JPS60160093A - Magnetic bubble generator - Google Patents

Magnetic bubble generator

Info

Publication number
JPS60160093A
JPS60160093A JP59016434A JP1643484A JPS60160093A JP S60160093 A JPS60160093 A JP S60160093A JP 59016434 A JP59016434 A JP 59016434A JP 1643484 A JP1643484 A JP 1643484A JP S60160093 A JPS60160093 A JP S60160093A
Authority
JP
Japan
Prior art keywords
slot
magnetic
hairpin
current
magnetic bubble
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.)
Granted
Application number
JP59016434A
Other languages
Japanese (ja)
Other versions
JPH0544754B2 (en
Inventor
Haruo Urai
浦井 治雄
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
NEC Corp
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 NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP59016434A priority Critical patent/JPS60160093A/en
Publication of JPS60160093A publication Critical patent/JPS60160093A/en
Publication of JPH0544754B2 publication Critical patent/JPH0544754B2/ja
Granted 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 improve the generation factor of magnetic fields and also to reduce the heat dissipation effect by forming a slot to a conductor pattern. CONSTITUTION:A hairpin-shaped conductor pattern 2 contains a rectangular heat dissipation fin 20 at its tip part, and a slot 22 is formed at the center part of the fin 20 in the direction parallel to a hairpin gap 21. A current pulse 3 is applied to an arm part of the pattern 2. Ths most of the current 31 passes through a part 32 held between the slot 22 and the gap 21, and only a part 33 of the current flows near a slot edge 22b. As a result, the temperature can be kept at a low level at the part of the fin 20.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、磁気バブルを情報の担体として用いるメモリ
装置に於ける磁気バブル発生器に関するものである。更
に詳しく述べれば、導体パタンに電流パルスを印加して
発生する局所磁場によシ磁気バブルをニュークリエーシ
ョン発生する磁気パズル発生器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a magnetic bubble generator in a memory device that uses magnetic bubbles as information carriers. More specifically, the present invention relates to a magnetic puzzle generator that nucleates magnetic bubbles using a local magnetic field generated by applying a current pulse to a conductor pattern.

(従来技術とその問題点) 磁気パルプを情報の担体として用いる磁気パプルメ峰り
素子では、磁気バブルを情報の有無に応じて発生する磁
気バブル発生器や、発生した磁気バブルを所定の位置に
転送する磁気バブル転送路は最重要機能要素である。近
年の磁気パズル発生器は、例えばティー・ジェイ・ネル
ソン(T、 J。
(Prior art and its problems) A magnetic pulp element that uses magnetic pulp as an information carrier uses a magnetic bubble generator that generates magnetic bubbles depending on the presence or absence of information, and a magnetic bubble generator that transfers the generated magnetic bubbles to a predetermined position. The magnetic bubble transfer path is the most important functional element. Recent magnetic puzzle generators include, for example, T.J. Nelson (T.J.

Ne1son )等によって、1980年にベルシステ
ム・テクニカルジャーナル誌(The Be1l Sy
atem Tech−nieal Journal )
 vol、29.1m2の第229頁から第257頁に
示される様にイメ盲人連接円状パタン7よりなる磁気パ
ズル転送路中の磁化が回転磁界の特定の方向で集中しや
すい箇所にヘアピン状導体パタンを配した形状を有し、
又アビン状導体に電流パルスを印加することKよシ発生
する局所磁界と集中した磁化からの局所磁界の和により
磁気バブルをニュークリエージ替ン発生する様になって
いる。
In 1980, the Bell System Technical Journal (The Bell System Technical Journal) was published by
atem Tech-nieal Journal)
Vol. 29.1m2, pages 229 to 257, a hairpin-shaped conductor is placed in a magnetic puzzle transfer path consisting of an image-blind connecting circular pattern 7 where magnetization tends to concentrate in a specific direction of the rotating magnetic field. It has a patterned shape,
Further, by applying a current pulse to the aperture-shaped conductor, a magnetic bubble is generated by the sum of the local magnetic field generated by K and the local magnetic field from the concentrated magnetization.

一方、この様なヘアピン状導体に電流パルスを印加する
場合、電流によるヘアピン導体の発熱の影響を少なくす
るために、ヘアピン導体の先端部に放熱フィンを投砂る
ことが特公昭57−36669号明細書中で述べられて
いる。これを磁気バブル発生器に適用した例が、アール
・イー・7オンタナ(R,E、 Fontana )等
によって、1980年アイ・イー・イー・イー・トラン
ザクシ嘗ン・オン・マグネティクス誌(I]Jg、 T
rans、 onMagn、 )第MAG−16号第1
101頁〜第1105頁の第15図に示されている。こ
の様な従来の放熱フィン付ヘアピン導体パタンを用いた
二瓢−クリエーシ菖ン屋磁気バブル発生器は、次に述べ
る問題点を有している。
On the other hand, when applying a current pulse to such a hairpin-shaped conductor, Japanese Patent Publication No. 57-36669 recommends placing heat dissipating fins at the tip of the hairpin conductor in order to reduce the effect of heat generation on the hairpin conductor due to the current. It is mentioned in the specification. An example of applying this to a magnetic bubble generator was published in 1980 by R.E. Fontana et al. in IE Transactions on Magnetics (I). Jg, T
rans, onMagn, ) No. MAG-16 No. 1
This is shown in FIG. 15 on pages 101 to 1105. The Nihyo-Creici Shonya magnetic bubble generator using such a conventional hairpin conductor pattern with radiation fins has the following problems.

第1図を用いて従来の磁気バブル発生器の問題点を説明
する。ここでは、従来例として、前述のFontana
 Kよるパーマロイで構成された磁気パズル転送路を先
のNe1aonによるイオン注入転送バタンI装置き換
えて説明する。この様に転送パタンを置換えても、問題
点を説明する上では本質的な差社ない。磁気パズルの二
為−クリエーシlン発生用ヘアピン状導体パタン2は、
その先端部に大き表面積を持つ放熱フィン20を持つ。
The problems of the conventional magnetic bubble generator will be explained using FIG. Here, as a conventional example, the aforementioned Fontana
A magnetic puzzle transfer path made of permalloy made by K. will be explained by replacing the ion implantation transfer pattern I device made by Ne1aon. Even if the transfer pattern is replaced in this way, there is no essential difference in explaining the problem. The second part of the magnetic puzzle - the hairpin-shaped conductor pattern 2 for generating creativity is
It has a radiation fin 20 with a large surface area at its tip.

更に、このヘアピン状導体パタンは、その間隙部21が
、4で示す面内回転磁界馬の所定の方向で強く磁化が集
中する連接円状パタン1の連接カスプ部10と重なる様
に配置されている。
Furthermore, this hairpin-shaped conductor pattern is arranged such that the gap 21 overlaps the connecting cusp portion 10 of the connecting circular pattern 1 where magnetization is strongly concentrated in a predetermined direction of the in-plane rotating magnetic field horse 4. There is.

磁気バブルを発生する際にはヘアピン状導体パタン2に
電流パルス3を印加する。電流パルスは導体パタン内を
矢印31の様に流れ、ヘアピン導体の放熱フィンのある
先端部では、間隙部21に近い所では矢印32で示す様
に短かい電流経路をたどシ、間隙部21から遠くなるに
従りて放熱フィン内で矢印33に示す様に分布して流れ
る。放熱フィン内を流れる電流成分は、導体間隙21及
び磁気バブル転送パタンの磁化集中する連接カスプ部1
00重なり部よりも遠く離れているために1実質的に発
生磁界的には殆んど寄与しな一0換言すれば、電流パル
スによる磁気バブルのニー−クリエージ冒ン発生には強
い磁界が必要であるにも拘らず、放熱フィンの存在によ
シ、発生磁界に実質的に寄与しない電流成分が放熱フィ
ン内を分布して流れ、このため印加電流パルスの磁界発
生効率が低下する。即ち、この様な従来例では磁気パズ
ル発生には、大きな電流パルスが必要となる問題点(欠
点)があった。
When generating magnetic bubbles, a current pulse 3 is applied to the hairpin-shaped conductor pattern 2. The current pulse flows within the conductor pattern as shown by the arrow 31, and at the tip of the hairpin conductor where the heat dissipation fin is located, the current pulse follows a short current path as shown by the arrow 32 near the gap 21; As the distance increases, the flow is distributed within the radiation fins as shown by arrows 33. The current component flowing inside the heat dissipation fins flows through the conductor gap 21 and the connecting cusp portion 1 where the magnetization of the magnetic bubble transfer pattern is concentrated.
00 Because it is further away than the overlapping part, 1 it makes almost no contribution to the generated magnetic field. 10 In other words, a strong magnetic field is required for the knee-crease generation of magnetic bubbles by current pulses. Despite this, due to the presence of the radiation fins, current components that do not substantially contribute to the generated magnetic field flow in a distributed manner within the radiation fins, thereby reducing the magnetic field generation efficiency of the applied current pulse. That is, in such a conventional example, a large current pulse is required to generate a magnetic puzzle.

(発明の目的) 本発明の目的は、この様な従来の欠点を除去せしめて、
磁界発生効率がよく、尚且、放熱効果は低下しない放熱
フィン付きヘアピン状導体パタンをもつ磁気バブル発生
器を提供する仁とにある。
(Object of the invention) The object of the present invention is to eliminate such conventional drawbacks,
It is an object of the present invention to provide a magnetic bubble generator having a hairpin-shaped conductor pattern with radiation fins that has good magnetic field generation efficiency and does not reduce the heat radiation effect.

更に本発明を用いれば、誤動作の少ない磁気バブル発生
器を提供することが可能となる。
Furthermore, by using the present invention, it is possible to provide a magnetic bubble generator with fewer malfunctions.

(発明の構成) 本発f14によれば、磁気バブルを保持し得る磁性材料
薄片上に設けた磁気バブル転送路の磁化集中部に導体パ
タンを配した二為−クリエーシ■ン屋磁気バブル発生器
に於いて、前記導体パタンに一スロットを設は九ことを
特徴とする磁気バブル発生器が得られる。
(Structure of the Invention) According to the present invention f14, a second creative magnetic bubble generator in which a conductor pattern is arranged in the magnetization concentrated part of the magnetic bubble transfer path provided on a thin piece of magnetic material capable of holding magnetic bubbles. In this case, a magnetic bubble generator is obtained, characterized in that one slot is provided in the conductor pattern.

(構成の鮮細な説明) 本発明は、上述の構成をとる仁とにより従来技術の問題
点を解決するものである。本発明の原理社、導体パタン
忙細長い溝状の導体非形成部分c以下スロットという。
(Detailed Description of Configuration) The present invention solves the problems of the prior art by adopting the above-described configuration. According to the principles of the present invention, the conductor pattern has an elongated groove-like non-conductor-forming portion c, which is referred to as a slot.

)がある場合、その導体に電流を印加すると、スロット
、の存在によりその部分を電流は流れる仁とが出来ずこ
れを迂回して流れ、従って電流によって発生する磁界の
分布はスロットの存在によシ大きく変化することに基〈
ものである。一方導体内の熱伝導は、導体内の長方形ス
ロットの長手方向に対しては、スロットの有無によ)殆
んど変化はない。以上の二つの原理に基いて、放熱効果
と効率的磁界発生効果が両立する導体パタンを本発明は
可能としている。
), when a current is applied to the conductor, the current cannot flow through that part due to the presence of the slot, but instead flows around it, and therefore the distribution of the magnetic field generated by the current changes due to the presence of the slot. It is based on the fact that the situation changes significantly.
It is something. On the other hand, there is almost no change in heat conduction within the conductor in the longitudinal direction of the rectangular slot within the conductor (depending on the presence or absence of the slot). Based on the above two principles, the present invention makes it possible to create a conductor pattern that achieves both a heat dissipation effect and an efficient magnetic field generation effect.

(実施例) 以下、本発明の実施例について図面を参照して詳細に説
明する。
(Example) Hereinafter, an example of the present invention will be described in detail with reference to the drawings.

実施例1 本発明の第1の実施例を第2図を用いて説明
する。
Example 1 A first example of the present invention will be described with reference to FIG.

本実施例の説明にあた夛、磁気バブルを保持する磁性材
料薄片及び磁気バブル転送パタンの存在は本質的でない
ため、とζでは記載を省く。磁気バブル発生用のヘアピ
ン状導体パタン2は、先端部に矩形状放熱フィン2oが
設けられてhて、その放熱フィン2oのはぼ中央部に、
ヘアピン間隙21とはげ平行な方向に長方形のスロット
(開孔)22が設けられている。このヘアピン状導体2
に電流パルスを矢印3で示す方向に印加する。ヘアピン
状導体のアーム部には31で示す様にこの電流パルスの
全てが流れる。この電流が、放熱フィン部20では、ス
ロット22の存在のため化フィン内で自由忙分布出来ず
、その殆んどが32に示す如く、スロット21とヘアピ
ン間隙に挾まれた部分(スロット端22の近傍)を通過
することKなる。そして、ごく一部のみ33に示す様に
スロットパタン22の今一つのスロット端22b近傍を
流れる。この33の電流成分は、スロットが充分に長い
と殆んど無視出来、またスロットを放熱フィン20の外
周部まで伸ばル、外部とつながった切れ込み状にすると
電流成分33は全く存在しない。(第2図破線部)この
様にスロットの存在によシ32で示す電流成分はきわめ
て大きく、従って、ヘアピン間隙部21に発生する局所
磁界も大きくなる。換言すれば、磁気バブルのエニーク
リエータ1フ発生に必要な一定の局所磁界を発生する電
流パルス振幅は小さくてよいととになる。
In the description of this embodiment, the presence of the magnetic material thin piece that holds the magnetic bubble and the magnetic bubble transfer pattern are not essential, so the description will be omitted in ζ. The hairpin-shaped conductor pattern 2 for generating magnetic bubbles has a rectangular heat dissipation fin 2o provided at its tip, and a rectangular heat dissipation fin 2o is provided at the center of the heat dissipation fin 2o.
A rectangular slot (opening) 22 is provided in a direction parallel to the hairpin gap 21 and the hairpin gap 21 . This hairpin conductor 2
A current pulse is applied in the direction shown by arrow 3. All of this current pulse flows through the arm portion of the hairpin-shaped conductor as shown at 31. In the radiation fin portion 20, this current cannot be freely distributed within the radiation fin due to the presence of the slot 22, and most of the current is distributed between the slot 21 and the hairpin gap (at the slot end 22), as shown at 32. ) in the vicinity of K. Then, only a small portion flows near the other slot end 22b of the slot pattern 22, as shown at 33. This current component 33 can be almost ignored if the slot is long enough, and if the slot is extended to the outer periphery of the heat dissipation fin 20 to form a notch that is connected to the outside, the current component 33 does not exist at all. (Dotted line in FIG. 2) As described above, due to the presence of the slot, the current component indicated by 32 is extremely large, and therefore the local magnetic field generated in the hairpin gap 21 is also large. In other words, the amplitude of the current pulse that generates a constant local magnetic field necessary for generating any creator 1 of magnetic bubbles may be small.

一方、この様なヘアピン状導体パタンに電流パルスを印
加する仁とにより発生するジーール熱社、ヘアピン間隙
部の先端付近で最大となる。一方、放熱フィン20には
前述の様に殆んど電流は流れること社なく、この部分で
はジ為−ル熱の発生社殆んど無視出来、温度は低く保た
れている。従って熱の流れは、ヘアピン間隙部21とス
ロット端22mの間からスロットの長手方向に平行にな
シ、スロットの存在は、先に述べた様に熱の流れKは殆
んど影響を及埋さない。即ち、放熱効果は何ら損なわれ
ないことを意味している。
On the other hand, the heat generated by applying a current pulse to such a hairpin-shaped conductor pattern is maximum near the tip of the hairpin gap. On the other hand, as mentioned above, almost no current flows through the heat dissipating fins 20, and the generation of thermal heat in this part can be almost ignored, and the temperature is kept low. Therefore, the heat flow is parallel to the longitudinal direction of the slot from between the hairpin gap 21 and the slot end 22m, and the existence of the slot has almost no effect on the heat flow K, as mentioned above. I don't. That is, it means that the heat dissipation effect is not impaired in any way.

従って本実施例のヘアピン導体パタンを用いれば、よシ
小さい電流振幅をもつ電流パルスで駆動することができ
、かつ熱放散がよいため温度上昇の少ない磁気バブル発
生器が容易に実現される。
Therefore, by using the hairpin conductor pattern of this embodiment, a magnetic bubble generator that can be driven with a current pulse having a much smaller current amplitude and that has good heat dissipation and has a small temperature rise can be easily realized.

実施例2 第3図に本発明の第2の実施例を示す。Embodiment 2 FIG. 3 shows a second embodiment of the present invention.

本実施例のヘアピン状導体パタン2の放熱フィン20の
形状社、その三辺に多数のくし状突起20mを設け、放
熱効果の向上を図るものである。この放熱フィン2oの
中央部に1第1の実施例と同様に、ヘアピン間隙2!と
鑞ぼ平行にスロット22が設けられている。しかし乍も
、その電流パルスに対する効果は、すでkのべた第1の
実施例と同様である。
The shape of the heat dissipation fin 20 of the hairpin-shaped conductor pattern 2 of this embodiment is such that a large number of comb-like protrusions 20m are provided on its three sides to improve the heat dissipation effect. At the center of the radiation fin 2o, there is a hairpin gap 2, similar to the first embodiment. A slot 22 is provided parallel to the head. However, the effect on the current pulse is the same as in the first embodiment described above.

!!JJL!−第4図は本発明の第3の実施例を示す図
である。
! ! JJL! - FIG. 4 is a diagram showing a third embodiment of the present invention.

本実施例は、前2つの実施例とはその目的が若干異なっ
て、磁気バブル発生器の動作誤動作を軽減する目的で、
導体バタン2内忙複数のスロット22.23,24.2
5を設けである。磁気バブル転送パタンlの磁化が集中
するカスプ部10には第1のスロット23のスロット端
23aがくる様に導体バタンか設けられて込る。第2の
スロット22は、第1のスロットと同じ方向に伸びてい
て、そのスロット1422 mと第1のスロット23の
スロッ) 端23 mが対置している。ス0y)22−
23の両側の幅の広いスロッF 24* 25 fl’
、ス” y F端22aと23mの対置部の両側に並ん
でいる。
The purpose of this embodiment is slightly different from that of the previous two embodiments, and the purpose of this embodiment is to reduce malfunctions of the magnetic bubble generator.
Multiple slots 22.23, 24.2 inside conductor button 2
5 is provided. A conductor button is provided in the cusp portion 10 where the magnetization of the magnetic bubble transfer pattern 1 is concentrated so that the slot end 23a of the first slot 23 is located. The second slot 22 extends in the same direction as the first slot, and its slot 1422m and the slot end 23m of the first slot 23 are opposite to each other. s0y)22-
Wide slots on both sides of 23 F 24* 25 fl'
, S''y are lined up on both sides of the opposing portion of F ends 22a and 23m.

磁気バブル発生時には、この導体バタン2忙電流パルス
3を印加する。との様なスロット配置では、電流の経路
がいくつもあるが、スロット端23b近傍の導体バタン
幅を狭くしておけば同図の実線矢印1lvc電流パルス
の大半が流れ、破線矢印33の経路及びその他の経路で
は僅がしか電流が流れない。その結果、スロット端23
aKh強い磁気ハyPル発生磁界が、スロッ)jll1
22m、23bKはそれとは逆極性の磁界が、22bI
/cは23mと同極性ではあるが、きわめて弱い磁界が
発生する。
When a magnetic bubble is generated, a current pulse 3 is applied to the conductor button 2. In a slot arrangement like this, there are several current paths, but if the width of the conductor button near the slot end 23b is narrowed, most of the current pulse 1lvc shown by the solid line arrow in the same figure will flow, and the path shown by the broken line arrow 33 and the path of the broken line arrow 33 will flow. Only a small amount of current flows in other paths. As a result, the slot end 23
aKhThe strong magnetic field generated by the magnetic field is
22m, 23bK have a magnetic field of opposite polarity, 22bI
/c has the same polarity as 23m, but an extremely weak magnetic field is generated.

従って磁気バブルはスロット230弱い発生方向の磁界
成分でカスプ部10Fc二ニークリエージに逆極性の磁
界が発生しているために1発生した磁気バブルは、スロ
ット端23mの近傍にのみしか存在し得ない。この点画
1図の従来例の場合で社、磁気バブル発生時にはヘアピ
ン間隙部21にはバブル発生と同極性の磁界が一面に発
生してぃ 。
Therefore, the magnetic bubble is a weak magnetic field component in the generation direction of the slot 230, and since a magnetic field of opposite polarity is generated in the cusp portion 10Fc second knee crease, the generated magnetic bubble can exist only in the vicinity of the slot end 23m. In the case of the conventional example shown in Figure 1, when a magnetic bubble occurs, a magnetic field of the same polarity as the bubble generation is generated all over the hairpin gap 21.

て、発生した磁気バブルは間隙内21で無狭序に伸びて
しまい、これが、磁気バブル発生誤動作となる欠点をも
っていた。本実施例では、発生した磁気バブルは、スロ
ット端23aにのみしか存在し得ないため、この様な誤
動作はあシ得ない。
As a result, the generated magnetic bubbles extend indefinitely within the gap 21, which has the disadvantage of causing magnetic bubble generation malfunction. In this embodiment, such a malfunction cannot be avoided because the generated magnetic bubble can exist only at the slot end 23a.

(発明の効果) 以上に述べた様に本発明を用いれば、磁気バブル発生の
ための電流パルスの振幅を減少して、電流効果の良い磁
気バブル発生器が実現する。更に1本発明を用いるとと
Kよシ、磁気バブル発生誤動作の少たい磁気で(プル発
生器が実現される。又、本発明の説明は、磁気バブル転
送バタンとしてイオン注入バタンを用いたが、これが、
パーマロイバタンであっても、又、穴明き型の2層導体
バタンであっても本発明が適用出来ることはいうまでも
ない。
(Effects of the Invention) As described above, by using the present invention, the amplitude of the current pulse for generating magnetic bubbles can be reduced, and a magnetic bubble generator with good current effect can be realized. Furthermore, when the present invention is used, a magnetic pull generator with fewer magnetic bubble generation malfunctions can be realized.Also, in the explanation of the present invention, an ion implantation button is used as a magnetic bubble transfer button. ,This is,
It goes without saying that the present invention is applicable to both permalloy battens and perforated two-layer conductor battens.

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

第1図は従来例のパズル発生器を示す図、第2図、第3
図、及び第4図は夫々本発明のバブル発生器の実施例を
示す図である。図に於いて、lは転送バタン、2は導体
バタン、3は電流パルス、4は面内回転磁4.10は、
磁化が集中するカスプ部、11は磁気バブル転送路、2
0は放熱用導体バタン、20mは放熱用突起バタン、2
1は、ヘアピン間隙部、22,23,24.25はスロ
ットバタン、22b* 22b* 23m+ 23b+
はスHyト端部、31,32.33は電流パルスの通過
経路を示す矢印を示すものである。
Figure 1 shows a conventional puzzle generator, Figures 2 and 3.
4 and 4 are diagrams showing embodiments of the bubble generator of the present invention, respectively. In the figure, l is a transfer button, 2 is a conductor button, 3 is a current pulse, 4 is an in-plane rotating magnet 4.10 is,
11 is a cusp portion where magnetization is concentrated; 2 is a magnetic bubble transfer path;
0 is a conductor button for heat radiation, 20m is a protrusion button for heat radiation, 2
1 is a hairpin gap, 22, 23, 24.25 is a slot baton, 22b* 22b* 23m+ 23b+
31, 32, and 33 are arrows indicating paths through which current pulses pass.

Claims (1)

【特許請求の範囲】[Claims] 磁気バブルを保持し得る磁性材料薄片上に設けた磁気バ
ブル転送路の磁化集中部忙、導体パタンを配した二為−
クリエーシ胃ン型磁気バブル発生器に於いて、前記導体
パタンにスロットを設は大ことを特徴とする磁気バブル
発生器。
The magnetization concentration part of the magnetic bubble transfer path provided on a thin piece of magnetic material capable of holding magnetic bubbles, and the second part with a conductor pattern arranged thereon.
1. A creative gas bubble generator, characterized in that the conductor pattern is provided with a slot.
JP59016434A 1984-01-31 1984-01-31 Magnetic bubble generator Granted JPS60160093A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59016434A JPS60160093A (en) 1984-01-31 1984-01-31 Magnetic bubble generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59016434A JPS60160093A (en) 1984-01-31 1984-01-31 Magnetic bubble generator

Publications (2)

Publication Number Publication Date
JPS60160093A true JPS60160093A (en) 1985-08-21
JPH0544754B2 JPH0544754B2 (en) 1993-07-07

Family

ID=11916123

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59016434A Granted JPS60160093A (en) 1984-01-31 1984-01-31 Magnetic bubble generator

Country Status (1)

Country Link
JP (1) JPS60160093A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5651198U (en) * 1979-09-28 1981-05-07

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5224992A (en) * 1975-08-22 1977-02-24 Dainippon Toryo Co Ltd Cholesteric liquid crystal composite

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5651198U (en) * 1979-09-28 1981-05-07

Also Published As

Publication number Publication date
JPH0544754B2 (en) 1993-07-07

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