Magnetic and thermoelectric properties of Co2MnT (T = Ga, Si) Heusler compounds
Introduction
Co-based Heusler alloys have been studied as ferromagnetic shape memory alloys (FSMAs), and their development as smart materials is generating strong interest [[1], [2], [3], [4], [5], [6], [7]]. Unlike the case of conventional shape memory alloys (SMAs) such as Ti–Ni alloys, the martensite variant rearrangement is induced by an applied magnetic field [[8], [9], [10]]. The response time of the shape changes accompanying magnetically controlled martensitic transformation in the FSMAs is therefore much faster than that of the shape changes accompanying thermally controlled martensitic transformation in the SMAs. It has been reported that Co-based Heusler alloys show half-metallic properties, making them attractive candidates for application to spin-polarized current devices [[11], [12], [13]]. Thus, the magnetic properties of Co-based Heusler alloys have been intensively studied in recent years.
Since the Fe2VAl Heusler alloy was reported to have exhibited attractive thermoelectric properties, the Heusler alloys have been both theoretically and experimentally studied as thermoelectric materials [[14], [15], [16], [17], [18]]. Co-based Heusler alloys are also possible thermoelectric materials, but they have mainly been studied as FSMAs and half-metallic materials [[19], [20], [21], [22]]. In this study, the thermoelectric properties of two typical Co-based Heusler alloys, Co2MnGa and Co2MnSi, were investigated [23,24]. As mentioned above, Co-based Heusler alloys are ferromagnetic. Therefore, both the magnetic and thermoelectric properties of these two Co-based Heusler alloys were investigated.
Section snippets
Experiment
Co2MnGa and Co2MnSi alloys were prepared by subjecting small ingots of Co (99.9 wt%), Mn (99.9 wt%), Ga (99.9 wt%), and Si (99.9 wt%) to induction melting. Small amounts of the alloy ingots were placed in a quartz crucible with an orifice of 0.6 mm at the bottom. The ingots were induction melted in an argon atmosphere and then ejected through the orifice with argon gas into a copper mold with a cavity of 3 mm in diameter and 50 mm in length. The cast specimens were annealed at 1073 K for 24 h
Results and discussion
In this study, we investigated the properties of Co2MnGa and Co2MnSi Heusler compounds produced by mold casting and subsequent annealing. Fig. 1 shows the XRD diffraction patterns of the Co2MnGa and Co2MnSi alloy ingots. It was found that the specimens were basically composed of the Heusler structure (L 21 structure).
The order of Heusler alloys is a significant determinant for their properties. Thus, the structures of the Co2MnGa and Co2MnSi specimens were further studied by TEM. Fig. 2 shows
Conclusion
It was found that the Co2MnGa Heusler phase transformed into the B2-type phase at 1200 K, whereas the Co2MnSi Heusler phase was stable up to the melting temperature of 1450 K. The magnetic measurements revealed that the Co2MnSi Heusler compound is a superior ferromagnetic material to the Co2MnGa Heusler compound. The Co2MnSi Heusler compound exhibited a saturation magnetization of 130 emu/g and a Curie temperature of 1015 K, both of which were higher than those of the Co2MnGa Heusler compound.
Data availability
The data required to reproduce these findings cannot be shared at this time as the data also form part of an ongoing study.
Declaration of competing interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgment
This work was performed using the facilities of the Institute for Solid State Physics, The University of Tokyo.
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2022, Results in PhysicsCitation Excerpt :Heusler alloys have been widely concerned by researchers due to its potential applications in many important fields [1–24]. As the most representative Co-based Heusler, it has also become a research hotspot because of their 100% spin polarization and high Curie temperatures [25–34]. High spin polarization is a typical feature of half-metallic (HM) ferromagnets and spin gapless semiconductors [35–40].