Matches in SemOpenAlex for { <https://semopenalex.org/work/W8518108> ?p ?o ?g. }
- W8518108 endingPage "2157" @default.
- W8518108 startingPage "2148" @default.
- W8518108 abstract "Estimates of the ${K}^{0}ensuremath{leftrightarrow}{overline{K}}^{0}$ transition amplitude and the resulting ${K}_{L}{K}_{S}$ mass difference are often based on an effective-Lagrangian treatment, where ${mathrm{L}}_{mathrm{eff}}$ is taken to be the four-quark operator extracted from a lowest-order calculation of the free-quark $overline{s}+densuremath{rightarrow}s+overline{d}$ scattering amplitude. For conventional SU(2) ifmmodetimeselsetexttimesfi{} U(1) models this effective Lagrangian has the form of a ($Vensuremath{-}A$) current-current interaction ${mathrm{O}}_{mathrm{JJ}}$, with coefficient $C$ parametrized by quark masses and mixing angles. An important question has to do with gluonic and other corrections to the coefficient, but, independent of this, it is also necessary to estimate the matrix element of ${mathrm{O}}_{mathrm{JJ}}$ between physical ${K}^{0}$ and ${overline{K}}^{0}$ states. We focus on this aspect of the problem. Earlier treatments have relied on a vacuum-insertion approximation. For an alternative approach, we employ the static MIT bag model. With the standard values for the bag parameters the matrix element is smaller than that obtained with vacuum insertion by about a factor of 2. This result is reasonably stable for small variations of the bag parameters." @default.
- W8518108 created "2016-06-24" @default.
- W8518108 creator A5010265679 @default.
- W8518108 creator A5085941621 @default.
- W8518108 date "1979-04-01" @default.
- W8518108 modified "2023-09-23" @default.
- W8518108 title "K0↔K¯0transition amplitude in the MIT bag model" @default.
- W8518108 cites W1830784226 @default.
- W8518108 cites W1975741267 @default.
- W8518108 cites W1979224787 @default.
- W8518108 cites W1989719773 @default.
- W8518108 cites W1990355630 @default.
- W8518108 cites W1992152154 @default.
- W8518108 cites W2002668600 @default.
- W8518108 cites W2013651360 @default.
- W8518108 cites W2018794521 @default.
- W8518108 cites W2028025282 @default.
- W8518108 cites W2035031418 @default.
- W8518108 cites W2049385248 @default.
- W8518108 cites W2057871911 @default.
- W8518108 cites W2070151728 @default.
- W8518108 cites W2101310208 @default.
- W8518108 cites W2117836026 @default.
- W8518108 cites W2128114549 @default.
- W8518108 cites W214481809 @default.
- W8518108 cites W2167184126 @default.
- W8518108 cites W2169090745 @default.
- W8518108 cites W2200155420 @default.
- W8518108 cites W2991355137 @default.
- W8518108 cites W43950810 @default.
- W8518108 doi "https://doi.org/10.1103/physrevd.19.2148" @default.
- W8518108 hasPublicationYear "1979" @default.
- W8518108 type Work @default.
- W8518108 sameAs 8518108 @default.
- W8518108 citedByCount "73" @default.
- W8518108 countsByYear W85181082014 @default.
- W8518108 countsByYear W85181082018 @default.
- W8518108 countsByYear W85181082020 @default.
- W8518108 countsByYear W85181082021 @default.
- W8518108 crossrefType "journal-article" @default.
- W8518108 hasAuthorship W8518108A5010265679 @default.
- W8518108 hasAuthorship W8518108A5085941621 @default.
- W8518108 hasConcept C10138342 @default.
- W8518108 hasConcept C101454708 @default.
- W8518108 hasConcept C104317684 @default.
- W8518108 hasConcept C106487976 @default.
- W8518108 hasConcept C109214941 @default.
- W8518108 hasConcept C121332964 @default.
- W8518108 hasConcept C153013531 @default.
- W8518108 hasConcept C158448853 @default.
- W8518108 hasConcept C159985019 @default.
- W8518108 hasConcept C162324750 @default.
- W8518108 hasConcept C166957645 @default.
- W8518108 hasConcept C17020691 @default.
- W8518108 hasConcept C176616139 @default.
- W8518108 hasConcept C180205008 @default.
- W8518108 hasConcept C182306322 @default.
- W8518108 hasConcept C185592680 @default.
- W8518108 hasConcept C192562407 @default.
- W8518108 hasConcept C2776249927 @default.
- W8518108 hasConcept C2779985612 @default.
- W8518108 hasConcept C2994345751 @default.
- W8518108 hasConcept C37914503 @default.
- W8518108 hasConcept C40976572 @default.
- W8518108 hasConcept C53469067 @default.
- W8518108 hasConcept C55493867 @default.
- W8518108 hasConcept C62520636 @default.
- W8518108 hasConcept C7602139 @default.
- W8518108 hasConcept C86339819 @default.
- W8518108 hasConcept C95457728 @default.
- W8518108 hasConceptScore W8518108C10138342 @default.
- W8518108 hasConceptScore W8518108C101454708 @default.
- W8518108 hasConceptScore W8518108C104317684 @default.
- W8518108 hasConceptScore W8518108C106487976 @default.
- W8518108 hasConceptScore W8518108C109214941 @default.
- W8518108 hasConceptScore W8518108C121332964 @default.
- W8518108 hasConceptScore W8518108C153013531 @default.
- W8518108 hasConceptScore W8518108C158448853 @default.
- W8518108 hasConceptScore W8518108C159985019 @default.
- W8518108 hasConceptScore W8518108C162324750 @default.
- W8518108 hasConceptScore W8518108C166957645 @default.
- W8518108 hasConceptScore W8518108C17020691 @default.
- W8518108 hasConceptScore W8518108C176616139 @default.
- W8518108 hasConceptScore W8518108C180205008 @default.
- W8518108 hasConceptScore W8518108C182306322 @default.
- W8518108 hasConceptScore W8518108C185592680 @default.
- W8518108 hasConceptScore W8518108C192562407 @default.
- W8518108 hasConceptScore W8518108C2776249927 @default.
- W8518108 hasConceptScore W8518108C2779985612 @default.
- W8518108 hasConceptScore W8518108C2994345751 @default.
- W8518108 hasConceptScore W8518108C37914503 @default.
- W8518108 hasConceptScore W8518108C40976572 @default.
- W8518108 hasConceptScore W8518108C53469067 @default.
- W8518108 hasConceptScore W8518108C55493867 @default.
- W8518108 hasConceptScore W8518108C62520636 @default.
- W8518108 hasConceptScore W8518108C7602139 @default.
- W8518108 hasConceptScore W8518108C86339819 @default.
- W8518108 hasConceptScore W8518108C95457728 @default.