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

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

Open Access
|Apr 2016

Figures & Tables

Fig. 1.

Three crystalline structures of CoNiMnSi.

Fig. 2.

Calculated total energy versus volume for CoNiMnSi.

Table 1.

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-type5.633a212.8a4.68a
5.634bb226bb
5.639cc214cc4.674cc

a [4]

a [4]

a [4]

bb [25]

bb [25]

cc [26]

cc [26]

cc [26]

Table 2.

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
Co2MnSi311.16a164.75a153.26a
316bc174bc143bc

a [4]

a [4]

a [4]

b [27]

c [28]

b [27]

c [28]

b [27]

c [28]

Table 3.

Calculated longitudinal, transverse and average sound velocity (v1, vt, and vm, in ms1) 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
Fig. 3.

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.

Fig. 5.

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.

Table 4.

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
Co2MnSi5.00abcd

a [4]

b [25]

c [29]

d [26]

Table 5.

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
Co2MnSi928a100 %
985bc

a [4]

b [27]

c [28]

Fig. 7.

The antiferromagnetic (AFM) configuration of CoNiMnSi.

DOI: https://doi.org/10.1515/msp-2016-0011 | Journal eISSN: 2083-134X (formerly 2083-124X) | Journal ISSN: 2083-1331
Language: English
Page range: 85 - 93
Submitted on: May 29, 2015
Accepted on: Nov 18, 2015
Published on: Apr 27, 2016
Published by: Wroclaw University of Science and Technology
In partnership with: Paradigm Publishing Services

© 2016 M.H. Elahmar, H. Rached, D. Rached, S. Benalia, R. Khenata, Z.E. Biskri, S. Bin Omran, published by Wroclaw University of Science and Technology
This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 3.0 License.