IEEE 2026 NSS MIC RTSD

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Photodetectors

Session chair: Retiere, Fabrice, (TRIUMF, Vancouver, Canada); Gundacker, Stefan, Dr. (Marietta Blau Institute for Particle Physics, Vienna, Austria)
 
Shortcut: NSS-21
Date: Thursday, 12 November, 2026, 9:00 - 11:00
Location: MACHADO
Session type: NSS Session

Contents

Click on an contribution to preview the abstract content.

The underlined authors are the presenters. The authors in bold are the main authors.

9:00 NSS-21-01

Development of a Cost-Effective PCCT Detector Based on Sub-Millimeter EQR SiPM and LYSO Array with High Count Rate and Adequate Energy Resolution (#6)

Y. Yan1, M. Huang1, X. Zhang1, K. Liang1, R. Yang1, D. Han1, 2

1 Beijing Normal University, school of Physics and Astronomy, Beijing, China
2 Beijing Normal University, Applied Optics Beijing Area Major Laboratory, Beijing, China

Abstract

Among the detector candidates for clinical photon-counting CT (PCCT), SiPM-based fast-scintillation photon-counting detectors (PCD) represent a cost-effective solution. However, their practical implementation is constrained by the incompatible trade-off between count-rate capability and energy resolution. To address this limitation, we developed a scintillation PCD designed to achieve both high counting rate and improved energy resolution. The detector consists of a 26-channel pixelated LYSO scintillator array coupled to an epitaxial-quenching-resistor (EQR) SiPM array with a 0.5-mm pixel pitch and 15-μm microcells. Benefiting from the EQR architecture, the SiPM pixels exhibit a fast recovery time of 3.2 ns, a 64% fill factor, and a photon detection efficiency exceeding 40% at 420 nm. A multi-channel FPGA-based photon-counting readout circuit with per-channel pole-zero cancellation was developed to suppress signal tailing and mitigate pulse pile-up. This PCD achieved a maximum count rate of 46.3 Mcps/mm² while maintaining an energy resolution of 33.7% at 59.5 keV. The spatial resolution of 1.86 lp/mm (537 μm) was achieved under 120-keV X-rays, which agreed closely with the 0.5-mm physical pixel pitch of the detector. A more sophisticated PCD based on a 64-channel EQR SiPM array with 0.25-mm pixel pitch and 10-μm microcells, coupled to a corresponding pixelated LYSO scintillator array, will also be presented. Those results indicate that the proposed scintillation PCD is a promising cost-effective candidate for clinical PCCT applications.

References
[1] Willemink, MJ, Persson, M, Pourmorteza, A, Pelc, NJ & Fleischmann. 2018, ‘Photon-counting CT: Technical Principles and Clinical Prospects’, Radiology, vol. 289, no. 2, pp. 293–312, Easton: Radiological Society of North America.
[2] Yan, Y, et al. 2026, ‘Epitaxial Quenching Resistor SiPM With Counting Rate Enhanced Technique Aiming at Photon-Counting CT Applications’, IEEE Transactions on Radiation and Plasma Medical Sciences, pp. 1-1, Piscataway: IEEE.
[3] Yan, Y, et al. 2026, ‘A high-count-rate X-ray photon-counting detector based on EQR SiPM array aiming at PCCT’, Nucl. Instrum. Methods Phys. Res. A, vol. 1087, p. 171393, Amsterdam: Elsevier.
[4] Zhang G. et al. 2010,'Demonstration of a silicon photomultiplier with bulk integrated quenching resistors on epitaxial silicon,'Nucl. Instrum. Methods Phys. Res. A, vol. 621, no. 1–3, pp. 116–120., Amsterdam: Elsevier.
Keywords: photon couting CT, SiPM, count rate, spatial resolution
9:15 NSS-21-02

First Characterisation Results on Backside-Illuminated SiPM Prototypes from the IBIS Project (#2930)

R. Preghenella1, F. Acerbi2, P. Antonioli1, E. Bertolin2, 4, F. Carnesecchi1, F. Caso2, D. Elgewaily2, G. Fadini1, 3, A. Ficorella2, C. Forza2, A. Gola2, P. Kachru2, E. Montagna1, A. Montanari1, R. Nania1, L. Parellada-Monreal2, G. Paternoster2, R. Ricci1, L. Rignanese1, E. Rovati1, 3, B. Sabiu1, 3, G. Sirri1, N. Tosi1, C. Trippl2, O. Villarreal2

1 Istituto Nazionale di Fisica Nucleare, Sezione di Bologna, Bologna, Italy
2 Fondazione Bruno Kessler, Trento, Italy
3 Università di Bologna, Bologna, Italy
4 Università di Milano Bicocca e INFN Sezione Milano Bicocca, Milano, Italy

On behalf of the IBIS and IBIS_NEXT Collaborations

Abstract

We report on the development and characterisation of innovative Backside-Illuminated Silicon Photomultipliers (BSI-SiPMs) within the INFN IBIS and IBIS_NEXT projects. The BSI architecture relocates the photon entrance window to the back side of the device, enabling high fill factor and improved photon detection efficiency while preserving compatibility with advanced front-end electronics integration, and offering the potential for enhanced sensitivity in the VUV region.
A preliminary experimental campaign has been performed on partially processed BSI prototype devices, including electrical characterisation over a wide temperature range, dark count rate measurements, irradiation studies, annealing tests, and timing performance evaluation using both pulsed laser excitation and minimum ionising particles (MIPs) at CERN.
Irradiation up to 109 neq/cm2 results in an increase in dark count rate. Preliminary annealing studies show recovery of dark current by nearly one order of magnitude. Timing measurements yield resolutions of order ~100 ps, demonstrating the potential of BSI-SiPMs for fast timing applications in high-energy physics.

AcknowledgmentThe authors acknowledge INFN and FBK for support and sensor production, and the CERN PS facility for beam test operations.
Keywords: Photodetectors, Silicon Photomultipliers, Backside-Illuminated SiPM, Radiation Damage, Timing Performance
9:30 NSS-21-03

Photon-to-Digital Converters Enabling Event Classification Through Pulse Shape Discrimination (#1301)

G. Lessard1, C. M. Pepin1, T. Rossignol1, N. Roy1, F. Vachon1, R. Espagnet1, G. Lemaire1, A. L. Steinhebel2, P. Hausladen2, L. Fabris2, R. Lecomte3, R. Fontaine1, J.-F. Pratte1, S. A. Charlebois1

1 Université de Sherbrooke, Interdisciplinary Institute for Technological Innovation and Department of Electrical and Computer Engineering, Sherbrooke, Québec, Canada
2 Oak Ridge National Laboratory, Oak Ridge, Tennessee, United States of America
3 Université de Sherbrooke, Sherbrooke Molecular Imaging Center and Department of Medical Imaging and Radiation Sciences, Sherbrooke, Québec, Canada

Abstract

Digital silicon photomultipliers (SiPMs) are being developed to circumvent many of the shortfalls inherent to analog SiPMs and their associated readout electronics. We design 3D-integrated digital SiPMs, called Photon-to-Digital Converters (PDCs), to simultaneously optimize the photosensitive area, remove analog noise contributions, and embed signal processing. With a low-power-optimized readout architecture providing high timing resolution, we demonstrate fully digital measurement approaches and their benefits across multiple fields, including time-of-flight medical imaging and neutron imaging. Leveraging the high-timing precision of the PDC through pulse shape discrimination, the components of an LGSO (Fast/Slow) phoswich scintillator assembly are precisely classified, while maintaining the expected energy resolution for the scintillators irradiated with calibration isotopes such as a 68Ge source. Coincidence timing resolution is also assessed for this configuration. These results position PDCs as great candidates for depth-of-interaction reconstruction in PET imaging, ToF measurement in CT imaging, and particle identification in neutron imaging.

AcknowledgmentThe present work was supported in part by the United States Department of Energy, Office of Defense Nuclear Nonproliferation Research and Development in the National Nuclear Security Administration.
References
[1] J.-F. Pratte et al., “3D Photon-To-Digital Converter for Radiation Instrumentation: Motivation and Future Works,” Sensors, vol. 21, no. 2, p.598, Jan. 2021,  number: 2 Publisher: Multidisciplinary Digital Publishing Institute. URL: https://www.mdpi.com/1424-8220/21/2/598
[2] S. Parent et al., “Wafer-Level Characterization and Monitoring Platform for Single-Photon Avalanche Diodes,” IEEE Journal of the Electron Devices Society, vol. 12, pp. 127–137, 2024. URL: https://doi.org/10.1109/JEDS.2024.3359088
[3] T. Rossignol et al., “A 3D photon-to-digital converter readout for low-power and large-area applications,” Journal of Instrumentation, vol. 19, no. 09, p. P09017, Sep. 2024. URL: https://dx.doi.org/10.1088/1748-0221/19/09/P09017
Keywords: single-photon avalanche diode, photon-to-digital converter, 3D integrated detector, CMOS, radiation detection
9:45 NSS-21-04

Progress on Single-cell-access TSVs for 3D-integrated microSiPM readout in fast-timing SiPM detectors (#2683)

A. Gola1, S. Bisi2, C. Bruschini2, E. Charbon2, S. Gundacker4, 3, K. Herweg3, 5, P. Kachru1, L. Parellada Monreal1, G. Paternoster1, M. Penna1, M. Ruzzarin1, D. Schug3, 5, V. Schulz5, 6, N. Zorzi1

1 Fondazione Bruno Kessler (FBK), Trento, Italy
2 Ecole Polythechnique federale de Lausanne (EPFL), AQUA Lab, Neuchatel, Switzerland
3 University Hospital RWTH Aachen, Aachen, Germany
4 Austrian Academy of Sciences, Institute of High Energy Physics, Vienna, Austria
5 RWTH Aachen University, Institute of Imaging and Computer Vision, Aachen, Germany
6 Hyperion Hybrid Imaging Systems GmbH, Aachen, Germany

Abstract

Segmentation of the SiPM active area into smaller, independently read out elements is one of the most promising routes to improve the single-photon time resolution (SPTR) required by next-generation time-of-flight PET systems. We report on Single-Cell Access through-silicon vias (SCA-TSVs), a custom TSV technology under development at Fondazione Bruno Kessler (FBK), Trento, and applied to the NUV-HD-MT SiPM platform. SCA-TSVs exploit the deep-trench isolation (DTI) already present in this technology to physically separate and independently access each SiPM microcell from the backside, with essentially no loss of fill factor. A backside redistribution layer (RDL) can then regroup microcells with an arbitrary segmentation level, according to application requirements. The first implementation targets the DIGILOG project, where a 3 × 3 mm² SiPM with 50 µm cells is segmented into 3 × 3- or 6 × 6-cell clusters, referred to as microSiPMs. These units are designed to be read out independently by a matched ASIC developed at EPFL and connected through chip-to-chip 3D integration. This approach preserves the SPTR of a single SPAD, approximately 25 ps FWHM, while avoiding the complexity of full single-cell readout. The first SCA-TSV learning cycle (LC1) required modifications to the original NUV-HD-MT technology, mainly an increase of the DTI depth beyond 20 µm. Front-side characterization showed that the timing performance was preserved. The first backside integration runs also revealed a reduced TSV yield. The analysis identified both layout-related and backside-process-related limitations, which are being addressed through optimized LC1 backend process splits and in the second technology learning cycle (LC2). The presentation will discuss the SCA-TSV concept, LC1 fabrication and characterization results, and the latest LC2 developments toward 3D-integrated microSiPM/ASIC chips for fast-timing applications.

References
[1] A. Gola, " FBK roadmap towards the next-generation of 3D-integrated SiPM and SPAD technologies.", PD 2024 Conference, Vancouver, Canada.
[2] S. Merzi et al., "NUV-HD SiPMs with metal-filled trenches," J. Instrum., vol. 18, no. 05, P05040, 2023.
[3] S. Gundacker et al., "DIGILOG: A digital-analog SiPM towards 10 ps prompt-photon tagging in TOF-PET," in 2023 IEEE NSS/MIC/RTSD, 2023.
[4] F. Acerbi et al., "Characterization of single-photon time resolution: from single SPAD to silicon photomultiplier," IEEE Trans. Nucl. Sci., vol. 61, no. 5, pp. 2678-2686, 2014.
Keywords: SiPM, TSV, Timing, 3D Integration
10:00 NSS-21-05

PlatonSPAD: A Scalable Sensor for Elementary Particle Detection (#1496)

K. Kaneyasu1, T. Dieminger2, J. Soerensen2, D. Sgalaberna2, C. Bruschini1, E. Charbon1

1 Ecole polytechnique fédérale de Lausanne (EPFL), Advanced Quantum Architecture lab, Neuchatel, Neuchâtel, Switzerland
2 ETH Zurich, Institute for Particle Physics and Astrophysics, Zurich, Zürich, Switzerland

Abstract

Precise detection of elementary particles such as neutrinos, gammas, or electrons in an unsegmented scintillating volume requires three-dimensional tracking with sub-nanosecond timing resolution [1], [2]. However, conventional detectors based on analog silicon photomultipliers are inherently constrained by trade-offs between spatial resolution and scalability, making them less suitable for large-scale implementations [3]. To overcome these limitations, CMOS single-photon avalanche diode (SPAD)-based detectors have emerged as a promising alternative for high-resolution particle detection [4], [5]. Here, we propose a dedicated large-format SPAD array sensor fabricated in 110 nm CMOS image sensor (CIS) technology, targeting both high timing precision and scalability. The sensor incorporates a high photon-detection-efficiency SPAD pixel architecture that triggers time-to-digital converters (TDCs) in an event-driven manner with a resolution of 200 ps to detect sparse photons generated by probabilistic events such as particle interactions. All TDCs are synchronized with a global reference clock distributed through an on-chip phase-locked loop, ensuring precise timing alignment across the entire sensor array. Furthermore, a tunable clock shifting feature is implemented to compensate for clock skew in multiple-chip operation. As a result, this chip serves as a fundamental building block for a scalable, multi-chip tiled detector system in which all timing information is globally synchronized, enabling future large-scale, high-resolution particle tracking applications.

AcknowledgmentThis work was supported by the SNSF grant PCEFP2 203261, Switzerland.
References
[1] D. Sgalaberna, The Super Fine-Grained Detector (SuperFGD) for the T2K neutrino oscillation experiment, Detector Seminar at CERN, December 13 (2024). https://indico.cern.ch/event/1484063.
[2] T. Dieminger et al., An ultrafast plenoptic-camera system for high-resolution 3D particle tracking in unsegmented scintillators, Nature Comm. (2026). DOI: 10.1038/s41467-026-70918-x
[3] D. Douqa et al., The SuperFGD for the T2K near detector upgrade, J. Phys. Conf. Ser. 1690, 012070 (2020). DOI: 10.1088/1742-6596/1690/1/012070
[4] M. Franks et al., Demonstration of particle tracking with scintillating fibres read out by a SPAD array sensor and application as a neutrino active target, Eur. Phys. J. C 84, 202 (2024). DOI: 10.1140/epjc/s10052-024-12509-y
[5] K. Kaneyasu et al., PlatonSPAD: a novel SPAD sensor for large-scale high-resolution particle detectors. In Proc. International Image Sensor Workshop (IISW), 1–4 (2025). DOI: 10.60928/486s-zwmd
Keywords: SAPD, Particle Detector, CMOS
10:15 NSS-21-06

Study of neutron irradiated CMOS SPADs for RICH detector applications (#2502)

R. Dolenec1, 2, H.K. Yildirim3, G.V. Tran3, A.G.P. Domenech3, B.C. Efe3, W.Y. Ha3, U. Karaca3, P. Singh3, G.G. Taylor3, S. Korpar4, 1, P. Križan1, 2, R. Pestotnik1, A. Seljak1, E. Charbon3, C. Bruschini3

1 Jožef Stefan Institute, Ljubljana, Slovenia
2 University of Ljubljana, Faculty of Mathematics and Physics, Ljubljana, Slovenia
3 École polytechnique fédérale de Lausanne, AQUA Laboratory, Neuchâtel, Switzerland
4 University of Maribor, Faculty of Chemistry and Chemical Engineering, Maribor, Slovenia

Abstract

Single-photon avalanche diodes (SPAD) produced in CMOS technologies are increasingly being considered as photodetector candidates for future Ring imaging Cherenkov (RICH) detectors. CMOS SPAD based sensors with integrated electronics can be designed and optimized specifically for RICH detector applications, making it easier to achieve the high photon detection efficiency, excellent single photon timing resolution and hardness to neutron radiation as required in the planned high energy physics experiments. To help guide the design of first digital SiPM targeting RICH detector applications being developed in the spadRICH project, existing single SPADs as well as a 144x32 SPAD array were studied in terms of their operation after neutron irradiation. Dark count rates were measured for neutron irradiation as high as 1012 1-MeV neutron equivalent/cm2. Thermal annealing and operation at temperatures down to liquid nitrogen were explored. In terms of cryogenic operation, afterpulsing probability and behavior of the photon detection efficiency were also studied. Simulations were used to assess the possible performance of microlenses specifically for the highly collimated Cherenkov photon light as expected in the upgraded LHCb RICH detector.

AcknowledgmentThis project has received funding from the Slovenian Research and Innovation Agency (project J1-50009) and the Swiss National Science Foundation (project No 200021E 218853).
References
[1] D. Consuegra Rodríguez et al., Characterization of neutron-irradiated SiPMs down to liquid nitrogen temperature, Eur. Phys. J. C (2024) 84:970.
[2] A. Muntean et al., Blumino: The First Fully Integrated Analog SiPM With On-Chip Time Conversion, IEEE Trans. Radiat. Plasma Med. Sci, 5(5) 671-678 (2020).
[3] F. Gramuglia et al., Engineering Breakdown Probability Profile for PDP and DCR Optimization in a SPAD Fabricated in a Standard 55 nm BCD Process, IEEE J. Sel. Top. Quantum Electron. 28(2) (2022) 3802410.
[4] G.G. Taylor et al., Developing photodetectors for future RICH particle detector applications, Proc. SPIE (2025) 13373. 
[5] R. Dolenec et al., SiPM and CMOS SPAD characterization at liquid nitrogen temperatures, JINST 20 (2025) P06052.
[6] C. Bruschini et al., Challenges and prospects for multi-chip microlens imprints on front-side illuminated SPAD imagers, Opt. Express 31, 21935-21953 (2023).
[7] H.K. Yildirim et al., Room-temperature, 96×96 pixel 3D-stacked InGaAs/InP SPAD sensor with complementary gating for flash LiDAR, Opt. Express. 34(3) (2026) 5064:5078.
[8] M.-Lo. Wu et al., Radiation Hardness Study of Single-Photon Avalanche Diode for Space and High Energy Physics Applications, Sensors. 22(8) (2022) 2919.
[9] F. Liu et al., Doping Engineering for PDP Optimization in SPADs Implemented in 55-nm BCD Process, IEEE J. Sel. Top. Quantum Electron. 30(1) (2024) 3801407.
Keywords: single-photon avalanche diode (SPAD), silicon photomultiplier (SiPM), ring imaging Cherenkov detectors (RICH), radiation hardness, neutron irradiation
10:30 NSS-21-07

Comparative Study of NIEL Effects on Dark Count Rate in 110 nm CMOS SPADs Under Neutron, Proton and Electron Irradiation (#1251)

M. Campajola1, A. Burdyko2, G. Collazuol3, M. Da Rocha Rolo4, G. De Nardo5, 1, F. Di Capua5, D. Falchieri6, F. Fienga5, G. Fiorillo5, 1, T. Floris7, F. Licciulli8, L. Maresca5, 1, M.N. Mazziotta8, L. Pancheri9, R. Preghenella6, L. Ratti7, L. Rignanese6, R. Santoro2, F. Shojaei7, C. Vacchi7

1 INFN, Sezione di Napoli, Napoli, Italy
2 Università degli Studi dell’Insubria and INFN Sezione di Milano, Como, Italy
3 Università degli Studi di Padova and INFN Sezione di Padova, Padova, Italy
4 INFN, Sezione di Torino, Torino, Italy
5 Università degli Sudi di Napoli 'Federico II', Napoli, Italy
6 INFN, Sezione di Bologna, Bologna, Italy
7 Università degli Sudi di Pavia and INFN Sezione di Pavia, Pavia, Italy
8 INFN, Sezione di Bari, Bari, Italy
9 Università di Trento and INFN TIFPA, Trento, Italy

Abstract

Single-photon avalanche diodes (SPADs) fabricated in a 110 nm CMOS technology were irradiated with neutrons, protons, and electrons over a range of fluences up to 1011 1 MeV neutron-equivalent cm-2. The dark count rate (DCR) evolution was systematically characterized as a function of displacement damage dose; online monitoring during neutron and proton irradiation allowed individual scattering events and short-term annealing dynamics to be resolved at the single-pixel level, providing direct insight into defect formation and recovery. Statistical characterization of the DCR distributions reveals that the average DCR alone is insufficient to describe radiation-induced degradation in SPAD arrays: the particle type critically determines both the magnitude and spatial uniformity of damage. These differences reflect distinct defect morphologies - clustered damage for hadrons, isolated point defects for electrons - a key aspect not captured by NIEL scaling alone.

References
[1] E. Charbon, “Single-photon imaging in complementary metal oxide semiconductor processes,” Philos. Trans. Roy. Soc. London A, vol. 372, article no. 20130100, Feb. 2014.
[2] S. Gundacker et al., “The silicon photomultiplier: fundamentals and applications of a modern solid-state photon detector,” Phys. Med. Biol. vol. 65, no. 17, 2020.
[3] C. Virmontois et al., “Similarities Between Proton and Neutron Induced Dark Current Distribution in CMOS Image Sensors,” IEEE Trans. Nucl. Sci., vol. 59, pp. 927–936, 2012.
[4] G. Torilla, A test platform for CMOS SPADs and digital SiPMs in a 110 nm technology, Ph.D. dissertation, Dept. Elect., Comput. Biomed. Eng., Univ. Pavia, Pavia, Italy, 2024.
[5] L. Ratti et al., “Total Ionizing Dose Effects on the Dark Count Rate in 110 nm CMOS SPADs,” to be presented at IEEE NSREC, 2026.
[6] A. Jouni et al., “Proton-Induced Displacement Damages in 2-D and Stacked CMOS SPADs: Study of Dark Count Rate Degradation,” IEEE Trans. Nucl. Sci., vol. 70, no. 4, pp. 515–522, Apr. 2023.
[7] M. Campajola et al., “Proton induced dark count rate degradation in 150-nm CMOS single-photon avalanche diodes,” Nucl. Instrum. Meth. A, vol. 947, 2019.
Keywords: Bulk damage, displacement damage, single-photon avalanche diode (SPAD), dark count rate (DCR)
10:45 NSS-21-08

First developments of NUV-DJ SiPM arrays forcryogenic operation for the LHCb SciFi tracker Upgrade II (#2830)

C.A. Trippl1, F. Acerbi1, E. Curras Rivera2, G. Haefeli2, O. Marti Villareal1, S. Sheng2, A. Gola1

1 Fondazione Bruno Kessler, CRS, Trento, Italy
2 École Polytechnique Fédérale de Lausanne, LPHE, Lausanne, Vaud, Switzerland

Abstract

This work presents the first cryogenic performance evaluation of the novel Near-Ultraviolet Deep-Junction (NUV-DJ) SiPM technology developed by Fondazione Bruno Kessler (FBK). By relocating the high-electric field region deeper within the substrate, the NUV-DJ architecture achieves a state-of-the-art photo-detection efficiency of approximately 70% at 420 nm and a timing resolution of 60 ps FWHM at room temperature with a 4 x 4 mm2 SiPM. We report on a comprehensive dark characterisation of these sensors from 300 K down to 77 K, extracting the activation energy (Ea​) to identify dominant carrier generation mechanisms, and evaluating the stability of correlated noise and gain. These studies serve as a foundation for a new dedicated production run for the LHCb Scintillating Fibre (SciFi) Tracker Upgrade II, in collaboration with EPFL, featuring custom 0.4 mm2 geometries and advanced afterpulsing suppression. The main goal is to assess whether the enhanced blue-green sensitivity of NUV-DJ, which is advantageous for the readout of irradiated blue-emitting scintillating fibres, can be combined with radiation tolerance and stable cryogenic operation at liquid-nitrogen temperature.

References
[1] Marti Villarreal, OA, Acerbi, F, Paternoster, G, Penna, M, Zorzi, N and Gola, A 2026, ‘Novel NUV-sensitive Deep-Junction Silicon Photomultiplier’, manuscript in preparation.
[2] Merzi, S et al. 2023, ‘NUV-HD SiPMs with metal-filled trenches’, Journal of Instrumentation, vol. 18, p. P05040.
[3] LHCb Collaboration 2021, ‘Technical Design Report for the LHCb Upgrade II: Framework TDR’, CERN, LHCB-TDR-023, Geneva: CERN.
[4] Witola, L and LHCb Collaboration 2025, ‘Performance of the LHCb Scintillating Fibre Tracker in Run 3’, Nuclear Instruments and Methods in Physics Research Section A, vol. 1079, p. 170606.
[5] Trippl, C 2024, ‘Development of high-resolution and radiation-tolerant Scintillating Fibre trackers for the LHCb experiment’, PhD Thesis, Lausanne: EPFL.
[6] Haefeli, G et al. 2025, ‘Microlens-enhanced SiPMs for the LHCb SciFi tracker Upgrade II: update and recent results’, Nuclear Instruments and Methods in Physics Research Section A, vol. 1080, p. 170607.
[7] Acerbi, F et al. 2017, ‘Cryogenic Characterization of FBK HD Near-UV Sensitive SiPMs’, IEEE Transactions on Electron Devices, vol. 64, no. 2, pp. 521-526.
Keywords: Silicon photomultipliers (SiPMs), LHCb SciFi, NUV-DJ, cryogenic operation, radiation tolerance


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