Invariant mass distributions for selected dimuon candidates in the kinematic range $6<p_{\mathrm{T}}^{\mu ^+\mu ^- }<40 {\mathrm{ Ge V /}c} $ and $2.0<y^{\mu ^+\mu ^- }<4.5$ for (left) data collected at $\sqrt{s} =7 \mathrm{TeV}$ and (right) $8 \mathrm{TeV}$. The three peaks on each plot correspond to the \Y1S, \Y2S and \Y3S signals (low-mass to high-mass). The result of the fit, described in the text, is illustrated with a red solid line, while the background component is shown with a blue dashed line.

Distributions of the corrected mass $m_{\Upsilon\mathrm{(nS)} \gamma }$ for the selected $\chi _{ b }$ candidates (black points) decaying into (top row) \Y1S, (middle row) \Y2S and (bottom row) \Y3S, in the transverse momentum ranges given in the text, for (left) $\sqrt{s} =7 \mathrm{TeV}$ and (right) $8 \mathrm{TeV}$ data. Each plot shows also the result of the fit (solid red curve), including the background (dotted blue curve) and the signal (dashed green and magenta curves) contributions. The green dashed curve corresponds to the $\chi _{ b 1}$ signal and the magenta dashed curve to the $\chi _{ b 2}$ signal.

Fractions $\mathcal{R}^{\chi _{ b }\mathrm{(mP)} }_{\Upsilon\mathrm{(nS)} }$ as functions of $p_{\mathrm{T}}^{\Upsilon }$. Points with blue open (red solid) symbols correspond to data collected at $\sqrt{s} =7(8) \mathrm{TeV}$, respectively. For better visualization the data points are slightly displaced from the bin centres. The inner error bars represent statistical uncertainties, while the outer error bars indicate statistical and systematic uncertainties added in quadrature.

Animated gif made out of all figures.

Yields of $\Upsilon\mathrm{(nS)}$ mesons, determined by fitting the dimuon invariant mass in the range $6<p_{\mathrm{T}}^{\mu ^+\mu ^- }<40 {\mathrm{ Ge V /}c} $ and $2.0<y^{\mu ^+\mu ^- }<4.5$, for data collected at $\sqrt{s} =7$ and $8 \mathrm{TeV}$. Only statistical uncertainties are shown.

Signal yields resulting from fits to the corrected mass $m_{\Upsilon\mathrm{(nS)} \gamma }$ distributions in the transverse momentum ranges $14<p_{\mathrm{T}}^{\Y1S}<40 {\mathrm{ Ge V /}c} $, $18<p_{\mathrm{T}}^{\Y2S}<40 {\mathrm{ Ge V /}c} $ and $24<p_{\mathrm{T}}^{\Y3S}<40 {\mathrm{ Ge V /}c} $. Only statistical uncertainties are shown.

Summary of the relative systematic uncertainties for the fractions $\mathcal{R}^{\chi _{ b }\mathrm{(mP)} }_{\Upsilon\mathrm{(nS)} }$.

Summary of systematic uncertainties for $m_{\chi _{ b 1}\mathrm{(3P)} }$.

Fractions $\mathcal{R}^{\chi _{ b }\mathrm{(mP)} }_{\Upsilon\mathrm{(nS)} }$ in bins of $p_{\mathrm{T}}^{\Upsilon }$, measured for data collected at $\sqrt{s} =7 \mathrm{TeV}$. The first block corresponds to $\mathcal{R}^{\chi _{ b }\mathrm{(mP)} }_{\Y1S}$, the second to $\mathcal{R}^{\chi _{ b }\mathrm{(mP)} }_{\Y2S}$ and the third to $\mathcal{R}^{\chi _{ b }\mathrm{(mP)} }_{\Y3S}$. The first uncertainty is statistical and the second systematic.

Fractions $\mathcal{R}^{\chi _{ b }\mathrm{(mP)} }_{\Upsilon\mathrm{(nS)} }$ in bins of $p_{\mathrm{T}}^{\Upsilon }$, measured for data collected at $\sqrt{s} =8 \mathrm{TeV}$. The first block corresponds to $\mathcal{R}^{\chi _{ b }\mathrm{(mP)} }_{\Y1S}$, the second to $\mathcal{R}^{\chi _{ b }\mathrm{(mP)} }_{\Y2S}$ and the third to $\mathcal{R}^{\chi _{ b }\mathrm{(mP)} }_{\Y3S}$. The first uncertainty is statistical and the second systematic.