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Numerical stabilization techniques are often employed in under-resolved simulations of convection-dominated flows to improve accuracy and mitigate spurious oscillations. Specifically, the evolve--filter--relax (EFR) algorithm is a framework which consists in evolving the solution, applying a filtering step to remove high-frequency noise, and relaxing through a convex combination of filtered and original solutions. The stability and accuracy of the EFR solution strongly depend on two parameters, the filter radius  and the relaxation parameter
  and the relaxation parameter  . Standard choices for these parameters are usually fixed in time, and related to the full order model setting, i.e., the grid size for
 . Standard choices for these parameters are usually fixed in time, and related to the full order model setting, i.e., the grid size for  and the time step for
  and the time step for  . The key novelties with respect to the standard EFR approach are: (i) time-dependent parameters
 . The key novelties with respect to the standard EFR approach are: (i) time-dependent parameters 


 and
  and 


 , and (ii) data-driven adaptive optimization of the parameters in time, considering a fully-resolved simulation as reference. In particular, we propose three different classes of optimized-EFR (Opt-EFR) strategies, aiming to optimize one or both parameters. The new Opt-EFR strategies are tested in the under-resolved simulation of a turbulent flow past a cylinder at
 , and (ii) data-driven adaptive optimization of the parameters in time, considering a fully-resolved simulation as reference. In particular, we propose three different classes of optimized-EFR (Opt-EFR) strategies, aiming to optimize one or both parameters. The new Opt-EFR strategies are tested in the under-resolved simulation of a turbulent flow past a cylinder at 





 . The Opt-EFR proved to be more accurate than standard approaches by up to 99
 . The Opt-EFR proved to be more accurate than standard approaches by up to 99 , while maintaining a similar computational time. In particular, the key new finding of our analysis is that such accuracy can be obtained only if the optimized objective function includes: (i) a global metric (as the kinetic energy), and (ii) spatial gradients' information.
 , while maintaining a similar computational time. In particular, the key new finding of our analysis is that such accuracy can be obtained only if the optimized objective function includes: (i) a global metric (as the kinetic energy), and (ii) spatial gradients' information.
 
            