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Definition of the five decay angles, $\theta$, $\theta_b$, $\phi_b$, $\theta_{l}$ and $\phi_l$ used to describe the kinematics of the \decay{\Lb}{\jpsi\Lz} decay. The angles are described in the text.
Mass distribution of selected \decay{\Lb}{\jpsi\Lz} candidates in (top-left) the 2011, (top-right) the 2012, (bottom-left) the 2015 and (bottom-right) the 2016 data sets. The long and downstream categories have been combined. The results of fits to the distributions are overlaid.
Mass distribution of selected \decay{\Lb}{\jpsi\Lz} candidates in (top-left) the 2011, (top-right) the 2012, (bottom-left) the 2015 and (bottom-right) the 2016 data sets. The long and downstream categories have been combined. The results of fits to the distributions are overlaid.
Mass distribution of selected \decay{\Lb}{\jpsi\Lz} candidates in (top-left) the 2011, (top-right) the 2012, (bottom-left) the 2015 and (bottom-right) the 2016 data sets. The long and downstream categories have been combined. The results of fits to the distributions are overlaid.
Mass distribution of selected \decay{\Lb}{\jpsi\Lz} candidates in (top-left) the 2011, (top-right) the 2012, (bottom-left) the 2015 and (bottom-right) the 2016 data sets. The long and downstream categories have been combined. The results of fits to the distributions are overlaid.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Angular distributions of $\cos\theta_b$, $\cos\theta_l$, $\cos\theta$, $\phi_b$ and $\phi_l$ for the background-subtracted candidates. The long and downstream categories for the different data-taking years have been combined. The result of the moment analysis, folded with the angular efficiency, is overlaid. The contribution from the long and downstream categories are indicated by the green and red lines, respectively.
Posterior probability distributions of $|a_{\pm}|$, ${\rm arg}(a_{\pm})$, $|b_{-}|$, ${\rm arg}(b_{-})$ and the transverse production polarisation of the \Lb baryons, $P_{b}$, at centre-of-mass energies of 7, 8 and 13\tev assuming uniform priors. The shaded regions indicate the 68\% and 95\% credibility intervals.
Posterior probability distributions of $|a_{\pm}|$, ${\rm arg}(a_{\pm})$, $|b_{-}|$, ${\rm arg}(b_{-})$ and the transverse production polarisation of the \Lb baryons, $P_{b}$, at centre-of-mass energies of 7, 8 and 13\tev assuming uniform priors. The shaded regions indicate the 68\% and 95\% credibility intervals.
Posterior probability distributions of $|a_{\pm}|$, ${\rm arg}(a_{\pm})$, $|b_{-}|$, ${\rm arg}(b_{-})$ and the transverse production polarisation of the \Lb baryons, $P_{b}$, at centre-of-mass energies of 7, 8 and 13\tev assuming uniform priors. The shaded regions indicate the 68\% and 95\% credibility intervals.
Posterior probability distributions of $|a_{\pm}|$, ${\rm arg}(a_{\pm})$, $|b_{-}|$, ${\rm arg}(b_{-})$ and the transverse production polarisation of the \Lb baryons, $P_{b}$, at centre-of-mass energies of 7, 8 and 13\tev assuming uniform priors. The shaded regions indicate the 68\% and 95\% credibility intervals.
Posterior probability distributions of $|a_{\pm}|$, ${\rm arg}(a_{\pm})$, $|b_{-}|$, ${\rm arg}(b_{-})$ and the transverse production polarisation of the \Lb baryons, $P_{b}$, at centre-of-mass energies of 7, 8 and 13\tev assuming uniform priors. The shaded regions indicate the 68\% and 95\% credibility intervals.
Posterior probability distributions of $|a_{\pm}|$, ${\rm arg}(a_{\pm})$, $|b_{-}|$, ${\rm arg}(b_{-})$ and the transverse production polarisation of the \Lb baryons, $P_{b}$, at centre-of-mass energies of 7, 8 and 13\tev assuming uniform priors. The shaded regions indicate the 68\% and 95\% credibility intervals.
Posterior probability distributions of $|a_{\pm}|$, ${\rm arg}(a_{\pm})$, $|b_{-}|$, ${\rm arg}(b_{-})$ and the transverse production polarisation of the \Lb baryons, $P_{b}$, at centre-of-mass energies of 7, 8 and 13\tev assuming uniform priors. The shaded regions indicate the 68\% and 95\% credibility intervals.
Posterior probability distributions of $|a_{\pm}|$, ${\rm arg}(a_{\pm})$, $|b_{-}|$, ${\rm arg}(b_{-})$ and the transverse production polarisation of the \Lb baryons, $P_{b}$, at centre-of-mass energies of 7, 8 and 13\tev assuming uniform priors. The shaded regions indicate the 68\% and 95\% credibility intervals.
Posterior probability distributions of $|a_{\pm}|$, ${\rm arg}(a_{\pm})$, $|b_{-}|$, ${\rm arg}(b_{-})$ and the transverse production polarisation of the \Lb baryons, $P_{b}$, at centre-of-mass energies of 7, 8 and 13\tev assuming uniform priors. The shaded regions indicate the 68\% and 95\% credibility intervals.
Measured transverse production polarisation of the \Lb baryons, $P_{b}$, as a function of the centre-of-mass energy, $\sqrt{s}$, of the data set. The points indicate the most probable value and the shaded regions the 68\% and 95\% credibility level intervals.
Posterior probability distribution of the parity-violating asymmetry parameter, $\alpha_b$. The shaded regions indicate the 68\% and 95\% credibility intervals.
Posterior probability distribution for $\alpha_{\Lz}$, assuming a uniform prior, with all external constraints removed. The shaded regions indicate the 68\% and 95\% credibility intervals.
Statistical correlation between the moments determined at $\sqrt{s}$ of 7\tev.
Statistical correlation between the moments determined at $\sqrt{s}$ of 8\tev.
Statistical correlation between the moments determined at $\sqrt{s}$ of 13\tev.