JPH0542741B2 - - Google Patents

Info

Publication number
JPH0542741B2
JPH0542741B2 JP59100926A JP10092684A JPH0542741B2 JP H0542741 B2 JPH0542741 B2 JP H0542741B2 JP 59100926 A JP59100926 A JP 59100926A JP 10092684 A JP10092684 A JP 10092684A JP H0542741 B2 JPH0542741 B2 JP H0542741B2
Authority
JP
Japan
Prior art keywords
light
signal
magneto
optical memory
linearly polarized
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 - Lifetime
Application number
JP59100926A
Other languages
Japanese (ja)
Other versions
JPS60243845A (en
Inventor
Yukinori Okazaki
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP59100926A priority Critical patent/JPS60243845A/en
Publication of JPS60243845A publication Critical patent/JPS60243845A/en
Publication of JPH0542741B2 publication Critical patent/JPH0542741B2/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

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、光磁気効果を用いて情報を読み出す
光磁気メモリの再生装置に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a magneto-optical memory reproducing device that reads information using the magneto-optical effect.

従来例の構成とその問題点 近年、レーザ光を用いて情報を高密度に記録
し、再生する光メモリ装置が開発されている。特
にその中でも、膜面に垂直方向に磁化の容易軸を
有するMnBi,アモルフアスのTbDyFe,
TbCdFe等の磁性薄膜をメモリ媒体に用いた光磁
気メモリは、情報の消去がたやすく行なえる高密
度記録担体として注目を集めている。光磁気メモ
リへの情報の記録方法を第1図を用いて説明す
る。磁性薄膜1は情報を記録する以前には第1図
イに示すように磁化2が膜面に垂直方向で、媒体
全体にわたつて一方向を向くように磁化されてい
る。この膜1上に第1図ロに示すようにレーザー
光3を照射して、膜の一部を加熱し局部的にキユ
リー点付近まで温度を上昇させると共に、この部
分を含む領域に外部磁界4を付加して、記録前の
磁化方向と反対の方向の磁界をかけると、レーザ
ー光3が照射された部分の磁化の方向が反射し、
情報が記録される。従つて情報は磁性薄膜1上
に、磁化の方向の違いとして蓄積される。一方、
蓄積された情報の読み出しも、やはりレーザー光
を磁性薄膜上に照射し、磁化の方向の違いを光学
的に検出して行なわれる。このレーザー光を用い
た検出方法は、カー効果、或いはフアラデー効果
を利用したもので、磁性体に照射した光の偏光方
向が、磁化の方向によつて変化する現象を用いて
いる。磁性薄膜に蓄積された情報によつて偏光方
向が変化を受けて磁性薄膜より戻つてくる再生光
には、膜からの反射光と透過光が考えられるが、
反射光、透過光共同じ方向の磁化に対しては、偏
光方向の変化は同じ向きに起こる。情報の検出方
法を透過光を例にとり、第2図を用いて説明す
る。第2図イに示すように情報が記録された磁性
薄膜5に、矢印6の方向に偏光したレーザー光7
を照射すると、透過光8は照射前の偏光方向6に
対して、+θk度回転して矢印9の方向の偏光とな
る。一方、第2図ロに示すように磁性薄膜上で、
磁化の方向が逆の方向を向いた部分に、同じく矢
印6の方向に偏光したレーザー光7を照射する
と、透過光10は偏光方向6に対して、−θk度回
転した矢印11の方向の偏光となる。従つて検光
子を用いて、これら偏光方向の異なつた2つの光
を区別すると、偏光方向の違いが検光子を通つた
光の強度の違いとなり、光電変換を行なう事によ
り、情報が再生されるわけである。
2. Description of the Related Art Structures of Conventional Examples and Their Problems In recent years, optical memory devices have been developed that use laser light to record and reproduce information at high density. Among them, MnBi, which has an easy axis of magnetization perpendicular to the film surface, amorphous TbDyFe,
Magneto-optical memories that use magnetic thin films such as TbCdFe as memory media are attracting attention as high-density recording carriers that allow information to be easily erased. A method for recording information in a magneto-optical memory will be explained using FIG. 1. Before recording information, the magnetic thin film 1 is magnetized so that the magnetization 2 is perpendicular to the film surface and oriented in one direction over the entire medium, as shown in FIG. 1A. This film 1 is irradiated with a laser beam 3 as shown in FIG. When a magnetic field is applied in the opposite direction to the magnetization direction before recording, the direction of magnetization of the part irradiated with the laser beam 3 is reflected,
Information is recorded. Therefore, information is stored on the magnetic thin film 1 as a difference in the direction of magnetization. on the other hand,
The stored information is also read out by irradiating the magnetic thin film with laser light and optically detecting the difference in the direction of magnetization. This detection method using laser light utilizes the Kerr effect or the Faraday effect, and uses a phenomenon in which the polarization direction of light irradiated onto a magnetic material changes depending on the direction of magnetization. The reproduction light that returns from the magnetic thin film with its polarization direction changed by the information stored in the magnetic thin film can include reflected light and transmitted light from the film.
If both reflected light and transmitted light are magnetized in the same direction, the polarization direction changes in the same direction. A method of detecting information will be described using transmitted light as an example, with reference to FIG. As shown in FIG.
When irradiated with , the transmitted light 8 is rotated by +θ k degrees with respect to the polarization direction 6 before irradiation, and becomes polarized light in the direction of an arrow 9. On the other hand, as shown in Figure 2B, on the magnetic thin film,
When laser light 7, which is also polarized in the direction of arrow 6, is irradiated onto a part whose magnetization direction is opposite, the transmitted light 10 is rotated by −θ k degrees with respect to the polarization direction 6, in the direction of arrow 11. It becomes polarized light. Therefore, if you use an analyzer to distinguish these two lights with different polarization directions, the difference in polarization direction will result in a difference in the intensity of the light that passes through the analyzer, and information will be reproduced by performing photoelectric conversion. That's why.

上に述べた再生方法を用いた光磁気メモリより
の情報の再生の従来例を第3図を用いて説明す
る。レーザー光源12よりの光はコリメート・レ
ンズ13によつて平行光束となり、グラン・トム
ソン・プリズム等の偏光子14によつて直線偏光
にされ、ハーフミラー15を通り、集光レンズ1
6によつて光磁気メモリ媒体17上に集光され
る。光磁気メモリ媒体17によつて偏光方向が回
転した反射光は、再びハーフミラー15を通り、
更にハーフミラー18で2分割され、各々検光子
19A,19Bを通つて光検出器20A,20B
に受光される。検光子19A,19Bはやはりグ
ラン・トムソン・プリズム等で構成され、各々偏
波面が磁気メモリ媒体17への入射光の偏光方向
に対し各々45゜をなし、かつ互いに直交する位置
に設定されている。光検出器20A,20Bの出
力は、差動増幅器21によつて差動出力が求めら
れ、磁化の方向変化による偏光方向の回転成分の
みが検出される構成になつている。
A conventional example of reproducing information from a magneto-optical memory using the above-described reproducing method will be described with reference to FIG. The light from the laser light source 12 is turned into a parallel beam by a collimating lens 13, linearly polarized by a polarizer 14 such as a Glan-Thompson prism, passed through a half mirror 15, and then sent to a condenser lens 1.
6, the light is focused onto a magneto-optical memory medium 17. The reflected light whose polarization direction has been rotated by the magneto-optical memory medium 17 passes through the half mirror 15 again.
It is further divided into two parts by a half mirror 18, and passes through analyzers 19A and 19B respectively to photodetectors 20A and 20B.
The light is received by the Analyzers 19A and 19B are also composed of Glan-Thompson prisms, etc., and their planes of polarization each form an angle of 45 degrees with respect to the polarization direction of the light incident on the magnetic memory medium 17, and are set at positions that are orthogonal to each other. . A differential amplifier 21 obtains a differential output from the photodetectors 20A and 20B, and the structure is such that only the rotational component of the polarization direction due to the change in the direction of magnetization is detected.

しかし一般に、偏光方向の回転角θkは1゜以下の
値の為、従来例の構成では光電変換過程を経て得
られる信号の振幅が非常に小さく、再生信号の
S/N比が充分でないという欠点を有している。
However, in general, the rotation angle θ k of the polarization direction is less than 1°, so in the conventional configuration, the amplitude of the signal obtained through the photoelectric conversion process is very small, and the S/N ratio of the reproduced signal is insufficient. It has drawbacks.

発明の目的 本発明は上記の欠点に鑑みてなされたもので、
光磁気メモリ媒体に記録された情報をより高品質
に、S/N比良く再生する事を目的としている。
Purpose of the Invention The present invention has been made in view of the above-mentioned drawbacks.
The purpose is to reproduce information recorded on a magneto-optical memory medium with higher quality and a good S/N ratio.

発明の構成 本発明は、レーザービームを光磁気メモリ上に
照射し、その反射光、或いは透過光を受光して、
光磁気メモリ上に磁化の変化として記録された情
報を光学的に再生するに際し、前記ビームとし
て、再生される情報信号が有する最高周波数の少
なくとも2倍以上の周波数差を持つ2つの直線偏
光ビームを用い、前記磁性薄膜上に前記直線偏光
ビームの1つを入射させて得られる磁性薄膜から
の反射光、或いは透過光と前記直線偏光ビームの
他の1つの偏光ビームとを第一の光検出器に入射
させて得られる信号を、前記2つの直線偏光ビー
ムを第二の光検出器に入射させて得られる信号を
基準にして、復調する事により、前記磁性薄膜上
の情報を、再生する事を特徴とするものである。
Structure of the Invention The present invention irradiates a magneto-optical memory with a laser beam, receives the reflected light or transmitted light, and
When optically reproducing information recorded as changes in magnetization on a magneto-optical memory, two linearly polarized beams having a frequency difference of at least twice the highest frequency of the information signal to be reproduced are used as the beams. A first photodetector detects the reflected light from the magnetic thin film obtained by making one of the linearly polarized beams incident on the magnetic thin film, or the transmitted light and the other one of the linearly polarized beams. The information on the magnetic thin film is reproduced by demodulating the signal obtained by making the two linearly polarized beams incident on the second photodetector, based on the signal obtained by making the two linearly polarized beams incident on the second photodetector. It is characterized by:

実施例の説明 以下、図面を参照して本発明の一実施例を詳細
に説明する。第4図は本発明を用いた光磁気メモ
リ再生装置の実施例の構成を示す図である。レー
ザー光源22より出た光はコリメート・レンズ2
3によつて平行光束にされ、偏光子24によつて
紙面に垂直方向の直線偏光になり、音響光学光変
調素子25に入いる。音響光学光変調素子25内
では、周波数fAの超音波によつて、入射したレー
ザービームが回折され、0次回折光26と1次回
折光27に分けられるが、この時これら2つの光
ビームの間には、超音波の周波数fAだけの周波数
差ができている。この2つの光ビームは第4図の
紙面に垂直な直線偏光のまま、ミラー28及び2
9で反射される。2つのビームの内、0次回折光
26は信号再生用のビームとしてハーフミラー3
0及び31、さらに集光レンズ32を通つて光磁
気メモリ媒体36に入射する。一方、1次回折光
27は光ビート信号検出用の参照用ビームとし
て、ハーフミラー33で反射されてハーフミラー
30に、又ハーフミラー33を通追し、ミラー3
4及びλ/2板35を通つてハーフミラー31に
各々入射する。ハーフミラー30では、光磁気メ
モリ媒体に入射する信号再生用ビームと参照用ビ
ームが重ね合わされ、光検出器37によつて2つ
のビームの周波数差fAに一致したビート信号が検
出される。一方ハーフミラー31では、光磁気メ
モリ媒体36より反射した光とλ/2板35によ
つて偏光方向が回転した参照用ビームが重ね合わ
され、光検出器38によつて2つのビームの周波
数差及び偏光方向によるビート信号が検出され
る。光磁気メモリ媒体上に蓄積された情報信号を
含んだ光検出器38の出力は、光検出器37の出
力を参照信号として、AM復調器39でAM復調
され、情報信号の再生が行なわれる。
DESCRIPTION OF EMBODIMENTS An embodiment of the present invention will be described in detail below with reference to the drawings. FIG. 4 is a diagram showing the configuration of an embodiment of a magneto-optical memory reproducing apparatus using the present invention. The light emitted from the laser light source 22 passes through the collimating lens 2
3 into a parallel beam of light, and a polarizer 24 into linearly polarized light perpendicular to the plane of the paper, which enters an acousto-optic light modulation element 25 . Inside the acousto-optic light modulator 25, the incident laser beam is diffracted by the ultrasonic wave of frequency fA and separated into 0th-order diffracted light 26 and 1st-order diffracted light 27, but at this time, there is a gap between these two light beams. There is a frequency difference equal to the ultrasonic frequency f A. These two light beams remain linearly polarized perpendicular to the plane of the paper in FIG.
It is reflected at 9. Of the two beams, the 0th order diffracted light 26 is sent to the half mirror 3 as a beam for signal reproduction.
0 and 31, and further enters the magneto-optical memory medium 36 through the condenser lens 32. On the other hand, the first-order diffracted light 27 serves as a reference beam for detecting the optical beat signal, is reflected by the half mirror 33, and is tracked to the half mirror 30 and through the half mirror 33.
The light enters the half mirror 31 through the λ/2 plate 35 and the λ/2 plate 35, respectively. In the half mirror 30, the signal reproduction beam and the reference beam incident on the magneto-optical memory medium are superimposed, and the photodetector 37 detects a beat signal that matches the frequency difference f A between the two beams. On the other hand, in the half mirror 31, the light reflected from the magneto-optical memory medium 36 and the reference beam whose polarization direction has been rotated by the λ/2 plate 35 are superimposed, and the photodetector 38 detects the frequency difference between the two beams. A beat signal depending on the polarization direction is detected. The output of the photodetector 38 containing the information signal stored on the magneto-optical memory medium is subjected to AM demodulation by the AM demodulator 39 using the output of the photodetector 37 as a reference signal, thereby reproducing the information signal.

次に光磁気メモリ媒体よりの反射光の偏光方向
の変化と光検出器38に検出されるビート信号の
関係について説明する。第5図に於いて、光磁気
メモリ媒体に入射した光の偏光方向が40の方向で
あつたと仮定すると、前記媒体上の磁化の方向に
よつて反射してくる光の偏光方向は41A及び4
1Bの方向の光になつている。この反射光に対
し、参照用ビームの偏光方向をλ/2板35によ
つて、前記反射光の2つの偏光方向のうちの一方
と直交する方向、例えば第5図の42の方向に変
える事ができる。これは、λ/2板35の結晶軸
方向を回転させる事で簡単に達成できる。従つて
第5図に示されたような偏光方向を持つ2つのビ
ームがハーフミラー31で重ね合わされ、光検出
器38に入射させる事ができる。ここで、42の
偏光方向を持つ参照用ビームと41A又は41B
の偏光方向を持つ光磁気メモリ媒体よりの反射光
の間にはやはりfAだけの周波数差が存在してい
る。一方、光のビート信号は2つの光の偏光方向
が直交している時は観測される事はなく、従つ
て、光検出器38では、光磁気メモリ媒体よりの
反射光の偏光方向が第5図の41Aの方向を向い
た時だけ光ビート信号が観察される事になる。す
なわち光検出器38の出力信号は、第6図cに示
したようになる。第6図でaは光磁気メモリ媒体
上の磁化の方向を、bは偏光方向の回転角の変化
を各々示している。第6図cに示された信号は、
光磁気メモリ媒体に記録された情報信号を、ビー
ト周波数fAで強度変調(AM)された形式になつ
ており、第4図のAM復調器39で復調して元の
情報信号を再生する事が可能となる。
Next, the relationship between the change in the polarization direction of the reflected light from the magneto-optical memory medium and the beat signal detected by the photodetector 38 will be explained. In FIG. 5, assuming that the polarization direction of the light incident on the magneto-optical memory medium is 40, the polarization directions of the reflected light are 41A and 41A, depending on the direction of magnetization on the medium.
The light is in the direction of 1B. With respect to this reflected light, the polarization direction of the reference beam is changed by the λ/2 plate 35 to a direction perpendicular to one of the two polarization directions of the reflected light, for example, the direction 42 in FIG. I can do it. This can be easily achieved by rotating the crystal axis direction of the λ/2 plate 35. Therefore, two beams having polarization directions as shown in FIG. 5 are superimposed by the half mirror 31 and can be made incident on the photodetector 38. Here, a reference beam with 42 polarization directions and 41A or 41B
There is still a frequency difference of f A between the reflected light from the magneto-optical memory medium with the polarization direction of . On the other hand, the optical beat signal is not observed when the polarization directions of the two lights are perpendicular to each other. The optical beat signal will be observed only when facing the direction 41A in the figure. That is, the output signal of the photodetector 38 becomes as shown in FIG. 6c. In FIG. 6, a indicates the direction of magnetization on the magneto-optical memory medium, and b indicates a change in the rotation angle of the polarization direction. The signal shown in FIG. 6c is
The information signal recorded on the magneto-optical memory medium is intensity modulated (AM) at the beat frequency fA , and is demodulated by the AM demodulator 39 in Fig. 4 to reproduce the original information signal. becomes possible.

本発明は、従来微弱な信号として検出されてい
た光磁気メモリによる偏光方向の微小な変化を、
光ビートを起こさせる事により、情報信号帯域の
最大周波数成分に対し2培以上の高い周波数をキ
ヤリアとする強度変調信号に変換し、信号を再生
しようとするものである。このような信号を高い
周波数で変調して検出する手法は、微小信号の検
出には従来より広く用いられている方法であり、 (i) キヤリア周波数に比べ充分帯域の狭い増幅器
で信号増幅でき、雑音が低下する。
The present invention detects minute changes in the polarization direction caused by magneto-optical memory, which were conventionally detected as weak signals.
By causing an optical beat, the signal is converted into an intensity modulation signal whose carrier is a frequency twice or more higher than the maximum frequency component of the information signal band, and the signal is reproduced. The method of detecting such a signal by modulating it at a high frequency has been widely used for detecting small signals. (i) The signal can be amplified by an amplifier with a sufficiently narrow band compared to the carrier frequency; Noise is reduced.

(ii) 強度変調された信号をキヤリア周波数で同期
検波する事により、信号の平滑化が行なわれ、
雑音が低下する。
(ii) The signal is smoothed by synchronously detecting the intensity modulated signal at the carrier frequency.
Noise is reduced.

等の効果があり、従来、偏光方向の変化を直接測
定していた場合と比べ、再生信号のS/N比の向
上をたやすく行なう事ができる。
As a result, the S/N ratio of the reproduced signal can be easily improved compared to the conventional case where changes in the polarization direction are directly measured.

本発明で、ビート周波数はサンプリング定理よ
り、再生される情報信号が有する最高の周波数に
対して、少なくとも2倍以上に選ぶ必要がある。
上述の実施例のように音響光学光変調素子を用い
た場合、ビート周波数を与える超音波の周波数fA
は、例えば80MHz程度にとる事ができ、40MHzま
での情報信号に対して本発明の再生方式を用いる
事が可能である。
In the present invention, according to the sampling theorem, the beat frequency must be selected to be at least twice the highest frequency of the information signal to be reproduced.
When using an acousto-optic light modulator as in the above embodiment, the frequency f A of the ultrasonic wave that provides the beat frequency
can be set to about 80 MHz, for example, and the reproduction method of the present invention can be used for information signals up to 40 MHz.

発明の効果 以上説明したように、本発明を用いる事により
光磁気メモリよりの情報の再生に際し、信号増幅
時の雑音を低下させ、又信号の平滑化による雑音
の除去ができ、高い品質で信号再生を行なう事が
可能になる。
Effects of the Invention As explained above, by using the present invention, when reproducing information from a magneto-optical memory, it is possible to reduce the noise during signal amplification, and also to remove noise by smoothing the signal, resulting in a high quality signal. It becomes possible to perform playback.

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

第1図は光磁気メモリの記録過程原理を示す斜
視図、第2図は光磁気メモリの再生過程原理を示
す斜視図、第3図は従来の光磁気メモリ再生方式
の構成を示すブロツク図、第4図は本発明の光磁
気メモリ再生方式の1実施例を示すブロツク図、
第5図は本発明の同実施例に於ける偏光方向の状
態を説明する図、第6図は本発明の同実施例に於
ける検出信号の例を示す図である。 22……レーザー光源、23……コリメートレ
ンズ、24……偏光子、25……音響光学光変調
素子、26……0次回折光、27……1次回折
光、28,29,34……ミラー、30,31,
33……ハーフミラー、32……集光レンズ、3
5……λ/2板、36……光磁気メモリ媒体、3
7,38……光検出器、39……AM復調器、4
0,41A,41B,42……偏光方向。
Fig. 1 is a perspective view showing the principle of the recording process of a magneto-optical memory, Fig. 2 is a perspective view showing the principle of the reproducing process of a magneto-optical memory, and Fig. 3 is a block diagram showing the configuration of a conventional magneto-optical memory reproducing method. FIG. 4 is a block diagram showing one embodiment of the magneto-optical memory reproducing method of the present invention.
FIG. 5 is a diagram for explaining the state of the polarization direction in the same embodiment of the present invention, and FIG. 6 is a diagram showing an example of a detection signal in the same embodiment of the present invention. 22... Laser light source, 23... Collimating lens, 24... Polarizer, 25... Acousto-optic light modulator, 26... 0th order diffracted light, 27... 1st order diffracted light, 28, 29, 34... Mirror, 30, 31,
33...Half mirror, 32...Condensing lens, 3
5...λ/2 plate, 36... Magneto-optical memory medium, 3
7, 38...Photodetector, 39...AM demodulator, 4
0, 41A, 41B, 42...Polarization direction.

Claims (1)

【特許請求の範囲】 1 磁性薄膜の膜面に垂直方向の磁化の変化とし
て記録された情報を光ビームにより読みとる際、
光ビームとして、再生される情報信号が有する最
高周波数の少なくとも2倍以上の周波数差を持つ
2つの直線偏光ビームを用い、前記磁性薄膜上に
前記直線偏光ビームの1つを入射させて得られる
磁性薄膜からの反射光、或いは透過光と前記直線
偏光ビームの他の1つの偏光ビームとを第一の光
検出器に入射させて得られる信号を、前記2つの
直線偏光ビームを第二の光検出器に入射させて得
られる信号を基準にして、復調する事により、前
記磁性薄膜上の情報を、再生する事を特徴とする
光磁気メモリ再生装置。 2 周波数差を有する2つの直線偏光ビームを作
り出す手段として、音響光学光変調素子を用いた
事を特徴とする特許請求の範囲第1項記載の光磁
気メモリ再生装置。
[Claims] 1. When reading information recorded as changes in magnetization perpendicular to the film surface of a magnetic thin film using a light beam,
Magnetism obtained by using two linearly polarized beams having a frequency difference of at least twice the highest frequency of the information signal to be reproduced as light beams, and making one of the linearly polarized beams incident on the magnetic thin film. A signal obtained by inputting the reflected light from the thin film or the transmitted light and the other one of the linearly polarized beams into a first photodetector, and the two linearly polarized beams are detected by a second photodetector. 1. A magneto-optical memory reproducing device characterized in that the information on the magnetic thin film is reproduced by demodulating the signal obtained by inputting the signal into the device. 2. The magneto-optical memory reproducing device according to claim 1, characterized in that an acousto-optic light modulation element is used as means for producing two linearly polarized beams having a frequency difference.
JP59100926A 1984-05-18 1984-05-18 Reproducing system of photomagnetic memory Granted JPS60243845A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59100926A JPS60243845A (en) 1984-05-18 1984-05-18 Reproducing system of photomagnetic memory

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59100926A JPS60243845A (en) 1984-05-18 1984-05-18 Reproducing system of photomagnetic memory

Publications (2)

Publication Number Publication Date
JPS60243845A JPS60243845A (en) 1985-12-03
JPH0542741B2 true JPH0542741B2 (en) 1993-06-29

Family

ID=14286952

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59100926A Granted JPS60243845A (en) 1984-05-18 1984-05-18 Reproducing system of photomagnetic memory

Country Status (1)

Country Link
JP (1) JPS60243845A (en)

Also Published As

Publication number Publication date
JPS60243845A (en) 1985-12-03

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