JPH1166503A - Perpendicular magnetic recording and reproducing method - Google Patents
Perpendicular magnetic recording and reproducing methodInfo
- Publication number
- JPH1166503A JPH1166503A JP23335097A JP23335097A JPH1166503A JP H1166503 A JPH1166503 A JP H1166503A JP 23335097 A JP23335097 A JP 23335097A JP 23335097 A JP23335097 A JP 23335097A JP H1166503 A JPH1166503 A JP H1166503A
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Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は、垂直磁気記録再生
方式に関し、さらに詳細には、軟磁性裏打ち層を、垂直
磁気異方性を有する磁気記録層の下側に配置した二層磁
気記録媒体に対してのマージ型磁気抵抗効果型磁気ヘッ
ドによる記録再生方式に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a perpendicular magnetic recording / reproducing system, and more particularly, to a two-layer magnetic recording medium in which a soft magnetic underlayer is arranged below a magnetic recording layer having perpendicular magnetic anisotropy. And a recording / reproducing method using a merged magnetoresistive effect type magnetic head.
【0002】[0002]
【従来の技術】磁気記録における高密度化のために、記
録面に垂直な方向に磁化容易軸を持つ垂直磁気記録媒体
を用いる垂直磁気記録再生方式が提案されている(岩
崎、大内:アイ・イー・イー・イー・トランザクション
オン マグネチックス、エムエージー14、849
(1987年)(S.Iwasaki and K.O
uchi:IEEE Trans. Magn.,MA
G−14,849(1987))。垂直磁気記録再生方
式は、現在実用化されている長手記録方式と異なり、記
録密度が高くなるほど自己減磁作用が小さくなる特徴が
ある。特に、軟磁性裏打ち層上に形成したCoCr磁性
膜に単磁極ヘッドを用いて記録すると600kFCI以
上の高線記録密度域においても再生出力が確認されてい
る。2. Description of the Related Art In order to increase the density of magnetic recording, a perpendicular magnetic recording / reproducing method using a perpendicular magnetic recording medium having an easy axis of magnetization in a direction perpendicular to the recording surface has been proposed (Iwasaki, Ouchi: Eye).・ EEE Transaction on Magnetics, MGE14, 849
(1987) (S. Iwasaki and KO)
uchi: IEEE Trans. Magn. , MA
G-14, 849 (1987)). The perpendicular magnetic recording / reproducing method is different from the longitudinal recording method currently in practical use in that the self-demagnetizing effect decreases as the recording density increases. In particular, when recording is performed on a CoCr magnetic film formed on a soft magnetic underlayer using a single pole head, a reproduction output has been confirmed even in a high linear recording density region of 600 kFCI or more.
【0003】しかしながら、日本応用磁気学会 第93
回研究会資料の第75頁からの「マージ型MRヘッドを
用いた垂直磁気記録」にも述べられているように、軟磁
性裏打ち層を有する二層磁気記録媒体に長手記録用に設
計されたマージ型MRヘッドを用いて記録再生した場合
には、充分なオーバーライト特性(以下、O/W特性と
略する場合がある)は得られるものの、分解能が著しく
低下するという問題点があった。また、特開平8−24
9601号公報には、単層媒体に、リーディングエッジ
側の飽和磁束密度を高めたリングヘッドを用いて記録し
た場合には、充分な特性が得られることが述べられてい
るが、更に高密度化し狭トラックした場合には、出力が
足りず、より高感度なMRヘッドによる再生が必要にな
る。However, the Japan Society of Applied Magnetics 93
As described in “Perpendicular Magnetic Recording Using a Merge MR Head” from page 75 of the JSCE, it was designed for longitudinal recording on a double-layer magnetic recording medium with a soft magnetic underlayer. When recording / reproducing is performed using a merge type MR head, although sufficient overwrite characteristics (hereinafter sometimes abbreviated as O / W characteristics) are obtained, there is a problem that the resolution is significantly reduced. Also, JP-A-8-24
Japanese Patent Application Publication No. 9601 describes that sufficient characteristics can be obtained when recording is performed on a single-layer medium using a ring head having an increased saturation magnetic flux density on the leading edge side. In the case of a narrow track, the output is insufficient, and reproduction with a more sensitive MR head is required.
【0004】[0004]
【発明が解決しようとする課題】そこで、本発明は、上
記二層磁気記録媒体にマージ型磁気抵抗効果型磁気ヘッ
ドで記録再生を行なう場合であっても、充分なO/W特
性と分解能を得ることができる垂直磁気記録再生方式を
提供することを目的とする。Therefore, the present invention provides a sufficient O / W characteristic and resolution even when recording / reproducing is performed with the merged magnetoresistive magnetic head on the double-layer magnetic recording medium. It is an object of the present invention to provide a perpendicular magnetic recording / reproducing method which can be obtained.
【0005】[0005]
【課題を解決するための手段】上記の目的は、以下の本
発明(1)〜(4)により達成される。 (1) 厚さ10nm以上50nm以下の軟磁性裏打ち
層を、垂直磁気異方性を有する磁気記録層の下側に配置
した二層磁気記録媒体に、記録ギャップ長が0.2μm
以上0.5μm以下の再生用磁気抵抗効果型素子を複合
させたマージ型磁気抵抗効果型磁気ヘッドで記録再生す
ることを特徴とする垂直磁気記録再生方式。 (2) 前記磁気ヘッドの後縁側磁極厚が前縁側磁極厚
よりも薄く、しかも後縁側磁極の飽和磁束密度が前縁側
磁極の飽和磁束密度より大きい上記(1)の垂直磁気記
録再生方式。 (3) 前記二層磁気記録媒体と前記磁気ヘッドとの磁
気的なスペーシングが60nm以下である上記(1)ま
たは(2)の垂直磁気記録再生方式。 (4) 前記二層磁気記録媒体の磁化容易軸方向の保磁
力が1800Oe以上である上記(1)〜(3)のいずれ
かの垂直磁気記録再生方式。The above object is achieved by the following present inventions (1) to (4). (1) A double-layer magnetic recording medium in which a soft magnetic underlayer having a thickness of 10 nm or more and 50 nm or less is arranged below a magnetic recording layer having perpendicular magnetic anisotropy has a recording gap length of 0.2 μm.
A perpendicular magnetic recording / reproducing method characterized in that recording / reproducing is performed by a merge type magnetoresistive magnetic head in which a reproducing magnetoresistive element having a size of 0.5 μm or less is combined. (2) The perpendicular magnetic recording / reproducing method according to the above (1), wherein the magnetic pole thickness at the trailing edge of the magnetic head is smaller than the magnetic pole thickness at the leading edge, and the saturation magnetic flux density of the trailing edge magnetic pole is larger than the saturation magnetic flux density of the leading edge magnetic pole. (3) The perpendicular magnetic recording / reproducing method according to (1) or (2), wherein the magnetic spacing between the double-layer magnetic recording medium and the magnetic head is 60 nm or less. (4) The perpendicular magnetic recording / reproducing method according to any one of (1) to (3), wherein the coercive force in the easy axis direction of the double-layer magnetic recording medium is 1800 Oe or more.
【0006】[0006]
【発明の作用・効果】本発明によれば、二層磁気記録媒
体の軟磁性裏打ち層の膜厚を10〜50nmとするとと
もに、マージ型磁気抵抗効果型磁気ヘッドの記録ギャッ
プ長を0.2〜0.5μmとしたことにより、60%以
上の高い分解能と、−30dB以下の低いO/W特性を
両立させることができた。According to the present invention, the thickness of the soft magnetic backing layer of the double-layer magnetic recording medium is set to 10 to 50 nm, and the recording gap length of the merge type magnetoresistive magnetic head is set to 0.2. By setting the thickness to 0.5 μm, both high resolution of 60% or more and low O / W characteristics of -30 dB or less can be achieved.
【0007】[0007]
【発明の実施の形態】以下、本発明の具体的構成につい
て詳細に説明する。BEST MODE FOR CARRYING OUT THE INVENTION Hereinafter, a specific configuration of the present invention will be described in detail.
【0008】本発明は、上記した二層磁気記録媒体に対
してマージ型磁気抵抗効果型磁気ヘッドで情報を記録再
生する垂直磁気記録再生方式であって、60%以上の高
い分解能と、−30dB以下の低いO/W特性を達成す
るため、上記二層磁気記録媒体の軟磁性裏打ち層の膜厚
を10nm以上50nm以下とし、またマージ型磁気抵
抗効果型磁気ヘッドの記録部の記録ギャップ長を0.2
μm以上0.5μm以下に設定した。The present invention relates to a perpendicular magnetic recording / reproducing system for recording / reproducing information on / from the above-mentioned two-layer magnetic recording medium by a merge-type magnetoresistive head, and has a high resolution of 60% or more, and -30 dB. In order to achieve the following low O / W characteristics, the thickness of the soft magnetic underlayer of the two-layer magnetic recording medium is set to 10 nm or more and 50 nm or less, and the recording gap length of the recording portion of the merged magnetoresistive magnetic head is reduced. 0.2
It was set to not less than μm and not more than 0.5 μm.
【0009】なお、O/W特性は、始めに記録媒体上に
所定の低周波信号(LF)で記録し、その後、その上に
所定の高周波信号(HF)で上書きし、これを再生した
場合の、LFの残留再生信号出力の値とオーバーライト
前のLFの再生信号出力の値との比、すなわち次の式で
表される。 O/W特性(dB)=LFの残留再生信号出力/オーバ
ーライト前のLFの再生信号出力The O / W characteristic is obtained by first recording on a recording medium with a predetermined low-frequency signal (LF), and then overwriting it with a predetermined high-frequency signal (HF) and reproducing it. Of the LF residual reproduction signal output value and the LF reproduction signal output value before overwriting, ie, expressed by the following equation. O / W characteristic (dB) = LF residual reproduction signal output / LF reproduction signal output before overwriting
【0010】また、分解能は、記録媒体上に所定の低周
波信号(LF)で記録した場合と、所定の高周波信号
(HF)で記録した場合の情報を別個に再生した場合
の、HFの再生信号出力の値とLFの再生信号出力の値
との比、すなわち次の式で表される。 分解能(%)=HFの再生信号出力/LFの再生信号出
力[0010] The resolution is defined as the HF reproduction between the case where information is recorded on a recording medium with a predetermined low frequency signal (LF) and the case where information recorded with a predetermined high frequency signal (HF) is reproduced separately. The ratio between the value of the signal output and the value of the LF reproduction signal output, that is, is represented by the following equation. Resolution (%) = HF reproduction signal output / LF reproduction signal output
【0011】図1に本発明の垂直磁気記録再生方式に用
いられる好ましい構造のマージ型磁気抵抗効果型磁気ヘ
ッドの一例を概略平面図で示す。FIG. 1 is a schematic plan view showing an example of a merge type magnetoresistive head having a preferable structure used in the perpendicular magnetic recording / reproducing system of the present invention.
【0012】この図において、磁気抵抗効果型磁気ヘッ
ドHは、再生部RにMR素子1を有し、このMR素子1
の両端には、電極2a、2bが接続されている。上記M
R素子1および電極2a、2bの両側には、それぞれ非
磁性絶縁層3a、3bが形成され、これらの非磁性絶縁
層3a、3b上にはそれぞれ下部および上部シールド磁
性層4a、4bが形成されている。以上の再生部Rは、
下地層5を介して基板6上に形成されている。In FIG. 1, a magneto-resistance effect type magnetic head H has an MR element 1 in a reproducing section R.
Are connected to electrodes 2a and 2b. M above
Non-magnetic insulating layers 3a and 3b are formed on both sides of the R element 1 and the electrodes 2a and 2b, respectively. Lower and upper shield magnetic layers 4a and 4b are formed on the non-magnetic insulating layers 3a and 3b, respectively. ing. The above playback unit R
It is formed on a substrate 6 via an underlayer 5.
【0013】一方、記録部Wはインダクティブ型薄膜ヘ
ッドとして構成され、再生部Rの上部シールド磁性層4
bを記録の下部磁極として共用し、この上部シールド磁
性層4b上に設けられた非磁性絶縁層9上に形成された
上部記録磁極8を有している。なお、図中、符号7はリ
ードギャップ、符号10は記録ギャップを示す。On the other hand, the recording section W is configured as an inductive type thin film head, and the upper shield magnetic layer 4 of the reproducing section R is formed.
b serves as a lower magnetic pole for recording, and has an upper recording magnetic pole 8 formed on a nonmagnetic insulating layer 9 provided on the upper shield magnetic layer 4b. In the figure, reference numeral 7 indicates a read gap, and reference numeral 10 indicates a recording gap.
【0014】上記MR素子1は、従来構造のいずれのも
のであってもよいので、これ以上の説明は省略するが、
現在のところ、NiFeRh/Ta/NiFeで形成さ
れたMR膜を有するものが一般的である。またスピンバ
ルブ素子を用いてもよい。Since the MR element 1 may have any conventional structure, further description is omitted.
At present, those having an MR film formed of NiFeRh / Ta / NiFe are generally used. Further, a spin valve element may be used.
【0015】上記電極2a、2bとしては、Ta,Cu
等により、500〜2000A程度の膜厚に形成され
る。As the electrodes 2a and 2b, Ta, Cu
For example, a film thickness of about 500 to 2000 A is formed.
【0016】上記非磁性絶縁層3a、3bとしては、A
l2O3,SiO2,SiN,BN,AlN等により、2
00〜2000A程度の膜厚に形成される。The nonmagnetic insulating layers 3a and 3b are made of A
1 2 O 3 , SiO 2 , SiN, BN, AlN, etc.
It is formed to a thickness of about 00 to 2000A.
【0017】上記シールド層4a、4bは、NiFe,
FeAlSi,Co系アモルファス合金(CoZrN
b,CoZrMoなど)等により、1〜4μm 程度の膜
厚に形成される。The shield layers 4a and 4b are made of NiFe,
FeAlSi, Co-based amorphous alloy (CoZrN
b, CoZrMo, etc.) to a thickness of about 1 to 4 μm.
【0018】上記下地層5は、Al2O3,SiO2等に
より、1〜10μm 程度の膜厚に形成される。The underlayer 5 is formed of Al 2 O 3 , SiO 2 or the like to a thickness of about 1 to 10 μm.
【0019】上記基板6は、AlTiC(Al2O3およ
びTiCを主成分とするセラミック)等である。The substrate 6 is made of AlTiC (ceramic mainly composed of Al 2 O 3 and TiC).
【0020】記録部Wにおいて、非磁性絶縁層9はAl
2O3,SiO2等により、0.1〜1μm 程度の膜厚に
形成される。すなわち記録ギャップ長は、0.1μm以
上、1μm以下に設定される。In the recording section W, the nonmagnetic insulating layer 9 is made of Al
It is formed to a thickness of about 0.1 to 1 μm using 2 O 3 , SiO 2, or the like. That is, the recording gap length is set to 0.1 μm or more and 1 μm or less.
【0021】また、上記上部記録磁極8は、NiFe,
Co系アモルファス合金(CoTaZr,CoZrNb
など)、FeTaN等により、0.5〜4μm 程度の膜
厚に形成される。The upper recording magnetic pole 8 is made of NiFe,
Co-based amorphous alloys (CoTaZr, CoZrNb
), And a film thickness of about 0.5 to 4 μm made of FeTaN or the like.
【0022】上記上部記録磁極8および上部シールド層
(共通ポール)4bは、同じ膜厚のものであってもよい
が、記録媒体の移動方向に対して後縁側(トレーリング
側)の磁極すなわち上部記録磁極8の方が前縁側(リー
ディング側)の磁極すなわち上部シールド層(共通ポー
ル)4bより膜厚が小さい方が好ましい。後縁側(トレ
ーリング側)の磁極の膜厚を1としたとき、前縁側(リ
ーディング側)の磁極の膜厚は、1〜5程度であること
が好ましい。また、後縁側(トレーリング側)の磁極す
なわち上部記録磁極8の飽和磁束密度Bsは、前縁側(リ
ーディング側)の磁極すなわち4bの飽和磁束密度Bsよ
り大きいことが好ましく、具体的には、後縁側(トレー
リング側)の磁極の飽和磁束密度Bsが0.8T〜1.8
T程度であり、前縁側(リーディング側)の磁極の飽和
磁束密度Bsが0.5T〜0.8T程度であり、後縁側
(トレーリング側)の磁極の飽和磁束密度Bsを1とした
とき、前縁側(リーディング側)の磁極の飽和磁束密度
Bsは、0.4〜1程度であることが好ましい。以上の条
件を満たさないときは、分解能およびO/W特性が劣化
する傾向がある。The upper recording magnetic pole 8 and the upper shield layer (common pole) 4b may have the same film thickness, but the magnetic pole on the trailing edge side (trailing side) with respect to the moving direction of the recording medium, that is, the upper pole. It is preferable that the recording magnetic pole 8 has a smaller film thickness than the magnetic pole on the front edge side (leading side), that is, the upper shield layer (common pole) 4b. Assuming that the thickness of the magnetic pole on the trailing edge side (trailing side) is 1, the thickness of the magnetic pole on the leading edge side (leading side) is preferably about 1 to 5. Further, the saturation magnetic flux density Bs of the magnetic pole on the trailing edge side (trailing side), ie, the upper recording magnetic pole 8 is preferably larger than the magnetic flux density Bs of the magnetic pole on the leading edge side (leading side), ie, 4b. The saturation magnetic flux density Bs of the magnetic pole on the edge side (trailing side) is 0.8T to 1.8.
T is about T, the saturation magnetic flux density Bs of the magnetic pole on the leading edge side (leading side) is about 0.5T to 0.8T, and the saturation magnetic flux density Bs of the magnetic pole on the trailing edge side (trailing side) is 1, Saturation magnetic flux density of the magnetic pole on the leading edge side (leading side)
Bs is preferably about 0.4 to 1. If the above conditions are not satisfied, the resolution and O / W characteristics tend to deteriorate.
【0023】そして、本発明のマージ型磁気抵抗効果型
磁気ヘッドHの上記記録ギャップ10の長さは、0.2
μm以上0.5μm以下に設定される。記録ギャップ長
が上記範囲より小さいと、O/W特性が劣化し、上記範
囲より大きいと分解能が劣化する。The length of the recording gap 10 of the merged magnetoresistive head H of the present invention is 0.2
It is set to be not less than μm and not more than 0.5 μm. If the recording gap length is smaller than the above range, the O / W characteristics deteriorate, and if it is larger than the above range, the resolution deteriorates.
【0024】上記二層磁気記録媒体は、厚さが0.5〜
2mm程度のガラスやアルミニウム製の基板の上に軟磁性
裏打ち層および磁気記録層を順次成膜したものである。The double-layer magnetic recording medium has a thickness of 0.5 to 0.5.
A soft magnetic underlayer and a magnetic recording layer are sequentially formed on a glass or aluminum substrate of about 2 mm.
【0025】上記磁気記録層はCoCr磁性層、Baフ
ェライト磁性層、Co−γFe2O3等の記録面に垂直な
方向に磁化容易軸を持つ磁気記録層で、その厚さは、2
0〜200nm程度に設定されることが好ましい。なお、
この二層磁気記録媒体の磁化容易軸方向の保磁力は、1
800Oe以上であることが好ましい。この保磁力が18
00Oe未満になると分解能が劣化する傾向がある。The magnetic recording layer is a magnetic recording layer having an easy axis of magnetization perpendicular to the recording surface, such as a CoCr magnetic layer, a Ba ferrite magnetic layer, or Co-γFe 2 O 3.
Preferably, it is set to about 0 to 200 nm. In addition,
The coercive force in the easy axis direction of this double-layer magnetic recording medium is 1
It is preferably at least 800 Oe. This coercive force is 18
If it is less than 00 Oe, the resolution tends to deteriorate.
【0026】上記軟磁性裏打ち層は、NiFe(パーマ
ロイ)、CoZrNb等で、10nm以上50nm以下
の範囲の膜厚に形成される。軟磁性裏打ち層の膜厚が、
上記の範囲より小さいとO/W特性が劣化し、上記の範
囲より大きいと分解能が劣化する。The soft magnetic underlayer is made of NiFe (permalloy), CoZrNb, or the like, and has a thickness of 10 nm or more and 50 nm or less. When the thickness of the soft magnetic backing layer is
If the value is smaller than the above range, the O / W characteristics deteriorate, and if the value is larger than the above range, the resolution deteriorates.
【0027】本発明の垂直磁気記録再生方式において
は、以上説明した二層磁気記録媒体に対して上記のマー
ジ型磁気抵抗効果型磁気ヘッドを用いて情報の記録再生
が行なわれる。上記磁気ヘッドは、上記記録再生の際、
媒体から浮上するタイプのものであり、このとき、上記
二層磁気記録媒体とマージ型磁気抵抗効果型磁気ヘッド
の磁気的なスペーシングは、60nm以下であることが
好ましい。この磁気的スペーシグが60nmを超える
と、分解能およびO/W特性が共に劣化する傾向があ
る。上記の磁気的スペーシングは、媒体と磁気ヘッドの
対向面に保護膜が形成されている場合、ヘッドの浮上量
にこれらの保護膜の膜厚を加えた値となる。In the perpendicular magnetic recording / reproducing method of the present invention, information is recorded / reproduced on / from the above-described double-layer magnetic recording medium by using the above-mentioned merge type magnetoresistive head. The magnetic head, during the recording and reproduction,
In this case, the magnetic spacing between the double-layer magnetic recording medium and the merge-type magnetoresistive magnetic head is preferably 60 nm or less. If the magnetic spacing exceeds 60 nm, both resolution and O / W characteristics tend to deteriorate. When a protective film is formed on the surface of the medium facing the magnetic head, the magnetic spacing is a value obtained by adding the thickness of the protective film to the flying height of the head.
【0028】[0028]
【実施例】以下、本発明の具体的実施例について詳細に
説明する。DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, specific embodiments of the present invention will be described in detail.
【0029】実施例1垂直磁気記録媒体 2.5インチガラスディスク基板上に成膜され、Hc⊥
=2400Oe、膜厚=100nmのCrCo磁性層であ
る磁性記録層を持つ。この磁性記録層の下側には、Ni
Fe膜の軟磁性裏打ち層を、0、10、20、30、4
0、50、60および100nmと変化させ、それぞれ
垂直磁気記録媒体のサンプルNo. M−1、M−2、M−
3、M−4、M−5、M−6、M−7およびM−8とし
た。Example 1 A film was formed on a 2.5 inch glass disk substrate of a perpendicular magnetic recording medium.
= 2400 Oe and a magnetic recording layer which is a CrCo magnetic layer with a film thickness of 100 nm. Under this magnetic recording layer, Ni
The soft magnetic backing layer of the Fe film is set to 0, 10, 20, 30, 4
0, 50, 60 and 100 nm, respectively, and sample Nos. M-1, M-2 and M-
3, M-4, M-5, M-6, M-7 and M-8.
【0030】マージ型磁気抵抗効果型磁気ヘッド このマージ型磁気抵抗効果型磁気ヘッドとしては、記録
部の上部磁極(図1の8に相当)および下部磁極(図1
の4bに相当)とも飽和磁束密度Bsが0.8TのNiF
e膜のものを用いた。この磁気ヘッドの他の仕様は次の
通りとした。 Merge type magnetoresistive head This merge type magnetoresistive head has an upper magnetic pole (corresponding to 8 in FIG. 1) and a lower magnetic pole (corresponding to 8 in FIG. 1).
4b) and NiF whose saturation magnetic flux density Bs is 0.8T
An e-film was used. Other specifications of this magnetic head were as follows.
【0031】 上部記録磁極幅 3.2μm 実効MRトラック幅 2.2μmUpper recording magnetic pole width 3.2 μm Effective MR track width 2.2 μm
【0032】 上部記録磁極厚 3.5μm 記録ギャップ長 0.45μm 上部シールド(共通ポール)厚 3.5μm リードギャップ長 0.27μm 下部シールド厚 1.0μmUpper recording magnetic pole thickness 3.5 μm Recording gap length 0.45 μm Upper shield (common pole) thickness 3.5 μm Read gap length 0.27 μm Lower shield thickness 1.0 μm
【0033】 スライダー形状 負圧正圧併用型 ヘッド浮上量 30nm 磁気的スペーシング量 50nmSlider shape Negative pressure / positive pressure combined type Head floating amount 30 nm Magnetic spacing amount 50 nm
【0034】以上の条件において、LF(16.7kF
CI)とHF(100kFCI)の電流をマージ型磁気
抵抗効果型磁気ヘッドの記録部に印加して、分解能とO
/W特性を測定した。分解能とO/W特性は上記の式に
より求めた。結果を表1に示した。Under the above conditions, LF (16.7 kF
CI) and HF (100 kFCI) are applied to the recording portion of the merged magnetoresistive magnetic head, and the resolution and O
/ W characteristics were measured. The resolution and the O / W characteristics were determined by the above equations. The results are shown in Table 1.
【0035】[0035]
【表1】 [Table 1]
【0036】次に、二層磁気記録媒体の軟磁性裏打ち層
の膜厚を20nmに固定し、記録ギャップ長を0.1、
0.2、0.3、0.4、0.5および0.6μm(そ
れぞれサンプルNo. H−1、H−2、H−3、H−4、
H−5およびH−6とした)に変化させた以外は上記と
同様にして、分解能とO/W特性は上記の式により求め
た。結果を表2に示した。Next, the thickness of the soft magnetic backing layer of the double-layer magnetic recording medium was fixed at 20 nm, the recording gap length was 0.1, and
0.2, 0.3, 0.4, 0.5 and 0.6 μm (sample Nos. H-1, H-2, H-3, H-4,
H-5 and H-6), and the resolution and O / W characteristics were determined by the above equations. The results are shown in Table 2.
【0037】[0037]
【表2】 [Table 2]
【0038】以上の結果から本発明の効果が明らかであ
る。The effects of the present invention are apparent from the above results.
【0039】実施例2 前記磁気ヘッドの後縁側磁極と前縁側磁極の膜厚と飽和
磁束密度を種々変化させた以外は上記実施例1と同様に
して分解能とO/W特性を測定したところ、前記磁気ヘ
ッドの後縁側磁極厚が前縁側磁極厚よりも薄く、しかも
後縁側磁極の飽和磁束密度が前縁側磁極の飽和磁束密度
より大きい場合にのみ、分解能およびO/W特性ともに
向上する傾向が得られた。Example 2 The resolution and O / W characteristics were measured in the same manner as in Example 1 except that the film thickness and the saturation magnetic flux density of the trailing edge magnetic pole and the leading edge magnetic pole of the magnetic head were variously changed. Only when the trailing edge magnetic pole thickness of the magnetic head is thinner than the leading edge magnetic pole thickness and the saturation magnetic flux density of the trailing edge magnetic pole is larger than the saturation magnetic flux density of the leading edge magnetic pole, both the resolution and the O / W characteristics tend to be improved. Obtained.
【0040】実施例3 実施例1において、前記二層磁気記録媒体と前記磁気ヘ
ッドとの磁気的なスペーシングの値のみを種々変化させ
て分解能とO/W特性を測定したところ、この磁気的ス
ペーシングが60nm以下のとき、分解能およびO/W
特性ともに向上する傾向が得られた。Example 3 In Example 1, the resolution and O / W characteristics were measured by varying only the value of the magnetic spacing between the double-layer magnetic recording medium and the magnetic head. When the spacing is 60 nm or less, the resolution and O / W
A tendency to improve both characteristics was obtained.
【0041】実施例4 前記二層磁気記録媒体の磁化容易軸方向の保磁力を種々
変化させた以外は実施例1と同様にして分解能とO/W
特性を測定したところ、この磁気的スペーシングが60
nm以下のとき、分解能およびO/W特性ともに向上す
る傾向が得られた。Example 4 The resolution and O / W were the same as in Example 1 except that the coercive force in the easy axis direction of the double-layer magnetic recording medium was changed variously.
When the characteristics were measured, the magnetic spacing was 60
At nm or less, both resolution and O / W characteristics tended to be improved.
【図1】本発明の磁気抵抗効果型磁気ヘッドの層構成の
一例を示す概略平面図である。FIG. 1 is a schematic plan view showing an example of a layer configuration of a magnetoresistive head according to the present invention.
H 磁気抵抗効果型磁気ヘッド 1 MR素子 2a 電極 2b 電極 3a 非磁性絶縁層 3b 非磁性絶縁層 4a 下部シールド磁性層 4b 上部シールド磁性層/下部記録磁極(共通ポー
ル) 7 リードギャップ 8 上部記録磁極 9 非磁性層 10 記録ギャップH Magnetoresistive magnetic head 1 MR element 2a Electrode 2b Electrode 3a Non-magnetic insulating layer 3b Non-magnetic insulating layer 4a Lower shield magnetic layer 4b Upper shield magnetic layer / lower recording magnetic pole (common pole) 7 Read gap 8 Upper recording magnetic pole 9 Non-magnetic layer 10 Recording gap
───────────────────────────────────────────────────── フロントページの続き (72)発明者 佐藤 勇武 東京都中央区日本橋一丁目13番1号 ティ ーディーケイ株式会社内 (72)発明者 大内 一弘 秋田県秋田市新屋町字砂奴寄4−21 秋田 県高度技術研究所内 (72)発明者 本多 直樹 秋田県秋田市新屋町字砂奴寄4−21 秋田 県高度技術研究所内 ──────────────────────────────────────────────────続 き Continuing on the front page (72) Inventor Yutake Sato 1-13-1 Nihonbashi, Chuo-ku, Tokyo Inside TDK Corporation (72) Inventor Kazuhiro Ouchi 4-Sunanu, Shinyacho, Akita City, Akita Prefecture 21 Within the Akita Prefectural Advanced Technology Research Institute (72) Inventor Naoki Honda 4-21, Sanda-Yoro, Niiyacho, Akita-shi, Akita Pref.
Claims (4)
裏打ち層を、垂直磁気異方性を有する磁気記録層の下側
に配置した二層磁気記録媒体に、記録ギャップ長が0.
2μm以上0.5μm以下の再生用磁気抵抗効果型素子
を複合させたマージ型磁気抵抗効果型磁気ヘッドで記録
再生することを特徴とする垂直磁気記録再生方式。1. A two-layer magnetic recording medium in which a soft magnetic underlayer having a thickness of 10 nm or more and 50 nm or less is disposed below a magnetic recording layer having perpendicular magnetic anisotropy, has a recording gap length of 0.1 mm.
A perpendicular magnetic recording / reproducing method characterized in that recording / reproducing is performed by a merged magnetoresistive magnetic head in which a reproducing magnetoresistive element of 2 μm or more and 0.5 μm or less is combined.
磁極厚よりも薄く、しかも後縁側磁極の飽和磁束密度が
前縁側磁極の飽和磁束密度より大きい請求項1の垂直磁
気記録再生方式。2. The perpendicular magnetic recording / reproducing method according to claim 1, wherein the thickness of the trailing edge magnetic pole of the magnetic head is smaller than the thickness of the leading edge magnetic pole, and the saturation magnetic flux density of the trailing edge magnetic pole is larger than the saturation magnetic flux density of the leading edge magnetic pole.
との磁気的なスペーシングが60nm以下である請求項
1または2の垂直磁気記録再生方式。3. The perpendicular magnetic recording / reproducing method according to claim 1, wherein a magnetic spacing between the double-layer magnetic recording medium and the magnetic head is 60 nm or less.
の保磁力が1800Oe以上である請求項1〜3の何れか
の垂直磁気記録再生方式。4. The perpendicular magnetic recording / reproducing method according to claim 1, wherein the coercive force in the easy axis direction of the double-layer magnetic recording medium is 1800 Oe or more.
Priority Applications (1)
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JP23335097A JPH1166503A (en) | 1997-08-14 | 1997-08-14 | Perpendicular magnetic recording and reproducing method |
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JP23335097A JPH1166503A (en) | 1997-08-14 | 1997-08-14 | Perpendicular magnetic recording and reproducing method |
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6657813B2 (en) | 2000-02-28 | 2003-12-02 | Hitachi, Ltd. | Perpendicular magnetic recording system |
US6707643B2 (en) | 2000-09-25 | 2004-03-16 | Kabushiki Kaisha Toshiba | Perpendicular magnetic recording head having narrow recording gap and perpendicular magnetic recording apparatus using the same |
-
1997
- 1997-08-14 JP JP23335097A patent/JPH1166503A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6657813B2 (en) | 2000-02-28 | 2003-12-02 | Hitachi, Ltd. | Perpendicular magnetic recording system |
US7088548B2 (en) | 2000-02-28 | 2006-08-08 | Hitachi Global Storage Technologies Japan, Ltd. | Perpendicular magnetic recording system |
US6707643B2 (en) | 2000-09-25 | 2004-03-16 | Kabushiki Kaisha Toshiba | Perpendicular magnetic recording head having narrow recording gap and perpendicular magnetic recording apparatus using the same |
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