JP3422720B2 - Laser module and optical scanning device having the same - Google Patents

Description

Detailed Description of the Invention

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention is used in, for example, a POS system, and is applied to an optical scanning device including a bar code reader installed in a counter of a store and reading a bar code attached to a product. Regarding modules. The present invention also relates to the optical scanning device as described above.

[0002] In recent years, in POS systems and physical distribution management, it is widely practiced to read a bar code attached to an article using a bar code reader and perform settlement processing and management of the article.

In such a bar code reader, a light beam such as a laser beam is emitted toward the bar code, the bar code surface is scanned, and the laser beam reflected by the bar code is detected to detect the bar code. We are reading.

[0004]

2. Description of the Related Art FIG. 62 is a drawing showing a conventional bar code reader, and in particular, is a transparent drawing so that the internal structure can be seen. A bar code reader uses a laser light source such as a semiconductor laser as a light source. In the figure, 201 is a laser module, which is constituted by a laser light source, a lens, and the like. A polygon mirror 202 is a polygonal mirror having a plurality of reflecting surfaces. The polygon mirror 202 is rotationally driven by a motor. The laser light emitted from the laser module 201 is reflected by a small plane mirror provided at the center of the concave mirror 203 and reaches the reflecting surface of the polygon mirror 202. The laser light is reflected by the reflecting surface of the polygon mirror 20, but since the polygon mirror 202 is driven to rotate, the laser light is scanned, for example, clockwise in the drawing.

Reference numeral 204 denotes a scanning line dividing mirror, on which the laser beam scanned by the polygon mirror 20 is incident. The laser light is reflected downward by the scanning line splitting mirror 204, upwardly reflected by the substantially V-shaped bottom mirror 205, and then emitted from the reading window 206.

The laser light emitted from the reading window 206 scans the article 207 passing on the bar code reader. The laser light that scans the article 207 is reflected by the barcode surface or the like and enters the barcode reader through the reading window 206.

Reflected light from the bar code incident on the bar code reader is reflected by the bottom mirror 205 and the scanning line division mirror 2.
04, it is reflected by the polygon mirror 202 and enters the concave mirror 203. The concave mirror 203 focuses the laser light diffused and reflected from the barcode toward the photodetector 208. The laser light received by the photodetector 208 is demodulated by a demodulation circuit provided in the barcode reader or the like and output to an external device.

The bar code reader shown in FIG. 62 has a reading window 206 on one side. When installing such a bar code reader on the checkout counter, there are a method of installing so that the reading window surface is flush with the counter surface, and a method of installing so that the reading window is almost vertical on the counter. Can be roughly divided into

[0009]

As described above, the bar code reader installed in the checkout counter has only one reading window.

On the other hand, in order to read the bar code, the article is passed over the bar code reader, but if the bar code is not oriented in the direction of the reading window, the bar code cannot be scanned by the scanning light. There is a problem that the barcode cannot be read.

This is because in the conventional bar code reader, the scanning range of the scanning light or the emitting direction of the scanning light is limited.

In order to solve such a problem, conventionally, a plurality of reading windows are provided, and scanning light is emitted from each reading window so that an article with a bar code can be scanned from a plurality of different directions. Bar code readers that have been devised have been devised.

FIGS. 63 and 64 show an example of the appearance of a bar code reader having such measures.

In these bar code readers, a reading window 206a is provided on the bottom surface of the device, and the bottom reading window 206a is provided.
It has a side reading window 206b which is set up at an angle almost vertical to a.

Scanning light is emitted from the lower reading window 206a in the direction toward the upper side reading window 206b.

On the other hand, scanning light is emitted from the side reading window 206b in a substantially horizontal direction (toward the operator).

As described above, a plurality of reading windows are provided, and the scanning light is emitted from the respective reading windows in a plurality of directions. Therefore, the article passing through the bar code reader is irradiated with the scanning light from a plurality of directions. As compared with a barcode reader having a single reading window, the barcode is more likely to be scanned.

FIG. 65 shows a checkout counter (checkout counter) in which such a bar code reader is installed. Checkout counter 211
A barcode reader 200 is installed on the top.
The operator uses the side reading window (side window 20 in the figure).
Stand at a position facing 6b).

On the upper side of the side window 206b, a keyboard 212 for inputting information about products without bar codes is attached. Also,
A conveyor 213 is provided upstream of the checkout counter and conveys a product to the position of the barcode reader 200.

A POS terminal 214 is provided next to the operator, and the settlement process is performed by the POS terminal 214.

The bar code reading range when the bar code readers of FIGS. 63 and 64 are used is shown in FIG.

Here, in the shaded area, the scanning light emitted from the side window 206b and the bottom window 206a (bottom reading window) is gathered, and even if the bar code is rotated 360 degrees in the horizontal direction. The area where the barcode can be read is shown.

As described above, since the scanning light is emitted from each of the two reading windows, the range in which the barcode can be read is widened, and even if the barcode surface does not completely face one of the reading windows. The barcode can be read.

In such a bar code reader, a single light source is used, the emitted light beams are divided, and scanning light emitted from each reading window is generated from these divided light beams. There is.

In this case, the desired reading performance cannot be achieved unless the laser light source, the means for splitting the light, or the focusing means such as a lens for focusing the laser beam are properly aligned. Occurs.

Further, the laser beam emitted from the semiconductor laser has a characteristic that the divergence angles of the beam differ between the vertical axis direction and the horizontal axis direction. Further, such a laser beam has a characteristic that the image forming position in the vertical axis direction is also different from the image forming position in the horizontal axis direction. Since such characteristics cause a problem that the reading performance and the light ray utilization efficiency are lowered particularly in a device such as a bar code reader, it is necessary to take some measures.

It is an object of the present invention to realize a laser module equipped with a laser light source and an optical scanning device equipped with the same, which solves the above problems.

[0028]

In order to solve the above-mentioned problems of the laser module using the conventional semiconductor laser, the present invention collects a semiconductor laser light source and a laser beam emitted from the laser light source. A condensing unit that emits light, a unit that converts a beam diameter corresponding to one axis of the orthogonal axes of the laser beam emitted from the converging unit, and a dividing unit that divides the laser beam emitted from the converting unit. The laser module equipped with it has been realized.

In the laser module, the splitting means is a half mirror.

Alternatively, the laser module is a prism having an apex angle corresponding to the beam diameter to be converted by the converting means, and the beam diameter is converted by refracting the beam incident on the prism in a predetermined direction.

Similarly, in the laser module, the conversion means is a cylindrical lens. For example, the cylindrical lens is a concave cylindrical lens and a convex cylindrical lens, or a double-sided cylindrical lens having a concave surface on one side and a convex surface on the other side. Can be

The present invention also realizes a laser module in which the converging means can be adjusted such that the axis of the converging means is inclined by a predetermined angle with respect to the optical axis of the laser beam emitted from the laser light source. Further, the light condensing means is mounted in the block, which can be moved in the direction along the optical axis in the laser module, tilted with respect to the optical axis of the laser light.

[0033]

1 is a perspective view of the external appearance of a bar code reader according to an embodiment of the present invention. Hereinafter, a barcode reader according to an embodiment of the present invention will be described with reference to the drawings.

The bar code reader according to the present embodiment is provided with a light source such as a semiconductor laser inside thereof, emits scanning light from the reading window to scan the bar code, and receives reflected light from the bar code. The barcode is read.

The bar code reader 1 according to the present embodiment is
The side scanner unit 2 and the bottom scanner unit 3 can be roughly divided into two parts. Side scanner unit 2
Has a reading window called a side window 4. The scanning light from the side scanner unit 2 is emitted from the side window 4 in a substantially horizontal direction and scans a product passing over the barcode reader 1.

On the other hand, the bottom window section 3 has a reading window called a bottom window 5. The scanning light emitted from the bottom window 5 is emitted upward. In order to scan the scanning light from different directions of the bar coded article, the scanning light emitted from the bottom window 5 is slightly inclined in the direction of the side window and is emitted, so that the products passing over the bar code 1 can be detected. To scan.

The side scanner section 2 and the bottom scanner section 3 which compose the bar code reader 1 are each provided with an optical system for generating scanning light. The details of the configuration of each optical system will be described later.

In the figure, 6 is a DIP switch, which is used to set various operations of the bar code reader 1. A restart switch 7 is used to reset the operation of the barcode reader 1. Although not shown in FIG. 1,
The bar code reader is provided with a display device such as an LED for notifying the operator of whether or not the bar code can be read, or a speaker that emits a notification sound.

Further, the surface of the bar code reader 1 according to this embodiment on which the bottom window 5 is provided is a scale, and the weight of the product can be measured by placing the product at this position. When the price of the product corresponds to the product weight, the individual product price can be determined by measuring the weight of the product.

FIG. 2 shows that the bar code reader according to the present embodiment is used as a checkout counter (checkout counter) of a store.
It is shown in the state installed in. The barcode reader 1 is installed on the settlement counter 11 so that the counter surface 12 of the settlement counter 11 and the upper surface 13 of the barcode reader 1 provided with the bottom window 5 are flush with each other. Therefore, the lower part of the barcode reader 1 is embedded in the settlement counter 11.

The operator stands at a position facing the side scanner section 2 of the settlement counter 11 and passes the article with the bar code on the barcode reader 1 to scan the article with the scanning light, thereby converting the article into the article. Read the attached barcode.

Since the settlement counter surface 12 and the bottom window surface 13 are flush with each other, the operator passes the commodity through the barcode reader and reads the barcode while keeping the operator in contact with the settlement counter surface. You can also

FIG. 3 is a side sectional view of the bar code reader of this embodiment, showing the arrangement of internal optical systems and the path of light emitted from the laser light source.

In the figure, 21 is a VLD module. The VLD module 21 is a light source that generates scanning light and includes a semiconductor laser. In the case of FIG. 3, VL
The D module 21 is attached in the vicinity of the lower surface on the right side in the figure, at a position farthest from the side scanner unit, and emits laser light toward the left side in the figure.

The bar code reader according to the present embodiment has one light source, but since it has two reading windows,
The laser light emitted from the VLD module 21 is divided on the way, and scanning light emitted from each reading window is generated. A half mirror 22 reflects a part of the laser light emitted from the VLD module 21 and allows a part of the laser light to pass therethrough, thereby dividing the laser light into two.

Reference numerals 23 and 24 are reflection mirrors, which reflect the laser light reflected by the half mirror 22 and introduce the laser light into a polygon mirror 25 described later. A small square mirror is used as the reflecting mirror.

Reference numeral 25 denotes a polygon mirror, which has a plurality of reflecting surfaces, in the case of the present embodiment, four reflecting surfaces. The polygon mirror 25 is attached to a Borgon motor and is rotationally driven by the polygon motor. On the reflecting surface of the polygon mirror 25, the laser light transmitted through the half mirror 22 or the laser light reflected by the half mirror 22 and the reflection mirrors 23 and 24 enters the polygon mirror 25 from different directions. Since the polygon mirror 25 is rotationally driven as described above, each laser beam reflected by the reflecting surface of the polygon mirror 25 is scanned in an arc.

The reflecting surface of the polygon mirror 25 is inclined at a predetermined angle, and the laser light reflected by the reflecting surface is reflected at a predetermined angle. In addition, the inclination angles of the reflecting surfaces are set to be different from each other. The angle of the reflecting surface of the polygon mirror 25 need not be different for all reflecting surfaces.

Reference numeral 26 is a mirror system A, and 27 is a mirror system B. Each mirror system is composed of a combination of a plurality of mirrors. Each mirror system is a polygon mirror 2
The scanning light scanned by 5 is divided into a plurality of scanning lines to increase the number of scanning lines emitted from the reading window. Further, the directions and inclinations of the reflecting surfaces of the mirrors constituting each mirror system are set so that the scanning directions (angles) of the scanning lines emitted from the reading window are various directions.

The scanning light reflected by the reflecting surface of the polygon mirror 25 after passing through the half mirror 22 enters the mirror system A26, and this scanning light is applied to the bottom window 5.
Is reflected so as to be emitted almost upward from. On the other hand, the mirror system B27 is a half mirror 22 and a reflection mirror 2.
The scanning light reflected by the reflecting surface of the polygon mirror 25 after being reflected by the mirrors 3 and 24 enters, and is reflected so that the scanning light is emitted from the side window 4 in a substantially horizontal direction.

As described above, the scanning light emitted from the side window 4 and the bottom window 5 is applied to the article passing on the barcode reader 1 to scan the barcode surface. The scanning light that scans the barcode surface is reflected by the barcode surface and enters the barcode reader from the side window 4 or the bottom window 5. The reflected light from the bar code incident through each reading window reaches the polygon mirror 25 along the same path as the scanning light is emitted, and reaches the polygon mirror 25.
Is reflected by each of the reflecting surfaces.

Next, the incident path of the reflected light from the bar code to the bar code reader 1 will be described. In FIG. 3, 28 is a detector B, which detects the reflected light from the bar code which is incident on the bar code reader through the bottom window 5. The light receiving surface of the detector B28 faces the right side in the figure, that is, the direction opposite to the side scanner unit. Further, 29 is the detector A, and the side window 4
The reflected light from the bar code incident on the bar code reader via the sensor is detected. The light receiving surface of the detector A29 is directed obliquely downward to the right in the drawing. These detectors 2
The reflected light from the bar code received by 8 and 29 is electrically processed into a binarized signal, demodulated by a demodulation circuit, and then output to an external device (for example, a POS terminal).

Here, 30 is a concave mirror, and the reflected light from the bar code incident from the bottom window 5 reflected by the reflecting surface of the polygon mirror 25 is detected by the detector B.
The light is focused on the light receiving surface 28. Since the reflected light reflected by the barcode surface is scattered light, the reflected light entering the barcode reader also has a certain spread. Therefore, the light amount of the reflected light reaching the light receiving surface of the detector becomes small as it is, and it is not possible to obtain a sufficient light amount for reading the barcode. Therefore, in the bar code reader of FIG. 3, the concave mirror 30 is used to increase the amount of reflected light received by the detector B28.

The concave mirror 30 reflects the reflected light from the bar code which is incident from the left side in the figure toward the left side in the figure, and thereby returns the reflected light. Further, a through hole 31 is provided at the center of the concave mirror 30,
The laser light emitted from the VLD module 21 passes through the through hole 31 and enters the polygon mirror 25.

As described above, the reflected light from the bar code is
The scanning light is incident on the detector through the same path as the exiting path. Therefore, in order to most efficiently read the barcode, the light emitted from the VLD module 21
The optical axes of the reflected light incident on the detector B28 need to coincide with each other. Therefore, the concave mirror must be arranged on the optical axis of the laser light emitted from the VLD module 21, but it should not block the optical axis of the emitted light. Therefore, a through hole 31 is provided at the center of the concave mirror 30 shown in FIG.

Reference numeral 32 is a Fresnel lens, which collects the reflected light from the bar code incident from the side window 4. This action is the same as that of the concave mirror 30 described above. The reflection mirror 24 is arranged on the front surface of the Fresnel lens 32, and the optical axis of the emitted light reflected by the reflection mirror 24 and the optical axis of the reflected light from the bar code incident on the Fresnel lens 32 also match. However, as described above, since the reflected light from the barcode has a spread, only a part of the light incident on the Fresnel lens 32 is reflected.
Most of the reflected light from the bar code enters the Fresnel lens 32.

The Fresnel lens 32 is the polygon mirror 2
It is arranged so as to be tilted according to the incident angle of the reflected light from No. 5. The reflected light collected by the Fresnel lens 32 is reflected upward by the C mirror 33 provided on the bottom surface of the barcode reader, and reaches the light receiving surface of the detector A29 facing downward.

Here, the mirror system A26, the concave mirror 30, and the detector B28 constitute a bottom scanner unit, and the reflection mirror 2
The 3/24, the optical system B27, the Fresnel lens 32, the mirror C33, and the detector A29 constitute a side scanner unit.
The VLD module 21, the half mirror 22, and the polygon mirror 25 are shared by the bottom scanner section and the side scanner section.

In the bar code reader according to this embodiment, a printed board 34 is further provided on the bottom surface of the bar code reader 1. On the printed circuit board 34, for example, a circuit for controlling the lighting of the laser, a circuit for controlling the operation of the detector, a circuit for controlling the rotating operation of the polygon motor, and the demodulation of the barcode based on the reflected light detected by the detector. It is equipped with a demodulation circuit and so on. On the printed circuit board 34,
A connector for connecting to an external device is provided, and a cable (I / F cable 35 in the figure) is connected,
The demodulated barcode data is output.

FIG. 4 shows a state in which the scanning light emitted from the bar code reader scans the bar code surface. As shown in FIG. 4, scanning light is emitted from the side window 4 in a substantially horizontal direction (or slightly upward). On the other hand, the light is emitted obliquely upward from the bottom window 5. Since the light emitted from the bottom window 5 is slightly inclined and emitted to the side window 4 side, the scanning light emitted from both the side window 4 and the bottom window 5 is collected in the portion a of FIG. Therefore, by passing the article with the bar code attached to this position, the scanning light emitted from each reading window can scan the article simultaneously (or in time division) from different directions of the article.

Therefore, even if the bar code does not face one of the reading windows, there is a high possibility that the scanning light emitted from the other reading window is applied to the bar code surface, and the bar code reading probability is increased. It becomes possible.

The scanning light for scanning the bar code surface is reflected by the bar code surface, but this reflected light is scattered as shown in FIG. Therefore, like the position of b in the figure,
Even if the bar code is oriented almost vertically to the bar code reader in the direction opposite to the side window 4, part of the reflected light from the bar code (shown by d) reaches the bottom window 5. . Especially the bottom window 5
Since the scanning light emitted from is emitted obliquely upward, when the barcode in the state as shown in FIG. 2B is scanned, the reflected light from the barcode is displayed on the reading window (bottom window 5). The probability of incidence is high.

Thus, since the scanning light scans the bar code surface from various directions of the article passing over the bar code reader, the bar code surface does not face any reading window as shown in FIG. As long as there is no barcode at a position where scanning light is not emitted at all, it is possible to read the barcode.

FIG. 5 is a view showing the outer dimensions of the bar code reader according to the present embodiment. The barcode reader according to the present embodiment has a width of about 292 mm and a height of about 24.
It is 7 mm. The depth of the barcode reader is approximately 508 mm (or 430 mm), and the height from the bottom surface to the counter surface is approximately 120 mm. The depth of the bar code reader may be set according to the width of the checkout counter or the like in which the bar code reader is installed.

FIG. 6 is a diagram showing a diagram of an optical system of the bar code reader according to the present embodiment. In the figure, the arrow indicates the path of the light beam, and the direction of the arrow indicates the emission direction of the light beam. In FIG. 6, the internal configuration of the bar code reader 1 is divided into a side scanner unit 2 and a bottom scanner unit 3 and drawn. In addition, the VLD module (VLD-ASSY in the drawing) 21 is actually shared, but it is illustrated separately in FIG. 6 for convenience. In addition, the VLD-ASSY 21 of the side scanner unit 2 includes a half mirror.

In the bottom scanner section 3, the laser light emitted from the VLD module 21 enters a polygon mirror 25 (Polygon ASSY in the figure) and is reflected by the reflecting surface of the polygon mirror 25. After that, the light is reflected by the mirror system A26 (Mirror-ASSY in the figure), and the bottom window 5 (Window-AS in the figure).
The barcode is illuminated via SY). The bottom window 5 is composed of two glass plates and is sealed so as to prevent water or the like from entering the inside of the barcode reader.

Here, as the glass, a hard glass such as sapphire glass is used, but the surface of the glass may be scratched or soiled by contact with a product, and the amount of transmitted laser light may decrease. There is. Therefore, two window glasses are used for the bottom window 5, and the lower glass that has no possibility of coming into contact with the product is fixed to the device, and the upper one that has a very high possibility of coming into contact with the product. Can be replaced if necessary. This makes it possible to replace the damaged window glass and prevent the bar code reading performance from deteriorating due to a decrease in the amount of laser light that passes through the bottom window 5. The lower glass, which is less likely to come into contact with the product, is less likely to be scratched on the surface than the upper glass. Therefore, for the lower glass, it is not necessary to use hard but expensive glass such as sapphire glass.

Further, as will be described in detail later, the bottom scanner section 3 irradiates a scanning pattern composed of four scanning lines in one direction in a total of 10 directions. This scanning pattern in 10 directions is emitted every one rotation of the polygon mirror 25, and the barcode is scanned by a total of 40 scanning lines. The four scanning lines forming each scanning pattern correspond to the reflecting surfaces of the polygon mirror 25, respectively.

The reflected light from the bar code enters the mirror system A 26 through the bottom window 5 and is reflected toward the polygon mirror 25. After this, the polygon mirror 25
By the reflective surface of, the reflected light from the barcode is reflected,
The concave mirror 30 detects the detector B28 (pin (PIN) in the figure).
The light is condensed and reflected toward the photodiode.

On the other hand, regarding the side scanner section 2, V
The laser light emitted from the LD module 21 and reflected by the half mirror is reflected by the reflection mirror (B mirror group 23 in the drawing) and introduced into the polygon mirror 25. The scanning light reflected by the reflecting surface of the polygon mirror 25 is reflected by the mirror system B27 (Mirror-ASSY in the figure), and the side window 4 (Window in the figure).
-ASSY) and the barcode is scanned.
The side window 4 is 2 as well as the bottom window 5.
It is composed of a sheet of glass. In the case of the side window 4, since it is rare to read the bar code by bringing the product into contact with the side window 4, from the hard gas side window 4, four scanning patterns in each direction are provided in six directions. A total of 24 scanning lines are emitted toward. The details will be described later.

The reflected light of the bar code enters the bar code reader 1 through the side window 4 and enters the mirror system B.
27, after being reflected by the reflecting surface of the polygon mirror 25, it is condensed by the Fresnel lens 32. Then, the light is reflected by the bottom mirror 33 (C mirror) and received by the detector A29. The Fresnel lens + bottom mirror may be replaced with a concave mirror having a light condensing function.

In the figure, the "ambient light sensor 36" detects a change in the amount of light around the bar code reader, and based on the result, controls the operation of the bar code reader, particularly controls the lighting of the VLD module. It is a thing.

Next, a more detailed arrangement of the optical system of the bar code reader according to the embodiment of the present invention will be described.

FIG. 7 is a view showing a state in which the cover on the lower surface of the bar code reader is removed. Further, in FIG. 7, the upper cover (where the bottom window is provided) of FIG. 1 is also removed. Here, the bottom glass refers to the glass located on the lower side of the two window glasses. 8 is a side view and a top view of the barcode reader shown in FIG.

In the figure, the mirror forming the bottom scanner unit 3 is provided inside the drawing 3, and the mirror forming the side scanner unit 2 is provided inside the drawing 2.
Further, the lower frame 41 and the upper frame 42 are C in the figure.
It is divided up and down at the position. Mirrors forming the bottom scanner unit 3 are attached to the inner wall surfaces of the lower frame 41 and the upper frame 42. Further, the cover portion 43 provided with the side window 4 is divided from the bar code reader lower frame 41 at a position D in the drawing, and a mirror frame to which a mirror forming a part of the mirror system B27 is attached inside thereof. 44 is attached.

FIG. 9 is a view showing an example of the apparatus lower frame 41 in a state where the bar code reader is vertically divided at the position C in FIG. The cover part 43 of the side scanner is also removed in FIG.

A polygon mirror is arranged substantially in the center of the lower frame 41 of the bar code reader. Although FIG. 9 shows the table 51 on which the polygon mirror is installed, the polygon mirror itself is omitted. On the lower surface of the base 51, a gap 52 for passing the laser light traveling from the reflection mirror 23 to the reflection mirror 24.
Is provided. Further, a total of nine mirrors constituting the mirror system A26 or the mirror system B27 are attached to the lower frame 41. Of these, ZB2,
VBRR, VBLL, HBR2, HBL2, ZML2,
ZMR2 is a mirror that constitutes the mirror system A26. On the other hand, VSR1 and VSL1 respectively form a part of the mirror system B27.

The mirrors ZMR2 and ZML2 are attached to the side surface of the lower frame 41, and are provided along the longitudinal direction of the bar code reader. The mirror ZB2 is arranged so that its reflection surface faces upward. The angle of the reflecting surface of ZB2 can be adjusted appropriately. Mirror v
The BRRs and VBLLs are arranged on the surface of the lower frame 41 farthest from the side scanner unit, with the reflecting surface tilted slightly obliquely upward in the direction facing the polygon mirror.

On the other hand, the mirrors VSR1 and VSL1 are attached to the side surfaces of the lower frame 41, with their reflecting surfaces facing slightly obliquely upward.

Reference numeral 53 is a printed board on which the detector A29 is attached. As shown in the figure, the printed circuit board 53 is attached to the device lower frame 41 so that the light receiving surface of the detector A29 faces obliquely downward. With such an arrangement, the depth of the device can be shortened.

Further, a Fresnel lens 32 installed at an angle is attached between the printed circuit board 53 and the polygon mirror. Further, a reflection mirror 24 is provided on the optical axis in front of the Fresnel lens 32.

On the other hand, a VLD module is housed on the lower surface of the mirror ZB2, and laser light is emitted from this position. Further, a reflection mirror 23 is attached to the rear side (left side in the drawing) of the mirror ZB2, and the laser light passing through the gap between the mirror ZB2 and the lower frame 41 is
It reflects toward the reflection mirror.

Further, the detector B is embedded in the lower surface of the device at the position A in the figure. The light receiving surface of the detector B faces the left side in the drawing, and an opening 54 for guiding the laser light reflected by the concave mirror to the detector B is provided on the front side of the light receiving surface of the detector B. The opening 54 is formed in a V shape according to the optical path on which the reflected light is condensed by the concave mirror. Further, the detector B is attached to the printed circuit board (shown in b).

FIG. 10 is a view showing a state in which the lower frame is viewed from the upper surface. Similarly, FIG. 11 is a side sectional view of the lower frame.

As shown in FIG. 10 or FIG. 11, the polygon mirror 25 is provided in the lower frame 41 at a position slightly closer to the center than the side scanner section. Further, a bottom surface mirror 33 is installed behind the Fresnel lens 32 with its reflecting surface facing slightly upward. On the other hand, a detector B28 is attached to the bottom surface of the lower frame 41. The detector B28 is attached to the printed circuit board b. In addition, on the light receiving surface side of the detector B28, approximately V
An opening 54 formed in a V shape is provided, and reflected light from the concave mirror 30 passes through the opening 54 and a detector B28.
Incident on.

Further, the VLD module 21, the reflection mirrors 23 and 24, the Fresnel lens 32, and the polygon mirror 2
5, the detector A29, the detector B28, and the concave mirror 30 are arranged on the center line of the lower frame 41, and the optical axes of the respective light rays are aligned with each other. The VLD module 21 and the concave mirror 30 are arranged on the lower surface of the mirror ZB2. A part of the mirror ZB2 is cut out in FIG. 10 so that the arrangement of the VLD module 21 can be easily understood.

As shown in the side sectional view of the lower frame in FIG. 11, since the detector B28 is on the bottom surface of the lower frame 41, it does not block the optical path of the emitted light, the reflected light from the bar code, or the like. The mirror ZB2 is attached slightly upward in the drawing. The reflection mirrors 23 and 24 are attached to the ends of the elongated frame so as not to obstruct the passage of light rays as much as possible.

Further, the bottom surface and the side surface of each mirror are provided with an abutting portion (c in the figure) for defining the mirror position and angle. When attaching the mirror to the lower frame, the mirror is abutted and fixed to this abutting portion. As a result, each mirror is attached to the lower frame 41 at a predetermined orientation and angle.

FIG. 12 shows the upper frame of the apparatus, and the lower frame is also shown. Each mirror is attached inside the top frame 42.
The upper frame 42 includes ZBR1, ZBL1, HBR1,
HBL1, VBR1, VBL1, VBR2, VBR2,
A total of 10 mirrors of ZMR1 and ZMR2 are provided. Each of these mirrors constitutes a part of the mirror system A26. The reflecting surface of each of the mirrors is located slightly obliquely downward, toward the respective mirrors constituting the bottom scanner unit attached to the lower frame.

FIG. 13 shows the cover portion 43 of the side scanner.
It is a four-sided view of the mirror frame 44 attached inside. Inside the mirror frame, ZHR, ZHL, ZR
R, ZLL, VSR2, VSL2, ZR, ZL total 8
A sheet of mirror is attached. These eight mirrors form a part of the mirror system B27. In the side view of FIG. 13, the left side in the drawing corresponds to the operator standing position side or the side window side. Of the eight mirrors, the reflecting surfaces of the mirrors ZR and ZL are directed obliquely upward, and the reflecting surfaces of the remaining six mirrors are directed slightly downward. Furthermore, the reflecting surfaces of the six mirrors other than ZR and ZL are directed slightly inward with respect to each other.

FIG. 14 is a diagram showing the shapes of the upper six mirrors of the mirrors attached to the mirror frame 44 and the rough attachment positions. These six mirrors are attached to the attachment surface provided inside the mirror frame 44 using an adhesive or the like.

FIG. 15 is a side sectional view of the bar code reader with the lower frame 41, the upper frame 42, the cover 43 and the mirror frame 44 assembled together. Figure 15
As shown in FIG. 6, the mirror attached to the upper frame 42 has its reflection surface facing slightly downward, and the reflected light from the mirror attached to the upper frame is incident on the mirror attached to the lower frame 41. . Also,
Mirrors ZR and ZL attached to the mirror frame 44
The positions of the reflecting surfaces of the mirrors VSR1 and VSL1 attached to the lower frame 41 are located at substantially the same height.

In FIG. 15, the detector A29 is arranged so that its light-receiving surface faces downward, and the printed circuit board is also arranged so as to be substantially perpendicular to the bar code reader in accordance with it. By taking such an arrangement,
The depth of the device can be reduced as compared with the case where the printed circuit board is arranged horizontally. In addition, the detector A29
The Fresnel lens 32 for introducing the reflected light from the barcode to the detector A29 and the bottom mirror 33 are provided at positions not blocking the path of the scanning light reflected from the polygon mirror 25 toward the mirrors VSL1 and ZL. There is.

FIG. 16 is a drawing showing the outline of the path of the scanning light emitted from the reading window of the bottom scanner section 3, and FIG. 17 is a drawing showing the outline of the path of the scanning light.

In the case of the bottom scanner unit 3, the laser light emitted from the VLD module 21 and reflected by the reflecting surface of the polygon mirror 25 is first ZBR, ZBL, HBR, HBL, VB attached to the upper frame 42.
R1, VBL1, VBR2, VBL2, ZMR1, ZM
Scan to L1. The scanning order is ZMR1, VBR2, V when the polygon mirror 25 is rotated clockwise.
BR1, HBR1, ZBR1, ZBL1, HBL1, V
The order is BL1, VBL2, ZML1.

Subsequently, the reflected light reflected by the mirror inside the upper frame 42 is emitted toward the mirror attached to the lower frame 41.

The scanning light reflected by ZMR1 is ZMR.
It is reflected upward by 2 and emitted from the bottom window 5 as a scanning pattern ZMR. VBR2 and V
The scanning light reflected by BR1 is reflected upward by VBRR and emitted from the bottom window 5 as scanning patterns VBL2 and VBL1. Scanning light incident on VBRR from VBR2, and VBR by VBR1
Since the incident position and angle of the scanning light incident on R are different, the scanning light is emitted from the bottom window 5 as scanning light having different directions and angles.

The scanning light reflected by the HBR is
It is reflected upward by the HBR 2 and the scanning pattern is emitted from the bottom window 5 as HBR. The scanning light reflected by ZBR1 is reflected upward by ZB2 and emitted from the bottom window 5 as a scanning pattern ZBR. ZBL1, HBL1, VBL1, VBL
The same applies to the case of 2 and ZML1. The scanning light of ZBL1 is reflected upward by ZB2 and emitted as a scanning pattern ZBL, and the scanning light of HBL1 is reflected upward by HBL2 to become a scanning pattern HBL. Also, VB
The scanning lights reflected by L1 and VBL2 are VB
The scanning pattern V is reflected upward by LL and is respectively scanned.
BL1 and VBL2. Subsequently, the scanning light reflected by ZML1 is reflected upward by ZML2 and emitted as a scanning pattern ZML, and one scanning cycle is completed.

Here, as also shown in FIG. 12, the scanning light reflected by the mirror ZML1 reaches the mirror ZML2 so as to cross the inside of the bottom scanner unit. Since a part of the scanning light traverses the bottom scanner in this manner, it is necessary to eliminate obstacles and provide a space that does not block the scanning light, especially in the bottom scanner.

Therefore, in the bar code reader according to the present embodiment, for example, as shown in FIG. 15, the VLD module 21, the concave mirror 30 and the like are moved to the left side in the drawing, and the detector B28 is attached to the bottom surface of the device. The polygon mirror 25 is also attached at a position where it does not block the space inside the bottom scanner unit.

Further, the mirror constituting the bottom scanner unit is composed of a lower frame 41 and an upper frame 4 which are divided into upper and lower parts.
2 is attached to the inner wall surface. Therefore, it is not necessary to provide a structure for arranging the mirror in the space of the bottom scanner section, and the arrangement of the mirror makes it possible to effectively use the space in the bottom scanner section.

On the other hand, in the side scanner unit 2, the scanning light reflected by the polygon mirror 25 first enters the VSR1 and VSL1 attached to the lower frame 41 and the ZR and ZL attached to the mirror frame 44. The order of scanning is VSL1, ZL, ZR, and VSR1.

The scanning light reflected by these mirrors is then reflected by the upper six mirrors mounted on the mirror frame 44. First, the scanning light reflected by VSL1 is reflected by VSL2 in a substantially horizontal direction, and the scanning pattern VS is emitted from the side window 4.
It is emitted as L. The scanning light reflected by ZL first enters the ZLL mirror and is emitted from the side window 4 as a scanning pattern ZLL. Then,
The scanning light reflected by ZL is reflected by ZHL and emitted from the side window 4 as a scanning pattern ZHL.

Subsequently, the scanning light reflected by ZR is first reflected by ZHR and emitted from the side window 4 as a scanning pattern ZHR. Next, the scanning light reflected by ZR is reflected by ZRR and emitted from side window 4 as scanning pattern ZRR.
The scanning light finally reflected by VSR1 is reflected by VSR2, and the scanning pattern V is emitted from the side window 4.
It is emitted as SL. This completes one scan cycle.

FIG. 18 is a diagram showing a scanning pattern emitted from the bottom window 5. As already mentioned, a total of 40 scanning lines are emitted from the bottom window 5. The 40 scanning lines are grouped into 10 groups every 4 lines.

FIG. 19 is a drawing showing a locus of the scanning pattern on the bottom window surface, which is drawn by representing one scanning line from the scanning pattern shown in FIG. The two scanning patterns ZMR and ZML are oriented in a direction substantially perpendicular to the operator and are arranged in the bottom window 5
Extends almost all over the longitudinal direction. for that reason,
The article to be read by the bar code, regardless of the position on the bottom window 5, passes at least the scanning pattern ZMR,
Scanned by ZML.

The remaining eight scanning patterns are scanned in a direction intersecting the scanning patterns ZMR and ZML with a slightly obliquely upward trajectory. By emitting the scanning pattern as shown in FIG. 18, even if the angle of the barcode passing through the barcode reader is different, the scanning lines constituting any of the scanning patterns can scan the barcode, The reading performance of the barcode can be improved.

Here, the reference numerals given to the respective scanning patterns correspond to the mirror names constituting the mirror system A26 and are reflected by the mirrors having the corresponding names.

Further, since the angles of the reflecting surfaces of the polygon mirror are different from each other, the scanning pattern corresponding to each reflecting surface emitted from the bottom window 5 has four scanning lines according to the reflecting surface angles of the polygon mirror. The lines are scanned substantially parallel and at positions separated by a predetermined distance. Thus, by configuring one scanning pattern with a plurality of scanning lines that are separated by a predetermined distance, it is possible to further increase the probability that the scanning lines scan the barcode, and further improve the barcode reading performance. be able to.

FIG. 20 is a drawing showing a scanning pattern emitted from the side window 4. From the side window 4, six scanning patterns (VS
R, VSL, ZRR, ZLL, ZHR, ZHL) are emitted. The names of these scanning patterns respectively correspond to the names of the mirrors that form the side scanner unit, and are scanning patterns generated by being reflected by the mirrors having the same names as in the case of FIG. As in the case of the scanning pattern emitted from the bottom window 5, the scanning positions of the four scanning lines in one scanning pattern are defined by the difference in the angle of each reflecting surface of the polygon mirror 25.

The scanning pattern shown in FIG. 20 is a pattern on the side window surface. However, since the mirrors attached to the mirror frame 44 face inward as described above, the scanning patterns are separated from the side window surface, respectively. Scanning patterns of the two approaches. Then, at the position most suitable for reading the barcode, the six scanning patterns are closest to each other, and the side pattern has the highest probability of scanning the barcode passing through the barcode reader.

The scanning pattern emitted from the bottom window 5 and the scanning pattern emitted from the side window 4 are arranged so as to be symmetrical with respect to the center line. Since both the bottom pattern and the side pattern are composed of scanning patterns of slightly different directions and angles, at least one of the scanning lines is irrespective of the inclination of the barcode passing over the barcode reader. It is very likely that the book will scan across the bar code.

FIG. 21 shows a scanning pattern (bottom pattern) emitted from the bottom window 5 and a scanning pattern (side pattern) emitted from the side window 4.
2 is a drawing showing only one side (left side) of the patterns. As described above, the left and right scanning patterns emitted from the respective reading windows are symmetrical with respect to the center line of the apparatus, and the right scanning pattern has a shape obtained by folding back the pattern shown in FIG. .

FIG. 21a shows scanning patterns VSL1 and VSL2 among the bottom patterns. V
SL1 draws a slightly upward-sloping scanning trajectory at a position close to the side window. On the other hand, VSL2 draws a position closer to the operator than VSL1, and a slightly upward-sloping scanning locus like VSL1.

FIG. 21b shows the scanning pattern ZML. ZML draws a locus that crosses substantially the longitudinal direction of the bottom window. Thereby, no matter which position on the bottom window 5 the article passes through, the article is scanned by at least the scanning pattern ZML.

FIG. 21c shows the scan patterns HBL and ZB.
It is the figure which showed L. The HBL is scanned at a position closer to the side scanner on the left side of the bottom window with a slightly upward scanning trace. On the other hand, ZBL is scanned at a position closer to the operator on the right side of the bottom window, with a slightly upward-sloping scanning trajectory.

FIG. 21d is a view showing a left side pattern among the scanning patterns emitted from the side window. The scanning pattern VSL extends in the vertical direction of the side window, and draws a scanning trajectory that slightly rises to the left.
Further, the scanning pattern ZLL draws a scanning locus that rises to the right. In addition, ZHL draws a slightly upward-sloping scanning trajectory on the upper side of the center of the side window.

By generating such a scanning pattern, the articles passing through the bar code reader can be
Every time the polygon mirror 25 makes one rotation, a total of 64 scanning lines are emitted from two directions. The greater the number of scanning lines that scan the article, and the more various scanning directions and angles are set, the higher the probability that the scanning line will pass through the barcode surface, and the barcode reading will succeed. The likelihood of doing so increases accordingly.

FIG. 22 is a drawing in which the locus of the laser light emitted from the VLD module 21 is drawn using the side sectional view of the bar code reader. Note that, in the case of the drawing, the mirrors attached to the upper frame 42 and the mirrors attached to the mirror frame 44 are not shown. The VLD module 21 includes a prism 61 that functions to change the emission angle of laser light and convert the beam diameter, and a half mirror 22 that divides the laser light into two.

After passing through the prism 61, the half mirror 22
The laser beam that has passed through is emitted in a slightly upward direction, passes through a through hole 31 provided in the central portion of the concave mirror 30, and enters the polygon mirror 25. Polygon mirror 2
The laser beam reflected by the bottom scanner unit 3
It is irradiated toward the mirror group constituting the.

On the other hand, the laser light reflected by the half mirror 22 enters the reflection mirror 23 through the gap between the mirror ZB2 and the lower frame 41, is reflected by the reflection mirror 23, and then the polygon mirror 25 is installed. The light enters the reflection mirror 24 through the gap 52 below the table 51. The laser light emitted from the reflection mirror 23 to the reflection mirror 24 is emitted in a substantially horizontal direction.

The reflection mirror 24 reflects the incident laser light toward the polygon mirror 25 and obliquely upward. The laser light incident on the polygon mirror 25 is reflected toward the mirror group that constitutes the mirror system of the side scanner unit 2.

Each scanning light reflected by the polygon mirror 25 is emitted slightly obliquely upward from the horizontal in FIG. 22, but the reflection direction of the reflected light from the polygon mirror 25 is the reflection surface of the polygon mirror 25. It is decided according to the angle of.

FIG. 23 is a perspective view of the lower frame 41 of the bar code reader, and is a drawing showing the path of the laser light emitted from the VLD module 21 to the polygon mirror. Note that, in FIG. 23, the polygon mirror itself is not shown for the sake of easy understanding of the trajectory of the light beam, and only the base 51 on which the polygon mirror is installed is shown. Further, the concave mirror is provided below the mirror ZB2, and thus is not shown.

As shown in FIG. 23, the laser light reflected by the reflection mirror 23 enters the reflection mirror 24 through the gap 52 at the bottom of the table 51, and the reflection mirror 24
Is reflected obliquely upward toward the polygon mirror 25. On the other hand, the laser light emitted through the through hole of the concave mirror directly enters the polygon mirror.

24 and 25 show the lower frame 41.
The upper frame 42 and the cover 4 of the side scanner 2
FIG. 24 is a side cross-sectional view of the barcode reader in a state where 3 is attached, FIG. 23 is a path of scanning light emitted from the bottom scanner unit 3, and FIG. 24 is a path of scanning light emitted from the side scanner unit 2. Are shown respectively.

As shown in FIG. 24, the scanning light of the bottom scanner section 3 reflected by the polygon mirror 25 through the through hole 31 of the concave mirror 30 is once folded back downward by the mirror attached to the upper frame 42. And is reflected upward by the mirror attached to the lower frame 41 in the direction of the bottom window 5.

For example, in the case of FIG. 24, the scanning light from the polygon mirror 25 is incident on the mirror ZBL1 and ZBL1
It is reflected by 1 and enters the mirror ZB2. ZB2
Reflects the incident scanning light obliquely upward, and the scanning light is emitted from the bottom window 5.

On the other hand, as shown in FIG. 25, the scanning light reflected by the polygon mirror 25 via the reflection mirrors 23 and 24 is attached to the mirror VSL1 attached to the lower frame 41 or the mirror frame 44. After being reflected upward by the mirror ZL, it is emitted from the side window 4 in a substantially horizontal direction by the other six mirrors attached to the mirror frame 44.

For example, in the case of FIG. 25, the scanning light from the polygon mirror 25 enters the mirror ZL and is reflected upward (almost in the vertical direction). Thereafter, the light enters the mirror ZHL attached to the mirror frame and is reflected in the horizontal direction, so that the scanning light forming the scanning pattern ZHL is generated.

FIG. 26 is a comparison of scanning patterns emitted from the bottom windows of the bar code reader according to this embodiment and the conventional bar code reader, respectively.
6a shows the scanning pattern according to the present embodiment, which is shown in FIGS.
Each show a scanning pattern by a conventional bar code reader. Compared with the conventional barcode reader, the number of scanning patterns emitted from the bottom window of the barcode reader according to the present embodiment is large, and the scanning patterns are directed in various directions. In the case of the conventional example (1), there are a total of 12 scanning lines, and in the case of the conventional example (2), there are only a total of 24 scanning lines. Therefore, the bar code reader according to the present embodiment has a higher probability of scanning the bar code, and the bar code reading performance is higher.

Also, the bottom window 5 according to the present embodiment.
Is longer than conventional readers.
Therefore, the range of the bottom window 5 through which the article passes in order to read the barcode becomes wide. Therefore, the operability of the reading work can be improved accordingly.

FIG. 27 is a diagram for explaining the difference in the size of the bar code reading range between the conventional bar code reader and the bar code reader according to the present embodiment. The reading range shown in FIG. 27 refers to a range in which the bar code can be reliably read when the bar code set up in the vertical direction is rotated 360 ° on the horizontal plane.

In the case of the conventional bar code reader, the size of the reading window is 6 inches × 6 inches, and the length of the reading window is short, so that the readable range particularly in the depth direction is necessarily narrowed. Since the reading area is located on the side window 4 side, the operator needs to bring the article closer to the side window 4 to pass the article, but some people may not reach this range, and the operability of the reading operation may be reduced. Is not so good. On the other hand, in the bar code reader according to the present embodiment, the reading window has a size of 4 inches × 7 inches, so that the readable range in the depth direction is widened to the operator side. Therefore, even a person with a short hand can easily pass the article within the readable range.

When the article passes over the bar code, the longer the depth of the reading window in the depth direction, the higher the possibility that the scanning light emitted from the reading window will scan the article. However, with respect to the length in the width direction, that is, the direction that coincides with the passing direction of the article, there is no problem in reading performance even if the width is not so wide. On the other hand, sapphire glass is expensive, and its price increases as the area increases. Therefore, the reading window having a width of 6 inches is disadvantageous in terms of cost and has an unnecessary width.

On the other hand, the reading window according to the present embodiment has a 4-inch width required to maintain the reading performance, and thus the reading performance is not deteriorated and the price of glass increases. It also has the advantage that it can be suppressed.

FIG. 28 is a drawing showing the path of the reflected light from the bar code in the bar code reader according to the present embodiment, and is shown from the position where the reflected light from the bar code enters the polygon mirror 25. The reflected light that has entered from the bottom window is reflected by the mirror system A and then enters the polygon mirror 25. Polygon mirror 2
The reflected light from the bar code reflected by the reflecting surface 5 is incident on the concave mirror 30. The reflected light from the polygon mirror 25 is reflected and condensed by the concave mirror 30, and the detector B2
Light is received at 8.

On the other hand, the reflected light that has entered from the side window enters the polygon mirror 25 after being reflected by the mirror system B. By the reflecting surface of the polygon mirror 25,
The reflected light from the bar code reflected downward enters the Fresnel lens 32. The Fresnel lens 32 collects the reflected light from the polygon mirror 25, and the bottom mirror C33.
Incident on. The bottom mirror C33 reflects the reflected light from the barcode toward the light receiving surface of the detector A29.

FIG. 29 is a drawing showing the relationship of the optical path length from the polygon mirror to the position where the laser beam is most narrowed. In FIG. 29, a-b-c-d represent scanning light emitted from the side window 4, and e-f-g-
h indicates scanning light emitted from the bottom window 5.

Here, in the apparatus of FIG. 29, a-b
The optical path length of −c−d is longer than the optical path length of ef−g−h. This is because the laser light source (LD in the figure) is provided at the lower left in the figure.

When the lens for forming the beam and the aperture (details of which will be described later) are located near the laser light source, the reading area of the barcode by the laser beam is determined depending on the distance from the laser light source. It Therefore, the mounting position of the laser light source in the bar code reader contributes to the determination of the size of the bar code reading area.

In the case of FIG. 29, the distance from the laser light source to the position where the beam is most narrowed is the same for both d and h. However, from the relation of the arrangement of the laser light sources, a is based on the polygon mirror 25. Two optical path lengths of -bcd and efgh are changed. a-b-c-d and ef
The optical path length difference of −g−h is the optical path length of a′−a from the laser light source to the polygon mirror and the optical path length of the laser light source to the mirror a ′.
It is absorbed by the difference from the optical path length of a'-a "-e to the polygon mirror via the. In the case of Fig. 29, the case where the length of the reading window in the depth direction is not so long is shown. Shows.

On the other hand, when the length of the reading window in the depth direction becomes long, the mirror f cannot be attached at the same position as in FIG. That is, if the mirror f is not moved to the right side in the figure by the length of the reading window, the mirror f obstructs the path of the scanning light and the emission of the scanning light is hindered. Therefore, in the case of FIG. 30, the mirror f has been moved to the right side of the drawing with respect to the device of FIG. Although the optical path length from the laser light source to the point d and the optical path length to the point h are equal, since the mirror f has moved to the right side in the drawing, e-f-g- is longer than the optical path length of a-b-c-d. h
The optical path length of becomes longer. Therefore, in the case of FIG. 30, the laser light source cannot be attached at the same position as in FIG.

Therefore, in the bar code reader according to the present embodiment, the laser light source is installed on the right side of the bar code reader in the drawing. With such a light source arrangement, a-b-c-d
The difference between the optical path length of a and the optical path length of ef-g-h is a'-
It can be absorbed by the difference in optical path length between a ″ -a and a′-e.

Since the side scanner section 2 is provided with a scanning mirror system and the like, it is impossible to secure a sufficient space inside. Therefore, it is difficult to route the laser light inside the side scanner unit 2 in order to increase the optical path length of the light emitted from the laser light source. In the case of the device according to the present embodiment (FIG. 30), by providing the laser light source on the right side of the device in the figure, it is possible to secure a space for routing the laser light for adjusting the optical path length.

Further, in the case of this embodiment, the laser light supplied to the side scanner unit 2 is supplied to the polygon mirror 25.
The lower surface of the polygon mirror is passed so that it intersects the rotation axis of the polygon mirror. If the laser light supplied to the side scanner unit 2 passes through the upper part of the polygon mirror 25, it is difficult to dispose a mirror (mirror system B) for guiding the laser light to the scanning optical system inside the side scanner. The problem arises. However, in the case of this embodiment,
By passing the laser light under the polygon mirror, the occurrence of such a problem is prevented.

FIG. 31 is a diagram illustrating an example of receiving reflected light from a bar code. In the case of FIG. 31,
The scanning light reflected by the polygon mirror 25 'enters the pattern generating mirror 71, is reflected downward, is further reflected upward by the bottom surface mirror 72, and is emitted from the bottom window 5'. The reflected light from the barcode reaches the polygon mirror 25 'through the same path as the emitted light,
It is reflected toward the detector 73.

The reflected light from the polygon mirror 25 'is condensed by the lens 74, reflected downward by the mirror 75 whose reflection surface is directed obliquely downward, and received by the detector 73.

In the case of such a bar code reader,
Due to the arrangement of the mirror 71 and the bottom mirror 72,
The lens 74 cannot be brought very close to the polygon mirror 25 '. Therefore, the dimension of the barcode reader in the depth direction cannot be made very small, and the apparatus of FIG. 31 requires a depth of 450 mm or more.

In the case of a store having a large area, the width of the settlement counter can be set to about 550 mm, for example.
In this case, it is possible to install the bar code reader in the checkout counter without reducing the width of the bar code reader so much. However, in the case of a store with a small area, especially in a store in Japan, the settlement counter width is 450 mm to 480.
It may be as narrow as mm. In this case, the bar code reader shown in FIG. 31 cannot be installed in the settlement counter.

FIG. 32 is a view for explaining the arrangement of the light receiving elements of the bar code reader according to this embodiment. As described above, the detector B28 according to the present embodiment is provided on the bottom surface of the barcode reader. And the concave mirror 3
By using 0, the reflected light from the polygon mirror 25 is reflected back in the middle of the barcode reader.

On the other hand, in order to emit scanning light from the bottom window 5, the scanning light reflected by the polygon mirror 25 is once reflected downward by the mirror a attached to the upper frame, and then, for example, the concave mirror 30, VLD. It is reflected upward by the mirror ZB2 provided on the module 21.

As described above, in order to emit the scanning light from the bottom window 5, there is no mirror corresponding to the bottom mirror in FIG. 31, and the optical system that contributes to the generation of the scanning light is arranged on the bottom surface of the bar code reader. Not not. Therefore, the detector B28 can be arranged on the bottom surface of the barcode reader, and the reflected light reflected by the polygon mirror 25 can be folded back inward and reflected using the concave mirror 30. Since the optical system is arranged as described above, the depth of the device in the depth direction can be made shorter than that of the conventional device even though the bottom window 5 has a long depth of 7 inches. 32, the device depth can be set to 440 mm or less.

FIG. 33 is a front view and a side view of the concave mirror 30 according to this embodiment. The through hole 31 is provided near the center of the concave mirror 30 as described above. Also,
The concave mirror 30 is attached to a fitting 75 for attaching the concave mirror to the frame of the barcode reader. The mounting bracket 75 is bent in a U shape,
The concave mirror 30 is urged to the right side in the figure by the elasticity of the mounting member 75.

The focus of the concave mirror 30 needs to be aligned with the light receiving surface of the detector B, but the focus of the concave mirror 30 may deviate from the light receiving surface of the detector B due to an error in mounting each part. The concave mirror according to the present embodiment has a mechanism capable of adjusting the mounting angle in the horizontal and vertical directions.

FIG. 34 is a bottom view of the barcode reader according to the present embodiment. The bottom of the barcode reader is equipped with three screws for adjusting the angle of the concave mirror. The adjustment screw α is a screw for aligning the vertical position of the concave mirror. The adjusting screw β is a screw for adjusting the horizontal position of the concave mirror.

FIG. 35 is a drawing for explaining the angle adjustment of the concave mirror. Folding part 75 'of the mounting bracket 75
Has screw holes 76 near both ends, and a hole 77 serving as a fulcrum near the center. On the other hand, the frame 41 of the bar code reader has a protrusion 78 and two fool holes 7.
9 is provided.

The hole 77 of the mounting bracket 75 is formed in the frame 4
The concave mirror 30 is fitted in the projection 78 of No. 1 and is rotatable in the horizontal direction around the projection 78. Concave mirror 30
In the horizontal alignment of the concave mirror 30, the concave mirror 30 is rotated around the fulcrum (projection 78) so that the focal point of the concave mirror 30 is located on the light receiving surface of the detector B, and then the mounting bracket is adjusted by the adjusting screw β. 75 is fixed to the frame 41.

On the other hand, in the case of FIG. 35, the concave mirror 30 is biased toward the front side in the figure by the elasticity of the mounting member 75 as described above. The tip of the adjusting screw α is butted against the back surface of the concave mirror 30. In order to adjust the angle of the concave mirror 30 in the vertical direction, the feeding amount of the adjusting screw α is adjusted to move the biased concave mirror 30 in the front-rear direction.

By using such a simple mechanism, it becomes possible to match the light reflected by the concave mirror 30 with the light receiving surface of the detector B by a simple operation.

FIGS. 36A and 36B are a top view and a side view of the C mirror 33 which makes the detector A enter the reflected light from the barcode. An attachment fitting 80 is attached to the bottom surface of the C mirror 33. The C mirror 33 is attached to the apparatus frame via the attachment fitting 80. The mounting bracket 80 is bent into a U shape, and the C mirror 33
Is urged downward by the elasticity of the metal fitting. The inclination of the C mirror 33 and the angle in the horizontal direction are also adjustable.

FIG. 37 is a view of the bottom surface of the bar code reader, showing an adjusting screw α and two adjusting screws β. The adjusting screw α adjusts the inclination of the C mirror 33, and the tip of the adjusting screw α is abutted against the bottom surface of the C mirror 33. By adjusting the amount of extension of the adjusting screw α, the inclination of the C mirror 33 can be adjusted and the reflection direction of the reflected light can be adjusted.

On the other hand, the tip ends of the adjusting screws β are screwed into the screw holes provided in the vicinity of both ends of the mounting member 80 via the stupid holes. The screw hole of the mounting member has the same shape as the mounting member of the concave mirror. The mounting bracket 80 is horizontally rotatable around a fulcrum as in the case of the concave mirror. After the orientation of the C mirror 33 is adjusted, the mounting bracket 8 is adjusted by the adjusting screw β.
Fix 0 to the device frame.

FIG. 38 is a view for explaining the bottom window 5 surface of the barcode reader according to the present embodiment. On a bottom surface 81 provided with the bottom window 5, a projection 82 having a triangular cross section and extending in the lateral direction of the device.
Is provided.

When reading a bar code, the article is passed through the space above the bar code reader, but depending on the operator, the article may be brought into contact with the bottom surface to move the article. In this case, if the bottom surface provided with the bottom window 5 is flat, the contact area between the bottom surface and the article becomes large and the frictional force between the article and the bottom surface becomes large, so that the article can be easily passed. Not be.

In order to deal with such a problem, in the bar code reader of this embodiment, the bottom window surface 81
By providing a projection 82 on the bottom surface to reduce the contact area between the article and the bottom surface, the frictional force between the article and the bottom surface 81 is reduced. The extending direction of the protrusions 82 coincides with the passing direction of the article, and the reduction of the frictional force can be realized more effectively.

The projections 82 can be formed by resin molding together with the bottom surface 81, or a member for forming the projections may be attached to the bottom surface.

In the bar code reader, the scanning lines are most concentrated and there is a position (optimal reading position) where the reading probability is highest. In this embodiment, the protrusion 8 of FIG.
2 is used so that the operator can easily recognize which position is the optimum reading position.

Portion corresponding to the optimum reading position (83 in the figure)
In, the intervals at which the protrusions 82 are arranged are narrowed. On the other hand, in the portion deviated from the optimum reading position (84 in the drawing), the interval between the protrusions 82 is wider than the interval between the protrusions at the optimum reading position 83. Since the optimum reading position is informed by the distance between the projections 82 provided on the bottom window surface 81 in this manner, the operator can easily recognize which position the optimum reading position is.

Further, when passing a small article, there is a problem that the article falls between the projections 82, and the operability of bar code reading may be deteriorated. Therefore, it is desirable that the protrusions 82 are not so far apart from each other. On the other hand, since the interval between the projections 82 is narrowed at the optimum reading position, it is possible to improve the operability when passing the article through the optimum reading position.

FIG. 39 is a diagram showing an example of a printed circuit board. On the printed circuit board of the bar code reader, photodetector circuits 1 and 2 to which photodetectors A and B are connected, VLD to which a VLD module is connected, and Moto to which a motor is connected.
r is provided, and the control unit provided on the printed circuit board controls the operation of each unit via them. The printed circuit board has a power cable connector for supplying power (power supply in the figure) and an interface (I / F) cable connector for transferring the read barcode information to a POS terminal (in the figure). POSt
external1), a power supply connector for supplying power to the scale device (Scale in the figure), a connector for connecting a handheld scanner (handheld scanner in the figure), etc. Becomes These connectors are often provided on a main printed circuit board (Main PCB).

Conventionally, as shown in FIG. 40, the main printed circuit board 85 was installed vertically on the back surface of the side scanner section 2, but in this case, the connector 86 faces downward. Therefore, when it is necessary to connect cables to the various connectors 86, the user needs to lift and incline the bar code reader as shown in FIG. 40 in order to confirm the connector type to be connected.

However, since the bar code reader is embedded in a checkout counter or the like, it is very difficult to lift and incline the bar code reader, and the workability of cable connection is very poor. It was

FIG. 41 is a view for explaining the cable connection of the bar code reader according to this embodiment. In the barcode reader according to the present embodiment, the main printed circuit board 85 is horizontally arranged on the bottom surface of the device, and the connector 86 is also oriented to the side surface. Therefore, even when the user confirms the connector type, the connector 86 can be confirmed with the barcode reader installed horizontally, and the connector connection work can be performed efficiently.

FIG. 42 is a rear view of the bar code reader according to the present embodiment, and illustrates various connectors arranged sideways. DC on the back of the device
Power cable connection connector 87 to which a power source is connected, interface connector 88, etc. FIG. 43 is a diagram showing the back surface of the bar code reader in which the main printed circuit board 85 is mounted. Various connectors 89 shown in FIG. 42 are attached to the printed circuit board 85.
A motor cable or the like connected to the polygon motor is pulled out from the bar code reader (FIG. 44 shows the back surface of the bar code reader with the main printed circuit board 85 removed). The cable is connected.

FIG. 45a is a drawing for explaining the structure of the laser module. The laser module includes a semiconductor laser 91, a collimator lens 92, and an aperture 93. Since the laser light emitted from the semiconductor laser 91 diverges at a predetermined divergence angle, the collimator lens 9
After narrowing the laser light by 2, the beam is shaped by the aperture 93, and the laser light is emitted to the barcode reading area.

Here, the laser light emitted from the semiconductor laser has different divergence properties in the vertical and horizontal directions as shown in FIG. Approximately 5 ° to 11 ° in the horizontal direction
Has a divergence angle of about 24 ° to 37 ° in the vertical direction. Further, the semiconductor laser has a large individual difference, and the divergence angle varies greatly depending on the individual semiconductor laser.

Here, the beam shape of the emitted laser light depends on the diameter of the aperture 93 and the like.
3, the beam diameter is shaped. FIG. 45b is a diagram illustrating the relationship between the distance from the aperture and the beam diameter when the laser light emitted after being shaped by the aperture is used. If the optimum beam diameter for bar code reading is 550 μm, the bar code readable area is, for example, the range shown in FIG. 45b. If the beam system becomes too large, it becomes impossible to recognize a bar code having a narrow bar width because the distance between the bars is narrow, and the bar code reading efficiency is reduced. Therefore, it is desirable that the beam diameter in the reading area be as narrow as possible.

Here, a problem caused by the divergence angles of the laser light emitted from the semiconductor laser 91 in the vertical direction and the horizontal direction will be described with reference to FIG. As shown in FIG. 47, for example, even when the optimum beam diameter is obtained in the horizontal direction where the beam divergence angle is small, the beam diameter incident on the aperture 93 is large because the divergence angle is large in the vertical direction. Become. The diameter of the aperture 93 has the same vertical and horizontal diameters for the purpose of beam shaping. Therefore, there is a problem that the laser light is kicked by the aperture 93 particularly in the vertical direction, and the utilization efficiency of the laser light is reduced. When the usage efficiency was the worst, it was possible to achieve a usage efficiency of at most 18%.

If the efficiency of light utilization is merely increased, the diameter of the aperture 93 is increased so that f of the collimator lens 92 is increased.
There are measures such as decreasing the value (shortening the focal length) or increasing the distance between the semiconductor laser and the collimator lens.

By increasing the diameter of the aperture 93, the kicking of light in the vertical direction is reduced, and the light utilization efficiency can be improved. However, since the diameter of the aperture 93 is large, it is difficult to narrow down the beam system,
Beam diameter 550 for optimum reading as shown in FIG.
The range of μm is narrower than that of FIG. 45b, and the position where the beam system is most narrowed is farther than that of FIG. 45b. And for the lateral direction,
When the aperture diameter becomes large, the beam almost passes through the aperture 93 as it is, and the beam cannot be substantially formed.

Further, when the f value of the collimator lens is reduced, the beam diameter is most narrowed in front of the case where a lens having a large f value is used. In this case, FIG.
As shown in (1), in the vertical direction where the beam divergence angle is large, both the beam shape and the light use efficiency can be ideal, and there is no particular problem with respect to the light use efficiency. However, in the lateral direction where the divergence angle is small, the beam is hardly kicked by the aperture 93, and the beam cannot be formed, which causes a problem that the beam shape is collapsed. Therefore, in the horizontal direction, the beam forms an image in a space in front of the reading space, and the image forming positions in the vertical direction and the horizontal direction are different, so that the reading range is narrowed (FIG. 48).

Semiconductor laser 91 and collimator lens 92
Even when the distance from the
The same problem occurs when the f value of 2 is reduced.

As described above, in order to read the bar code, it is necessary to improve the utilization efficiency of the laser light and to widen the reading range in which the bar code can be read optimally.

The laser module according to the present embodiment can solve the above problems and realizes a laser module capable of expanding the light quantity margin while ensuring a beam diameter that can achieve a predetermined resolution for bar code reading. is doing. In the laser module according to the present embodiment, by making the beam diameters in the vertical and horizontal directions the same, the kick amount by the aperture is reduced and the range in which the optimum beam diameter can be secured is widened.

FIG. 50 is a diagram for explaining a problem when a collimator lens having a relatively large f value is used and a solution thereof. In the case of the laser module of FIG. 50, in the lateral direction where the divergence angle of the beam is small, there is no problem with the beam shape, and the light use efficiency based on the vignetting by the aperture 93 is ideal. be able to. However, in the vertical direction where the divergence angle of the beam is large, there is no problem in the beam shape, but the amount of kick by the aperture increases, and the light use efficiency decreases.

In order to solve this problem, the beam diameter in the vertical direction can be changed to a small value without decreasing the light amount so that the beam diameter in the horizontal direction is almost the same.

FIG. 51 is an explanatory view of the principle of the above-mentioned solving means. A right angle prism 94 is shown in FIG. When laser light is incident on the rectangular prism at a predetermined angle, the rectangular prism 94 refracts the laser light.

Here, the ratio of the beam diameters in the vertical and horizontal directions is
Equal to the ratio of each divergence angle. If we use a specific value for the divergence angle range above, the ratio of the divergence angle in the vertical and horizontal directions,
That is, a value of 2.7: 1 is derived for the beam diameter ratio. Therefore, here, the beam diameter in the vertical direction is set to 2.7: 1.
It is necessary to reduce by the ratio of.

When the beam is refracted by the right-angle prism 94, the diameter of the beam emitted from the right-angle prism 94 is changed according to the refraction angle. Here, the above 2.
An example of achieving a 7: 1 beam diameter reduction is illustrated in Figure 51a.

The wavelength of the laser light of the semiconductor laser used is, for example, 670 nm. Further, the refractive index of the glass forming the right-angle prism 94 is n = 1.5134, and the angle θ of the right-angle prism is 37.828 °.
In this case, when the laser light is incident on the surface a of the right-angled prism 94 at a right angle, the laser light is emitted at an angle of 68.15 ° with respect to the perpendicular of the hypotenuse of the right-angled prism 94. Here, the illustrated plane direction corresponds to the vertical direction of the laser light. At this time, the ratio of the diameter of the beam incident from the collimator lens 92 to the right-angle prism 94 and the diameter of the laser light emitted from the right-angle prism 94 can be set to 2.7: 1 as shown in FIG. 51b. .

In the lateral direction, the right angle prism 94
Does not act, the beam diameter is not converted, and the beam diameter emitted from the semiconductor laser 91 is maintained.

FIG. 52 is a drawing showing an example of arrangement of the semiconductor laser 91, collimator lens 92, aperture 93, and right-angle prism 94. In this way, by using a right-angle prism to reduce the beam diameter in the vertical direction and make it the same (or almost the same) as the beam diameter in the horizontal direction, the amount of light kicked by the aperture is suppressed to a low level and the light use efficiency is improved. Can be made.

FIG. 53 shows a structure for solving the problem when a collimator lens having a small f value (f = 3.6 mm) is used, and the target laser module is the one shown in FIG. .

In the case of FIG. 49, no problem occurs in the vertical direction, and there is a problem that the aperture 94 hardly acts in the horizontal direction and the beam cannot be formed. Therefore,
In the case of FIG. 53, the beam diameter in the lateral direction is enlarged.

When the expansion of the beam diameter is set to 1: 2.7, the rectangular prism 94 used may be the same as that shown in FIG. The difference from FIG. 51 lies in the arrangement of the rectangular prism 94. In the case of FIG. 53, the laser beam is incident on the hypotenuse of the right-angle prism 94 at 68.15 ° with respect to the perpendicular. Here, the illustrated plane direction corresponds to the lateral direction of the laser light. This results in a lateral beam diameter of 2.7.
Can be doubled.

FIG. 54 shows a right-angle prism 94, a semiconductor laser 91, a collimator lens 92, and an aperture 93 shown in FIG.
It is drawing which shows the state which has arrange | positioned. As shown in FIG. 54, by using the right-angle prism 94, it is possible to expand the beam diameter in the lateral direction, and the aperture 9
The diameter of the beam incident on the beam 3 can be made the same in both the horizontal and vertical directions.

Here, the diameter of the laser beam emitted from the rectangular prism and reaching the aperture becomes larger (or smaller) than necessary depending on the angle tolerance of the rectangular prism and the positional relationship with the laser module. There are various problems such as the possibility of being lost.

FIG. 55a is a drawing explaining this problem. For example, when the incident light incident on the right-angle prism 94 is not parallel light, the position where the laser light is focused depends on the distance relationship between the semiconductor laser 91 and the collimator lens 92, and the focal position that should originally be f1. May become f2.

Such a problem is caused in the direction in which the beam is converted by the rectangular prism as shown in FIG. 55b.
This can be solved by making the collimator lens 92 rotatable about its optical axis. That is, the beam diameter reaching the rectangular prism can be reduced according to the inclination of the collimator lens 92. Therefore, it is particularly effective when the right-angle prism is adhered and fixed to the laser module and the right-angle prism 94 cannot be adjusted.

By adjusting the angle of the collimator lens 92 to reduce the beam diameter of the laser light reaching the rectangular prism 94, it is possible to cancel the expansion of the beam diameter of the laser light reaching the aperture 93.

The description so far has been made using the right-angled prism, but this is because the right-angled prism can be used to minimize the apex angle and also reduce the size of the entire laser module. Especially when it is not necessary to downsize the laser module, etc., FIG.
There is no problem with using a prism that is not a right angle as shown in FIG. In the case of the drawing, prisms having different angles a and b are shown.

FIG. 57 is a drawing showing an example of beam diameter conversion using means other than a prism. In the case of FIG. 57,
Cylindrical lenses 95a and 95b are used. When a cylindrical lens is used, since it has a condensing function only on one of the orthogonal axes, it can be applied to reduce (expand) the beam diameter of laser light in the vertical direction (horizontal direction).

FIG. 57a is a drawing explaining the means for reducing the beam diameter in the vertical direction. In FIG. 57a, a cylindrical convex lens 95a and a cylindrical concave lens 9 are shown.
5b is combined. The lenses are arranged in the order of closer to the semiconductor laser 91: the collimator lens 92, the cylindrical convex lens 95a, and the cylindrical concave lens 9.
The order is 5b.

The laser light focused by the collimator lens 92 is further focused only in the vertical direction by the cylindrical convex lens 95a. The horizontal direction is limited only by the collimator lens 92, but the vertical direction is limited by the collimator lens 9 and the cylindrical convex lens 95a, so that the vertical beam is longer than the horizontal beam that is not affected by the cylindrical convex lens 95a. The emitted laser light is imaged in front. In this state, the diameter of the beam entering the aperture 93 becomes smaller than that of the beam in the lateral direction, which causes a problem that the shape of the beam emitted to the reading space collapses.

As a means for correcting this beam shape, a cylindrical concave lens 95b is provided after the cylindrical convex lens 95a. Cylindrical concave lens 95b
Thus, the degree of focusing of the beam focused by the cylindrical convex lens 95a is reduced. In Figure 57a,
The transverse beam is shown in dotted lines. As shown in FIG. 57a, by the action of the cylindrical convex lens 95a and the concave lens 95b, the beam diameter incident on the aperture 93 can be made substantially the same in both the horizontal and vertical directions.

On the other hand, FIG. 57b is a drawing explaining a means for expanding the beam diameter in the vertical direction. In the case of FIG. 57b, the laser light emitted from the semiconductor laser 91 passes through the collimator lens 92, the cylindrical concave lens 95b, and the cylindrical convex lens 95a in this order, and the aperture 9
It is incident on 3. In Figure 57b, the solid line represents the lateral beam,
Dotted lines indicate vertical beams.

The lateral beam narrowed down by the collimator lens 92 is expanded at a predetermined magnification by the cylindrical concave lens 95b. On the other hand, since the vertical beam is not affected by the cylindrical concave lens 95b, the horizontal beam can be more narrowed.

Here, while the horizontal beam is expanded by the cylindrical concave lens 95b, the vertical beam is not affected by the cylindrical concave gate diagram 95b, so that the horizontal beam is located at a farther position. An image will be formed. Therefore, when a horizontal beam is emitted to the reading space, the beam shape may be destroyed.

As a countermeasure against this, in the case of FIG. 57b, a cylindrical convex lens 95a is inserted after the cylindrical concave lens 95b to correct the beam. By using the cylindrical convex lens 95a to suppress the degree of divergence of the beam in the horizontal direction to be small or to focus the beam, the degree of convergence of the beam can be made equal in both the horizontal and vertical directions.

In the case of FIGS. 57a and 57b, a cylindrical lens having two concave and convex portions is used. However, as shown in FIG. 57c, a cylindrical double-sided lens 95c obtained by bonding two cylindrical lenses together is used. Is also possible. However, in this case, the distance between the two lens surfaces becomes smaller, and since beam conversion is performed in the same medium, a lens surface with a smaller radius of curvature is used as compared with the case of using two cylindrical lenses. Need to be molded.

FIG. 58 shows that the laser light emitted from the laser module 21 is divided into different scanning lines A and B.
It is the figure which explained the means for generating.

The laser beam emitted from the laser module 21 is split into two beams by the beam splitting means 22. The two beams are reflected toward the polygon mirror 25 by a small reflecting mirror 30 ′ provided at the center of the concave mirror 30. The laser light reflected by the polygon mirror 25 is reflected by the scanning line division mirror 26 and emitted from the reading window, one of which is the scanning line A,
The other becomes the scanning line B.

The reflected light from the bar code enters the concave mirror 30 by the polygon mirror 25. The reflected light corresponding to the scanning line A enters the photodetector A by the concave mirror 30, and the reflected light corresponding to the scanning line B enters the photodetector B by the concave mirror 30.

FIG. 59 shows an example of the light splitting means. In FIG. 59a, the laser light emitted from the laser module 21 is split into a beam A and a beam B by a half mirror. In the case of FIG. 59b, the laser light emitted from the laser module is split into a beam A and a beam B by half cupping or PBS.

FIG. 60 shows these prisms, dividing means,
VL according to the present embodiment incorporating a collimator lens and the like
It is a two-sided view of a D module. In the figure, 101 is a semiconductor laser, and 102 is a collimator lens.
The collimator lens 102 is housed in a block 103 such as aluminum. The position of the block 103 can be adjusted in the left-right direction in the drawing, and the focus position of the laser light is adjusted by this. The block 103 is biased from above by a biasing plate 104 having elasticity,
As a result, the position of the block 103 is fixed.

Reference numeral 105 denotes a rectangular prism, and the laser light emitted from the semiconductor laser 101 enters the rectangular prism 105.

The laser light refracted by the rectangular prism 105 is beam-shaped by the aperture 106,
It is divided into a beam A and a beam B by the half mirror 107.

The beam A is applied to the polygon mirror 25 through the through hole 31 of the concave mirror 30 as shown in FIG. On the other hand, the beam B is emitted toward the reflection mirror 23.

FIG. 61 is a two-sided view of the block 103 containing the collimator lens 102. 61a is a top view, and FIG. 61b is a front view of the collimator lens 102 as viewed from the front.

The collimator lens 102 is attached to the block 103 at a predetermined angle with respect to the optical axis of the laser light. Semiconductor lasers have astigmatic differences as well as vertical and horizontal divergence angles. This is a decrease in the emission position of the beam in the horizontal direction and the emission position of the beam in the vertical direction, which causes a problem that the focal position of the laser beam is displaced.

Collimator lens 102 according to the present embodiment
In order to solve this astigmatic disparity or the problem shown in FIG. 55, it has been attached inclining with respect to the optical axis by a predetermined angle in advance. This mounting angle may be predetermined based on various conditions. Although the semiconductor lasers have individual differences, the mounting angle of the collimator lens 102 can achieve a certain degree of effect if the mounting angle is set to an angle corresponding to an average semiconductor laser in which individual differences do not pose a problem. .

[0223]

As described above, according to the present invention, a vertical prism or the like is used to convert one of the beam diameters in the vertical direction and the horizontal direction of the semiconductor laser, while the other is not converted. The beam diameters of the respective sides can be made substantially the same, and for example, it becomes possible to reduce the kick amount due to the aperture and prevent the beam diameter from collapsing.

Especially by using a right angle prism,
The laser module can be made smaller.

Further, by housing the laser light source, the beam diameter converting means, and the beam splitting means in one module, it is not necessary to perform the optical axis alignment work of each part.

[Brief description of drawings]

FIG. 1 is a perspective view of a barcode reader according to an embodiment of the present invention.

FIG. 2 is a view showing a state in which a barcode according to an embodiment is installed on a checkout counter.

FIG. 3 is a side sectional view of a barcode according to an embodiment.

FIG. 4 is a barcode reading range of the barcode reader according to the embodiment.

FIG. 5 is an external dimension of a barcode reader according to an embodiment.

FIG. 6 is an optical system diagram of a barcode reader according to an embodiment.

FIG. 7 shows a state where a barcode cover according to an embodiment is removed.

FIG. 8 is a top / side view of the barcode reader of FIG.

FIG. 9 is a perspective view of a lower frame.

FIG. 10 is a top view of the lower frame.

FIG. 11 is a side view of the lower frame.

FIG. 12 is a perspective view showing a state in which an upper frame and a lower frame are removed.

FIG. 13 is a four-sided view of a mirror frame.

FIG. 14: Mirror attached to mirror frame

FIG. 15 is a side sectional view showing an optical system arrangement of a barcode according to an embodiment.

FIG. 16 is a diagram showing the scanning light path of the bottom scanner unit.

FIG. 17 is a diagram showing the scanning light path of the side scanner unit.

FIG. 18: Scanning pattern emitted from the bottom window

FIG. 19 is a drawing in which one scanning light is extracted from each scanning pattern emitted from the bottom window.

FIG. 20: Scanning pattern emitted from the side window

FIG. 21 is a view showing emission of a scanning pattern.

FIG. 22 is a side sectional view of an apparatus showing a ray path until a ray emitted from a light source is reflected by a polygon mirror.

FIG. 23 is a device perspective view showing a ray path until a ray emitted from a light source is reflected by a polygon mirror.

FIG. 24 is a side sectional view of an apparatus showing a path of scanning light emitted from a bottom scanner unit.

FIG. 25 is a side sectional view of an apparatus showing a path of scanning light emitted from a side scanner unit.

FIG. 26 is a comparison of scanning patterns emitted from the bottom window of the bar code reader according to the embodiment and the conventional bar code reader.

FIG. 27 is a comparison of scanning / reading ranges of the barcode reader according to the embodiment and the conventional barcode reader.

FIG. 28 is a side sectional view of the device showing a path of reflected light from a barcode.

FIG. 29 is a drawing showing arrangement of light sources and respective optical paths.

FIG. 30 is a drawing showing arrangement of light sources and respective optical paths.

FIG. 31 is a drawing showing a conventional arrangement of light receiving means, a reading range, and a device depth.

FIG. 32 is a drawing showing the arrangement of the light receiving means, the reading range, and the device depth according to the embodiment.

FIG. 33 is a two-sided view of a concave mirror

FIG. 34: Adjustment screw arrangement for concave mirror angle

FIG. 35 is a view showing the attachment of the concave mirror to the frame and the angle adjustment.

FIG. 36 is a two-sided view of a bottom mirror

FIG. 37: Angle adjustment screw arrangement for bottom mirror

FIG. 38: Protrusions provided on the bottom window surface

FIG. 39 is an example of a printed circuit board

FIG. 40: Printed circuit board layout of conventional bar code reader

FIG. 41 is a printed circuit board layout of the barcode reader according to the embodiment.

[Fig. 42] Rear view of the barcode reader and various connector layout examples

FIG. 43: Back side of barcode reader with printed circuit board attached

FIG. 44 is the back surface of the barcode reader before the printed circuit board is attached.

FIG. 45: Laser module and barcode reading area

FIG. 46: Difference in beam diameter of semiconductor laser

FIG. 47: Beam eclipse due to aperture

FIG. 48: Change in barcode reading area when anti-eclipse measures are taken

FIG. 49 is a problem when using a collimator lens having a small f value

FIG. 50 is a problem when using a collimator lens having a large f value

FIG. 51: Beam diameter conversion using right angle prism

FIG. 52: Laser module using right-angle prism

FIG. 53: Beam diameter conversion using right-angle prism

FIG. 54: Laser module using right angle prism

FIG. 55: Reading area change when collimator lens is rotated

FIG. 56: Example of prism other than right-angle prism

FIG. 57: Beam diameter conversion using a cylindrical lens

FIG. 58 is an example of a bar code reader that splits laser light to generate two scanning lights.

FIG. 59 is an example of beam splitting means

FIG. 60 is a VLD module according to an embodiment.

FIG. 61 is a block that houses a collimator lens.

FIG. 62: Conventional barcode reader

[Fig. 63] A bar code reader (1) having a conventional two-sided reading window.

FIG. 64: Bar code reader (2) with a conventional two-sided reading window

FIG. 65 is a top view of the settlement counter.

66 is a bar code reading area diagram of a two-sided bar code reader, 1 is a bar code reader, 2 is a side scanner unit, 3 is a bottom scanner unit, 4 is a side window, FIG.
5 is a bottom window, 21 is a VLD module, 22
Is a half mirror, 23 and 24 are reflection mirrors, 25 is a polygon mirror, 26 and 27 are mirror systems for generating a scanning pattern, 28 and 29 are photodetectors, 30 is a concave mirror, 32 is a Fresnel lens, 33 is a bottom mirror, 41 is a lower frame, 42 is an upper frame, 43 is a side scanner cover, 44 is a side scanner mirror frame, 82 is a protrusion provided on the bottom window surface, 91 is a laser light source (semiconductor laser), and 92 is a collimator lens. , 93 is an aperture, 94 is a right angle prism, and 95 is a cylindrical lens.

   ─────────────────────────────────────────────────── ─── Continued front page    (72) Inventor Masanori Okawa               4-1, Kamiodanaka, Nakahara-ku, Kawasaki-shi, Kanagawa               No. 1 within Fujitsu Limited (72) Inventor Toshiyuki Ichikawa               4-1, Kamiodanaka, Nakahara-ku, Kawasaki-shi, Kanagawa               No. 1 within Fujitsu Limited (72) Inventor Hiroshi Watanuki               4-1, Kamiodanaka, Nakahara-ku, Kawasaki-shi, Kanagawa               No. 1 within Fujitsu Limited (72) Inventor Yuzo Yamazaki               4-1, Kamiodanaka, Nakahara-ku, Kawasaki-shi, Kanagawa               No. 1 within Fujitsu Limited                (56) Reference JP-A-6-265802 (JP, A)                 JP-A-6-102462 (JP, A)                 JP-A-5-157985 (JP, A)                 JP-A-5-45656 (JP, A)                 JP-A-3-262086 (JP, A)                 JP 62-232611 (JP, A)

Claims (3)

(57) [Claims] 1. A semiconductor laser light source, a condensing means for condensing a laser beam emitted from the laser light source, and one of the axes orthogonal to the laser beam emitted from the condensing means. means for converting the light beam diameter, and dividing means for dividing the laser beam emitted from the said conversion means, integrally includes, characterized in that for emitting the plurality of divided laser beams, and wherein the condensing The axis of the focusing means is the laser
Predetermined angle with respect to the optical axis of the laser beam emitted from the light source
A laser module characterized by being adjustable so that it only tilts . 2. A semiconductor laser light source and a movable member are formed on a base member so as to be movable in a direction along the emission direction of the light beam.
Light emitted from the semiconductor laser light source
The lens for condensing
And a block member attached so as to be inclined with respect to the axes of the light rays condensed by the lens, which are orthogonal to each other.
Arranged to convert the ray diameter corresponding to one of the axes
Prism and an aperture for shaping the light beam emitted from the prism
And split the rays emitted from the aperture into multiple rays.
A laser module comprising: a dividing unit for dividing . 3. A semiconductor laser light source, which is formed so as to be movable in a direction along the emission direction of the light beam.
Light emitted from the semiconductor laser light source
The lens for condensing
And a block member attached so as to be inclined with respect to the axes of the light rays condensed by the lens, which are orthogonal to each other.
Arranged to convert the ray diameter corresponding to one of the axes
Prism and an aperture for shaping the light beam emitted from the prism
And split the rays emitted from the aperture into multiple rays.
Splitting means for splitting, and the laser module provided on the base member
Optical scanning device you characterized in that mounted with.