CERN Accelerating science

 
Distributions of $\mll$ in the top control region of the 0-jet channel (left), $\costhetastar$ in the $\Zgtt$ control regions of the 0-jet channel (centre), and $\mll$ in a loose region including both the $WW$ control region and the signal region in the 1-jet channel. Model uncertainties shown are obtained from the fit result using a reweighting technique.
Distributions of $\mll$ in the top control region of the 0-jet channel (left), $\costhetastar$ in the $\Zgtt$ control regions of the 0-jet channel (centre), and $\mll$ in a loose region including both the $WW$ control region and the signal region in the 1-jet channel (right). The MC backgrounds are normalized by normalization factors obtained from signal plus background fits to the observable that is being plotted. Model uncertainties shown are obtained from the fit result using a reweighting technique.
Distributions of $\mll$ in the top control region of the 0-jet channel (left), $\costhetastar$ in the $\Zgtt$ control regions of the 0-jet channel (centre), and $\mll$ in a loose region including both the $WW$ control region and the signal region in the 1-jet channel. Model uncertainties shown are obtained from the fit result using a reweighting technique.
Distributions of $\mll$ in the top control region of the 0-jet channel (left), $\costhetastar$ in the $\Zgtt$ control regions of the 0-jet channel (centre), and $\mll$ in a loose region including both the $WW$ control region and the signal region in the 1-jet channel (right). The MC backgrounds are normalized by normalization factors obtained from signal plus background fits to the observable that is being plotted. Model uncertainties shown are obtained from the fit result using a reweighting technique.
Distributions of $\mll$ in the top control region of the 0-jet channel (left), $\costhetastar$ in the $\Zgtt$ control regions of the 0-jet channel (centre), and $\mll$ in a loose region including both the $WW$ control region and the signal region in the 1-jet channel. Model uncertainties shown are obtained from the fit result using a reweighting technique.
Distributions of $\mll$ in the top control region of the 0-jet channel (left), $\costhetastar$ in the $\Zgtt$ control regions of the 0-jet channel (centre), and $\mll$ in a loose region including both the $WW$ control region and the signal region in the 1-jet channel (right). The MC backgrounds are normalized by normalization factors obtained from signal plus background fits to the observable that is being plotted. Model uncertainties shown are obtained from the fit result using a reweighting technique.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the first bin of the transverse momentum $\ptH$: 0--30~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the first bin of the transverse momentum $\ptH$: 0--30~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the first bin of the transverse momentum $\ptH$: 0--30~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the first bin of the transverse momentum $\ptH$: 0--30~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the second bin of the transverse momentum $\ptH$: 30--60~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the second bin of the transverse momentum $\ptH$: 30--60~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the second bin of the transverse momentum $\ptH$: 30--60~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the second bin of the transverse momentum $\ptH$: 30--60~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the third bin of the transverse momentum $\ptH$: 60--120~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the third bin of the transverse momentum $\ptH$: 60--120~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the third bin of the transverse momentum $\ptH$: 60--120~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the third bin of the transverse momentum $\ptH$: 60--120~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the last bin of the transverse momentum $\ptH$: 120--1000~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the last bin of the transverse momentum $\ptH$: 120--1000~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the last bin of the transverse momentum $\ptH$: 120--1000~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Pre-fit (left) and post-fit (right) distribution of the transverse mass $\mT$ of the Higgs boson in the last bin of the transverse momentum $\ptH$: 120--1000~\GeV for $\Njet=0,1$. The last bin in $\mT$ contains the overflow of events with $\mT>160$~\GeV.
Measured differential fiducial cross section for \ptH in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \ptH in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \mll (left) and \Yll (right) in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bars on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \mll (left) and \Yll (right) in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bars on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \mll (left) and \Yll (right) in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bars on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \mll (left) and \Yll (right) in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bars on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \ptll (left) and \dphill (right) in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \ptll (left) and \dphill (right) in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \ptll (left) and \dphill (right) in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \ptll (left) and \dphill (right) in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for $\pt^{\ell0}$ (left) and \costhetastar (right) in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for $\pt^{\ell 0}$ (left) and \costhetastar (right) in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for $\pt^{\ell0}$ (left) and \costhetastar (right) in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for $\pt^{\ell 0}$ (left) and \costhetastar (right) in the 0+1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for $|y_{j0}|$ in the 1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for $|y_{j0}|$ in the 1-jet fiducial region using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \mll\ (left) and \dphill (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \mll\ (left) and \dphill (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \mll\ (left) and \dphill (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \mll\ (left) and \dphill (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \Yll (left) and \ptll (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \Yll (left) and \ptll (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \Yll (left) and \ptll (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for \Yll (left) and \ptll (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for $\pt^{\ell0}$ (left) and \costhetastar (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for $\pt^{\ell 0}$ (left) and \costhetastar (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for $\pt^{\ell0}$ (left) and \costhetastar (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Measured differential fiducial cross section for $\pt^{\ell 0}$ (left) and \costhetastar (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the regularized in-likelihood unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The legend includes $p$-values quantifying the level of agreement between the data and the predictions, including all sources of uncertainty. The systematic uncertainties of the data are shown separately.
Post-fit correlations of the observed cross sections for the bins of transverse momentum \ptH.
Post-fit correlations of the observed cross sections for the bins of transverse momentum \ptH. The legend on the right shows numbers in percentages.
Differential fiducial cross section for $\ptH$ in the 0+1-jet fiducial region using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for $\ptH$ in the 0+1-jet fiducial region using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \mll (left) and \Yll (right) in the 0+1-jet fiducial region using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \mll (left) and \Yll (right) in the 0+1-jet fiducial region using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \mll (left) and \Yll (right) in the 0+1-jet fiducial region using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \mll (left) and \Yll (right) in the 0+1-jet fiducial region using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \ptll (left) and \dphill (right) in the 0+1-jet fiducial region using the iterative bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \ptll (left) and \dphill (right) in the 0+1-jet fiducial region using the iterative bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \ptll (left) and \dphill (right) in the 0+1-jet fiducial region using the iterative bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \ptll (left) and \dphill (right) in the 0+1-jet fiducial region using the iterative bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for $\pt^{\ell0}$ (left) and $\costhetastar$ (right) in the 0+1-jet fiducial region using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for $\pt^{\ell 0}$ (left) and $\costhetastar$ (right) in the 0+1-jet fiducial region using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for $\pt^{\ell0}$ (left) and $\costhetastar$ (right) in the 0+1-jet fiducial region using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for $\pt^{\ell 0}$ (left) and $\costhetastar$ (right) in the 0+1-jet fiducial region using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for $|y_{j0}|$ in the 0+1-jet fiducial region using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for $|y_{j0}|$ in the 0+1-jet fiducial region using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \mll (left) and \dphill (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \mll (left) and \dphill (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \mll (left) and \dphill (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \mll (left) and \dphill (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \Yll (left) and \ptll (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \Yll (left) and \ptll (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \Yll (left) and \ptll (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for \Yll (left) and \ptll (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for $\pt^{\ell0}$ (left) and $\costhetastar$ (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for $\pt^{\ell 0}$ (left) and $\costhetastar$ (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for $\pt^{\ell0}$ (left) and $\costhetastar$ (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.
Differential fiducial cross section for $\pt^{\ell 0}$ (left) and $\costhetastar$ (right) versus~\Njet in the 0-jet and 1-jet fiducial regions using the iterative Bayesian unfolding method. Uncertainty bars on the data points include statistical and systematic uncertainties from experimental and theory sources as well as background normalization effects and shape effects from background and signal. Uncertainty bands on the predictions shown are dominated by normalization effects on the signal arising from showering, PDF models, \alphas and the QCD scale. The systematic uncertainties of the data are shown separately.