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].