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Chapter 5                                                               203















                Figure 5.1.6 Twisted beams: a) Hermite-Gaussian, b) Laguerre-Gaussian, c) Bessel

            The  Figure  5.1.6 demonstrates  the  phase  and  intensity  distribution of  three  types  of  beams:
            Hermite-Gaussian (HG), Laguerre-Gaussian (LG), and Bessel (B). Each set of beams consists
            of 6 modes. All images are reprinted with Dr. C. Guzman’s permission  from  [28]. The first
            column in each beam set reflects the phase variations while the second one gives the amplitude
            intensity. All beams except the zeroed modes (first, third, fourth, and fifth in the top raw) carry
            nonzero OAM.  A more detailed discussion would be the subject of the different book. The
            reader can find more information in [17, 28].

            Twisted  waves  is  widely  used  in  modern  applications  such  as  microwave  and
            optical  communications,  quantum  optics  spectroscopy,  and  microscopy.  In  particular,
            beams  with  (OAM)  have  been  used  as  optical  tweezers  [29],  in  high-resolution
            nanoscopy  and  optical  measurements  with  increased  angular  resolution.  Furthermore,
            quantum  information  carried  in  the  high-dimensional  spatial  structure  of  single  and
            entangled  photons  can  be  exploited  in  applications  such  as  multi-dimensional  quantum
            teleportation  and  sensitive  data  encryption  of  the  highest  level  to  ensure  confidentiality  and
            privacy.

            All  these  new  exciting  research  and  development  areas are  waiting  for  your  creative
            contribution.

            5.1.4  How Should Antenna Polarization Be Chosen?

            As  usual,  in  engineering  practice,  there  is  no  unique  and  best  answer  but  rather  a  range
            of solutions. A detailed discussion of this topic is far beyond the scope of this course because
            the selection of polarization is one of the most important system decision. So we will touch just
            the tip of the “polarization” iceberg in quite general terms:

            1.  All antennas in the system should be properly aligned and share the same polarization to
               get the maximum efficiency in any transmitting-receiving system. For example, the signal
               emitted by RHCP antenna basically cannot be received by LHCP antenna and vice versa.
               Practically we can lose up to 30 dB in signal strength without proper antenna alignments.
               The same applies if we mix up with Vertical (VLP) and Horizontal (HLP) polarization.
               Therefore, for optimal communication,  antenna’s  alignment  must be V/V, H/H,
               RHCP/RHCP and LHCP/LHCP.
            2.  Meanwhile, from the above discussion, it follows that a CP waves carry simultaneously
               the energy of two orthogonal LP waves that can be transmitted and received as a whole
               (i.e. classical CP ) or independently (i.e. each LP signal transports different data set at the
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