Hey thank you so much for this short course, it's a blessing being able to watch this for free !
@DeepakKumar-lo9lk2 жыл бұрын
Best video on KZbin for Fourier Optics
@JoelRTLCosta11 ай бұрын
Thank you for the classes!
@vladi21k2 жыл бұрын
Thank you for your video, it was very helpful and it inspired me with new ideas how to teach my graduate class. However please note that by performing the Fourier transform, it doesn't mean that lens do something fundamentally different to imaging. In fact, it can be shown with Fourier optics that the lens does imaging by converting frequency information (sum of plane waves incoming from different directions) to spatial information, proportional to the amplitude of the plane waves (imaging).
@eunsjun65823 жыл бұрын
You saved my life.
@vintech885 жыл бұрын
Thank you for the video Can you explain the spatial frequency in detail and little intuitive, my mind somehow not accepting these terms
@JordanEdmundsEECS5 жыл бұрын
Yeah, it’s a very challenging concept, I’ll probably make a few videos on it. If you understand frequency in time you can think of it in exactly the same way:
@thejll3 жыл бұрын
Nice! Might you do the 4f correlator one day? How a Lyot stop works?
@MM-vw1ck3 жыл бұрын
So what you're saying is, one can cure Gout just by simpy computing a fourier transforkm?
Phase transformation by the lens between g- and g+ . Where can I study such transformation by optical components like convex and concave lens? Thanks
@shihansajeed21103 жыл бұрын
that's an amazing video. thank you
@gamebm2 жыл бұрын
Many thanks for the excellent classes. I have a question, is there any way to show that at the high-frequency limit (Eikonal limit), the Fourier optics also leads to the Lens maker's equation?
@brianma875 Жыл бұрын
What if I cascade 2 lenses with a distance in between? I can't cancel the term which represents the propagation between 2 lenses. I'm doing something wrong or it just don't work for 2 lenses apart from each other? If that's the case, the objectives of a microscope can't be treated as a Fourier lens.
@nohaivce26144 ай бұрын
@brianma875 Hi, if I understood your question correctly, you might want to look into a 4f-system which describes this problem. tldr it's a reverse fourier transform by the second lens
@brianma8754 ай бұрын
@@nohaivce2614 Oh I mean the second lens is placed at a distance shorter than the focal length of the first lens. I'm doing this because I wish to get an adjustable joint focal length of those lenses by changing the distance between them.
@nohaivce26144 ай бұрын
@@brianma875 Hi, something that comes up for me as an idea when you say 'joint focal length' is using 2 lenses still in the focus of each other, but with different focus lengths each (so effectively it turns from a 4f into a 2*f_1 and 2*f_2 system. This would have the same effect as 4f where at the end-screen after the second lens you get a inverse fourier of the Fourier after the first plane, but with different size of the image. You can use ABCD law to get the magnification and other properties of this system.
@nohaivce26144 ай бұрын
@@brianma875 However, of course if you want to place the second one out of focus you can. I came across it being briefly discussed in J. Peatross' and M. Ware's Physics of Light and Optics in Section 11.1. As far as I udnerstood you can use Fresnel Prop. from aperture to the first lens, from the first lens to second and then get the Fraunhofer field of that in the focus of lens 2.
@abharadwaj68144 жыл бұрын
Thanks Jordan! I've a question. Suppose the object is placed at a distance greater than F from the lens, and the screen is placed at the imaging distance (as found out by lens equation) does g_out(x_image) = fourier transform of g_in(x_obj) ?
@JordanEdmundsEECS4 жыл бұрын
No, imaging is not the same (unfortunately) as the Fourier-Transforming property of a lens. For a FT you need to place both object and plane exactly 1f from the lens. For imaging, this would be 2f.
@marlonsaveri2 жыл бұрын
Suddenly a Ks appeared. What is Ks?
@poutineausyropderable71082 жыл бұрын
Isn't there a problem with the propagator. Isn't it. e^(ikf -ikx^2/2k) You're off by a facor of e^ikf. Which is a constant. Got it