NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = A.Titov Found 67 matches. 2020ST07 Phys.Rev. C 101, 045201 (2020) I.I.Strakovsky, L.Pentchev, A.I.Titov Comparative analysis of wp, φp, and J/γp scattering lengths from A2, CLAS, and GlueX threshold measurements NUCLEAR REACTIONS 1H(γ, X), E=1673.1-2216.7 MeV; analyzed differential σ(E, θ) data from CLAS experiment at Jefferson Laboratory within the vector-meson dominance (VMD) model; deduced total σ(E), and φp scattering lengths. Comparison with results of other experimental data.
doi: 10.1103/PhysRevC.101.045201
2017KI04 Phys.Rev. C 95, 055206 (2017) Decay angular distributions of K* and D* vector mesons in pion-nucleon scattering NUCLEAR REACTIONS 1H(π-, Κ0Λ), at pion momentum of 6.15 GeV/c; calculated unpolarized differential cross sections, spin-density matrix elements, angular distributions and azimuthal angle distributions for K* and D* excitations using quark-gluon string model.
doi: 10.1103/PhysRevC.95.055206
2014KI10 Few-Body Systems 55, 783 (2014) H.-Ch.Kim, H.-Y.Ryu, A.Titov, A.Hosaka φN photoproduction coupled with the K Λ* channel
doi: 10.1007/s00601-014-0883-6
2013EJ03 Phys.Rev. C 88, 054610 (2013) H.Ejiri, A.I.Titov, M.Boswell, A.Young Neutrino-nuclear response and photonuclear reactions NUCLEAR REACTIONS 76Se, 100Mo(polarized γ, n), E in MeV to GeV region; calculated angular distribution of neutrons emitted from 1-, 2+, 1+ and 2- photonuclear excitations. Use of electromagnetic (EM) matrix element to evaluate the single β+ (weak) matrix element associated with the 0νββ matrix element through IAS and non-IAS states. Discussed current and planned experimental facilities for such experiments.
doi: 10.1103/PhysRevC.88.054610
2008TI01 Eur.Phys.J. A 35, 307 (2008) Search for exotics in γD → φnp reactions near threshold NUCLEAR REACTIONS 1H(γ, p), E=2.02 GeV; 2H(γ, np), E=1.5-3.6 GeV; analyzed φ production σ.
doi: 10.1140/epja/i2007-10559-2
2008TI04 Phys.Rev. C 78, 025201 (2008) Exclusive charm production in (p-bar)p collisions at √ s ≤ 15 GeV
doi: 10.1103/PhysRevC.78.025201
2008TI06 Phys.Rev. C 78, 038201 (2008) Selected vector-meson decay distributions in reactions of polarized photons with protons
doi: 10.1103/PhysRevC.78.038201
2007TI10 Phys.Rev. C 76, 035202 (2007) Photoproduction of the φ meson off the deuteron near threshold
doi: 10.1103/PhysRevC.76.035202
2007TI13 Phys.Rev. C 76, 048202 (2007) A.I.Titov, T.Nakano, S.Date, Y.Ohashi Differential cross section of φ-meson photoproduction at threshold
doi: 10.1103/PhysRevC.76.048202
2007TI14 Phys.Rev. C 76, 065211 (2007) In-medium modification and decay asymmetry of ω mesons in cold nuclear matter
doi: 10.1103/PhysRevC.76.065211
2006TI07 J.Phys.(London) G32, 1097 (2006) A.I.Titov, M.Fujiwara, K.Kawase Parity non-conservation in nuclear excitation by circularly polarized photon beam NUCLEAR REACTIONS 14C, 14N, 15,16O, 18,19F, 20,21Ne(polarized γ, γ'), E ≈ 100-11000 keV; calculated parity non-conservation effects.
doi: 10.1088/0954-3899/32/8/002
2006TI09 Phys.Rev. C 74, 055206 (2006) A.I.Titov, B.Kampfer, S.Date, Y.Ohashi Θ+ formation in inclusive γD → pK- X NUCLEAR REACTIONS 2H(γ, pK-X), E=1.7-3.5 GeV; calculated missing mass spectra, pentaquark signal.
doi: 10.1103/PhysRevC.74.055206
2005NO02 Nucl.Phys. B(Proc.Supp.) S138, 221 (2005) M.Nomachi, P.Doe, H.Ejiri, S.R.Elliott, J.Engel, M.Finger, J.A.Formaggio, K.Fushimi, V.Gehman, A.Gorin, M.Greenfield, R.Hazama, K.Ichihara, Y.Ikegami, H.Ishii, T.Itahashi, P.Kavitov, V.Kekelidze, K.Kuroda, V.Kutsalo, I.Manouilov, K.Matsuoka, H.Nakamura, T.Ogama, A.Para, K.Rielage, A.Rjazantsev, R.G.H.Robertson, Y.Shichijo, T.Shima, Y.Shimada, G.Shirkov, A.Sissakian, Y.Sugaya, A.Titov, V.Vatulin, O.E.Vilches, V.Voronov, J.F.Wilkerson, D.I.Will, S.Yoshida MOON (Mo Observatory Of Neutrinos) for double beta decay
doi: 10.1016/j.nuclphysbps.2004.11.053
2005TI03 Phys.Rev. C 71, 035203 (2005) A.I.Titov, H.Ejiri, H.Haberzettl, K.Nakayama Some aspects of Θ+ parity determination in the reaction γN → Θ+ (K-bar) → NK(K-bar) NUCLEAR REACTIONS 1n, 1H(γ, K+K-), E ≈ threshold; calculated pentaquark production associated invariant mass spectra, spin observables. Implications for parity determination discussed.
doi: 10.1103/PhysRevC.71.035203
2005TI06 Phys.Rev. C 71, 062201 (2005) Spin correlations in the reaction π± (D(pol)) → (Σ(pol))±Θ+ and the parity of Θ+ NUCLEAR REACTIONS 2H(π+, Σ+X), (π-, Σ-X), E ≈ threshold; analyzed spin-transfer coefficients, deuteron spin anisotropy, sensitivity to pentaquark parity. Polarized target.
doi: 10.1103/PhysRevC.71.062201
2005TI10 Phys.Rev. C 72, 035206 (2005); Erratum Phys.Rev. C 72, 049901 (2005) A.I.Titov, B.Kampfer, S.Date, Y.Ohashi Coherent Θ+ and Λ(1520) photoproduction off the deuteron
doi: 10.1103/PhysRevC.72.035206
2004FU13 Phys.Rev. C 69, 065503 (2004) Parity violation in deuteron photodisintegration NUCLEAR REACTIONS 2H(polarized γ, np), (γ, np), E ≈ threshold; calculated σ, parity-nonconserving asymmetry, energy dependence features. Polarized and unpolarized targets.
doi: 10.1103/PhysRevC.69.065503
2004TI05 Phys.Rev. C 70, 042202 (2004) A.I.Titov, A.Hosaka, S.Date, Y.Ohashi Θ+ production at high energy
doi: 10.1103/PhysRevC.70.042202
2003DO13 Nucl.Phys. A721, 517c (2003) P.Doe, H.Ejiri, S.R.Elliott, J.Engel, M.Finger, K.Fushimi, V.Gehman, A.Gorine, M.Greenfield, R.Hazama, K.Ichihara, T.Itahashi, P.Kavitov, V.Kekelidze, K.Kuroda, V.Kutsalo, K.Matsuoka, I.Manouilov, M.Nomachi, A.Para, A.Rjazantsev, R.G.H.Robertson, Y.Shichijo, L.C.Stonehill, T.Shima, G.Shirkov, A.Sissakian, Y.Sugaya, A.Titov, V.Vatulin, V.Voronov, O.E.Vilches, J.F.Wilkerson, D.I.Will, S.Yoshida Neutrino Studies in 100Mo and MOON - Mo Observatory of Neutrinos -
doi: 10.1016/S0375-9474(03)01113-8
2003KA58 Nucl.Phys. A721, 583c (2003) B.Kampfer, A.I.Titov, B.L.Reznik Baryon Resonance Dynamics in πN → NV Reactions Near Threshold NUCLEAR REACTIONS 1H(π-, e+e-), 1n(π+, e+e-), E(cm)=1.5-2 GeV; calculated σ, invariant mass spectra, resonance effects.
doi: 10.1016/S0375-9474(03)01128-X
2003TI08 Phys.Rev. C 67, 065205 (2003) Spin effects and baryon resonance dynamics in φ-meson photoproduction at few GeV NUCLEAR REACTIONS 1H(γ, X), (polarized γ, X), E ≈ 2-4 GeV; calculated ω- and φ-meson production σ(E, θ), polarization observables; deduced resonance contributions.
doi: 10.1103/PhysRevC.67.065205
2003TI09 Yad.Fiz. 66, 1188 (2003); Phys.Atomic Nuclei 66, 1152 (2003) A.V.Titov, N.S.Mosyagin, T.A.Isaev, A.N.Petrov Accuracy and Efficiency of Modern Methods for Electronic Structure Calculation on Heavy- and Superheavy-Element Compounds
doi: 10.1134/1.1586430
2003TI12 Nucl.Phys. A721, 747c (2003) Non-diffractive processes and status of OZI-rule in ω and φ - meson photoproduction
doi: 10.1016/S0375-9474(03)01172-2
2002TI07 Phys.Rev. C65, 065202 (2002) A.I.Titov, B.Kampfer, B.L.Reznik Production of ω and φ Mesons in Near-Threshold πN Reactions: Baryon resonances and the Okubo-Zweig-Iizuka Rule NUCLEAR REACTIONS 1H(π-, X), E ≈ threshold; calculated ω, φ meson production σ, nucleon resonance effects.
doi: 10.1103/PhysRevC.65.065202
2002TI08 Phys.Rev. C66, 015204 (2002) Effective Lagrangian Approach to the ω Photoproduction Near Threshold NUCLEAR REACTIONS 1H(γ, X), E ≈ threshold; calculated ω production σ(θ), asymmetries. Effective Lagrangian approach.
doi: 10.1103/PhysRevC.66.015204
2002TI09 Phys.Rev. C66, 022202 (2002) A.I.Titov, M.Fujiwara, T.S.H.Lee Coherent φ and ω meson photoproduction from deuteron and nondiffractive channels NUCLEAR REACTIONS 2H(γ, X), E=1.92, 2.2 GeV; calculated φ and ω meson production σ(E, θ), nondiffractive channel contributions.
doi: 10.1103/PhysRevC.66.022202
2001OH01 Phys.Rev. C63, 025201 (2001) Nucleon Resonances in ω Photoproduction NUCLEAR REACTIONS 1H(γ, X), E=1.2-4.7 GeV; calculated ω meson production associated σ(E, θ); deduced resonance contributions.
doi: 10.1103/PhysRevC.63.025201
2001OH04 Nucl.Phys. A684, 354c (2001) Y.Oh, A.I.Titov, S.N.Yang, T.Morii Probing Nucleon Strangeness in φ Electroproduction NUCLEAR REACTIONS 1H(polarized e, e'X), E=high; calculated φ meson production σ(E), asymmetries; deduced sensitivity to nucleon strangeness. Comparison with data.
doi: 10.1016/S0375-9474(01)00372-4
2001RO21 Phys.Lett. 513B, 71 (2001) On a Possible Manifestation of f1 Trajectory in J/ψ Photoproduction NUCLEAR REACTIONS 1H(γ, X), E=20, 94 GeV; calculated J/ψ production σ, role of f1 trajectory.
doi: 10.1016/S0370-2693(01)00379-3
2001TI07 Eur.Phys.J. A 12, 217 (2001) Isoscalar-Isovector Interferences in πN → Ne+e- Reactions as a Probe of Baryon Resonance Dynamics NUCLEAR REACTIONS 1H(π-, e+e-), 1n(π+, e+e-), E(cm) ≈ 1.5-1.9 GeV; calculated σ, σ(θ); deduced resonance contributions, isoscalar-isovector interferences. Comparisons with data.
doi: 10.1007/s100500170030
2000RO14 Prog.Theor.Phys.(Kyoto) 103, 747 (2000) D.Roy, T.Morii, H.Toki, A.I.Titov Is There Window for a ' Supersoft ' Pomeron in J/ψ Photoproduction at Low Energy ? NUCLEAR REACTIONS 1H(γ, X), E=4-100 GeV; analyzed J/ψ production σ(θ); deduced role of supersoft Pomeron at low energy.
doi: 10.1143/PTP.103.747
2000TI03 Eur.Phys.J. A 7, 543 (2000) A.I.Titov, B.Kampfer, B.L.Reznik Production of φ Mesons in Near-Threshold πN and NN Reactions NUCLEAR REACTIONS 1H(π-, X), (p, pX), (n, nX), E(cm)=1-100 MeV; calculated φ production σ, σ(θ). Comparisons with data.
doi: 10.1007/s100500050427
1999OH08 Phys.Lett. 462B, 23 (1999) Y.Oh, A.I.Titov, S.N.Yang, T.Morii Probing Nucleon Strangeness Structure with φ Electroproduction NUCLEAR REACTIONS 1H(γ, X), E not given; calculated phi-meson production σ and double polarization asymetries. Virtual photons.
doi: 10.1016/S0370-2693(99)00912-0
1999TI02 Phys.Rev. C59, 999 (1999) A.I.Titov, B.Kampfer, V.V.Shklyar Polarization Observables in the Reaction NN → NNφ NUCLEAR REACTIONS 1H(polarized p, pX), E not given; calculated φ meson production σ, beam-target asymmetry. Extended OBE model.
doi: 10.1103/PhysRevC.59.999
1999TI06 Phys.Rev. C59, R2993 (1999) Isotopic Effect in φ Photoproduction at a Few GeV NUCLEAR REACTIONS 1n, 1H(γ, X), E(cm) ≈ 2-5 GeV; calculated φ photoproduction σ, decay asymmetry; deduced isotopic effect.
doi: 10.1103/PhysRevC.59.R2993
1999TI08 Phys.Rev. C60, 035205 (1999) A.I.Titov, T.-S.H.Lee, H.Toki, O.Streltsova Structure of the φ Photoproduction Amplitude at a Few GeV NUCLEAR REACTIONS 1n, 1H(γ, X), E(cm)=2-5 GeV; calculated φ meson production σ(θ), spin-density matrix elements, polarization observables. Pomeron-exchange and meson-exchange mechanisms.
doi: 10.1103/PhysRevC.60.035205
1998SH03 Nucl.Phys. A628, 255 (1998) V.V.Shklyar, B.Kampfer, B.L.Reznik, A.I.Titov Bremsstrahlung in Intermediate-Energy Nucleon Reactions within an Effective One-Boson Exchange Model NUCLEAR REACTIONS 1n, 1H(p, p'γ), E=high; calculated bremsstrahlung σ(E, θ). Effective one-boson exchange model.
doi: 10.1016/S0375-9474(97)00618-0
1998TI04 Phys.Lett. 422B, 33 (1998) Asymmetry in ω Meson Photoproduction and the Phase of ωπγ Coupling
doi: 10.1016/S0370-2693(98)00049-5
1998TI10 Phys.Rev. C58, 2429 (1998) A.I.Titov, Y.Oh, S.N.Yang, T.Morii Photoproduction of φ Mesons from the Proton: Polarization observables and strangeness in the nucleon NUCLEAR REACTIONS 1H(polarized γ, X), E ≈ 2 GeV; calculated spin observables for φ-meson production; deduced proton strangeness content related features.
doi: 10.1103/PhysRevC.58.2429
1997TI01 Nucl.Phys. A618, 259 (1997) Electroproduction of a φ Meson from the Proton and the Strangeness in the Nucleon NUCLEAR REACTIONS 1H(e, eX), E=11.5 GeV; calculated σ(Q2, W, t) forφ-meson production. 1H deduced strangeness content determination related features. Uud-s(s-bar) cluster model.
doi: 10.1016/S0375-9474(97)00022-5
1997TI04 Phys.Rev.Lett. 79, 1634 (1997) Polarization Observables in φ-Meson Photoproduction and the Strangeness Content of the Proton NUCLEAR REACTIONS 1H(γ, X), E=2 GeV; analyzed σ(θ) for φ-mesons; deduced longitudinal asymmetry, direct knockout process contribution to polarization observables. Pomeron-photon analogy, relativistic harmonic oscillator quark model.
doi: 10.1103/PhysRevLett.79.1634
1996GU05 Phys.Lett. 372B, 187 (1996) T.I.Gulamov, A.I.Titov, B.Kampfer Asymmetry of the Dielectron Emission Rate in an Isospin-Asymmetric Pion Medium
doi: 10.1016/0370-2693(96)00044-5
1996TI03 Phys.Lett. 372B, 15 (1996) A.I.Titov, B.Kampfer, B.L.Reznik, V.Shklyar The Reaction NN → NNγ in the 1 GeV Region Within an Effective One-Boson Exchange Model NUCLEAR REACTIONS 1H(p, γX), E=0.7-1.7 GeV; calculated σ(θ, θp) vs energy transfer; deduced reaction mechanisms energy dependence. Effective one-boson exchange model, other aspects, reactions discussed.
doi: 10.1016/0370-2693(96)00037-8
1995BR30 Phys.Lett. 362B, 17 (1995) E.L.Bratkovskaya, W.Cassing, U.Mosel, O.V.Teryaev, A.I.Titov, V.D.Toneev Decay Anisotropy of e+e- Sources from pN and pd Collisions NUCLEAR REACTIONS 2,1H, 1n(p, X), E=1.26, 2.1 GeV; calculated e+e--pair decay associated anisotropy.
doi: 10.1016/0370-2693(95)01207-7
1995GU11 Yad.Fiz. 58, No 2, 337 (1995); Phys.Atomic Nuclei 58, 290 (1995) Properties of Mesons at Finite Temperatures and Densities in the Nambu-Jona-Lasinio Model
1995TI01 Phys.Rev. C51, 227 (1995) A.I.Titov, B.Kampfer, E.L.Bratkovskaya Dielectron Production in Proton-Proton and Proton-Deuteron Collisions at 1-2 GeV NUCLEAR REACTIONS 1H(p, X), E=1.084, 2.948 GeV; analyzed Δ-production σ data. 2,1H(p, X), E=1-5 GeV; analyzed di-electron production σ(E) ratio data; deduced dielectron production mechanism.
doi: 10.1103/PhysRevC.51.227
1994BR13 Yad.Fiz. 57, No 5, 867 (1994); Phys.Atomic Nuclei 57, 924 (1994) E.L.Bratkovskaya, B.Kampfer, A.V.Molochkov, A.V.Titov, B.L.Reznik Hadronic Sources of Lepton-Pair Production in Proton-Deuteron Interactions at Initial Energies from 1 to 5 GeV NUCLEAR REACTIONS 2H(p, X), E=1-5 GeV; calculated various lepton pair production contributions; deduced dominant hadronic sources.
1993KA05 Phys.Lett. 301B, 123 (1993) B.Kampfer, A.I.Titov, E.L.Bratkovskaya Estimates of Dielectron Production in pp and pd Reactions at 1-2 GeV NUCLEAR REACTIONS 2,1H(p, X), E=1-2 GeV; calculated dielectron production σ. Vector dominance model, dynamical suppression mechanism.
doi: 10.1016/0370-2693(93)90732-W
1992GU09 Phys.Lett. 287B, 302 (1992) K.K.Gudima, A.I.Titov, V.D.Toneev Hadronic Sources of Dileptons from Heavy Ion Collisions at Intermediate and Relativistic Energies NUCLEAR REACTIONS 9Be(p, X), E=1-12 GeV; calculated e+e--pair production invariant mass distributions. Extended kinetic model.
doi: 10.1016/0370-2693(92)90987-F
1991BR12 Yad.Fiz. 53, 934 (1991); Sov.J.Nucl.Phys. 53, 577 (1991) E.L.Bratkovskaya, A.A.Goy, B.L.Reznik, A.I.Titov Electrodisintegration of Polarized Deuterons and the Interaction in the Final State NUCLEAR REACTIONS 2H(e, e'n), E not given; calculated σ, T20 vs neutron momentum, asymmetry vs Ep; deduced final state interactions role. Polarized target.
1990GO17 Yad.Fiz. 51, 1273 (1990); Sov.J.Nucl.Phys. 51, 809 (1990) A.A.Goy, B.L.Reznik, A.I.Titov, A.Yu.Umnikov Final-State Interaction in Deuteron Electrodisintegration NUCLEAR REACTIONS 2H(e, e'p), E=500 MeV; calculated σ(θ(e'), θp) vs nucleon momentum; deduced final state interaction role.
1990LU11 Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 2082 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, No.11, 1 (1990) Dibaryon States NUCLEAR REACTIONS 1H(n, pπ-), E not given; calculated σ fluctuations; deduced dibaryon Γ. Other data, calculations reviewed.
1988KA33 Pisma Zh.Eksp.Teor.Fiz. 47, 428 (1988); JETP Lett.(USSR) 47, 508 (1988) L.P.Kapitar, B.L.Reznik, A.I.Titov, A.Yu.Umnikov Meson Exchange Currents in Deep Inelastic Scattering by a Deuteron NUCLEAR STRUCTURE 2H; calculated meson exchange current corrections to structure function.
1987BA62 Yad.Fiz. 45, 910 (1987); Sov.J.Nucl.Phys. 45, 564 (1987) I.I.Bazhansky, L.P.Kapitar, A.I.Titov Ratio of the Yield of π+ and K+ Mesons in pD Collisions NUCLEAR REACTIONS 2H(p, π+), (p, K+), E=10, 100 GeV; calculated σ(E(K+)), pion yield ratio.
1984BU24 Z.Phys. A318, 67 (1984) V.V.Burov, V.K.Lukyanov, A.I.Titov The Six-Quark-Admixture in the Form Factor of the 3He at Large Transfer Momenta NUCLEAR REACTIONS 3He(e, e), E not given; calculated form factor; deduced quark nucleon interference. Gaussian type wave functions, six quark admixtures.
doi: 10.1007/BF02117215
1984BU42 Fiz.Elem.Chastits At.Yadra 15, 1249 (1984); Sov.J.Part.Nucl 15, 558 (1984) V.V.Burov, V.K.Lukyanov, A.I.Titov Multiquark Systems in Nuclear Processes NUCLEAR REACTIONS 2H(e, e), E not given; calculated recoil deuteron tensor polarization. NUCLEAR STRUCTURE 2H, 3He; calculated form factors. Multi-quark model.
1984DO07 Z.Phys. A316, 331 (1984) S.M.Dorkin, V.K.Lukyanov, A.I.Titov Six-Quark Admixtures in Two-Nucleon Systems NUCLEAR STRUCTURE 2H; calculated six quark state amplitudes. Coupled-channels model.
doi: 10.1007/BF01439905
1979KA21 Acta Phys.Pol. B10, 263 (1979) The Coulomb Disintegration of Relativistic Carbon Ions into Three Alpha Particles NUCLEAR REACTIONS 208Pb(12C, 2α), E=relativistic; calculated σ for dissociation of 12C into 3α. Coulomb mechanism.
1976GL03 Yad.Fiz. 23, 3 (1976); Sov.J.Nucl.Phys. 23, 1 (1976) Y.A.Glukhov, V.I.Manko, B.G.Novatsky, A.A.Ogloblin, S.B.Sakuta, D.N.Stepanov, A.I.Titov, V.I.Chuev Investigation of Coulomb-Nuclear Interference in Inelastic Scattering of 9Be Ions by 58Ni NUCLEAR REACTIONS 58Ni(9Be, 9Be'), (9Be, 9Be), E=26.3 MeV; measured σ(θ); deduced potential parameters. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0873. 1975LU04 Phys.Lett. 57B, 10 (1975) On a Fragmentation Mechanism of Relativistic Heavy Ions NUCLEAR REACTIONS Be(16O, X), E=2.1 GeV/nucl; analyzed data.
doi: 10.1016/0370-2693(75)90230-0
1975LU07 Yad.Fiz. 22, 83 (1975); Sov.J.Nucl.Phys. 22, 40 (1975) Two-Step Effects in Transfer Reactions in the Dispersion Theory NUCLEAR REACTIONS 12C(d, 3He), E=28, 50 MeV; calculated σ(E(3He), θ).
1974TI02 Yad.Fiz. 19, 292 (1974); Sov.J.Nucl.Phys. 19, 143 (1974) Quasiclassical Treatment of Lithium Spallation at Near-Barrier Energies NUCLEAR REACTIONS 58Ni, 208Pb(6Li, αd); measured nothing, calculated σ(θ).
1974TI06 Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 1733 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.8, 147 (1974) Study of the Nuclear Interaction Parameters in Reactions Involving the Near-Barrier Excitation of Nickel by Light Nuclei NUCLEAR REACTIONS 58Ni(3He, 3He'), E=11.2 MeV; 58Ni(6Li, 6Li'), E=11.8, 22.8 MeV; 58Ni(16O, 16O'), E=44 MeV; calculated Coulomb excitation probabilities.
1973LU09 Yad.Fiz. 18, 306 (1973); Sov.J.Nucl.Phys. 18, 157 (1974) Excitation of Nuclei by Particles of Near-Barrier Energies NUCLEAR REACTIONS 58Ni(6Li, X), (16O, X), 120Sn(6Li, X); calculated σ. Coupled channel.
1973TI04 Acta Phys.Pol. B4, 187 (1973) On the Problem of Angular Correlations in Direct Nuclear Reactions NUCLEAR REACTIONS 12C(6Li, d); calculated angular correlations.
1972TI01 JINR-P4-6591 (1972) On the Problem of Angular Correlations in Direct Nuclear Reactions
1972ZA05 JINR-P4-6278 (1972) B.N.Zakhariev, V.K.Lukyanov, A.I.Titov On Parametrization of Three-Particle Reaction Amplitudes. I. Quasielastic Deuteron Disintegration
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