NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = S.L.Mintz Found 45 matches. 2007MI35 Eur.Phys.J. A 33, 299 (2007) New results for the production of Λ and Σ0 hyperons in antineutrino scattering from protons
doi: 10.1140/epja/i2007-10472-8
2006MI02 Nucl.Phys. A766, 219 (2006) The weak production of Λ particles in antineutrino-proton scattering and the contributions of the form factors NUCLEAR REACTIONS 1H(ν, X), E=threshold-9 GeV; calculated hyperon production σ(θ), form factors.
doi: 10.1016/j.nuclphysa.2005.11.024
2005MI03 Nucl.Phys. B(Proc.Supp.) S142, 68 (2005) The weak production of Λ hyperons from lepton-proton scattering NUCLEAR REACTIONS 1H(e, νX), E=194.25 MeV; 1H(μ-, νX), E=0.265 GeV; calculated hyperon production σ(θ).
doi: 10.1016/j.nuclphysbps.2005.01.013
2004MI36 Nucl.Phys. A741, 149 (2004) The weak production of Λ particles in muon and tau scattering from protons NUCLEAR REACTIONS 1H(μ-, ν), E=5 GeV; calculated hyperon production σ(θ). τ scattering also discussed.
doi: 10.1016/j.nuclphysa.2004.06.004
2002MI08 J.Phys.(London) G28, 451 (2002) Inclusive Neutrino and Antineutrino Reactions in 56Fe NUCLEAR REACTIONS 56Fe(ν, eX), (ν-bar, e+X), (ν, μ-X), (ν-bar, μ+X), E < 300 MeV; calculated σ. Comparisons with data.
doi: 10.1088/0954-3899/28/3/307
2001MI21 Nucl.Phys. A690, 711 (2001) The Weak Electroproduction of Σ0 in Electron-Proton Scattering NUCLEAR REACTIONS 1H(e, X), E=0.5-6.0 GeV; calculated Σ0 production associated σ(θ).
doi: 10.1016/S0375-9474(01)00364-5
2001MI37 Int.J.Mod.Phys. E10, 387 (2001) Inclusive Electron Neutrino Reactions in Nuclei and the Neutron Number NUCLEAR REACTIONS 12,13C, 56Fe, 127I(ν, eX), E=spectrum; calculated σ. Comparison with data.
doi: 10.1142/S0218301301000599
2000MI10 Int.J.Mod.Phys. E9, 1 (2000) S.L.Mintz, G.M.Gerstner, M.A.Barnett, M.Pourkaviani Polarized Parity Violating Electron Scattering on 3H and Its Relation to the 3He Case NUCLEAR REACTIONS 3H(polarized e, e), E=1, 2, 4 GeV; 3He(polarized e, e), E=2 GeV; calculated asymmetry parameter vs angle, figures of merit for parity-violating scattering; deduced sensitivity to strange quark contributions.
doi: 10.1016/S0218-3013(00)00002-7
2000MI14 Nucl.Phys. A672, 503 (2000) Inclusive Neutrino Reactions in 13C NUCLEAR REACTIONS 13C(ν, e), (ν, μ), E < 300 MeV; calculated σ.
doi: 10.1016/S0375-9474(00)00049-X
1999MI10 Nucl.Phys. A650, 371 (1999) S.L.Mintz, G.M.Gerstner, M.A.Barnett, M.Pourkaviani Polarized Parity Violating Electron Scattering on 3He NUCLEAR REACTIONS 3He(polarized e, e), E=1, 4 GeV; calculated asymmetry parameters, figures of merit for parity violation measurement, possible strange quark contributions.
doi: 10.1016/S0375-9474(99)00123-2
1999MI18 Int.J.Mod.Phys. E8, 197 (1999) S.L.Mintz, G.M.Gerstner, M.A.Barnett, M.Pourkaviani Exclusive and Inclusive Anti-Neutrino Reactions in 3He NUCLEAR REACTIONS 3He(ν, e+), (ν, μ+), E < 1 GeV; 3He(ν, e-X), E < 300 MeV; calculated σ.
doi: 10.1142/S021830139900015X
1999MI28 Nucl.Phys. A657, 303 (1999) The Reaction e- + p → Λ + ν and the Contributions of the Individual Form Factors to the Differential Cross Section NUCLEAR REACTIONS 1H(e, X), E=0.5, 1, 2, 4, 6 GeV; calculated Λ production σ(θ), form factors contributions.
doi: 10.1016/S0375-9474(99)00344-9
1998MI13 Int.J.Mod.Phys. E7, 275 (1998) S.L.Mintz, G.M.Gerstner, M.A.Barnett, M.Pourkaviani The Neutrino Reaction in 3H NUCLEAR REACTIONS 3H(ν, e), (ν, μ-), E < 1 GeV; calculated σ.
doi: 10.1142/S0218301398000117
1997MI12 Int.J.Mod.Phys. E6, 111 (1997) S.L.Mintz, M.A.Barnett, G.M.Gerstner, M.Pourkaviani The Reaction e- + p → ν(e) + n at Intermediate Energies NUCLEAR REACTIONS 3,1H(e-, ν), E=0.1-6 GeV; calculated σ(θ).
doi: 10.1142/S021830139700007X
1996MI03 Nucl.Phys. A598, 367 (1996) S.L.Mintz, M.A.Barnett, G.M.Gerstner, M.Pourkaviani The Reaction e- + 3He → ν(e) + 3H and the Determination of the Weak Nuclear Form Factors NUCLEAR REACTIONS 3He(e-, ν), E=0.1-6 GeV; calculated σ(θ); deduced individual nuclear form factors contributions.
doi: 10.1016/S0375-9474(96)00009-7
1996MI17 Nucl.Phys. A609, 411 (1996) The Exclusive Muon Neutrino Reaction, ν(μ) + 12C → μ- + 12N(gs), and Present and Future Experiments NUCLEAR REACTIONS 12C(ν, μ-), E=threshold-300 MeV; calculated σ(E). Different assumptions for pseudoscalar form factor contribution.
doi: 10.1016/S0375-9474(96)00266-7
1995MI03 Nucl.Phys. A584, 665 (1995) Inclusive Neutrino Reactions in 127I NUCLEAR REACTIONS 127I(ν, e-X), (ν, X), E=threshold to 53 MeV; calculated σ(E). Two different models, Michel spectrum neutrinos.
doi: 10.1016/0375-9474(94)00490-E
1995MI11 Nucl.Phys. A589, 724 (1995) The Anti-Neutrino Reaction in 127I NUCLEAR REACTIONS 127I(ν-bar, X), E=threshold-53 MeV; calculated σ; deduced relation to σ for 127I(ν, X).
doi: 10.1016/0375-9474(95)00185-4
1995MI18 Nucl.Phys. A594, 346 (1995) The Inclusive Muon Neutrino Reaction in 12C NUCLEAR REACTIONS 12C(ν, μ-X), E=threshold-300 MeV; calculated charged current inclusive σ(E).
doi: 10.1016/0375-9474(95)00361-4
1995MI23 Int.J.Mod.Phys. E4, 163 (1995) Polarized and Unpolarized Inclusive Electron Scattering in Nuclei and the Inclusive Neutrino Cross-Section NUCLEAR REACTIONS 12C(e, e'X), E ≈ 20-120 MeV; calculated σ(θ) vs E. 12C(polarized e, e'X), E ≈ 20-120 MeV; calculated parity violating asymmetry vs E, θ; deduced relationship to inclusive σ for incident ν.
doi: 10.1142/S0218301395000079
1994MI15 J.Phys.(London) G20, 925 (1994) Inclusive Neutrino Reactions in Nuclei NUCLEAR REACTIONS 12C(ν, X), E=threshold-100 MeV; calculated reaction σ(E) for inclusive electron emission. Interaction hadronic part tensor elements from total muon capture rates, scattering data.
doi: 10.1088/0954-3899/20/6/008
1994PO10 Nucl.Phys. A573, 501 (1994) Inclusive Inelastic Neutral-Current Neutrino Reactions in 12C and the Charged-Current Reaction NUCLEAR REACTIONS 12C(ν, νX), E=thermal-100 MeV; calculated neutral current σ; deduced relationship to charge current σ.
doi: 10.1016/0375-9474(94)90228-3
1993MI03 Phys.Rev. C47, 873 (1993) Parity-Violating Muon and Heavy Lepton Scattering in the 12C → 12C(*) Nuclear Transition NUCLEAR REACTIONS 12C(polarized μ, μ'), E not given; calculated asymmetry vs lepton energy.
doi: 10.1103/PhysRevC.47.873
1992MI09 J.Phys.(London) G18, 1485 (1992) Calculations for Parity Violating Electron Scattering in the 12C → 12C(*) Nuclear Transition NUCLEAR REACTIONS 12C(polarized e, e'), E=0.1-4 GeV; calculated asymmetry parameter vs E; deduced Weinberg angle, nuclear form factor dependences. Parity violating electron scattering.
doi: 10.1088/0954-3899/18/9/010
1991PO04 J.Phys.(London) G17, 1139 (1991) Neutrino Reaction in 13C NUCLEAR REACTIONS 13C(ν, e-), (ν, μ-), E=threshold-280 MeV; calculated σ(E). Electron scattering, β-decay data input.
doi: 10.1088/0954-3899/17/7/012
1990PO01 J.Phys.(London) G16, 569 (1990) Neutrino-Induced Neutral Current Reaction in 12C NUCLEAR REACTIONS 12C(ν, ν'), E=20-180 MeV; calculated σ(E) for ν(e), ν(μ).
doi: 10.1088/0954-3899/16/4/007
1989MI11 J.Phys.(London) G15, 1241 (1989) Exclusive Neutrino-Induced Charged-Current Reactions in 12C at Large Momentum Transfer NUCLEAR REACTIONS 12C(ν, μ-), (ν, e-), E ≤ 300 MeV; calculated σ(θ), σ vs E.
doi: 10.1088/0954-3899/15/8/019
1989MI21 Phys.Rev. C40, 2458 (1989) Theoretical Calculations for Neutrino-Induced Charged Current Reactions in 12C and Recent Experimental Results NUCLEAR REACTIONS 12C(ν, e-), E=threshold-130 MeV; 12C(ν, μ-), E=threshold-160 MeV; calculated σ(E, θ), <σ> over projectile spectrum; deduced possible effects of large pseudoscalar interaction. New values for form factor.
doi: 10.1103/PhysRevC.40.2458
1988MI11 Phys.Rev. C37, 2249 (1988) Electron-Induced Weak Processes in 12C and the Behavior of the Cross Section Near the Maximal Angle NUCLEAR REACTIONS 12C(e-, ν), E=0.5, 1.5, 3, 6 GeV; calculated σ(θ, E) near the maximal angle; deduced contributions from individual form factors.
doi: 10.1103/PhysRevC.37.2249
1988MI20 Phys.Rev. C38, 2443 (1988) Lepton-Induced Weak Interactions in Nuclei in the 1 to 3 GeV Range NUCLEAR REACTIONS 12C(ν, μ), (e-, ν), E=1-3 GeV; calculated σ(θ).
doi: 10.1103/PhysRevC.38.2443
1987MI01 Phys.Rev. C35, 263 (1987) Muon and Neutrino Production in Inclusive Proton-12C Reactions NUCLEAR REACTIONS 12C(p, μ+ν), E(cm)=1076 MeV; calculated inclusive σ. Elementary particle type treatment.
doi: 10.1103/PhysRevC.35.263
1987MI08 J.Phys.(London) G13, 591 (1987) Pion Photoproduction in 13C and the Axial Current Form Factor in the Time-Like Region NUCLEAR REACTIONS 13C(γ, π-), E ≈ threshold; calculated σ(θ). Analytic continuation, gauge invariance.
doi: 10.1088/0305-4616/13/5/008
1987MI17 Phys.Rev. C36, 860 (1987) Weak Electron-Induced Charged Current Reactions in 12C at Intermediate Energies NUCLEAR REACTIONS 12C(e, ν), E=0.5-6 GeV; calculated σ(θ(12B)). First-order weak interaction.
doi: 10.1103/PhysRevC.36.860
1986MI09 Phys.Rev. C33, 2082 (1986) Reaction p + 12C → 13C + μ+ + ν(μ) and the Weak Form Factors in the Timelike Region NUCLEAR REACTIONS 12C(p, μ+), E(cm)=1.06-1.085 GeV; calculated σ(E); deduced nuclear partially conserved axial vector current threshold anomaly role detection.
doi: 10.1103/PhysRevC.33.2082
1985KI01 Phys.Rev. C31, 274 (1985) Total Neutrino-Scattering Cross Sections and Total Muon-Capture Rates in Nuclei NUCLEAR REACTIONS 12C(ν, μ-), E=150-250 MeV; calculated σ(E); deduced total muon capture rate, total inclusive neutrino scattering σ relation.
doi: 10.1103/PhysRevC.31.274
1985MI21 Phys.Rev. C32, 2179 (1985) Neutrino Reactions in 13C and the Behavior of the Axial Current Form Factor NUCLEAR REACTIONS 13C(ν, μ-), E=119, 170, 260 MeV; calculated σ(θ). 13C(ν, μ-), E=110-260 MeV; calculated σ; deduced axial current form factor dependence.
doi: 10.1103/PhysRevC.32.2179
1984MI11 Phys.Rev. C30, 1585 (1984) Neutral and Charged Current Inclusive Neutrino Reactions in 12C and the Pion-Electroproduction Cross Section NUCLEAR REACTIONS 12C(ν, μ-), E=150-250 MeV; 12C(ν, ν), E=50-150 MeV; calculated inclusive σ(E). Elementary particle method, total muon capture rate, inclusive pion electroproduction σ input.
doi: 10.1103/PhysRevC.30.1585
1983MI09 Phys.Rev. C28, 556 (1983) Differential Muon-Capture Rate and the Deuterium Form Factors in the Timelike Region NUCLEAR REACTIONS 2H(μ, ν), E at rest; calculated total capture rate, differential capture rate vs En. Different axial current form factor assumptions.
doi: 10.1103/PhysRevC.28.556
1983MI14 Phys.Rev. C28, 1389 (1983) Reaction μ- + 6Li → 3H + 3H + ν(μ) and the Axial Current Form Factor in the Timelike Region NUCLEAR REACTIONS 6Li(μ-, ν), E at rest; calculated differential capture rate, two-tritium target breakup. Different axial current form factor assumptions.
doi: 10.1103/PhysRevC.28.1389
1982BO11 Phys.Rev. C25, 1986 (1982) Nuclear Form Factors in the Timelike Region and Photoproduction of Pions in Nuclei NUCLEAR REACTIONS 6Li, 12C(γ, π+), E=threshold; calculated form factors. Gauge invariance, partially conserved axial vector current.
doi: 10.1103/PhysRevC.25.1986
1982MI05 Phys.Rev. C25, 1671 (1982) Neutrino Reactions in 12C NUCLEAR REACTIONS 12C(ν, μ-), E=threshold-250 MeV; calculated σ(θ), σ(total). 12C(ν-bar, e+), (ν, ν), (ν-bar, ν-bar), E=threshold-250 MeV; calculated σ(total); deduced pseudotensor form factor effects. Elementary particle model.
doi: 10.1103/PhysRevC.25.1671
1981MI01 Phys.Rev. C23, 421 (1981) Neutral Current Neutrino Reactions and Weak Charged Current Processes in Deuterium NUCLEAR REACTIONS 2H(ν, νn), (ν-bar, nν-bar), (ν, pe-), (ν, ne+), E=10-150 MeV; 2H(ν, μ-p), E=5-20 MeV; calculated σ(disintegration). Elementary particle model, SU(2) commutation relations.
doi: 10.1103/PhysRevC.23.421
1980MI14 Phys.Rev. C22, 2507 (1980) Pion Reactions in Deuterium and the Muon-Capture Rate and Weak Form Factors NUCLEAR REACTIONS 2H(μ-, ν), (π-, γ), E at rest; calculated capture rates, σ(photoproduction). Elementary particle model.
doi: 10.1103/PhysRevC.22.2507
1979MI04 Phys.Rev. C19, 476 (1979) Muon Capture in 6Li in the Ditriton Channel by the Use of the Elementary Particle Model NUCLEAR REACTIONS 6Li(μ-, νt), E at rest; calculated capture rate, differential capture rate. Elementary-particle model.
doi: 10.1103/PhysRevC.19.476
1979MI12 Phys.Rev. C20, 286 (1979) Differential Muon-Capture Rate for the Reaction μ- + 6Li → 3H + 3H + ν(μ) NUCLEAR REACTIONS 6Li(μ-, νt), E=at rest; calculated differential muon-captue rate. Elementary particle model.
doi: 10.1103/PhysRevC.20.286
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