Hi @tt33 , thanks for the compliments. FYI I have not personally used Roon PEQ, however there may be others on the Forum who have? Nevertheless I can confidently claim to understand what Roon PEQ is trying to do because since your posting I have been busy reading the manual and some online guidance for Roon PEQ.
In summary, the difference between Linn Space Optimisation and practically all other room compensation or correction methods is the Linn approach of using human hearing and room acoustics theory and computational modelling for room acoustics correction. My understanding is all other methods use microphone measurements. This is the key point that becomes relevant to answering your question:-
In Roon PEQ, it seems one can adjust the Qs of selected filter(s) that one might apply to tame low frequency room modes. But how does one make the choice of the right value or setting of ‘Q factor’ to get the best results? Is it by listening, or is it by measuring using a microphone? If by measuring, what measurement view might we use? Furthermore, if there are a number of modes closely spaced together (as there often are), how are the ‘Q’ values to be set for each separate nulling filter?
For those who have an awareness of the translations between impulse response (time domain) and frequency response (frequency domain), the setting of the ‘Q’ varies the bandwidth of the null of the filter, and correspondingly affects the length of the impulse response in the time domain. Ideally one wants to match the time decay of the filter, with the original extended time decay of the room resonance(s) so that the run time ‘correction’ added to the music, exactly cancels out the resonance in the room.
Linn SO solves all of these questions with the single slider of Flat Frequency vs Short Decay Time. If you set to the slider to give 100% Short Decay Time the correction simply applies the corrective impulse response (representing the best combination of nulls for your room) with the shortest impulse response. Of course this does equate to leaving more energy in the room at the room mode frequencies (with longer decaying room resonances), but that could be the preference for the listener, which is why Linn have done it this way!
I hope the above answers your question?
For your information, Phil Budd (Head of Acoustics and Mechanical Engineering, Linn) has a presentation that I sent him earlier this year describing a method that combines the ‘theoretical’ aspects of Linn SO, with my enhancements by using supplementary microphone measurements and REW analysis.
If you use REW, just respond to this posting and I will explain more how you may better set the Optimisation parameter for Linn SO, other than using your own ears and preference.