Single Slit Fraunhofer Diffraction

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SUMMARY

The discussion focuses on the Fraunhofer diffraction pattern produced by a single slit of width 'a' when illuminated by a coherent plane wave. The irradiance formula is established as I=I_0\left(\frac{\sin(\beta/2)}{\beta/2}\right)^2, where β=ka sin(θ). The integral for the electric field E is given as E=-\frac{ikE_0}{2\pi r_0}\int_{-a/2}^{a/2} e^{ikr} \, dx. The conversation highlights the importance of considering the illumination profile across the slit, especially for narrow slits, and suggests approaching the problem as a microwave slot antenna for more accurate results.

PREREQUISITES
  • Understanding of Fraunhofer diffraction principles
  • Familiarity with wave optics and plane waves
  • Knowledge of integral calculus in physics
  • Concept of electric field representation in wave propagation
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  • Study the derivation of the Fraunhofer diffraction formula for single slits
  • Explore the impact of slit width on diffraction patterns
  • Learn about microwave slot antennas and their applications
  • Investigate non-uniform illumination effects on diffraction
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Optics students, physicists, and engineers interested in wave propagation and diffraction phenomena, particularly those working with coherent light sources and antenna design.

Daniel Gallimore
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Just to clarify, this isn't homework. I took an Optics course a few years ago, but in the time between then and now, I've lost all my notes.

Suppose we have an infinitely tall slit of width a and a parallel screen a distance r_0 away. Let the x axis be parallel to the width of the slit, with the origin at the center of the slit (such that the slit extends from x=-a/2 to x=a/2). The z axis extends toward the screen from the origin. An angle \theta locates a point P on the screen (with respect to the z axis) a distance x=X along the screen. A ray drawn from the origin to P is length r.

Given a plane wave incident on the slit, what is the formula for the irradiance of the diffracted wave as it encounters the screen?

I know the answer is similar (if not equal to) I=I_0\left(\frac{\sin(\beta/2)}{\beta/2}\right)^2 where \beta\equiv ka\sin\theta I also know that E=-\frac{ikE_0}{2\pi r_0}\int_{-a/2}^{a/2} e^{ikr} \, dx To get from the electric field to the irradiance is not a problem.

Any recommendations?
 
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This is the standard formula, I think. The problem is with the limits of the integral. For a real case and a narrow slit, the illumination across the slit is not uniform so the profile should be included in the formula.
 
sophiecentaur said:
This is the standard formula, I think. The problem is with the limits of the integral. For a real case and a narrow slit, the illumination across the slit is not uniform so the profile should be included in the formula.
Does saying the incident wave is a (coherent) plane wave not specify the profile? If not, please assume the illumination is uniform across the width of the slit. Also, I know this is just a toy example, but I'd like to get it down before tackling anything more realistic, like a nonuniform incident wave front.

What I want to know is how to get from the integral to to the \sin(\beta/2)/(\beta/2) function. And if the integral is incorrect, I need some pointers to correct it.
 
Daniel Gallimore said:
If not, please assume the illumination is uniform across the width of the slit
If you assume that, then no problem. But a slit in a screen of finite, practical thickness could be several wavelengths deep and, depending on the material (say metal) it will definitely affect the distribution of luminosity at the way out of a narrow slit. It just depends on how far you want to go, I think. Thinking in terms of a microwave slot through a thick sheet of metal, there will be induced currents around the edges of the slit which will alter the effective width.
Imo, the problem of a narrow slit would probably be best approached not as the limiting case of a wide slit but rather as a microwave slot antenna.
 
sophiecentaur said:
If you assume that, then no problem. But a slit in a screen of finite, practical thickness could be several wavelengths deep and, depending on the material (say metal) it will definitely affect the distribution of luminosity at the way out of a narrow slit. It just depends on how far you want to go, I think. Thinking in terms of a microwave slot through a thick sheet of metal, there will be induced currents around the edges of the slit which will alter the effective width.
Imo, the problem of a narrow slit would probably be best approached not as the limiting case of a wide slit but rather as a microwave slot antenna.
I found a working of the problem in a book on Optics and was able to replicate the result in notation that was more familiar to me.

Thank you for your comments.
 
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