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We study the asymptotic response of polar ordered active fluids (“flocks”) to small external aligning fields . The longitudinal susceptibility diverges, in the thermodynamic limit, like as $h \rightarrow 0L\chi_{_\parallel}\sim L^\gamma\nu\gammad$, and are related to the dynamical exponent and the “roughness exponent” characterizing the unperturbed flock dynamics. Using a well supported conjecture for the values of these two exponents, we obtain , in and $\nu = 1/4\gamma = 2/5d = 3$. These values are confirmed by our simulations.

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