ic can be formed on a high resistance semi conductive substrate the dielectric lens antenna 3 1 3 4 may include the dielectric lens body 3 1 3 2 with relative dielectric conductivity u2208 1 and a dielectric lens fill piece the dielectric lens fill piece may be hyperboloid fill piece 3 4 with relative dielectric conductivity u2208 2 the hyperbolic fill piece 3 4 configured to enable a considerable reduction in dimensions of the controlled lens antenna apparatus in one example to transform a spherical wave to a plane wave a source of waves is placed in hyperboloid focus see fig4 in fig4 f 1 and f 2 indicate focuses of hyperboloids x and y indicate coordinate values of points forming the hyperboloids a wave from the focus f 2 of one of the hyperboloids may be deflected at an angle of u03b2 u2212 u03b1 at a point of the other hyperboloid a dashed line in fig4 may be a perpendicular line at the point of the hyperboloid a dependence of relative dielectric conductivities u2208 1 and u2208 2 of the dielectric lens antenna 3 1 3 4 may be expressed by the following relation where u03c6 is an angle between hyperboloid axes tg may be the tangent function thus in case u03c6 90 u00b0 u2208 2 2 u2208 1 if to consider dielectric losses the following relation may apply u2208 2 lt 2 u2208 1 u2208 1 lt u2208 2 lt 2 u2208 1 the dielectric lens antenna 3 1 3 4 may also have a matching dielectric lens covering 3 3 with relative dielectric conductivity u2208 3 in accordance with an alternative configuration the deflecting plate 4.