JPS5918773B2 - Optical spot size control device - Google Patents

Optical spot size control device

Info

Publication number
JPS5918773B2
JPS5918773B2 JP50060715A JP6071575A JPS5918773B2 JP S5918773 B2 JPS5918773 B2 JP S5918773B2 JP 50060715 A JP50060715 A JP 50060715A JP 6071575 A JP6071575 A JP 6071575A JP S5918773 B2 JPS5918773 B2 JP S5918773B2
Authority
JP
Japan
Prior art keywords
light beam
lens
recording
reflected
reflected light
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
Application number
JP50060715A
Other languages
Japanese (ja)
Other versions
JPS51135667A (en
Inventor
富夫 吉田
昌宏 出口
宏司 松島
彬史 中田
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP50060715A priority Critical patent/JPS5918773B2/en
Publication of JPS51135667A publication Critical patent/JPS51135667A/en
Publication of JPS5918773B2 publication Critical patent/JPS5918773B2/en
Expired legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording 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
    • G11B7/08Disposition or mounting of heads or light sources relatively to record carriers
    • G11B7/09Disposition or mounting of heads or light sources relatively to record carriers with provision for moving the light beam or focus plane for the purpose of maintaining alignment of the light beam relative to the record carrier during transducing operation, e.g. to compensate for surface irregularities of the latter or for track following
    • G11B7/0908Disposition or mounting of heads or light sources relatively to record carriers with provision for moving the light beam or focus plane for the purpose of maintaining alignment of the light beam relative to the record carrier during transducing operation, e.g. to compensate for surface irregularities of the latter or for track following for focusing only
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording 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
    • G11B7/12Heads, e.g. forming of the optical beam spot or modulation of the optical beam
    • G11B7/125Optical beam sources therefor, e.g. laser control circuitry specially adapted for optical storage devices; Modulators, e.g. means for controlling the size or intensity of optical spots or optical traces

Landscapes

  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Recording Or Reproduction (AREA)
  • Focusing (AREA)
  • Automatic Focus Adjustment (AREA)

Description

【発明の詳細な説明】 本発明は物体の表面に一定の大きさの光スポットを形成
する装置を提供することを目的とする。
DETAILED DESCRIPTION OF THE INVENTION An object of the present invention is to provide a device for forming a light spot of a constant size on the surface of an object.

光スポットによる情報の記録あるいは再生は色色の分野
で使用されている。例えば情報を光ビームによりマイク
ロフィルムに記録し、現像後読み出す装置、あるいは感
光性材料に例えばファクシミリ信号を記録する装置、ま
た近年になつて光学的に高密度の情報の記録または再生
できる材料の進歩にともなつて、微少の光スポットによ
つて多量の情報を高密度で記録再生することが試みられ
ている。上記のような装置においてはいずれも記録再生
物体上に形成される光スポットの大きさを一定に保ち情
報の記録または再生が品質良〈行なわれることが望まれ
る。とくに微少スポットによる多量情報の高密度記録再
生において重要な要素となる。上記の記録再生面上の光
スポットを微少(例えば数μ)にしかも一定の大きさに
保つために一般的には、微少スポットを作る光学系と記
録または再生物体面との距離を一定に保つことが行なわ
れる。上記の距離を一定に保つために光学的手段、磁気
的手段、静電的手段、流体力学的手段等が用いられてい
る。本発明は光学的手段により上記の光学系と記録また
は再生物体間の距離を検出し制御することによつて光ス
ポットを一定の大きさに保持する結像制御装置を提供す
る。
Recording or reproducing information using light spots is used in the color field. For example, there are devices that record information on microfilm using a light beam and read it out after development, or devices that record, for example, facsimile signals on photosensitive materials, and recent advances in materials that can optically record or reproduce high-density information. As a result, attempts have been made to record and reproduce large amounts of information at high density using minute light spots. In any of the above devices, it is desirable that the size of the light spot formed on the recording/reproducing object be kept constant so that information can be recorded or reproduced with good quality. This is particularly an important element in high-density recording and reproduction of a large amount of information using minute spots. In order to keep the above-mentioned light spot on the recording/playback surface small (for example, several μ) and at a constant size, the distance between the optical system that creates the small spot and the recording or playback object surface is generally kept constant. things will be done. Optical means, magnetic means, electrostatic means, hydrodynamic means, etc. are used to keep the above distance constant. The present invention provides an imaging control device that maintains a light spot at a constant size by detecting and controlling the distance between the optical system and the recording or reproducing object using optical means.

以下図面にしたがつて本発明の一実施例を詳細に説明す
る。
An embodiment of the present invention will be described in detail below with reference to the drawings.

第1図には本発明の一実施例を示す。FIG. 1 shows an embodiment of the present invention.

第1図において、1は上記の情報を記録または再生する
ための記録媒体で矢印の方向に移動する。
In FIG. 1, reference numeral 1 denotes a recording medium for recording or reproducing the above information, which moves in the direction of the arrow.

2は記録媒体1上のA点に微少光スポットを形成・ す
るためのレンズ、3は矢印の方向に移動可能なレンズホ
ルダー、4はシフトパルス発生回路で一定の繰り返しの
シフトパルスを発生する。
2 is a lens for forming a minute light spot at point A on the recording medium 1; 3 is a lens holder movable in the direction of the arrow; and 4 is a shift pulse generation circuit that generates a constant repetition of shift pulses.

5は光検出素子列で例えば30μ程度の大きさの光検出
素子が多数配置さ江それらの各出力は上記ンフ、 トパ
ルス発生回路4からのシフトパルスによつてシリーズに
出力される。
Reference numeral 5 denotes a photodetection element array in which a large number of photodetection elements each having a size of, for example, about 30 μm are arranged, and their respective outputs are outputted in series by shift pulses from the above-mentioned pulse generation circuit 4.

6は上記光検出素子列からシリーズに出力される電気信
号を検出して受光素子列5の受光ビームの太さに比例し
たパルス幅をもつた短形波を作る整形回路で、第2図a
に示す光電変換器列に印加されるクロツクパルス列に対
応して出力される第2図bに示す光電変換器列の出力を
第2図eに示すパルス幅出力に変換する。
6 is a shaping circuit that detects the electrical signals output in series from the photodetector array 5 and generates a rectangular wave having a pulse width proportional to the thickness of the light beam received by the photodetector array 5;
The output of the photoelectric converter array shown in FIG. 2b, which is output in response to the clock pulse train applied to the photoelectric converter array shown in FIG. 2, is converted into the pulse width output shown in FIG. 2e.

一般的に積分回路と波形整形回路からなる。7は整形回
路6のパルス幅信号を積分して上記パルス幅に比例した
出力を発生する回路、8は7の出力と端子Bに与えられ
る直流電圧の差を検出し増幅する回路、9は8から出力
される差信号に応じて、レンズホルダ3を駆動する回路
である。
It generally consists of an integrating circuit and a waveform shaping circuit. 7 is a circuit that integrates the pulse width signal of the shaping circuit 6 and generates an output proportional to the pulse width; 8 is a circuit that detects and amplifies the difference between the output of 7 and the DC voltage applied to terminal B; 9 is 8 This circuit drives the lens holder 3 according to the difference signal output from the lens holder 3.

φInは入射光ビームを示しレンズ2の光軸とずれた光
軸をもつて入射する。この図では平行光線を示している
が、平行光線以外でも実施できる。また微少スボツトを
得るためには一般にコヒーレントな光源が用いられる。
φInはレンズ2で絞られて記録再生媒体1上に微小な
光スポツトAを発生する。A点で反射された光はレンズ
2を通つてφ0utなる反射光ビームを発生する。φ0
utの太さが、光検出素子群5で検出される。また第1
図でdはレンズと記録再生媒体面1との距離を示す。本
発明は記録再生媒体1とレンズ系2が情報を記録または
再生するために相対運動するときに、この運動によつて
発生する距離dの変動を補償し常に一定の距離に保持し
、微少光スポツトAを一定の大きさに保持するものであ
る。また第1図のcはレンズ2の光軸を示す。第3図は
第1図の構成に卦いて距離dの変動を反射光ビームφ0
utの太さで検出できることを示す図である。
φIn represents an incident light beam, which enters with an optical axis shifted from the optical axis of the lens 2. Although parallel rays are shown in this figure, it can also be carried out with other than parallel rays. Furthermore, a coherent light source is generally used to obtain minute spots.
φIn is condensed by a lens 2 to generate a minute light spot A on the recording/reproducing medium 1. The light reflected at point A passes through lens 2 and generates a reflected light beam φ0ut. φ0
The thickness of ut is detected by the photodetecting element group 5. Also the first
In the figure, d indicates the distance between the lens and the recording/reproducing medium surface 1. The present invention compensates for fluctuations in the distance d caused by this movement when the recording/reproducing medium 1 and the lens system 2 move relative to each other in order to record or reproduce information, and maintains the distance d always at a constant distance. This is to maintain spot A at a constant size. Further, c in FIG. 1 indicates the optical axis of the lens 2. Figure 3 shows the configuration of Figure 1, and the variation of the distance d is reflected by the reflected light beam φ0.
It is a figure which shows that it can be detected by the thickness of ut.

ここでは説明の簡単のために反射光も平行光線として近
似している。第3図aはレンズ2と、記録再生材料1と
の距離DOが正規の値をとり微少光スポツトが点Aに生
じている例を示す。
Here, for ease of explanation, reflected light is also approximated as parallel rays. FIG. 3a shows an example in which the distance DO between the lens 2 and the recording/reproducing material 1 is a normal value and a minute light spot is generated at point A.

このとき反射光ビームφ0utの直径をD1とする。第
3図bは、上記の距離D。がレンズ2または記録再生材
料1のいずれかの動きによつて(DO−Δd)になつた
ときの図を示す。光点Aは上記材料面に対称なA点で微
少光スポツトとなるので反射光ビームφ0utの直径D
2は明らかにa図のD1より小さくなる。また第3図c
はaの距離D。がΔdだけ増加した場合を図示する。こ
の場合は図より明らかなように反射光は材料面に対して
A点に対称な点Aから発生したように分布するので反射
光ビームφ0utの直径D,はD,より大きくなる。し
たがつて反射光ビームの直径を第1図に示す光検出素子
列5で検出し、電気パルスの幅に変換する回路6でパル
ス幅に変換し、これを積分し、基準電圧との差をとれば
8の出力としてレンズ2を駆動する誤差電圧を発生する
。この誤差電圧と距離dの関係の一例を第4図に示す。
したがつてこの誤差電圧を用いてレンズホルダ3を移動
制御することによつて、レンズ2と記録再生材料1との
距離dを一定に保持することができる。
At this time, the diameter of the reflected light beam φ0ut is assumed to be D1. FIG. 3b shows the distance D mentioned above. The figure shows a case where the angle becomes (DO-Δd) due to the movement of either the lens 2 or the recording/reproducing material 1. Since the light point A becomes a minute light spot at point A symmetrical to the material surface, the diameter D of the reflected light beam φ0ut
2 is obviously smaller than D1 in figure a. Also, Figure 3c
is the distance D of a. The figure shows a case where Δd increases. In this case, as is clear from the figure, the reflected light is distributed as if it were generated from a point A that is symmetrical to point A with respect to the material surface, so the diameter D, of the reflected light beam φ0ut is larger than D. Therefore, the diameter of the reflected light beam is detected by the photodetecting element array 5 shown in FIG. If it is, an error voltage for driving the lens 2 is generated as the output of 8. An example of the relationship between this error voltage and the distance d is shown in FIG.
Therefore, by controlling the movement of the lens holder 3 using this error voltage, the distance d between the lens 2 and the recording/reproducing material 1 can be kept constant.

レンズホルダーは、例えばスピーカーのボイスコイルの
駆動装置のように磁気的な力によつて移動制御される。
また低速度の制御で良い場合には、例えばネジ機構とモ
ータを用いて上下の移動制御が行なわれる。第6図に光
検出素子列と反射光ビームの関係卦よび第1図4に示す
クロツクパルス発生器のクロツクパルス列と、光検出素
子列の出力電気パルス幅の関係を示す。
The movement of the lens holder is controlled by magnetic force, such as a driver for a voice coil of a speaker.
If low-speed control is sufficient, the vertical movement is controlled using, for example, a screw mechanism and a motor. FIG. 6 shows the relationship between the photodetector array and the reflected light beam, and the relationship between the clock pulse train of the clock pulse generator shown in FIG. 1 and the output electric pulse width of the photodetector array.

第5図Aは光検出素子の配列例を示し、Bはこれに対し
て入射する反射光ビームの関係を示す。
FIG. 5A shows an example of the arrangement of photodetecting elements, and FIG. 5B shows the relationship of reflected light beams incident thereon.

一般的には第1図のレンズ2または記録再生材料の傾き
に対しても確実な検出ができるように各光検出素子(1
,2・・―・・・・・・n)のたて方向の長さbを大き
くしておく方が良い。第5図C,Dは、第5図A,Bに
示した光検出素子列と反射光ビームとの関係において、
(すなわち5番目から(n一3)番目までの光検出素子
に反射光があたる状態)、光検出素子列に加えられるク
ロツクパルスCと第1図6の波形整形回路から出力され
る電気パルス幅の対応を示す。すなわち5番目のクロツ
クから(n−3)番目のクロツクパルスまで幅の矩形パ
ルスが出力される。このようなパルスが、クロツクの印
加の仕方に応じて周期的に発生する。以上に本発明の一
実施例を説明した。第6図には本発明の他の実施例を示
す。第1図の構成では一般に入射光ビームφInと反射
光ビームの距離が近くて、光検出素子列を挿入出来ない
場合がある。
In general, each photodetector element (1
, 2...n), it is better to increase the length b in the vertical direction. FIGS. 5C and 5D show the relationship between the photodetector array and the reflected light beam shown in FIGS. 5A and B.
(In other words, the state in which the reflected light hits the 5th to (n-3)th photodetector elements), the clock pulse C applied to the photodetector array and the electrical pulse width output from the waveform shaping circuit shown in FIG. Show correspondence. That is, a rectangular pulse having a width from the fifth clock pulse to the (n-3)th clock pulse is output. Such pulses occur periodically depending on how the clock is applied. One embodiment of the present invention has been described above. FIG. 6 shows another embodiment of the invention. In the configuration shown in FIG. 1, the distance between the incident light beam φIn and the reflected light beam is generally so short that it may not be possible to insert a photodetecting element array.

このような場合、第6図に示すように全反射ミラーに少
さい孔を開けこれを通して入射光ビームをレンズにあて
、反射光ビームは左方に反射して光検出素子列5に当て
るものである。このように孔開き全反射ミラーを用いる
ことによシ、、記録再生材料に照射する光エネルギ−の
利用効率を高め、しかも反射光としても強い強度のもの
が得られ確実な検出ができる。また反射光ビーム径が小
さいときにはレンズ系で拡大して光検出素子列に照射す
ることも可能である。なお、以上の実施例ではレンズの
光軸よりはずれた位置に光ビームを入射し、記録または
再生材料面からの反射光ビームも前記レンズの光軸より
はずれた位置に入射するように構成しているが、光ビー
ムをレンズの光軸に入射し、反射光ビームも前記レンズ
の光軸に入射するよう構成し、入射光ビームと反射光ビ
ームとが同一径路を通るよう構成した場合にも、ビーム
スプリツタやハーフミラーの使用により、反射光ビーム
のみを分離して光検出素子に導くよう構成しても良い。
以上のように本発明によればレンズと結像面との距離を
適正に制御することにより、前記レンズを介して照射さ
せる光ビームを記録または再生材料面に所定のスポツト
大きさで確実に照射できるものである。
In such a case, as shown in FIG. 6, a small hole is made in the total reflection mirror and the incident light beam is passed through the hole to hit the lens, and the reflected light beam is reflected to the left and hits the photodetector array 5. be. By using the apertured total reflection mirror in this manner, the utilization efficiency of the light energy irradiated onto the recording and reproducing material is increased, and moreover, high intensity reflected light can be obtained, allowing reliable detection. Furthermore, when the diameter of the reflected light beam is small, it is possible to magnify it using a lens system and irradiate the photodetecting element array. In the above embodiments, the light beam is incident on a position off the optical axis of the lens, and the light beam reflected from the surface of the recording or reproducing material is also made incident on a position off the optical axis of the lens. However, even when the light beam is made incident on the optical axis of the lens, the reflected light beam is also made incident on the optical axis of the lens, and the incident light beam and the reflected light beam are made to pass through the same path, By using a beam splitter or a half mirror, only the reflected light beam may be separated and guided to the photodetecting element.
As described above, according to the present invention, by appropriately controlling the distance between the lens and the imaging plane, the light beam irradiated through the lens is reliably irradiated onto the surface of the recording or reproducing material in a predetermined spot size. It is possible.

な卦、実施例に示す入射光ビームφInそれ自体を、記
録あるいは再生用のビームとしても良く、また、この入
射光ビームと異なる波長の入射光ビームを記録再生用ビ
ームとして前記レンズを介して記録または再生材料面に
照射しても良いものである。
Note that the incident light beam φIn shown in the embodiment itself may be used as a recording or reproducing beam, or an incident light beam having a wavelength different from this incident light beam may be used as a recording/reproducing beam for recording through the lens. Alternatively, the surface of the recycled material may be irradiated.

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

第1図本発明の一実施例における光スポツトサイズ宙u
御装置のプロツク図、第2図は要部の信号波形図、第3
図A,b,cは本発明の動作原理図、第4図は距離の変
動と誤差電圧の関係を示す図、第5図光検出素子列で受
光する反射光ビームの系を電気パルス幅に変換する手段
を説明するための図、第6図本発明の他の実施例を示す
図である。 1・・・・・・記録再生材料、2・・・・・・レンズ、
3・・・・・・移動可能なレンズホルダ、4・・・・・
・クロツクパルス発生器、5・・・・・・光検出素子列
、6・・・・・・波形成形回路、7・・・・・・積分回
路、8・・・・・・差動増幅器、9・・・・・ルンズホ
ルダ駆動回路、A・・・・・・微少光スポツト、φIn
・・・・・・入射光ビーム、φ0ut・・・・・・反射
光ビーム。
Fig. 1 Light spot size in the air in one embodiment of the present invention
Figure 2 shows the main part signal waveform diagram, Figure 3 shows the block diagram of the control device.
Figures A, b, and c are diagrams of the operating principle of the present invention. Figure 4 is a diagram showing the relationship between distance fluctuation and error voltage. Figure 5 is a diagram showing the system of reflected light beams received by the photodetector array in electrical pulse width. FIG. 6 is a diagram for explaining a means for converting, and a diagram showing another embodiment of the present invention. 1...Recording and reproducing material, 2...Lens,
3...Movable lens holder, 4...
・Clock pulse generator, 5...Photodetection element array, 6...Waveform shaping circuit, 7...Integrator circuit, 8...Differential amplifier, 9 .....Luns holder drive circuit, A..... faint light spot, φIn
...Incident light beam, φ0ut...Reflected light beam.

Claims (1)

【特許請求の範囲】[Claims] 1 一定の直径の光ビームをレンズを介して記録または
再生材料面に照射し、その光ビームの前記材料面からの
反射光ビームを前記レンズを介して複数個の光検出素子
が配列された光検出素子列に照射し、その光検出素子の
各出力の加算出力より前記反射光ビームの照射される前
記光検出素子の個数に応じたレベルの電気信号を作成し
、その電気信号のレベルに応じて前記レンズを駆動して
、そのレンズと前記材料面との距離を一定に保持するこ
とを特徴とする光スポットサイズ制御装置。
1. A light beam of a certain diameter is irradiated onto the surface of a recording or reproducing material through a lens, and the light beam reflected from the material surface is reflected through the lens into a light beam on which a plurality of photodetecting elements are arranged. irradiate a detection element array, create an electrical signal of a level corresponding to the number of the photodetection elements irradiated with the reflected light beam from the summed output of each output of the photodetection element, and according to the level of the electrical signal. A light spot size control device characterized in that the distance between the lens and the material surface is maintained constant by driving the lens.
JP50060715A 1975-05-20 1975-05-20 Optical spot size control device Expired JPS5918773B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP50060715A JPS5918773B2 (en) 1975-05-20 1975-05-20 Optical spot size control device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP50060715A JPS5918773B2 (en) 1975-05-20 1975-05-20 Optical spot size control device

Publications (2)

Publication Number Publication Date
JPS51135667A JPS51135667A (en) 1976-11-24
JPS5918773B2 true JPS5918773B2 (en) 1984-04-28

Family

ID=13150253

Family Applications (1)

Application Number Title Priority Date Filing Date
JP50060715A Expired JPS5918773B2 (en) 1975-05-20 1975-05-20 Optical spot size control device

Country Status (1)

Country Link
JP (1) JPS5918773B2 (en)

Also Published As

Publication number Publication date
JPS51135667A (en) 1976-11-24

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