cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.66915.v1/t45
title: "Table 45" of "Observation of double charm production involving open charm in pp collisions at $\sqrt{s}$=7 TeV"

description: Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^+ X \right)}{d m_{D^0 D^+} }$ for $2
description: The production of $J/\psi$ mesons accompanied by open charm, and of pairs of open charm hadrons
are observed in pp collisions at a centre-of-mass energy of 7 TeV using an integrated luminosity of 
355 pb$^{-1}$ collected with the LHCb detector. Model independent measurements of absolute
cross-sections are given together with ratios to the measured $J/\psi$ and open charm cross-sections. 
The properties of these events are studied and compared to theoretical predictions.
DOI: 10.17182/hepdata.66915.v1/t46
title: "Table 46" of "Observation of double charm production involving open charm in pp collisions at $\sqrt{s}$=7 TeV"

description: Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{D}^0 X \right)}{d m_{D^0 \bar{D}^0} }$ for $2
description: The production of $J/\psi$ mesons accompanied by open charm, and of pairs of open charm hadrons
are observed in pp collisions at a centre-of-mass energy of 7 TeV using an integrated luminosity of 
355 pb$^{-1}$ collected with the LHCb detector. Model independent measurements of absolute
cross-sections are given together with ratios to the measured $J/\psi$ and open charm cross-sections. 
The properties of these events are studied and compared to theoretical predictions.
DOI: 10.17182/hepdata.66915.v1/t47
title: "Table 47" of "Observation of double charm production involving open charm in pp collisions at $\sqrt{s}$=7 TeV"

description: Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^- X \right)}{d m_{D^0 D^-} }$ for $2
description: The production of $J/\psi$ mesons accompanied by open charm, and of pairs of open charm hadrons
are observed in pp collisions at a centre-of-mass energy of 7 TeV using an integrated luminosity of 
355 pb$^{-1}$ collected with the LHCb detector. Model independent measurements of absolute
cross-sections are given together with ratios to the measured $J/\psi$ and open charm cross-sections. 
The properties of these events are studied and compared to theoretical predictions.
DOI: 10.17182/hepdata.66915.v1/t48
title: "Table 48" of "Observation of double charm production involving open charm in pp collisions at $\sqrt{s}$=7 TeV"

description: Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D_s^- X \right)}{d m_{D^0 D_s^-} }$ for $2
description: The production of $J/\psi$ mesons accompanied by open charm, and of pairs of open charm hadrons
are observed in pp collisions at a centre-of-mass energy of 7 TeV using an integrated luminosity of 
355 pb$^{-1}$ collected with the LHCb detector. Model independent measurements of absolute
cross-sections are given together with ratios to the measured $J/\psi$ and open charm cross-sections. 
The properties of these events are studied and compared to theoretical predictions.
DOI: 10.17182/hepdata.66915.v1/t49
title: "Table 49" of "Observation of double charm production involving open charm in pp collisions at $\sqrt{s}$=7 TeV"

description: Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{\Lambda}_c^- X \right)}{d m_{D^0 D_s^-} }$ for $2
description: The production of $J/\psi$ mesons accompanied by open charm, and of pairs of open charm hadrons
are observed in pp collisions at a centre-of-mass energy of 7 TeV using an integrated luminosity of 
355 pb$^{-1}$ collected with the LHCb detector. Model independent measurements of absolute
cross-sections are given together with ratios to the measured $J/\psi$ and open charm cross-sections. 
The properties of these events are studied and compared to theoretical predictions.
DOI: 10.17182/hepdata.66915.v1/t50
title: "Table 50" of "Observation of double charm production involving open charm in pp collisions at $\sqrt{s}$=7 TeV"

description: Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D^- X \right)}{d m_{D^+ D^-} }$ for $2
description: The production of $J/\psi$ mesons accompanied by open charm, and of pairs of open charm hadrons
are observed in pp collisions at a centre-of-mass energy of 7 TeV using an integrated luminosity of 
355 pb$^{-1}$ collected with the LHCb detector. Model independent measurements of absolute
cross-sections are given together with ratios to the measured $J/\psi$ and open charm cross-sections. 
The properties of these events are studied and compared to theoretical predictions.
DOI: 10.17182/hepdata.66915.v1/t51
title: "Table 51" of "Observation of double charm production involving open charm in pp collisions at $\sqrt{s}$=7 TeV"

description: Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D_s^- X \right)}{d m_{D^+ D_s^-} }$ for $2
description: The production of $J/\psi$ mesons accompanied by open charm, and of pairs of open charm hadrons
are observed in pp collisions at a centre-of-mass energy of 7 TeV using an integrated luminosity of 
355 pb$^{-1}$ collected with the LHCb detector. Model independent measurements of absolute
cross-sections are given together with ratios to the measured $J/\psi$ and open charm cross-sections. 
The properties of these events are studied and compared to theoretical predictions.
DOI: 10.17182/hepdata.66915.v1/t52
title: "Table 52" of "Observation of double charm production involving open charm in pp collisions at $\sqrt{s}$=7 TeV"

description: Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ \bar{\Lambda}_c^- X \right)}{d m_{D^+ \bar{\Lambda}_c^-} }$ for $2
description: The production of $J/\psi$ mesons accompanied by open charm, and of pairs of open charm hadrons
are observed in pp collisions at a centre-of-mass energy of 7 TeV using an integrated luminosity of 
355 pb$^{-1}$ collected with the LHCb detector. Model independent measurements of absolute
cross-sections are given together with ratios to the measured $J/\psi$ and open charm cross-sections. 
The properties of these events are studied and compared to theoretical predictions.
DOI: 10.17182/hepdata.66916.v1/t1
title: "Table 1" of "Centrality determination of Pb-Pb collisions at sqrt(sNN) = 2.76 TeV with ALICE"

description: $N_\mathrm{part}$ for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV with the corresponding uncertainties derived from a Glauber calculation. The ${\langle N_\mathrm{part}^{\rm data} \rangle}$ are calculated from the NBD-Glauber fit to the VZERO amplitude, while the ${\langle N_\mathrm{part}^{\rm geo} \rangle}$ are obtained by slicing the impact parameter distribution. ${\langle N_\mathrm{part}^{\rm data} \rangle}$ is also calculated for two variations of the AP, i.e. moving it to 91 % (${\langle N_\mathrm{part}^{\rm data +} \rangle}$) and to 89 % (${\langle N_\mathrm{part}^{\rm data +} \rangle}$) respectively. The last three columns report the discrepancies between ${\langle N_\mathrm{part}^{\rm geo} \rangle}$ and ${\langle N_\mathrm{part}^{\rm data} \rangle}$ and ${\langle N_\mathrm{part}^{\rm data} \rangle}$ with the uncertainty of the AP.
description: CERN-LHC. This publication describes the methods used to measure the centrality of inelastic Pb-Pb collisions at a center-of-mass energy of 2.76 TeV per colliding nucleon pair with ALICE. The centrality is a key parameter in the study of the properties of QCD matter at extreme temperature and energy density, because it is directly related to the initial overlap region of the colliding nuclei. Geometrical properties of the collision, such as the number of participating nucleons and number of binary nucleon-nucleon collisions, are deduced from a Glauber model with a sharp impact parameter selection, and shown to be consistent with those extracted from the data. The centrality determination provides a tool to compare ALICE measurements with those of other experiments and with theoretical calculations.
DOI: 10.17182/hepdata.66916.v1/t2
title: "Table 2" of "Centrality determination of Pb-Pb collisions at sqrt(sNN) = 2.76 TeV with ALICE"

description: Same as Table A.1 for $N_\mathrm{coll}$.
description: CERN-LHC. This publication describes the methods used to measure the centrality of inelastic Pb-Pb collisions at a center-of-mass energy of 2.76 TeV per colliding nucleon pair with ALICE. The centrality is a key parameter in the study of the properties of QCD matter at extreme temperature and energy density, because it is directly related to the initial overlap region of the colliding nuclei. Geometrical properties of the collision, such as the number of participating nucleons and number of binary nucleon-nucleon collisions, are deduced from a Glauber model with a sharp impact parameter selection, and shown to be consistent with those extracted from the data. The centrality determination provides a tool to compare ALICE measurements with those of other experiments and with theoretical calculations.
DOI: 10.17182/hepdata.66916.v1/t3
title: "Table 3" of "Centrality determination of Pb-Pb collisions at sqrt(sNN) = 2.76 TeV with ALICE"

description: Same as Table A.1 for $T_\mathrm{AA}$.
description: CERN-LHC. This publication describes the methods used to measure the centrality of inelastic Pb-Pb collisions at a center-of-mass energy of 2.76 TeV per colliding nucleon pair with ALICE. The centrality is a key parameter in the study of the properties of QCD matter at extreme temperature and energy density, because it is directly related to the initial overlap region of the colliding nuclei. Geometrical properties of the collision, such as the number of participating nucleons and number of binary nucleon-nucleon collisions, are deduced from a Glauber model with a sharp impact parameter selection, and shown to be consistent with those extracted from the data. The centrality determination provides a tool to compare ALICE measurements with those of other experiments and with theoretical calculations.
DOI: 10.17182/hepdata.66916.v1/t4
title: "Table 4" of "Centrality determination of Pb-Pb collisions at sqrt(sNN) = 2.76 TeV with ALICE"

description: Same as above with bigger centrality classes.
description: CERN-LHC. This publication describes the methods used to measure the centrality of inelastic Pb-Pb collisions at a center-of-mass energy of 2.76 TeV per colliding nucleon pair with ALICE. The centrality is a key parameter in the study of the properties of QCD matter at extreme temperature and energy density, because it is directly related to the initial overlap region of the colliding nuclei. Geometrical properties of the collision, such as the number of participating nucleons and number of binary nucleon-nucleon collisions, are deduced from a Glauber model with a sharp impact parameter selection, and shown to be consistent with those extracted from the data. The centrality determination provides a tool to compare ALICE measurements with those of other experiments and with theoretical calculations.
DOI: 10.17182/hepdata.66916.v1/t5
title: "Table 5" of "Centrality determination of Pb-Pb collisions at sqrt(sNN) = 2.76 TeV with ALICE"

description: Same as above with bigger centrality classes.
description: CERN-LHC. This publication describes the methods used to measure the centrality of inelastic Pb-Pb collisions at a center-of-mass energy of 2.76 TeV per colliding nucleon pair with ALICE. The centrality is a key parameter in the study of the properties of QCD matter at extreme temperature and energy density, because it is directly related to the initial overlap region of the colliding nuclei. Geometrical properties of the collision, such as the number of participating nucleons and number of binary nucleon-nucleon collisions, are deduced from a Glauber model with a sharp impact parameter selection, and shown to be consistent with those extracted from the data. The centrality determination provides a tool to compare ALICE measurements with those of other experiments and with theoretical calculations.
DOI: 10.17182/hepdata.66916.v1/t6
title: "Table 6" of "Centrality determination of Pb-Pb collisions at sqrt(sNN) = 2.76 TeV with ALICE"

description: Same as above with bigger centrality classes.
description: CERN-LHC. This publication describes the methods used to measure the centrality of inelastic Pb-Pb collisions at a center-of-mass energy of 2.76 TeV per colliding nucleon pair with ALICE. The centrality is a key parameter in the study of the properties of QCD matter at extreme temperature and energy density, because it is directly related to the initial overlap region of the colliding nuclei. Geometrical properties of the collision, such as the number of participating nucleons and number of binary nucleon-nucleon collisions, are deduced from a Glauber model with a sharp impact parameter selection, and shown to be consistent with those extracted from the data. The centrality determination provides a tool to compare ALICE measurements with those of other experiments and with theoretical calculations.
DOI: 10.17182/hepdata.66933.v1/t1
title: "Table 1" of "Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: The estimated backgrounds, observed event yields, and expected number of signal events for the leptoquark search. For the simulation-based entries, the statistical and systematic uncertainties are shown separately, in that order.
description: CERN-LHC. Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at $\sqrt{s}$ = 8 TeV using 19.7 inverse femtobarns of data collected with the CMS detector. The leptoquark search considers each leptoquark decaying to a tau lepton and a bottom quark, or each top squark decaying via an R-parity violating coupling $\lambda^{\prime}_{333}$ to a tau lepton and a bottom quark. The top squark search considers top squarks undergoing a chargino-mediated decay involving the R-parity violating coupling $\lambda^{\prime}_{3jk}$, each decaying to a tau lepton, a bottom quark, and two light quarks.

Errata:
17 JUN 2015: Fixed one typo from the paper: systematic uncertainties on the $M_{\text{LQ}}=700$ signal in Table 1 were a factor of ten too high.
17 JUN 2015: Fixed one typo just in the HepData entry: the $M_{\widetilde{\text{t}}}$ masses listed in Table 2 were incorrect.

Selection:
- one e/$\mu$ ($\ell$)
- e: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 1.444 or 1.56 &lt; |$\eta$| &lt; 2.5
- $\mu$: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.1
- one $\tau_{\text{h}}$ (hadronically decaying tau lepton): $p_\text{T}$ &gt; 50 GeV, |$\eta$| &lt; 2.3
- $\Delta$R($\ell$,$\tau_{\text{h}}$) &gt; 0.5; vertex($\ell$) = vertex($\tau_{\text{h}}$); charge($\ell$) != charge($\tau_{\text{h}}$)
- veto opposite sign $\mu$/e
- veto opposite sign e/$\mu$
- jet: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.4
- $N_{\text{jet}}$ $\geq$ 2
- $N_{\text{b-jet}}$ $\geq$ 1
- $\Delta$R(jet,$\ell$) &gt; 0.5; $\Delta$R(jet,$\tau_{\text{h}}$) &gt; 0.5

Leptoquark search final selection:
- M($\tau_{\text{h}}$,jet) &gt; 250 GeV
(pairing is chosen that minimizes |M($\tau_{\text{h}}$,jet i) - M($\ell$,jet j)|)
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet)

Top squark search final selection:
- $N_\text{jet}$ $\geq$ 5
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet 1) + $p_\text{T}$(jet 2) + $p_\text{T}$(jet 3) + $p_\text{T}$(jet 4).
DOI: 10.17182/hepdata.66933.v1/t2
title: "Table 2" of "Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: The estimated backgrounds, observed event yields, and expected number of signal events for the top squark search. For the simulation-based entries, the statistical and systematic uncertainties are shown separately, in that order.
description: CERN-LHC. Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at $\sqrt{s}$ = 8 TeV using 19.7 inverse femtobarns of data collected with the CMS detector. The leptoquark search considers each leptoquark decaying to a tau lepton and a bottom quark, or each top squark decaying via an R-parity violating coupling $\lambda^{\prime}_{333}$ to a tau lepton and a bottom quark. The top squark search considers top squarks undergoing a chargino-mediated decay involving the R-parity violating coupling $\lambda^{\prime}_{3jk}$, each decaying to a tau lepton, a bottom quark, and two light quarks.

Errata:
17 JUN 2015: Fixed one typo from the paper: systematic uncertainties on the $M_{\text{LQ}}=700$ signal in Table 1 were a factor of ten too high.
17 JUN 2015: Fixed one typo just in the HepData entry: the $M_{\widetilde{\text{t}}}$ masses listed in Table 2 were incorrect.

Selection:
- one e/$\mu$ ($\ell$)
- e: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 1.444 or 1.56 &lt; |$\eta$| &lt; 2.5
- $\mu$: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.1
- one $\tau_{\text{h}}$ (hadronically decaying tau lepton): $p_\text{T}$ &gt; 50 GeV, |$\eta$| &lt; 2.3
- $\Delta$R($\ell$,$\tau_{\text{h}}$) &gt; 0.5; vertex($\ell$) = vertex($\tau_{\text{h}}$); charge($\ell$) != charge($\tau_{\text{h}}$)
- veto opposite sign $\mu$/e
- veto opposite sign e/$\mu$
- jet: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.4
- $N_{\text{jet}}$ $\geq$ 2
- $N_{\text{b-jet}}$ $\geq$ 1
- $\Delta$R(jet,$\ell$) &gt; 0.5; $\Delta$R(jet,$\tau_{\text{h}}$) &gt; 0.5

Leptoquark search final selection:
- M($\tau_{\text{h}}$,jet) &gt; 250 GeV
(pairing is chosen that minimizes |M($\tau_{\text{h}}$,jet i) - M($\ell$,jet j)|)
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet)

Top squark search final selection:
- $N_\text{jet}$ $\geq$ 5
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet 1) + $p_\text{T}$(jet 2) + $p_\text{T}$(jet 3) + $p_\text{T}$(jet 4).
DOI: 10.17182/hepdata.66933.v1/t3
title: "Table 3" of "Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: Selection efficiencies in % for the signal in the leptoquark search, estimated from the simulation.
description: CERN-LHC. Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at $\sqrt{s}$ = 8 TeV using 19.7 inverse femtobarns of data collected with the CMS detector. The leptoquark search considers each leptoquark decaying to a tau lepton and a bottom quark, or each top squark decaying via an R-parity violating coupling $\lambda^{\prime}_{333}$ to a tau lepton and a bottom quark. The top squark search considers top squarks undergoing a chargino-mediated decay involving the R-parity violating coupling $\lambda^{\prime}_{3jk}$, each decaying to a tau lepton, a bottom quark, and two light quarks.

Errata:
17 JUN 2015: Fixed one typo from the paper: systematic uncertainties on the $M_{\text{LQ}}=700$ signal in Table 1 were a factor of ten too high.
17 JUN 2015: Fixed one typo just in the HepData entry: the $M_{\widetilde{\text{t}}}$ masses listed in Table 2 were incorrect.

Selection:
- one e/$\mu$ ($\ell$)
- e: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 1.444 or 1.56 &lt; |$\eta$| &lt; 2.5
- $\mu$: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.1
- one $\tau_{\text{h}}$ (hadronically decaying tau lepton): $p_\text{T}$ &gt; 50 GeV, |$\eta$| &lt; 2.3
- $\Delta$R($\ell$,$\tau_{\text{h}}$) &gt; 0.5; vertex($\ell$) = vertex($\tau_{\text{h}}$); charge($\ell$) != charge($\tau_{\text{h}}$)
- veto opposite sign $\mu$/e
- veto opposite sign e/$\mu$
- jet: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.4
- $N_{\text{jet}}$ $\geq$ 2
- $N_{\text{b-jet}}$ $\geq$ 1
- $\Delta$R(jet,$\ell$) &gt; 0.5; $\Delta$R(jet,$\tau_{\text{h}}$) &gt; 0.5

Leptoquark search final selection:
- M($\tau_{\text{h}}$,jet) &gt; 250 GeV
(pairing is chosen that minimizes |M($\tau_{\text{h}}$,jet i) - M($\ell$,jet j)|)
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet)

Top squark search final selection:
- $N_\text{jet}$ $\geq$ 5
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet 1) + $p_\text{T}$(jet 2) + $p_\text{T}$(jet 3) + $p_\text{T}$(jet 4).
DOI: 10.17182/hepdata.66933.v1/t4
title: "Table 4" of "Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: Selection efficiencies in % for the signal in the top squark search, estimated from the simulation.
description: CERN-LHC. Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at $\sqrt{s}$ = 8 TeV using 19.7 inverse femtobarns of data collected with the CMS detector. The leptoquark search considers each leptoquark decaying to a tau lepton and a bottom quark, or each top squark decaying via an R-parity violating coupling $\lambda^{\prime}_{333}$ to a tau lepton and a bottom quark. The top squark search considers top squarks undergoing a chargino-mediated decay involving the R-parity violating coupling $\lambda^{\prime}_{3jk}$, each decaying to a tau lepton, a bottom quark, and two light quarks.

Errata:
17 JUN 2015: Fixed one typo from the paper: systematic uncertainties on the $M_{\text{LQ}}=700$ signal in Table 1 were a factor of ten too high.
17 JUN 2015: Fixed one typo just in the HepData entry: the $M_{\widetilde{\text{t}}}$ masses listed in Table 2 were incorrect.

Selection:
- one e/$\mu$ ($\ell$)
- e: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 1.444 or 1.56 &lt; |$\eta$| &lt; 2.5
- $\mu$: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.1
- one $\tau_{\text{h}}$ (hadronically decaying tau lepton): $p_\text{T}$ &gt; 50 GeV, |$\eta$| &lt; 2.3
- $\Delta$R($\ell$,$\tau_{\text{h}}$) &gt; 0.5; vertex($\ell$) = vertex($\tau_{\text{h}}$); charge($\ell$) != charge($\tau_{\text{h}}$)
- veto opposite sign $\mu$/e
- veto opposite sign e/$\mu$
- jet: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.4
- $N_{\text{jet}}$ $\geq$ 2
- $N_{\text{b-jet}}$ $\geq$ 1
- $\Delta$R(jet,$\ell$) &gt; 0.5; $\Delta$R(jet,$\tau_{\text{h}}$) &gt; 0.5

Leptoquark search final selection:
- M($\tau_{\text{h}}$,jet) &gt; 250 GeV
(pairing is chosen that minimizes |M($\tau_{\text{h}}$,jet i) - M($\ell$,jet j)|)
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet)

Top squark search final selection:
- $N_\text{jet}$ $\geq$ 5
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet 1) + $p_\text{T}$(jet 2) + $p_\text{T}$(jet 3) + $p_\text{T}$(jet 4).