JP2902872B2 - Magneto-optical recording medium - Google Patents
Magneto-optical recording mediumInfo
- Publication number
- JP2902872B2 JP2902872B2 JP25401792A JP25401792A JP2902872B2 JP 2902872 B2 JP2902872 B2 JP 2902872B2 JP 25401792 A JP25401792 A JP 25401792A JP 25401792 A JP25401792 A JP 25401792A JP 2902872 B2 JP2902872 B2 JP 2902872B2
- Authority
- JP
- Japan
- Prior art keywords
- magneto
- optical recording
- recording medium
- underlayer
- alternately laminated
- 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
Links
- 238000002441 X-ray diffraction Methods 0.000 claims description 17
- 239000000758 substrate Substances 0.000 claims description 16
- 229910000510 noble metal Inorganic materials 0.000 claims description 12
- 150000001875 compounds Chemical class 0.000 claims description 8
- 239000013078 crystal Substances 0.000 claims description 7
- 238000000034 method Methods 0.000 claims description 6
- 229910052723 transition metal Inorganic materials 0.000 claims description 6
- 150000003624 transition metals Chemical class 0.000 claims description 6
- 229910018072 Al 2 O 3 Inorganic materials 0.000 claims description 2
- 239000010408 film Substances 0.000 description 32
- 238000010586 diagram Methods 0.000 description 5
- 230000000694 effects Effects 0.000 description 5
- 230000005415 magnetization Effects 0.000 description 4
- 229910052697 platinum Inorganic materials 0.000 description 4
- 238000004544 sputter deposition Methods 0.000 description 4
- 230000005374 Kerr effect Effects 0.000 description 2
- 239000000969 carrier Substances 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 230000005291 magnetic effect Effects 0.000 description 2
- 238000001451 molecular beam epitaxy Methods 0.000 description 2
- 229910002546 FeCo Inorganic materials 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 238000009499 grossing Methods 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 238000010030 laminating Methods 0.000 description 1
- 238000003475 lamination Methods 0.000 description 1
- 229910052763 palladium Inorganic materials 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 238000000638 solvent extraction Methods 0.000 description 1
- 238000005477 sputtering target Methods 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- 238000001771 vacuum deposition Methods 0.000 description 1
Description
【0001】[0001]
【産業上の利用分野】本発明は、貴金属と遷移金属との
交互積層膜を基板上に成膜して成る書換え可能な光磁気
ディスク(光磁気記録媒体)に関し、詳しくは、信号再
生時に於けるC/Nの改良に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a rewritable magneto-optical disk (magneto-optical recording medium) formed by alternately laminating a noble metal and a transition metal on a substrate. C / N improvement.
【0002】[0002]
【従来の技術】図2のように、繰り返して記録・再生の
可能な光磁気ディスク(光磁気記録媒体)用の記録層
(垂直磁化膜)として、PtとCoとを、各々数Åづつ
交互に積層して成る交互積層膜1が提案されている。こ
の交互積層膜1は、総膜厚が数100Å以下の超薄膜領
域で垂直磁化膜になり、積層周期或いは膜厚等の条件を
変えることにより、保磁力やカ−回転角の特性を変える
ことができる。また、上記交互積層膜1と基板3との間
に、保磁力やカ−効果を改善する目的で、アモルファス
SiN等の誘電体膜20を下地層として成膜したものも
あり、さらに、その表面に、平滑化のために、エッチン
グ処理21を施したものもある(第14回日本応用磁気
学会講演概要集P65)。2. Description of the Related Art As shown in FIG. 2, as a recording layer (perpendicular magnetization film) for a magneto-optical disk (magneto-optical recording medium) which can be repeatedly recorded / reproduced, Pt and Co are alternately formed by several Å each. Have been proposed. This alternately laminated film 1 becomes a perpendicular magnetization film in an ultra-thin film region having a total film thickness of several hundreds degrees or less. By changing conditions such as a lamination period or a film thickness, it is possible to change characteristics of a coercive force and a car rotation angle. Can be. In some cases, a dielectric film 20 of amorphous SiN or the like is formed as a base layer between the alternately laminated film 1 and the substrate 3 for the purpose of improving the coercive force and the Kerr effect. In addition, there is a case where an etching process 21 is applied for smoothing (the 14th Annual Meeting of the Japan Society of Applied Magnetics P65).
【0003】かかる光磁気記録媒体の情報は、磁気光学
カ−効果を利用して再生される。即ち、直線偏光が磁化
を有する媒体の表面で反射されるときに、磁化が上向き
であるか下向きであるかによって、偏光面がθK 又は−
θK 回転される現象を利用して、これを検光子で検出す
ることにより、再生される。[0003] Information on such a magneto-optical recording medium is reproduced using the magneto-optical Carr effect. That is, when the linearly polarized light is reflected by the surface of the medium having the magnetization, the polarization plane is θ K or − depending on whether the magnetization is upward or downward.
Using the phenomenon of rotation by θ K , this is detected by an analyzer and reproduced.
【0004】[0004]
【発明が解決しようとする課題】磁気光学カ−効果での
回転角θK ,−θK の値は極めて小さく、略0.3°〜
1°程度である。このため、反射光に、ゆらぎ、或い
は、バラツキがあると、誤検出が生じて信号のノイズと
なり、再生信号のC/Nが低下する。The values of the rotation angles θ K and −θ K in the magneto-optical Kerr effect are extremely small, approximately 0.3 ° to
It is about 1 °. For this reason, if the reflected light fluctuates or fluctuates, erroneous detection will occur and signal noise will occur, and the C / N of the reproduced signal will decrease.
【0005】しかるに、図2の光磁気記録媒体では、ア
モルファス状態のSiN層20の上にPt/Coの交互
積層膜1が形成されているため、SiN層20の上のP
t層も、当初は〔111〕方向に綺麗に積層されない。
その結果、上記交互積層膜1の成長方向も図4のように
乱れて、反射光に、ゆらぎ、或いは、バラツキが発生す
る。即ち、再生信号のC/Nが低下する。本発明は上記
の事情に鑑みたものであり、情報再生時の反射光のゆら
ぎ,バラツキを低減して、再生信号のC/Nを改良する
ことを目的とする。However, in the magneto-optical recording medium of FIG. 2, since the Pt / Co alternating laminated film 1 is formed on the amorphous SiN layer 20, the Pt / Co
At the beginning, the t-layer is also not clearly stacked in the [111] direction.
As a result, the growth direction of the alternately laminated film 1 is also disturbed as shown in FIG. 4, and the reflected light fluctuates or fluctuates. That is, the C / N of the reproduced signal decreases. The present invention has been made in view of the above circumstances, and has as its object to reduce fluctuations and variations in reflected light during information reproduction and improve the C / N of a reproduced signal.
【0006】[0006]
【課題を解決するための手段】本発明は、貴金属を有す
る層と遷移金属を有する層が交互に積層されて成る交互
積層膜を基板上に成膜して成る光磁気記録媒体に於い
て、前記交互積層膜の貴金属のX線回折のロッキングカ
−ブの半値幅を18deg以下とした光磁気記録媒体で
ある。According to the present invention, there is provided a magneto-optical recording medium comprising an alternately laminated film in which layers having a noble metal and layers having a transition metal are alternately laminated on a substrate. A magneto-optical recording medium wherein the half-width of a locking curve of X-ray diffraction of the noble metal of the alternately laminated film is 18 deg or less.
【0007】また、本発明は、貴金属を有する層と遷移
金属を有する層が交互に積層されて成る交互積層膜を透
光性の下地層を介して基板上に成膜して成る光磁気記録
媒体に於いて、前記下地層を、X線回折を行ったとき結
晶の或る面のピ−クが現れる化合物により形成して成る
光磁気記録媒体である。前記化合物としては、下地層ロ
ッキングカ−ブの半値幅が20deg以下であるZn
O,Al2 O3 ,AlN,SiC,BeO,CoS等の
何れかを用いることができる。Further, the present invention provides a magneto-optical recording method comprising forming an alternately laminated film in which layers having a noble metal and layers having a transition metal are alternately laminated on a substrate via a light-transmitting underlayer. The medium is a magneto-optical recording medium in which the underlayer is formed of a compound which shows a peak on a certain surface of a crystal when subjected to X-ray diffraction. As the compound, Zn in which the half width of the underlayer locking curve is 20 deg or less is used.
Any of O, Al 2 O 3 , AlN, SiC, BeO, CoS and the like can be used.
【0008】[0008]
【作用】交互積層膜の貴金属の配向性を向上させて、そ
のX線回折のロッキングカ−ブの半値幅を18deg以
下にすると、情報再生時に於ける反射光のゆらぎ,バラ
ツキが低減され、再生信号のノイズが減少して、C/N
が向上する。貴金属の配向性の向上は、例えば、基板と
交互積層膜との間に、X線回折により結晶の或る面のピ
−クが現れる化合物を下地層として挟み込むことでも実
現できる。また、下地層として、上記の如き化合物を挟
み込むと、該下地層からの反射光のゆらぎ,バラツキも
低減される。この効果は、下地層のX線回折のロッキン
グカ−ブの半値幅を20deg以下としたときに顕著で
ある。When the half-width of the rocking curve for X-ray diffraction is reduced to 18 deg or less by improving the orientation of the noble metal in the alternately laminated film, fluctuations and variations in reflected light during information reproduction are reduced, and reproduction is performed. Signal noise is reduced and C / N
Is improved. The improvement in the orientation of the noble metal can also be realized, for example, by interposing, as an underlayer, a compound that shows a peak on a certain surface of the crystal by X-ray diffraction between the substrate and the alternately laminated film. Further, when the above-described compound is interposed between the underlayers, the fluctuation and variation in the reflected light from the underlayer are reduced. This effect is remarkable when the half width of the X-ray diffraction rocking curve of the underlayer is set to 20 deg or less.
【0009】[0009]
【実施例】以下、本発明の実施例を説明する。図1は、
実施例の光磁気記録媒体の断面を模式的に示す。図示の
ように、本光磁気記録媒体では、基板3の上に、ZnO
の下地層2が成膜され、その上に、Pt/Co交互積層
膜1が成膜されている。ZnOの下地層2の膜厚は、2
00〜3000Å程度である。また、Pt層の一層当た
りの膜厚は5〜20Å程度、Co層一層当たりの膜厚は
10Å以下であり、交互積層膜1の総膜厚は50〜40
0Å程度である。Embodiments of the present invention will be described below. FIG.
1 schematically illustrates a cross section of a magneto-optical recording medium according to an example. As shown in the figure, in the present magneto-optical recording medium, ZnO
The underlayer 2 is formed, and the Pt / Co alternately laminated film 1 is formed thereon. The thickness of the ZnO underlayer 2 is 2
It is about 00-3000 °. The thickness of one Pt layer is about 5 to 20 °, the thickness of one Co layer is 10 ° or less, and the total thickness of the alternate laminated film 1 is 50 to 40 °.
It is about 0 °.
【0010】上記の光磁気記録媒体は、図3に示すスパ
ッタリング装置を用いて、基板3の表面にZnOの下地
層2を成膜した後、該下地層2の表面に、PtとCoを
交互に成膜することで作成される。In the above magneto-optical recording medium, a ZnO underlayer 2 is formed on the surface of a substrate 3 using a sputtering apparatus shown in FIG. 3, and then Pt and Co are alternately formed on the surface of the underlayer 2. It is created by forming a film on the substrate.
【0011】図3の装置は、真空槽4と、真空槽4内の
上方に回転可能に配設された基板ホルダ7と、真空槽4
内を区分する遮蔽板5とを備えており、電源8から供給
されるRF又はDCの電力により、スパッタリングを行
う。基板ホルダ7の回転速度は制御可能である。また、
基板3は、基板ホルダ7の下面側に、回転の軸心から偏
心するようにして保持される。The apparatus shown in FIG. 3 includes a vacuum chamber 4, a substrate holder 7 rotatably disposed above the vacuum chamber 4, and a vacuum chamber 4.
And a shielding plate 5 for partitioning the inside, and sputtering is performed by RF or DC power supplied from a power supply 8. The rotation speed of the substrate holder 7 can be controlled. Also,
The substrate 3 is held on the lower surface side of the substrate holder 7 so as to be eccentric from the axis of rotation.
【0012】スパッタリングのタ−ゲット6は、遮蔽板
5で区分される真空槽4内の各空間下方の各保持板に各
々保持される。タ−ゲットとしては、下地層2の成膜時
にはZn又はZnOが用いられ、Pt/Co交互積層膜
の成膜時にはPtとCoとが用いられる。また、スパッ
タリングのガスとしては、Ar+O2 又はArが用いら
れ、これは、ボンベ9から弁及び配管等を介して供給さ
れる。The sputtering target 6 is held on each holding plate below each space in the vacuum chamber 4 divided by the shielding plate 5. As a target, Zn or ZnO is used when the underlayer 2 is formed, and Pt and Co are used when the Pt / Co alternately stacked film is formed. Ar + O 2 or Ar is used as a sputtering gas, which is supplied from a cylinder 9 via a valve, a pipe, or the like.
【0013】ZnOの下地層2は、X線回折で(000
2)面のピ−クが現れるように、結晶性良く成膜され
る。このZnOは六方晶であり、その(0001)面
は、Ptの(111)面と同じ並び方をしている。即
ち、Pt結晶は、図5に示すように面心立方格子であ
り、〔111〕方向から見ると、図6に示すように最密
な積み重ねの構造を成す。このため、下地層2が上記の
如く成膜されると、Pt層の結晶性・配向性も向上し
て、反射光のゆらぎ・バラツキが低減され、その結果、
情報再生時のノイズが減少して、C/Nが向上する。The underlayer 2 made of ZnO is (000
2) The film is formed with good crystallinity so that peaks on the surface appear. This ZnO is hexagonal, and its (0001) plane is arranged in the same manner as the (111) plane of Pt. That is, the Pt crystal is a face-centered cubic lattice as shown in FIG. 5, and has a close-packed structure as shown in FIG. 6 when viewed from the [111] direction. For this reason, when the underlayer 2 is formed as described above, the crystallinity and orientation of the Pt layer are also improved, and fluctuations and variations in reflected light are reduced.
Noise during information reproduction is reduced, and C / N is improved.
【0014】かかる下地層2の成膜条件は、例えば、タ
−ゲットへの投入電力300W,Arガス圧力7mTorr
である。また、交互積層膜1の成膜条件は、例えば、タ
−ゲットへの投入電力100W以下である。なお、成膜
条件は、上記投入電力・ガス圧力の他、基板の加熱温度
によっても調整可能である。The conditions for forming the underlayer 2 include, for example, a power input to the target of 300 W and an Ar gas pressure of 7 mTorr.
It is. The conditions for forming the alternately laminated film 1 are, for example, 100 W or less of electric power applied to the target. The film formation conditions can be adjusted by the heating temperature of the substrate in addition to the input power and gas pressure.
【0015】このようにして作成した下地層と、図2に
示す従来の光磁気記録媒体の下地層とについて、X線回
折像を測定した。その結果を、図7(本実施例)、図8
(従来例)に示す。図示のように、実施例の光磁気記録
媒体では、ZnOの(0002)面のピ−クが現れてい
る。また、ZnOのロッキングカ−ブの半値幅は11de
g であり、良好な配向性を示した。An X-ray diffraction image of the underlayer formed in this manner and the underlayer of the conventional magneto-optical recording medium shown in FIG. 2 were measured. The results are shown in FIG. 7 (this embodiment) and FIG.
(Conventional example). As shown in the figure, in the magneto-optical recording medium of the embodiment, a peak of the (0002) plane of ZnO appears. The half width of the ZnO rocking curve is 11 de.
g, indicating good orientation.
【0016】また、上記2つの光磁気記録媒体の交互積
層膜1のPtについて、X線回折のロッキングカ−ブを
各々測定した。その結果を、図9(本実施例)、図10
(従来例)に示す。図示のように、実施例の光磁気記録
媒体では、ロッキングカ−ブの半値幅は15deg であ
り、配向性が良好であるが、従来例の光磁気記録媒体で
は、19.5deg である。The rocking curves of X-ray diffraction were measured for Pt of the alternately laminated film 1 of the two magneto-optical recording media. The results are shown in FIG. 9 (this embodiment), FIG.
(Conventional example). As shown in the drawing, in the magneto-optical recording medium of the embodiment, the half width of the locking curve is 15 deg and the orientation is good, but in the magneto-optical recording medium of the conventional example, it is 19.5 deg.
【0017】また、上記2つの光磁気記録媒体につい
て、C/Nを測定した結果を、図11に示す。図示のよ
うに、キャリアは同程度であるが、図中正方形でプロッ
トされている実施例の光磁気記録媒体では、ノイズレベ
ルが小さい。このため、良好なC/Nを得られている。
なお、上記の如く良好なC/Nは、交互積層膜1のPt
のX線回折のロッキングカ−ブの半値幅を18deg 以下
としたときに得られ、また、ZnOのX線回折のロッキ
ングカ−ブの半値幅を20deg 以下としたときにも得ら
れた。FIG. 11 shows the result of measuring the C / N for the two magneto-optical recording media. As shown in the figure, the carriers are almost the same, but the noise level is small in the magneto-optical recording medium of the embodiment plotted by squares in the figure. Therefore, good C / N is obtained.
Incidentally, as described above, the good C / N is obtained by the Pt of the alternately laminated film 1.
It was also obtained when the half-width of the rocking curve for X-ray diffraction was 18 deg or less, and when the half-width of the rocking curve for X-ray diffraction of ZnO was 20 deg or less.
【0018】上記実施例では、スパッタリング法で光磁
気記録媒体を作成しているが、他の方法、例えば、真空
蒸着法、或いは、MBE(分子線エピタキシ−)法を用
いることによっても、本発明の光磁気記録媒体を得られ
る。また、上記実施例では、貴金属/遷移金属の交互積
層膜としてPt/Coを用いた場合について述べている
が、例えば、Pd/Co,PtPd/Co,Pt/Fe
Co,Pd/FeCo,Pt/Fe,等を用いた場合に
も、上記と同様の効果を得る。また、上記実施例に於い
て、交互積層膜1が基板3と接しない側の面に公知の誘
電体膜, 紫外線硬化樹脂膜, 反射膜を設けた場合も、同
様の効果を得る。In the above embodiment, the magneto-optical recording medium is prepared by a sputtering method. However, the present invention can be also applied by using another method, for example, a vacuum deposition method or an MBE (Molecular Beam Epitaxy) method. Is obtained. Further, in the above embodiment, the case where Pt / Co is used as the alternately laminated film of the noble metal / transition metal is described, but for example, Pd / Co, PtPd / Co, Pt / Fe
Even when Co, Pd / FeCo, Pt / Fe, or the like is used, the same effect as described above is obtained. Further, in the above-described embodiment, the same effect can be obtained also when a known dielectric film, ultraviolet curing resin film, or reflection film is provided on the surface of the alternate laminated film 1 on the side not in contact with the substrate 3.
【0019】[0019]
【発明の効果】以上、交互積層膜の貴金属の配向性を向
上させて、X線回折のロッキングカ−ブの半値幅を18
deg以下にした本発明では、情報再生時に於ける反射
光のゆらぎ,バラツキが低減され、再生信号のC/Nが
向上する。また、X線回折により結晶の或る面のピ−ク
が現れる化合物を下地層として用いた本発明では、該下
地層からの反射光のゆらぎ,バラツキが低減されるとと
もに、交互積層膜の貴金属の配向性も向上されるため、
反射光のゆらぎ,バラツキが一層低減されて、再生信号
のC/Nが一層向上する。この効果は、下地層ロッキン
グカ−ブの半値幅が20deg以下の場合に一層顕著で
ある。また、交互積層膜の結晶性・配向性が向上する
と、保磁力や垂直磁気異方性等も向上して、記録ビット
が安定する。As described above, the half value width of the rocking curve of X-ray diffraction is increased by improving the orientation of the noble metal of the alternately laminated film.
According to the present invention in which the deg or less is set, the fluctuation and variation of the reflected light at the time of reproducing the information are reduced, and the C / N of the reproduced signal is improved. Further, in the present invention using a compound in which a peak on a certain surface of a crystal appears by X-ray diffraction as an underlayer, fluctuations and variations in reflected light from the underlayer are reduced, and the noble metal of the alternately laminated film is reduced. Is also improved,
Fluctuations and variations in the reflected light are further reduced, and the C / N of the reproduced signal is further improved. This effect is more remarkable when the half width of the underlayer locking curve is 20 deg or less. Further, when the crystallinity and orientation of the alternately laminated film are improved, the coercive force, the perpendicular magnetic anisotropy, etc. are also improved, and the recording bit is stabilized.
【図1】実施例の光磁気記録媒体の断面構造を示す模式
図である。FIG. 1 is a schematic diagram illustrating a cross-sectional structure of a magneto-optical recording medium according to an example.
【図2】従来の光磁気記録媒体の断面構造を示す模式図
である。FIG. 2 is a schematic diagram showing a cross-sectional structure of a conventional magneto-optical recording medium.
【図3】実施例の光磁気記録媒体を作成するための装置
の構成図である。FIG. 3 is a configuration diagram of an apparatus for producing a magneto-optical recording medium according to an embodiment.
【図4】従来の光磁気記録媒体の結晶を示す模式図であ
る。FIG. 4 is a schematic view showing a crystal of a conventional magneto-optical recording medium.
【図5】Ptの結晶構造図である。FIG. 5 is a crystal structure diagram of Pt.
【図6】〔111〕方向から見た積み重ねの構造図であ
る。FIG. 6 is a structural view of the stack viewed from the [111] direction.
【図7】実施例の光磁気記録媒体下地層のX線回折像で
ある。FIG. 7 is an X-ray diffraction image of a magneto-optical recording medium underlayer of an example.
【図8】従来の光磁気記録媒体下地層のX線回折像であ
る。FIG. 8 is an X-ray diffraction image of a conventional magneto-optical recording medium underlayer.
【図9】実施例の光磁気記録媒体のX線回折のロッキン
グカ−ブである。FIG. 9 is a X-ray diffraction locking curve of the magneto-optical recording medium of the embodiment.
【図10】従来の光磁気記録媒体のX線回折のロッキン
グカ−ブである。FIG. 10 shows a locking curve for X-ray diffraction of a conventional magneto-optical recording medium.
【図11】実施例の光磁気記録媒体と従来の光磁気記録
媒体のキャリア,ノイズを示す特性図である。FIG. 11 is a characteristic diagram showing carriers and noise of the magneto-optical recording medium of the embodiment and a conventional magneto-optical recording medium.
1 Pt/Co交互積層膜 2 ZnO下地層 20 アモルファスSiN下地層 3 基板 DESCRIPTION OF SYMBOLS 1 Pt / Co alternating laminated film 2 ZnO underlayer 20 Amorphous SiN underlayer 3 Substrate
フロントページの続き (58)調査した分野(Int.Cl.6,DB名) G11B 11/10 506 Continuation of front page (58) Field surveyed (Int.Cl. 6 , DB name) G11B 11/10 506
Claims (4)
が交互に積層されて成る交互積層膜を基板上に成膜して
成る光磁気記録媒体に於いて、 前記交互積層膜の貴金属のX線回折のロッキングカ−ブ
の半値幅を18deg以下とした光磁気記録媒体。1. A magneto-optical recording medium comprising an alternately laminated film in which layers having a noble metal and layers having a transition metal are alternately laminated on a substrate, wherein X of the noble metal in the alternately laminated film is A magneto-optical recording medium having a half-width of a rocking curve for line diffraction of 18 deg or less.
が交互に積層されて成る交互積層膜を、透光性の下地層
を介して基板上に成膜して成る光磁気記録媒体に於い
て、前記下地層を、X線回折を行ったとき結晶の或る面
のピ−クが現れる化合物により形成して成る光磁気記録
媒体。2. A magneto-optical recording medium comprising an alternately laminated film in which layers having a noble metal and layers having a transition metal are alternately laminated on a substrate via a light-transmitting underlayer. A magneto-optical recording medium, wherein the underlayer is formed of a compound that shows a peak on a certain surface of the crystal when subjected to X-ray diffraction.
0deg以下である光磁気記録媒体。3. The X-ray diffraction rocking curve of the underlayer according to claim 2, wherein the half width of the rocking curve is 2.
A magneto-optical recording medium having 0 deg or less.
SiC,BeO,CoSから選ばれた何れかの化合物で
ある光磁気記録媒体。4. The method according to claim 2, wherein the compound of the underlayer is ZnO, Al 2 O 3 , AlN,
A magneto-optical recording medium that is any compound selected from SiC, BeO, and CoS.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP25401792A JP2902872B2 (en) | 1992-08-28 | 1992-08-28 | Magneto-optical recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP25401792A JP2902872B2 (en) | 1992-08-28 | 1992-08-28 | Magneto-optical recording medium |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0676382A JPH0676382A (en) | 1994-03-18 |
| JP2902872B2 true JP2902872B2 (en) | 1999-06-07 |
Family
ID=17259096
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP25401792A Expired - Fee Related JP2902872B2 (en) | 1992-08-28 | 1992-08-28 | Magneto-optical recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2902872B2 (en) |
-
1992
- 1992-08-28 JP JP25401792A patent/JP2902872B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0676382A (en) | 1994-03-18 |
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