4.6 Article

Confirming the trilinear form of the optical magnetoelectric effect in the polar honeycomb antiferromagnet Co2Mo3O8

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NPJ QUANTUM MATERIALS
卷 7, 期 1, 页码 -

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NATURE PORTFOLIO
DOI: 10.1038/s41535-021-00417-3

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资金

  1. Deutsche Forschungsgemeinschaft DFG via the Transregional Collaborative Research Center [TRR 80]
  2. project ANCD (Moldova) [20.80009.5007.19]
  3. National Research, Development, and Innovation Office - NKFIH [FK 135003, Bolyai 00318/20/11]
  4. Austrian Science Fund (FWF) [I 2816-N27, TAI 334-N]
  5. Austrian Agency for International Cooperation in Education and Research [WTZ HU 08/2020]

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Magnetoelectric phenomena are closely related to relativistic effects and require the breaking of spatial inversion symmetry and time-reversal invariance in materials. The optical magnetoelectric effect in materials with non-parallel magnetization and electric polarization generates a trilinear term in the refractive index, which can significantly affect light-matter interaction and lead to non-reciprocal light propagation. Co2Mo3O8, with its sharp magnetoelectric resonances in the terahertz regime, is an ideal compound to demonstrate this fundamental relation.
Magnetoelectric phenomena are intimately linked to relativistic effects and also require the material to break spatial inversion symmetry and time-reversal invariance. Magnetoelectric coupling can substantially affect light-matter interaction and lead to non-reciprocal light propagation. Here, we confirm on a fully experimental basis, without invoking either symmetry-based or material-specific assumptions, that the optical magnetoelectric effect in materials with non-parallel magnetization (M) and electric polarization (P) generates a trilinear term in the refractive index, delta n mu k . (P x M), where k is the propagation vector of light. Its sharp magnetoelectric resonances in the terahertz regime, which are simultaneously electric and magnetic dipole active excitations, make Co2Mo3O8 an ideal compound to demonstrate this fundamental relation via independent variation of M, P, and k. Remarkably, the material shows almost perfect one-way transparency in moderate magnetic fields for one of these magnetoelectric resonances.

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