This graph is the refractive index for water. The function of refraction index is not as simply dependent on wavelength as you are suggesting. The shape of the curve depends on the medium material, among other things. I hadn't considered dispersion before this conversation, and I appreciate your input, but I've already said that the function of refractive index by wavelength through spacetime could simply be a constant (i.e. not dependent on wavelength at all). The Einstein Lens could be proof of this. If you aren't satisfied with this response that's OK, but I'm not sure any further commentary on this topic is constructive.
This can't be true. Instead of peaks and troughs, imagine tennis balls. Observer A hits a ball down towards B every second, and numbers them. If observer B is receiving these tennis balls at a higher frequency than 1 per second (from A's perspective) then he would be receiving tennis balls not even served yet. We rectify this by allowing A to claim that the frequency is the same but the wavelength (i.e. distance between tennis balls) is shorter for B -- and it would literally look like that to A because hitting tennis balls into a field of dilated time is like hitting them into a puddle of syrup. The frequency remains constant, but the wavelength shortens. (Wavelength) * (frequency) = (c) locally, and (wavelength at B from A's perspective) * (frequency at B from A's perspective) = (c at B from A's perspective) which means that light is moving more slowly at B from A's perspective.
I did my best to explain my perspective on cavity interactions. If you think we still harbor a difference of opinion then I would agree that further discussion isn't going to be meaningful. Thanks though, Joigus.
With these objections, it makes me question the function of gamma and GR time dilation in general. Is it only useful relative to two points in spacetime? Is time dilation represented in the field equations? Can we derive even derive a complete, universally valid time dilation field in GR?