Yang Liang 1, 2, Xiang Xia 1, †, , Miao Xin-Xiang 2, ‡, , Li Li 1, Yuan Xiao-Dong 2, Yan Zhong-Hua 1, Zhou Guo-Rui 2, Lv Hai-Bing 2, Zheng Wan-Guo 2, Zu Xiao-Tao 1
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Electric field ∣E∣ distributions inx–zplane are parallel to the incident laser and pass through the center of the ellipsoid for different flattening of the ellipsoid: (a)a= 4λ,b=c=λ, (b)a= 4λ,b=c= 2λ, (c)a= 4λ,b=c= 3λ, (d)a=b=c= 4λ, and (e)a= 4λ,b=c= 5λas contaminant on the output surface. Left:Einx–zplane (y= 89δ), right:Emaxalongzdirection. |