|
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 | 20 nm – 20 µm | 20 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) |
Technical specifications and content are subject to change.
|
|
|