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Development of CMOS pixel sensors for tracking and vertexing in high energy physics experiments
CMOS pixel sensors (CPS) represent a novel technological approach to building charged particle detectors. CMOS processes allow to integrate a sensing volume and readout electronics in a single silicon die allowing to build sensors with a small pixel pitch ($\sim 20 \mu m$) and low material budget ($...
Autores principales: | , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2014
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Materias: | |
Acceso en línea: | http://cds.cern.ch/record/1647493 |
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author | Senyukov, Serhiy Baudot, Jerome Besson, Auguste Claus, Giles Cousin, Loic Dulinski, Wojciech Goffe, Mathieu Hippolyte, Boris Maria, Robert Molnar, Levente Sanchez Castro, Xitzel Winter, Marc |
author_facet | Senyukov, Serhiy Baudot, Jerome Besson, Auguste Claus, Giles Cousin, Loic Dulinski, Wojciech Goffe, Mathieu Hippolyte, Boris Maria, Robert Molnar, Levente Sanchez Castro, Xitzel Winter, Marc |
author_sort | Senyukov, Serhiy |
collection | CERN |
description | CMOS pixel sensors (CPS) represent a novel technological approach to building charged particle detectors. CMOS processes allow to integrate a sensing volume and readout electronics in a single silicon die allowing to build sensors with a small pixel pitch ($\sim 20 \mu m$) and low material budget ($\sim 0.2-0.3\% X_0$) per layer. These characteristics make CPS an attractive option for vertexing and tracking systems of high energy physics experiments. Moreover, thanks to the mass production industrial CMOS processes used for the manufacturing of CPS the fabrication construction cost can be significantly reduced in comparison to more standard semiconductor technologies. However, the attainable performance level of the CPS in terms of radiation hardness and readout speed is mostly determined by the fabrication parameters of the CMOS processes available on the market rather than by the CPS intrinsic potential. The permanent evolution of commercial CMOS processes towards smaller feature sizes and high resistivity epitaxial layers leads to the better radiation hardness and allows the implementation of accelerated readout circuits. The TowerJazz $0.18 \mu m$ CMOS process being one of the most relevant examples recently became of interest for several future detector projects. The most imminent of these project is an upgrade of the Inner Tracking System (ITS) of the ALICE detector at LHC. It will be followed by the Micro-Vertex Detector (MVD) of the CBM experiment at FAIR. Other experiments like ILD consider CPS as one of the viable options for flavour tagging and tracking sub-systems. |
id | cern-1647493 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2014 |
record_format | invenio |
spelling | cern-16474932021-12-31T03:07:28Zhttp://cds.cern.ch/record/1647493engSenyukov, SerhiyBaudot, JeromeBesson, AugusteClaus, GilesCousin, LoicDulinski, WojciechGoffe, MathieuHippolyte, BorisMaria, RobertMolnar, LeventeSanchez Castro, XitzelWinter, MarcDevelopment of CMOS pixel sensors for tracking and vertexing in high energy physics experimentsDetectors and Experimental TechniquesCMOS pixel sensors (CPS) represent a novel technological approach to building charged particle detectors. CMOS processes allow to integrate a sensing volume and readout electronics in a single silicon die allowing to build sensors with a small pixel pitch ($\sim 20 \mu m$) and low material budget ($\sim 0.2-0.3\% X_0$) per layer. These characteristics make CPS an attractive option for vertexing and tracking systems of high energy physics experiments. Moreover, thanks to the mass production industrial CMOS processes used for the manufacturing of CPS the fabrication construction cost can be significantly reduced in comparison to more standard semiconductor technologies. However, the attainable performance level of the CPS in terms of radiation hardness and readout speed is mostly determined by the fabrication parameters of the CMOS processes available on the market rather than by the CPS intrinsic potential. The permanent evolution of commercial CMOS processes towards smaller feature sizes and high resistivity epitaxial layers leads to the better radiation hardness and allows the implementation of accelerated readout circuits. The TowerJazz $0.18 \mu m$ CMOS process being one of the most relevant examples recently became of interest for several future detector projects. The most imminent of these project is an upgrade of the Inner Tracking System (ITS) of the ALICE detector at LHC. It will be followed by the Micro-Vertex Detector (MVD) of the CBM experiment at FAIR. Other experiments like ILD consider CPS as one of the viable options for flavour tagging and tracking sub-systems.CMOS pixel sensors (CPS) represent a novel technological approach to building charged particle detectors. CMOS processes allow to integrate a sensing volume and readout electronics in a single silicon die allowing to build sensors with a small pixel pitch ($\sim 20 \mu m$) and low material budget ($\sim 0.2-0.3\% X_0$) per layer. These characteristics make CPS an attractive option for vertexing and tracking systems of high energy physics experiments. Moreover, thanks to the mass production industrial CMOS processes used for the manufacturing of CPS the fabrication construction cost can be significantly reduced in comparison to more standard semiconductor technologies. However, the attainable performance level of the CPS in terms of radiation hardness and readout speed is mostly determined by the fabrication parameters of the CMOS processes available on the market rather than by the CPS intrinsic potential. The permanent evolution of commercial CMOS processes towards smaller feature sizes and high resistivity epitaxial layers leads to the better radiation hardness and allows the implementation of accelerated readout circuits. The TowerJazz $0.18 \mu m$ CMOS process being one of the most relevant examples recently became of interest for several future detector projects. The most imminent of these project is an upgrade of the Inner Tracking System (ITS) of the ALICE detector at LHC. It will be followed by the Micro-Vertex Detector (MVD) of the CBM experiment at FAIR. Other experiments like ILD consider CPS as one of the viable options for flavour tagging and tracking sub-systems.arXiv:1402.2172oai:cds.cern.ch:16474932014-02-10 |
spellingShingle | Detectors and Experimental Techniques Senyukov, Serhiy Baudot, Jerome Besson, Auguste Claus, Giles Cousin, Loic Dulinski, Wojciech Goffe, Mathieu Hippolyte, Boris Maria, Robert Molnar, Levente Sanchez Castro, Xitzel Winter, Marc Development of CMOS pixel sensors for tracking and vertexing in high energy physics experiments |
title | Development of CMOS pixel sensors for tracking and vertexing in high energy physics experiments |
title_full | Development of CMOS pixel sensors for tracking and vertexing in high energy physics experiments |
title_fullStr | Development of CMOS pixel sensors for tracking and vertexing in high energy physics experiments |
title_full_unstemmed | Development of CMOS pixel sensors for tracking and vertexing in high energy physics experiments |
title_short | Development of CMOS pixel sensors for tracking and vertexing in high energy physics experiments |
title_sort | development of cmos pixel sensors for tracking and vertexing in high energy physics experiments |
topic | Detectors and Experimental Techniques |
url | http://cds.cern.ch/record/1647493 |
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