Abstract:
Fourier domain a/LCI (faLCI) system and method which enables in vivo data acquisition at rapid rates using a single scan. Angle-resolved and depth resolved spectra information is obtained with one scan. The reference arm can remain fixed with respect to the sample due to only one scan required. A reference signal and a reflected sample signal are cross-correlated and dispersed at a multitude of reflected angles off of the sample, thereby representing reflections from a multitude of points on the sample at the same time in parallel. Information about all depths of the sample at each of the multitude of different points on the sample can be obtained with one scan on the order of approximately 40 milliseconds. From the spatial, cross-correlated reference signal, structural (size) information can also be obtained using techniques that allow size information of scatterers to be obtained from angle-resolved data.
Abstract:
The measurement accuracy of an apparatus for measuring the surface shape of an object utilizing a two-wavelength phase-shift interferometry is improved. A low-coherence light source, a plurality of wavelength filters with different transmission wavelengths, an angle control unit and an analysis unit are provided. When performing a two-wavelength phase shift method, the analysis unit detects the wavelength difference between two wavelengths, and corrects a calculated wavelength value and a calculated phase value of one of the wavelengths for preventing a fringe-order calculation error. Next, the angle of the wavelength filters is controlled for making the actual wavelength difference coincident with a designed value. Thus, the wavelength difference between the two wavelengths is continuously controlled to be constant, which enables measurements of surface shapes with high accuracy, even when there are wavelength fluctuations due to the temperature change or the time elapse.
Abstract:
An apparatus for measuring a layered object comprising a low coherence light source, a coherent light source, and an interferometer including a reference arm and a measurement arm. The reference arm is comprised of a first section of polarization maintaining optical fiber engaged with a first fiber stretcher. The measurement arm is comprised of a second section of polarization maintaining optical fiber engaged with a second fiber stretcher. The first and second fiber stretchers are driven so as to alternatingly vary the lengths of the first section of polarization maintaining optical fiber and the second section of polarization maintaining optical fiber, thereby causing interference signals with the low coherence light when the length of the reference arm is equal to the length of the measurement arm including the distance from the second section of polarization maintaining optical fiber to any of the surfaces of the layers of the object.
Abstract:
In general, in a first aspect, the invention features a system including an interferometer configured to direct test light to an overlay target and subsequently combine it with reference light to form an interference pattern, the test and reference light being derived from a common source, a multi-element detector, one or more optics to image the overlay target on the multi-element detector; and an electronic processor in communication with the multi-element detector. The overlay target includes a first pattern and a second pattern and the electronic processor is configured to determine information about the relative alignment between the first and second patterns.
Abstract:
An interference measuring device comprises light sources lenses, an aperture, an optical multiplexer, an optical branching filter, a half mirror, an imaging unit, an analyzing unit, a light receiving unit, a displacement detecting unit, a piezoelectric actuator, a drive unit, a mirror, a stage, a drive unit, and a control unit. According to a result of optical path length difference detection by the displacement detecting unit, the control unit controls optical path length difference adjusting operations by the piezoelectric actuator and stage through the drive units such that the optical path length difference becomes a plurality of target values in sequence. The control unit subjects the moving operation by the piezoelectric actuator to a feedback control such that the optical path length difference becomes each of the target values upon the moving operation by the stage as well.
Abstract:
An apparatus for the absolute measurement of a two dimensional optical path distribution comprising: a light source (4) for illuminating an object (26) with light having a plurality of wavelengths: an interferometer (12) for forming an image of at least part of the object, which image comprises a broad band interferogram; a hyperspectral imager (30) in optical communication with the interferometer for spectrally separating the broad band interferogram into a plurality of narrow band two dimensional interferograms (72, 74, 76); a register (38) for spatially registering the narrow band interferograms; an extractor for extracting one dimensional intensity signals from corresponding pixels in each narrow band interferogram; and a calculator (100) for calculating the frequency for each point on the object from a one dimensional intensity signal associated with that point.
Abstract:
A method for measuring spacings between optical surfaces of a multi-lens optical system includes detecting the centring state of the optical system by taking into consideration all optical surfaces of the optical system. Then the optical system is adjusted in such a way, taking the centring state into consideration, that the optical axis of the optical system is aligned as far as possible with a reference axis. In a next step the spacings between the optical surfaces are determined with the aid of a short-coherence interferometer. The measuring-light ray directed onto the optical system for this purpose runs likewise along the reference axis.
Abstract:
Provided is a temperature measuring method which can accurately measure a temperature of an object to be measured compared to a conventional method, even if a thin film is formed on the object. The temperature measuring method includes: transmitting a light from a light source to a measurement point of an object to be measured, the object being a substrate on which a thin film is formed; measuring a first interference wave caused by a reflected light from a surface of the substrate, and a second interference wave caused by reflected lights from an interface between the substrate and the thin film and from a rear surface of the thin film; calculating an optical path length from the first interference wave to the second interference wave; calculating a film thickness of the thin film based on an intensity of the second interference wave; calculating an optical path difference between an optical path length of the substrate and the calculated optical path length, based on the calculated film thickness of the thin film; compensating for the optical path length from the first interference wave to the second interference wave based on the calculated optical path difference; and calculating a temperature of the object at the measurement point based on the compensated optical path length.
Abstract:
A shape measuring apparatus includes: an optical system configured to guide a light from a light source having a wideband spectrum to an object to be measured and a reference face; an imaging unit configured to image the interfering light intensity distribution image output from the optical system; an optical path length difference changing unit configured to change the optical path length difference; and an arithmetic processing unit configured to obtain the peak value of an interfering light intensity sequence indicating the change in the interfering light intensity due to the change in the optical path length difference at each measurement position of the interfering light intensity distribution images stored in the image storing unit, and configured to obtain the peak value as the position in the direction of the optical axis at each measurement position of the object to be measured.
Abstract:
A spectral interferometry apparatus and method are disclosed, that can be used to monitor or measure an unknown length by following a characteristic of an indicating signal. The measurement is performed by adjusting an optical path difference (OPD) in an interferometer until sound or light or both are obtained with the desired strength and pitch. Embodiments are presented where the unknown length is the eye length. Sound of different pitches are produced by scanning the channeled spectrum output of an interferometer with the object returning at least one of the interferometer optical signals. The scanning is performed by reading the signal of an analogue photodetector array driven by a nonlinear clock or by tuning a low cost swept source using a distorted driving signal.