Matches in SemOpenAlex for { <https://semopenalex.org/work/W2800698716> ?p ?o ?g. }
- W2800698716 endingPage "293" @default.
- W2800698716 startingPage "284" @default.
- W2800698716 abstract "We analyze the possibility to accommodate current b→sℓ+ℓ− anomalies with TeV-scale mediators that couple to right-handed top quarks and muons, contributing to b→sℓ+ℓ− at the one-loop level. We use the Standard Model Effective Field Theory (SMEFT) framework but also look at specific scenarios by taking into account all possible irreducible representations of the Lorentz and Standard Model gauge group for the mediators. From a global fit of b→sℓ+ℓ− data and LEP-I observables we find that the Wilson coefficients of two SMEFT operators: Oℓu=(ℓ¯LμγαℓLμ)(t¯RγαtR) and Oeu=(μ¯RγαμR)(t¯RγαtR) need to satisfy Ceu∼Cℓu. New physics enters then in b→sℓ+ℓ− mainly through the operator O9=(s¯γμPLb)(ℓ¯γμℓ) of the Weak Effective Theory. After discussing all possible mediators, we concentrate on two scenarios: A vector boson in the irreducible representation Zμ′∼(1,1,0) of the Standard Model gauge group with vectorial coupling to muons, and a combination of two leptoquarks: the scalar R2∼(3,2,7/6) and the vector U˜1μ∼(3,1,5/3). We derive LHC constraints by recasting di-muon resonance, pp→tt¯tt¯ and SUSY searches. Additionally, we analyze the prospects for discovering these mediators during the high-luminosity phase of the LHC." @default.
- W2800698716 created "2018-05-17" @default.
- W2800698716 creator A5055770586 @default.
- W2800698716 creator A5064259346 @default.
- W2800698716 creator A5071317702 @default.
- W2800698716 date "2018-09-01" @default.
- W2800698716 modified "2023-10-17" @default.
- W2800698716 title "Anomalies in bottom from new physics in top" @default.
- W2800698716 cites W1975211291 @default.
- W2800698716 cites W1977860841 @default.
- W2800698716 cites W1990203542 @default.
- W2800698716 cites W2053598037 @default.
- W2800698716 cites W2070269325 @default.
- W2800698716 cites W2073659158 @default.
- W2800698716 cites W2074992256 @default.
- W2800698716 cites W2096742001 @default.
- W2800698716 cites W2101169317 @default.
- W2800698716 cites W2125102738 @default.
- W2800698716 cites W2130052854 @default.
- W2800698716 cites W2159449603 @default.
- W2800698716 cites W2188479714 @default.
- W2800698716 cites W2275801130 @default.
- W2800698716 cites W2302365184 @default.
- W2800698716 cites W2304374836 @default.
- W2800698716 cites W2342998666 @default.
- W2800698716 cites W2558595427 @default.
- W2800698716 cites W2592770160 @default.
- W2800698716 cites W2595159827 @default.
- W2800698716 cites W2607289206 @default.
- W2800698716 cites W2608209582 @default.
- W2800698716 cites W2609225800 @default.
- W2800698716 cites W2611805866 @default.
- W2800698716 cites W2613501810 @default.
- W2800698716 cites W2614185328 @default.
- W2800698716 cites W2615418135 @default.
- W2800698716 cites W2747178068 @default.
- W2800698716 cites W2753339657 @default.
- W2800698716 cites W2794765155 @default.
- W2800698716 cites W2803183822 @default.
- W2800698716 cites W2923724224 @default.
- W2800698716 cites W3104268686 @default.
- W2800698716 cites W3124780715 @default.
- W2800698716 doi "https://doi.org/10.1016/j.physletb.2018.07.051" @default.
- W2800698716 hasPublicationYear "2018" @default.
- W2800698716 type Work @default.
- W2800698716 sameAs 2800698716 @default.
- W2800698716 citedByCount "73" @default.
- W2800698716 countsByYear W28006987162018 @default.
- W2800698716 countsByYear W28006987162019 @default.
- W2800698716 countsByYear W28006987162020 @default.
- W2800698716 countsByYear W28006987162021 @default.
- W2800698716 countsByYear W28006987162022 @default.
- W2800698716 countsByYear W28006987162023 @default.
- W2800698716 crossrefType "journal-article" @default.
- W2800698716 hasAuthorship W2800698716A5055770586 @default.
- W2800698716 hasAuthorship W2800698716A5064259346 @default.
- W2800698716 hasAuthorship W2800698716A5071317702 @default.
- W2800698716 hasBestOaLocation W28006987161 @default.
- W2800698716 hasConcept C101454708 @default.
- W2800698716 hasConcept C109214941 @default.
- W2800698716 hasConcept C116674579 @default.
- W2800698716 hasConcept C121332964 @default.
- W2800698716 hasConcept C155700901 @default.
- W2800698716 hasConcept C158129726 @default.
- W2800698716 hasConcept C163387558 @default.
- W2800698716 hasConcept C166957645 @default.
- W2800698716 hasConcept C181830111 @default.
- W2800698716 hasConcept C184748400 @default.
- W2800698716 hasConcept C205334942 @default.
- W2800698716 hasConcept C207206121 @default.
- W2800698716 hasConcept C2524010 @default.
- W2800698716 hasConcept C2779430453 @default.
- W2800698716 hasConcept C32848918 @default.
- W2800698716 hasConcept C33923547 @default.
- W2800698716 hasConcept C40263606 @default.
- W2800698716 hasConcept C40976572 @default.
- W2800698716 hasConcept C57691317 @default.
- W2800698716 hasConcept C62520636 @default.
- W2800698716 hasConcept C7602139 @default.
- W2800698716 hasConcept C87668248 @default.
- W2800698716 hasConcept C95457728 @default.
- W2800698716 hasConceptScore W2800698716C101454708 @default.
- W2800698716 hasConceptScore W2800698716C109214941 @default.
- W2800698716 hasConceptScore W2800698716C116674579 @default.
- W2800698716 hasConceptScore W2800698716C121332964 @default.
- W2800698716 hasConceptScore W2800698716C155700901 @default.
- W2800698716 hasConceptScore W2800698716C158129726 @default.
- W2800698716 hasConceptScore W2800698716C163387558 @default.
- W2800698716 hasConceptScore W2800698716C166957645 @default.
- W2800698716 hasConceptScore W2800698716C181830111 @default.
- W2800698716 hasConceptScore W2800698716C184748400 @default.
- W2800698716 hasConceptScore W2800698716C205334942 @default.
- W2800698716 hasConceptScore W2800698716C207206121 @default.
- W2800698716 hasConceptScore W2800698716C2524010 @default.
- W2800698716 hasConceptScore W2800698716C2779430453 @default.
- W2800698716 hasConceptScore W2800698716C32848918 @default.
- W2800698716 hasConceptScore W2800698716C33923547 @default.
- W2800698716 hasConceptScore W2800698716C40263606 @default.