JPH0136274B2 - - Google Patents
Info
- Publication number
- JPH0136274B2 JPH0136274B2 JP56201243A JP20124381A JPH0136274B2 JP H0136274 B2 JPH0136274 B2 JP H0136274B2 JP 56201243 A JP56201243 A JP 56201243A JP 20124381 A JP20124381 A JP 20124381A JP H0136274 B2 JPH0136274 B2 JP H0136274B2
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- current
- ground plane
- base electrode
- josephson junction
- 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.)
- Expired
Links
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N60/00—Superconducting devices
- H10N60/10—Junction-based devices
- H10N60/12—Josephson-effect devices
Landscapes
- Superconductor Devices And Manufacturing Methods Thereof (AREA)
Description
【発明の詳細な説明】
(1) 発明の技術分野
本発明はジヨセフソン接合を有するジヨセフソ
ン集積回路に関する。DETAILED DESCRIPTION OF THE INVENTION (1) Technical Field of the Invention The present invention relates to a Josephson integrated circuit having a Josephson junction.
(2) 技術の背景
通常ジヨセフソン接合を形成している対向電極
は、基部電極、制御電極と異なる材料を用いてお
り(たとえば基部電極と制御電極は鉛、インジユ
ウム、金の合金に対して、対向電極は鉛、ビスマ
スの合金である。)一例として対向電極と、制御
電極を接続した場合には、グレーンマイグレーシ
ヨンが生じたり、対向電極の材料的な問題から接
触抵抗が生じたりする。これを避けるためにスイ
ツチ素子として使用しているジヨセフソン接合に
比べて十分広い面積で、ジヨセフソン接合を介し
て対向電極から基部電極に接続したのち基部電極
と制御電極とを接続する。(2) Background of the technology Normally, the opposing electrode that forms the Josephson junction uses a different material from the base electrode and the control electrode (for example, the base electrode and the control electrode are made of an alloy of lead, indium, and gold, while the opposing electrode (The electrode is an alloy of lead and bismuth.) For example, when a counter electrode and a control electrode are connected, grain migration may occur or contact resistance may occur due to problems with the material of the counter electrode. To avoid this, the opposite electrode is connected to the base electrode via a Josephson junction, which has a sufficiently wider area than the Josephson junction used as a switch element, and then the base electrode and the control electrode are connected.
(3) 従来技術の問題点
この際従来は配線のインダクタンスを小さくし
たり、ストリツプライン構成のためのグランドプ
レーンがこの接続部にも敷かれていた。(3) Problems with the prior art At this time, in the past, the inductance of the wiring was reduced, and a ground plane for the stripline configuration was also laid at this connection.
例えば第1図aに示すインライン型のジヨセフ
ソン接合を介して対向電極1と基部電極2が接続
され、グランドプレーン3がその接続部の下にも
設けられていると、グランドプレーン3に流れる
イメージ電流によりジヨセフソン接合の閾値は第
1図bに示すようになる。 For example, if the counter electrode 1 and the base electrode 2 are connected via an in-line Josephson junction as shown in FIG. Therefore, the threshold value of the Josephson junction becomes as shown in FIG. 1b.
その理由を、より詳細に説明する。 The reason will be explained in more detail.
第1図cは、同図aの断面図であり、基部電極
2を流れる電流i1は、ジヨセフソン接合4を介し
て対向電極1に電流i4として流れる。電流i1およ
びi4は各電極の下表面を流れる。この際、グラン
ドプレーン3の表面には、電流i1,i4のイメージ
電流i2が流れ、また基部電極2のジヨセフソン接
合と接する上表面には、電流i4のイメージ電流i3
が夫々、矢印の方向に流れる。この状況を第1図
cの右側から見た様子を同dに示す。 FIG. 1c is a cross-sectional view of FIG. Currents i 1 and i 4 flow on the lower surface of each electrode. At this time, an image current i 2 of currents i 1 and i 4 flows on the surface of the ground plane 3, and an image current i 3 of current i 4 flows on the upper surface in contact with the Josephson junction of the base electrode 2 .
flows in the direction of the arrow. This situation is shown in Fig. 1(d) when viewed from the right side of Fig. 1(c).
第1図dに明らかなように、対向電極1の下表
面を流れる電極i4は紙面に垂直な手前方向に、基
部電極2の上表面を流れるイメージ電流i3は紙面
奥方向に、基部電極2の下表面を流れる電極i1は
手前方向に、グランドプレーン3表面を流れるイ
メージ電流i2は奥方向にそれぞれ流れる。従つて
各電流によつて生じる磁界は各電流のまわりに矢
印で示す方向に生ずる。 As is clear from FIG. 1d, the electrode i 4 flowing on the lower surface of the counter electrode 1 is directed toward the front perpendicular to the paper, and the image current i 3 flowing on the upper surface of the base electrode 2 is directed toward the back of the paper. The electrode i 1 flowing on the lower surface of the ground plane 2 flows toward the front, and the image current i 2 flowing on the surface of the ground plane 3 flows toward the back. The magnetic field produced by each current therefore occurs around each current in the direction indicated by the arrow.
ここでジヨセフソン接合4の上下を流れる電流
i3とi4についてみると、各電流によつて発生する
磁界の向きは、ジヨセフソン接合に関してみれば
左から右方向に向かつたものとなる。 Here, the current flowing above and below Josephson junction 4
Regarding i 3 and i 4 , the direction of the magnetic field generated by each current is from the left to the right with respect to the Josephson junction.
即ち、グランドプレーンがある場合には、電流
i3,i4により、あたかも外部磁界が加わつた状態
と同様になる。 That is, if there is a ground plane, the current
Due to i 3 and i 4 , the state is the same as if an external magnetic field was applied.
従つて、ジヨセフソン接合4が超伝導状態でい
られる臨界電流Icの大きさは、接合本来の磁界が
加えられていない状態での臨界電流値より小さく
なる。 Therefore, the magnitude of the critical current Ic that allows the Josephson junction 4 to remain in a superconducting state is smaller than the critical current value when no magnetic field is applied to the junction.
また、外部より電流i3,i4により発生した磁界
を打ち消すだけの磁界を外部より加えて、はじめ
て最大の臨界電流となる。 Furthermore, the maximum critical current is achieved only when a magnetic field is applied from the outside that is sufficient to cancel out the magnetic field generated by the currents i 3 and i 4 .
以上の理由により、ジヨセフソン接合4は、第
1図bに示す特性となる。これまでの説明で明ら
かなように、グランドプレーンがある場合には、
外部磁界を加えていないにもかかわらず、接続面
積等によつて決定される最大の臨界電流を流すこ
とはできない。 For the above reasons, the Josephson junction 4 has the characteristics shown in FIG. 1b. As is clear from the previous discussion, if there is a ground plane,
Even though no external magnetic field is applied, the maximum critical current determined by the connection area etc. cannot flow.
従つて、ジヨセフソン接合が電圧状態とならず
に、大きな超伝導電流を流すためには、接合面積
を大きくしなければならず、高集積化のさまたげ
となつていた。 Therefore, in order for the Josefson junction to flow a large superconducting current without being in a voltage state, the junction area must be increased, which has been an obstacle to higher integration.
(4) 発明の目的
本発明の目的は、上記欠点をなくし、接続部の
面積を増大させることなく最大の臨界電流を流す
ことができるようにすることにある。(4) Purpose of the Invention The purpose of the present invention is to eliminate the above-mentioned drawbacks and to enable the maximum critical current to flow without increasing the area of the connection portion.
(5) 発明の構成
上記目的は、グランドプレーン上に基部電極お
よび対向電極を有するジヨセフソン集積回路にお
いて、該グランドプレーンに窓部が設けられ、該
窓部上で該基部電極と該対向電極とが接続される
ことにより達成される。(5) Structure of the Invention The above object is to provide a Josephson integrated circuit having a base electrode and a counter electrode on a ground plane, wherein the ground plane is provided with a window, and the base electrode and the counter electrode are connected on the window. This is achieved by being connected.
(6) 発明の実施例
第2図は本発明の一実施例を説明する図で、第
2図aは平面図、第2図bはその等価回路図であ
る。(6) Embodiment of the Invention FIG. 2 is a diagram illustrating an embodiment of the present invention, in which FIG. 2a is a plan view and FIG. 2b is an equivalent circuit diagram thereof.
第2図aにおいて21,21′はバイアス電流
Ibが流れる基部電極、22は負荷抵抗、23,2
3′は対向電極、24,24′は入力信号Sが入力
される制御電極、25は基部電極、26はグラン
ドプレーン、27はグランドプレーンに設けられ
た窓部である。グランドプレーン26は、対向電
極23と基部電極25の接続部の下の窓部27を
除いて一面に設けられている。 In Figure 2a, 21 and 21' are bias currents
Base electrode through which Ib flows, 22 is load resistance, 23,2
3' is a counter electrode, 24 and 24' are control electrodes to which the input signal S is input, 25 is a base electrode, 26 is a ground plane, and 27 is a window provided in the ground plane. The ground plane 26 is provided over one surface except for a window 27 below the connection between the counter electrode 23 and the base electrode 25.
第2図cは第2図aの窓部27上における基部
電極25と上部電極23との接続部を示す部分断
面図である。 FIG. 2c is a partial cross-sectional view showing the connecting portion between the base electrode 25 and the upper electrode 23 on the window portion 27 of FIG. 2a.
第2図aにおけるゲート用のジヨセフソン接合
J1が電圧状態となり、電流が、負荷抵抗22、制
御電極24′から成るループに流れると、その電
流は窓部27上において第2図cに示すように、
各電極の上下表面を矢印の方向に流れる。これを
右から見ると、第2図dに示すように、ジヨセフ
ソン接合4の上下に流れる電流は同じ紙面奥に向
かつて流れるので、両電流によつて発生する磁界
の向きは、接合4においては互いに逆向きとな
り、打消し合う。 Josephson junction for the gate in Figure 2a
When J 1 is in a voltage state and a current flows through the loop consisting of the load resistor 22 and the control electrode 24', the current flows across the window 27 as shown in FIG. 2c.
Flows in the direction of the arrow on the upper and lower surfaces of each electrode. Looking at this from the right, as shown in Figure 2 d, the currents flowing above and below Josephson junction 4 flow toward the same depth in the plane of the paper, so the direction of the magnetic field generated by both currents is They are opposite to each other and cancel each other out.
従つて外部から磁界を加えない限り、接合4に
は磁界は加わらない。 Therefore, no magnetic field is applied to the junction 4 unless a magnetic field is applied from the outside.
従つて外部磁界φ=0のときに最大の臨界電流
とする、即ち、第1図bの特性曲線のピーク点を
φ=0の点にもつてくることができる。 Therefore, the maximum critical current can be obtained when the external magnetic field φ=0, that is, the peak point of the characteristic curve shown in FIG. 1b can be brought to the point φ=0.
よつて接続部の面積を大きくすることなく、最
大臨界電流を流すことができるようになる。 Therefore, the maximum critical current can be passed without increasing the area of the connection portion.
第2図bは第2図aの等価回路であり、本発明
によれば負荷抵抗22を含むループに接続部面積
を増大させることなく、大きな電流を流すことが
できる。 FIG. 2b is an equivalent circuit of FIG. 2a, and according to the present invention, a large current can be passed through the loop including the load resistor 22 without increasing the connection area.
(7) 発明の効果
本発明によれば、ジヨセフソン集積回路におけ
る基部電極と対向電極の接続部面積を増大させる
ことなく最大の臨界電流を流すことができるので
ジヨセフソン接合による集積回路の集積度を高め
る事が出来る。(7) Effects of the Invention According to the present invention, the maximum critical current can be passed without increasing the connection area between the base electrode and the counter electrode in the Josephson integrated circuit, thereby increasing the degree of integration of the integrated circuit using the Josephson junction. I can do things.
第1図は従来例を説明する図、第2図は、本発
明の一実施例を説明する図である。21,21′,
25:基部電極、23,23′:対向電極、2
6:グランドプレーン、27:窓部。
FIG. 1 is a diagram for explaining a conventional example, and FIG. 2 is a diagram for explaining an embodiment of the present invention. 21, 21',
25: base electrode, 23, 23': counter electrode, 2
6: Ground plane, 27: Window section.
Claims (1)
極を有するジヨセフソン集積回路において、該グ
ランドプレーンに窓部が設けられ、該窓部上で該
基部電極と該対向電極とが接続されてなることを
特徴とするジヨセフソン集積回路。1. A Josephson integrated circuit having a base electrode and a counter electrode on a ground plane, characterized in that the ground plane is provided with a window, and the base electrode and the counter electrode are connected on the window. Josefson integrated circuit.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56201243A JPS58102579A (en) | 1981-12-14 | 1981-12-14 | Josephson integrated circuit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56201243A JPS58102579A (en) | 1981-12-14 | 1981-12-14 | Josephson integrated circuit |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58102579A JPS58102579A (en) | 1983-06-18 |
| JPH0136274B2 true JPH0136274B2 (en) | 1989-07-31 |
Family
ID=16437706
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56201243A Granted JPS58102579A (en) | 1981-12-14 | 1981-12-14 | Josephson integrated circuit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58102579A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60178675A (en) * | 1984-02-24 | 1985-09-12 | Agency Of Ind Science & Technol | Superconductive transformer |
| JP2007112548A (en) * | 2005-10-19 | 2007-05-10 | Gecoss Corp | Steel sheet pile lifting tool |
-
1981
- 1981-12-14 JP JP56201243A patent/JPS58102579A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58102579A (en) | 1983-06-18 |
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