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v2009.01.01 - Convex Optimization

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584 APPENDIX B. SIMPLE MATRICES<br />

N(u T )<br />

R(E) = N(v T )<br />

0 0 <br />

N(E)=R(u)<br />

R(v)<br />

R N = N(u T ) ⊕ N(E)<br />

R(v) ⊕ R(E) = R N<br />

Figure 134: v T u = 1/ζ . The four fundamental subspaces<br />

)<br />

[289,3.6] of<br />

elementary matrix E as a linear mapping E(x)=<br />

(I − uvT x .<br />

v T u<br />

By the nullspace and range of dyad sum theorem, doublet Π has<br />

N −2 ([ zero-eigenvalues ]) remaining and corresponding eigenvectors spanning<br />

v<br />

T<br />

N<br />

u T . We therefore have<br />

R(Π) = R([u v ]) , N(Π) = v ⊥ ∩ u ⊥ (1520)<br />

of respective dimension 2 and N −2.<br />

B.3 Elementary matrix<br />

A matrix of the form<br />

E = I − ζuv T ∈ R N×N (1521)<br />

where ζ ∈ R is finite and u,v ∈ R N , is called an elementary matrix or a<br />

rank-one modification of the identity. [178] Any elementary matrix in R N×N<br />

has N −1 eigenvalues equal to 1 corresponding to real eigenvectors that<br />

span v ⊥ . The remaining eigenvalue<br />

λ = 1 − ζv T u (1522)<br />

corresponds to eigenvector u . B.6 From [192, App.7.A.26] the determinant:<br />

detE = 1 − tr ( ζuv T) = λ (1523)<br />

B.6 Elementary matrix E is not always diagonalizable because eigenvector u need not be<br />

independent of the others; id est, u∈v ⊥ is possible.

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