JPS61112289A - Bar code reader - Google Patents

Bar code reader

Info

Publication number
JPS61112289A
JPS61112289A JP59234362A JP23436284A JPS61112289A JP S61112289 A JPS61112289 A JP S61112289A JP 59234362 A JP59234362 A JP 59234362A JP 23436284 A JP23436284 A JP 23436284A JP S61112289 A JPS61112289 A JP S61112289A
Authority
JP
Japan
Prior art keywords
spot
bar code
light beam
light
scanning direction
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
JP59234362A
Other languages
Japanese (ja)
Inventor
Nobuo Kanai
伸夫 金井
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.)
Minolta Co Ltd
Original Assignee
Minolta 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 Minolta Co Ltd filed Critical Minolta Co Ltd
Priority to JP59234362A priority Critical patent/JPS61112289A/en
Publication of JPS61112289A publication Critical patent/JPS61112289A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To increase the area of irradiation to obtain a sufficient quantity of irradiating light and also to avoid the deterioration of the image resolution even though the scanning direction has more inclination than the orthogonal position to the bars of a bar code, by forming an irradiating spot of a light beam into a diamond shape which is long in the rectangular direction. CONSTITUTION:The bar B of a bar code is scanned by shifting an irradiated spot P of a light beam toward an arrow head. A state where an adjacent bar code never gets inside the spot P is always secured even in case the scanning direction is tilted by theta, where the vertical angle and the length of a shorter diagonal line of a diamond shape of the spot P are set at 2theta and (b) respectively. As a result, the image resolution has no deterioration. The angle theta is set at about >=10 deg. and preferably in a range of 20-40 deg.. Furthermore it is preferably set at the minimum value 0.24mm of less of the bar code for the width of the spot P (also available enough with about 0.3mm).

Description

【発明の詳細な説明】 イ 産業上の利用分野 本発明は自己走査型のバーコードリー々°に関する。[Detailed description of the invention] B Industrial application field The present invention relates to self-scanning barcode readers.

口 従来の技術 自己走査型のバーコードリータ′は光ビームを走査手段
1こよって振らせてバーコード記録面を光ビームで走査
する醪匝1こなっているが、必要な分解能を得るたtに
は、被走査面上で光ビームを充分に小さなスポットに収
束させる必集がある。また信号処理の面からは、なるべ
くS/N比の高い読取り信号が得られることが望まれ、
そのため1こは光ビームの光量は多い程良い。被走査面
上の微小な光照射スポットに多量の光量を収束させる方
法の一つは云うまでもなく、なるべ(高輝度の光源を用
いることで、この点からは光源としてレーザが適してい
る。−万九源蚤こ発光ダイオード等実質的に面発光する
光源を用いる場合には照射光重を増せばよく、そのため
には被走査面において光ビームの照射面積を大きくする
ことも考えられる。
The conventional self-scanning type barcode reader' uses a scanning means (1) to swing a light beam to scan the barcode recording surface with the light beam, but in order to obtain the necessary resolution, It is necessary to focus the light beam onto a sufficiently small spot on the scanned surface. Also, from the perspective of signal processing, it is desirable to obtain a read signal with as high a S/N ratio as possible.
Therefore, the larger the amount of light beam, the better. Needless to say, one way to converge a large amount of light onto a minute spot on the scanned surface is to use a high-intensity light source, and from this point of view a laser is suitable as a light source. - Mankumoto When using a light source that emits light from a surface such as a light emitting diode, it is sufficient to increase the weight of the irradiated light, and for this purpose, it is possible to increase the irradiation area of the light beam on the surface to be scanned.

バーコードリータ゛の分解能はバーコードのバーと直交
する方向にのみ存在ずれはよく、バーと平行の方向には
分解能は要求されないので、光ビームの照射面積を大(
ζして、しかも分解能を低下させないためには光ビーム
の断面を矩形状に長(して、その長手方向を走査方向と
直交即ちバーコードのバーと平行にすれはよく、そのよ
うな提案か特開昭56−140467号においてなされ
ている。
The resolution of the barcode reader is good only in the direction perpendicular to the bars of the barcode, and resolution is not required in the direction parallel to the bars, so the irradiation area of the light beam can be increased (
ζ In order not to reduce the resolution, it is best to make the cross section of the light beam rectangular (and make the longitudinal direction perpendicular to the scanning direction, that is, parallel to the bar code bar). This is disclosed in Japanese Patent Application Laid-open No. 140467/1983.

この提案はレーザタ゛イオードにおいて、矩形の空洞又
(はレーザ発射絞りを用いて矩形のビームスポットを得
ることにより、同じ照射光量で円形スボットよりも高い
分解能を得ようとするものである。
This proposal attempts to obtain a rectangular beam spot using a rectangular cavity or a laser emitting aperture in a laser diode, thereby obtaining higher resolution than a circular subbot with the same amount of irradiation light.

以上要するに、被走査面上で光ビームの照射スポットを
バーコードのバーと平行方向1こ長い矩形にすれば、照
射スポットの照度が低くても高いSZN比が得られ、使
用し得る光源の選択範囲が広くなり、レーザのような光
源を用いる場合には同じ照射光量でより高い分解能が得
られると云うことである。
In summary, if the irradiation spot of the light beam on the scanned surface is made into a rectangle that is one length longer in the direction parallel to the bar code bar, a high SZN ratio can be obtained even if the illuminance of the irradiation spot is low, and it is possible to select a usable light source. This means that the range becomes wider, and when a light source such as a laser is used, higher resolution can be obtained with the same amount of irradiation light.

ハ 発明が解決しようとする問題点 上述した光ビームの照射スポットを矩形にすると云う方
法には次のような問題がある。
C. Problems to be Solved by the Invention The method of making the irradiation spot of the light beam rectangular as described above has the following problems.

第4図において斜線を入れた帯Bはバーコードのバーで
あり、矩形の枠Pは光ビームの照射スポットである。ま
た矢線は光ビームによる走査方向で、第4図Aは走査方
向が正しくバーコードのバーと直交している場合であり
、同図Bは走査方向が傾いている場合を示す。この図か
ら明かなように走査方向が傾くと、実効的に光ビームの
照射スポットがaからbに広がったのと同じになり分解
能が低下する。
In FIG. 4, the hatched band B is the bar code bar, and the rectangular frame P is the irradiation spot of the light beam. Further, the arrow indicates the scanning direction by the light beam, and FIG. 4A shows the case where the scanning direction is correctly orthogonal to the bars of the bar code, and FIG. 4B shows the case where the scanning direction is tilted. As is clear from this figure, when the scanning direction is tilted, the effective spot of the light beam is expanded from a to b, and the resolution is reduced.

しかるにバーコードリーダに対してノイーコードが正し
い方向にセットされるようにすることは困難であり、特
に手持ち型のバーコードリーグを商品の側面に当て\バ
ーコードを読取る場合にはバーコードとバーコードリー
グとの相対的関係を一定に規制することは実際上不可能
である。このような理由で光ビームの照射スポットを矩
形にすると云う案は読取りの正確さを保証する上で茜だ
不安がある。
However, it is difficult to set the Neue code in the correct direction for the barcode reader, especially when placing a handheld barcode league against the side of the product to read the barcode. It is practically impossible to regulate the relative relationship with the league. For this reason, the idea of making the irradiation spot of the light beam rectangular has some concerns in ensuring the accuracy of reading.

本発明は光ビームの照射スポットを細長くして、しかも
走査方向がバーコードのバーと直交する方向から傾いて
も分解能が低下しないよう番こしようとするものである
The present invention aims to elongate the irradiation spot of the light beam so that the resolution does not deteriorate even if the scanning direction is tilted from the direction perpendicular to the bars of the bar code.

二 問題点解決のための手段 本発明は光ビームの照射スポットを細長い菱形状にした
2. Means for Solving Problems In the present invention, the irradiation spot of the light beam is shaped into an elongated rhombus.

ホ 作用                     
   )゛啄第1図は本発明の詳細な説明するものであ
る。
E action
) Figure 1 provides a detailed explanation of the invention.

この図でBはバーコードのバーでPが光ビームの照射ス
ポットである。矢線は走査方向であり、同図aは走査方
向が正しい場合、同すは走査方向が傾いた場合である。
In this figure, B is a bar code bar, and P is a light beam irradiation spot. The arrow indicates the scanning direction, and the figure a shows the case where the scanning direction is correct, and the figure shows the case where the scanning direction is tilted.

全照射スポットPの菱形の頂角を20、短い方の対角線
の長さを2とすると、走査方向がθ傾いた第1′図すの
場合においても照射スポット内に隣接のバーコードが入
り込まない状態が必ず存在することが保証され、分解能
の低下は生じない。
If the apex angle of the rhombus of all irradiation spots P is 20, and the length of the shorter diagonal is 2, even in the case of Figure 1' where the scanning direction is tilted by θ, the adjacent barcode will not enter the irradiation spot. The state is guaranteed to exist, and no resolution loss occurs.

従ってこのθの値を人間が少し注意すれば走査方向のば
らつきは容易にこの範囲内に収まると云う範囲の端より
多小大きい角に設定すれば良く、θのおよその見当は1
00以上で20°〜400の範囲が望ましく、手持ち式
では5°以下では実効が殆んどない。また照射スポット
の幅はバーコードの最小幅0.24mm以下であること
が望ましいが、多少大きくてもよく、0.3 m m位
でも充分である。
Therefore, the value of θ can be set to an angle that is slightly larger than the end of the range, so that if a person is a little careful, the variation in the scanning direction can be easily settled within this range, and the rough estimate of θ is 1.
00 or higher and preferably in the range of 20° to 400°, and in a hand-held type, it is hardly effective at 5° or less. Further, the width of the irradiation spot is desirably equal to or less than the minimum width of the barcode, 0.24 mm, but it may be slightly larger, and about 0.3 mm is sufficient.

へ 実施例 第2図は本発明の一芙誰例を示す。1は光源の発光々°
イオード、2は光源1からの光を被走査面上に収束させ
るレンズ、3は光ビームを振らせる走査手段のポリゴン
ミラーでFが被走査面であり、4は被走査面からの反射
光を受光する受光素子である。5はバーコードリー々゛
の握り部内1こ収納さ跡 れた電気回録であり、6はポリゴンミラー3を回転させ
るモータである6図で光ビームLの走査方向は図の紙面
]ζ垂直であり、光ビームβの被走査面F上の照射スポ
ットは図の紙面1こ平行の方向1ζ長い菱形状になって
いる。
EXAMPLE FIG. 2 shows one example of the present invention. 1 is the light emission of the light source
2 is a lens that converges the light from the light source 1 onto the surface to be scanned, 3 is a polygon mirror of the scanning means that swings the light beam, F is the surface to be scanned, and 4 is the lens that converges the light from the surface to be scanned. It is a light receiving element that receives light. 5 is an electrical recorder stored in the grip of the barcode reader, and 6 is a motor that rotates the polygon mirror 3. In Figure 6, the scanning direction of the light beam L is perpendicular to the plane of the figure. The irradiation spot of the light beam β on the scanned surface F has a rhombic shape that is 1ζ long in the direction parallel to the plane of the drawing.

第3図は上記実施例で用いられている光源1の発光々°
イオードを示す。nはN型L pはP型層で発光はP−
N接合部で行われ、P型層を通して光が取出される。P
型層の表面には遮光膜Sが形成され、遮光膜に菱形の開
口Aが設けられていて、この開口が光学上の光源になっ
ており、レンズ2゜ポリゴンミラー3によってこの開口
の像が被走査面F上に形成される。
Figure 3 shows the light emission of the light source 1 used in the above embodiment.
Indicates an iode. n is N type L p is P type layer and the light emission is P-
This is done at the N-junction and the light is extracted through the P-type layer. P
A light-shielding film S is formed on the surface of the mold layer, and a diamond-shaped aperture A is provided in the light-shielding film, and this aperture serves as an optical light source. It is formed on the scanned surface F.

ト 効果 本発明バーコードリーダは上述したようす構成で、光ビ
ームの照射スポットを走査方向と直角の方向に長い菱形
としたから、照射面債が広くできて充分な照射光量が得
易く、しかも走査方向がバーコードのバーに対して直交
よりも多少類いても分解能が低下せず、信号処理が容易
かつ信頼性が高くなる。具体的にはバーコード読取り信
号のSZN比が向上し、バーコードの黒と白の部分の信
号レベル差が大となりかつ黒白の境界の立とり立下りが
急峻になって、信号処理が容易になる。また充分な照明
光量が得易いので、光源の選択自由度が増し、安価、小
型なバーコードリーダの設計が可能となる。
G. Effect Since the barcode reader of the present invention has the above-described configuration, and the irradiation spot of the light beam is long in the shape of a rhombus in the direction perpendicular to the scanning direction, the irradiation surface area can be widened, making it easy to obtain a sufficient amount of irradiation light. Even if the direction is more or less similar to the bar of the bar code than perpendicular to it, the resolution does not deteriorate, and signal processing becomes easier and more reliable. Specifically, the SZN ratio of the barcode reading signal is improved, the signal level difference between the black and white portions of the barcode becomes large, and the falling edge of the boundary between black and white becomes steeper, making signal processing easier. Become. Furthermore, since it is easy to obtain a sufficient amount of illumination light, the degree of freedom in selecting a light source increases, and it becomes possible to design an inexpensive and compact barcode reader.

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

第1図は本発明の詳細な説明する図、第2図は本発明の
−*社例のバーコードリーダの縦断側面図、第3図は同
実施例で使用される光源の発光ダイオードの要部拡大斜
視□□□、第4図は従来例の問題点を説明する図である
。 代理人 弁理士  昧    浩  介第1rM
Fig. 1 is a diagram explaining the present invention in detail, Fig. 2 is a longitudinal cross-sectional side view of a barcode reader of the -* company example of the present invention, and Fig. 3 is a diagram showing the main components of the light emitting diode of the light source used in the same embodiment. FIG. 4, an enlarged perspective view of a portion □□□, is a diagram illustrating the problems of the conventional example. Agent: Patent Attorney Kosuke Mai 1st RM

Claims (1)

【特許請求の範囲】[Claims] 光源と光ビームを被走査面上に収束せるレンズと光ビー
ムを振らせる光ビーム走査手段を有し、光ビームの被走
査面上における照射スポットを走査方向と直交する方向
に長い菱形状にしたことを特徴とするバーコードリーダ
It has a light source, a lens that focuses the light beam on the surface to be scanned, and a light beam scanning means that swings the light beam, and the irradiation spot of the light beam on the surface to be scanned has a long diamond shape in the direction orthogonal to the scanning direction. A barcode reader characterized by:
JP59234362A 1984-11-06 1984-11-06 Bar code reader Pending JPS61112289A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59234362A JPS61112289A (en) 1984-11-06 1984-11-06 Bar code reader

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59234362A JPS61112289A (en) 1984-11-06 1984-11-06 Bar code reader

Publications (1)

Publication Number Publication Date
JPS61112289A true JPS61112289A (en) 1986-05-30

Family

ID=16969813

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59234362A Pending JPS61112289A (en) 1984-11-06 1984-11-06 Bar code reader

Country Status (1)

Country Link
JP (1) JPS61112289A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63170613A (en) * 1986-12-22 1988-07-14 シンボル テクノロジイズ インコーポレイテッド Scan pattern generator for bar code symbol reader

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63170613A (en) * 1986-12-22 1988-07-14 シンボル テクノロジイズ インコーポレイテッド Scan pattern generator for bar code symbol reader
JPH0565851B2 (en) * 1986-12-22 1993-09-20 Symbol Technologies Inc

Similar Documents

Publication Publication Date Title
US4408120A (en) Bar code scanner
JPS61112289A (en) Bar code reader
JPH0193871A (en) Bar code reader
JPH0328712B2 (en)
JP2848477B2 (en) Optical reader
CA2169865C (en) Optical reflection sensing arrangement for scanning devices
JPH05323481A (en) Optical collector
JPS62199073A (en) Light emitting diode array
JP3996296B2 (en) Optical system and optical apparatus
JPH02291086A (en) Image reader
JPH11328298A (en) Code reader
JPS61201379A (en) Bar code reader
JPH0320951B2 (en)
JPS6455918U (en)
JPH0736603B2 (en) Image reader
JP2003195209A (en) Image exposure device
JPH0373189B2 (en)
JPH0591245A (en) Image sensor
JP3800756B2 (en) Optical information reader
JPS58124366A (en) Optical device for picture reading
JPH041511U (en)
JPH01245759A (en) Contact type image sensor
JPH08116407A (en) Image scanner
JPH1115913A (en) Bar code reader
JPH08220457A (en) Optical scanner