Fourier optics with concave (diverging) lenses

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Discussion Overview

The discussion revolves around the behavior of concave lenses in the context of Fourier optics, particularly how they relate to the Fourier transform of optical fields. Participants explore theoretical implications, practical challenges, and experimental setups involving concave and convex lenses.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Experimental/applied

Main Points Raised

  • One participant questions whether the Fourier transform of a field with a concave lens occurs in a virtual focus plane, contrasting it with the behavior of convex lenses.
  • Another participant suggests that the only difference in the diffraction integrals for concave lenses is the use of '-f' instead of 'f', noting that the planes of interest are virtual.
  • A different participant proposes that if an object is placed at the focus distance "f", the image plane with a perfect Fourier transform would be at "f/2", based on a ray diagram.
  • One participant presents a thought experiment involving a concave lens followed by a convex lens, questioning whether the original field function can be recovered, and expressing confusion about the implications of ray diagrams for point sources.
  • Another participant compares the setup to a telephoto lens, suggesting it can be used to magnify or demagnify, but expresses skepticism about recovering the original function with the lens combination.
  • One participant reflects on their attempts to experimentally observe the behavior of the lens system, noting challenges in accessing the intermediate Fourier plane in a 4f system with both lens types.

Areas of Agreement / Disagreement

Participants express varying viewpoints on the implications of using concave lenses in Fourier optics, with no consensus reached on whether the original field function can be recovered or the nature of the Fourier transform in this context. The discussion remains unresolved with multiple competing perspectives.

Contextual Notes

Participants highlight limitations in available literature on the topic and acknowledge challenges in experimental setups, particularly regarding the access to intermediate Fourier planes in lens 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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