Page 35 - ITU Journal Future and evolving technologies Volume 2 (2021), Issue 4 – AI and machine learning solutions in 5G and future networks
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ITU Journal on Future and Evolving Technologies, Volume 2 (2021), Issue 4




                                                ∗
          where we have used ⟨      (A),       (B)⟩ =     (A B) and the  the path is suf iciently signi icant to be included in the
          cyclic shift property of the trace.                  model, or whether to stop the OMP iterations. The value
                                                               of    is optimized using the dataset information as de‐
          The above maximization problem can be solved by      scribed later in Section 6.3.
          searching over a discretized set of values of the path pa‐
          rameters, (   ,    ,    ). We start by considering a small set  5.3 Re inement
                    ℓ
                       ℓ
                         ℓ
          of values for the path parameters equally spaced in their
          domains. We choose a resolution of 4   values for    ℓ  Once a path has been detected, we proceed to re ine the
          and of    /2 (   /2) values for    (   ). Since we are con‐  path components by iterative projections. We do this by
                 r     t             ℓ  ℓ
          sidering a smaller resolution for the angles than that re‐  freezing two of the variables and increasing the resolution
          quired for them to cover the entire angular spectrum, we  of the third, in an alternating fashion.
          substitute each    (   ) by a sector beam‐pattern ̂    (   )
                        R  ℓ                         R  ℓ
          of width 4  /   . The same manipulation applies to the  First steps:
                      r                                                     First, we adapt our estimation to handle a
          phase angles at the transmitter, and thus we can de ine  higher resolution due to the manipulation we did with the
                       ̄
          ̂     (   ,    ) = ̂    (   ) ⊗ ̂    (   ). The sector beam‐pattern
           R−T  ℓ  ℓ   T  ℓ    R  ℓ                            angular resolution.
          we consider is the same as the one de ined in [31]. With
          this de inition, we can extract a coarse version of the path  We start by increasing the time resolution by comput‐
                                                                                             ∗
                                                                                                  ̄
          parameters (   ,    ,    ) by maximizing             ing the maximum of | ̂    ∗ R−T (   ,    )         (   ))| for  ixed
                                                                                        ℓ
                                                                                                     ℓ
                                                                                          ℓ
                                                                                                   F
                      ℓ
                        ℓ
                                                                                                w
                           ℓ
                                                               (   ,    ) and    with a resolution of 32   equally spaced
                                                                    ℓ
                                                                           ℓ
                                                                 ℓ
                                       ∗
                         = | ̂    ∗  (   ,    )         (   )|.  (51)  points.
                                            ̄
                      ℓ ,   ℓ ,   ℓ  R−T  ℓ  ℓ  w  F  ℓ
                                                                                                        ∗
                                                               Then, by  ixing    and using the identity       (       ) =
                                                                              ℓ
          5.2 Detection                                           ̄    ∗
                                                               (   ⊗   )       (  ),we can simplify the expression to
          No  w  want  t  kno    those  parameters      con‐
                                                                                 ∗
          sidered      path  det  T      w  tak  into                          ∣ ̂    (   )  (   ) ̂    (   )∣  (56)
                                                                                    ℓ
                                                                                         ℓ
                                                                                              ℓ
                                                                                           T
                                                                                 R
          account    null  hypothesis  of     = 0    that    all                               ∗
                                                                                                    ̄
                                                                                                       ℓ
            of     ar  independent  whit  noise    thus        with   (   ) such that       (  (   )) =          (   ).
                                                                       ℓ
                                                                                        ℓ
                                                                                                  w
                                                                                                    F

            ̂  ∗  (   ,    )        ̄ (   ) is also comprised of white noise
                     ∗
           R−T  ℓ  ℓ    w  F  ℓ                                We then proceed to re ine the angle components with the
            Consequently                      Rayleigh
                                       ℓ ,   ℓ ,   ℓ           hig    of  ant  For  simplicity  let    as‐
          distribution,  which  has  the  cumulative  distribution
                                                               sume that    >       By increasing the resolution of    to
                                                                                                             ℓ
          funtion                                                              r
                                                               32   equally spaced points, we do not need to use the
                                                                   t
                                           2                   sec‐tor beam‐pattern manipulation, thus we can simply
                   (      ) = 1 − exp (−     ℓ ,   ℓ ,   ℓ  ) .  (52)  maximize
                                          2  
                        ℓ ,   ℓ ,   ℓ       2
                                                                                 ∗
                                                                               ∣ ̂    (   )  (   )   (   )∣  (57)
          Since there is a channel contribution only for a small num‐            R  ℓ    ℓ  T  ℓ
          ber of path parameters, we have that the median of all
                                                               over    while the other path parameters are  ixed.
                                                                     ℓ
          computed values of     should be close to that of the
                              ℓ ,   ℓ ,   ℓ                    Finally, we re ine the expression with respect to the re‐
          Rayleigh distribution   √2 ln(2). This insight is key to our  maining angle. Again, the manipulation is not required,
          algorithm. Then,    can be approximated as           and we can maximize
                                                                                 ∗
                         ≃   (     )/√2 ln(2).        (53)                     ∣   (   )  (   )   (   )∣    (58)
                                ℓ ,   ℓ ,   ℓ                                    R  ℓ    ℓ  T  ℓ
          Inthiscase, thecumulativefunctionofmax    canbecom‐  over    while the other path parameters are  ixed.
                                                 
                                                                     ℓ
          puted as     (  ) = ∏    (  ). Explicitly, it is given by
                  max           
                                                               Iteration  steps:   No  that        irst  st  w  re‐
               (max(      )) =
            max         ℓ ,   ℓ ,   ℓ                          moved the angle uncertainty caused by the sector beam‐
                                                      r    t   
                                  max(       ) 2               patt  we can proceed to repeat the same steps itera‐
                      (1 − exp (−          ℓ ,   ℓ ,   ℓ  ))  .  tively by substituting all sector beam‐patterns   ̂ by array
                                       2   2
                                                               responses   .
                                                      (54)
                                                                   parameters  of    path  hav    estimated,
          Using this, we can compute a detection threshold corre‐  (   ,    ,    ), we use them to reconstruct the path and sub‐
                                                                    ℓ
                                                                 ℓ
                                                                      ℓ
          sponding to a con idence level of    as              tract it from the received pilots, thereby altering the resid‐
                                                               ual. Then, the residual is updated, and the next path is ob‐
                                            1
                            √
                     (     ) − log (1 − (  )     r    t    ).  (55)  tained following the same   The residual is updated
                         ℓ ,   ℓ ,   ℓ  2
                                                               until  a  stopping  condition  is  reached,  as  discussed  in
          We compare the optimal value of      obtained by     Section 5.2. How to obtain the best stopping condition for
                                            ℓ ,   ℓ ,   ℓ
          solving (51) with the above threshold to decide whether  our algorithm is discussed in Section 6.3.
                                             © International Telecommunication Union, 2021                    19
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