Abstract:
Because of diffraction effects caused by slits or apertures in optical measurement systems, the radiation energy which is directed towards a particular region on a sample will be spread over a larger area than desirable. By employing an apodizing filter in the radiation path in such system, diffraction tails of the system will be reduced. The apodizing filter preferably has a pattern of alternating high transmittance areas and substantially opaque areas where the locally averaged transmittance function is an apodizing function. In the preferred embodiment, the locally averaged transmittance function varies smoothly and monotonically from the periphery to the center of the filter.
Abstract:
A polarimeter with a polarization state generator and a polarization state analyzer mounted together on a single rotary mount. This novel structure allows built-in alignment and synchronization of the polarization state analyzer and the polarization state generator. Because of this built-in alignment and synchronization, polarization properties of samples can be measured quickly, accurately, inexpensively, and reliably. The instrument can measure polarization properties of remote samples, without placing the sample inside the instrument. The surrounding lenses and mirrors are designed in such a way that light leaving the instrument will pass through the polarization state generator and light returning into the instrument will pass through the polarization state analyzer and onto a photodetector. Samples can be measured directly in reflection or in small-angle backscatter; or they can be measured in double-pass transmission with the addition of a mirror or retroreflector.
Abstract:
An optical measurement device is disclosed for evaluating the parameters of a sample. The device includes a polychromatic source for generating a probe beam. The probe beam is focused on the sample surface. Individual rays within the reflected probe beam are simultaneously analyzed as a function of the position within the beam to provide information at multiple wavelengths. A filter, dispersion element and a two-dimensional photodetector array may be used so that the beam may be simultaneously analyzed at multiple angles of incidence and at multiple wavelengths. A variable image filter is also disclosed which allows a selection to be made as to the size of the area of the sample to be evaluated.
Abstract:
A magnetooptic player reads magnetooptically recorded signals on a disk by using a differential detector. Intermediate areas on a storage member used to store the magnetooptically record signals are sector marks and ID fields formed by undulations in the surface of the disk. Such sector marks and ID fields are read by detecting the intensity modulation in a reading light beam; for detecting such embossed marks and D-ROM disks, one-half of the differential detector is disabled for facilitating such detection in a differentially arranged detector.
Abstract:
A spectroscopic ellipsometer comprises an illumination device having a focal point (F'.sub.2) for illuminating a surface of a sample (E) in accordance with a given angle of incidence and a device for analyzing the light reflected from the surface of the sample. The sample support comprises three translation plates (20,30,40) in accordance with three respective directions (T.sub.2, T.sub.3, T.sub.1). The translations in accordance with the first (T.sub.1) and second (T.sub.2) directions make it possible to realise cartographic representations of the sample (E) and the translation in accordance with the third direction (T.sub.3) makes it possible to cause a point on the surface of the same (E) to coincide with the focal point (F'.sub.2). Two plates (PT.sub.2, 12) rotating about the axes O.sub.1 and O.sub.2, respectively, parallel to the first (T.sub.1) and second (T.sub.2) directions and intersecting each other at the focal point (F'.sub.2) provide the possibility of orienting the sample (E) by means of rotation in two orthogonal planes about the focal point (F'.sub. 2).
Abstract:
The interferometer makes use of an acousto-optic device to perform a frequency shift of the beam sent along one of the interferometer branches, so as to allow the determination of the state of polarization by heterodyne radiofrequency detection. The acousto-optic device can be inserted downstream of the device for splitting the beam emitted by the source into the two beams sent along the two interferometer branches, or it can also act as the beam splitter.
Abstract:
A static interferometric ellipsometer, wherein a source (3) generates a coherent light-beam with two monochromatic radiations at slightly different frequencies. A first photodetector (6) generates a first beat between the two radiations, to be used as reference. A second photodetector (9) generates a second beat between the two radiations, after they have been polarized in perpendicular planes and separated so that one of them is reflected onto the photodetector (9) by the sample under test (1,2). A measuring and computing system (11) determines the optical properties of said sample starting from the intensity of the second beat and from the relative phase between the two beats.
Abstract:
A miniature Kerr effect probe is described which may be used to examine surfaces of magnetic material during electroplating or vacuum deposition, without requiring a specially shaped bath or chamber.The probe consists of a U-shaped core with adjacent pole tips of soft magnetic material wound with a coil to provide a magnetic field across the ends of the arms of the core which constitute probe tips. In use, these probe tips are placed adjacent to a surface being examined. Optic fibers are used to direct light to and from the surface.The polarizer and analyzer required for Kerr work may be at the probe tips or remote from the probe tips due to the availability of optic fibers which will transmit polarized light without distortion. The light beam at the probe tips may be collimated or focussed by the optic fiber.
Abstract:
A magneto-optic spectrophotometer for detection or identification of atoms or molecules contained in the sample by utilizing phenomena of birefringence or rotation of polarization caused by the atoms or the molecules in a magnetic field is constructed as follows. Linearly polarized lights are incident on a space where atoms or molecules to be detected exist in a magnetic field. The lights having passed through said space are separated into two beams of lights of polarization components perpendicular and parallel to the polarization of the incident lights. The perpendicular components are used as the signal lights, and the parallel components the reference lights. The signal lights and the reference lights are spectrally analyzed by a wavelength selector in which a signal light and a reference light of a wavelength to be selected are incident on an identical dispersive element. The signal lights and the reference lights are detected by respective detectors. Then, the ratios of the outputs of the signal light detectors to the outputs of the reference light detectors are obtained. By this construction the intensities of the scattered lights by atoms or molecules to be detected can precisely be measured.
Abstract:
A method and apparatus are disclosed for monitoring parameters of a film or coating by directing a beam of optical radiation at a film supported on a metal substrate at an angle to the film so as to plane polarize any radiation transmitted through the film, reflecting a portion of the radiation from the interface between the film and substrate, transmitting the radiation through a polarizing medium before and/or after it has been transmitted through the film to block any component of radiation other than that which is or will be transmitted through the film, and transducing the radiation reflected from the interface to provide an output signal which is a function of a parameter of the film.