay, V.Eremenko, L.Hlophe, F.M.Nunes, Ch.Elster, G.Arbanas, J.E.Escher, I.J.Thompson

Coulomb problem in momentum space without screening

NUCLEAR REACTIONS 2H(12C, p), E(cm)=30 MeV; 2H(48Ca, p), E(cm)=36 MeV; 2H(208Pb, p), E(cm)=36, 39 MeV; calculated Coulomb-distorted form factors for (d, p) reactions and dependence on charge, angular momentum, and energy. Regularization techniques using a separable interaction derived from realistic nucleon-nucleus optical potential

doi: 10.1103/PhysRevC.90.014615
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2013HL01      Phys.Rev. C 88, 064608 (2013)

L.Hlophe, Ch.Elster, R.C.Johnson, N.J.Upadhyay, F.M.Nunes, G.Arbanas, V.Eremenko, J.E.Escher, I.J.Thompson

Separable representation of phenomenological optical potentials of Woods-Saxon type

NUCLEAR REACTIONS 48Ca, 132Sn, 208Pb(n, X), E=0-50 MeV; calculated partial wave S matrices, separable representations of two-body transition matrix elements and potentials. Ernst-Shakin-Thaler (EST) scheme with CH89 potential.

doi: 10.1103/PhysRevC.88.064608
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2012KO36      Phys.Rev.Lett. 109, 172501 (2012)

R.L.Kozub, G.Arbanas, A.S.Adekola, D.W.Bardayan, J.C.Blackmon, K.Y.Chae, K.A.Chipps, J.A.Cizewski, L.Erikson, R.Hatarik, W.R.Hix, K.L.Jones, W.Krolas, J.F.Liang, Z.Ma, C.Matei, B.H.Moazen, C.D.Nesaraja, S.D.Pain, D.Shapira, J.F.Shriner, Jr., M.S.Smith, T.P.Swan

Neutron Single Particle Structure in 131Sn and Direct Neutron Capture Cross Sections

NUCLEAR REACTIONS 2H(130Sn, p), E=630 MeV; 130Sn(n, γ), E<5 MeV;measured reaction products, Ep, Ip; deduced σ(θ), energy levels, J, π, properties of single-particle states, direct-semidirect σ. Comparison with available data.

doi: 10.1103/PhysRevLett.109.172501
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1953. Data from this article have been entered in the XUNDL database. For more information, click here.


2012LE17      Nucl.Data Sheets 113, 3101 (2012)

L.Leal, K.Guber, D.Wiarda, G.Arbanas, H.Derrien, R.Sayer, N.Larson, M.Dunn

ORNL Resolved Resonance Covariance Generation for ENDF/B-VII.1

NUCLEAR REACTIONS 19F, 58,60Ni, 35,37Cl, 39,41K, 55Mn, 233,235,238U, 239Pu(n, γ), E<20 MeV; analyzed evaluated σ; deduced resonance region covariances. SAMMY code calculations.

doi: 10.1016/j.nds.2012.11.006
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2012ZH37      Phys.Rev. C 86, 032802 (2012)

S.-S.Zhang, M.S.Smith, G.Arbanas, R.L.Kozub

Structures of exotic 131, 133Sn isotopes and effect on r-process nucleosynthesis

NUCLEAR STRUCTURE 131,133Sn; calculated single-particle bound and unbound resonant levels self-consistently by the analytical continuation of the coupling constant method based on a relativistic mean field theory with BCS approximation (RMF+ACCC+BCS); deduced four single-particle bound levels and at most one single-particle level in the effective energy range for neutron captures in the r-process. Relevance to 130Sn(n, γ) capture rate, and synthesis of heavy elements in the r-process in supernovae. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.032802
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2011CH57      Nucl.Data Sheets 112, 2887 (2011)

M.B.Chadwick, M.Herman, P.Oblozinsky, M.E.Dunn, Y.Danon, A.C.Kahler, D.L.Smith, B.Pritychenko, G.Arbanas, R.Arcilla, R.Brewer, D.A.Brown, R.Capote, A.D.Carlson, Y.S.Cho, H.Derrien, K.Guber, G.M.Hale, S.Hoblit, S.Holloway, T.D.Johnson, T.Kawano, B.C.Kiedrowski, H.Kim, S.Kunieda, N.M.Larson, L.Leal, J.P.Lestone, R.C.Little, E.A.McCutchan, R.E.MacFarlane, M.MacInnes, C.M.Mattoon, R.D.McKnight, S.F.Mughabghab, G.P.A.Nobre, G.Palmiotti, A.Palumbo, M.T.Pigni, V.G.Pronyaev, R.O.Sayer, A.A.Sonzogni, N.C.Summers, P.Talou, I.J.Thompson, A.Trkov, R.L.Vogt, S.C.van der Marck, A.Wallner, M.C.White, D.Wiarda, P.G.Young

ENDF/B-VII.1 Nuclear Data for Science and Technology: Cross Sections, Covariances, Fission Product Yields and Decay 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, 7,9Be, 10,11B, C, 14,15N, 16,17O, 19F, 22,23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34,36S, 35,37Cl, 36,38,40Ar, 39,40,41K, 40,42,43,44,46,48Ca, 45Sc, 46,47,48,49,50Ti, 50,51V, 50,52,53,54Cr, 55Mn, 54,56,57,58Fe, 58,59Co, 58,59,60,61,62,64Ni, 63,65Cu, 65,66,67,68,70Zn, 69,71Ga, 70,72,73,74,76Ge, 74,75As, 74,76,77,78,79,80,82Se, 79,81Br, 78,80,82,83,84,85,86Kr, 85,86,87Rb, 84,86,87,88,89,90Sr, 89,90,91Y, 90,91,92,93,94,95,96Zr, 93,94,95Nb, 92,94,95,96,97,98,99,100Mo, 99Tc, 96,98,99,100,101,102,103,104,105,106Ru, 103,105Rh, 102,104,105,106,107,108,110Pd, 107,109,110,111Ag, 106,108,110,111,112,113,114,115,116Cd, 113,115In, 112,113,114,115,116,117,118,119,120,122,123,124,125,126Sn, 121,123,124,125,126Sb, 120,122,123,124,125,126,127,128,129,130,132Te, 127,129,130,131,135I, 123,124,126,128,129,130,131,132,133,134,135,136Xe, 133,134,135,136,137Cs, 130,132,133,134,135,136,137,138,140Ba, 138,139,140La, 136,138,139,140,141,142,143,144Ce, 141,142,143Pr, 142,143,144,145,146,147,148,150Nd, 147,148,149,151Pm, 144,147,148,149,150,151,152,153,154Sm, 151,152,153,154,155,156,157Eu, 152,153,154,155,156,157,158,160Gd, 159,160Tb, 156,158,160,161,162,163,164Dy, 165,166Ho, 162,164,166,167,168,170Er, 168,169,170Tm, 175,176Lu, 174,176,177,178,179,180Hf, 180,181,182Ta, 180,182,183,184,186W, 185,187Re, 191,193Ir, 197Au, 196,198,199,200,201,202,204Hg, 203,205Tl, 204,206,207,208Pb, 209Bi, 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, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), E=30 keV; calculated Maxwellian-averaged σ using ENDF/B-VII.1 evaluated neutron library. Comparison with ENDF/B-VII.0 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, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), (n, F), E=thermal; calculated thermal σ. Comparison with ENDF/B-VII.0, JENDL-4.0 and Atlas of Neutron Resonances values.

doi: 10.1016/j.nds.2011.11.002
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23170.


2011LE37      J.Korean Phys.Soc. 59, 1644s (2011)

L.Leal, H.Derrien, K.Guber, G.Arbanas, D.Wiarda

Evaluation of the Chromium Resonance Parameters Including Resonance Parameter Covariance

NUCLEAR REACTIONS 50,52,53,54Cr(n, γ), (n, X), E=1.E-8-20 keV; calculated thin, thick target capture, total σ, resonance parameters, parameter covariance using R-matrix code SAMMY. Comparison with data.

doi: 10.3938/jkps.59.1644
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2010GU19      Phys.Rev. C 82, 057601 (2010)

K.H.Guber, H.Derrien, L.C.Leal, G.Arbanas, D.Wiarda, P.E.Koehler, J.A.Harvey

Astrophysical reaction rates for 58, 60Ni(n, γ) from new neutron capture cross section measurements

NUCLEAR REACTIONS 58,60Ni(n, γ), E=0.100-600 keV; measured E(n), I(n) using time-of-flight method, Maxwellian-averaged σ in the region of astrophysics. R-matrix analysis. Comparison with evaluated reaction cross section libraries.

doi: 10.1103/PhysRevC.82.057601
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14246.


2008LE25      Nucl.Data Sheets 109, 2868 (2008)

L.C.Leal, G.Arbanas, D.Wiarda, H.Derrien

Resonance Region Covariance Analysis Method and New Covariance Data for 232Th, 233U, 235U, 238U, and 239Pu

doi: 10.1016/j.nds.2008.11.025
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2008LI51      Nucl.Data Sheets 109, 2828 (2008)

R.C.Little, T.Kawano, G.D.Hale, M.T.Pigni, M.Herman, P.Oblozinsky, M.L.Williams, M.E.Dunn, G.Arbanas, D.Wiarda, R.D.McKnight, J.N.McKamy, J.R.Felty

Low-fidelity Covariance Project

doi: 10.1016/j.nds.2008.11.018
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2008WI12      Nucl.Data Sheets 109, 2791 (2008)

D.Wiarda, G.Arbanas, L.Leal, M.E.Dunn

Recent Advances with the AMPX Covariance Processing Capabilities in PUFF-IV

doi: 10.1016/j.nds.2008.11.011
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2007TH15      Phys.Rev. C 76, 044302 (2007)

J.S.Thomas, G.Arbanas, D.W.Bardayan, J.C.Blackmon, J.A.Cizewski, D.J.Dean, R.P.Fitzgerald, U.Greife, C.J.Gross, M.S.Johnson, K.L.Jones, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, D.Shapira, M.S.Smith, D.W.Visser

Single-neutron excitations in neutron-rich 83Ge and 85Se

NUCLEAR REACTIONS 2H(82Ge, p), (84Se, p), E=330, 380 MeV; measured Ep, Ip, recoil-proton-coin, angular distributions; deduced asymptotic normalization coefficients, spectroscopic factors. 83Ge, 85Se; deduced levels, J, π, angular momentum using DWBA analysis. 82Ge, 84Se(n, γ), E=0-1 MeV; calculated cross sections.

doi: 10.1103/PhysRevC.76.044302
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1577. Data from this article have been entered in the XUNDL database. For more information, click here.


1995AR06      Phys.Rev. C51, R1078 (1995)

G.Arbanas, M.B.Chadwick, F.S.Dietrich, A.K.Kerman

Linking of Direct and Compound Chains in Multistep Nuclear Reactions

NUCLEAR REACTIONS 93Nb(n, n'), E=14 MeV; analyzed angle integrated σ data; deduced direct, compound chains linking role on emisssion probabilities. Modified DWBA, multi-step reactions.

doi: 10.1103/PhysRevC.51.R1078
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