Exotic Higgs Decay via Charged Higgs

preprint2016arXivOpen access

Abstract

The most common search channel for heavy neutral Higgses in models with an extension of the Standard Model Higgs sector is A/H0→ττA/H^0\rightarrow ττ, which becomes ineffective when new decay modes of A/H0A/H^0 open. In this paper, we analyzed two such channels involving charged Higgses in the final states: A/H0→W±H∓A/H^0 \rightarrow W^\pm H^\mp and H0→H+H−H^0 \rightarrow H^+H^-. With the consequent decay of H±→τνH^\pm\rightarrow τν, we found that the limits for σ×BR(gg→A/H0→W±H∓)×BR(H±→τν)σ\times{BR}(gg \rightarrow A/H^0 \rightarrow W^\pm H^\mp)\times {BR}(H^\pm \rightarrow τν) vary from 30 to 10 fb for mA/H0m_{A/H^0} between 300 and 1000 GeV for 95% C.L. exclusion, and about 80 to 30 fb for 5σσ discovery. For H+H−H^+H^- mode, 95% C.L. limits on σ×BR(gg→H0→H+H−)×BR2(H±→τν)σ\times {BR}(gg\to H^0\to H^+ H^-)\times {BR}^2(H^\pm\to τν) vary from 9 to 4 fb for mH0m_{H^0} between 400 and 1000 GeV, while the 5σσ reach is about 20 to 10 fb. We further interpret the cross section limits in the Type II 2HDM parameter space. While A→W±H∓A\rightarrow W^\pm H^\mp offers great sensitivity in both sin⁡(β−α)\sin(β-α) versus tan⁡β\tanβ and mAm_A versus tan⁡β\tanβ parameter space, H0→H+H−H^0\rightarrow H^+ H^- can cover most of the parameter space for H0H^0. Reach in H0→W±H∓H^0\rightarrow W^\pm H^\mp is more limited, especially for mH0>2mH±m_{H^0}>2 m_{H^\pm}. It is, however, complementary to H0→H+H−H^0\rightarrow H^+ H^- when BR(H0→H+H−){BR}(H^0\rightarrow H^+ H^-) is accidentally suppressed.

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