FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2916877376> ?p ?o ?g. }

• W2916877376 endingPage "114636" @default.
• W2916877376 startingPage "114636" @default.
• W2916877376 abstract "If neutrinos are Dirac particles, their right-handed partners must be present in the theory. Once introduced in the Standard Model (SM), the difference between the baryon number $B$ and the lepton number $L$ can be promoted to a local $U(1)_{B-L}$ symmetry since the corresponding gauge anomalies can be canceled by the right-handed neutrinos. Furthermore, the extremely small neutrino mass can be explained naturally if it is originated from the quantum correction. In this work, we propose simplest models of radiative Dirac neutrino mass using only $U(1)_{B-L}$ symmetry, and without introducing additional fermions and without imposing ad hoc symmetries. In this simple framework, we provide minimal models where Dirac neutrino mass appears at the (i) one-loop, (ii) two-loop and (iii) three-loop. By performing systematic analysis, we show that the minimal one-loop model requires three beyond SM scalar multiplets, whereas minimal two-loop and three-loop models require five. The presented two-loop and three-loop Dirac mass models have not appeared in the literature before." @default.
• W2916877376 created "2019-03-02" @default.
• W2916877376 creator A5015893170 @default.
• W2916877376 date "2019-06-01" @default.
• W2916877376 modified "2023-09-23" @default.
• W2916877376 title "Simplest radiative Dirac neutrino mass models" @default.
• W2916877376 cites W138462411 @default.
• W2916877376 cites W1611449462 @default.
• W2916877376 cites W1981218510 @default.
• W2916877376 cites W1995630875 @default.
• W2916877376 cites W1998573234 @default.
• W2916877376 cites W2000582865 @default.
• W2916877376 cites W2003170066 @default.
• W2916877376 cites W2003267894 @default.
• W2916877376 cites W2004000772 @default.
• W2916877376 cites W2012433125 @default.
• W2916877376 cites W2019019240 @default.
• W2916877376 cites W2019168416 @default.
• W2916877376 cites W2020963300 @default.
• W2916877376 cites W2022897627 @default.
• W2916877376 cites W2025747162 @default.
• W2916877376 cites W2042310721 @default.
• W2916877376 cites W2050261279 @default.
• W2916877376 cites W2050974769 @default.
• W2916877376 cites W2056119205 @default.
• W2916877376 cites W2067093548 @default.
• W2916877376 cites W2071128122 @default.
• W2916877376 cites W2088974938 @default.
• W2916877376 cites W2092319475 @default.
• W2916877376 cites W2111341905 @default.
• W2916877376 cites W2111859199 @default.
• W2916877376 cites W2125275384 @default.
• W2916877376 cites W2135062364 @default.
• W2916877376 cites W2188479714 @default.
• W2916877376 cites W2266724558 @default.
• W2916877376 cites W2273722452 @default.
• W2916877376 cites W2339339703 @default.
• W2916877376 cites W2402291169 @default.
• W2916877376 cites W2433601883 @default.
• W2916877376 cites W2464141815 @default.
• W2916877376 cites W2486800585 @default.
• W2916877376 cites W2488978209 @default.
• W2916877376 cites W2507653005 @default.
• W2916877376 cites W2510146569 @default.
• W2916877376 cites W2512040915 @default.
• W2916877376 cites W2513100569 @default.
• W2916877376 cites W2520465081 @default.
• W2916877376 cites W2576641335 @default.
• W2916877376 cites W2593878375 @default.
• W2916877376 cites W2731276465 @default.
• W2916877376 cites W2742926602 @default.
• W2916877376 cites W2770992702 @default.
• W2916877376 cites W2777740696 @default.
• W2916877376 cites W2785733326 @default.
• W2916877376 cites W2795094497 @default.
• W2916877376 cites W2798378541 @default.
• W2916877376 cites W2799604280 @default.
• W2916877376 cites W3023303758 @default.
• W2916877376 cites W3099252969 @default.
• W2916877376 cites W3100366459 @default.
• W2916877376 cites W3104547758 @default.
• W2916877376 cites W3121808161 @default.
• W2916877376 cites W3124317300 @default.
• W2916877376 doi "https://doi.org/10.1016/j.nuclphysb.2019.114636" @default.
• W2916877376 hasPublicationYear "2019" @default.
• W2916877376 type Work @default.
• W2916877376 sameAs 2916877376 @default.
• W2916877376 citedByCount "28" @default.
• W2916877376 countsByYear W29168773762019 @default.
• W2916877376 countsByYear W29168773762020 @default.
• W2916877376 countsByYear W29168773762021 @default.
• W2916877376 countsByYear W29168773762022 @default.
• W2916877376 countsByYear W29168773762023 @default.
• W2916877376 crossrefType "journal-article" @default.
• W2916877376 hasAuthorship W2916877376A5015893170 @default.
• W2916877376 hasBestOaLocation W29168773761 @default.
• W2916877376 hasConcept C101454708 @default.
• W2916877376 hasConcept C108243489 @default.
• W2916877376 hasConcept C109214941 @default.
• W2916877376 hasConcept C121332964 @default.
• W2916877376 hasConcept C147120987 @default.
• W2916877376 hasConcept C166957645 @default.
• W2916877376 hasConcept C179203047 @default.
• W2916877376 hasConcept C186453547 @default.
• W2916877376 hasConcept C2524010 @default.
• W2916877376 hasConcept C2779886137 @default.
• W2916877376 hasConcept C33923547 @default.
• W2916877376 hasConcept C40976572 @default.
• W2916877376 hasConcept C52233224 @default.
• W2916877376 hasConcept C57691317 @default.
• W2916877376 hasConcept C61039578 @default.
• W2916877376 hasConcept C62520636 @default.
• W2916877376 hasConcept C79955541 @default.
• W2916877376 hasConcept C95457728 @default.
• W2916877376 hasConceptScore W2916877376C101454708 @default.
• W2916877376 hasConceptScore W2916877376C108243489 @default.
• W2916877376 hasConceptScore W2916877376C109214941 @default.
• W2916877376 hasConceptScore W2916877376C121332964 @default.

• next