19-21 November 2018
AINSE Conference Centre New Illawarra Road Lucas Heights NSW 2234 Australia
Australia/Sydney timezone

Magnetocaloric Mn(Co1-xNix)Ge - Structural and magnetic transitions

Not scheduled
1h 30m
AINSE Conference Centre New Illawarra Road Lucas Heights NSW 2234 Australia

AINSE Conference Centre New Illawarra Road Lucas Heights NSW 2234 Australia

AINSE Conference Centre, New Illawarra Road, Lucas Heights, NSW 2234, Australia
Poster Advanced Materials Poster Session

Speaker

Prof. Stewart Campbell (School of Physical, Environmental and Mathematical Sciences, UNSW Canberra at the Australian Defence Force Academy, ACT 2610)

Description

The structural and magnetic properties of MnCoGe-based alloys have been studied extensively in recent years due to their potential application as magnetic cooling materials based on the magnetocaloric effect (MCE). The Mn(Co$_{1-x}$Ni$_x$)Ge series is of particular interest as magnetic transitions in the range 275 K to 345 K generally coincide with a martensitic structural transition $T$$_{M}$, with such an overlap then allowing scope for the formation of a magneto-structural transition (ferromagnetic orthorhombic to paramagnetic hexagonal) and hence an associated large MCE [e.g. 1].

Neutron diffraction, magnetisation and x-ray experiments on Mn(Co$_{1-x}$Ni$_x$)Ge compounds (x = 0.12 to 1.00) have demonstrated magnetic structures ranging from ferromagnetic for x < 0.50 to non-collinear spiral antiferromagnetic for x > 0.55 at low temperature (e.g. 5 K). $T$$_M$ is found to decrease initially with increasing Ni content and then increase. First-order magneto-structural transitions are observed in Mn(Co$_{1-x}$Ni$_x$)Ge samples for ~0.20 < x < ~0.65 with the presence of ferromagnetic and antiferromagnetic structures in Mn(Co$_{1-x}$Ni$_x$)Ge allowing investigation of both direct and inverse magnetocaloric effects. Our results (including the magnetic phase diagram for Mn(Co$_{1-x}$Ni$_x$)Ge) are discussed in terms of the increase of valence electron concentration on substitution of Ni (3$d$$^8$4s$^2$) for Co (3$d$$^7$4$s$$^2$) in the orthorhombic phase, leading to expansion of the unit cell and redistribution of the valence electrons [2].

[1] T. Trung, L. Zhang, L. Caron, K. H. J. Buschow, E. Brück, Appl. Phys. Lett. 2010, 96, 172504.
[2] Q. Ren, W. D. Hutchison, J. Wang, A. J. Studer and S. J. Campbell, Chem. Mater. 2018, 30, 1324.

Topic Advanced Materials

Primary authors

Dr Qingyong Ren (School of Physical, Environmental and Mathematical Sciences, UNSW Canberra at the Australian Defence Force Academy, ACT 2610; School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China) Dr Wayne Hutchison (School of Physical, Environmental and Mathematical Sciences, UNSW Canberra at the Australian Defence Force Academy, ACT 2610) Dr Jianli Wang (Institute for Superconductivity and Electronic Materials, University of Wollongong) Dr Andrew Studer (Australian Centre for Neutron Scattering, Kirrawee DC NSW 2232) Prof. Stewart Campbell (School of Physical, Environmental and Mathematical Sciences, UNSW Canberra at the Australian Defence Force Academy, ACT 2610)

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