Discovery prospects for the 150 GeV charged scalar at future $$e^+e^-$$ colliders

Abstract

The Real Higgs Triplet model, known as the

SM, is a minimal extension of the Standard Model (SM) obtained by adding a hypercharge 0 triplet (

$$\varDelta $$ Δ

). This simple model is motivated by the multi-lepton anomalies and excesses in di-photon,

$$Z\gamma $$ Z γ

, and WW spectra at

$$\approx 152$$ ≈ 152

 GeV. The model contains, in addition to the SM particle content, a CP -even neutral Higgs (

$$\varDelta ^0$$ Δ 0

) and a charged state (

$$\varDelta ^\pm $$ Δ ±

), which are quasi-degenerate in mass. Observing the charged scalar at the LHC and measuring its mass is very challenging, since it dominantly decays to WZ , tb , and

$$\tau \nu $$ τ ν

. In this article, we consider the discovery prospects of the charged Higgs with mass 150 GeV at future electron-positron colliders. Taking into account

$$e^+e^- \rightarrow \gamma ^*,Z^* \rightarrow \varDelta ^\pm \varDelta ^\mp $$ e + e - → γ ∗ , Z ∗ → Δ ± Δ ∓

as the production mechanism and the dominant decay modes, we define three signal regions (SR) to study the 150 GeV charged Higgs properties: SR1:

$$\ge 3j + 1\ell $$ ≥ 3 j + 1 ℓ

, SR2:

$$\ge 3\ell + \tau _{\text {had}}$$ ≥ 3 ℓ + τ had

, SR3:

$$\ge 4j + \tau _{\text {had}}$$ ≥ 4 j + τ had

. For

$$m_{\varDelta ^\pm }=150\,\text {GeV}$$ m Δ ± = 150 GeV

, a

$$5\sigma $$ 5 σ

significance can be achieved in SR1 with an integrated luminosity of less than

$$1\text {~fb}^{-1}$$ 1 fb - 1

. SR2 is very clean with leptonic final states having low background and small systematic uncertainties. Furthermore, SR3 is crucial for reconstructing the charged scalar invariant mass, which can be measured with

$$\mathcal {O}(1)$$ O ( 1 )

 GeV accuracy with an integrated luminosity of

$$500\text {~fb}^{-1}$$ 500 fb - 1

.