Dipole Radiation: Practical Considerations

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    Dipole Radiation
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The discussion revolves around the concept of dipole radiation and its practical implications in light-matter interaction as explained by Feynman. A key point raised is the requirement for the plate to be extremely thin, approximately 0.1 of the wavelength, for all dipoles to experience the same electric field phase. This condition is deemed impractical in real-world applications. However, it is suggested that a more feasible approach can be developed through integration methods. Overall, the conversation highlights the theoretical underpinnings of dipole radiation while acknowledging the challenges in practical implementation.
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Hi,

I an reading an interesting chapter of Feyman where he explains the basis of light-matter interaction with wave theory: http://cua.mit.edu/8.421_S08/Reading/Feyman_refr_index.pdf

I didn't understand there one thing... to explain it he says that all the dipoles on the plate ''feel'' the same electric field with the same phase [page 4, equation 31.10]. to say this the plate has to be very very very thin [something like 0.1 of the wavelength]... how this can be practical??


Lior
 
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On the first page, about halfway down, he writes:

Feynman said:
A source which we shall call "the external source is placed a large distance away from a thin plate of transparent material, say glass.

I added the boldface to point out the key word in his assumptions. He's assuming the plate is indeed very very thin, much less than a wavelength. It's not very practical, but one can build a more practical solution from it by integration.
 
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