JPH0731828B2 - Photothermal magnetic recording medium - Google Patents
Photothermal magnetic recording mediumInfo
- Publication number
- JPH0731828B2 JPH0731828B2 JP14580787A JP14580787A JPH0731828B2 JP H0731828 B2 JPH0731828 B2 JP H0731828B2 JP 14580787 A JP14580787 A JP 14580787A JP 14580787 A JP14580787 A JP 14580787A JP H0731828 B2 JPH0731828 B2 JP H0731828B2
- Authority
- JP
- Japan
- Prior art keywords
- layer
- transition metal
- magnetization
- read
- recording medium
- 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
- 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
Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、例えば光磁気メモリや磁気的表示素子等に
用いられる光熱磁気記録媒体に関する。The present invention relates to a magneto-optical recording medium used in, for example, a magneto-optical memory or a magnetic display element.
〔従来の技術〕 従来より高密度記録が可能な記録媒体として膜面垂直方
向に磁化容易軸を有する希土類遷移金属薄膜を用いる光
熱磁気記録媒体が検討されている。なかでも再生時のSN
比が良好で記録感度が高い媒体として、特開昭56−1535
46号公報に高保磁力の書き込み層と磁気光学効果の大き
な読み出し層からなる2層構造記録媒体が提案されてい
る。第2図はこのような2層構造の従来の光熱磁気記録
媒体の断面図で、図中(1)は基板、(2)は書き込み
層、(3)は読み出し層、(4)は透明な保護層、
(5)は読み出しに用いられるレーザー光、(6)
(7)はそれぞれ各層(2),(3)における遷移金属
副格子磁化の方向を示す矢印である。[Prior Art] Conventionally, as a recording medium capable of high-density recording, a magneto-optical recording medium using a rare earth transition metal thin film having an easy axis of magnetization in the direction perpendicular to the film surface has been studied. Above all, SN during playback
As a medium having a good ratio and high recording sensitivity, Japanese Patent Laid-Open No. 56-1535
Japanese Patent Laid-Open Publication No. 46-46 proposes a two-layer structure recording medium comprising a writing layer having a high coercive force and a reading layer having a large magneto-optical effect. FIG. 2 is a sectional view of a conventional magneto-optical recording medium having such a two-layer structure. In the figure, (1) is a substrate, (2) is a write layer, (3) is a read layer, and (4) is transparent. Protective layer,
(5) is a laser beam used for reading, (6)
(7) is an arrow indicating the direction of the transition metal sublattice magnetization in each of the layers (2) and (3).
次に上記従来例の情報読み出しに関する動作につき説明
する。情報は磁化の向きが上を向いているか下を向いて
いるかの磁化パターンで記録されている。まずレーザー
光(5)を透明保護層(4)の側から読み出し層(3)
に入射する。該レーザー光は反射する際、磁気光学効果
によりその偏光方位が、カー回転角だけ回転する。偏光
方位の回転は、検光子により光量の大小に変えられた
後、光電変換素子により電気信号に変換される。即ち媒
体の磁化パターンが電気信号として再生される。Next, the operation relating to the information reading of the above conventional example will be described. Information is recorded in a magnetization pattern indicating whether the magnetization direction is upward or downward. First, the laser light (5) is read from the transparent protective layer (4) side to the readout layer (3).
Incident on. When the laser light is reflected, its polarization direction rotates by the Kerr rotation angle due to the magneto-optical effect. The rotation of the polarization direction is converted into an electric signal by the photoelectric conversion element after the light amount is changed by the analyzer. That is, the magnetization pattern of the medium is reproduced as an electric signal.
上記の例で、書き込み層(2)としては記録特性に優れ
る希土類副格子磁化優勢な層を、読み出し層(3)とし
ては磁気光学効果の大きな遷移金属副格子磁化優勢な層
を用いる事が望ましいが、しかしながらこの場合、次の
様な問題点がある。即ち、読み出し層(3)の磁化反転
に要するエネルギーを保磁力エネルギーEc、書き込み層
(2)と読み出し層(3)の遷移金属副格子磁化の方向
(6)と(7)が逆方向を向く時に、変換力により両層
(2)(3)の界面に蓄えられる磁気的エネルギーをEw
とすると Ec>Ew の場合には、書き込み層の遷移金属副格子磁化の方向
(6)に対して、読み出し層の遷移金属副格子磁化が交
換力により同じ方向を向く事なく、第2図に示されてい
る如く、両層の遷移金属副格子磁化の方向(6)(7)
が互いに逆方向を向く。この場合、読み出し層のカー回
転角は、書き込み層の、符号が逆のカー回転角に一部相
殺され、全体としてのカー回転角は減少し、再生信号強
度が低下するという問題がある。In the above example, it is desirable to use a rare earth sublattice magnetization dominant layer having excellent recording characteristics as the writing layer (2) and a transition metal sublattice magnetization dominant layer having a large magneto-optical effect as the reading layer (3). However, in this case, there are the following problems. That is, the energy required for reversing the magnetization of the read layer (3) is the coercive force energy Ec, and the directions (6) and (7) of the transition metal sublattice magnetizations of the write layer (2) and the read layer (3) are opposite to each other. At times, the magnetic energy stored at the interface between both layers (2) and (3) due to the conversion force is Ew.
Then, in the case of Ec> Ew, the transition metal sublattice magnetization of the read layer does not face the same direction due to the exchange force with respect to the direction (6) of the transition metal sublattice magnetization of the write layer. As shown, the directions of transition metal sublattice magnetization in both layers (6) (7)
Face in opposite directions. In this case, there is a problem that the Kerr rotation angle of the reading layer is partially offset by the Kerr rotation angle of the writing layer having the opposite sign, the Kerr rotation angle as a whole is reduced, and the reproduction signal strength is lowered.
この発明は上記のような問題点を解消するためになされ
たものであり、優れた書き込み特性と、読み出し層の大
きなカー回転角を有効に利用して再生信号強度の大きな
光熱磁気記録媒体を得ることを目的としている。The present invention has been made in order to solve the above problems, and obtains a magneto-thermomagnetic recording medium having a high reproduction signal intensity by effectively utilizing excellent writing characteristics and a large Kerr rotation angle of a read layer. Is intended.
この発明の光熱磁気記録媒体は、膜面に垂直方向に磁化
容易軸を有し、希土類副格子磁化優勢な希土類遷移金属
から成る書き込み層と、膜面に垂直方向に磁化容易軸を
有し、遷移金属副格子磁化優勢な希土類遷移金属から成
る読み出し層とを基板に積層して構成するものにおい
て、上記書き込み層と読み出し層の遷移金属副格子磁化
の方向が逆を向くときに、両層の界面に蓄えられる磁気
的エネルギーが、読み出し層の保持力エネルギーより大
きいものである。The magneto-optical recording medium of the present invention has an easy axis of magnetization in the direction perpendicular to the film surface, a writing layer made of a rare earth transition metal having a rare earth sublattice magnetization dominant, and an easy axis of magnetization in the direction perpendicular to the film surface, In a case where a read layer made of a rare earth transition metal having a dominant transition metal sublattice magnetization is laminated on a substrate, when the directions of the transition metal sublattice magnetizations of the write layer and the read layer are opposite, The magnetic energy stored at the interface is larger than the coercive energy of the read layer.
この発明においては室温などの使用状態において、書き
込み層と読み出し層の遷移金属副格子磁化の方向が逆を
向くときに、交換力により希土類金属副格子磁化優勢な
層と遷移金属副格子磁化優勢な層の界面に蓄えられる磁
気的エネルギーが遷移金属副格子磁化優勢な層の保磁力
エネルギーより大きいことによつてカー回転角に寄与す
る両層の遷移金属副格子磁化の向きが同じ方向を向くた
めに両層のカー回転角は相殺される事がなく大きな再生
信号強度を得ることができる。According to the present invention, when the writing layer and the reading layer have opposite transition metal sublattice magnetization directions in the usage state such as room temperature, the rare earth metal sublattice magnetization predominant layer and the transition metal sublattice magnetization predominant layer are exchanged by the exchange force. Since the magnetic energy stored at the layer interface is larger than the coercive force energy of the layer in which the transition metal sublattice magnetization is dominant, the directions of the transition metal sublattice magnetization of both layers contributing to the Kerr rotation angle are oriented in the same direction. In addition, the Kerr rotation angles of both layers are not canceled and a large reproduction signal strength can be obtained.
以下この発明を実施例により具体的に説明する。 The present invention will be specifically described below with reference to examples.
実施例1 第1図はこの発明の一実施例の光熱磁気記録媒体の断面
図で(1)はポリカーボネイト製の透明基板、(2)は
基土類金属副格子磁化優勢な書き込み層であり、(3)
は遷移金属副格子磁化優勢な読み出し層であり両層の組
成は 書き込み層(2):Tb24(Fe95Co5)76 読み出し層(3):Tb18(Fe80Co20)82 である。(4)は透明保護層であるSi−N膜であり各層
(2),(3),(4)はスパツタ法により作製した。
(5),(6),(7)については、従来例を示す第2
図と全く同一である。Embodiment 1 FIG. 1 is a cross-sectional view of a magneto-optical recording medium according to an embodiment of the present invention, (1) is a transparent substrate made of polycarbonate, (2) is a sub-lattice magnetism-dominant writing layer of a basic earth metal, (3)
Is a read layer in which the transition metal sublattice magnetization is dominant, and the composition of both layers is write layer (2): Tb 24 (Fe 95 Co 5 ) 76 read layer (3): Tb 18 (Fe 80 Co 20 ) 82 . (4) is a Si-N film which is a transparent protective layer, and each layer (2), (3) and (4) was produced by the sputtering method.
Regarding (5), (6), and (7), the second example showing the conventional example
It is exactly the same as the figure.
上記のように構成された光熱磁気記録媒体において書き
込み層(2)と読み出し層(3)のそれぞれの遷移金属
副格子磁化の方向が互いに逆方向に向いた時に蓄えられ
る磁気的エネルギー(Ew)は、5erg/cm2であり読み出し
層の保磁力エネルギー(Ec)1.8erg/cm2を上回る値を示
した。この時、両層(2),(3)の遷移金属副格子磁
化の方向(6)と(7)は、互いに逆方向を向くより
は、例え、保磁力エネルギーに抗して読み出し層(3)
の磁化が反転してでも同一方向を向く方が、有するエネ
ルギーは低くなり結果として両層の遷移金属副格子磁化
は、常に第1図に示される如く互いに同方向を向く。再
生を行なう場合、レーザー光(5)は読み出し層(3)
で偏光方位が回転し又一部は、該読み出し層を透過して
書き込み層(2においても偏向方位が回転して反射され
るが、その回転方向は読み出し層(3)と書き込み層
(2)で同じ方向であり結果として両層(2)(3)で
のカー回転角は相殺されずむしろ加算され全体としての
カー回転角は大きな値となる。このことにより以下に示
す従来例における光熱磁気記録媒体に比べ、1.2倍から
1.5倍程度の再生信号強度が得られた。The magnetic energy (Ew) stored when the directions of the transition metal sublattice magnetizations of the write layer (2) and the read layer (3) in the magneto-optical recording medium having the above-described structure are opposite to each other is , 5 erg / cm 2 , which was higher than the coercive force energy (Ec) of the readout layer, 1.8 erg / cm 2 . At this time, the directions (6) and (7) of the transition metal sublattice magnetizations of the two layers (2) and (3) are opposed to the opposite directions to each other, for example, against the coercive force energy. )
If the magnetizations of the two layers are oriented in the same direction, the energy possessed by them will be lower, and as a result, the transition metal sublattice magnetizations of both layers will always be oriented in the same direction as shown in FIG. When reproducing, the laser beam (5) emits light to the readout layer (3).
The polarization azimuth is rotated by, and a part of the light is transmitted through the read layer and is reflected by the write layer (in the case of 2, the polarization azimuth is also rotated and reflected, but the rotation directions are the read layer (3) and the write layer (2). As a result, the Kerr rotation angles in both layers (2) and (3) are not offset but rather added and the Kerr rotation angle as a whole becomes a large value. From 1.2 times compared to recording media
A reproduction signal strength of about 1.5 times was obtained.
従来例 第2図において、書き込み層(2)および読み出し層
(3)の組成は 書き込み層:Dy24Fe76 読み出し層:Gd18Co82 である。この場合のEwは0.7、Ecは0.9であり、上記実施
例のように、磁気的エネルギー(Ew)が保磁力エネルギ
ー(Ec)を上回らなかった。Conventional Example In FIG. 2, the composition of the write layer (2) and the read layer (3) is: write layer: Dy 24 Fe 76 read layer: Gd 18 Co 82 . In this case, Ew was 0.7 and Ec was 0.9, and the magnetic energy (Ew) did not exceed the coercive force energy (Ec) as in the above-mentioned Examples.
実施例2〜5 書き込み層(2)と読み出し層(3)を、表に示す材料
で構成する以外は、実施例1と同様にしてこの発明の他
の実施例の光熱磁気記録媒体を得た。又、上記表には、
表に示す材料の組合せを用いた時のEwとEcの値も同時に
示す。これらの組み合せにおいてもEwはEcより大きな値
を示しており、両層(2),(3)は遷移金属副格子磁
化の方向(6)と(7)は互いに同方向を向いた。従つ
て実施例1と同様に、従来例における光熱磁気記録媒体
よりも1.1倍から1.3倍程度大きな再生信号強度が得られ
た。Examples 2 to 5 Photothermomagnetic recording media of other examples of the present invention were obtained in the same manner as in Example 1 except that the write layer (2) and the read layer (3) were made of the materials shown in the table. . Also, in the above table,
The values of Ew and Ec when the combinations of materials shown in the table are used are also shown at the same time. Even in these combinations, Ew showed a value larger than Ec, and the transition metal sublattice magnetization directions (6) and (7) in both layers (2) and (3) were oriented in the same direction. Therefore, similar to Example 1, a reproduction signal intensity 1.1 to 1.3 times larger than that of the magneto-optical recording medium in the conventional example was obtained.
なお上記実施例では保護層(4)の側から再生を行なつ
たが、読み出し層(3)と書き込み層(2)の位置を入
れ替えて、透明基板(1)の側からレーザー光(5)を
入射し再生を行なう様にしても同様の効果が得られる。
また、その場合、読み出し層(3)と透明基板(1)の
間にSi−N膜のような光干渉層を設けても本発明の効果
はかわらない。 Although reproduction was performed from the side of the protective layer (4) in the above example, the positions of the read layer (3) and the write layer (2) were exchanged, and laser light (5) was emitted from the transparent substrate (1) side. The same effect can be obtained even when the light beam is incident to perform reproduction.
In that case, the effect of the present invention is not changed even if an optical interference layer such as a Si-N film is provided between the readout layer (3) and the transparent substrate (1).
なお書き込み層(2)と読み出し層(3)の界面に蓄え
られるエネルギーEwは両層を構成する材料、及び両層の
界面の清浄度により決定される値であり、また読み出し
層の保磁力エネルギーEcは、該読み出し層の飽和磁化、
保磁力、膜厚の3者の積の2倍であらわされる。従つて
使用者は、Ec<Ewの条件をみたす範囲内で上記飽和磁
化、保磁力、膜厚等を適切に選択して、読み出し層、書
き込み層として上記実施例以外の組成、材料を用いる事
ができる。The energy Ew stored at the interface between the writing layer (2) and the reading layer (3) is a value determined by the materials forming both layers and the cleanliness of the interface between both layers, and the coercive energy of the reading layer. Ec is the saturation magnetization of the read layer,
It is expressed as twice the product of coercive force and film thickness. Therefore, the user should properly select the above-mentioned saturation magnetization, coercive force, film thickness, etc. within the range satisfying the condition of Ec <Ew, and use the composition and material other than those in the above-mentioned examples as the read layer and the write layer. You can
以上説明したとおり、この発明は膜面に垂直方向に磁化
容易軸を有し、希土類副格子磁化優勢な希土類遷移金属
から成る書き込み層と、膜面に垂直方向に磁化容易軸を
有し、遷移金属副格子磁化優勢な希土類遷移金属から成
る読み出し層とを基板に積層して構成するものにおい
て、上記書き込み層と読み出し層の遷移金属副格子磁化
の方向が逆を向くときに、両層の界面に蓄えられる磁気
的エネルギーが、読み出し層の保磁力エネルギーより大
きいものを用いることにより、読み出し層の大きなカー
回転角を有効に利用して再生信号強度の大きな光熱磁気
記録媒体を得ることができる。As described above, the present invention has a writing layer made of a rare earth transition metal having a rare earth sublattice magnetization dominant axis and an easy axis of magnetization in a direction perpendicular to the film surface, and a transition layer having a magnetization easy axis in the direction perpendicular to the film surface. In a structure in which a read layer composed of a rare earth transition metal having a metal sublattice magnetization predominant is laminated on a substrate, when the directions of the transition metal sublattice magnetizations of the write layer and the read layer are opposite to each other, the interface between the layers is formed. When the magnetic energy stored in the read layer is larger than the coercive force energy of the read layer, it is possible to effectively utilize the large Kerr rotation angle of the read layer to obtain a magneto-thermomagnetic recording medium having a high reproduction signal intensity.
第1図はこの発明の一実施例の光熱磁気記録媒体の断面
図、第2は従来の光熱磁気記録媒体の断面図である。図
において(1)は基板、(2)は書き込み層、(3)は
読み出し層、(6)(7)はそれぞれ該書き込み層、読
み出し層においける遷移金属副格子磁化の方向を示す矢
印である。 なお各図中同一符号は同一あるいは相当部分を示す。FIG. 1 is a sectional view of a magneto-optical recording medium according to an embodiment of the present invention, and FIG. 2 is a sectional view of a conventional magneto-optical recording medium. In the figure, (1) is a substrate, (2) is a writing layer, (3) is a reading layer, and (6) and (7) are arrows showing the directions of transition metal sublattice magnetization in the writing layer and the reading layer, respectively. is there. In the drawings, the same reference numerals indicate the same or corresponding parts.
Claims (1)
類副格子磁化優勢な希土類遷移金属から成る書き込み層
と、膜面に垂直方向に磁化容易軸を有し、遷移金属副格
子磁化優勢な希土類遷移金属から成る読み出し層とを基
板に積層して構成するものにおいて、上記書き込み層と
読み出し層の遷移金属副格子磁化の方向が逆を向くとき
に両層の界面に蓄えられる磁気的エネルギーが、読み出
し層の保持力エネルギーより大きいことを特徴とする光
熱磁気記録媒体。1. A rare-earth sublattice write layer having an easy axis of magnetization in the direction perpendicular to the film surface and a transition metal sublattice having an easy axis of magnetization in the direction perpendicular to the film surface. In a structure in which a read layer made of a rare earth transition metal having a dominant magnetization is laminated on a substrate, the magnetic field stored in the interface between the write layer and the read layer when the directions of the transition metal sublattice magnetizations are opposite. Energy is greater than the coercive energy of the read layer.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14580787A JPH0731828B2 (en) | 1987-06-10 | 1987-06-10 | Photothermal magnetic recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14580787A JPH0731828B2 (en) | 1987-06-10 | 1987-06-10 | Photothermal magnetic recording medium |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63308752A JPS63308752A (en) | 1988-12-16 |
| JPH0731828B2 true JPH0731828B2 (en) | 1995-04-10 |
Family
ID=15393598
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP14580787A Expired - Lifetime JPH0731828B2 (en) | 1987-06-10 | 1987-06-10 | Photothermal magnetic recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0731828B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02230535A (en) * | 1989-03-02 | 1990-09-12 | Seiko Epson Corp | magneto-optical recording medium |
-
1987
- 1987-06-10 JP JP14580787A patent/JPH0731828B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63308752A (en) | 1988-12-16 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JP2986622B2 (en) | Magneto-optical memory device and its recording / reproducing method | |
| JPH039545B2 (en) | ||
| US4842956A (en) | Opto-magnetic recording medium having three exchange-coupled magnetic layers | |
| EP0522840B1 (en) | Magneto-optical recording medium | |
| JPS61196445A (en) | Photomagnetic disk | |
| JPH036582B2 (en) | ||
| JP2685888B2 (en) | Magneto-optical recording medium | |
| JPH0731828B2 (en) | Photothermal magnetic recording medium | |
| JP2550633B2 (en) | Photothermal magnetic recording medium | |
| JPS6314342A (en) | Magneto-optical recording medium | |
| JP3108397B2 (en) | Magneto-optical recording medium | |
| JP3093340B2 (en) | Magneto-optical recording medium | |
| JPH0795376B2 (en) | Photothermal magnetic recording medium | |
| JPH0350344B2 (en) | ||
| JPH0614416B2 (en) | Magneto-optical recording / reproducing method | |
| JPS59132434A (en) | Magneto-optic storage element | |
| KR100209285B1 (en) | Short-wavelength magneto-optical disk | |
| JP2705066B2 (en) | Photothermal magnetic recording media | |
| KR930002168B1 (en) | Magneto-optical memory media | |
| JPS5956241A (en) | magneto-optical recording medium | |
| JPH0462140B2 (en) | ||
| JP2613885B2 (en) | Magneto-optical multilayer media | |
| JPH0458662B2 (en) | ||
| JPH0453047A (en) | Optical memory element | |
| JPS6316440A (en) | Magneto-optical recording medium |