CERN Accelerating science

The \PGmp\PGmm invariant mass distributions for dimuon candidates with $\PtDimuon> 7\GeV$ and $\RapDimuon< 1.2$, in two intervals of charged particle multiplicity, 0--6 (left) and 110--140 (right). The result of the fit is shown by the solid lines, with the various dotted lines giving the different components. The lower panel displays the pull distribution.

The \PGmp\PGmm invariant mass distributions for dimuon candidates with $\PtDimuon> 7\GeV$ and $\RapDimuon< 1.2$, in two intervals of charged particle multiplicity, 0--6 (left) and 110--140 (right). The result of the fit is shown by the solid lines, with the various dotted lines giving the different components. The lower panel displays the pull distribution.

The \PGmp\PGmm invariant mass distributions for dimuon candidates with $\PtDimuon> 7\GeV$ and $\RapDimuon< 1.2$, in two intervals of charged particle multiplicity, 0--6 (left) and 110--140 (right). The result of the fit is shown by the solid lines, with the various dotted lines giving the different components. The lower panel displays the pull distribution.

The \PGmp\PGmm invariant mass distributions for dimuon candidates with $\PtDimuon> 7\GeV$ and $\RapDimuon< 1.2$, in two intervals of charged particle multiplicity, 0--6 (left) and 110--140 (right). The result of the fit is shown by the solid lines, with the various dotted lines giving the different components. The lower panel displays the pull distribution.

The ratios \RatioA and \RatioB with $\PtDimuon > 7\GeV$ (left) and $\PtDimuon > 0\GeV$ (right) as a function of \Multiplicity. The lines are fits to the data with an exponential function. The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean. The results of Ref.~\cite{Chatrchyan:2013nza} are shown in the right plot for comparison, and a small correction is applied to the present results to account for the different rapidity ranges in the measurements, $\RapDimuon < 1.20$ here and $\RapDimuon < 1.93$ in Ref.~\cite{Chatrchyan:2013nza}.

The ratios \RatioA and \RatioB with $\PtDimuon > 7\GeV$ (left) and $\PtDimuon > 0\GeV$ (right) as a function of \Multiplicity. The lines are fits to the data with an exponential function. The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean. The results of Ref.~\cite{Chatrchyan:2013nza} are shown in the right plot for comparison, and a small correction is applied to the present results to account for the different rapidity ranges in the measurements, $\RapDimuon < 1.20$ here and $\RapDimuon < 1.93$ in Ref.~\cite{Chatrchyan:2013nza}.

The ratios \RatioA and \RatioB with $\PtDimuon > 7\GeV$ (left) and $\PtDimuon > 0\GeV$ (right) as a function of \Multiplicity. The lines are fits to the data with an exponential function. The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean. The results of Ref.~\cite{Chatrchyan:2013nza} are shown in the right plot for comparison, and a small correction is applied to the present results to account for the different rapidity ranges in the measurements, $\RapDimuon < 1.20$ here and $\RapDimuon < 1.93$ in Ref.~\cite{Chatrchyan:2013nza}.

The ratios \RatioA and \RatioB with $\PtDimuon > 7\GeV$ (left) and $\PtDimuon > 0\GeV$ (right) as a function of \Multiplicity. The lines are fits to the data with an exponential function. The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean. The results of Ref.~\cite{Chatrchyan:2013nza} are shown in the right plot for comparison, and a small correction is applied to the present results to account for the different rapidity ranges in the measurements, $\RapDimuon < 1.20$ here and $\RapDimuon < 1.93$ in Ref.~\cite{Chatrchyan:2013nza}.

Mean \PtDimuon values for the three \PgUn states as a function of \Multiplicity for $\PtDimuon > 7\GeV$ (left) and $> 0\GeV$ (right). The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean.

Mean \PtDimuon values for the three \PgUn states as a function of \Multiplicity for $\PtDimuon > 7\GeV$ (left) and $> 0\GeV$ (right). The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean.

Mean \PtDimuon values for the three \PgUn states as a function of \Multiplicity for $\PtDimuon > 7\GeV$ (left) and $> 0\GeV$ (right). The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean.

Mean \PtDimuon values for the three \PgUn states as a function of \Multiplicity for $\PtDimuon > 7\GeV$ (left) and $> 0\GeV$ (right). The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean.

The ratios \RatioA (left) and \RatioB (right) as a function of \Multiplicity, for different \PtDimuon intervals. The interval 0--5 \GeV corresponds to an integrated luminosity of 0.3\fbinv, the interval 5--7\GeV to 1.9\fbinv, and the rest to the full integrated luminosity of 4.8\fbinv. The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean.

The ratios \RatioA (left) and \RatioB (right) as a function of \Multiplicity, for different \PtDimuon intervals. The interval 0--5 \GeV corresponds to an integrated luminosity of 0.3\fbinv, the interval 5--7\GeV to 1.9\fbinv, and the rest to the full integrated luminosity of 4.8\fbinv. The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean.

The ratios \RatioA (left) and \RatioB (right) as a function of \Multiplicity, for different \PtDimuon intervals. The interval 0--5 \GeV corresponds to an integrated luminosity of 0.3\fbinv, the interval 5--7\GeV to 1.9\fbinv, and the rest to the full integrated luminosity of 4.8\fbinv. The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean.

The ratios \RatioA (left) and \RatioB (right) as a function of \Multiplicity, for different \PtDimuon intervals. The interval 0--5 \GeV corresponds to an integrated luminosity of 0.3\fbinv, the interval 5--7\GeV to 1.9\fbinv, and the rest to the full integrated luminosity of 4.8\fbinv. The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean.

Left: A schematic view in the azimuthal plane of the three $\Delta \phi$ regions with respect to the \PgUn momentum direction. Right: The ratios \RatioA and \RatioB, as a function of \MultiplicityDir for the three $\Delta \phi$ regions shown in the left plot. The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMeanDir for each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMeanDir.

Left: A schematic view in the azimuthal plane of the three $\Delta \phi$ regions with respect to the \PgUn momentum direction. Right: The ratios \RatioA and \RatioB, as a function of \MultiplicityDir for the three $\Delta \phi$ regions shown in the left plot. The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMeanDir for each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMeanDir.

Left: A schematic view in the azimuthal plane of the three $\Delta \phi$ regions with respect to the \PgUn momentum direction. Right: The ratios \RatioA and \RatioB, as a function of \MultiplicityDir for the three $\Delta \phi$ regions shown in the left plot. The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMeanDir for each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMeanDir.

Left: A schematic view in the azimuthal plane of the three $\Delta \phi$ regions with respect to the \PgUn momentum direction. Right: The ratios \RatioA and \RatioB, as a function of \MultiplicityDir for the three $\Delta \phi$ regions shown in the left plot. The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMeanDir for each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMeanDir.

The ratios \RatioA and \RatioB are shown as a function of the track multiplicity \Multiplicity: in four categories based on the number of charged particles produced in a $\Delta\mathrm{R} < 0.5$ cone around the \PgU~direction (left), and in different intervals of charged particle transverse sphericity, \ST (right). The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean.

The ratios \RatioA and \RatioB are shown as a function of the track multiplicity \Multiplicity: in four categories based on the number of charged particles produced in a $\Delta\mathrm{R} < 0.5$ cone around the \PgU~direction (left), and in different intervals of charged particle transverse sphericity, \ST (right). The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean.

The ratios \RatioA and \RatioB are shown as a function of the track multiplicity \Multiplicity: in four categories based on the number of charged particles produced in a $\Delta\mathrm{R} < 0.5$ cone around the \PgU~direction (left), and in different intervals of charged particle transverse sphericity, \ST (right). The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean.

The ratios \RatioA and \RatioB are shown as a function of the track multiplicity \Multiplicity: in four categories based on the number of charged particles produced in a $\Delta\mathrm{R} < 0.5$ cone around the \PgU~direction (left), and in different intervals of charged particle transverse sphericity, \ST (right). The outer vertical bars represent the combined statistical and systematic uncertainties in the ratios, while the horizontal bars give the uncertainty in \MultiplicityMean in each bin. Inner tick marks show only the statistical uncertainty, both in the ratio and in \MultiplicityMean.