2023
DOI: 10.1021/acs.inorgchem.3c03039
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Antimony Doping Enabled Photoluminescence Quantum Yield Enhancement in 0D Inorganic Bismuth Halide Crystals

Zhen Jia,
Pifu Gong,
Mingxing Chen
et al.
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Cited by 4 publications
(2 citation statements)
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“…There are disagreements in the interpretation of these bands in the PLE spectrum of In 3+ -based hexabromides without doping. ,,,, On the one hand, these excitation bands at 324–326 nm and 362–365 nm can be attributed to parity-forbidden exciton transitions in isolated [InBr 6 ] 3– , like the band at 380 in the absorption spectrum, or even associated with the 1 S 0 → 1 P 1 and 1 S 0 → 3 P 1 transitions of In 3+ ions, which seems not entirely correct to us. On the other hand, such bands in the PLE spectrum (Figure b) are characteristic specifically of ns 2 ions, for example, Sb 3+ ,, or Bi 3+ . , Many researchers point out that the presence of Sb as a native impurity in In-based halides is responsible for their luminescent properties ,, since materials based on pure In 3+ either do not emit or emit very weakly ,,,, due to the parity-forbidden transitions of In 3+ . Based on the latter, we can assume that the PLE spectrum of both undoped and Sb 3+ -doped (TUH) 6 [In 1– x Sb x Br 6 ]­Br 3 powders in the range of 290–450 nm, by monitoring at 600 nm, exhibits bands characteristic of the spin-forbidden 1 S 0 → 3 P 1 transition of the Sb 3+ ions, which is possible due to the strong spin–orbital coupling for heavy atoms.…”
Section: Resultsmentioning
confidence: 99%
“…There are disagreements in the interpretation of these bands in the PLE spectrum of In 3+ -based hexabromides without doping. ,,,, On the one hand, these excitation bands at 324–326 nm and 362–365 nm can be attributed to parity-forbidden exciton transitions in isolated [InBr 6 ] 3– , like the band at 380 in the absorption spectrum, or even associated with the 1 S 0 → 1 P 1 and 1 S 0 → 3 P 1 transitions of In 3+ ions, which seems not entirely correct to us. On the other hand, such bands in the PLE spectrum (Figure b) are characteristic specifically of ns 2 ions, for example, Sb 3+ ,, or Bi 3+ . , Many researchers point out that the presence of Sb as a native impurity in In-based halides is responsible for their luminescent properties ,, since materials based on pure In 3+ either do not emit or emit very weakly ,,,, due to the parity-forbidden transitions of In 3+ . Based on the latter, we can assume that the PLE spectrum of both undoped and Sb 3+ -doped (TUH) 6 [In 1– x Sb x Br 6 ]­Br 3 powders in the range of 290–450 nm, by monitoring at 600 nm, exhibits bands characteristic of the spin-forbidden 1 S 0 → 3 P 1 transition of the Sb 3+ ions, which is possible due to the strong spin–orbital coupling for heavy atoms.…”
Section: Resultsmentioning
confidence: 99%
“…Bright orange emission at 628 nm was reported in Sb 3+ doped Rb 3 BiCl 6 ·0.5H 2 O. 69 In contrast, the introduction of Sb 3+ into the Cs 2 Na(Bi, Sb)Cl 6 structure resulted in a PL peak in the blue-green region (480 nm), while the pristine host material emits orange-red light with a peak at 700 nm. 70 In Cs 2 MInCl 6 : x Sb 3+ , the emission color changes from blue to green for M = Na and M = K, respectively.…”
Section: Hdp Photoluminescencementioning
confidence: 99%