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Figure 10
Full polarimetry pattern of the (1/2 0 1/4) reflection of ErMn2O5 measured at T = 37 K. The maximum intensity in the rotated light channel (π–σ′, σ–π′) is caused by the magnetic contribution to the scattering peak. |
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Figure 10
Full polarimetry pattern of the (1/2 0 1/4) reflection of ErMn2O5 measured at T = 37 K. The maximum intensity in the rotated light channel (π–σ′, σ–π′) is caused by the magnetic contribution to the scattering peak. |