JP2955112B2 - 光磁気記憶媒体 - Google Patents

光磁気記憶媒体

Info

Publication number
JP2955112B2
JP2955112B2 JP4054622A JP5462292A JP2955112B2 JP 2955112 B2 JP2955112 B2 JP 2955112B2 JP 4054622 A JP4054622 A JP 4054622A JP 5462292 A JP5462292 A JP 5462292A JP 2955112 B2 JP2955112 B2 JP 2955112B2
Authority
JP
Japan
Prior art keywords
dielectric layer
magneto
layer
optical storage
film
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
Application number
JP4054622A
Other languages
English (en)
Other versions
JPH05258361A (ja
Inventor
直泰 池谷
博之 片山
純一郎 中山
賢司 太田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Consejo Superior de Investigaciones Cientificas CSIC
Original Assignee
Consejo Superior de Investigaciones Cientificas CSIC
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Publication date
Application filed by Consejo Superior de Investigaciones Cientificas CSIC filed Critical Consejo Superior de Investigaciones Cientificas CSIC
Priority to JP4054622A priority Critical patent/JP2955112B2/ja
Priority to CA002091490A priority patent/CA2091490C/en
Priority to EP93301891A priority patent/EP0560625B1/en
Priority to DE69320511T priority patent/DE69320511T2/de
Publication of JPH05258361A publication Critical patent/JPH05258361A/ja
Priority to US08/358,682 priority patent/US5643687A/en
Application granted granted Critical
Publication of JP2955112B2 publication Critical patent/JP2955112B2/ja
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording 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
    • G11B7/24Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/241Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • G11B7/252Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers
    • G11B7/257Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers
    • G11B7/2578Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers consisting essentially of inorganic materials
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
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    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
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    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
    • G11B11/10582Record carriers characterised by the selection of the material or by the structure or form
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    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
    • G11B11/10582Record carriers characterised by the selection of the material or by the structure or form
    • G11B11/10586Record carriers characterised by the selection of the material or by the structure or form characterised by the selection of the material
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    • GPHYSICS
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    • G11B2007/25705Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers consisting essentially of inorganic materials
    • G11B2007/25715Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers consisting essentially of inorganic materials containing oxygen
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    • G11B2007/25705Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers consisting essentially of inorganic materials
    • G11B2007/25718Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers consisting essentially of inorganic materials containing halides (F, Cl, Br, l)
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    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
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  • Chemical & Material Sciences (AREA)
  • Inorganic Chemistry (AREA)
  • Optical Record Carriers And Manufacture Thereof (AREA)

Description

【発明の詳細な説明】
【0001】
【産業上の利用分野】本発明はレーザー光により情報の
記録、再生及び消去を行う光磁気記憶媒体に関する。
【0002】
【従来の技術】現在、光磁気効果を利用した書き換え可
能な光磁気ディスクとして、希土類遷移金属膜の研究が
活発に行われ、実用化段階にある。しかし、希土類遷移
金属膜の場合、耐食性が良くないことからくる信頼性の
問題、カー回転角が小さいために再生信号レベルが低い
といった問題があった。再生信号レベルを高くするため
には、カー回転角を大きくする必要があり、光磁気記憶
媒体の構造を、光磁気記録層と誘電体層からなる反射防
止構造(例えば、IEEE Trans.Magn.MAG-16,p1194(1980)
参照)にしたり、光磁気記憶層、誘電体層とさらに反射
層を設ける反射膜構造によって、見かけのカー回転角を
向上させている。また、耐食性の点から光磁気記録層を
保護層で狭持し信頼性を向上する方法がとられている。
【0003】
【発明が解決しようとする課題】このように、ディスク
開発の重要な課題として、カー回転角を大きくすること
が挙げられ、そのためには誘電体層の屈折率を大きくし
てエンハンス効果を増大する必要がある。しかしなが
ら、従来用いられてきた誘電体層としては、AlN、A
lSiN、SiNといった窒化物系やAl23、SiO
といった酸化物系があったが、いずれの屈折率も約1.5
〜2.0前後であり、カー回転角増大効果としてはいまだ
不十分である。一方TiO2、BaTiO3のような酸化
物系では約2.4〜2.6といった高屈折率を有するものの、
成膜時の遊離酸素の悪影響もあって光磁気記録層の保護
という点から問題があり利用されなかった。
【0004】本発明は、誘電体層に成膜時の遊離酸素の
影響を避けながら高屈折率の酸化物材料を用いる方法を
提供するものである。
【0005】
【課題を解決するための手段】本発明の第1発明は、基
板上に、少なくとも誘電体層、光磁気記録層、保護層を
順に積層した光磁気記憶媒体において、前記誘電体層
は、基板側から、第1誘電体層と、第2誘電体層とから
なり、前記第1誘電体層は、屈折率が2.4以上3.5
以下の酸化物の層であり、前記第2誘電体層は、酸素を
含まず、前記第1誘電体層に比べ薄い層であることを特
徴とする光磁気記憶媒体である。 また、第2発明は、前
記第1誘電体層の層厚は45〜60nmであり、前記第
2誘電体層の層厚は1〜12nmであることを特徴とす
る第1発明の光磁気記憶媒体である。 また、第3発明
は、前記第1誘電体層がTiO2膜からなり、前記第2
誘電体層がTiN膜からなることを特徴とする第1また
は第2発明の光磁気記憶媒体である。
【0006】
【0007】
【作用】本発明によれば、第1誘電体層に従来の窒化物
系及び酸化物系より大きな屈折率を示す例えばTiO2
膜を用いることによりカー回転角を大きくすることがで
き、第2誘電体層に酸素を含んでいない例えばTiN膜
を用いることにより耐食性のための機能を付与すること
ができる。さらに、光吸収がほとんどない第1誘電体層
に比べ、第2誘電体層を薄くすることにより第2誘電体
層の光吸収を無視できるようになり、カー回転角のエン
ハンス効果を得ることができる。
【0008】
【実施例】
[実施例1]図1に本発明に係る光磁気記憶媒体の構成
図を示す。ここで、1は透光性基板、2は第一誘電体
層、3は第二誘電体層、4は光磁気記録層、5は保護層
を示す。上記の光磁気記憶媒体の製造方法に際しては、
例えば、ポリカーボネイト樹脂、アクリル樹脂、非晶質
ポリオレフィン等の合成樹脂またはガラス基板からなる
透光性基板1上に、第一誘電体層TiO2膜2、第二誘
電体層TiN膜3を形成する。続いて、TbFeCo、
DyTeCo、GdTbFe、Pt/Co多層膜等から
なる光磁気記録層4と例えばAlN、AlSiN膜等か
らなる保護層5を形成する。第一誘電体層TiO2膜2
と第二誘電体層TiN膜3の製造については、まず第一
誘電体層TiO2膜2はTiターゲットを用いて(Ar
+O2)ガス雰囲気中、スパッタパワー0.3〜0.6kw、ス
パッタ圧2.5〜3.0mTorr、O2分圧0.8〜1.0mTorrの条件
下、反応性スパッタリング法で形成することによって、
屈折率n=2.54を示す透明膜が得られる。また、第二誘
電体層TiN膜3は同一Tiターゲットを用いて、N2
ガス雰囲気中で反応性スパッタリング法にて形成する。
膜厚としては、反射防止構造によるカー回転角増大効果
を効率的にするために第一誘電体層は50.0〜60.0nmの範
囲内、第二誘電体層は第一誘電体層の遊離酸素の影響を
抑えるとともに、該層での吸収ロスを極力抑えるために
1.0〜6.0nmに設定されることが望ましい。このようにし
て形成された光磁気記憶媒体は、反射防止構造にn=2.
54という大きな屈折率を示すTiO2膜を用いるので、
従来誘電体層に屈折率n=2.05を示すAlNを用いてい
た場合より見かけのカー回転角が従来より約32〜66%大
きくなり、光磁気記録層の吸収も最大約14%増加でき再
生信号レベルも最大約1.4dB程高くなる。TiO2膜とT
iN膜は同一ターゲットを用いるため製造工程は複雑に
ならず、導入ガスを(Ar+O2)ガスからN2ガスへ例
えば徐々に切り換えていくことによって組成をある程度
連続的に変化させることが可能で、この場合、両層内の
内部応力を緩和できる。さらにTiN膜は酸素を含ま
ず、また第一誘電体層の成分酸素と光磁気記録層との成
膜時のミキシングや外部からの酸素の侵入を防ぐことが
できるので耐食性も確立され高い信頼性が得られる。
【0009】[実施例2]図2に本発明に係る他の光磁
気記憶媒体の構成図を示す。ここで、1は透光性基板、
2は第一誘電体層、3は第二誘電体層、4は光磁気記録
層、7は例えば屈折率が第一誘電体層と比べて相対的に
小さな LiF、MgF2膜などからなる第三誘電体層、
6は反射層を示す。上記の光磁気記憶媒体の製造に際し
ては、実施例1と同様に1〜4及び7を形成した後、例
えばAl、Ta、SUS、Ti、Au、Cu、Ag等か
らなる反射層6を形成する。第一誘電体層TiO2膜2
と第二誘電体層TiN膜3の製造については、実施例1
と同様に形成すればよい。膜厚としてはカー回転角増大
効果を効率的にするために第一誘電体層は45.0〜55.0nm
の範囲内、第二誘電体層は第一誘電体層の遊離酸素の影
響を抑えるとともに、該層での吸収ロスを極力抑えるた
めに1.0〜5.0nmに設定されることが望ましく、誘電体層
に屈折率n=2.05を示すAlNを用いていた従来の場合
より見かけのカー回転角が約40〜50%大きくなり、光磁
気記録層の吸収も最大約10%増加でき再生信号レベルも
最大約1.0dB程高くなる。本実施例では、上述の反射防
止によるカー効果増大とともに、光磁気記録層透過時の
ファラデー効果もさらに重畳されるため見かけのカー回
転角がさらに大きく再生信号レベルも高くなり、耐食性
もすぐれた高い信頼性の光磁気記憶媒体が得られる。
【0010】[実施例3]図3に本発明に係る他の光磁
気記憶媒体の構成図を示す。ここで、1は透光性基板、
2は第一誘電体層、3は第二誘電体層、4は光磁気記録
層、8は例えば酸素を含まないSiN膜からなる第三誘
電体層、9は第一誘電体層に比べて相対的に屈折率の小
さな例えばSiO2膜からなる第四誘電体層、6は反射
層である。上記の光磁気記憶媒体の製造に際しては、実
施例1と同様に1〜4を形成後、第三誘電体層SiN膜
8はSiターゲットを用いてN2ガス雰囲気中で反応性
スパッタリング法にて形成し、第四誘電体層SiO2
9は同一Siターゲットを用いて(Ar+O2)ガス雰
囲気中で反応性スパッタリング法にて形成する。その
後、例えばAl、Ta、SUS、Ti、Au、Cu、A
g等からなる反射層6を形成する。第一誘電体層TiO
2膜2と第二誘電体層TiN膜3の製造については、実
施例1と同様に形成すればよい。膜厚としてはカー回転
角増大効果を効率的にするために第一誘電体層は45.0〜
50.0nmの範囲内、第二誘電体層は第一誘電体層の遊離酸
素の影響を抑えるとともに、該層での吸収ロスを極力抑
えるために1.0〜12.0nmに設定されることが望ましい。
SiN膜の膜厚はSiO2の成分酸素と光磁気記録層と
の成膜時のミキシングを防げる程度、望ましくは1.0〜
10.0nmにすればよい。本構造においても、実施例
2と同様に誘電体層に屈折率n=2.05を示すAlN
を用いていた従来の場合より見かけのカー回転角が最大
10倍程度大きくすることが可能で光磁気記録層の吸収も
最大約30%増加でき再生信号レベルも最大約1.8dB高く
なる。
【0011】
【発明の効果】以上のように、本発明では、第1誘電体
層に従来の窒化物系及び酸化物系より大きな屈折率を示
す例えばTiO2膜を用いることによりカー回転角を大
きくすることができ再生信号レベルも高くなり、第2誘
電体層に酸素を含んでいない例えばTiN膜を用いるこ
とにより耐食性のための機能を付与することができ高い
信頼性が得られる。さらに、光吸収がほとんどない第1
誘電体層に比べ、第2誘電体層を薄くすることにより第
2誘電体層の光吸収を無視できるようになり、カー回転
角のエンハンス効果を得ることができる。
【図面の簡単な説明】
【図1】 本発明の光磁気記憶媒体の構成の概略断面図
である。
【図2】 本発明の他の光磁気記憶媒体の構成の概略断
面図である。
【図3】 本発明の他の光磁気記憶媒体の構成の概略断
面図である。
【符号の説明】
1 基板 2 第一誘電体層 3 第二誘電体層 4 光磁気記録層 5、7、8 第三誘電体層 6 反射層 9 第四誘電体層
───────────────────────────────────────────────────── フロントページの続き (72)発明者 太田 賢司 大阪府大阪市阿倍野区長池町22番22号 シャープ株式会社内 (56)参考文献 特開 昭61−227243(JP,A) 特開 昭58−200447(JP,A) 特開 平3−137838(JP,A) 特開 昭63−282942(JP,A) (58)調査した分野(Int.Cl.6,DB名) G11B 11/10

Claims (3)

    (57)【特許請求の範囲】
  1. 【請求項1】 基板上に、少なくとも誘電体層、光磁気
    記録層、保護層を順に積層した光磁気記憶媒体におい
    て、 前記誘電体層は、基板側から、第1誘電体層と、第2誘
    電体層とからなり、 前記第1誘電体層は、屈折率が2.4以上3.5以下の
    酸化物の層であり、 前記第2誘電体層は、酸素を含まず、前記第1誘電体層
    に比べ薄い層であることを特徴とする光磁気記憶媒体。
  2. 【請求項2】 前記第1誘電体層の層厚は45〜60n
    mであり、前記第2誘電体層の層厚は1〜12nmであ
    ることを特徴とする請求項1記載の光磁気記憶媒体。
  3. 【請求項3】 前記第1誘電体層がTiO2膜からな
    り、前記第2誘電体層がTiN膜からなることを特徴と
    する請求項1または2記載の光磁気記憶媒体。
JP4054622A 1992-03-13 1992-03-13 光磁気記憶媒体 Expired - Fee Related JP2955112B2 (ja)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP4054622A JP2955112B2 (ja) 1992-03-13 1992-03-13 光磁気記憶媒体
CA002091490A CA2091490C (en) 1992-03-13 1993-03-11 Magneto-optic memory medium and a method for producing the same
EP93301891A EP0560625B1 (en) 1992-03-13 1993-03-12 A magneto-optic memory medium and a method for producing the same
DE69320511T DE69320511T2 (de) 1992-03-13 1993-03-12 Magnetooptisches Speichermedium und Verfahren zu seiner Herstellung
US08/358,682 US5643687A (en) 1992-03-13 1994-12-19 Magneto-optic memory medium and a method for producing the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4054622A JP2955112B2 (ja) 1992-03-13 1992-03-13 光磁気記憶媒体

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JP2955112B2 true JP2955112B2 (ja) 1999-10-04

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EP (1) EP0560625B1 (ja)
JP (1) JP2955112B2 (ja)
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DE (1) DE69320511T2 (ja)

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JPH07182709A (ja) * 1993-11-15 1995-07-21 Minnesota Mining & Mfg Co <3M> 光磁気記録媒体
JPH1021586A (ja) * 1996-07-02 1998-01-23 Sony Corp Dcスパッタリング装置
US6477135B1 (en) 1998-03-26 2002-11-05 Matsushita Electric Industrial Co., Ltd. Optical information recording medium and method for recording and reproduction information thereon
WO2010151855A2 (en) * 2009-06-26 2010-12-29 Cornell University Iii-v semiconductor structures including aluminum-silicon nitride passivation
JP2011228462A (ja) * 2010-04-19 2011-11-10 Taiyo Yuden Co Ltd 薄膜キャパシタ

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JPS59110052A (ja) * 1982-12-15 1984-06-25 Sharp Corp 光メモリ素子
JPS6124041A (ja) * 1984-07-13 1986-02-01 Canon Inc 光学的磁気記録媒体
US4939023A (en) * 1984-08-13 1990-07-03 Canon Kabushiki Kaisha Opto-magnetic recording medium
JPS61227243A (ja) * 1985-03-30 1986-10-09 Olympus Optical Co Ltd 光磁気記録媒体
US4861671A (en) * 1985-10-23 1989-08-29 Kerdix, Inc. Magneto-optic recording media with protective layer
US4800112A (en) * 1986-04-10 1989-01-24 Seiko Epson Corporation Optical recording medium
JPS639050A (ja) * 1986-06-28 1988-01-14 Pioneer Electronic Corp 光磁気記録媒体
DE3716736A1 (de) * 1987-05-19 1988-12-01 Basf Ag Flaechenfoermiges, mehrschichtiges, magneto-optisches aufzeichnungsmaterial
US5228024A (en) * 1990-05-28 1993-07-13 Goldstar Co., Ltd. Magneto-optical disk possessing enhanced anti-reflective and anti-oxidative properties

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Publication number Publication date
EP0560625A3 (en) 1993-11-10
CA2091490A1 (en) 1993-09-14
EP0560625A2 (en) 1993-09-15
US5643687A (en) 1997-07-01
DE69320511T2 (de) 1999-04-01
EP0560625B1 (en) 1998-08-26
JPH05258361A (ja) 1993-10-08
DE69320511D1 (de) 1998-10-01
CA2091490C (en) 1997-10-14

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