pixel sensors
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2022 ◽  
Vol 17 (01) ◽  
pp. C01024
Author(s):  
W. Zhou ◽  
X. Niu ◽  
W. Han ◽  
X. Li ◽  
Q. Wang ◽  
...  

Abstract In this paper, a 5-Gbps serial link transmitter has been designed for monolithic active pixel sensor. The serial link is designed in a commercial 130-nm CMOS technology with a power supply of 1.2 V. The transmitter consists of a 16b/20b encoder, a three-stage 20:1 serializer core, the CML driver with pre-emphasis function, and a high-speed receiver to deal with the external clock. The root mean square jitter of this serial link transmitter is 2.2 ps, indicating a bit error rate of 1 × 10−14. This paper will discuss the design and performance of this serial link transmitter.


Instruments ◽  
2021 ◽  
Vol 5 (4) ◽  
pp. 39
Author(s):  
Lucio Anderlini ◽  
Marco Bellini ◽  
Chiara Corsi ◽  
Stefano Lagomarsino ◽  
Chiara Lucarelli ◽  
...  

Tracking detectors at future high luminosity hadron colliders are expected to be able to stand unprecedented levels of radiation as well as to efficiently reconstruct a huge number of tracks and primary vertices. To face the challenges posed by the radiation damage, new extremely radiation hard materials and sensor designs will be needed, while the track and vertex reconstruction problem can be significantly mitigated by the introduction of detectors with excellent timing capabilities. Indeed, the time coordinate provides extremely powerful information to disentangle overlapping tracks and hits in the harsh hadronic collision environment. Diamond 3D pixel sensors optimised for timing applications provide an appealing solution to the above problems as the 3D geometry enhances the already outstanding radiation hardness and allows to exploit the excellent timing properties of diamond. We report here the first full timing characterisation of 3D diamond sensors fabricated by electrode laser graphitisation in Florence. Results from a 270MeV pion beam test of a first prototype and from tests with a β source on a recently fabricated 55×55μm2 pitch sensor are discussed. First results on sensor simulation are also presented.


2021 ◽  
Vol 24 (9) ◽  
pp. 5-11
Author(s):  
Giuseppe Iacobucci ◽  
Lorenzo Paolozzi ◽  
Pierpaolo Valerio

2021 ◽  
Vol 16 (12) ◽  
pp. P12030
Author(s):  
F. Alcalde Bessia ◽  
J. Lipovetzky ◽  
I. Perić

Abstract This work presents the design of BUSARD, an application specific integrated circuit (ASIC) for the detection of ionizing particles. The ASIC is a monolithic active pixel sensor which has been fabricated in a High-Voltage Silicon-On-Insulator (HV-SOI) process that allows the fabrication of a buried N+ diffusion below the Buried OXide (BOX) as a standard processing step. The first version of the chip, BUSARD-A, takes advantage of this buried diffusion as an ionizing particle sensor. It includes a small array of 13×13 pixels, with a pitch of 80 μm, and each pixel has one buried diffusion with a charge amplifier, discriminator with offset tuning and digital processing. The detector has several operation modes including particle counting and Time-over-Threshold (ToT). An initial X-ray characterization of the detector was carried out, obtaining several pulse height and ToT spectra, which then were used to perform the energy calibration of the device. The Molybdenum 𝐊α emission was measured with a standard deviation of 127 e- of ENC by using the analog pulse output, and with 276 e- of ENC by using the ToT digital output. The resolution in ToT mode is dominated by the pixel-to-pixel variation.


2021 ◽  
Vol 16 (12) ◽  
pp. C12029
Author(s):  
A. Mulliri ◽  
M. Arba ◽  
P. Bhattacharya ◽  
E. Casula ◽  
C. Cicalò ◽  
...  

Abstract The aim of the pixel chamber project is to develop the first “solid-state bubble chamber” for high precision measurement of charm and beauty. In this paper we will describe the idea for the first silicon active target conceived as an ultra-high granular stack of hundreds of very thin monolithic active pixel sensors (MAPS), which provides continuous, high-resolution 3D tracking of all of the particles produced in proton-silicon interactions occurring inside the detector volume, including open charm and beauty. We will also discuss the high-precision tracking and vertexing performances, showing that the vertex resolution can be up to one order of magnitude better than state-of-the-art detectors like the LHCb one.


2021 ◽  
Vol 9 ◽  
Author(s):  
Coralie Neubüser ◽  
T. Corradino ◽  
G-F. Dalla Betta ◽  
L. De Cilladi ◽  
L. Pancheri

Fully depleted monolithic active pixel sensors (FD-MAPSs) represent a state-of-the-art detector technology and profit from a low material budget and cost for high-energy physics experiments and other fields of research like medical imaging and astro-particle physics. Compared to the MAPS currently in use, fully depleted pixel sensors have the advantage of charge collection by drift, which enables a fast and uniform response overall to the pixel matrix. The functionality of these devices has been shown in previous proof-of-concept productions. In this article, we describe the optimization of the test pixel designs that will be implemented in the first engineering run of the demonstrator chip of the ARCADIA project. These optimization procedures include radiation damage models that have been employed in Technology Computer Aided Design simulations to predict the sensors’ behavior in different working environments.


Universe ◽  
2021 ◽  
Vol 7 (11) ◽  
pp. 420
Author(s):  
Cristina Martin Perez ◽  
Luigi Vigani

Mu3e is a dedicated experiment designed to find or exclude the charged lepton flavor violating μ→ eee decay at branching fractions above 10−16. The search is pursued in two operational phases: Phase I uses an existing beamline at the Paul Scherrer Institute (PSI), targeting a single event sensitivity of 2·10−15, while the ultimate sensitivity is reached in Phase II using a high intensity muon beamline under study at PSI. As the μ→ eee decay is heavily suppressed in the Standard Model of particle physics, the observation of such a signal would be an unambiguous indication of the existence of new physics. Achieving the desired sensitivity requires a high rate of muons (108 stopped muons per second) along with a detector with large kinematic acceptance and efficiency, able to reconstruct the low momentum of the decay electrons and positrons. To achieve this goal, the Mu3e experiment is mounted with an ultra thin tracking detector based on monolithic active pixel sensors for excellent momentum and vertex resolution, combined with scintillating fibers and tiles for precise timing measurements.


2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Ashutosh V. Kotwal

AbstractThe reconstruction of charged particle trajectories at the Large Hadron Collider and future colliders relies on energy depositions in sensors placed at distances ranging from a centimeter to a meter from the colliding beams. We propose a method of detecting charged particles that decay invisibly after traversing a short distance of about 25 cm inside the experimental apparatus. One of the decay products may constitute the dark matter known to be 84% of all matter at galactic and cosmological distance scales. Our method uses graph computing to cluster spacepoints recorded by two-dimensional silicon pixel sensors into mathematically-defined patterns. The algorithm may be implemented on silicon-based integrated circuits using field-programmable gate array technology to augment or replace traditional computing platforms.


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