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. 2016 Aug 25;7:12592. doi: 10.1038/ncomms12592

Figure 1. Magnetic susceptibility at the polarization transition.

Figure 1

The data shown are from HTO, but are representative of both materials. (a) A schematic view of the pyrochlore lattice: spins are represented as black arrows, and tetrahedra are coloured light blue. The coloured lines show, starting from the white circle, a first (light blue), second (red) and two types of third (green and light green) nearest neighbour. (b) Sign convention for the angle shown in a single tetrahedron: rotations towards [112] are negative while those towards [110] are positive. (c) Magnetic susceptibility: when the field is rotated towards [110] the peak remains unique. (d) As the field is rotated towards [112], the peak splits into two, the upper one moves faster with field as the angle is increased. The temperature for all curves is fixed at 0.18 K and in all cases a smoothly varying background has been subtracted for clarity.