NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = F.W.Firk Found 37 matches. 2014FI07 Int.J.Mod.Phys. E23, 1450009 (2014) From resonances to fluctuations: A microscopic analysis of the cross-section for inelastic neutron scattering to a definite state
doi: 10.1142/S0218301314500098
1995FI06 J.Phys.(London) G21, 1341 (1995) Differential Polarization of Photoneutron from 16O NUCLEAR REACTIONS 16O(γ, n), E=20-26 MeV bremsstrahlung; measured polarization vs (En, θ); deduced polarization coefficients B(k), amplitudes, phase of reaction matrix elements. Time-of-flight spectromerter, spin-precession solenoid, liquid He and 12C polarimeters. Comparison with results of 15N(p, γ0)16O studies, model predictions.
doi: 10.1088/0954-3899/21/10/008
1991FI08 J.Phys.(London) G17, 1739 (1991) A Study of M1, E1 and E2 Strengths in 16O Below 25 MeV NUCLEAR REACTIONS 16O(γ, n), E=17-25 MeV; measured σ(θ=90°), polarization (θ=90°); deduced photoneutron to photoproton ratio. 16O resonances deduced Γ, Γγ, M1, E1, E2 transition features. Tof, 12C polarimeter. Self-consistent RPA, direct reaction calculations.
doi: 10.1088/0954-3899/17/11/019
1981CH12 Nucl.Phys. A364, 43 (1981) The Polarization and Differential Cross Section of Fast Neutrons Scattered from 6Li and an R-Function Analysis of the Interaction below 4 MeV NUCLEAR REACTIONS 6Li(n, n), (polarized n, n), E=2-4 MeV; measured A(E, θ), σ(Eθ). 7Li resonances deduced Γ, J, π. Enriched target. Reduced R-function analysis.
doi: 10.1016/0375-9474(81)90432-2
1977BO24 Nucl.Phys. A287, 317 (1977) Determination of R-Function and Physical-State Parameters for n-4He Elastic Scattering below 21 MeV NUCLEAR REACTIONS 4He(n, n), (polarized n, n), (n, X); analyzed data, σ(θ), A(θ). R-function analysis.
doi: 10.1016/0375-9474(77)90499-7
1976BO05 Nucl.Phys. A258, 189 (1976) The Polarization of MeV Neutrons Elastically Scattered from 4He NUCLEAR REACTIONS 4He(polarized n, n), E=1.5-6.0 MeV, θlab=20°-80°; measured A(E, θ). Liquid helium target.
doi: 10.1016/0375-9474(76)90001-4
1975HO01 Nucl.Phys. A237, 111 (1975) R.J.Holt, F.W.K.Firk, G.T.Hickey, R.Nath Experimental and Theoretical Studies of the Elastic Scattering of Polarized Neutrons from 6Li NUCLEAR REACTIONS 6Li(polarized n, n), E=2-5 MeV; measured A(E, θ). 7Li levels deduced level-width. R-matrix analysis also includes 6Li(n, α) channel. Enriched target.
doi: 10.1016/0375-9474(75)90466-2
1974HI04 Nucl.Phys. A225, 470 (1974) G.T.Hickey, F.W.K.Firk, R.J.Holt, R.Nath R-Matrix and Phase-Shift Analyses of Neutron Polarization Measurements From n-16O Scattering NUCLEAR REACTIONS 16O(n, n), E=1-4 MeV; calculated σ(E, θ), σ(E), P(n)(E, θ).
doi: 10.1016/0375-9474(74)90354-6
1974SE06 Nucl.Sci.Eng. 53, 415 (1974) A Study of the 2.8-keV Neutron Resonance of Sodium and an Analysis of the Total Neutron Cross Section up to 50 keV NUCLEAR REACTIONS 23Na(n, X); measured σ(E). 24Na deduced level-width, resonance, J.
doi: 10.13182/NSE74-A23372
1973HI09 Phys.Lett. 47B, 348 (1973) G.T.Hickey, F.W.K.Firk, R.J.Holt, R.Nath, H.L.Schultz Polarization of Neutrons Elastically Scattered from 16O NUCLEAR REACTIONS 16O(n, n), E=1-4 MeV; measured σ(E), n-polarization.
doi: 10.1016/0370-2693(73)90620-5
1973HO39 Nucl.Phys. A213, 147 (1973) R.J.Holt, F.W.K.Firk, R.Nath, H.L.Schultz The Absolute Polarization of Neutrons from n-12C Scattering NUCLEAR REACTIONS 12C(n, n), E=2 to 5 MeV; θ(lab)=20° to 150°; measured P(E, θ); R-function, phase-shift analyses.
doi: 10.1016/0375-9474(73)90189-9
1972BE06 Nucl.Phys. A179, 791 (1972) B.L.Berman, F.W.K.Firk, C.-P.Wu The 90° Differential Cross Section for the Reaction 4He(γ, n0)3He and Evidence for Isospin Mixing in the Dipole States of 4He NUCLEAR REACTIONS 4He(γ, n0), E < 35 MeV; measured σ(E;En). 4He dipole states deduced isospin mixing.
doi: 10.1016/0375-9474(72)90620-3
1972HO01 Phys.Rev.Lett. 28, 114 (1972) R.J.Holt, F.W.K.Firk, R.Nath, H.L.Schultz Polarization of Neutrons in n-12C Scattering: A Standard for Polarization Studies in the MeV Region NUCLEAR REACTIONS 12C(n, n), E=2-5 MeV; measured P(E;θ=50°).
doi: 10.1103/PhysRevLett.28.114
1972NA03 Nucl.Instrum.Methods 98, 385 (1972) R.Nath, F.W.K.Firk, R.J.Holt, H.L.Schultz Polarization Studies Using the Neutron Spin-Precession Method with a Continuous Energy Spectrum of Neutrons NUCLEAR REACTIONS 16O(γ, n), E < 63 MeV; measured P(n)(En). 12C(n, n), E=5.5-12.5 MeV; measured analyzing power(E).
doi: 10.1016/0029-554X(72)90220-0
1972NA15 Nucl.Phys. A194, 49 (1972) R.Nath, F.W.K.Firk, H.L.Schultz Differential Polarization of Photoneutrons from Deuterium NUCLEAR REACTIONS 2H(γ, n), Eγ=7-30 MeV; measured polarization P(En, θ). Unpolarized photons, unpolarized targets. 4He, 12C polarization analysers.
doi: 10.1016/0375-9474(72)91051-2
1970WU01 Nucl.Phys. A147, 19 (1970) C.-P.Wu, F.W.K.Firk, T.W.Phillips A Study of the Giant Dipole States of 28Si, 32S and 40Ca NUCLEAR REACTIONS 28Si, 32S, 40Ca(γ, n0), Eγ = 16-24 MeV; measured σ(En, θ = 90°). Natural targets.
doi: 10.1016/0375-9474(70)90506-3
1970WU02 Phys.Lett. 32B, 675 (1970) C.P.Wu, F.W.K.Firk, B.L.Berman Evidence for Isospin Splitting of the Giant Dipole State in 26Mg NUCLEAR REACTIONS 26Mg(γ, n), E < 28 MeV; measured σ(E;En). 26Mg deduced T-splitting of giant dipole resonance.
doi: 10.1016/0370-2693(70)90441-7
1969CO15 Phys.Letters 30B, 91 (1969) G.W.Cole, Jr., F.W.K.Firk, T.W.Phillips Polarization Studies of the 16O(γ, N)15O Reaction NUCLEAR REACTIONS 16O(γ, n), E < 30, 60 MeV; measured σ(E;En), P(n).
doi: 10.1016/0370-2693(69)90405-5
1969WU02 Phys.Letters 29B, 359 (1969) C.-P.Wu, J.E.E.Baglin, F.W.K.Firk, T.W.Phillips Correlations in the Energies and Widths of Structure Observed in the Reactions 40Ca(γ, n0)39Ca and 40Ca(γ, p0)39K NUCLEAR REACTIONS 40Ca(γ, n0), (γ, p0), E < 24 MeV; measured σ(E); deduced intermediate structure correlations.
doi: 10.1016/0370-2693(69)90384-0
1968WU01 Phys.Rev.Letters 20, 1182 (1968) C.-P.Wu, F.W.K.Firk, T.W.Phillips Energy Dependence of Isospin Mixing in the Giant-Dipole States of C12 and O16 NUCLEAR STRUCTURE 12C, 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.20.1182
1965MC08 Can.J.Phys. 43, 2156 (1965) K.G.McNeill, D.B.McConnell, F.W.K.Firk The Angular Distribution of 5.6-MeV Gamma Rays from the Capture by 124Sn of 62-eV Neutrons NUCLEAR STRUCTURE 125Sn; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p65-210
1964FI03 Nucl.Phys. 52, 437 (1964) Energy Spectra of Photoneutrons from the Reactions O16(γ, n), S32(γ, n) and Ca40(γ, n) NUCLEAR STRUCTURE 32S, 40Ca, 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90705-9
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
1962FI04 Phys.Rev.Letters, 8, 321 (1962) Energy Spectrum of Photoneutrons from the Reaction O16(γ, n)O15 NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.8.321
1962FI07 Conf.Low Energy Nuclear Phys. Harwell, AERE-R-4131, 11, 4.2 (September 1962) NUCLEAR STRUCTURE 10B; measured not abstracted; deduced nuclear properties.
1961FI03 Bull.Am.Phys.Soc. 6, No.3, 252, H7 (1961) Spectra of γ Rays from Capture of (30 ± 10) keV Neutrons
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.
1959BI09 Nuclear Phys. 13, 525 (1959) J.R.Bird, M.C.Moxon, F.W.K.Firk Gamma Ray Spectra and Parameters of Neutron Resonances in Mercury
doi: 10.1016/0029-5582(59)90334-7
1959EV81 Bull.Am.Phys.Soc. 4, No.4, 270, SA2 (1959) J.E.Evans, F.W.Firk, B.B.Kinsey, M.C.Moxon, J.R.Waters, G.H.Williams Analysis of the Low-Energy Neutron Resonances in Tungsten Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21317. 1959FI32 Nuclear Phys. 12, 552 (1959) Determination of Neutron Resonance Parameters of Tungsten by the Transmission Method
doi: 10.1016/0029-5582(59)90097-5
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. 1958FI33 Nuclear Phys. 9, 198 (1958) Neutron Resonances Parameters of Tantalium from 20 to 100 eV
doi: 10.1016/0029-5582(58)90391-2
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
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