Abstract:
A method for determining information about a transparent optical element including a lens portion and a plane parallel portion, the lens portion having at least one curved surface and the plane parallel portion having opposing first and second surfaces, includes: directing measurement light to the transparent optical element; detecting measurement light reflected from at least one location on the first surface of the plane parallel portion; detecting measurement light reflected from the second surface of the plane parallel portion at a location corresponding to the at least one location on the first surface; determining, based on the detected light, information about the plane parallel portion; and evaluating the transparent optical element based on the information about the plane parallel portion.
Abstract:
Calibrating a scanning interferometry imaging system includes: configuring the scanning interferometry imaging system for operation with an interference objective using light having a narrowband wavelength spectrum; using the scanning interferometry imaging system to direct measurement light and reference light along different paths and to overlap the measurement and reference light on a detector, the measurement and reference light having the narrowband wavelength spectrum; scanning an optical path length difference between the measurement light and the reference light at the detector while acquiring intensity data using the detector, the detector acquiring the intensity data at a frame rate and the scanning being performed at a scan speed; determining information about the scan speed based on the acquired intensity data, geometric information about the scanning interferometry imaging system, and the narrowband wavelength spectrum; and calibrating the scanning interferometry imaging system based on the information about the scan speed.
Abstract:
Systems and methods for generating 3D representations of shape and color texture of a test surface are described. In one aspect, surface topography interferometers are equipped with a multi-element detector and an illumination system to produce a true-color image of the measured object surface. Color information can be presented as a true-color two-dimensional image or combined with topography information to form a three-dimensional representation of the shape and color texture of the object, effectively creating for a human observer the impression of looking at the actual part.
Abstract:
An apparatus includes a broadband scanning interferometry system including optics for combining test light from a test object with reference light to form an interference pattern on a detector. The apparatus includes a stage configured to scan an optical path difference (OPD) between the test and reference light from a common source to the detector and a detector system including the detector for recording the interference pattern for each of a series of OPD increments, the frequency of each OPD increment defining a frame rate. The optics are configured to produce at least two monitor interferometry signals indicative of changes in the OPD as it's scanned, the detector system being configured to record the monitor interferometry signals. The apparatus includes a processor configured to determine information about the OPD increments with sensitivity to perturbations to the OPD increments at frequencies greater than the frame rate.
Abstract:
Interferometry methods and systems using coupled cavities and extended sources are disclosed. A main cavity (120) and a remote cavity (170) having similar optical properties are provided to compensate optical path differences (OPD) without degrading interference contrast in the image (109) of a camera (190). The remote cavity includes a stage (180) for adjusting the OPD. In one aspect the total OPD of the marginal rays is smaller than the wavelength when the total OPD of the chief rays is zero. In a further aspect the test and the reference light is coupled between the main cavity and the remote cavity with unit magnification. In another aspect two remote cavities are provided. In a further aspect a remote cavity is used to adjust a spherical portion of the optical measurement surface (150). In another aspect detachable optical assemblies are provided to form the main cavity.
Abstract:
A method for determining information about an object including a curved portion and a planar portion, the curved portion having a first curved surface having an apex and defining an axis of the object, includes: directing measurement light to the object; detecting measurement light reflected from the first curved surface of the curved portion; detecting measurement light reflected from at least one other surface of the object; and determining, based on the detected light, information about the apex of the first curved surface of the curved portion.
Abstract:
Apparatus include a microscope including an objective and a stage for positioning a test object relative to the objective, the stage being moveable with respect to the objective, and a sensor system including a sensor light source, an interferometric sensor configured to receive light from the sensor light source, to introduce an optical path difference (OPD) between first and second portions of the light, the OPD being related to a distance between the objective lens and the stage, and to combine the light portions to provide output light, a detector for detecting the output light from the interferometric sensor, a fiber waveguide for directing light between the sensor light source, the interferometric sensor and the detector, a tunable optical cavity between the sensor light source and the interferometric sensor, and an electronic controller configured to determine information related to the OPD based on the detected output light.
Abstract:
Conical surfaces (and other complex surface shapes) can be interferometrically characterized using a locally spherical measurement wavefront (e.g, spherical and aspherical wavefronts). In particular, complex surface shapes are measured relative to a measurement point datum. This is achieved by varying the radius of curvature of a virtual surface (152) corresponding to a theoretical test surface that would reflect a measurement wavefront to produce a constant optical path length difference (e.g., zero OPD) between the measurement and reference waveforms.