This is well-known: eigenvalues for this 3×3 are:
\[
\lambda_k = 2-2\cos\left(\frac{k\pi}{4}\right)\quad (k=1,2,3)
\]
which numerically give approximately \(2-2\cos(\pi/4)=2-\sqrt2\), \(2\) and \(2+ \sqrt2\).
Analytical factorization gives eigenvalues \(\lambda_1=2-\sqrt2,\ \lambda_2=2,\ \lambda_3=2+\sqrt2\).
Eigenvectors (up to scaling) can be chosen as:
\[
\lambda=2:\ v=[-1,0,1]^T,\quad
\lambda=2-\sqrt2:\ v=[1,\sqrt2,1]^T,\quad
\lambda=2+\sqrt2:\ v=[1,-\sqrt2,1]^T.
\]
(You can confirm by substitution \(Jv=\lambda v\).)