Abstract:
A surface state monitoring method and apparatus for performing in-situ monitoring of surface states of semiconductor substrates. The apparatus comprises condensing means 30 for condensing infrared radiation to an outer peripheral part of the substrate-to-be-monitored; control means 80 for controlling an incident angle of the infrared radiation condensed by the condensing means 30; condensing means 40 for condensing the infrared radiation which has undergone multiple reflection in the substrate-to-be-monitored; detecting means 50 for detecting the infrared radiation condensed by the infrared radiation condensing means 40, and analyzing means 60 for analyzing the detected infrared radiation detected and measuring contaminants staying on the surfaces of the substrate-to-be-monitored.
Abstract:
A transform spectrometer determines the spectrum of light based on the Talbot effect. Light to be analyzed is passed through a spatially periodic object, thereby generating a series of Talbot images. The intensities of these Talbot images at different optical distances from the spatially periodic object are then detected, and Fourier transformed to determine the spectrum of the light. Preferably, the detector comprises a spatial masking pattern such that the intensities detected are maximized at Talbot planes or at the midpoints between Talbot planes. In one embodiment, the optical distance between the spatially periodic object and the detector is changed in order to detect image intensities at different Talbot planes. In another embodiment, the detector and the spatially periodic object are positioned along a common optical axis at relative angle null such that different detector rows detect intensities at different Talbot planes. In yet another embodiment, the spatially periodic object is both a grating and a detector, and the Talbot images generated by the grating are reflected off a mirror back to the detector.
Abstract:
A procedure is described to calibrate an optical converter (1), especially for use in the field of reflectrometric interference spectroscopy. The converter (1) has a layer/substrate system with a layer (2) and a substrate (3). A light beam (4) shines from the substrate (3) side, and parts of it are reflected (8-10) or transmitted (11) at the interfaces of air/substrate (5), substrate/layer (6) and layer/air (7). The converter (1) in particular serves to convert the light beam (4) into a modulated (especially frequency modulated or phase modulated) signal. The light (4) is varied within a wavelength or frequency range from which a corresponding modulated spectrum is determined. In particular, it is assumed that the performance quantities of especially the converter and a radiation source generating the light (4) are subject to temporal fluctuations. The calibration is carried out in particular by determining reference values of the modulated spectrum at time tnull0, successively determining values of the modulated spectrum for times t>0, and calculating temporal changes in the modulated spectrum for t>0 using in particular a linear disturbance equation based on the assumed infinitisimal changes in at least one of the performance quantitieso the interference spectroscopy measuring setup.
Abstract:
Devices and techniques for performing highly-sensitive spectroscopic measurements in a sample vapor by using a four-wave-mixing optical system and an atomizer chamber. One embodiment of a spectrometer comprises a gas-phase atomizer having an atomizer chamber operable to vaporize a sample solution to produce a sample vapor, first and second alignment templates having apertures to align a probe beam, first and second pump beams to form a four-wave mixing configuration, a laser tunable to generate a laser beam at a desired wavelength corresponding to an absorption line in the sample vapor, and a set of optical elements disposed relative to the laser and the atomizer to split the laser beam into the probe beam, the first pump beam, and the second pump beam. The probe beam, the first and second pump beams are directed to overlap with one another in the sample vapor to produce a signal beam through a four-wave mixing process.
Abstract:
A method for standardizing a spectrometer generating an optical spectrum from a sample, comprising generating at least one optical spectrum from at least one standardization sample each having a chemical composition resulting in the optical spectrum showing a characteristic pattern in a predetermined frequency range, comparing information relating to the pattern(s) to corresponding information relating to at least one reference pattern previously defined as the desired standard response from the at least one standardization sample, determining, based on the comparison, standardizing parameters describing the transition of the pattern(s) of the generated spectrum or spectra to the reference pattern(s) and storing said standardizing parameters in the spectrometer or a computer connected thereto, so that the spectrometer, when presented to an unknown sample, will, using the standardization parameters, generate an optical spectrum substantially identical to that which would be generated in a corresponding spectrometer standardized with a sample of the same chemical composition using the same previously defined reference pattern(s). The present method relates to standardization of the instrument to a well-defined state into which any number of instruments may be brought. In this state, calibrations may be transferred freely from instrument to instrument.
Abstract:
A method of obtaining an FT spectrum according to Brault is improved in that the compensation filter is determined by recording a broad-band effective interferogram, carrying out complex Fourier transformation, forming a mean value of the phase spectra, converting the abscissa values into electrical frequencies, and establishing the transfer function of the detector and of the further signal processing elements, wherein the free parameters of the transfer function are chosen such that the phase response of the transfer function deviates as little as possible from the mean value of the phase spectrum of the effective recorded interferogram. If necessary, the determined transfer function is then digitized. The compensation filter is then determined as the inverse of the discrete transfer function. In this way, deconvolution of the signal processing elements transfer function from the spectra is facilitated in a particularly simple and effective manner.
Abstract:
A novel variation of Michelson's interferometer uses tilt- and shear-compensation optics to allow various mirror motions to produce variation of path difference. The tilt-compensation mechanism consists of two complementary reflections from a single plane mirror to produce a beam having a constant angle of propagation, typically the same as the input beam. Using a retroreflector to invert the image of the single plane mirror before the second reflection produces the complementary reflections. A particularly efficient embodiment of the present invention uses a balanced disk-shaped mirror to effect very rapid variation of path difference by nutation or precession. Other advantages of tilt-compensation include photometric stability. This interferometer has applications in spectrometry, spectral imaging and metrology.
Abstract:
An optical system for determining aberration in a source beam by comparison of a test beam with a reference beam. The optical system includes a test source for producing a source beam having a spacial intensity distribution including an aberration component, a wavefront analyzer for processing a fringe signal associated with the aberration component, and an interferometer. The interferometer is provided with a beamsplitter for splitting the source beam into a test beam and a reference beam, an imaging device for detecting the test beam and the reference beam, and a mirror disposed in a test beam path for reflecting the test beam toward the imaging device. The interferometer also includes a micromirror disposed in a reference beam path for reflecting a portion of the reference beam toward the imaging device and a piezoelectric translator operatively linked to the mirror and controlled by the wave front analyzer. The mirror is capable of moving relative to the path of the test beam. The micromirror has a lateral dimension not exceeding the approximate lateral dimension of a central lobe of the reference beam as focused thereon by focusing means so that when the test beam is reflected by the mirror and the portion of the reference beam is reflected by the micromirror, the reflected test beam and the reflected portion of the reference beam are both incident upon the imaging device forming an interference pattern including fringes which are converted into the fringe signal.
Abstract:
When positioning a sample, a sample position adjusting light source section with a long coherence length is inserted into an optical system, and the sample position is adjusted such that the interference fringe pattern observed becomes a predetermined pattern, whereby the position of a surface to be inspected can be easily set within a coherence range in a simple configuration in a light wave interference apparatus using light with a short coherence length. When a sample position adjusting light source section (31) is inserted into the optical system, a light beam with a long coherence length, which has been turned into divergent light, is irradiated on each of a reference surface (4a) and a surface to be inspected (5a), whereby spherical waves reach these two surfaces (4a, 5a). These two divergent light beams are respectively reflected by the reference surface (4a) and the surface to be inspected (5a) so as to become a reference light component and an inspection light component, which are then recombined together by a light-splitting surface (3a) of a beam splitter (3) while interfering with each other, thereby forming an interference fringe on a CCD (8). This interference fringe comprises a pattern of concentric circles. The sample (5) is moved by a minute distance in the optical-axis direction (B) so as to reduce the number of fringes, and then is stopped at the time when the circular interference fringe pattern disappears.
Abstract:
A method and apparatus for measuring partial pressures of gaseous components within a mixture. The apparatus comprises generally at least one tunable laser source, a beam splitter, mirrors, optical filter, an optical spectrometer, and a data recorder. Measured in the forward direction along the path of the laser, the intensity of the emission spectra of the gaseous component, at wavelengths characteristic of the gas component being measured, are suppressed. Measured in the backward direction, the peak intensities characteristic of a given gaseous component will be wavelength shifted. These effects on peak intensity wavelengths are linearly dependent on the partial pressure of the compound being measured, but independent of the partial pressures of other gases which are present within the sample. The method and apparatus allow for efficient measurement of gaseous components.