Abstract:
An amorphous silicon thin film is formed on a substrate first. Then the thin film is irradiated by a laser plus having an irradiation interval along a first direction to re-crystallize the thin film into a polysilicon thin film. A light source is thereafter focused into a micro spot having a diameter smaller than the irradiation interval, and the polysilicon thin film is irradiated by the micro spot moving along the first direction and having a relative moving distance to obtain a spectrum.
Abstract:
The method utilizes the physical phenomenon known as dispersion of the optical rotation. After passage of linearly polarized electromagnetic radiation through the optically active environment (rotator), with the rotating power characterized by a parameter p, and then through the analyzing polarizer, the function R(p) can be measured. For the given active medium and the relative orientation of polarization planes of the input light beam and the analyzing polarizer, R(p) has an unambiguous relation with the spectrum I(&lgr;) of the analyzed radiation (&lgr; stands for wavelength) and allows its unambiguous determination by special mathematical methods. In devices based on the above mentioned principle a linearly polarized collimated beam of analyzed radiation propagates through the optical rotator then passes through the analyzer and strikes a single-channel or multi-channel detector which measures R(p) as a function of the parameter p. Finally the desired spectrum is calculated from the known functional relation between the measured rotogram R(p) and I(&lgr;).
Abstract:
An ellipsometer, which detects polarization of light successively reflected from a reference sample and an objective sample to study the objective sample, comprises first and second sample holder units for holding first and second samples, a beam projecting portion for projecting a beam of plane-polarized light toward the first sample, a polarizer, a turn-around prism for turning around the light beam reflected from the first sample to direct it to the second sample, an analyzer, a light detector for detecting light transmitted through the analyzer, and a sample positioning mechanism for arranging the first and second samples at appropriate positions and in appropriate orientations. The sample positioning mechanism includes one of the first and second sample holder units, which holds the objective sample, and comprises a height/inclination adjusting section for adjusting height and inclination of the objective sample.
Abstract:
A spectropolarimetric reflectometer for measuring polarimetric reflection properties of materials over broad spectral wavelength regions is described wherein radiation from a Fourier transform spectrometer passes through a set of polarization elements that serve as a polarization state generator and is reflected off the sample and collected by optics that includes a polarization state analyzer, focusing mirror and detector.
Abstract:
An optical path switch divides sample path radiation into a time series of alternating first polarized components and second polarized components. The first polarized components are transmitted along a first optical path and the second polarized components along a second optical path. A first gasless optical filter train filters the first polarized components to isolate at least a first wavelength band thereby generating first filtered radiation. A second gasless optical filter train filters the second polarized components to isolate at least a second wavelength band thereby generating second filtered radiation. A beam combiner combines the first and second filtered radiation to form a combined beam of radiation. A detector is disposed to monitor magnitude of at least a portion of the combined beam alternately at the first wavelength band and the second wavelength band as an indication of the concentration of the substance in the sample path.
Abstract:
A gyro apparatus has a ring laser in which laser beams of different oscillation frequencies coexist and propagate in mutually opposite circulation directions in an optical resonator, a power source of driving for the ring laser, a device for measuring a difference between the oscillation frequencies of the laser beams, and a device for controlling the power source of driving according to the frequency difference.
Abstract:
An apparatus and method for enhancing the proportion of detected light that has been diffusely scattered by a surface light to light specularly reflected from the surface. A beam of light having a direction of predominant polarization is directed through a wedge module so as to illuminate the scene. The wedge module has two optically anisotropic wedges and an optical compensation plate. The polarization axes of the first and second wedges are substantially parallel to the direction of predominant polarization of the illuminating beam. Light scattered by the surface is detected through a polarizer.
Abstract:
In a process or device for very accurate determination of the plane of polarization of polarized light, the light from a light source (1) is polarized by means of a polarizing filter (2) which has a certain setting angle &thgr;0 with respect to the first reference plane, the plane of incidence on the reflecting surface (4). The polarized beam (12) passes through the sample in the measurement chamber (3), in which the angle of rotation is changed by the small angle &thgr;MG. The sum of &thgr;0 and &thgr;MG gives the angle of rotation &thgr;e , at which the beam (13) emerging from the measurement chamber is partially reflected at the surface of a medium of higher refractive index (4). The reflected beam is then separated into two partial beams (15a: extraordinary beam; 15b: ordinary beam), with vibration directions exactly perpendicular to each other, in a polarizing prism (5), the reference plane of which, the plane of vibration of the ordinary beam, has a certain setting angle (&thgr;*) with respect to the first reference plane. The intensities Io and Ia of the two partial beams are determined photometrically by detectors (6a,b) and the ratio (Q) of the measured intensities is determined (quotient determiner 8).
Abstract:
A real-time optical compensating apparatus reduces the PMD in an optical fiber by determining the principal states of polarization of the optical fiber and delaying one principal state of polarization with respect to the other.
Abstract:
A combination metrology tool is disclosed which is capable of obtaining both thermal wave and optical spectroscopy measurements on a semiconductor wafer. In a preferred embodiment, the principal combination includes a thermal wave measurement and a spectroscopic ellipsometric measurement. These measurements are used to characterize ion implantation processes in semiconductors over a large dosage range.