You can predistort for Q enhancement, but you run the risk of tempco effecting the filter.
If you go for a ladder approach, the localized Qs tend to be lower. I'm not sure if localized Q is a generally accepted term, but I learned it from Dan Senderovich. The idea is every node is a filter, even if only one node has the desired frequency response. If you examine the response at intermediate nodes of a cascade of biquadratic sections versus the nodes of a ladder, the ladder "localized" Q is lower. I don't believe there is a strict proof of this, but anecdotal evidence shows this.
The other advantage to a ladder is that the all the components interact in a manner where the sensitivity to an individual component is reduced.
Senderovich is quite the guru at this. I learned how to do bandpass and highpass ladders from him, something textbooks don't cover. His approach is totally signal flow graph. In fact, if you want to ponder dynamic range adjustment, signal flow graph is the way to go.
In ladder design using signal flow graph, the upper nodes represent voltage, and physically are op amp outputs. The lower nodes represent current. Going from the upper nodes to the lower nodes is done with integrators (physically an op amp with a cap as feedback, positive input to ground if single ended.).
Say the node is peaking. To dynamic range adjust a filter as shown on the signal flow graph, you scale down (attenuate) all the paths entering the node, then scale up (amplify) all the paths leaving the node. If you do this, the final output of the signal flow graph has remained unchanged.