JPS59135904A - Electronic scanning antenna - Google Patents

Electronic scanning antenna

Info

Publication number
JPS59135904A
JPS59135904A JP58010122A JP1012283A JPS59135904A JP S59135904 A JPS59135904 A JP S59135904A JP 58010122 A JP58010122 A JP 58010122A JP 1012283 A JP1012283 A JP 1012283A JP S59135904 A JPS59135904 A JP S59135904A
Authority
JP
Japan
Prior art keywords
phase
phase shifter
electronic scanning
shifter
scanning antenna
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP58010122A
Other languages
Japanese (ja)
Other versions
JPH0449282B2 (en
Inventor
Kuniaki Shiramatsu
白松 邦昭
Koichi Kitajima
北島 耕一
Shinkei Orime
晋啓 折目
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP58010122A priority Critical patent/JPS59135904A/en
Publication of JPS59135904A publication Critical patent/JPS59135904A/en
Publication of JPH0449282B2 publication Critical patent/JPH0449282B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q3/00Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system
    • H01Q3/26Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture
    • H01Q3/30Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture varying the relative phase between the radiating elements of an array
    • H01Q3/34Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture varying the relative phase between the radiating elements of an array by electrical means
    • H01Q3/36Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture varying the relative phase between the radiating elements of an array by electrical means with variable phase-shifters

Landscapes

  • Variable-Direction Aerials And Aerial Arrays (AREA)
  • Radar Systems Or Details Thereof (AREA)

Abstract

PURPOSE:To reduce the side lobe produced by a quantized phase error at beam scanning by adjusting a phase of an input signal of a phase shifter stepwise as specified with a phase adjuster and setting the phase shifter amount of the phase shifter to a prescribed value. CONSTITUTION:The phase of the input signal to a phase shifter 2i relating to the i-th element antenna 1i is adjusted stepwise by using a phase adjuster 9i based on the phase of an output terminal of a transmitter 7, for example as [-alphar<2m>]D, where alpha is an optional constant, (m) is a natural number, (r) is a distance from the center and [X]D is a value formed stepwise by a step width of D closest to the X. In setting the phase shift amount of the phase shifter 2i as expression I by a control signal from a control circuit 5, the phase of the signal applied to the element antenna 1i is expressed as expression II, where [X]B is a digital phase amount quantized by B closest to the X, beta is a constant corresponding to the beam scannig angle, and B and D are minimum unit phase angles. Thus, the side lobe produced by the quantized phase error at beam scanning is reduced.

Description

【発明の詳細な説明】 この発明は、複数の移相器を用いた電子走査アンテナに
関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electronic scanning antenna using multiple phase shifters.

筑1図は、従来の電子走査アンテナを示すもので、 (
1a)〜(1n)ld素子アンテナ、 r2a)〜r2
n)は移相器、C3a)〜(3n)け移相器駆動回路、
C4a)〜(4n)は給電用伝送線路、(5)は制御(
ロ)路、(61け送受信切替器、(7)は送信機、(8
)は受信機である。この電子走査アンテナは制御回路(
5)から制御信号を移相器駆動回路(3a)〜(3n)
に送り;移相器(2a)〜(2n)に移相量を設定する
ことによりビーム方向を制御するものである。算2図に
平面アレーアンテナの素子西装置を示す。この図におい
てXは水平方向、yは垂直方向、 (la)〜(1n)
け累子番会を示す。
Figure 1 shows a conventional electronic scanning antenna.
1a) ~ (1n) LD element antenna, r2a) ~ r2
n) is a phase shifter; C3a) to (3n) are phase shifter drive circuits;
C4a) to (4n) are transmission lines for power supply, and (5) is control (
b) path, (61 transmit/receive switcher, (7) transmitter, (8
) is the receiver. This electronic scanning antenna has a control circuit (
5) to the phase shifter drive circuits (3a) to (3n).
The beam direction is controlled by setting the amount of phase shift in the phase shifters (2a) to (2n). Figure 2 shows the element west device for a planar array antenna. In this figure, X is the horizontal direction, y is the vertical direction, (la) to (1n)
Indicates the number of children.

ところで、従来のこの種アンテナにおいて。By the way, in the conventional antenna of this kind.

ビーム走査にあたっては、@子計算機を用いてB = 
2π/2p(’P:ビット数)なる位相角を最小単位と
して、デジタル的々位相変化を行なわしめるが、各アン
テナ素子には、第3図のような±B/2  なる範囲の
位相誤差(量子化位相誤差)が生じ、このため、電子走
査アンテナの放射パターンにおいて特定の方向に大きな
サイト“ロープが生ずる欠点があっに0 この発明による電子走査アンテナは、前述の従来の欠点
を除去するため、特定の方向に大きなサイドローブを生
じさせる量子化位相誤差を分散させるよう給電用嵌送線
路の電気長を変化せしめるものである。また、実際には
給電用伝送線路の電気長を連続的に変化させて与えるこ
とはできないので、この発fjEのように階段状にして
与えることはハードウェアを実現する上に不可欠なこと
である。算4図はこの発明の実施例を示すもので以下詳
細に説明する。
For beam scanning, use @child computer to calculate B =
Digital phase changes are performed using a phase angle of 2π/2p ('P: number of bits) as the minimum unit, but each antenna element has a phase error (±B/2) as shown in Figure 3. The electronic scanning antenna according to the present invention eliminates the above-mentioned conventional drawbacks. , the electrical length of the feeding transmission line is changed to disperse the quantization phase error that causes large side lobes in a specific direction.Also, in reality, the electrical length of the feeding transmission line is changed continuously. Since it is not possible to change and give the expression fjE, it is essential to give it in a stepwise manner like this expression fjE in order to realize the hardware. Explain.

第4図において、 (ia)〜(1n)は素子アンテナ
、 (2a)−(2n)け移相5 、 (3a)−(3
n)け移相器駆動回路、 (4a)〜(4n)は給電用
伝送回路、(5)は制御回路、(6)は送受信切替器、
(7)は送信様、 (8jは受信機、 (9a)〜(9
n)け位相調整器である。
In Fig. 4, (ia) to (1n) are element antennas, (2a) to (2n) and phase shift 5, (3a) to (3
n) phase shifter drive circuit; (4a) to (4n) are power feeding transmission circuits; (5) is a control circuit; (6) is a transmission/reception switch;
(7) is the sender, (8j is the receiver, (9a) to (9
n) phase adjuster.

このようなst成において、1番目の素子アンテナ(1
1)に係る移相器(20の入力何畳の位相を、位相調整
器(91)を用いて1例えば送信機出力端の位相を基準
として、(1)式のように階段状に調整する。
In such a st configuration, the first element antenna (1
1) Adjust the phase of the input of the phase shifter (20) in a stepwise manner as shown in equation (1) using the phase adjuster (91), for example, with the phase of the transmitter output end as a reference .

〔−0γ2m)        ・・・・・・・・・・
・・・・・ (1)ただし、aは任意定数p +””1
 * 21・・・、 n、mは自然数(1、’2 、・
・・)である。ただし、 〔X)Dなる記号はXに一番
近い、Dのステップ幅で階段状にした時の値を意味して
いる。
[-0γ2m) ・・・・・・・・・・・・
... (1) However, a is an arbitrary constant p + ""1
*21..., n, m are natural numbers (1, '2, .
). However, the symbol [X)D means the value when the step width is the step width of D, which is closest to X.

前記移相器(2I)の移相量を制御回路(5)からの制
御信号にて(2)式のように設定すると、素子アンテナ
r11)に供給される信妥の位相は(3)式となる〔6
12m−β遍〕お    ・・・・−・・・・・・−・
・・(2)〔6γ2m−β、〕 −(、γ 〕0   ・・・・・・・・・・・・・・・
(3)ただし、[:XJ なる記号は、Xに一番近い。
When the phase shift amount of the phase shifter (2I) is set as shown in equation (2) using the control signal from the control circuit (5), the reliable phase supplied to the element antenna r11) is calculated as shown in equation (3). becomes [6
12m-β journey〕・・・・-・・・・・・-・
・・・(2) [6γ2m−β,] −(, γ ) 0 ・・・・・・・・・・・・・・・
(3) However, the symbol [:XJ is closest to X.

Bで量子化されたデジタル位相量をとることを意味して
いる。βはビーム走査角に対応する定数。
This means that the digital phase amount quantized by B is taken. β is a constant corresponding to the beam scanning angle.

これエリ、電子走査アンテナ全体としての放射パターン
E(のは、アンテナ素子間隔なd、伝搬定数にとすれば
(4)式で表わされ、(4)式が最大とたる主ロープ方
向は(6)式で表わされる。
In this case, the radiation pattern E of the electronic scanning antenna as a whole (is the antenna element spacing d, and the propagation constant is expressed by equation (4), and the main rope direction where equation (4) is maximum is ( 6) It is expressed by the formula.

E(θ)=f、、eJ kd l Sl nθjCaγ
′”−β・〕8星=1 −jCαγ2m〕9 e =夕11eJ(kdisinθ−βil jEe   
 ・・・・・・・・・・・・ (4)直=1 斤だし、Iiけi番目の素子アンテナの励振振幅。
E(θ)=f,,eJ kd l Sl nθjCaγ
′”-β・]8 stars=1 −jCαγ2m]9 e=Evening 11eJ(kdisinθ−βil jEe
・・・・・・・・・・・・ (4) Direct = 1 Excitation amplitude of the Ii-th element antenna.

E=〔αγ2m−βl〕 一〔〔αγ 〕ゎ−βI〕 ・・・・・曲・・・(5)
である。
E=[αγ2m-βl] 1 [[αγ]ゎ-βI] ... Song ... (5)
It is.

θ−カー”r−!!−)−9−1,−0−−−−−−、
(61d 更に(4)式に掲げfcE=car2−βr )s−〔
〔aγ21〕9−β1〕は、移相器の不連続性に生ずる
量子化位相誤差CBがOならDも0となる)である。
θ-car"r-!!-)-9-1,-0-------,
(61d Furthermore, given in equation (4), fcE=car2-βr)s-[
[aγ21]9−β1] is (if the quantization phase error CB caused by the discontinuity of the phase shifter is O, then D is also 0).

この誤差について、第5図を用いて説明する。第5図に
おいて、γ0〜γ9け中心から(I+)〜(II+9)
の素子捷での距離を示す。×方向にビームを走査する場
合を考えると、 (1i)〜(li+9)の素子のビー
ム走査に関する定数βIは同じであるが、γ0〜γ9の
距離が異なるため、(5)式のEの値が異なる値となり
2位相誤差が分散される。
This error will be explained using FIG. 5. In Figure 5, (I+) to (II+9) from the center of γ0 to γ9
Indicates the distance in terms of element width. Considering the case where the beam is scanned in the x direction, the constant βI regarding the beam scanning of elements (1i) to (li+9) is the same, but the distances of γ0 to γ9 are different, so the value of E in equation (5) is have different values, and the two phase errors are dispersed.

ここで1位相分布の与え方について図を用いて説明する
。箪6図は位相調整器にて与える位相分布を示す図であ
り、x−y平面がアンテナボアサイト方向に直交する面
で、Z軸が位相を表わすものである。各素子位置を位相
を示す図1であり、原点が0の曲面になっている。次(
二算6図に示す曲面のある断面を考える。第7図は断面
を示す図であり、aは階段状にする前の移相器(2a)
〜(2n)の入力信号の位相分布で1式(1)の〔〕の
中の式で表わされるものであり、bはaを階段状にした
もので式(1)を表わす位相分布である。位相調整器に
はこのbの位相分布を与える。Cけ移相器(2a)〜(
2n)の入力信号の位相分布を打消す位相分布で式(2
)の〔〕の中の第1項72m(r)示す位相分布であり
、dはビーム走査の移相量で2式(2)の〔〕の中のβ
IZ示しているo eはCの位相分布とdの位相分布を
加えた分布であり2式(2)の〔〕の中の式を表わすも
のである。f jd eの分布をディジタル化したもの
で式(2)を表わしている。よって1曲線fとbの合成
が素子アンテナ(1a)〜rln)に与えられる位相分
布である。以上で述べたように、給電用伝送線路の電気
襄を階段上に変化させて与えることができるので71−
ドウエアの実現を可能にしている。
Here, how to give the 1-phase distribution will be explained using diagrams. Figure 6 is a diagram showing the phase distribution given by the phase adjuster, where the xy plane is a plane perpendicular to the antenna boresight direction, and the Z axis represents the phase. FIG. 1 shows the phase of each element position, and is a curved surface with the origin at 0. Next(
Consider a cross section with a curved surface shown in Figure 6. FIG. 7 is a diagram showing a cross section, and a shows the phase shifter (2a) before it is made into a stepped shape.
It is the phase distribution of the input signal of ~(2n), which is expressed by the equation in [ ] of Equation 1 (1), and b is a stepwise version of a, which is the phase distribution that expresses Equation (1). . This phase distribution of b is given to the phase adjuster. C phase shifter (2a) ~ (
Equation (2) is a phase distribution that cancels the phase distribution of the input signal of
) is the phase distribution shown by the first term 72m(r) in [], where d is the phase shift amount of beam scanning and β in [] of Equation (2) is
o e shown in IZ is a distribution obtained by adding the phase distribution of C and the phase distribution of d, and represents the expression in [ ] of Equation 2 (2). The distribution of f jd e is digitized and represents equation (2). Therefore, the combination of one curve f and b is the phase distribution given to the element antennas (1a) to rln). As mentioned above, the electric sill of the power supply transmission line can be changed and provided on the stairs, so 71-
This enables the realization of software.

簗8図はこの発明の一実施例を示すもので第4図に示し
六位相調整器(9a)〜(9n)として位相評整用ディ
ジタル移相器(9a)〜(9n)を用い大ものであり、
原理は前記のものと同様である、第9図はこの発−の他
の実施fjlを示すもので、簗4図に示した位相調整器
(9a)〜(9n)として半固定移相器(9a)〜(9
n)を用いkものである。
Figure 8 shows one embodiment of the present invention, which is shown in Figure 4 and uses digital phase shifters (9a) to (9n) for phase adjustment as the six phase adjusters (9a) to (9n). and
The principle is the same as that described above. Fig. 9 shows another implementation of this generator, in which semi-fixed phase shifters (9a) to (9n) shown in Fig. 4 are used. 9a)~(9
k) using n).

第10図にそれぞれの半固定移相器に与える移相量を示
す図で、これはある断面におけるものである。簗10図
において、 (9a)〜(9n)は半固定移相器、φ0
〜φ3け移相量を示す。第10図に示すように、移相量
は素子位置に対応して、ステップ状の移相器φ1〜φ3
が与えられる。各半固定移相器にはその素子位置に対応
した移相量が与えられるため、ブロック毎に移相量を変
化させて与えることになる。 1111図にブロック化
の様子な示す。図において(1a)〜(1n)は素子ア
ンテナで、 BL、〜BL4が各ブロックの境界である
。第10図の様な断面になっている場合、y7EX1図
のBLlの内倶(の素子はφ0の移相量、 BL、とB
L2の間の素子けφ1の移相量、 BL2とBL3の間
の素子はへの移相量、 BL3と13L4の間の素子け
φ3の移相量が与えられる。
FIG. 10 is a diagram showing the amount of phase shift applied to each semi-fixed phase shifter in a certain cross section. In Figure 10, (9a) to (9n) are semi-fixed phase shifters, φ0
〜φ3 phase shift amount is shown. As shown in FIG. 10, the amount of phase shift is determined by step phase shifters φ1 to φ3 corresponding to the element position.
is given. Since each semi-fixed phase shifter is given a phase shift amount corresponding to its element position, the phase shift amount is changed and given to each block. Figure 1111 shows the state of blocking. In the figure, (1a) to (1n) are element antennas, and BL, to BL4 are the boundaries of each block. When the cross section is as shown in Fig. 10, the inner element of BLl in Fig. y7EX1 has a phase shift amount of φ0, BL, and B
A phase shift amount of element number φ1 between L2, a phase shift amount of element number φ3 between BL2 and BL3, and a phase shift amount of element number φ3 between BL3 and 13L4 are given.

第12図はこの発明の他の実施例を示すもので、算4図
に示した位相調整器(9a)〜(9n)として固定位相
器(9a)〜(9n)を用いたものである。各固定位相
器に与える移相量かブロック化されるのけ第9図に示し
たものと同じであり、この原理は前述のものと同様であ
る。また、この固定位相器は電気長乞変化させることが
できるものならば良く1例えば同軸線路や導波管の長さ
を変化させたものでも良い。
FIG. 12 shows another embodiment of the present invention, in which fixed phase shifters (9a) to (9n) are used as the phase adjusters (9a) to (9n) shown in FIG. The amount of phase shift applied to each fixed phase shifter is divided into blocks as shown in FIG. 9, and the principle is the same as that described above. Further, this fixed phase shifter may be of any type as long as it can change the electrical length; for example, it may be one in which the length of a coaxial line or waveguide is changed.

この発りによると、量子化位相誤差が分散され、特定方
向に生ずる大きなサイドローブを低減することができる
According to this idea, the quantization phase error is dispersed, and large side lobes occurring in a specific direction can be reduced.

【図面の簡単な説明】[Brief explanation of the drawing]

簗1図は従来の電子走査アンテナを示す概略図、第2図
は平面アレーアンテナの素子配置を示す図、簗3図は従
来のアンテナにおける量子化位相誤差を示す図、第4図
はこの発明によるアンテナの一実施9ilを示す概略図
、筆5図は中心から素子までの距離を示す図2軍6図は
位相調整器に与える位相分布を図す図、算7図は第6図
に示す位相分布の断面図、算8図はこの発明の一実施伝
を示す概略図、胆9図はこの発明の他の実施例を示す概
略図2第10図は移相器に与える移相量を示す図、第1
1図は移相量がブロック化されることを示す図、第12
図はこの発明の他の実施例を示す概略図であり、 (i
a)〜(10)は素子アンテナ、 (2a’1〜(2n
)け移相器、 (3a)〜(3n)け移相器駆動回路、
 (4a)〜(4n)は給電用伝送線路、(5)は制御
回路、(6)は送受信切替器、(7)は送信機、(8)
は受信機、 C9a)〜(9n)は位相調整器、γ0〜
γ9け中心からの距離、Xは水平方向、yは垂直方向暑
示す。 なお1図中同一あるいは相当部分には同−符号を付して
示しである。 代理人  葛 野 信 − 策1図 第2図 替 第4図 第5図 ) 第6図 第8図 第9図 第10図 第11図 第12図
Figure 1 is a schematic diagram showing a conventional electronic scanning antenna, Figure 2 is a diagram showing the element arrangement of a planar array antenna, Figure 3 is a diagram showing the quantization phase error in the conventional antenna, and Figure 4 is a diagram showing the present invention. Figure 5 shows the distance from the center to the element. Figure 6 shows the phase distribution given to the phase adjuster. Figure 7 shows the phase distribution given to the phase adjuster. A cross-sectional view of the phase distribution, Fig. 8 is a schematic diagram showing one embodiment of the present invention, Fig. 9 is a schematic diagram showing another embodiment of the invention, and Fig. 10 shows the amount of phase shift given to the phase shifter. Figure shown, 1st
Figure 1 shows that the amount of phase shift is divided into blocks, Figure 12
The figure is a schematic diagram showing another embodiment of the present invention, (i
a) to (10) are element antennas, (2a'1 to (2n
) phase shifter, (3a) to (3n) phase shifter drive circuit,
(4a) to (4n) are power feeding transmission lines, (5) is a control circuit, (6) is a transmission/reception switch, (7) is a transmitter, (8)
is the receiver, C9a) to (9n) are the phase adjusters, and γ0 to
The distance from the center of γ9, X is the horizontal direction, and y is the vertical direction. Note that the same or corresponding parts in FIG. 1 are indicated by the same reference numerals. Agent Makoto Kuzuno - Plan 1 Figure 2 Change Figure 4 Figure 5) Figure 6 Figure 8 Figure 9 Figure 10 Figure 11 Figure 12

Claims (1)

【特許請求の範囲】 複数の素子アンテナと、複数の素子アンテナそれぞれに
対応して設けられた複数の移相器と、上記複数の移相器
それぞれに対応して設けらtlJr移相器駆動回路と、
上記移相器駆動回路にビーム方向に対応する制御信号を
与える制御回路とを備え、送信機から送られてくるマイ
クロ波信呆に所要量の位相偏位を生じさせて主ビーム方
向を制御するようにしり電子走査アンテナにおいて、前
記移相器の入力信号位相をC−a72m〕。 のように階段状にして与え1位相調整器で調整し、かつ
各移相器の移相量を〔〔αγ ん−β1〕8なる値に設
足することにより、ビーム走査時の量子化位相誤差によ
って生ずるサイドローブを低減するようにしfCトとt
特徴とする電子走査アンテナ。 但し、B及びDけ最小重付位相角、aは(2)位相調整
器として位相調整ルディジタル移相器を用いたことを特
徴とする特許請求節囲第(1)項記載の電子走査アンテ
ナ。 (3)位相調整器として、半固定移相器を用いたことを
特徴とする特許請求範囲軍(1)項記載の電子走査アン
テナ。 (4)位相調整器として固定位相器を用い大ことを特徴
とする特許請求節囲軍(1)項記載の電子走査アンテナ
[Claims] A plurality of element antennas, a plurality of phase shifters provided corresponding to each of the plurality of element antennas, and a tlJr phase shifter drive circuit provided corresponding to each of the plurality of phase shifters. and,
and a control circuit that provides a control signal corresponding to the beam direction to the phase shifter drive circuit, and controls the main beam direction by causing a required amount of phase deviation in the microwave signal sent from the transmitter. In the electronic scanning antenna, the input signal phase of the phase shifter is C-a72m]. The quantization phase during beam scanning can be adjusted by applying a stepwise pattern as shown in FIG. To reduce sidelobes caused by errors, fC and t
Features an electronic scanning antenna. However, B and D are the minimum weighted phase angles, and a is (2) the electronic scanning antenna according to claim clause (1), characterized in that a phase adjustment digital phase shifter is used as the phase adjustment device. . (3) The electronic scanning antenna according to claim (1), characterized in that a semi-fixed phase shifter is used as the phase adjuster. (4) The electronic scanning antenna according to claim (1), characterized in that a fixed phase shifter is used as the phase adjuster.
JP58010122A 1983-01-25 1983-01-25 Electronic scanning antenna Granted JPS59135904A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58010122A JPS59135904A (en) 1983-01-25 1983-01-25 Electronic scanning antenna

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58010122A JPS59135904A (en) 1983-01-25 1983-01-25 Electronic scanning antenna

Publications (2)

Publication Number Publication Date
JPS59135904A true JPS59135904A (en) 1984-08-04
JPH0449282B2 JPH0449282B2 (en) 1992-08-11

Family

ID=11741490

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58010122A Granted JPS59135904A (en) 1983-01-25 1983-01-25 Electronic scanning antenna

Country Status (1)

Country Link
JP (1) JPS59135904A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61154203A (en) * 1984-12-26 1986-07-12 Toshiba Corp Circularly polarized wave array antenna
JPS63275207A (en) * 1987-05-06 1988-11-11 Mitsubishi Electric Corp Antenna apparatus
GB2470224A (en) * 2009-05-15 2010-11-17 Louis David Thomas A phase shifter for a phased array antenna

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61154203A (en) * 1984-12-26 1986-07-12 Toshiba Corp Circularly polarized wave array antenna
JPS63275207A (en) * 1987-05-06 1988-11-11 Mitsubishi Electric Corp Antenna apparatus
GB2470224A (en) * 2009-05-15 2010-11-17 Louis David Thomas A phase shifter for a phased array antenna

Also Published As

Publication number Publication date
JPH0449282B2 (en) 1992-08-11

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