JPS58111179A - Magnetic bubble memory device - Google Patents

Magnetic bubble memory device

Info

Publication number
JPS58111179A
JPS58111179A JP56208781A JP20878181A JPS58111179A JP S58111179 A JPS58111179 A JP S58111179A JP 56208781 A JP56208781 A JP 56208781A JP 20878181 A JP20878181 A JP 20878181A JP S58111179 A JPS58111179 A JP S58111179A
Authority
JP
Japan
Prior art keywords
bubble
magnetic
film
hole
magnetic film
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
JP56208781A
Other languages
Japanese (ja)
Inventor
Yasuyoshi Suzuki
鈴木 康好
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
NEC Corp
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 NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP56208781A priority Critical patent/JPS58111179A/en
Publication of JPS58111179A publication Critical patent/JPS58111179A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11CSTATIC STORES
    • G11C19/00Digital stores in which the information is moved stepwise, e.g. shift registers
    • G11C19/02Digital stores in which the information is moved stepwise, e.g. shift registers using magnetic elements
    • G11C19/08Digital stores in which the information is moved stepwise, e.g. shift registers using magnetic elements using thin films in plane structure
    • G11C19/0808Digital stores in which the information is moved stepwise, e.g. shift registers using magnetic elements using thin films in plane structure using magnetic domain propagation

Abstract

PURPOSE:To hold a bubble at a prescribed stop position even when an electric power supply is disconnected by forming a nonmagnetic intermediate film and the 2nd magnetic film between the 1st magnetic film and an insulating film and drilling a hole on the 2nd magnetic film at the same position as the bubble stop position. CONSTITUTION:A hard bubble film 2 is formed between a base plate 1 and the 1st magnetic film 3. A magnetic material used for the 2nd magnetic film 5 has a vertical magnetizable axis. An intermediate film 4 between the 1st magnetic film 3 and the 2nd magnetic film 5 is made of a nonmagnetic material. A hole C is drilled on the 2nd magnetic film 5. When there is no external rotating magnetic field, a bubble B is held at a position S, a permalloy pattern P is slightly magnetized by the hole C and also a local magnetic field generated due to said magnetization applies force in the direction to pull the bubble B to the position S. The position of the hole C is fixed on a position where the bubble is stopped at the time of no rotating magnetic field.

Description

【発明の詳細な説明】 本発明は磁気バブルメモリ装置に係り、特にスタート、
ストップ動作または電源停止時において磁気バブル(以
下バブルと呼ぶ)を所定の位置に保持するためO1!素
を持つバブルメモリチップに関する4のである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic bubble memory device, and particularly to a start,
O1! to hold the magnetic bubble (hereinafter referred to as bubble) in a predetermined position during stop operation or power outage! 4 concerning bubble memory chips with elements.

パズルメモリ装置において、情報の担体としてのバブル
を転送する一手段として、バブルメモリチク10面に平
行な回転磁界を印加して、骸パプルメそりチップの磁性
膜上に形成されたパー!ロイ転送パターンを磁化して局
部磁界を発生させ、該局部磁界により所定のパー!四イ
転送路上をバブルを転送させる方法は公知であり、従来
、実用化されて−るパプルメ篭り装置はすべてこの方式
%式% 上述のようなパズル転送方法において、転送路上で任意
にバブルなスタートさせたりストップさせ九りするスタ
ートストップ動作は、バブルメモリの重要な機能であL
lた電源等の切断によって回転磁界のない場合に4バブ
ルを所定の位置に保持し、バブルメモリの情報を破壊さ
せないことが重要である。      − 上述の機能を達成すゐ方法として、従来よりバブルメモ
リチップの面に平行に直流磁界を印加する方法があp1
実際のバブルメモリ装置1には主と1で2種類の方式が
実用化されている。この211[類の方式はともにバイ
アス磁界発生用の永久磁石による磁界を利用するもので
ある。1つはバイア5ス磁界発生用磁石に対してバブル
メモリチップ搭載基板を必要な角度だけ傾けるものであ
り、もう1つはバイアス磁界発生用磁石に接着し九整磁
板にテーパをつけて、バブルメモリチップの面に対して
テーパの角度分だけ傾−九直流バイアス磁界を印加する
方式である。
In the puzzle memory device, as a means of transferring bubbles as information carriers, a rotating magnetic field parallel to the 10 sides of the bubble memory chip is applied to transfer the bubbles formed on the magnetic film of the puzzle memory chip. The Roy transfer pattern is magnetized to generate a local magnetic field, and the local magnetic field produces a predetermined par! The method of transferring bubbles on the transfer path is well known, and all paplume cage devices that have been put to practical use use this method. The start-stop action of starting, stopping, and turning is an important function of bubble memory.
It is important to hold the four bubbles in a predetermined position in the absence of a rotating magnetic field by cutting off the power source, etc., so as not to destroy the information in the bubble memory. - As a method to achieve the above function, there is a conventional method of applying a DC magnetic field parallel to the surface of the bubble memory chip.
In the actual bubble memory device 1, two types of systems are put into practical use: main and 1. Both of these 211-type systems utilize a magnetic field generated by a permanent magnet for generating a bias magnetic field. One is to tilt the bubble memory chip mounting board by the required angle with respect to the bias magnetic field generating magnet, and the other is to attach it to the bias magnetic field generating magnet and taper the nine magnetic plate. This method applies a tilted DC bias magnetic field equal to the angle of the taper to the surface of the bubble memory chip.

上記の方法により、剛板磁界がない場合にも、パーマロ
イ転送パターンを磁化させておく仁とができ、これによ
りバブルを所定の位tK保持しておくことができる。
By the above method, it is possible to keep the permalloy transfer pattern magnetized even in the absence of a rigid plate magnetic field, thereby making it possible to maintain the bubble for a predetermined amount tK.

しかし上述の方法ではバブルメモリ装置を組立てる際、
バブルメモリチップを搭載した基板とバイアス磁石また
はテーパのついた整磁板に対して一定の角度を保つ必要
があるが、バブルメモリ装置を倉皇する場合、すべての
バブルメモリ装置に対して全く同じ角度に設定すること
は困難であり、必然的に各バブルメモリ装置間に特性の
はらつきが存在する。
However, in the above method, when assembling the bubble memory device,
It is necessary to maintain a certain angle between the board on which the bubble memory chip is mounted and the bias magnet or tapered magnetism plate, but when installing bubble memory devices, the angle must be exactly the same for all bubble memory devices. It is difficult to set this, and inevitably there are variations in characteristics between each bubble memory device.

本発明は上述のようなバブルメモリチップに面内磁界を
かけてバブルを所定の位置に保持しておく機能と同様な
機能を持つ要素をバブルメモリチップ内に作成し、常に
同一の情報保持能力をもつバブルメモリ装置を提供する
ものである。
The present invention creates an element in a bubble memory chip that has a function similar to the above-mentioned function of applying an in-plane magnetic field to a bubble memory chip to hold the bubble in a predetermined position, thereby maintaining the same information retention ability at all times. The present invention provides a bubble memory device having the following features.

本発明のバブルメモリ装置はパブ、ル謀体としての第−
磁性膜と絶縁膜との関に新九に非磁性の中間膜と前記第
一磁性膜と同様に膜面Kfi直な方向Kil化容易軸を
持つ第二磁性膜を設けゐと共に前配第二磁性腺において
、バブル転送の大めの回転磁界がないときのバブルの停
止位置と同じ位置にイオンミリング勢によって任意形状
の穴をあけるととくより、バブルを所定の停止位置に保
持することを特徴とするものである。
The bubble memory device of the present invention can be used as a bubble memory device as a bubble memory device.
Between the magnetic film and the insulating film, a non-magnetic intermediate film and a second magnetic film having an easy-to-Kil axis in the direction perpendicular to the film surface Kfi, like the first magnetic film, are provided. In the magnetic gland, the bubble is held at a predetermined stopping position by drilling a hole of an arbitrary shape using ion milling force at the same position where the bubble stops when there is no large rotating magnetic field for bubble transfer. That is.

第1図は本発明に係るパプルメ篭りチップの断面図であ
る。現在実用化されているバブルメモリチップで紘ハー
ドバブル抑制のため、バブル媒体の第一磁性113にイ
オン打ち込み層を形成するかまたはハードバブル抑制膜
を作成する。本発明に関しては、バブルメモリチップの
設計上および特性上の利点を考慮すればハードバブル抑
制膜2をGGG(カドリニウム゛・Wリウム・ガーネッ
ト)基板lと第一磁性1li13との間に作成すること
が望ましい。第二磁性IK5に用いられる磁性材料は族
1tlKIl直な磁化容易軸を持つものであれば何であ
ってもよい。また第一磁性膜3と第二磁性aSSとの間
の中間1114についてその材質は非磁性であれば何で
もよいが、バブルが安定に存在できれば磁性膜であって
も中間膜として使用可能である。たとえばハードバブル
抑制膜を中間膜とすることも可能である。第二磁性膜6
0穴Cは任意の形状でよいが設計上は円筒形が設計計算
しやすい。円筒形の穴CとバブルBは相互作用して互い
に引き合う。ここで第−磁性膜3の磁化をMl 、第二
磁性膜5の磁化をM、とすればバブルBと穴Cは尋価的
に第2図のように円筒形の磁石と考えることができ、バ
ブルBK相等する磁石の゛磁化は2M、穴CK相勢する
磁石の磁l″はM、として相互作用力を計算する仁とが
できる。第2図のように座標系をとるとバブルのy方向
の移動は不可能であるからバブルBK働゛く力11x成
分のみを青臭ればよく、これをFxとすれば、Fxd理
論針算によりて求める仁とができる。バブルBの中心と
穴Cの中心との距離なXとしてFxとXの定性的な関係
をグラフに表わせば第3図のようになる。Fxは引き合
う方向を正とすれば、X■0でFx■0.X〉0でFx
>Oであり、ある値Xpで最大値Fmaxをとゐ。
FIG. 1 is a sectional view of a paplume kogori chip according to the present invention. In order to suppress hard bubbles in bubble memory chips currently in practical use, an ion implantation layer is formed on the first magnetic layer 113 of the bubble medium or a hard bubble suppression film is formed. Regarding the present invention, in consideration of the design and characteristic advantages of the bubble memory chip, the hard bubble suppression film 2 may be created between the GGG (cadrinium W lium garnet) substrate l and the first magnetic layer 1li13. is desirable. The magnetic material used for the second magnetic IK5 may be any material as long as it has an easy axis of magnetization that is perpendicular to the group 1tlKI1. Further, the intermediate 1114 between the first magnetic film 3 and the second magnetic aSS may be made of any material as long as it is non-magnetic, but even a magnetic film can be used as the intermediate film as long as bubbles can stably exist. For example, it is also possible to use the hard bubble suppression film as an intermediate film. Second magnetic film 6
The zero hole C may have any shape, but a cylindrical shape is easier to design and calculate. The cylindrical hole C and the bubble B interact and attract each other. Here, if the magnetization of the first magnetic film 3 is Ml and the magnetization of the second magnetic film 5 is M, then bubble B and hole C can be thought of as cylindrical magnets as shown in Figure 2. , the interaction force can be calculated by assuming that the magnetization of bubble BK is 2M, and the magnetization of hole CK is M.If we take the coordinate system as shown in Figure 2, we can calculate the interaction force of the bubble. Since movement in the y direction is impossible, only the 11x component of the force acting on the bubble BK is required.If this is Fx, the distance obtained by Fxd theoretical calculation can be obtained.The center of the bubble B and the hole If we represent the qualitative relationship between Fx and X on a graph, where X is the distance from the center of C, it will be as shown in Figure 3.If Fx is positive in the direction of attraction, then X■0 and Fx■0. Fx at 0
>O, and reaches the maximum value Fmax at a certain value Xp.

次にバブルBの穴CおよびパーマロイパターンPとの相
互作用について説明する。簡単のためにパーマレイパタ
ーンPd棒状とし、穴Cは第4図めようにパーマロイパ
ターンPの一端の下にあるものとする。外部回転磁界が
ないときバブルBは位置8に保持され、また大OKよっ
てパーマロイパターンPはわずかKil化され、これに
よる局部磁界もバブル、Bを位置8に引きつけておく方
向の力を与える。  一 回転磁界Haを与えると、バブルBはパーマロイパター
ンPの作る局部磁界によりて移動させられる。仁のとき
パーマ四イパI−ンPKよるバブルBに働く力のX成分
FXIPは六〇によるパブルBK働く力のX成分Fxl
Cよりも常に大きくなるようにバブルメモリチップは設
計されなくてはならない。またFXICおよびFzlC
が極大となるときのバブルBと穴Cとの距離XPの値も
種々のパーマロイ転送パターンの形状に対して最適な設
計が必要である。
Next, the interaction of the bubble B with the hole C and the permalloy pattern P will be explained. For simplicity, it is assumed that the permalloy pattern Pd is rod-shaped, and the hole C is located below one end of the permalloy pattern P as shown in FIG. When there is no external rotating magnetic field, the bubble B is held at position 8, and the permalloy pattern P is slightly oxidized due to the large OK, and the resulting local magnetic field also provides a force in the direction of attracting the bubble B to position 8. When the magnetic field Ha is applied once, the bubble B is moved by the local magnetic field created by the permalloy pattern P. At the time of Jin, the X component of the force acting on bubble B due to PK is the X component FXIP of the force acting on bubble BK due to 60 FXl
Bubble memory chips must be designed so that they are always larger than C. Also FXIC and FzlC
The value of the distance XP between the bubble B and the hole C when becomes maximum also needs to be optimally designed for various shapes of permalloy transfer patterns.

本発明の実施例について説明する。Examples of the present invention will be described.

バブルメモリチップの記憶領域において、第1図に示す
ような躾構成とした。膜の材質および特性はハードバブ
ル抑制膜2がYIG(III厚300人)、第−磁性膜
3が(YLu8mCu ) @ (FeGe ) 60
11(膜厚1.65 fim * 4 gMm −46
0CG) )、中間膜4が810.展(膜厚2000A
) 、第二磁性aSがTb−re展(a厚3000A、
保磁力650j be ) )である。パーマロイ転送
パターンは非対称シュプロン形、バブル径は1.7〔μ
m〕とし、第二磁性膜の穴の径は2【μm〕としてその
位置は第6図に示す位置としえ。
The storage area of the bubble memory chip was configured as shown in FIG. Regarding the material and characteristics of the film, the hard bubble suppressing film 2 is YIG (III thickness 300), and the third magnetic film 3 is (YLu8mCu) @ (FeGe) 60
11 (film thickness 1.65 fim * 4 gMm -46
0CG) ), the intermediate film 4 is 810. Expansion (film thickness 2000A
), the second magnetic aS has Tb-re expansion (a thickness 3000A,
The coercive force is 650j be ). The permalloy transfer pattern is asymmetric spron-shaped, and the bubble diameter is 1.7 [μ
m], the diameter of the hole in the second magnetic film is 2 [μm], and its position is as shown in FIG.

本発明を実施するための設計において、最も重畳なこと
は第二磁性膜にあけゐ穴Cの位置でFLとれは従来の面
内磁界を有するバブルメモリ装置において、回転磁界の
ない場合にバブルが停止している、位置がよい、一般に
バブルメモリチップの記憶領域のパーマロイ転送パター
7社ループ状であるため、バブルの転送方向および面内
磁界の方向にようてバブルの停止位置が異なる。すなわ
ち第6図、第7図のような場合が考えられる。第6図、
第7図において破線の丸Cが第二磁性II5の穴を表わ
している。穴の大きさはバブル径、第一磁性膜の磁化お
よび濃厚、中間膜O展厚、第二磁性展の磁化および膜厚
、パーマpイパターンの形状等によりて決まる。パーマ
pイパターンとバブルとの距離状できるだけ短いはうが
望ましいので中間膜、第二磁性展の膜厚は第一磁性IN
K比較してできるだけ薄くする必要がある。したがって
バブルと穴との相互作用力を必要なだけ大きくするには
第二磁性膜の磁化を大きくするかまたは穴の大きさをバ
ブル径に比べて大きめに設計すればよい。
In the design for carrying out the present invention, the most important point is the position of the hole C formed in the second magnetic film. Generally, the storage area of the bubble memory chip is in a loop shape, so the bubble stopping position differs depending on the bubble transfer direction and the direction of the in-plane magnetic field. That is, cases such as those shown in FIGS. 6 and 7 can be considered. Figure 6,
In FIG. 7, the broken line circle C represents the hole of the second magnetic II5. The size of the hole is determined by the bubble diameter, the magnetization and concentration of the first magnetic film, the thickness of the intermediate film O, the magnetization and film thickness of the second magnetic film, the shape of the permanent P pattern, etc. Since it is desirable that the distance between the permanent p-pattern and the bubble be as short as possible, the thickness of the intermediate film and the second magnetic layer should be the same as the first magnetic layer.
It is necessary to make it as thin as possible compared to K. Therefore, in order to increase the interaction force between the bubble and the hole as much as necessary, the magnetization of the second magnetic film may be increased or the size of the hole may be designed to be larger than the bubble diameter.

一般的に第二磁性膜の膜厚が薄いとバブルによゐ局部磁
界によって骸第二磁性属の磁化が反転することがあるた
め、鋏第二磁性膜の材料の材質としてFi、保磁力の大
きな磁性材料である必要がある。
In general, if the second magnetic film is thin, the magnetization of the second magnetic layer may be reversed by the local magnetic field caused by bubbles. It needs to be a large magnetic material.

腺の構成方法としては D)、ハードバブル抑制御KYIG(イツトリウム・ア
イアン書ガーネット)、第−磁性膜および第二磁性膜に
磁性ガーネット、中間展をGGGとする、すべてガーネ
ット系の材料を用いる方法。
The method for constructing the gland is D), a method using all garnet-based materials, using KYIG (yttrium iron garnet) for hard bubble suppression, magnetic garnet for the first magnetic film and second magnetic film, and GGG for the intermediate layer. .

(2)、 (t)において第二磁性膜をアモルファス磁
性膜とする方法。
(2) A method in which the second magnetic film is an amorphous magnetic film in (t).

(3)% (1)において中間jllK8101膜また
aAjsOs膜等の絶縁層を用い、第二磁性膜としてア
モルファス磁性膜を作成する方法。
(3)% A method of forming an amorphous magnetic film as the second magnetic film using an insulating layer such as an intermediate jllK8101 film or an aAjsOs film in (1).

(4)%(1) 、 (2)において第−ia性膜にバ
ブルが存在する範1iにおいて、バブルがで自ないよう
に設計された磁性ガーネットを中間膜とする方法。
(4) In the range 1i in which bubbles are present in the -ia film in %(1) and (2), a method in which a magnetic garnet designed to prevent bubbles from forming is used as the intermediate film.

等があけられゐ。etc. are opened.

上述し九実論例の動作マージン特性祉従来の面内磁界を
有するパプルメそり装置と同様なものが得られた。tた
第1wJにおいてハードバブル抑制膜2をGGG基板l
と第一磁性膜3の間としたがハードバブル抑制膜を第一
磁性@3と中間114との間に作成し九パプルメそりチ
ップ、および第一磁性11にイオン注入することによる
バードバブル抑制方法を用いたパプルメ噛りチップにお
いても同様な効果がある。
The operating margin characteristics of the nine practical examples described above were similar to those of the conventional Papulume sled device having an in-plane magnetic field. In the first wJ, the hard bubble suppression film 2 is attached to the GGG substrate l.
A method of suppressing bird bubbles by creating a hard bubble suppressing film between the first magnetic layer 3 and the intermediate layer 114 and implanting ions into the nine-puplume sled chip and the first magnetic layer 11. A similar effect can be obtained with paplume chewing chips using .

本発明は既存のパーマロイ転送パターンを用い大磁界駆
動型のバブルメモリ装置に関するものであるが、197
9都、ベル・システム・テクニカル・ジャーナル(Be
1l 5yst@m technlcalJourna
l )第58巻第1453頁以降においてはじめて発表
された二層導体電流駆動型のバブメモリ装置にはきわめ
て有効である。カぜならば、二層導体電流駆動型のバブ
ルメモリ装置社パーマウイのような磁性体の転送パター
ンを用いないことを特徴としているため面内磁界をかけ
てもむだであり、電源停止時にバブルを所定の位置に保
持しておくことが困難であるからである・
The present invention relates to a large magnetic field driven bubble memory device using an existing Permalloy transfer pattern.
9 cities, Bell System Technical Journal (Be
1l 5yst@m technlcalJourna
l) It is extremely effective for the two-layer conductor current-driven bubble memory device that was first announced in Vol. 58, p. 1453 onwards. If it is cold, it is pointless to apply an in-plane magnetic field because it does not use a magnetic material transfer pattern like the two-layer conductor current-driven bubble memory device company Permaui, and it is useless to apply an in-plane magnetic field, and the bubble will be removed when the power is turned off. This is because it is difficult to keep it in place.

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

第1図は本発明に関するバブルメモリチップの断面図、
第2a!!l、第3図、第4図および第5図は本発明の
原理の152明WJ、第6図、第7図は本発明の実施例
である。 図において、l・・・・・・GGG基板、2・・・・・
・ハードバブル抑制展、i・・・・・・バブル媒体とし
ての第−磁性層、4・・・・・・中間層、5・・・・・
・バブル保持要素を有する第二磁性展、6・・・・・・
絶縁層である。 第1図 第2図 第3図 第4図 帥5図
FIG. 1 is a cross-sectional view of a bubble memory chip according to the present invention;
2nd a! ! 1, FIGS. 3, 4 and 5 illustrate the principles of the present invention, and FIGS. 6 and 7 illustrate embodiments of the present invention. In the figure, l...GGG board, 2...
・Hard bubble suppression exhibition, i... Third magnetic layer as bubble medium, 4... Intermediate layer, 5...
・Second magnetic field with bubble retention element, 6...
It is an insulating layer. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5

Claims (1)

【特許請求の範囲】[Claims] 磁気バブル媒体としての第−磁性層と絶縁膜との間に、
中間膜と第二磁性膜とを設けると共に、前記第二磁性J
IIにおいて磁気バブル転送のための回転磁界がないと
きの磁気バブルの停止位置に、任意形状の穴をあけるこ
とを1#黴とする磁気パブルメそり装置。
Between the first magnetic layer as a magnetic bubble medium and the insulating film,
In addition to providing an intermediate film and a second magnetic film, the second magnetic film J
In II, a magnetic bubble meshing device uses a 1# mold to make a hole of an arbitrary shape at the stop position of a magnetic bubble when there is no rotating magnetic field for magnetic bubble transfer.
JP56208781A 1981-12-23 1981-12-23 Magnetic bubble memory device Pending JPS58111179A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56208781A JPS58111179A (en) 1981-12-23 1981-12-23 Magnetic bubble memory device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56208781A JPS58111179A (en) 1981-12-23 1981-12-23 Magnetic bubble memory device

Publications (1)

Publication Number Publication Date
JPS58111179A true JPS58111179A (en) 1983-07-02

Family

ID=16561989

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56208781A Pending JPS58111179A (en) 1981-12-23 1981-12-23 Magnetic bubble memory device

Country Status (1)

Country Link
JP (1) JPS58111179A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2677482A1 (en) * 1991-06-10 1992-12-11 Sp K Tekh Device for stashing information for a magnetic-bubble memory

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2677482A1 (en) * 1991-06-10 1992-12-11 Sp K Tekh Device for stashing information for a magnetic-bubble memory

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