Abstract:
Le détecteur est destiné à recevoir un faisceau lumineux modulé à une fréquence qui constitue le paramètre significa tif à mesurer. Il est notamment utilisable dans un appareil utilisant deux faisceaux de lumière cohérente provenant d'une même source, dont l'un est soumis au phénomène physique à étudier, qui affecte la fréquence, les deux faisceaux de lumière étant ensuite mélangés sur une photo diode à avalanche. Le détecteur comprend un circuit (28) de mesure du courant moyen traversant la photodiode à avalanche et des moyens (32) commandés par ce circuit et appliquant à la diode une tension de polarisation V telle que le courant moyen soit sensiblement égal à une valeur de consigne ajustable.
Abstract:
A circuit is used to set the operating point of at least one opto-electronic component, e.g. a photodiode (10'), in which the opto-electronic component is part of a receiver for useful alternating light signals. In order to set the operating point below the saturation voltage of the opto-electronic component, a resistance circuit is connected in parallel with the opto-electronic component at least to compensate for direct light signals. The resistance circuit has a self-adjusting resistor, the resistance variation of which is at least voltage-dependent as soon as a given voltage below the saturation voltage is exceeded and thus loads the opto-electronic component until the set voltage is substantially attained. The compensation current required owing to the direct light is produced without an outside voltage in such a way that virtually no current need be taken from the power supply.
Abstract:
A photosensor arrangement for providing an exposure influencing control signal in a photographic camera apparatus includes an array of photoresponsive elements (P 1 -P 4 ) each arranged to have a different field of view, signal-generating means (R 14 -R 22 ) for generating the exposure-influencing signal in response to signals from the photoresponsive elements, and means (R 1 -R 8 ; D 1 -D 8 ; A,-As; 10-24) controlling the transmission of the output signals from the photoresponsive elements to the signal-generating means (R 14 -R 22 ) and operative to block the signal path to the signal-generating means from the photoresponsive element or elements detecting the highest and/or lowest scene light intensity, or from any photoresponsive element which detects a scene light intensity which is above a maximum light intensity threshold and/or any photosensitive element which detects a scene light intensity which is below a minimum light intensity threshold.
Abstract:
A sample and hold auto-zeroing feedback circuit (22) is utilized to drive the dark current of a solid state photodiode (10) to zero in the absence of incident light photons. The just previously attained compensation is then held during a subsequent quantitative measurement cycle when the photodiode is illuminated. A plurality of linear (24) and/or nonlinear (28) signal processing stages may also be included within the auto-zero compensation feedback loop such that their normal offset errors are also simultaneously compensated.
Abstract:
A circuit (10) prevents a photo diode (12) from reaching its saturation output voltage, thus ensuring the sensitivity of the photo diode to small changes in radiance at high radiance levels. The circuit (10) utilizes a transistor (30) that is allowed to conduct after the output voltage of the photo diode (12) has reached a predetermined level, thus shunt loading the photo diode and preventing it from reaching its saturation level. A resistor (28) - capacitor (32) time constant circuit is provided to prevent the transistor (30) from conducting until the output voltage of the photo diode (12) has reached a predetermined level for a predetermined period of time, thus preventing premature conduction of the transistor (30) in response to transient or spurious voltages.
Abstract:
A method of measuring optical power by means of an avalanche photodiode (1) comprises generating an electrical signal in response to and as an indication of the optical power (Pin) incident on the photodiode. When the incident optical power (Pin) is lower than a selected limit value (P1), the electrical signal is determined as a function of a current (Id) generated in the photodiode (1) by the optical power. When the incident optical power exceeds this limit value, the current in the photodiode (1) is limited to a constant value (Imax). The electrical signal is determined when the incident optical power (Pin) exceeds the limit value (P1) so that it comprises a contribution which is a function of the voltage (Vd) across the photodiode. A corresponding optical receiver comprises means for determining the electrical signal in response to a current (Id) in the photodiode, and means (3) for limiting the current in the photodiode (1) to a constant value (Imax) when the incident optical power (Pin) exceeds a selected limit value (P1). Further, the receiver comprises means (10, 11) for determining the electrical signal so that it comprises a contribution which is a function of the voltage (Vd) across the photodiode when the incident optical power (Pin) exceeds the limit value (P1).
Abstract:
A temperature independent dosimeter for measuring an amount of irradiation of a predetermined frequency. A photodiode (24) operating in its photovoltaic mode is irradiated with the irradiation to produce a signal that is amplitude-proportional to the amplitude of the irradiation. The signal is converted by a pair of operational amplifiers (89, 96) to a plurality of pulses that are proportional in frequency to the amplitude of the signal. The plurality of pulses is counted by a counter (20) and the irradiation is terminated when the count reaches a predetermined amount.
Abstract:
A circuit arrangement for a light signal receiver for receiving and recognising light signals which are transmitted in pulses and on which ambient light is superimposed in a parasitic manner with an undefinable intensity contains a two-pole light sensor and a separate current-voltage converter (N1, N2) for direct current for each terminal of the light sensor (1), in which each terminal is connected to an identical signal input of a current-voltage converter (N1, N2) which have the same transmission behaviour, are connected as amplifying filters and are negative feedback connected in d.c. array and frequency-dependently via the input to which the terminal of the light sensor (1) is connected so strongly that the d.c. voltage across the terminals of the light sensor (1) is constant, regardless of the intensity of the parasitic light and the outputs of the current-voltage converter are a.c. connected to an input of a differential amplifier (N3).
Abstract:
An avalanche photodiode quenching circuit (20) incorporates an avalanche photodiode (APD) (22) and a first comparator (C1) responsive to reduction in APD voltage. The comparator (C1) is arranged to activate an APD quench circuit (38) in response to APD avalanche initiation. The circuit (20) also includes a second comparator (C2) arranged to reset the first comparator input (N2) in response to a further reduction in APD voltage caused by initiation of quenching. The second comparator (C2) is also connected to a monostable circuit (48) arranged to latch the first comparator output response to resetting. The monostable circuit (48) maintains the first comparator output level constant until the APD (22) has recharged.