cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.78402.v1/t24
title: "Table 24" of "Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.
description: CERN-LHC. A search for heavy neutral Higgs bosons and $Z^{\prime}$ bosons is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC during 2015 and 2016.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.78402.v1/t25
title: "Table 25" of "Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.
description: CERN-LHC. A search for heavy neutral Higgs bosons and $Z^{\prime}$ bosons is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC during 2015 and 2016.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.78402.v1/t26
title: "Table 26" of "Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.
description: CERN-LHC. A search for heavy neutral Higgs bosons and $Z^{\prime}$ bosons is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC during 2015 and 2016.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.78402.v1/t27
title: "Table 27" of "Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.
description: CERN-LHC. A search for heavy neutral Higgs bosons and $Z^{\prime}$ bosons is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC during 2015 and 2016.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.78402.v1/t28
title: "Table 28" of "Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.
description: CERN-LHC. A search for heavy neutral Higgs bosons and $Z^{\prime}$ bosons is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC during 2015 and 2016.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.78402.v1/t29
title: "Table 7" of "Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.
description: CERN-LHC. A search for heavy neutral Higgs bosons and $Z^{\prime}$ bosons is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC during 2015 and 2016.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.78403.v1/t1
title: "Table 1" of "Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC $pp$ collision data at $\sqrt{s}=$ 7 and 8 TeV"

description: Best fit values of $\sigma_i \cdot \mathrm{B}^f$ for each specific channel $i \to H\to f$, as obtained from the generic parameterisation with 23 parameters for the combination of the ATLAS and CMS measurements, using the $\sqrt{s}$=7 and 8 TeV data. The cross sections are given for $\sqrt{s}$=8 TeV, assuming the SM values for $\sigma_i(7 \mathrm{TeV})/\sigma_i(8 \mathrm{TeV})$. The results are shown together with their total uncertainties and their breakdown into statistical and systematic components. The missing values are either not measured with a meaningful precision and therefore not quoted, in the case of the $H\to ZZ$ decay channel for the $WH$, $ZH$, and $ttH$ production processes, or not measured at all and therefore fixed to their corresponding SM predictions, in the case of the $H\to bb$ decay mode for the $gg\mathrm{F}$ and VBF production processes.
description: CERN-LHC. Combined ATLAS and CMS measurements of the Higgs boson production and decay rates, as well as constraints on its couplings to vector bosons and fermions, are presented. The combination is based on the analysis of five production processes, namely gluon fusion, vector boson fusion, and associated production with a $W$ or a $Z$ boson or a pair of top quarks, and of the six decay modes $H \to ZZ, WW$, $\gamma\gamma, \tau\tau, bb$, and $\mu\mu$. All results are reported assuming a value of 125.09 GeV for the Higgs boson mass, the result of the combined measurement by the ATLAS and CMS experiments. The analysis uses the CERN LHC proton-proton collision data recorded by the ATLAS and CMS experiments in 2011 and 2012, corresponding to integrated luminosities per experiment of approximately 5 fb$^{-1}$ at $\sqrt{s}$=7 TeV and 20 fb$^{-1}$ at $\sqrt{s}$ = 8 TeV. The Higgs boson production and decay rates measured by the two experiments are combined within the context of three generic parameterisations: two based on cross sections and branching fractions, and one on ratios of coupling modifiers. Several interpretations of the measurements with more model-dependent parameterisations are also given. The combined signal yield relative to the Standard Model prediction is measured to be 1.09 $\pm$ 0.11. The combined measurements lead to observed significances for the vector boson fusion production process and for the $H \to \tau\tau$ decay of 5.4 and 5.5 standard deviations, respectively. The data are consistent with the Standard Model predictions for all parameterisations considered.
DOI: 10.17182/hepdata.78403.v1/t2
title: "Table 2" of "Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC $pp$ collision data at $\sqrt{s}=$ 7 and 8 TeV"

description: Best fit values of $\sigma_i \cdot \mathrm{B}^f$ relative to their SM prediction for each specific channel $i \to H\to f$, as obtained from the generic parameterisation with 23 parameters for the combination of the ATLAS and CMS measurements, using the $\sqrt{s}$=7 and 8 TeV data. The results are shown together with their total uncertainties and their breakdown into statistical and systematic components. The missing values are either not measured with a meaningful precision and therefore not quoted, in the case of the $H\to ZZ$ decay channel for the $WH$, $ZH$, and $ttH$ production processes, or not measured at all and therefore fixed to their corresponding SM predictions, in the case of the $H\to bb$ decay mode for the $gg\mathrm{F}$ and VBF production processes.
description: CERN-LHC. Combined ATLAS and CMS measurements of the Higgs boson production and decay rates, as well as constraints on its couplings to vector bosons and fermions, are presented. The combination is based on the analysis of five production processes, namely gluon fusion, vector boson fusion, and associated production with a $W$ or a $Z$ boson or a pair of top quarks, and of the six decay modes $H \to ZZ, WW$, $\gamma\gamma, \tau\tau, bb$, and $\mu\mu$. All results are reported assuming a value of 125.09 GeV for the Higgs boson mass, the result of the combined measurement by the ATLAS and CMS experiments. The analysis uses the CERN LHC proton-proton collision data recorded by the ATLAS and CMS experiments in 2011 and 2012, corresponding to integrated luminosities per experiment of approximately 5 fb$^{-1}$ at $\sqrt{s}$=7 TeV and 20 fb$^{-1}$ at $\sqrt{s}$ = 8 TeV. The Higgs boson production and decay rates measured by the two experiments are combined within the context of three generic parameterisations: two based on cross sections and branching fractions, and one on ratios of coupling modifiers. Several interpretations of the measurements with more model-dependent parameterisations are also given. The combined signal yield relative to the Standard Model prediction is measured to be 1.09 $\pm$ 0.11. The combined measurements lead to observed significances for the vector boson fusion production process and for the $H \to \tau\tau$ decay of 5.4 and 5.5 standard deviations, respectively. The data are consistent with the Standard Model predictions for all parameterisations considered.