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Unstable Resonators

Author: the photonics expert

Definition: optical resonators which are dynamically unstable with respect to transverse beam offsets

More general term: optical resonators

Categories: article belongs to category general optics general optics, article belongs to category optical resonators optical resonators

DOI: 10.61835/pka   Cite the article: BibTex plain textHTML

Depending on details of its design, an optical resonator is either stable or unstable with respect to transverse beam offsets. Stability in that sense means that any geometrical ray injected into the system with some not too large initial transverse offset position and angle will stay within the system during many round trips. In an unstable resonator, such a ray will be ejected sooner or later. With the ABCD matrix algorithm, one can easily determine whether a resonator is operated in the stable or unstable regime, and what changes of resonator parameters would be required to move from one regime into the other.

A more comprehensive analysis of resonator properties requires wave optics and typically involves analyzing resonator modes. The properties of the resonator modes are very different in the stable or unstable regime. Unstable resonators have a number of special properties:

  • The modes always experience significant diffraction losses, which are often very high (order of 50 % per round trip or higher).
  • The diffraction losses generally become higher for higher mode orders. This intrinsic mode discrimination is often helpful for obtaining single transverse mode operation of a laser.
  • Particularly for resonators with diffraction at hard edges, the transverse mode profiles are rather complicated and usually exhibit pronounced ring structures. Only numerical methods can then be used for calculating the detailed mode profiles. For some soft-aperture resonators (see below), however, the mode properties can at least be estimated with reasonable accuracy using analytical methods.
  • In a linear unstable resonator, the wavefronts of the counterpropagating beams do not necessarily match each other, and they do not necessarily match the surfaces of the two end mirrors.

The attribute “unstable” should not be misunderstood as stating that such resonators are less robust than stable ones. To the contrary, the alignment sensitivity of unstable laser resonators can be even substantially lower than for stable resonators, and rather robust high-power lasers have been developed with unstable resonators.

Output Coupling in Unstable Laser Resonators

Unstable laser resonators are usually made such that the mentioned diffraction “losses” are taken as the useful laser output. The output coupler can be an ordinary laser mirror where the field distribution extends beyond the mirror edges, so that some light passes the mirror on the sides (see Fig. 1). Although the output beam profile has a hole in the near field, the beam divergence is quite small, and the beam quality for some very high-power lasers with such resonators is at least higher than achievable with stable resonators – particularly if large diffraction losses can be tolerated, so that the hole can be made relatively small.

unstable resonator with hard-edge mirror
Figure 1: An unstable laser resonator with output coupling at a hard-edge mirror.

In other cases, a scraper mirror (Fig. 2, e.g., a tilted mirror with an elliptical hole) is used, which “scrapes off” some light from the circulating intracavity beam.

unstable resonator with a scraper mirror
Figure 2: An unstable laser resonator with output coupling at a scraper mirror.

Another possibility is the use of a variable reflectivity mirror, where the reflectivity decreases with increasing distance to the beam axis – often according to a Gaussian or super-Gaussian function. This approach can avoid the otherwise typical ring structures in the near-field output beam profile and is often suitable for obtaining a rather high beam quality.

In some cases, a resonator is stable in one direction and unstable in the other direction. Such hybrid resonators are sometimes used in situations with highly elliptical beams [16].

In most cases, unstable resonators are substantially more difficult to analyze and optimize than stable resonators. While for stable resonators the ABCD matrix algorithm allows one to calculate a wide range of mode properties in a relatively simple way, one often requires numerical beam propagation for analyzing unstable resonator modes. In addition to suitable software, an understanding of various sophisticated concepts of optics, involving terms like the round-trip magnification <$M$> and the Fresnel number <$N_\textrm{F}$>, can be helpful.

Advantages and Limitations of Unstable Laser Resonators

Although most laser resonators are designed as stable resonators, unstable resonators can have substantial advantages in certain cases. In particular, they can help to generate a laser beam with very high optical power and still relatively high beam quality. A frequent problem with stable resonators in such cases is that a large enough fundamental resonator mode cannot be realized, or that this mode is highly sensitive to disturbances like thermal lensing or misalignment. An unstable resonator, however, can have a very large fundamental mode with a substantial net gain advantage over all higher-order modes, and with no excessive sensitivity.

However, this principle usually works well only when the gain medium can provide a rather large gain. This can be the case in pulsed flashlamp-pumped or diode-pumped YAG lasers, in metal vapor lasers, excimer lasers and chemical lasers, for example. The application to low-gain lasers such as continuous-wave CO2 lasers or lamp-pumped solid-state lasers is more difficult and often leads to a lower beam quality.

The more difficult analysis of unstable resonators can be considered as a disadvantage, making it harder to find optimized laser designs.

More to Learn

Encyclopedia articles:


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