Abstract:In this paper we shall study three binary alloy systems, one constituent of which is Mn. The other constituents are chosen from a particular column of the periodic table: Ni(3d), Pt (4d) and Pd (5d). As we go down the column, the d-bands become wider, discouraging spin-polarization. In a disordered alloy, the situation becomes more complicated, as the exchange interaction between two atoms is environment dependent. We shall compare and contrast their magnetic behaviour using robust electronic structure techniq… Show more
“…The main purpose of present study is to go more insight into the band structure and DOS and to find out the origin of magnetic moment. In our previous communication we have performed electronic and magnetic properties of binary and ternary alloys in their ordered (Pandey et al, 2014;Dahal et al, 2015;Lamichhane et al, 2016) as well as disordered (Pal et al, 2012;Kaphle et al, 2012;Kaphle et al, 2015) structures including perovskite (Lamichhane et al, 2014) indicating that TBLMTO approach is one of the effective model for the electronic structure problems. The other aim of present study is to use this approach for the analysis of electronic and magnetic behavior of full-Hustler alloy.…”
Heusler alloys have been of great interest because of their application in the field of modern technological applications. Electronic and magnetic properties of Co, Mn, Si and the Heusler alloy Co 2 MnSi have been studied using Density functional theory based Tight Binding Linear Muffin Tin Orbital with Atomic Sphere Approximation (TB-LMTO-ASA) approach. From the calculation lattice parameter of optimized structure of Co, Mn, Si and Co 2 MnSi are found to be 2.52Å, 3.49Å, 5.50Å, 5.53Å respectively. Band structure calculations show that Co and Mn are metallic, Si as semi-conducting while the Heusler alloy Co 2 MnSi as half-metallic in nature with band gap 0.29eV. The charge density plot indicates major bonds in Co 2 MnSi are ionic in nature. Magnetic property has been studied using the density of states (DOS), indicating that Co and Co 2 MnSi are magnetic with magnetic moments 2.85µ B and 4.91µ B respectively. The contribution of orbital in band structure, DOS and magnetic moments are due to d-orbital of Co and Mn and little from s and porbital of Si in Co 2 MnSi alloy.
“…The main purpose of present study is to go more insight into the band structure and DOS and to find out the origin of magnetic moment. In our previous communication we have performed electronic and magnetic properties of binary and ternary alloys in their ordered (Pandey et al, 2014;Dahal et al, 2015;Lamichhane et al, 2016) as well as disordered (Pal et al, 2012;Kaphle et al, 2012;Kaphle et al, 2015) structures including perovskite (Lamichhane et al, 2014) indicating that TBLMTO approach is one of the effective model for the electronic structure problems. The other aim of present study is to use this approach for the analysis of electronic and magnetic behavior of full-Hustler alloy.…”
Heusler alloys have been of great interest because of their application in the field of modern technological applications. Electronic and magnetic properties of Co, Mn, Si and the Heusler alloy Co 2 MnSi have been studied using Density functional theory based Tight Binding Linear Muffin Tin Orbital with Atomic Sphere Approximation (TB-LMTO-ASA) approach. From the calculation lattice parameter of optimized structure of Co, Mn, Si and Co 2 MnSi are found to be 2.52Å, 3.49Å, 5.50Å, 5.53Å respectively. Band structure calculations show that Co and Mn are metallic, Si as semi-conducting while the Heusler alloy Co 2 MnSi as half-metallic in nature with band gap 0.29eV. The charge density plot indicates major bonds in Co 2 MnSi are ionic in nature. Magnetic property has been studied using the density of states (DOS), indicating that Co and Co 2 MnSi are magnetic with magnetic moments 2.85µ B and 4.91µ B respectively. The contribution of orbital in band structure, DOS and magnetic moments are due to d-orbital of Co and Mn and little from s and porbital of Si in Co 2 MnSi alloy.
“…We believe that present work will assist to guide the scope of finding SGS, among LiMgPdSn-type quaternary Heusler compounds having 26 (or 28) valence electrons in the future. Number of works have been carried out using TBLMTO-ASA approach in ordered binary alloys [13][14], disordered alloys [15], perovskites [16][17] and Heusler alloys [18]. The other motivation or aim is to use TBLMTO-ASA approach on quaternary alloys.…”
We study the structural, electronic and magnetic properties of Co-based LiMgPdSn-types of quaternary Heusler compounds (CoFeCrAl, CoFeTiAs, CoFeCrGa, and CoMnVAS) using Density Functional Theory (DFT) implemented on Tight Binding Linear Muffin-Tin Orbital within Atomic Sphere Approximation (TB-LMTO-ASA) Code. The optimized value of lattice parameter for CoFeCrAl, CoFeTiAs, CoFeCrGa and CoMnVAs are found to be 5.61A˚, 5.76 A˚, 5.61A˚ and 5.71A˚ , respectively. From the calculation of electronic band structure and spin polarized total density of states (DOS), we found that CoFeCrAl and CoFeCrGa are spin-gapless semiconductors with halfmetallic gap of 0.82eV and 0.25eV respectively. CoFeTiAs half-metal (Nearly spin-gapless semiconductor) with half-metallic gap of 0.38 eV, and CoMnVAs is found to be nearly gapless halfmetal. Magnetic moment of these compounds almost obey the Slater-Pauling rules. All these compounds expected to have high curie temperature which makes them significant for spintroincs/magnetoelectroincs applications.
“…The main purpose of present study is to go more insight into the band structure and DOS and to find out the origin of magnetic moment. In our previous communication we have performed electronic and magnetic properties of binary and ternary alloys in their ordered [8,9,10 ] as well as disordered [11,12,13] structures including perovskite [14] indicating that TBLMTO approach, one of the effective model for the electronic structure problems. The other aim of present study to use this approach for the analysis of electronic and magnetic behavior of full-Hustler alloy.…”
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