JPS60242578A - Composite magnetic bubble memory element - Google Patents

Composite magnetic bubble memory element

Info

Publication number
JPS60242578A
JPS60242578A JP9645284A JP9645284A JPS60242578A JP S60242578 A JPS60242578 A JP S60242578A JP 9645284 A JP9645284 A JP 9645284A JP 9645284 A JP9645284 A JP 9645284A JP S60242578 A JPS60242578 A JP S60242578A
Authority
JP
Japan
Prior art keywords
transfer path
ion implantation
magnetic field
range
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
JP9645284A
Other languages
Japanese (ja)
Inventor
Naoki Kodama
直樹 児玉
Makoto Suzuki
良 鈴木
Teruaki Takeuchi
輝明 竹内
Masatoshi Takeshita
正敏 竹下
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 JP9645284A priority Critical patent/JPS60242578A/en
Publication of JPS60242578A publication Critical patent/JPS60242578A/en
Pending 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)
  • Hall/Mr Elements (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は、イオン打込みによって形成された転送路と、
軟磁性体(たとえばNiとFeの合金で6るパーマロイ
)によって形成された転送路を1チツプ内に共存させた
複合型磁気バブルメモリ素子に関する。
[Detailed Description of the Invention] [Field of Application of the Invention] The present invention provides a transfer path formed by ion implantation,
The present invention relates to a composite magnetic bubble memory element in which a transfer path formed by a soft magnetic material (for example, permalloy made of an alloy of Ni and Fe) coexists within one chip.

〔発明の背景〕[Background of the invention]

磁気バブルメモリ素子において、高密度、高集化および
完全不揮発性を保証したメモリを作成するために、イオ
ン打込みにより形成した転送路(以下、イオン打込み転
送路と略す)と、軟磁性体を用いた転送路(以下、パー
マロイ転送路と略す)を複合化した素子が提案されてい
る(!!ff開昭57−40791号公報)。これは高
密度化に容易イオン打込み転送路を用いて情報の蓄積部
分を形成し、パーマロイ転送路を用いて情報の書き込み
、読み出し等の機能部を形成したメモリ素子である。
In order to create a memory that guarantees high density, high integration, and complete non-volatility in magnetic bubble memory elements, we use a transfer path formed by ion implantation (hereinafter referred to as ion implantation transfer path) and a soft magnetic material. An element in which a conventional transfer path (hereinafter abbreviated as permalloy transfer path) is combined has been proposed (!!ff Patent Publication No. 57-40791). This is a memory element in which an information storage section is formed using an ion implantation transfer path that facilitates high density, and a functional section for writing and reading information is formed using a permalloy transfer path.

この素子では、イオン打込み転送路とパーマロイ転送路
との接続部が必要である。第1図は、本発明者等が用い
た従来の接続部付近を示したものである。第1図の右側
の部分はイオン打込み転送路3からパーマロイ転送路へ
の接続部であシ、に側の部分はパーマロイ転送路からイ
オン打込み転送路3への接続部であシ、磁気バブルは転
送方向を示す矢印5の方向に転送する。面内に印加する
回転磁界6の方向が、第1図の7の範囲にある場合、接
続部に用いた軟磁性体素片1の端部に最も近いイオン打
込み転送路の凹部4に磁気バブルが存在することになる
。このときイオン打込み転送路の凹部4に近い方の軟磁
性体素片1の端部には、磁気バブルを反発する磁極が発
生している。そのためイオン打込み転送路の凹部4にあ
る磁気バブルが存在できるバイアス磁界の上限値が減少
してしまい、接続部から十分能れたイオン打込み転送路
において磁気バブルが存在できるバイアス磁界の範囲よ
りせまくなってしまう問題が生じた。
This device requires a connection between the ion implantation transfer path and the permalloy transfer path. FIG. 1 shows the vicinity of a conventional connection part used by the present inventors. The part on the right side of Figure 1 is the connection part from the ion implantation transfer path 3 to the permalloy transfer path, and the part on the right side is the connection part from the permalloy transfer path to the ion implantation transfer path 3. The data is transferred in the direction of arrow 5 indicating the transfer direction. When the direction of the rotating magnetic field 6 applied in-plane is within the range 7 in FIG. will exist. At this time, a magnetic pole that repels the magnetic bubble is generated at the end of the soft magnetic material piece 1 closer to the recess 4 of the ion implantation transfer path. As a result, the upper limit of the bias magnetic field in which the magnetic bubble in the concave portion 4 of the ion implantation transfer path can exist is reduced, and the range of the bias magnetic field is narrower than the range in which the magnetic bubble can exist in the ion implantation transfer path that is fully formed from the connection part. A problem arose.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、接続部に用いている軟磁性体素片に最
も近いところにあるイオン打込み転送路の凹部において
、磁気バブルが存在できるパイアン磁界の範囲を、前記
軟磁性体から十分能れたところにあるイオン打込み転送
路における磁気バブルが存在できるバイアス磁界の範囲
と同じかあるいは広くなるようにすることである。
An object of the present invention is to sufficiently control the range of the Paian magnetic field in which magnetic bubbles can exist in the concave portion of the ion implantation transfer path that is closest to the soft magnetic material piece used for the connection part. The objective is to make the range of the bias magnetic field the same as or wider than the range of the bias magnetic field in which a magnetic bubble can exist in the ion implantation transfer path.

〔発明の概要〕[Summary of the invention]

上記目的を達成するために、接続部に用いている軟磁性
体素片とそれに最も近いところにあるイオン打込み転送
路の凹部の底との距離をパラメータとして、凹部にある
磁気バブルが存在できるバイアス磁界の範囲をめ、最適
な位置関係を調べた。ここでパラメータは、第1図に示
すように軟磁性体素片の端とカスプ底を結んだ直線の膜
面内に射影した長さtである。
In order to achieve the above objective, the distance between the soft magnetic material piece used for the connection part and the bottom of the concave part of the ion implantation transfer path closest to it is set as a parameter, and a bias is applied so that the magnetic bubble in the concave part can exist. We determined the range of the magnetic field and investigated the optimal positional relationship. Here, the parameter is the length t projected into the film plane of a straight line connecting the end of the soft magnetic material piece and the bottom of the cusp, as shown in FIG.

第2図に実験結果を示す。縦軸はバイアス磁界の大きさ
であシ、横軸は前記パラメータt2磁気バブルの直径d
で割った値である。実験には、1μm径の磁気バブルを
用い、tは0μmから5μmまで変化させた。また比較
のために接続部から十分能れたところにあるイオン打込
み転送路において磁気バブルが存在できるバイアス磁界
の範囲の上限値と下限値を示しである。また図には、回
転磁界の大きさが6006と4006の場合が示しであ
る。これより回転磁界の大きさが600eの場合には、
t/dが2,7以上であれば、前記の目的を達成できる
ことがわかった。また回転磁界の大きさが500eの場
合には、t/dが2以上であれば前記の目的を達成でき
ることがわかった。
Figure 2 shows the experimental results. The vertical axis is the magnitude of the bias magnetic field, and the horizontal axis is the parameter t2, the diameter d of the magnetic bubble.
It is the value divided by In the experiment, a magnetic bubble with a diameter of 1 μm was used, and t was varied from 0 μm to 5 μm. For comparison, the upper and lower limits of the bias magnetic field range in which magnetic bubbles can exist in the ion implantation transfer path located at a sufficient distance from the connection portion are also shown. The figure also shows cases where the magnitude of the rotating magnetic field is 6006 and 4006. From this, when the magnitude of the rotating magnetic field is 600e,
It has been found that the above objective can be achieved if t/d is 2.7 or more. It was also found that when the magnitude of the rotating magnetic field is 500e, the above objective can be achieved if t/d is 2 or more.

回転磁界の大きさによって1/dの最低値が変化するの
は、回転磁界が大きくなると、軟磁性体素片にできる反
発磁極が強くなり、イオン打込み転送路の凹部にある磁
気バブルを消滅し易くしてしまうためである。
The reason that the minimum value of 1/d changes depending on the magnitude of the rotating magnetic field is that as the rotating magnetic field increases, the repelling magnetic poles formed in the soft magnetic material pieces become stronger, extinguishing the magnetic bubbles in the recesses of the ion implantation transfer path. This is to make it easier.

第3図は、t/dが0.1,2,3,4.5の場合の回
転磁界依存性を示したものである。縦軸はバイアス磁界
の大きさであシ、横軸は回転磁界の大きさである。磁気
バブルが存在できるバイアス磁界の範囲の下限値はt/
dによらないが、上限値はt/dと回転磁界の大きさに
よっていることがわかった。軟磁性体素片から十分能れ
たところにあるイオン打込み転送路において磁気バブル
が存在できるバイアス磁界の範囲は、回転磁界の大きさ
が250e以上で一定であム第3図の右端に示したもの
である。実験結果より、/、/d≧3であれば、回転磁
界の大きさによらず問題の凹部における磁気バブルの存
在できるバイアス磁界範囲の減少が少なく、イオン打込
み転送路において磁気バブルが存在できるバイアス磁界
範囲と同じかあるいはそれよりも広くできることがわか
った。
FIG. 3 shows the dependence on the rotating magnetic field when t/d is 0.1, 2, 3, and 4.5. The vertical axis represents the magnitude of the bias magnetic field, and the horizontal axis represents the magnitude of the rotating magnetic field. The lower limit of the bias magnetic field range in which magnetic bubbles can exist is t/
It was found that the upper limit value does not depend on d, but depends on t/d and the magnitude of the rotating magnetic field. The range of the bias magnetic field in which magnetic bubbles can exist in the ion implantation transfer path that is sufficiently far away from the soft magnetic material element is shown on the right side of Figure 3 when the magnitude of the rotating magnetic field is constant over 250 e. It is something. From the experimental results, if /, /d≧3, the bias magnetic field range in which magnetic bubbles can exist in the concave portion in question will decrease little, regardless of the magnitude of the rotating magnetic field, and the bias in which magnetic bubbles can exist in the ion implantation transfer path will be small. It turns out that it can be made as wide as or even wider than the magnetic field range.

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

以下、本発明の一実施例を第4図により説明する。接続
部に用いている軟磁性体素片の先端とそれに最も近いイ
オン打込み転送路の凹部の底4との距離の膜面内へ射影
した距離tk4μmとした場合を示している。この接続
部において凹部の底4付近にある磁気バブルの存在でき
るバイアス磁界の範囲を測定したところ、接続部から十
分能れたところのイオン打込み転送路における磁気バブ
ルの存在できるバイアス磁界の範囲に比べて、上限値は
606大きく、下限値は30e小さくなり、イオン打込
み転送路よシも広いバイアス磁界の範囲が得られた。
An embodiment of the present invention will be described below with reference to FIG. The case is shown in which the distance between the tip of the soft magnetic material piece used for the connection portion and the bottom 4 of the concave portion of the ion implantation transfer path closest to the tip is projected into the film plane and is tk 4 μm. When we measured the range of the bias magnetic field in which the magnetic bubbles near the bottom 4 of the recess can exist in this connection part, we found that it is compared to the range of the bias magnetic field in which the magnetic bubbles can exist in the ion implantation transfer path that is far enough from the connection part. Therefore, the upper limit value was increased by 606 and the lower limit value was decreased by 30e, and a wide bias magnetic field range was obtained in the ion implantation transfer path.

第5図も実施例の一つであり、第4図と同じくt−1(
4μmとした場合である。第4図に比べて、イオン打込
み領域の境界の位置を軟磁性体素片の先端近くに設けた
ものである。この場合も第4図と同じ効果があることが
わかった。
FIG. 5 is also one of the examples, and like FIG. 4, t-1(
This is a case where the thickness is 4 μm. Compared to FIG. 4, the boundary of the ion implantation region is located closer to the tip of the soft magnetic material piece. It was found that the same effect as in FIG. 4 was obtained in this case as well.

第6図、第7図も各々実施例の一つであり、イオン打込
み転送路から74−マロイ転送路への接続部を示したも
のである。第6図はt=4μmの場合、第7図はt=8
μmの場合を示しである。いずれも、イオン打込み転送
路の凹部の底4付近にある磁気バブルが存在できる)く
イアス磁界の範囲は、接続部から十分術れたところのイ
オン打込み転送路における磁気バブルが存在できるバイ
アス磁界の範囲よ)広く、上限値は606大きく、下限
値は30e小さいことがわかった。
FIGS. 6 and 7 are also examples, each showing a connection portion from the ion implantation transfer path to the 74-Malloy transfer path. Figure 6 shows t=4μm, Figure 7 shows t=8
The figure shows the case of μm. In both cases, the range of the bias magnetic field (where a magnetic bubble exists near the bottom 4 of the recess of the ion implantation transfer path) is the range of the bias magnetic field where a magnetic bubble can exist in the ion implantation transfer path sufficiently far from the connection. It was found that the range is wide, the upper limit is 606 larger, and the lower limit is 30e smaller.

同様に種々の場合で実験した結果、t/dが3以上であ
れば、接続部に最も近いイオン打込み転送路の凹部にあ
る磁気バブルの存在できるバイアス磁界範囲が、イオン
打込み転送路における磁気バブルの存在できるバイアス
磁界範囲よりせまくならないことがわかった。
Similarly, as a result of experiments in various cases, when t/d is 3 or more, the bias magnetic field range in which the magnetic bubble in the concave part of the ion implantation transfer path closest to the connection part can exist is the same as that of the magnetic bubble in the ion implantation transfer path. It was found that the bias magnetic field range is not narrower than the range in which the bias magnetic field can exist.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、接続部の軟磁性体素片に最も近いイオ
ン打込み転送路の凹部におる磁気バブルが、前記軟磁性
体素片に生じる反発磁極のために磁気バブルが存在でき
るバイアス磁界の範囲を減少させることなく、接続部か
ら十分術れたところにあるイオン打込み転送路にある磁
気バブルが存在できるバイアス磁界の範囲と同等か、あ
るいは広くすることができた。
According to the present invention, the magnetic bubble in the concave portion of the ion implantation transfer path closest to the soft magnetic material piece of the connection part is affected by the bias magnetic field in which the magnetic bubble can exist due to the repulsive magnetic pole generated in the soft magnetic material piece. Without reducing the range, it was possible to equal or increase the range of the bias field in which a magnetic bubble in the ion implant transfer path, located far enough from the connection, could exist.

本発明を直径1μm未満、015μm以上の磁気バブル
の場合に適用して実験したところ、1μm径の場合と同
様の効果があることがわかった。
When the present invention was applied to a magnetic bubble with a diameter of less than 1 μm and 0.15 μm or more, it was found that the same effect as in the case of a magnetic bubble with a diameter of 1 μm was obtained.

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

第1図はイオン打込み転送路にパーマロイ転送路との接
続部付近を示す平面図、第2図はd/lの値に対して磁
気バブルが存在できるバイアス磁界の範囲を示す図、第
3図は回転磁界の大きさに対して磁気バブルが存在でき
るバイアス磁界の範囲を示す図、第4図から第7図はそ
れぞれ本発明の実施例を示す図である。 1・・・軟磁性体素片、2・−・イオン打込み転送路形
成のためのイオン打込み領域、3・・・イオン打込み転
送路、4・・・イオン打込み転送路の凹部の底、5・・
・磁気バブルの転送方向、6・・・回転磁界、7・・・
回転磁界の方向。 第 1 図 第 3 口 看4 図 柘 5 図 第 6 図 第 7 図
Fig. 1 is a plan view showing the vicinity of the connection between the ion implantation transfer path and the permalloy transfer path, Fig. 2 is a view showing the range of bias magnetic field where magnetic bubbles can exist with respect to the value of d/l, and Fig. 3 1 is a diagram showing the range of a bias magnetic field in which a magnetic bubble can exist with respect to the magnitude of a rotating magnetic field, and FIGS. 4 to 7 are diagrams each showing an embodiment of the present invention. DESCRIPTION OF SYMBOLS 1... Soft magnetic material piece, 2... Ion implantation area for forming an ion implantation transfer path, 3... Ion implantation transfer path, 4... Bottom of recess of ion implantation transfer path, 5.・
・Transfer direction of magnetic bubble, 6... Rotating magnetic field, 7...
Direction of rotating magnetic field. Fig. 1 Fig. 3 Mouth observation Fig. 4 Fig. 5 Fig. 6 Fig. 7

Claims (1)

【特許請求の範囲】[Claims] イオン打込みによって形成された第1の転送路と軟磁性
体によって形成された第2の転送路とを1チツプ内に共
存させた複合型磁気バブルメモリ素子において、前記第
1の転送路から第2の転送路への接続部および第2の転
送路から第1の転送路への接続部で、第1の転送路に含
まれる転送路の凹部の底と、その底に最も近いところに
存在する第2の転送路に含まれる軟磁性体素片の先端の
うち該凹部底と最も近い先端との距離を磁気バブルを保
持する膜面内に射影した長さtが、磁気バブルの直径d
に対して、t/d>3の関係にあるように前記凹部の底
と前記軟磁性体素片を配置したことを特徴とする複合型
磁気バブルメモリ素子。
In a composite magnetic bubble memory element in which a first transfer path formed by ion implantation and a second transfer path formed by a soft magnetic material coexist in one chip, The connection part to the transfer path and the connection part from the second transfer path to the first transfer path, which exist at the bottom of the concave part of the transfer path included in the first transfer path and at the place closest to the bottom. The length t obtained by projecting the distance between the bottom of the recess and the tip closest to the tip of the soft magnetic material piece included in the second transfer path into the surface of the film that holds the magnetic bubble is the diameter d of the magnetic bubble.
, the bottom of the recess and the soft magnetic material piece are arranged so that t/d>3.
JP9645284A 1984-05-16 1984-05-16 Composite magnetic bubble memory element Pending JPS60242578A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9645284A JPS60242578A (en) 1984-05-16 1984-05-16 Composite magnetic bubble memory element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9645284A JPS60242578A (en) 1984-05-16 1984-05-16 Composite magnetic bubble memory element

Publications (1)

Publication Number Publication Date
JPS60242578A true JPS60242578A (en) 1985-12-02

Family

ID=14165406

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9645284A Pending JPS60242578A (en) 1984-05-16 1984-05-16 Composite magnetic bubble memory element

Country Status (1)

Country Link
JP (1) JPS60242578A (en)

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