Abstract

The method of mode selection in optical resonators using a linear polarizer with the help of an anisotropic metal film is proposed. The film thickness is much less than a wavelength. The losses introduced by such a film into undesired oscillation modes are composed of ohmic losses and losses due to the change in radiation polarization caused by the film. The principle of operation has been investigated at 0.63 μm.

© 1972 Optical Society of America

Derivation of Optical Constants of Metals from Thin-Film Measurements at Oblique Incidence

J. E. Nestell and R. W. Christy
Appl. Opt. 11(3) 643-651 (1972)

Mode Selectivity and Mirror Misalignment Effects in Unstable Laser Resonators

Arthur N. Chester
Appl. Opt. 11(11) 2584-2590 (1972)

Optical Resonators with Paraxial Modes

Ernest E. Bergmann
Appl. Opt. 11(1) 113-119 (1972)

Output Beam from a Confocal Resonator with a Pinhole for Mode Selection

Tokuo Miyamoto
Appl. Opt. 11(9) 2040-2046 (1972)

Optical Detection of Magnetic Resonance in Alkali-Metal Vapor Using D₁ and D₂ Radiation Simultaneously

Takahiro Kubo
Appl. Opt. 11(7) 1521-1525 (1972)