= Two-dimensional flat-target Derrick obstruction
For smooth fields into $\mathbb R^l$ with nonnegative differentiable potential and finite energy, <Derrick scaling> in two spatial dimensions forces the potential integral to vanish. Thus the field takes values where $U=0$ and $\nabla U=0$, so its static field equation makes every component harmonic. Each first derivative is an entire harmonic function in <L2 space>; the mean-value inequality on arbitrarily large balls forces it to vanish. Hence the field is constant. The scale identity alone does not exclude a pure-gradient model; this additional argument uses the flat unconstrained target. Curved-target <harmonic maps>, for example the <O3 nonlinear sigma model>, can instead have finite-energy nonconstant solutions.
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