2016
DOI: 10.1016/j.chemphys.2016.08.002
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Dynamics of charge at water-to-semiconductor interface: Case study of wet [0 0 1] anatase TiO2 nanowire

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Cited by 5 publications
(3 citation statements)
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References 85 publications
(86 reference statements)
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“…As expected, the NAC between adjacent states (e.g., the subdiagonals) is larger than the couplings between energetically distant electronic states. This trend is consistent with the notion that the magnitude of NAC between two states is inversely proportional to the energy gap between them. , Comparing the average NAC between the HOMO and LUMO states in SiR- and GeR-based heterostructures, we observe larger magnitudes in the latter. The average NAC between HOMO and LUMO states is 0.04 meV in SiH/a-TiO 2 and 0.26 meV in SiH/r-TiO 2 , whereas it increases to 0.54 meV in GeH/a-TiO 2 and 3.00 meV in GeH/r-TiO 2 .…”
Section: Resultssupporting
confidence: 91%
“…As expected, the NAC between adjacent states (e.g., the subdiagonals) is larger than the couplings between energetically distant electronic states. This trend is consistent with the notion that the magnitude of NAC between two states is inversely proportional to the energy gap between them. , Comparing the average NAC between the HOMO and LUMO states in SiR- and GeR-based heterostructures, we observe larger magnitudes in the latter. The average NAC between HOMO and LUMO states is 0.04 meV in SiH/a-TiO 2 and 0.26 meV in SiH/r-TiO 2 , whereas it increases to 0.54 meV in GeH/a-TiO 2 and 3.00 meV in GeH/r-TiO 2 .…”
Section: Resultssupporting
confidence: 91%
“…The electronic structure of bulk anatase TiO 2 has been described elsewhere. , It is an indirect band gap semiconductor (E g ∼ 3.2 eV) with intense absorption in the UV region due to O 2p → Ti 3d ligand to metal charge transfer (LMCT). However, TiO 2 nanostructures with dimension <5 nm undergo significant changes in electronic structure due to quantum confinement and transition to a direct band gap semiconductor. In anatase TiO 2 nanosheets, quantum confinement leads to a slight negative shift of the conduction band edge potential of ∼0.08 V, and a positive shift of the valence band edge by ∼0.5 V yields a bandgap of ∼3.8 eV. , The thickness of TiO 2 NR and TiO 2 nanosheets are very similar, and both materials give rise to strongly blue-shifted UV–visible spectra …”
Section: Resultsmentioning
confidence: 99%
“…91,92 The thickness of TiO 2 NR and TiO 2 nanosheets are very similar, and both materials give rise to strongly blue-shifted UV−visible spectra. 93 Addition of transition metal ions to the surface of TiO 2 NR leads to changes in the UV−visible spectrum. The UV−visible spectra of M-TiO 2 samples were reported previously.…”
Section: ■ Experimental Sectionmentioning
confidence: 99%