Persistence filtering in spd arrays
US-2024406582-A1 · Dec 5, 2024 · US
US10612972B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10612972-B2 |
| Application number | US-201715846296-A |
| Country | US |
| Kind code | B2 |
| Filing date | Dec 19, 2017 |
| Priority date | Dec 22, 2016 |
| Publication date | Apr 7, 2020 |
| Grant date | Apr 7, 2020 |
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A light receiver ( 100 ), comprising: a plurality of avalanche photodiode elements ( 10 ) each being biased with a bias voltage above a breakdown voltage and thus operated in a Geiger mode in order to trigger a Geiger current upon light reception and a plurality of readout circuits ( 42, 44, 46 ) associated with individual avalanche photodiode elements ( 10 ) or a group of avalanche photodiode elements ( 10 ) for reading out a Geiger current generated upon light reception, wherein the readout circuits ( 42, 44, 46 ) each comprise a measurement path ( 42 ) and a blanking path ( 46 ) as well as a switching element ( 44 ) for selectively supplying the Geiger current, or a measurement current corresponding to the Geiger current, to the measurement path ( 42 ) or the blanking path ( 46 ).
Opening claim text (preview).
The invention claimed is: 1. A light receiver ( 100 ), comprising: a plurality of avalanche photodiode elements ( 10 ) each being biased with a bias voltage above a breakdown voltage and thus operated in a Geiger mode in order to trigger a Geiger current upon light reception; and a plurality of readout circuits ( 42 , 44 , 46 ) associated with individual avalanche photodiode elements ( 10 ) or a group of avalanche photodiode elements ( 10 ) for reading out a Geiger current generated upon light reception, wherein the readout circuits ( 42 , 44 , 46 ) each comprise a measurement path ( 42 ) and a blanking path ( 46 ) as well as a switching element ( 44 ) for selectively supplying the Geiger current, or a measurement current corresponding to the Geiger current, to the measurement path ( 42 ) or the blanking path ( 46 ) to switch regions of the light receiver ( 100 ) to the blanking path ( 46 ), such that the regions are muted or at least evaluated in a different manner than the avalanche photodiode elements ( 10 ), the readout circuits ( 42 , 44 , 46 ) thereof being connected to the measurement path ( 42 ). 2. The light receiver ( 100 ) according to claim 1 , wherein the switching element ( 44 ) is a readout transistor ( 48 ). 3. The light receiver ( 100 ) according to claim 1 , wherein the blanking path ( 46 ) is configured to let the Geiger current or the measurement current be drained without reading out. 4. The light receiver ( 100 ) according to claim 1 , wherein a signal detection circuit ( 12 ) is provided for the readout circuit ( 42 , 44 , 46 ) and the associated individual avalanche photodiode element ( 10 ) or the associated group of avalanche photodiode elements ( 10 ), the signal detection circuit ( 12 ) comprising an active coupling element ( 32 ) having an input ( 34 ) connected to the avalanche photodiode elements ( 10 ) and an output ( 36 ) which maps the Geiger current at the input ( 34 ) to the measurement current corresponding to the Geiger current in its course and level, wherein the input ( 34 ) forms a virtual short-circuit for the Geiger current to a potential (ground; −U BE ; U const −U BE ) and the output ( 36 ) is decoupled from the input ( 34 ). 5. The light receiver ( 100 ) according to claim 4 , wherein the coupling element ( 32 ) comprises one signal detection transistor. 6. The light receiver ( 100 ) according to claim 5 , wherein the base voltage of the signal detection transistor is adaptable for switching between the measurement path ( 42 ) and the blanking path ( 46 ). 7. The light receiver ( 100 ) according to claim 4 , wherein the readout circuit ( 42 , 44 , 46 ) is connected to the input ( 34 ). 8. The light receiver ( 100 ) according to claim 7 , wherein the readout circuit ( 42 , 44 , 46 ) comprises only one readout transistor ( 48 ). 9. The light receiver ( 100 ) according to claim 8 , wherein the base voltage of the readout transistor ( 48 ) is adaptable for switching between the measurement path ( 42 ) and the blanking path ( 46 ). 10. The light receiver ( 100 ) according to claim 4 , wherein the readout circuit ( 42 , 44 , 46 ) is connected to the output ( 36 ). 11. The light receiver ( 100 ) according to claim 10 , wherein the coupling element ( 32 ) comprises a signal detection transistor, and wherein the readout circuit ( 42 , 44 , 46 ) comprises at least two parallel readout transistors ( 48 a - b ) each in a cascode circuit with the signal detection transistor. 12. The light receiver ( 100 ) according to claim 1 , wherein the blanking path ( 46 ) comprises a measurement tap. 13. The light receiver ( 100 ) according to claim 1 , wherein the readout circuit ( 42 , 44 , 46 ) comprises at least one further measurement path ( 52 ). 14. The light receiver ( 100 ) according to claim 13 , wherein measurement path ( 42 ) and further measurement path ( 52 ) each have a measurement tap, the measurement taps having different attenuations of the Geiger current or the measurement current. 15. The light receiver ( 100 ) according to claim 14 , wherein measurement path ( 42 ) and further measurement path ( 52 ) comprise a voltage attenuation circuit or different working impedances. 16. The light receiver ( 100 ) according to claim 1 , wherein the avalanche photodiode elements ( 10 ) comprise an electrode ( 28 ) for providing the Geiger current with capacitive coupling, and wherein the readout circuit ( 42 , 44 , 46 ) is connected to the electrode ( 28 ). 17. An optoelectronic sensor having at least one light receiver ( 100 ), the light receiver ( 100 ) comprising: a plurality of avalanche photodiode elements ( 10 ) each being biased with a bias voltage above a breakdown voltage and thus operated in a Geiger mode in order to trigger a Geiger current upon light reception; and a plurality of readout circuits ( 42 , 44 , 46 ) associated with individual avalanche photodiode elements ( 10 ) or a group of avalanche photodiode elements ( 10 ) for reading out a Geiger current generated upon light reception, wherein the readout circuits ( 42 , 44 , 46 ) each comprise a measurement path ( 42 ) and a blanking path ( 46 ) as well as a switching element ( 44 ) for selectively supplying the Geiger current, or a measurement current corresponding to the Geiger current, to the measurement path ( 42 ) or the blanking path ( 46 ) to switch regions of the light receiver ( 100 ) to the blanking path ( 46 ), such that the regions are muted or at least evaluated in a different manner than the avalanche photodiode elements ( 10 ), the readout circuits ( 42 , 44 , 46 ) thereof being connected to the measurement path ( 42 ). 18. The optoelectronic sensor according to claim 17 , the sensor being configured as a sensor for measuring distances according to a time of flight method. 19. The optoelectronic sensor according to claim 17 , the sensor being configured as a code reader. 20. The optoelectronic sensor according to claim 17 , the sensor being configured for data transmission. 21. A method for reading out avalanche photodiode elements ( 10 ), each being biased with a bias voltage above a breakdown voltage and thus operated in a Geiger mode, wherein the avalanche photodiode elements ( 10 ) trigger a Geiger current upon light reception and wherein the Geiger current from individual avalanche photodiode elements ( 10 ) or groups of avalanche photodiode elements ( 10 ) is read out, and wherein the Geiger current, or a measurement current corresponding to the Geiger current, is selectively supplied to a measurement path ( 42 ) or to a blanking path ( 46 ) by switching a switching element ( 44 ) to switch regions of a light receiver ( 100 ) to the blanking path ( 46 ), such that the regions are muted or at least evaluated in a different manner than the avalanche photodiode elements ( 10 ), readout circuits ( 42 , 44 , 46 ) thereof being connected to the measurement path ( 42 ).
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