Abstract
Many scenarios of physics beyond the Standard Model that address the hierarchy problem also predict the existence of vector-like top quark partners, which are generally expected around the TeV scale. In this paper, we propose to search for a vector-like top quark partner with charge $2/3$ in a simplified model including only two free parameters, the coupling constant $g^{\ast}$ and top quark partner mass $m_T$. We investigate the observability of the top quark partner through the process $pp \to T(\to th)j\to t(\to b W^+\to b \ell^{+} \nu_{\ell})h( \to WW^{\ast}\to \ell^{+}\nu\ell^{-}\bar{\nu}) j$, where $T$ is the heavy top quark partner and $h$ the SM-like Higgs boson, at the Large Hadron Collider (LHC). The discovery prospects and exclusion limits on the parameter plane defined by ($m_T,g^{\ast}$) are obtained for the already scheduled LHC runs as well as at the future High-Luminosity~LHC (HL-LHC). The constraints and projected sensitivities are also interpreted in a realistic model, i.e., the minimal Composite Higgs Model with singlet top quark partners. We finally also analyze the projected sensitivity in terms of the production cross section times branching fraction at the (HL-)LHC.
Highlights
To solve the gauge hierarchy problem, many extensions of the Standard Model (SM) predict top quark partners, which play an important role in canceling potentially large top quark loop corrections to the Higgs boson mass
Because our results are obtained from fixed branching ratio (BR) in a simplified model, while the latter for different decay channels can be altered in other models, in Fig. 8, we plot the HL-Large Hadron Collider (LHC) projected sensitivity in terms of the production cross section times BR [σT × BRðT → thÞ] as a function of the vectorlike top quark partner mass
We find that single-T production and decay rates such that σT × BRðT → thÞ ∼ 80–160 fb could be discovered at the High-Luminosity LHC (HL-LHC) for mT ∈ 1⁄21.0; 1.6 TeV, while the cross sections ∼37–74 fb will be excluded
Summary
To solve the gauge hierarchy problem, many extensions of the Standard Model (SM) predict top quark partners, which play an important role in canceling potentially large top quark loop corrections to the Higgs boson mass (for a review, see [1]). Vectorlike top quark partner T’s with the same color and electroweak (EW) quantum numbers as the top quark ones have been introduced in many new physics (NP) scenarios, such as little Higgs models [2], extra dimensions [3], twin Higgs models [4], and composite Higgs models (CHMs) [5] These new particles are at or just below the TeV scale and might generate characteristic signatures at current and future high energy colliders.
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