NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = V.F.Dmitriev Found 40 matches. 2012BE32 J.Phys.:Conf.Ser. 337, 012043 (2012) J.C.Berengut, V.V.Flambaum, V.F.Dmitriev Quark-mass variation effect on big bang nucleosynthesis NUCLEAR REACTIONS 3H(d, n), E not given;3He(d, p), E not given; analyzed resonance influence on σ within big bang nucleosynthesis. 3He(α, γ), E not given; calculated 7Be and via β-capture 7Li abundances vs light quark mass.
doi: 10.1088/1742-6596/337/1/012043
2010BA14 Bull.Rus.Acad.Sci.Phys. 74, 743 (2010); Izv.Akad.Nauk RAS, Ser.Fiz 74, 780 (2010) L.M.Barkov, V.V.Gauzshtein, V.F.Dmitriev, B.A.Lazarenko, M.I.Levchuk, A.Yu.Loginov, S.I.Mishnev, D.M.Nikolenko, A.V.Osipov, I.A.Rachek, A.A.Sidorov, V.N.Stibunov, D.K.Toporkov, Yu.V.Shestakov, S.A.Zevakov Tensor asymmetry of π--meson photoproduction on polarized deuterons NUCLEAR REACTIONS 2H(γ, 2p)π-, E=300-750 MeV; measured reaction products, proton spectrum; deduced σ asymmetry. Comparison with Monte-Carlo calculations.
doi: 10.3103/S1062873810060031
2007AU07 Phys.Atomic Nuclei 70, 1654 (2007) N.Auerbach, V.F.Dmitriev, V.V.Flambaum, A.Lisetskiy, R.A.Senkov, V.G.Zelevinsky Is it possible to enhance the nuclear Schiff moment by nuclear collective modes? NUCLEAR MOMENTS 217,219,221Ra, 217,219,221Rn; calculated the nuclear Schiff moment using the QRPA formalism.
doi: 10.1134/S106377880709027X
2007RA09 Phys.Rev.Lett. 98, 182303 (2007) I.A.Rachek, L.M.Barkov, S.L.Belostotsky, V.F.Dmitriev, M.V.Dyug, R.Gilman, R.J.Holt, B.A.Lazarenko, S.I.Mishnev, V.V.Nelyubin, D.M.Nikolenko, A.V.Osipov, D.H.Potterveld, R.Sh.Sadykov, Yu.V.Shestakov, V.N.Stibunov, D.K.Toporkov, H.de Vries, S.A.Zevakov Measurement of Tensor Analyzing Powers in Deuteron Photodisintegration NUCLEAR REACTIONS 2H(γ, np), E=25-600 MeV; measured tensor analyzing powers.
doi: 10.1103/PhysRevLett.98.182303
2006AU02 Phys.Rev. C 74, 025502 (2006) N.Auerbach, V.F.Dmitriev, V.V.Flambaum, A.Lisetskiy, R.A.Sen'kov, V.G.Zelevinsky Nuclear Schiff moment in nuclei with soft octupole and quadrupole vibrations NUCLEAR STRUCTURE 217,219,221Ra; calculated Schiff moments, role of soft collective quadrupole and octupole vibrations. Quasiparticle RPA. NUCLEAR MOMENTS 217,219,221Ra; calculated Schiff moments, role of soft collective quadrupole and octupole vibrations. Quasiparticle RPA.
doi: 10.1103/PhysRevC.74.025502
2006DM01 Phys.Atomic Nuclei 69, 1461 (2006); Yad.Fiz. 69, 1496 (2006) Effect of Polarization on the Cross Section for the Reaction 11B(p, α)8Be* and Angular Distributions of its Products NUCLEAR REACTIONS 11B(polarized p, α), E not given; calculated σ(θ), polarization effects.
doi: 10.1134/S1063778806090043
2006DM02 Nucl.Phys. B(Proc.Supp.) S162, 53 (2006) Final State Interaction Effects in N(N-bar) Production near Threshold
doi: 10.1016/j.nuclphysbps.2006.09.163
2005DM01 Phys.Rev. C 71, 035501 (2005) V.F.Dmitriev, R.A.Senkov, N.Auerbach Effects of core polarization on the nuclear Schiff moment NUCLEAR MOMENTS 129Xe, 133Cs, 199Hg, 211Rn, 213,225Ra, 223Fr; calculated Schiff moments, core polarization contributions. NUCLEAR STRUCTURE 129Xe, 133Cs, 199Hg, 211Rn, 213,225Ra, 223Fr; calculated Schiff moments, core polarization contributions.
doi: 10.1103/PhysRevC.71.035501
2005DM02 Phys.Rev. C 71, 068501 (2005) Relativistic corrections to the nuclear Schiff moment NUCLEAR MOMENTS 199Hg, 205Tl; calculated Schiff moments, relativistic corrections.
doi: 10.1103/PhysRevC.71.068501
2004AR02 Yad.Fiz. 67, 191 (2004); Phys.Atomic Nuclei 67, 195 (2004) K.E.Arinstein, V.F.Dmitriev, I.B.Khriplovich Anapole Moment of an Exotic Nucleus NUCLEAR MOMENTS 11Be, 133Cs; calculated anapole moments. NUCLEAR STRUCTURE 11Be, 133Cs; calculated anapole moments.
doi: 10.1134/1.1644023
2004DM01 Phys.Rep. 391, 243 (2004) P and T odd nuclear moments
doi: 10.1016/j.physrep.2003.10.006
2004DM02 Yad.Fiz. 67, 1827 (2004); Phys.Atomic Nuclei 67, 1799 (2004) Schiff Moment of the Mercury Nucleus and the Proton Dipole Moment NUCLEAR MOMENTS 199Hg; calculated Schiff moment, core polarization effects, nucleon contributions. 1n, 1H deduced electric dipole moment upper limits.
doi: 10.1134/1.1811181
2003DM01 Yad.Fiz. 66, 1988 (2003); Phys.Atomic Nuclei 66, 1940 (2003) P- and T-Violating Schiff Moment of the Mercury Nucleus NUCLEAR STRUCTURE 199Hg; calculated Schiff moment, core polarization effects. RPA approach, P- and T-violating interaction. NUCLEAR MOMENTS 199Hg; calculated Schiff moment, core polarization effects. RPA approach, P- and T-violating interaction.
doi: 10.1134/1.1619505
2003DM02 Phys.Rev.Lett. 91, 212303 (2003) Schiff Moment of the Mercury Nucleus and the Proton Dipole Moment NUCLEAR MOMENTS 199Hg; calculated nucleon dipole moment contributions to Schiff moment. 1H deduced electric dipole moment upper limit.
doi: 10.1103/PhysRevLett.91.212303
2003NI02 Phys.Rev.Lett. 90, 072501 (2003) D.M.Nikolenko, H.Arenhovel, L.M.Barkov, S.L.Belostotsky, V.F.Dmitriev, M.V.Dyug, R.Gilman, R.J.Holt, L.G.Isaeva, C.W.de Jager, E.R.Kinney, R.S.Kowalczyk, B.A.Lazarenko, A.Yu.Loginov, S.I.Mishnev, V.V.Nelyubin, A.V.Osipov, D.H.Potterveld, I.A.Rachek, R.Sh.Sadykov, Yu.V.Shestakov, A.A.Sidorov, V.N.Stibunov, D.K.Toporkov, V.V.Vikhrov, H.de Vries, S.A.Zevakov Measurement of the Tensor Analyzing Powers T20 and T21 in Elastic Electron-Deuteron Scattering NUCLEAR REACTIONS 2H(e, e), E=2 GeV; measured tensor analyzing powers vs momentum transfer. 2H deduced form factors. Polarized target. Comparisons with model predictions and previous data.
doi: 10.1103/PhysRevLett.90.072501
2003NI08 Nucl.Phys. A721, 409c (2003) D.M.Nikolenko, H.Arenhovel, L.M.Barkov, S.L.Belostotsky, V.F.Dmitriev, M.V.Dyug, R.Gilman, R.J.Holt, L.G.Isaeva, C.W.de Jager, E.R.Kinney, R.S.Kowalczyk, B.A.Lazarenko, A.Yu.Loginov, S.I.Mishnev, V.V.Nelyubin, A.V.Osipov, D.H.Potterveld, I.A.Rachek, R.Sh.Sadykov, Yu.V.Shestakov, A.A.Sidorov, V.N.Stibunov, D.K.Toporkov, V.V.Vikhrov, H.de Vries, S.A.Zevakov Measurement of tensor analyzing power in elastic electron-deuteron scattering at momentum transfer range 2.8 - 4.6fm-1 NUCLEAR REACTIONS 2H(e, e), E=2 GeV; measured particle spectra, tensor analyzing powers. 2H deduced charge form factors. Polarized target.
doi: 10.1016/S0375-9474(03)01084-4
2002DM01 Phys.Rev. C65, 015803 (2002) V.F.Dmitriev, V.Zelevinsky, S.M.Austin Do Hadronic Charge Exchange Reactions Measure Electroweak L = 1 Strength ? NUCLEAR REACTIONS 12C(p, n), E=135 MeV; calculated σ(E, θ); deduced relationship with β-decay strengths. Eikonal model.
doi: 10.1103/PhysRevC.65.015803
2002SE04 Nucl.Phys. A706, 351 (2002) Nuclear Magnetization Distribution and Hyperfine Splitting in Bi82+ Ion NUCLEAR MOMENTS 207Pb, 209Bi; calculated hfs, core polarization effects for hydrogen-like ions.
doi: 10.1016/S0375-9474(02)00759-5
2001DM02 Yad.Fiz. 64, No 3, 503 (2001); Phys.Atomic Nuclei 64, 448 (2001) Nuclear Anapole Moment and Axial Neutral Current in Nuclei NUCLEAR STRUCTURE 133Cs, 135,137Ba, 205Tl, 207Pb, 209Bi; calculated anapole moments.
doi: 10.1134/1.1358468
2001NI07 Nucl.Phys. A684, 525c (2001) D.M.Nikolenko, H.Arenhovel, L.M.Barkov, S.L.Belostotsky, V.F.Dmitriev, M.V.Dyug, R.Gilman, R.J.Holt, L.G.Isaeva, C.W.de Jager, E.R.Kinney, R.S.Kowalczyk, B.A.Lazarenko, A.Yu.Loginov, S.I.Mishnev, V.V.Nelyubin, A.V.Osipov, D.H.Potterveld, I.A.Rachek, Yu.V.Shestakov, A.A.Sidorov, V.N.Stibunov, D.K.Toporkov, D.K.Vesnovsky, V.V.Vikhrov, H.de Vries, S.A.Zevakov Measurement of Polarization Observables in Elastic and Inelastic Electron-Deuteron Scattering at the VEPP-3 Storage Ring NUCLEAR REACTIONS 2H(e, e'X), E not given; measured recoil deuteron tensor polarization vs momentum transfer. Comparisons with previous data, model predictions.
doi: 10.1016/S0375-9474(01)00373-6
2000DM03 Nucl.Phys. A663-664, 1099c (2000) V.F.Dmitriev, G.N.Kulipanov, D.M.Nikolenko, I.A.Rachek, A.N.Skrinsky, D.K.Toporkov, N.A.Vinokurov, V.G.Zelevinsky New Possibilities for Nuclear Physics Experiments with Novosibirsk Race-Track Microtron-Recuperator
doi: 10.1016/S0375-9474(99)00786-1
2000DM04 Nucl.Phys. A674, 168 (2000) Many-Body Corrections to the Nuclear Anapole Moment II NUCLEAR STRUCTURE 133Cs, 135,137Ba, 205Tl, 207Pb, 209Bi; calculated anapole moments, many-body contributions. Core polarization, parity-violating effective interaction.
doi: 10.1016/S0375-9474(00)00158-5
1997DM01 Nucl.Phys. A613, 237 (1997) Many-Body Corrections to the Nuclear Anapole Moment NUCLEAR STRUCTURE 133Cs, 205Tl, 207,209Pb, 209Bi; calculated nuclear anapole moment, many body contribution. RPA with residual interaction.
doi: 10.1016/S0375-9474(96)00440-X
1997KA52 Phys.Lett. 408B, 12 (1997) Virtual Pion Scattering NUCLEAR REACTIONS 12C, 40Ca(p, π+n), E=800 MeV; 12C(3He, tπ+), E=2 GeV; calculated σ(E, θ); deduced reaction mechanism, pion rescattering role. Coupled-channel model, rescattering optical potential.
doi: 10.1016/S0370-2693(97)00773-9
1996DM04 Phys.Rev. C54, 3305 (1996) V.F.Dmitriev, V.B.Telitsin, V.V.Flambaum, V.A.Dzuba Core Contribution to the Nuclear Magnetic Quadrupole Moment NUCLEAR STRUCTURE 133Cs, 131Xe; calculated core contribution to magnetic quadrupole moment.
doi: 10.1103/PhysRevC.54.3305
1995DM03 Phys.Rev. C52, 1711 (1995) V.F.Dmitriev, I.B.Khriplovich, V.B.Telitsin Is Large Weak Mixing in Heavy Nuclei Consistent with Atomic Experiments ( Question ) NUCLEAR STRUCTURE 207Pb; analyzed parity nonconserving optical activity data; deduced inconsistency between data and large weak matrix element hypothesis.
doi: 10.1103/PhysRevC.52.1711
1995SA06 Phys.Rev. C51, 1945 (1995) T.Sams, C.Ellegaard, C.Gaarde, J.S.Larsen, J.L.Boyard, T.Hennino, J.C.Jourdain, B.Ramstein, M.Roy-Stephan, P.Radvanyi, A.Brockstedt, M.Osterlund, P.Zupranski, C.D.Goodman, M.Ichimura, V.F.Dmitriev Quasifree (d(pol), 2He) Data NUCLEAR REACTIONS 2,1H, 12C(polarized d, X), E=1.6, 2 GeV; measured σ(θ), tensor analyzing powers vs momentum transfer; deduced spin-isospin response in the quasifree region.
doi: 10.1103/PhysRevC.51.1945
1994DM01 Nucl.Phys. A577, 691 (1994) V.F.Dmitriev, I.B.Khriplovich, V.B.Telitsin Nuclear Anapole Moments in Single-Particle Approximation NUCLEAR STRUCTURE 133Cs, 203,205Tl, 207Pb, 209Bi; calculated nuclear anapole moments. Single particle approximation.
doi: 10.1016/0375-9474(94)90940-7
1994DM02 Phys.Rev. C50, 2358 (1994) V.F.Dmitriev, I.B.Khriplovich, V.B.Telitsin Nuclear Magnetic Quadrupole Moments in the Single-Particle Approximation NUCLEAR STRUCTURE 133Cs, 137Ba; calculated magnetic quadrupole moment; deduced model results stability features. Single particle approximation.
doi: 10.1103/PhysRevC.50.2358
1993DM01 Phys.Rev. C48, 357 (1993) Nuclear Response in Delta-Isobar Region in the (3He, t) Reaction NUCLEAR REACTIONS 12C(3He, t), E ≈ resonance; calculated σ(θt, Et); deduced Δ-hole excitation widths, coherent pion production contribution estimate. Relativistic nuclear response function approach.
doi: 10.1103/PhysRevC.48.357
1992SA07 Phys.Rev. C45, R2555 (1992) Distortion Effects in the Quasifree 12C(d(pol), 2p) Reaction NUCLEAR REACTIONS 12C(polarized d, 2p), E=1.6 GeV; calculated σ(θ), tensor polarization response vs energy transfer; deduced distortion role in quasifree excitation. Eikonal limit.
doi: 10.1103/PhysRevC.45.R2555
1989DM01 Phys.Lett. 226B, 219 (1989) Do the Medium Effects Exist for the (3He, t) Reaction at Intermediate Energies ( Question ) NUCLEAR REACTIONS 12C(3He, t), E=2 GeV; calculated σ(Et, θt); deduced medium effects role.
doi: 10.1016/0370-2693(89)91184-2
1989DM03 Yad.Fiz. 50, 357 (1989) Theoretical Analysis of (e, e'N) and (γ, N) Reaction on 16O NUCLEAR REACTIONS 16O(γ, n), (γ, p), E ≈ 13-30 MeV; calculated σ(E). 16O(e, e'p), (e, e'n), E=130 MeV; calculated σ(θ(e'), p), σ(θ(e'), n). Continuum RPA.
1987AB16 Yad.Fiz. 46, 549 (1987) V.G.Ableev, G.G.Vorobiev, Kh.Dimitrov, V.F.Dmitriev, S.M.Eliseev, S.A.Zaporozhets, V.I.Ionzemtsev, A.P.Kobushkin, A.G.Malinin, B.Naumann, L.Naumann, W.Neubert, A.A.Nomofilov, L.Penchev, N.M.Piskunov, I.M.Sitnik, E.A.Strokovsky, L.N.Strunov, V.I.Sharov Charge Exchange p(3He, t) at Momenta 4.4-18.3 GeV/c with Δ-Isobar Production NUCLEAR REACTIONS 1H(3He, t), E at 4.4, 6.81, 10.79, 18.3 GeV/c; measured σ(Et, θt). Glauber-Sitenko model calculations.
1987DM01 Nucl.Phys. A464, 237 (1987) V.F.Dmitriev, D.M.Nikolenko, S.G.Popov, I.A.Rachek, D.K.Toporkov, E.P.Tsentalovich, B.B.Woitsekhowski, V.G.Zelevinsky Coincidence Experiment on 16O Electroexcitation NUCLEAR REACTIONS 16O(e, e'p), (e, e'α), E=130 MeV; measured σ(E(e'), θp), σ(E(e'), θα) vs excitation; deduced reaction mechanism. 16O deduced resonance excitation σ, decay characteristics.
doi: 10.1016/0375-9474(87)90337-X
1987DM02 Yad.Fiz. 46, 770 (1987); Sov.J.Nucl.Phys. 46, 435 (1987) The (3He, t) Reaction in Nuclei in the Region of the Δ Isobar NUCLEAR REACTIONS C(3He, t), E=2.3 GeV; C(3He, t), E at 4.4, 10.79 GeV/c; calculated σ(θt, Et). Optical approximation.
1985DM01 Phys.Lett. 157B, 143 (1985) V.F.Dmitriev, D.M.Nikolenko, S.G.Popov, I.A.Rachek, Yu.M.Shatunov, D.K.Toporkov, E.P.Tsentalovich, Yu.G.Ukraintsev, B.B.Voitsekhovskii, V.G.Zelevinsky First Measurement of the Asymmetry in Electron Scattering by a Jet Target of Polarized Deuterium Atoms NUCLEAR REACTIONS 2H(e, e), E=290 MeV; measured electron asymmetry. Polarized gas jet internal target.
doi: 10.1016/0370-2693(85)91534-5
1983DM01 Phys.Lett. 125B, 1 (1983) V.F.Dmitriev, V.V.Flambaum, O.P.Sushkov, V.B.Telitsin The Parity Violating Rotation of the Neutron Spin in Helium NUCLEAR REACTIONS 4He(polarized n, n), E=low; calculated spin rotation angle. Parity violating nucleon-nucleon interaction.
doi: 10.1016/0370-2693(83)91221-2
1983DM02 Nucl.Phys. A402, 581 (1983) The Influence of the Spin-Orbit Quasiparticle Interaction on the Magnetic Properties of Nuclei NUCLEAR MOMENTS 209Bi, 205Tl; calculated muonic hfs. Finite Fermi system, core polarization, spin-orbit, velocity dependent forces. NUCLEAR STRUCTURE 209Bi; calculated B(λ) for magnetic multipole transitions; deduced two particle spin-orbit interaction role. Finite Fermi system, core polarization, spin-orbit, velocity dependent forces.
doi: 10.1016/0375-9474(83)90221-X
1983DM05 Yad.Fiz. 37, 1147 (1983); Sov.J.Nucl.Phys. 37, 681 (1983) Effect of Spin-Orbit Forces on the Magnetic Properties of Nuclei NUCLEAR STRUCTURE 209Bi; calculated B(M2); deduced spin-orbit effects. Finite Fermi system theory.
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