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

CMS-EXO-12-007 ; CERN-PH-EP-2015-119
Search for neutral color-octet weak-triplet scalar particles in proton-proton collisions at s= 8 TeV
J. High Energy Phys. 09 (2015) 201
Abstract: A search for pair production of neutral color-octet weak-triplet scalar particles (Θ0) is performed in processes where one Θ0 decays to a pair of b quark jets and the other to a Z boson plus a jet, with the Z boson decaying to a pair of electrons or muons. The search is performed with data collected by the CMS experiment at the CERN LHC corresponding to an integrated luminosity of 19.7 fb1 of proton-proton collisions at s= 8 TeV. The number of observed events is found to be in agreement with the standard model predictions. The 95% confidence level upper limit on the product of the cross section and branching fraction is obtained as a function of the Θ0 mass. The 95% confidence level lower bounds on the Θ0 mass are found to be 623 and 426 GeV, for two different octo-triplet theoretical scenarios. These are the first direct experimental bounds on particles predicted by the octo-triplet model.
Figures & Tables Summary CMS Publications
Figures

png pdf
Figure 3-a:
Distributions of Z+jet mass versus b jet pair mass for signal events with mG= 1100 GeV and mΘ0= 478 GeV (a) and background events (b), in the electron channel (distributions are similar in the muon channel). The open red rectangle on left indicates the signal region, as described in the text.

png pdf
Figure 3-b:
Distributions of Z+jet mass versus b jet pair mass for signal events with mG= 1100 GeV and mΘ0= 478 GeV (a) and background events (b), in the electron channel (distributions are similar in the muon channel). The open red rectangle on left indicates the signal region, as described in the text.

png pdf
Figure 4-a:
The Z+jet mass distribution in the Z+3jet (one b tag) control region after the appropriate correction factor has been applied, for the electron channel (a) and muon channel (b). The panels at the bottom show the ratio of data to background simulation, with the band representing the systematic uncertainty.

png pdf
Figure 4-b:
The Z+jet mass distribution in the Z+3jet (one b tag) control region after the appropriate correction factor has been applied, for the electron channel (a) and muon channel (b). The panels at the bottom show the ratio of data to background simulation, with the band representing the systematic uncertainty.

png pdf
Figure 5-a:
The Zeμ+jet (a) and b jet pair mass (b) distributions in the tˉt control region after the appropriate correction factor is applied. The panels at the bottom show the ratio of data to background simulation, with the band representing the systematic uncertainty.

png pdf
Figure 5-b:
The Zeμ+jet (a) and b jet pair mass (b) distributions in the tˉt control region after the appropriate correction factor is applied. The panels at the bottom show the ratio of data to background simulation, with the band representing the systematic uncertainty.

png pdf
Figure 6-a:
Distributions of the Z+jet mass versus b jet pair mass in data (a,b), and estimated background (c,d). The number of signal candidate events is counted in the rectangular boxes defined for each signal mass hypothesis, as discussed in Section "Selection".

png pdf
Figure 6-b:
Distributions of the Z+jet mass versus b jet pair mass in data (a,b), and estimated background (c,d). The number of signal candidate events is counted in the rectangular boxes defined for each signal mass hypothesis, as discussed in Section "Selection".

png pdf
Figure 6-c:
Distributions of the Z+jet mass versus b jet pair mass in data (a,b), and estimated background (c,d). The number of signal candidate events is counted in the rectangular boxes defined for each signal mass hypothesis, as discussed in Section "Selection".

png pdf
Figure 6-d:
Distributions of the Z+jet mass versus b jet pair mass in data (a,b), and estimated background (c,d). The number of signal candidate events is counted in the rectangular boxes defined for each signal mass hypothesis, as discussed in Section "Selection".

png pdf
Figure 7-a:
The b jet pair mass distributions for three different ranges of Z+jet mass in the electron channel (a) and the muon channel (b); Z+jet mass distributions for three different ranges of b jet pair mass in the electron channel (c) and the muon channel (d). The plotted regions correspond to three of the search regions. Predicted signal distributions are overlaid. The shaded band represents the statistical uncertainty combined with the systematic uncertainty in the simulated samples.

png pdf
Figure 7-b:
The b jet pair mass distributions for three different ranges of Z+jet mass in the electron channel (a) and the muon channel (b); Z+jet mass distributions for three different ranges of b jet pair mass in the electron channel (c) and the muon channel (d). The plotted regions correspond to three of the search regions. Predicted signal distributions are overlaid. The shaded band represents the statistical uncertainty combined with the systematic uncertainty in the simulated samples.

png pdf
Figure 7-c:
The b jet pair mass distributions for three different ranges of Z+jet mass in the electron channel (a) and the muon channel (b); Z+jet mass distributions for three different ranges of b jet pair mass in the electron channel (c) and the muon channel (d). The plotted regions correspond to three of the search regions. Predicted signal distributions are overlaid. The shaded band represents the statistical uncertainty combined with the systematic uncertainty in the simulated samples.

png pdf
Figure 7-d:
The b jet pair mass distributions for three different ranges of Z+jet mass in the electron channel (a) and the muon channel (b); Z+jet mass distributions for three different ranges of b jet pair mass in the electron channel (c) and the muon channel (d). The plotted regions correspond to three of the search regions. Predicted signal distributions are overlaid. The shaded band represents the statistical uncertainty combined with the systematic uncertainty in the simulated samples.

png pdf
Figure 8-a:
The 95% CL expected and observed upper limits on the cross section times branching fraction, σ×B(Θ0Zg)×B(Z)×B(Θ0b¯b)×2, as a function of Θ0 mass, for the case where mG=2.3mΘ0 (a) and mG=5mΘ0 (b) with the band on the color octet theoretical prediction indicating uncertainty in the signal yield due to PDF. These results assume B(Θ0b¯b) = 0.5 and B(Θ0Zg) + B(Θ0γg) = 0.5.

png pdf
Figure 8-b:
The 95% CL expected and observed upper limits on the cross section times branching fraction, σ×B(Θ0Zg)×B(Z)×B(Θ0b¯b)×2, as a function of Θ0 mass, for the case where mG=2.3mΘ0 (a) and mG=5mΘ0 (b) with the band on the color octet theoretical prediction indicating uncertainty in the signal yield due to PDF. These results assume B(Θ0b¯b) = 0.5 and B(Θ0Zg) + B(Θ0γg) = 0.5.
Tables

png pdf
Table 1:
Impact of systematic uncertainties on individual event yields. Ranges show the variation over the search regions that are considered. Dashes indicate cases where a systematic uncertainty is not applied. Sources appearing in more than one process are treated as correlated in the limit setting.

png pdf
Table 2:
The number of events after final selection for the signal, total background, and observed data, together with the statistical and systematic uncertainty. For the entries where a single uncertainty is shown, the statistical uncertainty is negligible.

png pdf
Table 3:
The number of background events, from all sources, after final selection, together with the statistical and systematic uncertainty. For the entries where a single uncertainty is shown, the systematic uncertainty is negligible.
Summary
A search for pair production of neutral color-octet weak-triplet scalar particles (Θ0) has been performed based on processes where one Θ0 decays to a pair of b quark jets and the other to a Z boson plus a jet, with the Z boson decaying to a pair of electrons or muons. This analysis is based on data collected with the CMS experiment in proton-proton collisions at s= 8 TeV, corresponding to an integrated luminosity of 19.7 fb1. The number of observed events is found to be in agreement with the standard model prediction. The CLs method is used to set a 95% confidence level limit on the cross section of octo-triplet particles, assuming B(Θ0bˉb)= 0.5, with the remaining Θ0 branching fraction shared between Zg and γg. By comparing the theoretical predictions of the octo-triplet model and the observed limits, masses of Θ0 below 623 GeV for mG=2.3mΘ0, and below 426 GeV for mG=5mΘ0, are excluded at 95% confidence level. These are the first direct experimental bounds on the Θ0 production model.
Compact Muon Solenoid
LHC, CERN