JPS5930255A - Magnetooptic head - Google Patents

Magnetooptic head

Info

Publication number
JPS5930255A
JPS5930255A JP13843782A JP13843782A JPS5930255A JP S5930255 A JPS5930255 A JP S5930255A JP 13843782 A JP13843782 A JP 13843782A JP 13843782 A JP13843782 A JP 13843782A JP S5930255 A JPS5930255 A JP S5930255A
Authority
JP
Japan
Prior art keywords
thin film
magnetic thin
magnetic
light
reflected
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.)
Granted
Application number
JP13843782A
Other languages
Japanese (ja)
Other versions
JPH0355894B2 (en
Inventor
Tatsuo Nomura
龍男 野村
Shozo Nakagawa
中川 省三
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.)
Japan Broadcasting Corp
Original Assignee
Nippon Hoso Kyokai NHK
Japan Broadcasting Corp
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 Nippon Hoso Kyokai NHK, Japan Broadcasting Corp filed Critical Nippon Hoso Kyokai NHK
Priority to JP13843782A priority Critical patent/JPS5930255A/en
Publication of JPS5930255A publication Critical patent/JPS5930255A/en
Publication of JPH0355894B2 publication Critical patent/JPH0355894B2/ja
Granted 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
    • 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

Abstract

PURPOSE:To read information at a high S/N ratio with high efficiency and high resolution, by laminating the 1st magnetic thin film, a metallic thin film, and the 2nd magnetic thin film in order on a transparent substrate, and making the 2nd magnetic thin film thicker than the 1st magnetic thin film. CONSTITUTION:The thicker magnetic thin film 15 and thinner magnetic thin film 13 are magnetized in their inward surface directions by a magnetic filed produced from a recording medium 1. Light from a light source 4 is passed through a polarizer 5 to obtain linear polarized light 18, which illuminates the transparent substrate 11 through a half-mirror 10 and is reflected by a side surface 12 after transmits the magnetic thin film 13 and then converged to the focus 17 of the parabola of the side surface 12. Part of this converged luminous flux is reflected by a metallic thin film 14 and the remaining luminous flux is reflected again by a magnetic thin film 15 to obtain parallel luminous flux 19 from the side surface 12, which enters a photodetector 9 from the half-mirror 10. Thus, the light is reflected by the magnetic thin film 13 and transmitted through the magnetic thin film 13 twice, so that its plane of polarization is rotated.

Description

【発明の詳細な説明】 本発明は磁気記録媒体(以下、単に記録媒体と呼ぶ)上
に記録された情報を光学的に読み出す磁気−光ヘッドに
関するものであり、特に磁化の変化として高密度に記録
された情報を高効率で高分解能かつ高い信号対雑音比を
もって読み出すことができるようにしたものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic-optical head that optically reads information recorded on a magnetic recording medium (hereinafter simply referred to as a recording medium). This allows recorded information to be read out with high efficiency, high resolution, and a high signal-to-noise ratio.

従来、このような磁化情報の読み出しには、第1図に示
すような構造の磁気−光変換器が提案されている。第1
図に示す記録媒体lから生じた磁界によって、この媒体
lの表面に接近し、この媒体lと平行にならないように
プリズムコと2′トニより保持された磁性薄膜3が磁化
される。その磁化部分に、光源ダから偏光子5およびレ
ンズ6を経て形成した収束光を当てると、カー効果ある
いはファラデー効果によって偏光面の回転が生じ、その
出力光をレンズクより検光子gに導き、更に光検出器9
により情報が読み出される。
Conventionally, for reading such magnetization information, a magneto-optical converter having a structure as shown in FIG. 1 has been proposed. 1st
The magnetic field generated from the recording medium 1 shown in the figure magnetizes the magnetic thin film 3 which approaches the surface of the medium 1 and is held by the prism head and the 2' edge so as not to be parallel to the medium 1. When the convergent light formed from the light source DA passes through the polarizer 5 and the lens 6 is applied to the magnetized part, the plane of polarization is rotated due to the Kerr effect or Faraday effect, and the output light is guided from the lens to the analyzer g, and further Photodetector 9
The information is read out.

しかし、この磁気−光変換器には次のような欠点がある
However, this magneto-optical converter has the following drawbacks.

(1)  磁性N膜3の磁化を検出して電気信号に変換
するための光学系り、5μ、7.ざおよび7が複雑であ
り、その変換器の小型化やこれを高速に動かして必要な
情報トラックへアクセスすることが困難である。
(1) Optical system for detecting the magnetization of the magnetic N film 3 and converting it into an electric signal, 5μ, 7. The complexity of the transducer and the difficulty in miniaturizing the transducer and moving it at high speed to access the necessary information tracks is difficult.

(,2)  7アラデー効果を用いて読み出しを行なう
ことから使用される磁性薄膜3の厚さがzoo X以下
と薄くものであるため、記録媒体/がら生じる磁界を有
効に磁性薄膜3に集めることができず、したがって、と
くに高密度に記録された情報の読み出しでは性能の低下
が生じる。
(,2) Since reading is performed using the 7 Alladay effect, the thickness of the magnetic thin film 3 used is as thin as less than zooX, so the magnetic field generated by the recording medium can be effectively collected on the magnetic thin film 3. Therefore, the performance deteriorates, especially when reading information recorded at high density.

そこで、本発明の目的は、かがる欠点を排除して、記録
媒体に高密度に記録された情報を高能率で高分解能かつ
高い信号対雑音比をもって読み出し得る小型にして、高
性能の磁気−光ヘッドを提供することにある。
SUMMARY OF THE INVENTION Therefore, an object of the present invention is to eliminate such drawbacks and to provide a compact and high-performance magnetic recording medium capable of reading out information recorded at high density on a recording medium with high efficiency, high resolution, and a high signal-to-noise ratio. - To provide an optical head.

=かかる目的を達成するために、本発明は、透明基板上
に第1の磁性薄膜と、金属#膜と、第一の磁性薄膜とを
′この順序で積層し、前記第一の磁性薄膜を前記第1の
磁性N膜よりも厚くしたことを特徴とするものである。
= In order to achieve such an object, the present invention laminates a first magnetic thin film, a metal film, and a first magnetic thin film in this order on a transparent substrate, and stacks the first magnetic thin film on a transparent substrate. It is characterized in that it is thicker than the first magnetic N film.

以下に図面を参照して本発明の詳細な説明する。The present invention will be described in detail below with reference to the drawings.

本発明磁気−光ヘッドの構成の一例を第、2図に示す。An example of the structure of the magnetic-optical head of the present invention is shown in FIG. 2.

ここで、//はガラスなどによる透明基板であり、その
断面の一方は放物線を形成するものとする。この側面7
.2は高い反射率をもつ金属膜(たとえば、アルミニウ
ム膜)で被覆しておく。透明基板//上には第1の磁性
薄膜/J1非磁性金属薄膜/11.および第一の磁性′
iIi膜/左をこの順序で積層し、更にその第コ磁性薄
膜/左上に保護膜/乙を形成する。
Here, // is a transparent substrate made of glass or the like, and one of its cross sections forms a parabola. This side 7
.. 2 is covered with a metal film (for example, an aluminum film) having a high reflectance. Transparent substrate //First magnetic thin film/J1 nonmagnetic metal thin film/11. and the first magnetism′
The iIi film/left is laminated in this order, and the protective film/B is further formed on the upper left of the comagnetic thin film.

ここで、積層された磁性薄膜/3および/3は記録媒体
/の表面に接近し、これと平行しないように保持してお
く。
Here, the laminated magnetic thin films /3 and /3 are kept close to the surface of the recording medium / so as not to be parallel to it.

第一図において、記録媒体lがら発生した磁界ハ、厚さ
XOOA〜3000 Xの磁性薄膜/!r(たとえばパ
ーマ四イ薄膜)および厚さ100X〜J00 Xの磁性
薄膜/3(たとえば鉄薄膜)をその面内方向に磁化する
In Fig. 1, the magnetic field generated by the recording medium l is a magnetic thin film with a thickness of XOOA~3000X/! A magnetic thin film/3 (for example, an iron thin film) with a thickness of 100X to J00X is magnetized in the in-plane direction.

光源ヶからの平行光は偏光子3を透過して直線偏光光/
gとなり、この光/gは半透明鏡10を通った後、本発
明光−磁気ヘッドの透明基板//に入射する。透明基板
//に入射した光束は側面7.2で反射されて、磁性薄
膜/3を透過した後、側面/コの放物線の焦点/7に収
束する。この焦点/7の位置には、反射率が高くかつ厚
さ50八〜、ZOOAの金属薄膜/りが配置されており
、ここに収束した光束の一部は金属薄膜/りで、また残
りの光束は磁性薄膜/3で再び反射され、さらに側面/
コで反射されて平行光束/9となる。
The parallel light from the light source passes through the polarizer 3 and becomes linearly polarized light/
After passing through the semi-transparent mirror 10, this light /g enters the transparent substrate // of the optical-magnetic head of the present invention. The light beam incident on the transparent substrate // is reflected by the side surface 7.2, passes through the magnetic thin film /3, and then converges at the focal point /7 of the parabola on the side surface /C. At the focal point /7, a ZOOA metal thin film with high reflectance and a thickness of 50 mm is placed, and part of the light beam converged here is absorbed by the metal thin film and the rest. The light flux is reflected again by the magnetic thin film /3 and further reflected by the side surface /3.
It is reflected by , resulting in a parallel beam of light /9.

平行光束/9は半透明鏡IOで反射されてレンズクを経
て検光子gに入射する。検光子gを透過した光は光検出
器9で電気信号に変換される。
The parallel light beam /9 is reflected by the semi-transparent mirror IO and enters the analyzer g through the lens. The light transmitted through the analyzer g is converted into an electrical signal by a photodetector 9.

平行光束/gは、透明基板//に入射して再びこの透明
基板//から出射するまでに記録媒体lから発生した磁
界によって磁化された磁性薄膜/3で反射され、または
この磁性薄膜/3を一回透過することによって、その偏
光面はカー効果およびファラデー効果によって回転する
The parallel light flux /g is reflected by the magnetic thin film /3 magnetized by the magnetic field generated from the recording medium l, or is reflected by the magnetic thin film /3 before it enters the transparent substrate // and exits from the transparent substrate // again. By passing through once, the plane of polarization is rotated by Kerr effect and Faraday effect.

次に本発明磁気−光ヘッドを使用した場合の読み出し可
能な記録密度について述べる。記録媒体lとして、第3
図に示すように、C0−Cr膜のような垂直磁化膜を用
いた場合、幅すのビットを正しく読み出すためには、b
以下の厚さをもつ磁性薄膜13を用いる必要がある。例
えば、磁性薄膜15の厚さを〃θθA −、?θθθA
とするときには、読み出し可能な線密度はioθKBP
I以上となる。また、前述の各薄膜/、3./’Iおよ
び/Sで示される積層した磁性薄膜の幅はりソグラフイ
技術によって5μm以下とすることができるので、読み
出し可能なトラ゛ンク密度はおよそ300θTPIとな
る。
Next, the readable recording density when using the magnetic-optical head of the present invention will be described. As the recording medium l, the third
As shown in the figure, when using a perpendicular magnetization film such as a C0-Cr film, in order to correctly read the bits of the width
It is necessary to use the magnetic thin film 13 having the following thickness. For example, the thickness of the magnetic thin film 15 is set to θθA −, ? θθθA
Then, the readable linear density is ioθKBP
I or more. In addition, each of the above-mentioned thin films/, 3. Since the width of the laminated magnetic thin films indicated by /'I and /S can be reduced to 5 μm or less using the lithography technique, the readable trunk density is approximately 300θTPI.

第q図は本発明磁気−光ヘッドの他の例を示し、ここで
は、各薄膜/3./’!および/jと保護膜/6とから
なる積層磁性簿膜ユニット〃、コ/および、2コを7個
の透明基板//に対して並置し、これらユニット〃、コ
/および、2jの各々を記録媒体l上の記録トラック、
2.?、2&およびJの位置に対応させる。ここで、透
明基板//に入射する光は、各ユニット曜、2/および
!、2に関連づけられた光ビーム、例えば各ユニッ)J
、、2/および二に対応する個別の光ビームあるいはこ
れらユニットをすべて光合するスリット状光ビームとす
る。かかる光ビームを透明基板//に入射させる″こと
によって、複数本のトラック、23゜−りおよび5の情
報を個別の光検出器、2A、27およびHによって同時
に読み出すことができる。
FIG. q shows another example of the magneto-optical head of the present invention, in which each thin film/3. /'! A laminated magnetic film unit consisting of a protective film /6 and a protective film /6 is placed side by side with respect to seven transparent substrates //, and each of these units 〃, ko/ and 2j is a recording track on a recording medium l;
2. ? , 2 & and J positions. Here, the light incident on the transparent substrate // is for each unit YO, 2/ and ! , 2, e.g. each unit) J
, 2/ and 2, or a slit-shaped light beam that combines all of these units. By making such a light beam incident on the transparent substrate //, information on a plurality of tracks 23 DEG and 5 can be read out simultaneously by individual photodetectors 2A, 27 and H.

以上述べたごとく、本発明磁気−光ヘッドは、記録媒体
lから発生する磁界を比較的厚い磁性薄膜/3によって
能率よく集めるとともに、磁性薄膜15に近接する簿い
磁性薄膜/3を用いて磁気光学的に読み出すものである
As described above, the magneto-optical head of the present invention efficiently collects the magnetic field generated from the recording medium 1 by the relatively thick magnetic thin film /3, and uses the thin magnetic thin film /3 adjacent to the magnetic thin film 15 to efficiently collect the magnetic field generated from the recording medium l. It is read out optically.

ここで、金属薄膜/4’は反射率を改善するとともに、
磁性薄膜/夕と磁性薄膜/3の磁気的相互作用を強める
働きをもつ。このため、記録媒体lから発生する磁界に
よって、磁性薄膜/3は強く磁化される0 この時、読み出しに用いる光の収束スポットの大きさは
、読み出しの分解能には無関係であり、磁性薄膜/3と
してファラデー効果が大きく、キュリ一温度の高い材料
(たとえば、鉄薄膜)を用いれば、読み出し時の入射光
の強度を大きくすることができることから、本発明によ
れば、大きな信号対雑音比を得ることができる。
Here, the metal thin film /4' improves the reflectance and
It has the function of strengthening the magnetic interaction between the magnetic thin film/3 and the magnetic thin film/3. Therefore, the magnetic thin film/3 is strongly magnetized by the magnetic field generated from the recording medium l. At this time, the size of the convergent spot of the light used for reading is unrelated to the reading resolution; If a material with a large Faraday effect and a high Curie temperature (for example, an iron thin film) is used, the intensity of the incident light during readout can be increased, so according to the present invention, a large signal-to-noise ratio can be obtained. be able to.

さらにまた、本発明では、光の入射および出射はヘッド
に対して垂直に行われるので、光学系の構成が単純化さ
れる。
Furthermore, in the present invention, since the light enters and exits perpendicularly to the head, the configuration of the optical system is simplified.

しかもまた、ヘッドの側面/、2の放物線の焦点をヘッ
ド先端部にもってくることができるため、記録媒体lか
ら生じる磁界によって強く磁化された磁性薄膜13の先
端部の信号を読み出すことができ、したがって確実な読
み出しが行なわれる。
Moreover, since the focus of the parabola on the side surface of the head can be brought to the tip of the head, it is possible to read the signal at the tip of the magnetic thin film 13, which is strongly magnetized by the magnetic field generated from the recording medium l. Therefore, reliable reading is performed.

さて、本発明磁気−光ヘッドでは磁性薄膜/Sの厚さが
Hoo Aの場合には、線密度10OKBPIまで読み
出し出力の低下はない。従来の読み出し方法では、主磁
極の磁性膜厚の整数倍の逆数にAる線密度で出力の大き
な減衰があるが、本発明磁気−光ヘッドではこのような
不都合を生じない。さらに、本発明による磁気−光ヘッ
ドは小型化(たとえば、直径/*mX長さコ朋以下)で
きるため、光ファイバへの接続が可能であり、また、軽
量であるからトラッキングあるいは高速アクセスに対し
て極めて有利である。
Now, in the magneto-optical head of the present invention, when the thickness of the magnetic thin film /S is Hoo A, there is no drop in readout output up to a linear density of 10 OK BPI. In the conventional readout method, there is a large attenuation of the output at a linear density A that is the reciprocal of the integer multiple of the magnetic film thickness of the main pole, but the magneto-optical head of the present invention does not suffer from this problem. Furthermore, the magneto-optical head according to the present invention can be miniaturized (for example, less than diameter/*m x length), so it can be connected to an optical fiber, and it is lightweight, making it suitable for tracking or high-speed access. This is extremely advantageous.

第夕図に示した実施例では、レンズ7によって反射光/
qをトラック23..2’lおよび、2左に対応して分
割し、それぞれに光検出器コ/、、、27および2gを
配置することにより複数トラックに対する読み出しが可
能であり、入射光/−ざの分割という複雑な光学系は必
要でない利点がある。
In the embodiment shown in FIG.
Track q23. .. It is possible to read out multiple tracks by dividing the tracks corresponding to 2'l and 2' left and arranging photodetectors 2'l and 27 and 2g, respectively, and it is possible to read out multiple tracks. This has the advantage that no optical system is required.

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

第1図は従来の磁気−光変換器の構成を示す断面図、第
2図は本発明磁気−光ヘッドの構成の一例を示す断面図
、第3図は本発明磁気−光へ゛ンドを垂直磁気記録媒体
に記録された情報の読み出しに用いる場合を示す断面図
、第9図は複数の記録トラックを読み出すようにした本
発明磁気−光へラードの他の例を示す構成図である。 l・・・記録媒体、 コ2.2′・・・プリズム、 3・・・磁性薄膜、 ダ・・・光源、 3・・・偏光子、 6.7・・・レンズ、 t・・・検光子、 ? 、 、u、 27. :tg・・・光検出器、10
・・・半透明鏡、 /か・・透明基板、 7.2・・・側面、 /3./!;・・・磁性薄膜、 /り・・・非磁性金MM膜、 /6・・・保護膜、 /7・・・焦点、 7g・・・直線偏光光、 /9・・・平行光束、 J、−/、ココ・・・ユニット1 、lJ、2<4.お・・・記録トラック。
FIG. 1 is a cross-sectional view showing the configuration of a conventional magneto-optical converter, FIG. 2 is a cross-sectional view showing an example of the configuration of the magnetic-optical head of the present invention, and FIG. 3 is a cross-sectional view showing an example of the configuration of the magnetic-optical head of the present invention. FIG. 9 is a cross-sectional view showing the case where the information is read out from a magnetic recording medium, and FIG. 9 is a configuration diagram showing another example of the magnetic-optical heald according to the present invention, which is adapted to read out a plurality of recording tracks. l...recording medium, 2.2'...prism, 3...magnetic thin film, da...light source, 3...polarizer, 6.7...lens, t...detection Photon, ? , ,u, 27. :tg...photodetector, 10
...semi-transparent mirror, /...transparent substrate, 7.2...side surface, /3. /! ;...magnetic thin film, /ri...non-magnetic gold MM film, /6...protective film, /7...focal point, 7g...linearly polarized light, /9...parallel light flux, J , -/, here... unit 1 , lJ, 2<4. Oh... recording track.

Claims (1)

【特許請求の範囲】 /)透明基板上に第1の磁性薄膜と、金属薄膜と、第一
の磁性薄膜とをこの順序で積層し、前記第一の磁性薄膜
を前記第1の磁性薄膜よりも厚くしたことを特徴とする
磁気−光ヘッド0 .2、特許請求の範囲第1項記載の磁気−光ヘッドにお
いて、前記第1の磁性薄膜の厚さをio。 rOA−MOAに設定し、前記第2の磁性薄膜機とする
磁気−光ヘッド。 3)特許請求の範囲第1項または第一項記載の磁気−光
ヘッドにおいて、前記透明基板を、その一方の側面が、
放物線へ状の断面を持つように形成したことを特徴とす
る磁気−光ヘッド0
[Scope of Claims] /) A first magnetic thin film, a metal thin film, and a first magnetic thin film are laminated in this order on a transparent substrate, and the first magnetic thin film is stacked on top of the first magnetic thin film. A magneto-optical head 0. 2. In the magneto-optical head according to claim 1, the thickness of the first magnetic thin film is io. The magneto-optical head is set to rOA-MOA and serves as the second magnetic thin film machine. 3) In the magneto-optical head according to claim 1 or 1, one side surface of the transparent substrate is
A magnetic-optical head 0 characterized in that it is formed to have a parabolic cross section.
JP13843782A 1982-08-11 1982-08-11 Magnetooptic head Granted JPS5930255A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13843782A JPS5930255A (en) 1982-08-11 1982-08-11 Magnetooptic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13843782A JPS5930255A (en) 1982-08-11 1982-08-11 Magnetooptic head

Publications (2)

Publication Number Publication Date
JPS5930255A true JPS5930255A (en) 1984-02-17
JPH0355894B2 JPH0355894B2 (en) 1991-08-26

Family

ID=15221957

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13843782A Granted JPS5930255A (en) 1982-08-11 1982-08-11 Magnetooptic head

Country Status (1)

Country Link
JP (1) JPS5930255A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
NL8403951A (en) * 1983-12-29 1985-07-16 Fuji Photo Film Co Ltd METHOD AND APPARATUS FOR REPRODUCING MAGNETIC INFORMATION.
US5488598A (en) * 1985-02-28 1996-01-30 Canon Kabushiki Kaisha Optical pickup using split beams impinging on different photodetector areas
US5689391A (en) * 1989-12-28 1997-11-18 Thomson Consumer Electronics Magneto-optic multitrack reading head having a plurality of reflective rays
KR100439374B1 (en) * 2001-09-13 2004-07-09 엘지전자 주식회사 Optical pickup
KR100508418B1 (en) * 1997-11-06 2005-11-24 후지제롯쿠스 가부시끼가이샤 Optical Heads and Optical Disc Devices
JP2008290246A (en) * 2008-08-25 2008-12-04 Yamato Protec Co Method and device for disassembling fire extinguisher

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5633781A (en) * 1979-08-28 1981-04-04 Omron Tateisi Electronics Co Line printer
JPS5727450A (en) * 1980-07-23 1982-02-13 Ricoh Co Ltd Magnetic recording medium

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5633781A (en) * 1979-08-28 1981-04-04 Omron Tateisi Electronics Co Line printer
JPS5727450A (en) * 1980-07-23 1982-02-13 Ricoh Co Ltd Magnetic recording medium

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
NL8403951A (en) * 1983-12-29 1985-07-16 Fuji Photo Film Co Ltd METHOD AND APPARATUS FOR REPRODUCING MAGNETIC INFORMATION.
US5488598A (en) * 1985-02-28 1996-01-30 Canon Kabushiki Kaisha Optical pickup using split beams impinging on different photodetector areas
US5689391A (en) * 1989-12-28 1997-11-18 Thomson Consumer Electronics Magneto-optic multitrack reading head having a plurality of reflective rays
KR100508418B1 (en) * 1997-11-06 2005-11-24 후지제롯쿠스 가부시끼가이샤 Optical Heads and Optical Disc Devices
KR100439374B1 (en) * 2001-09-13 2004-07-09 엘지전자 주식회사 Optical pickup
JP2008290246A (en) * 2008-08-25 2008-12-04 Yamato Protec Co Method and device for disassembling fire extinguisher

Also Published As

Publication number Publication date
JPH0355894B2 (en) 1991-08-26

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