Abstract:
A system and method for measuring lubricant thickness and degradation, carbon wear and carbon thickness, and surface roughness of thin film magnetic disks at angles that are not substantially Brewster's angle of the thin film (carbon) protective overcoat. A focused optical light whose polarization can be switched between P or S polarization is incident at an angle to the surface of the thin film magnetic disk. The range of angles can be from zero degrees from normal to near Brewster's angle and from an angle greater than Brewster's angle to 90 degrees. This range of angles allows the easy measurement of the change in lubricant thickness due to the interaction of the thin film head, the absolute lubricant thickness and degradation of the lubricant. It also allows the measurement of changes in carbon thickness and the absolute carbon thickness. The surface roughness can also be measured at any of the angles specified above. The present invention utilizes a first and second histogram representing disk properties (1) at two different time periods, (2) at two different locations on the disk, or (3) on two different disks.
Abstract:
A system and method for measuring lubricant thickness and degradation, carbon wear and carbon thickness, and surface roughness of thin film magnetic disks at angles that are not substantially Brewster's angle of the thin film (carbon) protective overcoat. A focused optical light whose polarization can be switched between P or S polarization is incident at an angle to the surface of the thin film magnetic disk. The range of angles can be from zero degrees from normal to near Brewster's angle and from an angle greater than Brewster's angle to 90 degrees. This range of angles allows the easy measurement of the change in lubricant thickness due to the interaction of the thin film head, the absolute lubricant thickness and degradation of the lubricant. It also allows the measurement of changes in carbon thickness and the absolute carbon thickness. The surface roughness can also be measured at any of the angles specified above. The present invention generates a histogram from the specular and scattered components of the reflected light, generates a centroid of the histogram and performs a symmetry operation to identify the characteristics of the thin film.
Abstract:
A system and method for measuring lubricant thickness and degradation, carbon wear and carbon thickness, and surface roughness of thin film magnetic disks at angles that are not substantially Brewster's angle of the thin film (carbon) protective overcoat. A focused optical light whose polarization can be switched between P or S polarization is incident at an angle to the surface of the thin film magnetic disk. The range of angles can be from zero degrees from normal to near Brewster's angle and from an angle greater than Brewster's angle to 90 degrees. This range of angles allows the easy measurement of the change in lubricant thickness due to the interaction of the thin film head, the absolute lubricant thickness and degradation of the lubricant. It also allows the measurement of changes in carbon thickness and the absolute carbon thickness. The surface roughness can also be measured at any of the angles specified above.
Abstract:
An angle independent optical surface inspector capable of generating a light beam, directing the light beam to a sample, and de-scanning a reflected light beam that is reflected from the sample, thereby generating a first de-scanned light beam. The de-scanning is performed at approximately one focal length of a de-scanning lens from an irradiation location where the light beam irradiates the sample. The optical inspector also capable of focusing the first de-scanned light beam, thereby generating a focused light beam, and measuring the location of the focused light beam. The measuring of the location is performed at approximately one focal length of a focusing lens from the focusing lens. The incident angle of the light beam is within ten degrees of Brewster's angle. The focusing is performed by an achromatic lens.
Abstract:
A system for defect detection and photoluminescence measurement of a sample may include a radiation source configured to target radiation to the sample. The system may also include an optics assembly positioned above the sample to receive a sample radiation. The system may also include a filter module configured to receive the sample radiation collected by the optics assembly. The filter module may separate the sample radiation collected by the optics assembly into a first radiation portion and a second radiation portion. The system may also include a defect detection module configured to receive the first radiation portion from the filter module. The system may further include a photoluminescence measurement module configured to receive the second radiation portion from the filter module. The defect detection module and the photoluminescence measurement module may be configured to receive the respective first radiation portion and the second radiation portion substantially simultaneously.
Abstract:
An optical inspector includes a radiating source, a time varying beam reflector, a telecentric scan lens, a first and second waveplate, a polarizing beam splitter, a first detector, a focusing lens, a blocker, and a second detector. The radiating source irradiates the first waveplate generating circularly polarized source beam that irradiates a first position of on the time varying beam reflector with a source beam. The time varying beam reflector directs the source beam to the telecentric scan lens, which in turn directs the source beam to a sample. Reflected radiation from a sample is directed to the second waveplate generating linearly polarized beam that irradiates the polarizing beam splitter which directs a portion of the reflected radiation to the first detector. Scattered radiation from the sample is directed by the focusing lens to the second detector. Contemporaneous measurements by the first and second detectors are compared to differentiate.
Abstract:
An optical inspector includes a radiating source, a time varying beam reflector, a telecentric scan lens, a blocker, a focusing lens, an aperture, and a detector. The radiating source irradiates a first position of on the time varying beam reflector with a source beam. The time varying beam reflector directs the source beam to the telecentric scan lens, which in turn directs the source beam to a transparent sample. A portion of the source beam travels through the transparent sample to another surface. The blocker blocks scattered radiation originating at the other surface. Scattered radiation originating from the transparent sample is not redirected by the blocker and is focused by the focusing lens to a first focal plane. The focused scattered radiation passes through the aperture before irradiating the detector. The detector output an intensity measurement of the scattered radiation that irradiates the detector.
Abstract:
An apparatus for inspecting an edge of a substrate. A light source produces a light beam, and a two-dimensional beam deflector receives the light beam and creates a semi-annular scanning beam. A first flared parabolic surface receives the semi-annular scanning beam and directs the semi-annular scanning beam onto the edge of the substrate, thereby creating specularly reflected light from the edge of the substrate. A second flared parabolic surface receives and directs the specularly reflected light to a detector. The detector receives the directed specularly reflected light and produces signals. An analyzer analyzes the signals and detects defects at the edge of the substrate.
Abstract:
An apparatus for inspecting an edge of a substrate. A light source produces a light beam, and a two-dimensional beam deflector receives the light beam and creates a semi-annular scanning beam. A first flared parabolic surface receives the semi-annular scanning beam and directs the semi-annular scanning beam onto the edge of the substrate, thereby creating specularly reflected light from the edge of the substrate. A second flared parabolic surface receives and directs the specularly reflected light to a detector. The detector receives the directed specularly reflected light and produces signals. An analyzer analyzes the signals and detects defects at the edge of the substrate.