JPS5911504A - Magnetic reproducer - Google Patents

Magnetic reproducer

Info

Publication number
JPS5911504A
JPS5911504A JP11953782A JP11953782A JPS5911504A JP S5911504 A JPS5911504 A JP S5911504A JP 11953782 A JP11953782 A JP 11953782A JP 11953782 A JP11953782 A JP 11953782A JP S5911504 A JPS5911504 A JP S5911504A
Authority
JP
Japan
Prior art keywords
magnetic
capacitance element
tuning
capacitance
high 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.)
Granted
Application number
JP11953782A
Other languages
Japanese (ja)
Other versions
JPH0344362B2 (en
Inventor
Junichi Akiyama
純一 秋山
Osamu Chiba
脩 千葉
Kenichi Sawazaki
沢崎 憲一
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
Tokyo Shibaura Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP11953782A priority Critical patent/JPS5911504A/en
Publication of JPS5911504A publication Critical patent/JPS5911504A/en
Publication of JPH0344362B2 publication Critical patent/JPH0344362B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/33Structure 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 obtain a reproduced output having a sufficiently large level with good S/N even for a very narrow recording track width, in a magnetic reproducer for reproducing signals by using the change in characteristics of a magnetic substance due to the change in a magnetic field formed with a magnetic recording medium. CONSTITUTION:The 1st capacitance element 1 is formed by covering plate- shaped metallic electrodes 3a, 3b on both sides of a plate-shaped insulating magnetic substance 2 so as to be embedded in a dielectric 5 of electrodes 6a, 6b of the 2nd capacitive element 4. The 1st capacitive element 1 constitutes the 1st LC parallel tuning circuit 8 together with a tuning inductance element 7. The 2nd capacitive element 4 forms similarly the 2nd tuning circuit 10 together with a tuning inductance element 9. The 2nd tuning circuit 10 is connected to a high frequency oscillator 12 via a matching circuit 11. Thus, a high frequency exciting signal from the high frequency oscillator 12 is coupled with the 1st capacitive element 1 via the 2nd capacitive element 4 in the form of an electric field by means of the capacitive coupling. Further, the 1st tuning circuit 8 is connected to a peak detecting circuit 16 comprising a diode 13, a resistor 14 and a capacitor 15.

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明は、磁気記録媒体が形成する磁界の変化による
磁性体の特性変化をオリ用して再生を行なう磁気再生装
置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a magnetic reproducing device that performs reproduction by making use of changes in characteristics of a magnetic material due to changes in a magnetic field formed by a magnetic recording medium.

〔発明の技術的背景とその問題点〕[Technical background of the invention and its problems]

磁気記録媒体に記録された信郵を再生ずる磁気再生装置
は従来、リング型の磁気ヘッドを用い、これに誘起され
る起電力を再生出力として取出す構成となっている。し
かし、この方式は再生出力レベルおよびそのS/Nが記
録トランク幅に大きく依存するため、高密度記録再生に
不利であり、現状では記録トラ、ツク幅が20μ。
Conventionally, a magnetic reproducing apparatus for reproducing mail recorded on a magnetic recording medium uses a ring-shaped magnetic head, and is configured to extract the electromotive force induced in the ring-shaped magnetic head as a reproducing output. However, this method is disadvantageous for high-density recording and reproduction because the reproduction output level and its S/N largely depend on the recording trunk width, and currently the recording track width is 20 μm.

S/Nが43 dB程度が限界とされている。The S/N is said to be at a limit of about 43 dB.

そこで、発明者らは既に特願昭55−110340号に
おいて新しい原理に基づく磁気再生装置を提案している
。この装置は磁気記録媒体からの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、
この磁性体を含むインダクタンス素子またはキャパシタ
ンス素子等のインピーダンス素子のインピーダンス変化
を利用して再生を行なうものである。即ち、上記インピ
ーダンス素子を同調集子の一部として同調回路を構成す
るとともに、このインピーダンス素子に高周波発振器か
らの高周波励振信号を供給する。この場合、磁気記録媒
体からの磁界によって上記磁性体の特性が変化し、これ
によってインビーダン7素子のインピーダンスが変化す
ると、これに伴い同調回路の共振周波数やQ(尖鋭度)
が変化するので、同調回路よりの高周波信号出力が変化
する。従ってこの高周波信号出力の変化を検波N路を通
して検出することにより、磁気記録媒体に記録された信
号に対応した再生出力が得られる。
Therefore, the inventors have already proposed a magnetic reproducing device based on a new principle in Japanese Patent Application No. 110340/1982. This device is equipped with a magnetic material that detects changes in the magnetic field from a magnetic recording medium as changes in characteristics such as magnetic permeability and high frequency loss.
Reproduction is performed using changes in impedance of an impedance element such as an inductance element or a capacitance element containing this magnetic material. That is, a tuning circuit is configured using the impedance element as part of a tuning collector, and a high frequency excitation signal from a high frequency oscillator is supplied to this impedance element. In this case, when the characteristics of the magnetic body change due to the magnetic field from the magnetic recording medium and the impedance of the seven impedance elements changes, the resonant frequency and Q (sharpness) of the tuned circuit change accordingly.
changes, so the high frequency signal output from the tuned circuit changes. Therefore, by detecting the change in the high frequency signal output through the detection N path, a reproduced output corresponding to the signal recorded on the magnetic recording medium can be obtained.

この方式によれば、磁気記録媒体が形成する磁界のわず
かな変化も磁性体の特性変化として検出され、再生出力
として取出されるとともに、再生出力エイ・ルギーが高
周波発振器から供給されるので、高レベルかつS/N 
 の良好な再生出力を得ることができ、記録トラック幅
を20μ以下にまで狭くしても十分に再生を行なうこと
が可能となる。
According to this method, even the slightest change in the magnetic field formed by the magnetic recording medium is detected as a change in the characteristics of the magnetic material, and is extracted as a playback output.The playback output energy is also supplied from a high-frequency oscillator. level and S/N
A good reproduction output can be obtained, and even if the recording track width is narrowed to 20 μm or less, sufficient reproduction can be performed.

以上のように、%願昭55−110340号等で提案し
た方式は原理的に従来の磁気再生装置に比べ高密度記録
再生に適しているが、その高密度化にはやはり限界があ
る。即ち、記録密度な土けるには記録トランク幅を狭く
するとともに、記録波長を短くすればよいが、その場合
上記の方式で拘止を行なおうとすると、記録トランク幅
に合せて磁性体の幅を小さくシ、かつ短い記録波長に合
せて磁性体の厚さも小さくする必要がある。磁性体の厚
さを小さくする理由は、磁気記録媒体が形成する磁界が
表面近傍程強く、シかも記録波長が短い程、つまり記録
信号周波数が高い程その傾向が強いためで、この厚さが
大きくなると磁界が両性体の一部にしか及ばず、磁界の
変化による磁性体の特性変化が小さくなるからである。
As mentioned above, although the system proposed in % Application No. 110340/1988 is theoretically more suitable for high-density recording and reproduction than conventional magnetic reproducing devices, there is still a limit to its high density. In other words, in order to reduce the recording density, it is possible to narrow the recording trunk width and shorten the recording wavelength, but in that case, if you try to use the above method for restraint, the width of the magnetic material will need to be adjusted to match the recording trunk width. In addition, it is necessary to reduce the thickness of the magnetic material to match the short recording wavelength. The reason for reducing the thickness of the magnetic material is that the magnetic field formed by a magnetic recording medium is stronger near the surface, and this tendency is stronger the shorter the recording wavelength, that is, the higher the recording signal frequency. This is because when the magnetic field becomes larger, the magnetic field only reaches a part of the amphoteric material, and the change in the characteristics of the magnetic material due to changes in the magnetic field becomes smaller.

このように、より高密度記録再生を行なおうとすると磁
性体の寸法を極力小さくする必要があり、それに伴いこ
の磁性体を含むインピーダンス素子の寸法も小さくしな
ければならない。
As described above, in order to perform higher density recording and reproduction, it is necessary to reduce the size of the magnetic body as much as possible, and accordingly, the size of the impedance element containing this magnetic body must also be reduced.

ところが、このインピーダンス素子の寸法を小さくして
ゆくと、その浮遊容量の影響が無視できなくなり、この
浮遊容量のためインピーダンス素子に高周波励振信号を
安定に供給することが困難となるとともに、同調回路の
Qが低下する。この結呆、磁気記録媒体からの磁界によ
る磁性体の特性変化を安定に効率よく電気信号に変換す
ることが困難となってくる′。
However, as the dimensions of this impedance element are reduced, the influence of its stray capacitance cannot be ignored, and this stray capacitance makes it difficult to stably supply a high-frequency excitation signal to the impedance element, and the tuning circuit Q decreases. As a result, it becomes difficult to stably and efficiently convert changes in the characteristics of the magnetic material due to the magnetic field from the magnetic recording medium into electrical signals.

〔発明の目的〕[Purpose of the invention]

この発明の目的は、記録トランク幅が非常に狭い場合で
も十分レベルの大きい再生出力をS/Nよく得ることが
できる磁気再生装置を提供することである。
An object of the present invention is to provide a magnetic reproducing apparatus that can obtain a sufficiently high level reproduction output with a good S/N ratio even when the recording trunk width is very narrow.

〔発明の概要〕[Summary of the invention]

この発明は、磁気記録媒体が形成する磁界を検出する絶
縁性磁性体を電極間物置として含む第1のキャパシタン
ス素子を形成するとともに、この第1のキャパシタンス
素子を電極間に保持した第2のキャパシタンス素子を形
成して、この第2のキャパシタンス素子を介して第1の
キャパシタンス素子に為周波励振信匈を結合させること
により、第1のキャパシタンス素子を同調集子の一部と
して構成した同調N路に流周波励振信号を供給し、上記
磁性体により検出された磁界の変化による磁性体の特性
変化に伴うこの同調回路の茜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よ5に
したことを特徴としている。
This invention forms a first capacitance element that includes an insulating magnetic material as an interelectrode storage device for detecting a magnetic field formed by a magnetic recording medium, and a second capacitance element that holds this first capacitance element between electrodes. a tuned N-path in which the first capacitance element is configured as part of a tuning collector by forming an element and coupling a frequency excitation signal to the first capacitance element through the second capacitance element; A current frequency excitation signal is supplied to the magnetic body, and a change in the Akane frequency signal output of this tuned circuit is detected due to a change in the characteristics of the magnetic body due to a change in the magnetic field detected by the magnetic body, and a signal recorded on the magnetic recording medium is detected. The feature is that it plays 5 times.

〔発明の効果〕〔Effect of the invention〕

この発明によれば、磁気記録媒体が形成するイa号磁′
界を検出する絶縁性磁性体を電極間物質とし、て含む第
1のキャパシタンス素子に対し、これを電極[SAJに
保持、つまりこの第1のキャパシタンス素子を包囲する
ように設けられた第2のキャパシタンスを介して高周波
励振信号を結合させるため、超高密度記録再生に対応す
べく磁性体の寸法を小さくしても、第1のキャパシタン
ス素子の浮遊容量の影響はM2のキャパシタンス索子の
谷世によって減少できるようになる。このため、第1の
キャパシタンス素子への高周波励振信号の結合を安定に
行なうことができるとともに、同調回路のQを低下させ
ることがなくなる。さらに、第2のキャパシタンス素子
が信号磁界以外の電磁界をシールドし、第1のキャパシ
タンス索子に作用するのを防止する効果もある〇 従って、記録トラック幅が20μm以下とい5ような超
高密度記録再生においても再生感度の低下がなく、高レ
ベルかつS/Nの良好な再生出力を得ることができる。
According to this invention, the number a magnetic field formed by the magnetic recording medium is
A first capacitance element that includes an insulating magnetic material as an interelectrode material that detects a field is held at an electrode [SAJ, that is, a second capacitance element provided to surround this first capacitance element. Since the high-frequency excitation signal is coupled through capacitance, even if the dimensions of the magnetic material are reduced to accommodate ultra-high density recording and reproduction, the influence of the stray capacitance of the first capacitance element will be reduced by the valley of the capacitance cord of M2. can be reduced by Therefore, the high frequency excitation signal can be stably coupled to the first capacitance element, and the Q of the tuning circuit is not lowered. Furthermore, the second capacitance element has the effect of shielding electromagnetic fields other than the signal magnetic field and preventing them from acting on the first capacitance element. Therefore, if the recording track width is 20 μm or less, ultra-high density recording such as 5. Even during recording and reproduction, there is no reduction in reproduction sensitivity, and reproduction output at a high level and with a good S/N ratio can be obtained.

〔発明の実施例〕[Embodiments of the invention]

第1図はこの発明の一実施例を示すものである。図にお
いて、第1のキャパシタンス索子1は板状の絶縁性磁性
体2の両面に板状金属電極3a、3bを被着して形成さ
れたもので、この第1のキャパシタンス索子1は第2の
キャパシタンス素子4の電極6a 、6b間の誘電体5
内に埋め込まれた形で設けられている。第1のキャパシ
タンス素子1は同調用インダクタンス素子7と共に第1
のLC並列同調回路8を構成する。一方、第2のキャパ
シタンス素子4も同様に同調用インダクタンス素子9と
ともに第2の同調回路10を構成する。この第2の同調
回路10は整合回路1ノを介して高周波発振器12に接
続されている。従って、第1のキャパシタンス素子1に
は高周波発振器12からの高周波励振信号が第2のキャ
パシタンス素子4を介して容蓋結合による電界の形で結
合されることになる。そして、第1の同調回路8はダイ
オード13と抵抗14及びフンデ/す15からなるピー
ク検波回wJ16に接続されてい゛る。
FIG. 1 shows an embodiment of the present invention. In the figure, a first capacitance cable 1 is formed by attaching plate-shaped metal electrodes 3a and 3b to both sides of a plate-shaped insulating magnetic material 2. Dielectric material 5 between electrodes 6a and 6b of capacitance element 4 of No. 2
It is installed in a way that it is embedded inside. The first capacitance element 1 together with the tuning inductance element 7
LC parallel tuning circuit 8 is constructed. On the other hand, the second capacitance element 4 similarly constitutes a second tuning circuit 10 together with the tuning inductance element 9. This second tuning circuit 10 is connected to a high frequency oscillator 12 via a matching circuit 1. Therefore, the high frequency excitation signal from the high frequency oscillator 12 is coupled to the first capacitance element 1 via the second capacitance element 4 in the form of an electric field due to capacitance coupling. The first tuning circuit 8 is connected to a peak detection circuit wJ16 consisting of a diode 13, a resistor 14, and a foundation/substrate 15.

このように構成された磁気再生装置におい℃、信号が記
録された磁気記録媒体18に第1、第2のキャパシタン
ス素子1.4を図のように交ツ向させると、−気記録媒
体18からの記録4M号に応じて変化する磁界(信号磁
界)が磁性体2に加わり、これにより磁性体2の透磁率
あるいは筒周V損失が変化する。ここで磁性体2として
磁界変化に対し透磁率や高周波損失の変化が大きく、シ
かも導電率の極めて小さい材料、例えば薄膜化したスピ
ネル系あるいはガーネット糸筒のフェライトを用いると
、磁性体2の透磁率や高周波損失の変化によって、この
磁性体2をif極間物實とする第1のキャパシタンス索
子1の見掛けのキャパシタンスか大きく変化し、これに
よってこの第1のギヤパンタンス素子1とインダクタン
ス素子7とで構成される第1のF[141回Bgのイン
ピーダンスが変化するので、この第1の同調回路8の両
14電圧も変化する。
In the magnetic reproducing apparatus configured as described above, when the first and second capacitance elements 1.4 are oriented crosswise as shown in the figure, the magnetic recording medium 18 on which a signal is recorded at -° C. A magnetic field (signal magnetic field) that changes according to the recording No. 4M is applied to the magnetic body 2, thereby changing the magnetic permeability or cylinder circumferential V loss of the magnetic body 2. If the magnetic material 2 is made of a material whose magnetic permeability and high-frequency loss change greatly in response to changes in the magnetic field, and which also has extremely low electrical conductivity, such as thin spinel or garnet thread ferrite, the permeability of the magnetic material 2 may be reduced. Due to changes in magnetic property and high frequency loss, the apparent capacitance of the first capacitance element 1 using the magnetic material 2 as an interpole material changes greatly, and as a result, the relationship between the first gear pantance element 1 and the inductance element 7 changes significantly. Since the impedance of the first F[141 times Bg composed of Bg changes, both 14 voltages of this first tuned circuit 8 also change.

即ち、高周波発振器12より第1のキャパシタンス素子
1に結合された高周波励振信号は、第1の同調回路8に
おいて磁気記録媒体18からの信号磁界により振幅変W
々を受けることになる。
That is, the high frequency excitation signal coupled from the high frequency oscillator 12 to the first capacitance element 1 is amplitude-changed W by the signal magnetic field from the magnetic recording medium 18 in the first tuning circuit 8.
You will receive many.

従って、この変調を受けた第1の同調回路8からの高周
波信号出力を検波回路16で検波することによって、信
号再生出力voutを得ることができる。
Therefore, by detecting the high frequency signal output from the first tuning circuit 8 that has undergone this modulation using the detection circuit 16, the signal reproduction output vout can be obtained.

このような構成とすれは、第1のキャパシタンス索子1
の浮遊容量は第2のキャパシタンス索子4の大きい各t
によつ”C無視することができる。また、第2のキャパ
シタンス索子4Q)#遊8には本来の客足に比べ十分小
さいため、これも無視できる。従って商拘波発振器12
から第1のキャパシタンス索子1への市周波励振侶号の
結合、供給を安定に行lよえるようになるとともに、第
1のキャパシタンス索子1のb(遊変量の影響による第
1の四W4回路s v)qの低十を抑えることができ゛
るので、非常に狭いトランクに筒密度記録された信号も
、十分なレベルでS/Nよく再生することが可能となる
With this configuration, the first capacitance cable 1
The stray capacitance of the second capacitance wire 4 is large for each t
In addition, since the second capacitance cable 4Q) is sufficiently small compared to the original number of customers, it can also be ignored.
It becomes possible to stably couple and supply the local frequency excitation link from Since the W4 circuit sv)q can be suppressed, even signals recorded in a very narrow trunk can be reproduced at a sufficient level and with a good S/N ratio.

第2図はこの発明の他の実施例を示すもので、第1図に
おける第1のキャパシタンス素子1の一方の電極3bを
第2のキャパシタンス素子4の一方の電極6bと共通と
することにより、構造の簡略化と製造工程数の減少を図
ったものである。
FIG. 2 shows another embodiment of the present invention, in which one electrode 3b of the first capacitance element 1 in FIG. 1 is shared with one electrode 6b of the second capacitance element 4. The aim is to simplify the structure and reduce the number of manufacturing steps.

この発明は特に、複数のb己録トランクから同時に丙午
を行なう多チヤンネル磁気再生装置に適用した場合、極
めて有オUである。第3図〜館6図はその実施例を示す
もので、1つの第2のキャパシタンス素子4内に第1の
キャパシタンス素子1を複数個設けている。この場合、
第1のキャパシタンス素子1の各々は共通の第2のキャ
パシタンス素子4を介して高周波励振信号の供給を受け
ることになる。
This invention is extremely useful, especially when applied to a multi-channel magnetic reproducing apparatus that simultaneously performs recording from a plurality of self-recording trunks. 3 to 6 show examples thereof, in which a plurality of first capacitance elements 1 are provided within one second capacitance element 4. in this case,
Each of the first capacitance elements 1 is supplied with a high frequency excitation signal via a common second capacitance element 4.

従って、第1のキャパシタンス素子1に個別に画周波励
振信号を結合させて供給する場合に比べてチャンネル毎
の結合度のバラツキがなく、再生出力レベルのバラツキ
も抑えることができる。しかも、結合部や高周波発揚器
12を含む励振回路の構造が簡単で済むとともに、配線
が簡略化されるので、工程上有利となり、LSI等の集
積N路技術を有効に生かすことができるというオU点が
ある。
Therefore, compared to the case where the image frequency excitation signal is individually coupled and supplied to the first capacitance element 1, there is no variation in the degree of coupling for each channel, and variation in reproduction output level can also be suppressed. Moreover, the structure of the excitation circuit including the coupling part and the high-frequency oscillator 12 is simple, and the wiring is simplified, which is advantageous in terms of process and allows effective use of integrated N-path technology such as LSI. There is a U point.

第3図に示す実施例ば、第1図の実施例の構成をほぼそ
のまま多チャンネル化したものであるのに対し、第4図
に示す実施例は第3図における第1のキャパシタンス素
子1の各々の磁性体2を一体に形成したものである。
For example, the embodiment shown in FIG. 3 is a multi-channel version of the structure of the embodiment shown in FIG. 1, whereas the embodiment shown in FIG. Each magnetic body 2 is integrally formed.

第5図に示す実施例は、第2図の実施例と同様に第1の
キャパシタンス素子1の一方の電極3bを第2のキャパ
シタンス素子4の一方の電極6bと共通にして、多チャ
ンネル化したものである。
The embodiment shown in FIG. 5 has multiple channels by making one electrode 3b of the first capacitance element 1 common to one electrode 6b of the second capacitance element 4, as in the embodiment of FIG. It is something.

熱6図に示す実施例は、さらに第5図における第1のキ
ャパシタンス素子1の各々の磁性体2を一体に形成した
ものである。
In the embodiment shown in FIG. 6, each magnetic body 2 of the first capacitance element 1 in FIG. 5 is further formed integrally.

図から明らかなように、構造および製造工程は第3図、
第4図、第5図、第6図の順で順次簡略化される。
As is clear from the figure, the structure and manufacturing process are as shown in Figure 3.
4, 5, and 6 are simplified in this order.

【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の構成を示す図、第2図は
この発明の他の実施例の要部構成を示。 す断面図、第3図はこの発明を多チヤンネル磁気再生装
置に適用した実施例を示す図、第4図〜第6図は同じく
この発明を多チヤンネル磁気再生装置に適用した場合の
他の実施例の要部構成を示す断面図である。 1・・・Kxのキャパシタンス素子、2・・・絶縁性磁
性体、3a、3b・・・電惨、4・・・pA2のキャパ
シタンス素子、5・誘電体、6a 、5b・・電極、8
・・・第1の同調回路”、1o・・・第2の同調回路、
12・・・尚周波発揚器、16・・・ピーク検波囲路。
FIG. 1 shows the structure of one embodiment of the invention, and FIG. 2 shows the main structure of another embodiment of the invention. FIG. 3 is a diagram showing an embodiment in which the present invention is applied to a multi-channel magnetic reproducing device, and FIGS. 4 to 6 show other embodiments in which the present invention is similarly applied to a multi-channel magnetic reproducing device. FIG. 3 is a cross-sectional view showing the main part configuration of an example. DESCRIPTION OF SYMBOLS 1...Kx capacitance element, 2...Insulating magnetic material, 3a, 3b...Electrode, 4...pA2 capacitance element, 5.Dielectric material, 6a, 5b...Electrode, 8
...first tuned circuit", 1o...second tuned circuit,
12... Frequency booster, 16... Peak detection enclosure.

Claims (4)

【特許請求の範囲】[Claims] (1)  磁気記録媒体が形成する磁界の変化を検出す
る絶縁性磁性体を電極間物質として含む第1のキャパシ
タンス素子と、この第1のキャパシタンス素子を同調素
子の一部として構成した同調回路と、前記第1のキャパ
シタンス素子をその1を極間に保持した第2のキャパシ
タンス素子と、この第2のキャパシタンス素子に介して
Ail Hd第1のキャノ(シタンス素子ニ高周阪励振
信号を結合せしめる励振手段と、前記磁界の変化による
前記磁性体の特性変化に伴う前記同調回路の高周波信号
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
号を再生する手段とを備えることを特徴とする磁気再生
装置。
(1) A first capacitance element that includes an insulating magnetic material as an interelectrode material that detects changes in the magnetic field formed by a magnetic recording medium, and a tuning circuit that includes this first capacitance element as part of a tuning element. , a second capacitance element holding the first capacitance element between the electrodes, and a high frequency vibration excitation signal is coupled to the Ail Hd first capacitance element through the second capacitance element. It is characterized by comprising an excitation means and a means for detecting a change in the high frequency signal output of the tuning circuit due to a change in the characteristics of the magnetic body due to a change in the magnetic field and reproducing the signal recorded on the magnetic recording medium. magnetic reproducing device.
(2)第1のキャパシタンス素子と第2のキャパシタン
ス素子の各々一方の電極を共通にしたことを特徴とする
特許M*の範囲第1項記載の磁気再生装置。
(2) A magnetic reproducing device according to item 1 of the scope of Patent M*, characterized in that one electrode of each of the first capacitance element and the second capacitance element is shared.
(3)第2のキャパシタンス素子の電極間に第1のキャ
パシタンス素子を複数個設けた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。
(3) A magnetic reproducing device according to claim 1 or 2, characterized in that a plurality of first capacitance elements are provided between the electrodes of the second capacitance element.
(4)励振手段は第2のキャパシタンス素子を同調素子
の一部とする同調回路を介して第1のキャパシタンス素
子に扁周彼励振信七を結合せしめ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。
(4) The excitation means couples an excitation signal to the first capacitance element via a tuning circuit in which the second capacitance element is a part of the tuning element. The magnetic reproducing device according to scope 1.
JP11953782A 1982-07-09 1982-07-09 Magnetic reproducer Granted JPS5911504A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11953782A JPS5911504A (en) 1982-07-09 1982-07-09 Magnetic reproducer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11953782A JPS5911504A (en) 1982-07-09 1982-07-09 Magnetic reproducer

Publications (2)

Publication Number Publication Date
JPS5911504A true JPS5911504A (en) 1984-01-21
JPH0344362B2 JPH0344362B2 (en) 1991-07-05

Family

ID=14763735

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11953782A Granted JPS5911504A (en) 1982-07-09 1982-07-09 Magnetic reproducer

Country Status (1)

Country Link
JP (1) JPS5911504A (en)

Also Published As

Publication number Publication date
JPH0344362B2 (en) 1991-07-05

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