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.

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.

Measured double-differential dijet cross sections for the range 1.5 <= y* < 2.0 and jet radius parameter R = 0.4. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 2.0 <= y* < 2.5 and jet radius parameter R = 0.4. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 2.5 <= y* < 3.0 and jet radius parameter R = 0.4. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 0.0 <= y* < 0.5 and jet radius parameter R = 0.6. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 0.5 <= y* < 1.0 and jet radius parameter R = 0.6. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 1.0 <= y* < 1.5 and jet radius parameter R = 0.6. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 1.5 <= y* < 2.0 and jet radius parameter R = 0.6. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 2.0 <= y* < 2.5 and jet radius parameter R = 0.6. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

Measured double-differential dijet cross sections for the range 2.5 <= y* < 3.0 and jet radius parameter R = 0.6. The statistical uncertainties from data and MC simulation have been combined. The three columns correspond to nominal, stronger or weaker correlations between jet energy scale uncertainty components.

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.

The particle-level di-jet differential cross section. The systematic uncertainty on the data contains contributions from track finding efficiency, track transverse momentum resolution, calorimeter energy resolution, and unfolding uncertainties. For the theory, values are given for the underlying event and hadronization (UEH) correction uncertainty and the quadrature sum of the UEH and theoretical uncertainties. Both the UEH and theoretical uncertainties include contributions from factorization and renormalization scale uncertainties and PDF uncertainties. An 8.8% uncertainty common to all points due to the integrated luminosity determination is also present, but not included in the systematic values quoted below.

Values of gluon X1 and X2 obtained from the PYTHIA detector-level simulation for the same-sign di-jet topology compared to the gluon X distribution for inclusive jets. The inclusive distribution has been scaled down by a factor of 20 compared to the di-jet distributions.

Values of gluon X1 and X2 obtained from the PYTHIA detector-level simulation for the opposite-sign di-jet topology compared to the gluon X distribution for inclusive jets. The inclusive distribution has been scaled down by a factor of 20 compared to the di-jet distributions.

Di-jet A_LL asymmetry vs parton-level invariant mass for the same-sign di-jet topology. The systematic uncertainty on the mass includes contributions from jet energy scale, the correction to parton-level, and the difference between NLO and PYTHIA cross sections. The systematic uncertainty on the asymmetry includes contributions from trigger and reconstruction bias and residual transverse beam polarization components. A 6.5% uncertainty common to all points due to uncertainty on the measured beam polarizations is also present, but not included in the uncertainties quoted below.

Theoretical predictions for the di-jet A_LL asymmetry for the same-sign topology using the DSSV14 and NNPDFpol1.1 polarized PDF sets. The DSSV14 prediction is presented without uncertainty while the systematic uncertainty on the NNPDFpol1.1 prediction contains contributions from factorization and renormalization scale uncertainties and PDF uncertainties.

Di-jet A_LL asymmetry vs parton-level invariant mass for the opposite-sign di-jet topology. The systematic uncertainty on the mass includes contributions from jet energy scale, the correction to parton-level, and the difference between NLO and PYTHIA cross sections. The systematic uncertainty on the asymmetry includes contributions from trigger and reconstruction bias and residual transverse beam polarization components. A 6.5% uncertainty common to all points due to uncertainty on the measured beam polarizations is also present, but not included in the uncertainties quoted below.

Theoretical predictions for the di-jet A_LL asymmetry for the opposite-sign topology using the DSSV14 and NNPDFpol1.1 polarized PDF sets. The DSSV14 prediction is presented without uncertainty while the systematic uncertainty on the NNPDFpol1.1 prediction contains contributions from factorization and renormalization scale uncertainties and PDF uncertainties.

The double differential cross section as a function of the di-jet mass for the range |y_max| = 1.5-2.0, where |y_max| = max(|y1,|y2|) of the two leading jets in the event.

The double differential cross section as a function of the di-jet mass for the range |y_max| = 2.0-2.5, where |y_max| = max(|y1,|y2|) of the two leading jets in the event.

No description provided.

No description provided.

No description provided.

Statistical correlation matrix from unfolding

Triple-differential dijet cross section as a function of the average transverse momentum of the leading two jets with detailed experimental uncertainties (symmetrised).

Statistical correlation matrix from unfolding

Triple-differential dijet cross section as a function of the average transverse momentum of the leading two jets with detailed experimental uncertainties (symmetrised).

Statistical correlation matrix from unfolding

Triple-differential dijet cross section as a function of the average transverse momentum of the leading two jets with detailed experimental uncertainties (symmetrised).

Statistical correlation matrix from unfolding

Triple-differential dijet cross section as a function of the average transverse momentum of the leading two jets with detailed experimental uncertainties (symmetrised).

Statistical correlation matrix from unfolding

Electroweak correction factor to triple-differential dijet cross section

Electroweak correction factor to triple-differential dijet cross section

Electroweak correction factor to triple-differential dijet cross section

Electroweak correction factor to triple-differential dijet cross section

Electroweak correction factor to triple-differential dijet cross section

Electroweak correction factor to triple-differential dijet cross section

Nonperturbative correction factor to triple-differential dijet cross section with uncertainty

Nonperturbative correction factor to triple-differential dijet cross section with uncertainty

Nonperturbative correction factor to triple-differential dijet cross section with uncertainty

Nonperturbative correction factor to triple-differential dijet cross section with uncertainty

Nonperturbative correction factor to triple-differential dijet cross section with uncertainty

Nonperturbative correction factor to triple-differential dijet cross section with uncertainty

Transverse $\langle N_\text{ch} / \delta\eta\,\delta\phi \rangle$ vs. $p_T^\text{lead}$ in $|\eta| < 2.5$ in incl jet / excl dijet events.

Trans-max $\langle N_\text{ch} / \delta\eta\,\delta\phi \rangle$ vs. $p_T^\text{lead}$ in $|\eta| < 2.5$ in incl jet / excl dijet events.

Trans-min $\langle N_\text{ch} / \delta\eta\,\delta\phi \rangle$ vs. $p_T^\text{lead}$ in $|\eta| < 2.5$ in incl jet / excl dijet events.

Transverse $\langle \sum E_T^\text{ch+neut} / \delta\eta\,\delta\phi \rangle$ vs. $p_T^\text{lead}$ in $|\eta| < 2.5$ in incl jet / excl dijet events.

Transverse $\langle \sum E_T^\text{ch+neut} / \delta\eta\,\delta\phi \rangle$ vs. $p_T^\text{lead}$ in $|\eta| < 4.8$ in incl jet / excl dijet events.

Transverse $\langle \sum p_T^\text{ch} / \sum E_T^\text{ch+neut} \rangle$ vs. $p_T^\text{lead}$ in $|\eta| < 2.5$ in incl jet / excl dijet events.

Transverse $\langle \text{mean}~p_T^\text{ch} \rangle$ vs. $p_T^\text{lead}$ in $|\eta| < 2.5$ in incl jet / excl dijet events.

Transverse $\langle \text{mean}~p_T^\text{ch} \rangle$ vs. $N_\text{ch}$ in $|\eta| < 2.5$ in incl jet events.

Transverse $\langle \text{mean}~p_T^\text{ch} \rangle$ vs. $N_\text{ch}$ in $|\eta| < 2.5$ in excl dijet events.

Transverse $\sum p_T^\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} > 20\;\text{GeV}$ in incl jet / excl dijet events.

Trans-max $\sum p_T^\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} > 20\;\text{GeV}$ in incl jet / excl dijet events.

Trans-min $\sum p_T^\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} > 20\;\text{GeV}$ in incl jet / excl dijet events.

Transverse $\sum p_T^\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} \in [20, 60]\;\text{GeV}$ in incl jet / excl dijet events.

Trans-max $\sum p_T^\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} \in [20, 60]\;\text{GeV}$ in incl jet / excl dijet events.

Trans-min $\sum p_T^\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} \in [20, 60]\;\text{GeV}$ in incl jet / excl dijet events.

Transverse $\sum p_T^\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} \in [60,210]\;\text{GeV}$ in incl jet / excl dijet events.

Trans-max $\sum p_T^\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} \in [60,210]\;\text{GeV}$ in incl jet / excl dijet events.

Trans-min $\sum p_T^\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} \in [60,210]\;\text{GeV}$ in incl jet / excl dijet events.

Transverse $\sum p_T^\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} > 210\;\text{GeV}$ in incl jet / excl dijet events.

Trans-max $\sum p_T^\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} > 210\;\text{GeV}$ in incl jet / excl dijet events.

Trans-min $\sum p_T^\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} > 210\;\text{GeV}$ in incl jet / excl dijet events.

Transverse $N_\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} > 20\;\text{GeV}$ in incl jet / excl dijet events.

Trans-max $N_\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} > 20\;\text{GeV}$ in incl jet / excl dijet events.

Trans-min $N_\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} > 20\;\text{GeV}$ in incl jet / excl dijet events.

Transverse $N_\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} \in [20, 60]\;\text{GeV}$ in incl jet / excl dijet events.

Trans-max $N_\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} \in [20, 60]\;\text{GeV}$ in incl jet / excl dijet events.

Trans-min $N_\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} \in [20, 60]\;\text{GeV}$ in incl jet / excl dijet events.

Transverse $N_\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} \in [60,210]\;\text{GeV}$ in incl jet / excl dijet events.

Trans-max $N_\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} \in [60,210]\;\text{GeV}$ in incl jet / excl dijet events.

Trans-min $N_\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} \in [60,210]\;\text{GeV}$ in incl jet / excl dijet events.

Transverse $N_\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} > 210\;\text{GeV}$ in incl jet / excl dijet events.

Trans-max $N_\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} > 210\;\text{GeV}$ in incl jet / excl dijet events.

Trans-min $N_\text{ch}$ in $|\eta| < 2.5$, $p_T^\text{lead} > 210\;\text{GeV}$ in incl jet / excl dijet events.