Aperture function of Diffraction Grating

The integral of the cos part is just a constant.In summary, the far-field irradiance diffraction pattern for a large diffraction grating with an amplitude transmission aperture function A(x) = 1/2[1+cos(kx)]e^(-x^2/a^2) is proportional to the Fourier transform of the aperture function. By expressing cos(kx) as a combination of exponential functions, the Fourier transform can be simplified to shifted Gaussian functions. When a >> 1/k, the Gaussian part becomes constant and the integral of the cos part is a constant. The limits of integration should be from -infinity to infinity. The resolving power of the grating can be found using appropriate resolving criteria in terms of k and
  • #1
makotech222
4
0

Homework Statement


A very large diffraction grating has an amplitude transmission aperture function A(x) = 1/2[1+cos(kx)]e^(-x^2/a^2)

a) What is the far-field irradiance diffraction pattern when a >>1/k
B) Plot the pattern
c) Using the appropriate resolving criteria, find the grating's chromatic resolving power in terms of k and a.


Homework Equations





The Attempt at a Solution



Well i know the irradiance pattern is proportional to the Fourier transform of the aperture function, but trying to take the Fourier of that monster function is pretty hard. Putting it in mathematica gives off a much too complicated function to plot. I assume the function simplifies when a>>1/k, but I'm not sure how. I have no idea how to get the resolving power, so some help there would be nice. Thanks
 
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  • #2
If you write

[tex]\cos (kx) = \frac{e^{ikx}+e^{-ikx}}{2},[/tex]

then you can express the Fourier transform in terms of shifted Gaussian functions (you might want to do a coordinate rescaling to get the factors of [itex]2\pi[/itex] correct). Mathematica probably doesn't know this trick for some reason.
 
  • #3
Can you clarify on how to change it to shifted Gaussian function?

Another question. Since it's not specified, what limits of integration do i take? I only assume it is -a/2 to a/2, from other examples I've seen.
 
  • #4
makotech222 said:
Can you clarify on how to change it to shifted Gaussian function?

Another question. Since it's not specified, what limits of integration do i take? I only assume it is -a/2 to a/2, from other examples I've seen.

Since the grating is large, you should integrate from [itex]-\infty[/itex] to [itex]\infty[/itex].

As for the shift, if the Fourier transform is

[tex] \hat{f}(\omega) = \frac{1}{\sqrt{2\pi}} \int_{-\infty}^\infty e^{-i\omega x} f(x)dx,[/tex]

then the Fourier transform of [itex]e^{ikx} f(x)[/itex] is

[tex] \frac{1}{\sqrt{2\pi}} \int_{-\infty}^\infty e^{-i\omega x} e^{ikx}f(x)dx =\frac{1}{\sqrt{2\pi}} \int_{-\infty}^\infty e^{-i(\omega-k) x} f(x)dx = \hat{f}(\omega-k).[/tex]
 
  • #5
Sorry, I'm still not getting it, I don't understand what I'm taking the Fourier transform of.
 
  • #6
simply take the limit a-> infinity, the Gaussian part becomes constant.
 

1. What is the aperture function of a diffraction grating?

The aperture function of a diffraction grating is a mathematical expression that describes the intensity of light diffracted by the grating at different angles. It takes into account the spacing and size of the grooves on the grating, as well as the wavelength of the incident light.

2. How does the aperture function affect the diffraction pattern of a grating?

The aperture function determines the shape and intensity of the diffraction pattern produced by a grating. A wider aperture function will result in a narrower central peak and more intense side lobes, while a narrower aperture function will result in a broader central peak and weaker side lobes.

3. What is the relationship between the aperture function and the resolution of a diffraction grating?

The aperture function plays a crucial role in determining the resolution of a diffraction grating. A wider aperture function allows for more diffracted orders to be resolved, resulting in a higher resolution. On the other hand, a narrower aperture function will limit the number of diffracted orders that can be resolved, leading to a lower resolution.

4. Can the aperture function be modified to improve the performance of a diffraction grating?

Yes, the aperture function can be modified by changing the spacing and size of the grooves on the grating. By carefully designing the aperture function, the diffraction grating can be optimized for specific applications and desired performance.

5. How does the aperture function of a diffraction grating differ from that of a single slit?

The aperture function of a diffraction grating is more complex than that of a single slit. While the aperture function of a single slit is a simple sinc function, the aperture function of a diffraction grating takes into account multiple grooves and their spacing, resulting in a more intricate pattern of peaks and valleys in the diffraction pattern.

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