Design of compensated ferrimagnetic Heusler alloys for giant tunable exchange bias.
Ajaya K. Nayak, Michael Nicklas, Stanislav Chadov, Panchanana Khuntia, Chandra Shekhar, Adel Kalache, Michael Baenitz, Yurii Skourski, Veerendra K. Guduru, Alessandro Puri, Uli Zeitler, J. M. D. Coey, Claudia Felser
Nature Materials 14, 679 (2015)
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a, Uncompensated magnetization, M, in Mn3−xPtxGa going through a compensation point (M = 0) at x
= 0.59 (upper panel): squares are results from theoretical
calculations. The line is a guide to eye. Lower panel: Experimental EB
field HEB at 4.2 K (solid circles). The solid line
corresponds to the result of our calculation. The regular and inverse
Heusler structures of the Mn3Ga and Mn2PtGa are shown to the left and right respectively. b–d, Magnetic moments of Mn in two different sublattices for Mn3Ga, Mn2.41Pt0.59Ga and Mn2PtGa.
Red arrows correspond to Mn in the Mn–Ga plane and blue arrows to Mn in
the Mn–Mn planes. The size and direction of the moment is indicated by
the arrow. Perfect magnetic compensation is expected in Mn2.41Pt0.59Ga. e, FM domains (boundaries indicated by dashed lines) inside the compensated AFM host.
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