Abstract

A Higgs boson lighter than $2{m}_{W}$ that decays mostly into invisible channels (e.g., dark matter particles) is theoretically well-motivated. We study the prospects for discovery of such an invisible Higgs, ${h}_{\mathrm{inv}}$, at the LHC and the Tevatron in three production modes: (1) in association with a $Z$, (2) through weak boson fusion (WBF), and (3) accompanied by a jet. In the $Z+{h}_{\mathrm{inv}}$ channel, we show that the LHC can yield a discovery signal above $5\ensuremath{\sigma}$ with $10\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ of integrated luminosity for a Higgs mass of 120 GeV. With $30\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ the discovery reach extends up to a Higgs mass of 160 GeV. We also study the extraction of the ${h}_{\mathrm{inv}}$ mass from production cross sections at the LHC, and find that combining WBF and $Z+{h}_{\mathrm{inv}}$ allows a relatively model-independent determination of the ${h}_{\mathrm{inv}}$ mass with an uncertainty of 35--50 GeV (15--20 GeV) with $10\text{ }(100)\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$. At the Tevatron, a $3\ensuremath{\sigma}$ observation of a 120 GeV ${h}_{\mathrm{inv}}$ in any single channel is not possible with less than $12\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ per detector. However, we show that combining the signal from WBF with the previously studied $Z+{h}_{\mathrm{inv}}$ channel allows a $3\ensuremath{\sigma}$ observation of ${h}_{\mathrm{inv}}$ with $7\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ per detector. Because of overwhelming irreducible backgrounds, ${h}_{\mathrm{inv}}+j$ is not a useful search channel at either the Tevatron or the LHC, despite the larger production rate.

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