The magnetic properties and magnetocaloric effect in Mn1-xNixCoGe
dc.contributor.author | Ren, QY | en_AU |
dc.contributor.author | Hutchison, WD | en_AU |
dc.contributor.author | Wang, JL | en_AU |
dc.contributor.author | Studer, AJ | en_AU |
dc.contributor.author | Campbell, SJ | en_AU |
dc.date.accessioned | 2021-08-13T03:40:22Z | en_AU |
dc.date.available | 2021-08-13T03:40:22Z | en_AU |
dc.date.issued | 2015-02-03 | en_AU |
dc.date.statistics | 2021-08-12 | en_AU |
dc.description.abstract | MnCoGe-based compounds reveal promise for magnetic refrigeration and as such have been extensively investigated over the last decade [1]. Refrigeration based on magnetic cooling via the magnetocaloric effect offers potential as an alternative to conventional gas-compression systems. MoCoGe-based compounds have two crystallographic structures: nominally low temperature TiNiSi-type orthorhombic structure (Pnma) and the high temperature Ni2In-type hexagonal structure (P63/mmc). When the structural transition temperature between these two structures is ‘tuned’ between the respective Curie temperatures of the phases (~345 K for the orthorhombic phase and ~275 K for the hexagonal phase [1]), a magneto-structural transition can be obtained. Such a transition allows a direct change from the ferromagnetic orthorhombic phase to the paramagnetic hexagonal phase [1]. For a magneto-structural transition, the lattice and magnetic entropy changes occur simultaneously, thereby providing scope for observation of a large magnetocaloric effect [2]. The crystallographic structures and magnetic properties of annealed Mn1-xNixCoGe (x = 0.02, 0.03, 0.04, 0.05, 0.06 and 0.07) have been investigated using variable temperature X-ray diffraction and neutron diffraction (T = 5 - 320 K) with neutron diffraction measurements carried out both with and without applied magnetic fields for Mn0.95Ni0.05CoGe (B = 0 - 8 T). Such experiments allow separation of the structural and magnetic contributions to the total entropy change at a magneto-structural transition [3]. The magnetic entropy changes have been derived in the conventional way from a series of isothermal magnetisation experiments, e.g. –ΔSm ~8.8 J kg-1 K-1 for a magnetic field change of ΔB = 0 - 5 T in Mn0.95Ni0.05CoGe. | en_AU |
dc.identifier.citation | Ren, Q, Y., Hutchinson, W. D., Wang, J. L., Studer, A. J., & Campbell, S, J. (2015). The magnetic properties and magnetocaloric effect in Mn1-xNixCoGe. Paper presented at the 39th Annual Condensed Matter and Materials Meeting, Charles Sturt University, Wagga Wagga, NSW, 3 February 2015 - 6 February 2015, (pp. 83). Retrieved from: https://physics.org.au/wp-content/uploads/cmm/2015/Wagga2015_10_Handbook.pdf | en_AU |
dc.identifier.conferenceenddate | 6 February 2015 | en_AU |
dc.identifier.conferencename | 39th Annual Condensed Matter and Materials Meeting | en_AU |
dc.identifier.conferenceplace | Wagga Wagga, NSW | en_AU |
dc.identifier.conferencestartdate | 3 February 2015 | en_AU |
dc.identifier.isbn | 978-0-646-96433-1 | en_AU |
dc.identifier.uri | https://physics.org.au/wp-content/uploads/cmm/2015/Wagga2015_10_Handbook.pdf | en_AU |
dc.identifier.uri | https://apo.ansto.gov.au/dspace/handle/10238/11350 | en_AU |
dc.language.iso | en | en_AU |
dc.publisher | Australian Institute of Physics | en_AU |
dc.subject | Cobalt compounds | en_AU |
dc.subject | Crystal structure | en_AU |
dc.subject | Entropy | en_AU |
dc.subject | Germanium | en_AU |
dc.subject | Magnetic refrigerators | en_AU |
dc.subject | Magneto-thermal effects | en_AU |
dc.subject | Manganese compounds | en_AU |
dc.subject | Nickel compounds | en_AU |
dc.subject | Thermodynamic properties | en_AU |
dc.title | The magnetic properties and magnetocaloric effect in Mn1-xNixCoGe | en_AU |
dc.type | Conference Abstract | en_AU |