JPH01123438A - Superconducting wiring integrated circuit - Google Patents
Superconducting wiring integrated circuitInfo
- Publication number
- JPH01123438A JPH01123438A JP62281695A JP28169587A JPH01123438A JP H01123438 A JPH01123438 A JP H01123438A JP 62281695 A JP62281695 A JP 62281695A JP 28169587 A JP28169587 A JP 28169587A JP H01123438 A JPH01123438 A JP H01123438A
- Authority
- JP
- Japan
- Prior art keywords
- wiring
- superconducting
- integrated circuit
- superconducting wiring
- temperature
- 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
- 239000000463 material Substances 0.000 claims abstract description 23
- 239000000126 substance Substances 0.000 claims abstract description 5
- 239000002184 metal Substances 0.000 abstract description 4
- 238000000034 method Methods 0.000 abstract 1
- 230000007257 malfunction Effects 0.000 description 5
- 238000010586 diagram Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 230000020169 heat generation Effects 0.000 description 3
- 239000004065 semiconductor Substances 0.000 description 3
- 239000004020 conductor Substances 0.000 description 2
- 239000012212 insulator Substances 0.000 description 2
- 239000000758 substrate Substances 0.000 description 2
- 239000002470 thermal conductor Substances 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 239000010410 layer Substances 0.000 description 1
- 239000002356 single layer Substances 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は超電導材料で形成された配線部を有する超電
導配線集積回路に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to a superconducting wiring integrated circuit having a wiring portion formed of a superconducting material.
半導体メモリ素子に代表されるような大規模集積回路に
おいては、その集積度が向上すればする程、全体の遅延
に対する配線部での遅延の割合が大きくなってきている
。従って大規模集積回路において、配線部を超電導材料
で形成するということは素子の高速化という点で非常に
有利であると考えられる。即ち、超電導材料は臨界温度
以下では電気抵抗が0Ωになるので、配線部を超電導材
料で形成した素子を臨界温度以下で動作させた場合には
配線部のCR時定数がOになり、配線遅延は全くなくな
る。In large-scale integrated circuits such as semiconductor memory devices, as the degree of integration increases, the proportion of delay in wiring to the total delay increases. Therefore, in large-scale integrated circuits, forming the wiring portion from a superconducting material is considered to be very advantageous in terms of increasing the speed of the device. In other words, the electrical resistance of superconducting materials becomes 0 Ω below the critical temperature, so when an element whose wiring part is made of superconducting material is operated below the critical temperature, the CR time constant of the wiring part becomes O, and the wiring delay completely disappears.
第2図に超電導材料を配線として用いた場合の一例を示
す0図において、1は半導体基板、2は絶縁体、3は超
電導配線、4は超電導配線3とのコンタクトを有する導
電体による配線である。In Fig. 2, which shows an example of a case where a superconducting material is used as wiring, 1 is a semiconductor substrate, 2 is an insulator, 3 is a superconducting wiring, and 4 is a wiring made of a conductor having contact with the superconducting wiring 3. be.
一般に集積回路素子の動作中のジュール発熱は局部的で
ある。従ってその素子内の配線の温度分布も一様でない
。従って第2図に示すような一層構造の超電導配線を有
する集積回路の場合も素子温度の上昇とともに配線を形
成する超電導材料は局部的に高温になると考えられる。Generally, Joule heating during operation of an integrated circuit device is localized. Therefore, the temperature distribution of the wiring within the element is also not uniform. Therefore, even in the case of an integrated circuit having a single-layer superconducting wiring structure as shown in FIG. 2, it is thought that as the element temperature rises, the superconducting material forming the wiring becomes locally hot.
そしてその温度がその超電導材料の臨界温度を超えると
その部分は抵抗体に変わるためにその部分で局部的に信
号遅延が生ずる事になり、素子内で信号間にタイミング
のずれが生じ、誤動作を起こすことになる。When that temperature exceeds the critical temperature of the superconducting material, that part turns into a resistor, causing a local signal delay in that part, causing a timing shift between signals within the element, which can lead to malfunction. I'll wake you up.
従来の超電導配線集積回路は以上のように構成されてい
るので、動作中、素子自体のジュール発熱により温度が
上昇し、配線を形成する超電導材料が局部的に臨界温度
を超えると、その部分は抵抗体に変わるためにその部分
で局部的に信号遅延が生ずることになり、素子内で信号
間にタイミングのずれが生じ、誤動作を起こす可能性が
あるという問題点があった。Conventional superconducting interconnect integrated circuits are configured as described above, so when the temperature rises due to the Joule heat generation of the element itself during operation and the superconducting material forming the interconnect locally exceeds the critical temperature, that part will Since the element is replaced by a resistor, a local signal delay occurs in that part, causing a timing shift between signals within the element, which may cause malfunction.
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、素子の動作中そのジュール発熱により素子温
度が上昇しても配線部を形成する超電導材料は臨界温度
を超えないような超電導配線集積回路を提供することを
目的とする。This invention was made in order to solve the above-mentioned problems, and the superconducting material forming the wiring part is made of superconducting material that does not exceed the critical temperature even if the element temperature rises due to Joule heat generation during the operation of the element. The purpose is to provide wiring integrated circuits.
この発明に係る超電導配線集積回路は、その超電導配線
を超電導材料からなる配線と金属のような熱伝導の良い
物質との2N構造配線にしたものである。The superconducting wiring integrated circuit according to the present invention has a 2N structure wiring including wiring made of a superconducting material and a material having good thermal conductivity such as metal.
この発明における超電導配線集積回路は、その超電導配
線を超電導材料からなる配線と例えば金属のような熱伝
導の良い物質との2N構造にしたので、配線を形成する
超電導材料の温度が局部的にも臨界温度を超えるという
ことがなくなり、素子内に信号間のタイミングのずれが
なくなり、誤動作を防ぐことができる。The superconducting wiring integrated circuit according to the present invention has a 2N structure in which the superconducting wiring is made of a superconducting material and a substance with good thermal conductivity such as metal, so that the temperature of the superconducting material forming the wiring can be locally reduced. The critical temperature will not be exceeded, there will be no timing deviation between signals within the device, and malfunctions can be prevented.
以下、本発明の一実施例を図について説明する。 An embodiment of the present invention will be described below with reference to the drawings.
第1図は本発明の一実施例による超電導配線集積回路を
示す図である。図において、1は半導体基板、2は絶縁
体、30は超電導配線部3と熱伝導の良い材料5との2
層構造により構成した超電導配線、4は超電導配線部3
とのコンタクトを有する感電体による配線である。FIG. 1 is a diagram showing a superconducting wiring integrated circuit according to an embodiment of the present invention. In the figure, 1 is a semiconductor substrate, 2 is an insulator, and 30 is a superconducting wiring part 3 and a material 5 with good thermal conductivity.
Superconducting wiring configured with a layered structure, 4 is superconducting wiring part 3
This is wiring using an electric shock body that has a contact with.
本実施例では超電導配線30を超電導配線部3と良熱伝
導体5との2N構造にしたので、この良熱伝導体5が超
電導配線部3の温度分布を均一に保ち、素子の動作中、
素子のジュール発熱により素子温度が上昇しても超電導
配線部の温度分布をより均一に保つことが出来、超電導
配線の一部が局部的に非常に高温になるという現象を避
けることができる。そのため、配線を形成する超電導材
料の温度が局部的にも臨界温度を超えるということがな
くなり、素子内に信号間のタイミングのずれがなくなり
、誤動作を防ぐことができる。In this embodiment, the superconducting wiring 30 has a 2N structure consisting of the superconducting wiring part 3 and the good thermal conductor 5, so that the good thermal conductor 5 keeps the temperature distribution of the superconducting wiring part 3 uniform, and during the operation of the element,
Even if the element temperature rises due to Joule heat generation in the element, the temperature distribution of the superconducting wiring can be kept more uniform, and it is possible to avoid a phenomenon in which a part of the superconducting wiring becomes locally extremely hot. Therefore, the temperature of the superconducting material forming the wiring does not locally exceed the critical temperature, there is no timing shift between signals within the device, and malfunctions can be prevented.
以上のようにこの発明に係る超電導配線集積回路によれ
ば、超電導配線を超電導材料からなる配線と例えば金属
のような熱伝導の良い材料との2層構造にしたので、超
′:ji導配線部の温度分布を均一に保たせることが出
来、それゆえに超電導配線部の温度が局部的にも臨界温
度を超えることを避けることができ、超電導配線部の一
部が局部的に抵抗体に変わることに起因する信号間のタ
イミングのずれによる誤動作を防止できる効果がある。As described above, according to the superconducting wiring integrated circuit according to the present invention, the superconducting wiring has a two-layer structure of the wiring made of a superconducting material and the material having good thermal conductivity such as metal, so that the superconducting wiring Therefore, the temperature of the superconducting wiring section can be prevented from exceeding the critical temperature locally, and a part of the superconducting wiring section locally turns into a resistor. This has the effect of preventing malfunctions due to timing shifts between signals caused by this.
第1図は本発明の一実施例の超電導配線集積回路図、第
2図は従来の超電導配線集積回路図である−6
1は半導体基板、2は絶縁体、3は超電導配線部、4は
導電体配線、5は熱伝導の良い物質、30は超電導配線
である。
なお図中同一符号は同−又は相当部分を示す。Fig. 1 is a diagram of a superconducting wiring integrated circuit according to an embodiment of the present invention, and Fig. 2 is a diagram of a conventional superconducting wiring integrated circuit. Conductor wiring, 5 is a material with good thermal conductivity, and 30 is superconducting wiring. Note that the same reference numerals in the figures indicate the same or equivalent parts.
Claims (1)
おいて、 上記超電導配線を超電導材料からなる配線と熱伝導の良
い物質との2層構造配線にしたことを特徴とする超電導
配線集積回路。(1) An integrated circuit having wiring formed of a superconducting material, characterized in that the superconducting wiring has a two-layer structure of wiring made of a superconducting material and a substance with good thermal conductivity.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62281695A JPH01123438A (en) | 1987-11-07 | 1987-11-07 | Superconducting wiring integrated circuit |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62281695A JPH01123438A (en) | 1987-11-07 | 1987-11-07 | Superconducting wiring integrated circuit |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01123438A true JPH01123438A (en) | 1989-05-16 |
Family
ID=17642693
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP62281695A Pending JPH01123438A (en) | 1987-11-07 | 1987-11-07 | Superconducting wiring integrated circuit |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01123438A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008301568A (en) * | 2007-05-29 | 2008-12-11 | Mitsubishi Electric Corp | Squirrel-cage rotor, induction motor, and method of manufacturing squirrel-cage rotor |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60154613A (en) * | 1984-01-25 | 1985-08-14 | Hitachi Ltd | Semiconductor device for ultra-low temperature |
JPS6413743A (en) * | 1987-07-08 | 1989-01-18 | Hitachi Ltd | Superconductive wiring structure |
JPS6427244A (en) * | 1987-04-08 | 1989-01-30 | Hitachi Ltd | Wiring construction of integrated circuit |
JPH01120845A (en) * | 1987-11-04 | 1989-05-12 | Seiko Epson Corp | Superconducting wiring |
-
1987
- 1987-11-07 JP JP62281695A patent/JPH01123438A/en active Pending
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60154613A (en) * | 1984-01-25 | 1985-08-14 | Hitachi Ltd | Semiconductor device for ultra-low temperature |
JPS6427244A (en) * | 1987-04-08 | 1989-01-30 | Hitachi Ltd | Wiring construction of integrated circuit |
JPS6413743A (en) * | 1987-07-08 | 1989-01-18 | Hitachi Ltd | Superconductive wiring structure |
JPH01120845A (en) * | 1987-11-04 | 1989-05-12 | Seiko Epson Corp | Superconducting wiring |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008301568A (en) * | 2007-05-29 | 2008-12-11 | Mitsubishi Electric Corp | Squirrel-cage rotor, induction motor, and method of manufacturing squirrel-cage rotor |
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