JPS62222609A - Photomagnetic recording medium - Google Patents

Photomagnetic recording medium

Info

Publication number
JPS62222609A
JPS62222609A JP6641586A JP6641586A JPS62222609A JP S62222609 A JPS62222609 A JP S62222609A JP 6641586 A JP6641586 A JP 6641586A JP 6641586 A JP6641586 A JP 6641586A JP S62222609 A JPS62222609 A JP S62222609A
Authority
JP
Japan
Prior art keywords
rare earth
film
recording
recording medium
magneto
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
JP6641586A
Other languages
Japanese (ja)
Inventor
Satoshi Shimokawato
下川渡 聡
Shin Funada
舩田 伸
Tatsuya Shimoda
達也 下田
Mamoru Sugimoto
守 杉本
Akira Aoyama
明 青山
Satoshi Nehashi
聡 根橋
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 JP6641586A priority Critical patent/JPS62222609A/en
Publication of JPS62222609A publication Critical patent/JPS62222609A/en
Pending legal-status Critical Current

Links

Landscapes

  • Thin Magnetic Films (AREA)

Abstract

PURPOSE:To enable fabrication of an alloy target of low oxygen concentration and to improve a recording sensitivity without damaging reproducing characteristics by composing a part of rare earth elements which compose a thin film of an amorphous rare earth - transition metal alloy as a recording film out of light rare earth element. CONSTITUTION:A part of rare earth elements for composing a thin film of an amorphous rare earth - transition metal alloy as a recording film of a photomagnetic recording medium is composed of light rare earth element. The rare earth element (LR) is composed of at least one of the elements Ce, PR, Nd, and Sm. The transition metal (TM) and the rare earth element are composed of at least one of Fe, Co, and Ni, and Gd, Tb, and Dy, respectively. When a composition formula of the recording film is (LRxHR1-x)yTM100-y, 0.01<x<=0.60, 10<=y<=50. As the recording medium, aluminum nitride AlN 2, a recording layer 3, and an AlN film 4 are grown on a polycarbonate substrate 1 provided with grooves by spattering technique.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、例えばレーザー光を照射することによって、
記録、再生、消去を行うことが可能な光磁気記録媒体に
件する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention provides, for example, by irradiating laser light,
Pertains to magneto-optical recording media that can be recorded, reproduced, and erased.

〔従来の技術〕[Conventional technology]

従来光磁気記録媒体の記録材料として提案されている材
料は、Gd 、Tb+Dyのうち少くとも一種以上の元
素と、Fe+Co+Niのうち少くとも−m以上の元素
から成る非晶質合金薄膜で、一般にはスパッタリング法
、真空蒸着法で作られる。
The material conventionally proposed as a recording material for magneto-optical recording media is an amorphous alloy thin film consisting of at least one element of Gd, Tb+Dy, and at least -m or more of Fe+Co+Ni. Manufactured using sputtering and vacuum evaporation methods.

さらに補償組成と呼ばれる、見かけ上磁化が1g1l 
11+1Jされない組成付近で用いられるのが普辿でち
る。
Furthermore, the apparent magnetization is called the compensation composition, which is 1g1l.
It is commonly used in compositions that do not exceed 11+1J.

一般に光磁気記録において、再生C/N(キャリヤ、ノ
イズ比)は、磁気光学回転角(磁気カー回転角”K r
およびファラデー回転角θF)に比例して大きくなる。
In general, in magneto-optical recording, the reproduction C/N (carrier-to-noise ratio) is determined by the magneto-optical rotation angle (magnetic Kerr rotation angle "K r
and the Faraday rotation angle θF).

又、書込み感度は、特にキーリ一点書込みの場合、キー
リ一温度に左右され、キーリ一温度が150〜200℃
の媒体が適切であるとされている。
In addition, the writing sensitivity, especially in the case of single-point writing, is affected by the temperature of the key, and the temperature of the key is 150 to 200°C.
medium is considered appropriate.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

ところがキーリ一温度と磁気光学回転角の間には、概ね
正の相関関係が、キ、 !J 一温度と書込み感度の間
には負の相関関係が成り立っている。従って、T b 
F e Co r G o l T b F e + 
T b D y F e Coのように磁気光学効果の
大きな材料は、書込みに大きなエネルギーを要し、T 
b F e r D y F eのようにキーリ一点の
低い材料は、再生信号が小さく大きなC/Nを得られな
いという欠点を有している。
However, there is a generally positive correlation between temperature and magneto-optical rotation angle. J There is a negative correlation between temperature and writing sensitivity. Therefore, T b
F e Cor G o l T b F e +
A material with a large magneto-optic effect such as T b D y F e Co requires a large amount of energy to write, and
A material with a low keying point such as bFerDyFe has the disadvantage that the reproduced signal is small and a large C/N cannot be obtained.

一方従来の光磁気記録に用いられる重希土類−心移金属
膜は、一般に保磁力の大きな補償組成近傍の組成のスパ
ッター膜が利用される。スパッタリング法で成膜するた
めには、所望の膜組成に近い組成のターゲットを用慧す
ることが不可欠である。ところが、このような合金系は
多数の金属間化合物を形成することが普通で、一般には
、鋳造法により作られた合金は、多種の化合物相の巨大
結晶粒を有する多結晶体となシ割れ易く、合金ターゲッ
トを作製するには特殊な技術を必要としている。そのた
め、スパッタリングで薄膜を作成するために複数の異る
ターゲットを同時に使用して、成膜の際に合金化する多
元同時スパッタ法や、複合ターゲツト法が用いられるこ
とが多い。しかしこれらの方法も、膜の特性の均一性、
組成制御などの点に問題を有する。さらに粉末冶金の手
法による焼結体をターゲットとして利用できるが、ター
ゲット中の酸素含有量を11000pp以下に抑えるこ
とが田無で、このことは記録膜の特性に重大な影響を与
えるため、より低酸素濃度のターゲットを使用すること
が望ましい。
On the other hand, as the heavy rare earth-centered metal film used in conventional magneto-optical recording, a sputtered film having a composition close to the compensation composition having a large coercive force is generally used. In order to form a film by sputtering, it is essential to use a target with a composition close to the desired film composition. However, such alloy systems usually form a large number of intermetallic compounds, and alloys made by casting methods generally become polycrystalline bodies with large grains of various compound phases and cracks. However, special techniques are required to produce alloy targets. Therefore, in order to create a thin film by sputtering, a multi-target simultaneous sputtering method or a composite target method is often used, in which a plurality of different targets are used simultaneously and alloyed during film formation. However, these methods also require uniformity of film properties,
There are problems with composition control, etc. Furthermore, a sintered body produced by powder metallurgy can be used as a target, but it is recommended that the oxygen content in the target be kept below 11,000 pp. This has a serious effect on the properties of the recording film, so It is desirable to use concentration targets.

そこで、本発明はこのような問題点を解決するもので、
その目的とするところは、低酸素濃度の合金ターゲット
のf’l−製を可能にし、再往特性を損うことなく記録
膜、度の優れた光磁気記録媒体を提供することにある。
Therefore, the present invention aims to solve these problems.
The purpose is to enable the production of f'l- alloy targets with low oxygen concentrations and to provide a magneto-optical recording medium with excellent recording film and strength without impairing the repeatability characteristics.

〔問題点を解決するだめの手段〕[Failure to solve the problem]

上記問題点を解決するために本発明の光磁気記録媒体は
、その記録膜である非晶質希土類−倦移金属合金薄膜を
構成する希土類元素の一部が軽希土類元素であることを
特徴とし、軽希土類元素(以下LRと記す)がCe +
PR+Nd、Smから、遷移金属(TM)がFe +C
o+Ntから、残る希土類がGd、Tb、D)’から選
ばれた一棟以上の元素よりなる。
In order to solve the above problems, the magneto-optical recording medium of the present invention is characterized in that a part of the rare earth elements constituting the amorphous rare earth-transfer metal alloy thin film which is the recording film thereof is a light rare earth element. , the light rare earth element (hereinafter referred to as LR) is Ce +
From PR+Nd, Sm, the transition metal (TM) is Fe +C
From o+Nt, the remaining rare earth is composed of one or more elements selected from Gd, Tb, and D)'.

上記記録膜の組成式を (LRXHRI−z )y TMt o o−yとした
とき、本発明ではα01くx≦α6o、1o≦y≦50
である。
When the compositional formula of the recording film is (LRXHRI-z)y TMto o-y, in the present invention, α01×x≦α6o, 1o≦y≦50
It is.

〔実施例〕〔Example〕

以下実施例に基いて本発明の詳細な説明する。 The present invention will be described in detail below based on Examples.

本発明の実施例はいずれもスパッタリング法により作成
したもので、特に断シのない限り低周波誘導加熱炉で俗
解、詩造した直径4インチ、厚さ411ILの合金ター
ゲットを記録膜作成にあたっては使用している。なお、
ターゲット中に含まれる酸素濃度はいずれのターゲット
も500ppm以下であった0スパツタリングはあらか
じめIXIG−’’l’orr以下に排気した真空槽内
に高純度アルゴンカ゛スを2×10″″3Torr導入
した後、高周波電力を投入して行った。
All of the examples of the present invention were created by the sputtering method, and unless otherwise noted, an alloy target of 4 inches in diameter and 411IL in thickness was used in a low-frequency induction heating furnace to create the recording film. are doing. In addition,
The oxygen concentration in the targets was less than 500 ppm for all targets. Sputtering was carried out after introducing a high purity argon gas of 2 x 10''3 Torr into a vacuum chamber that had been evacuated to less than IXIG-''l'orr in advance. , by applying high-frequency power.

第1表は、本実施例の薄膜の組成、および比較例の組成
を示す0なお比較例の試料は、Feターゲット上に希土
類、およびCOのチップを配置した複合ターゲットを用
いて作成した。
Table 1 shows the composition of the thin film of this example and the composition of the comparative example.The sample of the comparative example was prepared using a composite target in which rare earth and CO chips were arranged on an Fe target.

第   1   表 第2表は、上に記した実施例および比較例試料の磁気光
学効果の消失する温度(キーリ一点)およびM11%に
おけるカー回転角を示したものである。
Table 1 and Table 2 show the temperature at which the magneto-optic effect disappears (Kiely point) and the Kerr rotation angle at M11% for the examples and comparative samples described above.

第2表 試料名   キーリ一点(℃)   第−四軌角(度)
実施例1    250        [138//
2       300            α 
42//3       210          
  (L 55//4       220     
       α34tt5      210   
         α65〃  6      270
           0.39比較例1     2
40         [L37//2      2
80            Q、41これらの記録1
t!i!を用いて第1図に示す構成でディスクを作成し
た。すなわち溝付ポリカーボネイト基板1の上に窒化ア
ルミニウム(AIN)2を膜4を10(IOA各々スパ
ッタリング法で成膜した。このデノスクを光源にGaA
lAs半導体レーザー(g、長780nm)を用いたフ
ァラデー法による記録再生装置を用いて、記録再生特性
を比較した。記録再生条件は、媒体回転数90Orpm
記録周波数1M Hz +バイアス磁場5000 e 
を舟生レーザパワー1mWでC/Nはバンド幅KHzの
値でおる。
Table 2 Sample name Single point (°C) -4th orbital angle (degrees)
Example 1 250 [138//
2 300 α
42//3 210
(L 55//4 220
α34tt5 210
α65 6 270
0.39 Comparative example 1 2
40 [L37//2 2
80 Q, 41 These records 1
T! i! A disk was created using the configuration shown in Figure 1. That is, on a grooved polycarbonate substrate 1, a film 4 of aluminum nitride (AIN) 2 (IOA) was formed by sputtering.
The recording and reproducing characteristics were compared using a recording and reproducing apparatus based on the Faraday method using an lAs semiconductor laser (g, length 780 nm). The recording/reproducing conditions are a medium rotation speed of 90 Orpm.
Recording frequency 1MHz + bias magnetic field 5000e
When the Funao laser power is 1 mW, the C/N is the value of the bandwidth KHz.

第2図および第5図は、実施例1および比較例1の書込
みパワーに対する再生C/N(dB)と二次高調波抑圧
比(dB)の関係を示したものである。
2 and 5 show the relationship between reproduction C/N (dB) and second harmonic suppression ratio (dB) with respect to write power in Example 1 and Comparative Example 1.

二次高調波抑圧比が最小になる書込みパワーを最適書込
みパワーpw (mw )と表わせば、実施例1はP 
w = 5.5 m w + C/ N −52d B
 +比較例1はp vi −7,5m W+ C/ N
 −51d Bとなり、本発明の実施例1は記録感文が
良いにもかかわらず、再生C/Nも高い値が得られた。
If the write power at which the second-order harmonic suppression ratio is minimized is expressed as the optimal write power pw (mw), then in the first embodiment, P
w = 5.5 m w + C/N -52d B
+Comparative example 1 is p vi -7.5m W+ C/N
-51 dB, and although Example 1 of the present invention had good recording sensitivity, a high reproduction C/N value was obtained.

また、PW近傍でのC/Hの立上りが本実施例の方が急
峻なことは、再生時の誤書込み防止の観点からも望まし
い。
Further, it is desirable that the rise of C/H near PW is steeper in this embodiment from the viewpoint of preventing erroneous writing during reproduction.

@3表は、本実施例および比較例の最適書込みパワーと
再生C/Nを示したものである。
Table @3 shows the optimum write power and reproduction C/N of the present example and the comparative example.

第   3   表 先に示した例と同様、本実施例はすべて亮感度書込み可
能で、再生C/Nが高いものとなっている0 〔発明の効果〕 以上に述べたように本発明によれば、高記録感度で再生
C/Nが品いという今までにはない光磁気記録媒体を供
給することができる。なおこの効果はスパッタリング法
で作製した記録膜に限られるものではなく、従来から行
われている真空蒸着法やイオングレーティング法などに
も適用できもまた、カー効果を利用して再生する方式に
おいても同様の効果が得られることはもちろんである。
Table 3 Similar to the example shown earlier, all of the present examples are capable of high-sensitivity writing and have a high reproduction C/N ratio.0 [Effects of the Invention] As described above, according to the present invention, , it is possible to supply an unprecedented magneto-optical recording medium with high recording sensitivity and high quality reproduction C/N. This effect is not limited to recording films made by sputtering, but can also be applied to conventional vacuum evaporation methods and ion grating methods, as well as to reproduction methods that utilize the Kerr effect. Of course, similar effects can be obtained.

さらに基板、保護膜は実施例に示したものに限定されず
、例えば基板にアクリル系プラスチックやガラスを使用
し、保護膜としてSi3N4やAINと5iaN4の混
合物等の誘電体膜を用いてもよい。
Further, the substrate and the protective film are not limited to those shown in the embodiments. For example, the substrate may be made of acrylic plastic or glass, and the protective film may be a dielectric film such as Si3N4 or a mixture of AIN and 5iaN4.

さらに、スパッタリング法で記録膜を成膜する場合、低
酸素含有量の合金ターゲットを溶解、鋳造という簡単な
プロセスで作製できることから、品質、コスト共に優れ
た光磁気記録媒体を供給できる。
Furthermore, when a recording film is formed by sputtering, an alloy target with a low oxygen content can be produced by a simple process of melting and casting, so a magneto-optical recording medium with excellent quality and cost can be provided.

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

第1図は本発明の光磁気記録媒体の構成例を示す図、第
2図および第3図は各々、本発明の光磁気記録媒体およ
び従来の光tIkk気記録媒体の、記録パワーに対する
再生C/Nと二次高調波抑圧比との関係を示す図である
。 1・・・・・・面付透明基板 2・・・・・・透明誘電体層 3・・・・・・記録層 4・・・・・・透明誘電体層 以上 出願人 セイコーエプソン株式会社 乙ノア 蓼7図 レーリ゛−ノぐワー (売W〕 箪 21躬 0   2   μ   6    17   70レ
ープ゛−1ぐワー(m岬 4色  う  19
FIG. 1 is a diagram showing an example of the structure of a magneto-optical recording medium of the present invention, and FIGS. 2 and 3 show reproduction C with respect to recording power of a magneto-optical recording medium of the present invention and a conventional optical recording medium, respectively. FIG. 3 is a diagram showing the relationship between /N and second harmonic suppression ratio. 1... Surface-mounted transparent substrate 2... Transparent dielectric layer 3... Recording layer 4... Transparent dielectric layer and above Applicant Seiko Epson Corporation B Noah's 7-figure Ray No. 1 (Sold W) 21 0 2 μ 6 17 70 Ray No. 1 (M cape 4 colors U 19

Claims (3)

【特許請求の範囲】[Claims] (1)非晶質希土類−遷移金属合金薄膜を記録膜として
有する光磁気記録媒体において、希土類元素の一部が軽
希類元素であることを特徴とする光磁気記録媒体。
(1) A magneto-optical recording medium having an amorphous rare earth-transition metal alloy thin film as a recording film, wherein a part of the rare earth element is a light rare element.
(2)前記、軽希土類元素(LR)がCe、Pr、Nd
、Smから選ばれた一種以上の元素から構成され、遷移
金属(TM)がFe、Co、Niから選ばれた一種以上
の元素から構成されていることを特徴とする特許請求の
範囲第一項記載の光磁気記録媒体。
(2) The light rare earth elements (LR) are Ce, Pr, and Nd.
, Sm, and the transition metal (TM) is composed of one or more elements selected from Fe, Co, and Ni. The magneto-optical recording medium described above.
(3)前記記録膜の組成が原子比で {LR_xHR_1_−_x}_yTM_1_0_0_
−_y〔0.01<x≦0.6010≦y≦50〕 (但しHRはGd、Tb、Dyから選ばれた一種以上の
元素)と表されることを特徴とする特許請求の範囲第一
項記載の光磁気記録媒体。
(3) The composition of the recording film is {LR_xHR_1_-_x}_yTM_1_0_0_ in atomic ratio
-_y[0.01<x≦0.6010≦y≦50] (wherein, HR is one or more elements selected from Gd, Tb, and Dy) Claim 1 Magneto-optical recording medium as described in .
JP6641586A 1986-03-25 1986-03-25 Photomagnetic recording medium Pending JPS62222609A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6641586A JPS62222609A (en) 1986-03-25 1986-03-25 Photomagnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6641586A JPS62222609A (en) 1986-03-25 1986-03-25 Photomagnetic recording medium

Publications (1)

Publication Number Publication Date
JPS62222609A true JPS62222609A (en) 1987-09-30

Family

ID=13315138

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6641586A Pending JPS62222609A (en) 1986-03-25 1986-03-25 Photomagnetic recording medium

Country Status (1)

Country Link
JP (1) JPS62222609A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63164049A (en) * 1986-08-22 1988-07-07 Mitsui Petrochem Ind Ltd Magneto-optical recording medium and its production
JPS63173249A (en) * 1987-01-13 1988-07-16 Daicel Chem Ind Ltd Magneto-optical recording medium
JPH03113852A (en) * 1989-09-28 1991-05-15 Sanyo Electric Co Ltd Magneto-optical recording medium
US5565830A (en) * 1989-09-08 1996-10-15 Kabushiki Kaisha Toshiba Rare earth-cobalt supermagnetostrictive alloy

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63164049A (en) * 1986-08-22 1988-07-07 Mitsui Petrochem Ind Ltd Magneto-optical recording medium and its production
JPS63173249A (en) * 1987-01-13 1988-07-16 Daicel Chem Ind Ltd Magneto-optical recording medium
US5565830A (en) * 1989-09-08 1996-10-15 Kabushiki Kaisha Toshiba Rare earth-cobalt supermagnetostrictive alloy
JPH03113852A (en) * 1989-09-28 1991-05-15 Sanyo Electric Co Ltd Magneto-optical recording medium

Similar Documents

Publication Publication Date Title
JPH09320134A (en) Magneto-optical recording medium
US4995024A (en) Magneto-optical recording element
JPS62222609A (en) Photomagnetic recording medium
JPS609855A (en) Magnetic alloy
JPH0227545A (en) Magneto-optical recording layer and film formation thereof
JPS63316340A (en) Magneto-optical recording medium
JPH0619859B2 (en) Magneto-optical recording medium
JPS6243847A (en) Photomagnetic recording medium
JPS6376134A (en) Magneto-optical recording medium
KR940007286B1 (en) Optical-magnetic medium
JP2582059B2 (en) Magneto-optical recording medium
JPS63100636A (en) Magneto-optical recording medium
JPS6348636A (en) Magneto-optical recording medium
JPS63308750A (en) Magneto-optical recording medium
JP3079651B2 (en) Method for manufacturing magneto-optical recording medium
JPS61115317A (en) Manufacture of thin film material for magnetooptics recording and reproducing
JPS63316341A (en) Magneto-optical recording medium
JPS59162250A (en) Magnetic alloy
JPS6299937A (en) Photomagnetic recording medium
JPS60125933A (en) Production of magnetic medium
JPS59113162A (en) Magnetic alloy
JPS6148151A (en) Optical recording medium
JPS63316342A (en) Magneto-optical recording medium
JPS63155446A (en) Magneto-optical recording medium
JPS61153856A (en) Information recording medium