2016
DOI: 10.1016/j.solmat.2015.08.036
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Influence of surface disorder, oxygen defects and bandgap in TiO2 nanostructures on the photovoltaic properties of dye sensitized solar cells

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Cited by 77 publications
(29 citation statements)
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“…B 1g (2) , and 642 cm -1 for E g(2) [28]. The rutile phase is readily identified by the most intense rutile Raman modes at *448 cm -1 for E g and 612 cm -1 for A 1g [29,30], as shown in the inset of Fig. 3.…”
Section: Characterization Of Rgo-tio 2 Photoanodementioning
confidence: 84%
“…B 1g (2) , and 642 cm -1 for E g(2) [28]. The rutile phase is readily identified by the most intense rutile Raman modes at *448 cm -1 for E g and 612 cm -1 for A 1g [29,30], as shown in the inset of Fig. 3.…”
Section: Characterization Of Rgo-tio 2 Photoanodementioning
confidence: 84%
“…Apart from the surface phenomena, bulk characteristics of defective Titania like superficial and deep defect states offer a dominant pathway for charge transport [148][149][150][151][152][153][154][155][156][157][158]. Also, defective Titania absorbs visible light, and the defect concentration tunes their optical behavior [159][160][161][162]. Importantly, defective Titania possesses numerous dangling bonds and serve as a bridge to facilitate charge transfer once it is photo-excited.…”
Section: Role Of Defects Towards Photoelectrochemical Water Splittingmentioning
confidence: 99%
“…9). The diffuse reflectance can be converted into absorption coefficient equivalent using Kubelka-Munk function, F(R), as represented below [49] where, F(R) is the Kubelka-Munk function of the sample and R is the reflectance of the sample. In the parabolic band structure, the Eg and absorption coefficient are related through the well-known Tauc relation [50].…”
Section: Xps Analysismentioning
confidence: 99%