THREE DIMENSIONAL FEED THROUGH LENS WITH HEMISPHERICAL COVERAGE
    1.
    发明申请
    THREE DIMENSIONAL FEED THROUGH LENS WITH HEMISPHERICAL COVERAGE 审中-公开
    通过具有HEMISPHERAL覆盖的镜头的三维进给

    公开(公告)号:WO1988006808A2

    公开(公告)日:1988-09-07

    申请号:PCT/US1988000362

    申请日:1988-02-08

    CPC classification number: H01Q3/24 H01Q3/46 H01Q25/00

    Abstract: A lens antenna (10) having four phased array apertures (12, 14, 16, and 18) positioned for hemispherical coverage is disclosed. An array of phase shifters (52) is disclosed, each of which is interconnected with four radiating elements (54, 56, 58, and 60), one on each of the four apertures. A feed horn (30) is used to feed the lens and switches (48, 50) in the lens are used to switch the energy received from the feed horn to the phase shifter, and after phase shifting, to a selected aperture for radiation. The switches also perform a reciprocal function by switching energy received at an aperture to the phase shifter and then to an aperture for radiation to the feed horn. In a further embodiment, the mounting of transmitting and receiving components, such as a high power amplifier (70) and a low noise amplifier (72), with a combination of DPDT switches in the lens is disclosed and results in a solid state T/R type antenna array. In one embodiment, the switches enable the lens to radiate from three of the apertures for a scan angle of 270 degrees from a single feed horn. The addition of mor efeed horns per face results in multiple radiated beams from a single face.

    LOW SIDELOBE SOLID STATE ARRAY ANTENNA APPARATUS AND PROCESS FOR CONFIGURING AN ARRAY ANTENNA APERTURE
    2.
    发明申请
    LOW SIDELOBE SOLID STATE ARRAY ANTENNA APPARATUS AND PROCESS FOR CONFIGURING AN ARRAY ANTENNA APERTURE 审中-公开
    低边缘固体状态阵列天线装置和配置阵列天线孔的过程

    公开(公告)号:WO1988001106A1

    公开(公告)日:1988-02-11

    申请号:PCT/US1987001755

    申请日:1987-07-21

    CPC classification number: H01Q21/22 H01Q21/0025

    Abstract: A low sidelobe, solid state array antenna apparatus comprises a large radiating aperture divided into a large number, N, of small, closely spaced radiating apertures, each small radiating aperture having associated therewith a radiating element and a linearly polarized solid state power module. The large radiating aperture is divided into M, preferably between (3) and about (10), differently sized, elliptically shaped, concentric radiating zones superimposed, for analysis purposes, upon another. Each such zone has an output voltage amplitude, Ei, and semi-major and semi-minor axes of respective lengths, ai and bi, each zone being considered separately in the far field equation: G( theta , PHI ) = [f( theta ,$ gamma ( PHI ) (â theta cos PHI - â PHI sin PHI cos theta )] , wherein f( theta , PHI ) = (I), ui = (II), J1 i is the first order Bessel function, â theta and â PHI are unit vectors in the spherical coordinates and Ko is the wave number associated with the radiated field. Using the far field equation, values of Ei, ai and bi for each zone are computed which result in the far field sidelobe peak gain being a minimum or being a specified number of dB, for example, at least about 30 dB, below the far field mainlobe gain. The values of Ei in overlapping zones are summed to establish the required voltage amplitudes of the underlying power modules associated with the N radiation apertures.

    Abstract translation: 低旁瓣固体阵列天线装置包括被分成大量N个小的紧密间隔的辐射孔的大辐射孔,每个小辐射孔具有辐射元件和线偏振固态功率模块。 大的辐射孔被分成M,优选在(3)和(10)之间,不同尺寸的椭圆形同心辐射区域,用于分析目的叠加在另一个上。 每个这样的区域具有相应长度的输出电压幅度Ei和半主轴和半短轴ai和bi,每个区域在远场方程中分别考虑:G(θ,PHI)= [f ,其中f(θ,PHI)=(I),ui =(II),J1(i)),其中f(θ,PHI) 是第一阶贝塞尔函数,Θ和âPHI是球面坐标中的单位矢量,Ko是与辐射场相关联的波数,使用远场方程,计算每个区域的Ei,ai和bi值 这导致远场旁瓣峰值增益是最小值或者是指定数量的dB,例如至少约30dB,远远于主场主瓣增益,重叠区域中的Ei值相加以建立所需电压 与N个辐射孔相关联的底层功率模块的振幅。

    MILLIMETER-WAVE PHASE SHIFTING DEVICE
    3.
    发明申请
    MILLIMETER-WAVE PHASE SHIFTING DEVICE 审中-公开
    毫米波相移装置

    公开(公告)号:WO1984001472A1

    公开(公告)日:1984-04-12

    申请号:PCT/US1983001438

    申请日:1983-09-16

    CPC classification number: H01P1/19

    Abstract: A millimeter-wave phase shifter for use at high millimeter-wave frequencies. The phase shifter employs continuous aperture ferrite and corrugated horns to make a reciprocal phase shifter in the frequency range of interest. Applied linearly polarized energy is expanded in cross-section by means of a first corrugated horn (23). The expanded energy is focused by a first lens (27), circularly polarized (24) and applied to a ferrite phase shifting section (22). The phase shift applied to the energy is controlled by means of phase control circuitry (28) and a yoke (31) and coil (32) arrangement. The phase-shifted energy is then converted to linearly polarized energy by a second circular polarizer (34) focused by a second lens (37) and contracted in cross-section by a corrugated horn (38). The use of the corrugated horns, polarizers, lenses and ferrite phase shifting components allows a much larger device to be fabricated and hence physical tolerances are reduced by an order of magnitude for the frequency range of interest. In addition, both the efficiency and power handling capability are greatly improved. Both reciprocal and nonreciprocal phase shifters are disclosed.

    CONTINUOUS FERRITE APERTURE FOR ELECTRONIC SCANNING ANTENNAS
    4.
    发明申请
    CONTINUOUS FERRITE APERTURE FOR ELECTRONIC SCANNING ANTENNAS 审中-公开
    电子扫描天线的连续飞盘孔

    公开(公告)号:WO1984001669A1

    公开(公告)日:1984-04-26

    申请号:PCT/US1983001590

    申请日:1983-10-12

    CPC classification number: H01Q3/44

    Abstract: A radiating element (10) having a continuous aperture substantially greater than one half the center frequency wavelength for use in an electronically scanned phased array antenna operating in the range of 94 GHz. The new radiating element comprises a ferrite block (12) having a radiating aperture which measures 5 lambda by 5 lambda in contrast to the conventional discrete radiating element which measures one-half lambda by one-half lambda. A tapered magnetization (see lines 22) is applied to the continuous aperture ferrite block (12). The degree of phase shift can be varied by adjusting the slope of the tapered magnetization. This permits scanning of the continuous aperture pattern. When a plurality of such continuous aperture subarrays is used to form an antenna array (80 or 100), provision is made to adjust the phase at the center of each continuous aperture subarray with respect to the phase of the adjacent subarrays, thereby allowing scanning of the entire pattern of the phased array antenna (100).

    THREE DIMENSIONAL FEED THROUGH LENS WITH HEMISPHERICAL COVERAGE
    5.
    发明公开
    THREE DIMENSIONAL FEED THROUGH LENS WITH HEMISPHERICAL COVERAGE 失效
    与半球网路覆盖范围三维辐射电动镜头。

    公开(公告)号:EP0314713A1

    公开(公告)日:1989-05-10

    申请号:EP88903476.0

    申请日:1988-02-08

    Inventor: TANG, Raymond

    CPC classification number: H01Q3/24 H01Q3/46 H01Q25/00

    Abstract: Radiolentille (10) ayant quatre ouvertures (12, 14, 16, et 18) de réseau piloté en phase positionnées de manière à assurer une couverture hémisphérique. Un agencement de compensateurs de phase (52) dont chacun est interconnecté avec quatre éléments (54, 56, 58 et 60) radiants, un sur chacune des quatre ouvertures. Un cornet d'alimentation (30) est utilisé pour alimenter la lentille, et des commutateurs (48, 50) dans la lentille sont utilisés pour commuter l'énergie reçue du cornet d'alimentation vers les compensateurs de phase, et après compensation de phase, vers une ouverture sélectionnée afin de rayonner. Les commutateurs jouent également un rôle en commutant l'énergie reçue d'une ouverture compensateur de phase et ensuite au cornet d'alimentation. Dans un autre mode de réalisation, le montage de composants transmetteurs et récepteurs, tel qu'un amplificateur (70) de haute puissance et un amplificateur à faible bruit (72), avec une combinaison de commutateurs inverseurs bipolaires et bidirectionnels dans la lentille est divulgué et débouche sur un réseeau d'antenne de type à semi-conducteur transmetteur-récepteur. Dans un mode de réalisation, les commutateurs permettent à la lentille de rayonner à partir de trois des ouvertures, pour un angle de balayage de 270 degrés à partir d'un seul cornet d'alimentation. L'adjonction par face d'autres cornets d'alimentation produit des faisceaux radiant multiples à partir d'une face.

    LOW SIDELOBE SOLID STATE PHASED ARRAY ANTENNA APPARATUS
    6.
    发明授权
    LOW SIDELOBE SOLID STATE PHASED ARRAY ANTENNA APPARATUS 失效
    低侧隙固态相控阵天线装置

    公开(公告)号:EP0275303B1

    公开(公告)日:1993-10-13

    申请号:EP87905342.9

    申请日:1987-07-21

    CPC classification number: H01Q21/22 H01Q21/0025

    Abstract: A low sidelobe, solid state array antenna apparatus comprises a large radiating aperture divided into a large number, N, of small, closely spaced radiating apertures, each small radiating aperture having associated therewith a radiating element and a linearly polarized solid state power module. The large radiating aperture is divided into M, preferably between (3) and about (10), differently sized, elliptically shaped, concentric radiating zones superimposed, for analysis purposes, upon another. Each such zone has an output voltage amplitude, Ei, and semi-major and semi-minor axes of respective lengths, ai and bi, each zone being considered separately in the far field equation: G(,PHI) = [f(PHI) (â cos PHI - âPHI sin PHI cos )]2, wherein f(,PHI) = (I), ui = (II), J1(ui) is the first order Bessel function, â and âPHI are unit vectors in the spherical coordinates and Ko is the wave number associated with the radiated field. Using the far field equation, values of Ei, ai and bi for each zone are computed which result in the far field sidelobe peak gain being a minimum or being a specified number of dB, for example, at least about 30 dB, below the far field mainlobe gain. The values of Ei in overlapping zones are summed to establish the required voltage amplitudes of the underlying power modules associated with the N radiation apertures.

    Abstract translation: 低旁瓣固态阵列天线装置包括被分成大量N个小的,紧密间隔的辐射孔径的大辐射孔径,每个小辐射孔径具有与之相关联的辐射元件和线性极化固态功率模块。 为了分析的目的,将大辐射孔分成M,优选地在(3)和大约(10)之间,不同尺寸的,椭圆形的同心辐射区域叠加在另一个上。 每个这样的区域具有输出电压幅度Ei以及相应长度ai和bi的半长半短轴,每个区域在远场方程中被分别考虑:G(,PHI)= [f(PHI) (ΦPHI - ΦPHIN cos)] 2其中f(,PHI)=(I),ui =(II),J1(ui)是一阶贝塞尔函数,①和③是球面中的单位矢量 坐标和Ko是与辐射场相关的波数。 使用远场方程,计算每个区域的Ei,ai和bi的值,其导致远场旁瓣峰值增益最小或者是规定的dB数量,例如至少大约30dB,低于远处 现场主瓣增益。 叠加区域中的Ei的值被求和以建立与N个辐射孔径相关的底层功率模块的所需电压幅度。

    LOW SIDELOBE SOLID STATE ARRAY ANTENNA APPARATUS AND PROCESS FOR CONFIGURING AN ARRAY ANTENNA APERTURE
    7.
    发明公开
    LOW SIDELOBE SOLID STATE ARRAY ANTENNA APPARATUS AND PROCESS FOR CONFIGURING AN ARRAY ANTENNA APERTURE 失效
    SEMICONDUCTORS相控阵天线含小的边柱。

    公开(公告)号:EP0275303A1

    公开(公告)日:1988-07-27

    申请号:EP87905342.0

    申请日:1987-07-21

    CPC classification number: H01Q21/22 H01Q21/0025

    Abstract: Un appareil d'antenne à réseau à semi-conducteurs à faible rayonnement du lobe latéral comprend une grande ouverture de rayonnement divisée en un grand nombre N, de petites ouvertures de rayonnement étroitement espacées, chaque petite ouverture de rayonnement étant associée à un élément de rayonnement et à un module de puissance à semi-conducteurs polarisé linéairement. La grande ouverture de rayonnement est divisée en M, de préférence entre 3 et environ 10 zones de rayonnement concentriques, de forme elliptique et de dimensions différentes, superposées les unes sur les autres, à des fins d'analyse. Chacune de ces zones possède une amplitude de tension de sortie Ei, et des axes semi-majeurs et semi-mineurs de longueurs respectives, ai et bi, chaque zone étant considérée séparément dans l'équation du champ éloigné G(,PHI) = [f(,PHI) (â cos PHI - âg(F) sin PHI cos ) ]2, dans laquelle f(,PHI) = (I), ui = (II), J1(ui) est la fonction de Bessel de premier ordre, â et âPHI sont des vecteurs unitaires dans les coordonnés sphériques et Ko est le nombre d'ondes associées au champ de rayonnement. A l'aide de l'équation du champ éloigné, les valeurs de Ei, ai et bi pour chaque zone sont calculées, d'où il résulte un gain de crête du lobe latéral du champ éloigné qui se trouve à un minimum ou un nombre spécifique de dB, par exemple au moins 30dB, en dessous du gain du lob principal du champ éloigné. Les valeurs de Ei dans les zones de chevauchement sont aditionnées pour établir les amplitudes de tension requises des modules de puissance sous-jacents associés aux N ouvertures de rayonnement.

    THREE DIMENSIONAL FEED THROUGH LENS WITH HEMISPHERICAL COVERAGE
    8.
    发明授权
    THREE DIMENSIONAL FEED THROUGH LENS WITH HEMISPHERICAL COVERAGE 失效
    通过具有HEMISPHERAL覆盖的镜头的三维进给

    公开(公告)号:EP0314713B1

    公开(公告)日:1993-09-29

    申请号:EP88903476.5

    申请日:1988-02-08

    Inventor: TANG, Raymond

    CPC classification number: H01Q3/24 H01Q3/46 H01Q25/00

    Abstract: A lens antenna (10) having four phased array apertures (12, 14, 16, and 18) positioned for hemispherical coverage is disclosed. An array of phase shifters (52) is disclosed, each of which is interconnected with four radiating elements (54, 56, 58, and 60), one on each of the four apertures. A feed horn (30) is used to feed the lens and switches (48, 50) in the lens are used to switch the energy received from the feed horn to the phase shifter, and after phase shifting, to a selected aperture for radiation. The switches also perform a reciprocal function by switching energy received at an aperture to the phase shifter and then to an aperture for radiation to the feed horn. In a further embodiment, the mounting of transmitting and receiving components, such as a high power amplifier (70) and a low noise amplifier (72), with a combination of DPDT switches in the lens is disclosed and results in a solid state T/R type antenna array. In one embodiment, the switches enable the lens to radiate from three of the apertures for a scan angle of 270 degrees from a single feed horn. The addition of mor efeed horns per face results in multiple radiated beams from a single face.

    MILLIMETER-WAVE PHASE SHIFTING DEVICE
    9.
    发明授权
    MILLIMETER-WAVE PHASE SHIFTING DEVICE 失效
    毫米波相移装置

    公开(公告)号:EP0120915B1

    公开(公告)日:1988-11-30

    申请号:EP83903268.7

    申请日:1983-09-16

    CPC classification number: H01P1/19

    Abstract: A millimeter-wave phase shifter for use at high millimeter-wave frequencies. The phase shifter employs continuous aperture ferrite and corrugated horns to make a reciprocal phase shifter in the frequency range of interest. Applied linearly polarized energy is expanded in cross-section by means of a first corrugated horn (23). The expanded energy is focused by a first lens (27), circularly polarized (24) and applied to a ferrite phase shifting section (22). The phase shift applied to the energy is controlled by means of phase control circuitry (28) and a yoke (31) and coil (32) arrangement. The phase-shifted energy is then converted to linearly polarized energy by a second circular polarizer (34) focused by a second lens (37) and contracted in cross-section by a corrugated horn (38). The use of the corrugated horns, polarizers, lenses and ferrite phase shifting components allows a much larger device to be fabricated and hence physical tolerances are reduced by an order of magnitude for the frequency range of interest. In addition, both the efficiency and power handling capability are greatly improved. Both reciprocal and nonreciprocal phase shifters are disclosed.

    CONTINUOUS FERRITE APERTURE FOR ELECTRONIC SCANNING ANTENNAS
    10.
    发明授权
    CONTINUOUS FERRITE APERTURE FOR ELECTRONIC SCANNING ANTENNAS 失效
    用于电子扫描天线的连续飞盘孔

    公开(公告)号:EP0121568B1

    公开(公告)日:1988-06-01

    申请号:EP83903844.5

    申请日:1983-10-12

    CPC classification number: H01Q3/44

    Abstract: A radiating element (10) having a continuous aperture substantially greater than one half the center frequency wavelength for use in an electronically scanned phased array antenna operating in the range of 94 GHz. The new radiating element comprises a ferrite block (12) having a radiating aperture which measures 5 lambda by 5 lambda in contrast to the conventional discrete radiating element which measures one-half lambda by one-half lambda. A tapered magnetization (see lines 22) is applied to the continuous aperture ferrite block (12). The degree of phase shift can be varied by adjusting the slope of the tapered magnetization. This permits scanning of the continuous aperture pattern. When a plurality of such continuous aperture subarrays is used to form an antenna array (80 or 100), provision is made to adjust the phase at the center of each continuous aperture subarray with respect to the phase of the adjacent subarrays, thereby allowing scanning of the entire pattern of the phased array antenna (100).

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