cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.133032.v1/t7
title: "Table 7" of "Underlying-event properties in pp and p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Fig. A1: Number density $N_{\rm ch}$ (left) and $\Sigma p_{\rm T}$ (right) distributions as a function of $p_{\rm T}^{\rm trig}$ in Transverse, Away, and Toward regions for $p_{\rm T} &gt;$ 0.15 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.
description: This article reports about the properties of the underlying event measured with ALICE at
the LHC in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}= 5.02$ TeV. The event activity, quantified by charged-particle number and summed-$p_{\rm T}$ densities, is measured
as a function of the leading-particle transverse momentum ($p_{\rm T}^{\rm trig}$). These quantities are studied in three azimuthal-angle regions relative to the leading particle in the event: toward, away, and transverse. Results are presented for
three different $p_{\rm T}$ thresholds (0.15, 0.5 and 1 GeV/$c$) at mid-pseudorapidity ($|\\eta|&lt;0.8$).
The event activity in the transverse region, which is the most sensitive to the underlying event, exhibits similar behaviour in both pp and p-Pb
collisions, namely, a steep increase with $p_{\rm T}^{\rm trig}$ for low $p_{\rm T}^{\rm trig}$, followed by a saturation at $p_{\rm T}^{\rm trig} \approx 5$ GeV/$c$. The results from pp collisions are
compared with existing measurements at other centre-of-mass energies. The quantities in the toward and away regions are also analyzed after
the subtraction of the contribution measured in the transverse region. The remaining jet-like particle densities are consistent in pp and p-Pb
collisions for $p_{\rm T}^{\rm trig}&gt;10$ GeV/$c$, whereas for lower $p_{\rm T}^{\rm trig}$ values
the event activity is slightly higher in pPb than in pp collisions. The measurements are compared with predictions from the Monte Carlo event generators.
DOI: 10.17182/hepdata.133032.v1/t8
title: "Table 8" of "Underlying-event properties in pp and p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Fig. A2: Number density $N_{\rm ch}$ (left) and $\Sigma p_{\rm T}$ (right) distributions as a function of $p_{\rm T}^{\rm trig}$ in Transverse, Away, and Toward regions for $p_{\rm T} &gt;$ 1.0 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.
description: This article reports about the properties of the underlying event measured with ALICE at
the LHC in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}= 5.02$ TeV. The event activity, quantified by charged-particle number and summed-$p_{\rm T}$ densities, is measured
as a function of the leading-particle transverse momentum ($p_{\rm T}^{\rm trig}$). These quantities are studied in three azimuthal-angle regions relative to the leading particle in the event: toward, away, and transverse. Results are presented for
three different $p_{\rm T}$ thresholds (0.15, 0.5 and 1 GeV/$c$) at mid-pseudorapidity ($|\\eta|&lt;0.8$).
The event activity in the transverse region, which is the most sensitive to the underlying event, exhibits similar behaviour in both pp and p-Pb
collisions, namely, a steep increase with $p_{\rm T}^{\rm trig}$ for low $p_{\rm T}^{\rm trig}$, followed by a saturation at $p_{\rm T}^{\rm trig} \approx 5$ GeV/$c$. The results from pp collisions are
compared with existing measurements at other centre-of-mass energies. The quantities in the toward and away regions are also analyzed after
the subtraction of the contribution measured in the transverse region. The remaining jet-like particle densities are consistent in pp and p-Pb
collisions for $p_{\rm T}^{\rm trig}&gt;10$ GeV/$c$, whereas for lower $p_{\rm T}^{\rm trig}$ values
the event activity is slightly higher in pPb than in pp collisions. The measurements are compared with predictions from the Monte Carlo event generators.
DOI: 10.17182/hepdata.133032.v1/t9
title: "Table 9" of "Underlying-event properties in pp and p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Fig. A3: Number density $N_{\rm ch}$ (left) and $\Sigma p_{\rm T}$ (right) distributions as a function of $p_{\rm T}^{\rm trig}$ in Transverse, Away, and Toward regions for $p_{\rm T} &gt;$ 0.15 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.
description: This article reports about the properties of the underlying event measured with ALICE at
the LHC in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}= 5.02$ TeV. The event activity, quantified by charged-particle number and summed-$p_{\rm T}$ densities, is measured
as a function of the leading-particle transverse momentum ($p_{\rm T}^{\rm trig}$). These quantities are studied in three azimuthal-angle regions relative to the leading particle in the event: toward, away, and transverse. Results are presented for
three different $p_{\rm T}$ thresholds (0.15, 0.5 and 1 GeV/$c$) at mid-pseudorapidity ($|\\eta|&lt;0.8$).
The event activity in the transverse region, which is the most sensitive to the underlying event, exhibits similar behaviour in both pp and p-Pb
collisions, namely, a steep increase with $p_{\rm T}^{\rm trig}$ for low $p_{\rm T}^{\rm trig}$, followed by a saturation at $p_{\rm T}^{\rm trig} \approx 5$ GeV/$c$. The results from pp collisions are
compared with existing measurements at other centre-of-mass energies. The quantities in the toward and away regions are also analyzed after
the subtraction of the contribution measured in the transverse region. The remaining jet-like particle densities are consistent in pp and p-Pb
collisions for $p_{\rm T}^{\rm trig}&gt;10$ GeV/$c$, whereas for lower $p_{\rm T}^{\rm trig}$ values
the event activity is slightly higher in pPb than in pp collisions. The measurements are compared with predictions from the Monte Carlo event generators.
DOI: 10.17182/hepdata.133033.v1/t1
title: "Table 1" of "Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$
$60
description: No data abstract available.
DOI: 10.17182/hepdata.133033.v1/t2
title: "Table 2" of "Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$
$60
description: No data abstract available.
DOI: 10.17182/hepdata.133033.v1/t3
title: "Table 3" of "Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$
$60
description: No data abstract available.
DOI: 10.17182/hepdata.133033.v1/t4
title: "Table 4" of "Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$
$60
description: No data abstract available.
DOI: 10.17182/hepdata.133033.v1/t5
title: "Table 5" of "Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$
$60
description: No data abstract available.
DOI: 10.17182/hepdata.133033.v1/t6
title: "Table 6" of "Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$
$60
description: No data abstract available.
DOI: 10.17182/hepdata.133033.v1/t7
title: "Table 7" of "Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$
$60
description: No data abstract available.
DOI: 10.17182/hepdata.133033.v1/t8
title: "Table 8" of "Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$
$60
description: No data abstract available.
DOI: 10.25345/c53r0q688
title: MassIVE MSV000099913 - S. elongatus PCC 7942 Limited Proteolysis (LiP) Proteomics - Light vs Dark with Reduced/Non-reduced preparations in Dense Cultures
title: LiP experimental assays investigating structural alterations in Dense Light vs Dense Dark growth conditions with Reduced/Non-reduced preparations. Samples are Synechococcus elongatus PCC7942 cell lysates (BTO:0004304). Purpose: Probing light- and dark-induced conformational changes in dense cyanobacterial cultures using reduced and non-reduced sample preparation protocols. Technique: Limited proteolysis (LiP). Other details: Nonspecific protease used was pronase at an enzyme:substrate ratio of 1:200. The reduced samples were treated with 100 mM DTT prior to LiP. Data was searched with MaxQuant (using Label free quantification- Match between runs, LFQ-MBR).
DOI: 10.17182/hepdata.130653.v1/t1
title: "Figure 3" of "Multiplicity dependence of charged-particle jet production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Inclusive charged-particle jet cross sections in pp collisions at $\sqrt{s}$ = 13 TeV using the anti-kT algorithm for different jet resolution parameters R from 0.2 to 0.7, with UE subtraction. Statistical uncertainties are displayed as vertical error bars. The total systematic uncertainties are shown as solid boxes around the data points.
description: No data abstract available.
DOI: 10.17182/hepdata.130653.v1/t2
title: "Figure 5" of "Multiplicity dependence of charged-particle jet production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Ratio of charged-particle jet cross section for resolution parameter R = 0.2 to other radii R = X, with X ranging from 0.3 to 0.7, after UE subtraction. Data are compared with LO (PYTHIA) and NLO (POWHEG+PYTHIA8) predictions as shown in the bottom panels. The systematic uncertainties of the cross section ratios from data are indicated by solid boxes around data points in the upper panel and shaded bands around unity in the mid and lower panels. No uncertainties are shown for theoretical predictions for better visibility.
description: No data abstract available.
DOI: 10.17182/hepdata.130653.v1/t3
title: "Figure 7" of "Multiplicity dependence of charged-particle jet production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Charged-particle jet yields in different V0M multiplicity percentile intervals for resolution parameters R varied from 0.2 to 0.7 in pp collisions at s = 13 TeV. Statistical and total systematic uncertainties are shown as vertical error bars and boxes around the data points, respectively.
description: No data abstract available.
DOI: 10.17182/hepdata.130653.v1/t4
title: "Figure 8" of "Multiplicity dependence of charged-particle jet production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Ratio of charged-particle jet yield measured in different multiplicity classes with respect to that in MB events as a function of pT for different resolution parameters R from 0.2 to 0.7. Statistical and total systematic uncertainties are shown as vertical error bars and boxes around the data points, respectively.
description: No data abstract available.
DOI: 10.17182/hepdata.133033.v1/t10
title: "Table 10" of "Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$
$60
description: No data abstract available.
DOI: 10.17182/hepdata.133033.v1/t11
title: "Table 11" of "Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$
$60
description: No data abstract available.
DOI: 10.17182/hepdata.133033.v1/t12
title: "Table 12" of "Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$
$60
description: No data abstract available.
DOI: 10.17182/hepdata.133033.v1/t9
title: "Table 9" of "Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$
$60
description: No data abstract available.
DOI: 10.17182/hepdata.130653.v1/t5
title: "Figure 9" of "Multiplicity dependence of charged-particle jet production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Ratios of charged-particle jet spectra with R = 0.2 to that with other jet resolution parameters R from 0.3 to 0.7, shown in different V0M multiplicity classes. Statistical and systematic uncertainties are shown as vertical error bars and boxes around the data points, respectively
description: No data abstract available.
DOI: 10.17182/hepdata.130653.v1/t6
title: "Figure 12" of "Multiplicity dependence of charged-particle jet production in pp collisions at $\sqrt{s} = 13$ TeV"

description: a) Integrated jet yields, and b) $$ of jets with 5 $
description: No data abstract available.
DOI: 10.17182/hepdata.130653.v1/t7
title: "Figure 13" of "Multiplicity dependence of charged-particle jet production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Self-normalised jet yields as a function of the self-normalised charged-particle multiplicity for different resolution parameters R varied from 0.2 to 0.7 in different jet pT intervals: a) 5 $
description: No data abstract available.
DOI: 10.17182/hepdata.130653.v1/t8
title: "Figure A1" of "Multiplicity dependence of charged-particle jet production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Inclusive charged-particle jet cross sections in pp collisions at $\sqrt{s}$ = 13 TeV using the anti-kT algorithm for different jet resolution parameters R from 0.2 to 0.7, without UE subtraction. Statistical uncertainties are displayed as vertical error bars. The total systematic uncertainties are shown as solid boxes around the data points.
description: No data abstract available.
DOI: 10.17182/hepdata.130653.v1/t9
title: "Figure A3" of "Multiplicity dependence of charged-particle jet production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Ratio of charged-particle jet cross section for resolution parameter R = 0.2 to other radii R = X, with X ranging from 0.3 to 0.7, without UE subtraction. Data are compared with LO (PYTHIA) and NLO (POWHEG+PYTHIA8) predictions as shown in the bottom panels. The systematic uncertainties of the cross section ratios from data are indicated by solid boxes around data points in the upper panel and shaded bands around unity in the mid and lower panels. No uncertainties are shown for theoretical predictions for better visibility.
description: No data abstract available.
DOI: 10.17182/hepdata.138404.v2/t1
title: "Table 1a" of "Constraining hadronization mechanisms with $\rm \Lambda_{\rm c}^{+}$/D$^0$ production ratios in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Transverse-momentum-differential production yields of prompt $\mathrm{\Lambda_c^+}$ in central (0--10\%) and mid-central (30--50\%) Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV.
description: The production of prompt $\rm \Lambda_{\rm c}^{+}$ baryons at midrapidity ($|y|&lt;0.5$) was measured in central (0--10\%) and mid-central (30--50\%) Pb--Pb collisions at the center-of-mass energy per nucleon--nucleon pair $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV with the ALICE detector. The $\rm \Lambda_{\rm c}^{+}$ production yield, the $\rm \Lambda_{\rm c}^{+} / D^0$ production ratio, and the $\rm \Lambda_{\rm c}^{+}$ nuclear modification factor $R_{\rm AA}$ are reported. The results are more precise and more differential in transverse momentum ($p_{\rm T}$) and centrality with respect to previous measurements. The $\rm \Lambda_{\rm c}^{+} / D^0$ ratio, which is enhanced with respect to the pp measurement for $4
DOI: 10.17182/hepdata.138404.v2/t2
title: "Table 1b" of "Constraining hadronization mechanisms with $\rm \Lambda_{\rm c}^{+}$/D$^0$ production ratios in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: The $\mathrm{\Lambda_c^+ / D^0}$ production yield ratio in central (0--10\%) and mid-central (30--50\%) Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV.
description: The production of prompt $\rm \Lambda_{\rm c}^{+}$ baryons at midrapidity ($|y|&lt;0.5$) was measured in central (0--10\%) and mid-central (30--50\%) Pb--Pb collisions at the center-of-mass energy per nucleon--nucleon pair $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV with the ALICE detector. The $\rm \Lambda_{\rm c}^{+}$ production yield, the $\rm \Lambda_{\rm c}^{+} / D^0$ production ratio, and the $\rm \Lambda_{\rm c}^{+}$ nuclear modification factor $R_{\rm AA}$ are reported. The results are more precise and more differential in transverse momentum ($p_{\rm T}$) and centrality with respect to previous measurements. The $\rm \Lambda_{\rm c}^{+} / D^0$ ratio, which is enhanced with respect to the pp measurement for $4
DOI: 10.17182/hepdata.138404.v2/t3
title: "Table 2" of "Constraining hadronization mechanisms with $\rm \Lambda_{\rm c}^{+}$/D$^0$ production ratios in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: The nuclear modification factor of prompt $\mathrm{\Lambda_c^+}$ as a function transverse momentum in central (0--10\%) and mid-central (30--50\%) Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV.
description: The production of prompt $\rm \Lambda_{\rm c}^{+}$ baryons at midrapidity ($|y|&lt;0.5$) was measured in central (0--10\%) and mid-central (30--50\%) Pb--Pb collisions at the center-of-mass energy per nucleon--nucleon pair $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV with the ALICE detector. The $\rm \Lambda_{\rm c}^{+}$ production yield, the $\rm \Lambda_{\rm c}^{+} / D^0$ production ratio, and the $\rm \Lambda_{\rm c}^{+}$ nuclear modification factor $R_{\rm AA}$ are reported. The results are more precise and more differential in transverse momentum ($p_{\rm T}$) and centrality with respect to previous measurements. The $\rm \Lambda_{\rm c}^{+} / D^0$ ratio, which is enhanced with respect to the pp measurement for $4
DOI: 10.17182/hepdata.138866.v1/t1
title: "Table 1" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for WTA$\textendash$Standard for jets of $R=0.2$, in the interval $20
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t3
title: "Table 3" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for WTA$\textendash$SD with grooming setting ($z_{\rm cut}=0.1,\beta=1$) for jets of $R=0.2$, in the interval $20
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t2
title: "Table 2" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for WTA$\textendash$SD with grooming setting ($z_{\rm cut}=0.1,\beta=0$) for jets of $R=0.2$, in the interval $20
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t4
title: "Table 4" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for WTA$\textendash$SD with grooming setting ($z_{\rm cut}=0.1,\beta=2$) for jets of $R=0.2$, in the interval $20
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t5
title: "Table 5" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for WTA$\textendash$SD with grooming setting ($z_{\rm cut}=0.1,\beta=3$) for jets of $R=0.2$, in the interval $20
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t6
title: "Table 6" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for WTA$\textendash$SD with grooming setting ($z_{\rm cut}=0.2,\beta=1$) for jets of $R=0.2$, in the interval $20
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t7
title: "Table 7" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for WTA$\textendash$SD with grooming setting ($z_{\rm cut}=0.3,\beta=1$) for jets of $R=0.2$, in the interval $20
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t8
title: "Table 8" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for Standard$\textendash$SD with grooming setting ($z_{\rm cut}=0.3,\beta=1$) for jets of $R=0.2$, in the interval $20
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t9
title: "Table 9" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for Standard$\textendash$SD with grooming setting ($z_{\rm cut}=0.2,\beta=1$) for jets of $R=0.2$, in the interval $20
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t10
title: "Table 10" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for Standard$\textendash$SD with grooming setting ($z_{\rm cut}=0.1,\beta=0$) for jets of $R=0.2$, in the interval $20
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t11
title: "Table 11" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for Standard$\textendash$SD with grooming setting ($z_{\rm cut}=0.1,\beta=1$) for jets of $R=0.2$, in the interval $20
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t12
title: "Table 12" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for Standard$\textendash$SD with grooming setting ($z_{\rm cut}=0.1,\beta=2$) for jets of $R=0.2$, in the interval $20
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t13
title: "Table 13" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for Standard$\textendash$SD with grooming setting ($z_{\rm cut}=0.1,\beta=3$) for jets of $R=0.2$, in the interval $20
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t14
title: "Table 14" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for WTA$\textendash$Standard for jets of $R=0.2$, in the interval $40
description: No data abstract available.
DOI: 10.17182/hepdata.138866.v1/t15
title: "Table 15" of "Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $\Delta R_{\rm axis}$ distribution for WTA$\textendash$SD with grooming setting ($z_{\rm cut}=0.1,\beta=0$) for jets of $R=0.2$, in the interval $40
description: No data abstract available.