For a permutation $\sigma$ of the set $\{1,...,n\}$, and consider the $n \times n$ matrix $A_\sigma$, where the $i^{\text{th}}$ column is the standard vector $e_{\sigma (i)}$. For which $\sigma$ is $A_\sigma$ digonizable over $\mathbb{C}$, and which values for $\mathbb{R}$?
I don't exactly know what I should do. I think I should use the fact that a map is diagnizable iff the characteristic polynomial of t factors in linear factors over the field I'm in, and if $m_g(\lambda)=m_a(\lambda)$ for all eigenvalues
If anyone could start me up or help me out or do one of the examples it would be appreciated, thanks!
Small edit: I don't even know what the matrix looks like, maybe it's just me but I don't find it's clear
It is not hard to check that $A_{\sigma}$ has finite order for each $\sigma \in S_n$, where $S_n$ denotes the group of permutations of the set $\{1,\cdots,n\}$. This is because it is not hard to check that $A_{\sigma}^m = A_{\sigma^m}$, where $\sigma^m$ denotes the $m$-fold composition of $\sigma$ with itself. I don't know how much you are aware of representation theory, but it is a general result of the theory of representation of finite groups that given a (complex) representation $\rho : G \to \mathrm{GL}(V)$, for each $\sigma \in G$, $\rho(\sigma)$ is diagonalizable. I will sketch the proof below, in case you don't know about this. (I will not use the language of representation theory, only complex linear algebra.)
Let $\{e_1,\cdots,e_n\}$ be the $\mathbb C$-basis of $\mathbb C^n$ over which you write $A_{\sigma}$ as normally, i.e. so that $A_{\sigma}(e_i) = e_{\sigma(i)}$. Let $\langle - ,-\rangle$ denote the standard Hermitian inner product on $\mathbb C^n$, and define a new Hermitian inner product $(-,-)$ on $\mathbb C^n$ via $$ (x,y) \overset{def}= \frac 1{n!} \sum_{\sigma \in S_n} \langle A_{\sigma} x, A_{\sigma}y \rangle. $$ It is an easy check that $(-,-)$ satisfies the axiom of an Hermitian inner product (see here). Now since it is an Hermitian inner product, there exists an orthogonal basis $\{v_1,\cdots,v_n\}$ with respect to $(-,-)$. Then under this basis, for $\pi \in S_n$, we have $$ (A_{\pi}v_i, A_{\pi}v_j) = \frac 1{n!} \sum_{\sigma \in S_n} \langle A_{\sigma}(A_{\pi} v_i), A_{\sigma}(A_{\pi}v_j) \rangle = \frac 1{n!} \sum_{\sigma \in S_n} \langle A_{\sigma} v_i, A_{\sigma}v_j \rangle = (v_i, v_j) = \delta_{ij} $$ because summing over all permutations of the form $\sigma \pi$ is the same as summing over all permutations of the form $\sigma$. It follows from this that the vectors $\{A_{\pi}v_1,\cdots,A_{\pi}v_n\}$ are pairwise orthogonal under $(-,-)$, so that the matrix of $A_{\pi}$ over the basis $\{v_1,\cdots,v_n\}$ is unitary with respect to $(-,-)$, thus diagonalizable over $\mathbb C$.
Remark : You can also check that since $A_{\pi}^{n!} = A_{\pi^{n!}} = I$ the identity matrix, all the eigenvalues $\lambda$ of $A_{\pi}$ will satisfy $\lambda^{n!} = 1$, i.e. they are $n!$-roots of unity. (The number $n!$ is just to be safe ; for most eigenvalues the number will be actually much smaller, and $n!$ is actually never attained since $S_n$ is not a cyclic group.) I don't know much about representation theory over the real numbers, but there is probably a well-understood theory of this. I would be surprised that someone into real representation theory would not have characterized this already.
Hope that helps,