To collimate a laser diode or fiber's output using a lens, a common belief is to make the output beam's waist location as distant as possible form the lens. For example, see Saleh and Teich [1]. Well, this is only approximately correct.
The best collimation is achieved when the output beam has either:
(1) the smallest divergence angle; or
(2) the largest waist size; or
(3) the longest Rayleigh range.
The above three conditions are equivalent, i.e., achieving any single one means the other two are achieved simultaneously.
To reach the above conditions, the input waist needs be at exactly the object focal plane of the collimating lens. Then the output beam waist will be at exactly the conjugate (image) focal plane [2]:
Figure 1: Geometry of the perfect collimation. |
This figure also indicates that the output beam's waist location cannot be placed at infinity. The farthest distance one can make is when the input beam's waist is located at ZR + f from the lens (ZR is input beam's Rayleigh range and f is focal length). This is the common belief that the best collimation should be reached; however, the output waist size is not the largest.
References:
[1] Saleh and Teich, Fundamentals of Photonics, 2nd Ed. Page 90.
[2] Sidney A. Self, "Focusing of spherical Gaussian beams," Applied Optics 22, 658 (1983).
2 comments:
Thank you so much for posting this, its been very helpful to me.
Thank you a lot - I was searching to exactly this description of collimating Gaussian beams. It is very usefull and well written.
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