2015
DOI: 10.1016/j.jphotochem.2015.05.016
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Morphology-sensitive trapping states of photogenerated charge carriers on SrTiO3 particles studied by time-resolved visible to Mid-IR absorption spectroscopy: The effects of molten salt flux treatments

Abstract: A B S T R A C TThe effects of the morphology-change of SrTiO 3 particles on the behavior of photogenerated charge carriers are studied by time-resolved absorption (TA) spectroscopy from the visible to mid-IR region. In the case of as-purchased defect-rich commercial SrTiO 3 particles, most of the charge carriers are deeply trapped, showing a transient absorption peak at 11,000 cm À1 . Scanning electron microscopy reveals that the irregular-shaped primary particles are heavily aggregated and that the photocatal… Show more

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Cited by 68 publications
(63 citation statements)
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“…On the other hand, the absorption at 12,000 cm −1 (Figure c) becomes stronger both in O 2 and CH 3 OH than in vacuum. As reported in our previous paper, such a behavior can occur when both the photoexcited electrons and holes contributes to the absorption. Therefore, the transient absorption at 12,000 cm −1 is ascribed to a mixture of trapped electrons and holes.…”
Section: Resultssupporting
confidence: 77%
See 1 more Smart Citation
“…On the other hand, the absorption at 12,000 cm −1 (Figure c) becomes stronger both in O 2 and CH 3 OH than in vacuum. As reported in our previous paper, such a behavior can occur when both the photoexcited electrons and holes contributes to the absorption. Therefore, the transient absorption at 12,000 cm −1 is ascribed to a mixture of trapped electrons and holes.…”
Section: Resultssupporting
confidence: 77%
“…To obtain deeper understanding of the mechanism, it is essential to know how the behaviors of photoexcited electrons and holes are changed by doping. The transient absorption spectroscopy is a powerful tool to observe the photocarrier dynamics . In this work, we investigated the Na‐doping effect on photocarrier dynamics in SrTiO 3 by measuring transient absorption from visible to mid‐IR region.…”
Section: Introductionmentioning
confidence: 99%
“…The broad absorption from 14000 -4000 cm -1 can be assigned to the transient absorption of deeply trapped electrons and/or holes at the defects. This absorption intensity is higher in Na-Ta 3 N 5 than in Cd-Ta 3 N 5 and Na-Cd-Ta 3 N 5 , indicating that the electron and/or hole is deeply trapped at defects in Na-Ta 3 N 5 [45,46]. The absorption below 4000 cm -1 is associated with shallowly trapped electrons and/or free electrons.…”
Section: N 5 Andmentioning
confidence: 90%
“…The shape of the transient absorption spectra was dependent on the nitridation temperature, which suggests that trap states in the band gap of Ta 3 N 5 are altered by the nitridation temperature. The transient absorption in the mid‐IR region (3000–1000 cm −1 ) is assigned to free electrons in the conduction band or shallowly trapped electrons, while the absorption in the visible to near‐IR region (16000–3000 cm −1 ) is attributed to the deeply trapped electrons and/or holes in mid‐gap states . Nitrogen vacancies have been reported as the most probable trap states in Ta 3 N 5 ; therefore, the trap states in the band gap can be ascribed to nitrogen vacancies.…”
Section: Resultsmentioning
confidence: 97%
“…To investigate the difference in activity for CO 2 reduction using Ta 3 N 5 /SiO 2 prepared at various temperatures, the behavior of photogenerated electrons and holes in Ta 3 N 5 /SiO 2 was investigated by recording transient absorption spectra. Although quantitative comparison of the transient absorption signal remains a challenge, the technique gives us very useful information on carrier dynamics of semiconductor materials . Figure shows transient absorption spectra for Ta 3 N 5 /SiO 2 synthesized at various temperatures.…”
Section: Resultsmentioning
confidence: 99%