JPH02216640A - Magneto-optical recording medium - Google Patents
Magneto-optical recording mediumInfo
- Publication number
- JPH02216640A JPH02216640A JP3539989A JP3539989A JPH02216640A JP H02216640 A JPH02216640 A JP H02216640A JP 3539989 A JP3539989 A JP 3539989A JP 3539989 A JP3539989 A JP 3539989A JP H02216640 A JPH02216640 A JP H02216640A
- Authority
- JP
- Japan
- Prior art keywords
- magneto
- recording
- recording medium
- 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.)
- Pending
Links
- 239000000203 mixture Substances 0.000 claims abstract description 13
- 229910052777 Praseodymium Inorganic materials 0.000 claims abstract description 5
- 229910052742 iron Inorganic materials 0.000 claims abstract description 5
- 229910052759 nickel Inorganic materials 0.000 claims abstract description 4
- 239000010408 film Substances 0.000 claims abstract 5
- 239000010409 thin film Substances 0.000 claims abstract 2
- 229910052779 Neodymium Inorganic materials 0.000 claims description 5
- 229910000808 amorphous metal alloy Inorganic materials 0.000 claims description 2
- 230000005415 magnetization Effects 0.000 claims description 2
- 230000003287 optical effect Effects 0.000 abstract description 8
- 229910052761 rare earth metal Inorganic materials 0.000 abstract description 5
- 230000000704 physical effect Effects 0.000 abstract description 2
- 239000005300 metallic glass Substances 0.000 abstract 1
- 239000000463 material Substances 0.000 description 10
- 230000000694 effects Effects 0.000 description 7
- 230000000052 comparative effect Effects 0.000 description 6
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 239000000758 substrate Substances 0.000 description 3
- 230000007423 decrease Effects 0.000 description 2
- 150000002910 rare earth metals Chemical class 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- RZVAJINKPMORJF-UHFFFAOYSA-N Acetaminophen Chemical compound CC(=O)NC1=CC=C(O)C=C1 RZVAJINKPMORJF-UHFFFAOYSA-N 0.000 description 1
- 230000005374 Kerr effect Effects 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 229940059720 apra Drugs 0.000 description 1
- 238000005452 bending Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 229920000515 polycarbonate Polymers 0.000 description 1
- 239000004417 polycarbonate Substances 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 229910052723 transition metal Inorganic materials 0.000 description 1
- 150000003624 transition metals Chemical class 0.000 description 1
Landscapes
- Thin Magnetic Films (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は、光磁気記録に用いられる光…気記録媒体に関
するもので、特に、その光磁気記録層の材料に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a magneto-optical recording medium used for magneto-optical recording, and in particular to a material for its magneto-optical recording layer.
〔従来の技術1
従来公知である光磁気記録媒体は、案内溝を有するガラ
ス、または樹脂製の円盤状基板と、その上に成膜した記
録層から成り、記録層としてはTbFe、TbFeCo
、GdFeCo等の非晶質の重希土類と遷移金属の非晶
質合金膜が用いられる。これらの膜はキュリー温度が1
00〜200℃と半導体レーザーの集束光による記録・
消去に適しており、また非晶質であることから、Mn8
1等結晶材料の欠点である粒界ノイズがなく光磁気記録
材料としては望ましい特性を備えている。[Prior art 1] A conventionally known magneto-optical recording medium consists of a disk-shaped substrate made of glass or resin having a guide groove, and a recording layer formed on the substrate.
, GdFeCo, or other amorphous heavy rare earth and transition metal amorphous alloy films are used. These films have a Curie temperature of 1
Recording at 00 to 200℃ and using focused light from a semiconductor laser.
Mn8 is suitable for erasing and is amorphous.
It has desirable characteristics as a magneto-optical recording material without grain boundary noise, which is a drawback of primary crystal materials.
しかしながら、これらの材料には次の様な欠点がある。However, these materials have the following drawbacks.
即ち、光磁気記録においては情報の再生はカー効果もし
くはファラデー効果を用いて行われるが、これらの材料
においてはこの磁気光学効果が非常に小さい、一方、磁
気光学効果は動作温度においては記Bllのキュリー温
度と正の相関が経験的に知られている。したがって、記
録膜のキュリー温度を高めることによって磁気光学効果
な大きくすることができる。ところが、キュリー温度が
高くなると記録・消去に必要なレーザーパワーが高くな
る。そこで、このような欠点を改善するために重希土−
鉄系合金に軽希土類元素のSmを添加した材料が提案さ
れている。(特開昭59−17864yこの材料によっ
て記録感度を低下せしめることなく、光再生特性を向上
させることができる。That is, in magneto-optical recording, information is reproduced using the Kerr effect or the Faraday effect, but this magneto-optic effect is very small in these materials, while the magneto-optic effect is small at operating temperatures. It is empirically known that there is a positive correlation with the Curie temperature. Therefore, by increasing the Curie temperature of the recording film, the magneto-optic effect can be increased. However, as the Curie temperature rises, the laser power required for recording and erasing increases. Therefore, in order to improve these drawbacks, heavy rare earth
A material in which Sm, a light rare earth element, is added to an iron-based alloy has been proposed. (Unexamined Japanese Patent Publication No. 59-17864) This material makes it possible to improve optical reproduction characteristics without reducing recording sensitivity.
[発明が解決しようとする課題1
しかしながら、この材料には次に示すような改善すべき
間屈点が残されている。[Problem to be Solved by the Invention 1] However, this material still has the following bending points that should be improved.
光磁気記録においては情報の記録のためにはバイアス磁
界を必要とする。このような材料を記録層に用いた場合
、最低3000e程度以上のバイアス磁界を記録ビット
周囲に印加させないと、良好な記録を行うことができな
い。また、記録・再生装置の小型化・低消費電力化を実
現するためには、低バイアス磁界での記録・消去が可能
な材料が要求されている。一方、光磁気記録における重
ね書きを実現する方法として、磁界変調記録法が提案さ
れているが、この方式においても磁場感度の高い記録媒
体が望ましい、即ち、従来の光磁気記録媒体を用いた場
合、大きな磁界を高速でスイッチングする必要からコイ
ルに高電圧を印加することになる。さらに、高磁界を高
周波で得るためにコイルを媒体面より数μm程度まで近
づけると、光磁気記録の光メモリーとしての利点の大半
を失うことになる。Magneto-optical recording requires a bias magnetic field to record information. When such a material is used for the recording layer, good recording cannot be performed unless a bias magnetic field of at least about 3000 e or more is applied around the recording bit. Furthermore, in order to realize downsizing and lower power consumption of recording and reproducing devices, materials that can record and erase data in a low bias magnetic field are required. On the other hand, a magnetic field modulation recording method has been proposed as a method for realizing overwriting in magneto-optical recording, but even in this method, it is desirable to use a recording medium with high magnetic field sensitivity. , a high voltage is applied to the coil due to the need to switch a large magnetic field at high speed. Furthermore, in order to obtain a high magnetic field at high frequency, if the coil is brought closer to the surface of the medium by several micrometers, most of the advantages of magneto-optical recording as an optical memory will be lost.
本発明はこのような従来の光6ftft縁媒体の課・題
を解決するもので、その目的とするところは、低バイア
ス磁界でも良好な記録・消去を行うことができる光磁気
記録媒体を提供するところにある。The present invention solves the problems of the conventional optical 6ftft edge medium, and its purpose is to provide a magneto-optical recording medium that can perform good recording and erasing even in a low bias magnetic field. There it is.
[課題を解決するための手段]
本発明の光I気記録媒体は、記録層が膜面と垂直な方向
に磁化容易軸を有する非晶質膜であって、組成を原子比
で。[Means for Solving the Problems] In the optical recording medium of the present invention, the recording layer is an amorphous film having an axis of easy magnetization in a direction perpendicular to the film surface, and the composition is expressed in atomic ratio.
iNd、Pr1x (SmJy+−5ly fFe、’
Go、Nil 1oo−x−yと表した時。iNd, Pr1x (SmJy+-5ly fFe,'
Go, Nil When expressed as 1oo-x-y.
0<x≦10 15≦x+y≦40 0<z≦0.3 である事を特徴とする。0<x≦10 15≦x+y≦40 It is characterized in that 0<z≦0.3.
ここで、Fe、Co、Niの比率は媒体の記録・再生条
件によって、キュリー温度及び補償温度等の物性を所望
値にするな、め、任意に設定できる。但し、この組成系
においては光磁気記録媒体として必要条件である垂直m
化膜であるためには、(x+y)即ち膜中の全希土類の
比率を15at%から40at%の範囲にする必要があ
る。Here, the ratios of Fe, Co, and Ni can be arbitrarily set depending on the recording/reproducing conditions of the medium, so as not to set physical properties such as Curie temperature and compensation temperature to desired values. However, in this composition system, the perpendicular m, which is a necessary condition for a magneto-optical recording medium,
In order to form a chemical film, it is necessary that (x+y), that is, the ratio of all rare earth elements in the film, be in the range of 15 at % to 40 at %.
[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] The present invention will be described in detail below based on Examples.
(実施例1)
INdo、 5Pro、 sea、 o fsmo、
+5Dyo、 asl 23. O(Feo、 asc
。(Example 1) INdo, 5Pro, sea, o fsmo,
+5Dyo, asl 23. O(Feo, asc
.
。181?+。なる組成の非晶質膜を記録層とする光E
fl気記録媒体を1.6μmピッチのスパイラル状の案
内溝を有する直径120mmのポリカーボネート基板を
用いて作製した。また、比較例として(Smo、 l
Jyo、 ssl a3. a (Feo、 5scO
o、 l al t?、 oの組成の記録膜を有する光
6n気記録媒体を作製した。. 181? +. Light E whose recording layer is an amorphous film with the composition
A recording medium was fabricated using a polycarbonate substrate with a diameter of 120 mm and having spiral guide grooves with a pitch of 1.6 μm. In addition, as a comparative example (Smo, l
Jyo, ssl a3. a (Feo, 5scO
o, l alt? An optical 6n recording medium having a recording film having a composition of .
第1図は、本実施例のNdPrSmDyFeCo(0)
と比較例のSmDyFeCo (x)を記録膜とした光
磁気記録媒体の再生CN比の記録バイアス磁界依存性を
示したものである。本実施例の光磁気記録媒体のCN比
が約7000eで飽和するのに対し、比較例のNd、P
rを含有しない光磁気記録媒体は飽和するのに約300
0eのバイアス磁界が必要なことがわかる。また、再生
CN比も本発明の実施例における光m気記録媒体の方が
約2dB高く再生特性も優れている。Figure 1 shows the NdPrSmDyFeCo(0) of this example.
This figure shows the dependence of the reproduction CN ratio on the recording bias magnetic field of a magneto-optical recording medium using SmDyFeCo (x) as a recording film as a comparative example. The CN ratio of the magneto-optical recording medium of this example saturates at about 7000e, whereas the Nd, P of the comparative example
A magneto-optical recording medium that does not contain r takes about 300 mL to saturate.
It can be seen that a bias magnetic field of 0e is required. Furthermore, the reproduction CN ratio of the optical recording medium according to the embodiment of the present invention is about 2 dB higher, and the reproduction characteristics are also excellent.
(実施例2)
INdo、 aPra、 41 X fsmo、 l
on!10. sol 22. OfFeo、 soc
。(Example 2) INdo, aPra, 41 X fsmo, l
On! 10. sol 22. OfFeo, soc
.
。2゜)、8゜−8なる組成において、NdPr!xを
変化させて光磁気記録媒体を作製した。. 2°), 8°-8, NdPr! Magneto-optical recording media were produced by varying x.
第2図はN d P r l xに対して、CN比の飽
和に要する記録バイアスm界の大きさをプロットしたも
のである。飽和バイアス磁界はNdPrjlxの増加に
伴い減少し、x=6 (at%)で最小となった後、°
増大する。一方、第3図に示す様に光6n気記録媒体の
再生CN比はx=8 (at%)程度まで漸増した後、
急激に低下する。この様なことを総合するとNdPr量
としては10(at%)以下であれば、NdPr添加の
効果であるところの記録消去バイアス磁界の減少を再生
信号の劣化を伴わずに実現することができる。FIG. 2 is a plot of the magnitude of the recording bias m field required for saturation of the CN ratio versus N d P r l x. The saturation bias magnetic field decreases as NdPrjlx increases, reaches a minimum at x = 6 (at%), and then increases to °
increase On the other hand, as shown in FIG. 3, after the reproduction CN ratio of the optical 6n recording medium gradually increases to about x=8 (at%),
Declines rapidly. Taking all of these things into account, if the amount of NdPr is 10 (at%) or less, the reduction in the recording/erasing bias magnetic field, which is the effect of adding NdPr, can be achieved without deteriorating the reproduced signal.
(実施例3)
lNd、Pr l−1)1. o (Srao、 +
oDyo、 sol **、 o fFeo、 aoc
。(Example 3) lNd, Pr l-1)1. o (Srao, +
oDyo, sol**, o fFeo, aoc
.
。、。)1.。なる組成において、NdとPrの量比a
を変化させて光磁気記録媒体を作製した。. ,. )1. . In the composition, the amount ratio a of Nd and Pr is
Magneto-optical recording media were fabricated by varying the
第4図はN d l aに対して、CN比の飽和に必要
な記録バイアス磁界の大きさを表したものである6飽和
バイアス磁界は全域にわたってNdのみの場合やPrの
みの場合よりも小さく、NdとPrの両方の元素を混合
することによって、各々を単独で用いるよりもより小さ
な印加磁場での記録及び消去とより大きな磁気光学効果
が得られる事がわかる。Figure 4 shows the magnitude of the recording bias magnetic field necessary for saturation of the CN ratio with respect to N d l a. 6 The saturation bias magnetic field is smaller over the entire region than in the case of only Nd or only Pr. , it can be seen that by mixing both elements, Nd and Pr, recording and erasing with a smaller applied magnetic field and a larger magneto-optic effect can be obtained than when using each element alone.
(実施例4)
本発明の実施例として、第1表に示した組成の記録膜を
有する磁性膜を作製した。(Example 4) As an example of the present invention, a magnetic film having a recording film having the composition shown in Table 1 was produced.
更に、比較のために第2表に示す組成の記録膜を有する
光磁気記録媒体を作製したに
れらの実施例並びに比較例の光磁気記録媒体のCN比の
飽和に要する記録バイアス磁界とCN比を第3表に示し
た。Furthermore, for comparison, the recording bias magnetic field and CN required for saturation of the CN ratio of the magneto-optical recording media of these examples and comparative examples in which magneto-optical recording media having recording films having the compositions shown in Table 2 were fabricated are shown. The ratios are shown in Table 3.
本発明の実施例の飽和記録バイアス磁界はいずれも比較
例試料番号6よりも小さい。また、CN比もNd及びP
rの入らない比較例試料番号6と同等もしくは、それ以
上の値が得られている。更に、全希土類の比率が15(
at%)未満もしくは40 (at%)を超えたり、S
mとDyの比率が3ニアを超えてSmが多く含有してい
る場合やNd、Pr量が10(at%)を超えたいずれ
の場合も飽和バイアス磁界の改善は認められるものの、
大幅なCN比の低下を伴うため好ましくないことがわか
る。The saturation recording bias magnetic fields of the Examples of the present invention are all smaller than that of Comparative Example Sample No. 6. In addition, the CN ratio is also
A value equal to or higher than that of Comparative Example Sample No. 6 without r is obtained. Furthermore, the ratio of total rare earths is 15 (
(at%) or more than 40 (at%), S
Although an improvement in the saturation bias magnetic field is observed in both cases where the ratio of m and Dy exceeds 3 nia and a large amount of Sm is contained, and when the amount of Nd and Pr exceeds 10 (at%),
It can be seen that this is not preferable because it is accompanied by a significant decrease in the CN ratio.
第1表
第 3 表
第2表
[発明の効果]
以上に述べた様に本発明によれば、光磁気記録媒体のC
N比の低下を伴うことなく、CN比の飽和バイアス磁界
の低減を行うことができる。従つて、低バイアス磁界で
も良好な記録及び、消去がSmDyFeCo組成の記録
膜。Table 1 3 Table 2 [Effects of the invention] As described above, according to the present invention, the C
The saturation bias magnetic field of the CN ratio can be reduced without reducing the N ratio. Therefore, the recording film of the SmDyFeCo composition can perform good recording and erasing even in a low bias magnetic field.
可能な高性能な光磁気記録媒体を供することかできる。It is possible to provide a magneto-optical recording medium with the highest possible performance.
第1図は1本発明の実施例におけるNdPr5 m D
y F e Co IIと従来例のSmDyFeC。
膜を記録膜とする光磁気記録媒体のCN比と記録バイア
ス磁界の関係を示す図。
第2図は1本発明のfNdo、 aPro、 4)8(
Smo、 +oDyo、 sol tx、 o fFe
o、 5ocoa、 sol 2+1−Xを用いた光磁
気記録媒体の(NdPr)ffiXと飽和バイアス磁界
の関係を示す図。
第3図は、同じ< (NdPrl量XとCN比の関係を
示す図。
第4図は、 (NdaPr+−als、ofsmo、+
oDyo、*ol tz。
(Feo、 ao(:Oa、 zol tx、 aなる
組成式においてN d fi aとCN比の関係を示す
図。
出願人 セイコーエプソン株式会社
代理人 弁理士 上 柳 雅 誉(化1名)1− ・N
dPrSmDyFeCo組成の記録膜。
バイアス磁界(Oe)
第1図
NdPr1.X(at%)
第2図
NdPr量、X(at%)
Nd量比、aFIG. 1 shows NdPr5 m D in an embodiment of the present invention.
y F e Co II and the conventional example SmDyFeC. FIG. 3 is a diagram showing the relationship between the CN ratio and the recording bias magnetic field of a magneto-optical recording medium using a film as a recording film. Figure 2 shows 1 fNdo of the present invention, aPro, 4) 8 (
Smo, +oDyo, sol tx, o fFe
FIG. 3 is a diagram showing the relationship between (NdPr)ffiX and the saturation bias magnetic field of a magneto-optical recording medium using o, 5ocoa, sol 2+1-X. Figure 3 shows the relationship between the same < (NdPrl amount
oDyo, *ol tz. (Feo, ao(: Oa, zol tx, diagram showing the relationship between N d fi a and the CN ratio in the composition formula a. Applicant: Seiko Epson Corporation Representative Patent Attorney: Masayoshi Kamiyanagi (1st name) 1-・N
Recording film with dPrSmDyFeCo composition. Bias magnetic field (Oe) Figure 1 NdPr1. X (at%) Figure 2 NdPr amount, X (at%) Nd amount ratio, a
Claims (1)
であって、組成を原子比で、 (Nd,Pr)_x(Sm_zD_y_1_−_z)_
y(Fe,Co,Ni)_1_0_0_−_x_−_y
と表した時、 0<x≦10 15≦x+y≦40 0<z≦0.3 である事を特徴とする光磁気記録媒体。[Claims] An amorphous alloy thin film having an axis of easy magnetization in a direction perpendicular to the film surface, the composition of which is (Nd, Pr)_x(Sm_zD_y_1_-_z)_ in atomic ratio.
y(Fe, Co, Ni)_1_0_0_-_x_-_y
A magneto-optical recording medium characterized in that, when expressed as: 0<x≦10 15≦x+y≦40 0<z≦0.3.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3539989A JPH02216640A (en) | 1989-02-15 | 1989-02-15 | Magneto-optical recording medium |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3539989A JPH02216640A (en) | 1989-02-15 | 1989-02-15 | Magneto-optical recording medium |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02216640A true JPH02216640A (en) | 1990-08-29 |
Family
ID=12440838
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3539989A Pending JPH02216640A (en) | 1989-02-15 | 1989-02-15 | Magneto-optical recording medium |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02216640A (en) |
-
1989
- 1989-02-15 JP JP3539989A patent/JPH02216640A/en active Pending
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