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The FRT FTR bases on the superposition of light beams reflected at the boundaries of a thin film. The evaluation of the spectral interference pattern of the superposed light beams results in the film thickness. This measured reflectance spectrum is compared with a calculated one, where the unknown thickness is systematically varied until both spectra match. | |  | | | - measurement of thin films by spectral reflectance
- non-destructive, non-contact, high-resolution measurement
(10nm – 100µm) in less than a few seconds - measurement of single or multi-layer films
| |  | | | - measurement of thickness of oxides, nitrides, photoresist and other semiconductor process films
- measurement of antireflection coatings and antiscratch coatings
- measurement on opaque substrates e.g. aluminum, brass, ceramics, copper, steel and plastics
- measurement of thin films in the optics industry
- measurement of lacquers and thin foils
|  | | | | model | VIS | NIR | VIS/NIR | UV/VIS | UV/VIS/NIR | | wavelength | 400 nm – 850 nm | 650 nm – 1100 nm | 400 nm – 1100 nm | 250 nm – 850 nm | 250 nm – 1100 nm | | measuring range | 50 nm – 20 µm | 70 nm – 70 µm | 50 nm – 100 µm* | 10 nm – 20 µm | 10 nm – 70 µm | | light source | halogen | deuterium halogen | | resolution thickness | 1 nm | | resolution x,y | 200 µm - 800 µm without extra optic (better than 10 µm with extra optic) | *optional 1 μm - 20 μm Technical specifications and content are subject to change. |
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