We are dealing with the Brocard angle. Notice that, by the trigonometric form of Ceva's theorem,
$$ \sin(\omega)^3 = \sin(A-\omega)\sin(B-\omega)\sin(C-\omega). \tag{1}$$
Use the sine addition formulas to write the RHS of $(1)$ as a sum of sines, then write $\sin(A)$ as $\frac{2\Delta}{bc}$ and $\cos(A)$ as $\frac{b^2+c^2-a^2}{2bc}$. Do the same for $B$ and $C$ and that will lead to:
$$ \cot(\omega) = \frac{a^2+b^2+c^2}{4\Delta}=\cot(A)+\cot(B)+\cot(C).\tag{2} $$
You may prove the same by proving first that the trilinear coordinates of the Brocard points are
$$\left[\frac{b}{c};\frac{c}{a};\frac{a}{b}\right]\quad\text{and}\quad \left[\frac{c}{b};\frac{a}{c};\frac{b}{a}\right]. \tag{3}$$