JPH0159643B2 - - Google Patents

Info

Publication number
JPH0159643B2
JPH0159643B2 JP3749881A JP3749881A JPH0159643B2 JP H0159643 B2 JPH0159643 B2 JP H0159643B2 JP 3749881 A JP3749881 A JP 3749881A JP 3749881 A JP3749881 A JP 3749881A JP H0159643 B2 JPH0159643 B2 JP H0159643B2
Authority
JP
Japan
Prior art keywords
head
magnetic
plane
tape
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
Application number
JP3749881A
Other languages
Japanese (ja)
Other versions
JPS57169915A (en
Inventor
Takeshi Takahashi
Kyoshi Sasaki
Akio Kuroe
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 JP3749881A priority Critical patent/JPS57169915A/en
Publication of JPS57169915A publication Critical patent/JPS57169915A/en
Publication of JPH0159643B2 publication Critical patent/JPH0159643B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/133Structure or manufacture of heads, e.g. inductive with cores composed of particles, e.g. with dust cores, with ferrite cores with cores composed of isolated magnetic particles

Landscapes

  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Magnetic Heads (AREA)

Description

【発明の詳細な説明】 本発明はビデオテープレコーダ(VTR)等の
磁気記録再生装置に関するもので、磁性蒸着薄膜
層を有する記録媒体と単結晶フエライトよりなる
磁気ヘツドを用いることにより従来装置より極め
て小型で高性能な磁気記録再生装置を提案するも
のである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic recording/reproducing device such as a video tape recorder (VTR), which uses a recording medium having a magnetic vapor-deposited thin film layer and a magnetic head made of single crystal ferrite, thereby achieving an improved performance that is far superior to conventional devices. This paper proposes a compact and high-performance magnetic recording/reproducing device.

最近の磁気記録分野における記録の高密度化に
対する要求は極めて強く、この要求に応じるため
に記録媒体の高抗磁力(HC)化、高残留磁束密
度(Br)化と同時に磁気ヘツドの高感度化を目
ざし種々の対策がなされてきている。例えば
VTRにおけるビデオテープではγ−Fe2O3(Hc=
300Oe、Br=900ガウス)からCrO2(Hc=510Oe、
Br=1300ガウス)、更にはCo系酸化鉄テープ
(Hc=670Oe、Br=1400ガウス)へと移行してき
ており、又、ビデオヘツドにおいては、コア材
料・構造・製造方法の最適化により特に短波長領
域での感度が飛躍的に向上してきている。特に最
近家庭用VTR等に幅広く用いられている単結晶
フエライトの場合はその結晶方位を磁気コアとし
てどのように配置するかによつてヘツド−テープ
系の特性が大きく左右される。
In recent years, there has been an extremely strong demand for higher recording densities in the field of magnetic recording, and in order to meet this demand, recording media have been made to have high coercive force (HC) and residual magnetic flux density (Br), and at the same time, magnetic heads have been made to have high sensitivity. Various measures have been taken to achieve this goal. for example
For videotape in VTR, γ−Fe 2 O 3 (Hc=
300Oe, Br=900 Gauss) to CrO2 (Hc=510Oe,
Br = 1300 Gauss), and further to Co-based iron oxide tape (Hc = 670 Oe, Br = 1400 Gauss), and in video heads, optimization of the core material, structure, and manufacturing method has made it particularly short. Sensitivity in the wavelength region has improved dramatically. In particular, in the case of single-crystal ferrite, which has recently been widely used in household VTRs, etc., the characteristics of the head-tape system are greatly influenced by the crystal orientation and how the magnetic core is arranged.

従来は、第1図に示すようにヘツドギヤツプ3
を挾む2個の単結晶フエライトよりなるヘツドコ
ア1,1aの各テープとの摺動面2,2aを
{211}面(ここで、{211}面とは211、121、112、
211、211、211、121、121、121、11
2、112、112、211、211、211、1
21、121、121、112、112、11
2、211、121、112の24通りの面を総称
したものである。)とし、ヘツドギヤツプ形成面
5,5aを{111}面(ここで、{111}面とは、
111、111、111、111、111、111、
111、111の8通りの面を総称したものであ
る。)で構成するとともに、主磁路構成面の
{110}面(ここで、{110}面とは、110、101、
011、110、101、101、110、110、0
11、011、101、011の12通りの面を総称し
たものである。)内の<110>軸(ここで、<110>
軸とは110、101、011、110、101、101、1
10、110、011、011、101、011の12
通りの軸を総称したものである。)が左右のコア
1,1aでギヤツプ形成面5,5aに対して対称
で、かつ、前記ギヤツプに向かつてテープとの摺
動方向となす角度θ=35.3゜になるよう“ハ”の
字形に配置することにより最も良好な特性を得て
いる。
Conventionally, as shown in Fig. 1, the head gap 3
The sliding surfaces 2, 2a of the head cores 1, 1a made of two single-crystal ferrite sandwiching each tape are {211} planes (here, {211} planes are 211, 121, 112,
211, 211, 211, 121, 121, 121, 11
2, 112, 112, 211, 211, 211, 1
21, 121, 121, 112, 112, 11
It is a general term for 24 types of surfaces: 2, 211, 121, and 112. ), and the head gap forming surfaces 5, 5a are {111} planes (here, {111} planes are
111, 111, 111, 111, 111, 111,
111, 111 is a general term for eight types of surfaces. ), and the {110} plane of the main magnetic path configuration plane (here, the {110} plane means 110, 101,
011, 110, 101, 101, 110, 110, 0
It is a general term for 12 types of faces: 11, 011, 101, and 011. ) in the <110> axis (here, <110>
The axes are 110, 101, 011, 110, 101, 101, 1
10, 110, 011, 011, 101, 011 12
It is a general term for the axis of a street. ) is symmetrical with respect to the gap forming surfaces 5, 5a on the left and right cores 1, 1a, and is shaped like a "C" so that the angle θ between the gap and the sliding direction with the tape is 35.3°. The best characteristics are obtained by this arrangement.

最近の家庭用VTRにおいてはCo系酸化鉄テー
プと上述のような高感度のビデオヘツドを用いて
最短波長1μm程度を実用化して小型で高性能な
VTRを得ている。しかし、この分野における高
密度化の波はこれにとどまらず、更に軽量・小型
化が要求されており、最終的にはカメラとの1体
化が望まれている。これに応える為には第1にビ
デオヘツドを内蔵するシリンダーの径を小さくす
る必要があり、その結果例えば最短波長は0.6μm
程度を実用化する必要がある。又、狭トラツク化
により面積密度を上げることも必要になる。その
結果、再生出力は大幅に低下し現状のテープ−ヘ
ツド系では対応ができなくなる。そこで、更に高
Hc、高Brの磁気テープの開発が急がれている
が、その1つとして合金粉末テープの実用が考え
られている。このテープは通常Hcが1000〜
1400Oe程度Brが2000〜3500ガウス程度である為
超高密度記録が可能であるが、フエライトヘツド
では記録時にコアの飽和現象を生じ、充分にその
特性を発揮させることが出来ず、一方センダスト
等の金属強磁性材料をコア材としたヘツドを使用
すれば記録における問題点は解消されるが、再生
効率・耐摩耗性・製造のし易さ・コスト等の点で
フエライトヘツドに劣るのが現状である。
Recent home-use VTRs use Co-based iron oxide tape and the above-mentioned high-sensitivity video heads to achieve a minimum wavelength of about 1 μm, making them compact and high-performance.
I'm getting a VTR. However, the wave of higher density in this field does not stop there; there is also a demand for further reduction in weight and size, and ultimately there is a desire for integration with a camera. In order to meet this demand, it is first necessary to reduce the diameter of the cylinder that houses the video head, and as a result, the shortest wavelength is, for example, 0.6 μm.
It is necessary to put this degree into practical use. It is also necessary to increase the area density by narrowing the track. As a result, the reproduction output decreases significantly, and current tape-head systems cannot cope with this problem. Therefore, even higher
There is an urgent need to develop magnetic tapes with high Hc and high Br, and the practical use of alloy powder tapes is being considered as one of them. This tape usually has an Hc of 1000~
Ultra-high density recording is possible because the Br of about 1400 Oe is about 2000 to 3500 Gauss, but with ferrite heads, the core saturates during recording and cannot fully demonstrate its characteristics. Although recording problems can be solved by using a head with a metal ferromagnetic material as the core material, it is currently inferior to a ferrite head in terms of playback efficiency, wear resistance, ease of manufacture, cost, etc. be.

これに対し、我々が提案するものは磁性薄膜テ
ープを用いてフエライトヘツドで記録再生を行な
うというものである。薄膜テープは数μmないし
は10数μm程度の薄いプラスチツク・フイルム・
ベースにCo、Co−Ni、Co−Cr、Fe系等の磁性
体を真空蒸着あるいはスパツタリングすることに
より数100Åないしは数1000Å程度の薄膜を作成
したもので、一例をあげればHc800〜1000
〔Oe〕Br6000〔G〕程度のものが得られている。
In contrast, what we propose is to use a magnetic thin film tape for recording and reproduction with a ferrite head. Thin film tape is a thin plastic film of several micrometers or 10-odd micrometers.
A thin film of several 100 Å to several 1000 Å is created by vacuum evaporating or sputtering a magnetic material such as Co, Co-Ni, Co-Cr, or Fe based on a base.
[Oe] About Br6000 [G] has been obtained.

このように磁性薄膜テープはHc、Br共に前記
背景による短波長化に充分応じることが可能な値
を有すると同時に磁性層が極めて薄い為にフエラ
イトヘツドでも充分記録が可能でその高性能な特
性を発揮させることができる。
In this way, the magnetic thin film tape has both Hc and Br values that are sufficient to respond to the shortening of wavelength due to the above-mentioned background, and at the same time, since the magnetic layer is extremely thin, sufficient recording is possible even with a ferrite head, and its high performance characteristics can be achieved. It can be demonstrated.

一方、磁性薄膜の表面性は極めて滑らかな為、
ヘツド摩耗に関してはほとんど問題ないが、滑ら
かな故にヘツド表面に複雑な面荒れ現象を生じ
る。
On the other hand, since the surface properties of magnetic thin films are extremely smooth,
There is almost no problem with head wear, but because the head is smooth, a complicated surface roughness phenomenon occurs on the head surface.

第2図aは、第1図に示す従来タイプのヘツド
に対して、真空蒸着法により形成されたCo−Ni
系の磁性層を有する磁気記録媒体を相対速度3.75
m/secで一時間摺動させた場合のヘツド表面の
面荒れ状態を示すものであり、第2図bは同様に
θ=90゜のタイプのヘツド表面の面荒れ状態を示
したものである。また、第3図aは第2図aに示
すヘツドのテープ入側コア1の摺動面2の表面粗
さを示し、第3図bは第2図aに示すヘツドのテ
ープ出側コア1′の摺動面2aの表面粗さを示し、
第3図cは第2図bに示すヘツドのテープ出側コ
ア1′の摺動面2aの表面粗さを示す、それぞれ
の表面粗さは、記録媒体の摺動方向と直角な方向
に測定している。第3図bの場合は表面粗さで約
400〜500Åと大きく第3図a,cの場合に比して
約1桁大きい。このように表面荒れの現象は第1
図における<110軸>の傾きθと相関を有してお
り、この関係を第4図に示す。θ=0゜、90゜ある
いはこれらの近傍の場合テープの走行方向には関
係なく面荒れは生じないが、20〜70゜のの範囲で
は状態に差はあるものの面荒れ現象を生じ、前述
したように<110軸>とテープ走行方向との交錯
のし方によつて大きく異なる。この様な面荒れが
生じた場合、ヘツドギヤツプ部での面荒れに起因
する凹凸によりヘツドギヤツプと磁気記録媒体の
間でスペーシングロスが生じ、短波長出力が著る
しく劣化するとともにヘツド出力のエンベロープ
形状も影響を受けてSN比が悪くなるという問題
が発生する。
Figure 2a shows a Co-Ni head formed by vacuum evaporation in contrast to the conventional head shown in Figure 1.
A magnetic recording medium with a magnetic layer of the system at a relative speed of 3.75
This shows the surface roughness of the head when it is slid at m/sec for one hour, and Figure 2b also shows the roughness of the head surface of the type where θ=90°. . 3a shows the surface roughness of the sliding surface 2 of the tape inlet core 1 of the head shown in FIG. 2a, and FIG. 3b shows the surface roughness of the tape outlet core 1 of the head shown in FIG. 2a. ' indicates the surface roughness of the sliding surface 2a,
Figure 3c shows the surface roughness of the sliding surface 2a of the tape exit core 1' of the head shown in Figure 2b. Each surface roughness is measured in a direction perpendicular to the sliding direction of the recording medium. are doing. In the case of Figure 3b, the surface roughness is approximately
It is 400 to 500 Å, which is approximately one order of magnitude larger than the cases shown in Figures 3a and 3c. In this way, the phenomenon of surface roughness is the first
It has a correlation with the inclination θ of <110 axis> in the figure, and this relationship is shown in FIG. When θ = 0°, 90°, or around these angles, surface roughness does not occur regardless of the running direction of the tape, but in the range of 20 to 70°, surface roughness occurs although there are differences in conditions, and as described above. It varies greatly depending on how the <110 axis> intersects with the tape running direction. When such surface roughness occurs, spacing loss occurs between the head gap and the magnetic recording medium due to the unevenness caused by the surface roughness in the head gap, which significantly degrades the short wavelength output and changes the envelope shape of the head output. A problem arises in that the signal to noise ratio is also affected and the signal-to-noise ratio deteriorates.

θ=0゜と90゜のタイプはこのような面荒れ現象
が生じないが、θ=0゜のタイプは記録再生感度が
悪く更に短波長化が進んだ場合実用化の面で問題
が生ずる。従つて磁性薄膜テープを記録媒体とし
て使用する場合はθ=90゜のタイプのヘツド、す
なわち摺動面を{110}、空隙形成面を{100}面
(ここで、{100}面とは、100、010、001、100、
010、001の6通りの面を総称したものであ
る。)で構成した単結晶フエライトヘツドで記録
再生することにより、その高性能な特性を十分に
発揮できることになる。
Types with θ = 0° and 90° do not cause such a surface roughening phenomenon, but types with θ = 0° have poor recording and reproducing sensitivity and problems will arise in terms of practical use if wavelengths are further shortened. Therefore, when using a magnetic thin film tape as a recording medium, the θ=90° type head, that is, the sliding surface is the {110} plane, and the gap forming surface is the {100} plane (here, the {100} plane is 100, 010, 001, 100,
It is a general term for the six types of faces 010 and 001. ) can fully demonstrate its high performance characteristics by recording and reproducing data using a single-crystal ferrite head constructed of ferrite heads.

従来からCo系酸化鉄テープを記録媒体として
使用した場合において、フエライト結晶の摩耗が
その結晶方位によつて差があることは知られてい
るが、この場合、表面粗さが実質的に変化せず、
記録媒体と摺動するヘツド面の全体にわたつて、
ほぼ均一に摩耗が促進されるという現象が生じる
のみで、表面粗さが大きく変化する複雑な面荒れ
現象は起らない。すなわち、ヘツド表面が荒れ
ず、ほぼ全面にわたつて均一かつ除々に摩耗が進
行する場合においては、蒸着法によつて形成した
磁性薄膜を用いた場合のようなヘツドの面荒れが
生じないため、特性上の大きな変化、劣化が起こ
らない。
It has been known that when a Co-based iron oxide tape is used as a recording medium, the wear of ferrite crystals differs depending on the crystal orientation, but in this case, the surface roughness does not change substantially. figure,
Throughout the entire head surface that slides against the recording medium,
Only a phenomenon in which wear is accelerated almost uniformly occurs, and a complicated surface roughening phenomenon in which the surface roughness changes significantly does not occur. In other words, if the head surface is not rough and wear progresses uniformly and gradually over almost the entire surface, the head surface will not become rough as it would when using a magnetic thin film formed by vapor deposition. No major changes or deterioration in characteristics occur.

摩擦的視点から、耐摩耗性と耐面荒れ性とは必
ずしも一致せず、摩耗が少ないという観点に基づ
いて、その面荒れが少ないという結論づけはでき
ない。
From a friction point of view, wear resistance and surface roughness resistance do not necessarily match, and it cannot be concluded that the surface roughness is low based on the viewpoint that the wear is low.

上述のような、単結晶フエライトの結晶方位に
よつて異なる面荒れが生ずるという現象は、単結
晶フエライトと、磁性薄膜を蒸着法によつて形成
した磁気記録媒体との組み合わせにおいて生じる
もので、従来の摩耗と異なる新規な現象である。
本発明はこの現象の発見に基づきなされたもので
あり、非磁性基板上に磁性薄膜を蒸着法によつて
形成した磁気記録媒体と、単結晶フエライト磁気
ヘツドとの組み合わせにおいて、磁気記録媒体と
接触・摺動する面が{110}面ないしは{110}面
に対し20゜の範囲で傾斜した結晶面からなり、か
つ空隙形成面が{100}面ないしは{100}面に対
し20゜の範囲で傾斜した結晶面で構成した磁気ヘ
ツドを用いて記録再生を行なうことにより、その
高性能な特性を長時間にわたつて十分に発揮でき
る磁気記録再生装置を提供できたものである。
The above-mentioned phenomenon in which surface roughness differs depending on the crystal orientation of single-crystal ferrite occurs when a single-crystal ferrite is combined with a magnetic recording medium in which a magnetic thin film is formed by vapor deposition. This is a new phenomenon that is different from wear.
The present invention was made based on the discovery of this phenomenon, and is based on the combination of a magnetic recording medium in which a magnetic thin film is formed on a nonmagnetic substrate by vapor deposition, and a single crystal ferrite magnetic head, which makes contact with the magnetic recording medium.・The sliding surface consists of a {110} plane or a crystal plane inclined at an angle of 20° to the {110} plane, and the void forming plane is a {100} plane or an angle of 20° to the {100} plane. By performing recording and reproducing using a magnetic head composed of inclined crystal planes, it has been possible to provide a magnetic recording and reproducing device that can fully exhibit its high performance characteristics over a long period of time.

第5図は記録波長と相対ヘツド出力の関係を示
すものであり、曲線Aは本発明に係る単結晶フエ
ライトヘツド(θ=90゜のタイプのヘツド)とCo
−Ni系の磁性薄膜を蒸着法によつて形成した磁
気記録媒体との組み合わせによつて得られる記録
再生装置の出力特性を示し、曲線Bは、従来の
Co系酸化鉄テープと単結晶フエライトヘツド
(θ=35.3゜のタイプのヘツド)との組み合わせに
よつて得られる記録再生装置の出力特性を示す。
図から、本発明に係る記録再生装置の方が、従来
の装置に比して特に短波長領域で優れた出力特性
を得ることができることが分かる。したがつて、
シリンダ径を大幅に小さくしても十分な高品質の
画像が得られる。このような本発明の記録再生装
置における出力特性は、長時間使用した場合にお
いても何んら劣化が起つていない。
FIG. 5 shows the relationship between the recording wavelength and the relative head output, and curve A shows the relationship between the single crystal ferrite head (the θ=90° type head) according to the present invention and the Co
-Curve B shows the output characteristics of a recording/reproducing device obtained by combining a magnetic recording medium with a Ni-based magnetic thin film formed by vapor deposition.
This figure shows the output characteristics of a recording/reproducing device obtained by combining a Co-based iron oxide tape and a single-crystal ferrite head (head with θ = 35.3°).
From the figure, it can be seen that the recording/reproducing device according to the present invention can obtain superior output characteristics, especially in the short wavelength region, compared to the conventional device. Therefore,
Sufficient high-quality images can be obtained even if the cylinder diameter is significantly reduced. The output characteristics of the recording/reproducing apparatus of the present invention do not deteriorate at all even when used for a long time.

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

第1図は従来の単結晶フエライトを使用した磁
気ヘツドの構成を示す側面図、第2図aは第1図
に示す磁気ヘツドのテープ摺動面の面あれ状態を
示す顕微鏡写真、bは本発明の磁気ヘツドのテー
プ摺動面の面あれ状態を示す顕微鏡写真、第3図
a,b,cはそれぞれ第2図a,bの磁気ヘツド
コアの面あれ状態の測定図、第4図は、摺動方向
に対する<110軸>の傾θと表面あれの関係を示
す図、第5図は本発明による磁気ヘツドと従来の
磁気ヘツドの記録波長と相対ヘツド出力との関係
を示す図である。 1,1a……ヘツドコア、2,2a……摺動
面、3……ヘツドギヤツプ、5……ギヤツプ形成
面。
Fig. 1 is a side view showing the configuration of a conventional magnetic head using single crystal ferrite, Fig. 2a is a micrograph showing the roughness of the tape sliding surface of the magnetic head shown in Fig. 1, and b is a photomicrograph showing the roughness of the tape sliding surface of the magnetic head shown in Fig. Micrographs showing the surface roughness of the tape sliding surface of the magnetic head of the invention; FIGS. 3a, b, and c are measurement views of the surface roughness of the magnetic head core in FIGS. FIG. 5 is a diagram showing the relationship between the inclination θ of the <110 axis> with respect to the sliding direction and surface roughness, and FIG. 5 is a diagram showing the relationship between the recording wavelength and relative head output of the magnetic head according to the present invention and the conventional magnetic head. 1, 1a... Head core, 2, 2a... Sliding surface, 3... Head gap, 5... Gap forming surface.

Claims (1)

【特許請求の範囲】[Claims] 1 非磁性基板上に磁性薄膜を蒸着法によつて形
成した磁気記録媒体を用い、前記磁気記録媒体と
接触・摺動する面が{110}面ないしは{110}面
に対し20゜の範囲で傾斜した結晶面からなり、か
つ空隙形成面が{100}面ないしは{100}面に対
し20゜の範囲で傾斜した結晶面で構成される単結
晶フエライト磁気ヘツドで記録再生を行なうこと
を特徴とする磁気記録再生装置。
1. Using a magnetic recording medium in which a magnetic thin film is formed by vapor deposition on a non-magnetic substrate, the surface that contacts and slides on the magnetic recording medium is a {110} plane or within a range of 20° to the {110} plane. Recording and reproduction is performed using a single crystal ferrite magnetic head consisting of an inclined crystal plane, and the void forming plane is a {100} plane or a crystal plane inclined within a range of 20° with respect to the {100} plane. magnetic recording and reproducing device.
JP3749881A 1981-03-16 1981-03-16 Magnetic recorder and reproducer Granted JPS57169915A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3749881A JPS57169915A (en) 1981-03-16 1981-03-16 Magnetic recorder and reproducer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3749881A JPS57169915A (en) 1981-03-16 1981-03-16 Magnetic recorder and reproducer

Publications (2)

Publication Number Publication Date
JPS57169915A JPS57169915A (en) 1982-10-19
JPH0159643B2 true JPH0159643B2 (en) 1989-12-19

Family

ID=12499181

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3749881A Granted JPS57169915A (en) 1981-03-16 1981-03-16 Magnetic recorder and reproducer

Country Status (1)

Country Link
JP (1) JPS57169915A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03124313U (en) * 1990-03-30 1991-12-17

Also Published As

Publication number Publication date
JPS57169915A (en) 1982-10-19

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