Abstract
The laser transitions 4F3/2-4I9/2 of Nd-doped materials are of great interest for blue laser radiation generation using frequency doubling. The emission wavelength of Nd:YVO4 at 914 nm1 is considerably shorter than the corresponding wavelength of Nd:YAG at 946 nm.2 The second harmonic at 457 nm represents actually the ideal “blue” providing the greatest colour gamut in additive mixing of the primary colours. Bright laser displays are consequently one application of this system. Apart from this, the laser can be also used as powerful replacement of Dye lasers or as allsolid-state solution for precision spectroscopy, such as optical clocks based on Mg-atoms.3 Another advantage of Nd: YVO4 is the higher absorption cross section for pumping with laser diodes at 808 nm wavelength. Laser operation of Nd:YVO4 imposes however higher demands on pump power density and effective cooling of the crystal than Nd:YAG as the population of the lower laser level is considerably higher and the thermal properties (thermal conductivity) are less favourite. For both reasons, the thin disk laser design4 seems to be the most suitable choice for operation of Nd doped materials with wavelengths below 950 nm.
© 2002 Optical Society of America
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