FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2334871886> ?p ?o ?g. }

• W2334871886 abstract "Background: The determination of the density dependence of the nuclear incompressibility can be investigated using the isoscalar giant monopole resonance.Purpose: The importance of the so-called crossing density at subsaturation density is underlined.Methods: The measurements of the isoscalar giant monopole resonance (GMR), also called the breathing mode, are analyzed with respect to their constraints on the quantity ${M}_{c}$, e.g., the density dependence of the nuclear incompressibility around the so-called crossing density ${ensuremath{rho}}_{c}=0.1$ fm${}^{ensuremath{-}3}$.Results: The correlation between the centroid of the GMR, ${E}_{mathrm{GMR}}$, and ${M}_{c}$ is shown to be more accurate than the one between ${E}_{mathrm{GMR}}$ and the incompressibility modulus at saturation density, ${K}_{ensuremath{infty}}$, giving rise to an improved determination on the nuclear equation of state. The relationship between ${M}_{c}$ and ${K}_{ensuremath{infty}}$ is given as a function of the skewness parameter ${Q}_{ensuremath{infty}}$ associated with the density dependence of the equation of state. The large variation of ${Q}_{ensuremath{infty}}$ among different energy density functionals directly impacts the knowledge of ${K}_{ensuremath{infty}}$: A better knowledge of ${Q}_{ensuremath{infty}}$ is required to deduce more accurately ${K}_{ensuremath{infty}}$. Using the local density approximation, a simple and accurate expression relating ${E}_{mathrm{GMR}}$ and the quantity ${M}_{c}$ is derived and successfully compared to the fully microscopic predictions.Conclusions: The measurement of the GMR constrains the slope of the incompressibility ${M}_{c}$ at the crossing density rather than the incompressibility modulus at the saturation density." @default.
• W2334871886 created "2016-06-24" @default.
• W2334871886 creator A5016544741 @default.
• W2334871886 creator A5022780772 @default.
• W2334871886 date "2013-09-25" @default.
• W2334871886 modified "2023-09-30" @default.
• W2334871886 title "Determination of the density dependence of the nuclear incompressibility" @default.
• W2334871886 cites W1556590149 @default.
• W2334871886 cites W1561074997 @default.
• W2334871886 cites W1964809169 @default.
• W2334871886 cites W1967598125 @default.
• W2334871886 cites W1968880988 @default.
• W2334871886 cites W1988716226 @default.
• W2334871886 cites W1988959494 @default.
• W2334871886 cites W1990168871 @default.
• W2334871886 cites W1993195985 @default.
• W2334871886 cites W2001286547 @default.
• W2334871886 cites W2007779595 @default.
• W2334871886 cites W2014929617 @default.
• W2334871886 cites W2018766212 @default.
• W2334871886 cites W2022365403 @default.
• W2334871886 cites W2026155951 @default.
• W2334871886 cites W2032330192 @default.
• W2334871886 cites W2040277408 @default.
• W2334871886 cites W2043804322 @default.
• W2334871886 cites W2046586965 @default.
• W2334871886 cites W2050866523 @default.
• W2334871886 cites W2056392302 @default.
• W2334871886 cites W2057898405 @default.
• W2334871886 cites W2058958401 @default.
• W2334871886 cites W2061700345 @default.
• W2334871886 cites W2070858305 @default.
• W2334871886 cites W2077494662 @default.
• W2334871886 cites W2079135475 @default.
• W2334871886 cites W2079933760 @default.
• W2334871886 cites W2084515973 @default.
• W2334871886 cites W2138392346 @default.
• W2334871886 cites W2222022162 @default.
• W2334871886 cites W2481701895 @default.
• W2334871886 cites W3099852616 @default.
• W2334871886 cites W3101622313 @default.
• W2334871886 cites W4252257690 @default.
• W2334871886 cites W4299580424 @default.
• W2334871886 doi "https://doi.org/10.1103/physrevc.88.034319" @default.
• W2334871886 hasPublicationYear "2013" @default.
• W2334871886 type Work @default.
• W2334871886 sameAs 2334871886 @default.
• W2334871886 citedByCount "64" @default.
• W2334871886 countsByYear W23348718862014 @default.
• W2334871886 countsByYear W23348718862015 @default.
• W2334871886 countsByYear W23348718862016 @default.
• W2334871886 countsByYear W23348718862017 @default.
• W2334871886 countsByYear W23348718862018 @default.
• W2334871886 countsByYear W23348718862019 @default.
• W2334871886 countsByYear W23348718862020 @default.
• W2334871886 countsByYear W23348718862021 @default.
• W2334871886 countsByYear W23348718862022 @default.
• W2334871886 countsByYear W23348718862023 @default.
• W2334871886 crossrefType "journal-article" @default.
• W2334871886 hasAuthorship W2334871886A5016544741 @default.
• W2334871886 hasAuthorship W2334871886A5022780772 @default.
• W2334871886 hasConcept C114614502 @default.
• W2334871886 hasConcept C121332964 @default.
• W2334871886 hasConcept C149298590 @default.
• W2334871886 hasConcept C165410206 @default.
• W2334871886 hasConcept C172695262 @default.
• W2334871886 hasConcept C184779094 @default.
• W2334871886 hasConcept C26873012 @default.
• W2334871886 hasConcept C2778560529 @default.
• W2334871886 hasConcept C2780070031 @default.
• W2334871886 hasConcept C33923547 @default.
• W2334871886 hasConcept C37914503 @default.
• W2334871886 hasConcept C62520636 @default.
• W2334871886 hasConcept C9930424 @default.
• W2334871886 hasConceptScore W2334871886C114614502 @default.
• W2334871886 hasConceptScore W2334871886C121332964 @default.
• W2334871886 hasConceptScore W2334871886C149298590 @default.
• W2334871886 hasConceptScore W2334871886C165410206 @default.
• W2334871886 hasConceptScore W2334871886C172695262 @default.
• W2334871886 hasConceptScore W2334871886C184779094 @default.
• W2334871886 hasConceptScore W2334871886C26873012 @default.
• W2334871886 hasConceptScore W2334871886C2778560529 @default.
• W2334871886 hasConceptScore W2334871886C2780070031 @default.
• W2334871886 hasConceptScore W2334871886C33923547 @default.
• W2334871886 hasConceptScore W2334871886C37914503 @default.
• W2334871886 hasConceptScore W2334871886C62520636 @default.
• W2334871886 hasConceptScore W2334871886C9930424 @default.
• W2334871886 hasIssue "3" @default.
• W2334871886 hasLocation W23348718861 @default.
• W2334871886 hasOpenAccess W2334871886 @default.
• W2334871886 hasPrimaryLocation W23348718861 @default.
• W2334871886 hasRelatedWork W1158643890 @default.
• W2334871886 hasRelatedWork W2022603373 @default.
• W2334871886 hasRelatedWork W2027775129 @default.
• W2334871886 hasRelatedWork W2033392392 @default.
• W2334871886 hasRelatedWork W2052158509 @default.
• W2334871886 hasRelatedWork W2070858305 @default.
• W2334871886 hasRelatedWork W2077288934 @default.
• W2334871886 hasRelatedWork W2334871886 @default.
• W2334871886 hasRelatedWork W2462749094 @default.

• next