Carl-zeiss-stiftung

Klaus Freischlad

Michael Kuchel

Karl-Heinz Schuster

Andreas Dorsel

Uwe Vry

The invention relates to an evaluation method for interferograms and an interferometer corresponding thereto with which tile influence of coherent noise is reduced with simultaneously high interference contrast. Several phase maps are computed from interferograms which are recorded with coherent light. The interferogram components of the test object and the interferogram components of the coherent noise are displaced relative to each other in the camera plane between recording the interferograms. The influence of the coherent noise is suppressed by subsequently averaging the phase maps.

Method for evaluating interferograms and interferometer therefor

Described are a method and apparatus for the optical testing of samples in which a camera records a plurality of images of an interferogram or a bar pattern. Phase values are determined for each image point of each camera record, and then differences between the phase values of adjacent points in each image line and column are computed in modulo 2.pi.. These differences for each image point are summed over the plurality of camera images. After a number of images sufficient to assure desired accuracy have been summed, a single discontinuity elimination is carried out. This permits the rapid averaging of measurements over the plurality of camera images in real video time and remarkably reduces the measuring time and statistical errors.

Method and apparatus for optical testing of samples

The optical testing method of the invention permits the reliable elimination of discontinuities, i.e., the determination of the integer values of modulo 2.pi. phase differences, even when the measured data includes seriously noisy signals. The intensity signals from a two-dimensional raster of camera image points are used to compute differences in phase values between adjacent image points in lines, as well as between adjacent image points in columns. The phase differences are summed along a closed path around each of a plurality of partial fields which are delineated by a predetermined set of adjacent image points. A filter (21) searches the vector field of these phase differences; and those partial fields where vortexes exist, i.e., each field for which the sign-correct sum along its closed path is not zero, are masked, thereby creating holes in the image pattern. Additional closed paths are summed around these holes and, by masking further image points between these holes, the masked partial fields are combined until the path integral around each of these combined holes disappears. The final phase value data used for display of a phase map of the sample is calculated by path integration of the unmasked image points; and inconsistent measured values, e.g., due to noisy signals, do not corrupt the phase map.

Method for optical testing of samples

The injection current for a laser diode is modulated so that a pregiven coherence function is obtained which drops off continuously at both ends outside of the coherence length. Several laser diodes are used for a very short coherence length for which the modulated wave numbers of the emitted radiation follow one another or overlap.

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Aalen, Germany

Klaus Freischlad