Let $c$ be a complex number. Consider the family of $n\times n$ matrices $M_n$ which have $c$'s on one off-diagonal, $\bar{c}$'s on the other off-diagonal, and zero everywhere else. So $M_4$ looks like this:$$\left(\begin{array}{cccc}0&c&0&0\\\bar{c}&0&c&0\\0&\bar{c}&0&c\\0&0&\bar{c}&0\end{array}\right)$$How does one find a general formula for the operator norm of $M_n$?
2026-03-26 07:59:23.1774511963
Operator norm of a family of matrices
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Write $c=\alpha|c|$, with $|\alpha|=1$. Then $$ M_4=|c|\,\begin{bmatrix} 1&0&0&0\\ 0&\alpha&0&0\\ 0&0&\alpha^2&0\\ 0&0&0&\alpha^3\end{bmatrix} \begin{bmatrix} 0&1&0&0\\ 1&0&1&0\\ 0&1&0&1\\ 0&0&1&0 \end{bmatrix} \begin{bmatrix} 1&0&0&0\\ 0&\alpha&0&0\\ 0&0&\alpha^2&0\\ 0&0&0&\alpha^3\end{bmatrix}^*, $$ and so $M_4(c)$ is unitarily equivalent to $|c|\,M_4(1)$. Thus we only need to determine the spectrum of $M_4(1)$. The same argument applies for $M_n$ for any $n$.
The eigenvalues of $M_n(1)$ are $\lambda_k=2\cos\frac{k\pi}{n+1}$, where an eigenvector for $\lambda_k$ is $\sum_{s=1}^n\sin\frac{ks\pi}{n+1}e_s$, and $e_1,\ldots,e_n$ is the canonical basis.
As $M_n(1)$ is selfadjoint, its norm is the greatest eigenvalue in absolute value, so $$ \|M_n(c)\|=|c|\,\|M_n(1)\|=2|c|\,\cos\frac{\pi}{n+1}. $$
$\newcommand\abajo{\\ \ \\}$
Edit: The Eigenvalues of $M_n(1)$.
Let $e_1,\ldots,e_n$ be the canonical basis of $\mathbb C^n$. Let $\eta_k=\sum_{\ell=1}^n\sin\frac{k\ell\pi}{n+1}\,e_\ell$, $k=1,\ldots,n$. Then
\begin{align*} M_n(1)\eta_k &=\sum_{s=1}^{n-1}\sin\frac{sk\pi}{n+1}\,e_{s+1}+\sum_{s=2}^{n}\sin\frac{sk\pi}{n+1}\,e_{s-1} \abajo &=\sin\frac{2k\pi}{n+1}\,e_1+\sum_{s=2}^{n-1}\left(\sin\frac{(s-1)k\pi}{n+1}+\sin\frac{(s+1)k\pi}{n+1}\right)\,e_{s} +\sin\frac{(n-1)k\pi}{n+1}\,e_{n} \abajo &=2\cos\frac{k\pi}{n+1}\sin\frac{k\pi}{n+1}\,e_1+\sum_{s=2}^{n-1}2\cos\frac{k\pi}{n+1}\sin\frac{sk\pi}{n+1}\,e_s+2\cos\frac{k\pi}{n+1}\sin\frac{nk\pi}{n+1}\abajo &=2\cos\frac{k\pi}{n+1}\,\eta_k. \end{align*} All the above requires is the sine of a sum formula.