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Observing an invisible Higgs boson
High Energy Physics - Phenomenology · Submitted 13 Sep 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Distinctive kinematic distributions of the two quark jets of the signal as compared to Zjj and Wjj backgrounds allow to restrict the Higgs branching ratio to 'invisible' final states to some 13% with 10fb^{-1} of data, provided events with two energetic forward jets of high dijet invariant mass and with substantial missing transverse momentum can be triggered efficiently.
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The abstract, sentence by sentence
Given its weak coupling to bottom quarks and tau leptons, the Higgs boson may predominantly decay into invisible particles like gravitinos, neutralinos, or gravitons. We consider the manifestation of such an invisibly decaying Higgs boson in weak boson fusion at the CERN LHC. Distinctive kinematic distributions of the two quark jets of the signal as compared to Zjj and Wjj backgrounds allow to restrict the Higgs branching ratio to 'invisible' final states to some 13% with 10fb^{-1} of data, provided events with two energetic forward jets of high dijet invariant mass and with substantial missing transverse momentum can be triggered efficiently. It is also possible to discover these particles with masses up to 480 GeV in weak boson fusion, at the 5 sigma level, provided their invisible branching ratio is close to 100%.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Given its weak coupling to bottom quarks and tau leptons, the Higgs boson may predominantly decay into invisible particles like gravitinos, neutralinos, or gravitons. | background 1.00 | 0.05 | 0.04 | hedged possibility 1.00 |
| s1 | We consider the manifestation of such an invisibly decaying Higgs boson in weak boson fusion at the CERN LHC. | contribution 0.96 | 0.48 | 0.05 | unclear 0.54 |
| s2 | Distinctive kinematic distributions of the two quark jets of the signal as compared to Zjj and Wjj backgrounds allow to restrict the Higgs branching ratio to 'invisible' final states to some 13% with 10fb^{-1} of data, provided events with two energetic forward jets of high dijet invariant mass and with substantial missing transverse momentum can be triggered efficiently. | result 0.98 | 0.59 | 0.58 | asserted 0.52 |
| s3 | It is also possible to discover these particles with masses up to 480 GeV in weak boson fusion, at the 5 sigma level, provided their invisible branching ratio is close to 100%. | result 0.98 | 0.50 | 0.25 | hedged possibility 0.97 |
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The paper
Original abstract
Given its weak coupling to bottom quarks and tau leptons, the Higgs boson may predominantly decay into invisible particles like gravitinos, neutralinos, or gravitons. We consider the manifestation of such an invisibly decaying Higgs boson in weak boson fusion at the CERN LHC. Distinctive kinematic distributions of the two quark jets of the signal as compared to Zjj and Wjj backgrounds allow to restrict the Higgs branching ratio to 'invisible' final states to some 13% with 10fb^{-1} of data, provided events with two energetic forward jets of high dijet invariant mass and with substantial missing transverse momentum can be triggered efficiently. It is also possible to discover these particles with masses up to 480 GeV in weak boson fusion, at the 5 sigma level, provided their invisible branching ratio is close to 100%.
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References
How later papers used it
67 later papers cite it
2 later papers by other authors are listed below: 2 used its method or tool. 1 more paper by the same authors is listed: 1 used its method or tool.
Uses its method or tool 3 of 6 papers with this label · 1 by the same authors
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Applied the box cuts, a central jet veto, and the cut on the azimuthal tagging jet correlation to reproduce this paper's original analysis.
Spying an invisible Higgs (2014) · 0.89 · paraphrased: the licence does not allow quoting
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Loosely followed the selection criteria discussed in this paper to select final states with two jets and large missing transverse energy and to use the VBF jet topology to discriminate the invisible Higgs signal from background.
Search for invisible decays of Higgs bosons in the vector boson fusion and associated ZH production modes (2014) · 0.84 · paraphrased: the licence does not allow quoting
By the same authors
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Followed this paper's procedure.
Graviton production with 2 jets at the LHC in large extra dimensions (2008) (same authors) · 1.00 · paraphrased: the licence does not allow quoting
How the literature uses it
59 arXiv papers cite this in 81 sentences
Papers citing it · 57 sentences without a confident label
Uses its method or tool 5 papers
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To reproduce the original analysis of Ref. [ref] we apply the box cuts given in Eq.[ref], add a central jet veto, and finally include the cut on the azimuthal tagging jet correlation in Eq.[ref].
Spying an invisible Higgs · LHC Reach · 0.89
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The translation of the result into a weak interacting massive particle–nucleon scattering cross section relies on an effective field theory approach [ref] under the assumption that invisible Higgs decays to a pair of WIMPs are kinematically possible and that the WIMP is a scalar or a fermion [ref] , using the nuclear form factor $f_N=0.308±0.018$ [ref] .
Combination of searches for invisible Higgs boson decays with the ATLAS experiment · Introduction · 0.88
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Here we follow the procedure of Ref. [ref] .
Graviton production with 2 jets at the LHC in large extra dimensions · Calculations · 1.00
Uses its data or values 2 papers
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From the original analysis of the LHC sensitivity to an invisible Higgs [ref] we quote the cut values with the exception of a the maximum jet rapidity,
Spying an invisible Higgs · Signal kinematics · 0.96
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The LHC can “observe” invisible Higgs decays, but only for much larger branching fractions of roughly $13%$ ($5%$) for $10 fb^-1$ ($100 fb^-1$) of data [ref] .
Neutrino Mass and $\mu \rightarrow e + \gamma $ from a Mini-Seesaw · Hidden Higgs Decays · 0.91
Compares with it 1 paper
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Nevertheless, our signal and background rates after the box cuts are consistent with the original work [ref] .
Spying an invisible Higgs · LHC Reach · 0.99
Cites it as support 1 paper
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The WBF production process is the best way to search for invisible SM-like Higgs decays at the LHC [ref] .
Higgs Physics: It ain't over till it's over · LHC Analyses · 0.97
Cites it as background 15 papers
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For these proposals, there exist numerous phenomenological and experimental researches in search for the invisible Higgs decays, via the production channels, including VH [ref] [ref] , $tt̅H$ [ref] [ref] [ref] , ggH (monojet) [ref] [ref] , and VBF [ref] [ref] [ref] which has been presented the most sensitive limits on the invisible Higgs decay BR at the LHC.
Boosting Invisible Higgs Searches by Tagging a Gluon Jet for Gluon Fusion Process · Invisible Decay of Higgs · 0.83
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Another interesting avenue to explore is whether the Higgs boson, the last piece of the SM discovered by the ATLAS and CMS Collaborations in 2012 [ref] , can act as a portal between DM and the SM via either Yukawa-type couplings or other mechanisms [ref] .
Exploration at the high-energy frontier: ATLAS Run~2 searches investigating the exotic jungle beyond the Standard Model · Higgs portal · 0.93
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The feasibility of determining an invisible branching fraction of the Higgs for $√(s)=$ 7 TeV,8 TeV and 14 TeV at the LHC has been studied in various production modes of the Higgs [ref] which is described very briefly in the next section.
Looking for an Invisible Higgs Signal at the LHC · Introduction · 0.83
Discussion
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