scholarly journals Band Gap and Photo luminescence studies of Sm3+ doped TiO2 NP for wLED

IARJSET ◽  
2021 ◽  
Vol 8 (11) ◽  
Author(s):  
Venkatesha Babu K R ◽  
Renuka CG ◽  
Mohamed Zikriya
Materials ◽  
2021 ◽  
Vol 14 (14) ◽  
pp. 3918
Author(s):  
Ratshilumela S. Dima ◽  
Lutendo Phuthu ◽  
Nnditshedzeni E. Maluta ◽  
Joseph K. Kirui ◽  
Rapela R. Maphanga

Titanium dioxide (TiO2) polymorphs have recently gained a lot of attention in dye-sensitized solar cells (DSSCs). The brookite polymorph, among other TiO2 polymorphs, is now becoming the focus of research in DSSC applications, despite the difficulties in obtaining it as a pure phase experimentally. The current theoretical study used different nonmetals (C, S and N) and (C-S, C-N and S-N) as dopants and co-dopants, respectively, to investigate the effects of mono-doping and co-doping on the electronic, structural, and optical structure properties of (210) TiO2 brookite surfaces, which is the most exposed surface of brookite. The results show that due to the narrowing of the band gap and the presence of impurity levels in the band gap, all mono-doped and co-doped TiO2 brookite (210) surfaces exhibit some redshift. In particular, the C-doped, and C-N co-doped TiO2 brookite (210) surfaces exhibit better absorption in the visible region of the electromagnetic spectrum in comparison to the pure, S-doped, N-doped, C-S co-doped and N-S co-doped TiO2 brookite (210) surfaces.


1989 ◽  
Vol 11 (4) ◽  
pp. 583-613 ◽  
Author(s):  
D. Guidotti ◽  
E. Hasan ◽  
H. J. Hovel ◽  
M. Albert
Keyword(s):  
Band Gap ◽  

2020 ◽  
Vol 104 ◽  
pp. 109844 ◽  
Author(s):  
Majid Jahdi ◽  
Shivani B. Mishra ◽  
Edward N. Nxumalo ◽  
Sabelo D. Mhlanga ◽  
Ajay K. Mishra

2015 ◽  
Vol 68 (7) ◽  
pp. 1129 ◽  
Author(s):  
Pei Wen Koh ◽  
Leny Yuliati ◽  
Hendrik O. Lintang ◽  
Siew Ling Lee

The amount of rutile phase in chromium-doped titania photocatalyst was controlled by varying stirring time (0.5–2.0 h) at room temperature during a sol–gel synthesis process. The percentage of rutile phase increased from 15.1 % to 28.6 % when stirring time was prolonged from 0.5 to 1.5 h. Further increases in the stirring time had negligible effect on the rutile phase amount. As evidenced by analyses using diffuse reflectance ultraviolet–visible spectroscopy and X-ray photoelectron spectroscopy, a sufficient stirring time was important for more substitution of Cr3+ for Ti4+ in the lattice, resulting in anatase-to-rutile phase transformation. The formation of more rutile phase in Cr-doped TiO2 not only reduced the band gap energy, but also induced surface defects that retarded electron–hole recombination. It has been demonstrated that the Cr-doped TiO2 prepared with a stirring time of 1.5 h possessed the lowest band gap energy of 1.89 eV, and hence it achieved the highest photodegradation of methylene blue under visible light irradiation.


2013 ◽  
Vol 571 ◽  
pp. 49-53 ◽  
Author(s):  
T. Aguilar ◽  
J. Navas ◽  
R. Alcántara ◽  
C. Fernández-Lorenzo ◽  
J.J. Gallardo ◽  
...  

2014 ◽  
Vol 38 ◽  
pp. 278-285 ◽  
Author(s):  
Alamgir ◽  
Wasi Khan ◽  
Shabbir Ahmad ◽  
M. Mehedi Hassan ◽  
A.H. Naqvi

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