cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.79809.v1/t46
title: "Table 7a" of "Search for top squarks and dark matter particles in opposite-charge dilepton final states at $\sqrt{s}=$ 13 TeV"

description: Table 7 (upper). Covariance matrix for the background prediction in aggregate signal regions.
description: CERN-LHC. Search for top squarks and dark matter particles in opposite-charge dilepton final states at sqrt(s) = 13 TeV

A search for new physics is presented in final states with two oppositely charged leptons (electrons or muons), jets identified as originating from b quarks, and missing transverse momentum (pTmiss).
The search uses proton-proton collision data at 13 TeV amounting to 35.9 $fb^{−1}$ of integrated luminosity collected using the CMS detector in 2016.
Hypothetical signal events are efficiently separated from the dominant ttbar background with requirements on pTmiss and transverse mass variables.
No significant deviation is observed from the expected background.
Exclusion limits are set in the context of simplified supersymmetric models with pair-produced top squarks.
For top squarks, decaying exclusively to a top quark and a neutralino, exclusion limits are placed at 95% confidence level on the mass of the lightest top squark up to 800 GeV and on the lightest neutralino up to 360 GeV.
These results, combined with searches in the single-lepton and all-jet final states, raise the exclusion limits up to 1050 GeV for the lightest top squark and up to 500 GeV for the lightest neutralino.
For top squarks undergoing a cascade decay through charginos and sleptons, the mass limits reach up to 1300 GeV for top squarks and up to 800 GeV for the lightest neutralino.
The results are also interpreted in a simplified model with a dark matter (DM) particle coupled to the top quark through a scalar or pseudoscalar mediator.
For light DM, mediator masses up to 100 (50) GeV are excluded for scalar (pseudoscalar) mediators.
The result for the scalar mediator achieves some of the most stringent limits to date in this model.
DOI: 10.17182/hepdata.79809.v1/t47
title: "Table 7b" of "Search for top squarks and dark matter particles in opposite-charge dilepton final states at $\sqrt{s}=$ 13 TeV"

description: Table 7 (lower). Correlation matrix for the background prediction in aggregate signal regions.
description: CERN-LHC. Search for top squarks and dark matter particles in opposite-charge dilepton final states at sqrt(s) = 13 TeV

A search for new physics is presented in final states with two oppositely charged leptons (electrons or muons), jets identified as originating from b quarks, and missing transverse momentum (pTmiss).
The search uses proton-proton collision data at 13 TeV amounting to 35.9 $fb^{−1}$ of integrated luminosity collected using the CMS detector in 2016.
Hypothetical signal events are efficiently separated from the dominant ttbar background with requirements on pTmiss and transverse mass variables.
No significant deviation is observed from the expected background.
Exclusion limits are set in the context of simplified supersymmetric models with pair-produced top squarks.
For top squarks, decaying exclusively to a top quark and a neutralino, exclusion limits are placed at 95% confidence level on the mass of the lightest top squark up to 800 GeV and on the lightest neutralino up to 360 GeV.
These results, combined with searches in the single-lepton and all-jet final states, raise the exclusion limits up to 1050 GeV for the lightest top squark and up to 500 GeV for the lightest neutralino.
For top squarks undergoing a cascade decay through charginos and sleptons, the mass limits reach up to 1300 GeV for top squarks and up to 800 GeV for the lightest neutralino.
The results are also interpreted in a simplified model with a dark matter (DM) particle coupled to the top quark through a scalar or pseudoscalar mediator.
For light DM, mediator masses up to 100 (50) GeV are excluded for scalar (pseudoscalar) mediators.
The result for the scalar mediator achieves some of the most stringent limits to date in this model.
DOI: 10.17182/hepdata.79809.v1/t49
title: "Covariance" of "Search for top squarks and dark matter particles in opposite-charge dilepton final states at $\sqrt{s}=$ 13 TeV"

description: Additional Figure 2. Covariance matrix of the 13 signal regions, split into same-flavor (SF) and different-flavor (DF) regions.
description: CERN-LHC. Search for top squarks and dark matter particles in opposite-charge dilepton final states at sqrt(s) = 13 TeV

A search for new physics is presented in final states with two oppositely charged leptons (electrons or muons), jets identified as originating from b quarks, and missing transverse momentum (pTmiss).
The search uses proton-proton collision data at 13 TeV amounting to 35.9 $fb^{−1}$ of integrated luminosity collected using the CMS detector in 2016.
Hypothetical signal events are efficiently separated from the dominant ttbar background with requirements on pTmiss and transverse mass variables.
No significant deviation is observed from the expected background.
Exclusion limits are set in the context of simplified supersymmetric models with pair-produced top squarks.
For top squarks, decaying exclusively to a top quark and a neutralino, exclusion limits are placed at 95% confidence level on the mass of the lightest top squark up to 800 GeV and on the lightest neutralino up to 360 GeV.
These results, combined with searches in the single-lepton and all-jet final states, raise the exclusion limits up to 1050 GeV for the lightest top squark and up to 500 GeV for the lightest neutralino.
For top squarks undergoing a cascade decay through charginos and sleptons, the mass limits reach up to 1300 GeV for top squarks and up to 800 GeV for the lightest neutralino.
The results are also interpreted in a simplified model with a dark matter (DM) particle coupled to the top quark through a scalar or pseudoscalar mediator.
For light DM, mediator masses up to 100 (50) GeV are excluded for scalar (pseudoscalar) mediators.
The result for the scalar mediator achieves some of the most stringent limits to date in this model.
DOI: 10.17182/hepdata.79809.v1/t48
title: "Correlation" of "Search for top squarks and dark matter particles in opposite-charge dilepton final states at $\sqrt{s}=$ 13 TeV"

description: Additional Figure 1. Correlation matrix of the 13 signal regions, split into same-flavor (SF) and different-flavor (DF) regions.
description: CERN-LHC. Search for top squarks and dark matter particles in opposite-charge dilepton final states at sqrt(s) = 13 TeV

A search for new physics is presented in final states with two oppositely charged leptons (electrons or muons), jets identified as originating from b quarks, and missing transverse momentum (pTmiss).
The search uses proton-proton collision data at 13 TeV amounting to 35.9 $fb^{−1}$ of integrated luminosity collected using the CMS detector in 2016.
Hypothetical signal events are efficiently separated from the dominant ttbar background with requirements on pTmiss and transverse mass variables.
No significant deviation is observed from the expected background.
Exclusion limits are set in the context of simplified supersymmetric models with pair-produced top squarks.
For top squarks, decaying exclusively to a top quark and a neutralino, exclusion limits are placed at 95% confidence level on the mass of the lightest top squark up to 800 GeV and on the lightest neutralino up to 360 GeV.
These results, combined with searches in the single-lepton and all-jet final states, raise the exclusion limits up to 1050 GeV for the lightest top squark and up to 500 GeV for the lightest neutralino.
For top squarks undergoing a cascade decay through charginos and sleptons, the mass limits reach up to 1300 GeV for top squarks and up to 800 GeV for the lightest neutralino.
The results are also interpreted in a simplified model with a dark matter (DM) particle coupled to the top quark through a scalar or pseudoscalar mediator.
For light DM, mediator masses up to 100 (50) GeV are excluded for scalar (pseudoscalar) mediators.
The result for the scalar mediator achieves some of the most stringent limits to date in this model.
DOI: 10.17182/hepdata.79847.v1/t1
title: "Table 1" of "Measurement of the $W^+W^-$ production cross section in $pp$ collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV with the ATLAS experiment"

description: The measured fiducial cross section P P --&gt; WW --&gt; $e^\pm \mu^\mp$.
description: No description provided.
DOI: 10.17182/hepdata.79847.v1/t2
title: "Table 2" of "Measurement of the $W^+W^-$ production cross section in $pp$ collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV with the ATLAS experiment"

description: Detailed breakdown of the systematic uncertainties in the fiducial cross-section measurement as a result of the simultaneous fit to signal and control regions. Summarised in Table 4 of the paper.
description: No description provided.
DOI: 10.17182/hepdata.79847.v1/t3
title: "Table 3" of "Measurement of the $W^+W^-$ production cross section in $pp$ collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV with the ATLAS experiment"

description: Systematic uncertainty correlation matrix for the fiducial cross section.
description: No description provided.
DOI: 10.17182/hepdata.79847.v1/t4
title: "Table 4" of "Measurement of the $W^+W^-$ production cross section in $pp$ collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV with the ATLAS experiment"

description: Extrapolation factors AWW -- used to extrapolate from the fiducial particle level to the total phase space.
description: No description provided.
DOI: 10.17182/hepdata.79847.v1/t5
title: "Table 5" of "Measurement of the $W^+W^-$ production cross section in $pp$ collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV with the ATLAS experiment"

description: Cross sections and ratios (13/8 TeV) -- experimental and PDF uncertainties are treated as uncorrelated, scale uncertainties are correlated between the different centre-of-mass energies.
description: No description provided.
DOI: 10.17182/hepdata.79857.v1/t1
title: "Table 1" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q (\kappa=1.0)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t2
title: "Table 2" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q (\kappa=0.6)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t3
title: "Table 3" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q (\kappa=0.3)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t4
title: "Table 4" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q_L (\kappa=1.0)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t5
title: "Table 5" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q_L (\kappa=0.6)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t6
title: "Table 6" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q_L (\kappa=0.3)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t7
title: "Table 7" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q_T (\kappa=1.0)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t10
title: "Table 10" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q (\kappa=0.6)$ of leading jet with 400 &lt; pT &lt; 700 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t11
title: "Table 11" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q (\kappa=0.6)$ of leading jet with 700 &lt; pT &lt; 1000 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t12
title: "Table 12" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q (\kappa=0.6)$ of leading jet with 1000 &lt; pT &lt; 1800 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t13
title: "Table 13" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q_L (\kappa=0.6)$ of leading jet with 400 &lt; pT &lt; 700 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t14
title: "Table 14" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q_L (\kappa=0.6)$ of leading jet with 700 &lt; pT &lt; 1000 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t8
title: "Table 8" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q_T (\kappa=0.6)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t9
title: "Table 9" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q_T (\kappa=0.3)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t15
title: "Table 15" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q_L (\kappa=0.6)$ of leading jet with 1000 &lt; pT &lt; 1800 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t16
title: "Table 16" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q_T (\kappa=0.6)$ of leading jet with 400 &lt; pT &lt; 700 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t17
title: "Table 17" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q_T (\kappa=0.6)$ of leading jet with 700 &lt; pT &lt; 1000 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t18
title: "Table 18" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Jetcharge $Q_T (\kappa=0.6)$ of leading jet with 1000 &lt; pT &lt; 1800 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t19
title: "Table 19" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Covariance matrix of jetcharge $Q (\kappa=1.0)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t20
title: "Table 20" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Covariance matrix of jetcharge $Q (\kappa=0.6)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t21
title: "Table 21" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Covariance matrix of jetcharge $Q (\kappa=0.3)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t22
title: "Table 22" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Covariance matrix of jetcharge $Q_L (\kappa=1.0)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t23
title: "Table 23" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Covariance matrix of jetcharge $Q_L (\kappa=0.6)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t24
title: "Table 24" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Covariance matrix of jetcharge $Q_L (\kappa=0.3)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t25
title: "Table 25" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Covariance matrix of jetcharge $Q_T (\kappa=1.0)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t26
title: "Table 26" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Covariance matrix of jetcharge $Q_T (\kappa=0.6)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t27
title: "Table 27" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Covariance matrix of jetcharge $Q_T (\kappa=0.3)$ of leading jet with pT &gt; 400 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t28
title: "Table 28" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Covariance matrix of jetcharge $Q (\kappa=0.6)$ of leading jet with 400 &lt; pT &lt; 700 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t29
title: "Table 29" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Covariance matrix of jetcharge $Q (\kappa=0.6)$ of leading jet with 700 &lt; pT &lt; 1000 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t30
title: "Table 30" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Covariance matrix of jetcharge $Q (\kappa=0.6)$ of leading jet with 1000 &lt; pT &lt; 1800 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.79857.v1/t31
title: "Table 31" of "Measurements of jet charge with dijet events in pp collisions at sqrt(s) = 8 TeV"

description: Covariance matrix of jetcharge $Q_L (\kappa=0.6)$ of leading jet with 400 &lt; pT &lt; 700 GeV.
description: CERN-LHC. Jet charge distributions are measured in proton-proton collisions at sqrt(s)=8 TeV based on a data set corresponding to an integrated luminosity of 19.7/fb collected by the CMS detector at the CERN LHC.