NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.D.Bowman Found 56 matches. 2002FU16 J.Phys.(London) G28, 2627 (2002) W.I.Furman, E.V.Lychagin, A.Yu.Muzichka, G.V.Nekhaev, Yu.V.Safronov, A. V.Strelkov, E.I.Sharapov, V.N.Shvetsov, B.G.Levakov, V.I.Litvin, A.E.Lyzhin, E.P.Magda, C.R.Howell, G.E.Mitchell, W.Tornow, B.E.Crawford, S.L.Stephenson, C.D.Bowman Direct measurement of the neutron-neutron scattering cross section at the reactor YAGUAR NUCLEAR REACTIONS 63Cu, 197Au(n, γ), E=thermal; measured activation yields; deduced neutron flux density. Application to proposed neutron-neutron scattering experiment discussed.
doi: 10.1088/0954-3899/28/10/308
1998BO36 Ann.Rev.Nucl.Part.Sci. 48, 505 (1998) Accelerator-Driven Systems for Nuclear Waste Transmutation
doi: 10.1146/annurev.nucl.48.1.505
1993RO25 Nucl.Instrum.Methods Phys.Res. A326, 549 (1993) N.R.Roberson, C.D.Bowman, J.D.Bowman, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, R.N.Mortensen, S.I.Penttila, H.Postma, S.J.Seestrom, J.J.Szymanski, S.A.Wender, S.H.Yoo, V.W.Yuan, X.Zhu An Apparatus and Techniques of Tests for Fundamental Symmetries in Compound-Nucleus Scattering with Epithermal Polarized Neutron Beams NUCLEAR REACTIONS 238U(polarized n, X), E=5-300 eV; measured neutron transmission. 239U resonance deduced average parity violating asymmetry.
doi: 10.1016/0168-9002(93)90858-F
1992FR07 Phys.Rev. C45, 2143 (1992) C.M.Frankle, C.D.Bowman, J.D.Bowman, S.J.Seestrom, E.I.Sharapov, Yu.P.Popov, N.R.Roberson Neutron Resonance Spectroscopy on 113Cd: The p-wave levels NUCLEAR REACTIONS 113Cd(n, n), 113Cd, Cd(n, γ), E=0-500 eV; measured En, capture γ yield, σ(E). 114Cd deduced levels, resonance parameters, p-wave strength function, level density. Enriched target.
doi: 10.1103/PhysRevC.45.2143
1992PO13 Hyperfine Interactions 75, 153 (1992) H.Postma, J.D.Bowman, C.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.Knudson, G.E.Mitchell, S.Penttila, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration Parity Violation at Neutron p-Wave Resonances of 238U and 232Th and Related Questions NUCLEAR REACTIONS 238U, 232Th(n, X), E ≈ epithermal; measured transmission. 239U, 233Th deduced p-wave resonances, parity violation matrix element rms value.
doi: 10.1007/BF02398972
1992ZH12 Phys.Rev. C46, 768 (1992) X.Zhu, J.D.Bowman, C.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.W.Yuan, and the TRIPLE Collaboration Parity Nonconservation for Neutron Resonances in 238U NUCLEAR REACTIONS 238U(polarized n, X), E=6-300 eV; measured total σ; deduced P-odd, P-even effective nucleon-nucleon interaction. 239U deduced resonances, l, gΓn, p-wave parity nonconserving matrix element rms value, spreading width.
doi: 10.1103/PhysRevC.46.768
1991SZ05 Nucl.Phys. A527, 701c (1991) J.J.Szymanski, C.D.Bowman, J.D.Bowman, J.Knudson, S.Penttila, S.J.Seestrom, V.W.Yuan, J.E.Bush, C.M.Frankle, C.R.Gould, D.G.Haase, G.E.Mitchell, P.P.J.Delheij, H.Postma, N.R.Roberson, X.Zhu Parity and Time Reversal Symmetry Nonconservation in Neutron-Nucleus Interactions NUCLEAR REACTIONS 238U(polarized n, X), E=60-72 eV; measured transmission, resonance σ helicity dependence. 239U deduced p-, s-wave states mixing parity-violating rms matrix element, parity violating spreading width.
doi: 10.1016/0375-9474(91)90217-T
1991YU02 Phys.Rev. C44, 2187 (1991) V.W.Yuan, C.D.Bowman, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, X.Zhu Parity Nonconservation in Polarized-Neutron Transmission Through 139La NUCLEAR REACTIONS 139La(polarized n, X), E=0.5-1 eV; measured transmission. 140La resonance deduced asymmetry. Parity nonconservation, longitudinal beam polarization.
doi: 10.1103/PhysRevC.44.2187
1990BO26 Phys.Rev.Lett. 65, 1192 (1990) J.D.Bowman, C.D.Bowman, J.E.Bush, P.P.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.W.Yuan, X.Zhu Parity Nonconservation for Neutron Resonances in 238U NUCLEAR REACTIONS 238U(n, X), E=epithermal; measured transmission, σ(E) vs helicity. 239U levels deduced parity nonconservation.
doi: 10.1103/PhysRevLett.65.1192
1990BO46 Nucl.Instrum.Methods Phys.Res. A297, 183 (1990) J.D.Bowman, J.J.Szymanski, V.W.Yuan, C.D.Bowman, A.Silverman, X.Zhu Current-Mode Detector for Neutron Time-of-Flight Studies NUCLEAR REACTIONS 238U(n, X), E not given; measured neutron transmission spectra. Tof, current mode detector.
doi: 10.1016/0168-9002(90)91365-I
1990CO09 Nucl.Instrum.Methods Phys.Res. A288, 463 (1990) K.P.Coulter, T.E.Chupp, A.B.McDonald, C.D.Bowman, J.D.Bowman, J.J.Szymanski, V.Yuan, G.D.Cates, D.R.Benton, E.D.Earle Neutron Polarization with a Polarized 3He Spin Filter NUCLEAR REACTIONS 139La(polarized n, X), E=low; measured transmission; deduced helicity dependence on 140La resonance. Polarized 3He spin filter.
doi: 10.1016/0168-9002(90)90139-W
1990PE19 J.Phys.(Paris), Colloq.C-6, 523 (1990) S.Penttila, C.D.Bowman, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.M.Yuan, X.Zhu Parity Violation in 239U Neutron Resonances NUCLEAR REACTIONS 238U(polarized n, X), E ≤ 250 eV; measured asymmetry in transmission; deduced parity violating matrix element rms value, effective NN-interaction parameter. 239U resonances deduced parity-violating spreading width.
1989BO09 Phys.Rev. C39, 1721 (1989) C.D.Bowman, J.D.Bowman, V.W.Yuan Parity Violation in the 0.734-eV Neutron Resonance in 139La NUCLEAR REACTIONS 139La(n, X), E ≈ resonance; measured transmission. 140La deduced resonance parity violation. Neutron spin flipper between samples.
doi: 10.1103/PhysRevC.39.1721
1988BO15 J.Phys.(London) G14, Supplement S399 (1988) New Opportunities in Neutron Capture Research using Advanced Pulsed Neutron Sources NUCLEAR REACTIONS 7Be(n, p), E ≈ 0.02-10 eV; measured σ(E). R-matrix fit.
doi: 10.1088/0305-4616/14/S/040
1988KO03 Phys.Rev. C37, 917 (1988) P.E.Koehler, C.D.Bowman, F.J.Steinkruger, D.C.Moody, G.M.Hale, J.W.Starner, S.A.Wender, R.C.Haight, P.W.Lisowski, W.L.Talbert 7Be(n, p)7Li Total Cross Section from 25 MeV to 13.5 keV NUCLEAR REACTIONS 7Be(n, p), E=0.025-13500 eV; measured σ. 8Be levels deduced Γp, Γn, Γ. Calculated astrophysical reaction rate. R-matrix analysis.
doi: 10.1103/PhysRevC.37.917
1980BO02 Phys.Rev. C21, 58 (1980) Influence of Vibrations of Gas Molecules on Neutron Reaction Cross Sections NUCLEAR REACTIONS 238U(n, γ), E=6.67 eV; measured σ; deduced effect of molecular vibrations. U3O8 solid, UF6 gas targets.
doi: 10.1103/PhysRevC.21.58
1978BO02 Phys.Rev. C17, 654 (1978) Effects of Phonon Transfer on Near-Thermal Neutron Fission Cross Sections NUCLEAR REACTIONS 235U(n, F); calculated Doppler effect, phonon exchange, temperature dependence.
doi: 10.1103/PhysRevC.17.654
1978BO07 Phys.Rev. C17, 1086 (1978) C.D.Bowman, I.G.Schroder, K.C.Duvall, C.E.Dick Subthreshold Photofission of 235U and 232Th NUCLEAR REACTIONS 232Th, 236U(γ, F), E=3.25-5.75 MeV; 234U(γ, F), E=3.5 MeV; measured σ.
doi: 10.1103/PhysRevC.17.1086
1976HO03 Phys.Rev. C13, 195 (1976) R.E.Howe, T.W.Phillips, C.D.Bowman Prompt Fission Neutrons from eV Resonances in 235U: Measurement and Correlation with Other Fission Properties NUCLEAR REACTIONS 235U(n, F), E=0.5-125 eV; measured relative neutron multiplicity ν-bar; deduced correlations with other fission properties.
doi: 10.1103/PhysRevC.13.195
1975BO31 Phys.Rev. C12, 863 (1975) C.D.Bowman, I.G.Schroder, C.E.Dick, H.E.Jackson Very Low Energy Photofission of 238U NUCLEAR REACTIONS 238U(γ, F), E=2.75-6 MeV; measured σ(E). 238U deduced barrier penetration parameters.
doi: 10.1103/PhysRevC.12.863
1974BR05 Phys.Rev. C9, 1177 (1974) Investigation of the γ Decay of Subthreshold-Fission Resonances of 242Pu to a Fission Isomeric State NUCLEAR REACTIONS 242Pu(n, Fγ), E=400-3000 eV; measured σ(E), γ(t). 243Pu resonance deduced γ-branching.
doi: 10.1103/PhysRevC.9.1177
1974PH01 Phys.Rev. C9, 407 (1974) T.W.Phillips, C.D.Bowman, B.L.Berman Concerning the Question of Nonresonant Neutron Capture in 207Pb NUCLEAR REACTIONS 207Pb(n, γ), E < 41 keV; measured σ(E). 208Pb resonances deduced level-width.
doi: 10.1103/PhysRevC.9.407
1973AU03 Phys.Rev. C7, 2085 (1973); Erratum Phys.Rev. C8, 1968 (1973) Parameters of the Subthreshold Fission Structure in 242Pu NUCLEAR REACTIONS 242Pu(n, X), E=0.6-81 keV; measured σ(E). 243Pu deduced resonances, level-width.
doi: 10.1103/PhysRevC.7.2085
1972BR04 Phys.Rev.Lett. 28, 617 (1972) Investigation of γ-Ray Emission Preceding Isomeric Fission of 236U NUCLEAR REACTIONS, Fission 235U(n, γF), E=1-100 eV; measured (γ)(fragment)-delay; deduced limit on pre-fission γ-emission. 236U deduced relative double barrier penetrabilities.
doi: 10.1103/PhysRevLett.28.617
1971BA07 Phys.Rev. C3, 672 (1971) R.J.Baglan, C.D.Bowman, B.L.Berman Threshold Photoneutron Cross Sections for 206, 207, 208Pb, 56, 57Fe, 52, 53Cr, 24, 25, 26Mg, and 19F NUCLEAR REACTIONS 19F, 24,25,26Mg, 52,53Cr, 56,57Fe, 206,207,208Pb(γ, n), E= threshold+1 MeV; measured σ(E;En). 19F, 24,25,26Mg, 52,53Cr, 56,57Fe, 206,207,208Pb deduced resonances, J, π, level-width, isobaric analogs.
doi: 10.1103/PhysRevC.3.672
1971BA38 Phys.Rev. C3, 2475 (1971) R.J.Baglan, C.D.Bowman, B.L.Berman Evidence for Doorway States in 207Pb, 208Pb, and 57Fe from Threshold Photoneutron Cross-Section Measurements NUCLEAR REACTIONS 57Fe, 207,208Pb(γ, n), E < 12 MeV; measured σ(En). 57Fe, 207,208Pb deduced resonance, level-width, doorway states.
doi: 10.1103/PhysRevC.3.2475
1970BA42 UCRL Preprint (1970); See Also 70Bo24 R.J.Baglan, C.D.Bowman, B.L.Berman Threshold Photoneutron Cross Sections for 206,207,208Pb, 56,57Fe, 24,25,26Mg, and 19F
1970BE04 Phys.Rev.Lett. 24, 319 (1970) B.L.Berman, R.J.Baglan, C.D.Bowman Threshold Photoneutron Cross Section for Mg25 and Isobaric Analogs of Na25 NUCLEAR REACTIONS 25Mg(γ, n), E < 11 MeV; measured σ(E;En). 25Mg deduced resonances, level-width, isobaric analog. 25Mg-25Na deduced Coulomb displacement energy.
doi: 10.1103/PhysRevLett.24.319
1970BO24 Phys.Rev.Lett. 25, 1302 (1970); See Also 70Ba42 C.D.Bowman, R.J.Baglan, B.L.Berman, T.W.Phillips M1 Giant Resonance in 208Pb from Threshold Photoneutron Measurements NUCLEAR REACTIONS 208Pb(γ, n), E < 9.8 MeV; measured σ(En, θ). 208Pb deduced resonances, J, π, level-width, M1 giant resonance structure.
doi: 10.1103/PhysRevLett.25.1302
1969BE26 Phys.Rev.Letters 23, 386 (1969) B.L.Berman, R.L.Van Hemert, C.D.Bowman Threshold Photoneutron Cross Section for Mg26 and a Source of Stellar Neutrons NUCLEAR REACTIONS 26Mg(γ, n), E=0.01-1.5 MeV; measured σ(E;En); deduced resonances.
doi: 10.1103/PhysRevLett.23.386
1969BO14 Phys.Rev. 178, 1827 (1969) C.D.Bowman, B.L.Berman, H.E.Jackson Electromagnetic Transition Strengths in Pb206, Pb207, and Pb208 from Threshold Photoneutron Cross-Section Measurements NUCLEAR REACTIONS 206,207,208Pb(γ, n), E approx threshold; measured σ(E;En). 206,207,208Pb deduced resonances, level-width.
doi: 10.1103/PhysRev.178.1827
1969BO26 Phys.Rev.Letters 23, 796 (1969); Erratum Phys.Rev.Lett. 24, 193 (1970) C.D.Bowman, R.J.Baglan, B.L.Berman Detection of Nonresonant Neutron Capture in Pb207 via the Threshold Photoneutron Cross Section for Pb208 NUCLEAR REACTIONS 208Pb(γ, n), E < 9 MeV; measured σ(En);deduced nonresonant capture in 207Pb. 208Pb deduced resonances, J, π, level-width.
doi: 10.1103/PhysRevLett.23.796
1968AU07 Nucl.Phys. A112, 329 (1968) G.F.Auchampaugh, C.D.Bowman, J.E.Evans Neutron-Induced Fission Cross Sections Of 232U NUCLEAR REACTIONS 232U(n, n), (n, f), E=-0.6 eV-1.9 keV; measured products; deduced resonance parameters, σ, σ(E). Data were imported from EXFOR entry 12383.
doi: 10.1016/0375-9474(68)90205-4
1968BO57 Phys.Rev. 166, 1219 (1968) C.D.Bowman, G.F.Auchampaugh, S.C.Fultz, R.W.Hoff Neutron-Induced Fission Cross Section of Am242 NUCLEAR REACTIONS, Fission 242mAm(n, F), E=0.02 eV - 6 MeV; measured σ(E). 243Am deduced resonance parameters.
doi: 10.1103/PhysRev.166.1219
1968SA11 Phys.Rev. 174, 1413 (1968) Neutron Scattering Cross Sections of U233, U235, and Pu241 from 1 to 30 eV NUCLEAR STRUCTURE 234U, 242Pu; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.174.1413
1967BE49 Phys.Rev. 163, 958 (1967) B.L.Berman, R.L.Van Hemert, C.D.Bowman Threshold Photoneutron Cross Section for Be9 NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.163.958
1967BO28 Phys.Rev. 163, 951 (1967) C.D.Bowman, G.S.Sidhu, B.L.Berman Threshold Photoneutron Cross Section for Fe56 NUCLEAR STRUCTURE 56Fe; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.163.951
1967CA04 Phys.Rev. 155, 1309 (1967) J.T.Caldwell, S.C.Fultz, C.D.Bowman, R.W.Hoff Spontaneous Fission Half-Life of Am242m NUCLEAR STRUCTURE 242Am; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.155.1309
1967ST38 Phys.Rev. 154, 1111 (1967) W.F.Stubbins, C.D.Bowman, G.F.Auchampaugh, M.S.Coops Neutron-Induced Resonance Fission Cross Section of Pu238 NUCLEAR REACTIONS 238Pu(n, n), 238Pu(n, f), 238Pu(n, x), E=2.0-299.2 eV; measured products; deduced resonance parameters, σ, σ(). Data were imported from EXFOR entry 12489.
doi: 10.1103/PhysRev.154.1111
1966AU07 Phys.Rev. 146, 840 (1966) G.F.Auchampaugh, C.D.Bowman, M.S.Coops, S.C.Fultz Neutron total cross sections of 242Pu NUCLEAR REACTIONS 242Pu(n, n), 242Pu(n, x), E=0.0253-388.2 eV; measured products; deduced resonance parameters, σ, σ(E). Data were imported from EXFOR entry 12546.
doi: 10.1103/PhysRev.146.840
1965AU02 WASH-1064, p.46 (1965); and Priv.Comm. (1966) G.F.Auchampaugh, C.D.Bowman, M.S.Coops, S.C.Fultz Total Cross Section of Pu242
1965BO06 Phys.Rev. 137, B326 (1965) C.D.Bowman, M.S.Coops, G.F.Auchampaugh, S.C.Fultz Subthreshold Neutron-Induced Fission Cross Section of Am241 NUCLEAR STRUCTURE 241Am; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.137.B326
1965BO38 WASH-1064, p.54 (1965) The Spontaneous Fission Half-Life of Am242m NUCLEAR STRUCTURE 242Am; measured not abstracted; deduced nuclear properties.
1965SA10 Phys.Rev.Letters 15, 761 (1965) Scattering Measurements on Neutron Resonances in Pu239 NUCLEAR STRUCTURE 240Pu; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.15.761
1964BO03 Bull. Am. Phys. Soc. 9, No. 1, 19, BC4 (1964) C.D.Bowman, M.S.Coops, G.F.Auchampaugh, S.C.Fultz Subthreshold-Fission Cross Section of Am241 NUCLEAR STRUCTURE, Fission 242Am; measured not abstracted; deduced nuclear properties.
1964BO39 Phys.Rev. 133, B676 (1964) C.D.Bowman, G.F.Auchampaugh, S.C.Fultz Photodisintegration of U235 NUCLEAR REACTIONS 235U(γ, F), (γ, n), (γ, 2n), E=6-23 MeV; measured σ(E); deduced giant resonance structure. 235U deduced quadrupole moment.
doi: 10.1103/PhysRev.133.B676
1963BO48 Phys.Rev. 130, 1482 (1963) C.D.Bowman, G.Auchampaugh, S.C.Fultz Fission Cross Section Of U235 NUCLEAR REACTIONS 235U(n, n), 235U(n, f), E=-1.0-59.92 eV; measured products; deduced resonance parameters, σ, σ(E). Data were imported from EXFOR entry 12429.
doi: 10.1103/PhysRev.130.1482
1962BO01 Bull.Am.Phys.Soc. 7, No.1, 22, F2 (1962) C.D.Bowman, G.F.Auchampaugh, C.P.Jupiter, S.C.Fultz High-Resolution Neutron Time-of-Flight Measurements in the eV Region NUCLEAR STRUCTURE 236U; measured not abstracted; deduced nuclear properties.
1962BO04 Ann.Phys.(N.Y.) 17, 319 (1962) C.D.Bowman, E.G.Bilpuch, H.W.Newson s- and p-Wave Neutron Spectroscopy. Part VIII. Subshell Effect on Nuclear Level Spacing Near A = 50 NUCLEAR STRUCTURE 47Ti, 49Ti, 45Ca, 57Fe, 60Co, 56Mn, 55Fe, 55Cr, 52V, 42K; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0003-4916(62)90035-0
1962NE06 Bull.Am.Phys.Soc. 7, No.4, 289, G11 (1962) H.W.Newson, C.D.Bowman, E.G.Bilpuch Subshell Effect on Nuclear Level Spacing Near A = 50 NUCLEAR STRUCTURE 41Ca, 55Fe, 53Cr, 51Ti, 47Ti, 49Ti, 57Fe; measured not abstracted; deduced nuclear properties.
1961BI01 Bull.Am.Phys.Soc. 6, No.1, 69, X1 (1961) E.G.Bilpuch, K.K.Seth, C.D.Bowman, H.W.Newson Neutron Resonance Parameters in the keV Region
1961BI06 Ann.Phys.(N.Y.) 14, 387 (1961) E.G.Bilpuch, K.K.Seth, C.D.Bowman, R.H.Tabony, R.C.Smith, H.W.Newson s and p-Wave Neutron Spectroscopy Part VII. Widths of Neutron Resonances NUCLEAR STRUCTURE 131Te, 139Ba, 137Ba, 209Pb, 208Pb, 207Pb, 89Sr, 90Y, 61Ni, 57Fe, 59Ni, 58Fe, 41Ca, 51Cr, 55Cr, 55Fe, 53Cr, 45Ca, 49Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0003-4916(61)90063-X
1961BO03 Bull.Am.Phys.Soc. 6, No.1, 69, X2 (1961) C.D.Bowman, E.G.Bilpuch, R.H.Tabony, H.W.Newson High-Resolution Neutron Spectroscopy up to 650 keV NUCLEAR STRUCTURE 53Cr, 55Fe, 49Ti, 51Ti, 47Ti, 41Ca, 57Fe; measured not abstracted; deduced nuclear properties.
1961NE17 Ann.Phys.(New York) 14, 365 (1961) H.W.Newson, E.G.Bilpuch, F.P.Karriker, L.W.Weston, J.R.Patterson, C.D.Bowman s- and p-wave neutron spectroscopy: Part VI. Level density and neutron excess NUCLEAR REACTIONS 19F, Ca, 44Ca, 50,52,54Cr, Cr, Fe, 54Fe, Ti(n, X), E<420 keV; measured reaction products, En, In; deduced σ, resonance parameters.
doi: 10.1016/0003-4916(61)90062-8
1959BI19 Bull.Am.Phys.Soc. 4, No.1, 42, R4 (1959) E.G.Bilpuch, L.W.Weston, C.D.Bowman, H.W.Newson Recent total cross sections for Li, N, C, Cl, Co, Sr and Pb NUCLEAR REACTIONS Li, N, C, Cl, Co, Sr, Pb(n, X), E<0.13 MeV; measured reaction products, En, In; deduced σ, resonance parameters. Comparison with available data. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11266. 1958BI33 Bull.Am.Phys.Soc. 3, No.3, 164, B3 (1958) E.G.Bilpuch, L.W.Weston, C.D.Bowman, A.K.Furr, P.F.Nichols, H.W.Newson Narrow Neutron Resonances in the keV Region Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11599. Back to query form |