JPS62177738A - Transfer type photomagnetic head - Google Patents

Transfer type photomagnetic head

Info

Publication number
JPS62177738A
JPS62177738A JP1982086A JP1982086A JPS62177738A JP S62177738 A JPS62177738 A JP S62177738A JP 1982086 A JP1982086 A JP 1982086A JP 1982086 A JP1982086 A JP 1982086A JP S62177738 A JPS62177738 A JP S62177738A
Authority
JP
Japan
Prior art keywords
cantilever
magnetic pole
head
main
main magnetic
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
JP1982086A
Other languages
Japanese (ja)
Inventor
Tsutomu Matsui
勉 松井
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 JP1982086A priority Critical patent/JPS62177738A/en
Publication of JPS62177738A publication Critical patent/JPS62177738A/en
Pending legal-status Critical Current

Links

Classifications

    • 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
    • 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
    • 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

Landscapes

  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To perform the tracking control easily and smoothly by taking laser light for reproducing and reflected light from a main magnetic pole out of a cantilever, which performs the tracking servo of a vertical magnetic head part, through a polarization plane maintaining fiber to supply said laser light and detect said reflected light. CONSTITUTION:A main magnetic pole excitation type vertical magnetic head 20 where a yoke body 21 around which an exciting coil 22 is wound and a thin film main magnetic pole 25 protected by a transparent base body 26 are formed into one body is supported in one end of a cantilever 10. The laser light led from the other end of the cantilever 10 through a polarization plane maintaining fiber 28 is allowed to pass an optical system consisting of glass base bodies 23 and 24 including a distributed index lens 27 provided in one side part of the vertical magnetic head 20, and is multireflected in the transparent body 26 protecting the main magnetic pole 25 and reaches the main magnetic pole, and this reflected laser light is taken out of the cantilever 10 through the transparent base body 26, the optical system, and the polarization plane maintaining fiber 28 and is led to photodetectors 37 and 38.

Description

【発明の詳細な説明】 産業上の利用分野 この発明は、媒体への記録を垂直磁気ヘッドを用いζ行
い、記録された情報信号の再生をレーザ光を主磁極に反
射もしくは透過させて行う転写型光磁気ヘッドを用いた
再生手段の構造に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application This invention relates to a transfer method in which recording on a medium is performed using a perpendicular magnetic head, and the recorded information signal is reproduced by reflecting or transmitting a laser beam onto a main magnetic pole. This invention relates to the structure of a reproducing means using a magneto-optical head.

従来の技術 垂直異方性を有する記録媒体に情報のgき込みおよび読
み取りを行う方式として、磁気的に行う垂直磁化方式と
、光学的に行う方式がある。この垂直磁気記録方式は、
面内異方性を利用した水平面内磁気記録方式に比べて線
密度および面密度を高めることができる。
2. Description of the Related Art As methods for writing and reading information into a recording medium having perpendicular anisotropy, there are two methods: a magnetic perpendicular magnetization method and an optical method. This perpendicular magnetic recording method is
The linear density and areal density can be increased compared to the horizontal in-plane magnetic recording method that utilizes in-plane anisotropy.

この川向磁気記録においては、磁性薄膜を1ミ磁権とし
て行うので、光ビームスポットの照射による光変調を用
いた光学的記録方式に比べると線密度を高めることがで
きる。この爪直磁気記録方式では、記録トランクの幅を
狭くすれば而密度をも高めることかできるか、その分磁
気的再生を行うとき、再生出力すなわちCN比が劣下す
る。そのため、高いCN比を維持して信号irG生した
場合、而密度の点で垂直磁気記録方式に比べて光学的方
式の方がより高い値で行うことができる。それは、記録
トラックの幅が主磁極膜の幅に依存し、この幅を狭(す
ることには限界があるからである。
In this Kawamuka magnetic recording, the magnetic thin film is made with 1 mm magnetic domain, so the linear density can be increased compared to an optical recording method using optical modulation by irradiation with a light beam spot. In this direct magnetic recording system, the density can be increased by narrowing the width of the recording trunk, but the reproduction output, that is, the CN ratio, deteriorates accordingly when performing magnetic reproduction. Therefore, when the irG signal is generated while maintaining a high CN ratio, the optical method can achieve a higher density than the perpendicular magnetic recording method. This is because the width of the recording track depends on the width of the main pole film, and there is a limit to how narrow this width can be.

そこで、トラック幅を狭くシ、かつCN比を高めること
が考えられ、その−法として記録密度のより高密度化を
図るために、情報の書き込みを磁気的に行い、再生時に
情報の読み取りを磁化方向の変化を光の変化として取り
出して光学的に行う方法が考えられている。その場合、
高透磁率の磁性薄膜を主磁極膜として用い、垂直磁気記
録媒体に記録された磁化分布に応じてその漏れ磁界によ
って主磁極が磁化されるのを利用し、主磁極先端部にレ
ーザ光を照射集光してその反射光あるいは透過光を光学
系を介して光検出器に導き、を気信号に変換する方法に
よって行われる。主磁極先端部には接している磁気記録
媒体上の磁化情報すなわち記録ビットの極性に応じた嶋
化分布か現れる。このように、媒体の磁化分布に応じて
磁化方向が変化する主磁極に反射あるいは透過させたレ
ーザ光には磁気光学効果であるカー効果あるいはファラ
デー効果が生じる。これによる偏波面の回転を検知し、
再生信号が得られる。したがって、垂直磁化方式で記録
することによって、線密度では薄膜主磁極を用いるので
レーザ光記録(1μm/bit)より高い値(0,1μ
m/bit)を持つことができ、かつ再生時のCN比を
高めるためトラック密度すなわちトラック幅を元肥録並
みの値(1,6μm)とし、これまでの磁気記録再生の
限界であった値(4μm)を改善することができる。
Therefore, it has been considered to narrow the track width and increase the CN ratio.As a method for achieving this, in order to increase the recording density, information is written magnetically, and information is read by magnetization during reproduction. A method has been considered in which the change in direction is extracted as a change in light and carried out optically. In that case,
A high permeability magnetic thin film is used as the main pole film, and the main pole is magnetized by the leakage magnetic field according to the magnetization distribution recorded on the perpendicular magnetic recording medium, and the tip of the main pole is irradiated with laser light. This is done by concentrating light, guiding the reflected or transmitted light to a photodetector via an optical system, and converting it into an air signal. At the tip of the main pole, a slanted distribution appears that corresponds to the magnetization information, ie, the polarity of the recording bit, on the magnetic recording medium in contact with it. In this way, the Kerr effect or Faraday effect, which is a magneto-optical effect, occurs in the laser light reflected or transmitted through the main pole, whose magnetization direction changes depending on the magnetization distribution of the medium. Detecting the rotation of the polarization plane due to this,
A reproduced signal is obtained. Therefore, by recording with the perpendicular magnetization method, a thin film main pole is used for linear density, which is higher than laser light recording (1 μm/bit) (0.1 μm/bit).
m/bit), and in order to increase the CN ratio during reproduction, the track density, that is, the track width, was set to a value similar to Genferi recording (1.6 μm), which was the limit of magnetic recording and reproduction up until now. 4 μm).

発明か解決しようとする問題点 しかしながら、従来考えられてきたこの種の転写型光磁
気ヘッドは、主磁極側に光学的再生手段を一体に備える
構造であるため、特に主磁極を設けたヘッド部が重量が
大きく大型であるばかりか、動きが悪くトラッキングサ
ーボシステムにおいてトラッキングサーボが七分に達成
できず実用化するには種々の問題点があった。
Problems to be Solved by the Invention However, this type of transfer-type magneto-optical head that has been conventionally considered has a structure in which optical reproducing means is integrally provided on the main magnetic pole side, so the head section where the main magnetic pole is provided is particularly difficult to solve. Not only is it heavy and large, but it also has poor movement, making it impossible for a tracking servo system to achieve 70% tracking servo, and there are various problems in putting it into practical use.

また、転写型光磁気ヘッドにおいて主磁極励磁型の垂直
磁気ヘッドを適用すれば、ヘッド本体のトラッキング方
向への送り機構を簡単化できるが、励磁コイルを一体に
設ける構造となるため主磁極先端部にレーザ光を照射集
光するための光学系の構成に種々の解決すべき難点があ
った。
In addition, if a main pole excitation type perpendicular magnetic head is applied to a transfer type magneto-optical head, the mechanism for feeding the head body in the tracking direction can be simplified, but since the excitation coil is provided integrally, the tip of the main pole There were various problems that needed to be solved in the configuration of the optical system for irradiating and focusing laser light.

この発明は、主磁極励磁型の垂直磁気ヘッドを用いるも
のにおいて、容易にトラッキングサーボが行え、高いC
N比で確実に光学的再生が行える転写型光磁気ヘッドを
提供することを目的としている。
This invention uses a main pole excitation type perpendicular magnetic head, which allows easy tracking servo and high C.
It is an object of the present invention to provide a transfer type magneto-optical head that can reliably perform optical reproduction at an N ratio.

問題点を解決するための手段 この発明は、垂直磁気記録媒体に垂直磁気ヘッドにより
情報の書き込みを行い、再生時にレーザ光を媒体から磁
化転写される垂直磁気ヘッドの主磁極に照射し、この主
磁極からの反射あるいは透過レーザ光に現れる磁気光学
効果に基づく変化を光検出器により検出して情報の読み
取りを行う転写型光磁気ヘッドに係るもので、励磁コイ
ルを巻き付けたヨーク体と透明基体に保護された薄膜主
磁極とを一体に形成した主磁極励磁型の垂直磁気ヘッド
をカンチレバーの一端に支持し、このカンチレバーの他
端から偏波面保持ファイバーを介して導かれるレーザ光
を垂直磁気ヘッドの一側部に設けた屈折率分布型レンズ
を含むガラス基体からなる光学系を通し、かつ主磁極を
保護する透明基体中を多重反射させて主磁極に至らしめ
、この反射レーザ光を透明基体・光学系および偏波面保
持ファイバーを介してカンチレバー外に取り出し光検出
器に導くようにしたことを特徴としている。
Means for Solving the Problems This invention writes information on a perpendicular magnetic recording medium using a perpendicular magnetic head, and upon reproduction, a laser beam is irradiated onto the main pole of the perpendicular magnetic head whose magnetization is transferred from the medium. This is a transfer-type magneto-optical head that reads information by detecting changes caused by the magneto-optic effect that appear in reflected or transmitted laser light from a magnetic pole using a photodetector. A main pole excitation type perpendicular magnetic head integrally formed with a protected thin film main pole is supported at one end of the cantilever, and a laser beam guided from the other end of the cantilever via a polarization maintaining fiber is directed to the perpendicular magnetic head. The reflected laser beam passes through an optical system consisting of a glass substrate including a gradient index lens provided on one side, and is subjected to multiple reflections in a transparent substrate that protects the main magnetic pole to reach the main magnetic pole. It is characterized by being taken out of the cantilever and guided to a photodetector via an optical system and a polarization maintaining fiber.

作用 この発明の転写型光磁気ヘッドによれば、主磁極励磁型
の垂直磁気ヘッドがカンチレバーの一端に支持して設け
られ、主磁極に照射するレーザ光の光源と主磁極からの
反射レーザ光を検出する光検出器とがカンチレバーの作
動に影響しない外部の分離した位置に設けられ、偏波面
保持ファイバ−を介してレーザ光が主磁極に至るように
している。そして、ファイバーを介してヘッド部に導か
れるレーザ光は、ガラス基体および主磁極を保護する透
明基体中を通して主磁極先端部に至り、かつ戻されるよ
うにし、主磁極励磁型の励磁コイルを迂回する光路を形
成している。そのため媒体と接するへ、ド部が軽量化さ
れ、ヘッド部を支持するカンチレバーの動きが円滑にな
り、トラッキングサーボか容易となり、主磁極励磁型の
ヘッドを用いた光磁気ヘッドの光学的再生を高いCN比
で確実に実現可能にしている。
According to the transfer type magneto-optical head of the present invention, a main pole excitation type perpendicular magnetic head is supported at one end of the cantilever, and a light source of a laser beam irradiating the main pole and a laser beam reflected from the main pole are connected. A photodetector for detection is provided at a separate location outside that does not affect the operation of the cantilever, and the laser beam is directed to the main magnetic pole via a polarization maintaining fiber. The laser beam guided to the head part via the fiber passes through the glass base and the transparent base that protects the main pole, reaches the tip of the main pole, and returns, bypassing the excitation coil of the main pole excitation type. It forms an optical path. Therefore, the weight of the dome in contact with the medium is reduced, the movement of the cantilever that supports the head becomes smoother, and tracking servo operation becomes easier. The CN ratio makes it definitely possible.

実施例 以下、本発明の実施例について図面を参照して説明する
Embodiments Hereinafter, embodiments of the present invention will be described with reference to the drawings.

第1図〜第3図は本発明に係る転写型光磁気へ7ドの一
実施例を示すもので、第1図、第2図は主磁極励磁型の
ヘッド構造を示す図、第3図は再生光学系を示す図であ
る。図中、1はディスク媒体、10はカンチレバー、2
0は主磁極励磁型のヘッド部を示している。
1 to 3 show an embodiment of the transfer type magneto-optical head according to the present invention, and FIGS. 1 and 2 show the main pole excitation type head structure, and FIG. FIG. 2 is a diagram showing a reproduction optical system. In the figure, 1 is a disk medium, 10 is a cantilever, 2
0 indicates a main pole excitation type head section.

転写型光磁気へノドに適用されるディスク媒体1は、例
えばポリエステルフィルムからなる基板2にFe−Ni
層3を蒸着もしくはスパッタリング法により形成し、さ
らにその上に垂直磁気異方性を有するCo−Cr層4を
蒸着もしくはスパッタリング法により形成して構成され
ている。この媒体1のCo−Cr層4にカンチレバー1
0の一端に支持したヘッド部20を接触させて、媒体1
への情報の書き込みおよび媒体1からの情報の読み取り
が行われる。
A disk medium 1 applied to a transfer type magneto-optical converter has a substrate 2 made of, for example, a polyester film and a substrate 2 made of Fe-Ni.
A layer 3 is formed by vapor deposition or sputtering, and a Co--Cr layer 4 having perpendicular magnetic anisotropy is further formed thereon by vapor deposition or sputtering. A cantilever 1 is attached to the Co-Cr layer 4 of this medium 1.
The head unit 20 supported by the medium 1 is brought into contact with one end of the medium 1.
Information is written to and read from the medium 1.

ヘッド部分20を一端に支持したカンチレバー10は、
他端寄りの後端部がダンパー材11.11によってヘッ
ド(ピンクアンプ)装置本体(図示しない)側に中立支
持されている。カンチレバー10の他端には、永久磁石
12が取り付けられている。この永久磁石12を挾む両
側方には、トラッキング制御用励磁コイル13.13が
配設されている。
The cantilever 10 supporting the head portion 20 at one end is
The rear end near the other end is neutrally supported on the head (pink amplifier) device main body (not shown) side by a damper member 11.11. A permanent magnet 12 is attached to the other end of the cantilever 10. Tracking control excitation coils 13.13 are arranged on both sides of the permanent magnet 12.

一方、カンチレバー10の一端に支持されたヘッド部2
0は、両側端を下方に折曲したコ字状のヨーク体21と
、ヨーク体21の一方の折曲片に巻き付けられた励磁コ
イル22と、ヨーク体21の励磁コイル22側の一側部
に取り付けらえた方形上のガラス基体23と、このガラ
ス基体23のに而に取り付けられた直角三角柱状のガラ
ス基体24占、励磁コイル22の中心下部に位置するよ
うに垂直に設けた透磁率の高い磁性ガーネット薄膜等か
らなる主磁極25と、この主磁極25をサンドウィッチ
状に挾み付けて保護する透明基体26.26とを一体に
組み合わせて形成されている。主磁極25を保護する透
明基体26.26は、ヨーク体21の下方一端から方形
状のガラス基体23の下方他端にかかるように設けられ
、主磁極25の先端が媒体に接触するように側方上方に
傾斜する略直角三角形形状に形成されている。
On the other hand, the head portion 2 supported by one end of the cantilever 10
0 indicates a U-shaped yoke body 21 with both ends bent downward, an excitation coil 22 wound around one bent piece of the yoke body 21, and one side of the yoke body 21 on the side of the excitation coil 22. A rectangular glass base 23 is attached to the glass base 23, a right triangular prism-shaped glass base 24 is attached to the glass base 23, and a permeable glass base 24 is installed vertically at the bottom of the center of the excitation coil 22. It is formed by integrally combining a main magnetic pole 25 made of a highly magnetic garnet thin film or the like, and a transparent substrate 26, 26 that sandwiches and protects the main magnetic pole 25 in a sandwich-like manner. A transparent substrate 26.26 that protects the main magnetic pole 25 is provided so as to extend from one lower end of the yoke body 21 to the other lower end of the rectangular glass substrate 23, and is placed on the side so that the tip of the main magnetic pole 25 comes into contact with the medium. It is formed into a substantially right triangular shape that slopes upward.

そして、ヘッド部20の上部に設けた三角柱形状のガラ
ス基材24のカンチレバー10側の傾斜面には屈折率分
布型レンズ27が接触して取り付けられ、この屈折率分
布型レンズ27の他方にレーザ光の偏波面を保持して伝
送する偏波面保持ファイバー28の一端が接続されてい
る。偏波面保持ファイバー28は、カンチレバー10を
通してカンチレバー10の後部のヘッド装置本体にカン
チレバーから離れた位置に配設された光学系に至る位置
まで配設されている。偏波面保持ファイバー28は、レ
ンズ27からカンチレバー10の先端部に至る中間で、
カンチレバー移動時の揺れを防ぐため、保持部材29に
よってカンチレバー先端側に固定・保持されている。ま
た、ファイバー28は、その中間部分でカンチレバーの
一端側孔から入り、他端側孔から出ている。
A gradient index lens 27 is attached in contact with the inclined surface of the triangular prism-shaped glass substrate 24 on the cantilever 10 side provided on the upper part of the head section 20, and a laser beam is attached to the other of the gradient index lens 27. One end of a polarization-maintaining fiber 28 that transmits light while maintaining its polarization plane is connected thereto. The polarization maintaining fiber 28 is disposed through the cantilever 10 to a position in the head device main body at the rear of the cantilever 10 to reach an optical system disposed at a position away from the cantilever. The polarization maintaining fiber 28 is located in the middle from the lens 27 to the tip of the cantilever 10.
In order to prevent shaking when the cantilever moves, it is fixed and held at the tip side of the cantilever by a holding member 29. Further, the fiber 28 enters through a hole at one end of the cantilever at its intermediate portion, and exits from a hole at the other end.

偏波面保持ファイバー28を介して光か導かれるカンチ
レバー10後方のヘッド装置本体には、再生用光学系が
配設されている。この光学系は、偏波面保持ファイバー
28の他端に至る光軸方向に宇導体レーザ30と、コリ
メータレンズ31と、ハーフミラ−32と、ファイバー
カップリングレンズ33とが配設され、ファイバー28
を介して戻る戻りのレーザ光がハーフミラ−32を介シ
て偏向される方向に1/2彼長板34、凸レンズ35、
偏光ビームスプリッタ36が配設されている。さらに、
偏光ビームスプリッタ36を介して分光される直交2方
向に光検出器37.38が夫々配設されている。このよ
うに、光学系はいわゆるカー回転角の変化を検出して、
信号再生を行う光磁気検出系で構成されている。ハーフ
ミラ−32と偏波面保持ファイバー28は、カップリン
グレンズ33によって接続されている。
A reproducing optical system is provided in the head device main body behind the cantilever 10 to which light is guided via the polarization maintaining fiber 28. This optical system includes a diode laser 30, a collimator lens 31, a half mirror 32, and a fiber coupling lens 33 arranged in the optical axis direction reaching the other end of the polarization maintaining fiber 28.
A 1/2 length plate 34, a convex lens 35,
A polarizing beam splitter 36 is provided. moreover,
Photodetectors 37 and 38 are respectively arranged in two orthogonal directions in which the light is separated through the polarizing beam splitter 36. In this way, the optical system detects changes in the so-called Kerr rotation angle, and
It consists of a magneto-optical detection system that performs signal reproduction. The half mirror 32 and the polarization maintaining fiber 28 are connected by a coupling lens 33.

以上のように、光学系を配設した本体部とカンチレバー
10とヘッド部20とで構成された転写型光磁気ヘッド
装置は、主磁極25がディスク媒体1の半径方向すなわ
ちトラッキング方向に往復移動できるように周知の送り
機構によって支持されている。
As described above, in the transfer type magneto-optical head device, which is composed of a main body section provided with an optical system, a cantilever 10, and a head section 20, the main magnetic pole 25 can reciprocate in the radial direction of the disk medium 1, that is, in the tracking direction. It is supported by a known feeding mechanism.

次に、上記の転写型光磁気ヘッドによるディスク媒体1
への情報の書き込みおよび読み取りについて説明する。
Next, the disk medium 1 by the above-mentioned transfer type magneto-optical head is
Describe writing and reading information to.

先ず、ディスク媒体1への情報の書き込みを行うとき、
励磁コイル22に情報信号に基づいて電流を流し励磁す
る。そうすると、あらかじめ一方の極性に磁化されたデ
ィスク媒体1のCo−Cr層(記録層)4は、その情報
信号に応じて磁化極性が反転する。この場合、情報信号
と共にトラッキング信号として、ディスク媒体1が1回
転する毎に交仔に切り換わる異なる周波数の信号が情報
信″i予成分の低域にミキシングされる。すると、1木
毎に異なる周波数の成分を交互に含む記録トランクが記
録層4に磁化形成され、ディスク媒体1への情報の書き
込みが行われる。垂直磁気記録の原理については良(知
られているので、詳細な説明を省略する。
First, when writing information to the disk medium 1,
A current is applied to the excitation coil 22 based on the information signal to excite it. Then, the Co--Cr layer (recording layer) 4 of the disk medium 1, which has been previously magnetized to one polarity, has its magnetization polarity reversed in accordance with the information signal. In this case, a signal of a different frequency that switches between each revolution of the disk medium 1 is mixed as a tracking signal together with the information signal into the low frequency range of the information signal "i" pre-component. A recording trunk containing alternating frequency components is magnetized and formed in the recording layer 4, and information is written to the disk medium 1.Since the principle of perpendicular magnetic recording is well known, detailed explanation will be omitted. do.

次に、上述したように情報の書き込みが行われたディス
ク媒体1からの情報の読み取りを行うときは、半導体レ
ーザ30からレーザ光を主磁極先端部に導き照射する。
Next, when reading information from the disk medium 1 on which information has been written as described above, a laser beam is guided from the semiconductor laser 30 to the tip of the main pole and irradiated thereon.

半導体レーザ30から照射されるレーザ光は、コリメー
タレンズ31、ハーフミラ−32を通してファイバーカ
ップリングレンズ33に至り、偏波面保持ファイバー2
8の他端に集光され、ファイバー28を介してヘッド部
20に導かれる。ヘッド部20に導かれたレーザ光は、
屈折率分布型レンズ27を介して集光ビームとしてガラ
ス基体24に傾斜方向に照射され、方形のガラス基体2
3の一側面に至り全反射される。ガラス基体23の一側
面で全反射されたレー ゛ザ光は、下方に位置する主磁
極25を保護する一方の透明基体26に至り、透明基体
26の上下面に多重反射し、一対の透明基体2B、2B
の間に挟まれた主磁極25に至り反射される。このとき
、主磁極25には媒体1の記録層4に磁化形成された磁
界によって記録情報の磁化方向に応じて磁化転写されて
いる。したがって、先端部にレーザ光を集光させると、
主磁極25に反射させた反射レーザ光または透過光には
磁化方向に応じてカー効果・ファラデー効果等の磁気光
学効果によって異なる方向の偏波面の回転が与えられる
。この反射または透過レーザ光は、透明基体26、ガラ
ス基体23.24内を反射して屈折率分布レンズ27に
至り、偏波面保持ファイバー28を介して再び光学系に
戻される。光学系に戻されたレーザ光は、ハーフミラ−
32を介して偏向され、1/2波長板34、凸レンズ3
5、偏光ビームスプリンタ36に至り、偏光ビームスプ
リンタ36を介して2方向に分光され、光検出器37.
38に導かれる。光検出器37.38に受光検出された
光はその強弱に応じた電気信号に変換され、それぞれの
電気信号の差動出力を取り出すことによって再生RF信
号がtuられる。こうして、媒体1からの情報の読み取
りが行われる。一方、RF倍信号−f’A< 分はバン
ドパスフィルタに与えられ、記録の際にミキシングした
異なる周波数の成分が取り出され、整流回路によって直
流分に変換して差動出力される。これにより、励磁コイ
ル13.13を励磁するトラッキングエラー信号が得ら
れ、このエラー信号によってトラッキング制御用励磁コ
イル13.13を励磁してトラッキングサーボが行われ
る。
The laser beam irradiated from the semiconductor laser 30 passes through the collimator lens 31 and the half mirror 32 and reaches the fiber coupling lens 33, and then the polarization maintaining fiber 2
The light is focused on the other end of the fiber 8 and guided to the head section 20 via the fiber 28. The laser beam guided to the head section 20 is
The glass substrate 24 is irradiated in an oblique direction as a condensed beam through the gradient index lens 27, and the rectangular glass substrate 2
It reaches one side of 3 and is totally reflected. The laser beam that is totally reflected on one side of the glass substrate 23 reaches one transparent substrate 26 that protects the main magnetic pole 25 located below, is multiple reflected on the upper and lower surfaces of the transparent substrate 26, and is reflected between the pair of transparent substrates. 2B, 2B
The light reaches the main magnetic pole 25 sandwiched between them and is reflected. At this time, magnetization is transferred to the main magnetic pole 25 according to the magnetization direction of the recorded information by the magnetic field that is magnetized in the recording layer 4 of the medium 1 . Therefore, when the laser beam is focused on the tip,
The reflected laser beam or transmitted light reflected by the main magnetic pole 25 is given rotation of the plane of polarization in different directions by magneto-optical effects such as Kerr effect and Faraday effect depending on the magnetization direction. This reflected or transmitted laser light is reflected within the transparent substrate 26 and the glass substrates 23 and 24, reaches the gradient index lens 27, and is returned to the optical system via the polarization maintaining fiber 28. The laser beam returned to the optical system is passed through a half mirror.
32, a 1/2 wavelength plate 34, and a convex lens 3.
5, the light beam reaches the polarizing beam splinter 36, where the light is split into two directions, and the light is sent to the photodetector 37.
I am led to 38. The light received and detected by the photodetectors 37 and 38 is converted into an electric signal according to its intensity, and a reproduced RF signal is generated by extracting the differential output of each electric signal. In this way, information is read from the medium 1. On the other hand, the RF multiplied signal -f'A< is applied to a bandpass filter, and components of different frequencies mixed during recording are extracted, converted into DC components by a rectifier circuit, and differentially output. As a result, a tracking error signal that excites the excitation coil 13.13 is obtained, and this error signal excites the excitation coil 13.13 for tracking control to perform tracking servo.

発明の詳細 な説明したとおり、本発明の転写型光磁気ヘッドによれ
ば、再生用のレーザ光の供給および主磁極からの反射光
の検出を偏彼而保持ファイバーを介して垂直磁気ヘッド
部をトラッキングサーボするカンチレバーから離れた外
部に取り出して行うようにしているので、主磁極を設け
たヘッド部か軽量化されトラッキング制御を容易かつス
ムースに行うことができる。また、レーザ光を主磁極励
磁型の垂直磁気ヘッドの励磁コイルのF部に位置する主
磁極に至らしめるように、励磁フィルを迂回する光路を
ヘッド部に形成したので、主磁極励磁型の転写型光磁気
ヘッドの実用化が容易に実現できる。
As described in detail, according to the transfer type magneto-optical head of the present invention, the supply of laser light for reproduction and the detection of reflected light from the main magnetic pole are carried out via a polarizing fiber to the perpendicular magnetic head section. Since the tracking servo is carried out by taking it out to the outside away from the cantilever, the weight of the head section provided with the main magnetic pole is reduced, and tracking control can be performed easily and smoothly. In addition, an optical path that bypasses the excitation filter is formed in the head section so that the laser beam reaches the main pole located in the F section of the excitation coil of the main pole excitation type vertical magnetic head. It is easy to put a magneto-optical head into practical use.

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

第1図は本発明に係る転写型光磁気ヘッドのヘッド部分
を示す斜視図、第2図は同分解斜視図、第3図はそのヘ
ッド部分および光学系を示す構成図である。 1・・・ディスク媒体、 10・・Oカンチレバー、 20・・・ヘッド部、 22・・・励磁コイル、 23.24・・・ガラス基体、 25・・・主磁極、 26・・・透明基体、 27・・・屈折率分布型レンズ、 28・・−偏波面保持フアイバー、 3011・拳半導体レーザ、 37.38・拳・光検出器。
FIG. 1 is a perspective view showing a head portion of a transfer type magneto-optical head according to the present invention, FIG. 2 is an exploded perspective view of the same, and FIG. 3 is a configuration diagram showing the head portion and optical system. DESCRIPTION OF SYMBOLS 1... Disk medium, 10... O cantilever, 20... Head part, 22... Excitation coil, 23.24... Glass substrate, 25... Main magnetic pole, 26... Transparent substrate, 27...Gradient index lens, 28...-Polarization maintaining fiber, 3011-Fist semiconductor laser, 37.38-Fist photodetector.

Claims (1)

【特許請求の範囲】[Claims] (1)垂直磁気記録媒体に垂直磁気ヘッドにより情報の
書き込みを行い、再生時にレーザ光を前記媒体から磁化
転写される前記垂直磁気ヘッドの主磁極に照射し、この
主磁極からの反射あるいは透過レーザ光に現れる磁気光
学効果に基づく変化を光検出器により検出して情報の読
み取りを行う転写型光磁気ヘッドにおいて、励磁コイル
を巻き付けたヨーク体と透明基体に保護された薄膜主磁
極とを一体に形成した主磁極励磁型の垂直磁気ヘッドを
カンチレバーの一端に支持し、このカンチレバーの他端
から偏波面保持ファイバーを介して導かれるレーザ光を
前記垂直磁気ヘッドの一側部に設けた屈折率分布型レン
ズを含むガラス基体からなる光学系を通し、かつ前記主
磁極を保護する透明基体中を多重反射させて前記主磁極
に至らしめ、この反射レーザ光を前記透明基体・光学系
および偏波面保持ファイバーを介して前記カンチレバー
外に取り出して前記光検出器に導くようにしたことを特
徴とする転写型光磁気ヘッド。
(1) Information is written on a perpendicular magnetic recording medium by a perpendicular magnetic head, and during reproduction, a laser beam is irradiated onto the main magnetic pole of the perpendicular magnetic head whose magnetization is transferred from the medium, and the reflected or transmitted laser beam from this main magnetic pole is In a transfer-type magneto-optical head that reads information by detecting changes caused by the magneto-optic effect that appear in light using a photodetector, a yoke body around which an excitation coil is wound and a thin-film main pole protected by a transparent base are integrated. The formed main pole excitation type perpendicular magnetic head is supported at one end of a cantilever, and a laser beam guided from the other end of the cantilever via a polarization maintaining fiber is provided on one side of the perpendicular magnetic head. The reflected laser beam passes through an optical system made of a glass substrate including a molded lens and is multiple-reflected in a transparent substrate that protects the main magnetic pole to reach the main magnetic pole, and this reflected laser light is transmitted through the transparent substrate, optical system, and polarization maintaining. A transfer type magneto-optical head, characterized in that it is taken out of the cantilever via a fiber and guided to the photodetector.
JP1982086A 1986-01-30 1986-01-30 Transfer type photomagnetic head Pending JPS62177738A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1982086A JPS62177738A (en) 1986-01-30 1986-01-30 Transfer type photomagnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1982086A JPS62177738A (en) 1986-01-30 1986-01-30 Transfer type photomagnetic head

Publications (1)

Publication Number Publication Date
JPS62177738A true JPS62177738A (en) 1987-08-04

Family

ID=12009951

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1982086A Pending JPS62177738A (en) 1986-01-30 1986-01-30 Transfer type photomagnetic head

Country Status (1)

Country Link
JP (1) JPS62177738A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0283838A (en) * 1988-09-20 1990-03-23 Nec Kansai Ltd Magnetic head
WO1998009287A1 (en) * 1996-08-27 1998-03-05 Quinta Corporation Data storage system having an optical flying head
WO1998009288A1 (en) * 1996-08-27 1998-03-05 Quinta Corporation Offset optics for use with optical heads
WO1998009285A1 (en) * 1996-08-27 1998-03-05 Quinta Corporation Magneto-optical data storage system with high capacity
WO1998009392A3 (en) * 1996-08-27 1998-04-23 Quinta Corp System and method of using optical fibers in a data storage and retrieval system

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0283838A (en) * 1988-09-20 1990-03-23 Nec Kansai Ltd Magnetic head
WO1998009287A1 (en) * 1996-08-27 1998-03-05 Quinta Corporation Data storage system having an optical flying head
WO1998009288A1 (en) * 1996-08-27 1998-03-05 Quinta Corporation Offset optics for use with optical heads
WO1998009285A1 (en) * 1996-08-27 1998-03-05 Quinta Corporation Magneto-optical data storage system with high capacity
WO1998009392A3 (en) * 1996-08-27 1998-04-23 Quinta Corp System and method of using optical fibers in a data storage and retrieval system

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