JPS58137106A - Optical high-density recording device - Google Patents
Optical high-density recording deviceInfo
- Publication number
- JPS58137106A JPS58137106A JP1858282A JP1858282A JPS58137106A JP S58137106 A JPS58137106 A JP S58137106A JP 1858282 A JP1858282 A JP 1858282A JP 1858282 A JP1858282 A JP 1858282A JP S58137106 A JPS58137106 A JP S58137106A
- Authority
- JP
- Japan
- Prior art keywords
- mirror
- scan
- tape
- tracks
- specific speed
- 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
- 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
- G11B7/08—Disposition or mounting of heads or light sources relatively to record carriers
- G11B7/085—Disposition or mounting of heads or light sources relatively to record carriers with provision for moving the light beam into, or out of, its operative position or across tracks, otherwise than during the transducing operation, e.g. for adjustment or preliminary positioning or track change or selection
Landscapes
- Mechanical Optical Scanning Systems (AREA)
- Optical Recording Or Reproduction (AREA)
- Recording Or Reproducing By Magnetic Means (AREA)
Abstract
Description
【発明の詳細な説明】
この発明は%にビデオ記*4に適し九光141!直記鍮
装置にかかる。[Detailed Description of the Invention] This invention is suitable for video recording*4 in nine lights 141%! It takes directly to the brass device.
VTRは普及して来たが未だ光学8ミリカメツに比し八
−で重い欠点がある。Although VTRs have become popular, they still have the disadvantage of being 8mm and heavier than optical 8mm cameras.
本発明は8建リカメラと岡等の容積1重量で製作し青さ
カメラ一体VTRK:かかる。The present invention is manufactured with a volume of 1 weight such as an 8-frame camera and a VTRK with an integrated camera.
本発明は主にレーザ光によって磁化された磁気記録媒体
を信号に応じ消磁して記録する方式を採用する。The present invention mainly employs a method in which a magnetic recording medium magnetized by a laser beam is demagnetized according to a signal for recording.
この記鍮法において従来の如く工員の磁極性記碌法につ
いては発明者出願(18和66年12月29日特許願(
2))記載の方法で可能である。In this method, the inventor applied for a patent application filed on December 29, 1866 (December 29, 1866
2)) It is possible with the method described.
磁気テープに対する光学斜め記鎌方弐についても発明者
出願(18和66都12月!9日特許願(1))記載の
如くであるが、尚走査速度の一定性につき問題が残る。The optical diagonal recording system for magnetic tape is also described in the patent application filed by the inventor (Patent Application (1), December 9th, 1885), but there still remains a problem regarding the constancy of the scanning speed.
本発明は斜め走査を一定速度で行い得るコンパクトで新
規な手段を提供する。The present invention provides a compact and novel means for performing diagonal scanning at a constant speed.
fs1図は本発明装置によって記録され丸磁気テープl
を示す、2は並列し九記銀跡(トラ。The fs1 diagram is recorded by the device of the present invention on a round magnetic tape l.
Indicates 2 are parallel and Kuji silver marks (tora).
り)を示す、音声や制御トラ、りは図では省略しである
。The audio and control tracks (refer to the figure below) are omitted from the diagram.
1g2wAは本発明の態量的I!W14図である。磁気
テープlはリール6.7間で周知の如く走行する。6は
レーザであって赤外レーザが適轟である。4は反射鏡で
ありて、−転成い社振論してレーザの光を反射してlO
臘面に#IIIK示す 。1g2wA is the quantitative I! of the present invention! This is a W14 diagram. The magnetic tape l runs between reels 6 and 7 in a known manner. 6 is a laser, and an infrared laser is suitable. 4 is a reflecting mirror, which reflects the laser light and
#IIIK is shown on the back side.
ようなトラ、りを作る。しかしこの回転成いは振動は一
定適度で行われるとトラ、りの走査遭度は一定にならな
い、そこで再生を通常のVTRで行うと再生画像は喬直
方向に歪む、4の代りにレーず音直sameさ破る場合
も同様である0反射鏡4とテープとの距謔を大暑(する
と走査速度は一定に近づくが、かさばって来る。Make a tiger like this. However, if this rotational structure is vibrated at a certain level, the degree of scanning of the front and back will not be constant. Therefore, if playback is performed on a normal VTR, the reproduced image will be distorted in the vertical direction. The same goes for the case where the distance between the zero reflector 4 and the tape is increased (then the scanning speed approaches a constant value, but it becomes bulkier).
第sWAは2へ、ドVTR臘の光磁気記録装置を示す、
テープ1は#を埋半円形ガイドにガイドピン11,1!
を介してかけられ走行し、2つのレーずb1610つい
九−転体8によって走査される10は硝子中赤外透過体
で作れば単一体でもよい、10は従来のVTRKおける
如く不透体の2つに割れえ闇味を走査させてもよい。The sWA 2 shows a magneto-optical recording device for a VTR.
Tape 1 has # embedded into the semicircular guide with guide pins 11, 1!
10, which is scanned by the two laser beams B1610 and the non-transparent body 8, may be made of a single body as long as it is made of a glass medium infrared transmitting material. It is also possible to scan the darkness that splits into two.
菖4Eはガイド1G”がfiff@O’余の中心内を持
つようにされ、8つOレーザ6.6t、 6++のつい
先回転体8によりて同様にテープlを走査する。従来の
VTRのへ、トドラム4用スペース#i嬉8図でははt
!’f減、嬉4図ではV8近くに減る。In the irises 4E, the guide 1G'' has the center of the fiff@O', and the tape 1 is scanned in the same way by the 8 O lasers 6.6t, 6++ tip rotary body 8. To, space for drum 4 #i happy 8 in figure t
! 'f decreases, it decreases to near V8 in the Raku 4 figure.
116図はレーザー転体の給光部を示す、固定レーず6
の出力紘―合光ガイド17を経て回転光学結合部20か
ら必要に応じレンズ1g、Illを経て、テープを回転
走査する。結合部社周知の光オイド可―接続による。Figure 116 shows the light feeding part of the laser rolling body, fixed laser 6
The tape is rotated and scanned via the output light-combining guide 17, the rotating optical coupling section 20, and the lenses 1g and 111 if necessary. Coupling Department's well-known optical oid possible - by connection.
勿論前例$18,4gIにおいて、従来の回転トランス
等による電気的結合と回転レーザな用いてもよい。Of course, in the previous example $18.4gI, electrical coupling using a conventional rotary transformer or the like and a rotary laser may also be used.
菖6図ではレーザ6は固定し、Δ配列の鏡16を回転し
て、第4図の如きガイド10’上のテープを走査させる
。In FIG. 4, the laser 6 is fixed, and the mirror 16 in the Δ array is rotated to scan the tape on the guide 10' as shown in FIG.
嬉7図KsPいてはY配列の鏡型6を一転して、レーず
6の光をテープIK蟲りで走査させる。In Figure 7 KsP, the mirror type 6 in the Y array is turned around and the light from the laser 6 is scanned by the tape IK pin.
これらは第2図の場合のように往復運動でもよいが伺れ
にしても一定速度てテープを斜め走査させるには非被形
の運動をfaK与える必要がある。These may be reciprocating motions as in the case of FIG. 2, but even if they are, it is necessary to provide non-shaped motion faK in order to diagonally scan the tape at a constant speed.
第8図では上記の装置で一定回転の場合のテープ上の走
査変位2を(s)Ilfl!?で示す、横軸は時間であ
る。図のようにトラ、り為で高速、中央部で低連となる
。そこで伽)図に示すように鏡の一転成いは謔21Iの
往復運動は28で示すような変位を与えて、27の非線
形を補償しな叶ればならない。FIG. 8 shows the scanning displacement 2 on the tape in the case of constant rotation using the above device (s)Ilfl! ? The horizontal axis is time. As shown in the figure, it is fast at the top and low at the center. Therefore, as shown in the figure, the reciprocating motion of the mirror 21I must be achieved by giving a displacement as shown at 28 and compensating for the nonlinearity at 27.
第9図は一面鏡を用いて非線形を補償する本発明装置を
示す。so、at、sg社曲面鏡であって、軸88の周
を一定速度で回転する。鏡80はその位置でテープlの
トラ、り中央部8丁を走査するとし、次に右回転して8
0Iの位WIK来てlのトラ、り端88に来るには、鏡
が図の如(−りているので軸tSは余計回転しな1れば
なもない。そこで第8図27のような特性が、補償され
る。図のような場合は鏡が凸面であるので、レーずbの
光は発散すると思われるが、ビームat7w以下に対し
−の曲キ半径は最小数toopK作れるのでほぼ平面鏡
と同等と考えられる。必要に応じ補正レンズをレーずビ
ームにつけてもよい゛、この場合は平0的に1千を補正
する凹レンズとする。FIG. 9 shows an inventive device that uses a one-way mirror to compensate for nonlinearity. It is a curved mirror manufactured by SO, AT, and SG, and rotates around a shaft 88 at a constant speed. It is assumed that the mirror 80 is to scan the 8 central parts of the tape 1 at that position, and then it is rotated to the right and 8
In order to come to WIK at position 0I and reach end 88 of l, since the mirror is shaped like the figure (-), the axis tS has to be rotated more than 1. Therefore, as shown in Fig. In the case shown in the figure, the mirror has a convex surface, so the light from laser beam b is thought to diverge, but for beams at7w or less, the radius of curvature of - can be made with the minimum number toopK, so it is approximately It is considered to be equivalent to a plane mirror. If necessary, a correction lens may be attached to the laser beam. In this case, it is a concave lens that corrects 1,000 points in terms of flatness.
このような方法によりて一定速度の斜め走査が行われゐ
。纂6図に示すよりなΔ配列の鏡の面も同様に―げて同
じ効果を与えることがで龜る。By this method, diagonal scanning at a constant speed is performed. The same effect can be obtained by using mirror surfaces in a Δ arrangement as shown in Figure 6.
gto図は通常の平面鏡やレーザを直接回転させる場合
に要求される回転特性を示す、このような特性は近it
的にフィルド−と回転子との設計によって、通常の一転
機でも得られる。The GTO diagram shows the rotational characteristics required when directly rotating a normal plane mirror or laser.
Depending on the design of the field and the rotor, it can also be obtained with an ordinary single-turn machine.
1111図は第10図のような特性のモータ40を用い
たレー16.6’、6″Oa転装置を示す。FIG. 1111 shows a ray 16.6', 6'' Oa transfer device using the motor 40 having the characteristics as shown in FIG.
テープlの斜め走査は中はに一定速で行われる。The tape I is scanned diagonally at a constant speed.
勿論この他に所定の非S形回転を行うよう前特願記載の
ようなす−l系を併用してもよい。Of course, in addition to this, a -l system as described in the previous patent application may be used in combination to perform a predetermined non-S-shaped rotation.
本発明による紀鍮テープはVTR再生特に備えるよう幅
のある記鍮跡を作ることが望ましい。It is desirable that the brass tape according to the present invention produces a wide marking, especially for VTR playback.
それには発明看出願昭56都轡願 号記載の如く
帯状ビームレーザ中柱状レンズ等を用い、或い社回哲格
子による周知の方法、同時出願−の特願1857
M記載の方法等を応用する。これKよってアジアス
記鍮も行い得て、市販のV’l’Rで再生可能となる。For this purpose, as described in the invention patent application No. 1856, a strip-beam laser with a central columnar lens, etc. is used, or a well-known method using a social grid is used, and the simultaneous application of patent application No. 1857 is used.
Apply the method described in M. With this, it is possible to perform Asiatic recording, and it can be reproduced with commercially available V'l'R.
本発明はテープ以外の記鍮媒体にも適用できる。tたレ
ーザに代〉の赤外線源等をも併用できる。The present invention can also be applied to recording media other than tape. It is also possible to use an infrared source or the like in place of the laser.
本発明は上記特定例に限らすl!に種々の蜜形ヤ集施例
の部分的組合せができる。The present invention is limited to the above specific example! It is possible to make partial combinations of various honey-shaped yarn collection examples.
謔1図は斜め記―跡のある磁気テープを示す。
第2図は光磁気斜め記―装置を示す。
第8.4図は走査速度一定の本発明による斜め記II&
装置を示す。
嬉5図は光回転結合部を示す。
第6図は第4図の変形である。
菖7図は回転−による光磁気斜め記―装置を示す。
菖8図は菖7図の装置における走査速度の変化−)とこ
れを補正する特性部)を示す。
嬉seaは本発明による走査速度を一定にする回転鏡を
示す。
總10図は走査速度を一定とするモータ特性を示す。
第11図は總10図のモータを用いた走査速度一定の斜
め記録装置を示す。
図面の浄aF(内容に変更なし)
手続補正書(方式)
昭和57年 6月 8日
特許庁長官 殿
1、事件の表示
昭和57年特許願第18582号
2 発明の名称
先高密度記録装置
a 補正をする者
事件との関係 特許出願入
電 補正命令の日付
昭和67年 5月25日(発送日)
& 補正の対象
図面
0 補正の内容
別紙のとおりFigure 1 shows a magnetic tape with diagonal markings. FIG. 2 shows a magneto-optical oblique recording device. Figure 8.4 shows the diagonal II &
Show the device. Figure 5 shows the optical rotation coupling part. FIG. 6 is a modification of FIG. 4. Diagram 7 shows a magneto-optical diagonal writing device using rotation. Diagram 8 shows a change in scanning speed in the apparatus shown in diagram 7 and a characteristic section for correcting this change. Figure 1 shows a rotating mirror that maintains a constant scanning speed according to the present invention. Figure 10 shows the motor characteristics when the scanning speed is constant. FIG. 11 shows an oblique recording device with a constant scanning speed using the motor shown in FIG. Drawing aF (no change in content) Procedural amendment (method) June 8, 1980 Commissioner of the Japan Patent Office Sir 1, Indication of the case 1985 Patent Application No. 18582 2 Name of the invention High-density recording device a Relationship with the case of the person making the amendment Patent application call received Date of amendment order May 25, 1988 (shipment date) & 0 drawings subject to amendment Contents of amendment as shown in the attached sheet
Claims (1)
媒体に蚊光源を照射走査して並列した斜の記録め、を生
じる手段と、該照射走査が一定速度で行われる手段を備
えた光高密変記鍮装置。A light source modulated by a signal, a magnetic recording medium, means for scanning the armpit magnetic recording medium with a mosquito light source to produce parallel diagonal recording, and means for performing the irradiation scanning at a constant speed. A light high-density transcription brass device.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1858282A JPS58137106A (en) | 1982-02-08 | 1982-02-08 | Optical high-density recording device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1858282A JPS58137106A (en) | 1982-02-08 | 1982-02-08 | Optical high-density recording device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS58137106A true JPS58137106A (en) | 1983-08-15 |
Family
ID=11975617
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1858282A Pending JPS58137106A (en) | 1982-02-08 | 1982-02-08 | Optical high-density recording device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58137106A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US11137002B2 (en) * | 2019-05-01 | 2021-10-05 | Oshkosh Corporation | Temperature regulation system for vehicle hydraulic system |
-
1982
- 1982-02-08 JP JP1858282A patent/JPS58137106A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US11137002B2 (en) * | 2019-05-01 | 2021-10-05 | Oshkosh Corporation | Temperature regulation system for vehicle hydraulic system |
US11649838B2 (en) | 2019-05-01 | 2023-05-16 | Oshkosh Corporation | Temperature regulation system for vehicle hydraulic system |
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