2020
DOI: 10.1038/s41467-020-16101-2
|View full text |Cite
|
Sign up to set email alerts
|

Nanoengineering room temperature ferroelectricity into orthorhombic SmMnO3 films

Abstract: Orthorhombic RMnO 3 (R = rare-earth cation) compounds are type-II multiferroics induced by inversion-symmetry-breaking of spin order. They hold promise for magneto-electric devices. However, no spontaneous room-temperature ferroic property has been observed to date in orthorhombic RMnO 3. Here, using 3D straining in nanocomposite films of (SmMnO 3) 0.5 ((Bi,Sm) 2 O 3) 0.5 , we demonstrate room temperature ferroelectricity and ferromagnetism with T C,FM~9 0 K, matching exactly with theoretical predictions for t… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
5

Citation Types

3
19
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
9

Relationship

1
8

Authors

Journals

citations
Cited by 23 publications
(22 citation statements)
references
References 39 publications
3
19
0
Order By: Relevance
“…2A, a remanent polarization P r [= (P r + −P r − )/2] of 4.14 C/cm 2 is achieved in this SmFeO 3− film at RT. This is two orders of magnitude higher than that of its bulk (19,29) and larger than that achieved in stoichiometric SFO epitaxial films in previous studies (30)(31)(32)(33), as well as the record of 1.95 C/cm 2 for the o-REMO 3 systems (34). This ferroelectricity was double-confirmed by the positive-up-negative-down (PUND) method, which is more accurate than the polarization-electric field (P-E) hysteresis loops because it can exclude the possible contribution from nonferroelectric artifacts.…”
Section: Resultsmentioning
confidence: 51%
“…2A, a remanent polarization P r [= (P r + −P r − )/2] of 4.14 C/cm 2 is achieved in this SmFeO 3− film at RT. This is two orders of magnitude higher than that of its bulk (19,29) and larger than that achieved in stoichiometric SFO epitaxial films in previous studies (30)(31)(32)(33), as well as the record of 1.95 C/cm 2 for the o-REMO 3 systems (34). This ferroelectricity was double-confirmed by the positive-up-negative-down (PUND) method, which is more accurate than the polarization-electric field (P-E) hysteresis loops because it can exclude the possible contribution from nonferroelectric artifacts.…”
Section: Resultsmentioning
confidence: 51%
“…By extension, DMO epitaxially aligns with DSB with the same 45 relationship, as seen in other REMnO 3 phases. [21][22][23] This is also expected as DMO has the GdFeO 3 perovskite structure.…”
Section: Resultsmentioning
confidence: 54%
“…24 These observations are similar to previously reported (SmMnO 3 ) 0.5 ((-Bi,Sm) 2 O 3 ) 0.5 VAN lms. 21 In our lm, the DMO matrix plays an important role in stabilising the cubic DSB phase; the strained DMO and DSB have a $2% lattice mismatch. Thus, the strained DMO matrix acts as scaffold to stabilise and promote the formation of cubic DSB nanopillars.…”
Section: Resultsmentioning
confidence: 92%
“… 41 In another recent study, in orthorhombic R MnO 3 ( R = rare-earth cation) perovskites, specifically SmMnO 3 that is reported have room-temperature ferroelectricity prepared by nano-engineering room temperature, ferroelectricity has been found due to a spin-driven mechanism. 42 , 43 We report the room-temperature ferroelectricity with a negligible leakage current in GdFeO 3 nanoparticles for the first time to the best our knowledge, which possess wide applications.…”
Section: Resultsmentioning
confidence: 82%