JPH0266751A - magneto-optical recording medium - Google Patents

magneto-optical recording medium

Info

Publication number
JPH0266751A
JPH0266751A JP21893288A JP21893288A JPH0266751A JP H0266751 A JPH0266751 A JP H0266751A JP 21893288 A JP21893288 A JP 21893288A JP 21893288 A JP21893288 A JP 21893288A JP H0266751 A JPH0266751 A JP H0266751A
Authority
JP
Japan
Prior art keywords
film
light
refractive index
magneto
transparent 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.)
Pending
Application number
JP21893288A
Other languages
Japanese (ja)
Inventor
Rokuro Watabe
渡部 六郎
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.)
Ricoh Co Ltd
Original Assignee
Ricoh Co 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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP21893288A priority Critical patent/JPH0266751A/en
Publication of JPH0266751A publication Critical patent/JPH0266751A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To additionally improve reproduction performance by providing a transparent film for light interference between a light transparent substrate and a magnetic film and forming the transparent film of a material which causes a change in refractive index by the light and heat of laser. CONSTITUTION:A chalcogenide film is formed as the transparent film 2 for light interference on the polycarbonate substrate 1 and the magnetic film 3 and a protective film 4 are provided thereon to form the recording medium. The change in the refractive index arises in the chalcogenide film 2 and the reflectivity changes accordingly when this medium is irradiated with the laser light. The quantity of the light necessary for a signal level reflects at the time of recording and the balance is inverted in magnetization for the purpose of recording. The larger quantity of light is obtd. at the time of reproducing and further, the refractive index restores the original value when the magnetization is returned by erasing. The reproduction performance is additionally improved by forming the transparent film of the material which is changed in the refractive index in such a manner.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は書き換えが可能な光磁気記録媒体に関し、特に
再生時の反射光量を増加させて再生性能を向上させた光
磁気記録媒体に関するものである。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a rewritable magneto-optical recording medium, and particularly to a magneto-optical recording medium that improves reproduction performance by increasing the amount of reflected light during reproduction. be.

〔従来の技術〕[Conventional technology]

近年、書き換え可能な光記録媒体として、磁気光学効果
を利用した光磁気記録媒体をか精力的に研究開発され、
一部では実用化されるに至っている。この光磁気記録媒
体は大容量高密度記録、非接触記録再生、アクセスの容
易さ等の利点に加え、重ね書き(オーバーライド)が可
能という点で文書情報ファイル、ビデオ・静止画ファイ
ル、コンピューター用メモリ等への利用が期待されてい
る。
In recent years, magneto-optical recording media that utilize magneto-optic effects have been actively researched and developed as rewritable optical recording media.
In some cases, it has even been put into practical use. This magneto-optical recording medium has the advantages of large-capacity, high-density recording, non-contact recording and playback, and ease of access, as well as the ability to overwrite document information files, video and still image files, and computer memory. It is expected that it will be used for

上記光磁気記録媒体は、垂直磁化膜すなわち膜面に垂直
な方向に磁気容易軸を有する磁性膜を記録層とし、レー
ザービームを照射するとともに磁界を印加することによ
り情報の記録、再生及び消去が行えるようになっている
The above-mentioned magneto-optical recording medium has a perpendicular magnetization film, that is, a magnetic film having an easy magnetic axis in a direction perpendicular to the film surface, as a recording layer, and information can be recorded, reproduced, and erased by irradiating a laser beam and applying a magnetic field. It is now possible to do so.

すなわち、情報の記録は、垂直磁化膜の磁化方向を予め
一定方向にそろえておき、垂直磁化膜の微小部分にレー
ザービームを集光し、その部分のみを昇温させて磁化を
失わせ、その後温度が室温に戻る時に磁界をその部分の
磁化方向が周囲と逆になるように印加し磁化させること
によりビットを形成して行う。
In other words, to record information, the magnetization direction of the perpendicularly magnetized film is aligned in a certain direction in advance, a laser beam is focused on a minute part of the perpendicularly magnetized film, and only that part is heated to lose its magnetization. When the temperature returns to room temperature, a magnetic field is applied to the part so that the direction of magnetization is opposite to that of the surrounding area, thereby magnetizing the part to form a bit.

情報の再生は、一般に、再生用のレーザービーム(パワ
ーが記録用より小)を記録層に照射し、その照射部分の
磁化方向の違いにより反射ビームの偏光面の回転方向が
異なる磁気カー効果を利用して行う。
Generally, information is reproduced by irradiating the recording layer with a laser beam for reproduction (power is lower than that for recording), and using the magnetic Kerr effect, in which the direction of rotation of the polarization plane of the reflected beam differs depending on the magnetization direction of the irradiated part. Use and do it.

また情報の消去は、記録ビットにレーザービームを照射
するとともに、記録の際の磁界と逆方向の磁界を印加す
ることにより行う。
Information is erased by irradiating the recorded bits with a laser beam and applying a magnetic field in the opposite direction to the magnetic field used during recording.

一方、光磁気記録媒体に要求される特性の1つに再生性
能が良好なことが挙げられる。この再生性能は性能指数
、/Fak(R;反射率、θ、;カー回転角)で評価さ
れ、性能指数が大きいほど、すなわち反射率Rとカー回
転角θ、が大きいほどよいとされる。
On the other hand, one of the characteristics required of magneto-optical recording media is good reproduction performance. This reproduction performance is evaluated by a figure of merit, /Fak (R: reflectance, θ,; Kerr rotation angle), and it is said that the larger the figure of merit, that is, the larger the reflectance R and the Kerr rotation angle θ, the better.

従来、再生性能を向上させるために、カー回転角θ□の
できるだけ大きい記録材料を得るべく多くの努力がなさ
れており、種々の記録材料が特許公報、文献等に発表さ
れている。また、カー効果を増大させるために、基板と
磁性膜の間に光干渉用の透明膜を設ける技術も提案され
ている(特開昭63−18546号公報等)。このよう
に、従来は、再生性能を向上させるためにカー回転角θ
、のみに注目が集っていたのが実情である。
Conventionally, in order to improve reproduction performance, many efforts have been made to obtain recording materials with as large a Kerr rotation angle θ□ as possible, and various recording materials have been published in patent publications, literature, and the like. Furthermore, in order to increase the Kerr effect, a technique has been proposed in which a transparent film for optical interference is provided between the substrate and the magnetic film (Japanese Patent Application Laid-Open No. 18546/1983, etc.). In this way, conventionally, in order to improve playback performance, the Kerr rotation angle θ
The reality is that attention has been focused only on .

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

しかしながら、従来のようにカー回転角θ だけの改良
では再生性能に限界があることがわかった。その一方、
最近の情報処理の高速化、高精度化に対応するために、
より一層の再生性能の向上が期待されている。
However, it has been found that there is a limit to the reproduction performance by improving only the Kerr rotation angle θ as in the past. On the other hand,
In order to respond to recent advances in speed and precision of information processing,
Further improvements in playback performance are expected.

従って、本発明はこの点に鑑み、さらに再生性能を向上
させた光磁気記録媒体を提供することを目的とする。
Therefore, in view of this point, it is an object of the present invention to provide a magneto-optical recording medium with further improved reproduction performance.

〔課題を解決するための手段及び作用〕上述のように、
再生性能は反射率Rとカー回転角θ が大きいほどよい
とされている。ここで力に 一回転角θ の改良には限界がある。そこで、反に 射率Rに着目した場合、レーザー光で記録するとき、信
号レベルに必要な光量が反射し、残りは記録のための磁
化反転し、有効に使用されるのが望ましい。
[Means and actions for solving the problem] As mentioned above,
It is said that the reproduction performance is better as the reflectance R and the Kerr rotation angle θ are larger. Here, there is a limit to the improvement of force per rotation angle θ. Therefore, when focusing on the emissivity R, when recording with a laser beam, it is desirable that the amount of light necessary for the signal level is reflected, and the remainder is used effectively by inverting the magnetization for recording.

また、再生するときは、できるだけ多くのレーザ光が反
射して信号として使用されるのが望ましい。
Furthermore, during reproduction, it is desirable that as much laser light as possible is reflected and used as a signal.

換言すれば、記録するときは最小限の反射量であり、再
生するときはより多くの反射量があれば、再生性能をよ
り一層向上させることができる。
In other words, if there is a minimum amount of reflection when recording and a larger amount of reflection when reproducing, the reproducing performance can be further improved.

本発明者は以上のことを考慮しながら鋭意研究を重ねた
結果、本発明を完成するに至った。
The present inventor has completed the present invention as a result of extensive research while taking the above points into consideration.

すなわち、上記目的を達成するため、本発明によれば、
透光性の基板上に、直接もしくは下地層を介して光干渉
用の透明膜を設け、該透明膜上に磁性膜を設け、さらに
その上に保護膜を設けてなる光磁気記録媒体において、
前記透明膜が、レーザーの光熱により屈折率変化を起こ
す物質により構成されていることを特徴とする光磁気記
録媒体が提供される。
That is, in order to achieve the above object, according to the present invention,
A magneto-optical recording medium in which a transparent film for optical interference is provided on a transparent substrate directly or via an underlayer, a magnetic film is provided on the transparent film, and a protective film is further provided on the transparent film,
There is provided a magneto-optical recording medium, characterized in that the transparent film is made of a substance that causes a change in refractive index due to the light heat of a laser.

レーザーの光熱により屈折率変化を起こす物質としては
、例えばカルコゲン(S、Se、Te)を少なくとも1
種以上組成元素として含むものが好ましく使用される。
As a substance that causes a change in refractive index due to the light heat of the laser, for example, at least 1% of chalcogen (S, Se, Te) is used.
Those containing at least one kind of compositional element are preferably used.

その具体的な化合物例としては、As3SeSnS4G
e、 As、□5e4STe、、Ge□、、 GcJS
bSnSe、、、AsSe、5bGea等のカルコゲナ
イド(カルコゲンを含む化合物)が挙げられる。
As a specific example of the compound, As3SeSnS4G
e, As, □5e4STe,, Ge□,, GcJS
Examples include chalcogenides (compounds containing chalcogen) such as bSnSe, AsSe, and 5bGea.

一 上記物質を、基板と磁性膜との間に設ける透明膜に使用
した場合、磁化反転の前後で屈折率が変化し、それに伴
って反射率が変化することがわがった。すなわち、記録
時には最小限の反射量であり、再生するときはより多く
の反射量となるように変化する。これにより、再生特性
のより一層の向上が可能となる。また、これらの物質は
消去作用により磁化が元に戻れば、変化した屈折率も元
へ戻ることがわかった。この可逆性により書き換え可能
な光磁気記録媒体への適用が可能となる。
It has been found that when the above-mentioned substance is used in a transparent film provided between a substrate and a magnetic film, the refractive index changes before and after magnetization reversal, and the reflectance changes accordingly. That is, the amount of reflection is minimal during recording, and changes to a larger amount during reproduction. This makes it possible to further improve the reproduction characteristics. It was also found that if the magnetization of these materials is restored to its original state through an erasing action, the changed refractive index will also return to its original state. This reversibility allows application to rewritable magneto-optical recording media.

〔実施例〕〔Example〕

以下本発明を実施例により詳細に説明する。 The present invention will be explained in detail below with reference to Examples.

ポリカーボネート(pc)基板上に、RF(高周波)ス
パッタにより、光干渉用の透明膜としてカルコゲナイド
膜As3SeSnS4Geを800人の膜厚で付着させ
、次にその上に磁性膜丁bFeCoを700Aの膜厚で
付着させ、続いて保護膜SiNを900人の膜厚で付着
させ、第1図に示すような膜構成の光磁気記録媒体を得
た。なお、図中1は基板、2は光干渉用の透明膜、3は
磁性膜、4は保詣膜である。また、上記スパン夕の条件
は以下の通りである。
On a polycarbonate (PC) substrate, a chalcogenide film As3SeSnS4Ge was deposited to a thickness of 800 mm as a transparent film for optical interference by RF (radio frequency) sputtering, and then a magnetic film (FeCo) was deposited on top of it to a thickness of 700 mm. Then, a protective film of SiN was deposited to a thickness of 900 nm to obtain a magneto-optical recording medium having a film structure as shown in FIG. In the figure, 1 is a substrate, 2 is a transparent film for optical interference, 3 is a magnetic film, and 4 is a protection film. Moreover, the conditions for the above-mentioned span length are as follows.

・1チヤンバー複数ターゲツト(バッチタイプ)・ター
ゲットと基板との距1i9 80mm・真空度(バック
グラウンド) 1〜5 X LP’ Torr同(スパ
ッタ時)  4−9 X 1O−3Torr(Arガス
)・印加電力       0.75kW(RF 13
.6117)・スパッタレイト    3〜5人/ s
ec上記のようにして作製した光磁気記録媒体に、波長
820nmの半導体レーザーで記録を行うとき、全光量
の23.1%が反射され、残りの76.9%が磁性膜に
吸収され、磁化反転に必要な温度ヒ昇が起こり、磁化が
反転する。このとき、表−1に示すようにカルコゲナイ
ド膜As3SeSnS4Geに屈折率の変化が起こるこ
とがわかった。すなわち、磁化の反転の前後で屈折率が
2.3から2.1に変化した。そしてそれに伴って、反
射率が23.1%から26.7に変化した。
・One chamber, multiple targets (batch type) ・Distance between target and substrate 1980 mm ・Vacuum degree (background) 1 to 5 X LP' Torr (during sputtering) 4-9 X 1O-3 Torr (Ar gas) ・Apply Power 0.75kW (RF 13
.. 6117)・Sputter rate 3-5 people/s
ec When recording is performed on the magneto-optical recording medium prepared as described above using a semiconductor laser with a wavelength of 820 nm, 23.1% of the total amount of light is reflected, and the remaining 76.9% is absorbed by the magnetic film, causing magnetization. The temperature rise necessary for reversal occurs, and the magnetization is reversed. At this time, it was found that a change in refractive index occurred in the chalcogenide film As3SeSnS4Ge as shown in Table 1. That is, the refractive index changed from 2.3 to 2.1 before and after the reversal of magnetization. Along with this, the reflectance changed from 23.1% to 26.7.

表−1 また、消去作用によって磁化が元に戻ればカルコゲナイ
ド膜の屈折率も2.1から2.3に変化し、元へ戻るこ
とがわかった。これは、磁化反転の影響のほかにレーザ
ーの光熱[こよってカルコゲナイド膜に組成変化が起き
るためと考えられる。ここで第2図に上記の現象の概念
図を示す。
Table 1 It was also found that if the magnetization is returned to its original state by the erasing action, the refractive index of the chalcogenide film also changes from 2.1 to 2.3 and returns to its original state. This is thought to be due to the photothermal effect of the laser, which causes a compositional change in the chalcogenide film, in addition to the effect of magnetization reversal. Here, FIG. 2 shows a conceptual diagram of the above phenomenon.

本実施例の光磁気記録媒体の再生性能を評価したところ
、性能指数(1θ、)が≠]窮x 003=0.144
から≠、267 X 0.3=0.155と向上するこ
とによって、C/Nが53 d Bとなり、従来の屈折
率変化が起こらないもの(49dB)より4dB向上し
た。
When the playback performance of the magneto-optical recording medium of this example was evaluated, the figure of merit (1θ, ) was ≠] x 003 = 0.144
By improving from ≠, 267×0.3=0.155, the C/N became 53 dB, which was 4 dB better than the conventional one in which no refractive index change occurred (49 dB).

また、光干渉用の透明膜としてカルコゲナイド膜As、
□Se、、、Te1.Ge□。、Ge3SbSnSe5
、As5e4SbGe3をそれぞれ用いて上記実施例と
同様にして光磁気記録媒体を作製し、その再生性能を評
価したところ、上記と同等の効果を得ることができた。
In addition, as a transparent film for optical interference, chalcogenide film As,
□Se,,,Te1. Ge□. , Ge3SbSnSe5
, As5e4SbGe3 were used to prepare a magneto-optical recording medium in the same manner as in the above example, and the reproduction performance thereof was evaluated. As a result, effects equivalent to those described above could be obtained.

〔発明の効果〕〔Effect of the invention〕

以−1こ詳細に説明したように、本発明によれば、基板
と磁性膜の間に設けた光干渉用の保護膜を、レーザーの
光熱により屈折率変化を起こす物質で楕成したので、こ
の屈折率変化に伴って、記録時には最小限の反射量、再
生時にはより多くの反射量が得られるように反射率が変
化し、再生性能をより一層向上させることが可能となる
As explained in detail below, according to the present invention, the protective film for optical interference provided between the substrate and the magnetic film is made of an oval material that causes a change in refractive index due to the light heat of the laser. With this change in refractive index, the reflectance changes so that a minimum amount of reflection is obtained during recording and a larger amount of reflection is obtained during reproduction, making it possible to further improve reproduction performance.

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

第1図は本発明に係る光磁気記録媒体の膜構成を示す断
面図、第2図はに配光磁気記録媒体の光干渉用の透明膜
に生じる屈折率変化の概念図である。 1・・・基板 2・・・光干渉用の透明膜 3・磁性膜 4・・保護膜 特許出願人 株式会社 リ  コ
FIG. 1 is a sectional view showing the film structure of a magneto-optical recording medium according to the present invention, and FIG. 2 is a conceptual diagram of a change in refractive index occurring in a transparent film for optical interference of a light distribution magnetic recording medium. 1... Substrate 2... Transparent film for optical interference 3, Magnetic film 4... Protective film Patent applicant Rico Co., Ltd.

Claims (1)

【特許請求の範囲】[Claims] (1)透光性の基板上に、直接もしくは下地層を介して
光干渉用の透明膜を設け、該透明膜上に磁性膜を設け、
さらにその上に保護膜を設けてなる光磁気記録媒体にお
いて、 前記透明膜が、レーザーの光熱により屈折率変化を起こ
す物質により構成されていることを特徴とする光磁気記
録媒体。
(1) A transparent film for optical interference is provided on a transparent substrate directly or via an underlayer, and a magnetic film is provided on the transparent film,
A magneto-optical recording medium further comprising a protective film provided thereon, wherein the transparent film is made of a substance that causes a change in refractive index due to the light heat of a laser.
JP21893288A 1988-08-31 1988-08-31 magneto-optical recording medium Pending JPH0266751A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21893288A JPH0266751A (en) 1988-08-31 1988-08-31 magneto-optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21893288A JPH0266751A (en) 1988-08-31 1988-08-31 magneto-optical recording medium

Publications (1)

Publication Number Publication Date
JPH0266751A true JPH0266751A (en) 1990-03-06

Family

ID=16727581

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21893288A Pending JPH0266751A (en) 1988-08-31 1988-08-31 magneto-optical recording medium

Country Status (1)

Country Link
JP (1) JPH0266751A (en)

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