
Originally Posted by
taggalucci
I'm still confused by the terms slow and fast axis
It is confusing, but basically the two things to remember are that the fast and slow axis are defined pre-collimation, and the diameter/divergence proportional shift always applies.
Look at a G71 raw diode output shape on a wall, with the case pin north or south you'll have a "|" shape, so this is fast axis vertical and slow horizontal.
Add a single collimator to bring the fast axis into check, and the near-field beam shape is now say, 1mm wide by 2mm tall.
Because the near field vertical dimension is larger, the divergence is lower resulting in a smaller vertical dimension far-field.
Because the near field horizontal dimension is smaller, the divergence is higher and this results in a wider horizontal dimension far-field, but it is still the slow axis.
After collimation (and with no correction) the point along the beam path where the spot shape becomes very close to circular is where the two axis cross over.
A little bit werrrr, a little bit weyyyyyy, a little bit arrrrgggghhh