Abstract:
An adaptive optics apparatus includes a light modulation unit configured to modulate each of two polarization components of light at a position that is optically conjugate to an object, the light being emitted by a light source; and an irradiation unit configured to irradiate the object with light that is modulated by the light modulation unit.
Abstract:
The present invention provides a method, an optical inspection apparatus as well as a computer program product for optical inspection of a surface. The optical inspection apparatus can be effectively applied for optical inspection of periodic structures on e.g. a semi-conductor wafer for the purpose of quality control. By effectively splitting a light beam into a plurality of spatially separated light beams and by selective usage of these light beams, various surface segments of the surface can be inspected simultaneously by superposition of respective images. A resulting superposition image can then be compared with a reference image for detection of defects of the surface.
Abstract:
An optical inspection system or tool can be configured to inspect objects using dynamic illumination where one or more characteristics of the illumination is/are adjusted to meet the inspection needs of different areas. For example, the illumination intensity may be increased or decreased as the tool inspects areas of memory and periphery features in a wafer die. In some embodiments, the adjustment can be based on data obtained during a pre-inspection setup sequence in which images taken based on illumination with varying characteristics are evaluated for suitability in the remainder of the inspection process.
Abstract:
A gas sensor, whose chamber uses filters and choppers in either a semicircular geometry or annular geometry, and incorporates separate infrared radiation filters and optical choppers. This configuration facilitates the use of a single infrared radiation source and a single detector for infrared measurements at two wavelengths, such that measurement errors may be compensated.
Abstract:
In an inspection system for planar objects having periodic structures, programmable optical Fourier filtering in the focal plane of a telecentric lens system is used to directly identify physical phenomena indicative of non-periodic defects. Lens assemblies and a coherent optical source are used to generate and observe a spatial Fourier transform of a periodic structure in the Fourier plane. Optical Fourier filtering (OFF) is performed in the focal plane using an electrically programmable and electrically alignable spatial light modulator. The spatial light modulator with high signal to noise ratio is electrically reconfigurable according to a feedback-driven, filter construction and alignment algorithm. The OFF enhances any non-periodic components present in the Fourier plane and final image plane of the object. A system having a plurality of inspection channels provides high-throughput inspection of objects with small non-periodic defects while maintaining high detection sensitivity.
Abstract:
A SLM spectrometer is provided that employs an entrance slit or a collimator to provide parallel rays of radiation to a prism which disperses the incident radiation into an associated wavelength spectrum. The resulting spectrum from the prism is incident upon a spatial light modulator (SLM), such as a deformable mirror device (DMD). By selectively activating (or deactivating) a small portion of the surface of the SLM, i.e. a cell on the SLM, it is possible to selectively reflect or transmit a portion of the spectrum incident upon the SLM onto a focusing device, such as a parabolic focusing mirror. The focusing device in turn focuses the portion of the spectrum reflected by the selected cells on the SLM to a sensor. The wavelength selected is a function of which row of cells are activated (or deactivated) in the SLM. The SLM spectrometer of the present invention may be used to analyze visible light and light that is near visible, such as the near infrared or ultraviolet regions. The output of the sensor or detector may be appropriately amplified and after appropriate calibration employed to determine the amount of energy in a particular wavelength or band of wavelengths.
Abstract:
An optical detector comprises a plurality of pixels, each pixel comprising a photodiode operable to detect light incident on that pixel and to generate a signal indicative of an intensity of that light. The plurality of pixels comprises a plurality of pixel pairs, and for each pixel pair, in a configuration mode, the detector is arranged to compare the signal generated by a first pixel of the pair with the signal generated by a second pixel of the pair. A method of optical detection is also described, as is a system incorporating the described optical detector.
Abstract:
An apparatus includes a light source (100) configured to emit an electromagnetic wave; a spatial light modulator (102) configured to modulate a wavefront of the electromagnetic wave to irradiate a sample (105); a plate (107) with an aperture; a lens unit (106) configured to set a focal point in the sample (105); a detector (108) configured to detect light coming from the focal point of the sample (105) through the aperture; and a controller (103) configured to control the spatial light modulator (102) based on the detected light by the detector (108). The lens unit (106) and the aperture in plate (107) form a confocal system.
Abstract:
A system and method for high-resolution imaging terahertz radiation utilizing a spatial terahertz modulator based on interactions of photons at other energies with an intermediate screen to create very high speed modulation.
Abstract:
A device (1; 10; 20; 30; 40) for optically examining the interior of a turbid medium (5) is provided. The device comprises an illumination system (2; 12; 22; 32; 42) adapted for illuminating a turbid medium (5) to be examined and an imaging device (106) adapted for generating images from detected light. The illumination system (2; 12; 22; 32; 42) is adapted to be operable in at least a first mode in which a wide area image is acquired by illuminating the turbid medium (5) and a surrounding area. From this wide area image, the region or regions of interest (110) at which the turbid medium (5) is actually situated can be determined. Then, these regions of interest (110) can be illuminated in a second mode. Thus, no light which has not been coupled to the turbid medium (5) and which might cause overexposure of the detector unit of the imaging device (106) will reach the imaging device (106).