JPH02219013A - Laser bar code scanner - Google Patents

Laser bar code scanner

Info

Publication number
JPH02219013A
JPH02219013A JP1040097A JP4009789A JPH02219013A JP H02219013 A JPH02219013 A JP H02219013A JP 1040097 A JP1040097 A JP 1040097A JP 4009789 A JP4009789 A JP 4009789A JP H02219013 A JPH02219013 A JP H02219013A
Authority
JP
Japan
Prior art keywords
light
reading
lens
semiconductor laser
laser
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
Application number
JP1040097A
Other languages
Japanese (ja)
Inventor
Nobuyuki Baba
信行 馬場
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.)
Ricoh Co Ltd
Original Assignee
Ricoh 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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP1040097A priority Critical patent/JPH02219013A/en
Publication of JPH02219013A publication Critical patent/JPH02219013A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To prevent the light utilization efficiency from decreasing by providing a 1st light converging member which converges light emitted from a laser source part, and further providing a 2nd light converging member which stops down the light being converged by the 1st light converging member, to a specific beam diameter for reading. CONSTITUTION:The 1st light converging lens 7 is provided on the optical path of the light emitted by the semiconductor laser 1 and has a large lens diameter enough to converge the light emitted by the semiconductor laser 1 almost without any leak. Further, the 2nd light converging lens 8 is provided on the optical path of the light which is stopped down once by the 1st light converging lens 7 and passed through a light convergence point R to the specific beam diameter for reading. Then almost all of the light emitted by the semiconductor laser 1 is converged and stopped down once, then converged by the 2nd converging lens 8 to scan a bar code surface 6 having the specific beam diameter for reading, thereby reading stored information. Consequently, the light is prevented from being eclipsed to improve the light utilization efficiency more.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、レーザ光源からの出射光をホログラムディス
ク等により走査してバーコード面の情報を読取るレーザ
バーコードスキャナに関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a laser barcode scanner that reads information on a barcode surface by scanning a hologram disk or the like with light emitted from a laser light source.

従来の技術 従来におけるレーザバーコードスキャナを第2図に基づ
いて説明する。まず、その全体構成を簡略化して述べる
。レーザ光源としての半導体レーザ1から出射された光
は、コリメータレンズ2により平行化され、アパーチャ
3によりその平行化された光のうちの読取用の有効なビ
ーム径を形成するのに不必要な余分なビームを取り除い
た後、その平行光を集光レンズ4により集光して、光走
査部材としてのホログラムスキャナ5に通過させる。こ
のホログラムスキャナ5を通過した光は走査状態となり
、読取面としてのバーコード面6上を走査し、これによ
り、そのバーコード面6に記録された情報の読取りが行
われる。なお、光走査部材としては、前記ホログラムス
キャナ5の他に、図示しないポリゴンミラーや、ガルバ
ノミラ−などを用いることができる。
2. Description of the Related Art A conventional laser barcode scanner will be described with reference to FIG. First, the overall configuration will be briefly described. Light emitted from a semiconductor laser 1 as a laser light source is collimated by a collimator lens 2, and an aperture 3 removes unnecessary extraneous light from the collimated light to form an effective beam diameter for reading. After removing the beam, the parallel light is focused by a condenser lens 4 and passed through a hologram scanner 5 as a light scanning member. The light that has passed through the hologram scanner 5 is in a scanning state and scans over the barcode surface 6 as a reading surface, thereby reading the information recorded on the barcode surface 6. In addition to the hologram scanner 5, a polygon mirror, a galvano mirror, etc. (not shown) can be used as the optical scanning member.

上述したような装置においては、情報の読取りに用いら
れる有効なビーム径は、一般に、200μm前後と非常
に小さく、しかも、読取り深度を増すためにその小さい
ビーム径を一定の距離の間は同じ状態に保つ必要がある
。このため従来においては、アパーチャ3を用いて出射
光を予め2〜5mm程度に絞り、これにより有効なビー
ム径を得るようにしている。
In the devices described above, the effective beam diameter used for reading information is generally very small, around 200 μm, and in order to increase the reading depth, the small beam diameter is kept the same for a certain distance. need to be kept. For this reason, conventionally, the aperture 3 is used to narrow down the emitted light to about 2 to 5 mm in advance, thereby obtaining an effective beam diameter.

また、半導体レーザ1から出射された光の光量の低減を
防ぎ光利用効率を上げるために、半導体レーザ1からそ
の次の位置に来るコリメータレンズ2までの距離若しく
はホログラムディスク5までの距離をできる限り短くと
っている。
In addition, in order to prevent the reduction in the amount of light emitted from the semiconductor laser 1 and increase the light utilization efficiency, the distance from the semiconductor laser 1 to the collimator lens 2 located at the next position or the distance to the hologram disk 5 should be made as short as possible. I keep it short.

さらに、読取り深度をとるために、集光点であるバーコ
ード面6とこれに最も近いレンズとなる集光レンズ4と
の間の距離は、通常、200〜400II1m程度とっ
ており、このため、縦倍率は10oO〜3000倍程度
になることが多い。なお、この縦倍率とは、第3図に示
すように、出射点Pから集光レンズ4までの距離をaと
し、集光レンズ4から集光点Qまでの距離をbとすると
、その縦倍率Cは、 c#(b/a)”       ・・・ (1)で表わ
される。
Furthermore, in order to obtain a reading depth, the distance between the barcode surface 6, which is the condensing point, and the condensing lens 4, which is the closest lens, is usually about 200 to 400 II 1 m. The vertical magnification is often about 10oO to 3000x. Note that this vertical magnification is defined as the vertical magnification, where a is the distance from the emission point P to the condensing lens 4, and b is the distance from the condensing lens 4 to the condensing point Q, as shown in Fig. 3. The magnification C is expressed as c#(b/a)'' (1).

発明が解決しようとする課題 上述したような従来の装置においては、半導体レーザ1
からの出射光の発散角が20°〜40’と大きいために
、前述したような読取用の有効なビーム径を得るために
、予めアパーチャ3を用いて出射光のビーム径を絞って
おく必要があるが、しかし、このようにアパーチャ3を
用いる方法をとると光利用効率が悪いものとなってしま
う。
Problems to be Solved by the Invention In the conventional device as described above, the semiconductor laser 1
Since the divergence angle of the emitted light is as large as 20° to 40', it is necessary to narrow down the beam diameter of the emitted light using the aperture 3 in advance in order to obtain an effective beam diameter for reading as described above. However, if such a method using the aperture 3 is adopted, the light utilization efficiency will be poor.

また、出射光の発散角が大きいため、半導体レーザlと
この次の位置に来るコリメータレンズ2(若しくは集光
レンズ4)までの距離をできる限り短くとり、これによ
り光利用効率の低減を防ごうとしているが、しかし、こ
の一方で、読取り深度をとるために、バーコード面6と
集光レンズ4との間の距離を、通常、2.00 mm 
〜400 mm程度とっているため、縦倍率は数百倍か
ら数千倍程度となる。このため、半導体レーザ1の次の
位置にくる光学部品であるコリメータレンズ2の取付は
誤差が1μm程度あったとしても、その集光点となるバ
ーコード面6上ではその誤差(1μm)の数百倍から数
千倍の値となってビーム位置がズレることになる。この
ビーム位置のズレをなくすためには、(1)式において
、距fiaを長くとればよいわけであるが、従来の装置
においては、上述した理由により、どうしても距離a、
すなわち、半導体レーザlとコリメータレンズ2との間
の距離を長くとることはできない。このため、光学系の
組付は調整にかなりの高い精度が要求されることになり
、その調整に多大な労力と時間を要することになる。
In addition, since the divergence angle of the emitted light is large, the distance between the semiconductor laser l and the collimator lens 2 (or condensing lens 4) that comes in the next position should be kept as short as possible, thereby preventing a reduction in light utilization efficiency. However, on the other hand, in order to obtain a reading depth, the distance between the barcode surface 6 and the condensing lens 4 is usually set to 2.00 mm.
Since the width is approximately 400 mm, the vertical magnification is approximately several hundred times to several thousand times. For this reason, even if there is an error of about 1 μm when installing the collimator lens 2, which is an optical component that comes next to the semiconductor laser 1, the error (1 μm) will be reflected by the number of errors (1 μm) on the barcode surface 6, which is the focal point. The beam position will shift by a factor of 100 to several thousand times. In order to eliminate this deviation in the beam position, it is sufficient to make the distance fia long in equation (1), but in conventional devices, for the reasons mentioned above, the distance a,
That is, the distance between the semiconductor laser l and the collimator lens 2 cannot be increased. For this reason, assembly of the optical system requires very high precision in adjustment, and the adjustment requires a great deal of effort and time.

課題を解決するための手段 そこで、このような問題点を解決するために、本発明は
、レーザ光源から出射された光を光走査部材により走査
し、その走査光を読取面に照射することによりその読取
面に記録された情報を読取るレーザバーコードスキャナ
において、前記レーザ光源から出射された光を集光する
第一集光部材を設け、この第一集光部材により集光され
た光を所定の読取用のビーム径に絞る第二集光部材を設
けた。
Means for Solving the Problems Therefore, in order to solve such problems, the present invention scans the light emitted from a laser light source with a light scanning member, and irradiates the reading surface with the scanning light. A laser barcode scanner that reads information recorded on the reading surface is provided with a first condensing member that condenses the light emitted from the laser light source, and the light condensed by the first condensing member is directed to a predetermined area. A second condensing member was provided to focus the beam to a reading beam diameter of .

作用 これにより、レーザ光源から出射された光は、第一集光
部材によりほとんど漏れなく集光され一度絞り込んだ状
態とされた後、第二集光部材により所定の読取用のビー
ム径に変形され読取面に導かれることになり、これによ
り、従来のようにアパーチャを用いる必要がなくなり、
しかも、レーザ光源とコリメータレンズとの間の距離を
短くとる必要もなく縦倍率を従来に比べ一段と小さくす
ることができる。
As a result, the light emitted from the laser light source is focused with almost no leakage by the first focusing member and once focused, and then transformed into a beam diameter for predetermined reading by the second focusing member. This eliminates the need to use an aperture as in the past.
Furthermore, there is no need to shorten the distance between the laser light source and the collimator lens, and the vertical magnification can be made much smaller than in the past.

実施例 本発明の一実施例を第1図に基づいて説明する。Example An embodiment of the present invention will be described based on FIG.

なお、従来技術(第2図参照)と同一部分についての説
明は省略し、その同一部分については同一符号を用いる
Note that a description of the same parts as in the prior art (see FIG. 2) will be omitted, and the same parts will be denoted by the same reference numerals.

第一集光部材としての第一集光レンズ7は、半導体レー
ザ1から出射された光の光路上に位置して設けられてお
り、その半導体レーザ1の発散角(通常、20°〜40
°)から出射された光をほとんど漏れなく集光できるよ
うな大きなレンズ径を有したものとなっている。また、
第二集光部材としての第二集光レンズ8は、前記第一集
光レンズ7により一度絞り込まれて集光点Rを通過した
光の光路上に位置して設けられており、読取用の所定の
ビーム径(約200μm)に絞る程度の大きさのレンズ
径を有したものとなっている。
The first condensing lens 7 as a first condensing member is provided so as to be located on the optical path of the light emitted from the semiconductor laser 1, and the divergence angle of the semiconductor laser 1 (usually 20° to 40°) is provided.
The lens has a large diameter that allows it to condense the light emitted from the lens with almost no leakage. Also,
The second condensing lens 8 as a second condensing member is located on the optical path of the light that has been narrowed down by the first condensing lens 7 and passed through the condensing point R. The lens diameter is large enough to narrow down the beam to a predetermined beam diameter (approximately 200 μm).

このような構成において、半導体レーザlから出射され
た光は、第一集光レンズ7によりそのほとんどの光が集
光され一度絞り込まれた後、第二集光レンズ8により集
光して、ホログラムディスク5により走査することによ
り読取用の所定のビーム径の状態でバーコード面6上を
走査し、これにより記憶された情報の読取りが行われる
In such a configuration, most of the light emitted from the semiconductor laser l is focused by the first condensing lens 7 and narrowed down once, and then condensed by the second condensing lens 8 to form a hologram. By scanning with the disk 5, the barcode surface 6 is scanned with a predetermined beam diameter for reading, thereby reading the stored information.

この場合、第一集光レンズ7を設けたことにより、従来
のようにアパーチャ3を設ける必要がないため光のケラ
レ部分がなくなるため、出射光の光利用効率を一段と上
げることができる。また、第一集光レンズ7を用いたこ
とにより、半導体レーザ1と第一集光レンズ7との間の
距離aを、従来に比べて長くとることができるため、(
1)式より得られる縦倍率の値を従来の値(数百倍〜数
千倍)に比べて一段と小さくとることができる。
In this case, by providing the first condensing lens 7, there is no need to provide the aperture 3 as in the conventional case, so there is no vignetting of the light, and the light utilization efficiency of the emitted light can be further increased. Furthermore, by using the first condensing lens 7, the distance a between the semiconductor laser 1 and the first condensing lens 7 can be made longer than in the past.
1) The value of the vertical magnification obtained from the formula can be made much smaller than the conventional value (several hundred to several thousand times).

従って、従来では距離a(半導体レーザlとコリメータ
レンズ2との間の距離)の組付は精度を数μm以内の非
常に高い精度にとらなければならなかっだが、本発明で
は、縦倍率の低減化により、その距Haの組付は精度を
従来はど厳密にとる必要はなく、その結果、ある程度余
裕をもってその組付は調整を行うことができる。さらに
、半導体レーザ1と第一集光レンズ7との間の距離aを
十分とり、第二集光レンズ8を数mmのオーダで動かす
ことによって、バーコード面6における集光位置を変え
ることなく、精度良く光学系の組付は調整を行うことが
できる。
Therefore, in the past, the assembly of the distance a (distance between the semiconductor laser l and the collimator lens 2) had to be performed with very high precision within several μm, but in the present invention, the accuracy of the assembly for the distance a (distance between the semiconductor laser l and the collimator lens 2) must be maintained at a very high level of accuracy within several μm. Because of this, it is not necessary to assemble the distance Ha as precisely as conventionally, and as a result, the assembly can be adjusted with some margin. Furthermore, by keeping a sufficient distance a between the semiconductor laser 1 and the first condensing lens 7 and moving the second condensing lens 8 by several millimeters, the condensing position on the barcode surface 6 can be maintained without changing. , the assembly of the optical system can be adjusted with high precision.

なお、本発明に係る第−集光部材及び第二集光部材は、
光を集束させる機能をもつものであればよく、例えば、
ホロレンズやホログラムスキャナを用いるようにしても
よい。
In addition, the first light condensing member and the second light condensing member according to the present invention are as follows:
It only needs to have the function of focusing light, for example,
A hololens or a hologram scanner may also be used.

発明の効果 本発明は、第一集光部材によりレーザ光源から出射され
た光のほとんどを集光するようにしたので、従来のよう
にアパーチャを用いたときのような光のケラレをなくす
ことができるため光利用効率を一段と上げることができ
るものである。また、第一集光部材はレーザ光源から離
して設けることができるため、縦倍率を従来に比べ一段
と小さくとることが可能となり、これにより、従来のよ
うに非常に高い精度で光学系の組付は調整を行わなう必
要がなくなり、しかも、第二集光部材を111に光軸方
向に動かすことによって、バーコード面における集光位
置をズラすことなく精度良く光学系の組付は調整を行う
ことができるものである。
Effects of the Invention In the present invention, since most of the light emitted from the laser light source is focused by the first light focusing member, it is possible to eliminate the vignetting of light that occurs when an aperture is used as in the past. This makes it possible to further increase light utilization efficiency. In addition, since the first light condensing member can be placed away from the laser light source, it is possible to make the vertical magnification much smaller than in the past, which makes it possible to assemble the optical system with extremely high precision, unlike in the past. Moreover, by moving the second condensing member 111 in the optical axis direction, the assembly of the optical system can be adjusted accurately without shifting the condensing position on the barcode surface. It is something that can be done.

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

第1図は本発明の一実施例を示す光路図、第2図は従来
例を示す光路図、第3図は縦倍率の関係を示す説明図で
ある。 1・・・レーザ光源、5・・・光走査部材、6・・・読
取面、7・・・第1集光部材、8・・・第二集光部材用
 願 人    株式会社 リ コ
FIG. 1 is an optical path diagram showing an embodiment of the present invention, FIG. 2 is an optical path diagram showing a conventional example, and FIG. 3 is an explanatory diagram showing the relationship between vertical magnifications. DESCRIPTION OF SYMBOLS 1... Laser light source, 5... Light scanning member, 6... Reading surface, 7... First condensing member, 8... Second condensing member Applicant Rico Co., Ltd.

Claims (1)

【特許請求の範囲】[Claims] レーザ光源から出射された光を光走査部材により走査し
、その走査光を読取面に照射することによりその読取面
に記録された情報を読取るレーザバーコードスキャナに
おいて、前記レーザ光源から出射された光を集光する第
一集光部材を設け、この第一集光部材により集光された
光を所定の読取用のビーム径に絞る第二集光部材を設け
たことを特徴とするレーザバーコードスキャナ。
In a laser barcode scanner that scans the light emitted from a laser light source with an optical scanning member and irradiates the scanning light onto the reading surface to read information recorded on the reading surface, the light emitted from the laser light source is used. A laser barcode characterized by being provided with a first condensing member that condenses the light, and a second condensing member that narrows the light condensed by the first condensing member to a predetermined beam diameter for reading. scanner.
JP1040097A 1989-02-20 1989-02-20 Laser bar code scanner Pending JPH02219013A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1040097A JPH02219013A (en) 1989-02-20 1989-02-20 Laser bar code scanner

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1040097A JPH02219013A (en) 1989-02-20 1989-02-20 Laser bar code scanner

Publications (1)

Publication Number Publication Date
JPH02219013A true JPH02219013A (en) 1990-08-31

Family

ID=12571368

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1040097A Pending JPH02219013A (en) 1989-02-20 1989-02-20 Laser bar code scanner

Country Status (1)

Country Link
JP (1) JPH02219013A (en)

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