A ring laser is a laser with a ring resonator as its laser resonator. In contrast to a standing-wave (or linear) laser resonator, such a ring resonator does not have any end mirrors, hit with normal incidence, and it allows for two different propagation directions of the intracavity light.
Unidirectional Laser Operation
In many cases, unidirectional operation (where light propagates only in one of the two possible directions) is enforced by introducing an element into the resonator which leads to different losses for the propagation directions (Figure 1); this can be, e.g., a Faraday rotator combined with a polarizing element (e.g. a Brewster surface of the laser crystal).
Note that one normally requires only a tiny difference in round-trip propagation losses to obtain stable unidirectional operation. This is because in continuous-wave operation lasing leads to gain saturation such that the round-trip gain becomes zero; due to the loss difference, light propagating in the opposite direction then has a slightly negative round-trip gain, which means that it can never acquire any substantial optical power.
If unidirectional operation is achieved, there is no standing-wave interference pattern in the laser gain medium (except near reflection points), and consequently no spatial hole burning. Therefore, single-frequency operation is easily achieved. Particularly for solid-state bulk lasers, unidirectional ring laser designs can be considered as a standard approach to obtain stable single-frequency emission.
Typical Types of Ring Lasers
Nonplanar Ring Oscillators
A popular kind of solid-state ring laser is the nonplanar ring oscillator, also called NPRO or MISER. This is a monolithic laser design (Figure 3), where the whole laser resonator consists only of a coated laser crystal. While the fabrication of such crystals is somewhat more complicated than for ordinary laser crystals, alignment is fairly easy, and such lasers are very stable and robust.
Fiber Ring Lasers
There are also fiber lasers with ring resonator configurations. Fiber ring lasers are more often mode-locked lasers than single-frequency lasers. A frequently used configuration is that of the figure-of-eight laser , containing a nonlinear loop mirror as effective saturable absorber. The ring geometry then does not serve to avoid spatial hole burning, but rather follows from the principle of the artificial saturable absorber (a nonlinear loop mirror) as required for pulse shaping.
There are other fiber ring lasers, used e.g. in optical gyroscopes, where bidirectional operation is required. Outside the laser resonator, a beat note of the beams corresponding to the different propagation directions can be detected, and the beat frequency reveals the angular frequency of rotation of the laser (Sagnac effect). Special care is often required in order to avoid coherent locking of the counterpropagating waves. In particular, it is necessary to avoid even very weak parasitic reflections (e.g. on imperfect laser mirrors) which can couple the counterpropagating modes.
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See also: laser resonators, spatial hole burning, single-frequency lasers, single-frequency operation, nonplanar ring oscillators, fiber lasers
and other articles in the categories optical resonators, laser devices and laser physics