2018
DOI: 10.1103/physrevb.97.214418
|View full text |Cite
|
Sign up to set email alerts
|

Nonswitchable polarization and magnetoelectric coupling in the high-pressure synthesized doubly ordered perovskites NaYMnWO6 and NaHoCoWO6

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

3
30
0

Year Published

2019
2019
2024
2024

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 28 publications
(33 citation statements)
references
References 38 publications
3
30
0
Order By: Relevance
“…This choice is driven by the fact that double perovskite systems mostlikely exhibit clear layered ordering as validated by experimental observations. [23,24] In addition, this specific cut-off energy difference also complies with previous DFT-based investigation [25] that reports formation of cation-ordered polar phases based on such criteria. The distribution of the compositional space as shown in Figure 2 represents a wide range of charge distributions of the cation sites.…”
Section: A Datasets and Descriptorssupporting
confidence: 87%
“…This choice is driven by the fact that double perovskite systems mostlikely exhibit clear layered ordering as validated by experimental observations. [23,24] In addition, this specific cut-off energy difference also complies with previous DFT-based investigation [25] that reports formation of cation-ordered polar phases based on such criteria. The distribution of the compositional space as shown in Figure 2 represents a wide range of charge distributions of the cation sites.…”
Section: A Datasets and Descriptorssupporting
confidence: 87%
“…These double double (or doubly ordered) perovskites usually combine layered and rock-salt motifs of A and B cations respectively. [10][11][12][13] A new double double perovskite (DDPv) type was recently reported to combine a columnar arrangement of A-site cations with the rock-salt order of B and B 0 cations for RMnMnSbO 6 (R = rare earth). 14,15 This structure crystallizes with the tetragonal P4 2 /n space group and has five independent cation sites according to the composition AA 0 0.5 A 00 0.5 BB 0 O 6 ; A (Wyckoff position 4e), A 0 (2a) and A 00 (2b) sites with ten-fold, tetrahedral and square planar coordinations, respectively, and octahedral sites for B (4c) and B 0 (4d) cations.…”
mentioning
confidence: 99%
“…This behavior is similar to that of other pyroelectric compounds, NaYMnWO 6 and NaHoCoWO 6 . 25 The magnetic structure of NaHoCoWO 6 and NaYCoWO 6 is collinear with a k-vector of ( 1 / 2 , 0, 1 / 2 ), and NaYMnWO 6 has a helical structure with a k-vector of (0, 0.427, 1 / 2 ). 29,44 These magnetic structures infer that the change in polarization in doubly ordered perovskites could be due to magnetoelastic coupling.…”
Section: Resultsmentioning
confidence: 98%
“…Recently, a nonswitchable polarization is observed below the magnetic ordering temperature (T N = 9 K for both Mn 2+ and Co 2+ ) of NaYMnWO 6 and NaHoCoWO 6 . 25 A similar family of compounds NaLnNiWO 6 (Ln = Y, Dy−Lu) showed switching of polarization below the magnetic ordering temperature of Ni 2+ ions (T N ∼ 20 to 23 K). The neutron diffraction studies of NaYNiWO 6 revealed a spin density wave structure just below T N and transforms to a collinear structure below 18 K. 26 On the other hand, the doubly ordered perovskites NaLnMnWO 6 (Ln = La, Nd, and Tb), NaLnFeWO 6 (Ln = La, Nd, Pr, and Sm), and NaLnNiWO 6 (Ln = La, Pr, Nd, and Sm−Tb) did not exhibit any change in polarization below magnetic ordering temperature.…”
Section: Introductionmentioning
confidence: 99%