The temperature and frequency dependence of complex dynamical conductivity $$\sigma = \sigma_{1} + i\sigma_{2}$$ , penetration depth, and superfluid density of Ba(Fe1−xCox)2As2 are calculated in the framework of one- and two-gap models at terahertz frequencies for a temperature range of 2 K < T < TC (TC = 22 K). In the single-gap model, an isotropic s-wave gap without any node and a d-wave gap with possible nodes are considered. In the two-gap model, one of the gaps was considered isotropic s-wave gap with amplitude $$\varDelta_{A} = 3\;{\text{meV}}$$ , while the other gap was supposed to be an anisotropic d-wave gap with possible nodes, and its rms amplitude was $$\varDelta_{0} = 8\;{\text{meV}}$$ . The interaction between the gaps is waived, since it is small, and its description is problematic. Comparing the result with the experimental data proves that the two-gap model consistently describes the optical characteristics of Ba(Fe1−xCox)2As2. In the two-gap model, the temperature dependence of $$\sigma_{1}$$ demonstrated a coherence peak at frequencies below 15 cm−1. The temperature dependence of the penetration depth calculated from $$\sigma_{2}$$ shows power-law behavior at low temperatures, and the superfluid density varies steeply near TC.
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