The even-parity low configuration system of Ti II has been considered on the basis of the experimental data found in the literature, and its fine structure has been reanalyzed by simultaneous parameterization of one-and two-body interactions for the model space (3d + 4s) 3 . Furthermore, the main one-electron hyperfine structure parameters for these configurations have been evaluated. For instance, for 3d 2 4s 1 , a 01 3d = −63.2 (3.1) MHz and a 10 4s = −984.1 (7.1) MHz. Field shifts (FS) and specific mass shifts (SMS) of the main Ti II configurations are deduced by means of ab initio estimates combined with a small quantity of experimental isotope shift data available in the literature: FS(3d 3 ) = −63.3 MHz, FS(3d 2 4p 1 ) = −49.7 MHz, FS(3d 1 4s 2 ) = 98.2 MHz, FS(4s 2 4P 1 ) = 163.4 MHz and SMS(3d 3 ) = 1453.3 MHz, SMS(3d 1 4s 2 ) = −2179.7 MHz, . . ., referred to 3d 2 4s 1 for the pair Ti 46 -Ti 48 .