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. 2015 Jun 8;6:7377. doi: 10.1038/ncomms8377

Figure 2. Structural phase transitions without optical pumping.

Figure 2

(ac) Diffraction pattern of the (118)T lattice Bragg peak at temperatures in the vicinity of the structural (Ts) and magnetic (TN) phase transition. (d) Line cut on the area detector (dashed line in a) slowly cooling from a nominal temperature of T=140 to 137 K. The tetragonal (118)T Bragg peak splits first at Ts, due to the transition to the orthorhombic crystal structure, and then further at TN as a result of the onset of SDW order.