JP2698852B2 - Magneto-optical recording method - Google Patents
Magneto-optical recording methodInfo
- Publication number
- JP2698852B2 JP2698852B2 JP63048407A JP4840788A JP2698852B2 JP 2698852 B2 JP2698852 B2 JP 2698852B2 JP 63048407 A JP63048407 A JP 63048407A JP 4840788 A JP4840788 A JP 4840788A JP 2698852 B2 JP2698852 B2 JP 2698852B2
- Authority
- JP
- Japan
- Prior art keywords
- recording
- magneto
- groove
- optical recording
- guide groove
- 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
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording 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
- G11B11/10—Recording 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
- G11B11/105—Recording 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
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording 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
- G11B11/10—Recording 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
- G11B11/105—Recording 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
- G11B11/10582—Record carriers characterised by the selection of the material or by the structure or form
- G11B11/10584—Record carriers characterised by the selection of the material or by the structure or form characterised by the form, e.g. comprising mechanical protection elements
Description
【発明の詳細な説明】 〔技術分野〕 本発明は光磁気記録方法に関するものであり、特に光
磁気記録媒体に磁界変調方式により記録を行う光磁気記
録方法に関するものである。Description: TECHNICAL FIELD The present invention relates to a magneto-optical recording method, and more particularly to a magneto-optical recording method for performing recording on a magneto-optical recording medium by a magnetic field modulation method.
〔従来技術〕 光磁気記録は光変調方式が一般的であるが、この方法
はオーバーライトできないという欠点がある。[Prior Art] Magneto-optical recording generally uses an optical modulation method, but this method has a drawback that overwriting cannot be performed.
磁界変調方式によればオーバーライトは簡単である
が、信頼性を高めるためにサンドイッチ構造又は厚い保
護膜をつけた場合には磁気ヘッドを媒体面から離さざる
をえず、そのために磁気ヘッドで発生させる磁束が増
し、磁気ヘッドの消費電力が大きくなって現実的ではな
い。According to the magnetic field modulation method, overwriting is easy, but if a sandwich structure or a thick protective film is attached to improve reliability, the magnetic head must be separated from the medium surface, and as a result, it is generated by the magnetic head This increases the magnetic flux to be applied and increases the power consumption of the magnetic head, which is not practical.
空気浮上等の手段により、磁気ヘッドを近接させれば
上記の問題は解決されるが、サンドイッチ構造又は厚い
保護膜は使えず、記録媒体(磁気記録層、ガイドトラッ
ク、誘電層、反射層等)がほとんどむき出しになり、そ
の上、記録時には磁気ヘッドが接触に近い状態にあるた
め、すでに記録された情報および記録媒体自体が破壊さ
れる危険があり、信頼性に欠ける。特にTb−Fe系アモル
ファス膜の場合、歪応力により磁化が反転する性質があ
り、わずかな接触でも記録情報が破壊される危険があっ
た。The above problem can be solved by bringing the magnetic head close by means such as air levitation, but the sandwich structure or the thick protective film cannot be used, and the recording medium (magnetic recording layer, guide track, dielectric layer, reflection layer, etc.) In addition, since the magnetic head is almost in contact with the magnetic head at the time of recording, there is a danger that the already recorded information and the recording medium itself may be destroyed, and the reliability is lacking. In particular, in the case of a Tb-Fe-based amorphous film, there is a property that magnetization is reversed by strain stress, and there is a risk that recorded information is destroyed even by a slight contact.
本発明は、記録面がむき出しあるいはむき出しに近い
状態になっている光磁気記録媒体に、磁界変調方式によ
り磁気ヘッドを記録媒体に近接させて記録を行う光磁気
記録方法において、記録時のヘッドの媒体面への衝突
や、他の取扱い時の接触等による、すでに記録されてい
る情報の損傷や、磁気記録層、案内溝(ガイドトラッ
ク)、誘電層、反射層等の記録媒体そのものの破壊を防
止することにより、光磁気記録の信頼性を向上させるこ
とを目的とする。The present invention relates to a magneto-optical recording method in which a magnetic head is brought close to a recording medium by a magnetic field modulation method on a magneto-optical recording medium whose recording surface is bare or almost bare, Damage to already recorded information due to collision with the medium surface or contact during other handling, and destruction of the recording medium itself such as the magnetic recording layer, guide groove (guide track), dielectric layer and reflective layer. An object of the present invention is to improve the reliability of magneto-optical recording by preventing such a phenomenon.
本発明者は、前記目的を達成するために鋭意研究した
結果、案内溝を有する光磁気記録媒体に磁界印加手段を
用いる磁界変調方式により記録を行う光磁気記録方法に
おいて、前記光磁気記録媒体の案内溝が、λ/4n(λ=
読出し又は記録に使用するレーザ光の波長)(n=案内
溝を形成する部分の屈折率)より深い構造を有してお
り、記録の際には前記案内溝の溝部に磁界印加手段を近
接させて記録することを特徴とする光磁気記録方法を提
供することによって前記目的が達成できることを見出し
た。The present inventors have conducted intensive studies to achieve the above object, and as a result, in a magneto-optical recording method for performing recording on a magneto-optical recording medium having a guide groove by a magnetic field modulation method using a magnetic field applying means, The guide groove is λ / 4n (λ =
It has a structure that is deeper than the wavelength of the laser beam used for reading or recording (n = refractive index of the portion forming the guide groove). When recording, the magnetic field applying means is brought close to the groove of the guide groove. It has been found that the above-mentioned object can be achieved by providing a magneto-optical recording method characterized by performing recording.
案内溝(ガイドトラック)付光ディスクにおいて、溝
の深さとトラックエラー信号との関係はほぼ第1図の様
になる(実際には溝の形状によって、溝が深くなるに従
って第1図よりややトラックエラー信号が減少するのが
普通である)。トラックエラー信号はλ/8nの時に最大
となるが、RF信号強度との関係でλ/8nよりややずれた
ところに設計するのが通例であるが、記録方式等の違い
によりその深さはいろいろである。しかし、いずれの場
合にも、従来は溝の深さをλ/4nより浅く設計してい
た。その理由としてはトラックエラー信号、RF信号、ノ
イズの問題、加工の容易さ、いずれをとってもλ/4nよ
り深くする利点がなかったからである。In an optical disc with a guide groove (guide track), the relationship between the groove depth and the track error signal is almost as shown in FIG. 1 (actually, as the groove becomes deeper, the track error slightly increases as shown in FIG. Usually the signal is reduced). The track error signal is maximum at λ / 8n, but it is customary to design it slightly off λ / 8n in relation to the RF signal strength, but the depth varies depending on the recording method etc. It is. However, in any case, the depth of the groove was conventionally designed to be shallower than λ / 4n. The reason for this is that there was no advantage in making the track depth deeper than λ / 4n in any case of the track error signal, the RF signal, the problem of noise, and the ease of processing.
従来は光ディスクにおいて記録層は完全に保護されて
いて、外からの接触、損傷等は考えられなかったが、磁
気ヘッドを近接させ、磁界変調方式により記録を行う光
磁気ディスクにおいては厚い保護層はつけられず、接
触、損傷の危険は避けられない。特にTb−Fe系のアモル
ファス膜の場合は歪により磁化が反転する特性があり、
記録層が損傷しない程度のわずかな接触によっても記録
したビットが反転してしまう危険がある。Conventionally, the recording layer of an optical disk was completely protected, and no external contact or damage was considered.However, in a magneto-optical disk in which a magnetic head is brought close to and recording is performed by a magnetic field modulation method, a thick protective layer is not used. They are not attached and the danger of contact and damage is inevitable. In particular, in the case of a Tb-Fe-based amorphous film, there is a characteristic that magnetization is reversed by strain,
There is a danger that the recorded bits may be inverted even by a slight contact that does not damage the recording layer.
このような危険は、第2図に示したようなランド4上
の記録(非溝部への記録)の場合はもちろんのこと、第
3図に示したように溝3の幅を狭くし、溝3とランド4
との両方にかかって記録する場合にその危険性は大き
い。Such danger is caused not only by recording on the land 4 (recording on non-groove portions) as shown in FIG. 2 but also by narrowing the width of the groove 3 as shown in FIG. 3 and land 4
The risk is great when recording both.
第4図に示したように溝3の幅を広くし、ビットを完
全に溝の中に記録してしまう場合においても溝3の深さ
をλ/4n以下に設定すると、溝幅0.8〜1μm程度に対し
て溝の深さは0.13μm以下(λ=780nm、n=1.5の場
合)と非常に浅い溝となる。従って溝の底でも外部から
の接触の危険性が大きい。As shown in FIG. 4, even when the width of the groove 3 is widened and the bit is completely recorded in the groove, if the depth of the groove 3 is set to λ / 4n or less, the groove width is 0.8 to 1 μm. To the extent, the groove depth is 0.13 μm or less (when λ = 780 nm and n = 1.5), resulting in a very shallow groove. Therefore, there is a great risk of contact from outside even at the bottom of the groove.
一般的に好ましい溝の幅は0.4〜1.2μm程度であり、
特に溝内だけに記録する場合には0.8〜1.2μm程度であ
る。Generally preferred groove width is about 0.4 to 1.2 μm,
Particularly, when recording is performed only in the groove, the thickness is about 0.8 to 1.2 μm.
又、アモルファス光磁気膜等の場合は膜内の磁壁の移
動があり、第5図に示すように溝部とランド部が連続的
な膜になっている場合には溝部に物が接触しなくとも、
ランド部で接触等により反転した磁区が溝部まで広が
り、溝部に記録されていた情報ビットを破壊してしまう
こともある。In the case of an amorphous magneto-optical film or the like, the domain wall in the film moves. As shown in FIG. 5, when the groove and the land are continuous films, even if an object does not contact the groove. ,
The magnetic domain reversed at the land portion due to contact or the like spreads to the groove, and the information bit recorded in the groove may be destroyed.
本発明では、第6図に示すように、この溝3をλ/4n
以上に深くすることにより、溝部3の記録層2への外部
からの接触等による損傷の危険性を少なくしたことを特
徴とする。又、このように、溝を深くすることにより、
溝部3とランド部4との磁気記録膜が不連続となり、ラ
ンド部4が磁化反転した時の磁壁移動による溝部3の記
録の損傷の危険も小さくなる。In the present invention, as shown in FIG.
By making the groove deeper, the danger of damage due to external contact of the groove 3 with the recording layer 2 is reduced. Also, by making the groove deeper,
The magnetic recording film between the groove 3 and the land 4 becomes discontinuous, and the danger of damage to the recording of the groove 3 due to domain wall movement when the land 4 reverses magnetization is reduced.
本発明の光磁気記録媒体の構造の種類としては、
(a)磁気記録層/基板、(b)磁気記録層/誘電体層
/基板、(c)前記(a)または(b)の構造のものに
保護層を付加的に有するもの、(d)前記(a)または
(b)の構造のものに反射層を付加的に有するもの、
(e)前記(a)または(b)の構造のものに反射層/
誘電体層を付加的に有するもの、(f)前記(d)また
は(e)の構造のものに保護層を付加的に有するもの等
がある。As the type of the structure of the magneto-optical recording medium of the present invention,
(A) a magnetic recording layer / substrate, (b) a magnetic recording layer / dielectric layer / substrate, (c) one having a protective layer in addition to the structure of (a) or (b), (d) (A) or (b) having an additional reflective layer,
(E) The structure of the above (a) or (b) has a reflective layer /
There are those having an additional dielectric layer, and those (f) having a protective layer in addition to those having the structure (d) or (e).
使用される基板の材質としては、ガラス(コーニング
0313、0317、7059等)、PMMA、ポリカーボネート、エポ
キシ系樹脂等がある。The material of the substrate used is glass (Corning
0313, 0317, 7059, etc.), PMMA, polycarbonate, epoxy resin and the like.
磁気記録層の材質としては、RE−TMアモルファス合金
(Tb−Fe,Ga−Tb−Fe,Tb−Fe−Co,Gd−Tb−Fe−Co,Gd−
Co,Dy−Fe等)、β置換ガーネット、Coスピネルフェラ
イト、マグネトプランバイト型フェライト等がある。As the material of the magnetic recording layer, RE-TM amorphous alloy (Tb-Fe, Ga-Tb-Fe, Tb-Fe-Co, Gd-Tb-Fe-Co, Gd-
Co, Dy-Fe, etc.), β-substituted garnet, Co spinel ferrite, magnetoplumbite ferrite, and the like.
以下、本発明の実施態様の一例を第7図に従って説明
する。Hereinafter, an example of an embodiment of the present invention will be described with reference to FIG.
実施例 厚さ1.2mmのPMMA基板1に幅1μm、ピッチ2μm、
深さ0.3μmの案内溝3を形成し、その上にRFスパッタ
法によりTbFeCoアモルファス合金膜5を磁気記録層とし
て0.1μm厚に形成し、さらにその上に0.2μmのSi3N4
膜6を保護層として形成して光磁気記録媒体を作製し
た。Example A PMMA substrate 1 having a thickness of 1.2 mm was 1 μm wide, 2 μm pitch,
A guide groove 3 having a depth of 0.3 μm is formed, a TbFeCo amorphous alloy film 5 is formed thereon as a magnetic recording layer to a thickness of 0.1 μm by RF sputtering, and a 0.2 μm Si 3 N 4 is further formed thereon.
The magneto-optical recording medium was manufactured by forming the film 6 as a protective layer.
このようにして作製した光磁気記録媒体に磁界印加手
段を用いて磁界変調方式により記録を行い溝部3に情報
を記録した。記録した情報並びに記録層自体の損傷の危
険性はほとんどなかった。Recording was performed on the magneto-optical recording medium manufactured in this manner by a magnetic field modulation method using a magnetic field applying means, and information was recorded in the groove 3. There was little risk of damage to the recorded information or the recording layer itself.
以上述べたように、記録層がむき出しにあるいはむき
出しに近い状態に置かれている光磁気ディスクに磁気ヘ
ッドを近接させて記録を行う場合に、案内溝の深さが、
ある特定の深さより深く設けられていることにより、外
部からの接触等による記録層の損傷又はすでに記録され
ている情報の破壊等が防止でき、信頼性が向上する。As described above, when recording is performed by bringing the magnetic head close to the magneto-optical disk in which the recording layer is exposed or nearly exposed, the depth of the guide groove is
When the recording layer is provided deeper than a specific depth, damage to the recording layer or destruction of already recorded information due to contact from the outside can be prevented, and reliability is improved.
【図面の簡単な説明】 第1図は光ディスクの案内溝の溝の深さとトラックエラ
ー信号との関係を示す。 第2〜5図は従来の光ディスクの説明図である。 第6〜7図は本発明の光ディスクの説明図である。 1……基板、2……磁気記録層 3……案内溝、4……ランド部 5……TbFeCoアモルファス合金膜 6……Si3N4膜BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 shows the relationship between the depth of a guide groove of an optical disc and a track error signal. 2 to 5 are explanatory views of a conventional optical disk. 6 and 7 are explanatory views of the optical disk of the present invention. 1 ...... substrate, 2 ...... magnetic recording layer 3 ...... guide groove, 4 ...... land portion 5 ...... TbFeCo amorphous alloy film 6 ...... Si 3 N 4 film
Claims (1)
手段を用いる磁界変調方式により記録を行う光磁気記録
方法において、前記光磁気記録媒体の案内溝が、λ/4n
(λ=読出し又は記録に使用するレーザ光の波長)(n
=案内溝を形成する部分の屈折率)より深い構造を有し
ており、記録の際には前記案内溝の溝部に磁界印加手段
を近接させて記録することを特徴とする光磁気記録方
法。1. A magneto-optical recording method for performing recording on a magneto-optical recording medium having a guide groove by a magnetic field modulation method using a magnetic field applying means, wherein the guide groove of the magneto-optical recording medium is λ / 4n.
(Λ = wavelength of laser beam used for reading or recording) (n
A magneto-optical recording method having a structure deeper than (= refractive index of a portion forming a guide groove), and performing recording by bringing a magnetic field applying means close to the groove portion of the guide groove during recording.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63048407A JP2698852B2 (en) | 1988-03-01 | 1988-03-01 | Magneto-optical recording method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63048407A JP2698852B2 (en) | 1988-03-01 | 1988-03-01 | Magneto-optical recording method |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH01223650A JPH01223650A (en) | 1989-09-06 |
JP2698852B2 true JP2698852B2 (en) | 1998-01-19 |
Family
ID=12802452
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP63048407A Expired - Lifetime JP2698852B2 (en) | 1988-03-01 | 1988-03-01 | Magneto-optical recording method |
Country Status (1)
Country | Link |
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JP (1) | JP2698852B2 (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1426944A3 (en) * | 1993-04-02 | 2008-01-23 | Canon Kabushiki Kaisha | Method for manufacturing a magneto-optical recording medium |
KR100513437B1 (en) | 2000-05-31 | 2005-09-07 | 마쯔시다덴기산교 가부시키가이샤 | Magneto optical recording medium, manufacturing method for the same, and method and apparatus for reading the same |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01189039A (en) * | 1988-01-22 | 1989-07-28 | Mitsubishi Electric Corp | Optical information recording carrier |
JPH01213842A (en) * | 1988-02-23 | 1989-08-28 | Nippon Telegr & Teleph Corp <Ntt> | Rewriting type optical disk medium |
-
1988
- 1988-03-01 JP JP63048407A patent/JP2698852B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPH01223650A (en) | 1989-09-06 |
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