NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = F.Gabbard Found 41 matches. 1987LA12 Phys.Rev. C35, 1265 (1987) C.E.Laird, D.Flynn, R.L.Hershberger, F.Gabbard Proton-90Zr Interaction at Sub-Coulomb Proton Energies NUCLEAR REACTIONS, ICPND 90Zr(p, p), E=2-7 MeV; 90Zr(p, p'γ), E=3.9-5.7 MeV; 90Zr(p, γ), E=1.9-5.7 MeV; measured σ(θ), γ yields; deduced radiative capture σ(E), reaction σ(E). 91Nb deduced γ strength function.
doi: 10.1103/PhysRevC.35.1265
1985FL01 Phys.Rev. C31, 87 (1985) D.S.Flynn, R.L.Hershberger, F.Gabbard Energy Dependence of the Absorptive Potential for Sub-Coulomb Energy Proton Bombardment of Zirconium and Molybdenum Isotopes NUCLEAR REACTIONS 92,94,96Zr, 95,98,100Mo(p, p), (p, n), E=2-6.5 MeV; measured σ(θ) vs E; deduced proton absorptive potential strength and energy dependence. Optical model.
doi: 10.1103/PhysRevC.31.87
1983LI01 Phys.Rev. C27, 93 (1983) Charge Exchange Reactions and Solar Neutrino Detection in 81Br NUCLEAR REACTIONS 81Br(p, n), (3He, t), E not given; calculated Gamow-Teller matrix element; deduced 81Br suitability as solar neutrino detector. Charge exchange reaction.
doi: 10.1103/PhysRevC.27.93
1982FL03 Phys.Rev. C26, 1744 (1982) D.S.Flynn, R.L.Hershberger, F.Gabbard Isospin and the Proton-Absorptive-Potential Anomaly near Mass 100 NUCLEAR REACTIONS 96Zr, 100Mo(p, n), E=2-6.5 MeV; measured total σ(E); deduced absorptive potential strengths. Optical model analysis.
doi: 10.1103/PhysRevC.26.1744
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
1979FL07 Phys.Rev. C20, 1700 (1979) D.S.Flynn, R.L.Hershberger, F.Gabbard Sub-Coulomb Proton Absorption for Isotopes of Zirconium and Molybdenum NUCLEAR REACTIONS 92,94Zr, 94,95,96,98Mo(p, n), E=1.7-6.7 MeV; measured total σ(E); deduced proton strength functions, absorptive potentials. Optical-model analysis.
doi: 10.1103/PhysRevC.20.1700
1979SC27 Phys.Rev. C20, 1706 (1979) R.Schrils, D.S.Flynn, R.L.Hershberger, F.Gabbard Comparison of Optical-Model and Lane-Model Analyses of Sub-Coulomb Protons on 92,94Zr NUCLEAR REACTIONS 92,94Zr(p, p), E=2.0-6.5 MeV; measured σ(θ) at 135°, 165°. Lane-model, optical-model analyses of elastic scattering, absorption σ.
doi: 10.1103/PhysRevC.20.1706
1978FL07 Phys.Rev. C18, 1566 (1978) D.S.Flynn, K.K.Sekharan, B.A.Hiller, H.Laumer, J.L.Weil, F.Gabbard Cross Sections and Reaction Rates for 23Na(p, n)23Mg, 27Al(p, n)27Si, 27Al(α, n)30P, 29Si(α, n)32S, and 30Si(α, n)33S NUCLEAR REACTIONS 23Na, 27Al(p, n), E=5.0-6.5 MeV; 27Al, 29,30Si(α, n), E=2.8-6.8 MeV; measured σ(E). 27Si(n, p), E=0-0.55 MeV; 30P(n, α), E=0.4-0.9 MeV; 32,33S(n, α), E=0-2.3 MeV; deduced σ(E); deduced nucleosynthesis reaction rates. 23Mg(n, p), E=0-3 MeV; calculated σ(E); deduced nucleosynthesis reaction rates.
doi: 10.1103/PhysRevC.18.1566
1978KE10 Phys.Rev. C18, 1938 (1978) B.D.Kern, F.Gabbard, R.G.Kruzek, M.R.McPherson, K.K.Sekharan, F.D.Snyder Energy Levels of 96Tc via the 96Mo(p, nγ)96Tc Reaction NUCLEAR REACTIONS 96Mo(p, nγ), E=3.7-5.8 MeV; measured tof, γ spectra; deduced Q. 96Tc deduced levels, γ-branching, π. Enriched targets.
doi: 10.1103/PhysRevC.18.1938
1976SE05 Nucl.Instrum.Methods 133, 253 (1976) K.K.Sekharan, H.Laumer, B.D.Kern, F.Gabbard A Neutron Detector for Measurement of Total Neutron Production Cross Sections NUCLEAR REACTIONS 7Li(p, n), E=1.9-4.2 MeV; 27Al(p, n), E=5.6-6.4 MeV; 88Sr(p, n), E=4.3-5.9 MeV; measured σ(E, En).
doi: 10.1016/0029-554X(76)90617-0
1973MC04 Phys.Rev. C7, 2097 (1973) Excited States of 94Tc Studied Through the Enhancement of Neutron and Gamma-Ray Yields from the 94Mo(p, n)94Tc Reaction at Isobaric Analog Resonances NUCLEAR REACTIONS 94Mo(p, nγ), E=5.35-6.1 MeV; measured σ(E;En, Eγ), Q. 94Tc deduced levels, γ-branching, J, π.
doi: 10.1103/PhysRevC.7.2097
1972EG01 Phys.Rev. C5, 1562 (1972) J.J.Egan, K.K.Sekharan, G.C.Dutt, J.E.Wiest, F.Gabbard 2.335-MeV Isobaric Analog Resonance in 51V + p and the Excited States Of 51Cr Studied via the (p, n) and (p, nγ) Reactions NUCLEAR REACTIONS 51V(p, n), E=1.5-5 MeV; measured σ(E;Eγ, En, θ(γ), θ(n)); 51V(p, p), E=2.1-2.45 MeV; measured σ(E). 51Cr deduced levels, J, π. 52Cr deduced isobaric analog resonances, J, π, L(p).
doi: 10.1103/PhysRevC.5.1562
1972GA36 Phys.Rev. C6, 2167 (1972) F.Gabbard, G.Chenevert, K.K.Sekharan Gamma Decay of States of 88Y Excited by the 88Sr(p, n)88Y Reaction NUCLEAR REACTIONS 88Sr(p, n), (p, nγ), E=5.0-6.4 MeV; measured σ(E;Eγ, θ(γ)). 88Y deduced levels, J, π.
doi: 10.1103/PhysRevC.6.2167
1971WI21 Phys.Rev. C4, 2061 (1971) J.E.Wiest, C.Robertson, F.Gabbard, M.T.McEllistrem Levels and Transition Rates in 53Mn from the 53Cr(p, n)53Mn and 53Cr(p, nγ)53Mn Reactions NUCLEAR REACTIONS 53Cr(p, n), (p, nγ), E=2.6-5.9 MeV; measured σ(E;En, θ(n), θ(γ)). 53Mn deduced levels, J, π, γ-mixing.
doi: 10.1103/PhysRevC.4.2061
1970EG02 Phys.Rev. C1, 1767 (1970) J.J.Egan, G.C.Dutt, M.McPherson, F.Gabbard Isobaric Analog Resonances in the 68Zn(p, n)68Ga Reaction from 4 to 5 MeV NUCLEAR REACTIONS 68Zn(p, n), E=4-4.15, 4.7-5.0 MeV; measured σ(E;En, θ). 68Ga deduced levels. 69Ga deduced isobaric analog resonances, level-width, J, π.
doi: 10.1103/PhysRevC.1.1767
1970GA23 Phys.Rev. C2, 2227 (1970) F.Gabbard, T.I.Bonner, R.Proffitt, R.Schrils 88Sr(p, n)88Y Reaction in the Proton Energy Range from 4.4 to 8.0 MeV NUCLEAR REACTIONS 88Sr(p, n), E < 8 MeV; measured σ(Ep, En). 89Y deduced isobaric analog resonances, level-width.
doi: 10.1103/PhysRevC.2.2227
1969DU02 Phys.Rev. 178, 1770 (1969) Excited States of 88Y Studied by the 88Sr(p, n)88Y Reaction NUCLEAR REACTIONS 88Sr(p, n)88Y, E=5.3-5.5 MeV; measured σ(En, θ). 88Y deduced levels, J, π.
doi: 10.1103/PhysRev.178.1770
1969DU03 Phys.Rev. 180, 1222 (1969) G.C.Dutt, F.Gabbard, R.Schrils, J.J.Egan Measurements and Analyses of the s1/2 Analog Resonance in the 88Sr(p, n)88Y Reaction NUCLEAR REACTIONS 88Sr(p, n), E=4.8-6.2 MeV; measured σ(E). 89Y deduced isobaric analog resonance.
doi: 10.1103/PhysRev.180.1222
1969RI08 Phys.Letters 29B, 649 (1969) P.Richard, F.Gabbard, A.C.Porter, F.F.Hopkins The 88Sr(p, γ)89Y Reaction Near the d5/2 Ground-State Analogue NUCLEAR REACTIONS 88Sr(p, γ), (p, n), E=4.9-5.2 MeV; measured σ(E;Eγ). 89Y deduced resonances, level-width. Enriched 88Sr target, Ge(Li) detector.
doi: 10.1016/0370-2693(69)90099-9
1968DU10 Phys.Rev. 176, 1289(1968) G.C.Dutt, F.Gabbard, J.J.Egan, J.E.Wiest 2- Isobaric Analog Resonance in the 89Y(p, n2)89Zr Reaction and the Excited States of 89Zr NUCLEAR REACTIONS 89Y(p, n), E=4.807 MeV; measured σ(Ep), σ(En, θ). 89Zr deduced levels, J, π.
doi: 10.1103/PhysRev.176.1289
1968YO05 Phys.Rev. 172, 1148 (1968) T.M.Young, J.D.Brandenberger, F.Gabbard 40Ar(p, n)40K Reaction from Threshold to 5.0 MeV NUCLEAR STRUCTURE 41K, 40K; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.172.1148
1967BA40 Phys.Rev. 161, 928 (1967) A.W.Barrows, Jr., F.Gabbard, J.L.Weil 19F(d, n)20Ne Reaction from 2.5 to 6.5 MeV NUCLEAR STRUCTURE 19F, 20Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.161.928
1966YO02 Bull.Am.Phys.Soc. 11, No.4, 510, A13 (1966) T.Young, F.Gabbard, J.D.Brandenberger, J.D.Reber, J.J.Egan Ar40(p, n)K40 Reaction, 2.3 - 5.0 MeV NUCLEAR STRUCTURE 40K; measured not abstracted; deduced nuclear properties.
1964BA40 Bull. Am. Phys. Soc. 9, No. 6, 665, Y3 (1964) A.Barrows, F.Gabbard, J.L.Weil, T.Young F19(d, n)Ne20 Reaction, 2.5-6.0 MeV NUCLEAR STRUCTURE 19F, 20Ne; measured not abstracted; deduced nuclear properties.
1964GA07 Bull.Am.Phys.Soc. 9, No.6, 649, Q1 (1964) F.Gabbard, J.D.Brandenberger, L.W.Cochran, T.Young A40(p, n) Reaction and Isobaric Analogs in K41 NUCLEAR STRUCTURE 41K; measured not abstracted; deduced nuclear properties.
1963BA49 Bull.Am.Phys.Soc.Southeastern Section, p. 7, E1, (November 1963); Bull.Am.Phys.Soc. 9, No.3, 347, E1 (1964) Energy Spectra of α Particles from the Al27(n, α)Ne24 Reaction Induced by 14.8 MeV Neutrons NUCLEAR STRUCTURE 24Na; measured not abstracted; deduced nuclear properties.
1963DU12 Nucl.Phys. 46, 336 (1963) J.L.Duggan, P.D.Miller, R.F.Gabbard A Study of the Reactions Be9(He3, n)C11, Li7(He3, n)B9 and C13(He3, n)O15 NUCLEAR STRUCTURE 13C, 9Be, 7Li; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90604-7
1962DU03 ORNL-3268, p.12 (1962) J.L.Duggan, P.D.Miller, R.F.Gabbard A Study of the Reactions Be9(He3, n)C11, Li7(He3, n)B9, and C13(He3, n)O15 NUCLEAR STRUCTURE 13C, 7Li, 9Be; measured not abstracted; deduced nuclear properties.
1962GA18 Phys.Rev. 128, 1276 (1962) Cross Sections for Charged Particle Reactions Induced in Medium Weight Nuclei by Neutrons in the Energy Range 12-18 MeV NUCLEAR STRUCTURE 24Na, 28Al, 27Mg, 48Sc, 64Cu, 52V, 56Mn; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.128.1276
1961BA31 Nuclear Phys. 28, 478 (1961) R.Bass, H.P.Haenni, T.W.Bonner, F.Gabbard Disintegration of K39 by Fast Neutrons NUCLEAR STRUCTURE 39K, 39Ar, 40K; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(61)91069-0
1961DA16 Nuclear Phys. 27, 448 (1961) E.A.Davis, F.Gabbard, T.W.Bonner, R.Bass The Disintegration of B10 and F19 by Fast Neutrons NUCLEAR STRUCTURE 10B, 20F, 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(61)90338-8
1961GA08 Bull.Am.Phys.Soc. 6, No.5, 416, B6 (1961) R.F.Gabbard, P.D.Miller, J.L.Duggan C13(He3, n)O15 Reaction
1961MI01 Bull.Am.Phys.Soc. 6, No.1, 60, TA2 (1961) P.D.Miller, J.L.Duggan, R.F.Gabbard Angular Yield of Neutrons from the T(p, n)He3 Reaction NUCLEAR STRUCTURE 9B, 11C, 15O; measured not abstracted; deduced nuclear properties.
1960WO01 Bull.Am.Phys.Soc. 5, No.2, 109, M9 (1960) D.M.Worley, Jr., R.Bass, T.W.Bonner, E.A.Davis, F.Gabbard Disintegration of O16 by Fast Neutrons NUCLEAR STRUCTURE 17O, 13C; measured not abstracted; deduced nuclear properties.
1959BA02 Bull.Am.Phys.Soc. 4, No.2, 95, C2 (1959) R.Bass, T.W.Bonner, E.A.Davis, F.Gabbard, T.Retz-Schmidt Search for Excited States of He5
1959BE66 Nuclear Phys. 14, 270 (1959) R.J.Bell, T.W.Bonner, F.Gabbard The disintegration of Ne20 by fast neutrons
doi: 10.1016/0029-5582(59)90012-4
1959DA01 Bull.Am.Phys.Soc. 4, No.2, 95, C5 (1959); Oral Report E.A.Davis, R.Bass, T.W.Bonner, F.Gabbard, T.Retz-Schmidt Disintegration of B10 by Neutrons
1959GA02 Bull.Am.Phys.Soc. 4, No.2, 97, G1 (1959) F.Gabbard, R.J.Bell, T.W.Bonner Study of the Reaction Ne20(n, α)O17
1959GA08 Phys.Rev. 114, 201 (1959) F.Gabbard, R.H.Davis, T.W.Bonner Study of the Neutron Reactions Li6(n, α)H3, F19(n, γ)F20, and I127(n, γ)I128
doi: 10.1103/PhysRev.114.201
1959GA14 Nuclear Phys. 14, 277 (1959) F.Gabbard, H.Bischel, T.W.Bonner The Disintegration of Nitrogen by Fast Neutrons
doi: 10.1016/0029-5582(59)90013-6
1959HA02 Bull.Am.Phys.Soc. 4, No.2, 97, G3 (1959); Oral Report H.Haenni, R.Bass, T.W.Bonner, R.H.Davis, F.Gabbard, T.Retz-Schmidt Investigation of the K39(n, p) and K39(n, α) Reactions
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