FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2562865701> ?p ?o ?g. }

• W2562865701 abstract "The nucleon single-particle energies (SPEs) of the selected nuclei, that is, <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML id=M2><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=normal>O</mml:mi></mml:mrow><mml:mprescripts /><mml:none /><mml:mrow><mml:mn fontstyle=italic>16</mml:mn></mml:mrow></mml:mmultiscripts></mml:mrow></mml:math>, <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML id=M3><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=normal>C</mml:mi><mml:mi mathvariant=normal>a</mml:mi></mml:mrow><mml:mprescripts /><mml:none /><mml:mrow><mml:mn fontstyle=italic>40</mml:mn></mml:mrow></mml:mmultiscripts></mml:mrow></mml:math>, and <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML id=M4><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=normal>N</mml:mi><mml:mi mathvariant=normal>i</mml:mi></mml:mrow><mml:mprescripts /><mml:none /><mml:mrow><mml:mn fontstyle=italic>56</mml:mn></mml:mrow></mml:mmultiscripts></mml:mrow></mml:math>, are obtained by using the diagonal matrix elements of two-body effective interaction, which generated through the lowest-order constrained variational (LOCV) calculations for the symmetric nuclear matter with the <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML id=M5><mml:mrow><mml:msub><mml:mrow><mml:mi>A</mml:mi><mml:mi>υ</mml:mi></mml:mrow><mml:mrow><mml:mn fontstyle=italic>18</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math> phenomenological nucleon-nucleon potential. The SPEs at the major levels of nuclei are calculated by employing a Hartree-Fock inspired scheme in the spherical harmonic oscillator basis. In the scheme, the correlation influences are taken into account by imposing the nucleon effective mass factor on the radial wave functions of the major levels. Replacing the density-dependent one-body momentum distribution functions of nucleons, <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML id=M6><mml:mi>n</mml:mi><mml:mo stretchy=false>(</mml:mo><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>ρ</mml:mi><mml:mo stretchy=false>)</mml:mo></mml:math>, with the Heaviside functions, the role of <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML id=M7><mml:mi>n</mml:mi><mml:mo stretchy=false>(</mml:mo><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>ρ</mml:mi><mml:mo stretchy=false>)</mml:mo></mml:math> in the nucleon SPEs at the major levels of the selected closed shell nuclei is investigated. The best fit of spin-orbit splitting is taken into account when correcting the major levels of the nuclei by using the parameterized Wood-Saxon potential and the <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML id=M8><mml:mrow><mml:msub><mml:mrow><mml:mi>A</mml:mi><mml:mi>υ</mml:mi></mml:mrow><mml:mrow><mml:mn fontstyle=italic>18</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math> density-dependent mean field potential which is constructed by the LOCV method. Considering the point-like protons in the spherical Coulomb potential well, the single-proton energies are corrected. The results show the importance of including <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML id=M9><mml:mi>n</mml:mi><mml:mo stretchy=false>(</mml:mo><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>ρ</mml:mi><mml:mo stretchy=false>)</mml:mo></mml:math>, instead of the Heaviside functions, in the calculation of nucleon SPEs at the different levels, particularly the valence levels, of the closed shell nuclei." @default.
• W2562865701 created "2017-01-06" @default.
• W2562865701 creator A5064645058 @default.
• W2562865701 date "2016-01-01" @default.
• W2562865701 modified "2023-09-26" @default.
• W2562865701 title "The Calculation of Single-Nucleon Energies of Nuclei by Considering Two-Body Effective Interaction, n(k,ρ), and a Hartree-Fock Inspired Scheme" @default.
• W2562865701 cites W1526998169 @default.
• W2562865701 cites W1579672771 @default.
• W2562865701 cites W174937481 @default.
• W2562865701 cites W1967200826 @default.
• W2562865701 cites W1967324410 @default.
• W2562865701 cites W1967974620 @default.
• W2562865701 cites W1968986208 @default.
• W2562865701 cites W1975513956 @default.
• W2562865701 cites W1975942761 @default.
• W2562865701 cites W1976417308 @default.
• W2562865701 cites W1980262530 @default.
• W2562865701 cites W1980384226 @default.
• W2562865701 cites W1982086491 @default.
• W2562865701 cites W1983907592 @default.
• W2562865701 cites W1991160162 @default.
• W2562865701 cites W1991212332 @default.
• W2562865701 cites W1993723808 @default.
• W2562865701 cites W2004766095 @default.
• W2562865701 cites W2005459592 @default.
• W2562865701 cites W2007781256 @default.
• W2562865701 cites W2008601503 @default.
• W2562865701 cites W2009440364 @default.
• W2562865701 cites W2013568226 @default.
• W2562865701 cites W2014419790 @default.
• W2562865701 cites W2018147776 @default.
• W2562865701 cites W2018909176 @default.
• W2562865701 cites W2022871871 @default.
• W2562865701 cites W2024616797 @default.
• W2562865701 cites W2025239446 @default.
• W2562865701 cites W2027761417 @default.
• W2562865701 cites W2029013374 @default.
• W2562865701 cites W2031189803 @default.
• W2562865701 cites W2033439717 @default.
• W2562865701 cites W2034834282 @default.
• W2562865701 cites W2037308760 @default.
• W2562865701 cites W2042721135 @default.
• W2562865701 cites W2042762615 @default.
• W2562865701 cites W2043499236 @default.
• W2562865701 cites W2047276824 @default.
• W2562865701 cites W2049368631 @default.
• W2562865701 cites W2049886386 @default.
• W2562865701 cites W2050773679 @default.
• W2562865701 cites W2055716906 @default.
• W2562865701 cites W2057265173 @default.
• W2562865701 cites W2059535538 @default.
• W2562865701 cites W2059823880 @default.
• W2562865701 cites W2060768354 @default.
• W2562865701 cites W2066768197 @default.
• W2562865701 cites W2067920970 @default.
• W2562865701 cites W2069193162 @default.
• W2562865701 cites W2076908219 @default.
• W2562865701 cites W2077704283 @default.
• W2562865701 cites W2079190662 @default.
• W2562865701 cites W2080388803 @default.
• W2562865701 cites W2080984655 @default.
• W2562865701 cites W2088735851 @default.
• W2562865701 cites W2089630383 @default.
• W2562865701 cites W2092509450 @default.
• W2562865701 cites W2096487969 @default.
• W2562865701 cites W2103042358 @default.
• W2562865701 cites W2121327303 @default.
• W2562865701 cites W2123521731 @default.
• W2562865701 cites W2136600591 @default.
• W2562865701 cites W2154316819 @default.
• W2562865701 cites W2167360655 @default.
• W2562865701 cites W2249096513 @default.
• W2562865701 cites W2266298513 @default.
• W2562865701 cites W2289319316 @default.
• W2562865701 cites W2315088083 @default.
• W2562865701 cites W2318963387 @default.
• W2562865701 cites W2342542372 @default.
• W2562865701 cites W2766613685 @default.
• W2562865701 cites W2963946687 @default.
• W2562865701 cites W3099271055 @default.
• W2562865701 cites W3100519848 @default.
• W2562865701 cites W3101822323 @default.
• W2562865701 cites W48545552 @default.
• W2562865701 doi "https://doi.org/10.1155/2016/2398198" @default.
• W2562865701 hasPublicationYear "2016" @default.
• W2562865701 type Work @default.
• W2562865701 sameAs 2562865701 @default.
• W2562865701 citedByCount "0" @default.
• W2562865701 crossrefType "journal-article" @default.
• W2562865701 hasAuthorship W2562865701A5064645058 @default.
• W2562865701 hasBestOaLocation W25628657011 @default.
• W2562865701 hasConcept C11413529 @default.
• W2562865701 hasConcept C121332964 @default.
• W2562865701 hasConcept C41008148 @default.
• W2562865701 hasConceptScore W2562865701C11413529 @default.
• W2562865701 hasConceptScore W2562865701C121332964 @default.
• W2562865701 hasConceptScore W2562865701C41008148 @default.
• W2562865701 hasLocation W25628657011 @default.
• W2562865701 hasLocation W25628657012 @default.
• W2562865701 hasLocation W25628657013 @default.

• next