Addendum to "Invisible Higgs decay width versus dark matter direct detection cross section in Higgs portal dark matter models"

preprint2022arXivOpen access

Abstract

This article is an addendum to Ref.~\cite{Baek:2014jga}. Here, we discuss the invisible Higgs decay width ΓhinvΓ_{h}^{\rm inv} in the Higgs portal vector dark matter (VDM) model in the limit mV→0+m_V \rightarrow 0^+. In the effective field theory (EFT) approach where the VDM mass is attributed to the Stückelberg mechanism, (Γhinv)EFT( Γ_{h}^{\rm inv} )_{\rm EFT} is divergent, which is unphysical and puzzling. On the other hand (Γhinv)UV( Γ_{h}^{\rm inv} )_{\rm UV} becomes finite in a UV completion, where the VDM mass is generated by the dark Higgs mechanism. Then we can take the limit mV→0+m_V \rightarrow 0^+ by taking either {\it (i)} the dark gauge coupling gX→0+g_X \rightarrow 0^+ with a fixed dark Higgs vacuum expectation value vΦv_Φ, or {\it (ii)} vΦ→0+v_Φ\to 0^+ with a fixed gXg_X. Such a difference in the behavior of ΓhinvΓ_{h}^{\rm inv} in the massless VDM limit demonstrates another limitation of EFT for the Higgs portal VDM, and the importance of gauge-invariant and renormalizable models for the Higgs portal VDM.

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