Editing Active optics (section)

== Other applications ==
Complicated laser set-ups and interferometers can also be actively stabilized.

A small part of the beam leaks through beam steering mirrors and a four-quadrant-diode is used to measure the position of a laser beam and another in the focal plane behind a lens is used to measure the direction.  The system can be sped up or made more noise-immune by using a [[PID controller]]. For pulsed lasers the controller should be locked to the repetition rate. A continuous (non-pulsed) pilot beam can be used to allow for up to 10&nbsp;kHz bandwidth of stabilization (against vibrations, air turbulence, and acoustic noise) for low repetition rate lasers.

Sometimes [[Fabry–Pérot interferometer]]s have to be adjusted in length to pass a given wavelength. Therefore, the reflected light is extracted by means of a [[Faraday rotator]] and a [[polarizer]]. Small changes of the incident wavelength generated by an [[acousto-optic modulator]] or [[Interference (wave propagation)|interference]] with a fraction of the incoming radiation delivers the information whether the Fabry Perot is too long or too short.
 
Long [[optical cavity|optical cavities]] are very sensitive to the mirror alignment. A control circuit can be used to peak power. One possibility is to perform small rotations with one end mirror. If this rotation is about the optimum position, no power oscillation occurs. Any beam pointing oscillation can be removed using the beam steering mechanism mentioned above.

[[X-ray]] active optics, using actively deformable grazing incidence mirrors, are also being investigated.<ref>{{cite web|title=Research Partnership Advances X-ray Active Optics|url=http://www.adaptiveoptics.org/News_0305_1.html|work=adaptiveoptics.org|accessdate=2 June 2011|archiveurl=https://web.archive.org/web/20070311072126/http://www.adaptiveoptics.org/News_0305_1.html|date=March 2005|archivedate=March 11, 2007}} [http://www.mssl.ucl.ac.uk/smartoptics/Newsletter/SO_Newsletter_7.pdf Alt URL]</ref>