We consider the field-theory description of the Skyrme model incorporating quantum fluctuations of a condensed phase. This viewpoint clarifies the usefulness of the model for applications at the physical value of $F_{\pi }$, rather than $F_{\pi }$→∞. By creating covariant field-theory states associated with a translational-dependent condensate, we emphasize the effects of fluctuations and coherence in a calculation of the $q^2$ dependence of the baryon electromagnetic form factor F($q^2$). Using the impulse approximation at large $q^2$, we find the model predicts F($q^2$)∼exp(-‖$q^2$‖/${\lambda }^2$)/q ${}_{}{}^2{}_{}{}^{}$, where λ∼1 GeV is a calculable scale. Appending a pion form factor of O(1/$q^2$), we interpret this in terms of higher-twist corrections, at moderate values of momentum transfer, to a leading term of O(1/$q^4$). The dependence on a regularization scale ${\mu }^2$ and $F_{\pi }$${\mathrm{}}^2$ is such that this result applies for a specified range of $q^2$, ${\mu }^2$, and $F_{\pi }$${\mathrm{}}^2$. However, the detailed results of the calculation are such that the large-$F_{\pi }$${\mathrm{}}^2$ and large-${\mu }^2$ limits do not commute.

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