I guess when you say intuitively you mean
Nah more like that's my gut instinct, without any specific reasoning.
that you visually add the perturbation inside the feedback and observe the result on the output. I see it differently (injecting a signal before the A B blocks and seeing what's coming back) but I look at it with a very abstract view. If it works it's good enough for me
I know that putting it where I put it has a disadvantage, apparently to do it perfectly, I should add the input capacitance of the opamp in the feedback loop. By putting where you suggest I don't know with certainty what the implications are.
It's interesting to think about. I can't really explain my preference, so I resorted to doing a simulation to see the difference (if any), see attached.
I set up three perturbations sources:
A is the place in your schematic
B is where I suggested
C is on the reference input (for getting the closed loop transfer function)
The loop gain transfer functions according to A and B are plotted on top. The closed loop transfer function is plotted on the bottom. You can see loop gain B crosses 0dB around 680kHz with a phase margin of 34 degrees, which agrees with the closed loop gain peaking at that frequency. The loop gain A crosses 0dB at around 9.5MHz with a phase of around 100 degrees, which definitely isn't right. But maybe a different way of calculating loop loop gain is needed when perturbing at A.
By technology I mean, jfet input, bjt opamps,... this kind of things.
Eh, probably not critical unless you're really trying to push bandwidth/noise. I wouldn't go for a JFET-input opamp unless you also provide it a bipolar power supply.
Same question could apply about using a mosfet or a jfet I don't know what are the implications of that
For the power transistor, MOSFETs tend to do much better for these circuits, especially at high power levels. Would only consider BJTs if you need extreme noise/bandwidth (and don't care about the error from base current).