JPH02306445A - Magneto-optical recording medium - Google Patents

Magneto-optical recording medium

Info

Publication number
JPH02306445A
JPH02306445A JP12583689A JP12583689A JPH02306445A JP H02306445 A JPH02306445 A JP H02306445A JP 12583689 A JP12583689 A JP 12583689A JP 12583689 A JP12583689 A JP 12583689A JP H02306445 A JPH02306445 A JP H02306445A
Authority
JP
Japan
Prior art keywords
magnetic field
recording
information
magneto
magnetic
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
JP12583689A
Other languages
Japanese (ja)
Inventor
Satoshi Shimokawato
下川渡 聡
Masaya Ishida
方哉 石田
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.)
Seiko Epson Corp
Original Assignee
Seiko Epson Corp
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 Seiko Epson Corp filed Critical Seiko Epson Corp
Priority to JP12583689A priority Critical patent/JPH02306445A/en
Publication of JPH02306445A publication Critical patent/JPH02306445A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To allow the direct overwriting of information even with a small modulation magnetic field by holding the regions where the recording of information is not executed and which are adjacent to the regions where the recording of the information is executed in magnetic recording layers into a degaussing state. CONSTITUTION:This magneto-optical recording medium executes the recording of the information by irradiating the magnetic recording layers with the convergent light of a specified intensity or modulated according to the recording information simultaneously with the impression of the magnetic field modulated according to the recording information. The regions 102 where the recording of the information is executed and which are adjacent to the regions 101 where the recording of the information is executed in the magnetic recording layers are previously put into the degaussing state. Then, floating magnetic field intensity from the regions 102 is nearly zero and, therefore, the relation ¦HW¦=¦HE¦ of the magnetic field (HW) and the erasing magnetic field (HE) approximately holds and the modulation magnetic field in the magnetic field modulation recording system is lowered. The direct overwriting of the information even with the small modulation magnetic field is possible in this way.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明はレーザービーム等の収束光の熱エネルギーと磁
界の相互作用により情報の記録を行い、磁気光学効果に
よって再生を行う光磁気記録に関わり、特に磁界変調方
式によるダイレクトオーバーライドが可能な光磁気記録
媒体に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to magneto-optical recording in which information is recorded by the interaction between the thermal energy of convergent light such as a laser beam and a magnetic field, and is reproduced by the magneto-optic effect. In particular, the present invention relates to a magneto-optical recording medium that allows direct override using a magnetic field modulation method.

[従来の技術] 従来、磁界変調方式によるダイレクトオーバーライドが
可能な光磁気記録に用いられる光磁気記録媒体としては
、TbFeCo、DyFeCo等の合金薄膜を磁性記録
層とするものが用いられている。例えば、特開詳63−
217548に開示されている磁界変調用光磁気記録媒
体の例では、厚さ約1.2mmの透明基板上にTbFe
Co層を挟んで両側にSi3N4等の誘電体層を形成し
、更に保護コートを設けたものが示されている。ここで
特開昭51−107121に開示されているように、磁
性記録層の磁化方向を予め全体に一方向に揃えてから用
いるのが普通である。
[Prior Art] Conventionally, as a magneto-optical recording medium used for magneto-optical recording capable of direct override using a magnetic field modulation method, one in which a thin film of an alloy such as TbFeCo or DyFeCo is used as a magnetic recording layer has been used. For example, JP-A No. 63-
In the example of the magneto-optical recording medium for magnetic field modulation disclosed in No. 217548, TbFe is deposited on a transparent substrate with a thickness of about 1.2 mm.
A dielectric layer such as Si3N4 is formed on both sides of the Co layer, and a protective coat is further provided. As disclosed in Japanese Unexamined Patent Publication No. 51-107121, the magnetization direction of the magnetic recording layer is generally aligned in one direction in advance before use.

[発明が解決しようとする課題] ところで磁界変調方式においては、磁界を記録データに
応じて変調することが必要であるが、従来の光磁気記録
媒体に情報をダイレクトオーバーライドするためには2
00〜3000e程度の比較的大きな磁界を高速に変調
する必要がある。しかしながら、このような大きな磁界
を得るためにコイルの巻数を多くすると、コイルのイン
ダクタンスが増大し、高速な磁界反転を実現することが
非常に困難になる。従って、実用的な速度での情報のダ
イレクトオーバーライドが実現できないという問題点が
ある。
[Problems to be Solved by the Invention] Incidentally, in the magnetic field modulation method, it is necessary to modulate the magnetic field according to the recorded data, but in order to directly override information on a conventional magneto-optical recording medium, two steps are required.
It is necessary to modulate a relatively large magnetic field of about 00 to 3000 e at high speed. However, increasing the number of turns of the coil to obtain such a large magnetic field increases the inductance of the coil, making it extremely difficult to achieve high-speed magnetic field reversal. Therefore, there is a problem that direct override of information cannot be realized at a practical speed.

本発明はこのような課題を解決するもので、その目的と
するところは、小さな変調磁界でも情報のダイレクトオ
ーバーライドが可能な光磁気記録媒体を提供することに
ある。
The present invention is intended to solve these problems, and its purpose is to provide a magneto-optical recording medium that allows direct overwriting of information even with a small modulated magnetic field.

[課題を解決するための手段] 本発明の光磁気記録媒体は、記録情報に応じて変調した
磁界を印加すると同時に、一定の強度または記録情報に
応じて変調した収束光を磁性記録層に照射することによ
って情報の記録を行なう光磁気記録媒体において、該磁
性記録層のうち情報の記録が行われる領域に隣接する、
情報の記録が行われない領域が消磁状態にあることを特
徴とす[作用コ ところで、磁界変調記録方式において記録に必要な磁界
強度は、直流磁界と変調光パルスを用いたいわゆる光変
調方式記録方式における記録磁界(Hu)と消去磁界(
HE)の大きさで決まる。遷移金属リッチの磁性記録層
の場合一般には1Hul<IHEI  なる関係が成り
立つので磁界変調方式における変調磁界強度は、IME
I  以上必要である。これは磁性記録層の記録に用い
られていない部分からの浮遊磁界の向きが書き込み方向
にあるため、記録磁界や消去磁界に重畳してオフセット
磁界として働(からである。従って lHi+1=lH
EI  のとき変調磁界強度は最小になる。
[Means for Solving the Problems] The magneto-optical recording medium of the present invention applies a magnetic field modulated according to recorded information and simultaneously irradiates a magnetic recording layer with a fixed intensity or focused light modulated according to recorded information. In a magneto-optical recording medium in which information is recorded by
It is characterized in that the area where information is not recorded is in a demagnetized state. The recording magnetic field (Hu) and erasing magnetic field (
It is determined by the size of HE). In the case of a transition metal-rich magnetic recording layer, the relationship 1Hul<IHEI generally holds, so the modulation magnetic field strength in the magnetic field modulation method is IME
I or more is required. This is because the direction of the stray magnetic field from the part of the magnetic recording layer that is not used for recording is in the writing direction, so it is superimposed on the recording magnetic field and the erasing magnetic field and acts as an offset magnetic field. Therefore, lHi+1=lH
At EI, the modulated magnetic field strength is at its minimum.

第1図は本発明の構成を表す図で、磁性記録層を上から
見たものである。いま磁性記録層のうち情報の記録が行
われる領域101に隣接する、情報の記録が行われない
領域102を消磁状態にしておくと、領域102からの
浮遊磁界強度はほぼゼロになるため、l Hul = 
I HEIが近似的に成立ち、磁界変調記録方式におけ
る変調磁界強度を小さくすることが可能になる。
FIG. 1 is a diagram showing the configuration of the present invention, and shows the magnetic recording layer viewed from above. Now, if the area 102 of the magnetic recording layer where no information is recorded, which is adjacent to the area 101 where information is recorded, is demagnetized, the stray magnetic field strength from the area 102 will be almost zero, so l Hul =
I HEI approximately holds true, and it becomes possible to reduce the modulation magnetic field strength in the magnetic field modulation recording method.

[実施例] 以下、実施例に基づいて本発明の詳細な説明する。[Example] Hereinafter, the present invention will be described in detail based on Examples.

第2図は本発明の一例である光磁気記録媒体の断面を模
式的に示したものである。第2図においてディスク基板
201は直径130mm、厚さ1゜2mmの透明なガラ
ス基板で、図には示してはないがトラッキング用に螺旋
状の案内溝が設けられている。膜厚約30nmの磁性記
録層203を挟んで、基板側にAl−3t−Nからなる
膜厚9゜nmの干渉層202を、反対側に同じ<Al−
3i−Nからなる膜厚25nm保護層204を配した。
FIG. 2 schematically shows a cross section of a magneto-optical recording medium which is an example of the present invention. In FIG. 2, a disk substrate 201 is a transparent glass substrate with a diameter of 130 mm and a thickness of 1.degree. 2 mm, and is provided with a spiral guide groove for tracking, although not shown in the figure. An interference layer 202 with a thickness of 9 nm made of Al-3t-N is placed on the substrate side with a magnetic recording layer 203 with a thickness of about 30 nm in between, and the same <Al-
A protective layer 204 made of 3i-N and having a thickness of 25 nm was provided.

その上にはAIからなる膜厚40nmの反射層205を
形成し、さらに紫外線硬化樹脂からなる厚さ約10μm
の保護コート層206を設けた。
On top of that, a reflective layer 205 made of AI with a thickness of 40 nm is formed, and further made of ultraviolet curing resin with a thickness of about 10 μm.
A protective coat layer 206 was provided.

いま本発明の例として磁性記録層203の組成がNd6
Dy22F e62coIO(at%)である光磁気記
録媒体を作製した。なお磁性記録層203はスパッタ法
にて作製したが、ディスク全面にわたって多磁区の消磁
状態になっている。
As an example of the present invention, the composition of the magnetic recording layer 203 is Nd6.
A magneto-optical recording medium made of Dy22F e62coIO (at%) was produced. Although the magnetic recording layer 203 was manufactured by sputtering, the entire surface of the disk was in a multi-domain demagnetized state.

次にこの光磁気記録媒体の光アシストの磁界変調記録方
式による記録/再生特性の評価を行った。
Next, the recording/reproducing characteristics of this magneto-optical recording medium using an optically assisted magnetic field modulation recording method were evaluated.

第3図を用いて情報の記録方法について説明する。A method of recording information will be explained using FIG.

即ち第3図(b)に示すごとく、ディスク基板201側
から連続発光した半導体レーザの収束光をを照射し、磁
性記録層203の温度をキュリ一温度近傍まで加熱し保
磁力を低下させる。それと同時に保護コート層206側
に配した磁気ヘッドを用いて、記録信号(第3図(a)
)に応じて記録媒体に印加する磁界の極性を第3図(c
)のように変調する。この結果、印加磁界によって磁化
反転するに十分なだけ磁性記録層の保磁力が小さくなっ
ている領域のみ、磁性記録層の磁化が反転し記録信号に
対応した磁区パターンが磁性記録層に形成され(第3図
(d))情報の記録が完了する。
That is, as shown in FIG. 3(b), convergent light from a semiconductor laser continuously emitted from the disk substrate 201 side is irradiated to heat the magnetic recording layer 203 to a temperature close to the Curie temperature, thereby lowering the coercive force. At the same time, a magnetic head placed on the protective coat layer 206 side is used to generate a recording signal (see FIG. 3(a)).
) The polarity of the magnetic field applied to the recording medium is shown in Figure 3 (c
). As a result, the magnetization of the magnetic recording layer is reversed only in areas where the coercive force of the magnetic recording layer is small enough to reverse the magnetization by the applied magnetic field, and a magnetic domain pattern corresponding to the recording signal is formed in the magnetic recording layer ( FIG. 3(d)) Recording of information is completed.

ここでは媒体を毎分1800回転でまわし、記録半径5
7mm、  記録レーザパワー5mW、 磁界変調周波
数3.7MHzで記録を行った。比較のため同じ構成の
光磁気記録媒体の磁性記録層を予め一方向に磁化したも
のについても同様の記録を行った。第4図はこのように
して記録を行った媒体を、再生レーザパワー1mWで再
生したときの再生信号の搬送波対雑音比(CNR)の変
調磁界強度依存性を示したものである。本発明の実施例
の媒体は比較例に比べ飽和のCNRが1dB程度低いも
のの1、飽和に要する変調磁界強度は1000e程度低
く、実に500eの変調磁界で良好な記録を行うことが
できる。
Here, the medium is rotated at 1800 revolutions per minute, and the recording radius is 5.
7 mm, recording laser power of 5 mW, and magnetic field modulation frequency of 3.7 MHz. For comparison, similar recording was performed on a magneto-optical recording medium having the same configuration, the magnetic recording layer of which was previously magnetized in one direction. FIG. 4 shows the dependence of the carrier-to-noise ratio (CNR) of the reproduced signal on the intensity of the modulated magnetic field when the medium recorded in this manner is reproduced with a reproduction laser power of 1 mW. Although the medium of the embodiment of the present invention has a saturation CNR lower by about 1 dB than the comparative example, the modulation magnetic field strength required for saturation is about 1000e lower, and good recording can be performed with a modulation magnetic field of 500e.

なお同様な結果は、記録時に磁界のみでなくレーザ光も
記録信号に応じて変調した場合にも得られた。
Note that similar results were obtained when not only the magnetic field but also the laser beam was modulated according to the recording signal during recording.

[発明の効果] 以上に述べたように本発明によれば、磁界変調記録方式
において、小さな変調磁界でも情報のダイレクトオーバ
ーライドが可能な光磁気記録媒体を提供するこ・とが可
能になる。この結果、これまで磁界変調方式の課題とさ
れていたデータ転送レートの高速化を容易に実現するこ
とができるという効果を有する。なおこのような効果は
、本願実施例に示された構造、構成の光磁気記録媒体に
のみ得られるものではなく、他の材料、構成を用いた光
磁気記録媒体においても同様な効果が得られることは言
うまでもない。
[Effects of the Invention] As described above, according to the present invention, it is possible to provide a magneto-optical recording medium in which information can be directly overridden even with a small modulated magnetic field in a magnetic field modulation recording method. As a result, it is possible to easily achieve a higher data transfer rate, which has been a problem with magnetic field modulation methods. Note that such an effect is not only obtained with the magneto-optical recording medium having the structure and configuration shown in the examples of this application, but also with a magneto-optical recording medium using other materials and configurations. Needless to say.

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

第1図は本発明の構成を表す、磁性記録層の平面図。 101・・・データ記録部 102・・・非記録部 第2図は実施例における光磁気記録媒体の構成を表す図
。 201・・・ディスク基板 202・・・干渉層 203・・・磁性記録層 204・・・保護層 205・・・反射層 206・・・保護コート層 第3図は磁界変調方式による情報の記録について説明す
る図。 第4図は搬送波対雑音比の変調磁界強度依存性を示す図
。 以上
FIG. 1 is a plan view of a magnetic recording layer showing the configuration of the present invention. 101...Data recording section 102...Non-recording section FIG. 2 is a diagram showing the configuration of a magneto-optical recording medium in an embodiment. 201...Disk substrate 202...Interference layer 203...Magnetic recording layer 204...Protective layer 205...Reflection layer 206...Protective coat layer Figure 3 shows information recording by magnetic field modulation method. Diagram to explain. FIG. 4 is a diagram showing the dependence of carrier wave-to-noise ratio on modulated magnetic field strength. that's all

Claims (1)

【特許請求の範囲】[Claims] 記録情報に応じて変調した磁界を印加すると同時に、一
定の強度または記録情報に応じて変調した収束光を磁性
記録層に照射することによって情報の記録を行なう光磁
気記録媒体において、該磁性記録層のうち情報の記録が
行われる領域に隣接する、情報の記録が行われない領域
が消磁状態にあることを特徴とする光磁気記録媒体。
In a magneto-optical recording medium in which information is recorded by applying a magnetic field modulated according to the recorded information and simultaneously irradiating the magnetic recording layer with a fixed intensity or focused light modulated according to the recorded information, the magnetic recording layer A magneto-optical recording medium characterized in that an area where information is not recorded adjacent to an area where information is recorded is in a demagnetized state.
JP12583689A 1989-05-19 1989-05-19 Magneto-optical recording medium Pending JPH02306445A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12583689A JPH02306445A (en) 1989-05-19 1989-05-19 Magneto-optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12583689A JPH02306445A (en) 1989-05-19 1989-05-19 Magneto-optical recording medium

Publications (1)

Publication Number Publication Date
JPH02306445A true JPH02306445A (en) 1990-12-19

Family

ID=14920142

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12583689A Pending JPH02306445A (en) 1989-05-19 1989-05-19 Magneto-optical recording medium

Country Status (1)

Country Link
JP (1) JPH02306445A (en)

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