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    • 1. 发明授权
    • Antenna device, array antenna, multi-sector antenna, high-frequency wave transceiver
    • 天线装置,阵列天线,多扇区天线,高频波收发器
    • US07724200B2
    • 2010-05-25
    • US12177935
    • 2008-07-23
    • Nobumasa KitamoriTomohiro Nagai
    • Nobumasa KitamoriTomohiro Nagai
    • H01Q1/38H01Q9/28H01Q21/08
    • H01Q9/285H01Q19/24H01Q19/30H01Q21/08
    • An antenna device having a feeder electrode that extends linearly on a top surface of a dielectric substrate. A balanced electrode having two balanced transmission electrodes vertical to the extending direction of the feeder electrode and extending in parallel. The two balanced transmission electrodes are connected to the feeder electrode and separated by an interval of ½ of a wavelength of a transmission/reception signal. A radiation electrode having a first electrode connected to the one of the two balanced transmission electrodes and a second electrode connected to the other of the two balanced transmission electrodes and is positioned parallel to the feeder electrode. A waveguide electrode is formed at a position separated from the radiation electrode by a predetermined interval and in parallel to the radiation electrode. A ground electrode is formed at an area of a back surface of the dielectric substrate corresponding to an area including a portion where the feeder electrode is positioned. By connecting the two balanced electrodes to the feeder electrode at an interval of ½ of a wavelength in this manner, this branch portion has a signal branching function and a balun function at the same time.
    • 一种天线装置,其具有在电介质基板的顶面上线性延伸的供电电极。 平衡电极,其具有与供电电极的延伸方向垂直且平行延伸的两个平衡的传输电极。 两个平衡的发送电极连接到馈电电极并以发送/接收信号的波长的1/2的间隔隔开。 一种辐射电极,具有连接到所述两个平衡透射电极之一的第一电极和与所述两个平衡透射电极中的另一个连接的第二电极,并且平行于所述馈电电极定位。 波导电极形成在与辐射电极分开预定间隔并与辐射电极平行的位置处。 接地电极形成在电介质基板的背面的与包含供电电极所在部位的区域对应的区域。 通过以这种方式将两个平衡电极以一半的波长连接到馈电电极,该分支部分同时具有信号分支功能和平衡 - 不平衡转换功能。
    • 2. 发明申请
    • Antenna Device, Array Antenna, Multi-Sector Antenna, High-Frequency Wave Transceiver
    • 天线装置,阵列天线,多扇区天线,高频波收发器
    • US20080272976A1
    • 2008-11-06
    • US12177935
    • 2008-07-23
    • Nobumasa KitamoriTomohiro Nagai
    • Nobumasa KitamoriTomohiro Nagai
    • H01Q9/16H01Q9/04
    • H01Q9/285H01Q19/24H01Q19/30H01Q21/08
    • An antenna device having a feeder electrode that extends linearly on a top surface of a dielectric substrate. A balanced electrode having two balanced transmission electrodes vertical to the extending direction of the feeder electrode and extending in parallel. The two balanced transmission electrodes are connected to the feeder electrode and separated by an interval of ½ of a wavelength of a transmission/reception signal. A radiation electrode having a first electrode connected to the one of the two balanced transmission electrodes and a second electrode connected to the other of the two balanced transmission electrodes and is positioned parallel to the feeder electrode. A waveguide electrode is formed at a position separated from the radiation electrode by a predetermined interval and in parallel to the radiation electrode. A ground electrode is formed at an area of a back surface of the dielectric substrate corresponding to an area including a portion where the feeder electrode is positioned. By connecting the two balanced electrodes to the feeder electrode at an interval of ½ of a wavelength in this manner, this branch portion has a signal branching function and a balun function at the same time.
    • 一种天线装置,其具有在电介质基板的顶面上线性延伸的供电电极。 平衡电极,其具有与供电电极的延伸方向垂直且平行延伸的两个平衡的传输电极。 两个平衡的发送电极连接到馈电电极并以发送/接收信号的波长的1/2的间隔隔开。 一种辐射电极,具有连接到所述两个平衡透射电极中的一个的第一电极和与所述两个平衡透射电极中的另一个连接并且平行于所述馈电电极定位的第二电极。 波导电极形成在与辐射电极分开预定间隔并与辐射电极平行的位置处。 接地电极形成在电介质基板的背面的与包含供电电极所在部位的区域对应的区域。 通过以这种方式将两个平衡电极以一半的波长连接到馈电电极,该分支部分同时具有信号分支功能和平衡 - 不平衡转换功能。
    • 3. 发明授权
    • Antenna device and transmitting/receiving device
    • 天线装置和发射/接收装置
    • US07064726B2
    • 2006-06-20
    • US10526448
    • 2003-08-13
    • Nobumasa KitamoriTomohiro Nagai
    • Nobumasa KitamoriTomohiro Nagai
    • H01Q13/00H01Q13/10
    • H01P1/062H01Q3/04H01Q13/02
    • An antenna apparatus includes two circular waveguides including a fixed-side circular waveguide and a rotation-side circular waveguide, each having a propagation mode in a TM01 mode, and being arranged coaxially with each other while a waveguide-side choke is provided between the two waveguides. A rectangular waveguide is connected to the fixed-side circular waveguide. Thereby, the high-frequency signal fed from the rectangular waveguide to the fixed-side circular waveguide can be radiated from a primary radiator to which the rotation-side circular waveguide is connected. While the circular waveguides and the waveguide-side choke can constitute a rotary joint, by rotating the primary radiator together with the rotation-side circular waveguide, scanning can be carried out with a high-frequency signal radiated from the primary radiator.
    • 天线装置包括两个圆形波导,包括固定侧圆形波导和旋转侧圆形波导,每个圆形波导具有TM01模式的传播模式,并且彼此同轴布置,同时在两个波导侧扼流圈之间 波导。 矩形波导连接到固定侧圆形波导。 因此,从矩形波导馈送到固定侧圆形波导的高频信号可以从连接有旋转侧圆形波导的初级辐射器辐射。 虽然圆形波导和波导侧扼流圈可以构成旋转接头,但是通过使主辐射器与旋转侧圆形波导一起旋转,可以用从一次辐射器辐射的高频信号进行扫描。
    • 4. 发明申请
    • Antenna device and transmitting/receiving device
    • 天线装置和发射/接收装置
    • US20050270247A1
    • 2005-12-08
    • US10526448
    • 2003-08-13
    • Nobumasa KitamoriTomohiro Nagai
    • Nobumasa KitamoriTomohiro Nagai
    • H01P1/06H01Q3/04H01Q13/02H01Q21/20H01Q19/06
    • H01P1/062H01Q3/04H01Q13/02
    • An antenna apparatus includes two circular waveguides including a fixed-side circular waveguide and a rotation-side circular waveguide, each having a propagation mode in a TM01 mode, and being arranged coaxially with each other while a waveguide-side choke is provided between the two waveguides. A rectangular waveguide is connected to the fixed-side circular waveguide. Thereby, the high-frequency signal fed from the rectangular waveguide to the fixed-side circular waveguide can be radiated from a primary radiator to which the rotation-side circular waveguide is connected. While the circular waveguides and the waveguide-side choke can constitute a rotary joint, by rotating the primary radiator together with the rotation-side circular waveguide, scanning can be carried out with a high-frequency signal radiated from the primary radiator.
    • 天线装置包括两个圆形波导,包括固定侧圆形波导和旋转侧圆形波导,每个圆形波导具有TM01模式的传播模式,并且彼此同轴布置,同时在两个波导侧扼流圈之间 波导。 矩形波导连接到固定侧圆形波导。 因此,从矩形波导馈送到固定侧圆形波导的高频信号可以从连接有旋转侧圆形波导的初级辐射器辐射。 虽然圆形波导和波导侧扼流圈可以构成旋转接头,但是通过使主辐射器与旋转侧圆形波导一起旋转,可以用从一次辐射器辐射的高频信号进行扫描。
    • 7. 发明授权
    • Waveguide horn antenna array and radar device
    • 波导喇叭天线阵列和雷达装置
    • US07423604B2
    • 2008-09-09
    • US11283802
    • 2005-11-22
    • Tomohiro Nagai
    • Tomohiro Nagai
    • H01Q13/00
    • H01Q21/0037H01Q21/064
    • A conductor member contains a linear feed waveguide extending in a fixed direction and a plurality of horn antennas coupled to the feed waveguide and set at an interval of about one half of a wavelength in the extending direction of the feed waveguide. The horn antennas are formed by horns and coupling waveguides, and the coupling waveguides are set so as to partially enter the feed waveguide. When the size of the spatial coupling portion formed by the entrance is changed, the degree of coupling between the feed waveguide and each of the coupling waveguides changes.
    • 导体构件包括沿固定方向延伸的线性馈电波导和耦合到馈电波导的多个喇叭天线,并且以馈送波导的延伸方向上的波长的大约一半的间隔设置。 喇叭天线由喇叭和耦合波导形成,并且耦合波导被设置成部分地进入馈送波导。 当由入口形成的空间耦合部分的尺寸改变时,馈送波导和每个耦合波导之间的耦合程度发生变化。
    • 8. 发明授权
    • Dielectric lens, dielectric lens device, design method of dielectric lens, manufacturing method and transceiving equipment of dielectric lens
    • 介质透镜,介质透镜装置,介质透镜的设计方法,介质透镜的制造方法和收发设备
    • US07355560B2
    • 2008-04-08
    • US11385658
    • 2006-03-22
    • Tomohiro Nagai
    • Tomohiro Nagai
    • H01Q15/08
    • H01Q15/08
    • A design process first determines a desired aperture distribution, then converts the electric power conservation law, Snell's law on the rear face side of a dielectric lens, and the formula representing light-path-length constraint, into simultaneous equations, and computes the shapes of the surface and rear face of the dielectric lens depending on the azimuthal angle θ of a primary ray from the focal point of the dielectric lens to the rear face of the dielectric lens, and then reduces the light path length in the formula showing light-path-length constraint by an integral multiple of the wavelength when the coordinates on the surface of the dielectric lens reach a predetermined restriction thickness position. A dielectric lens is designed by sequentially changing the lazimuthal angle θ from its initial value, and also repeating the second and third steps. Thus, downsizing and quantification is realized by zoning while keeping antenna properties at the time of constituting a dielectric lens antenna in a good condition.
    • 设计过程首先确定期望的孔径分布,然后将电功率守恒定律,介质透镜背面侧的斯内尔定律和表示光路长度约束的公式转换为联立方程,并计算形状 电介质透镜的表面和背面根据从电介质透镜的焦点到介质透镜的后表面的初级射线的方位角θ,然后在示出光路的公式中减小光路长度 当介质透镜的表面上的坐标达到预定的限制厚度位置时,长度约束是波长的整数倍。 通过从其初始值顺序地改变l角θ而设计介电透镜,并且还重复第二和第三步骤。 因此,通过分区实现小型化和定量化,同时在构成介质透镜天线的状态下保持天线性能。
    • 10. 发明申请
    • Dielectric lens, dielectric lens device, design method of dielectric lens, manufacturing method and transceiving equipment of dielectric lens
    • 介质透镜,介质透镜装置,介质透镜的设计方法,介质透镜的制造方法和收发设备
    • US20060202909A1
    • 2006-09-14
    • US11385658
    • 2006-03-22
    • Tomohiro Nagai
    • Tomohiro Nagai
    • H01Q15/08H01Q15/02
    • H01Q15/08
    • A design process first determines a desired aperture distribution, then converts the electric power conservation law, Snell's law on the rear face side of a dielectric lens, and the formula representing light-path-length constraint, into simultaneous equations, and computes the shapes of the surface and rear face of the dielectric lens depending on the azimuthal angle θ of a primary ray from the focal point of the dielectric lens to the rear face of the dielectric lens, and then reduces the light path length in the formula showing light-path-length constraint by an integral multiple of the wavelength when the coordinates on the surface of the dielectric lens reach a predetermined restriction thickness position. A dielectric lens is designed by sequentially changing the lazimuthal angle θ from its initial value, and also repeating the second and third steps. Thus, downsizing and quantification is realized by zoning while keeping antenna properties at the time of constituting a dielectric lens antenna in a good condition.
    • 设计过程首先确定期望的孔径分布,然后将电功率守恒定律,介质透镜背面侧的斯内尔定律和表示光路长度约束的公式转换为联立方程,并计算形状 电介质透镜的表面和背面根据从电介质透镜的焦点到介质透镜的后表面的初级射线的方位角θ,然后在示出光路的公式中减小光路长度 当介质透镜的表面上的坐标达到预定的限制厚度位置时,长度约束是波长的整数倍。 通过从其初始值顺序地改变l角θ而设计介电透镜,并且还重复第二和第三步骤。 因此,通过分区实现小型化和定量化,同时在构成介质透镜天线的状态下保持天线性能。