Jurusan Fisika, FMIPA, Universitas Diponegoro, Jl. Prof Soedarto, Tembalang, Semarang, Indonesia.
J Phys Condens Matter. 2012 Oct 10;24(40):406003. doi: 10.1088/0953-8984/24/40/406003. Epub 2012 Sep 18.
We present a theoretical discussion of surface polaritons on a ferroelectric-antiferromagnet with magnetoelectric coupling which allows the magnetic subsystem to be canted. Canting of the antiferromagnet results in weak ferromagnetism. The surface polaritons for a semi-infinite film are calculated for a propagation parallel to the uniaxial easy axis, leading to mixed modes. A superposition of two plane waves is needed to generate mixed surface modes. We find two branches, one near the magnon resonance frequency and the other near the phonon resonance frequency. We also find that the surface modes are non-reciprocal due to magnetoelectric interaction, such that ω(k) ≠ ω(-k), where ω is the frequency and k is the propagation vector.
我们提出了一个关于具有磁电耦合的铁电-反铁磁体表面极化激元的理论讨论,该耦合允许磁子系统倾斜。反铁磁体的倾斜导致弱铁磁性。对于沿单轴易轴平行传播的半无限薄膜,我们计算了表面极化激元,导致混合模式。需要两个平面波的叠加来产生混合表面模式。我们发现有两个分支,一个在磁振子共振频率附近,另一个在声子共振频率附近。我们还发现,由于磁电相互作用,表面模式是不可逆的,使得 ω(k) ≠ ω(-k),其中 ω 是频率,k 是传播矢量。