The Fix: Design for the Cone
If the working focal ratio is known in advance, the collimated center wavelength can be placed deliberately to the red side of the target line. The fast cone then shifts the band down onto the line on purpose, using the same coating physics that causes the problem in the first place.
Image: same bandwidth, same focal ratio, same emission line. The only difference is whether the filter was designed for the cone.
+27 pts more Hα signal at f/3, at the same 3 nm bandwidth, when the filter is optimized for that focal ratio
An f/3-optimized design holds about 99% on-line transmission through f/3 and 92% at f/2.5. Optimization is tuned to a target focal ratio, not a universal fix at every speed, so the practical move is matching the design to the focal ratio actually in use, not the telescope's native ratio. Focal reducers and correctors change the working ratio the filter sees.
The shift also scales with wavelength. At f/3, Hβ and OIII move about 0.7 nm, while Hα and SII move about 1.1 nm. In an SHO set, Hα and SII carry more focal-ratio risk than OIII.