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which shows that

Ib+U(ΣσiIn)1U(4.2) I_b + U (\Sigma - \sigma_i^* I_n)^{-1} U \quad (4.2)

is a singular matrix. The singularity of (4.2) implies

Qi(Ib+U(ΣσiIn)1U)Pi=(Ri1Ri200),(4.3) Q_i (I_b + U (\Sigma - \sigma_i^* I_n)^{-1} U) P_i = \begin{pmatrix} R_{i1} & R_{i2} \\ \mathbf{0} & \mathbf{0} \end{pmatrix}, \quad (4.3)

i. e., a QR factorization with column pivoting (Golub and Van Loan [17]) with $1 \le m \le b$, an orthonormal matrix $Q_i \in \mathbb{R}^{b \times b}$, a permutation matrix $P_i \in \mathbb{R}^{b \times b}$ (i. e., $Q_i Q_i = P_i P_i = I_b$), a nonsingular upper triangular matrix $R_{i1} \in \mathbb{R}^{(b \ m_1) \times (b \ m_1)}$, and a matrix $R_{i2} \in \mathbb{R}^{(b \ m_2) \times (b \ m_2)}$. The matrix

Xi:=Pi(Ri1Ri2Im)Rb×m(4.4) X_i := P_i \begin{pmatrix} -R_{i1}^{\top} R_{i2} \\ I_m \end{pmatrix} \in \mathbb{R}^{b \times m} \quad (4.4)

has rank m and (because of (4.3)) its columns span the null space of (4.2), i. e.,

(Ib+U(ΣσiIn)1U)Xi=0.(4.5) (I_b + U (\Sigma - \sigma_i^* I_n)^{-1} U) X_i = 0. \quad (4.5)

Computation of the Eigenvectors. Compute the QR factorization of the $n \times m$ matrix

(ΣσiIn)1UXi=ZiSi(4.6) (\Sigma - \sigma_i^* I_n)^{-1} U X_i = Z_i S_i \quad (4.6)

with $Z_i \in \mathbb{R}^{n \times m}$ and nonsingular upper triangular $S_i \in \mathbb{R}^{m \times m}$. The column vectors of $Z_i$ form a set of $l$ orthonormal eigenvectors of $S$. From

(Σ+UUσiIn)Zi=UU(ΣσiIn)1UXiSi1+UXiSi1=U(U(ΣσiIn)1U+Ib)XiSi1=0according to (4.5) \begin{align*} & (\Sigma + UU - \sigma_i^* I_n) Z_i = \\ & UU (\Sigma - \sigma_i^* I_n)^{-1} U X_i S_i^{-1} + U X_i S_i^{-1} = \\ & U (U (\Sigma - \sigma_i^* I_n)^{-1} U + I_b) X_i S_i^{-1} = 0 \quad \text{according to (4.5)} \end{align*}

it follows that $(\Sigma + UU) Z_i = \sigma_i^* Z_i$, i. e., the columns of $Z_i$ are eigenvectors of $S$ corresponding to $\sigma_i^*$. They are orthonormal by construction.

It remains to be shown that all $l$ eigenvectors corresponding to the eigenvalue $\sigma_i^*$ have been found, that is, $m = l$. First, since the geometric multiplicity of an eigenvalue is less or equal its algebraic multiplicity (Horn and Johnson [19]), $m \le l$. Equality can be shown indirectly. Assume that $m < l$. Then there must be another eigenvector $z_i$ of $S$ with $|z_i|_2 = 1$, $z_i^T Z_i z_i = 0$, and, according to (4.1),

(Σ+UUσiIn)zi=0(4.7) (\Sigma + UU - \sigma_i^* I_n) z_i = 0 \quad (4.7)

(Ib+U(ΣσiIn)1U)Uzi=0. (I_b + U (\Sigma - \sigma_i^* I_n)^{-1} U) U z_i = 0.

This implies that $U z_i$ lies in the null space of

Ib+U(ΣσiIn)1U, I_b + U (\Sigma - \sigma_i^* I_n)^{-1} U,

and since $X_i$ is a basis of this null space (according to (4.5)), there exists a vector $y \in \mathbb{R}^m$ such that $U z_i = X_i y$. Thus

(ΣσiIn)1UUzi=(ΣσiIn)1UXiy=(4.6)=ZiSiy. (\Sigma - \sigma_i^* I_n)^{-1} U U z_i = (\Sigma - \sigma_i^* I_n)^{-1} U X_i y = (4.6) = Z_i S_i y.