cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.70788.v1/t4
title: "Table 4" of "Measurement of jet charge in dijet events from sqrt(s)=8 TeV pp collisions with the ATLAS detector"

description: The jet charge distribution standard deviation for kappa = 0.3 and the more central jet. Values are given in units of the positron charge, e.
description: CERN-LHC. Measurements of the jet charge in dijet events in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012. The jet charge is a momentum-weighted sum of charges of tracks associated to the jet. The momentum is regulated by an exponent kappa. Measurements are reported for the average and standard deviation of the jet charge distribution as a function of the magnitude of the jet transverse momentum for kappa = 0.3, 0.5, 0.7 and separately for the more forward and more central jets (in pseudo-rapidity). The event selection is minimal, with only a requirement that the magnitude of the transverse momenta of the two leading jets be above 50 GeV and that these momenta be within 50% of each other.
DOI: 10.17182/hepdata.70788.v1/t5
title: "Table 5" of "Measurement of jet charge in dijet events from sqrt(s)=8 TeV pp collisions with the ATLAS detector"

description: The jet charge mean for kappa = 0.5 and the more forward jet. Values are given in units of the positron charge, e.
description: CERN-LHC. Measurements of the jet charge in dijet events in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012. The jet charge is a momentum-weighted sum of charges of tracks associated to the jet. The momentum is regulated by an exponent kappa. Measurements are reported for the average and standard deviation of the jet charge distribution as a function of the magnitude of the jet transverse momentum for kappa = 0.3, 0.5, 0.7 and separately for the more forward and more central jets (in pseudo-rapidity). The event selection is minimal, with only a requirement that the magnitude of the transverse momenta of the two leading jets be above 50 GeV and that these momenta be within 50% of each other.
DOI: 10.17182/hepdata.70788.v1/t10
title: "Table 10" of "Measurement of jet charge in dijet events from sqrt(s)=8 TeV pp collisions with the ATLAS detector"

description: The jet charge distribution standard deviation for kappa = 0.7 and the more forward jet. Values are given in units of the positron charge, e.
description: CERN-LHC. Measurements of the jet charge in dijet events in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012. The jet charge is a momentum-weighted sum of charges of tracks associated to the jet. The momentum is regulated by an exponent kappa. Measurements are reported for the average and standard deviation of the jet charge distribution as a function of the magnitude of the jet transverse momentum for kappa = 0.3, 0.5, 0.7 and separately for the more forward and more central jets (in pseudo-rapidity). The event selection is minimal, with only a requirement that the magnitude of the transverse momenta of the two leading jets be above 50 GeV and that these momenta be within 50% of each other.
DOI: 10.17182/hepdata.70788.v1/t11
title: "Table 11" of "Measurement of jet charge in dijet events from sqrt(s)=8 TeV pp collisions with the ATLAS detector"

description: The jet charge mean for kappa = 0.7 and the more central jet. Values are given in units of the positron charge, e.
description: CERN-LHC. Measurements of the jet charge in dijet events in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012. The jet charge is a momentum-weighted sum of charges of tracks associated to the jet. The momentum is regulated by an exponent kappa. Measurements are reported for the average and standard deviation of the jet charge distribution as a function of the magnitude of the jet transverse momentum for kappa = 0.3, 0.5, 0.7 and separately for the more forward and more central jets (in pseudo-rapidity). The event selection is minimal, with only a requirement that the magnitude of the transverse momenta of the two leading jets be above 50 GeV and that these momenta be within 50% of each other.
DOI: 10.17182/hepdata.70788.v1/t6
title: "Table 6" of "Measurement of jet charge in dijet events from sqrt(s)=8 TeV pp collisions with the ATLAS detector"

description: The jet charge distribution standard deviation for kappa = 0.5 and the more forward jet. Values are given in units of the positron charge, e.
description: CERN-LHC. Measurements of the jet charge in dijet events in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012. The jet charge is a momentum-weighted sum of charges of tracks associated to the jet. The momentum is regulated by an exponent kappa. Measurements are reported for the average and standard deviation of the jet charge distribution as a function of the magnitude of the jet transverse momentum for kappa = 0.3, 0.5, 0.7 and separately for the more forward and more central jets (in pseudo-rapidity). The event selection is minimal, with only a requirement that the magnitude of the transverse momenta of the two leading jets be above 50 GeV and that these momenta be within 50% of each other.
DOI: 10.17182/hepdata.70788.v1/t7
title: "Table 7" of "Measurement of jet charge in dijet events from sqrt(s)=8 TeV pp collisions with the ATLAS detector"

description: The jet charge mean for kappa = 0.5 and the more central jet. Values are given in units of the positron charge, e.
description: CERN-LHC. Measurements of the jet charge in dijet events in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012. The jet charge is a momentum-weighted sum of charges of tracks associated to the jet. The momentum is regulated by an exponent kappa. Measurements are reported for the average and standard deviation of the jet charge distribution as a function of the magnitude of the jet transverse momentum for kappa = 0.3, 0.5, 0.7 and separately for the more forward and more central jets (in pseudo-rapidity). The event selection is minimal, with only a requirement that the magnitude of the transverse momenta of the two leading jets be above 50 GeV and that these momenta be within 50% of each other.
DOI: 10.17182/hepdata.70788.v1/t8
title: "Table 8" of "Measurement of jet charge in dijet events from sqrt(s)=8 TeV pp collisions with the ATLAS detector"

description: The jet charge distribution standard deviation for kappa = 0.5 and the more central jet. Values are given in units of the positron charge, e.
description: CERN-LHC. Measurements of the jet charge in dijet events in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012. The jet charge is a momentum-weighted sum of charges of tracks associated to the jet. The momentum is regulated by an exponent kappa. Measurements are reported for the average and standard deviation of the jet charge distribution as a function of the magnitude of the jet transverse momentum for kappa = 0.3, 0.5, 0.7 and separately for the more forward and more central jets (in pseudo-rapidity). The event selection is minimal, with only a requirement that the magnitude of the transverse momenta of the two leading jets be above 50 GeV and that these momenta be within 50% of each other.
DOI: 10.17182/hepdata.70788.v1/t9
title: "Table 9" of "Measurement of jet charge in dijet events from sqrt(s)=8 TeV pp collisions with the ATLAS detector"

description: The jet charge mean for kappa = 0.7 and the more forward jet. Values are given in units of the positron charge, e.
description: CERN-LHC. Measurements of the jet charge in dijet events in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012. The jet charge is a momentum-weighted sum of charges of tracks associated to the jet. The momentum is regulated by an exponent kappa. Measurements are reported for the average and standard deviation of the jet charge distribution as a function of the magnitude of the jet transverse momentum for kappa = 0.3, 0.5, 0.7 and separately for the more forward and more central jets (in pseudo-rapidity). The event selection is minimal, with only a requirement that the magnitude of the transverse momenta of the two leading jets be above 50 GeV and that these momenta be within 50% of each other.
DOI: 10.17182/hepdata.70788.v1/t12
title: "Table 12" of "Measurement of jet charge in dijet events from sqrt(s)=8 TeV pp collisions with the ATLAS detector"

description: The jet charge distribution standard deviation for kappa = 0.7 and the more central jet. Values are given in units of the positron charge, e.
description: CERN-LHC. Measurements of the jet charge in dijet events in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012. The jet charge is a momentum-weighted sum of charges of tracks associated to the jet. The momentum is regulated by an exponent kappa. Measurements are reported for the average and standard deviation of the jet charge distribution as a function of the magnitude of the jet transverse momentum for kappa = 0.3, 0.5, 0.7 and separately for the more forward and more central jets (in pseudo-rapidity). The event selection is minimal, with only a requirement that the magnitude of the transverse momenta of the two leading jets be above 50 GeV and that these momenta be within 50% of each other.
DOI: 10.17182/hepdata.70833.v1/t1
title: "Table 1" of "Jet Production in ep Collisions at High Q^2 and Determination of alpha_s"

description: Normalised inclusive jet cross section in bins of $Q^{2}$.
description: DESY-HERA. The production of jets is studied in deep-inelastic ep scattering at large negative four momentum transfer squared 150
DOI: 10.17182/hepdata.70833.v1/t2
title: "Table 2" of "Jet Production in ep Collisions at High Q^2 and Determination of alpha_s"

description: Normalised 2-jet cross section in bins of $Q^{2}$.
description: DESY-HERA. The production of jets is studied in deep-inelastic ep scattering at large negative four momentum transfer squared 150
DOI: 10.17182/hepdata.70833.v1/t3
title: "Table 3" of "Jet Production in ep Collisions at High Q^2 and Determination of alpha_s"

description: Normalised 3-jet cross section in bins of $Q^{2}$.
description: DESY-HERA. The production of jets is studied in deep-inelastic ep scattering at large negative four momentum transfer squared 150
DOI: 10.17182/hepdata.70833.v1/t4
title: "Table 4" of "Jet Production in ep Collisions at High Q^2 and Determination of alpha_s"

description: 3-jet cross section normalised to 2-jet cross section in bins of $Q^{2}$.
description: DESY-HERA. The production of jets is studied in deep-inelastic ep scattering at large negative four momentum transfer squared 150
DOI: 10.17182/hepdata.70833.v1/t5
title: "Table 5" of "Jet Production in ep Collisions at High Q^2 and Determination of alpha_s"

description: Normalised inclusive jet cross section in bins of $Q^{2}$ and $P_{T}$.
description: DESY-HERA. The production of jets is studied in deep-inelastic ep scattering at large negative four momentum transfer squared 150
DOI: 10.17182/hepdata.70833.v1/t6
title: "Table 6" of "Jet Production in ep Collisions at High Q^2 and Determination of alpha_s"

description: Normalised 2-jet cross section in bins of $Q^{2}$ and $\langle P_{T} \rangle$.
description: DESY-HERA. The production of jets is studied in deep-inelastic ep scattering at large negative four momentum transfer squared 150
DOI: 10.17182/hepdata.70833.v1/t7
title: "Table 7" of "Jet Production in ep Collisions at High Q^2 and Determination of alpha_s"

description: Normalised 2-jet cross sections in bins of $Q^2$ and $\xi$.
description: DESY-HERA. The production of jets is studied in deep-inelastic ep scattering at large negative four momentum transfer squared 150
DOI: 10.17182/hepdata.70834.v1/t1
title: "Table 1" of "Centrality evolution of the charged-particle pseudorapidity density over a broad pseudorapidity range in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Measurement of $\mbox{d}N_{\mbox{ch}}/\mbox{d}\eta$ for all centralities and a broad $\eta$ range. Combined and symmetrised $\mbox{d}N_{\mbox{ch}}/\mbox{d}\eta$ over 30-90 PCT centrality from both SPD and FMD. Previously published results for 0-30 PCT over the full pseudorapidity range available elsewhere [PLB726.610]. Please note the systematic uncertainty from the centrality determination is encoded as a qualifier in the table header.
description: CERN-LHC. The centrality dependence of the charged-particle pseudorapidity density measured with ALICE in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ over a broad pseudorapidity range is presented. This Letter extends the previous results reported by ALICE to more peripheral collisions. The broad pseudorapidity range allows precise estimates of the total number of produced charged particles.
DOI: 10.17182/hepdata.70834.v1/t2
title: "Table 2" of "Centrality evolution of the charged-particle pseudorapidity density over a broad pseudorapidity range in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Full--width half--maximum of the charged--particle pseudorapidity distributions versus the average number of participants. The uncertainties on the ALICE measurements are from the fit of $f_{\text{GG}}$ only and evaluated at $95\%$ confidence level.
description: CERN-LHC. The centrality dependence of the charged-particle pseudorapidity density measured with ALICE in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ over a broad pseudorapidity range is presented. This Letter extends the previous results reported by ALICE to more peripheral collisions. The broad pseudorapidity range allows precise estimates of the total number of produced charged particles.
DOI: 10.17182/hepdata.70834.v1/t3
title: "Table 3" of "Centrality evolution of the charged-particle pseudorapidity density over a broad pseudorapidity range in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: The charged--particle pseudorapidity density distributions scaled by the average number of participants in various pseudorapidity intervals as a function of the number of participants. Data for the 0 to 30 PCT most central events, and in ETARAP &lt; 0.5 is available in previously published results [PLB726.610,PRC88.044910]. The uncertainties on $\left\langle N_{\text{part}}\right\rangle$ from the Glauber calculations not included (see [PRC88.044910]).
description: CERN-LHC. The centrality dependence of the charged-particle pseudorapidity density measured with ALICE in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ over a broad pseudorapidity range is presented. This Letter extends the previous results reported by ALICE to more peripheral collisions. The broad pseudorapidity range allows precise estimates of the total number of produced charged particles.
DOI: 10.17182/hepdata.70834.v1/t4
title: "Table 4" of "Centrality evolution of the charged-particle pseudorapidity density over a broad pseudorapidity range in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Extrapolation to the total number of charged particles as a function of the number of participating nucleons [PRC88.044909]. Data on the 0 to 30 PCT most central events are available in previous publication [PLB726.610].
description: CERN-LHC. The centrality dependence of the charged-particle pseudorapidity density measured with ALICE in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ over a broad pseudorapidity range is presented. This Letter extends the previous results reported by ALICE to more peripheral collisions. The broad pseudorapidity range allows precise estimates of the total number of produced charged particles.
DOI: 10.17182/hepdata.70846.v1/t1
title: "Table 1" of "Rapidity and transverse-momentum dependence of the inclusive J/$\mathbf{\psi}$ nuclear modification factor in p-Pb collisions at $\mathbf{\sqrt{\textit{s}_{NN}}}=5.02$ TeV"

description: $p_{\rm T}$-differential inclusive cross section ${\rm d}^2\sigma^{J/\psi}/{\rm d}y{\rm d}p_{T}$ in the backward rapidity range (-4.46&lt;$y_{\rm cms}$&lt;-2.96). 
The first uncertainty is statistical, the second one is the $p_{\rm T}$-uncorrelated systematic uncertainty, while the third is the $p_{\rm T}$-correlated one.
description: CERN-LHC. Measurement of the rapidity and transverse-momentum dependence of the inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at CERN LHC, in three center-of-mass rapidity ($y_{\rm cms}$) regions, down to zero $p_{\rm T}$. The measurements are performed at forward (2.03&lt;$y_{\rm cms}$&lt;3.53), mid (-1.37&lt;$y_{\rm cms}$&lt;0.43) and backward (-4.46&lt;$y_{\rm cms}$&lt;-2.96) centre of mass rapidities.
DOI: 10.17182/hepdata.70846.v1/t2
title: "Table 2" of "Rapidity and transverse-momentum dependence of the inclusive J/$\mathbf{\psi}$ nuclear modification factor in p-Pb collisions at $\mathbf{\sqrt{\textit{s}_{NN}}}=5.02$ TeV"

description: $p_{\rm T}$-differential inclusive cross section ${\rm d}^2\sigma^{J/\psi}/{\rm d}y{\rm d}p_{T}$ in the mid-rapidity range (-1.37&lt;$y_{\rm cms}$&lt;0.43). 
The first uncertainty is statistical, the second one is the $p_{\rm T}$-uncorrelated systematic uncertainty, while the third is the $p_{\rm T}$-correlated one.
description: CERN-LHC. Measurement of the rapidity and transverse-momentum dependence of the inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at CERN LHC, in three center-of-mass rapidity ($y_{\rm cms}$) regions, down to zero $p_{\rm T}$. The measurements are performed at forward (2.03&lt;$y_{\rm cms}$&lt;3.53), mid (-1.37&lt;$y_{\rm cms}$&lt;0.43) and backward (-4.46&lt;$y_{\rm cms}$&lt;-2.96) centre of mass rapidities.
DOI: 10.17182/hepdata.70846.v1/t3
title: "Table 3" of "Rapidity and transverse-momentum dependence of the inclusive J/$\mathbf{\psi}$ nuclear modification factor in p-Pb collisions at $\mathbf{\sqrt{\textit{s}_{NN}}}=5.02$ TeV"

description: $p_{\rm T}$-differential inclusive cross section ${\rm d}^2\sigma^{J/\psi}/{\rm d}y{\rm d}p_{T}$ in the forward rapidity range (2.03&lt;$y_{\rm cms}$&lt;3.53). 
The first uncertainty is statistical, the second one is the $p_{\rm T}$-uncorrelated systematic uncertainty, while the third is the $p_{\rm T}$-correlated one.
description: CERN-LHC. Measurement of the rapidity and transverse-momentum dependence of the inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at CERN LHC, in three center-of-mass rapidity ($y_{\rm cms}$) regions, down to zero $p_{\rm T}$. The measurements are performed at forward (2.03&lt;$y_{\rm cms}$&lt;3.53), mid (-1.37&lt;$y_{\rm cms}$&lt;0.43) and backward (-4.46&lt;$y_{\rm cms}$&lt;-2.96) centre of mass rapidities.
DOI: 10.17182/hepdata.70846.v1/t4
title: "Table 4" of "Rapidity and transverse-momentum dependence of the inclusive J/$\mathbf{\psi}$ nuclear modification factor in p-Pb collisions at $\mathbf{\sqrt{\textit{s}_{NN}}}=5.02$ TeV"

description: $p_{\rm T}$ dependence of the J/$\psi$ nuclear modification factor $R_{\rm pA}$ in the backward rapidity range (-4.46&lt;$y_{\rm cms}$&lt;-2.96). 
The first uncertainty is statistical, the second one is the $p_{\rm T}$-uncorrelated systematic uncertainty, the third is the partially $p_{\rm T}$-correlated, while the fourth is the $p_{\rm T}$-correlated one.
description: CERN-LHC. Measurement of the rapidity and transverse-momentum dependence of the inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at CERN LHC, in three center-of-mass rapidity ($y_{\rm cms}$) regions, down to zero $p_{\rm T}$. The measurements are performed at forward (2.03&lt;$y_{\rm cms}$&lt;3.53), mid (-1.37&lt;$y_{\rm cms}$&lt;0.43) and backward (-4.46&lt;$y_{\rm cms}$&lt;-2.96) centre of mass rapidities.
DOI: 10.17182/hepdata.70846.v1/t5
title: "Table 5" of "Rapidity and transverse-momentum dependence of the inclusive J/$\mathbf{\psi}$ nuclear modification factor in p-Pb collisions at $\mathbf{\sqrt{\textit{s}_{NN}}}=5.02$ TeV"

description: $p_{\rm T}$ dependence of the J/$\psi$ nuclear modification factor $R_{\rm pA}$ in the mid-rapidity range (-1.37&lt;$y_{\rm cms}$&lt;-0.43). 
The first uncertainty is statistical, the second one is the $p_{\rm T}$-uncorrelated systematic uncertainty, the third is the $p_{\rm T}$-correlated one.
description: CERN-LHC. Measurement of the rapidity and transverse-momentum dependence of the inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at CERN LHC, in three center-of-mass rapidity ($y_{\rm cms}$) regions, down to zero $p_{\rm T}$. The measurements are performed at forward (2.03&lt;$y_{\rm cms}$&lt;3.53), mid (-1.37&lt;$y_{\rm cms}$&lt;0.43) and backward (-4.46&lt;$y_{\rm cms}$&lt;-2.96) centre of mass rapidities.
DOI: 10.17182/hepdata.70846.v1/t6
title: "Table 6" of "Rapidity and transverse-momentum dependence of the inclusive J/$\mathbf{\psi}$ nuclear modification factor in p-Pb collisions at $\mathbf{\sqrt{\textit{s}_{NN}}}=5.02$ TeV"

description: $p_{\rm T}$ dependence of the J/$\psi$ nuclear modification factor $R_{\rm pA}$ in the forward rapidity range (2.03&lt;$y_{\rm cms}$&lt;3.53). 
The first uncertainty is statistical, the second one is the $p_{\rm T}$-uncorrelated systematic uncertainty, the third is the partially $p_{\rm T}$-correlated, while the fourth is the $p_{\rm T}$-correlated one.
description: CERN-LHC. Measurement of the rapidity and transverse-momentum dependence of the inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at CERN LHC, in three center-of-mass rapidity ($y_{\rm cms}$) regions, down to zero $p_{\rm T}$. The measurements are performed at forward (2.03&lt;$y_{\rm cms}$&lt;3.53), mid (-1.37&lt;$y_{\rm cms}$&lt;0.43) and backward (-4.46&lt;$y_{\rm cms}$&lt;-2.96) centre of mass rapidities.
DOI: 10.17182/hepdata.70846.v1/t7
title: "Table 7" of "Rapidity and transverse-momentum dependence of the inclusive J/$\mathbf{\psi}$ nuclear modification factor in p-Pb collisions at $\mathbf{\sqrt{\textit{s}_{NN}}}=5.02$ TeV"

description: Estimate of the $p_{\rm T}$-dependence of the Cold Nuclear Matter effects in Pb-Pb collisions calculated as $R^2_{\rm pPb}$. 
The first uncertainty is statistical, the second one is the $p_{\rm T}$-uncorrelated systematic uncertainty, the third is the $p_{\rm T}$-correlated one.
description: CERN-LHC. Measurement of the rapidity and transverse-momentum dependence of the inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at CERN LHC, in three center-of-mass rapidity ($y_{\rm cms}$) regions, down to zero $p_{\rm T}$. The measurements are performed at forward (2.03&lt;$y_{\rm cms}$&lt;3.53), mid (-1.37&lt;$y_{\rm cms}$&lt;0.43) and backward (-4.46&lt;$y_{\rm cms}$&lt;-2.96) centre of mass rapidities.
DOI: 10.17182/hepdata.70846.v1/t8
title: "Table 8" of "Rapidity and transverse-momentum dependence of the inclusive J/$\mathbf{\psi}$ nuclear modification factor in p-Pb collisions at $\mathbf{\sqrt{\textit{s}_{NN}}}=5.02$ TeV"

description: Estimate of the $p_{\rm T}$-dependence of the Cold Nuclear Matter effects in Pb-Pb collisions calculated as $R_{\rm pPb}$(-4.46
description: CERN-LHC. Measurement of the rapidity and transverse-momentum dependence of the inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at CERN LHC, in three center-of-mass rapidity ($y_{\rm cms}$) regions, down to zero $p_{\rm T}$. The measurements are performed at forward (2.03&lt;$y_{\rm cms}$&lt;3.53), mid (-1.37&lt;$y_{\rm cms}$&lt;0.43) and backward (-4.46&lt;$y_{\rm cms}$&lt;-2.96) centre of mass rapidities.