Far field intensity distribution

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Homework Statement


Describe the far-field intensity distribution if

[itex]f(x',y') = circ(\frac{\rho}{D}) cos(\frac{k \theta x'}{2}[/itex]

where [itex]\rho = \sqrt{x^{2} + y^{2}}[/itex].

Homework Equations


The Fourier transform of the circ function was given to us earlier:
[itex]\textbf{F} [ circ(\frac{\rho}{D}) ] = \frac{\pi D^{2}}{4} Jinc(\frac{k_{\rho} D}{2})[/itex]
where Jinc is a bessel function

I know that the Fourier transform of a product of two functions is the convolution of the two Fourier transforms. (Convolution theorem)

The far field intensity is given by [itex]\textbf{I}^{(z)} = \frac{\textbf{I}_{0}}{\lambda^{2} z^{2}} |\textbf{F}[f(x',y')]|^{2}[/itex]

Also [itex]k_{x} = \frac{k x}{z} = k \theta[/itex]

The Attempt at a Solution



so the Fourier transform reads: [itex]\frac{\pi D^{2}}{4} Jinc(\frac{k_{\rho} D}{2}) \otimes \delta ( k_{x} - \frac{k \theta}{2} ) + \delta ( k_{x} + \frac{k \theta}{2} )[/itex]

then the [itex]\delta ( k_{x} - \frac{k \theta}{2} )[/itex] simplifies to [itex]\delta (k_{x}/2 )[/itex] and similar for the other one.
So there would be two bessel functions on the far field plane.
Is this right?
 
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The far field intensity should then be \frac{\textbf{I}_{0}}{\lambda^{2} z^{2}} |\frac{\pi D^{2}}{4} Jinc(\frac{k_{x} D}{2}) \otimes \delta ( k_{x}/2 ) + \delta ( - k_{x}/2 )|^{2} = \frac{\textbf{I}_{0}}{\lambda^{2} z^{2}} (\frac{\pi D^{2}}{2} Jinc(\frac{k_{x} D}{2}) )^{2} Is this right?