Lead fluoride Cherenkov detector read out by avalanche photodiodes for measuring the intensities of pulsed antiproton beams

TL;DR

This paper presents a lead fluoride Cherenkov detector with avalanche photodiodes for measuring pulsed antiproton beam intensities, comparing different radiators and analyzing photodiode effects.

Contribution

It introduces a novel detector setup using lead fluoride crystals and avalanche photodiodes, and compares its performance with other radiators for antiproton flux measurement.

Findings

Lead fluoride crystals produced higher photon yields.

Avalanche photodiodes showed reduced nuclear counter effects.

The detector effectively measured secondary particle flux from antiproton annihilation.

Abstract

A Cherenkov detector based on an array of five lead fluoride ($\beta$-PbF$_2$) crystals of size 30 mm$\times$30 mm$\times$160 mm read out by reverse-type avalanche photodiodes (APD's) of active area 10 mm$\times$10 mm was used to measure the flux of secondary particles emerging from the annihilation of pulsed beams of antiprotons at the Antiproton Decelerator of CERN. We compared the relative photon yields of radiators made of $\beta$-PbF$_2$, fused silica, UV-transparent acrylic, lead glass, and a lead-free, high-refractive-index glass. Some {\it p-i-n} photodiodes were also used for the readout, but the output signals were dominated by the nuclear counter effect (NCE) of secondary particles traversing the 300 $\mu{\rm m}$ thick depletion regions of the photodiodes. Smaller NCE were observed with the APD's, as the maximum electronic gain in them occurred predominately for electron-ion pairs that were generated in the thin ${\it p}$-type semiconductor layer that proceeded the {\it p-n} junction of high electric field where amplification took place.