JPS647437B2 - - Google Patents
Info
- Publication number
- JPS647437B2 JPS647437B2 JP59223837A JP22383784A JPS647437B2 JP S647437 B2 JPS647437 B2 JP S647437B2 JP 59223837 A JP59223837 A JP 59223837A JP 22383784 A JP22383784 A JP 22383784A JP S647437 B2 JPS647437 B2 JP S647437B2
- Authority
- JP
- Japan
- Prior art keywords
- bubble
- detector
- output
- magnetic field
- transfer
- 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
Links
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メモリ素子における磁気バ
ブル検出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 detector in a magnetic bubble memory device.
磁気バブルメモリ装置はバブル用結晶の上に軟
磁性薄膜転送路、あるいは軟磁性薄膜転送路とイ
オン注入転送路を形成しておき、バブル磁区発生
器により情報に従つてバブルを発生させ、これを
前記バブル転送路に転送して情報を記憶させるよ
うになつている。格納された情報の読み出しは磁
気抵抗効果を利用した磁気バブル検出器にバブル
を転送して読み出すようになつている。 In a magnetic bubble memory device, a soft magnetic thin film transfer path, or a soft magnetic thin film transfer path and an ion implantation transfer path are formed on a bubble crystal, and a bubble is generated according to information using a bubble magnetic domain generator. The information is transferred to the bubble transfer path and stored. The stored information is read by transferring the bubbles to a magnetic bubble detector that utilizes the magnetoresistive effect.
従来、この磁気バブル検出器には軟磁性薄膜転
送路と同時に作製するいわゆる厚膜型の検出器が
用いられている。この厚膜型の検出器の出力はバ
ブルを駆動する回転磁界強度に大きく依存するた
め、出力ピークを与える駆動磁界と素子の中心駆
動磁界を一致させなければ良好な素子全体の特性
を得ることが出来ない。 Conventionally, this magnetic bubble detector uses a so-called thick film type detector that is manufactured at the same time as a soft magnetic thin film transfer path. Since the output of this thick-film detector largely depends on the strength of the rotating magnetic field that drives the bubble, it is difficult to obtain good overall device characteristics unless the driving magnetic field that gives the output peak matches the central driving magnetic field of the element. Can not.
第5図は従来の磁気バブル検出器を示す図であ
る。これは1.9μmバブル、8μm周期ハーフデイス
クパターンを転送路に用いた1Mビツト素子に採
用されているパターン幅1μm、パターン周期
10.4μmの非対称シエブロン型デイテクタである。
同図において、1はバブル拡大器、2は検出器、
矢印はバブルの進行方向を示している。この磁気
バブル検出器の特性は第6図に示すように出力ピ
ーク(矢印Aで示す)と素子の中心駆動磁界(矢
印Bで示す)は良く一致している。
FIG. 5 is a diagram showing a conventional magnetic bubble detector. This is the pattern width of 1 μm and pattern period used in a 1M bit device that uses a 1.9 μm bubble and 8 μm period half disk pattern for the transfer path.
It is a 10.4μm asymmetric chevron type detector.
In the figure, 1 is a bubble expander, 2 is a detector,
The arrow indicates the direction of bubble travel. As shown in FIG. 6, the characteristics of this magnetic bubble detector are such that the output peak (indicated by arrow A) and the central driving magnetic field of the element (indicated by arrow B) match well.
上記の磁気バブル検出器は、そのまま1.3μmバ
ブル、4μm周期のワイドギヤツプパターンを転
送路に用いた4Mビツト素子に採用すると素子の
中心駆動磁界が高い方に移動し、検出器の出力ピ
ークを与える駆動磁界から大きくずれて出力値が
劣化するという欠点があつた。
In the magnetic bubble detector described above, if a 4M-bit element with a 1.3 μm bubble and a 4 μm period wide gap pattern is used as the transfer path, the center driving magnetic field of the element will move to the higher side, and the output peak of the detector will rise. The drawback was that the output value deteriorated due to a large deviation from the driving magnetic field that gave the output.
本発明は、上記問題点を解消した磁気バブル検
出器を提供するもので、その手段は、軟磁性薄膜
を用いた非対称シエブロンパターンで形成された
磁気バブル検出器において、バブルの転送に寄与
する素片と、検出器前段のバブル拡大器とのつな
ぎは入り組み型で見かけ上のギヤツプが零であ
り、バブル検出出力に寄与する素片と後段のバブ
ル拡大器とのつなぎは約1μmのギヤツプを保つ
て接するようにそれぞれが配置されていることを
特徴とする磁気バブル検出器によつてなされる。
The present invention provides a magnetic bubble detector that solves the above problems, and the present invention provides a magnetic bubble detector formed with an asymmetric chevron pattern using a soft magnetic thin film, which contributes to the transfer of bubbles. The connection between the elemental piece and the bubble expander at the front stage of the detector is intricate and has an apparent gap of zero, and the connection between the elemental piece that contributes to the bubble detection output and the bubble expander at the rear stage is a gap of about 1 μm. This is done using magnetic bubble detectors, which are characterized in that they are arranged so that they are in contact with each other while maintaining the same.
上記磁気バブル検出器は、そのバブル転送に寄
与する部分の素片とその前段のバブル拡大器との
つながりを見かけ上のギヤツプを零とし、バブル
検出出力に寄与する部分の素片とその後段のバブ
ル拡大器とのつながりを約1μmのギヤツプをも
たせることにより、検出器の出力ピークを与える
駆動磁界と、素子の中心駆動磁界とを一致させ、
出力値の劣化を防止することができる。
The above-mentioned magnetic bubble detector has an apparent gap of zero in the connection between the elemental piece that contributes to bubble transfer and the bubble expander at the preceding stage, and the elemental piece that contributes to the bubble detection output and the subsequent stage. By providing a gap of approximately 1 μm between the connection with the bubble expander, the driving magnetic field that gives the output peak of the detector matches the central driving magnetic field of the element.
Deterioration of the output value can be prevented.
以下図面を参照して本発明の実施例を詳細に説
明する。
Embodiments of the present invention will be described in detail below with reference to the drawings.
第1図に本発明の一実施例の要部を平面図とし
て示し、第2図にその一部拡大図を示す。同図に
おいて、10はバブル検出器、11はそのバブル
転送に寄与する部分、12はバブル検出出力に寄
与する部分、13は検出器前段のバブル拡大器、
14は検出器後段のバブル拡大器をそれぞれ示し
ている。 FIG. 1 shows a main part of an embodiment of the present invention as a plan view, and FIG. 2 shows a partially enlarged view thereof. In the figure, 10 is a bubble detector, 11 is a part that contributes to bubble transfer, 12 is a part that contributes to bubble detection output, 13 is a bubble expander in the front stage of the detector,
Reference numeral 14 indicates a bubble expander located after the detector.
本実施例は第1図及び第2図に示すようにバブ
ル転送に寄与する部分11のパターン周期bを長
く、出力に寄与する部分12のパターン周期aを
短かく、且つ転送に寄与する部分11のパターン
幅cを出力に寄与する部分12のパターン幅dよ
り太くして全体として非対称シエブロン型とし、
バブル転送に寄与する部分11の素片の前段のバ
ブル拡大器13とのつなぎを入りくみ型として見
かけ上のギヤツプがないようにすると共に、出力
に寄与する部分12の素片と後段のバブル拡大器
14とのつなぎは直線同士で相対するようにし、
その間に1μm程度のギヤツプGを設けている。 In this embodiment, as shown in FIGS. 1 and 2, the pattern period b of the portion 11 that contributes to bubble transfer is long, the pattern period a of the portion 12 that contributes to output is shortened, and the portion 11 that contributes to transfer is made short. The pattern width c is made thicker than the pattern width d of the portion 12 that contributes to the output, so that the overall shape is asymmetric chevron type,
The connection between the elemental piece of part 11 that contributes to bubble transfer and the bubble expander 13 in the previous stage is made in a convoluted manner to avoid any apparent gap, and the elemental piece of part 12 that contributes to the output and the bubble expander 13 in the latter stage are connected in a convoluted manner. The connection with the vessel 14 should be made so that the straight lines face each other,
A gap G of about 1 μm is provided between them.
このように形成された本実施例の特性を第3図
に示す。図は縦軸にバイアス磁界を、横軸に三角
波駆動磁界をとり、バブル検出出力3.5mv〜8
mvの各出力特性を曲線a〜gで示した。なお矢
印hは素子転送の中心磁界、矢印iはバブル検出
出力のピークを与える駆動磁界をそれぞれ示して
いる。図より転送特性を劣化させずに出力ピーク
を高駆動側(この場合は70Oe)に移行できたこ
とがわかる。 The characteristics of this embodiment formed in this manner are shown in FIG. The figure shows the bias magnetic field on the vertical axis and the triangular wave drive magnetic field on the horizontal axis, and the bubble detection output is 3.5 mv ~ 8
The output characteristics of mv are shown by curves a to g. Note that the arrow h indicates the central magnetic field for element transfer, and the arrow i indicates the driving magnetic field that provides the peak of the bubble detection output. The figure shows that the output peak could be shifted to the high drive side (70Oe in this case) without deteriorating the transfer characteristics.
第4図は検出器の出力ピークを与える駆動磁界
のパターン幅、周期依存性を示す図である。図中
曲線Aは検出器のパターン幅と駆動磁界の関係、
曲線Bは検出器のパターン周期と駆動磁界との関
係を示す。図の如く検出器の出力ピークを与える
駆動磁界は、検出器のパターン幅が太くなる程高
駆動磁界側に移行し、パターン周期が長くなる程
低駆動磁界側に移行する。第5図に示した従来の
検出器のパターン幅は1.1μm、パターン周期は
10.4μmで出力ピークを与える駆動磁界は素子の
中心駆動磁界57Oeに一致している。従つてこの
検出器を中心駆動磁界70Oeの高密度素子にその
まま用いると出力ピークを与える駆動磁界と異な
り、特に高駆動磁界で十分な出力を得ることがで
きない。一方バブルの検出はバブルをストライプ
状に引伸ばし行なうもので出力特性の他にストラ
イプされたバブルを転送する十分な駆動力が必要
である。一般にパターン周期を長くするとバブル
を引伸ばし転送する能力が増大するが、逆に出力
特性は第4図に示すように出力ピークが低駆動側
に移行し、高駆動側が劣化する。そこで本実施例
は前述の第1図及び第2図で説明した構成とした
ものである。 FIG. 4 is a diagram showing the pattern width and cycle dependence of the driving magnetic field that gives the output peak of the detector. Curve A in the figure is the relationship between the detector pattern width and the driving magnetic field.
Curve B shows the relationship between the detector pattern period and the driving magnetic field. As shown in the figure, the driving magnetic field that gives the output peak of the detector shifts to the higher driving magnetic field side as the pattern width of the detector becomes thicker, and shifts to the lower driving magnetic field side as the pattern period becomes longer. The pattern width of the conventional detector shown in Figure 5 is 1.1 μm, and the pattern period is
The driving magnetic field that gives the output peak at 10.4 μm corresponds to the central driving magnetic field of the element, 57 Oe. Therefore, if this detector is used as it is in a high-density element with a central driving magnetic field of 70 Oe, it will not be possible to obtain sufficient output, especially in a high driving magnetic field, unlike the driving magnetic field that gives an output peak. On the other hand, bubble detection involves stretching the bubbles into stripes, and requires sufficient driving force to transfer the striped bubbles in addition to output characteristics. Generally, when the pattern period is lengthened, the ability to stretch and transfer bubbles increases, but conversely, as shown in FIG. 4, the output characteristic shifts to the low drive side, and the high drive side deteriorates. Therefore, this embodiment has the configuration described above in FIGS. 1 and 2.
以上説明したように本発明によれば、検出器形
状を第1図及び第2図に示したような形状にする
ことにより、検出器の出力ピークを与える駆動磁
界と素子の中心駆動磁界とを一致させ、出力値の
劣化を防止することができる。
As explained above, according to the present invention, by making the detector shape as shown in FIGS. 1 and 2, the driving magnetic field that gives the output peak of the detector and the central driving magnetic field of the element can be separated. This makes it possible to prevent deterioration of the output value.
第1図及び第2図は本発明の磁気バブル検出器
の一実施例を説明するための図、第3図は本発明
の磁気バブル検出器の特性を示す図、第4図は検
出器の出力ピークを与える駆動磁界のパターン
幅、周期依存性を示す図、第5図は従来の磁気バ
ブル検出器を示す図、第6図はその特性を示す図
である。
図中、10はバブル検出器、11はそのバブル
転送に寄与する部分、12はバブル検出出力に寄
与する部分、13は検出器前段のバブル拡大器、
14は検出器後段のバブル拡大器をそれぞれ示
す。
Figures 1 and 2 are diagrams for explaining one embodiment of the magnetic bubble detector of the present invention, Figure 3 is a diagram showing the characteristics of the magnetic bubble detector of the present invention, and Figure 4 is a diagram for explaining the characteristics of the magnetic bubble detector of the present invention. FIG. 5 is a diagram showing the pattern width and cycle dependence of a driving magnetic field that gives an output peak, FIG. 5 is a diagram showing a conventional magnetic bubble detector, and FIG. 6 is a diagram showing its characteristics. In the figure, 10 is a bubble detector, 11 is a part that contributes to bubble transfer, 12 is a part that contributes to bubble detection output, 13 is a bubble expander in the front stage of the detector,
Reference numeral 14 indicates a bubble expander located after the detector.
Claims (1)
ンで形成された磁気バブル検出器において、バブ
ルの転送に寄与する素片と、検出器前段のバブル
拡大器とのつなぎは入り組み型で見かけ上のギヤ
ツプが零であり、バブル検出出力に寄与する素片
と後段のバブル拡大器とのつなぎは約1μmのギ
ヤツプを保つて接するようにそれぞれが配置され
ていることを特徴とする磁気バブル検出器。 2 特許請求の範囲第1項記載の磁気バブル検出
器において、バブルの転送に寄与する素片と出力
に寄与する素片のパターン幅の関係が約3:1で
あり、転送に寄与する素片のパターン周期が出力
に寄与する素片のパターン周期の1.3から1.6倍の
範囲の形状であることを特徴とする磁気バブル検
出器。[Claims] 1. In a magnetic bubble detector formed with an asymmetric chevron pattern using a soft magnetic thin film, the connection between the elemental piece that contributes to bubble transfer and the bubble expander in the front stage of the detector is complicated. The mold has an apparent gap of zero, and the connection between the elemental piece that contributes to the bubble detection output and the bubble expander in the subsequent stage is characterized by being arranged so that they are in contact with each other with a gap of approximately 1 μm. Magnetic bubble detector. 2. In the magnetic bubble detector according to claim 1, the relationship between the pattern widths of the elemental pieces that contribute to bubble transfer and the elemental pieces that contribute to output is about 3:1, and the elemental pieces that contribute to transfer A magnetic bubble detector characterized in that the pattern period of the magnetic bubble detector is 1.3 to 1.6 times the pattern period of the elemental piece contributing to the output.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59223837A JPS61104484A (en) | 1984-10-26 | 1984-10-26 | Magnetic bubble detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59223837A JPS61104484A (en) | 1984-10-26 | 1984-10-26 | Magnetic bubble detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61104484A JPS61104484A (en) | 1986-05-22 |
| JPS647437B2 true JPS647437B2 (en) | 1989-02-08 |
Family
ID=16804495
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59223837A Granted JPS61104484A (en) | 1984-10-26 | 1984-10-26 | Magnetic bubble detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61104484A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2639594B2 (en) * | 1989-12-23 | 1997-08-13 | 株式会社河合楽器製作所 | Electronics |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5488738A (en) * | 1977-12-26 | 1979-07-14 | Nippon Telegr & Teleph Corp <Ntt> | Detector for magnetic domain |
| JPS5746383A (en) * | 1980-09-05 | 1982-03-16 | Nippon Telegr & Teleph Corp <Ntt> | Enlarging device of bubble magnetic domain |
-
1984
- 1984-10-26 JP JP59223837A patent/JPS61104484A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61104484A (en) | 1986-05-22 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| KR940004989B1 (en) | Thin film magnetic head | |
| JPS5940316A (en) | Magnetism sensor | |
| JPS647437B2 (en) | ||
| US5682284A (en) | Read sensitivity function for barberpole bias design magnetoresistive sensor having curved current contacts | |
| US4601013A (en) | Magnetic bubble memory device | |
| US20030068462A1 (en) | Manufacturing method for magnetic recording medium, and master information carrier used therefor | |
| JPH01116957A (en) | Head with floating slider | |
| JPH0668430A (en) | Magneto-resistance effect type read converter | |
| JPH03241510A (en) | magnetic head | |
| JPS5855592B2 (en) | magnetic bubble detection device | |
| JPS5826312A (en) | Multitrack magnetic recording head for vertical magnetization | |
| JPS61264580A (en) | Magnetic bubble memory | |
| JPS6212593B2 (en) | ||
| JPH06215322A (en) | Magnetic head | |
| JPS6145313B2 (en) | ||
| JPS6366785A (en) | Magnetic bubble memory device | |
| JPS6163995A (en) | Detector for bubble magnetic domain | |
| JPH0646498B2 (en) | Magnetic bubble expander | |
| JPS6336073B2 (en) | ||
| JPS6122403A (en) | Magnetic recording and reproducing system | |
| JPS6120943B2 (en) | ||
| JPS58188320A (en) | Combination type magnetic head | |
| JPS6216219A (en) | Thin film magnetic head | |
| JPS6330716B2 (en) | ||
| JPH0481205U (en) |