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We restrict ourselves to statistical invariance under rotations but not necessarily under reflections.
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The energy densities decay exponentially at large wave numbers in the far-dissipation range. We have therefore assumed convergence of the integrals appearing in Eqs. (11)-(14), which appears reasonable considering the presence of a naturally occurring viscous cutoff at large wave numbers.
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There is a typographical error in the equations given in Ref. [12]. This does not affect their results. We have corrected this error in Eq. (15).
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