Active particles are capable of self-propelling by consuming energy from the environment. [1] The particles may be living, such as bacteria, or synthetic, such as bimetallic rods or spherical Janus particles. Due to persistent energy input, active materials are examples of out-of-equilibrium systems. They exhibit variety of intriguing phenomena such as the onset of collective behavior, [2,3] reduction of effective viscosity, [4-6] extraction of useful energy, [7-9] and enhanced mixing. [10-12] Typically, active microswimmers show a preferred orientation which determines the self-propulsion direction. Distribution of active particle orientation may have a significant impact on the macroscopic properties of the active material. It was shown in refs. [13-15] that reduction of effective viscosity in the suspension of active microswimmers, exemplified by bacteria, may be explained by a specific form of orientational distribution with respect to the background shear flow. In refs. [16,17] authors showed how the orientation of active microswimmers in the background shear flow leads to the formation of depletion regions, where particles' number density is significantly lower than the average value. Chemically-driven synthetic microswimmers, mimicking motility of living microorganisms , were first introduced by Paxton et al. [18] Since then the repertoire of synthetic microswimmers, as well as mechanisms which can be used to activate their self-propulsion, have significantly expanded. [1] The importance of synthetic microswimmers is twofold. On the one hand, their development leads to a variety of potential applications, for example in medicine [19,20] and materials science. [21] On the other hand, their study sheds new light on fundamental motility mechanisms and biological self-organization.