continuous-wave operation (original) (raw)
Author: the photonics expert (RP)
Definition: operation mode of a laser with continuous light emission
Alternative term: cw operation
Category:
laser devices and laser physics
Related: modes of laser operationquasi-continuous-wave operationresonator modesself-terminating laser transitions
Page views in 12 months: 1674
DOI: 10.61835/n8h Cite the article: BibTex BibLaTex plain textHTML Link to this page! LinkedIn
Content quality and neutrality are maintained according to our editorial policy.
Contents
What is Continuous-wave Operation of Lasers?
Continuous-wave (cw) operation of a light source means that it is continuously operated, i.e., not pulsed. The term is most frequently applied to lasers but also to gas discharge lamps, for example.
For a laser, continuous-wave operation implies that it is continuously pumped and continuously emits light. The emission can occur in a single resonator mode (→ single-frequency operation) or in multiple modes.
The first continuous-wave laser was a helium–neon laser operating at 1153 nm [1]. A version working with the now common emission wavelength of 632.8 nm was demonstrated soon after that. Later on, many other types of lasers were developed which can also be operated continuously: other gas lasers, many types of solid-state lasers (including semiconductor lasers), and dye lasers.
Figure 1: A simple continuous-wave laser consists only of a diode-pumped laser head and two mirrors around it. Source: Cutting Edge Optronics.
For many lasers with low-gain laser transitions, continuous-wave operation is difficult to achieve, while operation with pulsed pumping is easy to obtain. In some cases, continuous-wave operation is only possible with fiber lasers, but not with bulk lasers, as the fiber geometry greatly increases the gain efficiency. Some so-called self-terminating laser transitions are not suitable at all for continuous-wave operation, or only with additional measures.
The output power of a continuous-wave laser is approximately constant on longer time scales, but it can exhibit substantial power variations e.g. due to mode beating (if single-frequency operation is not achieved) and other kinds of laser noise. Various techniques for the stabilization of lasers concerning output power and/or optical frequency can be applied, often involving additional optical elements in or around the laser resonator.
Quasi-continuous-wave Operation
In continuous-wave operation, some lasers would exhibit too strong heating of the gain medium. The heating can then be reduced by quasi-continuous-wave operation, where the pump power is only switched on for limited time intervals, but long enough to reach steady-state optical conditions. The latter implies that the on time is much longer than the relaxation oscillation damping time.
Continuous-wave Mode Locking
Some lasers are called continuous-wave mode-locked. This means that the laser is mode-locked, and the pulse energy (or average power) is constant, i.e. there is no Q-switched mode locking. Despite the emission of pulses, mode locking can be considered as a kind of continuous-wave operation in the sense that the resonator modes are excited with constant powers.
Frequently Asked Questions
This FAQ section was generated with AI based on the article content and has been reviewed by the article’s author (RP).
What is continuous-wave (CW) operation of a laser?
Continuous-wave (CW) operation of a laser means that it is continuously pumped and continuously emits light, in contrast to pulsed operation.
Why can't all lasers be operated in continuous-wave mode?
Some lasers have low-gain or self-terminating laser transitions, or would get too hot for prolonged pumping, which makes continuous-wave operation difficult or impossible. For such lasers, pulsed pumping is often required.
What is quasi-continuous-wave operation?
Quasi-continuous-wave (QCW) operation is used for lasers that would overheat in true CW operation. The laser is pumped in intervals long enough to reach steady-state optical conditions, which reduces the average thermal load.
Bibliography
| [1] | A. Javan, W. R. Bennett Jr. and D. R. Herriott, “Population inversion and continuous optical maser oscillation in a gas discharge containing a He–Ne mixture”, Phys. Rev. Lett. 6 (3), 106 (1961); doi:10.1103/PhysRevLett.6.106 |
|---|
(Suggest additional literature!)
Questions and Comments from Users
Here you can submit questions and comments. As far as they get accepted by the author, they will appear above this paragraph together with the author’s answer. The author will decide on acceptance based on certain criteria. Essentially, the issue must be of sufficiently broad interest.
Please do not enter personal data here. (See also our privacy declaration.) If you wish to receive personal feedback or consultancy from the author, please contact him, e.g. via e-mail.
By submitting the information, you give your consent to the potential publication of your inputs on our website according to our rules. (If you later retract your consent, we will delete those inputs.) As your inputs are first reviewed by the author, they may be published with some delay.