JPH02201726A - Superconducting magnetic recording medium and production thereof and recording method - Google Patents

Superconducting magnetic recording medium and production thereof and recording method

Info

Publication number
JPH02201726A
JPH02201726A JP2160989A JP2160989A JPH02201726A JP H02201726 A JPH02201726 A JP H02201726A JP 2160989 A JP2160989 A JP 2160989A JP 2160989 A JP2160989 A JP 2160989A JP H02201726 A JPH02201726 A JP H02201726A
Authority
JP
Japan
Prior art keywords
magnetic
superconducting
recording medium
recording
microrings
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.)
Pending
Application number
JP2160989A
Other languages
Japanese (ja)
Inventor
Yoshitaka Kawanishi
義隆 川西
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 Home Electronics Ltd
NEC Corp
Original Assignee
NEC Home Electronics Ltd
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 Home Electronics Ltd, Nippon Electric Co Ltd filed Critical NEC Home Electronics Ltd
Priority to JP2160989A priority Critical patent/JPH02201726A/en
Publication of JPH02201726A publication Critical patent/JPH02201726A/en
Pending legal-status Critical Current

Links

Landscapes

  • Magnetic Record Carriers (AREA)
  • Manufacturing Of Magnetic Record Carriers (AREA)

Abstract

PURPOSE:To induce perpendicular magnetic moments by the annular current generated in the superconducting microrings constituting recording units by providing a recording layer arranged with the above-mentioned microrings on a substrate and impressing external magnetic fields to the respective superconducting microrings. CONSTITUTION:The many microrings 12 are arranged and disposed along track lines on the disk substrate 14. A nonmagnetic film 22 or a magnetic film 24 consisting of a soft magnetic material is formed to cover the ultra-microrings 12 and the layer consisting of the microrings 12 and the nonmagnetic film 22 or magnetic film 24 is used as the recording layer 26. A protective film is thereafter formed on the outside surface, by which the magnetic recording medium 10 is produced. The perpendicular magnetic moments can be generated and recorded in the respective microrings 12 by passing the magnetic recording medium 10 in the impressed magnetic fields. The induction of the perpendicular magnetic moments by the annular currents generated in the microrings 12 is enabled in this way.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は超電導磁気記録媒体およびその製造方法に係り
、特にコンピュータの記録メモリー、メモリーカード、
その他の磁気記録媒体に適用することのできる超電導磁
気記録媒体およびその製造方法に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a superconducting magnetic recording medium and a method for manufacturing the same, and particularly relates to a computer recording memory, a memory card,
The present invention relates to a superconducting magnetic recording medium that can be applied to other magnetic recording media and a method for manufacturing the same.

〔従来の技術〕[Conventional technology]

従来、パーソナルのコンピュータの記録メモリ、メモリ
ーカード等の記録媒体は磁気テープ、フロッピーディス
ク、ハードディスク、磁気カード、光磁気ディスクのよ
うに磁性体を用いた磁気記録媒体であった。この種の磁
気記録媒体は基板上に磁性層と保護層を積層して製造し
、磁気へ・ンド等により前記磁性層の磁区毎に磁界印加
を施して記録するようにしている。この場合、水平方向
に磁化する方法と、垂直磁化しこれを光学的に検出する
方法とした磁気記録媒体があるが、いずれも磁性層を直
接的に磁化するものとなっていた。
Conventionally, recording media such as recording memories and memory cards for personal computers have been magnetic recording media using magnetic materials, such as magnetic tapes, floppy disks, hard disks, magnetic cards, and magneto-optical disks. This type of magnetic recording medium is manufactured by laminating a magnetic layer and a protective layer on a substrate, and records are made by applying a magnetic field to each magnetic domain of the magnetic layer using a magnetic field or the like. In this case, there are magnetic recording media that use a method of horizontal magnetization and a method of perpendicular magnetization and optical detection, but in both cases the magnetic layer is directly magnetized.

〔発明を解決しようとする課題〕[Problems to be solved by the invention]

しかしながら、上記従来のフロッピーディスクやハード
ディスク等の磁気記録媒体は、使用する磁性体材料によ
り保磁力、および磁気モーメントなどの磁気的性質が限
定されており自由に変化させることができないという問
題があった。また、利用できる磁性体が限定されるでい
るため、高い保磁力が得られないという欠点があった。
However, the above conventional magnetic recording media such as floppy disks and hard disks have a problem in that magnetic properties such as coercive force and magnetic moment are limited depending on the magnetic material used, and cannot be changed freely. . Furthermore, since the usable magnetic materials are limited, there is a drawback that a high coercive force cannot be obtained.

しかも磁区の境界で磁化方向が不明瞭となることがあり
、記録密度が充分に大きくならない問題もあった。
Moreover, the magnetization direction may become unclear at the boundaries of magnetic domains, and there is also the problem that the recording density cannot be sufficiently increased.

本発明は、高い保磁力と記録密度を増しても充分な信号
区分が可能であり、記録信号の自由度を増すことのでき
る超電導磁気記録媒体とその製造方法および記録方法を
提供することを目的とする。
An object of the present invention is to provide a superconducting magnetic recording medium, a method for producing the same, and a recording method for the same, which can sufficiently divide signals even with increased coercive force and recording density, and increase the degree of freedom of recorded signals. shall be.

より具体的には、超電導材からなる微小環をテープやデ
ィスク等の基板上に配置してこれを磁性媒体とし、また
、外部磁場を変化させることで垂直磁気モーメントの向
き及び大きさを自由に変化させることを可能とする。ま
た、磁性媒体中にこの微小環を配置することで、容易に
垂直磁気モーメントを発生させることを可能にし、いま
まで磁性記録媒体として使用できなかった軟磁性材料を
記録媒体として用いることを可能とするものである。
More specifically, by placing a microring made of superconducting material on a substrate such as a tape or disk and using it as a magnetic medium, the direction and magnitude of the perpendicular magnetic moment can be freely controlled by changing the external magnetic field. Allows for change. In addition, by arranging this microring in a magnetic medium, it is possible to easily generate a perpendicular magnetic moment, making it possible to use soft magnetic materials as a recording medium, which until now could not be used as a magnetic recording medium. It is something to do.

[問題を解決するための手段] 上記目的を達成するために、本発明に係る超電導磁気記
録媒体は、基板上に記録単位を構成する超電導材微小環
を配列した記録層を設け、前記各超電導材微小環に外部
磁場を印加することにより前記微小環に発生した環状電
流により垂直磁気モーメントを誘起可能としたものであ
る。また、前記記録層の超電導材微小環の少なくとも環
内に軟磁性体を設ける構成とすることもできる。更には
、前記超電導微小環を含む記録層を2層以上形成して多
層化構造とすることも可能である。
[Means for Solving the Problem] In order to achieve the above object, a superconducting magnetic recording medium according to the present invention includes a recording layer in which superconducting material micro-rings constituting recording units are arranged on a substrate, and each of the superconducting By applying an external magnetic field to the material microring, a perpendicular magnetic moment can be induced by a circular current generated in the microring. Furthermore, a soft magnetic material may be provided at least within the superconducting material microring of the recording layer. Furthermore, it is also possible to form a multilayer structure by forming two or more recording layers containing the superconducting microrings.

また、本発明に係る超電導磁気記録媒体の製造方法は、
基板上に蒸着により超電導膜を形成した後にホトレジス
トおよびエツチングにより多数の微小環を残存配列し、
この微小環の周囲に非磁性膜または磁性膜を形成して記
録層を形成し、記録層の外層に保護膜を形成するものと
する。
Further, the method for manufacturing a superconducting magnetic recording medium according to the present invention includes:
After forming a superconducting film on a substrate by vapor deposition, a large number of remaining micro rings are arranged by photoresist and etching.
A recording layer is formed by forming a nonmagnetic film or a magnetic film around this microring, and a protective film is formed on the outer layer of the recording layer.

更に、本発明に係る超電導磁気記録媒体の記録方法は、
基板上に記録単位を構成する超電導材微小環を配列した
記録層を設けた超電導磁気記録媒体の前記各微小環に記
録信号に応じた外部磁場を印加することにより垂直磁気
モーメントを誘起させ、この記録信号を磁気ヘッドによ
り再生可能とした。また、基板上に記録単位を構成する
超電導材微小環を配列した記録層を設けた超電導磁気記
録媒体に一様な外部磁界を印加して垂直磁気モーメント
を誘起した後、記録信号に応じて微小環をレーザ光を照
射して超電導破壊をなすことにより前記垂直磁気モーメ
ントを消去し、垂直磁気モーメントの有無によりデジタ
ル信号を形成する構成としている。
Furthermore, the recording method of the superconducting magnetic recording medium according to the present invention includes:
A perpendicular magnetic moment is induced by applying an external magnetic field according to a recording signal to each of the microrings of a superconducting magnetic recording medium, which has a recording layer in which microrings of superconducting material constituting recording units are arranged on a substrate. Recorded signals can be reproduced using a magnetic head. In addition, after inducing a perpendicular magnetic moment by applying a uniform external magnetic field to a superconducting magnetic recording medium, which has a recording layer in which superconducting material microrings constituting recording units are arranged on a substrate, The perpendicular magnetic moment is erased by irradiating the ring with a laser beam to break the superconductivity, and a digital signal is generated depending on the presence or absence of the perpendicular magnetic moment.

〔作用〕[Effect]

この発明によれば、超電導材製の微小環に垂直外部磁場
を印加することで右ねじの法則により微小環に環状電流
が流れる。垂直外部磁場を取り除いた後も微小環には、
超電導現象により環状電流が流れ続は垂直磁気モーメン
トが残留し、これを磁気記録として利用する。今まで保
磁力が小さいため記録媒体として使用できなかった軟磁
性材料をこの微小環と併用することで記録媒体として使
用することによってより高い保磁力を持たせるこ= 6 とができる。また、超電導材微小環を存する記録層を微
小環相互が重ならないように多層化することにより、記
録密度を大幅に向上することができる。前記超電導磁気
記録媒体は、基板状に超電導材を物理的蒸着あるいは化
学的蒸着して超電導膜を成膜し、これをホトレジスト、
エツチング法などにより所望の微小環を簡単に形成でき
る。したがって非常に簡便に超電導材微小環を有する磁
気記録媒体を製作することが可能となっている。また、
上記磁気記録媒体に対し、記録信号に基づく外部磁場を
印加することにより、各超電導材微小環には印加磁界の
方向と大きさにしたがった垂直磁気モーメントが発生し
、これを磁気ヘッドにより読み取ることで記録再生がで
きる。また、磁気記録媒体に対し予め一様な外部磁場に
置いて環状電流を生成させておき、デジタル信号に対応
するように所定の微小環にレーザ光を照射すればその超
電導状態が破壊されて垂直磁気モーメントが消滅する。
According to this invention, by applying a vertical external magnetic field to a microring made of a superconducting material, a circular current flows through the microring according to the right-handed screw rule. Even after removing the vertical external magnetic field, the microannulus remains
Due to the superconducting phenomenon, a circular current flows and a perpendicular magnetic moment remains, which is used for magnetic recording. A soft magnetic material, which until now could not be used as a recording medium due to its small coercive force, can be given a higher coercive force by using it as a recording medium in combination with this microring. Further, by forming a multilayer recording layer containing superconducting material micro-rings so that the micro-rings do not overlap with each other, the recording density can be greatly improved. The superconducting magnetic recording medium is produced by forming a superconducting film by physically or chemically depositing a superconducting material on a substrate, and then applying a photoresist or a superconducting film to the substrate.
Desired micro-rings can be easily formed by etching or the like. Therefore, it is possible to manufacture a magnetic recording medium having a superconducting material microring very easily. Also,
By applying an external magnetic field based on a recording signal to the magnetic recording medium, a perpendicular magnetic moment is generated in each superconducting microring according to the direction and magnitude of the applied magnetic field, and this is read by a magnetic head. You can record and play back. In addition, if a magnetic recording medium is placed in a uniform external magnetic field in advance to generate a ring current, and a laser beam is irradiated onto a predetermined micro ring in response to a digital signal, the superconducting state is destroyed and the vertical current is generated. The magnetic moment disappears.

したがって垂直磁気モーメントの有無により当該磁気記
録媒体にデジタル信号の記録ができる。その読み取りは
カー効果やファラデー効果によって識別できる。
Therefore, digital signals can be recorded on the magnetic recording medium depending on the presence or absence of the perpendicular magnetic moment. The reading can be identified by the Kerr effect or Faraday effect.

〔実施例〕〔Example〕

以下に、本発明に係る超電導磁気記録媒体とその製造方
法および記録方法の具体的実施例を図面を参照して詳細
に説明する。
EMBODIMENT OF THE INVENTION Below, specific examples of a superconducting magnetic recording medium, its manufacturing method, and a recording method according to the present invention will be described in detail with reference to the drawings.

第1図は実施例に係る超電導磁気記録媒体lOの部分斜
視図である。この図に示すように、超電導磁気記録媒体
10は多数の超電導材微小環12をディスク基板14に
渦巻き線に沿って整列して配置されている。この微小環
12はイツトリウム系、タリウム系酸化物等の超電導材
料によって形成されており、直径をμm単位の極小サイ
ズとしている。
FIG. 1 is a partial perspective view of a superconducting magnetic recording medium IO according to an example. As shown in this figure, a superconducting magnetic recording medium 10 has a large number of superconducting micro-rings 12 arranged on a disk substrate 14 in alignment along a spiral line. The micro ring 12 is made of a superconducting material such as yttrium-based or thallium-based oxide, and has a diameter as small as micrometers.

このような磁気記録媒体10ば、第2図に示したような
方法で製造される。すなわち、ディスク基板14の片面
にイツトリウム系、タリウム系酸化物等の超電導材料を
PVD法、CVD法、あるいはスパッタリング法により
拡散蒸着させる。この超電導膜16を数μmまで成長さ
せた後、紫外線硬化樹脂等のホトレジスト18を成膜し
、このホトレジスト18に対し微小環12に相当する紫
外線等を照射してリング状に硬化させた型20を形成す
る。これはディスク基板14に形成すべきトラック線に
沿って所定ピッチで多数形成するのはいうまでもない。
Such a magnetic recording medium 10 is manufactured by the method shown in FIG. That is, a superconducting material such as yttrium-based or thallium-based oxide is diffused and deposited on one side of the disk substrate 14 by PVD, CVD, or sputtering. After growing this superconducting film 16 to several micrometers, a photoresist 18 such as an ultraviolet curable resin is formed, and this photoresist 18 is irradiated with ultraviolet rays corresponding to the micro rings 12 to harden it into a ring shape. form. Needless to say, a large number of these are formed at a predetermined pitch along the track line to be formed on the disk substrate 14.

そして、この型20の形成後に前記超電導膜16をエツ
チング処理し、当該型20に対応して超電導材微小環1
2を残存形成するのである。ディスク基板14上にはト
ラック線に沿って多数の微小環12が整列配置されるが
、この微小環12を被覆するように非磁性膜22、ある
いは軟磁性体の磁性膜24を形成し、これら微小環12
と非磁性膜22あるいは磁性膜24とからなる層を記録
層26とする。その後は外表面に保護膜28を成膜して
磁気記録媒体10が製造される。
After forming this mold 20, the superconducting film 16 is etched, and superconducting material micro-rings 1 are etched corresponding to the mold 20.
2 remains. A large number of micro-rings 12 are arranged along the track line on the disk substrate 14, and a non-magnetic film 22 or a magnetic film 24 made of soft magnetic material is formed to cover the micro-rings 12. Microcircle 12
A recording layer 26 is composed of a nonmagnetic film 22 or a magnetic film 24. Thereafter, a protective film 28 is formed on the outer surface, and the magnetic recording medium 10 is manufactured.

このように形成された磁気記録媒体10を印加磁界中に
通すことによって、各微小環12に垂直磁気モーメント
30を発生記録させることができる。すなわち、第3図
に示すように、記録する信号電流を入力し、これにより
信号磁力線32を微小環12の中心方向(図では上下方
向)に発生する記録手段34をトラック線に沿って移動
させる。
By passing the thus formed magnetic recording medium 10 through an applied magnetic field, a perpendicular magnetic moment 30 can be generated and recorded in each microring 12. That is, as shown in FIG. 3, a recording signal current is input, thereby causing a signal magnetic field line 32 to be generated in the direction of the center of the micro ring 12 (in the vertical direction in the figure), and the recording means 34 is moved along the track line. .

この記録手段34の与える印加磁界により微小環12に
は誘導起電力によって環状電流が流れ、これは微小環1
2が超電導材からなっているため永久電流として保存さ
れる。この場合において、超電導現象は現在のところ一
定の冷却状態のもとで現れているので、これらの一連の
処理は、第6図に示されるような冷却系内で行うものと
する。もちろん、常温超電導材が得られれば、冷却系外
にて可能となる。このようにして永久環状電流が流され
た微小環12には、右ねじの法則によって垂直磁気モー
メント30が発生し、これは前記信号磁力線32によっ
て方向、大きさが異なり、これば記録信号に対応してい
る(第5図参照)。
Due to the magnetic field applied by the recording means 34, a ring current flows in the micro ring 12 due to an induced electromotive force, and this causes a ring current to flow through the micro ring 12.
Since 2 is made of superconducting material, it is stored as a persistent current. In this case, since the superconducting phenomenon is currently occurring under a constant cooling condition, these series of processes are carried out in a cooling system as shown in FIG. Of course, if a room-temperature superconducting material is obtained, this can be done outside the cooling system. A perpendicular magnetic moment 30 is generated in the micro ring 12 through which a permanent ring current is passed in this way according to the right-handed screw law, and this has a different direction and magnitude depending on the signal magnetic field lines 32, and this corresponds to the recorded signal. (See Figure 5).

このようにして記録された磁気記録媒体10を用いて信
号再生を行うには磁気ヘッド36を用いればよい。すな
わち、第5図に示すように、磁気ヘッド36を磁気記録
媒体10のトラ゛ツク線に対応させ、両者を相対的に移
動させればよい。記録層26の各微小環12に記録保持
されている垂直MA気モーメント30は磁気ヘッド36
のコイルに着磁の方向、大きさに応じる出力電流が流れ
、これにより記録内容を磁気ヘッド36から検出するこ
とができるのである。
To reproduce signals using the magnetic recording medium 10 recorded in this manner, the magnetic head 36 may be used. That is, as shown in FIG. 5, the magnetic head 36 may be made to correspond to the track line of the magnetic recording medium 10, and the two may be moved relative to each other. The vertical MA moment 30 recorded and held in each micro ring 12 of the recording layer 26 is transferred to the magnetic head 36.
An output current corresponding to the direction and magnitude of magnetization flows through the coil, and thereby the recorded content can be detected from the magnetic head 36.

このような磁気記録媒体10とそのドライブユニット3
8は、第6図に示すように、冷却ボックス40内に収容
し、超電導現象の破壊がないようにする。
Such a magnetic recording medium 10 and its drive unit 3
8 is housed in a cooling box 40, as shown in FIG. 6, to prevent destruction of the superconducting phenomenon.

このように構成された磁気記録媒体10によれば、超電
導材微小環12を含む記録層26をディスク基板14に
形成し、各微小環12に記録信号に基づく環状電流を流
すことによって垂直磁気モーメント30を発生させるの
で、磁区の境界が明確になり、かつ記録密度を増しても
高い保磁力が得られる。特に磁性膜24に軟磁性体を採
用することができるので、記録に際しての立ち上がり性
能が良くなり、また保磁力がより向上する。
According to the magnetic recording medium 10 configured in this way, the recording layer 26 including the superconducting material micro-rings 12 is formed on the disk substrate 14, and the perpendicular magnetic moment is created by flowing a ring current based on the recording signal through each micro-ring 12. 30, the boundaries of the magnetic domains become clear and a high coercive force can be obtained even when the recording density is increased. In particular, since a soft magnetic material can be used for the magnetic film 24, the start-up performance during recording is improved and the coercive force is further improved.

次に第7図および第8図は前記記録層26を多層構造に
した磁気記録媒体10A、IOBの例である。第7図の
磁気記録媒体10Aは二層の記録層26を有するが、上
下の微小環12が同心配置となるようにしたものであり
、第8図の磁気記録媒体10Bは上下微小環12が重合
しないように位置をトラック線方向に位置をずらした配
置構成としたものである。前者の場合には垂直磁気モー
メント30の強度を高めて再生を容易にすることができ
、後者の場合には単位トラック当たりの微小環12数を
多くして記録密度を拡大することができる。
Next, FIGS. 7 and 8 show examples of magnetic recording media 10A and IOB in which the recording layer 26 has a multilayer structure. The magnetic recording medium 10A shown in FIG. 7 has a two-layer recording layer 26, with the upper and lower micro-rings 12 arranged concentrically, and the magnetic recording medium 10B shown in FIG. 8 has the upper and lower micro-rings 12 arranged concentrically. The arrangement is such that the positions are shifted in the track line direction to prevent overlapping. In the former case, the strength of the perpendicular magnetic moment 30 can be increased to facilitate reproduction, and in the latter case, the number of micro-rings 12 per unit track can be increased to increase the recording density.

第9図には前記磁気記録媒体10に対する記録方法を変
え、光磁気記録媒体として利用することができるように
したものである。この記録方法は、前述した磁気記録媒
体10を印加磁石42によって生成される一様な印加磁
界44におき、これによって各微小環12に環状電流を
発生させ、かつ垂直磁気モーメント30の方向を揃える
。そして、記録装置としてレーザ発光装置46を用い、
磁気記録媒体10を回転させながら所定の微小環12に
レーザ光を照射する。レーザ光が照射された微小環12
は超電導臨界温度以上に加熱され、超電導状態が破壊さ
れて常電導状態になる。これによってレーザ光が照射さ
れた微小環12はいわゆるビット48となり、垂直磁気
モーメント30の有無によりデジタル信号として記録さ
れるのである。
In FIG. 9, the recording method for the magnetic recording medium 10 is changed so that it can be used as a magneto-optical recording medium. This recording method places the magnetic recording medium 10 described above in a uniform applied magnetic field 44 generated by an applying magnet 42, thereby generating a circular current in each microring 12 and aligning the directions of the perpendicular magnetic moments 30. . Then, using a laser emitting device 46 as a recording device,
A predetermined micro ring 12 is irradiated with a laser beam while the magnetic recording medium 10 is rotated. Micro ring 12 irradiated with laser light
is heated above the superconducting critical temperature, the superconducting state is destroyed and it becomes a normal conducting state. As a result, the micro ring 12 irradiated with the laser beam becomes a so-called bit 48, which is recorded as a digital signal depending on the presence or absence of the perpendicular magnetic moment 30.

このように記録された光磁気記録媒体10を再生する場
合には垂直磁気モーメント30の有無によってレーザ光
の反射や透過光に偏光が生じるカー効果やファラデー効
果を利用して記録情報を読み出す。これは、第10図に
示すように、レーザ光源52から発射したレーザ光54
を偏光子55を通して各微小環12にて反射させ、検光
子56を通過させ光検出素子58で検出するようにする
が、垂直磁気モーメント30がある場合には反射光の偏
光面が角度θだけ回転し、垂直磁気モーメント30が消
磁されている場合にはθ−0となる。
When reproducing the magneto-optical recording medium 10 recorded in this manner, the recorded information is read out using the Kerr effect and the Faraday effect, in which reflected or transmitted laser light is polarized depending on the presence or absence of the perpendicular magnetic moment 30. As shown in FIG. 10, the laser beam 54 emitted from the laser light source 52
is reflected by each micro ring 12 through a polarizer 55, passed through an analyzer 56, and detected by a light detection element 58. However, if there is a perpendicular magnetic moment 30, the polarization plane of the reflected light changes by an angle θ. When it rotates and the vertical magnetic moment 30 is demagnetized, it becomes θ-0.

したがってθの値により「1」、「0」の判別ができ、
これによってデジタル信号として記録された信号を検出
することができる。
Therefore, it is possible to distinguish between "1" and "0" by the value of θ,
This makes it possible to detect signals recorded as digital signals.

前記光磁気記録媒体IOの記録を消去する場合は、第1
1図に示すように、印加磁石42を走査させ、全部の微
小環12に垂直磁気モーメント30を発生させればよい
When erasing the record on the magneto-optical recording medium IO, the first
As shown in FIG. 1, the application magnet 42 may be scanned to generate a perpendicular magnetic moment 30 in all the micro-rings 12.

なお、光磁気記録媒体10における記録層26を構成す
る磁性膜24には、Biを多量置換したイツトリウム鉄
ガーネット(YTG)、稀土類鉄ガーネット(GIG)
を用いる。これにより特にヴエルデ定数を大きくできフ
ァラデー効果を利用した再生が容易になる効果が得られ
る。
The magnetic film 24 constituting the recording layer 26 of the magneto-optical recording medium 10 is made of yttrium iron garnet (YTG) with a large amount of Bi substituted, rare earth iron garnet (GIG), etc.
Use. This particularly has the effect of increasing the Welde constant and facilitating regeneration using the Faraday effect.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明によれば、超電導材微小環
により大きさ方向を自由に変えられる垂直磁気モーメン
トをもつ新しい磁気記録媒体として利用することができ
るとともに、従来の磁性媒体と併用することで立ち上が
りに優れた垂直磁気モーメントの生成を可能とし、軟磁
性体の使用も可能となる効果が得られる。そして、記録
方法の選択により光磁気記録媒体としても利用すること
ができ、特に高い記録密度にしつつ記録再生が容易であ
って、消去やオーバライドの可能な光磁気記録媒体とす
ることができる。すなわち、本発明は、高い保磁力と記
録密度を増しても充分な信号区分が可能であり、記録信
号の自由度を増すことのできる超電導磁気記録媒体とそ
の製造方法および記録方法であって、超電導材からなる
微小環をテープやディスク等の基板上に配置してこれを
磁性媒体とし、また、外部磁場を変化させることで垂直
磁気モーメントの向き及び大きさを自由に変化させるこ
とを可能となる。また、磁性媒体中にこの微小環を配置
することで、容易に垂直磁気モーメントを発生させるこ
とを可能にし、いままで磁性記録媒体として使用できな
かった軟磁性材料を記録媒体として用いることが可能と
なる。
As explained above, according to the present invention, it can be used as a new magnetic recording medium that has a perpendicular magnetic moment whose size direction can be freely changed due to superconducting material microrings, and it can also be used in combination with conventional magnetic media. This makes it possible to generate a perpendicular magnetic moment with excellent rise, and allows the use of soft magnetic materials. Depending on the recording method, it can also be used as a magneto-optical recording medium, and can be used as a magneto-optical recording medium that can be easily recorded and reproduced while achieving particularly high recording density, and can be erased and overridden. That is, the present invention provides a superconducting magnetic recording medium, a method for manufacturing the same, and a recording method for the same, in which sufficient signal division is possible even with increased coercive force and recording density, and the degree of freedom of recorded signals is increased. A micro ring made of superconducting material is placed on a substrate such as a tape or disk and used as a magnetic medium, and by changing the external magnetic field, it is possible to freely change the direction and magnitude of the perpendicular magnetic moment. Become. In addition, by arranging this microring in a magnetic medium, it is possible to easily generate a perpendicular magnetic moment, making it possible to use soft magnetic materials as a recording medium, which until now could not be used as a magnetic recording medium. Become.

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

第1図は実施例に係る磁気記録媒体の部分斜視図、第2
図はその製造方法の説明図、第3回は磁気記録媒体にお
ける環状電流の発生状態の説明図、第4図は環状電流に
よる垂直磁気モーメントの発生状態の説明図、第5図は
磁気記録媒体からの記録再生状態の説明図、第6図は冷
却系の説明図、第7図は磁気記録媒体の記録層を多層化
した変形実施例の部分断面図、第8図は更に他の多層構
造の磁気記録媒体の部分断面図、第9図は磁気記録媒体
を光磁気記録媒体として利用する場合の記録方法の説明
図、第10図は光磁気記録媒体の続出原理の説明図、第
11図は光磁気記録媒体の記録消去の説明図である。 10、IOA、IOB・・・・・・超電導磁気記録媒水
12・・・・・・超電導材微小環、14・・・・・・デ
ィスク基板、16・・・・・・超電導膜、18・・・・
・・ホトレジスト、22・・・・・・非磁性膜、24・
・・・・・磁性膜、26・・・・・・記録層、28・・
・・・・保護膜、30・・・・・・垂直磁気モーメント
、36・・・・・・磁気ヘッド、46・・・・・・レー
ザ発光装置、52・・・・・・レーザ光源、54・・・
・・・レーザ光。
FIG. 1 is a partial perspective view of a magnetic recording medium according to an embodiment, and FIG.
The figure is an explanatory diagram of the manufacturing method, Part 3 is an explanatory diagram of the state in which a circular current is generated in the magnetic recording medium, Figure 4 is an explanatory diagram of the state in which the perpendicular magnetic moment is generated by the circular current, and Figure 5 is the magnetic recording medium FIG. 6 is an explanatory diagram of the cooling system, FIG. 7 is a partial cross-sectional view of a modified embodiment in which the recording layer of the magnetic recording medium is multilayered, and FIG. 8 is a further example of another multilayer structure. FIG. 9 is an explanatory diagram of the recording method when the magnetic recording medium is used as a magneto-optical recording medium, FIG. 10 is an explanatory diagram of the principle behind the successive development of magneto-optical recording media, and FIG. 11 FIG. 2 is an explanatory diagram of recording and erasing of a magneto-optical recording medium. 10, IOA, IOB... superconducting magnetic recording medium water 12... superconducting material micro ring, 14... disk substrate, 16... superconducting film, 18... ...
...Photoresist, 22...Nonmagnetic film, 24.
...Magnetic film, 26...Recording layer, 28...
...Protective film, 30... Perpendicular magnetic moment, 36... Magnetic head, 46... Laser light emitting device, 52... Laser light source, 54 ...
...Laser light.

Claims (6)

【特許請求の範囲】[Claims] (1)、基板上に記録単位を構成する超電導材微小環を
配列した記録層を設け、前記各超電導材微小環に外部磁
場を印加することにより前記微小環に発生した環状電流
により垂直磁気モーメントを誘起可能としたことを特徴
とする超電導磁気記録媒体。
(1) A recording layer in which superconducting material micro-rings constituting a recording unit are arranged is provided on a substrate, and by applying an external magnetic field to each of the superconducting material micro-rings, a perpendicular magnetic moment is generated by an annular current generated in the micro-rings. A superconducting magnetic recording medium characterized by being capable of inducing.
(2)、前記記録層の超電導材微小環の少なくとも環内
に軟磁性体を設けたことを特徴とする請求項1に記載の
超電導磁気記録媒体。
(2) The superconducting magnetic recording medium according to claim 1, characterized in that a soft magnetic material is provided at least within the superconducting material microring of the recording layer.
(3)、前記超電導微小環を含む記録層を2層以上形成
したことを特徴とする請求項1に記載の超電導磁気記録
媒体。
(3) The superconducting magnetic recording medium according to claim 1, characterized in that two or more recording layers containing the superconducting microrings are formed.
(4)、基板上に物理的蒸着法あるいは化学的蒸着法に
より超電導膜を形成した後に多数の微小環を残存配列し
、この微小環の周囲に非磁性膜または磁性膜を形成して
記録層を形成し、記録層の外層に保護膜を形成すること
を特徴とする超電導磁気記録媒体の製造方法。
(4) After forming a superconducting film on a substrate by physical vapor deposition or chemical vapor deposition, a large number of micro-rings remain and are arranged, and a non-magnetic film or a magnetic film is formed around these micro-rings to form a recording layer. 1. A method of manufacturing a superconducting magnetic recording medium, comprising forming a protective film on the outer layer of the recording layer.
(5)、基板上に記録単位を構成する超電導材微小環を
配列した記録層を設けた超電導磁気記録媒体の前記各微
小環に記録信号に応じた外部磁場を印加することにより
垂直磁気モーメントを誘起させ、この記録信号を磁気ヘ
ッドにより再生可能としたことを特徴とする超電導磁気
記録媒体の記録方法。
(5) A perpendicular magnetic moment is generated by applying an external magnetic field according to a recording signal to each microring of a superconducting magnetic recording medium, which has a recording layer in which superconducting material microrings constituting a recording unit are arranged on a substrate. 1. A method for recording a superconducting magnetic recording medium, characterized in that the recorded signal is made reproducible by a magnetic head.
(6)、基板上に記録単位を構成する超電導材微小環を
配列した記録層を設けた超電導磁気記録媒体に一様な外
部磁界を印加して垂直磁気モーメントを誘起した後、記
録信号に応じて微小環をレーザ光を照射して超電導破壊
をなすことにより前記垂直磁気モーメントを消去し、垂
直磁気モーメントの有無によりデジタル信号を形成する
ことを特徴とする超電導磁気記録媒体の記録方法。
(6) After inducing a perpendicular magnetic moment by applying a uniform external magnetic field to a superconducting magnetic recording medium having a recording layer in which superconducting material micro-rings constituting recording units are arranged on a substrate, A method for recording a superconducting magnetic recording medium, characterized in that the perpendicular magnetic moment is erased by irradiating the microring with a laser beam to destroy the superconductivity, and a digital signal is formed depending on the presence or absence of the perpendicular magnetic moment.
JP2160989A 1989-01-31 1989-01-31 Superconducting magnetic recording medium and production thereof and recording method Pending JPH02201726A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2160989A JPH02201726A (en) 1989-01-31 1989-01-31 Superconducting magnetic recording medium and production thereof and recording method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2160989A JPH02201726A (en) 1989-01-31 1989-01-31 Superconducting magnetic recording medium and production thereof and recording method

Publications (1)

Publication Number Publication Date
JPH02201726A true JPH02201726A (en) 1990-08-09

Family

ID=12059779

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2160989A Pending JPH02201726A (en) 1989-01-31 1989-01-31 Superconducting magnetic recording medium and production thereof and recording method

Country Status (1)

Country Link
JP (1) JPH02201726A (en)

Similar Documents

Publication Publication Date Title
JPH0997419A (en) Magnetic disk, method of manufacturing magnetic disk, and magnetic recording device
US5978186A (en) Magnetic head and reproducing apparatus with head having central core with winding thereabout and wire therethrough
JPS5963005A (en) Magnetic recording system
US3793639A (en) Device for the magnetic storage of data
US7738203B2 (en) Magnetic recording medium Formatted with ROM and RAM regions
JPH02201726A (en) Superconducting magnetic recording medium and production thereof and recording method
JP4036602B2 (en) Master disk positioning mark recognition method
JPH0442417A (en) Magnetic head and magnetoresistive element
EP0178423A2 (en) Magneto-optical recording medium
JPS6289201A (en) magnetic recording and reproducing device
JP2661472B2 (en) Recording medium and its recording / reproducing method
JP3443971B2 (en) Magnetic recording signal reproduction method
JPH11185312A (en) Magneto-optical recording medium
JPH05182266A (en) Magneto-optical recording medium and manufacturing method thereof
JP2812113B2 (en) Recording medium and its recording / reproducing method
Kryder Magnetic information storage
JPH10334422A (en) Magnetic recording device
JPS581802A (en) Magnetic recording and reproducing system and magnetic head
JPH01223649A (en) Magneto-optical disk carrier and its manufacture
JP2000215402A (en) Information recording medium, information recording / reproducing method, and information recording / reproducing device
JPH0793837A (en) Magnetic recording / reproducing method and reproducing head using the same
JPH02187918A (en) Magnetic recording medium
JPH03113854A (en) Recording and playback method
JP2001195702A (en) Information recording method, information recording reproducing method, and information recording medium
JPH0456363B2 (en)