Fourier transform spectroscopy

Click For Summary
SUMMARY

The discussion centers on the relationship between the length of an interferogram and the resolution of the resulting frequency-domain spectrum in Fourier transform spectroscopy. It is established that a longer interferogram leads to higher resolution due to the properties of the Fourier transform and the convolution theorem. Specifically, the Fourier transform of a rectangular function becomes sharper as the width of the rectangle increases, enhancing resolution. This principle is fundamentally linked to the uncertainty principle, which explains the difficulty in distinguishing closely spaced wavelengths in shorter intervals.

PREREQUISITES
  • Understanding of Fourier transform principles
  • Familiarity with the convolution theorem
  • Knowledge of interferograms in spectroscopy
  • Basic grasp of the uncertainty principle in physics
NEXT STEPS
  • Research the mathematical foundations of the Fourier transform
  • Study the convolution theorem in detail
  • Explore the concept of rectangular apertures in signal processing
  • Investigate the implications of the uncertainty principle in spectroscopy
USEFUL FOR

Researchers, physicists, and engineers involved in spectroscopy, particularly those focusing on Fourier transform techniques and resolution enhancement in frequency-domain analysis.

Chemistopher
Messages
2
Reaction score
0
Hey guys,

There is something I have known and applied for a long time, that the greater the length of an interferogram the greater the resolution of the resulting frequency-domain spectrum. But I've never fully understood why, I've always waved it off as something to do with the uncertainty principle because this is what I was told many years ago in secondary school. I've read around and I can't really find a good explanation.

It'd be great if somebody here knew. Thanks :)

Regards,

Chris.
 
Physics news on Phys.org
This is easy but it is the other way around. The uncertainty principle derives from the property of the Fourier transform that you describe. It basically works like this: If you have an interferogram of a certain length, then you can describe this as an infinite interferogram multiplied with a function that is 1 on the finite domain, and 0 outside. But the convolution theorem states that the Fourier transform of a product of two functions is the convolution of both functions Fourier transforms. The Fourier transform of the rectangular function can be calculated, and it gets sharper and sharper the wider the rectangle gets. This makes the resolution get sharper and sharper. Maybe look up Fourier transform, convolution theorem and rectangular aperture.

It is also a general property of a function's Fourier transform to get thinner the wider the function gets even when they are not cut of at the ends, but this requires higher mathematics, I think it is linked to [tex]\ell^p[/tex]-spaces
 
A less technical way of saying the same thing as 0xDEADBEEF it that it's quite easy to tell the difference between 324 and 325 wavelengths (in a long interval) but it's a lot harder to tell the difference between 3.24 and 3.25 wavelengths (in a 100 times shorter interval), especially if they are corrupted by noise.
 

Similar threads

  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 29 ·
Replies
29
Views
7K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 13 ·
Replies
13
Views
3K
  • · Replies 8 ·
Replies
8
Views
2K