We report data on the Hall coefficient (R H ) of the carbon substituted Mg(B 1-x C x ) 2 single crystals with x in the range from 0 to 0.1. The temperature dependences of R H obtained for the substituted crystals differ systematically at low temperatures, but all of them converge to the value of 1.8 10 -10 m 3 C -1 at room temperature. The R H (T) data together with results of the thermoelectric power and electrical resistivity measurements are interpreted within a quasi-classical transport approach, where the presence of four different conducting sheets is considered. The main influence of the carbon substitution on the transport properties in the normal state is associated with enhanced scattering rates rather than modified concentration of charge carriers. Presumably the carbon substitution increases the electron-impurity scattering mainly in the band. For the Hall effect measurements, we chose single crystals of Mg(B 1-x C x ) 2 with x = 0 (unsubstituted), 0.02, 0.06, and 0.1. The thermoelectric power at room temperature was also evaluated for these samples and, additionally, for one with x = 0.05. The resistivity measurements were performed on the crystals with x = 0 and x = 0.06. The Hall coefficient (R H ) was measured by a standard procedure in the magnetic field of 13 T. Samples were rotated by 180° and the current direction was reversed many times to exclude the influence of mismatching of the Hall contacts positions and of detrimental emf's. Methods to measure the resistivity ( ) and thermoelectric power (S) were described in detail in Refs.[7] and [12], respectively.
3The crystals were grown under high pressure using a cubic anvil press. The applied pressure and temperature conditions for the growth of MgB2 single crystals were determined in our earlier study of the Mg-B-N phase diagram [13]. A mixture of Mg, B, BN and C (in the case of C-substituted crystals) was ground and cold-pressed into a pellet. Then, the pellet was put into a BN container of 8 mm internal diameter and 8 mm length. Both unsubstituted and C-substituted crystals were grown in similar way. First, pressure was applied using a pyrophylite pressure transmitting cube as a medium. Then, the temperature was increased The temperature dependence of the dc magnetization in an external magnetic fields of 0.3 -0.5 mT was recorded for both zero-field-cooled and field-cooled conditions.