silicon sensor
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2021 ◽  
Vol 16 (11) ◽  
pp. P11028
Author(s):  
W. Adam ◽  
T. Bergauer ◽  
D. Blöch ◽  
M. Dragicevic ◽  
R. Frühwirth ◽  
...  

Abstract During the operation of the CMS experiment at the High-Luminosity LHC the silicon sensors of the Phase-2 Outer Tracker will be exposed to radiation levels that could potentially deteriorate their performance. Previous studies had determined that planar float zone silicon with n-doped strips on a p-doped substrate was preferred over p-doped strips on an n-doped substrate. The last step in evaluating the optimal design for the mass production of about 200 m2 of silicon sensors was to compare sensors of baseline thickness (about 300 μm) to thinned sensors (about 240 μm), which promised several benefits at high radiation levels because of the higher electric fields at the same bias voltage. This study provides a direct comparison of these two thicknesses in terms of sensor characteristics as well as charge collection and hit efficiency for fluences up to 1.5 × 1015 neq/cm2. The measurement results demonstrate that sensors with about 300 μm thickness will ensure excellent tracking performance even at the highest considered fluence levels expected for the Phase-2 Outer Tracker.


2021 ◽  
Vol 16 (11) ◽  
pp. P11020
Author(s):  
C. Leroy ◽  
C. Papadatos ◽  
M. Usman ◽  
M. Boussa

Abstract The phenomenon of charge sharing in pixelated particle detectors and its relationship to a variety of physical parameters is investigated using a Timepix3 (TPX3) detector with a 500 μm thick silicon sensor. A probing technique is used with H, Li, and C ion beams produced at the Tandem Van de Graaff (VdG) accelerator at the University of Montreal (UdeM), as well as alpha particles from an 241Am radioactive source, to determine a direct relationship between particle depth and cluster size. Additionally, the primacy of a particle's energy on the determination of its corresponding cluster's size is confirmed.


2021 ◽  
Vol 16 (10) ◽  
pp. P10034
Author(s):  
S. Fernandez-Perez ◽  
V. Boccone ◽  
C. Broennimann ◽  
C. Disch ◽  
L. Piazza ◽  
...  

2021 ◽  
Vol 16 (09) ◽  
pp. P09028
Author(s):  
D. Brundu ◽  
A. Cardini ◽  
G.M. Cossu ◽  
G.-F. Dalla Betta ◽  
M. Garau ◽  
...  
Keyword(s):  

2021 ◽  
Vol 16 (08) ◽  
pp. P08009
Author(s):  
K. Heijhoff ◽  
K. Akiba ◽  
R. Bates ◽  
M. van Beuzekom ◽  
P. Bosch ◽  
...  
Keyword(s):  

Molecules ◽  
2021 ◽  
Vol 26 (12) ◽  
pp. 3734
Author(s):  
Yuri D. Ivanov ◽  
Tatyana S. Romanova ◽  
Kristina A. Malsagova ◽  
Tatyana O. Pleshakova ◽  
Alexander I. Archakov

The review covers some research conducted in the field of medical and biomedical application of devices based on silicon sensor elements (Si-NW-sensors). The use of Si-NW-sensors is one of the key methods used in a whole range of healthcare fields. Their biomedical use is among the most important ones as they offer opportunities for early diagnosis of oncological pathologies, for monitoring the prescribed therapy and for improving the people’s quality of life.


2021 ◽  
Vol 16 (01) ◽  
pp. P01022-P01022
Author(s):  
P. Smolyanskiy ◽  
P. Azzarello ◽  
B. Bergmann ◽  
P. Burian ◽  
P. Broulím ◽  
...  
Keyword(s):  

2021 ◽  
Vol 253 ◽  
pp. 11012
Author(s):  
H. Imam

The particle flux increase (pile-up) at the HL-LHC with luminosities of L = 7.5 × 1034 cm−2 s−1 will have a significant impact on the reconstruction of the ATLAS detector and on the performance of the trigger. The forward region and the end-cap where the internal tracker has poorer longitudinal track impact parameter resolution, and where the liquid argon calorimeter has coarser granularity, will be significantly affected. A High Granularity Time Detector (HGTD) is proposed to be installed in front of the LAr end-cap calorimeter for the mitigation of the pileup effect, as well as measurement of luminosity. It will have coverage of 2.4 to 4.0 from the pseudo-rapidity range. Two dual-sided silicon sensor layers will provide accurate timing information for minimum-ionizing particles with a resolution better than 30 ps per track (before irradiation), for assigning each particle to the correct vertex. The readout cells are about 1.3 mm × 1.3 mm in size, which leads to a high granular detector with 3 million channels. The technology of low-gain avalanche detectors (LGAD) with sufficient gain was chosen to achieve the required high signal-to-noise ratio. A dedicated ASIC is under development with some prototypes already submitted and evaluated. The requirements and general specifications of the HGTD will be maintained and discussed. R&D campaigns on the LGAD are carried out to study the sensors, the related ASICs and the radiation hardness. Both laboratory and test beam results will be presented.


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