Publication data of Bennaceur, Karim: Link to Inspire

Created with Highcharts 9.0.1CitationsCitationsw/o self-citaionself-citaion200020052010201520202025050010001500200025003000
Created with Highcharts 9.0.1Publicationspublications per yearPublicationsPublications per yearCumulative publications2000200520102015202020250122436486001.534.567.5
Created with Highcharts 9.0.1h-indexh-indexh-indexh-index w/o self-citaion200020052010201520202025051015202530
Created with Highcharts 9.0.1CitationsBreakdown of Most Cited PapersrestHalo phenomenon in finite many-fermion systems. Atom-positron complexes and large-scale study of atomic nucleiHalo phenomenon in finite many-fermion systems. Atom-positron complexes …Constraining the surface properties of effective Skyrme interactionsEffective theory for low-energy nuclear energy density functionalsEffective theory for low-energy nuclear energy density functionalsNuclear response for the Skyrme effective interaction with zero-range tensor terms. II. Sum rules and instabilitiesNuclear response for the Skyrme effective interaction with zero-range tensor …Nuclear response for the Skyrme effective interaction with zero range tensor termsNuclear response for the Skyrme effective interaction with zero range tensor …Continuum effects for the mean field and pairing properties of weakly bound nucleiContinuum effects for the mean field and pairing properties of weakly bound…Spurious finite-size instabilities in nuclear energy density functionalsAnalysis of the 0-16(p,gamma)F-17 capture reaction using the shell model embedded in the continuumAnalysis of the 0-16(p,gamma)F-17 capture reaction using the shell model e…Non-empirical pairing energy density functional. First order in the nuclear plus Coulomb two-body interactionNon-empirical pairing energy density functional. First order in the nuclear plu…Study of the Be-7(p, gamma)B-8 and Li-7(n, gamma)Li-8 capture reactions using the shell model embedded in the continuumStudy of the Be-7(p, gamma)B-8 and Li-7(n, gamma)Li-8 capture reactions u…Pairing anti-halo effectIsovector splitting of nucleon effective masses, ab-initio benchmarks and extended stability criteria for Skyrme energy functionalsIsovector splitting of nucleon effective masses, ab-initio benchmarks and ext…Particle-Number Restoration within the Energy Density Functional formalism: Are terms depending on non-integer powers of the density matrices viable?Particle-Number Restoration within the Energy Density Functional formalism: …Tensor part of the Skyrme energy density functional. II: Deformation properties of magic and semi-magic nucleiTensor part of the Skyrme energy density functional. II: Deformation properti…Coordinate-space solution of the Skyrme-Hartree-Fock-Bogolyubov equations within spherical symmetry. The Program HFBRAD (v1.00)Coordinate-space solution of the Skyrme-Hartree-Fock-Bogolyubov equations …Microscopic determination of the nuclear incompressibility within the nonrelativistic frameworkMicroscopic determination of the nuclear incompressibility within the nonrela…Gamow shell model description of neutron rich nucleiThe Tensor part of the Skyrme energy density functional. I. Spherical nuclei200020052010201520202025050010001500200025003000
Created with Highcharts 9.0.1Fraction [%]Breakdown of Most Cited Papers (Fraction)Halo phenomenon in finite many-fermion systems. Atom-positron complexes and large-scale study of atomic nucleiHalo phenomenon in finite many-fermion systems. Atom-positron complexes …Constraining the surface properties of effective Skyrme interactionsEffective theory for low-energy nuclear energy density functionalsEffective theory for low-energy nuclear energy density functionalsNuclear response for the Skyrme effective interaction with zero-range tensor terms. II. Sum rules and instabilitiesNuclear response for the Skyrme effective interaction with zero-range tensor …Nuclear response for the Skyrme effective interaction with zero range tensor termsNuclear response for the Skyrme effective interaction with zero range tensor …Continuum effects for the mean field and pairing properties of weakly bound nucleiContinuum effects for the mean field and pairing properties of weakly bound…Spurious finite-size instabilities in nuclear energy density functionalsAnalysis of the 0-16(p,gamma)F-17 capture reaction using the shell model embedded in the continuumAnalysis of the 0-16(p,gamma)F-17 capture reaction using the shell model e…Non-empirical pairing energy density functional. First order in the nuclear plus Coulomb two-body interactionNon-empirical pairing energy density functional. First order in the nuclear plu…Study of the Be-7(p, gamma)B-8 and Li-7(n, gamma)Li-8 capture reactions using the shell model embedded in the continuumStudy of the Be-7(p, gamma)B-8 and Li-7(n, gamma)Li-8 capture reactions u…Pairing anti-halo effectIsovector splitting of nucleon effective masses, ab-initio benchmarks and extended stability criteria for Skyrme energy functionalsIsovector splitting of nucleon effective masses, ab-initio benchmarks and ext…Particle-Number Restoration within the Energy Density Functional formalism: Are terms depending on non-integer powers of the density matrices viable?Particle-Number Restoration within the Energy Density Functional formalism: …Tensor part of the Skyrme energy density functional. II: Deformation properties of magic and semi-magic nucleiTensor part of the Skyrme energy density functional. II: Deformation properti…Coordinate-space solution of the Skyrme-Hartree-Fock-Bogolyubov equations within spherical symmetry. The Program HFBRAD (v1.00)Coordinate-space solution of the Skyrme-Hartree-Fock-Bogolyubov equations …Microscopic determination of the nuclear incompressibility within the nonrelativistic frameworkMicroscopic determination of the nuclear incompressibility within the nonrela…Gamow shell model description of neutron rich nucleiThe Tensor part of the Skyrme energy density functional. I. Spherical nuclei2000200520102015202020250255075100
Created with Highcharts 9.0.1Citations/1 YearCitations/PeriodCitations / 1 YearMoving average200020052010201520202025050100150200250