Author Affiliations
1MOE Key Laboratory of Advanced Micro-Structured Materials, School of Physics Science and Engineering, Tongji University, Shanghai 200092, China2Institute of Precision Optical Engineering, School of Physics Science and Engineering, Tongji University, Shanghai 200092, China3School of Aerospace Engineering and Applied Mechanics, Tongji University, Shanghai 200092, Chinashow less
Fig. 1. (a) 1BZ diagram of the tetragonal lattice; (b) the section of the elliptical nanowire array primitive cell model.
Fig. 2. Comparison of the central elliptical nanowires (a) before and (b) after rotation.
Fig. 3. TE and TM modes band structure calculated along the high symmetry lines (a) for and (b) for .
Fig. 4. Stereograms of (a) band 1, (b) band 2, (c) band 3, and (d) band 4 that are calculated in the whole first BZ for the parallel elliptical nanowires array. The band values are projected to the plane of to form a contour map at the bottom.
Fig. 5. Contour map of the four lowest TE mode energy bands of the PC when is 0°, 15°, 30°, 45°, 60°, 75°, and 90°. (a1)–(g1) band 1, (a2)–(g2) band 2, (a3)–(g3) band 3, (a4)–(g4) band 4.
Fig. 6. Contour map of the four lowest TM mode energy bands of the PC when is 0°, 15°, 30°, 45°, 60°, 75°, and 90°.
Fig. 7. First TE mode bandgap width of the arrays with the central element under different rotation angles.
Fig. 8. (a) Contour map of the four lowest TE mode energy bands of the perpendicular elliptical nanowires arrays at different rotations. The first, second, and third rows are array diagrams and energy bands rotated with respect to the array in Fig. 5 by 15°, 30°, and 45°. (b) The first TE mode bandgap width of the perpendicular arrays under different rotation angles.