Organic light-emitting diodes (OLEDs) permit the monolithic integration of microelectronic circuits and light-emitting devices on the same silicon chip. By the use of integrated photodetectors, low-cost CMOS processes and simple packaging; economically produced optoelectronic integrated circuits (OEICs) with combined sensors and actuating elements can be realized. The OLEDs are deposited directly on the top metal layer. The metal layer serves as electrode and defines the bright area. Furthermore, the area below the electrodes can be used for integrated circuits. Due to efficient emitter with low operating voltage it is possible to renounce high-voltage devices depending on selected CMOS process. Thus manufg. cost can be further reduced. Different CMOS metalizations were examd. and their effects on org. light-emitting diodes were analyzed. Red (628nm) and orange (597nm) emitting p-i-n OLEDs with a radiance of 5W/m2sr at 2.8V and 3.0V and a half angle of +-45 Deg were realized on metal layer with low roughness. Near infra-red emitters are in development. We will present an optical microsystem. The functionality of combined sensors and actuating elements as well as advantages and difficulties of the monolithic integration of OLEDs and CMOS will be discussed. The chip was manufd. in a com. 1micro m CMOS technol. The fabricated microsystem combines three different types of sensors: a reflective sensor, a color sensor and a particle flow sensor
Modern miniaturized scanning grating spectrometers (SGSs) are often based on microelectromechanical system devices. In contrast to classical spectrometers, such systems exhibit additional design constraints, like a symmetrical motion of the grating with a limited deflection. A detailed mathematical analysis of typical SGS configurations based on the grating equation considering these constraints is presented. Equations that relate the basic angles on a scanning grating to the grating properties and the attainable wavelength range of a spectrometer are derived, and the solution set is examined. Furthermore, the analytical description can be used to optimize SGSs with symmetrically moving gratings. The attainable spectral range for a given deflection amplitude of the grating can be calculated. Alternatively, the required grating properties can be determined for a given spectral range.
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