Avalanche Transients of Thick 0.35 µm CMOS Single-Photon Avalanche Diodes

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<sup>-</sup> epi-layer with diameters of...

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Main Authors: Bernhard Goll, Bernhard Steindl, Horst Zimmermann
Format: Article
Language:English
Published: MDPI AG 2020-09-01
Series:Micromachines
Subjects:
Online Access:https://www.mdpi.com/2072-666X/11/9/869
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spelling doaj-329272ad230a474495504b321f713ea52020-11-25T02:31:23ZengMDPI AGMicromachines2072-666X2020-09-011186986910.3390/mi11090869Avalanche Transients of Thick 0.35 µm CMOS Single-Photon Avalanche DiodesBernhard Goll0Bernhard Steindl1Horst Zimmermann2Institute of Electrodynamics, Microwave and Circuit Engineering, TU Wien, Gusshausstrasse 25/E354-02, A-1040 Wien, AustriaInstitute of Electrodynamics, Microwave and Circuit Engineering, TU Wien, Gusshausstrasse 25/E354-02, A-1040 Wien, AustriaInstitute of Electrodynamics, Microwave and Circuit Engineering, TU Wien, Gusshausstrasse 25/E354-02, A-1040 Wien, AustriaTwo 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<sup>-</sup> 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.https://www.mdpi.com/2072-666X/11/9/869single-photon avalanche diode (SPAD)gatingavalanche transients3.3 V/0.35 µm complementary metal-oxide-semiconductor (CMOS)
collection DOAJ
language English
format Article
sources DOAJ
author Bernhard Goll
Bernhard Steindl
Horst Zimmermann
spellingShingle Bernhard Goll
Bernhard Steindl
Horst Zimmermann
Avalanche Transients of Thick 0.35 µm CMOS Single-Photon Avalanche Diodes
Micromachines
single-photon avalanche diode (SPAD)
gating
avalanche transients
3.3 V/0.35 µm complementary metal-oxide-semiconductor (CMOS)
author_facet Bernhard Goll
Bernhard Steindl
Horst Zimmermann
author_sort Bernhard Goll
title Avalanche Transients of Thick 0.35 µm CMOS Single-Photon Avalanche Diodes
title_short Avalanche Transients of Thick 0.35 µm CMOS Single-Photon Avalanche Diodes
title_full Avalanche Transients of Thick 0.35 µm CMOS Single-Photon Avalanche Diodes
title_fullStr Avalanche Transients of Thick 0.35 µm CMOS Single-Photon Avalanche Diodes
title_full_unstemmed Avalanche Transients of Thick 0.35 µm CMOS Single-Photon Avalanche Diodes
title_sort avalanche transients of thick 0.35 µm cmos single-photon avalanche diodes
publisher MDPI AG
series Micromachines
issn 2072-666X
publishDate 2020-09-01
description 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<sup>-</sup> 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.
topic single-photon avalanche diode (SPAD)
gating
avalanche transients
3.3 V/0.35 µm complementary metal-oxide-semiconductor (CMOS)
url https://www.mdpi.com/2072-666X/11/9/869
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