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Laser Resonators

Author: the photonics expert

Definition: optical resonators serving as basic building blocks of lasers

Alternative term: laser cavities

More general term: optical resonators

Categories: article belongs to category optical resonators optical resonators, article belongs to category laser devices and laser physics laser devices and laser physics

DOI: 10.61835/gur   Cite the article: BibTex plain textHTML   Link to this page   LinkedIn

A laser generally requires a laser resonator (or laser cavity), in which the laser radiation can circulate and pass a gain medium which compensates the optical power losses. Exceptions are a few cases (e.g. some free electron lasers) where a medium with very high gain is used, so that amplified spontaneous emission extracts significant power in a single pass through the gain medium.

A laser resonator typically contains multiple laser mirrors, one of them being an output coupler, a laser gain medium, and possibly additional optical elements e.g. for wavelength tuning, Q switching or mode locking. It can be a linear resonator, having two end mirrors, or a ring resonator.

The laser radiation is automatically generated at one or several frequencies corresponding to resonances (resonator modes), possibly with small deviations caused by “gain pulling”. No special measures are required for operating on the resonance; this is different for external resonators, e.g. resonant enhancement cavities.

linear and ring laser resonator
Figure 1: Two simple solid-state laser resonators with a laser crystal as gain medium. Output beams are generated where resonator mirrors are partially transmissive. For the ring laser (right), unidirectional operation is enforced with a Faraday isolator; without that, one would obtain two output beams.

Laser Resonators of Solid-state Lasers

Solid-state bulk lasers are usually built with several dielectric mirrors (laser mirrors), which may be plane or curved. Figure 1 shows a linear resonator and a ring resonator built in that way, and containing a laser crystal (hidden in a laser head) as the gain medium. In some cases, a dielectric mirror coating is placed on the gain medium itself; see the article on monolithic solid-state lasers. One of the mirrors, usually an end mirror, is the partially transmissive output coupler.

simple laser resonator
Figure 2: A simple laser resonator consists only of two mirrors around a diode-pumped laser head. Source: Cutting Edge Optronics.

The design of the laser resonator (comprising optical elements, angles of incidence, and distances between the components) determines the beam radius of the fundamental mode at all locations along the beam, together with other important properties. For maximum beam quality (→ diffraction-limited output), the beam radius in the gain medium has to approximately match the radius of the pumped region. For smaller beam radii, operation with multiple spatial modes is obtained, leading to a non-ideal beam quality; however, such multimode lasers have other advantages such as much wider stability zones and a lower sensitivity to misalignment.

RP Resonator

Calculation of Mode Properties

The software RP Resonator is a particularly flexible tool for calculating all kinds of mode properties, even including misalignment effects, and allowing sophisticated design optimizations. This is vital for laser development, for example. You can take into account alignment sensitivity and thermal lensing, and even design a resonator for operation in a specific stability zone.

In many cases, the laser resonator design should have additional features. For example, it can be optimized

Particularly for high-power lasers with good beam quality, thermal lensing in the gain medium is very important. The resonator design should be made so that changes of the thermal lens do not affect too much the mode sizes. Also, it should have a low sensitivity to thermal aberrations [2] and misalignment [1]. The importance of these factors should not be underestimated; there are cases where two resonators even with equal mode sizes in the gain medium lead to very different laser performance and are radically different in terms of alignment.

Although it is normally not that difficult to evaluate the properties of a given laser resonator, it can be challenging to find a resonator design which satisfies multiple criteria such as those listed above. Numerical optimization, using special resonator design software, can be the only way to find good solutions, particularly for some mode-locked lasers. Also, a solid understanding of resonator properties can help considerably when trying to find resonator configurations with special combinations of properties, such as large mode areas and short lengths. For advanced design issues, a great deal of experience is at least as important as a versatile design software.

Some high-power lasers (for example with slab designs) are operated with unstable resonators, allowing a reasonable (but typically not diffraction-limited) beam quality to be achieved despite the presence of strong thermal effects in the gain medium. Due to the high diffraction losses, such laser cavities require relatively high gain.

There are various types of monolithic solid-state lasers which have the whole beam path within the laser crystal. Beam reflections are then typically realized either with dielectric coatings on crystal surfaces, or with total internal reflection.

Physical Limitations

Although various properties of laser resonators can be optimized with a suitable resonator design, there are limitations, particularly for certain combinations of properties. For example, one can only to a limited extent combine the features of a short resonator length, large mode areas and low alignment sensitivity. Even optimized resonator designs can not fully meet desirable specifications for certain lasers, particularly for high-power lasers.

Note also that laser resonators should not be considered as power-scalable in a useful sense, as discussed in the Spotlight article of 2009-09-19. This means that certain design challenges are more severe for lasers with higher output powers.

Alignment of Laser Resonators

For laser resonators with simple designs, e.g. with just two mirrors around some gain medium, the initial alignment is often quite easy to find. Once the laser works, the alignment can be further optimized, simply maximizing the output power.

For more complicated resonators, it can be quite challenging to find some approximate initial alignment where the laser starts operating. In such cases, one may require some visible alignment laser, which should preferably have an appropriate wavelength, such that the laser mirrors have a high enough reflectivity for that beam. In other case, one may make a simple resonator with temporarily used mirrors for starting, use the resulting output beam(s) for alignment of further components, and then remove the mentioned mirrors.

Particularly laser resonators with large mode sizes can have a high alignment sensitivity. Even small tilts of laser mirrors, for example, may move the resonator mode such that the output power drops and possibly the beam quality is degraded.

Lasers without Laser Resonator

There are some devices which do not contain an optical resonator and are nevertheless sometimes called lasers. In particular, that applies to free electron lasers with very high gain, where strong amplified spontaneous emission occurs. Similar to an ordinary laser, they may exhibit efficient and strongly directed emission, since the gain is high, but only along a well-defined line. One may argue, however, that these should not be called lasers, but superluminescent sources.

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Bibliography

[1]V. Magni, “Multielement stable resonators containing a variable lens”, J. Opt. Soc. Am. A 4 (10), 1962 (1987); https://doi.org/10.1364/JOSAA.4.001962
[2]R. Paschotta, “Beam quality deterioration of lasers caused by intracavity beam distortions”, Opt. Express 14 (13), 6069 (2006); https://doi.org/10.1364/OE.14.006069
[3]A. E. Siegman, Lasers, University Science Books, Mill Valley, CA (1986)
[4]N. Hodgson and H. Weber, Laser Resonators and Beam Propagation, Springer Series in Optical Sciences, Springer, Berlin (2005)
[5]R. Paschotta, case study on automatic resonator optimization with the RP Resonator software

(Suggest additional literature!)


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This encyclopedia is authored by Dr. Rüdiger Paschotta, the founder and executive of RP Photonics AG. How about a tailored training course from this distinguished expert at your location? Contact RP Photonics to find out how his technical consulting services (e.g. product designs, problem solving, independent evaluations, training) and software could become very valuable for your business!


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