The equation $f(x+1)-f(x)=\sin(x)$ determines $f$ up to the interval $[0,1)$ Thus, any function $[0,1)\to\mathbb{R}$ can be extended to be a solution of the functional equation above over $\mathbb{R}.$ Let $\alpha\in[0,1),$ hence $f(\alpha+1)-f(\alpha)=\sin(\alpha).$ The equation holding for all $x$ in $\mathbb{R}$ thus implies that $f(\alpha+2)-f(\alpha+1)=
\sin(\alpha+1),$ and in general, $f(\alpha+n+1)-f(\alpha+n)=\sin(\alpha+n).$ Thus, $$\sum_{n=0}^{m-1}f(\alpha+n+1)-f(\alpha+n)=\sum_{n=0}^{m-1}\sin(\alpha+n)=f(\alpha+m)-f(\alpha).$$ Hence, for all $\alpha\in[0,1),$ $$f(\alpha+m)=f(\alpha)+\sum_{n=0}^{m-1}\sin(\alpha+n).$$ Notice that $\sin(\alpha+n)=\sin(\alpha)\cos(n)+\cos(\alpha)\sin(n),$ so $$f(\alpha+m)=f(\alpha)+\sum_{n=0}^{m-1}[\sin(\alpha)\cos(n)+\cos(\alpha)\sin(n)]$$ $$=f(\alpha)+\sin(\alpha)\sum_{n=0}^{m-1}\cos(n)+\cos(\alpha)\sum_{n=0}^{m-1}\sin(n).$$ Remember that $$\cos(n)=\frac{e^{in}+e^{-in}}2,$$ so $$\sum_{n=0}^{m-1}\cos(n)=\frac12\left[\sum_{n=0}^{m-1}(e^i)^n+\sum_{n=0}^{m-1}(e^{-i})^n\right]=\frac12\left[\frac{1-e^{im}}{1-e^i}+\frac{1-e^{-im}}{1-e^{-i}}\right]=\frac12\left[\frac{1-e^{im}}{1-e^i}\frac{1-e^{-i}}{1-e^{-i}}+\frac{1-e^{-im}}{1-e^{-i}}\frac{1-e^i}{1-e^i}\right]=\frac14\left[\frac{(1-e^{im})(1-e^{-i})+(1-e^{-im})(1-e^i)}{1-\cos(1)}\right]=\frac14\left[\frac{1-e^{-i}-e^{im}+e^{i(m-1)}+1-e^i-e^{-im}+e^{-i(m-1)}}{1-\cos(1)}\right]=\frac12\left[\frac{1-\cos(1)-\cos(m)+\cos(m-1)}{1-\cos(1)}\right]=\frac12\left[1+\frac{\cos(m-1)-\cos(m)}{1-\cos(1)}\right].$$ Also, $$\sin(n)=\frac{e^{in}-e^{-in}}{2i},$$ so $$\sum_{n=0}^{m-1}\sin(n)=\frac1{2i}\left[\sum_{n=0}^{m-1}(e^i)^m-\sum_{n=0}^{m-1}(e^{-i})^m\right]=\frac1{4i}\left[\frac{(1-e^{im})(1-e^{-i})-(1-e^{-im})(1-e^i)}{1-\cos(1)}\right]=\frac1{4i}\left[\frac{1-e^{-i}-e^{im}+e^{i(m-1)}-1+e^i+e^{-im}-e^{-i(m-1)}}{1-\cos(1)}\right]=\frac12\left[\frac{\sin(m-1)-\sin(m)+\sin(1)}{1-\cos(1)}\right].$$ Therefore, $$f(\alpha+m)=f(\alpha)+\frac{\sin(\alpha)}2+\frac{\sin(\alpha)[\cos(m-1)-\cos(m)]}{2[1-\cos(1)]}+\frac{\sin(1)\cos(\alpha)}{2[1-\cos(1)]}+\frac{\cos(\alpha)[\sin(m-1)-\sin(m)]}{2[1-\cos(1)]}.$$ This can be simplified further. Notice that $$\cos(m-1)-\cos(m)=\cos(1)\cos(m)+\sin(1)\sin(m)-\cos(m)$$ $$=[\cos(1)-1]\cos(m)+\sin(1)\sin(m),$$ hence $$\frac{\sin(\alpha)[\cos(m-1)-\cos(m)]}{2[1-\cos(1)]}=-\frac{\sin(\alpha)\cos(m)}2+\frac{\sin(1)\sin(\alpha)\sin(m)}{2[1-\cos(1)]}$$ while $$\sin(m-1)-\sin(m)=-\sin(1)\cos(m)+\cos(1)\sin(m)-\sin(m)=-\sin(1)\cos(m)+[\cos(1)-1]\sin(m)$$ hence $$\frac{\cos(\alpha)[\sin(m-1)-\sin(m)]}{2[1-\cos(1)]}=-\frac{\sin(1)\cos(\alpha)\cos(m)}{2[1-\cos(1)]}-\frac{\cos(\alpha)\sin(m)}2.$$ Therefore, $$f(\alpha+m)=f(\alpha)+\frac{\sin(\alpha)}2-\frac{\sin(\alpha)\cos(m)}2+\frac{\sin(1)\sin(\alpha)\sin(m)}{2[1-\cos(1)]}-\frac{\sin(1)\cos(\alpha)\cos(m)}{2[1-\cos(1)]}-\frac{\cos(\alpha)\sin(m)}2=f(\alpha)+\frac{\sin(\alpha)}2-\frac{[\sin(\alpha)\cos(m)+\cos(\alpha)\sin(m)]}2-\frac{\sin(1)}{2[1-\cos(1)]}[\cos(\alpha)\cos(m)-\sin(\alpha)\sin(m)]=f(\alpha)+\frac{\sin(\alpha)}2-\frac{\sin(\alpha+m)}2-\frac{\sin(1)\cos(\alpha+m)}{2[1-\cos(1)]}.$$ This works for all $m\in\mathbb{N},$ but exploiting symmetries and antisymmetries with respect to parity, this works for all $m\in\mathbb{Z}.$ Choose some $f$ defined on $[0,1).$ Then $f$ can be extended to $\mathbb{R}$ via the above solution, and it will satisfy the functional equation everywhere. Also, notice that for all $m\in\mathbb{Z}$ and every $\alpha\in[0,1),$ there exists some $x\in\mathbb{R}$ such that $m=\lfloor{x}\rfloor$ and $\alpha=x\;\mathrm{mod}\;1=x-\lfloor{x}\rfloor.$ Therefore, $x=\alpha+m,$ and so $$f(x)=f(x\;\mathrm{mod}\;1)+\frac{\sin(x\;\mathrm{mod}\;1)}2-\frac{\sin(x)}2-\frac{\sin(1)}{2[1-\cos(1)]}\cos(x).$$ This solution determines $f$ uniquely up to its determination on $[0,1)$ as a solution to the functional equation. All that is required for further unique determination is $f(x\;\mathrm{mod}\;1).$
To finish this off, notice that $$\frac{\sin(1)}{1-\cos(1)}=\cot\left(\frac12\right),$$ and so $$-\frac{\sin(1)}{2[1-\cos(1)]}\cos(x)=-\frac{\cot\left(\frac12\right)\cos(x)}2=\frac{\cot\left(\frac12\right)}2-\frac{\cot\left(\frac12\right)\cos(x)}2-\frac{\cot\left(
\frac12\right)}2$$ $$=\cot\left(\frac12\right)\left[\frac{1-\cos(x)}2\right]-\frac{\cot\left(\frac12\right)}2=-\frac{\cot\left(\frac12\right)}2+\cot\left(\frac12\right)\sin\left(\frac{x}2\right)^2.$$ Therefore, $$f(x)=f(x\;\mathrm{mod}\;1)+\frac{\sin(x\;\mathrm{mod}\;1)}2-\frac{\cot\left(\frac12\right)}2-\frac{\sin(x)}2+\cot\left(\frac12\right)\sin\left(\frac{x}2\right)^2.$$ Finally, let $$C_1(x\;\mathrm{mod}\;1)=f(x\;\mathrm{mod}\;1)+\frac{\sin(x\;\mathrm{mod}\;1)}2-\frac{\cot\left(\frac12\right)}2,$$ and thus $$f(x)=C_1(x\;\mathrm{mod}\;1)-\frac{\sin(x)}2+\cot\left(\frac12\right)\sin\left(\frac{x}2\right)^2.$$ This is precisely the solution in your post, although in your post, it is notated sloppily, since it is not specified that $C_1$ is an arbitrary function $[0,1)\to\mathbb{R},$ and it instead suggests that $C_1$ is some arbitrary real number. Anyway, $f$ solves the equation, and this is the complete family of solutions.