Scintillation light yield of Tb: Sr2Gd8(SiO4)6O2

Author(s):  
Kenichi Watanabe ◽  
Takayuki YANAGIDA ◽  
Daisuke NAKAUCHI ◽  
Noriaki KAWAGUCHI
1966 ◽  
Vol 21 (7) ◽  
pp. 1075-1080
Author(s):  
W. Schött ◽  
A. Flammersfeld

The scintillation light yield S of three anorganic [NaJ (Tl), KJ (Tl), CsJ (Tl)], of two organic (p-terphenyl, anthracene) crystals, and of plastic NE 102 by bombardement with deuterons in the energy range from 10,0—27,5 MeV, α-particles from 8,0—55,0 MeV, and electrons has been measured. The time constants of the electronic circuit have been chosen to τ1 = 0,5 sec and τ2 = 2,0 µsec. The pulse-height ratios SD/Sβ and Sα/Sβ are slightly different for the two time constants. The anorganic crystals have a higher pulse-height ratio for the short time constant, whereas the organic crystals and plastic show the inverse effect.


Crystals ◽  
2019 ◽  
Vol 9 (2) ◽  
pp. 88 ◽  
Author(s):  
Francesco Maddalena ◽  
Liliana Tjahjana ◽  
Aozhen Xie ◽  
Arramel ◽  
Shuwen Zeng ◽  
...  

Trends in scintillators that are used in many applications, such as medical imaging, security, oil-logging, high energy physics and non-destructive inspections are reviewed. First, we address traditional inorganic and organic scintillators with respect of limitation in the scintillation light yields and lifetimes. The combination of high–light yield and fast response can be found in Ce 3 + , Pr 3 + and Nd 3 + lanthanide-doped scintillators while the maximum light yield conversion of 100,000 photons/MeV can be found in Eu 3 + doped SrI 2 . However, the fabrication of those lanthanide-doped scintillators is inefficient and expensive as it requires high-temperature furnaces. A self-grown single crystal using solution processes is already introduced in perovskite photovoltaic technology and it can be the key for low-cost scintillators. A novel class of materials in scintillation includes lead halide perovskites. These materials were explored decades ago due to the large X-ray absorption cross section. However, lately lead halide perovskites have become a focus of interest due to recently reported very high photoluminescence quantum yield and light yield conversion at low temperatures. In principle, 150,000–300,000 photons/MeV light yields can be proportional to the small energy bandgap of these materials, which is below 2 eV. Finally, we discuss the extraction efficiency improvements through the fabrication of the nanostructure in scintillators, which can be implemented in perovskite materials. The recent technology involving quantum dots and nanocrystals may also improve light conversion in perovskite scintillators.


Author(s):  
Md. Shahinur Rahman ◽  
Wayne D. Hutchison ◽  
Lindsey Bignell ◽  
Gregory Lane ◽  
Lei Wang ◽  
...  

Abstract The SABRE (Sodium-iodide with Active Background Rejection) experiment consists of 50 kg of ultrapure NaI(Tl) crystal contained within a 10.5 ton liquid scintillator (LS) veto detector, and will search for dark matter interactions in the inner NaI(Tl) detector. The relative scintillation light yield in NaI(Tl) scintillator for different incident particle energies is not constant and is important for characterizing the detector response. The relative scintillation light yield in two different NaI(Tl) scintillators was measured with a 10 µCi 137Cs radioactive source using the Compton coincidence technique (CCT) for scattering angles 30? - 135? using electron energies ranging from 60 to 500 keVee, and these measurements are compared to the previously published results. Light yield was proportional within 3.5% at energies between 60 and 500 keVee, but non-proportionality increases drastically below 60 keVee which might be due to the non-uniform ionization density and multiple Compton scattering background events in the scintillator. An improved experimental setup with ultrapure NaI(Tl) scintillator and proper coincidence timing of radioactive events could allow scintillation light yield measurement at lower electron recoil energy. The obtained light yield non-proportionality results will be useful for the SABRE dark matter detector experiment.


2020 ◽  
pp. 499-542
Author(s):  
Hermann Kolanoski ◽  
Norbert Wermes

The detection of scintillation light, which is generated when an ionising particle passes certain media or when radiation is absorbed, belongs to the oldest detection techniques. Scintillation detectors are read out electronically by employing the photon detectors described in a previous chapter. Scintillators are either made of organic or of inorganic materials (crystals) with essential differences of their properties and application field. For both scintillation mechanisms, the light yield and the time dependence of the signals are explained and the specific application areas pointed out. Typical assemblies of scintillation detectors are presented which include organic scintillators as trigger and timing counters, scintillating fibres for tracking and calorimetry and inorganic crystal arrangements for calorimetry.


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