JPS6043584B2 - magnetic bubble element - Google Patents

magnetic bubble element

Info

Publication number
JPS6043584B2
JPS6043584B2 JP6365478A JP6365478A JPS6043584B2 JP S6043584 B2 JPS6043584 B2 JP S6043584B2 JP 6365478 A JP6365478 A JP 6365478A JP 6365478 A JP6365478 A JP 6365478A JP S6043584 B2 JPS6043584 B2 JP S6043584B2
Authority
JP
Japan
Prior art keywords
bubble
magnetic
magnetic bubble
shape
magnetic field
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
JP6365478A
Other languages
Japanese (ja)
Other versions
JPS54154940A (en
Inventor
久雄 松寺
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.)
NEC Corp
Original Assignee
Nippon Electric Co 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP6365478A priority Critical patent/JPS6043584B2/en
Publication of JPS54154940A publication Critical patent/JPS54154940A/en
Publication of JPS6043584B2 publication Critical patent/JPS6043584B2/en
Expired legal-status Critical Current

Links

Description

【発明の詳細な説明】 本発明はバブルラテイス構造の磁気バブル素子に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic bubble element having a bubble lattice structure.

近年磁気バブル素子はより高密度化のために種々の開
発研究がなされている。
In recent years, various research and development efforts have been made to increase the density of magnetic bubble elements.

その結果、同じ磁気バブルドメイン(以下バブル)のサ
イズでより高密度な磁気バブル素子としてバブルラテイ
スが提唱された(工・アイ・ピー・コンファレンス・プ
ロソーディング(AIPC0nf、Pr()C、)第2
4号第617〜619ページ(1975lf−)参照)
。 バブル、ラテイスのアクセス法は、当初電流による
方法が提唱されたが、最近、回転磁場による方法が提唱
されている(アプライド・フイジクス、レターズ(Ap
pl、Phys、Letters)第2捲第3号第16
6頁(197時)参照)。 これ等バブルラテイス構造
を有する磁気バブル素子はバブルの磁壁状態の違い(即
ち5=1あるいは5=0)によりコーディングする特徴
がある。
As a result, bubble latex was proposed as a higher density magnetic bubble element with the same magnetic bubble domain (hereinafter referred to as bubble) size (Institute of Engineering, IP Conference Proceedings (AIPC0nf, Pr()C,) 2nd
(See No. 4, pages 617-619 (1975lf-))
. Initially, a method using electric current was proposed to access bubbles and lattice, but recently a method using rotating magnetic fields has been proposed (Applied Physics, Letters).
pl, Phys, Letters) Volume 2, No. 3, No. 16
(See page 6 (197 hours)). These magnetic bubble elements having a bubble lattice structure are characterized by coding depending on the domain wall state of the bubble (ie, 5=1 or 5=0).

しカルバブルラテイスを用いた磁気バブル素子では、
その情報の読み出し機構に実用に適うものはまだ見出さ
れていない。
In the magnetic bubble element using carbubble lattice,
A practically applicable mechanism for reading out this information has not yet been found.

唯一の方法はバブルの磁壁状態の差により、磁場勾配
に対するバブルの移動方向の偏り角θがsinθ=85
V/γdΔH2(但し、Sは、バブル磁壁のステート、
Vはバブルの速度、γはジヤイロマグネテイツク・レシ
オ、dはバブル径、Δルはバブル径の間のバイアス磁場
勾配)に従つて異なることを利用することが提唱されて
いるのみである。
The only way is that the deflection angle θ of the moving direction of the bubble with respect to the magnetic field gradient is sin θ = 85 due to the difference in the domain wall state of the bubble.
V/γdΔH2 (where S is the state of the bubble domain wall,
It has only been proposed to utilize the fact that V is the velocity of the bubble, γ is the gyromagnetic ratio, d is the bubble diameter, and ΔL is the bias magnetic field gradient between the bubble diameters. .

本発明の目的は、バブルラテイス構造、わけても駆動
回転磁場によりアクセスするバブルラテイスにおいて新
規のすぐれた情報読み出し機構を有する磁気バブル素子
を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a magnetic bubble element having a new and superior information readout mechanism in a bubble lattice structure, particularly in a bubble lattice accessed by a driving rotating magnetic field.

即ち、バブル磁壁状態の差によつて、磁場勾配方向に対
するバブルの偏り角θが異なることにより、バイアス磁
場の転送可能領域に差が生じることを利用し、S=0バ
ブルでは正常に転送されるがS=1バブルでは消滅する
ようにすれば、以後の状態では情報はバルブの有無によ
つて読み出しができることを用いた素子を提案するもの
である。さらに具体的に表現すれば、本発明はバブルの
磁壁状態がS=1の時にバイアス磁場のバブル転送可能
領域がS=0状態に比較して小さく、高バイアス磁場で
はやく消滅し、バブル磁壁状態がS=1あるいはS=0
のいずれであるかを明瞭に識別検出しうる機構を有する
磁気バブル素子を得んとするものである。駆動回転磁場
によつて磁気バブルを転送させる場合、バブル支持膜、
すなわちバブルを保持するガーネット等の磁性材料から
適当な間隔をもつて軟磁性体(パーマロイが良く使用さ
れる)による転送路(以下パターンと称する)を設け、
駆動回転磁場によりこのパターンに誘起する磁荷により
バブルを転送させる。
In other words, by utilizing the fact that the deflection angle θ of the bubble with respect to the magnetic field gradient direction differs due to the difference in the bubble domain wall state, a difference occurs in the transferable region of the bias magnetic field, and the transfer is performed normally in the S=0 bubble. We propose an element that takes advantage of the fact that if S=1 bubble is made to disappear, information can be read out in subsequent states depending on the presence or absence of the valve. More specifically, the present invention provides that when the bubble domain wall state is S = 1, the bubble transferable region of the bias magnetic field is smaller than in the S = 0 state, and disappears quickly in a high bias magnetic field, and the bubble domain wall state is is S=1 or S=0
The object of the present invention is to obtain a magnetic bubble element that has a mechanism that can clearly identify and detect which of the following is the case. When a magnetic bubble is transferred by a driving rotating magnetic field, a bubble supporting film,
In other words, a transfer path (hereinafter referred to as a pattern) made of soft magnetic material (permalloy is often used) is provided at an appropriate distance from the magnetic material such as garnet that holds the bubble.
The magnetic charges induced in this pattern by the driving rotating magnetic field cause the bubbles to be transferred.

パターンの形状には色々なものが提唱されているが、バ
ブル磁壁状態がS=1で磁場勾配に対するバブル進行方
向の偏りがある時、この偏りがバブルの進行方向に対し
て時計方向か反時計方向かで、この偏りに対する安定度
に、パターンの形状により、その程度は異なるが、差が
生じることを一発見した。
Various patterns have been proposed for the shape of the pattern, but when the bubble domain wall state is S = 1 and there is a bias in the bubble traveling direction with respect to the magnetic field gradient, this bias is either clockwise or counterclockwise with respect to the bubble traveling direction. We have discovered that the stability against this bias differs depending on the direction, although the degree varies depending on the shape of the pattern.

即ち、バイアス磁場の向きが手前に向くよう眺めた時、
駆動回転磁場の回転方向を反時計回りにした時は、S=
1状態のバブルの偏りに対しても安定であるが、駆動回
転磁場の回転方向を時計回.りにした時はS=1状態の
バブルの偏りに対し安定でなくなり、特にバイアス磁場
を高くして、バブル径が小さくなつた時、S=1バブル
は、はやく消滅する。
In other words, when viewed so that the direction of the bias magnetic field is facing you,
When the rotation direction of the driving rotating magnetic field is counterclockwise, S=
It is stable even against the deviation of a bubble in one state, but if the rotation direction of the driving rotating magnetic field is rotated clockwise. When the bias is increased, the S=1 bubble becomes unstable with respect to the bias of the bubble, and especially when the bias magnetic field is increased and the bubble diameter becomes small, the S=1 bubble disappears quickly.

このような効果は特に、第1図のようなY字形(状1、
U字形状2、V字形状3、X字形状4あるいはU字の底
に突起をつけた形状5等のパターンで顕著である。
This effect is especially noticeable in the Y-shape (shape 1,
This is noticeable in patterns such as a U-shape 2, a V-shape 3, an X-shape 4, or a shape 5 in which a protrusion is added to the bottom of a U-shape.

本発明はこの効果を利用したもので、バブル検出機構に
上記のような形状のパターンの転送路を設け、駆動回転
磁場の向きを、バイアス磁場の方向が手前に向くよう眺
めた時、時計回りに回転するように設計し、バイアス磁
場を適当な値に設定し、磁壁状態がS=1バブルはこの
パターン転送中に消滅し、S=0バブルは正常に転送さ
れ、バブル磁壁状態がS=1か0かをバブルの無か有か
で識別、検出するようになされている。
The present invention takes advantage of this effect by providing the bubble detection mechanism with a transfer path having a pattern as described above, and changing the direction of the driving rotating magnetic field clockwise when viewed so that the direction of the bias magnetic field faces toward you. By setting the bias magnetic field to an appropriate value, bubbles with domain wall state S = 1 will disappear during this pattern transfer, bubbles S = 0 will be transferred normally, and bubble domain wall state will become S = 1 or 0 is identified and detected based on the absence or presence of bubbles.

本発明を実施例によつて更に詳細に説明する。The present invention will be explained in more detail by way of examples.

ノ第2図は(YSnlLuCa)3(GeFe)501
。(h=3.28μM,l=0.44μM,4πm=2
89GaL!SO)のバブル支持膜上にハードバブル抑
制のため800AのYIG膜を接して成長させたものに
、Y字形状パターンを有するバブル磁壁状態検出機構を
1.5μm−のスペーシングを介して設け、370KH
zで駆動した場合の、S=1及びS=0状態のバブルの
駆動可能領域を示したものである。図中斜線部がS=0
バブルのみが駆動可能でS=1バブルは消滅してバブル
磁壁状態が検出可能な領域である。第3図は、250e
,370KHzの駆動回転磁場でのバブル磁壁状態検出
可能領域を示したもので、スペーシングが1.5μm以
上では50e以上のマージンを有し、スペーシング2.
1μmでは70eのマージンを有する。第4図は本発明
のバブル素子の検出機構の一実施例である。
Figure 2 shows (YSnlLuCa)3(GeFe)501
. (h=3.28μM, l=0.44μM, 4πm=2
89GaL! A YIG film of 800 A was grown in contact with the bubble support film of SO) to suppress hard bubbles, and a bubble domain wall state detection mechanism having a Y-shaped pattern was provided with a spacing of 1.5 μm. 370KH
This figure shows the drivable region of the bubble in the S=1 and S=0 states when driven by z. The shaded area in the diagram is S=0
This is a region where only bubbles can be driven, S=1 bubbles disappear, and the bubble domain wall state can be detected. Figure 3 shows 250e
, 370 KHz drive rotating magnetic field shows the bubble domain wall state detectable region, where the spacing is 1.5 μm or more, there is a margin of 50 e or more, and the spacing 2.5 μm or more has a margin of 50 e or more.
At 1 μm, there is a margin of 70e. FIG. 4 shows an embodiment of the bubble element detection mechanism of the present invention.

パーマロイパターンとガーネットからなるバブル支持層
の間隔は1.8μmでバブルのストレージ領域6から検
出部に向つて送られたバブルは、バイアス磁場の方向が
手前に向くように眺めたとき時計方向に回転する駆動回
転磁場でY字形状パターンの転送路8を転送される間に
第2図で説明したようにS=1バブルは消滅し、S=0
バブルのみがストレッチャー部9に転送され、従来のパ
ーマロイの磁気抵抗効果を用いた検出器10によりS=
Oバブルが出力信号として検出される。したがつてS=
1バブルは検出出力が0として識別される。上記検出部
の転送路8の形状がY字形状以外の例えば■字形状、U
字形状ないしはX字形状等の場合も同様な結果を得るこ
とができる。以上説明した如く、本発明によつてフイー
ルドアクセスバブルラテイス構成のための有効な検出機
構を有する磁気バブル素子が得られる。
The interval between the permalloy pattern and the bubble support layer made of garnet is 1.8 μm, and the bubbles sent from the bubble storage area 6 toward the detection unit rotate clockwise when viewed with the direction of the bias magnetic field facing you. As explained in FIG. 2, the S=1 bubble disappears while being transferred through the transfer path 8 of the Y-shaped pattern by the driving rotating magnetic field, and the S=0 bubble disappears.
Only the bubbles are transferred to the stretcher section 9, and S=
O-bubble is detected as an output signal. Therefore S=
One bubble is identified as having a detection output of 0. The shape of the transfer path 8 of the detection unit is other than Y-shape, for example, ■-shape, U-shape, etc.
Similar results can be obtained in the case of a letter shape or an X shape. As described above, the present invention provides a magnetic bubble element having an effective detection mechanism for a field access bubble lattice configuration.

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

第1図は本発明における検出機構の転送路で用いられる
パターン形状の幾つかの例を示す図。 第2図は本発明の一実施例の作用を説明する図で、バブ
ル磁壁状態検出機構の正常駆動可能領域を示したもので
斜線部が磁壁状態検出可能領域である。第3図も同実施
例の作用を説明する図で、回転磁場を260eに固定し
、上記磁壁状態検出機構とバブル支持層のスペーシング
をかえた場合の磁壁状態検出可能領域(斜線部)を示し
たものである。第4図は本発明に用いる検出機構の一実
施例を示す路線図である。1・・・Y字形状パターン、
2・・・U字形状パターン、3・・・■字形状パターン
、4・・・X字形状パターン、5・・・U字の底に突起
のある形状のパターン、6・・・ストレージ領域、7・
・・バブル進行方向、8・・・転送路、9・・・ストレ
ッチャー部、10・・・検出器。
FIG. 1 is a diagram showing some examples of pattern shapes used in the transfer path of the detection mechanism in the present invention. FIG. 2 is a diagram illustrating the operation of an embodiment of the present invention, and shows a normally drivable region of the bubble domain wall state detection mechanism, with the shaded area being the domain wall state detectable region. FIG. 3 is also a diagram illustrating the operation of the same embodiment, and shows the domain wall state detectable region (shaded area) when the rotating magnetic field is fixed at 260e and the spacing of the domain wall state detection mechanism and bubble support layer is changed. This is what is shown. FIG. 4 is a route map showing one embodiment of the detection mechanism used in the present invention. 1...Y-shaped pattern,
2... U-shaped pattern, 3... ■-shaped pattern, 4... X-shaped pattern, 5... U-shaped pattern with a protrusion at the bottom, 6... Storage area, 7.
... Bubble traveling direction, 8... Transfer path, 9... Stretcher section, 10... Detector.

Claims (1)

【特許請求の範囲】 1 磁気バブルドメインを保持する磁性材料上に設けら
れた、面内駆動回転磁場によつて磁気バブルドメインを
転送させ得る機構を有する磁気バブル素子において、バ
イアス磁場を所定強度に設定し、S=1バブルは消滅せ
しめるがS=0バブルは残存せしめることにより、磁気
バブルドメインの磁壁状態を検出する機構を有すること
を特徴とする磁気バブル素子。 2 磁気バブルドメインの磁壁状態を検出する機構はY
字形状、U字形状、V字形状、X字形状あるいはU字の
底に突起がついた形状等の軟磁性膜を有してなる特許請
求の範囲第1項記載の磁気バブル素子。 3 磁気バブルドメインの磁壁状態を検出する機構にお
いてはバイアス磁場の方向が手前に向かうよう眺めた時
、駆動回転磁場の回転方向は時計回りである特許請求の
範囲第1項記載の磁気バブル素子。 4 磁気バブルドメインの磁壁状態を検出する機構と磁
気バブルドメインを保持する磁性材料との間隔が1.5
μm以上である特許請求の範囲第1項記載の磁気バブル
素子。
[Claims] 1. In a magnetic bubble element that is provided on a magnetic material holding magnetic bubble domains and has a mechanism capable of transferring magnetic bubble domains by an in-plane driving rotating magnetic field, a bias magnetic field is set to a predetermined intensity. 1. A magnetic bubble element having a mechanism for detecting a domain wall state of a magnetic bubble domain by setting S=1 bubbles to disappear but allowing S=0 bubbles to remain. 2 The mechanism for detecting the domain wall state of magnetic bubble domains is Y
The magnetic bubble element according to claim 1, comprising a soft magnetic film having a shape such as a U-shape, a V-shape, an X-shape, or a U-shape with a protrusion at the bottom. 3. The magnetic bubble element according to claim 1, wherein in the mechanism for detecting the domain wall state of the magnetic bubble domain, the direction of rotation of the drive rotating magnetic field is clockwise when viewed so that the direction of the bias magnetic field is directed toward the front. 4 The distance between the mechanism that detects the domain wall state of the magnetic bubble domain and the magnetic material that holds the magnetic bubble domain is 1.5
The magnetic bubble element according to claim 1, which has a diameter of μm or more.
JP6365478A 1978-05-26 1978-05-26 magnetic bubble element Expired JPS6043584B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6365478A JPS6043584B2 (en) 1978-05-26 1978-05-26 magnetic bubble element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6365478A JPS6043584B2 (en) 1978-05-26 1978-05-26 magnetic bubble element

Publications (2)

Publication Number Publication Date
JPS54154940A JPS54154940A (en) 1979-12-06
JPS6043584B2 true JPS6043584B2 (en) 1985-09-28

Family

ID=13235542

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6365478A Expired JPS6043584B2 (en) 1978-05-26 1978-05-26 magnetic bubble element

Country Status (1)

Country Link
JP (1) JPS6043584B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5760583A (en) * 1980-09-26 1982-04-12 Nec Corp Discriminating method for magnetic wall of bubble

Also Published As

Publication number Publication date
JPS54154940A (en) 1979-12-06

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