Cargando…

Thin n-in-p pixel sensors and the SLID-ICV vertical integration technology for the ATLAS upgrade at the HL-LHC

The R&D activity presented is focused on the development of new modules for the upgrade of the ATLAS pixel system at the High Luminosity LHC (HL-LHC). The performance after irradiation of n-in-p pixel sensors of different active thicknesses is studied, together with an investigation of a novel i...

Descripción completa

Detalles Bibliográficos
Autores principales: Macchiolo,A, Andricek,L, Ellenburg,M, Nisius,R, Richter,R.H, Terzo,S, Weigell,P
Formato: info:eu-repo/semantics/article
Lenguaje:eng
Publicado: Nucl. Instrum. Methods Phys. Res., A 2013
Materias:
Acceso en línea:http://cds.cern.ch/record/1693128
_version_ 1780935901457678336
author Macchiolo,A
Andricek,L
Ellenburg,M
Nisius,R
Richter,R.H
Terzo,S
Weigell,P
author_facet Macchiolo,A
Andricek,L
Ellenburg,M
Nisius,R
Richter,R.H
Terzo,S
Weigell,P
author_sort Macchiolo,A
collection CERN
description The R&D activity presented is focused on the development of new modules for the upgrade of the ATLAS pixel system at the High Luminosity LHC (HL-LHC). The performance after irradiation of n-in-p pixel sensors of different active thicknesses is studied, together with an investigation of a novel interconnection technique offered by the Fraunhofer Institute EMFT in Munich, the Solid-Liquid-InterDiffusion (SLID), which is an alternative to the standard solder bump-bonding. The pixel modules are based on thin n-in-p sensors, with an active thickness of 75 m or 150 m, produced at the MPI Semiconductor Laboratory (MPI HLL) and on 100 m thick sensors with active edges, fabricated at VTT, Finland. Hit efficiencies are derived from beam test data for thin devices irradiated up to a fluence of 4 1015neq=cm2. For the active edge devices, the charge collection properties of the edge pixels before irradiation is discussed in detail, with respect to the inner ones, using measurements with radioactive sources. Beyond the active edge sensors, an additional ingredient needed to design four side buttable modules is the possibility of moving the wire bonding area from the chip surface facing the sensor to the backside, avoiding the implementation of the cantilever extruding beyond the sensor area. The feasibility of this process is under investigation with the FE-I3 SLID modules, where Inter Chip Vias are etched, employing an EMFT technology, with a cross section of 3 mx10 m, at the positions of the original wire bonding pads.
format info:eu-repo/semantics/article
id cern-1693128
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2013
publisher Nucl. Instrum. Methods Phys. Res., A
record_format invenio
spelling cern-16931282021-08-10T13:09:45Z http://cds.cern.ch/record/1693128 eng Macchiolo,A Andricek,L Ellenburg,M Nisius,R Richter,R.H Terzo,S Weigell,P Thin n-in-p pixel sensors and the SLID-ICV vertical integration technology for the ATLAS upgrade at the HL-LHC Detectors and Experimental Techniques 9: Advanced infrastructures for detector R&D 9.3: Precision Pixel Detectors The R&D activity presented is focused on the development of new modules for the upgrade of the ATLAS pixel system at the High Luminosity LHC (HL-LHC). The performance after irradiation of n-in-p pixel sensors of different active thicknesses is studied, together with an investigation of a novel interconnection technique offered by the Fraunhofer Institute EMFT in Munich, the Solid-Liquid-InterDiffusion (SLID), which is an alternative to the standard solder bump-bonding. The pixel modules are based on thin n-in-p sensors, with an active thickness of 75 m or 150 m, produced at the MPI Semiconductor Laboratory (MPI HLL) and on 100 m thick sensors with active edges, fabricated at VTT, Finland. Hit efficiencies are derived from beam test data for thin devices irradiated up to a fluence of 4 1015neq=cm2. For the active edge devices, the charge collection properties of the edge pixels before irradiation is discussed in detail, with respect to the inner ones, using measurements with radioactive sources. Beyond the active edge sensors, an additional ingredient needed to design four side buttable modules is the possibility of moving the wire bonding area from the chip surface facing the sensor to the backside, avoiding the implementation of the cantilever extruding beyond the sensor area. The feasibility of this process is under investigation with the FE-I3 SLID modules, where Inter Chip Vias are etched, employing an EMFT technology, with a cross section of 3 mx10 m, at the positions of the original wire bonding pads. info:eu-repo/grantAgreement/EC/FP7/262025 info:eu-repo/semantics/openAccess Education Level info:eu-repo/semantics/article http://cds.cern.ch/record/1693128 Nucl. Instrum. Methods Phys. Res., A Nucl. Instrum. Methods Phys. Res., A, (2013) pp. 210-215 2013
spellingShingle Detectors and Experimental Techniques
9: Advanced infrastructures for detector R&D
9.3: Precision Pixel Detectors
Macchiolo,A
Andricek,L
Ellenburg,M
Nisius,R
Richter,R.H
Terzo,S
Weigell,P
Thin n-in-p pixel sensors and the SLID-ICV vertical integration technology for the ATLAS upgrade at the HL-LHC
title Thin n-in-p pixel sensors and the SLID-ICV vertical integration technology for the ATLAS upgrade at the HL-LHC
title_full Thin n-in-p pixel sensors and the SLID-ICV vertical integration technology for the ATLAS upgrade at the HL-LHC
title_fullStr Thin n-in-p pixel sensors and the SLID-ICV vertical integration technology for the ATLAS upgrade at the HL-LHC
title_full_unstemmed Thin n-in-p pixel sensors and the SLID-ICV vertical integration technology for the ATLAS upgrade at the HL-LHC
title_short Thin n-in-p pixel sensors and the SLID-ICV vertical integration technology for the ATLAS upgrade at the HL-LHC
title_sort thin n-in-p pixel sensors and the slid-icv vertical integration technology for the atlas upgrade at the hl-lhc
topic Detectors and Experimental Techniques
9: Advanced infrastructures for detector R&D
9.3: Precision Pixel Detectors
url http://cds.cern.ch/record/1693128
http://cds.cern.ch/record/1693128
work_keys_str_mv AT macchioloa thinninppixelsensorsandtheslidicvverticalintegrationtechnologyfortheatlasupgradeatthehllhc
AT andricekl thinninppixelsensorsandtheslidicvverticalintegrationtechnologyfortheatlasupgradeatthehllhc
AT ellenburgm thinninppixelsensorsandtheslidicvverticalintegrationtechnologyfortheatlasupgradeatthehllhc
AT nisiusr thinninppixelsensorsandtheslidicvverticalintegrationtechnologyfortheatlasupgradeatthehllhc
AT richterrh thinninppixelsensorsandtheslidicvverticalintegrationtechnologyfortheatlasupgradeatthehllhc
AT terzos thinninppixelsensorsandtheslidicvverticalintegrationtechnologyfortheatlasupgradeatthehllhc
AT weigellp thinninppixelsensorsandtheslidicvverticalintegrationtechnologyfortheatlasupgradeatthehllhc