JPS6299938A - Magnetooptical recording and reproducing device - Google Patents

Magnetooptical recording and reproducing device

Info

Publication number
JPS6299938A
JPS6299938A JP23975385A JP23975385A JPS6299938A JP S6299938 A JPS6299938 A JP S6299938A JP 23975385 A JP23975385 A JP 23975385A JP 23975385 A JP23975385 A JP 23975385A JP S6299938 A JPS6299938 A JP S6299938A
Authority
JP
Japan
Prior art keywords
magnetic pole
recording
signal
magnetic
cantilever
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
JP23975385A
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 JP23975385A priority Critical patent/JPS6299938A/en
Publication of JPS6299938A publication Critical patent/JPS6299938A/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

Landscapes

  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To apply easily tracking control by using a refractive index distribution type lens and a polarization plane maintaining fiber so as to fit a laser light supply source and a detection optical system at a position separated from a main magnetic pole. CONSTITUTION:A thin film main magnetic pole 4 is supported to one end of a cantilever 10, a laser light is led from the other end of the cantilever 10 via the polarization plane maintaining fiber 9 and the laser light is irradiated to the tip of the main magnetic pole through the optical system including the refractive index distribution lenses 8, 6. Then the reflected or transmitted laser light is extracted at the outside of the cantilever via the original optical system and fiber and fed to a photodetector. thus, the part in contact with a medium is made light to facilitate the movement of the cantilever supporting the main magnetic pole and the tracking control is facilitated.

Description

【発明の詳細な説明】 産業上の利用分野 この発明は垂直磁気記録さI]、た媒体からレーザ光を
用い一〇光再生する磁気、光記録再生装置に係り、特に
補助磁極励磁型の垂直磁気ヘッドを用いた再生手段の構
造に係るものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application This invention relates to a magnetic/optical recording and reproducing apparatus for reproducing perpendicular magnetic recording media using a laser beam, and particularly relates to an auxiliary magnetic pole excitation type perpendicular recording/reproducing apparatus. This relates to the structure of a reproducing means using a magnetic head.

従来の技術 磁気記録媒体に垂直磁気記録する一方式として、薄j摸
主磁極と補助磁極を媒体の両面から向い合わせに配置し
、補助磁極を記録信号で励磁することによるものがある
。垂直磁気記・緑は周知のように、従来の長手方向の面
内磁気記録に比べて暖奮度および面密度を高めることが
できる。面密度は記録トラックの幅を狭くすれば良いが
、その分再生出力すなわちC/N比が磁気再生の場合劣
化することが知られている。
BACKGROUND OF THE INVENTION One type of perpendicular magnetic recording on a magnetic recording medium is to arrange a thin main magnetic pole and an auxiliary magnetic pole facing each other on both sides of the medium, and to excite the auxiliary magnetic pole with a recording signal. As is well known, perpendicular magnetic recording can increase the heating degree and areal density compared to conventional longitudinal longitudinal magnetic recording. Although the areal density can be improved by narrowing the width of the recording track, it is known that the reproduction output, that is, the C/N ratio, deteriorates accordingly in the case of magnetic reproduction.

そこで、トラック幅を狭くし、かつC/Nを高めること
が考えられてきた。その方法として再生時において磁化
方向の変化を光の変化として取り出すことが考えられて
きた。その場合、用いられる光はレーザ光が適切であり
、レーザ光を薄膜主磁極の先端部に集光させ主磁極面か
らの反射光あるいは透過光を光学系を介して取り出し光
検出器により電気信号に変換する。
Therefore, attempts have been made to narrow the track width and increase the C/N. As a method for this, it has been considered to extract changes in the magnetization direction as changes in light during reproduction. In that case, the appropriate light to be used is a laser beam, which is focused on the tip of the thin-film main pole, and the reflected or transmitted light from the main pole surface is extracted through an optical system and sent to a photodetector to generate an electrical signal. Convert to

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磁化分布が現われる
。その磁化分布から得られるレーザ光の反射光ある−い
(d透過光には、カー効果あるいはファラデー効果と呼
ばれる磁気光学効果に基づいて偏波面の回転が与えられ
る。光検出器はこれを光の強弱として感知し、電気信号
に変換する。
At the tip of the main pole, a magnetization distribution appears that corresponds to the magnetization information on the magnetic recording medium that is in contact with it, that is, the polarity of the recording bit. The reflected light of the laser beam obtained from the magnetization distribution (d) The transmitted light is given a rotation of the plane of polarization based on the magneto-optic effect called the Kerr effect or the Faraday effect. It senses strength and weakness and converts it into an electrical signal.

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1莫主磁極を用いるのでレーザ光記録(1μ
m/bit)  より高い値(o、1 μm/bit)
を持つことができ、かつ再生時のC/Nを高めるためト
ラック密度すなわちトラック幅を光記録並の値(1,6
μm)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6発明が解決しよう
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磁気・光ヘ
ツド装置では、主磁極側がレーザ光の照射を行う手段を
一体に備えた構造であるため大型であるばかりか重量が
大きいため動きが悪く、トラッキングサーボが十分に実
施し得す、実用化に未だ適していなかった。
Therefore, by recording with the perpendicular magnetization method, a thin 1μ main magnetic pole is used for linear density, so laser light recording (1μ
m/bit) Higher value (o, 1 μm/bit)
In order to increase the C/N during reproduction, the track density, that is, the track width, is set to a value similar to that of optical recording (1,6
6. Problems to be Solved by the Invention However, this type of magnetic/optical head device that has been conventionally considered is Since the main magnetic pole side has a structure in which the means for irradiating the laser beam is integrated, it is not only large but also heavy, making it difficult to move, and the tracking servo cannot be fully implemented, so it is not yet suitable for practical use. Ta.

したがって、この発明の目的は、容易にトラッキングサ
ーボが適用できる磁気・光ヘツド装置の構成を与えるこ
とにある。
Therefore, an object of the present invention is to provide a configuration of a magnetic/optical head device to which tracking servo can be easily applied.

問題を解決するだめの手段) この発明は、垂直磁気記録媒体の一方の面に励磁型、補
助磁極を配置し、この補助磁極に対応して媒体の他方の
面に薄膜主磁極を配置し、補助磁極を記録信号で励磁す
ることにより媒体に垂直磁気記録を施し、再生時にはレ
ーザ光を主磁極先端部に照射し、その先端部の反射光あ
るいは透過光に現わ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再生信号を得るようにした磁気・
光記録再生装置に適用されるものである。すなわち、薄
膜主磁極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レーザ光
を導びき、そのレーザ光を屈折率分布型レンズを含む光
学系を通して前記主磁極の先端部に照射し、反射あるい
は透過レーザ光を元の光学系および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供給するようにし
たことを特徴としたものである。
Means for Solving the Problem) This invention arranges an excitation type auxiliary magnetic pole on one side of a perpendicular magnetic recording medium, and arranges a thin film main magnetic pole on the other side of the medium corresponding to the auxiliary magnetic pole, Perpendicular magnetic recording is performed on the medium by exciting the auxiliary magnetic pole with a recording signal, and during playback, a laser beam is irradiated to the tip of the main magnetic pole, and changes due to the magneto-optic effect that appear in the reflected or transmitted light from the tip are optically detected. Magnetic /
It is applied to optical recording and reproducing devices. That is, a thin film main pole is supported at one end of the cantilever, a laser beam is guided from the other end of the cantilever via a polarization maintaining fiber, and the laser beam is directed to the main pole through an optical system including a gradient index lens. The feature is that the tip is irradiated, and the reflected or transmitted laser light is taken out of the cantilever via the original optical system and fiber and supplied to a photodetector.

作用 この発明の磁気・光記録再生装置によれば、薄膜主磁極
をカンチレバーに取り付け、主磁極の先端部に照射する
レーザ光の光源と反射光あるいは透過光を検出する光検
出器とをカンチレバーから分離した位置に設け、偏波面
保持ファイバーを用イ’t−ソの間のレーザ光のやりと
ユヲ行うようにしている。その結果、媒体と接する部分
が軽量となって主磁極を支持するカンチレバーの動きが
容易となり、トラッキング制御を行えるようになった。
According to the magnetic/optical recording and reproducing device of the present invention, a thin film main pole is attached to a cantilever, and a light source of a laser beam that irradiates the tip of the main pole and a photodetector that detects reflected light or transmitted light are connected from the cantilever. The polarization maintaining fibers are installed at separate positions, and the polarization maintaining fiber is used as a laser beam beam between the laser beam and the laser beam. As a result, the portion in contact with the medium has become lighter, making it easier for the cantilever that supports the main pole to move, making it possible to perform tracking control.

実施例 この発明の実施例について以下図面を参胆して説明する
。第1図乃至第3図は主磁極とカンチレバーの部分につ
いて示す図である。
Embodiments Examples of the present invention will be described below with reference to the drawings. FIGS. 1 to 3 are diagrams showing the main magnetic pole and the cantilever.

1はポリエステルフィルムからなるディスクで、その一
方の面には例えばCo−Crの垂直磁気記録媒体のスパ
ッタ薄膜2が形成されている。この媒体2の一方の面、
すなわちポリエステルフィルム1側には励磁型の補助磁
極3が配置され、また他方の面にはCo−Zr−Taな
どの誂1磁気異方性を持つ薄膜主磁極4の先端が接触す
るように配置されている。主磁極4の回りはガラス保持
体5によって囲まれている。主磁極4の他端側には屈折
率分布型レンズ6が接触され、その上にはミラー7、屈
折率分布型レンズ8が設けられている。屈折率分布型レ
ンズ6.8は円柱状レンズで、入射光を所定の屈折率分
布に従って集光させる働きをする。
Reference numeral 1 denotes a disk made of a polyester film, on one surface of which a sputtered thin film 2 of, for example, a Co--Cr perpendicular magnetic recording medium is formed. One side of this medium 2,
That is, an excitation type auxiliary magnetic pole 3 is arranged on the polyester film 1 side, and the tip of a thin film main magnetic pole 4 having a magnetic anisotropy such as Co-Zr-Ta is arranged so as to be in contact with the other side. has been done. The main magnetic pole 4 is surrounded by a glass holder 5. A gradient index lens 6 is in contact with the other end of the main pole 4, and a mirror 7 and a gradient index lens 8 are provided above it. The refractive index gradient lens 6.8 is a cylindrical lens that functions to condense incident light according to a predetermined refractive index distribution.

レンズ6の場合、ミラー7を経て入射するレーザ光を主
磁極4の先端部へ集めるが、この種のレンズid rs
elfoc J (商標)として市販されているもので
ある。また、レンズ8は入射光の偏波面を保持して伝送
する偏波面保持ファイバー9へ反射光を注入するために
配置される。偏波面保持ファイバー9・はカンチレバー
10の一端側の孔から内部に入り、他端側の孔から取り
出されて後述する光学系へ導びかれる。カンチレバー1
0は一端に主磁極4を含む光学ブロックを支持しており
、他端において中立位置保持ダンパー11によって、図
示してないがディスク上をリニア駆動する周知の構造の
ヘッドキャリアに支持されている。ダンパー11より更
に端部には永久磁石12が取り付けられ℃おり、励磁コ
イル13によってカンチレバー10が握られ、主磁極4
がディスク面上を水平にかつ記録トラック15に対して
実質的に直角方向移動できるようになっている。すなわ
ち、記録トラック15の所定のものを再生時に正確にト
レースするトラッキング制御機構を構成している。
In the case of the lens 6, the laser beam incident through the mirror 7 is focused on the tip of the main magnetic pole 4, but this type of lens id rs
It is commercially available as elfoc J (trademark). Further, the lens 8 is arranged to inject reflected light into a polarization-maintaining fiber 9 that transmits the incident light while maintaining its polarization plane. The polarization maintaining fiber 9 enters the cantilever 10 through a hole at one end, is taken out from a hole at the other end, and is guided to an optical system to be described later. cantilever 1
0 supports an optical block including a main magnetic pole 4 at one end, and is supported at the other end by a neutral position holding damper 11 on a head carrier (not shown) having a well-known structure that linearly drives the disk. A permanent magnet 12 is attached to the end further than the damper 11, and the cantilever 10 is gripped by the excitation coil 13, and the main magnetic pole 4
can move horizontally on the disk surface and in a direction substantially perpendicular to the recording track 15. In other words, it constitutes a tracking control mechanism that accurately traces a predetermined portion of the recording track 15 during reproduction.

第4図はカンチレバーを省略して示したものであるが、
レーザ光の流れが理解できる。20はレーザダイオード
、21はコリメータレンズ、22はビームスプリッタ、
23はIA波長板、24は単レンズ、25け偏光ビーム
スプリッタ、26および27は光検出器であり、これら
は周知の構成である。ビームスプリッタ22と偏波面保
持ファイバー9との間にはカップリングレンズ14が設
けられ℃いる。
Although the cantilever is omitted in Figure 4,
Understand the flow of laser light. 20 is a laser diode, 21 is a collimator lens, 22 is a beam splitter,
23 is an IA wavelength plate, 24 is a single lens, 25 polarizing beam splitters, and 26 and 27 are photodetectors, which are of well-known construction. A coupling lens 14 is provided between the beam splitter 22 and the polarization maintaining fiber 9.

記録時においては、補助磁極3を記録信号で励磁すると
、予め一方の極性に磁化された垂直磁気記録媒体2け、
その信号に応じて磁化極性が反転する。この場合、記録
信号中にはトラッキング信号として、ディスクの1回転
置きに交互に切換わる異なる周波数f、、f、の信号が
第6図のスペクトラムに示すように一情報信号成分16
の低域にミキシングされる。すると、第3図に示すよう
に1本毎にfh、f−の成分を交互に含む記録トラック
15が媒体2に磁化形成される。
During recording, when the auxiliary magnetic pole 3 is excited with a recording signal, two perpendicular magnetic recording media magnetized to one polarity in advance,
The magnetization polarity is reversed according to the signal. In this case, in the recording signal, as a tracking signal, signals of different frequencies f, , f, which are alternately switched every other rotation of the disk, are included in one information signal component 16 as shown in the spectrum of FIG.
is mixed into the low range. Then, as shown in FIG. 3, recording tracks 15 are magnetized and formed on the medium 2, each of which alternately contains fh and f- components.

再生時においては、レーザダイオード2oから発射され
るレーザ光がコリメータレンズ21、ビームスフリツタ
22、カップリングレンズ14、偏波面保持ファイバー
9、屈折率分布型レンズ8、ミラー7、屈折率分布型レ
ンズ6を介して媒体2と接触する薄膜主磁極4の先端部
へ照射される。
During reproduction, the laser beam emitted from the laser diode 2o passes through the collimator lens 21, beam fritter 22, coupling lens 14, polarization maintaining fiber 9, gradient index lens 8, mirror 7, gradient index lens The beam is irradiated onto the tip of the thin film main pole 4 which contacts the medium 2 through the beam 6 .

主磁極4の先端部は、媒体2からの漏洩磁界によってそ
の磁化方向が変化する。したがって、先端“部に直線偏
光のレーザ光を集光させると、薄膜主磁極4の反射光あ
るい(d透過光には、カー効果あるいはファラデー効果
等の磁気光学効果に基づいた偏波面の回転が与えられる
。この反射光および透過光は屈折率分布型レンズ6、ミ
ラー7、屈折率分布型レンズ8、偏波面保持ファイバー
9、カップリングレンズ14、スプリッタ22.捧波長
板23、単レンズ24、偏光ビームスプリンタ25を介
して′・光検出器26.27に伝送され、電気信号に変
換される。
The magnetization direction of the tip of the main pole 4 changes due to the leakage magnetic field from the medium 2. Therefore, when a linearly polarized laser beam is focused on the tip, the reflected light from the thin-film main magnetic pole 4 or the transmitted light has a rotation of the plane of polarization based on magneto-optic effects such as the Kerr effect or the Faraday effect. This reflected light and transmitted light are transmitted through a gradient index lens 6, a mirror 7, a gradient index lens 8, a polarization maintaining fiber 9, a coupling lens 14, a splitter 22, a dedicated wavelength plate 23, and a single lens 24. , are transmitted to the photodetectors 26 and 27 via the polarization beam splinter 25 and converted into electrical signals.

光検出器26,28は入射光の偏波面の回転を光の強弱
として感知するが、それぞれで変換された電気信号は対
応する各増幅器3()、31を介して差動増幅器32に
与えられ、その出力はRF倍信号して記録情報の再生回
路に端子33から与えられる。一方、RF倍信号一部分
はバンドパスフィルタ34.35に与えられ、周波数f
、およびf2の信号が取り出され、整流回路36.37
によって各直流分に変換される。各直流信号は差動増幅
器38に与えられ、トラッキングエラー信号として端子
39より取り出さ11−1励磁コイル13を励磁するト
ラッキング制御信号として用いられる。
The photodetectors 26 and 28 sense the rotation of the plane of polarization of the incident light as the strength and weakness of the light, and the electrical signals converted by each are given to the differential amplifier 32 via the corresponding amplifiers 3() and 31. , the output thereof is converted into an RF signal and is applied from a terminal 33 to a recording information reproducing circuit. On the other hand, a part of the RF multiplied signal is given to a bandpass filter 34.35, and the frequency f
, and f2 signals are taken out and rectified circuits 36 and 37
is converted into each DC component by Each DC signal is applied to a differential amplifier 38, taken out from a terminal 39 as a tracking error signal, and used as a tracking control signal to excite the 11-1 excitation coil 13.

発明の詳細 な説明してきたように、この発明の磁気・光記録再生装
置によれば、磁気記録媒体に垂直磁気記録し、再生時に
は記録時に用いた薄膜主磁極の先端部にレーザ光を照射
し、反射光あるいは透過光の磁気光学効果を検出して再
生信号を得るようにしており、したがって再生専用のヘ
ッドを準備する必要がない。
As described in detail, the magnetic/optical recording and reproducing apparatus of the present invention performs perpendicular magnetic recording on a magnetic recording medium, and during reproduction, irradiates the tip of the thin film main pole used during recording with a laser beam. The reproduction signal is obtained by detecting the magneto-optic effect of reflected light or transmitted light, and therefore there is no need to prepare a head exclusively for reproduction.

また、屈折率分布型レンズと偏波面保持ファイバーを用
いることによりレーザ光供給源および反射光、透過光の
検出を行う光学系を主磁極から分離した位置に取り付け
ることができ、その結果、主磁極側を極力軽量化したの
でカンチレバーで主磁極を支持することによって容易に
トラッキング制御ができるようになった。
In addition, by using a gradient index lens and polarization maintaining fiber, the laser light source and the optical system for detecting reflected light and transmitted light can be installed in a position separated from the main magnetic pole. By reducing the side weight as much as possible, tracking control can now be easily performed by supporting the main magnetic pole with a cantilever.

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

第1図はこの発明の実施例に係る磁気・光記録再生装置
のヘッド部分を示す正面図、第2図は同平面図、第3図
は同斜視図、第4図は同光学系の構成を示す説明用構造
図、第5図は信号再生系のブロック回路図、第6図は周
波数スペクトラム図である。 2・・・・・・垂直磁気記碌媒体、 3・・・・・・励磁型補助磁極、 4・・・・・・薄膜主磁極、 6および8・・・・・・屈折率分布型レンズ、7・・・
・・・ミラー、 9・・・・・・偏波面保持ファイバー、10・・・・・
・カンチレバー、 20・・・・・・ レーザダイオード、26および27
・・・−光検出器。 特許出願人  日本取気ホームエレクトロニクス株式会
社 第  1  図 第  2 図
FIG. 1 is a front view showing the head portion of a magnetic/optical recording/reproducing device according to an embodiment of the present invention, FIG. 2 is a plan view thereof, FIG. 3 is a perspective view thereof, and FIG. 4 is a configuration of the optical system. FIG. 5 is a block circuit diagram of a signal reproducing system, and FIG. 6 is a frequency spectrum diagram. 2... Perpendicular magnetic recording medium, 3... Excitation type auxiliary magnetic pole, 4... Thin film main magnetic pole, 6 and 8... Gradient index lens. ,7...
... Mirror, 9 ... Polarization maintaining fiber, 10 ...
・Cantilever, 20... Laser diode, 26 and 27
...-photodetector. Patent Applicant Nihon Toki Home Electronics Co., Ltd. Figure 1 Figure 2

Claims (2)

【特許請求の範囲】[Claims] (1)、垂直磁気記録媒体の一方の面に励磁型補助磁極
を配置し、この補助磁極に対応して前記媒体の他方の面
に薄膜主磁極を配置し、前記補助磁極を記録信号で励磁
することにより前記媒体に垂直磁気記録を施し、再生時
にはレーザ光を前記主磁極先端部にて照射し、前記先端
部の反射光あるいは透過光に現わ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再生信号を得るよう
にした磁気・光記録再生装置において、前記薄膜主磁極
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びかれるレーザ
光を屈折率分布型レンズを含む光学系を通して前記薄膜
主磁極の先端部に照射し、反射あるいは透過レーザ光を
前記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前記光検出器に供給することを
特徴とする磁気・光記録再生装置。
(1) An excitation type auxiliary magnetic pole is placed on one side of a perpendicular magnetic recording medium, a thin film main magnetic pole is placed on the other side of the medium corresponding to this auxiliary magnetic pole, and the auxiliary magnetic pole is excited with a recording signal. By doing so, perpendicular magnetic recording is performed on the medium, and during reproduction, a laser beam is irradiated at the tip of the main magnetic pole, and a photodetector detects a change based on the magneto-optic effect that appears in the light reflected or transmitted from the tip. In a magnetic/optical recording and reproducing apparatus which obtains a reproduced signal using irradiating the tip of the thin film main pole through an optical system including a distributed lens, and taking out reflected or transmitted laser light out of the cantilever via the optical system and polarization maintaining fiber and supplying it to the photodetector. Characteristic magnetic/optical recording and reproducing device.
(2)、記録信号成分は情報信号と共にトラッキング信
号として所定の周波数を持つ信号をミキシングしたもの
をスペクトラムとして持ち、再生信号から前記トラッキ
ング信号を分離して取り出して前記主磁極のトラッキン
グ制御を行うことを特徴とする特許請求の範囲第1項記
載の磁気・光記録再生装置。
(2) The recording signal component has a spectrum obtained by mixing a signal having a predetermined frequency as a tracking signal with an information signal, and the tracking signal is separated and extracted from the reproduction signal to perform tracking control of the main magnetic pole. A magnetic/optical recording/reproducing device according to claim 1, characterized in that:
JP23975385A 1985-10-25 1985-10-25 Magnetooptical recording and reproducing device Pending JPS6299938A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23975385A JPS6299938A (en) 1985-10-25 1985-10-25 Magnetooptical recording and reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23975385A JPS6299938A (en) 1985-10-25 1985-10-25 Magnetooptical recording and reproducing device

Publications (1)

Publication Number Publication Date
JPS6299938A true JPS6299938A (en) 1987-05-09

Family

ID=17049411

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23975385A Pending JPS6299938A (en) 1985-10-25 1985-10-25 Magnetooptical recording and reproducing device

Country Status (1)

Country Link
JP (1) JPS6299938A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1998009285A1 (en) * 1996-08-27 1998-03-05 Quinta Corporation Magneto-optical data storage system with high capacity
WO1998009287A1 (en) * 1996-08-27 1998-03-05 Quinta Corporation Data storage system having an optical flying head
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 (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1998009285A1 (en) * 1996-08-27 1998-03-05 Quinta Corporation Magneto-optical data storage system with high capacity
WO1998009287A1 (en) * 1996-08-27 1998-03-05 Quinta Corporation Data storage system having an optical flying head
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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