As a general comment, an op amp's rail window is generally not a problem in technical terms. This is a limitation which can be overcome rather easily. I stay reserved and say "generally" because obviously, to increase the overall voltage swing from a +/- 15 V op amp to say +/- 50V or whatever, you will need additional electronics to "translate" the voltages.
This can be a problem, depending on the implementation. For example, if it's a phono RIAA eq/amp stage you are making, additional electronics mean additional noise, exactly what you do NOT want in that case. But if it's a power amp, the little additional noise will be quite insignificant even in absolute terms, let alone in terms of what you gain.
Regarding the slew rate, I'd like to make a comment. The actual slew rate on its own is NOT a problem; calculate what you need for a +/ 12V output swing (typical for +/-15V op amps) at TWICE the max frequency, i.e. not at 20 but at 40 kHz, and you come up with a number of +/- 4.25V/uS, or 8.5V/uS. Thus, say 80+% of modern op amps make the grade hands down.
The problem is not in the sheer value of the slew rate, but much more in the way HOW it has been obtained. It could have been done by biasing the input pair rather high and that's it, or it could have been done by making the whole op amp really fast. Compare say LF357 (first group, FET inputs) with say AD817 (second group, fast all around) and you will notice that the full power bandwidth varies by far more than the slew rate specs would lead you to believe.
In other words, you don't want slew rate as such if it's above 15V/uS, you want a wide bandwidth. OP27, for example, has a slew rate of 4V/uS, but a bandwidth of 60 MHz (sic!), which explains why it sounds great even if it appears to be a slowpoke.
But a high slew rate can be a problem, and a serious one. If it has been achieved by having a wide bandwidth, any such circuit is more and more prone to oscillation than a limited bandwidth one. Also, such cicruits will pick up RF far easier than slower ones. All this means is that to apply properly, they need special consideration and precautions, which includes outlay - exactly what you can't change when modding.
Lastly, what you definitely MUST look at, in my view much harder than the slew rate, is the settling time of the op amp. Yes, we want them to be fast and have good rise times, but by the same token, we want them to settle down as fast as possible once the signal has passes; if they tend to take their time, or overhang, your ambience and spatial information goes out of the window.
Typical op amps have settling times of 2,000 nanosecs, which is long. Better op amps (e.g. OP275) cut this to just 1/10, 200 nanosecs, and really cool cucumbers like AD817, AD825, AD826, etc decrease this further to just 45 nanosecs. 45 nanosecs is 44 TIMES faster than 2,000 nanosecs. Hardly surprising then that AD826AN has such wonderful voicing of ambient and spatial information, if applied properly.
Just a few thoughts.
Cheers,
DVV