JPH1168416A - Dielectric waveguide line - Google Patents

Dielectric waveguide line

Info

Publication number
JPH1168416A
JPH1168416A JP9226174A JP22617497A JPH1168416A JP H1168416 A JPH1168416 A JP H1168416A JP 9226174 A JP9226174 A JP 9226174A JP 22617497 A JP22617497 A JP 22617497A JP H1168416 A JPH1168416 A JP H1168416A
Authority
JP
Japan
Prior art keywords
conductor
line
frequency signal
dielectric
bent portion
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
JP9226174A
Other languages
Japanese (ja)
Inventor
Takeshi Takenoshita
健 竹之下
Hiroshi Uchimura
弘志 内村
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.)
Kyocera Corp
Original Assignee
Kyocera 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 Kyocera Corp filed Critical Kyocera Corp
Priority to JP9226174A priority Critical patent/JPH1168416A/en
Priority to US09/137,195 priority patent/US6057747A/en
Priority to EP98115812A priority patent/EP0898322B1/en
Priority to DE69841265T priority patent/DE69841265D1/en
Priority to EP08021077A priority patent/EP2043192B1/en
Priority to EP03020458A priority patent/EP1396901B1/en
Priority to DE69839785T priority patent/DE69839785D1/en
Priority to EP03020457A priority patent/EP1396903B1/en
Priority to DE69836302T priority patent/DE69836302T2/en
Publication of JPH1168416A publication Critical patent/JPH1168416A/en
Priority to US09/497,792 priority patent/US6380825B1/en
Priority to US09/498,128 priority patent/US6359535B1/en
Pending legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To provide a dielectric waveguide line having high transmission characteristics which do not radiate nor leak electromagnetic waves of a high frequency signal even when a bent part exists in a transmission line and have reduced transmission losses. SOLUTION: This waveguide line is provided with a pair of conductive layers 2 holding a dielectric substrate in-between, and two lines of through conductive groups 4 formed at a repetitive interval (p) less than a half of cutoff wavelength and fixed width (d). In the above structure, bent parts are formed on the two lines of the conductive groups 4, one line arranged on the bent part position is formed like a broken line having one through conductor 6 as a bent point, and the other line is formed like a circular arc having the fixed width (d) as a radius. Consequently the radiation of electromagnetic waves on the bent can be almost eliminated and a high frequency signal can be transmitted with a low transmission loss.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、マイクロ波帯やミ
リ波帯等の高周波信号を伝達するための誘電体導波管線
路に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a dielectric waveguide line for transmitting a high frequency signal in a microwave band, a millimeter wave band or the like.

【0002】[0002]

【従来技術】マイクロ波帯やミリ波帯等の高周波信号を
扱う高周波回路において高周波信号を伝送するための伝
送線路には小型で伝送損失が小さいことが求められてお
り、特に回路を構成する基板上または基板内に形成でき
ると小型化の面で有利となることから、従来、そのよう
な伝送線路としてストリップ線路やマイクロストリップ
線路・コプレナ線路・誘電体導波管線路などが用いられ
てきた。
2. Description of the Related Art In a high-frequency circuit for handling a high-frequency signal such as a microwave band or a millimeter wave band, a transmission line for transmitting a high-frequency signal is required to be small and small in transmission loss. Since it is advantageous in terms of miniaturization if it can be formed on or in a substrate, strip lines, microstrip lines, coplanar lines, dielectric waveguide lines, and the like have been conventionally used as such transmission lines.

【0003】これらのうちストリップ線路・マイクロス
トリップ線路・コプレナ線路は誘電体基板と導体層から
成る信号線路とグランド導体層とで構成されており、信
号線路とグランド導体層の周囲の空間および誘電体中を
高周波信号の電磁波が伝播するものであるが、これらの
線路は30GHz帯域までの信号伝送に対しては問題ない
が、30GHz以上では伝送損失が生じやすい。
[0003] Among them, strip lines, microstrip lines and coplanar lines are composed of a signal line comprising a dielectric substrate and a conductor layer and a ground conductor layer, and the space around the signal line and the ground conductor layer and the dielectric material are formed. Although electromagnetic waves of high-frequency signals propagate through the inside, these lines have no problem for signal transmission up to the 30 GHz band, but transmission loss easily occurs at 30 GHz or higher.

【0004】これに対して導波管型の線路は30GHz以
上のミリ波帯域においても伝送損失が小さい点で有利で
あり、このような導波管の優れた伝送特性を活かし、多
層基板内に形成可能な線路も提案されている。
On the other hand, a waveguide type line is advantageous in that the transmission loss is small even in a millimeter wave band of 30 GHz or more. Formable lines have also been proposed.

【0005】例えば特開平6−53711 号公報において、
誘電体基板を一対の導体層で挟み、さらに導体層間を接
続する2列の複数のビアホールによって側壁を形成した
導波管線路が提案されている。この導波管線路によれ
ば、誘電体材料の四方を導体層とビアホールによる疑似
的な導体壁で囲むことによって導体壁内の領域を信号伝
送用の線路としたものであり、構成がいたって簡単とな
って装置全体の小型化も図り得るというものである。
For example, in JP-A-6-53711,
There has been proposed a waveguide line in which a dielectric substrate is sandwiched between a pair of conductor layers, and a sidewall is formed by a plurality of rows of via holes connecting the conductor layers. According to this waveguide line, the area inside the conductor wall is used as a signal transmission line by surrounding the four sides of the dielectric material with a pseudo conductor wall formed by the conductor layer and the via hole. Thus, the size of the entire apparatus can be reduced.

【0006】[0006]

【発明が解決しようとする課題】一般に、高周波回路を
構成する場合、伝送線路の配線回路において屈曲部を設
けることが避けられないことが多い。
Generally, when a high-frequency circuit is formed, it is often inevitable to provide a bent portion in a wiring circuit of a transmission line.

【0007】ところが、特開平6−53711 号公報に提案
されたような誘電体導波管線路において、その一対の導
体層と2列のビアホールによる疑似的な導体壁で囲まれ
た信号伝送用の線路に単純に屈曲部を設けた場合、電磁
界に乱れが生じることから、伝送損失が大きくなるとい
う問題点があった。
However, in a dielectric waveguide line proposed in Japanese Patent Application Laid-Open No. Hei 6-53711, a signal transmission signal surrounded by a pair of conductor layers and pseudo conductor walls formed by two rows of via holes. When a bent portion is simply provided on a line, there is a problem that a transmission loss increases because an electromagnetic field is disturbed.

【0008】本発明は上記事情に鑑みて案出されたもの
であり、その目的は、伝送線路に屈曲部が存在しても高
周波信号の電磁波の放射・漏洩が無く、伝送損失が小さ
い良好な伝送特性を有する誘電体導波管線路を提供する
ことにある。
SUMMARY OF THE INVENTION The present invention has been made in view of the above circumstances, and has as its object the advantage that even if a bent portion exists in a transmission line, electromagnetic waves of high-frequency signals are not radiated or leaked and transmission loss is small. An object of the present invention is to provide a dielectric waveguide line having transmission characteristics.

【0009】[0009]

【課題を解決するための手段】本発明者等は、上記の問
題点に対して検討を重ねた結果、誘電体導波管線路につ
いて、誘電体基板中に設けた2列のビアホール群の上下
をこれらビアホール群と電気的に導通した一対の導体層
で完全に覆って形成される構造の伝送線路に設けた屈曲
部において2列のビアホール群のビアホールの配列を所
定の配列構造とすることにより、伝送線路に屈曲部が存
在しても高周波信号の電磁波の放射・漏洩がほとんど無
く、低伝送損失の良好な伝送特性とできることを見いだ
した。
Means for Solving the Problems The present inventors have studied the above problems, and as a result, have found that a dielectric waveguide line has two rows of via holes provided in a dielectric substrate. The via holes of the two rows of via holes are arranged in a predetermined arrangement at the bent portion provided in the transmission line having a structure formed by completely covering the pair of conductor layers electrically connected to the via holes. It has been found that even if there is a bent portion in the transmission line, there is almost no radiation and leakage of high-frequency signal electromagnetic waves, and good transmission characteristics with low transmission loss can be achieved.

【0010】本発明の誘電体導波管線路は、誘電体基板
を挟持する一対の導体層と、高周波信号の伝送方向に前
記高周波信号の遮断波長の2分の1以下の繰り返し間隔
で、かつ前記伝送方向と直交する方向に一定の幅で前記
導体層間を電気的に接続するよう形成された2列の貫通
導体群とを具備し、前記導体層および前記貫通導体群に
囲まれた領域によって高周波信号を伝送する誘電体導波
管線路であって、前記2列の貫通導体群はその一部に屈
曲部を有し、この屈曲部に位置する一方の列は1つの貫
通導体を屈曲点とした折れ線状に形成されており、他方
の列は前記1つの貫通導体を中心とし、前記一定の幅を
半径とする円弧状に形成されていることを特徴とするも
のである。
A dielectric waveguide line according to the present invention has a pair of conductor layers sandwiching a dielectric substrate, and a repetition interval in a transmission direction of a high-frequency signal at a half or less of a cutoff wavelength of the high-frequency signal, and A two-row penetrating conductor group formed to electrically connect the conductor layers with a constant width in a direction perpendicular to the transmission direction, and a region surrounded by the conductor layer and the penetrating conductor group. A dielectric waveguide line for transmitting a high-frequency signal, wherein the two rows of through conductor groups have a bent portion in a part thereof, and one row located at the bent portion is connected to one through conductor by a bending point. And the other row is formed in an arc shape having the one width as the center and the radius having the constant width.

【0011】また、本発明の誘電体導波管線路は、誘電
体基板を挟持する一対の導体層と、高周波信号の伝送方
向に前記高周波信号の遮断波長の2分の1以下の繰り返
し間隔で、かつ前記伝送方向と直交する方向に一定の幅
で前記導体層間を電気的に接続するよう形成された2列
の貫通導体群とを具備し、前記導体層および前記貫通導
体群に囲まれた領域によって高周波信号を伝送する誘電
体導波管線路であって、前記2列の貫通導体群はその一
部に屈曲部を有し、この屈曲部に位置する一方の列は1
つの貫通導体を屈曲点とした折れ線状に形成されてお
り、他方の列は前記一方の列の前記屈曲点を頂点とし前
記一定の幅を高さとする二等辺三角形の底辺に対応する
折れ線状に形成されていることを特徴とするものであ
る。
Further, the dielectric waveguide line according to the present invention has a pair of conductor layers sandwiching a dielectric substrate and a repetition interval in a transmission direction of a high-frequency signal at a half or less of a cutoff wavelength of the high-frequency signal. And two rows of through conductor groups formed so as to electrically connect the conductor layers with a constant width in a direction orthogonal to the transmission direction, and are surrounded by the conductor layers and the through conductor groups. A dielectric waveguide line for transmitting a high-frequency signal by a region, wherein the two rows of through conductor groups have a bent portion in a part thereof, and one row located in the bent portion has one bend.
Two through conductors are formed in a polygonal line shape having a bending point, and the other row is a polygonal line shape corresponding to the base of an isosceles triangle having the height of the certain width with the bending point of the one row as a vertex. It is characterized by being formed.

【0012】また、本発明の誘電体導波管線路は、誘電
体基板を挟持する一対の導体層と、高周波信号の伝送方
向に前記高周波信号の遮断波長の2分の1以下の繰り返
し間隔で、かつ前記伝送方向と直交する方向に一定の幅
で前記導体層間を電気的に接続するよう形成された2列
の貫通導体群とを具備し、前記導体層および前記貫通導
体群に囲まれた領域によって高周波信号を伝送する誘電
体導波管線路であって、前記2列の貫通導体群は、その
各列が同心円弧状に配列された屈曲部を有することを特
徴とするものである。
Further, the dielectric waveguide line of the present invention has a pair of conductor layers sandwiching a dielectric substrate and a repetition interval in a transmission direction of a high-frequency signal at a half or less of a cutoff wavelength of the high-frequency signal. And two rows of through conductor groups formed so as to electrically connect the conductor layers with a constant width in a direction orthogonal to the transmission direction, and are surrounded by the conductor layers and the through conductor groups. A dielectric waveguide line for transmitting a high-frequency signal by a region, wherein the two rows of through conductor groups each have a bent portion in which each row is arranged in a concentric arc shape.

【0013】本発明の誘電体導波管線路によれば、誘電
体基板を挟持する一対の導体層と、高周波信号の伝送方
向に前記高周波信号の遮断波長の2分の1以下の繰り返
し間隔で、かつ前記伝送方向と直交する方向に一定の幅
で前記導体層間を電気的に接続するよう形成された2列
の貫通導体群とを具備することから、これら導体層と貫
通導体群がそれぞれ誘電体導波管のE面とH面もしくは
H面とE面に平行な疑似的な導体壁にあたる部分を形成
する。従って、誘電体基板を用いた平板構造で誘電体導
波管に類似した特性を有する高周波信号用の伝送線路を
得られる。
According to the dielectric waveguide line of the present invention, the pair of conductor layers sandwiching the dielectric substrate and the repetition interval in the transmission direction of the high-frequency signal are equal to or less than half the cutoff wavelength of the high-frequency signal. And two rows of through conductor groups formed so as to electrically connect the conductor layers with a certain width in a direction orthogonal to the transmission direction. A part corresponding to a pseudo conductor wall parallel to the E-plane and the H-plane or the H-plane and the E-plane of the body waveguide is formed. Therefore, a transmission line for a high-frequency signal having a characteristic similar to that of a dielectric waveguide in a flat plate structure using a dielectric substrate can be obtained.

【0014】そして、本発明の誘電体導波管線路によれ
ば、伝送線路の配線において屈曲部を設けるに際し、2
列の貫通導体群を前記特定構造に配列することにより、
屈曲部における電磁波の放射がほとんど無く、伝送損失
が小さく良好な伝送特性を有するものとなる。
According to the dielectric waveguide line of the present invention, when providing a bent portion in the wiring of the transmission line,
By arranging the through conductor group of the row in the specific structure,
There is almost no electromagnetic wave radiation at the bent portion, and the transmission loss is small and good transmission characteristics are obtained.

【0015】[0015]

【発明の実施の形態】以下、本発明を図面を参照しなが
ら説明する。図1および図2は、それぞれ本発明の誘電
体導波管線路の実施の形態の一例を説明するための概略
斜視図およびその平面図である。これらの図において、
1は誘電体基板、2は誘電体基板1を挟持する一対の導
体層、3は一対の導体層2間を電気的に接続するよう形
成された貫通導体であり、4は高周波信号の伝送方向に
その高周波信号の遮断波長の2分の1以下の繰り返し間
隔pで、かつその伝送方向と直交する方向に一定の幅d
で貫通導体3を配設することにより形成された2列の貫
通導体群である。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described below with reference to the drawings. 1 and 2 are a schematic perspective view and a plan view, respectively, for explaining an example of an embodiment of a dielectric waveguide line according to the present invention. In these figures,
1 is a dielectric substrate, 2 is a pair of conductor layers sandwiching the dielectric substrate 1, 3 is a through conductor formed to electrically connect the pair of conductor layers 2, and 4 is a transmission direction of a high-frequency signal. A constant width d at a repetition interval p equal to or less than half the cutoff wavelength of the high-frequency signal and in a direction orthogonal to the transmission direction.
Are two rows of through conductor groups formed by disposing the through conductors 3.

【0016】図1によれば、所定の厚みaの平板状の誘
電体基板1を挟持する位置に一対の導体層2・2が形成
されている。導体層2・2は誘電体基板1の少なくとも
伝送線路形成位置を挟む上下面に形成されている。ま
た、導体層2・2間には導体層2・2間を電気的に接続
する貫通導体3が多数設けられている。これら貫通導体
3は、図1および図2に示すように、高周波信号の伝送
方向すなわち線路形成方向にこの線路により伝送される
高周波信号の遮断波長の2分の1以下の所定の繰り返し
間隔pで、かつ前記伝送方向と直交する方向に所定の一
定の間隔(幅)dをもって2列に形成されることによ
り、伝送線路となる貫通導体群4を形成している。
According to FIG. 1, a pair of conductor layers 2 are formed at positions sandwiching a flat dielectric substrate 1 having a predetermined thickness a. The conductor layers 2 are formed on the upper and lower surfaces of the dielectric substrate 1 sandwiching at least the transmission line forming position. A large number of through conductors 3 are provided between the conductor layers 2 to electrically connect the conductor layers 2 to each other. As shown in FIGS. 1 and 2, these through conductors 3 are arranged at a predetermined repetition interval p which is equal to or less than half the cutoff wavelength of the high-frequency signal transmitted through the line in the transmission direction of the high-frequency signal, that is, the line forming direction. In addition, the through conductor group 4 which is a transmission line is formed by being formed in two rows at a predetermined constant interval (width) d in a direction orthogonal to the transmission direction.

【0017】平行に配置された一対の導体層2・2間に
はTEM波が伝播できるため、貫通導体群4の各列にお
ける貫通導体3の間隔pが遮断波長の2分の1よりも大
きいと、この線路に電磁波を給電してもここで作られる
疑似的な導波管に沿って伝播しなくなる。しかし、貫通
導体3の間隔pが遮断波長の2分の1以下であると電気
的な側壁を形成することとなって、電磁波は伝送線路に
対して垂直方向に伝播することができず、反射しながら
伝送線路方向に伝播されることとなる。その結果、この
ような構造の導体層2と貫通導体群4とにより囲まれる
断面積がa×dのサイズの領域により誘電体導波管と非
常に良く類似した良好な伝送特性が得られる。
Since the TEM wave can propagate between the pair of conductor layers 2 arranged in parallel, the distance p between the through conductors 3 in each row of the through conductor group 4 is larger than half the cutoff wavelength. Then, even if this line is supplied with electromagnetic waves, it does not propagate along the pseudo waveguide made here. However, if the distance p between the penetrating conductors 3 is less than half the cutoff wavelength, an electric side wall is formed, and the electromagnetic wave cannot propagate in the direction perpendicular to the transmission line and is reflected. The light is then propagated in the direction of the transmission line. As a result, a good transmission characteristic very similar to that of a dielectric waveguide can be obtained in a region having a cross section of a × d size surrounded by the conductor layer 2 and the through conductor group 4 having such a structure.

【0018】ここで、誘電体基板1の厚みaに対する制
限は特にないが、シングルモードで用いる場合には前記
一定の幅dに対して2分の1程度または2倍程度とする
ことがよく、図1の例では誘電体導波管のH面とE面に
当たる部分が各々導体層2と貫通導体群4で形成され、
幅dに対して厚みaを2倍程度とすれば、誘電体導波管
のE面とH面に当たる部分が各々導体層2と貫通導体群
4で形成されることとなる。
Here, there is no particular limitation on the thickness a of the dielectric substrate 1, but when it is used in the single mode, it is preferably about one half or twice the fixed width d. In the example of FIG. 1, portions corresponding to the H plane and the E plane of the dielectric waveguide are formed by the conductor layer 2 and the through conductor group 4, respectively.
If the thickness a is about twice as large as the width d, portions corresponding to the E-plane and the H-plane of the dielectric waveguide are formed by the conductor layer 2 and the through conductor group 4, respectively.

【0019】なお、5は貫通導体群4の各列を形成する
貫通導体3同士を電気的に接続する補助導体層であり、
所望により適宜形成される。また、この図1および図2
の例では貫通導体群4は2列に形成したが、この貫通導
体群4を4列あるいは6列に配設して貫通導体群4によ
る疑似的な導体壁を2重・3重に形成することにより、
導体壁からの電磁波の漏れをより効果的に防止すること
もできる。
Reference numeral 5 denotes an auxiliary conductor layer for electrically connecting the through conductors 3 forming each column of the through conductor group 4 to each other.
It is formed appropriately as required. 1 and FIG.
In this example, the through conductor groups 4 are formed in two rows, but the through conductor groups 4 are arranged in four or six rows to form pseudo conductor walls formed by the through conductor groups 4 in two or three layers. By doing
Leakage of electromagnetic waves from the conductor wall can be prevented more effectively.

【0020】このような導波管線路構造によれば、誘電
体基板1の比誘電率をεr とすると導波管サイズは通常
の導波管の1/εr 1/2 の大きさになる。従って、誘電
体基板1を構成する材料を比誘電率の大きいものとする
ほど、導波管サイズを小さくすることができ、高密度に
配線が形成される多層配線基板または半導体素子収納用
パッケージの伝送線路として利用可能な大きさとなる。
According to such a waveguide structure, to 1 / epsilon r 1/2 the size of the relative permittivity of the dielectric substrate 1 and epsilon r is the waveguide size conventional waveguide Become. Therefore, as the material constituting the dielectric substrate 1 has a higher relative dielectric constant, the waveguide size can be reduced, and a multilayer wiring board or a semiconductor element housing package in which wiring is formed with high density can be formed. This is a size that can be used as a transmission line.

【0021】また、図1および図2に示すように、本発
明の誘電体導波管線路はその伝送線路である貫通導体群
4の一部に屈曲部を有し、この屈曲部の内側に位置する
一方の列は1つの貫通導体6を屈曲点とした折れ線状に
形成されており、外側に位置する他方の列はこの1つの
貫通導体6を中心とする円弧状に形成されていることを
特徴とするものである。そのような屈曲部は、例えば図
2に示すような構造で構成される。
As shown in FIGS. 1 and 2, the dielectric waveguide line of the present invention has a bent portion in a part of the through conductor group 4 which is the transmission line, and has a bent portion inside the bent portion. One row positioned is formed in a polygonal line shape with one through conductor 6 as a bending point, and the other row positioned outside is formed in an arc shape centered on the one through conductor 6. It is characterized by the following. Such a bent portion has a structure as shown in FIG. 2, for example.

【0022】図2に記載される通り、屈曲部においては
高周波信号の伝送方向に直交する線路の幅が一定の幅d
となるように貫通導体群4が配置されており、屈曲部の
内側に位置する貫通導体群4の列は1つの貫通導体6を
屈曲点とした折れ線状となるように貫通導体3が配設さ
れ、他方、屈曲部の外側に位置する貫通導体群4の列は
屈曲部の内側にあたる列の屈曲点である1つの貫通導体
6を中心として半径dの円弧を描くように配置される。
As shown in FIG. 2, the width of the line orthogonal to the transmission direction of the high-frequency signal at the bent portion has a constant width d.
The through conductor group 4 is arranged so that the through conductor group 4 located inside the bent portion is arranged in a broken line with one through conductor 6 as a bending point. On the other hand, the rows of the through-conductor groups 4 located outside the bent portion are arranged so as to draw an arc having a radius d around one through-conductor 6 which is a bending point of the row inside the bent portion.

【0023】なお、貫通導体群4を構成する貫通導体3
は前述のように遮断波長の2分の1以下の繰り返し間隔
pで配設されており、この繰り返し間隔pは良好な伝送
特性を実現するためには一定の繰り返し間隔とすること
が望ましいが、遮断波長の2分の1以下の間隔であれば
適宜変化させたりいくつかの値を組み合わせたりしても
よいことは言うまでもない。従って、屈曲部の外側にあ
たる貫通導体群4の列を構成する貫通導体3の繰り返し
間隔pも、電磁波の放射を十分に抑制して良好な伝送特
性を実現するためには一定の値とすることが望ましい
が、同様に遮断波長の2分の1以下の値で種々変化させ
てもよいものである。
The through conductors 3 constituting the through conductor group 4
Are arranged at a repetition interval p equal to or less than a half of the cutoff wavelength as described above. The repetition interval p is desirably a constant repetition interval in order to realize good transmission characteristics. It goes without saying that the interval may be changed as appropriate or some values may be combined as long as the interval is equal to or less than half the cutoff wavelength. Therefore, the repetition interval p of the through conductors 3 forming the row of the through conductor group 4 corresponding to the outside of the bent portion is also set to a constant value in order to sufficiently suppress the radiation of the electromagnetic wave and realize the good transmission characteristics. However, similarly, it may be changed variously at a value equal to or less than half the cutoff wavelength.

【0024】本発明における誘電体基板1としては、誘
電体として機能し高周波信号の伝送を妨げることのない
特性を有するものであればとりわけ限定するものではな
いが、伝送線路を形成する際の精度および製造の容易性
の点からは、誘電体基板1はセラミックスからなること
が望ましい。
The dielectric substrate 1 according to the present invention is not particularly limited as long as it functions as a dielectric and has a characteristic that does not hinder the transmission of a high-frequency signal. It is desirable that the dielectric substrate 1 be made of ceramics from the viewpoint of easiness of manufacture.

【0025】このようなセラミックスとしてはこれまで
様々な比誘電率を持つセラミックスが知られているが、
本発明の導波管線路によって高周波信号を伝送するため
には常誘電体であることが望ましい。これは、一般に強
誘電体セラミックスは高周波領域では誘電損失が大きく
伝送損失が大きくなるためである。従って、誘電体基板
1の比誘電率εr は4〜100 程度が適当である。
As such ceramics, ceramics having various relative dielectric constants are known.
In order to transmit a high-frequency signal by the waveguide line of the present invention, it is desirable that the waveguide line be a paraelectric substance. This is because ferroelectric ceramics generally have large dielectric loss and high transmission loss in a high frequency range. Therefore, the relative dielectric constant ε r of the dielectric substrate 1 is suitably about 4 to 100.

【0026】また、一般に多層配線基板や半導体素子収
納用パッケージに形成される配線層の線幅は最大でも1
mmであることから、比誘電率が100 の材料を用い、上
部がH面すなわち磁界が上側の面に平行に巻く電磁界分
布になるように用いた場合、用いることのできる最小の
周波数は15GHzと算出され、マイクロ波帯の領域でも
利用可能となる。一方、一般的に誘電体基板1として用
いられる樹脂からなる誘電体は、比誘電率εr が2程度
であるため、線幅が1mmの場合、約100 GHz以上で
ないと利用することができないものとなる。
In general, the line width of a wiring layer formed on a multilayer wiring board or a package for housing a semiconductor element has a maximum of 1
mm, the minimum frequency that can be used is 15 GHz when a material having a relative dielectric constant of 100 is used and the upper surface is an H plane, that is, an electromagnetic field distribution in which the magnetic field is wound parallel to the upper surface. , And can be used in the microwave band region. On the other hand, a dielectric made of a resin generally used as the dielectric substrate 1 has a relative dielectric constant ε r of about 2, and therefore cannot be used unless the line width is 1 mm or more than about 100 GHz. Becomes

【0027】また、このような常誘電体セラミックスの
中にはアルミナ・シリカ等のように誘電正接が非常に小
さなものが多いが、全ての常誘電体セラミックスが利用
可能であるわけではない。誘電体導波管線路の場合は導
体による損失はほとんどなく、信号伝送時の損失のほと
んどは誘電体による損失であり、誘電体による損失α
(dB/m)は下記のように表わされる。 α=27.3×tanδ/λ/{1−(λ/λc )2 1/2 式中、tanδ:誘電体の誘電正接 λ :誘電体中の波長 λc :遮断波長 規格化された矩形導波管(WRJシリーズ)形状に準ず
ると、上式中の{1−(λ/λc )2 1/2 は0.75程度
である。
Further, among such paraelectric ceramics, many have very small dielectric loss tangents, such as alumina and silica, but not all paraelectric ceramics can be used. In the case of a dielectric waveguide line, there is almost no loss due to the conductor, and most of the loss during signal transmission is due to the dielectric, and the loss due to the dielectric α
(DB / m) is expressed as follows. α = 27.3 × tanδ / λ / {1- (λ / λc) 21/2 where tanδ: dielectric loss tangent of dielectric λ: wavelength in dielectric λc: cut-off wavelength Standardized rectangular waveguide According to the (WRJ series) shape, {1- (λ / λc) 2 } 1/2 in the above equation is about 0.75.

【0028】従って、実用に供し得る伝送損失である−
100 (dB/m)以下にするには、下記の関係が成立す
るように誘電体を選択することが必要である。
Therefore, the transmission loss is practically usable.
In order to make it 100 (dB / m) or less, it is necessary to select a dielectric so that the following relationship is satisfied.

【0029】f×εr 1/2 ×tanδ≦0.8 式中、fは使用する周波数(GHz)である。F × ε r 1/2 × tan δ ≦ 0.8 where f is a frequency (GHz) to be used.

【0030】このような誘電体基板1としては、例えば
アルミナセラミックスやガラスセラミックス・窒化アル
ミニウムセラミックス等があり、例えばセラミックス原
料粉末に適当な有機溶剤・溶媒を添加混合して泥漿状に
なすとともにこれを従来周知のドクターブレード法やカ
レンダーロール法等を採用してシート状となすことによ
って複数枚のセラミックグリーンシートを得、しかる
後、これらセラミックグリーンシートの各々に適当な打
ち抜き加工を施すとともにこれらを積層し、アルミナセ
ラミックスの場合は1500〜1700℃、ガラスセラミックス
の場合は850 〜1000℃、窒化アルミニウムセラミックス
の場合は1600〜1900℃の温度で焼成することによって製
作される。
Examples of such a dielectric substrate 1 include alumina ceramics, glass ceramics, and aluminum nitride ceramics. For example, an appropriate organic solvent or solvent is added to and mixed with ceramic raw material powder to form a slurry. A plurality of ceramic green sheets are obtained by forming a sheet by employing a conventionally known doctor blade method or calender roll method, and thereafter, each of these ceramic green sheets is subjected to appropriate punching and laminated. It is manufactured by firing at a temperature of 1500 to 1700 ° C for alumina ceramics, 850 to 1000 ° C for glass ceramics, and 1600 to 1900 ° C for aluminum nitride ceramics.

【0031】また、一対の導体層2としては、例えば誘
電体基板1がアルミナセラミックスから成る場合、タン
グステン等の金属粉末に適当なアルミナ・シリカ・マグ
ネシア等の酸化物や有機溶剤・溶媒等を添加混合してペ
ースト状にしたものを厚膜印刷法により少なくとも伝送
線路を完全に覆うようにセラミックグリーンシート上に
印刷し、しかる後、約1600℃の高温で焼成し、厚み10〜
15μm以上となるようにして形成する。なお、金属粉末
としては、ガラスセラミックスの場合は銅・金・銀が、
窒化アルミニウムセラミックスの場合はタングステン・
モリブデンが好適である。また、導体層2の厚みは一般
的に5〜50μm程度とされる。
When the dielectric substrate 1 is made of alumina ceramics, for example, a suitable oxide such as alumina, silica, magnesia, or an organic solvent or solvent is added to a metal powder such as tungsten when the dielectric substrate 1 is made of alumina ceramics. The mixed paste was printed on a ceramic green sheet by a thick film printing method so as to completely cover at least the transmission line, and then fired at a high temperature of about 1600 ° C.
It is formed so as to have a thickness of 15 μm or more. In the case of glass ceramics, copper / gold / silver is used as the metal powder,
Tungsten for aluminum nitride ceramics
Molybdenum is preferred. The thickness of the conductor layer 2 is generally about 5 to 50 μm.

【0032】また、貫通導体3としては、例えばビアホ
ール導体やスルーホール導体等により形成すればよく、
その断面形状も製作が容易な円形の他、矩形や菱形等の
多角形であってもよい。これら貫通導体3は、例えばセ
ラミックグリーンシートに打ち抜き加工を施して作製し
た貫通孔に前記導体層2と同様の金属ペーストを埋め込
み、しかる後、誘電体基板1と同時に焼成し形成する。
なお、貫通導体3は直径50〜300 μmが適当である。
The through conductor 3 may be formed of, for example, a via-hole conductor or a through-hole conductor.
The cross-sectional shape may be a polygon, such as a rectangle or a rhombus, in addition to a circular shape that is easy to manufacture. These through conductors 3 are formed by embedding a metal paste similar to that of the conductor layer 2 in a through hole formed by, for example, punching a ceramic green sheet, and then firing the same at the same time as the dielectric substrate 1.
The diameter of the through conductor 3 is suitably 50 to 300 μm.

【0033】次に、本発明の誘電体導波管線路の実施の
形態の他の例を図3に図2と同様の平面図で示す。
Next, another embodiment of the dielectric waveguide line according to the present invention is shown in FIG. 3 in a plan view similar to FIG.

【0034】図3に示す構造によれば、本発明の誘電体
導波管線路はその伝送線路である貫通導体群4の一部に
屈曲部を有し、屈曲部においては高周波信号の伝送方向
に直交する線路の幅が一定の幅dとほぼ同じとなるよう
に貫通導体群4が配置されており、この屈曲部の内側に
位置する貫通導体群4の一方の列は図2と同様に1つの
貫通導体7を屈曲点とした折れ線状に貫通導体3が配設
されて形成されており、屈曲部の外側に位置する貫通導
体群4の他方の列はこの1つの貫通導体7を頂点とし一
定の幅dを高さとする二等辺三角形8の底辺8aに対応
する折れ線状に貫通導体3が配設されて形成されている
ことを特徴とするものである。
According to the structure shown in FIG. 3, the dielectric waveguide line of the present invention has a bent portion in a part of the through conductor group 4 which is the transmission line, and the bent portion has a transmission direction of the high-frequency signal. The through-conductor group 4 is arranged so that the width of the line perpendicular to the line is substantially the same as the constant width d. One row of the through-conductor group 4 located inside the bent portion is similar to FIG. The penetrating conductors 3 are arranged and formed in a polygonal line with one penetrating conductor 7 as a bending point, and the other row of the penetrating conductor group 4 located outside the bent portion has this one penetrating conductor 7 as a vertex. The penetrating conductor 3 is formed in a polygonal shape corresponding to the base 8a of the isosceles triangle 8 having a certain width d and a height.

【0035】図3に示す例は屈曲部の角を斜めにカット
した形状であると言え、図2に示した例における屈曲部
に比較して、屈曲部の製作が容易になるものである。
The example shown in FIG. 3 can be said to have a shape in which the corners of the bent portion are obliquely cut, and the manufacture of the bent portion is easier than the bent portion in the example shown in FIG.

【0036】次に、本発明の誘電体導波管線路の実施の
形態のさらに他の例を図4に図2・図3と同様の平面図
で示す。
Next, still another example of the embodiment of the dielectric waveguide line of the present invention is shown in FIG. 4 in a plan view similar to FIGS.

【0037】図4に示す構造によれば、本発明の誘電体
導波管線路はその伝送線路である貫通導体群4の一部に
屈曲部を有し、屈曲部においては高周波信号の伝送方向
に直交する線路の幅が一定の幅dとほぼ同じとなるよう
に貫通導体群4が配置されており、この屈曲部の内側に
位置する貫通導体群4の一方の列はこの列の屈曲した内
側の仮想的な中心点9を中心とし所定の半径rの円弧状
に貫通導体3が配設されて形成されており、屈曲部の外
側に位置する貫通導体群4の他方の列はこの中心点9を
中心とし前記半径rに一定の幅dを加えた半径r+dの
円弧状すなわち内側の列と同心の円弧状に貫通導体3が
配設されて形成されていることによって、貫通導体群4
の列の各列が同心円弧状に配列された屈曲部を有してい
ることを特徴とするものである。
According to the structure shown in FIG. 4, the dielectric waveguide line of the present invention has a bent portion in a part of the through conductor group 4 which is the transmission line, and the bent portion has a transmission direction of the high frequency signal. Are arranged such that the width of the line perpendicular to the line is substantially the same as the constant width d. One row of the through conductor group 4 located inside the bent portion is bent in this row. The through conductors 3 are arranged and formed in an arc shape having a predetermined radius r around the inner virtual center point 9, and the other row of the through conductor group 4 located outside the bent portion is positioned at the center. Since the through conductors 3 are arranged and formed in an arc shape having a radius r + d obtained by adding a certain width d to the radius r with the center at the point 9, that is, an arc shape concentric with the inner row, the through conductor group 4 is formed.
Are provided with bent portions arranged in concentric arcs.

【0038】図4に示す例は屈曲部の内側・外側共に滑
らかな形状に形成されるため、電磁界の乱れが非常に小
さく、伝送損失が小さくなるという利点を有する。
The example shown in FIG. 4 has the advantage that the disturbance of the electromagnetic field is very small and the transmission loss is small because both the inside and outside of the bent portion are formed in a smooth shape.

【0039】[0039]

【実施例】図1および図2に示した構成の本発明の誘電
体導波管線路について、屈曲部を含む伝送線路の伝送特
性を有限要素法により計算した。導体層2および貫通導
体3の材料には導電率が5.8 ×107 (1/Ωm)の純銅
を用い、誘電体基板1には比誘電率が5で誘電正接が0.
001 の、ほう珪酸ガラス75重量%とアルミナ25重量%と
を焼成して作製したガラスセラミックス焼結体を用い、
誘電体基板1の厚みa=1mm、貫通導体3の直径を0.
16mm、貫通導体群4の繰り返し間隔p=1.58mm、貫
通導体群4の一定の幅d=2mm(WRJ−34規格対
応)とし、線路の長さは30mmとしてSパラメータの周
波数特性を算出した。
EXAMPLE A transmission characteristic of a transmission line including a bent portion of the dielectric waveguide line of the present invention having the structure shown in FIGS. 1 and 2 was calculated by the finite element method. The conductor layer 2 and the through conductor 3 are made of pure copper having a conductivity of 5.8 × 10 7 (1 / Ωm), and the dielectric substrate 1 has a relative permittivity of 5 and a dielectric loss tangent of 0.
Using a glass-ceramic sintered body prepared by firing 75% by weight of borosilicate glass and 25% by weight of alumina of 001,
The thickness a of the dielectric substrate 1 is 1 mm, and the diameter of the through conductor 3 is set to 0.
The frequency characteristics of the S parameters were calculated assuming that 16 mm, the repetition interval p of the through conductor group 4 was 1.58 mm, the fixed width d of the through conductor group 4 was 2 mm (corresponding to the WRJ-34 standard), and the length of the line was 30 mm.

【0040】その結果、遮断周波数は約42GHzとな
り、それ以上の周波数では信号が良好に透過することが
分かった。また、屈曲部の出口では入口と同様な電界分
布になっており、屈曲部が電界強度の分布に影響を与え
るのは屈曲部内のみに限られ、屈曲部において伝送線路
の外側に電界強度の分布は見られず、従って、屈曲部に
おける電磁波の放射は無いことも分かった。
As a result, it was found that the cutoff frequency was about 42 GHz, and that at higher frequencies, the signal was transmitted well. In addition, the electric field distribution at the outlet of the bent portion is similar to that at the inlet, and the bent portion affects the distribution of the electric field strength only in the bent portion, and the distribution of the electric field intensity is outside the transmission line at the bent portion. No electromagnetic wave was emitted at the bent portion.

【0041】また、同様の構成の誘電体導波管線路試料
を作製してその伝送特性を評価したところ、上記算出結
果と同様の良好な伝送特性が得られた。
Further, when a dielectric waveguide line sample having the same configuration was prepared and its transmission characteristics were evaluated, good transmission characteristics similar to the above calculation results were obtained.

【0042】さらに、図3ならびに図4に示した構造の
本発明の誘電体導波管線路についても同様に有限要素法
による計算と作製した試料についての伝送特性の評価を
行なったところ、いずれも屈曲部における電磁波の放射
が無く良好な伝送特性を有することが確認できた。
Further, the dielectric waveguide of the present invention having the structure shown in FIGS. 3 and 4 was similarly calculated by the finite element method and evaluated the transmission characteristics of the manufactured sample. It was confirmed that there was no electromagnetic wave radiation at the bent portion and that the device had good transmission characteristics.

【0043】[0043]

【発明の効果】以上詳述した通り、本発明の誘電体導波
管線路によれば、誘電体基板を一対の導体層で挟持し、
導波管線路の側壁を貫通導体群により形成することによ
って、従来のセラミックス積層技術を応用して容易に作
製することができ、また、導波管線路の一部に設ける屈
曲部の構成について、2列の貫通導体群を前述のように
折れ線状と円弧状、あるいは折れ線状と折れ線状、ある
いは同心円弧状に形成したことによって、屈曲部におけ
る電磁波の放射・漏洩による伝送損失をほとんど無くす
ることができ、高周波信号の良好な伝送特性を有する誘
電体導波管線路を提供することができた。
As described above in detail, according to the dielectric waveguide line of the present invention, the dielectric substrate is sandwiched between the pair of conductor layers,
By forming the side wall of the waveguide line with a group of through conductors, it can be easily manufactured by applying the conventional ceramic lamination technology, and regarding the configuration of the bent portion provided in a part of the waveguide line, By forming the penetrating conductor group in two rows in the form of a polygonal line and an arc, or a polygonal line and a polygonal line, or a concentric arc as described above, transmission loss due to radiation and leakage of electromagnetic waves at the bent portion is almost eliminated. As a result, a dielectric waveguide line having good transmission characteristics of a high-frequency signal can be provided.

【0044】中でも、誘電体基板に比誘電率の高いセラ
ミックスを用いることによって、高密度配線の多層配線
基板や半導体素子収納用パッケージ等に好適なものとな
り、マイクロ波帯からミリ波帯まで安定した伝送特性の
導波管線路を形成することができる。
In particular, the use of ceramics having a high relative dielectric constant for the dielectric substrate makes it suitable for high-density wiring multilayer wiring boards, packages for housing semiconductor elements, and the like, and is stable from the microwave band to the millimeter wave band. A waveguide line having transmission characteristics can be formed.

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

【図1】本発明の誘電体導波管線路の実施の形態の例を
説明するための概略斜視図である。
FIG. 1 is a schematic perspective view for explaining an example of an embodiment of a dielectric waveguide line according to the present invention.

【図2】本発明の誘電体導波管線路の実施の形態の例を
説明するための図1の平面図である。
FIG. 2 is a plan view of FIG. 1 for explaining an example of an embodiment of the dielectric waveguide line of the present invention.

【図3】本発明の誘電体導波管線路の実施の形態の他の
例を説明するための図2と同様の平面図である。
FIG. 3 is a plan view similar to FIG. 2 for describing another example of the embodiment of the dielectric waveguide line of the present invention.

【図4】本発明の誘電体導波管線路の実施の形態のさら
に他の例を説明するための図2と同様の平面図である。
FIG. 4 is a plan view similar to FIG. 2 for explaining still another example of the embodiment of the dielectric waveguide line of the present invention.

【符号の説明】[Explanation of symbols]

1・・・・・誘電体基板 2・・・・・導体層 3・・・・・貫通導体 4・・・・・貫通導体群 6、7・・・1つの貫通導体(屈曲点) 8・・・・・二等辺三角形 8a・・・・底辺 1 ... dielectric substrate 2 ... conductor layer 3 ... through conductor 4 ... through conductor group 6, 7 ... one through conductor (bending point) 8. .... Isosceles triangle 8a .... Base

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 誘電体基板を挟持する一対の導体層と、
高周波信号の伝送方向に前記高周波信号の遮断波長の2
分の1以下の繰り返し間隔で、かつ前記伝送方向と直交
する方向に一定の幅で前記導体層間を電気的に接続する
よう形成された2列の貫通導体群とを具備し、前記導体
層および前記貫通導体群に囲まれた領域によって高周波
信号を伝送する誘電体導波管線路であって、前記2列の
貫通導体群はその一部に屈曲部を有し、該屈曲部に位置
する一方の列は1つの貫通導体を屈曲点とした折れ線状
に形成されており、他方の列は前記1つの貫通導体を中
心とし、前記一定の幅を半径とする円弧状に形成されて
いることを特徴とする誘電体導波管線路。
A pair of conductor layers sandwiching a dielectric substrate;
In the transmission direction of the high-frequency signal, the cutoff wavelength of the high-frequency signal is 2
Two rows of through conductor groups formed so as to electrically connect the conductor layers with a constant width in a direction orthogonal to the transmission direction at a repetition interval of 1 / th or less, and the conductor layer and A dielectric waveguide line for transmitting a high-frequency signal by a region surrounded by the through conductor group, wherein the two rows of through conductor groups have a bent portion in a part thereof, and Is formed in a polygonal line shape with one through conductor as a bending point, and the other row is formed in an arc shape with the one through conductor as a center and a radius having the constant width. Characteristic dielectric waveguide line.
【請求項2】 誘電体基板を挟持する一対の導体層と、
高周波信号の伝送方向に前記高周波信号の遮断波長の2
分の1以下の繰り返し間隔で、かつ前記伝送方向と直交
する方向に一定の幅で前記導体層間を電気的に接続する
よう形成された2列の貫通導体群とを具備し、前記導体
層および前記貫通導体群に囲まれた領域によって高周波
信号を伝送する誘電体導波管線路であって、前記2列の
貫通導体群はその一部に屈曲部を有し、該屈曲部に位置
する一方の列は1つの貫通導体を屈曲点とした折れ線状
に形成されており、他方の列は前記一方の列の前記屈曲
点を頂点とし前記一定の幅を高さとする二等辺三角形の
底辺に対応する折れ線状に形成されていることを特徴と
する誘電体導波管線路。
2. A pair of conductor layers sandwiching a dielectric substrate,
In the transmission direction of the high-frequency signal, the cutoff wavelength of the high-frequency signal is 2
Two rows of through conductor groups formed so as to electrically connect the conductor layers with a constant width in a direction orthogonal to the transmission direction at a repetition interval of 1 / th or less, and the conductor layer and A dielectric waveguide line for transmitting a high-frequency signal by a region surrounded by the through conductor group, wherein the two rows of through conductor groups have a bent portion in a part thereof, and Are formed in a polygonal line shape having one through conductor as a bending point, and the other row corresponds to a base of an isosceles triangle having the bending point of the one row as a vertex and the constant width as a height. A dielectric waveguide line formed in a polygonal line shape.
【請求項3】 誘電体基板を挟持する一対の導体層と、
高周波信号の伝送方向に前記高周波信号の遮断波長の2
分の1以下の繰り返し間隔で、かつ前記伝送方向と直交
する方向に一定の幅で前記導体層間を電気的に接続する
よう形成された2列の貫通導体群とを具備し、前記導体
層および前記貫通導体群に囲まれた領域によって高周波
信号を伝送する誘電体導波管線路であって、前記2列の
貫通導体群は、その各列が同心円弧状に配列された屈曲
部を有することを特徴とする誘電体導波管線路。
3. A pair of conductor layers sandwiching a dielectric substrate,
In the transmission direction of the high-frequency signal, the cutoff wavelength of the high-frequency signal is 2
Two rows of through conductor groups formed so as to electrically connect the conductor layers with a constant width in a direction orthogonal to the transmission direction at a repetition interval of 1 / th or less, and the conductor layer and A dielectric waveguide line for transmitting a high-frequency signal by a region surrounded by the through conductor group, wherein the two rows of through conductor groups have a bent portion in which each row is arranged in a concentric arc shape. Characteristic dielectric waveguide line.
JP9226174A 1997-08-22 1997-08-22 Dielectric waveguide line Pending JPH1168416A (en)

Priority Applications (11)

Application Number Priority Date Filing Date Title
JP9226174A JPH1168416A (en) 1997-08-22 1997-08-22 Dielectric waveguide line
US09/137,195 US6057747A (en) 1997-08-22 1998-08-20 Dielectric waveguide line and its branch structure
EP03020458A EP1396901B1 (en) 1997-08-22 1998-08-21 Dielectric waveguide bend
DE69841265T DE69841265D1 (en) 1997-08-22 1998-08-21 Elbow for dielectric waveguide
EP08021077A EP2043192B1 (en) 1997-08-22 1998-08-21 Dielectric waveguide bend
EP98115812A EP0898322B1 (en) 1997-08-22 1998-08-21 Dielectric waveguide line and its branch structure
DE69839785T DE69839785D1 (en) 1997-08-22 1998-08-21 Dielectric waveguide and its branch structure
EP03020457A EP1396903B1 (en) 1997-08-22 1998-08-21 Dielectric waveguide line and its branch structure
DE69836302T DE69836302T2 (en) 1997-08-22 1998-08-21 Dielectric waveguide and its branch structure
US09/497,792 US6380825B1 (en) 1997-08-22 2000-02-03 Branch tee dielectric waveguide line
US09/498,128 US6359535B1 (en) 1997-08-22 2000-02-03 Dielectric waveguide line bend formed by rows of through conductors

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9226174A JPH1168416A (en) 1997-08-22 1997-08-22 Dielectric waveguide line

Publications (1)

Publication Number Publication Date
JPH1168416A true JPH1168416A (en) 1999-03-09

Family

ID=16841051

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9226174A Pending JPH1168416A (en) 1997-08-22 1997-08-22 Dielectric waveguide line

Country Status (1)

Country Link
JP (1) JPH1168416A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6774748B1 (en) 1999-11-15 2004-08-10 Nec Corporation RF package with multi-layer substrate having coplanar feed through and connection interface
US6992548B2 (en) 2002-12-16 2006-01-31 Tdk Corporation RF module and method for arranging through holes in RF module
JP2010232778A (en) * 2009-03-26 2010-10-14 Kyocera Corp Waveguide type rat race circuit

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6774748B1 (en) 1999-11-15 2004-08-10 Nec Corporation RF package with multi-layer substrate having coplanar feed through and connection interface
US6992548B2 (en) 2002-12-16 2006-01-31 Tdk Corporation RF module and method for arranging through holes in RF module
JP2010232778A (en) * 2009-03-26 2010-10-14 Kyocera Corp Waveguide type rat race circuit

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