Abstract

Biexcitonic collision kinetics with prescribed diffusion in the ion track core have been applied for scintillation response due to heavy ions in liquid argon. The quenching factors q = EL/E, where E is the ion energy and EL is the energy expended for luminescence, for 33.5 MeV/n 18O and 31.9 MeV/n 36Ar ions in liquid Ar at zero field are found to be 0.73 and 0.46, compared with measured values of 0.59 and 0.46, respectively. The quenching model is also applied for 80–200 keV Pb recoils in α-decay, background candidates in direct dark matter searches, in liquid argon. Values obtained are ~0.09. A particular feature of Birks’ law has been found and exploited in evaluating the electronic quenching factor qel in liquid Xe. The total quenching factors qT for 0.5–20 keV Xe recoils needed for weakly interacting massive particle (WIMP) searches are estimated to be ~0.12–0.14, and those for Pb recoils of 103 and 169 keV are 0.08 and 0.09, respectively. In the calculation, the nuclear quenching factor qnc = Eη/E, where Eη is the energy available for the electronic excitation, is obtained by Lindhard theory and a semi-empirical theory by Ling and Knipp. The electronic linear energy transfer plays a key role.

Highlights

  • Noble liquids are used in various fields of study in particle physics, high energy physics, cosmology and medicine

  • A different approach was taken for Xe and Pb recoil ions in liquid Xe (LXe) as described below

  • N0 is given by N0 = {(E/We)·(1 + Nex/Ni)·(Tc/T)}/R, where We is the W-value for electrons, 23.6 and 15.6 eV in liquid Ar (LAr) and LXe, respectively

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Summary

Introduction

Noble liquids are used in various fields of study in particle physics, high energy physics, cosmology and medicine. Noble liquids can be used for various types of detectors, including ionization chambers, scintillation detectors, proportional counters, proportional scintillation counters, photoionization detectors (PIDs), γ-cameras, positron emission tomography (PET), calorimeters and time projection chambers (TPCs) [1,2,3,4]. Noble liquids make ideal detector material because of high density and high Z (Xe), as well as high stopping power for γ-rays and β-rays, providing self-shielding from external backgrounds. Noble liquids have high electron mobility and no size limits, and they suffer no permanent radiation damage. Scintillation is in the vacuum ultraviolet (VUV) region, various wavelength shifters are available, and a VUV sensitive photomultiplier tube (PMT) with a high quantum efficiency, as high as 34%, has been developed for liquid Xe (LXe) [5]

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