JPH08147757A - Information recording medium and its reproducing method - Google Patents
Information recording medium and its reproducing methodInfo
- Publication number
- JPH08147757A JPH08147757A JP6280204A JP28020494A JPH08147757A JP H08147757 A JPH08147757 A JP H08147757A JP 6280204 A JP6280204 A JP 6280204A JP 28020494 A JP28020494 A JP 28020494A JP H08147757 A JPH08147757 A JP H08147757A
- Authority
- JP
- Japan
- Prior art keywords
- film
- recording medium
- laser beam
- light
- information recording
- 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
- 238000000034 method Methods 0.000 title claims description 20
- 239000000758 substrate Substances 0.000 claims abstract description 25
- 230000002093 peripheral effect Effects 0.000 claims abstract description 13
- 230000003287 optical effect Effects 0.000 claims description 52
- 238000002834 transmittance Methods 0.000 claims description 9
- 125000005678 ethenylene group Chemical group [H]C([*:1])=C([H])[*:2] 0.000 claims description 3
- 230000009021 linear effect Effects 0.000 claims description 3
- 238000002310 reflectometry Methods 0.000 abstract description 2
- 238000001514 detection method Methods 0.000 abstract 1
- 238000010586 diagram Methods 0.000 description 11
- 230000000694 effects Effects 0.000 description 11
- 239000000463 material Substances 0.000 description 6
- 239000011347 resin Substances 0.000 description 6
- 229920005989 resin Polymers 0.000 description 6
- 229910004298 SiO 2 Inorganic materials 0.000 description 4
- 238000004364 calculation method Methods 0.000 description 4
- 239000013078 crystal Substances 0.000 description 4
- 239000000126 substance Substances 0.000 description 4
- YMWUJEATGCHHMB-UHFFFAOYSA-N Dichloromethane Chemical compound ClCCl YMWUJEATGCHHMB-UHFFFAOYSA-N 0.000 description 3
- 230000001681 protective effect Effects 0.000 description 3
- 230000005684 electric field Effects 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 230000001678 irradiating effect Effects 0.000 description 2
- 239000010410 layer Substances 0.000 description 2
- 230000010287 polarization Effects 0.000 description 2
- 239000004417 polycarbonate Substances 0.000 description 2
- 229920000515 polycarbonate Polymers 0.000 description 2
- 230000004044 response Effects 0.000 description 2
- WGTYBPLFGIVFAS-UHFFFAOYSA-M tetramethylammonium hydroxide Chemical compound [OH-].C[N+](C)(C)C WGTYBPLFGIVFAS-UHFFFAOYSA-M 0.000 description 2
- LXWZQZDNCPHJIE-UHFFFAOYSA-N C[SH+]C.[Cl-].C[SH+]C.[Cl-] Chemical compound C[SH+]C.[Cl-].C[SH+]C.[Cl-] LXWZQZDNCPHJIE-UHFFFAOYSA-N 0.000 description 1
- QGJOPFRUJISHPQ-UHFFFAOYSA-N Carbon disulfide Chemical compound S=C=S QGJOPFRUJISHPQ-UHFFFAOYSA-N 0.000 description 1
- 239000004593 Epoxy Substances 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 239000007864 aqueous solution Substances 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 229910010293 ceramic material Inorganic materials 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 229920001940 conductive polymer Polymers 0.000 description 1
- 238000013500 data storage Methods 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 230000006870 function Effects 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 238000003384 imaging method Methods 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- GBMDVOWEEQVZKZ-UHFFFAOYSA-N methanol;hydrate Chemical compound O.OC GBMDVOWEEQVZKZ-UHFFFAOYSA-N 0.000 description 1
- 239000011259 mixed solution Substances 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 229940028444 muse Drugs 0.000 description 1
- 230000009022 nonlinear effect Effects 0.000 description 1
- 229920003229 poly(methyl methacrylate) Polymers 0.000 description 1
- 229920000015 polydiacetylene Polymers 0.000 description 1
- 239000002861 polymer material Substances 0.000 description 1
- 238000006116 polymerization reaction Methods 0.000 description 1
- 239000004926 polymethyl methacrylate Substances 0.000 description 1
- 239000002244 precipitate Substances 0.000 description 1
- GMVPRGQOIOIIMI-DWKJAMRDSA-N prostaglandin E1 Chemical compound CCCCC[C@H](O)\C=C\[C@H]1[C@H](O)CC(=O)[C@@H]1CCCCCCC(O)=O GMVPRGQOIOIIMI-DWKJAMRDSA-N 0.000 description 1
- 239000011241 protective layer Substances 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 238000004528 spin coating Methods 0.000 description 1
- 238000003756 stirring Methods 0.000 description 1
- JOXIMZWYDAKGHI-UHFFFAOYSA-M toluene-4-sulfonate Chemical compound CC1=CC=C(S([O-])(=O)=O)C=C1 JOXIMZWYDAKGHI-UHFFFAOYSA-M 0.000 description 1
Landscapes
- Optical Record Carriers And Manufacture Thereof (AREA)
- Optical Recording Or Reproduction (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は情報記録媒体及びその再
生方法に係り、特にレーザ光を用いて情報を再生する書
き換え型、追記型あるいは再生専用型の情報記録媒体及
びその再生方法に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an information recording medium and a reproducing method thereof, and more particularly to a rewritable, write-once or read-only information recording medium for reproducing information using a laser beam and a reproducing method thereof.
【0002】[0002]
【従来の技術】図9は従来の情報記録媒体及びその再生
方法の一例を説明する図である。同図(B)に示すよう
に、この従来の情報記録媒体1は円盤状の透明基板2上
にレジスト3、反射膜4及び紫外線硬化樹脂5が順次に
積層された構成とされており、レジスト3に記録情報に
応じて断続するピットの列、すなわち凹部と凸部の繰り
返しが形成された、コンパクトディスク−リード・オン
リ・メモリ(CD−ROM)などの再生専用型の光ディ
スクである。2. Description of the Related Art FIG. 9 is a diagram for explaining an example of a conventional information recording medium and a reproducing method thereof. As shown in FIG. 1B, this conventional information recording medium 1 has a structure in which a resist 3, a reflective film 4 and an ultraviolet curable resin 5 are sequentially laminated on a disk-shaped transparent substrate 2, 3 is a read-only type optical disc such as a compact disc-read only memory (CD-ROM) in which a row of pits intermittently formed in accordance with the recorded information, that is, a concave portion and a convex portion are formed repeatedly.
【0003】この従来の情報記録媒体1の既記録情報の
再生時には、図9(B)に示すように、光学ヘッド6内
の対物レンズ7によりレーザ光源(図示せず)よりのレ
ーザビーム8を透明基板2を介してレジスト3に合焦す
る。これにより、反射膜4には図9(A)に示す如く直
径Dで、光軸に垂直な面に対してガウシアン分布を示す
光強度の光スポットが形成される。この光スポットの反
射光の光強度がレジスト3の凹部と凸部とで変化するた
め、この反射光の光強度の変化を検出することにより、
既記録情報を再生することができる。At the time of reproducing already recorded information on the conventional information recording medium 1, as shown in FIG. 9B, a laser beam 8 from a laser light source (not shown) is emitted by an objective lens 7 in an optical head 6. The resist 3 is focused through the transparent substrate 2. As a result, a light spot having a diameter D and a light intensity having a Gaussian distribution is formed on the surface perpendicular to the optical axis on the reflective film 4 as shown in FIG. 9A. Since the light intensity of the reflected light of this light spot changes between the concave portion and the convex portion of the resist 3, by detecting the change of the light intensity of this reflected light,
The recorded information can be reproduced.
【0004】このような情報記録媒体1では、近年ます
ます高密度化が要求されており、そのための技術の一つ
として光スポットの直径(スポット径)Dを小さくする
技術が従来より知られている。例えば、光源からの光を
平行光にした後、この光路中に遮蔽板あるいはV字形の
プリズムを置くことで、光ディスク上には回折パターン
が現れ、中央に現れるスポット径は光源の波長で決まる
スポット径よりも20%小さくなり、記録密度が1.5
倍となる超解像ヘッド技術がある。In the information recording medium 1 as described above, higher density has been demanded in recent years, and as one of the techniques therefor, a technique for reducing the diameter (spot diameter) D of the light spot has been conventionally known. There is. For example, if the light from the light source is collimated and then a shield plate or a V-shaped prism is placed in this optical path, a diffraction pattern appears on the optical disc, and the spot diameter appearing in the center is a spot determined by the wavelength of the light source. 20% smaller than the diameter, recording density 1.5
There is double the super-resolution head technology.
【0005】この超解像ヘッド技術を用いた情報記録媒
体として、光磁気ディスクやMUSE方式レーザディス
ク用の光ディスクについて次の文献1〜文献3に記載が
ある。ここで文献1:”High Density Optical Recordi
ng by Superresolution",International Symposium on
Optical Memory 1989 Technical Digest,27D-17,pp.99-
100,Sept.1989。文献2:「超解像光ヘッドによる高密
度光磁気ディスクの再生C/N特性」,『第39回応用
物理学関係連合講演会講演予稿集No.3』,31p-L-6,
p.1002,1992年3月。文献3:"High Density Video Disc Us
ing Superresolution and Green Laser",International
Symposium on Optical Memory and Optical Data Stor
age '93,Tul.4,July 1993。As an information recording medium using this super-resolution head technology, optical discs for magneto-optical discs and MUSE type laser discs are described in the following documents 1 to 3. Here Document 1: "High Density Optical Recordi
ng by Superresolution ", International Symposium on
Optical Memory 1989 Technical Digest, 27D-17, pp.99-
100, Sept. 1989. Reference 2: “Reproduction C / N Characteristics of High Density Magneto-Optical Disk with Super-Resolution Optical Head”, Proceedings of the 39th Joint Lecture in Applied Physics, No. 3 ”, 31p-L-6,
p.1002, March 1992. Reference 3: "High Density Video Disc Us
ing Superresolution and Green Laser ", International
Symposium on Optical Memory and Optical Data Stor
age '93, Tul.4, July 1993.
【0006】また、従来の情報記録媒体には位相差を利
用して既記録情報が再生される光媒体があり、そのピッ
ト形成記録媒体として、Pb−Te−Se膜(M.Terao,
et al.:J.Appl.Phys.,62(3),1029(1987).)、Te−T
i−Ag−Se膜、Te−C膜(市原勝太郎、大川秀
樹:エレクトロニク・セラミックス,11月号,p.5(19
87). M/Mashita,N.Yasuda:Proc.SPIE,329,p190(198
2).)、CS2−Te膜(H.Yamazaki,et al.:Rev.Elect
r.Commun.Lab.,32,260(1984))が知られている。また、
有機記録膜として、特開昭62−119755号公報に
開示された技術がすでに商品化されている。In addition, there is an optical medium in which already recorded information is reproduced by utilizing a phase difference as a conventional information recording medium, and a Pb-Te-Se film (M. Terao,
et al .: J. Appl. Phys., 62 (3), 1029 (1987)., Te-T.
i-Ag-Se film, Te-C film (Katsutaro Ichihara, Hideki Okawa: Electronic Ceramics, November issue, p.5 (19)
87) .M / Mashita, N.Yasuda: Proc.SPIE, 329, p190 (198
2).), CS2-Te film (H. Yamazaki, et al .: Rev. Elect
r.Commun.Lab., 32, 260 (1984)) is known. Also,
As the organic recording film, the technology disclosed in Japanese Patent Laid-Open No. 62-119755 has already been commercialized.
【0007】更に、光スポット径を小さくすることによ
り記録密度を高密度化する従来の情報記録媒体として、
低照度の光ビームに対しては光透過率が低く、高照度の
光ビームに対しては光透過率が高くなる光透過率特性を
有する光制御膜を、透明基板と記録膜又は反射膜との間
に設けた情報記録媒体も従来より知られている(特開平
6−44609号公報)。Further, as a conventional information recording medium for increasing the recording density by reducing the light spot diameter,
A transparent substrate and a recording film or a reflective film having a light control film having a light transmittance characteristic that the light transmittance is low for a light beam of low illuminance and high for a light beam of high illuminance. An information recording medium provided between the two is also conventionally known (JP-A-6-44609).
【0008】[0008]
【発明が解決しようとする課題】しかるに、上記の位相
差を利用して再生信号を得る従来の情報記録媒体におい
ては、超解像光学系の再生ビームの回折パターン中心部
のメインローブ成分と回折パターン円周部のサイドロー
ブ成分とが媒体面上のピット(記録部)により位相変調
を受けることで、メインローブ成分とサイドローブ成分
とが干渉し合い、再結像点でのビームプロファイルが変
化してピンホールやスリット通過後の再生信号に位相パ
ターン依存性のあるエッジシフトが起こるため、再生信
号に歪みが生じ、ジッタ値が増加するという問題点があ
る。However, in the conventional information recording medium for obtaining a reproduction signal by utilizing the above-mentioned phase difference, the main lobe component of the reproduction beam center of the reproduction beam of the super-resolution optical system and the diffraction The side lobe component of the pattern circumference is subjected to phase modulation by the pit (recording part) on the medium surface, and the main lobe component and side lobe component interfere with each other, and the beam profile at the re-imaging point changes. Then, the reproduced signal after passing through the pinhole or the slit undergoes an edge shift having a phase pattern dependence, so that the reproduced signal is distorted and the jitter value increases.
【0009】また、上記の光制御膜を設けた従来の情報
記録媒体においては、光制御膜が光ビームの照度に応じ
て光透過率が変化するため、反射光の光量が減少し、再
生信号の劣化が生じ、また、トラックサーボがかかりに
くいという欠点を有する。Further, in the conventional information recording medium provided with the above-mentioned light control film, the light control film changes the light transmittance according to the illuminance of the light beam, so that the light amount of the reflected light is reduced and the reproduction signal is reproduced. Is deteriorated and the track servo is hard to be applied.
【0010】本発明は以上の点に鑑みなされたもので、
再生時のサイドローブ成分のメインローブ成分への影響
を減少し、かつ、反射光中心と周辺部分とで光量変化の
無い情報記録媒体及びその再生方法を提供することを目
的とする。The present invention has been made in view of the above points,
An object of the present invention is to provide an information recording medium which reduces the influence of the side lobe component on the main lobe component at the time of reproduction and has no change in the light amount between the center of the reflected light and the peripheral portion and a reproducing method thereof.
【0011】[0011]
【課題を解決するための手段】上記の目的を達成するた
め本発明の情報記録媒体は、透明基板上方の記録膜の形
状変化若しくは特性変化を利用して情報をレーザビーム
により記録し、これを再生する書き換え型、追記型の光
学的情報記録媒体、あるいは形状変化により記録膜に記
録されている情報をレーザビームにより再生する再生専
用型の光学的情報記録媒体において、透明基板と記録膜
との間に、所定光強度より大なる光強度の前記レーザビ
ームに対する屈折率の変化が、所定光強度以下の光強度
のレーザビームに対する屈折率の変化が大である、少な
くとも一層以上の非線形屈折率特性を有する光調整膜を
設けたものである。In order to achieve the above object, the information recording medium of the present invention records information by a laser beam by utilizing the shape change or the characteristic change of the recording film above the transparent substrate, In a rewritable or write-once type optical information recording medium for reproduction, or a reproduction-only type optical information recording medium for reproducing information recorded on a recording film due to a change in shape, a transparent substrate and a recording film are used. In the meantime, the change in the refractive index with respect to the laser beam having a light intensity higher than the predetermined light intensity is large, and the change in the refractive index with respect to the laser beam having the light intensity less than or equal to the predetermined light intensity is large. Is provided with a light adjusting film.
【0012】また、本発明の光調整膜は、次式The light control film of the present invention has the following formula:
【0013】[0013]
【化2】 で表されるポリ−(2、5−チェニレンビニレン)を用
いることが、使用波長範囲が広く、高速応答性を有し、
かつ、動作入力光強度が小さいので実用に供して望まし
い。Embedded image The use of poly- (2,5-chenylene vinylene) represented by the following has a wide wavelength range to be used and has high-speed response,
Moreover, since the operation input light intensity is low, it is desirable for practical use.
【0014】また、本発明の情報記録媒体の再生方法で
は、透明基板上方の情報面上の記録膜の形状変化若しく
は特性変化を利用して記録された情報をレーザビームに
より再生する書き換え型、追記型の光学的情報記録媒
体、あるいは形状変化により記録膜に記録されている情
報をレーザビームにより再生する再生専用型の光学的情
報記録媒体の再生方法において、透明基板と記録膜との
間に設けられた上記の光調整膜により、再生時に記録膜
の形状変化若しくは特性変化により生じる、反射率、吸
収率、透過率及び記録部と未記録部の位相差とを調整
し、光調整膜が情報面の焦点深度内に位置するようにし
て再生することにより、上記の目的を達成する。Further, in the reproducing method of the information recording medium of the present invention, the rewritable type, the additional recording in which the information recorded by utilizing the shape change or the characteristic change of the recording film on the information surface above the transparent substrate is reproduced by the laser beam. Type optical information recording medium or a read-only type optical information recording medium for reproducing information recorded on a recording film by a shape change by a laser beam, the method is provided between a transparent substrate and a recording film. The above-mentioned light adjusting film adjusts the reflectance, the absorptance, the transmittance, and the phase difference between the recorded portion and the unrecorded portion, which are caused by the shape change or the characteristic change of the recording film during reproduction, and The above-mentioned object is achieved by reproducing the image data so as to be positioned within the depth of focus of the surface.
【0015】[0015]
【作用】本発明では、非線形光学効果の一つである非線
形屈折率効果を有する光調整膜を透明基板と記録膜との
間に設けることにより、記録レーザビームのスポット径
を実質的に小径化することができ、また、超解像光学系
による再生時のサイドローブ成分のメインローブ成分へ
の影響を大幅に減少させることができる。In the present invention, the spot diameter of the recording laser beam is substantially reduced by providing the light adjusting film having the nonlinear refractive index effect, which is one of the nonlinear optical effects, between the transparent substrate and the recording film. Further, it is possible to significantly reduce the influence of the side lobe component on the main lobe component at the time of reproduction by the super-resolution optical system.
【0016】ここで、上記の非線形光学効果とは、物質
に光が入射した時の当該物質の電気分極を、次の一般式 χ(1)E+χ(2)E2+χ(3)E3+・・・ で表したときに、第2項以降で表される効果をいう。こ
こで、χ(i)はi次の電気感受率、Eは光の電界強度で
ある。特に、第2項による第2次高調波発生(SHG)
や第3項による第3次高調波発生(THG)は変換効果
としてよく知られているが、第3項はまた、光強度に応
じた光学定数の変化、例えば非線形屈折率効果や非線形
吸収効果を与えるものとして重要である。例えば、非線
形屈折率効果は物質の屈折率nが入射光強度に比例して
変化するものであり、n=n0+n2Iで記述される。こ
こで、n0は定数、n2は非屈折率係数である。Here, the above-mentioned nonlinear optical effect means the electric polarization of a substance when light is incident on the substance, which is expressed by the following general formula χ (1) E + χ (2) E 2 + χ (3) E 3 + When expressed by ..., it means the effect expressed by the second and subsequent terms. Here, χ (i) is the i-th order electric susceptibility, and E is the electric field intensity of light. In particular, second harmonic generation (SHG) according to the second term
The third harmonic generation (THG) by the third term and the third term is well known as the conversion effect, but the third term also changes the optical constant according to the light intensity, such as the nonlinear refractive index effect and the nonlinear absorption effect. Is important as giving. For example, the nonlinear refractive index effect is such that the refractive index n of a substance changes in proportion to the incident light intensity, and is described by n = n 0 + n 2 I. Here, n 0 is a constant and n 2 is a non-refractive index coefficient.
【0017】次に、光調整膜の作用について説明する。
情報記録媒体に適用される記録・再生用光ビームとして
は、一般的にレーザビームが用いられる。レーザビーム
の光強度分布は、前記したように光軸に垂直な面に対し
てガウシアン分布になっており、中心部が強く、周辺部
に至るに従って弱くなる。かかる光強度分布を有するレ
ーザビームを、情報記録媒体の情報面の焦点深度内に前
記非線形屈折率効果を有する光調整膜が設けられた情報
記録媒体に透明基板側から照射すると、前記所定光強度
以下の低照度レーザビームが照射されている周辺部は屈
折率の変化を殆ど発生しないため、光調整膜の膜厚調整
により記録部と未記録部の位相差が無くなり、再生信号
として検出されなくなり、中央部の前記所定光強度より
大なる高照度のレーザビームが照射されている光調整膜
のみが屈折率変化を生じ、記録部と未記録部に反射率と
位相差が発生し、再生信号として検出が可能となる。こ
のような作用は反射率差あるいは位相差を用いて再生を
行うすべての情報記録媒体にあてはまる。Next, the function of the light adjusting film will be described.
A laser beam is generally used as the recording / reproducing light beam applied to the information recording medium. As described above, the light intensity distribution of the laser beam is a Gaussian distribution with respect to the plane perpendicular to the optical axis, and the central portion is strong and becomes weaker toward the peripheral portion. When the laser beam having such a light intensity distribution is irradiated from the transparent substrate side to the information recording medium provided with the light adjusting film having the nonlinear refractive index effect within the depth of focus of the information surface of the information recording medium, the predetermined light intensity is obtained. Since the peripheral part irradiated with the following low illuminance laser beam hardly changes the refractive index, the phase difference between the recorded part and the unrecorded part is eliminated by adjusting the film thickness of the light adjustment film, and it is no longer detected as a reproduction signal. , A refractive index change occurs only in the light adjustment film irradiated with a laser beam having a high illuminance higher than the predetermined light intensity in the central portion, and a reflectance and a phase difference occur between a recorded portion and an unrecorded portion, and a reproduction signal Can be detected as. Such an action is applicable to all information recording media that are reproduced by using the reflectance difference or the phase difference.
【0018】つぎに、光調整膜を有する情報記録媒体を
超解像光学系で再生したときの作用について説明する。
光ヘッド内の対物レンズの中心部を遮光するか、あるい
は対物レンズの中心部を透過する光の位相を対物レンズ
の周辺部を透過する光の位相よりも早めると、記録膜又
は反射膜上に合焦されるレーザビームの半値幅径を小さ
くすることができる。Next, the operation when the information recording medium having the light adjusting film is reproduced by the super-resolution optical system will be described.
If the central part of the objective lens in the optical head is shielded or the phase of the light passing through the central part of the objective lens is made earlier than the phase of the light passing through the peripheral part of the objective lens, the recording film or the reflective film will be The half-width diameter of the focused laser beam can be reduced.
【0019】このようにして小径化されたレーザビーム
を前記光調整膜を有する本発明情報記録媒体に照射する
ことによって、記録膜又は反射膜上に照射されるスポッ
ト径のより一層の小径化を達成できる。なお、対物レン
ズ中心を遮光するか、あるいは対物レンズ中心部を透過
する光の位相を対物レンズの周辺部を透過する光の位相
よりも早めると、小径化されたメインローブの周辺にサ
イドローブが発生するが、サイドローブの光強度はメイ
ンローブの光強度に比べて格段に小さいので、光調整膜
に屈折率変化が実質的に発生しない。By irradiating the information recording medium of the present invention having the above-mentioned light adjusting film with the laser beam thus reduced in diameter, the spot diameter irradiated on the recording film or the reflective film can be further reduced. Can be achieved. If the center of the objective lens is shielded or the phase of the light passing through the center of the objective lens is made earlier than the phase of the light passing through the peripheral part of the objective lens, side lobes will appear around the reduced main lobe. Although generated, the light intensity of the side lobes is much smaller than the light intensity of the main lobes, so that the refractive index change does not substantially occur in the light adjustment film.
【0020】[0020]
【実施例】次に、本発明の各実施例について説明する。
図1は本発明になる情報記録媒体及びその再生方法の第
1実施例の説明図を示す。同図中、図9と同一構成部分
には同一符号を付してある。図1(B)の断面図に示す
ように、本実施例の情報記録媒体10は、透明基板2上
に光調整膜11、記録膜12、反射膜4及び紫外線硬化
樹脂5が順次に積層された構成であり、前記レジスト3
に相当する記録膜12に記録情報に応じて断続するピッ
トの列、すなわち凹部と凸部の繰り返しが形成された再
生専用型の光ディスクである。EXAMPLES Next, examples of the present invention will be described.
FIG. 1 shows an explanatory diagram of a first embodiment of an information recording medium and a reproducing method thereof according to the present invention. In the figure, the same components as those in FIG. 9 are designated by the same reference numerals. As shown in the cross-sectional view of FIG. 1B, in the information recording medium 10 of this embodiment, a light adjusting film 11, a recording film 12, a reflecting film 4 and an ultraviolet curable resin 5 are sequentially laminated on a transparent substrate 2. And the resist 3
Is a read-only type optical disc in which a row of pits intermittently formed according to the recording information, that is, a concave portion and a convex portion are formed on the recording film 12 corresponding to the above.
【0021】透明基板2は、例えばガラスなどの透明セ
ラミックや、ポリカーボネート、ポリメチルメタアクリ
レート、ポリネチルペンテン、エポキシなどの透明樹脂
材料を用いて、ディスク状あるいはカード状などの所望
の形状に形成されるが、ここでは一例としてディスク状
であるものとしている。The transparent substrate 2 is formed in a desired shape such as a disk shape or a card shape by using a transparent ceramic material such as glass or a transparent resin material such as polycarbonate, polymethylmethacrylate, polynetylpentene or epoxy. However, here, as an example, it is assumed that it is disk-shaped.
【0022】光調整膜11は、図2に示すように、光強
度Ib以下の低照度のレーザビームに対する屈折率の変
化が、光強度Ibより大なる高照度のレーザビームに対
する屈折率の変化よりも低い非線形屈折率特性を有す
る。このような非線形屈折率特性を有する光調整膜11
としては、前記の化1で示した式で表されるポリ−
(2、5−チェニレンビニレン)(略称PTV)や、分
子回転非線形効果(光電界に応じた分子の回転配列によ
り屈折率が光強度依存性を示す)を作動原理とする非線
形光学液体の二硫化炭素(CS2)を満たしたガラスセ
ル、非線形屈折率効果が純粋に電子分極に由来するポリ
ジアセチレンビスー(パラトルエンスルホネート)(略
称PTS)などが存在する。As shown in FIG. 2, the light adjusting film 11 has a change in the refractive index with respect to a laser beam with a low illuminance equal to or lower than the light intensity Ib from a change in the refractive index with respect to a laser beam with a high illuminance greater than the light intensity Ib. Also has a low nonlinear refractive index characteristic. Light adjusting film 11 having such a nonlinear refractive index characteristic
Is a poly-represented by the formula shown in Chemical Formula 1 above.
(2,5-Chenylene vinylene) (abbreviated as PTV) and two types of non-linear optical liquids whose working principle is a molecular rotation non-linear effect (refractive index shows light intensity dependence due to rotational arrangement of molecules according to optical electric field). There are glass cells filled with carbon sulfide (CS 2 ), polydiacetylene bis- (paratoluene sulfonate) (abbreviated as PTS) whose nonlinear refractive index effect is purely derived from electronic polarization, and the like.
【0023】特に、PTVはアモルファス構造を持つ導
電性ポリマ材料として既に知られており、使用波長範囲
が広く、高速応答性を有し、かつ、動作入力光強度が小
さい実用に供し得る高性能非線形光学材料で、光調整膜
11に適している。In particular, PTV is already known as a conductive polymer material having an amorphous structure, has a wide wavelength range to be used, has a high-speed response, and has a small operating input light intensity, and is a high-performance nonlinear material that can be put to practical use. It is an optical material and is suitable for the light adjusting film 11.
【0024】次に、PTVによる光調整膜11の作成方
法について説明する。まず、2,5−チェニレンビス
(ジメチルスルホニウム)ジクロライドを0℃条件下で
アルカリ水溶液で処理した後、メタノール−水混合溶液
中で0.3モルのテトラメチル水酸化アンモニウムを加
え、−30℃条件下で攪拌しポリマ化した。得られた黄
色の沈殿物を採取し、ジクロロメタンに溶解させた後、
これをスピンコーティング法により石英ガラス基板上に
フィルム化し、風乾した。最後にこれを200〜250
℃、5時間、10−2Torrの真空下で加熱すること
により、光学品質に優れたPTV光調整膜11を得るこ
とができる。Next, a method of forming the light adjusting film 11 by PTV will be described. First, 2,5-chenylene bis (dimethylsulfonium) dichloride was treated with an alkaline aqueous solution at 0 ° C., then 0.3 mol of tetramethyl ammonium hydroxide was added in a methanol-water mixed solution, and the mixture was heated at −30 ° C. Polymerization was performed by stirring with. After collecting the obtained yellow precipitate and dissolving it in dichloromethane,
This was formed into a film on a quartz glass substrate by a spin coating method and air dried. Finally this is 200-250
The PTV light adjusting film 11 having excellent optical quality can be obtained by heating at a temperature of 5 ° C. for 5 hours under a vacuum of 10 −2 Torr.
【0025】次に図1(B)に示した記録膜12は、書
換型、追記型、あるいは再生専用型の情報記録媒体の情
報記録層として形成されるものであって、公知に属する
任意の材質からなるものを用いることができる。一方、
反射膜4は書換型、追記型、再生専用型の情報記録媒体
の記録膜面上に積層されるものであって、公知に属する
任意の材質からなるものを用いることができる。Next, the recording film 12 shown in FIG. 1 (B) is formed as an information recording layer of a rewritable, write-once, or read-only type information recording medium, and is any known one. A material made of a material can be used. on the other hand,
The reflection film 4 is laminated on the recording film surface of a rewritable, write-once, and read-only information recording medium, and may be made of any known material.
【0026】この情報記録媒体10の既記録情報の再生
には、図1(B)に示すように、光学ヘッド6内の対物
レンズ7によりレーザ光源(図示せず)よりのレーザビ
ーム8を透明基板2を介して記録膜12又は反射膜4に
合焦する。光学ヘッド6はレーザ光源として半導体レー
ザを備え、オートフォーカス用のアクチュエータを備え
た従来より公知の構成のものがそのまま適用される。To reproduce already recorded information on the information recording medium 10, a laser beam 8 from a laser light source (not shown) is made transparent by an objective lens 7 in the optical head 6 as shown in FIG. 1 (B). The recording film 12 or the reflective film 4 is focused via the substrate 2. The optical head 6 includes a semiconductor laser as a laser light source and has a conventionally known configuration including an actuator for autofocusing, and is applied as it is.
【0027】次に、この情報記録媒体10の既記録情報
の再生動作について説明する。対物レンズ7により回折
限界まで絞られたレーザビーム8は、透明基板2を透過
し光調整膜11を介して記録膜12又は反射膜4上に合
焦される。これにより、反射膜4には図1(A)に示す
如く、光軸に垂直な面に対してガウシアン分布を示す光
強度の光スポットが形成される。この光スポットの反射
光の光強度が記録膜12の凹部と凸部とで変化するた
め、この反射光の光強度の変化を検出することにより、
既記録情報を再生することができる。Next, the reproducing operation of the recorded information on the information recording medium 10 will be described. The laser beam 8 narrowed down to the diffraction limit by the objective lens 7 passes through the transparent substrate 2 and is focused on the recording film 12 or the reflective film 4 via the light adjusting film 11. As a result, as shown in FIG. 1A, a light spot having a light intensity showing a Gaussian distribution is formed on the surface perpendicular to the optical axis on the reflective film 4. Since the light intensity of the reflected light of the light spot changes between the concave portion and the convex portion of the recording film 12, by detecting the change of the light intensity of the reflected light,
The recorded information can be reproduced.
【0028】ここで、前記したように、光調整膜11は
光強度がIb以下の低照度レーザビームに対しては屈折
率の変化が小さいため、レーザビーム8の周辺部の光強
度がIb以下の部分は光調整膜11の屈折率に対して実
質的に影響を及ぼさない。一方、レーザビーム8の中央
部の光強度がIbより大なる部分は、光調整膜11の屈
折率を高めた後、記録膜12又は反射膜4に達する。As described above, since the light adjusting film 11 has a small change in the refractive index with respect to the low illuminance laser beam having the light intensity of Ib or less, the light intensity of the peripheral portion of the laser beam 8 is Ib or less. The portion does not substantially affect the refractive index of the light adjustment film 11. On the other hand, the portion of the central portion of the laser beam 8 where the light intensity is higher than Ib reaches the recording film 12 or the reflecting film 4 after increasing the refractive index of the light adjusting film 11.
【0029】光調整膜11の屈折率変化によって情報記
録媒体10の光学特性(反射率、吸収率、透過率、位
相)が光強度Ibを境界として変化する。従って、予め
情報記録媒体10の光学設計条件を光調整膜11の屈折
率変化のない状態において記録部(例えば凹部)と未記
録部(例えば凸部)との光学特性(反射率、吸収率、透
過率、位相)がほぼ同等となるように設定し、かつ、光
調整膜11の屈折率変化が発生した状態で、光学特性
(反射率、吸収率、透過率、位相)に違いが生じるよう
に設定しておくことにより、光強度Ibより大である範
囲の光調整膜11を透過した光により再生信号が検出可
能となる。Due to the change in the refractive index of the light adjusting film 11, the optical characteristics (reflectance, absorptance, transmittance, phase) of the information recording medium 10 change with the light intensity Ib as a boundary. Therefore, the optical characteristics (reflectance, absorptivity, etc.) of the recorded portion (for example, the concave portion) and the unrecorded portion (for example, the convex portion) are set in advance in the optical design condition of the information recording medium 10 in a state where the refractive index of the light adjustment film 11 does not change. The optical characteristics (reflectance, absorptance, transmittance, phase) may be different under the condition that the transmittance and the phase are set to be almost equal and the refractive index of the light adjusting film 11 is changed. By setting to 1, the reproduction signal can be detected by the light that has passed through the light adjustment film 11 in the range having the light intensity Ib higher.
【0030】従って、再生信号の検出が可能となる光強
度がIbより大である光スポット部分は、図1(A)に
示したようにスポット径がD2であり、実際の光スポッ
ト径のD1よりも小径の範囲で再生信号の検出ができ、
スポット径を小径化したのと同等の効果が得られる。こ
れにより、従来よりも高密度に記録された情報記録媒体
に対しても、既記録情報を再生することができる。Therefore, the light spot portion having a light intensity higher than Ib at which the reproduction signal can be detected has a spot diameter D2 as shown in FIG. 1A, and the actual light spot diameter D1. It is possible to detect the reproduced signal in the range of smaller diameter than
An effect equivalent to that of reducing the spot diameter can be obtained. As a result, it is possible to reproduce already recorded information even on an information recording medium that is recorded at a higher density than before.
【0031】次に、本発明の第2実施例について説明す
る。図3は本発明になる情報記録媒体及びその再生方法
の第1実施例の説明図を示す。同図中、図1と同一構成
部分には同一符号を付し、その説明を省略する。図3
(B)の断面図に示すように、本実施例の情報記録媒体
10は、図1(B)に示した情報記録媒体10と同一構
造の再生専用型の光ディスクである。Next, a second embodiment of the present invention will be described. FIG. 3 shows an explanatory diagram of a first embodiment of an information recording medium and a reproducing method thereof according to the present invention. In the figure, the same components as those in FIG. 1 are designated by the same reference numerals, and their description will be omitted. FIG.
As shown in the sectional view of (B), the information recording medium 10 of the present embodiment is a read-only type optical disc having the same structure as the information recording medium 10 shown in FIG. 1 (B).
【0032】本実施例は再生方法が第1実施例と異な
る。すなわち、本実施例は、光学ヘッド13が対物レン
ズ7の光入射側の中央部に、不透明な遮光板14を配置
した構成である点に特徴がある。このように、対物レン
ズ7の光入射側の中央部に遮光板14を披着してレーザ
ビーム8を遮光すると、記録膜12又は反射膜4に合焦
するレーザビーム8の光強度分布として、図3(A)に
実線で示すように、遮光板14が設けられていない場合
の同図(A)に破線で示す光強度分布よりもスポット径
がD3で示すように小さなメインローブ8aが対物レン
ズ7の中心部を通る光軸上に形成され、また、その周辺
部にメインローブ8aよりも光強度が小さなサイドロー
ブ8b及び8cが発生する。The reproducing method of this embodiment is different from that of the first embodiment. That is, the present embodiment is characterized in that the optical head 13 has a configuration in which the opaque light shielding plate 14 is arranged at the center of the objective lens 7 on the light incident side. In this way, when the light shield plate 14 is attached to the center of the objective lens 7 on the light incident side to shield the laser beam 8, the light intensity distribution of the laser beam 8 focused on the recording film 12 or the reflective film 4 becomes As shown by the solid line in FIG. 3A, the main lobe 8a having a smaller spot diameter D3 than the light intensity distribution shown by the broken line in FIG. Side lobes 8b and 8c, which are formed on the optical axis passing through the center of the lens 7 and have a light intensity smaller than that of the main lobe 8a, are generated in the peripheral portion.
【0033】従って、メインローブ8aのピーク値より
も低く、サイドローブ8b及び8cのピーク値よりも高
い光強度をしきい値Ibとする光調整膜11を透明基板
2と記録膜12との間に設けた情報記録媒体10を用い
ることにより、前記した光調整膜11の非線形屈折率効
果と情報記録媒体の光学設計の効果により、記録膜12
又は反射膜4上に照射されるスポット径をより一層小径
化することができ、第1実施例よりもなお一層の高密度
化が可能となる。Therefore, a light adjusting film 11 having a threshold Ib which is lower than the peak value of the main lobe 8a and higher than the peak values of the side lobes 8b and 8c is provided between the transparent substrate 2 and the recording film 12. By using the information recording medium 10 provided in the recording film 12, the recording film 12 can be formed by the non-linear refractive index effect of the light adjusting film 11 and the optical design effect of the information recording medium.
Alternatively, the diameter of the spot irradiated on the reflection film 4 can be further reduced, and the density can be further increased as compared with the first embodiment.
【0034】次に、本発明の情報記録媒体の第2実施例
について説明する。図4は本発明になる情報記録媒体の
第2実施例を従来の情報記録媒体の一例と対比して示す
断面図である。同図(A)は本発明の情報記録媒体の第
2実施例の断面図で、情報記録媒体20は透明基板21
上に、光調整膜22、下地保護膜23、記録膜24、光
干渉保護膜25、反射膜26及び紫外線硬化樹脂27が
順次に積層された構造である。Next, a second embodiment of the information recording medium of the present invention will be described. FIG. 4 is a sectional view showing a second embodiment of the information recording medium according to the present invention in comparison with an example of a conventional information recording medium. FIG. 1A is a sectional view of the second embodiment of the information recording medium of the present invention, in which the information recording medium 20 is a transparent substrate 21.
It has a structure in which a light adjustment film 22, a base protection film 23, a recording film 24, a light interference protection film 25, a reflection film 26, and an ultraviolet curable resin 27 are sequentially laminated on top.
【0035】本実施例は図4(B)に示す従来の情報記
録媒体と比較すると、透明基板21と下地保護膜23と
の間に光調整膜22が設けられている点に特徴がある。
本実施例は記録膜23に情報を相状態の変化として記録
する、書き換え型の一例の相変化型情報記録媒体で、例
えば透明基板21がポリカーボネートにより1.2mm
の膜厚で、光調整膜22はPTVにより50nmの膜厚
で、下地保護膜23はZnS−SiO2により140n
mの膜厚で、記録膜24はGe2Sb2Te5により2
0nmの膜厚で、光干渉保護膜25はZnS−SiO2
により100nmの膜厚で、反射膜26はAlにより6
0nmの膜厚で、更に紫外線硬化樹脂27は50μmの
膜厚でそれぞれ形成されている。The present embodiment is characterized in that the light adjusting film 22 is provided between the transparent substrate 21 and the base protective film 23 as compared with the conventional information recording medium shown in FIG. 4B.
The present embodiment is an example of a rewritable phase change type information recording medium that records information on the recording film 23 as a change in phase state. For example, the transparent substrate 21 is made of polycarbonate and has a thickness of 1.2 mm.
The thickness of the light adjusting film 22 is 50 nm by PTV, and the base protection film 23 is 140 n by ZnS—SiO 2 .
The recording film 24 is made of Ge 2 Sb 2 Te 5 with a thickness of m.
A film thickness of 0 nm, light interference protective layer 25 is ZnS-SiO 2
And the reflective film 26 is made of Al.
The film thickness is 0 nm, and the ultraviolet curable resin 27 is formed with a film thickness of 50 μm.
【0036】光調整膜22は図1及び図3に示した光調
整膜11と同様に、図2に示した光強度対屈折率特性を
有している。なお、図4(B)に示す従来のZnS−S
iO2光干渉保護膜25の膜厚は20nmである。The light adjusting film 22 has the light intensity-refractive index characteristic shown in FIG. 2 similarly to the light adjusting film 11 shown in FIGS. The conventional ZnS-S shown in FIG.
The film thickness of the iO 2 light interference protection film 25 is 20 nm.
【0037】次に、この図4(A)に示した情報記録媒
体20の光調整膜22の膜厚変化に対する記録部と未記
録部との反射率と位相差の変化の各例について説明す
る。まず、図5は情報記録媒体20において低照度のレ
ーザビームの照射により屈折率変化が低い状態のPTV
光調整膜22の膜厚変化に対する、記録膜24の記録部
(アモルファス)と未記録部(結晶)の反射率と位相差
の変化を、680nmのレーザビームの波長における光
学計算結果を示す。Next, examples of changes in the reflectance and the phase difference between the recorded portion and the unrecorded portion with respect to the change in the film thickness of the light adjustment film 22 of the information recording medium 20 shown in FIG. 4A will be described. . First, FIG. 5 shows a PTV in a state in which the information recording medium 20 has a low refractive index change due to irradiation with a laser beam of low illuminance
The optical calculation result at the wavelength of the laser beam of 680 nm is shown about the change of the reflectance and phase difference of the recording part (amorphous) and the unrecorded part (crystal) of the recording film 24 with respect to the film thickness change of the light adjusting film 22.
【0038】図5において、破線Iは未記録部の反射
率、実線IIは記録部の反射率、+は記録部と未記録部の
位相差を示す。同図からわかるように、本実施例では低
照度のレーザビームに対して、光調整膜22の膜厚によ
らず、記録部と未記録部の反射率が45%と差異がな
く、位相差も約10°と低くできる。In FIG. 5, the broken line I indicates the reflectance of the unrecorded portion, the solid line II indicates the reflectance of the recorded portion, and + indicates the phase difference between the recorded portion and the unrecorded portion. As can be seen from the figure, in the present embodiment, there is no difference in the reflectance of the recorded portion and the unrecorded portion with respect to the laser beam of low illuminance, that is, 45%, regardless of the film thickness of the light adjustment film 22, and there is no phase difference. Can be as low as about 10 °.
【0039】図6は情報記録媒体20において高照度の
レーザビームの照射により屈折率変化が高い状態のPT
V光調整膜22の膜厚変化に対する、記録膜24の記録
部(アモルファス)と未記録部(結晶)の反射率と位相
差の変化を、680nmのレーザビームの波長における
光学計算結果を示す。FIG. 6 shows a PT in which the information recording medium 20 has a high refractive index change due to irradiation with a laser beam of high illuminance.
The optical calculation result at the wavelength of the laser beam of 680 nm is shown about the change of the reflectance and the phase difference of the recorded part (amorphous) and the unrecorded part (crystal) of the recording film 24 with respect to the change of the film thickness of the V light adjusting film 22.
【0040】図6において、破線IIIは未記録部の反射
率、実線IVは記録部の反射率、+は記録部と未記録部の
位相差を示す。同図からわかるように、本実施例では高
照度のレーザビームに対して、光調整膜22の膜厚が3
0[nm]≦d(PTV)≦60[nm]にかけて、記
録部と未記録部の反射率差が約20%存在し、位相差も
約10°と低くでき、再生信号として検出が可能であ
る。In FIG. 6, the broken line III indicates the reflectance of the unrecorded portion, the solid line IV indicates the reflectance of the recorded portion, and + indicates the phase difference between the recorded portion and the unrecorded portion. As can be seen from the figure, in this embodiment, the thickness of the light adjusting film 22 is 3 with respect to the laser beam of high illuminance.
When 0 [nm] ≦ d (PTV) ≦ 60 [nm], the reflectance difference between the recorded portion and the unrecorded portion is about 20%, the phase difference can be reduced to about 10 °, and it can be detected as a reproduced signal. is there.
【0041】図7は情報記録媒体20において、ZnS
−SiO2光干渉保護膜25の膜厚を150nmとした
とき、低照度のレーザビームの照射により屈折率変化が
低い状態のPTV光調整膜22の膜厚変化に対する、記
録膜24の記録部(アモルファス)と未記録部(結晶)
の反射率と位相差の変化を、680nmのレーザビーム
の波長における光学計算結果を示す。FIG. 7 shows the information recording medium 20 with ZnS.
When the film thickness of the -SiO 2 light interference protection film 25 is set to 150 nm, the recording portion of the recording film 24 with respect to the film thickness change of the PTV light adjusting film 22 in a state where the refractive index change is low due to the irradiation of the laser beam of low illuminance ( Amorphous) and unrecorded area (crystal)
The optical calculation results of the change in the reflectance and the phase difference at the wavelength of the laser beam of 680 nm are shown.
【0042】図7において、破線Vは未記録部の反射
率、実線VIは記録部の反射率、+は記録部と未記録部の
位相差を示す。同図からわかるように、本実施例では低
照度のレーザビームに対して、光調整膜22の膜厚によ
らず、記録部と未記録部の反射率が約60%と差異がな
く、位相差も約6°と低くできる。In FIG. 7, the broken line V indicates the reflectance of the unrecorded portion, the solid line VI indicates the reflectance of the recorded portion, and + indicates the phase difference between the recorded portion and the unrecorded portion. As can be seen from the figure, in the present embodiment, the reflectance of the recorded portion and the unrecorded portion is about 60% with respect to the laser beam of low illuminance, regardless of the film thickness of the light adjustment film 22, and there is no difference. The phase difference can be as low as about 6 °.
【0043】図8は情報記録媒体20において、ZnS
−SiO2光干渉保護膜25の膜厚を150nmとした
とき、高照度のレーザビームの照射により屈折率変化が
高い状態のPTV光調整膜22の膜厚変化に対する、記
録膜24の記録部(アモルファス)と未記録部(結晶)
の反射率と位相差の変化を、680nmのレーザビーム
の波長における光学計算結果を示す。FIG. 8 shows the information recording medium 20 with ZnS
When the film thickness of the —SiO 2 light interference protection film 25 is set to 150 nm, the recording portion of the recording film 24 (for the film thickness change of the PTV light adjusting film 22 in the state where the refractive index change is high due to the irradiation of the laser beam with high illuminance) ( Amorphous) and unrecorded area (crystal)
The optical calculation results of the change in the reflectance and the phase difference at the wavelength of the laser beam of 680 nm are shown.
【0044】図8において、破線VIIは未記録部の反射
率、実線VIIIは記録部の反射率、+は記録部と未記録部
の位相差を示す。同図からわかるように、本実施例では
高照度のレーザビームに対して、光調整膜22の膜厚が
70[nm]≦d(PTV)≦90[nm]にかけて、
記録部と未記録部の反射率差が約20%存在し、位相差
も約6°と低くでき、再生信号として検出が可能であ
る。In FIG. 8, the broken line VII indicates the reflectance of the unrecorded portion, the solid line VIII indicates the reflectance of the recorded portion, and + indicates the phase difference between the recorded portion and the unrecorded portion. As can be seen from the figure, in the present embodiment, with respect to the laser beam of high illuminance, the film thickness of the light adjustment film 22 is set to 70 [nm] ≦ d (PTV) ≦ 90 [nm],
The reflectance difference between the recorded portion and the unrecorded portion is about 20%, the phase difference can be reduced to about 6 °, and it can be detected as a reproduced signal.
【0045】なお、本発明は以上の実施例に限定される
ものではなく、1回のみ記録ができ、再生は繰り返しで
きる追記型の情報記録媒体、書き換え型情報記録媒体の
一例である情報を磁化の方向の変化として記録する光磁
気記録媒体などにも適用することができる。また、光調
整膜11、22は2層以上の構成でもよい。The present invention is not limited to the above embodiments, but it is possible to record information only once, and to reproduce information, which is an example of a write-once type information recording medium or rewritable type information recording medium. It can also be applied to a magneto-optical recording medium for recording as a change in the direction of. Further, the light adjustment films 11 and 22 may have a structure of two or more layers.
【0046】[0046]
【発明の効果】以上説明したように、本発明によれば、
光調整膜により、所定光強度以下の低照度レーザビーム
が照射されている周辺部は屈折率の変化を殆ど発生しな
いため、記録部と未記録部の位相差が殆ど無くなり、再
生信号として検出されず、所定光強度より大なる高照度
のレーザビームが照射されている中央部は屈折率変化を
生じて、記録部と未記録部に反射率と位相差が発生する
ため、再生信号として検出でき、従って、レーザビーム
を照射することにより記録膜上のスポット径を実質的に
小径化でき、これにより記録密度を高密度化できる。As described above, according to the present invention,
The light adjustment film causes almost no phase difference between the recorded portion and the unrecorded portion in the peripheral portion irradiated with the low illuminance laser beam having the predetermined light intensity or less, so that it is detected as a reproduction signal. However, the central part irradiated with the laser beam of high illuminance higher than the predetermined light intensity changes the refractive index, and the reflectivity and the phase difference occur between the recorded part and the unrecorded part. Therefore, by irradiating the laser beam, the spot diameter on the recording film can be substantially reduced, and the recording density can be increased.
【0047】また、本発明によれば、光ヘッド内の対物
レンズの中心部を遮光するか、あるいは対物レンズの中
心部を透過する光の位相を対物レンズの周辺部を透過す
る光の位相よりも早めて、記録膜又は反射膜上に合焦さ
れるレーザビームの半値幅径を小さくすることにより、
記録膜又は反射膜上に照射されるスポット径のより一層
の小径化を達成できる。Further, according to the present invention, the central portion of the objective lens in the optical head is shielded or the phase of the light transmitted through the central portion of the objective lens is determined from the phase of the light transmitted through the peripheral portion of the objective lens. As soon as possible, by reducing the full width at half maximum of the laser beam focused on the recording film or the reflective film,
It is possible to further reduce the diameter of the spot irradiated on the recording film or the reflective film.
【0048】また、本発明によれば、対物レンズ中心を
遮光するか、あるいは対物レンズ中心部を透過する光の
位相を対物レンズの周辺部を透過する光の位相よりも早
めたときに、小径化されたメインローブの周辺に発生す
るサイドローブは、光調整膜により記録部と未記録部の
位相差を減少されるためにメインローブへの影響を大幅
に低減させることができ、よって記録密度の高密度化を
実現できる。Further, according to the present invention, when the center of the objective lens is shielded or the phase of the light passing through the central part of the objective lens is made earlier than the phase of the light passing through the peripheral part of the objective lens, a small diameter is obtained. The side lobe generated around the converted main lobe can significantly reduce the influence on the main lobe because the phase difference between the recorded portion and the unrecorded portion is reduced by the light adjustment film, and thus the recording density can be reduced. Higher density can be realized.
【0049】更に、本発明によれば、光調整膜は屈折率
を照度に応じて変化させている構成であり、従来の情報
記録媒体のような光制御膜が光ビームの照度に応じて光
透過率が変化するものではないため、反射光の光量が減
少することはなく、よって再生信号の劣化が生じたり、
トラックサーボがかかりにくいという不具合を防止する
ことができる。Further, according to the present invention, the light adjusting film has a structure in which the refractive index is changed according to the illuminance, and a light control film such as a conventional information recording medium is used for adjusting the light according to the illuminance of the light beam. Since the transmittance does not change, the amount of reflected light does not decrease, which causes deterioration of the reproduction signal,
It is possible to prevent the problem that the track servo is hard to be applied.
【図1】本発明の情報記録媒体及び再生方法の第1実施
例の説明図である。FIG. 1 is an explanatory diagram of a first embodiment of an information recording medium and a reproducing method of the present invention.
【図2】本発明の要部の光調整膜の一例の特性図であ
る。FIG. 2 is a characteristic diagram of an example of a light adjustment film of a main part of the present invention.
【図3】本発明の情報記録媒体の第1実施例及び再生方
法の第2実施例の説明図である。FIG. 3 is an explanatory diagram of a first embodiment of an information recording medium of the present invention and a second embodiment of a reproducing method.
【図4】本発明の情報記録媒体の第2実施例と従来の情
報記録媒体とを対比して示す断面図である。FIG. 4 is a sectional view showing a second embodiment of the information recording medium of the present invention and a conventional information recording medium in comparison.
【図5】低照度のレーザビームに対するPTV光調整膜
の膜厚と反射率及び位相差との関係の一例を示す特性図
である。FIG. 5 is a characteristic diagram showing an example of the relationship between the film thickness of the PTV light adjusting film with respect to a low illuminance laser beam, and the reflectance and phase difference.
【図6】高照度のレーザビームに対するPTV光調整膜
の膜厚と反射率及び位相差との関係の一例を示す特性図
である。FIG. 6 is a characteristic diagram showing an example of the relationship between the film thickness of the PTV light adjusting film with respect to a high illuminance laser beam, and the reflectance and phase difference.
【図7】低照度のレーザビームに対するPTV光調整膜
の膜厚と反射率及び位相差との関係の他の例を示す特性
図である。FIG. 7 is a characteristic diagram showing another example of the relationship between the film thickness of the PTV light adjusting film with respect to a laser beam of low illuminance and the reflectance and the phase difference.
【図8】高照度のレーザビームに対するPTV光調整膜
の膜厚と反射率及び位相差との関係の他の例を示す特性
図である。FIG. 8 is a characteristic diagram showing another example of the relationship between the film thickness of the PTV light adjusting film with respect to a high-illuminance laser beam, and the reflectance and phase difference.
【図9】従来の情報記録媒体及び再生方法の一例の説明
図である。FIG. 9 is an explanatory diagram of an example of a conventional information recording medium and a reproducing method.
2、21 透明基板 4、26 反射膜 5、27 紫外線硬化樹脂 6、13 光学ヘッド 7 対物レンズ 8 レーザビーム 8a メインローブ 8b、8c サイドローブ 10 第1実施例の情報記録媒体 11、22 光調整膜 12、23 記録膜 20 第2実施例の情報記録媒体 23 下地保護膜 25 光干渉保護膜 2, 21 Transparent substrate 4, 26 Reflective film 5, 27 UV curable resin 6, 13 Optical head 7 Objective lens 8 Laser beam 8a Main lobe 8b, 8c Side lobe 10 Information recording medium of the first embodiment 11, 22 Light adjusting film 12, 23 recording film 20 information recording medium of the second embodiment 23 underlayer protective film 25 optical interference protective film
Claims (4)
は特性変化を利用して情報をレーザビームにより記録
し、これを再生する書き換え型、追記型の光学的情報記
録媒体、あるいは形状変化により記録膜に記録されてい
る情報をレーザビームにより再生する再生専用型の光学
的情報記録媒体において、 前記透明基板と記録膜との間に、所定光強度より大なる
光強度の前記レーザビームに対する屈折率の変化が、該
所定光強度以下の光強度の該レーザビームに対する屈折
率の変化が大である、少なくとも一層以上の非線形屈折
率特性を有する光調整膜を設けたことを特徴とする情報
記録媒体。1. A rewritable or write-once type optical information recording medium for recording information by a laser beam by utilizing a shape change or a characteristic change of a recording film above a transparent substrate, or recording by a shape change. In a read-only optical information recording medium for reproducing information recorded on a film by a laser beam, a refractive index for the laser beam having a light intensity higher than a predetermined light intensity is provided between the transparent substrate and the recording film. Change in the refractive index with respect to the laser beam having a light intensity less than or equal to the predetermined light intensity is large, and an information recording medium having at least one or more non-linear refractive index characteristics is provided. .
いることを特徴とする請求項1記載の情報記録媒体。2. The light control film has the following formula: The information recording medium according to claim 1, wherein poly- (2,5-chenylene vinylene) represented by the following is used.
変化若しくは特性変化を利用して記録された情報をレー
ザビームにより再生する書き換え型、追記型の光学的情
報記録媒体、あるいは形状変化により記録膜に記録され
ている情報をレーザビームにより再生する再生専用型の
光学的情報記録媒体の再生方法において、 前記透明基板と記録膜との間に設けられた、所定光強度
より大なる光強度の前記レーザビームに対する屈折率の
変化が、該所定光強度以下の光強度の該レーザビームに
対する屈折率の変化が大である、少なくとも一層以上の
光調整膜により、再生時に前記記録膜の形状変化若しく
は特性変化により生じる、反射率、吸収率、透過率及び
記録部と未記録部の位相差とを調整し、該光調整膜が前
記情報面の焦点深度内に位置するようにして再生するこ
とを特徴とする情報記録媒体の再生方法。3. A rewritable or write-once type optical information recording medium for reproducing information recorded by a laser beam by utilizing a shape change or a characteristic change of a recording film on an information surface above a transparent substrate, or a shape change. In a reproducing method of a reproduction-only type optical information recording medium for reproducing information recorded on a recording film by a laser beam, a light having a intensity higher than a predetermined light intensity provided between the transparent substrate and the recording film. The shape of the recording film at the time of reproduction by at least one or more light adjusting films, in which the change in the refractive index with respect to the laser beam with respect to the intensity is largely changed with respect to the laser beam with the light intensity equal to or lower than the predetermined light intensity. The reflectance, the absorptance, the transmittance, and the phase difference between the recorded portion and the unrecorded portion, which are caused by the change or the characteristic change, are adjusted, and the light adjustment film is positioned within the depth of focus of the information surface. The method of reproducing the information recording medium, characterized in that to play manner.
て前記記録膜上に合焦させる光ヘッド内の対物レンズ中
心を遮光するか、あるいは該対物レンズ中心部を透過す
る光の位相を該対物レンズの周辺部を透過する光の位相
よりも早めて再生を行うことを特徴とする請求項3記載
の情報記録媒体の再生方法。4. The objective lens center in an optical head for making the laser beam incident from a transparent substrate to focus on the recording film is shielded, or the phase of light transmitted through the central portion of the objective lens is set to the objective. 4. The reproducing method for an information recording medium according to claim 3, wherein the reproducing is performed earlier than the phase of the light transmitted through the peripheral portion of the lens.
Priority Applications (1)
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JP6280204A JP3068420B2 (en) | 1994-11-15 | 1994-11-15 | Reproducing method of optical information recording medium |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6280204A JP3068420B2 (en) | 1994-11-15 | 1994-11-15 | Reproducing method of optical information recording medium |
Publications (2)
Publication Number | Publication Date |
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JPH08147757A true JPH08147757A (en) | 1996-06-07 |
JP3068420B2 JP3068420B2 (en) | 2000-07-24 |
Family
ID=17621769
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR20000019987A (en) * | 1998-09-17 | 2000-04-15 | 구자홍 | High-density optical recording medium |
US8426005B2 (en) | 2009-03-18 | 2013-04-23 | Nec Corporation | Optical information recording medium |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02292742A (en) * | 1989-05-02 | 1990-12-04 | Pioneer Electron Corp | Optical head |
JPH06162570A (en) * | 1992-11-17 | 1994-06-10 | Victor Co Of Japan Ltd | Optical information recording medium disk and its production |
-
1994
- 1994-11-15 JP JP6280204A patent/JP3068420B2/en not_active Expired - Fee Related
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02292742A (en) * | 1989-05-02 | 1990-12-04 | Pioneer Electron Corp | Optical head |
JPH06162570A (en) * | 1992-11-17 | 1994-06-10 | Victor Co Of Japan Ltd | Optical information recording medium disk and its production |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR20000019987A (en) * | 1998-09-17 | 2000-04-15 | 구자홍 | High-density optical recording medium |
US8426005B2 (en) | 2009-03-18 | 2013-04-23 | Nec Corporation | Optical information recording medium |
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JP3068420B2 (en) | 2000-07-24 |
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