Sensitive birefringence measurement in a high-finesse resonator using diode laser optical self-locking

• Published in: Applied physics. B, Lasers and optics Vol. 74; no. 6; pp. 495 - 501
• Main Authors: MORVILLE, J, ROMANINI, D
• Format: Journal Article
• Language: English
• Published: Berlin Springer 01.04.2002; Springer Nature B.V
• Subjects: Applied physics; Biological and medical applications; Birefringence; Dielectric strength; Diode lasers; Exact sciences and technology; Feedback; Frequency locking; Fundamental areas of phenomenology (including applications); Holes; Lasers; Locks; Mathematical analysis; Metrological applications; Mirrors; Optical feedback; Optics; Physics; Resonance; Semiconductor lasers; Semiconductor lasers; laser diodes; Spatial resolution; Wave optics; Frequency locking; Dielectric materials; Indium Gallium Arsenides Phosphides; Line widths; Experimental device; Laser beam applications; Experimental study; Laser cavity resonators; Laser diodes; Optical measurement; Semiconductor lasers; Optical feedback; Line narrowing; Metrology; Birefringence; Intracavity; Quaternary compounds; Spatial resolution; Rotation angle; Electrostatic mirrors
• ISSN: 0946-2171; 1432-0649
• DOI: 10.1007/s003400200854

We demonstrate a new method to measure weak birefringence of dielectric mirrors with excellent spatial resolution and sensitivity (<10-7 radians). We exploit a well-known optical feedback scheme for line-width narrowing and frequency locking of a diode laser to a high-finesse cavity. Feedback comes from the intracavity field which builds up at resonance, selected by its change in polarization with respect to the incident field. This change, due to the residual birefringence of the cavity mirror coatings, was already exploited for birefringence measurements using an active laser-locking scheme. Here we measure the optical feedback rate as a function of rotation angle of one of the cavity mirrors (around the cavity axis). A stable feedback signal is obtained since the laser, as soon as it locks to a cavity resonance, effectively behaves as a monochromatic source. By fitting the data with a theoretical expression, we determine quantitatively the local birefringence vectors of both mirrors, which are around 10-6 radians. Our scheme is simple, works with cavities of very high finesse (F∼105), and is promising for measuring birefringence in gases induced by external fields.