Abstract:
An apparatus for use in wave division multiplexing optical telecommunication systems includes a dual photodiode array which converts parallel and perpendicularly polarized light beams at given wavelengths to electrical signals which are digitized and used to rapidly and simultaneously determine all wavelengths and associated components of power and angle of polarization. This information can be displayed for monitoring purposes, or can be used to control signals travelling through optical fiber.
Abstract:
Imaging apparatus which images the changes in height of reactive spots on the surface of a slide requires the surface roughness of the slide to be small enough to distinguish the changes in height from the roughness features of the slide.
Abstract:
In the present invention, measuring the one-dimensional or two-dimensional voltage distribution or electrical field distribution in a measured device is made possible, and a reduction in the measuring time can be implemented. The present invention comprises a first optical system (2, 3) wherein light emitted from the light source is shaped into a line-shaped light beam and irradiates a desired measurement line in the measured device via the electrooptic element, a second optical system (7, 8, 9) that maintains as-is the shape of the line-shaped light beam reflected from the desired measurement line in the measured device after transiting the electro-optic element, a light receiving device (10) that receives the line-shaped light beam emitted from the second optical system and converts each of the measured points to an electrical signal depending on the strength of each light beam reflected at each of the measured points on the desired measurement line on the measured device and outputs the result, and a signal processing device (11, 12, 13, 14, 16) that calculates the voltage or electrical field at each of the measured points of the measured device from the output signal of the light receiving device and calculates the electrical field distribution or the voltage distribution at the measured part of measured device.
Abstract:
A polarization bearing detection type two-dimensional light reception timing detecting device for implementing a fast surface shape measurement that can accommodate an animal body measurement, and a surface shape measuring device using it. The polarization bearing of a detection light is turned in synchronization with slit light scanning, and the polarization bearing is two-dimensionally recorded by two sets of analyzers and storage type image detectors in a crossed Nicols arrangement, and thereby it is possible to determine, with only one-time imaging, timing at which a slit light is beamed into respected pixels in the storage type image detectors.
Abstract:
In a spectroscopic ellipsometer (1), a lighting part (3) comprises a light source part for measurement (measurement light source) (31) and a polarizer (32), and the polarizer (32) obtains polarized light from light outputted from the measurement light source (31) and guides the polarized light to a substrate (9). A light receiving part (4) comprises an analyzer (41) on which reflected light which is the polarized light reflected on the substrate 9 is incident and a spectroscope (42), and the reflected light through the analyzer (41) enters the spectroscope (42), where a polarization state at each wavelength is acquired. The spectroscopic ellipsometer (1) has a construction in which mirrors are disposed only between the measurement light source (31) and the polarizer (32) and between the analyzer (41) and the spectroscope (42). In the spectroscopic ellipsometer (1), with this construction, the polarization state of the polarized light or its reflected light is not changed by mirrors and it is therefore possible to achieve measurements with high accuracy.
Abstract:
A polarization control system includes a beam source that generates a first beam component containing light with a first polarization and a first frequency and a second beam component containing light with a second polarization and a second frequency. A polarization state modulator adjusts the polarizations of the components for transmission on a single optical fiber. A detector system measures polarizations of the components when output from the optical fiber and determines how to adjust the polarization state modulator in order to give the first and the second components the desired output polarization states. The beam source can be implemented using a Zeeman-split laser, a laser containing a birefringent element, a pair of phase-locked lasers, and/or a variety of configurations of electro-optic or acousto-optic crystals operated to create or enhance the frequency difference between the beam components.
Abstract:
An optical measurement system for evaluating a sample has a motor-driven rotating mechanism coupled to an azimuthally rotatable measurement head, allowing the optics to rotate with respect to the sample. A polarimetric scatterometer, having optics directing a polarized illumination beam at non-normal incidence onto a periodic structure on a sample, can measure optical properties of the periodic structure. An E-O modulator in the illumination path can modulate the polarization. The head optics collect light reflected from the periodic structure and feed that light to a spectrometer for measurement. A beamsplitter in the collection path can ensure both S and P polarization from the sample are separately measured. The measurement head can be mounted for rotation of the plane of incidence to different azimuthal directions relative to the periodic structures. The instrument can be integrated within a wafer process tool in which wafers may be provided at arbitrary orientation.
Abstract:
In a measurement arrangement comprising an optical device, into which a diverging beam coming from a specimen is coupled for measurement, and further comprising a detector, which is arranged following said optical device and comprises a multiplicity of detector pixels arranged in one plane and evaluable independently of each other, wherein the optical device spectrally disperses the diverging beam in a first direction transversely of the propagation direction of the beam and directs it to the detector, the optical device also parallels the beam, before it impinges on the detector, in a second direction transversely of the propagation direction (C) such that rays of the beam impinging on the detector, which are adjacent to each other in the second direction, extend parallel to each other.
Abstract:
An ellipsometer includes a light source for generating a probe beam of polychromatic light for interacting with a sample. The probe beam is passed through a first polarizer that imparts a known polarization state to the probe beam. The polarized probe beam is then directed to reflect from the sample. A second illumination source is switched on and off at a predetermined frequency to create an intensity modulated pump beam (the beam may also be chopped). The pump beam is directed normally against the subject producing a small illumination spot within the area illuminated by the probe beam. The pump induces localized changes in the dielectric properties of the subject. The pump-beam induced oscillations are picked up by the portion of the probe beam that is reflected from within the illumination spot of the pump beam. By analyzing only the portion of the reflected probe beam that includes the pump beam induced oscillation, the size of the measurement spot is effectively limited to the illumination spot size of the normally directed pump beam.
Abstract:
A flat spectrum illumination source for use in optical metrology systems includes a first light source generating a visible light beam and a second light source generating an ultraviolet light beam. The illumination source also includes an auxiliary light source generating a light beam at wavelengths between the visible light beam and the ultraviolet light beam. The three light beams are combined to provide a broadband probe beam that has substantially even illumination levels across a broad range of wavelengths. Alternately, the illumination source may be fabricated as an array of light emitting diodes selected to cover a range of separate wavelengths. The outputs of the LED array are combined to produce the broadband probe beam.