JPH0576706B2 - - Google Patents
Info
- Publication number
- JPH0576706B2 JPH0576706B2 JP59186406A JP18640684A JPH0576706B2 JP H0576706 B2 JPH0576706 B2 JP H0576706B2 JP 59186406 A JP59186406 A JP 59186406A JP 18640684 A JP18640684 A JP 18640684A JP H0576706 B2 JPH0576706 B2 JP H0576706B2
- Authority
- JP
- Japan
- Prior art keywords
- recording
- recording medium
- light
- laser
- traveling
- 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 - Fee Related
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/007—Arrangement of the information on the record carrier, e.g. form of tracks, actual track shape, e.g. wobbled, or cross-section, e.g. v-shaped; Sequential information structures, e.g. sectoring or header formats within a track
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/12—Heads, e.g. forming of the optical beam spot or modulation of the optical beam
- G11B7/122—Flying-type heads, e.g. analogous to Winchester type in magnetic recording
Landscapes
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Recording Or Reproduction (AREA)
- Optical Head (AREA)
Description
【発明の詳細な説明】
(技術の分野)
本発明はトラツク案内用の溝を有する走行記録
媒体と光ヘツドを用いてデータの記録再生を行う
光記録再生方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION (Field of Technology) The present invention relates to an optical recording and reproducing method for recording and reproducing data using a traveling recording medium having track guide grooves and an optical head.
(従来の技術)
本発明者らは先に光ヘツドに関する発明をなし
特許出願中(特願昭58−166731)である。この光
ヘツドを用いた光記録再生方式を、第5図につい
て説明する。1は半導体レーザ、2−1,2−2
は光検出器、3は分岐形光導波路、3−1は分岐
形光導波路3の開口端、3−2は解放開口端、4
は基板、5は解放開口端3−2から射出するレー
ザビーム、6は溝付走行記録媒体、7は保護膜付
の記録層、8はスライダ軸受である。(Prior Art) The present inventors have previously made an invention related to an optical head and are currently applying for a patent (Japanese Patent Application No. 166,731/1983). An optical recording/reproducing method using this optical head will be explained with reference to FIG. 1 is a semiconductor laser, 2-1, 2-2
3 is a photodetector, 3 is a branched optical waveguide, 3-1 is an open end of the branched optical waveguide 3, 3-2 is an open open end, 4
5 is a substrate, 5 is a laser beam emitted from the open opening end 3-2, 6 is a grooved running recording medium, 7 is a recording layer with a protective film, and 8 is a slider bearing.
半導体レーザ1より射出したレーザビームは、
開口端3−1から基板4に埋め込まれた分岐形光
導波路3に入射し、解放開口端3−2より射出す
る。記録時は高いレーザパワーを照射し、溝に沿
いデータを反射率変化により記録する。再生時は
低いレーザパワーを照射し、走行記録媒体6から
の反射光を検出する。溝の断面形状は矩形に近い
形状であるため、媒体照射光は垂直方向に多く反
射され、分岐形光導波路3に帰還する。データ列
に従い強度変化した光が光検出器2−2で検出さ
れる。 The laser beam emitted from the semiconductor laser 1 is
The light enters the branched optical waveguide 3 embedded in the substrate 4 through the open end 3-1, and exits through the open open end 3-2. During recording, high laser power is irradiated and data is recorded along the grooves by changes in reflectance. During reproduction, a low laser power is applied and reflected light from the running recording medium 6 is detected. Since the cross-sectional shape of the groove is nearly rectangular, the medium irradiation light is largely reflected in the vertical direction and returns to the branched optical waveguide 3. Light whose intensity changes according to the data string is detected by a photodetector 2-2.
(発明が解決しようとする問題点)
このような光記録再生方式では、半導体レーザ
1への戻り光がレーザ共振器内で発振光と干渉
し、レーザの出力変動が生ずる。このようなこと
を防ぐため、(i)光導波路3の分岐路数を増やし、
走行記録媒体6からの反射光を分散させ、半導体
レーザ1への戻り光を低減させる、(ii)光検出器側
の分岐形光導波路3の屈折率nを半導体レーザ側
の屈折率nより大きく半導体レーザ1への戻り光
を減少させるなどの方法が考えられている。とこ
ろで、このような方法では、(1)ヘツドの作製工程
が複雑となる、(2)半導体レーザから光導波路への
伝達効率が50〜80%となり、媒体照射レーザパワ
ーが減少する、などの問題点があつた。(Problems to be Solved by the Invention) In such an optical recording/reproducing system, the light returned to the semiconductor laser 1 interferes with the oscillated light within the laser resonator, causing fluctuations in the output of the laser. To prevent this, (i) increase the number of branches of the optical waveguide 3,
(ii) The refractive index n of the branched optical waveguide 3 on the photodetector side is made larger than the refractive index n on the semiconductor laser side. Methods such as reducing the amount of light returning to the semiconductor laser 1 have been considered. However, with this method, there are problems such as (1) the manufacturing process of the head becomes complicated, and (2) the transmission efficiency from the semiconductor laser to the optical waveguide is 50 to 80%, reducing the laser power for irradiating the medium. The dot was hot.
(発明の構成)
上記問題点を解決するため、本発明ではトラツ
ク案内用の溝を有する走行記録媒体とレーザ光源
の両側に光検出器を配置した光ヘツドとを備え、
該光ヘツドを該走行記録媒体上に近接浮上させ、
データの記録再生を行う光記録再生方法におい
て、上記走行記録媒体の走行方向と直交する方向
に断面がV形で該V形の頂角が140゜以上150゜以下
の溝を連続的に形成し、該V形溝の山部又は谷部
にデータを記録し、該山部又は谷部からの反射光
を上記レーザ光源の両側に配置した光検出器で受
光するようにして信号再生を行うことを特徴とす
る。(Structure of the Invention) In order to solve the above-mentioned problems, the present invention includes a traveling recording medium having track guiding grooves and an optical head in which photodetectors are arranged on both sides of a laser light source.
floating the optical head close to the traveling recording medium;
In an optical recording and reproducing method for recording and reproducing data, grooves having a V-shaped cross section and an apex angle of 140° or more and 150° or less are continuously formed in a direction perpendicular to the traveling direction of the traveling recording medium. , data is recorded on the peaks or valleys of the V-shaped groove, and signal reproduction is performed by receiving reflected light from the peaks or valleys with photodetectors placed on both sides of the laser light source. It is characterized by
(作用)
上記構成によれば、レーザ光源からのレーザビ
ームの反射光が両側に位置する光検出器に集中す
るので、レーザ光源への戻り光が減少する。(Function) According to the above configuration, the reflected light of the laser beam from the laser light source is concentrated on the photodetectors located on both sides, so that the amount of light returning to the laser light source is reduced.
(実施例)
第1図は本発明の第1の実施例であつて、従来
例と同一構成部分は同一符号をもつて表す。1は
レーザ光源としての半導体レーザ、2−1,2−
2は半導体レーザ1の両側に設けた光検出器、4
は基板、5はレーザビーム、6はトラツク案内溝
付走行記録媒体、7は保護膜付の記録層、8はス
ライダ軸受、9は断面V形の溝で、走行記録媒体
6の走行方向と直交する方向に連続的に形成され
る。光ヘツド(半導体レーザ1、光検出器2−
1,2−2、基板4)は第6図と同様スライダ軸
受8に設置される。(Embodiment) FIG. 1 shows a first embodiment of the present invention, in which the same components as those of the conventional example are denoted by the same reference numerals. 1 is a semiconductor laser as a laser light source, 2-1, 2-
2 is a photodetector provided on both sides of the semiconductor laser 1;
5 is a substrate, 5 is a laser beam, 6 is a running recording medium with track guide grooves, 7 is a recording layer with a protective film, 8 is a slider bearing, 9 is a groove with a V-shaped cross section, which is perpendicular to the running direction of the running recording medium 6. It is formed continuously in the direction of Optical head (semiconductor laser 1, photodetector 2-
1, 2-2, and the substrate 4) are installed on the slider bearing 8 as in FIG.
記録時、半導体レーザ1より射出したレーザビ
ーム5は、V形溝9の山部9aに追随し、強度変
調によりデータを反射率変化、あるいは屈折率変
化として媒体に記録する。この際、山部9aから
の反射光はその斜面によつて左右に分離される。
したがつて、媒体に垂直方向の反射光、すなわ
ち、半導体レーザ1への戻り光は溝の形状効果に
より大幅に抑えられる。 During recording, the laser beam 5 emitted from the semiconductor laser 1 follows the peak 9a of the V-shaped groove 9, and records data on the medium as a change in reflectance or a change in refractive index by intensity modulation. At this time, the reflected light from the mountain portion 9a is separated into left and right sides by the slope.
Therefore, the reflected light in the direction perpendicular to the medium, that is, the light returning to the semiconductor laser 1, is significantly suppressed due to the shape effect of the groove.
記録媒体としては、金属、非晶質薄膜などの穴
あけ記録媒体、あるいは、カルコゲナイト系材料
をベースとし、結晶、非晶質間の相変態を記録メ
カニズムとする記録媒体などが考えられる。 Possible recording media include perforated recording media such as metals and amorphous thin films, or recording media based on chalcogenite materials whose recording mechanism is phase transformation between crystal and amorphous.
再生時、半導体レーザ1より射出したレーザビ
ーム5はV形溝9の山部9aに追随し、該山部9
aからの反射光はその斜面によつて左右に分離さ
れ、各斜面に対応する光検出器2−1,2−2で
検出される。したがつて、媒体に垂直方向の反射
光、すなわち、半導体レーザ1への戻り光は溝の
形状効果により大幅に押えられる。一例として、
ビーム半径2.0μmのV形溝に照射し、媒体面上、
3.0μmでの反射回折光強度分布の計算結果を第2
図に示す。計算はフレネルキルヒホツフ積分を用
い、near fieldでの光強度分布を数値計算により
求めた。横軸は、光検出器上の座標、縦軸は相対
強度である。V溝角θが増大するにつれ、垂直方
向の反射光量は減少する。 During reproduction, the laser beam 5 emitted from the semiconductor laser 1 follows the peak 9a of the V-shaped groove 9, and
The reflected light from a is separated into left and right sides by the slope, and detected by photodetectors 2-1 and 2-2 corresponding to each slope. Therefore, the reflected light in the direction perpendicular to the medium, that is, the light returning to the semiconductor laser 1, is significantly suppressed by the shape effect of the groove. As an example,
Irradiates a V-shaped groove with a beam radius of 2.0 μm, and
The second calculation result of the reflected diffraction light intensity distribution at 3.0μm
As shown in the figure. The calculation used the Fresner-Kirchhoff integral, and the light intensity distribution in the near field was determined by numerical calculation. The horizontal axis is the coordinate on the photodetector, and the vertical axis is the relative intensity. As the V-groove angle θ increases, the amount of reflected light in the vertical direction decreases.
V溝角θの許容範囲は半導体レーザへの戻り光
量の許容条件により決定されるが、ほぼ15゜以上
20゜以下、いいかえればV形の頂角が140゜以上150゜
以下の範囲であれば良い。 The permissible range of the V-groove angle θ is determined by the permissible condition of the amount of light returned to the semiconductor laser, but it should be approximately 15° or more.
It is sufficient if the apex angle of the V shape is 20° or less, or in other words, the apex angle of the V-shape is in the range of 140° or more and 150° or less.
トラツク信号は光検出器2−1,2−2の差動
出力により検出される。レーザビーム5がV形溝
9の中心からずれた場合、V形溝9による反射回
折光強度分布は非対称となり、光検出器2−1,
2−2に入射するレーザパワーが異なる。 The track signal is detected by the differential outputs of photodetectors 2-1 and 2-2. When the laser beam 5 deviates from the center of the V-shaped groove 9, the intensity distribution of reflected and diffracted light by the V-shaped groove 9 becomes asymmetric, and the photodetectors 2-1,
The laser power incident on 2-2 is different.
一例として第3図に位置ずれ量0.5μmにおける
反射回折光強度分布の違いを示す。媒体面上
3.0μmにおいても、非対称光分布が生じトラツク
信号検出が可能となる。このように検出されたト
ラツク信号に従い、例えば第1図に示すスライダ
軸受8が設置されているヘツドアームが駆動さ
れ、トラツク制御が行われる。 As an example, FIG. 3 shows the difference in the intensity distribution of reflected diffracted light when the amount of positional shift is 0.5 μm. On the media surface
Even at 3.0 μm, an asymmetric light distribution occurs and track signal detection becomes possible. According to the track signal detected in this way, the head arm on which the slider bearing 8 shown in FIG. 1 is installed, for example, is driven, and track control is performed.
フオーカス制御は光学ヘツド全体を第1図に示
すスライダ軸受8の端面に設置し、空気浮上作用
を利用して行われる。スライダ軸受8の空気浮上
作用については、磁気デイスクに用いられる浮動
ヘツドスライダ軸受と同一であるため、ここでは
説明を省略する。走行記録媒体6から浮上距離
は、走行記録媒体6上の所要ビーム径より設定さ
れる。このような浮動ヘツド方式では従来装置に
おけるフオーカスアクチユエータを用いることな
くフオーカス制御が可能となる。 Focus control is performed by installing the entire optical head on the end face of the slider bearing 8 shown in FIG. 1 and utilizing air levitation. The air levitation effect of the slider bearing 8 is the same as that of a floating head slider bearing used in a magnetic disk, so a description thereof will be omitted here. The flying distance from the traveling recording medium 6 is set based on the required beam diameter on the traveling recording medium 6. Such a floating head system allows focus control without using a focus actuator in conventional devices.
前記実施例では、V形溝9の山部9aに追随し
てデータ記録を行うようにしたが、V形溝9の谷
部9bに追随してデータ記録し、これを再生する
ようにしても前記実施例と同様の効果が得られ
る。 In the embodiment described above, data is recorded following the peaks 9a of the V-shaped groove 9, but data may be recorded following the valleys 9b of the V-shaped groove 9 and then reproduced. The same effects as in the embodiment described above can be obtained.
第4図に上記光学ヘツドの製造方法を示す。第
4図において10はp−GaAs、11はp−
AlGaAs、12はGaAs、13はn−AlGaAs、
14はn−GaAsであり、14の基板上に半導体
レーザ、光検出器が一体形成される。15は電極
であり、Au−Cr、あるいは、Au−Ge−Ni等で
作製される。このような層を多層エピタキシヤル
成長により作製後、第4図に示すように幅1μm程
度のトレンチ16を設け、中心部と中心部の左右
両側に存在するp−n接合部とを電気的に絶縁す
る。中心部(実線斜線)はレーザ発光部となり、
左右のp−n接合部(点線斜線)は、逆バイアス
を与えられ、光検出部となる。トレンチを設ける
方法としては例えばイオンミリングによる穴あけ
加工がある。 FIG. 4 shows a method of manufacturing the optical head. In FIG. 4, 10 is p-GaAs and 11 is p-GaAs.
AlGaAs, 12 is GaAs, 13 is n-AlGaAs,
14 is n-GaAs, and a semiconductor laser and a photodetector are integrally formed on the substrate 14. Reference numeral 15 denotes an electrode, which is made of Au-Cr, Au-Ge-Ni, or the like. After producing such a layer by multilayer epitaxial growth, a trench 16 with a width of approximately 1 μm is provided as shown in FIG. Insulate. The center part (solid diagonal line) is the laser emitting part,
The left and right p-n junctions (dotted diagonal lines) are given a reverse bias and become photodetectors. A method for providing the trench is, for example, drilling by ion milling.
(発明の効果)
以上説明したように本発明によれば、トラツク
案内用の溝を有する走行記録媒体とレーザ光源の
両側に光検出器を配置した光ヘツドとを備え、該
光ヘツドを該走行記録媒体上に近接浮上させ、デ
ータの記録再生を行う光記録再生方法において、
上記走行記録媒体の走行方向と直交する方向に断
面がV形で該V形の頂角が140゜以上150゜以下の溝
を連続的に形成し、該V形溝の山部又は谷部にデ
ータを記録し、該山部又は谷部からの反射光を上
記レーザ光源の両側に配置した光検出器で受光す
るようにして信号再生を行うので、走行記録媒体
に照射されたレーザ光は半導体レーザにほとんど
戻ることがなく、したがつて、従来のものの如く
戻り光防止手段を設けることなく、安定した記録
再生を実現できるとともに、2つの光検出器に対
称な反射光が得られ、これによつてトラツク信号
が得られるため、簡単な構成の光記録再生装置を
実現できる利点がある。(Effects of the Invention) As explained above, according to the present invention, the optical head is provided with a traveling recording medium having a track guide groove and a photodetector disposed on both sides of a laser light source, and the optical head is In an optical recording and reproducing method in which data is recorded and reproduced by floating close to the recording medium,
A groove with a V-shaped cross section and an apex angle of 140° or more and 150° or less is continuously formed in the direction perpendicular to the running direction of the running recording medium, and the groove is formed in the peaks or troughs of the V-shaped groove. Since data is recorded and signals are reproduced by receiving the reflected light from the peaks or valleys with photodetectors placed on both sides of the laser light source, the laser light irradiated onto the running recording medium is Almost no light returns to the laser, so stable recording and playback can be achieved without the need for a means to prevent return light as in conventional systems, and symmetrical reflected light can be obtained on the two photodetectors. Since a track signal is thus obtained, there is an advantage that an optical recording/reproducing apparatus with a simple configuration can be realized.
第1図は本発明の一実施例を示すヘツド媒体構
成図、第2図は光強度分布のV溝角依存性を説明
するグラフ、第3図は位置ずれ量0.5μmでの光強
度分布を説明するグラフ、第4図は光ヘツドの構
成図、第5図は従来の光記録再生方式を説明する
ための光ヘツド及び記録媒体の概略構成図であ
る。
1……半導体レーザ、2−1,2−1……光検
出器、4……基板、5……レーザビーム、6……
溝付走行記録媒体、7……保護膜付の記録層、8
……スライダ軸受、9……V形溝。
Fig. 1 is a head medium configuration diagram showing an embodiment of the present invention, Fig. 2 is a graph explaining the dependence of the light intensity distribution on the V-groove angle, and Fig. 3 is the light intensity distribution at a positional deviation of 0.5 μm. FIG. 4 is a diagram of the structure of an optical head, and FIG. 5 is a schematic diagram of the structure of an optical head and a recording medium for explaining a conventional optical recording/reproducing system. 1... Semiconductor laser, 2-1, 2-1... Photodetector, 4... Substrate, 5... Laser beam, 6...
Grooved running recording medium, 7... Recording layer with protective film, 8
...Slider bearing, 9...V-shaped groove.
Claims (1)
レーザ光源の両側に光検出器を配置した光ヘツド
とを備え、該光ヘツドを該走行記録媒体上に近接
浮上させ、データの記録再生を行う光記録再生方
法において、 上記走行記録媒体の走行方向と直交する方向に
断面がV形で該V形の頂角が140゜以上150゜以下の
溝を連続的に形成し、 該V形溝の山部又は谷部にデータを記録し、 該山部又は谷部からの反射光を上記レーザ光源
の両側に配置した光検出器で受光するようにして
信号再生を行う ことを特徴とする光記録再生方法。[Scope of Claims] 1. A traveling recording medium having a track guide groove and an optical head having photodetectors arranged on both sides of a laser light source, the optical head being levitated close above the traveling recording medium, and data In an optical recording and reproducing method for recording and reproducing, continuously forming grooves having a V-shaped cross section and an apex angle of 140° or more and 150° or less in a direction perpendicular to the traveling direction of the traveling recording medium, Data is recorded on the peaks or valleys of the V-shaped groove, and signal reproduction is performed by receiving reflected light from the peaks or valleys with photodetectors placed on both sides of the laser light source. Characteristic optical recording and reproducing method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59186406A JPS6166238A (en) | 1984-09-07 | 1984-09-07 | Optical recording and reproducing method and optical head |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59186406A JPS6166238A (en) | 1984-09-07 | 1984-09-07 | Optical recording and reproducing method and optical head |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6166238A JPS6166238A (en) | 1986-04-05 |
| JPH0576706B2 true JPH0576706B2 (en) | 1993-10-25 |
Family
ID=16187850
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59186406A Granted JPS6166238A (en) | 1984-09-07 | 1984-09-07 | Optical recording and reproducing method and optical head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6166238A (en) |
Family Cites Families (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4888951A (en) * | 1972-02-23 | 1973-11-21 | ||
| JPS51100628A (en) * | 1975-03-03 | 1976-09-06 | Hitachi Ltd | |
| JPS51131283A (en) * | 1975-05-12 | 1976-11-15 | Hitachi Ltd | Semi-conductor unit |
| JPS57105828A (en) * | 1980-12-19 | 1982-07-01 | Matsushita Electric Ind Co Ltd | Optical disk recording and reproducing system |
-
1984
- 1984-09-07 JP JP59186406A patent/JPS6166238A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6166238A (en) | 1986-04-05 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |