Essential spectrum of squared operator 
Let $A\colon D(A) \to \mathcal H$ be a self-adjoint operator on a separable Hilbert space $\mathcal H$. Prove that 
  $$\sigma_{\text{ess}}(A^2) = \left( \sigma_{\text{ess}}(A) \right)^2,$$where $\sigma_{\text{ess}}(A^2)$ denotes the essential spectrum, that is 
  $$\sigma_{\text{ess}}(A) := \\ \sigma(A) \setminus \{\lambda \in \sigma(A):  \lambda \text{ is an eigenvalue of } A \text{ isolated in } \sigma(A) \text{ and has finite mult.}\}$$

I attempted this using Weyl sequences: Let $\{x_n\}_{n\in \mathbb N}$ be a (singular) Weyl sequence, that is $\lVert x_n \rVert = 1, \lVert (A-\lambda) x_n \rVert \to 0$ strongly, $x_n \rightharpoonup 0$ weakly. I want to show that $-\sqrt{\lambda}$ or $\sqrt{\lambda}$ is in the essential spectrum of $A$. To that end, I think I can claim that $\{x_n\}_{n\in \mathbb N}$ is a singular Weyl sequence for $-\sqrt{\lambda}$ or, if not, $\left((A+\sqrt{\lambda})x_n\right)_{n\in \mathbb N}$ is a Weyl sequence for $\sqrt{\lambda}$. However, this ended in messy calculations and I couldn't conclude without knowing $A$ to be bounded. Any hints appreciated.
(Removed wrong proof)
 A: Check the following:


*

*If a point $\lambda\in \sigma(A)$ is not an eigenvalue of $A$ then $\lambda$ is not isolated in $\sigma(A)$.

*$\lambda$ is "isolated from" $\sigma(A)^2 \iff \pm\sqrt{\lambda}$ are both "isolated from" $\sigma(A)$. This tells you: $\lambda$ is not isolated from $\sigma(A)^2 \iff $ at least one of $\pm\sqrt\lambda$ is not isolated from $\sigma(A)$.  Here "isolated from" just means isolated point except that the point is not necessarily in the set.

*The eigenspace $E_\lambda(A^2) = E_{+\sqrt\lambda}(A) + E_{-\sqrt\lambda}(A)$, in particular if the lefthand side is an infinite dimensional space one of the spaces on the righthand side is infinite dimensional.
Now make use of $\sigma(A^2)=\sigma(A)^2$.
A point $\lambda$ is in $\sigma_{ess}(A^2)$ if and only if it is either not an eigenvalue of $A^2$ (in which case both of $\pm\sqrt\lambda$ are not an eigenvalue of $A$), it is not isolated from $\sigma(A^2)$ (in which case one of $\pm\sqrt\lambda$ is not isolated from $\sigma(A)$), or its eigenspace is infinite dimensional (in which case one of the eigenspaces of $\pm\sqrt\lambda$ must be infinite dimensional). This gives $\sigma_{ess}(A^2)\subseteq \sigma_{ess}(A)^2$.
A point $\lambda$ is in $\sigma_{ess}(A)^2$ if and only if either one of the roots $\pm\sqrt\lambda$ is not an eigenvalue (in which case that root is not isolated in $\sigma(A)$, hence its square $\lambda$ is not an isolated point of $\sigma(A^2)$), one of the roots is not isolated in $\sigma(A)$ (in which case the square also is not isolated), or the eigenspace to $A$ of one of the roots is infinite dimensional (in which case the eiegenspace to $A^2$ of $\lambda$ is also infinite dimensional). This gives $\sigma_{ess}(A)^2\subseteq \sigma_{ess}(A^2)$.
