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We consider uniformly rotating incompressible Euler and
Navier-Stokes equations. We study the suppression of vertical
gradients of Lagrangian displacement ("vertical" refers to the
direction of the rotation axis). We employ a formalism that
relates the total vorticity to the gradient of the back-to-labels
map (the inverse Lagrangian map, for inviscid flows, a diffusive
analogue for viscous flows). We obtain bounds for the vertical
gradients of the Lagrangian displacement that vanish linearly with
the maximal local Rossby number. Consequently, the change in
vertical separation between fluid masses carried by the flow
vanishes linearly with the maximal local Rossby number.