2018
DOI: 10.1016/j.materresbull.2018.04.050
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Photoluminescence, photoacoustic, and scintillation properties of Te 4+ -doped Cs 2 HfCl 6 crystals

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Cited by 30 publications
(13 citation statements)
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“…It is necessary to mention research reported in [21], where the question of doping of CHC crystal by Te 4+ ions was addressed. In this study the photoluminescence (PL) and scintillation properties of 1.0, 3.0, 5.0, and 10 mol% Te 4+ -doped Cs 2 HfCl 6 crystals were investigated along with photoacoustic (PA) spectroscopy, which enables direct monitoring of the non-radiative de-excitation processes that take place in the sample after absorption of irradiation energy.…”
Section: Crystal Typementioning
confidence: 99%
“…It is necessary to mention research reported in [21], where the question of doping of CHC crystal by Te 4+ ions was addressed. In this study the photoluminescence (PL) and scintillation properties of 1.0, 3.0, 5.0, and 10 mol% Te 4+ -doped Cs 2 HfCl 6 crystals were investigated along with photoacoustic (PA) spectroscopy, which enables direct monitoring of the non-radiative de-excitation processes that take place in the sample after absorption of irradiation energy.…”
Section: Crystal Typementioning
confidence: 99%
“…Therefore, the research strategy has been transferred to the substitution of aliovalent metal ions for Pb 2+ . It is worth noting that two B can be replaced by B I and B III , for example, Cs 2 NaBiCl 6 , Cs 2 (Ag 0.6 Na 0.4 )­InCl 6 , Cs 2 NaBi 1– x In x Cl 6 , Cs 2 Na 1– x Ag x BiCl 6 , etc. The second way is to explore perovskites with new chemical formulas AB III X 4 A 3 B III 2 X 9 and A 2 B′X 4 (B′ = Fe 2+ , Cu 2+ , Zn 2+ , and Mn 2+ ). The third way is to replace the B-site Pb 2+ in ABX 3 with B IV (B IV = Sn 4+ , Hf 4+ , Zr 4+ , Pd 4+ , Ti 4+ , and Te 4+ ). Based on this strategy, vacancy-ordered double perovskites A 2 B IV X 6 with good chemical stability have been formed, such as Cs 2 SnCl 6 , Cs 2 HfCl 6 , and Cs 2 ZrCl 6 . Among them, Cs 2 ZrCl 6 has been early explored about its luminescence. However, the emission of Cs 2 ZrCl 6 requires high-energy wavelength excitation, and it has not attracted widespread attention in the field of optoelectronics in the early years.…”
mentioning
confidence: 99%
“…Similar results were observed in Cs 2 HfCl 6 :Te 4+ crystalline scintillators in an earlier study. (30) To date, there are no theories to predict the performance of scintillators, and one phenomenological model (Robbins' model) is commonly used to explain the scintillation efficiency. (31,32) The model is formulated as LY SC = E/(βE g ) × S × Q, where LY SC is the scintillation LY, E is the deposited energy of ionizing radiation, β is the constant parameter, E g is the band gap energy, S is the energy migration efficiency from the host to emission centers, and Q is the fluorescence QE of the emission centers.…”
Section: Resultsmentioning
confidence: 99%