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The effect of antisite disorder on magnetic and magnetocaloric properties of Ni-Co-Mn-In alloys: ab initio and Monte Carlo studies

机译:抗烧伤紊乱对Ni-Co-Mn合金磁性性能的影响:AB Initio和Monte Carlo研究

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Nowadays, the Ni-Co-Mn-In Heusler alloys have drawn a much attention due to a series of functional properties such as the shape memory effect, giant magnetoresistance and magnetocaloric effects etc., which are promising for future technologies [1]-[3]. Usually, the most of unique properties are associated with the martensitic transformation between the martensite with complex magnetic order and the austenite with ferromagnetic order. Moreover, there are strong competing magnetic interactions in the vicinity of magnetostructural phase transition, which are responsible for the change in magnetization. Evidently, the manipulation of magnetic interactions in both martensite and austenite leads to change the magnitude of the magnetization drop and to achieve the better magnetocaloric properties across the martensitic transformation. The present theoretical study is addressed the question of effect of competing magnetic interactions on magnetic and magnetocaloric properties of Ni-Co-Mn-In alloys through the addition of structural defects. Evidently, samples prepared experimentally without an additional annealing can contain many impurities and defects. Opposite, the influence of additional annealing can result to a highly ordered structure with minimum defect concentration. In this connection for compositions without additional annealing, we focused attention on the formation of structural (antisite) disorder between In and Mn atoms on the corresponding In and Mn sublattices with concentration y which can be described by Ni2 Mn1+x In1-x = Ni2Mn1-ySnyMnx+y In1-x-y, where x is the Mn excess concentration and y is the degree of antisite disorder) [4]. While for the samples upon additional annealing, the ordered structure (without defects, y = 0 is proposed. Our methodology consists of ab initio calculations and Monte Carlo (MC) simulations based on the Potts-Blume-Emery-Griffiths model allowing to simulate austenite-martensite transformation as well as magnetic and magnetocaloric properties [5]-[7]. Two subsequent steps were used in our calculations. Firstly, we calculated the exchange coupling constants (Jij) using the SPR-KKR package [8] within the general gradient approximation in the form of Perdew-Burke-Ernzerhof. The chemical and structural disorders were simulated in the coherent potential approximation. The Jij calculations were done for cubic austenite (c/a = 1) and tetragonal martensite (c/a = 1.21) of Ni43 Co7 Mn37+y In13-y. Here, y takes values as follows: 1.5, 3.25, and 6.5. We note that the equilibrium lattice parameters for austenite and martensite were taken from our previous calculations (See Ref. [7]), an
机译:如今,Ni-Co-Mn-In Heusler合金由于一系列功能性质,例如形状记忆效应,巨型磁阻和磁热效应等,这是非常重要的,这对未来技术有前途[1] - [ 3]。通常,最大的独特性质与马氏体之间的马氏体转化与具有复合磁秩序的马氏体和铁磁序列的奥氏体相关联。此外,在磁性结构相变附近存在强大的竞争磁相互作用,其负责磁化的变化。显然,在马氏体和奥氏体中的磁相互作用的操纵导致改变磁化下降的大小,并在马氏体转化中实现更好的磁热性能。本理论研究通过添加结构缺陷解决了通过添加结构缺陷来解决竞争磁性相互作用对Ni-Co-Mn-In合金的磁性和磁热性性质的影响问题。显然,没有额外退火的实验制备的样品可以含有许多杂质和缺陷。相反,额外退火的影响可能导致高度有序的结构,具有最小缺陷浓度。在这种情况下,对于没有额外退火的组合物,我们将注意力集中在与浓度Y描述的相应的和Mn子组中的结构(Antisite)紊乱的形成,其可以通过Ni描述 2 m 1 + x 1-x = NI. 2 m 1-y y m x + y 1-x-y ,其中x是Mn过量浓度,y是反烧结障碍的程度)[4]。在额外退火时的样品,提出有序结构(没有缺陷,y = 0。我们的方法包括基于Potts-Blume-Emery-Griffiths模型的AB Initio计算和Monte Carlo(MC)模拟,允许模拟奥氏体模拟 - 矿物转化以及磁性和磁热性质[5] - [7]。在我们的计算中使用了两个后续步骤。首先,我们计算了交换耦合常数(J ij )使用SPR-KKR封装[8]在普通卷发-ERNZERHOF的形式中的一般梯度近似。在相干电位近似下模拟化学和结构障碍。为立方奥氏体(C / A = 1)和Ni的四方马氏体(C / A = 1.21)进行JIJ计算 43 CO. 7 m 37 + y 13-y 。这里,y采用如下:1.5,3.25和6.5。我们注意到,从我们以前的计算中取出了奥氏体和马氏体的平衡晶格参数(参见参考文献[7])

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