Bayesian upper exclusion limits on the ratio $g_{W'}/g_{W}$ for an SSM-like W$\prime$ boson are shown. The unity coupling ratio (blue dotted curve) corresponds to the SSM common benchmark. The 68 and 95% quantiles of the limits are represented by the green and yellow bands, respectively.

Bayesian lower exclusion limits on the NUGIM G(221) mixing angle $\cot(\theta_{E})$ are shown as a function of the W$\prime$ boson mass. The theoretically excluded region is shaded in grey. The 68 and 95% quantiles of the limits are represented by the green and yellow bands, respectively.

Bayesian upper exclusion limits at 95% CL on the product of the production cross section and branching fraction of a QBH in an associated $ au$ lepton and neutrino final state. Minimum threshold masses $m_{th}$ of up to 6.6 TeV are excluded at 95% CL. The observed limit (solid line) is obtained from the intersection with the LO QBH cross section (blue dotted curve). The 68 and 95% quantiles of the limits are represented by the green and yellow bands, respectively.

Bayesian upper limits at 95% CL on the cross section of the process $pp\rightarrow\tau\nu$ mediated via LQ exchange in the t-channel. The inner (green) band and the outer (yellow) band indicate the regions containing 68 and 95%, respectively, of the distribution of limits expected under the background-only hypothesis. The predicted LQ cross section at LO in the three coupling benchmark scenarios is depicted in different colors for $g_{U}=1$. The uncertainty bandy correspond to the sum in quadrature of PDF and scale variations. The first benchmark scenario considers only couplings to left-handed SM fermions (i.e. $\beta_{\text{R}}^{ij}=0$) and is referred to as "best fit LH". The second benchmark, referred to as "best fit LH+RH", considers $|\beta_{\text{R}}^{\text{b}\tau}|=1$ and all other $\beta_{\text{R}}^{ij}=0$. In the third "democratic" benchmark, equal couplings only to LH fermions are assumed, i.e. $\beta_{\text{L}}^{ij}=1$ and $\beta_{\text{R}}^{ij}=0$ for all $i$ and $j$.

Expected and observed lower limits of the LQ mass as a function of the coupling $g_{U}$ in the LH scenario. The blue band shows the 68% and 95% regions of $g_{U}$ preferred by the fit to the b anomalies data.

Expected and observed lower limits of the LQ mass as a function of the coupling $g_{U}$ in the LH+RH scenario. The blue band shows the 68% and 95% regions of $g_{U}$ preferred by the fit to the b anomalies data.

Expected and observed lower limits of the LQ mass as a function of the coupling $g_{U}$ in the democratic scenario. The blue band shows the 68% and 95% regions of $g_{U}$ preferred by the fit to the b anomalies data.

Bayesian upper exclusion limits at 95% CL on each of the Wilson coefficients described by the EFT model based on 2016-2018 data. The three different coupling types represent a left-handed vector coupling ($\epsilon^{cb}_{L}$), tensor-like coupling ($\epsilon^{cb}_{T}$), and scalar-tensor-like coupling ($\epsilon^{cb}_{S_{L}}$). The 68 and 95% quantiles of the limits are represented by the green and yellow bands, respectively.

Summary of exclusion limits (expected and observed) calculated at 95% CL for full Run-2 CMS data.

Background prediction and observed data yields in the signal region bins. The background yields are obtained from the background-only fit and serve as input to the simplified likelihood reinterpretation scheme. The naming of the bins is "year_binnumber", following the binning from Figure 4.

Matrix of covariance coefficients between signal region bins. The coefficients are obtained from the background-only fit and serve as input to the simplified likelihood reinterpretation scheme. The naming of the bins is "year_binnumber", following the binning used in Figure 4.

Predicted signal yields for the 2017 data-taking period, corresponding to 41.3 fb$^{-1}$, after the application of each search requirement (cumulative) for various signal hypothesis. The requirements listed are presented as total efficiencies w.r.t. the previous selection step.

THESE ARE CORRECTED DATA FROM YF 40, 34. PROPER TABLES IN YF 40, 34 MUST. BE REPLACED BY THE GOOD ONES.

THESE ARE CORRECTED DATA FROM YF 40, 34. PROPER TABLES IN YF 40, 34 MUST. BE REPLACED BY THE GOOD ONES.

No description provided.

The inclusive charged particle differential cross section.

The K0 + K0BAR inclusive differential cross section. The last line in the table is the integral over the full X range of the measurement.. There is an additional 3.4 PCT normalization error (included in the integral).

The LAMBDA + LAMBDABAR inclusive differential cross section. The last line in the table is the integral over the full X range of the measurement.. There is an additional 3.4 PCT normalization error (included in the integral).

No description provided.

The K*0 + K*BAR0 inclusive differential cross section. The last line in the table is the integral over the full X range of the measurement.. There is an additional 3.4 PCT normalization error (included in the integral).

The PHI meson inclusive differential cross section. The last line in the table is the integral over the full X range of the measurement.. There is an additional 3.4 PCT normalization error (included in the integral).

Measured differential cross section for the production of charged pions perZ0 decay into light, charm and bottom quarks separately. The errors given are t he sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

The ratios of light to heavy quark production of charged pions. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

Measured differential cross section for the production of charged kaons perZ0 decay into light, charm and bottom quarks separately. The errors given are t he sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

The ratios of light to heavy quark production of charged kaons. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

Measured differential cross section for the production of neutral K* mesonsper Z0 decay into light, charm and bottom quarks separately. The errors given a re the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

The ratios of light to heavy quark production of neutral K* mesons. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

Measured differential cross section for proton/antiproton production per Z0decay into light, charm and bottom quarks separately. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours arenot included.

The ratios of light to heavy quark production of proton/antiprotons. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to thethree flavours are not included.

Measured differential cross section for lambda/antilambda production per Z0decay into light, charm and bottom quarks separately. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours arenot included.

The ratios of light to heavy quark lambda/lambdabar production. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

Measured differential cross section for the production of neutral kaons perZ0 decay into light, charm and bottom quarks separately. The errors given are t he sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

The ratios of light to heavy quark for neutral kaon production. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

Measured differential cross section for phi meson production per Z0 decay into light, charm and bottom quarks separately. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from theunfolding procedure. Systematic errors common to the three flavours are not inc luded.

The ratios of light to heavy quark for phi meson production. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

Corrected total cross sections per hadronic Z decay, and per decay into light, CQ or BQ primary flavour separately. The errors given are the sum in quadrature of experimental and extrapolation uncertainties.

Differences of total cross sections per hadronic Z decay, between CQ (and BQ) and light quarks decays. The errors given are the sum in quadrature of experimental and extrapolation uncertainties.

The differential cross sections for the production of positive and negativepions in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The normalized difference between the differential cross sections for the production of positive and negative pions in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The differential cross sections for the production of neutral K* and K*BAR mesons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given arethe sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The normalized difference between the differential cross sections for the production of neutral K* and K*BAR mesons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The differential cross sections for the production of positive and negativeK mesons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The normalized difference between the differential cross sections for the production of positive and negative kaons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The differential cross sections for the production of proton and antiprotons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising fromthe light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The normalized difference between the differential cross sections for the production of protons and antiprotons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. CCT. = Here QUARK (QUARKBAR) means any light quark (antiquark).

The differential cross sections for the production of lambdas and antilambdas in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are thesum in quadrature of statistical errors and those systematic errors arising fro m the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The normalized difference between the differential cross sections for the production of protons and antiprotons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).