NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = F.Tabakin Found 39 matches. 2006JU02 Phys.Rev. C 73, 055204 (2006) B.Julia-Diaz, B.Saghai, T.-S.H.Lee, F.Tabakin Dynamical coupled-channels approach to hadronic and electromagnetic kaon-hyperon production on the proton NUCLEAR REACTIONS 1H(π-, K0X), (γ, K+X), E(cm) ≈ 1.6-2.3 GeV; calculated hyperon production associated σ(θ), recoil polarization asymmetry, excitation functions. Dynamical coupled-channels approach, comparison with data.
doi: 10.1103/PhysRevC.73.055204
2005JU08 Nucl.Phys. A755, 463c (2005) B.Julia-Diaz, B.Saghai, F.Tabakin, W.-T.Chiang, T.-S.H.Lee, Z.Li Dynamical coupled-channel study of K+Λ photoproduction NUCLEAR REACTIONS 1H(γ, K+X), E(cm) ≈ 1.6-2.3 GeV; calculated hyperon production σ(θ), excitation functions. Constituent quark model, coupled-channels approach, comparison with data.
doi: 10.1016/j.nuclphysa.2005.03.056
2004CH32 Phys.Rev. C 69, 065208 (2004) W.-T.Chiang, B.Saghai, F.Tabakin, T.-S.H.Lee Dynamical coupled-channel model of kaon-hyperon interactions NUCLEAR REACTIONS 1H(π-, K0X), E=high; calculated hyperon production σ(θ), σ, polarization asymmetries. Dynamical coupled-channels model.
doi: 10.1103/PhysRevC.69.065208
2004KR13 Few-Body Systems 34, 57 (2004) R.Krivec, V.B.Mandelzweig, F.Tabakin Quasilinear Approximation and WKB
doi: 10.1007/s00601-004-0045-3
2001CH65 Phys.Lett. 517B, 101 (2001) W.-T.Chiang, F.Tabakin, T.-S.H.Lee, B.Saghai Coupled-Channel Study of γp → K+Λ NUCLEAR REACTIONS 1H(γ, K+), E(cm)=1.6-2.5 GeV; analyzed σ; deduced parameters. Coupled-channels approach.
doi: 10.1016/S0370-2693(01)00945-5
2000KE16 Phys.Rev. C62, 064601 (2000) Mixing of the f0 and a0 Scalar Mesons in Threshold Photoproduction NUCLEAR REACTIONS 1H(γ, X), E ≈ threshold; calculated scalar meson production associated invariant mass distributions, role of isospin-violating mixing.
doi: 10.1103/PhysRevC.62.064601
2000KL01 Phys.Rev. C61, 015501 (2000) Constraints on Vector Meson Photoproduction Spin Observables
doi: 10.1103/PhysRevC.61.015501
2000KL04 Nucl.Phys. A663-664, 425c (2000) Constraints in Vector Meson Photoproduction
doi: 10.1016/S0375-9474(99)00674-0
2000KL08 Nucl.Phys. A675, 325c (2000) Vector Meson Photoproduction - Model Independent Aspects
doi: 10.1016/S0375-9474(00)00275-X
1998KL08 Phys.Rev. C58, 1086 (1998) W.M.Kloet, W.-T.Chiang, F.Tabakin Spin Information from Vector-Meson Decay in Photoproduction
doi: 10.1103/PhysRevC.58.1086
1998KL22 Acta Phys.Pol. B29, 3331 (1998) W.M.Kloet, W.-T.Chiang, F.Tabakin Spin Self-Analysis of Photoproduced Meson and Baryon Resonances
1998SA06 Nucl.Phys. A628, 645 (1998) Quark-Antiquark Bound States within a Dyson-Schwinger Bethe-Salpeter Formalism
doi: 10.1016/S0375-9474(97)00648-9
1997CH10 Phys.Rev. C55, 2054 (1997) Completeness Rules for Spin Observables in Pseudoscalar Meson Photoproduction
doi: 10.1103/PhysRevC.55.2054
1997SA06 Phys.Rev. C55, 917 (1997) Pseudoscalar Meson Photoproduction: From known to undiscovered resonances NUCLEAR REACTIONS 1H(γ, π+), E=220, 650 MeV; analyzed T-asymmetry data. Density matrix approach, multipole truncated framework.
doi: 10.1103/PhysRevC.55.917
1996PI01 Phys.Rev. C53, 593 (1996) M.Pichowsky, C.Savkli, F.Tabakin Polarization Observables in Vector Meson Photoproduction
doi: 10.1103/PhysRevC.53.593
1996SA01 Phys.Rev. C53, 66 (1996) Nodal Trajectories of Spin Observables and Kaon Photoproduction Dynamics NUCLEAR REACTIONS 1H(γ, X), E=0.92, 1.4 GeV; calculated sixteen observables for kaon photoproduction. Three different dynamical models.
doi: 10.1103/PhysRevC.53.66
1996SA05 Phys.Rev. C53, 1132 (1996) Multipole Analysis of Spin Observables in Vector Meson Photoproduction
doi: 10.1103/PhysRevC.53.1132
1994TA04 Nucl.Phys. A570, 311c (1994) Polarization Observables in Vector Meson Photoproduction
doi: 10.1016/0375-9474(94)90297-6
1991TA16 Phys.Rev. C44, 1749 (1991) F.Tabakin, R.A.Eisenstein, Y.Lu Spin Observables at Threshold for the Reaction (p-bar)p → (Lambda-bar)Lambda NUCLEAR REACTIONS 1H(p-bar, X), E at 1.435-1.697 GeV/c; analyzed σ, polarization, spin-correlation data for (Lambda)(Lambda-bar) production; deduced partial wave amplitudes.
doi: 10.1103/PhysRevC.44.1749
1990LI02 Phys.Rev. C41, 665 (1990) Coupled-Channels Study of Antiproton-Proton Reactions NUCLEAR REACTIONS 1H(p-bar, p-bar), (p-bar, K+), (p-bar, π+), E at 590-780 MeV/c; calculated σ(θ). Coupled-channels analysis.
doi: 10.1103/PhysRevC.41.665
1989SA51 Ann.Phys.(New York) 195, 223 (1989) Electroproduction of Charged Pions from Light Nuclei NUCLEAR REACTIONS 1H(e, π+), E not given; 12C(e, π+), E=195 MeV; 10B(e, π+), E=158.5, 163, 160.3, 165 MeV; calculated σ(θ, E(π)). DWIA, Blomquist-Laget pion photoproduction operator.
doi: 10.1016/0003-4916(89)90245-5
1988RO11 Ann.Phys.(New York) 184, 33 (1988) A.S.Rosenthal, D.Halderson, K.Hodgkinson, F.Tabakin Hypernuclear Photoproduction NUCLEAR REACTIONS 1H(γ, K+), E at 1.2 GeV/c; calculated σ(θ). 12C(γ, K+), E=1.8 GeV; calculated σ(θ, E). 208Pb(γ, K+), E at 1.84 GeV/c; calculated σ(θ).
doi: 10.1016/0003-4916(88)90269-2
1986DY02 Phys.Rev. C33, 1699 (1986) Medium Effects in Photopion Reactions NUCLEAR REACTIONS 14N(γ, π+), E=173, 200 MeV; 12C(γ, π+), 13C(γ, π-), E not given; calculated σ(θ); deduced medium effects. DWIA, coordinate space.
doi: 10.1103/PhysRevC.33.1699
1986RO25 Phys.Lett. 182B, 143 (1986) A.S.Rosenthal, D.Halderson, F.Tabakin Hypernuclear Photoproduction NUCLEAR REACTIONS 12C, 208Pb(γ, K+), E=1.8 GeV/c; calculated hypernuclear excitation σ(θ); deduced spin-flip mode dominance, distortion effects. Full Coulomb, optical distortions, complete photoproduction vertex.
doi: 10.1016/0370-2693(86)91565-0
1986SI13 Phys.Rev. C34, 637 (1986) Radiative Pion Capture on 13C NUCLEAR REACTIONS 13C(π+, γ), E=115.5 MeV; calculated radiative capture σ(θ); deduced small core polarization, precursor effects. 13C(γ, π-), E not given; calculated σ(θ). DWIA.
doi: 10.1103/PhysRevC.34.637
1983TO17 Phys.Rev. C28, 1725 (1983) Propagator Nonlocalities in Nuclear Photopion Reactions NUCLEAR REACTIONS 14,15N, 12,13C(γ, π+), E not given; calculated σ(θ). DWIA, pion, nucleon, isobar propagator nonlocality effects.
doi: 10.1103/PhysRevC.28.1725
1981RE04 Phys.Rev. C23, 2652 (1981) Radiative Capture of In-Flight Pions by 15N NUCLEAR REACTIONS 15N(π+, γ), E=50, 80, 116, 150, 180 MeV; calculated σ(θ), σ(total); deduced pion propagator, enhanced isobar contributions. In-flight capture, shell model form factors, distorted waves.
doi: 10.1103/PhysRevC.23.2652
1981SI09 Ann.Phys.(New York) 135, 71 (1981) Charged Pion Photoproduction from Light Nuclei NUCLEAR REACTIONS 12C(γ, π-), E=17, 50, 116 MeV; 12C(γ, π+), E=17, 29 MeV; 10B(γ, π+), E=15, 50, 112 MeV; 14N(γ, π-), E=30, 50, 80 MeV; 14N(γ, π+), E=30, 50, 80, 112 MeV; 6Li(γ, π+), E=38 MeV; calculated σ(θ). DWIA, optical potentials, pion-nucleus final state interactions.
doi: 10.1016/0003-4916(81)90144-5
1980RO15 Phys.Rev. C22, 711 (1980) Kaon-Nucleus Scattering NUCLEAR REACTIONS 12C(K+, K+), (K+, K+'), (K-, K-), (K-, K-'), E=100-1000 MeV; calculated σ(θ), total σ; deduced role of kaon distortions, nuclear motion. DWIA, optical model.
doi: 10.1103/PhysRevC.22.711
1980SI07 Phys.Rev. C21, 1039 (1980) Role of Gamow-Teller Suppression and M1 Radiative Widths on π- Photoproduction from 14N NUCLEAR REACTIONS 14N(γ, π-), E=145-325 MeV; calculated σ(θ), total σ; deduced structure effects, pion distortions, Blomqvist-Laget operator.
doi: 10.1103/PhysRevC.21.1039
1979SI16 Phys.Rev.Lett. 43, 1476 (1979) M.K.Singham, G.N.Epstein, F.Tabakin Photoproduction of 0-200 MeV Pions from 12C and 7Li NUCLEAR REACTIONS 7Li, 12C(γ, π-), E not given; calculated σ. Blomqvist-Laget operator, distorted waves.
doi: 10.1103/PhysRevLett.43.1476
1978EP01 Phys.Rev. C17, 702 (1978) G.N.Epstein, M.K.Singham, F.Tabakin 12C(γ, π-)12N(g.s.) Near Threshold NUCLEAR REACTIONS 12C(γ, π-), E ≤ threshold + 10 MeV; calculated σ(E), total σ(E).
doi: 10.1103/PhysRevC.17.702
1978EP02 Phys.Rev. C17, 1501 (1978) G.N.Epstein, F.Tabakin, C.M.Vincent, A.Gal, L.S.Kisslinger Distorted-Wave Impulse-Approximation Evaluation of Sum Rule for Hypernuclear Formation in Forward (K-, π-) NUCLEAR REACTIONS 12C, 40Ca(K-, π-), E=900 MeV/c; calculated σ.
doi: 10.1103/PhysRevC.17.1501
1977CO04 Phys.Rev. C15, 1379 (1977) Kaon-Nucleus Inelastic Scattering NUCLEAR REACTIONS 12C(K+, K+'), E < 300 MeV; calculated σ(E, θ).
doi: 10.1103/PhysRevC.15.1379
1974KI01 Phys.Rev. C9, 188 (1974) Pion-Nucleus Coordinate-Space Potential NUCLEAR REACTIONS 12C(π, π), E=120-280 MeV; calculated σ(θ): optical potential deduced from multiple-scattering theory.
doi: 10.1103/PhysRevC.9.188
1974LA22 Nucl.Phys. A231, 445 (1974) The Role of Off-Shell Scattering in the Pion Optical Potential NUCLEAR REACTIONS 12C(π, π), E=30-280 MeV; calculated σ(E, θ).
doi: 10.1016/0375-9474(74)90508-9
1973PH01 Phys.Rev. C7, 1803 (1973) S.C.Phatak, F.Tabakin, R.H.Landau Pion-Oxygen Elastic Scattering in the 3-3 Resonance Region NUCLEAR REACTIONS 16O(π-, π-), E=60-300 MeV; calculated σ(E, θ).
doi: 10.1103/PhysRevC.7.1803
1972LE21 Nucl.Phys. A191, 332 (1972) Relativistic Nuclear Matter Calculations and the Deficiency of One-Boson Exchange Potentials
doi: 10.1016/0375-9474(72)90519-2
1972RI15 Phys.Rev. C6, 1143 (1972) K.C.Richards, M.I.Haftel, F.Tabakin Estimate of the Importance of Retardation in Nuclear Binding
doi: 10.1103/PhysRevC.6.1143
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