JPS60129907A - Magnetic reproducer - Google Patents

Magnetic reproducer

Info

Publication number
JPS60129907A
JPS60129907A JP23866283A JP23866283A JPS60129907A JP S60129907 A JPS60129907 A JP S60129907A JP 23866283 A JP23866283 A JP 23866283A JP 23866283 A JP23866283 A JP 23866283A JP S60129907 A JPS60129907 A JP S60129907A
Authority
JP
Japan
Prior art keywords
magnetic
high frequency
inductance element
recording medium
signal
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
JP23866283A
Other languages
Japanese (ja)
Inventor
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 JP23866283A priority Critical patent/JPS60129907A/en
Publication of JPS60129907A publication Critical patent/JPS60129907A/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

Landscapes

  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To attain the reproduction of signals with an extremely high S/N and high sensitivity by setting inductances of the primary and secondary sides orthogonal to each other for a high-frequency coupling circuit having its coupling degree changing with the high-frequency characteristics of a magnetic substance due to a signal magnetic field given from a magnetic recording medium. CONSTITUTION:An inductance element 7 of the primary side is obtained by forming a thin film conductor on the end face of the 1st substrate 10. While an inductance element 8 of the secondary side is obtained by coating a thin film conductor on the plane of the 2nd substrate 11 at the area near a magnetic recording medium 1. A magnetic substance 9 is obtained by providing a minute magnetic substance between the substance 11 and the thin film conductor forming the element 8. The high frequency energy which is produced by the electromagnetic connection secured between both elements 7 and 8 in terms of an electric circuit and transmitted to the secondary side from the primary side can be extremely suppressed since those elements 7 and 8 are orthogonal to each other. Thus this energy is almost equal to the changing component of a signal magnetic field. This ensures the reproduction of signals with an extremely high S/N and high sensitivity.

Description

【発明の詳細な説明】 [弁明の技術分野] この発明は、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による磁
性体の高周波特性の変化を利用して信号再生を行なう磁
気再生装置に関する。
[Detailed Description of the Invention] [Technical Field of Defense] The present invention relates to a device for reproducing signals recorded on a magnetic recording medium, and in particular to a device that reproduces signals recorded on a magnetic recording medium, and in particular, utilizes changes in the high frequency characteristics of a magnetic material due to a signal magnetic field from the magnetic recording medium. The present invention relates to a magnetic reproducing device for reproducing signals.

[発明の技術的背景とその問題点] 従来の面内配向型の磁気記録媒体を利用する磁気記録再
生方式は、リング型の磁気ヘッドを用い、記録の場合は
ヘッドの巻線に電流を流してヘッドのギャップに発生す
る磁界で媒体を磁化して信号を記録し、一方、再生の場
合は媒体の信号磁化に応じてこれに誘起される起電力を
再生出力として取り出す方式でめる。この方式では、記
録に関しては記録波長が短くなればなるほど減磁界の効
果が強くなって記録が回能となるし、さらに再生に関し
てはリング型のヘッド自体が本来、11束検出型である
ことにより再生出力の大きさが1−ラック幅に依存する
ため、本質的に高密度記録再生には不利であった。
[Technical background of the invention and its problems] The conventional magnetic recording and reproducing method using an in-plane oriented magnetic recording medium uses a ring-shaped magnetic head, and in the case of recording, current is passed through the winding of the head. The magnetic field generated in the gap between the heads magnetizes the medium and records signals, while for reproduction, the electromotive force induced by the signal magnetization of the medium is extracted as a reproduction output. In this system, the shorter the recording wavelength, the stronger the demagnetizing field effect becomes, making the recording more efficient.Furthermore, the ring-shaped head itself is originally an 11-bundle detection type, and as for reproduction, the ring-shaped head itself is originally an 11-flux detection type. Since the magnitude of the reproduction output depends on the 1-rack width, it is essentially disadvantageous for high-density recording and reproduction.

一方、最近提案されている垂直磁気記録再生方式は信号
磁化が媒体の面に垂直な方向となるように記録する方式
であるため、減磁界による悪影響が無く、記録信号が短
波長であればあるほど安定した記録が可能であり、本質
的に高密度記録に適している。しかしながら、再生に関
してはやはり磁束検出型であっ゛C再生出力の大きさが
トラック幅に依存するため、S/Nや再生感度の観点に
立つと、特にトラック幅方向の高密度化に自ずと限界が
ある。 − そこで、磁気記録媒体からの信号磁界を検出することに
よって、再生を行なう方式が提案されている。この方式
は磁気ヘッドとして磁性体にインダクタンス素子を結合
したものを用い、この磁気ヘッドを同調素子のひとつと
して同調回路を構成し、磁気記録媒体からの磁界の変化
により磁気ヘッドを構成する磁性体の透磁率が変わり同
調周波数が変わること、または磁気記録媒体からの磁界
の変化により同調回路のQが変化すること、あるいはこ
れらの両方を利用し、同調周波数やQの変化を電圧の変
化として取り出すようにしたものである。この方式によ
れば磁気記録媒体からのわずかな信号磁界の変化に対し
ても大きな電圧の変化が1号られ、従って記録トラック
幅が狭くてもS/Nが極めて良好な再生出力を得ること
ができ、これにより高密度記録再生が可能となるもので
ある。
On the other hand, the recently proposed perpendicular magnetic recording/reproduction method records in such a way that the signal magnetization is perpendicular to the surface of the medium, so there is no negative effect from demagnetizing fields and recording signals can be recorded with short wavelengths. This enables more stable recording and is essentially suitable for high-density recording. However, playback is still of the magnetic flux detection type, and since the magnitude of the C playback output depends on the track width, from the standpoint of S/N and playback sensitivity, there is a natural limit to increasing the density, especially in the track width direction. be. - Therefore, a method has been proposed in which reproduction is performed by detecting a signal magnetic field from a magnetic recording medium. This method uses a magnetic head with an inductance element coupled to a magnetic material, and uses this magnetic head as one of the tuning elements to configure a tuning circuit. Changes in the magnetic field from the magnetic recording medium cause the magnetic material constituting the magnetic head to change. The tuning frequency changes due to changes in magnetic permeability, or the Q of the tuning circuit changes due to changes in the magnetic field from the magnetic recording medium, or both of these are used to extract changes in the tuning frequency and Q as changes in voltage. This is what I did. According to this method, even a slight change in the signal magnetic field from the magnetic recording medium causes a large voltage change, and therefore it is possible to obtain a reproduction output with an extremely good S/N ratio even if the recording track width is narrow. This enables high-density recording and reproduction.

一般に、磁気ヘッドに用いられる高透磁率の磁性体は高
周波領域では強磁性共鳴吸収現象を起し、これに伴う高
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。従って、上述したような磁性体
により信号磁界を検出して再生を行なう方式は、再生出
力レベルが信号磁界の強度に依存しtxt束には依存し
ないことより、原理的に狭1−ラック幅の高密度磁気記
録再生に適している。
In general, magnetic materials with high magnetic permeability used in magnetic heads cause a ferromagnetic resonance absorption phenomenon in the high frequency range, and the accompanying magnetic permeability and loss at high frequencies change significantly even with changes in the weak external magnetic field. show. Therefore, the above-mentioned method of detecting the signal magnetic field using a magnetic material and performing reproduction is theoretically suitable for a narrow 1-rack width, since the reproduction output level depends on the strength of the signal magnetic field and does not depend on the Txt flux. Suitable for high-density magnetic recording and reproduction.

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
1qるようにしたものが既に提案されている。この場合
、信号磁界により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人きくするかが、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 in which the playback output is reduced by 1q has already been proposed. In this case, how to make the change in the degree of coupling of the high frequency coupling circuit sensitive 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t+i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惨めで高感度にかつ良りI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[発明の概要] この弁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り結合度が変化する高周波結合回
路を、磁気記録媒体のベース層側に高周波信号が供給さ
れる1次側インダクタンス素子を、また記録層側に2次
側インダクタンス素子を、直交して対向するように配置
して構成し、2次側インダクタンス素子を上記磁性体と
結合させるように構成して、磁気記録媒体に記録された
信号を、この高周波結合回路の高周波出力電圧の変化と
して取出して再生することを特徴としている。
[Objective of the Invention] An 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 the change in the high frequency characteristics of the magnetic material due to the signal t+i field from the magnetic recording medium. A signal with high sensitivity and good I S
,/N [Summary of the Invention] This defense is based on a magnetic reproducing device that is capable of reproducing data with a signal magnetic field from a magnetic recording medium, and the degree of coupling changes due to a change in the high frequency characteristics of a magnetic material. The coupling circuit is configured by arranging a primary inductance element to which a high frequency signal is supplied on the base layer side of the magnetic recording medium and a secondary inductance element on the recording layer side so as to face each other at right angles, The secondary inductance element is configured to be coupled with the magnetic material, and the signal recorded on the magnetic recording medium is extracted and reproduced as a change in the high frequency output voltage of the high frequency coupling circuit.

[発明の効果コ この発明によれば、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により結合度が変化づる高周波結合
回路の1次側および2次側インダクタンスが直交するよ
うに対向しているため、両者間にはほとんど電気回路的
な電磁結合は無いが、磁気記録媒体からの信号磁界によ
り磁性体が高周波特性の変化、例えば強磁性共鳴現象に
よるテンツル透磁率の変化を生じると、両者間の結合度
が大きく変化する。
[Effects of the Invention] According to the present invention, the primary and secondary inductances of a high frequency coupling circuit whose degree of coupling changes depending on the high frequency characteristics of the magnetic material due to the signal magnetic field from the magnetic recording medium are opposed so as to be perpendicular to each other. Therefore, there is almost no electromagnetic coupling between the two in the form of an electric circuit, but if the signal magnetic field from the magnetic recording medium causes a change in the high-frequency characteristics of the magnetic material, such as a change in Tentzle permeability due to the ferromagnetic resonance phenomenon, the two The degree of connectivity between them changes greatly.

従って、磁気記録媒体に記録された信号変化によって高
周波結合回路の電磁結合に大きな変化を生じ、2次側へ
の高周波エネルギの流入量が大きく変化づ“るため、信
号の変化分に相当する高周波エネルギだけが前記2次側
へ伝達されることになって、極めて高S /’ N、高
感度の信号再生が可能となる。
Therefore, a change in the signal recorded on the magnetic recording medium causes a large change in the electromagnetic coupling of the high-frequency coupling circuit, and the amount of high-frequency energy flowing into the secondary side changes greatly. Only the energy is transmitted to the secondary side, making it possible to reproduce signals with extremely high S/'N and high sensitivity.

さらに、この弁明ては1次側および2次側インダクタン
ス素子が磁気′記録媒体を挾んで対向していることから
、1次側に供給された高周波信号°により発生する高周
波磁界は、磁性体の特性変化に伴い2次側インダクタン
スと同じ記録層側にある磁性体に対し、媒体表面に近い
先端部分、ず′なわち記録波長の短い高密度記録信号に
基く信号磁界が集中している領域側から印加される。こ
のため、前記磁性体の先端部分でm性体が強磁性共鳴を
より起し易くなり、この点で一層短波長側で高感度な再
生が期待できる。
Furthermore, since the primary and secondary inductance elements are opposed to each other with the magnetic recording medium in between, the high-frequency magnetic field generated by the high-frequency signal supplied to the primary side is generated by the magnetic material. As the characteristics change, the magnetic material is located on the same recording layer side as the secondary inductance, and the tip part near the medium surface, that is, the area where the signal magnetic field based on the high-density recording signal with a short recording wavelength is concentrated. Applied from For this reason, the m-type material is more likely to cause ferromagnetic resonance at the tip of the magnetic material, and in this respect, highly sensitive reproduction can be expected on the shorter wavelength side.

[弁明の実施例] 図はこの発明の一実施例を示すものである。1は矢印へ
方向に走行する磁気記録媒体、2,3はそのベース層お
よび記録層、4は記録トラック、5は記録された信号磁
化を示し、この磁気記録媒体1を挾む形で、この発明に
基く再生へラド6が配置されている。
[Example of explanation] The figure shows an example of the present invention. 1 is a magnetic recording medium running in the direction of the arrow, 2 and 3 are its base layer and recording layer, 4 is a recording track, and 5 is a recorded signal magnetization. A regeneration radar 6 according to the invention is arranged.

再生へラド6は、磁気記録媒体1のベース層2側に記録
1〜ラツク4の長さ方向に沿って配置された細長い板状
またはIHtA状の1次側インダクタンス素子7と、記
録層3側に記録トラック4の幅方向に配置されたやはり
細長い板状または薄膜状の2次側インダクタンス素子8
、および2次側インダクタンス素子8に結合して設けら
れ磁気記録媒体1からの信号磁界により高周波特性が変
化する磁性体9からなる高周波結合回路を主体として構
成されている。
The reproduction head 6 includes an elongated plate-shaped or IHtA-shaped primary inductance element 7 arranged along the length direction of the recording 1 to rack 4 on the base layer 2 side of the magnetic recording medium 1, and a primary inductance element 7 arranged on the recording layer 3 side. A secondary inductance element 8, also in the form of an elongated plate or thin film, is arranged in the width direction of the recording track 4.
, and a magnetic body 9 which is coupled to the secondary inductance element 8 and has its high frequency characteristics changed by the signal magnetic field from the magnetic recording medium 1.

なお、再生へラド6の具体的な実装構造として−は、例
えば1次側インダクタンス素子7については第1の基板
10の端面上に薄膜導体を被着することにより形成でき
、2次側インダクタンス素子8についても第2の基板1
1のm気記録媒体1近傍の平面上に薄膜導体を被着する
ことにより形成できる。また磁性体9については、基板
11ど2次側インダクタンス素子8を構成する薄膜導体
との間に微小な薄膜磁性体を被着づればよい。
As for the specific mounting structure of the reproducing electrode 6, for example, the primary inductance element 7 can be formed by depositing a thin film conductor on the end surface of the first substrate 10, and the secondary inductance element 7 can be formed by depositing a thin film conductor on the end surface of the first substrate 10. 8 also for the second substrate 1
It can be formed by depositing a thin film conductor on a plane near the recording medium 1 of 1 m. As for the magnetic material 9, a fine thin film magnetic material may be deposited between the substrate 11 and the thin film conductor constituting the secondary inductance element 8.

1次側インダクタンス素子7は同調用コンデンサ12と
ともに高周波結合回路の1次側同調回路を構成し、一方
、2次側インダクタンス素子8も同様に同調用コンデン
サ15とともに前記高周波結合回路の2次側同調回路を
構成する。これら1次側と2次側の同調回路は同調周波
数を一致あるいはほぼ一致させておく。
The primary side inductance element 7 constitutes the primary side tuning circuit of the high frequency coupling circuit together with the tuning capacitor 12, and the secondary side inductance element 8 similarly constitutes the secondary side tuning circuit of the high frequency coupling circuit together with the tuning capacitor 15. Configure the circuit. The tuning frequencies of these primary and secondary tuning circuits are made to match or almost match.

1次側同調回路に高周波結合用のコンデンサ13を介し
て高周波源14から高周波信号を供給すると、1次側イ
ンダクタンス素子7から高周波磁界が発生され、これが
磁性体9と結合する。ここで、1次側インダクタンス素
子7と2次側インダクタンス素子′8は直交しているた
め、電気回路としての電磁的結合はほとんど無い。とこ
ろが、磁気記録媒体1を磁性体9と当接しながら、矢印
へ方向に走行せしめると、信号磁化5によって形成され
る信号磁界が磁性体9に加わるので、前記同調周波数を
磁性体9が強磁性共鳴吸収を起す周波数に合わせておく
と、この信号磁界の変化によつU rn磁性体のテンソ
ル透磁率が変化する。その結果、インダクタンス素子7
.8が大きな電磁結合を生じ、信号磁界の変化に応じた
高周波エネルギが高周波結合回路の1次側同調回路から
2次側同調回路へと流入することとなる。従って2次側
同調回路のコンデンサ15の両端に、信号磁界の変化に
応じた高周波出力電圧が現われる。そこでこれをピーク
検波回路16で検波することにより゛、磁気記録媒体1
に記録された信号の再生出力17を得ることができる。
When a high frequency signal is supplied from the high frequency source 14 to the primary side tuning circuit via the high frequency coupling capacitor 13, a high frequency magnetic field is generated from the primary side inductance element 7, and this is coupled with the magnetic body 9. Here, since the primary inductance element 7 and the secondary inductance element '8 are orthogonal to each other, there is almost no electromagnetic coupling as an electric circuit. However, when the magnetic recording medium 1 is moved in the direction of the arrow while in contact with the magnetic material 9, the signal magnetic field formed by the signal magnetization 5 is applied to the magnetic material 9, so that the tuning frequency is changed to the magnetic material 9 due to its ferromagnetic nature. When tuned to a frequency that causes resonance absorption, the tensor permeability of the Urn magnetic material changes due to changes in this signal magnetic field. As a result, the inductance element 7
.. 8 causes a large electromagnetic coupling, and high frequency energy corresponding to changes in the signal magnetic field flows from the primary side tuning circuit of the high frequency coupling circuit to the secondary side tuning circuit. Therefore, a high frequency output voltage corresponding to the change in the signal magnetic field appears across the capacitor 15 of the secondary side tuning circuit. Therefore, by detecting this with the peak detection circuit 16, the magnetic recording medium 1
It is possible to obtain a reproduction output 17 of the signal recorded in the .

このように、インダクタンス素子7.8が直交関係にあ
ることから1次側から2次側へ伝達される高周波エネル
ギは、両インダクタンス素子7゜8間の電気回路的な電
磁的結合によるものが極力抑えられ、はとんど信号磁界
の変化分だけからなる。このため極めて高S/N、高感
度の信号再生ができるという利点がある。
In this way, since the inductance elements 7 and 8 are in an orthogonal relationship, the high frequency energy transmitted from the primary side to the secondary side is due to electromagnetic coupling between the two inductance elements 7 and 8 as much as possible. is suppressed and consists mostly of changes in the signal magnetic field. Therefore, it has the advantage of being able to reproduce signals with extremely high S/N and high sensitivity.

また、高周波磁界は1次側インダクタンス素子7から磁
気記録媒体1を通して磁性体9に加わるため、媒体1の
表面の極く近傍に存在する短波長領域の信号磁界に対す
る検出感度が向上し、長波長領域の信号磁界に対する検
出感度が相対的に低下するので、記録波長の短い高密度
記録信号の再生に一層有利となり、再生周波数帯域も特
に高周波域側に拡大されるという効果がある。
Furthermore, since the high-frequency magnetic field is applied to the magnetic body 9 from the primary inductance element 7 through the magnetic recording medium 1, the detection sensitivity to the signal magnetic field in the short wavelength range that exists very close to the surface of the medium 1 is improved, and Since the detection sensitivity to the signal magnetic field in the region is relatively lowered, it becomes more advantageous for reproducing high-density recorded signals with short recording wavelengths, and the reproduction frequency band is also expanded particularly to the high frequency side.

なお、この発明は上記実施例に限定されるものではなく
、例えば必要に応じて磁性体9に適当な直流バイアス磁
界を加えてもよい。また磁気記録媒体が垂直磁気記録媒
体の場合も同様の効果が1qられる。さらに再生信号の
検出手段に関しては、検波する前にあらかじめ同調用コ
ンデンサ15の両端に現われた高周波信号を増幅してか
らピーク検波する等の手段であってもよい。
It should be noted that the present invention is not limited to the above-mentioned embodiment, and for example, an appropriate DC bias magnetic field may be applied to the magnetic body 9 as necessary. Further, when the magnetic recording medium is a perpendicular magnetic recording medium, a similar effect of 1q can be obtained. Furthermore, the means for detecting the reproduced signal may be a means for amplifying the high frequency signal appearing at both ends of the tuning capacitor 15 before detecting the signal, and then performing peak detection.

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

図はこの発明の一実施例に係る磁気再生装置の′構成を
示す図である。 1・・・txt気記録媒体、2・・・ベース層、3・・
・記録層、4・・・記録トラック、5・・・信号磁化、
6・・・再生ヘッド、7・・・1次側インダクタンス素
子、8・・・2次側−インダクタンス素子、9・・・磁
性体、io、il・・・基板、12.15・・・同調用
コンデンサ、13・・・高周波結合用コンデンサ、14
・・・高周波源、16・・・ピーク検波回路。 出願入代11人 弁理士 鈴江武彦
The figure is a diagram showing the configuration of a magnetic reproducing device according to an embodiment of the present invention. 1... txt recording medium, 2... base layer, 3...
- Recording layer, 4... Recording track, 5... Signal magnetization,
6... Reproduction head, 7... Primary side inductance element, 8... Secondary side inductance element, 9... Magnetic material, io, il... Substrate, 12.15... Tuning Capacitor for use, 13... Capacitor for high frequency coupling, 14
...High frequency source, 16...Peak detection circuit. 11 applicants Patent attorney Takehiko Suzue

Claims (3)

【特許請求の範囲】[Claims] (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、前記磁気記録媒体に記録された信号を再生する磁気
再生装置において、前記高周波結合回路は、前記磁気記
録媒体のベース層側に配置され高周波信号が供給される
1次側インダクタンス素子と、この1次側インダクタン
ス素子と直交して対向するように前記磁気記録媒体の記
録層側に配置され前記磁性体と結合する2次側インダク
タンス素子と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。
(1) It has a high frequency, wave coupling circuit in which the degree of coupling changes due to the change in the high frequency characteristics of the magnetic material due to the signal magnetic field from the magnetic recording medium, and from this high frequency coupling circuit based on the change in the degree of coupling of this high frequency coupling circuit. In a magnetic reproducing device that detects a change in a high frequency output voltage of a magnetic recording medium and reproduces a signal recorded on the magnetic recording medium, the high frequency coupling circuit is arranged on a base layer side of the magnetic recording medium and is supplied with a high frequency signal. a primary inductance element, and a secondary inductance element arranged on the recording layer side of the magnetic recording medium so as to face orthogonally to the primary inductance element and coupled to the magnetic material. A magnetic reproducing device characterized by:
(2) 高周波結合回路は、信@磁界による前記磁性体
の磁気共鳴により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
(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 magnetic resonance of the magnetic body caused by a magnetic field. The magnetic reproducing device according to item 1.
(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、信号磁界による前記磁性体の
磁気共鳴により大きな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2項記載の磁気再生装置
(3) In a 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 large electromagnetic coupling occurs due to the magnetic resonance of the magnetic material caused by the signal magnetic field. A magnetic reproducing device according to claim 2, characterized in that:
JP23866283A 1983-12-17 1983-12-17 Magnetic reproducer Pending JPS60129907A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23866283A JPS60129907A (en) 1983-12-17 1983-12-17 Magnetic reproducer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23866283A JPS60129907A (en) 1983-12-17 1983-12-17 Magnetic reproducer

Publications (1)

Publication Number Publication Date
JPS60129907A true JPS60129907A (en) 1985-07-11

Family

ID=17033457

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23866283A Pending JPS60129907A (en) 1983-12-17 1983-12-17 Magnetic reproducer

Country Status (1)

Country Link
JP (1) JPS60129907A (en)

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