cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.85868.v1/t27
title: "Figure 11 c" of "Measurement of associated Z + charm production in proton-proton collisions at $\sqrt{s} = $ 8 TeV"

description: Differential Z + c cross section as a function of the transverse momentum of the jet
description: A study of the associated production of a Z boson and a charm quark jet (Z+c), and a comparison to production with a b quark jet (Z+b), in pp collisions at a centre-of-mass energy of 8 TeV are presented. The analysis uses a data sample corresponding to an integrated luminosity of 19.7 fb$^{-1}$, collected with the CMS detector at the CERN LHC. The Z boson candidates are identified through their decays into pairs of electrons or muons. Jets originating from heavy flavour quarks are identified using semileptonic decays of c or b flavoured hadrons and hadronic decays of charm hadrons. The measurements are performed in the kinematic region with two leptons with $p_T^l &gt; 20$ GeV, $|\eta_l| &lt; 2.1$, $71 &lt; m_{\ell\ell} &lt; 111$ GeV, and heavy flavour jets with $p_T^{\text{jet}} &gt; 25$ GeV and $|\eta_\text{jet}| &lt; 2.5$. The Z+c production cross section is measured to $\sigma(pp \to Z + c + X) \mathcal{B}(Z \to \ell^+\ell^-) = 8.8 \pm 0.5$ (stat) $\pm 0.6$ (syst) pb. The ratio of the Z+c and Z+b production cross sections is measured to be $\sigma(pp \to Z + c + X)/\sigma(pp \to Z + b + X) = 2.0 \pm 0.2$ (stat) $\pm 0.2$ (syst). The Z+c production cross section and the cross section ratio are also measured as a function of the transverse momentum of the Z boson and of the heavy flavour jet. The measurements are compared with theoretical predictions.
DOI: 10.17182/hepdata.85868.v1/t28
title: "Figure 11 d" of "Measurement of associated Z + charm production in proton-proton collisions at $\sqrt{s} = $ 8 TeV"

description: (Z +c)/(Z +b) cross section ratio as a function of the transverse momentum of the jet.
description: A study of the associated production of a Z boson and a charm quark jet (Z+c), and a comparison to production with a b quark jet (Z+b), in pp collisions at a centre-of-mass energy of 8 TeV are presented. The analysis uses a data sample corresponding to an integrated luminosity of 19.7 fb$^{-1}$, collected with the CMS detector at the CERN LHC. The Z boson candidates are identified through their decays into pairs of electrons or muons. Jets originating from heavy flavour quarks are identified using semileptonic decays of c or b flavoured hadrons and hadronic decays of charm hadrons. The measurements are performed in the kinematic region with two leptons with $p_T^l &gt; 20$ GeV, $|\eta_l| &lt; 2.1$, $71 &lt; m_{\ell\ell} &lt; 111$ GeV, and heavy flavour jets with $p_T^{\text{jet}} &gt; 25$ GeV and $|\eta_\text{jet}| &lt; 2.5$. The Z+c production cross section is measured to $\sigma(pp \to Z + c + X) \mathcal{B}(Z \to \ell^+\ell^-) = 8.8 \pm 0.5$ (stat) $\pm 0.6$ (syst) pb. The ratio of the Z+c and Z+b production cross sections is measured to be $\sigma(pp \to Z + c + X)/\sigma(pp \to Z + b + X) = 2.0 \pm 0.2$ (stat) $\pm 0.2$ (syst). The Z+c production cross section and the cross section ratio are also measured as a function of the transverse momentum of the Z boson and of the heavy flavour jet. The measurements are compared with theoretical predictions.
DOI: 10.17182/hepdata.85869.v1/t1
title: "Table 1" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: The dielectron cross section in inelastic pp collisions at $\sqrt{s}$ = 13 TeV as a function of invariant mass for $p_{\rm T,ee}$ &lt; 6.0 GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t2
title: "Table 2" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: The dielectron cross section in inelastic pp collisions at $\sqrt{s}$ = 13 TeV as a function of pair transverse momentum for $m_{\rm ee}$ &lt; 0.14 GeV/$c^{2}$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t3
title: "Table 3" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: The dielectron cross section in inelastic pp collisions at $\sqrt{s}$ = 13 TeV as a function of pair transverse momentum for 0.14 &lt; $m_{\rm ee}$ &lt; 0.7 GeV/$c^{2}$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t4
title: "Table 4" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: The dielectron cross section in inelastic pp collisions at $\sqrt{s}$ = 13 TeV as a function of pair transverse momentum for 0.7 &lt; $m_{\rm ee}$ &lt; 1.03 GeV/$c^{2}$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t5
title: "Table 5" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: Ratio of dielectron spectra in HM and INEL events scaled by the charged-particle multiplicity as a function of invariant mass for $p_{\rm T,ee}$ &lt; 6.0 GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t6
title: "Table 6" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: Ratio of dielectron spectra in HM and INEL events scaled by the charged-particle multiplicity as a function of invariant mass for $p_{\rm T,ee}$ &lt; 1.0 GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t7
title: "Table 7" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: Ratio of dielectron spectra in HM and INEL events scaled by the charged-particle multiplicity as a function of invariant mass for 1.0 &lt; $p_{\rm T,ee}$ &lt; 2.0 GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t10
title: "Table 10" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: The dielectron cross section in inelastic pp collisions at $\sqrt{s}$ = 13 TeV as a function of pair transverse momentum for 1.03 &lt; $m_{\rm ee}$ &lt; 2.86 GeV/$c^{2}$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t11
title: "Table 11" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: The dielectron cross section in inelastic pp collisions at $\sqrt{s}$ = 13 TeV as a function of invariant mass for $p_{\rm T,ee}$ &lt; 1.0 GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t12
title: "Table 12" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: The dielectron cross section in inelastic pp collisions at $\sqrt{s}$ = 13 TeV as a function of invariant mass for 1.0 &lt; $p_{\rm T,ee}$ &lt; 2.0 GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t13
title: "Table 13" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: The dielectron cross section in inelastic pp collisions at $\sqrt{s}$ = 13 TeV as a function of invariant mass for 2.0 &lt; $p_{\rm T,ee}$ &lt; 3.0 GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t14
title: "Table 14" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: The dielectron cross section in inelastic pp collisions at $\sqrt{s}$ = 13 TeV as a function of invariant mass for 3.0 &lt; $p_{\rm T,ee}$ &lt; 6.0 GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t16
title: "Table 16" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: Ratio of direct to inclusive photon cross sections extracted from the dielectron spectra in high-multiplicity pp collisions at $\sqrt{s}$ = 13 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t8
title: "Table 8" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: Ratio of dielectron spectra in HM and INEL events scaled by the charged-particle multiplicity as a function of invariant mass for 2.0 &lt; $p_{\rm T,ee}$ &lt; 3.0 GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t9
title: "Table 9" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: Ratio of dielectron spectra in HM and INEL events scaled by the charged-particle multiplicity as a function of invariant mass for 3.0 &lt; $p_{\rm T,ee}$ &lt; 6.0 GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.85869.v1/t15
title: "Table 15" of "Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV"

description: Ratio of direct to inclusive photon cross sections extracted from the dielectron spectra in inelastic pp collisions at $\sqrt{s}$ = 13 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.85886.v1/t1
title: "Table 1" of "Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and two $\tau$ leptons in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Expected and observed 95% CL upper limits on (sigma(pp-&gt;h)/sigma(pp-&gt;hSM)) * B(h -&gt; aa -&gt; mumutautau) as a function of m(a), where h(SM) is the Higgs boson of the standard model, h is the observed particle with mass of 125 GeV, and a denotes a light Higgs-like state, as obtained from the 13 TeV data.
description: CERN-LHC. The analysis searches for exotic Higgs boson decays to two light pseudoscalars, in the final state of two muons and two tau leptons. This signature is sensitive to the Higgs sector of the next to minimal supersymmetric standard model (NMSSM) as well as two Higgs doublet models extended with a scalar singlet (2HDM+S). The analysis is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC, in 2016 corresponding to an integrated luminosity of 35.9 fb-1. No signal above the standard model background expectation is observed. The tables give upper limits on the cross section times branching fraction for Higgs bosons with masses between 15 and 62 GeV.
DOI: 10.17182/hepdata.86132.v1/t2
title: "Table 2" of "Observation of Higgs boson decay to bottom quarks"

description: Best-fit value of the H--&gt;b bbar signal strength with its 1 sigma systematic (red) and total (blue) uncertainties for the five individual production modes considered, as well as the overall combined result. The vertical dashed line indicates the standard model expectation. All results are extracted from a single fit combining all input analyses, with mH = 125.09 GeV. Data from Figure 3.
description: No data abstract available.
DOI: 10.17182/hepdata.86132.v1/t1
title: "Table 1" of "Observation of Higgs boson decay to bottom quarks"

description: Expected and observed significances, in number of standard deviations, and observed signal strengths for the VH production process with H--&gt;b bbar. Results are shown separately for 2017 data, combined Run 2 (2016 and 2017 data), and for the combination of the Run 1 and Run 2 data. For the 2017 analysis, results are shown separately for the individual mu value for each channel from a combined simultaneous fit to all channels. All results are obtained for mH=125.09 GeV. Data are from Table 2 and 2016 added from Figure 1b.
description: No data abstract available.
DOI: 10.17182/hepdata.86133.v1/t1
title: "Table 1" of "Search for beyond the standard model Higgs bosons decaying into a $\mathrm{b\overline{b}}$ pair in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed 95% CL upper limits on sigma(pp-&gt;b+H(MSSM)+X) * B(H(MSSM) -&gt; bb) in pb as a function of m(H(MSSM)), where H(MSSM) denotes a heavy Higgs-like state like the H and A bosons of MSSM and 2HDM, as obtained from the 13 TeV data.
description: CERN-LHC. The analysis searches for neutral Higgs bosons which decay into a bb quark pair and are produced in association with at least one additional b quark. This signature is sensitive to the Higgs sector of the minimal supersymmetric standard model (MSSM) with large values of the parameter tan(beta) as well as two Higgs doublet models (2HDM). The analysis is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 35.7 fb-1. No signal above the standard model background expectation is observed. The tables give upper limits on the cross section times branching fraction for Higgs bosons with masses up to 1300 GeV, and upper limits for the MSSM parameter tan(beta) as function of the mass of the pseudoscalar MSSM Higgs bosons H/A within different MSSM benchmark scenarios.

Only selected tables are displayed here. Please see the full paper for interpretations in other MSSM benchmark scenarios and 2HDM.
DOI: 10.17182/hepdata.86133.v1/t2
title: "Table 2" of "Search for beyond the standard model Higgs bosons decaying into a $\mathrm{b\overline{b}}$ pair in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed 95% CL upper limits on tan(beta) as a function of m(A) in the mhmodp benchmark scenario for a higgsino mass parameter of mu=+200 GeV. Since theoretical predictions are not reliable for tan(beta)&gt;60, entries for which tan(beta) would exceed this value are indicated by N/A.
description: CERN-LHC. The analysis searches for neutral Higgs bosons which decay into a bb quark pair and are produced in association with at least one additional b quark. This signature is sensitive to the Higgs sector of the minimal supersymmetric standard model (MSSM) with large values of the parameter tan(beta) as well as two Higgs doublet models (2HDM). The analysis is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 35.7 fb-1. No signal above the standard model background expectation is observed. The tables give upper limits on the cross section times branching fraction for Higgs bosons with masses up to 1300 GeV, and upper limits for the MSSM parameter tan(beta) as function of the mass of the pseudoscalar MSSM Higgs bosons H/A within different MSSM benchmark scenarios.

Only selected tables are displayed here. Please see the full paper for interpretations in other MSSM benchmark scenarios and 2HDM.
DOI: 10.17182/hepdata.86133.v1/t3
title: "Table 3" of "Search for beyond the standard model Higgs bosons decaying into a $\mathrm{b\overline{b}}$ pair in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed 95% CL upper limits on tan(beta) as a function of m(A) in the hMSSM benchmark scenario. Since theoretical predictions are not reliable for tan(beta)&gt;60, entries for which tan(beta) would exceed this value are indicated by N/A.
description: CERN-LHC. The analysis searches for neutral Higgs bosons which decay into a bb quark pair and are produced in association with at least one additional b quark. This signature is sensitive to the Higgs sector of the minimal supersymmetric standard model (MSSM) with large values of the parameter tan(beta) as well as two Higgs doublet models (2HDM). The analysis is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 35.7 fb-1. No signal above the standard model background expectation is observed. The tables give upper limits on the cross section times branching fraction for Higgs bosons with masses up to 1300 GeV, and upper limits for the MSSM parameter tan(beta) as function of the mass of the pseudoscalar MSSM Higgs bosons H/A within different MSSM benchmark scenarios.

Only selected tables are displayed here. Please see the full paper for interpretations in other MSSM benchmark scenarios and 2HDM.
DOI: 10.17182/hepdata.86134.v1/t1
title: "Table 1" of "Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV"

description: The observed and expected upper limits on the cross section for a spin-2 resonance X $\rightarrow$ H(bb) H(bb) at 95% CL, using the asymptotic CLs method
description: Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV. The 95% CL upper limits on the production cross section times branching fraction on the resonant (spin-0 and spin-2) are provided.
DOI: 10.17182/hepdata.86134.v1/t2
title: "Table 2" of "Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV"

description: The observed and expected upper limits on the cross section for a spin-0 resonance X $\rightarrow$ H(bb) H(bb) at 95% CL, using the asymptotic CLs method
description: Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV. The 95% CL upper limits on the production cross section times branching fraction on the resonant (spin-0 and spin-2) are provided.
DOI: 10.17182/hepdata.86140.v1/t1
title: "Table 1" of "Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $\sqrt{s}= $ 13 TeV"

description: Normalized inclusive 2-jet cross section differential in $\Delta\phi_{1,2}$ for $200 &lt; p_{T}^{max} &lt; 300$ GeV
description: CERN-LHC. CMS. Azimuthal correlations between the two jets with the largest transverse momenta $p_{T}$ in inclusive 2-, 3-, and 4-jet events are presented for several regions of the leading jet $p_{T}$ up to 4 TeV. For 3- and 4-jet scenarios, measurements of the minimum azimuthal angles between any two of the three or four leading $p_{T}$ jets are also presented. Jets are reconstructed using the infrared- and collinear-safe anti-$k_{T}$ clustering algorithm with a distance parameter $R=0.4$.
DOI: 10.17182/hepdata.86140.v1/t2
title: "Table 2" of "Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $\sqrt{s}= $ 13 TeV"

description: Normalized inclusive 2-jet cross section differential in $\Delta\phi_{1,2}$ for $300 &lt; p_{T}^{max} &lt; 400$ GeV
description: CERN-LHC. CMS. Azimuthal correlations between the two jets with the largest transverse momenta $p_{T}$ in inclusive 2-, 3-, and 4-jet events are presented for several regions of the leading jet $p_{T}$ up to 4 TeV. For 3- and 4-jet scenarios, measurements of the minimum azimuthal angles between any two of the three or four leading $p_{T}$ jets are also presented. Jets are reconstructed using the infrared- and collinear-safe anti-$k_{T}$ clustering algorithm with a distance parameter $R=0.4$.
DOI: 10.17182/hepdata.86140.v1/t3
title: "Table 3" of "Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $\sqrt{s}= $ 13 TeV"

description: Normalized inclusive 2-jet cross section differential in $\Delta\phi_{1,2}$ for $400 &lt; p_{T}^{max} &lt; 500$ GeV
description: CERN-LHC. CMS. Azimuthal correlations between the two jets with the largest transverse momenta $p_{T}$ in inclusive 2-, 3-, and 4-jet events are presented for several regions of the leading jet $p_{T}$ up to 4 TeV. For 3- and 4-jet scenarios, measurements of the minimum azimuthal angles between any two of the three or four leading $p_{T}$ jets are also presented. Jets are reconstructed using the infrared- and collinear-safe anti-$k_{T}$ clustering algorithm with a distance parameter $R=0.4$.
DOI: 10.17182/hepdata.86140.v1/t4
title: "Table 4" of "Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $\sqrt{s}= $ 13 TeV"

description: Normalized inclusive 2-jet cross section differential in $\Delta\phi_{1,2}$ for $500 &lt; p_{T}^{max} &lt; 600$ GeV
description: CERN-LHC. CMS. Azimuthal correlations between the two jets with the largest transverse momenta $p_{T}$ in inclusive 2-, 3-, and 4-jet events are presented for several regions of the leading jet $p_{T}$ up to 4 TeV. For 3- and 4-jet scenarios, measurements of the minimum azimuthal angles between any two of the three or four leading $p_{T}$ jets are also presented. Jets are reconstructed using the infrared- and collinear-safe anti-$k_{T}$ clustering algorithm with a distance parameter $R=0.4$.
DOI: 10.17182/hepdata.86140.v1/t5
title: "Table 5" of "Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $\sqrt{s}= $ 13 TeV"

description: Normalized inclusive 2-jet cross section differential in $\Delta\phi_{1,2}$ for $600 &lt; p_{T}^{max} &lt; 700$ GeV
description: CERN-LHC. CMS. Azimuthal correlations between the two jets with the largest transverse momenta $p_{T}$ in inclusive 2-, 3-, and 4-jet events are presented for several regions of the leading jet $p_{T}$ up to 4 TeV. For 3- and 4-jet scenarios, measurements of the minimum azimuthal angles between any two of the three or four leading $p_{T}$ jets are also presented. Jets are reconstructed using the infrared- and collinear-safe anti-$k_{T}$ clustering algorithm with a distance parameter $R=0.4$.
DOI: 10.17182/hepdata.86140.v1/t6
title: "Table 6" of "Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $\sqrt{s}= $ 13 TeV"

description: Normalized inclusive 2-jet cross section differential in $\Delta\phi_{1,2}$ for $700 &lt; p_{T}^{max} &lt; 800$ GeV
description: CERN-LHC. CMS. Azimuthal correlations between the two jets with the largest transverse momenta $p_{T}$ in inclusive 2-, 3-, and 4-jet events are presented for several regions of the leading jet $p_{T}$ up to 4 TeV. For 3- and 4-jet scenarios, measurements of the minimum azimuthal angles between any two of the three or four leading $p_{T}$ jets are also presented. Jets are reconstructed using the infrared- and collinear-safe anti-$k_{T}$ clustering algorithm with a distance parameter $R=0.4$.
DOI: 10.17182/hepdata.86140.v1/t10
title: "Table 10" of "Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $\sqrt{s}= $ 13 TeV"

description: Normalized inclusive 3-jet cross section differential in $\Delta\phi_{1,2}$ for $200 &lt; p_{T}^{max} &lt; 300$ GeV
description: CERN-LHC. CMS. Azimuthal correlations between the two jets with the largest transverse momenta $p_{T}$ in inclusive 2-, 3-, and 4-jet events are presented for several regions of the leading jet $p_{T}$ up to 4 TeV. For 3- and 4-jet scenarios, measurements of the minimum azimuthal angles between any two of the three or four leading $p_{T}$ jets are also presented. Jets are reconstructed using the infrared- and collinear-safe anti-$k_{T}$ clustering algorithm with a distance parameter $R=0.4$.