Abstract:
An apparatus and method for differential spectral interferometry comprising providing an interferometer comprising a light source; employing an element to provide a dithered relative phase shift between target and reference arms of the interferometer, detecting output from the interferometer, demodulating signals received from the detector at different multiples of the dither frequencies, generating more than one real-valued interferograms from demodulated signals, and using the real- valued interferograms to obtain the complex spectral interferogram.
Abstract:
A method and system for determining a characteristic of an analyte in a biological sample. Disclosed in several exemplary embodiments are high-sensitivity low coherence interferometric (LCI) systems (instruments) for optical metrology, which in an exemplary embodiment are miniaturized for use in a variety of sensing and monitoring applications, including medical sensing such as non-invasive glucose monitoring and others. The instrument is miniaturized, using integrated optics components such as waveguides, splitters and modulators on a single substrate such as a LiNb03 (Lithium Niobate) chip. Exemplary embodiments may also involve the use of a "circulator" type of optical component, including a polarizing beam splitter and quaterwave plate, which can be combined with the light source and detector into a miniature module that prevents optical feedback into the light source while doubling the detected light. Alternatively, one or more isolators and a waveguide coupler may be employed in a similar module to accomplish the same purpose.
Abstract:
A method including comparing information derivable from a scanning interferometry signal for a first surface location of a test object to information corresponding to multiple models of the test objects, wherein the multiple models are parametrized by a series of characteristics for the test object. The information corresponding to the multiple models may include information about at least one amplitude component of a transform (eg. A Fourier transform) of a scanning interferometry signal corresponding to each of the models of the test object. In a second aspect the models correspond to a fixed surface height and they are parametrized by a series of characteristics different from the fixed surface height. In a third aspect the comparing comprises accounting for systematic contributions to the interferometry signal.
Abstract:
Techniques and systems for using optical interferometers to obtain full-field optical measurements of surfaces, such as surfaces of flat panels, patterned surfaces of wafers and substrates. Applications of various shearing interferometers for measuring surfaces are described.
Abstract:
OCT apparatus includes an interferometer, having an input beam splitter and a 50/50 output splitter. The splitting ratio of the input splitter may be optimized depending on the source power of light source and on the mismatch of the balanced receiver. The input splitter is a plate beam-splitter to minimize the stray reflected light in the interferometer and allow sequential operation of the apparatus in the OCT or in the confocal regime. The switching between the two regimes may be at will, or synchronous with the en-face scanning which results in quasi-simultaneous OCT/confocal imaging or in alternatives frames, confocal and OCT. By using polarization sensitive elements, two channels are provided in each regime, OCT and confocal. The two confocal polarization sensitive channels may allow adjustments of compensators prior to OCT measurements or OCT imaging.
Abstract:
A system and method for an endoscopic optical coherence tomography (OCT) system based on a CMOS-MEMS mirror to facilitate lateral light scanning. The laser scanning scope, adapted to the instrument channel of a commercially-available endoscopic sheath, allows for the real-time cross-sectional imaging of living biological tissue via direct endoscopic visual guidance. A conventional rod lens imaging system may be used for the visual guidance. The MEMS mirror is preferably actuated using either or both of a thermal-mechanical or electrostatic actuation system. More than one MEMS micromirror may be used in a single system for 3D imaging.
Abstract:
The invention provides interferometric apparatus and methods for reducing the effects of coherent artifacts in interferometers. Fringe contrast in interferograms is preserved while coherent artifacts that would otherwise be present in the interferogram because of coherent superposition of unwanted radiation generated in the interferogram are suppressed. Use is made of illumination and interferogrammetric imaging architectures that generate individual interferograms of the selected characteristics of a test surface from the perspective of different off-axis locations of illumination in an interferometer and then combine them to preserve fringe contrast while at the same time arranging for artifacts to exist at different field locations so that their contribution to the combined interferogram is diluted.
Abstract:
The present invention relates to a method and apparatus (10) for determining the instantaneous value of one or more properties of a sample examined by means of an interference technique, such as optical coherence tomography. The apparatus (10) includes an interferometer (12) which produces an interferogram signal (14), a phase comparator (16), a voltage-controlled oscillator VCO (18) and a low-pass filter (22). The phase comparator (16), VCO (18) and low-pass filter (22) together form an feedback loop in the form of phase-locked loop (30) wherein an output (24) of the low-pass filter (22) is linearly related to a scatterer's velocity nu s in the sample. The apparatus also includes a phase shifter (32), a mixer (38) and a low-pass filter (42) which generate a reflectivity signal (44).
Abstract:
Apparatus for splitting, imaging, and measuring wavefronts with a reference wavefront and an object wavefront. A wavefront-combining element receives and combines into a combined wavefront (66) an object wavefront (58) from an object and a reference wavefront (56). A wavefront-splitting element (80) splits the combined wavefront (66) into a plurality of sub-wavefronts (70a, 70b, 70c, 70d) in such a way that each of the sub-wavefronts (70a, 70b, 70c, 70d) is substantially contiguous with at least one other sub-wavefront. The wavefront-splitting element (80) may shift the relative phase between the reference wavefront and the object wavefront of the sub-wavefronts (70a, 70b, 70c, 70d) to yield a respective plurality of phase-shifted sub-wavefronts. The wavefront-splitting element (80) may then interfere the reference and object wavefronts of the phase-shifted sub-wavefronts to yield a respective plurality of phase-shifted interferograms (74a, 74b, 74c, 74d). An imaging element (76) receives and images the phase-shifted interferograms (74a-d). A computer connected to the imaging element (76) measures various parameters of the objects based on the phase-shifted interferograms (74a-d). Examples of measurements include flow parameters such as the concentrations of selected gaseous species, temperature distributions, particle and droplet distributions, density, and so on. In addition to flow parameters, the displacement (e.g., the vibration) and the profile of an object may be measured.
Abstract:
According to the invention, a single laser (31) is time-sequentially stabilized on different wavelengths ( lambda 1, lambda 2) during constant, preferably linear transition between both wavelengths in order to measure absolute optical interferometric length. The number of interferences which pass through are counted in a measuring channel during the transition from one wavelength to the other wavelength. The length (L) of a measuring distance can be absolutely measured by using known and stabile wavelengths ( lambda 1, lambda 2) and by measuring the phases ( phi 1, phi 2) of both wavelengths. Compared to known methods, the invention considerably increases the preciseness of measurement and the resolution by using an active integrated optical system and by measuring the residual phases by compensating the integrated optical system so that differences in wave lengths of 10 lambda can be detected.