NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = J.E.Lynn Found 59 matches. 2020LY02 J.Phys.(London) G47, 045109 (2020) J.E.Lynn, D.Lonardoni, J.Carlson, J.-W.Chen, W.Detmold, S.Gandolfi, A.Schwenk Ab initio short-range-correlation scaling factors from light to medium-mass nuclei NUCLEAR STRUCTURE 2,3H, 3,4,6He, 6Li, 12C, 16O, 40Ca, 63Cu, 56Fe, 197Au; calculated two-nucleon distributions, short-range-correlation(SRC) scaling factors, binding energies from ab initio low-energy nuclear theory.
doi: 10.1088/1361-6471/ab6af7
2019LI17 Phys.Rev. C 99, 044904 (2019) S.H.Lim, J.Carlson, C.Loizides, D.Lonardoni, J.E.Lynn, J.L.Nagle, J.D.Orjuela Koop, J.Ouellette Exploring new small system geometries in heavy ion collisions
doi: 10.1103/PhysRevC.99.044904
2018KL03 Phys.Rev. C 98, 034004 (2018) P.Klos, S.Konig, H.-W.Hammer, J.E.Lynn, A.Schwenk Signatures of few-body resonances in finite volume
doi: 10.1103/PhysRevC.98.034004
2018LO06 Phys.Rev.Lett. 120, 122502 (2018) D.Lonardoni, J.Carlson, S.Gandolfi, J.E.Lynn, K.E.Schmidt, A.Schwenk, X.B.Wang Properties of Nuclei up to A=16 using Local Chiral Interactions NUCLEAR STRUCTURE 6He, 6Li, 12C, 16O; calculated ground-state energies and charge radii, form factors. Continuum quantum Monte Carlo (QMC) method, comparison with available data.
doi: 10.1103/PhysRevLett.120.122502
2018LO09 Phys.Rev. C 97, 044318 (2018) D.Lonardoni, S.Gandolfi, J.E.Lynn, C.Petrie, J.Carlson, K.E.Schmidt, A.Schwenk Auxiliary field diffusion Monte Carlo calculations of light and medium-mass nuclei with local chiral interactions NUCLEAR STRUCTURE 3H, 3,4,6He, 6Li, 12C, 16O; calculated constrained and unconstrained ground state binding energies, charge radii, charge form factors, and Coulomb sum rule by auxilliary field diffusion Monte Carlo (AFDMC) method using AV6' potential in combination with local chiral two- and three-nucleon interactions up to next-to-next-to-leading order; analyzed p-wave n-α elastic scattering phase shifts compared to an R-matrix analysis of experimental data. Comparison with GFMC predictions for Coulomb sum rule.
doi: 10.1103/PhysRevC.97.044318
2018LY03 Phys.Rev. C 97, 064601 (2018) Reexamining the role of the (n, γf) process in the low-energy fission of 235U and 239Pu NUCLEAR REACTIONS 239Pu(n, γF), E=10-110 eV; 239Pu(n, γF), E=0-40 eV; compiled experimental and evaluated (from ENDF/B-VII.1) data for average prompt fission neutron multiplicity; calculated M1 and E1 photon strength functions, reaction widths, prefission γ-ray spectrum and spin- and parity-dependent fission probabilities for 240Pu* using secondary and tertiary vibrational model, resonance parameters. 235U, 239Pu(n, γF), E=0.001-2 MeV; calculated capture and fission σ(E), compound nucleus level density, M1 scissors mode contributions to the total γ strength function. 239Pu(n, F), E=0-210 MeV; 235U(n, F), E=0-100 MeV; calculated average total kinetic energy (TKE) of the fission fragments, and compared with experimental values. 235U(d, pF), 238Pu(t, pF), E*=4.5-6.5 MeV; calculated fission probability. Comparison with experimental values.
doi: 10.1103/PhysRevC.97.064601
2017CH55 Phys.Rev.Lett. 119, 262502 (2017) J.-W.Chen, W.Detmold, J.E.Lynn, A.Schwenk Short-Range Correlations and the EMC Effect in Effective Field Theory NUCLEAR STRUCTURE 3H, 3,4He, 9Be, 12C; calculated scaling factors, parameters. Comparison with available data.
doi: 10.1103/PhysRevLett.119.262502
2017GA10 Phys.Rev.Lett. 118, 232501 (2017) S.Gandolfi, H.-W.Hammer, P.Klos, J.E.Lynn, A.Schwenk Is a Trineutron Resonance Lower in Energy than a Tetraneutron Resonance?
doi: 10.1103/PhysRevLett.118.232501
2017HU17 Phys.Rev. C 96, 054003 (2017) L.Huth, I.Tews, J.E.Lynn, A.Schwenk Analyzing the Fierz rearrangement freedom for local chiral two-nucleon potentials NUCLEAR STRUCTURE 2H, 4He; calculated binding energies, radii, phase-shifts in the framework of Chiral effective field theory (EFT), by constructing leading order (LO) and next-to-leading order (NLO) potentials for all possible LO-operator pairs.Calculated energy of neutron matter at different densities.
doi: 10.1103/PhysRevC.96.054003
2017LY01 Phys.Rev. C 96, 054007 (2017) J.E.Lynn, I.Tews, J.Carlson, S.Gandolfi, A.Gezerlis, K.E.Schmidt, A.Schwenk Quantum Monte Carlo calculations of light nuclei with local chiral two- and three-nucleon interactions NUCLEAR STRUCTURE 2H; calculated deuteron wave functions, binding energy, asymptotic D/S ratio, quadrupole moment, root-mean-square (rms) matter radius, momentum distributions and tensor polarization at N2LO, deuteron energy at LO, NLO, and N2LO as function of radius. 3H, 3,4He; calculated wave functions for AV18+UIX at N22LO, energies using Green's function Monte Carlo (GFMC) method, kinetic and potential energy contributions to the GFMC energy, point-proton radii at LO, NLO, and N2LO, one-body proton and neutron distributions for 3,4He at N2LO, longitudinal charge form factor for 4He. Quantum Monte Carlo (QMC) calculations for light nuclei with local chiral NN and 3N interactions.
doi: 10.1103/PhysRevC.96.054007
2016KL06 Phys.Rev. C 94, 054005 (2016) P.Klos, J.E.Lynn, I.Tews, S.Gandolfi, A.Gezerlis, H.-W.Hammer, M.Hoferichter, A.Schwenk Quantum Monte Carlo calculations of two neutrons in finite volume NUCLEAR STRUCTURE 2n; calculated ground state, energy and nodal surface of the first excited state for a two neutron-system in a box; extracted low-energy S-wave scattering parameters from ground- and excited-state energies for different box sizes using Luscher formula. Auxiliary-field diffusion Monte Carlo (AFDMC) calculations, and chiral EFT interactions. Relevance to effective field theories of strong interaction.
doi: 10.1103/PhysRevC.94.054005
2016LY02 Phys.Rev.Lett. 116, 062501 (2016) J.E.Lynn, I.Tews, J.Carlson, S.Gandolfi, A.Gezerlis, K.E.Schmidt, A.Schwenk Chiral Three-Nucleon Interactions in Light Nuclei, Neutron-α Scattering, and Neutron Matter NUCLEAR STRUCTURE 4He; analyzed available data; deduced binding and ground-state energies. Quantum Monte Carlo calculations of light nuclei using local two- and three-nucleon (3N) interactions derived from chiral effective field theory up to next-to-next-to-leading order (N2LO).
doi: 10.1103/PhysRevLett.116.062501
2014BO14 Nucl.Data Sheets 118, 211 (2014) The Impact of Intermediate Structure on the Average Fission Cross Sections NUCLEAR REACTIONS 239,240Pu(n, F), E not given; calculated width fluctuation correction factor, average fission σ using Porter-Thomas hypothesis within Monte Carlo R-matrix.
doi: 10.1016/j.nds.2014.04.039
2014LY02 Phys.Rev.Lett. 113, 192501 (2014) J.E.Lynn, J.Carlson, E.Epelbaum, S.Gandolfi, A.Gezerlis, A.Schwenk Quantum Monte Carlo Calculations of Light Nuclei Using Chiral Potentials NUCLEAR STRUCTURE 3,4He, 2,3H; calculated one- and two-body proton distributions, nuclear radii, binding energies; deduced the necessity of a three-body force.
doi: 10.1103/PhysRevLett.113.192501
2014NA29 Phys.Rev.Lett. 113, 112301 (2014) J.L.Nagle, A.Adare, S.Beckman, T.Koblesky, J.Orjuela Koop, D.McGlinchey, P.Romatschke, J.Carlson, J.E.Lynn, M.McCumber Exploiting Intrinsic Triangular Geometry in Relativistic He3+Au Collisions to Disentangle Medium Properties
doi: 10.1103/PhysRevLett.113.112301
2013BO29 Phys.Rev. C 88, 054612 (2013); Erratum Phys.Rev. C 101, 039901 (2020) R-matrix analysis and prediction of low-energy neutron-induced fission cross sections for a range of Pu isotopes NUCLEAR REACTIONS 236,237,238,239,240,241,242,243,244Pu(n, F), 236,240,241,243Pu(n, γ), 236,243Pu(n, n'), E=0.005-5 MeV; calculated σ(E). 237,238,239,240,241,242,243,244,245Pu; calculated inner and outer fission barrier heights, neutron and proton pairing gaps. Hauser-Feshbach statistical theory, and fission decay channel in the R-matrix formalism. Comparison with several previous theoretical and empirical calculations and evaluated data libraries. 243Pu predicted to be fissile in contrast to data in ENDF/B-VII.1 and JEFF-3.1.2 evaluated libraries. Discussed level spacing distributions.
doi: 10.1103/PhysRevC.88.054612
2012LY01 Phys.Rev. C 86, 014324 (2012) Real-space imaginary-time propagators for non-local nucleon-nucleon potentials
doi: 10.1103/PhysRevC.86.014324
2011BO25 J.Korean Phys.Soc. 59, 833s (2011) O.Bouland, G.M.Hale, J.E.Lynn, P.Talou, D.Bernard, O.Litaize, G.Noguere, C.De saint Jean, O.Serot Towards Consistent Nuclear Models and Comprehensive Nuclear Data Evaluations NUCLEAR REACTIONS 12C(n, X), E=0-6.5 MeV; analyzed σ using R matrix; deduced resonance widths. A=60-175(n, n'), E not given; calculated average prompt neutron multiplicity.
doi: 10.3938/jkps.59.833
2011TA21 J.Korean Phys.Soc. 59, 797s (2011) P.Talou, T.Kawano, J.E.Lynn, P.Moller, O.Bouland, M.B.Chadwick Recent Advances in Nuclear Fission Theory: Pre- and Post-Scission Physics NUCLEAR REACTIONS 239,240,241,242Pu(n, f), E≈0.01-20 MeV; calculated σ using R-matrix formalism in Bjornholm-Lynn model. 235U(n, f), E=thermal, 0.5 MeV; calculated prompt fission neutron multiplicity using Monte Carlo Hauser-Feshbach; compared to data, ENDF/B-VII.0.
doi: 10.3938/jkps.59.797
2009KA24 Phys.Rev. C 80, 024611 (2009) T.Kawano, P.Talou, J.E.Lynn, M.B.Chadwick, D.G.Madland Calculation of nuclear reaction cross sections on excited nuclei with the coupled-channels method NUCLEAR REACTIONS 169Tm(n, n), (n, n'), (n, γ), (n, X), E<20 MeV; calculated σ. 239Pu(n, X), E=0.01-10 MeV; calculated fission σ. Coupled-channels and statistical Hauser-Feshbach model calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.024611
2004RA23 Phys.Rev. C 70, 044318 (2004) S.Raman, X.Ouyang, M.A.Islam, J.W.Starner, E.T.Jurney, J.E.Lynn, G.Martinez-Pinedo Thermal-neutron capture by 58Ni, 59Ni, and 60Ni NUCLEAR REACTIONS 58,59,60Ni(n, γ), E=thermal; measured Eγ, Iγ, σ. 59,60,61Ni deduced levels, J, π, neutron separation energies. Comparison with shell-model predictions.
doi: 10.1103/PhysRevC.70.044318
2003LY02 Phys.Rev. C 67, 014607 (2003) Theoretical evaluations of the fission cross section of the 77 eV isomer of 235U NUCLEAR REACTIONS 235U(n, F), E < 2 MeV; calculated fission σ for ground and isomeric states. 235U(n, n'), (n, γ), E < 2 MeV; calculated capture and inelastic σ. 237U, 239Pu(n, F), E < 2 MeV; calculated fission σ. Comparisons with data.
doi: 10.1103/PhysRevC.67.014607
2002BL08 Phys.Rev. C65, 045801 (2002) J.C.Blackmon, S.Raman, J.K.Dickens, R.M.Lindstrom, R.L.Paul, J.E.Lynn Thermal-Neutron Capture by 208Pb NUCLEAR REACTIONS 206,207,208Pb(n, γ), E=subthermal; measured Eγ, Iγ, σ. 209Pb deduced levels, J, π, neutron separation energy. Direct capture model, astrophysical s process.
doi: 10.1103/PhysRevC.65.045801
2000RA14 Phys.Rev. C61, 067303 (2000) S.Raman, E.T.Jurney, J.W.Starner, J.E.Lynn Direct Thermal-Neutron Capture by 30Si NUCLEAR REACTIONS 30Si(n, γ), E=thermal; calculated σ(E). Direct capture theory, input data from (d, p) reaction, comparison with data.
doi: 10.1103/PhysRevC.61.067303
1997JU02 Phys.Rev. C56, 118 (1997) E.T.Jurney, J.W.Starner, J.E.Lynn, S.Raman Thermal-Neutron Capture by 14N NUCLEAR REACTIONS 14N(n, γ), E=thermal; measured Eγ, Iγ; deduced capture σ(E). 15N deduced resonances, width parameters. Other data input.
doi: 10.1103/PhysRevC.56.118
1996RA04 Phys.Rev. C53, 616 (1996) S.Raman, E.K.Warburton, J.W.Starner, E.T.Jurney, J.E.Lynn, P.Tikkanen, J.Keinonen Spectroscopy of 20F Levels NUCLEAR REACTIONS 19F(n, γ), E=thermal; measured Eγ, Iγ. 20F deduced levels, J, π, γ-branching ratios, spectroscopic strengths, γ multipolarity. Other reaction data input.
doi: 10.1103/PhysRevC.53.616
1994PA02 Phys.Rev. C49, 672 (1994) W.E.Parker, J.E.Lynn, G.L.Morgan, P.W.Lisowski, A.D.Carlson, N.W.Hill Intermediate Structure in the Neutron-Induced Fission Cross Section of 236U NUCLEAR REACTIONS 236U(n, F), E=5 eV-100 keV; measured fission σ, resonance fission widths; deduced intermediate resonance structure. 237U deduced fission barrier parameters.
doi: 10.1103/PhysRevC.49.672
1993MO10 Phys.Rev. C48, 553 (1993) M.C.Moxon, J.A.Harvey, S.Raman, J.E.Lynn, W.Ratynski Neutron Resonance Parameters and Thermal-Neutron Capture by 43Ca NUCLEAR REACTIONS 43Ca(n, X), E=0.005-500 keV; measured transmission. 44Ca deduced resonances, J, Γn.
doi: 10.1103/PhysRevC.48.553
1992RA19 Phys.Rev. C46, 972 (1992) S.Raman, E.T.Jurney, J.W.Starner, J.E.Lynn Thermal-Neutron Capture by Silicon Isotopes NUCLEAR REACTIONS 28,29,30Si(n, γ), E=thermal; measured Eγ, Iγ following capture; deduced σ. 29,30,31Si deduced neutron separation energies, transition γ-multipolarity. Direct capture interpretation.
doi: 10.1103/PhysRevC.46.972
1992WA06 Phys.Rev. C45, 1597 (1992) T.A.Walkiewicz, S.Raman, E.T.Jurney, J.W.Starner, J.E.Lynn Thermal-Neutron Capture by Magnesium Isotopes NUCLEAR REACTIONS 24,25,26Mg(n, γ), E=thermal; measured Eγ, Iγ; deduced capture σ. 26,27,25Mg deduced levels, neutron separation energies, γ-multipolarity. Direct capture theory.
doi: 10.1103/PhysRevC.45.1597
1991LY01 Phys.Rev. C44, 764 (1991) Direct and Valence Neutron Capture by 7Li NUCLEAR REACTIONS 7Li(n, γ), E=thermal; measured Eγ, Iγ, capture σ. Direct, valence capture.
doi: 10.1103/PhysRevC.44.764
1991RA11 Phys.Rev. C44, 518 (1991) S.Raman, J.A.Fernandez-Baca, R.M.Moon, J.E.Lynn Thermal-Neutron Scattering Length and Capture by 46Ca NUCLEAR REACTIONS 46Ca(n, n), E=thermal; measured neutron spectra; deduced coherent scattering amplitude, capture σ, mechanism.
doi: 10.1103/PhysRevC.44.518
1990LY01 At.Data Nucl.Data Tables 44, 191 (1990) Resonance Effects in Neutron Scattering Lengths of Rare-Earth Nuclides NUCLEAR REACTIONS Sm, Eu, Gd, Er, Yb, 149Sm, 151Eu, 155,157Gd, 164Dy, 167Er, 168,174Yb, 176Lu(n, n), E=0.01-0.5 eV; analyzed data; deduced coherent scattering lengths. Generalized single-level formalism.
doi: 10.1016/0092-640X(90)90013-A
1990RA03 Phys.Rev. C41, 458 (1990) S.Raman, M.Igashira, Y.Dozono, H.Kitazawa, M.Mizumoto, J.E.Lynn Valence Capture Mechanism in Resonance Neutron Capture by 13C NUCLEAR REACTIONS 13C(n, γ), E=resonance; measured Eγ, Iγ. 14C levels deduced partial, total Γγ. Valence capture mechanism.
doi: 10.1103/PhysRevC.41.458
1989RA06 Phys.Rev. C39, 1297 (1989) S.Raman, S.Kahane, R.M.Moon, J.A.Fernandez-Baca, J.L.Zarestky, J.E.Lynn, J.W.Richardson, Jr. Thermal-Neutron Scattering Lengths and Capture by Even Calcium Isotopes NUCLEAR REACTIONS 40,42,43,44,48Ca(n, n), E=thermal; measured Bragg diffration patterns; deduced thermal neutron scattering lengths. 40,42,43,44,48Ca(n, γ), E=thermal; analyzed σ(E(γ)). Lane-Lynn-Raman model.
doi: 10.1103/PhysRevC.39.1297
1989SU13 Nucl.Sci.Eng. 103, 37 (1989) M.Sugimoto, P.T.Guenther, J.E.Lynn, A.B.Smith, J.F.Whalen The Interaction of Fast Neutrons with Beryllium NUCLEAR REACTIONS 9Be(n, n), E=1-10 MeV; measured σ(E), σ(θ). 9Be(n, n'), E=4.5-10 MeV; measured σ(θ); deduced angle-integrated σ.
doi: 10.13182/NSE89-A23658
1988RA10 J.Phys.(London) G14, Supplement S223 (1988) Direct Thermal Neutron Capture NUCLEAR REACTIONS 9Be, 12,13C, 24,25,26Mg, 32,34,33S, 40,44Ca(n, γ), E=slow; calculated capture σ.
doi: 10.1088/0305-4616/14/S/024
1987KA28 Phys.Rev. C36, 533 (1987) Analysis of Primary Electric Dipole Gamma Rays from Slow-Neutron Capture by Ca Isotopes NUCLEAR REACTIONS 40,42,44,46,48Ca(n, γ), E=thermal; calculated direct capture σ. 41,43,45,47,49Ca deduced resonance parameters. Optical model.
doi: 10.1103/PhysRevC.36.533
1987LY01 Phys.Rev. C35, 26 (1987) Analysis of Slow Neutron Capture by 9Be, 12C, and 13C NUCLEAR REACTIONS 9Be, 12,13C(n, γ), E=thermal; calculated capture σ. Optical model, Lane-Lynn-Raman method.
doi: 10.1103/PhysRevC.35.26
1987LY03 Phys.Rev. C36, 671 (1987) Coriolis Interaction and Variable Reflection Asymmetry in Fission Vibrational Resonances NUCLEAR REACTIONS 230Th(n, F), E=0.69-0.75 MeV; analyzed fission σ(E), fragment angular anisotropy vs E. Vibrational model.
doi: 10.1103/PhysRevC.36.671
1985RA15 Phys.Rev. C32, 18 (1985) S.Raman, R.F.Carlton, J.C.Wells, E.T.Jurney, J.E.Lynn Thermal Neutron Capture Gamma Rays from Sulfur Isotopes: Experiment and theory NUCLEAR REACTIONS 34,33,32,36S(n, γ), E=thermal; measured Eγ, Iγ; deduced model dependent effects. 33,34,35,37S deduced levels, γ-branching, J, π, E1 transition. Potential capture theory.
doi: 10.1103/PhysRevC.32.18
1983LY02 J.Phys.(London) G9, 665 (1983) The Concept of Vibrational Resonances Associated with the Secondary and Tertiary Wells of a Multi-Humped Fission Barrier NUCLEAR REACTIONS 230,232,228Th, 231Pa(n, F), E not given; calculated vibrational resonances, fission strengths. Secondary, tertiary wells, multi-humped fission barrier. Single particle, vibrational motion coupling.
doi: 10.1088/0305-4616/9/6/011
1980BJ02 Rev.Mod.Phys. 52, 725 (1980) The Double-Humped Fission Barrier NUCLEAR STRUCTURE A=231-245; analyzed resonance structure, fission data; deduced fission features. Double-humped fission barrier concept.
doi: 10.1103/RevModPhys.52.725
1980LY01 J.Phys.(London) G6, 1271 (1980) Line-Fitting Procedures for Intermediate Structure NUCLEAR REACTIONS, Fission 237Np, 238Pu, 234U(n, F), E=slow; analyzed fine structure underlying intermediate resonances. 238Np, 239Pu, 235U resonances deduced spreading widths. Basic Lorentzian line fitting procedure.
doi: 10.1088/0305-4616/6/10/014
1974LY01 J.Phys.(London) A7, 395 (1974) Sub-Barrier Fission Probability for a Double-Humped Barrier NUCLEAR REACTIONS 240Pu(t, nF), 236U(3He, dF), 237Np(d, pF); measured nothing, calculated σ.
doi: 10.1088/0305-4470/7/3/011
1972JA11 Nucl.Phys. A189, 225 (1972) G.D.James, J.E.Lynn, L.G.Earwaker Nuclear Spectroscopy of Highly Deformed 231Th NUCLEAR REACTIONS 230Th(n, F), En=625 keV-1.4 MeV; measured σ(E, θ(fragment)). 231Th deduced moment of inertia in shape isomeric state.
doi: 10.1016/0375-9474(72)90292-8
1971BR39 Phys.Rev. C4, 1444 (1971) H.C.Britt, S.C.Burnett, B.H.Erkkila, J.E.Lynn, W.E.Stein Systematics of Spontaneously Fissioning Isomers RADIOACTIVITY, Fission 235m,237m,238m,239m,240m,241mPu, 241m,242m,243m,244m,245mCm, 236mU, 239m,240m,242m,243m,244mAm(SF); measured T1/2, T1/2 lower limits. NUCLEAR REACTIONS 233,235,236,238U, 237Np, 239,240,242,244Pu(α, xn), E=20-29 MeV; 235U, 237Np, 239,240,242,244Pu, 243Am(d, p), (d, np), E=20-29 MeV; measured isomeric σ ratios(E); deduced thresholds for SF-isomer production.
doi: 10.1103/PhysRevC.4.1444
1966CU04 Nucl.Phys. 84, 49 (1966) J.G.Cuninghame, K.Fritze, J.E.Lynn, C.B.Webster The Ratio Of Asymmetric To Symmetric Fission In Fission Of 239Pu By Neutrons Of Energies From 30 Kev To 14.7 Mev NUCLEAR REACTIONS 239Pu(n, f), E=30 keV-14.7 MeV; measured products, 111Ag, 99Mo, 113Ag; deduced yields. Data were imported from EXFOR entry 22053.
doi: 10.1016/0029-5582(66)90432-9
1963FI03 Nucl.Phys. 41, 614 (1963) F.W.K.Firk, J.E.Lynn, M.C.Moxon Resonance Parameters of the Neutron Cross Section of U238 NUCLEAR STRUCTURE 238U; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90541-8
1963FI06 Nucl.Phys. 44, 431 (1963) F.W.K.Firk, J.E.Lynn, M.C.Moxon Resonances in the Neutron Cross Section of Bismuth NUCLEAR STRUCTURE 210Bi; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90036-1
1963FI11 Proc.Phys.Soc.(London) 82, 477 (1963) F.W.K.Firk, J.E.Lynn, M.C.Moxon Analysis and Interpretation of the Neutron Cross Section of Vanadium below 25 keV NUCLEAR STRUCTURE 52V; measured not abstracted; deduced nuclear properties.
doi: 10.1088/0370-1328/82/4/301
1962JA15 Phys.Rev. 127, 461 (1962) Resonant Absorption Of Neutrons By Crystals NUCLEAR REACTIONS Os(n, n), Os(n, x), U(n, n), U(n, x), E=6.65-6.71 eV; measured products; deduced resonance parameters. Data were imported from EXFOR entry 11373.
doi: 10.1103/PhysRev.127.461
1961LY01 Bull.Am.Phys.Soc. 6, No.1, 70, X9 (1961) NUCLEAR STRUCTURE 52V; measured not abstracted; deduced nuclear properties.
1960FI06 Proc.Intern.Conf.Nuclear Structure, Kingston, Canada, D.A.Bromley, E.W.Vogt, Eds., Univ.Of Toronto Press, p.757 (1960) F.W.K.Firk, J.E.Lynn, M.C.Moxon Parameters of Neutron Resonances in U238 + n up to 1.8 keV NUCLEAR STRUCTURE 239U; measured not abstracted; deduced nuclear properties.
1960LA05 Nuclear Phys. 17, 586 (1960) Anomalous Radiative Capture in the Neutron Resonance Region: Analysis of the experimentatl data on electric dipole transitions NUCLEAR STRUCTURE 208Pb, 207Pb, 56Mn, 41Ca, 40K; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90147-4
1959FI33 Bull.Am.Phys.Soc. 4, No.1, 34, M4 (1959) F.W.K.Firk, M.C.Moxon, J.E.Lynn Neutron Total Cross Sections of Vanadium, Cobalt, and Bismuth from 3 to 30 keV Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21277. 1958LY03 Nuclear Phys. 5, 603 (1958) J.E.Lynn, F.W.K.Firk, M.C.Moxon The 2.85 keV Neutron Resonance of Sodium
doi: 10.1016/0029-5582(58)90059-2
1958LY63 Nuclear Phys. 7, 613 (1958) J.E.Lynn, M.C.Moxon, F.W.K.Firk The Low Energy Neutron Resonances of Bismuth
doi: 10.1016/0029-5582(58)90299-2
1958RA06 Nuclear Phys. 5, 89 (1958) E.R.Rae, E.R.Collins, B.B.Kinsey, J.E.Lynn, E.R.Wiblin Analyses of Slow Neutron Resonances in Silver
doi: 10.1016/0029-5582(58)90010-5
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