JPH03230307A - Magnetic head - Google Patents

Magnetic head

Info

Publication number
JPH03230307A
JPH03230307A JP2455490A JP2455490A JPH03230307A JP H03230307 A JPH03230307 A JP H03230307A JP 2455490 A JP2455490 A JP 2455490A JP 2455490 A JP2455490 A JP 2455490A JP H03230307 A JPH03230307 A JP H03230307A
Authority
JP
Japan
Prior art keywords
magnetic head
main body
electrodes
magnetic
magnetization
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
JP2455490A
Other languages
Japanese (ja)
Inventor
Toshio Inao
俊雄 稲生
Akio Kondo
近藤 昭夫
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.)
Tosoh Corp
Original Assignee
Tosoh 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 Tosoh Corp filed Critical Tosoh Corp
Priority to JP2455490A priority Critical patent/JPH03230307A/en
Publication of JPH03230307A publication Critical patent/JPH03230307A/en
Pending legal-status Critical Current

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  • Magnetic Heads (AREA)

Abstract

PURPOSE:To simplify the construction of a magnetic head and to facilitate the production thereof by holding a part of a magnetic head body with a structure which holds piezoelectric materials with electrodes and forming the body part held with this structure CoF2. CONSTITUTION:A part of the body 1 is held and formed of the structure which helds the piezoelectric materials 8 with the electrodes 2. The held part A of the body 1 is formed of CoF2 or MnF2. An electric field is generated in the materials 8 and the materials oscillate when the AC voltage corresponding to an input signal is impressed to the electrodes 2 from lead wires 3. Magnetization is induced in the part A by this oscillation and a leak magnetic field is generated in the gap part B of the body 1. The recording and reproducing to the recording medium are executed by this leak magnetic field. The need for winding a coil on the magnetic head is eliminated in this way and the construction is simplified, by which the production is facilitated.

Description

【発明の詳細な説明】 5産業上の利用分野コ 本発明は、VTRやビデオ、フロッピーディスクあるい
はハードディスクなどの磁気記録媒体の5己録IT) 
15に用いることのできる磁気ヘッドに関するものであ
る。
[Detailed Description of the Invention] 5 Industrial Application Fields The present invention is applicable to 5 industrial applications of magnetic recording media such as VTRs, videos, floppy disks, and hard disks (IT).
The present invention relates to a magnetic head that can be used in 15.

[従来の技術] 一般的に磁気ヘッドは第2図に示すように、フェライト
などの軟磁性体からなり、ギャップ部分Bを有するヘッ
ド本体5にコイル4を巻いた構造を有しており、コイル
4に電流を流すことにより、ヘッド本体5に磁化を誘起
させ、該磁化の誘起によりギャップBにもれ磁場を発生
させ、このもれ磁場を利用することにより磁気記録媒体
への記録が行なわれる。また再生は、媒体に記録された
磁気的な信号をギャップBから取り込み、この信号の取
り込みによりコイル4に再生電圧を誘起させ、再生電圧
を検知することにより行なわれる。しかしながら、近年
媒体の記録密度の向上に伴ない、小型化した磁気ヘッド
が要望されており、第2図に示すようなコイルを巻いた
構造を有する磁気ヘッドでは加工が難しいという点で上
記磁気ヘッドの小型化に対して対応が困難である。
[Prior Art] Generally, as shown in FIG. 2, a magnetic head is made of a soft magnetic material such as ferrite and has a structure in which a coil 4 is wound around a head body 5 having a gap portion B. By passing a current through the head body 5, magnetization is induced in the head body 5, and the induced magnetization generates a leakage magnetic field in the gap B. Recording on the magnetic recording medium is performed by using this leakage magnetic field. . Further, reproduction is performed by taking in a magnetic signal recorded on the medium from the gap B, inducing a reproducing voltage in the coil 4 by taking in this signal, and detecting the reproducing voltage. However, as the recording density of media has improved in recent years, there has been a demand for smaller magnetic heads, and magnetic heads with a coil-wound structure as shown in Figure 2 are difficult to process. It is difficult to respond to the miniaturization of

[発明が解決しようとする課題] 本発明の目的は作製が簡単で、生産性向上を図ることの
できる磁気ヘッドを提供することにある。
[Problems to be Solved by the Invention] An object of the present invention is to provide a magnetic head that is easy to manufacture and can improve productivity.

[課題を解決するための手段] 本発明者らは上記課題を解決するために鋭意検討を行な
った結果、ピエゾ磁気効果を利用することにより簡単な
構造を有する磁気ヘッドが得られれることを見出たし、
本発明を完成するに至った。
[Means for Solving the Problems] As a result of intensive studies to solve the above problems, the present inventors found that a magnetic head having a simple structure can be obtained by utilizing the piezo magnetic effect. It came out,
The present invention has now been completed.

すなわち本発明は、本体の一部を、圧電物質を電極で挟
んだ構造物により挟み、少なくとも上記構造物により挟
まれた本体の部分をCo F 2またはM n F 2
により構成することを特徴とする磁気ヘッドである。
That is, in the present invention, a part of the main body is sandwiched between structures in which a piezoelectric material is sandwiched between electrodes, and at least the part of the main body sandwiched between the structures is made of Co F 2 or M n F 2 .
This is a magnetic head characterized in that it is configured by:

[作用コ 第1図に本発明の磁気へツ す。第1図中、1は磁気ヘラ 3は入出力信号を伝達するり 質を示す。本発明の磁気ヘラ ドの構造の一例を示 ドの本体、2は電極、 ド線、8は圧電物 ドは本体lの一部か 圧電物質8を電極2で挟んだ構造物により挟まれ、少な
くとも上記構造物により挟まれた本体の部分AがCoF
  またはM n F 2により構成される。
[Operations] Figure 1 shows the magnetism of the present invention. In FIG. 1, 1 indicates the quality of the magnetic spatula 3 through which input/output signals are transmitted. An example of the structure of a magnetic helad according to the present invention is shown in which the main body 2 is an electrode; Part A of the main body sandwiched between the above structures is CoF
Or composed of M n F 2.

ここで、本発明の磁気ヘッドにおける圧電物質8は、電
極2から印加される電圧によって本体のAの部分に歪み
を与えるため又は本体のAの部分に生ずる歪みを感知し
てこれを電圧として電極2に伝達するために配置され、
例えばリン酸カリウムやロッシェル塩(酒石酸ナトリウ
ムカリウム)などを用いる二とができる。また、電極2
としては電気伝導性を示すものであればどのようなもの
でも用いることかできるが、例えばアルミニウムなどが
好ましく用いられる。更に本体は少なくともAの部分が
CoF  またはM n F 2で構成されていればよ
く、本体のAの部分以外については磁性を示すものであ
れば特にその構成材料は限定されない。本体Aの部分以
外については例えば本体Aの部分を構成するために用い
た材料やフェライトなどを用いて構成することができる
Here, the piezoelectric material 8 in the magnetic head of the present invention is used to apply a strain to the portion A of the main body by the voltage applied from the electrode 2, or to sense the strain generated in the portion A of the main body and use this as a voltage to be applied to the electrode. arranged to communicate to 2;
For example, potassium phosphate or Rochelle's salt (sodium potassium tartrate) can be used. In addition, electrode 2
Although any material can be used as long as it exhibits electrical conductivity, for example, aluminum is preferably used. Further, it is sufficient that at least the portion A of the main body is made of CoF or M n F 2 , and the constituent materials of the main body other than the portion A are not particularly limited as long as they exhibit magnetism. Portions other than the main body A can be constructed using, for example, the same material used to construct the main body A, ferrite, or the like.

ところで、本発明の磁気ヘッドにおいて、本体のAの部
分を構成するC o F 2またはM n F 2はピ
エゾ磁気効果(以下、PM効果という)を示す物質であ
って、該効果により本発明の磁気ヘッドは作用する。従
って、本発明の磁気ヘッドは従来の磁気ヘッドのように
コイルを巻く必要がなくなり、構造が簡単なものとなる
ため、その作製は容易に行なうことができる。なお、上
記PM効果とは、応力を与えた場合にその応力に比例し
て磁化が誘起されたり、磁化に比例して応力が誘起され
る現象である。
By the way, in the magnetic head of the present invention, C o F 2 or M n F 2 constituting the part A of the main body is a substance that exhibits a piezo magnetic effect (hereinafter referred to as PM effect), and this effect makes it possible to achieve the magnetic head of the present invention. The magnetic head works. Therefore, unlike the conventional magnetic head, the magnetic head of the present invention does not need to be wound with a coil and has a simple structure, so that it can be manufactured easily. Note that the PM effect is a phenomenon in which when stress is applied, magnetization is induced in proportion to the stress, or stress is induced in proportion to magnetization.

以下、本発明の磁気ヘッドを用いた媒体への記録及び媒
体からの記録の読み出しについて説明する。
Hereinafter, recording on a medium and reading recording from the medium using the magnetic head of the present invention will be explained.

媒体への記録はリード線3から伝達された入力信号に々
・1応する交流電圧を、本体1のAの部分に電極2によ
って印加することにより行なわれる。
Recording on the medium is performed by applying an alternating current voltage corresponding to the input signal transmitted from the lead wire 3 to a portion A of the main body 1 through the electrode 2.

この電圧の印加により、圧電物質8には電場が発生し、
電圧物質8が振動する。この振動によって本体1のAの
部分には応力が生じる。ここで、本体1のAの部分はP
M効果を示すため、への部分には磁化が誘起され、この
磁化の誘起により本体1中では第3図に示すように磁化
6が誘起される。
By applying this voltage, an electric field is generated in the piezoelectric material 8,
The voltage substance 8 vibrates. This vibration generates stress in the portion A of the main body 1. Here, part A of main body 1 is P
In order to exhibit the M effect, magnetization is induced in the portion , and this magnetization induces magnetization 6 in the main body 1 as shown in FIG.

更に誘起された磁化6は、第3図の示すように上記本体
1のギャップの部分Bにもれ磁場7を与えるので、この
もれ磁場7を利用することにより媒体への記録が可能と
なる。
Furthermore, the induced magnetization 6 gives a leakage magnetic field 7 to the gap portion B of the main body 1 as shown in FIG. 3, so that recording on the medium becomes possible by utilizing this leakage magnetic field 7. .

一方、再生は次のとおり行なわれる。はじめに本体1の
ギャップ部分Bから媒体のもれ磁束を取り込む。これに
より、本体1内には磁化が生じ、該磁化は本体1のAの
部分まで誘導される。この誘導された磁化により、本体
1のAの部分にはPM効果によって歪みが生じ、この歪
みが圧電物質8に伝わり、圧電物質8には交流の電気分
極Pが発生する。ここで、電極2ての面電荷密度をσと
した場合、電気分極Pは、 P−σ と表される。更に、電極2の面積を81電極に誘起され
る全電荷量をQ、容量をCとした場合、電極2間に生じ
る電位差Vは、 Q寓σS −P S −Cv となり、このことから電極2間には V−3P/C の電位差が生じる。従って、上記した圧電物質8に発生
した電気分極Pは電極2間の電位差Vとしてリード線3
を通して検出され、この検出によって媒体から出力信号
を読み出すことが可能となる。
On the other hand, playback is performed as follows. First, the leakage magnetic flux of the medium is taken in from the gap portion B of the main body 1. As a result, magnetization is generated within the main body 1, and the magnetization is induced to the portion A of the main body 1. This induced magnetization causes distortion in the part A of the main body 1 due to the PM effect, and this distortion is transmitted to the piezoelectric material 8, causing alternating current electric polarization P to occur in the piezoelectric material 8. Here, when the surface charge density of the electrodes 2 is σ, the electric polarization P is expressed as P−σ. Furthermore, if the area of the electrode 2 is 81, and the total amount of charge induced in the electrode is Q, and the capacitance is C, then the potential difference V generated between the electrodes 2 is: A potential difference of V-3P/C occurs between them. Therefore, the electrical polarization P generated in the piezoelectric material 8 described above is converted into a potential difference V between the electrodes 2 and the lead wire 3.
This detection allows the output signal to be read from the medium.

[発明の効果] 以上述べたとおり、本発明の磁気ヘッドはその構造が簡
単であり、作製が容易となるため、近年の磁気ヘッドの
小型化に対応し得るものとなる。
[Effects of the Invention] As described above, the magnetic head of the present invention has a simple structure and is easy to manufacture, so that it can respond to the miniaturization of magnetic heads in recent years.

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

第1図は本発明の磁気ヘッドの構造の一例を示す図であ
る。 第2図は従来の磁気ヘッドの構造を示す図である。 第3図は本発明の磁気ヘッドの例において、誘起される
磁化の方向を示す図である。 図中、 1.5・・・本体    2・・・電極3・・・リード
線4 ・・・コイル 6・・・磁化      7・・・もれ磁場8・・・圧
電物質 A・・・本体の圧電物質を電極で挟んだ構造物により挟
まれた部分 B・・・本体のギャップ部分 を各々示す。
FIG. 1 is a diagram showing an example of the structure of the magnetic head of the present invention. FIG. 2 is a diagram showing the structure of a conventional magnetic head. FIG. 3 is a diagram showing the direction of magnetization induced in an example of the magnetic head of the present invention. In the figure, 1.5...Main body 2...Electrode 3...Lead wire 4...Coil 6...Magnetization 7...Leakage magnetic field 8...Piezoelectric material A...Main body A portion B sandwiched between structures in which a piezoelectric material is sandwiched between electrodes indicates a gap portion of the main body.

Claims (2)

【特許請求の範囲】[Claims] (1)本体の一部を、圧電物質を電極で挟んだ構造物に
より挟み、少なくとも上記構造物により挟まれた本体の
部分をCoF_2により構成したことを特徴とする磁気
ヘッド。
(1) A magnetic head characterized in that a part of the main body is sandwiched between structures in which a piezoelectric material is sandwiched between electrodes, and at least the part of the main body sandwiched between the structures is made of CoF_2.
(2)本体の一部を、圧電物質を電極で挟んだ構造物に
より挟み、少なくとも上記構造物により挟まれた本体の
部分をMnF_2により構成したことを特徴とする磁気
ヘッド。
(2) A magnetic head characterized in that a part of the main body is sandwiched between structures in which a piezoelectric material is sandwiched between electrodes, and at least the part of the main body sandwiched between the structures is made of MnF_2.
JP2455490A 1990-02-05 1990-02-05 Magnetic head Pending JPH03230307A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2455490A JPH03230307A (en) 1990-02-05 1990-02-05 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2455490A JPH03230307A (en) 1990-02-05 1990-02-05 Magnetic head

Publications (1)

Publication Number Publication Date
JPH03230307A true JPH03230307A (en) 1991-10-14

Family

ID=12141377

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2455490A Pending JPH03230307A (en) 1990-02-05 1990-02-05 Magnetic head

Country Status (1)

Country Link
JP (1) JPH03230307A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001028466A (en) * 1999-07-14 2001-01-30 Sony Corp Magnetic functional element and magnetic recording device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001028466A (en) * 1999-07-14 2001-01-30 Sony Corp Magnetic functional element and magnetic recording device

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