Browsing by Subject "2HDM"
Results Per Page
Sort Options
-
Institution PublicationSearch for new particles in an extended Higgs sector with four b quarks in the final state at s=13TeV( 2022-12-10)
;Tumasyan A. ;Adam W. ;Andrejkovic J.W. ;Bergauer T. ;Chatterjee S. ;Damanakis K. ;Dragicevic M. ;Escalante Del Valle A. ;Frühwirth R. ;Jeitler M. ;Krammer N. ;Lechner L. ;Liko D. ;Mikulec I. ;Paulitsch P. ;Pitters F.M. ;Schieck J. ;Schöfbeck R. ;Schwarz D. ;Templ S. ;Waltenberger W. ;Wulz C.E. ;Chekhovsky V. ;Litomin A. ;Makarenko V. ;Darwish M.R. ;De Wolf E.A. ;Janssen T. ;Kello T. ;Lelek A. ;Rejeb Sfar H. ;Van Mechelen P. ;Van Putte S. ;Van Remortel N. ;Bols E.S. ;D'Hondt J. ;De Moor A. ;Delcourt M. ;El Faham H. ;Lowette S. ;Moortgat S. ;Morton A. ;Müller D. ;Sahasransu A.R. ;Tavernier S. ;Van Doninck W. ;Vannerom D. ;Beghin D. ;Bilin B. ;Clerbaux B. ;De Lentdecker G. ;Favart L. ;Kalsi A.K. ;Lee K. ;Lee K. ;Mahdavikhorrami M. ;Makarenko I. ;Moureaux L. ;Paredes S. ;Pétré L. ;Popov A. ;Postiau N. ;Starling E. ;Thomas L. ;Vanden Bemden M. ;Vander Velde C. ;Vanlaer P. ;Cornelis T. ;Dobur D. ;Knolle J. ;Lambrecht L. ;Mestdach G. ;Niedziela M. ;Rendón C. ;Roskas C. ;Samalan A. ;Skovpen K. ;Tytgat M. ;Vermassen B. ;Wezenbeek L. ;Benecke A. ;Bethani A. ;Bruno G. ;Bury F. ;Caputo C. ;David P. ;Delaere C. ;Donertas I.S. ;Giammanco A. ;Jaffel K. ;Jain S. ;Lemaitre V. ;Mondal K. ;Prisciandaro J. ;Taliercio A. ;Teklishyn M. ;Tran T.T. ;Vischia P. ;Wertz S. ;Alves G.A.Hensel C.A search for a massive resonance X decaying to a pair of spin-0 bosons ϕ that themselves decay to pairs of bottom quarks, is presented. The analysis is restricted to the mass ranges mϕ from 25 to 100 GeV and mX from 1 to 3 TeV. For these mass ranges, the decay products of each ϕ boson are expected to merge into a single large-radius jet. Jet substructure and flavor identification techniques are used to identify these jets. The search is based on CERN LHC proton-proton collision data at s=13TeV, collected with the CMS detector in 2016–2018, corresponding to an integrated luminosity of 138fb−1. Model-specific limits, where the two new particles arise from an extended Higgs sector, are set on the product of the production cross section and branching fraction for X→ϕϕ→(bb‾)(bb‾) as a function of the resonances' masses, where both the X→ϕϕ and ϕ→bb‾ branching fractions are assumed to be 100%. These limits are the first of their kind on this process, ranging between 30 and 1 fb at 95% confidence level for the considered mass ranges.