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TEL AVIV UNIVERSITY Gaddi Blumrosen

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4.4.4 OSTBC with linear antenna weighting, based on only channel covariance<br />

feedback (ML sub-optimal)<br />

As we seen from previous chapters, the optimal weights are thus obtained by the<br />

conditioned value of the first two moments. If we assume, as in [31], the following<br />

scenario of no direct measurement of the channel is known to the transmitter, but only<br />

the channel covariance matrix, we can assume, in the case of the Rayleigh channel a<br />

zero mean value , m 0 , and no correlation between the channel covariance<br />

hh | ˆ<br />

approximation and its real value, R R .<br />

hh| hˆ<br />

Consequently, the solution can be substantially simplified, especially for the case of<br />

correlated channel coefficients. Note that although [31] does not use conditional<br />

covariance matrix (measure of CSI quality), it has shown that for this scenario of<br />

Gaussian channel with zero conditional channel mean value, same antenna weights<br />

are derived also for non perfect CSI.<br />

Using those relations and multiplying (4.14) by , we obtain:<br />

<br />

l( Z) log det I RhhZ (4.24)<br />

Let us further perform Singular Value decomposition (SVD) over the channel<br />

covariance matrix, , where is the unitary eigenvector matrix and<br />

is the corresponding square root eigenvalue matrix.<br />

<br />

<br />

H<br />

Rhh Uh DhU h<br />

h U<br />

D h<br />

Let us further define, as in [30], the diagonal matrix D as:<br />

2<br />

f<br />

<br />

D W U W U<br />

H<br />

T h T h<br />

(4.25)<br />

2<br />

As in [30], maximization of (4.24) force the matrices RhhZ and DD h f to be diagonal.<br />

Now, by substitution of Rhh Uh<br />

DhU h and Z WTWT<br />

into (4.24) and simple<br />

algebraic manipulation, relying on the symmetry of the matrices R and Z and the<br />

unitary of U , we obtain the same minimization expression as in [30]:<br />

h<br />

2 <br />

l( D f ) log det I DhD f <br />

hh<br />

H<br />

(4.26)<br />

Explicit expressions, for the k th beam obtained after power loading according to the<br />

power loading algorithm in [30] in the direction corresponding to the k th eigenvector,<br />

which minimizes (4.26), was found to be:<br />

H<br />

Wk D f Uk<br />

(4.27)<br />

The assumptions above, 0 and R <br />

R , make sense in fast fading<br />

mhh | ˆ <br />

hh| hˆ<br />

scenarios. Since both algorithms (in [25] and in [31]) minimize PEP, we expect the<br />

performance of the system of [25], and [31], to be the same in fast fading channel. In<br />

case of slow fading, if we have strong nonzero conditional channel mean value, as in<br />

Rician fading, we expect the solution in (4.14) to enhance the system performance.<br />

R hh<br />

hh<br />

f<br />

H<br />

hh

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