JPS61229247A - Photomagnetic medium - Google Patents
Photomagnetic mediumInfo
- Publication number
- JPS61229247A JPS61229247A JP6981485A JP6981485A JPS61229247A JP S61229247 A JPS61229247 A JP S61229247A JP 6981485 A JP6981485 A JP 6981485A JP 6981485 A JP6981485 A JP 6981485A JP S61229247 A JPS61229247 A JP S61229247A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- track
- recording
- external magnetic
- recording track
- 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
Abstract
Description
【発明の詳細な説明】
(発明の背景)
光磁気媒体への信号の書き込みには光変調方式と磁気変
調方式とが知られているが、前者はデータの高周波信号
の記録(高速データレート)が可能であるが重ね書きが
出来ない為書き込みと消去の切り換えに時間が掛かる事
及び記録済みの媒体を消去するのに書き込み時間と同時
間必要で時間が掛かると言う欠点があった。[Detailed Description of the Invention] (Background of the Invention) Optical modulation methods and magnetic modulation methods are known for writing signals on magneto-optical media, and the former method is used to record high-frequency signals of data (high-speed data rate). However, since overwriting is not possible, it takes time to switch between writing and erasing, and erasing a recorded medium requires the same amount of time as the writing time, so it takes time.
一方後者は重ね書きが可能であるが垂直磁化膜と電磁コ
イルとは構造上2IIIIl1以上離れるので媒体の必
要とする磁界を得る為には電磁コイルの巻回数を増すか
大電流を流す事になり、これは過渡応答性を劣化させ、
所定の磁界を得る為に要する時間を長くすることとなり
、記録周波数の上限を引き下げる事となり、又装置の大
型化を招(事となる。On the other hand, the latter allows overwriting, but the perpendicular magnetization film and the electromagnetic coil are structurally separated by more than 2III11, so in order to obtain the magnetic field required by the medium, the number of turns of the electromagnetic coil must be increased or a large current must be passed. , this degrades the transient response,
This increases the time required to obtain a predetermined magnetic field, lowers the upper limit of the recording frequency, and increases the size of the device.
(発明の目的)
本発明はこれらの欠点を解決し、光磁気媒体に於いて高
周波信号の記録が可能で且つ重ね書きを可能とする事を
目的とする。(Objective of the Invention) An object of the present invention is to solve these drawbacks and to make it possible to record high-frequency signals on a magneto-optical medium and to enable overwriting.
(発明の概要)
本発明は光磁気媒体の記録トラックの両脇にそれぞれ方
向のことなる磁化方向の外部磁界発生用トラックを予め
設け、記録に当たって該両外部磁界発生用トラックのい
ずれかの磁界を選択的に使用する事を技術的要点として
いる。(Summary of the Invention) The present invention provides external magnetic field generating tracks with different magnetization directions on both sides of a recording track of a magneto-optical medium, and when recording, the magnetic field of either of the external magnetic field generating tracks is applied. The technical point is to use it selectively.
(実施例)
第1図は本発明の実施例であり、(a)は同心円状の記
録トラックを有する溝付円板状の光磁気ディスク(以下
単に光磁気ディスクと称する)の一部平面図、(b)は
本発明による光磁気ディスクの一部断面図で、第1図の
A−A矢視断面図である。(Embodiment) FIG. 1 shows an embodiment of the present invention, and (a) is a partial plan view of a grooved disk-shaped magneto-optical disk (hereinafter simply referred to as magneto-optical disk) having concentric recording tracks. , (b) are partial cross-sectional views of the magneto-optical disk according to the present invention, which are cross-sectional views taken along the line A--A in FIG.
第1図(a) 、 (b)に於いて、1,2.3はレー
ザ出力の光磁気媒体の記録面への照射スポットで1は円
形レーザスポット、2.3は楕円レーザスポットであり
、これらは3個の半導体レーザと1つの対物レンズによ
って得られる。4は同心円状の記録トラックを設定する
為の同心円状の溝が予め設けられたディスク基板でイン
ジェクシヨン、キャスティング等によって製造される。In FIGS. 1(a) and (b), 1, 2.3 are spots irradiated with the laser output onto the recording surface of the magneto-optical medium, 1 is a circular laser spot, 2.3 is an elliptical laser spot, These are obtained by three semiconductor lasers and one objective lens. Reference numeral 4 denotes a disk substrate in which concentric grooves for setting concentric recording tracks are provided in advance, and is manufactured by injection, casting, or the like.
該ディスク基板4の溝を設けた面には飽和磁化の大きい
TbFe等の垂直磁化膜5〜9が形成される。Perpendicular magnetization films 5 to 9 made of TbFe or the like having high saturation magnetization are formed on the surface of the disk substrate 4 on which the grooves are provided.
垂直磁化膜5.6は記録トラック、?、8.9は外部磁
界発生用トラックで、該外部磁界発生用トラック?、8
.9.・−・−−−一−−は順次磁化方向が反転する様
に信号記録に先立って予め磁化しておく。The perpendicular magnetization film 5.6 is a recording track, ? , 8.9 is a track for generating an external magnetic field, and the track for generating an external magnetic field? , 8
.. 9.・−・−−−1−− is magnetized in advance prior to signal recording so that the magnetization direction is sequentially reversed.
第1図では外部磁界発生用トラック7.9は上向き、8
は下向きに磁化している。In FIG. 1, the track 7.9 for generating an external magnetic field is directed upward, and
is magnetized downward.
この信号記録に先立って予め磁化する予備磁化は先ず光
磁気媒体全体を強力な上向き外部磁界内に置いて垂直磁
化膜5〜9を全て上向きに磁化する。In pre-magnetization, which is carried out in advance before signal recording, the entire magneto-optical medium is first placed in a strong upward external magnetic field to magnetize all the perpendicularly magnetized films 5 to 9 upward.
次に弱い下向き外部磁界と直流点灯のレーザスポットに
より外部磁界発生用トラックを1つおきに下向きに磁化
する。Next, every other external magnetic field generation track is magnetized downward using a weak downward external magnetic field and a laser spot lit with direct current.
第1図(b)中矢印は垂直磁化膜の磁化方向を現わす。The arrow in FIG. 1(b) indicates the magnetization direction of the perpendicularly magnetized film.
この様にして出来た本発明の光磁気媒体の信号記録及び
重ね書きにつき以下説明する。Signal recording and overwriting on the magneto-optical medium of the present invention produced in this manner will be explained below.
ここでは上向き磁化を1”、下向き磁化をO”とする。Here, upward magnetization is assumed to be 1'', and downward magnetization is assumed to be O''.
第2図、第3図は本発明の光磁気媒体の信号記録及び重
ね書きの原理を説明する為の部分断面図であり、第2図
は1”の記録の時の原理説明用、第3図は0”の記録の
時の原理説明用である。2 and 3 are partial sectional views for explaining the principle of signal recording and overwriting of the magneto-optical medium of the present invention. The figure is for explaining the principle when recording 0''.
(イ)■”の記録
第2図に於いて、円形レーザスポット1はレーザを直流
点灯し、記録トラックをキュリ一温度以上に加熱しなが
らトレースする。(a) Recording of "■" In FIG. 2, the circular laser spot 1 is traced by lighting the laser with direct current and heating the recording track to a temperature above one Curie.
一方楕円レーザスポット3は111”の記録に際して上
向き磁界の記録された外部磁界発生用トラック7に照射
されて該照射部分がキュリ一温度付近まで上昇し、飽和
磁化は減少する。すると前記円形レーザスポット1の照
射された部分は下向き磁界の記録された外部磁界発生用
トラック8の浮遊磁界13が支配的となり、キュリ一温
度以上に加熱された記録トラック5の円形レーザスボッ
)1が照射された部分は上向きに磁化される。On the other hand, when recording 111'', the elliptical laser spot 3 is irradiated onto the external magnetic field generation track 7 on which the upward magnetic field has been recorded, and the irradiated portion rises to around the Curie temperature, and the saturation magnetization decreases.Then, the circular laser spot 3 The floating magnetic field 13 of the external magnetic field generating track 8 on which the downward magnetic field was recorded is dominant in the irradiated part of 1, and the circular laser beam 1 of the recording track 5 heated to above Curie temperature is irradiated with Magnetized upward.
即ち1”が記録された事になる。In other words, 1" is recorded.
(ロ)O”の記録
笛9ml?y妨2八プ 田μ!、 −−upηギー、L
lす+し−ザを直流点灯し、記録トラックをキュリ一温
度以上に加熱しながらトレースする。(b) O” record whistle 9ml?
The laser is turned on with direct current, and the recording track is traced while being heated to a temperature above one Curtain temperature.
一方楕円レーザスポット2は0”の記録に際して下向き
磁界の記録された外部磁界発生用トラック8に照射され
て該照射部分がキュリ一温度付近まで上昇し、飽和磁化
は減少する。すると前記円形レーザスポット1の照射さ
れた部分は上向き磁界の記録された外部磁界発生用トラ
ック7の浮遊磁界15が支配的となり、キュリ一温度以
上に加熱された記録トラック5の円形レーザスポット1
が照射された部分は下向きに磁化される。On the other hand, when recording 0'', the elliptical laser spot 2 is irradiated onto the external magnetic field generation track 8 on which the downward magnetic field has been recorded, and the irradiated portion rises to around the Curie temperature, and the saturation magnetization decreases.Then, the circular laser spot 2 The irradiated portion of 1 is dominated by the floating magnetic field 15 of the external magnetic field generating track 7 in which an upward magnetic field is recorded, and the circular laser spot 1 of the recording track 5 is heated to a temperature of one Curie or higher.
The irradiated part is magnetized downward.
即ち10″が記録された事になる。In other words, 10'' has been recorded.
以上の説明の様に記録トラック5の両脇に設けられた外
部磁界発生用トラック7.8へ照射される楕円スポット
を選択的に照射する事によって記録トラックへ2値信号
が記録可能である。As described above, a binary signal can be recorded on the recording track by selectively irradiating the elliptical spot onto the external magnetic field generating tracks 7.8 provided on both sides of the recording track 5.
ここで楕円スポットを選択的に照射する制御は高速で行
える事から高周波信号の記録が可能であり、高速データ
レートが可能となり、又外部磁界発生用トラックと記録
トラックとは隣接して設けられる事から外部磁界発生用
トラックの浮遊磁界が記録トラックへ影響する磁界は強
力である為記録トラックの信号にかかわりなく磁化され
る事になり、即ち重ね書きが可能となる。Here, the selective irradiation of the elliptical spot can be controlled at high speed, making it possible to record high-frequency signals and high-speed data rates.Also, the external magnetic field generation track and the recording track can be placed adjacent to each other. Since the magnetic field exerted by the floating magnetic field of the external magnetic field generation track on the recording track is strong, the recording track is magnetized regardless of the signal on the recording track, that is, overwriting is possible.
尚、記録トラック6への信号記録では両脇に設けられた
外部磁界発生用トラックの磁化方向が記録トラック5と
逆になるが、これは例えば■アクセスに使用する為に記
録トラックに付された連続番号であるアドレス番号を記
録時に読取り、奇偶を判別して楕円スポット2.3の点
灯制御を切り換えて記録トラックへの書き込み信号の磁
界の方向と0,1 との対応を記録トラックによらず
一定とする。In addition, when recording a signal on the recording track 6, the magnetization direction of the external magnetic field generating tracks provided on both sides is opposite to that of the recording track 5, but this is because, for example, The address number, which is a continuous number, is read during recording, and it is determined whether it is odd or even, and the lighting control of the elliptical spot 2.3 is switched to determine the correspondence between 0 and 1 and the direction of the magnetic field of the write signal to the recording track, regardless of the recording track. It is assumed to be constant.
■アドレス番号を再生時に読取り、奇偶を判別して再生
信号の極性を切り換える。■Read the address number during playback, determine whether it is odd or even, and switch the polarity of the playback signal.
■記録トラックに予め楕円スポット2.3と110“、
11″との対応即ち両脇の外部磁界発生トラックの磁化
方向を書き込んでおき、記録時この情報を読取り、記録
トラックへの書き込み信号の磁界の方向と110”、1
1″との対応を記録トラックによらず一定とする。■Oval spots 2.3 and 110" are placed on the recording track in advance.
11'', that is, the magnetization direction of the external magnetic field generating tracks on both sides, is written in advance, and this information is read during recording, and the direction of the magnetic field of the write signal to the recording track and 110'', 1 are written.
1'' is constant regardless of the recording track.
■記録トラックに予め楕円スポット2.3と0″、1”
との対応即ち両脇の外部磁界発生トラックの磁化方向を
書き込んでおき、記録時には使わずに再生時この情報を
読取り、再生信号の極性を切り換える。■Oval spots 2.3, 0″, 1″ on the recording track in advance
That is, the magnetization directions of the external magnetic field generation tracks on both sides are written in advance, and this information is not used during recording but is read during reproduction to switch the polarity of the reproduced signal.
等の方法によって解決出来る。This can be solved by methods such as
ここで上述の実施例では同心円状トラックについて説明
したが渦巻状のトラックにも適用可能で、その場合は第
5図に示す如(外部磁界発生トラックの磁化方向を、1
周毎に異ならせる様にすれば良い、第5図において7
(点線にて表示)は上向き、8 (一点FA線にて表示
)は下向きの磁界がそれぞれ予め書き込まれた外部磁界
発生トラックである。In the above embodiment, concentric tracks were explained, but it is also applicable to spiral tracks. In that case, as shown in FIG.
7 in Figure 5.
8 (indicated by a dotted line) indicates an upward magnetic field, and 8 (indicated by a dotted FA line) indicates an external magnetic field generation track in which a downward magnetic field is written in advance.
又、媒体の外形も円板状に限定されず、例えばカード状
の媒体を往復駆動する様にしても良い。Further, the outer shape of the medium is not limited to a disk shape, and for example, a card-shaped medium may be driven back and forth.
又本実施例では、外部磁界発生トラックへのレーザビー
ムを楕円としたがこれに限られる事は無い。Further, in this embodiment, the laser beam directed to the external magnetic field generating track is elliptical, but the laser beam is not limited to this.
又本実施例では2値記録について説明したが多値記録も
以下に説明する如く可能である。Furthermore, although binary recording has been described in this embodiment, multi-value recording is also possible as explained below.
更に実施例では凹凸を設けてトラックの区分をしたもの
を示したが、例えば信号トラックのビット列でトラッキ
ングの可能な3ビーム法を用いれば必ずしも凹凸トラッ
クは必要では無い。Further, in the embodiment, tracks are divided by providing unevenness, but if a three-beam method is used, which allows tracking of the bit string of a signal track, for example, the uneven track is not necessarily necessary.
第4図は本発明の光磁気ディスクの一部断面図で第1.
2.3図と同符号は同効部材である。FIG. 4 is a partial sectional view of the magneto-optical disk of the present invention.
The same symbols as in Figure 2.3 indicate the same effective members.
第4図の様に楕円レーザスポットを照射せずに円形レー
ザスポット1を記録外ラック5に照射すると記録トラッ
ク5の左右がそれぞれ異なる磁化方向に磁化され、上記
のO”と1”と1士”の3値が記録可能となる。As shown in Fig. 4, when the circular laser spot 1 is irradiated onto the non-recording rack 5 without irradiating the elliptical laser spot, the left and right sides of the recording track 5 are magnetized in different magnetization directions. ” can be recorded.
又、外部磁界発生トラック7.8へ照射するレーザビー
ムのパワーを制御して媒体の温度を制御する事により、
記録トラックでの上下方向の磁化面積を制御して多値の
記録が可能となる。In addition, by controlling the power of the laser beam irradiated to the external magnetic field generating track 7.8 and controlling the temperature of the medium,
Multi-level recording is possible by controlling the magnetized area in the vertical direction on the recording track.
(発明の効果)
以上の様に本発明によれば2つのレーザビームの照射を
コントロールして浮遊磁界の向きを高速で制御して高速
磁場変調が行える為光磁気媒体に高周波信号の重ね書き
が可能となる。(Effects of the Invention) As described above, according to the present invention, high-speed magnetic field modulation can be performed by controlling the irradiation of two laser beams and controlling the direction of the floating magnetic field at high speed, so that high-frequency signals can be overwritten on the magneto-optical medium. It becomes possible.
更に2つのレーザビームの照射をコントロールす
−る事によって多値記録も可能となる。Furthermore, the irradiation of two laser beams is controlled.
- multivalue recording is also possible.
第1図は本発明による光磁気ディスクの説明図、第2図
、第3図は本発明による光磁気ディスクの記録原理を示
す説明図、第4図は多値記録の場合の記録原理を示す説
明図、第5図は渦巻状トラックの場合の実施例図である
。
(主要部分の符号の説明)
1.2.3−・・−・−レーザビーム
4・−・−・−・・−・−・・・−・・ディスク基板5
.6−−−−−・−・−・−−一−−−記録トラック?
、8.9・−・・−・−外部磁界発生トラック第1図
(Illl)
(b)
第2図
第3図
第4図
第5図
手続補正書(自発
昭和60年 5月10日
秒表示
昭和60年噂犠第69814号
東京都千代田区丸の内3丁目2番3号
(411)日本光学工業株式会社
4、代理人
@140東京部品川区西大井1丁目6番3号王の対象
図面G4面FIG. 1 is an explanatory diagram of a magneto-optical disk according to the present invention, FIGS. 2 and 3 are explanatory diagrams showing the recording principle of the magneto-optical disk according to the present invention, and FIG. 4 is a diagram showing the recording principle in the case of multilevel recording. The explanatory diagram, FIG. 5, is an example diagram in the case of a spiral track. (Explanation of symbols of main parts) 1.2.3-...--Laser beam 4---------------Disc substrate 5
.. 6-------・------1-- Recording track?
, 8.9...--External magnetic field generation track Figure 1 (Illll) (b) Figure 2 Figure 3 Figure 4 Figure 5 Procedural amendment (self-initiated May 10, 1985, second display) 1985 Rumored Sacrifice No. 69814 3-2-3 Marunouchi, Chiyoda-ku, Tokyo (411) Nippon Kogaku Kogyo Co., Ltd. 4, Agent @ 140 1-6-3 Nishi-Oi, Honbunagawa-ku, Tokyo King's target drawing G4
Claims (4)
磁界を予め記録した外部磁界発生用トラックを設けた事
を特徴とする光磁気媒体。(1) A magneto-optical medium characterized in that an external magnetic field generating track is provided on both sides of a recording track, on which perpendicular magnetic fields in different directions are recorded in advance.
囲第1項記載の光磁気媒体。(2) The magneto-optical medium according to claim 1, which has a disk-like outer shape.
同心円状で交互に設けられ、該外部磁界発生用トラック
は交互に上向きと下向きの垂直磁界を予め記録した事を
特徴とする特許請求の範囲第2項記載の光磁気媒体。(3) The recording track and the external magnetic field generating track are arranged concentrically and alternately, and the external magnetic field generating track is prerecorded with an upward and downward vertical magnetic field alternately. 2. The magneto-optical medium according to item 2.
渦巻状であり、外部磁界発生用トラックは記録トラック
の一方の側に設け、一周毎交互に上向きと下向きの垂直
磁界を予め記録した事を特徴とする特許請求の範囲第2
項記載の光磁気媒体。(4) The recording track and the external magnetic field generating track are spiral-shaped, and the external magnetic field generating track is provided on one side of the recording track, and an upward and downward vertical magnetic field is recorded in advance alternately every round. Claim No. 2
Magneto-optical medium as described in Section 1.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6981485A JPS61229247A (en) | 1985-04-02 | 1985-04-02 | Photomagnetic medium |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6981485A JPS61229247A (en) | 1985-04-02 | 1985-04-02 | Photomagnetic medium |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61229247A true JPS61229247A (en) | 1986-10-13 |
Family
ID=13413603
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP6981485A Pending JPS61229247A (en) | 1985-04-02 | 1985-04-02 | Photomagnetic medium |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61229247A (en) |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS62110638A (en) * | 1985-11-08 | 1987-05-21 | Matsushita Electric Ind Co Ltd | Optical recording medium |
JPS63166050A (en) * | 1986-12-27 | 1988-07-09 | Hitachi Maxell Ltd | Magneto-optical recording medium |
US4789972A (en) * | 1986-12-22 | 1988-12-06 | International Business Machines Corporation | Selectively controlling the erasure in a magneto-optic recording medium |
JPH0237544A (en) * | 1988-07-28 | 1990-02-07 | Toshiba Corp | Magneto-optical recording medium |
US5309415A (en) * | 1989-08-01 | 1994-05-03 | Mitsubishi Denki Kabushiki Kaisha | Information recording method for overwriting a magneto-optic recording medium with two intensities of light beams |
-
1985
- 1985-04-02 JP JP6981485A patent/JPS61229247A/en active Pending
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS62110638A (en) * | 1985-11-08 | 1987-05-21 | Matsushita Electric Ind Co Ltd | Optical recording medium |
US4789972A (en) * | 1986-12-22 | 1988-12-06 | International Business Machines Corporation | Selectively controlling the erasure in a magneto-optic recording medium |
JPS63166050A (en) * | 1986-12-27 | 1988-07-09 | Hitachi Maxell Ltd | Magneto-optical recording medium |
JPH0237544A (en) * | 1988-07-28 | 1990-02-07 | Toshiba Corp | Magneto-optical recording medium |
US5309415A (en) * | 1989-08-01 | 1994-05-03 | Mitsubishi Denki Kabushiki Kaisha | Information recording method for overwriting a magneto-optic recording medium with two intensities of light beams |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
KR910003935B1 (en) | Magneto-opticla recording system | |
US4495530A (en) | Method of processing information signal with respect to opto-magnetic record medium | |
US6069852A (en) | Magneto-optical recording-reproducing method for recording an asymmetrical magnetic domain on a magneto-optical recording medium | |
JPH0721894B2 (en) | Magneto-optical recording method | |
JPS61229247A (en) | Photomagnetic medium | |
US5357493A (en) | Magneto-optic memory device for overwriting information on magneto-optic recording medium by using a pair of light spots without using an external magnetic field | |
EP0241222B1 (en) | Opto-magnetic recording apparatus for sequentially driving optical head drive means and biasing magnetic field generation means | |
EP0328667B1 (en) | Magneto-optical storage | |
JPH03242841A (en) | Magneto-optical disk | |
JPH0721893B2 (en) | Magneto-optical recording method | |
JPS6265202A (en) | Auxiliary magnetic field impressing device | |
US7277363B1 (en) | Magneto-optical recording or reproducing device | |
JP2714085B2 (en) | Information recording method | |
JP2604702B2 (en) | Magneto-optical recording / reproduction / erasing method and apparatus | |
JPS6234333A (en) | Optical information recording and reproducing device | |
JP2749877B2 (en) | Information recording device | |
JP2855918B2 (en) | Optical information recording method and device | |
JPS62208445A (en) | Photomagnetic recording method | |
JPS62208444A (en) | Photomagnetic recording method | |
JPS59140605A (en) | Erasing system of photomagnetic recorder | |
JPH04105236A (en) | Magnetic recording, erasing, and reading system | |
JPS63225931A (en) | Reloadable optical disk device | |
JPH01107349A (en) | Magneto-optical recording medium | |
JPS63311646A (en) | Method for recording magneto-optical recording medium | |
JPS6150235A (en) | System and apparatus for erasing and reproducing optomagnetic recording |