3.6 Appendix


3.6.1 Proofs for Section 3.3.1

Proof of Theorem 3.1

Denote graphics/161fig02.gif and graphics/161fig03.gif . We have the following differential (at Y ):

Equation 3.231

graphics/03equ231.gif


The differential of the form II group -blind detector,

Equation 3.232

graphics/03equ232.gif


is then given by

Equation 3.233

graphics/03equ233.gif


It then follows from Lemma 2.6 that graphics/w1.gif is asymptotically Gaussian. To find C w , notice that u 1 range ( U s ). Hence, by Proposition 2.6, we have

Equation 3.234

graphics/03equ234.gif


with

Equation 3.235

graphics/03equ235.gif


Equation 3.236

graphics/03equ236.gif


Therefore, the asymptotic covariance of graphics/w1.gif is given by

Equation 3.237

graphics/03equ237.gif


It is easily verified that QY u 1 = . Using this and the facts that w 1 = Y u 1 and QU n = U n , by substituting (3.234) into (3.237), we obtain (3.61).

Proof of Corollary 3.1

In this appendix e k denotes the k th unit vector in graphics/rk.gif and graphics/etilde.gif denotes the k th unit vector in graphics/rktilde.gif . Denote graphics/163fig01.gif and graphics/163fig09.gif . Denote further that graphics/163fig03.gif and graphics/163fig04.gif . Note that ( Ys k ) is the linear MMSE detector for the k th user , given by

Equation 3.238

graphics/03equ238.gif


Denote

Equation 3.239

graphics/03equ239.gif


Equation 3.240

graphics/03equ240.gif


Equation 3.241

graphics/03equ241.gif


Equation 3.242

graphics/03equ242.gif


First we compute the term tr ( C w C r ). Using (3.61) and the facts that graphics/163fig01a.gif graphics/163fig01b.gif , we have

Equation 3.243

graphics/03equ243.gif


The term ( graphics/163fig06.gif ) in (3.243) can be computed as

Equation 3.244

graphics/03equ244.gif


Using the fact that graphics/163fig07.gif , the term tr ( QYQ T X ) in (3.243) is given by

Equation 3.245

graphics/03equ245.gif


To compute the second term in (3.243), first note that graphics/164fig01.gif . We have

Equation 3.246

graphics/03equ246.gif


where the first equality follows from the fact that QY graphics/stilde.gif = . Moreover,

Equation 3.247

graphics/03equ247.gif


where we used the fact that YXY = Y . In (3.246) graphics/dbar.gif is given by

Equation 3.248

graphics/03equ248.gif


Equation 3.249

graphics/03equ249.gif


Substituting (3.247) and (3.249) into (3.246) we obtain the second term in (3.243):

Equation 3.250

graphics/03equ250.gif


Finally, we compute t in the last term in (3.243). By definition,

Equation 3.251

graphics/03equ251.gif


where

Equation 3.252

graphics/03equ252.gif


Equation 3.253

graphics/03equ253.gif


Equation 3.254

graphics/03equ254.gif


with graphics/165fig01.gif . Substituting (3.244), (3.245), (3.250), and (3.251) into (3.243), we have

Equation 3.255

graphics/03equ255.gif


Moreover, we have

Equation 3.256

graphics/03equ256.gif


Next we compute w 1 2 . Since

Equation 3.257

graphics/03equ257.gif


Equation 3.258

graphics/03equ258.gif


we have

Equation 3.259

graphics/03equ259.gif


By (3.255) “(3.259) we obtain the corollary.

SINR Calculation for Example 2

Substituting (2.338) “(2.340) and A 2 = A 2 I K into (3.66) “(3.68), we have

Equation 3.260

graphics/03equ260.gif


Equation 3.261

graphics/03equ261.gif


Equation 3.262

graphics/03equ262.gif


Equation 3.263

graphics/03equ263.gif


Equation 3.264

graphics/03equ264.gif


where graphics/166fig01.gif , graphics/166fig02.gif , graphics/1tilde.gif denotes an all-1 graphics/ktilde.gif -vector, and graphics/1bar.gif denotes an all-1 ( graphics/110fig05.gif )-vector. After some manipulations, we obtain the following expressions:

Equation 3.265

graphics/03equ265.gif


Equation 3.266

graphics/03equ266.gif


Equation 3.267

graphics/03equ267.gif


Equation 3.268

graphics/03equ268.gif


Equation 3.269

graphics/03equ269.gif


Equation 3.270

graphics/03equ270.gif


Substituting (3.265) “(3.270) into (3.69) “(3.72), and letting

Equation 3.271

graphics/03equ271.gif


Equation 3.272

graphics/03equ272.gif


Equation 3.273

graphics/03equ273.gif


Equation 3.274

graphics/03equ274.gif


Equation 3.275

graphics/03equ275.gif


we obtain (3.82).

3.6.2 Proofs for Section 3.3.2

Proof of Theorem 3.2

We prove this theorem for the case of a linear group-blind hybrid detector (i.e., graphics/166fig03.gif ). The proof for a linear group-blind MMSE detector is essentially the same.

Denote e k as the k th unit vector in graphics/rn.gif . Let Q 1 be an orthogonal transformation such that

Equation 3.276

graphics/03equ276.gif


For any graphics/167fig02.gif , denote graphics/167fig01.gif . The corresponding projection matrix in the Q 1 - rotated coordinate system is

Equation 3.277

graphics/03equ277.gif


Equation 3.278

graphics/03equ278.gif


Equation 3.279

graphics/03equ279.gif


Denote

Equation 3.280

graphics/03equ280.gif


Equation 3.281

graphics/03equ281.gif


where the dimension of graphics/c11q.gif is (N “ graphics/ktilde.gif ) x (N “ graphics/ktilde.gif ). Hence

Equation 3.282

graphics/03equ282.gif


Let the eigendecomposition of graphics/c11q.gif be [1]

[1] The eigenvalues are unchanged by similarity transformations.

Equation 3.283

graphics/03equ283.gif


Define another orthogonal transformation,

Equation 3.284

graphics/03equ284.gif


For any graphics/167fig02.gif , denote graphics/167fig03.gif . In what follows, we compute the asymptotic covariance matrix of the detector in the Q 1 Q 2 -rotated coordinate system. In this new coordinate system, we have

Equation 3.285

graphics/03equ285.gif


Equation 3.286

graphics/03equ286.gif


Equation 3.287

graphics/03equ287.gif


Equation 3.288

graphics/03equ288.gif


Furthermore, after rotation, graphics/168fig01.gif has the form

Equation 3.289

graphics/03equ289.gif


for some graphics/168fig08.gif . After some manipulations, the form I group-blind hybrid detector in the new coordinate system has the form

Equation 3.290

graphics/03equ290.gif


where E s consists of the first graphics/168fig03.gif columns of graphics/168fig09.gif (i.e., graphics/168fig09.gif = [ E s E n ]). Let the estimated autocorrelation matrix in the rotated coordinate system be

Equation 3.291

graphics/03equ291.gif


Let the corresponding eigendecomposition of graphics/168fig02.gif be

Equation 3.292

graphics/03equ292.gif


Then the estimated detector in the same coordinate system is given by

graphics/168equ01.gif


Note that in such a rotated coordinate system, estimation error occurs only in the first graphics/168fig03.gif elements of graphics/168fig04.gif . Denote

Equation 3.293

graphics/03equ293.gif


Equation 3.294

graphics/03equ294.gif


Hence graphics/mcirc.gif is a function of graphics/168fig05.gif and its differential at graphics/168fig10.gif (i.e., graphics/168fig06.gif and graphics/168fig07.gif is given by

Equation 3.295

graphics/03equ295.gif


By Lemma 2.6, graphics/mcirc.gif is then asymptotically Gaussian with a covariance matrix given by

Equation 3.296

graphics/03equ296.gif


We next compute the three terms T 1 , T 2 , and T 3 in (3.296).

We first compute T 1 . Denote z k and x k as the subvectors of graphics/169fig01.gif containing, respectively, the first N graphics/ktilde.gif and the last graphics/ktilde.gif elements of graphics/169fig01.gif (i.e., graphics/169fig02.gif ) for k = graphics/ktilde.gif + 1, . . . , K . Let graphics/169fig05.gif . It is clear that graphics/169fig06.gif range ( U s ), and therefore graphics/169fig03.gif range ( graphics/ubars.gif ). Expressed in the rotated coordinate system, we have graphics/169fig04.gif range ( E s ). We can therefore apply Proposition 2.6 to T 1 to obtain

Equation 3.297

graphics/03equ297.gif


with

Equation 3.298

graphics/03equ298.gif


Equation 3.299

graphics/03equ299.gif


The term T 2 can be computed following a similar derivation as in the proof of Theorem 1 for the DMI blind detector. Specifically, we have, similar to (2.302),

Equation 3.300

graphics/03equ300.gif


Writing (3.300) in matrix form, we have

Equation 3.301

graphics/03equ301.gif


with

Equation 3.302

graphics/03equ302.gif


Hence the second term in (3.296) is

Equation 3.303

graphics/03equ303.gif


where we have used the fact that graphics/170fig01.gif , and the definition in (3.293).

Finally, we calculate T 3 . Denote graphics/170fig02.gif . By following the same derivation leading to (2.313), we get for i K graphics/ktilde.gif ,

Equation 3.304

graphics/03equ304.gif


As before, we only have to consider [ T 3 ] i,j for i,j K graphics/ktilde.gif or i,j > K graphics/ktilde.gif . However, all terms corresponding to i,j > K graphics/ktilde.gif will be nulled out because of the multiplication of Y on T 3 . Using Lemma 2.5, we then get (for i,j K graphics/ktilde.gif )

Equation 3.305

graphics/03equ305a.gif


graphics/03equ305b.gif

Writing this in matrix form, we have

Equation 3.306

graphics/03equ306.gif


Equation 3.307

graphics/03equ307.gif


Hence the third term in (3.296) is given by

Equation 3.308

graphics/03equ308.gif


Substituting (3.297), (3.303), and (3.308) into (3.296), we obtain

Equation 3.309

graphics/03equ309.gif


where D 1 and D 2 are given, respectively, by (3.299) and (3.302), and t is given by (3.298). Theorem 3 is now easily obtained by transforming (3.309) back to the original coordinate system according to the following mappings: graphics/171fig04.gif , graphics/171fig03.gif , graphics/171fig06.gif , graphics/171fig07.gif and graphics/171fig01.gif graphics/171fig02.gif .



Wireless Communication Systems
Wireless Communication Systems: Advanced Techniques for Signal Reception (paperback)
ISBN: 0137020805
EAN: 2147483647
Year: 2003
Pages: 91

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