Something to remember with transformers is the self inductance, leakage and self capacitance (or transmission line length in this case), and interaction with circuit capacitances (mainly the transistor itself here). And since you have two cascaded, the same applies to input, middle, and output ports.
The thing that stands out to me is the completely unloaded collector, at certain frequencies. U2C for example resonates with Q2 Ccb, which also feeds back to the input (Miller capacitance). Now, magnetizing inductance is surely handled by emitter feedback (for which R9 acts as termination), but there could still be a mode with leakage where the collector has high voltage gain and wild phase shift, acting somewhat (if not entirely?) outside of feedback mechanisms.
The important part about such a mode is, it's also a path. If it's U2C leakage against the other windings, then a voltage rise there corresponds to a current rise elsewhere; it could therefore be handled by some impedance above U2C (so, add ESR to C8, more or less?), or below U2A or B. These would be alternatives to an R+C from collector to GND (the most obvious way to dampen a ringing capacitance).
And yes, some of these already have impedance -- that is, the bottom end of U2C has high impedance (well, except for Ccb), the top end of U2A has impedance, surely impedance at the other end doesn't matter? Well, keep in mind there is a common mode element to the transformer. It's not ideal, there is leakage and capacitance between windings, so it can matter which end has what impedance.
"Neutralization" could also be applied, i.e. some impedance C-B. I use quotes, because a typical form is simply an R+C here, which basically kills gain above the cutoff frequency, not really neutralizing in the sense of cancelling capacitance or correcting phase shifts. But that can do well enough anyway.
Now, I don't have this thing in front of me, I'm not probing it and testing which of these mechanisms is at play; and I don't have a good feel for the typical behavior of an emitter-feedback circuit like this. So several of these might be completely off base. This is more just to give some ideas to think about how it's behaving.
Also keep in mind, any given resonant mode has some characteristic frequency defined by its elements. Example: say leakage (U2C referred) is 100nH, Ccb is ~5pF: they should resonate around 225MHz -- probably too high to be the culprit in question. You can use the frequency or time constant to trace things around as well.
(My guess for 25MHz, being in the passband more or less, but towards the high end, is stray capacitance over the board, coupling just enough feedback to make it oscillate. This would also be touch-sensitive, since touch disturbs the E-field over the board. If not, perhaps it's a local feedback thing, and neutralization would do the best.)
Another thing that might help is, notice the inter-stage impedance is poorly defined. The base input impedance is quite high due to emitter degeneration; collector output is basically Early effect, negligible compared to even core loss I'd guess. This might give you very high gain, but it also makes an easy node for crosstalk or oscillation to be introduced.
A stability analysis should be able to show up any oscillation, or potential thereof, and, keep an eye on the transfer function too (peaks may suggest potential instability).
An "unconditionally stable" amplifier means no oscillation for any input *or* output impedance (anywhere on the half-plane of the Smith chart); this would obviously be a pain to test exhaustively, but there are methods to determine it from s parameters or what have you.
Cheers!
Tim