cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.146693.v1/t384
title: "Table 21" of "Inclusive and differential cross-section measurements of $t\bar{t}Z$ production in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector, including EFT and spin-correlation interpretations"

description: Observed and expected 68% and 95% credible intervals for Fisher-rotated directions of EFT sensitivity, in the marginalised linear fit.
description: Inclusive and differential cross section measurements of $t\bar{t}Z$ production in $pp$ collisions at $\sqrt{s}$=13 TeV with the ATLAS detector, including EFT and spin correlations interpretations

The fiducial regions for the dilepton channel are defined as:
- Exactly 2 leptons ($e$ or $\mu$) with transverse momentum greater than 30, 15 GeV for leading and subleading lepton, respectively.
- The sum of the two lepton charges is required to be zero.
- Exactly one opposite-sign-same-flavour (OSSF) lepton pair (considered to be lepton pair from $Z$ boson) with invaraint mass compatible with $Z$ boson ($|m_{\ell\ell}^{Z}-m_{Z}|&lt;10$ GeV).
- Three orthogonal signal regions defined based on the jet and $b$-jet multiplicity.
- At least 5 jets with transverse momentum greater than 25 GeV.
- $b$-jets requirements: at least one $b$-jet tagged with fixed 77% $b$-tagging working point.

The fiducial regions for the trilepton channel are defined as:
- Exactly 3 leptons ($e$ or $\mu$) with transverse momentum greater than 27, 20, 15 GeV for leading, subleading and third lepton, respectively.
- The sum of the three lepton charges is required to be $\pm$1.
- At least one opposite-sign-same-flavour (OSSF) lepton pair (considered to be lepton pair from $Z$ boson) with invaraint mass compatible with $Z$ boson ($|m_{\ell\ell}^{Z}-m_{Z}|&lt;10$ GeV) and $m_{OSSF}&gt;10$ GeV for each OSSF lepton pair.
- Three orthogonal signal regions combined for both inclusive and differential cross section measurements.
- At least 3 jets with transverse momentum greater than 25 GeV.
- $b$-jets requirements: at least one $b$-jet tagged with fixed 85% $b$-tagging working point.
- Signal regions definitions based on the values of the deep neural network discriminants and $b$-jets requirements.

The fiducial regions for the tetralepton channel are defined as:
- Exactly 4 leptons ($e$ or $\mu$) with transverse momentum greater than 27, 7, 7, 7 GeV for leading, subleading, third and fourth lepton, respectively.
- The sum of the four lepton charges is required to be zero.
- At least one opposite-sign-same-flavor (OSSF) lepton pair (considered to be lepton pair from $Z$ boson) with invaraint mass compatible with $Z$ boson ($|m_{\ell\ell}^{Z}-m_{Z}|&lt;20$ GeV) and $m_{OSSF}&gt;10$ GeV for each OSSF lepton pair.
- Four signal regions separated based on based on the flavour composition of the non-$Z$ lepton pair (same flavour, different flavour) and value of the deep neural network discriminant.
- At least 2 jets with transverse momentum greater than 25 GeV.
- At least one $b$-jet tagged with the 85% $b$-tagging working point.
DOI: 10.17182/hepdata.146693.v1/t385
title: "EFT correlation matrix" of "Inclusive and differential cross-section measurements of $t\bar{t}Z$ production in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector, including EFT and spin-correlation interpretations"

description: Correlation matrix of the input particle-level observables used in the EFT fit.
description: Inclusive and differential cross section measurements of $t\bar{t}Z$ production in $pp$ collisions at $\sqrt{s}$=13 TeV with the ATLAS detector, including EFT and spin correlations interpretations

The fiducial regions for the dilepton channel are defined as:
- Exactly 2 leptons ($e$ or $\mu$) with transverse momentum greater than 30, 15 GeV for leading and subleading lepton, respectively.
- The sum of the two lepton charges is required to be zero.
- Exactly one opposite-sign-same-flavour (OSSF) lepton pair (considered to be lepton pair from $Z$ boson) with invaraint mass compatible with $Z$ boson ($|m_{\ell\ell}^{Z}-m_{Z}|&lt;10$ GeV).
- Three orthogonal signal regions defined based on the jet and $b$-jet multiplicity.
- At least 5 jets with transverse momentum greater than 25 GeV.
- $b$-jets requirements: at least one $b$-jet tagged with fixed 77% $b$-tagging working point.

The fiducial regions for the trilepton channel are defined as:
- Exactly 3 leptons ($e$ or $\mu$) with transverse momentum greater than 27, 20, 15 GeV for leading, subleading and third lepton, respectively.
- The sum of the three lepton charges is required to be $\pm$1.
- At least one opposite-sign-same-flavour (OSSF) lepton pair (considered to be lepton pair from $Z$ boson) with invaraint mass compatible with $Z$ boson ($|m_{\ell\ell}^{Z}-m_{Z}|&lt;10$ GeV) and $m_{OSSF}&gt;10$ GeV for each OSSF lepton pair.
- Three orthogonal signal regions combined for both inclusive and differential cross section measurements.
- At least 3 jets with transverse momentum greater than 25 GeV.
- $b$-jets requirements: at least one $b$-jet tagged with fixed 85% $b$-tagging working point.
- Signal regions definitions based on the values of the deep neural network discriminants and $b$-jets requirements.

The fiducial regions for the tetralepton channel are defined as:
- Exactly 4 leptons ($e$ or $\mu$) with transverse momentum greater than 27, 7, 7, 7 GeV for leading, subleading, third and fourth lepton, respectively.
- The sum of the four lepton charges is required to be zero.
- At least one opposite-sign-same-flavor (OSSF) lepton pair (considered to be lepton pair from $Z$ boson) with invaraint mass compatible with $Z$ boson ($|m_{\ell\ell}^{Z}-m_{Z}|&lt;20$ GeV) and $m_{OSSF}&gt;10$ GeV for each OSSF lepton pair.
- Four signal regions separated based on based on the flavour composition of the non-$Z$ lepton pair (same flavour, different flavour) and value of the deep neural network discriminant.
- At least 2 jets with transverse momentum greater than 25 GeV.
- At least one $b$-jet tagged with the 85% $b$-tagging working point.
DOI: 10.17182/hepdata.146723.v1/t1
title: "Table 1" of "Prompt and non-prompt J$/\psi$ production at midrapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Non-prompt J/$\psi$ fraction as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%
description: The transverse momentum ($p_T$) and centrality dependence of the nuclear modification factor $R_{AA}$ of prompt and non-prompt J/$\psi$, the latter originating from the weak decays of beauty hadrons, have been measured by the ALICE collaboration in Pb--Pb collisions at 5.02 TeV. The measurements are carried out through the e^+e^- decay channel at midrapidity ($|y| &lt; 0.9$) in the transverse momentum region $1.5 &lt; $p_T$ &lt; 10$~\GeVc. Both prompt and non-prompt J/$\psi$ measurements indicate a significant suppression for $p_T$ $&gt;$ 5~\GeVc, which becomes stronger with increasing collision centrality. The results are consistent with similar LHC measurements in the overlapping $p_T$ intervals, and cover the kinematic region down to $p_T$ = 1.5 \GeVc at midrapidity, not accessible by other LHC experiments. The suppression of prompt J/$\psi$ in central and semicentral collisions exhibits a decreasing trend towards lower transverse momentum, described within uncertainties by models implementing J/$\psi$ production from recombination of c and $\overline{\rm c}$ quarks produced independently in different partonic scatterings. At high transverse momentum, transport models including quarkonium dissociation are able to describe the suppression for prompt J/$\psi$. For non-prompt J/$\psi$, the suppression predicted by models including both collisional and radiative processes for the computation of the beauty-quark energy loss inside the quark--gluon plasma is consistent with measurements within uncertainties.
DOI: 10.17182/hepdata.146723.v1/t2
title: "Table 2" of "Prompt and non-prompt J$/\psi$ production at midrapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Non-prompt J/$\psi$ fraction as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 10-30%
description: The transverse momentum ($p_T$) and centrality dependence of the nuclear modification factor $R_{AA}$ of prompt and non-prompt J/$\psi$, the latter originating from the weak decays of beauty hadrons, have been measured by the ALICE collaboration in Pb--Pb collisions at 5.02 TeV. The measurements are carried out through the e^+e^- decay channel at midrapidity ($|y| &lt; 0.9$) in the transverse momentum region $1.5 &lt; $p_T$ &lt; 10$~\GeVc. Both prompt and non-prompt J/$\psi$ measurements indicate a significant suppression for $p_T$ $&gt;$ 5~\GeVc, which becomes stronger with increasing collision centrality. The results are consistent with similar LHC measurements in the overlapping $p_T$ intervals, and cover the kinematic region down to $p_T$ = 1.5 \GeVc at midrapidity, not accessible by other LHC experiments. The suppression of prompt J/$\psi$ in central and semicentral collisions exhibits a decreasing trend towards lower transverse momentum, described within uncertainties by models implementing J/$\psi$ production from recombination of c and $\overline{\rm c}$ quarks produced independently in different partonic scatterings. At high transverse momentum, transport models including quarkonium dissociation are able to describe the suppression for prompt J/$\psi$. For non-prompt J/$\psi$, the suppression predicted by models including both collisional and radiative processes for the computation of the beauty-quark energy loss inside the quark--gluon plasma is consistent with measurements within uncertainties.
DOI: 10.17182/hepdata.146723.v1/t3
title: "Table 3" of "Prompt and non-prompt J$/\psi$ production at midrapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Non-prompt J/$\psi$ fraction as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%
description: The transverse momentum ($p_T$) and centrality dependence of the nuclear modification factor $R_{AA}$ of prompt and non-prompt J/$\psi$, the latter originating from the weak decays of beauty hadrons, have been measured by the ALICE collaboration in Pb--Pb collisions at 5.02 TeV. The measurements are carried out through the e^+e^- decay channel at midrapidity ($|y| &lt; 0.9$) in the transverse momentum region $1.5 &lt; $p_T$ &lt; 10$~\GeVc. Both prompt and non-prompt J/$\psi$ measurements indicate a significant suppression for $p_T$ $&gt;$ 5~\GeVc, which becomes stronger with increasing collision centrality. The results are consistent with similar LHC measurements in the overlapping $p_T$ intervals, and cover the kinematic region down to $p_T$ = 1.5 \GeVc at midrapidity, not accessible by other LHC experiments. The suppression of prompt J/$\psi$ in central and semicentral collisions exhibits a decreasing trend towards lower transverse momentum, described within uncertainties by models implementing J/$\psi$ production from recombination of c and $\overline{\rm c}$ quarks produced independently in different partonic scatterings. At high transverse momentum, transport models including quarkonium dissociation are able to describe the suppression for prompt J/$\psi$. For non-prompt J/$\psi$, the suppression predicted by models including both collisional and radiative processes for the computation of the beauty-quark energy loss inside the quark--gluon plasma is consistent with measurements within uncertainties.
DOI: 10.17182/hepdata.146723.v1/t4
title: "Table 4" of "Prompt and non-prompt J$/\psi$ production at midrapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Non-prompt J/$\psi$ fraction as a function of average number of participants in Pb-Pb at 5.02 TeV
description: The transverse momentum ($p_T$) and centrality dependence of the nuclear modification factor $R_{AA}$ of prompt and non-prompt J/$\psi$, the latter originating from the weak decays of beauty hadrons, have been measured by the ALICE collaboration in Pb--Pb collisions at 5.02 TeV. The measurements are carried out through the e^+e^- decay channel at midrapidity ($|y| &lt; 0.9$) in the transverse momentum region $1.5 &lt; $p_T$ &lt; 10$~\GeVc. Both prompt and non-prompt J/$\psi$ measurements indicate a significant suppression for $p_T$ $&gt;$ 5~\GeVc, which becomes stronger with increasing collision centrality. The results are consistent with similar LHC measurements in the overlapping $p_T$ intervals, and cover the kinematic region down to $p_T$ = 1.5 \GeVc at midrapidity, not accessible by other LHC experiments. The suppression of prompt J/$\psi$ in central and semicentral collisions exhibits a decreasing trend towards lower transverse momentum, described within uncertainties by models implementing J/$\psi$ production from recombination of c and $\overline{\rm c}$ quarks produced independently in different partonic scatterings. At high transverse momentum, transport models including quarkonium dissociation are able to describe the suppression for prompt J/$\psi$. For non-prompt J/$\psi$, the suppression predicted by models including both collisional and radiative processes for the computation of the beauty-quark energy loss inside the quark--gluon plasma is consistent with measurements within uncertainties.
DOI: 10.17182/hepdata.146723.v1/t5
title: "Table 5" of "Prompt and non-prompt J$/\psi$ production at midrapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Non-prompt J/$\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%
description: The transverse momentum ($p_T$) and centrality dependence of the nuclear modification factor $R_{AA}$ of prompt and non-prompt J/$\psi$, the latter originating from the weak decays of beauty hadrons, have been measured by the ALICE collaboration in Pb--Pb collisions at 5.02 TeV. The measurements are carried out through the e^+e^- decay channel at midrapidity ($|y| &lt; 0.9$) in the transverse momentum region $1.5 &lt; $p_T$ &lt; 10$~\GeVc. Both prompt and non-prompt J/$\psi$ measurements indicate a significant suppression for $p_T$ $&gt;$ 5~\GeVc, which becomes stronger with increasing collision centrality. The results are consistent with similar LHC measurements in the overlapping $p_T$ intervals, and cover the kinematic region down to $p_T$ = 1.5 \GeVc at midrapidity, not accessible by other LHC experiments. The suppression of prompt J/$\psi$ in central and semicentral collisions exhibits a decreasing trend towards lower transverse momentum, described within uncertainties by models implementing J/$\psi$ production from recombination of c and $\overline{\rm c}$ quarks produced independently in different partonic scatterings. At high transverse momentum, transport models including quarkonium dissociation are able to describe the suppression for prompt J/$\psi$. For non-prompt J/$\psi$, the suppression predicted by models including both collisional and radiative processes for the computation of the beauty-quark energy loss inside the quark--gluon plasma is consistent with measurements within uncertainties.
DOI: 10.17182/hepdata.146723.v1/t6
title: "Table 6" of "Prompt and non-prompt J$/\psi$ production at midrapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Prompt J/$\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%
description: The transverse momentum ($p_T$) and centrality dependence of the nuclear modification factor $R_{AA}$ of prompt and non-prompt J/$\psi$, the latter originating from the weak decays of beauty hadrons, have been measured by the ALICE collaboration in Pb--Pb collisions at 5.02 TeV. The measurements are carried out through the e^+e^- decay channel at midrapidity ($|y| &lt; 0.9$) in the transverse momentum region $1.5 &lt; $p_T$ &lt; 10$~\GeVc. Both prompt and non-prompt J/$\psi$ measurements indicate a significant suppression for $p_T$ $&gt;$ 5~\GeVc, which becomes stronger with increasing collision centrality. The results are consistent with similar LHC measurements in the overlapping $p_T$ intervals, and cover the kinematic region down to $p_T$ = 1.5 \GeVc at midrapidity, not accessible by other LHC experiments. The suppression of prompt J/$\psi$ in central and semicentral collisions exhibits a decreasing trend towards lower transverse momentum, described within uncertainties by models implementing J/$\psi$ production from recombination of c and $\overline{\rm c}$ quarks produced independently in different partonic scatterings. At high transverse momentum, transport models including quarkonium dissociation are able to describe the suppression for prompt J/$\psi$. For non-prompt J/$\psi$, the suppression predicted by models including both collisional and radiative processes for the computation of the beauty-quark energy loss inside the quark--gluon plasma is consistent with measurements within uncertainties.
DOI: 10.17182/hepdata.146723.v1/t7
title: "Table 7" of "Prompt and non-prompt J$/\psi$ production at midrapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%. Global uncertainty 2.3%
description: The transverse momentum ($p_T$) and centrality dependence of the nuclear modification factor $R_{AA}$ of prompt and non-prompt J/$\psi$, the latter originating from the weak decays of beauty hadrons, have been measured by the ALICE collaboration in Pb--Pb collisions at 5.02 TeV. The measurements are carried out through the e^+e^- decay channel at midrapidity ($|y| &lt; 0.9$) in the transverse momentum region $1.5 &lt; $p_T$ &lt; 10$~\GeVc. Both prompt and non-prompt J/$\psi$ measurements indicate a significant suppression for $p_T$ $&gt;$ 5~\GeVc, which becomes stronger with increasing collision centrality. The results are consistent with similar LHC measurements in the overlapping $p_T$ intervals, and cover the kinematic region down to $p_T$ = 1.5 \GeVc at midrapidity, not accessible by other LHC experiments. The suppression of prompt J/$\psi$ in central and semicentral collisions exhibits a decreasing trend towards lower transverse momentum, described within uncertainties by models implementing J/$\psi$ production from recombination of c and $\overline{\rm c}$ quarks produced independently in different partonic scatterings. At high transverse momentum, transport models including quarkonium dissociation are able to describe the suppression for prompt J/$\psi$. For non-prompt J/$\psi$, the suppression predicted by models including both collisional and radiative processes for the computation of the beauty-quark energy loss inside the quark--gluon plasma is consistent with measurements within uncertainties.
DOI: 10.17182/hepdata.146723.v1/t8
title: "Table 8" of "Prompt and non-prompt J$/\psi$ production at midrapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 10-30%. Global uncertainty 2.3%
description: The transverse momentum ($p_T$) and centrality dependence of the nuclear modification factor $R_{AA}$ of prompt and non-prompt J/$\psi$, the latter originating from the weak decays of beauty hadrons, have been measured by the ALICE collaboration in Pb--Pb collisions at 5.02 TeV. The measurements are carried out through the e^+e^- decay channel at midrapidity ($|y| &lt; 0.9$) in the transverse momentum region $1.5 &lt; $p_T$ &lt; 10$~\GeVc. Both prompt and non-prompt J/$\psi$ measurements indicate a significant suppression for $p_T$ $&gt;$ 5~\GeVc, which becomes stronger with increasing collision centrality. The results are consistent with similar LHC measurements in the overlapping $p_T$ intervals, and cover the kinematic region down to $p_T$ = 1.5 \GeVc at midrapidity, not accessible by other LHC experiments. The suppression of prompt J/$\psi$ in central and semicentral collisions exhibits a decreasing trend towards lower transverse momentum, described within uncertainties by models implementing J/$\psi$ production from recombination of c and $\overline{\rm c}$ quarks produced independently in different partonic scatterings. At high transverse momentum, transport models including quarkonium dissociation are able to describe the suppression for prompt J/$\psi$. For non-prompt J/$\psi$, the suppression predicted by models including both collisional and radiative processes for the computation of the beauty-quark energy loss inside the quark--gluon plasma is consistent with measurements within uncertainties.
DOI: 10.17182/hepdata.146723.v1/t10
title: "Table 10" of "Prompt and non-prompt J$/\psi$ production at midrapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Prompt J/$\psi$ nuclear modification factor as a function of average number of participants in Pb-Pb at 5.02 TeV. Global uncertainty 2.2%
description: The transverse momentum ($p_T$) and centrality dependence of the nuclear modification factor $R_{AA}$ of prompt and non-prompt J/$\psi$, the latter originating from the weak decays of beauty hadrons, have been measured by the ALICE collaboration in Pb--Pb collisions at 5.02 TeV. The measurements are carried out through the e^+e^- decay channel at midrapidity ($|y| &lt; 0.9$) in the transverse momentum region $1.5 &lt; $p_T$ &lt; 10$~\GeVc. Both prompt and non-prompt J/$\psi$ measurements indicate a significant suppression for $p_T$ $&gt;$ 5~\GeVc, which becomes stronger with increasing collision centrality. The results are consistent with similar LHC measurements in the overlapping $p_T$ intervals, and cover the kinematic region down to $p_T$ = 1.5 \GeVc at midrapidity, not accessible by other LHC experiments. The suppression of prompt J/$\psi$ in central and semicentral collisions exhibits a decreasing trend towards lower transverse momentum, described within uncertainties by models implementing J/$\psi$ production from recombination of c and $\overline{\rm c}$ quarks produced independently in different partonic scatterings. At high transverse momentum, transport models including quarkonium dissociation are able to describe the suppression for prompt J/$\psi$. For non-prompt J/$\psi$, the suppression predicted by models including both collisional and radiative processes for the computation of the beauty-quark energy loss inside the quark--gluon plasma is consistent with measurements within uncertainties.