Distributions of $ p_{\rm T} $ and $y$ for background-subtracted (top) $ B ^+ $ , (middle) $ B ^0$ and (bottom) $ B ^0_ s $ decays for data collected in proton-proton collisions at the centre-of-mass energies of (left) 7 and (right) 8 $\mathrm{ Te V}$ . The binning schemes are superimposed.

Distributions of (left) invariant mass and (right) decay time for (top) $ B ^0 \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^{*0} $, (middle) $ B ^0_ s \rightarrow D ^-_ s \pi ^+ $ and (bottom) of invariant mass for $ B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^+ $ decays, with the results of the fit overlaid. The data were collected in proton-proton collisions at the centre-of-mass energy of 7 $\mathrm{ Te V}$ . The contributions of the various background sources are also shown. Below each plot are the normalized residual distributions.

Distributions of (left) invariant mass and (right) decay time for (top) $ B ^0 \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^{*0} $, (middle) $ B ^0_ s \rightarrow D ^-_ s \pi ^+ $ and (bottom) of invariant mass for $ B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^+ $ decays, with the results of the fit overlaid. The data were collected in proton-proton collisions at the centre-of-mass energy of 8 $\mathrm{ Te V}$ . The contributions of the various background sources are also shown. Below each plot are the normalized residual distributions.

Time-dependent raw asymmetries for candidates in the (top) $ B ^0 \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^{*0} $ and (bottom) $ B ^0_ s \rightarrow D ^-_ s \pi ^+ $ signal mass regions with the results of the global fits overlaid. Left and right plots correspond to data recorded in proton-proton collisions at centre-of-mass energies of 7 and 8 $\mathrm{ Te V}$ , respectively. For the $ B ^0_ s $ decay, the asymmetries are obtained by folding the decay-time distributions into one oscillation period, and the offset $t_{0}= 0.2$ ps corresponds to the selection requirement on the decay time.

Dependence of $A_\mathrm{P}(B^+)$, for data collected in proton-proton collisions with centre-of-mass of energies of (top) 7 and (bottom) 8 $\mathrm{ Te V}$ , on (left) $p_{\rm T}$ and (right) $y$. The results of fits using a straight line with zero (solid line) or floating slope parameter (dashed line) are also shown. The fits take into account the correlations amongst the bins.

Dependence of $A_\mathrm{P}(B^0)$, for data collected in proton-proton collisions with centre-of-mass of energies of (top) 7 and (bottom) 8 $\mathrm{ Te V}$ , on (left) $p_{\rm T}$ and (right) $y$. The results of fits using a straight line with zero (solid line) or floating slope parameter (dashed line) are also shown. The fits take into account the correlations amongst the bins.

Dependence of $A_\mathrm{P}( B ^0_ s )$, for data collected in proton-proton collisions with centre-of-mass of energies of (top) 7 and (bottom) 8 $\mathrm{ Te V}$ , on (left) $p_{\rm T}$ and (right) $y$. The results of fits with a straight line with zero (solid line) or floating slope parameter (dashed line) are also shown. The fits take into account the correlations amongst the bins.

Dependence of $A_\mathrm{P}(\Lambda ^0_ b )$, for data collected in proton-proton collisions with centre-of-mass of energies of (top) 7 and (bottom) 8 $\mathrm{ Te V}$ , on (left) $p_{\rm T}$ and (right) $y$. The results of fits with a straight line with zero (solid line) or floating slope parameter (dashed line) are also shown. The fits take into account the correlations amongst the bins.

Animated gif made out of all figures.

Values of the various physical inputs used in the fits, as reported in Ref. [33].

Values of signal yields, $A_{\rm P}$ and $A_{\rm D}$ obtained from global fits for the two neutral $ B $ -meson decays under study.

Values of signal yields and raw asymmetries obtained from global fits in the case of the $ B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^+ $ decay.

Absolute values of systematic uncertainties for integrated production asymmetries. The total systematic uncertainties are obtained by summing the individual contributions in quadrature.

Values for $m$ and $q$ and their correlation coefficient ($\rho$) obtained from fits to the values reported in Tables 10--17 with a first order polynomial function (FOPF), $A_{\mathrm{P}}(b \mathrm{hadron}) = a x + b$ with $x = p_{\rm T} ,y$. The label SL indicates the fit to the values with a straight line.

Values of $A_{\rm P}( B ^0_ s )$ and $A_{\rm P}(\Lambda ^0_ b )$ in each kinematic bin for data collected in proton-proton collisions at centre-of-mass energy of 7 $\mathrm{ Te V}$ . The first uncertainties are statistical and the second systematic.

Values of $A_{\rm P}( B ^0_ s )$ and $A_{\rm P}(\Lambda ^0_ b )$ in each kinematic bin for data collected in proton-proton collisions at centre-of-mass energy of 8 $\mathrm{ Te V}$ . The first uncertainties are statistical and the second systematic.

Values of the production asymmetries in bins of $ p_{\rm T} $, integrated over $y$, for $ B ^+ $ and $ B ^0$ mesons for data collected in proton-proton collisions at the centre-of-mass energy of 7 $\mathrm{ Te V}$ . The first uncertainties are statistical and the second systematic. The uncertainties among the bins are correlated due to the external inputs: $A_{ C P }( B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^+ )$ and $A_{\rm D}(\overline{ K }{} {}^0 )$ for $A_{\rm P}( B ^+ )$, and $|q/p|$ for $A_{\rm P}( B ^0 )$.

Values of the production asymmetries in bins of $y$, integrated over $ p_{\rm T} $, for $ B ^+ $ and $ B ^0$ mesons for data collected in proton-proton collisions at the centre-of-mass energy of 7 $\mathrm{ Te V}$ . The first uncertainties are statistical and the second systematic. The uncertainties among the bins are correlated due to the external inputs: $A_{ C P }( B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^+ )$ and $A_{\rm D}(\overline{ K }{} {}^0 )$ for $A_{\rm P}( B ^+ )$, and $|q/p|$ for $A_{\rm P}( B ^0 )$.

Values of the production asymmetries in bins of $ p_{\rm T} $, integrated over $y$, for $ B ^+ $ and $ B ^0$ mesons for data collected in proton-proton collisions at the centre-of-mass energy of 8 $\mathrm{ Te V}$ . The first uncertainties are statistical and the second systematic. The uncertainties among the bins are correlated due to the external inputs: $A_{ C P }( B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^+ )$ and $A_{\rm D}(\overline{ K }{} {}^0 )$ for $A_{\rm P}( B ^+ )$, and $|q/p|$ for $A_{\rm P}( B ^0 )$.

Values of the production asymmetries in bins of $y$, integrated over $ p_{\rm T} $, for $ B ^+ $ and $ B ^0$ mesons for data collected in proton-proton collisions at the centre-of-mass energy of 8 $\mathrm{ Te V}$ . The first uncertainties are statistical and the second systematic. The uncertainties among the bins are correlated due to the external inputs: $A_{ C P }( B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^+ )$ and $A_{\rm D}(\overline{ K }{} {}^0 )$ for $A_{\rm P}( B ^+ )$, and $|q/p|$ for $A_{\rm P}( B ^0 )$.

Values of the production asymmetries in bins of $ p_{\rm T} $, integrated over $y$, for the $ B ^0_ s $ meson and the $\Lambda ^0_ b $ baryon for data collected in proton-proton collisions at the centre-of-mass energy of 7 $\mathrm{ Te V}$ . The first uncertainties are statistical and the second systematic. The uncertainties among the bins are correlated due to the external inputs: $A_{ C P }( B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^+ )$, $A_{\rm D}(\overline{ K }{} {}^0 )$, $|q/p|_{ B ^0 }$ and $|q/p|_{ B ^0_ s }$ for $A_{\rm P}(\Lambda ^0_ b )$, and $|q/p|_{ B ^0_ s }$ for $A_{\rm P}( B ^0_ s )$.

Values of the production asymmetries in bins of $y$, integrated over $ p_{\rm T} $, for the $ B ^0_ s $ meson and the $\Lambda ^0_ b $ baryon for data collected in proton-proton collisions at the centre-of-mass energy of 7 $\mathrm{ Te V}$ . The first uncertainties are statistical and the second systematic. The uncertainties among the bins are correlated due to the external inputs: $A_{ C P }( B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^+ )$, $A_{\rm D}(\overline{ K }{} {}^0 )$, $|q/p|_{ B ^0 }$ and $|q/p|_{ B ^0_ s }$ for $A_{\rm P}(\Lambda ^0_ b )$, and $|q/p|_{ B ^0_ s }$ for $A_{\rm P}( B ^0_ s )$.

Values of the production asymmetries in bins of $ p_{\rm T} $, integrated over $y$, for the $ B ^0_ s $ meson and the $\Lambda ^0_ b $ baryon for data collected in proton-proton collisions at the centre-of-mass energy of 8 $\mathrm{ Te V}$ . The first uncertainties are statistical and the second systematic. The uncertainties among the bins are correlated, due to the external inputs: $A_{ C P }( B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^+ )$, $A_{\rm D}(\overline{ K }{} {}^0 )$, $|q/p|_{ B ^0 }$ and $|q/p|_{ B ^0_ s }$, for $A_{\rm P}(\Lambda ^0_ b )$ and $|q/p|_{ B ^0_ s }$ for $A_{\rm P}( B ^0_ s )$.

Values of the production asymmetries in bins of $y$, integrated over $ p_{\rm T} $, for the $ B ^0_ s $ meson and the $\Lambda ^0_ b $ baryon for data collected in proton-proton collisions at the centre-of-mass energy of 8 $\mathrm{ Te V}$ . The first uncertainties are statistical and the second systematic. The uncertainties among the bins are correlated, due to the external inputs: $A_{ C P }( B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} K ^+ )$, $A_{\rm D}(\overline{ K }{} {}^0 )$, $|q/p|_{ B ^0 }$ and $|q/p|_{ B ^0_ s }$, for $A_{\rm P}(\Lambda ^0_ b )$ and $|q/p|_{ B ^0_ s }$ for $A_{\rm P}( B ^0_ s )$.