JPS5918788B2 - Magnetic bubble generation method - Google Patents

Magnetic bubble generation method

Info

Publication number
JPS5918788B2
JPS5918788B2 JP50017889A JP1788975A JPS5918788B2 JP S5918788 B2 JPS5918788 B2 JP S5918788B2 JP 50017889 A JP50017889 A JP 50017889A JP 1788975 A JP1788975 A JP 1788975A JP S5918788 B2 JPS5918788 B2 JP S5918788B2
Authority
JP
Japan
Prior art keywords
magnetic
pulse current
bubble
magnetic bubble
bubbles
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
JP50017889A
Other languages
Japanese (ja)
Other versions
JPS5193639A (en
Inventor
庄治 吉本
博文 太田
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 JP50017889A priority Critical patent/JPS5918788B2/en
Publication of JPS5193639A publication Critical patent/JPS5193639A/ja
Publication of JPS5918788B2 publication Critical patent/JPS5918788B2/en
Expired legal-status Critical Current

Links

Description

【発明の詳細な説明】 本発明は磁気バブル発生方式に関するものである。[Detailed description of the invention] The present invention relates to a magnetic bubble generation method.

一般に、磁気バブル装置は磁気バブルの発生および消去
を制御する機構、ついで磁気バブルを転送する機構、さ
らには磁気バブルを記憶する記憶ループ、最後に磁気バ
ブルの存在を検出してこれを電気信号として取り出す検
出機構を具備している。
In general, a magnetic bubble device has a mechanism that controls the generation and erasure of magnetic bubbles, a mechanism that transfers the magnetic bubbles, a memory loop that stores the magnetic bubbles, and finally a mechanism that detects the presence of magnetic bubbles and converts them into electrical signals. It is equipped with a detection mechanism for taking out the device.

本発明は特に上記磁気バブルを発生する機構に関するも
のである。一般に、オルソフェライトや磁性ガーネット
などの磁気バブル用の磁気バブルメモリチップ中に磁気
バブルを発生するバブル発生器は大別してディスク型と
ヘアピンコンダクタ型に分けられ、後者のものは、小さ
なループ状のヘアピンコンダクタを磁性薄板上にフォト
エッチングなどで作成Lこのヘアピンコンダクタに振幅
の比較的大きいパルス電流を流して強い磁界を作ること
により磁気バブルを形成するものである。
The present invention particularly relates to a mechanism for generating the above-mentioned magnetic bubbles. In general, bubble generators that generate magnetic bubbles in magnetic bubble memory chips for magnetic bubbles such as orthoferrite and magnetic garnet can be roughly divided into disk type and hairpin conductor type. A conductor is created on a magnetic thin plate by photo-etching or the like.A magnetic bubble is formed by passing a pulse current with a relatively large amplitude through this hairpin conductor to create a strong magnetic field.

この場合、上記ヘアピンコンダクタに流れる電流により
得られる磁界は核発生磁界HN(Nucleation
Fie1d)をこえなければならない。上記核発生磁界
HNの大きさはほぼ異方性磁界HKに等しく、この値は
ほぼ″20000e程度の大きさを有している。上記異
方性磁界HKはバブル径が小さい程大きくなり、また温
度が上昇するにつれて小さくなる傾向がある。一方、磁
気バブルを記憶する記憶ループのビット密度を上げるに
は磁気バブルの径を小さくしなければならないことが知
られているが、このようにその径を小さくするとそれに
伴なつて上記核発生磁界HNが大きくなり上記ヘアピン
コンダクタに供給するパルス電流の振幅を大きく設定し
なければならない。
In this case, the magnetic field obtained by the current flowing through the hairpin conductor is the nucleation magnetic field HN (Nucreation magnetic field HN).
Fie1d) must be exceeded. The magnitude of the nucleation magnetic field HN is approximately equal to the anisotropic magnetic field HK, and this value has a magnitude of approximately 20,000e. The anisotropic magnetic field HK increases as the bubble diameter becomes smaller; They tend to become smaller as the temperature rises.On the other hand, it is known that in order to increase the bit density of the memory loop that stores magnetic bubbles, the diameter of the magnetic bubbles must be reduced; As HN decreases, the nucleation magnetic field HN increases accordingly, and the amplitude of the pulse current supplied to the hairpin conductor must be set large.

しかしこのようにパルス電流の振幅を大きくすると、ヘ
アピンコンダクタの許容電流値をオーバしてしまいヘア
ピンコンダクタに焼損を与える場合があり、また、バブ
ルの発生が困難となり、しかも大きな振幅の電流を発生
する回路を必要とすることから経済的にも不利となる。
したがつて、本発明の目的は磁気バブルの発生に要する
パルス電流の振幅を小さくできるようにしてヘアピンコ
ンダクタなどのバブル発生器の信頼性を確保するととも
に、パルスを発生する回路の簡略化を図り経済性を確保
し、さらにバブルを確実に発生できるようにするもので
ある。本発明はこのような目的を達成するために、ヘア
ピンコンダクタなどのバブル発生器に対してバブル発生
用のパルス電流を流す前にこのパルス電流と逆極性のパ
ルス電流を流すようにするものであり、以下実施例を用
いて詳細に説明する。
However, if the amplitude of the pulse current is increased in this way, the permissible current value of the hairpin conductor may be exceeded and the hairpin conductor may be burnt out. Also, it becomes difficult to generate bubbles, and a current with a large amplitude is generated. Since it requires a circuit, it is also economically disadvantageous.
Therefore, an object of the present invention is to ensure the reliability of bubble generators such as hairpin conductors by reducing the amplitude of the pulse current required to generate magnetic bubbles, and to simplify the circuit that generates the pulses. This ensures economic efficiency and also ensures the generation of bubbles. In order to achieve such an object, the present invention supplies a bubble generator such as a hairpin conductor with a pulse current having a polarity opposite to that of the bubble generation pulse current. will be described in detail below using examples.

一般に、上記異方性磁界HKは磁気バブルメモリチップ
の温度が上昇すればそれに伴なつて小さくなることが知
られている0したがつて、この場合上記異方性磁界HK
が小さくなることにより当然上記パルス電流の振幅も小
さくできる0図面はかかる原理にもとづきバブルを発生
する直前にヘアピンコンダクタの形成される磁気バブル
メモリチツプの周辺をあらかじめ予熱するための電流波
形を示す。図において、P,は磁気バブル発生用の振幅
A1のパルス電流である。また、P2は時刻T,以前に
おいて形成されるパルス電流P1とは逆極性のパルス電
流である。この場合、電流P2は、通電によるジユール
熱でヘアコンダクタの形成されたバブルチツプの周辺を
加熱して上記異方性磁界HKを小さくするに十分な振幅
とパルス幅に設定されている。したがつて、このパルス
電流P2を供給することにより、ヘアピンコンダクタの
周辺部をバブルドメイン発生前にあらかじめ加熱でき、
異方性磁界HKを小さくできるため、磁気バブル発生用
のパルス電流P,の振幅A1を小さくできる。ここで、
パルス電流P2は一個形成することに限定される磁気バ
ブル発生前に複数個形成するようにしてもよい。
Generally, it is known that the anisotropic magnetic field HK decreases as the temperature of the magnetic bubble memory chip increases. Therefore, in this case, the anisotropic magnetic field HK
By reducing the amplitude of the pulse current, the amplitude of the pulse current can naturally be reduced. Based on this principle, the drawing shows a current waveform for preheating the periphery of a magnetic bubble memory chip where a hairpin conductor is formed immediately before generating a bubble. In the figure, P is a pulse current of amplitude A1 for generating magnetic bubbles. Further, P2 is a pulse current having a polarity opposite to that of the pulse current P1 formed before time T. In this case, the current P2 is set to have an amplitude and a pulse width sufficient to reduce the anisotropic magnetic field HK by heating the periphery of the bubble chip in which the hair conductor is formed with the Joule heat generated by energization. Therefore, by supplying this pulse current P2, the peripheral part of the hairpin conductor can be heated in advance before the bubble domain is generated.
Since the anisotropic magnetic field HK can be made small, the amplitude A1 of the pulse current P for generating magnetic bubbles can be made small. here,
A plurality of pulse currents P2 may be formed before the generation of the magnetic bubble, which is limited to the formation of one pulse current P2.

このように、予熱用のパルス電流P2は磁気バブル発生
用のパルス電流P,と逆極性のため、たとえ振幅が大き
くても磁気バブルを発生することはない。
In this way, since the preheating pulse current P2 has a polarity opposite to that of the magnetic bubble generation pulse current P, magnetic bubbles are not generated even if the amplitude is large.

したがつて、パルス電流P2の振幅は任意に設定できる
ため、パルスを発生する回路の構成を簡略化でき、経済
性が確保できる。以上説明したように本発明による磁気
バブル発生方式によると、磁気バブルメモリチツプに形
成されたヘアピンコンダクタねどのバブル発生器にパル
ス電流を流して磁気バブルを発生させるに際し、あらか
じめ上記パルス電流と逆極性のパルス電流を流してバブ
ル発生器の周辺を加熱し、その異方性磁界HKを小さく
した。
Therefore, since the amplitude of the pulse current P2 can be set arbitrarily, the configuration of the circuit that generates the pulse can be simplified and economical efficiency can be ensured. As explained above, according to the magnetic bubble generation method of the present invention, when a pulse current is passed through a bubble generator such as a hairpin conductor wire formed in a magnetic bubble memory chip to generate a magnetic bubble, the polarity of the pulse current is reversed in advance. The surrounding area of the bubble generator was heated by passing a pulsed current of , and its anisotropic magnetic field HK was reduced.

このために、磁気バブル発生用のパルス電流の振幅を小
さくできるので、磁気バブル発生器の焼損を防止でき、
また低温中においてもサブミクロンバブルなど径の小さ
い磁気バブルを確実に形成できるとともに、予熱用パル
ス電流は振幅を任意に設定できるのでパルスを発生する
回路の構成を簡略化できるなど種種の効果を奏する。
For this reason, the amplitude of the pulse current for generating magnetic bubbles can be reduced, which prevents burnout of the magnetic bubble generator.
In addition, small-diameter magnetic bubbles such as submicron bubbles can be reliably formed even at low temperatures, and the amplitude of the preheating pulse current can be set arbitrarily, so the configuration of the circuit that generates the pulses can be simplified, and various other effects can be achieved. .

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

Claims (1)

【特許請求の範囲】[Claims] 1 磁気バブルメモリチップに形成されたバブル発生器
に、磁気バブル発生用のパルス電流を供給する前にこの
パルス電流と逆極性のパルス電流を供給して磁気バブル
発生部分を予熱するようにしたことを特徴とする磁気バ
ブル発生方式。
1. Before supplying the pulse current for magnetic bubble generation to the bubble generator formed in the magnetic bubble memory chip, a pulse current of opposite polarity to this pulse current is supplied to preheat the magnetic bubble generation part. A magnetic bubble generation method featuring
JP50017889A 1975-02-14 1975-02-14 Magnetic bubble generation method Expired JPS5918788B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP50017889A JPS5918788B2 (en) 1975-02-14 1975-02-14 Magnetic bubble generation method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP50017889A JPS5918788B2 (en) 1975-02-14 1975-02-14 Magnetic bubble generation method

Publications (2)

Publication Number Publication Date
JPS5193639A JPS5193639A (en) 1976-08-17
JPS5918788B2 true JPS5918788B2 (en) 1984-04-28

Family

ID=11956265

Family Applications (1)

Application Number Title Priority Date Filing Date
JP50017889A Expired JPS5918788B2 (en) 1975-02-14 1975-02-14 Magnetic bubble generation method

Country Status (1)

Country Link
JP (1) JPS5918788B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4156936A (en) * 1977-05-31 1979-05-29 International Business Machines Corporation Apparatus and method for improved operation of bubble devices
JPS5416942A (en) * 1977-07-08 1979-02-07 Hitachi Ltd Writing device for magnetic bubble information

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5099231A (en) * 1973-12-28 1975-08-06

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5099231A (en) * 1973-12-28 1975-08-06

Also Published As

Publication number Publication date
JPS5193639A (en) 1976-08-17

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