JPS59215478A - Amorphous magneto-optical layer - Google Patents
Amorphous magneto-optical layerInfo
- Publication number
- JPS59215478A JPS59215478A JP8755683A JP8755683A JPS59215478A JP S59215478 A JPS59215478 A JP S59215478A JP 8755683 A JP8755683 A JP 8755683A JP 8755683 A JP8755683 A JP 8755683A JP S59215478 A JPS59215478 A JP S59215478A
- Authority
- JP
- Japan
- Prior art keywords
- film
- optical layer
- magneto
- amorphous
- amorphous magneto
- 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.)
- Pending
Links
- 230000005415 magnetization Effects 0.000 claims abstract description 6
- 229910017052 cobalt Inorganic materials 0.000 claims description 4
- 239000010941 cobalt Substances 0.000 claims description 4
- GUTLYIVDDKVIGB-UHFFFAOYSA-N cobalt atom Chemical compound [Co] GUTLYIVDDKVIGB-UHFFFAOYSA-N 0.000 claims description 4
- 239000010408 film Substances 0.000 description 11
- 239000010409 thin film Substances 0.000 description 9
- 230000005291 magnetic effect Effects 0.000 description 4
- 239000000203 mixture Substances 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 238000004544 sputter deposition Methods 0.000 description 3
- 239000005300 metallic glass Substances 0.000 description 2
- 238000007740 vapor deposition Methods 0.000 description 2
- 229910000640 Fe alloy Inorganic materials 0.000 description 1
- 230000005374 Kerr effect Effects 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 229910002091 carbon monoxide Inorganic materials 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 230000000295 complement effect Effects 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000005294 ferromagnetic effect Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 239000004033 plastic Substances 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
- 239000000758 substrate Substances 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
Landscapes
- Physical Vapour Deposition (AREA)
- Thin Magnetic Films (AREA)
Abstract
Description
【発明の詳細な説明】
技術分野
本発明は光磁気記録操体に用いられる非晶質磁気光学層
に関する。DETAILED DESCRIPTION OF THE INVENTION Technical Field The present invention relates to an amorphous magneto-optic layer used in a magneto-optical recording device.
従来技術
従来、膜面と垂直な方向に磁化容易軸を有する強磁性薄
膜としてはMnB1に代表される多結晶金属薄膜、Gd
−Co、Gd−Feなどに代表される非晶質金属薄膜
、GIGに代表される化合物単結晶薄膜が知られている
。これらの薄膜は種々の利点を有するが、MnB1はキ
ューリ一点が賜いために書き込みに大きなエネルギーを
必要とし寸た薄膜の作製が技術的に困難であるという欠
点がある。まだ、Gd−Co、 Gd−Feの非晶質金
属薄膜は室温における保磁力が小さく’(300〜50
00e)記録された情報が不安定であるという欠点を有
している。そこで、上記のような従来の磁性薄膜記録媒
体の欠点を除去する新しい磁性薄膜記録媒体として18
〜28原子係のDyを含む非晶質Dy−Fe系合金膜を
備えだものが提案されている(特公昭57−20692
号公報参照)。この合金膜はキュリ一温度Tcが約70
’Cと低いので小さなレーザーパワーで書き込むことが
可能であるが、カー(Kerr)回転角θ1(が0゜1
5 deg前後と小さく充分な再生出方を得ることがで
きないという問題があった。Prior Art Conventionally, as ferromagnetic thin films having an axis of easy magnetization perpendicular to the film surface, polycrystalline metal thin films represented by MnB1, Gd
Amorphous metal thin films represented by -Co, Gd-Fe, etc., and compound single crystal thin films represented by GIG are known. Although these thin films have various advantages, MnB1 has the disadvantage that it requires a large amount of energy for writing and is technically difficult to fabricate thin films due to its single Curie point. However, amorphous metal thin films such as Gd-Co and Gd-Fe have a small coercive force at room temperature (300 to 50
00e) has the disadvantage that the recorded information is unstable. Therefore, we developed 18 as a new magnetic thin film recording medium that eliminates the drawbacks of conventional magnetic thin film recording media as described above.
An amorphous Dy-Fe alloy film containing ~28 atoms of Dy has been proposed (Japanese Patent Publication No. 57-20692).
(see publication). This alloy film has a Curie temperature Tc of approximately 70
Since the C is low, it is possible to write with a small laser power, but the Kerr rotation angle θ1 (0°1
There was a problem in that it was small, around 5 deg, and it was not possible to obtain a sufficient reproduction output.
目 的
本発明は上記問題に鑑みてなされたものであつて、その
目的はキュリ一温度が低くしがもカー回転角の大きい非
晶質磁気光学層を後供することである。Purpose The present invention was made in view of the above problems, and its purpose is to provide an amorphous magneto-optical layer having a low Curie temperature and a large Kerr rotation angle.
オ(・〒 成
本発明の非晶質磁気プ゛C字層は膜面と折直な方向に磁
化容易軸を有するDy−Fe膜に少なくとも0.5原子
俤のコバルトを含むものである。本発明においてコバル
トの含有量を少なくとも0.5原子俤と限定するのは、
大きなカー回転角を得るためであり% 0.5原子チ未
満では充分なカー回転角が得られず本発明の効果が達成
されない。The amorphous magnetic C-shaped layer of the present invention contains at least 0.5 atoms of cobalt in a Dy-Fe film having an axis of easy magnetization perpendicular to the film surface. The content of cobalt is limited to at least 0.5 atomic tons because
The purpose is to obtain a large Kerr rotation angle, and if it is less than 0.5%, a sufficient Kerr rotation angle will not be obtained and the effects of the present invention will not be achieved.
一方、コバルトの含有量をあまシ大きくするとキュリ一
温度が土が9すぎるので05〜2(]原子俤の範囲が好
ましい。On the other hand, if the cobalt content is slightly increased, the Curie temperature will be too high, so the range of 05 to 2 (] atoms is preferable.
本発明の磁気光学層はガラス、プラスティック、セラミ
ックなどからなる非磁性基板上に。The magneto-optical layer of the present invention is formed on a nonmagnetic substrate made of glass, plastic, ceramic, or the like.
スパッタ法、蒸着法、イオンブレーティング法などによ
り、少なくとも0.5原子チのCo、f含むDy−Fe
膜を形成させることにより作製することができる。膜
の作製はスパッタ法によって行なうのが望ましい。ター
ゲットは例えばコンボジツ!・法を用い、Fe円板の上
にDyおよびCOデツプをのせて宿成しそして組成はタ
ーゲット表面の面積比でコントロールする。また、本発
明の磁気光学層を光磁気記録媒体に1史用する場合はそ
れを単独で用いてもよいしあるいは他の)1「yと一緒
に用いてもよい。例えば保箇膜は1イ・りえば5102
、Sin、 Si3N4などからなる膜をDy−Fe−
C。Dy-Fe containing at least 0.5 atoms of Co and f by sputtering, vapor deposition, ion blating, etc.
It can be produced by forming a film. Preferably, the film is formed by sputtering. For example, the target is combojitsu!・Using the method, Dy and CO deposits are deposited on an Fe disk, and the composition is controlled by the area ratio of the target surface. In addition, when the magneto-optic layer of the present invention is used in a magneto-optical recording medium, it may be used alone or together with another (1). Lee Rieba 5102
Dy-Fe-
C.
−膜の上にスパッタ法、蒸着法、イオンブレーティング
法などにより設けることができる。- It can be provided on the film by sputtering, vapor deposition, ion blating, etc.
実施例
以下に実施例をあげて本発明を具体的に説明するが、こ
れに限定されるものではない。EXAMPLES The present invention will be specifically explained with reference to Examples below, but the present invention is not limited thereto.
本実施例では以下の作製条件でスライドガラス上に2(
1001の膜厚の)良を作製し、Hcの大きい補イr(
組成付近のFs 0078 Dy O,22の組成にお
いてFeの一部をCoで置換していく場合のカー回転角
θにおよびキュリ一温度Tcの変化をみた。In this example, 2 (
A film with a film thickness of 1001 mm was prepared, and a complementary film with a large Hc was prepared.
Changes in the Kerr rotation angle θ and the Curie temperature Tc were observed when part of Fe was replaced with Co in a composition of Fs 0078 Dy O, 22 near the composition.
〈作製金件〉
残留ガス圧: 8X 10−7TorrArガス圧:
2X 10−2Torr放′1d々力ニ400w
プレスパツタ時間:60m1n
メインスパッタ時間:8m1n
カー回転角θには基板側からHe−Neレーザ(λ=
6s2sX )を照射してカー効果により求めた。<Production requirements> Residual gas pressure: 8X 10-7 TorrAr gas pressure:
2
6s2sX ) was irradiated and determined by the Kerr effect.
また、キュ9一温度Tcは振動試料型磁化測定装随によ
り測定した。(Fe 1−XCOX) 0.78 DY
o、22巾のC。Further, the cu-91 temperature Tc was measured using a vibrating sample type magnetization measuring device. (Fe 1-XCOX) 0.78 DY
o, 22 width C.
の添加量又とθにとの関係を求めた第1図の結果から明
らかなように、Coの添加量Xを増すとθには0.15
degから0.28deg増加するがx=0.10付
近でほぼ飽和傾向を示した。一方、キュリー温JiTc
は第2図に示したようにCo添加J’ xを増すと70
℃からほぼ直線的に上昇するが、光磁気記録媒体のTc
としては100〜200℃の範囲が適していると考えら
れ高すぎると大きな記録エネルギーが必要となり不利で
ある。本実施例ではθkがX=0.10付近で飽和傾向
を示していることがらTcが余り高くならないx=0.
1[]付近の値でθkが太き(Tcが低い最適条件であ
ると結論できる。As is clear from the results shown in Figure 1, which show the relationship between the amount of Co added and θ, when the amount of Co added is increased, θ increases by 0.15.
deg by 0.28 deg, but it showed an almost saturated tendency around x=0.10. On the other hand, Curie Wen JiTc
becomes 70 as the Co addition J' x is increased as shown in Figure 2.
The Tc of the magneto-optical recording medium increases almost linearly from °C.
A temperature in the range of 100 to 200°C is considered suitable; however, if the temperature is too high, a large amount of recording energy is required, which is disadvantageous. In this example, since θk shows a tendency to saturate around X=0.10, Tc does not become too high when x=0.10.
It can be concluded that a value around 1[] is the optimum condition where θk is large (Tc is low).
効 果
本発明の非晶質磁気光学層はキュリー温抹(が低くしか
もカー回転角の大きい光磁気記録媒体を提供できる効果
がある。Effects The amorphous magneto-optic layer of the present invention has the effect of providing a magneto-optical recording medium with a low Curie temperature and a large Kerr rotation angle.
第1図および第2図は本発明の磁気9°C学層の最適条
件を決定するにあたっての組成変化に対するカー回転角
とキュリー温)圧との11系をそれぞれ示す図である。
特許出願人 株式会社 リ コ −イ、い、Pつ
よ、4エ e、’、)、J、−1゜゛ しニジ−↓゛
区 16°2′J″0
滅
図 rつ。皿
へ
緘FIGS. 1 and 2 are diagrams respectively showing 11 systems of Kerr rotation angle and Curie temperature/pressure with respect to changes in composition for determining the optimum conditions for the magnetic 9°C layer of the present invention. Patent applicant Riko Co., Ltd.
Claims (1)
少なくとも0.5原子チのコバルトを含むことを特徴と
する、非晶質磁気光学層。An amorphous magneto-optical layer comprising at least 0.5 atoms of cobalt in a D7-Fe film having an axis of easy magnetization in a direction perpendicular to the film surface.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP8755683A JPS59215478A (en) | 1983-05-20 | 1983-05-20 | Amorphous magneto-optical layer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP8755683A JPS59215478A (en) | 1983-05-20 | 1983-05-20 | Amorphous magneto-optical layer |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59215478A true JPS59215478A (en) | 1984-12-05 |
Family
ID=13918257
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP8755683A Pending JPS59215478A (en) | 1983-05-20 | 1983-05-20 | Amorphous magneto-optical layer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59215478A (en) |
-
1983
- 1983-05-20 JP JP8755683A patent/JPS59215478A/en active Pending
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