My question pertains to the material in the book "The Algebraic Eigenvalue Problem" by J.H. Wilkinson. Section "Symmetric matrix of rank unity", pages 96-97.
The setup is as follows. We have a symmetric $n \times n$ matrix $A$ and $B = vv^T$ is a rank one projector. It is possible to show that there exists an orthogonal matrix $Q$ such that $$ Q^T(A + B)Q = \begin{bmatrix} \alpha & b^T \\ b & \text{diag}(\alpha_i) \\ \end{bmatrix} + \begin{bmatrix} \rho & O \\ O & O \\ \end{bmatrix}. \tag{1} $$ Here $\rho$ is a non-zero eigenvalue of $B$, $O$ denotes blocks of zeroes, $\alpha$ is a scalar and $\text{diag}(\alpha_i)$ is a diagonal submatrix.
The eigenvalue of $A$ denoted as $\lambda_i(A)$ and eigenvalue $\lambda_i(A+B)$ of $A+B$ are therefore those of $$ \begin{bmatrix} \alpha & b^T \\ b & \text{diag}(\alpha_i) \\ \end{bmatrix} \textrm{ and } \begin{bmatrix} \alpha + \rho & b^T \\ b & \text{diag}(\alpha_i) \\ \end{bmatrix}.\tag{2} $$
The claim is that $\lambda_i(A+B)$ satisfies the following relation: $$ \lambda_i(A+B) = \lambda_i(A) + m_i \rho, $$ where $0 \leq m_i \leq 1$ and $\sum m_i = 1.$
I don't understand where this $m_i$ comes from and why all $m_i \in [0,1]$ add up to 1? How does this follow from (1) and (2)?
Let $Q^TAQ = A_1$ and $Q^TBQ = B_1.$ Consider the former's characteristic polynomial: $$p_{A_1}(x) = \det(xI-A_1) = \prod_{i=1}^n(x-\alpha_i) - \prod_{i=2}^n(x-\alpha_i)\sum_{i=2}^n\dfrac{b_i^2}{x-\alpha_i} = f(x)\left(x-\alpha-\sum_{i=2}^n\dfrac{b_i^2}{x-\alpha_i}\right)$$ with the notation $\alpha = \alpha_1$ and $\text{diag}(\alpha_i) = \text{diag}(\alpha_2,\ldots ,\alpha_n)$ and $f(x) = (x-\alpha_2)\ldots (x-\alpha_n),$ which is simply due to the Laplace expansion formula along the first row. So one also has: $$p_{A_1+B_1}(x) = f(x)\left(x-\alpha-\rho-\sum_{i=2}^n\dfrac{b_i^2}{x-\alpha_i}\right).$$
Now the conclusion should follow almost immediately. First, note that $\dfrac{b_i^2}{x-\alpha_i}$ is simply a notational convenience, since it is not defined at $x = \alpha_i.$ Second, if $A_1$ had an eigenvalue $\lambda$ with multiplicity greater than $1,$ then $p_{A_1+B_1}$ also has $\lambda$ as it's eigenvalue with multiplicity one less than the former, so we have: $$\lambda_{A+B} = \lambda_A + m_i\rho$$ with $m_i = 0.$ So let's only focus on simple eigenvalues from now on (this implies $\alpha_i$ cannot be an eigenvalue). If $\lambda$ is an eigenvalue of $A$, then (and assue WLOG $\rho > 0$): $$\dfrac{p_{A_1+B_1}(\lambda)}{f(\lambda)} = -\rho <0$$ and $$\dfrac{p_{A_1+B_1}(\lambda+\rho)}{f(\lambda+\rho)} = \lambda-\alpha-\sum_{i=2}^n\dfrac{b_i^2}{\lambda+\rho-\alpha_i} = \sum_{i=2}^n\left(\dfrac{b_i^2}{\lambda-\alpha_i}-\dfrac{b_i^2}{\lambda+\rho-\alpha_i}\right)>0.$$ Therefore, $p_{A_1+B_1}(\mu) = 0$ for some $\mu\in(\lambda, \lambda+\rho),$ which you can write as $\mu = \lambda + m\rho$ for some $m\in(0,1).$ This and the part about repeated eigenvalues finish the conclusion if you observe that: $$\text{Tr}(A_1+B_1) = \text{Tr}(A_1) + \rho.$$
Note: The solution isn't written perfectly here. Specifically, the notation short hand: $$\dfrac{f(x)}{x-\alpha_i} = \prod_{j=2, j\neq i}(x-\alpha_j)$$ could probably be made better.