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横电波激励下亚波长一维金属光栅的异常透射性

王亚伟 刘明礼 刘仁杰 雷海娜 邓晓斌

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横电波激励下亚波长一维金属光栅的异常透射性

王亚伟, 刘明礼, 刘仁杰, 雷海娜, 邓晓斌

Extraordinary transmission through one-dimensional metallic gratings with sub-wavelength slits under transverse electric wave excitation

Wang Ya-Wei, Liu Ming-Li, Liu Ren-Jie, Lei Hai-Na, Deng Xiao-Bin
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  • 针对一维亚波长金属光栅异常透射现象实现的问题,利用时域有限差分法,对横电波(TE波)激励带电介质的亚波长一维金属光栅的光场分布进行了模拟分析,得到了TE波的透射率与电介质折射率的变化关系,从而发现TE波在所研究的模型下具有异常透射现象.基于导模共振理论建立了类导模共振理论,并应用该理论较好地解释了TE波在所研究模型下的异常透射现象,确定类导模共振是TE波产生异常透射性的主要原因.应用所建立的理论解决了传统透射理论无法解决的问题.类导模共振理论揭示了异常透射现象的物理本质,为进一步研究异常透射性的物理本质提
    To show how to achieve the extraordinary transmission of one-dimensional metallic gratings with sub-wavelenghth slits, the transmission distribution of transverse electric (TE) wave through one-dimensional metallic gratings with sub-wavelenghth slits with a dielectric substance applied on it in different ways has been simulated by the finite-difference time-domain method. The relations between the refractive index of dielectric and the transmission efficiency is elicited from simulation, which show that the extraordinary transmission can be produced at several special wavelengths. Then, a new theory named the guided-mode-like resonance theory is put forward based on the guided-mode resonance theory, which is well suited for the extraordinary transmission under the TE-polarized wave excitation, and it is concluded that the guided-mode-like resonance is the main reason for the extraordinary transmission of TE-polarized wave. Thus, the new theory can explain the problems which cant be explained by the traditional theory. In a word, the guided-mode like resonance theory reveals the physical nature of the extraordinary transmission phenomenon which provides a theoretical basis for the further study of the extraordinary transmission phenomenon.
    • 基金项目: 江苏省高校自然科学研究计划重大项目(批准号:09KJA14001)和江苏省自然科学基金(批准号:BK2008230)资助的课题.
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    [2]

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    [3]

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    [4]Rindzevicius T, Alaverdyan Y, Sepulveda B, Pakizeh T, Kll M, Hillenbrand R 2007 J. Phys. Chem. C 111 1207

    [5]

    [5]Rodrigo S G, García-Vidal F J, Martín-Moreno L 2008 Phys. Rev. B 77 075401

    [6]

    [6]Bravo-Abad J, Degiron A, Przybilla F, Genet C, García-Vidal F J, Martín-Moreno L, Ebbesen T W 2006 Nat. Phys. 2 120

    [7]

    [7]Xie Y, Zakharian A R, Moloney J V, Mansuripur M 2006 Opt. Express 14 6400

    [8]

    [8]Crouse D, Keshavareddy P 2007 Opt. Express 15 1415

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    [9]Wu F Q, Han D Z, Li X, Liu X H 2008 Opt. Express 16 6619

    [10]

    ]Belotelov V I, Doskolovich L L, Kotov V A, Bezus E A, Bykov D A, Zvezdin A K 2007 Opt. Coummun. 278 104

    [11]

    ]Wurtz G A, Dickson W, Connor D O, Atkinson R, Hendren W, Evans P, Pollard R, Zayats A V 2008 Opt. Express 16 7460

    [12]

    ]García-Vidal F J, Martín-Moreno L 2002 Phys. Rev. B 66 155412

    [13]

    ]Pendry J B, Martín-Moreno L, García-Vidal F J 2004 Science 305 847

    [14]

    ]Moreno E, Martín-Moreno L, García-Vidal F J 2006 J.Opt. A 8 S94

    [15]

    ]Yuan G H, Wang P, Zhang D G 2006 Proc. IEEE 7803 9774

    [16]

    ]Yuan G H, Wang P, Zhang D G 2007 Chin. Phys. Lett. 24 1600

    [17]

    ]Taflove A, Hagness S C 2000 Computational Electrodynamics: The Finite-Difference Time-Domain Method (3rd ed)(Boston: Artech House) p236

    [18]

    ]Aleksandar D R, Aleksandra B D, Jovan M E, Marian L M 1998 Appl. Opt. 37 5271

    [19]

    ]Young J L, Nelson R O 2001 IEEE Antennas Propag. Mag. 43 61

    [20]

    ]Han M H, Dutton R W 2006 IEEE Microw. Wireless Compon.Lett. 16 3

    [21]

    ]Ma J Y,Liu S J,Wei C Y,Xu C,Jin Y X,Zhao Y A,Shao J D,Fan Z X 2008 Acta Phys. Sin. 57 827 (in Chinese)[麻健勇、刘世杰、魏朝阳、许程、晋云霞、赵元安、邵建达、范正修 2008 物理学报 57 827]

    [22]

    ]Xie Y, Zakharian A R, Moloney J V, Mansuripur M 2005 Opt. Express 13 4485

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出版历程
  • 收稿日期:  2009-07-15
  • 修回日期:  2009-10-31
  • 刊出日期:  2010-03-05

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