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NSR database version of April 11, 2024.

Search: Author = A.I.Titov

Found 61 matches.

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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
Citations: PlumX Metrics


2017KI04      Phys.Rev. C 95, 055206 (2017)

S.-H.Kim, Y.Oh, A.I.Titov

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
Citations: PlumX Metrics


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
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2008TI01      Eur.Phys.J. A 35, 307 (2008)

A.I.Titov, B.Kampfer

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
Citations: PlumX Metrics


2008TI04      Phys.Rev. C 78, 025201 (2008)

A.I.Titov, B.Kampfer

Exclusive charm production in (p-bar)p collisions at √ s ≤ 15 GeV

doi: 10.1103/PhysRevC.78.025201
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2008TI06      Phys.Rev. C 78, 038201 (2008)

A.I.Titov, B.Kampfer

Selected vector-meson decay distributions in reactions of polarized photons with protons

doi: 10.1103/PhysRevC.78.038201
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2007TI10      Phys.Rev. C 76, 035202 (2007)

A.I.Titov, B.Kampfer

Photoproduction of the φ meson off the deuteron near threshold

doi: 10.1103/PhysRevC.76.035202
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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
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2007TI14      Phys.Rev. C 76, 065211 (2007)

A.I.Titov, B.Kampfer

In-medium modification and decay asymmetry of ω mesons in cold nuclear matter

doi: 10.1103/PhysRevC.76.065211
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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
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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
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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
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2005TI06      Phys.Rev. C 71, 062201 (2005)

A.I.Titov, B.Kampfer

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
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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
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2004FU13      Phys.Rev. C 69, 065503 (2004)

M.Fujiwara, A.I.Titov

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
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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
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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
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2003TI08      Phys.Rev. C 67, 065205 (2003)

A.I.Titov, T.-S.H.Lee

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
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2003TI12      Nucl.Phys. A721, 747c (2003)

A.I.Titov

Non-diffractive processes and status of OZI-rule in ω and φ - meson photoproduction

doi: 10.1016/S0375-9474(03)01172-2
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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
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2002TI08      Phys.Rev. C66, 015204 (2002)

A.I.Titov, T.-S.H.Lee

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
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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
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2001OH01      Phys.Rev. C63, 025201 (2001)

Y.Oh, A.I.Titov, T.-S.H.Lee

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
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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
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2001RO21      Phys.Lett. 513B, 71 (2001)

D.Roy, T.Morii, A.I.Titov

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
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2001TI07      Eur.Phys.J. A 12, 217 (2001)

A.I.Titov, B.Kampfer

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
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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
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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
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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
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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
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1999TI06      Phys.Rev. C59, R2993 (1999)

A.I.Titov, T.-S.H.Lee, H.Toki

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
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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
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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
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1998TI04      Phys.Lett. 422B, 33 (1998)

A.I.Titov, Y.Oh

Asymmetry in ω Meson Photoproduction and the Phase of ωπγ Coupling

doi: 10.1016/S0370-2693(98)00049-5
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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
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1997TI01      Nucl.Phys. A618, 259 (1997)

A.I.Titov, S.N.Yang, Y.Oh

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
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1997TI04      Phys.Rev.Lett. 79, 1634 (1997)

A.I.Titov, Y.Oh, S.N.Yang

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
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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
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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
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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
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1995GU11      Yad.Fiz. 58, No 2, 337 (1995); Phys.Atomic Nuclei 58, 290 (1995)

T.I.Gulamov, A.I.Titov

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
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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
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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
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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.


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
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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
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1979KA21      Acta Phys.Pol. B10, 263 (1979)

L.P.Kapitar, A.I.Titov

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)

V.K.Lukyanov, A.I.Titov

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
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1975LU07      Yad.Fiz. 22, 83 (1975); Sov.J.Nucl.Phys. 22, 40 (1975)

V.K.Lukyanov, A.I.Titov

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)

A.I.Titov

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)

A.I.Titov

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)

V.K.Lukyanov, A.I.Titov

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)

A.I.Titov

On the Problem of Angular Correlations in Direct Nuclear Reactions

NUCLEAR REACTIONS 12C(6Li, d); calculated angular correlations.


1972TI01      JINR-P4-6591 (1972)

A.I.Titov

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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