synch said:
So images seen through a oxygen(III) filter are only seeing the photosphere hotter oxygen, with the bulk main emission being absorbed by the upper layers?
Well, it's a combination of that, along with the very, very narrow bandwidth of the etalon.
By the way, I made a mistake in my last post regarding the bandwidth of a typical etalon. Originally I stated that they are typically a few nanometers in bandwidth, but what I should have said is that they are typically a fraction of an angstrom in bandwidth. That's very narrow.
As you know, if you shine white light through a cold gas you'll see absorption lines in the spectrum. We see this with the sun. But these absorption lines are smeared out somewhat due to the Doppler shift of the gas moving around at or near the "surface" of the sun (by "surface," of course I don't mean a solid surface, rather I mean the photosphere).
But if you observe the sun without an etalon, instead looking at the broad spectrum, you won't see much contrast since the black body spectrum totally dominates, washing out any effect of any Doppler shift. (
@Baluncore mentions this in the above post.)
Figure 1. White light solar viewing. You'll still be able to see sunspots, but the contrast on the photosphere is nothing to write home about.
Now consider viewing the sun with an etalon that blocks out nearly all the sun's light with the exception of less than 1 angstrom of bandwidth, centered right around one of the absorption lines.
If a particular part of the sun's surface (and surrounding gas) produces an absorption line smack in the middle of the etalon's passband, that portion of the sun will appear a little bit dimmer. That's because that wavelength of light was absorbed in that portion of the sun, and etalon blocks out all the other wavelengths, so there isn't as much that gets through to the eyepiece or camera (relatively speaking).
Now consider a different portion of the sun's surface that's moving toward or away from you. That absorption line is now shifted, possibly outside the etalon's passband. That means that the light at the etalon's passband wavelength
isn't blocked by the cooler gas. So that portion of the sun appears relatively brighter.
Figure 2. H-Alpha Solar Viewing. Here you can see a big boost in contrast. By the way, I'm sure the orange color in the photo was added in post processing; I'm guessing the image was obtained using a monochrome camera. The contrast is what's important here, not the orange color.
Etalons are commonly tunable, like with a dial or knob or whatnot, allowing you to tune into just the right Doppler shifted absorption line to get the most contrast of whatever feature on the sun you're interested in at that particular time. They're also very expensive.
(Images grabbed from Lunt Solar Systems,
https://luntsolarsystems.com/)