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@ARTICLE{King:617744,
author = {King, Finn and Diehl, Inge and Feyens, Ono and Gregor,
Ingrid-Maria and Hansen, Karsten and Lachnit, Stephan and
Poblotzki, Frauke and Rastorguev, Daniil and Spannagel,
Simon and Vanat, Tomas and Vignola, Gianpiero},
title = {{T}est {B}eam {C}haracterization of a {D}igital {S}ilicon
{P}hotomultiplier},
journal = {Nuclear instruments $\&$ methods in physics research /
Section A},
volume = {1081},
issn = {0167-5087},
address = {[Amsterdam]},
publisher = {Elsevier},
reportid = {PUBDB-2024-07022},
pages = {170874},
year = {2025},
abstract = {Conventional silicon photomultipliers (SiPMs) are well
established as light detectors with single-photon-detection
capability and used throughout high energy physics, medical,
and commercial applications. The possibility to produce
single photon avalanche diodes (SPADs) in commercial CMOS
processes creates the opportunity to combine a matrix of
SPADs and an application-specific integrated circuit in the
same die. The potential of such digital SiPMs (dSiPMs) is
still being explored, while it already is an established
technology in certain applications, like light detection and
ranging (LiDAR). A prototype dSiPM, produced in the LFoundry
150-nm CMOS technology, was designed and tested at DESY. The
dSiPM central part is a matrix of 32 by 32 pixels. Each
pixel contains four SPADs, a digital front-end, and has an
area of 69.6 × 76 µm2. The chip has four time-to-digital
converters and includes further circuitry for data
serialization and data links.This work focuses on the
characterization of the prototype in an electron beam at the
DESY II Test Beam facility, to study its capability as a
tracking and timing detector for minimum ionizing particles
(MIPs). The MIP detection efficiency is found to be
dominated by the fill factor and on the order of 31 $\%.$
The position of the impinging MIPs can be measured with a
precision of about 20 µm, and the time of the interaction
can be measured with a precision better than 50 ps for about
85 $\%$ of the detected events. In addition, laboratory
studies on the breakdown voltage, dark count rate, and
crosstalk probability, as well as the experimental methods
required for the characterization of such a sensor type in a
particle beam are presented.},
cin = {ATLAS / CMS / FE},
ddc = {530},
cid = {I:(DE-H253)ATLAS-20120731 / I:(DE-H253)CMS-20120731 /
I:(DE-H253)FE-20120731},
pnm = {622 - Detector Technologies and Systems (POF4-622)},
pid = {G:(DE-HGF)POF4-622},
experiment = {EXP:(DE-H253)TestBeamline21-20150101},
typ = {PUB:(DE-HGF)16},
doi = {10.1016/j.nima.2025.170874},
url = {https://bib-pubdb1.desy.de/record/617744},
}