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Encyclopedia of Laser Physics and Technology

© Dr. Rüdiger Paschotta

Last update: 2008-04-03

Definition: solid-state lasers based on tungstate crystals as gain media

Before the development of Nd:YAG, Nd³⁺:CaWO₄ was a very important rare-earth-doped laser gain medium. It was in fact used in the first continuously operating crystal laser. However, once Nd³⁺:YAG was commercially available, the interest in CaWO₄ dropped sharply. In later years, certain other tungstate crystals started to receive a lot of attention.

Tungstate Crystal Materials

Monoclinic Double Tungstates

Various ytterbium-doped monoclinic double tungstates Yb³⁺:KGd(WO₄)₂ (Yb:KGW, potassium gadolinium tungstate) and Yb³⁺:KY(WO₄)₂ (Yb:KYW, potassium yttrium tungstate) have become particularly popular. Also under consideration is Yb³⁺:KLu(WO₄)₂ (Yb:KLuW, also called Yb:KLW). Besides, other rare-earth dopants can be used in tungstates, for example neodymium (Nd³⁺), erbium (Er³⁺), thulium (Tm³⁺), and praseodymium (Pr³⁺).

Tetragonal Double Tungstates

Another interesting group of crystals is that of tetragonal double tungstates such as Yb³⁺:NaGd(WO₄)₂ (Yb:NGW) [7] and Yb³⁺:NaY(WO₄)₂ (Yb:NYW). Unlike their monoclinic cousins, the tetragonal tungstates are disordered crystal materials, where e.g. the Na⁺ and Gd³⁺ ions are randomly distributed on the same type of lattice sites. As the dopant ions (e.g. Yb³⁺) replace the other rare-earth ions (e.g. Gd³⁺), this disordered structure results in inhomogeneous broadening and thus to a broader gain bandwidth. Some of these crystals can be grown with good quality only when using sophisticated (and often slow) growth methods, whereas others (e.g. the two mentioned above) are suitable for the common Czochralski method.

Properties of Rare-earth Doped Tungstates

Rare-earth-doped tungstate crystals have a number of special properties:

• The gain bandwidth e.g. of Yb:KGW and Yb:KYW is very large compared to that of Yb:YAG. This allows for wide wavelength tunability and for much shorter pulse durations from mode-locked lasers. Values well below 100 fs have been achieved with passive mode locking.
• Compared with other ytterbium-doped gain media (crystals or glasses) with similarly high gain bandwidth, ytterbium-doped tungstates have rather high emission cross sections. This is essential for passive mode locking, since it helps to avoid Q-switching instabilities.
• While ytterbium-doped gain media generally exhibit a small quantum defect, ytterbium-doped tungstates allow for particularly small values. For example, a 1030-nm Yb:YAG laser would normally be pumped around 940 nm, whereas Yb:KGW or Yb:KYW could be most efficiently pumped around 981 nm. At the same time, a shorter laser wavelength can be obtained; it is possible to operate with a quantum defect well below 1%. As a consequence, the heat generation can be so small that this partly compensates the lower thermal conductivity.
• For tungstates, the ytterbium doping concentration can be very high without significant quenching, because the replaced ions have a very similar ion radius. An example for this is Yb:KYW, which actually becomes KYbW = Yb:KYb(WO₄)₂ for 100% ytterbium doping. It is not clear, however, whether such high doping levels can be utilized in lasers.
• The thermal conductivity of common double tungstates is of the order to 3 to 4 W/(K m) – which is not bad compared to other laser crystals (although several times less than for YAG), and quite large compared to the thermal conductivity of typical glasses. The comparison to glasses is appropriate since the large gain bandwidth allows e.g. tungstate femtosecond lasers and tunable lasers to compete with glass lasers.
• The monoclinic crystal structures results in a natural birefringence, helping to avoid thermally induced polarization rotation and depolarization loss.
• Tungstates tend to have high Raman coefficients. Therefore, they can generate significant Raman gain at moderate optical intensities. It is possible to use the laser crystal itself as a Raman converter.

For some applications, tungstates offer a combination of various useful properties. In particular for passive mode locking, ytterbium-doped double tungstates are often superior over other media in terms of the combination of high gain bandwidth, high cross sections, and relatively good thermal properties – even though in each particular discipline, better materials could be found. Even for continuous-wave high-power thin-disk lasers, tungstates offer advantages over Yb:YAG in terms of efficiency, although the fabrication of thin disks from such materials is not easy. (Yb:YAG is certainly easier to handle.) A passively mode-locked thin disk Yb:KYW laser [4] has probably generated the highest output power in sub-300-fs pulses which has been achieved with a bulk laser with no amplifier.

Bibliography

See also: rare-earth-doped gain media, YAG lasers, ytterbium-doped gain media, cross sections

Categories: lasers, materials