NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = Y.N.Uzikov Found 59 matches. 2023PL03 Phys.Atomic Nuclei 86, 1267 (2023) M.N.Platonova, N.T.Tursunbayev, Yu.N.Uzikov Elastic Polarized-Proton Scattering off 3He Nuclei in the Glauber Model with Accounting for Spin Dependence NUCLEAR REACTIONS 3He(p, p), E=156-1000 MeV; calculated σ(θ), proton analyzing powers on the basis of the Glauber diffraction model with allowance for the spin dependence of nucleon–nucleon amplitudes. Comparison with experimental data.
doi: 10.1134/S1063778824010447
2020UZ01 Bull.Rus.Acad.Sci.Phys. 84, 455 (2020) Short-Range NN Correlations in the Reaction 12C + p → 10A + pp + N
doi: 10.3103/S1062873820040346
2018IB01 Phys.Atomic Nuclei 81, 479 (2018) Elastic Deuteron Scattering on the 12C Nucleus within a Three-Body Model NUCLEAR REACTIONS 12C(d, d), E=270 MeV; calculated σ(θ) vs θcm, vector analyzing power using the Glauber theory; compared with published data.
doi: 10.1134/S1063778818040063
2017UZ01 Bull.Rus.Acad.Sci.Phys. 81, 739 (2017) Role of the Δ isobar excitation mechanism in the reaction pp → pp sπ0
doi: 10.3103/S1062873817060235
2016UZ01 Phys.Rev. C 94, 035501 (2016) Polarized proton-deuteron scattering as a test of time-reversal invariance NUCLEAR REACTIONS 2H(polarized p, p), E=100-1000 MeV; calculated Time-reversal violating but parity-conserving (TVPC) observables using spin-dependent Glauber theory. Scattering of transversal polarization of protons on deuterons with tensor polarization.
doi: 10.1103/PhysRevC.94.035501
2016UZ02 Eur.Phys.J. A 52, 243 (2016) Search for scaling onset in exclusive reactions with the lightest nuclei NUCLEAR REACTIONS 2H(d, n), (d, p), E=0.3-2.2 GeV; calculated σ(θ) using ONE (One-Nucleon-Exchange) mechanism; analyzed available σ(θ) data; deduced σ(θ) dimensional scaling.
doi: 10.1140/epja/i2016-16243-6
2015TE03 Bull.Rus.Acad.Sci.Phys. 79, 493 (2015); Izv.Akad.Nauk RAS, Ser.Fiz 79, 535 (2015) Searching for T -invariance violation effects in spin observables of pd -scattering
doi: 10.3103/S1062873815040322
2015UZ01 Phys.Rev. C 92, 014002 (2015) Null-test signal for T-invariance violation in pd scattering NUCLEAR REACTIONS 2H(p, p), E=100-1000 MeV; calculated spin observables for the pd elastic scattering, energy dependence of the time-reversal invariance violating but P-parity conserving (TVPC) cross section. Glauber theory for the double-polarized pd scattering. Comparison with experimental data.
doi: 10.1103/PhysRevC.92.014002
2014UZ01 Few-Body Systems 55, 1005 (2014) Spin Effects in the Interaction of Antiprotons with the Deuteron at Low and Intermediate Energies NUCLEAR REACTIONS 2H(p-bar, p-bar), E=179 MeV; calculated σ. Glauber calculations, comparison with available data.
doi: 10.1007/s00601-013-0792-0
2013UZ01 Phys.Rev. C 87, 054003 (2013) Elastic p(pol)d scattering and total p(pol)d cross sections NUCLEAR REACTIONS 2H(p-bar, p-bar), (p-bar, X), E=50-300 MeV; calculated σ(E, θ), analyzing powers, total σ(E). Glauber theory based on single-scattering (SS) and double-scattering (DS) mechanisms.
doi: 10.1103/PhysRevC.87.054003
2013UZ02 Phys.Rev. C 88, 027001 (2013) Elastic p(bar)d scattering and total p(bar)d cross sections reexamined NUCLEAR REACTIONS 2H(p-bar, p-bar), E<300 MeV; analyzed σ(θ), total σ, analyzing powers, Dependence of the longitudinal and transversal polarization on the beam energy. Glauber theory including the single and double p-bar, N scattering mechanisms.
doi: 10.1103/PhysRevC.88.027001
2011DU06 Physics of Part.and Nuclei 42, 251 (2011) Astrophysical S factors of reactions with light nuclei NUCLEAR REACTIONS 2,3H, 6Li, 12C(p, p), 12C(α, α), 4He(3He, 3He), (t, t), (d, d), E<10 MeV; calculated σ(θ), S-factors. Two-cluster model.
doi: 10.1134/S1063779611020031
2011HA16 Few-Body Systems 50, 275 (2011) Forward p(bar)d Elastic Scattering and Total Spin-Dependent pd Cross Sections NUCLEAR REACTIONS 2H(p-bar, X), E=20-300 MeV; calculated σ, σ(E). Glauber theory, Julich models, comparison with experimental data.
doi: 10.1007/s00601-010-0147-z
2011UZ01 Phys.Rev. C 84, 054011 (2011) Yu.N.Uzikov, J.Haidenbauer, B.A.Prmantayeva Antiproton scattering off 3He and 4He nuclei at low and intermediate energies NUCLEAR REACTIONS 3,4He(p-bar, p-bar'), E<300 MeV; analyzed differential Σ(θ), integrated elastic and total reaction cross sections; deduced dependence of longitudinal and transverse polarizations on beam energy using Glauber-Sitenko approach.
doi: 10.1103/PhysRevC.84.054011
2011VA14 Phys.Rev. C 84, 055207 (2011) Yu.Valdau, V.Koptev, S.Barsov, M.Buscher, A.Dzyuba, M.Hartmann, A.Kacharava, I.Keshelashvili, A.Khoukaz, S.Mikirtychiants, M.Nekipelov, A.Polyanskiy, F.Rathmann, H.Stroher, Yu.N.Uzikov, C.Wilkin Comparison of inclusive K+ production in proton-proton and proton-neutron collisions
doi: 10.1103/PhysRevC.84.055207
2009UZ01 Phys.Rev. C 79, 024617 (2009) Forward p(bar)d elastic scattering and total spin-dependent p(bar)d cross sections at intermediate energies NUCLEAR REACTIONS 1H, 2H(p-bar, p-bar), (p-bar, p-bar'), E=10-300 MeV; 1n(p-bar, p-bar), E=10-300 MeV; calculated spin-dependent total, σ(θ) using single-scattering approximation. Nucleon-antinucleon (N-barN) interaction model used for polarized deuteron target. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.024617
2008UZ01 Nucl.Phys. A801, 114 (2008) Spin observables of the reaction pd → 3Heη and quasi-bound 3He-η pole
doi: 10.1016/j.nuclphysa.2007.12.010
2007UZ01 Phys.Rev. C 75, 014008 (2007) Yu.N.Uzikov, J.Haidenbauer, C.Wilkin Dynamics of 1S0 diproton formation in the pd → [pp]sn and pN → [pp]sπ reactions in the GeV region NUCLEAR REACTIONS 2H(p, 2p), (p, d), E=0.5-2 GeV; calculated σ(θ), diproton formation features.
doi: 10.1103/PhysRevC.75.014008
2005UZ01 Pisma Zh.Eksp.Teor.Fiz. 81, 387 (2005); JETP Lett. 81, 303 (2005) Indication of Asymptotic Scaling in the Reactions dd → p3H, dd → n3He, and pd → pd NUCLEAR REACTIONS 2H(d, n), (d, p), E ≈ 0.5-1.2 GeV; 2H(p, p), E ≈ 0.5-4.5 GeV; analyzed σ(E, θ); deduced scaling behavior.
doi: 10.1134/1.1944067
2003HA10 Phys.Lett. B 562, 227 (2003) The reaction pd → (pp)n at high momentum transfer and short-range N N properties NUCLEAR REACTIONS 2H(p, 2p), E=0.6-1.9 GeV; analyzed σ(E, θ), sensitivity to short-range nucleon-nucleon interaction.
doi: 10.1016/S0370-2693(03)00580-X
2003UZ01 Phys.Rev. C 68, 014001 (2003) 3He structure and mechanisms of p 3He backward elastic scattering NUCLEAR REACTIONS 3He(p, p), E=0-2 MeV; calculated σ(θ=180°); deduced reaction mechanism features.
doi: 10.1103/PhysRevC.68.014001
2003UZ02 Eur.Phys.J. A 18, 317 (2003) Yu.N.Uzikov, V.I.Komarov, F.Rathmann, H.Seyfarth Short-range NN properties in the processes pd → dp and pd → (pp)n NUCLEAR REACTIONS 2H(p, d), (p, 2p), E=0.2-2.8 GeV; analyzed σ(θ); deduced short-range nucleon-nucleon properties.
doi: 10.1140/epja/i2002-10225-3
2002UZ01 Phys.Lett. 524B, 303 (2002) Yu.N.Uzikov, V.I.Komarov, F.Rathmann, H.Seyfarth Singlet-to-Triplet Ratio in the Deuteron Breakup Reaction pd → pnp at 585 MeV NUCLEAR REACTIONS 2H(p, np), E=585 MeV; analyzed σ(E, θ); deduced final state spin-triplet contribution. Faldt-Wilkin extrapolation theorem.
doi: 10.1016/S0370-2693(01)01398-3
2002UZ02 Pisma Zh.Eksp.Teor.Fiz. 75, 7 (2002); JETP Lett. 75, 5 (2002) On the Contribution of Three-Body Forces to Nd Interaction at Intermediate Energies NUCLEAR REACTIONS 1H(p, p), E=135-498 MeV; 2H(p, n), E=200 MeV; calculated σ(θ), Ay(θ); deduced three-nucleon force contribution. Comparison with data.
doi: 10.1134/1.1463105
2002UZ03 J.Phys.(London) G28, B13 (2002) A Possibility to Observe Short-Range NN Properties in the Deuteron Breakup pd → ppn NUCLEAR REACTIONS 2H(p, n), E=0.2-2.9 GeV; calculated σ(θ), analyzing power, spin-spin correlation parameter.
doi: 10.1088/0954-3899/28/4/401
2001AB34 Phys.Lett. 521B, 158 (2001) V.Abaev, M.Buscher, S.Dymov, M.Hartmann, A.Kacharava, V.I.Komarov, V.Koptev, V.Kurbatov, S.Mikirtychiants, M.Nekipelov, A.Petrus, H.Stroher, Yu.N.Uzikov, C.Wilkin, S.Yashenko Spin-Triplet Final-State Dominance in the pp → pnπ+ Reaction at 492 MeV NUCLEAR REACTIONS 1H(p, pπ+), E=492 MeV; measured proton momenta, σ(E, θ). Comparison with model predictions.
doi: 10.1016/S0370-2693(01)01229-1
2001UZ02 Phys.Lett. 511B, 191 (2001) Model-Independent Analysis of the Neutron-Proton Final-State Interaction Region in the pp → pnπ+ Reaction NUCLEAR REACTIONS 1H(p, pπ+), E=800 MeV; analyzed σ(E, θ), Ay(θ); deduced no final-state spin-singlet contribution.
doi: 10.1016/S0370-2693(01)00633-5
1999UZ02 Yad.Fiz. 62, No 12, 2292 (1999); Phys.Atomic Nuclei 62, 2109 (1999) Manifestation of the High-Momentum Component of the 3He Wave Function in Backward Elastic p3He Scattering NUCLEAR REACTIONS 3He(p, p), E < 3 GeV; calculated σ(θ=180°); deduced sensitivity to high-momentum component of target wave function.
1998BL08 Nucl.Instrum.Methods Phys.Res. A402, 386 (1998) L.D.Blokhintsev, A.V.Lado, Yu.N.Uzikov Backward Elastic p 3He Scattering at Energies 1-2 GeV NUCLEAR REACTIONS 3He(p, p), E=0.2-1.7 GeV; calculated backward scattering σ(θ); deduced sequential transfer role.
doi: 10.1016/S0168-9002(97)00868-1
1998SM04 Yad.Fiz. 61, No 3, 421 (1998); Phys.Atomic Nuclei 61, 361 (1998) Deuteron Disintegration by Protons in the Kinematics of Quasielastic Backward pd Scattering NUCLEAR REACTIONS 2H(p, 2p), E=0.2-2.2 GeV; calculated backscattered neutrons σ(E, θ); deduced off-shell effects. One-nucleon-exchange mechanism.
1998UZ01 Phys.Rev. C58, R36 (1998) Backward Elastic p-3He Scattering and High Momentum Components of the 3He Wave Function NUCLEAR REACTIONS 3He(p, p), E < 3 GeV; analyzed back-angle σ(θ); deduced role of 3He wave function high momentum components.
doi: 10.1103/PhysRevC.58.R36
1998UZ02 Fiz.Elem.Chastits At.Yadra 29, 1010 (1998); Phys.Part.Nucl. 29, 417 (1998) Backward Elastic p3He Scattering and Structure of the 3He Nucleus NUCLEAR REACTIONS 3He(p, p), E=0.5-2 GeV; calculated σ(θ=180°); deduced sequential pair transfer contribution, role of three-particle properties, other reaction mechanism features.
1998UZ03 Nucl.Phys. A644, 321 (1998) Structure of 3He in Backward Elastic p-3He Scattering NUCLEAR REACTIONS 2H, 3He(p, p), E < 3 GeV; calculated σ(θ=180°); deduced np-pair transfer mechanism role, other reaction mechanism features. Fadeev wave function, high-momentum components. Comparison with data.
doi: 10.1016/S0375-9474(98)00565-X
1998UZ04 Fiz.Elem.Chastits At.Yadra 29, 1405 (1998); Phys.Part.Nucl. 29, 583 (1998) Backward Elastic pd Scattering at Intermediate Energies NUCLEAR REACTIONS 2H(p, p), E ≈ 0.5-2 GeV; analyzed backward angle σ(E, θ); deduced exchange, single-scatter, resonance contributions.
1997KO15 Yad.Fiz. 60, No 3, 542 (1997); Phys.Atomic Nuclei 60, 468 (1997) Meson Production in pd → 3HeX Reaction in a Two-Step Model NUCLEAR REACTIONS 2H(p, X), E ≤ 3 GeV; calculated η-, φ-, ω-producttion associated σ(θ), spin-spin correlation parameter vs E. Two-step mechanism.
1997UZ01 Yad.Fiz. 60, No 9, 1603 (1997); Phys.Atomic Nuclei 60, 1458 (1997) Short-Range Structure of the Deuteron and the Process p + d → d + p NUCLEAR REACTIONS, ICPND 2H(p, p), E=0-4 GeV; calculated σ vs E, deuteron tensor polarization at 180°; 2H(p, p), E=1.016, 1.5, 2.09, 2.5 GeV; calculated σ(θ); 2H(p, p), E=1.5 GeV; calculated T20(θ); deduced rescattering effects.
1997UZ02 Yad.Fiz. 60, No 10, 1771 (1997); Phys.Atomic Nuclei 60, 1616 (1997) Contribution of the NN(*) Components of the Deuteron to the Reaction pd → dN(*) NUCLEAR REACTIONS 2H(p, dX), E=1-3 GeV; calculated N(*)-isobar emmision σ at 180°; deduced neutron exchange, kinematic features. Implications for study of nN(*)(1440), nN(*)(1710) deuteron components.
1996BL01 Nucl.Phys. A597, 487 (1996) L.D.Blokhintsev, A.V.Lado, Yu.N.Uzikov np Pair Transfer Mechanism for Backward Elastic p 3He Scattering at Intermediate Energies NUCLEAR REACTIONS 3He(p, p), E=0.5-1.7 GeV; analyzed σ(θ); deduced two-body transfer mechanism, rearrangement scattering related features.
doi: 10.1016/0375-9474(95)00411-4
1996KO22 Yad.Fiz. 59, No 5, 842 (1996); Phys.Atomic Nuclei 59, 804 (1996) V.I.Komarov, A.V.Lado, Yu.N.Uzikov Mechanisms of the Reaction pd → 3H(Λ)K+ NUCLEAR REACTIONS 2H(p, X), E=threshold-3 GeV; analyzed K+-, η-production σ(θ); deduced K+ production mechanism related features. One-, two-step mechanisms included.
1996KO64 Acta Phys.Pol. B27, 2977 (1996) Two-Step Mechanism of Meson Production in pd → 3He X Reaction
1995KO31 Yad.Fiz. 58, No 3, 525 (1995); Phys.Atomic Nuclei 58, 473 (1995) L.A.Kondratyuk, A.V.Lado, Yu.N.Uzikov Production of (Eta) Mesons Near the Threshold of the Reaction pD → 3He(Eta) and the Possibility of the Existence of a Quasi-Bound State in the (Eta)3He System NUCLEAR REACTIONS 2H(p, X), E ≈ 1-2.5 GeV; calculated σ(θ) vs E for eta production; deduced sub-threshold (eta+3He) system quasibound state possibility, parameters. Two-step mechanism.
1995KO42 J.Phys.(London) G21, L69 (1995) V.I.Komarov, A.V.Lado, Yu.N.Uzikov The pd → 3H(Λ)K+ Reaction Cross Section NUCLEAR REACTIONS 2H(p, K+), E=1.13-3 GeV; calculated hypernucleus production σ(θ) vs E, one-, two-step mechanisms.
doi: 10.1088/0954-3899/21/9/001
1993BL07 Yad.Fiz. 56, No 7, 139 (1993); Phys.Atomic Nuclei 56, 933 (1993) L.D.Blokhintsev, A.V.Lado, Yu.N.Uzikov Mechanism of Breakward Elastic p3He Scattering at Energies 1-1.5 GeV NUCLEAR REACTIONS 3He(p, p), E=0.9-1.7 GeV; calculated σ(θ); deduced np-pair transfer mechanism role.
1993LA20 Yad.Fiz. 56, No 9, 114 (1993); Phys.Atomic Nuclei 56, 1216 (1993) Exchange of an np Pair in Elastic p3He Backward Scattering at Intermediate Energies NUCLEAR REACTIONS 3He(p, p), E ≤ 1.6 GeV; calculated σ(θ); deduced dominant mechanism. Feynmann diagram approach, Faddeev five channel 3He wave function.
1993LA26 Bull.Rus.Acad.Sci.Phys. 57, 875 (1993) d(*) + p-Structure of 3He Nucleus in Elastic p, 3He Backward Scattering at E(p) = 0.5-1.7 GeV NUCLEAR REACTIONS 3He(p, p), E=0.5-1.7 GeV; calculated σ(θ); deduced role of singlet deuteron in 3He. Faddeev, cluster 3He wave functions.
1992LA06 Phys.Lett. 279B, 16 (1992) The Mechanism of Two-Nucleon Transfer in Backward Elastic p3He Scattering at Intermediate Energies NUCLEAR REACTIONS 3He(p, p), E ≈ 0.2-1.6 GeV; calculated σ(θ); deduced two-nucleon transfer mechanism. Glauber rescattering effects.
doi: 10.1016/0370-2693(92)91832-T
1992UZ01 Yad.Fiz. 55, 2374 (1992); Sov.J.Nucl.Phys. 55, 1319 (1992) Effects of Relativistic Dynamics in the Quasielastic Knockout Reaction d(e, ep)N(*) NUCLEAR REACTIONS 2H(e, e'p), E=high; calculated transverse, longitudinal structure functions. Relativistic three-body, light cone dynamics.
1990IM05 Yad.Fiz. 52, 1361 (1990); Sov.J.Nucl.Phys. 52, 862 (1990) Formation of a Singlet NN Pair in the Process p + d → N + (NN) at Large Momentum Transfers NUCLEAR REACTIONS 2H(p, n), E ≈ 0.6-1.8 GeV; calculated σ(θ(n), E(pp)) vs E, tensor analyzing power; deduced singlet NN-pair role.
1989IM01 Z.Phys. A332, 349 (1989) O.Imambekov, Yu.N.Uzikov, L.V.Shevchenko Elastic Backward pd-Scattering in Δ-Resonance Region NUCLEAR REACTIONS 2H(p, p), (polarized p, p), E=0.5-0.8 GeV; analyzed σ(θd, θp, Ep); deduced Δ-resonance role.
1989LA26 Yad.Fiz. 50, 1309 (1989) The Mechanism of Two-Nucleon Exchange in the Backward Elastic p3He Scattering NUCLEAR REACTIONS 3He(p, p), (n, n), E=2 MeV; calculated σ(θ); deduced reaction mechanism. K-matrix approach.
1988IM01 Yad.Fiz. 47, 1089 (1988) Analysis of the pp → pnπ+ Reaction at 800 MeV in Δ-Resonance Region NUCLEAR REACTIONS 1H(p, pπ+), E=800 MeV; calculated σ(θp, θ(π)) vs proton momentum; deduced meson exchange effect role.
1987IM04 Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 947 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.5, 107 (1987) Cross Section Ratio of Quasi-Elastic Knockout of Prompt Deuteron in the Reaction (p, nd) and (p, pd) and the Elastic pd-Reaction Mechanism at an Angle of 180° NUCLEAR REACTIONS 6,7Li(p, nd), (p, pd), E=670 MeV; calculated (p, nd) to (p, pd) σ(θ=180°) ratios.
1987ZH10 Fiz.Elem.Chastits At.Yadra 18, 323 (1987); Sov.J.Part.Nucl 18, 136 (1987) Quasielastic Knockout of Clusters by Fast Protons at Large Momentum Transfers and Nuclear Structure NUCLEAR REACTIONS, MECPD 4He(p, p), E at 50-900 MeV/c; calculated elastic σ(Ep, θp), σ(θ). 12C(p, pt), (p, p3He), (p, pα), (p, nt), (p, nα), (p, pd), E ≈ 0.7 GeV; calculated σ(E1, θ1, θ2), residue excitation spectra. 6Li(p, pd), E=670 MeV; calculated 4He excitation spectra.
1986IM01 Yad.Fiz. 44, 1459 (1986) O.Imambekov, Yu.N.Uzikov, L.V.Shevchenko Mechanisms of Production of Fast Deuterons in Quasielastic Knockout 6Li(p, pd)α in α - n - p Model of 6Li NUCLEAR REACTIONS 6Li(p, pd), (polarized p, pd), E=0.5-1.0 GeV; calculated σ(θd, θp, Ep), deuteron tensor polarization. Cluster model.
1986ZH03 Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 178 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.1, 172 (1986) M.A.Zhusupov, O.Imambekov, Yu.N.Uzikov Quasielastic Knockout of Fast Deuterons in the Reaction (p, pd) on 1p-Shell Nuclei at 670 MeV Energy NUCLEAR REACTIONS 12C, 6Li(p, pd), E=670 MeV; measured σ(θd, θp, Ep), σ(θp, θd) vs residual nucleus excitation; deduced deuteron emission mechanism.
1982ZH02 J.Phys.(London) G8, L99 (1982) The Role of Processes with Cluster Rearrangement in the (p, pα) Reaction at Large Momentum Transfer NUCLEAR REACTIONS 12C(p, pα), E=700 MeV; calculated σ(θα, θp, Ep), σ(θα, θp) vs excitation energy; deduced reaction mechanism. Feynman diagram method, one pion exchange, heavy particle stripping.
doi: 10.1088/0305-4616/8/7/003
1982ZH06 Yad.Fiz. 36, 1396 (1982) The Production of Fast α Particles in (p, pα) Reaction at High Energy NUCLEAR REACTIONS 12C(p, pα), E=665 MeV; calculated σ(θα, θp, Ep) vs excitation; deduced fast α-production mechanism. Quasifree knockout, Feynman diagrams.
1982ZH08 Izv.Akad.Nauk SSSR, Ser.Fiz. 46, 2084 (1982) Elastic pα-Scattering at Large Angles in the Resonance Energy Region NUCLEAR REACTIONS 4He(p, p), E ≈ 100-800 MeV; calculated σ(θ) vs E. Triton, nucleon exchange contribution, Feynman diagrams.
1981ZH03 J.Phys.(London) G7, 1621 (1981) Large-Angle pα Elastic Scattering at Energies in the Resonance Region NUCLEAR REACTIONS 4He(p, p), E=200-450 MeV; analyzed σ(θ, E). Feynman triangle diagrams.
doi: 10.1088/0305-4616/7/12/010
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