Fourier optics with concave (diverging) lenses

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SUMMARY

The discussion centers on the behavior of concave lenses in Fourier optics, specifically regarding the location of the Fourier transform in relation to virtual focus planes. It is established that for concave lenses, the Fourier transform occurs in a virtual focus plane, contrasting with convex lenses where it occurs in a real focus plane. The participant concludes that when using a concave lens in conjunction with a convex lens, the original field function cannot be recovered due to the divergence of light rays from the concave lens. This highlights the limitations of using concave lenses in Fourier optics setups, particularly in 4F systems.

PREREQUISITES
  • Understanding of Fourier optics principles
  • Knowledge of lens types: concave and convex lenses
  • Familiarity with diffraction integrals
  • Experience with ray diagram analysis
NEXT STEPS
  • Study the mathematical foundations of diffraction integrals for concave lenses
  • Research the applications of 4F systems in optical setups
  • Explore experimental methods for observing Fourier transforms with concave lenses
  • Learn about the implications of virtual focus planes in optical systems
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Optical engineers, physicists, and students studying Fourier optics who are interested in the practical applications and theoretical implications of concave lenses in optical systems.

Qiao
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Hey,

I was wondering, since for a convex lens the Fourier transform of a fields is in their real focus plane. Is it for a concave lens that the Fourier transform of a field is in the virtual focus plane?

I can't find any book or paper that talks about how concave lenses work in terms of Fourier optics.
 
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There's no conceptual difficulty- the only difference is using '-f' instead of 'f' in the diffraction integrals. The practical difficulty is that the planes of interest are virtual, rather than real.
 
Thanks. So then I would assume that if the object is at focus distance "f", the image plane with a perfect Fourier transform of the object will be at "f/2". I concluded this by drawing a quick ray diagram.
 
actually, I've thought about this some more with the following thought experiment. Take a concave lens, put an object on the left focal plane, next place a convex lens so that it's focus plane is at the virtual image plane of the concave lens. So now the second lens should in principle do another Fourier transform giving back you original field function, right? (this is based on the 4F system in the link without the transmission mask http://upload.wikimedia.org/wikiped...4F_Correlator.svg/430px-4F_Correlator.svg.png)

But if you draw a ray diagram, it would tell another story, for a collimated beam everything goes as expected they enter collimated and exit collimated.
But for a point source, when it passes the concave lens it diverges even more and all the information will never be refocused back to a point. This means that it is impossible to get your original function back, right?

This is confusing to me, this experiment contradicts the idea that the Fourier transform lies in the virtual planeo_O:confused:
 
Seems to me, all you are describing is a telephoto lens which can be used forwards or backwards to magnify or demagnify.
 
It is sort of a basic telescope setup. Except I don't expect go to get my function back when if I use a concave lens + convex lens.
 
I have been thinking of this problem for a while now and like you guys, i have not found much online on this topic. From ray diagrams, all I can make out is that we do not have access to the intermediate Fourier plane in a 4f system built using a convex and a concave lens. So effectively it is magnifying or diminishing lens combo. You already know this. I tried to experimentally observe this once but I was not successful. I must admit it was not a sincere effort. I will try again to do this experiment and let you guys know.
 

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