Observed and predicted mTtot distribution in the b-tag category of the 2tau_h channel. Despite listing this as an exclusive final state (as there must be at least one b-jets), there is no explicit selection on the presence of additional light-flavour jets. Please note that the bin content is divided by the bin width in the paper figure, but not in the HepData table. The last bin includes overflows. The combined prediction for A and H bosons with masses of 300, 500 and 800 GeV and $\tan\beta$ = 10 in the hMSSM scenario are also provided.

Observed and predicted mTtot distribution for the b-inclusive selection in the 1l1tau_h channel. Please note that the bin content is divided by the bin width in the paper figure, but not in the HepData table. In the paper, the first bin is cut off at 60 GeV for aesthetics but contains underflows down to 50 GeV as in the HepData table. The last bin includes overflows. The prediction for a SSM Zprime with masses of 1500, 2000 and 2500 GeV are also provided.

Observed and predicted mTtot distribution for the b-inclusive selection in the 2tau_h channel. Please note that the bin content is divided by the bin width in the paper figure, but not in the HepData table. The last bin includes overflows. The prediction for a SSM Zprime with masses of 1500, 2000 and 2500 GeV are also provided.

Observed and expected 95% CL upper limits on the b-associated Higgs boson production cross section times ditau branching fraction as a function of the boson mass.

Observed and expected 95% CL upper limits on the Drell Yan production cross section times ditau branching fraction as a function of the Zprime boson mass.

Observed and expected 95% CL upper limits on the Higgs boson production cross section times ditau branching fraction as a function of the boson mass and the relative strength of the b-associated production.

Ratio of the 95% CL upper limits on the production cross section times branching fraction for alternate Zprime models with respect to the SSM, both observed and expected are shown.

Acceptance, acceptance times efficiency and b-tag category fraction for a scalar boson produced by gluon-gluon fusion as a function of the scalar boson mass.

Acceptance, acceptance times efficiency and b-tag category fraction for a scalar boson produced by b-associated production as a function of the scalar boson mass.

Acceptance and acceptance times efficiency for a heavy gauge boson produced by Drell Yan as a function of the gauge boson mass.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Two dimensional likelihood scan of the gluon-gluon fusion cross section times braching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the Higgs boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. Vaules are provided for the fit to the observed data and to the expected data, which is the sum of Standard Model contributions not including the SM Higgs boson. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively.

Observed and expected 95% CL upper limits on the gluon-gluon fusion Higgs boson production cross section times ditau branching fraction as a function of the boson mass.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 1$^\text{st}$ jet $p_{\text{T}}$, $p_{\text{T}}(\text{j}_1)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 2$^\text{nd}$ jet $p_{\text{T}}$, $p_{\text{T}}(\text{j}_2)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 2$^\text{nd}$ jet $p_{\text{T}}$, $p_{\text{T}}(\text{j}_2)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 3$^\text{rd}$ jet $p_{\text{T}}$, $p_{\text{T}}(\text{j}_3)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 3$^\text{rd}$ jet $p_{\text{T}}$, $p_{\text{T}}(\text{j}_3)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 4$^\text{th}$ jet $p_{\text{T}}$, $p_{\text{T}}(\text{j}_4)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 4$^\text{th}$ jet $p_{\text{T}}$, $p_{\text{T}}(\text{j}_4)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 5$^\text{th}$ jet $p_{\text{T}}$, $p_{\text{T}}(\text{j}_5)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 5$^\text{th}$ jet $p_{\text{T}}$, $p_{\text{T}}(\text{j}_5)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 1$^\text{st}$ jet $|y|$, $|y(\text{j}_1)|$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 1$^\text{st}$ jet $|y|$, $|y(\text{j}_1)|$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 2$^\text{nd}$ jet $|y|$, $|y(\text{j}_2)|$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 2$^\text{nd}$ jet $|y|$, $|y(\text{j}_2)|$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 3$^\text{rd}$ jet $|y|$, $|y(\text{j}_3)|$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 3$^\text{rd}$ jet $|y|$, $|y(\text{j}_3)|$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 4$^\text{th}$ jet $|y|$, $|y(\text{j}_4)|$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 4$^\text{th}$ jet $|y|$, $|y(\text{j}_4)|$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 5$^\text{th}$ jet $|y|$, $|y(\text{j}_5)|$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the 5$^\text{th}$ jet $|y|$, $|y(\text{j}_5)|$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the Z boson $|y|$, $|y(\text{Z})|$, for events with at least one jet and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the Z boson $|y|$, $|y(\text{Z})|$, for events with at least one jet.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the Z boson $|y|$, $|y(\text{Z})|$ for events with at least one jet and $p_\text{T}(\text{Z}) > 150\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the Z boson $|y|$, $|y(\text{Z})|$ for events with at least one jet and $p_\text{T}(\text{Z}) > 150\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the Z boson $|y|$, $|y(\text{Z})|$ for events with at least $p_\text{T}(\text{Z}) > 300\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the Z boson $|y|$, $|y(\text{Z})|$ for events with at least $p_\text{T}(\text{Z}) > 300\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the Z boson and the leading jet, $y_{\text{diff}}(\text{Z}, \text{j}_1)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the Z boson and the leading jet, $y_{\text{diff}}(\text{Z}, \text{j}_1)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the Z boson and the leading jet, $y_{\text{diff}}(\text{Z}, \text{j}_1)$ for events with $p_{\text{T}}(\text{Z}) > 150\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the Z boson and the leading jet, $y_{\text{diff}}(\text{Z}, \text{j}_1)$ for events with $p_{\text{T}}(\text{Z}) > 150\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the Z boson and the leading jet, $y_{\text{diff}}(\text{Z}, \text{j}_1)$ for events with $p_{\text{T}}(\text{Z}) > 300\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the Z boson and the leading jet, $y_{\text{diff}}(\text{Z}, \text{j}_1)$ for events with $p_{\text{T}}(\text{Z}) > 300\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the Z boson and the 2$^\text{nd}$leading jet, $y_{\text{diff}}(\text{Z}, \text{j}_2)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the Z boson and the 2$^\text{nd}$leading jet, $y_{\text{diff}}(\text{Z}, \text{j}_2)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the Z boson and the 3$^\text{rd}$leading jet, $y_{\text{diff}}(\text{Z}, \text{j}_3)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the Z boson and the 3$^\text{rd}$leading jet, $y_{\text{diff}}(\text{Z}, \text{j}_3)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the Z boson and the system constituted of the two leading jets, $y_{\text{diff}}(\text{Z}, \text{dijet})$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the Z boson and the system constituted of the two leading jets, $y_{\text{diff}}(\text{Z}, \text{dijet})$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the two leading jets, $y_{\text{diff}}(\text{j}_1, \text{j}_2)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{diff}}$ of the two leading jets, $y_{\text{diff}}(\text{j}_1, \text{j}_2)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the two leading jets, $y_{\text{sum}}(\text{j}_1, \text{j}_2)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the two leading jets, $y_{\text{sum}}(\text{j}_1, \text{j}_2)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the Z boson and the leading jet, $y_{\text{sum}}(\text{Z}, \text{j}_1)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the Z boson and the leading jet, $y_{\text{sum}}(\text{Z}, \text{j}_1)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the Z boson and the leading jet, $y_{\text{sum}}(\text{Z}, \text{j}_1)$ for events with $p_{\text{T}}(\text{Z}) > 150\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the Z boson and the leading jet, $y_{\text{sum}}(\text{Z}, \text{j}_1)$ for events with $p_{\text{T}}(\text{Z}) > 150\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the Z boson and the leading jet, $y_{\text{sum}}(\text{Z}, \text{j}_1)$ for events with $p_{\text{T}}(\text{Z}) > 300\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the Z boson and the leading jet, $y_{\text{sum}}(\text{Z}, \text{j}_1)$ for events with $p_{\text{T}}(\text{Z}) > 300\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the Z boson and the 2$^\text{nd}$leading jet, $y_{\text{sum}}(\text{Z}, \text{j}_2)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the Z boson and the 2$^\text{nd}$leading jet, $y_{\text{sum}}(\text{Z}, \text{j}_2)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the Z boson and the 3$^\text{rd}$leading jet, $y_{\text{sum}}(\text{Z}, \text{j}_3)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the Z boson and the 3$^\text{rd}$leading jet, $y_{\text{sum}}(\text{Z}, \text{j}_3)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the Z boson and the system constituted of the two leading jets, $y_{\text{sum}}(\text{Z}, \text{dijet})$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the $y_{\text{sum}}$ of the Z boson and the system constituted of the two leading jets, $y_{\text{sum}}(\text{Z}, \text{dijet})$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of $H_\text{T}$ for events with at least one jet, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of $H_\text{T}$ for events with at least one jet.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of $H_\text{T}$ for events with at least two jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of $H_\text{T}$ for events with at least two jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of $H_\text{T}$ for events with at least three jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of $H_\text{T}$ for events with at least three jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of $H_\text{T}$ for events with at least four jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of $H_\text{T}$ for events with at least four jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of $H_\text{T}$ for events with at least five jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of $H_\text{T}$ for events with at least five jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet for events with at least ine jet, $\Delta\Phi(\text{Z},\text{j}_1)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet for events with at least ine jet, $\Delta\Phi(\text{Z},\text{j}_1)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet for events with at least two jets, $\Delta\Phi(\text{Z},\text{j}_1)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet for events with at least two jets, $\Delta\Phi(\text{Z},\text{j}_1)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet for events with at least three jets, $\Delta\Phi(\text{Z},\text{j}_1)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet for events with at least three jets, $\Delta\Phi(\text{Z},\text{j}_1)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 2$^\text{nd}$ leading jet for events with at least three jets, $\Delta\Phi(\text{Z},\text{j}_1)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 2$^\text{nd}$ leading jet for events with at least three jets, $\Delta\Phi(\text{Z},\text{j}_1)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 3$^\text{rd}$ leading jet for events with at least three jets, $\Delta\Phi(\text{Z},\text{j}_1)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 3$^\text{rd}$ leading jet for events with at least three jets, $\Delta\Phi(\text{Z},\text{j}_1)$.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet$\Delta\Phi(\text{Z},\text{j}_1)$, for events with $p_{\text{T}}(\text{Z})>150\,$GeV and at least two jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet$\Delta\Phi(\text{Z},\text{j}_1)$, for events with $p_{\text{T}}(\text{Z})>150\,$GeV and at least two jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet$\Delta\Phi(\text{Z},\text{j}_1)$, for events with $p_{\text{T}}(\text{Z})>150\,$GeV and at least two jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet$\Delta\Phi(\text{Z},\text{j}_1)$, for events with $p_{\text{T}}(\text{Z})>150\,$GeV and at least two jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet$\Delta\Phi(\text{Z},\text{j}_1)$, for events with $p_{\text{T}}(\text{Z})>150\,$GeV and at least three jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet$\Delta\Phi(\text{Z},\text{j}_1)$, for events with $p_{\text{T}}(\text{Z})>150\,$GeV and at least three jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 2$^{\text{nd}}$ leading jet$\Delta\Phi(\text{Z},\text{j}_2)$, for events with $p_{\text{T}}(\text{Z})>150\,$GeV and at least three jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 2$^{\text{nd}}$ leading jet$\Delta\Phi(\text{Z},\text{j}_2)$, for events with $p_{\text{T}}(\text{Z})>150\,$GeV and at least three jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 3$^{\text{rd}}$ leading jet$\Delta\Phi(\text{Z},\text{j}_3)$, for events with $p_{\text{T}}(\text{Z})>150\,$GeV and at least three jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 3$^{\text{rd}}$ leading jet$\Delta\Phi(\text{Z},\text{j}_3)$, for events with $p_{\text{T}}(\text{Z})>150\,$GeV and at least three jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet, $\Delta\Phi(\text{Z},\text{j}_1)$, for events with $p_{\text{T}}(\text{Z})>300\,$GeV and at least one jet, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet, $\Delta\Phi(\text{Z},\text{j}_1)$, for events with $p_{\text{T}}(\text{Z})>300\,$GeV and at least one jet.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet, $\Delta\Phi(\text{Z},\text{j}_1)$, for events with $p_{\text{T}}(\text{Z})>300\,$GeV and at least two jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet, $\Delta\Phi(\text{Z},\text{j}_1)$, for events with $p_{\text{T}}(\text{Z})>300\,$GeV and at least two jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet, $\Delta\Phi(\text{Z},\text{j}_1)$, for events with $p_{\text{T}}(\text{Z})>300\,$GeV and at least three jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet, $\Delta\Phi(\text{Z},\text{j}_1)$, for events with $p_{\text{T}}(\text{Z})>300\,$GeV and at least three jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 2$^{\text{nd}}$ leading jet, $\Delta\Phi(\text{Z},\text{j}_2)$, for events with $p_{\text{T}}(\text{Z})>300\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 2$^{\text{nd}}$ leading jet, $\Delta\Phi(\text{Z},\text{j}_2)$, for events with $p_{\text{T}}(\text{Z})>300\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 3$^{\text{rd}}$ leading jet, $\Delta\Phi(\text{Z},\text{j}_3)$, for events with $p_{\text{T}}(\text{Z})>300\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 3$^{\text{rd}}$ leading jet, $\Delta\Phi(\text{Z},\text{j}_3)$, for events with $p_{\text{T}}(\text{Z})>300\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet, $\Delta\Phi(\text{Z},\text{j}_1)$, for events with at least three jets, $p_{\text{T}}(\text{Z})>150\,$GeV, and $H_{\text{T}}>300\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the leading jet, $\Delta\Phi(\text{Z},\text{j}_1)$, for events with at least three jets, $p_{\text{T}}(\text{Z})>150\,$GeV, and $H_{\text{T}}>300\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 2$^{\text{nd}}$ leading jet, $\Delta\Phi(\text{Z},\text{j}_2)$, for events with at least three jets, $p_{\text{T}}(\text{Z})>150\,$GeV, and $H_{\text{T}}>300\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 2$^{\text{nd}}$ leading jet, $\Delta\Phi(\text{Z},\text{j}_2)$, for events with at least three jets, $p_{\text{T}}(\text{Z})>150\,$GeV, and $H_{\text{T}}>300\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 3$^{\text{rd}}$ leading jet, $\Delta\Phi(\text{Z},\text{j}_1)$, for events with at least three jets, $p_{\text{T}}(\text{Z})>150\,$GeV, and $H_{\text{T}}>300\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the Z boson and the 3$^{\text{rd}}$ leading jet, $\Delta\Phi(\text{Z},\text{j}_1)$, for events with at least three jets, $p_{\text{T}}(\text{Z})>150\,$GeV, and $H_{\text{T}}>300\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the two leading jets, $\Delta\Phi(\text{j}_1,\text{j}_2)$, for events with at least three jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the two leading jets, $\Delta\Phi(\text{j}_1,\text{j}_2)$, for events with at least three jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the two 1$^{\text{st}}$ and 3$^{\text{rd}}$ leading jets, $\Delta\Phi(\text{j}_1,\text{j}_3)$, for events with at least three jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the two 1$^{\text{st}}$ and 3$^{\text{rd}}$ leading jets, $\Delta\Phi(\text{j}_1,\text{j}_3)$, for events with at least three jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the two 2$^{\text{nd}}$ and 3$^{\text{rd}}$ leading jets, $\Delta\Phi(\text{j}_1,\text{j}_3)$, for events with at least three jets, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the two 2$^{\text{nd}}$ and 3$^{\text{rd}}$ leading jets, $\Delta\Phi(\text{j}_1,\text{j}_3)$, for events with at least three jets.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the two leading jets, $\Delta\Phi(\text{j}_1,\text{j}_2)$, for events with at least three jets and $p_{\text{T}}(\text{Z})>150\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the two leading jets, $\Delta\Phi(\text{j}_1,\text{j}_2)$, for events with at least three jets and $p_{\text{T}}(\text{Z})>150\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the 1$^{\text{st}}$ and 3$^{\text{rd}}$ leading jets, $\Delta\Phi(\text{j}_1,\text{j}_3)$, for events with at least three jets and $p_{\text{T}}(\text{Z})>150\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the 1$^{\text{st}}$ and 3$^{\text{rd}}$ leading jets, $\Delta\Phi(\text{j}_1,\text{j}_3)$, for events with at least three jets and $p_{\text{T}}(\text{Z})>150\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the 2$^{\text{nd}}$ and 3$^{\text{rd}}$ leading jets, $\Delta\Phi(\text{j}_2,\text{j}_3)$, for events with at least three jets and $p_{\text{T}}(\text{Z})>150\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the 2$^{\text{nd}}$ and 3$^{\text{rd}}$ leading jets, $\Delta\Phi(\text{j}_2,\text{j}_3)$, for events with at least three jets and $p_{\text{T}}(\text{Z})>150\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the 1$^{\text{st}}$ and 2$^{\text{nd}}$ leading jets, $\Delta\Phi(\text{j}_1,\text{j}_2)$, for events with at least three jets and $p_{\text{T}}(\text{Z})>300\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the 1$^{\text{st}}$ and 2$^{\text{nd}}$ leading jets, $\Delta\Phi(\text{j}_1,\text{j}_2)$, for events with at least three jets and $p_{\text{T}}(\text{Z})>300\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the 1$^{\text{st}}$ and 3$^{\text{rd}}$ leading jets, $\Delta\Phi(\text{j}_1,\text{j}_3)$, for events with at least three jets and $p_{\text{T}}(\text{Z})>300\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the 1$^{\text{st}}$ and 3$^{\text{rd}}$ leading jets, $\Delta\Phi(\text{j}_1,\text{j}_3)$, for events with at least three jets and $p_{\text{T}}(\text{Z})>300\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the 2$^{\text{nd}}$ and 3$^{\text{rd}}$ leading jets, $\Delta\Phi(\text{j}_1,\text{j}_3)$, for events with at least three jets and $p_{\text{T}}(\text{Z})>300\,$GeV, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the azimuthal angle between the 2$^{\text{nd}}$ and 3$^{\text{rd}}$ leading jets, $\Delta\Phi(\text{j}_1,\text{j}_3)$, for events with at least three jets and $p_{\text{T}}(\text{Z})>300\,$GeV.

The cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the mass of the system made of the two leading jets, $m_{\text{j}_1\text{j}_1}$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production measured as a function of the mass of the system made of the two leading jets, $m_{\text{j}_1\text{j}_1}$.

The cross section for Z($\rightarrow\ell\ell$) + jets production as a function of the leading jet transverse momentum and rapidity

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production as a function of the leading jet transverse momentum and rapidity

The cross section for Z($\rightarrow\ell\ell$) + jets production as a function of the Z boson and leading jet rapidities

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production as a function of the Z boson and leading jet rapidities

The cross section for Z($\rightarrow\ell\ell$) + jets production as a function of the rapidities of the Z boson and leading jet, and of the transverse momentum of the jet for the same configuration.

Bin-to-bin correlation in the the cross section for Z($\rightarrow\ell\ell$) + jets production as a function of the rapidities of the Z boson and leading jet, and of the transverse momentum of the jet for the same configuration.

Unfolded measurements of AFB in each M-|y| bin (e+e-).

Covariance matrix of Drell-Yan AFB in muon channel for |y|<1 for cos(theta)<0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for |y|<1 for cos(theta)<0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for |y|<1 for cos(theta)>0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for |y|<1 for cos(theta)>0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for 1<|y|<1.25 for cos(theta)<0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for 1<|y|<1.25 for cos(theta)<0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for 1<|y|<1.25 for cos(theta)>0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for 1<|y|<1.25 for cos(theta)>0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for 1.25<|y|<1.5 for cos(theta)<0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for 1.25<|y|<1.5 for cos(theta)<0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for 1.25<|y|<1.5 for cos(theta)>0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for 1.25<|y|<1.5 for cos(theta)>0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for 1.5<|y|<2.4 for cos(theta)<0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for 1.5<|y|<2.4 for cos(theta)<0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for 1.5<|y|<2.4 for cos(theta)>0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in muon channel for 1.5<|y|<2.4 for cos(theta)>0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for |y|<1 for cos(theta)<0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for |y|<1 for cos(theta)<0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for |y|<1 for cos(theta)>0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for |y|<1 for cos(theta)>0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 1<|y|<1.25 for cos(theta)<0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 1<|y|<1.25 for cos(theta)<0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 1<|y|<1.25 for cos(theta)>0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 1<|y|<1.25 for cos(theta)>0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 1.25|y|<1.5 for cos(theta)<0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 1.25|y|<1.5 for cos(theta)<0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 1.25|y|<1.5 for cos(theta)>0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 1.25|y|<1.5 for cos(theta)>0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 1.5<|y|<2.4 for cos(theta)<0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 1.5<|y|<2.4 for cos(theta)<0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 1.5<|y|<2.4 for cos(theta)>0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 1.5<|y|<2.4 for cos(theta)>0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 2.4<|y|<5 for cos(theta)<0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 2.4<|y|<5 for cos(theta)<0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 2.4<|y|<5 for cos(theta)>0 and cos(theta)<0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Covariance matrix of Drell-Yan AFB in electron channel for 2.4<|y|<5 for cos(theta)>0 and cos(theta)>0. The covariance matrix is built in 2 dimensions, 14x14(mass) for cos(theta), --, -+, +-, ++ combination where + means positive cos(theta) and - implies the negative cos(theta).

Fig. 7. The 95% CL exclusion limit on $\sigma (pp \to H)\mathcal{B}(H \to \mu\mu\gamma)$, with $m_{\mu\mu}$ < 20 GeV, for a Higgs-like particle, as a function of the mass hypothesis, $m_{H}$.

The $\gamma$ differential transverse momentum cross-section in an inclusive $\gamma+\mathrm{jets}$, $N_{\mathrm{jets}} \geq2$ selection for central rapidities $\vert y_{\gamma} \vert > 1.4$.

The Z boson differential transverse momentum cross-section in an inclusive $Z/\gamma^{*}+\mathrm{jets}$, $N_{\mathrm{jets}} \geq2$ over $Z/\gamma^{*}+\mathrm{jets}$, $N_{\mathrm{jets}} \geq1$ selection.

The $\gamma$ boson differential transverse momentum cross-section in an inclusive $\gamma+\mathrm{jets}$, $N_{\mathrm{jets}} \geq2$ over $Z+\mathrm{jets}$, $N_{\mathrm{jets}} \geq1$ selection for central rapidities $\vert y_{\gamma} \vert < 1.4$.

The Z boson differential transverse momentum over $H_{\mathrm{T}}$ cross-section in an inclusive $Z/\gamma^{*}+\mathrm{jets}$, $N_{\mathrm{jets}} \geq2$ selection.

The Z boson differential transverse momentum over $H_{\mathrm{T}}$ cross-section in an inclusive $Z/\gamma^{*}+\mathrm{jets}$, $N_{\mathrm{jets}} \geq3$ selection.

The log (base 10) of the Z boson differential transverse momentum over the leading jet transverse momentum cross-section in an inclusive $Z/\gamma^{*}+\mathrm{jets}$, $N_{\mathrm{jets}} \geq2$ selection.

The log (base 10) of the Z boson differential transverse momentum over the leading jet transverse momentum cross-section in an inclusive $Z/\gamma^{*}+\mathrm{jets}$, $N_{\mathrm{jets}} \geq3$ selection.

Differential cross-section ratio of Z over $\gamma$ as a function of the total transverse momentum cross-section and for central bosons ($\vert y_{\mathrm{V}}\vert < 1.4$) in an inclusive $ N_{\mathrm{jets}}\geq 1 $ selection.

Differential cross-section ratio of Z over $\gamma$ as a function of the total transverse momentum cross-section and for central bosons ($\vert y_{\mathrm{V}}\vert < 1.4$) in a $ H_{\mathrm{T}}$% > 300 GeV, N_{\mathrm{jets}}\geq 1 $ selection.

Differential cross-section ratio of Z over $\gamma$ as a function of the total transverse momentum cross-section and for central bosons ($\vert y_{\mathrm{V}}\vert < 1.4$) in an inclusive $ N_{\mathrm{jets}}\geq 2 $ selection.

Differential cross-section ratio of Z over $\gamma$ as a function of the total transverse momentum cross-section and for central bosons ($\vert y_{\mathrm{V}}\vert < 1.4$) in an inclusive $ N_{\mathrm{jets}}\geq 3 $ selection.

Measured differential cross section dsigma/dET in pb/GeV given q_T < 10 GeV. For the data values, the first uncertainty is statistical and the second is systematic. For the theory values, the uncertainty combines statistical, PDF, and renormalization/factorization scale components.

Measured differential cross section dsigma/dET in pb/GeV given q_T > 50 GeV. For the data values, the first uncertainty is statistical and the second is systematic. For the theory values, the uncertainty combines statistical, PDF, and renormalization/factorization scale components.

Measured differential cross section dsigma/dDR in pb/radians. For the data values, the first uncertainty is statistical and the second is systematic. For the theory values, the uncertainty combines statistical, PDF, and renormalization/factorization scale components.

Measured differential cross section dsigma/dDR in pb/radians given q_T < 10 GeV. For the data values, the first uncertainty is statistical and the second is systematic. For the theory values, the uncertainty combines statistical, PDF, and renormalization/factorization scale components.

Measured differential cross section dsigma/dDR in pb/radians given q_T > 50 GeV. For the data values, the first uncertainty is statistical and the second is systematic. For the theory values, the uncertainty combines statistical, PDF, and renormalization/factorization scale components.

The Drell-Yan pre-FSR dilepton rapidity distribution D(SIG)/DABS(YRAP) within the detector acceptance, for the mass bin 30-45 GeV, as measured in the combined dilepton channel.

The Drell-Yan pre-FSR dilepton rapidity distribution D(SIG)/DABS(YRAP) within the detector acceptance, for the mass bin 45-60 GeV, as measured in the combined dilepton channel.

The Drell-Yan pre-FSR dilepton rapidity distribution D(SIG)/DABS(YRAP) within the detector acceptance, for the mass bin 60-120 GeV, as measured in the combined dilepton channel.

The Drell-Yan pre-FSR dilepton rapidity distribution D(SIG)/DABS(YRAP) within the detector acceptance, for the mass bin 120-200 GeV, as measured in the combined dilepton channel.

The Drell-Yan pre-FSR dilepton rapidity distribution D(SIG)/DABS(YRAP) within the detector acceptance, for the mass bin 200-1500 GeV, as measured in the combined dilepton channel.

Measured ratio of the Drell-Yan normalized differential cross sections at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel for the full phase space.

Measured ratio of the Drell-Yan normalized differential cross sections as a function of the absolute dilepton rapidity within the detector acceptance, at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel. The mass bin 20-30 GeV.

Measured ratio of the Drell-Yan normalized differential cross sections as a function of the absolute dilepton rapidity within the detector acceptance, at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel. The mass bin 30-45 GeV.

Measured ratio of the Drell-Yan normalized differential cross sections as a function of the absolute dilepton rapidity within the detector acceptance, at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel. The mass bin 45-60 GeV.

Measured ratio of the Drell-Yan normalized differential cross sections as a function of the absolute dilepton rapidity within the detector acceptance, at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel. The mass bin 60-120 GeV.

Measured ratio of the Drell-Yan normalized differential cross sections as a function of the absolute dilepton rapidity within the detector acceptance, at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel. The mass bin 120-200 GeV.

Measured ratio of the Drell-Yan normalized differential cross sections as a function of the absolute dilepton rapidity within the detector acceptance, at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel. The mass bin 200-1500 GeV.

Normalised differential TOP TOPBAR production cross section as a function of the number of additional jets with PT(JET) > 30 GeV in the lepton+jets channel. The total uncertainties are shown and include the statistical and systematic uncertainties.

Measured gap fraction in the dilepton channel as a function of the additional jet transverse momentum, GAPFRAC(PT) = N(PT)/N(TOTAL) where N(PT) is the number of events that do not contain additional jets above the given PT threshold.

Measured gap fraction in the dilepton channel as a function of the scalar sum of the transverse momentum of the additional jets, HT = SUM(PT(ADD. JETS)), GAPFRAC(HT) = N(HT)/N(TOTAL) where N(HT) is the number of events in which HT (with PT > 30 GeV) is less than the given threshold.

The DY pre-FSR cross section measurements for the combined dimuon and dielectron channels normalized to the Z-peak region in the full acceptance.

The DY dimuon rapidity spectrum within the detector acceptance, normalized to the Z-peak region, for the mass bin 20-30 GeV. The two columns correspond to pre-FSR and post-FSR. The uncertainties are the total experimental uncertainties.

The DY dimuon rapidity spectrum within the detector acceptance, normalized to the Z-peak region, for the mass bin 30-45 GeV. The two columns correspond to pre-FSR and post-FSR. The uncertainties are the total experimental uncertainties.

The DY dimuon rapidity spectrum within the detector acceptance, normalized to the Z-peak region, for the mass bin 45-60 GeV. The two columns correspond to pre-FSR and post-FSR. The uncertainties are the total experimental uncertainties.

The DY dimuon rapidity spectrum within the detector acceptance, normalized to the Z-peak region, for the mass bin 60-120 GeV. The two columns correspond to pre-FSR and post-FSR. The uncertainties are the total experimental uncertainties.

The DY dimuon rapidity spectrum within the detector acceptance, normalized to the Z-peak region, for the mass bin 120-200 GeV. The two columns correspond to pre-FSR and post-FSR. The uncertainties are the total experimental uncertainties.

The DY dimuon rapidity spectrum within the detector acceptance, normalized to the Z-peak region, for the mass bin 200-1500 GeV. The two columns correspond to pre-FSR and post-FSR. The uncertainties are the total experimental uncertainties.

Normalized DPhi(Z, j2) distributions for Njets >= 3.

Normalized DPhi(Z, j3) distributions for Njets >= 3.

Normalized DPhi(j1, j2) distributions for Njets >= 3.

Normalized DPhi(j1, j3) distributions for Njets >= 3.

Normalized DPhi(j2, j3) distributions for Njets >= 3.

Normalized DPhi(Z, j1) distributions for Njets >= 1 and PT(Z) >= 150 GeV.

Normalized DPhi(Z, j1) distributions for Njets >= 2 and PT(Z) >= 150 GeV.

Normalized DPhi(Z, j1) distributions for Njets >= 3 and PT(Z) >= 150 GeV.

Normalized DPhi(Z, j2) distributions for Njets >= 3 and PT(Z) >= 150 GeV.

Normalized DPhi(Z, j3) distributions for Njets >= 3 and PT(Z) >= 150 GeV.

Normalized DPhi(j1, j2) distributions for Njets >= 3 and PT(Z) >= 150 GeV.

Normalized DPhi(j1, j3) distributions for Njets >= 3 and PT(Z) >= 150 GeV.

Normalized DPhi(j2, j3) distributions for Njets >= 3 and PT(Z) >= 150 GeV.

Normalized distributions in ln(tauT) for all PT(Z) and Njets >=1.

Normalized distributions in ln(tauT) for PT(Z) > 150 GeV and Njets >=1.