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THERE ARE NO ASSOCIATED LAB BACKWARD PROTONS.

THERE ARE ASSOCIATED PROTONS IN LAB BACKWARD HEMISPHERE.

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Mean PL and PT of PI-.

Production rate for the $\pi^{0}$ production in the rapidity range $9.2 < y < 9.4$ in $p+p$ collisions and in the rapidity range $-9.2 > y_\rm{lab} > -9.4$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $9.4 < y < 9.6$ in $p+p$ collisions and in the rapidity range $-9.4 > y_\rm{lab} > -9.6$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $9.6 < y < 9.8$ in $p+p$ collisions and in the rapidity range $-9.6 > y_\rm{lab} > -9.8$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $9.8 < y < 10.0$ in $p+p$ collisions and in the rapidity range $-9.8 > y_\rm{lab} > -10.0$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $10.0 < y < 10.2$ in $p+p$ collisions and in the rapidity range $-10.0 > y_\rm{lab} > -10.2$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $10.2 < y < 10.4$ in $p+p$ collisions and in the rapidity range $-10.2 > y_\rm{lab} > -10.4$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $10.4 < y < 10.6$ in $p+p$ collisions and in the rapidity range $-10.4 > y_\rm{lab} > -10.6$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $10.6 < y < 10.8$ in $p+p$ collisions and in the rapidity range $-10.6 > y_\rm{lab} > -10.8$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the $p_\rm{T}$ range $0.0 < p_\rm{T} < 0.2$ GeV in $p+p$ and $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the $p_\rm{T}$ range $0.2 < p_\rm{T} < 0.4$ GeV in $p+p$ and $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the $p_\rm{T}$ range $0.4 < p_\rm{T} < 0.6$ GeV in $p+p$ and $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the $p_\rm{T}$ range $0.6 < p_\rm{T} < 0.8$ GeV in $p+p$ and $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the $p_\rm{T}$ range $0.8 < p_\rm{T} < 1.0$ GeV in $p+p$ and $p+\rm{Pb}$ collisions.

Nuclear modification factor for the $\pi^{0}$s in the rapidity ranges $-8.8>y_\rm{lab}>-9.0$, $-9.0>y_\rm{lab}>-9.2$, and $-9.2>y_\rm{lab}>-9.4$ in $p+\rm{Pb}$ collisions at $\sqrt{s_\rm{NN}}=5.02$ TeV. The uncertainties include both statistical and systematic uncertainties.

Nuclear modification factor for the $\pi^{0}$s in the rapidity ranges $-9.4>y_\rm{lab}>-9.6$, $-9.6>y_\rm{lab}>-9.8$, and $-9.8>y_\rm{lab}>-10.0$ in $p+\rm{Pb}$ collisions at $\sqrt{s_\rm{NN}}=5.02$ TeV. The uncertainties include both statistical and systematic uncertainties.

Nuclear modification factor for the $\pi^{0}$s in the rapidity ranges $-10.0>y_\rm{lab}>-10.2$, $-10.2>y_\rm{lab}>-10.4$, and $-10.4>y_\rm{lab}>-10.6$ in $p+\rm{Pb}$ collisions at $\sqrt{s_\rm{NN}}=5.02$ TeV. The uncertainties include both statistical and systematic uncertainties.

Nuclear modification factor for the $\pi^{0}$s in the rapidity ranges $-10.6>y_\rm{lab}>-10.8$ in $p+\rm{Pb}$ collisions at $\sqrt{s_\rm{NN}}=5.02$ TeV. The uncertainties include both statistical and systematic uncertainties.

Fully corrected average charged particle scalar Sum(pT) per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 2.76 TeV in the TransMAX region.

Fully corrected average charged particle multiplicity per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 2.76 TeV in the TransMIN region.

Fully corrected average charged particle scalar Sum(pT) per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 2.76 TeV in the TransMIN region.

Fully corrected average charged particle multiplicity per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 2.76 TeV in the TransDIF region.

Fully corrected average charged particle scalar Sum(pT) per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 2.76 TeV in the TransDIF region.

Inclusive J/$\psi$ $R_{\rm AA}$ and Pb-Pb yields as a function of centrality, $p_{\rm T}<2$ GeV/$c$ and $2.5<y<4.0$. Statistical and systematic uncertainties are also reported. A global systematic uncertainty of 15% (12%) affects all the $R_{\rm AA}$ (yields) values.

Inclusive J/$\psi$ $R_{\rm AA}$ and Pb-Pb yields as a function of centrality, $2<p_{\rm T}<5$ GeV/$c$ and $2.5<y<4.0$. Statistical and systematic uncertainties are also reported. A global systematic uncertainty of 14% (11%) affects all the $R_{\rm AA}$ (yields) values.

Inclusive J/$\psi$ $R_{\rm AA}$ and Pb-Pb yields as a function of centrality, $5<p_{\rm T}<8$ GeV/$c$ and $2.5<y<4.0$. Statistical and systematic uncertainties are also reported. A global systematic uncertainty of 18% (10%) affects all the $R_{\rm AA}$ (yields) values.

Inclusive J/$\psi$ $R_{\rm AA}$ and Pb-Pb yields as a function of $p_{\rm T}$ for the 0-20% centrality class and $2.5<y<4.0$. Statistical and systematic uncertainties are also reported. A global systematic uncertainty of 8% (4%) affects all the $R_{\rm AA}$ (yields) values.

Inclusive J/$\psi$ $R_{\rm AA}$ and Pb-Pb yields as a function of $p_{\rm T}$ for the 20-40% centrality class and $2.5<y<4.0$. Statistical and systematic uncertainties are also reported. A global systematic uncertainty of 8% (4%) affects all the $R_{\rm AA}$ (yields) values.

Inclusive J/$\psi$ $R_{\rm AA}$ and Pb-Pb yields as a function of $p_{\rm T}$ for the 0-40% centrality class and $2.5<y<4.0$. Statistical and systematic uncertainties are also reported. A global systematic uncertainty of 8% (4%) affects all the $R_{\rm AA}$ (yields) values.

Inclusive J/$\psi$ $R_{\rm AA}$ and Pb-Pb yields as a function of $p_{\rm T}$ for the 40-90% centrality class and $2.5<y<4.0$. Statistical and systematic uncertainties are also reported. A global systematic uncertainty of 9% (4%) affects all the $R_{\rm AA}$ (yields) values.

Inclusive J/$\psi$ $R_{\rm AA}$ and Pb-Pb yields as a function of $p_{\rm T}$ for the 0-90% centrality class and $2.5<y<4.0$. Statistical and systematic uncertainties are also reported. A global systematic uncertainty of 8% (4%) affects all the $R_{\rm AA}$ (yields) values.

Inclusive J/$\psi$ $R_{\rm AA}$ and Pb-Pb yields as a function of $y$ for the 0-90% centrality class and $p_{\rm T}<8$ GeV/$c$. Statistical and systematic uncertainties are also reported. A global systematic uncertainty of 8% (4%) affects all the $R_{\rm AA}$ (yields) values.

Inclusive J/$\psi$ $R_{\rm AA}$ as a function of centrality, $0.3 <p_{\rm T}<8$ GeV/$c$ and $0.3<p_{\rm T}<2$ GeV/$c$ in the rapidity range $2.5<y<4.0$. Statistical and systematic uncertainties are also reported. A global systematic uncertainty of 15% affects all the $R_{\rm AA}$ values.

Inclusive J/$\psi$ $R_{\rm AA}$ for $2.5<y<4.0$ in the centrality classes 0-90%, 0-20%, 20-40 and 40-90% for the lowest $p_{\rm T}$ range when the $0.3$ GeV/$c$ $p_{\rm T}$ cut is applied. Statistical and systematic uncertainties are also reported. A global systematic uncertainty of 8%, 8%, 8% and 9% affect the $R_{\rm AA}$ values, respectively.

Inclusive $[\psi\text{(2S)/J/}\psi]_{\rm Pb-Pb}$ and $[\psi\text{(2S)/J/}\psi]_{\rm Pb-Pb}\;/\;[\psi\text{(2S)/J/}\psi]_{\rm pp}$ ratios as a function of centrality for $p_{\rm T}<3$ GeV/$c$. Statistical and systematic uncertainties are reported when the value is not given as an upper limit.

Inclusive $[\psi\text{(2S)/J/}\psi]_{\rm Pb-Pb}$ and $[\psi\text{(2S)/J/}\psi]_{\rm Pb-Pb}\;/\;[\psi\text{(2S)/J/}\psi]_{\rm pp}$ ratios as a function of centrality for $3<p_{\rm T}<8$ GeV/$c$.

The nuclear modification factor $R_{\rm AA}$ of inclusive J/$\psi$ measured at mid-rapidity in Pb-Pb collisions (0-40 % most central) as a function of the transverse momentum $p_{\rm T}$.

The nuclear modification factor $R_{\rm AA}$ of inclusive J/$\psi$ measured at mid-rapidity in Pb-Pb collisions (0-50 % most central) as a function of the transverse momentum $p_{\rm T}$.

The fraction of J/$\psi$ from beauty hadron decays $f_{\rm B}$ at mid-rapidity in the $p_{\rm T}$ interval 1.5 - 10 GeV/$c$ as a function of the number of participants.

The fraction of J/$\psi$ from beauty hadron decays $f_{\rm B}$ at mid-rapidity as a function of transverse momentum $p_{\rm T}$.

The nuclear modification factor $R_{\rm AA}$ of non-prompt J/$\psi$ at mid-rapidity as a function of transverse momentum $p_{\rm T}$.

The nuclear modification factor $R_{\rm AA}$ of prompt J/$\psi$ at mid-rapidity as a function of transverse momentum $p_{\rm T}$.

dN/dy and MEAN(PT) extracted from Levy-Tsallis fits to the measured PI, K, P spectra at mid-rapidity in inelastic pp collisions at SQRT(S) = 7 TeV. Combined statistical and systematic uncertainties (statistical uncertainties are negligible) are reported. The systematic uncertainty on dN/dy due to normalization to inelastic collisions (+7-4%) is not included. Integrated yields of Kaon/Pion and Proton/Pion ratios are also reported with combined statistical and systematic uncertainties (statistical uncertainties are negligible).

dN/dy and MEAN(PT) extracted from Levy-Tsallis fits to the measured PI, K, P spectra at mid-rapidity in inelastic pp collisions at SQRT(S) = 2.76 TeV. Combined statistical and systematic uncertainties (statistical uncertainties are negligible) are reported. The systematic uncertainty on dN/dy due to normalization to inelastic collisions (+6-4%) is not included. Integrated yields of Kaon/Pion and Proton/Pion ratios are also reported with combined statistical and systematic uncertainties (statistical uncertainties are negligible).

The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the away side (|$\Delta\phi$ - $\pi$| < $\pi$/3). Shown is the high FTPC-Au activity data. Trigger and associated particles have 1 < $p_T$ < 3 GeV/c and |$\eta$| < 1.

The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the away side (|$\Delta\phi$ - $\pi$| < $\pi$/3). Shown is the high-activity data after subtracting the unscaled low-activity data. Trigger and associated particles have 1 < $p_T$ < 3 GeV/c and |$\eta$| < 1.

The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the away side (|$\Delta\phi$ - $\pi$| < $\pi$/3). Shown is the high-activity data after subtracting the unscaled low-activity data. Trigger and associated particles have 1 < $p_T$ < 3 GeV/c and |$\eta$| < 1.

The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the near (|$\Delta\phi$| < $\pi$/3) side. Shown is the high-activity data after subtracting the unscaled low-activity data. Trigger and associated particles have 1 < $p_T$ < 3 GeV/c and |$\eta$| < 1.

The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the near (|$\Delta\phi$| < $\pi$/3, solid circles) and away side (|$\Delta\phi$ - $\pi$| < $\pi$/3, open circles). Shown are the (a) low and (b) high FTPC-Au activity data, and the high-activity data after subtracting the (c) unscaled. Trigger and associated particles have 1 < $p_T$ < 3 GeV/c and |$\eta$| < 1.

(a) The near-side jetlike correlated yield obtained from Gaussian fit as in Fig. 1 as function of the uncorrected dN/d$\eta$ at midrapidity measured in the TPC. Two event selections are used: FTPC-Au multiplicity and ZDC-Au energy. The curve is the result from a HIJING calculation.

(a) The near-side jetlike correlated yield obtained from Gaussian fit as in Fig. 1 as function of the uncorrected dN/d$\eta$ at midrapidity measured in the TPC. Two event selections are used: FTPC-Au multiplicity and ZDC-Au energy. The curve is the result from a HIJING calculation.

$p_T^{(a)}$ dependence. The ratio of the correlated yields in high over low FTPC-Au multiplicity events as a function of $p_T^{(a)}$ $p_T^{(t)}$ where $p_T^{(a)}$ $p_T^{(t)}$ is fixed.

$p_T^{(a)}$ dependence. The ratio of the correlated yields in high over low FTPC-Au multiplicity events as a function of $p_T^{(a)}$ $p_T^{(t)}$ where $p_T^{(a)}$ $p_T^{(t)}$ is fixed.

(a) The dihadron correlated yield normalized per radian per unit of pseudorapidity as a function of $\Delta\phi$ in d+Au collisions at high (0-20%) FTPC-Au multiplicities. Trigger and associated particles are 1 < $p_T$ < 3 GeV/c within 0.5 < |$\Delta\eta$| < 0.7. ZYAM positions are indicated with arrows.

(a) The dihadron correlated yield normalized per radian per unit of pseudorapidity as a function of $\Delta\phi$ in d+Au collisions at low (40-100%) FTPC-Au multiplicities. Trigger and associated particles are 1 < $p_T$ < 3 GeV/c within 0.5 < |$\Delta\eta$| < 0.7. ZYAM positions are indicated with arrows.multiplicity versus $\Delta\phi$.

The raw associated yield at high FTPC-Au multiplicity minus the unscaled ZYAM-subtracted correlated yields at low FTPC-Au multiplicity versus $\Delta\phi$.

The raw associated yield at high FTPC-Au multiplicity minus the scaled ZYAM-subtracted correlated yields at low FTPC-Au multiplicity versus $\Delta\phi$.