JPH0437490B2 - - Google Patents

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Publication number
JPH0437490B2
JPH0437490B2 JP59012566A JP1256684A JPH0437490B2 JP H0437490 B2 JPH0437490 B2 JP H0437490B2 JP 59012566 A JP59012566 A JP 59012566A JP 1256684 A JP1256684 A JP 1256684A JP H0437490 B2 JPH0437490 B2 JP H0437490B2
Authority
JP
Japan
Prior art keywords
polycarbonate
magneto
unit
optical recording
substrate
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 - Lifetime
Application number
JP59012566A
Other languages
Japanese (ja)
Other versions
JPS60157747A (en
Inventor
Masaru Sato
Nagayoshi Tsukane
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.)
Daicel Corp
Original Assignee
Daicel Chemical Industries Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Daicel Chemical Industries Ltd filed Critical Daicel Chemical Industries Ltd
Priority to JP1256684A priority Critical patent/JPS60157747A/en
Publication of JPS60157747A publication Critical patent/JPS60157747A/en
Publication of JPH0437490B2 publication Critical patent/JPH0437490B2/ja
Granted 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
    • G11B7/253Record 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 substrates
    • G11B7/2533Record 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 substrates comprising resins
    • G11B7/2534Record 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 substrates comprising resins polycarbonates [PC]
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording 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
    • 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
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording 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
    • 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

Description

【発明の詳細な説明】[Detailed description of the invention]

(産業上の利用分野) 本発明はポリカーボネートを基板とし、光磁気
メモリー、磁気記録表示素子などに用いられる磁
性薄膜記録デイスクに関するものである。 (従来技術) 希土類−遷移金属アモルフアス層を真空蒸着、
スパツタリングあるいはイオンプレーテイング等
の手段で基板上に形成し、このアモルフアス層に
レーザービームを当てて熱磁気効果により情報の
書き込み及び消去を行い、熱磁気効果により情報
の読み取りを行う光磁気記録方法は公知であり、
上記アモルフアス層を形成する基板としてはガラ
ス板、アクリル樹脂あるいはポリカーボネート樹
脂のような透明プラスチツク板、さらに不透明材
料ではあるが、アルミニウムやシリコンウエハー
のような金属板が提案されている。 しかしこれら各種基板が提案されている中で、
ガラス基板の場合には垂直磁化可能なアモルフア
ス層を形成することが可能であるが光磁気記録デ
イスクとした場合には、デイスクの重量が大き
くなる誤つて落下させた場合の破損の危険性、
高速回転に耐えない研磨する為に高価である
レーザービームのトラツキングに用いる案内溝
を直接形成できないというような欠点を有してお
り工業的生産には不向きである。一方アルミニウ
ムやシリコンウエハーの様な金属材料もガラスと
同様に垂直磁化可能なアモルフアス層を形成する
ことが可能であるが、ガラスと同様に、表面研
磨を行う為、非常に高価であるシリコンの場合
大面積のものができない。レーザービームのト
ラツキングに用いる案内溝を直接形成できない
不透明であるために、透明材料の如く基板から書
き込みや再生ができない。従つて表面に付着した
ゴミやキズにより信号/雑音比(S/N比)が大
きな影響をうけるという欠点を有する。さらにア
クリル樹脂やポリカーボネートの如き、透明プラ
スチツク材料の場合では、アモルフアス垂直磁化
膜の形成技術は確立されていないうえに、次のよ
うな欠点がある: アクリル樹脂は光学的には性能は十分である
が吸湿量が大きいため吸湿変形を生じる事、又
成形条件にも依存するが熱変形も大きいという
欠点を有する。これら変形により垂直磁化膜や
この上に形成するSiO2,TiO2,Al2O3,Ta2
O5,MgF2等の保護膜にクラツクが入つたり、
基板からこれら薄膜が剥落するという現象を生
じ易い。又、薄膜とアクリル樹脂との密着性が
ガラスや金属に比較して非常に低く、他のプラ
スチツク材料に比較しても低いという欠点も有
する。 ポリカーボネート樹脂はアクリル樹脂の如
き、吸湿変形及び熱変形は少いのであるが、光
学的には複屈折率が大きく事及び薄膜の密着性
が低いという欠点を有している。 この他にも透明プラスチツクはあるが、スチレ
ン系樹脂は複屈折がポリカーボネートより更に大
きく、塩化ビニル樹脂は、残留塩素による薄膜の
腐触及び光学的性能に、ポリエステル系樹脂は光
学的透明性、及び複屈折に夫々問題点を有し、い
ずれの材料も光磁気記録デイスク用基板としては
欠点を有するため、実用化されていないのが現状
である。従つて大量生産性に優れ、取り扱いが容
易なプラスチツク基板上に安定な垂直磁化膜を形
成し光磁気記録デイスクを生産する技術の確立が
強く望まれている。 本発明者らはかかる問題点に対し、プラスチツ
ク材料の中でポリカーボネート樹脂が総合的な物
性に最も優れており、その問題点である複屈折
性及び密着性を改良すれば、ガラスやアルミ等
の無機質基板と同等以上の優れた光磁気記録デイ
スクを製造できると考え、本発明に到達した。 なお希土類−遷移金属アモルフアス層を用いる
光磁気記録デイスクに於いて複屈折率密着性
が重要である理由は希土類−遷移金属アモルフ
アス層にレーザービームを照射し、極カー効果
(Polar kerr effect)を用いて情報の書き込み再
生を行うが、このカー効果に基づくカー回転角
θkが約0.1〜0.5と非常に小さいため複屈折率が大
きいと直径約1μ程度の微少な反転磁化よりなる
情報点の境界が不明瞭になり、書き込み再生消去
等ができなくなる為である基板と薄膜の密着性
に起因する薄膜中の歪と垂直磁化特性の間に密接
な関係があるとされている(H.Takagi et al J.
Appl.Physics 50(3)P1642〜1644参照)ためであ
る。 (本発明の目的) 従つて本発明の目的は、プラスチツク基板を用
いて、光磁気特性がガラス等の無機材料と同等又
はそれ以上で、取り扱い性や、大量生産性に優れ
た光磁気デイスクを提供することにある。 (発明の構成) 本発明の第1の特徴は透明プラスチツク基板上
に希土類−遷移金属のアモルフアス層を支持した
光磁気記録デイスクにおいて、上記透明プラスチ
ツク基板がポリカーボネートである点にある。 上記ポリカーボネートとしては現在工業的に生
産されているものの中でビス(ヒドロキシフエニ
ル)アルカン系ポリカーボネートが好ましい。 ビス(ヒドロキシフエニル)アルカン系ポリカ
ーボネートとは、ビス(4ヒドロキシフエニル)
アルカンのようなヒドロキシジ(単核もしくは複
核アリール)化合物とカーボネートプリカーサー
たとえばホスゲン、ホスメート又はカーボネート
エステルとを反応させて得られる芳香族炭化水素
重合体であり一般式 (但し式中、Aは2価フエノールの2価芳香族
基) で示される。 2価フエノールは官能基として2個の水酸基を
含有し、芳香族の炭素原子にじかに結合してい
る。代表的なものとして、2,2−ビス−(4−
ヒドロキシフエニル)−プロパン、ハイドロキノ
ン、レゾルシノール、2,2−ビス−(4−ヒド
ロキシフエニル)−ペンタン、2,4′ジヒドロキ
シジフエニルメタン、ビス−(2−ヒドロキシフ
エニル)−メタン、ビス−(4−ヒドロキシフエニ
ル)メタン、ビス−(4−ヒドロキシ−5−ニト
ロフエニル)−メタン、1,1−ビス−(4−ヒド
ロキシフエニルエタン)、3,3−ビス−(4−ヒ
ドロキシフエニル)−ペンタン、2,2′−ジヒド
ロキシシエニル、2,6−ジヒドロキシナフタレ
ン、ビス−(4ヒドロキシフエニル)スルホン、
2,4′−ジヒドロキシジフエニルスルホン、5′−
クロル−2,4′ジヒドロキシジフエニルスルホ
ン、ビス−(4−ヒドロキシフエニル)ジフエニ
ルジスルホン、4,4′−ジヒドロキシジフエニル
エーテル、3′ジクロルジフエニルエーテル、4,
4′ジヒドロキシ−2,5−ジエトキシジフエニル
エーテル、2,2(4,4′−ジヒドロキシ−3,
3′、5,5′テトラハロジフエニル)プロパンがあ
る。 カーボネートエステルはジフエニルカーボネー
トが有利であるがジメチルカーボネート、ジメチ
ルカーボネート、ジエチルカーボネート、フエニ
ルメチルカーボネート、フエニルトリルカーボネ
ート、ジ(トリル)カーボネートなども使用する
ことができる。 カーボネートプリカーサーとしてホスゲンのよ
うなカーボニルハイライドを使用した場合には遊
離酸捕捉体の存在下で縮合反応を行ない、カーボ
ネートエステルを使用する場合は減圧下でのエス
テル交換反応によつてポリカーボネートを合成す
ることができる。 ポリカーボネート樹脂の分子量は機械的特性と
成形性とのかね合いで、平均分子量が14000〜
22000であるのが好ましい。すなわち、平均分子
量が14000未満のものでは衝撃強度等の機械的特
性が不足し、22000を超えると溶融粘度が高過ぎ
るため転写性等の光デイスク基板特性が低下す
る。 ポリカーボネート樹脂の溶融時の劣化、分解を
防止するための酸化防止剤を添加することもでき
るが、光デイスク基板の記録媒体への悪影響を無
くするために、添加剤は極力用いないのが望まし
い。 本発明が適用可能な光磁気記録媒体は公知の任
意の希土類−遷移金属アモルフアス合金でよく、
例えばTb−Fe系合金(特公昭57−20691号)、Dy
−Fe系合金(特公昭57−20692号)、Gd−Tb−
Fe系合金(特開昭56−126907号)、Gd−Tb−Dy
−Fe系合金(特開昭57−94948号)、Gd−Co(特
開昭54−121719号)、Tb−Fe−Co系等があげら
れる。これらの希土類−遷移金属アモルフアス層
は蒸着、スパツタリング、イオンプレーテイング
等の方法で形成するのが好ましい。このアモルフ
アス層の厚さは一般に500〜1500Åである。 本発明の第2の特徴は前記ポリカーボネート製
のプラスチツク基板の複屈折(Δnd)の絶対値が
波長632.8nmのHe−Neレーザを用いて常温で測
定した時に25nm以下である点にある。 上記のような複屈折率の低いポリカーボネート
基板は射出成形によつて作ることができる。一般
に、ポリカーボネート樹脂を射出成形で作ると複
屈折率が高くなり、それを防止する方法が特開昭
58−126119号および特開昭58−180553号に記載さ
れている。しかし、これら公報に記載されたポリ
カーボネート基板は直径が130mm以下の小径のも
のであり、130mmを超える大径のポリカーボネー
ト基板の射出成形法は本出願人の同時出願である
特願昭(59−12565)号(特公平3−41048号公
報)に開示されており、詳細はこの出願明細書を
参照されたい。 上記本出願人による上記特願昭 号に記載されたポリカーボネート基板の射出成
形法の要点は下記の点にある: 偏平環状キヤビテイーの中心部より溶融したポ
リカーボネート樹脂を射出して厚さdが1.0mm〜
2.0mmで半径Rが65mm以下且つ175mm以下である高
密度情報記録担体用ポリカーボネート製デイスク
基板の射出成形方法において、 1 ポリカーボネート樹脂として平均分子量が
14000〜22000のポリカーボネートを用い、射出
シリンダー温度Tを330〜400℃に設定し、金型
温度を80〜130℃に設定し、かつ射出シリンダ
ー内でのポリカーボネート樹脂の滞留時間
(t:単位=分)が t≦14−1/10(T−300) 〔ここで、Tは上記射出シリンダー温度(単
位=℃)〕となるようにする。 2 射出工程における射出速度すなわちキヤビテ
イー内への流入速度(v:単位=ml/秒)を
R/dを等間隔目盛の横軸、vを対数目盛の縦
軸とした片対数表上で下記の領域内に選択す
る: 32.5≦R/d≦100の範囲では、 log2/100(R/d)−1.5log2+1≦log v≦1/10
0(R/d)+1.5 100≦R/d≦175の範囲では、 1/100(R/d)−0.5log2≦log v≦1/100(R
/d)+1.5 3 前記偏平環状キヤビテイーの中心部近傍に設
けたゲートの開口の総断面積(S:単位mm2)を 1/10R/d+10≦S≦2/10R/d+35 (ここでRはデイスクの半径・単位=mm、d
はデイスクの厚さ:単位=mm)にする。 上記成形法によつて作つたポリカーボネート基
板は半径上の40〜170mmの記録領域における複屈
折が2.5nm以下になる。 本発明の光磁気デイスクは第1図に示すよう
に、ポリカーボネート基板1とアモルフアス記録
層2と、表面保護層3とで構成することができる
が、第2図に示すように、本発明の第3の特徴に
よつて、上記ポリカーボネート製プラスチツク基
板と上記アモルフアス層との間にポリマー層4を
設けるのが好ましい。 上記ポリマー層4はポリカーボネート基板との
密着性が強いものでなければならず、本出願人に
よる特願昭58−185094号に記載されたものである
のが好ましい。 上記本出願人の特願昭58−185094号に記載され
ているように、上記ポリマーは架橋性ポリマーで
あるのが好ましく、具体的には、ポリアリル化合
物、多官能性アクリル化合物、熱硬化性樹脂、ア
ルキルシリケート加水分解物およびオルガノポリ
シロキサンが好ましい。 C/N比を向上させるために、上記ポリマー層
とは反対側のアモルフアス層の表面に反射層およ
び/または誘電層を設けることもできる。 また、上記ポリマー層の厚さは0.01〜10μであ
るのが好ましい。 上記ポリマー層を設けることによりアモルフア
ス記録層の垂直磁化特性は大巾に向上し、結果と
して、実用可能なC/N比45dB以上の光磁気デ
イスクが得られる。 以上の説明から明らかなように、 本発明者は光磁気記録デイスクの実用上の問題
であつた。 複屈折(Δnd)が高いことに起因する信号/
雑音比(C/N)の低下と、 ポリカーボネート基板と光磁気記録媒体との
密着性の悪さに起因する垂直磁化特性の低下と
を一挙に解決して、実用可能な光磁気デイスク
を完成させたものである。 以上、本発明を実施例によつて説明するが、先
ず、実施例中に記載された諸物性の測定法を説明
する。 (イ) 複屈折:He−Neレーザーを光源としてセナ
ルモン補償器(λ/4波長板)を用い常温で測
定したレターデーシヨンΔndの絶対値で表示し
た。ここでΔnは複屈折率、dは基板の厚さで
ある。 (ロ) Kerr回転角θk及び保磁力Hc: 第3図に示す磁気光学効果測定装置を用いて
測定した。 すなわち、HeNeレーザー1からのレーザー
光線10をポーラライザー2およびビームスプ
リツター3を介して、電磁コイル4の電磁場内
に置かれたサンプル5に当て、反射光をビーム
スプリツター3で分離し、アナライザー6を介
して光検出器7で検知し、増幅器8を介してレ
コーダー9に記録させる。なお、11は上記電
磁コイル4の駆動手段である。 (ハ) C/N:第4図に示す書き込み再生消却装置
により下記条件で測定した。 書き込みレーザーパワー 4〜10mW 再生レーザーパワー 0.8〜1.5mW デイスク回転数 900〜1350rpm キヤリヤー周波数 1MHz 分解能帯域巾 30kHz 印加磁界 200〜1000Oe すなわち、光磁気デイスク1をモーター2で回
転させながら、その表面に波長830nmのレーザー
光を当てる。このレーザー光は信号発生回路6に
よつて駆動される半導体レーザー7からミラー
8、ポーラライザー9、ハーフミラー10を介し
て送られる。デイスク1からの反射光はハーフミ
ラー10で分離され、他のハーフミラー15でさ
らに分離され、各偏光光線は各々アナライザー1
1および光検出器12を介して差動増幅器13に
入れられ、その結果がスペクトルアナライザー1
4に表示される。なお、3は書込み−消去用電磁
コイルで、このコイル3は駆動手段5を介して駆
動される。 (ニ) ポリカーボネートおよびアクリル樹脂の
MFI:JISK−6719に基づいて測定した。 (荷重=3800g、測定温度=230℃) 表示は(g)/10分で表わした。 実施例 1〜3 本出願人の同時願の特願昭59−12565号(特公
平3−41048号公報)に記載された方法を用い、
ポリカーボネート樹脂(MFI=15)を射出成形
機により直径200mm、厚さ1.2mmのデイスク状に成
形した。この基板をクリーンルーム内でフレオン
により洗浄した後、日本真空技術(株)製RFマ
グネトロンスパツタリング装置を用い、希土類−
遷移金属アモルフアス垂直磁化膜を約1000Å及び
保護膜を約1500Å形成し物性測定に供した。結果
を表−1に示す。 実施例 4 実施例1に記載の方法で、ポリカーボネート基
板を成形しこれに特願昭58−185094号実施例2記
載のダイセル化学製ポリオルガノシロキサン膜を
0.2μ形成した後、実施例1〜3と同様にアモルフ
アス垂直磁化膜を約1000Å及び保護膜を約1500Å
形成した後物性を測定した結果を表−1に示す。 比較例 1〜2 ポリカーボネート樹脂(MFI−15)を従来方
法に従つて射出成形し基板デイスクを得た。これ
を実施例と同一条件でアモルフアス垂直磁化膜を
約1000Å及び保護膜を約1500Å形成したが、表−
1に記載されている如く、C/Nを測定すること
ができなかつた。 比較例 3〜4 基板として、ポリメチルメタクリル樹脂
(MFI=2)を射出成形して直径200mm厚さ1.2mm
のデイスク基板を得た。別に直径200mm厚さ1.2mm
のホウ硅酸ガラス製デイスクを準備した。実施例
と同一条件でスパツタリングによりアモルフアス
垂直磁化膜を約1000Å及び保護膜を約1500Å形成
し物性を測定した。結果を表−1に示す。
(Industrial Application Field) The present invention relates to a magnetic thin film recording disk using polycarbonate as a substrate and used in magneto-optical memories, magnetic recording display elements, etc. (Prior art) Vacuum deposition of rare earth-transition metal amorphous layer,
A magneto-optical recording method involves forming an amorphous layer on a substrate by means such as sputtering or ion plating, writing and erasing information using a thermomagnetic effect by applying a laser beam to this amorphous layer, and reading information using the thermomagnetic effect. It is publicly known,
As the substrate for forming the amorphous layer, a glass plate, a transparent plastic plate such as acrylic resin or polycarbonate resin, and a metal plate made of an opaque material such as aluminum or silicon wafer have been proposed. However, while these various substrates have been proposed,
In the case of a glass substrate, it is possible to form an amorphous layer that can be perpendicularly magnetized, but in the case of a magneto-optical recording disk, the weight of the disk increases and there is a risk of damage if it is accidentally dropped.
It is unsuitable for industrial production because it cannot withstand high-speed rotation and cannot directly form guide grooves used for laser beam tracking, which is expensive. On the other hand, metal materials such as aluminum and silicon wafers can also be used to form an amorphous layer that can be perpendicularly magnetized in the same way as glass, but in the case of silicon, which requires surface polishing like glass, it is very expensive. Large area cannot be produced. Since it is opaque, and guide grooves used for laser beam tracking cannot be directly formed, it cannot be written on or reproduced from the substrate like transparent materials. Therefore, there is a drawback that the signal/noise ratio (S/N ratio) is greatly affected by dust or scratches attached to the surface. Furthermore, in the case of transparent plastic materials such as acrylic resin and polycarbonate, the formation technology for amorphous perpendicular magnetization films has not been established, and there are also the following drawbacks: Acrylic resin has sufficient optical performance. However, it has the disadvantage that it absorbs a large amount of moisture, causing deformation due to moisture absorption, and also suffers from large thermal deformation, depending on the molding conditions. Due to these deformations, the perpendicularly magnetized film and the SiO 2 , TiO 2 , Al 2 O 3 , Ta 2 formed thereon are
Cracks may occur in the protective film of O 5 , MgF 2, etc.
These thin films tend to peel off from the substrate. Another drawback is that the adhesion between the thin film and the acrylic resin is very low compared to glass or metal, and even lower than other plastic materials. Although polycarbonate resin has less hygroscopic deformation and thermal deformation than acrylic resin, it has optical disadvantages of high birefringence and low thin film adhesion. There are other transparent plastics, but styrene resins have even higher birefringence than polycarbonate, vinyl chloride resins have problems with thin film corrosion due to residual chlorine and optical performance, and polyester resins have optical transparency and Each of these materials has its own problems with birefringence, and all of these materials have drawbacks as substrates for magneto-optical recording disks, so they have not been put to practical use at present. Therefore, it is strongly desired to establish a technology for producing magneto-optical recording disks by forming a stable perpendicular magnetization film on a plastic substrate, which is excellent in mass productivity and easy to handle. The present inventors have found that among plastic materials, polycarbonate resin has the best overall physical properties, and if the problems of birefringence and adhesion are improved, it will be possible to solve this problem by The present invention was developed based on the belief that it would be possible to produce a magneto-optical recording disk that is as good as or better than an inorganic substrate. The reason why birefringence adhesion is important in a magneto-optical recording disk using a rare earth-transition metal amorphous layer is that the rare earth-transition metal amorphous layer is irradiated with a laser beam and the Polar Kerr effect is used to However, since the Kerr rotation angle θk based on the Kerr effect is very small at approximately 0.1 to 0.5, if the birefringence is large, the boundary of the information point is formed by a minute reversed magnetization with a diameter of approximately 1μ. It is said that there is a close relationship between the strain in the thin film caused by the adhesion between the thin film and the substrate and the perpendicular magnetization characteristics (H. Takagi et al. J.
Appl.Physics 50(3)P1642-1644). (Object of the present invention) Therefore, the object of the present invention is to create a magneto-optical disk using a plastic substrate, which has magneto-optical properties equivalent to or better than those of inorganic materials such as glass, and which is easy to handle and can be mass-produced. It is about providing. (Structure of the Invention) The first feature of the present invention is that in a magneto-optical recording disk in which an amorphous layer of rare earth-transition metal is supported on a transparent plastic substrate, the transparent plastic substrate is made of polycarbonate. Among the polycarbonates currently produced industrially, bis(hydroxyphenyl)alkane polycarbonates are preferred. Bis(hydroxyphenyl)alkane polycarbonate is bis(4-hydroxyphenyl)
An aromatic hydrocarbon polymer obtained by reacting a hydroxy di(mononuclear or dinuclear aryl) compound such as an alkane with a carbonate precursor such as phosgene, phosmate or carbonate ester, and has the general formula (In the formula, A is a divalent aromatic group of divalent phenol.) Divalent phenol contains two hydroxyl groups as functional groups and is directly bonded to an aromatic carbon atom. A typical example is 2,2-bis-(4-
hydroxyphenyl)-propane, hydroquinone, resorcinol, 2,2-bis-(4-hydroxyphenyl)-pentane, 2,4'dihydroxydiphenylmethane, bis-(2-hydroxyphenyl)-methane, bis- (4-hydroxyphenyl)methane, bis-(4-hydroxy-5-nitrophenyl)-methane, 1,1-bis-(4-hydroxyphenylethane), 3,3-bis-(4-hydroxyphenyl) )-pentane, 2,2'-dihydroxycyenyl, 2,6-dihydroxynaphthalene, bis-(4hydroxyphenyl)sulfone,
2,4'-dihydroxydiphenyl sulfone, 5'-
Chlor-2,4'dihydroxydiphenyl sulfone, bis-(4-hydroxyphenyl)diphenyldisulfone, 4,4'-dihydroxydiphenyl ether, 3'dichlorodiphenyl ether, 4,
4'dihydroxy-2,5-diethoxydiphenyl ether, 2,2(4,4'-dihydroxy-3,
3',5,5'tetrahalodiphenyl)propane. Diphenyl carbonate is advantageously used as the carbonate ester, but dimethyl carbonate, dimethyl carbonate, diethyl carbonate, phenylmethyl carbonate, phenyltolyl carbonate, di(tolyl) carbonate and the like can also be used. When a carbonyl hydride such as phosgene is used as a carbonate precursor, the condensation reaction is carried out in the presence of a free acid scavenger, and when a carbonate ester is used, the polycarbonate is synthesized by transesterification under reduced pressure. be able to. The molecular weight of polycarbonate resin is a balance between mechanical properties and moldability, and the average molecular weight is 14,000 ~
Preferably it is 22000. That is, if the average molecular weight is less than 14,000, mechanical properties such as impact strength are insufficient, and if it exceeds 22,000, the melt viscosity is too high, resulting in a decrease in optical disk substrate properties such as transferability. Although it is possible to add an antioxidant to prevent deterioration and decomposition of the polycarbonate resin during melting, it is desirable to avoid using additives as much as possible in order to eliminate any adverse effects on the recording medium of the optical disk substrate. The magneto-optical recording medium to which the present invention is applicable may be any known rare earth-transition metal amorphous alloy,
For example, Tb-Fe alloy (Special Publication No. 57-20691), Dy
-Fe-based alloy (Special Publication No. 57-20692), Gd-Tb-
Fe-based alloy (JP-A-56-126907), Gd-Tb-Dy
-Fe-based alloys (JP-A-57-94948), Gd-Co (JP-A-54-121719), Tb-Fe-Co, etc. These rare earth-transition metal amorphous layers are preferably formed by methods such as vapor deposition, sputtering, and ion plating. The thickness of this amorphous layer is generally 500-1500 Å. A second feature of the present invention is that the absolute value of birefringence (Δnd) of the polycarbonate plastic substrate is 25 nm or less when measured at room temperature using a He--Ne laser with a wavelength of 632.8 nm. A polycarbonate substrate with a low birefringence as described above can be made by injection molding. In general, when polycarbonate resin is made by injection molding, it has a high birefringence, and a method to prevent this has been proposed in Japanese Patent Application Laid-Open No.
58-126119 and Japanese Patent Application Laid-open No. 58-180553. However, the polycarbonate substrates described in these publications have a small diameter of 130 mm or less, and the injection molding method for polycarbonate substrates with a large diameter exceeding 130 mm is disclosed in Japanese Patent Application No. 59-12565 filed simultaneously by the present applicant. ) (Japanese Patent Publication No. 3-41048), and please refer to the specification of this application for details. The key points of the injection molding method for polycarbonate substrates described in the above patent application No. 1 by the applicant are as follows: Molten polycarbonate resin is injected from the center of the flat annular cavity to form a mold with a thickness d of 1.0 mm. ~
In an injection molding method for a polycarbonate disk substrate for a high-density information recording carrier having a diameter R of 2.0 mm and a radius R of 65 mm or less and 175 mm or less, 1. The average molecular weight of the polycarbonate resin is
14,000 to 22,000 polycarbonate, the injection cylinder temperature T was set to 330 to 400°C, the mold temperature was set to 80 to 130°C, and the residence time of the polycarbonate resin in the injection cylinder (t: unit = min. ) is set so that t≦14-1/10 (T-300) [Here, T is the above-mentioned injection cylinder temperature (unit=°C)]. 2 The injection speed in the injection process, that is, the inflow speed into the cavity (v: unit = ml/sec), is expressed as follows on a semi-logarithmic table with R/d as the horizontal axis of the evenly spaced scale and v as the vertical axis of the logarithmic scale. Select within the range: In the range of 32.5≦R/d≦100, log2/100 (R/d)-1.5log2+1≦log v≦1/10
0(R/d)+1.5 In the range of 100≦R/d≦175, 1/100(R/d)−0.5log2≦log v≦1/100(R
/d)+1.5 3 The total cross-sectional area (S: unit mm 2 ) of the gate opening provided near the center of the flat annular cavity is 1/10R/d+10≦S≦2/10R/d+35 (here, R is the radius of the disk, unit = mm, d
is the thickness of the disk (unit = mm). The polycarbonate substrate made by the above molding method has birefringence of 2.5 nm or less in the recording area of 40 to 170 mm on the radius. As shown in FIG. 1, the magneto-optical disk of the present invention can be composed of a polycarbonate substrate 1, an amorphous recording layer 2, and a surface protective layer 3. However, as shown in FIG. According to feature 3, it is preferable to provide a polymer layer 4 between the polycarbonate plastic substrate and the amorphous layer. The polymer layer 4 must have strong adhesion to the polycarbonate substrate, and is preferably the one described in Japanese Patent Application No. 185094/1985 by the present applicant. As described in the applicant's Japanese Patent Application No. 185094/1985, the polymer is preferably a crosslinkable polymer, and specifically, polyallyl compounds, polyfunctional acrylic compounds, thermosetting resins, etc. , alkyl silicate hydrolysates and organopolysiloxanes are preferred. In order to improve the C/N ratio, a reflective layer and/or a dielectric layer can also be provided on the surface of the amorphous layer opposite to the polymer layer. Further, the thickness of the polymer layer is preferably 0.01 to 10μ. By providing the above-mentioned polymer layer, the perpendicular magnetization characteristics of the amorphous recording layer are greatly improved, and as a result, a magneto-optical disk with a practical C/N ratio of 45 dB or more can be obtained. As is clear from the above description, the inventor of the present invention was concerned with a practical problem with magneto-optical recording disks. Signal due to high birefringence (Δnd) /
We have completed a practical magneto-optical disk by solving the problem of a decrease in the noise ratio (C/N) and a decrease in perpendicular magnetization characteristics caused by poor adhesion between the polycarbonate substrate and the magneto-optical recording medium. It is something. The present invention will be described above with reference to Examples. First, methods for measuring the various physical properties described in the Examples will be explained. (a) Birefringence: Expressed as the absolute value of retardation Δnd measured at room temperature using a Senarmont compensator (λ/4 wavelength plate) using a He--Ne laser as a light source. Here, Δn is the birefringence index, and d is the thickness of the substrate. (b) Kerr rotation angle θk and coercive force Hc: Measured using the magneto-optical effect measuring device shown in FIG. That is, a laser beam 10 from a HeNe laser 1 is applied to a sample 5 placed within the electromagnetic field of an electromagnetic coil 4 via a polarizer 2 and a beam splitter 3, and the reflected light is separated by the beam splitter 3 and sent to an analyzer 6. It is detected by a photodetector 7 via an amplifier 8 and recorded by a recorder 9. Note that 11 is a driving means for the electromagnetic coil 4. (c) C/N: Measured under the following conditions using the writing/reproducing/erasing device shown in FIG. Writing laser power 4 to 10 mW Reproduction laser power 0.8 to 1.5 mW Disk rotation speed 900 to 1350 rpm Carrier frequency 1 MHz Resolution bandwidth 30 kHz Applied magnetic field 200 to 1000 Oe In other words, while the magneto-optical disk 1 is rotated by the motor 2, a wavelength of 830 nm is applied to the surface of the magneto-optical disk 1. shine a laser beam on it. This laser light is sent from a semiconductor laser 7 driven by a signal generation circuit 6 via a mirror 8, a polarizer 9, and a half mirror 10. The reflected light from the disk 1 is separated by a half mirror 10, further separated by another half mirror 15, and each polarized light beam is sent to an analyzer 1.
1 and a photodetector 12 into a differential amplifier 13, and the result is sent to a spectrum analyzer 1.
4 will be displayed. Note that 3 is a write-erase electromagnetic coil, and this coil 3 is driven via a drive means 5. (d) Polycarbonate and acrylic resin
MFI: Measured based on JISK-6719. (Load = 3800g, measurement temperature = 230°C) The display is (g)/10 minutes. Examples 1 to 3 Using the method described in Japanese Patent Application No. 59-12565 (Japanese Patent Publication No. 3-41048) filed concurrently by the present applicant,
Polycarbonate resin (MFI = 15) was molded into a disk shape with a diameter of 200 mm and a thickness of 1.2 mm using an injection molding machine. After cleaning this substrate with Freon in a clean room, rare earth sputtering was performed using an RF magnetron sputtering device manufactured by Japan Vacuum Technology Co., Ltd.
A transition metal amorphous perpendicular magnetization film with a thickness of about 1000 Å and a protective film with a thickness of about 1500 Å were formed and used for physical property measurements. The results are shown in Table-1. Example 4 A polycarbonate substrate was molded by the method described in Example 1, and a polyorganosiloxane film manufactured by Daicel Chemical Co., Ltd. described in Example 2 of Japanese Patent Application No. 185094/1982 was applied to it.
After forming 0.2 μm, the amorphous perpendicular magnetization film was formed to a thickness of about 1000 Å and the protective film was formed to a thickness of about 1500 Å, as in Examples 1 to 3.
Table 1 shows the results of measuring the physical properties after formation. Comparative Examples 1-2 A substrate disk was obtained by injection molding polycarbonate resin (MFI-15) according to a conventional method. An amorphous perpendicular magnetization film of about 1000 Å and a protective film of about 1500 Å were formed under the same conditions as in the example.
As described in 1, it was not possible to measure the C/N. Comparative Examples 3 to 4 Injection molded polymethyl methacrylic resin (MFI=2) as a substrate with a diameter of 200 mm and a thickness of 1.2 mm.
A disk substrate was obtained. Separately diameter 200mm thickness 1.2mm
A borosilicate glass disk was prepared. An amorphous perpendicular magnetization film with a thickness of about 1000 Å and a protective film with a thickness of about 1500 Å were formed by sputtering under the same conditions as in Examples, and the physical properties were measured. The results are shown in Table-1.

【表】 表1より明らかななように、本発明による複屈
折率が25nm以下のポリカーボネート基板を用い
た場合にのみ良好なC/N比の光磁気デイスクが
得られ、特に、本発明のポリマー層を介在させる
ことによつてC/N比はさらに向上させることが
できる。
[Table] As is clear from Table 1, a magneto-optical disk with a good C/N ratio can be obtained only when the polycarbonate substrate of the present invention having a birefringence of 25 nm or less is used. The C/N ratio can be further improved by interposing a layer.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は本発明の実施例のデイスク構成の概略
図。第2図は本発明の他の実施例のデイスク構成
の概略図。第3図は磁気光学定数測定装置の概略
図。第4図は光磁気デイスクの書き込み再生消去
装置の構成図。 図中符号、1……ポリカーボネート基板、2…
…アモルフアス記録層、3……表面保護層、4…
…ポリマー層。
FIG. 1 is a schematic diagram of a disk configuration according to an embodiment of the present invention. FIG. 2 is a schematic diagram of a disk configuration according to another embodiment of the present invention. FIG. 3 is a schematic diagram of the magneto-optical constant measuring device. FIG. 4 is a configuration diagram of a magneto-optical disk writing/reproducing/erasing device. Symbols in the figure, 1... polycarbonate substrate, 2...
...Amorphous recording layer, 3...Surface protection layer, 4...
...polymer layer.

Claims (1)

【特許請求の範囲】 1 透明なポリカーボネート基板上に希土類−遷
移金属のアモルフアス層を支持した光磁気記録デ
イスクにおいて、 上記ポリカーボネートのプラスチツク基板の複
屈折(Δnd)の絶対値が波長632.8nmのHe−Ne
レーザを用いて常温で測定した時に25nm以下で
あることを特徴とする光磁気記録デイスク。 2 ポリカーボネート製プラスチツク基板と上記
アモルフアス層との間にポリマー層が設けられて
いる特許請求の範囲第1項に記載の光磁気記録デ
イスク。 3 ポリカーボネート製プラスチツク基板が下記
条件で射出成形された基板である特許請求の範囲
第1項に記載の光磁気記録デイスク: (a) 平均分子量が14000〜22000のポリカーボネー
トを用い、 (b) 射出シリンダー温度Tを330〜400℃に設定
し、金型温度を80〜130℃に設定しかつ射出シ
リンダー内でのポリカーボネート樹脂の滞留時
間(t:単位=分)を t≦14−1/10(T−300) (ここで、Tは射出シリンダー温度(単位=
℃) となるように設定し、 (c) 射出工程における射出速度すなわちキヤビテ
イー内への流入速度(v:単位=ml/秒)を
R/dを等間隔目盛の横軸、vを対数目盛の縦
軸とした片対数表上で下記の領域内に選択す
る: 32.5≦R/d≦100の範囲では、 log2/100R/d−1.5log2 +1≦log v≦1/100R/d+1.5 100≦R/d≦175の範囲では、 1/100R/d−0.5log2≦log v ≦1/100R/d+1.5 (d) 偏平環状キヤビテイーの中心部近傍に設けた
ゲートの開口の総断面積(s:単位md)を 1R/10d+10≦S≦2/10R/d+35 (ここでRはデイスクの半径・単位=mm、dは
デイスクの厚さ:単位=mm) にする。
[Claims] 1. In a magneto-optical recording disk in which an amorphous layer of rare earth-transition metal is supported on a transparent polycarbonate substrate, the absolute value of the birefringence (Δnd) of the polycarbonate plastic substrate is He- with a wavelength of 632.8 nm. Ne
A magneto-optical recording disk characterized by a diameter of 25 nm or less when measured using a laser at room temperature. 2. The magneto-optical recording disk according to claim 1, wherein a polymer layer is provided between the polycarbonate plastic substrate and the amorphous layer. 3. The magneto-optical recording disk according to claim 1, wherein the polycarbonate plastic substrate is injection molded under the following conditions: (a) using polycarbonate having an average molecular weight of 14,000 to 22,000; (b) an injection cylinder; The temperature T was set at 330-400℃, the mold temperature was set at 80-130℃, and the residence time (t: unit = minutes) of the polycarbonate resin in the injection cylinder was set at t≦14-1/10 (T −300) (where T is the injection cylinder temperature (unit =
(c) The injection speed in the injection process, that is, the inflow speed into the cavity (v: unit = ml/sec), where R/d is the horizontal axis of the evenly spaced scale, and v is the horizontal axis of the logarithmic scale. Select within the following range on the semi-logarithm table with the vertical axis: In the range of 32.5≦R/d≦100, log2/100R/d−1.5log2 +1≦log v≦1/100R/d+1.5 100≦ In the range of R/d≦175, 1/100R/d−0.5log2≦log v≦1/100R/d+1.5 (d) Total cross-sectional area of the opening of the gate provided near the center of the flat annular cavity (s : Unit md) is set to 1R/10d+10≦S≦2/10R/d+35 (where R is the radius of the disk, unit = mm, and d is the thickness of the disk, unit = mm).
JP1256684A 1984-01-26 1984-01-26 Photomagnetic recording disk Granted JPS60157747A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1256684A JPS60157747A (en) 1984-01-26 1984-01-26 Photomagnetic recording disk

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1256684A JPS60157747A (en) 1984-01-26 1984-01-26 Photomagnetic recording disk

Related Child Applications (3)

Application Number Title Priority Date Filing Date
JP27909493A Division JPH06342537A (en) 1993-10-12 1993-10-12 Magneto-optical recording disk
JP5279095A Division JPH0746445B2 (en) 1993-10-12 1993-10-12 Magneto-optical recording disk and manufacturing method thereof
JP27909693A Division JPH06318347A (en) 1993-10-12 1993-10-12 Magneto-optical recording disk

Publications (2)

Publication Number Publication Date
JPS60157747A JPS60157747A (en) 1985-08-19
JPH0437490B2 true JPH0437490B2 (en) 1992-06-19

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ID=11808900

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Country Link
JP (1) JPS60157747A (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0620784B2 (en) * 1986-03-26 1994-03-23 三菱化成株式会社 Method for manufacturing optical disk substrate made of polycarbonate resin
JP2543832B2 (en) * 1986-09-03 1996-10-16 ティーディーケイ株式会社 Magneto-optical recording medium
JP2604381B2 (en) * 1987-07-22 1997-04-30 日本電気株式会社 Magneto-optical recording device
JPH06342537A (en) * 1993-10-12 1994-12-13 Daicel Chem Ind Ltd Magneto-optical recording disk
JP2568978B2 (en) * 1993-11-30 1997-01-08 株式会社ソルベックス Universal test equipment

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5538655A (en) * 1978-09-08 1980-03-18 Sumitomo Chem Co Ltd Optical signal recording and reproducing member
JPS56169240A (en) * 1980-05-29 1981-12-25 Sharp Corp Manufacture of magnetooptical storage disk

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