Matches in SemOpenAlex for { <https://semopenalex.org/work/W2091270708> ?p ?o ?g. }
- W2091270708 endingPage "16" @default.
- W2091270708 startingPage "1" @default.
- W2091270708 abstract "We consider the scenario in which the mass matrices of the charged fermions in the SO(10) Grand Unified Theory are generated exclusively by renormalizable Yukawa couplings to one $mathbf{10} oplus mathbf{120}$ representation of scalars. We analyze, partly analytically and partly numerically, this scenario in the three-generations case. We demonstrate that it leads to unification of the $b$ and $tau$ masses at the GUT scale. Testing this scenario against the mass values at the GUT scale, obtained from the renormalization-group evolution in the minimal SUSY extension of the Standard Model, we find that it is not viable: either the down-quark mass or the top-quark mass must be unrealistically low. If we include the CKM mixing angles in the test, then, in order that the mixing angles are well reproduced, either the top-quark mass or the strange-quark mass together with the down-quark mass must be very low. We conclude that, assuming a SUSY SO(10) scenario, charged-fermion mass generation based exclusively on one $mathbf{10} oplus mathbf{120}$ representation of scalars is in contradiction with experiment." @default.
- W2091270708 created "2016-06-24" @default.
- W2091270708 creator A5039022330 @default.
- W2091270708 creator A5040811602 @default.
- W2091270708 creator A5068327568 @default.
- W2091270708 date "2006-10-01" @default.
- W2091270708 modified "2023-09-25" @default.
- W2091270708 title "Charged-fermion masses in : Analysis with scalars in" @default.
- W2091270708 cites W1489445685 @default.
- W2091270708 cites W1877342203 @default.
- W2091270708 cites W1894770353 @default.
- W2091270708 cites W1971501420 @default.
- W2091270708 cites W1976640883 @default.
- W2091270708 cites W1994413830 @default.
- W2091270708 cites W2000187595 @default.
- W2091270708 cites W2036294220 @default.
- W2091270708 cites W2051238465 @default.
- W2091270708 cites W2065927088 @default.
- W2091270708 cites W2071066963 @default.
- W2091270708 cites W2071881521 @default.
- W2091270708 cites W2077957873 @default.
- W2091270708 cites W2086841760 @default.
- W2091270708 cites W2089507017 @default.
- W2091270708 cites W2089723933 @default.
- W2091270708 cites W2093545060 @default.
- W2091270708 cites W2101073879 @default.
- W2091270708 cites W2113845947 @default.
- W2091270708 cites W2144755732 @default.
- W2091270708 cites W2147827569 @default.
- W2091270708 cites W2159108216 @default.
- W2091270708 cites W2164299440 @default.
- W2091270708 cites W2166252135 @default.
- W2091270708 cites W2171074980 @default.
- W2091270708 cites W2600135814 @default.
- W2091270708 cites W3100349832 @default.
- W2091270708 cites W3105944759 @default.
- W2091270708 doi "https://doi.org/10.1016/j.nuclphysb.2006.07.024" @default.
- W2091270708 hasPublicationYear "2006" @default.
- W2091270708 type Work @default.
- W2091270708 sameAs 2091270708 @default.
- W2091270708 citedByCount "26" @default.
- W2091270708 countsByYear W20912707082012 @default.
- W2091270708 countsByYear W20912707082014 @default.
- W2091270708 countsByYear W20912707082015 @default.
- W2091270708 countsByYear W20912707082016 @default.
- W2091270708 countsByYear W20912707082017 @default.
- W2091270708 countsByYear W20912707082019 @default.
- W2091270708 countsByYear W20912707082020 @default.
- W2091270708 countsByYear W20912707082021 @default.
- W2091270708 crossrefType "journal-article" @default.
- W2091270708 hasAuthorship W2091270708A5039022330 @default.
- W2091270708 hasAuthorship W2091270708A5040811602 @default.
- W2091270708 hasAuthorship W2091270708A5068327568 @default.
- W2091270708 hasBestOaLocation W20912707082 @default.
- W2091270708 hasConcept C101454708 @default.
- W2091270708 hasConcept C109214941 @default.
- W2091270708 hasConcept C116674579 @default.
- W2091270708 hasConcept C121332964 @default.
- W2091270708 hasConcept C138777275 @default.
- W2091270708 hasConcept C150522085 @default.
- W2091270708 hasConcept C151195881 @default.
- W2091270708 hasConcept C166957645 @default.
- W2091270708 hasConcept C187783895 @default.
- W2091270708 hasConcept C207206121 @default.
- W2091270708 hasConcept C37914503 @default.
- W2091270708 hasConcept C40976572 @default.
- W2091270708 hasConcept C52233224 @default.
- W2091270708 hasConcept C62520636 @default.
- W2091270708 hasConcept C68532491 @default.
- W2091270708 hasConcept C7602139 @default.
- W2091270708 hasConcept C95457728 @default.
- W2091270708 hasConceptScore W2091270708C101454708 @default.
- W2091270708 hasConceptScore W2091270708C109214941 @default.
- W2091270708 hasConceptScore W2091270708C116674579 @default.
- W2091270708 hasConceptScore W2091270708C121332964 @default.
- W2091270708 hasConceptScore W2091270708C138777275 @default.
- W2091270708 hasConceptScore W2091270708C150522085 @default.
- W2091270708 hasConceptScore W2091270708C151195881 @default.
- W2091270708 hasConceptScore W2091270708C166957645 @default.
- W2091270708 hasConceptScore W2091270708C187783895 @default.
- W2091270708 hasConceptScore W2091270708C207206121 @default.
- W2091270708 hasConceptScore W2091270708C37914503 @default.
- W2091270708 hasConceptScore W2091270708C40976572 @default.
- W2091270708 hasConceptScore W2091270708C52233224 @default.
- W2091270708 hasConceptScore W2091270708C62520636 @default.
- W2091270708 hasConceptScore W2091270708C68532491 @default.
- W2091270708 hasConceptScore W2091270708C7602139 @default.
- W2091270708 hasConceptScore W2091270708C95457728 @default.
- W2091270708 hasIssue "1-2" @default.
- W2091270708 hasLocation W20912707081 @default.
- W2091270708 hasLocation W20912707082 @default.
- W2091270708 hasLocation W20912707083 @default.
- W2091270708 hasOpenAccess W2091270708 @default.
- W2091270708 hasPrimaryLocation W20912707081 @default.
- W2091270708 hasRelatedWork W1533308835 @default.
- W2091270708 hasRelatedWork W1847194422 @default.
- W2091270708 hasRelatedWork W1855396010 @default.
- W2091270708 hasRelatedWork W1994106981 @default.