Finding a function whose double covariant derivative is delta function I have a function $f$ defined as $\frac{\overline{z}-\overline{w}}{(z-w)(1 + z\overline{z})(1+w\overline{w})}$.
I want to prove that $$\partial_{\overline{z}}^2 f + \frac{2z}{1+z\overline{z}}\partial_{\overline{z}}f = \pi \frac{2}{(1+ z\overline{z})^2}\delta(z-w).$$
This is basically a double covariant derivative wrt to $\overline{z}$ taking the metric in unit sphere in stereographic coordinates.
I found that $\partial_{\overline{z}}f = \delta(z-w)\frac{(1+z\overline{z})(\overline{z}-\overline{w})}{1+w\overline{w}} + \frac{1}{z-w}\frac{(1+2z\overline{z}-z\overline{w})}{1+w\overline{w}}$.
If I differentiate again I am encountering a derievative of a delta function which I do not know how to do.
But since I know the result I calculated back what the derivative of delta function should be a found out to be $\frac{2\delta(z-w)}{\overline{z}-\overline{w}}\frac{w\overline{w}-z\overline{z}}{1+z\overline{z}}$.
Basically during the calculation I used the product rule and took $\frac{1}{z-w}$ as one function and rest as another and did the diffrentiation.I also used the fact that $\partial_{\overline{z}}\frac{1}{z-w}=\delta(z-w)$.
I would like to know whether the procedure I have done is correct.Is the derivative of the delta function I have mentioned is correct or not.Pls help me.
This problem is basically involved during computing the BMS charge
 A: Note
$$
D_{\bar z}^2f = \gamma_{z\bar z} \partial_{\bar z}( \gamma^{z\bar z} \partial_{\bar z} f ) 
$$
We are solving the equation
\begin{align}
D_{\bar z}^2f &= \pi \gamma_{z\bar z} \delta^2(z-w)\\
\gamma_{z\bar z} \partial_{\bar z}( \gamma^{z\bar z} \partial_{\bar z} f ) &=  \pi \gamma_{z\bar z} \delta^2(z-w) \\
\partial_{\bar z}( \gamma^{z\bar z} \partial_{\bar z} f ) &=  \frac{1}{2} \partial_{\bar z} \frac{1}{z-w} \\
\gamma^{z\bar z} \partial_{\bar z} f  &=  \frac{1}{2} \frac{1}{z-w} + g ( z,w,\bar w)\\
\partial_{\bar z} f  &=  \frac{1}{2} \frac{\gamma_{z\bar z} }{z-w} + \gamma_{z\bar z}  g( z,w,\bar w)
\end{align} 
Note that we have
$$
f = \frac{ \bar z - \bar w}{ (z-w)(1+z\bar z)(1+w\bar w)}
$$
so that
$$
\partial_{\bar z} f =  \frac{ 2\pi \delta^2 ( z - w )( \bar z - \bar w )}{  (1+z\bar z)(1+w\bar w)}   +   \frac{1}{2} \frac{\gamma_{z\bar z} }{z-w} + \frac{1}{2} \gamma_{z\bar z} \frac{ \bar w }{ ( 1 + w \bar w ) } 
$$
The first term is zero. The rest of this is precisely the of the required form.
