Optipedia • SPIE Press books opened for your reference.
Dye Lasers
Excerpt from Field Guide to Lasers
A dye can selectively absorb light with certain wavelengths corresponding to certain electronic transitions. However, it may also emit fluorescence and even exhibit laser gain. A wide range of emission wavelengths—from the ultraviolet to the near-infrared region—is accessible with different laser dyes, most often used in a liquid solution. They offer a broad gain bandwidth and thus broad wavelength tunability as well as the potential for ultrashort pulse generation with passive mode locking (see p. 107). Upper-state lifetimes are typically a few nanoseconds, and the gain per unit length can be rather high (on the order of 103/cm).
Most dye lasers use a thin jet (with or without a thin cuvette) of dye solution. The dye molecules are exposed to the pump light only for a short time interval. From time to time, the dye solution has to be exchanged because it degrades during operation. The laser resonator may contain a birefringent tuner (or some other kind of tuner) for adjusting the emission wavelength.
There are also dye lasers that utilize a large volume of dye solution pumped with a flash lamp or a Q-switched laser. Such dye lasers can generate pulses with many millijoules.
While dye lasers have dominated the fields of tunable lasers and ultrashort pulse generation for a long time, they have been largely replaced by solid-state lasers (often based on Ti:sapphire), which avoid the disadvantages of handling poisonous dye solutions, a limited lifetime, and limited output power. However, dye lasers are still used in some areas, such as spectroscopy with wavelengths that are otherwise hard to generate.
Properties of Dye Lasers
Aspect | Properties |
important types | continuous-wave or mode-locked Rhodamine 6G lasers; flashlamp-pumped lasers with various dyes |
applications | spectroscopy; ultrashort pulse generation |
pump sources | other lasers or flash lamps |
power efficiency | a few percent to an order of 50% |
accessible wavelengths | mostly visible and near infrared |
wavelength tuning | possible over tens of nanometers |
average output power | typically between 10 mW and 1 W, but >1 kW is possible |
beam quality | normally diffraction-limited; worse for pulsed high-power devices |
continuous-wave operation | yes |
nanosecond pulse generation | yes, with pulsed pumping |
picosecond & femtosecond pulse generation | yes, with mode locking |
R. Paschotta, Field Guide to Lasers, SPIE Press, Bellingham, WA (2008).
View SPIE terms of use.