Consider the two-point function $$ \langle\mathcal{O}_1(x_1)\mathcal{O}_2(x_2)\rangle=f(x_1,x_2) $$ If the operators are in a CFT, we can constrain this function using the symmetries of the theory. Using translational symmetries and the symmetries of the Lorentz group we have $$ f(x_1,x_2) = f(X_{12}) $$ where $X_{12} := (x_1-x_2) $
When we impose dilatation symmetry we get $$ \langle\mathcal{O}_1(x_1)\mathcal{O}_2(x_2)\rangle=\frac{C_{12}}{|x_1-x_2|^{\Delta_1+\Delta_2}} $$ where $\Delta_1,\Delta_2$ the dilatation weights of the operators.
Now if we impose special conformal symmetries we have$$ \left(-2x_{1\mu}\Delta_1-2x_{2\mu}\Delta_2+k_{1\mu}+k_{2\mu}\right)\frac{C_{12}}{|x_1-x_2|^{\Delta_1+\Delta_2}}=0 $$ If we make use of $$ (k_{1\mu}+k_{2\mu})|x_1-x_2|=-(x_{1\mu}+x_{2\mu})|x_1-x_2| $$ we should be able to derive $$ \langle\mathcal{O}_1(x_1)\mathcal{O}_2(x_2)\rangle=\frac{C_{12}}{|x_1-x_2|^{2\Delta}} $$ for $\Delta_1=\Delta_2=\Delta$ and $0$ otherwise.
I can't derive the final equation from the given identity of $k$'s, is there something else that I'm missing?
Edit:$$ k_\mu=x^2\partial_\mu-2x_\mu x^\nu\partial_\nu $$ The operator associated to special conformal transformations.