Cross-section measurements of the Higgs boson decaying into a pair of $\tau$-leptons in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

A measurement of production cross sections of the Higgs boson in proton-proton collisions is presented in the $H\rightarrow\tau\tau$ decay channel. The analysis is performed using 36.1 fb$^{-1}$ of data recorded by the ATLAS experiment at the Large Hadron Collider at a center-of-mass energy of $\sqrt{s}=13$ TeV. All combinations of leptonic ($\tau \rightarrow l \nu \bar{\nu}$ with $l = e$, $\mu$) and hadronic ($\tau \to$ hadrons $\nu$) tau decays are considered. The $H\rightarrow\tau\tau$ signal over the expected background from other Standard Model processes is established with an observed (expected) significance of 4.4 (4.1) standard deviations. Combined with results obtained using data taken at 7 and 8 TeV center-of-mass energies, the observed (expected) significance amounts to 6.4 (5.4) standard deviations and constitutes an observation of $H\rightarrow\tau\tau$ decays. Using the data taken at $\sqrt{s}=13$ TeV, the total cross section in the $H\rightarrow\tau\tau$ decay channel is measured to be $3.77^{+0.60}_{-0.59}\mathrm{(stat.)}^{+0.87}_{-0.74}\mathrm{(syst.)}$ pb, for a Higgs boson of mass 125 GeV assuming the relative contributions of its production modes as predicted by the Standard Model. Total cross sections in the $H\rightarrow\tau\tau$ decay channel are determined separately for vector-boson-fusion production and gluon-gluon-fusion production to be $0.28 \pm 0.09\mathrm{(stat.)}^{+0.11}_{-0.09}\mathrm{(syst.)}$ pb and $3.1 \pm 1.0\mathrm{(stat.)}^{+1.6}_{-1.3}\mathrm{(syst.)}$ pb, respectively. Similarly, results of a fit are reported in the framework of simplified template cross sections. All measurements are in agreement with Standard Model expectations.

21 November 2018

Contact: Higgs conveners internal

Figures

Figure 01


Expected signal and background composition in 6 control regions (CRs) and the 13 signal regions (SRs) used in the analysis.

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Figure 02a


Comparisons between data and predictions as computed by the fit of (top) the pT of the Higgs-boson candidate (pTττ) in the boosted inclusive category and (bottom) the invariant mass of the two highest-pT jets (mjj) in the VBF inclusive category for (left) the τlepτlep channel, (center) the τlepτhad channel and (right) the τhadτhad channel. The ratios of the data to the background model are shown in the lower panels. The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 02b


Comparisons between data and predictions as computed by the fit of (top) the pT of the Higgs-boson candidate (pTττ) in the boosted inclusive category and (bottom) the invariant mass of the two highest-pT jets (mjj) in the VBF inclusive category for (left) the τlepτlep channel, (center) the τlepτhad channel and (right) the τhadτhad channel. The ratios of the data to the background model are shown in the lower panels. The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 02c


Comparisons between data and predictions as computed by the fit of (top) the pT of the Higgs-boson candidate (pTττ) in the boosted inclusive category and (bottom) the invariant mass of the two highest-pT jets (mjj) in the VBF inclusive category for (left) the τlepτlep channel, (center) the τlepτhad channel and (right) the τhadτhad channel. The ratios of the data to the background model are shown in the lower panels. The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 02d


Comparisons between data and predictions as computed by the fit of (top) the pT of the Higgs-boson candidate (pTττ) in the boosted inclusive category and (bottom) the invariant mass of the two highest-pT jets (mjj) in the VBF inclusive category for (left) the τlepτlep channel, (center) the τlepτhad channel and (right) the τhadτhad channel. The ratios of the data to the background model are shown in the lower panels. The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 02e


Comparisons between data and predictions as computed by the fit of (top) the pT of the Higgs-boson candidate (pTττ) in the boosted inclusive category and (bottom) the invariant mass of the two highest-pT jets (mjj) in the VBF inclusive category for (left) the τlepτlep channel, (center) the τlepτhad channel and (right) the τhadτhad channel. The ratios of the data to the background model are shown in the lower panels. The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 02f


Comparisons between data and predictions as computed by the fit of (top) the pT of the Higgs-boson candidate (pTττ) in the boosted inclusive category and (bottom) the invariant mass of the two highest-pT jets (mjj) in the VBF inclusive category for (left) the τlepτlep channel, (center) the τlepτhad channel and (right) the τhadτhad channel. The ratios of the data to the background model are shown in the lower panels. The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 03a


Observed and expected distributions in the Z→ττ validation regions (VRs) corresponding to (a)–(d) the τlepτhad VBF inclusive category and (e)–(i) the τlepτhad boosted inclusive category. Shown are, in the respective region: (a) the pseudorapidity separation (|Δηjj|) and (b) the invariant mass (mjj) of the two highest-pT jets; (c) and (e) the pT of the di-lepton system (pTll); (d) and (g) the pT of the highest-pT jet (pTj1); (f) the angular distance between the light leptons (Δ Rll); (h) the pT of the highest-pT light lepton (pTl1); and (i) the pT of the second-highest-pT light lepton (pTl2). The predictions in these validation regions are not computed by the fit, but are simply normalized to the event yield in data. The size of the combined statistical, experimental and theoretical uncertainties is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels together with the theoretical uncertainties in the Sherpa simulation of Z→ll, which are indicated by the blue lines.

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Figure 03b


Observed and expected distributions in the Z→ττ validation regions (VRs) corresponding to (a)–(d) the τlepτhad VBF inclusive category and (e)–(i) the τlepτhad boosted inclusive category. Shown are, in the respective region: (a) the pseudorapidity separation (|Δηjj|) and (b) the invariant mass (mjj) of the two highest-pT jets; (c) and (e) the pT of the di-lepton system (pTll); (d) and (g) the pT of the highest-pT jet (pTj1); (f) the angular distance between the light leptons (Δ Rll); (h) the pT of the highest-pT light lepton (pTl1); and (i) the pT of the second-highest-pT light lepton (pTl2). The predictions in these validation regions are not computed by the fit, but are simply normalized to the event yield in data. The size of the combined statistical, experimental and theoretical uncertainties is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels together with the theoretical uncertainties in the Sherpa simulation of Z→ll, which are indicated by the blue lines.

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Figure 03c


Observed and expected distributions in the Z→ττ validation regions (VRs) corresponding to (a)–(d) the τlepτhad VBF inclusive category and (e)–(i) the τlepτhad boosted inclusive category. Shown are, in the respective region: (a) the pseudorapidity separation (|Δηjj|) and (b) the invariant mass (mjj) of the two highest-pT jets; (c) and (e) the pT of the di-lepton system (pTll); (d) and (g) the pT of the highest-pT jet (pTj1); (f) the angular distance between the light leptons (Δ Rll); (h) the pT of the highest-pT light lepton (pTl1); and (i) the pT of the second-highest-pT light lepton (pTl2). The predictions in these validation regions are not computed by the fit, but are simply normalized to the event yield in data. The size of the combined statistical, experimental and theoretical uncertainties is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels together with the theoretical uncertainties in the Sherpa simulation of Z→ll, which are indicated by the blue lines.

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Figure 03d


Observed and expected distributions in the Z→ττ validation regions (VRs) corresponding to (a)–(d) the τlepτhad VBF inclusive category and (e)–(i) the τlepτhad boosted inclusive category. Shown are, in the respective region: (a) the pseudorapidity separation (|Δηjj|) and (b) the invariant mass (mjj) of the two highest-pT jets; (c) and (e) the pT of the di-lepton system (pTll); (d) and (g) the pT of the highest-pT jet (pTj1); (f) the angular distance between the light leptons (Δ Rll); (h) the pT of the highest-pT light lepton (pTl1); and (i) the pT of the second-highest-pT light lepton (pTl2). The predictions in these validation regions are not computed by the fit, but are simply normalized to the event yield in data. The size of the combined statistical, experimental and theoretical uncertainties is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels together with the theoretical uncertainties in the Sherpa simulation of Z→ll, which are indicated by the blue lines.

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Figure 03e


Observed and expected distributions in the Z→ττ validation regions (VRs) corresponding to (a)–(d) the τlepτhad VBF inclusive category and (e)–(i) the τlepτhad boosted inclusive category. Shown are, in the respective region: (a) the pseudorapidity separation (|Δηjj|) and (b) the invariant mass (mjj) of the two highest-pT jets; (c) and (e) the pT of the di-lepton system (pTll); (d) and (g) the pT of the highest-pT jet (pTj1); (f) the angular distance between the light leptons (Δ Rll); (h) the pT of the highest-pT light lepton (pTl1); and (i) the pT of the second-highest-pT light lepton (pTl2). The predictions in these validation regions are not computed by the fit, but are simply normalized to the event yield in data. The size of the combined statistical, experimental and theoretical uncertainties is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels together with the theoretical uncertainties in the Sherpa simulation of Z→ll, which are indicated by the blue lines.

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Figure 03f


Observed and expected distributions in the Z→ττ validation regions (VRs) corresponding to (a)–(d) the τlepτhad VBF inclusive category and (e)–(i) the τlepτhad boosted inclusive category. Shown are, in the respective region: (a) the pseudorapidity separation (|Δηjj|) and (b) the invariant mass (mjj) of the two highest-pT jets; (c) and (e) the pT of the di-lepton system (pTll); (d) and (g) the pT of the highest-pT jet (pTj1); (f) the angular distance between the light leptons (Δ Rll); (h) the pT of the highest-pT light lepton (pTl1); and (i) the pT of the second-highest-pT light lepton (pTl2). The predictions in these validation regions are not computed by the fit, but are simply normalized to the event yield in data. The size of the combined statistical, experimental and theoretical uncertainties is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels together with the theoretical uncertainties in the Sherpa simulation of Z→ll, which are indicated by the blue lines.

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Figure 03g


Observed and expected distributions in the Z→ττ validation regions (VRs) corresponding to (a)–(d) the τlepτhad VBF inclusive category and (e)–(i) the τlepτhad boosted inclusive category. Shown are, in the respective region: (a) the pseudorapidity separation (|Δηjj|) and (b) the invariant mass (mjj) of the two highest-pT jets; (c) and (e) the pT of the di-lepton system (pTll); (d) and (g) the pT of the highest-pT jet (pTj1); (f) the angular distance between the light leptons (Δ Rll); (h) the pT of the highest-pT light lepton (pTl1); and (i) the pT of the second-highest-pT light lepton (pTl2). The predictions in these validation regions are not computed by the fit, but are simply normalized to the event yield in data. The size of the combined statistical, experimental and theoretical uncertainties is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels together with the theoretical uncertainties in the Sherpa simulation of Z→ll, which are indicated by the blue lines.

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Figure 03h


Observed and expected distributions in the Z→ττ validation regions (VRs) corresponding to (a)–(d) the τlepτhad VBF inclusive category and (e)–(i) the τlepτhad boosted inclusive category. Shown are, in the respective region: (a) the pseudorapidity separation (|Δηjj|) and (b) the invariant mass (mjj) of the two highest-pT jets; (c) and (e) the pT of the di-lepton system (pTll); (d) and (g) the pT of the highest-pT jet (pTj1); (f) the angular distance between the light leptons (Δ Rll); (h) the pT of the highest-pT light lepton (pTl1); and (i) the pT of the second-highest-pT light lepton (pTl2). The predictions in these validation regions are not computed by the fit, but are simply normalized to the event yield in data. The size of the combined statistical, experimental and theoretical uncertainties is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels together with the theoretical uncertainties in the Sherpa simulation of Z→ll, which are indicated by the blue lines.

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Figure 03i


Observed and expected distributions in the Z→ττ validation regions (VRs) corresponding to (a)–(d) the τlepτhad VBF inclusive category and (e)–(i) the τlepτhad boosted inclusive category. Shown are, in the respective region: (a) the pseudorapidity separation (|Δηjj|) and (b) the invariant mass (mjj) of the two highest-pT jets; (c) and (e) the pT of the di-lepton system (pTll); (d) and (g) the pT of the highest-pT jet (pTj1); (f) the angular distance between the light leptons (Δ Rll); (h) the pT of the highest-pT light lepton (pTl1); and (i) the pT of the second-highest-pT light lepton (pTl2). The predictions in these validation regions are not computed by the fit, but are simply normalized to the event yield in data. The size of the combined statistical, experimental and theoretical uncertainties is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels together with the theoretical uncertainties in the Sherpa simulation of Z→ll, which are indicated by the blue lines.

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Figure 04a


For the control regions (CRs) defined in Section 5, comparisons between data and predictions as computed by the fit for the reconstructed di-τ invariant mass (mττMMC). Shown are (a) the τlepτlep VBF Z→ll control region (CR), (b) the τlepτlep boosted top CR and (c) the τlepτhad VBF top CR. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels.

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Figure 04b


For the control regions (CRs) defined in Section 5, comparisons between data and predictions as computed by the fit for the reconstructed di-τ invariant mass (mττMMC). Shown are (a) the τlepτlep VBF Z→ll control region (CR), (b) the τlepτlep boosted top CR and (c) the τlepτhad VBF top CR. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels.

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Figure 04c


For the control regions (CRs) defined in Section 5, comparisons between data and predictions as computed by the fit for the reconstructed di-τ invariant mass (mττMMC). Shown are (a) the τlepτlep VBF Z→ll control region (CR), (b) the τlepτlep boosted top CR and (c) the τlepτhad VBF top CR. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels.

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Figure 05a


Observed distributions and predictions computed by the fit for (a) mττMMC in the W-enhanced region of the τlepτhad boosted inclusive category, and (b) Δη between the two τhad-vis, for events in the boosted low-pTττ signal region (SR) of the τhadτhad channel. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels.

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Figure 05b


Observed distributions and predictions computed by the fit for (a) mττMMC in the W-enhanced region of the τlepτhad boosted inclusive category, and (b) Δη between the two τhad-vis, for events in the boosted low-pTττ signal region (SR) of the τhadτhad channel. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands. The ratios of the data to the background model are shown in the lower panels.

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Figure 06


Fractional impact of systematic uncertainties in σH→ττ as computed by the fit. The systematic uncertainties are listed in decreasing order of their impact on σH→ττ on the y-axis. The hatched blue and open blue boxes show the variations of σH→ττ referring to the top x-axis (impact), as described in the text. The filled circles, referring to the bottom x-axis, show the pulls of the fitted nuisance parameters, i.e. the deviations of the fitted parameters θ from their nominal values θ0, normalized to their nominal uncertainties Δθ. The black lines show the uncertainties of the nuisance parameters resulting from the fit. Several sources of uncertainties such as the jet energy scale and resolution as well as the b-mistag rate are described by their principal components in the fit. For the Z→ττ and Z→ll; normalization factors in the boosted category, the fitted values and the uncertainties resulting from the fit are shown, which excludes uncertainties in total simulated cross sections extrapolated to the selected phase space.

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Figure 07a


The measured values for σH→ττ when only the data of (a) individual channels or (b) individual categories are used. Also shown is the result from the combined fit. The total ±1σ uncertainty in the measurement is indicated by the black error bars, with the individual contribution from the statistical uncertainty in blue. The theory uncertainty in the predicted signal cross section is shown by the yellow band.

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Figure 07b


The measured values for σH→ττ when only the data of (a) individual channels or (b) individual categories are used. Also shown is the result from the combined fit. The total ±1σ uncertainty in the measurement is indicated by the black error bars, with the individual contribution from the statistical uncertainty in blue. The theory uncertainty in the predicted signal cross section is shown by the yellow band.

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Figure 08a


Distributions of the reconstructed di-τ invariant mass (mττMMC) for the sum of (left) all τlepτlep, (center) all τlepτhad and (right) all τhadτhad signal regions (SRs). The bottom panels show the differences between observed data events and expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 08b


Distributions of the reconstructed di-τ invariant mass (mττMMC) for the sum of (left) all τlepτlep, (center) all τlepτhad and (right) all τhadτhad signal regions (SRs). The bottom panels show the differences between observed data events and expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 08c


Distributions of the reconstructed di-τ invariant mass (mττMMC) for the sum of (left) all τlepτlep, (center) all τlepτhad and (right) all τhadτhad signal regions (SRs). The bottom panels show the differences between observed data events and expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 09a


Distribution of the reconstructed di-τ invariant mass (mττMMC) for the sum of (a) all VBF and (b) all boosted signal regions (SRs). The bottom panels show the differences between observed data events and expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 09b


Distribution of the reconstructed di-τ invariant mass (mττMMC) for the sum of (a) all VBF and (b) all boosted signal regions (SRs). The bottom panels show the differences between observed data events and expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 10


Distribution of the reconstructed di-τ invariant mass (mττMMC) for the sum of all signal regions (SRs). The contributions of the different SRs are weighted by a factor of ln(1+S/B), where S and B are the expected numbers of signal and background events in that region, respectively. The bottom panel shows the differences between observed data events and expected background events after applying the same weights (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 11


Likelihood contours for the combination of all channels in the (σH→ττggF, σH→ττVBF) plane. The 68% and 95% CL contours are shown as dashed and solid lines, respectively, for mH=125GeV. The SM expectation is indicated by a plus symbol and the best fit to the data is shown as a star.

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Figure 12a


Observed and expected mττMMC distributions as used in the fit in all signal regions (SRs) in the VBF category for the τlepτlep (left), τlepτhad (middle) and τhadτhad (right) analysis channels. The bottom panels show the ratio of observed data events to expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 12b


Observed and expected mττMMC distributions as used in the fit in all signal regions (SRs) in the VBF category for the τlepτlep (left), τlepτhad (middle) and τhadτhad (right) analysis channels. The bottom panels show the ratio of observed data events to expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 12c


Observed and expected mττMMC distributions as used in the fit in all signal regions (SRs) in the VBF category for the τlepτlep (left), τlepτhad (middle) and τhadτhad (right) analysis channels. The bottom panels show the ratio of observed data events to expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 12d


Observed and expected mττMMC distributions as used in the fit in all signal regions (SRs) in the VBF category for the τlepτlep (left), τlepτhad (middle) and τhadτhad (right) analysis channels. The bottom panels show the ratio of observed data events to expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 12e


Observed and expected mττMMC distributions as used in the fit in all signal regions (SRs) in the VBF category for the τlepτlep (left), τlepτhad (middle) and τhadτhad (right) analysis channels. The bottom panels show the ratio of observed data events to expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 12f


Observed and expected mττMMC distributions as used in the fit in all signal regions (SRs) in the VBF category for the τlepτlep (left), τlepτhad (middle) and τhadτhad (right) analysis channels. The bottom panels show the ratio of observed data events to expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

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Figure 12g


Observed and expected mττMMC distributions as used in the fit in all signal regions (SRs) in the VBF category for the τlepτlep (left), τlepτhad (middle) and τhadτhad (right) analysis channels. The bottom panels show the ratio of observed data events to expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

png (125kB)  pdf (17kB) 

Figure 13a


Observed and expected mττMMC distributions as used in the fit in all signal regions (SRs) in the boosted category for the τlepτlep (left), τlepτhad (middle) and τhadτhad (right) analysis channels. The bottom panels show the ratio of observed data events to expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

png (129kB)  pdf (18kB) 

Figure 13b


Observed and expected mττMMC distributions as used in the fit in all signal regions (SRs) in the boosted category for the τlepτlep (left), τlepτhad (middle) and τhadτhad (right) analysis channels. The bottom panels show the ratio of observed data events to expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

png (115kB)  pdf (17kB) 

Figure 13c


Observed and expected mττMMC distributions as used in the fit in all signal regions (SRs) in the boosted category for the τlepτlep (left), τlepτhad (middle) and τhadτhad (right) analysis channels. The bottom panels show the ratio of observed data events to expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

png (123kB)  pdf (18kB) 

Figure 13d


Observed and expected mττMMC distributions as used in the fit in all signal regions (SRs) in the boosted category for the τlepτlep (left), τlepτhad (middle) and τhadτhad (right) analysis channels. The bottom panels show the ratio of observed data events to expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

png (135kB)  pdf (18kB) 

Figure 13e


Observed and expected mττMMC distributions as used in the fit in all signal regions (SRs) in the boosted category for the τlepτlep (left), τlepτhad (middle) and τhadτhad (right) analysis channels. The bottom panels show the ratio of observed data events to expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

png (114kB)  pdf (17kB) 

Figure 13f


Observed and expected mττMMC distributions as used in the fit in all signal regions (SRs) in the boosted category for the τlepτlep (left), τlepτhad (middle) and τhadτhad (right) analysis channels. The bottom panels show the ratio of observed data events to expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

png (124kB)  pdf (18kB) 

Tables

Table 01


Monte Carlo generators used to describe all signal and background processes together with the corresponding PDF set and the model of parton showering, hadronization and underlying event (UEPS). In addition, the order of the total cross-section calculation is given. The total cross section for VBF production is calculated at approximate-NNLO QCD. More details are given in the text.

png (23kB)  pdf (67kB) 

Table 02


Summary of the triggers used to select events for the three analysis channels during 2015 and 2016 data-taking and the corresponding pT requirements applied in the analysis. For the electron+muon trigger the first number corresponds to the electron pT requirement, the second to the muon pT requirement. For the τhadτhad channel, at least one high-pT jet in addition to the two τhad-vis candidates is required for the 2016 dataset (see Section 5.1).

png (16kB)  pdf (35kB) 

Table 03


Summary of the event selection requirements for the three analysis channels that are applied in addition to the respective lepton pT requirements listed in Table 2. ETmiss, hard is an alternative ETmiss calculated only from the physics objects without the soft-track term. The transverse mass (mT) is calculated from ETmiss and the momentum of the selected light lepton. The visible momentum fractions x1 and x2 of the respective τ-lepton and the collinear di-τ mass (mττcoll) are calculated in the collinear approximation [98].

png (36kB)  pdf (73kB) 

Table 04


Definition of the VBF and boosted analysis categories and of their respective signal regions (SRs). The selection criteria, which are applied in addition to those described in Table 3, are listed for each channel. The VBF high-pTττ SR is only defined for the τhadτhad channel, resulting in a total of seven VBF SRs and six boosted SRs. All SRs are exclusive and their yields add up to those of the corresponding VBF and boosted inclusive regions.

png (33kB)  pdf (58kB) 

Table 05


Definitions of the six control regions (CRs) used to constrain the Z→ll and top backgrounds to the event yield in data in the τlepτlep and τlepτhad channels. SF denotes a selection of same-flavor light leptons.

png (24kB)  pdf (53kB) 

Table 06


Normalization factors for backgrounds that have their normalization constrained using data in the fit, including all statistical and systematic uncertainties described in Section 7, but without uncertainties in total simulated cross sections extrapolated to the selected phase space. Systematic uncertainties are the dominant contribution to the normalization factor uncertainties. Also shown are the analysis channels to which the normalization factors are applied.

png (17kB)  pdf (65kB) 

Table 07


Observed event yields and predictions as computed by the fit in the τlepτlep signal regions. Uncertainties include statistical and systematic components.

png (41kB)  pdf (65kB) 

Table 08


Observed event yields and predictions as computed by the fit in the τlepτhad signal regions. Uncertainties include statistical and systematic components.

png (37kB)  pdf (58kB) 

Table 09


Observed event yields and predictions as computed by the fit in the τhadτhad signal regions. Uncertainties include statistical and systematic components.

png (36kB)  pdf (57kB) 

Table 10


Summary of different sources of uncertainty in decreasing order of their impact on σH→ττ. Their observed and expected fractional (%) impacts, both computed by the fit, are given, relative to the σH→ττ value. Experimental uncertainties in reconstructed objects combine efficiency and energy/momentum scale and resolution uncertainties. Background statistics includes the bin-by-bin statistical uncertainties in the simulated backgrounds as well as statistical uncertainties in misidentified τ backgrounds, which are estimated using data. Background normalization describes the combined impact of all background normalization uncertainties.

png (33kB)  pdf (65kB) 

Table 11


Measurement of the VBF and ggF production cross sections in three mutually exclusive regions of phase space of particle-level events. The number of jets Njets in ggF events comprises all jets with pT>30GeV. The cross section of ggF events that fail the particle-level requirements of the two ggF regions is set to the measured σH→ττggF value. Results are shown along with the SM predictions in the respective particle-level regions. The definitions of the regions closely follow the framework of simplified template cross sections [101].

png (16kB)  pdf (56kB) 

Auxiliary material

Figure 01a


mττMMC distribution for H→ττ and Z→ττ events split by (a) VBF and boosted category and (b) split by analysis channel.

png (55kB)  eps (20kB)  pdf (6kB) 

Figure 01b


mττMMC distribution for H→ττ and Z→ττ events split by (a) VBF and boosted category and (b) split by analysis channel.

png (108kB)  eps (26kB)  pdf (7kB) 

Figure 02a


Observed and expected event yields in the (a) VBF and (b) boosted Z→ττ validation regions. The total background is normalized to data in the respective inclusive Z→ττ validation region.

png (137kB)  eps (31kB)  pdf (9kB) 

Figure 02b


Observed and expected event yields in the (a) VBF and (b) boosted Z→ττ validation regions. The total background is normalized to data in the respective inclusive Z→ττ validation region.

png (119kB)  eps (31kB)  pdf (8kB) 

Figure 03


Schematic view of the signal and control regions that are used in the fit and their associations to analysis channels and categories. Arrows indicate how the background normalizations are correlated in the fit.

png (165kB)  pdf (91kB) 

Figure 04


Distribution of the reconstructed di-τ invariant mass (mττMMC) for the sum of all signal regions (SRs). The bottom panel shows the differences between observed data events and expected background events (black points). The observed Higgs-boson signal (μ = 1.09) is shown with the solid red line. Entries with values that would exceed the x-axis range are shown in the last bin of each distribution. The signal and background predictions are determined in the likelihood fit. The size of the combined statistical, experimental and theoretical uncertainties in the background is indicated by the hatched bands.

png (125kB)  eps (45kB)  pdf (11kB) 

Figure 05


Likelihood contours for the combination of all channels in the plane of the ggF and VBF signal strengths. The 68% and 95% CL contours are shown as dashed and solid lines, respectively, for mH=125GeV. The SM expectation indicated by a plus symbol and the best fit to the data is shown as a star.

png (35kB)  pdf (17kB) 

Figure 06


Display of an event in the τlepτlep final state of the boosted category, where one τ-lepton decays to an electron and the other to a muon. The electron is indicated by a green track and the muon indicated by a red track. The dashed line represents the direction of the ETmiss vector and there is a jet marked with a grey cone. The pT of the electron is pT=73.0GeV, of the muon pT=111.8GeV and of the jet pT=462.2GeV. The event has further ETmiss=284.6GeV and mττMMC=122.9GeV.

png (2MB) 

Figure 07


Display of an event in the τlepτhad final state of the VBF category, where one τ-lepton decays to an electron and there are two VBF jets. The pT of the electron is pT=45.9GeV, of the τhad pT=32.5GeV. The event has a di-jet mass of mjj=1372.7GeV and a di-τ mass of mττMMC=125.2GeV.

png (923kB) 

Figure 08


Display of an event in the τhadτhad final state of the boosted category. The pT of the τhad is pT=120.8GeV and pT=102.2GeV and the pT of the jet is pT=231.0GeV. The event has further ETmiss=23.5GeV, pTττ=237GeV and mττMMC=124.0GeV.

png (1MB)