Cargando…
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(-) epi-layer with diameters of 50, 100, 200, and 400...
Autores principales: | , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2020
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7569859/ https://www.ncbi.nlm.nih.gov/pubmed/32961756 http://dx.doi.org/10.3390/mi11090869 |
_version_ | 1783596816179134464 |
---|---|
author | Goll, Bernhard Steindl, Bernhard Zimmermann, Horst |
author_facet | Goll, Bernhard Steindl, Bernhard Zimmermann, Horst |
author_sort | Goll, Bernhard |
collection | PubMed |
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(-) 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. |
format | Online Article Text |
id | pubmed-7569859 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-75698592020-10-27 Avalanche Transients of Thick 0.35 µm CMOS Single-Photon Avalanche Diodes Goll, Bernhard Steindl, Bernhard Zimmermann, Horst Micromachines (Basel) Article 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. MDPI 2020-09-19 /pmc/articles/PMC7569859/ /pubmed/32961756 http://dx.doi.org/10.3390/mi11090869 Text en © 2020 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Goll, Bernhard Steindl, Bernhard Zimmermann, Horst Avalanche Transients of Thick 0.35 µm CMOS Single-Photon Avalanche Diodes |
title | 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_short | 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 |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7569859/ https://www.ncbi.nlm.nih.gov/pubmed/32961756 http://dx.doi.org/10.3390/mi11090869 |
work_keys_str_mv | AT gollbernhard avalanchetransientsofthick035μmcmossinglephotonavalanchediodes AT steindlbernhard avalanchetransientsofthick035μmcmossinglephotonavalanchediodes AT zimmermannhorst avalanchetransientsofthick035μmcmossinglephotonavalanchediodes |