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Radiation hardness of MALTA2 monolithic CMOS imaging sensors on Czochralski substrates
/ van Rijnbach, Milou (CERN ; Oslo U.) ; Berlea, Dumitru Vlad (DESY, Zeuthen) ; Dao, Valerio (CERN) ; Gaži, Martin (Oxford U.) ; Allport, Phil (Birmingham U.) ; Asensi Tortajada, Ignacio (CERN) ; Behera, Prafulla (Indian Inst. Tech., Madras) ; Bortoletto, Daniela (Oxford U.) ; Buttar, Craig (Glasgow U.) ; Dachs, Florian (CERN) et al.
MALTA2 is the latest full-scale prototype of the MALTA family of Depleted Monolithic Active Pixel Sensors (DMAPS) produced in Tower Semiconductor 180 nm CMOS technology. In order to comply with the requirements of High Energy Physics (HEP) experiments, various process modifications and front-end changes have been implemented to achieve low power consumption, reduce Random Telegraph Signal (RTS) noise, and optimise the charge collection geometry. [...]
arXiv:2308.13231.-
2024-03-10 - 16 p.
- Published in : Eur. Phys. J. C 84 (2024) 251
Fulltext: document - PDF; 2308.13231 - PDF;
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2.
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Performance of the MALTA Telescope
/ van Rijnbach, Milou (CERN ; Oslo U.) ; Gustavino, Giuliano (CERN) ; Allport, Phil (Birmingham U.) ; Asensi, Igancio (CERN) ; Berlea, Dumitru Vlad (DESY, Zeuthen) ; Bortoletto, Daniela (Oxford U.) ; Buttar, Craig (Glasgow U.) ; Charbon, Edoardo (Ecole Polytechnique, Lausanne) ; Dachs, Florian (CERN) ; Dao, Valerio (CERN) et al.
MALTA is part of the Depleted Monolithic Active Pixel sensors designed in Tower 180nm CMOS imaging technology. A custom telescope with six MALTA planes has been developed for test beam campaigns at SPS, CERN, with the ability to host several devices under test. [...]
arXiv:2304.01104.-
2023-07-08 - 22 p.
- Published in : Eur. Phys. J. C 83 (2023) 581
Fulltext: 2304.01104 - PDF; document - PDF;
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3.
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Timing performance of radiation hard MALTA monolithic Pixel sensors
/ Gustavino, G. (CERN) ; Allport, P. (Birmingham U.) ; Asensi, I. (CERN) ; Berlea, D.V. (DESY, Zeuthen) ; Bortoletto, D. (U. Oxford (main)) ; Buttar, C. (Glasgow U.) ; Dachs, F. (CERN) ; Dao, V. (CERN) ; Denizli, H. (Abant Izzet Baysal U.) ; Dobrijevic, D. (CERN ; U. Zagreb (main)) et al.
The MALTA family of Depleted Monolithic Active Pixel Sensor (DMAPS) produced in Tower 180 nm CMOS technology targets radiation hard applications for the HL-LHC and beyond. Several process modifications and front-end improvements have resulted in radiation hardness up to $2 \times 10^{15}~1~\text{MeV}~\text{n}_{eq}/\text{cm}^2$ and time resolution below 2 ns, with uniform charge collection efficiency across the Pixel of size $36.4 \times 36.4~\mu\text{m}^2$ with a $3~\mu\text{m}^2$ electrode size. [...]
arXiv:2209.14676.-
2023-03-15 - 10 p.
- Published in : JINST
Fulltext: 2209.14676 - PDF; document - PDF;
In : 23rd International Workshop for Radiation Imaging Detectors, Riva Del Garda, It, 26 - 30 Jun 2022, pp.C03011
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4.
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Development of the radiation-hard MALTA CMOS sensor for tracking applications
/ Gustavino, G (CERN) ; Allport, P (Birmingham U.) ; Asensi Tortajada, I (CERN) ; Behera, P (Indian Inst. Tech., Madras) ; Berlea, D V (DESY, Zeuthen) ; Bortoletto, D (Oxford U.) ; Buttar, C (Glasgow U.) ; Dachs, F (CERN) ; Dao, V (CERN) ; Dash, G (Indian Inst. Tech., Madras) et al.
The MALTA family of Depleted Monolithic Active Pixel Sensors (DMAPS) is produced using Tower 180 nm CMOS technology, specifically targeting radiation-hard applications in the HL-LHC and beyond. Several process modifications have resulted in radiation hardness up to ${3 \times 10^{15}~1 ~\text{MeV}~\text{n}_{\text{eq}} /\text{cm}^2}$ and time resolution below 2 ns, with uniform charge collection efficiency across the chip formed of $512 \times 224$ pixels with a size of $36.4 \times 36.4~\mu\text{m}^2$. [...]
2024 - 7 p.
- Published in : PoS VERTEX2023 (2024) 048
Fulltext: PDF;
In : 32nd International Workshop on Vertex Detectors (VERTEX 2023), Sestri Levante, Italy, 16 - 20 Oct 2023, pp.048
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5.
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Depletion depth studies with the MALTA2 sensor, a depleted monolithic active pixel sensor
/ Berlea, D V (DESY, Zeuthen ; Humboldt U., Berlin) ; Allport, P (Birmingham U.) ; Asensi Tortajada, I (CERN) ; Behera, P (Indian Inst. Tech., Madras) ; Bortoletto, D (Oxford U.) ; Buttar, C (Glasgow U.) ; Dachs, F (CERN) ; Dao, V (CERN) ; Dash, G (Indian Inst. Tech., Madras) ; Dobrijevic, D (CERN ; Boskovic Inst., Zagreb) et al.
MALTA2 is a depleted monolithic active pixel sensor (DMAPS) developed in the Tower 180 nm CMOS imaging process. Monolithic CMOS sensors offer advantages over current hybrid imaging sensors both in terms of increased tracking performance due to lower material budget but also in terms of ease of integration and construction costs due to the monolithic design. [...]
2024 - 6 p.
- Published in : Nucl. Instrum. Methods Phys. Res., A 1063 (2024) 169262
Fulltext: PDF;
In : 13th International "Hiroshima" Symposium on the Development and Application of Semiconductor Tracking Detectors, Vancouver, Canada, 3 - 8 Dec 2023, pp.169262
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MALTA-Cz: A radiation hard full-size monolithic CMOS sensor with small electrodes on high-resistivity Czochralski substrate
/ Pernegger, H. (CERN) ; Allport, P. (Birmingham U.) ; Berlea, D.V. (DESY, Zeuthen) ; Birman, A. (Technion) ; Bortoletto, D. (Oxford U.) ; Buttar, C. (Glasgow U.) ; Charbon, E. (LPHE, Lausanne) ; Dachs, F. (CERN) ; Dao, V. (CERN) ; Denizli, H. (Abant Izzet Baysal U.) et al.
Depleted Monolithic Active Pixel Sensor (DMAPS) sensors developed in the Tower Semiconductor 180 nm CMOS imaging process have been designed in the context of the ATLAS ITk upgrade Phase-II at the HL-LHC and for future collider experiments. The "MALTA-Czochralski (MALTA-Cz)" full size DMAPS sensor has been developed with the goal to demonstrate a radiation hard, thin CMOS sensor with high granularity, high hit-rate capability, fast response time and superior radiation tolerance. [...]
arXiv:2301.03912.-
2023-09-13 - 24 p.
- Published in : JINST 18 (2023) P09018
Fulltext: 2301.03912 - PDF; Publication - PDF;
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Data preservation in high energy physics
/ DPHEP Collaboration
Data preservation is a mandatory specification for any present and future experimental facility and it is a cost-effective way of doing fundamental research by exploiting unique data sets in the light of the continuously increasing theoretical understanding. This document summarizes the status of data preservation in high energy physics. [...]
arXiv:2302.03583; DPHEP-2023-01.-
2023-09-08 - 41 p.
- Published in : Eur. Phys. J. C 83 (2023) 795
Fulltext: FERMILAB-FN-1223-CSAID-PPD - PDF; 2302.03583 - PDF; Fulltext from Publisher: PDF; External link: Fermilab Library Server
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Higgs physics at the CLIC electron–positron linear collider
/ Abramowicz, H. (Tel Aviv U.) ; Abusleme, A. (Chile U., Catolica) ; Afanaciev, K. (Belarus State U.) ; Tehrani, N.Alipour (CERN) ; Balázs, C. (Monash U.) ; Benhammou, Y. (Tel Aviv U.) ; Benoit, M. (Geneva U.) ; Bilki, B. (Argonne) ; Blaising, J.J. (Annecy, LAPP) ; Boland, M.J. (Melbourne U.) et al.
The Compact Linear Collider (CLIC) is an option for a future e+e- collider operating at centre-of-mass energies up to 3 TeV, providing sensitivity to a wide range of new physics phenomena and precision physics measurements at the energy frontier. This paper is the first comprehensive presentation of the Higgs physics reach of CLIC operating at three energy stages: sqrt(s) = 350 GeV, 1.4 TeV and 3 TeV. [...]
arXiv:1608.07538; CLICDP-PUB-2016-001.-
Geneva : CERN, 2017-07-17 - 40 p.
- Published in : Eur. Phys. J. C 77 (2017) 475
Accepted version for publication: PDF; Article from SCOAP3: PDF; Fulltext: PDF;
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Jet-like correlations with respect to K$^{0}_{\rm S}$ and $\Lambda$ ($\bar{\Lambda}$) in pp and Pb-Pb collisions at $\mathbf{\it\sqrt{s_\mathrm{NN}}}$ = 5.02 TeV
/ ALICE Collaboration
Two-particle correlations with ${\rm K}^{0}_{\rm{S}}$, $\Lambda$/$\overline{\Lambda}$, and charged hadrons as trigger particles in the transverse momentum range $8 < p_\mathrm{T,trig}<16$ GeV/$c$, and associated charged particles within $1 < p_\mathrm{T,assoc}<8$ GeV/$c$, are studied at mid-rapidity in pp and central Pb-Pb collisions at a centre-of-mass energy per nucleon-nucleon collision $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV with the ALICE detector at the LHC. After subtracting the contributions of the flow background, the per-trigger yields are extracted on both the near and away sides, and the ratio in Pb-Pb collisions with respect to pp collisions ($I_{\mathrm {AA}}$) is computed. [...]
arXiv:2211.01197; CERN-EP-2022-225.-
Geneva : CERN, 2023-06-12 - 27 p.
- Published in : Eur. Phys. J. C 83 (2023) 497
Draft (restricted): PDF; Fulltext: document - PDF; 2211.01197 - PDF;
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