Abstract

Two types of single-photon avalanche diodes (SPADs) with different diameters are investigated regarding their avalanche behavior. SPAD type A was designed in standard 0.35-µm complementary metal-oxide-semiconductor (CMOS) including a 12-µm thick p- epi-layer with diameters of 50, 100, 200, and 400 µm; and type B was implemented in the high-voltage (HV) line of this process with diameters of 48.2 and 98.2 µm. Each SPAD is wire-bonded to a 0.35-µm CMOS clocked gating chip, which controls charge up to a maximum 6.6-V excess bias, active, and quench phase as well as readout during one clock period. Measurements of the cathode voltage after photon hits at SPAD type A resulted in fall times (80 to 20%) of 10.2 ns for the 50-µm diameter SPAD for an excess bias of 4.2 V and 3.45 ns for the 200-µm diameter device for an excess bias of 4.26 V. For type B, fall times of 8 ns for 48.2-µm diameter and 5.4-V excess bias as well as 2 ns for 98.2-µm diameter and 5.9-V excess bias were determined. In measuring the whole capacitance at the cathode of the SPAD with gating chip connected, the avalanche currents through the detector were calculated. This resulted in peak avalanche currents of, e.g., 1.19 mA for the 100-µm SPAD type A and 1.64 mA for the 98.2-µm SPAD type B for an excess bias of 5 and 4.9 V, respectively.

Highlights

  • Avalanche photodiodes (APDs) operated with a reverse voltage larger than the breakdown voltage (Geiger mode) are usually capable of detecting single photons and are termed single-photonavalanche-diodes (SPADs)

  • There are many reasons for afterpulses, e.g., the release of a carrier by a deep-level trap, which has been filled during a previous current flow, or, e.g., the diffusion of secondary charge carriers into the high-field zone of the single-photon avalanche diode (SPAD), which were generated by photons originating from recombination during avalanche current flow

  • After an avalanche has happened in a SPAD, it needs a dead time, which is controlled by surrounding circuitry, until it is recharged again and ready for a new photon detection

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Summary

Introduction

Avalanche photodiodes (APDs) operated with a reverse voltage larger than the breakdown voltage (Geiger mode) are usually capable of detecting single photons and are termed single-photonavalanche-diodes (SPADs). This paper presents measurement results of the cathode voltage drop of two types of SPADs with different diameters when an avalanche occurs. The voltage transient response with a measurement of its 80 to 20% fall time of SPAD type A with 50 μm diameter was already published in [25].

Results
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