"}    ----------- -------------------------- ------------------------- ---------------------------- -------------------------                                                                                                     $|\eta|$   $\langle |\eta| \rangle$                             $\langle  |\eta | \rangle$       0.00-0.00  0.00                       0.00$\pm$0.00$\pm$0.00    0.00                         0.00$\pm$0.00$\pm$0.00    0.00-0.00  0.00                       0.00$\pm$0.00$\pm$0.00    0.00                         0.00$\pm$0.00$\pm$0.00    0.00-0.00  0.00                       00.00$\pm$0.00$\pm$0.00   0.00                         0.00$\pm$0.00$\pm$0.00    0.00-0.00  0.00                       00.00$\pm$0.00$\pm$0.00   0.00                         0.00$\pm$0.00$\pm$0.00    0.00-0.00  0.00                       0.00$\pm$0.00$\pm$0.00    0.00                         0.00$\pm$0.00$\pm$0.00                                                                                                     $|\eta|$   $\langle |\eta| \rangle$                             $\langle  |\eta | \rangle$       0.00-0.00  0.00                       0.00$\pm$0.00$\pm$0.00    0.00                         00.00$\pm$0.00$\pm$0.00    0.00-0.00  0.00                       0.00$\pm$0.00$\pm$0.00    0.00                         00.00$\pm$0.00$\pm$0.00    0.00-0.00  0.00                       0.00$\pm$0.00$\pm$0.00    0.00                         00.00$\pm$0.00$\pm$0.00    0.00-0.00  0.00                       0.00$\pm$0.00$\pm$0.00    0.00                         00.00$\pm$0.00$\pm$0.00    0.00-0.00  0.00                       0.00$\pm$0.00$\pm$0.00    0.00                         00.00$\pm$0.00$\pm$0.00   ----------- -------------------------- ------------------------- ---------------------------- -------------------------    : Differential inclusive charged hadron production cross-sections $\dseta$ for $\pt>0