JPH0443338B2 - - Google Patents

Info

Publication number
JPH0443338B2
JPH0443338B2 JP25200283A JP25200283A JPH0443338B2 JP H0443338 B2 JPH0443338 B2 JP H0443338B2 JP 25200283 A JP25200283 A JP 25200283A JP 25200283 A JP25200283 A JP 25200283A JP H0443338 B2 JPH0443338 B2 JP H0443338B2
Authority
JP
Japan
Prior art keywords
magnetic
head
thin film
light beam
magnetic head
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
JP25200283A
Other languages
Japanese (ja)
Other versions
JPS60143463A (en
Inventor
Kanichi Naito
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.)
Fujifilm Holdings Corp
Original Assignee
Fuji Photo Film 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 Fuji Photo Film Co Ltd filed Critical Fuji Photo Film Co Ltd
Priority to JP25200283A priority Critical patent/JPS60143463A/en
Priority to NL8403950A priority patent/NL8403950A/en
Publication of JPS60143463A publication Critical patent/JPS60143463A/en
Publication of JPH0443338B2 publication Critical patent/JPH0443338B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/31Structure or manufacture of heads, e.g. inductive using thin films
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording 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
    • G11B11/10Recording 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
    • G11B11/105Recording 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
    • G11B11/10532Heads
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording 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
    • G11B11/10Recording 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
    • G11B11/105Recording 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
    • G11B11/10532Heads
    • G11B11/10541Heads for reproducing
    • G11B11/10543Heads for reproducing using optical beam of radiation
    • G11B11/10547Heads for reproducing using optical beam of radiation interacting with the magnetisation of an intermediate transfer element, e.g. magnetic film, included in the head

Description

【発明の詳細な説明】 (発明の分野) 本発明は薄膜磁気ヘツドを利用して磁気テー
プ、磁気デイスク等の記録媒体から磁気記録情報
を読み出す再生方法および装置、さらに詳しくは
誘導型薄膜磁気ヘツドに光ビームを投影し、この
光ビームの反射光の、カー効果による強度変化を
検出して内部磁化の方向を検出することにより記
録情報を再生する磁気記録再生方法および装置に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of the Invention) The present invention relates to a reproducing method and apparatus for reading magnetically recorded information from a recording medium such as a magnetic tape or a magnetic disk using a thin film magnetic head, and more particularly to an inductive thin film magnetic head. The present invention relates to a magnetic recording and reproducing method and apparatus for reproducing recorded information by projecting a light beam onto a surface, detecting changes in intensity of reflected light of the light beam due to the Kerr effect, and detecting the direction of internal magnetization.

(従来技術) 磁気テープ、磁気デイスク等の磁気記録媒体に
情報を記録、再生する方法には種々の形式のもの
が知られているが、記録密度の向上のために磁性
材料や磁気ヘツドに種々の改良がなされ、各種の
新技術が開発されている。記録密度を大幅に向上
させるためには、磁気テープやデイスクのヘツド
に対する相対移動速度を相当遅くしても十分な出
力で再生ができることが必要になるが、再生時の
テープスピード(デイスクの回転スピード)を小
さくすると磁気誘導型の磁気ヘツドでは必然的に
出力が低下し、実用にならなくなる。また、この
磁気誘導型ヘツドではトラツク幅の大きさによつ
て再生出力信号のレベルが左右されるため、トラ
ツク幅を小さくしてトラツク密度を高くするのに
も限界があり、トラツク密度をより高くすること
が望まれている。
(Prior Art) Various methods are known for recording and reproducing information on magnetic recording media such as magnetic tapes and magnetic disks, but various types of magnetic materials and magnetic heads are used to improve recording density. improvements have been made, and various new technologies have been developed. In order to significantly improve recording density, it is necessary to be able to reproduce with sufficient output even if the relative movement speed of the magnetic tape or disk to the head is considerably slowed down. ), the output of a magnetic induction type magnetic head inevitably decreases, making it impractical. In addition, with this magnetic induction type head, the level of the reproduced output signal is affected by the track width, so there is a limit to increasing the track density by reducing the track width. It is desired to do so.

そこで、磁気誘導型のように磁気ヘツド内の内
部磁化の変化のスピードを出力するものに代え
て、磁気記録媒体内の磁化の方向および大きさに
直接応答する磁束反応型の磁気ヘツドが開発され
ている。これはMR(マグネトレジスト)ヘツド
と称されるもので、テープの送り速度やラツク幅
に出力が左右されない再生が可能であるため、高
密度の記録の再生を可能とするものであるが、こ
れは温度変化による再生出力変動が大きく、また
ヘツドの構造が特殊なため製造コストが高く、さ
らに特性の一定したヘツドを製造するのが困難な
ため実用上難点がある。
Therefore, instead of the magnetic induction type that outputs the speed of change in internal magnetization within the magnetic head, a magnetic flux responsive type magnetic head was developed that directly responds to the direction and magnitude of magnetization within the magnetic recording medium. ing. This is called an MR (magnetoresist) head, and its output is not affected by tape feed speed or rack width, making it possible to play back high-density recordings. The reproduction output fluctuates greatly due to temperature changes, and the manufacturing cost is high because the head has a special structure.Furthermore, it is difficult to manufacture a head with consistent characteristics, which presents practical difficulties.

また、光磁気記録という、特殊な光磁気記録媒
体光ビームを投影し、その反射光を検出してカー
効果を利用してこの媒体の内部磁化を読み取る方
式も開発されているが、これも特殊な光磁気記録
媒体を使用しなければならないため、実用上に難
点がある。
Additionally, a method called magneto-optical recording has been developed in which a light beam is projected onto a special magneto-optical recording medium, the reflected light is detected, and the internal magnetization of this medium is read using the Kerr effect, but this is also a special method. This method is difficult in practice because it requires the use of a magneto-optical recording medium.

(発明の目的) 本発明は従来の磁気テープ等の記録媒体をその
まま使用することができ、磁気ヘツドとしても従
来の誘導型薄膜磁気ヘツドの一部に変更を加える
だけで磁束応答型の再生ができる実用に適した高
密度記録情報の再生方法および装置を提供するこ
とを目的とするものである。
(Objective of the Invention) The present invention allows conventional recording media such as magnetic tapes to be used as they are, and can also be used as a magnetic head by simply making some changes to the conventional induction type thin film magnetic head. The object of the present invention is to provide a method and apparatus for reproducing high-density recorded information that is suitable for practical use.

(発明の構成) 本発明は、薄膜磁気ヘツドの基板に透明な材料
を使用し、この基板側からヘツドに斜めに光ビー
ムを入射させ、この光ビームの横カー効果による
反射光の強度変化を検出してヘツドの内部磁化の
方向を読み取ることを特徴とするものである。
(Structure of the Invention) The present invention uses a transparent material for the substrate of a thin-film magnetic head, allows a light beam to enter the head obliquely from the substrate side, and changes the intensity of reflected light due to the transverse Kerr effect of the light beam. This is characterized by detecting and reading the direction of internal magnetization of the head.

すなわち、縦カー効果を利用して薄膜磁気ヘツ
ド内の内部磁化の方向と大きさを光電的に読み取
るようにしたことを特徴とするもので、これによ
り誘導型でなく、磁束応答型の読取りを可能に
し、したがつて極低速でテープを走行させても記
録情報を読むことができるようにしたことを特徴
とするものである。
In other words, it is characterized by photoelectrically reading the direction and magnitude of internal magnetization in the thin-film magnetic head using the longitudinal Kerr effect. Therefore, the recorded information can be read even when the tape is running at an extremely low speed.

(発明の効果) 本発明によれば、従来のテープ、デイスク等の
磁気記録媒体をそのまま使用することができ、磁
気ヘツドとしても従来の薄膜磁気ヘツドを基板を
透明にするだけで使用することができ、これによ
り磁束応答型の再生ができるので、低コストで高
密度の再生が実現され、実用上の効果はきわめて
大きい。
(Effects of the Invention) According to the present invention, conventional magnetic recording media such as tapes and disks can be used as they are, and a conventional thin film magnetic head can also be used as a magnetic head by simply making the substrate transparent. As a result, magnetic flux response type reproduction can be performed, and high-density reproduction can be realized at low cost, and the practical effect is extremely large.

特に、再生出力信号のレベルはトラツク幅に左
右されず、再生に使用するレーザビーム等の光の
パワーに左右されるので、トラツク幅は小さくて
もレーザ光パワーにより再生出力の低下を防げる
ので、トラツク幅を小さくしてトラツク密度を大
きくした再生が可能になる。
In particular, the level of the reproduced output signal is not affected by the track width, but by the power of the light such as the laser beam used for reproduction, so even if the track width is small, the laser light power can prevent the reproduction output from decreasing. It becomes possible to perform playback with a smaller track width and larger track density.

(実施態様) 以下、図面により本発明の実施態様を詳細に説
明する。
(Embodiments) Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.

第1図は薄膜磁気ヘツド1の基板的構成を示す
正面図、第2図はその縦断面である。薄膜磁気ヘ
ツド1は、透明な基板10の上に下部磁極11、
絶縁層12、導電コイル層13、絶縁層14、上
部磁極15をこの順に積層してなるもので、下部
磁極11と上部磁極15の端縁はギヤツプ16を
介して対向し、この間には絶縁層12の端縁が介
在して磁気回路のギヤツプを形成している。導電
コイル層13は外部の電気回路に接続されるよう
に一端13Aが外方へ延び、他端13Bが導電体
17に接続されている。このような薄膜磁気ヘツ
ド1の基本的構成はよく知られており、例えば特
開昭58−111115号に開示されているのでその詳細
は省略する。
FIG. 1 is a front view showing the structure of a substrate of a thin film magnetic head 1, and FIG. 2 is a longitudinal section thereof. The thin film magnetic head 1 has a lower magnetic pole 11 on a transparent substrate 10,
The insulating layer 12, the conductive coil layer 13, the insulating layer 14, and the upper magnetic pole 15 are laminated in this order. Twelve edges are interposed to form a gap in the magnetic circuit. One end 13A of the conductive coil layer 13 extends outward so as to be connected to an external electric circuit, and the other end 13B is connected to the conductor 17. The basic structure of such a thin film magnetic head 1 is well known and is disclosed in, for example, Japanese Patent Application Laid-open No. 111115/1983, so its details will be omitted.

本発明においては、基板10に透明で滑らかな
表面(鏡面)を有する、しかも硬度の高い材料を
使用する。このような性質を持つた材料として
は、例えばサフアイヤの単結晶がある。
In the present invention, a material having a transparent, smooth surface (mirror surface) and high hardness is used for the substrate 10. An example of a material having such properties is a single crystal of sapphire.

上記のような透明な基板10を備えた薄膜磁気
ヘツド1を、第3図に示すように磁気テープ等の
磁気記録媒体20の上に、前記ギヤツプ16が接
するように配設し、基板10を通して下部磁極1
1の表面にレーザ光のような光ビーム30を斜め
に入射させる。この入射の方向は、薄膜磁気ヘツ
ド1の内部磁化の方向(矢印で示す)と垂直な面
内を前記下部磁極11の表面に斜めに入射する方
向とする。ここで斜めとは、上記面内での入射角
θが80゜(磁極がパーマロイの場合はθ80゜。他
の磁性材料に対しては各々最適値がある)程度と
なる角度を言うもとする。
As shown in FIG. 3, the thin film magnetic head 1 equipped with the transparent substrate 10 as described above is arranged on a magnetic recording medium 20 such as a magnetic tape so that the gap 16 is in contact with the magnetic recording medium 20, and the substrate 10 is passed through the thin film magnetic head 1. Lower magnetic pole 1
A light beam 30 such as a laser beam is obliquely incident on the surface of the substrate 1. The direction of this incidence is such that it is obliquely incident on the surface of the lower magnetic pole 11 in a plane perpendicular to the direction of internal magnetization (indicated by the arrow) of the thin-film magnetic head 1. Here, oblique refers to the angle at which the incident angle θ in the above plane is approximately 80° (θ80° if the magnetic pole is made of permalloy. There are optimum values for other magnetic materials). .

この入射光ビーム30は、下部磁極11の表面
で反射され、基板10の表面から入射と反射方向
へ反射される。このとき、下部磁極11の表面で
反射率は横カー効果の作用により内部磁化の変化
に応じて変化するので、この反射光31をフオト
センサ35により光電的に検出すれば、その出力
が内部磁化の方向と大きさを示すことになり、磁
気記録媒体20に記録されている情報を読み出す
こと、すなわち再生が可能になる。
This incident light beam 30 is reflected by the surface of the lower magnetic pole 11 and reflected from the surface of the substrate 10 in the direction of incidence and reflection. At this time, the reflectance on the surface of the lower magnetic pole 11 changes according to the change in internal magnetization due to the effect of the transverse Kerr effect, so if this reflected light 31 is photoelectrically detected by the photo sensor 35, its output will change depending on the internal magnetization. The direction and size are indicated, and the information recorded on the magnetic recording medium 20 can be read out, that is, reproduced.

上記実施態様は本発明の基本的構成を示すもの
であるが、磁気ヘツド1の構造を、下部磁極を多
数並列した形とし、そのチヤンネル数だけの光学
系を用意すればマルチヘツド型の再生が可能にな
る。第4図はその一例を示す水平断面図(下部電
極11Aと共通の基板10Aのみ示し、他の部分
は省略)であり、第5図はその平面図、第6図は
第4図と対応させてその断面を示すものである。
第1図から第3図に示した前述の実施態様と共通
する部分は同じ符号で表わし、その説明は省略す
る。第5図中、テープ20の中に示す記号はテー
プ20に記録されているデイジタル信号の磁化方
向を示す。
Although the embodiment described above shows the basic configuration of the present invention, multi-head type reproduction is possible by making the structure of the magnetic head 1 into a form in which a large number of lower magnetic poles are arranged in parallel, and by preparing optical systems corresponding to the number of channels. become. FIG. 4 is a horizontal sectional view showing one example (only the substrate 10A common to the lower electrode 11A is shown, other parts are omitted), FIG. 5 is a plan view thereof, and FIG. 6 corresponds to FIG. 4. This figure shows a cross section of it.
Portions common to the above-described embodiments shown in FIGS. 1 to 3 are designated by the same reference numerals, and a description thereof will be omitted. In FIG. 5, the symbols shown inside the tape 20 indicate the magnetization direction of the digital signals recorded on the tape 20.

このようにマルチヘツド型にすれば、マルチチ
ヤンネルの記録、再生が可能となり、1つの磁気
ヘツドでマルチチヤンネルの再生を同時に行なう
ことができる。
This multi-head type allows multi-channel recording and reproduction, and multi-channel reproduction can be performed simultaneously with one magnetic head.

さらに、第7図に示すように1つの磁気ヘツド
に多数の下部磁極を配したヘツドアレイチツプ
(マルチヘツド型構造)40を使用し、これに光
ビームを走査するようにすれば、1本のレーザー
ビームを使用して多数のヘツドの読出しを行なう
ことができる。すなわち、レーザ光源41からの
レーザビーム41Aを回転プリズム42により偏
向させ、対物レンズ43を通してヘツドアレイチ
ツプ40に入射させてこのチツプ上を走査させ、
この反射光41Bをコリメータレンズ44により
平行光にした後、集光レンズ45によりフオトマ
ル46に入射させ、フオトマル46の出力を増幅
器47により増幅して、ヘツドアレイスイツプ4
0上の反射率の変化を検出し、磁気記録媒体の記
録情報を読み取ることができる。
Furthermore, as shown in FIG. 7, if a head array chip (multi-head type structure) 40 in which a number of lower magnetic poles are arranged in one magnetic head is used, and a light beam is scanned over this chip, one laser beam can be scanned. The beam can be used to read out multiple heads. That is, a laser beam 41A from a laser light source 41 is deflected by a rotating prism 42, is incident on a head array chip 40 through an objective lens 43, and is scanned over this chip.
After this reflected light 41B is made into parallel light by a collimator lens 44, it is made incident on a photographic lens 46 by a condensing lens 45, and the output of the photographic material 46 is amplified by an amplifier 47.
By detecting changes in reflectance above 0, it is possible to read recorded information on a magnetic recording medium.

磁気テープ等の記録媒体20を、第4図におい
て矢印A方向に走行させつつ、読取りのためのレ
ーザ光を30A,30B…30Nのように切り換
えれば、記録媒体20の幅方向に僅かに斜めに読
み取り、これを繰返すことによつてテープ全体に
亘つてストライプ状に読取りを行なうことができ
る。また、このストライプ状のトラツクを第8図
に示すように第1トラツク(○印で示す1ビツト
単位の読取り域をつないだもの)と第2トラツク
(×印で示すもの)を交互に配した形とすること
によりテープの記録密度を一層高くすることがで
きる。第8図中矢印B,Cで示すのは、それぞれ
第1トラツクと第2トラツクの帰線方向である。
If the recording medium 20 such as a magnetic tape is run in the direction of arrow A in FIG. 4 and the laser beam for reading is switched to 30A, 30B...30N, the recording medium 20 will be slightly diagonal in the width direction. By repeating this process, the entire tape can be read in stripes. In addition, as shown in Figure 8, these striped tracks are arranged alternately as the first track (connecting the reading area of 1 bit unit, indicated by the circle mark) and the second track (the track indicated by the cross mark). By changing the shape, the recording density of the tape can be further increased. Arrows B and C in FIG. 8 indicate the return directions of the first track and the second track, respectively.

上記各実施態様においては磁気テープの場合を
説明したが、これは磁気デイスクの場合でも全く
同様であり、デイスクの半径方向にヘツドを多数
並べたマルチヘツドにすることもできるし、この
とき多数のレーザビームを平行に入射させて同時
にマルチチヤンネル方式で再生することもできる
し、一本のレーザビームを走査させて(前記第7
図の例のように)第8図のような走査により再生
することもできる。
In each of the above embodiments, the case of a magnetic tape has been explained, but this is exactly the same in the case of a magnetic disk, and it is also possible to have a multi-head with many heads arranged in the radial direction of the disk, and in this case, a large number of lasers It is also possible to make the beams incident in parallel and perform simultaneous reproduction using a multi-channel method, or to scan with a single laser beam (the seventh method described above).
It is also possible to reproduce the data by scanning as shown in FIG. 8 (as in the example shown in the figure).

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

第1図は本発明による磁気記録情報再生方法に
使用する薄膜磁気ヘツドの一例を示す正面図、第
2図はその縦断面図、第3図は本発明の再生方法
の一実施態様の概略を示す斜視図、第4図は本発
明の再生方法の他の実施態様を示す平面図、第5
図はその正面図、第6図はその縦断面図、第7図
は本発明のさらに異なる実施態様を示す平面図、
第8図は本発明の一実施態様により再生される磁
気テープのマルチトラツクの例を示す平面図であ
る。 1……薄膜磁気ヘツド、10……透明基板、1
1……下部磁極、12,14……絶縁層、13…
…導電コイル層、15……上部磁極、16……ギ
ヤツプ、20……磁気テープ、30……入射光、
31……反射光。
FIG. 1 is a front view showing an example of a thin film magnetic head used in the method for reproducing magnetically recorded information according to the present invention, FIG. 2 is a longitudinal sectional view thereof, and FIG. FIG. 4 is a plan view showing another embodiment of the regeneration method of the present invention, and FIG.
The figure is a front view thereof, FIG. 6 is a longitudinal sectional view thereof, and FIG. 7 is a plan view showing still another embodiment of the present invention.
FIG. 8 is a plan view showing an example of a multi-track magnetic tape reproduced according to an embodiment of the present invention. 1... Thin film magnetic head, 10... Transparent substrate, 1
1... Lower magnetic pole, 12, 14... Insulating layer, 13...
... Conductive coil layer, 15 ... Upper magnetic pole, 16 ... Gap, 20 ... Magnetic tape, 30 ... Incident light,
31...Reflected light.

Claims (1)

【特許請求の範囲】 1 磁気回路のギヤツプに接して移動する磁気記
録媒体の記録情報を内部磁化の変化として読み取
る誘導型薄膜磁気ヘツドの磁性層の表面の一部
に、該一部における内部磁化の方向と略垂直な面
内を前記表面に対して斜めに進む光ビームを入射
させ、この光ビームの前記一部からの反射光を検
出し、その反射光の強度から前記内部磁化の方向
を読み取る磁気記録媒体再生方法。 2 磁気回路のギヤツプに接して移動する磁気記
録媒体の記録情報を内部磁化の変化として読み取
る誘導型薄膜磁気ヘツドの層構成を透明な基板上
に積層してなる薄膜磁気ヘツド、この薄膜磁気ヘ
ツドの前記基板を通して磁性層の表面の一部に該
一部における内部磁化の方向と略垂直な面内を前
記表面に対して斜めに進む光ビームを入射させる
光ビーム投影手段、および前記光ビームの前記一
部からの反射光を受光し、その反射光の強度を電
気信号に変換する光電変換手段からなる磁気記録
情報再生装置。
[Scope of Claims] 1. An inductive thin film magnetic head that reads recorded information on a magnetic recording medium that moves in contact with a gap in a magnetic circuit as a change in internal magnetization. A light beam traveling obliquely to the surface in a plane substantially perpendicular to the direction of is incident, the reflected light from the part of the light beam is detected, and the direction of the internal magnetization is determined from the intensity of the reflected light. A method for reading and reproducing magnetic recording media. 2. A thin film magnetic head, which is made by laminating the layer structure of an inductive thin film magnetic head on a transparent substrate, which reads information recorded on a magnetic recording medium that moves in contact with the gap of a magnetic circuit as changes in internal magnetization. a light beam projecting means for projecting a light beam that travels obliquely to the surface in a plane substantially perpendicular to the direction of internal magnetization in the part through the substrate; A magnetic recording information reproducing device comprising photoelectric conversion means that receives reflected light from a portion and converts the intensity of the reflected light into an electrical signal.
JP25200283A 1983-12-29 1983-12-29 Method and device for reproducing magnetic recording information Granted JPS60143463A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP25200283A JPS60143463A (en) 1983-12-29 1983-12-29 Method and device for reproducing magnetic recording information
NL8403950A NL8403950A (en) 1983-12-29 1984-12-27 METHOD AND APPARATUS FOR REPRODUCING MAGNETIC INFORMATION.

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25200283A JPS60143463A (en) 1983-12-29 1983-12-29 Method and device for reproducing magnetic recording information

Publications (2)

Publication Number Publication Date
JPS60143463A JPS60143463A (en) 1985-07-29
JPH0443338B2 true JPH0443338B2 (en) 1992-07-16

Family

ID=17231190

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25200283A Granted JPS60143463A (en) 1983-12-29 1983-12-29 Method and device for reproducing magnetic recording information

Country Status (2)

Country Link
JP (1) JPS60143463A (en)
NL (1) NL8403950A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0760537B2 (en) * 1985-09-27 1995-06-28 株式会社日立製作所 Recording / reproducing method
DE3750060T2 (en) * 1986-02-05 1994-09-22 Information Storage Inc METHOD AND DEVICE FOR INCREASING THE STORAGE CAPACITY OF THE RECORDING MEDIA.
JPH0283838A (en) * 1988-09-20 1990-03-23 Nec Kansai Ltd Magnetic head

Also Published As

Publication number Publication date
JPS60143463A (en) 1985-07-29
NL8403950A (en) 1985-07-16

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