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Structural stability, electronic structure and magnetic properties of the new hypothetical half-metallic ferromagnetic full-Heusler alloy CoNiMnSi


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Fig. 1.

Three crystalline structures of CoNiMnSi.
Three crystalline structures of CoNiMnSi.

Fig. 2.

Calculated total energy versus volume for CoNiMnSi.
Calculated total energy versus volume for CoNiMnSi.

Fig. 3.

Total and partial densities of states (TDOS, PDOS) for CoNiMnSi in its stable structure types calculated using the GGA approximation.
Total and partial densities of states (TDOS, PDOS) for CoNiMnSi in its stable structure types calculated using the GGA approximation.

Fig. 4.

Total and partial densities of states (TDOS, PDOS) for CoNiMnSi in its stable structure types calculated using the GGA + U approximation.
Total and partial densities of states (TDOS, PDOS) for CoNiMnSi in its stable structure types calculated using the GGA + U approximation.

Fig. 5.

Charge density distribution in the (1 1 0) plane of the CoNiMnSi quaternary Heusler compound calculated using the GGA approximation.
Charge density distribution in the (1 1 0) plane of the CoNiMnSi quaternary Heusler compound calculated using the GGA approximation.

Fig. 6.

Charge density distribution in the (1 1 0) plane of the CoNiMnSi quaternary Heusler compound calculated using the GGA + U approximation.
Charge density distribution in the (1 1 0) plane of the CoNiMnSi quaternary Heusler compound calculated using the GGA + U approximation.

Fig. 7.

The antiferromagnetic (AFM) configuration of CoNiMnSi.
The antiferromagnetic (AFM) configuration of CoNiMnSi.

Calculated single crystal elastic constants Cij (GPa), polycrystalline elastic modulus (GPa), shear modulus G (GPa), Young’s modulus E (GPa), Poisson’s ratio ν and shear anisotropic factor A for the CoNiMnSi compound.

MaterialC11C12C44GEνA
CoNiMnSi425.7568.52172.49174.94400.370.1440.966
Co2MnSi311.16

[4]

164.75

[4]

153.26

[4]

316

[27]

[28]

174

[27]

[28]

143

[27]

[28]

Calculated equilibrium lattice parameters a0 (Å), bulk modulus B0 (GPa), its pressure derivative B′0 (GPa) and equilibrium energy E0 (Ryd) for the CoNiMnSi compound in the different structures considered in this work.

MaterialStructurea0(Å)B0 (GPa)B′E0 (Ryd)
CoNiMnSiHg2CuTi-type5.6256179.513.50−8726.0826
Cu2MnAl-type5.6810187.895.06−8726.1164
LiMgPbSb-type5.6787187.64.81−8726.1177
Co2MnSiCu2MnAl-type5.633

[4]

212.8

[4]

4.68

[4]

5.634

[25]

226

[25]

5.639

[26]

214

[26]

4.674

[26]

Calculated spin-polarization, exchange energy (∆E(FM−AFM), and Curie temperature (Tc).

Compounds∆E(FM–AFM) (mRy/Atom)TC (K)Spin polarization ratio (%)
CoNiMnSi−0.011871.89 GGA56 % GGA
1107.19 GGA + U100 % GGA+U
Co2MnSi928

[4]

100 %
985

[27]

[28]

Calculated longitudinal, transverse and average sound velocity (v1, vt, and vm, in ms−1) and Debye temperature (θD, K) for the CoNiMnSi compound.

(T = 0) MaterialVSV1VmθD
(P = 0)[m/s][m/s][m/s][K]
CoNiMnSi4902.707604.255381.81445.20

Total, interstitial and local magnetic moments.

CompoundsμTotal (μB/Cell)μinterstitialB/Cell)μatomic (μB/Cell)
Co1Ni/Co2MnSi
CoNiMnSiGGA4.690.0381.0360.4583.180.022 0.038
GGA+U5.99−0.033771.6130.5673.89
Co2MnSi5.00

[4]

[25]

[29]

[26]

eISSN:
2083-134X
Language:
English
Publication timeframe:
4 times per year
Journal Subjects:
Materials Sciences, other, Nanomaterials, Functional and Smart Materials, Materials Characterization and Properties