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Review Article

Looking for a hidden sector in exotic Higgs boson decays with the ATLAS experimentFootnote

| (Reviewing Editor)
Article: 1054679 | Received 13 Apr 2015, Accepted 14 May 2015, Published online: 24 Jun 2015

Figures & data

Figure 1. Distribution of the number of tracks (left) and the logarithmic ratio of the energy deposited in the hadronic and in the electromagnetic calorimeters (right). Notes: The dashed (dotted) histogram is for jets originating from πv decays in the hadronic calorimeter (inner detector). The filled histogram is for multi-jet data events used for estimating the background in the signal region.

Figure 1. Distribution of the number of tracks (left) and the logarithmic ratio of the energy deposited in the hadronic and in the electromagnetic calorimeters (right). Notes: The dashed (dotted) histogram is for jets originating from πv decays in the hadronic calorimeter (inner detector). The filled histogram is for multi-jet data events used for estimating the background in the signal region.

Figure 2. Observed 95% confidence level limits on the exotic Higgs decays to πv pairs. Note: The production cross-section is taken to be 19.0 pb.

Figure 2. Observed 95% confidence level limits on the exotic Higgs decays to πv pairs. Note: The production cross-section is taken to be 19.0 pb.

Figure 3. Schematic pictures of the lepton-jet classification according to the γd decay products. Notes: Three flavors are considered: lepton-jets formed of only muons (TYPE0), a mixed scenario with both muons and a jet (TYPE1), or only a jet (TYPE2).

Figure 3. Schematic pictures of the lepton-jet classification according to the γd decay products. Notes: Three flavors are considered: lepton-jets formed of only muons (TYPE0), a mixed scenario with both muons and a jet (TYPE1), or only a jet (TYPE2).

Figure 4. Parameter space exclusion plot for dark photons as a function of the kinetic mixing parameter ϵ and of the mass. Notes: Shown are existing 90% CL exclusion regions from beam-dump or fixed-target experiments, as well as low-energy electron colliders, astrophysical observations, and data on the anomalous magnetic moments of the electron and the muon. The plot includes the ATLAS exclusion limit in a previously unexplored region, looking at Higgs boson decays to displaced lepton-jets. The NNLO gluon fusion Higgs production cross-section is used and decay branching ratios to dark photons of 5, 10, 20, and 40% are assumed.

Figure 4. Parameter space exclusion plot for dark photons as a function of the kinetic mixing parameter ϵ and of the mass. Notes: Shown are existing 90% CL exclusion regions from beam-dump or fixed-target experiments, as well as low-energy electron colliders, astrophysical observations, and data on the anomalous magnetic moments of the electron and the muon. The plot includes the ATLAS exclusion limit in a previously unexplored region, looking at Higgs boson decays to displaced lepton-jets. The NNLO gluon fusion Higgs production cross-section is used and decay branching ratios to dark photons of 5, 10, 20, and 40% are assumed.

Figure 5. Distribution of the missing transverse momentum for the events with the invariant mass of the dilepton system consistent with the leptons originating from a Z boson decay (left) and after the full selection (right).

Figure 5. Distribution of the missing transverse momentum for the events with the invariant mass of the dilepton system consistent with the leptons originating from a Z boson decay (left) and after the full selection (right).

Figure 6. Limits on the DM–nucleon scattering cross-section at 90% confidence level, extracted from the branching ration Hinv. limit in a Higgs portal scenario and compared to results from direct-search experiments. The results from the direct-search experiments do not depend on the assumptions of the Higgs portal scenario.

Figure 6. Limits on the DM–nucleon scattering cross-section at 90% confidence level, extracted from the branching ration H→inv. limit in a Higgs portal scenario and compared to results from direct-search experiments. The results from the direct-search experiments do not depend on the assumptions of the Higgs portal scenario.