Abstract:We present a fast white-light interference method for measuring surface depth profiles at nanometer scales. Previously reported white-light profilers have relied either on path difference scanning or on spectral analysis of the reflection from a fixed interferometer. We show that by performing this spectral analysis with an imaging Fourier transform spectrometer, the high speed of spectral techniques may be combined with the simple data interpretation characteristic of the scanning method. Giving experimental … Show more
“…One method of determining surface height involves the use of a broad-spectral-width light source in an interferometer and measurement of the degree of modulation contrast as a function of path difference. [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15] Because of the large spectral bandwidth of the source, the coherence length of the source is short, so good contrast fringes will be obtained only when the two paths of the interferometer are closely matched in length. By looking at the sample position for which the fringe contrast is a maximum while the optical path difference is varied, one can determine the height variations across the sample.…”
Section: Introductionmentioning
confidence: 99%
“…Many excellent features of whitelight vertical scanning interferometry were published previously. [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15] Although this is a good technique for measuring many surfaces, it does not work especially well with step heights 16 that are less than the coherence length of the light source in use. The problem has been known as batwings because of the shape of the false information.…”
An interference fringe modulation skewing effect in white-light vertical scanning interferometry that can produce a batwings artifact in a step height measurement is described. The skewing occurs at a position on or close to the edge of a step in the sample under measurement when the step height is less than the coherence length of the light source used. A diffraction model is used to explain the effect.
“…One method of determining surface height involves the use of a broad-spectral-width light source in an interferometer and measurement of the degree of modulation contrast as a function of path difference. [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15] Because of the large spectral bandwidth of the source, the coherence length of the source is short, so good contrast fringes will be obtained only when the two paths of the interferometer are closely matched in length. By looking at the sample position for which the fringe contrast is a maximum while the optical path difference is varied, one can determine the height variations across the sample.…”
Section: Introductionmentioning
confidence: 99%
“…Many excellent features of whitelight vertical scanning interferometry were published previously. [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15] Although this is a good technique for measuring many surfaces, it does not work especially well with step heights 16 that are less than the coherence length of the light source in use. The problem has been known as batwings because of the shape of the false information.…”
An interference fringe modulation skewing effect in white-light vertical scanning interferometry that can produce a batwings artifact in a step height measurement is described. The skewing occurs at a position on or close to the edge of a step in the sample under measurement when the step height is less than the coherence length of the light source used. A diffraction model is used to explain the effect.
“…It has the disadvantage of utilizing mechanical scanning in the depth direction to localize the fringes in the vicinity of zero OPD, which is time consuming and permits measurement only for stationary objects [9]. As for WSI and SD-LCI, they belong to spectral interferometry, which takes advantage of spectral interference fringes for a wide range of wavelengths without any mechanical scanning [8,10,11].…”
We present a spectral domain low-coherence interferometry (SD-LCI) method that is effective for applications in on-line surface inspection because it can obtain a surface profile in a single shot. It has an advantage over existing spectral interferometry techniques by using cylindrical lenses as the objective lenses in a Michelson interferometric configuration to enable the measurement of long profiles. Combined with a modern high-speed CCD camera, general-purpose graphics processing unit, and multicore processors computing technology, fast measurement can be achieved. By translating the tested sample during the measurement procedure, real-time surface inspection was implemented, which is proved by the large-scale 3D surface measurement in this paper. ZEMAX software is used to simulate the SD-LCI system and analyze the alignment errors. Two step height surfaces were measured, and the captured interferograms were analyzed using a fast Fourier transform algorithm. Both 2D profile results and 3D surface maps closely align with the calibrated specifications given by the manufacturer.
“…As a consequence, scanning white-light interferometry (SWLI) has been extensively used for unambiguous distance measurement with nanometer resolution along the propagation direction of a light beam. The use of a low coherence light source combined with the scanning of one arm of the interferometer provided a very useful way of measuring surface profiles [3][4][5]. Different techniques were developed to increase the system resolution over the coherence length of the source [6] and continuously provide diverse solutions to a variety of configurations [7,8].…”
In this work we present the concept of wide band interferometry as opposed to white-light interferometry to introduce a thickness measurement method that gains precision when the bandwidth is reduced to an adequate compromise in order to avoid the distortions arising from the material dispersion. The use of the widest possible band is a well established dogma when the highest resolution is desired in distance measurements with white-light interferometry. We will show that the dogma falls when thickness measurements must be carried out due to material dispersion. In fact the precise knowledge of the frequency dependence of the refractive index is essential for adequate thickness retrieval from the optical experiments. The device we present is also useful to obtain the group refractive index that is necessary to calculate the absolute thickness value. As an example, we show the spreading of a silicone oil on a reference surface in real time.
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