Abstract:
In a temperature measuring device (1) an IR-radiation detector (2) and a reference element (3) are provided, connected to a surface (6) of an object (7) in a heat-conducting fashion, with a first area (4) with high emissivity and a second area (5) with high reflectivity formed at the reference element (3), and the IR-radiation detector (2) is equipped for a separate detection of IR-radiation (9, 10, 11) from the first and second areas (4, 5) and a surface area (12) of the object (7). A computer (13) in the IR-radiation detector (2) is equipped to deduct a temperature measurement for the object (7), corrected for emissions and reflections from the detected IR-radiations (9, 10, 11).
Abstract:
A method for measuring the differential emissivity between two sites on the surface of a body and the temperature of the two sites. The method includes a plurality of measurements of the infrared radiation arising from each of the two sites under a number of different conditions. Some of the measurements include irradiation by external infrared radiation at a known wavelength and intensity. The infrared radiation arising from each of the sites may include emitted radiation, reflected ambient radiation, and reflected external radiation. Additionally, the temperature determined using the method described can be used to calibrate infrared imaging devices used to inspect the entire body.
Abstract:
In a process for heating, e.g., a semiconductor wafer within a processing chamber, the wafer is exposed to a flux of electromagnetic radiation from lamps energized by alternating electric current. The surface temperature of the wafer is measured, and responsively, the radiation flux is controlled. The temperature measurement procedure includes collecting radiation propagating away from the wafer in a first light-pipe probe, collecting radiation propagating toward the wafer in a second light-pipe probe, and detecting radiation collected in the respective probes. This procedure further involves determining, in the signal received from each probe, a magnitude of a time-varying component resulting from time-variations of the energizing current, and combining at least these magnitudes according to a mathematical expression from which the temperature can be inferred. At least some of the radiation collected by the second probe is collected after reflection from a diffusely reflecting surface. The second probe effectively samples this radiation from an area of the diffusely reflecting surface that subtends a solid angle .OMEGA..sub.2 at the wafer surface. The first probe effectively samples radiation from an area of the wafer that subtends a solid angle .OMEGA..sub.1 at the first probe. The radiation sampling is carried out such that .OMEGA..sub.2 is at least about .OMEGA..sub.1.
Abstract:
A method and apparatus for detecting the temperature of gray and non-gray bodies in the presence of interfering radiation. A gray body has a constant emissivity less than 1 and a non-gray body has an emissivity which varies with wavelength. The emissivity and reflectivity of the surface is determined over a range of wavelengths. Spectra are also measured of the extraneous interference radiation source and the surface of the object to be measured in the presence of the extraneous interference radiation source. An auxiliary radiation source is used to determine the reflectivity of the surface and also the emissivity. The measured spectrum of the surfaces in the presence of the extraneous interference radiation source is set equal to the emissivity of the surface multiplied by a Planck function containing a temperature term T plus the surface reflectivity multiplied by the spectrum of the extraneous interference radiation source. The equation is then solved for T to determine the temperature of the surface.
Abstract:
The temperature and radiant energy emissivity of a semiconductor substrate or wafer undergoing processing are monitored by combining indications derived from an interferometer and the intensity of radiant energy emitted from the substrate. The radiant energy intensity is detected at adjacent maxima or minima in the intensity of the interference pattern.
Abstract:
The present invention constitutes a pyrometer device and an associated method of operation for measuring temperature based on the radiation emitted by a heated body in which increased accuracy is achieved by actively ascertaining the emittance of the body whose temperature is being measured. The pyrometer device includes a light source for intermittently illuminating the heated body and a radiation sensing mechanism for measuring the amount of light reflected and radiated by the body. The pyrometer device further includes a signal processing unit for processing the information developed by the radiation sensing mechanism and deriving the temperature of the body based on a calculated emittance factor and the amount of light radiated by the body.
Abstract:
An optical technique for determining surface temperature utilizes the Christiansen effect that is exhibited by dielectric materials; i.e., strong absorption bands at certain wavenumber values, causing the radiance of the material to be that which would characterize a theoretical black body at that wavenumber value.
Abstract:
A first and second pyrometer (26-28) are optically coupled by a light pipe (24) to a wafer (30) in an apparatus (10). The light pipe (24) passes through a shroud (16) of a heating lamp module (14). A computer (74) is interconnected to the pyrometers (26-28) and a lamp module power supply (80). A laser (48) emits a laser beam (50) through a power meter (86) onto an infrared mirror (56) over the light pipe (24). The mirror (56) directs the beam onto wafer (30) which reflects a portion of the beam back to the infrared mirror (56). The beam is then guided to an infrared photo-detector (58) which provides, in combination with the incident laser beam power meter (86), reflectance of the wafer surface for the laser beam which is related to wafer emissivity. The spectral infrared emissivity measurement can be performed more accurately over an extended temperature range if the transmissivity of the wafer is determined by another infrared photodetector (59) and both the measured wafer reflectance and transmissivity data are used to calculate the emissivity. Wafer emissivity data and pyrometers reading data are evaluated by the computer (74) to determine the true wafer temperature in real-time and to raise or lower the power output from the power supply (80) to adjust the wafer temperature within the apparatus (10).
Abstract:
Embodiments disclosed herein include a method of calibrating a processing tool. In an embodiment, the method comprises providing a first substrate with a first emissivity, a second substrate with a second emissivity, and a third substrate with a third emissivity. In an embodiment, the process may include running a recipe on each of the first substrate, the second substrate, and the third substrate, where the recipe includes a set of calibration attributes. In an embodiment, the method may further comprise measuring a layer thickness on each of the first substrate, the second substrate, and the third substrate. In an embodiment, the method further comprises determining if the layer thicknesses are uniform.
Abstract:
A computer-eimplemented thermal imaging device having an optically-sensitive layer that includes a superpixel having at least one pixel. The at least one pixel includes a plasmonic absorber configured to obtain radiance measurements of electromagnetic radiation emitted from an object at a plurality of wavelengths. The device further includes a processor configured to determine an emissivity and temperature for the electromagnetic radiation received at the plasmonic material from the object using the radiance measurements and to form an image of the object from the determined emissivity and temperature.