Digital Signal Processing Reference
In-Depth Information
where Λ h is the diagonal matrix of J singular values of H in the order
σ h, 0
σ h, 1
...
σ h,M− 1
....
(14 . 19)
We then have the following result:
Lemma 14.1. Bound on φ. For a given channel H the quantity φ in Eq.
(14.17) is bounded as
1
M− 1
k =0
φ
(14 . 20)
σ h,k
The bound is achieved by choosing the M
×
J equalizer G to be
G =[ U h ] M×J ,
(14 . 21)
where the right-hand side denotes the submatrix defined by the first M rows of
U h .
=0in
the denominator of Eq. (14.20). To proceed with the proof of the lemma, it is
convenient to represent G in terms of its SVD matrices:
Note that the assumption that H has rank
M ensures that σ h,k
0 ] V g ,
G = U g [ Σ g
(14 . 22)
where U g is M
×
M unitary, V g is J
×
J unitary, and Σ g is M
×
M diagonal
with positive diagonal elements (singular values of G ).
Proof of Lemma 14.1. Using Hadamard's inequality for positive definite
matrices (Appendix B) we have
M− 1
M− 1
det( GG )
det( GHH G )
[( GHH G ) 1 ] kk
[ GG ] kk
φ =
(14 . 23)
k =0
k =0
with equality if and only if ( GG )and[( GHH G )] are diagonal. From
Eq. (14.22) we have
0 ] V g V g Σ g
0 ] Σ g
0
GG = U g [ Σ g
U g = U g [ Σ g
U g
0
and
0 ] V g HH V g Σ g
GHH G = U g [ Σ g
U g .
0
So
det( GG )=det( Σ g Σ g )
(14 . 24 a )
and
det( GHH G )=det( Σ g Σ g )det( V g HH V g ) M
(14 . 24 b )
 
Search WWH ::




Custom Search