JPS61280052A - Photomagnetic disk device - Google Patents
Photomagnetic disk deviceInfo
- Publication number
- JPS61280052A JPS61280052A JP12047285A JP12047285A JPS61280052A JP S61280052 A JPS61280052 A JP S61280052A JP 12047285 A JP12047285 A JP 12047285A JP 12047285 A JP12047285 A JP 12047285A JP S61280052 A JPS61280052 A JP S61280052A
- Authority
- JP
- Japan
- Prior art keywords
- signal
- detection system
- magneto
- header
- detected
- 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
Links
Abstract
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は消去可能光ディスクの一種である光磁気ディス
ク装置に係り、特に番地情報を含む反射率変化のヘッダ
ー信号と、データである光磁気信号とを有する光磁気デ
ィスクの信号処理に好適な光磁気ディスク装置に関する
。[Detailed Description of the Invention] [Field of Application of the Invention] The present invention relates to a magneto-optical disk device, which is a type of erasable optical disk, and particularly relates to a magneto-optical disk device that is a type of erasable optical disk, and in particular, a header signal of change in reflectance including address information, a magneto-optical signal that is data, The present invention relates to a magneto-optical disk device suitable for signal processing of a magneto-optical disk having a magneto-optical disk.
光磁気ディスクは記録膜に垂直磁化膜を用い、磁化の上
向き、下向きで情報を記録するもので、さらには消去が
可能であり、光ディスクの大容量。Magneto-optical disks use a perpendicular magnetization film for the recording film, and record information with the magnetization pointing upwards or downwards.Furthermore, they are erasable, and have a large capacity.
非接触記録、磁気ディスクの書き換え可能という特徴を
合わせもったファイルメモリとして近年開発が活発にな
ってきた。光磁気ディスクの信号検出は、特願昭58−
242006号に記載のようにディスク上にあらかじめ
凹凸ビットの形態で記録されている番地情報を含むヘッ
ダー信号と、データである光磁気信号は別々の検出器を
用いて検出しているヘッダ信号は従来の再生専用および
ライトワンス(Writo 0nce)型光ディスクと
同じように反射率変化として検出され、また光磁気信号
はカー(Kerr)効果による磁化の上向き、下向きに
よる偏光面のわずかな回転を検光子で光量変化として検
出されることになる。このように検出原理の違いから別
々の光検出器を用いており、これらの信号を上位コント
ローラへ送出する場合には従来はアナログ信号の状態で
混合していた。In recent years, development has been active as a file memory that combines the features of non-contact recording and rewritability of magnetic disks. Signal detection of magneto-optical disks was proposed in a patent application filed in 1983.
As described in No. 242006, the header signal containing address information recorded in advance in the form of uneven bits on the disk and the magneto-optical signal which is data are detected using separate detectors. The magneto-optical signal is detected as a change in reflectance in the same way as for read-only and write-once optical discs, and the magneto-optical signal is detected using an analyzer as a slight rotation of the plane of polarization due to the upward and downward directions of magnetization due to the Kerr effect. This will be detected as a change in the amount of light. As described above, separate photodetectors are used due to the difference in detection principles, and conventionally, when these signals are sent to a host controller, they are mixed in the form of analog signals.
しかし、アナログ信号の状態で混合するには、■それぞ
れの信号振幅を合わせなければならない、■アナログ的
に切換えるとその切換え時間がかかりすぎるなどの問題
があった。However, to mix analog signals, there are problems such as (1) the amplitude of each signal must be matched, and (2) switching in an analog manner takes too much time.
本発明の目的は、上述の如き振幅合わせ、切換え時間の
問題のない光磁気ディスク装置を提供することにある。An object of the present invention is to provide a magneto-optical disk device that does not have the problems of amplitude adjustment and switching time as described above.
本発明は、別々に検出された2つの信号を別々にディジ
タル化した後に混合することを特徴とする。The present invention is characterized in that two separately detected signals are separately digitized and then mixed.
光磁気ディスクの高速化を考えた場合、2つの信号の混
合時の切換え時間を無視できなくなり、アナログ状態で
混合するよりもディジタル化した後に混合する方がその
切換え時間が短かいので有効となる。When considering increasing the speed of magneto-optical disks, the switching time when mixing two signals cannot be ignored, and mixing after digitizing is more effective than mixing in an analog state because the switching time is shorter. .
以下、本発明の一実施例を第1図により説明する。レー
ザ1 (例えば半導体レーザ)から出た光はカップリン
グレンズ2で集光されて平行光となり、ビームスプリッ
タ3.ガルバノミラ−4を通り、絞り込みレンズ5でデ
ィスク6上の垂直磁化膜7にスポット径1μm程度に絞
り込まれる。垂直磁化膜7は初期状態として全面上向き
あるいは下向きに磁化されている。情報の記録/消去は
通常、キューり黒記録と呼ばれ、レーザ光照付により垂
直磁化膜7をキューり点温度まで上昇させて消磁し、そ
れと同時に電磁コイル8により外部磁場を印加して、外
部磁場の向きが初期状態の向きと逆の時が記録、同方向
の時が消去となる。垂直磁化膜7で反射された光は絞り
込みレンズ5.ガルバノミラ−4を通り、ビームスプリ
ッタ3で光路を分離され信号検出系に導かれる。信号検
出系は光磁気信号検出系とサーボ信号およびヘッダ信号
検出系があり、第2のビームスプリッタ9で分離される
。An embodiment of the present invention will be described below with reference to FIG. Light emitted from a laser 1 (for example, a semiconductor laser) is condensed by a coupling lens 2 to become parallel light, and then transmitted to a beam splitter 3. The light passes through the galvanometer mirror 4 and is focused onto the perpendicularly magnetized film 7 on the disk 6 by the focusing lens 5 to a spot diameter of about 1 μm. In the initial state, the perpendicular magnetization film 7 is entirely magnetized upward or downward. Recording/erasing of information is usually called cue black recording, in which the perpendicularly magnetized film 7 is heated to the cue point temperature by laser beam irradiation to demagnetize it, and at the same time, an external magnetic field is applied by the electromagnetic coil 8. Recording occurs when the direction of the magnetic field is opposite to the initial state, and erasure occurs when the direction is the same. The light reflected by the perpendicular magnetization film 7 passes through the aperture lens 5. The light passes through a galvanometer mirror 4, has an optical path separated by a beam splitter 3, and is guided to a signal detection system. The signal detection system includes a magneto-optical signal detection system and a servo signal and header signal detection system, which are separated by a second beam splitter 9.
光磁気信号検出系は検光子10.レンズ11゜光検出器
12からなっており、垂直磁化膜7の磁化の上向き、下
向きに対応して反射光の偏光面がわずかに回転するK
err効果を利用し、このわずかな偏光面の回転を検光
子10で光量変化に変換して、こ九を光検出器12で検
出する。サーボ信号およびヘッダ信号検出系は検出光学
系13と光検出器14からなっており、これらは通常の
ビデオディスク、オーディオディスクに用いられている
もので、自動焦点検出信号、トラック追跡信号の検出と
ディスクにあらかじめ凹凸ビットの形で記録されている
ヘッダ信号が検出される。The magneto-optical signal detection system is an analyzer 10. It consists of a lens 11 and a photodetector 12, and the plane of polarization of the reflected light rotates slightly in accordance with the upward and downward magnetization of the perpendicularly magnetized film 7.
Using the err effect, this slight rotation of the plane of polarization is converted into a change in light amount by the analyzer 10, and this is detected by the photodetector 12. The servo signal and header signal detection system consists of a detection optical system 13 and a photodetector 14, which are used for ordinary video discs and audio discs, and are used to detect automatic focus detection signals and track tracking signals. A header signal pre-recorded on the disc in the form of uneven bits is detected.
光検出器12で検出された光磁気信号と光検出器14で
検出されたヘッダ信号は第2図に示すような関係にある
。光磁気信号は増幅器15で増幅された後第2図(a)
に示すようなアナログ信号となり、ヘッダ信号を含んだ
ものとなっているが、データとなる光磁気信号を最大と
する検光子10の角度においてはヘッダ信号は光磁気信
号の3〜5倍となっているために、これをコンパレータ
回路を含むディジタル化回路16を通すとディジタル信
号となるが、ヘッダ信号部はコンパレートレベルが光磁
気信号部と異なるのでヘッダ信号部は利用できないこと
になる(第2図(b))。そこで、別の光検出器14で
検出したヘッダ信号を用いる。The magneto-optical signal detected by the photodetector 12 and the header signal detected by the photodetector 14 have a relationship as shown in FIG. After being amplified by the amplifier 15, the magneto-optical signal is shown in Fig. 2(a).
The signal becomes an analog signal as shown in , and includes a header signal. However, at the angle of the analyzer 10 where the magneto-optical signal serving as data is at its maximum, the header signal becomes 3 to 5 times as large as the magneto-optical signal. Therefore, when this is passed through the digitization circuit 16 including a comparator circuit, it becomes a digital signal, but since the comparator level of the header signal part is different from that of the magneto-optical signal part, the header signal part cannot be used (the header signal part cannot be used). Figure 2(b)). Therefore, a header signal detected by another photodetector 14 is used.
この信号は増幅、器17で増幅された後、第2図(C)
に示すアナログ信号となっており、これを光磁気信号の
場合と同様にディジタル化回路18を通してディジタル
信号とする(第2図(d))。上位コントローラへ再生
信号を送出するには、アドレス情報とDATAを含むも
のとする必要があり、第2図(b)と(d)を合成する
。光磁気信号の中からヘッダ信号部をとり除くためのタ
イミング信号(第2図(e))はヘッダー信号をタイミ
ング発生回路19へ通して作る。このタイミング発生回
路19はヘッダ信号の中に含まれるセクタマークを検出
してこれをもとにヘッダ信号期間、データ期間を示すタ
イミングを作り、(e)の抜き取りタイミング信号を発
生する。ディジタル化された光磁気信号(b)を抜き取
りタイミング信号(e)はAND論理素子20へ入力さ
れ、これによりヘッダー信号部が抜きとられデータ部の
みとなる(第2図(f))。After this signal is amplified by the amplifier 17, it is shown in Fig. 2 (C).
This is an analog signal shown in FIG. 2, and is converted into a digital signal through the digitization circuit 18 in the same way as the magneto-optical signal (FIG. 2(d)). In order to send the reproduced signal to the upper controller, it is necessary to include address information and DATA, and the signals shown in FIGS. 2(b) and 2(d) are combined. A timing signal (FIG. 2(e)) for removing the header signal portion from the magneto-optical signal is generated by passing the header signal through the timing generation circuit 19. This timing generation circuit 19 detects the sector mark included in the header signal, creates timings indicating the header signal period and data period based on this, and generates the sampling timing signal (e). The digitized magneto-optical signal (b) is extracted and the timing signal (e) is input to the AND logic element 20, whereby the header signal portion is extracted and only the data portion is left (FIG. 2(f)).
最後にディジタル化されたヘッダ信号(d)と抜き取り
後の光磁気信号(f)をOR論理素子2Iへ入力してヘ
ッダ信号付光磁気信号として上位コントローラへ送付す
る。以上の説明ではヘッダ信号の抜き取り9合成にAN
D、OR論理素子を用いたが、データセレクタであるT
I社のIC,5N74157などを用いても(bL (
dL (e)各信号から先述のヘッダ信号付光磁気信号
(g)を作ることができる。Finally, the digitized header signal (d) and the extracted magneto-optical signal (f) are input to the OR logic element 2I and sent to the upper controller as a magneto-optical signal with a header signal. In the above explanation, AN is used for extraction and synthesis of header signals.
D, an OR logic element is used, but T, which is a data selector,
Even if you use IC from company I, 5N74157, etc. (bL (
dL (e) The above-mentioned magneto-optical signal with header signal (g) can be created from each signal.
本発明の第2の実施例を第3図により説明する。A second embodiment of the present invention will be explained with reference to FIG.
これは第1図において光磁気信号検出系に差動検出を用
いたものでレーザ1からディスク6までは同じであるか
ら省略しである。ディスクからの反射光はビームスプリ
ッタ9へ入射し、ここでヘッダ信号検出系と光磁気信号
検出系に導かれる。ヘッダ信号検出系は実施例1で説明
したようにディジタル化されたヘッダ信号は光学系13
.光検出器14および増幅器17.ディジタル化回路1
8により得られる。光磁気信号検出系は172波長板2
2と偏光プリズム23を用いて反射光を2分した後、そ
れぞれをレンズ24と光検出器25゜レンズ26と光検
出器27の組合せで検出して差動増幅器28で光磁気信
号を検出する。この光磁気信号は第4図(b)のように
なっており、第1の実施例の場合とちがってヘッダ信号
部が表われない。したがって上位コントローラへ送出す
るヘッダ付光磁気信号は(b)のアナログ信号をディジ
タル化回路29に通してディジタル信号(c)として。This uses differential detection as the magneto-optical signal detection system in FIG. 1, and since the components from the laser 1 to the disk 6 are the same, they are omitted. The reflected light from the disk enters the beam splitter 9, where it is guided to a header signal detection system and a magneto-optical signal detection system. As explained in the first embodiment, the header signal detection system detects the digitized header signal using the optical system 13.
.. Photodetector 14 and amplifier 17. Digitization circuit 1
8. The magneto-optical signal detection system is a 172 wavelength plate 2.
2 and a polarizing prism 23, each is detected by a combination of a lens 24, a photodetector 25, a lens 26, and a photodetector 27, and a magneto-optical signal is detected by a differential amplifier 28. . This magneto-optical signal is as shown in FIG. 4(b), and unlike the first embodiment, the header signal portion does not appear. Therefore, the header-attached magneto-optical signal to be sent to the host controller is the analog signal (b) passed through the digitization circuit 29 to be converted into a digital signal (c).
さらに(a)と(c)の両信号をOR論理素子へ入力す
ると得られる。この様に光磁気信号を差動検出で検出す
る場合にはヘッダ信号抜き取り用のタイミング回路は不
要となる。Further, it is obtained by inputting both signals (a) and (c) to an OR logic element. In this way, when detecting magneto-optical signals by differential detection, a timing circuit for extracting header signals is not required.
本発明によれば、別々の光検出器で検出された2つの信
号をディジタル信号の状態で合成するので2つの信号の
レベル合わせをする必要がない、切換え時間が短くてす
むなどの効果がある。According to the present invention, since two signals detected by separate photodetectors are combined in a digital signal state, there is no need to adjust the levels of the two signals, and the switching time is shortened. .
第1図は本発明の第1の実施例を示す図、第2図は第1
の実施例における各部の波形を示す図、第3図は本発明
の第2の実施例を示す図、第4図は第2の実施例におけ
る各部の波形を示す図である。
l・・・レーザ光源、7・・・垂直磁化膜、8・・・電
磁コイル、19・・・タイミング発生回路、22・・・
1/2波長板、23・・・偏光プリズム、28・・・差
動増幅器。
¥J1国FIG. 1 is a diagram showing a first embodiment of the present invention, and FIG. 2 is a diagram showing a first embodiment of the present invention.
FIG. 3 is a diagram showing the second embodiment of the present invention, and FIG. 4 is a diagram showing the waveforms of each part in the second embodiment. l... Laser light source, 7... Perpendicular magnetization film, 8... Electromagnetic coil, 19... Timing generation circuit, 22...
1/2 wavelength plate, 23... polarizing prism, 28... differential amplifier. ¥J1 country
Claims (1)
垂直磁化膜に微小スポットとして集束する光学系と、該
垂直磁化膜の磁化の方向を検出して光量変化に換える第
1の検出系とあらかじめ記録媒体上に凹凸ビットの状態
で記録されているヘッダ信号を検出する第2の検出系と
から成る光磁気ディスク装置において、該第1の検出系
と該第2の検出系をそれぞれにディジタル化回路を設け
、それぞれディジタル化された後の両信号を合成するこ
とを特徴とする光磁気ディスク装置。1. A laser light source, an optical system that focuses the light from the laser light source as a minute spot on a perpendicularly magnetized film of a recording medium, and a first detection system that detects the direction of magnetization of the perpendicularly magnetized film and converts it into a change in light amount. and a second detection system for detecting a header signal recorded in advance in the form of concave and convex bits on a recording medium, in which the first detection system and the second detection system are each configured separately. 1. A magneto-optical disk device characterized by being provided with a digitizing circuit and synthesizing both signals after they have been digitized.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60120472A JPH07109671B2 (en) | 1985-06-05 | 1985-06-05 | Magneto-optical disk device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60120472A JPH07109671B2 (en) | 1985-06-05 | 1985-06-05 | Magneto-optical disk device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS61280052A true JPS61280052A (en) | 1986-12-10 |
JPH07109671B2 JPH07109671B2 (en) | 1995-11-22 |
Family
ID=14787016
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP60120472A Expired - Fee Related JPH07109671B2 (en) | 1985-06-05 | 1985-06-05 | Magneto-optical disk device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH07109671B2 (en) |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6085727U (en) * | 1983-11-18 | 1985-06-13 | 三洋電機株式会社 | information reading device |
JPS61237247A (en) * | 1985-04-15 | 1986-10-22 | Sanyo Electric Co Ltd | Information reader |
JPS61253657A (en) * | 1985-05-02 | 1986-11-11 | Olympus Optical Co Ltd | Reproducing device for photomagnetic disk |
-
1985
- 1985-06-05 JP JP60120472A patent/JPH07109671B2/en not_active Expired - Fee Related
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6085727U (en) * | 1983-11-18 | 1985-06-13 | 三洋電機株式会社 | information reading device |
JPS61237247A (en) * | 1985-04-15 | 1986-10-22 | Sanyo Electric Co Ltd | Information reader |
JPS61253657A (en) * | 1985-05-02 | 1986-11-11 | Olympus Optical Co Ltd | Reproducing device for photomagnetic disk |
Also Published As
Publication number | Publication date |
---|---|
JPH07109671B2 (en) | 1995-11-22 |
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