• Photonics Research
  • Vol. 5, Issue 5, 436 (2017)
Zhao Chen1, Fan Zhang1, Qi Zhang1, Juanjuan Ren1, He Hao1, Xueke Duan1, Pengfei Zhang2、3, Tiancai Zhang2、3, Ying Gu1、2、*, and Qihuang Gong1、2
Author Affiliations
  • 1State Key Laboratory for Mesoscopic Physics, Collaborative Innovation Center of Quantum Matter, Department of Physics, Peking University, Beijing 100871, China
  • 2Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan, Shanxi 030006, China
  • 3State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Opto-Electronics, Shanxi University, Taiyuan 030006, China
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    DOI: 10.1364/PRJ.5.000436 Cite this Article Set citation alerts
    Zhao Chen, Fan Zhang, Qi Zhang, Juanjuan Ren, He Hao, Xueke Duan, Pengfei Zhang, Tiancai Zhang, Ying Gu, Qihuang Gong. Blue-detuned optical atom trapping in a compact plasmonic structure[J]. Photonics Research, 2017, 5(5): 436 Copy Citation Text show less
    (a) Schematic of the array of nanoholes in a metallic film. Inset shows the unit cell of the presented nanohole arrays and the geometrical parameter symbols. (b) Simulation results of the normalized zero-order transmission spectrum. (c) Field distribution of |E| in the nanohole at the air–gold interface when a 760 nm laser illuminates from the −z direction.
    Fig. 1. (a) Schematic of the array of nanoholes in a metallic film. Inset shows the unit cell of the presented nanohole arrays and the geometrical parameter symbols. (b) Simulation results of the normalized zero-order transmission spectrum. (c) Field distribution of |E| in the nanohole at the air–gold interface when a 760 nm laser illuminates from the z direction.
    (a) Field distributions of |E| in the x–z plane when y is 0 nm. (b) Normalized intensity distributions of |E|2 along the dark dashed line in (a).
    Fig. 2. (a) Field distributions of |E| in the xz plane when y is 0 nm. (b) Normalized intensity distributions of |E|2 along the dark dashed line in (a).
    (a) Calculated total potential along the dark dashed line in Fig. 2(a). (b) Potential distributions for point P in the x–y plane. Ux and Utot−x represent the optical dipole potential and the total potential along the x direction, respectively. The incident optical power P0=1 mW.
    Fig. 3. (a) Calculated total potential along the dark dashed line in Fig. 2(a). (b) Potential distributions for point P in the xy plane. Ux and Utotx represent the optical dipole potential and the total potential along the x direction, respectively. The incident optical power P0=1  mW.
    (a) Contour plot of a trapping total potential in the x–y plane at z=372 nm for a unit cell. (b) Periodic arrays.
    Fig. 4. (a) Contour plot of a trapping total potential in the xy plane at z=372  nm for a unit cell. (b) Periodic arrays.
    Zhao Chen, Fan Zhang, Qi Zhang, Juanjuan Ren, He Hao, Xueke Duan, Pengfei Zhang, Tiancai Zhang, Ying Gu, Qihuang Gong. Blue-detuned optical atom trapping in a compact plasmonic structure[J]. Photonics Research, 2017, 5(5): 436
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