JPH0439726B2 - - Google Patents
Info
- Publication number
- JPH0439726B2 JPH0439726B2 JP59251724A JP25172484A JPH0439726B2 JP H0439726 B2 JPH0439726 B2 JP H0439726B2 JP 59251724 A JP59251724 A JP 59251724A JP 25172484 A JP25172484 A JP 25172484A JP H0439726 B2 JPH0439726 B2 JP H0439726B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetization
- magnetic field
- magnetic
- medium
- light
- 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 - Lifetime
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
Landscapes
- Recording Or Reproducing By Magnetic Means (AREA)
Description
【発明の詳細な説明】
[発明の技術分野]
この発明は、磁性媒体の面に光を照射して該媒
体の光照射部分の温度を上昇せしめることにより
保磁力を低下させられた前記光照射部分に磁場を
印加して前記光照射部分の磁化方向を印加磁場の
方向に設定する熱磁気記録方式に関する。Detailed Description of the Invention [Technical Field of the Invention] The present invention provides a method for reducing the coercive force by irradiating light onto the surface of a magnetic medium and increasing the temperature of the light irradiated portion of the medium. The present invention relates to a thermomagnetic recording method in which a magnetic field is applied to a portion and the magnetization direction of the light irradiated portion is set in the direction of the applied magnetic field.
[発明の技術的背景および問題点]
熱磁気記録方式は、大容量の情報記憶装置を得
る手段として従来から着目されているものであ
る。この熱磁気記録方式は、平板状の磁性媒体に
該媒体の常温における保磁力(Hc)より小さい
磁場を印加しつつ微小径に集光した光を照射して
該媒体の光照射部分の温度を上昇せしめ、温度上
昇による媒体の保磁力の低下を利用して前記光照
射部分の磁化方向を印加磁場の方向にならわせる
ものであり、光磁気記録方式とも称されている。[Technical Background and Problems of the Invention] The thermomagnetic recording method has been attracting attention as a means of obtaining a large-capacity information storage device. This thermomagnetic recording method applies a magnetic field smaller than the coercive force (Hc) of the medium at room temperature to a flat magnetic medium, and irradiates the medium with light focused on a minute diameter, thereby increasing the temperature of the light-irradiated portion of the medium. This method uses the decrease in the coercive force of the medium due to the temperature rise to align the magnetization direction of the light irradiated portion with the direction of the applied magnetic field, and is also called a magneto-optical recording method.
熱磁気記録方式には、媒体の磁化容易軸が該媒
体の面に垂直であつて、媒体面の垂直方向に磁化
を残留せしめる垂直熱磁気記録方式と、媒体面内
に磁化を残留せしめる水平熱磁気記録方式とがあ
る。また、媒体材料の温度上昇による保磁力変化
の特性によりキユーリ温度記録方式と補償温度記
録方式に分けられる。例えば、Tb−Fe材を用い
る記録はキユーリ温度記録型垂直熱磁気記録方
式、Gd−Co材を用いる記録は補償温度記録型垂
直熱磁気記録方式、CrO2を用いる記録はキユー
リ温度記録型水平熱磁気記録方式である。 There are two types of thermomagnetic recording methods: vertical thermomagnetic recording, in which the axis of easy magnetization of the medium is perpendicular to the surface of the medium, and magnetization remains in the direction perpendicular to the surface of the medium, and horizontal thermomagnetic recording, in which magnetization remains in the plane of the medium. There is a magnetic recording method. Furthermore, depending on the characteristics of coercive force change due to temperature rise of the medium material, it can be divided into the Kuyuri temperature recording method and the compensated temperature recording method. For example, recording using Tb-Fe material is based on the Currie temperature recording vertical thermomagnetic recording method, recording using Gd-Co material is using the compensated temperature recording type vertical thermomagnetic recording method, and recording using CrO 2 is using the Cuyuri temperature recording type horizontal thermal recording method. It is a magnetic recording method.
ところでこのようないずれの方式においても、
光を微小スポツトに絞つて媒体を昇温せしめて記
録を行なつているので、通常の磁気記録に比べて
高いトラツク密度が得られるという特徴がある反
面、微小な領域に情報を記録する結果、媒体に微
小な欠陥があると、エラーとなりやすい問題が従
来あつた。また、微小な領域に正確に位置決めし
て記録再生を行なう必要があるため、光の位置決
め装置が複雑となり、部品数、回路構成が多く、
価格が高くなるという問題も従来あつた。更に、
集光できる最小の径は原理的に光の波長で制限さ
れるため、一層の高密度化は困難であるという欠
点もある。 By the way, in any of these methods,
Since recording is performed by focusing the light onto a tiny spot and raising the temperature of the medium, it is characterized by a higher track density than normal magnetic recording, but as a result of recording information in a tiny area, Conventionally, there has been a problem that small defects in media tend to cause errors. In addition, since it is necessary to accurately position in a minute area to perform recording and playback, the optical positioning device becomes complex, requiring a large number of parts and circuit configurations.
There has also been the problem of high prices. Furthermore,
Since the minimum diameter that can be focused is theoretically limited by the wavelength of the light, there is also the drawback that it is difficult to further increase the density.
また、記録方法としてみた場合、一定の磁場を
印加しつつ瞬時的に光を照射して記録を行なう磁
場バイアス型と、相対的に移動する媒体に連続的
に光を照射しつつ磁場を反転せしめて記録を行な
う熱バイアス型とがあるが、磁場バイアス型では
新たに情報を記録する前に予め消去を行なう必要
があり、また熱バイアス型では記録密度を高くで
きないという欠点がある。 In terms of recording methods, there are two types: magnetic field bias type, which performs recording by instantaneously irradiating light while applying a constant magnetic field; There is a thermal bias type in which recording is performed using a magnetic field, but the magnetic field bias type requires erasing before new information can be recorded, and the thermal bias type has the disadvantage that it is not possible to increase the recording density.
[発明の目的]
この発明は、上記に鑑みてなされたもので、そ
の目的とするところは、情報の記録を、高密度か
つ、高信頼性をもつて行なえるようにした熱磁気
記録方式を提供することにある。[Object of the Invention] This invention has been made in view of the above, and its purpose is to provide a thermomagnetic recording method that allows information to be recorded with high density and high reliability. It is about providing.
[発明の概要]
上記目的を達成するため、この発明は、面内の
磁化特性が等方的な多結晶構造の磁気媒体と、前
記磁気媒体の前記面の所望の位置に所定の大きさ
に集光した光を照射する光照射手段と、該光照射
手段によつて光を照射された前記所望の位置の面
内に所望の方向の磁化を残留させ、該磁化の方向
により情報を記憶すべく、少なくとも前記所望の
位置の面内に前記磁化の方向に対応する磁場を印
加する磁場印加手段とを有することを要旨とす
る。[Summary of the Invention] In order to achieve the above object, the present invention provides a magnetic medium having a polycrystalline structure with isotropic in-plane magnetization characteristics, and a magnetic medium having a predetermined size at a desired position on the surface of the magnetic medium. A light irradiation means for irradiating condensed light, and magnetization in a desired direction remaining in the plane of the desired position irradiated with light by the light irradiation means, and information is stored according to the direction of the magnetization. In order to achieve this, the present invention includes a magnetic field applying means for applying a magnetic field corresponding to the direction of magnetization at least within the plane of the desired position.
[発明の実施例]
以下、図面を用いてこの発明の実施例を説明す
る。[Embodiments of the Invention] Examples of the invention will be described below with reference to the drawings.
第1図はこの発明の一実施例を示すものであ
る。同図において、平板状四辺形の磁気媒体1は
該媒体の面内方向で等方的な磁化特性を有する等
方性磁性材料、例えば多結晶γFe2O3薄膜、Co−
P系合金薄膜等で形成されている。この磁気媒体
1の各辺の側近には各辺に平行に棒状の直交磁場
発生器3,5,7,9がそれぞれ配設されてい
る。また、磁気媒体1の表面には光偏向器13で
偏向され集光装置15で集光された光源11から
の光が照射され、この照射された部分の磁気媒体
1の温度を上昇させるようになつている。そし
て、この温度が媒体のキユーリ温度に近づくにつ
れて磁気媒体1のその部分の保磁力が低下するよ
うになつている。 FIG. 1 shows an embodiment of the present invention. In the figure, a flat quadrilateral magnetic medium 1 is made of an isotropic magnetic material having isotropic magnetization characteristics in the in-plane direction of the medium, such as a polycrystalline γFe 2 O 3 thin film, Co-
It is formed of a P-based alloy thin film or the like. Near each side of the magnetic medium 1, rod-shaped orthogonal magnetic field generators 3, 5, 7, and 9 are arranged parallel to each side. Further, the surface of the magnetic medium 1 is irradiated with light from the light source 11 that is deflected by the optical deflector 13 and focused by the condenser 15, and the temperature of the irradiated portion of the magnetic medium 1 is increased. It's summery. As this temperature approaches the Curie temperature of the medium, the coercive force of that portion of the magnetic medium 1 decreases.
直交磁場発生器3,5,7,9はそれぞれ磁気
媒体1の面内、すなわち第1図に示すXYZ軸に
おいてXY面内に所定の方向の磁場を発生するよ
うになつている。更に詳しくは、例えば直交磁場
発生器3はY軸の正方向を向いた磁場、直交磁場
発生器5はX軸の正方向を向いた磁場、直交磁場
発生器7はY軸の負方向を向いた磁場、直交磁場
発生器9はX軸の負方向を向いた磁場をそれぞれ
発生するようになつている。そして、直交磁場発
生器3,5,7,9は図示しない制御装置により
制御されていずれかが作動し、磁気媒体1の面内
にその作動した直交磁場発生器により発生する所
定方向の磁場が印加されるようになつている。ま
た、この場合、2つ以上の直交磁場発生器を同時
に作動して両直交磁場発生器が発生する磁場の合
成により形成される方向の磁場を磁気媒体1に印
加するようにしてもよい。 The orthogonal magnetic field generators 3, 5, 7, and 9 are each designed to generate a magnetic field in a predetermined direction within the plane of the magnetic medium 1, that is, within the XY plane of the XYZ axes shown in FIG. More specifically, for example, the orthogonal magnetic field generator 3 generates a magnetic field oriented in the positive direction of the Y-axis, the orthogonal magnetic field generator 5 generates a magnetic field oriented in the positive direction of the X-axis, and the orthogonal magnetic field generator 7 generates a magnetic field oriented in the negative direction of the Y-axis. The orthogonal magnetic field generator 9 is designed to generate a magnetic field directed in the negative direction of the X-axis. Then, one of the orthogonal magnetic field generators 3, 5, 7, and 9 is operated under the control of a control device (not shown), and a magnetic field in a predetermined direction is generated in the plane of the magnetic medium 1 by the operated orthogonal magnetic field generator. It is starting to be applied. Further, in this case, two or more orthogonal magnetic field generators may be operated simultaneously to apply a magnetic field to the magnetic medium 1 in a direction formed by combining the magnetic fields generated by both orthogonal magnetic field generators.
以上のように構成されたものにおいて、磁気媒
体1の面内の所望の位置に所望の磁気情報を記憶
するには、前記光源11からの光を光偏向器13
および集光装置15で制御して磁気媒体1の所望
の位置の面に照射すると共に、前記直交磁場発生
器3,5,7,9のいずれかを駆動して該駆動さ
れた直交磁場発生器が発生する所望の方向の磁場
を前記光照射部分に印加するようにする。する
と、前記光が照射された部分はその温度が上昇し
て該部分の磁気媒体1の保磁力は低下するため、
この部分の磁気媒体1の磁化は前記直交磁場発生
器から印加される磁場の方向に配列される。この
ようにして該部分の磁化の方向を所望の方向に配
列した後、光の照射を停止すれば、該部分には磁
化の方向による情報が記憶されることになるので
ある。 In the device configured as described above, in order to store desired magnetic information at a desired position within the plane of the magnetic medium 1, the light from the light source 11 is directed to the optical deflector 13.
and irradiates the surface of the magnetic medium 1 at a desired position by controlling the light condensing device 15, and drives any of the orthogonal magnetic field generators 3, 5, 7, and 9 to generate the driven orthogonal magnetic field generator. A magnetic field generated in a desired direction is applied to the light irradiated portion. Then, the temperature of the portion irradiated with the light rises and the coercive force of the magnetic medium 1 in that portion decreases.
The magnetization of the magnetic medium 1 in this portion is aligned in the direction of the magnetic field applied from the orthogonal magnetic field generator. After arranging the direction of magnetization of the portion in a desired direction in this manner, if light irradiation is stopped, information based on the direction of magnetization will be stored in the portion.
すなわち、本発明の熱磁気記録装置において
は、磁化の方向により情報を記憶しているのであ
る。これは従来のものが1つのある単位記憶領
域、すなわち1つの情報を記憶する単位記憶領域
において一方向の磁化の反転を利用して2値の情
報(すなわち、1ビツト)を記憶していたのに対
して、本発明の熱磁気記録装置においては1つの
ある単位記憶領域における磁化の方向により情報
を記憶しており、その磁化の方向の数に相当する
数の多くの情報を1つの単位記憶領域に記憶する
ことができ、飛躍的に記憶容量を増大することが
できるものである。 That is, in the thermomagnetic recording device of the present invention, information is stored according to the direction of magnetization. This is because conventional devices store binary information (i.e., 1 bit) using reversal of magnetization in one direction in one unit storage area, that is, a unit storage area that stores one piece of information. On the other hand, in the thermomagnetic recording device of the present invention, information is stored according to the direction of magnetization in one unit storage area, and a large amount of information corresponding to the number of directions of magnetization is stored in one unit storage area. It can be stored in an area, and the storage capacity can be dramatically increased.
より具体的には、磁気媒体1の面内における磁
化方向を例えば16の方向に分割、すなわち22.5゜
ずつの等角度間隔で16の方向に分割して記憶でき
るように制御すれば、1つの単位記憶領域、例え
ば前記集光された光が照射される最小の単位記憶
領域で16の情報、すなわち4ビツト相当の情報を
記憶することができ、また5.5゜ずつの等角度間隔
で64の方向に分割すれば、6ビツト相当の情報を
記憶することができるのである。 More specifically, if the in-plane magnetization direction of the magnetic medium 1 is controlled to be divided into, for example, 16 directions, that is, divided into 16 directions at equal angular intervals of 22.5 degrees and stored, one unit can be stored. The storage area, for example, the smallest unit storage area that is irradiated with the focused light, can store 16 pieces of information, that is, information equivalent to 4 bits, and can store information in 64 directions at equal angular intervals of 5.5 degrees. By dividing it, it is possible to store information equivalent to 6 bits.
更に、従来の熱磁気記録方式においては、磁化
の強度によつて情報の有無を判断していたから、
局部的に媒体の磁化に変化があつた場合には誤り
を生じ易かつたのに対して、本発明では磁化の方
向で情報を記憶しているので、媒体の磁化に変化
があつても誤りを生じないようになつている。媒
体の磁化変化は一種のゆらぎであるので、対象と
する領域が小さいほど変動が大きくなることは統
計力学の原理であり、従来の方式では高密度化す
るほど誤りが増加するのに対して、本発明では磁
化方向により情報を記憶して1つの単位記憶領域
に多数の情報を記憶できるようにしているので、
媒体の磁化変化による誤りを低減することができ
る。 Furthermore, in conventional thermomagnetic recording methods, the presence or absence of information was determined based on the strength of magnetization.
Errors could easily occur if there was a local change in the magnetization of the medium, but in the present invention, information is stored in the direction of magnetization, so errors can occur even if there is a change in the magnetization of the medium. It is designed not to cause this. Since the magnetization change of the medium is a type of fluctuation, it is a principle of statistical mechanics that the smaller the target area, the larger the fluctuation.In contrast to conventional methods, errors increase as the density increases. In the present invention, information is stored according to the magnetization direction so that a large amount of information can be stored in one unit storage area.
Errors caused by changes in magnetization of the medium can be reduced.
次に、以上のようにして磁化の方向で磁気媒体
1に記憶された情報を読み取る方法について説明
する。 Next, a method of reading information stored on the magnetic medium 1 in the direction of magnetization as described above will be explained.
この読み取り方法には種々の方法があるが、第
2図に示す装置は、再生用光源17,19からの
光を偏光子21,23を介してそれぞれ磁気媒体
1の所望の同一領域に2本の独立な直線偏向とし
て照射し、磁気光学効果によつて発生する該領域
の磁化による光の偏向面の回転をそれぞれ直線偏
向に対応したアナライザである検光子25,27
で検出し、これを例えばホトトランジスタ等から
なる受光素子29,31で電気出力として取り出
し、この両出力から角度、すなわち該領域におけ
る磁化の方向を検出するようにしているものであ
る。今、例えば2つの直線偏向A,Bを照射する
方向を直交させ、これらの各方向をX,Y方向と
して磁化Mの磁化方向がX方向からみてθ方向で
あるとすると、X方向の磁化がM・sinθ、Y方向
の磁化がM・cosθである場合と同様の偏向面の回
転が直線偏向A,Bに生じ、受光素子31,29
からX出力、Y出力として検出できる。従つて、
この直線偏向A,Bの出力を直交表現すれば磁化
方向が判別できるのである。また、個々の電気出
力自体は磁化Mの変動の影響を受けるが、磁化の
大きさは次式で求められるので、規格化すること
が可能である。 There are various methods for this reading, but the apparatus shown in FIG. Analyzers 25 and 27 are analyzers that each correspond to linear polarization, and the rotation of the plane of deflection of light due to the magnetization of the region generated by the magneto-optic effect.
This is detected as an electrical output by light receiving elements 29 and 31 made of, for example, phototransistors, and the angle, that is, the direction of magnetization in the region, is detected from both outputs. Now, for example, if the directions of irradiation with two linear polarizations A and B are orthogonal, and these directions are the X and Y directions, and the magnetization direction of the magnetization M is the θ direction when viewed from the X direction, then the magnetization in the X direction is Rotation of the deflection plane similar to that when the magnetization in the Y direction is M·sinθ and M·cosθ occurs in the linear polarizations A and B, and the light receiving elements 31 and 29
It can be detected as X output and Y output. Therefore,
If the outputs of the linear deflections A and B are expressed orthogonally, the magnetization direction can be determined. Furthermore, although the individual electrical outputs themselves are affected by fluctuations in magnetization M, the magnitude of magnetization can be determined by the following equation, so it can be standardized.
M=[(M・sinθ)2+(M・cosθ)2]1/2
=[(A出力)2+(B出力)2]1/2
結局、磁化のゆらぎ等があつてもA出力とB出
力から磁化方向を完全に検出することができるの
である。なお、上記実施例においては、2本の独
立な直線偏向が直交している場合について説明し
たが、2本の直線偏向が平行でない限りは2つの
出力を回路的に処理する等の後処理により磁化方
向を検出することが可能である。M = [(M・sinθ) 2 + (M・cosθ) 2 ] 1/2 = [(A output) 2 + (B output) 2 ] 1/2 In the end, even if there are fluctuations in magnetization, the A output and The magnetization direction can be completely detected from the B output. In the above embodiment, the case where the two independent linear deflections are orthogonal was explained, but unless the two linear deflections are parallel, the two outputs can be processed by post-processing such as circuit processing. It is possible to detect the magnetization direction.
また、磁気媒体1の所望の記憶位置に所望の情
報、すなわち所望の方向の磁化を記憶するのに、
第1図に示すように、磁気媒体1の外側に配設さ
れたヘルムホルツコイル等を用いて任意の方向の
磁場を発生するとともに、例えばガルバノミラ
ー、超音波偏向器等のような適当な光偏向器を用
いて磁気媒体1の所望の位置に光を照射するよう
に位置決めしてもよいが、直交磁場発生器と光学
系とを一体化して媒体より小さく形成し、これを
磁気媒体に対して相対的に移動させて記憶位置を
位置決めしてもよい。 Furthermore, in order to store desired information, that is, magnetization in a desired direction, at a desired storage position of the magnetic medium 1,
As shown in FIG. 1, a magnetic field in an arbitrary direction is generated using a Helmholtz coil or the like disposed outside the magnetic medium 1, and a suitable optical deflection device such as a galvanometer mirror or an ultrasonic deflector is used. Alternatively, the orthogonal magnetic field generator and the optical system may be integrated and formed smaller than the medium, and this may be positioned to irradiate the magnetic medium 1 with light at a desired position using a device. The storage position may be determined by relative movement.
第3図はこのように構成した本発明の他の実施
例を示しているものである。同図においては円盤
状の磁気媒体33が使用され、この円盤状磁気媒
体33はスピンドルモータ35により回転させら
れるようになつている。そして、この磁気媒体3
3の下面の下側には近接して前述した直交磁場発
生器と光学系とを一体的に組合せた装置37が配
設され、この装置37はアクチユエータ39によ
つて矢印41で示すように磁気媒体33の半径方
向に移動し得るように構成されている。その結
果、通常の磁気デイスク装置における様にアクチ
ユエータ39により装置37の磁気媒体33の半
径方向のトラツクに対する位置を決定し、スピン
ドルモータ35による磁気媒体33の回転でその
周方向のセクタに対する位置を決定して磁気媒体
33における記憶位置を決定すれば、大容量の場
合においても比較的高速に情報を読み書きするこ
とができる。 FIG. 3 shows another embodiment of the present invention constructed in this manner. In the figure, a disk-shaped magnetic medium 33 is used, and this disk-shaped magnetic medium 33 is rotated by a spindle motor 35. And this magnetic medium 3
A device 37 that integrally combines the above-described orthogonal magnetic field generator and an optical system is disposed adjacent to the lower side of the lower surface of 3. It is configured to be able to move in the radial direction of the medium 33. As a result, as in a normal magnetic disk device, the actuator 39 determines the position of the device 37 with respect to the radial track of the magnetic medium 33, and the rotation of the magnetic medium 33 by the spindle motor 35 determines the position with respect to the sector in the circumferential direction. If the storage position on the magnetic medium 33 is determined by the following steps, information can be read and written at relatively high speed even in the case of a large capacity.
なお、上述した装置37に収納される直交磁場
発生器は第4図に示すように磁気媒体33の片側
に近接して配設された一対の磁極43,45、お
よび図示していないが、この一対の磁極43,4
5の磁場の方向に対して磁気媒体33の面内で例
えば直交する方向の磁場を発生するように磁極4
3,45に対して例えば直交して配設された別の
一対の磁極を設け、さらに磁極43,45に磁場
発生巻線47,49を巻回すると共に、図示しな
い磁極にも同様に磁場発生巻線を巻回して構成し
て磁気媒体33の片側から磁気媒体33に合成磁
場を印加するようになつている。この場合、磁気
媒体33に対して完全な面内磁場を発生するわけ
ではないが、磁場発生器の中心線51上ではほぼ
磁気媒体33の面に平行となるので、この部分を
利用し、この部分に光を照射すればよい。そし
て、上述したように、1つの単位記憶領域に多数
の情報を記憶でき、一回に記憶する領域が大きく
てもよいので、位置決めはそれほど精度を必要と
せず、位置決め用の装置構成は簡単である。 The orthogonal magnetic field generator housed in the device 37 described above includes a pair of magnetic poles 43 and 45 disposed close to one side of the magnetic medium 33 as shown in FIG. A pair of magnetic poles 43, 4
The magnetic pole 4 is configured to generate a magnetic field in a direction perpendicular to the direction of the magnetic field 5 in the plane of the magnetic medium 33, for example.
For example, another pair of magnetic poles are arranged perpendicularly to the magnetic poles 43 and 45, and magnetic field generating windings 47 and 49 are wound around the magnetic poles 43 and 45, and magnetic field generating coils 47 and 49 are similarly wound around the magnetic poles (not shown). It is configured by winding a winding so that a composite magnetic field is applied to the magnetic medium 33 from one side of the magnetic medium 33. In this case, a complete in-plane magnetic field is not generated for the magnetic medium 33, but since it is approximately parallel to the plane of the magnetic medium 33 on the center line 51 of the magnetic field generator, this portion can be used to All you have to do is irradiate the area with light. As mentioned above, a large amount of information can be stored in one unit storage area, and the area to be stored at one time may be large, so positioning does not require much precision and the configuration of the positioning device is simple. be.
また、直交磁場発生器は磁気媒体33の面内の
任意の方向に所定の大きさの磁場を発生できれば
よいので、対称構造である必要もなく、例えば通
常の磁気ヘツドのように構成し、磁気ヘツドのギ
ヤツプに相当する空隙部分から発生するようにす
る。そして、この空隙、すなわち前記磁極43,
45間の空隙を数百μ以下に構成し、該空隙先端
の磁極43,45を磁気媒体33の面に対して空
隙長の半分程度に近接配設すれば、1000 Oe程度
の磁場を発生しながら、磁気ヘツドと同様に高い
周波数でこの磁場を反転することができる。そし
て、前記磁極43,45の間の空隙から光を磁気
媒体33に向けて光を連続的に照射しながら、磁
場発生巻線47,49に流す電流を制御すれば磁
化の方向を決定できる熱バイアス型の記録が可能
となるのである。なお、この場合、従来の熱バイ
アス型においては前述したように高記録密度がで
きないという欠点があつたが、本発明においては
単位記録面積を小さくすることなく、磁化方向の
数で記録密度を高くしている高密度記録が可能と
なつている。従つて、光学系は簡単である上、既
に記録された情報があつてもその上に新たな情報
を記憶することができる。 Further, since the orthogonal magnetic field generator only needs to be able to generate a magnetic field of a predetermined magnitude in any direction within the plane of the magnetic medium 33, it does not need to have a symmetrical structure. It should be generated from the gap corresponding to the gap in the head. Then, this gap, that is, the magnetic pole 43,
If the gap between 45 and 45 is configured to be several hundred μ or less, and the magnetic poles 43 and 45 at the tips of the gap are placed close to the surface of the magnetic medium 33 at about half the gap length, a magnetic field of about 1000 Oe can be generated. However, similar to magnetic heads, this magnetic field can be reversed at high frequencies. Then, by controlling the current flowing through the magnetic field generating windings 47 and 49 while continuously irradiating light toward the magnetic medium 33 from the gap between the magnetic poles 43 and 45, the direction of magnetization can be determined. This makes bias type recording possible. In this case, the conventional thermal bias type had the disadvantage of not being able to achieve high recording density as described above, but in the present invention, the recording density can be increased by increasing the number of magnetization directions without reducing the unit recording area. High-density recording is now possible. Therefore, the optical system is simple, and even if there is already recorded information, new information can be stored thereon.
なお、磁極の方向を決定する方法としては、上
記実施例のように磁場の合成により行なう方法に
限定されず、例えば磁場発生器を回転させてその
磁場を任意の方向に向けるようにすることもでき
る。 Note that the method of determining the direction of the magnetic pole is not limited to the method of combining magnetic fields as in the above embodiment; for example, it is also possible to rotate a magnetic field generator to direct the magnetic field in an arbitrary direction. can.
[発明の効果]
以上説明したように、この発明によれば、面内
の磁化特性が等方的な多結晶構造の磁気媒体を使
用し、この磁気媒体の面内の残留磁化の方向によ
り情報を記憶するようにしているので、その単位
記憶領域における磁化の方向を増大するだけで単
位記憶領域を小さくすることなく、高密度記録を
行なうことができ、かつ単位記憶領域を小さくす
る必要もないため、光学系、位置決め装置等の周
辺装置の構成を簡単にできる。また、単位記憶領
域を小さくする必要もなく、情報を磁化の方向に
より記憶していて、従来のように磁化の反転や強
度等を利用していないので、磁化の変化があつて
も誤りを生ぜず、信頼性の高い記憶装置が可能で
ある。[Effects of the Invention] As explained above, according to the present invention, a magnetic medium having a polycrystalline structure with isotropic in-plane magnetization characteristics is used, and information is generated by the direction of the in-plane residual magnetization of this magnetic medium. By simply increasing the direction of magnetization in the unit storage area, high-density recording can be performed without reducing the unit storage area, and there is no need to make the unit storage area smaller. Therefore, the configuration of peripheral devices such as an optical system and a positioning device can be simplified. In addition, there is no need to reduce the unit storage area, and information is stored based on the direction of magnetization, rather than using magnetization reversal or strength as in the past, so errors can occur even if magnetization changes. First, a highly reliable storage device is possible.
第1図はこの発明の一実施例を示す熱磁気記録
装置の構成を示す斜視図、第2図は第1図の熱磁
気記録記憶の再生装置の構成を示す図、第3図は
この発明の他の実施例を示す熱磁気記録装置の構
成図、第4図は第3図の装置に使用される直交磁
場発生器の部分構成図である。
1…磁気媒体、3,5,7,9…直交磁場発生
器、11…光源、13…光偏向器、15…集光装
置。
FIG. 1 is a perspective view showing the configuration of a thermomagnetic recording device showing an embodiment of the present invention, FIG. 2 is a diagram showing the configuration of a reproducing device for the thermomagnetic recording storage shown in FIG. 1, and FIG. Fig. 4 is a partial block diagram of an orthogonal magnetic field generator used in the apparatus of Fig. 3; DESCRIPTION OF SYMBOLS 1... Magnetic medium, 3, 5, 7, 9... Orthogonal magnetic field generator, 11... Light source, 13... Optical deflector, 15... Light condensing device.
Claims (1)
媒体と、前記磁気媒体の前記面の所望の位置に所
定の大きさに集光した光を照射する光照射手段
と、該光照射手段によつて光を照射された前記所
望の位置の面内に所望の方向の磁化を残留させ、
該磁化の方向により情報を記憶すべく、少なくと
も前記所望の位置の面内に前記磁化の方向に対応
する磁場を印加する磁場印加手段とを有すること
を特徴とする熱磁気記録方式。1. A magnetic medium having a polycrystalline structure with isotropic in-plane magnetization characteristics, a light irradiation means for irradiating light focused to a predetermined size onto a desired position on the surface of the magnetic medium, and the light irradiation means. causing magnetization in a desired direction to remain in the plane of the desired position irradiated with light by the means;
A thermomagnetic recording system comprising a magnetic field applying means for applying a magnetic field corresponding to the direction of magnetization within a plane at least at the desired position in order to store information according to the direction of magnetization.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP25172484A JPS61131202A (en) | 1984-11-30 | 1984-11-30 | Thermomagnetic recording system |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP25172484A JPS61131202A (en) | 1984-11-30 | 1984-11-30 | Thermomagnetic recording system |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61131202A JPS61131202A (en) | 1986-06-18 |
| JPH0439726B2 true JPH0439726B2 (en) | 1992-06-30 |
Family
ID=17227031
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP25172484A Granted JPS61131202A (en) | 1984-11-30 | 1984-11-30 | Thermomagnetic recording system |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61131202A (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS51134614A (en) * | 1975-05-19 | 1976-11-22 | Teac Co | Photomagnetic recorder |
-
1984
- 1984-11-30 JP JP25172484A patent/JPS61131202A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61131202A (en) | 1986-06-18 |
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