JPH03195105A - Rectangular waveguide slot array antenna - Google Patents

Rectangular waveguide slot array antenna

Info

Publication number
JPH03195105A
JPH03195105A JP33554289A JP33554289A JPH03195105A JP H03195105 A JPH03195105 A JP H03195105A JP 33554289 A JP33554289 A JP 33554289A JP 33554289 A JP33554289 A JP 33554289A JP H03195105 A JPH03195105 A JP H03195105A
Authority
JP
Japan
Prior art keywords
power
power supply
rectangular waveguide
antenna
metal plates
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.)
Pending
Application number
JP33554289A
Other languages
Japanese (ja)
Inventor
Kunitaka Arimura
國孝 有村
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.)
Arimura Giken KK
Original Assignee
Arimura Giken KK
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 Arimura Giken KK filed Critical Arimura Giken KK
Priority to JP33554289A priority Critical patent/JPH03195105A/en
Publication of JPH03195105A publication Critical patent/JPH03195105A/en
Pending legal-status Critical Current

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  • Variable-Direction Aerials And Aerial Arrays (AREA)
  • Waveguide Aerials (AREA)

Abstract

PURPOSE:To obtain an antenna capable of receiving both satellite broadcast and satellite communication by composing the antenna of a rectangular waveguide line, which is composed of a lot of slots for power radiation arranged in any one of a pair of almost rectangular metal plates, and a feeding means. CONSTITUTION:A pair of almost rectangular metal plates 1 and 2 are arranged so as to be faced each other while being mutually separated, and two openings 5 and 6 for power supply are provided on two faced sides in the lengthwise direction. The rectangular waveguide line is provided to be composed of a lot of slots 1a for power radiation, which are arranged in any one 1 of a pair of metal plates 1 and 2, and feeding means 8 and 9 are provided while being connected to the respective openings 5 and 6 for power supply. Power from the respective feeding means 8 and 9 is supplied as the almost parallel waves of a fundamental mode which electric field direction is parallel to the vertical direction of the openings 5 and 6 for power supply. Thus, both the satellite broadcast and the stellite communication can be received by one antenna. Further, for the antenna, the structure can be made simple and light in weight and production cost can be reduced.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、通f3用アンテナ・放送用アンテナ等に用い
て好適の方形導波管スロットアレイアレイに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a rectangular waveguide slot array array suitable for use in an F3 antenna, a broadcasting antenna, etc.

〔従来の技術〕[Conventional technology]

従来の方形導波管内の伝播モードとしては、第7t21
の直交座標系における電波伝播の説明図(同図(a)は
電磁界分布を示し、(h)は電流分布を示す、)に示す
ように、直交座標系で表される減衰の最も小さい基本モ
ード(T E +。、TE、、波)が用いられる。した
がって方形導波管は、遮断周波数く遮断周波数をrc、
光の速さをC5方形導波管の長辺をaとするとrc= 
c/ 2 a)から他の高次モードの減衰域となるよう
な周波数(f(” =c/a)まての範囲内で使用され
るため、長辺aは、λを自由空間波長とするとa=λ/
1.06〜1.56の範囲にあり、短辺すはほぼa/2
となるのが一般的である。
The propagation mode in the conventional rectangular waveguide is 7t21.
As shown in the explanatory diagram of radio wave propagation in the orthogonal coordinate system ((a) shows the electromagnetic field distribution, and (h) shows the current distribution), the basic principle with the smallest attenuation expressed in the orthogonal coordinate system mode (T E +., TE,, wave) is used. Therefore, the rectangular waveguide has a cutoff frequency rc,
If the speed of light is a, the long side of the C5 rectangular waveguide is rc=
Since it is used within the range from c/2 a) to a frequency (f('' = c/a) that is the attenuation range of other higher-order modes, the long side a is defined by λ as the free space wavelength. Then a=λ/
It is in the range of 1.06 to 1.56, and the short side is approximately a/2
It is common that

そして、従来のスロットアレイアンテナは、上述のよう
な方形導波管の管壁にスロットを切ったものであり、こ
のアンテナでは、第8図の斜視図に示すように、管壁の
電流が半波長λg/2(λgを管内波長とする)ごとに
方向が逆になるので、それに会わせてスロットの傾斜方
向も交互に逆になっている。これにより、一対のスロッ
トから放射される電波のさ成型界のZ成分は同位相とな
って加え3わゼられ、Y成分は逆位相となって相殺され
る。したがって、第8図のような配置の場きは、直線偏
波を放射する。放射される電波の指向性は、XY面では
ビーム幅が16°〜20°と広く、xZ面ではビーノ、
幅がスロワl−のアレイ数に比例して1° 〜2°と秋
くなる。
A conventional slot array antenna is a rectangular waveguide with slots cut into the wall of the rectangular waveguide as described above. In this antenna, as shown in the perspective view of Figure 8, the current in the wall of the tube is reduced by half. Since the directions are reversed every wavelength λg/2 (λg is the tube wavelength), the inclination directions of the slots are also alternately reversed accordingly. As a result, the Z components of the shaping field of the radio waves radiated from the pair of slots are in the same phase and added together, and the Y components are in opposite phase and cancel each other out. Therefore, the arrangement shown in FIG. 8 emits linearly polarized waves. The directivity of the emitted radio waves is wide in the XY plane with a beam width of 16° to 20°, and in the xZ plane with a beam width of 16° to 20°.
The width varies from 1° to 2° in proportion to the number of thrower arrays.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

衛星放送と命星通f、Eとでは、それぞれの電波の到来
方向が約40°違うため、従来それぞれ用に個別にアン
テナを設置する必要があった。
Because the directions of arrival of radio waves for satellite broadcasting and Meisei Dori F and E differ by approximately 40 degrees, it was previously necessary to install separate antennas for each.

また、スロットアレイアンテリ′を攻数並べると、ビー
ム幅を狭くてき、利得を高くてきるが構造が複雑になり
重量がまし、生産コストが高くなるという問題点がある
Furthermore, arranging a number of slot array antennas narrows the beam width and increases the gain, but there are problems in that the structure becomes complicated, the weight increases, and the production cost increases.

本発明は、これらの問題点の解決をはかろうとするもの
で、t17星放送用と衛星通信用との給電部をアンテナ
の左右に別個に取f・1゛け、また、それぞれのビーム
を大きくチルトさせたり、左右円偏波を発生さぜたり、
円偏波直線偏波を発生さぜたりすることにより、1′ノ
のアンテナで、衛星放送と衛星通信とを共に受信できる
とともに、簡単な構造て軽量となり生産コストを下げる
ことができる、方形導波管スロワI・アレイアンテナを
提供することを目的とする。
The present invention attempts to solve these problems by separately installing power feeding parts for T17 star broadcasting and satellite communication on the left and right sides of the antenna, and By tilting it greatly or generating left and right circularly polarized waves,
By generating circularly polarized waves and linearly polarized waves, it is possible to receive both satellite broadcasting and satellite communications with a 1' antenna. The present invention aims to provide a wave tube thrower I array antenna.

〔課題を解決するための手段〕[Means to solve the problem]

このため、本発明の方形導波管スロワI・アレイアンテ
ナは、相互に離隔して対向するように配設されたほぼ1
ノ形な一対の金属板と、同一対の金属板の長さ方向の対
向する二辺に設けられた2つの電力aF、給用開用開口
上記一対の金属板のいずれか一方に列設された多数の電
力放射用スロワ1へとで構成される方形導波管線路と、
上記各電力供給用開口に接続された給電手段とをそなえ
、上記の各給電手段から電力が、電界方向が上記電力供
給用開口の高さ方向に平行な基本モードのほぼ平面波と
して給電されることを特徴としている。
Therefore, the rectangular waveguide thrower I-array antenna of the present invention has approximately one
A pair of metal plates having a shape of a rectangular waveguide line consisting of a large number of power radiation throwers 1;
power supply means connected to each of the power supply openings, and power is supplied from each of the power supply means as a substantially plane wave with a fundamental mode in which the electric field direction is parallel to the height direction of the power supply openings. It is characterized by

〔作  用〕[For production]

上述の本発明の方形導波管スロットアレイアンテリでは
、左右2り所に設けられた給電手段によって方形導波管
線路空間へほぼ平面波である電力が左右から供給される
と、電力放射用スロットを通じて電力が自由空間へ放射
される。
In the rectangular waveguide slot array antenna of the present invention described above, when power, which is substantially a plane wave, is supplied from the left and right to the rectangular waveguide line space by the power feeding means provided at the two left and right places, the power radiation slot Power is radiated into free space through the

そしてまた、上記作用に加えて、左右2つの給電部へそ
れぞれ異なる周波数で電力を給電することにより、1つ
のアンテナで2つの異なる周波数の電波をそれぞれ異な
る方向へ放射する作用が行なわれる。
In addition to the above-mentioned effect, by feeding power at different frequencies to the two left and right power feeding sections, one antenna can radiate radio waves of two different frequencies in different directions.

〔実 施 例〕〔Example〕

以下、図面により本発明の一実施例としての方形導波管
スロットアレイアンテナについて説明すると、第1図は
その斜視図、第2図は第1図のものとは別の形のスロッ
ト配置の場合の斜視図、第3図は導波管中に遅波手段を
配置したスロットアレイアンテナでの電波の遅波率(管
内波長の短縮率)の周波数特性を示すグラフ、第4図お
よび第5図はその指向性を説明する説明図である。第6
図はその給電部の変形例を示した斜視図である。
Below, a rectangular waveguide slot array antenna as an embodiment of the present invention will be explained with reference to the drawings. Fig. 1 is a perspective view thereof, and Fig. 2 shows a case where the slot arrangement is different from that in Fig. 1. Fig. 3 is a graph showing the frequency characteristics of the radio wave slowing rate (shortening rate of the channel wavelength) in a slot array antenna in which slow wave means is arranged in the waveguide, and Figs. 4 and 5. is an explanatory diagram explaining the directivity. 6th
The figure is a perspective view showing a modified example of the power feeding section.

第1図に示すように、相互に離隔して対向するように奥
行きすなわち幅がW(3λ。以上、ここでλ0は自由空
間波長である)、長さがL(Lは10λ0以上でLAW
)のほぼ方形な一対の金属板1゜2が配設され、これら
一対の金属板1,2の長さ方向の向き音う二辺は互いに
金属壁3.4により連結されて内部に方形導波管空間S
を形成している。一対の金属板1.2の幅方向の向き合
う二辺間には、それぞれ電力供給用開口5.6が形成さ
れ、金属板1には幅方向に平行な多数の電力放射用スロ
ットI11が一定間隔のもとに列設されている。そして
、これら金属板1.2と金属壁3.4とで方形導波管線
路が構成されている。導波管線路内部には、電波を遅波
させるための誘電体製の遅波手段7が配置されている。
As shown in Figure 1, the depth or width is W (3λ or more, where λ0 is the free space wavelength) and the length is L (L is 10λ0 or more, where LAW is 10λ0 or more).
), a pair of substantially rectangular metal plates 1 and 2 are arranged, and the two longitudinal sides of the pair of metal plates 1 and 2 are connected to each other by a metal wall 3 and 4, and a rectangular conductor is provided inside. Wave tube space S
is formed. Power supply openings 5.6 are formed between two opposite sides in the width direction of the pair of metal plates 1.2, and a large number of power radiation slots I11 parallel to the width direction are formed at regular intervals in the metal plate 1. They are lined up under the. These metal plates 1.2 and metal walls 3.4 constitute a rectangular waveguide line. Inside the waveguide line, a dielectric slow wave means 7 for slowing down radio waves is arranged.

また電力供給用開口5.6には給電手段としてのホーン
型導波管8.9が接続されている。なお、ホーン型導波
管8.9の内部には誘電体製の電波レンズ10.11が
配設されている。ここではホーン型導波管8,9の内部
に設ける電波レンズ10.11に誘電体を用いたが、こ
れらの遅波手段のほかにも金属板や、コルゲート等の電
波レンズを用いることもてきる。
Further, a horn-shaped waveguide 8.9 as a power supply means is connected to the power supply opening 5.6. Note that a dielectric radio wave lens 10.11 is disposed inside the horn-shaped waveguide 8.9. Here, a dielectric material was used for the radio wave lenses 10 and 11 provided inside the horn-shaped waveguides 8 and 9, but in addition to these slow wave means, it is also possible to use a metal plate, a corrugated wave lens, etc. Ru.

上述の構成により、ホーン型導波管8.9のそれぞれに
電界方向がZ方向を向く電力が給電されると、各々の電
力は、同位相面が仮想波源点を中心とするほぼ同心円状
に伝播していくが、この各々の電力は電波レンズ10.
11を通過する間にほぼ平面波と見なせるモードに変換
される。
With the above-described configuration, when power is supplied to each of the horn-shaped waveguides 8.9 with the electric field direction in the Z direction, the same phase plane of each power is formed in approximately concentric circles centered on the virtual wave source point. The power of each of these propagates through the radio wave lens 10.
11, it is converted into a mode that can be regarded as almost a plane wave.

ポーン型導波管8からBS用の周波数帯の電波を給電し
、ポーン型導波管9からC8用の周波数帯の電波を給″
;すると、両側から給電された電波は、それぞれ電力放
射用スロワ1司」を励振して電力を自由空間に放射する
0周波数と遅波率〈自由空間波長^O1管内波長λgと
して、ξ−λビ/λOとなる〉との関係は、スロットの
特性から第3図のように変化し、スロットの共振周波数
の前後で遅波率は大きく変化する。この性質を利用する
と1つの遅波回路で異なる2つの遅波率を共振周波数の
前後の周波数で得られる。
A radio wave in the frequency band for BS is fed from the pawn type waveguide 8, and a radio wave in the frequency band for C8 is fed from the pawn type waveguide 9.
Then, the radio waves fed from both sides excite the power radiating thrower 1 and radiate the power into free space.The zero frequency and slow wave rate <free space wavelength ^ O1 internal wavelength λg, ξ - λ The relationship between B/λO changes as shown in FIG. 3 depending on the characteristics of the slot, and the slow wave rate changes greatly around the resonant frequency of the slot. By utilizing this property, one slow wave circuit can obtain two different slow wave rates at frequencies before and after the resonant frequency.

ちなみにBSの周波数帯は11.7〜12.0[G[I
zlて、CSの周波数帯は12.25〜12.75が[
[:lIz]である。
By the way, the frequency band of BS is 11.7~12.0[G[I
zlThe frequency band of CS is 12.25 to 12.75 [
[:lIz].

したがって、この画周波数帯の間に共振周波数が存在す
るように設定すると、C3,[3S用にそれぞれに異な
る遅波率が得られる。また、第4図において、信白波長
をλg、自由空間波長をλO,電力放射用スロット間隔
をSP、電力の放射角をθとすると、θ−cos−’ 
(λ。/Sp−λ。/′λビ)というr’A 係が成り
立つので、この2つの異なる遅波率(例えば、[lSの
周波数帯では0.76、CSの周波数帯では0.81)
となる遅波回路を使用し、スロット間隔Spを15.3
mmにすれば、第5図に示すようにBSのビームP1は
正面方向からA方向l\約20°傾!Jることができく
この場合θ−70,26°となる)、C8のビームP2
は正面方向からB方向l\約20’傾0ることができく
この場合θ−70,55°となる)、両名′のビーム間
には約40°の開きが生じる。こりにより、■白のアン
テナてBSとC5との両電波を受信することが可能とな
る。
Therefore, if the resonant frequency is set to exist between the image frequency bands, different slow wave rates can be obtained for C3 and [3S. In addition, in Fig. 4, if the bright white wavelength is λg, the free space wavelength is λO, the power radiation slot interval is SP, and the power radiation angle is θ, then θ-cos-'
Since the r'A relationship (λ./Sp-λ./'λ Bi) holds true, these two different slow wave factors (for example, 0.76 in the [lS frequency band and 0.81 in the CS frequency band) )
Using a slow wave circuit, the slot interval Sp is set to 15.3.
mm, the beam P1 of the BS is tilted at about 20° from the front direction in the A direction, as shown in Figure 5! (in this case θ-70, 26°), beam P2 of C8
can be tilted approximately 20' from the front direction in the B direction (in this case, the angle is θ-70,55°), and there is a gap of approximately 40° between the two beams. This makes it possible for the white antenna to receive both BS and C5 radio waves.

また第2図のようなスロット配置、すなわちス〜]ツト
1aのほかに各スロットIILをはさんで互いに直交す
る傾斜をもつスロット1bと10とからなるスロワ1へ
パターンにすれば、左右円偏波を異なる方向に発生させ
ることもできる。
In addition, if the slots are arranged as shown in Fig. 2, that is, the slot 1 is patterned to include slots 1b and 10, which have slots 1b and 10 that are orthogonal to each other, with each slot IIL in addition to slot 1a, the left and right circular deviation can be achieved. Waves can also be generated in different directions.

また、ビームをチル1へさせる必要があるため、遅波回
路がなくてもスロット間隔が1波長より大きくならない
。よって遅波回路をなくすことも可能である。
Furthermore, since it is necessary to direct the beam to the chill 1, the slot interval does not become larger than one wavelength even without a slow wave circuit. Therefore, it is also possible to eliminate the slow wave circuit.

さらに、金属壁3.4は給電された電力がほぼ下面波と
なるため、取り外すこともてきる。
Furthermore, the metal wall 3.4 can be removed because the supplied power becomes almost a bottom wave.

次に、第6図により給電部の変形例について説明リーる
と、連結孔12a 、 13bを設りられた穴あき導波
管12.13が給電手段として用いられている。そして
ここでは連結孔12m、IIL+が約手波長スロワl−
とされたものが示されている。なおその他の構成は第1
図に示したものと同様である。この構成により給電電力
は、連結孔12a、13bを通して方形導波管空間S内
に平面波として伝播されていく。
Next, referring to FIG. 6, a modification of the power feeding section will be explained. A perforated waveguide 12, 13 provided with connecting holes 12a and 13b is used as the power feeding means. And here, the connecting hole is 12m, and IIL+ is about the wavelength thrower l-
What has been said is shown. The other configurations are as follows.
It is similar to that shown in the figure. With this configuration, the feeding power is propagated as a plane wave into the rectangular waveguide space S through the connecting holes 12a and 13b.

ところζ、連結孔12a 、 13L+は、スロワ1−
の場合はその幅、長さ、傾斜角度および配置などを変え
ることにより、はぼ円形な穴の場合はその大きさを変え
ることにより、方形導波管S内を伝する内部電磁界の分
布を制御でき、これにより放射電力の開口分布を一様に
することができる。その他の作用効果は前述の第1図の
ものの場合と同様である。
However, the connecting holes 12a and 13L+ are connected to the thrower 1-
In the case of a rectangular waveguide S, by changing its width, length, inclination angle, arrangement, etc., and in the case of a roughly circular hole, by changing its size, the distribution of the internal electromagnetic field propagating inside the rectangular waveguide S can be controlled. This allows the aperture distribution of radiated power to be made uniform. Other functions and effects are the same as those in FIG. 1 described above.

なお、給電手段としてはこれらの実施例のほかに、オフ
セット型反射鏡、グレゴリアン型反射鏡、カセグレン型
反射鏡およびパラボラ型反射鏡等を用いることができる
。その場合も前述の第1図のものの場合と同様な作用効
果が得られる。
In addition to these embodiments, an offset type reflector, a Gregorian type reflector, a Cassegrain type reflector, a parabolic type reflector, etc. can be used as the power feeding means. In that case as well, the same effects as in the case of FIG. 1 described above can be obtained.

〔発明の効果〕〔Effect of the invention〕

以上詳述したように、本発明の方形導波管スロットアレ
イアンテナによれば、次のような効果ないし利点が得ら
れる。
As detailed above, according to the rectangular waveguide slot array antenna of the present invention, the following effects and advantages can be obtained.

(1)左右2つの給電部l\それぞれ異なる周波数で電
力を給電することにより、1つのアンテナで2つの異な
る周波数の電波をそれぞれ異なる方向へ放射するアンテ
ナが得られる。
(1) By feeding power at different frequencies to the two left and right power feeding sections, an antenna that radiates radio waves at two different frequencies in different directions can be obtained using one antenna.

(2)上記(1)の理由により、衛星放送と衛星通信と
を共に受信可能なアンテナを得ることができる。
(2) Due to the reason (1) above, it is possible to obtain an antenna that can receive both satellite broadcasting and satellite communication.

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

第1〜4図は本発明の一実施例としての方形導波管スロ
ットアレイアンテナを示すもので、第1図はその斜視図
、第2図は第1図のものと異なったスロワ1〜配列をそ
なえたものの斜視図、第3図は遅波率と周波数の関係を
示すグラフ、第11図およ第5図はいずれもその指向性
を説明する説明図、第6図は第1図のものと異なった給
電部をそなえたものの斜視図、第7〜8図は従来の技術
を示すもので、第7図(a)JUよび(b)はいずれも
その直交座標系における電波伝播の説明図、第8図はそ
のストフッI・アレイアンテナの斜視図。 1.2・・・金属板、la、11+・・・電力放射用ス
ロット、3、・・1・・・金属壁、5,6・・・電力供
給用開口、7−・・遅波回路、8.9・・・ホーン型導
波管、10.11・・・ホーン型導波管、12.13・
・・方形導波管、13m 、 14m・・連結孔、S・
・方形導波管空間、SP・・・スロット間隔、d・・・
方形導波管線路の高さ、W・・・方形導波管線路の幅、
L・・・方形導波管線路の長さ、p、pt、Pz・・・
主tコープ。
1 to 4 show a rectangular waveguide slot array antenna as an embodiment of the present invention, FIG. 1 is a perspective view thereof, and FIG. Fig. 3 is a graph showing the relationship between slow wave rate and frequency, Fig. 11 and Fig. 5 are both explanatory diagrams explaining the directivity, and Fig. 6 is a graph showing the relationship between the slow wave rate and frequency. Figures 7 and 8, which are perspective views of a device equipped with a different power feeding section, show the conventional technology, and Figures 7 (a), JU, and (b) both explain radio wave propagation in the orthogonal coordinate system. FIG. 8 is a perspective view of the Stiff I array antenna. 1.2... Metal plate, la, 11+... Slot for power radiation, 3,... 1... Metal wall, 5, 6... Opening for power supply, 7-... Slow wave circuit, 8.9... Horn type waveguide, 10.11... Horn type waveguide, 12.13.
・・Square waveguide, 13m, 14m・・Connection hole, S・
・Square waveguide space, SP...Slot spacing, d...
Height of rectangular waveguide line, W...width of rectangular waveguide line,
L...Length of rectangular waveguide line, p, pt, Pz...
Main t corp.

Claims (1)

【特許請求の範囲】[Claims] 相互に離隔して対向するように配設されたほぼ方形な一
対の金属板と、同一対の金属板の長さ方向の対向する二
辺に設けられた2つの電力供給用開口と、上記一対の金
属板のいずれか一方に列設された多数の電力放射用スロ
ットとで構成される方形導波管線路と、上記各電力供給
用開口に接続された給電手段とをそなえ、上記の各給電
手段から電力が、電界方向が上記電力供給用開口の高さ
方向に平行な基本モードのほぼ平面波として給電される
ことを特徴とする、方形導波管スロットアレイアンテナ
A pair of substantially rectangular metal plates arranged to face each other and separated from each other, two power supply openings provided on two opposite sides in the length direction of the same pair of metal plates, and the pair of metal plates described above. A rectangular waveguide line consisting of a large number of power radiation slots arranged in a row on either side of the metal plate, and a power supply means connected to each of the power supply openings, each of the above power supply A rectangular waveguide slot array antenna, characterized in that power is supplied from the means as a substantially plane wave with a fundamental mode in which the electric field direction is parallel to the height direction of the power supply aperture.
JP33554289A 1989-12-25 1989-12-25 Rectangular waveguide slot array antenna Pending JPH03195105A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP33554289A JPH03195105A (en) 1989-12-25 1989-12-25 Rectangular waveguide slot array antenna

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP33554289A JPH03195105A (en) 1989-12-25 1989-12-25 Rectangular waveguide slot array antenna

Publications (1)

Publication Number Publication Date
JPH03195105A true JPH03195105A (en) 1991-08-26

Family

ID=18289742

Family Applications (1)

Application Number Title Priority Date Filing Date
JP33554289A Pending JPH03195105A (en) 1989-12-25 1989-12-25 Rectangular waveguide slot array antenna

Country Status (1)

Country Link
JP (1) JPH03195105A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05129832A (en) * 1991-11-07 1993-05-25 Mitsubishi Electric Corp Antenna system and feeding part
WO1999056346A1 (en) * 1998-04-27 1999-11-04 Mitsubishi Denki Kabushiki Kaisha Slot array antenna
JP2011099766A (en) * 2009-11-06 2011-05-19 Furuno Electric Co Ltd Antenna device and radar device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05129832A (en) * 1991-11-07 1993-05-25 Mitsubishi Electric Corp Antenna system and feeding part
WO1999056346A1 (en) * 1998-04-27 1999-11-04 Mitsubishi Denki Kabushiki Kaisha Slot array antenna
JP2011099766A (en) * 2009-11-06 2011-05-19 Furuno Electric Co Ltd Antenna device and radar device

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