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Chapter 5                                                               233

            1.  Suitable selection  of radiating elements forming  LSAS.  The traditional choice  is  the
               electrical dipole in a shape of metal patch printed on array common dielectric substrate.
               The surface of such patch is typically less than /2 x /2 =  /4 depending on substrate
                                                                 2
               dielectric constant. In mm-wave range it means something around (15 – 100) mm . If so,
                                                                                 2
               the extremely high density of conductivity current on the patch surface is expected that
               leads to excessive Ohmic loss and consequently low antenna efficiency. Add the extra loss
               in LSAS feeding network and expect the efficiency something around and below 50%.
            2.  Meanwhile, it is a well-established theoretically and practically fact that in mm-wave as
               well optical band the power dissipation greatly diminishes as soon as all metal parts are
               completely or partially excluded and replaced by elements manufactured from dielectric
               with tanδ ≤ 10 . If so, a better candidate for array radiator might be an exceptionally
                            −4
               broadband (octave and more) dielectric waveguide similar to one in Figure 6.3.4 of Chapter










                   a)                                                     b)

                                Figure 5.3.8 Dielectric waveguide as radiator

               6. Careful choice of waveguide and substrate materials leads to high concertation of EM
               energy inside  waveguide  as  Figure 5.3.8a demonstrates  reducing  by that the  expected
                                                    interactions between  adjacent  radiators of
                                                    highly populated MIMO array. The front end
                                                    of waveguide is cut as Figure 5.3.8 depicts
                                                    being  open  and  matched  to free space
                                                    creating down tilting pattern. It radiates the
                                                    same  way as limited set of  Huygens’
                                                    elements (look at Figure 4.3.9 from Chapter
                                                    4). Then the transmitting / receiving module
                                                    as well the interface to switching box could
                                                    be integrated with radiating elements of total
                                                    length in order of mm.  The whole  brick-
                  Figure 5.3.9 Average atmospheric   architecture of array might be organized as
              absorption of mm-waves at sea level, 20°C   depicted in Figure 5.6.6a of Section 5.6 (see
                                                    later in this chapter).
            3.  Configuration and deployment of the arrays including the feed circuitry. It can be, for
               example, the planar or circular phased array (conformal or more intricate 3D structure)
               similar to be discussed later in Section 5.6 of this chapter.
            4.  Due to the tight placement, the mutual coupling, i.e. crosstalk interference between the
               closely-packed antenna elements appears. As a result, the signal received or transmitted
               each radiator is a vector sum of  fractional  signals  received or transmitted by all its
               neighbors. It makes the development of array and its beamformer a quite challenging task
               requiring an all-inclusive LSAS electrodynamics simulation to estimate a-priori unknown
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