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Design and performance of a 96-channel resistive PICOSEC Micromegas detector for ENUBET
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Abstract
The PICOSEC-Micromegas (PICOSEC-MM) detector is a fast
gaseous detector concept that achieves picosecond-level timing. It
couples a Cherenkov radiator, typically an MgF
2
crystal,
to a Micromegas-based photodetector equipped with a photocathode,
allowing the fast photoelectron-induced signal to suppress the
intrinsic time jitter characteristic of gaseous detectors. This
design enables sub-20 ps timing precision while preserving the
robustness and scalability of Micro-Pattern Gaseous Detector (MPGD)
technologies. The 96-pad PICOSEC-MM detector represents the latest
advancement in this development, optimized for precision timing in
high-energy physics. Building upon the R&D insights obtained with
earlier 7-pad resistive prototypes, this large-area demonstrator was
developed to validate the scalability, uniformity, and robustness of
the technology for integration into the ENUBET project. The detector
employs a 2.5 nm Diamond-Like Carbon (DLC) photocathode with a
Micromegas board equipped with surface resistivity of
10 MΩ/□, providing an excellent timing
performance. The prototype was characterized using 150 GeV/
c
muons at the CERN SPS beamline, with one-third of the active area
instrumented during each run. A dedicated alignment procedure,
developed for multi-pad PICOSEC-MM systems, was used to reconstruct
the pad centers and combine measurements across different detector
regions. The measured timing resolution was 43 ps across the
instrumented pads, while the Signal Arrival Time (SAT) distributions
exhibited a good uniformity among the detector area that was
tested. Mechanical flatness was identified as a key factor
influencing timing precision. Maintaining a planarity tolerance
within 10 μm is therefore critical to preserve a good timing
resolution over large active areas. The successful operation of the
96-pad demonstrator confirms the scalability of the PICOSEC-MM
concept marking a significant step toward implementing robust,
high-granularity, picosecond-level gaseous timing detectors in
monitored neutrino beam experiments such as ENUBET.
IOP Publishing
A. Kallitsopoulou
S. Aune
Y. Angelis
R. Aleksan
A. Bonenfant
J. Bortfeldt
F. Brunbauer
M. Brunoldi
J. Datta
D. Desforge
G. Fanourakis
D. Fiorina
K.J. Floethner
M. Gallinaro
F. Garcia
I. Giomataris
K. Gnanvo
F.J. Iguaz
D. Janssens
F. Jeanneau
M. Kebbiri
M. Kovacic
B. Kross
P. Legou
M. Lisowska
J. Liu
C. Loiseau
M. Lupberger
I. Maniatis
J. McKisson
B. Moreno
Y. Meng
H. Muller
E. Oliveri
G. Orlandini
A. Pandey
T. Papaevangelou
M. Pomorski
E.F. Ribas
L. Ropelewski
D. Sampsonidis
L. Scharenberg
T. Schneider
E. Scorsone
L. Sohl
M. van Stenis
Y. Tsipolitis
S.E. Tzamarias
A. Utrobicic
I. Vai
R. Veenhof
P. Vitulo
X. Wang
S. White
W. Xi
Z. Zhang
Y. Zhou
Title: Design and performance of a 96-channel resistive PICOSEC Micromegas detector for ENUBET
Description:
Abstract
The PICOSEC-Micromegas (PICOSEC-MM) detector is a fast
gaseous detector concept that achieves picosecond-level timing.
It
couples a Cherenkov radiator, typically an MgF
2
crystal,
to a Micromegas-based photodetector equipped with a photocathode,
allowing the fast photoelectron-induced signal to suppress the
intrinsic time jitter characteristic of gaseous detectors.
This
design enables sub-20 ps timing precision while preserving the
robustness and scalability of Micro-Pattern Gaseous Detector (MPGD)
technologies.
The 96-pad PICOSEC-MM detector represents the latest
advancement in this development, optimized for precision timing in
high-energy physics.
Building upon the R&D insights obtained with
earlier 7-pad resistive prototypes, this large-area demonstrator was
developed to validate the scalability, uniformity, and robustness of
the technology for integration into the ENUBET project.
The detector
employs a 2.
5 nm Diamond-Like Carbon (DLC) photocathode with a
Micromegas board equipped with surface resistivity of
10 MΩ/□, providing an excellent timing
performance.
The prototype was characterized using 150 GeV/
c
muons at the CERN SPS beamline, with one-third of the active area
instrumented during each run.
A dedicated alignment procedure,
developed for multi-pad PICOSEC-MM systems, was used to reconstruct
the pad centers and combine measurements across different detector
regions.
The measured timing resolution was 43 ps across the
instrumented pads, while the Signal Arrival Time (SAT) distributions
exhibited a good uniformity among the detector area that was
tested.
Mechanical flatness was identified as a key factor
influencing timing precision.
Maintaining a planarity tolerance
within 10 μm is therefore critical to preserve a good timing
resolution over large active areas.
The successful operation of the
96-pad demonstrator confirms the scalability of the PICOSEC-MM
concept marking a significant step toward implementing robust,
high-granularity, picosecond-level gaseous timing detectors in
monitored neutrino beam experiments such as ENUBET.
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