JPH081709B2 - Magneto-optical recording medium - Google Patents

Magneto-optical recording medium

Info

Publication number
JPH081709B2
JPH081709B2 JP16201889A JP16201889A JPH081709B2 JP H081709 B2 JPH081709 B2 JP H081709B2 JP 16201889 A JP16201889 A JP 16201889A JP 16201889 A JP16201889 A JP 16201889A JP H081709 B2 JPH081709 B2 JP H081709B2
Authority
JP
Japan
Prior art keywords
magneto
optical recording
layer
recording medium
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 - Fee Related
Application number
JP16201889A
Other languages
Japanese (ja)
Other versions
JPH0325737A (en
Inventor
崇 冨江
公夫 木下
和富 鈴木
忠則 中谷
潔 千葉
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.)
Teijin Ltd
Original Assignee
Teijin 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 Teijin Ltd filed Critical Teijin Ltd
Priority to JP16201889A priority Critical patent/JPH081709B2/en
Publication of JPH0325737A publication Critical patent/JPH0325737A/en
Publication of JPH081709B2 publication Critical patent/JPH081709B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Description

【発明の詳細な説明】 <利用分野> 本発明はレーザー等の光により、情報の記録、再生、
消去等を行なう光磁気記録媒体に関する。更に詳細に
は、透明基板上に膜面に垂直な方向に磁化容易方向を有
した金属薄膜よりなる記録層を形成し、光熱磁気効果に
より情報を記録し、磁気光学効果により再生する光磁気
記録媒体に関する。
DETAILED DESCRIPTION OF THE INVENTION <Field of Use> The present invention uses information from a laser or the like to record or reproduce information.
The present invention relates to a magneto-optical recording medium that erases data. More specifically, a magneto-optical recording in which a recording layer made of a metal thin film having an easy magnetization direction in a direction perpendicular to the film surface is formed on a transparent substrate, information is recorded by the photothermomagnetic effect, and is reproduced by the magnetooptical effect. Regarding the medium.

<従来の技術> 光記録媒体は高密度・大容量の情報記録媒体として種
々の研究開発が行なわれている。特に情報の消去可能な
光磁気記録媒体は応用分野が広く種々の材料・システム
が発表されており、その実用化が待望されている。
<Prior Art> Various researches and developments have been made on optical recording media as high-density and large-capacity information recording media. In particular, a magneto-optical recording medium capable of erasing information has a wide range of application fields, and various materials and systems have been announced, and their practical application is expected.

上述の光磁気記録材料としては、例えば、特開昭52−
31703号公報記載のFeTb、特開昭56−126907号公報記載
のFeTbGd、特開昭58−73746号公報記載のFeTbCo、FeCoD
y、特開昭61−165846号公報記載のFeNd等既に多くの提
案がある。しかし、これらの情報の消去可能な光磁気記
録媒体の実用化には、記録、再生特性のより一層の向上
が必要である。
Examples of the above-mentioned magneto-optical recording material include, for example, JP-A-52-
FeTb described in JP 31703, FeTbGd described in JP-A-56-126907, FeTbCo described in JP-A-58-73746, FeCoD
y, many proposals such as FeNd described in JP-A-61-165846 have already been made. However, in order to put these magneto-optical recording media into which information can be erased into practical use, it is necessary to further improve the recording and reproducing characteristics.

これに対し、光磁気記録層上、もしくはその上に誘電
体層を介して金属反射層を設ける方法が提案されてい
る。この方法はカー効果とファラデー効果の併用により
高いC/N比を得る点で優れている。従来この金属反射層
として、Alを用いたもの(特開昭58−83346号公報、特
開昭59−132434号公報、)、Cuを用いたもの(特開昭59
−8150号公報)、Al系合金を用いたもの(特開昭62−13
7743号公報、特開昭64−4938号公報)、ステンレスを用
いたもの(特開昭59−171054号公報)、Teを用いたもの
(特開昭62−52744号公報)、非晶質金属膜を用いたも
の(特開昭61−57053号公報)等が提案されている。し
かしながら、高反射率のAl,Cu等を用いた場合にはその
高熱伝導性のため記録感度が大幅に低下し、一方比較的
熱伝導性の低いステンレス、Teを用いた場合には記録感
度は向上するが反射率が低いため、十分なC/N比が得ら
れないという欠点を有する。
On the other hand, a method of providing a metal reflective layer on the magneto-optical recording layer or on the magneto-optical recording layer via a dielectric layer has been proposed. This method is excellent in that a high C / N ratio can be obtained by using the Kerr effect and the Faraday effect together. Conventionally, as the metal reflection layer, one using Al (Japanese Patent Laid-Open No. 58-83346, Japanese Patent Laid-Open No. 59-132434), and one using Cu (Japanese Patent Laid-Open No. 59-59434).
-8150), using an Al alloy (Japanese Patent Laid-Open No. 62-13
7743, JP 64-4938), those using stainless steel (JP 59-171054), those using Te (JP 62-52744), amorphous metal Those using a membrane (Japanese Patent Laid-Open No. 61-57053) have been proposed. However, when high reflectivity Al, Cu, etc. is used, the recording sensitivity is greatly reduced due to its high thermal conductivity, while when stainless steel and Te, which have relatively low thermal conductivity, are used, the recording sensitivity is Although it is improved, it has a drawback that a sufficient C / N ratio cannot be obtained because the reflectance is low.

<発明の目的> 本発明はかかる現状に鑑みなされたもので、高感度で
高C/N比の光磁気記録媒体を提供することを目的とした
ものである。
<Object of the Invention> The present invention has been made in view of the above circumstances, and an object thereof is to provide a magneto-optical recording medium having high sensitivity and a high C / N ratio.

<発明の構成及び作用> 本発明者らは、上述の欠点を克服すべく鋭意検討した
結果、特定の物質で金属反射層を形成することにより、
記録感度、C/N比が高く、更に経時安定性に優れた光磁
気記録媒体が得られることを見出した。
<Structure and Action of Invention> As a result of intensive studies to overcome the above-mentioned drawbacks, the present inventors formed a metal reflective layer with a specific substance,
It has been found that a magneto-optical recording medium having a high recording sensitivity and a high C / N ratio and excellent stability over time can be obtained.

即ち本発明は、金属反射層を有する光磁気記録媒体に
おいて、該金属反射層がAgにCuを0.5〜30at%(原子
%)含有せしめ、さらにTa又はTiの少くとも一種を0.5
〜15at%含有せしめたAg合金からなることを特徴とする
光磁気記録媒体である。
That is, the present invention provides a magneto-optical recording medium having a metal reflective layer, wherein the metal reflective layer contains Ag in an amount of 0.5 to 30 at% (atomic%), and at least one of Ta and Ti is 0.5 to 0.5.
A magneto-optical recording medium characterized by comprising an Ag alloy containing about 15 at%.

上述の本発明は以下のようにしてなされたものであ
る。すなわち、本発明者らは、C/N向上目的に高反射率
のAg膜に着目したが、Agは耐食性のわるい材料であり、
Ag膜のみでは実用的でない。そこで、この改良として他
金属の添加を検討したところ、スライドガラス上に形成
したCuを0.5〜30at%添加したAgCu合金膜は高反射率
で、光磁気記録媒体の標準的な加速劣化テスト条件であ
る80℃85%相対湿度雰囲気下で72時間以上放置しても反
射率が低下せず、耐久性もあることが判明した。なお、
Cuの含有量が0.5at%より少くても、30at%より多くて
も24時間以内に反射率は初期値の9割以下に低下した。
AgCu合金膜は上述の通り高反射率(例えばAg85Cu15(添
字はat%組成)合金膜では830nmの波長で98%の反射
率)であり、耐久性も悪くないが、このAgCu膜は熱伝導
性が高く、そのためこれを反射膜とする光磁気記録媒体
では記録感度が低下することがさらに判明した。
The present invention described above has been made as follows. That is, the present inventors have focused on the Ag film of high reflectance for the purpose of improving C / N, Ag is a poor corrosion resistance material,
Ag film alone is not practical. Therefore, as a result of studying addition of other metals as an improvement, the AgCu alloy film formed by adding 0.5 to 30 at% Cu formed on the slide glass has a high reflectance, and the standard accelerated deterioration test condition of the magneto-optical recording medium is used. It has been found that the reflectance does not decrease even when left for 72 hours or more in an atmosphere of 80 ° C and 85% relative humidity, and it has durability. In addition,
Even if the Cu content was less than 0.5 at% or more than 30 at%, the reflectance decreased to 90% or less of the initial value within 24 hours.
As described above, the AgCu alloy film has a high reflectance (eg, Ag 85 Cu 15 (subscript is at% composition) alloy film has a reflectance of 98% at a wavelength of 830 nm) and durability is not bad, but this AgCu film is It was further found that the magneto-optical recording medium having a high thermal conductivity and using it as a reflective film has a lower recording sensitivity.

本発明者らは、さらにこの点の改良を第3元素の添加
に着目し、鋭意研究の結果、AgCu膜にTa又はTiの少なく
とも一種を0.5〜15at%添加すると、記録感度と耐食性
が大きく向上することを見い出し、本発明に想到した。
The present inventors further focused on the improvement of this point by adding the third element, and as a result of earnest research, as a result of adding 0.5 to 15 at% of at least one of Ta or Ti to the AgCu film, the recording sensitivity and corrosion resistance are significantly improved. As a result, they have come to the present invention.

なお、Ta,Tiの含有量がこの範囲より少いと記録感度
の向上の効果はなく、また逆に多くなると反射が低下
し、C/Nが悪くなる。更にTa,Tiの含有量は、感度向上効
果が大きく、且つC/N向上の効果が阻害されない点で2
〜10at%がより好ましい。なお、経時安定性を更に改善
するために、Cr、Nb、Reなどの他の元素を少量添加して
もよい。
If the content of Ta or Ti is less than this range, there is no effect of improving the recording sensitivity, and conversely, if it is more than this range, the reflection decreases and the C / N deteriorates. Furthermore, the content of Ta and Ti has a large effect of improving the sensitivity, and the effect of improving the C / N is not hindered.
-10at% is more preferable. Incidentally, in order to further improve the stability over time, a small amount of another element such as Cr, Nb or Re may be added.

この金属反射層の膜厚は100〜1000Åが好ましく、200
〜700Åが更に好ましい。厚すぎる場合には感度が低下
し、薄すぎる場合には反射率が低下しC/Nがわるくな
る。
The thickness of this metal reflective layer is preferably 100 to 1000Å, 200
~ 700Å is more preferable. If it is too thick, the sensitivity decreases, and if it is too thin, the reflectance decreases and the C / N becomes poor.

なお、本発明において金属反射層の光磁気記録層側と
反対側に接して、付加的にTi等の熱伝導率の小さい金属
膜、又は誘電体膜を設けてもよい。特に熱伝導を抑える
ために本発明の金属反射層が400Å以下と薄いときにはT
i層の金属膜を設けると反射率の低下を防止するととも
に耐食性が向上して更に好ましい結果が得られる。同様
に誘電体膜は、光磁気記録媒体がきわめてきびしい環境
下で使用されることが想定される時は、保護層として設
けるとよい。
In the present invention, a metal film having a low thermal conductivity such as Ti or a dielectric film may be additionally provided in contact with the side of the metal reflection layer opposite to the magneto-optical recording layer side. Especially when the metal reflective layer of the present invention is as thin as 400 Å or less to suppress heat conduction, T
Providing an i-layer metal film prevents a decrease in reflectance and improves corrosion resistance, and more preferable results are obtained. Similarly, the dielectric film may be provided as a protective layer when the magneto-optical recording medium is expected to be used in an extremely harsh environment.

前記金属反射層の形成方法としては、公知の真空蒸着
法、スパッタリング法、イオンビームスパッタリング
法、CVD法などが考えられるが、下地層との接着性、合
金組成の制御性、組成分布などの点でスパッタリング法
が好ましい。また膜の堆積速度、スパッタガス圧など
は、生産性、膜応力を考慮し、適宜選択される。
The method for forming the metal reflective layer may be a known vacuum vapor deposition method, sputtering method, ion beam sputtering method, CVD method, or the like, but the adhesiveness with the underlying layer, the controllability of the alloy composition, the composition distribution, etc. Therefore, the sputtering method is preferable. The deposition rate of the film, the sputtering gas pressure, etc. are appropriately selected in consideration of productivity and film stress.

本発明の光磁気記録層としては、光熱磁気効果により
記録できるものであればよく、公知の、膜面に垂直な方
向に磁化容易方向を有し、磁気光学効果の大きい磁性金
属薄膜、例えば前述のFeTb合金、FeTbCo合金、FeTbGd合
金及びNdDvFeCo合金、等の希土類元素−遷移金属元素の
非晶質合金が代表例として挙げられる。光磁気記録層の
膜厚は150〜1000Å、好ましくは200〜500Åである。
The magneto-optical recording layer of the present invention may be any as long as it can record by the photo-thermomagnetic effect, and it is well known that a magnetic metal thin film having a direction of easy magnetization in a direction perpendicular to the film surface and having a large magneto-optical effect, for example, A typical example is an amorphous alloy of a rare earth element-transition metal element such as FeTb alloy, FeTbCo alloy, FeTbGd alloy and NdDvFeCo alloy. The film thickness of the magneto-optical recording layer is 150 to 1000Å, preferably 200 to 500Å.

本発明における光磁気記録媒体は、その金属反射層が
光磁気記録層の光入射面と反対側に形成される点を除い
てその構成は特に限定されない。なお、金属反射層は光
磁気記録層上に直接設けても、またその上に感度、C/N
向上の目的で透明誘電体層を介して設けてもよい。しか
し本発明の前述のTa又はTiの少なくとも一方とCuを含有
するAg合金からなる金属反射膜は光磁気記録層に接して
直接設けた構成で、その記録感度とC/Nにおいて実用上
充分な性能を示し、上記透明誘電体層が不要となるの
で、この構成が生産性と媒体コストの観点より好まし
い。
The structure of the magneto-optical recording medium of the present invention is not particularly limited except that the metal reflection layer is formed on the side opposite to the light incident surface of the magneto-optical recording layer. Even if the metal reflection layer is provided directly on the magneto-optical recording layer, the sensitivity, C / N
It may be provided via a transparent dielectric layer for the purpose of improvement. However, the metal reflective film made of an Ag alloy containing at least one of Ta or Ti and Cu of the present invention is directly provided in contact with the magneto-optical recording layer, and is practically sufficient in its recording sensitivity and C / N. This structure is preferable from the viewpoints of productivity and medium cost because it exhibits performance and the transparent dielectric layer is not necessary.

なお、光磁気記録層と金属反射層との間に、透明誘電
体層を設ける場合においても、この透明誘電体層は最適
性能を得るためには600Å以下と薄くする必要があり、
その断熱作用が小さくなるため、本発明は効果的であ
る。また、一般的に、該透明誘電体層が厚くなる程、そ
の断熱効果が高くなり、本発明の金属反射膜のTa又はTi
の含有量は少なくてよい。
Even when a transparent dielectric layer is provided between the magneto-optical recording layer and the metal reflective layer, this transparent dielectric layer needs to be as thin as 600Å or less to obtain optimum performance.
The present invention is effective because its heat insulating effect is reduced. In general, the thicker the transparent dielectric layer is, the higher its heat insulating effect is, and Ta or Ti of the metal reflective film of the present invention is increased.
The content of may be small.

本発明の光磁気記録媒体は、また、基板と光磁気記録
層の間に、C/N向上、媒体の反射率低減、さらには透湿
防止の目的で透明誘電体層を設けてもよい。
In the magneto-optical recording medium of the present invention, a transparent dielectric layer may be provided between the substrate and the magneto-optical recording layer for the purpose of improving C / N, reducing the reflectance of the medium, and preventing moisture permeation.

上記構成に用いる光磁気記録層の基板側、金属反射層
側の両透明誘電体層としては、その目的により光干渉効
果、カー効果エンハンスメント等の効果を奏することが
必要で、ある程度以上の高屈折率を有することが好まし
い。また使用するレーザー光に透明であることが必要で
あり、透明誘電体層としては公知の通り金属の酸化物、
窒化物、硫化物、炭化物、弗化物もしくはこれらの複合
体が適用できる。具体的には酸化ケイ素、酸化インジウ
ム、酸化タンタル、酸化アルミニウム、チッ化ケイ素、
チッ化アルミニウム、チッ化チタン、硫化亜鉛、フッ化
マグネシウム、フッ化アルミニウム、炭化ケイ素及びこ
れらの複合物が挙げられるが、これに限定されないこと
は言うまでもない。またパリレン、ポリイミド、パラフ
ィンなど有機物も適用でき、これら透明誘電体層の膜厚
は、媒体構成、屈折率により最適値が変化し、一義的に
決めることはできないが、通常400〜1500Å程度、特に5
00〜1000Åが好適に用いられる。これら透明電体層は常
法により形成される。例えば前述の無機物よりなるもの
は公知の真空蒸着法、スパッタリング法、イオンビーム
スパッタリング法、CVD法等で作製される。
Both the transparent dielectric layer on the substrate side of the magneto-optical recording layer and the metal reflection layer side used in the above-mentioned structure, it is necessary to exhibit the effects of optical interference effect, Kerr effect enhancement, etc. depending on the purpose, and high refraction of a certain level or more. It is preferable to have a rate. In addition, it is necessary that the laser light used is transparent, and as a transparent dielectric layer, a metal oxide, as is known,
Nitrides, sulfides, carbides, fluorides or composites thereof can be applied. Specifically, silicon oxide, indium oxide, tantalum oxide, aluminum oxide, silicon nitride,
Needless to say, examples thereof include, but are not limited to, aluminum nitride, titanium nitride, zinc sulfide, magnesium fluoride, aluminum fluoride, silicon carbide, and composites thereof. Further, organic materials such as parylene, polyimide, and paraffin can be applied, and the film thickness of these transparent dielectric layers cannot be uniquely determined because the optimum value changes depending on the medium structure and refractive index, but it is usually about 400 to 1500 Å, especially Five
A value of 00 to 1000Å is preferably used. These transparent electric conductor layers are formed by a conventional method. For example, the above-mentioned inorganic material is produced by a known vacuum deposition method, sputtering method, ion beam sputtering method, CVD method, or the like.

また基板としては、ガラス、アクリル樹脂、ポリカー
ボネート樹脂、エポキシ樹脂、4−メチルペンテン樹脂
及びそれらの変成品などが好適に用いられるが、機械的
強度、価格、耐候性、耐熱性、透湿量の点でポリカーボ
ネート樹脂が好ましい。
Further, as the substrate, glass, acrylic resin, polycarbonate resin, epoxy resin, 4-methylpentene resin and modified products thereof are preferably used, but mechanical strength, price, weather resistance, heat resistance, moisture permeability Polycarbonate resin is preferable from the viewpoint.

以下、本発明の実施例を説明するが、本発明は以下の
実施例に限定されるものではない。
Examples of the present invention will be described below, but the present invention is not limited to the following examples.

<実施例,比較例> 直径130mm、厚さ1.2mmの円盤で1.6μmピッチのグル
ーブを有するポリカーボネート樹脂(PC)製のディスク
基板を、3ターゲット設置可能な高周波マグネトロンス
パッタ装置(アネルバ(株)製SPF−430H型)の真空槽
内に配置し、4×10-7Torrになるまで排気した。
<Examples and Comparative Examples> A high frequency magnetron sputtering device (available from Anelva Corp.) capable of installing 3 targets on a disk substrate made of polycarbonate resin (PC) having a disk of diameter 130 mm, thickness 1.2 mm and grooves of 1.6 μm pitch. It was placed in a vacuum chamber (SPF-430H type) and evacuated to 4 × 10 −7 Torr.

次にAr、N2の混合ガス(Ar:N2=70:30vol%)を真空
槽内に導入し、圧力10m TorrになるようにAr/N2混合ガ
ス流量を調整した。ターゲットとしては直径100mm、厚
さ5mmのAl50Si50(以下、添数字は組成(原子%)を示
す)の焼結体からなる円盤を用い、放電電力500W、放電
周波数13.56MHzで高周波スパッタリングを行ない、PC基
板を回転(自転)させながら、透明誘電体としてAlSiN
膜を800Å堆積した。
Next, a mixed gas of Ar and N 2 (Ar: N 2 = 70: 30 vol%) was introduced into the vacuum chamber, and the flow rate of the Ar / N 2 mixed gas was adjusted so that the pressure was 10 m Torr. As the target, a disk made of a sintered body of 100 mm in diameter and 5 mm in thickness of Al 50 Si 50 (hereinafter, the subscripts indicate the composition (atomic%)) was used, and high frequency sputtering was performed at a discharge power of 500 W and a discharge frequency of 13.56 MHz. AlSiN as a transparent dielectric while rotating (rotating) the PC substrate
A film of 800 Å was deposited.

続いて光磁気記録層として、Tb21Fe71Co8合金ターゲ
ットを用い、Arガス圧2m Torr、放電電力150Wの条件で
高周波スパッタリングを行ない、約300ÅのTbFeCo合金
膜を堆積した。
Subsequently, using a Tb 21 Fe 71 Co 8 alloy target as the magneto-optical recording layer, high frequency sputtering was performed under the conditions of Ar gas pressure of 2 m Torr and discharge power of 150 W to deposit a TbFeCo alloy film of about 300 Å.

更に引き続いて、Ag85Cu15合金ターゲットを用い、適
宜5mm角×1mm tのTaチップをターゲット上に配し、Arガ
ス圧2m Torr、放電電力100Wの条件で高周波スパッタリ
ングを行い、表−1の各組成で400Åの金属反射層を堆
積し、PC基板/AlSiN/TbFeCo/金属反射層の積層構成の光
磁気ディスクを得た。金属反射層の各AgCuTa合金膜のTa
量はAgCu合金ターゲット上のTaチップの数を変化させて
各組成に調整した。
Further subsequently, using an Ag 85 Cu 15 alloy target, a 5 mm square × 1 mm t Ta tip was appropriately arranged on the target, and high frequency sputtering was performed under the conditions of Ar gas pressure of 2 m Torr and discharge power of 100 W. A 400 Å metal reflective layer was deposited with each composition to obtain a magneto-optical disk having a laminated structure of PC substrate / AlSiN / TbFeCo / metal reflective layer. Ta of each AgCuTa alloy film of the metal reflection layer
The amount was adjusted to each composition by changing the number of Ta chips on the AgCu alloy target.

これら各層の形成時において、PC基板は20rpmで回転
させた。
During the formation of each of these layers, the PC substrate was rotated at 20 rpm.

得られた光磁気ディスクは光磁気記録再生装置(ナカ
ミチ(株)製OMS−1000型)を用い、下記条件でC/Nと最
適記録レーザーパワーを評価した。書込み時の半導体レ
ーザーパワーを変化させ、再生信号の二次高周波が最小
となる時が最適記録条件とした。
The obtained magneto-optical disk was evaluated for C / N and optimum recording laser power under the following conditions using a magneto-optical recording / reproducing apparatus (OMS-1000 type manufactured by Nakamichi Co., Ltd.). The optimum recording condition was set when the semiconductor laser power during writing was changed and the secondary high frequency of the reproduced signal was minimized.

[記録条件] ディスク回転速度:1800rpm、記録トラック位置:半径
30mm位置、記録周波数:3.7MHz、記録時の印加磁界:500
エルステッド [再生条件] ディスク回転速度:1800rpm、読出レーザーパワー:1.2
mW 最適記録レーザーパワー及びC/Nの測定結果を表−1
に示す。
[Recording conditions] Disk rotation speed: 1800 rpm, recording track position: radius
30 mm position, recording frequency: 3.7 MHz, applied magnetic field during recording: 500
Oersted [Playback conditions] Disc rotation speed: 1800 rpm, Read laser power: 1.2
Table 1 shows the measurement results of mW optimum recording laser power and C / N.
Shown in

なお、表−1の比較例1は金属反射層以外は実施例1
〜4と同じ構成で、金属反射層を実施例1〜4のTaチッ
プを除去して形成したTaを含有しないAg85Cu15合金とし
た光磁気ディスクである。
In addition, Comparative Example 1 in Table 1 is the same as Example 1 except for the metal reflection layer.
4 is a magneto-optical disk made of Ag 85 Cu 15 alloy containing no metal and having a metal reflection layer formed by removing the Ta chips of Examples 1-4.

また、比較例2として、金属反射層を除いた他の構成
は実施例1〜4と同じで、金属反射層としてTaチップを
配したAlターゲットを用い、実施例1〜4の金属反射層
と同じように高周波数スパッタリングすることにより、
Al92Ta8合金膜を400Å積層形成した光磁気ディスクを作
製し、同様に評価した。
In addition, as Comparative Example 2, the configuration other than the metal reflective layer is the same as that of Examples 1 to 4, and an Al target provided with a Ta chip is used as the metal reflective layer, and the metal reflective layer of Examples 1 to 4 is used. By high frequency sputtering in the same way,
A magneto-optical disk in which an Al 92 Ta 8 alloy film was formed in a 400 Å laminated structure was prepared and evaluated in the same manner.

また表−1の比較例1の最適記録レーザーパワー10mW
以上は、用いたレーザー最大出力10mWでも記録できなか
ったことを表わす。
Also, the optimum recording laser power of 10 mW in Comparative Example 1 in Table-1
The above shows that recording was not possible even with the maximum laser output of 10 mW used.

また実施例2と比較例2のディスクの金属反射層上
に、スピンコーターで紫外線硬化型のフェノールノボラ
ックエポキシアクリレート樹脂を塗布し、その後紫外線
照射により硬化させ、約20μmの有機保護層を設けた。
これらのサンプルを、温度80℃、湿度85%の条件で1000
時間の加速試験を行なったところ、実施例2では全く変
化が見られなかったが、比較例2ではピンホールが十数
個発生した。
Further, an ultraviolet curable phenol novolac epoxy acrylate resin was applied by a spin coater on the metal reflective layers of the disks of Example 2 and Comparative Example 2 and then cured by ultraviolet irradiation to provide an organic protective layer of about 20 μm.
These samples were tested at a temperature of 80 ° C and a humidity of 85% for 1000
When the time acceleration test was conducted, no change was observed in Example 2, but in Comparative Example 2, ten or more pinholes were generated.

更に、実施例1〜4と同じにして、ただTaのかかわり
にTiのチップをAgCuターゲット上に配置して金属反射層
を表−2のAgCuTi合金とした以外は全く同じ構成の光磁
気ディスクのサンプルを作成し、同じようにして評価し
た。その結果を表−2に示す。
Further, in the same manner as in Examples 1 to 4, a magneto-optical disk having exactly the same configuration except that a Ti chip was placed on an AgCu target instead of Ta and the metal reflection layer was the AgCuTi alloy shown in Table 2 was used. Samples were prepared and evaluated in the same way. The results are shown in Table-2.

以上、実施例に示した如く、本発明のCuと、Ta又はTi
の少なくとも一方とを含有したAg合金からなる金属反射
膜ではC/N、感度が優れ、かつ耐久性も高い光磁気記録
媒体を得ることができる。特にTa,Tiの含有量が2at%以
上の範囲では、最適記録レーザーパワーの低下すなわち
記録感度の向上が顕著で、かつC/Nも公知の、例えばAlT
a合金膜を反射膜とする光磁気ディスクより格段にすぐ
れている。かかる効果の点でTa、Tiの含有量は2〜10at
%が特に好ましい。
As described above, as shown in the examples, Cu of the present invention, Ta or Ti
With a metal reflective film made of an Ag alloy containing at least one of the above, it is possible to obtain a magneto-optical recording medium having excellent C / N, sensitivity, and high durability. In particular, when the content of Ta, Ti is 2 at% or more, the decrease of the optimum recording laser power, that is, the improvement of the recording sensitivity is remarkable, and the C / N is also known, such as AlT.
It is far superior to a magneto-optical disk that uses an alloy film as a reflective film. In terms of such effects, the content of Ta and Ti is 2 to 10 at
% Is particularly preferred.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 中谷 忠則 東京都日野市旭が丘4丁目3番2号 帝人 株式会社東京研究センター内 (72)発明者 千葉 潔 東京都日野市旭が丘4丁目3番2号 帝人 株式会社東京研究センター内 (56)参考文献 特開 昭59−8150(JP,A) ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Tadanori Nakatani 4-3-2 Asahigaoka, Hino-shi, Tokyo Inside Teijin Ltd. Tokyo Research Center (72) Inventor Kiyoshi Chiba 4-32-3 Asahigaoka, Hino-shi, Tokyo Teijin Limited Tokyo Research Center (56) References JP 59-8150 (JP, A)

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】金属反射層を有する光磁気記録媒体におい
て、該金属反射層がAgにCuを0.5〜30at%含有せしめ、
さらにTa又はTiの少くとも一種を0.5〜15at%含有せし
めたAg合金からなることを特徴とする光磁気記録媒体。
1. A magneto-optical recording medium having a metal reflective layer, wherein the metal reflective layer contains Ag in an amount of 0.5 to 30 at%.
Furthermore, a magneto-optical recording medium comprising an Ag alloy containing at least 0.5 to 15 at% of Ta or Ti.
【請求項2】前記金属反射層が光磁気記録層に接して設
けられた請求項第1項記載の光磁気記録媒体。
2. The magneto-optical recording medium according to claim 1, wherein the metal reflective layer is provided in contact with the magneto-optical recording layer.
【請求項3】前記Ta又はTiの含有量の合計が2〜10at%
である請求項第1項又は第2項記載の光磁気記録媒体。
3. The total content of Ta or Ti is 2 to 10 at%.
The magneto-optical recording medium according to claim 1 or 2.
JP16201889A 1989-06-23 1989-06-23 Magneto-optical recording medium Expired - Fee Related JPH081709B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16201889A JPH081709B2 (en) 1989-06-23 1989-06-23 Magneto-optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16201889A JPH081709B2 (en) 1989-06-23 1989-06-23 Magneto-optical recording medium

Publications (2)

Publication Number Publication Date
JPH0325737A JPH0325737A (en) 1991-02-04
JPH081709B2 true JPH081709B2 (en) 1996-01-10

Family

ID=15746494

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16201889A Expired - Fee Related JPH081709B2 (en) 1989-06-23 1989-06-23 Magneto-optical recording medium

Country Status (1)

Country Link
JP (1) JPH081709B2 (en)

Families Citing this family (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5948497A (en) * 1992-10-19 1999-09-07 Eastman Kodak Company High stability silver based alloy reflectors for use in a writable compact disk
JPH073435A (en) * 1993-04-22 1995-01-06 Mitsubishi Materials Corp Highly corrosion resistant ag-mg alloy and thin film using the same
US6852384B2 (en) 1998-06-22 2005-02-08 Han H. Nee Metal alloys for the reflective or the semi-reflective layer of an optical storage medium
US7314657B2 (en) 2000-07-21 2008-01-01 Target Technology Company, Llc Metal alloys for the reflective or the semi-reflective layer of an optical storage medium
US7045187B2 (en) 1998-06-22 2006-05-16 Nee Han H Metal alloys for the reflective or the semi-reflective layer of an optical storage medium
US6764735B2 (en) 1998-06-22 2004-07-20 Target Technology Company, Llc Metal alloys for the reflective or the semi-reflective layer of an optical storage medium
US7384677B2 (en) 1998-06-22 2008-06-10 Target Technology Company, Llc Metal alloys for the reflective or semi-reflective layer of an optical storage medium
US6790503B2 (en) 1998-06-22 2004-09-14 Target Technology Company, Llc Metal alloys for the reflective or the semi-reflective layer of an optical storage medium
US6905750B2 (en) 1998-06-22 2005-06-14 Target Technology Company, Llc Metal alloys for the reflective or the semi-reflective layer of an optical storage medium
US7374805B2 (en) 2000-07-21 2008-05-20 Target Technology Company, Llc Metal alloys for the reflective or the semi-reflective layer of an optical storage medium
US7316837B2 (en) 2000-07-21 2008-01-08 Target Technology Company, Llc Metal alloys for the reflective or the semi-reflective layer of an optical storage medium
US7314659B2 (en) 2000-07-21 2008-01-01 Target Technology Company, Llc Metal alloys for the reflective or semi-reflective layer of an optical storage medium
EP1560704B1 (en) 2003-04-18 2012-06-13 Target Technology Company, LLC. Metal alloys for the reflective or the semi-reflective layer of an optical storage medium

Also Published As

Publication number Publication date
JPH0325737A (en) 1991-02-04

Similar Documents

Publication Publication Date Title
US5093174A (en) Optical recording medium
JPH081709B2 (en) Magneto-optical recording medium
KR970001374B1 (en) Magneto optical recording medium
US5512364A (en) Magneto-optical recording medium
US5087340A (en) Method of making magneto-optical recording disk
JP2541677B2 (en) Optical recording medium
US5009762A (en) Magneto-optical recording medium having protective film with increased kerr effect and improved protection characteristic and manufacturing method of the same
JP2507592B2 (en) Optical recording medium
JP2559871B2 (en) Optical recording medium
JPH03122845A (en) Optical recording medium
JP2804165B2 (en) Magneto-optical recording medium
JP2921590B2 (en) Magneto-optical recording medium
JPH03142728A (en) Optical recording medium
JP2000067466A (en) Optical recording medium and its production
JPH02308454A (en) Magneto-optical recording medium
KR100194131B1 (en) Optical recording media
JP2834846B2 (en) Method for manufacturing magneto-optical recording medium
JP2528184B2 (en) Magneto-optical recording medium
JPH01269258A (en) Optical recording medium
JP2960470B2 (en) Magneto-optical recording medium
JP2552345B2 (en) Method for manufacturing magneto-optical recording medium
JP2775853B2 (en) Magneto-optical recording medium
JP2918600B2 (en) Magneto-optical recording medium
JP2550698B2 (en) Magneto-optical recording medium
JP2750177B2 (en) Magneto-optical recording medium

Legal Events

Date Code Title Description
LAPS Cancellation because of no payment of annual fees