JPS6145487A - Ion implantation type magnetic bubble memory element - Google Patents

Ion implantation type magnetic bubble memory element

Info

Publication number
JPS6145487A
JPS6145487A JP60137718A JP13771885A JPS6145487A JP S6145487 A JPS6145487 A JP S6145487A JP 60137718 A JP60137718 A JP 60137718A JP 13771885 A JP13771885 A JP 13771885A JP S6145487 A JPS6145487 A JP S6145487A
Authority
JP
Japan
Prior art keywords
ion implantation
magnetic bubble
detector
cusp
magnetic
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
JP60137718A
Other languages
Japanese (ja)
Inventor
Hitoshi Ikeda
池田 整
Makoto Suzuki
良 鈴木
Naoki Kodama
兒玉 直樹
Ken Sugita
杉田 愃
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP60137718A priority Critical patent/JPS6145487A/en
Publication of JPS6145487A publication Critical patent/JPS6145487A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain an ion implantation type magnetic bubble memory element having a magnetic bubble tansfer line prevented from the generation of abnormal transfer at a position close to a magnetic bubble detector by forming a non- ion implantation area close to the detector as a prescribed shape. CONSTITUTION:The ion implantation area is formed as a prescribed shape and a non-ion implantation layer 2' on the back of a transfer line 6 is removed at a cusp B arranged before a cusp A detecting a magnetic bubble of an ion implantation transfer line 6 by one bit at a position close to the detector. Since the charged wall from the cusp B to the cusp A is easily formed on the basis of the shape of the layer 2', the magnetic bubble reaches the cusp A precisely. Consequently, the ion implantation type magnetic bubble memory element having the magnetic bubble transfer line prevented from the generation of abnormal transfer near the magnetic bubble detector is obtained.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は、磁気バブルメモリ素子、特に、イオン打込み
転送路を有する磁気バブルメモリ素子における検出器近
傍の転送路の改良に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a magnetic bubble memory device, and more particularly to an improvement of a transfer path near a detector in a magnetic bubble memory device having an ion implantation transfer path.

〔発明の背景〕[Background of the invention]

イオン打込み転送路を有する磁気バブルメモリ素子にお
いて、従来、良好な特性を有するとされていた検出器は
、第1図に示すような非イオン打込み領域2,2′の上
に形成されたものである(なお、3は打込み領域を示す
。)なお、第1図の構成はT−J 、Ne1son他、
″イオン打込み転送路に用いるためのバブルデバイスエ
レメントの設計(Design of bubble 
device elements employing
ion implanシed propagat、io
n pat、erns)”、ベルシステムテクニカルジ
ャーナル(B ell S yst、emTechni
cal Journal) ff、59巻、@129頁
(1980)に記載されている。
In a magnetic bubble memory element having an ion-implanted transfer path, the detector that was conventionally considered to have good characteristics was one formed on the non-ion-implanted regions 2, 2' as shown in FIG. (The number 3 indicates the implantation area.) The configuration shown in FIG. 1 is based on T-J, Nelson et al.
``Design of bubble device element for use in ion implantation transfer path
device elements employing
ion implan seed propagat, io
Bell System Technical Journal
Cal Journal) ff, Vol. 59, p. 129 (1980).

読み出すための磁気バブル1は、メジャーライン6 (
Major Line)に沿って検出器に至る。磁気バ
ブル1が転送路の凹部A(カスプA)に到達したときA
uコンダクタからなる磁気バブル伸長器(Sヒretc
her)5によって磁気バブルlはストレッチャ5の溝
に沿って帯状に伸びる。帯状磁区が磁気抵抗効果素子か
らなる検出線4の下にくると検出線4の磁気抵抗が変化
し、磁気バブル(ここでは帯状磁区)が検出される。こ
こで、磁気バブルが帯状に伸びる検出領域2′は、いわ
ゆるハードバブル抑制のための浅いイオン打込み(50
〜10100nのみが行なわれている。第2図は、第1
図の検出器の断面構造を模式的に示したものである。同
図において、5in2膜などのスペーサ、8,8′は磁
化方向、9はハードバブル抑制層、10はガーネット膜
、1′は帯状磁区である。検出領域2′において磁気バ
ブル転送路を形成するような深いイオン打込み(磁気バ
ブルの膜厚の3/1o〜1/3程度)を行なわない理由
は、(1)磁気バブル(帯状磁区)1′と検出線4との
距離を近づけて検出感度の向上を図る、(ii)磁気バ
ブル1′の高さを出来るだけ大きく保ち、磁気バブル1
′の検出信号(磁気バブル1′からの漏洩磁界(str
ay  field))を強める等のためである。
The magnetic bubble 1 for reading is attached to the major line 6 (
Major Line) to the detector. When magnetic bubble 1 reaches recess A (cusp A) of the transfer path, A
Magnetic bubble expander (S Hiretc) consisting of U-conductor
her) 5 causes the magnetic bubbles l to extend in a band-like manner along the grooves of the stretcher 5. When a strip-shaped magnetic domain comes under a detection line 4 made of a magnetoresistive element, the magnetic resistance of the detection line 4 changes, and a magnetic bubble (here, a strip-shaped magnetic domain) is detected. Here, the detection region 2' where the magnetic bubbles extend in a band-like shape is formed by shallow ion implantation (50°C) to suppress so-called hard bubbles.
~10100n only. Figure 2 shows the first
It is a diagram schematically showing the cross-sectional structure of the detector shown in the figure. In the figure, a spacer such as a 5in2 film, 8 and 8' are magnetization directions, 9 is a hard bubble suppressing layer, 10 is a garnet film, and 1' is a strip-shaped magnetic domain. The reason why deep ion implantation (approximately 3/1 to 1/3 of the film thickness of the magnetic bubble) is not performed to form a magnetic bubble transfer path in the detection region 2' is as follows: (1) The magnetic bubble (strip magnetic domain) 1' (ii) Keep the height of the magnetic bubble 1' as large as possible, and
' detection signal (leakage magnetic field from magnetic bubble 1' (str
This is to strengthen the ay field).

しかし、本転送路における磁気バブル1の転送特性を詳
細に検討した結果、検出器の近傍で次のような転送の異
常を起しやすいことを見出した。
However, as a result of a detailed study of the transfer characteristics of the magnetic bubble 1 in this transfer path, it was found that the following transfer abnormality is likely to occur near the detector.

つまり、第3図(a)、 (b)において、(a)  
M気バブル1が検出器の中央のカスプAの手前のカスプ
Bまで転送して来た後、カスプAを素通りしてカスプC
に飛んで(スキップモード)しまうため磁気バブル1の
検出が出来ない(同図(a))。
In other words, in Figures 3(a) and (b), (a)
After M air bubble 1 is transferred to cusp B in front of cusp A in the center of the detector, it passes through cusp A and reaches cusp C.
The magnetic bubble 1 cannot be detected because the magnetic bubble 1 flies away (skip mode) (FIG. 4(a)).

(b)  磁気バブル1がカスプB、または、それより
も前のカスプに捕捉され(トラップモード)、その後の
磁気バブル1の転送が不能となる(同図(b)) 。
(b) The magnetic bubble 1 is captured by the cusp B or a cusp before it (trap mode), and subsequent transfer of the magnetic bubble 1 becomes impossible ((b) in the same figure).

などの不都合が生じ、何らかの改善が望まれていた。Such inconveniences arose, and some kind of improvement was desired.

〔発明の目的〕[Purpose of the invention]

したがって、本発明の目的は、上記したような磁気バブ
ル検出器の近傍において転送異常を生じない磁気バブル
転送路を有するイオン打込み型磁気バブルメモリ素子を
提供することにある。
Therefore, an object of the present invention is to provide an ion implantation type magnetic bubble memory element having a magnetic bubble transfer path that does not cause transfer abnormalities in the vicinity of the magnetic bubble detector as described above.

〔発明の概夏〕[Summer of invention]

本発明の要旨は、磁気バブルを転送するための凹部を有
する転送路からなる第1の非イオン打込み領域と、磁気
バブル検出器を形成するため上記転送路から直角に、か
つ、上記転送路に対して反対方向に設けら九た第2の非
イオン打込み領域とを儲え、上記第1の非イオン打込み
領域と上記第2の非イオン打込み領域とが接合する上記
第2の非イオン打込み領域部の端面が少なくとも上記磁
気バブル検出器に対応した上記転送路上の凹部と上記凹
部より1ビット手前の凹部との中間位置にあるように構
成されていることを特徴とするイオン打込み型磁気バブ
ルメモリ素子にある。
The gist of the invention is to provide a first non-ion implanted region consisting of a transfer path with a recess for transferring magnetic bubbles, and a first non-ion implanted region perpendicular to and on the transfer path for forming a magnetic bubble detector. a second non-ion implantation region provided in the opposite direction, and the second non-ion implantation region where the first non-ion implantation region and the second non-ion implantation region join together. An ion implantation type magnetic bubble memory characterized in that an end face of the portion is located at least at an intermediate position between a recess on the transfer path corresponding to the magnetic bubble detector and a recess 1 bit before the recess. It's in Motoko.

上記目的達成のためには、上記の転送異常の原因を追求
することが必要である。このため、イオン打込み型磁気
バブルメモリ素子において磁気バブルの駆動力となる特
殊磁壁(面内磁化層に形成さ九る磁極をもった磁壁、い
わゆる、チャージドウオール(charged  wa
ll))の挙動を詳細に検討した。第4図は、磁性流体
を試料表面に滴下してkn ?Xしたcharged 
 wallの様子を模式的に示だものである。検出器の
近傍において、charged  wal’l 11の
位相θ2 (回転磁界HRの方向に対するcharge
d  wall 11の位置)が他の転送路の位相θ、
よりも常に遅れることが判明した。この原因は、図の矢
印にM工。
In order to achieve the above objective, it is necessary to investigate the cause of the above transfer abnormality. For this reason, in an ion-implanted magnetic bubble memory element, a special domain wall (a domain wall with nine magnetic poles formed in an in-plane magnetization layer, so-called a charged wall) is used as a driving force for magnetic bubbles.
We investigated the behavior of ll)) in detail. In Figure 4, magnetic fluid is dropped onto the sample surface and kn? X charged
It schematically shows the state of the wall. In the vicinity of the detector, the phase θ2 of the charged wall 11 (the phase θ2 of the charged wall 11 relative to the direction of the rotating magnetic field HR
d wall 11 position) is the phase θ of the other transfer path,
It turns out that it always lags behind. The cause of this is the M-work indicated by the arrow in the figure.

M2で示した面内磁化の向き及び大きさが、検出器の近
傍と他の部分とで異なることにある。さらに詳しく述べ
ると、検出器の近傍では磁化M2の方向をとりにくいた
め、charged  wall 11の出現が他より
も遅れるのである。すなわち、検出器のための非イオン
打込み領域2′が、磁気バブル転送路6の背面に位置す
ることによって、この近傍におけるcharged  
wall 11の位相0□が他の位相0□よりも異なり
、上記した転送異?ニジ′をひき起すことになる。
The reason is that the direction and magnitude of in-plane magnetization indicated by M2 are different between the vicinity of the detector and other parts. More specifically, since it is difficult for the magnetization M2 to take the same direction near the detector, the appearance of the charged wall 11 is delayed compared to other areas. That is, by positioning the non-ion implantation region 2' for the detector on the back side of the magnetic bubble transfer path 6, the charged
Is the phase 0□ of wall 11 different from the other phases 0□ and the above transfer difference? This will cause a problem.

したがって、転送異常を改善するためには、検1出器部
での非イオン打込み層をなくすのが最もよい。しかし、
従来技術の項で述べたように、検出出力の向上のために
は非イオン打込み層が必要である。そこで、本発明にお
いては、非イオン打込み層の存在を認めたうえで、磁気
バブルの検出に支障がなく、かつ、転送異常の生じない
磁気バブルの転送路を提供するものである。
Therefore, in order to improve the transfer abnormality, it is best to eliminate the non-ion implanted layer in the detector section. but,
As mentioned in the prior art section, a non-ion implanted layer is necessary to improve the detection output. Therefore, the present invention recognizes the existence of the non-ion implanted layer and provides a magnetic bubble transfer path that does not impede detection of magnetic bubbles and does not cause transfer abnormalities.

〔発明の実施例〕[Embodiments of the invention]

以下、本発明を実施例を参照して詳細に説明する。 Hereinafter, the present invention will be explained in detail with reference to Examples.

第5図(a)〜(f)は、いずれも上記転送異常を改善
するために発明されたイオン打込み型磁気バブルメモリ
素子における検出器の近傍でのイオン打込み転送路の実
施例である6同図(a)は、磁気バブルを検出すべきカ
スプAよリービット手前のカスプBから磁気バブルがカ
スプAに移る過程において、転送路6の背面の非イオン
打込みM2’ を除いてカスプB→カスプAにおけるc
hargedwallの形成を容易ならしめ、磁気バブ
ルを首尾よく検出場所、つまり、カスプAに到達させる
ようにしたものである。同図(b)は、非イオン打込み
層2′の幅を転送路6に近づくにしたがって徐々に狭く
した実施例、同図(C)は非イオン打込み層2′の幅を
一様に狭くした実施例、同図(d)は検出器の非イオン
打込みJ″!:12′を転送路6の非イオン打込み層2
から隔離させた実施例、同図(e)は、転送路6の背面
にも磁気バブル転送路6′を形成した実施例、そして、
同図(f)は検出器の近傍における磁気バブル転送路6
の同期を他の部分のそ、1シよりも長くし、相対的に検
出器部分の幅を狭くしたものである。なお、第5図(a
) 、 (b) 、 (c) 。
5(a) to 5(f) are examples of the ion implantation transfer path near the detector in the ion implantation type magnetic bubble memory device invented to improve the above-mentioned transfer abnormality. Figure (a) shows that in the process of a magnetic bubble moving from cusp A, where a magnetic bubble is to be detected, from cusp B, which is in front of Leavitt, to cusp A, from cusp B to cusp A, excluding the non-ion implantation M2' on the back side of transfer path 6. c in
This facilitates the formation of a harged wall and allows the magnetic bubble to successfully reach the detection location, that is, the cusp A. Figure (b) shows an example in which the width of the non-ion implanted layer 2' is gradually narrowed as it approaches the transfer path 6, and Figure (C) shows an example in which the width of the non-ion implanted layer 2' is uniformly narrowed. In the example, the figure (d) shows that the non-ion implantation J''!:12' of the detector is connected to the non-ion implantation layer 2 of the transfer path 6.
Figure (e) shows an example in which a magnetic bubble transfer path 6' is also formed on the back side of the transfer path 6, and
Figure (f) shows the magnetic bubble transfer path 6 near the detector.
The length of the synchronization is made longer than that of the other parts, and the width of the detector part is made relatively narrower. In addition, Fig. 5 (a
), (b), (c).

(e) 、 (f)において、非イオン打込み領域2と
接する非イオン打込み領域2′の接合部分はカスプAと
カスプBとの中間位置以上にその幅を狭めなければいけ
ない、これは中間位置未満程度の幅の狭めかたでは転送
異常を全(抑制できないことが確認されたことによる。
In (e) and (f), the width of the joint between the non-ion implanted region 2 and the non-ion implanted region 2' must be narrower than the intermediate position between cusp A and cusp B, which is less than the intermediate position. This is because it has been confirmed that it is not possible to completely suppress transfer abnormalities by narrowing the range.

中間位置以上ならば転送異常の抑制効果が得られ、同図
(d)に示したように全くなくしてもよい。ただし、こ
の場合は領域2と領域2′との間隔が余り大きくなると
磁気バブルの拡大に支障が生じるので好ましくない。上
記した第5図(a)〜(f)の転送パターンを用いた結
果。
If the position is above the intermediate position, the effect of suppressing transfer abnormalities can be obtained, and it may be completely eliminated as shown in FIG. 2(d). However, in this case, if the distance between region 2 and region 2' becomes too large, it is not preferable because it will hinder the expansion of the magnetic bubble. Results using the transfer patterns shown in FIGS. 5(a) to 5(f) above.

従来の検出器の近傍での磁気バブルの転送異常を極めて
顕著に抑制することができた。
We were able to significantly suppress the abnormal transfer of magnetic bubbles in the vicinity of conventional detectors.

〔発明の効果〕〔Effect of the invention〕

以上述べた如く、本発明によって検出器近傍における磁
気バブル転送路上の磁気バブルの転送異常を全く瑯消し
たイオン打込み型磁気バブルメモリ素子を提供できるよ
うになった。
As described above, according to the present invention, it has become possible to provide an ion implantation type magnetic bubble memory element that completely eliminates abnormal transfer of magnetic bubbles on a magnetic bubble transfer path in the vicinity of a detector.

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

第1図は従来のイオン打込み型磁気バブルメモリ素子に
おける検出器近傍の構成図、第2図は第1図における磁
気バブルメモリ素子の一断面図、第3図(a)、 (b
)は各々検出器近傍における転送異常を説明するための
模式図、第4図は本発明の詳細な説明するための模式図
、第5図(a)〜(f)は各々本発明によるイオン打込
み型磁気バブルメモリ素子における検出器近傍の実施例
の構成図である。 1・・・磁気バブル、2,2′・・・非イオン打込み領
域、3・・・イオン打込み領域、4・・・検出線、5・
・・ストレッチャ、6・・・転送路、7・・・スペーサ
、8.8’ 、1’2・・・磁化方向、9・・・ハード
バブル抑制層、10・・・ガーネット膜、11・・・チ
ャージドウオール、A、B、C・・・カスプ、0□、θ
2・・・位相角、ト11□・・・回転磁界。 WJ 3  図 第 4 (2) 2′ (α) (e) ■ (b> C子)
Figure 1 is a block diagram of the vicinity of the detector in a conventional ion implantation type magnetic bubble memory element, Figure 2 is a sectional view of the magnetic bubble memory element in Figure 1, and Figures 3 (a) and (b).
) are schematic diagrams for explaining transfer abnormalities in the vicinity of the detector, FIG. 4 is a schematic diagram for explaining the present invention in detail, and FIGS. 5(a) to (f) are schematic diagrams for explaining the ion implantation according to the present invention, respectively. FIG. 2 is a configuration diagram of an embodiment near a detector in a type magnetic bubble memory element. DESCRIPTION OF SYMBOLS 1... Magnetic bubble, 2, 2'... Non-ion implantation area, 3... Ion implantation area, 4... Detection line, 5...
...Stretcher, 6...Transfer path, 7...Spacer, 8.8', 1'2...Magnetization direction, 9...Hard bubble suppression layer, 10...Garnet film, 11...・Charged wall, A, B, C...cusp, 0□, θ
2...Phase angle, 11□...Rotating magnetic field. WJ 3 Figure 4 (2) 2' (α) (e) ■ (b>C child)

Claims (1)

【特許請求の範囲】[Claims] 1、磁気バブルを転送するための凹部を有する転送路か
らなる第1の非イオン打込み領域と、磁気バブル検出器
を形成するため上記転送路から直角に、かつ、上記転送
路に対して反対方向に設けられた第2の非イオン打込み
領域とを備え、上記第1の非イオン打込み領域と上記第
2の非イオン打込み領域とが接合する上記第2の非イオ
ン打込み領域部の端面が少なくとも上記磁気バブル検出
器に対応した上記転送路上の凹部と上記凹部より1ビッ
ト手前の凹部との中間位置にあるように構成されている
ことを特徴とするイオン打込み型磁気バブルメモリ素子
1. A first non-ion implantation region consisting of a transfer path having a recess for transferring magnetic bubbles, and a first non-ion implantation region perpendicular to and in the opposite direction from the transfer path to form a magnetic bubble detector; a second non-ion implantation region provided in the second non-ion implantation region, the end face of the second non-ion implantation region where the first non-ion implantation region and the second non-ion implantation region are joined to at least the second non-ion implantation region; An ion implantation type magnetic bubble memory element, characterized in that it is configured to be located at an intermediate position between a recess on the transfer path corresponding to a magnetic bubble detector and a recess 1 bit before the recess.
JP60137718A 1985-06-26 1985-06-26 Ion implantation type magnetic bubble memory element Pending JPS6145487A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60137718A JPS6145487A (en) 1985-06-26 1985-06-26 Ion implantation type magnetic bubble memory element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60137718A JPS6145487A (en) 1985-06-26 1985-06-26 Ion implantation type magnetic bubble memory element

Publications (1)

Publication Number Publication Date
JPS6145487A true JPS6145487A (en) 1986-03-05

Family

ID=15205198

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60137718A Pending JPS6145487A (en) 1985-06-26 1985-06-26 Ion implantation type magnetic bubble memory element

Country Status (1)

Country Link
JP (1) JPS6145487A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5612009A (en) * 1991-08-29 1997-03-18 Basf Aktiengesellschaft Catalytic decomposition of dinitrogen monoxide

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5612009A (en) * 1991-08-29 1997-03-18 Basf Aktiengesellschaft Catalytic decomposition of dinitrogen monoxide

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