Nuclear Science References (NSR)

NUCLEAR REACTIONS ¹H, ²H(p-bar, X), E not given; calculated imaginary part of scattering length as a function of imaginary part of Woods-Saxon potential. Comparison with data. S-wave poles reaction mechanism proposed.

doi: 10.1007/s100500070098
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1999CA38 Eur.Phys.J. A 6, 9 (1999)

J.Carbonell, V.A.Karmanov

Deuteron Electromagnetic Form Factors in the Light-Front Dynamics

NUCLEAR STRUCTURE ²H; calculated electromagnetic form factors, structure functions; deduced influence of nucleon form factors. Relativistic nucleon-meson dynamics.

doi: 10.1007/s100500050311
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1998KA58 Nucl.Phys. A644, 165 (1998)

V.A.Karmanov

The Nucleon Wave Function in Light-Front Dynamics

NUCLEAR STRUCTURE ¹n, ¹H; calculated nucleon wave function spin structure. Light-front dynamics.

doi: 10.1016/S0375-9474(98)00579-X
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1998SC42 Phys.Rev. C58, 3093 (1998)

N.C.J.Schoonderwoerd, B.L.G.Bakker, V.A.Karmanov

Entanglement of Fock-Space Expansion and Convariance in Light-Front Hamiltonian Dynamics

doi: 10.1103/PhysRevC.58.3093
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1996KA19 Nucl.Phys. A602, 388 (1996)

V.A.Karmanov, J.-F.Mathiot

On the Calculation of the Nucleon Electromagnetic Form Factors in Light-Front Dynamics

doi: 10.1016/0375-9474(96)00101-7
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1996KA32 Nucl.Phys. A608, 316 (1996)

V.A.Karmanov

On Ambiguities of the Spin-1 Electromagnetic Form Factors in Light-Front Dynamics

doi: 10.1016/S0375-9474(96)00260-6
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1995CA03 Nucl.Phys. A581, 625 (1995)

J.Carbonell, V.A.Karmanov

Relativistic Deuteron Wave Function in the Light-Front Dynamics

NUCLEAR STRUCTURE ²H; calculated relativistic wave functions. Light front dynamics.

doi: 10.1016/0375-9474(94)00430-U
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1995CA19 Nucl.Phys. A589, 713 (1995)

J.Carbonell, V.A.Karmanov

Relativistic Wave Function of the np System in the J(π) = 0⁺ Continuous Spectrum State

doi: 10.1016/0375-9474(95)00129-O
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1995DE20 Nucl.Phys. A589, 697 (1995)

B.Desplanques, V.A.Karmanov, J.-F.Mathiot

Isovector Meson-Exchange Currents in the Light-Front Dynamics

doi: 10.1016/0375-9474(95)00088-I
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1994AM02 Nucl.Phys. A567, 919 (1994)

A.Amghar, B.Desplanques, V.A.Karmanov

The Deuteron Electrodesintegration Near Threshold in the Light-Front Dynamics

NUCLEAR REACTIONS ²H(e, X), E ≈ threshold; calculated electrodisintegration σ(θ, E). Light front dynamics.

doi: 10.1016/0375-9474(94)90334-4
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1994KA21 Nucl.Phys. A575, 520 (1994)

V.A.Karmanov, A.V.Smirnov

Deuteron Electromagnetic Form Factors in the Light-Front Dynamics

NUCLEAR STRUCTURE ²H; calculated charge, quadrupole, other form factors; deduced nonphysical contributions role. Light-front dynamics.

doi: 10.1016/0375-9474(94)90374-3
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1991KA39 Nucl.Phys. A532, 401c (1991)

V.A.Karmanov

Relativistic Effects in Deuteron and the Reaction D(e, e'p)n

NUCLEAR REACTIONS ²H(e, e'p), E=4 GeV; calculated σ(θ(e), θp, E(e')); deduced relativistic effects consequences.

doi: 10.1016/0375-9474(91)90716-J
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1988DA07 Nucl.Phys. A478, 635c (1988)

O.D.Dalkarov, V.A.Karmanov

Low-Energy Antiprotons as a New Probe of Nuclear Reaction Mechanism

NUCLEAR REACTIONS ¹²C, ²⁰⁸Pb(p-bar, p-bar), E=46.8 MeV; ⁴⁰Ca(p-bar, p-bar), E=47.8 MeV; ¹²C, ⁴⁰Ca(p-bar, p-bar), E=179.7 MeV; ²⁰⁸Pb(p-bar, p-bar), E=180.3 MeV; ²⁷Al, Cu(p-bar, p-bar), E at 514, 633 MeV/c; deduced reaction mechanism. Glauber-Sitenko approach.

doi: 10.1016/0375-9474(88)90902-5
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1988KA23 Pisma Zh.Eksp.Teor.Fiz. 47, 70 (1988); JETP Lett.(USSR) 47, 82 (1988)

V.A.Karmanov, A.V.Trukhov

Mechanisms for the Suppression of Annihilationless Breakup of Nuclei by Low-Energy Antiprotons

NUCLEAR REACTIONS ²H, ⁴He(p-bar, p-bar), (p-bar, X), E=50, 180 MeV; calculated elastic, reaction, total σ.

1987DA12 Yad.Fiz. 45, 688 (1987)

O.D.Dalkarov, V.A.Karmanov, A.V.Trukhov

Antiproton-Nucleus Scattering at Intermediate and Low Energies

NUCLEAR REACTIONS ¹²C, ²⁰Ne, ²⁷Al, ⁴⁰Ca, ⁶⁴Cu(p-bar, p-bar), E=20-200 MeV; calculated σ(E), σ(θ). Glauber approximation.

1986KA10 Nucl.Phys. A453, 707 (1986)

V.A.Karmanov

Relativistic Deuteron Wave Function from the ed → enp Reaction Cross Section

NUCLEAR REACTIONS ²H(e, e'p), E not given; calculated exclusive electrodisintegration σ, ratio. Relativistic approach.

doi: 10.1016/0375-9474(86)90258-7
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1985DA06 Pisma Zh.Eksp.Teor.Fiz. 41, 47 (1985); JETP Lett.(USSR) 41, 58 (1985)

O.D.Dalkarov, V.A.Karmanov

The Ratio of the Real Part to the Imaginary Part of the Elementary Amplitude for the Scattering of Hadrons by Nuclei

NUCLEAR REACTIONS ¹²C(p-bar, p-bar), E=179.7 MeV; calculated σ(θ); deduced (p-bar)(nucleon), (p-bar)(nucleus) scattering amplitude ratio. Eikonal approximation.

1985DA24 Nucl.Phys. A445, 579 (1985)

O.D.Dalkarov, V.A.Karmanov

Scattering of Low-Energy Antiprotons from Nuclei

NUCLEAR REACTIONS ¹²C(p, p), (p, p'), (p-bar, p-bar'), E=46.8, 179.7 MeV; ¹⁶O(p-bar, p-bar), ⁴⁰Ca(p-bar, p-bar), (p-bar, p-bar'), E=46.8 MeV; calculated σ(θ).

doi: 10.1016/0375-9474(85)90561-5
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1984DA20 Phys.Lett. 147B, 1 (1984)

O.D.Dalkarov, V.A.Karmanov

Elastic and Inelastic Scattering of Low Energy Antiprotons from ¹²C and ¹⁶O Nuclei

NUCLEAR REACTIONS ¹²C, ¹⁶O(p-bar, p-bar), (p-bar, p-bar'), E=46.8 MeV; calculated σ(θ). Glauber approximation.

doi: 10.1016/0370-2693(84)90580-X
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1984DA23 Pisma Zh.Eksp.Teor.Fiz. 39, 288 (1984); JETP Lett.(USSR) 39, 345 (1984)

O.D.Dalkarov, V.A.Karmanov

Scattering of Low-Energy Antiprotons by Carbon and Oxygen Nuclei

NUCLEAR REACTIONS ¹²C, ¹⁶O(p-bar, p-bar), (p-bar, p-bar'), E=46.8 MeV; calculated σ(θ). Glauber approximation.

1983KA42 Pisma Zh.Eksp.Teor.Fiz. 38, 311 (1983); JETP Lett.(USSR) 38, 372 (1983)

V.A.Karmanov

Manifestation in the Reaction ed → enp of Relativistic Effects in the Deuteron

NUCLEAR REACTIONS ²H(e, en), E=high; calculated σ(θ(e), E(e)) following breakup; deduced deuteron relativistic description relevance.

1982KA14 Yad.Fiz. 35, 848 (1982)

V.A.Karmanov

High Energy Hadron Scattering on ¹⁶O Nucleus in the Framework of the Nuclear Molecular Model

NUCLEAR REACTIONS ¹⁶O(p, p), (p, p'), (π, π), (π, π'), E ≈ 1 GeV; calculated σ(θ). ¹⁶O level deduced excitation mechanism. Nuclear molecular model.

1981KA29 Pisma Zh.Eksp.Teor.Fiz. 33, 300 (1981); JETP Lett.(USSR) 33, 284 (1981)

V.A.Karmanov

Sensitivity to Polarization and Quadrupolarization in Elastic Backward pd Scattering at an Energy in the Region of 1 GeV

NUCLEAR REACTIONS ²H(polarized p, p), E=1.03, 1.53 GeV; calculated analyzing power vs θ. ¹H(polarized d, d), E=1-2 GeV; calculated T₂₀(θ=180°). Single-nucleon exchange model.

1981KA45 Yad.Fiz. 34, 1020 (1981)

V.A.Karmanov

Polarization Phenomena in Elastic pd Backward Scattering at the Energy near 1 GeV

NUCLEAR REACTIONS ²H(polarized p, p), E ≥ 1 GeV; calculated analyzing power, deuteron alignment. One-nucleon exchange, background amplitudes.

1976BU19 Pisma Zh.Eksp.Teor.Fiz. 23, 302 (1976); JETP Lett.(USSR) 23, 272 (1976)

N.A.Burgov, M.K.Vlasov, S.A.Gerzon, Y.T.Kiselev, V.A.Karmanov, A.V.Manko, A.M.Martemyanov, Y.V.Terekhov, V.I.Ushakov, M.M.Chukamov

π-⁴He and π-¹⁶O Elastic Scattering and Excitation of the 3^- (6.13 MeV) Level of the ¹⁶O Nucleus by π^- Mesons at 1 GeV/c

NUCLEAR REACTIONS ⁴He, ¹⁶O(π^-, π^-), E=1.02 GeV/c; measured σ.

1975KA27 Pisma Zh.Eksp.Teor.Fiz. 21, 289 (1975); JETP Lett.(USSR) 21, 132 (1975)

V.A.Karmanov

Elastic Backward pd Scattering at High Energies

NUCLEAR REACTIONS ²H(p, p), E=0.316-2.5 GeV; calculated σ(θ).

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