JPH0222451B2 - - Google Patents

Info

Publication number
JPH0222451B2
JPH0222451B2 JP57150430A JP15043082A JPH0222451B2 JP H0222451 B2 JPH0222451 B2 JP H0222451B2 JP 57150430 A JP57150430 A JP 57150430A JP 15043082 A JP15043082 A JP 15043082A JP H0222451 B2 JPH0222451 B2 JP H0222451B2
Authority
JP
Japan
Prior art keywords
recording
optical recording
laser beam
optical
reproducing
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.)
Expired - Lifetime
Application number
JP57150430A
Other languages
Japanese (ja)
Other versions
JPS5940325A (en
Inventor
Nobuhiko Sakai
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.)
Dai Nippon Printing Co Ltd
Original Assignee
Dai Nippon Printing Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Dai Nippon Printing Co Ltd filed Critical Dai Nippon Printing Co Ltd
Priority to JP15043082A priority Critical patent/JPS5940325A/en
Publication of JPS5940325A publication Critical patent/JPS5940325A/en
Publication of JPH0222451B2 publication Critical patent/JPH0222451B2/ja
Granted legal-status Critical Current

Links

Classifications

    • G—PHYSICS
    • G11—INFORMATION STORAGE
    • G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor

Landscapes

  • Mechanical Optical Scanning Systems (AREA)
  • Optical Recording Or Reproduction (AREA)

Description

【発明の詳細な説明】 本発明は光学記録材料の記録位置精度のばらつ
きをレーザー光の走査方式により補なう光学記録
再生方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical recording and reproducing method that compensates for variations in recording position accuracy of optical recording materials using a laser beam scanning method.

光学記録材料の光学記録層の一部をレーザー光
の照射により揮散、変形若しくは反射率を変化さ
せ、これらの結果、光の反射率や透過率の差によ
る記録を行ない、或いはこのようにして得られる
記録済の光学記録材料の光学記録層にレーザー光
を照射して情報を再生する光学記録再生方法自体
は既に知られている。光学記録再生方法は非接触
で情報の再生が出来、しかも記録密度が他の記録
再生方法にくらべて高い利点を有している。しか
しながら光学記録再生方法においては情報はせい
ぜい1μ巾程度のトラツクに収まるため、情報の
記録位置を正確に検出し、トラツクから外れない
ように走査して再生する必要がある。代表的な光
学記録材料として光デイスクが知られているが、
光デイスクにおいては情報はレコードの音溝のよ
うにらせん状若しくは同心円状に記録されてお
り、このため中心の位置精度が或る程度維持され
ていれば光デイスクの周辺部から中心部に向かつ
てほぼ直線状に走査を行なえばトラツクの検出、
及び追随は比較的容易に行なえ光デイスクの駆動
の偏りは周期的であつて対応が可能である。この
ような光デイスクは記録容量が大きく、ランダム
アクセスも可能なため画像、オーデイオ、電子計
算機の記憶媒体の分野に利用されている。一方、
光学記録再生方法は記録密度が高いため、小型の
携帯可能な記録媒体としても利用可能であり、例
えば、現在、磁気カード、情報カード、商品タ
グ、英合話カード等の磁気方式が利用されている
分野に利用すると同じ大きさの記録媒体により多
くの情報を記録再生することが可能である。しか
し、これらの記録媒体を商業的に利用する際には
記録媒体の寸法精度、記録位置の精度に加えて記
録媒体の走行精度のばらつきがあり、又、これら
の記録媒体における記録は直線状になされている
ため記録部分の検出及び追随には精密な走行のた
めの駆動装置を要し、しかも駆動の偏りはランダ
ムであり、光デイスクにくらべると特に再生上の
困難さを有している。例えば磁気カードを光学記
録再生方式のカードに置き換えたものを例にとる
とその寸法精度は±50μ〜±100μ程度であり、レ
ーザービームの径が1μ程度であることを考慮す
ると再生時には記録部の検出とその追随のための
手段を講じなければならない。記録部の検出と追
随のため、光学記録による線や、機械的加工によ
る溝を予め案内用に設けておき、光学的、機械的
にこれらの案内用の線や溝を検出して追随する一
方、本来の情報記録はこれらの線や溝と平行なあ
る間隔を保つた位置に行なつておき、再生を容易
に行なおうとする試みが提案されている。しかし
このように案内用の溝や線を設ける事及びこれら
の検出のための手段が記録再生の手段以外に必要
であり煩雑さが避けられないものである。
A part of the optical recording layer of an optical recording material is volatilized, deformed, or has its reflectance changed by irradiation with a laser beam, and as a result, recording is performed based on the difference in light reflectance or transmittance, or the recording obtained in this way is performed. The optical recording and reproducing method itself is already known in which information is reproduced by irradiating the optical recording layer of a recorded optical recording material with a laser beam. Optical recording and reproducing methods can reproduce information without contact, and have the advantage of higher recording density than other recording and reproducing methods. However, in the optical recording and reproducing method, since information is contained within a track of about 1 micron width at most, it is necessary to accurately detect the recording position of the information and to scan and reproduce the information without deviating from the track. Optical disks are known as a typical optical recording material, but
On optical discs, information is recorded in a spiral or concentric pattern like the sound grooves of a record, and therefore, if the positional accuracy of the center is maintained to a certain degree, information can be recorded from the periphery to the center of the optical disc. Tracks can be detected by scanning almost in a straight line.
Tracking is relatively easy, and deviations in the drive of the optical disk are periodic and can be dealt with. Such optical disks have a large storage capacity and can be accessed randomly, so they are used in the fields of image, audio, and computer storage media. on the other hand,
Since the optical recording and reproducing method has a high recording density, it can also be used as a small and portable recording medium.For example, magnetic methods are currently used for magnetic cards, information cards, product tags, English cards, etc. When used in various fields, it is possible to record and reproduce more information on a recording medium of the same size. However, when these recording media are used commercially, there are variations in the dimensional accuracy of the recording media, the accuracy of the recording position, and the running accuracy of the recording media, and the recording on these recording media is not linear. Because of this, a drive device for precise movement is required to detect and follow the recorded portion, and the drive bias is random, making playback particularly difficult compared to optical disks. For example, when a magnetic card is replaced with an optical recording/playback type card, the dimensional accuracy is about ±50μ to ±100μ, and considering that the diameter of the laser beam is about 1μ, the recording part is Measures must be taken for detection and follow-up. In order to detect and follow the recording section, optical recording lines and mechanically processed grooves are prepared in advance for guidance, and these guiding lines and grooves are detected and followed optically and mechanically. An attempt has been made to record the original information at a position parallel to these lines and grooves, keeping a certain distance therebetween, and to facilitate reproduction. However, provision of such guide grooves and lines and means for detecting these are necessary in addition to recording and reproducing means, and complexity is unavoidable.

本発明者は上記の従来技術における欠点を解消
するため種々研究の結果、上記のような直線状に
情報を記録する記録媒体においては、その直線方
向の記録密度が高いことが要求されるが、反面、
巾方向の記録密度は比較的問題にならないことが
多く、このため、巾方向に拡大して記録を行なえ
ば、直線方向の記録密度、ひいては記録媒体自体
の記録密度は低下せず、却つて再生時の走行精度
のばらつきを吸収しうることを見い出し、しかも
このように記録されている記録媒体を再生する際
のレーザー光をその走査方向に直角に振動させる
ことにより情報の再生が容易になることも見い出
して本発明に到達したものである。
The inventor of the present invention has conducted various studies in order to eliminate the drawbacks of the above-mentioned conventional techniques, and has found that the above-mentioned recording medium that records information in a straight line is required to have a high recording density in the straight direction. On the other hand,
The recording density in the width direction is often relatively unproblematic, so if you expand the recording in the width direction, the recording density in the linear direction, and by extension the recording density of the recording medium itself, will not decrease, and on the contrary, playback will be affected. They discovered that it is possible to absorb variations in the running accuracy of time, and that information can be easily reproduced by vibrating the laser beam perpendicular to the scanning direction when reproducing a recording medium on which information is recorded in this way. The present invention was also achieved by discovering the following.

即ち、本発明は光学記録材料の光学記録層にレ
ーザー光を集光して走査することにより記録再生
を行なう光学記録再生方法において、レーザー光
を記録時には走査方向に対して直角方向に振動さ
せることにより記録巾を拡大させつつピツトを形
成し、更に再生時にも走査方向に対して直角方向
に振動させつつ走査することを特徴とする光学記
録再生方法をその要旨とするものである。
That is, the present invention provides an optical recording and reproducing method in which recording and reproducing is performed by focusing and scanning a laser beam on an optical recording layer of an optical recording material, in which the laser beam is vibrated in a direction perpendicular to the scanning direction during recording. The gist of this optical recording and reproducing method is to form pits while enlarging the recording width, and to scan while vibrating in a direction perpendicular to the scanning direction during reproduction.

以下、本発明について詳細に説明を行なう。 The present invention will be explained in detail below.

本発明において用いる光学記録材料としては光
学記録層の一部がレーザー光の照射により光の反
射率や透過率の差を生じるものであればいずれも
使用可能である。これらの光学記録材料は例えば
平滑で耐熱性のある基材上に光学記録層として
Te、Bi、Sn、In等の低融点金属を薄膜状に設け
たものや、或いは異種の金属を2層積層したもの
を挙げることができる。
As the optical recording material used in the present invention, any material can be used as long as a portion of the optical recording layer produces a difference in light reflectance or transmittance when irradiated with laser light. These optical recording materials can be used, for example, as an optical recording layer on a smooth, heat-resistant substrate.
Examples include those in which low melting point metals such as Te, Bi, Sn, and In are provided in the form of a thin film, and those in which two different types of metals are laminated.

これらの光学記録材料に記録を行なうには通常
の方法を利用し、更に部分的に改変して行なう。
例えば第1図に示すごとくレーザー光源1より出
射されたレーザー光を固定ミラー2により反射さ
せ集光レンズ3を用いて集光させ光学記録材料4
上に照射すると通常の記録が行なえ、第2図に示
すごとくレーザー光源5を用い固定ミラー6で反
射させた後、集光レンズ7を用いて光学記録材料
の表面を照射し、得られる反射光を1/4波長板8
を通し更に偏光ビームスプリツター9によりフオ
トダイオード10に導入して読み取りが行なえ
る。
Recording on these optical recording materials is carried out using conventional methods with some further modifications.
For example, as shown in FIG. 1, a laser beam emitted from a laser light source 1 is reflected by a fixed mirror 2 and condensed by a condenser lens 3 to form an optical recording material 4.
Ordinary recording can be performed by irradiating the light onto the surface of the optical recording material.As shown in FIG. 1/4 wavelength plate 8
The light can then be introduced into a photodiode 10 by a polarizing beam splitter 9 for reading.

上記の記録方法において、本発明においては特
にレーザー光と光学記録材料とを相対的に直線的
に移動させつつ直線状に記録を行ない、なおか
つ、直線の長さ方向とは直角の方向に記録巾を拡
大させる。拡大は種々の方法で行ない得るが、後
述する再生と同一の方法で行なうとすればレーザ
ー光を巾方向に振動させるのがよく、振動は第1
図中符号2で示す固定ミラーを機械的に振動させ
るか、或いは固定ミラーを用いるかわりにTeO2、
LiNbO3等の結晶(「音響光学偏光器」と呼ばれ
る)を用い、該結晶内に超音波を発生させてレー
ザー光を回折させる方法によつて行なうことがで
きる。振動の周波数、振巾等は光学記録材料の製
作精度、レーザービームの径等の条件によつても
異なるので一概には言えないが、前記した記録媒
体用であれば光学記録材料の寸法精度は±50μ〜
±100μであり、レーザービームの集光状態での
直径を1μ、光学記録材料の走査速度を100mm/sec
とすれば、振動の周波数は例えば100KHz以上、
振巾は光学記録材料上で少くとも100μ〜200μで
ある。上記条件や振動については以上の数値は一
例であつてこれらに拘束されるものではないが、
レーザービーム径は通常0.5μ〜1.5μ程度であり、
レーザービーム径を太くすると各ピツトの形状の
精度が悪くなるため、細い方が好ましい。各ピツ
トの直線走査方向の長さは通常5μ〜50μ程度であ
る。又、光学記録材料の走査速度は現在の磁気カ
ードの走査速度(80mm/sec)を基準とすればよ
いが、これに拘束されるものではない。走査時の
レーザービームの振動数は光学記録材料の走査速
度をレーザービーム径で除して得られる数値を目
安とし、又、振巾は光学記録材料の寸法のバラツ
キの範囲を充分カバーできればよい。
In the above recording method, in the present invention, in particular, recording is performed in a straight line while relatively linearly moving the laser beam and the optical recording material, and the recording width is moved in a direction perpendicular to the length direction of the straight line. Expand. Enlargement can be done in various ways, but if it is done in the same way as the reproduction described later, it is best to vibrate the laser beam in the width direction, and the vibration is the first
Instead of mechanically vibrating the fixed mirror indicated by reference numeral 2 in the figure, or using TeO 2 , instead of using a fixed mirror,
This can be accomplished by using a crystal such as LiNbO 3 (called an "acousto-optic polarizer"), generating ultrasonic waves within the crystal, and diffracting laser light. The frequency, amplitude, etc. of vibration vary depending on the manufacturing precision of the optical recording material, the diameter of the laser beam, and other conditions, so it cannot be generalized, but if it is for the above-mentioned recording medium, the dimensional accuracy of the optical recording material is ±50μ~
±100μ, the diameter of the focused laser beam is 1μ, and the scanning speed of the optical recording material is 100mm/sec.
If so, the frequency of vibration is, for example, 100KHz or more,
The amplitude is at least 100μ to 200μ on the optical recording material. Regarding the conditions and vibrations above, the above values are just examples and are not restrictive.
The laser beam diameter is usually about 0.5μ to 1.5μ,
If the diameter of the laser beam is increased, the accuracy of the shape of each pit will deteriorate, so a narrower diameter is preferable. The length of each pit in the linear scanning direction is usually about 5μ to 50μ. Further, the scanning speed of the optical recording material may be based on the current scanning speed of magnetic cards (80 mm/sec), but is not limited to this. The frequency of the laser beam during scanning is determined by dividing the scanning speed of the optical recording material by the diameter of the laser beam, and the amplitude should be sufficient to cover the range of variations in the dimensions of the optical recording material.

このように光学記録の施された光学記録材料を
再生するには第2図に示すような公知の方法を用
い、但し上記の記録とほぼ同様に集光されたレー
ザービームを前記したような方法により走査方向
とは直角方向に振動させることを付加して行なえ
ばよく、振動の周波数及び振巾は記録の際と同様
に、出来れば振巾についてはやや大きめにして行
なうとよい。
In order to reproduce the optical recording material that has been optically recorded in this way, a known method as shown in FIG. Therefore, it is only necessary to add vibration in a direction perpendicular to the scanning direction, and the frequency and amplitude of the vibration should be the same as in recording, but if possible, the amplitude should be slightly larger.

なお、このようにレーザービームを振動させつ
つ再生するときは、レーザービームが記録された
ピツトより若干ずれて走査することが多く、ずれ
ていると本来0と1のON―OFF信号で記録再生
がなされるべきところが、ずれた分だけ少ない信
号、例えば0と0.5のように検出されるので、本
来の0と1に戻すための論理回路を適宜に付加し
てもよい。又、このような論理回路の付加によ
り、記録部分に若干の傷があつても、記録の巾よ
りも狭い傷であれば再生可能とすることもでき
る。
Note that when reproducing data while vibrating the laser beam in this way, the laser beam often scans with a slight deviation from the recorded pit, and if the laser beam is misaligned, recording and playback will normally be performed using ON-OFF signals of 0 and 1. Since what should be detected is detected as a smaller signal corresponding to the deviation, such as 0 and 0.5, a logic circuit may be added as appropriate to restore the original 0 and 1. Further, by adding such a logic circuit, even if there is a slight scratch on the recorded portion, it is possible to reproduce the scratch as long as the scratch is narrower than the width of the recording.

本発明は以上のような構成からなるため、光学
記録再生の際に記録トラツクの検出、及び記録ト
ラツクに対する再生ヘツドの追随が容易であり、
光学記録再生方式の記録媒体の製造上のばらつき
があつても確実に再生が行なえ、しかもレーザー
ビームを振動させる事自体は公知の技術を利用し
て行なえるので容易であり、本発明の方法により
記録密度の高い記録媒体の利用時の確実さが確保
できる。
Since the present invention has the above-described configuration, it is easy to detect a recording track during optical recording and reproduction, and the reproduction head can easily follow the recording track.
Even if there are manufacturing variations in optical recording and reproducing recording media, reproducing can be performed reliably, and furthermore, vibrating the laser beam itself can be easily done using a known technique, and the method of the present invention Reliability can be ensured when using a recording medium with high recording density.

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

第1図及び第2図は従来のレーザー光を用いる
記録及び再生の方法を示す説明図である。 1,5……レーザー光源、2,6……固定ミラ
ー、3,7……集光レンズ、4……光学記録材
料、8……1/4波長板、9……偏光ビームスプリ
ツター、10……フオトダイオード。
FIGS. 1 and 2 are explanatory diagrams showing a conventional recording and reproducing method using laser light. 1, 5... Laser light source, 2, 6... Fixed mirror, 3, 7... Condensing lens, 4... Optical recording material, 8... 1/4 wavelength plate, 9... Polarizing beam splitter, 10 ...Photodiode.

Claims (1)

【特許請求の範囲】[Claims] 1 光学記録材料の光学記録層にレーザー光を集
光して、走査することにより記録再生を行なう光
学記録再生方法において、レーザー光を記録時に
は走査方向に対して直角方向に振動させることに
より記録巾を拡大させつつピツトを形成し、更に
再生時にも走査方向に対して直角方向に振動させ
つつ走査することを特徴とする光学記録再生方
法。
1. In an optical recording and reproducing method in which recording and reproducing is performed by concentrating a laser beam on the optical recording layer of an optical recording material and scanning it, the recording width is changed by vibrating the laser beam in a direction perpendicular to the scanning direction during recording. An optical recording and reproducing method characterized in that pits are formed while enlarging the pits, and further, during reproduction, scanning is performed while vibrating in a direction perpendicular to the scanning direction.
JP15043082A 1982-08-30 1982-08-30 Optical recording and reproducing method Granted JPS5940325A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15043082A JPS5940325A (en) 1982-08-30 1982-08-30 Optical recording and reproducing method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15043082A JPS5940325A (en) 1982-08-30 1982-08-30 Optical recording and reproducing method

Publications (2)

Publication Number Publication Date
JPS5940325A JPS5940325A (en) 1984-03-06
JPH0222451B2 true JPH0222451B2 (en) 1990-05-18

Family

ID=15496750

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15043082A Granted JPS5940325A (en) 1982-08-30 1982-08-30 Optical recording and reproducing method

Country Status (1)

Country Link
JP (1) JPS5940325A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01133226U (en) * 1988-02-26 1989-09-11
JPH04113359U (en) * 1991-03-25 1992-10-02 日野自動車工業株式会社 Transmission oil leak prevention structure

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58153236A (en) * 1982-03-05 1983-09-12 Photo Composing Mach Mfg Co Ltd Storage system for character and picture signal

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01133226U (en) * 1988-02-26 1989-09-11
JPH04113359U (en) * 1991-03-25 1992-10-02 日野自動車工業株式会社 Transmission oil leak prevention structure

Also Published As

Publication number Publication date
JPS5940325A (en) 1984-03-06

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