I'm trying to find the spectrum of the convolution operator and understand $$T : L_2 \left[ -\pi, \pi \right] \longrightarrow L_2\left[ -\pi, \pi \right],$$ $$ f(t) \longmapsto \int_{-\pi}^\pi \sin^2(t-s)f(s) \, \mathrm{d}s. $$
I think the best option would be to go over to the Fourier transform $F$ due to this answer enter link description here. But the Fourier transformation is defined in space $L_2 (\mathbb{R}) $ (as a limit on the Schwarz class) ($F : L_2 (\mathbb{R}) \longrightarrow L_2 (\mathbb{R}) $). Then we know that $L_2\left[ -\pi, \pi \right] \subset L_2 (\mathbb{R}) $ and $F \circ T \circ F^{-1} : F \left( L_2\left[ -\pi, \pi \right] \right) \longrightarrow F \left( L_2\left[ -\pi, \pi \right] \right)$.
In this case we get that the operator $F \circ T \circ F^{-1} $ is the multiplication operator $F \circ T \circ F^{-1} = M_{g}$, where $$g(x) = \int_{-\pi}^\pi \sin^2 (t) e^{-ixt } \, \mathrm{d}t$$
We know also that $\sigma(M_g) = \sigma \left(F \circ T \circ F^{-1} \right) =\sigma(T)$. But then we want to define spectrum of $T$. We know that in $ B \left(L_2 \left( \mathbb{R} \right) \right)$ spectrum of $M_g$ is essential range of $g$ (in this case is simply range).
But our space is not all $L_2\left( \mathbb{R} \right)$, we only have a part $ \operatorname{Im}(F) = F \left( L_2\left[ -\pi, \pi \right] \right) $ and i don't know how to show that in $B(\operatorname{Im}(F))$ operator $M_g$ has the same spectrum.
Sorry for my english and thank you very much!
Using standard trig identities: \begin{align} \cos(2(t-s)) & = \cos^2(t-s)-\sin^2(t-s) \\ & = 1-2\sin^2(t-s)\\ \sin^2( t -s) & = \frac{1-\cos(2(t-s))}{2} \\ & = \frac{1-\cos(2t)\cos(2s)-\sin(2t)\sin(2s)}{2}. \end{align} Therefore, $T$ has a simple form: $$ Tf = \frac{1}{2}\langle f,1\rangle 1 - \frac{1}{2}\langle f,\sin(2s)\rangle\sin(2t) - \frac{1}{2}\langle f,\cos(2s)\rangle\cos(2t). $$ Your operator $T$ reduces to a matrix operator on the subspace $M$ spanned by the orthonormal basis $\left\{\frac{1}{\sqrt{\pi}},\sqrt{\frac{2}{\pi}}\cos(2t),\sqrt{\frac{2}{\pi}}\sin(2t)\right\}$, and $T$ is $0$ on the orthogonal complement of $M$. These basis elements are eigenvectors of $T$. So the operator $T$ is diagonalized on this orthonormal basis. The spectrum is the union of these eigenvalues and $0$. A finite rank operator such as this one is always compact.