US RE40102 E1
An optical scanner for reading indicia having areas of different light reflectivity, such as bar code symbols includes a stationary, multi-surface, fold mirror having a first surface of a first aplanar profile and a second surface of a second, different aplanar profile.
1. An optical scanner for scanning indicia having areas of different light reflectivity, comprising:
a light source for producing a light beam; and
a scanning optical element for receiving the light beam and producing a scanning light beam therefrom, and a stationary, beam-shaping fold mirror comprising a cylindrical mirror for shaping the light beam.
2. An optical scanner for scanning indicia, the scanner comprising:
a light source producing a light beam that converges in both x and y directions so that the light beam has a waist in both the x and y directions, where x and y are orthogonal directions; and
a scanning element positioned to receive the light beam and reflect the light beam in a scanning motion along the x direction across the indicia, and a stationary fold mirror including a convex beam-shaping surface shaped to diverge light in the y direction to at least reduce convergence of the light beam in the y direction.
3. The optical scanner of
4. In an optical scanner for reading indicia having parts of different light reflectivity, the scanner having a laser light source, a reciprocally oscillatable scanning mirror for reflecting light from the light source to the indicia in a scan across the indicia thereby reflecting light of variable light intensity off the indicia, and a light sensor for detecting at least a portion of the light reflected off the indicia and generating an electrical signal indicative of the detected light intensity, an optical component comprising:
a stationary mirror having a generally concave first surface portion for collecting at least a portion of the light reflected off the indicia, and for directing the collected portion of light to the light sensor, and a generally aplanar second surface portion for directing the light from the light source to the scanning mirror.
5. An optical scanner for scanning indicia such as bar code symbols, comprising:
a laser source comprising a laser diode for producing a light beam along a path, the light beam having a profile that converges in both x and y directions so that the beam has a waist in each of the respective x and y directions, where x and y are orthogonal directions in a plane substantially orthogonal to the path of the light beam;
a convex mirror disposed in the path of the light beam from the laser source and shaped to diverge light in the y direction; and
a scanning element positioned to receive the light beam and functioning to move the light beam in a scanning motion along the x direction across the indicia.
6. In an optical scanner for scanning indicia, the scanner including a photodetector for detecting light of variable intensity reflected from the indicia and for generating an electrical signal indicative of the detected light intensity, an arrangement comprising:
a light source for emitting a laser beam;
a scanning element disposed in a path of the emitted laser beam and operative to reflect the laser beam in a scanning path for scanning indicia; and
a stationary multi-surface fold mirror having a first surface with a concave curvature positioned for collecting and reflecting the light reflected from the indicia for receipt by the photodetector, and at least a second beam shaping surface located substantially in a central region of the fold mirror and having a convex curvature for shaping the emitted laser beam, wherein the second beam shaping surface is positioned to reflect the emitted laser beam either as the beam passes from the light source to the scanning element or from the s g element to the indicia.
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This application is a division of U.S. patent application Ser. No. 09/009,231, filed Jan. 20, 1998, now U.S. Pat. No. 5,988,502 which, in turn, is a continuation-in-part of application No. 08/912,147, filed on Aug. 15, 1997, now U.S. Pat. No. 5,859,417, which is a continuation-in-part of U.S. patent application Ser. No. 08/405,585, filed Mar. 17, 1995, now abandoned, which is a continuation-in-part of U.S. patent application Ser. No. 08/268,982, filed Jun. 30, 1994, now U.S. Pat. No. 5,742,038, which is a continuation-in-part of U.S. patent application Ser. No. 08/314,519, filed Sep. 28, 1994, now U.S. Pat. No. 5,506,392, which is a divisional of U.S. patent application Ser. No. 08/109,021, filed Aug. 19, 1993, now U.S. Pat. No. 5,352,922, which is a divisional of U.S. patent application Ser. No. 07/735,573, filed Jul. 25, 1991, now U.S. Pat. No. 5,278,397, and is related to U.S. patent application Ser. No. 08/864,452, filed May 28, 1997,now allowed.
1. Field of the Invention
The invention relates generally to optical scanners, and in particular to scanners having dual or multiple working ranges.
Most optical scanners such as bar code scanners are adapted for use at a particular distance, or a range of distances, from an indicia to be scanned. If the user holds the scanner too close to the indicia, or too far away, the indicia and/or the flying spot beam will not be in focus, and decoding will not be possible.
Such scanners may not be particularly convenient in environments where a series of indicia to be read are presented to the scanner at various distances, and where it is difficult or impossible for the user to alter the distance between the scanner and the indicia. To deal with such situations, attempts have been made to expand the acceptable working range of conventional scanners, to give the user as much leeway as possible, and also to provide multi-distance scanners which can operate, for example, at a first working range or at a second working range according to the user's preference or requirements. One possibility is for the provision of a two-position switch on the scanner, with the scanner operating at a first working distance in a first position of the switch and at a second working distance in a second position. A disadvantage of such scanners is that they require additional moving parts to provide for operation at the two separate working ranges. Such systems are also not “automatic” in the sense that the user has manually to select the correct working range, according to the distance of the current indicia to be read; if the incorrect working range is chosen, a decode will not result.
One or the difficulties that bar code reader designers face when attempting to produce increased working ranges is that the greater the working range, and the greater the range of possible indicia that might be read, the lower tends to be the resultant signal to noise ratio in light that is reflected from the indicia. One approach for dealing with this involves the provision of non-conventional optics, in which the optics associated with either the laser or with the photodetector have two distinct focal points. An example of this is shown in U.S. Pat. No. 5,332,892, which is commonly assigned with the present application. In the device shown in that document, the two focal points are associated with corresponding circuitry to provide two separate channels of data derived from the scanned bar code. The two channels have differing resolutions. As the working angle and density vary, at least one of the resolutions is likely to be appropriate for sensing all or most of the bar coded data, regardless of the distance of the bar code with respect to the scanner and/or the size or density of the code. The scanning beams of bar code readers are typically derived from laser diodes. Such diodes are robust and relatively inexpensive, but they do suffer from the disadvantages that the beam emerging from a laser diode is astigmatic. The astigmatic laser diode can be characterized as having two apparent light sources spaced apart from each other along the optical path. One of the light sources lies in a horizontal plane, appears to be coming from inside the laser diode chip, and has a low angular divergence. The other apparent light source lies in a vertical plane, appears to be coming from a facet of the chip, and has a high angular divergence. The two apparent light sources, which are spaced apart from each other by typically about 20 micrometers, form two beam waists in different planes and in different directions, as measured relative to the planar junction of the chip.
The resultant relatively complex beam profile may need selective shaping before it can efficiently be used in an optical scanner. Some methods of providing such beam shaping are described in our co-pending U.S. patent application Ser. No. 08/268,982, filed Jun. 30, 1994, the teachings of which are incorporated herein by reference.
A simpler option is simply to provide separate long and short range visible laser diodes, as is suggested in our earlier patent U.S. Pat. No. 5,420,411.
A further problem associated with known arrangements is that of distinguishing the respective images received corresponding to objects in each working range.
The present invention, in various other embodiments, further relates to optical scanning stations having a conveyor for moving articles carrying indicia to be read past an optical scanner, and to optical scanners having means for manually or automatically selecting one of a plurality of desired scan patterns.
The invention further relates, in yet further embodiments, to scanners having an extended working range using two lasers, each focused to cover a different portion of the scan distance. Present systems turn on one laser for a full scan, and then the second laser for the next scan, alternating on a scan-by-scan basis. Since, in general, only one of the lasers is capable of reading a bar pattern at any given distance, this technique typically doubles the length of time that it takes to generate a successful decode over single-laser embodiments. There is a need to regain the aggressiveness of a one-laser scanner, while maintaining the range benefits of the two-laser system. One device making use of two lasers is disclosed in our application Ser. No. 08/405,585, filed Mar. 17, 1995, now abandoned, the disclosure of which is incorporated herein by reference.
Objects of the Invention
It is an object of the present invention at least to alleviate the problems of the prior art.
It is a further object to provide a multiple working range optical system, for example for a scanner arrangement capable of distinguishing between respective images corresponding to images in different working ranges.
It is yet a further object of the invention to provide a multiple working range optical scanner arrangement having a minimum of imaging and image-recording elements.
It is yet a further object of the invention to provide an optical scanner capable of being easily and conveniently mounted for optimum operation and user comfort.
It is yet a further object of the invention to provide a convenient and easily-operable optical scanning station, for example for use at a point of sale.
It is a further object to provide an optical scanner capable of generating different scan patterns using a single scanning mechanism.
It is yet a further object to provide an optical scanner which maintains the range benefits of a two-laser system, while providing the rapid decoding typical of a one-laser system.
According to the present invention there is provided a multi scan-pattern optical scanner including a laser assembly for producing a plurality of laser beams of differing wavelengths and a scanning mechanism including a wavelength selector for selectively passing a beam of predefined wavelength, thereby producing at least a first scan pattern from a beam which is passed by the selector and a second scan pattern from a beam which is stopped by the selector.
A device of this type allows for the creation of multiple scan patterns without the need to have individual scanning mechanisms for each pattern. In a preferred embodiment, parts of the scanning mechanism are coated or otherwise provided with filters to absorb, or to prevent the reflection of, at least one of the beams. Alternatively, parts of the mechanism may be coated so that only those coated parts reflect one of the beams. Preferably, the coatings may be thin coatings which achieve their reflective/absorptive effect by optical interferences.
It would also be possible to provide holographic optical elements and/or diffraction gratings to separate two laser beams of differing wavelengths, and thereby allow them to be deflected differently by a single scanning mechanism.
Preferably, each laser is provided with its own optical assembly, providing individual focusing and allowing each laser to scan efficiently at a given working distance. To extend the overall working range even further, more than two lasers could be used, each having its own working distance.
The invention extends to any individual feature described above or set out in the specific description, and to any compatible combination of features. It is to be understood, in particular, that features shown in relation to one figure may be combined, where compatible, with features shown in connection with any other figure.
The invention may be carried into practice in a number of ways and several specific embodiments will now be described, by way of example, with reference to the accompanying drawings, in which:
Referring first to
The lens system shown in
Associated with each lens element L1, L2 is a respective spectral narrow band filter NBF1, NBF2. The filters NBF1, NBF2 are arranged to pass different wavebands of light received from the objects S1,S2. As a result the images of the objects S1, S2 at plane P are composed of light of different wavelengths and can be resolved from one another. In order to do this, the system is provided with additional movable, filters NBF1′, NBF2′. Each filter can be moved into position in front of the detector D to allow light of the relevant wavelength to pass dependent on which working range is selected. If the working range W1 is selected, light from the object S1 passes through the lens element L1, is filtered at NBF1, and then passes through the movable filter NBF1′ (now in position in front of the detector D); light which may have passed through NBF2 and lens element L2 is blocked at NBF1′ and so cannot form an image at D. If the working range W2 is selected, NBF2′ is moved into position, and S2 is imaged; light from S1 passing through L1 and NBF1 is then blocked at NBF2′.
The scanner of
In order to modify the bar code scanner a multiple working range optical system described in detail below is included in the system. The system can be inserted at an appropriate point in the path of the light beam reflected from the indicia 9, for example between the window 7 and the collecting mirror 10 or between the collecting mirror 10 and the photodetector 11. Indeed components of the standard bar code scanner such as the collecting mirror can be removed and replaced by the optical system according to the present invention.
The arrangement of
It will be seen that the scanner 20 is mounted on a strap 23 and, as shown in
It will be seen that this arrangement can be advantageously used in association with the multiple range optical scanner system described above; the working ranges of the scanner can be determined to correspond with parameters determined ergonomically by the user; for example a first working range can correspond to the arrangement shown in
In a further preferred option the scanner 30 can be detechably mounted on the arch 33 for example by including resilient gripping means on the arch 33. Accordingly the scanner 30 can be removed from the arch 33 and held in the user's hand 38 as shown in FIG. 4b. The end face and scanning window point outwardly away from the user's body and a control button 39 is placed on the planar side face so as to be easily operable by the user's thumb. The curved surface of the scanner 30 then fits snugly and comfortably into the user's hand 38. The scanner 30 can be simply aimed at an article to be scanned and operated by actuating button 39. As a result the scanner 30 can be used in a wide variety of applications and in particular, for example, applications where items are too bulky or heavy or inappropriately positioned to be passed under the arch 31 and scanned.
The scanner 20 includes a light source 43 such as a laser or LED and a scanning mirror 44 which is rotated in a known manner to oscillate about an axis A. The light beam 45 generated by the laser 43 is reflected by the mirror 44 through the scanning window 42 onto a printed indicia such as a bar code symbol 46 to be read. Light reflected from the bar code symbol 46 passes back through the window 42 and is reflected once more by the mirror 44 via the lens system L1, L2 onto a detector 47 such as a CCD array aligned with the image conjugate plane P. As discussed above, narrow band filters NBF1′, NBF2′ are associated with the lenses L1, L2 respectively and can be moved in the direction implicated by the double-headed arrows in and out of position in order to select a desired working range. The filters are mounted for reciprocal movement by means of a rack 48 which is driven back and forth by a toothed wheel 49 driven by a motor and controller (not shown). Of course, any suitable method can be used.
It will be appreciated that the lens elements L1, L2 can be replaced by any suitable optical arrangements such as holographic elements, prisms or gratings. The narrow hand filters may be of any known type.
The desired working range can be selected manually by user input, or automatically by identifying for which working range an object is focused, for example by introducing each of the filters in turn and ascertaining which of the narrow band images is in focus.
An alternative scanner housing is illustrated schematically in
The scanner housing of
The housing incorporates front and rear feet 110,112, enabling the scanner to be laid down in the position shown on a flat desk top or other surface 114 (FIG. 6a).
One method of achieving multiple working distances, for example within a bar code scanner, has already been described with reference to FIG. 1a. Reference should now be made to
This embodiment incorporates dual laser assemblies 1310, 1311 emitting parallel beams. The laser assembly 1310 is focused for short-range operation. This will be referred to, for shorthand, as the “short-range laser”. Similarly, the laser assembly 1311 is focused for long-range operation. This will be referred to, for shorthand, as the “long-range laser”. Appropriate optics 1312, 1314 define the working range and different beam profile characteristics of the lasers. Alternatively, the short-range laser, and its optics, may be identical with the lone-range laser and its optics.
The beam from the long-range laser 1311 is reflected by a pair of parallel angled mirrors (or by an appropriately shaped prism) so that the two resultant laser beams are closely parallel to each other. The beams impinge upon a scanning mirror 1322 from which they are reflected onto an indicia to be read (not shown, but off to the left of the drawing in FIG. 11).
Instead of there being separate long range and short range lasers, a single laser could be used instead with appropriate optics (for example a beam splitter).
Light reflected back from the indicia is collected by the mirror 1322 (which acts as a collection mirror as well as a scanning mirror) and is directed to a photodetector 1324).
Details of the mirror 1322 are shown in FIG. 12. As will be seen, the mirror is generally curved, and includes a large area of collecting surface 1323 with a central section which is split into two. The left side of the central section 1325 has a cylindrical profile, and the right hand section 1327 a flat profile. The light beam from the short-range laser 1310 impinges upon the portion 1325, and the light from the long-range laser 1311 impinges upon the portion 1327.
In use, a laser control 1326 operates the lasers so that they are switched on and off alternatively. The system is controlled so that two scans (left to right, then right to left) are performed with the long-range laser on, and then two scans with the short-range laser on. The alternation continues until a successful decode has been achieved.
The system also provides for an aiming mode which is initiated by a user selecting a first position of a trigger 1328 on the scanner housing 1330. In this mode, the controller 1326 causes the long-range laser 1311 to blink on and off while moving the mirror 1322. In this mode the user can easily see the scanning beam and he can align the indicia accordingly. As soon as the indicia has been properly aligned with respect to the scanner, the user moves the trigger 1328 to a second position to commence scanning proper.
In another embodiment, the laser assemblies 1310, 1311 have lasers of different frequencies. Visible laser diodes are now available in two different wavelengths, 635 mm and 670 mm. The shorter wavelength device (635 mm) is more visible to the eye, and may preferably be used in high ambient light conditions or for aiming. Thus, in the preferred implementation, the 670 mm laser diode could be focused as the “short range laser” and the 635 mm laser diode focused as the “long range laser” since at long range the brightest beam is desirable for visibility and aiming. In high ambient light conditions, it is possible to use both lasers on, rather than alternate between the lasers. Although there will be two beams, if the beams are properly focused at the target plane so the spots are overlapping or very closely adjacent, the bar code symbol can be effectively read.
In still another embodiment, one of the laser assemblies 1310, 1311 is a visible laser and the other assembly an IR laser, whose beam is generally not visible to the eye. IR lasers are suitable for use in applications such as reading security badges that require an IR reading beam, reading direct thermal printed bar codes; and reading certain colored bar codes. The same arrangement as shown in
Yet another embodiment is shown in FIG. 7. Here lasers 201,202 are used, each having its own separate focusing optics 203,204. The optics differ in focal length, giving the two laser beams 205,206 differing points of focus and hence differing working ranges. Both beams are scanned by a scanning mechanism such as an oscillating mirror 207, and are directed towards an indicia 208 to be read. It will be understood that because of the differing focus lengths of the optics 203,204, only one of the two scanning beams will properly be in focus at the indicia 208. If the distance to the indicia is small, the beam corresponding to the optics of shorter focal length will be in focus; if the diameter is large, the other beam will be in focus.
Light 210 which has been reflected from the indicia 208 is collected by a collecting mirror 211, and passed to a photodetector 212. This produces an electrical output signal on a line 213 which is representative of the changes in intensity within the reflected light.
The lasers 201,202 are repeatedly pulsed by a controller 260, at the same rate but out of phase so that one laser is on while the other is off. The controller also sends a signal along a line 261 to a time divisional sampler and demultiplexer 214 which accepts as input the signals on the line 213, and separates them out into a first pulse stream on a line 215 representing pulses from the first laser 201, and a second pulse stream on a second line 216 representing pulses from the second laser 202. In order to ensure that the sampling is accurate, the time division demultiplexer 214 samples at a rate greater than the Nyquist limit (twice the highest frequency contained in the signal on the line 213).
The individual pulse streams on the lines 215,216 are each individually processed by respective decoders 217,218 to provide respective high level outputs 219,220. The simultaneous processing/decoding allows for the indicia 208 to be decoded without delay, regardless of whether it is positioned at a distance suitable for scanning by the laser 201, or at a distance suitable for scanning by the laser 202. It will be understood, of course, that typically only one of the decoders 217,218 will produce a “valid decode” output for a given indicia at a given distance from the scanner.
The output signal on the line 213 is then sampled at 229, and the sampled signal is passed through the two bandpass filters 230,231. The filter 230 has a passband of f1 plus or minus fs, whereas the second filter 231 has a passband of f2 plus or minus fs. This filtering separates the output of the two lasers in the frequency domain, so that the output of the filter 230 on the line 232 represents the signal just from the laser 201, and the output from the filter 231 on the line 233 represents just the other laser 202. The two signals are processed/decoded simultaneously by respective decoders 234,235 to produce individual outputs 236,237. As before, this simultaneous decoding eliminates delay.
In either the embodiment of
Depending on the set-up of the lasers, the reflected light from the two regions may differ either in intensity, frequency, or pulsing frequency. Such differences provide a convenient way of discriminating between light which has been reflected from the individual regions, thereby enabling the two data streams to be conveniently separated. This applies whether the two regions are entirely separate from each other within the field of view, or whether they overlap.
It will be understood that both the embodiment of FIG. 7 and the variation of
In some implementations it may be desirable not only to change the working distance, but also to change the scan pattern generated by an optical scanner. This may be achieved by means of the embodiment of FIG. 9.
A laser 300 generates a beam 302 which is focused and shaped by beam optics 304 and directed to a stationary flat mirror 306. The beam is reflected from the mirror and onto a rotating polygon 308, which is driven for rotation about an axis 309. The reflections from the polygon produce a scanning laser beam 310.
The scanning beam next impinges upon an arrangement of fixed mirrors 312 in a crown configuration, with the various reflection 314 from the individual mirrors making up the crown, as the scanning beam 310 moves across, resulting in the omni-directional scan pattern shown in FIG. 10a. In order to achieve this pattern, all of the reflecting surfaces are appropriately coated to provide a high level of reflectivity at the wavelength of the laser 300 (preferably 670 nm).
The scanning mechanism shown in
By coating all of the relevant surfaces for reflection at 670 nm, and only some of the surfaces for reflection at 630 nm, two different scan patterns may be generated by user selection or automatic selection of the appropriate laser. Manual selection could be achieved by means of a user-operable trigger, such as the trigger 3 shown in
A further benefit of the method is that the 630 nm beam may be focused differently from the 670 nm beam.
It will be understood of course that more than two lasers could be used, each having a different wavelength. The described wavelengths of 670 and 630 nm, while preferred, could be varied if necessary accordingly to the particular application.
It will be appreciated, in connection with
While the optical system of
While the invention has been illustrated and described with reference to a number of particular embodiments, it is not intended to be limited to any of the details shown, since various modifications and structural changes may be made without departing in any way from the spirit of the present invention.
Without further analysis, the foregoing will so fully reveal the gist of the present invention that others can, by applying current knowledge, readily adapt it for various applications without omitting features that, from the stand point of prior art, fairly constitute essential characteristics of the generic or specific aspects of this invention. Accordingly, such adaptations should be and are intended to be comprehended within the meaning and range of equivalence of the following claims.
According to another aspect of the present invention there is provided an optical scanner for scanning indicia having areas of different light reflectivity, comprising:
By reflecting from an aplanar surface, any desirable beam shape may be achieved. If the reflector is shaped both in the X direction and in the Y direction, beam shaping in both dimensions may be achieved. Alternatively, if a cylindrical mirror is used, the beam may be shaped only in one dimension. The aplanar surface may comprise the scanning mirror, or alternatively a stationary fold mirror.
Proper beam shaping using a cylindrical mirror in this way can enable the designer to reduce the spot size in the vertical (Y) direction at large scanning distances. This improves visibility. In addition, spot size for near distances (0-30 inches) is increased, thereby improving dot matrix performance.
In addition, the shaping may be carried out by reflecting the light beam from one or more stationary mirrors either after or before the light has impinged upon a scanning element. In its most general form, beam shaping is carried out by reflecting the beam from one or more aplanar surfaces.
The indicia 426 is shown at three possible positions, a near position 428 corresponding to the working distance of the mirror portion 420, a middle distance 430 corresponding to the working distance of the mirror portion 418, and a far distance 432 corresponding to the working portion of the mirror portion 416. It will be appreciated, of course, that in a practical embodiment there will be considerably greater spacing between the positions 428, 430 and 432: in the drawing the spacings are shown closer than they would be in reality, merely for the sake of clarity.
The result of the three separate mirror portions is that three separate scan lines are produced, the first at the position 428, the second at the position 430 and the third at the position 432. The intention is, accordingly, that whatever the distance of the indicia 426 from the scanner, it has a very good chance of being read by at least one of the scan lines. It will be appreciated of course that the indicia does not need to be exactly at one of the distances 428, 430, 432 in order to be decodable; there is in each case a substantial depth of field, and depending upon the actual distances these depths of field may even overlap so that they effectively merge into one complete “working region” within which the bar code symbol will almost certainly be decodable.
The mirror portions are suitably angled so that the respective scan lines lie on top of one another, but are merely focused at different distances.
It is not essential that there are exactly three mirror portions; there could be two, or more than three, according to the requirements of the particular application. The exact mirror profiles may also be chosen according to the particular application (e.g., cylindrical). The profiles chosen will depend upon the required working ranges and also upon the profile of the scanning mirror 412. The scanning mirror 412 may preferably be flat, but may in some circumstances be aplanar, for example cylindrical or spherical. The mirror 412 could also be replaced by a rotating prism, polygon, hologram, lens, zone plate, or any other convenient optical scanning element. If the scanning element comprises a polygon, each facet of the polygon may have a different curvature. In that case, the mirror portions 416, 418, 420 may (but need not) all have the same profile since the curvature of the polygon facets. An exemplary polygon suitable for use with three planar fold mirror portions is shown at 436.
Further spacing of the beam may be achieved by the use of optics 438 in front of the laser 410.
In the embodiment of