JPS60138703A - Magnetic reproducing device - Google Patents

Magnetic reproducing device

Info

Publication number
JPS60138703A
JPS60138703A JP24457183A JP24457183A JPS60138703A JP S60138703 A JPS60138703 A JP S60138703A JP 24457183 A JP24457183 A JP 24457183A JP 24457183 A JP24457183 A JP 24457183A JP S60138703 A JPS60138703 A JP S60138703A
Authority
JP
Japan
Prior art keywords
magnetic
signal
coupling
frequency
inductance element
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
JP24457183A
Other languages
Japanese (ja)
Inventor
Shigeru Yatabe
谷田部 茂
Junichi Akiyama
純一 秋山
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 JP24457183A priority Critical patent/JPS60138703A/en
Publication of JPS60138703A publication Critical patent/JPS60138703A/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

Abstract

PURPOSE:To reproduce a signal recorded with high density on a narrow track while keeping high sensitivity and excellent S/N by arranging inductance elements orthogonally to a recording layer of a magnetic recording medium while clipping a magnetic substance to form a high-frequency coupling circuit. CONSTITUTION:A support base 11 made of a high-hardness insulating material is arranged vertically in opposition to a recording layer 1 of the magnetic recording medium 3, the secondary side inductance element 7b made of a band- shape thin film conductor in the broadwise direction of a recording track 5 is formed on the tip side face of the base 11 with coating, a thin film magnetic substance 6 is formed through coating so that a part of the lower end is overlapped on the element 7b and the primary-side inductance element 7a made of a band-shape thin film conductor is formed through coating so as to be orthogonal to the element 7b on the magnetic substance 6. As a result, a high-frequency signal applied to the primary side of the high-frequency coupling circuit appears at the secondary side as a change in an output of the high-frequency signal through the change in the degree of coupling by the change of the high-frequency characteristic of the magnetic substance 6 and a signal reproducing output 16 is formed by a peak detection circuit 15.

Description

【発明の詳細な説明】 [発明の技術分野] この発明は磁気記録された信号を再生する装置に係り、
特に磁気記録媒体が形成する信号磁界の変化による磁性
体の高周波特性の変化を利用して再生を行なう磁気記録
再生装置に関する。
[Detailed Description of the Invention] [Technical Field of the Invention] The present invention relates to a device for reproducing magnetically recorded signals,
In particular, the present invention relates to a magnetic recording and reproducing apparatus that performs reproduction by utilizing changes in the high frequency characteristics of a magnetic material due to changes in a signal magnetic field formed by a magnetic recording medium.

[発明の技術的前!−とその間°照点コ従゛来一般の磁
気記録再生装置は、リング型の磁気ヘッドを用い、記録
の場合はヘッドのギャップに発生させた信号磁界で磁気
記録媒体を磁化して記録を行ない、再生は媒体からの磁
束変化によるヘッドの誘起起電力を再生出力として取り
出す方式であった。この方式では、面内配向の磁気記録
媒体を使用する場合、記録波長を短かくすればするほど
減磁界の効果が強まって記録を困難にし、再生において
もリング型磁気ヘッドが磁束検出型であることで再生出
力がトラック幅に依存するため、原理的に高曲度記録再
生には不利であった。
[Technical pre-invention! Conventional magnetic recording and reproducing devices use a ring-shaped magnetic head, and when recording, the magnetic recording medium is magnetized by a signal magnetic field generated in the gap between the heads. For reproduction, the electromotive force induced in the head due to changes in magnetic flux from the medium was extracted as reproduction output. In this method, when using a magnetic recording medium with in-plane orientation, the shorter the recording wavelength, the stronger the demagnetizing field effect becomes, making recording difficult, and the ring-shaped magnetic head is a magnetic flux detection type even during playback. As a result, the reproduction output depends on the track width, which is fundamentally disadvantageous for recording and reproduction of high curvature.

一方、最近注目されている垂直磁気記録方式は信号磁化
を磁気記録媒体の面に垂直な方向に向けて記録を行なう
方式のため、記録波長を短かくした方が記録が安定する
といった特徴をもつことがら^密度記録に適した方式で
ある。しかし、垂直磁気記録方式でも再生にはリング型
ヘッド又は主磁極と副磁極からなるヘッド構成など磁束
検出の方式が従来用いられているため、面内配向の場合
と同様に再生出力がトラック幅による制限を受ける。
On the other hand, the perpendicular magnetic recording method, which has recently been attracting attention, records by directing the signal magnetization in a direction perpendicular to the surface of the magnetic recording medium, so it has the characteristic that recording becomes more stable when the recording wavelength is shortened. This method is suitable for density recording. However, even with perpendicular magnetic recording, a magnetic flux detection method such as a ring-shaped head or a head configuration consisting of a main magnetic pole and a sub-magnetic pole is conventionally used for reproduction, so the reproduction output depends on the track width as in the case of in-plane orientation. subject to restrictions.

ところで、特願昭55−110340号等において提案
されている磁気再生装置は、磁気記録媒体からの信号磁
界の変化を透磁率や高周波損失等の特性変化として検出
する磁性体を設け、この磁性体に巻回したコイル(イン
ダクタンス素子〉のインダクタンス変化を利用して再生
を行なうものである。この装置では、上記コイルがキャ
パシタンス素子とともに同調回路を構成し、この同調回
路に高周波信号が供給される。この場合、磁気記録媒体
からの信号磁界の強さによって生じる上記磁性体の特性
変化によって、同調回路の共振周波数やQの変化が起こ
り高周波信号が振幅変調を受ける。従って振幅変調を受
けた信号を検波回路で検出することで、・再生出力が得
られる。
By the way, the magnetic reproducing device proposed in Japanese Patent Application No. 110340/1983 is equipped with a magnetic material that detects changes in the signal magnetic field from a magnetic recording medium as changes in characteristics such as magnetic permeability and high frequency loss. Regeneration is performed by utilizing changes in inductance of a coil (inductance element) wound around the oscillator. In this device, the coil constitutes a tuned circuit together with a capacitance element, and a high-frequency signal is supplied to this tuned circuit. In this case, changes in the characteristics of the magnetic material caused by the strength of the signal magnetic field from the magnetic recording medium cause changes in the resonant frequency and Q of the tuning circuit, causing the high frequency signal to undergo amplitude modulation. By detecting it with a detection circuit, a reproduced output can be obtained.

この方式で用いられる高透磁率の磁性体の高周波での透
磁率及び損失は、微弱な外部磁界の変化に対しても著し
い変化を示す上、上記のようにこの磁性体により信号磁
界を検出して再生を行なうと再生出力レベルが信号磁界
の強度に依存し磁束に゛は依存しないことにより、原理
的に極めて狭トラツク幅の高密度磁気再生が可能となる
The magnetic permeability and loss at high frequencies of the high-permeability magnetic material used in this method change significantly even with changes in a weak external magnetic field, and as mentioned above, the signal magnetic field cannot be detected by this magnetic material. When reproduction is performed, the reproduction output level depends on the strength of the signal magnetic field and does not depend on the magnetic flux, so that high-density magnetic reproduction with an extremely narrow track width is theoretically possible.

ところで、この方式による磁気再生装置として、特に信
号磁界による磁性体の高周波特性の変化により結合度が
変化する高周波結合回路を構成し、この高周波結合回路
からの高周波出力電圧の変化を検出して信号再生出力を
得るようにしたものが既に提案されている(特願昭〜号
)。この場合、信号磁界による磁性体の高周波特性の変
化に対し高周波結合回路の結合度変化をいかに大きくす
るかが、高感度、高S/Nの信号再生を行なう上で重要
な課題となる。
By the way, a magnetic reproducing device using this method includes a high-frequency coupling circuit in which the degree of coupling changes due to a change in the high-frequency characteristics of a magnetic material caused by a signal magnetic field, and detects changes in the high-frequency output voltage from this high-frequency coupling circuit to generate a signal. A device that obtains a playback output has already been proposed (Special Application No. Sho-1). In this case, how to increase the change in the coupling degree of the high frequency coupling circuit with respect to the change in the high frequency characteristics of the magnetic material due to the signal magnetic field becomes an important issue in performing signal reproduction with high sensitivity and high S/N.

[発明の目的] この発明の目的は、磁気記録媒体からの信号磁界による
磁性体の高周波特性変化によって高周波結合回路の結合
度が大きく変化するようにして、狭トラツク幅で高密度
に記録された信号を極めて高感度にかつ良好なS/Nを
もって再生することを可能とした磁気再生装置を提供す
ることである。
[Objective of the Invention] The object of the present invention is to record data at high density with a narrow track width so that the coupling degree of the high-frequency coupling circuit changes greatly due to changes in the high-frequency characteristics of the magnetic material due to the signal magnetic field from the magnetic recording medium. It is an object of the present invention to provide a magnetic reproducing device capable of reproducing signals with extremely high sensitivity and good S/N ratio.

[発明の概要] ゛この発明は、磁気記録媒体からの信号磁界による磁性
体の高周波特性の変化によって結合度が変化する高周波
結合回路を構成する1次側インダクタンス素子および2
次側インダクタンス素子を磁気記録媒体の記録層側に、
画素子間に磁性体を挾んで互いに直交させて配置し、こ
の高周波結合回路の結合度の変化に基く高周波信号出力
を検出して、磁気記録媒体に記録された信号を再生する
ようにしたことを特徴としている。
[Summary of the Invention] ゛The present invention provides a primary side inductance element and a secondary
The next inductance element is placed on the recording layer side of the magnetic recording medium,
A magnetic material is sandwiched between the pixel elements and arranged orthogonally to each other, and the high frequency signal output based on the change in the degree of coupling of this high frequency coupling circuit is detected to reproduce the signal recorded on the magnetic recording medium. It is characterized by

[発明の効果] この発明によれば、信号磁界による磁性体のテンソル透
磁率等の高周波特性の変化を利用して高周波結合回路の
結合度を変化させて、磁気記録媒体からの信号磁界を検
出する際、高周波結合回路を構成する1次側および2次
側のインダクタンス素子が直交しているため、無信号時
では電磁結合がほとんどなく、高周波結合回路から得ら
れる高周波出力はわずかであるが、信号磁界が磁性体に
加わるとテンソル透磁率によって新たな電磁結合が発生
し、これが高周波出力の大きな変化として現れるため、
高感度かつS/Nの良好な信号再生出力が得られる。
[Effects of the Invention] According to the present invention, a signal magnetic field from a magnetic recording medium is detected by changing the degree of coupling of a high-frequency coupling circuit by using changes in high-frequency characteristics such as tensor permeability of a magnetic material caused by a signal magnetic field. Because the inductance elements on the primary and secondary sides that make up the high-frequency coupling circuit are orthogonal, there is almost no electromagnetic coupling when there is no signal, and the high-frequency output obtained from the high-frequency coupling circuit is small. When a signal magnetic field is applied to a magnetic material, new electromagnetic coupling occurs due to tensor magnetic permeability, and this appears as a large change in high frequency output.
Signal reproduction output with high sensitivity and good S/N ratio can be obtained.

また、高周波結合回路を構成する1次側および2次側の
インダクタンス素子の両方を磁性体とともに磁気記録媒
体の記録層側に配置するため、これらを例えば一つの支
持基体上に積層形成することにより、再生ヘッドをコン
パクトに一体化することができるという利点がある。
In addition, in order to arrange both the primary side and secondary side inductance elements constituting the high frequency coupling circuit on the recording layer side of the magnetic recording medium together with the magnetic material, it is possible to laminate them on one support base, for example. This has the advantage that the playback head can be integrated in a compact manner.

[発明の実施例] 第1図はこの発明の一実施例を示すものである。[Embodiments of the invention] FIG. 1 shows an embodiment of the present invention.

記録層1とベース層2からなる磁気記録媒体3の記録層
1に信号磁化4による記録トラック5が形成され、この
記録媒体3上に信号磁化4による信号磁界により高周波
特性が変化する磁性体6が記録トラック5に当接し、か
つ対向させて配置されている。
A recording track 5 based on signal magnetization 4 is formed on the recording layer 1 of a magnetic recording medium 3 consisting of a recording layer 1 and a base layer 2, and a magnetic material 6 whose high frequency characteristics change due to the signal magnetic field caused by the signal magnetization 4 is formed on this recording medium 3. are placed in contact with and facing the recording track 5.

磁性体6は板状または薄膜状の磁性体であり、その一方
の面に接して1次側インダクタンス素子7aが設けられ
ている。この1次側インダクタンス素子7aは同調用コ
ンデンサ8aとともにLCC同調回路路構成し、このL
CIiili1!回路には高周波発振器9から高周波結
合用コンデンサ10を介して高周波信号が供給される。
The magnetic body 6 is a plate-shaped or thin-film magnetic body, and a primary inductance element 7a is provided in contact with one surface thereof. This primary side inductance element 7a constitutes an LCC tuning circuit path together with a tuning capacitor 8a, and this LCC
CIiiili1! A high frequency signal is supplied to the circuit from a high frequency oscillator 9 via a high frequency coupling capacitor 10.

また、磁性体6の他方の面に接して、1次側インダクタ
ンス素子7aと幾何学的に直交する様に2次側インダク
タンス素子7bが設けられている。この2次側インダク
タンス素子7bも同調用コンデンサ8bとともにLC同
調回路を構成する。この2次側LC同調回路と1次側L
C同調回路および磁性体6によって高周波結合回路が形
成されている。ここで高周波発振器9の発振周波数と、
高周波結合回路の1次側および2次側のLC同調回路の
同調周波数はほぼ一致させておく。
Further, a secondary inductance element 7b is provided in contact with the other surface of the magnetic body 6 so as to be geometrically perpendicular to the primary inductance element 7a. This secondary inductance element 7b also constitutes an LC tuning circuit together with the tuning capacitor 8b. This secondary side LC tuning circuit and the primary side L
A high frequency coupling circuit is formed by the C tuning circuit and the magnetic body 6. Here, the oscillation frequency of the high frequency oscillator 9,
The tuning frequencies of the LC tuning circuits on the primary side and the secondary side of the high frequency coupling circuit are made substantially the same.

なお、このように構成される高周波結合回路の具体的な
実装構造としては、例えば図に示すように磁気記録媒体
3の記録層1上に対向して、ガラスやサファイヤ等の高
硬度絶縁材料からなる支持基体11を垂直に配置し、こ
の支持基体11の先端側側面上に記録トラック5の幅方
向に帯状の薄膜導体からなる2次側インダクタンス素子
7bを被着形成し、この2次側インダクタンス素子7b
に下端側が一部重なるように薄膜の磁性体6を被着形成
し、さらにこの磁性体6上に2次側インダクタンス素子
7bと直交するように帯状のWIM導、体からなる1次
側インダクタンス7aを被着形成すればよい。
The specific mounting structure of the high frequency coupling circuit configured in this way is, for example, as shown in the figure, a high frequency coupling circuit made of high hardness insulating material such as glass or sapphire, facing the recording layer 1 of the magnetic recording medium 3. A supporting base 11 is arranged vertically, and a secondary inductance element 7b made of a strip-shaped thin film conductor is formed on the side surface of the leading end side of the supporting base 11 in the width direction of the recording track 5. Element 7b
A thin film magnetic body 6 is deposited so that its lower end side partially overlaps the magnetic body 6, and a primary inductance 7a made of a strip-shaped WIM conductor is disposed on the magnetic body 6 so as to be perpendicular to the secondary inductance element 7b. It is sufficient to deposit and form.

上記のように1次側インダクタンス素子7aと2次側イ
ンダクタンス素子7bを直交させると、両インダクタン
ス素子7a、7bのみに−よる高周波結合回路の電磁結
合はほとんどない。しかしインダクタンス素子7a、7
bの間に磁性体6があるため、記録トラック5にある信
号磁化4からの信号磁界を受けて磁性体6が磁気共鳴等
の高周波特性の変化を起こすと、磁性体6を介して高周
波結合回路の1次側と2次側の電磁結合が新たに磁性体
6のテンソル透磁率によって発生する。
When the primary inductance element 7a and the secondary inductance element 7b are orthogonal to each other as described above, there is almost no electromagnetic coupling in the high frequency coupling circuit due only to the two inductance elements 7a and 7b. However, the inductance elements 7a, 7
Since there is a magnetic material 6 between b, when the magnetic material 6 receives a signal magnetic field from the signal magnetization 4 in the recording track 5 and causes a change in high frequency characteristics such as magnetic resonance, high frequency coupling occurs via the magnetic material 6. Electromagnetic coupling between the primary side and the secondary side of the circuit is newly generated due to the tensor magnetic permeability of the magnetic body 6.

このため高周波結合回路の1次側に供給された高周波信
号は、信号磁界により生じた磁性体6の高周波特性の変
化による結合度の変化によって、2次側に高周波信号出
力の変化として現れる。そこでこの高周波信号出力を検
出回路、例えばダイオード12と抵抗13およびコンデ
ンサ14からなるピーク検波回路15で検出することに
より、検波出力として信号再生出力16が得られる。
Therefore, the high frequency signal supplied to the primary side of the high frequency coupling circuit appears as a change in the high frequency signal output on the secondary side due to a change in the degree of coupling due to a change in the high frequency characteristics of the magnetic body 6 caused by the signal magnetic field. Therefore, by detecting this high frequency signal output with a detection circuit, for example, a peak detection circuit 15 consisting of a diode 12, a resistor 13, and a capacitor 14, a signal reproduction output 16 is obtained as a detection output.

こように1、無信号時には高周波結合回路の電気回路と
しての電磁結合がほとんどないため、2次側の高周波信
号出力として得られる成分は主に信号磁界の変化に起因
し、このことより高感度、高S/Nの信号再生出力が得
られる。また、高周波結合回路の1次側、2次側とも磁
気記録媒体の記録層側に配置するので、再生ヘッドの一
体化が容易となり、装置構成上極めて有利である。
In this way, 1. When there is no signal, there is almost no electromagnetic coupling in the electric circuit of the high-frequency coupling circuit, so the component obtained as the high-frequency signal output on the secondary side is mainly due to changes in the signal magnetic field, which makes it possible to achieve high sensitivity. , high S/N signal reproduction output can be obtained. Furthermore, since both the primary and secondary sides of the high-frequency coupling circuit are arranged on the recording layer side of the magnetic recording medium, it is easy to integrate the reproducing head, which is extremely advantageous in terms of device configuration.

第2図はこの発明の他の実施例を示したもので、1次側
インダクタンス素子7aと磁性体6との間に、1次側イ
ンダクタンス素子7a側に絶縁膜18を介してシールド
用の導電体膜17を配置したものである。この実施例に
よれば、1次側インダクタンス素子7aと2次側インダ
クタンス素子7bの直交による電磁結合の抑制効果が導
電体膜17によるシールド効果によって更に上がるため
、信号再生出力16のS/Nを一層向上させることがで
きる。
FIG. 2 shows another embodiment of the present invention, in which a conductive film for shielding is provided between the primary inductance element 7a and the magnetic body 6 via an insulating film 18 on the primary inductance element 7a side. A body membrane 17 is arranged. According to this embodiment, the effect of suppressing electromagnetic coupling due to orthogonality between the primary inductance element 7a and the secondary inductance element 7b is further increased by the shielding effect of the conductive film 17, so that the S/N of the signal reproduction output 16 is increased. This can be further improved.

なお、この発明は上述した実施例に限定されるものでは
なく、例えば磁気記録媒体が面内配向の記録媒体の場合
でも垂直磁気記録媒体の場合でもこの発明を同様に適用
できる。また高周波結合回路を構成する場合に、磁性体
6の高周波特性変化に基づかない電磁結合を減少させる
ため、1次側と2次側のインダクタンス素子7a、7b
の相対的配置を調整できる手段を付加してもよい。さら
に無信号時の電磁結合を小さくしたり、磁性体6の高周
波特性変化を大きくする目的で、磁性体6にバイアス磁
界を与えてもよいことは勿論である。
Note that the present invention is not limited to the embodiments described above, and the present invention can be similarly applied, for example, to cases where the magnetic recording medium is an in-plane oriented recording medium or a perpendicular magnetic recording medium. In addition, when configuring a high frequency coupling circuit, in order to reduce electromagnetic coupling that is not based on changes in high frequency characteristics of the magnetic body 6, inductance elements 7a and 7b on the primary side and the secondary side are used.
A means for adjusting the relative arrangement of the two may be added. Furthermore, it goes without saying that a bias magnetic field may be applied to the magnetic body 6 in order to reduce electromagnetic coupling when there is no signal or to increase changes in the high frequency characteristics of the magnetic body 6.

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

第1図はこの発明の一実施例に係る磁気再生装置の構成
を示す図、第2図は他の実施例を示す図である。 1・・・記録層、2・・・ベース層、3・・・磁気記録
媒体、4・・・信号磁化、5・・・記録トラック、6・
・・磁性体、7a、7b・・・1次側および2次側イン
ダクタンス素子、8a、8b・・・同調用コンデンサ、
9・・・高周波発振器、10・・・高周波結合用コンデ
ンサ、11・・・支持基体、15・・・検波回路、16
・・・信号再生出力、17・・・シールド用導電体膜。 第1図 第2図
FIG. 1 is a diagram showing the configuration of a magnetic reproducing apparatus according to one embodiment of the present invention, and FIG. 2 is a diagram showing another embodiment. DESCRIPTION OF SYMBOLS 1... Recording layer, 2... Base layer, 3... Magnetic recording medium, 4... Signal magnetization, 5... Recording track, 6...
...Magnetic material, 7a, 7b...Primary side and secondary side inductance elements, 8a, 8b...Tuning capacitor,
9... High frequency oscillator, 10... High frequency coupling capacitor, 11... Support base, 15... Detection circuit, 16
...Signal reproduction output, 17...Conductor film for shielding. Figure 1 Figure 2

Claims (1)

【特許請求の範囲】 (1)磁気記録媒体からの信号磁界による磁性体の高周
波特性の変化により結合度が変化する高周波結合回路を
有し、この高周波結合回路の結合度の変化に基く高周波
出力電圧の変化を検出して、前記磁気記録媒体に記録さ
れた信号を再生する装置において、前記高周波結合回路
は前記磁気記録媒体の記録層側に対向しかつ前記磁性体
を間に挾んで互いに直交して配置された1次側および2
次側インダクタンス素子を含んで構成されていることを
特徴とする磁気再生装置。 (′2 高周波結合回路は、信号磁界による前記磁性体
の磁気共鳴によって1次側インダクタンス素°子と2次
側インダクタンス素子との結合度が変化するものである
ことを特徴とする特許請求の範囲第1項記載の磁気再生
装置。 (3)高周波結合回路は、信号磁界がないときは1次側
インダクタンス素子と2次側インダクタンス素子との電
磁結合がほとんどなく、前記磁性体の磁気共鳴によって
大きい電磁結合を生じるものであることを特徴とする特
許請求の範囲第1項または第2項記載の磁気再生装置。 (4)前記磁性体と1次側および2゛次側インダクタン
ス素子が同一の支持基体上に積層形成されていることを
特徴とする特許請求の範囲第1項〜第3項のいずれかに
記載の磁気再生装置。
[Scope of Claims] (1) A high-frequency coupling circuit whose degree of coupling changes due to a change in the high-frequency characteristics of a magnetic material due to a signal magnetic field from a magnetic recording medium, and a high-frequency output based on a change in the degree of coupling of this high-frequency coupling circuit. In an apparatus for detecting a change in voltage and reproducing a signal recorded on the magnetic recording medium, the high frequency coupling circuits are arranged opposite to the recording layer side of the magnetic recording medium and orthogonal to each other with the magnetic body interposed therebetween. The primary and secondary
A magnetic reproducing device comprising a next-side inductance element. ('2) The high-frequency coupling circuit is characterized in that the degree of coupling between the primary inductance element and the secondary inductance element changes due to the magnetic resonance of the magnetic body caused by the signal magnetic field. The magnetic reproducing device according to paragraph 1. (3) In the high-frequency coupling circuit, when there is no signal magnetic field, there is almost no electromagnetic coupling between the primary inductance element and the secondary inductance element, and the magnetic coupling is large due to the magnetic resonance of the magnetic body. The magnetic reproducing device according to claim 1 or 2, characterized in that the magnetic reproducing device generates electromagnetic coupling. (4) The magnetic body and the primary and secondary inductance elements are supported on the same side. A magnetic reproducing device according to any one of claims 1 to 3, characterized in that the magnetic reproducing device is formed in layers on a base.
JP24457183A 1983-12-27 1983-12-27 Magnetic reproducing device Pending JPS60138703A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP24457183A JPS60138703A (en) 1983-12-27 1983-12-27 Magnetic reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP24457183A JPS60138703A (en) 1983-12-27 1983-12-27 Magnetic reproducing device

Publications (1)

Publication Number Publication Date
JPS60138703A true JPS60138703A (en) 1985-07-23

Family

ID=17120695

Family Applications (1)

Application Number Title Priority Date Filing Date
JP24457183A Pending JPS60138703A (en) 1983-12-27 1983-12-27 Magnetic reproducing device

Country Status (1)

Country Link
JP (1) JPS60138703A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63113902A (en) * 1986-10-31 1988-05-18 Toshiba Corp Magnetic reproducing device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63113902A (en) * 1986-10-31 1988-05-18 Toshiba Corp Magnetic reproducing device

Similar Documents

Publication Publication Date Title
CA1203898A (en) Magnetic recording and reproducing apparatus
JPH0414745B2 (en)
JPH0323962B2 (en)
US4677512A (en) Magnetic reproducing apparatus
US4635152A (en) Magnetic resonance-type playback apparatus including a magnetic material having magnetic anisotropy
KR100257106B1 (en) Magnetic head unit, method of manufacturing the same and magnetic recording and reproducing apparatus using the same
JPH0370844B2 (en)
JPH0370843B2 (en)
JPS60138703A (en) Magnetic reproducing device
JPH05234170A (en) Magnetic head
JPS60138704A (en) Magnetic reproducing device
JPS60129907A (en) Magnetic reproducer
JPS6028007A (en) Magnetic recording and reproducing device
JPS5848203A (en) Magnetic recording and reproducing device
JPS6028005A (en) Magnetic recording and reproducing device
JPS6028006A (en) Magnetic recording and reproducing device
JPS626419A (en) Magnetic head
JPH0344363B2 (en)
JPH01184709A (en) Thin film magnetic head
JP2878738B2 (en) Recording / reproducing thin film magnetic head
JPH0344362B2 (en)
CA1203899A (en) Magnetic recording and reproducing apparatus
JPS60129906A (en) Magnetic reproducer
JPS5812105A (en) Magnetic reproducer
JPS593706A (en) Magnetic recording and reproducing device