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NSR database version of May 3, 2024.

Search: Author = V.M.Shilov

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2012SH17      Phys.Atomic Nuclei 75, 449 (2012); Yad.Fiz. 75, 485 (2012)

V.M.Shilov

Subbarrier fusion of spherical nuclei of intermediate atomic number

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁶O, X), ⁶⁴Ni(⁶⁴Ni, X), ⁸⁹Y(⁶⁰Ni, X), ⁹²Zr(⁹⁰Zr, X), ⁶⁴Ni(²⁸Si, X), E<110 MeV; calculated σ. Two-humped model, comparison with available data.

doi: 10.1134/S1063778812030179
Citations: PlumX Metrics

1995BA15      Phys.Scr. 51, 54 (1995)

S.I.Bastrukov, I.V.Molodtsova, V.M.Shilov

Torsional Multipole Magnetic Response of a Heavy Spherical Nucleus

NUCLEAR STRUCTURE ²⁸Si, ⁹⁰Zr, ¹⁴⁰Ce, ²⁰⁸Pb; calculated B(λ). ¹⁴⁰Ce; calculated collective transition current density. Distorted Fermi sphere model.

NUCLEAR REACTIONS ¹⁴⁰Ce(e, e'), E=20-120 MeV; calculated σ(θ) vs E, θ=165°. Distorted Fermi sphere model.

doi: 10.1088/0031-8949/51/1/008
Citations: PlumX Metrics

1995BA56      Phys.Rev. C52, 1114 (1995)

S.I.Bastrukov, I.V.Molodtsova, V.M.Shilov

Integral Characteristic Parameters of the Giant M1 Resonance

NUCLEAR STRUCTURE ⁹⁰Zr, ¹²⁰Sn, ¹⁴⁰Ce, ^206,208Pb; calculated giant M1 resonance energy, B(λ), Γ. Semi-classical model.

doi: 10.1103/PhysRevC.52.1114
Citations: PlumX Metrics

1995BA91      Yad.Fiz. 58, No 6, 989 (1995); Phys.Atomic Nuclei 58, 916 (1995)

S.I.Bastrukov, I.V.Molodtsova, V.M.Shilov

Macroscopic Mechanism of the Excitation of Mλ, T = 0 Resonances in Inelastic Electron Scattering

NUCLEAR STRUCTURE ⁹⁰Zr, ²⁸Si, ¹⁴⁰Ce, ²⁰⁸Pb; calculated collective magnetic torsional excitations, B(λ), energy for M2, M3 resonances. Nuclear fluid dynamics model.

NUCLEAR REACTIONS ⁹⁰Zr(e, e'), E not given; calculated torsional, magnetic quadrupole modes associated form factors. Nuclear fluid dynamics model.

1995SH23      Bull.Rus.Acad.Sci.Phys. 59, 145 (1995)

V.M.Shilov

Cross Sections for Evaporation of Particles from a Compound Nucleus on Near-Barrier Collisions of Heavy Nuclei

NUCLEAR REACTIONS, ICPND ¹⁰⁰Mo(¹⁰⁰Mo, X), E(cm) ≈ 170-250 MeV; ¹¹⁰Pd(¹⁰⁰Mo, X), E(cm) ≈ 190-220 MeV; ¹¹⁰Pd(¹¹⁰Pd, X), E(cm) ≈ 230-290 MeV; calculated residuals production σ vs E. ' Critical distance ' model.

1994SH33      Yad.Fiz. 57, No 7, 1275 (1994); Phys.Atomic Nuclei 57, 1207 (1994)

V.M.Shilov

Complete Fusion of Heavy Semimagic Nuclei at Energies Near the Coulomb Barrier

NUCLEAR REACTIONS ¹⁸⁰Hf(⁴⁰Ar, xn), ¹²⁴Sn(⁹⁶Zr, xn), ¹³⁶Xe(⁸⁶Kr, xn), E not given; analyzed neutron evaporation σ data following complete fusion. Critical distance model.

1993BA77      Bull.Rus.Acad.Sci.Phys. 57, 1796 (1993)

S.I.Bastrukov, I.V.Molodtsova, V.M.Shilov

Widths of Magnetic Twist Resonances

1993SH16      Yad.Fiz. 56, No 6, 55 (1993); Phys.Atomic Nuclei 56, 741 (1993)

V.M.Shilov, A.V.Tarakanov

Distribution of Effective Barriers in Heavy-Ion Fusion at Near-Barrier Energies

NUCLEAR REACTIONS, ICPND ¹⁰⁰Mo(³²S, X), (³⁶S, X), E(cm) ≈ 75-90 MeV; analyzed fusion σ(E); deduced transfer channels role.

1991TA17      Yad.Fiz. 53, 1285 (1991); Sov.J.Nucl.Phys. 53, 791 (1991)

A.V.Tarakanov, V.M.Shilov, R.Schmidt

Semiclassical Description of Heavy-Ion Fusion at Near-Barrier Energies

NUCLEAR REACTIONS ¹²⁴Sn(⁹⁶Zr, X), ¹²³Sb(⁸⁶Kr, X), E not given; ⁹⁰Zr(⁹⁰Zr, X), E=180 MeV; ²⁰⁸Pb(⁵⁰Ti, X), E ≈ 190-215 MeV; calculated potential parameters. ²⁰⁸Pb(⁵⁰Ti, X), E ≈ 190-215 MeV; calculated fusion σ(E). Critical distance model, near-barrier energies.

1989PE16      Fiz.Elem.Chastits At.Yadra 20, 1396 (1989); Sov.J.Part.Nucl 20, 594 (1989)

V.P.Permyakov, V.M.Shilov

Below-Barrier Fusion of Complex Nuclei

NUCLEAR REACTIONS, ICPND ⁹⁰Zr(⁵⁰Ti, X), E(cm) ≈ 100-120 MeV; ²⁷Al(¹⁶O, X), E not given; calculated fusion σ(E). Multi-channel model, converging wave boundary condition. Other data, models considered.

1988TA25      Yad.Fiz. 48, 109 (1988); Sov.J.Nucl.Phys. 48, 68 (1988)

A.V.Tarakanov, V.M.Shilov

Tunneling in Decay and Fusion of Compound Nuclei

RADIOACTIVITY ²²²Ra(¹⁴C); calculated Coulomb barrier transmission asymmetry. Fusion, multi-channel boundary condition.

1984PE18      Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 866 (1984)

V.P.Permyakov, V.M.Shilov

Nuclear Shape Deformations and Effective Fusion Barriers

NUCLEAR REACTIONS ²⁰⁸Pb(²⁶Mg, X), (²⁷Al, X), (⁵⁰Ti, X), (⁵²Cr, X), (⁵⁸Fe, X), (⁶⁴Ni, X), (⁴⁸Ca, X), E not given; calculated fusion barriers.

1984PO16      Phys.Scr. 30, 238 (1984)

V.Yu.Ponomarev, A.I.Vdovin, V.M.Shilov, Nguyen Dinh Dang

Transversal E1-Resonance in Spherical Nuclei

NUCLEAR STRUCTURE ⁵⁸Ni; calculated spin-flip dipole state charge, current densities.

NUCLEAR REACTIONS ⁵⁸Ni(e, e'), E=40, 60, 80 MeV; calculated σ(θ) for isovector dipole, spin dipole state excitation. RPA.

doi: 10.1088/0031-8949/30/4/004
Citations: PlumX Metrics

1981VD01      Yad.Fiz. 34, 1009 (1981)

A.I.Vdovin, V.Yu.Ponomarev, V.M.Shilov

Electroexcitation of M1 and M2 Resonances in Spherical Nuclei

NUCLEAR REACTIONS ⁵⁸Ni, ⁹⁰Zr, ²⁰⁸Pb, ¹⁴⁰Ce(e, e'), E=40 MeV; calculated σ(θ), form factors. DWBA, quasiparticle-phonon model current transition densities.

NUCLEAR STRUCTURE ⁵⁸Ni, ⁹⁰Zr, ²⁰⁸Pb, ¹⁴⁰Ce; calculated 1⁺, 2^- level current transition densities. Quasiparticle-phonon model.

1980BA52      Yad.Fiz. 31, 585 (1980); Sov.J.Nucl.Phys. 31, 303 (1980)

M.I.Baznat, N.I.Pyatov, V.M.Shilov

Transition Densities and Electro Excitation of Nuclear Dipole States

NUCLEAR REACTIONS ⁵⁸Ni(e, e'), E=102 MeV; ¹⁴⁰Ce(e, e'), E=92.1 MeV; ⁹⁰Zr(e, e'), E=150, 183, 250 MeV; calculated E1 transition densities, form factors. Self-consistent microscopic method.

NUCLEAR STRUCTURE ⁹⁰Zr, ²⁰⁸Pb, ¹⁴⁰Ce; calculated dipole excitation transition densities, rms charge radii; deduced shape dependence on excitation. Self-consistent microscopic method.

1980PO08      Phys.Lett. B97, 4 (1980)

V.Yu.Ponomarev, V.M.Shilov, A.I.Vdovin, V.V.Voronov

On the M1 and M2 Strengths in ¹⁴⁰Ce

NUCLEAR REACTIONS ¹⁴⁰Ce(e, e'), E=20-140; calculated σ(θ). ¹⁴⁰Ce deduced M1, M2 transition strengths.

doi: 10.1016/0370-2693(80)90533-X
Citations: PlumX Metrics

1978AF01      Izv.Akad.Nauk SSSR, Ser.Fiz. 42, 181 (1978); Bull.Acad.Sci.USSR, Phys.Ser. 42, No.1, 157 (1978)

G.N.Afanasev, V.M.Shilov

Distribution of Electrical Moments in the Nuclei of Even Tin Isotopes

NUCLEAR REACTIONS ^116,120,124Sn(e, e'), E=209 MeV; calculated form factors, transition densities. Microscopic model.

1978AF02      Izv.Akad.Nauk SSSR, Ser.Fiz. 42, 1961 (1978); Bull.Acad.Sci.USSR, Phys.Ser. 42, No.9, 140 (1978)

G.N.Afanasev, R.V.Jolos, V.M.Permyakov, V.M.Shilov

Coulomb Energy Dissipation in Reactions with Heavy Ions

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, X), E=60-140 MeV; calculated σ(reaction), σ(fusion); deduced influence of Coulomb energy dissipation.

1978AK01      Yad.Fiz. 28, 51 (1978); Sov.J.Nucl.Phys. 28, 25 (1978)

S.V.Akulinichev, V.M.Shilov

Possibility of Observing Giant Resonances of High Multipolarity in Inelastic Scattering of Fast Protons

NUCLEAR REACTIONS ¹⁵⁴Sm(p, p'), E=1 GeV; calculated σ in giant resonance region.

1978AK02      Yad.Fiz. 28, 883 (1978); Sov.J.Nucl.Phys. 28, 453 (1978)

S.V.Akulinichev, G.N.Afanasev, A.I.Vdovin, C.Stoyanov, V.M.Shilov

Study of Giant Resonances in Nuclei with the Aid of Proton and Electron Scattering

NUCLEAR STRUCTURE ⁹⁰Zr; calculated resonances. One-phonon approximation, level fragmentation.

1978AK03      Yad.Fiz. 27, 670 (1978); Sov.J.Nucl.Phys. 27, 358 (1978)

S.V.Akulinichev, V.M.Shilov

Electron Excitation of Giant Resonances in Deformed Nuclei

NUCLEAR REACTIONS ¹⁵²Sm(e, e'), E=60-105 MeV; calculated σ for excitation of giant multipole resonances. DWBA with semi-microscopic wave function.

1977AF03      Yad.Fiz. 25, 301 (1977); Sov.J.Nucl.Phys. 25, 164 (1977)

G.N.Afanasev, V.M.Shilov, S.M.Eliseev

Effect of Nucleon Electromagnetic Structure on the Differential Cross Sections for the Scattering of Electrons by Nuclei

NUCLEAR REACTIONS ^54,58Fe, ^58,60,62Ni, ^62,64,66,68Zn(e, e); calculated σ(θ); deduced effect of nucleon electromagnetic structure.

1977AF04      Izv.Akad.Nauk SSSR, Ser.Fiz. 41, 1650 (1977); Bull.Acad.Sci.USSR, Phys.Ser. 41, No.8, 98 (1977)

G.N.Afanasev, M.B.Dobromyslov, Kim Yng Phung, V.M.Shilov

Description of the Reaction and Fusion Cross Sections in the Model of The Boundary Conditions

NUCLEAR REACTIONS ²⁷Al(¹⁶O, X), E=50-200 MeV; ⁴⁰Ca(¹⁶O, X), E(cm)=20-140 MeV; ¹⁰⁹Ag(⁴⁰Ar, X), E=150-350 MeV; calculated σ. Blatt, Weisskopf-Thomas model.

1977AK02      J.Phys.(London) G3, L-213 (1977)

S.V.Akulinichev, V.M.Shilov

Excitation of Giant Resonances in Deformed Nuclei by Fast Protons

NUCLEAR REACTIONS ¹⁵⁴Sm(p, p'), E=1 GeV; calculated σ(θ), E2, E3 resonance region. Glauber theory.

doi: 10.1088/0305-4616/3/9/004
Citations: PlumX Metrics

1972KA52      Acta Phys.Pol. B3, 475 (1972)

B.N.Kalinkin, W.P.Permyakov, V.M.Shilov

Dynamic Deformation Effects in the Compound Nucleus Reaction

1971KA46      JINR-P4-6152 (1971)

B.N.Kalinkin, V.P.Permyakov, V.M.Shilov

Dynamic Deformation Effects in the Compound Nucleus Reactions