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    • 2. 发明授权
    • Multiple-frequency common antenna
    • 多频普通天线
    • US07145518B2
    • 2006-12-05
    • US10673336
    • 2003-09-30
    • Makoto TanakaKazuoki MatsugataniHao Xin
    • Makoto TanakaKazuoki MatsugataniHao Xin
    • H01Q15/02H01Q1/00
    • H01Q9/42H01Q9/44H01Q15/008
    • A multiple-frequency common antenna has a first substrate sheet and a second substrate sheet respectively structured by an HIP consisting of a metal plate, small metal plates disposed in two dimensions and linear metal bars connecting these elements. The antenna restricts propagation of surface currents of the first and second frequency bands which are not overlapping with each other. An inverse L-shape antenna and a monopole antenna which are fed with a center conductor and an external conductor of the coaxial line respectively operate as the antenna on the first substrate sheet in the first frequency band and second frequency band. The second substrate sheet does not propagate the radiated wave of the monopole antenna, thereby avoiding unwanted re-radiation.
    • 多频共用天线具有分别由金属板,设置在二维上的小金属板和连接这些元件的线性金属棒构成的HIP构成的第一基板和第二基板。 天线限制彼此不重叠的第一和第二频带的表面电流的传播。 馈送有同轴线的中心导体和外部导体的反向L形天线和单极天线分别在第一频带和第二频带中作为第一基片上的天线工作。 第二基板不传播​​单极天线的辐射波,从而避免不必要的再辐射。
    • 7. 发明授权
    • Dynamic control of planck radiation in photonic crystals
    • 光子晶体中平面辐射的动态控制
    • US07257333B2
    • 2007-08-14
    • US11030621
    • 2005-01-06
    • Ross D RosenwaldNitesh N. ShahDelmar L. BarkerWilliam R. OwensHao Xin
    • Ross D RosenwaldNitesh N. ShahDelmar L. BarkerWilliam R. OwensHao Xin
    • H04B10/04
    • G02B6/1225B82Y20/00
    • A band gap discontinuity is propagated across a Photonic Crystal (PC) to capture thermal energy in a region near the primary emission wavelength of the Planck spectral distribution and transfer that energy to a different spectral region where it is emitted. To extend the range of frequency shifting beyond the width of a single band gap, the intrinsic control parameters (e.g., lattice geometry factors, scattering element geometric factors, and variations in the index of refraction) are spatially varied across the PC to form a band gap gradient. Propagation of the band gap discontinuity, starting in the infrared wavelength region where the thermally generated electromagnetic energy is concentrated and propagating towards the long wavelength region, locally captures the thermal electromagnetic radiation, shifts it downwards in frequency, and pushes the lower-frequency thermal electromagnetic radiation on to the next region. The same principles apply to shift the frequency to shorter wavelengths. A PC-based power combining and waveguide structure can be constructed in the same or a surrounding structure to combine and guide the shifted radiation to an antenna or exit aperture.
    • 通过光子晶体(PC)传播带隙不连续性,以在普朗克光谱分布的主发射波长附近的区域捕获热能,并将该能量转移到其发射的不同光谱区域。 为了将频移的范围扩展到单个带隙的宽度之外,固有控制参数(例如,晶格几何因子,散射元件几何因子和折射率的变化)在PC之间在空间上变化以形成带 间隙梯度。 从热产生的电磁能量集中并向长波长区域传播的红外波长区域开始的带隙不连续的传播局部地捕获热电磁辐射,频率向下移动,并推动低频热电磁 辐射到下一个地区。 相同的原理适用于将频率移动到较短的波长。 基于PC的功率组合和波导结构可以构造在相同或周围的结构中,以将移动的辐射组合并引导到天线或出口孔。