How Silicon and Boron Dopants Govern the Cryogenic Scintillation Properties of N-type GaAs

TL;DR

This study investigates how silicon and boron dopant concentrations influence the cryogenic scintillation properties of n-type GaAs, revealing optimal doping ranges for efficient light emission suitable for dark matter detection.

Contribution

It is the first to systematically analyze the impact of silicon and boron doping levels on GaAs scintillation properties at cryogenic temperatures.

Findings

Higher free carrier densities increase radiative recombination rates.

Luminosity exceeds 70 photons/keV in several samples within optimal doping ranges.

Decay times decrease significantly with increased free carrier concentration.

Abstract

This paper is the first report describing how the concentrations of silicon and boron govern the cryogenic scintillation properties of n-type GaAs. It shows that valence band holes are promptly trapped on radiative centers and then combine radiatively with silicon donor band electrons at rates that increase with the density of free carriers. It also presents the range of silicon and boron concentrations needed for efficient light emission under X-ray excitation, which along with its low band gap and apparent absence of afterglow, make scintillating GaAs suitable for the detection of rare, low-energy electronic excitations from interacting dark matter particles. A total of 29 samples from four different suppliers were studied. Luminosities and timing responses were measured for the four principal emission bands centered at 860, 930, 1070, and 1335 nm, and for the total emissions. Excitation pulses of 40 kVp X-rays were provided by a light-excited X-ray tube driven by an ultra-fast laser. Scintillation emissions from 800 to 1350 nm were measured using an InGaAs photomultiplier. Within the concentration ranges of free carriers from 2 x 10^16/cm3 to 6 x 10^17/cm3 and boron from 1.5 x 10^18/cm3 to 6 x 10^18/cm3, nine samples have luminosities > 70 photons/keV and two have luminosities > 110 photons/keV. Other samples in that range have lower luminosities due to higher concentrations of non-radiative centers. The decay times decrease by typically a factor of ten with increasing free carrier concentrations from 10^17/cm3 to 2 x 10^18/cm3.