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002727821 0247_ $$2DOI$$9bibmatch$$a10.1051/epjconf/202024506006
002727821 037__ $$9arXiv$$aarXiv:2007.11943$$chep-ph
002727821 037__ $$9arXiv:reportnumber$$aADP-20-18/T1128
002727821 035__ $$9arXiv$$aoai:arXiv.org:2007.11943
002727821 035__ $$9Inspire$$aoai:inspirehep.net:1808543$$d2021-02-04T08:03:53Z$$h2021-02-06T03:00:11Z$$mmarcxml$$ttrue$$uhttp://old.inspirehep.net/oai2d
002727821 035__ $$9Inspire$$a1808543
002727821 041__ $$aeng
002727821 100__ $$aCarragher, Ethan$$methan.carragher@adelaide.edu.au$$uAdelaide U.$$vDepartment of Physics, ARC Centre of Excellence for Particle Physics at the Terascale, University of Adelaide, Australia
002727821 245__ $$9arXiv$$aMinimal 4D Composite Higgs Models Under Current LHC Constraints
002727821 269__ $$c2020-07-23
002727821 260__ $$c2020
002727821 300__ $$a7 p
002727821 500__ $$9arXiv$$aAccepted for publication in CHEP 2019 proceedings
002727821 520__ $$9EDP Sciences$$aWe present preliminary results of the first convergent global fits of several minimal composite Higgs models. Our fits are performed using the differential evolution optimisation package Diver. A variety of physical constraints are taken into account, including a wide range of exclusion bounds on heavy resonance production from Run 2 of the LHC. As a by-product of the fits, we analyse the collider phenomenology of the lightest new up-type and downtype resonances in the viable regions of our models, finding some low-mass resonances that can be probed in future collider searches.
002727821 520__ $$9arXiv$$aWe present preliminary results of the first convergent global fits of several minimal composite Higgs models. Our fits are performed using the differential evolution optimisation package $\texttt{Diver}$. A variety of physical constraints are taken into account, including a wide range of exclusion bounds on heavy resonance production from Run 2 of the LHC. As a by-product of the fits, we analyse the collider phenomenology of the lightest new up-type and down-type resonances in the viable regions of our models, finding some low-mass resonances that can be probed in future collider searches.
002727821 540__ $$3preprint$$aCC0 1.0$$uhttp://creativecommons.org/publicdomain/zero/1.0/
002727821 540__ $$3publication$$aCC-BY-4.0$$bEDP Sciences$$uhttps://creativecommons.org/licenses/by/4.0/
002727821 542__ $$3publication$$f© The Authors
002727821 65017 $$2arXiv$$ahep-ph
002727821 65017 $$2SzGeCERN$$aParticle Physics - Phenomenology
002727821 690C_ $$aCERN
002727821 690C_ $$aARTICLE
002727821 693__ $$aCERN LHC
002727821 700__ $$aMurnane, Daniel$$mdaniel.murnane@adelaide.edu.au$$uAdelaide U.$$vDepartment of Physics, ARC Centre of Excellence for Particle Physics at the Terascale, University of Adelaide, Australia
002727821 700__ $$aStangl, Peter$$mpeter.stangl@lapth.cnrs.fr$$uAnnecy, LAPTH$$vLaboratoire d'Annecy-le-Vieux de Physique Théorique, UMR5108, CNRS, F-74941 Annecy-le-Vieux Cedex, France
002727821 700__ $$aSu, Wei$$mwei.su@adelaide.edu.au$$uAdelaide U.$$vDepartment of Physics, ARC Centre of Excellence for Particle Physics at the Terascale, University of Adelaide, Australia
002727821 700__ $$aWhite, Martin$$mmartin.white@adelaide.edu.au$$uAdelaide U.$$vDepartment of Physics, ARC Centre of Excellence for Particle Physics at the Terascale, University of Adelaide, Australia
002727821 700__ $$aWilliams, Anthony G.$$manthony.williams@adelaide.edu.au$$uAdelaide U.$$vDepartment of Physics, ARC Centre of Excellence for Particle Physics at the Terascale, University of Adelaide, Australia
002727821 773__ $$c06006$$pEPJ Web Conf.$$v245$$wC19-11-04$$y2020
002727821 8564_ $$82243254$$s25209$$uhttp://cds.cern.ch/record/2727821/files/plot_3G_14-14-10_NP50000_convthresh-5_mU_mD_like2D.png$$y00004 Profile likelihood ratios of the masses of the lightest up-type (U) and down-type (D) composite resonances in (a) the M4DCHM$^{5-5-5}$, (b) the M4DCHM$^{14-14-10}$, (c) the M4DCHM$^{14-1-10}$.
002727821 8564_ $$82243255$$s17370$$uhttp://cds.cern.ch/record/2727821/files/plot_3G_5-5-5_NP50000_convthresh-5_mU_mD_like2D.png$$y00003 Profile likelihood ratios of the masses of the lightest up-type (U) and down-type (D) composite resonances in (a) the M4DCHM$^{5-5-5}$, (b) the M4DCHM$^{14-14-10}$, (c) the M4DCHM$^{14-1-10}$.
002727821 8564_ $$82243256$$s200360$$uhttp://cds.cern.ch/record/2727821/files/U_multiple_14-14-10.png$$y00008 Cross sections for the pair-production of the lightest up-type (U) and down-type (D) resonances decaying into various final states at the $\sqrt{s}=13$~TeV LHC for viable points in (top) the M4DCHM$^{5-5-5}$, (middle) the M4DCHM$^{14-14-10}$, (bottom) the M4DCHM$^{14-1-10}$.
002727821 8564_ $$82243257$$s6464$$uhttp://cds.cern.ch/record/2727821/files/plot_3G_14-1-10_NP50000_convthresh-5_f_like1D.png$$y00002 Profile likelihood ratios of the Higgs decay constant $f$ in (a) the M4DCHM$^{5-5-5}$, (b) the M4DCHM$^{14-14-10}$, (c) the M4DCHM$^{14-1-10}$. For reference, the best-fit points found in these models have respective negative log likelihoods of $15.3$, $15.1$, and $15.4$.
002727821 8564_ $$82243258$$s22132$$uhttp://cds.cern.ch/record/2727821/files/plot_3G_14-1-10_NP50000_convthresh-5_mU_mD_like2D.png$$y00005 Profile likelihood ratios of the masses of the lightest up-type (U) and down-type (D) composite resonances in (a) the M4DCHM$^{5-5-5}$, (b) the M4DCHM$^{14-14-10}$, (c) the M4DCHM$^{14-1-10}$.
002727821 8564_ $$82243259$$s136913$$uhttp://cds.cern.ch/record/2727821/files/U_multiple_5-5-5.png$$y00006 Cross sections for the pair-production of the lightest up-type (U) and down-type (D) resonances decaying into various final states at the $\sqrt{s}=13$~TeV LHC for viable points in (top) the M4DCHM$^{5-5-5}$, (middle) the M4DCHM$^{14-14-10}$, (bottom) the M4DCHM$^{14-1-10}$.
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002727821 8564_ $$82243261$$s191648$$uhttp://cds.cern.ch/record/2727821/files/U_multiple_14-1-10.png$$y00010 Cross sections for the pair-production of the lightest up-type (U) and down-type (D) resonances decaying into various final states at the $\sqrt{s}=13$~TeV LHC for viable points in (top) the M4DCHM$^{5-5-5}$, (middle) the M4DCHM$^{14-14-10}$, (bottom) the M4DCHM$^{14-1-10}$.
002727821 8564_ $$82243262$$s143869$$uhttp://cds.cern.ch/record/2727821/files/D_multiple_14-1-10.png$$y00011 Cross sections for the pair-production of the lightest up-type (U) and down-type (D) resonances decaying into various final states at the $\sqrt{s}=13$~TeV LHC for viable points in (top) the M4DCHM$^{5-5-5}$, (middle) the M4DCHM$^{14-14-10}$, (bottom) the M4DCHM$^{14-1-10}$.
002727821 8564_ $$82243263$$s7738$$uhttp://cds.cern.ch/record/2727821/files/plot_3G_5-5-5_NP50000_convthresh-5_f_like1D.png$$y00000 Profile likelihood ratios of the Higgs decay constant $f$ in (a) the M4DCHM$^{5-5-5}$, (b) the M4DCHM$^{14-14-10}$, (c) the M4DCHM$^{14-1-10}$. For reference, the best-fit points found in these models have respective negative log likelihoods of $15.3$, $15.1$, and $15.4$.
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002727821 8564_ $$82243265$$s252994$$uhttp://cds.cern.ch/record/2727821/files/D_multiple_14-14-10.png$$y00009 Cross sections for the pair-production of the lightest up-type (U) and down-type (D) resonances decaying into various final states at the $\sqrt{s}=13$~TeV LHC for viable points in (top) the M4DCHM$^{5-5-5}$, (middle) the M4DCHM$^{14-14-10}$, (bottom) the M4DCHM$^{14-1-10}$.
002727821 8564_ $$82243266$$s129085$$uhttp://cds.cern.ch/record/2727821/files/D_multiple_5-5-5.png$$y00007 Cross sections for the pair-production of the lightest up-type (U) and down-type (D) resonances decaying into various final states at the $\sqrt{s}=13$~TeV LHC for viable points in (top) the M4DCHM$^{5-5-5}$, (middle) the M4DCHM$^{14-14-10}$, (bottom) the M4DCHM$^{14-1-10}$.
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