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On a 2n-dimensional phase-space with coordinates $x$ and $p$, the Moyal product can be written explicitly as

$$g(x,p) \star h(x,p) = g(x,p) e^{\frac{i}{2}\left( \overleftarrow{\partial_x} \cdot \overrightarrow{\partial_p} - \overrightarrow{\partial_x} \cdot \overleftarrow{\partial_p}\right)} h(x,p) \, .$$

Assume now that we have something like $f(x,p)=g(x,p)\star h(x,p),$ where we have to solve for $g(x,p)$. I suppose it's not always possible, but how would one go about solving that when it is? And what would the invertibility conditions even be? I can't seem to find the answer anywhere.

Maybe even a simpler problem, $f(x,p)=g(x,p)\star g(x,p) $ with $f(x,p)$ known. How would one take the $\star$-square root and when would it be possible?

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The inversion is conveniently described in terms of the Fourier transform $$g(x,p)=\int dy\,e^{-iyp}G(x+y/2,x-y/2).$$ Then the composition $f(x,p)=g(x,p)\star h(x,p)$ is a matrix multiplication [1], $$F(x,y)=\int dz\, G(x,z)H(z,y).\qquad(\ast)$$ So to find $h$ if $f$ and $g$ are given one would first calculate the Fourier transforms $F$ and $G$, $$G(x+y/2,x-y/2)=\frac{1}{2\pi}\int dp\,e^{iyp}g(x,p),$$ then solve the integral equation $(\ast)$ for $G$, and finally transform back to $g$. Whether this is doable will of course entirely depend on the details of the particular problem. But this is the general recipe.

[1] Map of Witten's $\star$ to Moyal's $\star$, Itzhak Bars, 2001.

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  • $\begingroup$ Ah, of course, very nice! Thank you. $\endgroup$
    – lel
    Commented Jul 25, 2018 at 19:50

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