While I don't have an argument with the general concepts described, I do think there is likely more to the impact dynamics than "sometimes it just happens that way".
I never said or implied what you put in quotes, in fact, quite the opposite. Further research
is needed, the point is to evaluate which additional factors
could and
could not influence the nature of the ejecta. But, as discussed further below, I think you are getting closer.
The focusing of the secondary bombarding objects in two tight streams does not seem to be consistent with other observations of lunar impacts, nor with the 3D simulations.
I reiterate that you're too categorical on both instances.
Have you looked at the examples of other lunar impacts I have given to @who knows? You'll see examples of other tight streams. In fact, basically all ejecta blankets show strong anisotropy with rays. The canyons radiating from the Schrödinger Basin are special as a matter of
degree, not of
quality.
You can also see two tight streams of high-speed ejecta (even separated from the rest of the ejecta in their ballistic path) in some of the 3D-simulated scenarios (as well as more complex patterns with more than two such streams). What does not match the two canyons radiating from the Schrödinger Basin is the
exact pattern (especially the angle relative to the crater).
But, I think that there could be more than one part to the impactor. And I wonder whether a trailing part or parts could be deflected or cause shock waves in the already raised ejecta to deflect the secondary impactors to be separated at the angle observed while still not scattering them more than is observed.
Yes, you are getting closer to an understanding of what should be looked into. But you are still trying to break it down into the interplay of a very limited number of distinct objects or events, instead of thinking of waves travelling in a continuous medium.
At shallow impact angles, the shock wave is certainly shaped into something more complex than an expanding oval by the subsequent impact of subsequent parts of the impactor. But your earlier scenario of the impact of a contact binary is the only case where you can even
approximate that as the subsequent impact of two point objects. More realistically, we can say that there will be a continuous generation of shock waves with changing intensity over the 2-3 second duration of the impactor's demise (in the case of the Schrödinger Basin).
The crater excavation process, that is the launch of the ejecta by the shock wave, will continue on for several more seconds. So the timescales are different; basically no part of the blasted-out ground has yet turned ballistic by the time all of the impactor made contact.
So, instead of some direct association with parts of the impactor, you can think of the ejecta anisotropies as the result of interference patterns emerging in the shock wave. You could then think of possible factors that can produce very pronounced interference patterns.
With the above in mind, both of your original ideas can be adapted for something more realistic. Your contact binary idea was already a good replacement for the earlier asteroid-breaking-in-two hypothesis. Note however that there are more freedoms to explore in simulations if you think of interference patterns: it may be that a contact binary impacting with the two parts at the same time (with the axis through the two parts parallel to the ground and perpendicular to the impact direction) can produce the pattern we need.
As for your surface-feature does-focusing hypothesis, instead of that, inhomogeneities in the material properties of the blasted-out ground (say a large deep lava flow or just the deformed basin rocks of a prior giant impact) could very well cause the shock wave to travel at slightly different speeds in different directions, with a focusing end result.
Both ideas worth studying in additional research, IMO.