Matches in SemOpenAlex for { <https://semopenalex.org/work/W2952906481> ?p ?o ?g. }
- W2952906481 endingPage "134953" @default.
- W2952906481 startingPage "134953" @default.
- W2952906481 abstract "Multi-top quark production is a staple program at the LHC. Single-top and tt¯ productions are studied extensively, while current efforts are zooming in on four-top search, where the Standard Model (SM) cross section is at O(10) fb. In contrast, only at the fb level in SM, triple-top production has not been targeted for study so far. But such a small cross section makes it a unique probe for New Physics. Without the usual discrete Z2 symmetry, the general two Higgs doublet model (g2HDM) can naturally raise the triple-top production to pb level. We illustrate how certain signal regions of four-top search can be utilized to constrain triple-top production, but urge a dedicated search. As an aside, we note that the CMS study at 13 TeV of scalar tt¯ resonance interfering with QCD production background indicate some activity at 400 GeV. We comment that this could be explained in principle in g2HDM via the extra top Yukawa coupling." @default.
- W2952906481 created "2019-06-27" @default.
- W2952906481 creator A5044774783 @default.
- W2952906481 creator A5061590059 @default.
- W2952906481 creator A5072011448 @default.
- W2952906481 date "2019-11-01" @default.
- W2952906481 modified "2023-10-14" @default.
- W2952906481 title "Implications of four-top and top-pair studies on triple-top production" @default.
- W2952906481 cites W1959811897 @default.
- W2952906481 cites W2016818241 @default.
- W2952906481 cites W2041988351 @default.
- W2952906481 cites W2054655081 @default.
- W2952906481 cites W2062437705 @default.
- W2952906481 cites W2111808546 @default.
- W2952906481 cites W2118199673 @default.
- W2952906481 cites W2125102738 @default.
- W2952906481 cites W2137640558 @default.
- W2952906481 cites W2156379501 @default.
- W2952906481 cites W2159449603 @default.
- W2952906481 cites W2185981987 @default.
- W2952906481 cites W2257687385 @default.
- W2952906481 cites W2269845032 @default.
- W2952906481 cites W2746294272 @default.
- W2952906481 cites W2766934496 @default.
- W2952906481 cites W2767188499 @default.
- W2952906481 cites W2771179919 @default.
- W2952906481 cites W2798177768 @default.
- W2952906481 cites W2885235876 @default.
- W2952906481 cites W2899140785 @default.
- W2952906481 cites W2906894445 @default.
- W2952906481 cites W2923724224 @default.
- W2952906481 cites W3121642222 @default.
- W2952906481 doi "https://doi.org/10.1016/j.physletb.2019.134953" @default.
- W2952906481 hasPublicationYear "2019" @default.
- W2952906481 type Work @default.
- W2952906481 sameAs 2952906481 @default.
- W2952906481 citedByCount "19" @default.
- W2952906481 countsByYear W29529064812020 @default.
- W2952906481 countsByYear W29529064812021 @default.
- W2952906481 countsByYear W29529064812022 @default.
- W2952906481 countsByYear W29529064812023 @default.
- W2952906481 crossrefType "journal-article" @default.
- W2952906481 hasAuthorship W2952906481A5044774783 @default.
- W2952906481 hasAuthorship W2952906481A5061590059 @default.
- W2952906481 hasAuthorship W2952906481A5072011448 @default.
- W2952906481 hasBestOaLocation W29529064811 @default.
- W2952906481 hasConcept C101454708 @default.
- W2952906481 hasConcept C109214941 @default.
- W2952906481 hasConcept C117137515 @default.
- W2952906481 hasConcept C121332964 @default.
- W2952906481 hasConcept C139719470 @default.
- W2952906481 hasConcept C151195881 @default.
- W2952906481 hasConcept C158129726 @default.
- W2952906481 hasConcept C162324750 @default.
- W2952906481 hasConcept C166957645 @default.
- W2952906481 hasConcept C184748400 @default.
- W2952906481 hasConcept C185544564 @default.
- W2952906481 hasConcept C207206121 @default.
- W2952906481 hasConcept C2524010 @default.
- W2952906481 hasConcept C2778348673 @default.
- W2952906481 hasConcept C33923547 @default.
- W2952906481 hasConcept C40976572 @default.
- W2952906481 hasConcept C47085818 @default.
- W2952906481 hasConcept C57691317 @default.
- W2952906481 hasConcept C87668248 @default.
- W2952906481 hasConcept C95457728 @default.
- W2952906481 hasConceptScore W2952906481C101454708 @default.
- W2952906481 hasConceptScore W2952906481C109214941 @default.
- W2952906481 hasConceptScore W2952906481C117137515 @default.
- W2952906481 hasConceptScore W2952906481C121332964 @default.
- W2952906481 hasConceptScore W2952906481C139719470 @default.
- W2952906481 hasConceptScore W2952906481C151195881 @default.
- W2952906481 hasConceptScore W2952906481C158129726 @default.
- W2952906481 hasConceptScore W2952906481C162324750 @default.
- W2952906481 hasConceptScore W2952906481C166957645 @default.
- W2952906481 hasConceptScore W2952906481C184748400 @default.
- W2952906481 hasConceptScore W2952906481C185544564 @default.
- W2952906481 hasConceptScore W2952906481C207206121 @default.
- W2952906481 hasConceptScore W2952906481C2524010 @default.
- W2952906481 hasConceptScore W2952906481C2778348673 @default.
- W2952906481 hasConceptScore W2952906481C33923547 @default.
- W2952906481 hasConceptScore W2952906481C40976572 @default.
- W2952906481 hasConceptScore W2952906481C47085818 @default.
- W2952906481 hasConceptScore W2952906481C57691317 @default.
- W2952906481 hasConceptScore W2952906481C87668248 @default.
- W2952906481 hasConceptScore W2952906481C95457728 @default.
- W2952906481 hasFunder F4320322795 @default.
- W2952906481 hasLocation W29529064811 @default.
- W2952906481 hasLocation W29529064812 @default.
- W2952906481 hasLocation W29529064813 @default.
- W2952906481 hasLocation W29529064814 @default.
- W2952906481 hasOpenAccess W2952906481 @default.
- W2952906481 hasPrimaryLocation W29529064811 @default.
- W2952906481 hasRelatedWork W2039618455 @default.
- W2952906481 hasRelatedWork W2100513662 @default.
- W2952906481 hasRelatedWork W2120933240 @default.
- W2952906481 hasRelatedWork W2616179064 @default.
- W2952906481 hasRelatedWork W2787991305 @default.