Abstract:
In order to improve the noise performance of a charge balance type photodiode array by reducing error influences, e.g. due to offset voltages, flicker and/or thermal noise, on a desired signal a compensation circuit is inserted in each channel of this array. The basic concept under lying this compensation circuit is to effect a correlated double sampling method without any significant increase in space or power demand for the silicon chip of at least one channel of said photodiode array. Because the wanted signal is primarily an amount of charge, the compensating circuit comprises a switchable compensating capacitor to compensate an error contribution of the desired signal. In a first “calibration period” the compensating capacitor is charged or discharged in dependence on the actual noise contribution. In a second compensation period the compensation capacitor provides a voltage which is used to correct a predetermined reference voltage to insure compensation of the error contribution. These periods are synchronized to the charge balance technique used in connection with the photodiode array.
Abstract:
A charge balance type of photodiode array uses parallel A/D conversion in each channel of the photodiode array. The charge caused by the photocurrent of a photodiode in each channel is removed in predetermined charge packets provided by a dumping circuit and the binary encoded number of delivered charge packets corresponds to the actual photocurrent. Charge balance photodiode arrays have a wide variety of applications. It is therefore useful to adapt photodiode arrays to the specific requirements of an individual application. The intention therefore provides a photodiode array having at least one switching circuit to vary signal processing parameters such as a gain factor g or an attenuation factor k. This improvement facilitates a multifunctional photodiode array for a plurality of different applications.
Abstract:
Spectrometers often use a so called charge balance photodiode array. This type of photodiode array uses parallel AID conversion in each channel of said photodiode array, whereby a charge provided by a photocurrent is accumulated at an integrator circuit, and a dumping circuit removes this charge by well defined charge packets to keep the system in balance. In order to expand the field of application of these photodiode arrays, a storage circuit is inserted to buffer a possible charge overflow caused by a light beam of high intensity, as often occurs when flash light lamps are used in the spectrometers. The storage circuit includes a capacitor, and a current limiter which linearly conducts the photocurrent below a process limit defined by the saturation limit of the dumping circuitry and which, above this limit, converts a photocurrent pulse into a constant overflow current having a duration corresponding to the amplitude of the photocurrent pulse.