Geiger mode APD light receiver having an active readout forming a virtual short-circuit

US10018505B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-10018505-B2
Application numberUS-201615216086-A
CountryUS
Kind codeB2
Filing dateJul 21, 2016
Priority dateJul 27, 2015
Publication dateJul 10, 2018
Grant dateJul 10, 2018

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  1. Title

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  5. First independent claim

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Abstract

Official abstract text for this publication.

A light receiver ( 10, 50 ) having a plurality of avalanche photo diode elements ( 10, 12 a - c ) which are biased with a bias voltage greater than a breakthrough voltage and are thus operated in a Geiger mode in order to trigger a Geiger current upon light reception, and having a signal detection circuit ( 50 ) for reading out the avalanche photo diode elements ( 10, 12 a - c ), wherein the signal detection circuit ( 50 ) comprises an active coupling element ( 52 ) having an input ( 54 ) connected to the avalanche photo diode elements ( 10, 12 a - c ) and an output ( 56 ), the active coupling element ( 52 ) mapping the Geiger current at the input ( 54 ) to a measuring current corresponding to the Geiger current in its course and level, wherein the input ( 54 ) forms a virtual short-circuit for the Geiger current with respect to a potential (ground, −U BE ; U const −U BE ), and the output ( 56 ) is decoupled from the input ( 54 ).

First claim

Opening claim text (preview).

The invention claimed is: 1. A light receiver ( 10 , 50 ) having a plurality of avalanche photo diode elements ( 10 , 12 a - c ) which are biased with a bias voltage greater than a breakthrough voltage and are thus operated in a Geiger mode in order to trigger a Geiger current upon light reception, and having a signal detection circuit ( 50 ) for reading out the avalanche photo diode elements ( 10 , 12 a - c ), wherein the signal detection circuit ( 50 ) comprises an active coupling element ( 52 ) having an input ( 54 ) connected to the avalanche photo diode elements ( 10 , 12 a - c ) and an output ( 56 ), the active coupling element ( 52 ) mapping the Geiger current at the input ( 54 ) to a measuring current corresponding to the Geiger current in its course and level, wherein the input ( 54 ) forms a virtual short-circuit for the Geiger current with respect to a potential (ground, −U BE ; U const −U BE ), and the output ( 56 ) is decoupled from the input ( 54 ). 2. The light receiver ( 10 , 50 ) according to claim 1 , wherein the course of the measuring current deviates from the Geiger current only for fluctuations in a higher Gigahertz range. 3. The light receiver ( 10 , 50 ) according to claim 2 , wherein the course of the measuring current deviates from the Geiger current only for fluctuations in a range above 2 Ghz or 3 GHz. 4. The light receiver ( 10 , 50 ) according to claim 1 , wherein a measurement circuit is connected to the output ( 56 ). 5. The light receiver ( 10 , 50 ) according to claim 1 , wherein the signal detection circuit ( 50 ) comprises a constant current source ( 58 ) connected to the coupling element ( 52 ) for setting its operating point. 6. The light receiver ( 10 , 50 ) according to claim 1 , wherein the signal detection circuit ( 50 ) comprises a resistor ( 60 ) connected to the coupling element ( 52 ) for setting its operating point. 7. The light receiver ( 10 , 50 ) according to claim 1 , wherein the coupling element ( 52 ) is configured to maintain a constant voltage at the input ( 54 ) side. 8. The light receiver ( 10 , 50 ) according to claim 1 , wherein the coupling element ( 52 ) comprises exactly one transistor. 9. The light receiver ( 10 , 50 ) according to claim 8 , wherein the transistor is operated in a common base circuit or gate circuit in that the input ( 54 ) is connected to emitter or source, the output ( 56 ) is connected to collector or drain, and base or gate is connected to a fixed potential. 10. The light receiver ( 10 , 50 ) according to claim 1 , wherein the avalanche photo diode elements ( 10 , 12 a - c ) comprise a first electrode ( 16 ) and a second electrode ( 18 ) used for biasing. 11. The light receiver ( 10 , 50 ) according to claim 10 , wherein a charging unit ( 20 a - c ) is arranged between a respective avalanche photo diode element ( 12 a ) and the first electrode ( 16 ) or the second electrode ( 18 ). 12. The light receiver ( 10 , 50 ) according to claim 10 , wherein the avalanche photo diode elements ( 10 , 12 a - c ) comprise a third electrode ( 24 ) as a capacitively coupled output for the Geiger current. 13. The light receiver ( 10 , 50 ) according to claim 12 , wherein the input ( 54 ) is connected to the third electrode ( 24 ). 14. The light receiver ( 10 , 50 ) according to claim 1 , wherein an additional signal channel is provided at the input ( 54 ) for capacitively feeding an additional signal into the signal detection circuit ( 50 ). 15. An optoelectronic sensor comprising at least one light detector ( 10 , 50 ) having a plurality of avalanche photo diode elements ( 10 , 12 a - c ) which are biased with a bias voltage greater than a breakthrough voltage and are thus operated in a Geiger mode in order to trigger a Geiger current upon light reception, and having a signal detection circuit ( 50 ) for reading out the avalanche photo diode elements ( 10 , 12 a - c ), wherein the signal detection circuit ( 50 ) comprises an active coupling element ( 52 ) having an input ( 54 ) connected to the avalanche photo diode elements ( 10 , 12 a - c ) and an output ( 56 ), the active coupling element ( 52 ) mapping the Geiger current at the input ( 54 ) to a measuring current corresponding to the Geiger current in its course and level, wherein the input ( 54 ) forms a virtual short-circuit for the Geiger current with respect to a potential (ground, −U BE ; U const −U BE ), and the output ( 56 ) is decoupled from the input ( 54 ), wherein the sensor is configured for at least one of distance measurement according to a light time of flight method, code reading and data transmission. 16. A readout method for avalanche photo diode elements ( 10 , 12 a - c ) which are biased with a bias voltage greater than a breakthrough voltage and are thus operated in a Geiger mode and trigger a Geiger current upon light reception, wherein the Geiger current flows through a connection between avalanche photo diode element ( 10 ) and an input ( 54 ) of an active coupling element ( 52 ) due to a virtual short-circuit with respect to a potential (ground, −U BE ; U const −U BE ), wherein, in the coupling element ( 52 ), the Geiger current is mapped to a measuring current corresponding to the Geiger current in its course and level at an output ( 56 ) of the coupling element ( 52 ), and wherein the output ( 56 ) is decoupled from the input ( 54 ) so that the Geiger current is unaffected by further processing of the measuring current.

Assignees

Inventors

Classifications

  • Detector arrays, e.g. charge-transfer gates · CPC title

  • Electricity · mapped topic

  • Avalanche · CPC title

  • G01J1/44Primary

    Electric circuits {(for command of an exposure part G03B7/02)} · CPC title

  • G01J1/46Primary

    using a capacitor · CPC title

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What does patent US10018505B2 cover?
A light receiver ( 10, 50 ) having a plurality of avalanche photo diode elements ( 10, 12 a - c ) which are biased with a bias voltage greater than a breakthrough voltage and are thus operated in a Geiger mode in order to trigger a Geiger current upon light reception, and having a signal detection circuit ( 50 ) for reading out the avalanche photo diode elements ( 10, 12 a - c ), wherein th…
Who is the assignee on this patent?
Sick Ag
What technology area does this patent fall under?
Primary CPC classification G01J1/44. Mapped technology areas include Physics.
When was this patent published?
Publication date Tue Jul 10 2018 00:00:00 GMT+0000 (Coordinated Universal Time) (B2). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 8 related publications on this page (citations in our corpus or others sharing the same primary CPC).