Loading [MathJax]/jax/output/HTML-CSS/jax.js
CMS logoCMS event Hgg
Compact Muon Solenoid
LHC, CERN

CMS-HIG-14-025 ; CERN-PH-EP-2015-131
Search for exotic decays of a Higgs boson into undetectable particles and photons
Phys. Lett. B 753 (2016) 363
Abstract: A search is presented for exotic decays of a Higgs boson into undetectable particles and one or two isolated photons in pp collisions at a center-of-mass energy of 8 TeV. The data correspond to an integrated luminosity of up to 19.4 fb1 collected with the CMS detector at the LHC. Higgs bosons produced in gluon-gluon fusion and in association with a Z boson are investigated, using models in which the Higgs boson decays into a gravitino and a neutralino or a pair of neutralinos, followed by the decay of the neutralino to a gravitino and a photon. The selected events are consistent with the background-only hypothesis, and limits are placed on the product of cross sections and branching fractions. Assuming a standard model Higgs boson production cross-section, a 95% confidence level upper limit is set on the branching fraction of a 125 GeV Higgs boson decaying into undetectable particles and one or two isolated photons as a function of the neutralino mass. For neutralino masses from 1 to 120 GeV an upper limit in the range of 7 to 13% is obtained. Further results are given as a function of the neutralino lifetime, and also for a range of Higgs boson masses.
Figures & Tables Summary Additional Figures CMS Publications
Figures

png pdf
Figure 1-a:
Feynman diagrams for the Hundetectable+γ final state produced via ggH (a) and ZH (b).

png pdf
Figure 1-b:
Feynman diagrams for the Hundetectable+γ final state produced via ggH (a) and ZH (b).

png pdf
Figure 2-a:
The mEmissTT and EmissT distributions for data, background estimates, and signal after the model-independent selection for the ggH channel. The bottom panels in each plot show the ratio of (databackground)/background and the gray band includes both the statistical and systematic uncertainties in the background prediction. The signal is shown for mH= 125 GeV and m˜χ01= 120 GeV.

png pdf
Figure 2-b:
The mEmissTT and EmissT distributions for data, background estimates, and signal after the model-independent selection for the ggH channel. The bottom panels in each plot show the ratio of (databackground)/background and the gray band includes both the statistical and systematic uncertainties in the background prediction. The signal is shown for mH= 125 GeV and m˜χ01= 120 GeV.

png pdf
Figure 3:
The expected and observed 95% CL upper limit on the product of cross section, acceptance, and efficiency (σ(ppγ+EmissT)Aϵ) for mEmissTT> 100 GeV, as function of the EmissT threshold for the ggH channel.

png pdf
Figure 4-a:
Distributions in signal where mH= 125 GeV and m˜χ01= 95 GeV, backgrounds and data for mEmissTT (a) and |ηγ| (b) after applying all requirements. The uncertainty band for the backgrounds includes both statistical and systematic uncertainties. The signal model assumes a SM ZH production rate for a Higgs boson with mH= 125 GeV and a 10% branching fraction.

png pdf
Figure 4-b:
Distributions in signal where mH= 125 GeV and m˜χ01= 95 GeV, backgrounds and data for mEmissTT (a) and |ηγ| (b) after applying all requirements. The uncertainty band for the backgrounds includes both statistical and systematic uncertainties. The signal model assumes a SM ZH production rate for a Higgs boson with mH= 125 GeV and a 10% branching fraction.

png pdf
Figure 5:
Expected and observed 95% CL upper limits on σB/σSM for mH= 125 GeV as a function of m˜χ01 assuming the SM Higgs boson cross sections, for the ZH and ggH channels and their combination, with BB(H˜χ01˜χ01)B(˜χ01˜G+γ)2 for m˜χ01<mH/2 and BB(H˜χ01˜G)B(˜χ01˜G+γ) for m˜χ01mH/2.

png pdf
Figure 6-a:
Expected and observed 95% CL upper limits on σggHB as a function of the Higgs boson mass with m˜χ01=mH 30 GeV in ggH channel (a) and in the ZH channel (b).

png pdf
Figure 6-b:
Expected and observed 95% CL upper limits on σggHB as a function of the Higgs boson mass with m˜χ01=mH 30 GeV in ggH channel (a) and in the ZH channel (b).

png pdf
Figure 7:
Expected and observed 95% CL upper limits on σHB as a function of cτ˜χ01 for mH= 125 GeV and m˜χ01= 95 GeV, where BB(H˜χ01˜G)B(˜χ01˜G+γ).
Tables

png pdf
Table 1:
Summary of ggH selection for both the quasi model-independent analysis and the analysis with the SUSY benchmark model with the cumulative efficiencies of the selection requirements relative to the preselection for Zγν¯νγ, γ+jet and for a signal in a SUSY benchmark model with ggH production of a Higgs boson with mass 125 GeV decaying into a neutralino of mass 120 GeV and a photon.

png pdf
Table 2:
Summary of ZH selection.

png pdf
Table 3:
Summary of all relative systematic uncertainties in percent for the signal and background estimates for the Higgs model (model-independent in parenthesis) selection in the ggH analysis.

png pdf
Table 4:
Summary of relative systematic uncertainties in percent for the signal and background estimates in the ZH analysis.

png pdf
Table 5:
Observed yields and background estimates at 8 TeV in the ggH channel after the model-independent selection. Statistical and systematic uncertainties are shown.

png pdf
Table 6:
Observed yields, background estimates, and signal predictions at 8 TeV in the ggH channel for different values of the m˜χ01 and for different cτ˜χ01 of the ˜χ01. These correspond to B(Hundetectable+γ)=100%, assuming the SM cross section at the given mH hypothesis. Statistical and systematic uncertainties are shown for the yields.

png pdf
Table 7:
Observed yields, background estimates, and signal predictions at 8 TeV in the ZH channel. The signal predictions correspond to B(Hundetectable+γ)= 100% assuming the SM ZH cross section at the given mH hypothesis. Statistical and systematic uncertainties are shown.
Summary
A search is presented for exotic decays of a Higgs boson into undetectable particles and one or two isolated photons in pp collisions at a center-of-mass energy of 8 TeV. The data correspond to an integrated luminosity of up to 19.4 fb1 collected with the CMS detector at the LHC. Higgs bosons produced in gluon-gluon fusion or in association with a Z boson are investigated. Models including Higgs boson decays into a gravitino and a neutralino or a pair of neutralinos, followed by the neutralino decay to a gravitino and a photon, are tested. The measurements for the selected events in data are consistent with the background only hypothesis, and the results are interpreted as limits on the product of cross sections and branching fractions. Assuming a standard model Higgs production cross-section, a 95% CL upper limit is set on the branching fraction of a 125 GeV Higgs boson decaying into undetectable particles and one or two isolated photons as a function of the neutralino mass. For neutralino masses from 1 to 120 GeV an upper limit in the range of 7 to 13% is obtained. Further results are given as a function of the neutralino lifetime, and also for a range of Higgs boson masses.
Additional Figures

png pdf
Additional Figure 1-a:
Highest photon transverse energy candidate event for the model independent selection. Only tracks with minimum energy of 2 GeV and jets with minimum transverse momenta of 30 GeV are shown. Photon transverse energy: 1623 GeV; MET = 1671 GeV. a: ρ-ϕ view; b: 3D tower view.

png pdf
Additional Figure 1-b:
Highest photon transverse energy candidate event for the model independent selection. Only tracks with minimum energy of 2 GeV and jets with minimum transverse momenta of 30 GeV are shown. Photon transverse energy: 1623 GeV; MET = 1671 GeV. a: ρ-ϕ view; b: 3D tower view.

png pdf
Additional Figure 2-a:
Highest photon transverse energy candidate event for the SUSY benchmark model selection. Although this event has a track pointing to the electromagnetic cluster, it passes all photon identification selection criteria. A possible background interpretation is that this is likely a W+1 jet event. Only tracks with minimum energy of 2 GeV and jets with minimum transverse momenta of 30 GeV are shown. Photon transverse energy: 60 GeV; MET = 57 GeV. a: ρ-ϕ view; b: 3D tower view.

png pdf
Additional Figure 2-b:
Highest photon transverse energy candidate event for the SUSY benchmark model selection. Although this event has a track pointing to the electromagnetic cluster, it passes all photon identification selection criteria. A possible background interpretation is that this is likely a W+1 jet event. Only tracks with minimum energy of 2 GeV and jets with minimum transverse momenta of 30 GeV are shown. Photon transverse energy: 60 GeV; MET = 57 GeV. a: ρ-ϕ view; b: 3D tower view.

png pdf
Additional Figure 3-a:
Z(μμ) H(γ+MET) candidate: two high transverse momentum and isolated muons recoiling against MET and an isolated photon. a: ρ-ϕ view; b: 3D tower view.

png pdf
Additional Figure 3-b:
Z(μμ) H(γ+MET) candidate: two high transverse momentum and isolated muons recoiling against MET and an isolated photon. a: ρ-ϕ view; b: 3D tower view.
Compact Muon Solenoid
LHC, CERN