论文标题
光子伪源1/2系统的有效培养基理论
Effective medium theory for photonic pseudospin-1/2 system
论文作者
论文摘要
近年来,已经对光子伪源1/2系统在布里烯区的角落表现出狄拉克锥体色散。然而,众所周知,在二维光子系统中,两个频段的线性频带交叉无法出现在布里鲁因区域的中心,这尊重时间逆转对称性。使用椭圆形磁光圆柱的平方晶格,我们在布里渊区中心构建了一个未配对的迪拉克点,因为第二和第三个带的相交对应于单极和偶极激发。有效的培养基理论可以应用于两个线性交叉带,其使用边界有效培养基方法计算出有效的本构参数。结果表明,只有有效的介电性接近零,而非零有效渗透率的决定因素在狄拉克点频率下消失,显示出与从伪季节1扭转点的双零指数层材料的不同行为,用于时间反向对称系统。从有效的媒体描述中可以很好地理解异国现象,例如Klein Tunneling和Zitterbewegung。升起狄拉克点时,可以通过有效的本构参数准确预测$γ$点附近的边缘状态分散。我们还通过引入一种特定类型的非赫米特扰动,进一步实现了广泛频率范围的磁光复合物结合物的超材料,这些扰动使两个线性频带合并以在实际频率下形成异常点。
Photonic pseudospin-1/2 systems, which exhibit Dirac cone dispersion at Brillouin zone corners in analogy to graphene, have been extensively studied in recent years. However, it is known that a linear band crossing of two bands cannot emerge at the center of Brillouin zone in a two-dimensional photonic system respecting time reversal symmetry. Using a square lattice of elliptical magneto-optical cylinders, we constructed an unpaired Dirac point at the Brillouin zone center as the intersection of the second and third bands corresponding to the monopole and dipole excitations. Effective medium theory can be applied to the two linearly crossed bands with the effective constitutive parameters numerically calculated using the boundary effective medium approach. It is shown that only the effective permittivity approaches zero while the determinant of the nonzero effective permeability vanishes at the Dirac point frequency, showing a different behavior from the double-zero index metamaterials obtained from the pseudospin-1 triply degenerate points for time reversal symmetric systems. Exotic phenomena, such as the Klein tunneling and Zitterbewegung, in the pseudospin-1/2 system can be well understood from the effective medium description. When the Dirac point is lifted, the edge state dispersion near the $Γ$ point can be accurately predicted by the effective constitutive parameters. We also further realized magneto-optical complex conjugate metamaterials for a wide frequency range by introducing a particular type of non-Hermittian perturbations which make the two linear bands coalescence to form exceptional points at the real frequency.