First study of single-event burnout in very-thin planar silicon sensors
This paper investigates the single-event burnout (SEB) effect in thin irradiated positive-intrinsic-negative (PiN) diodes and low-gain avalanche diodes (LGAD). SEB is a destructive event triggered in silicon sensors by the passage of a high-momentum charged particle. This effect arises in planar sen...
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| Main Authors: | , , , , , , , , , , |
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| Format: | Article |
| Language: | English |
| Published: |
Frontiers Media S.A.
2025-05-01
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| Series: | Frontiers in Physics |
| Subjects: | |
| Online Access: | https://www.frontiersin.org/articles/10.3389/fphy.2025.1575672/full |
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| Summary: | This paper investigates the single-event burnout (SEB) effect in thin irradiated positive-intrinsic-negative (PiN) diodes and low-gain avalanche diodes (LGAD). SEB is a destructive event triggered in silicon sensors by the passage of a high-momentum charged particle. This effect arises in planar sensors under specific conditions: a significant ionization event caused by the particle’s passage and a very high electric field in the entire bulk region. The investigation of SEB was performed in two beam test campaigns: one at Deutsches Elektronen-Synchrotron (DESY) with an electron beam of 3.6 GeV/c momentum and the second at CERN with a pion and proton beam of 120 GeV/c momentum. The sensors under test had active thicknesses from 15 μm to 55 μm and active surfaces from 1.7 mm2 to 433 mm2. In preparation for this study, most sensors were irradiated with neutrons up to a fluence of 1⋅1016 neq/cm2. The experimental setup for the beam tests included a frame for the alignment of the sensor with six available slots, two of which were equipped with trigger boards to monitor the beam rate during the test campaigns. This frame was placed inside a cold box to operate the irradiated sensors at very high electric fields while keeping their leakage current low. The experimental results show an inversely proportional relationship between the electric field at the SEB (SEB field) and the active thickness of the sensors. In this study, the SEB field increases from 11-12 V/μm in a 55-μm-thick sensor to 14 V/μm in a 15–20 μm-thick sensor. |
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| ISSN: | 2296-424X |