Electromagnetic wave beam splitter
    11.
    发明授权
    Electromagnetic wave beam splitter 有权
    电磁波分束器

    公开(公告)号:US08729511B2

    公开(公告)日:2014-05-20

    申请号:US14118015

    申请日:2011-11-21

    Abstract: Embodiments of the present invention relate to an electromagnetic wave beam splitter, comprising a functional layer made of at least one metamaterial sheet, wherein different metamaterial sheets have the same refractive index distribution; the metamaterial sheet may be divided into a circular region and an annular region concentric to the circular region; a refractive index increases continuously as a radius increases and refractive indices at the same radius are the same within the circular region; and a refractive index decreases continuously as a radius increases and refractive indices are the same at the same radius within the annular region. The circular region of the functional layer of the beam splitter according to the present invention has the function of diverging an electromagnetic wave; the annular region has the function of converging an electromagnetic wave; the electromagnetic wave incident on the circular region of the functional layer deflects toward edges on two sides of the functional layer respectively; the electromagnetic wave incident on the annular region deflects in a direction toward a circle center; and after an electromagnetic wave emitted by a signal source is incident on the beam splitter, an emergent electromagnetic wave forms an annular radiation region. This can satisfy the requirements of, for example, avoiding an obstacle and interference.

    Abstract translation: 本发明的实施例涉及一种电磁波束分离器,包括由至少一个超材料片制成的功能层,其中不同的超材料片具有相同的折射率分布; 超材料片可以分为圆形区域和与圆形区域同心的环形区域; 随着半径的增加,折射率连续增加,同一半径的折射率在圆形区域内相同; 并且折射率随着半径增加而连续减小,并且折射率在环形区域内的相同半径处相同。 根据本发明的分束器的功能层的圆形区域具有发散电磁波的功能; 环形区域具有会聚电磁波的功能; 入射到功能层的圆形区域上的电磁波分别偏向功能层两侧的边缘; 入射到环形区域的电磁波在朝向圆心的方向上偏转; 并且在由信号源发射的电磁波入射到分束器上之后,出现的电磁波形成环形辐射区域。 这可以满足例如避免障碍和干扰的要求。

    METAMATERIAL FOR DIVERGING AN ELECTROMAGNETIC WAVE
    12.
    发明申请
    METAMATERIAL FOR DIVERGING AN ELECTROMAGNETIC WAVE 有权
    用于分流电磁波的元件

    公开(公告)号:US20130050058A1

    公开(公告)日:2013-02-28

    申请号:US13521743

    申请日:2011-11-24

    CPC classification number: H01Q15/0086

    Abstract: The present disclosure relates to a metamaterial for diverging an electromagnetic wave, which comprises at least one metamaterial sheet layer. Refractive indices of the metamaterial sheet layer are distributed in a circular form with a center of the metamaterial sheet layer, and the refractive indices remain unchanged at a same radius and increase gradually with the radius. The present disclosure changes electromagnetic parameters at each point of the metamaterial through punching or by attaching man-made microstructures so that the electromagnetic wave can be diverged after passing through the metamaterial. The metamaterial of the present disclosure features a simple manufacturing process and a low cost, and is easy to be implemented. Moreover, the metamaterial of the present disclosure has small dimensions and does not occupy a large space, so it is easy to miniaturize apparatuses made of the metamaterial of the present disclosure.

    Abstract translation: 本公开涉及用于发散电磁波的超材料,其包括至少一个超材料片层。 超材料片层的折射率分布为具有超材料片层的中心的圆形形状,并且折射率在相同半径处保持不变,并随着半径逐渐增加。 本公开通过冲压或通过附接人造微结构来改变超材料的每个点处的电磁参数,使得电磁波可以在通过超材料之后发散。 本公开的超材料具有简单的制造工艺和低成本,并且易于实施。 此外,本公开的超材料具有小的尺寸并且不占据大的空间,因此容易使由本公开的超材料制成的装置小型化。

    Man-made composite material and man-made composite material antenna

    公开(公告)号:US20130002499A1

    公开(公告)日:2013-01-03

    申请号:US13522958

    申请日:2011-11-16

    CPC classification number: H01Q15/08 H01Q19/06

    Abstract: The present invention relates to a man-made composite material and a man-made composite material antenna. The man-made composite material is disposed in a propagation direction of a plane electromagnetic wave and convert it into a spherical wave. Reverse extensions of the spherical wave intersect at a virtual focus. A line connecting the virtual focus to a point on the second surface of the man-made composite material and a line perpendicular to the man-made composite material form an angle θ therebetween, which uniquely corresponds to a curved surface in the man-made composite material. A set formed by points having the same angle θ forms a boundary of the curved surface to which the angle θ uniquely corresponds. Each point on the curved surface to which the angle θ uniquely corresponds has a same refractive index. Refractive indices of the man-made composite material increase gradually as the angle θ increases.

    Impedance matching component, metamaterial panel, converging component and antenna
    15.
    发明授权
    Impedance matching component, metamaterial panel, converging component and antenna 有权
    阻抗匹配元件,超材料面板,会聚部件和天线

    公开(公告)号:US09214735B2

    公开(公告)日:2015-12-15

    申请号:US13522971

    申请日:2011-11-28

    CPC classification number: H01Q15/0086

    Abstract: An impedance matching component is disclosed. The impedance matching component is disposed on and closely attached to a first side surface of a function dielectric sheet. The impedance matching component comprises a first plurality of impedance matching layers, each of which has a refractive index distribution represented as follows: n i ⁡ ( r ) = n m ⁢ ⁢ i ⁢ ⁢ n × ( n g ⁡ ( r ) n m ⁢ ⁢ i ⁢ ⁢ n ) i c + 1 ⁢ ; where, i represents a serial number of each of the impedance matching layers and is a positive integer; ni(r) represents refractive indices of points in the ith impedance matching layer that have a distance of r from a center of the ith impedance matching layer; ng(r) represents refractive indices of points in the function dielectric sheet that have a distance of r from a center of the function dielectric sheet; nmin represents the minimum refractive index of the function dielectric sheet; and c represents the number of the impedance matching layers.

    Abstract translation: 公开了阻抗匹配部件。 阻抗匹配部件设置在功能电介质片的第一侧表面上并且紧密附着在功能电介质片的第一侧表面上。 阻抗匹配部件包括第一多个阻抗匹配层,每个阻抗匹配层的折射率分布表示如下:ni(⁡(r))= nm≠i≠n×(ng⁡(r)nm, n)ic + 1; 其中,i表示每个阻抗匹配层的序号,为正整数; ni(r)表示第i个阻抗匹配层中与第i个阻抗匹配层的中心距离为r的点的折射率; ng(r)表示功能电介质片中与功能电介质片的中心距离为r的点的折射率; nmin表示功能电介质片材的最小折射率; c表示阻抗匹配层的数量。

    FRONT FEED MICROWAVE ANTENNA
    16.
    发明申请
    FRONT FEED MICROWAVE ANTENNA 有权
    前馈麦克风天线

    公开(公告)号:US20140320361A1

    公开(公告)日:2014-10-30

    申请号:US14235079

    申请日:2011-11-24

    Abstract: A front feed microwave antenna, which comprises a radiation source, a first metamaterial panel used for radiating an electromagnetic wave emitted by the radiation source, a second metamaterial panel, and a reflective panel affixed to the back of the first metamaterial panel. The electromagnetic wave is emitted via the first metamaterial panel, refracted by entering the second metamaterial panel, reflected by the reflective panel, and finally re-refracted by reentering the second metamaterial panel, then finally parallel-emitted. Employment of the principle of metamaterial for manufacturing the antenna allows the antenna to break away from restrictions of conventional concave lens shape, convex lens shape, and parabolic shape, thereby allowing the shape of the antenna to be panel-shaped or any shape as desired, while allowing for reduced thickness, reduced size, facilitated processing and manufacturing, reduced costs, and improved gain effect.

    Abstract translation: 一种前馈微波天线,其包括辐射源,用于辐射由辐射源发射的电磁波的第一超材料面板,第二超材料面板和固定到第一超材料面板背面的反射面板。 电磁波通过第一超材料面板发射,通过进入第二超材料面板进行折射,由反射板反射,最后通过重新进入第二超材料面板再次折射,然后最终平行发射。 采用超材料制造天线的原理可以使天线摆脱常规凹透镜形状,凸透镜形状和抛物线形状的限制,从而使天线的形状成为面板形状或任意形状, 同时允许减小厚度,减小尺寸,促进加工和制造,降低成本和改善增益效果。

    Man-made composite material and man-made composite material antenna
    17.
    发明申请
    Man-made composite material and man-made composite material antenna 有权
    人造复合材料和人造复合材料天线

    公开(公告)号:US20130027782A1

    公开(公告)日:2013-01-31

    申请号:US13522964

    申请日:2011-11-16

    CPC classification number: G02B3/0087 H01Q15/02 H01Q19/065

    Abstract: The present invention relates to a man-made composite material and a man-made composite material antenna. The man-made composite material is divided into a plurality of regions. An electromagnetic wave is incident on a first surface exits from a second surface of the man-made composite material opposite to the first surface. A line connecting a radiation source to a point on the bottom surface of the ith region and a line perpendicular to the man-made composite material form an angle θ therebetween, which uniquely corresponds to a curved surface in the ith region. A set formed by points on the bottom surface of the ith region that have the same angle θ forms a boundary of the curved surface to which the angle θ uniquely corresponds. The refraction, diffraction and reflection of the present invention at the abrupt transition points can be reduced.

    Abstract translation: 本发明涉及人造复合材料和人造复合材料天线。 人造复合材料被分成多个区域。 电磁波入射在与第一表面相对的人造复合材料的第二表面上离开的第一表面上。 将辐射源连接到第i区域的底表面上的点和垂直于人造复合材料的线形成角度的线; 其间唯一地对应于第i个区域中的曲面。 由第i个区域的底部表面上具有相同角度和角度的点组成的集合; 形成角度与角度的曲面的边界; 唯一对应。 可以减少本发明在突变转变点的折射,衍射和反射。

    Metamaterial and metamaterial antenna

    公开(公告)号:US20130002500A1

    公开(公告)日:2013-01-03

    申请号:US13522969

    申请日:2011-11-16

    CPC classification number: H01Q15/08 H01Q19/06

    Abstract: The present invention relates to a metamaterial and a metamaterial antenna. The metamaterial is disposed in a propagation direction of the electromagnetic waves emitted from a radiation source. A line connecting the radiation source to a point on a first surface of the metamaterial and a line perpendicular to the metamaterial form an angle θ therebetween, which uniquely corresponds to a curved surface in the metamaterial. Each point on the curved surface to which the angle θ uniquely corresponds has a same refractive index. Refractive indices of the metamaterial decrease gradually as the angle θ increases. The electromagnetic waves propagating through the metamaterial exits in parallel from a second surface of the metamaterial. The refraction, diffraction and reflection at the abrupt transition points can be significantly reduced in the present disclosure and the problems caused by interferences are eased, which further improves performances of the metamaterial and the metamaterial antenna.

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