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Lanthanum Doping into A-sites of BaBiO3 via Thin Film Synthesis
BaBiO 3 is an insulator with perovskite structure. While the hole doping of BaBiO 3 has been achieved long ago, its electron doping has not been realized yet because trivalent La ions, for example, tend to substitute for tetravalent Bi ions in B sites rather than divalent Ba ions in A-sites. We have...
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Published in: | Journal of the Korean Physical Society 2020, 76(3), , pp.215-220 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | BaBiO
3
is an insulator with perovskite structure. While the hole doping of BaBiO
3
has been achieved long ago, its electron doping has not been realized yet because trivalent La ions, for example, tend to substitute for tetravalent Bi ions in B sites rather than divalent Ba ions in A-sites. We have used thin film synthesis to substitute La ions for Ba ions in BaBiO
3
; we first deposit, on a substrate, a buffer layer of BaBiO
3
to overcome the lattice mismatch and then deposit a triple unit of a monolayer of Ba-deficit BaBiO
3
, the necessary amount of La
2
O
3
to fill in the A-site vacancies, and lastly a monolayer of pure BaBiO
3
. This triple unit of Ba-deficit Ba
1−
x
BiO
3
/La
2
O
3
/pure BaBiO
3
is repeated several times for a certain thickness sample, and then the whole structure is treated thermally at 550 °C. Scanning TEM image analysis confirms that La ions go indeed to the A-sites and La doped BaBiO
3
remains in perovskite structure. It is found that La substitution for Ba in BaBiO
3
causes the Raman peak related to the breathing mode of BaBiO
3
to decrease in intensity as a function of the doping level. Dielectric measurements of La doped BaBiO
3
also reveal an upward shift in temperature and associated relaxation behaviors for the octahedral tilt-driven structural transition which occurs at
T
c
∼ 140 K for pure BaBiO
3
. |
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ISSN: | 0374-4884 1976-8524 |
DOI: | 10.3938/jkps.76.215 |