Magnetic Properties of the Double Perovskite Bi2FeCrO6

Idrissi, S.; Labrim, H.; Ziti, S.; Khalladi, R.; Mekkaoui, N. El; Housni, I. El; Mtougui, S.; Bahmad, L.

doi:10.1007/s11664-019-07110-z

“…41 Technologically, the capability to adjust the magnetic properties of these materials by using an applied electric field received special attention for electronic devices with low energy consumption. 42,43 Furthermore, Sr 2 MMoO 6 double-perovskite molybdates (M = Ni, Mg, and Fe) exhibit an interesting electrochemical performance leading to their use as an anode material for solid oxide fuel cells. [44][45][46][47] On the other hand, further studies have been performed on double-perovskite oxides containing cobalt.…”

Section: Introductionmentioning

confidence: 99%

Crystallography at non-ambient conditions and physical properties of the synthesized double perovskites, Sr₂(Co_1−xFe_x)TeO₆

Zaraq

¹

,

Orayech²,

Igartua

³

et al. 2023

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“…[ 24 ] Moreover, the Monte Carlo study has been conducted to underline the critical behavior of several double perovskites including: Sr 2 VMoO 6 , [ 25 ] Sr 2 CrIrO 6 , [ 26 ] Ba 2 NiUO 6 , [ 27 ] Sr 2 RuHoO 6 , [ 28 ] Lu 2 MnCoO 6 , [ 29 ] and Bi 2 FeCrO 6 . [ 30 ]…”

Section: Introductionmentioning

confidence: 99%

“…[24] Moreover, the Monte Carlo study has been conducted to underline the critical behavior of several double perovskites including: Sr 2 VMoO 6 , [25] Sr 2 CrIrO 6 , [26] Ba 2 NiUO 6 , [27] Sr 2 RuHoO 6 , [28] Lu 2 MnCoO 6 , [29] and Bi 2 FeCrO 6 . [30] As far as we know, no theoretical or experimental research has been done to date on the physical properties of the ScBiTe 3 . Therefore, in this paper, the structural, electronic, optical, and thermoelectric characteristics have been studied.…”

Section: Introductionmentioning

confidence: 99%

Biaxial and Uniaxial Tensile Strains Effects on Electronic, Optical, and Thermoelectric Properties of ScBiTe₃ Compound

Benyoussef,

Jabar,

Bahmad

2023

Cryst. Res. Technol.

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Using first‐principles density‐functional theory (DFT), this study thoroughly investigates the effects of biaxial and uniaxial tensile strains on the electronic, optical, and thermoelectric properties of the perovskite ScBiTe3. This latter compound is a semiconductor material, according to its electronic band structures, with an indirect bandgap value of 0.891 eV. Additionally, the bandgap of each structure exhibits a decreasing tendency under compressive strain and an increasing trend under tensile strain, and the bandgap changes from indirect to direct bandgap when the tensile strain is applied along the a and b directions. Due to their band properties, these materials have excellent absorption ability in the visible region, as evidenced by optical properties like dielectric functions, absorption coefficients, and electron loss functions. It is found that the highest value of the power factor (PF) is 4.1 × 1011 W−1K−2s−1 and the highest value of the figure of merit (ZT) is 0.84. Such values are obtained for the specific strain value of 10% strain along the “a” and “b” directions. This confirms that this material can be a potential candidate for thermoelectric device applications.

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“…The anomalies possess unusual transport and magnetic properties that emphasize the strong interplay of spin, charge, and orbital degrees of freedom. In some of our recent works, [14][15][16][17][18][19][20][21][22][23] we have provided the magnetic behavior and phase diagrams using Monte Carlo simulations for the perovskite BiFeO 3 , also we have presented and discussed the corresponding hysteresis cycles.…”

Section: Introductionmentioning

confidence: 99%

Magnetic properties of the double perovskite compound Sr₂YRuO₆

Mekkaoui¹,

Idrissi²,

Mtougui³

et al. 2019

Chinese Phys. B

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We study the magnetic properties of the double perovskite ruthenate compound Sr2YRuO6 using Monte Carlo simulations (MCS). We elaborate the ground state phase diagrams for all possible and stable configurations. The magnetizations and the susceptibilities as a function of temperature for the studied system are also reported. The effects of the exchange coupling interactions and the crystal field are examined and discussed. On the other hand, since the compound Sr2YRuO6 exhibits an antiferromagnetic behavior, we find its Néel temperature, T N ≈ 31 K , which is in good agreement with the experimental results in the literature. To complete this study, the hysteresis loops and the coercive field as a function of the external magnetic field are also obtained for fixed values of the physical parameters.

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Magnetic Properties of the Double Perovskite Bi2FeCrO6

Cited by 31 publications

References 43 publications

Crystallography at non-ambient conditions and physical properties of the synthesized double perovskites, Sr₂(Co_1−xFe_x)TeO₆

Crystallography at non-ambient conditions and physical properties of the synthesized double perovskites, Sr₂(Co_1−xFe_x)TeO₆

Biaxial and Uniaxial Tensile Strains Effects on Electronic, Optical, and Thermoelectric Properties of ScBiTe₃ Compound

Magnetic properties of the double perovskite compound Sr₂YRuO₆

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Magnetic Properties of the Double Perovskite Bi2FeCrO6

Cited by 31 publications

References 43 publications

Crystallography at non-ambient conditions and physical properties of the synthesized double perovskites, Sr2(Co1−xFex)TeO6

Crystallography at non-ambient conditions and physical properties of the synthesized double perovskites, Sr2(Co1−xFex)TeO6

Biaxial and Uniaxial Tensile Strains Effects on Electronic, Optical, and Thermoelectric Properties of ScBiTe3 Compound

Magnetic properties of the double perovskite compound Sr2YRuO6

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Product

Resources

About

Crystallography at non-ambient conditions and physical properties of the synthesized double perovskites, Sr₂(Co_1−xFe_x)TeO₆

Crystallography at non-ambient conditions and physical properties of the synthesized double perovskites, Sr₂(Co_1−xFe_x)TeO₆

Biaxial and Uniaxial Tensile Strains Effects on Electronic, Optical, and Thermoelectric Properties of ScBiTe₃ Compound

Magnetic properties of the double perovskite compound Sr₂YRuO₆