JPH06101155B2 - Magneto-optical recording / reproducing method - Google Patents
Magneto-optical recording / reproducing methodInfo
- Publication number
- JPH06101155B2 JPH06101155B2 JP10585187A JP10585187A JPH06101155B2 JP H06101155 B2 JPH06101155 B2 JP H06101155B2 JP 10585187 A JP10585187 A JP 10585187A JP 10585187 A JP10585187 A JP 10585187A JP H06101155 B2 JPH06101155 B2 JP H06101155B2
- Authority
- JP
- Japan
- Prior art keywords
- wavelength
- magneto
- reflectance
- optical recording
- 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.)
- Expired - Lifetime
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Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、書き込み用と読み出し用に異なる波長を用
いた光磁気記録再生方法に関する。The present invention relates to a magneto-optical recording / reproducing method using different wavelengths for writing and reading.
従来、光磁気記録媒体として、希土類−遷移金属非晶質
合金がよく知られている。例えばTbFeCo3元系媒体は、
約170℃のキュリー温度を有し、カー回転も大きい優れ
た記録媒体である。しかし、磁性膜単層では、記録感
度、及び読み出し時のSN比(シグナル、イノズ)が不充
分であり、磁性層表面での反射を防止し熱効率を高める
と同時に、カーエンハンスメント効果によるカー回転角
の増大を計る反射防止膜が必要である。特開昭56−1569
43号公報等で提案されている単層反射防止膜では、実用
的な誘電体材料と膜厚の範囲において得られる反射率の
最小値とエンハンスされたカー回転角は制限があり、記
録感度および読み出し時のSN比の向上に対する効果は限
られる。また、特開昭59−227054号公報等で提案されて
いる多層構成の反射防止においては、反射率の最小値を
零まで小さくすることが可能であり、良好な記録感度が
得られると共に、反射率が零に近いところで大きなカー
回転角が得られ高SN比が得られる。しかし、記録されて
いる情報を、破壊することなく読み出すためには、読み
出し時のレーザー光強度に上限が存在し、従つてレーザ
ーの波長に対し一定値以上の反射率が必要とされる。逆
に大きな光強度で読み出し可能なように、媒体のキュリ
ー温度を上げると記録感度が劣化することになる。Conventionally, a rare earth-transition metal amorphous alloy is well known as a magneto-optical recording medium. For example, the TbFeCo ternary medium is
It is an excellent recording medium having a Curie temperature of about 170 ° C. and a large Kerr rotation. However, with a single magnetic layer, the recording sensitivity and the SN ratio (signal, inos) during reading are insufficient, preventing reflection on the surface of the magnetic layer to improve thermal efficiency, and at the same time the car rotation angle due to the car enhancement effect. It is necessary to have an antireflection film that can increase JP 56-1569
In the single-layer antireflection film proposed in Japanese Patent Laid-Open No. 43, etc., the minimum value of the reflectance and the enhanced Kerr rotation angle obtained in a practical dielectric material and film thickness range are limited, and the recording sensitivity and the The effect on improving the SN ratio during reading is limited. Further, in the antireflection of the multilayer structure proposed in Japanese Patent Laid-Open No. 59-227054, it is possible to reduce the minimum value of the reflectance to zero, and good recording sensitivity can be obtained and When the ratio is close to zero, a large Kerr rotation angle is obtained and a high S / N ratio is obtained. However, in order to read the recorded information without destroying it, there is an upper limit to the laser light intensity at the time of reading, and accordingly, a reflectance of a certain value or more with respect to the wavelength of the laser is required. On the contrary, if the Curie temperature of the medium is increased so that reading can be performed with a high light intensity, the recording sensitivity will be deteriorated.
このように光磁気記録媒体に対し、一波長の光源にて書
き込み、読み出しを行う場合、多層構成の反射防止膜を
有する媒体においても、記録感度と読み出し時のSN比を
同時に向上させるのに限界があり、十分な効果を得るこ
とができない。In this way, when writing and reading to / from a magneto-optical recording medium with a light source of one wavelength, there is a limit to simultaneously improving the recording sensitivity and the SN ratio at the time of reading even in a medium having an antireflection film with a multilayer structure. However, there is no sufficient effect.
この発明はかかる問題点を解決するためになされたもの
で、書き込み効率が向上し、読み出し時のSN比を向上さ
せた光磁気記録再生方法を得ることを目的とする。The present invention has been made to solve the above problems, and an object of the present invention is to obtain a magneto-optical recording / reproducing method in which the writing efficiency is improved and the SN ratio at the time of reading is improved.
この発明の光磁気記録再生方法は、基板、この基板に設
けた反射防止膜、この反射防止膜に設けた記録磁性膜を
備えた光磁気記録媒体に、上記反射防止膜に対して反射
率が小さい第1波長で上記記録磁性膜に書き込み、上記
反射防止膜に対して反射率が大きい第2波長で上記記録
磁性膜から読み出しを行なうものである。In the magneto-optical recording / reproducing method of the present invention, a magneto-optical recording medium including a substrate, an antireflection film provided on the substrate, and a recording magnetic film provided on the antireflection film has a reflectance of the antireflection film. Writing is performed on the recording magnetic film at a small first wavelength, and reading is performed from the recording magnetic film at a second wavelength having a large reflectance with respect to the antireflection film.
この発明において、書き込み用と読み出し用に異なる波
長を用いることにより、書き込み用の波長を反射防止膜
に対して反射率を小さく、例えば零又はその近傍とし、
書き込み効率を大とするとともに、読み出し時に十分な
反射光強度と高SN比を得ることができる。さらに書き込
み効率の増大により、媒体のキュリー温度の上昇に伴う
記録感度の低下を補わせ、読み出し用レーザー光強度の
増加から低反射率化を達成しSN比をさらに向上させるこ
とが可能である。In the present invention, by using different wavelengths for writing and reading, the wavelength for writing has a small reflectance with respect to the antireflection film, for example, zero or its vicinity,
It is possible to increase the writing efficiency and obtain a sufficient reflected light intensity and a high SN ratio at the time of reading. Furthermore, by increasing the writing efficiency, it is possible to compensate for the decrease in recording sensitivity that accompanies an increase in the Curie temperature of the medium, achieve a low reflectance and increase the SN ratio by increasing the intensity of the laser light for reading.
この発明に係わる第1波長および第2波長としては、例
えば二波長にてスイツチングおよび同時発振可能な半導
体レーザーは、例えば刊行物{App1.Phys.Lett,Vo1、4
9,No.24(1629)}徳田等が発表しているGaAsレーザー
で、波長804nmと844nmでスイツチングするものにより得
られる。As the first wavelength and the second wavelength according to the present invention, for example, a semiconductor laser capable of switching and simultaneous oscillation at two wavelengths is disclosed in, for example, the publication {App1.Phys.Lett, Vo1,4.
9, No.24 (1629)} Obtained by the GaAs laser announced by Tokuda et al., Which switches at wavelengths of 804 nm and 844 nm.
又、別々のレーザーで各々発振された波長を用いても良
いのは言うまでもない。Needless to say, the wavelengths oscillated by different lasers may be used.
この発明に係わる基板としては、例えばガラスおよびプ
ラスチツク等書き込み用および読み出し用波長に対して
透過性のものが用いられる。As the substrate according to the present invention, for example, glass, plastic, or the like that is transparent to the writing and reading wavelengths is used.
この発明に係わる反射防止膜は、例えば単層であれば、
第1図に示すように基板の屈折率をns,磁性層の屈折率
をnmとすると、反射防止膜の屈折率nと膜厚dは(1)
式で与えられることが一般に知られている。If the antireflection film according to the present invention is, for example, a single layer,
As shown in FIG. 1, when the refractive index of the substrate is ns and the refractive index of the magnetic layer is nm, the refractive index n and the film thickness d of the antireflection film are (1)
It is generally known that it is given by a formula.
ここで、λは光の波長を示し、ns<n<nmである。 Here, λ indicates the wavelength of light, and ns <n <nm.
実際には、ns,nmの値に対し、(1)式を満たしかつ実
用に適する適当な物質は少なく、反射率を低減させるの
には限度がある。なお第1図はこの発明の一実施例に係
わる光磁気記録媒体の断面図で、(1)は基板、(2)
は反射防止膜、(3)は記録磁性膜で、矢印は光の進行
方向を示す。In reality, there are few suitable substances that satisfy the expression (1) and are suitable for practical use with respect to the values of ns and nm, and there is a limit to reducing the reflectance. 1 is a sectional view of a magneto-optical recording medium according to an embodiment of the present invention, in which (1) is a substrate and (2) is
Is an antireflection film, (3) is a recording magnetic film, and the arrow indicates the traveling direction of light.
そこで反射防止効果を増大させるために、反射防止膜を
多層構成にすることが効果的であり例えば屈折率n1およ
びn2の二層膜をそれぞれnd=λ/4の条件で作るとその強
度反射率は となり、反射防止のためには のように選べばよい。これによつて反射率は1%以下に
することができる。一般にこれらの効果を高めるため
に、高屈折率層(H)と低屈折率層(L)を交互に積み
重ねる方法が採用される。Therefore, in order to increase the antireflection effect, it is effective to make the antireflection film into a multi-layered structure. For example, if two-layer films with refractive indices n 1 and n 2 are made under the condition of nd = λ / 4, the Reflectance is And to prevent reflection You can choose like. Thereby, the reflectance can be reduced to 1% or less. Generally, in order to enhance these effects, a method of alternately stacking high refractive index layers (H) and low refractive index layers (L) is adopted.
第2図はこの発明の他の実施例に係わる光磁気記録媒体
の断面図で、(22)、(24)、(26)は高屈折率膜、
(23)、(25)は低屈折率膜である。FIG. 2 is a sectional view of a magneto-optical recording medium according to another embodiment of the present invention, in which (22), (24) and (26) are high refractive index films,
(23) and (25) are low refractive index films.
実施例1 第1図において、基板(1)としてガラス又はプラスチ
ツク基板を用い、反射防止膜(2)としてSi3N4を用
い、記録磁性膜(3)としてTbFeCoを用いる。Si3N4反
射防止膜厚は、第1波長800nmに対し反射率が最小値、
カー回転角が最大値を示す70nmであり、記録磁性膜は10
0nmである。ここでこの発明の一実施例に係わる光磁気
記録媒体に対する反射率Rとカー回転角θkの波長依存
性を示す特性図を第3図に示す。Example 1 In FIG. 1, a glass or plastic substrate is used as the substrate (1), Si 3 N 4 is used as the antireflection film (2), and TbFeCo is used as the recording magnetic film (3). The Si 3 N 4 antireflection film has a minimum reflectance for the first wavelength of 800 nm,
The Kerr rotation angle is 70 nm, which is the maximum value, and the recording magnetic film is 10 nm.
It is 0 nm. FIG. 3 is a characteristic diagram showing the wavelength dependence of the reflectance R and the Kerr rotation angle θk for the magneto-optical recording medium according to the embodiment of the present invention.
図において、横軸は波長(nm)、縦軸は反射率(%)お
よびカー回転角(deg・)を第1波長800nmにおける反射
率17%に対し、第2波長850nmにおける反射率は18.5%
を示す。この媒体に、第1波長で書き込み、第2波長で
読み出しを行つたところ、読み出し時のSN比は第2波長
のみで書き込み読み出しを行つた場合とほぼ同程度のま
ま、書き込み時の記録感度を約0.5%良くすることかで
きた。In the figure, the horizontal axis is the wavelength (nm), and the vertical axis is the reflectance (%) and the Kerr rotation angle (deg.) For the reflectance of 17% at the first wavelength of 800 nm and the reflectance of 18.5% at the second wavelength of 850 nm.
Indicates. When this medium was written at the first wavelength and read at the second wavelength, the SN ratio at the time of reading was almost the same as that at the time of writing and reading at the second wavelength only, and the recording sensitivity at the time of writing was improved. I was able to improve it by about 0.5%.
しかし、第3図を見てもわかるように、反射防止膜が単
層の場合、通常の基板(n=1.5〜1.8)に対して物理化
学的に安定で高耐久性の膜を得ようとすると材料が限ら
れる。また反射率も、実用的な膜厚(均一な膜が得られ
る最小膜厚から成膜に困難でない程度の膜厚)におい
て、最小値が10%以下になることは難しく、波長依存性
も緩やかになるため、第1波長と第2波長での反射率差
を十分得られない。従つて、2波長で書き込みと読み出
しをそれぞれ行うことの利点を十分に発揮するために
は、波長依存性の立ち上がりの急峻な多層構造の反射防
止膜を用いる方が望ましい。However, as can be seen from FIG. 3, when the antireflection film is a single layer, it is attempted to obtain a physicochemically stable and highly durable film for an ordinary substrate (n = 1.5 to 1.8). Then the materials are limited. In addition, it is difficult for the reflectance to have a minimum value of 10% or less in a practical film thickness (thickness from the minimum film thickness at which a uniform film can be obtained to a film thickness at which film formation is not difficult), and the wavelength dependence is gentle. Therefore, a sufficient difference in reflectance between the first wavelength and the second wavelength cannot be obtained. Therefore, in order to fully exert the advantages of writing and reading at two wavelengths, it is desirable to use an antireflection film having a multilayer structure with a sharp rise in wavelength dependence.
実施例2 光磁気記録媒体における反射防止膜としては高屈折率膜
に例えば屈折率2.0のTa2O5膜、屈折力1.9のZrO2膜、TiO
2膜等を、低屈折率膜に例えば屈折率1.45のSiO2膜、屈
折率1.38のMgF2膜等を、又、GaAsレーザーを用い804nm
と844nmを得る。Example 2 As the antireflection film in the magneto-optical recording medium, a high refractive index film such as a Ta 2 O 5 film having a refractive index of 2.0, a ZrO 2 film having a refractive power of 1.9, and TiO 2 are used.
2 film, low refractive index film such as SiO 2 film with a refractive index of 1.45, MgF 2 film with a refractive index of 1.38, and 804 nm using a GaAs laser.
And get 844 nm.
ここで、第2図において、ガラス基板またはプラスチッ
ク基板(1)上に高屈折率膜(22)(24)(26)と低屈
折率(23)、(25)を、波長804nmに対しnd=λ/4とな
る膜厚にて交互に5層(HLHLH)設け、さらにTbFeCo3元
系非晶質記録磁性層(3)を設けたこの発明の他の実施
例に係わる光磁気記録媒体を得、その反射率の波長依存
性を示す特性図を第4図に得た。Here, in FIG. 2, high refractive index films (22), (24) and (26) and low refractive indexes (23) and (25) are provided on a glass substrate or a plastic substrate (1) at a wavelength of 804 nm. A magneto-optical recording medium according to another embodiment of the present invention is provided in which five layers (HLHLH) are alternately provided with a film thickness of λ / 4, and further a TbFeCo ternary amorphous recording magnetic layer (3) is provided. A characteristic diagram showing the wavelength dependence of the reflectance is obtained in FIG.
図において、軸横は波長(nm)縦軸は反射率(%)を示
す。第4図から明らかなように第一波長804nmにおいて
反射率は約4%に低減された。これに対し第二波長844n
mにおける反射率は約20〜30%であり、第一波長により
書き込み、第二波長にして読み出すことにより、従来の
読み出し光強度と高SN比を保持したまま、書き込み時の
最適光強度を約10%低減させることができた。In the figure, the horizontal axis represents wavelength (nm) and the vertical axis represents reflectance (%). As is clear from FIG. 4, the reflectance was reduced to about 4% at the first wavelength of 804 nm. On the other hand, the second wavelength 844n
The reflectivity at m is about 20 to 30%, and by writing at the first wavelength and reading at the second wavelength, the optimum light intensity at the time of writing is kept at about the same while maintaining the conventional read light intensity and high SN ratio. It could be reduced by 10%.
また、記録磁性媒体のキュリー温度を約5%高めること
により、従来の書き込み時の光強度を約4%低減させか
つ読み出し時の光強度を約4%上昇させることによりSN
比を約2%増大させることができた。Moreover, by increasing the Curie temperature of the recording magnetic medium by about 5%, the conventional light intensity during writing is reduced by about 4% and the light intensity during reading is increased by about 4%.
The ratio could be increased by about 2%.
以上説明したとおり、この発明は基板、この基板に設け
た反射防止膜、この反射防止膜に設けた記録磁性膜を備
えた光磁気記録媒体に、上記反射防止膜に対して反射率
が小さい第1波長で上記記録磁性膜に書き込み、上記反
射防止膜に対して反射率が大きい第2波長で上記記録磁
性膜から読み出しを行なうことにより、書き込み効率が
向上し、読み出し時のSN比を向上させた光磁気記録再生
方法を得ることができる。As described above, the present invention provides a magneto-optical recording medium including a substrate, an antireflection film provided on the substrate, and a recording magnetic film provided on the antireflection film. By writing to the recording magnetic film at one wavelength and reading from the recording magnetic film at the second wavelength having a large reflectance with respect to the antireflection film, the writing efficiency is improved and the SN ratio at the time of reading is improved. It is possible to obtain a magneto-optical recording / reproducing method.
第1図はこの発明の一実施例に係わる光磁気記録媒体の
断面図、第2図はこの発明の他の実施例に係わる光磁気
記録媒体の断面図、第3図はこの発明の一実施例に係わ
る光磁気記録媒体の反射率(%)およびカー回転角(de
g)の波長(nm)依存性を示す特性図、第4図はこの発
明の他の実施例に係わる光磁気記録媒体の反射率(%)
の波長依存性を示す特性図を示す。 図において、(1)は基板、(2)は反射防止膜、
(3)は記録磁性膜を示す。 なお、各図中同一符号は同一又は相当部分を示す。FIG. 1 is a sectional view of a magneto-optical recording medium according to an embodiment of the present invention, FIG. 2 is a sectional view of a magneto-optical recording medium according to another embodiment of the present invention, and FIG. 3 is an embodiment of the present invention. The magneto-optical recording medium according to the example has a reflectance (%) and a Kerr rotation angle (de
FIG. 4 is a characteristic diagram showing the wavelength (nm) dependence of g), and FIG. 4 is the reflectance (%) of the magneto-optical recording medium according to another embodiment of the present invention.
The characteristic view which shows the wavelength dependence of is shown. In the figure, (1) is a substrate, (2) is an antireflection film,
(3) shows a recording magnetic film. In the drawings, the same reference numerals indicate the same or corresponding parts.
Claims (3)
反射防止膜に設けた記録磁性膜を備えた光磁気記録媒体
に、上記反射防止膜に対して反射率が小さい第1波長で
上記記録磁性膜に書き込み、上記反射防止膜に対して反
射率が大きい第2波長で上記記録磁性膜から読み出しを
行なう光磁気記録再生方法。1. A magneto-optical recording medium comprising a substrate, an antireflection film provided on the substrate, and a recording magnetic film provided on the antireflection film, at a first wavelength having a small reflectance with respect to the antireflection film. A magneto-optical recording / reproducing method of writing to the recording magnetic film and reading from the recording magnetic film at a second wavelength having a large reflectance with respect to the antireflection film.
1項記載の光磁気記録再生方法。2. The magneto-optical recording / reproducing method according to claim 1, wherein the antireflection film has a multi-layer structure.
反射率が最小値又はその近傍値を示し、読み出し用第2
波長に対して反射率が20〜30%程度である特許請求の範
囲第1項又は第2項記載の光磁気記録再生方法。3. The antireflection film has a minimum reflectance or a value close to it for the first wavelength for writing, and the second reflectance for reading
The magneto-optical recording / reproducing method according to claim 1 or 2, wherein the reflectance is about 20 to 30% with respect to the wavelength.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10585187A JPH06101155B2 (en) | 1987-04-28 | 1987-04-28 | Magneto-optical recording / reproducing method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10585187A JPH06101155B2 (en) | 1987-04-28 | 1987-04-28 | Magneto-optical recording / reproducing method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63269359A JPS63269359A (en) | 1988-11-07 |
| JPH06101155B2 true JPH06101155B2 (en) | 1994-12-12 |
Family
ID=14418500
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10585187A Expired - Lifetime JPH06101155B2 (en) | 1987-04-28 | 1987-04-28 | Magneto-optical recording / reproducing method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH06101155B2 (en) |
-
1987
- 1987-04-28 JP JP10585187A patent/JPH06101155B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63269359A (en) | 1988-11-07 |
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