Questions about current limits of laser beam widths

AI Thread Summary
The current limits of laser beam widths for available technologies typically range from a few millimeters for Gaussian beams, with potential reductions using beam reducers like telescopes, constrained by the light's wavelength. The theoretical minimum waist size for Gaussian beams is noted, and practical setups can achieve focal spots around 200 micrometers using long focal length lenses, particularly in deep UV applications. Smaller beam widths, such as 10 microns, can be achieved within fiber optics, but maintaining such widths in free space is challenging. Resources for further understanding Gaussian beam optics are available online. This information highlights the complexities and limitations of achieving narrow laser beams in practical applications.
CFlower
Messages
15
Reaction score
0
Hi there,

I'm looking for some information on the current limits of the beam width of currently available lasers. I'm less interested in experimental setups that are not on the market yet, but I suppose if one of them is markedly different it would be interesting to know.

Specifically, what is the smallest available beam width, what kinds of lasers can achieve it, and what are the specs for such a beam (i.e. power etc.)

I've looked around a good deal so far and haven't found anything, so if you know or could just point me in the right direction I would be very thankful! This is a bit out of my field so any advice is appreciated.

Cheers,
CFlower
 
Physics news on Phys.org
For a Gaussian beam the usual limit is a few millimeters as it exits the laser system, and enters your free space optical setup.

You can reduce this with a "beam reducer", which is simply a telescope, but the results are limited by the wavelength of the light. The theoretical limit would be the waist size for a Gaussian beam.

With a bit of patience you can work your way through the Gaussian beam tutorial here:
http://www.newport.com/Gaussian-Beam-Optics/144899/1033/content.aspx

The technique I have used in the lab is to input the collimated laser beam into a very long focal length lens (e.g., 2 meter), and place my point of activity at the focal point. I've done this with 260 nm (deep UV) which had to be taken into a vacuum chamber. The focal spot was about 200 um, this is not the optical limit.

Of course you can obtain smaller beams inside of fiber optics; 10 microns is easy enough, but you cannot maintain this once the beam is in free space.This may help: http://www.miyachiamerica.com/servlet/servlet.FileDownload?retURL=%2Fapex%2FEducationalResources_Articles&file=01580000001ake3
 
Thread 'Motional EMF in Faraday disc, co-rotating magnet axial mean flux'
So here is the motional EMF formula. Now I understand the standard Faraday paradox that an axis symmetric field source (like a speaker motor ring magnet) has a magnetic field that is frame invariant under rotation around axis of symmetry. The field is static whether you rotate the magnet or not. So far so good. What puzzles me is this , there is a term average magnetic flux or "azimuthal mean" , this term describes the average magnetic field through the area swept by the rotating Faraday...

Similar threads

Back
Top