Abstract:
A technique for measuring the unknown subsurface temperature T.sub.s of a bulk transparent medium such as ocean water by generating a continuous (cw) laser beam and pulsed laser beam both having the same wavelength, with the intensity of the pulsed laser beam exceeding the intensity required to produce stimulated Brillouin scattering in the water. By directing the pulsed laser beam into the water, it causes a return phase-conjugate beam to emanate therefrom. The return phase-conjugate beam and the pulsed laser beam are separated, and the phase-conjugate beam and the cw beam are mixed together thereby producing a heterodyne frequency proportional to the temperature T.sub.s. By converting the heterodyne frequency into a temperature value, yields the desired unknown T.sub.s.
Abstract:
A fiber optic sensor, a process for utilizing a fiber optic sensor, and a process for fabricating a fiber optic sensor are described, where a double-side-polished silicon pillar is attached to an optical fiber tip and forms a Fabry-Pérot cavity. In an implementation, a fiber optic sensor in accordance with an exemplary embodiment includes an optical fiber configured to be coupled to a light source and a spectrometer; and a single silicon layer or multiple silicon layers disposed on an end face of the optical fiber, where each of the silicon layer(s) defines a Fabry-Pérot interferometer, and where the sensor head reflects light from the light source to the spectrometer. In some implementations, the fiber optic sensor may include the light source coupled to the optical fiber; a spectrometer coupled to the optical fiber; and a controller coupled to the high speed spectrometer.
Abstract:
The present invention relates to thermal detectors and the application of such to devices and methods of detecting the infrared images using thermal detectors. For example, by using optical measuring systems in combination with at least one light source to measure changes position of a movable anchored surface coupled to an absorption surface such that the movable anchored surface changes position due to absorption of infrared radiation by the absorption surface. In another example, by combining a detector pixel (infrared radiation sensitive) with an optical measuring device such as an interferometer.
Abstract:
A temperature measuring apparatus and a temperature measuring method that may simultaneously measure temperatures of objects in processing chambers. The temperature measuring apparatus includes a first light separating unit which divides light from the light source into measurement lights; second light separating units which divide the measurement lights from the first light separating unit into measurement lights and reference lights; third light separating units which further divide the measurement lights into first to n-th measurement lights; a reference light reflecting unit which reflects the reference lights; an light path length changing unit which changes light path lengths of the reference lights reflected by the reference light reflecting unit; and photodetectors which measure interference between the first to n-th measurement lights reflected by the objects to be measured and the reference lights reflected by the reference light reflecting unit.
Abstract:
The temperature measuring apparatus includes a data input portion, a peak interval calculation portion, an optical path length calculation portion, and a temperature calculation portion. The data input portion inputs a spectrum of interference light that is obtained when measuring light is irradiated onto a surface of the object and the measuring light reflected from the surface and the measuring light reflected from a rear surface interfere with each other. The peak interval calculation portion calculates a peak interval of the input spectrum. The optical path length calculation portion calculates an optical path length based on the peak interval. The temperature calculation portion calculates the temperature of the object based on the optical path length.
Abstract:
A temperature measuring apparatus and a temperature measuring method that may simultaneously measure temperatures of objects in processing chambers. The temperature measuring apparatus includes a first light separating unit which divides light from the light source into measurement lights; second light separating units which divide the measurement lights from the first light separating unit into measurement lights and reference lights; third light separating units which further divide the measurement lights into first to n-th measurement lights; a reference light reflecting unit which reflects the reference lights; an light path length changing unit which changes light path lengths of the reference lights reflected by the reference light reflecting unit; and photodetectors which measure interference between the first to n-th measurement lights reflected by the objects to be measured and the reference lights reflected by the reference light reflecting unit.
Abstract:
The temperature control system includes: a susceptor which allows an object to be processed to be held on a top surface thereof and includes a flow path, through which a temperature adjusting medium flows, formed therein; a temperature measuring unit which measures a temperature of the object to be processed held on the top surface of the susceptor; a first temperature adjusting unit which adjusts a temperature of the temperature adjusting medium flowing through the flow path; and a second temperature adjusting unit which is disposed between the susceptor and the first temperature adjusting unit, and adjusts a temperature of the temperature adjusting medium based on a result of the measurement of the temperature measuring unit.
Abstract:
A method and device for determining the temperature of a sample, wherein a probing light beam is directed onto the sample whereby at least two partial beams of the probing light pass through paths of different lengths inside the sample by backscattering or reflecting the beams from at least two different depths in the sample, returning the partial beams to an analysis unit, and producing an interference pattern in the analysis unit by means of an interferometric device which uses one light beam as a reference for evaluating the interference pattern in an evaluating unit, wherein the signal intensity of the partial beam is determined counter to the optical path and the temperature displacement and temperature of the sample are determined by the temperature adjustment of the signal intensity.
Abstract:
The present invention relates to thermal detectors and the application of such to devices and methods of detecting the infrared images using thermal detectors. For example, by using optical measuring systems in combination with at least one light source to measure changes position of a movable anchored surface coupled to an absorption surface such that the movable anchored surface changes position due to absorption of infrared radiation by the absorption surface. In another example, by combining a detector pixel (infrared radiation sensitive) with an optical measuring device such as an interferometer.
Abstract:
Remote sensing of the temperature of a greybody or blackbody radiator is effected by passing its radiation (24) through a modulated infrared filter spectrometer. The infrared filter comprises, in sequence, a band pass filter (20), a first polariser (21) which polarises the radiation, an electro-optical element (22) which splits the polarised radiation into two orthogonally polarised components, and a second polariser (23). A lens (28) images the radiation leaving the second polariser onto a detector (27). The electrical signal from the detector (27) is input to a numerical analyser. The electro-optical element (22), typically comprising a birefringent crystal assembly (25) and a birefringent trim plate (26), is configured so that the net optical delay of the orthogonally polarised components passed through it is such that the recombined components are at or near a peak or trough in their interferogram. A sinusoidally varying voltage is applied to the electro-optical element to modulate the net delay of the components passed through the electro-optical element. The numerical analyser is programmed to compute the harmonic amplitude ratio (the ratio of signal amplitudes at the fundamental and second harmonic of the frequency of the modulating voltage) of the signal that it receives from the detector (27). The harmonic amplitude ratio is a function of the temperature of the radiator, which can be estimated by reference to a calibration look-up table.