2018
DOI: 10.1039/c8ra00654g
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Green emission of indium oxide via hydrogen treatment

Abstract: H2-treated In2O3 gives rise to photoemission ranging from blue to green-yellow, while air-calcined In2O3 shows only blue emission. EPR and optical spectroscopies reveal singly ionized oxygen vacancies induced by H2 treatment responsible for the green-yellow emission.

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Cited by 38 publications
(35 citation statements)
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“…19a). The rising baseline in the near infrared spectral range could be caused by free electrons in the conduction band, generated by the homolytic splitting of H 2 30 . The absence of indium hydrides in the region of 1100−4000 cm −1 implies homolysis of H 2 , which is different from the former study over In 2 O 3−x (OH) y that exhibited heterolysis of H 2 31 .…”
Section: How Does Black Indium Oxide Function As a Photocatalyst?mentioning
confidence: 99%
“…19a). The rising baseline in the near infrared spectral range could be caused by free electrons in the conduction band, generated by the homolytic splitting of H 2 30 . The absence of indium hydrides in the region of 1100−4000 cm −1 implies homolysis of H 2 , which is different from the former study over In 2 O 3−x (OH) y that exhibited heterolysis of H 2 31 .…”
Section: How Does Black Indium Oxide Function As a Photocatalyst?mentioning
confidence: 99%
“…The peak at 132 cm −1 is attributed to the In-O vibration of [InO6] structural units, the peak at 307.7 cm −1 is due to the bending vibration of the δ-[InO6] octahedrons, Characteristic Raman vibrational modes corresponding to the body-centered cubic In 2 O 3 are observed at 132, 307.7, 366.7, 494.6, and 628.5 cm −1 and their positions are in agreement with previously reported data [44][45][46]. The peak at 132 cm −1 is attributed to the In-O vibration of [InO 6 ] structural units, the peak at 307.7 cm −1 is due to the bending vibration of the δ-[InO 6 ] octahedrons, the peaks at 494.6 and 628.5 cm −1 are assigned to the stretching vibrations of the ν-[InO 6 ] octahedrons, and the peak at 366.7 cm −1 is attributed to the stretching vibrations of the In-O-In bonds [47][48][49]. The broad peak at 458 cm −1 probably has the same nature as SnO 2 wide band at 563 cm −1 corresponding to a local structural defects due to small particle size of nanocrystalline In 2 O 3 [50].…”
Section: Characteristics Of Nanocrystalline Semiconductor Oxidesmentioning
confidence: 99%
“…Nanomaterials 2020, 10, x FOR PEER REVIEW 7 of 23 the peaks at 494.6 and 628.5 cm −1 are assigned to the stretching vibrations of the ν-[InO6] octahedrons, and the peak at 366.7 cm −1 is attributed to the stretching vibrations of the In-O-In bonds [47][48][49]. The broad peak at 458 cm −1 probably has the same nature as SnO2 wide band at 563 cm −1 corresponding to a local structural defects due to small particle size of nanocrystalline In2O3 [50].…”
Section: Characteristics Of Ru (Ii) Heterocyclic Complexmentioning
confidence: 99%
“…Peak 4 was included in the luminescence range of the In 2 O 3 particle [ 20 ]. All peaks in the visible light region are believed to originate from the defects in the structure of indium oxide [ 5 , 9 , 11 , 23 , 24 , 25 , 26 ]. This strong emission peak could be the evidence for the existence of defects, contributing to the lower resistivity and the degenerate semiconductor behavior.…”
Section: Resultsmentioning
confidence: 99%