I think this is consistent with what I was suggesting. To be clear, I am not even attempting to correct John here, and if at any point I stumble in the right direction, it is by no means through any real expertise like he has, and corrections are welcome 😆
But, the reason I think it might help a bit, is because yes, energy remains the same, but the energy is spread over a larger area. Probably the closer the reflecting surface on the filter is to the sensor, the more severe the reflection artifact will be in the image. 3mm probably wont be a game changer, but better to have the filter as far away as possible and deal with bigger but fainter spots than smaller but stronger ones.
There are a couple of other things not in the diagram that I think are in play. The sensor window and the microlenses.
Suppose the filter is perfect in terms of blocking and is not leaking any NIR light. What I think will happen is that the incoming light will hit the sensor, and reflect back through the microlenses (little domes over the pixel photosites), up to the sensor window. The light that reflects directly out at 0 degrees will pass through the filter again, out the top of the scope.
But, because the microlenses are domes (this is to catch light that is heading towards the area between pixels, and angle it back into the pixel), it’s actually going to reverse that reflect some light OUT at all different angles.
When that returned light travels towards the filter, the steeper angles are going to blue shift outside of the narrowband, turning that filter into a mirror. Then it comes back down onto the sensor again.
The more I think about it, the less I feel like the IR leakage would have enough energy to cause the multiple artifacts. It would definitely contribute to halos. But intuition is that it would need a LOT of energy to penetrate that weak spot at 710nm and reflect back through the microlens, the filter window, and hit the sensor again.
If it’s purely the off-axis reflection caused by the microlenses, I think the only mitigations are:
Wider bandpass, to tolerate eviction of more of the reflected angles
Larger spacing, as mentioned above, to diffuse the effect over larger area
Actually, a second advantage with larger spacing could be more of the steeper reflection rays terminating on a wall, and not hitting the filter to bounce back at all (John’s example might not account for this? But it might be negligible)
A better AR coating on the sensor window. I don’t know much about those, but I think they target a specific wavelength and are akin to phase cancellation, but I’m really talking out of my ass here. I seem to remember looking into it at one point and concluding that it’s likely a dead end as far as a fix goes for the extremes involved with astro. I think I remember someone else posting that they tried removing the window entirely and seeing no difference, and if it was helping, one would expect the artifacts to get worse?
All this to say, my only slighty-above-layperson level of knowledge does not see a solution here. It’s very interesting that John’s ONAG doesn’t show it though.
I think with the right math you could actually calculate whether or not a potential NIR leak is contributing, based on both the spacing of the artifacts, and the relative difference in energy making it through the filter vs the adjacent signal. There could be something else about the ONAG that is mitigating it too.