JPS63158902A - Waveguide type branching filter - Google Patents
Waveguide type branching filterInfo
- Publication number
- JPS63158902A JPS63158902A JP30716086A JP30716086A JPS63158902A JP S63158902 A JPS63158902 A JP S63158902A JP 30716086 A JP30716086 A JP 30716086A JP 30716086 A JP30716086 A JP 30716086A JP S63158902 A JPS63158902 A JP S63158902A
- Authority
- JP
- Japan
- Prior art keywords
- waveguide
- main
- coupling
- coupling holes
- main waveguide
- 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
Links
- 230000008878 coupling Effects 0.000 claims abstract description 47
- 238000010168 coupling process Methods 0.000 claims abstract description 47
- 238000005859 coupling reaction Methods 0.000 claims abstract description 47
- 210000000554 iris Anatomy 0.000 claims abstract description 10
- 239000002184 metal Substances 0.000 claims description 3
- 230000010287 polarization Effects 0.000 description 20
- 238000010586 diagram Methods 0.000 description 12
- 230000001965 increasing effect Effects 0.000 description 4
- 239000000463 material Substances 0.000 description 2
- 230000006866 deterioration Effects 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000001939 inductive effect Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000035699 permeability Effects 0.000 description 1
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Abstract
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波帯及びミリ波帯で使用される導波
管形分波器に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a waveguide duplexer used in microwave bands and millimeter wave bands.
[従来の技術]
第3図は例えば電子通信学会マイクロ波研究会資料の資
料番号MW72−73(1972年9月)に示された従
来の導波管形分波器を示す概略構成図であり、図におい
て(1)は方形導波管からなる主導波管、(2)は第1
の導波管形帯域通過フィルタ、(3)は第2の導波管形
帯域通過フィルタ、(4)(5)は方形導波管、(6a
)〜(6c) 、 (7a)〜(7c)はアイリス、(
8)(9)は結合孔、(10)は主導波管(1)の短絡
板である6導波管形帯域通過フィルタ(2)及び(3)
は、方形導波管(4)(5)、アイリス(6a)〜(6
c) 、 (7a)〜(7c)及び結合孔(8)(9)
からなり、複数の共振器を構成し、その管軸が主導波管
(1)の管軸と直角になるように接続されている。結合
孔(8)及び(9)は帯域通過フィルタ(2)及び(3
)と主導波管(1)の接続面のほぼ中央に設けられてい
る。また、主導波管(1)の先端は短絡板(10)によ
り短絡されている。[Prior Art] Fig. 3 is a schematic configuration diagram showing a conventional waveguide type duplexer shown in, for example, Material No. MW72-73 (September 1972) of the Microwave Study Group material of the Institute of Electronics and Communication Engineers. In the figure, (1) is the main waveguide made of a rectangular waveguide, and (2) is the first waveguide.
(3) is a second waveguide bandpass filter, (4) and (5) are rectangular waveguides, (6a
) ~ (6c), (7a) ~ (7c) are iris, (
8) Six waveguide bandpass filters (2) and (3), where (9) is the coupling hole and (10) is the shorting plate of the main waveguide (1).
are rectangular waveguides (4) (5), iris (6a) to (6
c) , (7a) to (7c) and binding holes (8) (9)
constitute a plurality of resonators, and are connected so that their tube axes are perpendicular to the tube axis of the main wave tube (1). The coupling holes (8) and (9) are connected to bandpass filters (2) and (3).
) and the main wave tube (1) at approximately the center of the connecting surface. Further, the tip of the main waveguide (1) is short-circuited by a short-circuit plate (10).
次に動作について説明する。第1の帯域通過フィルタ(
2)が周波数f1を中心周波数として通過するよう共振
周波数及びアイリス(6a)〜(6c)の大きさが調整
され、第2の帯域通過フィルタ(3)が周波数f2を中
心周波数として通過するよう共振周波数及びアイリス(
7a)〜(7c)の大きさが調整されており、結合孔(
8)及び(9)と短絡板(10)の距離がそれぞれ周波
数f1及びf2に対する管内振長λg1及び1g8の1
72の整数倍に選ばれていると、主導波管(1)からの
周波数f□及びf2の入射波は短絡板(lO)からの距
離が1g0/2及び1g2/2の整数倍の位置で磁界が
最大となり、その位置に設けられた結合孔(8)及び(
9)を介して効率よく帯域通過フィルタ(2)及び(3
)に分波される。Next, the operation will be explained. The first bandpass filter (
The resonance frequency and the size of the irises (6a) to (6c) are adjusted so that the second bandpass filter (3) passes the frequency f1 as the center frequency, and the second bandpass filter (3) resonates so that the second bandpass filter (3) passes the frequency f2 as the center frequency. Frequency and Iris (
The sizes of 7a) to (7c) are adjusted, and the binding holes (
The distance between 8) and (9) and the shorting plate (10) is 1 of the in-tube vibration lengths λg1 and 1g8 for frequencies f1 and f2, respectively.
72, the incident waves of frequencies f□ and f2 from the main waveguide (1) are located at a distance from the shorting plate (lO) that is an integer multiple of 1g0/2 and 1g2/2. When the magnetic field becomes maximum, the coupling holes (8) and (
9) to efficiently pass bandpass filters (2) and (3).
).
第4図は、この分波器における主導波管(1)と帯域通
過フィルタ(2)の方形導波管(4)との接合部(以下
T分岐部という)を示し、第4図(a)はT分岐部の縦
断面図、第4図(b)はそれの横断面図、第4図(c)
はそれの等価回路図である。等価回路定数Ba及びBb
は次式で与えられる。Figure 4 shows the junction (hereinafter referred to as T branch) between the main waveguide (1) and the rectangular waveguide (4) of the bandpass filter (2) in this duplexer. ) is a longitudinal sectional view of the T-junction, FIG. 4(b) is a cross-sectional view thereof, and FIG. 4(c)
is its equivalent circuit diagram. Equivalent circuit constants Ba and Bb
is given by the following equation.
ただし、Y、は導波管の特性アドミッタンス、a、bは
それぞれ導波管断面の横幅及び高さ、λ。Here, Y is the characteristic admittance of the waveguide, a and b are the width and height of the waveguide cross section, respectively, and λ.
λgはそれぞれ自由空間中及び管内の波長であり、P、
Mはそれぞれ結合孔(8) (9)の周波数特性を考慮
した電気偏極率及び磁気編棒率である。磁気編棒率Mは
結合孔の厚さを無視した場合次式で表わされる。λg are the wavelengths in free space and in the tube, P,
M is an electric polarization ratio and a magnetic braid ratio, respectively, taking into account the frequency characteristics of the coupling holes (8) and (9). The magnetic braid ratio M is expressed by the following equation when the thickness of the coupling hole is ignored.
ここで、Moは結合孔の周波数特性を考慮しない磁気偏
極率、Ωは結合孔の長さである。Qは通常λ/2より小
さな寸法とする。このMを用いて、主導波管(1)と帯
域通過フィルタ(2)及び(3)の結合Qe(外部Q)
及び帯域通過フィルタ内の共振器間の結合k(段間結合
量)は次式で表わされる。Here, Mo is the magnetic polarization ratio without considering the frequency characteristics of the coupling hole, and Ω is the length of the coupling hole. Q is usually a dimension smaller than λ/2. Using this M, the coupling Qe (external Q) of the main waveguide (1) and bandpass filters (2) and (3)
And the coupling k (interstage coupling amount) between resonators in the bandpass filter is expressed by the following equation.
k:!!−MH2・・・・・(5)
ここで、hは主導波管(1)の横断面内の磁界成分、H
は帯域通過フィルタ内の共振器の横断面内の共振磁界成
分、λgは入出力方形導波管(2a)(2b)の管内波
長、μは透磁率である。k:! ! -MH2...(5) Here, h is the magnetic field component in the cross section of the main waveguide (1), H
is the resonant magnetic field component in the cross section of the resonator in the bandpass filter, λg is the tube wavelength of the input/output rectangular waveguides (2a) (2b), and μ is the magnetic permeability.
[発明が解決しようとする問題点1
以上のように構成された従来の導波管形分波器は、広帯
域な特性を得るためには大きな結合量が必要であり、結
合孔の長さΩ或は幅Wを長くする゛必要があった。しか
し、結合孔の長さを長くすると2党が帯域通過フィルタ
の中心周波数f0における自由空間波長λ。に近づくた
め磁気偏極率Mの周波数に対する変化率が大きくなる。[Problem to be solved by the invention 1 The conventional waveguide type duplexer configured as above requires a large amount of coupling in order to obtain broadband characteristics, and the length of the coupling hole Ω Alternatively, it was necessary to increase the width W. However, when the length of the coupling hole is increased, the free space wavelength λ at the center frequency f0 of the bandpass filter becomes two. , the rate of change of the magnetic polarization factor M with respect to frequency becomes large.
第5図はM/M、とλ/λ。の関係を2Q/λ。をパラ
メータにして示したもので、例えば、λlλ。=1にお
いてQが大きくなる程M/M、のλ/λ。に対する傾き
が大きくなっている。このため、周波数変化によって結
合量が大きく変化し、従来の導波管形分波器は広帯域な
通過帯域において良好なVSIIR特性が得られないと
いう問題点があった。また、結合孔の幅を大きくすると
、第6図に示すように磁気偏極率Mは大きくなるが、第
7図に示すように電気偏極率Pも大きくなる。このため
、第4図(b)に示した誘導サセプタンスが大きくなり
、分波特性が劣化するので容量性ポストを設ける必要が
あり大形となるという問題点があった。なお、第7図に
おいてP、は結合孔の周波数特性を考慮しない電気偏極
率である。Figure 5 shows M/M and λ/λ. The relationship is 2Q/λ. is expressed as a parameter, for example, λlλ. = 1, the larger Q is, the λ/λ of M/M. The slope is increasing. For this reason, the amount of coupling changes greatly depending on the frequency change, and the conventional waveguide type duplexer has a problem in that good VSIIR characteristics cannot be obtained in a wide passband. Further, when the width of the coupling hole is increased, the magnetic polarization ratio M increases as shown in FIG. 6, but the electric polarization ratio P also increases as shown in FIG. 7. For this reason, the inductive susceptance shown in FIG. 4(b) becomes large, deteriorating the splitting characteristics, and it is necessary to provide a capacitive post, resulting in a large size. In addition, in FIG. 7, P is an electric polarization rate without considering the frequency characteristics of the coupling hole.
この発明は上記のような問題点を解消するためになされ
たもので、小形で広帯域な通過特性を有する導波管形分
波器を得ることを目的とする。The present invention has been made to solve the above-mentioned problems, and an object of the present invention is to obtain a waveguide duplexer that is small and has broadband pass characteristics.
[問題点を解決するための手段]
この発明に係る導波管形分波器は、主導波管と導波管形
帯域通過フィルタとの接合部における結合孔として、細
長い結合孔を複数個設けたものである。[Means for Solving the Problems] The waveguide duplexer according to the present invention includes a plurality of elongated coupling holes provided as coupling holes at the junction between the main waveguide and the waveguide bandpass filter. It is something that
[作 用]
この発明においては、細長い結合孔を複数個用いている
ため大きな磁気偏極率が得られる。また、結合孔1個当
りの電気偏極率は充分小さいため全体の電気偏極率も小
さく抑えられる。このため容量性ポストを設けることな
く広帯域な分波特性が得られる。[Function] In this invention, a large magnetic polarization ratio can be obtained because a plurality of elongated coupling holes are used. Furthermore, since the electric polarization rate per bonding hole is sufficiently small, the overall electric polarization rate can also be kept small. Therefore, wideband demultiplexing characteristics can be obtained without providing capacitive posts.
[実施例]
以下、この発明の一実施例を図について説明する。第1
図はこの発明の一実施例を示す概略構成図で1図におい
て、(1)は方形導波管からなる主導波管、(2)は第
1の導波管形帯域通過フィルタ、(3)は第2の導波管
形帯域通過フィルタ、 (4)(5)は方形導波管、(
6a)〜(6c) 、 (7a)〜(7c)はアイリス
、(10)は主導波管(1)の短絡板で、以上は第3図
と同様のものである。 (11)(12)は共に複数の
細長い結合孔で、これらは互いに接近して設けられてい
る。[Example] Hereinafter, an example of the present invention will be described with reference to the drawings. 1st
The figure is a schematic configuration diagram showing an embodiment of the present invention. In figure 1, (1) is a main waveguide made of a rectangular waveguide, (2) is a first waveguide band-pass filter, and (3) is a main waveguide made of a rectangular waveguide. is the second waveguide bandpass filter, (4) and (5) are the rectangular waveguides, (
6a) to (6c) and (7a) to (7c) are iris, and (10) is a shorting plate of the main wave tube (1), which are the same as those shown in FIG. 3. (11) and (12) are both a plurality of elongated coupling holes, which are provided close to each other.
この実施例の動作は、第3図に示した従来の導波管形分
波器と同様である。The operation of this embodiment is similar to the conventional waveguide type duplexer shown in FIG.
この分波器では、例えば細長い結合孔(11)(12)
の長さQと横幅Wの比W/Qを0.2とした時、第6図
及び第7図より、M、/ Q ”は0.0g、P、IQ
”は0.007である。この結合孔(11) (!2)
を3個用いた場合、その磁気偏極率、電気偏極率はそれ
ぞれ結合孔が1個の場合の磁気偏極率、電気偏極率を3
倍した値、すなわちM、/ jm ”は0.24、pH
/Q3ハ0.021となる。ところが、結合孔の横幅W
を大きくして結合孔1個でM、/ a ”の値を0.2
4とするには、W/flを0.9とする必要がある。そ
うするとP、IQ3の値は0.072トなり、W/fl
が0.2ノ結合孔を3個用いた場合の約3.4倍の大き
さとなる。従って、同じ大きさの磁気偏極率を得るため
には、1つ結合孔を大きくするより、W/Qの値が小さ
い細長い結合孔を複数個用いる方が電気偏極率を小さく
抑えることができ、分波器の特性劣化を小さくすること
がてきる。この実施例の分波器では、結合孔が複数個あ
るため全てを短絡板(10)からλg/2の整数倍の位
置に配設できないが、磁界分布が正弦波状であるため中
央の結合孔をλg/2の整数倍の位置に配設すれば、複
数の結合孔を接近させて゛設けているので結合孔間の磁
界強度の差は無視し得る程度である。また、結合孔の長
さの2倍2Qを中心周波数f、における自由空間波長λ
。In this duplexer, for example, elongated coupling holes (11) (12)
When the ratio W/Q of length Q and width W of
” is 0.007. This binding hole (11) (!2)
When three are used, the magnetic polarization rate and electric polarization rate are respectively the magnetic polarization rate and electric polarization rate when there is one coupling hole, respectively.
The multiplied value, that is, M, / jm ” is 0.24, pH
/Q3ha becomes 0.021. However, the width W of the coupling hole
By increasing the value of M,/a'' for one bonding hole, the value is 0.2.
4, it is necessary to set W/fl to 0.9. Then, the value of P, IQ3 becomes 0.072, W/fl
is approximately 3.4 times larger than when three 0.2 binding holes are used. Therefore, in order to obtain the same magnitude of magnetic polarization, it is better to use multiple elongated coupling holes with a small W/Q value to keep the electrical polarization smaller than by making one coupling hole larger. This makes it possible to reduce deterioration in the characteristics of the duplexer. In the duplexer of this embodiment, since there are multiple coupling holes, all of them cannot be arranged at positions that are integral multiples of λg/2 from the shorting plate (10), but since the magnetic field distribution is sinusoidal, the coupling holes in the center If they are arranged at positions that are integral multiples of λg/2, the difference in magnetic field strength between the coupling holes is negligible because the plurality of coupling holes are provided close to each other. Also, the free space wavelength λ at the center frequency f is twice the length of the coupling hole 2Q
.
より短くしておけば、周波数変化による磁気偏極率の変
化の問題もなくなる。従って、広帯域にわたって良好な
分波特性が得られる。If it is made shorter, the problem of changes in magnetic polarization due to changes in frequency will also be eliminated. Therefore, good demultiplexing characteristics can be obtained over a wide band.
第2図はこの発明の他の実施例を示す概略構成図で、ア
イリスのかわりに金属ポスト(13a)〜(13c)、
(14a)〜(14c)を用いた場合である。この場合
も第1図に示す実施例と同様に広帯域な分波特性が得ら
れる。FIG. 2 is a schematic configuration diagram showing another embodiment of the present invention, in which metal posts (13a) to (13c) are used instead of the iris.
This is the case when (14a) to (14c) are used. In this case as well, broadband demultiplexing characteristics can be obtained as in the embodiment shown in FIG.
なお、上記実施例では結合孔を3個設けた場合について
述べたが、この発明は結合孔の数が3個に限定されるも
のではない。In the above embodiment, a case was described in which three coupling holes were provided, but the present invention is not limited to three coupling holes.
また、フィルタの段数が3段の場合について説明したが
、この発明はフィルタの段数が3段に限定されるもので
はない。Furthermore, although the case where the number of stages of the filter is three has been described, the present invention is not limited to the number of stages of the filter being three.
[発明の効果]
以上のようにこの発!によれば、細長い結合孔を複数個
設けるため、大きな結合量の広帯域な分波特性を持つ導
波管形分波器が得られるという効果がある。[Effect of the invention] As mentioned above, this invention! According to the method, since a plurality of elongated coupling holes are provided, it is possible to obtain a waveguide type duplexer having a large amount of coupling and a broadband demultiplexing characteristic.
第1図はこの発明の一実施例を示す概略構成図、第2図
はこの発明の他の一実施例を示す概略構成図、第3図は
従来の導波管形分波器を示す概略構成図、第4図はT分
岐部の縦断面図、横断面図及び等価回路図、第5図は磁
気偏極率の周波数特性を示す特性図、第6図は結合孔の
大きさと磁気偏極率との関係を示す特性図、第7図は結
合孔の大きさと電気偏極率との関係を示す特性図である
。
図において、(1)は主導波管、 (2)(3)は導波
管形帯域通過フィルタ、(4)(5)は方形導波管、(
6a)〜(6c) 、(7a) 〜(7c)はアイリス
、(10)は短絡板、(11)(12)は共に複数の細
長い結合孔、(13a)〜(13c) 、 (14a)
〜(14c)は金属ポストである。
なお、図中同一符号は同−或は相当部分を示す。FIG. 1 is a schematic block diagram showing one embodiment of the present invention, FIG. 2 is a schematic block diagram showing another embodiment of the present invention, and FIG. 3 is a schematic diagram showing a conventional waveguide type duplexer. 4 is a longitudinal cross-sectional view, a cross-sectional view, and an equivalent circuit diagram of the T-branch, FIG. 5 is a characteristic diagram showing the frequency characteristics of magnetic polarization, and FIG. 6 is a diagram showing the size of the coupling hole and magnetic polarization. A characteristic diagram showing the relationship between the polarization ratio and FIG. 7 is a characteristic diagram showing the relationship between the size of the bonding hole and the electrical polarization ratio. In the figure, (1) is a main waveguide, (2) and (3) are waveguide bandpass filters, (4) and (5) are rectangular waveguides, (
6a) to (6c), (7a) to (7c) are iris, (10) is a short circuit plate, (11) and (12) are both a plurality of elongated coupling holes, (13a) to (13c), (14a)
- (14c) are metal posts. Note that the same reference numerals in the figures indicate the same or corresponding parts.
Claims (6)
、異なつた通過周波数をもつ2つ以上の導波管形帯域通
過フィルタ、及び上記主導波管と上記導波管形帯域通過
フィルタとの接続面の管壁に設けられた結合孔とで構成
される導波管形分波器において、上記結合孔として、細
長い結合孔を複数個設けたことを特徴とする導波管形分
波器。(1) A main waveguide with one end short-circuited, two or more waveguide bandpass filters coupled to the main waveguide having different pass frequencies, and the main waveguide and the waveguide bandpass filter. A waveguide type duplexer comprising a coupling hole provided in a tube wall on a connection surface with a waveguide type duplexer, characterized in that a plurality of elongated coupling holes are provided as the coupling holes. Wave equipment.
方形導波管で構成されている特許請求の範囲第1項記載
の導波管形分波器。(2) The main waveguide and waveguide type bandpass filter described above are:
The waveguide type duplexer according to claim 1, which is constituted by a rectangular waveguide.
ィルタの管軸とは、互いに直交するよう配設されている
特許請求の範囲第1または第2項記載の導波管形分波器
。(3) The waveguide according to claim 1 or 2, wherein the tube axis of the main waveguide and the tube axis of each of the waveguide bandpass filters are arranged to be orthogonal to each other. shape splitter.
ィルタとの複数の結合孔は、それらの中央の結合孔が上
記主導波管の短絡端から、結合する夫々の導波管形帯域
通過フィルタの通過周波数の管内波長の1/2の整数倍
の位置になるよう配設させてなる特許請求の範囲第1項
〜第3項の何れかに記載の導波管形分波器。(4) A plurality of coupling holes between the main waveguide and the first and second waveguide bandpass filters are such that the coupling hole in the center connects each guide to be coupled from the short-circuited end of the main waveguide. The waveguide type according to any one of claims 1 to 3, which is arranged at a position that is an integral multiple of 1/2 of the pipe wavelength of the pass frequency of the wave tube type band-pass filter. Duplexer.
内部に複数のアイリスを設けた複数の共振器からなるも
のである特許請求の範囲第1項〜第4項の何れかに記載
の導波管形分波器。(5) The first and second waveguide bandpass filters are:
A waveguide type duplexer according to any one of claims 1 to 4, which comprises a plurality of resonators each having a plurality of irises provided therein.
内部に複数対の金属ポストを設けた複数の共振器からな
るものである特許請求の範囲第1項〜第4項の何れかに
記載の導波管形分波器。(6) The first and second waveguide bandpass filters are:
The waveguide type duplexer according to any one of claims 1 to 4, which comprises a plurality of resonators each having a plurality of pairs of metal posts provided inside.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP30716086A JPS63158902A (en) | 1986-12-23 | 1986-12-23 | Waveguide type branching filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP30716086A JPS63158902A (en) | 1986-12-23 | 1986-12-23 | Waveguide type branching filter |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63158902A true JPS63158902A (en) | 1988-07-01 |
Family
ID=17965750
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP30716086A Pending JPS63158902A (en) | 1986-12-23 | 1986-12-23 | Waveguide type branching filter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63158902A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2003289201A (en) * | 2002-03-28 | 2003-10-10 | Anritsu Corp | Post-wall waveguide and junction conversion structure for cavity waveguide |
US7487555B2 (en) | 2002-07-03 | 2009-02-10 | Takeda Leg Wear Co., Ltd. | Socks |
-
1986
- 1986-12-23 JP JP30716086A patent/JPS63158902A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2003289201A (en) * | 2002-03-28 | 2003-10-10 | Anritsu Corp | Post-wall waveguide and junction conversion structure for cavity waveguide |
US7487555B2 (en) | 2002-07-03 | 2009-02-10 | Takeda Leg Wear Co., Ltd. | Socks |
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