2020
DOI: 10.1002/er.6339
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First‐principles study ofCs2Ti1−xMxBr6(M = Pb, Sn) and numerical simulation of the solar cells based onCs2Ti0.25Sn0.75Br6perovskite

Abstract: The impact of partial substitution by replacing 'Ti' atom with Pb and Sn respectively in vacancy ordered perovskites Cs 2 Ti 1−x M x Br 6 (M = Pb, Sn) has been studied using density functional theory calculations. Our results indicate the unexpected presence of intermediate bands (IBs) in the forbidden gap of electronic structure for lead substituted compounds (x = 0.25, 0.5, 0.75) Cs 2 Ti 1 −x Pb x Br 6. These IBs located above the valence band could be tuned from 0.60 to 0.45 eV with appropriate Pb doping pe… Show more

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Cited by 6 publications
(4 citation statements)
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“…[ 44 ] In achieving an ideal bandgap while catering to the high and indirect bandgap issue of Cs 2 TiBr 6 , Ti can partially be replaced with another cation. Through DFT calculations (VASP), Shrivastava et al studied the impact of partial substitution of the Ti atom with other cations, specifically Sn and Pb, resulting in compounds with a chemical formula Cs 2 Ti 1– x M x Br 6 [ 45 ] where M = Sn and Pb. Pb substitution or doping will not be reviewed here.…”
Section: Optical Propertiesmentioning
confidence: 99%
See 1 more Smart Citation
“…[ 44 ] In achieving an ideal bandgap while catering to the high and indirect bandgap issue of Cs 2 TiBr 6 , Ti can partially be replaced with another cation. Through DFT calculations (VASP), Shrivastava et al studied the impact of partial substitution of the Ti atom with other cations, specifically Sn and Pb, resulting in compounds with a chemical formula Cs 2 Ti 1– x M x Br 6 [ 45 ] where M = Sn and Pb. Pb substitution or doping will not be reviewed here.…”
Section: Optical Propertiesmentioning
confidence: 99%
“…The structure is derived from conventional perovskites by doubling the ABX 3 unit cell along all three crystallographic axes and removing every other B-site cation to form a face-centered lattice of isolated BX 6 octahedral units bridged by A-site cations in the void (vacancy-ordered DHPs). [18,19] The absence of one B-site cation in the double perovskite A 2 B 2 X 6 yields the vacancy-ordered double perovskite structure, [20] as illustrated in the schematic diagram in Figure 2. The A 2 BX 6 structure shows similar features to ABX 3 perovskites, mostly of cubic structures.…”
Section: Introductionmentioning
confidence: 99%
“…It is well known that perovskites based on mixed halides and metal cations offer a wide range of tunability in their optoelectronic properties including absorption, and photoluminescence (PL). [47,48] In this work, mixed halide tunability of Cs 2 PtCl 6Àx Br x by anion exchange technique using bromide salt solutions was investigated. The Cs 2 PtCl 6 is mixed with 1.5 M LiBr solution and the anion exchange studies were carried out over a period of time.…”
Section: Resultsmentioning
confidence: 99%
“…It is well known that perovskites based on mixed halides and metal cations offer a wide range of tunability in their optoelectronic properties including absorption, and photoluminescence (PL). [ 47,48 ]…”
Section: Resultsmentioning
confidence: 99%