JPS5891582A - Magnetic bubble transfer pattern - Google Patents
Magnetic bubble transfer patternInfo
- Publication number
- JPS5891582A JPS5891582A JP56188808A JP18880881A JPS5891582A JP S5891582 A JPS5891582 A JP S5891582A JP 56188808 A JP56188808 A JP 56188808A JP 18880881 A JP18880881 A JP 18880881A JP S5891582 A JPS5891582 A JP S5891582A
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- pattern
- electric conductor
- magnetic
- bubble
- 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.)
- Granted
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11C—STATIC STORES
- G11C19/00—Digital stores in which the information is moved stepwise, e.g. shift registers
- G11C19/02—Digital stores in which the information is moved stepwise, e.g. shift registers using magnetic elements
- G11C19/08—Digital stores in which the information is moved stepwise, e.g. shift registers using magnetic elements using thin films in plane structure
- G11C19/0866—Detecting magnetic domains
Abstract
Description
【発明の詳細な説明】
本発明は電流駆動型磁気バブル転送パタンに関するもの
である。史に詳しく述べれば、磁気バブルをその進行方
向とほぼ垂直に引き伸ばすことの出来る胤流駆wJ型両
気バブル私送バタンに関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a current driven magnetic bubble transfer pattern. More specifically, it relates to the Tane-ryu-kun WJ-type double-air bubble transporting slam, which can stretch a magnetic bubble almost perpendicular to its direction of travel.
一般に面内回転磁場によって磁気バブルを転送するフィ
ールドアクセス型磁気バブル素子では、バブル両区を情
報として読み出すデータ読み出し速度は面内回転磁場の
周波数によって定まり、尚々l0UK〜300にビット
/秒−こしかすきない。この様なデータ読み田しfi麓
で体、大dtの情報の処理には適さない。In general, in a field access type magnetic bubble device that transfers magnetic bubbles using an in-plane rotating magnetic field, the data readout speed at which both bubble sections are read out as information is determined by the frequency of the in-plane rotating magnetic field, and ranges from 10 to 300 bits/sec. I don't like it. This type of data reading is not suitable for processing large dt information.
磁気バブルを高速で転送するには、゛−流駆動方式に依
ればaJ能となる。磁気バブルの′電流駆動方法は、単
一の蛇行状導体バタンと、バイアス川のパーマロイド、
トの如き磁性パターンを有するバブル転送路を用いる単
層導体法、二1−の導体lこ設けた八明きバタン列を用
いる穴明き二層導体法、蛇行バタンを用いる蛇行二項導
体法、三層の尋犀に設けた穴明バタン列を用いる穴明き
三l−導体法、一層の導体lこ穴パタンを設け、これに
回転嵐tILを印加してバブルを転送する回転1FL流
法がよく知られている。To transfer magnetic bubbles at high speed, it is possible to use the current drive system. The current driving method of the magnetic bubble is a single serpentine conductor button and a bias river permaloid.
A single-layer conductor method using a bubble transfer path with a magnetic pattern such as 1, a perforated two-layer conductor method using a row of eight-bright battens with 21 conductors, and a meandering binomial conductor method using meandering battens. , a perforated three-conductor method using a row of perforated button holes provided in a three-layer conductor, and a rotary 1FL method in which a single-layer conductor perforation pattern is provided and a rotating storm tIL is applied to it to transfer bubbles. The law is well known.
高速で磁気バブルを読み出すためには、上述の両党バフ
ルの尚速転送方法と供に、磁気バブルの高速検出方法が
必要となる。磁気バブルの構出ζこは、パーマロイ薄膜
の磁気抵抗効果を用いるのが近年では一般的である。磁
気a抗効果により磁気バブルを効率よく構出するために
は、長し)ノ櫂−マロイ漣゛涙のストライプを用いて1
、且罎気バブルをそのパーマロイ・ストライプとばば同
じ長さに伸ばすことがν【く行われている。In order to read magnetic bubbles at high speed, a high-speed detection method for magnetic bubbles is required in addition to the above-mentioned high-speed transfer method using both party baffles. In recent years, it has become common to create magnetic bubbles using the magnetoresistive effect of permalloy thin films. In order to efficiently construct magnetic bubbles due to the magnetic anti-resistance effect, it is necessary to
, and extending the air bubble to the same length as its permalloy stripe is often done.
磁気バブルの磁壁移動度は有限であるため、一気バフル
を所定の長さに伸ばすのにある一定の時間が必要となる
。従って磁気バブルの高速転送中に、急激に両紙バブル
を引き伸ばそうとしても不可能であり、効率良い検出が
出来なくなる。このため、特lこ高速検出を行なう場合
は、@気バブルを徐々に引き伸ばす磁気バブルストレツ
ナヤーか必要となる。Since the domain wall mobility of a magnetic bubble is finite, a certain amount of time is required to extend the baffle to a predetermined length at once. Therefore, it is impossible to rapidly stretch both paper bubbles during high-speed transfer of magnetic bubbles, and efficient detection becomes impossible. Therefore, especially when performing high-speed detection, a magnetic bubble stretcher is required to gradually stretch the bubble.
フィールド・アクセス型−気バプル素子では、シェブロ
ン型パーマロイバタンを徐々に積み重ねてユ<一気バブ
ルストレッチャーが実現さnている。しかし乍ら、これ
は、前述の如<m気バフルの高速転送、高速検出には適
していない。電流駆動型両党バブル素子では%罎気バブ
ルストレツナヤートL、T:ハ、ホヘック(A 、 H
、Bobeck ) 号によって1979年のベル・シ
ステム・テクニカルレジャーナル誌第58巻第1453
負〜1540頁で八明き二層導体磁気バブル転送パタン
に接続するものとして発表されているの6で、他の駆動
法に関しては伺ら公知とはなっていない。しかも、前記
文献で示されているl気バブルス゛トレ、チャーは、通
常の一気バブル転送路でのバブルm*iii:流よりも
大きな駆WW流を必要とする欠点を有している。In the field access type air bubble device, a bubble stretcher is realized by gradually stacking chevron type permalloy batons. However, this is not suitable for high-speed transfer and high-speed detection of the air baffle as described above. In the current-driven two-party bubble element, the % air bubble stretsnayat L, T: Ha, Hohek (A, H
, Bobeck) 1979 Bell System Technical Journal Vol. 58 No. 1453
On page 1,540 of this paper, it is announced that the method is connected to a two-layer conductor magnetic bubble transfer pattern, and no other driving methods are known. Moreover, the 1-air bubble stream shown in the above-mentioned literature has the disadvantage that it requires a larger driving WW flow than the bubble m*iii: flow in a normal bubble transfer path.
本発明の目的は、穴明き二層導体磁気バブル駆動方式に
通した、大きな駆動電流を必要としない磁気バブルスト
レッチャー転送路’F[供することにある。更−こ不発
明の今一つの目的は、他の甑流駆勧方式の踪気バブル転
込バタンζこも適用出来るffl気バブルストレッチャ
ー転迷路を提供することにある。The object of the present invention is to provide a magnetic bubble stretcher transfer path 'F which does not require a large drive current, which is passed through a perforated two-layer conductor magnetic bubble drive system. Another object of the present invention is to provide an FFL air bubble stretcher turning maze which can also be applied to other electric current driving methods.
本発明の構成は次の遡りである。−気バプルを保持し伶
る崗性材料博片と、その博片上に設けたI!iJ記纒体
層に形成され、その帯状導体の幅よりも狭い幅の導体で
形成され且つ前記帯状導体と電気的に接続された蛇行バ
タンで構成した磁気バブル転送バタンである。The structure of the present invention is as follows. - A piece of granite material that holds and bends the air bubble, and an I that is placed on the piece. This magnetic bubble transfer button is formed on an iJ recording layer, is formed of a conductor having a width narrower than the width of the band-shaped conductor, and is constituted by a meandering button electrically connected to the band-shaped conductor.
次に不発明を一面を用いて説明する。第1図は不発明の
第1の実施例を示す図である。バブル田保持用−性薄片
1上に、第1の導体層に形成さnた8A1の導体バタン
2と第1の導体層と磁気的lこ絶縁された第2の導体層
に形成された第2の導体パタン3が設けら眉ている。第
1の4にバタン2は、公明きバタン若くは切り欠きバタ
ン21.21’をもつ帯状導体部20及び蛇行等体部2
2で444成されていて、夫々は一気的接続部23で鮎
びつtブらイ′1ている。蛇行等体部22の導体バタン
幅は帯状導体部20の幅よりも■くなっている。同様に
第2の導体パタン3も、穴明きバタン若くは切り欠きバ
タン31,3]’をもつ帯状導体部30及び虹竹専14
−都32で捕取されていて、夫々は磁気「9按絖都32
で粕びつけら11.ている。蛇行導体部3゛2の導体バ
タン幅も常状4体部30の暢よりも狭くなっている。蛇
行等体部22と32は9間鼠相がほぼ90°ずれて設置
されている。又、蛇行の振幅も保々に大きくなっている
。Next, non-invention will be explained using one aspect. FIG. 1 is a diagram showing a first embodiment of the invention. On the bubble field holding thin strip 1, an 8A1 conductor button 2 formed on the first conductor layer and a second conductor button 2 formed on the second conductor layer magnetically insulated from the first conductor layer are placed. Two conductor patterns 3 are provided. The first 4th button 2 includes a band-shaped conductor portion 20 having an open button or a notched button 21, 21', and a meandering body portion 2.
There are 444 pieces of 2 pieces each, each of which is connected at a single connection part 23. The conductor batten width of the meandering body portion 22 is smaller than the width of the strip-shaped conductor portion 20. Similarly, the second conductor pattern 3 also includes a band-shaped conductor portion 30 having a perforated button or a cut-out button 31, 3'
- Captured in 32 cities, each with magnetic "9
11. ing. The conductor batten width of the meandering conductor portion 3'2 is also narrower than that of the normal four-body portion 30. The meandering isobody parts 22 and 32 are installed with their angles shifted by approximately 90 degrees. Moreover, the amplitude of the meandering is also steadily increasing.
帯状パタン20 、30の幅vvO及び蛇行導体部22
゜32の+g Wlの比をR=vVo/Wt トス6ト
、蛇行a体部の電流密度はsm状4f4−バタン部の平
均゛−流@にの8倍になる。従って磁気バブル駆動に必
要な磁場強度もほぼ蛇行バタン部は帯状導体/fタン部
の8倍となる。これは即ち、磁気ノイブルを保持するた
めのバイアス磁場成分も通常転送バタン部に比べて、大
きく、従って磁気バブルが伸びやすくなることである。Width vvO of strip patterns 20 and 30 and meandering conductor portion 22
When the ratio of +g Wl of ゜32 is set to R=vVo/Wt, the current density in the meandering a-body part is eight times the average current in the sm-shaped 4f4-button part. Therefore, the magnetic field strength required for driving the magnetic bubble is approximately eight times that of the band-shaped conductor/f tongue portion in the meandering button portion. This means that the bias magnetic field component for holding the magnetic bubbles is also larger than that of the normal transfer button portion, and therefore the magnetic bubbles are more likely to expand.
−J述のボベック等Iこよって発表された文献lこよn
ば、ffl気バブルのストレッチに必要な嵐流誓度は、
約2〜3倍以上である。従って本発明ではバタン鴨比R
を2〜3以上にしておけば艮いとと着こなる。- Literature published by Bobek et al.
For example, the Arashiryu oath required to stretch the ffl ki bubble is
It is about 2 to 3 times more. Therefore, in the present invention, the batan kamo ratio R
If you set it to 2 or 3 or more, it will look like a costume.
不実施例で、導体バタン2,3に夫々90°時間位相の
ずれた父W篭流i1. I2を印加すると、帯状バタン
20 、30部転送していた磁気バブル41゜42は、
蛇行バタン22,32では、強い発生磁場のために43
.44の如く伸びた形で転送してゆく。In a non-example, the conductor buttons 2 and 3 have father W cage flows i1. When I2 is applied, the magnetic bubbles 41 and 42, which were transferring 30 parts of the band-shaped bang 20, become
At meandering batons 22 and 32, 43
.. It is transferred in an elongated form like 44.
不実施例の様に、蛇行バタン部の振幅を保々に大きくし
て、所定の振幅に達する様にm成しておくと、最初から
皮定の振幅の蛇行バタンを用いるよりも、4体抵抗値を
小さくすることが出来てMオりとなる0
次に不発明の第2の実IM圀を第2図そ用いC=明する
、不実施例では、−7−の導体層2が磁性薄片l上に設
けられている。導体r−2には切り欠き若くは、八引き
バタン21を有する帯11.4体パタン20と振幅が徐
々に大きくなった蛇状導体バタン22が′#4L気的接
続都23を介して設けられている。不実施−jでは−1
−の導体で磁気バブル転造を行なっための、−気バプル
父定1J置確保用バイアス効果を生じせしめるパーマロ
イ等の磁気的焚系50が設けられている。導体バタンに
父番パルス状亀尤■そ印加すく1と、ある極性のパルス
時で40の位置にいたのびたバフルは電匠が断時には低
気的安累に引きつけられて41の位置にくる。この両気
的要索は又、咀随断時に伸びたバブルを細才ない球に確
保する役割を担っている。導体幅比ルのイ直は第1の実
施例の場合と同様である。As in the non-example, if the amplitude of the serpentine bang section is constantly increased until it reaches a predetermined amplitude, the four-body resistance will be better than using a serpentine bang with a predetermined amplitude from the beginning. The value can be made small and the M value is 0.Next, the uninvented second real IM field is shown in FIG. It is provided on the thin piece l. The conductor r-2 has a notch, and a band 11 with an eight-pull button 21, a four-body pattern 20, and a serpentine conductor button 22 whose amplitude gradually increases are provided via a '#4L air connection 23. It is being Not implemented -1 for j
A magnetic firing system 50, such as permalloy, is provided to create a biasing effect to ensure that the - air bubble is set at 1 J for magnetic bubble rolling in the - conductor. When a pulse-like pulse is applied to the conductor button, the extended baffle, which was at position 40 when the pulse of a certain polarity was applied, is attracted by the low energy and comes to position 41 when the electric conductor is disconnected. This ambidextrous point also plays the role of securing the bubble that extends during mastication into a fine ball. The conductor width ratio is the same as in the first embodiment.
木見四の第3の実施例を第3図を用いて説明する。互f
<−記録された三層の導体層2,3.6が出性博片1に
設けられている。4俸1tl 2* 3+ 6には、大
々入門きバタン21,31.61を有する螢状導体20
、30 、60が蛇行導体22,32.62と電気的
接続部分23,33.63を介して設けられている。The third embodiment of Kimi Shishi will be explained with reference to FIG. Mutual f
<- Three recorded conductor layers 2, 3.6 are provided on the printed circuit board 1. 4 salary 1 tl 2* 3+ 6 has a large introductory button 21, a firefly-shaped conductor 20 with a 31.61
, 30, 60 are provided via meandering conductors 22, 32.62 and electrical connection portions 23, 33.63.
蛇行導体(ま大々120°の空間位相のずれをもって互
に重ね合わされている。導体バタン幅比Rは第1の実施
例の場合と同様である。この様な導体バタン20 、3
0 、601こ夫々120’の時間t1相のずれをもつ
三相父釜電流II、I2.I3を印加することにより%
虹行尋坏都にl気バブルがあれば、伸びながら転送され
てしpくことは、第一の実施例から容易に判る。Meandering conductors (which are superimposed on each other with a spatial phase shift of approximately 120°).The conductor batten width ratio R is the same as in the first embodiment.Such conductor battens 20, 3
0, 601, respectively, with a time t1 phase shift of 120'. % by applying I3
It is easy to see from the first example that if there is a qi bubble in the rainbow-filled city, it will be transferred as it expands.
以上に述べた様に本発明を用いれば、従来の電流駆wJ
杢−気バプル素子で困難であった、罎ゾ(バブル恢出を
第4よく何うための磁気バブルストレッチャーか、 1
14体、二層導体、及び三t*i導体躯鯛の場合に対し
容易に実現される。文、不発明の実施例では#ii気バ
ブルの引き伸しのためのストレッチャーにつき王として
説明してきたが、不発ゆ」は、一度伸ひたバブルを徐々
に縮めて一つの逼當峰気バブル転送路に尋く転送バタン
にも直ちに通用川床ることは云うまでもない。As described above, if the present invention is used, the conventional current drive wJ
4.What is the best use of a magnetic bubble stretcher?1.
This is easily realized for the cases of 14 conductors, a two-layer conductor, and a three-t*i conductor body. In the example of the sentence and non-invention, #ii has been explained as a stretcher for enlarging the bubble, but the "non-explosion" is a stretcher that gradually shrinks the bubble that has been stretched once and makes it into one tight peak. Needless to say, the transfer slam that occurs on the bubble transfer path will also be immediately available.
第1図、第2図 第3図は夫々不発明の粥1゜第2.及
び第3の実施例を示す。1は@気iiプル保持用罎性薄
片、2,3.6iま夫々第1.@2及び第3の4体を−
120、30、60fま夫々4体1−2゜3.6に設け
られた蛍状導体バタン、21,21,31゜31’、6
1は帝状寺棒バタン20 、30 、60に設けたバブ
ル駆動用入明看しくは切り欠きバタン22,32゜6−
2(ま4庫+@2,3.6に設けた蛇行導体]でタン、
23 、33 、63 +工夫々21友ひ22,31及
び32並びに61及び62をつなぐ屯気的接d部である
。
40.41,42,43,441;!afi気バブル及
び1左くプルの反軍位置、5旧ま峰Aバブル安定位置の
/くイアス用磁気的要素である。
?、1図
−1
第2図Figures 1, 2 and 3 show uninvented porridge 1° and 2nd. and a third example. 1 is a flexible thin piece for holding the pull, 2 and 3.6i are respectively 1st. @2 and 3rd 4 bodies-
120, 30, 60f, four firefly-shaped conductor buttons provided at 1-2° 3.6, 21, 21, 31° 31', 6
1 is a bubble drive opening or notch button 22, 32°6- provided on the Teishoji bar button 20, 30, 60.
2 (Meandering conductor installed in 4 chambers + @2, 3.6) to turn the button,
23 , 33 , 63 + Ingenuity 21 This is a part that connects 22, 31 and 32, and 61 and 62. 40.41,42,43,441;! It is a magnetic element for afi bubble and 1 left pull in the anti-military position, 5 old peak A bubble in the stable position. ? , Figure 1-1 Figure 2
Claims (1)
に設けた少くとも一層の導体層と、該導体j−に形成ざ
した穴状パタン若しくは切り欠きパタンを有する第一の
帯状導座バタンと%前記導体層に形成され、該帝状勢体
パタンの輪よりも狭く、且fm紀帯状導体バタンと電気
的iこ接続された蛇行導体パタンで構成されたことを特
徴とする磁気バブル転送バタン。 2)蛇行パタンの振幅が徐々に増大若しくは減少するこ
とを特徴とする特許請求の範囲第一項記載の磁気バブル
パタン。 3)互に電気的に絶縁された二層の導体層と、各導体層
に形成された空間位相がほぼ90〜しくは270ずれて
lね合わさrした蛇行導体パタンを有することを特徴と
する特許請求の範囲第一項記載の磁気バフル転送バタン
。 4)互Iこ電気的に絶縁された三層の導体層と、谷溝体
層の夫々に形成された空間位相がはば±120゜ずれて
重ね合された蛇行導体パタンを有するこおを特徴とする
特許請求の範囲第一項記載の磁気バブル転送バタン。[Claims] l) A thin piece of material capable of holding a magnetic bubble, at least one conductor layer provided on the thin piece, and a hole-like pattern or cutout pattern formed in the conductor. a meandering conductor pattern formed on the conductor layer, narrower than the loop of the impermeable body pattern, and electrically connected to the fm period band-shaped conductor batten; Featuring a magnetic bubble transfer bang. 2) The magnetic bubble pattern according to claim 1, wherein the amplitude of the meandering pattern gradually increases or decreases. 3) It is characterized by having two conductor layers that are electrically insulated from each other and a meandering conductor pattern formed on each conductor layer that is aligned with the spatial phase shifted by approximately 90 to 270 degrees. A magnetic baffle transfer button according to claim 1. 4) A steel having a meandering conductor pattern in which three conductor layers electrically insulated from each other and a valley-groove body layer are overlaid with spatial phases shifted by ±120°. A magnetic bubble transfer button according to claim 1, characterized in that:
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56188808A JPS5891582A (en) | 1981-11-25 | 1981-11-25 | Magnetic bubble transfer pattern |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56188808A JPS5891582A (en) | 1981-11-25 | 1981-11-25 | Magnetic bubble transfer pattern |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5891582A true JPS5891582A (en) | 1983-05-31 |
JPH0232708B2 JPH0232708B2 (en) | 1990-07-23 |
Family
ID=16230161
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP56188808A Granted JPS5891582A (en) | 1981-11-25 | 1981-11-25 | Magnetic bubble transfer pattern |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5891582A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2677795A1 (en) * | 1991-06-13 | 1992-12-18 | Sp K Tekhn | Readout device for magnetic bubbles |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH04125811U (en) * | 1991-05-10 | 1992-11-17 | ポーラ化成工業株式会社 | cosmetic compact |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5766586A (en) * | 1980-10-09 | 1982-04-22 | Oki Electric Ind Co Ltd | Magnetic bubble detector |
JPS57120287A (en) * | 1981-01-19 | 1982-07-27 | Oki Electric Ind Co Ltd | Magnetic bubble detector |
-
1981
- 1981-11-25 JP JP56188808A patent/JPS5891582A/en active Granted
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5766586A (en) * | 1980-10-09 | 1982-04-22 | Oki Electric Ind Co Ltd | Magnetic bubble detector |
JPS57120287A (en) * | 1981-01-19 | 1982-07-27 | Oki Electric Ind Co Ltd | Magnetic bubble detector |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2677795A1 (en) * | 1991-06-13 | 1992-12-18 | Sp K Tekhn | Readout device for magnetic bubbles |
Also Published As
Publication number | Publication date |
---|---|
JPH0232708B2 (en) | 1990-07-23 |
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