J/psi-->e+e- invariant yield in Cu+Cu collisions as a function of p_T at mid-rapidity for the 20-40 centrality range. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.

J/PSI yield versus transverse momentum PT, at mid rapidity : -0.35<y<0.35, for a centrality range of 40-60%.

J/psi-->e+e- invariant yield in Cu+Cu collisions as a function of p_T at mid-rapidity for the 40-60 centrality range. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.

J/PSI yield versus transverse momentum PT, at mid rapidity : -0.35<y<0.35, for a centrality range of 60-94%.

J/psi-->e+e- invariant yield in Cu+Cu collisions as a function of p_T at mid-rapidity for the 60-94 centrality range. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.

J/PSI yield versus transverse momentum PT, at forward rapidity : absolute value of y belongs to [1.22.2], for a centrality range of 0-20%.

J/psi-->mu+mu- invariant yield in Cu+Cu collisions as a function of p_T at forward rapidity for the 0-20, 20-40, 40-60 and 60-94 centrality ranges. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.

J/PSI yield versus transverse momentum PT, at forward rapidity : absolute value of y belongs to [1.22.2], for a centrality range of 20-40%.

J/psi-->e+e- average momentum squared in Cu+Cu collisions as a function of N_part at forward rapidity (p_T integrated). The statistical and systematic uncertainties vary point-to-point and are listed for each measured value.

J/PSI yield versus transverse momentum PT, at forward rapidity : absolute value of y belongs to [1.22.2], for a centrality range of 40-60%.

J/psi-->mu+mu- average momentum squared in Cu+Cu collisions as a function of N_part at forward rapidity (p_T integrated). The statistical and systematic uncertainties vary point-to-point and are listed for each measured value.

J/PSI yield versus transverse momentum PT, at forward rapidity : absolute value of y belongs to [1.22.2], for a centrality range of 60-94%.

J/psi-->mu+mu- and J/psi-->e+e- nuclear modification in Cu+Cu collisions as a function of p_T at forward and mid-rapidity for the 0-20 centrality range. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.

Mean PT^2 versus Npart, number of participants, at mid rapidity : -0.35<y<0.35.

J/psi-->mu+mu- and J/psi-->e+e- nuclear modification in Cu+Cu collisions as a function of y at forward and mid-rapidity for the 0-20 centrality range. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.

Mean PT^2 versus Npart, number of participants, at forward rapidity : absolute value of y belongs to [1.22.2].

J/psi-->e+e- nuclear modification in Cu+Cu collisions as a function of N_part at mid-rapidity for the 0-20 centrality range. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.

Nuclear modification factor RAA versus transverse momentum PT at mid rapidity : -0.35<y<0.35, for the 0-20% most central events.

J/psi-->mu+mu- nuclear modification in Cu+Cu collisions as a function of N_part at forward rapidity for the 0-20 centrality range. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.

Nuclear modification factor RAA versus transverse momentum PT at forward rapidity : absolute value of y belongs to [1.22.2], for the 0-20% most central events.

J/psi-->mu+mu- in Cu+Cu collisions as a function of $N_{part}$ at forward rapidity expressed as a ratio with respect to J/psi-->e+e- nuclear modification at mid-rapidity. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.

Nuclear modification factor RAA versus rapidity, for the 0-20% most central events.

Nuclear modification factor RAA versus number of participants, at mid rapidity : -0.35<y<0.35.

Nuclear modification factor RAA versus number of participants, at forward rapidity : absolute value of y belongs to [1.22.2].

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/$c$.

With respect to the virtual photon axis.

With respect to the sphericity axis.

With respect to the thrust axis.

With respect to the virtual photon axis.

With respect to the sphericity axis.

With respect to the thrust axis.

With respect to the virtual photon axis.

With respect to the sphericity axis.

With respect to the thrust axis.

Distribution with respect to the sphericity axis.

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Distribution with respect to the sphericity axis.

Distribution with respect to the sphericity axis.

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With respect to the sphericity axis.

With respect to the thrust axis used for comparison with e+ e-.

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J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus PT at mid rapidity (-0.35<y<0.35) in D+AU collisions.

J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus PT at forward rapidity (1.2<y<2.2) in D+AU collisions.

J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus centrality at backward rapidity (-2.2<y<-1.2) in D+AU collisions.

J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus centrality at mid rapidity (-0.35<y<0.35) in D+AU collisions.

J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus centrality at forward rapidity (1.2<y<2.2) in D+AU collisions.

Nuclear modification factor versus rapidity in D+AU collisions, over 3 bins of rapidity.

Nuclear modification factor versus rapidity in D+AU collisions, over 5 bins of rapidity.

Nuclear modification factor versus PT at backward rapidity (-2.2<y<-1.2) in D+AU collisions.

Nuclear modification factor versus PT at mid rapidity (-0.35<y<0.35) in D+AU collisions.

Nuclear modification factor versus PT at forward rapidity (1.2<y<2.2) in D+AU collisions.

Nuclear modification factor versus centrality at backward rapidity (-2.2<y<-1.2) in D+AU collisions.

Nuclear modification factor versus centrality at mid rapidity (-0.35<y<0.35) in D+AU collisions.

Nuclear modification factor versus centrality at forward rapidity (1.2<y<2.2) in D+AU collisions.

Mean PT^2 versus rapidity, extracted from a fit to the data, for DEUT + Au reactions. The mean value of PT^2 is calculated from the data for PT < 5 Gev/c.

Mean PT^2 versus rapidity, extracted from a fit to the data, for P + P reactions. The mean value of PT^2 is calculated from the data for PT < 5 Gev/c.

Breakup cross section of c-c_bar pairs inside cold nuclear matter,integrated over the whole domain of rapidity.The breakup cross section is calculated with two models of shadowing for nuclear PDFs ; the EKS model and the NDSG model. The uncertainties given, containing statistical and systematical error, are corresponding to one standard deviation.

Breakup cross section of c-c_bar pairs inside cold nuclear matter for different ranges of rapidity.The breakup cross section is calculated with two models of shadowing for nuclear PDFs ; the EKS model and the NDSG model. The uncertainties given, containing statistical and systematical error, are corresponding to one standard deviation.

Breakup cross section of c-c_bar pairs inside cold nuclear matter, integrated over the whole domain of rapidity.The breakup cross section is calculated with two models of shadowing for nuclear PDFs ; the EKS model and the NDSG model. The uncertainties given, containing statistical and systematical error, are corresponding to one standard deviation.

Breakup cross section of c-c_bar pairs inside cold nuclear matter for different ranges of rapidity.The breakup cross section is calculated with two models of shadowing for nuclear PDFs ; the EKS model and the NDSG model. The uncertainties given, containing statistical and systematical error, are corresponding to one standard deviation.

Mean PT^2 value at forward rapidities : absolute value of y belongs to [1.2;2.2] The mean PT is obtained with a phenomonological fit of the J/PSI distribution in PT of the form (1/(2*PI*PT))*D(SIG)/DPT = A ( 1+(PT/B)^2)^-6 .The systematic error includes the incertainty from the maximum shape deviation permitted by the point-to-point correlated errors and from allowing the exponent of the fit fonctionto be a free parameter.

J/PSI differential cross section times dilepton branching ratio versus rapidity.

Total cross-section for J/PSI production. The value of the total cross section has been determined by fitting the rapidity distribution with many theoretical and phenomenological shapes. The systematic error quotedwas estimated from the maximum variation allowed by shifting the mid and forward rapidity data independantely by their point-to-point correlated systematic errors.There is a +- 18 nanobarn normalization error in addition to the statistical and systematical errors shown.

Mean PT^2 values at forward rapidities (absolute value of y belongs to [1.2;2.2]), for different bins of centrality.

J/PSI invariant yield versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrality, at mid rapidity :,-0.35<y<0.35 An up/down correction, to translate each point at the center of it's relative bin, have been applied to the data.

J/PSI invariant yield versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrality,at forward rapidities (absolute value of y belongs to [1.2;2.2]). An up/down correction, to translate each point at the center of it's relative bin, have been applied to the data.

Nuclear modification factor Raa versus transverse momentum for 0-20%, 20-40%, 40-60%, 60-92% centrality, at mid rapidities :-0.35<y<0.35. An additional +- 10% (resp. +- 10%, +- 13%, +- 28%) global uncertainty, associated with the calculation of the number of binary collisions and the J/PSI yield in p+p, is not shown for the 0-20% (resp. 20-40%,40-60%, 60-92%) centrality bin.

Nuclear modification factor Raa versus transverse momentum for 0-20%, 20-40%, 40-60%, 60-92% centrality, at forward rapidities : absolute value of y belongs to [1.2;2.2] An additional +- 10% (resp. +- 10%, +- 13%, +- 28%) global uncertainty, associated with the calculation of the number of binary collisions and the J/PSI yield in p+p, is not shown for the 0-20% (resp. 20-40%,40-60%, 60-92%) centrality bin. An up/down correction, to translate each point at the center of it's relative bin, have been applied to the data.

Nuclear modification factor Raa versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrality, at mid rapidities :,-0.35<y<0.35. An additional +- 10% (resp. +- 10%, +- 13%, +- 28%) global uncertainty, associated with the calculation of the number of binary collisions and the J/PSI yield in p+p, is not shown for the 0-20% (resp. 20-40%,40-60%, 60-92%) centrality bin.

Nuclear modification factor Raa versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrality, at forward rapidities : absolute value of y belongs to [1.2;2.2] An additional +- 10% (resp. +- 10%, +- 13%, +- 28%) global uncertainty, associated with the calculation of the number of binary collisions and the J/PSI yield in p+p, is not shown for the 0-20% (resp. 20-40%,40-60%, 60-92%) centrality bin.

The number of participants Npart and the nuclear modification factor Raa versus centrality at mid rapidities :,-0.35<y<0.35. An additional +- 12% global uncertainty, associated with the calculation of the number of binary collisions and the J/PSI yield in p+p, is not shown.

The number of participants Npart and the nuclear modification factor Raa versus centrality at forward rapidities : absolute value of y belongs to [1.2;2.2] An additional +- 7% global uncertainty, associated with the calculation of the number of binary collisions and the J/PSI yield in p+p, is not shown.

Ratio of nuclear modification factors RAA(forward rapidity)/RAA(mid rapidity), versus centrality. For the two most central bins, mid rapidity points have been combined to form the ratio with the forward rapidity points. See previous tables. An additional globaluncertainty of +- 14% is not included.

Mean PT^2 values at negative, null and positive XF for D+AU reaction The mean PT is obtained with a phenomenological fit of the J/PSI distribution in PT of the form (1/(2*PI*PT))*D2(SIG)/DPT*DY = A ( 1+(PT/B)^2)^-6.

Mean PT^2 values at negative,null and positive XF for P+P reaction The mean PT is obtained with a phenomenological fit of the J/PSI distribution in PT of the form (1/(2*PI*PT))*D2(SIG)/DPT*DY = A ( 1+(PT/B)^2)^-6.

PT dependence of the Alpha power for Xf ~ -0.08.

PT dependance of the Alpha power for Xf ~ 0.

PT dependance of the Alpha power for Xf ~ 0.09.

Centrality dependance of the Nuclear modification factor for rapidity : y=-1.7. Centrality is represented by the number of collisions.

Centrality dependance of the Nuclear modification factor for rapidity y=0.Centrality is represented by the number of collisions.

Centrality dependance of the Nuclear modification factor for rapidity y=1.8.Centrality is represented by the number of collisions.

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THETA IS DEFINED IN NUCLEON NUCLEON C.M.S.

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