To prove the radial symmetry, the method of moving plane is a very useful tool.
But how to do the moving planes for equations like
-\Delta u =|\nable u|^p in B_1,
u=0 on \partial B_1(0).
I doubt it as it relies on maximum principle.
Here he have plenty of constant sols to eq.
Look up the book of Dupaigne eg for refs.
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