Abstract:
Apparatus and a method for performing high resolution optical imaging in the near infrared of internal features of semiconductor wafers (110) uses an optical device (112) made from a material having a high index of refraction and held in very close proximity to the wafer (110). The optical device (112) may either be a prism (130) or a plano-convex lens (112). The plano-convex lens (112) may be held in contact with the wafer (110) or separated from the wafer via an air bearing (112') or an optical coupling fluid (214) to allow the sample to be navigated beneath the lens (112). The lens (112) may be used in a number of optical instruments such as a bright field microscope, a Schlieren microscope, a dark field microscope, a Linnik interferometer, a Raman spectroscope and an absorption spectroscope.
Abstract:
A method and apparatus for measuring a defect distribution comprising introducing a narrowed laser beam into an object to be observed, receiving scattering lights generated at the defect portions of the object by a photoelectric conversion element, and measuring automatically the density and density distribution of the defects inside the object on the basis of the output image data of the photoelectric conversion element.
Abstract:
Two independent detection systems are provided for measuring thermal waves generated in a sample (22) by a periodic, localized heating cause by a laser beam (34) modulated by a modulator (32). One detection system generates output signals that are primarily a function of the surface temperature of the sample. The other detection system generates signals that are primarily a function of the integral of the temperature beneath the sample surface. The two independent thermal wave measurements permit analysis of both thickness and compositional variables. Both detection systems are implemented efficiently by one apparatus consisting of an He-Ne laser (50) directing a probe beam (52) through a polarising splitter (54) and a dichroic mirror (36) and the objective (38) of the heating beam (34) onto a spot at the heated spot of the sample (22). The probe beam (52) is reflected at an intensity that depends on the surface temperature and is deflected by an angle that depends on the integral of temperature beneath the surface. The reflected beam passes back to the splitter (54) where it is reflected to a split photodetector (80) from which the differential output indicates integral of temperature and sum output indicates surface temperature to a processor (58) determining thickness and compositional variables therefrom.
Abstract:
Two independent detection systems are provided for measuring thermal waves generated in a sample (22) by a periodic, localized heating cause by a laser beam (34) modulated by a modulator (32). One detection system generates output signals that are primarily a function of the surface temperature of the sample. The other detection system generates signals that are primarily a function of the integral of the temperature beneath the sample surface. The two independent thermal wave measurements permit analysis of both thickness and compositional variables. Both detection systems are implemented efficiently by one apparatus consisting of an He-Ne laser (50) directing a probe beam (52) through a polarising splitter (54) and a dichroic mirror (36) and the objective (38) of the heating beam (34) onto a spot at the heated spot of the sample (22). The probe beam (52) is reflected at an intensity that depends on the surface temperature and is deflected by an angle that depends on the integral of temperature beneath the surface. The reflected beam passes back to the splitter (54) where it is reflected to a split photodetector (80) from which the differential output indicates integral of temperature and sum output indicates surface temperature to a processor (58) determining thickness and compositional variables therefrom.
Abstract:
The description relates to a device for handling, treating and observing small particles, especially biological particles. A first laser (4) generates light beams in a first wavelength range which are focussed by a first optical device (12, 13; 14, 15) and form an optical trap. A slide (22) holds corresponding particles. There is also a light source (17) for observation purposes and observation and recording devices for observing the particles and recording their behaviour. A second laser (3) generates light beams in a second wavelength range which are focussed so that particles on the slide may be treated. The optical devices for the light beams can be positioned and adjusted independently of each other and thus the light beams can be focussed in the same object plane of the slide at the start of treatment and observation independently of their wavelengths.
Abstract:
Apparatus and a method for performing high resolution optical imaging in the near infrared of internal features of semiconductor wafers (110) uses an optical device (112) made from a material having a high index of refraction and held in very close proximity to the wafer (110). The optical device (112) may either be a prism (130) or a plano-convex lens (112). The plano-convex lens (112) may be held in contact with the wafer (110) or separated from the wafer via an air bearing (112') or an optical coupling fluid (214) to allow the sample to be navigated beneath the lens (112). The lens (112) may be used in a number of optical instruments such as a bright field microscope, a Schlieren microscope, a dark field microscope, a Linnik interferometer, a Raman spectroscope and an absorption spectroscope.
Abstract:
A specific small area of a crystal sample (11) is scanned by a laser beam in a spiral pattern (2a, 2b). The laser beam is reflected different amounts for different beam positions to produce a reflectance pattern indicative of crystallographic orientation. The reflected beam radiation may be determined with a photodetector (12) and the reflectance pattern may be interpreted with circuitry (13) which also controls steering of the beam.
Abstract:
A fluorometer for measuring a particular fluorescence emanating from a specimen, including producing a burst of concentrated light energy and directing the concentrated light energy toward the specimen to produce a fluorescence from the specimen including the particular fluorescence. Preferably producing an image of the fluoresence. Detecting the fluorescence and producing a signal in accordance with the fluorescence. Controlling the passage of the image of the fluorescence for detecting within a particular time period so as to optimize the detection of the particular fluorescence. Timing the operation to sequence the detection of the fluorescence within the particular time period after the production of the burst of concentrated light energy. Scanning the fluorescence from the specimen for forming signals representative of the fluorescence from the specimen. Analyzing the signals to enhance the portion of the signal representing the particular fluorescence relative to the portion of the signal.