JPH03141050A - Optical recording medium - Google Patents
Optical recording mediumInfo
- Publication number
- JPH03141050A JPH03141050A JP1279211A JP27921189A JPH03141050A JP H03141050 A JPH03141050 A JP H03141050A JP 1279211 A JP1279211 A JP 1279211A JP 27921189 A JP27921189 A JP 27921189A JP H03141050 A JPH03141050 A JP H03141050A
- Authority
- JP
- Japan
- Prior art keywords
- layer
- light
- recording medium
- substrate
- resin
- 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
- 230000003287 optical effect Effects 0.000 title claims abstract description 27
- 239000010410 layer Substances 0.000 claims abstract description 57
- 229920005989 resin Polymers 0.000 claims abstract description 55
- 239000011347 resin Substances 0.000 claims abstract description 55
- 239000000758 substrate Substances 0.000 claims abstract description 36
- 239000011241 protective layer Substances 0.000 claims abstract description 18
- 229910052751 metal Inorganic materials 0.000 abstract description 7
- 239000002184 metal Substances 0.000 abstract description 7
- 239000011521 glass Substances 0.000 abstract description 4
- 150000002739 metals Chemical class 0.000 abstract description 3
- 238000010030 laminating Methods 0.000 abstract 1
- 239000000463 material Substances 0.000 description 9
- 239000010408 film Substances 0.000 description 7
- 238000000034 method Methods 0.000 description 6
- 239000000919 ceramic Substances 0.000 description 4
- 230000006866 deterioration Effects 0.000 description 4
- 239000013078 crystal Substances 0.000 description 3
- 239000000975 dye Substances 0.000 description 3
- 238000001746 injection moulding Methods 0.000 description 3
- NIXOWILDQLNWCW-UHFFFAOYSA-N acrylic acid group Chemical group C(C=C)(=O)O NIXOWILDQLNWCW-UHFFFAOYSA-N 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000031700 light absorption Effects 0.000 description 2
- 230000005389 magnetism Effects 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 239000004033 plastic Substances 0.000 description 2
- 229920003023 plastic Polymers 0.000 description 2
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- 239000004593 Epoxy Substances 0.000 description 1
- 229910015189 FeOx Inorganic materials 0.000 description 1
- -1 TeOx and TbFeCo Chemical class 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 230000002238 attenuated effect Effects 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 239000000428 dust Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000004744 fabric Substances 0.000 description 1
- 230000006870 function Effects 0.000 description 1
- 238000002347 injection Methods 0.000 description 1
- 239000007924 injection Substances 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 239000002923 metal particle Substances 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 239000004417 polycarbonate Substances 0.000 description 1
- 229920000515 polycarbonate Polymers 0.000 description 1
- 229910052761 rare earth metal Inorganic materials 0.000 description 1
- 150000002910 rare earth metals Chemical class 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- 239000012780 transparent material Substances 0.000 description 1
- 238000001771 vacuum deposition Methods 0.000 description 1
Landscapes
- Optical Record Carriers And Manufacture Thereof (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野1
本発明は、レーザ光により情報の記録、再生を行う光デ
ィスク等の光メモリに用いられる光記録媒体に関するも
のである。DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application 1] The present invention relates to an optical recording medium used in an optical memory such as an optical disk on which information is recorded and reproduced using laser light.
1従米扶111
従来、トラッキング用の案内溝を有するがラス、アクリ
ル、ボリカーボネーシ等の基板上に記録層を形成したよ
く知られた光記録媒体の他に、平坦な記録層上に透明な
樹脂で案内溝を形成している光記録媒体があった。第9
図に示すように、この光記録媒体90は、G G G
(GdzGaso 、2)等の透明単結晶基板91上に
液相成長法等で成長させたY I G (Y 3F e
5012)等の磁性〃−ネット単結晶膜92と、その上
に設けられトラッキング用案内溝を有する紫外線硬化樹
脂93と、AI等の反射層94と、5i02等の保護層
95とから構成される。磁性が一ネット膜92は、Tb
Fe=TbFeC。1 Jubei Fu 111 In addition to the well-known optical recording media that have guide grooves for tracking and have a recording layer formed on a substrate made of lath, acrylic, polycarbonate, etc., optical recording media that have a recording layer formed on a flat recording layer are There was an optical recording medium that formed a guide groove. 9th
As shown in the figure, this optical recording medium 90 consists of G G G
Y I G (Y 3 F e
It is composed of a magnetic net single crystal film 92 such as 5012), an ultraviolet curing resin 93 provided thereon and having a tracking guide groove, a reflective layer 94 such as AI, and a protective layer 95 such as 5i02. . The one-net magnetic film 92 has Tb
Fe=TbFeC.
等の希土jl[!移金属7モル7Tス合金と比べて光の
吸収が小さいため、基板911Ilから照射されたレー
ザ光は磁性〃−ネット膜92を透過し、反射7194で
反射する0反射層94の形状は、透明樹脂71193の
案内溝に倣った凹凸形状を成しでいるため、この案内溝
を利用してトラッキングをとることができる。すなわち
、案内溝を正確にトレースして記録再生を行うためにプ
ッシュプル法が用いられる。レーザビームが案内溝の中
央にあるときはトラッキング溝による回折パターンがト
ラックの中心線に対し、左右対称となるため、回折光を
エサm7オトグイオードで受光すると、その差動出力は
Oとなる。これに対しレーザビームが案内溝の中央から
左右にずれると、トラッキング溝による回折パターンが
非対称となるため、二分割7すトダイオードで受光した
ときの差動出力は正または負の出力となる。そして、こ
の二分割7tトダイオードの差動出力が常に0となるよ
うにレーザビームの位置がフィードバック制御されトラ
ッキングが行われる。Rare earth jl [! Since the absorption of light is smaller than that of the transfer metal 7M 7T alloy, the laser beam irradiated from the substrate 911Il passes through the magnetic net film 92 and is reflected by the reflection layer 94.The shape of the reflection layer 94 is transparent. Since it has an uneven shape that follows the guide groove of resin 71193, tracking can be performed using this guide groove. That is, the push-pull method is used to accurately trace the guide groove and perform recording and reproduction. When the laser beam is at the center of the guide groove, the diffraction pattern due to the tracking groove is symmetrical with respect to the center line of the track, so when the diffracted light is received by the bait m7 otodiode, its differential output becomes O. On the other hand, if the laser beam deviates from the center of the guide groove to the left or right, the diffraction pattern due to the tracking groove becomes asymmetrical, so that the differential output when received by the two-split seven-piece diode becomes a positive or negative output. Then, the position of the laser beam is feedback-controlled and tracking is performed so that the differential output of this two-divided 7t diode is always zero.
[発明が解決しようとする課題)
しかしながら、前述した磁性が一ネット単結晶腋を記t
iMとする記録媒体では、記録層に単結晶を用いる必要
があるため、基板は、記録層と同じ結晶構造を有し、か
つ格子定数もほぼ等しいという条件を満たす必要がある
。このため、基板材料は大きく制限され一般に高価であ
る。また、このような基板材料は、一般に加工性が悪い
ため、トラッキング用案内溝を基板表面に形成すること
は極めて困難である。このため、トラッキングを行うた
めには透明樹脂で溝を形成し、さらに反射層を設ける必
要があり、製造工程が複雑になることから、高価になる
と同時に信頼性も低くなる。なお、従来の溝付基板を用
いた記録媒体では、記録層が基板の溝形状を倣った凹凸
形状を成しているため、その段差部分で膜厚が不均一に
なり、ビット形状がくずれることによるS/Nの低下や
段差部分からの記録層の劣化が生じるという問題がある
。[Problem to be solved by the invention] However, the above-mentioned magnetism
In the iM recording medium, since it is necessary to use a single crystal for the recording layer, the substrate must have the same crystal structure as the recording layer and satisfy the conditions that the lattice constants are also approximately the same. For this reason, substrate materials are severely limited and generally expensive. Further, since such substrate materials generally have poor workability, it is extremely difficult to form tracking guide grooves on the substrate surface. Therefore, in order to perform tracking, it is necessary to form grooves with transparent resin and further provide a reflective layer, which complicates the manufacturing process, resulting in high cost and low reliability. In addition, in recording media using conventional grooved substrates, the recording layer has an uneven shape that follows the groove shape of the substrate, so the film thickness becomes uneven at the stepped portions and the bit shape may be distorted. There are problems in that the S/N ratio is lowered due to this and the recording layer deteriorates from the step portion.
[発明の目的]
本発明は、上述した問題点を解決するためになされたも
のであり、その目的とするところは、基板上に平坦な記
録層を形成し、その上に光吸収性の樹脂を用いて溝を構
成し、樹脂側から記録、再生を行うことにより、ff?
ス、樹脂等の透明な基板以外にも幅広い材料の基板を用
いることができ、記録特性が優れ、経年変化が少い、安
定で高品質の光記録媒体を安価に提供することにある。[Object of the Invention] The present invention has been made in order to solve the above-mentioned problems, and its purpose is to form a flat recording layer on a substrate, and coat a light-absorbing resin on the flat recording layer. By constructing the groove using ff? and performing recording and playback from the resin side, ff?
The object of the present invention is to provide, at a low cost, a stable, high-quality optical recording medium that can use a wide range of substrate materials other than transparent substrates such as glass and resin, has excellent recording characteristics, and exhibits little deterioration over time.
[課題を解決するための手段]
この目的を達成するために本発明の光記録媒体では、プ
ラス、樹脂、金属あるいはセラミック等の基板上に平坦
な記録層を形成し、その上に光吸収性の樹脂を用いてト
ラッキング用案内溝を形成している。そして、光吸収性
樹脂側から情報の記録再生あるいは消去をするようにし
ている。[Means for Solving the Problems] In order to achieve this object, in the optical recording medium of the present invention, a flat recording layer is formed on a substrate made of plastic, resin, metal, ceramic, etc., and a light-absorbing layer is formed on the flat recording layer. The tracking guide groove is formed using resin. Then, information is recorded, reproduced, or erased from the light-absorbing resin side.
[作用]
上記の構成を有する本発明の光記録媒体では、光吸収性
の樹脂を用いてトラッキング用案内溝を形成しており、
樹脂の厚い凸部は、照射された光が樹脂によって吸収さ
れるため、結果的に記録層から反射されてくる光量は小
さくなる。これに対し、樹脂が薄い凹部では光がほとん
ど吸収されないため、記録層に十分強い光が達し、また
反射光量も十分大きいため情報の記録再生および7オー
カシングサーボを行うことができる。トラッキングサー
ボは、樹脂層凸部と四部の厚さの違いによる反射光量の
差を利用して3ビーム法によって行う、記ttMは平坦
な基板の上に形成されているため、平坦であり均一な記
録特性が得られると共に膜劣化の原因となる段差部分は
生じない。なお、案内溝付光吸収性樹脂層は、通常の溝
付スタンパを用い、射出成形や紫外線硬化樹脂を用いて
安価に生産性よく作製することができる。[Function] In the optical recording medium of the present invention having the above configuration, the tracking guide groove is formed using a light-absorbing resin,
Since the resin absorbs the irradiated light on the thick convex portion of the resin, the amount of light reflected from the recording layer becomes small as a result. On the other hand, in the recesses where the resin is thin, almost no light is absorbed, so the sufficiently strong light reaches the recording layer, and the amount of reflected light is also sufficiently large, making it possible to record and reproduce information and perform 7-ocusing servo. Tracking servo is performed by a three-beam method using the difference in the amount of reflected light due to the difference in thickness between the convex and four parts of the resin layer.Since the ttM is formed on a flat substrate, it is flat and uniform. Recording characteristics can be obtained, and step portions that cause film deterioration do not occur. Note that the light-absorbing resin layer with guide grooves can be manufactured at low cost and with high productivity using a normal grooved stamper, injection molding, or ultraviolet curing resin.
[実施例]
以下、本発明を具体化した一実施例を図面を参照して説
明する。[Example] Hereinafter, an example embodying the present invention will be described with reference to the drawings.
第1図は本発明の一実施例である光記録媒体10の要部
断面図であり、この光記録媒体10は、ガラスあるいは
アクリル、ポリカーボネート等の樹脂およびA1等の金
属あるいはセラミック等から成る基板11にS io
2− S io −A I N等の保護層12、Te、
TeOx、TbFeCo等の金属、相変化記録材料、光
磁気記録材料、色素等から成る記i屑13、保護層14
、光吸収性樹脂15お上り透明樹脂から成る保護層16
を順次積層したものである。FIG. 1 is a sectional view of a main part of an optical recording medium 10 according to an embodiment of the present invention. S io on 11
2- Protective layer 12 such as Sio-AIN, Te,
Scraps 13 and protective layer 14 made of metals such as TeOx and TbFeCo, phase change recording materials, magneto-optical recording materials, dyes, etc.
, a light-absorbing resin 15 and a protective layer 16 made of a transparent resin.
are sequentially laminated.
情報の記録再生は基板11とは反対側がら行うため、基
板11には、ガラス、If脂等の透明な材料の他に金属
やセラミック等の不透明な材料を用いることができる。Since information is recorded and reproduced from the side opposite to the substrate 11, the substrate 11 can be made of an opaque material such as metal or ceramic in addition to a transparent material such as glass or If resin.
特に基板にセラミックを用いることにより、軽くて高速
回転が可能であり、変形しにくく安定な光記録媒体を提
供することができる。In particular, by using ceramic for the substrate, it is possible to provide an optical recording medium that is lightweight, can be rotated at high speed, and is resistant to deformation and is stable.
記!i層13およびその両側の保N層12.14は、よ
く知られている真空蒸着法、スパッタリング法等の薄膜
形成手段により作製される。なお、保llI股12およ
び14は、必ずしも必要ではなく、その一方あるいは両
方がなくてもよい、基板11の表面は平坦であるため、
記録層13も平坦となる。これにより記録層に断差部分
が生じず、略均−な厚さで形成されているため、均一な
記録特性が得られると共に膜劣化が生じにくく、信頼性
が大幅に向上する。さらに、溝の段差によるビット形状
の乱れもなくなるため、ビット形状の乱れによるノイズ
の発生がなくS/Nが向上する。Record! The i-layer 13 and the N-holding layers 12 and 14 on both sides thereof are produced by a well-known thin film forming method such as a vacuum evaporation method or a sputtering method. Note that the retainers 12 and 14 are not necessarily necessary, and one or both of them may be omitted.Since the surface of the substrate 11 is flat,
The recording layer 13 also becomes flat. As a result, there is no difference in the recording layer and the recording layer is formed with a substantially uniform thickness, so that uniform recording characteristics can be obtained, and film deterioration is less likely to occur, greatly improving reliability. Further, since there is no disturbance in the bit shape due to the step difference in the groove, there is no noise caused by the disturbance in the bit shape, and the S/N ratio is improved.
案内溝を有する光吸収性樹脂層15は、例えば第2図に
示されているようにして形成される。まず、同図(a)
のように基板11に保護層12.記録層13.保護層1
4を順次積層する1次に同図(b)のようにあらかじめ
渦巻状若しくは同心円状に溝が形成されている金属スタ
ンパ21を記録層13および保!I層12.14が形成
された基板11に近接させ、そのすきまに光吸収性樹脂
を射出成形する。冷却後、スタンパ21を除去すること
によ、り同図(e)のように案内溝25を有する光吸収
性樹脂15が形成される。光吸収性樹脂15の溝部(凹
g)25は、薄いため、照射されたレーザ光はほとんど
吸収されずに記録M13に達し、また記録W113から
の反射光もほとんど減衰せずに図示されない光学ヘッド
で受光される。光吸収性樹脂15の凸部26は溝部25
と比べて十分厚いためレーザ光が凸部26に照射され、
記録層13に達し、さらに記録層13から反射されて再
び光吸収性樹脂15の凸W626を通過してディスク外
部へ反射されるまでに光吸収性樹脂15によって吸収さ
れるため、反射光強度は弱くなる。すなわち、光吸収性
樹脂15の溝部25に照射されたレーザ光は、はとんど
減衰せずに反射され、反射光強度は大きいのに対し、凸
部26に照射されたレーザ光の反射光強度は小さくなり
、反射光量に差が生じる。The light-absorbing resin layer 15 having guide grooves is formed, for example, as shown in FIG. 2. First, the same figure (a)
A protective layer 12 is formed on the substrate 11 as shown in FIG. Recording layer 13. Protective layer 1
First, as shown in FIG. 4(b), a metal stamper 21 in which grooves are previously formed in a spiral or concentric pattern is placed on the recording layer 13 and the recording layer 13. It is brought close to the substrate 11 on which the I layers 12 and 14 are formed, and a light-absorbing resin is injection molded into the gap. After cooling, the stamper 21 is removed, thereby forming the light-absorbing resin 15 having guide grooves 25 as shown in FIG. 2(e). Since the groove portion (concave g) 25 of the light-absorbing resin 15 is thin, the irradiated laser light reaches the recording M13 without being absorbed, and the reflected light from the recording W113 is hardly attenuated and is connected to the optical head (not shown). The light is received by The convex portion 26 of the light-absorbing resin 15 is the groove portion 25
Since it is sufficiently thick compared to the laser beam, the convex portion 26 is irradiated with
The intensity of the reflected light is absorbed by the light absorbing resin 15 before it reaches the recording layer 13, is further reflected from the recording layer 13, passes through the convex W626 of the light absorbing resin 15, and is reflected to the outside of the disc. become weak. In other words, the laser beam irradiated onto the groove portion 25 of the light-absorbing resin 15 is reflected without attenuation and the intensity of the reflected light is high, whereas the reflected light of the laser beam irradiated onto the convex portion 26 is The intensity becomes smaller and a difference occurs in the amount of reflected light.
このような反射光量の差を利用して第3図のように3ビ
ーム法によってトラッキングを行う、すなわち、記録再
生用のビーム31の他に、光吸収性樹脂の溝部25と凸
部26の境界にほぼ中心をもつ光ビーム32.33を溝
部25の両側に配置する。ビーム31が溝部25の中心
にあるときには、ビーム32.33の反射光量は等しく
なる。Utilizing such a difference in the amount of reflected light, tracking is performed by a three-beam method as shown in FIG. Light beams 32, 33 approximately centered at are placed on both sides of the groove 25. When the beam 31 is at the center of the groove 25, the amounts of reflected light of the beams 32 and 33 are equal.
ビームが右側にずれたときは、ビーム32の反射光量が
減少し、ビーム33の反射光量は増大する。When the beam shifts to the right, the amount of reflected light of beam 32 decreases and the amount of reflected light of beam 33 increases.
逆に、ビームが左側へずれたときは、ビーム32の反射
光量が増大し、ビーム33の反射光量が減少する。従っ
て、ビーム32.33の反射光量出力の差動をとること
によりトラッキングエラー信号が得られトラッキングサ
ーボを行うことができる。Conversely, when the beam shifts to the left, the amount of reflected light of beam 32 increases and the amount of reflected light of beam 33 decreases. Therefore, by calculating the difference between the outputs of the reflected light quantities of the beams 32 and 33, a tracking error signal can be obtained and tracking servo can be performed.
この上うな光吸収性樹脂15は、レーザ光の波長で光を
吸収する色素を混入した樹脂あるいは紫外線硬化樹脂を
用いることができる。紫外線硬化樹脂を用いるときは、
スタンパ21とのFl 間ニat脂を流し込んだ後、紫
外線を照射して硬化させ溝を形成する。また、@4図(
a)のように、紫外線硬化樹脂あるいは7オトレジスト
41を!布した後、(b)のように溝形状に対応したパ
ターンをもつマスク45をあて、紫外線を照射すること
により照射部分のみを硬化させ、同図(c)のように溝
を形成してもよい、このとき、第2図(c)のように溝
の底部25は、必ずしもなくてもよい。また、第5図の
ように溝の形状は、矩形である必要はなく、例えば角が
丸くなってもよい。As the light-absorbing resin 15, a resin mixed with a dye that absorbs light at the wavelength of the laser beam or an ultraviolet curing resin can be used. When using ultraviolet curing resin,
After pouring the resin between Fl and the stamper 21, it is cured by irradiation with ultraviolet rays to form grooves. Also, @Figure 4 (
As in a), use ultraviolet curing resin or 7 Otoresist 41! After applying the cloth, as shown in (b), a mask 45 with a pattern corresponding to the groove shape is applied, and by irradiating ultraviolet rays, only the irradiated parts are cured, and grooves are formed as shown in (c) of the same figure. In this case, the groove bottom 25 does not necessarily have to be provided as shown in FIG. 2(c). Further, the shape of the groove does not have to be rectangular as shown in FIG. 5, and may have rounded corners, for example.
光吸収性樹脂15は、アクリル、エポキシ、紫外線硬化
樹脂等の透明樹脂に色素の代わりに、炭素、金属粒子等
を分散させて作製してもよい、*た、光吸収性樹脂の凸
部の厚さは、?llI部に対して十分光を吸収する程度
の厚さであればよ(、特に限定しない、すなわち、樹脂
の光吸収係数に応じて適当な厚さに定められる。The light-absorbing resin 15 may be made by dispersing carbon, metal particles, etc. instead of dyes in a transparent resin such as acrylic, epoxy, or ultraviolet curing resin. What is the thickness? The thickness is not particularly limited as long as it can absorb enough light for the llI portion (in other words, it is determined to be an appropriate thickness depending on the light absorption coefficient of the resin).
なお、透明保N層16は、光吸収性樹脂15上にスピン
コード、射出成形等の方法により簡単に形成することが
できる。透明保1171qlGの材質、厚さについては
特に限定しない。また、透明保護層は必ずしも必要では
なく、形成されな(でもよし1゜
以上、本発明の一実施例を図面に基づいて詳細に説明し
たが、本発明は他の1!様で実施することもできる0例
えば、@6図のように基板11と保1!層12の間にA
1等の反射層61を設けてもよい、このとき記録層13
は、レーザ光が透過する程度に薄いか、多結晶となりノ
イズが増加するが磁性が−ネッシのように透光性の大ト
な材料で作製すればよい、なお、基板11にAI等の金
属板を用いれば反射層61は省略してもよい。Note that the transparent N-layer 16 can be easily formed on the light-absorbing resin 15 by a method such as spin cord or injection molding. There are no particular limitations on the material and thickness of the transparent case 1171qlG. Also, the transparent protective layer is not necessarily required and may not be formed (although it is acceptable.) Although one embodiment of the present invention has been described in detail based on the drawings, the present invention may be practiced in other ways. For example, as shown in Figure @6, there is A between the substrate 11 and the protective layer 12.
A first reflective layer 61 may be provided, in which case the recording layer 13
The substrate 11 may be made of a material that is thin enough to allow the laser beam to pass through it, or made of a material that is polycrystalline, which increases noise but is highly translucent, such as magnetism. If a plate is used, the reflective layer 61 may be omitted.
第7図のようにガラス等の基板71上にTa。As shown in FIG. 7, Ta is deposited on a substrate 71 made of glass or the like.
A1′!4?のトラッキング案内115!?2.5iO
z等の平坦化層73、Te、FeOx、TbFeCo等
の記録層74.5i02等の保護層75を順次積層する
。さらに、A1等の反射層あるいは光吸収層76を形成
し、保@M12.記1iJ113.保@I@14.溝付
光吸収性樹脂15.透明保護層16を順次形成してもよ
い。このようにすることで、基板側および光吸収性樹脂
層側の両側から記録、再生を行うことができる。さらに
、第8図のように基板11の両側に記録層13.光吸収
性樹脂15等を形成しても、両側から記録再生すること
ができる。これにより、2枚の光ディスクをはり合わせ
る必要がなく、また、薄(て記録密度の高い光記録媒体
を提供することができる。A1′! 4? Tracking guide 115! ? 2.5iO
A flattening layer 73 such as ZZ, a recording layer 74 such as Te, FeOx, TbFeCo, etc., and a protective layer 75 such as 5i02 are sequentially laminated. Furthermore, a reflective layer or light absorbing layer 76 such as A1 is formed to protect @M12. Note 1iJ113. Ho@I@14. Grooved light-absorbing resin 15. The transparent protective layer 16 may be formed sequentially. By doing so, recording and reproduction can be performed from both the substrate side and the light-absorbing resin layer side. Further, as shown in FIG. 8, recording layers 13 are provided on both sides of the substrate 11. Even if the light-absorbing resin 15 or the like is formed, recording and reproduction can be performed from both sides. Thereby, it is not necessary to bond two optical disks together, and a thin optical recording medium with high recording density can be provided.
また、基板形状はディスクである必要はなく、カード状
でもよい、このとき、光吸収性1#脂の溝は、カードの
一辺に平行あるいは円弧状に形成してもよい。Further, the shape of the substrate does not have to be a disk, but may be a card. In this case, the groove of the light-absorbing 1# resin may be formed parallel to one side of the card or in the shape of an arc.
その他−々例示はしないが、本発明は当業者の知識に基
づいて種々の変更、改良を加えた態様で実施することが
できる。Although other examples are not provided, the present invention can be implemented with various modifications and improvements based on the knowledge of those skilled in the art.
F発明の効果]
以上詳述したことから明らかなように、本発明によれば
、基板上に平坦な記録層を形成し、その上に光吸収性樹
脂を用いてトラッキング用案内溝を形成しており、光吸
収性樹脂側から情報の記録、再生あるいは消去をするよ
うにしているため、プラス、樹脂、金属、セラミック等
を基板として用いることができ、基板の種類を選ばない
、これにより、高速回転に耐えうる転送速度の速い記録
媒体を提供することがでさる。*た、光吸収性樹脂は、
通常の溝付スタンバを用い射出成形や紫外線硬化樹脂を
用いて安価に生産性よく製造できる。F. Effects of the Invention] As is clear from the detailed description above, according to the present invention, a flat recording layer is formed on a substrate, and a tracking guide groove is formed thereon using a light-absorbing resin. Since information is recorded, reproduced, or erased from the light-absorbing resin side, plastics, metals, ceramics, etc. can be used as the substrate, and any type of substrate can be used. It is possible to provide a recording medium that can withstand high-speed rotation and has a high transfer rate. *The light-absorbing resin is
It can be manufactured at low cost and with high productivity using an ordinary grooved stand bar, injection molding, or ultraviolet curing resin.
さらに、記ti屑が平坦であるため、均一な記録特性が
得られると共に膜劣化の原因となる段差部分が生じない
ため、S/Nが向上すると共に信頼性も大幅に向上する
。Furthermore, since the Ti dust is flat, uniform recording characteristics can be obtained and no step portions that cause film deterioration occur, so that the S/N ratio and reliability are significantly improved.
第1図からPJ8図までは本発明を具体化した実施例を
示すもので、第1図は本発明の一実施例である光記録媒
体の要部断面図であり、第2図は第1図の光記録媒体の
作製方法の一例を説明する図であり、第3図は第1図の
光記録媒体においてトラッキングを行うためのビーム配
置を示す説明図であり、第4図は本発明の光記録媒体の
他の作製法の一例を説明する図であり、第5図は本発明
の光記録媒体の光吸収性樹脂の一変形例を示す要部断面
図であり、第6図から第8図までは本発明の光記録媒体
の一変形例を示す要部断面図であり、第9図は従来の光
記録媒体の一例を示す要部断面図である。
11・・・基板、13・・・記録層、15・・・光吸収
性樹脂。1 to PJ8 show embodiments embodying the present invention. FIG. 3 is an explanatory diagram showing a beam arrangement for tracking in the optical recording medium of FIG. 1, and FIG. FIG. 5 is a diagram illustrating an example of another method for manufacturing an optical recording medium, and FIG. 5 is a cross-sectional view of a main part showing a modified example of the light-absorbing resin of the optical recording medium of the present invention, and FIGS. 8 to 8 are main part sectional views showing a modified example of the optical recording medium of the present invention, and FIG. 9 is a main part sectional view showing an example of a conventional optical recording medium. 11... Substrate, 13... Recording layer, 15... Light absorbing resin.
Claims (1)
上に設けられ、案内溝を有する光吸収性の樹脂とから成
ることを特徴とする光記録媒体。 2、請求項1記載の光記録媒体において、前記記録層の
両側あるいは片側に保護層を設けたことを特徴とする光
記録媒体。 3、請求項1記載の光記録媒体において、透明基板と、
その上に同心円あるいは渦巻状に設けられたトラッキン
グ用反射膜と、前記トラッキング用反射膜によって生じ
る凹凸を略平坦とする平坦化層と、前記平坦化層上に設
けられた第1の記録層と、その上に設けられた保護層と
、前記保護層上に設けられた第2の記録層と、前記第2
の記録層上に設けられ案内溝を有する光吸収性の樹脂と
から成ることを特徴とする光記録媒体。Claims: 1. An optical recording medium comprising a substrate, a recording layer provided on the substrate, and a light-absorbing resin provided on the recording layer and having a guide groove. 2. The optical recording medium according to claim 1, further comprising a protective layer provided on both sides or one side of the recording layer. 3. The optical recording medium according to claim 1, comprising: a transparent substrate;
a tracking reflective film provided thereon in a concentric or spiral shape; a flattening layer that substantially flattens unevenness caused by the tracking reflective film; and a first recording layer provided on the flattening layer. , a protective layer provided on the protective layer, a second recording layer provided on the protective layer, and a second recording layer provided on the protective layer.
1. An optical recording medium comprising a light-absorbing resin provided on a recording layer and having a guide groove.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1279211A JPH03141050A (en) | 1989-10-26 | 1989-10-26 | Optical recording medium |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1279211A JPH03141050A (en) | 1989-10-26 | 1989-10-26 | Optical recording medium |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH03141050A true JPH03141050A (en) | 1991-06-17 |
Family
ID=17607981
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1279211A Pending JPH03141050A (en) | 1989-10-26 | 1989-10-26 | Optical recording medium |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH03141050A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5714748A (en) * | 1992-10-02 | 1998-02-03 | Goldstar Co., Ltd. | Magnetic cards employing optical recording material |
JP2001284712A (en) * | 2000-03-29 | 2001-10-12 | Pioneer Electronic Corp | Distribution feedback ridge type semiconductor laser |
JP2002117585A (en) * | 2000-06-09 | 2002-04-19 | Tdk Corp | Optical information medium |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58146042A (en) * | 1982-02-25 | 1983-08-31 | Matsushita Electric Ind Co Ltd | Photomagnetic recording medium |
JPS6085450A (en) * | 1983-10-14 | 1985-05-14 | Sanyo Electric Co Ltd | Optical recording disc |
-
1989
- 1989-10-26 JP JP1279211A patent/JPH03141050A/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58146042A (en) * | 1982-02-25 | 1983-08-31 | Matsushita Electric Ind Co Ltd | Photomagnetic recording medium |
JPS6085450A (en) * | 1983-10-14 | 1985-05-14 | Sanyo Electric Co Ltd | Optical recording disc |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5714748A (en) * | 1992-10-02 | 1998-02-03 | Goldstar Co., Ltd. | Magnetic cards employing optical recording material |
JP2001284712A (en) * | 2000-03-29 | 2001-10-12 | Pioneer Electronic Corp | Distribution feedback ridge type semiconductor laser |
JP2002117585A (en) * | 2000-06-09 | 2002-04-19 | Tdk Corp | Optical information medium |
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