NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = J.Britz Found 18 matches. 1998BR09 At.Data Nucl.Data Tables 69, 125 (1998) Coefficients of the Isobaric Mass Equation and Their Correlations with Various Nuclear Parameters NUCLEAR STRUCTURE A=1-59; calculated isobaric multiplets mass coefficients. ATOMIC MASSES A=1-59; calculated isobaric multiplets mass coefficients.
doi: 10.1006/adnd.1998.0773
1997AN07 At.Data Nucl.Data Tables 66, 1 (1997) Coulomb Displacement Energies between Analog Levels for 3 ≤ A ≤ 239 COMPILATION A=3-249; compiled Coulomb displacement energies.
doi: 10.1006/adnd.1997.0740
1989AB08 J.Phys.Soc.Jpn. 58, 9 (1989) A.Abzouzi, M.S.Antony, J.B.Bueb, J.Britz, V.B.Ndocko Ndongue Prediction of Charge Radii of Medium and Heavy Spherical and Deformed Nuclei by Semi-Empirical Formalism NUCLEAR STRUCTURE A=12-242; analyzed charge radii data; deduced radial charge distributions. Least squares fits.
doi: 10.1143/JPSJ.58.9
1988AN15 At.Data Nucl.Data Tables 40, 9 (1988) Coulomb Displacement Energies between Analog Levels for 44 ≤ A ≤ 239 NUCLEAR STRUCTURE A=44-239; compiled Coulomb displacement energies.
doi: 10.1016/0092-640X(88)90003-4
1987AN01 J.Phys.(London) G13, 671 (1987) M.S.Antony, J.Britz, J.B.Bueb, J.Diaz, V.B.N'Docko N'Dongue Elastic Scattering of Tritons on 27Al between 2 and 3.3 MeV NUCLEAR REACTIONS 27Al(t, t), E=2-3.3 MeV; measured σ(θ). Si-Li detector. Folding model analyses.
doi: 10.1088/0305-4616/13/5/015
1987AN08 Nuovo Cim. 97A, 255 (1987) Systematics of Experimental Charge Radii of Elements and Elementary Particles NUCLEAR STRUCTURE Z=1-92; 1n; compiled experimental rms charge radii; deduced systematics.
doi: 10.1007/BF02734935
1986AN07 At.Data Nucl.Data Tables 34, 279 (1986) Predicted Masses and Excitation Energies in Higher Isospin Multiplets for 9 ≤ A ≤ 60 COMPILATION A=9-60; compiled mass excesses, T≤6 isospin mutiplet level energies.
doi: 10.1016/0092-640X(86)90005-7
1986AN10 Nuovo Cim. 91A, 283 (1986) Systematic of 21+, 02+, 22+, 41+ and 31- States in Even-Even Nuclei NUCLEAR STRUCTURE A=8-256; analyzed level systematics. A=74-254; calculated B(λ) ratios, asymmetry parameter. Davydov-Filippov model.
doi: 10.1007/BF02819306
1985AN17 Nuovo Cim. 88A, 265 (1985) M.S.Antony, J.Britz, J.B.Bueb, V.B.Ndocko-Ndongue Mass Excess of 20O and Isobaric Multiplet Mass Equation Applied to Assign T, J(π) Values to Analog States NUCLEAR STRUCTURE 21F, 21Ne, 21Na, 21Mg; calculated IAS energies, quartet mass equation coefficients. 26Si, 26Mg, 26Al; calculated Coulomb energy corrections. 40Ti, 40Sc, 40Ca, 40K, 40Ar; calculated T=2 quintet mass, IAS energies. RADIOACTIVITY 20O(β-) [from 18O(t, p), E=3.201 MeV]; deduced Q. Mass excess data input. NUCLEAR REACTIONS 16,18O(t, p), E=3.201 MeV; measured σ(Ep); deduced isobaric mass multiplet equation parameters. 20O deduced mass excess. 18O(t, p), E=3.201 MeV; 18O(α, 2p), 16O(18O, 16O), E not given; analyzed data; deduced Q.
1985AN28 At.Data Nucl.Data Tables 33, 447 (1985) M.S.Antony, J.Britz, J.B.Bueb, A.Pape Isobaric Mass Equation for A = 1-45 and Systematics of Coulomb Displacement Energies COMPILATION A=1-45; compiled T=1/2, 1, 3/2, 2 multiplet members mass excesses; deduced isobaric multiplet mass equation coefficients, Coulomb displacement energy systematics.
doi: 10.1016/0092-640X(85)90011-7
1984AN03 Nuovo Cim. 79A, 100 (1984) M.S.Antony, J.Britz, J.B.Bueb, A.Pape Mass Defect of 39Cl from 37Cl(t, p)39Cl: Coulomb displacement energy of the T = 5/2, J(π) = (3/2)+ states in 39Cl-39Ar NUCLEAR REACTIONS 37Cl(t, p), E=3.301 keV; measured σ(Ep), σ(θ); deduced Q. 39Cl deduced ground state mass defect. 39Cl, 39Ar deduced Coulomb displacement energy.
doi: 10.1007/BF02831081
1984AN17 Nuovo Cim. 81A, 414 (1984) M.S.Anthony, J.Britz, J.Bueb, A.Pape Masses of 21F, 25Na and 29Al by (t, p) Reactions and Coulomb Displacement Energies NUCLEAR REACTIONS 19F, 23Na, 27Al(t, p), E=3.3 MeV; measured σ(Ep), Q. 21F, 25Na, 29Al deduced ground state mass defects. 21F, 21Ne, 25Na, 25Mg, 29Al, 29Si deduced Coulomb energy differences, radius parameter.
1983AN15 J.Phys.(London) G9, L245 (1983) M.S.Anthony, J.Britz, J.B.Bueb, A.Pape Mass Defect of 13B and the Isobaric Mass Equation for the A = 13 Quartet NUCLEAR REACTIONS 11B(t, p), E=3.293 MeV; measured σ(Ep) at θ=30°; deduced Q, isobaric mass multiplet equation coefficients. 13B deduced mass defect.
doi: 10.1088/0305-4616/9/11/004
1976BR15 Nucl.Phys. A262, 189 (1976) J.Britz, A.Chevallier, J.Chevallier, B.Haas Lifetime of the 8040 keV State in 44Ti NUCLEAR REACTIONS 42Ca(α, 2nγ), (α, nαγ), (α, α'γ), E=31 MeV; measured γ(t), γγ(t). 44Ti level deduced T1/2, effective charge. 41,42Ca levels deduced T1/2. Pulsed beam electronic timing, enriched target, Ge(Li) detectors.
doi: 10.1016/0375-9474(76)90612-6
1975HA12 Phys.Rev. C11, 1179 (1975) Properties of Excited States of 49V NUCLEAR REACTIONS 46Ti(α, pγ), E=10.6 MeV; 49Ti(p, nγ), E=2.1 MeV; measured Eγ, pγ-, nγ-, γγ-coin, pγ, nγ, γγ(t), pγ(θ), DSA. 49V deduced levels, K, J, π, T1/2, γ-mixing, B(M1), B(E2), γ-branching.
doi: 10.1103/PhysRevC.11.1179
1972GE14 Nucl.Phys. A195, 65 (1972) C.Gehringer, B.Haas, J.Chevallier, J.Britz Probabilities de Transition γ dans le Noyau 58Co NUCLEAR REACTIONS 55Mn(α, nγ), E=7.9, 10 MeV; 58Fe(p, nγ), E=3.8 MeV; measured DSA, σ(Eγ, θ(nγ)). 58Co levels deduced T1/2, J, π.
doi: 10.1016/0375-9474(72)90721-X
1968GO06 J.Phys.(Paris) 29, 135 (1968) S.Gorodetzky, J.Britz, P.Chevallier, B.Rabin, G.Sutter, R.Drouin Desexcitation Electromagnetique du Niveau 4, 51 MeV de 48Ca NUCLEAR STRUCTURE 49Sc, 48Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1051/jphys:01968002902-3013501
1966GO33 Compt.Rend. 262B, 1455 (1966) S.Gorodetzky, J.Britz, P.Chevallier, R.Drouin, B.Rabin, G.Sutter Mise en Evidence de la Desexcitation Electromagnetique du Premier Niveau du 48Ca NUCLEAR REACTIONS 48Ca(p, p'), E=4.5-6.6 MeV; measured σ(E; Ep', Eγ). 48Ca deduced no J, π=0, + states. Ge(Li) detector.
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