cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.69985.v1/t16
title: "Table 16" of "Two and Three-Pion Quantum Statistics Correlations in Pb-Pb Collisions at sqrt(sNN)=2.76 TeV at the LHC"

description: r3 for 10-20% centrality.
description: CERN-LHC. The r3 variable is measured with charged pions in Pb-Pb collisions at the LHC. The following measurements are reported:
- C2 for same- and mixed-charge pairs versus qinv for six kT intervals and two centrality intervals.
- C2 fit parameters: lambda and Rch
- C3 and c3 for same- and mixed-charge triplets versus Q3 in two KT3 intervals and six centrality intervals.
- r3 versus Q3 in two different KT3 intervals and six different centrality intervals.
DOI: 10.17182/hepdata.69985.v1/t17
title: "Table 17" of "Two and Three-Pion Quantum Statistics Correlations in Pb-Pb Collisions at sqrt(sNN)=2.76 TeV at the LHC"

description: r3 for 20-30% centrality.
description: CERN-LHC. The r3 variable is measured with charged pions in Pb-Pb collisions at the LHC. The following measurements are reported:
- C2 for same- and mixed-charge pairs versus qinv for six kT intervals and two centrality intervals.
- C2 fit parameters: lambda and Rch
- C3 and c3 for same- and mixed-charge triplets versus Q3 in two KT3 intervals and six centrality intervals.
- r3 versus Q3 in two different KT3 intervals and six different centrality intervals.
DOI: 10.17182/hepdata.69985.v1/t18
title: "Table 18" of "Two and Three-Pion Quantum Statistics Correlations in Pb-Pb Collisions at sqrt(sNN)=2.76 TeV at the LHC"

description: r3 for 30-40% centrality.
description: CERN-LHC. The r3 variable is measured with charged pions in Pb-Pb collisions at the LHC. The following measurements are reported:
- C2 for same- and mixed-charge pairs versus qinv for six kT intervals and two centrality intervals.
- C2 fit parameters: lambda and Rch
- C3 and c3 for same- and mixed-charge triplets versus Q3 in two KT3 intervals and six centrality intervals.
- r3 versus Q3 in two different KT3 intervals and six different centrality intervals.
DOI: 10.17182/hepdata.69985.v1/t19
title: "Table 19" of "Two and Three-Pion Quantum Statistics Correlations in Pb-Pb Collisions at sqrt(sNN)=2.76 TeV at the LHC"

description: r3 for 40-50% centrality.
description: CERN-LHC. The r3 variable is measured with charged pions in Pb-Pb collisions at the LHC. The following measurements are reported:
- C2 for same- and mixed-charge pairs versus qinv for six kT intervals and two centrality intervals.
- C2 fit parameters: lambda and Rch
- C3 and c3 for same- and mixed-charge triplets versus Q3 in two KT3 intervals and six centrality intervals.
- r3 versus Q3 in two different KT3 intervals and six different centrality intervals.
DOI: 10.17182/hepdata.70010.v1/t1
title: "Table 1" of "Search for anomalous single top quark production in association with a photon in pp collisions at sqrt(s) = 8 TeV"

description: The expected and observed $95\%$ CL upper limits on the FCNC $tu\gamma$ and $tc\gamma$ cross sections times branching fraction, the anomalous couplings $\kappa_{tu\gamma}$ and $\kappa_{tc\gamma}$, and the corresponding branching fractions B($t \rightarrow u \gamma$)and B($t\rightarrow c \gamma$)at LO are given. The one and two standard deviation ($\sigma$) ranges on the LO expected limits are also presented.
description: CERN-LHC. The result of a search for flavor changing neutral currents (FCNC) through single top quark production in association with a photon is presented. The study is based on proton-proton collisions at a center-of-mass energy of 8 TeV using data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 19.8 inverse femtobarns. The search for t gamma events where t $\rightarrow$ Wb and W to $\mu$ $\nu$ is conducted in final states with a muon, a photon, at least one hadronic jet with at most one being consistent with originating from a bottom quark, and missing transverse momentum. No evidence of single top quark production in association with a photon through a FCNC is observed. Upper limits at the 95% confidence level are set on the tu gamma and tc gamma anomalous couplings and translated into upper limits on the branching fraction of the FCNC top quark decays: B(t $\rightarrow u \gamma$) &lt; 1.3$\times$10$^{-4}$ and B(t $\rightarrow c \gamma$) &lt; 1.7$\times$10$^{-3}$. Upper limits are also set on the cross section of associated t gamma production in a restricted phase-space region. These are the most stringent limits currently available.
DOI: 10.17182/hepdata.70010.v1/t2
title: "Table 2" of "Search for anomalous single top quark production in association with a photon in pp collisions at sqrt(s) = 8 TeV"

description: The expected and observed $95\%$ CL upper limits on the FCNC $tu\gamma$ and $tc\gamma$ cross sections times branching fraction, the anomalous couplings $\kappa_{tu\gamma}$ and $\kappa_{tc\gamma}$, and the corresponding branching fractions B($t \rightarrow u \gamma$)and B($t\rightarrow c \gamma$)at NLO are given. The one and two standard deviation ($\sigma$) ranges on the NLO expected limits are also presented.
description: CERN-LHC. The result of a search for flavor changing neutral currents (FCNC) through single top quark production in association with a photon is presented. The study is based on proton-proton collisions at a center-of-mass energy of 8 TeV using data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 19.8 inverse femtobarns. The search for t gamma events where t $\rightarrow$ Wb and W to $\mu$ $\nu$ is conducted in final states with a muon, a photon, at least one hadronic jet with at most one being consistent with originating from a bottom quark, and missing transverse momentum. No evidence of single top quark production in association with a photon through a FCNC is observed. Upper limits at the 95% confidence level are set on the tu gamma and tc gamma anomalous couplings and translated into upper limits on the branching fraction of the FCNC top quark decays: B(t $\rightarrow u \gamma$) &lt; 1.3$\times$10$^{-4}$ and B(t $\rightarrow c \gamma$) &lt; 1.7$\times$10$^{-3}$. Upper limits are also set on the cross section of associated t gamma production in a restricted phase-space region. These are the most stringent limits currently available.
DOI: 10.17182/hepdata.70010.v1/t3
title: "Table 3" of "Search for anomalous single top quark production in association with a photon in pp collisions at sqrt(s) = 8 TeV"

description: Upper limits on the signal cross sections are also determined for a restricted phase-space region
in which the detector is fully efficient. This removes the need to extrapolate to phase-space
regions where the analysis has little or no sensitivity. The fiducial region is defined as:.
description: CERN-LHC. The result of a search for flavor changing neutral currents (FCNC) through single top quark production in association with a photon is presented. The study is based on proton-proton collisions at a center-of-mass energy of 8 TeV using data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 19.8 inverse femtobarns. The search for t gamma events where t $\rightarrow$ Wb and W to $\mu$ $\nu$ is conducted in final states with a muon, a photon, at least one hadronic jet with at most one being consistent with originating from a bottom quark, and missing transverse momentum. No evidence of single top quark production in association with a photon through a FCNC is observed. Upper limits at the 95% confidence level are set on the tu gamma and tc gamma anomalous couplings and translated into upper limits on the branching fraction of the FCNC top quark decays: B(t $\rightarrow u \gamma$) &lt; 1.3$\times$10$^{-4}$ and B(t $\rightarrow c \gamma$) &lt; 1.7$\times$10$^{-3}$. Upper limits are also set on the cross section of associated t gamma production in a restricted phase-space region. These are the most stringent limits currently available.
DOI: 10.17182/hepdata.70010.v1/t4
title: "Table 4" of "Search for anomalous single top quark production in association with a photon in pp collisions at sqrt(s) = 8 TeV"

description: For the tu$\gamma$ signal channel, the total number of observed selected events in the data
(N$_{obs}$), the SM expectations (N$_{SM}$), the efficiencies ($\epsilon$), and the upper limits on the cross sections
$\sigma_{fid}$ at the 95% CL in the fiducial region, without and with a requirement on the presence of a
single accompanying b jet.
description: CERN-LHC. The result of a search for flavor changing neutral currents (FCNC) through single top quark production in association with a photon is presented. The study is based on proton-proton collisions at a center-of-mass energy of 8 TeV using data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 19.8 inverse femtobarns. The search for t gamma events where t $\rightarrow$ Wb and W to $\mu$ $\nu$ is conducted in final states with a muon, a photon, at least one hadronic jet with at most one being consistent with originating from a bottom quark, and missing transverse momentum. No evidence of single top quark production in association with a photon through a FCNC is observed. Upper limits at the 95% confidence level are set on the tu gamma and tc gamma anomalous couplings and translated into upper limits on the branching fraction of the FCNC top quark decays: B(t $\rightarrow u \gamma$) &lt; 1.3$\times$10$^{-4}$ and B(t $\rightarrow c \gamma$) &lt; 1.7$\times$10$^{-3}$. Upper limits are also set on the cross section of associated t gamma production in a restricted phase-space region. These are the most stringent limits currently available.
DOI: 10.17182/hepdata.70010.v1/t5
title: "Table 5" of "Search for anomalous single top quark production in association with a photon in pp collisions at sqrt(s) = 8 TeV"

description: For the tc$\gamma$ signal channel, the total number of observed selected events in the data
(N$_{obs}$), the SM expectations (N$_{SM}$), the efficiencies ($\epsilon$), and the upper limits on the cross sections
$\sigma_{fid}$ at the 95% CL in the fiducial region, without and with a requirement on the presence of a
single accompanying b jet.
description: CERN-LHC. The result of a search for flavor changing neutral currents (FCNC) through single top quark production in association with a photon is presented. The study is based on proton-proton collisions at a center-of-mass energy of 8 TeV using data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 19.8 inverse femtobarns. The search for t gamma events where t $\rightarrow$ Wb and W to $\mu$ $\nu$ is conducted in final states with a muon, a photon, at least one hadronic jet with at most one being consistent with originating from a bottom quark, and missing transverse momentum. No evidence of single top quark production in association with a photon through a FCNC is observed. Upper limits at the 95% confidence level are set on the tu gamma and tc gamma anomalous couplings and translated into upper limits on the branching fraction of the FCNC top quark decays: B(t $\rightarrow u \gamma$) &lt; 1.3$\times$10$^{-4}$ and B(t $\rightarrow c \gamma$) &lt; 1.7$\times$10$^{-3}$. Upper limits are also set on the cross section of associated t gamma production in a restricted phase-space region. These are the most stringent limits currently available.
DOI: 10.17182/hepdata.70017.v1/t1
title: "Table 1" of "Study of $\chi_{b}$ meson production in pp collisions at $\sqrt{s}=7$ and 8TeV and observation of the decay $\chi_{b}\rightarrow \Upsilon(3S) \gamma$"

description: Fractions $R_{\Upsilon(1S)}^{\chi_{b}(mP)}$ in bins of $p_{\mathrm{T}}^{\Upsilon}$, measured for data collected at $\sqrt{s}= 7$ TeV.
description: CERN-LHC. A study of $\chi_{b}$ meson production at LHCb is performed on proton-proton collision data, corresponding to 3.0 fb$^{-1}$ of integrated luminosity collected at centre-of-mass energies $\sqrt{s}=$7 and 8 TeV. The fraction of $\Upsilon(nS)$ mesons originating from $\chi_{b}$ decays is measured as a function of the $\Upsilon$ transverse momentum in the rapidity range $2.0 &lt; y^{\Upsilon} &lt; 4.5$. The radiative transition of the $\chi_{b}(3P)$ meson to $\Upsilon(3S)$ is observed for the first time. The $\chi_{b1}(3P)$ mass is determined to be $m_{\chi_{b1}(3P)} = 10511.3 \pm 1.7 \pm 2.5$ MeV/$c^2$, where the first uncertainty is statistical and the second is systematic.
DOI: 10.17182/hepdata.70017.v1/t2
title: "Table 2" of "Study of $\chi_{b}$ meson production in pp collisions at $\sqrt{s}=7$ and 8TeV and observation of the decay $\chi_{b}\rightarrow \Upsilon(3S) \gamma$"

description: Fractions $R_{\Upsilon(2S)}^{\chi_{b}(mP)}$ in bins of $p_{\mathrm{T}}^{\Upsilon}$, measured for data collected at $\sqrt{s}= 7$ TeV.
description: CERN-LHC. A study of $\chi_{b}$ meson production at LHCb is performed on proton-proton collision data, corresponding to 3.0 fb$^{-1}$ of integrated luminosity collected at centre-of-mass energies $\sqrt{s}=$7 and 8 TeV. The fraction of $\Upsilon(nS)$ mesons originating from $\chi_{b}$ decays is measured as a function of the $\Upsilon$ transverse momentum in the rapidity range $2.0 &lt; y^{\Upsilon} &lt; 4.5$. The radiative transition of the $\chi_{b}(3P)$ meson to $\Upsilon(3S)$ is observed for the first time. The $\chi_{b1}(3P)$ mass is determined to be $m_{\chi_{b1}(3P)} = 10511.3 \pm 1.7 \pm 2.5$ MeV/$c^2$, where the first uncertainty is statistical and the second is systematic.
DOI: 10.17182/hepdata.70017.v1/t3
title: "Table 3" of "Study of $\chi_{b}$ meson production in pp collisions at $\sqrt{s}=7$ and 8TeV and observation of the decay $\chi_{b}\rightarrow \Upsilon(3S) \gamma$"

description: Fractions $R_{\Upsilon(3S)}^{\chi_{b}(mP)}$ in bins of $p_{\mathrm{T}}^{\Upsilon}$, measured for data collected at $\sqrt{s}= 7$ TeV.
description: CERN-LHC. A study of $\chi_{b}$ meson production at LHCb is performed on proton-proton collision data, corresponding to 3.0 fb$^{-1}$ of integrated luminosity collected at centre-of-mass energies $\sqrt{s}=$7 and 8 TeV. The fraction of $\Upsilon(nS)$ mesons originating from $\chi_{b}$ decays is measured as a function of the $\Upsilon$ transverse momentum in the rapidity range $2.0 &lt; y^{\Upsilon} &lt; 4.5$. The radiative transition of the $\chi_{b}(3P)$ meson to $\Upsilon(3S)$ is observed for the first time. The $\chi_{b1}(3P)$ mass is determined to be $m_{\chi_{b1}(3P)} = 10511.3 \pm 1.7 \pm 2.5$ MeV/$c^2$, where the first uncertainty is statistical and the second is systematic.
DOI: 10.17182/hepdata.70017.v1/t5
title: "Table 5" of "Study of $\chi_{b}$ meson production in pp collisions at $\sqrt{s}=7$ and 8TeV and observation of the decay $\chi_{b}\rightarrow \Upsilon(3S) \gamma$"

description: Fractions $R_{\Upsilon(1S)}^{\chi_{b}(mP)}$ in bins of $p_{\mathrm{T}}^{\Upsilon}$, measured for data collected at $\sqrt{s}= 8$ TeV.
description: CERN-LHC. A study of $\chi_{b}$ meson production at LHCb is performed on proton-proton collision data, corresponding to 3.0 fb$^{-1}$ of integrated luminosity collected at centre-of-mass energies $\sqrt{s}=$7 and 8 TeV. The fraction of $\Upsilon(nS)$ mesons originating from $\chi_{b}$ decays is measured as a function of the $\Upsilon$ transverse momentum in the rapidity range $2.0 &lt; y^{\Upsilon} &lt; 4.5$. The radiative transition of the $\chi_{b}(3P)$ meson to $\Upsilon(3S)$ is observed for the first time. The $\chi_{b1}(3P)$ mass is determined to be $m_{\chi_{b1}(3P)} = 10511.3 \pm 1.7 \pm 2.5$ MeV/$c^2$, where the first uncertainty is statistical and the second is systematic.
DOI: 10.17182/hepdata.70017.v1/t6
title: "Table 6" of "Study of $\chi_{b}$ meson production in pp collisions at $\sqrt{s}=7$ and 8TeV and observation of the decay $\chi_{b}\rightarrow \Upsilon(3S) \gamma$"

description: Fractions $R_{\Upsilon(1S)}^{\chi_{b}(mP)}$ in bins of $p_{\mathrm{T}}^{\Upsilon}$, measured for data collected at $\sqrt{s}= 8$ TeV.
description: CERN-LHC. A study of $\chi_{b}$ meson production at LHCb is performed on proton-proton collision data, corresponding to 3.0 fb$^{-1}$ of integrated luminosity collected at centre-of-mass energies $\sqrt{s}=$7 and 8 TeV. The fraction of $\Upsilon(nS)$ mesons originating from $\chi_{b}$ decays is measured as a function of the $\Upsilon$ transverse momentum in the rapidity range $2.0 &lt; y^{\Upsilon} &lt; 4.5$. The radiative transition of the $\chi_{b}(3P)$ meson to $\Upsilon(3S)$ is observed for the first time. The $\chi_{b1}(3P)$ mass is determined to be $m_{\chi_{b1}(3P)} = 10511.3 \pm 1.7 \pm 2.5$ MeV/$c^2$, where the first uncertainty is statistical and the second is systematic.
DOI: 10.17182/hepdata.70017.v1/t4
title: "Table 4" of "Study of $\chi_{b}$ meson production in pp collisions at $\sqrt{s}=7$ and 8TeV and observation of the decay $\chi_{b}\rightarrow \Upsilon(3S) \gamma$"

description: Fractions $R_{\Upsilon(1S)}^{\chi_{b}(mP)}$ in bins of $p_{\mathrm{T}}^{\Upsilon}$, measured for data collected at $\sqrt{s}= 8$ TeV.
description: CERN-LHC. A study of $\chi_{b}$ meson production at LHCb is performed on proton-proton collision data, corresponding to 3.0 fb$^{-1}$ of integrated luminosity collected at centre-of-mass energies $\sqrt{s}=$7 and 8 TeV. The fraction of $\Upsilon(nS)$ mesons originating from $\chi_{b}$ decays is measured as a function of the $\Upsilon$ transverse momentum in the rapidity range $2.0 &lt; y^{\Upsilon} &lt; 4.5$. The radiative transition of the $\chi_{b}(3P)$ meson to $\Upsilon(3S)$ is observed for the first time. The $\chi_{b1}(3P)$ mass is determined to be $m_{\chi_{b1}(3P)} = 10511.3 \pm 1.7 \pm 2.5$ MeV/$c^2$, where the first uncertainty is statistical and the second is systematic.
DOI: 10.17182/hepdata.70048.v2/t1
title: "Table 1" of "Measurement of forward $J/\psi$ production cross-sections in $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Double differential cross-section for prompt $J/\psi$ mesons as a function of $p_\perp$ in bins of $y$. The first uncertainties are statistical, the second are the correlated systematic
uncertainties shared between bins and the last are the uncorrelated systematic uncertainties.
description: CERN-LHC. The production of $J/\psi$ mesons in proton-proton collisions at a centre-of-mass energy of $\sqrt{s} = 13$ TeV is studied with the LHCb detector. 
Cross-section measurements are performed as a function of the transverse momentum $p_\perp$ and the rapidity $y$ of the $J/\psi$ meson in the region $p_\perp &lt; 14$ GeV/$c$ and $2.0 &lt; y &lt; 4.5$, for both prompt $J/\psi$ mesons and $J/\psi$ mesons from $b$-hadron decays. 
The production cross-sections integrated over the kinematic coverage are $15.30 \pm 0.03 \pm 0.86$ $\mu$b for prompt $J/\psi$ and $2.34 \pm 0.01 \pm 0.13$ $\mu$b for $J/\psi$ from $b$-hadron decays, assuming zero polarization of the $J/\psi$ meson. 
The first uncertainties are statistical and the second systematic. 
The cross-section reported for $J/\psi$ mesons from $b$-hadron decays is used to extrapolate to a total $b\bar{b}$ cross-section.
The ratios of the cross-sections with respect to $\sqrt{s} = 8$ TeV are also determined.
DOI: 10.17182/hepdata.70048.v2/t2
title: "Table 2" of "Measurement of forward $J/\psi$ production cross-sections in $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Double differential cross-section for $J/\psi$-from-$b$ mesons as a function of $p_\perp$ in bins of $y$. The first uncertainties are statistical, the second are the correlated systematic uncertainties shared between bins and the last are the uncorrelated systematic uncertainties.
description: CERN-LHC. The production of $J/\psi$ mesons in proton-proton collisions at a centre-of-mass energy of $\sqrt{s} = 13$ TeV is studied with the LHCb detector. 
Cross-section measurements are performed as a function of the transverse momentum $p_\perp$ and the rapidity $y$ of the $J/\psi$ meson in the region $p_\perp &lt; 14$ GeV/$c$ and $2.0 &lt; y &lt; 4.5$, for both prompt $J/\psi$ mesons and $J/\psi$ mesons from $b$-hadron decays. 
The production cross-sections integrated over the kinematic coverage are $15.30 \pm 0.03 \pm 0.86$ $\mu$b for prompt $J/\psi$ and $2.34 \pm 0.01 \pm 0.13$ $\mu$b for $J/\psi$ from $b$-hadron decays, assuming zero polarization of the $J/\psi$ meson. 
The first uncertainties are statistical and the second systematic. 
The cross-section reported for $J/\psi$ mesons from $b$-hadron decays is used to extrapolate to a total $b\bar{b}$ cross-section.
The ratios of the cross-sections with respect to $\sqrt{s} = 8$ TeV are also determined.
DOI: 10.17182/hepdata.70048.v2/t3
title: "Table 3" of "Measurement of forward $J/\psi$ production cross-sections in $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The fraction of $J/\psi$-from-$b$ mesons (in %) in bins of the $J/\psi$ $p_\perp$ and $y$. The uncertainties are statistical only. The systematic uncertainties are negligible.
description: CERN-LHC. The production of $J/\psi$ mesons in proton-proton collisions at a centre-of-mass energy of $\sqrt{s} = 13$ TeV is studied with the LHCb detector. 
Cross-section measurements are performed as a function of the transverse momentum $p_\perp$ and the rapidity $y$ of the $J/\psi$ meson in the region $p_\perp &lt; 14$ GeV/$c$ and $2.0 &lt; y &lt; 4.5$, for both prompt $J/\psi$ mesons and $J/\psi$ mesons from $b$-hadron decays. 
The production cross-sections integrated over the kinematic coverage are $15.30 \pm 0.03 \pm 0.86$ $\mu$b for prompt $J/\psi$ and $2.34 \pm 0.01 \pm 0.13$ $\mu$b for $J/\psi$ from $b$-hadron decays, assuming zero polarization of the $J/\psi$ meson. 
The first uncertainties are statistical and the second systematic. 
The cross-section reported for $J/\psi$ mesons from $b$-hadron decays is used to extrapolate to a total $b\bar{b}$ cross-section.
The ratios of the cross-sections with respect to $\sqrt{s} = 8$ TeV are also determined.
DOI: 10.17182/hepdata.70048.v2/t4
title: "Table 4" of "Measurement of forward $J/\psi$ production cross-sections in $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Differential cross-sections as a function of $p_\perp$ integrated over $y$ for prompt $J/\psi$ mesons. The first uncertainties are statistical and the second (third) are uncorrelated (correlated) systematic uncertainties amongst bins.
description: CERN-LHC. The production of $J/\psi$ mesons in proton-proton collisions at a centre-of-mass energy of $\sqrt{s} = 13$ TeV is studied with the LHCb detector. 
Cross-section measurements are performed as a function of the transverse momentum $p_\perp$ and the rapidity $y$ of the $J/\psi$ meson in the region $p_\perp &lt; 14$ GeV/$c$ and $2.0 &lt; y &lt; 4.5$, for both prompt $J/\psi$ mesons and $J/\psi$ mesons from $b$-hadron decays. 
The production cross-sections integrated over the kinematic coverage are $15.30 \pm 0.03 \pm 0.86$ $\mu$b for prompt $J/\psi$ and $2.34 \pm 0.01 \pm 0.13$ $\mu$b for $J/\psi$ from $b$-hadron decays, assuming zero polarization of the $J/\psi$ meson. 
The first uncertainties are statistical and the second systematic. 
The cross-section reported for $J/\psi$ mesons from $b$-hadron decays is used to extrapolate to a total $b\bar{b}$ cross-section.
The ratios of the cross-sections with respect to $\sqrt{s} = 8$ TeV are also determined.