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JPS6059666B2 - magnetic bubble expander - Google Patents
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JPS6059666B2 - magnetic bubble expander - Google Patents

magnetic bubble expander

Info

Publication number
JPS6059666B2
JPS6059666B2 JP9457378A JP9457378A JPS6059666B2 JP S6059666 B2 JPS6059666 B2 JP S6059666B2 JP 9457378 A JP9457378 A JP 9457378A JP 9457378 A JP9457378 A JP 9457378A JP S6059666 B2 JPS6059666 B2 JP S6059666B2
Authority
JP
Japan
Prior art keywords
magnetic bubble
pattern
magnetic
bubble
expander
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
JP9457378A
Other languages
Japanese (ja)
Other versions
JPS5522255A (en
Inventor
実 広島
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 JP9457378A priority Critical patent/JPS6059666B2/en
Publication of JPS5522255A publication Critical patent/JPS5522255A/en
Publication of JPS6059666B2 publication Critical patent/JPS6059666B2/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をひも状の細長いバブルに引き延
はす働きをする磁気バブル拡大器に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic bubble expander that serves to stretch magnetic bubbles into string-like elongated bubbles.

磁気バブルの有無を電気信号に変換する磁気バルブ検
出器の信号出力は、磁気バブルの長さに比例して大きく
なるから、磁気バブル検出器入力側に磁気バブル拡大器
を設け、ここで円筒状バブルを百倍ないし数百倍の長さ
のひも状バブルに引き延は七たのちに検出させることが
行われている。
The signal output of a magnetic valve detector that converts the presence or absence of a magnetic bubble into an electrical signal increases in proportion to the length of the magnetic bubble. Therefore, a magnetic bubble expander is installed on the input side of the magnetic bubble detector, and a cylindrical It has been carried out to elongate the bubble into a string-like bubble that is 100 to several hundred times as long and detect it after seven seconds.

第1図は従来の磁気バブル拡大器のパターンの一例を
示す図である。図中、1000は磁気バブル拡大器、2
00は磁気バブル検出器である。磁気バブル拡大器10
00は、パーマロイ等の軟強磁性体薄膜からなるシエブ
ロンパターン10を横方向にn個配列した横列100を
、さらに縦方向にl段配列して構成されている。通常、
nは100〜4囲程度、1は10〜2C@度である。図
中HBは、磁気バブルを安定に存在させるためにバブル
媒体面に垂直に外部から加えているバイアス磁界で、図
の場合、紙面の裏から表への向きに加えられている。ま
たHRは磁気バブルを転送するために外部から加えてい
る、バブル媒体面内で反時計方向に回転している回転磁
界である。この回転磁界HRによつて、磁気バルブBは
、磁気バブル拡大器1000中を矢印Pて示す方向に、
回転磁界HRが1回転するたびに一段ずつ上に進む。
磁気バブルBは、磁気バブル拡大器1000中を上方に
転送されるとき、図中にQと示す横方向にも引き延ばさ
れて、ひも状バブルに拡大される。
FIG. 1 is a diagram showing an example of a pattern of a conventional magnetic bubble expander. In the figure, 1000 is a magnetic bubble expander, 2
00 is a magnetic bubble detector. magnetic bubble expander 10
00 is constructed by arranging n rows 100 of chevron patterns 10 made of soft ferromagnetic thin films such as permalloy in the horizontal direction, and further arranging them in l stages in the vertical direction. usually,
n is about 100 to 4 degrees, and 1 is about 10 to 2 degrees Celsius. In the figure, HB is a bias magnetic field that is externally applied perpendicularly to the surface of the bubble medium in order to make the magnetic bubble exist stably, and in the case of the figure, it is applied from the back to the front of the page. Further, HR is a rotating magnetic field that is applied from the outside to transfer magnetic bubbles and is rotating counterclockwise within the plane of the bubble medium. This rotating magnetic field HR causes the magnetic valve B to move in the direction indicated by the arrow P in the magnetic bubble expander 1000.
Each time the rotating magnetic field HR rotates once, it moves up one stage.
When the magnetic bubble B is transferred upward through the magnetic bubble expander 1000, it is also stretched in the lateral direction indicated by Q in the figure, and expanded into a string-like bubble.

磁気バブルBが横方向Qに引き延ばされる速度は有限で
あるから、磁気バブルBは、磁気バブル拡大器1000
内を上方Pに一段転送されるごとに横方向Qにも少しず
つ引き延はされて、図中E、、E。と例示したように、
延びて行く。磁気バブル拡大器1000が正常に動作す
るときは、磁気バブルBが、磁気バブル拡大器の最終段
1の位置に転送されるまでに、拡大器1000の横方向
全幅に引き延ばされる(フルストレッチ)ことになる。
しカル従来の磁気バブル拡大器では、バイアス磁界H
Bが大きくなつたり、回転磁界HRが弱くなつたり、あ
るいは回転磁界HRの周波数が高くなつたりすると、バ
ブルの延びが十分大きくならず、図中にE″1,E″2
と例示した程度の延び方にとどまり、フルストレッチさ
れなくなるという問題があつた。
Since the speed at which the magnetic bubble B is stretched in the lateral direction Q is finite, the magnetic bubble B is
Each time the inside is transferred one step upward P, it is also slightly extended in the lateral direction Q, resulting in E, E in the figure. As exemplified,
It gets longer. When the magnetic bubble expander 1000 operates normally, the magnetic bubble B is stretched to the full lateral width of the expander 1000 (full stretch) before being transferred to the final stage 1 position of the magnetic bubble expander. It turns out.
In conventional magnetic bubble expanders, the bias magnetic field H
If B becomes larger, the rotating magnetic field HR becomes weaker, or the frequency of the rotating magnetic field HR becomes higher, the bubble extension will not be large enough, resulting in E″1 and E″2 in the figure.
There was a problem in that the stretching was limited to the extent shown in the example above, and it was not fully stretched.

この状態を改善するために、従来も磁気バブル拡大器の
改良形がいくつか発表されている。
In order to improve this situation, several improved versions of magnetic bubble expanders have been announced.

第2図A,b,cはこれら従来の磁気バブル拡大器の改
良形のパターンの3例について、それぞれ横列100を
1段ずつ示している。これら従来の改良形磁気バブル拡
大器の特徴は、磁性体薄膜パターンの横列100を構成
する基本のパターンとして、第1図中の例に用いられて
いる対称シエプロンパターン10にかわつて、非対称シ
エプロンパターンを用いている点にある。このような非
対称シエプロンパターンは、対称シエプロンパターンに
比べて磁気バブルを転送する特性がすぐれていることが
良く知られており、これら転送特性の優れた非対称シエ
プロンパターンを基本のパターンとして、磁気バブル拡
大器1000の横列100を構成することによつて、磁
気バブルBを横方向Qに引き延はす速度を大きくしてい
る。本発明の目的は、バイアス磁界H8の大きい領域、
回転磁界HRの小さい領域、あるいは回転磁界HRの周
波数の高い領域でも、フルストレッチできる、さらに特
性を改善した磁気バブル拡大器を提供することにある。
FIGS. 2A, 2B and 2C illustrate one row 100 in each of three examples of improved patterns of these conventional magnetic bubble expanders. The characteristics of these conventional improved magnetic bubble expanders are that, as the basic pattern constituting the rows 100 of the magnetic thin film pattern, an asymmetrical apron pattern is used instead of the symmetrical apron pattern 10 used in the example in FIG. The point lies in the use of patterns. It is well known that such an asymmetrical apron pattern has better properties for transferring magnetic bubbles than a symmetrical apron pattern, and these asymmetrical apron patterns with excellent transfer properties can be used as a basic pattern. By configuring the rows 100 of the magnetic bubble expanders 1000, the speed at which the magnetic bubbles B are stretched in the lateral direction Q is increased. The object of the present invention is to provide a region with a large bias magnetic field H8,
It is an object of the present invention to provide a magnetic bubble expander which can be fully stretched even in a region where the rotating magnetic field HR is small or a region where the frequency of the rotating magnetic field HR is high and has further improved characteristics.

本発明者が第1図、第2図に示した従来の磁気バブル拡
大器が、磁気バブルを横に引き延ばす動作を詳細に検討
した結果、下記の如きことが判明した。
As a result of a detailed study by the present inventor of the operation of the conventional magnetic bubble expander shown in FIGS. 1 and 2 to laterally extend magnetic bubbles, the following findings were found.

第3図は、磁気バブル拡大器1000中の磁気バブルB
の転送過程を部分的に示す図で、図中の符号は第1図の
場合と同様てある。
FIG. 3 shows the magnetic bubble B in the magnetic bubble expander 1000.
This is a diagram partially showing the transfer process of , and the reference numerals in the diagram are the same as in FIG.

B(0)は、回転磁界HRが0合方向のときの、同様に
B.(90)、B(180)は、それぞれHRが90方
向のときの磁気バブル位置である。こうして回転磁界H
Rが0気から1800の方向まで半回転すると、当初B
(0)位置にあつた磁気バブルがB(180)位置まで
転送されることになる。磁気バブールBは縦方向Pに転
送されるとき、同時に横方向Qに引き延ばされるのであ
るが、その際一定速度で横方向に引き延ばされるのでは
なく、回転磁界HRの位相に関連して、その特定の位相
の近傍でのみ急に引き延ばされ、それ以外の位相の所で
は延びないことがわかつた。いま磁気バブルBの回転磁
界HRの位相XOの時の位置、状態を前記の如くB(x
)とあられすこととする。第4図は従来の磁気バブル拡
大器について、磁気バブルB(x)がいかなる位相の時
に横方向Qに引き延ばされるかを求めた結果であつて、
同図中に斜線を引いて示した位相範囲内にあるときだけ
延びていた。すなわち従来の磁気バブル拡大器の場合、
”360わの全位相範囲のうち、磁気バブルB(x)を
横方向Qに引き延ばすのに有効な位相Xの範囲は、x=
0に近傍とx=180効近傍の2個所の限られた極めて
わすかな範囲にすぎない。第3図のB(0)、B(18
0)の位置では磁気バブルは横方向Qに引き延ばされる
が、それ以外の位置ではほとんど引き延ばされず、B(
90)の位置では全く引き延ばされない。本発明の基本
的な考え方は、360のの全位相範囲の中で、磁気バブ
ルを横方向に引き延ばすのに有効に利用される位相範囲
を拡大しようとするものである。
Similarly, B(0) is B. when the rotating magnetic field HR is in the 0 direction. (90) and B(180) are the magnetic bubble positions when HR is in the 90 direction, respectively. In this way, the rotating magnetic field H
When R rotates half a turn from 0 to 1800, initially B
The magnetic bubble located at the (0) position will be transferred to the B (180) position. When the magnetic bubble B is transferred in the longitudinal direction P, it is simultaneously stretched in the transverse direction Q, but in this case it is not stretched transversely at a constant speed, but in relation to the phase of the rotating magnetic field HR. It was found that it was suddenly elongated only near that particular phase, and not at other phases. Now, the position and state of magnetic bubble B at phase XO of rotating magnetic field HR are expressed as B(x
) and hail. FIG. 4 shows the results of determining the phase at which the magnetic bubble B(x) is stretched in the lateral direction Q for a conventional magnetic bubble expander.
It extended only when it was within the phase range indicated by diagonal lines in the figure. In other words, for a conventional magnetic bubble expander,
``Out of the total phase range of 360 degrees, the range of phase X that is effective for stretching the magnetic bubble B(x) in the lateral direction Q is x=
There are only two very narrow ranges, one near 0 and one near the x=180 effect. B(0), B(18) in Figure 3
At position 0), the magnetic bubble is stretched in the lateral direction Q, but at other positions it is hardly stretched, and at position B(
90), it is not stretched at all. The basic idea of the present invention is to expand the phase range that is effectively used to stretch the magnetic bubble laterally within the total phase range of 360.

これに対して第2図に示した従来の改良形磁気バブル拡
大器は、横方向Qに引き延ばす速度を大きくしようとし
たものと言うべきである。いま、ある磁気バブル拡大器
において、それが磁気バブルを横方向Qに引き延ばす速
度を■,とし、3600の全位相範囲の中で、横方向に
引き延ばすのに有効に利用される位相範囲をΔ0にとす
ると、回転磁界HRが1回転する間に横方向に引き延ば
される量ΔIは次式のようになる。ここでTは、回転磁
界HRが1回転する時間すなわちHRの時間周期である
。フルストレッチの特性を改良することは、式(1)の
ΔIを大きくすることで、第2図に示した従来の改良形
磁気バブル拡大器は、式(1)中のVQを大きくしよう
としたものである。
In contrast, the conventional improved magnetic bubble expander shown in FIG. 2 is an attempt to increase the speed of expansion in the lateral direction Q. Now, in a certain magnetic bubble expander, let the speed at which it stretches the magnetic bubble in the lateral direction Q be . Then, the amount ΔI by which the rotating magnetic field HR is stretched in the lateral direction during one rotation is expressed by the following equation. Here, T is the time for one rotation of the rotating magnetic field HR, that is, the time period of HR. Improving the full stretch characteristics is by increasing ΔI in equation (1), and the conventional improved magnetic bubble expander shown in Figure 2 attempts to increase VQ in equation (1). It is something.

第5図aは従来の基本パターンであるシエプロンパター
ン10を示す図である。
FIG. 5a is a diagram showing a conventional basic pattern, a chevron pattern 10.

このパターンは磁気バブルの転送方向Pに対して前部に
ある第1素片1と、後部にある第2素片2の2部分が、
図中に破線で示した個所で結合したものと考えられ、第
1素片1と第2素片2はバブル転送方向に対しそれぞれ
逆方向に傾斜しており、両素片の幅は相等しい。第5図
bはいわゆる非対称シエプロンパターン1『を示し、第
1素片1″の幅が第2素片2″の幅より広くなつている
。このようにすると、磁気バブルがある段のパターンの
横列100から次段の横列100に転送されやすくなる
ものと考えられ、第2図A,b,cに示した従来の磁気
バブル拡大器の改良形パターンは、おおむねこの様な考
え方に沿つて、速度■Qの向上をはかつたものと言える
。これに対し本発明は既述の如く磁気バブルを横方向に
引き延ばすのに利用される位相範囲Δθを拡大するため
に、第6図に示すように、Δθが従来の様に、00、1
80に近傍だけでなく、45135にの近傍にも生ずる
ようにパターン形状を改良することとした。
This pattern consists of two parts: the first elemental piece 1 at the front with respect to the transfer direction P of the magnetic bubble, and the second elemental piece 2 at the rear.
It is thought that they are joined at the points indicated by broken lines in the figure, and the first elemental piece 1 and the second elemental piece 2 are inclined in opposite directions with respect to the bubble transfer direction, and the widths of both pieces are equal. . FIG. 5b shows a so-called asymmetrical chevron pattern 1'', in which the width of the first element 1'' is wider than the width of the second element 2''. In this way, it is thought that magnetic bubbles can be easily transferred from one row 100 of a pattern to the next row 100, an improvement on the conventional magnetic bubble expander shown in FIGS. 2A, b, and c. It can be said that the shape pattern is designed to improve the speed Q based on this idea. In contrast, in the present invention, as described above, in order to expand the phase range Δθ used to extend the magnetic bubble in the horizontal direction, as shown in FIG.
We decided to improve the pattern shape so that it occurs not only near 80 but also near 45135.

第7図A,bl第8図A,bに、Δθを45た、135
A近傍にも生じさせるための本発明に係る改良した基本
パターン11,11″,12,12″の形状を示す。パ
ターン11は第1素片1が第2素片2と等しい幅を有し
、かつ両者の結合個所から伸びた突出部分1aを有して
おり、パターン1「は第1素片1″が第2素片2″より
幅が広く、かつ両者の結合個所から伸びた突出部分1″
aを有している。パターン12は第2素片2が第1素片
1と等しい幅を有し、かつ両者の結合個所から伸びた突
出部分2aを有しており、パターン12″は第2素片2
″が第1素片1″より幅が狭く、かつ両者の結合個所か
ら伸びた突出部分2″aを有している。本発明磁気バブ
ル拡大器は、前記の様な基本パターン10,10″,1
1,1「,12,12″を組合わせて用いるが、その結
果、第1素片の突出部分が隣接(時には更にその隣りの
)パターンの第2素片に結合したり、第2素片の突出部
分が隣接(時には更にその隣りの)パターンの第1素片
に結合したりして、結局、第1素片が複数の第2素片に
結合したパターン、および、第2素片が複数の第1素片
に結合したパターン、が混在するパターンよりなる横列
を多段に重ねたものとなる。第9図aは基本パターン1
1,12を交互に組合せたものを示し、第9図bは基本
パターン10,11を組合せたパターンと、基本パター
ン10,12を組合せたパターンを、交互に配列したも
のを示す図である。第10図aは基本パターン1「,1
2″を交互に合せたもの、第10図bは基本パターン1
0″,1「の組合せと、1『,125の組合せを、交互
に配列したものを示す図である。これらのパターンを用
いた本発明磁気バブル拡大器の動作を検討した結果、磁
気バブルは所期の如く、第6図に斜線を施して示した位
相範囲内で引き延ばされていることがわかつた。第11
図A,bl第12図A,bは、それぞれ本発明に用いる
更に異なるパターンの例を示す。以上説明したごとく本
発明によれば、バイアス磁界の大きい領域、回転磁界が
弱かつたり、その周波数の高い領域で、フルストレッチ
できる、特性の一層改善された磁気バブル拡大器が得ら
れる効果がある。
Figure 7 A, bl Figure 8 A, b, Δθ is 45, 135
The shapes of improved basic patterns 11, 11'', 12, 12'' according to the present invention to be generated also in the vicinity of A are shown. In the pattern 11, the first elemental piece 1 has the same width as the second elemental piece 2, and has a protruding portion 1a extending from the joining point of the two, and in the pattern 1 ``the first elemental piece 1'' has the same width as the second elemental piece 2. A protruding portion 1″ that is wider than the two pieces 2″ and extends from the joint of the two pieces.
It has a. In the pattern 12, the second elemental piece 2 has the same width as the first elemental piece 1, and has a protruding portion 2a extending from the joining point of both, and the pattern 12'' has the same width as the first elemental piece 1.
'' is narrower than the first piece 1'' and has a protruding portion 2''a extending from the joint portion of the two pieces.The magnetic bubble expander of the present invention has basic patterns 10, 10'' as described above. ,1
1, 1", 12, 12" are used in combination, but as a result, the protruding part of the first element is connected to the second element of an adjacent (and sometimes even adjacent) pattern, or The protruding portion of the pattern is connected to the first element of an adjacent (sometimes even adjacent) pattern, resulting in a pattern in which the first element is connected to a plurality of second elements, and a pattern in which the second element is connected to a plurality of second elements. The pattern is formed by stacking rows of patterns in which patterns are combined with a plurality of first elemental pieces in multiple stages. Figure 9a is basic pattern 1
FIG. 9b shows a pattern in which basic patterns 10 and 11 are combined and a pattern in which basic patterns 10 and 12 are arranged alternately. Figure 10a shows the basic pattern 1",1
2" alternately, Figure 10b is basic pattern 1
It is a diagram showing a combination of 0'', 1'' and a combination of 1'', 125 arranged alternately. As a result of examining the operation of the magnetic bubble expander of the present invention using these patterns, it was found that the magnetic bubble As expected, it was found that the phase range was elongated within the shaded phase range in Fig. 6.
FIGS. 12A and 12B each show examples of further different patterns used in the present invention. As explained above, according to the present invention, it is possible to obtain a magnetic bubble expander with further improved characteristics that can be fully stretched in areas where the bias magnetic field is large, the rotating magnetic field is weak, and its frequency is high. .

”図面の簡単な説明 第1図は従来の磁気バブル拡大器のパターンを示す図、
第2図A,b,cは磁気バブル拡大器の従来の改良パタ
ーン例図、第3図、第4図は従来の磁気バブル拡大器の
動作説明図、第5図A,bは従来の基本パターン図、第
6図は本発明バブル拡大器の動作特性図、第7図A,b
、第8図A,bは本発明に係る基本パターン例図、第9
図A,b、第10図A,b、第11図A,bl第12図
A,bは本発明実施例に用いたそれぞれ異なるパ“ター
ンを示す図である。
``Brief Description of the Drawings Figure 1 is a diagram showing the pattern of a conventional magnetic bubble expander;
Figures 2A, b, and c are examples of conventional improved patterns of magnetic bubble expanders; Figures 3 and 4 are explanatory diagrams of the operation of conventional magnetic bubble expanders; Figures 5A and b are conventional basic patterns. The pattern diagram, Figure 6 is the operational characteristic diagram of the bubble expander of the present invention, and Figure 7 A, b.
, Figures 8A and b are basic pattern example diagrams according to the present invention, Figure 9
Figures A and b, Figures 10A and b, Figures 11A and bl, and Figures 12A and b are diagrams showing different patterns used in the embodiment of the present invention.

1,1″・・・・・・第1素片、1a,1″a・・・・
・・第1素片突出部分、2,2″・・・・第2素片、2
a,2″a・・・・第2素片突出部分、10,1『,1
1,11″,12,12″・・・・基本パターン、10
0・・・磁気バブル拡大器の横列、1000・・・・・
・磁気バブル拡大器。
1,1″...first elemental piece, 1a,1″a...
...Protruding portion of the first elemental piece, 2,2''...Second elemental piece, 2
a, 2″a... second elemental piece protruding portion, 10, 1″, 1
1,11″,12,12″・・・Basic pattern, 10
0... Row of magnetic bubble expanders, 1000...
・Magnetic bubble expander.

Claims (1)

【特許請求の範囲】[Claims] 1 磁気バブル媒体面に、バブル転送方向に対してそれ
ぞれ逆方向に傾斜した第1素片と第2素片を結合したシ
エブロンパターンあるいは非対称シエブロンパターンを
基本パターンとして、軟強磁性体薄膜で形成した磁気バ
ブル拡大器において、そのパターンが、第1素片が複数
の第2素片に結合したもの、及び、第2素片が複数の第
1素片に結合したもの、を混在させてなることを特徴と
する磁気バブル拡大器。
1. A soft ferromagnetic thin film is formed on the surface of the magnetic bubble medium using a basic pattern of a chevron pattern or an asymmetric chevron pattern, which is a combination of a first element and a second element tilted in opposite directions relative to the bubble transfer direction. In the formed magnetic bubble expander, the pattern is a mixture of a first elemental piece coupled to a plurality of second elemental pieces and a pattern in which a second elemental piece is coupled to a plurality of first elemental pieces. A magnetic bubble expander featuring:
JP9457378A 1978-08-04 1978-08-04 magnetic bubble expander Expired JPS6059666B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9457378A JPS6059666B2 (en) 1978-08-04 1978-08-04 magnetic bubble expander

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9457378A JPS6059666B2 (en) 1978-08-04 1978-08-04 magnetic bubble expander

Publications (2)

Publication Number Publication Date
JPS5522255A JPS5522255A (en) 1980-02-16
JPS6059666B2 true JPS6059666B2 (en) 1985-12-26

Family

ID=14114033

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9457378A Expired JPS6059666B2 (en) 1978-08-04 1978-08-04 magnetic bubble expander

Country Status (1)

Country Link
JP (1) JPS6059666B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61149447U (en) * 1985-03-07 1986-09-16

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58185086A (en) * 1982-04-21 1983-10-28 Nec Corp Magnetic bubble storage element

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61149447U (en) * 1985-03-07 1986-09-16

Also Published As

Publication number Publication date
JPS5522255A (en) 1980-02-16

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