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Sensor response and radiation damage effects for 3D pixels in the ATLAS IBL Detector

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Sensor response and radiation damage effects for 3D pixels in the ATLAS IBL Detector. / The ATLAS collaboration.
In: Journal of Instrumentation, Vol. 19, No. 10, P10008, 04.10.2024.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

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The ATLAS collaboration 2024, 'Sensor response and radiation damage effects for 3D pixels in the ATLAS IBL Detector', Journal of Instrumentation, vol. 19, no. 10, P10008. https://doi.org/10.1088/1748-0221/19/10/p10008

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The ATLAS collaboration. Sensor response and radiation damage effects for 3D pixels in the ATLAS IBL Detector. Journal of Instrumentation. 2024 Oct 4;19(10):P10008. doi: 10.1088/1748-0221/19/10/p10008

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The ATLAS collaboration. / Sensor response and radiation damage effects for 3D pixels in the ATLAS IBL Detector. In: Journal of Instrumentation. 2024 ; Vol. 19, No. 10.

Bibtex

@article{6eb2bca8b4a54b32afe8074768f29262,
title = "Sensor response and radiation damage effects for 3D pixels in the ATLAS IBL Detector",
abstract = "Pixel sensors in 3D technology equip the outer ends of the staves of the Insertable B Layer (IBL), the innermost layer of the ATLAS Pixel Detector, which was installed before the start of LHC Run 2 in 2015. 3D pixel sensors are expected to exhibit more tolerance to radiation damage and are the technology of choice for the innermost layer in the ATLAS tracker upgrade for the HL-LHC programme. While the LHC has delivered an integrated luminosity of {\^a}‰ƒ 235 fb-1 since the start of Run 2, the 3D sensors have received a non-ionising energy deposition corresponding to a fluence of {\^a}‰ƒ 8.5 {\~A}— 1014 1 MeV neutron-equivalent cm-2 averaged over the sensor area. This paper presents results of measurements of the 3D pixel sensors' response during Run 2 and the first two years of Run 3, with predictions of its evolution until the end of Run 3 in 2025. Data are compared with radiation damage simulations, based on detailed maps of the electric field in the Si substrate, at various fluence levels and bias voltage values. These results illustrate the potential of 3D technology for pixel applications in high-radiation environments.",
keywords = "Detector modelling and simulations II (electric fields, charge transport, multiplication and induction, pulse formation, electron emission, etc), Particle tracking detectors (Solid-state detectors)",
author = "{The ATLAS collaboration} and Zainab Alsolami and A.E. Barton and G. Borissov and E.V. Bouhova-Thacker and Ruby Ferguson and James Ferrando and H. Fox and Alina Hagan and R.C.W. Henderson and R.W.L. Jones and V. Kartvelishvili and P.A. Love and E.J. Marshall and L. Meng and D. Muenstermann and N. Ribaric and Elliot Sampson and M. Smizanska and A.M. Wharton",
year = "2024",
month = oct,
day = "4",
doi = "10.1088/1748-0221/19/10/p10008",
language = "English",
volume = "19",
journal = "Journal of Instrumentation",
issn = "1748-0221",
publisher = "Institute of Physics Publishing",
number = "10",

}

RIS

TY - JOUR

T1 - Sensor response and radiation damage effects for 3D pixels in the ATLAS IBL Detector

AU - The ATLAS collaboration

AU - Alsolami, Zainab

AU - Barton, A.E.

AU - Borissov, G.

AU - Bouhova-Thacker, E.V.

AU - Ferguson, Ruby

AU - Ferrando, James

AU - Fox, H.

AU - Hagan, Alina

AU - Henderson, R.C.W.

AU - Jones, R.W.L.

AU - Kartvelishvili, V.

AU - Love, P.A.

AU - Marshall, E.J.

AU - Meng, L.

AU - Muenstermann, D.

AU - Ribaric, N.

AU - Sampson, Elliot

AU - Smizanska, M.

AU - Wharton, A.M.

PY - 2024/10/4

Y1 - 2024/10/4

N2 - Pixel sensors in 3D technology equip the outer ends of the staves of the Insertable B Layer (IBL), the innermost layer of the ATLAS Pixel Detector, which was installed before the start of LHC Run 2 in 2015. 3D pixel sensors are expected to exhibit more tolerance to radiation damage and are the technology of choice for the innermost layer in the ATLAS tracker upgrade for the HL-LHC programme. While the LHC has delivered an integrated luminosity of ≃ 235 fb-1 since the start of Run 2, the 3D sensors have received a non-ionising energy deposition corresponding to a fluence of ≃ 8.5 × 1014 1 MeV neutron-equivalent cm-2 averaged over the sensor area. This paper presents results of measurements of the 3D pixel sensors' response during Run 2 and the first two years of Run 3, with predictions of its evolution until the end of Run 3 in 2025. Data are compared with radiation damage simulations, based on detailed maps of the electric field in the Si substrate, at various fluence levels and bias voltage values. These results illustrate the potential of 3D technology for pixel applications in high-radiation environments.

AB - Pixel sensors in 3D technology equip the outer ends of the staves of the Insertable B Layer (IBL), the innermost layer of the ATLAS Pixel Detector, which was installed before the start of LHC Run 2 in 2015. 3D pixel sensors are expected to exhibit more tolerance to radiation damage and are the technology of choice for the innermost layer in the ATLAS tracker upgrade for the HL-LHC programme. While the LHC has delivered an integrated luminosity of ≃ 235 fb-1 since the start of Run 2, the 3D sensors have received a non-ionising energy deposition corresponding to a fluence of ≃ 8.5 × 1014 1 MeV neutron-equivalent cm-2 averaged over the sensor area. This paper presents results of measurements of the 3D pixel sensors' response during Run 2 and the first two years of Run 3, with predictions of its evolution until the end of Run 3 in 2025. Data are compared with radiation damage simulations, based on detailed maps of the electric field in the Si substrate, at various fluence levels and bias voltage values. These results illustrate the potential of 3D technology for pixel applications in high-radiation environments.

KW - Detector modelling and simulations II (electric fields, charge transport, multiplication and induction, pulse formation, electron emission, etc)

KW - Particle tracking detectors (Solid-state detectors)

U2 - 10.1088/1748-0221/19/10/p10008

DO - 10.1088/1748-0221/19/10/p10008

M3 - Journal article

VL - 19

JO - Journal of Instrumentation

JF - Journal of Instrumentation

SN - 1748-0221

IS - 10

M1 - P10008

ER -