Publication

Searches for heavy Higgs bosons in two-Higgs-doublet models and for $t→ch$ decay using multilepton and diphoton final states in $pp$ collisions at 8 TeV

Abstract

Searches are presented for heavy scalar (H\mathrm{H}) and pseudoscalar (A\mathrm{A}) Higgs bosons posited in the two doublet model (2HDM) extensions of the standard model (SM). These searches are based on a data sample of pp\mathrm{p}\mathrm{p} collisions collected with the CMS experiment at the LHC at a center-of-mass energy of s=8 TeV\sqrt{s} = 8~\mathrm{TeV} and corresponding to an integrated luminosity of 19.5 fb119.5~\mathrm{fb}^{-1}. The decays Hhh\mathrm{H} \rightarrow \mathrm{h} \mathrm{h} and AZh\mathrm{A} \rightarrow \mathrm{Z} \mathrm{h}, where h\mathrm{h} denotes an SM-like Higgs boson, lead to events with three or more isolated charged leptons or with a photon pair accompanied by one or more isolated leptons. The search results are presented in terms of the H\mathrm{H} and A\mathrm{A} production cross sections times branching fractions and are further interpreted in terms of 2HDM parameters. We place 95% CL cross section upper limits of approximately 7 pb7~\mathrm{pb} on σB\sigma \mathcal{B} for Hhh\mathrm{H} \rightarrow \mathrm{h} \mathrm{h} and 2 pb2~\mathrm{pb} for AZh\mathrm{A} \rightarrow \mathrm{Z} \mathrm{h}. Also presented are the results of a search for the rare decay of the top quark that results in a charm quark and an SM Higgs boson, tch\mathrm{t} \rightarrow \mathrm{c} \mathrm{h}, the existence of which would indicate a nonzero flavor-changing Yukawa coupling of the top quark to the Higgs boson. We place a 95% CL upper limit of 0.56% on B(tch)\mathcal{B}(\mathrm{t} \rightarrow \mathrm{c} \mathrm{h}).

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Related concepts (33)
Higgs boson
The Higgs boson, sometimes called the Higgs particle, is an elementary particle in the Standard Model of particle physics produced by the quantum excitation of the Higgs field, one of the fields in particle physics theory. In the Standard Model, the Higgs particle is a massive scalar boson with zero spin, even (positive) parity, no electric charge, and no colour charge that couples to (interacts with) mass. It is also very unstable, decaying into other particles almost immediately upon generation.
Quark
A quark (kwɔːrk,_kwɑːrk) is a type of elementary particle and a fundamental constituent of matter. Quarks combine to form composite particles called hadrons, the most stable of which are protons and neutrons, the components of atomic nuclei. All commonly observable matter is composed of up quarks, down quarks and electrons. Owing to a phenomenon known as color confinement, quarks are never found in isolation; they can be found only within hadrons, which include baryons (such as protons and neutrons) and mesons, or in quark–gluon plasmas.
Top quark
The top quark, sometimes also referred to as the truth quark, (symbol: t) is the most massive of all observed elementary particles. It derives its mass from its coupling to the Higgs Boson. This coupling is very close to unity; in the Standard Model of particle physics, it is the largest (strongest) coupling at the scale of the weak interactions and above. The top quark was discovered in 1995 by the CDF and DØ experiments at Fermilab.
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