JPS63234418A - Multilayered magneto-optical disk device - Google Patents
Multilayered magneto-optical disk deviceInfo
- Publication number
- JPS63234418A JPS63234418A JP6820787A JP6820787A JPS63234418A JP S63234418 A JPS63234418 A JP S63234418A JP 6820787 A JP6820787 A JP 6820787A JP 6820787 A JP6820787 A JP 6820787A JP S63234418 A JPS63234418 A JP S63234418A
- Authority
- JP
- Japan
- Prior art keywords
- light source
- recording layer
- light
- optical disk
- electrostrictive element
- 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
Links
- 239000000758 substrate Substances 0.000 claims abstract description 14
- 125000006850 spacer group Chemical group 0.000 claims description 15
- 230000000694 effects Effects 0.000 claims description 5
- 230000005684 electric field Effects 0.000 abstract description 4
- 239000010410 layer Substances 0.000 description 56
- 238000000034 method Methods 0.000 description 10
- 230000003287 optical effect Effects 0.000 description 9
- 238000010586 diagram Methods 0.000 description 4
- 239000000463 material Substances 0.000 description 4
- 238000007796 conventional method Methods 0.000 description 2
- 239000010408 film Substances 0.000 description 2
- 239000002223 garnet Substances 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 239000011241 protective layer Substances 0.000 description 2
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 238000013459 approach Methods 0.000 description 1
- 229910002113 barium titanate Inorganic materials 0.000 description 1
- JRPBQTZRNDNNOP-UHFFFAOYSA-N barium titanate Chemical compound [Ba+2].[Ba+2].[O-][Ti]([O-])([O-])[O-] JRPBQTZRNDNNOP-UHFFFAOYSA-N 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 238000006073 displacement reaction Methods 0.000 description 1
- 239000000428 dust Substances 0.000 description 1
- 238000005566 electron beam evaporation Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- ZPDRQAVGXHVGTB-UHFFFAOYSA-N gallium;gadolinium(3+);oxygen(2-) Chemical compound [O-2].[O-2].[O-2].[Ga+3].[Gd+3] ZPDRQAVGXHVGTB-UHFFFAOYSA-N 0.000 description 1
- 238000010030 laminating Methods 0.000 description 1
- 229910052451 lead zirconate titanate Inorganic materials 0.000 description 1
- HFGPZNIAWCZYJU-UHFFFAOYSA-N lead zirconate titanate Chemical compound [O-2].[O-2].[O-2].[O-2].[O-2].[Ti+4].[Zr+4].[Pb+2] HFGPZNIAWCZYJU-UHFFFAOYSA-N 0.000 description 1
- 230000005415 magnetization Effects 0.000 description 1
- 239000004576 sand Substances 0.000 description 1
- 239000002356 single layer Substances 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 239000002344 surface layer Substances 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- 229910052723 transition metal Inorganic materials 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔概要〕
複数の記録層を備えて形成される光磁気ディスクの任意
の記録層にレーザ光の焦点合わせを行う方法として、第
1の光源で最上層の記録層に照射した反射光を用いて自
動焦点サーボを行うと共に、第2の光源を電歪素子上に
設け、電歪素子に電圧を加えて第2の光源と固定レンズ
との距離を変え、任意の記録層に焦点を合わせて記録・
再生および消去を行う光磁気ディスク装置。[Detailed Description of the Invention] [Summary] As a method for focusing a laser beam on an arbitrary recording layer of a magneto-optical disk formed with a plurality of recording layers, a first light source is used to focus a laser beam on an arbitrary recording layer of a magneto-optical disk formed with a plurality of recording layers. In addition to performing autofocus servo using the reflected light, a second light source is provided on the electrostrictive element, and a voltage is applied to the electrostrictive element to change the distance between the second light source and the fixed lens, allowing arbitrary recording. Record and focus on layers
A magneto-optical disk device that performs playback and erasing.
本発明は多層光磁気ディスクの各記録層への焦点合わせ
法に関する。The present invention relates to a method for focusing on each recording layer of a multilayer magneto-optical disk.
光磁気ディスクはレーザ光を用いて高密度の情報記録を
行うメモリであり、光ディスクと同様に記録容量が大き
く、非接触で記録・再生を行うことができ、また塵埃の
影響を受けないなど優れた特徴をもっている。A magneto-optical disk is a memory that uses laser light to record high-density information. Like an optical disk, it has a large storage capacity, can record and read without contact, and is unaffected by dust. It has certain characteristics.
か\る光磁気ディスクは同心円状あるいは渦巻き状の案
内溝を備えたディスク状の基板の上に希土類−遷移金属
系の非晶質合金の薄膜からなる記録層を設け、この上に
保護層を形成して構成されているが、小形大容量化を行
うために、か−る単板タイプの他に光磁気ディスクの保
護層を内側として背中合わせに接合したサンドインチタ
イプも実用化されている。Such magneto-optical disks have a recording layer made of a thin film of an amorphous rare earth-transition metal alloy on a disk-shaped substrate with concentric or spiral guide grooves, and a protective layer on top of this. In addition to the single-plate type, a sandwich type in which magneto-optical disks are bonded back to back with the protective layer on the inside has also been put into practical use in order to achieve a smaller size and larger capacity.
本発明は更に一段と小形大容量化を行った光磁気ディス
クに関するものである。The present invention also relates to a magneto-optical disk that is even more compact and has a larger capacity.
発明者等は光磁気ディスクの小形大容量化の方法として
第4図に示すような多層光磁気ディスクを提案している
。The inventors have proposed a multilayer magneto-optical disk as shown in FIG. 4 as a method for downsizing and increasing the capacity of magneto-optical disks.
すなわち、案内溝を備えた透明基板lの上に第1の記録
層2.第1のスペーサ層3.第2の記録層4.第2のス
ペーサ層5.第3の記録層6・・・と記録層とスペーサ
層とを交互に積層し、矢印で示すレーザ光7を図に示す
ように表面の記録層(この図の場合は第3の記録層6)
の側から照射するか、或いは透明基板1の側から照射し
、任意の記録層(図の場合は第1〜第3の記録層)にレ
ーザ光を集光して情報の記録・再生・消去を行うもので
ある。That is, a first recording layer 2. is formed on a transparent substrate l provided with a guide groove. First spacer layer 3. Second recording layer 4. Second spacer layer5. A third recording layer 6..., a recording layer, and a spacer layer are alternately laminated, and the laser beam 7 indicated by the arrow is directed to the surface recording layer (in this figure, the third recording layer 6). )
The laser beam is irradiated from the side of the transparent substrate 1 or from the side of the transparent substrate 1, and the laser beam is focused on any recording layer (in the case of the figure, the first to third recording layers) to record, reproduce, and erase information. This is what we do.
ここで、多層光磁気ディスクの構成を述べると、透明基
板lは光ディスクと同様に約1.2mmのガラスからな
り、この上にスパッタ法或いは電子ビーム蒸着法などの
方法で厚さが3000〜5000人の記録Id2,4.
6と厚さが5000人〜1μmのスペーサ層3.5で形
成されている。Here, to describe the structure of the multilayer magneto-optical disk, the transparent substrate l is made of glass with a thickness of about 1.2 mm, similar to the optical disk, and is coated with a thickness of 3000 to 5000 mm using a method such as sputtering or electron beam evaporation. Person record Id2, 4.
6 and a spacer layer 3.5 having a thickness of 5,000 to 1 μm.
ここで、記録層2.4.6の構成材料はγ二三酸化鉄(
γ−Pesos)や磁性ガーネットなど透明な垂直磁性
膜であり、またスペーサ3.5の構成材料はガラスや非
磁性ガーネット(ガドリニウム・ガリウム・ガーネット
Ga=GasOt□ 略称GGG)などを用いて形成さ
れている。Here, the constituent material of the recording layer 2.4.6 is γ diiron oxide (
The spacer 3.5 is made of a transparent perpendicular magnetic film such as γ-Pesos) or magnetic garnet, and the spacer 3.5 is made of glass or non-magnetic garnet (Gadolinium-Gallium-Garnet (Ga=GasOt□, abbreviated as GGG)). There is.
このように複数の垂直磁性膜を積層して記録層を形成し
、従来と同様に基板に垂直に磁場を加えている状態で任
意の記録層にレンズで集光したレーザ光を照射し、被照
射部の記録層の温度が上昇してキュリ一温度に近づき、
磁場の方向に磁化反転するのを利用して情報の記録を行
う。A recording layer is formed by stacking multiple perpendicular magnetic films in this way, and a laser beam focused by a lens is irradiated onto any recording layer while applying a magnetic field perpendicular to the substrate as in the conventional method. The temperature of the recording layer in the irradiated area rises and approaches the Curie temperature,
Information is recorded by utilizing magnetization reversal in the direction of the magnetic field.
このようにじて記録を行うと単層やサンドインチタイプ
に較ベムかに多量の情報を記録することができる。By recording in this manner, a much larger amount of information can be recorded than with a single layer or sand inch type.
然し、この場合の問題は如何にしてレーザ光を必要とす
る記録層に精度よく集光して記録し、また高速回転する
基板をサーボするかにある。However, the problem in this case lies in how to accurately focus the laser beam on the necessary recording layer for recording, and how to servo a substrate rotating at high speed.
第2図は今まで考えられていた焦点合わせ法(フォーカ
スシング法)を説明するもので、同図(A)は表面層の
第2の記録層4に焦点を合わせる場合、また同図(B)
は第1の記録層2に焦点を合わせる場合である。Figure 2 explains the focusing method that has been considered up to now. )
This is the case when focusing on the first recording layer 2.
すなわち、同図(A)はレーザ光源8からの光を固定レ
ンズ9を用いて平行光とした後、対物レンズ10を上下
動させて第2の記録層4の上に直径が1μm程度の微小
スポットに集光した場合で、第2の記録層4からの反射
光を二分割ディテクタと差動増幅器を用いて対物レンズ
10をボイスコイルで駆動して焦点合わせを行っている
。That is, in the figure (A), after the light from the laser light source 8 is made into parallel light using the fixed lens 9, the objective lens 10 is moved up and down to form a microscopic beam with a diameter of about 1 μm on the second recording layer 4. When the light is focused on a spot, the reflected light from the second recording layer 4 is focused using a two-split detector and a differential amplifier, and the objective lens 10 is driven by a voice coil.
また同様に同図(B)は第1の記録層2からの反射光で
サーボ機構を動作し、対物レンズ10を上下動させて第
1の記録層2に焦点合ねセし°た状態を示している。Similarly, (B) in the same figure shows a state in which the servo mechanism is operated by the reflected light from the first recording layer 2, and the objective lens 10 is moved up and down to focus on the first recording layer 2. It shows.
ここで、同図(A)のような場合は空気の屈折率と第2
の記録層4の屈折率が異なることから反射光量が多く、
従って反射光の検出は容易であるが、同図(B)のよう
な場合は記録層とスペーサ層との屈折率の差は殆どな(
、反射光量は僅かなために焦点合わせは非常に困難であ
る。Here, in the case shown in the same figure (A), the refractive index of air and the second
Since the refractive index of the recording layer 4 is different, the amount of reflected light is large,
Therefore, it is easy to detect the reflected light, but in a case like the one shown in the same figure (B), there is almost no difference in the refractive index between the recording layer and the spacer layer (
Since the amount of reflected light is small, focusing is extremely difficult.
以上記したように多層構造をとる各記録層への焦点合わ
せは、記録・再生・消去を行う記録層がらの反射光を検
出し、この信号電流により対物レンズを駆動して行って
いるが、記録層構成材料とスペーサ構成材料との屈折率
差が僅かなため反則光の検出が難しいことが問題である
。As described above, focusing on each recording layer with a multilayer structure is achieved by detecting the reflected light from the recording layer that performs recording, reproduction, and erasing, and driving the objective lens using this signal current. The problem is that the difference in refractive index between the material constituting the recording layer and the material constituting the spacer is small, making it difficult to detect reflected light.
C問題点を解決するための手段〕
上記の問題はディスク状をなす透明基板上にそれぞれ透
明な記録層とスペーサ層とを交互に複数偏積層して構成
される光磁気ディスクにおいて、第1の光源から最上層
の記録層に照射したレーザ光を用いて自動焦点サーボを
行うと共に、第2の光源を電歪素子上に設け、自動焦点
サーボを行う対物レンズを通してレーザ光を照射し、該
第2の光源と該光源の前に設けられている固定レンズと
の距離を前記電歪素子の電歪効果を用いて変化させ、任
意の記録層にレーザ光を集光させて情報の記録・再生お
よび消去を行う多層光磁気ディスクにより解決すること
ができる。Means for Solving Problem C] The above problem occurs when a magneto-optical disk is constructed by alternately laminating a plurality of transparent recording layers and spacer layers on a disk-shaped transparent substrate. Autofocus servo is performed using a laser beam irradiated from a light source to the uppermost recording layer, and a second light source is provided on the electrostrictive element, and the laser beam is irradiated through an objective lens that performs autofocus servo. The distance between the light source No. 2 and a fixed lens provided in front of the light source is changed using the electrostrictive effect of the electrostrictive element, and the laser beam is focused on an arbitrary recording layer to record and reproduce information. This problem can be solved by using a multilayer magneto-optical disk that performs erasing and erasing.
多層構造の任意の記録層にレーザ光を1μ請径のスポッ
トに集光して記録・再生および消去を行うには従来のフ
i法では無理である。It is impossible to perform recording, reproduction, and erasing on an arbitrary recording layer of a multilayer structure by focusing a laser beam onto a spot with a diameter of 1 μm using the conventional FI method.
すなわち、周速10w/s程度の高速回転し°ζいる基
板は100μ閣程度のうねりを伴っており、か−るディ
スク基板の表面層からの反射光を捕らえ、二分割ディテ
クタなどを用いて信号を得、これによりボイスコイルを
動かして対物レンズを最適位置に順応させるサーボa構
は光ディスクに使用されているが、これを反射光量の少
ない内部の記録層の焦点合わせに適用することは難しい
。In other words, a substrate rotating at a high speed of about 10 w/s has undulations of about 100 μm, and the reflected light from the surface layer of the disk substrate is captured and a signal is detected using a two-split detector or the like. A servo a mechanism is used in optical disks, which moves the voice coil to adapt the objective lens to the optimal position, but it is difficult to apply this to focusing on an internal recording layer where the amount of reflected light is small.
そこで、本発明はディスク基板のサーボ機構とは別に情
報の記録・再生および消去を行う第2のレーザ光源を設
けるもので、このレーザ光源とこの光源の前に設けであ
る固定レンズとの距離を変えることにより第2の光源か
らのレーザ光の焦点を多層光磁気ディスクの表面位置よ
り変え、層構造をとる複数の記録層のそれぞれに正確に
焦点を結ばせるようにしたものである。Therefore, the present invention provides a second laser light source for recording, reproducing, and erasing information separately from the servo mechanism of the disk substrate, and the distance between this laser light source and a fixed lens provided in front of this light source is By changing the focus of the laser beam from the second light source, the focus of the laser beam from the second light source is changed from the surface position of the multilayer magneto-optical disk, and the focus is accurately focused on each of the plurality of recording layers having a layered structure.
この場合、各記録層を隔てるスペーサ層の厚さは500
0人〜111m1と薄く、そのため第2のレーザ光源と
固定レンズとの距離は高精度に調節する必要がある。In this case, the thickness of the spacer layer separating each recording layer is 500 mm.
The distance between the second laser light source and the fixed lens must be adjusted with high precision because it is thin, measuring 0 to 111 m1.
本発明はこの位置の調節を電歪素子を用いて行うもので
、ランタン添加のチタン酸ジルコン酸鉛(略称PLZT
)やチタン酸バリウム(BaTiOs)のように圧電気
(Piezoelectrici ty)をもつ材料に
電界を加えると圧電効果により変形するのを利用して行
うものである。The present invention adjusts this position using an electrostrictive element, and uses lanthanum-doped lead zirconate titanate (abbreviated as PLZT).
) or barium titanate (BaTiOs), which deforms due to the piezoelectric effect when an electric field is applied to a piezoelectric material.
第1図は本発明を説明するもので、同図(A)は電歪素
子11の上に第2のレーザ光源(以下略して第2の光源
) 13を設け、従来と同様に固定レンズ9を用いて平
行光とし、対物レンズ10を図示を省略したサーボ機構
により駆動させて第2の記録層4に焦点を合わせた状態
を示している。FIG. 1 explains the present invention, and FIG. 1A shows a second laser light source (hereinafter abbreviated as second light source) 13 provided on an electrostrictive element 11, and a fixed lens 9 as in the conventional case. The object lens 10 is focused on the second recording layer 4 by driving the objective lens 10 by a servo mechanism (not shown).
次に同図(B)は電歪素子11に電界を印加して厚さ方
向に伸長させ、第2の光源13と固定レンズ9との距離
を縮めて焦点距離よりずらせた状態を示しており、対物
レンズ10の位置が同図(A)と変わらないために集光
位置は先に伸び、第1の記録層2に集光させたものであ
る。Next, the same figure (B) shows a state in which an electric field is applied to the electrostrictive element 11 to cause it to expand in the thickness direction, and the distance between the second light source 13 and the fixed lens 9 is shortened to deviate from the focal length. , since the position of the objective lens 10 is the same as in FIG.
ここで、電歪素子11は電極12の間に加える電圧と変
位量との関係と固定レンズ9の焦点位置からずらせた場
合のレーザ光の集光位置の移動量は判っており、また記
録層とスペーサ層の厚さは判っているので、電歪素子1
1の電極12に加える電圧により集光位置を調節するこ
とができる。Here, the relationship between the voltage applied between the electrodes 12 and the amount of displacement of the electrostrictive element 11 and the amount of movement of the focusing position of the laser beam when shifted from the focal position of the fixed lens 9 are known, and the recording layer Since the thickness of the spacer layer is known, electrostrictive element 1
The light focusing position can be adjusted by applying a voltage to one electrode 12.
本発明はこのように対物レンズ10の位置を変えず第2
の光源の位置を変えることにより焦点合わせを行うもの
である。In this way, the present invention provides a second lens without changing the position of the objective lens 10.
Focusing is performed by changing the position of the light source.
第3図は本発明に係る駆動法を説明する模式図であって
、サーボ系と情報の記録・再生および消去を行う信号系
とは別個に形成されている。FIG. 3 is a schematic diagram illustrating the driving method according to the present invention, in which a servo system and a signal system for recording, reproducing, and erasing information are formed separately.
すなわち、波長が780no+で出力が5 mWの第1
の光源15をサーボ系の光源として用い、一方波長83
0nsで出力10 mWの第2の光源13を信号系とし
て用いた。That is, the first wave with a wavelength of 780no+ and an output of 5 mW
The light source 15 is used as a servo system light source, while the wavelength 83
A second light source 13 with an output of 10 mW at 0 ns was used as a signal system.
そしてサーボ機構としては従来と同様に第1の光源15
からの光をハーフミラ−16,グイクロイックミラー1
7.対物レンズ10を通して多層光ディスク18を照射
し、この反射光19をグイクロイックミラー17.ハー
フミラ−16を通し°ζ二分υ1ディテクタ20に導き
、これより得る二つの信号を差動増幅器21に入力し、
ボイスコイル22により対物レンズlOを調整して多層
光ディスク18の表面に集光させる。As for the servo mechanism, the first light source 15 is used as before.
Half mirror 16, Gikroic mirror 1
7. A multilayer optical disk 18 is irradiated through an objective lens 10, and this reflected light 19 is reflected by a guichroic mirror 17. The signal is guided through the half mirror 16 to the °ζ half-divided υ1 detector 20, and the two signals obtained from this are input to the differential amplifier 21.
The objective lens lO is adjusted by the voice coil 22 to focus the light onto the surface of the multilayer optical disk 18.
一方、本発明に係る信号系は電歪素子11の上に設けた
第2の光源13を先ず固定レンズ9の焦点距離に置き、
レーザ光が多層光ディスク18の表面で焦点を結ぶのを
背後に設けた信号用ディテクタ23により確かめた後、
電源24の回路を閉じて電歪素子11に電界を加え、固
定レンズ9との距離を変えて図示するように集光位置を
変えることにより任意の記録層にレーザスポットを結ば
せることができる。On the other hand, the signal system according to the present invention first places the second light source 13 provided on the electrostrictive element 11 at the focal distance of the fixed lens 9,
After confirming that the laser beam is focused on the surface of the multilayer optical disk 18 using the signal detector 23 provided at the back,
By closing the circuit of the power supply 24, applying an electric field to the electrostrictive element 11, changing the distance from the fixed lens 9, and changing the focusing position as shown in the figure, a laser spot can be focused on any recording layer.
以上記したようにサーボ系と信号系とを別とし、多層光
ディスクを構成する各記録層への集光は従来のように対
物レンズのfI整によらず、第2の光源を移動して行う
本発明の実施により屈折率差の少ない記録層とスペーサ
層が積層してなる多層光ディスクにおいても任意の記録
層に正確に集光させることができる。As described above, the servo system and the signal system are separated, and light is focused on each recording layer that makes up the multilayer optical disk by moving the second light source instead of adjusting the fI of the objective lens as in the conventional method. By implementing the present invention, light can be accurately focused on any recording layer even in a multilayer optical disc in which a recording layer and a spacer layer with a small difference in refractive index are laminated.
第1図は本発明に係る焦点合わせ法を説明する模式図、
第2図は従来の焦点合わせ法を説明する模式図、第3図
は本発明に係る駆動法を説明する模式図、第4図は多層
光磁気ディスクの断面模式図、である。
図において、
1は透明基板、 2は第1の記録層、3は
第1のスペーサ層、 4は第2の記録層、5は第2の
スペーサ層、 6は第3の記録層、8はレーザ光源、
9は固定レンズ、10は対物レンズ、
11は電歪素子、13は第2の光源、
15は第1の光源、16はハーフミラ−1
17はグイクロイックミラー、18は多層光ディスク、
20は二分割ディテクタ、 21は差動増幅器、22
はボイスコイル、
23は信号用ディテクタFIG. 1 is a schematic diagram explaining the focusing method according to the present invention, FIG. 2 is a schematic diagram explaining the conventional focusing method, FIG. 3 is a schematic diagram explaining the driving method according to the present invention, and FIG. The figure is a schematic cross-sectional view of a multilayer magneto-optical disk. In the figure, 1 is a transparent substrate, 2 is a first recording layer, 3 is a first spacer layer, 4 is a second recording layer, 5 is a second spacer layer, 6 is a third recording layer, and 8 is a laser light source,
9 is a fixed lens, 10 is an objective lens,
11 is an electrostrictive element, 13 is a second light source,
15 is a first light source, 16 is a half mirror 1, 17 is a graphical mirror, 18 is a multilayer optical disk,
20 is a two-split detector, 21 is a differential amplifier, 22
is the voice coil, 23 is the signal detector
Claims (1)
スペーサ層とを交互に複数個積層して構成される光磁気
ディスクにおいて、 第1の光源から最上層の記録層に照射したレーザ光を用
いて自動焦点サーボを行うと共に、第2の光源を電歪素
子上に設け、自動焦点サーボを行う対物レンズを通して
レーザ光を照射し、該第2の光源と該光源の前に設けら
れている固定レンズとの距離を前記電歪素子の電歪効果
を用いて変化させ、必要とする記録層にレーザ光を集光
させて情報の記録・再生および消去を行うことを特徴と
する多層光磁気ディスク装置。[Claims] In a magneto-optical disk configured by alternately stacking a plurality of transparent recording layers and spacer layers on a disk-shaped transparent substrate, a first light source is provided to the topmost recording layer. Auto-focus servo is performed using the irradiated laser light, and a second light source is provided on the electrostrictive element, and the laser light is irradiated through the objective lens that performs auto-focus servo. The recording/reproducing and erasing of information is performed by changing the distance from a fixed lens provided in the electrostrictive element using the electrostrictive effect of the electrostrictive element, and focusing a laser beam on a required recording layer. A multilayer magneto-optical disk device.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6820787A JPS63234418A (en) | 1987-03-23 | 1987-03-23 | Multilayered magneto-optical disk device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6820787A JPS63234418A (en) | 1987-03-23 | 1987-03-23 | Multilayered magneto-optical disk device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63234418A true JPS63234418A (en) | 1988-09-29 |
Family
ID=13367118
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP6820787A Pending JPS63234418A (en) | 1987-03-23 | 1987-03-23 | Multilayered magneto-optical disk device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63234418A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5408453A (en) * | 1990-12-21 | 1995-04-18 | U.S. Philips Corporation | Method of and apparatus for optically writing, reading and erasing a multi-plane record carrier, and record carrier suitable for said method and apparatus |
EP0762403A2 (en) * | 1995-09-12 | 1997-03-12 | Hitachi, Ltd. | Optical disk apparatus and optical head thereof |
JPH09120556A (en) * | 1991-06-04 | 1997-05-06 | Internatl Business Mach Corp <Ibm> | Optical data storage medium |
EP0776004A2 (en) * | 1995-11-02 | 1997-05-28 | Konica Corporation | Optical system for recording and reproducing an optical recording medium |
-
1987
- 1987-03-23 JP JP6820787A patent/JPS63234418A/en active Pending
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5408453A (en) * | 1990-12-21 | 1995-04-18 | U.S. Philips Corporation | Method of and apparatus for optically writing, reading and erasing a multi-plane record carrier, and record carrier suitable for said method and apparatus |
JPH09120556A (en) * | 1991-06-04 | 1997-05-06 | Internatl Business Mach Corp <Ibm> | Optical data storage medium |
JPH09120552A (en) * | 1991-06-04 | 1997-05-06 | Internatl Business Mach Corp <Ibm> | Optical data storage medium |
EP0762403A2 (en) * | 1995-09-12 | 1997-03-12 | Hitachi, Ltd. | Optical disk apparatus and optical head thereof |
EP0762403A3 (en) * | 1995-09-12 | 1997-07-02 | Hitachi Ltd | Optical disk apparatus and optical head thereof |
EP0776004A2 (en) * | 1995-11-02 | 1997-05-28 | Konica Corporation | Optical system for recording and reproducing an optical recording medium |
EP0776004A3 (en) * | 1995-11-02 | 1997-07-16 | Konishiroku Photo Ind | Optical system for recording and reproducing an optical recording medium |
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