NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = F.M.Lev Found 23 matches. 2000LE15 Nucl.Phys. A663-664, 365c (2000) A Poincare-Covariant Current Operator for Interacting Systems and Deuteron Electromagnetic Form Factors NUCLEAR STRUCTURE 2H; calculated form factors. Comparisons with data.
doi: 10.1016/S0375-9474(99)00618-1
2000LE35 Phys.Rev. C62, 064004 (2000) Poincare Covariant Current Operator and Elastic Electron-Deuteron Scattering in the Front-Form Hamiltonian Dynamics NUCLEAR REACTIONS 2H(e, e), E not given; calculated form factors, tensor polarization vs Q2. Front-form Hamiltonian dynamics, Poincare covariant current operator.
doi: 10.1103/PhysRevC.62.064004
1999LE21 Yad.Fiz. 62, No 6, 1098 (1999); Phys.Atomic Nuclei 62, 1031 (1999) Aspects of the Theory of Deep-Inelastic Scattering
1999LE55 Phys.Rev.Lett. 83, 5250 (1999) Deuteron Magnetic and Quadrupole Moments with a Poincare Covariant Current Operator in the Front-Form Dynamics NUCLEAR STRUCTURE 2H; calculated μ, Q. Poincare covariant current operator. Comparison with data.
doi: 10.1103/PhysRevLett.83.5250
1998BU04 Fiz.Elem.Chastits At.Yadra 29, 212 (1998); Phys.Part.Nucl. 29, 88 (1998) The Problem of Okubo-Zweig-Iizuka Rule Violation in Nucleon-Antinucleon Annihilation at Rest NUCLEAR REACTIONS 1H(p-bar, X), E at rest; calculated σ, branching ratios; deduced OZI-rule violation related features.
1998LE21 Few-Body Systems 24, 109 (1998) Problems with Initial- and Final-State Interactions in Deep-Inelastic Scattering
doi: 10.1007/s006010050081
1998LE31 Nucl.Phys. A641, 229 (1998) Electromagnetic and Weak Current Operators for Interacting Systems within the Front-Form Dynamics
doi: 10.1016/S0375-9474(98)00469-2
1998PA14 Phys.Rev. C57, 2655 (1998) Deep Inelastic Scattering and Final State Interaction in an Exactly Solvable Relativistic Model
doi: 10.1103/PhysRevC.57.2655
1996BU04 Phys.Rev. C53, 1453 (1996) Reply to ' Comment on ' Okubo-Zweig-Iizuka Rule Violation in the Reaction (p-bar)p → φπ0 ' ' NUCLEAR REACTIONS 1H(p-bar, X), E not given; analyzed, reviewed φπ branching ratio related features; deduced data statistics related uncertainities.
doi: 10.1103/PhysRevC.53.1453
1996BU07 Yad.Fiz. 59, No 2, 300 (1996); Phys.Atomic Nuclei 59, 280 (1996) Some Aspects of OZI-Rule Violation in the Reaction (p-bar)p → φπ0 NUCLEAR REACTIONS 1H(p-bar, X), E at ≤ 0.4 GeV/c; analyzed OZI-rule violation related features in φπ0 production.
1996LE16 Nucl.Phys. A606, 459 (1996) Some Aspects of Nuclear Deep Inelastic Scattering
doi: 10.1016/0375-9474(96)00222-9
1995BU12 Phys.Rev. C51, R2893 (1995) Okubo-Zweig-Iizuka Rule Violation in the Reaction (p-bar)p → φπ0 NUCLEAR REACTIONS 1H(p-bar, X), E not given; analyzed Okubo-Zweig-Iizuka rule violation explanation compatibility with absence of annihilation from P state.
doi: 10.1103/PhysRevC.51.R2893
1995BU19 Yad.Fiz. 58, No 3, 531 (1995); Phys.Atomic Nuclei 58, 480 (1995) Violation of the Okubo-Zweig-Izuki Rule in the Annihilation of Slow Antiprotons on Deuterons NUCLEAR REACTIONS 2H(p-bar, X), E=low; calculated relative differential branching ratio vs p(p) for (omega π-p), (φπ-p) production; deduced Okubo-Zweig-Izuki rule violation related features.
1994BU15 Phys.Lett. 329B, 143 (1994) On the Role of K(*)K Intermediate States in OZI-Rule Violating Reactions of Antiproton Annihilation NUCLEAR REACTIONS 1n, 1H(p-bar, X), E not given; calculated reactions branching ratio in annihilation process. On-shell approximation.
doi: 10.1016/0370-2693(94)90530-4
1994BU21 Yad.Fiz. 57, No 10, 1897 (1994); Phys.Atomic Nuclei 57, 1827 (1994) On the Role of K(*)K Intermediate States in OZI-Rule Violating Reactions of Antiproton Annihilation NUCLEAR REACTIONS 1n, 1H(p-bar, X), E not given; analyzed branching ratios data; deduced K(*)K intermediate states related features.
1994LE03 Nucl.Phys. A567, 797 (1994) On the Problem of Constructing the Electromagnetic-Current Operator of a Composite System
doi: 10.1016/0375-9474(94)90328-X
1993LE29 Riv.Nuovo Cimento Soc.Ital.Fis. 16, No.2, 1 (1993) Relativistic Quantum Mechanics and Its Applications to Few-Nucleon Systems
1990LE29 Fiz.Elem.Chastits At.Yadra 21, 1251 (1990); Sov.J.Part.Nucl. 21, 534 (1990) Calculation of the Triton Binding Energy in Relativistic Quantum Mechanics NUCLEAR STRUCTURE 3H; calculated binding energy. Relativistic corrections, Faddeev formalism, plane wave expansion.
1989KO49 Few-Body Systems 7, 55 (1989) L.A.Kondratyuk, F.M.Lev, V.V.Soloviev Relativistic Correction to the Triton Binding Energy in the Framework of Relativistic Hamiltonian Dynamics NUCLEAR STRUCTURE 3H; calculated binding energy, relativistic corrections. Relativistic Hamiltonian dynamics.
doi: 10.1007/BF01078437
1982KO31 Yad.Fiz. 36, 377; Sov.J.Nucl.Phys. 36, 220 (1982) L.A.Kondratyuk, F.M.Lev, L.V.Shevchenko Relativistic Model for πd Backward Scattering at Medium Energies NUCLEAR REACTIONS 2H(π, π), E at 0.4-1.5 GeV/c; calculated σ(θ), deuteron polarization tensor vs pion momentum; deduced dibaryon resonance contributions. Relativistic model.
1981KO09 Phys.Lett. 100B, 448 (1981) L.A.Kondratyuk, F.M.Lev, L.V.Shevchenko Possible Manifestation of Tribaryon Resonances in pD Backward Scattering NUCLEAR REACTIONS 2H(n, n), E=800 MeV; 2H(p, p), E=150-1000 MeV; analyzed σ(θ=180°); deduced tribaryon resonance contributions. Stretched rotating quark bag model.
doi: 10.1016/0370-2693(81)90602-X
1981KO17 Yad.Fiz. 33, 1208 (1981) L.A.Kondratyuk, F.M.Lev, L.V.Shevchenko Large-Angle Nucleon-Deuteron Scattering and Three-Baryon Resonances NUCLEAR REACTIONS 2H(p, p), E=0.3-1 GeV; calculated σ(θ); deduced three baryon resonance effects.
1977KO48 Yad.Fiz. 26, 294 (1977); Sov.J.Nucl.Phys. 26, 153 (1977) Elastic Backward pd Scattering in the Resonance Region NUCLEAR REACTIONS 2H(p, p), E=0.4-1 GeV; calculated σ(E, θ).
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