Predicted and observed yields as a function of $m_{4\ell}$ in the VBS-Suppressed region. Overflow events are included in the last bin of the distribution.

Relative systematic uncertainties in the unfolded differential cross section for 4ljj production in the VBS-Enhanced region as a function of m_{jj}

Relative systematic uncertainties in the unfolded differential cross section for 4ljj production in the VBS-Enhanced region as a function of m_{4\ell}

Differential cross-sections for inclusive 4ljj production in the VBS-Enhanced region as a function of $m_{jj}$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Suppressed region as a function of $m_{jj}$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Enhanced region as a function of $m_{4\ell}$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Suppressed region as a function of $m_{4\ell}$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Enhanced region as a function of $ p_{T,4l}$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Suppressed region as a function of $ p_{T,4l}$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Enhanced region as a function of $\Delta\phi_{jj}$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Suppressed region as a function of $\Delta\phi_{jj}$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Enhanced region as a function of $|\Delta y_{jj}|$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Suppressed region as a function of $|\Delta y_{jj}|$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Enhanced region as a function of $cos(\theta^{*}_{12})$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Suppressed region as a function of $cos(\theta^{*}_{12})$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Enhanced region as a function of $cos(\theta^{*}_{34})$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Suppressed region as a function of $cos(\theta^{*}_{34})$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Enhanced region as a function of $p_{T,jj}$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Suppressed region as a function of $p_{T,jj}$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Enhanced region as a function of $p_{T,4ljj}$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Suppressed region as a function of $p_{T,4ljj}$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Enhanced region as a function of $S_{T,4ljj}$. Overflow events are included in the last bin of the distribution.

Differential cross-sections for inclusive 4ljj production in the VBS-Suppressed region as a function of $S_{T,4ljj}$. Overflow events are included in the last bin of the distribution.

Statistical correlation between different bins of the unfolded cross-section for all the measured observables in the VBS-Enhanced region.

Statistical correlation between different bins of the unfolded cross-section for all the measured observables in the VBS-Suppressed region.

Final state radiation correction used in the $\phi_{\eta}^{*}$ cross-section measurement. The first uncertainty is statistical and the second is systematic.

Final state radiation correction used in the $y^{Z}-p_{T}^{Z}$ cross-section measurement. The first uncertainty is statistical and the second is systematic.

Final state radiation correction used in the $y^{Z}-\phi_{\eta}^{*}$ cross-section measurement. The first uncertainty is statistical and the second is systematic.

Correlation matrix of statistical uncertainty for one-dimensional $y^Z$ measurement.

Correlation matrix of statistical uncertainty for one-dimensional $p_{T}^{Z}$ measurement.

Correlation matrix of statistical uncertainty for one-dimensional $\phi_{\eta}^{*}$ measurement.

Correlation matrix of statistical uncertainty for two-dimensional $y^Z-p_{T}^{Z}$ measurement.

Correlation matrix of statistical uncertainty for two-dimensional $y^Z-\phi_{\eta}^{*}$ measurement.

Correlation matrix of efficiency uncertainty for one-dimensional $y^Z$ measurement.

Correlation matrix of efficiency uncertainty for one-dimensional $p_{T}^{Z}$ measurement.

Correlation matrix of efficiency uncertainty for one-dimensional $\phi_{\eta}^{*}$ measurement.

Correlation matrix of efficiency uncertainty for two-dimensional $y^Z-p_{T}^{Z}$ measurement.

Correlation matrix of efficiency uncertainty for two-dimensional $y^Z-\phi_{\eta}^{*}$ measurement.

Measured total $Z$-boson cross-section for different datasets. The first uncertainty is statistical, the second systematic, and the third is due to the luminosity.

Measured single differential cross-sections in interval regions of $y^{Z}$. The first uncertainty is statistical, the second systematic, and the third is due to the luminosity.

Measured single differential cross-sections in interval regions of $p_{T}^{Z}$. The first uncertainty is statistical, the second systematic, and the third is due to the luminosity.

Measured single differential cross-sections in interval regions of $\phi_{\eta}^{*}$. The first uncertainty is statistical, the second systematic, and the third is due to the luminosity.

Measured double differential cross-sections in interval regions of $y^{Z}$ and $p_{T}^{Z}$. The first uncertainty is statistical, the second systematic, and the third is due to the luminosity.

Measured double differential cross-sections in interval regions of $y^{Z}$ and $\phi_{\eta}^{*}$. The first uncertainty is statistical, the second systematic, and the third is due to the luminosity.

Systematic uncertainties in the single differential cross-sections in interval regions of $y^{Z}$, presented in percentage. The contributions from efficiency (Eff), background (BKG), final state radiation (FSR), closure test (Closure), and alignment and calibration (Alignment) are shown.

Systematic uncertainties in the single differential cross-sections in interval regions of $p_{T}^{Z}$, presented in percentage. The contributions from efficiency (Eff), background (BKG), final state radiation (FSR), closure test (Closure), and alignment and calibration (Alignment) are shown.

Systematic uncertainties in the single differential cross-sections in interval regions of $\phi_{\eta}^{*}$, presented in percentage. The contributions from efficiency (Eff), background (BKG), final state radiation (FSR), closure test (Closure), and alignment and calibration (Alignment) are shown.

Systematic uncertainties in the double differential cross-sections in interval regions of $y^{Z}$ and $p_{T}^{Z}$, presented in percentage. The contributions from efficiency (Eff), background (BKG), final state radiation (FSR), closure test (Closure), and alignment and calibration (Alignment) are shown.

Systematic uncertainties in the double differential cross-sections in interval regions of $y^{Z}$ and $\phi_{\eta}^{*}$, presented in percentage. The contributions from efficiency (Eff), background (BKG), final state radiation (FSR), closure test (Closure), and alignment and calibration (Alignment) are shown.

Differential cross-sections for EW $Zjj$ production as a function of $\Delta\phi_{jj}$ with breakdown of associated uncertainties. The statistical uncertainty is correlated across bins according to the statistical cross correlation matrix presented in Table 21.

Differential cross-sections for inclusive $Zjj$ production in the EW $Zjj$ signal region ($N^\mathrm{gap}_\mathrm{jets}=0$, $\xi_Z < 0.5$) as a function of $m_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in the EW $Zjj$ signal region ($N^\mathrm{gap}_\mathrm{jets}=0$, $\xi_Z < 0.5$) as a function of $\Delta y_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in the EW $Zjj$ signal region ($N^\mathrm{gap}_\mathrm{jets}=0$, $\xi_Z < 0.5$) as a function of $p_{\mathrm{T},\ell\ell}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in the EW $Zjj$ signal region ($N^\mathrm{gap}_\mathrm{jets}=0$, $\xi_Z < 0.5$) as a function of $\Delta\phi_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRa ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z < 0.5$) as a function of $m_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRa ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z < 0.5$) as a function of $\Delta y_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRa ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z < 0.5$) as a function of $p_{\mathrm{T},\ell\ell}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRa ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z < 0.5$) as a function of $\Delta\phi_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRb ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z > 0.5$) as a function of $m_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRb ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z > 0.5$) as a function of $\Delta y_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRb ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z > 0.5$) as a function of $p_{\mathrm{T},\ell\ell}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRb ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z > 0.5$) as a function of $\Delta\phi_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRc ($N^\mathrm{gap}_\mathrm{jets} = 0$, $\xi_Z > 0.5$) as a function of $m_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRc ($N^\mathrm{gap}_\mathrm{jets} = 0$, $\xi_Z > 0.5$) as a function of $\Delta y_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRc ($N^\mathrm{gap}_\mathrm{jets} = 0$, $\xi_Z > 0.5$) as a function of $p_{\mathrm{T},\ell\ell}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRc ($N^\mathrm{gap}_\mathrm{jets} = 0$, $\xi_Z > 0.5$) as a function of $\Delta\phi_{jj}$ with breakdown of associated uncertainties.

Statistical correlation between bins of the differential cross-section measurements of EW $Zjj$ production in the signal region ($N^\mathrm{gap}_\mathrm{jets} = 0$, $\xi_Z < 0.5$). The associated measured central values, statistical uncertainty magnitude and bin ranges are presented in Tables 1-4. The bins are presented in order such that for example mjj_bin_1 spans $m_{jj} \in (1000,1500)$ GeV (see Table 1), while pT_ll_bin7 spans $p_\mathrm{T}^{ll} \in (200,275)$ GeV (see Table 3).

Differential cross-section D(SIG)/DETARAP(JET) for photons in the given X(GAMMA) range accompanied by a jet. The corresponding hadronisation corrections are also given.

Differential cross-section D(SIG)/DXOBS(P) for photons in the given X(GAMMA) range accompanied by a jet. The corresponding hadronisation corrections are also given.

Differential cross-section D(SIG)/D(ETARAP(GAMMA) - ETARAP(JET)) for photons in the given X(GAMMA) range accompanied by a jet. The corresponding hadronisation corrections are also given.

Differential cross-section D(SIG)/DDELTA(PHI) for photons in the given X(GAMMA) range accompanied by a jet. The corresponding hadronisation corrections are also given.

Correlation coefficients for the differential cross-section of $Z \to e^+ e^-$ at 7 TeV between bins of $Z$ rapidity, $y_{Z}$. Both statistical and systematic contributions are included.

Correlation coefficients for the differential cross-section of $Z \to e^+ e^-$ at 7 TeV between bins of $\phi^*$. Both statistical and systematic contributions are included.

Normalized differential cross-section $d\ln\sigma(pp\rightarrow J/\psi \Lambda_c^+ X)/dp_T(J/\psi)$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(\Lambda_c^+)<4$, $3<p_T(\Lambda_c^+) <12$ GeV/$c$ region.

Normalized differential cross-section $d\ln\sigma(pp\rightarrow J/\psi D^0 X)/dp_T(D^0)$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $d\ln\sigma(pp\rightarrow J/\psi D^+ X)/dp_T(D^+)$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $d\ln\sigma(pp\rightarrow J/\psi D_s^+ X)/dp_T(D_s^+)$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D_s^+)<4$, $3<p_T(D_s^+)<12$ GeV/$c$ region.

Normalized differential cross-section $d\ln\sigma(pp\rightarrow J/\psi \Lambda_c^+ X)/dp_T(\Lambda_c^+)$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(\Lambda_c^+)<4$, $3<p_T(\Lambda_c^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^0 X \right)}{dp_T( D^0 )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^+ X \right)}{dp_T( D )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D_s^+ X \right)}{dp_T( D )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D_s^+)<4$, $3<p_T(D_s^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D^+ X \right)}{dp_T( D^+ )}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D_s^+ X \right)}{dp_T( D )}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(D_s^+)<4$, $3<p_T(D_s^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{D}^0 X \right)}{dp_T( D )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^- X \right)}{dp_T( D )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12~GeV/c$, $2<y(D^-)<4$, $3<p_T(D^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D_s^- X \right)}{dp_T( D )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{\Lambda}_c^- X \right)}{dp_T( C )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(\bar{\Lambda}_c^-)<4$, $3<p_T(\bar{\Lambda}_c^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D- X \right)}{dp_T( D )}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D_s- X \right)}{dp_T( D )}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ \bar{\Lambda}_c^- X \right)}{dp_T( C )}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(\bar{\Lambda}_c^-)<4$, $3<p_T(\bar{\Lambda}_c^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D^0 X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D^+ X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D_s^+ X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D_s^+)<4$, $3<p_T(D_s^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D^0 X \right)}{d \Delta y }$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D^+ X \right)}{d \Delta y }$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D_s^+ X \right)}{d \Delta y}$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D_s^+)<4$, $3<p_T(D_s^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^0 X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^+ X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^0 X \right)}{d \left| \Delta y \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12~GeV/c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^+ X \right)}{d \left| \Delta y \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{D}^0 X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^- X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ , $2<y(D^-)<4$, $3<p_T(D^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D_s^- X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ , $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D^- X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D_s^- X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{D}^0 X \right)}{d \left| \Delta y \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12~GeV/c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^- X \right)}{d \left| \Delta y \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ , $2<y(D^-)<4$, $3<p_T(D^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D_s^- X \right)}{d \left| \Delta y \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D^- X \right)}{d \left| \Delta y \right|}$ for $2<y(D^-)<4$, $3<p_T(D^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D_s^- X \right)}{d \left| \Delta y \right|}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D^0 X \right)}{d m_{J/\psi D^0} }$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D^+ X \right)}{d m_{J/\psi D^+} }$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D_s^+ X \right)}{d m_{J/\psi D_s^+} }$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D_s^+)<4$, $3<p_T(D_s^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^0 X \right)}{d m_{D^0 D^0} }$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^+ X \right)}{d m_{D^0 D^+} }$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{D}^0 X \right)}{d m_{D^0 \bar{D}^0} }$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^- X \right)}{d m_{D^0 D^-} }$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D^-)<4$, $3<p_T(D^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D_s^- X \right)}{d m_{D^0 D_s^-} }$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{\Lambda}_c^- X \right)}{d m_{D^0 D_s^-} }$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(\bar{\Lambda}_c^-)<4$, $3<p_T(\bar{\Lambda}_c^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D^- X \right)}{d m_{D^+ D^-} }$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D_s^- X \right)}{d m_{D^+ D_s^-} }$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ \bar{\Lambda}_c^- X \right)}{d m_{D^+ \bar{\Lambda}_c^-} }$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(\bar{\Lambda}_c^-)<4$, $3<p_T(\bar{\Lambda}_c^-)<12$ GeV/$c$ region.

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.

Diphoton production cross section as a function of the diphoton rapidity.

Diphoton production cross section differential in the cosine of the polar angle in the Collins-Soper frame.

Diphoton production cross section differential in the sub-leading to leading photon transverse momentum ratio (z).

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.