Microcrystalline silicon carbide (lc-SiC:H) deposited by hot wire chemical vapor deposition (HWCVD) and plasma-enhanced chemical vapor deposition (PECVD) provide advantageous optoelectronic properties, making it attractive as a window layer material in silicon thin-film and silicon heterojunction solar cells. However, it is still not clear which electrical transport mechanisms yield dark conductivities up to 10 À3 S/cm without the active use of any doping gas and how the transport mechanisms are related to the morphology of lc-SiC:H. To investigate these open questions systematically, we investigated HWCVD and PECVD grown layers that provide a very extensive range of dark conductivity values from 10 À12 S/cm to 10 À3 S/cm. We found out by secondary ion mass spectrometry measurements that no direct correlation exists between oxygen or nitrogen concentrations and high dark conductivity r d , high charge carrier density n, and low activation energy Ea. Higher r d seems to rise from lower hydrogen concentrations or/and larger coherent domain sizes L SiC . On the one hand, the decrease of r d with increasing hydrogen concentration might be due to the inactivation of donors by hydrogen passivation that gives rise to decreased n. On the other hand, qualitatively consistent with the Seto model, the lower r d and lower n might be caused by smaller L SiC , since the fraction of depleted grain boundaries with higher Ea increases accordingly. Published by AIP Publishing. [http://dx