Abstract:
Disclosed is an apparatus and method for measuring a changing amount of insertion loss of an optical device depending on a polarization state of an incident light, i.e., a polarization-dependent loss. An incident light that is periodically subject to all polarization states passes through a testing optical device by a polarization scrambler including a piezoelectric element type optical fiber birefringence modulator, and an optical detector measures intensity of the passing light, in which the measured intensity values are averaged for birefringence modulation having a constant period, and then the polarization-dependent loss is computed from a ratio of maximum power to minimum power for the period. Use of the birefringence modulator shortens measuring time, and decreases an affect of external disturbance to the incident light that is incident into the testing optical component or occurrence probability of the external disturbance, so that the polarization-dependent loss can be precisely measured.
Abstract:
The invention concerns an ellipsometer comprising a source (S) supplying at least an infrared radiation, a sample-holder (PE), a sensor (D), a first optical system mounted between the source (S) and the sample-holder (PE), so as to illuminate a sample placed on the sample-holder, under oblique view with a polarised light beam and a second optical system mounted between the sample-holder (PE) and the sensor (D) for collecting the light reflected by the sample. The ellipsometer further comprises a blocking device (F2) mounted on the reflection path in the focal plane of the focusing device (M2) of the second optical system, and adapted to block parasite rays (RP) derived from the rear surface (FAR) of the sample and to allow through useful rays (RU) derived from the front surface (FAV) of the sample towards the sensor (D), thereby enabling to obtain a resolution with respect to the sample front and rear surfaces.
Abstract:
Die Erfindung bezieht sich auf ein Polarimeter zur Ermittlung von Eigenschaften einer Probe über Phasenauflösung und Fourieranalyse mit einer Quelle (1, 2, 3, 4, 5) für linear polarisierte Strahlung, einer Probenkammer zur Aufnahme der Polarimeterröhre (6) für die Probe, einen Analysator (7), der am Ausgang der Probenkammer (6) angeordnet ist, der das von der Probe optisch beeinflusste Licht erhält und der kontinuierlich drehbar ist, einen Motor mit Inkrementalgeber (10) als Antrieb für den Analysator (7), einen Detektor (9) mit Linse (8), der das vom Analysator (7) ausgegebene Signal hinsichtlich Analysatorstellung und Intensitätssignal erfasst und an einen Analog-Digitalwandler (11) abgibt, der von dem Inkrementalgeber (19) getriggert wird, und einen Rechner (12), der das Ausgangssignal vom Analog-Digitalwandler (11) erhält und über eine Fourieranalyse eine Aussage über die Eigenschaften der Probe macht.
Abstract:
An ellipsometer for analyzing a sample (2) using a broad range of wavelengths includes a light source (4) for generating a beam of polychromatic light for interacting with the sample (2). A polarizer (6) polarizes the light beam before the light beam (14) interacts with the sample (2). A rotating compensator (8) induces phase retardations of a polarization state of the light beam. The range of wavelengths and the compensator (8) are such that at least a first phase retardation value is induced that is within a primary range of effective retardations of substantially 90° to 180°. An analyzer (10) interacts with the light beam after the light beam interacts with the sample (2). A detector (12) measures the intensity of light after interacting with the analyzer (10) as a function of compensator angle and of wavelength, preferably at all wavelengths simultaneously. A processor (23) determines the polarization state of the light, after interacting with the analyzer (10), from the light intensities measured by the detector (12).
Abstract:
A practical system and method for measuring waveplate retardation. The system employs a photoelastic modulator (22) in an optical setup and provides high sensitivity. The analysis is particularly appropriate for quality-control testing of waveplates (26). The system is also adaptable for slightly varying the retardation provided by a waveplate (26) (or any other retarder device) in a given optical setup. To this end, the waveplate (26) position may be precisely altered to introduce correspondingly precise adjustments of the retardation values that the waveplate (26) provides. The system is further refined to permit one to compensate for errors in the retardation measurements just mentioned. Such errors may be attributable to static birefringence present in the optical element of the photoelastic modulator (22) that is incorporated in the system.
Abstract:
A practical system and method for precisely measuring low-level birefrigence properties (retardance and fast axis orientation) of optical materials (26). The system permits multiple measurements to be taken across the area of a sample to detect and graphically display (100) variations in the birefrigence properties across the sample area. In a preferred embodiment, the system incorporates a photoelastic modulator (24) for modulating polarized light that is then directed through a sample (26). The beam ('Bi') propagating from the sample is separated into two parts, with one part ('B1') having a polarization direction different than the polarization direction of the other beam part ('B2'). These separate beam parts are then processed as distinct channels. Detection mechanisms (32, 50) associated with each channel detect the time varying light intensity corresponding to each of the two parts of the beam. This information is combined for calculating a precise measure of the retardance induced by the sample, as well as the sample's fast axis orientation.
Abstract:
An apparatus for measuring magneto-optical effect includes a light source 102, a spectroscope 120, a first polarizer 150 to polarize the light with a required wavelength taken out by the spectroscope 120, means 172 for applying magnetic field on a sample 176, a second polarizer 156 to admit the light transmitted or reflected by a sample 176 to pass, a photo-detector 162 for detecting intensity of light that has passed the second polarizer 156. The light source 102 includes a heavy hydrogen lamp and the spectroscope does not contain a lens and/or prism. A light path from the light source to the photo-detector is housed in a container, and the container is filled with a gas containing no oxygen.