How can I calculate the divergence of a laser beam by diffraction? I want to find the following relation,

$$ \Delta\Omega = \frac{\lambda^2}{A}, $$

where $\lambda$ is the wavelength and $A$ is the area. laser in cavity

this is the laser in a cavity.

  • $\begingroup$ What exactly is the question? You want a derivation of the diffraction equation? Or do you want to see how this equation is applied in a special case? $\endgroup$
    – Johannes
    Sep 20 '14 at 13:51
  • 1
    $\begingroup$ really i wanna find angular laser beam divergence by diffraction relations. ΔΩ=λ^2/A = (∆θ)^2 $\endgroup$
    – Natali
    Sep 20 '14 at 14:30
  • $\begingroup$ Presumably $\Omega$ is the solid angle, in which case your expression is essentially the square of the expression for the width of an Airy disk. $\endgroup$ Sep 20 '14 at 15:27

I will assume that you are asking about laser beams in the fundamental, diffraction limited Gaussian mode. The standard expression for the divergence angle of a Gaussian beam in the far field is (see the Wikipedia page on Gaussian beams) $$ \theta=\frac{\lambda}{\pi\omega_0} $$ where $\omega_0$ is the so-called waist size of the Gaussian beam. From here you can calculate the solid angle subtended by the beam which is given, in the small $\theta$ limit, as $$ \Theta\simeq\pi\theta^2=\frac{\lambda^2}{\pi\omega_0^2}=\frac{\lambda^2}{A}, $$ where $A$ is the area of the beam's waist.

If you are looking for a derivatation which starts at a more fundamental level than that, then you should pick up any textbook on lasers. Any textbook you can find will cover the derivation of the Gaussian modes of a laser beam from the wave/Helmholtz equation. You can also look at section 2.1 of my thesis where I sketch out the derivation from the Helmholtz equation although I stop slightly short of deriving the divergence angle.


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