Yes, you can obtain the $O(n^{-2})$ bound for each sum for almost all values of $c$, the edge case being $c=2\pi n,\ n\in\mathbb{Z}\ $ in which case $\sin(cj)=0$ and $\cos(cj)=1$ giving $O(n^{-1})$. From now I'll assume that $c\not= 2\pi n$ for convenience.
Firstly, it's useful to know that the sum of $\sin(cn)$ on its own is bounded by a constant depending on $c$, remember we already handled the edge case. You can show this using $\sin(x)=(e^{ix}-e^{-ix})/2i$ and the formula for a geometric series, but a proof is also given here.
To take advantage of this fact, we use partial summation. If you define
$$S_c(n) := \sum_{k=1}^n{\sin(cn)} = O_c(1)$$
or equivalently using $\cos(cn)$, then for $N\ge n$ we have
$$\sum_{j=n}^N{\frac{\sin(cj)}{j^2}} = \sum_{j=n}^N{\frac{S_c(n)-S_c(n-1)}{j^2}}$$
$$= \sum_{j=n}^N{\frac{S_c(n)}{j^2}} - \sum_{j=n-1}^{N-1}{\frac{S_c(n)}{(j+1)^2}}\tag{re-indexing to make the $S_c(n)$'s the same}$$
$$= \frac{S_c(n-1)}{n^2} + \frac{S_c(N)}{(N+1)^2} + \sum_{j=n}^N{S_c(n)\left(\frac{1}{j^2} - \frac{1}{(j+1)^2}\right)}$$
$$= O_c\left(\frac{1}{n^2}\right) + O_c\left(\frac{1}{N^2}\right) + \sum_{j=n}^N{O_c\left(\frac{1}{j^3}\right)} = O_c(n^{-2}) + O_c(N^{-2})$$
Letting $N\to\infty$ gives you the result. Although I skipped the sum containing $\cos(cj)$, using $\cos(x) = (e^{ix}+e^{-ix})/2$ and the same method as above you should get the same result.
Remark: The same process can be done with pretty much any nice function, not necessarily $j^p$ however, Abel Summation is probably more suited for this as it uses integration which will give the bound directly.