Gaseous argon time projection chamber with electroluminescence enhanced optical readout

TL;DR

This paper presents the design and initial results of a gaseous argon time projection chamber with electroluminescence enhancement, aiming to improve neutrino-nucleus interaction studies by increasing light yield and reducing uncertainties.

Contribution

It introduces a novel optical readout method for a gaseous argon TPC with electroluminescence, demonstrating increased light yield through moderate electric fields.

Findings

Light yield increases up to three times with 3 kV/cm electric field.

Photon yield per secondary electron is approximately 18.3.

The detector operates effectively at atmospheric pressure with a single-stage GEM amplification.

Abstract

Systematic uncertainties in accelerator oscillation neutrino experiments arise mostly 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 yield 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 per charge gain of a ThGEM, giving a value of 18.3 photons detected per secondary electron.