A Question about Imaging and PSFs

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In astronomical imaging, the convolution of every point in the image plane with the Point Spread Function (PSF) is only noticeable for bright point sources due to the presence of diffraction artifacts like rings and spikes, which are less visible for dimmer stars as they fall below the detection limit. Extended objects like galaxies and nebulae appear clearer because their features are averaged out, making the images look less blurred despite the underlying PSF effects. Everyday imaging often sidesteps these issues because typical scenes are complex and busy, which disguises optical aberrations and allows for a perception of sharpness with increased pixel count. The optics in consumer cameras are generally not diffraction-limited, and the combination of blurring and compression further masks potential artifacts. Ultimately, the behavior of pixelated imaging systems differs significantly from continuous systems, emphasizing the importance of pixel size relative to the PSF for optimal image quality.
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Hi,

If every point in the image plane is convolved with the PSF, why is it that this is only obvious in certain cases?

Take astronomical imaging: for images of bright point sources (e.g., the brightest stars), we see rings, spikes etc. Why do we not see these features for dimmer stars? Furthermore, what about images of extended objects? Why is it that galaxies and nebulae look fine, and don't look like some sort of blurred mess?

Also, what is it fundamentally about everyday/terrestrial imaging that makes it so that these concerns don't seem to matter at all? Why is it that I can feel confident that more pixels = a sharper image, without having to worry about the actual *optics?* One would think that the miniscule lenses included with ever smaller consumer digital electronics would offer pretty lousy angular resolution.
 
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cepheid said:
If every point in the image plane is convolved with the PSF, why is it that this is only obvious in certain cases?
It's only a problem for diffraction limited images. And only obvious for point on a dark background.
Take astronomical imaging: for images of bright point sources (e.g., the brightest stars), we see rings, spikes etc. Why do we not see these features for dimmer stars?
Because they are below the detection limit for the detector. If only 0.1% of the energy goes into the spikes you might see if for a 6mag star but not a 25mag galaxy.
Furthermore, what about images of extended objects? Why is it that galaxies and nebulae look fine, and don't look like some sort of blurred mess?
They are a blurred mess at the scale < arcsec

Also, what is it fundamentally about everyday/terrestrial imaging that makes it so that these concerns don't seem to matter at all? Why is it that I can feel confident that more pixels = a sharper image, without having to worry about the actual *optics?*
The optics generaly aren't diffraction limited an the scenes are normally confused enough that you don't see them. If you are one of the sad bores on photo forums who look at individual pixels on photos of test charts to prove your camera is best - you will.
One would think that the miniscule lenses included with ever smaller consumer digital electronics would offer pretty lousy angular resolution.
They are pretty bad - but this leads to blurring which combined with the heavy jpeg compression mean you don't see the effects
 
Thank you for the explanations mgb_phys. I just wanted to see if I could trust the physics and apply it to the situation in as straightforward a way as I was attempting to.

I guess for terrestrial imaging, it is, as you said, a question of not ever really having to worry about the kind of angular resolution that you need in astronomy. Nobody worries about why you can't see individual trees in a forest tens of kilometres away. Things look reasonable, like the way you'd expect them to look.

One more thing, if I may. You mentioned that the scenes (obviously much busier than a bunch of bright points on a dark background) are "confused." What exactly does that mean? I have some vague idea that the confusion limit occurs when you're looking deep enough that you see so many sources, it is impossible to distinguish them from the background noise (again speaking in an astronomy-specific context, sorry).
 
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I didn't mean it in a technical sense, I meant that a random background of trees/people etc disguises obvious optical abberation whereas bright point sources on an empty background emphasizes them.
 
Right okay...that makes sense. Thanks for the clarification.
 
cepheid said:
Hi,

If every point in the image plane is convolved with the PSF, why is it that this is only obvious in certain cases?

Take astronomical imaging: for images of bright point sources (e.g., the brightest stars), we see rings, spikes etc. Why do we not see these features for dimmer stars? Furthermore, what about images of extended objects? Why is it that galaxies and nebulae look fine, and don't look like some sort of blurred mess?

Also, what is it fundamentally about everyday/terrestrial imaging that makes it so that these concerns don't seem to matter at all? Why is it that I can feel confident that more pixels = a sharper image, without having to worry about the actual *optics?* One would think that the miniscule lenses included with ever smaller consumer digital electronics would offer pretty lousy angular resolution.

Introducing a discrete detector (pixels) invalidates an optical system from being shift-invariant, so it is not proper to consider imaging as a convolution operation anymore.

That said, if the pixels are smaller than the PSF, one can approximate the system as being linearly shift-invariant. The rings/spikes. etc are diffractive artifacts of the aperture, and depending on how the overall brightness of the image is scaled, the details of dimmer objects can be lost- note that on order to view these artifacts, there is usually blooming present in the central peak. There's no contradiction with imaging points and extended objects- the diffraction artifacts may be lessened by the fact that those "side-lobes" are much dimmer than the center peak, and get washed out by imaging extended objects- the image will simply appear blurry.

Pixelated imaging systems can behave very differently from continuous systems- aliasing is the main effect people recognize, and the key is proper matching of the pixel size to the PSF, something that is accomplished by adjusting the numercal aperture of the system. An excellent resource for this topic is "Analysis of Sampled Imaging Systems" by Ronald Driggers (SPIE proess). But yes, those little cameras in consumer electronics are quite impressive- I wouldn't mind seeing the optical layout.
 
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