NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = C.H.Johnson Found 72 matches. 1991JO08 Phys.Rev. C44, 657 (1991) C.H.Johnson, R.F.Carlton, R.R.Winters Evidence for Parity Dependence in the Neutron-40Ar Optical Model Potential NUCLEAR REACTIONS 40Ar(n, n), E < 40 MeV; analyzed data; deduced model parameters, potential parity dependence. Dispersive optical model.
doi: 10.1103/PhysRevC.44.657
1991WI02 Phys.Rev. C43, 492 (1991) R.R.Winters, R.F.Carlton, C.H.Johnson, N.W.Hill, M.R.Lacerna Total Cross Section and Neutron Resonance Spectroscopy for n + 40Ar NUCLEAR REACTIONS 40Ar(n, n), E=0.007-50 MeV; measured σ(E). 41Ar deduced resonances, J, π, (gΓn), reduced widths, strength functions. R-matrix analysis.
doi: 10.1103/PhysRevC.43.492
1989JO01 Phys.Rev. C39, 415 (1989) C.H.Johnson, R.F.Carlton, R.R.Winters Extrapolation of the Dispersive Optical Model to the Resonance Region for Neutrons on 86Kr NUCLEAR REACTIONS 86Kr(n, n), E ≤ 1 MeV; analyzed σ(E); deduced optical model parameter.
doi: 10.1103/PhysRevC.39.415
1988CA17 Phys.Rev. C38, 1605 (1988); Erratum Phys.Rev. C39, 1646 (1989) R.F.Carlton, R.R.Winters, C.H.Johnson, N.W.Hill, J.A.Harvey Total Cross Section and Resonance Spectroscopy for n + 86Kr NUCLEAR REACTIONS 86Kr(n, X), E=0.015-1 MeV; measured transmission; deduced σ(E). 87Kr deduced resonances, L, J, (gΓn), (g(γ(λn))2).
doi: 10.1103/PhysRevC.38.1605
1988JE03 Phys.Rev. C38, 2573 (1988) J.-P.Jeukenne, C.H.Johnson, C.Mahaux Surface Contributions to the Complex Neutron-208Pb Mean Field between -20 and +20 MeV NUCLEAR REACTIONS 208Pb(n, n), E=7-14 MeV; analyzed data; model parameters. Local optical model.
doi: 10.1103/PhysRevC.38.2573
1988JO05 Phys.Rev. C37, 2340 (1988) Evidence for State Dependence of the Imaginary Part of the Empirical Optical Potential NUCLEAR REACTIONS 208Pb(n, n), E=10 MeV; 89Y(n, n), E=5 MeV; calculated optical potential; deduced imaginary term shape dependence.
doi: 10.1103/PhysRevC.37.2340
1988JO07 Phys.Rev. C38, 2589 (1988) Neutron-40Ca Mean Field between -80 and +80 MeV from a Dispersive Optical-Model Analysis NUCLEAR REACTIONS 40Ca(n, n), E=5.3-40 MeV; analyzed data; deduced model parameters. Dispersive optical model analysis.
doi: 10.1103/PhysRevC.38.2589
1987CA11 Nucl.Phys. A465, 274 (1987) R.F.Carlton, J.A.Harvey, R.L.Macklin, C.H.Johnson, B.Castel Nuclear Structure of 49Ca above 5 MeV Excitation from n + 48Ca and Astrophysics for 30 keV Neutrons NUCLEAR REACTIONS 48Ca(n, n), (n, γ), (n, X), E < 2 MeV; measured total, capture σ(E), transmission. 49Ca deduced levels, J, π, (gΓnGγ/Γ), Γn, Γγ. R-matrix formalism.
doi: 10.1016/0375-9474(87)90435-0
1987JO04 Phys.Rev. C36, 2252 (1987) C.H.Johnson, D.J.Horen, C.Mahaux Unified Description of the Neutron-208Pb Mean Field between - 20 and + 165 MeV from the Dispersion Relation Constraint NUCLEAR REACTIONS 208Pb(n, n), (polarized n, n), E=1-25 MeV; measured σ(θ), analyzing power vs θ, σ(E). 208Pb deduced single particle densities, spectroscopic factors, rms radii, occupation numbers. Unified model, dispersion relation constraint.
doi: 10.1103/PhysRevC.36.2252
1986HO19 Phys.Rev. C34, 429 (1986) D.J.Horen, C.H.Johnson, J.L.Fowler, A.D.MacKellar, B.Castel 208Pb + n Reaction and the Mean Nuclear Field near Threshold NUCLEAR REACTIONS 208Pb(n, X), 208Pb(n, n), E=50-1005 keV; measured transmission, σ(E), σ(θ); deduced model parameters. 209Pb deduced resonances, J, π, Γn, neutron reduced width, strength function. Optical model, R-matrix analysis.
doi: 10.1103/PhysRevC.34.429
1985HA24 Phys.Rev. C32, 1114 (1985) J.A.Harvey, C.H.Johnson, R.F.Carlton, B.Castel Single-Particle 2d5/2 Strength in the 48Ca + n Reaction NUCLEAR REACTIONS 48Ca(n, n), E=0.01-2 MeV; measured σ(E). 49Ca deduced resonances, reduced widths, single particle strength fraction. R-matrix analysis.
doi: 10.1103/PhysRevC.32.1114
1985HO23 Phys.Lett. 161B, 217 (1985) D.J.Horen, C.H.Johnson, A.D.Mackellar lJ-Dependence of the Real Optical Potential near Neutron Threshold NUCLEAR REACTIONS 208Pb(n, X), (n, n), E=0.05-1.005 MeV; measured transmission, σ(θ). 208Pb(n, n), E=4, 7 MeV; analyzed σ(θ); deduced optical model parameters, l-, j-dependences.
doi: 10.1016/0370-2693(85)90748-8
1985WI02 Phys.Rev. C31, 384 (1985) R.R.Winters, C.H.Johnson, A.D.MacKellar Optical Model for Low-Energy Neutrons on 60Ni NUCLEAR REACTIONS 60Ni(n, n), E=1-450 keV; analyzed σ(E); deduced optical model parameters.
doi: 10.1103/PhysRevC.31.384
1984CA15 Phys.Rev. C29, 1988 (1984) R.F.Carlton, J.A.Harvey, C.H.Johnson s- and p-Wave Neutrons on 30Si and 34S: Spherical optical model analysis. NUCLEAR REACTIONS 30Si, 34S(n, n), E=0-1.4 MeV; analyzed s-, p-wave strength function data; deduced optical model parameters. Analytic approximation method.
doi: 10.1103/PhysRevC.29.1988
1983DA07 Nucl.Sci.Eng. 83, 22 (1983) J.W.T.Dabbs, C.H.Johnson, C.E.Bemis, Jr. Measurement of the 241Am Neutron Fission Cross Section NUCLEAR REACTIONS 241Am(n, F), E=0.00002-20 MeV; measured fission σ(E); deduced fission resonance integral.
doi: 10.13182/NSE83-A17986
1983JO01 Phys.Rev. C27, 416 (1983) Average Scattering Matrix Elements from High Resolution Neutron Total Cross Sections for 32S NUCLEAR REACTIONS 32S(n, n), E=25-1100 keV; analyzed data; deduced s-, p-wave optical model parameters.
doi: 10.1103/PhysRevC.27.416
1983JO07 Phys.Rev. C27, 1913 (1983) C.H.Johnson, N.M.Larson, C.Mahaux, R.R.Winters Calculation of the Energy-Averaged Scattering Function from High Resolution Low-Energy Neutron Scattering Data NUCLEAR REACTIONS 32S(n, n), E ≈ 0.2-0.9 MeV; calculated σ(compound nucleus), σ(shape elastic) vs E. Optical model scattering function, energy averaging, p-wave neutrons.
doi: 10.1103/PhysRevC.27.1913
1980HA04 Phys.Rev. C21, 545 (1980) J.Halperin, C.H.Johnson, R.R.Winters, R.L.Macklin Resonance Structure of 32S + n from Measurements of Neutron Total and Capture Cross Sections NUCLEAR REACTIONS 32S(n, n), E=25-1100 keV; 32S(n, γ), E=2.5-1100 keV; measured total σ(E). 33S deduced resonances, L, J, π, Γn, Γγ, resonance parameters. Valency model.
doi: 10.1103/PhysRevC.21.545
1980HE03 Phys.Rev. C21, 896 (1980) R.L.Hershberger, D.S.Flynn, F.Gabbard, C.H.Johnson Systematics of Proton Absorption Deduced from (p, p) and (p, n) Cross Sections for 2.0- to 6.7-MeV Protons on 107,109Ag and 115In NUCLEAR REACTIONS 107,109Ag, 115In(p, p), (p, n), E=2-6.7 MeV; measured σ(θp), total σ(p, n); deduced model parameters. Statistical, optical model analyses.
doi: 10.1103/PhysRevC.21.896
1980JO04 Phys.Rev. C21, 2190 (1980) Neutron Total Cross Section of Sulfur: Single Level to Multilevel to Optical Model NUCLEAR REACTIONS 32S(n, n), E=25-1100 keV; analyzed total σ(E); deduced optical model parameters. 33S deduced resonances, J, π, s-, p-strength functions. Single-, multilevel R-matrix, optical model analyses.
doi: 10.1103/PhysRevC.21.2190
1979JO09 Phys.Rev. C20, 2052 (1979) C.H.Johnson, A.Galonsky, R.L.Kernell (p, n) Reaction for 89 < A < 130 and an Anomalous Optical Model Potential for Sub-Coulomb Protons NUCLEAR REACTIONS 105,106,108,110Pd, 107,109Ag, 111,112,113,114,116Cd, 125,126,128,130Te, 89Y, 93Nb, 103Rh(p, n), E=2.5-5.8 MeV; measured σ; deduced optical model parameters. Enriched targets. Pd, Ag, Cd, In, Te(p, n), E=2.5-5.8 MeV; measured σ; deduced optical model parameters. Natural targets.
doi: 10.1103/PhysRevC.20.2052
1977JO01 Phys.Rev. C15, 196 (1977) C.H.Johnson, J.K.Bair, C.M.Jones, S.K.Penny, D.W.Smith p-Wave Size Resonances Observed by the (p, n) Reaction for 2.6- to 7-MeV Protons Incident on Isotopes of Sn NUCLEAR REACTIONS 117,118,119,120,122,124Sn(p, n), E=2.6-7 MeV; measured total σ, σ(E). 118,119,120,121,123,125Sb deduced resonances. Statistical, optical model analysis.
doi: 10.1103/PhysRevC.15.196
1977JO03 Phys.Rev. C15, 915 (1977) C.H.Johnson, J.K.Bair, C.M.Jones Thresholds for 116Sn(p, n) and 118Sn(p, n) NUCLEAR REACTIONS 116,118Sn(p, n), E ≈ threshold; measured thick target integrated σ; deduced Q.
doi: 10.1103/PhysRevC.15.915
1977JO11 Phys.Rev.Lett. 39, 1604 (1977) C.H.Johnson, A.Galonsky, R.L.Kernell Anomalous Optical-Model Potential for Sub-Coulomb Protons for 89 < A < 130 NUCLEAR REACTIONS 89Y, In, 93Nb, 103Rh, 105,110Pd, 107,109Ag, 111,113,114,116Cd, 128,130Te(p, n), E=2.5-5.8 MeV; measured nothing, reanalyzed data, absolute σ.
doi: 10.1103/PhysRevLett.39.1604
1976RO15 Phys.Rev. C14, 2126 (1976) R.L.Robinson, J.K.Bair, C.H.Johnson, P.H.Stelson, W.B.Dress, C.M.Jones Cross Sections for the Ni, Cu, Zn(16,18O, xn) Reactions Near the Coulomb Barrier NUCLEAR REACTIONS 58,60,61,62,64Ni, 63,65Cu, 64,66,67,68,70Zn(16O, xn), (18O, xn), E=36-55 MeV; measured total σ(E).
doi: 10.1103/PhysRevC.14.2126
1973FO11 Phys.Rev. C8, 545 (1973) J.L.Fowler, C.H.Johnson, R.M.Feezel Level Structure of 17O from Neutron Total Cross Sections NUCLEAR REACTIONS 16O(n, γ), E=0.6-4.3 MeV; measured σ(E). 17O deduced levels, J, π, level-width.
doi: 10.1103/PhysRevC.8.545
1973JO01 Phys.Rev. C7, 561 (1973); Erratum Phys.Rev. C8, 851 (1973) Unified R-Matrix-Plus-Potential Analysis for 16O + n Cross Sections NUCLEAR REACTIONS 16O(n, X), (n, α), E < 5.8 MeV; analyzed σ(E). 17O deduced resonances, J, π, level-width, S.
doi: 10.1103/PhysRevC.7.561
1972HA56 Nucl.Phys. A193, 65 (1972) F.X.Haas, C.H.Johnson, J.K.Bair The Energy Levels of 21Na NUCLEAR REACTIONS 20Ne(p, γ), E=0.98-2.2 MeV; measured Eγ, Iγ, Q-value. 20Ne(d, n), E=3.6-6 MeV; measured absolute σ(θ). 21Na deduced levels, level-width, S.
doi: 10.1016/0375-9474(72)90236-9
1971KE21 Nucl.Phys. A176, 449 (1971) R.L.Kernell, H.J.Kim, R.L.Robinson, C.H.Johnson The 117,119Sn(p, n)117,119Sb Reactions Near 0+ Analogue States NUCLEAR REACTIONS 117,119Sn(p, n), E=4.4-4.8 MeV; measured σ(Ep), σ(θ), Q. 117,119Sb deduced levels, J, π.
doi: 10.1016/0375-9474(71)90927-4
1971KI06 Nucl.Phys. A167, 65 (1971) H.J.Kim, R.L.Robinson, C.H.Johnson Spin-Parity Assignments for the Low-Lying States in 95,97Tc via the Neutron Decay of 0+ and 2+ Analogue States NUCLEAR REACTIONS 91Zr, 95,97Mo(p, n), E=3.5-4.4 MeV; measured σ(E;En, θ). 92Nb, 96,98Tc deduced isobaric analog resonances, level-width. 91Nb, 95,97Tc deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(71)90581-1
1970FO03 Phys.Rev. C2, 124 (1970) Differential Scattering of Neutrons at Narrow Levels in 17O NUCLEAR REACTIONS 16O(n, n), E=1.116-3.67 MeV; measured σ(E;θ). 17O deduced resonances, L, J, π, level-width.
doi: 10.1103/PhysRevC.2.124
1970JO15 Phys.Rev. C2, 639 (1970) (p, n) Cross Sections and the Strength Functions for 3- to 5.5-MeV Protons on In and Sn Isotopes NUCLEAR REACTIONS In, Sn, 117,119,120,122,124Sn(p, n), E=3-5.5 MeV; measured σ(E); deduced Q for 120Sn(p, n).
doi: 10.1103/PhysRevC.2.639
1970KI01 Nucl.Phys. A142, 35 (1970) H.J.Kim, R.L.Robinson, C.H.Johnson, S.Raman Energy Levels of 91Nb, 93Mo, 95Tc and 97Tc via (p, n) Reactions and the Reaction Q-Values NUCLEAR REACTIONS 91Zr, 93Nb, 95,97Mo(p, n), E=4-5.4 MeV; measured σ(E;En, θ). 91Zr, 95,97Mo(p, n); measured Q. 91Nb, 93Mo, 95,97Tc deduced levels.
doi: 10.1016/0375-9474(70)90472-0
1970KI18 Bull.Amer.Phys.Soc. 15, No.2, 191, FA11 (1970) H.J.Kim, R.L.Robinson, C.H.Johnson The Spin-Parities of the Second and Third Excited States of 91Nb via the Neutron Decay of an Analogue States NUCLEAR REACTIONS 91Zr(p, n), E=4-5 MeV; measured σ(E;En, θ). 92Nb deduced isobaric analog resonance. 91Nb deduced levels, J, π.
1969JO11 Phys.Rev.Letters 23, 20 (1969) Proton Strength Functions for Sn and the Optical Model below the Coulomb Barrier NUCLEAR REACTIONS 117,119,120,122,124Sn(p, n), E=3-5.5 MeV; measured σ(E); deduced proton strength functions.
doi: 10.1103/PhysRevLett.23.20
1969KI07 Phys.Rev. 180, 1167 (1969) H.J.Kim, R.L.Robinson, C.H.Johnson Characteristics of the Differential Cross Sections for the Low-Energy (p, n) Reaction on the Spin-1/2 Medium-Mass Nuclei NUCLEAR REACTIONS 111,113Cd, 117,119Sn(p, n), E=5.35 MeV; measured σ(En, θ). Enriched targets.
doi: 10.1103/PhysRev.180.1167
1969KI08 Phys.Rev. 180, 1175 (1969) H.J.Kim, R.L.Robinson, C.H.Johnson Low-Lying States of 111In via the 111Cd(p, n)111In Reaction NUCLEAR REACTIONS 111Cd(p, nγ), E=4.2-5.35 MeV; measured σ(E;En, Eγ, θ). 111In deduced levels, J.
doi: 10.1103/PhysRev.180.1175
1969KI10 Priv.Comm. (1969)
1968CU05 Nucl.Instr.Methods 63, 221(1968) A Twin-Target Technique for the Measurement of Nuclear Lifetimes by the Doppler Shift Attenuation Method NUCLEAR REACTIONS 12C(16O, α), E = 26 MeV; measured Eγ, σ(Eγ, Eα), Doppler-shift attenuation. 24Mg levels deduced T1/2.
doi: 10.1016/0029-554X(68)90333-9
1968JO01 Nucl.Phys. A107, 21 (1968) C.H.Johnson, R.L.Kernell, S.Ramavataram The 89Y(p, n)89Zr Cross Section Near the First Two Analogue Resonances NUCLEAR REACTIONS 89Y(p, n), E = 3.6-5.8 MeV; measured Q, σ(E). 90Zr, 89Zr, deduced levels.
doi: 10.1016/0375-9474(68)90720-3
1968JO21 Phys.Rev. 169, 974 (1968) Use of the (p, n) Reaction to Measure Proton Atomic Stopping Powers in Ag, Cd, In, and Sn NUCLEAR REACTIONS Ag(p, n), Cd(p, n), In(p, n), Sn(p, n), E=-1.0 eV-5.7 MeV; measured products, Eν, Iν; deduced σ, σ(E). Data were imported from EXFOR entry C0775.
doi: 10.1103/PhysRev.169.974
1968JO22 Bull.Am.Phys.Soc. 13, 601 DE1 (1968) C.H.Johnson, F.X.Haas, J.L.Fowler 17O states observed by scattering of neutrons from 16O NUCLEAR REACTIONS 16O(n, X), E=1.116, 1.95-3.67 MeV; measured reaction products. 17O; deduced resonances and widths.
1967JO12 Phys.Rev. 162, 890 (1967) Scattering of Neutrons from 16O in the 2.2- to 4.2-MeV Energy Range NUCLEAR STRUCTURE 16O, 17O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.162.890
1967KI06 Phys.Rev.Lett. 19, 325 (1967) H.J.Kim, R.L.Robinson, R.L.Kernell, C.H.Johnson Spin-Parity Assignments via Neutron Decay of Analog Resonance NUCLEAR STRUCTURE 119Sb; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.19.325
1966KE05 Bull.Am.Phys.Soc. 11, No.4, 630, S29 (1966) Cross Sections for Analog Resonances in 75As, 111Cd, and 113Cd(p, n) Reactions NUCLEAR STRUCTURE 76Se, 112In, 114In; measured not abstracted; deduced nuclear properties.
1965JO19 Rev.Mod.Phys. 37, 437 (1965) C.M.Jones, J.K.Bair, C.H.Johnson, H.B.Willard, M.Reeves III Sequential Emission in the Reaction 7Li(d, n)2a NUCLEAR REACTIONS 7Li(d, n), E=1.8-7.0 MeV; measured Eα, αα-coin; deduced sequential decay.
doi: 10.1103/RevModPhys.37.437
1964FO09 ORNL-3582, p.90 (1964) The Scattering of 3 to 4 MeV Neutrons from O16 NUCLEAR STRUCTURE 17O; measured not abstracted; deduced nuclear properties.
1964JO04 Phys.Rev. 133, B1183 (1964) Neutron Spectra from Li7(d, n)Be8 and F19(d, n)Ne20 for 1.98-MeV Deuterons NUCLEAR STRUCTURE 19F, 7Li; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.133.B1183
1964JO05 Bull.Am.Phys.Soc. 9, No.4, 445, FC11 (1964) Phase-Shift Analysis of Neutron Scattering from 16O NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
1964JO11 Phys.Rev. 136, B1719 (1964) C.H.Johnson, C.C.Trail, A.Galonsky Thresholds for (p, n) Reactions on 26 Intermediate-Weight Nuclei NUCLEAR STRUCTURE 112In, 89Zr, 93Mo, 82Br, 80Br, 106Ag, 108Ag, 73As, 70Ga, 71Ge, 69Ge, 68Ga, 67Ga, 75Se, 74As, 48Sc, 49V, 59Ni, 57Co, 37Ar, 41Ca, 55Fe, 51Cr, 53Mn, 61Cu, 65Zn; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.136.B1719
1963JO04 Nucl.Phys. 41, 167 (1963) C.H.Johnson, F.Pleasonton, T.A.Carlson An Absolute Measurement of the 6He Decay Energy NUCLEAR STRUCTURE 6He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90488-7
1963JO05 Bull.Am.Phys.Soc. 8, No.4, 333, J18 (1963) C.H.Johnson, F.Pleasonton, T.A.Carlson Experimental Limit to Tensor Interaction in β-Decay of He6 NUCLEAR STRUCTURE 6He; measured not abstracted; deduced nuclear properties.
1963JO13 Bull.Am.Phys.Soc.Southeastern Section, p.8, E4 (November 1963) Differential Eleastic Scattering of Neutrons from O16 NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
1963JO15 Phys.Rev. 132, 1149 (1963) C.H.Johnson, F.Pleasonton, T.A.Carlson Precision Measurement of the Recoil Energy Spectrum from the Decay of He6 NUCLEAR STRUCTURE 6He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.132.1149
1962JO03 ORNL-3268, p.61 (1962) C.H.Johnson, F.Pleasonton, T.A.Carlson An Absolute Determination of the He6 Beta-Decay Energy NUCLEAR STRUCTURE 6He; measured not abstracted; deduced nuclear properties.
1961JO05 Bull.Am.Phys.Soc. 6, No.3, 227, B1 (1961) C.H.Johnson, F.Pleasonton, T.A.Carlson Recoil Energy Spectrum for the β Decay of He6 NUCLEAR STRUCTURE 6He; measured not abstracted; deduced nuclear properties.
1961JO09 Bull.Am.Phys.Soc. 6, No.5, 459, D5 (1961) C.H.Johnson, F.Pleasonton, T.A.Carlson An Absolute Determination of the He6 β-Decay Energy NUCLEAR STRUCTURE 6He; measured not abstracted; deduced nuclear properties.
1961JO11 Ann.Inform.Meeting Phys.Div. Electronuclear Div., Oak Ridge Natl. Lab., (April 1961) C.H.Johnson, F.Pleasonton, T.A.Carlson NUCLEAR STRUCTURE 6He; measured not abstracted; deduced nuclear properties.
1960JO05 Bull.Am.Phys.Soc. 5, No.6, 443, C13 (1960) Thresholds for (p, n) Reactions
1959JO42 ORNL-2718, p.5 (1959) C.H.Johnson, F.Pleasonton, A.H.Snell
1959PL52 Bull.Am.Phys.Soc. 4, No.1, 78, C3 (1959) F.Pleasonton, C.H.Johnson, A.H.Snell Recoil Momentum Spectra for the β-Decay of He6
1958JO01 Phys.Rev. 109, 1243 (1958) C.H.Johnson, A.Galonsky, J.P.Ulrich Proton Strength Functions from (p, n) Cross Sections
doi: 10.1103/PhysRev.109.1243
1958JO24 ORNL-2501, p.29 (1958) C.H.Johnson, A.Galonsky, C.N.Inskeep
1956GA51 Phys.Rev. 104, 421 (1956) Cross Sections for the T(d, n)He4 Reaction
doi: 10.1103/PhysRev.104.421
1955FO27 Phys.Rev. 98, 728 (1955) Differential Elastic Scattering Cross Section for Neutron on Nitrogen
doi: 10.1103/PhysRev.98.728
1954JO17 Phys.Rev. 96, 985 (1954) C.H.Johnson, H.B.Willard, J.K.Bair Total Cross Section of Li6 for Neutrons
doi: 10.1103/PhysRev.96.985
1954JO22 Phys.Rev. 93, 924 (K3) (1954) Yields near Threshold for (p, n) Reactions in Intermediate Nuclei NUCLEAR REACTIONS 75As(p, n), E=2.5 MeV; measured reaction products, En, In; deduced yields. The Oak Ridge 2.5-MeV Van de Graaff
1953TR21 Phys.Rev. 91, 474A (1953) (p, n) Thresholds of Nuclei with 49 ≤ A ≤ 75
doi: 10.1103/PhysRev.91.474A
1951JO22 Phys.Rev. 82, 117 (1951) C.H.Johnson, C.K.Bockelman, H.H.Barschall Disintegration Of Neon By Fast Neutrons NUCLEAR REACTIONS 20Ne(n, α), E=1.8-3.3 MeV; measured products, 17O, 4He; deduced σ, σ(E). Data were imported from EXFOR entry 11385.
doi: 10.1103/PhysRev.82.117
1951JO23 Phys.Rev. 84, 775 (1951) C.H.Johnson, B.Petree, R.K.Adair Total Cross Section of Nitrogen for Fast Neutrons NUCLEAR REACTIONS N(n, x), E=149.2 keV-1.4 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 14122.
doi: 10.1103/PhysRev.84.775
1951PE18 Phys.Rev. 83, 1148 (1951) B.Petree, C.H.Johnson, D.W.Miller Disintegration of Boron by Fast Neutrons
doi: 10.1103/PhysRev.83.1148
1950JO57 Phys.Rev. 80, 818 (1950) Interaction of Fast Neutrons with Nitrogen
doi: 10.1103/PhysRev.80.818
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