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NSR database version of May 1, 2024.

Search: Author = L.Shvedov

Found 15 matches.

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2010SH09      Phys.Rev. C 81, 054605 (2010)

L.Shvedov, M.Colonna, M.Di Toro

Breakup mechanisms in heavy-ion collisions at low energies

NUCLEAR REACTIONS ⁹⁶Zr(³⁶Ar, X), E=9, 16 MeV/nucleon; ¹⁹⁷Au(¹⁹⁷Au, X), E=15 MeV/nucleon; calculated contour plots of the density, dependence of excitation energies, intrinsic angular momentum, quadrupole and octupole moments on fusion σ, deep inelastic and fragmentation (breakup) σ using stochastic mean-field (SMF) model.

doi: 10.1103/PhysRevC.81.054605
Citations: PlumX Metrics

2008KO06      Int.J.Mod.Phys. E17, 259 (2008)

M.Kowal, L.Shvedov, A.Sobiczewski

Saddle-point shell effects of heaviest nuclei

NUCLEAR STRUCTURE Z=96-126; N=136-194; calculated shell corrections at the saddle points and ground states of the considered nuclei. Contour maps using macroscopic-microscopic approach.

doi: 10.1142/S021830130800977X
Citations: PlumX Metrics

2008SH10      Int.J.Mod.Phys. E17, 265 (2008)

L.Shvedov, S.G.Rohozinski, M.Kowal, S.Belchikov, A.Sobiczewski

Deformations of multipolarity six at the saddle point of heaviest nuclei

NUCLEAR STRUCTURE Z=98-122; N=138-190; calculated deformation parameters and potential energies. Contour maps using Macroscopic-microscopic approach.

doi: 10.1142/S0218301308009781
Citations: PlumX Metrics

2008SO06      Int.J.Mod.Phys. E17, 168 (2008)

A.Sobiczewski, M.Kowal, L.Shvedov

Saddle-point shapes of heavy and superheavy nuclei

NUCLEAR STRUCTURE Z=98-126; N=138-194; calculated deformation parameters and shapes of nuclei at their saddle-points and ground states using 10 dimensions macroscopic-microscopic approach.

doi: 10.1142/S0218301308009665
Citations: PlumX Metrics

2007SH20      Acta Phys.Pol. B38, 1583 (2007)

L.Shvedov, A.Sobiczewski

Non-Axial Hexadecapole Deformations of Heaviest Nuclei

NUCLEAR STRUCTURE ²⁵⁰Cf; calculated potential energy in 5-dimensional deformation space.

2007SO05      Int.J.Mod.Phys. E16, 402 (2007)

A.Sobiczewski, L.Shvedov, M.Kowal

Test of approximation used in description of non-axial hexadecapole shapes of heaviest nuclei

NUCLEAR STRUCTURE ²⁶²Sg, ²⁸⁴Fl; calculated total energy vs deformation. Five-dimensional deformation space.

doi: 10.1142/S0218301307005831
Citations: PlumX Metrics

2007SO11      Acta Phys.Pol. B38, 1577 (2007)

A.Sobiczewski, M.Kowal, L.Shvedov

Search for Less Important Deformations in the Shapes of Heaviest Nuclei

NUCLEAR STRUCTURE ²⁶²Sg; calculated potential energy in 5-dimensional deformation space.

2006BL04      Int.J.Mod.Phys. E15, 426 (2006)

J.Blocki, L.Shvedov, J.Wilczynski

Dynamical hindrance of fusion of superheavy nuclei

NUCLEAR REACTIONS ²⁰⁸Pb(⁴⁸Ca, X), (⁵⁰Ti, X), (⁵⁴Cr, X), (⁵⁸Fe, X), (⁶⁴Ni, X), (⁷⁰Zn, X), (⁸⁶Kr, X), E not given; calculated fusion probabilities, dynamical hindrance effects.

doi: 10.1142/S0218301306004302
Citations: PlumX Metrics

2005BL11      Int.J.Mod.Phys. E14, 315 (2005)

J.Blocki, L.Shvedov, J.Wilczynski

Deformation energies of nuclear systems

NUCLEAR REACTIONS ¹³⁶Cs(¹³⁶Cs, X), ²⁵²Fm(²⁰Ne, X), E not given; calculated potential energy surfaces, deformation energy.

doi: 10.1142/S0218301305003053
Citations: PlumX Metrics

2005SH17      Int.J.Mod.Phys. E14, 321 (2005)

L.Shvedov, J.Blocki, J.Wilczynski

Tests of the dynamics of deep inelastic collisions

NUCLEAR REACTIONS ¹⁶⁶Er(⁸⁶Kr, X), E=8.18 MeV/nucleon; ¹⁵⁴Sm(¹⁵⁴Sm, X), E=6.3 MeV/nucleon; calculated σ(E, θ), dynamical trajectories. Rayleigh-Lagrange equations.

doi: 10.1142/S0218301305003065
Citations: PlumX Metrics

2003SH42      Acta Phys.Pol. B34, 1815 (2003)

L.Shvedov, J.Blocki, J.Wilczynski

Potential energy surface in nucleus-nucleus collisions corrected for exact nuclear masses

NUCLEAR STRUCTURE Z=71-100; A=173-255; calculated fusion and fission barrier energies. Macroscopic approach, comparison with data.

NUCLEAR REACTIONS ¹⁴⁴Sm(¹⁶O, X), E(cm)=55-70 MeV; calculated fusion barrier distribution. ¹⁶⁶Er(⁸⁶Kr, X), E=8.18 MeV/nucleon; calculated σ(E, θ). Macroscopic approach, comparison with data.

2002SH03      Acta Phys.Pol. B33, 439 (2002)

L.Shvedov, J.Blocki, J.Wilczynski

Calculations of Fission Barriers with Deformation-Dependent Attenuation of Shell Corrections

NUCLEAR STRUCTURE Z=66-100; calculated fission barrier energies, shell effects. Comparison with data.

2001FI25      Bull.Rus.Acad.Sci.Phys. 65, 689 (2001)

G.F.Filippov, Yu.A.Lashko, L.P.Shvedov

Photodisintegration of Light Neutron-Rich Nuclei and Radiative Capture of Two Neutrons by Light Nuclei

NUCLEAR STRUCTURE ⁶He, ¹¹Li; calculated photodisintigration matrix elements, resonance effects, related features.

2000FI21      Iader.Fiz.Enerh. 1, no.1, 39 (2000)

G.F.Filippov, Yu.A.Lashko, L.P.Shvedov

Soft dipole mode of neutron-rich light nuclei in asymptotic potential approximation

NUCLEAR STRUCTURE ⁶He; calculated wavefunctions. Three-cluster model with resonating group method.

NUCLEAR REACTIONS ¹¹Li(γ, 2n), E<MeV; calculated σ of photodisintegration, resonance energy.

doi: 10.15407/jnpae
Citations: PlumX Metrics

1999FI11      Yad.Fiz. 62, No 10, 1772 (1999); Phys.Atomic Nuclei 62, 1651 (1999)

G.F.Filippov, Yu.A.Lashko, L.P.Shvedov

Asymptotic-Potential Approximation and Soft Dipole Mode in the ⁶He Nuclear System

NUCLEAR STRUCTURE ⁶He; calculated soft dipole mode wave functions, transition matrix elements. Three-cluster approach, zero-range nuclear force approximation.

Note: The following list of authors and aliases matches the search parameter L.Shvedov: , L.P.SHVEDOV