JPH0357536B2 - - Google Patents

Info

Publication number
JPH0357536B2
JPH0357536B2 JP57158323A JP15832382A JPH0357536B2 JP H0357536 B2 JPH0357536 B2 JP H0357536B2 JP 57158323 A JP57158323 A JP 57158323A JP 15832382 A JP15832382 A JP 15832382A JP H0357536 B2 JPH0357536 B2 JP H0357536B2
Authority
JP
Japan
Prior art keywords
film
concentration
grain interface
columnar crystal
medium
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
Application number
JP57158323A
Other languages
Japanese (ja)
Other versions
JPS5948823A (en
Inventor
Ryuji Sugita
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP57158323A priority Critical patent/JPS5948823A/en
Publication of JPS5948823A publication Critical patent/JPS5948823A/en
Publication of JPH0357536B2 publication Critical patent/JPH0357536B2/ja
Granted legal-status Critical Current

Links

Classifications

    • G—PHYSICS
    • G11—INFORMATION STORAGE
    • G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/62—Record carriers characterised by the selection of the material
    • G11B5/64—Record carriers characterised by the selection of the material comprising only the magnetic material without bonding agent
    • G11B5/65—Record carriers characterised by the selection of the material comprising only the magnetic material without bonding agent characterised by its composition
    • G11B5/656—Record carriers characterised by the selection of the material comprising only the magnetic material without bonding agent characterised by its composition containing Co

Landscapes

  • Magnetic Record Carriers (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 本発明は高密度記録特性の優れた、垂直磁気記
録用の媒体に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a medium for perpendicular magnetic recording that has excellent high-density recording characteristics.

従来例の構成とその問題点 短波長記録特性の優れた磁気記録方式として、
垂直磁気記録方式がある。この方式においては媒
体の膜面に略垂直方向が磁化容易軸である垂直磁
気記録媒体が必要となる。このような媒体に信号
を記録すると残留磁化は媒体の膜面に略垂直方向
を向き、従つて信号が短波長になる程媒体内反磁
界は減少し、優れた再生出力が得られる。垂直磁
気記録媒体は基板上にCoとCrを主成分とし膜面
に略垂直方向に磁化容易軸を有する磁性層(以下
この磁性層をCo−Cr垂直磁化膜と呼ぶ)を、一
般的にはスパツタリング法により形成したもので
ある。しかし、スパツタリング法は膜の形成速度
が遅く量産性が悪い。スパツタリング法に対し、
真空蒸着法(イオンプレーテイング法のように蒸
発原子の一部をイオン化して蒸着する方法も含
む)によれば、膜の形成速度は2桁以上高くな
り、量産性が向上する。本発明者は、真空蒸着法
にてもCo−Cr垂直磁化膜が得られることを見に
出したが、真空蒸着法により得られたCo−Cr膜
が電磁変換特性の優れた垂直磁化膜であるための
条件は見い出されていなかつた。
Conventional configuration and its problems As a magnetic recording system with excellent short wavelength recording characteristics,
There is a perpendicular magnetic recording method. This method requires a perpendicular magnetic recording medium whose axis of easy magnetization is approximately perpendicular to the film surface of the medium. When a signal is recorded on such a medium, the residual magnetization is oriented in a direction substantially perpendicular to the film surface of the medium. Therefore, the shorter the wavelength of the signal, the smaller the demagnetizing field within the medium, and excellent reproduction output can be obtained. Perpendicular magnetic recording media generally have a magnetic layer on a substrate, which is mainly composed of Co and Cr and has an axis of easy magnetization approximately perpendicular to the film surface (hereinafter this magnetic layer is referred to as a Co-Cr perpendicular magnetization film). It was formed by a sputtering method. However, the sputtering method has a slow film formation rate and is not suitable for mass production. In contrast to the sputtering method,
According to a vacuum evaporation method (including a method in which a portion of evaporated atoms are ionized and deposited, such as an ion plating method), the film formation rate is increased by more than two orders of magnitude, and mass productivity is improved. The present inventors have found that a Co-Cr perpendicular magnetization film can also be obtained by vacuum evaporation, and found that the Co-Cr film obtained by vacuum evaporation is a perpendicular magnetization film with excellent electromagnetic conversion characteristics. The conditions for this have not been found.

発明の目的 本発明は真空蒸着法により得られたCo−Cr膜
が電磁変換特性の優れた垂直磁化膜になるための
条件を与えることを目的とする。
OBJECTS OF THE INVENTION The object of the present invention is to provide conditions for a Co--Cr film obtained by vacuum evaporation to become a perpendicularly magnetized film with excellent electromagnetic conversion characteristics.

発明の構成 本発明は真空蒸着法により形成された柱状構造
をしているCo−Cr垂直磁化膜において、柱状結
晶粒の粒界面近傍にCrが偏析しており、粒界面
近傍領域におけるCr濃度が、この膜の平均のCr
濃度の1.7倍以上であることを特徴とするもので
ある。
Structure of the Invention The present invention provides that in a Co-Cr perpendicularly magnetized film having a columnar structure formed by vacuum evaporation, Cr is segregated near the grain interface of columnar crystal grains, and the Cr concentration in the region near the grain interface is , the average Cr of this film
It is characterized by having a concentration of 1.7 times or more.

実施例の説明 第1図〜第5図を用いて本発明を説明する。第
1図はCo−Cr蒸着膜の破断面の模式図である。
1は基板である。基板としては、アルミニウム板
や高分子材料より成るフイルム、あるいはこれら
の非磁性体の上にパーマロイ膜を形成したもの等
が用いられる。2はCo−Cr垂直磁化膜、3は柱
状結晶粒である。Co−Cr垂直磁化膜は、一般に
柱状結晶構造をしており、柱状結晶粒の粒径は膜
厚の1/10程度である。たとえば、膜厚1μmのCo
−Cr垂直磁化膜は約1000Åの粒径の柱状結晶粒
から構成されている。このような構造を有する
Co−Cr垂直磁化膜の磁気特性は、柱状結晶粒の
粒界面近傍におけるCrの備析量に、大きく依存
することが実験の結果明らかになつた。
DESCRIPTION OF EMBODIMENTS The present invention will be described with reference to FIGS. 1 to 5. FIG. 1 is a schematic diagram of a fractured surface of a Co--Cr vapor deposited film.
1 is a substrate. As the substrate, an aluminum plate, a film made of a polymer material, or a permalloy film formed on a non-magnetic material thereof is used. 2 is a Co--Cr perpendicular magnetization film, and 3 is a columnar crystal grain. A Co--Cr perpendicularly magnetized film generally has a columnar crystal structure, and the grain size of the columnar crystal grains is about 1/10 of the film thickness. For example, Co
The -Cr perpendicular magnetization film is composed of columnar crystal grains with a grain size of approximately 1000 Å. has a structure like this
Experiments have revealed that the magnetic properties of a Co-Cr perpendicularly magnetized film largely depend on the amount of Cr present near the grain interface of columnar grains.

第2図に柱状結晶粒の粒界面近傍にCrが偏析
しているCo−Cr垂直磁化膜の破断面の模式図を
示す。4はCrが偏析したCo−Cr垂直磁化膜、5
はCrが偏析した柱状結晶粒、6は柱状結晶粒の
粒界面近傍におけるCrの偏析している部分であ
る。なお、柱状結晶粒の粒界面とは、第3図の実
線7で示される部分のことであり、破線8の部分
は含まない。柱状結晶粒の粒界面近傍の組成は、
例えばオージエ電子分光分析等の方法により、調
べることができる。
FIG. 2 shows a schematic diagram of a fractured surface of a Co--Cr perpendicularly magnetized film in which Cr is segregated near the grain interface of columnar crystal grains. 4 is a Co-Cr perpendicular magnetization film in which Cr is segregated, 5
6 is a columnar crystal grain in which Cr is segregated, and 6 is a portion in which Cr is segregated near the grain interface of the columnar crystal grain. Note that the grain interface of columnar crystal grains refers to the portion indicated by the solid line 7 in FIG. 3, and does not include the portion indicated by the broken line 8. The composition near the grain interface of columnar grains is
For example, it can be investigated by methods such as Auger electron spectroscopy.

Co−Cr垂直磁化膜において、柱状結晶粒の粒
界面近傍の略10Åの厚みの領域におけるCr濃度
(Cr/(Co+Cr))と、膜全体の平均のCr濃度と
の比と、Mr⊥/Mrとの関係を第4図に示す。
ただし、Mr⊥は反磁場補正を行なつていない、
膜面に垂直方向の残留磁化であり、Mrは膜面
内の残留磁化である。第4図より、柱状結晶粒の
粒界面近傍の略10Åの厚みの領域におけるCr濃
度と、膜全体の平均のCr濃度との比が大きくな
るに従い、Mr⊥/Mrも大きくなり、比が1.7
以上になると1以上のMr⊥/Mrを有するCo
−Cr垂直磁化膜が得られることがわかる。
In a Co-Cr perpendicularly magnetized film, the ratio of the Cr concentration (Cr/(Co+Cr)) in a region approximately 10 Å thick near the grain interface of columnar grains to the average Cr concentration of the entire film, Mr⊥/Mr Figure 4 shows the relationship between
However, Mr⊥ is not demagnetically corrected,
This is the residual magnetization in the direction perpendicular to the film surface, and Mr is the residual magnetization within the film surface. From FIG. 4, as the ratio of the Cr concentration in the approximately 10 Å thick region near the grain interface of the columnar crystal grains to the average Cr concentration of the entire film increases, Mr⊥/Mr also increases, and the ratio becomes 1.7.
If it becomes more than 1, then Co with Mr⊥/Mr of 1 or more
It can be seen that a -Cr perpendicular magnetization film can be obtained.

Mr⊥/MrはCo−Cr垂直磁化膜に信号を記
録し再生した場合の特性(この特性を電磁変換特
性と言う)に、密接に関係している。第5図に公
知の補助磁極励磁型ヘツドで、Co−Cr垂直磁化
膜に100KFRPI(1インチ当たり磁化反転数が
100000回あるような、デイジタル記録の状態を
100KFRPIと言う)の信号を記録し、再生した際
の再生出力とMr⊥/Mrとの関係を示す。この
図から、Mr⊥/Mrが1未満になると再生出力
が大幅に低下してしまうことがわかる。この原因
はMr⊥/Mrが1以上であれば、信号を記録す
ると媒体内の残留磁化は、主に膜面に垂直方向を
向いており垂直記録された状態であるのに対し、
Mr⊥/Mrが1未満になると膜面内方向にも残
留磁化が向くようになり、一部面内記録のような
状態になつてしまうためだと思われる。以上、第
4図及び第5図の結果をまとめると、柱状結晶粒
の粒界面近傍の略10Åの厚みの領域におけるCr
濃度とCo−Cr垂直磁化膜全体の平均のCr濃度と
の比が1.7以上になると、膜のMr⊥/Mrが1
以上になり、優れた電磁変換特性が得られるとい
うことである。
Mr⊥/Mr is closely related to the characteristics when a signal is recorded and reproduced in a Co--Cr perpendicularly magnetized film (this characteristic is called electromagnetic conversion characteristic). Figure 5 shows a well-known auxiliary pole excitation type head with a Co-Cr perpendicular magnetization film of 100 KFRPI (the number of magnetization reversals per inch).
The state of digital records, like 100,000 times.
This shows the relationship between the playback output and Mr⊥/Mr when a signal of 100KFRPI is recorded and played back. From this figure, it can be seen that when Mr⊥/Mr becomes less than 1, the reproduction output decreases significantly. The reason for this is that if Mr⊥/Mr is greater than or equal to 1, when a signal is recorded, the residual magnetization in the medium is mainly oriented perpendicular to the film surface, resulting in perpendicular recording.
This is thought to be because when Mr⊥/Mr becomes less than 1, the residual magnetization also becomes oriented in the in-plane direction of the film, resulting in a state similar to in-plane recording. To summarize the results shown in Figures 4 and 5 above, Cr in the approximately 10 Å thick region near the grain interface of columnar grains
When the ratio of the concentration to the average Cr concentration of the entire Co-Cr perpendicularly magnetized film becomes 1.7 or more, Mr⊥/Mr of the film becomes 1.
This means that excellent electromagnetic conversion characteristics can be obtained.

以下に具体的な実施例の説明を行う。 A specific example will be explained below.

第1の実施例 第6図を用いて第1の実施例について説明す
る。9は膜厚50μmの耐熱性高分子材料より成る
フイルムであり、その上に膜厚1μmのパーマロイ
膜10、さらにその上に膜厚1μmのCo−Cr垂直
磁化膜11がいずれも真空蒸着法により形成され
いる。このCo−Cr垂直磁化膜の柱状結晶粒の粒
界面近傍の略10Åの厚みの領域におけるCr濃度
と、膜全体の平均のCr濃度との比は、オージエ
電子分光分析によれば2.1であり、Mr⊥/Mr
は2.3であつた。この媒体に補助磁極励磁型垂
直ヘツドで100KFRPIの信号を記録し再生する
と、従来のCo含有酸化鉄塗布型媒体に対し、
24dB高い出力が得られた。
First Example The first example will be described using FIG. 9 is a film made of a heat-resistant polymer material with a film thickness of 50 μm, on which a permalloy film 10 with a film thickness of 1 μm and a Co-Cr perpendicular magnetization film 11 with a film thickness of 1 μm are further formed on the film by vacuum evaporation. formed. According to Auger electron spectroscopy, the ratio of the Cr concentration in a region approximately 10 Å thick near the grain interface of the columnar crystal grains of this Co-Cr perpendicularly magnetized film to the average Cr concentration of the entire film is 2.1. Mr⊥/Mr
was 2.3. When a 100 KFRPI signal is recorded and reproduced on this medium using an auxiliary magnetic pole excitation type vertical head, it becomes
A 24dB higher output was obtained.

第2の実施例 第7図を用いて第2の実施例について説明す
る。Co−Cr垂直磁化膜11とパーマロイ膜10
との間に、膜厚400ÅにTi蒸着膜12が存在する
以外は、第1の実施例と殆ど同じ構造の媒体を作
製した。Ti蒸着膜はCo−Cr垂直磁化膜の配向性
を良くするために設けてある。この媒体における
Co−Cr膜の柱状結晶粒の粒界面近傍の略10Åの
厚みの領域におけるCr濃度を、膜全体の平均の
Cr濃度との比、及びMr⊥/Mrはそれぞれ2.0
及び2.4であつた。この媒体に補助磁極励磁型垂
直ヘツドで100KFRPIの信号を記録し再生する
と、従来のCo含有酸化鉄塗布型媒体に対し、
28dB高い出力が得られた。
Second Example A second example will be described using FIG. Co-Cr perpendicular magnetization film 11 and permalloy film 10
A medium having almost the same structure as the first example was fabricated, except that a Ti vapor deposited film 12 with a thickness of 400 Å was present between the two. The Ti vapor deposited film is provided to improve the orientation of the Co--Cr perpendicular magnetization film. in this medium
The Cr concentration in the approximately 10 Å thick region near the grain interface of the columnar grains of the Co-Cr film is calculated based on the average of the entire film.
The ratio to the Cr concentration and Mr⊥/Mr are each 2.0.
and 2.4. When a 100 KFRPI signal is recorded and reproduced on this medium using an auxiliary magnetic pole excitation type vertical head, it becomes
28dB higher output was obtained.

発明の効果 本発明によれば、電磁変換特性の非常に優れた
垂直磁気記録媒体を提供できる。
Effects of the Invention According to the present invention, a perpendicular magnetic recording medium with extremely excellent electromagnetic conversion characteristics can be provided.

【図面の簡単な説明】[Brief explanation of drawings]

第1図はCo−Cr蒸着膜の破断図、第2図は柱
状結晶粒の粒界面近傍にCrが偏析しているCo−
Cr垂直磁化膜の破断面の模式図、第3図は粒界
面を説明するための図、第4図は柱状結晶粒の粒
界面近傍の略10Åの厚みの領域におけるCr濃度
と磁性層の平均のCr濃度との比と、Mr⊥/Mr
との関係を示す図、第5図はMr⊥/Mrと再
生出力との関係を示す図、第6図及び第7図はそ
れぞれ本発明の第1、第2の実施例である垂直磁
気記録媒体の断面図である。 4……Crの偏析したCo−Cr垂直磁化膜、5…
…Crの偏析した柱状結晶粒、6……柱状結晶粒
の粒界面近傍におけるCrの偏析している部分、
7……結晶粒の粒界面。
Figure 1 is a broken view of a Co-Cr vapor deposited film, and Figure 2 is a Co-Cr-deposited film with Cr segregated near the grain interface of columnar grains.
A schematic diagram of the fracture surface of a perpendicularly magnetized Cr film. Figure 3 is a diagram for explaining the grain interface. Figure 4 shows the average Cr concentration and magnetic layer in a region approximately 10 Å thick near the grain interface of columnar crystal grains. and the ratio of Cr concentration to Mr⊥/Mr
FIG. 5 is a diagram showing the relationship between Mr FIG. 3 is a cross-sectional view of the medium. 4... Co-Cr perpendicular magnetization film with Cr segregation, 5...
... Columnar crystal grains with Cr segregated, 6... Parts where Cr is segregated near the grain interface of the columnar crystal grains,
7... Grain interface of crystal grains.

Claims (1)

【特許請求の範囲】[Claims] 1 基板上に膜面に略垂直方向に磁化容易軸を有
しCoとCrを主成分とする薄膜磁性層が形成され、
前記磁性層を構成している柱状結晶粒の粒界面近
傍にCrが偏析し、かつ、前記粒界面近傍領域に
おけるCr濃度が前記磁性層の平均のCr濃度の1.7
倍以上であることを特徴とする垂直磁気記録媒
体。
1. A thin magnetic layer containing Co and Cr as main components is formed on a substrate and has an axis of easy magnetization in a direction substantially perpendicular to the film surface,
Cr is segregated near the grain interface of the columnar crystal grains constituting the magnetic layer, and the Cr concentration in the region near the grain interface is 1.7 of the average Cr concentration of the magnetic layer.
A perpendicular magnetic recording medium characterized in that it is more than twice as large.
JP57158323A 1982-09-10 1982-09-10 perpendicular magnetic recording medium Granted JPS5948823A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57158323A JPS5948823A (en) 1982-09-10 1982-09-10 perpendicular magnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57158323A JPS5948823A (en) 1982-09-10 1982-09-10 perpendicular magnetic recording medium

Publications (2)

Publication Number Publication Date
JPS5948823A JPS5948823A (en) 1984-03-21
JPH0357536B2 true JPH0357536B2 (en) 1991-09-02

Family

ID=15669123

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57158323A Granted JPS5948823A (en) 1982-09-10 1982-09-10 perpendicular magnetic recording medium

Country Status (1)

Country Link
JP (1) JPS5948823A (en)

Also Published As

Publication number Publication date
JPS5948823A (en) 1984-03-21

Similar Documents

Publication Publication Date Title
JPH01158618A (en) Magnetic recording medium
US4621030A (en) Perpendicular magnetic recording medium and manufacturing method thereof
JPH09212855A (en) Magnetic recording medium, magnetic head, and magnetic recording / reproducing apparatus using the same
US4544591A (en) Perpendicular magnetic recording medium
JPH06105499B2 (en) Magnetic recording medium
JP2988188B2 (en) Magnetic recording medium and method of manufacturing the same
JPS6153769B2 (en)
JP4232564B2 (en) Perpendicular magnetic recording medium
JPS5868234A (en) Composite magnetic recording medium
JP2725502B2 (en) Magnetic recording media
JPS5948823A (en) perpendicular magnetic recording medium
JPS5975429A (en) perpendicular magnetic recording medium
JPH03178028A (en) Magnetic recording medium
JP2000215437A (en) Magnetic recording medium and magnetic recording device using the same
JP3203943B2 (en) Magnetic recording / reproducing device
JPS6184005A (en) Magnetic recording material
JPH0573877A (en) Magnetic recording medium
JPH0682442B2 (en) Magnetic recording method
JPH071535B2 (en) Magnetic recording medium
JPH01173312A (en) Magnetic recording medium
JPS61269226A (en) Production of vertical magnetic recording medium
JPS61220117A (en) Vertical magnetic recording medium and magnetic recording and reproducing method
JPS6216230A (en) Perpendicular magnetic recording medium and magnetic recording and reproducing method
JPH05159264A (en) Magnetic recording medium
JPH04206017A (en) Magnetic recording medium and its manufacturing method