<%@ Language=VBScript %> Home
All contents copyright © ST Instruments B.V. 2006
Last update 16-06-2007
News&Events Support Home About Contact us

Links

 SPM / AFM
 Optical profilers
 Stylus profilers
 Thin film metrology
 Mechanical testing
 Surface analysis
 Analyse software
 
Interferometry has been a technique in existence for more than one hundred years and consists of viewing the optical path difference between a sample beam and a reference beam; the beams undergo constructive and destructive interference and this results in a pattern of bright and dark fringes. In the case of an interference microscope, the objective lens is coupled with a beam splitter so that some of the light is reflected from a reference mirror at 90 degrees (Michelson type) or co-linear with the light path (Mirau type) see figure.

Illumination from a white light beam passes through a filter, then through a microscope objective lens to the sample surface. The light reflecting back from the surface recombines with the reference beam and interference fringes are formed. The pattern of these fringes is captured on a CCD camera array. If the sample is a perfectly flat mirror but tilted, and the illumination is by monochromatic light then the resulting interference pattern will be a series of fringes. The distance between the maximum of the dark or light fringes is proportional to the wavelength of light used and the tilt of the mirror. Each band in the interference pattern represents a contour height difference of half the wavelength of light used in the measurement. The contour bands are purely sinusoidal and the phase of the interference fringe pattern can be measured to very high accuracy.  

Two techniques of interferometry are described, Phase Shift Interferometry (PSI) and Vertical Scanning Interferometry (VSI). 
Phase Shift Interferometers have been developed to measure the surface height of very smooth and continuous surfaces with sub-nanometer resolution. The sample, which must be in focus, is scanned vertically in a few steps, which are a very precise fraction of the wavelength. The profiling algorithms produce a phase map of the surface, which is converted to the corresponding height map by means of a suitable unwrapping procedure. PSI profiling provides sub-nanometer vertical resolution for all NA. Very low magnifications (2.5X) can be employed to measure large fields of view with the same height resolution. However, the measurement range is limited by the coherence length to a few micrometers. PSI algorithms enable to profile shape features on the nanometer scale, as well as to assess texture parameters of super smooth surfaces on the sub-nanometer scale.

White-light vertical scanning interferometers have been developed to measure the surface height of smooth to moderately rough surfaces. Maximum fringe contrast occurs at the best focus position for each point on the surface of the sample. The sample is scanned vertically in steps so that every point on the surface passes through the focus. The height of the surface at each pixel location is found by detecting the peak of the narrow fringe envelopes. VSI profiling provides nanometer vertical resolution for all NA. The VSI algorithms enable to use all the available magnifications to profile shape features with the same height resolution. The measurement range is intrinsically unlimited although in practice it is limited. Scan speeds and data acquisition rates can be very fast, although this leads to a significant loss of vertical resolution.



   
 
Confocal
Interferometry
Dual-head
Point sensor
Topomicroscopy
Digital Holography
Back
   
   
   
   
   
   
   
   
   

 

 
top