JPS6353702A - Generating device for high frequency modulated magnetic field - Google Patents

Generating device for high frequency modulated magnetic field

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Publication number
JPS6353702A
JPS6353702A JP19561486A JP19561486A JPS6353702A JP S6353702 A JPS6353702 A JP S6353702A JP 19561486 A JP19561486 A JP 19561486A JP 19561486 A JP19561486 A JP 19561486A JP S6353702 A JPS6353702 A JP S6353702A
Authority
JP
Japan
Prior art keywords
magnetic field
magnetic material
main
frequency modulated
pole
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
JP19561486A
Other languages
Japanese (ja)
Inventor
Takehiro Nagaki
永木 猛弘
Masahiko Kaneko
正彦 金子
Masatoshi Hayakawa
正俊 早川
Hiroshi Yamanoi
山ノ井 博
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.)
Sony Corp
Original Assignee
Sony 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 Sony Corp filed Critical Sony Corp
Priority to JP19561486A priority Critical patent/JPS6353702A/en
Publication of JPS6353702A publication Critical patent/JPS6353702A/en
Pending legal-status Critical Current

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  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To attain the reduction of power consumption, and a fast operation, by constituting a device by arranging the soft magnetic material part, and the hard magnetic material part of a main magnetic pole in the longitudinal direction of the main magnetic pole. CONSTITUTION:In the main magnetic pole 2, the soft magnetic material parts S1 and S2 made of a soft magnetic material, and the hard magnetic material part H1 made of a hard magnetic material, are arranged in the longitudinal direction that is an axial direction, and the winding 3 for driving is wound about the main magnetic pole 2, and a tip part 5 that is one end of the main magnetic pole 2, is used confronting with a magneto-optical recording medium. Also, a yoke part 4 which forms the return path of a magnetic flux is arranged at the base end side of the main magnetic pole 2, from which a required magnetic field can be generated. The winding 3 is the one to magnetize the hard magnetic material H1 of the main magnetic pole 2, and by setting the direction of a current to be supplied to the in winding 3 adversely, it is possible to set the direction of a magnetic field adversely. In this way, since it is possible to generate the magnetic field in a prescribed direction of magnetic field by inversing the direction of magnetization, the fast operation can be performed, and the power consumption can be reduced to a minimum level.

Description

【発明の詳細な説明】 A、産業上の利用分野 本発明は、光磁気記録媒体に対して変調磁界を印加する
ための高周波変調磁界発生装置に関し、特にオーバーラ
イド(重ね書き)を低消費電力等を実現しながら行うも
のである。
DETAILED DESCRIPTION OF THE INVENTION A. Industrial Application Field The present invention relates to a high frequency modulated magnetic field generator for applying a modulated magnetic field to a magneto-optical recording medium. This is done while realizing the following.

B1発明の概要 本発明は、光磁気記録媒体に対向する主磁極と該主磁極
に巻回される巻線とを有する高周波変調磁界発生装置に
おいて、軟磁性材料部分と硬磁性材料部分をその長手方
向に配列した主磁極を用いることにより、光磁気記録を
低消費電力等を実現しながら行うものである。
B1 Summary of the Invention The present invention provides a high-frequency modulated magnetic field generator having a main magnetic pole facing a magneto-optical recording medium and a winding wound around the main magnetic pole, in which a soft magnetic material portion and a hard magnetic material portion are connected to each other along their longitudinal sides. By using main magnetic poles arranged in the same direction, magneto-optical recording can be performed while achieving low power consumption.

C3従来の技術 光磁気記録再生において、実時間でのオーバーライドを
可能とするため方法の一つとして、磁気変調方式で記録
を行う方法がある。
C3 Prior Art In magneto-optical recording and reproduction, one method for enabling override in real time is to perform recording using a magnetic modulation method.

ここで、磁界変調方式による情報信号の記録・再生方法
について、第12図を参照しながら簡単に説明すると、
先ず、レンズ102を介してレーザービームで光磁気記
録媒体100を加熱するためのレーザー装置101と、
入力信号に応じて変調する磁界を発生させる磁界発生装
置103によって記録・再生が行われる。すなわち、上
記レーザー装置101により光磁気記録媒体100の記
録すべき部分が加熱され、この加熱された部分に磁界発
生装置103によって所定の方向の磁界を印加すること
で、その方向に上記加熱部分が磁化され、この磁化によ
り記録・消去が行われる。
Here, the method of recording and reproducing information signals using the magnetic field modulation method will be briefly explained with reference to FIG.
First, a laser device 101 for heating the magneto-optical recording medium 100 with a laser beam through a lens 102;
Recording and reproduction are performed by a magnetic field generating device 103 that generates a magnetic field that is modulated according to an input signal. That is, the portion of the magneto-optical recording medium 100 to be recorded is heated by the laser device 101, and by applying a magnetic field in a predetermined direction to the heated portion by the magnetic field generator 103, the heated portion is heated in that direction. It is magnetized, and recording and erasing are performed by this magnetization.

D0発明が解決しようとする問題点 ところで、上述の磁界発生装置103は、所定の方向に
磁界を発生させる機能が必要とされ、このような磁界発
生装置103の例としては、主磁極が軟磁性材料により
構成される装置と、主磁極が永久磁石等の硬磁性材料に
より構成される装置がある。
D0 Problems to be Solved by the Invention By the way, the magnetic field generating device 103 described above is required to have a function of generating a magnetic field in a predetermined direction. There are devices whose main magnetic pole is made of a hard magnetic material such as a permanent magnet.

しかしながら、主磁極が軟磁性材料により構成される装
置では、核上磁極に巻回されてなる巻線によって励磁を
行う必要があり、このため、磁界を発生させるときは連
続的な通電が必要となり、このような通電によっては、
その消費電力が増大することになる。また、主磁極が軟
磁性材料により構成される装置では、励磁を行う場合に
供給する電流が必要であり、この電流は巻線抵抗FM失
を伴い、この損失を低減しなければ、光磁気記録用の磁
界発生装置全体としての損失は大きなものとなる。
However, in devices where the main magnetic pole is made of a soft magnetic material, it is necessary to excite the winding wound around the nuclear magnetic pole, and therefore, continuous energization is required to generate a magnetic field. , depending on such energization,
The power consumption will increase. In addition, in devices where the main pole is made of a soft magnetic material, a current is required to be supplied when excitation is performed, and this current is accompanied by winding resistance FM loss, and if this loss is not reduced, magneto-optical recording will occur. The loss of the magnetic field generator as a whole is large.

また、主磁極が永久磁石等の硬磁性材料により構成され
る装置にあっては、機械的動作によって磁界の方向を反
転させてなるものがあり、その場合に、反転速度の高速
化が困難であることや、長期間使用した場合の信頼性の
面で不安が残されることになる。
Additionally, in some devices where the main magnetic pole is made of hard magnetic material such as a permanent magnet, the direction of the magnetic field is reversed by mechanical operation, and in that case, it is difficult to increase the reversal speed. However, there are still concerns about reliability when used for a long period of time.

そこで、本発明は上述の問題点に鑑み、消費電力の低減
を実現しながら、必要な磁界を発生させ、しかも高速動
作や信頼性の面で優れる高周波変調磁界発生装置の提供
を目的とする。
SUMMARY OF THE INVENTION In view of the above-mentioned problems, it is an object of the present invention to provide a high-frequency modulated magnetic field generating device that can generate a necessary magnetic field while reducing power consumption, and is excellent in high-speed operation and reliability.

E0問題点を解決するための手段 本発明は、光磁気記録媒体に一端で対向する主磁極と、
該主磁極を励磁するための巻線とを有する高周波変調磁
界発生装置において、上記主磁極は軟磁性材料部分と硬
磁性材料部分が該主磁極の長手方向に配列されて構成さ
れていることを特徴とする高周波変調磁界発生装置によ
り上述の問題点を解決する。
Means for Solving the E0 Problem The present invention provides a main magnetic pole facing a magneto-optical recording medium at one end;
In the high frequency modulated magnetic field generating device having a winding for exciting the main magnetic pole, the main magnetic pole is configured such that a soft magnetic material portion and a hard magnetic material portion are arranged in the longitudinal direction of the main magnetic pole. The above-mentioned problems are solved by the characteristic high-frequency modulated magnetic field generator.

また、このような高周波変調磁界発生装置を制御する信
号電流としては、第3図+alに示すような双方向のパ
ルス信号電流Aであっても良く、或いは、第3図(bl
に示すように、パルスの部分に付随して残留磁化を補正
するようなレベル信号を付加する信号電流αであっても
良い。
Further, the signal current for controlling such a high frequency modulated magnetic field generator may be a bidirectional pulse signal current A as shown in Fig. 3+al, or a bidirectional pulse signal current A as shown in Fig. 3 (bl).
The signal current α may be a signal current α that adds a level signal that corrects residual magnetization along with the pulse portion, as shown in FIG.

20作用 本発明の高周波変調磁界発生装置の主磁極は、軟磁性材
料部分と硬磁性材料部分とにより構成されている。この
うち硬磁性材料は、そのヒシテリシス特性からパルス電
流等により着磁の方向を逆転して所定の磁界方向の磁界
を発生させるものである。また、軟磁性材料は、硬磁性
材料のみで主磁極を構成した場合と比較して、硬磁性材
料のみによる減磁界を軽減することができるものである
20 Effects The main pole of the high frequency modulated magnetic field generator of the present invention is composed of a soft magnetic material portion and a hard magnetic material portion. Among these materials, hard magnetic materials generate a magnetic field in a predetermined magnetic field direction by reversing the direction of magnetization using a pulse current or the like due to their hysteresis characteristics. In addition, the soft magnetic material can reduce the demagnetizing field caused only by the hard magnetic material, compared to the case where the main pole is made of only the hard magnetic material.

即ち、本発明の高周波変調磁界発生装置は、このような
軟磁性材料と硬磁性材料を長手方向に配列させており、
主VjL極に巻回される巻線に所定の方向の電流を供給
することによって、上記硬磁性材料に所定の方向(双方
向)の着磁が施されることになる。そして、この硬磁性
材料に施された着磁によって、磁界が発生し、その発生
磁界が光磁気記録媒体に印加されるが、本発明の高周波
変調磁界発生装置では上記軟磁性材料によって減磁界が
軽減されるため、励磁電流は小さくて済み、また光磁気
記録媒体に印加する磁界を発生させる残留磁化も大きい
ものとなる。
That is, the high frequency modulated magnetic field generating device of the present invention has such soft magnetic materials and hard magnetic materials arranged in the longitudinal direction,
By supplying a current in a predetermined direction to the winding wound around the main VjL pole, the hard magnetic material is magnetized in a predetermined direction (bidirectional). A magnetic field is generated by the magnetization applied to this hard magnetic material, and the generated magnetic field is applied to the magneto-optical recording medium. However, in the high frequency modulated magnetic field generating device of the present invention, the demagnetizing field is generated by the soft magnetic material. Since the magnetism is reduced, the excitation current can be small, and the residual magnetization that generates the magnetic field applied to the magneto-optical recording medium can also be large.

G、実施例 本発明の好適な実施例を図面を参照しながら説明する。G. Example Preferred embodiments of the present invention will be described with reference to the drawings.

】」」γ笈旅」L 本発明の第1の実施例の高周波変調磁界発生装置1は、
第1図及び第2図に示すように、主磁極2が軟磁性材料
にて構成される軟磁性材料部S1、S2と硬磁性材料に
て構成される硬磁性材料部H1を軸方向である長手方向
に配列しており、該主磁極2には励磁を行うための巻線
3が巻回され、該主磁極2の一端側である先端部5は光
磁気記録媒体に対向して用いられる。また、上記主磁極
2の基端側からは磁束のリターンパスとなるヨーク部4
が配設されており、所要の磁界を発生させることができ
る。
】” γ-tabi ” L The high-frequency modulated magnetic field generating device 1 of the first embodiment of the present invention has the following features:
As shown in FIGS. 1 and 2, the main pole 2 has soft magnetic material portions S1 and S2 made of soft magnetic material and hard magnetic material portion H1 made of hard magnetic material in the axial direction. They are arranged in the longitudinal direction, and a winding 3 for excitation is wound around the main magnetic pole 2, and the tip 5, which is one end of the main magnetic pole 2, is used to face the magneto-optical recording medium. . In addition, from the base end side of the main magnetic pole 2, a yoke portion 4 serves as a return path for magnetic flux.
is installed to generate the required magnetic field.

上記主磁極2は、上記巻線3に供給される信号によって
所定の方向に励磁(着磁)され、この主磁極2の先端側
に配される光磁気記録媒体1に変調磁界を印加すること
ができる。このような主磁極2は、軟磁性材料部SL、
硬磁性材料部H1゜軟磁性材料部S2と積層された構造
になっており、このうち硬磁性材料部H1がそのヒシテ
リシス特性から後述するような電流の供給によって着磁
され、その残留磁化が発生磁界として用いられる。
The main magnetic pole 2 is excited (magnetized) in a predetermined direction by a signal supplied to the winding 3, and applies a modulated magnetic field to the magneto-optical recording medium 1 disposed on the tip side of the main magnetic pole 2. Can be done. Such a main magnetic pole 2 includes a soft magnetic material portion SL,
It has a structure in which the hard magnetic material part H1 and the soft magnetic material part S2 are laminated, and of these, the hard magnetic material part H1 is magnetized by the supply of current as described later due to its hysteresis characteristics, and residual magnetization occurs. Used as a magnetic field.

そして、軟磁性材料部SL、S2はそれぞれ高透磁率材
料により構成されるから、残留磁化による発生磁界を効
率良く光磁気記録媒体に供給させることができ、また、
着磁の際には、その励磁電流を低減させることができる
。このような主磁極2の先端の形状は、テーパーを有す
るようにしても良く、また、主磁極2は円筒状でも良く
、ディスク等を媒体とするときは、記録層の全幅に亘る
ような形状であっても良い。
Since the soft magnetic material parts SL and S2 are each made of a high magnetic permeability material, the magnetic field generated by residual magnetization can be efficiently supplied to the magneto-optical recording medium, and
During magnetization, the excitation current can be reduced. The shape of the tip of the main magnetic pole 2 may be tapered, or the main magnetic pole 2 may be cylindrical, and when a disk or the like is used as a medium, the main magnetic pole 2 may have a shape that spans the entire width of the recording layer. It may be.

ここで、硬磁性材料部H1は、例えば保磁力600(O
e)、残留磁束密度1900 (Oe)(垂直方向)程
度のBaフェライト等を用いることができ、また、これ
に限定されず、Cu−Ni−Fe等の金属磁石、酸化物
又は金属の微粒子形磁石、各種モールド磁石等を用いる
ことができる。
Here, the hard magnetic material portion H1 has a coercive force of 600 (O
e) Ba ferrite with a residual magnetic flux density of about 1900 (Oe) (in the vertical direction) can be used, but is not limited to this, and metal magnets such as Cu-Ni-Fe, oxides or metal fine particles can be used. A magnet, various molded magnets, etc. can be used.

また、軟磁性材料部Sl、S2としては、例えば透磁率
800〜l 000 (IMHz)のMn−Znフェラ
イト或いはNi−Znフェライト等を用いることができ
、また、これに限定されず各種フェライト、積層パーマ
ロイ、積層アモルファス、センダスト、圧粉鉄心等を用
いることができる。なお、上記硬磁性材料H1は、スパ
ッタリング法等により形成した薄膜であっても良い。
In addition, as the soft magnetic material portions Sl and S2, for example, Mn-Zn ferrite or Ni-Zn ferrite having a magnetic permeability of 800 to 1000 (IMHz) can be used, but the material is not limited thereto, and various ferrites, laminated layers, etc. can be used. Permalloy, laminated amorphous, sendust, powdered iron core, etc. can be used. Note that the hard magnetic material H1 may be a thin film formed by a sputtering method or the like.

上記巻線3は、上記主磁極2の上記硬磁性材料H1を着
磁するためのものであり、この巻線3に供給する電流の
方向を逆方向とすることにより、発生する磁界の方向を
逆方向とすることができる。
The winding 3 is for magnetizing the hard magnetic material H1 of the main pole 2, and by setting the direction of the current supplied to the winding 3 in the opposite direction, the direction of the generated magnetic field can be changed. It can be in the opposite direction.

また、後述するように単に着磁のためのみならず、発生
磁界が弱いときには、通電により記録・消去のための磁
界を補償することもできる。
Further, as will be described later, when the generated magnetic field is weak, it is possible to compensate for the magnetic field not only for magnetization but also for recording and erasing by energizing.

ここで、このような本実施例の高周波変調磁界発生装置
lの具体的な寸法の一例について説明すると、例えば高
周波変調磁界発生装置1の高さhが5關1幅Wが811
.主磁極2の先端部5が2×11m、ヨーク部4の厚み
tが1m、 ヨーク部4の先端と先端部5の間隔gが2
關、そして、上記軟磁性材料部S1の厚み11がlux
、上記硬磁性材料部H1の厚み12がI鶴の各寸法に設
定することができる。なお、ヨーク部4の形状について
は、主磁極2の方向にそれぞれ延在するようにしても良
い。
Here, an example of specific dimensions of the high frequency modulated magnetic field generating device l of this embodiment will be explained. For example, the high frequency modulating magnetic field generating device 1 has a height h of 5 mm and a width W of 811 mm.
.. The tip portion 5 of the main magnetic pole 2 is 2×11 m, the thickness t of the yoke portion 4 is 1 m, and the distance g between the tip of the yoke portion 4 and the tip portion 5 is 2
Also, the thickness 11 of the soft magnetic material portion S1 is lux
, the thickness 12 of the hard magnetic material portion H1 can be set to each dimension of the I-tsuru. Note that the shape of the yoke portion 4 may be such that it extends in the direction of the main magnetic pole 2.

次に、このように本実施例の高周波変調磁界発生装置1
の動作について、第3図及び第4図を参照しながら、特
に主磁極を軟磁性材料のみで構成した場合や主磁極を硬
磁性材料のみで構成した場合との比較において説明する
Next, as described above, the high frequency modulated magnetic field generating device 1 of this embodiment will be described.
The operation will be explained with reference to FIGS. 3 and 4, especially in comparison with the case where the main pole is made of only soft magnetic material and the case where the main pole is made of only hard magnetic material.

先ず、第3図は横軸に時間をとり、[al及び(blの
縦軸は電流値1.(e)の縦軸は磁化M、(dlの縦軸
は発生する磁界の強度H(垂直方向)をそれぞれ示して
いる。
First, in Figure 3, the horizontal axis is time, the vertical axis of [al and (bl) is the current value 1, the vertical axis of (e) is the magnetization M, and the vertical axis of (dl is the intensity H (vertical) of the generated magnetic field. direction).

この第3図(alに示す波形信号Aが、本実施例の高周
波変調磁界発生装置1に供給される信号電流の一例であ
り、この波形信号Aによって、主磁極2の硬磁性材料部
H1が双方向に着磁される。即ち、この波形信号Aの中
、パルスAl(A3)の電流によって、一方向に上記硬
磁性材料部H1が着磁され、次にパルスA2の電流によ
って、反対方向に上記硬磁性材料部H1が着磁される。
The waveform signal A shown in FIG. In other words, in this waveform signal A, the hard magnetic material portion H1 is magnetized in one direction by the current of pulse Al (A3), and then in the opposite direction by the current of pulse A2. The hard magnetic material portion H1 is magnetized.

尚、第3図は順次反対方向の磁界を発生させるときの信
号電流の例について示したものである。
Incidentally, FIG. 3 shows an example of a signal current when magnetic fields in opposite directions are sequentially generated.

これに対して、主磁極を全て軟磁性材料によって構成し
たときには、(alに破線で示すように一定期間連続し
た通電を必要とする波形信号Bとなる。
On the other hand, when the main pole is entirely made of soft magnetic material, the waveform signal B becomes a waveform signal that requires continuous energization for a certain period of time, as shown by the broken line in (al).

そして、この波形信号Bと上記波形信号Aを比較してみ
ると、消費電力の面で明らかにパルス電流である波形信
号Aの方が有利であり、従って、軟磁性材料と硬磁性材
料を配列させた主磁極2を有する本実施例の高周波変調
磁界発生装置1が低消費電力を実現できることが示され
る。
Comparing this waveform signal B and the above waveform signal A, it is clear that waveform signal A, which is a pulsed current, is more advantageous in terms of power consumption. It is shown that the high-frequency modulated magnetic field generating device 1 of this embodiment, which has the main magnetic pole 2 having the above-mentioned shape, can realize low power consumption.

第3図(C)は、硬磁性材料部H1の磁化を示したもの
であり、実線で示す磁化曲線Cが上記信号電流Aを供給
したときの硬磁性材料部H1の磁化を示している。ここ
で、この硬磁性材料部H1における磁化過程を第4図a
を参照しながら説明すると、上記信号電流Aのパルス電
流A1に対応して磁化曲線Cもパルス波形状の値alを
とり、これは第4図aに示すようなヒレテリシスループ
上のalに対応する。次に、信号電流Aが零となり、外
部磁界は零となるが、残留磁界と反磁界から当該硬磁性
材料部H1の磁化は、磁化曲線C上の51であり、これ
は第4図aのパーミアンス線上のblとなる。
FIG. 3(C) shows the magnetization of the hard magnetic material portion H1, and a magnetization curve C shown by a solid line shows the magnetization of the hard magnetic material portion H1 when the signal current A is supplied. Here, the magnetization process in this hard magnetic material portion H1 is shown in Figure 4a.
To explain with reference to FIG. 4, the magnetization curve C also takes a value al of the pulse waveform in correspondence with the pulse current A1 of the signal current A, and this corresponds to al on the hereteresis loop as shown in Fig. 4a. do. Next, the signal current A becomes zero and the external magnetic field becomes zero, but due to the residual magnetic field and demagnetizing field, the magnetization of the hard magnetic material portion H1 is 51 on the magnetization curve C, which is shown in Figure 4a. bl is on the permeance line.

続いて、逆方向の磁界の発生のためには、逆方向のパル
ス電流A2を供給することが必要であり、信号電流Aの
パルス電流A2を本実施例の高周波変調磁界発生装置1
に供給したときには、硬磁性材料部H1は前述の場合と
反対の磁化過程をとる。
Next, in order to generate a magnetic field in the opposite direction, it is necessary to supply the pulse current A2 in the opposite direction, and the pulse current A2 of the signal current A is supplied to the high frequency modulated magnetic field generator 1 of this embodiment.
When the hard magnetic material portion H1 is supplied with a magnet, the hard magnetic material portion H1 undergoes a magnetization process opposite to that described above.

即ち、磁化曲線Cは逆方向の値c1からdlをとなり、
これら’L+dLはそれぞれ第4図aのヒレテリシスル
ープ上のcl、dlに対応したものとなる。
That is, the magnetization curve C becomes dl from the value c1 in the opposite direction,
These 'L+dL correspond to cl and dl on the hereteresis loop in FIG. 4a, respectively.

このような履歴を示す本実施例の高周波変調磁界発生装
置1を、軟磁性材料部を除去し特に硬磁性材料部のみで
主磁極を構成したものと比較してみると、第3図fC1
中、波形りが硬磁性材料のみで主磁極を構成した装置の
磁化過程を示すことになり、この波形り上の点a3.b
3.c3.d3の各点の値は、いずれも上述の高周波変
調磁界発生装置1にかかる磁化曲線Cとの比較において
小さい値となることが示される。また、このときのヒシ
テリシスルーブは、第4図Cに示すように小さいループ
となる。なお、第4図C中a3.b3゜C3+d3の各
点は波形りの同記号の各点と対応している。
Comparing the high frequency modulated magnetic field generating device 1 of this embodiment, which exhibits such a history, with one in which the soft magnetic material portion is removed and the main magnetic pole is composed of only the hard magnetic material portion, it is found that Fig. 3 fC1
The waveform in the middle shows the magnetization process of a device whose main magnetic pole is made of only hard magnetic material, and points a3. on this waveform. b
3. c3. It is shown that the value of each point of d3 is a small value when compared with the magnetization curve C related to the above-described high frequency modulated magnetic field generating device 1. Further, the hysteresis loop at this time becomes a small loop as shown in FIG. 4C. In addition, a3. in FIG. 4C. Each point of b3°C3+d3 corresponds to each point of the same symbol on the waveform.

このことは、仮に軟磁性材料を除いて硬磁性材料のみで
主磁極を構成したときには、軟磁性材料がなくなったこ
とから主磁極に集束されていた磁束が減少してシテリシ
スルーブが小さくなり、このように硬磁性材料のみで主
磁極を構成したときは、発生磁界が小さくなるため、光
磁気記録媒体に用いることのできる磁界も小さくなるこ
とになる。従って、本実施例のように硬磁性材料と軟磁
性材料を配列させてなる高周波変調磁界発生装置の方が
、記録消去の特性に優れることになる。
This means that if the main magnetic pole were made of only hard magnetic material without the soft magnetic material, the magnetic flux that was focused on the main magnetic pole would decrease due to the absence of the soft magnetic material, and the sithesis loop would become smaller. When the main pole is made of only a hard magnetic material, the generated magnetic field becomes smaller, and therefore the magnetic field that can be used in the magneto-optical recording medium also becomes smaller. Therefore, a high-frequency modulated magnetic field generating device made by arranging a hard magnetic material and a soft magnetic material as in this embodiment has better recording and erasing characteristics.

以上のように本実施例の高周波変調磁界発生装置1によ
って発生する磁界は、主磁極を軟磁性材料のみで構成し
た場合に比較して低消費電力で発生させることができ、
また、主磁極を硬磁性材料のみで構成した場合に比較し
て強い磁界となる。
As described above, the magnetic field generated by the high frequency modulated magnetic field generating device 1 of this embodiment can be generated with lower power consumption than when the main pole is made of only soft magnetic material.
Furthermore, the magnetic field is stronger than when the main pole is made of only hard magnetic material.

そして、この本実施例の高周波変調磁界発生装置lによ
り発生する磁界は、上記硬磁性材料部H1の磁化曲線C
に対応して、第3図fdlに示すような磁界曲線Eとな
り、この磁化曲線Eが励磁のための信号電流Aに対する
光磁気記録媒体への印加磁界となる。
The magnetic field generated by the high frequency modulated magnetic field generator l of this embodiment is based on the magnetization curve C of the hard magnetic material portion H1.
Correspondingly, a magnetic field curve E as shown in FIG. 3 fdl is obtained, and this magnetization curve E becomes the magnetic field applied to the magneto-optical recording medium with respect to the signal current A for excitation.

ところで、本実施例の高周波変調磁界発生装置1は、上
述のように主磁極を軟磁性材料のみや硬磁性材料のみで
構成した場合に比較して、光磁気記録媒体への印加磁界
として好適なものを発生させることが可能であるが、さ
らに本実施例の高周波変調磁界発生装置1では、第3図
(blに示すように、パルスの部分に付随して残留磁化
を補正するようなレベル信号を付加する信号電流αによ
り、残留磁化が不足する部分を補償して、良好かつ確実
な光磁気記録を実現することが可能である。
By the way, the high-frequency modulated magnetic field generating device 1 of the present embodiment is more suitable for applying a magnetic field to a magneto-optical recording medium than when the main pole is made of only soft magnetic material or only hard magnetic material as described above. In addition, the high-frequency modulated magnetic field generating device 1 of this embodiment generates a level signal that corrects residual magnetization accompanying the pulse portion, as shown in FIG. 3 (bl). By adding the signal current α, it is possible to compensate for the insufficient residual magnetization and realize good and reliable magneto-optical recording.

即ち、第3図(b)に示すように、パルス電流部B1及
びレベル信号部B2からなる信号電流Bを高周波変調磁
界発生装置1に供給する。この場合において、パルス電
流部B1は、上述の信号電流Aのパルス電流A1と同様
に上記硬磁性材料部+11の磁化の方向を着磁し反転さ
せる機能を有するが、さらにレベル信号部B2によって
、電流を零としたときに減少する残留磁化を補償して強
い磁界を発生させることができる。第3図(C1に二点
鎖線で示す磁化曲線βは、上記信号電流αによって形成
される硬磁性材料部H1の磁化の値を示したものであり
、ここで第4図すのヒシテリシスルーブとの対応におい
て説明すると、先ず、上記パルス電流部B1が加わった
ときには、硬磁性材料部H1の状態は点a2の状態であ
るが、このパルス電流部B1に付随するレベル信号部B
2の信号に対応して硬磁性材料部H1の磁化は点b2と
なる。この点b2は、第4図す上では、第4図aのパー
ミアンス線よりも急峻な傾きを有するパーミアンス線b
2d、上に位置しており、上記残留磁化を補償するため
のレベル信号部B2によって、減磁界が相殺されて、有
効な発生磁界が高くなっていることが分かる。なお、反
対方向の磁界の発生についても、磁化曲線β及び第し図
すのヒレテリシスループ上の点d2に示されるように、
減磁界が相殺されて、有効な発生磁界が高くなる。また
、第3図Cdl中、二点鎖線で示す波形Tは、このよう
にレベル信号部B2により残留磁界が補償されてなる本
実施例の高周波変調磁界発生装置1の発生磁界を示して
いる。
That is, as shown in FIG. 3(b), a signal current B consisting of a pulse current section B1 and a level signal section B2 is supplied to the high frequency modulated magnetic field generating device 1. In this case, the pulse current section B1 has the function of magnetizing and reversing the direction of magnetization of the hard magnetic material section +11 in the same way as the pulse current A1 of the signal current A described above; It is possible to generate a strong magnetic field by compensating for the residual magnetization that decreases when the current is reduced to zero. The magnetization curve β shown by the two-dot chain line in Figure 3 (C1) shows the value of magnetization of the hard magnetic material portion H1 formed by the signal current α, and here the hysteresis curve shown in Figure 4 First, when the pulse current section B1 is added, the state of the hard magnetic material section H1 is at point a2, but the level signal section B attached to this pulse current section B1 is
In response to the signal No. 2, the magnetization of the hard magnetic material portion H1 becomes point b2. This point b2 is located on the permeance line b, which has a steeper slope than the permeance line in Fig. 4a in Fig. 4.
It can be seen that the demagnetizing field is canceled out by the level signal section B2 located above 2d and for compensating the residual magnetization, and the effective generated magnetic field is increased. Regarding the generation of a magnetic field in the opposite direction, as shown at point d2 on the magnetization curve β and the hereteresis loop in Figure 2,
The demagnetizing fields cancel each other out, increasing the effective generated magnetic field. Further, in FIG. 3 Cdl, the waveform T shown by the two-dot chain line shows the generated magnetic field of the high frequency modulated magnetic field generating device 1 of this embodiment in which the residual magnetic field is compensated by the level signal section B2 in this way.

上述のように本実施例の高周波変調磁界発生装置1は、
連続的な通電を必要とする軟磁性材料のみで主磁極を構
成する磁界発生装置に比較して、励磁のための電流が少
なくて済むことから、低消費電流を実現することができ
、また、この場合の巻線抵抗による電力損失の低減も可
能である。また、硬磁性材料のみで主磁極を構成した場
合に比べて、軟磁性材料が近傍に配列されていることか
ら、効率良く強い磁界を発生させることができ、双方向
の着磁も容易となる。
As mentioned above, the high frequency modulated magnetic field generating device 1 of this embodiment has the following features:
Compared to magnetic field generators in which the main pole is made of only soft magnetic materials that require continuous energization, the current required for excitation is smaller, resulting in lower current consumption. In this case, it is also possible to reduce power loss due to winding resistance. In addition, compared to a case where the main pole is made of only hard magnetic materials, since the soft magnetic materials are arranged nearby, it is possible to generate a strong magnetic field more efficiently, and bidirectional magnetization is also easier. .

ここで、このような高周波変調磁界発生装置1の有効範
囲について説明すると、巻線抵抗による電力損失が、配
列した硬磁性材料部のコア損失を上回ることが前提とな
るため、 式       +2 R>fvS (I;巻線実効電流(A)、f;電流周波数(Hz〕、
R;巻線抵抗〔Ω〕、S;硬磁性材料部断面積(wb−
A/ボ〕、V;硬磁性材料堆積Cm1が有効範囲を定め
ることになる。
Here, to explain the effective range of such a high frequency modulated magnetic field generator 1, it is assumed that the power loss due to the winding resistance exceeds the core loss of the arranged hard magnetic material parts, so the formula +2 R>fvS (I: winding effective current (A), f: current frequency (Hz),
R: Winding resistance [Ω], S: Cross-sectional area of hard magnetic material (wb-
A/V], V: The hard magnetic material deposition Cm1 determines the effective range.

なお、硬磁性材料部については、主磁極2の一断面に亘
って配されるようなものであれば良く、特に形状は限定
されるものではない。また、複数の硬磁性材料部を配設
しても良い。
Note that the hard magnetic material portion is not particularly limited in shape as long as it is disposed over one cross section of the main magnetic pole 2. Moreover, a plurality of hard magnetic material parts may be provided.

■1豊実臭医 本発明の第2の実施例の高周波変調磁界発生装置50は
、第5図に示すように、略E字状の磁極を有しており、
その主磁極52は硬磁性材料部S51と軟磁性材料35
1により構成されているが、上記硬磁性材料部1151
が光磁気記録媒体に対向する一端に配列されている。こ
のように硬磁性材料部H1のように軟磁性材料部に挟持
されて用いられるのみならず、端部に配するようにして
も良(、同様に低消費電力や効率良く強い磁界を発生さ
せることができる。なお、材料や動作等については、第
1の実施例の高周波変調磁界発生装置1と同様である。
■1 Toyomi Odor Doctor A high-frequency modulated magnetic field generating device 50 according to a second embodiment of the present invention has approximately E-shaped magnetic poles, as shown in FIG.
The main magnetic pole 52 includes a hard magnetic material portion S51 and a soft magnetic material portion 35.
1, the hard magnetic material portion 1151
are arranged at one end facing the magneto-optical recording medium. In this way, it can be used not only by being sandwiched between the soft magnetic material parts like the hard magnetic material part H1, but also by placing it at the end (similarly, it can generate a strong magnetic field with low power consumption and efficiency). Note that the materials, operations, etc. are the same as those of the high frequency modulated magnetic field generating device 1 of the first embodiment.

築主互尖土何 本発明の第3の実施例の高周波変調磁界発生装置60は
、第6図に示すように、上述の高周波変調磁界発生装置
lをその中心軸で回転させたような構造を有している。
As shown in FIG. 6, a high-frequency modulated magnetic field generating device 60 according to a third embodiment of the present invention has a structure in which the above-described high-frequency modulated magnetic field generating device 1 is rotated about its central axis. have.

即ち、円筒形状とされる主磁極63で軟磁性材料にて構
成される軟磁性材料部S61、S62と硬磁性材料にて
構成される硬磁性材料部H61を軸方向である長手方向
に配列しており、該主磁極63には第3図に示すような
信号電流によって効果的に励磁を行うことができる巻線
64が巻回され、核上磁極63の一端側である先端部6
5は光磁気記録媒体に対向して用いられる。また、上記
主磁極63の基端側からは略円筒状に直立して磁束のリ
ターンバスとなるヨーク部66が配設されており、所要
の磁界を発生させることができる。
That is, in the main pole 63 having a cylindrical shape, soft magnetic material parts S61 and S62 made of soft magnetic material and hard magnetic material part H61 made of hard magnetic material are arranged in the longitudinal direction which is the axial direction. The main magnetic pole 63 is wound with a winding 64 that can be effectively excited by a signal current as shown in FIG.
5 is used facing the magneto-optical recording medium. Further, a yoke portion 66 is provided from the base end side of the main magnetic pole 63 in a substantially cylindrical shape and serves as a return bus for magnetic flux, so that a required magnetic field can be generated.

このような回転体形状の高周波変調磁界発生装置60で
あっても同様に、低消費電力や効率良く強い磁界を発生
させることができる。なお、材料や動作等については、
第1の実施例の高周波変調磁界発生装置1と同様である
Even with such a rotating body-shaped high frequency modulated magnetic field generating device 60, it is possible to similarly generate a strong magnetic field with low power consumption and efficiency. Regarding materials, operation, etc.,
This is similar to the high frequency modulated magnetic field generating device 1 of the first embodiment.

男」」巧EJL皿 本発明の第4の実施例の高周波変調磁界発生装置70は
、第7図に示すように、上述の高周波変調磁界発生装置
50をその中心軸で回転させたような構造を有している
。即ち、光磁気記録媒体に対向する一端側には硬磁性材
料部H71が形成され、主磁極72はこの硬磁性材料部
H71と高透磁率材料である軟磁性材料S71によって
外観円柱形状に構成されている。そして、これに励磁の
ための巻線74が配設され、この巻線74には、第3図
に示したようなパルス電流やパルス電流とレベル信号の
組からなる信号等を供給することができる。また、ヨー
ク部75も円筒形状に形成されている。
A high-frequency modulated magnetic field generator 70 according to a fourth embodiment of the present invention has a structure in which the above-described high-frequency modulated magnetic field generator 50 is rotated about its central axis, as shown in FIG. have. That is, a hard magnetic material portion H71 is formed on one end side facing the magneto-optical recording medium, and the main magnetic pole 72 is formed into a cylindrical shape in appearance by this hard magnetic material portion H71 and a soft magnetic material S71 which is a high magnetic permeability material. ing. A winding 74 for excitation is disposed on this, and this winding 74 can be supplied with a pulse current or a signal consisting of a combination of a pulse current and a level signal as shown in FIG. can. Further, the yoke portion 75 is also formed in a cylindrical shape.

このような回転体形状であっても同様に、低消費電力や
効率良く強い磁界を発生させることができる。尚、材料
や動作等については、第1の実施例の高周波変調磁界発
生装置1と同様である。
Even with such a rotating body shape, a strong magnetic field can be generated with low power consumption and efficiency. Note that the materials, operation, etc. are the same as those of the high frequency modulated magnetic field generating device 1 of the first embodiment.

芽畳しl実」1舛 本発明の第5の実施例の高周波変調磁界発生装置80は
、第8図に示すように、略I字状の主磁極83を有して
なる高周波変調磁界発生装置80であり、その主磁極8
3は、軟磁性材料部S81゜硬磁性材料部H81,軟磁
性材料S82と積層配列されて形成されている。この主
磁極83の形状は略角柱状であるが、三角柱状9円柱状
、六角柱状であっても良い。この軟磁性材料と硬磁性材
料を配列させてなる主磁極83には、励磁のための巻線
84が巻回されており、上述の第3図に示したようなパ
ルス電流やレベル信号電流を付加して残留磁化を補償す
るように信号電流によって、有効な磁界を発生させて、
光磁気記録に用いることができる。
A high-frequency modulated magnetic field generating device 80 according to a fifth embodiment of the present invention is a high-frequency modulated magnetic field generating device having a substantially I-shaped main magnetic pole 83, as shown in FIG. 80, and its main magnetic pole 8
3 is formed by laminating and arranging a soft magnetic material portion S81°, a hard magnetic material portion H81, and a soft magnetic material S82. The main magnetic pole 83 has a substantially prismatic shape, but may also have a triangular column shape, a cylindrical shape, or a hexagonal column shape. A winding 84 for excitation is wound around the main magnetic pole 83, which is made by arranging a soft magnetic material and a hard magnetic material, and receives a pulse current or level signal current as shown in FIG. generating an effective magnetic field by means of a signal current to compensate for the residual magnetization;
It can be used for magneto-optical recording.

尚、材料や動作等については、第1の実施例の高周波変
調磁界発生装置1と同様であり、また、低消費電力を実
現でき、効率良く強い磁界を発生させうろことは言うま
でもない。
It goes without saying that the materials, operation, etc. are the same as those of the high-frequency modulated magnetic field generating device 1 of the first embodiment, and that low power consumption can be realized and a strong magnetic field can be efficiently generated.

第」J巧む1皿 本発明の第6の実施例の高周波変調磁界発生装置90は
、第9図に示すように、略I字状の主磁極93を有して
なる高周波変調磁界発生装置90であり、その主磁極9
3の光磁気記録媒体対向面側の一端には、例えばBaフ
ェライト等の保持力の大きく、残留磁化の大きい硬磁性
材料部H91が形成され、他の主磁極93の部分は軟磁
性材料部S91によって構成されている。また、巻線9
4も巻回されてなり、動作、形状、材料等の点について
上記第5の実施例と同様である。
A high-frequency modulated magnetic field generating device 90 according to a sixth embodiment of the present invention is a high-frequency modulated magnetic field generating device having a main magnetic pole 93 having a substantially I-shape, as shown in FIG. 90, and its main magnetic pole 9
A hard magnetic material portion H91 having a large coercive force and large residual magnetization, such as Ba ferrite, is formed at one end of the magneto-optical recording medium facing surface of No. 3, and the other main pole 93 is formed by a soft magnetic material portion S91. It is made up of. Also, the winding 9
4 is also wound, and is similar to the fifth embodiment in terms of operation, shape, material, etc.

第1少災流■ 本発明の第7の実施例の高周波変調磁界発生装置30は
、第5の実施例の高周波変調磁界発生装置80において
、その主磁極83の形状を略U字状としたものである。
First Minor Disaster■ The high frequency modulated magnetic field generating device 30 according to the seventh embodiment of the present invention is the same as the high frequency modulated magnetic field generating device 80 according to the fifth embodiment, in which the main magnetic pole 83 has a substantially U-shaped shape. It is something.

この主磁極33は、第10図に示すように、着磁するた
めの巻線34が巻回される部分で軟磁性材料部S31.
硬磁性材料部H31,軟磁性材料S32と積層配列され
て形成されている。動作、形状、材料等の点について上
記第5の実施例と同様である。
As shown in FIG. 10, this main magnetic pole 33 has a soft magnetic material portion S31.
A hard magnetic material portion H31 and a soft magnetic material S32 are formed in a stacked arrangement. It is similar to the fifth embodiment in terms of operation, shape, material, etc.

爪主互尖施狙 本発明の第8の実施例の高周波変調磁界発生装置40は
、第11図に示すように、第6の実施例の高周波変調磁
界発生装置90において、その主磁極83の形状を略U
字状としたものである。このU字状の主磁極43の光磁
気記録媒体と対向する面の一端には、その端面に亘って
硬磁性材料部H41が形成されており、その他の主磁極
43の部分は軟磁性材料部S41によって構成されてい
る。
The high frequency modulated magnetic field generating device 40 of the eighth embodiment of the present invention has a main pole 83 of the high frequency modulated magnetic field generating device 90 of the sixth embodiment, as shown in FIG. Shape is abbreviated as U
It is shaped like a letter. At one end of the surface of the U-shaped main pole 43 facing the magneto-optical recording medium, a hard magnetic material portion H41 is formed over the end surface, and the other portions of the main magnetic pole 43 are formed with soft magnetic material portions. It is configured by S41.

このような形状の高周波変調磁界発生装置40であって
も同様に、低消費電力を実現でき、効率良く強い磁界を
発生させることができる。
Even with the high frequency modulated magnetic field generating device 40 having such a shape, low power consumption can be achieved and a strong magnetic field can be generated efficiently.

H,発明の効果 本発明の高周波変調磁界発生装置は、その主磁極が軟磁
性材料部分と硬磁性材料部分とにより構成されているた
め、先ず硬磁性材料部分のヒシテリシス特性からパルス
電流等により着磁の方向を逆転して所定の磁界方向の磁
界を発生させることができ、従って、磁極の機械的な反
転操作は不要であり、高速動作や信頼性の点で優れてい
ると共に軟磁性材料のみの場合等における連続的な通電
を不要とし、光磁気記録媒体に所定方向の磁界を印加す
ることができ、その消費電力は小さなものとなる。
H. Effects of the Invention In the high frequency modulated magnetic field generator of the present invention, since its main magnetic pole is composed of a soft magnetic material part and a hard magnetic material part, first, it is generated by a pulsed current or the like based on the hysteresis characteristic of the hard magnetic material part. It is possible to generate a magnetic field in a predetermined magnetic field direction by reversing the direction of the magnetic field.Therefore, there is no need for mechanical reversal of the magnetic poles, and it is superior in terms of high-speed operation and reliability, and only requires soft magnetic materials. It is possible to apply a magnetic field in a predetermined direction to the magneto-optical recording medium without the need for continuous energization in cases such as the above, and the power consumption becomes small.

そして、本発明の高周波変調磁界発生装置は、上記軟磁
性材料によって減磁界が軽減され、その高透磁率特性か
ら励磁電流は小さくて済み、また光磁気記録媒体に印加
する磁界を発生させる残留磁化も大きいものとなる。
The high-frequency modulated magnetic field generator of the present invention reduces the demagnetizing field by the soft magnetic material, requires only a small excitation current due to its high magnetic permeability, and has residual magnetization that generates the magnetic field applied to the magneto-optical recording medium. will also be large.

また、着磁のための信号電流も単にパルス電流による場
合に躍定されず、残留磁化を補償するような信号電流を
供給することができ、極めて光磁気記録に通したものと
なる。
Furthermore, the signal current for magnetization is not abrupt when simply using a pulse current, and a signal current that compensates for residual magnetization can be supplied, making it extremely suitable for magneto-optical recording.

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

第1図は本発明の第1の実施例の高周波変調磁界発生装
置を説明するための断面図、第2図はその斜視図、第3
図は本発明の高周波変調磁界発生装置の動作を説明する
ための波形図であって、第3図(a)はパルス電流Aに
かかる波形図、第3図(blは残留磁化を?lli償す
る信号電流の波形図、第3図tc+は硬磁性材料部の磁
化を示すための波形図、第3図fdlは発生する磁界の
強さを示すための波形図である。 また、第4図a −cは、それぞれ硬磁性材料部の磁化
過程を示すための特性図であって、第4図aは磁化曲線
Cに対応する特性図、第4図すは磁化曲線βに対応する
特性図、第4図Cは波形りに対応する特性図である。 また、第5図は本発明の第2の実施例の高周波変調磁界
発生装置を説明するための斜視図、第6図は本発明の第
3の実施例の高周波変調磁界発生装置を説明するための
斜視図、第7図は本発明の第4の実施例の高周波変調磁
界発生装置を説明するための斜視図、第8図は本発明の
第5の実施例の高周波変調磁界発生装置を説明するため
の斜視図、第9図は本発明の第6の実施例の高周波変調
磁界発生装置を説明するための斜視図、第10図は本発
明の第7の実施例の高周波変調磁界発生装置を説明する
ための斜視図、第11図は本発明の第8の実施例の高周
波変調磁界発生装置を説明するための斜視図である。 また、第12図は磁界変調方式の原理を説明するための
模式図である。 1.30,40,50,60,70.80.90−−−
一−−−−〜−−=−−−−−−−・・・−−−−−一
高周波変調磁界発生装置2.33,43,52,63,
72,83.93−・・・−・−−一−−・・・・−一
−−−−・・−・・・−・主磁極3.34.44,53
.64,73,84.94−・・・−・・−・・−−一
−−−・・−−一−−−−−−−・−巻線ill、  
H31,H41,H51,H61,H71゜H81,H
91−・・・−・−・−・〜−−−−−−硬磁性材料部
SL、S2.S31.S32.  S41.S51゜S
61.S62.S71.S81.S82.S91 ・−
・・−一−−−−−−−−−−−−−−・・・−・−・
軟磁性材料部特 許 出 願 人  ソニー株式会社代
理人   弁理士     手漉 見間       
  田村榮− 第1図 第2図 第3図 第4図a   第4図b   第4図C第5図 第6図 奏−穴宛佇J 第7図 第らの一辺セ号」 第8図 第るめ契殉刑 第9図 簗gfi**4クリ 第11図
FIG. 1 is a cross-sectional view for explaining a high-frequency modulated magnetic field generator according to the first embodiment of the present invention, FIG. 2 is a perspective view thereof, and FIG.
The figures are waveform diagrams for explaining the operation of the high-frequency modulated magnetic field generator of the present invention, in which Fig. 3(a) is a waveform diagram applied to pulse current A, and Fig. 3(bl indicates residual magnetization? FIG. 3 tc+ is a waveform diagram showing the magnetization of the hard magnetic material part, and FIG. 3 fdl is a waveform diagram showing the strength of the generated magnetic field. 4a to 4c are characteristic diagrams showing the magnetization process of the hard magnetic material portion, respectively, and FIG. 4a is a characteristic diagram corresponding to magnetization curve C, and FIG. 4 is a characteristic diagram corresponding to magnetization curve β. , FIG. 4C is a characteristic diagram corresponding to the waveform.Furthermore, FIG. 5 is a perspective view for explaining a high frequency modulated magnetic field generating device according to a second embodiment of the present invention, and FIG. 6 is a characteristic diagram corresponding to the waveform. FIG. 7 is a perspective view for explaining the high frequency modulated magnetic field generating device according to the fourth embodiment of the present invention, and FIG. 8 is a perspective view for explaining the high frequency modulated magnetic field generating device according to the fourth embodiment of the present invention. FIG. 9 is a perspective view for explaining a high frequency modulated magnetic field generating device according to a fifth embodiment of the present invention; FIG. 9 is a perspective view for explaining a high frequency modulated magnetic field generating device according to a sixth embodiment of the present invention; FIG. The figure is a perspective view for explaining a high frequency modulated magnetic field generator according to a seventh embodiment of the present invention, and FIG. 11 is a perspective view for explaining a high frequency modulated magnetic field generator according to an eighth embodiment of the present invention. Also, Fig. 12 is a schematic diagram for explaining the principle of the magnetic field modulation method. 1.30, 40, 50, 60, 70.80.90---
- - - - - - = - - - - - - - - - - - - - - - - - - - - - - - - High frequency modulation magnetic field generator 2.33, 43, 52, 63,
72,83.93-------1-------Main magnetic pole 3.34.44,53
.. 64,73,84.94-・・・・・・−−1−−−・・−1−−−−−−・−Winding ill,
H31, H41, H51, H61, H71°H81, H
91--...----------Hard magnetic material portion SL, S2. S31. S32. S41. S51゜S
61. S62. S71. S81. S82. S91 ・-
・・−1−−−−−−−−−−−−−−・−・−・
Soft Magnetic Materials Department Patent Applicant Sony Corporation Representative Patent Attorney Tezuki Mima
Ei Tamura - Fig. 1 Fig. 2 Fig. 3 Fig. 4 Fig. 4 a Fig. 4 b Fig. 4 C Fig. 5 Rumeki Martyr's Punishment Figure 9 Yan gfi**4 Kuri Figure 11

Claims (1)

【特許請求の範囲】 光磁気記録媒体に一端で対向する主磁極と、該主磁極を
励磁するための巻線とを有する高周波変調磁界発生装置
において、 上記主磁極は軟磁性材料部分と硬磁性材料部分が該主磁
極の長手方向に配列されて構成されていることを特徴と
する高周波変調磁界発生装置。
[Claims] A high-frequency modulated magnetic field generator having a main magnetic pole facing a magneto-optical recording medium at one end and a winding for exciting the main magnetic pole, wherein the main magnetic pole has a soft magnetic material portion and a hard magnetic material portion. A high frequency modulated magnetic field generating device characterized in that material portions are arranged in the longitudinal direction of the main magnetic pole.
JP19561486A 1986-08-22 1986-08-22 Generating device for high frequency modulated magnetic field Pending JPS6353702A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19561486A JPS6353702A (en) 1986-08-22 1986-08-22 Generating device for high frequency modulated magnetic field

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19561486A JPS6353702A (en) 1986-08-22 1986-08-22 Generating device for high frequency modulated magnetic field

Publications (1)

Publication Number Publication Date
JPS6353702A true JPS6353702A (en) 1988-03-08

Family

ID=16344093

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19561486A Pending JPS6353702A (en) 1986-08-22 1986-08-22 Generating device for high frequency modulated magnetic field

Country Status (1)

Country Link
JP (1) JPS6353702A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5373305A (en) * 1992-05-19 1994-12-13 Martin Marietta Corporation RF-transparent antenna sunshield membrane

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5373305A (en) * 1992-05-19 1994-12-13 Martin Marietta Corporation RF-transparent antenna sunshield membrane

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