JPS61290794A - Wiring board - Google Patents

Wiring board

Info

Publication number
JPS61290794A
JPS61290794A JP60131739A JP13173985A JPS61290794A JP S61290794 A JPS61290794 A JP S61290794A JP 60131739 A JP60131739 A JP 60131739A JP 13173985 A JP13173985 A JP 13173985A JP S61290794 A JPS61290794 A JP S61290794A
Authority
JP
Japan
Prior art keywords
wiring
wiring board
characteristic impedance
present
dielectric
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
JP60131739A
Other languages
Japanese (ja)
Inventor
和民 川本
稔 田中
和夫 廣田
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP60131739A priority Critical patent/JPS61290794A/en
Publication of JPS61290794A publication Critical patent/JPS61290794A/en
Pending legal-status Critical Current

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  • Waveguides (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は、電子回路、特に電子計算機や通信機等の高速
、高周波電子回路に用いられる配線基板に関するもので
ある。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a wiring board used in electronic circuits, particularly high-speed, high-frequency electronic circuits such as electronic computers and communication devices.

〔発明の背景〕[Background of the invention]

計算機・通信機などの配線においては、その配線本数の
増大に対応して多層配線基板が用いられている。特に高
周波や立ち上りの早いパルスを扱う基板では、第5図に
示すように信号層とは別に全面のアース(グランド)層
を持ち、その特性インピーダンスを一定にしている。な
お、図において1は信号パターン、2はアース層、3は
絶縁層(誘電体層)である。
BACKGROUND ART Multilayer wiring boards are used in wiring for computers, communication devices, etc. in response to an increase in the number of wires. In particular, boards that handle high frequencies or pulses with a fast rise have a ground layer on the entire surface in addition to the signal layer, as shown in FIG. 5, to keep the characteristic impedance constant. In the figure, 1 is a signal pattern, 2 is a ground layer, and 3 is an insulating layer (dielectric layer).

しかしながら、配線本数がさらに増大した場合、これに
対応して配線層数を増やすと基板厚が厚くなりすぎ、実
際上配線層数には上限がある。さらに重要な問題は、各
配線層間とスルホールを用いて電気的に接続する必要が
あるが、スルホール作成技術の限界からスルホールの歩
留りが配線層数の増大に対応して低下することである。
However, if the number of wirings increases further, increasing the number of wiring layers correspondingly increases the thickness of the substrate, and there is actually an upper limit to the number of wiring layers. A more important problem is that although it is necessary to electrically connect each wiring layer using through-holes, the yield of through-holes decreases as the number of wiring layers increases due to limitations in through-hole production technology.

また、配線層数が増えるとスルホール部の長さも長くな
り、スルホール部での信号の伝搬遅延も無視しえなくな
る。これらの問題を解決するためには誘電体層の厚さを
薄くすればよいが、誘電体層を薄くすると配線の特性イ
ンピーダンスが低下し、半導体論理回路と配線のインピ
ーダンスを整合させる必要のある電子計算機用などでは
、特性インピーダンスの低下は許容されえないことにな
る。即ち、これまでの配線基板においては特性インピー
ダンスおよび基板厚を一定としたI!ま多くの配線を収
容しえず、また、スルホール形成の歩留りが良好でない
という不具合がある。
Furthermore, as the number of wiring layers increases, the length of the through-hole portion also increases, and the signal propagation delay in the through-hole portion cannot be ignored. In order to solve these problems, it is possible to reduce the thickness of the dielectric layer, but thinning the dielectric layer lowers the characteristic impedance of the wiring, and it is necessary to match the impedance of the semiconductor logic circuit and the wiring. For applications such as computers, a decrease in characteristic impedance is unacceptable. That is, in conventional wiring boards, I! with constant characteristic impedance and board thickness. However, there are problems in that a large number of wiring lines cannot be accommodated, and the yield of through-hole formation is not good.

なお、適切碌特性インピーダンスを確保し念多層配線基
板についての公知文献としては、例えば特開昭55−1
32773号公報が挙げられる。
In addition, as a known document regarding a multilayer wiring board that ensures appropriate characteristic impedance, for example, Japanese Patent Laid-Open No. 55-1
32773 is mentioned.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、上記した従来技術の欠点をなくし、誘
電体層の厚さが薄くても適切な特性インピーダンスを確
保しうる配線基板を供するlこある。
SUMMARY OF THE INVENTION An object of the present invention is to eliminate the above-mentioned drawbacks of the prior art and to provide a wiring board that can ensure an appropriate characteristic impedance even if the dielectric layer is thin.

〔発明の概要〕[Summary of the invention]

本発明は上記目的を達成するために、これまでの全面ア
ース層に代えて、アース層に所定にスリットを設けるこ
とによって、誘電体の厚さを薄くした場合でも特性イン
ピーダンスを一定に保ちうるようになしたものである。
In order to achieve the above object, the present invention provides slits in the ground layer at predetermined locations in place of the conventional full-surface ground layer, thereby making it possible to maintain a constant characteristic impedance even when the thickness of the dielectric is reduced. This is what was done.

〔発明の実施例〕[Embodiments of the invention]

以下、本発明を第1図から第4図により説明する。 The present invention will be explained below with reference to FIGS. 1 to 4.

先ず第2図はこれまでの全面アース層を用いた配線基板
での電界分布を電気力線4を用いて模式的に示したもの
である。この場合特性インピーダンスZoは、線路の損
失を無視すればZo=Jゴ、/C−と表わされることは
公知の事実であり、また、単位長当りのインダクタンス
LおよびキャパシタンスCは線路幅W、誘電体厚りおよ
び誘電体の比誘電率ε1によって決定されるものとなっ
ている。よって、誘電体厚りを小さくすればCが大きく
なって特性インピーダンスzoカ低下することになるが
、誘電体厚りを小さくし、しかもこのときの特性インピ
ーダンスの低下を防ぎこれを一定に保持するには、Cを
実質的に不変にすればよいことになる。このことは、h
が一定であれば、Lをほとんど変化させずCを実質的に
小さくしてZoを増大させることと等価である。
First, FIG. 2 schematically shows, using electric lines of force 4, the electric field distribution in a wiring board using a conventional full-surface ground layer. In this case, it is a well-known fact that the characteristic impedance Zo can be expressed as Zo=Jgo,/C- if line loss is ignored, and the inductance L and capacitance C per unit length are determined by the line width W, dielectric It is determined by the body thickness and the dielectric constant ε1. Therefore, if the dielectric thickness is made smaller, C increases and the characteristic impedance zoka decreases, but it is necessary to reduce the dielectric thickness and prevent the characteristic impedance from decreasing and keep it constant. For this purpose, it is sufficient to make C essentially unchanged. This means that h
If is constant, it is equivalent to substantially decreasing C and increasing Zo without changing much L.

本発明はこれを効果的に行なうため、信号配線1の両側
端部の直下あるいは直上のアース層2にスリットを設け
るようになし念ものである。
In order to effectively accomplish this, the present invention is designed to provide slits in the ground layer 2 directly below or directly above both ends of the signal wiring 1.

これを第2図および第1図を用いて定性的に説明する。This will be qualitatively explained using FIGS. 2 and 1.

第2図には電界分布に併せて信号配線上の電荷分布5が
模式的に示されているが、これより電荷は配線側端部に
集中していることが知れる。電荷分布が第2図に示すよ
うになることは公知であるが、このような電荷分布5に
より電気力線4は信号配線側端部に集中し、よって配線
のキャパシタンスCは主としてこの側端部効果により決
まることになる。従ってキャパシタンスCを小さくして
特性インピーダンスZ。
FIG. 2 schematically shows the charge distribution 5 on the signal wiring along with the electric field distribution, and it can be seen from this that the charges are concentrated at the ends of the wiring. It is well known that the charge distribution becomes as shown in FIG. 2. Due to such a charge distribution 5, the electric lines of force 4 are concentrated at the end of the signal wiring, and therefore the capacitance C of the wiring is mainly caused by the end of this side. It will depend on the effect. Therefore, the characteristic impedance Z is reduced by reducing the capacitance C.

を増大させるには、配線側端部が形成するキャパシタン
スを低減することが効果的である。第1図に示す本発明
による配線基板の一例での基本的な構成はこのような原
理に基づくものであり、配線側端部直下に設けたアース
層のスリットにより電界分布が電気力線を用いて示した
ようになり、これより配線側端部が形成するキャパシタ
ンスを低減しうるものである。
In order to increase this, it is effective to reduce the capacitance formed at the end of the wiring. The basic configuration of an example of the wiring board according to the present invention shown in Fig. 1 is based on this principle, and the electric field distribution is changed using electric lines of force by the slit in the ground layer provided directly under the wiring side end. This makes it possible to reduce the capacitance formed at the wiring side end.

以上定性的に述べた点を定量化するにはラプラスの方程
式を解く必要があるが、第3図はその計算結果を示した
も′のである。スリット幅5(=St + 82 )に
対する特性インピーダンスZo増大の割合を示したもの
であるが、これよりhを小さくしてもスリット幅Sを適
当に設定することによって、特性インピーダンスZoを
一定に保つことが可能となるものである。
In order to quantify the points described qualitatively above, it is necessary to solve Laplace's equation, and Figure 3 shows the calculation results. This shows the rate of increase in the characteristic impedance Zo with respect to the slit width 5 (=St + 82).Even if h is smaller than this, the characteristic impedance Zo can be kept constant by appropriately setting the slit width S. This makes it possible.

第4図は本発明による配線基板が多層配線基板として構
成された場合での断面を示すが、これについては説明は
要しない。
Although FIG. 4 shows a cross section of the wiring board according to the present invention configured as a multilayer wiring board, no explanation is necessary for this.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明による場合は、特性インピー
ダンスを一定に保ったまま誘電体層の厚さを薄くしるる
なめ、配線基板、特に多層配線基板の製造時での歩留り
向上に効果があり、またスルホール部の長さ茅;短かく
なるためこの部分での信号伝搬時間が短縮されうる。ま
た、配線層数を増大させうるから、多数の配線数を収容
することによって大規模回路が比較的コンパクトに形成
されることになる。すなわち、高集積実装が可能で、計
算速度の高速化の要求等に対処しうろこととなる。しか
も本発明では、比較的小さなスリット幅で効果的に特性
インピーダンスを高くすることが達成されるため、充分
なシールド効果を有する、漏洩雑音の小さい配線基板が
得られることになる、
As explained above, according to the present invention, the thickness of the dielectric layer can be reduced while keeping the characteristic impedance constant, which is effective in improving the yield when manufacturing wiring boards, especially multilayer wiring boards. Furthermore, since the length of the through-hole portion is shortened, the signal propagation time in this portion can be shortened. Furthermore, since the number of wiring layers can be increased, a large-scale circuit can be formed relatively compactly by accommodating a large number of wirings. In other words, it is possible to implement highly integrated systems, and it will be possible to meet the demands for faster calculation speeds. Moreover, in the present invention, it is possible to effectively increase the characteristic impedance with a relatively small slit width, so a wiring board with sufficient shielding effect and low leakage noise can be obtained.

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

第1図は、本発明による配線基板の一例での基本的な構
成を示す図、第2図は、これまでの配線基板における電
界分布を模式的に示す図、第5図は、本発明に係るスリ
ットの幅に対する特性インピーダンスの増大の割合を示
す図、第4図は、本発明に係る多層配線基板の断面構成
を示す図、第5図は、これまでの配線基板の断面構成を
示す図である。 1・・・信号配線 2・・・アース層 3・・・誘電体層
FIG. 1 is a diagram showing the basic configuration of an example of the wiring board according to the present invention, FIG. 2 is a diagram schematically showing the electric field distribution in a conventional wiring board, and FIG. 5 is a diagram showing the basic configuration of an example of the wiring board according to the present invention. FIG. 4 is a diagram showing a cross-sectional configuration of a multilayer wiring board according to the present invention, and FIG. 5 is a diagram showing a cross-sectional configuration of a conventional wiring board. It is. 1...Signal wiring 2...Earth layer 3...Dielectric layer

Claims (1)

【特許請求の範囲】[Claims] 1、誘電体をはさんで信号配線とアース層を設けた構成
の配線基板において、信号配線に沿つて該配線の両側端
部の直下、直上の少なくとも何れか一方の側のアース層
の対応部分を除去しスリットを設けてなる構成を特徴と
する配線基板。
1. In a wiring board with a structure in which a signal wiring and a ground layer are provided across a dielectric, the corresponding part of the ground layer on at least one side directly below or directly above both ends of the wiring along the signal wiring. A wiring board characterized by having a structure in which a slit is provided by removing the .
JP60131739A 1985-06-19 1985-06-19 Wiring board Pending JPS61290794A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60131739A JPS61290794A (en) 1985-06-19 1985-06-19 Wiring board

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60131739A JPS61290794A (en) 1985-06-19 1985-06-19 Wiring board

Publications (1)

Publication Number Publication Date
JPS61290794A true JPS61290794A (en) 1986-12-20

Family

ID=15065058

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60131739A Pending JPS61290794A (en) 1985-06-19 1985-06-19 Wiring board

Country Status (1)

Country Link
JP (1) JPS61290794A (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4855537A (en) * 1987-09-25 1989-08-08 Kabushiki Kaisha Toshiba Wiring substrate having mesh-shaped earth line
JPH0397975U (en) * 1990-01-24 1991-10-09
JP2003204128A (en) * 2002-01-10 2003-07-18 Sharp Corp Printed wiring board, converter for receiving radio wave, and antenna device
JP2013157308A (en) * 2012-01-06 2013-08-15 Murata Mfg Co Ltd High-frequency signal line
WO2013190859A1 (en) * 2012-06-19 2013-12-27 株式会社村田製作所 Layered multi-core cable
JPWO2017090181A1 (en) * 2015-11-27 2018-09-06 富士通株式会社 Circuit board and electronic device
JP2019216492A (en) * 2018-06-11 2019-12-19 三菱電機株式会社 Electric power conversion system

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4855537A (en) * 1987-09-25 1989-08-08 Kabushiki Kaisha Toshiba Wiring substrate having mesh-shaped earth line
JPH0397975U (en) * 1990-01-24 1991-10-09
JP2003204128A (en) * 2002-01-10 2003-07-18 Sharp Corp Printed wiring board, converter for receiving radio wave, and antenna device
US7378599B2 (en) 2002-01-10 2008-05-27 Sharp Kabushiki Kaisha Printed circuit board, radio wave receiving converter, and antenna device
JP2013157308A (en) * 2012-01-06 2013-08-15 Murata Mfg Co Ltd High-frequency signal line
US20140376199A1 (en) * 2012-01-06 2014-12-25 Murata Manufacturing Co., Ltd. Laminated multi-conductor cable
US9781832B2 (en) * 2012-01-06 2017-10-03 Murata Manufacturing Co., Ltd. Laminated multi-conductor cable
WO2013190859A1 (en) * 2012-06-19 2013-12-27 株式会社村田製作所 Layered multi-core cable
CN104205249A (en) * 2012-06-19 2014-12-10 株式会社村田制作所 Layered multi-core cable
JPWO2017090181A1 (en) * 2015-11-27 2018-09-06 富士通株式会社 Circuit board and electronic device
JP2019216492A (en) * 2018-06-11 2019-12-19 三菱電機株式会社 Electric power conversion system

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