JPS6057211B2 - Manufacturing method of magnetic recording media - Google Patents
Manufacturing method of magnetic recording mediaInfo
- Publication number
- JPS6057211B2 JPS6057211B2 JP7890477A JP7890477A JPS6057211B2 JP S6057211 B2 JPS6057211 B2 JP S6057211B2 JP 7890477 A JP7890477 A JP 7890477A JP 7890477 A JP7890477 A JP 7890477A JP S6057211 B2 JPS6057211 B2 JP S6057211B2
- Authority
- JP
- Japan
- Prior art keywords
- film
- magnetic
- manufacturing
- thin film
- magnetic recording
- 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
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- Thin Magnetic Films (AREA)
- Compounds Of Iron (AREA)
- Magnetic Record Carriers (AREA)
- Manufacturing Of Magnetic Record Carriers (AREA)
Description
【発明の詳細な説明】
本発明は、磁気ディスク装置などに用いる’高密度磁
気記録媒体の製作法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method of manufacturing a high-density magnetic recording medium used in a magnetic disk device or the like.
磁気記録装置では高密度記録が1つの重要な問題であ
り、そして高密度記録には記録媒体の厚みを薄くし、保
磁力Hcを大にすることが必要である。High-density recording is an important issue in magnetic recording devices, and high-density recording requires reducing the thickness of the recording medium and increasing the coercive force Hc.
磁気ディスクでは媒体形成には塗布つまり円盤上にγF
e。O。の微粒子とバインダーとの混合物を塗布して磁
性膜を作る方式が広く用いられている。しかしこの方法
ではバインダーがあるので薄膜化に限度があり、0.5
〜0.7μm以下にするのは難しい。媒体形成にはこの
他に、反応スパッタ法、反応蒸着法、CD(Chemi
calDeposition)法、CVD(Che−m
icalVaporedDeposition)法など
があり、これらの方法によると更に薄い連続媒体薄膜の
形成が可能であり、例えば前者のスパッタ法、蒸着法な
どでは0.05μm程度、実用的には0.15μmのも
のが得られる。 しかしながら、かゝる磁気記録媒体薄
膜を従来J法で作ると、その製造工程および得られる媒
体の磁気特性に種々難点がある。例えば前述の反応スパ
ッタ法では、10−゜Torr程度の酸素を含むアルゴ
ンガス雰囲気中で鉄(Fe)をスパッタして基板にα−
Fe2O3非磁性膜を被着し、この膜を還元してFe3
O4(マグネタイト)磁性膜を作るが、この還元工程の
温度マージンが狭く、還元温度も高く、しかも保磁力お
よび角形比も比較的小さいという欠点がある。本発明は
か)る点を改善しようとするもので、鉄(Fe)に銅(
Cu)およびコバルト(CO)、それにマンガン(Mn
)、ニッケル(Ni)、アルミニウム(Ae)、亜鉛(
Zn)、ジルコニウム(Zr)、錫(Sn)、タンタル
(Ta)の1つ以上を添加してなる鉄合金を用いて反応
スパッタ法などにより膜厚1μm以下のα−Fe2O3
膜形成を行なうことを特徴とするものである。In magnetic disks, γF is applied on the disk to form the medium.
e. O. A widely used method is to make a magnetic film by coating a mixture of fine particles and a binder. However, since this method requires a binder, there is a limit to how thin the film can be made;
It is difficult to reduce the thickness to 0.7 μm or less. Other methods for forming the medium include reactive sputtering, reactive vapor deposition, and CD (chemistry).
calDeposition) method, CVD (Che-m
These methods allow the formation of even thinner continuous medium thin films. For example, the former sputtering method and vapor deposition method can yield a thin film of about 0.05 μm, and practically 0.15 μm. It will be done. However, when such a magnetic recording medium thin film is manufactured by the conventional J method, there are various difficulties in the manufacturing process and the magnetic properties of the resulting medium. For example, in the above-mentioned reactive sputtering method, iron (Fe) is sputtered onto a substrate in an argon gas atmosphere containing oxygen at about 10-° Torr.
A Fe2O3 nonmagnetic film is deposited, and this film is reduced to form Fe3.
Although an O4 (magnetite) magnetic film is produced, there are disadvantages in that the temperature margin of this reduction process is narrow, the reduction temperature is high, and the coercive force and squareness ratio are also relatively small. The present invention is an attempt to improve this point.
Cu) and cobalt (CO), and manganese (Mn
), nickel (Ni), aluminum (Ae), zinc (
Using an iron alloy containing one or more of Zn), zirconium (Zr), tin (Sn), and tantalum (Ta), α-Fe2O3 with a film thickness of 1 μm or less is formed by reactive sputtering or the like.
It is characterized by forming a film.
こうして得られたα一Fe2O3膜を還元してFe3O
4膜にすると高保磁力の磁性膜が得られ、しかもその還
元工程の所要温度が低くかつ許容温度範囲が広いので基
板に悪影響を与えず、還元処理が容易であり、高い歩留
りが得られる。更にこのFe3O4高保磁力膜を空気中
で熱処理すると酸化してγ−Fe2O3膜になり、これ
は基板との密着性がよくかつ角型比も従来法ではOゐ程
度てあるのに対しO名程度と高くなる。次に実施例を参
照しながらこれを詳細に説明する。第1図はα−Fe2
O3からFe3O4への還元工程の温度対電気抵抗の関
係を示す。曲線C1は無添加のFeをターゲットとして
02−N混合ガス中で反応スパッタリンク几てアルミニ
ウム基板上にα−Fe2O,膜を作り、水蒸気を含む水
素ガス中でこれを還元した場合、また曲線C2は3%(
重量%、以下同じ)Mnl2%Cu、2%COを含むF
e合金をターゲットとして同じ条件で反応スパッタリン
グし、かつ生成したα−Fe2O3膜を還元した楊合の
還元温度対電気抵抗特性である。点線間の1σ〜104
Ω−Cmの範囲がFe3O4の領域であり、101Ω−
Cm以上の範囲(まα−Fe2O3の領域、1σΩ−C
m以の範囲はFeの領域である。これらの曲線Cl,.
C2から明らかなように、無添加Fe使用の場合は還元
温度マージンは280〜325℃と非常に狭く、これ以
下の温度ては非磁性かつ絶縁性のα−Fe2O3のま)
てあり、これ以上の温度では単なるFe金属になつてし
まう。熱処理温度の許容変動範囲が,約50℃というの
は実際には可成り厳しく、精密な温度制御を必要とする
。これに対して曲線C2のFe−Mn−Cu−CO合金
使用の場合は還元温度マージンは200〜375℃に拡
大し、温度管理が容易である。またこのグラフから明ら
かなように上記鉄合金使用の場合は還元温度が低く、即
ち無添加Feの場合は300℃程度であるのに対して、
200℃程度でもよくなり、これは大きな利点である。The α-Fe2O3 film thus obtained is reduced to form Fe3O
By using four films, a magnetic film with high coercive force can be obtained, and since the required temperature for the reduction process is low and the allowable temperature range is wide, it does not adversely affect the substrate, the reduction process is easy, and a high yield can be obtained. Furthermore, when this Fe3O4 high coercive force film is heat-treated in air, it oxidizes and becomes a γ-Fe2O3 film, which has good adhesion to the substrate and a squareness ratio of about O2, compared to about O2 in the conventional method. It becomes high. Next, this will be explained in detail with reference to examples. Figure 1 shows α-Fe2
The relationship between temperature and electrical resistance in the reduction process from O3 to Fe3O4 is shown. Curve C1 shows the case where an α-Fe2O film is formed on an aluminum substrate by reaction sputtering in 02-N mixed gas using additive-free Fe as a target, and this is reduced in hydrogen gas containing water vapor, and curve C2 is 3% (
(wt%, same hereinafter) F containing Mnl2%Cu, 2%CO
This is the reduction temperature vs. electrical resistance characteristic of Yanghe, which was subjected to reactive sputtering using e-alloy as a target under the same conditions and the resulting α-Fe2O3 film was reduced. 1σ~104 between dotted lines
The range of Ω-Cm is the Fe3O4 region, and 101Ω-
Cm or more range (α-Fe2O3 region, 1σΩ-C
The range after m is the Fe region. These curves Cl, .
As is clear from C2, when additive-free Fe is used, the reduction temperature margin is extremely narrow at 280 to 325°C; at temperatures below this, nonmagnetic and insulating α-Fe2O3 remains).
At temperatures higher than this, it becomes mere Fe metal. The allowable variation range of heat treatment temperature of about 50° C. is actually quite strict and requires precise temperature control. On the other hand, in the case of using the Fe-Mn-Cu-CO alloy of curve C2, the reduction temperature margin is expanded to 200 to 375°C, and temperature control is easy. Also, as is clear from this graph, the reduction temperature is low when using the above iron alloy, that is, about 300°C when using Fe without additives.
A temperature of about 200° C. is sufficient, which is a great advantage.
即ち熱処理温度が300℃を越えると大面積のアルミニ
ウム基板では円板に反りが発生して磁気ヘッドが媒体か
ら一定の間隔を保つてトラック追跡することができなく
なるので、還元処理温度は300℃以下でノよいことが
望ましい。この点、上記鉄合金の場合200℃程度でよ
いということは極めて好ましいことであり、媒体基板に
アルミニウムの使用を可能にし、還元温度マージンが広
いという特徴と相俟つてこれに所定の良好な特性の磁性
薄膜を確実に被着することができる。こ)で実施例を挙
げると、3%Mnl2%CUl2%COを含む鉄合金タ
ーゲットを用い、50%02一50%N混合ガス中で反
応スパッタし、アルマイト処理をしたアルミニウム基板
上にα−Fe2O3・薄膜を形成した。That is, if the heat treatment temperature exceeds 300°C, the disk of a large-area aluminum substrate will warp, making it impossible for the magnetic head to keep track of the medium at a constant distance, so the reduction treatment temperature should be below 300°C. It is desirable that it be good. In this respect, it is extremely preferable that the temperature for the above-mentioned iron alloys is around 200°C, which makes it possible to use aluminum for the media substrate, and together with the feature of a wide reduction temperature margin, this makes it possible to achieve certain good properties. magnetic thin film can be reliably deposited. In this example, an iron alloy target containing 3% Mnl, 2% CUl, 2% CO was used, reactive sputtering was performed in a 50% 02-50% N mixed gas, and α-Fe2O3 was deposited on an alumite-treated aluminum substrate.・A thin film was formed.
その後水分を含んだ水素ガス雰囲気中で250′C1約
1時間還元を行ない、高保磁力のFe3O4膜を得た。
このFe3α膜を空気中300℃で熱処理し、保磁力7
000e、角型比0.8の、基板と密着性のよい良磁気
特性のγ−Fe2O3膜を得た。添加物のうちコバルト
(CO)は、保磁力の改善に役立つ。Thereafter, 250'C1 reduction was carried out for about 1 hour in a hydrogen gas atmosphere containing moisture to obtain a Fe3O4 film with high coercive force.
This Fe3α film was heat-treated in air at 300°C, and the coercive force was 7.
A γ-Fe2O3 film having a squareness ratio of 0.000e and a squareness ratio of 0.8 and good magnetic properties with good adhesion to the substrate was obtained. Among the additives, cobalt (CO) is useful for improving coercive force.
3%Mn−2%Cu−X%CO鉄合を用いた場合のCO
添加量と保磁力Hcとの関係を第2図の曲線C1に示す
。CO when using 3%Mn-2%Cu-X%CO iron alloy
The relationship between the amount added and the coercive force Hc is shown in the curve C1 in FIG.
この図に示すようにCOが零つまり無添加てあるとFe
3O4膜のHcは3500e程度であるのに対し、CO
を10%添加するとHcは19000e近くにもなり、
この間HcはほS゛直線状に増加する。Mnの代りにN
i.sAeNZn..Zr..Sn..Taを加えても
同様な結果が得られる。As shown in this figure, when CO is zero or no addition is made, Fe
The Hc of the 3O4 film is about 3500e, while the CO
When 10% of is added, Hc becomes nearly 19000e,
During this period, Hc increases almost linearly with S. N instead of Mn
i. sAeNZn. .. Zr. .. Sn. .. Similar results can be obtained by adding Ta.
第1図の曲線C3は3%Zn、2%Cu、2%COを含
むFe合金を、第3図曲線C2は3%N1、2%CUl
2%COを含むFe合金を、同図の曲線C3は3%Sn
l2%CUl2%COを含むFe合金を、第5図の曲線
C3は3%Ta、2%CUl2%COを含むFe合金を
、同図の曲線C2は3%Zrl2%CUl2%COを含
むFe合金を、そして第7図の曲線C2は3%Afl2
%CUl2%COを含むFe合金をそれぞれターゲット
として反応スパッタリングを行ない、得られたα−Fe
2O3を還元した場合のの還元温度一電気抵抗特性を示
す。また第2図の曲線C2は3%Znl2%CuにCO
を0〜10%の範囲で添加したCO合金を用いた場合の
添加量に対する保磁力Hcの変化を示し、同様に第4図
の曲線C1は3%Nil2%Cuにおける、同図の曲線
C2は3%Snl2%Cuにおける、また第6図の曲線
C1は3%Zrl2%Cuにおける、同図の曲線C2は
3%Tal2%Cuにおける、そして第8図の曲線C1
は3%Af、2%CuにおけるCO添加量に対するHc
の変化を示す。Curve C3 in Figure 1 is for Fe alloy containing 3% Zn, 2% Cu, 2% CO, and curve C2 in Figure 3 is for Fe alloy containing 3% N1, 2% CUL.
Curve C3 in the same figure shows Fe alloy containing 2% CO and 3% Sn.
Curve C3 in Figure 5 is for an Fe alloy containing 3% Ta, 2% CUl2% CO, and curve C2 in the same figure is for an Fe alloy containing 3% Zrl2% CUl2% CO. , and the curve C2 in Figure 7 is 3% Afl2
The α-Fe
The reduction temperature-electrical resistance characteristics when 2O3 is reduced are shown. In addition, curve C2 in Figure 2 shows CO2 in 3%Znl2%Cu.
It shows the change in coercive force Hc with respect to the amount of CO added in the range of 0 to 10%. Similarly, curve C1 in FIG. 3%Snl2%Cu, and curve C1 in FIG. 6 is at 3%Zrl2%Cu, curve C2 in the same figure is at 3%Tal2%Cu, and curve C1 in FIG.
is Hc relative to the amount of CO added at 3% Af and 2% Cu.
shows the change in
Nlnの代りに前記のNi.Ae・・・・ ・・・・を
添加した鉄合金ターゲットを用いる場合も、Mnを用い
た場合と同様にしてFe3O4膜、更にはγ−Fe2O
3膜を作ることができる。In place of Nln, the above Ni. Even when using an iron alloy target added with Ae......, Fe3O4 film or even γ-Fe2O is formed in the same way as when using Mn.
3 membranes can be made.
各場合につき、Cu..COはいずれも2%、Ni.A
′、Zn..Zr..Sn..Taはいずれも3%とし
、Mnの場合の実施例と同じ条件でγ−Fe2O3膜を
得た所、該膜のHcはZrlzn..Ae..Niの場
合が7000e..Taの場合が7500esSnの場
合が6500eとなり、角型比はいずれも0.8てあつ
た。添加物中、Cu!1Mn.Ni・・・ ・・・・等
と共に還元性の改善に寄与している。In each case, Cu. .. CO was 2% in both cases, Ni. A
', Zn. .. Zr. .. Sn. .. A γ-Fe2O3 film was obtained under the same conditions as in the example for Mn, with Ta being 3% in each case, and the Hc of the film was Zrlzn. .. Ae. .. In the case of Ni, it is 7000e. .. In the case of Ta, the value was 7500es, and in the case of Sn, it was 6500e, and the squareness ratio was 0.8 in both cases. Among the additives, Cu! 1Mn. Together with Ni... etc., it contributes to the improvement of reducibility.
この点COは専らHcの改善に役立つており、これが2
%もあれば7000e程度の目標のHcが得られる。添
加物、特に非磁性添加物は多量に入ると磁性を損なうの
で余り多量にするのは好ましくない。そこでCUlおよ
びCOlならびにNi..MnlZnlAe..Zr.
.Sn..Taは0.1〜10%の範囲、好ましくは前
記実施例のようにCUNCOが2%、Ni..Mn・・
・・ ・・・・が3%の範囲でFeに混合するのがよい
。Ni,.Mn・・ ・・・・等は単独で又は2種以
上混合して用いてもよい。N1、Mn..Znは1〜5
%の範囲でまたA′、ZnlSn.Taは1〜4%の範
囲て混入すれば角型比Br/Bsは0.7以上になる。
10%を越えるとAe2O3、ZrO2、SnO2、T
a2O5の析出物がフェライト中に生成し、磁気特性が
劣化する。In this respect, CO is exclusively useful for improving Hc, and this
%, the target Hc of about 7000e can be obtained. Additives, especially non-magnetic additives, impair magnetism if added in large amounts, so it is not preferable to use too large amounts. Therefore, CUl and COl and Ni. .. MnlZnlAe. .. Zr.
.. Sn. .. Ta is in the range of 0.1 to 10%, preferably CUNCO is 2% as in the previous example, Ni. .. Mn...
... is preferably mixed with Fe in a range of 3%. Ni,. Mn, etc. may be used alone or in combination of two or more. N1, Mn. .. Zn is 1 to 5
% and A', ZnlSn. If Ta is mixed in a range of 1 to 4%, the squareness ratio Br/Bs will be 0.7 or more.
If it exceeds 10%, Ae2O3, ZrO2, SnO2, T
Precipitates of a2O5 are formed in the ferrite, deteriorating the magnetic properties.
第9図および第10図は添加物Ae.zrlSn.Ta
およびMn.Ni..Znの量に対する残留磁気Brの
変化を、また第11図および第12図は添加物Ae..
Zr..Sn..Taの量に対する角型比(Br/Bs
)の変化を示す。Figures 9 and 10 show additive Ae. zrlSn. Ta
and Mn. Ni. .. FIGS. 11 and 12 show the change in remanence Br with respect to the amount of Zn, and FIGS. ..
Zr. .. Sn. .. Squareness ratio (Br/Bs
).
以上詳細に説明したように本発明によれば、極めて薄い
、かつ良好な保磁力および角型比の磁性薄膜を容易に歩
留りよく作ることができ、高密度記録用媒体として優れ
た媒体を廉価に提供することができる。As explained in detail above, according to the present invention, an extremely thin magnetic thin film with good coercive force and squareness ratio can be easily produced with good yield, and a medium excellent as a high-density recording medium can be produced at a low cost. can be provided.
易図面の簡単な説明
第1図、第3図、第5図、第7図は還元温度に対する電
気抵抗の変化を示すグラフ、第2図、第4図、第6図、
第8図はCO添加による保磁力の変化を示すグラフで、
いずれも本発明の効果を示・す。Brief explanation of the drawings Figures 1, 3, 5, and 7 are graphs showing changes in electrical resistance with respect to reduction temperature, Figures 2, 4, 6,
Figure 8 is a graph showing the change in coercive force due to CO addition.
All of them show the effects of the present invention.
Claims (1)
ウム、亜鉛、ジルコニウム、錫、タンタルのうちの1つ
以上とを含む鉄合金を用いて基板に膜厚1μm以下のα
−Fe_2O_3の薄膜を作り、該薄膜を還元してFe
_3O_4の磁性膜とすることを特徴とする、磁気記録
媒体の製作法。 2 α−Fe_2O_3の薄膜を、酸素アルゴンガス雰
囲気中で鉄合金を反応スパッタリングすることにより基
板に被着形成することを特徴とした特許請求の範囲第1
項記載の磁気記録媒体の製作法。 3 銅と、コバルトと、マンガン、ニッケル、アルミニ
ウム、亜鉛、ジルコニウム、錫、タンタルのうちの1つ
以上とを含む鉄合金を用いて基板に膜厚1μm以下のα
−Fe_2O_3の薄膜を作り、該薄膜を還元してFe
_3O_4磁性膜としたのち、該Fe_3O_4磁性膜
をさらに酸化してγ−Fe_2O_3とすることを特徴
とする磁気記録媒体の製作法。 4 α−Fe_2O_3の薄膜を、酸素アルゴンガス雰
囲気中で鉄合金を反応スパッタリングすることにより基
板に被着形成することを特徴とした特許請求の範囲第3
項記載の磁気記録媒体の製作法。 [Claims] 1. An iron alloy containing copper, cobalt, and one or more of manganese, nickel, aluminum, zinc, zirconium, tin, and tantalum is used to coat a substrate with a film thickness of 1 μm or less.
-Create a thin film of Fe_2O_3 and reduce the thin film to make Fe_2O_3
A method for manufacturing a magnetic recording medium, characterized by forming a magnetic film of _3O_4. 2. Claim 1, characterized in that a thin film of α-Fe_2O_3 is formed on a substrate by reactive sputtering of an iron alloy in an oxygen-argon gas atmosphere.
2. Method for manufacturing the magnetic recording medium described in Section 1. 3. α film thickness of 1 μm or less is applied to the substrate using an iron alloy containing copper, cobalt, and one or more of manganese, nickel, aluminum, zinc, zirconium, tin, and tantalum.
-Create a thin film of Fe_2O_3 and reduce the thin film to make Fe_2O_3
A method for manufacturing a magnetic recording medium, which comprises forming a Fe_3O_4 magnetic film and then further oxidizing the Fe_3O_4 magnetic film to form γ-Fe_2O_3. 4. Claim 3, characterized in that a thin film of α-Fe_2O_3 is deposited on a substrate by reactive sputtering of an iron alloy in an oxygen-argon gas atmosphere.
2. Method for manufacturing the magnetic recording medium described in Section 1.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7890477A JPS6057211B2 (en) | 1977-07-01 | 1977-07-01 | Manufacturing method of magnetic recording media |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7890477A JPS6057211B2 (en) | 1977-07-01 | 1977-07-01 | Manufacturing method of magnetic recording media |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5413995A JPS5413995A (en) | 1979-02-01 |
| JPS6057211B2 true JPS6057211B2 (en) | 1985-12-13 |
Family
ID=13674806
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7890477A Expired JPS6057211B2 (en) | 1977-07-01 | 1977-07-01 | Manufacturing method of magnetic recording media |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6057211B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6016109U (en) * | 1983-07-11 | 1985-02-02 | 日本電気株式会社 | Optical semiconductor device equipped with optical fiber |
-
1977
- 1977-07-01 JP JP7890477A patent/JPS6057211B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5413995A (en) | 1979-02-01 |
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