Abstract

Mechanical polishing of glass is a time consuming process especially for lenses deviating from spherical surface such as aspheres. With laser polishing, the processing time can be significantly reduced and the wear of hard tooling can be avoided. Using laser radiation for polishing, a thin surface layer of the glass is heated up just below evaporation temperature due to the interaction of glass material and laser radiation. With increasing temperature, the reduced viscosity in the surface layer leads to the reduction of the roughness due to the surface tension. Hence, a contactless polishing method can be realized nearly without any loss of material or need of polishing agent. In this paper, results for laser polishing of fused silica, BK7, and S-TIH6 are presented with area rates up to 5 cm2/s. However, the results show that the achieved roughness with laser polishing is strongly influenced by the thermal properties of the type of glass. During laser polishing, the glass material is relocated at the surface, thus no shape errors can be corrected. To reduce the residual waviness and shape errors after laser polishing, the authors investigated a further laser-based process step (laser beam figuring, LBF) which ablates material for a shape correction. Ablation depths <5 nm allow a high precision laser ablation for selective processing. For both processes, a CO2 laser is used.

Highlights

  • Mechanical polishing of glass is a time consuming process especially for lenses deviating from spherical surface such as aspheres

  • The glass material is relocated at the surface, no shape errors can be corrected

  • Richmann et al and Hildebrand et al.3,4 investigated laser polishing with a quasiline with cw CO2 laser radiation

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Summary

STATE OF THE ART

Research has already been conducted on laser polishing of fused silica since 1982 by Temple. Using defocused cw CO2 laser radiation and a meandering scanning strategy, an initial roughness of rms 1⁄4 0.33 nm could be reduced by Temple to rms 0.27 nm (measuring field 500 Â 400 lm). Due to a fast movement of the defocused laser beam (dS > 6 mm), a homogenous temperature distribution in the quasiline on the surface was achieved Using this quasiline for polishing an initial roughness Sa in the range of 300–700 nm on flat fused silica samples was reduced to a Sa value below 15 nm.. The economic efficiency is significantly reduced by using another technology after laser polishing to finish optics with high precision and low roughness. In this paper, another approach to correct the lens shape is applied by using the same laser source that is used for laser polishing. Ultrashort pulse laser radiation. both methods possess poor reproducibility and low spatial lateral resolution (>250 lm (Ref. 22)), which are not yet sufficient for shape correction

Laser polishing
Laser beam figuring
Laser polishing of optical glass
Shape correction
CONCLUSION AND OUTLOOK

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