High-voltage pixel detectors in commercial CMOS technologies for ATLAS, CLIC and Mu3e experiments

Perić, I.; Fischer, P.; Kreidl, Christian; Nguyen, Hong Hanh; Augustin, Heiko; Berger, N.; Kiehn, M.; Perrevoort, A.; Schöning, A.; Wiedner, D.; Feigl, S.; Heim, T.; Meng, L.; Münstermann, D.; Benoit, M.; Dannheim, D.; Bompard, F.; Breugnon, P.; Clémens, J. C.; Fougeron, D.; Liu, J.; Pangaud, P.; Rozanov, A.; Barbero, M.; Backhaus, M.; Huegging, F.; Krüger, Hans; Lütticke, F.; Mariñas, C.; Obermann, T.; Garcia-Sciveres, M.; Schwenker, B.; Dierlamm, A.; Rosa, A. La; Miucci, A.

doi:10.1016/j.nima.2013.05.006

Cited by 60 publications

(43 citation statements)

References 9 publications

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“…State-of-the-art silicon pixel detectors can reach very good position resolutions (∼ 3 µm), with a thickness of 50 µm Si + 25 µm Kapton per layer [21], corresponding to ∼ 10 −3 radiation lengths per layer. On the other hand, the complete drift-chamber spectrometers of MEG or MEG-II amount to less than 3 × 10 −3 radiation lengths over the whole track length within the tracking volume, nonetheless material effects gave a significant contribution in MEG and will almost be dominant in MEG-II.…”

Section: Positron Energymentioning

confidence: 99%

The quest for $$\mu \rightarrow e \gamma $$ μ → e γ and its experimental limiting factors at future high intensity muon beams

et al. 2018

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The search for the lepton flavor violating decay μ + → e + γ will reach an unprecedented level of sensitivity within the next five years thanks to the MEG-II experiment. This experiment will take data at the Paul Scherrer Institut where continuous muon beams are delivered at a rate of about 10 8 muons per second. On the same time scale, accelerator upgrades are expected in various facilities, making it feasible to have continuous beams with an intensity of 10 9 or even 10 10 muons per second. We investigate the experimental limiting factors that will define the ultimate performances, and hence the sensitivity, in the search for μ + → e + γ with a continuous beam at these extremely high rates. We then consider some conceptual detector designs and evaluate the corresponding sensitivity as a function of the beam intensity.

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Section: Positron Energymentioning

confidence: 99%

The quest for $$\mu \rightarrow e \gamma $$ μ → e γ and its experimental limiting factors at future high intensity muon beams

et al. 2018

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“…Hardware assemblies with planar silicon and active HV-CMOS [2] sensors have been tested in the lab and during test-beam campaigns at DESY and CERN using the EUDET/AIDA telescope [3] containing 6 planes of Mimosa26 pixel sensors. Figure 1a shows a picture of the testbeam setup at DESY.…”

Section: Randd On Sensor and Readoutmentioning

confidence: 99%

CLIC vertex detector R&D

Tehrani

2016

Nuclear Instruments and Methods in Physics Research Section A:

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A vertex-detector concept is under development for the proposed multi-TeV linear e + eCompact Linear Collider (CLIC). To perform precision physics measurements in a challenging environment, the CLIC vertex detector pushes the technological requirements to the limits. This paper reviews the requirements for the CLIC vertex detector and gives an overview of recent R&D achievements in the domains of sensor, readout, powering and cooling. To perform precision physics measurements in a challenging environment, the CLIC vertex detector pushes the technological requirements to the limits. This paper reviews the requirements for the CLIC vertex detector and gives an overview of recent R&D achievements in the domains of sensor, readout, powering and cooling.

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“…It has 25 µm pixel size, supports power-pulsing and is implemented in 65 nm technology. As a first step, this chip work in progress was glued to a CCPDv3 HV-CMOS sensor [9], creating a capacitive coupling between the two. The assembly was tested at the CERN PS test beam in August 2014 and successfully took data, showing a correlation between recorded hit position and reconstructed track position.…”

Section: Thin Sensor Assembliesmentioning

confidence: 99%

R&D for the Vertexing at CLIC

Redford¹

2015

Proceedings of the 23rd International Workshop on Vertex Detectors — PoS(Vertex2014)

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The Compact Linear Collider is a candidate to be the next high-energy particle physics collider. Using a novel acceleration technique, electrons and positrons would be brought into collision with a centre-of-mass energy of up to 3 TeV. Despite challenging levels of beam-induced background, this would provide a relatively clean environment in which to perform precision physics measurements. The vertex detector would be crucial in achieving this, and would need to provide accurate particle tracking information to facilitate secondary vertex reconstruction and jet flavour-tagging. With this goal in mind, current technological limits are being stretched to design a low occupancy, low mass and low-power dissipation vertex detector for CLIC. A concept comprising thin hybrid pixel detectors coupled to high-performance readout ASICs, power-pulsing and air-flow cooling is under development. In this paper, the CLIC vertex detector requirements are reviewed and the current status of R&D on sensors, readout, powering, cooling and supports is presented.

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High-voltage pixel detectors in commercial CMOS technologies for ATLAS, CLIC and Mu3e experiments

Cited by 60 publications

References 9 publications

The quest for $$\mu \rightarrow e \gamma $$ μ → e γ and its experimental limiting factors at future high intensity muon beams

The quest for $$\mu \rightarrow e \gamma $$ μ → e γ and its experimental limiting factors at future high intensity muon beams

CLIC vertex detector R&D

R&D for the Vertexing at CLIC

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