Single-frequency Operation | previous | next | feedback |
You can buy equipment for achieving single-frequency operation of lasers from:
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Ask RP Photonics for advice on how to ensure single-frequency operation of a laser, or how to characterize single-frequency lasers in terms of noise.
Definition: an operation mode of a laser where only a single resonator mode acquires a significant power
A laser can be made to operate on a single mode of its resonator, and is then called a single-frequency laser. The linewidth of the laser radiation can then be very small – often only a few kilohertz – and the coherence length accordingly long. In contrast, multimode operation causes the linewidth to be a multiple of the mode spacing (free spectral range) of the resonator. Single-frequency operation is required e.g. to drive resonant cavities (e.g. for efficient frequency doubling in an external enhancement cavity), for high-resolution spectroscopy, for coherent beam combining of laser outputs, and for applications where the intensity noise must be very low.
Single-frequency operation is usually obtained when the bandwidth of the net gain is smaller than the frequency spacing of the resonator modes. (The laser should operate on the fundamental transverse mode only, i.e. emit a diffraction-limited beam, in order to eliminate the different mode frequencies of higher-order transverse modes.) For gain media with large bandwidth, single-frequency operation can be achieved by using some optical filters (e.g. an etalon) in the resonator and/or by making the resonator short (thus increasing the mode spacing to obtain a large free spectral range).
Note that reduced mode competition, e.g. inhomogeneous gain saturation caused by spatial hole burning in a standing-wave resonator, can make it difficult to achieve single-frequency operation. Therefore, single-frequency operation is often realized with unidirectional ring lasers, or sometimes with the twisted-mode technique. In fiber lasers and amplifiers, additional problems arise from stimulated Brillouin scattering.
It might be expected that intracavity frequency doubling is not readily compatible with single-frequency operation, but the opposite is true: via sum frequency generation, the intracavity nonlinearity even protects the lasing modes by introducing higher losses for other modes.
The concept of distributed feedback lasers is often used for achieving single-frequency operation, particularly for semiconductor lasers and fiber lasers. This usually leads to fairly short laser resonators.
Thermal drifts, e.g. of the gain medium, can cause occasional mode hopping, i.e. the change from one oscillating resonator mode to another. To a limited extent, this can be acceptable for applications.
If a high optical power in a single-frequency signal is required, a master oscillator power amplifier configuration can be employed. An alternative with potentially lower laser noise is injection locking of a high-power laser with a single-frequency low-power laser.
The article on single-frequency lasers discusses different types of lasers for single-frequency operation.
See also: single-frequency lasers, single-mode operation, modes of laser operation, resonator modes, mode competition, mode hopping, twisted-mode technique, Spotlight article 2006-09-03b
Since October 2008, the Encyclopedia of Laser Physics and Technology is also available in the form of a two-volume book. Maybe you would enjoy reading it also in that form! The print version has a carefully designed layout and can be considered a must-have for any institute library, laser research group, or laser company.
You may order the print version via Wiley-VCH.
