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JPH05800B2 - - Google Patents
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JPH05800B2 - - Google Patents

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Publication number
JPH05800B2
JPH05800B2 JP57027612A JP2761282A JPH05800B2 JP H05800 B2 JPH05800 B2 JP H05800B2 JP 57027612 A JP57027612 A JP 57027612A JP 2761282 A JP2761282 A JP 2761282A JP H05800 B2 JPH05800 B2 JP H05800B2
Authority
JP
Japan
Prior art keywords
current
switch element
branch
voltage state
icirc
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 - Lifetime
Application number
JP57027612A
Other languages
Japanese (ja)
Other versions
JPS58146093A (en
Inventor
Ichiro Ishida
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.)
NEC Corp
Original Assignee
Nippon Electric Co 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP57027612A priority Critical patent/JPS58146093A/en
Priority to US06/467,631 priority patent/US4601015A/en
Priority to EP83101704A priority patent/EP0087163B1/en
Priority to DE8383101704T priority patent/DE3380156D1/en
Publication of JPS58146093A publication Critical patent/JPS58146093A/en
Publication of JPH05800B2 publication Critical patent/JPH05800B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11CSTATIC STORES
    • G11C11/00Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor
    • G11C11/21Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using electric elements
    • G11C11/44Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using electric elements using super-conductive elements, e.g. cryotron

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Hardware Design (AREA)
  • Superconductor Devices And Manufacturing Methods Thereof (AREA)

Description

【発明の詳細な説明】 本発明は一般的には少なくとも一つの情報を循
環電流の形で記憶するジヨセフソン記憶回路の駆
動方法に関する。より具体的には記憶された2進
情報を非破壊的に読み出す(以下NDROという)
ことのできるジヨセフソン記憶回路に関する。更
に特定すれば、本発明は上記記憶装置において超
伝導閉ループを形成している分枝の対の1つに1
つの書き込みゲートを有するジヨセフソン
NDRO記憶回路に関するものである。更に特定
すれば本発明は上記記憶回路において、第1のゲ
ートの制御線内に第2のゲートを配置したジヨセ
フソンNDRO記憶回路の駆動方法に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION The present invention generally relates to a method of driving a Josephson storage circuit that stores at least one piece of information in the form of a circulating current. More specifically, reading stored binary information non-destructively (hereinafter referred to as NDRO)
Concerning the Josephson memory circuit that can be used. More particularly, the present invention provides that in the storage device one of the pairs of branches forming a superconducting closed loop is
Josefson with two write gates
This relates to the NDRO storage circuit. More specifically, the present invention relates to a method for driving a Josephson NDRO memory circuit, in which the second gate is disposed within the control line of the first gate in the memory circuit.

第1図はジヨセフソンNDRO記憶回路の従来
例の一つを説明する為の図である。この例ではス
イツチ素子8とスイツチ素子9はそれぞれ第2図
a,bの特性を有し、書き込み時に行ライン7に
流す電流と読み出し時に行ライン7に流す電流と
はその大きさが異り、2つのレベルの電流を用い
る必要があつた。
FIG. 1 is a diagram for explaining one of the conventional examples of Josephson NDRO storage circuit. In this example, the switch element 8 and the switch element 9 each have the characteristics shown in FIG. It was necessary to use two levels of current.

すなわち、スイツチ素子8と9はそれぞれ下記
のイ,ロの特性を有する。
That is, switch elements 8 and 9 have the following characteristics (a) and (b), respectively.

イ 制御電流(1−K)IYと(1−K)IY+Icirc
に対し零電圧状態にあるバイアス電流IX1領域
と制御電流(1−K)IYに対して零電圧状態に
あり制御電流(1−K)IY+Icircに対して電圧
状態にあるバイアス電流IX0領域とを有する
(第2図b) ロ 上記バイアス電流IX0を制御電流として該制
御電流IX0に対してバイアス電流がKIYの場合に
も更にKIY−Icircの場合にも零電圧状態にあ
り、制御電流IX1+IY′に対してバイアス電流が
KIYの場合にも更にKIY−Icircの場合にも電圧
状態にある(第2図a) 但しIYは列ライン5に流れ超伝導閉ループ2に
流入するバイアス電流であり、Kは(分枝4の自
己インダクタンス)/(分枝3と分枝4の自己イ
ンダクタンスの和)より求まる回路定数であり、
Icircは超伝導閉ループ2に保持される循環電流
でありIX0は読み出し時は行ライン7を流れる電
流であり、IX1は書き込み時に行ライン7を流れ
る電流でありIY′は列ライン6を流れる制御電流
である。初期状態によらず超伝導閉ループ2に循
環電流Icircを流すにはバイアス電流IY及び制御電
流IX1とIY′を同時にそれぞれ列ライン5及び制御
線7,6に流しスイツチ素子8の制御特性によ
り、スイツチ素子8を一時電圧状態としてIYから
スイツチ素子8の最低駆動電流Iminを差し引い
た残りの電流IY−Iminを分枝4に流した後上記バ
イアス電流IY及び制御電流IXとIY′を全て0にす
る。その結果超伝導閉ループ2内に循環電流
Icircが保持される。初期状態によらず超伝導閉
ループ2に循環電流Icircを流さない為にはバイ
アス電流IYを0にして制御電流IX1とIY′のみを流
し、スイツチ素子8を電圧状態にし、超伝導閉ル
ープ2に循環電流Icircが既にある場合にはIcirc
を0とし、既に循環電流Icircが0の場合には超
伝導閉ループ2内に流れ込む電流がないのでその
後制御電流IXとIY′を全て0とすれば該超伝導閉
ループ2内に循環電流は存在しない。
A Control current (1-K) I Y and (1-K) I Y +Icirc
Bias current I in zero voltage state for X1 region and control current (1-K) I Y Bias current I in zero voltage state and in voltage state for Y +Icirc X0 region (Fig. 2b) (b) With the bias current I X0 as the control current, the bias current is KI Y with respect to the control current I , and the bias current is
It is in a voltage state both in the case of KI Y and also in the case of KI Y −Icirc (Fig. 2a). However, I Y is the bias current flowing into the column line 5 and flowing into the superconducting closed loop 2, and K is (min. It is a circuit constant determined from (self-inductance of branch 4)/(sum of self-inductance of branches 3 and 4),
Icirc is the circulating current held in the superconducting closed loop 2, I X0 is the current flowing through the row line 7 during reading, I X1 is the current flowing through the row line 7 during writing, and I This is the control current that flows. In order to cause the circulating current Icirc to flow in the superconducting closed loop 2 regardless of the initial state, bias current I Y and control currents I Then, the switch element 8 is temporarily put in a voltage state, and the remaining current I Y −Imin obtained by subtracting the lowest drive current Imin of the switch element 8 from I Y is passed through the branch 4, and then the bias current I Y and control current I Set all I Y ′ to 0. As a result, a circulating current exists within the superconducting closed loop 2.
Icirc is retained. In order to prevent the circulating current Icirc from flowing in the superconducting closed loop 2 regardless of the initial state, the bias current I Y is set to 0 and only the control currents I If there is already a circulating current Icirc in 2, Icirc
When the circulating current Icirc is already 0, there is no current flowing into the superconducting closed loop 2, so if the control currents I not exist.

超伝導閉ループ2内に循環電流Icircが流れて
いるか否かを読み出す為にはバイアス電流IYと制
御電流IX0を同時にそれぞれ列ライン5と行ライ
ン7に流す。その結果循環電流Icircが保持され
ている場合は分枝4に流れる電流は(1−K)IY
+Icircとなりスイツチ素子9は第2図bに示す
制御特性により電圧状態になり、あるいは循環電
流Icircが保持されていなければ分枝4に流れる
電流は(1−K)IYでスイツチ素子9は第2図b
に示す制御特性により零電圧状態を維持し、この
二つの状態が弁別される。
In order to read whether or not the circulating current Icirc is flowing in the superconducting closed loop 2, a bias current I Y and a control current I X0 are simultaneously passed through the column line 5 and the row line 7, respectively. As a result, if the circulating current Icirc is maintained, the current flowing in branch 4 is (1-K)I Y
+Icirc, and the switch element 9 enters the voltage state according to the control characteristics shown in Figure 2b, or if the circulating current Icirc is not maintained, the current flowing in the branch 4 is (1-K)I Y , and the switch element 9 becomes the Figure 2b
The zero voltage state is maintained by the control characteristics shown in Figure 1, and these two states are discriminated.

書き込み過程においてスイツチ素子9は第2図
bに示す制御特性により零電圧状態を維持し、一
方読み出し過程において行ライン7に電流IX0
流してもスイツチ素子8は第2図aに示す制御特
性により零電圧状態を維持する。
During the write process, the switch element 9 maintains a zero voltage state with the control characteristics shown in FIG. 2b, while in the read process, even if current IX0 is applied to the row line 7, the switch element 8 maintains the control characteristics shown in FIG. 2a. The zero voltage state is maintained by

すなわち従来技術では行ラインに流す電流は書
き込み時と読み出し時では電流レベルを違える必
要があつた。
That is, in the prior art, it was necessary for the current level to be applied to the row line to be different between writing and reading.

本発明の目的は従来の回路機能を維持しながら
その動作機構を簡略化せしめた新規なるジヨセフ
ソン記憶回路の駆動方法を提供する事にある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a novel method for driving a Josephson memory circuit, which simplifies its operating mechanism while maintaining conventional circuit functions.

本発明によれば第1の分枝と第2の分枝から成
る超伝導閉ループと上記第1の分枝中に配置され
たジヨセフソン電流を流しうる第1のスイツチ素
子と、上記第1のスイツチ素子と電磁的に結合す
るように配置された複数の制御線と該制御線の内
の少なくとも一本の制御線内に、上記第2の分枝
と電磁的に結合するように配置されたジヨセフソ
ン電流を流しうる第2のスイツチ素子とから成
り、上記第1のスイツチ素子を書き込みゲートと
して用いて流れる向きの異なる循環電流として
か、あるいは循環電流の有無として進情報を上記
超伝導閉ループに貯え、上記第のスイツチ素子を
読み出しゲートとして用いるジヨセフソン記憶装
置に於いて、上記第2のスイツチ素子は第1の方
向のバイアス電流に対しては上記循環電流の有無
にかかわらず零電圧状態を維持し、第1の方向と
逆向きのバイアス電流に対しては上記循環電流の
ない場合は零電圧状態を維持し、上記循環電流の
ある場合は電圧状態となる非対称特性を有し、上
記第2のスイツチ素子を含む上記第1のスイツチ
素子の制御線に流れる電流の向きが書き込み時と
読み出し時とで異なるように駆動する事と特徴と
するジヨセフソン記憶回路の駆動方法が得られ
る。
According to the present invention, a superconducting closed loop consisting of a first branch and a second branch, a first switch element arranged in the first branch and capable of flowing Josephson current, and a superconducting closed loop comprising a first branch and a second branch; a plurality of control lines arranged so as to be electromagnetically coupled to the element; and within at least one of the control lines, a Josephson arranged so as to be electromagnetically coupled to the second branch. a second switch element capable of passing a current; the first switch element is used as a write gate to store lead information in the superconducting closed loop as circulating currents flowing in different directions or as the presence or absence of circulating current; In the Josephson memory device using the first switch element as a read gate, the second switch element maintains a zero voltage state with respect to the bias current in the first direction regardless of the presence or absence of the circulating current; With respect to the bias current in the opposite direction to the first direction, the second switch has an asymmetric characteristic in which it maintains a zero voltage state when there is no circulating current and becomes a voltage state when there is the circulating current. There is obtained a method of driving a Josephson memory circuit characterized in that the direction of the current flowing through the control line of the first switch element including the element is driven to be different during writing and reading.

以下図面を参照して本発明を詳細に説明する。
本発明の原理はそれぞれ第3図a,bに示す制御
特性、すなわち イ 非対称性の為にIX=IX0の場合は制御電流
(1−K)IYと(1−K)IY+Icircに対して零
電圧状態にあり、IX=−IX0の場合には制御電
流(1−K)IYに対して零電圧状態にあり、一
方制御電流(1−K)IY+Icircに対しては電圧
状態にある正と負のバイアス電流IX0領域を有
する特性(第3図b) ロ 上記正と負のバイアス電流IX0を制御電流と
して該正と負の制御電流IX0に対してバイアス
電流がKIYの場合にもKIY−Icircの場合にも零
電圧状態にあり制御電流IX0+IY′に対してバイ
アス電流がKIYの場合にもKIY−Icircの場合に
も電圧状態にある特性(第3図a) を有する2つのスイツチ素子を第1図に示す如く
超伝導閉ループ2内の第1の分枝3内に上記特性
ロを有するスイツチ素子8を用いて書き込みゲー
トを設け、更に上記書き込みスイツチ8と電磁的
に結合した制御線6及び7を設け、その内の一つ
の制御線7内に上記超伝導閉ループ2内を構成す
る第2の分枝4と電磁的に結合し、且つ特性イを
有するスイツチ素子9を用いて読み出しゲートを
設ける事にある。但しIYは列ライン5を流れ超伝
導閉ループ2に流入するバイアス電流であり、K
は(分枝4の自己インダクタンス)/(分枝3と
分枝4の自己インダクタンスの和)より求まる回
路定数であり、Icircは超伝導閉ループ2に保持
される循環電流であり、IX0は書き込み時に行ラ
イン7を流れる電流であり、−Ixpは読み出し時に
行ライン7を流れる電流であり、IY′は列ライン
6を流れる制御電流である。
The present invention will be described in detail below with reference to the drawings.
The principle of the present invention is based on the control characteristics shown in Fig . 3a and b , respectively. When I X = -I Characteristics having positive and negative bias current I X0 regions in a voltage state ( Fig . 3b) When the bias current is KI Y and when KI Y −Icirc , it is in a zero voltage state , and with respect to the control current I The two switch elements having the characteristic (FIG. 3a) in the state of FIG. Further, control lines 6 and 7 are provided which are electromagnetically coupled to the write switch 8, and one of the control lines 7 is connected to the second branch 4 that constitutes the superconducting closed loop 2. The purpose of the present invention is to provide a read gate using a switch element 9 which is coupled to a switch element 9 and has a characteristic A. However, I Y is the bias current flowing through the column line 5 and flowing into the superconducting closed loop 2, and K
is a circuit constant determined from (self-inductance of branch 4)/(sum of self-inductance of branches 3 and 4), Icirc is the circulating current maintained in superconducting closed loop 2, and I -I xp is the current flowing through the row line 7 during readout, and I Y ' is the control current flowing through the column line 6 during reading.

次に実例をあげて説明する。第4図に本発明を
説明するための図で駆動しようとするジヨセフソ
ンNDRO記憶装置の2×2アレイを示す。
Next, an example will be given and explained. FIG. 4 shows a 2×2 array of Josephson NDRO storage devices to be driven in a diagram for explaining the present invention.

スイツチ素子8及び9はそれぞれ第3図a,b
の制御特性を持つように設計される。Aの記憶状
態によらずAの超伝導閉ループ2に循環電流
Icircを流すにはAの超伝導閉ループ2を含む記
憶セル1に作用するバイアス電流IY及び制御電流
IX0とIY′を同時にそれぞれAに関係する列ライン
5及び制御線7,6にそれぞれ電源10,12,
11より流しAのスイツチ素子8の制御特性によ
りAのスイツチ素子8を一時電圧状態としてIY
らAのスイツチ素子8の最低駆動電流Iminを差
し引いた残りの電流IY−IminをAの分枝4に流し
た後、上記バイアス電流IY及び制御電流IXとIY′を
全て0にする。その結果Aの超伝導閉ループ2内
に循環電流Icircが保持される。
Switch elements 8 and 9 are shown in FIG. 3a and b, respectively.
It is designed to have the control characteristics of Circulating current in superconducting closed loop 2 of A regardless of the memory state of A
To flow Icirc, bias current I Y and control current acting on memory cell 1 including superconducting closed loop 2 of A
I _
According to the control characteristics of the switch element 8 of sink A from 11, the switch element 8 of A is temporarily put in a voltage state, and the remaining current I Y −Imin obtained by subtracting the minimum drive current Imin of the switch element 8 of A from I Y is branched to A. 4, the bias current I Y and control currents I X and I Y ' are all set to zero. As a result, the circulating current Icirc is maintained within the superconducting closed loop 2 of A.

Aの記憶状態によらずAの超伝導閉ループ2に
循環電流Icircを流さない為にはAの記憶セル1
に作用する行ライン7と列ライン6にそれぞれ制
御電流IX0とIY′のみを流し、Aに関係する列ライ
ン5にバイアス電流IYを流さずにおく。その結果
Aのスイツチ素子8は電圧状態になり超伝導閉ル
ープ2に循環電流Icircが既にある場合にはIcirc
を0とし、既に循環電流Icircが0の場合にはA
の超伝導閉ループ2内に流れ込む電流がないの
で、その後制御電流IXとIY′を全て0にすれば該
超伝導ループ2内に循環電流は存在しない。以上
の過程に於いてAの行ライン7にIX0を流しても
Aのスイツチ素子9はその制御特性により零電圧
状態を維持する。Aの超伝導閉ループ2内に循環
電流Icircが流れているか否かを読み出す為には
該超伝導閉ループ2を含む記憶セル1に作用する
バイアス電流IYと制御電流−IX0を同時にそれぞれ
Aに関係する列ライン5と行ライン7に流す。そ
の結果循環電流Icircが保持されている場合はA
の分枝4に流れる電流は(1−K)IY+Icircとな
りAのスイツチ素子9は第3図bに示す制御特性
により電圧状態になり、あるいは循環電流Icirc
が保持されていなければAの分枝4に流れる電流
は(1−K)IYでスイツチ素子9は第3図bに示
す制御特性により零電圧状態を維持し、この二つ
の状態がAに関係する検出器13で弁別される。
この場合Aに関係する行ライン7に電流−IX0
流してもAのスイツチ素子8は第3図aに示す制
御特性によりスイツチする事はない。以上の結果
ジヨセフソンNDRO記憶回路において配線の本
数とそれに対応する電源の個数を減らしたメモリ
回路の機能を維持して回路動作機構を簡略せしめ
る事が出来る。
In order to prevent the circulating current Icirc from flowing in the superconducting closed loop 2 of A regardless of the storage state of A, the memory cell 1 of A is
Only control currents I X0 and I Y ' are allowed to flow through the row line 7 and column line 6 that act on A, respectively, and no bias current I Y is caused to flow through the column line 5 that affects A. As a result, the switch element 8 of A becomes in a voltage state, and if there is already a circulating current Icirc in the superconducting closed loop 2, Icirc
is set to 0, and if the circulating current Icirc is already 0, then A
Since there is no current flowing into the superconducting closed loop 2, if the control currents IX and IY ' are then all set to 0, no circulating current will exist in the superconducting loop 2. In the above process, even if IX0 is applied to the row line 7 of A, the switch element 9 of A maintains a zero voltage state due to its control characteristics. In order to read whether or not the circulating current Icirc is flowing in the superconducting closed loop 2 of A, the bias current I Y and the control current -I It flows to the related column line 5 and row line 7. As a result, if the circulating current Icirc is maintained, A
The current flowing in the branch 4 of is (1-K)I Y +Icirc, and the switch element 9 of A becomes a voltage state due to the control characteristics shown in Fig. 3b, or the circulating current Icirc
If the current is not maintained, the current flowing in the branch 4 of A is (1-K)I Y , and the switch element 9 maintains the zero voltage state according to the control characteristics shown in Figure 3b, and these two states become A. Discrimination is made by the associated detector 13.
In this case, even if a current -I X0 is applied to the row line 7 related to A, the switch element 8 of A will not switch due to the control characteristics shown in FIG. 3a. As a result of the above, in the Josephson NDRO memory circuit, it is possible to maintain the function of the memory circuit by reducing the number of wiring lines and the number of corresponding power supplies, and to simplify the circuit operation mechanism.

第6図に本発明の他の好ましい実施例を説明す
るための図で記憶すべき2進情報が循環電流の向
きによるジヨセフソンNDRO記憶回路の2×2
アレイを示す。スイツチ素子8及び9はそれぞれ
第5図a,bの制御特性を持つように設計され
る。Aの記憶状態によらずAの超伝導閉ループ2
に時計回りのIcirc(以下+Icircという)を流す為
にはAに関係する制御線6と行ライン7に制御電
流ID及びIX0とAに関係する列ライン5にバイアス
電流IYを同時に流しAのスイツチ素子8の制御特
性に従つてAのスイツチ素子8を一時電圧状態と
しバイアス電流IYからAのスイツチ素子8の最低
駆動電流Iminを差し引いた電流IY−IminをAの
分枝4に流しその後制御電流ID及びIXとバイアス
電流IYとを全て0とする。その結果Aの超伝導閉
ループ内に+Icircが保持される。
FIG. 6 is a diagram for explaining another preferred embodiment of the present invention, in which the binary information to be stored is 2×2 of the Josephson NDRO storage circuit according to the direction of the circulating current.
An array is shown. Switch elements 8 and 9 are designed to have the control characteristics shown in FIGS. 5a and 5b, respectively. Superconducting closed loop 2 of A regardless of the memory state of A
In order to flow clockwise Icirc (hereinafter referred to as +Icirc), a control current I D is applied to the control line 6 and row line 7 related to A, and a bias current I Y is applied to I X0 and column line 5 related to A at the same time. According to the control characteristics of the switch element 8 of A, the switch element 8 of A is temporarily put in a voltage state, and the current I Y −Imin obtained by subtracting the lowest drive current Imin of the switch element 8 of A from the bias current I Y is applied to the branch 4 of A. After that, the control currents I D and I X and the bias current I Y are all set to 0. As a result, +Icirc is maintained within the superconducting closed loop of A.

Aの記憶状態によらずAの超伝導閉ループ2に
反時計回りの循環電流Icirc(以下−Icircという)
を流す為にはAに関係する制御線6と行ライン7
に制御電流ID及びIX0とAに関係する列ライン5に
バイアス電流−IYを同時に流し、Aのスイツチ素
子8の制御特性に従つてAのスイツチ素子8を一
時電圧状態とし、バイアス電流IYからAのスイツ
チ素子8の最低駆動電流−Iminを差し引いた電
流−(IY−Imin)をAの分枝4に流し、その後制
御電流ID及びIXとバイアス電流−IYを全て0とす
る。その結果Aの超伝導閉ループ内に−Icircが
保持される。以上の二通りの書き込み過程におい
て、スイツチ素子9は第5図bに示す制御特性に
より、零電圧状態を維持する。
A counterclockwise circulating current Icirc (hereinafter referred to as −Icirc) is generated in the superconducting closed loop 2 of A regardless of the memory state of A.
In order to flow the control line 6 and row line 7 related to A.
A bias current -I Y is simultaneously applied to the control currents I D and I A current obtained by subtracting the lowest driving current -Imin of the switch element 8 of A from I Y (I Y - Imin) is passed through the branch 4 of A, and then all of the control currents I D and I X and the bias current - I Y are passed through the branch 4 of A. Set to 0. As a result, -Icirc is maintained within the superconducting closed loop of A. In the above two write processes, the switch element 9 maintains the zero voltage state due to the control characteristics shown in FIG. 5b.

Aの超伝導閉ループ2に循環電流Icircがいず
れの向きに流れているかを判定するには、Aに関
係する列ライン5にバイアス電流IY、Aに関係す
る行ライン7に読み出し電流−IX0を同時に流し
その結果+Icircが保持されている場合はAの分
枝4に(1−K)IY+Icircの電流が流れスイツチ
素子9は第5図bに示す制御特性に従つて電圧状
態となり−Icircが保持されている場合はAの分
枝4に(1−K)IY−Icircの電流が流れスイツチ
素子9は零電圧状態を維持し、この二つの状態が
Aに関係する検出器15で弁別される。この読み
出し過程に於いてAに関係する行ライン7に電流
−IX0を流してもAのスイツチ素子8は第5図a
に示す制御特性によりスイツチする事はない。
To determine in which direction the circulating current Icirc is flowing in the superconducting closed loop 2 of A, a bias current I Y is applied to the column line 5 related to A, and a readout current −I X0 is applied to the row line 7 related to A. are simultaneously applied, and as a result, if +Icirc is maintained, a current of (1-K)I Y +Icirc flows in branch 4 of A, and switch element 9 becomes in a voltage state according to the control characteristics shown in Figure 5b. When Icirc is maintained, a current of (1-K)I Y -Icirc flows through the branch 4 of A, and the switch element 9 maintains a zero voltage state, and these two states are detected by the detector 15 related to A. It is distinguished by In this readout process, even if a current -I X0 is applied to the row line 7 related to A, the switch element 8 of A is
There is no switching due to the control characteristics shown in .

以上実施例につき説明したが、本発明の主要部
分は第1のゲートの制御線内に第2のゲートを設
けたジヨセフソンNDRO記憶回路に於いて第2
のゲートを含む第1のゲートの制御線を流れる電
流の向きを書き込み時と読み出し時とで違えた事
によりメモリ機能を実現できる事である。
Although the embodiments have been described above, the main part of the present invention is that the second
The memory function can be realized by changing the direction of the current flowing through the control line of the first gate including the gate during writing and reading.

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

第1図は従来技術及び本発明を説明する為のジ
ヨセフソンNDRO記憶回路の1つのセルを示す
図である。第2図a,bはそれぞれ第1図のセル
に用いられた従来技術によるスイツチ素子の制御
特性を示す図である。第3図は本発明の一実施例
を説明するためのスイツチ素子の制御特性を示す
図である。第4図は本発明の一実施例を説明する
ための図でジヨセフソンNDRO記憶回路の2×
2アレイを示す図である。第5図は本発明の他の
実施例を説明するためのスイツチ素子の制御特性
を示す図である。第6図は本発明の他の実施例を
説明するためのジヨセフソンNDRO記憶回路の
2×2アレイを示す図である。 図において、1は記憶セル、2は超伝導閉ルー
プ、3,4は分枝路、5は列ライン、6は制御列
ライン、7は行ライン、8,9はスイツチ素子、
10,11,12は電源、13は検出器である。
FIG. 1 is a diagram illustrating one cell of a Josephson NDRO storage circuit for explaining the prior art and the present invention. FIGS. 2a and 2b are diagrams showing the control characteristics of the conventional switch element used in the cell of FIG. 1, respectively. FIG. 3 is a diagram showing control characteristics of a switch element for explaining one embodiment of the present invention. FIG. 4 is a diagram for explaining one embodiment of the present invention, and is a diagram for explaining an embodiment of the present invention.
FIG. 2 is a diagram showing two arrays. FIG. 5 is a diagram showing control characteristics of a switch element for explaining another embodiment of the present invention. FIG. 6 is a diagram illustrating a 2×2 array of Josephson NDRO storage circuits to illustrate another embodiment of the present invention. In the figure, 1 is a storage cell, 2 is a superconducting closed loop, 3 and 4 are branch circuits, 5 is a column line, 6 is a control column line, 7 is a row line, 8 and 9 are switch elements,
10, 11, and 12 are power supplies, and 13 is a detector.

Claims (1)

【特許請求の範囲】[Claims] 1 第1の分枝と第2の分枝からなる超伝導閉ル
ープと、上記第1の分枝中に配置されたジヨセフ
ソン電流を流しうる第1のスイツチ素子と、上記
第1のスイツチ素子と電磁的に結合するように配
置された複数の制御線と該制御線の内の少なくと
も一本の制御線内に、上記第2の分枝と電磁的に
結合するように配置されたジヨセフソン電流を流
しうる第2のスイツチ素子とから成り、上記第1
のスイツチ素子を書き込みゲートとして用いて流
れる向きの異なる循環電流、あるいは循環電流の
有無として2進情報を上記超伝導閉ループに貯
え、上記第2のスイツチ素子を読み出しゲートと
して用いるジヨセフソン記憶回路の駆動に於い
て、上記第2のスイツチ素子は第1の方向のバイ
アス電流に対しては上記循環電流の有無にかかわ
らず零電圧状態を維持し、第1の方向と逆向きの
バイアス電流に対しては上記循環電流のない場合
は零電圧状態を維持し、上記循環電流のある場合
は電圧状態となる非対称特性を有し、上記第2の
スイツチ素子を含む上記第1のスイツチ素子の制
御線に流れる電流の向きが書き込み時と読み出し
時とで異なるように駆動する事を特徴とするジヨ
セフソン記憶回路の駆動方法。
1. A superconducting closed loop consisting of a first branch and a second branch, a first switch element arranged in the first branch and capable of flowing Josephson current, and A Josephson current is passed through at least one of the plurality of control lines arranged so as to be coupled to the second branch electromagnetically. and a second switch element that is
The second switch element is used as a write gate to store binary information in the superconducting closed loop as circulating currents flowing in different directions or the presence or absence of the circulating current, and the second switch element is used as a read gate to drive a Josephson memory circuit. The second switch element maintains a zero voltage state with respect to the bias current in the first direction regardless of the presence or absence of the circulating current, and maintains a zero voltage state with respect to the bias current in the opposite direction to the first direction. It has an asymmetrical characteristic that maintains a zero voltage state when there is no circulating current and becomes a voltage state when there is a circulating current, and flows in the control line of the first switch element including the second switch element. A method for driving a Josephson memory circuit characterized by driving the current in different directions during writing and reading.
JP57027612A 1982-02-23 1982-02-23 Method for driving josephson storage circuit Granted JPS58146093A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP57027612A JPS58146093A (en) 1982-02-23 1982-02-23 Method for driving josephson storage circuit
US06/467,631 US4601015A (en) 1982-02-23 1983-02-18 Josephson memory circuit
EP83101704A EP0087163B1 (en) 1982-02-23 1983-02-22 Josephson memory circuit
DE8383101704T DE3380156D1 (en) 1982-02-23 1983-02-22 Josephson memory circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57027612A JPS58146093A (en) 1982-02-23 1982-02-23 Method for driving josephson storage circuit

Publications (2)

Publication Number Publication Date
JPS58146093A JPS58146093A (en) 1983-08-31
JPH05800B2 true JPH05800B2 (en) 1993-01-06

Family

ID=12225751

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57027612A Granted JPS58146093A (en) 1982-02-23 1982-02-23 Method for driving josephson storage circuit

Country Status (1)

Country Link
JP (1) JPS58146093A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS613396A (en) * 1984-06-15 1986-01-09 Agency Of Ind Science & Technol Josephine memory device of bipolar current drive type

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4130893A (en) * 1977-03-29 1978-12-19 International Business Machines Corporation Josephson memory cells having improved NDRO sensing

Also Published As

Publication number Publication date
JPS58146093A (en) 1983-08-31

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