JPH02180408A - Plane antenna - Google Patents

Plane antenna

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Publication number
JPH02180408A
JPH02180408A JP33460888A JP33460888A JPH02180408A JP H02180408 A JPH02180408 A JP H02180408A JP 33460888 A JP33460888 A JP 33460888A JP 33460888 A JP33460888 A JP 33460888A JP H02180408 A JPH02180408 A JP H02180408A
Authority
JP
Japan
Prior art keywords
output point
polarized wave
array
linearly polarized
synthesized
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
JP33460888A
Other languages
Japanese (ja)
Inventor
Futoshi Deguchi
太志 出口
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.)
DX Antenna Co Ltd
Original Assignee
DX Antenna Co Ltd
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 DX Antenna Co Ltd filed Critical DX Antenna Co Ltd
Priority to JP33460888A priority Critical patent/JPH02180408A/en
Publication of JPH02180408A publication Critical patent/JPH02180408A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To improve the axis ratio characteristic of an antenna and to expand an operating band width by successively differentiating the physical posture of a butch antenna element at every 90 deg. by means of each linearly polarized wave, and successively differentiating the length of a line from an antenna element to the output point of a sub-array at every 1/4 wavelength. CONSTITUTION:Four linearly polarized wave batch antenna elements 11-14 are synthesized at an output point Q of the array in same phase. When received frequencies are set outside central frequencies f0 of the antenna, and respective pairs synthesize elliptically polarized waves, the direction of the elliptically polarized waves synthesized by second pairs 13 and 14 is different from the elliptically polarized wave synthesized by the first pairs 11 and 12 by 180 deg.. However, the direction of the elliptically polarized wave synthesized by the fourth and first antenna elements 14 and 11 is different from the elliptically polarized wave synthesized by the first pair by 270 deg.. As a result, a circularly polarized wave is generated at the array output point Q by synthesizing the elliptically polarized wave. Consequently the band width which can receive the circularly polarized wave can drastically be expanded.

Description

【発明の詳細な説明】 〈産業上の利用分野〉 この発明は、マイクロウェーブ用の指向性平面アンテナ
、特に衛星放送受信用の円偏波マイクロストリップパッ
チアンテナに関する。
DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to a directional planar antenna for microwaves, and in particular to a circularly polarized microstrip patch antenna for satellite broadcast reception.

〈従来の技術〉 第4図に示すような各種の形状の直線偏波パッチアンテ
ナ素子の多数を、平面誘電体基板上に配列した平面アン
テナが、マイクロストリップパッチアンテナとして知ら
れている。同図中の矢印は、素子の方向、即ち物理的姿
勢を示すものである。
<Prior Art> A planar antenna in which a large number of linearly polarized patch antenna elements of various shapes as shown in FIG. 4 are arranged on a planar dielectric substrate is known as a microstrip patch antenna. The arrows in the figure indicate the direction of the element, that is, the physical posture.

第5図に示すように、これらの直線偏波パッチアンテナ
素子l及び2は、2個づってベア3を形成する。ベア3
内においては、素子lと2とは物理的姿勢を90°異に
し、ベアの出力点Pに、線路長が4分の1波長異なる線
路4及び5によって接続されている。
As shown in FIG. 5, two of these linearly polarized patch antenna elements 1 and 2 form a bare 3. bear 3
Inside, the elements 1 and 2 have physical positions different by 90 degrees, and are connected to the bare output point P by lines 4 and 5 whose line lengths are different by a quarter wavelength.

第6図に示すように、2gの同形ベア3.3′は、共通
の出力点Qに、等長の線路6,6′・によって接続され
、サブアレイ7または8を構成する。各サブアレイ内に
おいては、各直線偏波パッチアンテナ素子は4辺形の頂
点上に位置し、素子lと 1′は同姿勢、素子2、2′
は同姿勢である。そして、サブアレイ8は、サブアレイ
7の姿勢を180°回転したものである。
As shown in FIG. 6, 2 g of identical bears 3.3' are connected to a common output point Q by lines 6, 6' of equal length, forming a subarray 7 or 8. Within each subarray, each linearly polarized patch antenna element is located on the vertex of a quadrilateral, with elements l and 1' in the same position, elements 2 and 2'
are in the same position. The subarray 8 is obtained by rotating the attitude of the subarray 7 by 180°.

2個のサブアレイ7と2個のサブアレイ8とは、第7図
Ca)のように組合せられて、16素子アレイ9を構成
する。4個の16素子は第7図(b)のように組合せら
れて64素子アレイ10を構成し、更に4個の64素子
アレイlOは第7図(c)のように組合せられて、25
6素子アレイを構成する。このようにして、平面アンテ
ナ全体では、多数のアレイか、順に上位のアレイを構成
するように結合されて、最終的には1つの出力端に結合
される。
The two sub-arrays 7 and the two sub-arrays 8 are combined as shown in FIG. 7 Ca) to constitute a 16-element array 9. Four 16-element arrays 10 are combined as shown in FIG. 7(b) to form a 64-element array 10, and four 64-element arrays 10 are combined as shown in FIG. 7(c) to form a 25-element array 10.
A 6-element array is constructed. In this way, the entire planar antenna is combined to form multiple arrays or higher order arrays, and finally to one output end.

〈発明が解決しようとする課題〉 上述のアンテナにおける各ベア3は、各直線偏波パッチ
アンテナ素子l及び2の物理的姿勢の違いと、素子から
出力点Pに至る線路長の違いとによって、出力点Pにお
いて円偏波か合成されるように構成されているが、正確
に円偏波が合成されるのは受信周波数がアンテナの中心
周波数foの場合に限られ、受信周波数かfOから外れ
ると、次第に楕円偏波か合成されるようになる。この傾
向は、2つのベア3、3′を組合せてサブアレイ7.8
を構成させても、各サブアレイ内では2つのベアか同姿
勢であるために改善されない。また、4個のサブアレイ
を組合せてアレイ9を構成させる際も、サブアレイ7.
7と8.8とは姿勢か180’違うだけであるから、上
述の傾向は改善されない。そのために軸比特性か悪く、
アンテナの動作帯域幅を拡げることかできない欠点があ
った。
<Problems to be Solved by the Invention> Each bear 3 in the above-mentioned antenna has the following problems due to the difference in the physical posture of each linearly polarized patch antenna element 1 and 2 and the difference in the line length from the element to the output point P. It is configured so that circularly polarized waves are combined at output point P, but circularly polarized waves are accurately combined only when the reception frequency is the antenna center frequency fo, and the reception frequency deviates from fO. Gradually, elliptically polarized waves will be synthesized. This tendency can be seen by combining the two bears 3, 3' into subarray 7.8.
Even if configuring , there is no improvement because within each subarray there are two bears or the same posture. Also, when configuring array 9 by combining four subarrays, subarray 7.
7 and 8.8 are only different in attitude by 180', so the above-mentioned tendency cannot be improved. As a result, the axial ratio characteristics are poor.
The drawback was that the operating bandwidth of the antenna could only be expanded.

く課題を解決するための手段〉 この発明は、上述のような従来の平面アンテナの軸比特
性を改善するために、4個の直線偏波パッチアンテナ素
子によりサブアレイを構成させるに際し、各直線偏波パ
ッチアンテナ素子の物理的姿勢を順に90″づつ異なら
せ、かつこれら直線偏波パッチアンテナ素子から当該サ
ブアレイの出力点に至る線路の長さを順に4分の1波長
づつ異ならせたものである。
Means for Solving the Problems> In order to improve the axial ratio characteristics of the conventional planar antenna as described above, the present invention provides a method for configuring a subarray using four linearly polarized patch antenna elements. The physical postures of the wave patch antenna elements are sequentially varied by 90'', and the lengths of the lines from these linearly polarized patch antenna elements to the output point of the subarray are sequentially varied by 1/4 wavelength. .

望ましい実施態様においては、この発明によるサブアレ
イは、第1及び第2の直線偏波パッチアンテナ素子で構
成される第1のベアと、第3及び第4の直線偏波パッチ
アンテナ素子で構成される第2のベアとからなり、第1
及び第4の直線偏波パッチアンテナ素子は隣接関係lに
あり、第2及び第3の直線偏波パッチアンテナ素子も隣
接関係にある。第2の直線偏波パッチアンテナ素子から
第1のベアの出力点に至る線路長は、第1の直線偏波パ
ッチアンテナ素子から同出力点に至る線路長よりも4分
の1波長だけ長く、同様に第4の直線偏波パッチアンテ
ナ素子から第2のベアの出力点に至る線路長は、第3の
直線偏波パッチアンテナ素子から同出力点に至る線路長
よりも4分の1波長だけ長い、そして、第1のベアの出
力点からアレイの出力点に至る線路長と、第2のベアの
出力点からアレイの出力点に至る線路長とは、2分の1
波長だけ相違する。
In a preferred embodiment, a sub-array according to the invention comprises a first bare comprising first and second linearly polarized patch antenna elements and a third and fourth linearly polarized patch antenna element. the second bear, and the first
and the fourth linearly polarized patch antenna element are in an adjacent relationship l, and the second and third linearly polarized patch antenna elements are also in an adjacent relationship. The line length from the second linearly polarized patch antenna element to the first bare output point is longer by a quarter wavelength than the line length from the first linearly polarized patch antenna element to the same output point, Similarly, the line length from the fourth linearly polarized patch antenna element to the second bare output point is one-quarter wavelength longer than the line length from the third linearly polarized patch antenna element to the same output point. The length of the line from the output point of the first bear to the output point of the array and the length of the line from the output point of the second bear to the output point of the array are 1/2.
Only the wavelength is different.

〈作  用〉 この発明においては、4個の直線偏波パッチアンテナ素
子の電波が、同相でアレイの出力点て合成される。受信
周波数かアンテナの中心層波数f。
<Operation> In this invention, radio waves from four linearly polarized patch antenna elements are combined in phase at the output point of the array. Reception frequency or antenna center layer wave number f.

から外れて、各ベアか楕円偏波を合成するようになった
場合、第2のベアで合成される楕円偏波の方向は、第1
のベアで合成される楕円偏波と180’異なる。しかし
、これらベアの他に、第2と第3のアンテナ素子によっ
て合成される楕円偏波の方向は、第1のベアが合成する
楕円偏波に較べて90°異なり、第4と第1のアンテナ
素子によって合成される楕円偏波の方向は、第1のベア
が合成する楕円偏波に較べて270°異なる。その結果
、アレイの出力点では、これらの方向を異にする楕円偏
波の合成によって、円偏波を生ずる。
If the elliptically polarized waves are synthesized from each bear, the direction of the elliptically polarized waves synthesized by the second bear will be the same as the first one.
It differs by 180' from the elliptically polarized wave synthesized by the bare beam. However, in addition to these bears, the direction of the elliptically polarized waves synthesized by the second and third antenna elements is 90° different from that of the elliptically polarized waves synthesized by the first bear, and The direction of the elliptically polarized waves synthesized by the antenna element differs by 270 degrees from that of the elliptically polarized waves synthesized by the first bear. As a result, at the output point of the array, a circularly polarized wave is produced by combining these elliptically polarized waves having different directions.

従って、円偏波の受信が可能な帯域幅が大幅に拡大され
る。
Therefore, the bandwidth in which circularly polarized waves can be received is greatly expanded.

〈実 施 例〉 第1図において、直線偏波パッチアンテナ素子11、1
2.13.14は物理的姿勢を順に90°づつ変えて、
正方形状にに配置されている。アンテナ素子11と12
とはベアを構成し、ベアの出力点Pに、アンテナ素子1
1は線路15によって接続され、アンテナ素子12は線
路15よりも4分の1波長だけ長い線路16によって接
続されている。同様に、アンテナ素子13と14とはベ
アを構成し、ベアの出力点P′に、アンテナ素子13は
線路15と同じ長さの線路17により、アンテナ素子1
4は線路16と同じ長さの線路18によって、それぞれ
接続されている。そして、一方のベアの出力点Pは線路
19によりアレイの出力点Qに、他方のベアの出力点P
″は線路19よりも半波長だけ長い線路20によりアレ
イの出力点Qに、それぞれ接続されている。21は、出
力点Qに接続された出力線路である。
<Example> In FIG. 1, linearly polarized patch antenna elements 11, 1
2.13.14 change the physical posture by 90 degrees in order,
They are arranged in a square shape. antenna elements 11 and 12
constitutes a bear, and antenna element 1 is attached to the output point P of the bear.
1 are connected by a line 15, and the antenna element 12 is connected by a line 16 which is longer than the line 15 by a quarter wavelength. Similarly, antenna elements 13 and 14 constitute a bare, and antenna element 13 is connected to antenna element 1 by a line 17 having the same length as line 15 at output point P' of the bare.
4 are connected to each other by a line 18 having the same length as the line 16. Then, the output point P of one bear is connected to the output point Q of the array by the line 19, and the output point P of the other bear is connected to the output point P of the other bear.
'' are respectively connected to the output point Q of the array by a line 20 which is longer than the line 19 by half a wavelength. 21 is an output line connected to the output point Q.

第2図は第1図の実施例の変形を示し、各アンテナ素子
11.12.13.14の姿勢が第1図示の実施例とは
45°異なるが、各アンテナ素子の物理的姿勢が順に9
0°相違している点、線路15及び17に較べて線路1
6及び18が4分の1波長だけ長い点、及び線路19に
較べて線路20が2分の1波長だけ長い点については同
じである。
FIG. 2 shows a modification of the embodiment shown in FIG. 1, in which the orientation of each antenna element 11, 12, 13, 14 differs by 45° from the embodiment shown in FIG. 9
0° difference, track 1 compared to tracks 15 and 17
6 and 18 are longer by a quarter wavelength, and the line 20 is longer by a half wavelength than the line 19.

第3図は、第2図に示した4素子アレイを4個で構成し
た16素子アレイを示す、4素子アレイ22a 、 2
2b 、 22c 、 22dは物理的姿勢が順に90
゜づつ異なっている。4素子アレイ22a及び22bの
出力点Qa及びQbは、それぞれ線路23及び24によ
って結合点Rに接続され、4素子アレイ22c及び22
dの出力点Qc及びQdは、それぞれ線路25及び26
によって結合点R′に接続されている。結合点R及びR
′は、それぞれ線路27及び28によって、16素子ア
レイの出力点Sに接続されている。ここで、線路23と
25とは等長であり、線路24及び26は線路23.2
5よりも4分の1波長だけ長い。また、線路28は線路
27よりも2分の1波長だけ長い。
FIG. 3 shows a 16-element array made up of four 4-element arrays shown in FIG. 2, 4-element arrays 22a and 2.
2b, 22c, and 22d have physical postures of 90 in order.
Each degree is different. Output points Qa and Qb of the four-element arrays 22a and 22b are connected to the coupling point R by lines 23 and 24, respectively, and the four-element arrays 22c and 22
The output points Qc and Qd of d are connected to the lines 25 and 26, respectively.
is connected to the connection point R' by. Connection points R and R
' are connected to the output point S of the 16-element array by lines 27 and 28, respectively. Here, the lines 23 and 25 are of equal length, and the lines 24 and 26 are the lines 23.2 and 25.
5 by a quarter wavelength. Further, the line 28 is longer than the line 27 by one-half wavelength.

第8図は、第3図に示した16素子アレイ多数を使用し
たこの発明によるアンテナの軸比−周波数特性(実線)
と、第6図に示した4素子アレイ多数を第7図に示した
態様で使用した従来のアンテナの軸比−周波数特性(点
線)とを示す線図で、軸比1dBのレベルで比較すると
、従来例では±1%弱の帯域幅しか得られないのに対し
、上記実施例では実に±3%強の帯域幅を得ることがで
きる。
FIG. 8 shows the axial ratio-frequency characteristic (solid line) of the antenna according to the present invention using a large number of 16-element arrays shown in FIG.
This is a diagram showing the axial ratio-frequency characteristics (dotted line) of a conventional antenna using the 4-element array shown in Fig. 6 in the manner shown in Fig. 7, and when compared at the level of an axial ratio of 1 dB. In the conventional example, a bandwidth of just less than ±1% can be obtained, whereas in the above embodiment, a bandwidth of just over ±3% can be obtained.

第9図は、上述のこの発明によるアンテナの交差偏波保
護比−周波数特性(実線)と、上述の従来例の交差偏波
保護比−周波数特性(点線)とを示す線図で、交差偏波
保護比25dBのレベルで比較すると、従来例では、 
1.05%の帯域幅しか得られないのに対し、上記実施
例では実に4.25%の帯域幅を得ることができる。
FIG. 9 is a diagram showing the cross-polarization protection ratio-frequency characteristic (solid line) of the antenna according to the present invention described above and the cross-polarization protection ratio-frequency characteristic (dotted line) of the conventional example described above. Comparing at a level with a wave protection ratio of 25 dB, in the conventional example,
While only 1.05% of the bandwidth can be obtained, in the above embodiment, a bandwidth of 4.25% can be obtained.

〈発明の効果〉 以上のように、この発明によるときは、マイクロストリ
ップパッチアンテナの各サブアレイ内での直線偏波パッ
チアンテナ素子の姿勢及び結線を改めることにより、ア
ンテナの軸比特性を改善し、動作帯域幅を大幅に拡げる
ことができる。
<Effects of the Invention> As described above, according to the present invention, the axial ratio characteristics of the antenna are improved by changing the attitude and connection of the linearly polarized patch antenna elements in each subarray of the microstrip patch antenna, The operating bandwidth can be greatly expanded.

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

第1図はこの発明を実施したサブアレイの構成図、第2
図はこの発明によるサブアレイの他の実施例の構成図、
第3図は第2図示のサブアレイを用いた16素子アレイ
の構成図、第4図は従来の各種の直線偏波パッチアンテ
ナ素子の平面図、第5図はアンテナ素子ベアの構成図、
第6図は従来のサブアレイの構成図、第7図は従来の1
6素子アレイ、64素子アレイ及び256素子アレイの
構成図、第8図はこの発明及び従来例のアンテナの軸比
−周波数特性線図、第9図はこの発明及び従来例のアン
テナの交差偏波保護比−周波数特性線図である。 11・・・第1の直線偏波パッチアンテナ素子、12・
・・第2の直線偏波パッチアンテナ素子、13・・・第
3の直線偏波パッチアンテナ素子、14・・・第4の直
線偏波パッチアンテナ素子、15〜21・・・線路、P
・・・第1のベアの出力点、P′・拳・第2のベアの出
力点、Q・・・サブアレイの出力点。 特許出願人 デイエックスアンテナ株式会社代 理 人
  清  水   哲 ほか2名才! 図 才2図 才 図 ヤ 図 才 図 (b) (C) 才5 図 牙 図 周 波 紋(f/f、) 用 戒 敦Cf/f、)
Figure 1 is a configuration diagram of a sub-array implementing this invention, Figure 2
The figure is a configuration diagram of another embodiment of the subarray according to the present invention.
FIG. 3 is a configuration diagram of a 16-element array using the subarray shown in FIG. 2, FIG. 4 is a plan view of various conventional linearly polarized patch antenna elements, and FIG. 5 is a configuration diagram of an antenna element bare.
Figure 6 is a configuration diagram of a conventional sub-array, and Figure 7 is a diagram of a conventional sub-array.
Configuration diagrams of a 6-element array, a 64-element array, and a 256-element array; FIG. 8 is an axial ratio-frequency characteristic diagram of antennas of the present invention and a conventional example; FIG. 9 is a cross-polarization diagram of antennas of the present invention and a conventional example. It is a protection ratio-frequency characteristic diagram. 11... first linearly polarized patch antenna element, 12...
...Second linearly polarized patch antenna element, 13...Third linearly polarized patch antenna element, 14...Fourth linearly polarized patch antenna element, 15-21...Line, P
...output point of the first bear, output point of P', fist, second bear, Q...output point of the sub-array. Patent applicant DAYX Antenna Co., Ltd. Agent Satoshi Shimizu and 2 other talented people! Zuzai 2 Zuzaizu ya Zuzaizu (b) (C) Sai 5 Zugazu frequency ripples (f/f,) Yokai Atsushi Cf/f,)

Claims (1)

【特許請求の範囲】[Claims] (1)平面誘電体基板上に配設され共通のアンテナ出力
点に各々接続されている多数の直線偏波パッチアンテナ
素子を、第1乃至第4の4個づつまとめてサブアレイを
形成させ、各サブアレイ内においては、第1と第2、第
2と第3、第3と第4、第4と第1の直線偏波パッチア
ンテナ素子を互に隣接する形で4辺形の各頂点上に位置
させ、これら直線偏波パッチアンテナ素子を当該サブア
レイの出力点に接続してなり、第1乃至第4の直線偏波
パッチアンテナ素子は、物理的姿勢を順に90°づつ異
にし、かつ順に線路長を4分の1波長づつ異にする線路
によって上記サブアレイの出力点に接続されていること
を特徴とする円偏波の平面アンテナ。
(1) A large number of linearly polarized patch antenna elements arranged on a planar dielectric substrate and connected to a common antenna output point are grouped together into four subarrays (first to fourth), and each Within the subarray, first and second, second and third, third and fourth, and fourth and first linearly polarized patch antenna elements are arranged adjacent to each other on each vertex of the quadrilateral. and these linearly polarized patch antenna elements are connected to the output point of the sub-array, and the first to fourth linearly polarized patch antenna elements have their physical postures sequentially different by 90 degrees and are connected to the line in order. A circularly polarized planar antenna, characterized in that it is connected to the output point of the sub-array by lines whose lengths differ by a quarter wavelength.
JP33460888A 1988-12-29 1988-12-29 Plane antenna Pending JPH02180408A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP33460888A JPH02180408A (en) 1988-12-29 1988-12-29 Plane antenna

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP33460888A JPH02180408A (en) 1988-12-29 1988-12-29 Plane antenna

Publications (1)

Publication Number Publication Date
JPH02180408A true JPH02180408A (en) 1990-07-13

Family

ID=18279285

Family Applications (1)

Application Number Title Priority Date Filing Date
JP33460888A Pending JPH02180408A (en) 1988-12-29 1988-12-29 Plane antenna

Country Status (1)

Country Link
JP (1) JPH02180408A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03151703A (en) * 1989-11-08 1991-06-27 Mitsubishi Electric Corp Antenna system
JPH04354403A (en) * 1991-05-31 1992-12-08 Toshiba Corp array antenna
WO2016047779A1 (en) * 2014-09-26 2016-03-31 日本電気株式会社 Antenna array, wireless communication apparatus, and method for making antenna array
JP2016092564A (en) * 2014-11-04 2016-05-23 株式会社日立国際八木ソリューションズ Circular polarized antenna

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS621304A (en) * 1985-06-25 1987-01-07 コミユニケイシヨンズ サテライト コ−ポレ−シヨン Microstrip antenna array and manufacture thereof
JPS6434002A (en) * 1987-07-30 1989-02-03 Sony Corp Plane antenna

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS621304A (en) * 1985-06-25 1987-01-07 コミユニケイシヨンズ サテライト コ−ポレ−シヨン Microstrip antenna array and manufacture thereof
JPS6434002A (en) * 1987-07-30 1989-02-03 Sony Corp Plane antenna

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03151703A (en) * 1989-11-08 1991-06-27 Mitsubishi Electric Corp Antenna system
JPH04354403A (en) * 1991-05-31 1992-12-08 Toshiba Corp array antenna
WO2016047779A1 (en) * 2014-09-26 2016-03-31 日本電気株式会社 Antenna array, wireless communication apparatus, and method for making antenna array
JP2016092564A (en) * 2014-11-04 2016-05-23 株式会社日立国際八木ソリューションズ Circular polarized antenna

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