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Praise for Fundamentals of WiMAX

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170 Chapter 5 • Multiple-Antenna Techniques5.4.1 DOA-Based Beam<strong>for</strong>mingThe incoming signals to a receiver may consist <strong>of</strong> desired energy and interference energy—<strong>for</strong>example, from other users or from multipath reflections. The various signals can be characterizedin terms <strong>of</strong> the DOA or the angle <strong>of</strong> arrival (AOA) <strong>of</strong> each received signal. Each DOA canbe estimated by using signal-processing techniques, such as the MUSIC, ESPRIT, and MLEalgorithms (see [27, 38] and the references therein). From these acquired DOAs, a beam<strong>for</strong>merextracts a weighting vector <strong>for</strong> the antenna elements and uses it to transmit or receive the desiredsignal <strong>of</strong> a specific user while suppressing the undesired interference signals.When the plane wave arrives at the d-spaced uni<strong>for</strong>m linear array (ULA) with AOA θ, thewave at the first antenna element travels an additional distance <strong>of</strong> d sin θ to arrive at the secondelement. This difference in propagation distance between the adjacent antenna elements can be<strong>for</strong>mulated as an arrival-time delay, τ = dcsin / θ. As a result, the signal arriving at the secondantenna can be expressed in terms <strong>of</strong> signal at the first antenna element asy2()= t y1() t exp( − j2 πfcτ),d sin θ= y1( t) exp( − j2 π ).λN r(5.43)For an antenna array with elements all spaced by d , the resulting received signal vectorcan there<strong>for</strong>e be expressed asT()=[ t y1() t y2() t … yN ()] trd sin θd sin θ T= y1( t)[1 exp( − j2 π ) … exp( −j2 π( Nr−1) )] ,λλa( θ)(5.44)where a( θ)is the array response vector.In the following, we show an example to demonstrate the principle <strong>of</strong> DOA-based beam<strong>for</strong>ming.Consider a three-element ULA with d = λ/2spacing between the antenna elements.Assume that the desired user’s signal is received with an AOA <strong>of</strong> θ 1=0—that is, the signal iscoming from the broadside <strong>of</strong> the ULA—and two interfering signals are received with AOAs <strong>of</strong>θ 2 = π/3 and θ 3 = –π/6, respectively. The array response vectors are then given by3πT⎡ − j π2 3a θa θπ⎤− j⎡ j2( 1) =111 [ ] , ( 2)= ⎢1 e e ⎥ , and a( θ3) = ⎢1e e⎣⎢⎦⎥⎣TjπT⎤⎥ .⎦(5.45)The beam<strong>for</strong>ming weight vector w =[ w should increase the antenna gain in the1w2 w ]T3direction <strong>of</strong> the desired user while simultaneously minimizing the gain in the directions <strong>of</strong> interferers.Thus, the weight vector w should satisfy the following criterion:( ) ( ) ( ) ⎦ [ ] T*w ⎡⎣a θ1 a θ2 a θ ⎤3=100 ,(5.46)

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