  The magnetization anisotropy of a layered superconductor FeTe0.65Se0.35
sample is experimentally studied in a magnetic field directed either along the
layers of the plane, or perpendicular to them. The value of the vortex pinning
potential in a weak magnetic field, and the critical current density ratio are
determined for these directions. The results are discussed within the framework
of presenting the sample as layers of fine single crystals, divided by weak
interlayer superconducting bonds with magnetic inclusions.
