JPH038023B2 - - Google Patents
Info
- Publication number
- JPH038023B2 JPH038023B2 JP62160671A JP16067187A JPH038023B2 JP H038023 B2 JPH038023 B2 JP H038023B2 JP 62160671 A JP62160671 A JP 62160671A JP 16067187 A JP16067187 A JP 16067187A JP H038023 B2 JPH038023 B2 JP H038023B2
- Authority
- JP
- Japan
- Prior art keywords
- film
- recording
- magneto
- track
- 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
Links
- 239000010408 film Substances 0.000 claims description 42
- 230000005291 magnetic effect Effects 0.000 claims description 19
- 239000000758 substrate Substances 0.000 claims description 15
- 239000010409 thin film Substances 0.000 claims description 11
- 230000005415 magnetization Effects 0.000 claims description 2
- 230000005374 Kerr effect Effects 0.000 description 5
- 230000000694 effects Effects 0.000 description 5
- 229910004298 SiO 2 Inorganic materials 0.000 description 4
- 239000000696 magnetic material Substances 0.000 description 4
- 238000005260 corrosion Methods 0.000 description 3
- 230000007797 corrosion Effects 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 230000003287 optical effect Effects 0.000 description 3
- 125000006850 spacer group Chemical group 0.000 description 3
- 229910016629 MnBi Inorganic materials 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 239000002902 ferrimagnetic material Substances 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- -1 MnBiCu Inorganic materials 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 239000000428 dust Substances 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 229920003217 poly(methylsilsesquioxane) Polymers 0.000 description 1
- 229910052761 rare earth metal Inorganic materials 0.000 description 1
- 238000012827 research and development Methods 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000011232 storage material Substances 0.000 description 1
- 229920003002 synthetic resin Polymers 0.000 description 1
- 239000000057 synthetic resin Substances 0.000 description 1
- 229910052723 transition metal Inorganic materials 0.000 description 1
- 150000003624 transition metals Chemical class 0.000 description 1
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
- G11B11/10582—Record carriers characterised by the selection of the material or by the structure or form
- G11B11/10586—Record carriers characterised by the selection of the material or by the structure or form characterised by the selection of the material
- G11B11/10589—Details
Description
【発明の詳細な説明】
〈技術分野〉
本発明はレーザ光により情報の記録・再生・消
去を行う磁気光学記憶素子に関する。DETAILED DESCRIPTION OF THE INVENTION Technical Field The present invention relates to a magneto-optical storage element that records, reproduces, and erases information using laser light.
〈従来技術〉
近年、高密度・大容量・高速アクセス等種々の
要求を満足し得る光メモリ装置の研究開発が活発
に推進されている。各種光メモリ装置のうちでも
特に記憶材料として垂直磁化膜を用いた磁気光学
記憶装置は不要になつた情報を消去し新しい情報
を再記録出来るという事から注目されている。<Prior Art> In recent years, research and development of optical memory devices that can satisfy various demands such as high density, large capacity, and high speed access have been actively promoted. Among various optical memory devices, magneto-optical memory devices that use perpendicularly magnetized films as storage materials are attracting attention because they can erase information that is no longer needed and re-record new information.
しかし上記の利点を有する一方で磁気光学記憶
装置は再生信号レベルが低いという欠点があり、
特に磁気光学記憶素子からの反射光を利用して情
報の再生を行う所謂カー効果再生方式においては
カー回転角が小さいため信号雑音比(S/N)を
高める事が困難であつた。その為従来では記録媒
体である磁性材料を改良したり或いは記録媒体上
にSiOやSiO2の誘電体膜を形成したりしてカー回
転角を高める工夫がなされていた。そして後者の
例としてMnBi磁性体膜上にSiO膜を形成するこ
とによつてカー回転角が0.7度から3.6度に増大し
た例が報告されている。(J.APPl.Phys.
Vo145no8August1974)。しかしながらこのよう
な磁性体膜上への誘電体膜の形成ではカー回転角
の増大に伴つて反射光量が減退し実質的なS/N
は約2倍程度にしか増大していない。又、SiOや
SiO2等の誘電体膜を形成しただけでは、磁性体
に腐蝕の恐れのある場合はその腐蝕の実質的な防
御とはなり得ない事や記録ビツト径が1μm程度で
あるため1μm程度の小さなほこりやゴミが該誘電
体膜に付着した場合は該ビツト検出が不可能にな
る事等のため、実質的な記録素子とするためには
厚さ0.5〜2.0mm程度のガラス又は透明樹脂を使用
する事が望ましく、そうする事によりカー回転角
の増大(従つてS/Nの増大)の効果も理論値程
の期待はできなくなつた。 However, while having the above advantages, magneto-optical storage devices have the disadvantage that the reproduction signal level is low.
In particular, in the so-called Kerr effect reproduction method in which information is reproduced using reflected light from a magneto-optical storage element, it is difficult to increase the signal-to-noise ratio (S/N) because the Kerr rotation angle is small. Therefore, conventional efforts have been made to increase the Kerr rotation angle by improving the magnetic material of the recording medium or by forming a dielectric film of SiO or SiO 2 on the recording medium. As an example of the latter, it has been reported that the Kerr rotation angle was increased from 0.7 degrees to 3.6 degrees by forming a SiO film on a MnBi magnetic film. (J.APPl.Phys.
Vo145no8August1974). However, when forming a dielectric film on such a magnetic film, the amount of reflected light decreases as the Kerr rotation angle increases, resulting in a substantial S/N ratio.
has increased only about twice. Also, SiO and
Merely forming a dielectric film such as SiO 2 cannot provide substantial protection against corrosion if there is a risk of corrosion in the magnetic material, and since the recording bit diameter is approximately 1 μm, small If dust or dirt adheres to the dielectric film, it will become impossible to detect the bit, so use glass or transparent resin with a thickness of about 0.5 to 2.0 mm to make it a practical recording element. It is desirable to do this, and by doing so, the effect of increasing the Kerr rotation angle (and thus increasing the S/N ratio) cannot be expected to be as great as the theoretical value.
又、光メモリ装置は高密度記録が基本的な条件
であるためその記録ビツト径は上述したごとく
1μm程度であり従つて記録・再生・消去の過程で
フオーカスサーボ、トラツクサーボ等のサーボ技
術が不可欠となる。さもないと記録装置は複雑で
かつ精巧なものとなり実用には適さなくなる。そ
して特にトラツクサーボをかける場合には、信号
の記録トラツクに隣接したサーボ用のガイドトラ
ツクがある事が望ましい(特に記録・再生・消去
を行なうものでは必要である。)。 In addition, since high-density recording is a basic requirement for optical memory devices, the recording bit diameter is as described above.
The diameter is approximately 1 μm, so servo technology such as focus servo and track servo is essential in the recording, reproducing, and erasing processes. Otherwise, the recording device would be complicated and sophisticated and would not be suitable for practical use. Particularly when applying track servo, it is desirable to have a servo guide track adjacent to the signal recording track (this is especially necessary for recording, reproducing, and erasing).
〈目的〉
本発明は以上の点に鑑みなされたものであつ
て、反射光量を減らす事なく磁気光学効果を増大
させしかもサーボ用のガイドトラツクをも形成す
ることを目的とすると同時に、記録媒体である磁
性体薄膜が実質的に腐食される虞れのない磁気光
学記憶素子を提供することを目的とする。<Purpose> The present invention was made in view of the above points, and an object of the present invention is to increase the magneto-optical effect without reducing the amount of reflected light, and also to form a guide track for a servo. It is an object of the present invention to provide a magneto-optical memory element in which there is no risk that a certain magnetic thin film will be substantially corroded.
〈実施例〉
次に本発明の具体的な実施例を以下図面を参照
しながら詳説する。<Examples> Next, specific examples of the present invention will be described in detail with reference to the drawings.
第1図は本発明の一実施例である磁気光学記憶
素子の一部拡大側面断面図である。 FIG. 1 is a partially enlarged side sectional view of a magneto-optical memory element according to an embodiment of the present invention.
同図において符号5は支持基板であつて、この
支持基板5の上にAl,Au,Ag等の反射膜4を形
成する。反射膜4上にはSiO2等の誘電体膜3が
配され、この誘電体膜3上にGdTbFe,
SmTbFe,TbFe,GdDyFe,TbCo,GdCo等の
希土類と遷移金属よりなるアモルフアスフエリ磁
性体の垂直磁化膜を記録トラツク2として帯状に
形成する。例えば磁気光学記憶素子が円盤である
場合は記録トラツク2は同心円状もしくは螺旋状
をなす。こうして反射膜4、誘導体膜3及び記録
トラツク2を形成した支持基板5とガラス又は合
成樹脂の透明な基板1とをスペーサ6を介して、
適当な大きさの間〓部7を設けて、この間〓部7
にガスを充填した上で接合する。ガスとしては
N2又はArガスを用いる。この構成においてガイ
ドトラツクは記録トラツク2の間のガス体部分で
ある。即ち磁化膜2と反射膜4との反射率の相違
によりガイドトラツクと記録トラツク2が区別さ
れている。記録トラツク2を形成する磁性膜2は
充分に薄く、従つて磁性体層に入射した再生光は
磁性体面からの反射によるカー効果と磁性体膜を
通り抜け反射層4で反射され再び磁性体膜を通り
抜けることで起こるフアラデイ効果が合わさるこ
とによつて単なるカー効果のみによる回転角に比
べて数倍回転角が増大し、かつ返り光量はほとん
ど減少しないためS/Nが大きく増大するもので
ある。 In the figure, reference numeral 5 denotes a support substrate, on which a reflective film 4 of Al, Au, Ag, etc. is formed. A dielectric film 3 such as SiO 2 is disposed on the reflective film 4, and GdTbFe, GdTbFe, etc. are disposed on this dielectric film 3.
A perpendicularly magnetized film of an amorphous ferrimagnetic material made of a rare earth element such as SmTbFe, TbFe, GdDyFe, TbCo, or GdCo and a transition metal is formed in a strip shape as a recording track 2. For example, when the magneto-optical storage element is a disk, the recording track 2 has a concentric or spiral shape. The supporting substrate 5 on which the reflective film 4, the dielectric film 3, and the recording track 2 have been formed in this way is connected to the transparent substrate 1 made of glass or synthetic resin via a spacer 6.
A section 7 of an appropriate size is provided, and the section 7 is
are filled with gas and then bonded. As a gas
Use N2 or Ar gas. In this configuration, the guide track is the gas body section between the recording tracks 2. That is, the guide track and the recording track 2 are distinguished from each other by the difference in reflectance between the magnetized film 2 and the reflective film 4. The magnetic film 2 forming the recording track 2 is sufficiently thin, so that the reproducing light incident on the magnetic layer is reflected by the Kerr effect from the magnetic surface, passes through the magnetic film, is reflected by the reflective layer 4, and returns to the magnetic film. Due to the combination of the Faraday effect caused by passing through the light, the rotation angle increases several times compared to the rotation angle due to the Kerr effect alone, and the amount of returned light hardly decreases, so the S/N ratio increases greatly.
以上素子の作成は次の様にして行なう。 The above element is produced as follows.
支持基板5の上に反射膜4、SiO2等の誘電体
膜3を形成し、更に垂直磁化膜による帯状の記録
トラツク2を形成しその4層構造からなる記録素
子と透明な基板1とをスペーサー6を介して重ね
合わせる構造をとる。そして記録トラツクと保護
板との間隙部7にN2又はArガスを充填する。 A reflective film 4 and a dielectric film 3 such as SiO 2 are formed on a supporting substrate 5, and a strip-shaped recording track 2 is formed by a perpendicular magnetization film, and a recording element having a four-layer structure and a transparent substrate 1 are connected to each other. A structure is adopted in which they are overlapped with a spacer 6 in between. Then, the gap 7 between the recording track and the protection plate is filled with N 2 or Ar gas.
この実施例において、ガイドトラツクは記録ト
ラツク2の間の透明な部分であり、記録トラツク
2と反射膜4との反射率の差によりガイドトラツ
クと記録トラツクとの区別を行う。 In this embodiment, the guide track is a transparent portion between the recording tracks 2, and the guide track and the recording track are distinguished from each other by the difference in reflectance between the recording track 2 and the reflective film 4.
以上の実施例の構成以外にも本発明の主旨の範
囲内で種々の構成の変更は可能である。 In addition to the configurations of the above-described embodiments, various configuration changes are possible within the scope of the gist of the present invention.
たとえば磁性体は上記のアモルフアスフエリ磁
性体に限定されずMnBi,MnBiCu,EuO等の結
晶性垂直磁化膜でも良い。 For example, the magnetic material is not limited to the above-mentioned amorphous ferrimagnetic material, but may also be a crystalline perpendicularly magnetized film such as MnBi, MnBiCu, or EuO.
又、上記実施例において磁性体膜による記録ト
ラツク2と反射膜4の間に誘電体膜3が形成され
るが該誘電体膜は記録トラツク2に情報をレーザ
光を用いて熱磁気記録を行う時熱伝導により反射
膜4に熱が逃げるのを防ぐために設けられたもの
であり、レーザ光等のエネルギーが充分の場合は
誘電体膜はなくても良い。 Further, in the above embodiment, a dielectric film 3 is formed between the recording track 2 made of a magnetic film and the reflective film 4, and the dielectric film performs thermomagnetic recording of information on the recording track 2 using a laser beam. This dielectric film is provided to prevent heat from escaping to the reflective film 4 due to thermal conduction, and if the energy of laser light or the like is sufficient, the dielectric film may be omitted.
更に記録トラツク2やガイドトラツクは必ずし
も平行な帯状である必要がなくトラツク番号やト
ラツクをセクターごとに分ける場合の情報を入れ
ても良い。 Furthermore, the recording track 2 and the guide track do not necessarily have to be in the form of parallel strips, and track numbers and information for dividing the tracks into sectors may be included.
本発明はもちろんその製造方法には依存しな
い、たとえば記録トラツクはエツチング法で形成
しても強力なレーザ光等で形成してもかまわな
い。又第1図において支持基板5の裏側に同様な
構成の磁気光学記憶素子を形成することで記録素
子の両面を利用し記憶容量の倍増を計る事も可能
である。 Of course, the present invention is not dependent on the manufacturing method; for example, the recording track may be formed by an etching method or by a powerful laser beam. Furthermore, by forming a magneto-optical storage element having a similar structure on the back side of the support substrate 5 in FIG. 1, it is also possible to double the storage capacity by utilizing both sides of the recording element.
以上のように本実施例においては、反射膜を設
けることによつて、磁性体薄膜での反射によるカ
ー効果と磁性体薄膜を通り抜けることで起こるフ
アラデイ効果とが合わされるので、入射したレー
ザ光の波面は単なるカー効果のみによる回転角に
比べて回転角が増大し、このためにS/Nの良い
信号を記録、再生することができる。また、帯状
になした磁性体薄膜と反射膜との間に誘電体膜を
介しているので、レーザ光を用いて磁性体薄膜に
対して熱磁気記録を行う時に発生する反射膜への
熱の散逸を防止することができる。 As described above, in this embodiment, by providing a reflective film, the Kerr effect caused by reflection on the magnetic thin film and the Faraday effect caused by passing through the magnetic thin film are combined, so that the incident laser beam The rotation angle of the wavefront is increased compared to the rotation angle caused only by the Kerr effect, and therefore signals with good S/N can be recorded and reproduced. In addition, since a dielectric film is interposed between the strip-shaped magnetic thin film and the reflective film, the heat generated when thermomagnetic recording is performed on the magnetic thin film using laser light is absorbed by the reflective film. Dissipation can be prevented.
〈効果〉
反射膜と磁性体薄膜とを設けた支持基板と透明
な基板とを、間にN2又はArガスを充填した間〓
を設けて接合してあるので、磁性体薄膜の腐食を
実質的に防止することができ、その結果、経時変
化がなく記録、再生の信頼性の高い磁気光学記憶
素子を提供することができる。さらに、記録トラ
ツクとなる磁性体薄膜を帯状に構成して、記録ト
ラツク相互の間を上記ガスを充填して分離してあ
るため、レーザ光が照射される記録トラツクから
隣接する記録トラツクへ熱が逃げないので、少な
いレーザパワーで効率的に熱磁気記録を実行する
ことができる。<Effect> A support substrate provided with a reflective film and a magnetic thin film and a transparent substrate filled with N 2 or Ar gas
Since the magnetic thin film is bonded with the magnetic material, corrosion of the magnetic thin film can be substantially prevented, and as a result, it is possible to provide a magneto-optical storage element that does not change over time and has high reliability in recording and reproducing. Furthermore, since the magnetic thin film serving as the recording track is formed into a band shape and the recording tracks are separated from each other by being filled with the above-mentioned gas, heat is transferred from the recording track irradiated with the laser beam to the adjacent recording track. Since it does not escape, thermomagnetic recording can be performed efficiently with less laser power.
第1図は本発明に係わる磁気光学記憶素子の一
実施例の一部拡大側面断面図を示す。
図中、1:基板、2:記録トラツク、3:誘電
体膜、4:反射膜、5:支持基板、6:スペー
サ、7:間隙部。
FIG. 1 shows a partially enlarged side cross-sectional view of an embodiment of a magneto-optic storage element according to the present invention. In the figure, 1: substrate, 2: recording track, 3: dielectric film, 4: reflective film, 5: support substrate, 6: spacer, 7: gap.
Claims (1)
射膜と、前記反射膜の上に帯状に形成した垂直磁
化容易軸を有する磁性体薄膜と、第2の基板とを
有し、反射膜と磁性体薄膜とを設けた前記第1の
基板と前記第2の基板とを間〓を設けて接合した
磁気光学記憶素子において、 前記間〓にN2又はArガスを充填したことを特
徴とする磁気光学記憶素子。[Scope of Claims] 1. A first substrate, a reflective film provided on the first substrate, a magnetic thin film having a perpendicular easy axis of magnetization formed in a band shape on the reflective film, and a second substrate. In the magneto-optical memory element, the first substrate provided with a reflective film and a magnetic thin film and the second substrate are bonded with a gap between them, and the gap is filled with N 2 or Ar. A magneto-optical memory element characterized by being filled with gas.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16067187A JPS63841A (en) | 1987-06-26 | 1987-06-26 | Magneto-optical memory element |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16067187A JPS63841A (en) | 1987-06-26 | 1987-06-26 | Magneto-optical memory element |
Related Parent Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP14915680A Division JPS5774852A (en) | 1980-10-23 | 1980-10-23 | Magnetic optical storing element |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS63841A JPS63841A (en) | 1988-01-05 |
JPH038023B2 true JPH038023B2 (en) | 1991-02-05 |
Family
ID=15719964
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP16067187A Granted JPS63841A (en) | 1987-06-26 | 1987-06-26 | Magneto-optical memory element |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63841A (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2549426B2 (en) * | 1988-10-28 | 1996-10-30 | シャープ株式会社 | Optical memory device |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS52156605A (en) * | 1976-06-18 | 1977-12-27 | Thomson Brandt | Data carrier and method of producing same |
JPS531002A (en) * | 1976-05-13 | 1978-01-07 | Philips Corp | Radiation sensitive record |
JPS5534340A (en) * | 1978-08-31 | 1980-03-10 | Nippon Hoso Kyokai <Nhk> | Recording reproducing system by light beam |
-
1987
- 1987-06-26 JP JP16067187A patent/JPS63841A/en active Granted
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS531002A (en) * | 1976-05-13 | 1978-01-07 | Philips Corp | Radiation sensitive record |
JPS52156605A (en) * | 1976-06-18 | 1977-12-27 | Thomson Brandt | Data carrier and method of producing same |
JPS5534340A (en) * | 1978-08-31 | 1980-03-10 | Nippon Hoso Kyokai <Nhk> | Recording reproducing system by light beam |
Also Published As
Publication number | Publication date |
---|---|
JPS63841A (en) | 1988-01-05 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
JPS6227458B2 (en) | ||
US4694358A (en) | Magneto-optic recording structure and method | |
JPH0444333B2 (en) | ||
JPH02779B2 (en) | ||
JPH034974B2 (en) | ||
JP2547768B2 (en) | Optical magnetic recording medium | |
JPH0263261B2 (en) | ||
JPH0263262B2 (en) | ||
JPS6314342A (en) | Magneto-optical recording medium | |
JPH038023B2 (en) | ||
JPH09198731A (en) | Magneto-optical recording medium | |
JP2565884B2 (en) | Magneto-optical storage element | |
JPH034973B2 (en) | ||
JPH0427617B2 (en) | ||
JP2604475B2 (en) | Magneto-optical recording medium | |
JP2689856B2 (en) | Optical recording medium | |
JPH0421936B2 (en) | ||
JP2817505B2 (en) | Single-plate optical disk for magneto-optical recording and its recording / reproducing method | |
JPH04313833A (en) | Magneto-optical recording medium and magneto-optical recording and reproducing method using this medium | |
JPH0350342B2 (en) | ||
JP2549426B2 (en) | Optical memory device | |
JPS59132434A (en) | Magneto-optic storage element | |
JPH0734272B2 (en) | Magneto-optical recording medium | |
JP2607476B2 (en) | Magneto-optical recording method | |
JP2636694B2 (en) | Recording / reproducing method and recording / reproducing apparatus for magneto-optical recording medium |