JPS608551B2 - Cylindrical domain element - Google Patents

Cylindrical domain element

Info

Publication number
JPS608551B2
JPS608551B2 JP2846277A JP2846277A JPS608551B2 JP S608551 B2 JPS608551 B2 JP S608551B2 JP 2846277 A JP2846277 A JP 2846277A JP 2846277 A JP2846277 A JP 2846277A JP S608551 B2 JPS608551 B2 JP S608551B2
Authority
JP
Japan
Prior art keywords
cylindrical
magnetic domain
cylindrical magnetic
domain
conductor
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
Application number
JP2846277A
Other languages
Japanese (ja)
Other versions
JPS53112620A (en
Inventor
昭男 森本
治雄 浦井
幸一 吉見
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 JP2846277A priority Critical patent/JPS608551B2/en
Publication of JPS53112620A publication Critical patent/JPS53112620A/en
Publication of JPS608551B2 publication Critical patent/JPS608551B2/en
Expired legal-status Critical Current

Links

Description

【発明の詳細な説明】 本発明は円筒磁区を利用する磁気記憶素子に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic memory element that utilizes cylindrical magnetic domains.

ガーネットのような膜面に垂直な方向に磁化容易軸を有
する磁性膜に適当な大きさの均一バイアス磁場を加える
と磁性膜内に周辺部と磁化の方向が逆の単一磁壁よりな
る円筒磁区が出来ることが知られている。
When a uniform bias magnetic field of an appropriate magnitude is applied to a magnetic film such as garnet, which has an axis of easy magnetization in the direction perpendicular to the film surface, a cylindrical magnetic domain consisting of a single domain wall whose magnetization direction is opposite to that of the periphery is created in the magnetic film. It is known that it can be done.

この円筒磁区に磁場勾配を与えると円筒磁区はその磁場
勾配にそって移動する。この性質を用いることによって
磁気記憶装置を実現することが可能である。円筒磁区を
移動させる方法としては磁性膜の上にT文字、1文字の
ような欧磁性薄膜パターンを配列し、磁性膜の面内方向
に回転磁場を加える方法がもっともよく用いられている
When a magnetic field gradient is applied to this cylindrical magnetic domain, the cylindrical magnetic domain moves along the magnetic field gradient. By using this property, it is possible to realize a magnetic storage device. The most commonly used method for moving the cylindrical magnetic domain is to arrange European magnetic thin film patterns such as the letters T and 1 on a magnetic film and apply a rotating magnetic field in the in-plane direction of the magnetic film.

磁気記憶装置に用いられる円筒滋区素子を実現するため
には円筒磁区の単純な移動の他に円筒滋区の発生、検出
、消去を行なう手段が必要である。
In order to realize a cylindrical magnetic domain element used in a magnetic storage device, a means for generating, detecting, and erasing the cylindrical magnetic domain is required in addition to the simple movement of the cylindrical magnetic domain.

さらに、円筒磁区素子ではメジャー・ループとマイナー
・ループと呼ばれる2種類の転送路を設けアクセス時間
を短縮する方法が一般に使用されている。
Furthermore, in cylindrical magnetic domain elements, a method is generally used in which two types of transfer paths, called major loops and minor loops, are provided to shorten the access time.

この方法はメジャーノマィナ一方式(M/m方式)と称
されている。M/m方式の円筒滋区素子ではメジャール
ープとマイナーループの間に円筒滋区の授受を行なうト
ランスフア・ゲートあるいは円筒滋区の分割を行なうリ
プリケータ(replicator)が必要である。リ
プリケータとしては例えばアイ・イー・イー・イー・ト
ランザクシヨンズ・オン・マグネテイツクス(mEET
ransactionsonMa靴etics)第MA
G−9巻477ページ(1973年)のFig−8に例
示されている。しかし乍ら上記文献におけるリプリケー
タはリプリケータ部における円筒磁区の進行方向が互い
に逆方向である。
This method is called a major-minor one-way method (M/m method). In the M/m type cylindrical element, a transfer gate for transferring and receiving the cylindrical area between the major loop and the minor loop or a replicator for dividing the cylindrical area is required. An example of a replicator is IE Transactions on Magnetics (mEET).
ranactionsonMa shoes etics) No. MA
This is illustrated in Fig-8 of Volume G-9, page 477 (1973). However, in the replicator in the above-mentioned document, the cylindrical magnetic domains in the replicator portion travel in opposite directions.

このため、この部分での円筒磁区の相互作用が増加する
ため円筒滋区の転送マージンが低下する。又、このリプ
リケータは、円筒磁区を導体ループで引伸し、この引伸
された円筒磁区が前記導体ループと交叉してから、円筒
磁区切断のための電流を流す必要がある。ところが円筒
磁区が導体ループと交叉するまでの期間が長いために、
バイアス磁界が高くなると引伸された円橋磁区が、縮ん
でしまい、円筒磁区を分割することができなくなり、動
作マージンが低下する欠点がある。本発明の目的は従来
知られているリブリケータと形式が異なりかつ、十分な
動作マージンを有するリプリケータを提供することにあ
る。
Therefore, the interaction between the cylindrical magnetic domains increases in this part, and the transfer margin of the cylindrical magnetic domains decreases. Further, in this replicator, it is necessary to stretch the cylindrical magnetic domain with a conductor loop, and after the stretched cylindrical magnetic domain intersects the conductor loop, a current for cutting the cylindrical magnetic domain must be applied. However, because it takes a long time for the cylindrical magnetic domain to intersect with the conductor loop,
When the bias magnetic field becomes high, the elongated cylindrical magnetic domain contracts, making it impossible to divide the cylindrical magnetic domain, resulting in a reduction in operating margin. An object of the present invention is to provide a replicator which is different in type from conventionally known replicators and has a sufficient operating margin.

以下実施例を用いて詳細に説明する。This will be explained in detail below using examples.

第1図は本発明の一実施例のリプリケータ部を示してい
る。
FIG. 1 shows a replicator section according to an embodiment of the present invention.

第1の円筒磁区転送路11と第2の円筒磁区転送路12
が接近したりプリケータ中心部13の付近には円筒磁区
引伸用の第1の導体14と円筒滋区切断用の第2の導体
15が配置されている。
First cylindrical domain transfer path 11 and second cylindrical domain transfer path 12
A first conductor 14 for enlarging the cylindrical magnetic domain and a second conductor 15 for cutting the cylindrical magnetic domain are arranged near the applicator center 13.

ここでは第1の導体と第2の導体が絶縁層を介して別の
層で形成されていることが本質的であり、従来の公知例
との相違点でもある。通常は製造プロセスの工数をなる
べく少〈することが要求されるので、例えば第1の導体
を第1の薄膜層で形成すればL第2の導体は円筒磁区転
送路を形成するものと同じ第2の薄膜層で形成するのが
よい。
Here, it is essential that the first conductor and the second conductor are formed of different layers with an insulating layer interposed therebetween, which is also a difference from conventional known examples. Normally, it is required to reduce the number of steps in the manufacturing process as much as possible, so for example, if the first conductor is formed of the first thin film layer, the second conductor is formed of the same layer as that forming the cylindrical domain transfer path. It is preferable to form it with two thin film layers.

円筒磁区転送路を形成する薄膜層は通常パーマロィ膜等
の磁性膜層が用いられているが電気伝導度を増すために
金、アルミ、銅等の膜が磁性薄膜に重ね合わされていて
もよい。第2の導体を第1の薄膜層で形成し、第1の導
体を第2の薄膜層で形成してもよいことはもちろんであ
る。さらに第1図による実施例では第1の導体!4と第
2の導体15はリプリケータ中心部13付近において交
叉するように配置されている。ここで第1の導体14と
第2の導体15は電気的に短絡しないよう絶縁層を介し
て配置されている。第1又は第2の円筒磁区転送路】6
717のいずれかから入ってきた円筒磁区が円筒磁区引
伸用の第1の導体ループ部14に到達したとき、第1の
導体ループに電流を流すと円筒磁区が第1と第2の円筒
滋区転送路の両方にまたがるように引伸ばすことができ
る。一般に円筒滋区を保持するためのバイアス磁場が強
くなると円筒磁区が伸びにくくなるため第1の導体ルー
プの電流を切ってしまうと円筒磁区が再び縮んで第1又
は第2の円筒磁区転送路の一方にしか存在しなくなる傾
向にある。従来報告されているリプリケータにおいては
いずれも一旦のびた円筒磁区が円筒滋区引伸用の電流を
切っても縮まないバイアス範囲でのみ動作するように設
計されている。一方本発明によるリプリケー外こおいて
は円筒滋区引伸用の第1の導体と円筒磁区切断用の第2
の導体が交叉するように配置されているので円筒磁区引
伸用の電流を流している状態で円筒滋区切断用の電流を
同時に流すことができる。したがって本発明のリプリケ
ー外こよれば従来のリプリケータより高いバイアス磁場
の所まで動作させることが出来、結局動作マージンが広
くなる。
The thin film layer forming the cylindrical magnetic domain transfer path is usually a magnetic film layer such as a permalloy film, but a film of gold, aluminum, copper, etc. may be superimposed on the magnetic thin film to increase electrical conductivity. Of course, the second conductor may be formed from the first thin film layer, and the first conductor may be formed from the second thin film layer. Furthermore, in the embodiment according to FIG. 1, the first conductor! 4 and the second conductor 15 are arranged so as to intersect near the replicator central portion 13. Here, the first conductor 14 and the second conductor 15 are arranged with an insulating layer interposed therebetween so as not to be electrically short-circuited. First or second cylindrical domain transfer path】6
When the cylindrical magnetic domain entering from either of the cylindrical magnetic domains 717 reaches the first conductor loop section 14 for enlarging the cylindrical magnetic domain, when a current is passed through the first conductor loop, the cylindrical magnetic domain is divided into the first and second cylindrical magnetic domains. It can be stretched to span both transfer paths. Generally, when the bias magnetic field for holding the cylindrical magnetic domain becomes strong, the cylindrical magnetic domain becomes difficult to expand, so when the current in the first conductor loop is cut off, the cylindrical magnetic domain shrinks again and the cylindrical magnetic domain transfers into the first or second cylindrical magnetic domain transfer path. It tends to exist only on one side. All of the replicators that have been reported so far are designed to operate only within a bias range in which the once expanded cylindrical magnetic domain does not contract even when the current for enlarging the cylindrical area is turned off. On the other hand, in the replicator according to the present invention, a first conductor for enlarging the cylindrical magnetic domain and a second conductor for cutting the cylindrical magnetic domain are used.
Since the conductors are arranged so as to intersect, it is possible to simultaneously flow a current for cutting the cylindrical magnetic domain while a current for expanding the cylindrical magnetic domain is flowing. Therefore, the replicator of the present invention can be operated up to a higher bias magnetic field than the conventional replicator, resulting in a wider operating margin.

第1図の実施例においてはリプリケータ中心部付近の第
1および第2の円筒磁区転送路は山形(シェブロン)パ
ターンをそれぞれ3段重ねたものから構成されているが
この段数はこれ以外でもよいことはもちろんのこと〜Y
形、半円形等他の形のパターンから構成されていてもよ
い。
In the embodiment shown in FIG. 1, the first and second cylindrical domain transfer paths near the center of the replicator each consist of three layers of chevron patterns, but the number of layers may be other than this. Of course~Y
It may also be composed of patterns of other shapes, such as a semicircular shape or a semicircular shape.

図において導体パターン14,15は直線状であるよう
に示されているが曲がっていてもよいことはもちろんで
あり、太さも一様である必要はない。
Although the conductor patterns 14 and 15 are shown to be straight in the figure, they may of course be curved, and the thickness does not need to be uniform.

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

図は本発明の一実施例におけるリブリケータ部を示す平
面図である。 11は第1の円筒磁区転送路、12は第2の円筒磁区転
送路、13はリプリケータ中心部、14は円筒磁区引伸
用導体、15は円筒磁区切断用導体「 16,17は円
筒磁区の進行方向である。
The figure is a plan view showing a ribricator section in an embodiment of the present invention. 11 is a first cylindrical domain transfer path, 12 is a second cylindrical domain transfer path, 13 is the center of the replicator, 14 is a cylindrical domain expansion conductor, 15 is a cylindrical domain cutting conductor; It is the direction.

Claims (1)

【特許請求の範囲】[Claims] 1 円筒磁区を保有しうる磁性膜とその磁性膜中の円筒
磁区を安定に存在させるための磁気的手段および円筒磁
区を移動させるための磁気的手段を有する磁気記憶装置
において、第1の円筒磁区転送路と第2の円筒磁区転送
路と、これら2種の転送路の接近部に円筒磁区引伸用の
第1の導体と円筒磁区切断用の第2の導体とを別の層に
形成しかつ交叉するように配置したリプリケータとを備
えてなることを特徴とする円筒磁区素子。
1. In a magnetic storage device having a magnetic film capable of holding a cylindrical magnetic domain, a magnetic means for stably existing the cylindrical magnetic domain in the magnetic film, and a magnetic means for moving the cylindrical magnetic domain, a first cylindrical magnetic domain A transfer path, a second cylindrical magnetic domain transfer path, a first conductor for expanding the cylindrical magnetic domain, and a second conductor for cutting the cylindrical magnetic domain are formed in separate layers at a close portion of these two types of transfer paths, and A cylindrical magnetic domain element comprising: replicators arranged to intersect with each other.
JP2846277A 1977-03-14 1977-03-14 Cylindrical domain element Expired JPS608551B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2846277A JPS608551B2 (en) 1977-03-14 1977-03-14 Cylindrical domain element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2846277A JPS608551B2 (en) 1977-03-14 1977-03-14 Cylindrical domain element

Publications (2)

Publication Number Publication Date
JPS53112620A JPS53112620A (en) 1978-10-02
JPS608551B2 true JPS608551B2 (en) 1985-03-04

Family

ID=12249315

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2846277A Expired JPS608551B2 (en) 1977-03-14 1977-03-14 Cylindrical domain element

Country Status (1)

Country Link
JP (1) JPS608551B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62112325U (en) * 1985-12-31 1987-07-17
JPH0536641B2 (en) * 1985-08-14 1993-05-31 Toyota Jido Shotsuki Seisakusho Kk

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0536641B2 (en) * 1985-08-14 1993-05-31 Toyota Jido Shotsuki Seisakusho Kk
JPS62112325U (en) * 1985-12-31 1987-07-17

Also Published As

Publication number Publication date
JPS53112620A (en) 1978-10-02

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