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Wide-angle method for vortex electromagnetic wave generation using field transformation

Feng Jia-Lin Shi Hong-Yu Wang Yuan Zhang An-Xue Xu Zhuo

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Wide-angle method for vortex electromagnetic wave generation using field transformation

Feng Jia-Lin, Shi Hong-Yu, Wang Yuan, Zhang An-Xue, Xu Zhuo
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  • The Field transformation (FT) is a novel theory for controlling the polarization and impedance of electromagnetic waves, which is independent on the angle of incidence. Thus, the FT method is superior for wide-angle devices design. In this paper, we propose a wide-angle method for generating vortex beam based on the FT theory. According to this method, an artificial media for vortex beam generation is designed and simulated, which demonstrates the proposed method. The designed artificial media is a multi-layered structure, which can generate vortex beam of order 2 with an incident angle stability up to 60°.
      Corresponding author: Shi Hong-Yu, honyo.shi1987@gmail.com
    [1]

    Bliokh K Y, Bekshaev A Y, Nori F 2013 New J. Phys. 15 33026Google Scholar

    [2]

    Menglin C, Li J, Wei S 2018 Appl. Sci. 8 362Google Scholar

    [3]

    Wang J, Yang J Y, Fazal I M 2012 Nat. Photonics 6 488Google Scholar

    [4]

    苏志锟, 王发强, 路轶群, 金锐博, 梁瑞生, 刘颂豪 2008 57 3016Google Scholar

    Su Z K, Wang F Q, Lu Y Q, Jin R B, Liang R B, Liu S H 2008 Acta Phys. Sin. 57 3016Google Scholar

    [5]

    Lemaitre-Auger P, Abielmona S, Caloz C 2013 IEEE Trans. Antennas Propag. 61 1838Google Scholar

    [6]

    David G 2003 Nature 424 810Google Scholar

    [7]

    刘义东, 高春清, 高明伟, 李丰 2007 56 854Google Scholar

    Liu Y D, Gao C Q, Gao M W, Li F 2007 Acta Phys. Sin. 56 854Google Scholar

    [8]

    Oemrawsingh S S R, Houwelingen J A W, Eliel E R, Woerdman J P, Verstegen E J K, Kloosterboer J G 2004 Appl. Opt. 43 688Google Scholar

    [9]

    Beijersbergen M W, Coerwinkel R P C, Kristensen M, Woerdman J P 1994 Opt. Commun. 112 321Google Scholar

    [10]

    Turnbull G A, Robertson D A, Smith G M, Allen L, Padgett M J 1996 Opt. Commun. 127 183Google Scholar

    [11]

    Marrucci L, Manzo C, Paparo D 2006 Phys. Rev. Lett. 96 163905Google Scholar

    [12]

    Paterson C, Smith R 1996 Opt. Commun. 124 121Google Scholar

    [13]

    Mohammadi S M, Daldorff L K S, Bergman J E S, Karlsson R L, Thide B, Forozesh K 2010 IEEE Trans. Antennas Propag. 2 565

    [14]

    Genevet P, Y u, N, Aieta F, Lin J, Kats M A, Blanchard R 2012 Appl. Phys. Lett. 100 1

    [15]

    Pu M, Li X, Ma X, Wang Y, Zhao Z, Wang C 2015 Sci. Adv. 1 e1500396Google Scholar

    [16]

    Huang L, Chen X, Holger Mühlenbernd, Li G, Zhang S 2012 Nano Lett. 12 5750Google Scholar

    [17]

    Arbabi A, Horie Y, Bagheri M 2015 Nat. Nanotechnol. 10 937Google Scholar

    [18]

    Yue F, Wen D, Xin J, Gerardot B D, Li J, Chen X 2016 ACS Photonics acsphotonics 6 b00392

    [19]

    Yang H, Niu J, Zhang K, Ding X, Wu Q 2016 IEEE International Conference on Electronic Information and Communication Technology (ICEICT) Harbin, China, August 20–22, 2016 p552

    [20]

    Tamburini F, Mari E, Thideì Bo, Barbieri C, Romanato F 2011 Appl. Phys. Lett. 99 204102Google Scholar

    [21]

    Vaishnavi V, Priya V G, Sharmila Devi A, Manoj Kumar M, Venkatesh S, Sundaram G A 2014 International Conference on Communication and Signal Processing Melmaruvathur, India, April 3–5, 2014 p1414

    [22]

    Liu F, Liang Z, Li J 2013 Phys. Rev. Lett. 111 033901Google Scholar

    [23]

    Liu F, Li J S 2015 Phys. Rev. Lett. 114 103902Google Scholar

    [24]

    Zhao J M, Zhang L H, Li J S, Feng Y J, Dyke A, Haq S, Hao Y 2015 Sci. Rep. 5 17532Google Scholar

    [25]

    Shi H Y, Hao Y 2013 Opt. Express 26 20132

    [26]

    Shi H, Giddens H, Hao Y 2019 IET Microwaves Antennas Propag. 13 1450Google Scholar

    [27]

    Shi H Y, Giddens H, Hao Y 2017 IEEE Antennas Wirel. Propag. Lett. 16 2869

    [28]

    Chen M L N, Jiang L J, Sha W E I 2019 IEEE Antennas Wirel. Propag. Lett. 18 477Google Scholar

    [29]

    Schurig D, Mock J J, Justice B J, Cummer S A, Pendry J B, Starr A F, Smith D R 2016 Science 314 977

    [30]

    Born M, Wolf E, Bhatia A B 2002 Principles of Optics: Electromagnetic Theory of Propagation, Interference and Diffraction of Light 7th (expanded) (Cambridge: Cambridge University Press) pp220–225

    [31]

    Chen M L N, Jiang L J, Sha W E I 2016 J. Appl. Phys. 119 064506Google Scholar

    [32]

    Kang M, Chen J, Wang X, Wang H 2012 J.Opt. Soc. Am. B: Opt. Phys. 29 572Google Scholar

  • 图 1  场变换示意图

    Figure 1.  Schematic diagram of the FT medium.

    图 2  人工双折射材料: $xyz$轴绕y轴旋转45°变成${x'}y{z'}$, 入射波在$xy$平面内, $\theta $为入射角, ${k_0}$是入射波的波数

    Figure 2.  Artificial birefringence medium: The $xyz$ coordinate is twisted along the y -axis by 45° to the ${x'}y{z'}$ coordinate. The incident plane is x-y plane, $\theta $ is the incident angle, ${k_0}$ is the wave vector of the incident wave.

    图 3  Pancharatnam-Berry(几何)相位, 入射波沿y方向照射到单元上, 单元绕y轴旋转$\alpha $, 带来$2\alpha $的相位变化

    Figure 3.  Pancharatnam-Berry phase: When the EM wave incident on the unit along y direction, and the unit rotates $\alpha $ around the y axis, the phase changed $2\alpha $.

    图 4  单元模型

    Figure 4.  The model of unit cell.

    图 5  (a) ${J_{xx}}$${J_{yy}}$的幅度 ; (b) ${J_{xx}}$${J_{yy}}$的相位

    Figure 5.  (a) The amplitude of ${J_{xx}}$ and ${J_{yy}}$; (b) the phase of ${J_{xx}}$ and ${J_{yy}}$.

    图 6  ${J_{xy}}$${J_{yx}}$的幅度

    Figure 6.  The amplitude of ${J_{xy}}$ and ${J_{yx}}$.

    图 7  (a)旋转所形成的介质圆环的主视图, 由100个圆环组成每个圆环的半径为4 mm; (b)介质圆环的侧视图

    Figure 7.  (a) Main view of dielectric rings, it’s consists of 100 rings with radius of 4 mm and thickness of dielectric rings is 30 mm; (b) side view of dielectric rings.

    图 8  (a)垂直入射的透射波; (b)介质圆环周围空间的电场分布; (c)13 GHz时右旋圆极化波的幅度; (d)13 GHz时右旋圆极化波的相位

    Figure 8.  (a) The transmission wave while incident angle is 0°; (b) E-field distribution around dielectric rings; (c) amplitude of RCP wave at 13 GHz ; (d) phase of RCP wave at 13 GHz.

    图 9  (a) 20°斜入射时的透射波; (b)介质圆环周围空间的电场分布; (c) 20°斜入射时13 GHz的右旋圆极化波的幅度; (c) 20°斜入射时在13 GHz的右旋圆极化波的相位

    Figure 9.  (a) The transmission wave while incident angle is 20°; (b) E-field distribution around dielectric rings; (c) amplitude of RCP wave at 20° oblique incidence; (d) phase of RCP wave at 20° oblique incidence.

    图 10  (a) 40°斜入射时的透射波; (b)介质圆环周围空间的电场分布; (c) 40°斜入射时13 GHz的右旋圆极化波的幅度; (d) 40°斜入射时13 GHz的右旋圆极化波的相位

    Figure 10.  (a) The transmission wave while incident angle is 40°; (b) E-field distribution around dielectric rings; (c) amplitude of RCP wave at 40° oblique incidence; (d) phase of RCP wave at 40° oblique incidence.

    图 11  (a) 50°斜入射时的透射波; (b)介质圆环周围空间的电场分布; (c) 50°斜入射时13 GHz的右旋圆极化波的幅度; (d) 50°斜入射时在13 GHz的右旋圆极化波的相位

    Figure 11.  (a) The transmission wave while incident angle is 50°; (b) E-field distribution around dielectric rings; (c) amplitude of RCP wave at 50° oblique incidence; (d) phase of RCP wave at 50° oblique incidence.

    图 12  (a) 60°斜入射时的透射波; (b) 60°入射时介质圆环周围的电场分布; (c) 60°斜入射时13 GHz的右旋圆极化波的幅度; (d) 60°斜入射时13 GHz的右旋圆极化波的相位

    Figure 12.  (a) The transmission wave while incident angle is 60°; (b) E-field distribution around dielectric rings at 60° oblique incidence; (c) amplitude of RCP wave at 60° oblique incidence; (d) phase of RCP wave at 60° oblique incidence.

    表 1  垂直入射时不同频点的右旋分量的最大值

    Table 1.  Maximum values of RCP at different frequencies when normal incidence.

    频率/GHz右旋圆极化分量最大值/dBi
    1114.70
    1215.80
    1316.90
    1417.30
    1517.50
    DownLoad: CSV

    表 2  20°斜入射时不同频点的右旋分量的最大值

    Table 2.  Maximum values of RCP at different frequencies when incident angle is 20°.

    频率/GHz右旋圆极化分量最大值/dBi
    1115.30
    1216.10
    1317.20
    1417.70
    1517.40
    DownLoad: CSV

    表 3  40°斜入射时不同频点右旋分量的最大值

    Table 3.  Maximum values of RCP at different frequencies when incident angle is 40°.

    频率/GHz右旋圆极化分量最大值/dBi
    1116.0
    1216.7
    1317.4
    1418.6
    1518.5
    DownLoad: CSV

    表 4  50°斜入射时不同频点的左旋和右旋分量的最大值

    Table 4.  Maximum values of RCP at different frequencies when incident angle is 50°.

    频率/GHz右旋圆极化分量最大值/dBi
    1116.8
    1217.2
    1317.6
    1418.6
    1519.6
    DownLoad: CSV

    表 5  60°斜入射时不同频点的左旋和右旋分量的最大值

    Table 5.  Maximum values of RCP at different frequencies when incident angle is 60°.

    频率/GHz右旋圆极化分量最大值/dBi
    1116.1
    1216.9
    1317.9
    1418.5
    1519.6
    DownLoad: CSV
    Baidu
  • [1]

    Bliokh K Y, Bekshaev A Y, Nori F 2013 New J. Phys. 15 33026Google Scholar

    [2]

    Menglin C, Li J, Wei S 2018 Appl. Sci. 8 362Google Scholar

    [3]

    Wang J, Yang J Y, Fazal I M 2012 Nat. Photonics 6 488Google Scholar

    [4]

    苏志锟, 王发强, 路轶群, 金锐博, 梁瑞生, 刘颂豪 2008 57 3016Google Scholar

    Su Z K, Wang F Q, Lu Y Q, Jin R B, Liang R B, Liu S H 2008 Acta Phys. Sin. 57 3016Google Scholar

    [5]

    Lemaitre-Auger P, Abielmona S, Caloz C 2013 IEEE Trans. Antennas Propag. 61 1838Google Scholar

    [6]

    David G 2003 Nature 424 810Google Scholar

    [7]

    刘义东, 高春清, 高明伟, 李丰 2007 56 854Google Scholar

    Liu Y D, Gao C Q, Gao M W, Li F 2007 Acta Phys. Sin. 56 854Google Scholar

    [8]

    Oemrawsingh S S R, Houwelingen J A W, Eliel E R, Woerdman J P, Verstegen E J K, Kloosterboer J G 2004 Appl. Opt. 43 688Google Scholar

    [9]

    Beijersbergen M W, Coerwinkel R P C, Kristensen M, Woerdman J P 1994 Opt. Commun. 112 321Google Scholar

    [10]

    Turnbull G A, Robertson D A, Smith G M, Allen L, Padgett M J 1996 Opt. Commun. 127 183Google Scholar

    [11]

    Marrucci L, Manzo C, Paparo D 2006 Phys. Rev. Lett. 96 163905Google Scholar

    [12]

    Paterson C, Smith R 1996 Opt. Commun. 124 121Google Scholar

    [13]

    Mohammadi S M, Daldorff L K S, Bergman J E S, Karlsson R L, Thide B, Forozesh K 2010 IEEE Trans. Antennas Propag. 2 565

    [14]

    Genevet P, Y u, N, Aieta F, Lin J, Kats M A, Blanchard R 2012 Appl. Phys. Lett. 100 1

    [15]

    Pu M, Li X, Ma X, Wang Y, Zhao Z, Wang C 2015 Sci. Adv. 1 e1500396Google Scholar

    [16]

    Huang L, Chen X, Holger Mühlenbernd, Li G, Zhang S 2012 Nano Lett. 12 5750Google Scholar

    [17]

    Arbabi A, Horie Y, Bagheri M 2015 Nat. Nanotechnol. 10 937Google Scholar

    [18]

    Yue F, Wen D, Xin J, Gerardot B D, Li J, Chen X 2016 ACS Photonics acsphotonics 6 b00392

    [19]

    Yang H, Niu J, Zhang K, Ding X, Wu Q 2016 IEEE International Conference on Electronic Information and Communication Technology (ICEICT) Harbin, China, August 20–22, 2016 p552

    [20]

    Tamburini F, Mari E, Thideì Bo, Barbieri C, Romanato F 2011 Appl. Phys. Lett. 99 204102Google Scholar

    [21]

    Vaishnavi V, Priya V G, Sharmila Devi A, Manoj Kumar M, Venkatesh S, Sundaram G A 2014 International Conference on Communication and Signal Processing Melmaruvathur, India, April 3–5, 2014 p1414

    [22]

    Liu F, Liang Z, Li J 2013 Phys. Rev. Lett. 111 033901Google Scholar

    [23]

    Liu F, Li J S 2015 Phys. Rev. Lett. 114 103902Google Scholar

    [24]

    Zhao J M, Zhang L H, Li J S, Feng Y J, Dyke A, Haq S, Hao Y 2015 Sci. Rep. 5 17532Google Scholar

    [25]

    Shi H Y, Hao Y 2013 Opt. Express 26 20132

    [26]

    Shi H, Giddens H, Hao Y 2019 IET Microwaves Antennas Propag. 13 1450Google Scholar

    [27]

    Shi H Y, Giddens H, Hao Y 2017 IEEE Antennas Wirel. Propag. Lett. 16 2869

    [28]

    Chen M L N, Jiang L J, Sha W E I 2019 IEEE Antennas Wirel. Propag. Lett. 18 477Google Scholar

    [29]

    Schurig D, Mock J J, Justice B J, Cummer S A, Pendry J B, Starr A F, Smith D R 2016 Science 314 977

    [30]

    Born M, Wolf E, Bhatia A B 2002 Principles of Optics: Electromagnetic Theory of Propagation, Interference and Diffraction of Light 7th (expanded) (Cambridge: Cambridge University Press) pp220–225

    [31]

    Chen M L N, Jiang L J, Sha W E I 2016 J. Appl. Phys. 119 064506Google Scholar

    [32]

    Kang M, Chen J, Wang X, Wang H 2012 J.Opt. Soc. Am. B: Opt. Phys. 29 572Google Scholar

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Publishing process
  • Received Date:  12 March 2020
  • Accepted Date:  13 June 2020
  • Available Online:  15 June 2020
  • Published Online:  05 July 2020

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