2021
DOI: 10.1039/d1nr00374g
|View full text |Cite
|
Sign up to set email alerts
|

The CdTiO3/BaTiO3 superlattice interface from first principles

Abstract: LaAlO3/SrTiO3 (LAO/STO) interface has been studied extensively in the past decade which exhibits different properties from the constituent bulks. Using first-principles electronic structure calculations we investigate the CdTiO3/ BaTiO3 (CTO/BTO)...

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
3

Relationship

0
3

Authors

Journals

citations
Cited by 3 publications
(1 citation statement)
references
References 47 publications
0
1
0
Order By: Relevance
“…Furthermore, as shown in Table , although the earlier-reported FEPV materials, especially for conventional ABO 3 -type perovskite oxides and related heterostructures such as BiFeO 3 , BiFeO 3 /BaTiO 3 , Pb­[(Mg 1/3 Nb 2/3 ) 0.70 Ti 0.30 ]­O 3 , etc ., present pretty strong ferroelectric polarization, they generally have a much wider band gap than the optimal one (around 1.5 eV) predicted by the Shockley–Queisser limit, which is not conducive to the absorption of the solar spectrum, resulting in a pretty poor photoelectric conversion efficiency. TmFeO 3 and ASnX 3 (A = Cs, Rb; X = Br, I) are just the opposite. , Their ferroelectric polarizations are too weak to satisfy the application requirements.…”
Section: Results and Discussionmentioning
confidence: 99%
“…Furthermore, as shown in Table , although the earlier-reported FEPV materials, especially for conventional ABO 3 -type perovskite oxides and related heterostructures such as BiFeO 3 , BiFeO 3 /BaTiO 3 , Pb­[(Mg 1/3 Nb 2/3 ) 0.70 Ti 0.30 ]­O 3 , etc ., present pretty strong ferroelectric polarization, they generally have a much wider band gap than the optimal one (around 1.5 eV) predicted by the Shockley–Queisser limit, which is not conducive to the absorption of the solar spectrum, resulting in a pretty poor photoelectric conversion efficiency. TmFeO 3 and ASnX 3 (A = Cs, Rb; X = Br, I) are just the opposite. , Their ferroelectric polarizations are too weak to satisfy the application requirements.…”
Section: Results and Discussionmentioning
confidence: 99%