Two approaches to three-dimensional array foci of generalized Fibonacci structures

Jie Ke; Junyong Zhang; Zhiyuan Ren

doi:doi:10.3788/col201614.060501

Collection Of theses on high power laser and plasma physics, 2016, 14 (1): 060501, Published Online: May. 26, 2017

Two approaches to three-dimensional array foci of generalized Fibonacci structures

Jie Ke ^1,2Junyong Zhang ^1,*Zhiyuan Ren ¹

Author Affiliations

¹ National Laboratory on High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China

² University of Chinese Academy of Sciences, Beijing 100049, China

Figures & Tables

Fig. 1. Fibonacci structure unit (a) in polar coordinates and (b) in Cartesian coordinates.

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Fig. 2. Intensity contours at two focal planes against a polar Fibonacci structure (a) in 3D space, (b) at the first focal plane, and (c) at the second focal plane.

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Fig. 3. Intensity contours at two focal planes against a Cartesian Fibonacci structure (a) in 3D space, (b) at the first focal plane, and (c) at the second focal plane.

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Fig. 4. (a) A Fibonacci structure based on the diffractive optical lever. (b) Intensity contours at four focal planes in 3D space.

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Fig. 5. Intensity contours at four focal planes compared against Fig. 4(a).

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Fig. 6. (a) A multi-hybrid Fibonacci structure. (b) Intensity contours at four focal planes in 3D space.

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Fig. 7. Intensity contours at four focal planes compared against Fig. 6(a).

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Jie Ke, Junyong Zhang, Zhiyuan Ren. Two approaches to three-dimensional array foci of generalized Fibonacci structures[J]. Collection Of theses on high power laser and plasma physics, 2016, 14(1): 060501.

Two approaches to three-dimensional array foci of generalized Fibonacci structures

Fig. 1. Fibonacci structure unit (a) in polar coordinates and (b) in Cartesian coordinates.

Fig. 2. Intensity contours at two focal planes against a polar Fibonacci structure (a) in 3D space, (b) at the first focal plane, and (c) at the second focal plane.

Fig. 3. Intensity contours at two focal planes against a Cartesian Fibonacci structure (a) in 3D space, (b) at the first focal plane, and (c) at the second focal plane.

Fig. 4. (a) A Fibonacci structure based on the diffractive optical lever. (b) Intensity contours at four focal planes in 3D space.

Fig. 5. Intensity contours at four focal planes compared against Fig. 4(a).

Fig. 6. (a) A multi-hybrid Fibonacci structure. (b) Intensity contours at four focal planes in 3D space.

Fig. 7. Intensity contours at four focal planes compared against Fig. 6(a).

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Two approaches to three-dimensional array foci of generalized Fibonacci structures

Fig. 1. Fibonacci structure unit (a) in polar coordinates and (b) in Cartesian coordinates.

Fig. 2. Intensity contours at two focal planes against a polar Fibonacci structure (a) in 3D space, (b) at the first focal plane, and (c) at the second focal plane.

Fig. 3. Intensity contours at two focal planes against a Cartesian Fibonacci structure (a) in 3D space, (b) at the first focal plane, and (c) at the second focal plane.

Fig. 4. (a) A Fibonacci structure based on the diffractive optical lever. (b) Intensity contours at four focal planes in 3D space.

Fig. 5. Intensity contours at four focal planes compared against Fig. 4(a).

Fig. 6. (a) A multi-hybrid Fibonacci structure. (b) Intensity contours at four focal planes in 3D space.

Fig. 7. Intensity contours at four focal planes compared against Fig. 6(a).

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