2017
DOI: 10.1016/j.ijhydene.2017.01.015
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Impact of In 2 S 3 shells thickness on the electrochemical and optical properties of oriented ZnO/In 2 S 3 core/shell nanowires

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Cited by 20 publications
(18 citation statements)
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“…The increasing in size with aniline concentrations from 0.01 M (composite I) to 0.03 M (composite II) is due to increasing of the nucleation sites that cause more coalescence of the deposited nano/microcomposite 41 . But with further increasing of the aniline concentration to 0.05 M (composite III), the particles sizes decrease due to the reduction of the Vander Waals force interactions that exist between the crystals because of disorder the particles deposition during the formation of core-shell composite 42 .…”
Section: Resultsmentioning
confidence: 99%
“…The increasing in size with aniline concentrations from 0.01 M (composite I) to 0.03 M (composite II) is due to increasing of the nucleation sites that cause more coalescence of the deposited nano/microcomposite 41 . But with further increasing of the aniline concentration to 0.05 M (composite III), the particles sizes decrease due to the reduction of the Vander Waals force interactions that exist between the crystals because of disorder the particles deposition during the formation of core-shell composite 42 .…”
Section: Resultsmentioning
confidence: 99%
“…With increased coverage and shell thickness, such absorptions are higher, consistent with the observed increased visible absorption of incident photon flux (Figure ). In addition, the spatial charge separation due to staggered energy band alignment in type-II heterostructure composed of ZnO NRs and CdS QDs may efficiently suppress the radiative recombination of photoinduced carriers and quenching the luminescence from ZnO, which is the dominant contribution to the reduction in NBE peak intensity of ZnO/CdS NRs. ,,, Such a suppression of charge carrier recombination suggests the occurrence of prolonged carriers’ lifetime in ZnO/CdS NRs heterostructure, beneficial for their photoelectrochemical cell (PEC) performance.…”
Section: Resultsmentioning
confidence: 99%
“…In addition, the spatial charge separation due to staggered energy band alignment in type-II heterostructure composed of ZnO NRs and CdS QDs may efficiently suppress the radiative recombination of photoinduced carriers and quenching the luminescence from ZnO, which is the dominant contribution to the reduction in NBE peak intensity of ZnO/CdS NRs. 13,15,26,45 Such a suppression of charge carrier recombination suggests the occurrence of prolonged carriers' lifetime in ZnO/CdS NRs heterostructure, beneficial for their photoelectrochemical cell (PEC) performance. Furthermore, a weak and broad visible emission band in the wavelength range of 500−750 nm (having two shoulder peaks P1 at ∼570 nm and P2 at ∼630 nm) is observed in measured PL spectra (inset of Figure 8a).…”
Section: X-ray Diffraction (Xrd)mentioning
confidence: 99%
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“…To overcome this limitation, different attempts have been undertaken such as (1) modulation of the morphology, which facilitates high light absorbance and the separation of photogenerated charge carriers, (2) elemental doping, which helps to tune the band gap of ZnO, (3) development of an efficient heterostructure of ZnO with some other narrow-band-gap semiconductors such as In 2 S 3 , CdS, etc., which helps to increase the spectral absorbance as well as to separate photogenerated electron–hole pairs, (4) sensitization with plasmonic nanoparticles to increase the optical absorbance. What is important is that semiconductor-based heterostructure formation has drawn tremendous attention in PEC water splitting recently by improving the light absorbance, and depending on the band alignment, it helps to increase the charge-carrier lifetime through proper separation. There are few reports on such heterostructure development for PEC water splitting.…”
Section: Introductionmentioning
confidence: 99%