How to show the explicit form of rotation operator?

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Suppose $P_R(\alpha) f(x,y)=f(x\cos\alpha +y\sin\alpha, y\cos\alpha-x\sin\alpha)$

How to show that the operator $P_R(\alpha)$ has the form:

$$ P_R(\alpha)=1+\sum_{n=1}^\infty \frac{1}{n!}(-i\alpha)^n l_z^n $$

where $l_z=-i(x\frac{\partial}{\partial y}-y\frac{\partial}{\partial x})$.

I tried to expand the right hand side, but don't know how to collect the terms:

$$ f(x\cos\alpha +y\sin\alpha, y\cos\alpha-x\sin\alpha) =\sum_{m,n}\frac{1}{m!n!}f^{(m,n)}(0,0)(x\cos\alpha +y\sin\alpha)^m (y\cos\alpha-x\sin\alpha)^n $$

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(up to factors of $i$): Start by showing that $l_z = {\partial\over{\partial \alpha}}$ and then show that $e^{\beta {\partial \over {\partial \alpha}} }$ is the shift operator, and satisfies $ e^{\beta {\partial \over {\partial \alpha}} } g(\alpha)=g(\alpha +\beta)$ for smooth enough $g's$. Once you've gotten that far you will notice that $P_R(\alpha)$ is essentially the shift operator.