JPS6360451B2 - - Google Patents

Info

Publication number
JPS6360451B2
JPS6360451B2 JP56086151A JP8615181A JPS6360451B2 JP S6360451 B2 JPS6360451 B2 JP S6360451B2 JP 56086151 A JP56086151 A JP 56086151A JP 8615181 A JP8615181 A JP 8615181A JP S6360451 B2 JPS6360451 B2 JP S6360451B2
Authority
JP
Japan
Prior art keywords
writing
polarization plane
magneto
reading
optical system
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP56086151A
Other languages
Japanese (ja)
Other versions
JPS57200959A (en
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 filed Critical
Priority to JP56086151A priority Critical patent/JPS57200959A/en
Publication of JPS57200959A publication Critical patent/JPS57200959A/en
Publication of JPS6360451B2 publication Critical patent/JPS6360451B2/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

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  • Optical Head (AREA)

Description

【発明の詳細な説明】 本発明は、いわゆる光磁気デイスクメモリーを
用いた情報記録再生装置に関し、特に、かかる情
報記録再生装置に用いる書込読取装置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an information recording/reproducing apparatus using a so-called magneto-optical disk memory, and particularly to a writing/reading apparatus used in such an information recording/reproducing apparatus.

いわゆる光磁気デイスクメモリーは、円盤状の
ガラス、プラスチツク等からなる基盤と、該基盤
上に設けられた通常数ミクロンの厚さの垂直磁化
膜とからなつている。垂直磁化膜は、アモルフア
ス合金等からなり膜面に対して垂直方向にのみ磁
化される特性を有するものである。
A so-called magneto-optical disk memory consists of a disk-shaped base made of glass, plastic, etc., and a perpendicularly magnetized film, usually several microns thick, provided on the base. The perpendicularly magnetized film is made of an amorphous alloy or the like and has the property of being magnetized only in the direction perpendicular to the film surface.

かかる光磁気デイスクメモリーに情報を記録す
るに当つては、まず光磁気デイスクメモリの垂直
磁化膜の磁化方向を予め一方向に揃えておき、次
いで、比較的弱いバイアス磁界を該方向とは反対
に垂直磁化膜に与えておくと共に情報信号によつ
てデイジタル的に変調されたレーザビームスポツ
トを該垂直磁化膜に照射して該垂直磁化膜の温度
をいわゆるキユリー温度に近づける。そうする
と、レーザビームスポツトの照射された部分は、
バイアス磁界方向に従つて該照射部分の磁化方向
が反転して論理“1”(又は“0”)が記録される
のである。記録された情報は室温下においてはバ
イアス磁界によつては変化することはないのであ
る。
To record information on such a magneto-optical disk memory, first, the magnetization direction of the perpendicular magnetization film of the magneto-optical disk memory is aligned in one direction, and then a relatively weak bias magnetic field is applied in the opposite direction. A laser beam spot applied to the perpendicularly magnetized film and digitally modulated by an information signal is irradiated onto the perpendicularly magnetized film to bring the temperature of the perpendicularly magnetized film close to the so-called Curie temperature. Then, the part irradiated by the laser beam spot will be
The magnetization direction of the irradiated portion is reversed according to the direction of the bias magnetic field, and a logic "1" (or "0") is recorded. The recorded information is not changed by the bias magnetic field at room temperature.

上記した垂直磁化膜用の合金材料としてはガド
リニウムコバルト(GdCo)、ガドリニウム・テ
ルビウム・鉄(GdTbFe)等のアモルフアス合金
がある。特に、GdTbFe合金は特性が秀れてお
り、例えば、1cm2当り500万ビツト程度密度で情
報がわずか数mWの光パワーによつて記録される
ということが判つている。
Examples of alloy materials for the perpendicular magnetization film mentioned above include amorphous alloys such as gadolinium cobalt (GdCo) and gadolinium-terbium-iron (GdTbFe). In particular, it has been found that GdTbFe alloys have excellent properties, such that information can be recorded at a density of about 5 million bits per cm 2 with an optical power of only a few mW.

こうして光磁気デイスクメモリーに記録された
情報を読み取るためには、垂直磁化膜に読取用ビ
ームスポツトを照射し、垂直磁化膜の磁化方向の
相違により反射ビームの偏波面の傾きに相違が生
ずるといういわゆるカー(Kerr)効果現象を利
用するのである。
In order to read the information recorded in the magneto-optical disk memory in this way, a reading beam spot is irradiated onto the perpendicularly magnetized film, and the difference in the direction of magnetization of the perpendicularly magnetized film causes a difference in the slope of the polarization plane of the reflected beam. It uses the Kerr effect phenomenon.

上記した如き光磁気デイスクメモリーを用いて
ビデオあるいはオーデイオ情報を記録再生するた
めの光磁気デイスク記録再生装置の開発が進めら
れている。かかる光磁気デイスク記録再生装置に
用いられる書込読取装置は比較的高価であり、か
つ記録光学系及び読取光学系の両方を備えている
ため大形となる恐れがある。
Development of a magneto-optical disk recording and reproducing apparatus for recording and reproducing video or audio information using the above-mentioned magneto-optical disk memory is progressing. The writing/reading device used in such a magneto-optical disk recording/reproducing device is relatively expensive and may be large because it includes both a recording optical system and a reading optical system.

そこで、本発明は、安価にしてかつ小形な書込
読取装置を提供することを目的とする。
Therefore, an object of the present invention is to provide a writing/reading device that is inexpensive and compact.

本発明による書込読取装置は、単一のレーザ光
源を切替手段を用いて書込光学系及び読取光学系
に兼用するようになされている。
The writing/reading device according to the present invention uses a single laser light source as both a writing optical system and a reading optical system using a switching means.

以下、本発明の実施例を添付図面によつて詳細
に説明する。
Embodiments of the present invention will be described in detail below with reference to the accompanying drawings.

第1図において、レーザ光源1から発したレー
ザビームは平面ミラー2、偏光子3、集束レンズ
4を経て光変調器5に入射する。光変調器5は、
例えば、音響光変調器(Acoustic Optical
Modulator)からなり、書き込まれるべき入力信
号に応じたドライバー6からの駆動信号によつて
入射ビームの強さを変調する。変調されたビーム
は移動自在なキヤリア部材7に担持されたλ/2
板8を経て偏光プリズム9に入射する。λ/2板
は、その結晶軸方向に対してαなる角度だけ偏波
したビームが入射した場合、透過ビームには角度
2αの偏波面を与えるという性質を持つている。
従つて、光源1からのビームの偏波面あるいは偏
光子3の偏光方向をλ/2板8の結晶軸に対して
適当に設定することにより偏光プリズム9の偏光
面9aに対する入射ビームがλ/2板8を経た場
合はS偏光となり、λ/2板8を経ない場合はP
偏光となるようにすることが出来る。今、λ/2
板8が光変調器5を経たビームの光路外にあると
すれば、偏光プリズム9への入射ビームはP偏光
であり、偏光面9aを透過して書込光学系10の
平面ミラー11に入射する。平面ミラー11によ
つて反射されたビームは偏光面12aを有する偏
光プリズム12を透過し、更に、λ/4板13、
平面ミラー14及び対物レンズ15を経て光磁気
デイスクメモリー16の垂直磁化膜面にスポツト
として照射される。光磁気デイスクメモリー16
はターンテーブル17上に載置されてクランパ1
8によつて固定されている。ターンテーブル19
は、スピンドル20を介して駆動モータ21によ
り所定速度にて回転せしめられる。駆動モータ2
1は矢印Aの方向に移動自在であつて書込ビーム
が渦巻状トラツクにて情報を書き込むようになさ
れている。光磁気デイスクメモリ16を挟んで対
物レンズ15の反対側にはバイアス磁界発生コイ
ル22が設けられている。バイアス磁界発生コイ
ル22は端子22a,22bを介して供給される
バイアス電流に応じた方向のバイアス磁界を発生
し、書込ビームと協働して光磁気デイスクメモリ
ー16に磁気的変化を与えて書込作用をなす。一
方、書込ビームの反射ビームは偏光プリズム12
aによつて反射されて光検知器23に入射し、光
検知器23の出力はサーボ信号として用いられ
る。
In FIG. 1, a laser beam emitted from a laser light source 1 passes through a plane mirror 2, a polarizer 3, and a focusing lens 4, and then enters an optical modulator 5. The optical modulator 5 is
For example, an acoustic optical modulator (Acoustic Optical Modulator)
modulator), which modulates the intensity of the incident beam by a drive signal from the driver 6 in accordance with the input signal to be written. The modulated beam is λ/2 carried on a movable carrier member 7.
The light passes through the plate 8 and enters the polarizing prism 9. When a beam polarized by an angle α with respect to the crystal axis direction is incident on a λ/2 plate, the transmitted beam has an angle
It has the property of giving a polarization plane of 2α.
Therefore, by appropriately setting the polarization plane of the beam from the light source 1 or the polarization direction of the polarizer 3 with respect to the crystal axis of the λ/2 plate 8, the incident beam on the polarization plane 9a of the polarizing prism 9 becomes λ/2. If it passes through plate 8, it becomes S polarized light, and if it does not pass through λ/2 plate 8, it becomes P polarized light.
It can be made to be polarized light. Now, λ/2
If the plate 8 is located outside the optical path of the beam that has passed through the optical modulator 5, the beam incident on the polarizing prism 9 is P-polarized light, passes through the polarization plane 9a, and enters the plane mirror 11 of the writing optical system 10. do. The beam reflected by the plane mirror 11 passes through a polarizing prism 12 having a polarizing plane 12a, and further passes through a λ/4 plate 13,
The light is irradiated as a spot onto the perpendicularly magnetized film surface of the magneto-optical disk memory 16 through the plane mirror 14 and the objective lens 15. Magneto-optical disk memory 16
is placed on the turntable 17 and the clamper 1
8. turntable 19
is rotated at a predetermined speed by a drive motor 21 via a spindle 20. Drive motor 2
1 is movable in the direction of arrow A, and the writing beam writes information in a spiral track. A bias magnetic field generating coil 22 is provided on the opposite side of the objective lens 15 with the magneto-optical disk memory 16 in between. The bias magnetic field generating coil 22 generates a bias magnetic field in a direction corresponding to the bias current supplied through the terminals 22a and 22b, and cooperates with the writing beam to apply a magnetic change to the magneto-optical disk memory 16 to perform writing. It has an embedding effect. On the other hand, the reflected beam of the writing beam is reflected by the polarizing prism 12.
a and enters the photodetector 23, and the output of the photodetector 23 is used as a servo signal.

次に、λ/2板8が光変調器5を透過したビー
ムの光路内にある場合、λ/2板8を透過したビ
ームはS偏光となり偏光プリズム9の偏光面9a
にて反射されて別のλ/2板24を経て所定角度
だけ偏波面が補正された後平面ミラー25,26
を経てハーフミラー27に入射する。ハーフミラ
ー27を透過したビームは平面ミラー28、対物
レンズ29を経て読取ビームとして光磁気デイス
ク16の垂直磁化膜面に投射される。投射された
読取ビームは垂直磁化膜面にて反射される際、垂
直磁化膜の磁化方向によつて偏波面の回転が生じ
る(カー効果)。この反射ビームは再び対物レン
ズ29、平面ミラー28を経てハーフミラー27
に入射し、反射ビームの半分が別のハーフミラー
30に入射する。ハーフミラー30によつて2分
割されたビームは検光子31,32を経て光検知
器33,34に入射する。検光子31,32の透
過特性は入射ビームの偏光角度すなわち基準面に
対する偏波面の傾きθに対して第2図の実線a,
bの如くなつており、ハーフミラー27,30を
経た戻りビームの偏波面の傾きに応じた強さの信
号が読取信号として差動アンプ34から出力され
ることになる。
Next, when the λ/2 plate 8 is in the optical path of the beam that has passed through the optical modulator 5, the beam that has passed through the λ/2 plate 8 becomes S-polarized light, and the polarization plane 9a of the polarizing prism 9
After being reflected by another λ/2 plate 24 and having its polarization plane corrected by a predetermined angle, the plane mirrors 25 and 26
The light then enters the half mirror 27. The beam transmitted through the half mirror 27 passes through a plane mirror 28 and an objective lens 29, and is projected onto the perpendicularly magnetized film surface of the magneto-optical disk 16 as a reading beam. When the projected reading beam is reflected by the surface of the perpendicularly magnetized film, the plane of polarization rotates depending on the magnetization direction of the perpendicularly magnetized film (Kerr effect). This reflected beam passes through the objective lens 29 and the plane mirror 28 again, and then passes through the half mirror 27.
half of the reflected beam is incident on another half mirror 30. The beam split into two by the half mirror 30 passes through analyzers 31 and 32 and enters photodetectors 33 and 34. The transmission characteristics of the analyzers 31 and 32 are determined by the solid line a in FIG.
b, and a signal with an intensity corresponding to the inclination of the plane of polarization of the returned beam after passing through the half mirrors 27 and 30 is outputted from the differential amplifier 34 as a read signal.

差動アンプ35を用いて偏波面の傾きの変位を
検出するのは、レーザ光源からのレーザビームに
元来含まれるノイズ成分を相殺せんがためであ
る。
The reason why the differential amplifier 35 is used to detect the displacement of the tilt of the plane of polarization is to cancel the noise component originally contained in the laser beam from the laser light source.

なお、読取光学系においても図示しないサーボ
光学系が設けられて読取ビームのフオーカス及び
トラツキングサーボが行なわれることは言うまで
もなく、種々のサーボ方式が既に公知となつてい
るのでここでは詳述しない。
It goes without saying that the reading optical system is also provided with a servo optical system (not shown) to perform focusing and tracking servo of the reading beam, and since various servo systems are already known, they will not be described in detail here.

上記した本発明による光磁気デイスクメモリー
を用いた書込読取装置においては、単一のレーザ
光源からのレーザビームを簡単な切替手段によつ
て書込光学系と読取光学系とに兼用しており、装
置全体のコストダウン、小形化が容易になつてい
る。
In the above-mentioned writing/reading device using the magneto-optical disk memory according to the present invention, the laser beam from a single laser light source is used as both the writing optical system and the reading optical system by a simple switching means. It is becoming easier to reduce the cost and size of the entire device.

また、上記実施例においては、偏波面回転手段
としてλ/2板を使用しているが、印加電界によ
つて偏光特性の変化するいわゆるフアラデー回転
素子を用いることも出来るのである。
Further, in the above embodiment, a λ/2 plate is used as the polarization plane rotation means, but a so-called Faraday rotation element whose polarization characteristics change depending on the applied electric field can also be used.

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

第1図は、本発明の実施例を示す図、第2図は
第1図に用いられた検光子の出力特性を示すグラ
フである。 主要部分の符号の説明、1……レーザ光源、3
……偏光子、5……光変調器、6……ドライバ、
8,24……λ/2板、9……偏光プリズム、1
0……書込光学系、12……偏光プリズム、16
……光磁気デイスクメモリー、19……ターンテ
ーブル、21……駆動モータ、22……バイアス
磁界発生コイル、23,34……光検知器、2
7,30……ハーフミラー、31,32……検光
子、35……差動アンプ。
FIG. 1 is a diagram showing an embodiment of the present invention, and FIG. 2 is a graph showing the output characteristics of the analyzer used in FIG. 1. Explanation of symbols of main parts, 1... Laser light source, 3
...Polarizer, 5...Optical modulator, 6...Driver,
8, 24...λ/2 plate, 9...Polarizing prism, 1
0...Writing optical system, 12...Polarizing prism, 16
... magneto-optical disk memory, 19 ... turntable, 21 ... drive motor, 22 ... bias magnetic field generating coil, 23, 34 ... photodetector, 2
7, 30... Half mirror, 31, 32... Analyzer, 35... Differential amplifier.

Claims (1)

【特許請求の範囲】 1 垂直磁化特性を有する光磁気記録デイスクを
回転自在に担持するターンテーブル手段と、前記
光磁気記録デイスクに向けて書込ビームを発する
書込光学系と、前記光磁気記録デイスクに読取ビ
ームを照射してその反射ビームの偏波面の変位を
検知して情報を読み取る読取光学系と、単一のレ
ーザ光源と、前記レーザ光源からの偏光ビームを
切替指令信号に応じて前記書込光学系及び読取光
学系に択一的に供給する切替手段とからなり、前
記切替手段が前記偏光ビームの偏波面を前記切替
指令信号に応じて所定角度だけ回転せしめる偏波
面回転手段と、前記偏波面回転手段を通過した偏
光ビームが入射する偏光面を有する偏光プリズム
とからなることを特徴とする書込読取装置。 2 前記偏波面回転手段は、λ/2板と、前記
λ/2板を前記切替信号に応じて前記偏ビームの
光路に選択的に配置せしめる駆動手段とからなる
ことを特徴とする特許請求の範囲第1項記載の書
込読取装置。 3 前記偏波面回転手段は、フアラデー回転素子
と、前記切替信号に応じて前記フアラデー回転素
子の偏光特性を変化せしめる制御手段とからなる
ことを特徴とする特許請求の範囲第1項記載の書
込読取装置。
[Scope of Claims] 1. A turntable means rotatably supporting a magneto-optical recording disk having perpendicular magnetization characteristics, a writing optical system that emits a writing beam toward the magneto-optical recording disk, and a magneto-optical recording disk. a reading optical system that irradiates a reading beam onto the disk and detects the displacement of the polarization plane of the reflected beam to read information; a single laser light source; a polarization plane rotation means, comprising a switching means for selectively supplying the polarized light beam to the writing optical system and the reading optical system, the switching means rotating the polarization plane of the polarized beam by a predetermined angle in accordance with the switching command signal; A writing/reading device comprising: a polarizing prism having a polarizing plane onto which the polarized beam that has passed through the polarization plane rotating means is incident. 2. The polarization plane rotating means comprises a λ/2 plate and a driving means for selectively arranging the λ/2 plate on the optical path of the polarized beam according to the switching signal. The writing/reading device according to scope 1. 3. The writing according to claim 1, wherein the polarization plane rotation means includes a Faraday rotation element and a control means for changing the polarization characteristics of the Faraday rotation element according to the switching signal. reading device.
JP56086151A 1981-06-04 1981-06-04 Write and read device of optical magnetic recording system Granted JPS57200959A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56086151A JPS57200959A (en) 1981-06-04 1981-06-04 Write and read device of optical magnetic recording system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56086151A JPS57200959A (en) 1981-06-04 1981-06-04 Write and read device of optical magnetic recording system

Publications (2)

Publication Number Publication Date
JPS57200959A JPS57200959A (en) 1982-12-09
JPS6360451B2 true JPS6360451B2 (en) 1988-11-24

Family

ID=13878730

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56086151A Granted JPS57200959A (en) 1981-06-04 1981-06-04 Write and read device of optical magnetic recording system

Country Status (1)

Country Link
JP (1) JPS57200959A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0785311B2 (en) * 1984-05-15 1995-09-13 セイコーエプソン株式会社 Multi optical head
JP3400939B2 (en) 1998-02-03 2003-04-28 富士通株式会社 Information reading / writing device for optical disk

Also Published As

Publication number Publication date
JPS57200959A (en) 1982-12-09

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