Jet multiplicity measured for a leading-pT jet ($p_{T1}$) with 400 < $p_{T1}$ < 800 GeV and for an azimuthal separation between the two leading jets of $0 < \Delta\Phi_{1,2} < 150^{\circ}$. The full breakdown of the uncertainties is displayed, with PU corresponding to Pileup, PREF to Trigger Prefering, PTHAT to the hard-scale (renormalization and factorization scales), MISS and FAKE to the inefficienties and background, LUMI to integrated luminosity. With JES, JER and stat. unc. following the notation in the paper.

Jet multiplicity measured for a leading-pT jet ($p_{T1}$) with 400 < $p_{T1}$ < 800 GeV and for an azimuthal separation between the two leading jets of $150 < \Delta\Phi_{1,2} < 170^{\circ}$. The full breakdown of the uncertainties is displayed, with PU corresponding to Pileup, PREF to Trigger Prefering, PTHAT to the hard-scale (renormalization and factorization scales), MISS and FAKE to the inefficienties and background, LUMI to integrated luminosity. With JES, JER and stat. unc. following the notation in the paper.

Jet multiplicity measured for a leading-pT jet ($p_{T1}$) with 400 < $p_{T1}$ < 800 GeV and for an azimuthal separation between the two leading jets of $170 < \Delta\Phi_{1,2} < 180^{\circ}$. The full breakdown of the uncertainties is displayed, with PU corresponding to Pileup, PREF to Trigger Prefering, PTHAT to the hard-scale (renormalization and factorization scales), MISS and FAKE to the inefficienties and background, LUMI to integrated luminosity. With JES, JER and stat. unc. following the notation in the paper.

Jet multiplicity measured for a leading-pT jet ($p_{T1}$) with $p_{T1}$ > 800 and for an azimuthal separation between the two leading jets of $0 < \Delta\Phi_{1,2} < 150^{\circ}$. The full breakdown of the uncertainties is displayed, with PU corresponding to Pileup, PREF to Trigger Prefering, PTHAT to the hard-scale (renormalization and factorization scales), MISS and FAKE to the inefficienties and background, LUMI to integrated luminosity. With JES, JER and stat. unc. following the notation in the paper.

Jet multiplicity measured for a leading-pT jet ($p_{T1}$) with $p_{T1}$ > 800 and for an azimuthal separation between the two leading jets of $150 < \Delta\Phi_{1,2} < 170^{\circ}$. The full breakdown of the uncertainties is displayed, with PU corresponding to Pileup, PREF to Trigger Prefering, PTHAT to the hard-scale (renormalization and factorization scales), MISS and FAKE to the inefficienties and background, LUMI to integrated luminosity. With JES, JER and stat. unc. following the notation in the paper.

Jet multiplicity measured for a leading-pT jet ($p_{T1}$) with $p_{T1}$ > 800 and for an azimuthal separation between the two leading jets of $170 < \Delta\Phi_{1,2} < 180^{\circ}$. The full breakdown of the uncertainties is displayed, with PU corresponding to Pileup, PREF to Trigger Prefering, PTHAT to the hard-scale (renormalization and factorization scales), MISS and FAKE to the inefficienties and background, LUMI to integrated luminosity. With JES, JER and stat. unc. following the notation in the paper.

Measured transverse momentum of the leading $p_{T}$ jet ($p_{T1}$). The full breakdown of the uncertainties is displayed, with PU corresponding to Pileup, PREF to Trigger Prefering, PTHAT to the hard-scale (renormalization and factorization scales), MISS and FAKE to the inefficienties and background, LUMI to integrated luminosity. With JES, JER and stat. unc. following the notation in the paper.

Measured transverse momentum of the subleading $p_{T}$ jet ($p_{T2}$). The full breakdown of the uncertainties is displayed, with PU corresponding to Pileup, PREF to Trigger Prefering, PTHAT to the hard-scale (renormalization and factorization scales), MISS and FAKE to the inefficienties and background, LUMI to integrated luminosity. With JES, JER and stat. unc. following the notation in the paper.

Measured transverse momentum of the third leading $p_{T}$ jet ($p_{T3}$). The full breakdown of the uncertainties is displayed, with PU corresponding to Pileup, PREF to Trigger Prefering, PTHAT to the hard-scale (renormalization and factorization scales), MISS and FAKE to the inefficienties and background, LUMI to integrated luminosity. With JES, JER and stat. unc. following the notation in the paper.

Measured transverse momentum of the fourth leading $p_{T}$ jet ($p_{T4}$). The full breakdown of the uncertainties is displayed, with PU corresponding to Pileup, PREF to Trigger Prefering, PTHAT to the hard-scale (renormalization and factorization scales), MISS and FAKE to the inefficienties and background, LUMI to integrated luminosity. With JES, JER and stat. unc. following the notation in the paper.

Jet multiplicity distribution in TUnfold binning ($N_{jets},\Delta\phi_{1,2},p_{T1}$) as indicated in the XML file provided as additional resource. The uncertainties follow the notation of Table 1.

Correlation matrix at particle level for the measured jet multiplicity in TUnfold binning ($N_{jets},\Delta\phi_{1,2},p_{T1}$) as indicated in the XML file provided as additional resource.

Jet $p_{T}$ distributions in TUnfold binning ($p_{T1},p_{T2},p_{T3},p_{T4}$) as indicated in the XML file provided as additional resource. The uncertainties follow the notation of Table 1.

Correlation matrix at particle level for the measured jet $p_{T}$ distributions in TUnfold binning ($p_{T1},p_{T2},p_{T3},p_{T4}$) as indicated in the XML file provided as additional resource.

Bin-to-bin correlation in the measured cross section as a function of the rapidity absolute value of the first jet, $|y(\text{j}_1)|$.

Measured cross section as a function of the transverse momenum of the first jet, $p_{\text{T}}(\text{j}_1)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section as a function of the transverse momenum of the first jet, $p_{\text{T}}(\text{j}_1)$.

Measured cross section as a function of the rapidity absolute value of the second jet, $|y(\text{j}_2)|$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section as a function of the rapidity absolute value of the second jet, $|y(\text{j}_2)|$.

Measured cross section as a function of the transverse momenum of the second jet, $p_{\text{T}}(\text{j}_2)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section as a function of the transverse momenum of the second jet, $p_{\text{T}}(\text{j}_2)$.

Measured cross section as a function of the rapidity absolute value of the third jet, $|y(\text{j}_3)|$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section as a function of the rapidity absolute value of the third jet, $|y(\text{j}_3)|$.

Measured cross section as a function of the transverse momenum of the third jet, $p_{\text{T}}(\text{j}_3)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section as a function of the transverse momenum of the third jet, $p_{\text{T}}(\text{j}_3)$.

Measured cross section as a function of the $H_{\text{T}}$ observable for events with at least one jet and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section as a function of the $H_{\text{T}}$ observable for events with at least one jet.

Measured cross section as a function of the $H_{\text{T}}$ observable for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section as a function of the $H_{\text{T}}$ observable for events with at least two jets.

Measured cross section as a function of the $H_{\text{T}}$ observable for events with at least three jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section as a function of the $H_{\text{T}}$ observable for events with at least three jets.

Measured differential cross section as a function of dijet mass, $M_{\text{j}_1\text{j}_2}$, for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of dijet mass, $M_{\text{j}_1\text{j}_2}$, for events with at least two jets.

Measured differential cross section as a function of Z boson rapidity absolute value, $|y(\text{Z})|$ for events with at least one jet and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of Z boson rapidity absolute value, $|y(\text{Z})|$ for events with at least one jet.

Measured differential cross section as a function of the leading and subleading jet rapidity difference, $y_{\text{diff}}(\text{j}_1,\text{j}_2)$, for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the leading and subleading jet rapidity difference, $y_{\text{diff}}(\text{j}_1,\text{j}_2)$, for events with at least two jets.

Measured differential cross section as a function of the leading and subleading jet rapidity sum, $y_{\text{sum}}(\text{j}_1,\text{j}_2)$, for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the leading and subleading jet rapidity sum, $y_{\text{sum}}(\text{j}_1,\text{j}_2)$, for events with at least two jets.

Measured differential cross section as a function of the Z boson and leading jet rapidity difference, $y_{\text{diff}}(\text{Z},\text{j}_1)$, for events with at least one jet and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and leading jet rapidity difference, $y_{\text{diff}}(\text{Z},\text{j}_1)$, for events with at least one jet.

Measured differential cross section as a function of the Z boson and leading jet rapidity sum, $y_{\text{sum}}(\text{Z},\text{j}_1)$, for events with at least one jet and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and leading jet rapidity sum, $y_{\text{sum}}(\text{Z},\text{j}_1)$, for events with at least one jet.

Measured differential cross section as a function of the Z boson and leading jet rapidity difference, $y_{\text{diff}}(\text{Z},\text{j}_1)$, for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and leading jet rapidity difference, $y_{\text{diff}}(\text{Z},\text{j}_1)$, for events with at least two jets.

Measured differential cross section as a function of the Z boson and leading jet rapidity sum, $y_{\text{sum}}(\text{Z},\text{j}_1)$, for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and leading jet rapidity sum, $y_{\text{sum}}(\text{Z},\text{j}_1)$, for events with at least two jets.

Measured differential cross section as a function of the Z boson and subleading jet rapidity difference, $y_{\text{diff}}(\text{Z},\text{j}_2)$, for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and subleading jet rapidity difference, $y_{\text{diff}}(\text{Z},\text{j}_2)$, for events with at least two jets.

Measured differential cross section as a function of the Z boson and subleading jet rapidity sum, $y_{\text{sum}}(\text{Z},\text{j}_2)$, for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and subleading jet rapidity sum, $y_{\text{sum}}(\text{Z},\text{j}_2)$, for events with at least two jets.

Measured differential cross section as a function of the Z boson and dijet rapidity difference, $y_{\text{diff}}(\text{Z},\text{dijet})$, for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and dijet rapidity difference, $y_{\text{diff}}(\text{Z},\text{dijet})$, for events with at least two jets.

Measured differential cross section as a function of the Z boson and dijet rapidity sum, $y_{\text{sum}}(\text{Z},\text{dijet})$, for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and dijet rapidity sum, $y_{\text{sum}}(\text{Z},\text{dijet})$, for events with at least two jets.

Measured differential cross section as a function of the Z boson and leading jet azimuthal difference, $\Delta\phi(\text{Z},\text{j}_1)$, for events with at least one jet and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and leading jet azimuthal difference, $\Delta\phi(\text{Z},\text{j}_1)$, for events with at least one jet.

Measured differential cross section as a function of the Z boson and leading jet azimuthal difference, $\Delta\phi(\text{Z},\text{j}_1)$, for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and leading jet azimuthal difference, $\Delta\phi(\text{Z},\text{j}_1)$, for events with at least two jets.

Measured differential cross section as a function of the Z boson and leading jet azimuthal difference for events, $\Delta\phi(\text{Z},\text{j}_1)$, with at least three jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and leading jet azimuthal difference for events, $\Delta\phi(\text{Z},\text{j}_1)$, with at least three jets.

Measured differential cross section as a function of the Z boson and subleading jet azimuthal difference for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and subleading jet azimuthal difference for events with at least two jets.

Measured differential cross section as a function of the Z boson and subleading jet azimuthal difference, $\Delta\phi(\text{Z},\text{j}_2)$, for events with at least three jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and subleading jet azimuthal difference, $\Delta\phi(\text{Z},\text{j}_2)$, for events with at least three jets.

Measured differential cross section as a function of the Z boson and third jet azimuthal difference, $\Delta\phi(\text{Z},\text{j}_3)$, for events with at least three jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the Z boson and third jet azimuthal difference, $\Delta\phi(\text{Z},\text{j}_3)$, for events with at least three jets.

Measured differential cross section as a function of the leading and subleading jet azimuthal difference, $\Delta\phi(\text{j}_1,\text{j}_2)$, for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the leading and subleading jet azimuthal difference, $\Delta\phi(\text{j}_1,\text{j}_2)$, for events with at least two jets.

Measured differential cross section as a function of the leading and subleading jet azimuthal difference, $\Delta\phi(\text{j}_1,\text{j}_2)$, for events with at least three jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the leading and subleading jet azimuthal difference, $\Delta\phi(\text{j}_1,\text{j}_2)$, for events with at least three jets.

Measured differential cross section as a function of the leading and third jet azimuthal difference, $\Delta\phi(\text{j}_1,\text{j}_3)$, for events with at least three jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the leading and third jet azimuthal difference, $\Delta\phi(\text{j}_1,\text{j}_3)$, for events with at least three jets.

Measured differential cross section as a function of the subleading and third jet azimuthal difference, $\Delta\phi(\text{j}_2,\text{j}_3)$, for events with at least three jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured differential cross section as a function of the subleading and third jet azimuthal difference, $\Delta\phi(\text{j}_2,\text{j}_3)$, for events with at least three jets.

Measured cross section as a function of the leading jet transverse momentum, $p_{\text{T}}(\text{j}_1)$, and rapidity absolute value, $|y(\text{j}_1)|$ for events with at least one jet and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section as a function of the leading jet transverse momentum, $p_{\text{T}}(\text{j}_1)$, and rapidity absolute value, $|y(\text{j}_1)|$ for events with at least one jet.

Measured cross section as a function of the leading jet and Z boson rapidity abosolute values, $|y(\text{j}_1|$ and $|y(\text(Z))|$, for events with at least one jet with $p_\text{T}>20\,\text{Gev}$ and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section as a function of the leading jet and Z boson rapidity abosolute values, $|y(\text{j}_1|$ and $|y(\text(Z))|$, for events with at least one jet with $p_\text{T}>20\,\text{Gev}$.

Measured cross section as a function of the transverse momementum, $p_{\text{T}}(\text{Z})$, and rapidity, $y(\text{Z})$, of the Z boson, for events with at least one jet with $p_\text{T}>20\,\text{Gev}$ and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section as a function of the transverse momementum, $p_{\text{T}}(\text{Z})$, and rapidity, $y(\text{Z})$, of the Z boson, for events with at least one jet with $p_\text{T}>20\,\text{Gev}$.

Visible cross section for inclusive D*+- production with two jets.

Ratio of visible cross sections of inclusive D*+- production with and without the two jets.

Ratio of visible cross sections of inclusive D*+- production with and without the two jets.

Differential cross section for inclusive D*+- production in the visible kinematic region as a function of Q**2.

Differential cross section for inclusive D*+- production in the visible kinematic region as a function of Q**2.

Differential cross section for inclusive D*+- production in the visible kinematic region as a function of X.

Differential cross section for inclusive D*+- production in the visible kinematic region as a function of X.

Differential cross section for inclusive D*+- production in the visible kinematic region as a function of W.

Differential cross section for inclusive D*+- production in the visible kinematic region as a function of W.

Differential cross section for inclusive D*+- production in the visible kinematic region as a function of PT.

Differential cross section for inclusive D*+- production in the visible kinematic region as a function of PT.

Differential cross section for inclusive D*+- production in the visible kinematic region as a function of ETARAP.

Differential cross section for inclusive D*+- production in the visible kinematic region as a function of ETARAP.

Differential cross section for inclusive D*+- production in the visible kinematic region as a function of Z.

Differential cross section for inclusive D*+- production in the visible kinematic region as a function of Z.

Double differential cross section for inclusive D*+- production in bins of Q**2 and X.

Double differential cross section for inclusive D*+- production in bins of Q**2 and X.

Double differential cross section for inclusive D*+- production in bins of Q**2 and X.

Double differential cross section for inclusive D*+- production in bins of Q**2 and X.

Double differential cross section for inclusive D*+- production in bins of Q**2 and X.

Double differential cross section for inclusive D*+- production in bins of Q**2 and X.

Double differential cross section for inclusive D*+- production in bins of Q**2 and X.

Double differential cross section for inclusive D*+- production in bins of Q**2 and X.

Double differential cross section for inclusive D*+- production in bins of Q**2 and X.

Double differential cross section for inclusive D*+- production in bins of Q**2 and X.

Differential cross section for inclusive D*+- production as a function of Q**2 with the constraint that the transverse momentum of the D* in the virtual photon-proton centre-of-mass frame is > 2 GeV.

Differential cross section for inclusive D*+- production as a function of Q**2 with the constraint that the transverse momentum of the D* in the virtual photon-proton centre-of-mass frame is > 2 GeV.

Differential cross section for inclusive D*+- production as a function of X with the constraint that the transverse momentum of the D* in the virtual photon-proton centre-of-mass frame is > 2 GeV.

Differential cross section for inclusive D*+- production as a function of X with the constraint that the transverse momentum of the D* in the virtual photon-proton centre-of-mass frame is > 2 GeV.

Differential cross section for inclusive D*+- production as a function of PT with the constraint that the transverse momentum of the D* in the virtual photon-proton centre-of-mass frame is > 2 GeV.

Differential cross section for inclusive D*+- production as a function of PT with the constraint that the transverse momentum of the D* in the virtual photon-proton centre-of-mass frame is > 2 GeV.

Differential cross section for inclusive D*+- production as a function of ETARAP with the constraint that the transverse momentum of the D* in the virtualphoton-proton centre-of-mass frame is > 2 GeV.

Differential cross section for inclusive D*+- production as a function of ETARAP with the constraint that the transverse momentum of the D* in the virtualphoton-proton centre-of-mass frame is > 2 GeV.

Differential cross section for D*+- production with dijets as a function of Q**2.

Differential cross section for D*+- production with dijets as a function of Q**2.

Differential cross section for D*+- production with dijets as a function of X.

Differential cross section for D*+- production with dijets as a function of X.

Differential cross section for D*+- production with dijets as a function of ET(C=JET1).

Differential cross section for D*+- production with dijets as a function of ET(C=JET1).

Differential cross section for D*+- production with dijets as a function of M(C=JET2).

Differential cross section for D*+- production with dijets as a function of M(C=JET2).

Double differential cross section for D*+- production with dijets in bins of Q**2 and PHI(JET1)-PHI(JET2).

Double differential cross section for D*+- production with dijets in bins of Q**2 and PHI(JET1)-PHI(JET2).

Double differential cross section for D*+- production with dijets in bins of Q**2 and PHI(JET1)-PHI(JET2).

Double differential cross section for D*+- production with dijets in bins of Q**2 and PHI(JET1)-PHI(JET2).

Differential cross section for D*+- production with dijets as a function of pseudorapidity of the jet containing D*.

Differential cross section for D*+- production with dijets as a function of pseudorapidity of the jet containing D*.

Differential cross section for D*+- production with dijets as a function of pseudorapidity of the other jet.

Differential cross section for D*+- production with dijets as a function of pseudorapidity of the other jet.

Differential cross section for D*+- production with dijets as a function of the pseudorapidity difference of the two jets.

Differential cross section for D*+- production with dijets as a function of the pseudorapidity difference of the two jets.

Differential cross section for D*+- production with dijets as a function of X(C=GAMMA), the observed fraction of the virtual photon momentum carried by the partons.

Differential cross section for D*+- production with dijets as a function of X(C=GAMMA), the observed fraction of the virtual photon momentum carried by the partons.

Double differential cross section for D*+- production with dijets in bins of Q**2 and X(C=GAMMA), the observed fraction of the virtual photon momentum carried by the partons.

Double differential cross section for D*+- production with dijets in bins of Q**2 and X(C=GAMMA), the observed fraction of the virtual photon momentum carried by the partons.

Differential cross section for D*+- production with dijets as a function of X(C=GLUON), the observed fraction of the proton momentum carried by the gluon.

Differential cross section for D*+- production with dijets as a function of X(C=GLUON), the observed fraction of the proton momentum carried by the gluon.

Double differential cross section for D*+- production with dijets in bins of Q**2 and X(C=GLUON), the observed fraction of the proton momentum carried by the gluon.

Double differential cross section for D*+- production with dijets in bins of Q**2 and X(C=GLUON), the observed fraction of the proton momentum carried by the gluon.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of inclusive jet multiplicity, $N_{\text{jets}}^{\text{min}}$.

Measured cross section for Z+jets as a function of the transverse momementum of the Z boson, $p_{\text{T}}(\text{Z})$, for events with at least one jet and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momementum of the Z boson, $p_{\text{T}}(\text{Z})$, for events with at least one jet.

Measured cross section for Z+jets as a function of the transverse momenum of the first jet, $p_{\text{T}}(\text{j}_1)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momenum of the first jet, $p_{\text{T}}(\text{j}_1)$.

Measured cross section for Z+jets as a function of the transverse momenum of the second jet, $p_{\text{T}}(\text{j}_2)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momenum of the second jet, $p_{\text{T}}(\text{j}_2)$.

Measured cross section for Z+jets as a function of the transverse momenum of the third jet, $p_{\text{T}}(\text{j}_3)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momenum of the third jet, $p_{\text{T}}(\text{j}_3)$.

Measured cross section for Z+jets as a function of the absolute rapidity of the first jet, $|y(\text{j}_1)|$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the absolute rapidity of the first jet, $|y(\text{j}_1)|$.

Measured cross section for Z+jets as a function of the absolute rapidity of the second jet, $|y(\text{j}_2)|$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the absolute rapidity of the second jet, $|y(\text{j}_2)|$.

Measured cross section for Z+jets as a function of the absolute rapidity of the third jet, $|y(\text{j}_3)|$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the absolute rapidity of the third jet, $|y(\text{j}_3)|$.

Measured cross section for Z+jets as a function of the $H_{\text{T}}$ observable for event with at least one jet and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the $H_{\text{T}}$ observable for event with at least one jet.

Measured cross section for Z+jets as a function of the $H_{\text{T}}$ observable for event with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the $H_{\text{T}}$ observable for event with at least two jets.

Measured cross section for Z+jets as a function of the $H_{\text{T}}$ observable for event with at least three jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the $H_{\text{T}}$ observable for event with at least three jets.

Measured cross section for Z+jets as a function of the transverse momentum balance between the Z boson and the accompanying jets, $p_{\text{T}}^{\text{bal}}$, for events with at least one jet and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momentum balance between the Z boson and the accompanying jets, $p_{\text{T}}^{\text{bal}}$, for events with at least one jet.

Measured cross section for Z+jets as a function of the transverse momentum balance between the Z boson and the accompanying jets, $p_{\text{T}}^{\text{bal}}$, for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momentum balance between the Z boson and the accompanying jets, $p_{\text{T}}^{\text{bal}}$, for events with at least two jets.

Measured cross section for Z+jets as a function of the transverse momentum balance between the Z boson and the accompanying jets, $p_{\text{T}}^{\text{bal}}$, for events with at least three jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momentum balance between the Z boson and the accompanying jets, $p_{\text{T}}^{\text{bal}}$, for events with at least three jets.

Measured cross section for Z+jets as a function of the JZB variable with no restriction on $p_{\text{T}}(\text{Z})$ and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the JZB variable with no restriction on $p_{\text{T}}(\text{Z})$.

Measured cross section for Z+jets as a function of the JZB variable for $p_{\text{T}}(\text{Z})\leq50\,$GeV) and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the JZB variable for $p_{\text{T}}(\text{Z})\leq50\,$GeV).

Measured cross section for Z+jets as a function of the JZB variable for $p_{\text{T}}(\text{Z})>50\,$GeV and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the JZB variable for $p_{\text{T}}(\text{Z})>50\,$GeV.

The cross section measurement as a function of the inclusive jet multiplicity, for jet multiplicities of up to 7.

The differential cross section measurement as a function of the transverse momentum of the first leading jet.

The differential cross section measurement as a function of the transverse momentum of the first leading jet.

The differential cross section measurement as a function of the transverse momentum of the second leading jet.

The differential cross section measurement as a function of the transverse momentum of the second leading jet.

The differential cross section measurement as a function of the transverse momentum of the third leading jet.

The differential cross section measurement as a function of the transverse momentum of the third leading jet.

The differential cross section measurement as a function of the transverse momentum of the fourth leading jet.

The differential cross section measurement as a function of the transverse momentum of the fourth leading jet.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for events with one or more jets.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for events with one or more jets.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for events with two or more jets.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for events with two or more jets.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for events with three or more jets.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for events with three or more jets.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for events with four or more jets.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for events with four or more jets.

The differential cross section measurement as a function of the transverse momentum of the dijet system of the two highest pT jets for events with two or more jets.

The differential cross section measurement as a function of the transverse momentum of the dijet system of the two highest pT jets for events with two or more jets.

The differential cross section measurement as a function of the transverse momentum of the dijet system of the two highest pT jets for events with three or more jets.

The differential cross section measurement as a function of the transverse momentum of the dijet system of the two highest pT jets for events with three or more jets.

The differential cross section measurement as a function of the transverse momentum of the dijet system of the two highest pT jets for events with four or more jets.

The differential cross section measurement as a function of the transverse momentum of the dijet system of the two highest pT jets for events with four or more jets.

The differential cross section measurement as a function of the dijet invariant mass of the two highest pT jets for events with two or more jets.

The differential cross section measurement as a function of the dijet invariant mass of the two highest pT jets for events with two or more jets.

The differential cross section measurement as a function of the dijet invariant mass of the two highest pT jets for events with three or more jets.

The differential cross section measurement as a function of the dijet invariant mass of the two highest pT jets for events with three or more jets.

The differential cross section measurement as a function of the dijet invariant mass of the two highest pT jets for events with four or more jets.

The differential cross section measurement as a function of the dijet invariant mass of the two highest pT jets for events with four or more jets.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the first leading jet.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the first leading jet.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the second leading jet.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the second leading jet.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the third leading jet.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the third leading jet.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the fourth leading jet.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the fourth leading jet.

The differential cross section measurement as a function of the rapidity difference between the two highest pT jets for events with two or more jets.

The differential cross section measurement as a function of the rapidity difference between the two highest pT jets for events with two or more jets.

The differential cross section measurement as a function of the rapidity difference between the two highest pT jets for events with three or more jets.

The differential cross section measurement as a function of the rapidity difference between the two highest pT jets for events with three or more jets.

The differential cross section measurement as a function of the rapidity difference between the two highest pT jets for events with four or more jets.

The differential cross section measurement as a function of the rapidity difference between the two highest pT jets for events with four or more jets.

The differential cross section measurement as a function of the rapidity difference between the first and the third highest pT jets for events with three or more jets.

The differential cross section measurement as a function of the rapidity difference between the first and the third highest pT jets for events with three or more jets.

The differential cross section measurement as a function of the rapidity difference between the second and the third highest pT jets for events with three or more jets.

The differential cross section measurement as a function of the rapidity difference between the second and the third highest pT jets for events with three or more jets.

The differential cross section measurement as a function of the rapidity difference between the most forward and the most backward jets for events with two or more jets.

The differential cross section measurement as a function of the rapidity difference between the most forward and the most backward jets for events with two or more jets.

The differential cross section measurement as a function of the rapidity difference between the most forward and the most backward jets for events with three or more jets.

The differential cross section measurement as a function of the rapidity difference between the most forward and the most backward jets for events with three or more jets.

The differential cross section measurement as a function of the rapidity difference between the most forward and the most backward jets for events with four or more jets.

The differential cross section measurement as a function of the rapidity difference between the most forward and the most backward jets for events with four or more jets.

The differential cross section measurement as a function of the azimuthal angle separation between the two highest pT jets for events with two or more jets.

The differential cross section measurement as a function of the azimuthal angle separation between the two highest pT jets for events with two or more jets.

The differential cross section measurement as a function of the azimuthal angle separation between the most forward and the most backward jets for events with two or more jets.

The differential cross section measurement as a function of the azimuthal angle separation between the most forward and the most backward jets for events with two or more jets.

The differential cross section measurement as a function of DeltaR separation between the two highest pT jets for events with two or more jets.

The differential cross section measurement as a function of DeltaR separation between the two highest pT jets for events with two or more jets.

The differential cross section measurement as a function of the azimuthal angle separation between the first leading jet and the muon.

The differential cross section measurement as a function of the azimuthal angle separation between the first leading jet and the muon.

The differential cross section measurement as a function of the azimuthal angle separation between the second leading jet and the muon.

The differential cross section measurement as a function of the azimuthal angle separation between the second leading jet and the muon.

The differential cross section measurement as a function of the azimuthal angle separation between the third leading jet and the muon.

The differential cross section measurement as a function of the azimuthal angle separation between the third leading jet and the muon.

The differential cross section measurement as a function of the azimuthal angle separation between the fourth leading jet and the muon.

The differential cross section measurement as a function of the azimuthal angle separation between the fourth leading jet and the muon.

Average number of jets as a function of HT for events with one or more jets.

Average number of jets as a function of HT for events with one or more jets.

Average number of jets as a function of HT for events with two or more jets.

Average number of jets as a function of HT for events with two or more jets.

Average number of jets as a function of the rapidity difference between the two highest pT jets for events with two or more jets.

Average number of jets as a function of the rapidity difference between the two highest pT jets for events with two or more jets.

Average number of jets as a function of the rapidity difference between the most forward and the most backward jets for events with two or more jets.

Average number of jets as a function of the rapidity difference between the most forward and the most backward jets for events with two or more jets.

Measured charged jet differential cross section ratios for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV for $15<p_{T}^{ch jet}<20$ GeV/$c$.

Measured cross sections for isolated-photon plus jet production as a function of $m^{\gamma-\rm jet}$.

Measured cross sections for isolated-photon plus jet production as a function of $|\cos\theta^{\star}|$.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $467 < m^{\gamma-\rm jet1} < 510$ GeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $510 < m^{\gamma-\rm jet1} < 590$ GeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $590 < m^{\gamma-\rm jet1} < 670$ GeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $670 < m^{\gamma-\rm jet1} < 760$ GeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $760 < m^{\gamma-\rm jet1} < 850$ GeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $850 < m^{\gamma-\rm jet1} < 950$ GeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $0.95 < m^{\gamma-\rm jet1} < 1.05$ TeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $1.05 < m^{\gamma-\rm jet1} < 1.25$ TeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $1.25 < m^{\gamma-\rm jet1} < 2.45$ TeV.

Measured cross sections for isolated-photon plus 2jet production as a function of $E_{\rm T}^{\gamma}$.

Measured cross sections for isolated-photon plus 2jet production as a function of $p_{\rm T}^{\rm jet2}$.

Measured cross sections for isolated-photon plus 2jet production as a function of $\Delta\phi^{\rm \gamma-jet2}$.

Measured cross sections for isolated-photon plus 2jet production as a function of $\Delta\phi^{\rm jet1-jet2}$.

Measured cross sections for isolated-photon plus 2jet production as a function of $\Delta\phi^{\rm \gamma-jet2}$ for the range $130< E_{\rm T}^{\gamma} <300$ GeV.

Measured cross sections for isolated-photon plus 2jet production as a function of $\Delta\phi^{\rm \gamma-jet2}$ for the range $E_{\rm T}^{\gamma} >300$ GeV.

Measured cross sections for isolated-photon plus 2jet production as a function of $\Delta\phi^{\rm jet1-jet2}$ for the range $130< E_{\rm T}^{\gamma} <300$ GeV.

Measured cross sections for isolated-photon plus 2jet production as a function of $\Delta\phi^{\rm jet1-jet2}$ for the range $E_{\rm T}^{\gamma} >300$ GeV.

Measured cross sections for isolated-photon plus 2jet production as a function of $\beta^{\rm jet1}$.

Measured cross sections for isolated-photon plus 2jet production as a function of $\beta^{\gamma}$.

Ratio of measured cross sections for isolated-photon plus 2jet production as a function of $\beta$.

Measured cross sections for isolated-photon plus 3jet production as a function of $E_{\rm T}^{\gamma}$.

Measured cross sections for isolated-photon plus 3jet production as a function of $p_{\rm T}^{\rm jet3}$.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm \gamma-jet3}$.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm jet1-jet3}$.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm jet2-jet3}$.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm \gamma-jet3}$ for the range $130< E_{\rm T}^{\gamma} <300$ GeV.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm \gamma-jet3}$ for the range $E_{\rm T}^{\gamma} >300$ GeV.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm jet1-jet3}$ for the range $130< E_{\rm T}^{\gamma} <300$ GeV.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm jet1-jet3}$ for the range $E_{\rm T}^{\gamma} >300$ GeV.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm jet2-jet3}$ for the range $130< E_{\rm T}^{\gamma} <300$ GeV.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm jet2-jet3}$ for the range $E_{\rm T}^{\gamma} >300$ GeV.

The differential cross section measurement as a function of the transverse momentum of the second leading jet.

The differential cross section measurement as a function of the transverse momentum of the third leading jet.

The differential cross section measurement as a function of the transverse momentum of the fourth leading jet.

The differential cross section measurement as a function of the absolute value of the rapidity of the first leading jet.

The differential cross section measurement as a function of the absolute value of the rapidity of the second leading jet.

The differential cross section measurement as a function of the absolute value of the rapidity of the third leading jet.

The differential cross section measurement as a function of the absolute value of the rapidity of the fourth leading jet.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for events with one or more jets.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for events with two or more jets.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for events with three or more jets.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for events with four or more jets.

The differential cross section measurement as a function of the azimuthal angle separation between the first leading jet and the muon.

The differential cross section measurement as a function of the azimuthal angle separation between the second leading jet and the muon.

The differential cross section measurement as a function of the azimuthal angle separation between the third leading jet and the muon.

The differential cross section measurement as a function of the azimuthal angle separation between the fourth leading jet and the muon.

The differential cross section measurement as a function of DeltaR separation between the muon and the closest jet for events with one or more jets.

Differential cross section as a function of the transverse momentum PT of the leading other jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, sample purity, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the transverse momentum PT of the subleading other jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, sample purity, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the pseudorapidity ETA of the leading b-jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, sample purity, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the pseudorapidity ETA of the subleading b-jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, sample purity, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the pseudorapidity ETA of the leading other jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, sample purity, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the pseudorapidity ETA of the subleading other jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, sample purity, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the azimuthal angle DeltaPhi between the two other jets, normalized to the total number of selected events. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, sample purity, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the normalized PT balance DELTARELPT between the third and the fourth jet, normalized to the total number of selected events. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, sample purity, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the azimuthal angle between the two dijet planes (leading-subleading b- and leading-subleading other jets), normalized to the total number of selected events. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, sample purity, model dependence and jet energy resolution and trigger efficiency correction.

Results for the DeltaR distribution. Statistical and systematic uncertainties are quoted.

Results for the pT distribution. Statistical and systematic uncertainties are quoted.

Results for the y_B distribution. Statistical and systematic uncertainties are quoted.

$p_{\rm T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector, centrality 40-60%.

$p_{\rm T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector, centrality 60-80%.

$p_{\rm T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector, centrality 80-100%.

pp reference spectrum, obtained by scaling down the measured charged jets at 7 TeV to 5.02 TeV for R = 0.4 jets.

$p_{\rm T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 measured with the ALICE detector, centrality 0-20%.

$p_{\rm T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 measured with the ALICE detector, centrality 20-40%.

$p_{\rm T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 measured with the ALICE detector, centrality 40-60%.

$p_{\rm T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 measured with the ALICE detector, centrality 60-80%.

$p_{\rm T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 measured with the ALICE detector, centrality 80-100%.

Nuclear modification factor $Q_{\rm pPb}$ of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector, centrality 0-20%.

Nuclear modification factor $Q_{\rm pPb}$ of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector, centrality 20-40%.

Nuclear modification factor $Q_{\rm pPb}$ of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector, centrality 40-60%.

Nuclear modification factor $Q_{\rm pPb}$ of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector, centrality 60-80%.

Nuclear modification factor $Q_{\rm pPb}$ of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector, centrality 80-100%.

Nuclear modification factor $Q_{\rm pPb}$ of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 measured with the ALICE detector, centrality 0-20%.

Nuclear modification factor $Q_{\rm pPb}$ of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 measured with the ALICE detector, centrality 20-40%.

Nuclear modification factor $Q_{\rm pPb}$ of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 measured with the ALICE detector, centrality 40-60%.

Nuclear modification factor $Q_{\rm pPb}$ of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 measured with the ALICE detector, centrality 60-80%.

Nuclear modification factor $Q_{\rm pPb}$ of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 measured with the ALICE detector, centrality 80-100%.

Centrality evolution of charged jet $Q_{\rm pPb}$ in p-Pb collisions at 5.02 TeV for R = 0.4 and 20 < $p_{\rm {T, ch. jet}}$ < 30 GeV/c measured with the ALICE detector.

Centrality evolution of charged jet $Q_{\rm pPb}$ in p-Pb collisions at 5.02 TeV for R = 0.4 and 40 < $p_{\rm {T, ch. jet}}$ < 50 GeV/c measured with the ALICE detector.

Centrality evolution of charged jet $Q_{\rm pPb}$ in p-Pb collisions at 5.02 TeV for R = 0.4 and 70 < $p_{\rm {T, ch. jet}}$ < 80 GeV/c measured with the ALICE detector.

Charged jet production cross section ratio for different resolution parameter R=0.2/R=0.4 measured with ALICE in p-Pb collisions at 5.02 TeV, minimum bias events.

Charged jet production cross section ratio for different resolution parameter R=0.2/R=0.4 measured with ALICE in p-Pb collisions at 5.02 TeV, 0-20% centrality.

Charged jet production cross section ratio for different resolution parameter R=0.2/R=0.4 measured with ALICE in p-Pb collisions at 5.02 TeV, 20-40% centrality.

Charged jet production cross section ratio for different resolution parameter R=0.2/R=0.4 measured with ALICE in p-Pb collisions at 5.02 TeV, 40-60% centrality.

Charged jet production cross section ratio for different resolution parameter R=0.2/R=0.4 measured with ALICE in p-Pb collisions at 5.02 TeV, 60-80% centrality.

Charged jet production cross section ratio for different resolution parameter R=0.2/R=0.4 measured with ALICE in p-Pb collisions at 5.02 TeV, 80-100% centrality.

Inclusive Jet Cross Section ${\rm\frac{d\sigma_{jet}}{dP_T}}$.

2-Jet Cross Section ${\rm\frac{d\sigma_{2-jet}}{d\langle P_T \rangle}}$.

3-Jet Cross Section ${\rm\frac{d\sigma_{3-jet}}{d\langle P_T \rangle}}$.

Inclusive Jet Cross Section ${\rm\frac{d^2\sigma_{jet}}{dQ^2dP_T}}$.

2-Jet Cross Section ${\rm\frac{d^2\sigma_{2-jet}}{dQ^2d\langle P_T \rangle}}$.

2-Jet Cross Section ${\rm\frac{d^2\sigma_{2-jet}}{dQ^2d\xi}}$.

3-Jet Cross Section ${\rm\frac{d^2\sigma_{3-jet}}{dQ^2d\langle P_T \rangle}}$.

3-Jet to 2-Jet Cross Sections Ratio ${\rm\frac{d\sigma_{3-jet}}{dQ^2}/\frac{d\sigma_{2-jet}}{dQ^2}}$.

3-Jet to 2-Jet Cross Sections Ratio ${\rm\frac{d\sigma_{3-jet}}{d\langle P_T \rangle}/\frac{d\sigma_{2-jet}}{d\langle P_T \rangle}}$.

3-Jet to 2-Jet Cross Sections Ratio ${\rm\frac{d^2\sigma_{3-jet}}{dQ^2d\langle P_T \rangle}/\frac{d^2\sigma_{2-jet}}{dQ^2d\langle P_T \rangle}}$.

Measurement of the $t\overline{t}$ cross-section as a function of the jet multiplicity for jets with $p_{\mathrm{T}}$ larger than 80 GeV. The uncertainties given correspond to the individual contributions of each source of systematic uncertainty as described in the paper.

Measurement of the $t\overline{t}$ cross-section as a function of the transverse momentum of the leading jet in $t\overline{t}$ events. The uncertainties given correspond to the individual contributions of each source of systematic uncertainty as described in the paper.

Measurement of the $t\overline{t}$ cross-section as a function of the transverse momentum of the 2nd leading jet in $t\overline{t}$ events. The uncertainties given correspond to the individual contributions of each source of systematic uncertainty as described in the paper.

Measurement of the $t\overline{t}$ cross-section as a function of the transverse momentum of the 3rd leading jet in $t\overline{t}$ events. The uncertainties given correspond to the individual contributions of each source of systematic uncertainty as described in the paper.

Measurement of the $t\overline{t}$ cross-section as a function of the transverse momentum of the 4th leading jet in $t\overline{t}$ events. The uncertainties given correspond to the individual contributions of each source of systematic uncertainty as described in the paper.

Measurement of the $t\overline{t}$ cross-section as a function of the transverse momentum of the 5th leading jet in $t\overline{t}$ events. The uncertainties given correspond to the individual contributions of each source of systematic uncertainty as described in the paper.

Measured differential four-jet cross section for R=0.4 jets, in bins of pT4, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of HT, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of m_4j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of min(m_2j)/m_4j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as m_2j>500 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of min(m_2j)/m_4j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as m_2j>1000 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of min(m_2j)/m_4j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as m_2j>1500 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of min(m_2j)/m_4j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as m_2j>2000 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>400 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>700 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>1000 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>400 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>700 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>1000 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>400 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>700 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>1000 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>400 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>700 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>1000 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of maxDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of maxDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>250 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of maxDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>400 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of maxDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>550 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>1. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>1, as well as pT1>250 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>1, as well as pT1>400 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>1, as well as pT1>550 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>2. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>2, as well as pT1>250 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>2, as well as pT1>400 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>2, as well as pT1>550 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>3. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>3, as well as pT1>250 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>3, as well as pT1>400 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>3, as well as pT1>550 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>4. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>4, as well as pT1>250 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>4, as well as pT1>400 GeV. All other details are as for pT1.

Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>4, as well as pT1>550 GeV. All other details are as for pT1.

Differential cross-section for $Z$+jet in the leading jet pseudorapidity, $\eta^{\mathrm{jet}}$.

Differential cross-section for $Z$+jet in the boson $Z$ rapidity, $y^Z$.

Cross-section for $Z$+jet production, differential in the $Z$ boson transverse momentum, $p_{T}^{Z}$.

Cross-section for $Z$+jet production, differential in the difference in $\phi$ between the $Z$ boson and the leading jet, $\Delta \phi$.

Cross-section for $Z$+jet production, differential in the difference in rapidity between the $Z$ boson and the leading jet, $\Delta y$.

$p_\mathrm{T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector. Eta-Interval -0.65 < $\eta$ < -0.25.

$p_\mathrm{T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 measured with the ALICE detector.

$p_\mathrm{T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 calculated with a Lorentz-boosted NLO pQCD calculation using POWHEG+PYTHIA8 with CTEQ6.6+EPS09.

$p_\mathrm{T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 calculated with a Lorentz-boosted NLO pQCD calculation using POWHEG+PYTHIA8 with CTEQ6.6.

Nuclear modification factors $R_\mathrm{pPb}$ of charged jets in p-Pb at 5.02 TeV measured with ALICE. Resolution parameter R = 0.2.

Nuclear modification factors $R_\mathrm{pPb}$ of charged jets in p-Pb at 5.02 TeV measured with ALICE. Resolution parameter R = 0.4.

Charged jet production cross section ratio for different resolution parameter R=0.2/R=0.4 measured with ALICE in p-Pb collisions at 5.02 TeV.

Charged jet production cross section ratio for different resolution parameter R=0.2/R=0.4 obtained by Lorentz-boosted NLO pQCD calculations using POWHEG+PYTHIA8 with CTEQ6.6+EPS09 at 5.02 TeV. Errors are syst.+stat. errors added in quadrature.

Charged jet production cross section ratio for different resolution parameter R=0.2/R=0.4 obtained by PYTHIA6 calculations using tune Perugia 2011 at 5.02 TeV.

Charged jet production cross section ratio for different resolution parameter R=0.2/R=0.4 measured with ALICE in pp collisions at 7 TeV.

Measured charged jet differential cross sections for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV.

Measured charged jet differential cross sections for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV.

Measured charged jet differential cross sections for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV.

Measured charged jet differential cross sections for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV.

Measured charged jet differential cross sections for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV.

Measured charged jet differential cross sections for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV.

Measured charged jet differential cross sections for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV.

Measured charged jet differential cross sections for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV.

Measured charged jet differential cross sections for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV.

Measured charged jet differential cross section ratios for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV.

Measured charged jet differential cross section ratios for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV.

Average charged particle multiplicity in charged jets.

Average charged particle multiplicity in charged jets.

Average charged particle multiplicity in charged jets.

Average transverse momentum density distribution within a charged jet.

Average transverse momentum density distribution within a charged jet.

Average transverse momentum density distribution within a charged jet.

Average transverse momentum density distribution within a charged jet.

Average transverse momentum density distribution within a charged jet.

Average transverse momentum density distribution within a charged jet.

Average transverse momentum density distribution within a charged jet.

Average transverse momentum density distribution within a charged jet.

Average transverse momentum density distribution within a charged jet.

Average transverse momentum density distribution within a charged jet.

Average transverse momentum density distribution within a charged jet.

Average transverse momentum density distribution within a charged jet.

Average radius containing 80% of the total reconstructed jet transverse momentum.

Average radius containing 80% of the total reconstructed jet transverse momentum.

Average radius containing 80% of the total reconstructed jet transverse momentum.

Transverse momentum of particles in charged jet.

Transverse momentum of particles in charged jet.

Transverse momentum of particles in charged jet.

Transverse momentum of particles in charged jet.

Charged particle scaled pT spectra dN/dz.

Charged particle scaled pT spectra dN/dz.

Charged particle scaled pT spectra dN/dz.

Charged particle scaled pT spectra dN/dz.

Charged particle scaled pT spectra dN/dxi.

Charged particle scaled pT spectra dN/dxi.

Charged particle scaled pT spectra dN/dxi.

Charged particle scaled pT spectra dN/dxi.

Measured charged jet differential cross sections for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV without UE subtraction.

Measured charged jet differential cross sections for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV without UE subtraction.

Average charged particle multiplicity in charged jets without UE subtraction.

Average charged particle multiplicity in charged jets without UE subtraction.

Average charged particle multiplicity in charged jets without UE subtraction.

Average transverse momentum density distribution within a charged jet without UE subtraction.

Average transverse momentum density distribution within a charged jet without UE subtraction.

Average transverse momentum density distribution within a charged jet without UE subtraction.

Average transverse momentum density distribution within a charged jet without UE subtraction.

Average transverse momentum density distribution within a charged jet without UE subtraction.

Average transverse momentum density distribution within a charged jet without UE subtraction.

Average transverse momentum density distribution within a charged jet without UE subtraction.

Average transverse momentum density distribution within a charged jet without UE subtraction.

Average transverse momentum density distribution within a charged jet without UE subtraction.

Average transverse momentum density distribution within a charged jet without UE subtraction.

Average transverse momentum density distribution within a charged jet without UE subtraction.

Average transverse momentum density distribution within a charged jet without UE subtraction.

Transverse momentum of particles in charged jet without UE subtraction.

Transverse momentum of particles in charged jet without UE subtraction.

Transverse momentum of particles in charged jet without UE subtraction.

Transverse momentum of particles in charged jet without UE subtraction.

Charged particle scaled pT spectra dN/dz without UE subtraction.

Charged particle scaled pT spectra dN/dz without UE subtraction.

Charged particle scaled pT spectra dN/dz without UE subtraction.

Charged particle scaled pT spectra dN/dz without UE subtraction.

Charged particle scaled pT spectra dN/dxi without UE subtraction.

Charged particle scaled pT spectra dN/dxi UE subtracted.

Charged particle scaled pT spectra dN/dxi without UE subtraction.

Charged particle scaled pT spectra dN/dxi without UE subtraction.

The cross section measurement as a function of the transverse momentum of the second leading jet.

The cross section measurement as a function of the transverse momentum of the third leading jet.

The cross section measurement as a function of the transverse momentum of the fourth leading jet.

The cross section measurement as a function of the absolute value of the pseudorapidity of the leading jet.

The cross section measurement as a function of the absolute value of the pseudorapidity of the second leading jet.

The cross section measurement as a function of the absolute value of the pseudorapidity of the third leading jet.

The cross section measurement as a function of the absolute value of the pseudorapidity of the fourth leading jet.

The cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for jet multiplicities of one or more.

The cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for jet multiplicities of two or more.

The cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for jet multiplicities of three or more.

The cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for jet multiplicities of four or more.

The differential cross section measurement as a function of the transverse momentum of the second leading jet.

The differential cross section measurement as a function of the transverse momentum of the third leading jet.

The differential cross section measurement as a function of the transverse momentum of the fourth leading jet.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for jet multiplicities of one or more.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for jet multiplicities of two or more.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for jet multiplicities of three or more.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for jet multiplicities of four or more.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the first leading jet.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the first second jet.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the third leading jet.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the fourth leading jet.

The differential cross section measurement as a function of the absolute value of the azimuthal separation between the first leading jet and the muon.

The differential cross section measurement as a function of the absolute value of the azimuthal separation between the second leading jet and the muon.

The differential cross section measurement as a function of the absolute value of the azimuthal separation between the third leading jet and the muon.

The differential cross section measurement as a function of the absolute value of the azimuthal separation between the fourth leading jet and the muon.

Differential cross section as a function of the transverse momentum PT of the third jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the transverse momentum PT of the fourth jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the pseudorapidity eta of the leading jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the pseudorapidity eta of the subleading jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the pseudorapidity eta of the third jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the pseudorapidity eta of the fourth jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the azimuthal angle DeltaPhi between the third and the fourth jet, normalized to the total number of selected events. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the normalized PT balance DELTARELPT between the third and the fourth jet, normalized to the total number of selected events. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.

Differential cross section as a function of the azimuthal angle between the two dijet planes (first-second and third-fourth jets), normalized to the total number of selected events. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.

Breakdown of systematic uncertainties (in %) for the inclusive $b$-jet cross-section $\sigma(Zb)\times N_{b\text{-jet}}$ as a function of $b$-jet $p_T$.

The inclusive $b$-jet cross-section $\sigma(Zb)\times N_{b\text{-jet}}$ as a function of $b$-jet $|y|$ together with the corresponding non-perturbative corrections.

Breakdown of systematic uncertainties (in %) for the inclusive $b$-jet cross-section $\sigma(Zb)\times N_{b\text{-jet}}$ as a function of $b$-jet $|y|$.

The inclusive $b$-jet cross-section $\sigma(Zb)\times N_{b\text{-jet}}$ as a function of $y_{\text{boost}}(Z,b)$ together with the corresponding non-perturbative corrections.

Breakdown of systematic uncertainties (in %) for the inclusive $b$-jet cross-section $\sigma(Zb)\times N_{b\text{-jet}}$ as a function of $y_{\text{boost}}(Z,b)$.

The inclusive $b$-jet cross-section $\sigma^{*}(Zb)\times N_{b\text{-jet}}$ as a function of $\Delta y(Z,b)$ together with the corresponding non-perturbative corrections.

Breakdown of systematic uncertainties (in %) for the inclusive $b$-jet cross-section $\sigma^{*}(Zb)\times N_{b\text{-jet}}$ as a function of $\Delta y(Z,b)$.

The inclusive $b$-jet cross-section $\sigma^{*}(Zb)\times N_{b\text{-jet}}$ as a function of $\Delta\phi(Z,b)$ together with the corresponding non-perturbative corrections.

Breakdown of systematic uncertainties (in %) for the inclusive $b$-jet cross-section $\sigma^{*}(Zb)\times N_{b\text{-jet}}$ as a function of $\Delta\phi(Z,b)$.

The inclusive $b$-jet cross-section $\sigma^{*}(Zb)\times N_{b\text{-jet}}$ as a function of $\Delta R(Z,b)$ together with the corresponding non-perturbative corrections.

Breakdown of systematic uncertainties (in %) for the inclusive $b$-jet cross-section $\sigma^{*}(Zb)\times N_{b\text{-jet}}$ as a function of $\Delta R(Z,b)$.

The cross-section $\sigma(Zb)$ as a function of $Z$ boson $p_T$ together with the corresponding non-perturbative corrections.

Breakdown of systematic uncertainties (in %) for the cross-section $\sigma(Zb)$ as a function of $Z$ boson $p_T$.

The cross-section $\sigma(Zb)$ as a function of $Z$ boson $|y|$ together with the corresponding non-perturbative corrections.

Breakdown of systematic uncertainties (in %) for the cross-section $\sigma(Zb)$ as a function of $Z$ boson $|y|$.

Integrated $Z+\ge 2$ $b$-jets cross-section.

Breakdown of systematic uncertainties (in %) for the integrated $Z+\ge 2$ $b$-jets cross-section.

The cross-section $\sigma(Zbb)$ as a function of $\Delta R(b,b)$ together with the corresponding non-perturbative corrections.

Breakdown of systematic uncertainties (in %) for the cross-section $\sigma(Zbb)$ as a function of $\Delta R(b,b)$.

The cross-section $\sigma(Zbb)$ as a function of $\Delta m(b,b)$ together with the corresponding non-perturbative corrections.

Breakdown of systematic uncertainties (in %) for the cross-section $\sigma(Zbb)$ as a function of $\Delta m(b,b)$.

The cross-section $\sigma(Zbb)$ as a function of $Z$ boson $p_T$ together with the corresponding non-perturbative corrections.

Breakdown of systematic uncertainties (in %) for the cross-section $\sigma(Zbb)$ as a function of $Z$ boson $p_T$.

The cross-section $\sigma(Zbb)$ as a function of $Z$ boson $|y|$ together with the corresponding non-perturbative corrections.

Breakdown of systematic uncertainties (in %) for the cross-section $\sigma(Zbb)$ as a function of $Z$ boson $|y|$.

Inclusive double differential b-jet cross section as a function of PT for the |rapidity| range 1.2-2.1 from the lifetime-based analysis.

Differential b-jet cross sections as a function of PT from summing the data in the previous tables.

Differential b-jet cross sections as a function of PT from the muon-based analysis.

Differential b-bbar dijet cross sections as a function of dijet mass from the lifetime-based analysis.

Differential b-bbar dijet cross sections as a function of azimuthal angle difference between the jets from the lifetime-based analysis.

Double differential b-bbar dijet cross sections as a function of the angular variable chi between the jets for two different jet mass ranges from the lifetime-based analysis.

Double differential b-bbar dijet cross sections as a function of the angular variable chi between the jets for two different jet mass ranges from the lifetime-based analysis.

Cross section dsigma/dpt as a function of the leading jet pt corrected to the lepton common fiducial region and for QED radiation effects.

Cross section dsigma/dpt as a function of the second-leading jet pt corrected to the lepton common fiducial region and for QED radiation effects.

Inclusive jet differential cross section dsigma/dy corrected to the lepton common fiducial region and for QED radiation effects.

Jet differential cross section dsigma/dy as a function of the leading jet y corrected to the lepton common fiducial region and for QED radiation effects.

Jet differential cross section dsigma/dy as a function of the second-leading jet y corrected to the lepton common fiducial region and for QED radiation effects.

Differential cross section dsigma/dmjj as a function of the dijet invariant mass mjj corrected to the lepton common fiducial region and for QED radiation effects.

Differential cross section dsigma/d DeltaYjj as a function of the dijet rapidity separation DeltaYjj corrected to the lepton common fiducial region and for QED radiation effects.

Differential cross section dsigma/d DeltaPhijj as a function of the dijet azimuthal separation DeltaPhijj corrected to the lepton common fiducial region and for QED radiation effects.

Differential cross section dsigma/d DeltaRjj as a function of the dijet angular separation DeltaRjj corrected to the lepton common fiducial region and for QED radiation effects.

Cross section for Inclusive Jet Multiplicity for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

Ratio of cross sections for N/N-1 inclusive jet multiplicities for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

Measured normalized inclusive jet differential cross section 1/sigma_DY dsigma/dpt for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

Measured normalized leading jet differential cross section 1/sigma_DY dsigma/dpt for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

Measured normalized second-leading jet differential cross section 1/sigma_DY dsigma/dpt for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

Measured normalized inclusive jet differential cross section 1/sigma_DY dsigma/dy for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

Measured normalized leading jet differential cross section 1/sigma_DY dsigma/dy for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

Measured normalized second leading jet differential cross section 1/sigma_DY dsigma/dy for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

Measured normalized differential cross section as a function of dijet invariant mass 1/sigma_DY dsigma/dmjj for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

Measured normalized differential cross section as a function of dijet rapidity separation 1/sigma_DY dsigma/dDeltaYjj for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

Measured normalized differential cross section as a function of dijet azimuthal separation 1/sigma_DY dsigma/dDeltaPhijj (1/rad.) for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

Measured normalized differential cross section as a function of dijet angular separation 1/sigma_DY dsigma/dDeltaRjj for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

Unfolded normalised differential Z+2j cross section as a function of the rapidity separation between the leading jets in the search region.

Unfolded normalised differential cross section distribution as a function of the number of jets in the rapidity interval between the two leading jets in the high mass region.

Unfolded normalised differential cross section distribution as a function of the normalised transverse momentum balance in the high mass region.

Unfolded normalised differential cross section distribution as a function of the azimuthal angle between the two leading jets in the high mass region.

Unfolded jet veto efficiency as a function of the dijet invariant mass in the baseline region.

Unfolded jet veto efficiency as a function of the rapidity separation between the two leading jets in the baseline region.

Unfolded average number of jets in the rapidity interval between the two leading jets as a function of the dijet invariant mass in the baseline region.

Unfolded average number of jets in the rapidity interval between the two leading jets as a function of the rapidity separation between the two leading jets in the baseline region.

Unfolded transverse momentum balance veto efficiency as a function of the dijet invariant mass in the baseline region.

Unfolded transverse momentum balance veto efficiency as a function of the rapidity separation between the two leading jets in the baseline region.

Unfolded normalised differential Z+2j cross section as a function of dijet invariant mass in the high-pt region.

Unfolded normalised differential Z+2j cross section as a function of dijet invariant mass in the control region.

Unfolded normalised differential Z+2j cross section as a function of the rapidity separation between the leading jets in the high-pt region.

Unfolded normalised differential Z+2j cross section as a function of the rapidity separation between the leading jets in the control region.

Unfolded jet veto efficiency as a function of the dijet invariant mass in the high-pt region.

Unfolded jet veto efficiency as a function of the rapidity separation between the two leading jets in the high-pt region.

Unfolded average number of jets in the rapidity interval between the two leading jets as a function of the dijet invariant mass in the high-pt region.

Unfolded average number of jets in the rapidity interval between the two leading jets as a function of the rapidity separation between the two leading jets in the high-pt region.

Unfolded transverse momentum balance veto efficiency as a function of the dijet invariant mass in the high-pt region.

Unfolded transverse momentum balance veto efficiency as a function of the rapidity separation between the two leading jets in the high-pt region.

Measured differential cross sections as function of the lepton pseudo-rapidity of the production of a W boson with a D meson or a D* meson times the branching ratio W -> l nu in the fiducial regions together with the statistical and systematic uncertainties. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events.

Measured cross section ratios of the production of a W boson with a D meson or a D* meson and the inclusive production of a W boson in the fiducial regions together with the statistical and systematic uncertainties. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events.

Measured differential cross section ratios of the production of a W boson with a D meson or a D* meson and the inclusive production of a W boson in the fiducial regions as function of the D/D* meson pT together with the statistical and systematic uncertainties. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events.

Measured integrated cross sections of the production of a W boson in association with a single c-jet and exactly zero or one additional non-c-jets times the branching ratio W -> l nu in the fiducial regions together with the statistical and systematic uncertainties. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. The cross sections are defined for OS-SS events.

Measured integrated cross sections ratio of the production of a W+ and W- bosons in association with a single c-jet and exactly zero or one additional non-c-jets in the fiducial regions together with the statistical and systematic uncertainties. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. The cross sections are defined for OS-SS events.

Measured integrated cross sections of the production of a W boson in association with a single c-jet decaying into a soft muon in the fiducial regions together with the statistical and systematic uncertainties. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. Soft muons are associated to c-jets within a cone of DeltaR<0.5. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events.

Correlation matrix corresponding to the total uncertainties of measured integrated cross sections of the production of a W boson with a single c-jet, a D meson or a D* meson times the branching ratio W -> l nu in the fiducial regions.

Systematic uncertainties after the averaging procedure of the inclusive cross sections in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels. The luminosity is included in these correlated systematic uncertainties.

Systematic uncertainties after the averaging procedure of the differential cross sections as function of the lepton pseudo-rapidity in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels and bins. The luminosity is included in these correlated systematic uncertainties. The systematic uncertainties for the W+ + cbar-jet channel are shown in this table.

Systematic uncertainties after the averaging procedure of the differential cross sections as function of the lepton pseudo-rapidity in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels and bins. The luminosity is included in these correlated systematic uncertainties. The systematic uncertainties for the W- + c-jet channel are shown in this table.

Systematic uncertainties after the averaging procedure of the differential cross sections as function of the lepton pseudo-rapidity in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels and bins. The luminosity is included in these correlated systematic uncertainties. The systematic uncertainties for the W+ D- and W- D+ channels are shown in this table.

Systematic uncertainties after the averaging procedure of the differential cross sections as function of the lepton pseudo-rapidity in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels and bins. The luminosity is included in these correlated systematic uncertainties. The systematic uncertainties for the W+ D*- and W- D*+ channels are shown in this table.

Theoretical Predictions for the integrated cross section of the production of W+ and W- bosons associated with a single c-jet, a D meson or a D* meson in the fiducial regions together with the statistical and systematic uncertainties. For the W+c-jet cross sections events with more than one c-jet are discarded. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events. The predictions have been obtained the aMC@NLO MC simulation interfaced to the Herwig++ parton shower programme. The uncertainties on the predictions entail PDF uncertainties, parton shower, fragmentation and scale uncertainties. The predictions are reweighted using LHAPDF from the CT10nlo PDF set to the following PDF sets with the LHAPDF IDs given in brackets: CT10nlo (11000), MSTW2008nlo68cl (21100), NNPDF23_nlo_as_0119 (230000), NNPDF23_nlo_collider_as_0119 (236000), HERAPDF15NLO (EIG+VAR, 60700+60730), ATLAS-epWZ12 (EIG+VAR, 65000+65040).

PDF uncertainty for each of the used PDF sets as well as the combined parton shower, fragmentation and scale uncertainties (given in percent) for the theoretical Predictions for the integrated cross section of the production of W+ and W- bosons associated with a single c-jet, a D meson or a D* meson in the fiducial regions together with the statistical and systematic uncertainties. If added quadratically, these uncertainties represent the total uncertainty on the quoted theory prediction. For the W+c-jet cross sections events with more than one c-jet are discarded. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events. The predictions have been obtained the aMC@NLO MC simulation interfaced to the Herwig++ parton shower programme. The uncertainties on the predictions entail PDF uncertainties, FSR uncertainties and scale uncertainties. The predictions are reweighted using LHAPDF from the CT10nlo PDF set to the following PDF sets with the LHAPDF IDs given in brackets: CT10nlo (11000), MSTW2008nlo68cl (21100), NNPDF23_nlo_as_0119 (230000), NNPDF23_nlo_collider_as_0119 (236000), HERAPDF15NLO (EIG+VAR, 60700+60730), ATLAS-epWZ12 (EIG+VAR, 65000+65040). The determination of the parton shower, fragmentation and scale uncertainties is detailed in the paper.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of fourth jet rapidity for events with four or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton transverse momentum for events with one or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton transverse momentum for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton transverse momentum for events with three or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton transverse momentum for events with four or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton pseudorapidity for events with one or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton pseudorapidity for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton pseudorapidity for events with three or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton pseudorapidity for events with four or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of rapidity separation between the two highest pT jets for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of rapidity separation between the two highest pT jets for events with three or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of rapidity separation between the two most rapidity-separated hard (pT>20 GeV) jets for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of rapidity separation between the two most rapidity-separated hard (pT>20 GeV) jets for events with three or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of azimuthal angle separation between the two highest pT jets for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of azimuthal angle separation between the two most rapidity-separated hard (pT>20 GeV) jets for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of DeltaR separation between the two highest pT jets for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

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Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of W boson pT for events with one or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of W boson pT for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of W boson pT for events with three or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of W boson pT for events with four or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of the transverse momentum of the dijet system of the two highest pT jets for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of the transverse momentum of the dijet system of the two highest pT jets for events with three or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of dijet invariant mass of the two highest pT jets for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of dijet invariant mass of the two highest pT jets for events with three or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of HT for events with one or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of HT for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of HT for events with three or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of HT for events with four or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Average number of jets as a function of HT for events with one or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Average number of jets as a function of HT for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Average number of jets as a function of the rapidity separation between the two highest pT jets for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Average number of jets as a function of the rapidity separation between the two most rapidity separated jets for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Probability of third jet emission as a function of the rapidity separation of the two highest pT jets for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Probability of third jet emission as a function of the rapidity separation of the two most rapidity-separated hard (pT>20 GeV) for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Probability of third jet emission as a function of rapidity separation between the two highest pT jets with the requirement that the additional jet be emitted into the rapidity interval defined by the two highest pT jets, for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Fraction of events with two jets produced in association with a W boson that do not contain a third hard (pT>20 GeV) jet in the rapidity interval between the two highest pT jets, as a function of rapidity separation between the two highest pT jets. First uncertainty is statistical, second uncertainty is systematic.

Fraction of events with two jets produced in association with a W boson that do not contain a third hard (pT>20 GeV) jet in the rapidity interval between the two most rapidity-separated jets, as a function of rapidity separation between the two most rapidity-separated jets. First uncertainty is statistical, second uncertainty is systematic.

Inclusive b-jet double-differential cross sections and their ratio to inclusive jet cross sections in the |rapidity| range 0.0 to 0.5, using a jet resolution R value of 0.5.

Inclusive b-jet double-differential cross sections and their ratio to inclusive jet cross sections in the |rapidity| range 0.5 to 1.0, using a jet resolution R value of 0.5.

Inclusive b-jet double-differential cross sections and their ratio to inclusive jet cross sections in the |rapidity| range 1.0 to 1.5, using a jet resolution R value of 0.5.

Inclusive b-jet double-differential cross sections and their ratio to inclusive jet cross sections in the |rapidity| range 1.5 to 2.0, using a jet resolution R value of 0.5.

Inclusive b-jet double-differential cross sections and their ratio to inclusive jet cross sections in the |rapidity| range 2.0 to 2.2, using a jet resolution R value of 0.5.

Inclusive b-jet (with muon) differential cross sections in the |rapidity| range 0.0 to 2.4, using a jet resolution R value of 0.5. Muon visible range corresponds to PT(MU) > 9 GeV and |pseudorapidity(MU)| range 0.0 to 2.4.

Inclusive b-jet differential cross sections in the |rapidity| range 0.0 to 2.4, using a jet resolution R value of 0.5. Extrapolated result from muuon visible range PT(MU) > 9 GeV and |pseudorapidity(MU)| < 2.4.

Inclusive b-jet (with muon) differential cross sections in the PT range greater than 30 GeV, using a jet resolution R value of 0.5. Muon visible range corresponds to PT(MU) > 9 GeV and |pseudorapidity(MU)| < 2.4.

Inclusive b-jet differential cross sections in the PT range greater than 30 GeV, using a jet resolution R value of 0.5. Extrapolated result from muon visible range PT(MU) > 9 GeV and |pseudorapidity(MU)| < 2.4.

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.

Measured differential cross section as a function of the muon pseudorapidity.

Measured differential cross section as a function of the jet transverse momentum.

Measured differential cross section as a function of the jet pseudorapidity.

Measured cross sections for beauty production with a muon and jet for the Q**2 bin 2 to 4 GeV**2.

Measured cross sections for beauty production with a muon and jet for the Q**2 bin 4 to 20 GeV**2.

Measured cross sections for beauty production with a muon and jet for the Q**2 bin 20 to 45 GeV**2.

Measured cross sections for beauty production with a muon and jet for the Q**2 bin 45 to 100 GeV**2.

Measured cross sections for beauty production with a muon and jet for the Q**2 bin 100 to 250 GeV**2.

Measured cross sections for beauty production with a muon and jet for the Q**2 bin 250 to 3000 GeV**2.

Extracted values of F2 for B-BBAR production at an X value of 0.00013. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.

Extracted values of F2 for B-BBAR production at an X value of 0.0002. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.

Extracted values of F2 for B-BBAR production at an X value of 0.0005. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.

Extracted values of F2 for B-BBAR production at an X value of 0.002. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.

Extracted values of F2 for B-BBAR production at an X value 0.005.

Extracted values of F2 for B-BBAR production at an X value of 0.013. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.

Bin averaged differential cross section as a function of ET in the defined phase space.

Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range -1.00 to -0.57.

Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range -0.57 to 0.20.

Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range 0.20 to 0.94.

Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range 0.94 to 1.42.

Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range 1.42 to 2.43.

Bin averaged differential cross section for prompt photon plus jet as a function of the photon transverse energy.

Bin averaged differential cross section for prompt photon plus jet as a function of the photon pseudorapidity.

Bin averaged differential cross section for prompt photon plus jet as a function of the jet transverse energy.

Bin averaged differential cross section for prompt photon plus jet as a function of the jet pseudorapidity.

Bin averaged differential cross section for prompt photon plus jet as a function of X(C=GAMMA,LO) thelongitudinal momentum fraction of the partons in the photon in LO approximation.

Bin averaged differential cross section for prompt photon plus jet as a function of X(C=P,LO) thelongitudinal momentum fraction of the partons in the proton in LO approximation.

Bin averaged differential cross section for prompt photon plus jet as a function of the photons transverse momentum perpendicular to the jet direction separated into two regions of X(C=GAMMA,LO).

Bin averaged differential cross section for prompt photon plus jet as a function of the difference in azimuthal angle between the photon and the jet separated into two regions of X(C=GAMMA,LO).

Differential cross section w.r.t. the muon transverse momentum.

Differential cross section w.r.t. the muon pseudorapidity.

Differential cross section w.r.t. the JET transverse energy.

Distribution of the total energy outside the reconstructed jets for the completed data samples. Also tabulated is the estimated background.

Distribution of the total energy outside the reconstructed jets for the 'Dir' domain. Also tabulated is the estimated background.

Distribution of the total energy outside the reconstructed jets for the 'SR' domain. Also tabulated is the estimated background.

Distribution of the total energy outside the reconstructed jets for the 'DR' domain. Also tabulated is the estimated background.

Observed distribution of the charged particle multiplicity.

Observed distribution of the charged particle invariant mass.

Observed distribution of the mean of X(C=GAMMA-PLUS) and X(GAMMA-MINUS).

Observed mean number of particles in the reconstructed jets.

Differential cross sections as a function of X(C=GAMMA) from beauty and charm quarks.

Differential cross sections for the most energetic jet as a function of ET from beauty and charm quarks.

Differential cross sections for the most energetic jet as a function of ET from beauty and charm quarks.

Differential cross sections as a function of the electron ET for the jet associated to the electron from beauty or charm decays.

Differential cross section for events with at least 3-jets as a function of the pseudorapidity of each jet.

Differential cross section for events with at least 3-jets as a function of the pseudorapidity of each jet.

Differential cross section for events with at least 3-jets as a function of X1.

Differential cross section for events with at least 3-jets as a function of X2.

Differential cross section for events with at least 3-jets as a function of the three jet angle THETA (see text of article).

Differential cross section for events with at least 3-jets as a function of the three jet angle PHI (see text of article).

Differential cross section for events with at least 3-jets as a function of the PT of the leading jet in GAMMA P centre of mass frame.

Differential cross section for events with at least 3-jets as a function of the pseudorapidity difference between the two leading.

Differential cross section as a function of x for events with at least 3 jets with one forward jet and two central jets.

Differential cross section as a function of the pseudorapidity of the leading jet for events with at least 3 jets with one forward jet and two central jets.

Differential cross section as a function of the PT of the leading jet in the GAMMA* P rest frame for events with at least 3 jets with one forward jet and two central jets.

Differential cross section as a function of X for events with at least 3 jets with two forward jets and one central jet.

Differential cross section as a function of the pseudorapidity of the leading jet for events with at least 3 jets with two forward jets and one central jet.

Differential cross section as a function of the PT of the leading jet in the GAMMA* P rest frame for events with at least 3 jets with two forward jets and one central jet.

Differential cross section as a function of the pseudorapidity of the leading jet for events with at least 3 jets and the PT of the leading jet in the GAMMA* P rest frame > 20 GeV.

Differential cross section as a function of X for events with at least 3 jets and the PT of the leading jet in the GAMMA* P rest frame > 20 GeV.

Differential cross section as a function of the difference in the pseudorapidity of the leading and fourth jets for events with at least 4 jets.

Differential cross section as a function X2 for events with at least 4 jets.

Differential cross section as a function the jet angle THETA for events with at least 4 jets.

Differential cross section as a function the PT of the leading jet in GAMMA* P rest frame for events with at least 4 jets.

Bin averaged differential cross sections of diffractive di-jet production as a function of Z(NAME=POMERON).

Bin averaged differential cross sections of diffractive di-jet production as a function centre of mass PT of the leading jet.

Bin averaged differential cross sections of diffractive di-jet production as a function of the pseudorapidity difference.

Bin averaged double differential cross sections of diffractive di-jet production as a function of Z(NAME=POMERON) in the (Q**2 + PT(LEADING JET)**2) range 29 to 50 GeV.

Bin averaged double differential cross sections of diffractive di-jet production as a function of Z(NAME=POMERON) in the (Q**2 + PT(LEADING JET)**2) range 50 to 70 GeV.

Bin averaged double differential cross sections of diffractive di-jet production as a function of Z(NAME=POMERON) in the (Q**2 + PT(LEADING JET)**2) range 70 to 100 GeV.

Bin averaged double differential cross sections of diffractive di-jet production as a function of Z(NAME=POMERON) in the (Q**2 + PT(LEADING JET)**2) range 100 to 200 GeV.

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Bin averaged differential cross section for inclusive D* production in bins of PT(D*).

Bin averaged differential cross section for inclusive D* production in bins of ETARAP(D*).

Bin averaged differential cross section for inclusive D* production in bins of Z(D*).

Bin averaged differential cross section for inclusive D* production in bins of W.

Bin averaged differential cross section for inclusive D* production in bins of ETARAP for different PT ranges.

Bin averaged differential cross section for D*+ other jet production where 'other' jet does not contain D*.

Bin averaged differential cross section for D*+ other jet production where 'other' jet does not contain D*.

Bin averaged differential cross section for D*+ other jet production where 'other' jet does not contain D*.

Bin averaged differential cross section for D*+ other jet production where 'other' jet does not contain D*.

Bin averaged differential cross section for D*+ other jet production where 'other' jet does not contain D*.

Bin averaged differential cross section for D* tagged dijet production in bins of X(C=GAMMA), the fraction of the longitudinal photon momentum entering the hard scattering process.

Bin averaged differential cross section for D*+ other jet data sample as a function of the difference in the azimuthal angle of the D* and the jet.