JPS63166001A - Magnetic reproducing device - Google Patents

Magnetic reproducing device

Info

Publication number
JPS63166001A
JPS63166001A JP31533986A JP31533986A JPS63166001A JP S63166001 A JPS63166001 A JP S63166001A JP 31533986 A JP31533986 A JP 31533986A JP 31533986 A JP31533986 A JP 31533986A JP S63166001 A JPS63166001 A JP S63166001A
Authority
JP
Japan
Prior art keywords
magnetic
signal
film
region
frequency
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.)
Pending
Application number
JP31533986A
Other languages
Japanese (ja)
Inventor
Shigeru Yatabe
谷田部 茂
Junichi Akiyama
純一 秋山
Hitoshi Iwasaki
仁志 岩崎
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP31533986A priority Critical patent/JPS63166001A/en
Publication of JPS63166001A publication Critical patent/JPS63166001A/en
Pending 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
    • G11B5/33Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only
    • G11B5/332Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using thin films
    • 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
    • G11B5/33Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only

Abstract

PURPOSE:To improve reproducing sensitivity and a frequency character without increasing noise, by setting the film thickness of an area being connected to a resonance circuit of magnetic material film larger than that of the area which detects a signal magnetic field. CONSTITUTION:The magnetic material film 1 consists of the area 11 connected to the coil 2 of the resonance circuit 4 and the area 12 which detects the signal magnetic field from a magnetic recording medium, and the film thickness of the coupling area 11 is formed larger than that of the detecting area 12. Therefore, the film thickness of the detecting area 12 is thin, and the diamagnetic field of the magnetic material film 1 in a direction of length is suppressed, thereby, the signal magnetic field H can be detected with resulting superior sensitivity. Also, the coupling area 11 of the magnetic material field 1 and the coil 2 of the resonance circuit 4 are coupled electromagnetically, and is taken out as a reproducing signal output Vout via a peak detection circuit 10. In this case, the noise of the output is increased when the coil 2 is coupled with the magnetic material film 1 and it depends on the film thickness of the coupling area 11. In such a way, it is possible to improve the reproducing sensitivity and the frequency characteristic and to effectively reduce the noise included in the output of a reproducing signal.

Description

【発明の詳細な説明】 C発明の目的] (産業上の利用分野) 本発明は磁気記録媒体に記録された信号を再生する装置
に係り、特に磁気記録媒体からの信号磁界を磁性体膜の
高周波磁気特性の変化として検出して再生を行なう磁気
的再生装置に関する。
[Detailed Description of the Invention] CObject of the Invention] (Industrial Field of Application) The present invention relates to an apparatus for reproducing signals recorded on a magnetic recording medium, and in particular, the present invention relates to a device for reproducing signals recorded on a magnetic recording medium. The present invention relates to a magnetic reproduction device that performs reproduction by detecting changes in high frequency magnetic characteristics.

(従来の技術) 磁気記録媒体に記録された信号を再生する装置において
、高密度記録再生に極めて適した方式として、磁気記録
媒体に記録された信号に基づく信号磁界を、磁性体膜の
高周波磁気特性の変化、例えば高周波透磁率の実部およ
びその虚部の変化として検出し、この高周波磁気特性の
変化を利用して再生を行なう方式が既に出願されている
(特開昭57−36407号公報等)。
(Prior Art) In an apparatus for reproducing signals recorded on a magnetic recording medium, as a method extremely suitable for high-density recording and reproducing, a signal magnetic field based on a signal recorded on a magnetic recording medium is transmitted to a high-frequency magnetic field of a magnetic film. A method has already been filed in which a change in characteristics is detected, for example, a change in the real part of high-frequency magnetic permeability and a change in its imaginary part, and reproduction is performed using this change in high-frequency magnetic characteristics (Japanese Patent Laid-Open No. 57-36407). etc).

第6図はこの方式に基づく磁気的再生装置の従来技術に
よる構成を示したものであり、磁性体膜1と結合した薄
膜導体からなるコイル2および共振用コンデンサ3によ
り構成される共振回路4に、高周波発振器5から結合用
コンデンサ6を介して例えば600〜700MH2程度
の周波数の高周波信号を供給し、磁気記録媒体(図示せ
ず)からの信号磁界Hによる磁性体111の高周波透磁
率の変化に応じた共振回路4の高周波信号出力の変化を
検出回路、例えばダイオード7、コンデンサ8および抵
抗9により構成されるピーク検波回路1oによって検出
し、磁気記録媒体に記録された信号に対応した再生信号
出力■outを得るものである。
FIG. 6 shows a prior art configuration of a magnetic reproducing device based on this method, in which a resonant circuit 4 consisting of a coil 2 made of a thin film conductor coupled to a magnetic film 1 and a resonant capacitor 3 is shown. A high frequency signal with a frequency of, for example, about 600 to 700 MH2 is supplied from the high frequency oscillator 5 via the coupling capacitor 6, and the high frequency permeability of the magnetic body 111 changes due to the signal magnetic field H from the magnetic recording medium (not shown). A detecting circuit, for example, a peak detecting circuit 1o composed of a diode 7, a capacitor 8, and a resistor 9, detects a change in the high-frequency signal output of the resonant circuit 4 according to the response, and outputs a reproduced signal corresponding to the signal recorded on the magnetic recording medium. ■It is something to get out.

すなわち、磁気記録媒体からの信号磁界Hにより磁性体
!11の高周波磁気特性が変化すると、共振回路4の共
振周波数やQが変化することにより、共振回路4に供給
されている高周波信号が振幅変調を受けるので、この振
幅変調を受けた信号をピーク検波回路10で検波するこ
とで、再生信号出゛ 力VOutを得ることができる。
In other words, the signal magnetic field H from the magnetic recording medium causes the magnetic material! When the high-frequency magnetic characteristics of 11 change, the resonant frequency and Q of the resonant circuit 4 change, and the high-frequency signal supplied to the resonant circuit 4 undergoes amplitude modulation, so the signal that has undergone this amplitude modulation is peak-detected. By detecting the signal in the circuit 10, a reproduced signal output VOut can be obtained.

このような磁気的再生装置において、再生信号出力yo
utの大きさは磁性体1111の膜厚dに依存すること
が知られている。すなわち、膜厚dが大きいと磁性体膜
1の長さhの方向の反磁界が増大し、磁気記録媒体から
の信号磁界Hを感度よく検出できないが、磁性体111
の幅Wおよび長さhに比べて膜厚dが非常に小さければ
、この反磁界が小さくなり、感度の高い良好な再生が可
能となる。
In such a magnetic reproducing device, the reproduced signal output yo
It is known that the size of ut depends on the film thickness d of the magnetic material 1111. That is, when the film thickness d is large, the demagnetizing field in the direction of the length h of the magnetic film 1 increases, and the signal magnetic field H from the magnetic recording medium cannot be detected with high sensitivity.
If the film thickness d is very small compared to the width W and length h of , this demagnetizing field becomes small and good reproduction with high sensitivity becomes possible.

また、磁気記録媒体を磁性体膜1の膜厚dの方向に移動
させた場合の再生信号出力voutの周波数特性を測定
すると、リング型磁気ヘッドのギャップ損失と同様の効
果によって、膜厚dとほぼ等しい記録波長に相当する周
波数で再生信号出力v outは急激に低下する。換言
すれば膜厚dが小さい程、記録波長の短い信号の再生が
できる。
Furthermore, when the frequency characteristics of the reproduced signal output vout when the magnetic recording medium is moved in the direction of the film thickness d of the magnetic film 1 are measured, it is found that due to an effect similar to the gap loss of a ring-type magnetic head, the film thickness d The reproduced signal output v out sharply decreases at a frequency corresponding to approximately the same recording wavelength. In other words, the smaller the film thickness d, the more signals with shorter recording wavelengths can be reproduced.

このように再生感度や周波数特性の面からは、磁性体1
11の膜厚dは小さい方が好ましい。ところが、本発明
者らの研究によれば、磁性体膜1の膜厚dを小さくする
と、再生信号出力voutに含まれるノイズが増大する
ことが見出された。
In this way, from the perspective of reproduction sensitivity and frequency characteristics, magnetic material 1
It is preferable that the film thickness d of No. 11 is smaller. However, according to research conducted by the present inventors, it has been found that when the film thickness d of the magnetic film 1 is reduced, the noise included in the reproduced signal output vout increases.

第7図は磁性体膜111としてNi−Fe合金薄膜を用
いた場合のノイズ対周波数特性を磁性体膜1の膜厚dを
種々変えて示したものである。同図に示すように、膜厚
dが0.4μm〜0.2μm〜0.1μmと小さくなる
に従って、ノイズは増大している。
FIG. 7 shows the noise versus frequency characteristics when a Ni--Fe alloy thin film is used as the magnetic film 111 with various thicknesses d of the magnetic film 1. As shown in the figure, the noise increases as the film thickness d decreases from 0.4 μm to 0.2 μm to 0.1 μm.

(発明が解決しようとする問題点) このように従来の磁気的再生装置では、磁気記録媒体か
らの信号磁界を検出する磁性体膜の膜厚を小さくすると
、再生感度や周波数特性は向上するが、再生信号出力に
含まれるノイズが増大すると、いう問題があった。
(Problems to be Solved by the Invention) In this way, in conventional magnetic reproducing devices, if the thickness of the magnetic film that detects the signal magnetic field from the magnetic recording medium is reduced, the reproducing sensitivity and frequency characteristics improve. , there is a problem in that the noise included in the reproduced signal output increases.

従って、本発明はノイズの増大を伴なうことなく、再生
感度および周波数特性の向上を達成できる磁気的再生装
置を提供することを目的とする。
Accordingly, an object of the present invention is to provide a magnetic reproducing device that can improve reproduction sensitivity and frequency characteristics without increasing noise.

[発明の構成〕 (問題点を解決するための手段) 本発明では、磁気記録媒体に記録された信号に基づく信
号磁界を検出して高周波磁気特性が変化する磁性体膜と
、この磁性体膜に結合され、高周波信号が供給されるこ
とによって該磁性体膜に^周波磁界を印加するとともに
、該磁性体膜の高周波磁気特性の変化に伴なってその高
周波信号出力が変化する共振回路と、、この共振回路の
高周波信号出力の変化を検出して磁気記録媒体に記録さ
れた信号を再生する検出回路とを備えた磁気的再生装置
において、磁性体膜の共振回路と結合する領域の膜厚を
、信号磁界を検出する領域の膜厚より大きくしたことを
特徴とする。
[Structure of the Invention] (Means for Solving the Problems) The present invention provides a magnetic film whose high frequency magnetic properties change by detecting a signal magnetic field based on a signal recorded on a magnetic recording medium, and a magnetic film that changes high frequency magnetic properties by detecting a signal magnetic field based on a signal recorded on a magnetic recording medium. a resonant circuit that is coupled to and applies a ^-frequency magnetic field to the magnetic film by being supplied with a high-frequency signal, and whose high-frequency signal output changes as the high-frequency magnetic characteristics of the magnetic film change; In a magnetic reproducing device equipped with a detection circuit that detects a change in the high frequency signal output of this resonant circuit and reproduces a signal recorded on a magnetic recording medium, the film thickness of the region of the magnetic film that is coupled to the resonant circuit. is larger than the film thickness of the region where the signal magnetic field is detected.

(作用) 本発明においては、磁性体膜の磁気記録媒体からの信号
磁界を検出する領域は膜厚が小さいため、反磁界が小さ
く、信号磁界を高感度に検出する。また、この領域の膜
厚が小さいことは、周波数特性の面でも有利となる。
(Function) In the present invention, since the region of the magnetic film that detects the signal magnetic field from the magnetic recording medium has a small film thickness, the demagnetizing field is small and the signal magnetic field is detected with high sensitivity. Furthermore, a small film thickness in this region is advantageous in terms of frequency characteristics.

一方、再生出力に含まれるノイズの主な成分は、本発明
者らの検討によると磁性体膜に共振回路を結合させ磁性
体膜に高周波磁界を作用させたときに初めて現われるも
のであり、このことからノイズは主として磁性体IW!
;4のうち共振回路と結合する領域で発生する。従って
、この領域の膜厚を大きくすれば、磁性体膜の膜厚に依
存するノイズは減少することになる。
On the other hand, the main components of noise included in the reproduced output appear only when a resonant circuit is coupled to the magnetic film and a high-frequency magnetic field is applied to the magnetic film, according to studies by the present inventors. Therefore, the noise is mainly caused by the magnetic material IW!
;Of 4, it occurs in the region that couples with the resonant circuit. Therefore, if the film thickness in this region is increased, the noise that depends on the film thickness of the magnetic film will be reduced.

(実論例) 第1図は本発明の一実施例に係る磁気的再生装置の構成
を示したものであり、磁性体膜1と結合したi[I導体
からなるコイル2および共振用コンデンサ3により共振
回路4(高周波回路)を構成し、この共振回路4に高周
波発振器5から結合用コンデンサ6を介して例えば60
0〜700MH2というような非常に高い周波数の高周
波信号を供給し、磁気記録媒体からの信号磁界Hによる
磁性体l111の高周波透磁率等の高周波磁気特性の変
化に応じた共振回路4の高周波信号出力の変化を検出回
路、例えばダイオード7、コンデンサ8および抵抗9に
より構成されるピーク検波回路10によって検出して、
磁気記録媒体に記録された信号に対応した再生出力■o
utを得る、という基本的な構成は第6図に示した従来
装置と同様である。
(Example of Practical Theory) FIG. 1 shows the configuration of a magnetic reproducing device according to an embodiment of the present invention. A resonant circuit 4 (high-frequency circuit) is configured, and a high-frequency oscillator 5 is connected to a high-frequency oscillator 5 via a coupling capacitor 6 to form a resonant circuit 4 (high-frequency circuit).
The high frequency signal output of the resonant circuit 4 is performed by supplying a high frequency signal with a very high frequency such as 0 to 700 MH2, and responding to changes in high frequency magnetic properties such as high frequency permeability of the magnetic material 111 due to the signal magnetic field H from the magnetic recording medium. A change in is detected by a detection circuit, for example, a peak detection circuit 10 composed of a diode 7, a capacitor 8, and a resistor 9,
Playback output corresponding to the signal recorded on the magnetic recording medium
The basic configuration of obtaining ut is the same as the conventional device shown in FIG.

なお、磁性体膜1およびコイル2は、iiI膜技術によ
り図示しない再生ヘッド基板上に形成される。
The magnetic film 1 and the coil 2 are formed on a reproducing head substrate (not shown) using III film technology.

ここで、磁性体iiは共振回路4のコイル2と結合する
領域(以下、結合領域という)11と、磁気記録媒体か
らの信号磁界を検出する領域(以下、検出領域という)
12とからなり、結合領域11の膜厚が検出傾i*12
の膜厚より大きくなっている。
Here, the magnetic body ii has a region 11 that couples with the coil 2 of the resonant circuit 4 (hereinafter referred to as the coupling region) and a region that detects the signal magnetic field from the magnetic recording medium (hereinafter referred to as the detection region).
12, and the film thickness of the bonding region 11 is the detection slope i*12
It is larger than the film thickness of .

このような構成にすると、検出領域12は膜厚が小さい
ので、磁性体ll11の長さ方向の反磁界が抑制される
ことにより、信号磁界Hを感度よく検出でき、また記録
波長のより短い信号の再生ができる。すなわち、再生感
度および周波数特性とも良好な特性が得られる。
With this configuration, since the detection area 12 has a small film thickness, the demagnetizing field in the length direction of the magnetic body 111 is suppressed, so that the signal magnetic field H can be detected with high sensitivity, and the signal magnetic field H can be detected with a shorter recording wavelength. can be played. That is, good reproduction sensitivity and frequency characteristics can be obtained.

一方、結合領域11の膜厚が大きいことにより、再生信
号出力Voutに含まれるノイズが低減する。
On the other hand, since the film thickness of the coupling region 11 is large, noise included in the reproduced signal output Vout is reduced.

すなわち、信号磁界Hにより磁性体WA1は磁化し、こ
れによる結合領域11の高周波磁気特性の変化は、磁性
体Illの結合領域11と共振回路4コイル2とが電磁
的に結合することで、共振回路4の共振周波数やQの変
化として検出され、この変化がピーク検波回路10を介
して再生信号出力■Outとして取出される。この場合
、観測される出力のノイズは、コイル2を磁性体111
に結合させたときの方が大きく、例えば図のように高周
波発振器5をコイル2に接続したままコイル2を磁性体
ll11から離した場合は、観測される出力のノイズは
小さくなる(勿論、信号成分は観測されない)。このこ
とよりノイズの主な成分は磁性体膜1とコイル2との電
磁結合が強い部分、すなわち結合領域11の膜厚に依存
して第7図に示した関係から発生するものと推測される
。従って、この結合領域11の膜厚を大きくすることで
、再生信号出力voutに含まれるノイズは効果的に減
少することになる。
That is, the magnetic body WA1 is magnetized by the signal magnetic field H, and the resulting change in the high frequency magnetic characteristics of the coupling region 11 is caused by the electromagnetic coupling between the coupling region 11 of the magnetic body Ill and the coil 2 of the resonant circuit 4, which causes resonance. It is detected as a change in the resonant frequency or Q of the circuit 4, and this change is taken out via the peak detection circuit 10 as a reproduced signal output ■Out. In this case, the observed output noise is caused by connecting the coil 2 to the magnetic material 111.
For example, if the high-frequency oscillator 5 is connected to the coil 2 and the coil 2 is separated from the magnetic material ll11 as shown in the figure, the observed output noise will be smaller (of course, the signal components are not observed). From this, it is inferred that the main component of noise is generated from the relationship shown in FIG. 7 depending on the film thickness of the coupling region 11, which is the part where the electromagnetic coupling between the magnetic film 1 and the coil 2 is strong. . Therefore, by increasing the thickness of the coupling region 11, the noise contained in the reproduced signal output vout can be effectively reduced.

なお、信号磁界Hによる磁性体膜1の高周波磁気特性の
変化は、検出領域12のみならず結合鎖li!11にも
及び、それによって高周波磁気特性の変化が共振回路4
の共振周波数やQの変化に変換されるわけであるが、前
述した反磁界の抑制効果(短波長記録信号に対する再生
感度)や周波数特性は、検出領域12、すなわち信号磁
界Hが強く検出される領域の膜厚に大きく依存するので
、結合鎖[11の膜厚が大きくとも再生感度および周波
数特性に悪影響が及ぶことはない。
Note that the change in the high frequency magnetic properties of the magnetic film 1 due to the signal magnetic field H affects not only the detection region 12 but also the bond chain li! 11, thereby causing a change in the high frequency magnetic properties of the resonant circuit 4.
However, the above-mentioned suppression effect of the demagnetizing field (reproduction sensitivity to short wavelength recorded signals) and frequency characteristics are such that the detection region 12, that is, the signal magnetic field H is strongly detected. Since it largely depends on the film thickness of the region, even if the film thickness of the bonding chain [11 is large, the reproduction sensitivity and frequency characteristics are not adversely affected.

上述した結合領域11と検出傾1J112の膜厚が異な
る磁性体111は、例えば第2図や第3図に示す方法に
よって得ることができる。第2図は磁性体111全体を
結合領域11の膜厚で蒸着、スパッタリング等により形
成した後、検出領域12の部分のみをエツチング、逆ス
パッタリングまたはイオンミリング等の方法で所要の膜
厚となるまで薄くする方法である。
The magnetic material 111 in which the coupling region 11 and the detection slope 1J112 have different thicknesses can be obtained, for example, by the method shown in FIGS. 2 and 3. In FIG. 2, the entire magnetic material 111 is formed by vapor deposition, sputtering, etc. to the thickness of the coupling region 11, and then only the detection region 12 is formed by etching, reverse sputtering, ion milling, etc. until the required film thickness is achieved. This is a method to make it thinner.

第3図は磁性体膜1全体を検出領域12の膜厚で形成し
た後、結合領域11の部分にさらに第2層の磁性体膜1
3を選択的に形成する方法である。
FIG. 3 shows that after the entire magnetic film 1 has been formed to the thickness of the detection region 12, a second layer of magnetic film 1 is further formed on the coupling region 11.
This is a method of selectively forming 3.

この場合、第2層の磁性体1113は磁性体1111と
同一材質でもよいが、結合領域11に設けられるものな
ので、検出領域12と別の材質の軟磁性体であっても十
分である。
In this case, the second layer magnetic material 1113 may be made of the same material as the magnetic material 1111, but since it is provided in the coupling region 11, it is sufficient that it is a soft magnetic material made of a different material from the detection region 12.

第4図は本発明の他の実施例を示したもので、結合領域
11と検出領域12とを蛎々に形成し、これらを例えば
因のように一部で重ねることによって磁気的に結合した
ものである。この場合、結合領域11と検出領域12と
は同一材質でもよいし、異なった材質であってもよい。
FIG. 4 shows another embodiment of the present invention, in which a coupling region 11 and a detection region 12 are formed in the shape of a spider, and are magnetically coupled by partially overlapping them, for example. It is something. In this case, the coupling region 11 and the detection region 12 may be made of the same material or may be made of different materials.

第5図は本発明のさらに別の実施例を示すもので、磁気
記録媒体がベース1i121の上に裏打ち高透磁率層2
2を介して膜面に垂直方向に磁化容易軸を有する磁気記
録層23を形成した垂直磁気記録媒体20の場合である
FIG. 5 shows yet another embodiment of the present invention, in which a magnetic recording medium is arranged on a base 1i121 with a high magnetic permeability layer 2
This is the case of a perpendicular magnetic recording medium 20 in which a magnetic recording layer 23 having an axis of easy magnetization in a direction perpendicular to the film surface is formed with a magnetic recording layer 23 interposed therebetween.

このような垂直磁気記録媒体20に記録された信号を再
生する場合は、磁性体膜1の検出領域12側(磁気記録
媒体20に対向する側)と反対側(結合領域11)の端
部と媒体20との間に磁性体ヨーク14を介在させ、磁
性体ll11と裏打ち高透磁率層22および磁性体ヨー
ク14によって磁気回路を構成する。
When reproducing a signal recorded on such a perpendicular magnetic recording medium 20, it is necessary to A magnetic yoke 14 is interposed between the magnetic material 111 and the medium 20, and a magnetic circuit is constituted by the magnetic material 111, the high magnetic permeability lining layer 22, and the magnetic material yoke 14.

このような磁気回路を形成すると、磁性体111の検出
領域12の反磁界は小さくなることが知られているが、
周波数特性を向上するためには検出領域12の膜厚をや
はり十分に小さくする必要がある。そこで、この実施例
においても結合領域11の膜厚を検出領域12の膜厚よ
り大きくすることで、先と同様の原理によりノイズを低
減させている。
It is known that when such a magnetic circuit is formed, the demagnetizing field in the detection region 12 of the magnetic body 111 becomes smaller.
In order to improve the frequency characteristics, it is necessary to make the film thickness of the detection region 12 sufficiently small. Therefore, in this embodiment as well, the thickness of the coupling region 11 is made larger than the thickness of the detection region 12, thereby reducing noise based on the same principle as described above.

本発明は上記した実施例に限定されるものではなく、そ
の要旨を逸脱しない範囲で種々変形して実施することが
できる。
The present invention is not limited to the embodiments described above, and can be implemented with various modifications without departing from the gist thereof.

[発明の効果] 本発明によれば、磁気記録媒体からの信号磁界を検出す
るとともに、共振回路と結合する磁性体膜の共振回路の
結合領域の膜厚を、信号磁界を検出する領域の膜厚より
太き(することによって、再生感度および周波数特性の
向上を図ると同時に、再生信号出力な含まれるノイズを
効果的に低減させることができる。
[Effects of the Invention] According to the present invention, the signal magnetic field from the magnetic recording medium is detected, and the film thickness of the coupling region of the resonant circuit of the magnetic film coupled to the resonant circuit is determined by the thickness of the film in the region where the signal magnetic field is detected. By making it thicker than the thickness, it is possible to improve the reproduction sensitivity and frequency characteristics, and at the same time, effectively reduce the noise contained in the reproduction signal output.

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

第1図は本発明の一実施例に係る磁気的再生装置の構成
図、第2図および第3図は同実施例における磁性体膜の
形成方法を説明するための図、第4図および第5図はそ
れぞれ本発明の他の実施例に係る磁気的再生装置の構成
図、第6図は従来の磁気的再生装置の構成図、第7図は
従来の磁気的再生装置における磁性体膜の膜厚とノイズ
との関係を示す図である。 1・・・磁性体膜、2・・・コイル、3・・・共振用コ
ンデンサ、4・・・共振回路、5・・・高周波発振器、
6・・・結合用コンデンサ、7・・・ダイオード、8・
・・コンデンサ、9・・・抵抗、10・・・ピーク検波
回路(検出回路)、11・・・結合領域、12・・・検
出領域、13・・・第2層磁性体躾、14・・・磁性体
ヨーク、20・・・垂直磁気記録媒体、21・・・ベー
ス層、22・・・裏打ち高透磁率層、23・・・磁気記
録層。 出願人代理人 弁理士 鈴江武彦 第1図 第2図 第3図 第 4 図 第5図
FIG. 1 is a block diagram of a magnetic reproducing device according to an embodiment of the present invention, FIGS. 2 and 3 are diagrams for explaining a method of forming a magnetic film in the same embodiment, and FIGS. 5 is a block diagram of a magnetic reproducing device according to another embodiment of the present invention, FIG. 6 is a block diagram of a conventional magnetic reproducing device, and FIG. 7 is a block diagram of a magnetic film in a conventional magnetic reproducing device. FIG. 3 is a diagram showing the relationship between film thickness and noise. DESCRIPTION OF SYMBOLS 1... Magnetic film, 2... Coil, 3... Resonant capacitor, 4... Resonant circuit, 5... High frequency oscillator,
6... Coupling capacitor, 7... Diode, 8...
... Capacitor, 9... Resistor, 10... Peak detection circuit (detection circuit), 11... Coupling area, 12... Detection area, 13... Second layer magnetic material control, 14... - Magnetic material yoke, 20... Perpendicular magnetic recording medium, 21... Base layer, 22... Backing high permeability layer, 23... Magnetic recording layer. Applicant's Representative Patent Attorney Takehiko Suzue Figure 1 Figure 2 Figure 3 Figure 4 Figure 5

Claims (6)

【特許請求の範囲】[Claims] (1)磁気記録媒体に記録された信号に基づく信号磁界
を検出して高周波磁気特性が変化する磁性体膜と、この
磁性体膜に結合され、高周波信号が供給されることによ
って該磁性体膜に高周波磁界を印加するとともに、該磁
性体膜の高周波磁気特性の変化に伴なってその高周波信
号出力が変化する共振回路と、この共振回路の高周波信
号出力の変化を検出して前記磁気記録媒体に記録された
信号を再生する検出回路とを備えた磁気的再生装置にお
いて、 前記磁性体膜の前記共振回路と結合する領域の膜厚を、
前記信号磁界を検出する領域の膜厚より大きくしたこと
を特徴とする磁気的再生装置。
(1) A magnetic film whose high-frequency magnetic properties change by detecting a signal magnetic field based on a signal recorded on a magnetic recording medium, and a magnetic film that is coupled to this magnetic film and is supplied with a high-frequency signal. A high-frequency magnetic field is applied to the magnetic recording medium, and a resonant circuit whose high-frequency signal output changes as the high-frequency magnetic characteristics of the magnetic film changes, and a change in the high-frequency signal output of this resonant circuit is detected to detect the magnetic recording medium. a detection circuit for reproducing a signal recorded on a magnetic reproducing device, the film thickness of a region of the magnetic film coupled to the resonant circuit;
A magnetic reproducing device characterized in that the thickness of the signal magnetic field is greater than that of a region where the signal magnetic field is detected.
(2)磁性体膜は信号磁界を検出する領域および共振回
路と結合する領域が一体に形成され、信号磁界を検出す
る領域がエッチング、逆スパッタリングまたはイオンミ
リング等により薄く加工されたものであることを特徴と
する特許請求の範囲第1項記載の磁気的再生装置。
(2) The magnetic film must have a region that detects the signal magnetic field and a region that couples with the resonant circuit integrally formed, and the region that detects the signal magnetic field must be thinned by etching, reverse sputtering, ion milling, etc. A magnetic reproducing device according to claim 1, characterized in that:
(3)磁性体膜は共振回路と結合する領域が選択的に2
層構造に形成されたものであることを特徴とする特許請
求の範囲第1項記載の磁気的再生装置。
(3) The magnetic film selectively has two regions that couple with the resonant circuit.
The magnetic reproducing device according to claim 1, characterized in that it is formed in a layered structure.
(4)磁性体膜の共振回路と結合する領域における第2
層が軟磁性体からなることを特徴とする特許請求の範囲
第3項記載の磁気的再生装置。
(4) The second region in the region coupled to the resonant circuit of the magnetic film
4. The magnetic reproducing device according to claim 3, wherein the layer is made of a soft magnetic material.
(5)磁性体膜は共振回路と結合する領域と信号磁界を
検出する領域とが別々に形成され、これらの両領域が磁
気的に結合されたものであることを特徴とする特許請求
の範囲第1項記載の磁気的再生装置。
(5) Claims characterized in that the magnetic film has a region that couples with a resonant circuit and a region that detects a signal magnetic field are formed separately, and these two regions are magnetically coupled. 2. The magnetic reproducing device according to item 1.
(6)磁性体膜の磁気記録媒体に対向する側と反対側の
端部と磁気記録媒体との間に磁性体ヨークを設けたこと
を特徴とする特許請求の範囲第1項記載の磁気的再生装
置。
(6) A magnetic yoke according to claim 1, characterized in that a magnetic yoke is provided between the end of the magnetic film on the side opposite to the magnetic recording medium and the magnetic recording medium. playback device.
JP31533986A 1986-12-26 1986-12-26 Magnetic reproducing device Pending JPS63166001A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP31533986A JPS63166001A (en) 1986-12-26 1986-12-26 Magnetic reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP31533986A JPS63166001A (en) 1986-12-26 1986-12-26 Magnetic reproducing device

Publications (1)

Publication Number Publication Date
JPS63166001A true JPS63166001A (en) 1988-07-09

Family

ID=18064217

Family Applications (1)

Application Number Title Priority Date Filing Date
JP31533986A Pending JPS63166001A (en) 1986-12-26 1986-12-26 Magnetic reproducing device

Country Status (1)

Country Link
JP (1) JPS63166001A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05189726A (en) * 1992-01-09 1993-07-30 Nippon Telegr & Teleph Corp <Ntt> Magneto-resistance effect type magnetic head

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05189726A (en) * 1992-01-09 1993-07-30 Nippon Telegr & Teleph Corp <Ntt> Magneto-resistance effect type magnetic head

Similar Documents

Publication Publication Date Title
CA2044047A1 (en) Magnetic pole configuration for high density thin film recording head
US4677512A (en) Magnetic reproducing apparatus
US4635152A (en) Magnetic resonance-type playback apparatus including a magnetic material having magnetic anisotropy
US5910870A (en) Magnetoresistive effect composite head with laminated magnetic layer isolated from magnetic pole layer
JPS63166001A (en) Magnetic reproducing device
JPH03286413A (en) Magneto-resistance effect type head
JPH0229904A (en) Perpendicular magnetic recording head
JP3160947B2 (en) Magnetoresistive magnetic head
JPH0327963B2 (en)
JP2878738B2 (en) Recording / reproducing thin film magnetic head
JPS60129907A (en) Magnetic reproducer
JPS6057520A (en) Magnetic head
JPH061524B2 (en) Magnetic reproducing device
JPS60185214A (en) Magnetic head
JPS6371914A (en) Reproducing head
JPH01184709A (en) Thin film magnetic head
JPS60209906A (en) Ring head for vertical magnetic recording
EP0088099A1 (en) Method for recording information on magnetic tape and head for recording information on and reproducing information from magnetic tape
JPS60138703A (en) Magnetic reproducing device
JPH01159814A (en) Recording and reproducing composite type magnetic head
JPS60151818A (en) Vertical magnetic head
JPS60138704A (en) Magnetic reproducing device
JPS61271603A (en) Magnetic reproducing device
JPH0554337A (en) Production of magneto-resistance effect type head
JPS6028005A (en) Magnetic recording and reproducing device