JPH07120596B2 - Method of forming ferromagnetic thin film - Google Patents
Method of forming ferromagnetic thin filmInfo
- Publication number
- JPH07120596B2 JPH07120596B2 JP62268818A JP26881887A JPH07120596B2 JP H07120596 B2 JPH07120596 B2 JP H07120596B2 JP 62268818 A JP62268818 A JP 62268818A JP 26881887 A JP26881887 A JP 26881887A JP H07120596 B2 JPH07120596 B2 JP H07120596B2
- Authority
- JP
- Japan
- Prior art keywords
- atomic
- film
- substrate
- thin film
- straight line
- 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
Links
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- Physical Vapour Deposition (AREA)
- Manufacturing Of Magnetic Record Carriers (AREA)
- Thin Magnetic Films (AREA)
Description
【発明の詳細な説明】 (産業上の利用分野) この発明は磁気記録媒体や高性能小型モータ等に用いら
れる強磁性薄膜に係り,最大エネルギ積(BH)maxを大
きくする形成方法に関する。The present invention relates to a ferromagnetic thin film used in a magnetic recording medium, a high-performance small motor, etc., and relates to a forming method for increasing the maximum energy product (BH) max.
(従来の技術) 大きな保磁力と最大エネルギ積(BH)maxを有するNd−F
e−B系磁石は機器の小型化に貢献するためその利用が
進められている。ところが,この磁石は成形性と加工性
が困難なため薄肉化や特殊形状での使用ができない。そ
のため,液体急冷法,スパッタ法,スプレー法等によ
り,任意の形状の薄膜を形成する研究が行われており,
たとえば,スパッタ法の例は,J.Magn.Magn.Mat.54−57
(1986)P535,あるいは,本出願人が出願した特願昭61
−229130号などに示されている。(Prior art) Nd-F with large coercive force and maximum energy product (BH) max
The use of e-B magnets is being promoted in order to contribute to the miniaturization of equipment. However, since this magnet is difficult to form and work, it cannot be thinned or used in a special shape. Therefore, research has been conducted to form thin films of arbitrary shape by liquid quenching, sputtering, spraying, etc.
For example, the sputtering method is described in J. Magn. Magn. Mat. 54-57.
(1986) P535, or Japanese Patent Application No. Sho 61 filed by the applicant.
−229130 and the like.
(発明が解決しようとする問題点) 磁気を利用した装置を高性能化,小型化する場合には最
大エネルギ積(BH)maxが大きく,たとえば10MGOe以上
の値のものが必要であるが,特に膜厚方向に異方性をそ
なえたもので最大エネルギ積(BH)maxが上記の値を超
えるものは前項文献に示されているように得られていな
いのが現状である。(Problems to be solved by the invention) In order to improve the performance and size of a device using magnetism, the maximum energy product (BH) max is large, for example, a value of 10 MGOe or more is required. In the present situation, as shown in the above-mentioned literature, the one having anisotropy in the film thickness direction and the maximum energy product (BH) max exceeding the above value has not been obtained at present.
この発明の目的は上記の問題点を解決した最大エネルギ
積(BH)maxの高い膜厚方向に異方性をもつ膜の形成方
法を提供するものである。An object of the present invention is to provide a method for forming a film having a high maximum energy product (BH) max and having anisotropy in the film thickness direction, which solves the above problems.
(問題点を解決するための手段) このためNdが13〜27原子%,Bが3〜17原子%,Feが28原
子%以上,残部は,Co,Alの一種以上からなる合金薄膜を
スパッタリング法により形成したのち,膜厚方向の角形
比が0.7以上のものを真空中もしくは非酸化性ガス雰囲
気中(例えばN2ガス中)で所定の温度で所定時間アニー
ル処理を行う。(Means for solving the problem) For this reason, an alloy thin film consisting of 13 to 27 atomic% of Nd, 3 to 17 atomic% of B, 28 atomic% or more of Fe, and the balance of at least one of Co and Al is sputtered. After being formed by the method, a film having a squareness ratio in the film thickness direction of 0.7 or more is annealed at a predetermined temperature for a predetermined time in a vacuum or a non-oxidizing gas atmosphere (for example, N 2 gas).
(作用) スパッタリング法により膜厚方向に異方性のついた膜を
上記の条件でアニールすることにより結晶化が計られる
と共に磁性層が,結晶粒界に生成した非磁性層に取り囲
まれた状態になり,このため,外部磁界が作用しても磁
壁の移動が妨げられるので,高エネルギ積を有する膜厚
方向に異方性をもった膜が得られる。(Function) A state in which a film having anisotropy in the film thickness direction by the sputtering method is annealed under the above conditions to be crystallized and the magnetic layer is surrounded by the non-magnetic layer formed at the grain boundary. Therefore, the movement of the domain wall is prevented even when an external magnetic field is applied, so that a film having a high energy product and having anisotropy in the film thickness direction is obtained.
第1図は本発明の垂直磁化膜を形成するための多極マグ
ネトロンスパッタリング装置の断面図である。真空容器
1の中にターゲット2を設け,これと対向させて25mmの
間隔を置き基板3を基板取付台4に配置している。FIG. 1 is a sectional view of a multipole magnetron sputtering apparatus for forming a perpendicularly magnetized film of the present invention. A target 2 is provided in a vacuum container 1, and a substrate 3 is placed on a substrate mounting base 4 facing the target 2 with a space of 25 mm.
基板はヒータ6によって加熱することができ,基板の温
度をヒータ電源13によってコントロールするようにして
ある。ターゲット2と基板3の間にはスパッタリング初
期に飛散する粒子が基板に付着するのを防ぐためシャッ
タ5を配設しており,ターゲット2にはターゲット電源
7によって直流電圧または高周波電圧を印加できるよう
にしてある。ターゲットの近傍にはフィラメント8とア
ノード電極10を配置しフィラメント電源9によりフィラ
メントを加熱し熱電子を発生させてアノード電極10へ集
めるようにしており,フィラメント電源9とアノード電
源11によりターゲット電流は任意に変えられるのでター
ゲット電圧とターゲット電流は独立に変えることが可能
である。The substrate can be heated by the heater 6, and the temperature of the substrate is controlled by the heater power supply 13. A shutter 5 is provided between the target 2 and the substrate 3 to prevent particles scattered in the initial stage of sputtering from adhering to the substrate, and a DC voltage or a high frequency voltage can be applied to the target 2 by a target power supply 7. I am doing it. The filament 8 and the anode electrode 10 are arranged in the vicinity of the target, and the filament power source 9 heats the filament to generate thermoelectrons and collect them in the anode electrode 10. The filament power source 9 and the anode power source 11 allow the target current to be arbitrary. The target voltage and the target current can be changed independently.
ターゲット2は薄膜中のNdが15原子%,Bが5原子%,Fe
が63原子%,Coが10原子%,Alが7原子%になるように各
粉末を混合し,真空中で焼結したものを用い,このター
ゲットをスパッタリング電極に取り付け,基板3を基板
台4に設置した後,真空容器内を排気系14により2×10
-6Torr以下に排気する。ヒータ電源13を調整しながら基
板を300℃に加熱しておき,フィラメント電源9を調整
してフィラメント8を加熱した後,アルゴンガス導入バ
ルブ12を開いてアルゴンガスを導入し、圧力が8×10-3
Torrになるように調整した。アノード電源を調整してタ
ーゲット電流を0.5Aにした後,シャッタ5を閉じたまま
ターゲット電源7により負の直流電圧300Vを印加して15
分間予備スパッタリングを行い,ターゲット表面の酸化
物等を除去し,シャッタを開いて20分間スパッタリング
を行い,約2μmの厚さの膜を形成した。この後,再び
真空容器内を2×10-6Torr以下に排気し,基板温度が室
温になるまで冷却した。膜厚方向の角型比が0.7以上の
ものを選択して急加熱急冷が可能な赤外線イメージ炉に
セットし炉内を2×10-6Torr以下に排気した後,640℃に
急加熱して10秒間加熱してアニールを行った後ただちに
冷却した。この結果,10MGOe以上のエネルギー積の強磁
性膜が得られた。第2図は温度と時間を種々変えてアニ
ールをしたときの膜の特性の測定値を10MGOe以上と以下
に分けた分布を示す。丸印はアニール後膜厚方向の最大
エネルギ積(BH)maxが10MGOe以上となったものであ
る。すなわち斜線で示した領域の条件でアニールを行え
ば膜厚方向の最大エネルギ積(BH)maxが10MGOe以上の
ものが得られる。アニール温度が800℃を超えると常磁
性相の成長により磁気特性が損われ,逆に400℃に満た
ないといくら時間をかけても結晶化が促進されず磁気特
性が向上しない。Target 2 is 15 at% Nd, 5 at% B in the thin film, Fe
Was mixed in such a manner that the powder content was 63 atomic%, Co was 10 atomic%, and Al was 7 atomic%, and the powder was sintered in vacuum. This target was attached to the sputtering electrode, and the substrate 3 was mounted on the substrate table 4. 2 x 10 inside the vacuum container by the exhaust system 14
Exhaust below -6 Torr. The substrate is heated to 300 ° C. while adjusting the heater power supply 13, the filament power supply 9 is adjusted to heat the filament 8, and then the argon gas introduction valve 12 is opened to introduce the argon gas, and the pressure is 8 × 10 5. -3
Adjusted to be Torr. After adjusting the anode power supply to a target current of 0.5 A, the target power supply 7 applies a negative DC voltage of 300 V with the shutter 5 closed.
Pre-sputtering was performed for minutes to remove oxides and the like on the target surface, the shutter was opened, and sputtering was performed for 20 minutes to form a film having a thickness of about 2 μm. After that, the inside of the vacuum vessel was evacuated again to 2 × 10 −6 Torr or less and cooled to the substrate temperature of room temperature. Select a squareness ratio of 0.7 or more in the film thickness direction, set it in an infrared image furnace capable of rapid heating and cooling, exhaust the inside of the furnace to 2 × 10 -6 Torr or less, and then rapidly heat it to 640 ° C. After heating for 10 seconds to anneal, it was immediately cooled. As a result, a ferromagnetic film with an energy product of more than 10 MGOe was obtained. Fig. 2 shows the distribution of the measured values of the film characteristics when annealing was performed at various temperatures and times, divided into 10 MGOe and above. The circles indicate that the maximum energy product (BH) max in the film thickness direction after annealing was 10 MGOe or more. That is, if annealing is performed under the conditions of the shaded region, a maximum energy product (BH) max in the film thickness direction of 10 MGOe or more can be obtained. When the annealing temperature exceeds 800 ° C, the magnetic properties are impaired by the growth of the paramagnetic phase. Conversely, when the annealing temperature is less than 400 ° C, crystallization is not promoted and the magnetic properties do not improve no matter how long it takes.
またアニール保持時間はアニール温度により異なり,た
とえばアニール温度640℃〜800℃のときは保持時間10秒
で良いが,アニール温度が600℃のときは保持時間45秒,
500℃のときは1700秒というようにアニール温度が低い
ほど保持時間が長くなるが,保持時間が20時間を超える
ときはアニール温度は400〜800℃の間であれば10MGOeの
ものが得られる。The annealing holding time differs depending on the annealing temperature. For example, when the annealing temperature is 640 ° C to 800 ° C, the holding time is 10 seconds, but when the annealing temperature is 600 ° C, the holding time is 45 seconds.
The lower the annealing temperature is, such as 1700 seconds at 500 ° C, the longer the holding time becomes, but when the holding time exceeds 20 hours, the annealing temperature between 400 and 800 ° C gives 10MGOe.
なお,合金薄膜の組成を変え,調べたところ,表に示す
組成で角形比0.7以上のものを選び,前記アニール条件
で実験した結果は,いずれも良好な結果が得られた。す
なわちNdが13〜27原子%,Bが3〜17原子%,Feが28原子
%以上,残部,Co,Alの一種以上からなる組成の膜を上記
アニール条件でアニールすることにより最大エネルギ積
(BH)maxが10MGOe以上でかつ膜厚方向に異方性のつい
た膜が得られる。When the composition of the alloy thin film was changed and examined, a good result was obtained as a result of selecting a composition having a squareness ratio of 0.7 or more and performing the experiment under the above annealing conditions. That is, a film having a composition of 13 to 27 atomic% of Nd, 3 to 17 atomic% of B, 28 atomic% or more of Fe, and the balance of one or more of Co and Al is annealed under the above annealing conditions to obtain the maximum energy product ( A film having a BH) max of 10 MGOe or more and having anisotropy in the film thickness direction can be obtained.
(発明の効果) 以上説明したように本発明によれば,最大エネルギ積
(BH)maxが10MGOe以上の垂直磁化膜が得られる効果が
あり,このため磁気を利用した装置を高性能化,小型化
することができる。 (Effects of the Invention) As described above, according to the present invention, there is an effect that a vertically magnetized film having a maximum energy product (BH) max of 10 MGOe or more can be obtained. Therefore, a device using magnetism has high performance and is small in size. Can be converted.
第1図は本発明の垂直磁化膜を形成するための多極マグ
ネトロンスパッタリング装置の例を示す断面図,第2図
は本発明のアニール条件を示す特性図である。 図において2はターゲット,3は基板,5はシャッタであ
る。FIG. 1 is a sectional view showing an example of a multi-pole magnetron sputtering apparatus for forming a perpendicularly magnetized film of the present invention, and FIG. 2 is a characteristic diagram showing annealing conditions of the present invention. In the figure, 2 is a target, 3 is a substrate, and 5 is a shutter.
Claims (1)
が28原子%以上、残部がCo、Alのうち一種以上からなる
合金薄膜をスパッタリング法により基板上に形成し、膜
厚方向の角形比が0.7以上の合金薄膜を有する基板を選
択して真空中または非酸化性ガス雰囲気中で、アニール
保持時間s(秒)をlog(s)としてX軸にとり、アニ
ール保持温度(℃)をY軸にとったとき、直線Y=80
0、直線X=1、直線Y=400、直線X=6および点(1,
640)と点(4.8,400)を結ぶ直線で囲まれる範囲でアニ
ールすることを特徴とする強磁性薄膜の形成方法。1. Nd of 13 to 27 atomic%, B of 3 to 17 atomic%, Fe
Is 28 atomic% or more and the balance is at least one of Co and Al on the substrate by sputtering, and select a substrate with an alloy thin film with a squareness ratio of 0.7 or more in the film thickness direction in vacuum. Or, in an atmosphere of non-oxidizing gas, when the annealing holding time s (sec) is taken as log (s) on the X axis and the annealing holding temperature (° C) is taken on the Y axis, a straight line Y = 80
0, straight line X = 1, straight line Y = 400, straight line X = 6 and point (1,
640) and the point (4.8,400) are annealed in a range surrounded by a straight line.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62268818A JPH07120596B2 (en) | 1987-10-23 | 1987-10-23 | Method of forming ferromagnetic thin film |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62268818A JPH07120596B2 (en) | 1987-10-23 | 1987-10-23 | Method of forming ferromagnetic thin film |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01110715A JPH01110715A (en) | 1989-04-27 |
| JPH07120596B2 true JPH07120596B2 (en) | 1995-12-20 |
Family
ID=17463682
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62268818A Expired - Lifetime JPH07120596B2 (en) | 1987-10-23 | 1987-10-23 | Method of forming ferromagnetic thin film |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH07120596B2 (en) |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5633810A (en) * | 1979-08-29 | 1981-04-04 | Sony Corp | Preparation of magnetic recording medium |
| JPS60200887A (en) * | 1984-03-23 | 1985-10-11 | Nippon Sheet Glass Co Ltd | Manufacture of magnetic film |
| JPS60128606A (en) * | 1983-12-15 | 1985-07-09 | Seiko Instr & Electronics Ltd | Photo-magnetic recording medium |
-
1987
- 1987-10-23 JP JP62268818A patent/JPH07120596B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01110715A (en) | 1989-04-27 |
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