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JPS6040113B2 - magnetic bubble element - Google Patents
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JPS6040113B2 - magnetic bubble element - Google Patents

magnetic bubble element

Info

Publication number
JPS6040113B2
JPS6040113B2 JP57153772A JP15377282A JPS6040113B2 JP S6040113 B2 JPS6040113 B2 JP S6040113B2 JP 57153772 A JP57153772 A JP 57153772A JP 15377282 A JP15377282 A JP 15377282A JP S6040113 B2 JPS6040113 B2 JP S6040113B2
Authority
JP
Japan
Prior art keywords
magnetic
hairpin
bubble
magnetic bubble
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
JP57153772A
Other languages
Japanese (ja)
Other versions
JPS5942689A (en
Inventor
治雄 浦井
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.)
DENSHI KEISANKI KIPPON GIJUTSU KENKYU KUMIAI
Original Assignee
DENSHI KEISANKI KIPPON GIJUTSU KENKYU KUMIAI
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 DENSHI KEISANKI KIPPON GIJUTSU KENKYU KUMIAI filed Critical DENSHI KEISANKI KIPPON GIJUTSU KENKYU KUMIAI
Priority to JP57153772A priority Critical patent/JPS6040113B2/en
Publication of JPS5942689A publication Critical patent/JPS5942689A/en
Publication of JPS6040113B2 publication Critical patent/JPS6040113B2/en
Expired 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
    • G11C11/02Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using magnetic elements
    • G11C11/14Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using magnetic elements using thin-film elements

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Hardware Design (AREA)

Description

【発明の詳細な説明】 本発明はヘアピン状導体を有する磁気バブル素子に関し
、特に、磁気バブル若しくは伸長した磁気バブルを消去
若しくは収縮するためのヘアピン状導体を持つ磁気バブ
ル素子に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic bubble element having a hairpin-like conductor, and more particularly to a magnetic bubble element having a hairpin-like conductor for erasing or deflating a magnetic bubble or an elongated magnetic bubble.

磁気バブルを用いて情報を記録、記憶する素子(以下磁
気バブル素子と称す)においては、情報としての磁気バ
ブルを発生する手段および貯蔵する手段の他に、磁気バ
ブルの存在を情報として読み出す手段すなわち磁気バブ
ル検出器が不可欠な機能要素である。
In an element that records and stores information using magnetic bubbles (hereinafter referred to as a magnetic bubble element), in addition to means for generating and storing magnetic bubbles as information, there is also a means for reading out the presence of magnetic bubbles as information, i.e. A magnetic bubble detector is an essential functional element.

近年、磁気バブル素子で用いる磁気バブルの径は、記憶
密度の増大に伴ない微小化する方向に進んできている。
読み出すべき磁気バブルの径が微小化すると、これに伴
ない、一般に、磁気バブルの検出出力が低下する。この
ような磁気バブルの微小化に伴なう検出出力の低下を補
償するために、磁気バブルストレッチャーが種々提案さ
れている。磁気バブルストレッチャーを用いた磁気バブ
ル検出出力の補償は次のようにして行なわれる。
In recent years, the diameter of magnetic bubbles used in magnetic bubble elements has been becoming smaller as storage density has increased.
As the diameter of the magnetic bubble to be read becomes smaller, the detection output of the magnetic bubble generally decreases accordingly. Various magnetic bubble stretchers have been proposed in order to compensate for the decrease in detection output due to miniaturization of magnetic bubbles. Compensation of the magnetic bubble detection output using the magnetic bubble stretcher is performed as follows.

磁気バブルストレッチャーにより大きく引き伸ばされた
磁気バブル(以下伸長バブルと称する)からは、通常径
の磁気バブルから発生する漏洩磁束よりも大きな漏洩磁
束が発生する。磁気バブルを直線的に伸長する場合には
伸長バブルからの漏洩磁束はその伸長比に比例して増大
する。一般に、磁束を検出する材料、例えば、パーマロ
ィ等の磁気抵抗効果を示す料を磁気バブルの伸長する長
さに合せて検出素子として設けると、その漏洩磁束によ
り検出素子の抵抗値は変化し、変化の絶対値は伸長長さ
に比例して大きくなる。すなわち、大きな磁気バブル検
出出力が得られる。このような磁気バブルストレッチャ
−には大きく分けて次の二種類がよく知られている。
A magnetic bubble that has been greatly stretched by the magnetic bubble stretcher (hereinafter referred to as an extended bubble) generates leakage magnetic flux that is larger than that generated from a magnetic bubble with a normal diameter. When a magnetic bubble is stretched linearly, the leakage magnetic flux from the stretched bubble increases in proportion to the stretching ratio. Generally, when a material that detects magnetic flux, for example, a material that exhibits a magnetoresistive effect such as permalloy, is provided as a detection element in accordance with the length of extension of a magnetic bubble, the resistance value of the detection element changes due to the leakage magnetic flux. The absolute value of increases in proportion to the elongated length. That is, a large magnetic bubble detection output can be obtained. The following two types of magnetic bubble stretchers are well known.

第1は、ストラウス等によって磁性および磁気材料会議
で発表された文献(AIPConfefencePro
C.No.10,202(1972)に記載のパーマロ
ィ等の敏磁性体シェフロンパタンの積重なり部で磁気バ
ブルを徐々に伸長するシェブロンストレツチヤ−である
。第2は、ネルソン等らによってベル・システム・テク
ニカルジャーナル誌に発表された文献(既TJ,59,
229(1980))に記載のヘアピン状導体に電流パ
ルスを通じ、このヘアピン状導体間隙部に生じる磁気的
ポテンシャルにより磁気バブルを急激に伸長するヘアピ
ン導体ストレッチャーである。このヘアピン導体ストレ
ッチヤーは主として、磁気バブル材料に選択的にイオン
注入することにより形成した連接円形パタン(以下CD
パタンと称す)により構成された磁気バブル転送路中に
配置された磁気バブル検出器部に用いられることが多い
。ヘアピン導体ストレッチャーは、導体に印加する電流
パルスにより磁気バブルを急速に伸長するため、磁気バ
ブルを伸長する直前でも任意にバブルの転送を止めるこ
とができ、磁気バブル検出用転送路中での磁気バブルの
スタート・ストップが前述のシェブロンストレッチャー
に比べて任意に行なえる特徴がある。
The first is the paper presented at the Magnetism and Magnetic Materials Conference by Strauss et al.
C. No. 10, 202 (1972), the chevron stretcher gradually stretches magnetic bubbles at the stacked part of a chevron pattern made of a sensitive magnetic material such as permalloy. The second is the literature published by Nelson et al. in the Bell System Technical Journal (already TJ, 59,
229 (1980)), in which a current pulse is passed through a hairpin-shaped conductor, and a magnetic bubble is rapidly expanded by the magnetic potential generated in the gap between the hairpin-shaped conductors. This hairpin conductor stretcher mainly consists of a continuous circular pattern (CD) formed by selectively implanting ions into a magnetic bubble material.
It is often used in a magnetic bubble detector section arranged in a magnetic bubble transfer path formed by a pattern (referred to as a pattern). The hairpin conductor stretcher rapidly stretches magnetic bubbles by applying a current pulse to the conductor, so it is possible to stop the transfer of bubbles at will even just before the magnetic bubbles are stretched. Compared to the above-mentioned chevron stretcher, the bubble can be started and stopped at will.

さらに、このヘアピン導体ストレッチャーは、ストレッ
チャー近傍に配置した検出器で磁気バブルを検出したあ
との磁気バブルを、もしそれが不要なら、ヘアピン導体
に逆極性の電流パルスを印加することにより消去するこ
とが可能である。伸長した磁気バブルを同様な電流パル
スで通常径の磁気バブルに収縮させることも可能である
。しかしながら、従来のヘアピン導体ストレッチャーを
磁気バブルの消去器又は収縮器として用いる場合には次
に図面を用いて説明するような、動作が不安定になると
いう重大な欠点を有している。
Furthermore, this hairpin conductor stretcher eliminates magnetic bubbles after they are detected by a detector placed near the stretcher, by applying a current pulse of opposite polarity to the hairpin conductor if they are not needed. Is possible. It is also possible to contract an elongated magnetic bubble into a normal diameter magnetic bubble with a similar current pulse. However, when the conventional hairpin conductor stretcher is used as a magnetic bubble eraser or constrictor, it has a serious drawback of unstable operation, as will be explained below with reference to the drawings.

第1図は従来のヘアピン導体ストレッチャーを用いた磁
気バブル検出器を示す図である。
FIG. 1 is a diagram showing a magnetic bubble detector using a conventional hairpin conductor stretcher.

磁気バブルを保持し得る磁性材料1に、例えば、イオン
注入等で形成された面内回転磁場で磁気バブルを転送し
得る磁気バブル転送路11設けられている。この磁気バ
ブル転送路1 1には、ヘァピン導体ストレッチャー2
及びヘアピン間隙部にパーマロィ薄膜ストライプ磁気抵
抗素子等でなる磁気バブル検出素子3が配置してある。
バイアス磁場の方向は矢印HBで示す方向に印加されて
いるものとする。磁気バブルがこのヘアピン導体ストレ
ツチャー、検出器部に転送されてきたときに導体2にス
トレッチャー電流ls22を矢印21に示す方向に通ず
ると、磁気バブルはストレッチ検出される。検出後の不
要磁気バブルは逆極性の電流パルス23を導体パタン2
に印加してヘアピン内に生じる逆極I性磁場で消滅させ
られる。このとき磁気バブル転送路周辺に不要の磁気バ
ブル42が残る現象がいまいま生じる。転送路周辺の不
要磁気バブルの存在は、磁気バブル素子の大きな誤動作
の原因となる。上述した磁気バブル消滅時の不要磁気バ
ブルの存在の原因を第2図A〜Cを参照して説明する。
A magnetic material 1 capable of holding magnetic bubbles is provided with a magnetic bubble transfer path 11 capable of transferring magnetic bubbles using an in-plane rotating magnetic field formed by, for example, ion implantation. This magnetic bubble transfer path 11 includes a hairpin conductor stretcher 2.
A magnetic bubble detection element 3 made of a permalloy thin film stripe magnetoresistive element or the like is arranged in the hairpin gap.
It is assumed that the direction of the bias magnetic field is applied in the direction indicated by arrow HB. When the magnetic bubble is transferred to the hairpin conductor stretcher and the detector section, when a stretcher current ls22 is passed through the conductor 2 in the direction shown by the arrow 21, the magnetic bubble is detected as being stretched. After detection, the unnecessary magnetic bubble passes through the conductor pattern 2 with a current pulse 23 of opposite polarity.
It is annihilated by the reverse polarity I magnetic field generated inside the hairpin. At this time, a phenomenon occurs in which unnecessary magnetic bubbles 42 remain around the magnetic bubble transfer path. The presence of unnecessary magnetic bubbles around the transfer path causes major malfunctions of the magnetic bubble element. The cause of the presence of unnecessary magnetic bubbles when the magnetic bubbles disappear will be explained with reference to FIGS. 2A to 2C.

第2図Aに示すように、ヘァピン導体2で伸長された磁
気バブル4はヘアピン内部に存在している。次に、伸長
磁気バブル消去用逆極性電流パルスをヘアピン導体2に
印加すると、第2図Bに示すバイアス磁場がヘアピン導
体の近傍の分布する。ヘアピン導体の間隙部では、バイ
アス磁場分は上に凸であるため内部の伸長磁気バブルは
位置的に不安定となる。このため第2図Cに示すように
ヘアピン間隙の伸長磁気バブルの一部は磁場分布のより
安定な方向(この場合はヘアピン導外外部の方向)に移
動し、伸長磁気バブルの一部41がヘアピン導体外には
み出す。一方ヘアピン内部にある伸長磁気バブルの一部
4川ま、バイアス磁場の増大により最後にはその部分で
切断される。この結果、ヘアピン導体外すなわち、転送
路11近傍に不要な磁気バブルが生じることになる。又
、伸長磁気バブルを収縮させる場合にも、同様に、ヘア
ピン導体間隙部で縮まずに導体外部にとび出して縮むと
いう誤動作が容易に生じる。本発明の目的は、従来のヘ
アピン導体磁気バブルトレッチャーの磁気バブル消去若
しくは収縮動作の不安定性を取り除いた安定消去・収縮
動作が可能なヘアピン導体磁気バブル消去器を持つ磁気
バブル素子を提供することにある。本発明に係る磁気バ
ブル素子は、磁気バブルを保持し得る磁性材料薄膜と、
該磁性材料薄膜上に設けられた磁気バブル転送路と、該
転送路中に配置された磁気バブル検知手段をその近傍に
伴なう第1のヘアピン状導体パタンとを有し、該第1の
ヘアピン状導体パタンの間隙部と共通の間隙部を持つ第
2のヘアピン状導体パタンが前記第1の導体パタン近傍
に設けられた構成を有する。
As shown in FIG. 2A, the magnetic bubble 4 extended by the hairpin conductor 2 exists inside the hairpin. Next, when a reverse polarity current pulse for eliminating the elongated magnetic bubble is applied to the hairpin conductor 2, a bias magnetic field shown in FIG. 2B is distributed in the vicinity of the hairpin conductor. In the gap between the hairpin conductors, the bias magnetic field is convex upward, so the internal elongated magnetic bubble becomes unstable in position. Therefore, as shown in FIG. 2C, a part of the elongated magnetic bubble in the hairpin gap moves in the direction where the magnetic field distribution is more stable (in this case, the direction outside the hairpin), and a part of the elongated magnetic bubble 41 It protrudes outside the hairpin conductor. On the other hand, a portion of the elongated magnetic bubble inside the hairpin is finally cut off at that portion due to the increase in the bias magnetic field. As a result, unnecessary magnetic bubbles are generated outside the hairpin conductor, that is, in the vicinity of the transfer path 11. Furthermore, when an elongated magnetic bubble is contracted, a similar malfunction easily occurs in which the bubble does not contract in the gap between the hairpin conductors, but instead protrudes to the outside of the conductor and contracts. An object of the present invention is to provide a magnetic bubble element having a hairpin conductor magnetic bubble eliminator that is capable of stable erasure and contraction operations that eliminate the instability of the magnetic bubble erasure and contraction operations of conventional hairpin conductor magnetic bubble stretchers. It is in. The magnetic bubble element according to the present invention includes a thin film of magnetic material capable of holding magnetic bubbles;
a magnetic bubble transfer path provided on the thin film of magnetic material; and a first hairpin-shaped conductor pattern with a magnetic bubble detection means disposed in the transfer path in the vicinity thereof; A second hairpin-shaped conductor pattern having a common gap with the gap of the hairpin-shaped conductor pattern is provided near the first conductor pattern.

次に本発明の原理について図面を参照して詳細に説明す
る。
Next, the principle of the present invention will be explained in detail with reference to the drawings.

まず、本発明の基本概念を第3図を参照して説明する。First, the basic concept of the present invention will be explained with reference to FIG.

第3図Aに示すヘアビン状導体パタン5は、従来のもの
に比べてその導体ストライプの中心間距離2Wを従来の
ものに比べてある程度大きくしてある。中心間距離2W
がある程度大きくなると、そのヘアピン状導体部に生じ
る発生磁場分布は、3図Bの24に示すように、導体間
隙部の磁場分布の中央部にその両側より発生磁場の小さ
な部分(即ちポテンシャル極小部分)が生じることが本
願出願人による計算等で明らかにされた。従って、第3
図Aに示すように、伸長磁気バブル4がヘアピン状導体
5の中央部隊間に存在するときに、同図Bの磁場分布を
磁気バブルの磁化方向に印加すると、中央間隙部では磁
気的ポテンシャルが極小となるため、その磁気バルブは
導体間隙部分から離れることなく、全体に磁気的ポテン
シャルが高くなり、第3図Cに示すように、導体中央間
隙部でその伸長磁気バブルは滋区幅が狭くなり最後には
消滅する。換言すれば、磁気バブルの確実、安定な消去
動作が行なえることになる。伸長磁気バブルの収縮に関
しても、発生磁場を弱くし、かつ、磁気バブルが消滅し
ない内に磁場発生を停止することにより安定に動作する
ことは同様に明らかである。本発明の原理について第4
図A〜Dを参照してさらに詳しく述べる。
The hairbin-shaped conductor pattern 5 shown in FIG. 3A has a distance 2W between the centers of its conductor stripes that is somewhat larger than that of the conventional pattern. Center distance 2W
When becomes large to a certain extent, the generated magnetic field distribution generated in the hairpin-shaped conductor part will become smaller in the central part of the magnetic field distribution in the conductor gap part (i.e., the minimum potential part) from both sides, as shown in 24 in Figure 3B. ) has been revealed through calculations etc. by the applicant. Therefore, the third
As shown in Figure A, when the elongated magnetic bubble 4 exists between the central sections of the hairpin-shaped conductor 5, when the magnetic field distribution shown in Figure B is applied in the magnetization direction of the magnetic bubble, the magnetic potential increases in the central gap. Because it is extremely small, the magnetic bulb does not move away from the conductor gap, and the magnetic potential increases throughout, and as shown in Figure 3C, the elongated magnetic bubble has a narrow width at the conductor center gap. and eventually disappear. In other words, a reliable and stable erasing operation of magnetic bubbles can be performed. It is similarly clear that the contraction of the elongated magnetic bubble can be stably operated by weakening the generated magnetic field and stopping the magnetic field generation before the magnetic bubble disappears. Part 4 about the principle of the present invention
Further details will be described with reference to Figures A to D.

本発明に係るヘアピン状導体5のストライプ幅と厚さは
、第4図B、に示すように、それぞれ0.6仏mおよび
0.3山mである。このとき、第4図Aに示すように、
このヘアピン状導体5を磁気バブルを保持し得る磁性材
料1の中心と導体中心間の距離が日になるように設けて
おく。ヘアピン状導体の間隔は、双方の導体ストライプ
幅の中心間で測って2Wとなるようにしておく。磁気バ
ブルが感じる導体からの磁場を前記の磁性材料の中心磁
場で代表すると、本発明に必要であるヘアピン導体中央
間隙部で磁気ポテンシャルの極小を生じさせるためには
、日と2Wとの間に第4図D又はDに示すような非常に
限定された関係が必要であることが明らかにされた。ヘ
アピン導体間隔2Wを変化させたとき、ヘアピン状導体
中央間隙部に磁気ポテンシャルの極小を生じさせる最大
の磁性材料導体間距離日を2Wで規格化して4図Cに示
す。比H/(2W)は2Wが大きくなるにつれて0.2
5丘づくことが示されている。同様に、距離日を変化さ
せたときの中央間隙部での磁気ポテンシャル極小を生じ
せしめる最小の導体間隔2Wを距離日で規格化して第4
図Dに示す。比2W/日は日の増大に伴なし、4.0に
近づく。以上から、ヘアピン状導体で伸長磁気バブルを
安定消滅、若しくは安定収縮させるためには比2W/日
がなくとも4.0より大きいことが必要であることが明
らかになった。さらに、ヘアピン状導体5のパタン幅及
び厚さをそれぞれ2.0仏mおよび0.5仏mと変化さ
せても中央間隙部での磁気ポテンシャル極小を生じせし
めるためには比2W/日が少なくとも4.0より大きい
ことが必要であるとには変りないことが明らかになつた
The stripe width and thickness of the hairpin-shaped conductor 5 according to the present invention are 0.6 m and 0.3 m, respectively, as shown in FIG. 4B. At this time, as shown in Figure 4A,
The hairpin-shaped conductor 5 is provided so that the distance between the center of the magnetic material 1 capable of holding a magnetic bubble and the center of the conductor is equal to the distance between the center of the conductor and the center of the magnetic material 1 capable of holding a magnetic bubble. The spacing between the hairpin-shaped conductors is set to 2W as measured between the centers of both conductor stripe widths. If the magnetic field from the conductor that the magnetic bubble feels is represented by the central magnetic field of the magnetic material mentioned above, in order to generate the minimum magnetic potential in the central gap of the hairpin conductor, which is necessary for the present invention, it is necessary to It has become clear that a very specific relationship as shown in FIG. 4D or D is required. When the hairpin conductor spacing 2W is changed, the maximum distance between magnetic material conductors that causes a minimum magnetic potential in the center gap of the hairpin conductor is normalized by 2W and is shown in Figure 4C. The ratio H/(2W) becomes 0.2 as 2W increases.
It is shown that there are 5 hills. Similarly, when the distance day is changed, the minimum conductor spacing 2W that causes the minimum magnetic potential in the center gap is normalized by the distance day, and the fourth
Shown in Figure D. The ratio 2W/day approaches 4.0 as the day increases. From the above, it has become clear that in order to stably extinguish or stably shrink an elongated magnetic bubble in a hairpin-shaped conductor, the ratio needs to be greater than 4.0, even if the ratio is not 2 W/day. Furthermore, even if the pattern width and thickness of the hairpin-shaped conductor 5 are changed to 2.0 French m and 0.5 French m, respectively, the ratio of at least 2 W/day is required to generate the minimum magnetic potential in the central gap. It became clear that a value greater than 4.0 was still necessary.

従って、本発明に係る磁気バブル素子の構成をさらに詳
しく述べると次のようになる。
Therefore, the structure of the magnetic bubble element according to the present invention will be described in more detail as follows.

すなわち、磁気バブルトレッチャーを形成する第1のヘ
アピン状導体パタンの近傍に、中央間隙部を共通に持つ
磁気バブル消去用第2ヘアピン状導体を設け、第2のヘ
アピン状導体パタンの両側導体の中心間距離(2W)と
バブル磁区保持用磁性材料薄膜中心と第2ヘアピン状導
体の膜厚中心間距離(H)との比(2W/H)が4.0
以上であるこを特徴とする磁気バブル素子である。本発
の実施例を次に述べる。
That is, a second hairpin-like conductor for magnetic bubble erasure having a common central gap is provided near the first hairpin-like conductor pattern forming the magnetic bubble stretcher, and the conductors on both sides of the second hairpin-like conductor pattern are The ratio (2W/H) of the center-to-center distance (2W) to the center-to-center distance (H) between the center of the magnetic material thin film for bubble domain retention and the film thickness of the second hairpin-shaped conductor is 4.0.
This is a magnetic bubble element characterized by the above. An example of this invention will be described below.

第5図A〜Cは本発明の第1の実施例を説明する図であ
る。第5図Aの平面図に示すように本実施例は、バブル
滋区転送路11に設けられた磁気バブルトレッチャー2
および磁気バブル検知手段3ならびに磁気バブルトレッ
チヤー2の周囲に第2のヘアピン状導体パタン5が中央
間隙部を磁気バブルストレッチャー2と共通部をもつよ
うに配置された磁気バブル素子である。第5図Bに本実
施例に係る磁気バブル素子の断面図を示す。
FIGS. 5A to 5C are diagrams illustrating a first embodiment of the present invention. As shown in the plan view of FIG.
A second hairpin-shaped conductor pattern 5 is arranged around the magnetic bubble detecting means 3 and the magnetic bubble stretcher 2 so that the central gap is in common with the magnetic bubble stretcher 2. FIG. 5B shows a cross-sectional view of the magnetic bubble element according to this example.

本実施例では、第1のヘアピン状導体2による段差を平
滑化処理により無くして第2のヘアピン状導体パタン5
がバブル磁区保持用材料薄膜1に設けられている。第2
のヘアピン状導体間隙2Wとヘアピン状導体層の中心と
バブル磁区材料薄膜中心間距離日の比(2W/H)は4
.0以上になるように構成されている。これらのヘアピ
ン状導体パタンによる発生バイアス成分磁場分布は第5
図Cのようになる。第1のヘアピン状導体パタンはパタ
ン間隙が第2のそれより充分小さいので、第5図Cの2
4′に示すように一つの谷をもつ磁場分布を示す。これ
より磁気バブルを伸長し、次に、第2ヘアピン状導体パ
タンに伸長磁気バブル消去用電流パルスを印加する。第
2のヘアピン状導体パタンによる磁場分布は24に示す
ようにヘアピン中央間隙部に極小部を有するため、伸長
磁気バブルは位置ずれを起こさずに安定に消滅する。次
に本発明の第2の実施例を第6図に示す。
In this embodiment, the level difference caused by the first hairpin-shaped conductor 2 is eliminated by a smoothing process, and the second hairpin-shaped conductor pattern 5 is formed.
is provided in the bubble magnetic domain holding material thin film 1. Second
The ratio (2W/H) between the hairpin-shaped conductor gap 2W and the center of the hairpin-shaped conductor layer and the center of the bubble magnetic domain material thin film is 4.
.. It is configured to be 0 or more. The bias component magnetic field distribution generated by these hairpin conductor patterns is the fifth
It will look like Figure C. Since the first hairpin-like conductor pattern has a sufficiently smaller pattern gap than the second,
4' shows a magnetic field distribution with one valley. From this, the magnetic bubble is extended, and then a current pulse for erasing the extended magnetic bubble is applied to the second hairpin-shaped conductor pattern. Since the magnetic field distribution due to the second hairpin-shaped conductor pattern has a minimum part at the center gap of the hairpin as shown in 24, the elongated magnetic bubble disappears stably without causing positional deviation. Next, a second embodiment of the present invention is shown in FIG.

本実施例では、第2のヘアピン状導体パタン5は、第1
のヘアピン状導体パタンと同一面上に設けられている。
従って、導体パタン2および5は同一の導体層で構成す
ることができる。又、比2W/日は充分に4.0より大
きくなっている。本発明の第3の実施例を第7図に示す
In this embodiment, the second hairpin-like conductor pattern 5
It is provided on the same surface as the hairpin-shaped conductor pattern.
Therefore, conductor patterns 2 and 5 can be constructed from the same conductor layer. Further, the ratio 2W/day is sufficiently larger than 4.0. A third embodiment of the invention is shown in FIG.

本実施例では、第1のヘアピン状導体パタン2のバブル
磁区材料薄膜1のスベーサーを第1のヘアピン状導体パ
タンの周りで掘り下げて、第2のヘアピン導体とバブル
磁区材料薄膜1との距離日をさらに小さくして比2W/
日を大きくした構造の磁気バブル素子が示されている。
本発明の第4の実施例を第8図に示す。
In this example, the spacer of the bubble magnetic domain material thin film 1 of the first hairpin-shaped conductor pattern 2 is dug down around the first hairpin-shaped conductor pattern to determine the distance between the second hairpin conductor and the bubble magnetic domain material thin film 1. further reduce the ratio to 2W/
A magnetic bubble element with an enlarged structure is shown.
A fourth embodiment of the invention is shown in FIG.

本実例では、磁気バブル消去用の第2のヘアピン状導体
2と、バブル磁区材料薄膜1の間に設けられている。こ
のようにしておくと、日をきわめて小さくすることがで
きる。日を小さくすると単位流当りの発生磁場強度が強
くなり、伸長磁気バブルの消去電流を少なくすることが
できる。以上に述べたように、本発明を用いれば、長く
伸長された磁気バブルを安定に消去若くは収縮せしめる
ことのできる磁気バブル消去器を有する磁気バブル素子
が実現される。
In this example, it is provided between the second hairpin-shaped conductor 2 for magnetic bubble erasure and the bubble magnetic domain material thin film 1. By doing this, you can make the days extremely small. When the number of days is reduced, the generated magnetic field strength per unit current becomes stronger, and the erasing current of the elongated magnetic bubble can be reduced. As described above, by using the present invention, a magnetic bubble element having a magnetic bubble eraser capable of stably erasing or shrinking a long elongated magnetic bubble can be realized.

さらに、本発明を実施することにより新たな効果が生じ
る。すなわち、第1のヘアピン状導体パタンと第2のヘ
アピン状導体パタンとを必要に応じて外部で直列に俵続
し、磁気バブルストレッチャーとして使用する場合、き
わめて微小な電流パルスで充分にトレッチできるだけの
磁場を発することが可能となる。この際は、第2のヘア
ピン導体パタンにおける2W/日の比は必しも4.0以
上である必要はないことは明白である。又、本発明の説
明では、磁気バブルの転送路の例として、選択的にイオ
ン注入して形成したパタン列によるものを挙げたが、軟
磁性体のパタンにより形成したもの等を用いてもよく転
送路の形成法を規定するものではない。
Furthermore, new effects arise by implementing the present invention. That is, when the first hairpin-shaped conductor pattern and the second hairpin-shaped conductor pattern are connected in series externally as necessary and used as a magnetic bubble stretcher, sufficient stretching can be achieved with an extremely small current pulse. It becomes possible to emit a magnetic field of In this case, it is clear that the ratio of 2W/day in the second hairpin conductor pattern does not necessarily need to be 4.0 or more. Furthermore, in the description of the present invention, as an example of the transfer path of magnetic bubbles, a pattern array formed by selective ion implantation is given, but a path formed by a pattern of soft magnetic material may also be used. It does not specify how to form a transfer path.

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

第1図は本発明に係る従来例を示す図、第2図A〜Cは
従来例の欠点を説明するための図、第3図A〜Cは本発
明の概念を示す図、第4図A〜Dは本発明の原理を示す
図、第5図A〜Cは本発明の第1の実例を示す図ならぴ
に第6図〜第8図はそれぞれ本発明の第2〜第4の実施
例を示す図である。 図において、1は磁気バブル保持用磁性材料薄膜、2は
第1のヘアピン状導体パタン、3は磁気バブル検出器、
4は伸長した磁気バブル、5は第2のヘアピン状導体パ
タン、11は磁気バブル転送路、21は電流パルス印加
方向を示す矢印、22は磁気バブルストレッチ電流パル
ス、23は同消滅若しくは収縮パルス、24,24′は
ヘアピン導体部の磁場分布、40は磁気バブル消滅部分
、41は磁気バブルがヘアピン導体外にはみ出した部分
、42は消滅残りの不要磁気バブルである。 第6図 策7図 第8図 弟‘図 第2図 努3図 幕4図 髪S図
FIG. 1 is a diagram showing a conventional example according to the present invention, FIGS. 2 A to C are diagrams for explaining the drawbacks of the conventional example, FIGS. 3 A to C are diagrams illustrating the concept of the present invention, and FIG. A to D are diagrams showing the principle of the invention, FIGS. 5A to C are diagrams showing the first example of the invention, and FIGS. 6 to 8 are diagrams showing the second to fourth examples of the invention, respectively. It is a figure showing an example. In the figure, 1 is a magnetic material thin film for holding magnetic bubbles, 2 is a first hairpin-shaped conductor pattern, 3 is a magnetic bubble detector,
4 is an elongated magnetic bubble, 5 is a second hairpin-shaped conductor pattern, 11 is a magnetic bubble transfer path, 21 is an arrow indicating the current pulse application direction, 22 is a magnetic bubble stretch current pulse, 23 is an extinction or contraction pulse, Reference numerals 24 and 24' indicate the magnetic field distribution of the hairpin conductor, 40 the magnetic bubble extinguished area, 41 the area where the magnetic bubble protrudes outside the hairpin conductor, and 42 the unnecessary magnetic bubble remaining after the extinguishment. Figure 6: Measures 7: Figure 8: Younger brother's figure: Figure 2: Tsutomu 3: Curtain 4: Hair S figure

Claims (1)

【特許請求の範囲】 1 バブル磁区を保持し得る磁性材料薄膜と、該磁性材
料薄膜上に設けられたバブル磁区転送路と、該転送路に
配置されたバブル磁区検出手段とその近傍に伴なう第1
のヘアピン状導体パタンとを有し、該第1のヘアピン状
導体パタンの間隙部と共通の間隙部を持つ第2のヘアピ
ン状導体パタンが前記第1の導体パタン近傍に設けられ
たことを特徴とする磁気バブル素子。 2 前記第2のヘアピン状導体パタンの両側導体の中心
間距離(2W)と、前記バブル磁区保持用磁性材料薄膜
と前記第2のヘアピン状導体の膜厚中心との間の距離(
H)との比(2W/H)が4.0以上であることを特徴
とする特許請求の範囲第1項記載の磁気バブル素子。
[Scope of Claims] 1. A magnetic material thin film capable of retaining a bubble magnetic domain, a bubble magnetic domain transfer path provided on the magnetic material thin film, a bubble magnetic domain detecting means disposed in the transfer path, and the vicinity thereof. First
a hairpin-like conductor pattern, and a second hairpin-like conductor pattern having a common gap with a gap of the first hairpin-like conductor pattern is provided in the vicinity of the first conductor pattern. magnetic bubble element. 2 The distance between the centers of both side conductors of the second hairpin-shaped conductor pattern (2W) and the distance between the center of the film thickness of the bubble domain holding magnetic material thin film and the second hairpin-shaped conductor (
2. The magnetic bubble element according to claim 1, wherein the ratio (2W/H) to H) is 4.0 or more.
JP57153772A 1982-09-03 1982-09-03 magnetic bubble element Expired JPS6040113B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57153772A JPS6040113B2 (en) 1982-09-03 1982-09-03 magnetic bubble element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57153772A JPS6040113B2 (en) 1982-09-03 1982-09-03 magnetic bubble element

Publications (2)

Publication Number Publication Date
JPS5942689A JPS5942689A (en) 1984-03-09
JPS6040113B2 true JPS6040113B2 (en) 1985-09-09

Family

ID=15569795

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57153772A Expired JPS6040113B2 (en) 1982-09-03 1982-09-03 magnetic bubble element

Country Status (1)

Country Link
JP (1) JPS6040113B2 (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5920499U (en) * 1982-07-27 1984-02-07 富士通株式会社 bubble memory device

Also Published As

Publication number Publication date
JPS5942689A (en) 1984-03-09

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