JPH02130701A - Magneto-optical recording device - Google Patents
Magneto-optical recording deviceInfo
- Publication number
- JPH02130701A JPH02130701A JP28443488A JP28443488A JPH02130701A JP H02130701 A JPH02130701 A JP H02130701A JP 28443488 A JP28443488 A JP 28443488A JP 28443488 A JP28443488 A JP 28443488A JP H02130701 A JPH02130701 A JP H02130701A
- Authority
- JP
- Japan
- Prior art keywords
- magneto
- optical disk
- recorded
- modulation
- coils
- 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
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
- G11B11/10532—Heads
- G11B11/10534—Heads for recording by magnetising, demagnetising or transfer of magnetisation, by radiation, e.g. for thermomagnetic recording
- G11B11/10536—Heads for recording by magnetising, demagnetising or transfer of magnetisation, by radiation, e.g. for thermomagnetic recording using thermic beams, e.g. lasers
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
Landscapes
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Recording Or Reproducing By Magnetic Means (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は光及び磁界を光磁気ディスクに与えて、情報を
記録する光磁気記録装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a magneto-optical recording device that records information by applying light and a magnetic field to a magneto-optical disk.
光磁気記録装置は、情報を記録すべき光磁気ディスクの
一面側にレーザ光を投射し、このレーザ光が投射された
位置の光磁気ディスクの他面側に記録すべき信号に関連
した磁界を与えて、光磁気ディスクに情報を記録するよ
う構成されている。A magneto-optical recording device projects a laser beam onto one side of a magneto-optical disk on which information is to be recorded, and emits a magnetic field related to the signal to be recorded on the other side of the magneto-optical disk at the position where the laser beam is projected. and is configured to record information on the magneto-optical disk.
第2図はこの種の光磁気記録装置の要部を示す模式的部
分断面斜視図である。光磁気ディスク1の一面側にはレ
ーザ光を出射する光ヘッド4が位置しており、そのレー
ザ光5は光磁気ディスク1の基板2を透過して記録膜3
に合焦点を得るように投射されている。光磁気ディスク
1の他面側には記録すべき情報の信号を入力する単一の
変調コイル7を備えている励磁素子6が位置している。FIG. 2 is a schematic partial cross-sectional perspective view showing the main parts of this type of magneto-optical recording device. An optical head 4 that emits a laser beam is located on one surface side of the magneto-optical disk 1, and the laser beam 5 is transmitted through the substrate 2 of the magneto-optical disk 1 to form a recording film 3.
It is projected so that it is in focus. On the other side of the magneto-optical disk 1, an excitation element 6 having a single modulation coil 7 for inputting a signal of information to be recorded is located.
この励磁素子6は、例えば直方体状に形成されていて、
その−側軸端面6aが光磁気ディスク1と対向している
。そして前記変調コイル7に通電することにより、励磁
素子6は光磁気ディスク1の情報記録位置に、記録すべ
き情報に応じた方向の垂直磁界を与え得るようになって
いる。即ち、レーザ光の合焦点位置で加熱された光磁気
ディスク1の情報記録位置は、光磁気ディスク1の回転
によってレーザ光の照射位置から外れて温度が低下し、
その温度が記録膜3のキューリー点まで降下したときに
、励磁素子6から与えた磁界により、その磁界の方向に
記録膜3の磁化方向を固定させ得る位置として励磁素子
6の一側軸端面6aを位置決めしである。一方、記録す
べき情報の信号を発生させる記録情報発生回路9の記録
信号を電流供給回路86入力しており、電流供給回路8
の出力但Bよ変調コイル7と接続されている。This excitation element 6 is formed, for example, in the shape of a rectangular parallelepiped,
The negative side shaft end surface 6a faces the magneto-optical disk 1. By energizing the modulation coil 7, the excitation element 6 can apply a perpendicular magnetic field to the information recording position of the magneto-optical disk 1 in a direction corresponding to the information to be recorded. That is, the information recording position of the magneto-optical disk 1 heated at the focused position of the laser beam moves away from the irradiation position of the laser beam due to the rotation of the magneto-optical disk 1, and the temperature decreases.
When the temperature drops to the Curie point of the recording film 3, the magnetic field applied from the excitation element 6 serves as a position where the magnetization direction of the recording film 3 can be fixed in the direction of the magnetic field. is positioned. On the other hand, a recording signal from a recording information generation circuit 9 that generates a signal of information to be recorded is inputted to a current supply circuit 86.
The output B is connected to the modulation coil 7.
この光磁気記録装置は、光磁気ディスクに記録すべき信
号を記録信号発生回路9で発生させて、その信号を電流
供給回路8へ入力すると、電流供給回路8は入力された
信号に相応する電流を変調コイル7へ供給する。それに
より励磁素子6は記録すべき信号に相応して変調磁界を
光磁気ディスク1へ与えることになる。そして光磁気デ
ィスク1の一面側にレーザ光5を投射し、他面側に前述
した変調磁界を与えることにより、記録すべき情報が光
磁気ディスク1へ記録される。In this magneto-optical recording device, when a signal to be recorded on a magneto-optical disk is generated by a recording signal generation circuit 9 and the signal is input to a current supply circuit 8, the current supply circuit 8 generates a current corresponding to the input signal. is supplied to the modulation coil 7. Thereby, the excitation element 6 applies a modulated magnetic field to the magneto-optical disk 1 in accordance with the signal to be recorded. Information to be recorded is recorded on the magneto-optical disk 1 by projecting the laser beam 5 onto one side of the magneto-optical disk 1 and applying the above-described modulated magnetic field to the other side.
前述した従来の光磁気記録装置は、励磁素子6に単一の
変調コイル7を備えている。この変調コイル7のインダ
クタンスは通常、数μHであり、この変調コイル7には
数MHz以上の高周波電流を流すことになるため、その
変調コイル7の励磁電力が大きく、またそれに流す励磁
電流の立上り時間が長いという問題がある。The conventional magneto-optical recording device described above includes a single modulation coil 7 in the excitation element 6. The inductance of this modulation coil 7 is usually several μH, and a high frequency current of several MHz or more is passed through this modulation coil 7. Therefore, the excitation power of the modulation coil 7 is large, and the rise of the excitation current that is passed through it is large. The problem is that it takes a long time.
本発明は斯かる問題に鑑み、励磁素子の励磁電力を低減
でき、しかも変調コイルの励磁電流の立上り時間が短い
光磁気記録装置を提供することを目的とする。In view of such problems, it is an object of the present invention to provide a magneto-optical recording device in which the excitation power of the excitation element can be reduced and the rise time of the excitation current of the modulation coil is short.
本発明に係る光磁気記録装置は、励磁素子に、変調コイ
ルを複数個設け、その各変調コイルに、各別の電流供給
回路を夫々接続する。In the magneto-optical recording device according to the present invention, the excitation element is provided with a plurality of modulation coils, and each of the modulation coils is connected to a separate current supply circuit.
複数の電流供給回路に共通に記録信号が入力される。夫
々の電流供給回路は夫々と対応する変調コイルに各別に
電流を供給する。各変調コイルは記録信号に相応する変
調磁界を発生する。各変調磁界の和の変調磁界が光磁気
ディスクへ与えられる。A recording signal is commonly input to the plurality of current supply circuits. Each current supply circuit separately supplies current to its corresponding modulation coil. Each modulation coil generates a modulation magnetic field corresponding to a recording signal. A modulated magnetic field that is the sum of each modulated magnetic field is applied to the magneto-optical disk.
これにより、単一の変調コイルで発生する磁界の強さを
、総和の巻回数が、単一の変調コイルの巻回数と等しい
複数の変調コイルで発生させる場合は、各変調コイルの
電流が低下し、よって励磁素子の励磁電力が低下する。As a result, if the strength of the magnetic field generated by a single modulation coil is generated by multiple modulation coils whose total number of turns is equal to the number of turns of the single modulation coil, the current in each modulation coil will decrease. Therefore, the excitation power of the excitation element decreases.
以下本発明をその実施例を示す図面により詳述する。第
1図は本発明に係る光磁気記録装置の要部を示す模式的
部分断面斜視図である。光磁気ディスク1の一面側には
レーザ光を出射する光ヘッド4が位置しており、そのレ
ーザ光5は光磁気ディスク1の基板2を透過して記録膜
3に合焦点を得るように投射されている。光磁気ディス
ク1の他面側には記録すべき情報の信号を入力する第1
゜第2の2つの変調コイル7A、 7Bを夫々備えてい
る磁性材からなる励磁素子6が位置している。これらの
変調コイル7A、 7Bは例えば同一巻回方向で同一巻
回数であり、また変調コイルを1個用いる場合のその巻
回数と同一巻回数に夫々選定しである。The present invention will be described in detail below with reference to drawings showing embodiments thereof. FIG. 1 is a schematic partial cross-sectional perspective view showing the main parts of a magneto-optical recording device according to the present invention. An optical head 4 that emits a laser beam is located on one side of the magneto-optical disk 1, and the laser beam 5 is transmitted through the substrate 2 of the magneto-optical disk 1 and projected onto the recording film 3 so as to obtain a focused point. has been done. On the other side of the magneto-optical disk 1, there is a first disk for inputting a signal of information to be recorded.
゜An excitation element 6 made of magnetic material is located which is provided with two second modulation coils 7A and 7B, respectively. These modulation coils 7A and 7B have, for example, the same winding direction and the same number of turns, and are each selected to have the same number of turns as the number of turns when one modulation coil is used.
この励磁素子6は、例えば直方体状に形成されていて、
その−側軸端面6aが光磁気ディスク1と対向している
。そして前記変調コイル7に通電することにより、励磁
素子6は光磁気ディスク1の情報記録位置に、記録すべ
き情報に応じた方向の垂直磁界を与え得るようになって
いる。即ちレーザ光の合焦点位置で加熱された光磁気デ
ィスク1の情報記録位置が、光磁気ディスクlの回転に
よってレーザ光の照射位置から外れて温度が低下し、そ
の温度が記録膜3のキューリー点まで降下したときに、
励磁素子6から与えた磁界により、その磁界の方向に記
録膜3の磁化方向を固定させ得る位置として励磁素子6
の一側軸端面6aを位置決めしである。一方、記録すべ
き情報の信号を発生させる記録情報発生回路9の記録信
号を第1の電流供給回路8A及び第2の電流供給回路8
Bへ入力しており、電流供給回路8A、 8Bの各出力
側は第1.第2の変調コイル7A、 7Bと接続されて
いる。This excitation element 6 is formed, for example, in the shape of a rectangular parallelepiped,
The negative side shaft end surface 6a faces the magneto-optical disk 1. By energizing the modulation coil 7, the excitation element 6 can apply a perpendicular magnetic field to the information recording position of the magneto-optical disk 1 in a direction corresponding to the information to be recorded. That is, the information recording position of the magneto-optical disk 1 heated at the focal point position of the laser beam moves away from the irradiation position of the laser beam due to the rotation of the magneto-optical disk l, and the temperature decreases, and the temperature reaches the Curie point of the recording film 3. When it descended to
The excitation element 6 is a position where the magnetization direction of the recording film 3 can be fixed in the direction of the magnetic field by the magnetic field applied from the excitation element 6.
This is for positioning the shaft end surface 6a on one side. On the other hand, the recording signal of the recording information generation circuit 9 that generates the signal of information to be recorded is transmitted to the first current supply circuit 8A and the second current supply circuit 8.
B, and each output side of the current supply circuits 8A and 8B is connected to the first.B. It is connected to second modulation coils 7A and 7B.
このように構成した本発明の光磁気記録装置は、光磁気
ディスク1に記録すべき信号を記録信号発生回路9で発
生させて、その信号を第1.第2の電流供給回路8A、
8Bへ入力すると、各電流供給回路8A、 8Bは入
力された信号に相応する電流を変調コイル7A、 7B
へ供給する。それにより、変調コイル7A、 7Bに通
電されて励磁素子6は記録すべき信号に相応して励磁さ
れ、各変調コイル7A、 7Bにより発生した変調磁界
が光磁気ディスク1へ与えられる。したがって、光磁気
ディスク1の一面側にレーザ光5を投射して、他面側に
前述した変調磁界を与えることにより、記録すべき情報
を光磁気ディスクlに記録する。In the magneto-optical recording device of the present invention configured as described above, the recording signal generating circuit 9 generates a signal to be recorded on the magneto-optical disk 1, and the signal is transmitted to the first . second current supply circuit 8A,
8B, each current supply circuit 8A, 8B modulates the current corresponding to the input signal to the modulating coil 7A, 7B.
supply to Thereby, the modulation coils 7A, 7B are energized, the excitation element 6 is excited in accordance with the signal to be recorded, and the modulated magnetic field generated by each modulation coil 7A, 7B is applied to the magneto-optical disk 1. Therefore, information to be recorded is recorded on the magneto-optical disk 1 by projecting the laser beam 5 onto one surface of the magneto-optical disk 1 and applying the above-described modulated magnetic field to the other surface.
ところで、夫々の変調コイル7Δ、 7Bによって発生
する変調磁界Hは夫々の変調コイルの電流に比例する。Incidentally, the modulating magnetic field H generated by each modulating coil 7Δ, 7B is proportional to the current of each modulating coil.
また変調コイルの電流の立上りelf/eatは、 θ t L 但し、■は変調コイルの電流 tは時間 ■は電流供給回路の出力電圧 りは変調コイルのインダクタンス で表わされる。Also, the rise of the current in the modulation coil elf/eat is θ t L However, ■ is the current of the modulation coil t is time ■ is the output voltage of the current supply circuit is the inductance of the modulation coil It is expressed as
それ故、単一の変調コイルにより発生させる磁界の強さ
を、変調コイル7A、 7Bで得るには、各変調コイル
7A、 7Bの夫々の電流は単一の変調コイルの電流の
2でよいことにより、その電流の立上り時間が短くなる
。Therefore, in order to obtain the strength of the magnetic field generated by a single modulation coil with the modulation coils 7A and 7B, the respective current of each modulation coil 7A and 7B should be twice the current of the single modulation coil. This shortens the rise time of the current.
また、変調コイル74.7Bの各励磁電力は、変調コイ
ルのインダクタンスと、それに流れる電流の2乗との積
であるから、個々の変調コイルの電流が例えばAになれ
ば各変調コイルの励磁電力はχとなり、2つの変調コイ
ル7A、 7Bの励磁電力は、Aを変調コイルの個数倍
した2となる。したがって、単一の変調コイルを用いた
場合と同じ磁界の強さを得る励磁電力は、変調コイルを
複数にした場合は、その個数分の−に低減できることに
なり、低電力で情報を記録し得る。Furthermore, since each excitation power of the modulation coil 74.7B is the product of the inductance of the modulation coil and the square of the current flowing through it, if the current of each modulation coil is, for example, A, the excitation power of each modulation coil is is χ, and the excitation power of the two modulation coils 7A and 7B is 2, which is A times the number of modulation coils. Therefore, when using multiple modulation coils, the excitation power required to obtain the same magnetic field strength as when using a single modulation coil can be reduced by the number of modulation coils, allowing information to be recorded with low power. obtain.
更に高密度記録ができて転送レートを上昇させることが
できる。Furthermore, high-density recording is possible and the transfer rate can be increased.
なお、本実施例では変調コイルを2個用いたが、それ以
上の数であってもよく、その個数が多くなるにともない
、励磁電力のより低電力化が図れることになるのは勿論
である。Although two modulation coils are used in this embodiment, it is possible to use a larger number of modulation coils, and it goes without saying that as the number of modulation coils increases, the excitation power can be further reduced. .
また本実施例では光ヘッド4と励磁素子6とが光磁気デ
ィスク1の異なる面側に別々に位置しているが、一方の
面側に光ヘッド4及び励磁素子6を位置させた構造であ
っても前述した効果と同様の効果が得られる。Further, in this embodiment, the optical head 4 and the excitation element 6 are located separately on different sides of the magneto-optical disk 1, but the structure is such that the optical head 4 and the excitation element 6 are located on one side. However, the same effect as described above can be obtained.
また、励磁素子6は直方体状(■型)としたが、これに
限らす略C字状、U字状、E字状等としてもよい。更に
変調コイル7A、 7Bの各巻回数を同一にせず、夫々
の変調コイルの電流を異ならせて、夫々の電流に関連し
て巻回数が異なる変調コイルを巻回した励磁素子6を用
いても同様の効果が得られるのは言うまでもない。更に
本実施例は光磁気記録装置としたが、光磁気記録再生装
置であっても同様の効果を得る。Furthermore, although the excitation element 6 is formed into a rectangular parallelepiped shape (■-shape), it may be substantially C-shaped, U-shaped, E-shaped, etc., but is not limited to this. Furthermore, the same effect can be achieved even if the number of turns of the modulation coils 7A and 7B is not made the same, but the current of each modulation coil is made different, and the excitation element 6 is wound with a modulation coil having a different number of turns in relation to each current. Needless to say, this effect can be obtained. Further, although this embodiment uses a magneto-optical recording device, similar effects can be obtained even if a magneto-optical recording/reproducing device is used.
以上詳述したように本発明の光磁気記録装置によれば、
記録すべき情報を低電力で、高精度に光磁気ディスクへ
記録することができる。また高密度記録が可能になり転
送レートを上昇させ得る等の優れた効果を奏する。As detailed above, according to the magneto-optical recording device of the present invention,
Information to be recorded can be recorded on a magneto-optical disk with low power and with high precision. Further, it has excellent effects such as enabling high-density recording and increasing the transfer rate.
第1図は本発明に係る光磁気記録装置の要部を示す模式
的部分断面斜視図、第2図は従来の光磁気記録装置の要
部を示す模式的部分断面斜視図である。
1・・・光磁気ディスク 3・・・記録膜 4・・・光
ヘッド 6・・・励磁素子 7^、7B・・・変調コイ
ル8A、8B・・・電流供給回路 9・・・記録信号発
生回路なお、図中、同一符号は同一、又は相当部分を示
す。FIG. 1 is a schematic partial cross-sectional perspective view showing the main parts of a magneto-optical recording apparatus according to the present invention, and FIG. 2 is a schematic partial cross-sectional perspective view showing the main parts of a conventional magneto-optical recording apparatus. 1... Magneto-optical disk 3... Recording film 4... Optical head 6... Excitation element 7^, 7B... Modulation coils 8A, 8B... Current supply circuit 9... Recording signal generation Circuit Note that in the figures, the same reference numerals indicate the same or equivalent parts.
Claims (1)
ルを備えている励磁素子を設けている光磁気記録装置に
おいて、 前記変調コイルを複数個設けており、該各 変調コイルに各別の電流供給回路を夫々接続しているこ
とを特徴とする光磁気記録装置。[Claims] 1. In a magneto-optical recording device provided with an excitation element having a modulation coil in order to apply an external magnetic field to a magneto-optical disk, a plurality of the modulation coils are provided, and each modulation coil 1. A magneto-optical recording device characterized in that a separate current supply circuit is connected to each.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28443488A JPH02130701A (en) | 1988-11-09 | 1988-11-09 | Magneto-optical recording device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28443488A JPH02130701A (en) | 1988-11-09 | 1988-11-09 | Magneto-optical recording device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02130701A true JPH02130701A (en) | 1990-05-18 |
Family
ID=17678501
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP28443488A Pending JPH02130701A (en) | 1988-11-09 | 1988-11-09 | Magneto-optical recording device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02130701A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH04103322U (en) * | 1991-01-28 | 1992-09-07 | テイアツク株式会社 | magnetic head device |
JP2006242332A (en) * | 2005-03-04 | 2006-09-14 | Kanefusa Corp | Power transmission mechanism |
-
1988
- 1988-11-09 JP JP28443488A patent/JPH02130701A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH04103322U (en) * | 1991-01-28 | 1992-09-07 | テイアツク株式会社 | magnetic head device |
JP2006242332A (en) * | 2005-03-04 | 2006-09-14 | Kanefusa Corp | Power transmission mechanism |
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