2009
DOI: 10.1016/j.solmat.2008.12.014
|View full text |Cite
|
Sign up to set email alerts
|

Structural, optical and luminescent characteristics of sprayed fluorine-doped In2O3 thin films for solar cells

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

2
5
0

Year Published

2014
2014
2019
2019

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 25 publications
(7 citation statements)
references
References 30 publications
2
5
0
Order By: Relevance
“…For InN, the variation in photon attenuation length with excitation energy is shown in Figure d . The authors in ref reported the cathodoluminescence spectra of fluorine-doped c-In 2 O 3 , which matches well with our spectra, but they were not able to measure the spectra lower than 330 nm and higher than 975 nm because of instrumental limitations. They observed two broad peaks at 410 and 650 nm and claimed that the origin of the former peak corresponds the indirect conduction band to the valence band transition of c-In 2 O 3 and the 650 nm peak originates from oxygen defects.…”
Section: Resultssupporting
confidence: 86%
See 1 more Smart Citation
“…For InN, the variation in photon attenuation length with excitation energy is shown in Figure d . The authors in ref reported the cathodoluminescence spectra of fluorine-doped c-In 2 O 3 , which matches well with our spectra, but they were not able to measure the spectra lower than 330 nm and higher than 975 nm because of instrumental limitations. They observed two broad peaks at 410 and 650 nm and claimed that the origin of the former peak corresponds the indirect conduction band to the valence band transition of c-In 2 O 3 and the 650 nm peak originates from oxygen defects.…”
Section: Resultssupporting
confidence: 86%
“…In this analysis the center position of all Gaussians remained constant for each excitation energy. Note that the luminescence feature of c-In 2 O 3 at around 667 nm is due to oxygen defects. It is shown that the c-In 2 O 3 luminescence spectrum is present for all excitation energies, and its intensity is almost identical for all excitation energies (for different attenuation lengths), indication with presence of c-In 2 O 3 throughout the InN samples. From the fitting, a small g 3 Gaussian feature is observed in the same position (at 651 nm) of the luminescence spectrum of c-In 2 O 3 .…”
Section: Resultsmentioning
confidence: 91%
“…Two of these PL bands (with the peaks near 2 and 3 eV) are not associated with the recombination in the synthesized silicon suboxide as they dominate in the photoluminescence spectrum of the sample with In particles after the H 2 plasma treatment (see 6 curve on Figure , inset). According to the literature data, these PL bands correspond to the transitions in the In 2 O 3 , which indicates the formation of the In 2 O 3 and is in complete agreement with the results of the X‐ray EDS analysis mentioned above. It should be noted that the PL bands from In 2 O 3 nanoparticles are best resolved in the structures with silicon suboxide films.…”
Section: Resultssupporting
confidence: 89%
“…[http://dx.doi.org/10.1063/1.4875457] Indium tin oxide (ITO) or Sn doped In 2 O 3 nanowires (NWs) are important as transparent conducting oxides (TCOs) for the fabrication of solar cells, [1][2][3] flexible displays, 4 and ultra violet light emitting diodes [5][6][7][8][9] because it has been suggested that higher Sn doping levels and conductivities can be attained in ITO NWs compared to bulk ITO. So far ITO NWs have been grown by carbothermal reduction of In 2 O 3 and SnO 2 5 but the control of stoichiometry is not trivial as it has been observed that SnO 2 NWs may be obtained even when a higher content of In 2 O 3 is used during carbothermal reduction carried out under an inert gas flow at elevated temperatures 10,11 which also leads to the non-intentional incorporation of carbon.…”
Section: Fermi Level Position © 2014 Author(s) All Article Contentmentioning
confidence: 99%