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NSR database version of April 11, 2024.

Search: Author = N.Mobed

Found 11 matches.

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2005MO38      Phys.Rev. C 72, 045204 (2005)

N.Mobed, J.Zhang, D.Singh

Pion-induced pion production in heavy-baryon chiral perturbation theory

NUCLEAR REACTIONS 1H(π-, π+π-), (π-, π-π0), (π-, 2π0), (π+, 2π+), (π+, π+π0), E ≈ 150-400 MeV; calculated reaction σ, σ(θ), polarization observables. Heavy-baryon chiral perturbation theory of chiral order three, comparisons with data.

doi: 10.1103/PhysRevC.72.045204
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1999CH13      Nuovo Cim. 114B, 199 (1999)

C.X.Chen, G.Papini, N.Mobed, G.Lambiase, G.Scarpetta

Maximal Acceleration Corrections to the Lamb Shift of Muonic Hydrogen

ATOMIC PHYSICS, Mesic-atoms 1H; calculated muonic hydrogen Lamb shift corrections.

1999LE08      Phys.Rev. D59, 073002 (1999)

R.Lewis, N.Mobed

Isospin Violation and the Proton's Neutral Weak Magnetic Form Factor

NUCLEAR STRUCTURE 1H; calculated neutral weak magnetic form factor, isospin violation effects, resonance contributions. Two-flavor chiral perturbation theory.

doi: 10.1103/PhysRevD.59.073002
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1998FE02      Nucl.Phys. A631, 735c (1998)

H.W.Fearing, R.Lewis, N.Mobed, S.Scherer

Radiative and Non Radiative Muon Capture on the Proton in Heavy Baryon Chiral Perturbation Theory

doi: 10.1016/S0375-9474(98)00101-8
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1997FE10      Phys.Rev. D56, 1783 (1997)

H.W.Fearing, R.Lewis, N.Mobed, S.Scherer

Muon Capture by a Proton in Heavy Baryon Chiral Perturbation Theory

NUCLEAR REACTIONS 1H(μ-, n), E not given; calculated form factors. Chiral Perturbation Theory, Ecker-Mojzis Lagrangian.

doi: 10.1103/PhysRevD.56.1783
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1992ZH34      Can.J.Phys. 70, 711 (1992)

J.Zhang, N.Mobed

Threshold Pion Photoproduction in the Skyrme Model

NUCLEAR REACTIONS 1H(γ, π+), 1n(γ, π-), 1H(γ, π0), E=threshold; measured threshold photoproduction amplitudes. Skyrme model.

doi: 10.1139/p92-114
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1987MO13      Phys.Lett. 190B, 25 (1987)

N.Mobed, S.S.M.Wong

Symmetry in (p, p'γ) and Relativistic Models of Intermediate Energy Proton-Nucleus Scattering

NUCLEAR REACTIONS 12C(p, p'γ), E=150, 500 MeV; calculated correlation function vs proton scattering angle. Relativistic models.

doi: 10.1016/0370-2693(87)90834-3
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1987ZH08      Nucl.Phys. A466, 623 (1987)

X.Q.Zhu, N.Mobed, S.S.M.Wong

Impulse Approximation and Spin Observables in Inelastic Nucleon-Nucleus Scattering

NUCLEAR REACTIONS 12C, 28Si(p, p'), (polarized p, p'), E=150, 200 MeV; calculated polarization, analyzing power, spin transfer parameters. Impulse approximation.

doi: 10.1016/0375-9474(87)90460-X
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1986MO12      Nucl.Phys. A456, 644 (1986)

N.Mobed, S.S.M.Wong, X.Zhu

Gamma-Ray Angular Correlation in Intermediate Energy Proton-Nucleus Scattering

NUCLEAR REACTIONS 12C(polarized p, p'γ), E=200 MeV; calculated γp(θ), γ-, proton polarization; deduced scattering amplitude independent parameters.

doi: 10.1016/0375-9474(86)90080-1
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1986ZH04      Phys.Lett. 174B, 142 (1986)

X.Zhu, S.S.M.Wong, N.Mobed

Difference between P and A(y) in forward Angle Inelastic Proton-Nucleus Scattering at Intermediate Energies

NUCLEAR REACTIONS 12C(polarized p, p'), E=150 MeV; 24Mg, 28Si(polarized p, p'), E=200 MeV; calculated polarization, analyzing power difference vs θ; deduced kinematic effect role.

doi: 10.1016/0370-2693(86)90729-X
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1981MO06      Can.J.Phys. 59, 255 (1981)

N.Mobed, M.L.Chatterjee, P.Beeley, J.K.P.Lee

Deuteron Induced Fission in 233U

NUCLEAR REACTIONS, Fission 233U(d, F), E=18, 31, 44 MeV; measured relative independent yields for 86,87,88,89,90,91,92,93,94Rb, 115,116,117,118,119,120,121,122,123,124,125,126In, 130,131,132,133,134,135,136,137,138,139,140,141,142,143Cs; deduced neutron multiplicity, mass distribution width, charge division mechanism. Moment analysis.

doi: 10.1139/p81-033
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2447.

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