2020
DOI: 10.1063/5.0004530
|View full text |Cite
|
Sign up to set email alerts
|

Emergent behavior of LaNiO3 in short-periodic nickelate superlattices

Abstract: Heterostructure engineering provides an efficient way to obtain several emergent phases of LaNiO3, as demonstrated in recent studies. In this work, a new class of short-periodic superlattice, consisting of LaNiO3 and EuNiO3, has been grown by pulsed laser interval deposition to investigate the effect of structural symmetry mismatch on the electronic and magnetic behaviors. Using synchrotron-based soft and hard x-ray resonant scattering experiments, we have found that these heterostructures undergo simultaneous… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

1
15
0

Year Published

2020
2020
2023
2023

Publication Types

Select...
5
2

Relationship

4
3

Authors

Journals

citations
Cited by 11 publications
(17 citation statements)
references
References 60 publications
1
15
0
Order By: Relevance
“…81,170 The properties of perovskite rare-earth nickelates, RNiO 3 (R = La-Lu), have been attracting enormous attention owing to a rich temperature-composition phase diagram including a metal-to-insulator phase transition coinciding with a nickel charge ordering. 16,171,172 The origin of the metal-to-insulator transition has been widely debated in the literatures. [173][174][175][176] The unoccupied states at the bottom of the conduction band have substantial oxygen character, corresponding to an oxygen ligand hole consistent with a negative charge transfer character for the system.…”
Section: Metal-insulator Transitionsmentioning
confidence: 99%
“…81,170 The properties of perovskite rare-earth nickelates, RNiO 3 (R = La-Lu), have been attracting enormous attention owing to a rich temperature-composition phase diagram including a metal-to-insulator phase transition coinciding with a nickel charge ordering. 16,171,172 The origin of the metal-to-insulator transition has been widely debated in the literatures. [173][174][175][176] The unoccupied states at the bottom of the conduction band have substantial oxygen character, corresponding to an oxygen ligand hole consistent with a negative charge transfer character for the system.…”
Section: Metal-insulator Transitionsmentioning
confidence: 99%
“…Since RENiO 3 members have a strong tendency to retain their bulk-like symmetry even in thin-film form [80], a strong structural competition is anticipated at the interface between LNO and other members of RENiO 3 . This effect has been indeed observed in ultrathin n uc EuNiO 3 /m uc LaNiO 3 [nENO/mLNO] superlattices (here uc is unit cell in pseudocubic notation, n and m =1, 2) [78,[81][82][83]. The 1ENO/2LNO SL having rhombohedral symmetry remains metallic, whereas the superlattices with n ≥ m have orthorhombic/monoclinic symmetry and exhibit first-order MIT as a function of temperature.…”
Section: Emergent Phases Of Renio3 Through Octahedral Engineeringmentioning
confidence: 66%
“…The competition between interfacial unit cell and bulk-like unit cells were further investigated by growing nENO/nLNO SLs (Fig. 2(a)) [77,78]. The SL with n=8 uc remains metallic, similar to bulk LNO, whereas all short periodic SLs exhibit simultaneous MIT and antiferromagnetic transition (Fig.…”
Section: Emergent Phases Of Renio3 Through Octahedral Engineeringmentioning
confidence: 99%
“…The tremendous advancement in thin film growth technologies over the last two decades have enabled the research community to grow artificial structures of these complex oxides with unit cell precision [5][6][7][8][9][10][11]. Such heterostructuring [9,[12][13][14][15][16][17][18][19][20][21][22][23][24][25] leads to subtle modifications in spin, charge, orbital, and lattice sectors at the interface, resulting in a variety of emergent magnetic behaviors such as interfacial ferromagnetism, exchange bias, spin spiral magnetic phase, enhanced magnetic ordering temperature, topological Hall effect (THE), etc. THE arises in materials with non-zero scalar spin chirality [𝜒 𝑖,𝑗,𝑘 = 𝑺 𝒊 .…”
Section: Introductionmentioning
confidence: 99%