旋转方形散射体对三角晶格磁振子晶体带结构的优化  

Spin-wave band gaps created by rotating square rods in triangular lattice magnonic crystals

作　　者：胡晓颖[1] 郭晓霞[1] 胡文弢[1] 呼和满都拉[1] 郑晓霞[1] 荆丽丽[1] 

机构地区：[1]集宁师范学院物理系,集宁012000

出　　处：《物理学报》2015年第10期250-254,共5页Acta Physica Sinica

基　　金：内蒙古自治区高等学校科学技术研究项目(批准号:NJZY13281)资助的课题~~

摘　　要：用改进的平面波展开法数值计算了正方形散射体三角排列的二维磁振子晶体当散射体旋转时的带结构.结果显示,同样的填充率下,旋转正方柱散射体可以在新的频率范围内打开更多的带隙,或者使低频带隙加宽.说明旋转散射体可以有效地优化带隙.Recently, magnonic crystals which are the magnetic counterparts of photonic crystals or phononic crystals are becoming a hot area of research. In this paper, band structure of two-dimensional magnotic crystal composed of square rods triangularly arranged are calculated by using the plane-wave expansion method. Spimwave band structures of two-dimensional magnonic crystal composed of Fe triangularly arranged Fe in an EuO matrix. The results show that when the filling ratio f = 0.4, only two absolute band gaps can be found in the case of ~ -- 0~. The first gap appears between the first band and the second band, the second gap between the sixth band and the seventh band. However, the number of band gaps can be improved by rotating the square rods through ~ ^-- 25~, there are eight absolute band gaps that can be found. The first gap appears between the first band and the second band, the fifth gap between the sixth band and the seventh band. The new band gaps can be found, the second gap appears between the third band and the fourth band, the third gap between the fourth band and the fifth band, the fourth gap between the fifth band and the sixth band, the sixth gap between the seventh band and the eighth band, the seventh gap between the eighth band and the ninth band, the eighth gap between the ninth band and the tenth band. These results show that it is possible to create spin-wave gaps by rotating square rods in a two-dimensional magnotic crystal. The numerical results of the normalized gap width △Ω/Ωg of the first gap between the first band and the second band always changes with filling fraction f and rotational angles 8. When f = 0.6 we calculated the first normalized gap width △Ω/Ωg. when f = 0.6 and θ = 0°, the first gap width △Ω = 0.812（μoω/g） and the normalized gap width △Ω/Ωg = 0.9187. The results show that from the first normalized gap widths the largest one can be found when f = 0.6 and θ = 5°, the first gap width △Ω = 0.937（μoω/g） and the normalized gap width △Ω/Ωg

关 键 词：磁振子晶体 带隙 平面波展开法 

分 类 号：O481[理学—固体物理]