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NSR database version of May 19, 2024.

Search: Author = M.Shmatikov

Found 22 matches.

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1999SH02      Phys.Rev. C59, 41 (1999)

M.Shmatikov

Pion Correlations and Two-Particle Bound States

doi: 10.1103/PhysRevC.59.41
Citations: PlumX Metrics

1999SH18      Phys.Rev. C59, 2241 (1999)

M.Shmatikov

Weak Chiral Lagrangian and π+ Emission in Λ4He

NUCLEAR STRUCTURE 4He; calculated hypernucleus pionic decay amplitudes; deduced possible decay mechanism.

doi: 10.1103/PhysRevC.59.2241
Citations: PlumX Metrics

1997SH03      Nucl.Phys. A612, 449 (1997)

M.Shmatikov

Why the Heavy-Flavored Strange Pentaquark Does not Exist

doi: 10.1016/S0375-9474(96)00410-1
Citations: PlumX Metrics

1996PO16      Yad.Fiz. 59, No 9, 1705 (1996); Phys.Atomic Nuclei 59, 1650 (1996)

M.Polyakov, M.Shmatikov

(p-bar)p Annihilation: Manifestations of the instanton-induced pair production of quarks ( Question )

NUCLEAR REACTIONS 1H(p-bar, X), E not given; analyzed qualitative strangeness production features; deduced nonperturbative QCD mechanism role.

1996SH01      Nucl.Phys. A596, 425 (1996)

M.Shmatikov

On the Width of Molecular States

doi: 10.1016/0375-9474(95)00402-5
Citations: PlumX Metrics

1995MA11      Phys.Rev. C51, 1576 (1995)

K.Maltman, M.Shmatikov

Factorization Contributions and the Breaking of the ΔI = 1/2 Rule in Weak (Lambda)Nρ and ΣNρ Couplings

doi: 10.1103/PhysRevC.51.1576
Citations: PlumX Metrics

1995SH15      Phys.Lett. 349B, 411 (1995)

M.Shmatikov

Hadronic Molecules: Meson-baryon hybrids

NUCLEAR STRUCTURE 2H; calculated binding energy; deduced best fit model parameters, one-pion exchange induced long-range correlations role. Hadronic molecules, meson-baryon hybrids.

doi: 10.1016/0370-2693(95)00287-U
Citations: PlumX Metrics

1994MA44      Phys.Lett. 331B, 1 (1994)

K.Maltman, M.Shmatikov

Large Violations of the ΔI = 1/2 Rule in (Lambda)N → NN

doi: 10.1016/0370-2693(94)90934-2
Citations: PlumX Metrics

1994SH04      Phys.Lett. 322B, 311 (1994)

M.Shmatikov

Two-Pion Exchange and the Role of Closed Channels in the Induced (Lambda)-Hyperon Decay

doi: 10.1016/0370-2693(94)91158-4
Citations: PlumX Metrics

1994SH27      Phys.Lett. 337B, 48 (1994)

M.Shmatikov

Induced (Lambda)-Hyperon Decay: How many nucleons are involved ( Question )

NUCLEAR STRUCTURE A=415; calculated nonmesonic hypernuclei decay widths ratio; deduced (lambda)NN-NNN channel role.

doi: 10.1016/0370-2693(94)91441-9
Citations: PlumX Metrics

1994SH28      Nucl.Phys. A580, 538 (1994)

M.Shmatikov

Mechanisms of Induced (Lambda)-Hyperon Decay Revisited: Contribution of correlated two-pion exchange

doi: 10.1016/0375-9474(94)90780-3
Citations: PlumX Metrics

1993GR12      Phys.Lett. 316B, 467 (1993)

I.Grach, M.Shmatikov

Parity Violation in pp-Scattering and Quark Degrees of Freedom

NUCLEAR REACTIONS 1H(polarized p, p), E ≤ 250 MeV; calculated longitudinal analyzing power vs E. Quark model, parity violation.

doi: 10.1016/0370-2693(93)91029-M
Citations: PlumX Metrics

1992SH02      Nucl.Phys. A539, 584 (1992)

M.Shmatikov

Isovector P-Odd ππ Exchange in the pp-System: Δ-Isobar contribution

NUCLEAR REACTIONS 1H(p, p), (polarized p, p), E=14-45 MeV; calculated isovector P-odd ππ-exchange interaction, analyzing power. Potential quark model, Δ-isobar contribution.

doi: 10.1016/0375-9474(92)90127-6
Citations: PlumX Metrics

1991GR07      Nucl.Phys. A529, 701 (1991)

I.Grach, M.Shmatikov

Weak NN Forces - from Mesons to Quarks

NUCLEAR REACTIONS 1H(polarized p, p), E=15, 45 MeV; calculated longitudinal analyzing power. Weak nucleon-nucleon interaction, parity violation mechanism.

doi: 10.1016/0375-9474(91)90593-U
Citations: PlumX Metrics

1990GR15      Z.Phys. A337, 321 (1990)

I.Grach, M.Shmatikov

Quark Contribution to Weak NN Interaction

NUCLEAR REACTIONS 1H(polarized p, p), E=15, 45 MeV; calculated weak quark interaction to longitudinal analyzing power.

1989GR26      Yad.Fiz. 50, 1108 (1989)

I.L.Grach, M.Zh.Shmatikov

Quark Contribution to Weak NN Interaction

NUCLEAR REACTIONS 1H(polarized p, p), E(cm)=15, 45 MeV; calculated contact weak interaction contribution to analyzing power.

1988SH41      Yad.Fiz. 47, 760 (1988); Sov.J.Nucl.Phys. 47, 488 (1988)

M.Zh.Shmatikov

Circular Polarization of Bremsstrahlung γ Rays in pp Scattering

NUCLEAR REACTIONS 1H(p, γ), E=low; calculated bremsstrahlung γ CP; deduced odd-parity effects role.

1988SH44      Yad.Fiz. 48, 979 (1988)

M.Zh.Shmatikov

P-Odd Effects in the Radiative Capture of π Mesons

NUCLEAR REACTIONS 1n, 1H(π, γ), E not given; calculated σ asymmetry; deduced P-odd effect role in radiative capture.

1987GR14      Yad.Fiz. 45, 933 (1987)

I.L.Grach, M.Zh.Shmatikov

Properties of Six-Quark Bag following from the Data on the Capture of Polarized Thermal Neutrons by Protons

NUCLEAR REACTIONS 1H(polarized n, γ), E=thermal; calculated γ CP. Six quark bag.

1985KO03      Yad.Fiz. 41, 222 (1985)

L.A.Kondratyuk, M.Zh.Shmatikov

EMC Effect and Multiquark Bags in Nuclei

NUCLEAR STRUCTURE 4He, 9Be, 27Al, Ca, Fe, Ag, 197Au; calculated large momentum transfer structure functions; deduced quark structure role. Deep inelastic lepton scattering input.

1984GR35      Yad.Fiz. 40, 440 (1984); Sov.J.Nucl.Phys. 40, 280 (1984)

I.L.Grach, M.Zh.Shmatikov

Circular Polarization of Photons Emitted in the Capture of Polarized Neutrons by Protons, and the Quark Composite Bag Model

NUCLEAR REACTIONS 1H(polarized n, γ), E=thermal; calculated γ CP; deduced nucleon M1, E2 contributions. 2H deduced quark admixture upper limit. Composite bag model.

1984KO28      Pisma Zh.Eksp.Teor.Fiz. 39, 324 (1984); JETP Lett.(USSR) 39, 389 (1984)

L.A.Kondratyuk, M.Zh.Shmatikov

Quark-Parton Distributions in Nuclei and the EMC Effect

NUCLEAR REACTIONS 4He(e, e), E not given; calculated form factor; deduced role of quark-parton distribution in nuclei.

NUCLEAR STRUCTURE Fe, 27Al, 2H; calculated structure function ratio; deduced role of quark-parton distribution in nuclei.

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Note: The following list of authors and aliases matches the search parameter M.Shmatikov: , M.Z.SHMATIKOV