cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.146016.v1/t2
title: "Figure 3" of "Extracting the speed of sound in the strongly interacting matter created in ultrarelativistic lead-lead collisions at the LHC"

description: The average transverse momentum of charged particles, $\langle p_{\mathrm{T}}\rangle$, as a function of the charged-particle multiplicity, $N_{\mathrm{ch}}$, within the kinematic range of $|\eta|&lt;0.5$ and extrapolated to the full $p_{\mathrm{T}}$ range in PbPb collisions at $\sqrt{s_{_{\mathrm{NN}}}}=5.02$ TeV. Both $\langle p_{\mathrm{T}}\rangle$ and $N_{\mathrm{ch}}$ are normalized by their values in the $0-5\%$ centrality class (${\langle p_{\mathrm{T}}\rangle}^{0}$ and $N_{\mathrm{ch}}^{0}$).
description: Ultrarelativistic nuclear collisions create a strongly interacting state of hot and dense quark-gluon matter that exhibits a remarkable collective flow behavior with minimal viscous dissipation. To gain deeper insights into its intrinsic nature and fundamental degrees of freedom, we extracted the speed of sound in this medium created using lead-lead (PbPb) collisions at a center-of-mass energy per nucleon pair of 5.02 TeV. The data were recorded by the CMS experiment at the CERN LHC and correspond to an integrated luminosity of $0.607 \mathrm{nb}^{-1}$. The measurement is performed by studying the multiplicity dependence of the average transverse momentum of charged particles emitted in head-on PbPb collisions. Our findings reveal that the speed of sound in this matter is nearly half of the speed of light, with its squared value being $0.241\pm0.002 (\mathrm{stat})\pm0.016 (\mathrm{syst})$ in natural units at a medium temperature of $219\pm8(\mathrm{syst})\mathrm{MeV}$, precisely aligning with predictions from lattice quantum chromodynamic (QCD) calculations. This result provides a stringent constraint on the equation of state of the created medium and a direct evidence for a deconfined QCD phase being attained in relativistic nuclear collisions.
DOI: 10.17182/hepdata.146016.v1/t3
title: "Figure 4" of "Extracting the speed of sound in the strongly interacting matter created in ultrarelativistic lead-lead collisions at the LHC"

description: The speed of sound, $c^2_{\mathrm{s}}$, as a function of the effective temperature, $T_{\mathrm{eff}}$, with the CMS data point obtained from ultra-central PbPb collision data at $\sqrt{s_{_{\mathrm{NN}}}}=5.02$ TeV.
description: Ultrarelativistic nuclear collisions create a strongly interacting state of hot and dense quark-gluon matter that exhibits a remarkable collective flow behavior with minimal viscous dissipation. To gain deeper insights into its intrinsic nature and fundamental degrees of freedom, we extracted the speed of sound in this medium created using lead-lead (PbPb) collisions at a center-of-mass energy per nucleon pair of 5.02 TeV. The data were recorded by the CMS experiment at the CERN LHC and correspond to an integrated luminosity of $0.607 \mathrm{nb}^{-1}$. The measurement is performed by studying the multiplicity dependence of the average transverse momentum of charged particles emitted in head-on PbPb collisions. Our findings reveal that the speed of sound in this matter is nearly half of the speed of light, with its squared value being $0.241\pm0.002 (\mathrm{stat})\pm0.016 (\mathrm{syst})$ in natural units at a medium temperature of $219\pm8(\mathrm{syst})\mathrm{MeV}$, precisely aligning with predictions from lattice quantum chromodynamic (QCD) calculations. This result provides a stringent constraint on the equation of state of the created medium and a direct evidence for a deconfined QCD phase being attained in relativistic nuclear collisions.
DOI: 10.17182/hepdata.146016.v1/t1
title: "Figure 2" of "Extracting the speed of sound in the strongly interacting matter created in ultrarelativistic lead-lead collisions at the LHC"

description: The event fraction distribution as a function of the charged-particle multiplicity, $N_{\mathrm{ch}}$, within the kinematic range of $|\eta|&lt;0.5$ and extrapolated to the full $p_{\mathrm{T}}$ range, in PbPb collisions at $\sqrt{s_{_{\mathrm{NN}}}}=5.02$ TeV. The $N_{\mathrm{ch}}$ value is normalized by its value in the $0-5\%$ centrality class ($N_{\mathrm{ch}}^{0}$).
description: Ultrarelativistic nuclear collisions create a strongly interacting state of hot and dense quark-gluon matter that exhibits a remarkable collective flow behavior with minimal viscous dissipation. To gain deeper insights into its intrinsic nature and fundamental degrees of freedom, we extracted the speed of sound in this medium created using lead-lead (PbPb) collisions at a center-of-mass energy per nucleon pair of 5.02 TeV. The data were recorded by the CMS experiment at the CERN LHC and correspond to an integrated luminosity of $0.607 \mathrm{nb}^{-1}$. The measurement is performed by studying the multiplicity dependence of the average transverse momentum of charged particles emitted in head-on PbPb collisions. Our findings reveal that the speed of sound in this matter is nearly half of the speed of light, with its squared value being $0.241\pm0.002 (\mathrm{stat})\pm0.016 (\mathrm{syst})$ in natural units at a medium temperature of $219\pm8(\mathrm{syst})\mathrm{MeV}$, precisely aligning with predictions from lattice quantum chromodynamic (QCD) calculations. This result provides a stringent constraint on the equation of state of the created medium and a direct evidence for a deconfined QCD phase being attained in relativistic nuclear collisions.
DOI: 10.17182/hepdata.146018.v1/t1
title: "q^2 bin yields & BF" of "Test of lepton flavor universality in B$^{\pm}$$\to$ K$^{\pm}\mu^+\mu^-$ and B$^{\pm}$$\to$ K$^{\pm}$e$^+$e$^-$ decays in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The differential $\text{B}^+ \to \text{K}^+\mu^+\mu^-$ branching fraction measured in the individual $q^2$ bins. The uncertainties in the yields are statistical uncertainties from the fit, while the branching fraction uncertainties include both the statistical and systematic components.
description: A test of lepton flavor universality in $\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-$ and $\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-$ decays, as well as a measurement of differential and integrated branching fractions of a nonresonant$\text{B}^\pm \to \text{K}^\pm\mu^+\mu^-$ decay are presented. The analysis is made possible by a dedicated data set of proton-proton collisions at $\sqrt{s} = 13$ TeV recorded in 2018, by the CMS experiment at the LHC, using a special high-rate data stream designed for collecting about 10 billion unbiased b hadron decays. The ratio of the branching fractions $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-)$ to $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-)$ is determined from the measured double ratio $R(\text{K})$ of these decays to the respective branching fractions of the $\text{B}^\pm\to\text{J}\psi\text{K}^\pm$ with $\text{J}\psi\to\mu^+\mu^-$ and $\text{e}^+\text{e}^-$ decays, which allow for significant cancellation of systematic uncertainties. The ratio $R(\text{K})$ is measured in the range $1.1
DOI: 10.17182/hepdata.146018.v1/t2
title: "Differential BF" of "Test of lepton flavor universality in B$^{\pm}$$\to$ K$^{\pm}\mu^+\mu^-$ and B$^{\pm}$$\to$ K$^{\pm}$e$^+$e$^-$ decays in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Differential branching fraction $d\mathcal{B}/dq^2$, with theoretical predictions obtained with the HEPFiT, SuperIso, Flavio, and EOS packages. The HEPFiT predictions are available only for $q^2 &lt; 8\ \mathrm{GeV}^2$.
description: A test of lepton flavor universality in $\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-$ and $\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-$ decays, as well as a measurement of differential and integrated branching fractions of a nonresonant$\text{B}^\pm \to \text{K}^\pm\mu^+\mu^-$ decay are presented. The analysis is made possible by a dedicated data set of proton-proton collisions at $\sqrt{s} = 13$ TeV recorded in 2018, by the CMS experiment at the LHC, using a special high-rate data stream designed for collecting about 10 billion unbiased b hadron decays. The ratio of the branching fractions $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-)$ to $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-)$ is determined from the measured double ratio $R(\text{K})$ of these decays to the respective branching fractions of the $\text{B}^\pm\to\text{J}\psi\text{K}^\pm$ with $\text{J}\psi\to\mu^+\mu^-$ and $\text{e}^+\text{e}^-$ decays, which allow for significant cancellation of systematic uncertainties. The ratio $R(\text{K})$ is measured in the range $1.1
DOI: 10.17182/hepdata.146018.v1/t3
title: "Uncertainty components" of "Test of lepton flavor universality in B$^{\pm}$$\to$ K$^{\pm}\mu^+\mu^-$ and B$^{\pm}$$\to$ K$^{\pm}$e$^+$e$^-$ decays in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Relative uncertainties in the differential branching fraction measurement of $\mathrm{B}^+\to\mathrm{K}^+\mu^+\mu^-$ per $q^2$ bin.
description: A test of lepton flavor universality in $\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-$ and $\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-$ decays, as well as a measurement of differential and integrated branching fractions of a nonresonant$\text{B}^\pm \to \text{K}^\pm\mu^+\mu^-$ decay are presented. The analysis is made possible by a dedicated data set of proton-proton collisions at $\sqrt{s} = 13$ TeV recorded in 2018, by the CMS experiment at the LHC, using a special high-rate data stream designed for collecting about 10 billion unbiased b hadron decays. The ratio of the branching fractions $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-)$ to $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-)$ is determined from the measured double ratio $R(\text{K})$ of these decays to the respective branching fractions of the $\text{B}^\pm\to\text{J}\psi\text{K}^\pm$ with $\text{J}\psi\to\mu^+\mu^-$ and $\text{e}^+\text{e}^-$ decays, which allow for significant cancellation of systematic uncertainties. The ratio $R(\text{K})$ is measured in the range $1.1
DOI: 10.17182/hepdata.146018.v1/t4
title: "Correlation matrix" of "Test of lepton flavor universality in B$^{\pm}$$\to$ K$^{\pm}\mu^+\mu^-$ and B$^{\pm}$$\to$ K$^{\pm}$e$^+$e$^-$ decays in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Correlation matrix for the differential branching fraction extraction between different $q^2$ bins in the simultaneous fit.
description: A test of lepton flavor universality in $\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-$ and $\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-$ decays, as well as a measurement of differential and integrated branching fractions of a nonresonant$\text{B}^\pm \to \text{K}^\pm\mu^+\mu^-$ decay are presented. The analysis is made possible by a dedicated data set of proton-proton collisions at $\sqrt{s} = 13$ TeV recorded in 2018, by the CMS experiment at the LHC, using a special high-rate data stream designed for collecting about 10 billion unbiased b hadron decays. The ratio of the branching fractions $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-)$ to $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-)$ is determined from the measured double ratio $R(\text{K})$ of these decays to the respective branching fractions of the $\text{B}^\pm\to\text{J}\psi\text{K}^\pm$ with $\text{J}\psi\to\mu^+\mu^-$ and $\text{e}^+\text{e}^-$ decays, which allow for significant cancellation of systematic uncertainties. The ratio $R(\text{K})$ is measured in the range $1.1
DOI: 10.17182/hepdata.146018.v1/t5
title: "Efficiency" of "Test of lepton flavor universality in B$^{\pm}$$\to$ K$^{\pm}\mu^+\mu^-$ and B$^{\pm}$$\to$ K$^{\pm}$e$^+$e$^-$ decays in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The product of acceptance and efficiency ($A\epsilon$) of the $\mathcal{B}(\mathrm{B}^+\to\mathrm{K}^+\mu^+\mu^-)$ channel, as a function of the muon pair $q^2$, as measured in simulated signal events, after all the corrections applied. In the figure, regions corresponding to resonances are displayed with red markers.
description: A test of lepton flavor universality in $\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-$ and $\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-$ decays, as well as a measurement of differential and integrated branching fractions of a nonresonant$\text{B}^\pm \to \text{K}^\pm\mu^+\mu^-$ decay are presented. The analysis is made possible by a dedicated data set of proton-proton collisions at $\sqrt{s} = 13$ TeV recorded in 2018, by the CMS experiment at the LHC, using a special high-rate data stream designed for collecting about 10 billion unbiased b hadron decays. The ratio of the branching fractions $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-)$ to $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-)$ is determined from the measured double ratio $R(\text{K})$ of these decays to the respective branching fractions of the $\text{B}^\pm\to\text{J}\psi\text{K}^\pm$ with $\text{J}\psi\to\mu^+\mu^-$ and $\text{e}^+\text{e}^-$ decays, which allow for significant cancellation of systematic uncertainties. The ratio $R(\text{K})$ is measured in the range $1.1
DOI: 10.17182/hepdata.146018.v1/t6
title: "Resonance efficiency" of "Test of lepton flavor universality in B$^{\pm}$$\to$ K$^{\pm}\mu^+\mu^-$ and B$^{\pm}$$\to$ K$^{\pm}$e$^+$e$^-$ decays in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Same as Table 5, but for the bins containing the J$\psi$ and $\psi$(2S) resonances.
description: A test of lepton flavor universality in $\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-$ and $\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-$ decays, as well as a measurement of differential and integrated branching fractions of a nonresonant$\text{B}^\pm \to \text{K}^\pm\mu^+\mu^-$ decay are presented. The analysis is made possible by a dedicated data set of proton-proton collisions at $\sqrt{s} = 13$ TeV recorded in 2018, by the CMS experiment at the LHC, using a special high-rate data stream designed for collecting about 10 billion unbiased b hadron decays. The ratio of the branching fractions $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-)$ to $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-)$ is determined from the measured double ratio $R(\text{K})$ of these decays to the respective branching fractions of the $\text{B}^\pm\to\text{J}\psi\text{K}^\pm$ with $\text{J}\psi\to\mu^+\mu^-$ and $\text{e}^+\text{e}^-$ decays, which allow for significant cancellation of systematic uncertainties. The ratio $R(\text{K})$ is measured in the range $1.1
DOI: 10.17182/hepdata.146018.v1/t7
title: "Integrated BF" of "Test of lepton flavor universality in B$^{\pm}$$\to$ K$^{\pm}\mu^+\mu^-$ and B$^{\pm}$$\to$ K$^{\pm}$e$^+$e$^-$ decays in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Integrated branching fraction $\mathcal{B}(\mathrm{B}^\pm \to \mathrm{K}^\pm\mu^+\mu^-)$ in the low-$q^2$ region.
description: A test of lepton flavor universality in $\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-$ and $\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-$ decays, as well as a measurement of differential and integrated branching fractions of a nonresonant$\text{B}^\pm \to \text{K}^\pm\mu^+\mu^-$ decay are presented. The analysis is made possible by a dedicated data set of proton-proton collisions at $\sqrt{s} = 13$ TeV recorded in 2018, by the CMS experiment at the LHC, using a special high-rate data stream designed for collecting about 10 billion unbiased b hadron decays. The ratio of the branching fractions $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-)$ to $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-)$ is determined from the measured double ratio $R(\text{K})$ of these decays to the respective branching fractions of the $\text{B}^\pm\to\text{J}\psi\text{K}^\pm$ with $\text{J}\psi\to\mu^+\mu^-$ and $\text{e}^+\text{e}^-$ decays, which allow for significant cancellation of systematic uncertainties. The ratio $R(\text{K})$ is measured in the range $1.1
DOI: 10.17182/hepdata.146018.v1/t8
title: "R(K) measurement" of "Test of lepton flavor universality in B$^{\pm}$$\to$ K$^{\pm}\mu^+\mu^-$ and B$^{\pm}$$\to$ K$^{\pm}$e$^+$e$^-$ decays in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Ratio of branching fractions $\mathcal{B}(\text{B}^\pm \to \text{K}^\pm\mu^+\mu^-)$ to $\mathcal{B}(\text{B}^\pm \to \text{K}^\pm\text{e}^+\text{e}^-)$, determined from the measured double ratio $R$(K) of these decays to the respective branching fractions of the decay chains $\text{B}^\pm\to\text{J/}\psi\text{K}^\pm$ with $\text{J/}\psi\to\mu^+\mu^-$ and $\text{e}^+\text{e}^-$.
description: A test of lepton flavor universality in $\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-$ and $\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-$ decays, as well as a measurement of differential and integrated branching fractions of a nonresonant$\text{B}^\pm \to \text{K}^\pm\mu^+\mu^-$ decay are presented. The analysis is made possible by a dedicated data set of proton-proton collisions at $\sqrt{s} = 13$ TeV recorded in 2018, by the CMS experiment at the LHC, using a special high-rate data stream designed for collecting about 10 billion unbiased b hadron decays. The ratio of the branching fractions $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-)$ to $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-)$ is determined from the measured double ratio $R(\text{K})$ of these decays to the respective branching fractions of the $\text{B}^\pm\to\text{J}\psi\text{K}^\pm$ with $\text{J}\psi\to\mu^+\mu^-$ and $\text{e}^+\text{e}^-$ decays, which allow for significant cancellation of systematic uncertainties. The ratio $R(\text{K})$ is measured in the range $1.1
DOI: 10.17182/hepdata.146018.v1/t9
title: "Likelihood" of "Test of lepton flavor universality in B$^{\pm}$$\to$ K$^{\pm}\mu^+\mu^-$ and B$^{\pm}$$\to$ K$^{\pm}$e$^+$e$^-$ decays in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Negative log likelihood function from the fit profiled as a function of the inverse ratio $R(\mathrm{K})^{-1}$.
description: A test of lepton flavor universality in $\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-$ and $\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-$ decays, as well as a measurement of differential and integrated branching fractions of a nonresonant$\text{B}^\pm \to \text{K}^\pm\mu^+\mu^-$ decay are presented. The analysis is made possible by a dedicated data set of proton-proton collisions at $\sqrt{s} = 13$ TeV recorded in 2018, by the CMS experiment at the LHC, using a special high-rate data stream designed for collecting about 10 billion unbiased b hadron decays. The ratio of the branching fractions $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\mu^+\mu^-)$ to $\mathcal{B}(\text{B}^\pm \to\text{K}^\pm\text{e}^+\text{e}^-)$ is determined from the measured double ratio $R(\text{K})$ of these decays to the respective branching fractions of the $\text{B}^\pm\to\text{J}\psi\text{K}^\pm$ with $\text{J}\psi\to\mu^+\mu^-$ and $\text{e}^+\text{e}^-$ decays, which allow for significant cancellation of systematic uncertainties. The ratio $R(\text{K})$ is measured in the range $1.1
DOI: 10.17182/hepdata.146026.v1/t1
title: "Table 1" of "Search for high-mass resonances in final states with a $\tau$-lepton and missing transverse momentum with the ATLAS detector"

description: Observed and predicted $m_{\rm T}$ distributions including SSM and NU (cot$\theta$ = 5.5) $W^{\prime}$ signals with masses of 4 TeV. Please note that in the paper figure the bin content is divided by the bin width, but this is not done in the HepData table.
description: CERN-LHC. Search for high-mass resonances in final states with a $\tau$-lepton and missing transverse momentum with the ATLAS detector

 Units of GeV and pb are used for all data in this entry, which may be different to those used in the publication. 

 Fiducial region: 
 - No electrons or muons 
 - $p_{\rm T}$(e) &gt; 20 GeV, |$\eta$(e)| &lt; 2.47
 - $p_{\rm T}$($\mu$) &gt; 20 GeV, |$\eta$($\mu$)| &lt; 2.5
 - At least one hadronic tau decay ($\tau_{\rm had-vis}$)
 - $p_{\rm T}$($\tau_{\rm had-vis}$) &gt; 30 GeV, |$\eta$($\tau_{\rm had-vis}$)| &lt; 2.4
 - Choose $\tau_{\rm had-vis}$ with highest $p_{\rm T}$
 - $E_{\rm T}^{\rm miss}$ &gt; 150 GeV
 - 0.7 &lt; $p_{\rm T}$($\tau_{\rm had-vis}$) / $E_{\rm T}^{\rm miss}$ &lt; 1.3 
 - $\Delta\phi$($\tau_{\rm had-vis}$, $E_{\rm T}^{\rm miss}$) &gt; 2.4 rad 
 - $m_{\rm T}$($\tau_{\rm had-vis}$, $E_{\rm T}^{\rm miss}$) &gt; threshold 
 - Choose threshold in range 200-2950 GeV in 50 GeV steps

 Note: significant activity near the chosen $\tau_{\rm had-vis}$ would reduce its identification efficiency. If signals with a busy final state are considered we suggest to reject events if the scalar sum $p_{\rm T}$ of stable charged particles within $\Delta R$ = 0.4 or neutral particles within $\Delta R$ = 0.2 of the chosen $\tau_{\rm had-vis}$ is larger than a few GeV (not including pileup or decay products of the chosen $\tau_{\rm had-vis}$)
 
 These results can be reinterpreted for alternate signal models using the limits on the visible $\tau\nu$ production cross section ($\sigma_{\rm vis} = \sigma \times \mathcal{A} \times \varepsilon$) provided in Table 4. 

 Reinterpretation requires calculation of: 
 - $\sigma$: signal cross section including production and decay
 - $\mathcal{A}$: acceptance of fiducial selection at generator level
 - $\varepsilon$: reconstruction efficiency

 First, calculate the visible cross section for each $m_{\rm T}$ threshold at a single parameter-space point of the signal model is question. The parameter-space point is excluded if the visible cross section is larger than the limit at any $m_{\rm T}$ threshold. Repeat the process for all parameter-space points and models to determine the excluded regions. 

 The reconstruction efficiency is dependent on $m_{\rm T}$, and therefore on the $m_{\rm T}$ distribution of the signal model. It can be incorporated by weighting generated events by the parameterized efficiency: 
 $\varepsilon$($m_{\rm T}$ [TeV]) =0.8143 - 0.3094$m_{\rm T}$+ 0.0863$m_{\rm T}^2$ - 0.00545$m_{\rm T}^3$

 For reference, the acceptance and acceptance times efficiency for the SSM model can be found in Tables 7 and 8.