Measuring the ATLAS ITk pixel detector material via multiple scattering of positrons at the CERN PS

The ITk is a new silicon tracker for the ATLAS experiment designed to increase detector resolution, readout capacity, and radiation hardness, in preparation for the larger number of simultaneous proton-proton interactions at the High Luminosity LHC. This paper presents the first direct measurement of the material budget of an ATLAS ITk pixel module, performed at a testbeam at the CERN Proton Synchrotron via the multiple scattering of low energy positrons within the module volume. Using a four plane telescope of thin monolithic pixel detectors from the MALTA Collaboration, scattering datasets were recorded at a beam energy of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mn>1.2</mml:mn> <mml:mspace></mml:mspace> <mml:mtext>GeV</mml:mtext></mml:mrow> </mml:math> . Kink angle distributions were extracted from tracks derived with and without information from the ITk pixel module, and were fit to extract the RMS scattering angle, which was converted to a fractional radiation length <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>x</mml:mi> <mml:mo>/</mml:mo> <mml:msub><mml:mi>X</mml:mi> <mml:mn>0</mml:mn></mml:msub> </mml:mrow> </mml:math> . The average <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>x</mml:mi> <mml:mo>/</mml:mo> <mml:msub><mml:mi>X</mml:mi> <mml:mn>0</mml:mn></mml:msub> </mml:mrow> </mml:math> across the module was measured as <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mo>[</mml:mo> <mml:mn>0.89</mml:mn> <mml:mo>±</mml:mo> <mml:mn>0.01</mml:mn> <mml:mspace></mml:mspace> <mml:mtext>(resolution)</mml:mtext> <mml:mo>±</mml:mo> <mml:mn>0.01</mml:mn> <mml:mspace></mml:mspace> <mml:mtext>(subtraction)</mml:mtext> <mml:mspace></mml:mspace> <mml:mspace></mml:mspace> <mml:mo>±</mml:mo> <mml:mspace></mml:mspace> <mml:mspace></mml:mspace> <mml:mn>0.08</mml:mn> <mml:mspace></mml:mspace> <mml:mtext>(beam momentum band)</mml:mtext> <mml:mo>]</mml:mo> <mml:mo>%</mml:mo></mml:mrow> </mml:math> , which agrees within uncertainties with an estimate of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mn>0.88</mml:mn> <mml:mo>%</mml:mo></mml:mrow> </mml:math> derived from material component expectations.

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Journal
The European Physical Journal C
Published
2025-04-03
DOI
https://doi.org/10.1140/epjc/s10052-025-14092-2
Primary Topic
Particle Detector Development and Performance
Type
article
Field-Weighted Citation Impact
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article

Measuring the ATLAS ITk pixel detector material via multiple scattering of positrons at the CERN PS

V. Dao, S. F. Koch, B. Moser, Hans Ludwig Joos et al.
The European Physical Journal C
Particle Detector Development and Performance
article

Measuring the ATLAS ITk pixel detector material via multiple scattering of positrons at the CERN PS

V. Dao, S. F. Koch, B. Moser, Hans Ludwig Joos, M. Van Rijnbach, Carlos Solans Sánchez, Ignacio Asensi Tortajada, A. Sharma, Y. Wei, D. Bortoletto, A. Lindner, F. Dachs, I. Siral, Marianne Brekkum
article en

Abstract

The ITk is a new silicon tracker for the ATLAS experiment designed to increase detector resolution, readout capacity, and radiation hardness, in preparation for the larger number of simultaneous proton-proton interactions at the High Luminosity LHC. This paper presents the first direct measurement of the material budget of an ATLAS ITk pixel module, performed at a testbeam at the CERN Proton Synchrotron via the multiple scattering of low energy positrons within the module volume. Using a four plane telescope of thin monolithic pixel detectors from the MALTA Collaboration, scattering datasets were recorded at a beam energy of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mn>1.2</mml:mn> <mml:mspace></mml:mspace> <mml:mtext>GeV</mml:mtext></mml:mrow> </mml:math> . Kink angle distributions were extracted from tracks derived with and without information from the ITk pixel module, and were fit to extract the RMS scattering angle, which was converted to a fractional radiation length <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>x</mml:mi> <mml:mo>/</mml:mo> <mml:msub><mml:mi>X</mml:mi> <mml:mn>0</mml:mn></mml:msub> </mml:mrow> </mml:math> . The average <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>x</mml:mi> <mml:mo>/</mml:mo> <mml:msub><mml:mi>X</mml:mi> <mml:mn>0</mml:mn></mml:msub> </mml:mrow> </mml:math> across the module was measured as <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mo>[</mml:mo> <mml:mn>0.89</mml:mn> <mml:mo>±</mml:mo> <mml:mn>0.01</mml:mn> <mml:mspace></mml:mspace> <mml:mtext>(resolution)</mml:mtext> <mml:mo>±</mml:mo> <mml:mn>0.01</mml:mn> <mml:mspace></mml:mspace> <mml:mtext>(subtraction)</mml:mtext> <mml:mspace></mml:mspace> <mml:mspace></mml:mspace> <mml:mo>±</mml:mo> <mml:mspace></mml:mspace> <mml:mspace></mml:mspace> <mml:mn>0.08</mml:mn> <mml:mspace></mml:mspace> <mml:mtext>(beam momentum band)</mml:mtext> <mml:mo>]</mml:mo> <mml:mo>%</mml:mo></mml:mrow> </mml:math> , which agrees within uncertainties with an estimate of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mn>0.88</mml:mn> <mml:mo>%</mml:mo></mml:mrow> </mml:math> derived from material component expectations.

The European Physical Journal CVol. 85(4)
University of Oslo (NO), University of Oxford (GB), Stony Brook University (US), European Organization for Nuclear Research (CH), University of Göttingen (DE)
CERN, European Commission, Science and Technology Facilities Council
Openalex Percentile: Top 96%
Particle Detector Development and Performance
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