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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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