2017
DOI: 10.1088/2053-1591/aa90af
|View full text |Cite
|
Sign up to set email alerts
|

DFT investigation on electronic, magnetic, mechanical and thermodynamic properties under pressure of some EuMO3(M  =  Ga, In) perovskites

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

1
23
0

Year Published

2020
2020
2023
2023

Publication Types

Select...
5
1

Relationship

0
6

Authors

Journals

citations
Cited by 58 publications
(24 citation statements)
references
References 37 publications
1
23
0
Order By: Relevance
“…12 The alterations in the ratio or replacement of constituent cations and anions in the basic structure of perovskites AMX 3 alter their optoelectronic and magneto electronic properties 13 by resultingA 2 MX 6, 12 AMX 3 14 and A 2 BMX 6 15 like compounds (where, A, B and M are cations, and X is anion). Among the resulting compounds, some are halfmetallic [16][17][18][19][20][21][22][23][24] ferromagnetic having excellent physical properties. These have 100% spin polarization at Fermi level, as; they are metallic in one spin state and insulating or semiconducting in other spin state.…”
Section: Introductionmentioning
confidence: 99%
“…12 The alterations in the ratio or replacement of constituent cations and anions in the basic structure of perovskites AMX 3 alter their optoelectronic and magneto electronic properties 13 by resultingA 2 MX 6, 12 AMX 3 14 and A 2 BMX 6 15 like compounds (where, A, B and M are cations, and X is anion). Among the resulting compounds, some are halfmetallic [16][17][18][19][20][21][22][23][24] ferromagnetic having excellent physical properties. These have 100% spin polarization at Fermi level, as; they are metallic in one spin state and insulating or semiconducting in other spin state.…”
Section: Introductionmentioning
confidence: 99%
“…To deal with the electrons of d‐ states in Ta atom, the Hubbard parameter ( U = U eff ̶ J ) was also added to GGA (GGA + U ). [ 13 ] The value of J (on‐site exchange term) was selected as 0, where U eff was found to be optimized at 3.5 eV. For this value of U , the Rb 2 TaZ 6 (Z = Cl, Br) compounds were found stable in both spin configurations.…”
Section: Computational Methodologymentioning
confidence: 99%
“…Half‐metallic ferromagnets that fall under the category of spin‐polarized materials have zero band gap in one spin state and a nonzero band gap in the opposite spin state. Since the prediction of half‐metallic character in PtMnSb and NiMnSb, [ 7 ] many experimental and theoretical studies confirmed half‐metallic behavior in other materials, such as metal oxides CrO 2 [ 8 ] and Fe 3 O 4 ; [ 9 ] full‐Heusler alloys Co 2 FeSi [ 10 ] and Co 2 MnSi; [ 11 ] perovskites and their alloys BaCfO 3 , [ 12 ] Eu(Ga, In)O 3 , [ 13 ] BaNpO 3 , [ 14 ] EuRhO 3 , [ 15 ] La 1‐ x Sr x O 3 , [ 3 ] and La 0.7 Sr 0.3 MnO 3 ; [ 16 ] double perovskites Sr 2 FeMoO 6 , [ 17 ] and La 2 NbMnO 4 ; [ 18 ] Cr‐doped BeTe and BeSe; [ 19,20 ] transition metal‐doped pinctides and chalcogenides; [ 21 ] ; and Mn‐doped AlSb and GaN, [ 22,23 ] Al 1‐ x Cr x As, [ 24 ] and Zn 1‐ x Cr x Se. [ 25 ] However, most of them suffer from a number of drawbacks that hinder their efficient use in practical applications.…”
Section: Introductionmentioning
confidence: 99%
“…Poisson's ratio (ν) describes the nature of bonding forces. The upper and lower limits of Poisson's ratio are 0.25 and 0.50 [20][21][22][23][24]. The (ν) value varies from material to material.…”
Section: Elastic and Mechanical Propertiesmentioning
confidence: 99%
“…Perovskites with ABO 3 structure like BaPuO 3 , SrPuO 3 , BaAmO 3 , SrAmO 3 , EuGaO 3 , EuInO 3 etc. have been reported for spintronic applications [20][21][22][23][24]. Further materials like BaMoO 3 , SrMoO 3 , XReO 3 (X = Rb, Cs, Tl), SnTaO 3 , PbMoO 3 [25][26][27][28] have been recently reported for fuel cell applications.…”
Section: Introductionmentioning
confidence: 99%