JPS59172191A - Magnetic bubble transferring path - Google Patents

Magnetic bubble transferring path

Info

Publication number
JPS59172191A
JPS59172191A JP58045937A JP4593783A JPS59172191A JP S59172191 A JPS59172191 A JP S59172191A JP 58045937 A JP58045937 A JP 58045937A JP 4593783 A JP4593783 A JP 4593783A JP S59172191 A JPS59172191 A JP S59172191A
Authority
JP
Japan
Prior art keywords
magnetic field
magnetic bubble
magnetic
basic
transfer path
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
JP58045937A
Other languages
Japanese (ja)
Inventor
Minoru Hiroshima
実 広島
Shinzo Matsumoto
信三 松本
Mitsuru Sekino
充 関野
Masahiro Yanai
雅弘 箭内
Naoki Miyamoto
直樹 宮本
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 JP58045937A priority Critical patent/JPS59172191A/en
Publication of JPS59172191A publication Critical patent/JPS59172191A/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)

Abstract

PURPOSE:To obtain a sufficient bias magnetic field margin by triangular wave driving by obliquely setting the direction of the gap between basic patterns to a magnetic bubble transferring direction. CONSTITUTION:The direction Q of gaps (g) between each pattern 2 adjacently arranged is obliquely set to a magnetic bubble transferring direction P. When the oblique angle is designated by theta, a phase at which a rotary magnetic field 1 becomes minimum and another phase at which a magnetic bubble crosses the gap section (g) can be shifted by theta'. When the obliqud angle is set in a range of 5 deg.-30 deg., a sufficiently large bias magnetic field margin DELTAHB can be obtained. By obliquely setting the direction of the gaps between the basic patterns to the magnetic bubble transferring direction in this way, a sufficiently large bias magnetic field margin can be obtained by triangular wave driving even when the arranging cycle of the basic pattern is reduced.

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転送路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 transfer path.

〔発明の背景〕[Background of the invention]

近年、磁気バブル転送路としてはパーマロイ方式が主に
実用化されている。これはパーマロイ薄膜をエツチング
して形成したバタンを、該バタン面内で回転する外部か
ら加える磁界で磁化することによシ、磁気バブルを転送
する方式であシ、本発明はこの方式の転送路に関するも
のである。
In recent years, the permalloy method has mainly been put into practical use as a magnetic bubble transfer path. This is a method of transferring magnetic bubbles by magnetizing a batten formed by etching a permalloy thin film with an externally applied magnetic field that rotates within the batten plane.The present invention is directed to a transfer path using this method. It is related to.

第1図(a) 、 (b)はパーマロイ方式の磁気バブ
ル転送路の一例を示す要部拡大平面図である。同図にお
いて、外部回転磁界lが反時計回転するとき、磁気バブ
ルが右から左へ矢印P方向に転送する。
FIGS. 1(a) and 1(b) are enlarged plan views of essential parts showing an example of a permalloy magnetic bubble transfer path. In the figure, when the external rotating magnetic field l rotates counterclockwise, the magnetic bubbles are transferred from right to left in the direction of arrow P.

そして、回転磁界lが1回転すると、磁気バブルは基本
パタン2を18期分転送される。ここで同図(a) K
示す基本パタン2は非対称シェブロンバタン、同図(b
)はハーフディスクバタンと称され、両者共に近年では
広く用いられているバタンである。
Then, when the rotating magnetic field l rotates once, the magnetic bubble is transferred 18 periods of the basic pattern 2. Here, in the same figure (a) K
The basic pattern 2 shown is an asymmetrical chevron batten, shown in the same figure (b
) are called half-disc slams, and both are batans that have been widely used in recent years.

これらのバタンは、基本バタン2間のギャップ2部分の
方向Qが磁気バブル転送方向Pに対して直交して磁気バ
ブル転送路3を構成している。
These batons constitute a magnetic bubble transfer path 3 in which the direction Q of the gap 2 portion between the basic battens 2 is perpendicular to the magnetic bubble transfer direction P.

しかしながら、前記構成による磁気バブル転送路3は、
基本パタン2の磁気バブル転送特性が、バタンの配列周
期λを小さくしてゆくと、また外部回転磁界1の軌跡が
円形あるいは入角形ではなく同図に示す四角形の場合に
低下し、バイアス磁界マージンが減少するという問題が
あった。ここで、外部回転磁界lが円形の場合をサイン
波駆動。
However, the magnetic bubble transfer path 3 with the above configuration,
The magnetic bubble transfer characteristics of basic pattern 2 decrease as the batten arrangement period λ decreases, and when the locus of external rotating magnetic field 1 is square as shown in the figure rather than circular or diagonal, the bias magnetic field margin decreases. There was a problem that the number decreased. Here, when the external rotating magnetic field l is circular, sine wave driving is used.

六角形の場合を台形波駆動、四角形の場合を三角波駆動
と称している。
The hexagonal shape is called trapezoidal wave drive, and the square shape is called triangular wave drive.

〔発明の目的〕[Purpose of the invention]

したがって、本発明は前述した問題点に鑑みてなされた
ものであシ、その目的とするところは、基本パターンの
配列周期λを縮小しても、三角波駆動で充分なバイアス
磁界マージンが得られる磁気バブル転送路を補供するこ
とにある。
Therefore, the present invention has been made in view of the above-mentioned problems, and its purpose is to provide a magnetic field that can provide a sufficient bias magnetic field margin with triangular wave drive even if the arrangement period λ of the basic pattern is reduced. The purpose is to provide a bubble transfer path.

〔発明の概要〕[Summary of the invention]

このような目的を達成するために本発明は、基本パタン
間のギャップの方向を、磁気パズル転送方向に対して斜
交させたものである。
In order to achieve this object, the present invention makes the direction of the gap between basic patterns oblique to the magnetic puzzle transfer direction.

す々わち、パタンの配列周期λを縮小した基本パタンは
、三角波駆動の場合、バイアス磁界マージンが低下する
理由は、次のように考えられる。
In other words, the reason why the bias magnetic field margin of a basic pattern with a reduced pattern arrangement period λ decreases in the case of triangular wave driving is considered to be as follows.

すなわち第2図において、同図(a)はサイン波駆動。That is, in FIG. 2, (a) is a sine wave drive.

台形波駆動、三角波駆動の場合の回転磁界ベクトル)(
Hの軌跡の比較である。同図(a)に示すように三角波
駆動の場合の特徴は、回転磁界ベクトルHRの大きさが
45°方向のとき、最小となる点であシ、その大きさは
サイン波0台形波の場合に比べて1/v’2”に減小し
ている。他方、第21図(b)は磁気バブルを10 Q
KHz ”−200K)izで転送したときの転送回路
上の磁気バブルの位置と回転磁界lの方向との関係を示
した図である。同図によると、磁気バブルBの位置は回
転磁界lの方向に対して20″〜40°の範囲で位相が
遅れている。すなわち、同図(a)に示す回転磁界lの
方向が00,90°、270゜のとき、磁気バブルBは
同図(b)に示すようにそれぞれ20°遅れの磁気バブ
ルB1+ 110’遅れの磁気バブルB!1310”遅
れの磁気バブルB3となる。このうちで最も位相が遅れ
るのは、基本パタン2のギヤ212部を渡るときで磁気
バブルB3で示すように40″aIi遅れている。そし
て、バイアス磁界マージンを決めるのはこのギヤ212
部を渡るときである。このバイアス磁界マージンを決め
るところの磁気バブルがギャップgを渡るときの回転磁
界lの強度を大きくすべきであるのが、三角波、駆動の
場合は逆に40’程度の位相連れがあるため、最も小さ
な値の近傍になってしまう。これがバイアス磁界マージ
ンの低下の原因となっていた。
Rotating magnetic field vector for trapezoidal wave drive and triangular wave drive) (
This is a comparison of the trajectories of H. As shown in Figure (a), the characteristic of triangular wave drive is that when the magnitude of the rotating magnetic field vector HR is in the 45° direction, it becomes the minimum, and the magnitude is the same for a sine wave and a trapezoidal wave. On the other hand, Fig. 21(b) shows that the magnetic bubble is reduced to 1/v'2''.
This is a diagram showing the relationship between the position of the magnetic bubble on the transfer circuit and the direction of the rotating magnetic field l when data is transferred at KHz "-200K) iz. According to the figure, the position of the magnetic bubble B is in the direction of the rotating magnetic field l. The phase is delayed in the range of 20'' to 40° with respect to the direction. That is, when the directions of the rotating magnetic field l shown in Figure (a) are 00°, 90°, and 270°, magnetic bubble B is delayed by 20° as shown in Figure (b), and magnetic bubble B1 is delayed by 110', respectively. Magnetic bubble B! The magnetic bubble B3 is delayed by 1310''. Among these, the phase is delayed the most when it crosses the gear 212 portion of basic pattern 2, and as shown by the magnetic bubble B3, it is delayed by 40''aIi. This gear 212 determines the bias magnetic field margin.
It's time to cross departments. The strength of the rotating magnetic field l when the magnetic bubble crosses the gap g, which determines the bias magnetic field margin, should be increased, because in the case of triangular wave driving, on the contrary, there is a phase shift of about 40'. It ends up being close to a small value. This caused a decrease in the bias magnetic field margin.

したがって、本発明は、三角波駆動で回転磁界Haが最
小となる位相と、磁気バブルがギヤ212部を渡る位相
とが重ならないようにずらそうとするものである。
Therefore, the present invention attempts to shift the phase in which the rotating magnetic field Ha is minimized by triangular wave driving so that the phase in which the magnetic bubble crosses the gear 212 portion does not overlap.

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

次に図面を用いて本発明の実施例を詳細に説明する。 Next, embodiments of the present invention will be described in detail using the drawings.

第3@は本発明による磁気バブル転送路の実施例を示す
要部拡大平面図であり、同図(a)は非対称シェブロン
パタンを基本パタン2とした磁気バブル転送路、同図(
b)はハーフディスクパタンを基本パタン2とした磁気
バブル転送路である。これらの図において、隣接配置さ
れる基本パタン2の相互間のギャップgの方向Qが磁気
バブル転送方向Pに対して斜交している点に特徴がある
。このような構成において、斜交角をθにすれば、前記
回転磁界lが最小となる位相と、磁気バブルがギヤ21
2部を渡る位相をθ分ずらすことができる。
The third @ is an enlarged plan view of the main part showing an embodiment of the magnetic bubble transfer path according to the present invention, and FIG.
b) is a magnetic bubble transfer path in which the basic pattern 2 is a half-disk pattern. These figures are characterized in that the direction Q of the gap g between adjacent basic patterns 2 is oblique to the magnetic bubble transfer direction P. In such a configuration, if the oblique angle is set to θ, the rotational magnetic field l is at its minimum phase and the magnetic bubble is aligned with the gear 21.
The phase across the two parts can be shifted by θ.

第4図は斜交角θを各種変えたときのバイアス磁界マー
ジン幅ΔHnを実験的に求めた結果を示したもので砿)
シ、同図からqt+らかなように斜交角θを50S−3
06の範囲内に設定することによって、充分に大き々バ
イアス磁、界マージンΔHBを得ることができた。
Figure 4 shows the experimental results of the bias magnetic field margin width ΔHn when varying the oblique angle θ.
From the same figure, set the oblique angle θ to 50S-3 so that qt+ is smooth.
By setting within the range of 0.06, it was possible to obtain a sufficiently large bias field margin ΔHB.

なお、前述した実施例においては、基本パタンとして非
対称シェブロンパタン、ノ九−フディスクバタンを用い
た場合について説明したが、本発明はこれに限定される
ものではなく、前述したパタンの類似ないしは変形パタ
ンを用いても前述と全く同様の効果が得られることは勿
論である。
In addition, in the above-mentioned embodiment, a case was explained in which an asymmetrical chevron pattern and a nine-fold disk pattern were used as the basic pattern, but the present invention is not limited to this, and similar or modified patterns of the above-mentioned patterns are used. Of course, the same effect as described above can be obtained even if a pattern is used.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明によれば、基本バタン間のギ
ャップの方向を、磁気バブル転送方向に対して斜交させ
たことによって、基本パタンの配列周期を縮小しても三
角波駆動で充分大きなバイアス磁界マージンが得られる
という極めて優れた効果を有する。
As explained above, according to the present invention, by making the direction of the gap between the basic patterns oblique to the magnetic bubble transfer direction, even if the arrangement period of the basic pattern is reduced, a sufficiently large bias can be applied by triangular wave driving. This has an extremely excellent effect of providing a magnetic field margin.

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

第1図(a) 、 (b)は従来の磁気バブル転送路の
−例を示す要部拡大平面図、第2図(a) 、 (b)
は従来の磁気バブル転送路の問題点を説明するための図
、第3図(a) 、 (b)は本発明による磁気バブル
転送路の一例を示す要部拡大平面図、第4図は本発明に
よる磁気バブル転送路の効果を示す図である。 1・・・・回転磁界、2・・・・基本バタン、3・・・
・磁気バブル転送路。 7− 弔1反
FIGS. 1(a) and (b) are enlarged plan views of main parts showing an example of a conventional magnetic bubble transfer path, and FIGS. 2(a) and (b)
3(a) and 3(b) are enlarged plan views of essential parts showing an example of the magnetic bubble transfer path according to the present invention, and FIG. 4 is a diagram for explaining the problems of the conventional magnetic bubble transfer path. FIG. 3 is a diagram showing the effect of the magnetic bubble transfer path according to the invention. 1... Rotating magnetic field, 2... Basic slam, 3...
・Magnetic bubble transfer path. 7- Condolence 1 anti

Claims (1)

【特許請求の範囲】 1、 基本バタンを一定のギャップを介して複数配列し
て磁気バブルを転送させる磁気バブル転送路において、
前記基本バタン間のギャップの方向を、磁気バブルの転
送方向に対して斜交させたことを特徴とする磁気バブル
転送路。 2、前記斜交角度を5°〜30°の範Hに設定すること
を特徴とする特許請求の範囲第1項記載の磁気バブル転
送路。
[Claims] 1. A magnetic bubble transfer path that transfers magnetic bubbles by arranging a plurality of basic batons with a certain gap between them,
A magnetic bubble transfer path characterized in that the direction of the gap between the basic batons is oblique to the transfer direction of magnetic bubbles. 2. The magnetic bubble transfer path according to claim 1, wherein the oblique angle is set in a range H of 5° to 30°.
JP58045937A 1983-03-22 1983-03-22 Magnetic bubble transferring path Pending JPS59172191A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58045937A JPS59172191A (en) 1983-03-22 1983-03-22 Magnetic bubble transferring path

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58045937A JPS59172191A (en) 1983-03-22 1983-03-22 Magnetic bubble transferring path

Publications (1)

Publication Number Publication Date
JPS59172191A true JPS59172191A (en) 1984-09-28

Family

ID=12733183

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58045937A Pending JPS59172191A (en) 1983-03-22 1983-03-22 Magnetic bubble transferring path

Country Status (1)

Country Link
JP (1) JPS59172191A (en)

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