cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.75256.v1/t54
title: "Table 54" of "Transverse momentum, rapidity, and centrality dependence of inclusive charged-particle production in $\sqrt{s_{NN}}=5.02$ TeV p+Pb collisions measured by the ATLAS experiment"

description: $R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.
description: CERN-LHC. Measurements of the per-event charged-particle yield as a function of the charged-particle transverse momentum and rapidity are performed using $p+$Pb collision data collected by the ATLAS experiment at the LHC at a centre-of-mass energy of $\sqrt{s_{NN}}=5.02$ TeV. Charged particles are reconstructed over pseudorapidity $|\eta|&lt;2.3$ and transverse momentum between $0.1$ GeV and $22$ GeV in a dataset corresponding to an integrated luminosity of $1$ $\mu b^{-1}$. The results are presented in the form of charged-particle nuclear modification factors, where the $p+$Pb charged-particle multiplicities are compared between central and peripheral $p+$Pb collisions as well as to charged-particle cross sections measured in pp collisions. The $p+$Pb collision centrality is characterized by the total transverse energy measured in $-4.9&lt;\eta&lt;-3.1$, which is in the direction of the outgoing lead beam. Three different estimations of the number of nucleons participating in the $p+$Pb collision are carried out using the Glauber model and two Glauber-Gribov colour-fluctuation extensions to the Glauber model. The values of the nuclear modification factors are found to vary significantly as a function of rapidity and transverse momentum. A broad peak is observed for all centralities and rapidities in the nuclear modification factors for charged-particle transverse momentum values around $3$ GeV. The magnitude of the peak increases for more central collisions as well as rapidity ranges closer to the direction of the outgoing lead nucleus.
DOI: 10.17182/hepdata.75256.v1/t55
title: "Table 55" of "Transverse momentum, rapidity, and centrality dependence of inclusive charged-particle production in $\sqrt{s_{NN}}=5.02$ TeV p+Pb collisions measured by the ATLAS experiment"

description: $R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.
description: CERN-LHC. Measurements of the per-event charged-particle yield as a function of the charged-particle transverse momentum and rapidity are performed using $p+$Pb collision data collected by the ATLAS experiment at the LHC at a centre-of-mass energy of $\sqrt{s_{NN}}=5.02$ TeV. Charged particles are reconstructed over pseudorapidity $|\eta|&lt;2.3$ and transverse momentum between $0.1$ GeV and $22$ GeV in a dataset corresponding to an integrated luminosity of $1$ $\mu b^{-1}$. The results are presented in the form of charged-particle nuclear modification factors, where the $p+$Pb charged-particle multiplicities are compared between central and peripheral $p+$Pb collisions as well as to charged-particle cross sections measured in pp collisions. The $p+$Pb collision centrality is characterized by the total transverse energy measured in $-4.9&lt;\eta&lt;-3.1$, which is in the direction of the outgoing lead beam. Three different estimations of the number of nucleons participating in the $p+$Pb collision are carried out using the Glauber model and two Glauber-Gribov colour-fluctuation extensions to the Glauber model. The values of the nuclear modification factors are found to vary significantly as a function of rapidity and transverse momentum. A broad peak is observed for all centralities and rapidities in the nuclear modification factors for charged-particle transverse momentum values around $3$ GeV. The magnitude of the peak increases for more central collisions as well as rapidity ranges closer to the direction of the outgoing lead nucleus.
DOI: 10.17182/hepdata.75256.v1/t57
title: "Table 57" of "Transverse momentum, rapidity, and centrality dependence of inclusive charged-particle production in $\sqrt{s_{NN}}=5.02$ TeV p+Pb collisions measured by the ATLAS experiment"

description: $R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.
description: CERN-LHC. Measurements of the per-event charged-particle yield as a function of the charged-particle transverse momentum and rapidity are performed using $p+$Pb collision data collected by the ATLAS experiment at the LHC at a centre-of-mass energy of $\sqrt{s_{NN}}=5.02$ TeV. Charged particles are reconstructed over pseudorapidity $|\eta|&lt;2.3$ and transverse momentum between $0.1$ GeV and $22$ GeV in a dataset corresponding to an integrated luminosity of $1$ $\mu b^{-1}$. The results are presented in the form of charged-particle nuclear modification factors, where the $p+$Pb charged-particle multiplicities are compared between central and peripheral $p+$Pb collisions as well as to charged-particle cross sections measured in pp collisions. The $p+$Pb collision centrality is characterized by the total transverse energy measured in $-4.9&lt;\eta&lt;-3.1$, which is in the direction of the outgoing lead beam. Three different estimations of the number of nucleons participating in the $p+$Pb collision are carried out using the Glauber model and two Glauber-Gribov colour-fluctuation extensions to the Glauber model. The values of the nuclear modification factors are found to vary significantly as a function of rapidity and transverse momentum. A broad peak is observed for all centralities and rapidities in the nuclear modification factors for charged-particle transverse momentum values around $3$ GeV. The magnitude of the peak increases for more central collisions as well as rapidity ranges closer to the direction of the outgoing lead nucleus.
DOI: 10.17182/hepdata.75256.v1/t56
title: "Table 56" of "Transverse momentum, rapidity, and centrality dependence of inclusive charged-particle production in $\sqrt{s_{NN}}=5.02$ TeV p+Pb collisions measured by the ATLAS experiment"

description: $R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.
description: CERN-LHC. Measurements of the per-event charged-particle yield as a function of the charged-particle transverse momentum and rapidity are performed using $p+$Pb collision data collected by the ATLAS experiment at the LHC at a centre-of-mass energy of $\sqrt{s_{NN}}=5.02$ TeV. Charged particles are reconstructed over pseudorapidity $|\eta|&lt;2.3$ and transverse momentum between $0.1$ GeV and $22$ GeV in a dataset corresponding to an integrated luminosity of $1$ $\mu b^{-1}$. The results are presented in the form of charged-particle nuclear modification factors, where the $p+$Pb charged-particle multiplicities are compared between central and peripheral $p+$Pb collisions as well as to charged-particle cross sections measured in pp collisions. The $p+$Pb collision centrality is characterized by the total transverse energy measured in $-4.9&lt;\eta&lt;-3.1$, which is in the direction of the outgoing lead beam. Three different estimations of the number of nucleons participating in the $p+$Pb collision are carried out using the Glauber model and two Glauber-Gribov colour-fluctuation extensions to the Glauber model. The values of the nuclear modification factors are found to vary significantly as a function of rapidity and transverse momentum. A broad peak is observed for all centralities and rapidities in the nuclear modification factors for charged-particle transverse momentum values around $3$ GeV. The magnitude of the peak increases for more central collisions as well as rapidity ranges closer to the direction of the outgoing lead nucleus.
DOI: 10.17182/hepdata.75256.v1/t58
title: "Table 58" of "Transverse momentum, rapidity, and centrality dependence of inclusive charged-particle production in $\sqrt{s_{NN}}=5.02$ TeV p+Pb collisions measured by the ATLAS experiment"

description: $R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.
description: CERN-LHC. Measurements of the per-event charged-particle yield as a function of the charged-particle transverse momentum and rapidity are performed using $p+$Pb collision data collected by the ATLAS experiment at the LHC at a centre-of-mass energy of $\sqrt{s_{NN}}=5.02$ TeV. Charged particles are reconstructed over pseudorapidity $|\eta|&lt;2.3$ and transverse momentum between $0.1$ GeV and $22$ GeV in a dataset corresponding to an integrated luminosity of $1$ $\mu b^{-1}$. The results are presented in the form of charged-particle nuclear modification factors, where the $p+$Pb charged-particle multiplicities are compared between central and peripheral $p+$Pb collisions as well as to charged-particle cross sections measured in pp collisions. The $p+$Pb collision centrality is characterized by the total transverse energy measured in $-4.9&lt;\eta&lt;-3.1$, which is in the direction of the outgoing lead beam. Three different estimations of the number of nucleons participating in the $p+$Pb collision are carried out using the Glauber model and two Glauber-Gribov colour-fluctuation extensions to the Glauber model. The values of the nuclear modification factors are found to vary significantly as a function of rapidity and transverse momentum. A broad peak is observed for all centralities and rapidities in the nuclear modification factors for charged-particle transverse momentum values around $3$ GeV. The magnitude of the peak increases for more central collisions as well as rapidity ranges closer to the direction of the outgoing lead nucleus.
DOI: 10.17182/hepdata.75256.v1/t59
title: "Table 59" of "Transverse momentum, rapidity, and centrality dependence of inclusive charged-particle production in $\sqrt{s_{NN}}=5.02$ TeV p+Pb collisions measured by the ATLAS experiment"

description: $R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.
description: CERN-LHC. Measurements of the per-event charged-particle yield as a function of the charged-particle transverse momentum and rapidity are performed using $p+$Pb collision data collected by the ATLAS experiment at the LHC at a centre-of-mass energy of $\sqrt{s_{NN}}=5.02$ TeV. Charged particles are reconstructed over pseudorapidity $|\eta|&lt;2.3$ and transverse momentum between $0.1$ GeV and $22$ GeV in a dataset corresponding to an integrated luminosity of $1$ $\mu b^{-1}$. The results are presented in the form of charged-particle nuclear modification factors, where the $p+$Pb charged-particle multiplicities are compared between central and peripheral $p+$Pb collisions as well as to charged-particle cross sections measured in pp collisions. The $p+$Pb collision centrality is characterized by the total transverse energy measured in $-4.9&lt;\eta&lt;-3.1$, which is in the direction of the outgoing lead beam. Three different estimations of the number of nucleons participating in the $p+$Pb collision are carried out using the Glauber model and two Glauber-Gribov colour-fluctuation extensions to the Glauber model. The values of the nuclear modification factors are found to vary significantly as a function of rapidity and transverse momentum. A broad peak is observed for all centralities and rapidities in the nuclear modification factors for charged-particle transverse momentum values around $3$ GeV. The magnitude of the peak increases for more central collisions as well as rapidity ranges closer to the direction of the outgoing lead nucleus.
DOI: 10.17182/hepdata.75316.v1/t1
title: "Table 1" of "Measurement of the $b\overline{b}$ dijet cross section in $pp$ collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: Results for the m_bb distribution. Statistical and systematic uncertainties are quoted.
description: CERN-LHC. Measurement of the dijet production cross section for jets containing a b-hadron (b-jets) in proton proton collisions at a centre-of-mass energy of 7 TeV, with 4.2 fb^-1 of data collected by the ATLAS detector in 2011. The cross section is measured for events with two identified b-jets with a transverse momentum pT &gt; 20 GeV and a minimum separation in the eta-phi plane of Delta R = 0.4. At least one of the jets in the event is required to have pT &gt; 270 GeV. The cross section is measured differentially as a function of the dijet invariant mass, dijet transverse momentum, boost of the dijet system, and of the rapidity difference, azimuthal angle and angular distance between the b-jets. 





Ranges of the variables of the measured differential cross sections:

- m_bb : 50 - 1000 GeV (mass of the b-bbar di-jet system)

- pT_bb : 0 - 400 GeV (transverse momentum of the b-bbar di-jet system)

- y_B : 0 - 2.5 (boost of the b-bbar dijet system y_b = (y1+y2)/2 )

- Delta phi : 0 - pi (azimuthal angle between the two b-jets) 

- Delta R : 0.4 - 4.0 (angular distance between the two b-jets) 

- y* : 0 - 1.7 (rapidity difference between the two b-jets y* = |y1 -y2|/2 )





Cuts defining the fiducial region:

- Leading jet pT &gt; 270 GeV and |eta| &lt; 3.2

- Both b-jets with pT &gt; 20 GeV and |eta| &lt; 2.5


- The two b-jets must have an angular separation Delta R &gt; 0.4.
DOI: 10.17182/hepdata.75316.v1/t2
title: "Table 2" of "Measurement of the $b\overline{b}$ dijet cross section in $pp$ collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: Results for the DeltaPhi distribution. Statistical and systematic uncertainties are quoted.
description: CERN-LHC. Measurement of the dijet production cross section for jets containing a b-hadron (b-jets) in proton proton collisions at a centre-of-mass energy of 7 TeV, with 4.2 fb^-1 of data collected by the ATLAS detector in 2011. The cross section is measured for events with two identified b-jets with a transverse momentum pT &gt; 20 GeV and a minimum separation in the eta-phi plane of Delta R = 0.4. At least one of the jets in the event is required to have pT &gt; 270 GeV. The cross section is measured differentially as a function of the dijet invariant mass, dijet transverse momentum, boost of the dijet system, and of the rapidity difference, azimuthal angle and angular distance between the b-jets. 





Ranges of the variables of the measured differential cross sections:

- m_bb : 50 - 1000 GeV (mass of the b-bbar di-jet system)

- pT_bb : 0 - 400 GeV (transverse momentum of the b-bbar di-jet system)

- y_B : 0 - 2.5 (boost of the b-bbar dijet system y_b = (y1+y2)/2 )

- Delta phi : 0 - pi (azimuthal angle between the two b-jets) 

- Delta R : 0.4 - 4.0 (angular distance between the two b-jets) 

- y* : 0 - 1.7 (rapidity difference between the two b-jets y* = |y1 -y2|/2 )





Cuts defining the fiducial region:

- Leading jet pT &gt; 270 GeV and |eta| &lt; 3.2

- Both b-jets with pT &gt; 20 GeV and |eta| &lt; 2.5


- The two b-jets must have an angular separation Delta R &gt; 0.4.
DOI: 10.17182/hepdata.75316.v1/t3
title: "Table 3" of "Measurement of the $b\overline{b}$ dijet cross section in $pp$ collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: Results for the y* distribution. Statistical and systematic uncertainties are quoted.
description: CERN-LHC. Measurement of the dijet production cross section for jets containing a b-hadron (b-jets) in proton proton collisions at a centre-of-mass energy of 7 TeV, with 4.2 fb^-1 of data collected by the ATLAS detector in 2011. The cross section is measured for events with two identified b-jets with a transverse momentum pT &gt; 20 GeV and a minimum separation in the eta-phi plane of Delta R = 0.4. At least one of the jets in the event is required to have pT &gt; 270 GeV. The cross section is measured differentially as a function of the dijet invariant mass, dijet transverse momentum, boost of the dijet system, and of the rapidity difference, azimuthal angle and angular distance between the b-jets. 





Ranges of the variables of the measured differential cross sections:

- m_bb : 50 - 1000 GeV (mass of the b-bbar di-jet system)

- pT_bb : 0 - 400 GeV (transverse momentum of the b-bbar di-jet system)

- y_B : 0 - 2.5 (boost of the b-bbar dijet system y_b = (y1+y2)/2 )

- Delta phi : 0 - pi (azimuthal angle between the two b-jets) 

- Delta R : 0.4 - 4.0 (angular distance between the two b-jets) 

- y* : 0 - 1.7 (rapidity difference between the two b-jets y* = |y1 -y2|/2 )





Cuts defining the fiducial region:

- Leading jet pT &gt; 270 GeV and |eta| &lt; 3.2

- Both b-jets with pT &gt; 20 GeV and |eta| &lt; 2.5


- The two b-jets must have an angular separation Delta R &gt; 0.4.
DOI: 10.17182/hepdata.75316.v1/t4
title: "Table 4" of "Measurement of the $b\overline{b}$ dijet cross section in $pp$ collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: Results for the DeltaR distribution. Statistical and systematic uncertainties are quoted.
description: CERN-LHC. Measurement of the dijet production cross section for jets containing a b-hadron (b-jets) in proton proton collisions at a centre-of-mass energy of 7 TeV, with 4.2 fb^-1 of data collected by the ATLAS detector in 2011. The cross section is measured for events with two identified b-jets with a transverse momentum pT &gt; 20 GeV and a minimum separation in the eta-phi plane of Delta R = 0.4. At least one of the jets in the event is required to have pT &gt; 270 GeV. The cross section is measured differentially as a function of the dijet invariant mass, dijet transverse momentum, boost of the dijet system, and of the rapidity difference, azimuthal angle and angular distance between the b-jets. 





Ranges of the variables of the measured differential cross sections:

- m_bb : 50 - 1000 GeV (mass of the b-bbar di-jet system)

- pT_bb : 0 - 400 GeV (transverse momentum of the b-bbar di-jet system)

- y_B : 0 - 2.5 (boost of the b-bbar dijet system y_b = (y1+y2)/2 )

- Delta phi : 0 - pi (azimuthal angle between the two b-jets) 

- Delta R : 0.4 - 4.0 (angular distance between the two b-jets) 

- y* : 0 - 1.7 (rapidity difference between the two b-jets y* = |y1 -y2|/2 )





Cuts defining the fiducial region:

- Leading jet pT &gt; 270 GeV and |eta| &lt; 3.2

- Both b-jets with pT &gt; 20 GeV and |eta| &lt; 2.5


- The two b-jets must have an angular separation Delta R &gt; 0.4.
DOI: 10.17182/hepdata.75316.v1/t5
title: "Table 5" of "Measurement of the $b\overline{b}$ dijet cross section in $pp$ collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: Results for the pT distribution. Statistical and systematic uncertainties are quoted.
description: CERN-LHC. Measurement of the dijet production cross section for jets containing a b-hadron (b-jets) in proton proton collisions at a centre-of-mass energy of 7 TeV, with 4.2 fb^-1 of data collected by the ATLAS detector in 2011. The cross section is measured for events with two identified b-jets with a transverse momentum pT &gt; 20 GeV and a minimum separation in the eta-phi plane of Delta R = 0.4. At least one of the jets in the event is required to have pT &gt; 270 GeV. The cross section is measured differentially as a function of the dijet invariant mass, dijet transverse momentum, boost of the dijet system, and of the rapidity difference, azimuthal angle and angular distance between the b-jets. 





Ranges of the variables of the measured differential cross sections:

- m_bb : 50 - 1000 GeV (mass of the b-bbar di-jet system)

- pT_bb : 0 - 400 GeV (transverse momentum of the b-bbar di-jet system)

- y_B : 0 - 2.5 (boost of the b-bbar dijet system y_b = (y1+y2)/2 )

- Delta phi : 0 - pi (azimuthal angle between the two b-jets) 

- Delta R : 0.4 - 4.0 (angular distance between the two b-jets) 

- y* : 0 - 1.7 (rapidity difference between the two b-jets y* = |y1 -y2|/2 )





Cuts defining the fiducial region:

- Leading jet pT &gt; 270 GeV and |eta| &lt; 3.2

- Both b-jets with pT &gt; 20 GeV and |eta| &lt; 2.5


- The two b-jets must have an angular separation Delta R &gt; 0.4.
DOI: 10.17182/hepdata.75316.v1/t6
title: "Table 6" of "Measurement of the $b\overline{b}$ dijet cross section in $pp$ collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector"

description: Results for the y_B distribution. Statistical and systematic uncertainties are quoted.
description: CERN-LHC. Measurement of the dijet production cross section for jets containing a b-hadron (b-jets) in proton proton collisions at a centre-of-mass energy of 7 TeV, with 4.2 fb^-1 of data collected by the ATLAS detector in 2011. The cross section is measured for events with two identified b-jets with a transverse momentum pT &gt; 20 GeV and a minimum separation in the eta-phi plane of Delta R = 0.4. At least one of the jets in the event is required to have pT &gt; 270 GeV. The cross section is measured differentially as a function of the dijet invariant mass, dijet transverse momentum, boost of the dijet system, and of the rapidity difference, azimuthal angle and angular distance between the b-jets. 





Ranges of the variables of the measured differential cross sections:

- m_bb : 50 - 1000 GeV (mass of the b-bbar di-jet system)

- pT_bb : 0 - 400 GeV (transverse momentum of the b-bbar di-jet system)

- y_B : 0 - 2.5 (boost of the b-bbar dijet system y_b = (y1+y2)/2 )

- Delta phi : 0 - pi (azimuthal angle between the two b-jets) 

- Delta R : 0.4 - 4.0 (angular distance between the two b-jets) 

- y* : 0 - 1.7 (rapidity difference between the two b-jets y* = |y1 -y2|/2 )





Cuts defining the fiducial region:

- Leading jet pT &gt; 270 GeV and |eta| &lt; 3.2

- Both b-jets with pT &gt; 20 GeV and |eta| &lt; 2.5


- The two b-jets must have an angular separation Delta R &gt; 0.4.
DOI: 10.17182/hepdata.75323.v1/t1
title: "Table 1" of "Measurement of top quark pair differential cross-sections in the dilepton channel in $pp$ collisions at $\sqrt{s}$ = 7 and 8 TeV with ATLAS"

description: Parton-level normalized $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 7 TeV. The cross-sections in the last bins include events (if any) beyond of the bin edges. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. Measurements of normalized differential cross-sections of top quark pair ($t\bar t$) production are presented as a function of the mass, the transverse momentum and the rapidity of the $t\bar t$ system in proton-proton collisions at center-of-mass energies of $\sqrt{s}$ = 7 TeV and 8 TeV. The dataset corresponds to an integrated luminosity of 4.6 fb$^{-1}$ at 7 TeV and 20.2 fb$^{-1}$ at 8 TeV, recorded with the ATLAS detector at the Large Hadron Collider. Events with top quark pair signatures are selected in the dilepton final state, requiring exactly two charged leptons and at least two jets with at least one of the jets identified as likely to contain a $b$-hadron. The measured distributions are corrected for detector effects and selection efficiency to cross-sections at the parton level. The differential cross-sections are compared with different Monte Carlo generators and theoretical calculations of $t\bar t$ production. The results are consistent with the majority of predictions in a wide kinematic range.