JPS58169358A - Optical reproducing device - Google Patents

Optical reproducing device

Info

Publication number
JPS58169358A
JPS58169358A JP5209882A JP5209882A JPS58169358A JP S58169358 A JPS58169358 A JP S58169358A JP 5209882 A JP5209882 A JP 5209882A JP 5209882 A JP5209882 A JP 5209882A JP S58169358 A JPS58169358 A JP S58169358A
Authority
JP
Japan
Prior art keywords
medium
light
optical
information
passes
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
JP5209882A
Other languages
Japanese (ja)
Inventor
Masaharu Moritsugu
森次 政春
Yasuyuki Ozawa
靖之 小沢
Toshitaka Iwamoto
岩本 敏孝
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP5209882A priority Critical patent/JPS58169358A/en
Publication of JPS58169358A publication Critical patent/JPS58169358A/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
    • G11B11/10532Heads

Abstract

PURPOSE:To obtain detection sensitivity having high accuracy, by detecting a state variation of light which repeats reflection by a photomagnetic disk plural times, and reading the information. CONSTITUTION:A reflecting device R having a total reflector 8 is provided on the upper part of an objective lens 6. Laser light passes through a hole 10 of the reflecting device R, is condensed to one point 9 of a magnetic recording medium 1, is reflected, passes through the lens 6, passes through a reverse optical path again by the total reflector 8, and is returned from the hole 10, by which information is read. In this case, the laser light is influenced by a magnetic field 2 times from the medium 1, therefore, by a magnetooptic Kerr effect, the polarizing face is rotated on a comparatively large scale. Therefore, detection sensitivity having high accuracy can be obtained, and an S/N ratio is improved.

Description

【発明の詳細な説明】 (1)発明の技術分野 本発明は、媒体上の情報を光学的に再生する装置に係り
、特に磁気光学カー効果すなわち磁化媒体による偏光面
の回転によって生じる偏光状態の変化を検出するること
により情報の読取りを行う情報再生方式に関する。とこ
ろで磁気光学カー効−とは周知の如く磁場内の物質ある
いは磁性体によって光が反射されたる際偏光面が回転す
る現象を言う。
DETAILED DESCRIPTION OF THE INVENTION (1) Technical Field of the Invention The present invention relates to a device for optically reproducing information on a medium, and particularly relates to a device for optically reproducing information on a medium, and in particular, it relates to a device for optically reproducing information on a medium, and in particular, it relates to a device for optically reproducing information on a medium, and in particular, it relates to a device for optically reproducing information on a medium, and in particular, it relates to a device for optically reproducing information on a medium. The present invention relates to an information reproducing method that reads information by detecting changes. By the way, the magneto-optical Kerr effect, as is well known, refers to a phenomenon in which the plane of polarization rotates when light is reflected by a substance or magnetic material in a magnetic field.

(2)技術の背景 近年における光エレクトロニクスの発達は著しく、特に
レーザ等を用いた光ディスクあるいは光磁気ディスク等
については、最近特に注目を集めている。そして、実用
化が既に始まっている光デイスク装置において、再生装
置も種々提案されてきており、従って高性能な装置の要
望も高まっている。
(2) Background of the Technology The development of optoelectronics has been remarkable in recent years, and in particular, optical disks or magneto-optical disks using lasers or the like have recently been attracting particular attention. Various playback devices have been proposed for optical disk devices, which have already been put into practical use, and there is therefore an increasing demand for high-performance devices.

(3)従来技術と問題点 −磁気光学カー効果による情報再生方式において、従来
の再生方式では、光と磁気との相互作用のために光の偏
光面i転角は例えばガドミウムテルビウム鉄(GdTb
Fe)の場合的0.5°と極めて僅かなために同時に発
生する雑音と相俟って検出感度が比較的低いと言う欠点
を有している。
(3) Prior art and problems - In the information reproducing method using the magneto-optical Kerr effect, in the conventional reproducing method, due to the interaction between light and magnetism, the polarization plane i inversion angle of light is
Since the angle is extremely small (0.5° in the case of Fe), it has the disadvantage that the detection sensitivity is relatively low due to the noise generated at the same time.

(4)発明の目的 本発明の目的は、光磁気ディスクにおける情報再生に際
して磁気媒体の同一箇所へ反射鏡等により複数回に亘り
光ビームを入射させることにより、磁気媒体への入射前
の光の偏光面と複数回に亘る磁気媒体での反射光の偏光
面とに比較的大きな偏光状態の変化を発生させて精度の
高い検出感度を得ることのできる光学式再生装置を提供
することにある。
(4) Purpose of the Invention The purpose of the present invention is to make the light beam incident on the same spot on the magnetic medium multiple times using a reflector, etc. when reproducing information on a magneto-optical disk. An object of the present invention is to provide an optical reproducing device that can obtain highly accurate detection sensitivity by generating a relatively large change in the polarization state in the polarization plane and the polarization plane of light reflected by a magnetic medium multiple times.

(5)発明の構成 本発明の特徴は、光学的に読み出し可能に情報の記録を
施された媒体において、前記媒体から情報を光学的に再
生する光学式再生方式において、前記媒体での反射を複
数回繰り返した光の状!l!変化を検出することにより
、前記媒体からの情報を読み取る光学式再生装置を提供
することによって達成される。
(5) Structure of the Invention A feature of the present invention is that in an optical reproduction method for optically reproducing information from a medium on which information is recorded in an optically readable manner, reflection on the medium is prevented. The shape of light repeated multiple times! l! This is achieved by providing an optical playback device that reads information from the medium by detecting changes.

(6)発明の実施例 最初に磁気光学カー効果について第1図によりて説明す
る。
(6) Embodiments of the Invention First, the magneto-optical Kerr effect will be explained with reference to FIG.

第1図は光と磁気との相互作用である磁気光学カー効果
により、入射光ビームの偏光状態が光磁気記録媒体によ
り反射されるときに変化を受けて偏光面に回転が発生す
ることを示す説明図である。
Figure 1 shows that due to the magneto-optic Kerr effect, which is an interaction between light and magnetism, the polarization state of an incident light beam changes when reflected by a magneto-optical recording medium, causing rotation in the plane of polarization. It is an explanatory diagram.

すなわち同図(a)の如く入射光ビームと光磁気記録媒
体1におけるビーム照射部との磁界の向きが同、、+1
1・ −の場合には光磁気記録媒体1にて反射した後の光の偏
光面が時針回りにθに0回転する。(同図中(1)及び
(2))また同図中)の如く入射光ビームと光磁気記録
媒体1來おけるビーム照射部の磁界の向きが逆方向の場
合には光磁気記録媒体1にて反射した光の偏光面は反時
計回りに同じくθに°回転する。(同図(3)及び(4
))従ってこのレーザ光の光磁気記録媒体1への入射光
と反射光における偏光状態の変化によって生ずる光量の
差を検出することにより媒体上の情報を再生することが
可能である。しかしながら、この偏光状態の変化は非常
に小さいためSN比が悪いという問題があった。
In other words, as shown in FIG. 3(a), the direction of the magnetic field between the incident light beam and the beam irradiation part of the magneto-optical recording medium 1 is the same, +1
In the case of 1.-, the polarization plane of the light after being reflected by the magneto-optical recording medium 1 rotates 0 around the hour hand in θ. ((1) and (2) in the same figure) When the directions of the incident light beam and the magnetic field of the beam irradiation part on the magneto-optical recording medium 1 are opposite, the magneto-optical recording medium 1 The plane of polarization of the reflected light is also rotated counterclockwise by θ. ((3) and (4)
)) Therefore, it is possible to reproduce information on the medium by detecting the difference in the amount of light caused by the change in the polarization state between the incident light of the laser light on the magneto-optical recording medium 1 and the reflected light. However, since this change in polarization state is very small, there is a problem in that the signal-to-noise ratio is poor.

次に本発明の一実施例を第2WJと第3図にて説明する
Next, one embodiment of the present invention will be explained with reference to the second WJ and FIG. 3.

第2図は、本発明の光磁気媒体における再生方法を示す
光路図である。光の進む経路としては、例えばレーザダ
イオード(LD)2より発生した光は集束用レンズ(カ
ップリングレンズ)3で集められ、さらに平行光線束と
なり偏光子4を通過する。ところで、偏光子とは例えば
グラントンプソンプリズム等で良く知られている如く、
特定の偏光面、偏光状態を持つ光だけを取り出す装置で
ある。
FIG. 2 is an optical path diagram showing the reproduction method for the magneto-optical medium of the present invention. As for the path along which light travels, for example, light generated from a laser diode (LD) 2 is collected by a focusing lens (coupling lens) 3, and further becomes a parallel beam of light and passes through a polarizer 4. By the way, a polarizer is, for example, as well known as a Glan-Thompson prism.
This is a device that extracts only light with a specific polarization plane or state.

また、偏光面とは光振動面といい、この偏光面が一平面
に限られているとき直線偏光と呼ばれる。
The plane of polarization is called the plane of optical vibration, and when this plane of polarization is limited to one plane, it is called linearly polarized light.

偏光子4を通過して直線偏光となった光はレーザ光はハ
ーフミラ−5にて半分は反射されて対物レンズ6に入射
し、さらに光磁気媒体1で反射されるため偏光面に例え
ばθに’(θK”<<1″″)の回転が発生し、さらに
光磁気媒体!で反射された光は反射#8へ入射され再び
反射されて光磁気媒体1に再入射され、その反射光は再
びハーフミラ−5を通り、そのうち半分が透過されすな
わち元の光量のAが検光子4゛に入射することとなる。
The laser light that passes through the polarizer 4 and becomes linearly polarized light is half reflected by the half mirror 5 and enters the objective lens 6, and is further reflected by the magneto-optical medium 1, so that the polarization plane is changed to, for example, θ. '(θK''<<1'''') rotation occurs, and the light reflected by the magneto-optical medium ! enters reflection #8, is reflected again, and re-enters the magneto-optical medium 1, and the reflected light is The light passes through the half mirror 5 again, and half of it is transmitted, that is, the original amount of light A enters the analyzer 4'.

その後検光子4′で規定された偏光成分の光のみがレン
ズ3′で集光される。これを以て情報の再生を図ろうと
するのが本発明の光学式再生装置である。
Thereafter, only the light having the polarized component determined by the analyzer 4' is focused by the lens 3'. The optical reproducing apparatus of the present invention attempts to reproduce information using this method.

ここで、高検出感度を得るための本発明光学式再生装置
の対物レンズ6と磁気媒体1とに関係する一連の光学経
路図を第3図に示すと共に説明する。同図中(a)は光
学経路を示すための正面図、伽)は平面図を各々示す。
Here, a series of optical path diagrams related to the objective lens 6 and the magnetic medium 1 of the optical reproducing apparatus of the present invention for obtaining high detection sensitivity are shown in FIG. 3 and will be explained. In the figure, (a) is a front view showing the optical path, and (a) is a plan view.

対物レンズ6の上部の反射袋WRに設けられた孔lOを
通過して、対物レンズ6に入射したレーザ光は磁気記録
媒体1の一点9に集光して対物レンズ6を通過して反射
装置Rに設けられた全反射鏡8にて再び逆の光路を通っ
て孔10よりレーザ光は戻るが、上記の経路の中でレー
ザ光は磁気記録媒体1から2度に亘って磁界の影響を受
けるため一度につきθに°都合2θに′°反時計方向に
偏光面が回転することになる。従って偏光面の変化の検
出感度が高くなりSN比が向上する。
The laser beam that passes through the hole lO provided in the reflective bag WR at the upper part of the objective lens 6 and enters the objective lens 6 is focused on a point 9 on the magnetic recording medium 1, passes through the objective lens 6, and then passes through the reflection device. The laser beam returns from the hole 10 again through the opposite optical path at the total reflection mirror 8 provided at R, but in the above path, the laser beam is twice influenced by the magnetic field from the magnetic recording medium 1. As a result, the plane of polarization rotates counterclockwise by 2θ for every θ. Therefore, the detection sensitivity for changes in the plane of polarization is increased, and the S/N ratio is improved.

第4図は本発明の反射鏡を用いた他の実施例であり、第
3図と同一部分には同一番号を付した。
FIG. 4 shows another embodiment using the reflecting mirror of the present invention, and the same parts as in FIG. 3 are given the same numbers.

上述した如く本発明に係る光学式再生装置は、対物レン
ズ上方に全反射鏡−個を設けて実施したが、同図の如く
全反射鏡8を、光軸に関して角度を適切に設けて3箇所
に配設して都合4度反射させることにより偏光面をさら
に大きく回転することが可能であり検出感度を一層高め
ることが可能になることは勿論である。また、反射装置
Rを反射鏡で構成し、この反射鏡に孔10を設けてもよ
い。
As described above, the optical reproducing apparatus according to the present invention was implemented by installing a total reflection mirror above the objective lens, but as shown in the figure, total reflection mirror 8 was installed at three locations at appropriate angles with respect to the optical axis. Of course, by arranging the light beam and reflecting it four times in total, the plane of polarization can be rotated even more, and the detection sensitivity can be further increased. Further, the reflecting device R may be constituted by a reflecting mirror, and the hole 10 may be provided in this reflecting mirror.

また、この方式は光磁気記録媒体の再生用だけを対象と
するものではなく、ビット形式もしくは反射率の変化に
より記録された媒体に対しても情報の再生時の感度の向
上を図ることができることは言うまでもない。
In addition, this method is not only intended for reproduction of magneto-optical recording media, but can also improve the sensitivity when reproducing information from media recorded in bit format or with changes in reflectance. Needless to say.

(7)発明の効果 以上本発明によれば、媒体面での反射回数を増やすこと
により検出感度を増加することができSN比が向上する
(7) Effects of the Invention According to the present invention, detection sensitivity can be increased by increasing the number of reflections on the medium surface, and the S/N ratio can be improved.

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

第1図は本発明において用いられている磁気光学カー効
果、・第2図は光磁気媒体による再生方法を示す光路図
、第3図(a)、 (b)は各々光磁気媒体附近におけ
る光経路を示′す本発明装置の正面図、平面図、第4図
は4回反射による本発明の他の実施例を説明する図であ
る。 1・・・磁気記録媒体、 4・・・偏光子、4゛・・・
検出子、 6・・・対物レンズ、 8・・・全反射鏡、
 10・・・孔、 R・・・反射装置。 (1)C2ノ 第 C3ノf4ノ 1 図 第2図 第 4 図
Figure 1 shows the magneto-optical Kerr effect used in the present invention, Figure 2 is an optical path diagram showing the reproduction method using a magneto-optical medium, and Figures 3 (a) and (b) show the light in the vicinity of the magneto-optical medium. A front view and a plan view of the device of the present invention showing the path, and FIG. 4 are diagrams for explaining another embodiment of the present invention using four reflections. 1... Magnetic recording medium, 4... Polarizer, 4゛...
Detector, 6... Objective lens, 8... Total reflection mirror,
10...hole, R...reflector. (1) C2 No. C3 No. F4 No. 1 Figure 2 Figure 4

Claims (1)

【特許請求の範囲】 光学的に読み出し可能に情報の記録を施された媒体から
情報を光学的に再生 する光学式再生方式において、前記媒体での反射を複数
回繰り返した光の状態表化を検出することにより、前記
媒体からの情報を読み取ることを特徴とする光学式再生
装置。
[Claims] In an optical reproduction method that optically reproduces information from a medium on which information is recorded in an optically readable manner, a state table of light that is reflected multiple times on the medium is created. An optical playback device characterized in that information is read from the medium by detection.
JP5209882A 1982-03-30 1982-03-30 Optical reproducing device Pending JPS58169358A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5209882A JPS58169358A (en) 1982-03-30 1982-03-30 Optical reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5209882A JPS58169358A (en) 1982-03-30 1982-03-30 Optical reproducing device

Publications (1)

Publication Number Publication Date
JPS58169358A true JPS58169358A (en) 1983-10-05

Family

ID=12905364

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5209882A Pending JPS58169358A (en) 1982-03-30 1982-03-30 Optical reproducing device

Country Status (1)

Country Link
JP (1) JPS58169358A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5241520A (en) * 1990-12-28 1993-08-31 Sony Corporation System and method of reproducing signals recorded on a magneto-optic recording medium

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5241520A (en) * 1990-12-28 1993-08-31 Sony Corporation System and method of reproducing signals recorded on a magneto-optic recording medium

Similar Documents

Publication Publication Date Title
US4451863A (en) Information reproducing apparatus based on opto-magnetic effect
JPH06101156B2 (en) Magneto-optical head
US4660187A (en) Light signal reading method and apparatus using interference between two light beams of different frequency and polarization
KR920007294B1 (en) Optical head for magneto-optical memory
JPS5982646A (en) Optomagnetic storage device
US5119352A (en) Magneto optic data storage read out apparatus and method
JPH0522305B2 (en)
JPH08306091A (en) Optical head
JPS58169358A (en) Optical reproducing device
JPH0355894B2 (en)
JPS62177738A (en) Transfer type photomagnetic head
JPH0327978B2 (en)
JPH03268252A (en) Optical information recording and reproducing system
JP2574915B2 (en) Optical device for reproducing magneto-optical recording media
KR100207645B1 (en) Optical beam control method of optical device and optical device for optical head therefor
KR100357094B1 (en) apparatus and method for magneto-optical writing/reading using near field
JP2859519B2 (en) Optical information reproducing device
JPS60157745A (en) Photomagnetic recorder
JPH053666B2 (en)
JPH0746440B2 (en) Optical recording / reproducing device
JPS6318550A (en) Optical head for magneto-optical disk
JPS613343A (en) Optical reproducing head of magnetooptic system
JPH04181537A (en) Optical information reproducer
JPS60173747A (en) Optical head of magnetooptic memory
JPS63193334A (en) Magneto-optical head