JPH0626171B2 - Method for producing amorphous magnetic thin film - Google Patents
Method for producing amorphous magnetic thin filmInfo
- Publication number
- JPH0626171B2 JPH0626171B2 JP1423385A JP1423385A JPH0626171B2 JP H0626171 B2 JPH0626171 B2 JP H0626171B2 JP 1423385 A JP1423385 A JP 1423385A JP 1423385 A JP1423385 A JP 1423385A JP H0626171 B2 JPH0626171 B2 JP H0626171B2
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- rare earth
- magnetic thin
- earth metal
- target
- 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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- Thin Magnetic Films (AREA)
Description
【発明の詳細な説明】 〔発明の利用分野〕 本発明は非晶質磁性薄膜の製造方法に係り、特に光磁気
記録媒体や磁気バブルメモリ媒体に好適な希土類・遷移
金属非晶質磁性薄膜の製造方法に関する。Description: FIELD OF THE INVENTION The present invention relates to a method for producing an amorphous magnetic thin film, and more particularly to a rare earth / transition metal amorphous magnetic thin film suitable for a magneto-optical recording medium or a magnetic bubble memory medium. It relates to a manufacturing method.
光磁気記録媒体や磁気バルブメモリ媒体に用いる磁性薄
膜の必要条件は、磁化が膜面に対して垂直に向いている
ことである。すなわち次式、 Ku>2πMs2 …(1) を満足していなければならない。ここでKuは垂直磁気
異方性エネルギー、Msは磁化である。A necessary condition of the magnetic thin film used for the magneto-optical recording medium or the magnetic valve memory medium is that the magnetization is perpendicular to the film surface. That is, the following expression, Ku> 2πMs 2 (1) must be satisfied. Here, Ku is the perpendicular magnetic anisotropy energy, and Ms is the magnetization.
(1)式から垂直磁気異方性エネルギーには、ある一定値
以上の値が必要である。また、磁気バブルメモリ媒体に
おいて、特定の直径のバブルメインを保持するために
は、飽和磁化と垂直磁気異方性エネルギーの両方をある
特定の値に制御する必要がある。From the equation (1), the perpendicular magnetic anisotropy energy needs to be a certain value or more. Further, in the magnetic bubble memory medium, it is necessary to control both the saturation magnetization and the perpendicular magnetic anisotropy energy to a certain specific value in order to hold the bubble main having a specific diameter.
従来、希土類・遷移金属非晶質磁性薄膜の垂直磁気異方
性エネルギーの大きさを制御する方法として、例えば特
公昭59-31970号公報に示されるように、スパッタ法で非
晶質磁性薄膜を作製する際、スパツタガス中に反応性ガ
スを混入する方法が知られている。Conventionally, as a method for controlling the magnitude of the perpendicular magnetic anisotropy energy of a rare earth / transition metal amorphous magnetic thin film, for example, as shown in Japanese Patent Publication No. 59-31970, an amorphous magnetic thin film is formed by a sputtering method. A method is known in which a reactive gas is mixed into the spatula gas at the time of manufacturing.
この方法は、混入する反応性ガスの分圧量を調整するこ
とにより、非晶質磁性薄膜の垂直磁気異方性エネルギー
を制御する方法である。しかし、垂直磁気異方性エネル
ギーの大きさは、混入した反応性ガスを分圧量だけでな
く、薄膜の成長速度などの他の薄膜作製条件にも敏感に
依存することが判明した。そのため、垂直磁気異方性エ
ネルギーが膜厚方向や膜面内で変動したり、再現性が低
下して、垂直磁気異方性エネルギーを精度よく制御でき
ないという問題を生ずる。This method is a method of controlling the perpendicular magnetic anisotropy energy of the amorphous magnetic thin film by adjusting the partial pressure amount of the reactive gas to be mixed. However, it was found that the magnitude of the perpendicular magnetic anisotropy energy sensitively depends not only on the partial pressure amount of the mixed reactive gas but also on other thin film forming conditions such as the growth rate of the thin film. Therefore, the perpendicular magnetic anisotropy energy fluctuates in the film thickness direction or in the film plane, and the reproducibility is deteriorated, which causes a problem that the perpendicular magnetic anisotropy energy cannot be controlled accurately.
本発明の目的は、希土類金属と遷移金属からなる非晶質
磁性薄膜の垂直磁気異方性エネルギーを精度よく制御し
得る非晶質磁性薄膜の製造方法を提供することにある。An object of the present invention is to provide a method for producing an amorphous magnetic thin film which can control the perpendicular magnetic anisotropy energy of the amorphous magnetic thin film made of a rare earth metal and a transition metal with high accuracy.
本発明者らは従来のスパツタガス中に反応性ガスを混入
する方法において、垂直磁気異方性エネルギーの均一性
や制御性が低下する原因が次の二点であることを見出し
た。The present inventors have found that in the conventional method of mixing the reactive gas into the sputtering gas, the following two points cause the deterioration of the uniformity and controllability of the perpendicular magnetic anisotropy energy.
(1) 薄膜中に取り込まれる反応性ガスの量が、反応性ガ
スの分圧量だけでなく、薄膜の成長速度と基板とターゲ
ツト間の距離あるいは基板温度によつて変化する。(1) The amount of the reactive gas taken into the thin film changes depending on not only the partial pressure amount of the reactive gas but also the growth rate of the thin film and the distance between the substrate and the target or the substrate temperature.
(2) スパツタガス中に混入した反応性ガスが、ターゲツ
トから飛び出す粒子や種類や数に影響を与え、作製した
薄膜の組成や成長速度を変化させる。(2) The reactive gas mixed in the sputtering gas influences the particles, types and number of particles ejected from the target, and changes the composition and growth rate of the produced thin film.
本発明は、これらの原因を初めて認識し、反応性ガス元
素を含む希土類金属の化合物をスパツタターゲツトの一
部として用いることにより、上記原因を取り除き本発明
の目的を達成するものである。この本発明の構成によれ
ば、ターゲツトに含まれる希土類金属化合物の割合を調
節することによつて、非晶質強磁性薄膜の垂直磁気異方
性エネルギーは容易に制御できる。すなわち、反応性ガ
ス元素は、希土類元素との化合となつた状態でターゲツ
トから供給されるため、薄膜の成長速度や基板とターゲ
ツト間の距離あるいは基板温度に依らず、常に一定の割
合で薄膜中に取り込まれる。また、スパツタガス中に反
応性ガスを含まないため、ターゲツト表面で遷移金属あ
るいは希土類金属と反応性ガスと反応が生じず、ターゲ
ツト表面のスパツタ条件は一定に保たれる。このよう
に、所望の磁性薄膜の界面層のように非常に薄い磁性層
であっても、垂直磁気異方性エネルギーを精度よく制御
できる。The present invention recognizes these causes for the first time and uses a compound of a rare earth metal containing a reactive gas element as a part of a spatula target to eliminate the above causes and achieve the object of the present invention. According to the configuration of the present invention, the perpendicular magnetic anisotropy energy of the amorphous ferromagnetic thin film can be easily controlled by adjusting the ratio of the rare earth metal compound contained in the target. That is, since the reactive gas element is supplied from the target in a state of being combined with the rare earth element, the reactive gas element does not depend on the growth rate of the thin film, the distance between the substrate and the target, or the substrate temperature. Is taken into. Further, since the sputter gas does not contain a reactive gas, the transition metal or the rare earth metal does not react with the reactive gas on the target surface, and the spatter condition on the target surface is kept constant. In this way, the perpendicular magnetic anisotropy energy can be accurately controlled even with a very thin magnetic layer such as an interface layer of a desired magnetic thin film.
本発明における非晶質磁性薄膜の製造方法には、高周波
スパツタ法をはじめとする各種スパツタ法およびイオン
ビームスパツタ法を含む。反応性ガス元素を含む希土類
金属の化合物には、酸化物、窒化物、塩化物、フツ化
物、水素化物などがある。ターゲツトの作製方法として
は、遷移金属と希土類金属および希土類金属化合物の単
体を組み合わせて構成したターゲツト、いわゆる複合タ
ーゲツトとする方法の他に、遷移金属と希土類金属を反
応性ガス雰囲気中で合金または焼結体として、希土類金
属と反応性ガス元素との化合物を含むターゲツトとする
方法がある。または、遷移金属と希土類金属から成るタ
ーゲツトを反応性ガス雰囲気中で熱処理して作製するこ
ともできる。尚、反応性ガス雰囲気中で合金若しくは焼
結体とする場合、又は熱処理する場合、希土類金属の反
応性ガス元素との化合物のターゲツトに占める割合は反
応性ガスの供給圧力等によつて変えることができる。The method for producing an amorphous magnetic thin film according to the present invention includes various sputter methods including the high frequency sputter method and the ion beam sputter method. The rare earth metal compound containing a reactive gas element includes oxides, nitrides, chlorides, fluorides, hydrides, and the like. As a method for producing the target, in addition to a method in which a transition metal and a rare earth metal and a rare earth metal compound are combined to form a target, a so-called composite target, the transition metal and the rare earth metal are alloyed or burned in a reactive gas atmosphere. As a binder, there is a method of forming a target containing a compound of a rare earth metal and a reactive gas element. Alternatively, it can be manufactured by heat-treating a target composed of a transition metal and a rare earth metal in a reactive gas atmosphere. When forming an alloy or a sintered body in a reactive gas atmosphere, or when performing heat treatment, the ratio of the compound of the rare earth metal and the reactive gas element in the target should be changed according to the supply pressure of the reactive gas. You can
以下、本発明の実施例として、Gd2O3をターゲツトの
一部として用いて作製したGd−Coの非晶質磁性薄膜
とTbF3とTb4O7をそれぞれ用いて作製したTb−
Fe非晶質磁性薄膜の例について述べる。同様な効果
は、Gd−Fe,Tb−Co,Ho−Co,Tb−Fe
−Co,Gd−Tb−Fe−Coなどの希土類遷移金属
非晶質磁性薄膜においても得られる。また、Bi,S
n,Au,Cu,Mo,Al,Niなどの元素を添加し
た希土類遷移金属非晶質薄膜においても、実施例と同様
の効果が得られる。Hereinafter, as an example of the present invention, an amorphous magnetic thin film of Gd—Co prepared by using Gd 2 O 3 as a part of a target and Tb− prepared by using TbF 3 and Tb 4 O 7 , respectively.
An example of the Fe amorphous magnetic thin film will be described. Similar effects are obtained with Gd-Fe, Tb-Co, Ho-Co, Tb-Fe.
It can also be obtained in rare-earth transition metal amorphous magnetic thin films such as -Co and Gd-Tb-Fe-Co. Also, Bi, S
The same effect as that of the embodiment can be obtained also in the rare earth transition metal amorphous thin film to which an element such as n, Au, Cu, Mo, Al or Ni is added.
第1図に、直径110mm、厚さ1mmのCo円板上に4mm
×4mm、厚さ1mmのGd小片とGd2O3小片を均一に配
置した複合ターゲツトを用いて、イオンビームスパツタ
法で作製したGd−Co非晶質性薄膜の垂直磁気異方性
エネルギーと磁化の大きさの関係を示す。スパツタ条件
は、基板:Si基板、スパツタガス圧(Arガス):1.
9×10-2Pa、加速電圧:1.1kV、イオン電流
量:60mA、スパツタ時間:40分であり、膜厚が約
0.4μmの薄膜を作製した。Fig. 1 shows 4mm on a Co disk with a diameter of 110mm and a thickness of 1mm.
The perpendicular magnetic anisotropy energy of a Gd-Co amorphous thin film prepared by the ion beam sputtering method using a composite target in which Gd pieces and Gd 2 O 3 pieces each having a thickness of 4 mm and a thickness of 1 mm are uniformly arranged. The relationship of the magnitude of magnetization is shown. The sputtering conditions are: substrate: Si substrate, sputtering gas pressure (Ar gas): 1.
9 × 10 −2 Pa, accelerating voltage: 1.1 kV, ion current amount: 60 mA, sputtering time: 40 minutes, and a thin film having a thickness of about 0.4 μm was prepared.
第1図に示すように、ターゲツトの希土類成分(Gd,
Gd2O3)の中でGd2O3の割合が増す程、大きな垂直
磁気異方性エネルギーが得られる。また、GdとG2O3の
面積比が一定の場合、Coの面積比が大きい程、飽和磁
化は大きくなる。すなわち、GdとGd2O3およびCo
の面積比を調節することによつて、所望の垂直磁気異方
性エネルギーと飽和磁化を持つ薄膜を得ることができ
る。As shown in FIG. 1, the target rare earth component (Gd,
Gd 2 O 3) higher the ratio of Gd 2 O 3 increases in the large perpendicular magnetic anisotropy energy is obtained. Further, when the area ratio of Gd and G 2 O 3 is constant, the larger the area ratio of Co, the larger the saturation magnetization. That is, Gd, Gd 2 O 3 and Co
A thin film having desired perpendicular magnetic anisotropy energy and saturation magnetization can be obtained by adjusting the area ratio of.
第2図に、上述の方法で作製したGd−Co非晶質磁性
薄膜の垂直磁気異方性エネルギーの成長速度依存性を示
す。イオン電流量を変化させて、薄膜の成長速度を制御
した。また、膜厚が約0.4μmとなるようにスパツタ時
間を設定した。その他のスパツタ条件は上述の条件と同
じである。垂直磁気異方性エネルギーは成長速度に依存
せず、一定の大きさである。FIG. 2 shows the growth rate dependence of the perpendicular magnetic anisotropy energy of the Gd-Co amorphous magnetic thin film produced by the above method. The amount of ion current was changed to control the growth rate of the thin film. The sputtering time was set so that the film thickness was about 0.4 μm. The other spatula conditions are the same as the above-mentioned conditions. The perpendicular magnetic anisotropy energy does not depend on the growth rate and has a constant magnitude.
第3図に、直径110mm、厚さ1mmのFe円板上に4mm
×4mm、厚さ1mmのTb小片とTbF3小片およびTb
小片とTb4O7小片をそれぞれ配置した複合ターゲツト
を用いて、高周波スパツタ法で作製したTb−Fe非晶
質磁性薄膜の垂直磁気異方性エネルギーを示す。横軸は
ターゲツトにおける希土類金属成分(Tb+TbF3,
Tb+Tb4O7)のうち、希土類金属化合物(Tb
F3,Tb4O7)の割合を示す。Tb−Fe非晶質磁性
薄膜においても、ターゲツトに占めるTbF3とTb4O
7の割合が増すに従つて、垂直磁気異方性エネルギーが
増加する。Fig. 3 shows 4 mm on a Fe disk with a diameter of 110 mm and a thickness of 1 mm.
× 4mm, 1mm thick Tb piece, TbF 3 piece and Tb piece
Using the composite Tagetsuto disposed respectively pieces and Tb 4 O 7 small pieces, showing a perpendicular magnetic anisotropy energy of Tb-Fe amorphous magnetic thin films prepared by RF sputter method. The horizontal axis is the rare earth metal component (Tb + TbF 3 ,
Tb + Tb 4 O 7 ), a rare earth metal compound (Tb
F 3, shows the percentage of Tb 4 O 7). Also in Tb-Fe amorphous magnetic thin film, TbF 3 and Tb 4 O occupying the Tagetsuto
The perpendicular magnetic anisotropy energy increases as the ratio of 7 increases.
以上本発明によれば、ターゲツトの一部として反応性ガ
ス元素を含む希土類金属の化合物を用いているので垂直
磁気異方性エネルギーを容易に増大させ、かつ再現性良
く制御することが可能となる。磁気特性の異なる非常に
薄い非晶質磁性薄膜を多層に積層する場合にも、垂直磁
気異方性を精度よく制御することが可能となる。As described above, according to the present invention, since the compound of the rare earth metal containing the reactive gas element is used as a part of the target, it is possible to easily increase the perpendicular magnetic anisotropy energy and control it with good reproducibility. . It is possible to control the perpendicular magnetic anisotropy with high precision even when a very thin amorphous magnetic thin film having different magnetic properties is laminated in multiple layers.
第1図はGd2O3をターゲツトの一部として用いて作製
したGd−Coの非晶質薄膜の垂直磁気異方性エネルギ
ーと磁化の関係を示す図、第2図は垂直磁気異方性エネ
ルギーの成長速度依存性を示す図、第3図はTb−Fe
非晶質薄膜における垂直磁気異方性エネルギーのターゲ
ツト中のTbF3,Tb4O7の割合に対する依存性を示
す図である。FIG. 1 is a diagram showing the relationship between the perpendicular magnetic anisotropy energy and the magnetization of an amorphous thin film of Gd—Co produced by using Gd 2 O 3 as a part of the target, and FIG. 2 is the perpendicular magnetic anisotropy. Figure 3 shows the dependence of energy on the growth rate. Figure 3 shows Tb-Fe.
It is a diagram showing the dependence on the ratio of TbF 3, Tb 4 O 7 in Tagetsuto the perpendicular magnetic anisotropy energy in amorphous thin film.
Claims (3)
らなる非晶質磁性薄膜を製造する方法において、反応性
ガス元素を含む希土類金属の化合物をターゲットの一部
として用いることを特徴とする非晶質磁性薄膜の製造方
法。1. A method for producing an amorphous magnetic thin film composed of a rare earth metal and a transition metal by a sputtering method, wherein a compound of a rare earth metal containing a reactive gas element is used as a part of the target. Of manufacturing a magnetic thin film.
希土類金属成分のうち20%以上を占めることを特徴と
する特許請求の範囲第1項記載の非晶質磁性薄膜の製造
方法。2. The method for producing an amorphous magnetic thin film according to claim 1, wherein the rare earth metal compound accounts for 20% or more of the rare earth metal component in the target.
合物として、酸化物、窒化物、塩化物、フッ化物および
水素化物からなる群から選ばれる少なくとも一の化合物
を用いることを特徴とする特許請求の範囲第1項記載の
非晶質磁性薄膜の製造方法。3. A patent using at least one compound selected from the group consisting of oxides, nitrides, chlorides, fluorides and hydrides as the compound of the rare earth metal containing the reactive gas element. The method for producing an amorphous magnetic thin film according to claim 1.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1423385A JPH0626171B2 (en) | 1985-01-30 | 1985-01-30 | Method for producing amorphous magnetic thin film |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1423385A JPH0626171B2 (en) | 1985-01-30 | 1985-01-30 | Method for producing amorphous magnetic thin film |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61174616A JPS61174616A (en) | 1986-08-06 |
| JPH0626171B2 true JPH0626171B2 (en) | 1994-04-06 |
Family
ID=11855355
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1423385A Expired - Lifetime JPH0626171B2 (en) | 1985-01-30 | 1985-01-30 | Method for producing amorphous magnetic thin film |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0626171B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2746206B1 (en) * | 1996-03-15 | 1998-04-10 | MAGNETO-OPTICAL RECORDING MEDIUM AND PRODUCTION METHOD | |
| US6859998B2 (en) * | 2002-04-12 | 2005-03-01 | International Business Machines Corporation | Method of fabricating a narrow projection such as a write pole extending from a substrate |
| JP2015502455A (en) * | 2011-11-11 | 2015-01-22 | ビーコ・インストゥルメンツ・インコーポレイテッド | Deposition method of fluorine-based optical thin film by ion beam |
-
1985
- 1985-01-30 JP JP1423385A patent/JPH0626171B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61174616A (en) | 1986-08-06 |
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