The booster board will also increase the O2's slew rate.
I added some information about that to the build instructions at the Google Drive link yesterday after the good discussion in this thread made me realize that was another benefit of the board I had forgotten about.
The O2's orginal NJM4556A's have a slew rate of 3V/uS while the NJM2068 gain chip is 6V/uS from the datasheets. The NIM4556A would be the limiting factor end-to-end in the O2 amp then, giving an O2 amp slew rate of around the 3V/uS.
[snip]
The O2's designer had a good point about slew rate in his blog. He notes real world audio sources don't slew much faster than 0.6V/uS and the signal processing chain at the studios has similar limitations. So he doubled that to around 1.2V/uS just to be safe, if I'm remembering correctly, then noted the NJM4556A's 3V/uS is still about twice that making it more than adequate in his view. He also noted the only downside to more slew is the potential for oscillations from a badly designed circuit. I've measured the booster out to 200mHz so that isn't a problem here.
On the other hand there is that link to a good writeup on slew that was posted a few posts ago. That author makes similar remarks to the O2 designer about real world source slew limitations, but then goes on to say something like "that is for 20kHz but well designed amplifiers are usually designed to be flat out to 100kHz, requiring a slew of 10V/uS" (paraphrased) and goes into some supporting detail. So there are certainly other interesting opinions about how much slew is needed and why.