Nd:YAG Laser: Bohren und Gravieren - Fakultät 06 - Hochschule ...
Nd:YAG Laser: Bohren und Gravieren - Fakultät 06 - Hochschule ...
Nd:YAG Laser: Bohren und Gravieren - Fakultät 06 - Hochschule ...
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<strong>Nd</strong>:<strong>YAG</strong> <strong>Laser</strong>: <strong>Bohren</strong> <strong>und</strong> <strong>Gravieren</strong><br />
Version 3.1<br />
and frequency quadrupling, respectively. Other emission lines are at 946, 1123, 1319, 1338<br />
and 1444 nm. When used at the 946-nm transition, <strong>Nd</strong>:<strong>YAG</strong> is a quasi-three-level gain<br />
medium, requiring significantly higher pump intensities.<br />
<strong>Nd</strong>:<strong>YAG</strong> is usually used in monocrystalline form, fabricated with the Czochralski growth<br />
method, but there is also ceramic (polycrystalline) <strong>Nd</strong>:<strong>YAG</strong> available in high quality and in<br />
large sizes. For both monocrystalline and ceramic <strong>Nd</strong>:<strong>YAG</strong>, absorption and scattering losses<br />
within the length of a laser crystal are normally negligible, even for relatively long crystals.<br />
Typical neodymium doping concentrations are of the order of 1 at. %. High doping<br />
concentrations can be advantageous e.g. because they reduce the pump absorption length, but<br />
too high concentrations lead to quenching of the upper-state lifetime e.g. via upconversion<br />
processes. Also, the density of dissipated power can become too high in high-power lasers.<br />
Note that the neodymium doping density does not necessarily have to be the same in all parts;<br />
there are composite laser crystals with doped and <strong>und</strong>oped parts, or with parts having different<br />
doping densities.<br />
Property Value<br />
chemical formula <strong>Nd</strong> 3+ :Y3Al5O12<br />
crystal structure cubic<br />
mass density 4.56 g/cm 3<br />
Moh hardness 8–8.5<br />
Young's modulus 280 GPa<br />
tensile strength 200 MPa<br />
melting point 1970 °C<br />
thermal conductivity 10–14 W / (m K)<br />
thermal expansion coefficient 7–8 × 10 −6 /K<br />
thermal shock resistance parameter 790 W/m<br />
birefringence none (only thermally induced)<br />
refractive index at 1<strong>06</strong>4 nm 1.82<br />
temperature dependence of refractive index 7–10 × 10 −6 /K<br />
<strong>Nd</strong> density for 1 at. % doping 1.36 × 10 20 cm −3<br />
fluorescence lifetime 230 μs<br />
absorption cross section at 808 nm 7.7 × 10 −20 cm 2<br />
emission cross section at 1<strong>06</strong>4 nm 28 × 10 −20 cm 2<br />
gain bandwidth 0.6 nm<br />
Table 1: Some properties of <strong>Nd</strong>:<strong>YAG</strong> = neodymium-doped yttrium aluminum garnet.<br />
Other <strong>Laser</strong>-active Dopants in <strong>YAG</strong><br />
In addition to <strong>Nd</strong>:<strong>YAG</strong>, there are several <strong>YAG</strong> gain media with other laser-active dopants:<br />
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