Gaseous argon time projection chamber with electroluminescence enhanced optical readout
Systematic uncertainties in accelerator oscillation neutrino experiments arise from nuclear models describing neutrino-nucleus interactions. To mitigate these uncertainties, we can study neutrino-nuclei interactions with detectors possessing enhanced hadron detection capabilities at energies below t...
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Veröffentlicht in: | Journal of instrumentation 2023-12, Vol.18 (12), p.P12001 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Systematic uncertainties in accelerator oscillation neutrino
experiments arise from nuclear models describing neutrino-nucleus
interactions. To mitigate these uncertainties, we can study
neutrino-nuclei interactions with detectors possessing enhanced
hadron detection capabilities at energies below the nuclear Fermi
level. Gaseous detectors not only lower the particle detection
threshold but also enable the investigation of nuclear effects on
various nuclei by allowing for changes in the gas composition. This
approach provides valuable insights into the modelling of
neutrino-nucleus interactions and significantly reduces associated
uncertainties. Here, we discuss the design and first operation of a
gaseous argon time projection chamber optically read. The detector
operates at atmospheric pressure and features a single stage of
electron amplification based on a thick GEM. Here, photons are
produced with wavelengths in the vacuum ultraviolet regime. In an
optical detector, the primary constraint is the light yield. This
study explores the possibility of increasing the light by applying a
low electric field downstream of the ThGEM. In this region, called
the electroluminescence gap, electrons propagate and excite the
argon atoms, leading to the subsequent emission of photons. This
process occurs without any further electron amplification, and it is
demonstrated that the total light yield increases up to three times
by applying moderate electric fields of the order of
3 kV/cm. Finally, an indirect method is discussed for determining
the photon yield/charge gain of a ThGEM, giving a value of
18.3 photons detected per secondary electron. |
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ISSN: | 1748-0221 1748-0221 |
DOI: | 10.1088/1748-0221/18/12/P12001 |