Restore optimal cubic L2 convergence for pressure-robust Taylor–Hood elements
Determine a remedy that restores the cubic L2-velocity convergence rate for the pressure-robust Taylor–Hood finite element family, whose commuting-diagram-constrained Nédélec interpolation currently causes a loss of one convergence order relative to the standard non-pressure-robust method.
References
In the $L2$ norm, however, we only get the bound
|u-u_h|{L2} \lesssim h2\,(h|u|{H3}+|\Delta u|_{H2}),
which is only quadratic, one order below the cubic rate of the standard, non-pressure-robust $P2P1$ method: the term $\nu(\Delta u - N{0}(\Delta u), Q{1} w)$ - following the same steps as in the proof of \Cref{thm:mini_l2} - is now only of order $h2$ by \Cref{prop:consistency_low}. Since $N{k-1}$ is tied to the pressure space by the commuting diagram, no choice of $k$ can improve on this loss of one order for the Taylor--Hood family. So far we have not been able to find a remedy for this, and we leave it as an open problem.