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CMS-PAS-EXO-16-019
Search for high-mass resonances in Zγe+eγ/μ+μγ final states in proton-proton collisions at s= 13 TeV
Abstract: A search for a heavy resonance decaying to Zγ, with the Z boson further decaying to pairs of electrons or muons is presented. The search makes use of 13 TeV proton-proton collision data collected by the CMS experiment at the LHC, corresponding to an integrated luminosity of 2.7 fb1. The analysis extracts the background directly from data, through an unbinned likelihood fit. No significant excess over the background-only hypothesis is observed, therefore limits at 95% confidence level are set on the production cross section of particles with a mass between 350 GeV and 2 TeV, with two different assumptions on the resonance width.
Figures Summary Additional Figures CMS Publications
Figures

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Figure 1:
Expected signal efficiency after full selections, as a function of the generated resonance mass, for the e+eγ (red) and μ+μγ (blue) channels in narrow-width signals.

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Figure 2-a:
Fits of the mZγ distribution in the data, for the e+eγ channel (a) and the μ+μγ channel (b). Data are shown as black markers, in bins of 20 GeV, and the fitted function is represented by a red line, with the 68% uncertainty band as gray shade.

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Figure 2-b:
Fits of the mZγ distribution in the data, for the e+eγ channel (a) and the μ+μγ channel (b). Data are shown as black markers, in bins of 20 GeV, and the fitted function is represented by a red line, with the 68% uncertainty band as gray shade.

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Figure 3-a:
Observed (solid) and expected (dashed) 95% C.L. exclusion limits on σ(AZγ+γ), as a function of signal mass, together with the 68% and 95% ranges of expectation in the background-only hypothesis, separately for the e+eγ (a) and μ+μγ (b) channels. The top row shows limits on a narrow width signal, the bottom row on a wide width signal.

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Figure 3-b:
Observed (solid) and expected (dashed) 95% C.L. exclusion limits on σ(AZγ+γ), as a function of signal mass, together with the 68% and 95% ranges of expectation in the background-only hypothesis, separately for the e+eγ (a) and μ+μγ (b) channels. The top row shows limits on a narrow width signal, the bottom row on a wide width signal.

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Figure 3-c:
Observed (solid) and expected (dashed) 95% C.L. exclusion limits on σ(AZγ+γ), as a function of signal mass, together with the 68% and 95% ranges of expectation in the background-only hypothesis, separately for the e+eγ (a) and μ+μγ (b) channels. The top row shows limits on a narrow width signal, the bottom row on a wide width signal.

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Figure 3-d:
Observed (solid) and expected (dashed) 95% C.L. exclusion limits on σ(AZγ+γ), as a function of signal mass, together with the 68% and 95% ranges of expectation in the background-only hypothesis, separately for the e+eγ (a) and μ+μγ (b) channels. The top row shows limits on a narrow width signal, the bottom row on a wide width signal.

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Figure 4-a:
Observed (solid) and expected(dashed) 95% C.L. exclusion limits on σ(AZγ) as a function of signal mass, together with the 68% (green) and 95% (yellow) ranges of expectation in the background-only hypothesis. The range 350 <mZγ< 2000 GeV is shown, for narrow width (a) and wide width signals (b).

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Figure 4-b:
Observed (solid) and expected(dashed) 95% C.L. exclusion limits on σ(AZγ) as a function of signal mass, together with the 68% (green) and 95% (yellow) ranges of expectation in the background-only hypothesis. The range 350 <mZγ< 2000 GeV is shown, for narrow width (a) and wide width signals (b).
Summary
A search for heavy resonances with mass between 350 GeV and 2 TeV decaying to Zγ, with further decay Z+, with =e, μ, has been presented. The search makes use of 13 TeV proton-proton collision data collected by the CMS experiment at the LHC, corresponding to an integrated luminosity of 2.7 fb1. The search strategy measures the non-resonant background directly on data, and looks for localized excesses. No significant excess over the Standard Model expectation is found, and limits at 95% confidence level are set on the production cross section of resonances for masses between 350 GeV and 2 TeV for two different hypothetical signal widths.
Additional Figures

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Additional Figure 1-a:
The invariant mass spectra of Z(e+e)γ events. The points with error bars represent the data. The stacked histograms represent the expectations from Zγ and Z+jets SM processes. The gray bands indicate the background uncertainty. The ratio of the data to the background prediction is shown at the bottom.

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Additional Figure 1-b:
The invariant mass spectra of Z(μ+μ)γ events. The points with error bars represent the data. The stacked histograms represent the expectations from Zγ and Z+jets SM processes. The gray bands indicate the background uncertainty. The ratio of the data to the background prediction is shown at the bottom.
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