Fig. 6b: Number density $N_{\rm ch}$ (left) and $\Sigma p_{\rm T}$ (right) distributions as a function of $p_{\rm T}^{\rm trig}$ in Away and Toward regions after the subtraction of Number density $N_{\rm ch}$ and $\Sigma p_{\rm T}$ distributions in the transverse region for p-Pb collisions for $p_{\rm T} >$ 0.5 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.

Fig. 7a: $<p_{\rm T}>$ as a function of $p_{\rm T}^{\rm trig}$ in Toward (left) and Away (right) regions after the subtraction of transverse region for pp collisions for $p_{\rm T} >$ 0.5 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.

Fig. 7b: $<p_{\rm T}>$ as a function of $p_{\rm T}^{\rm trig}$ in Toward (left) and Away (right) regions after the subtraction of transverse region for p-Pb collisions for $p_{\rm T} >$ 0.5 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.

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 $p_{\rm T} >$ 0.15 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.

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 $p_{\rm T} >$ 1.0 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.

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 $p_{\rm T} >$ 0.15 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.

Fig. A4: 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 $p_{\rm T} >$ 1.0 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.

Parton dijet $M_{inv}$ vs $A_{LL}$ values with associated uncertainties, for topology C.

Parton dijet $M_{inv}$ vs $A_{LL}$ values with associated uncertainties, for topology D.

The correlation matrix for the point-to-point uncertainties (statistical and systematics) for the inclusive jet measurements.The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (statistical and systematics) for the inclusive jet measurements coupling with the forward-forward dijet measurements (topology A). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (statistical and systematics) for the inclusive jet measurements coupling with the forward-forward dijet measurements (topology B). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (statistical and systematics) for the inclusive jet measurements coupling with the forward-forward dijet measurements (topology C). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (statistical and systematics) for the inclusive jet measurements coupling with the forward-forward dijet measurements (topology D). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (systematics only) for forward-forward dijet measurements (topology A). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (systematics only) coupling forward-forward dijet measurements (topology A) with forward-central dijet measurements (topology B). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (systematics only) coupling forward-forward dijet measurements (topology A) with forward-central dijet measurements (topology C). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (systematics only) coupling forward-forward dijet measurements (topology A) with forward-central dijet measurements (topology D). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (systematics only) for forward-forward dijet measurements (topology B). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (systematics only) coupling forward-forward dijet measurements (topology B) with forward-central dijet measurements (topology C). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (systematics only) coupling forward-forward dijet measurements (topology B) with forward-central dijet measurements (topology D). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (systematics only) for forward-forward dijet measurements (topology C). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (systematics only) coupling forward-forward dijet measurements (topology C) with forward-central dijet measurements (topology D). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

The correlation matrix for the point-to-point uncertainties (systematics only) for forward-forward dijet measurements (topology D). The relative luminosity and beam polarization uncertainties are not included because they are the same for all points.

Parton inclusive-jet $p_T$ and $A_{LL}$ values with associated uncertainties for jet-$\eta$ region $0.5<|\eta|<1$.

Parton inclusive-jet $p_T$ and $A_{LL}$ values with associated uncertainties for jet-$\eta$ region $|\eta|<0.5$.

Parton dijet invariant mass $M_{inv}$ and $A_{LL}$ values with associated uncertainties for the $\textrm{sign}(\eta_1) = \textrm{sign}(\eta_2)$ topology.

Parton dijet invariant mass $M_{inv}$ and $A_{LL}$ values with associated uncertainties for the $\textrm{sign}(\eta_1) \neq \textrm{sign}(\eta_2)$ topology.

Parton inclusive-jet $p_T$, $x_T$, and $A_{LL}$ values with associated uncertainties for jet-$\eta$ region $|\eta|<1$.

The correlation matrix for the point-to-point uncertainties for inclusive jet measurements with jets in the $0.5<|\eta|<1$ region. The $A_{LL}$ uncertainty contribution of $0.0007$ from uncertainty in the relative luminosity measurement and $6.1\%$ from the beam polarization uncertainty, which are common to all the data points, are separated from the listed values.

The correlation matrix for the point-to-point uncertainties for inclusive jet measurements with jets in the $|\eta|<0.5$ region. The $A_{LL}$ uncertainty contribution of $0.0007$ from uncertainty in the relative luminosity measurement and $6.1\%$ from the beam polarization uncertainty, which are common to all the data points, are separated from the listed values.

The correlation matrix for the point-to-point uncertainties for inclusive jet measurements with jets in the $|\eta|<1$ region. The $A_{LL}$ uncertainty contribution of $0.0007$ from uncertainty in the relative luminosity measurement and $6.1\%$ from the beam polarization uncertainty, which are common to all the data points, are separated from the listed values.

The correlation matrix for the point-to-point uncertainties coupling inclusive jet measurements with jets in the $|\eta|<0.5$ region and jets in the $0.5<|\eta|<1$ region. The $A_{LL}$ uncertainty contribution of $0.0007$ from uncertainty in the relative luminosity measurement and $6.1\%$ from the beam polarization uncertainty, which are common to all the data points, are separated from the listed values.

The correlation matrix for the point-to-point uncertainties coupling inclusive jet measurements with jets in the $0.5<|\eta|<1$ region with dijet measurements with the the $\textrm{sign}(\eta_1) = \textrm{sign}(\eta_2)$ topology. The $A_{LL}$ uncertainty contribution of $0.0007$ from uncertainty in the relative luminosity measurement and $6.1\%$ from the beam polarization uncertainty, which are common to all the data points, are separated from the listed values.

The correlation matrix for the point-to-point uncertainties coupling inclusive jet measurements with jets in the $0.5<|\eta|<1$ region with dijet measurements with the the $\textrm{sign}(\eta_1) \neq \textrm{sign}(\eta_2)$ topology. The $A_{LL}$ uncertainty contribution of $0.0007$ from uncertainty in the relative luminosity measurement and $6.1\%$ from the beam polarization uncertainty, which are common to all the data points, are separated from the listed values.

The correlation matrix for the point-to-point uncertainties coupling inclusive jet measurements with jets in the $|\eta|<0.5$ region with dijet measurements with the the $\textrm{sign}(\eta_1) = \textrm{sign}(\eta_2)$ topology. The $A_{LL}$ uncertainty contribution of $0.0007$ from uncertainty in the relative luminosity measurement and $6.1\%$ from the beam polarization uncertainty, which are common to all the data points, are separated from the listed values.

The correlation matrix for the point-to-point uncertainties coupling inclusive jet measurements with jets in the $|\eta|<0.5$ region with dijet measurements with the the $\textrm{sign}(\eta_1) \neq \textrm{sign}(\eta_2)$ topology. The $A_{LL}$ uncertainty contribution of $0.0007$ from uncertainty in the relative luminosity measurement and $6.1\%$ from the beam polarization uncertainty, which are common to all the data points, are separated from the listed values.

The correlation matrix for the point-to-point uncertainties coupling inclusive jet measurements with jets in the $|\eta|<1$ region with dijet measurements with the the $\textrm{sign}(\eta_1) = \textrm{sign}(\eta_2)$ topology. The $A_{LL}$ uncertainty contribution of $0.0007$ from uncertainty in the relative luminosity measurement and $6.1\%$ from the beam polarization uncertainty, which are common to all the data points, are separated from the listed values.

The correlation matrix for the point-to-point uncertainties coupling inclusive jet measurements with jets in the $|\eta|<1$ region with dijet measurements with the the $\textrm{sign}(\eta_1) \neq \textrm{sign}(\eta_2)$ topology. The $A_{LL}$ uncertainty contribution of $0.0007$ from uncertainty in the relative luminosity measurement and $6.1\%$ from the beam polarization uncertainty, which are common to all the data points, are separated from the listed values.

The correlation matrix for the point-to-point uncertainties for dijet measurements with the $\textrm{sign}(\eta_1) = \textrm{sign}(\eta_2)$ topology. The $A_{LL}$ uncertainty contribution of $0.0007$ from uncertainty in the relative luminosity measurement and $6.1\%$ from the beam polarization uncertainty, which are common to all the data points, are separated from the listed values.

The correlation matrix for the point-to-point uncertainties for dijet measurements with the $\textrm{sign}(\eta_1) \neq \textrm{sign}(\eta_2)$ topology. The $A_{LL}$ uncertainty contribution of $0.0007$ from uncertainty in the relative luminosity measurement and $6.1\%$ from the beam polarization uncertainty, which are common to all the data points, are separated from the listed values.

The correlation matrix for the point-to-point uncertainties coupling dijet measurements with the $\textrm{sign}(\eta_1) \neq \textrm{sign}(\eta_2)$ topology and the $\textrm{sign}(\eta_1) = \textrm{sign}(\eta_2)$ topology. The $A_{LL}$ uncertainty contribution of $0.0007$ from uncertainty in the relative luminosity measurement and $6.1\%$ from the beam polarization uncertainty, which are common to all the data points, are separated from the listed values.

Inclusive jet $A_{LL}$ vs. parton jet $p_T$ for 0.5<|eta|<1.0.

The uncertainties on the parton jet pT values are strongly correlated across the bins. The point-to-point statistical and systematic uncertainties on the measured A_LL values given above are only weakly correlated among the bins. The correlation matrix for the quadrature sum of the point-to-point statistical and systematic uncertainties is given below. In that matrix, the order of the rows and columns matches the bin numbering above. In addition to the point-to-point statistical and systematic uncertainties, there are two systematic uncertainties that are common to all the measured A_LL values (and not included in the systematic uncertainty numbers quoted above): (a) +/-0.0005 vertical shift uncertainty from relative luminosity and (b) +/-6.5% vertical scale uncertainty from polarization.

$A_{LL}$ model predictions for |eta|<0.5.

$A_{LL}$ model predictions for 0.5<|eta|<1.0.

The measured inclusive jet double-differential cross section in the rapidity bin 1.2 <= |y| < 2.1 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 2.1 <= |y| < 2.8 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 2.8 <= |y| < 3.6 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 3.6 <= |y| < 4.4 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin |y| < 0.3 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 0.3 <= |y| < 0.8 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 0.8 <= |y| < 1.2 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 1.2 <= |y| < 2.1 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 2.1 <= |y| < 2.8 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 2.8 <= |y| < 3.6 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured inclusive jet double-differential cross section in the rapidity bin 3.6 <= |y| < 4.4 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin |y| < 0.3 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.3 <= |y| < 0.8 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.8 <= |y| < 1.2 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 1.2 <= |y| < 2.1 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.1 <= |y| < 2.8 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.8 <= |y| < 3.6 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 3.6 <= |y| < 4.4 for anti-kt jets with R = 0.4 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin |y| < 0.3 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.3 <= |y| < 0.8 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.8 <= |y| < 1.2 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 1.2 <= |y| < 2.1 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.1 <= |y| < 2.8 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.8 <= |y| < 3.6 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 3.6 <= |y| < 4.4 for anti-kt jets with R = 0.6 as a function of the jet XT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin |y| < 0.3 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.3 <= |y| < 0.8 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.8 <= |y| < 1.2 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 1.2 <= |y| < 2.1 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.1 <= |y| < 2.8 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.8 <= |y| < 3.6 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 3.6 <= |y| < 4.4 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin |y| < 0.3 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.3 <= |y| < 0.8 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.8 <= |y| < 1.2 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 1.2 <= |y| < 2.1 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.1 <= |y| < 2.8 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.8 <= |y| < 3.6 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 3.6 <= |y| < 4.4 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.

Normalised cross-section as a function of the mass of Cambridge-Aachen jets with R=1.2.

Normalised cross-section as a function of the mass of Cambridge-Aachen jets with R=1.2 after splitting and filtering.

Normalised cross-section as a function of the mass of Cambridge-Aachen jets with R=1.2 after splitting and filtering.

Normalised cross-section as a function of the mass of Cambridge-Aachen jets with R=1.2 after splitting and filtering.

Normalised cross-section as a function of the mass of Cambridge-Aachen jets with R=1.2 after splitting and filtering.

Normalised cross-section as a function of the mass of anti-kT jets with R=1.0.

Normalised cross-section as a function of the mass of anti-kT jets with R=1.0.

Normalised cross-section as a function of the mass of anti-kT jets with R=1.0.

Normalised cross-section as a function of the mass of anti-kT jets with R=1.0.

Normalised cross-section as a function of the the splitting scale variable sqrt(d12) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the the splitting scale variable sqrt(d12) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the the splitting scale variable sqrt(d12) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the the splitting scale variable sqrt(d12) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the the splitting scale variable sqrt(d23) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the the splitting scale variable sqrt(d23) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the the splitting scale variable sqrt(d23) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the the splitting scale variable sqrt(d23) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(12) of Cambridge-Aachen jets with R=1.2.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(12) of Cambridge-Aachen jets with R=1.2.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(12) of Cambridge-Aachen jets with R=1.2.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(12) of Cambridge-Aachen jets with R=1.2.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(32) of Cambridge-Aachen jets with R=1.2.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(32) of Cambridge-Aachen jets with R=1.2.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(32) of Cambridge-Aachen jets with R=1.2.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(32) of Cambridge-Aachen jets with R=1.2.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(21) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(21) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(21) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(21) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(32) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(32) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(32) of anti-kT jets with R=1.0.

Normalised cross-section as a function of the N-subjettiness ratio variable tau(32) of anti-kT jets with R=1.0.

Inclusive jet PT distribution for the |y| range 1.2-2.1 and R=0.4.

Inclusive jet PT distribution for the |y| range 2.1-2.8 and R=0.4.

Inclusive jet PT distribution for the |y| range 2.8-3.6 and R=0.4.

Inclusive jet PT distribution for the |y| range 3.6-4.4 and R=0.4.

Inclusive jet PT distribution for the |y| range 0.0-0.3 and R=0.6.

Inclusive jet PT distribution for the |y| range 0.3-0.8 and R=0.6.

Inclusive jet PT distribution for the |y| range 0.8-1.2 and R=0.6.

Inclusive jet PT distribution for the |y| range 1.2-2.1 and R=0.6.

Inclusive jet PT distribution for the |y| range 2.1-2.8 and R=0.6.

Inclusive jet PT distribution for the |y| range 2.8-3.6 and R=0.6.

Inclusive jet PT distribution for the |y| range 3.6-4.4 and R=0.6.

Dijet Mass distribution for the |y*| range 0.0-0.5 and R=0.4.

Dijet Mass distribution for the |y*| range 0.5-1.0 and R=0.4.

Dijet Mass distribution for the |y*| range 1.0-1.5 and R=0.4.

Dijet Mass distribution for the |y*| range 1.5-2.0 and R=0.4.

Dijet Mass distribution for the |y*| range 2.0-2.5 and R=0.4.

Dijet Mass distribution for the |y*| range 2.5-3.0 and R=0.4.

Dijet Mass distribution for the |y*| range 3.0-3.5 and R=0.4.

Dijet Mass distribution for the |y*| range 3.5-4.0 and R=0.4.

Dijet Mass distribution for the |y*| range 4.0-4.4 and R=0.4.

Dijet Mass distribution for the |y*| range 0.0-0.5 and R=0.6.

Dijet Mass distribution for the |y*| range 0.5-1.0 and R=0.6.

Dijet Mass distribution for the |y*| range 1.0-1.5 and R=0.6.

Dijet Mass distribution for the |y*| range 1.5-2.0 and R=0.6.

Dijet Mass distribution for the |y*| range 2.0-2.5 and R=0.6.

Dijet Mass distribution for the |y*| range 2.5-3.0 and R=0.6.

Dijet Mass distribution for the |y*| range 3.0-3.5 and R=0.6.

Dijet Mass distribution for the |y*| range 3.5-4.0 and R=0.6.

Dijet Mass distribution for the |y*| range 4.0-4.4 and R=0.6.

Charged particle fragmentation function in the jet-Pt range 80 TO 110 GeV.

Charged particle fragmentation function in the jet-Pt range 110 TO 160 GeV.

Charged particle fragmentation function in the jet-Pt range 160 TO 210 GeV.

Charged particle fragmentation function in the jet-Pt range 210 TO 260 GeV.

Charged particle fragmentation function in the jet-Pt range 260 TO 310 GeV.

Charged particle fragmentation function in the jet-Pt range 310 TO 400 GeV.

Charged particle fragmentation function in the jet-Pt range 400 TO 500 GeV.

Charged particle Rho distribution in the jet-Pt range 25 TO 40 GeV.

Charged particle Rho distribution in the jet-Pt range 40 TO 60 GeV.

Charged particle Rho distribution in the jet-Pt range 60 TO 80 GeV.

Charged particle Rho distribution in the jet-Pt range 80 TO 110 GeV.

Charged particle Rho distribution in the jet-Pt range 110 TO 160 GeV.

Charged particle Rho distribution in the jet-Pt range 160 TO 210 GeV.

Charged particle Rho distribution in the jet-Pt range 210 TO 260 GeV.

Charged particle Rho distribution in the jet-Pt range 260 TO 310 GeV.

Charged particle Rho distribution in the jet-Pt range 310 TO 400 GeV.

Charged particle Rho distribution in the jet-Pt range 400 TO 500 GeV.

Charged particle ptRel distribution in the jet-Pt range 25 TO 40 GeV.

Charged particle ptRel distribution in the jet-Pt range 40 TO 60 GeV.

Charged particle ptRel distribution in the jet-Pt range 60 TO 80 GeV.

Charged particle ptRel distribution in the jet-Pt range 80 TO 110 GeV.

Charged particle ptRel distribution in the jet-Pt range 110 TO 160 GeV.

Charged particle ptRel distribution in the jet-Pt range 160 TO 210 GeV.

Charged particle ptRel distribution in the jet-Pt range 210 TO 260 GeV.

Charged particle ptRel distribution in the jet-Pt range 260 TO 310 GeV.

Charged particle ptRel distribution in the jet-Pt range 310 TO 400 GeV.

Charged particle ptRel distribution in the jet-Pt range 400 TO 500 GeV.

Double differential cross sections for charged particle jets as a function of the jet PT in the |rapidity| range 1.5-1.9, shown separately for the two R values. The first (sys) errors is the correlated efficiency uncertainty and the second (sys) error is the correlated vetex splitting uncertainty. The third (sys) error is the quadratic sum of all the uncorrelated systematic uncertainties.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-0.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-0.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-0.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-0.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-0.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.5-1.0 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.5-1.0 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.5-1.0 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.5-1.0 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.5-1.0 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.0-1.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.0-1.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.0-1.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.0-1.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.0-1.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.5-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.5-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.5-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.5-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.5-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-0.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-0.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-0.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-0.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-0.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.5-1.0 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.5-1.0 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.5-1.0 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.5-1.0 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.5-1.0 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.0-1.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.0-1.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.0-1.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.0-1.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.0-1.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.5-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.5-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.5-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.5-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.5-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-0.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-0.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-0.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-0.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-0.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.5-1.0 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.5-1.0 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.5-1.0 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.5-1.0 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.5-1.0 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.0-1.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.0-1.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.0-1.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.0-1.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.0-1.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.5-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.5-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.5-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.5-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.5-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-0.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-0.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-0.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-0.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-0.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.5-1.0 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.5-1.0 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.5-1.0 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.5-1.0 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.5-1.0 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.0-1.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.0-1.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.0-1.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.0-1.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.0-1.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.5-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.5-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.5-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.5-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.5-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.