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By flatter he means closer to parallel (0 mrad divergence) but not actually parallel since 0 divergence is impossible. Divergence is inversely proportional to initial beam diameter, so the wider the beam diameter at the aperture, the lower the divergence can be with good optics. Divergence is also a function of cavity length, which is why lasers with longer cavities have lower divergence than those with short cavities. Working with laser diodes is different than most other kinds of lasers. With a HeNe laser, the cavity is at least several inches long, which gives a nicely collimated beam with no collimating lenses at all. Diodes have cavities <1mm long which means their uncorrected output (no lens) is highly divergent. By placing a collimating lens a few mm away from the diode allows this highly divergent beam to expand a bit before being collimated, which means that diodes can be collimated to extremely low divergence numbers using just a collimating assembly. Here's a couple diagrams I made awhile back that help illustrate these concepts:
this diagram shows how a beam expander influences divergence in the far-field:
You can see how the spot in the far field is smaller than it would be without the expander, and overall divergence is less but not eliminated.
this illustrates the effect cavity length has on uncorrected divergence:
this diagram shows how a beam expander influences divergence in the far-field:
You can see how the spot in the far field is smaller than it would be without the expander, and overall divergence is less but not eliminated.
this illustrates the effect cavity length has on uncorrected divergence:
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