A Threshold Gas \v{C}erenkov Detector for the Spin Asymmetries of the Nucleon Experiment

TL;DR

This paper details the design and performance of a gas renkov detector used in the Spin Asymmetries of the Nucleon Experiment at Jefferson Lab, achieving high photo-electron yield and effective particle identification in a high luminosity environment.

Contribution

It introduces a novel open geometry renkov counter with high photo-electron yield for electron identification in a polarized scattering experiment.

Findings

Achieved about 20 photoelectrons per track.

Successfully identified electrons and rejected pions.

Resolved electron-positron pairs from photon conversions.

Abstract

We report on the design, construction, commissioning, and performance of a threshold gas \v{C}erenkov counter in an open configuration, which operates in a high luminosity environment and produces a high photo-electron yield. Part of a unique open geometry detector package known as the Big Electron Telescope Array, this \v{C}erenkov counter served to identify scattered electrons and reject produced pions in an inclusive scattering experiment known as the Spin Asymmetries of the Nucleon Experiment E07-003 at the Thomas Jefferson National Accelerator Facility (TJNAF) also known as Jefferson Lab. The experiment consisted of a measurement of double spin asymmetries $A_{\parallel}$ and $A_{\perp}$ of a polarized electron beam impinging on a polarized ammonia target. The \v{C}erenkov counter's performance is characterised by a yield of about 20 photoelectrons per electron or positron track. Thanks to this large number of photoelectrons per track, the \v{C}erenkov counter had enough resolution to identify electron-positron pairs from the conversion of photons resulting mainly from $\pi^0$ decays.