Anamorphic laser scanning device
The invention relates to an anamorphic laser scanning device comprising a light source and means for generating a writing beam with a particular on/off frequency in function of particular data, e.g. text, photos, images. The invention also relates to a method for writing data on a medium, using an anamorphic laser scanning device according the invention.
The anamorphic system substantially reduces the imaging system's sensitivity to cross scan errors of the scanning optic by compressing the beam in the cross scan direction onto the scanning optic. The errors may be either fixed or random, such as wobble or pyramidal error. This technique is previously known in the art, as described in US patent number 3750189 (J.M. Fleischer) .
Anamorphic system laser scanning devices are known in the state of the art, as shown in Figure 1 and to now reference is made (Fig. 1 illustrates a schematic view of a prior art laser scanning device) . Such devices comprise a laser source (1) which produces a writing beam (2) and a polygon (5) which receives the laser beam.
The polygon (5) has a plurality of facets whereby only on is operative at a given time to reflect the writing beam (2) via an optical system (3; ; 5; 6; 7 ; 8 ; 9) towards an image plane (10) . Each facet is operative to scan at least one line of the plane.
In order for a laser scanning device to operate at high accuracy and resolution, it must accurately control the location of the writing beam (2) on the image plane (10) . Therefore it is known in current system on the market to work with two photocells (23; 24), whereby one photocell (23) detects the start of the scan and the other photocell (24) detects the end of the scan. The two photocell signals are fed into an oscillator (17) whereby the oscillator (17) generates a clock signal (18) in phase of the two photocell signals. The laser driver (19) switches the laser on or off in function of the clock signal (18) and the computer data (20).
Another known principle use the two photocells to detect the velocity of the scan line, this is used to modify a clock coming from a separate oscillator resident in the system electronics, which creates a pixel clock.
In a third known principle only one photocell is used at the start of the scan. This oscillator triggers a separate oscillator, which creates a pixel clock.
The disadvantage of the current systems, as shown in Figure 2 to which now reference is made (Fig. 2 illustrates the disadvantage of the prior art scanning devices) is that the two photocells (23; 24) measuring the total time between the start of the scan and the end of the scan (see Fig. 2b) . Out of this total time, a pixel clock is generated (see Fig. 2c) . However, if a polygon speed variation (as illustrate in Fig. 2a) occurs during the time from begin of scan and end of scan, than
this polygon speed variation will only be detected by the end photocell at the end of scan. Because on the one hand the pixel clock will not been corrected during the scan and on the other hand the laser driver will send the data on the wrong time to the laser, as a result the pixels will be placed on the wrong position on the image plane (see Fig. 2d) .
Also the systems described above cannot generally compensate for residual inaccuracies in the system design (image distortion) or for inaccuracies due to misalignment of the system optics.
Some of the current systems apply a fixed "curve" to create a non-linear pixel clock, so these systems can compensate for fixed errors (i.e. image distortion), but they can't still correct for changing inaccuracies, such as those due to speed variations, thermal misalignments or misalignments due to mechanical shock and vibration. Therefore it is the purpose of this invention to provide an anamorphic laser scanning device which is independent from speed variations in the polygon speed.
This purpose is achieved by an anamorphic laser scanning device comprising a light source and means for generating a writing beam with a particular on/off frequency, in function of particular data whereby the device comprises:
- a reference laser source for generating a reference beam, provided to follow at least a part of the optical path of the writing beam;
- means for detecting the position and/or speed of the reference beam;
- and means for controlling said frequency in function of the detected position and/or speed of the reference beam.
The reference beam is folded into the optical system and travels virtually the same path as the writing beam. If any inaccuracies (speed variation, distortion, misalignments) occur during the scan, than this variation is the same for the writing beam as for the reference beam. The difference between the path of the writing beam and the path of the reference beam occurs preferably after passing the final mirror.
In a preferred embodiment of the invention said detecting means comprises a reference scale and means for generating a reference signal indicating the position and/or speed of the reference beam relative to said reference scale.
According to a more preferred embodiment of the laser scanning device, the detecting means comprises a number of light detectors provided along the reference scale in order to detect the position and/or speed of the reference beam relative to the reference scale. The light detectors are preferable photo cells. The reference scale is divided into non-transparent zones and transparent zones, and the said light detectors are provided for generating a reference signal if the reference beam
travels through the transparent zone and reach said light detectors .
According to a specific embodiment said controlling means comprises an oscillator provided for generating a clock signal based on the reference signal and a laser driver provided for controlling the on/off frequency in accordance with this clock signal. The clock signal is preferable a pixel clock signal.
In a more specific embodiment of the scanning device according to the invention, the laser driver is provided for switching the light source on or off in function of the clock signal and the data stored in a computer memory.
In a most preferred embodiment the light source is a red laser. The advantage of a red laser is the fact that most media on the market is not sensitive for red laser light. As a result, any uncontrolled stray reference light will have no influence on the media. However, other laser colours can be used, if the eventually stray light is blocked from the media.
This patent application also relates to a method for writing data on a medium, using an anamorphic laser scanning device whereby :
- a writing beam is generated in accordance with particular data and with a particular on/off frequency; - a reference beam is generated such that is follows at least a part of the optical path of the writing beam;
- the position and/or speed of the reference beam is detected;
- the on/off frequency of the writing beam is controlled in function of the detected position or speed of the reference beam.
The characteristics and further advantages of the invention will be further explained on the basis of non- restricting exemplifying embodiments represented in the attached drawings and in the following detailed description. In this description reference is made to the following drawings in which :
- Figure 1 is a schematic view of a prior art laser scanning device;
- Figure 2 illustrates the disadvantage of the prior art scanning devices; Fig. 2a is a graphical representation of the polygon speed; Fig. 2b is a graphical representation of the start and end photo cell; Fig. 2c is a graphical representation of the pixel clock signal; Fig. 2d is a graphical representation of the pixels on the image plane;
- Figure 3 the anamorphic laser scanning device according an embodiment of the invention;
- Figure 4 is a detailed view of the reference means;
- Figure 5 illustrates the effect of the invention on the image plan when for example a speed variation occur during the scan; Fig. 5a is a graphical representation of the polygon speed; Fig. 5b is a graphical representation of the reference
signal; Fig. 5c is a graphical representation of the pixel clock signal; Fig. 5d is a graphical representation of the pixels on the image plane.
The device (25) according to the invention can be applied to expose one or several photosensitive plates over their entire width.
As represented in figure 3, the laser scanning device (25) consists of a light source (1) , preferably a red laser, and means for generating a writing beam (2) with a particular on/off frequency, in function of particular data (20) . The data (20) can be for example text, kanji characters, photographs or drawings and is stored in a computer memory (21) .
The laser emanate a writing beam (2) with a wavelength of e.g. 405, 532 nm. onto a cylindrical lens (3) after which the writing beam (2) become an anamorphic beam (2b) .
After being reflected by a mirror (4), the writing beam (2b) passes via a rotating scanning optic, e.g. a polygon (5), to a lens system (6). After passing the lens system (β) the writing beam (2b) reflects on a first folding mirror (7) to the final folding mirror (8). After reflecting the final folding mirror (8), the writing beam (2b) proceeds via a third mirror (9) to the image plane (10) .
The anamorphic laser scanning device (25) further comprises a reference laser source (11), e.g. 635 nm red, for generating a reference beam (12) . As shown in figure 3 the reference beam (12) is folded into the optical system and travels virtually the same path as the writing beam (2b) , obtaining all the same inaccuracies that the writing beam (2b) obtains. Instead of proceeding to the image plane (10), the reference beam (12) will travel, after reflecting on the final folding mirror (8), towards detecting means (13) for detecting the position and/or speed of the reference beam (12) .
The detecting means (13) comprises a reference scale (14) and means (15) for generating a reference signal (16) indicating the position and/or speed of the reference beam (12) relative to said reference scale (14). As shown in figure 4 the detecting means (13) comprises a number of light detectors (15) , preferably photocells, provided along the reference scale (14) in order to detect the position and/or speed of the reference beam (12) relative to the reference scale (14) . The reference scale (14) is divided into non-transparent zones (26) and transparent zones (27) . When the reference beam (12) passes through the reference scale (14) and is detected by the photocells (15) , the photocells (15) will generate a reference signal (16) .
The anamorphic laser scanning device further comprise means for controlling (17, 18, 19) said on/off frequency of the writing beam (2b) in function of the detected position and/or speed of the reference beam (12) . The
controlling means comprises an oscillator (17) for generating a clock signal (18), preferably a pixel clock signal, based on the reference signal (16) and a laser driver (19) provided for controlling the on/off frequency. The reference signal (16) is fed into the oscillator (17), the oscillator (17) will generate the clock signal (18) and the laser driver (19) switches the laser (1) on or off in function of the clock signal (18) and the computer data (20) .
The advantage of the anamorphic laser scanning device according to the invention is that if any inaccuracies for example speed variation of the polygon (5) , distortion, misalignments, ... occurs during the scan, than this variation is the same for the writing beam (2b) as for the reference beam (12) .
For example (see figure 5), if a speed increase (fig. 5a) occurs, the reference beam (12) moves faster over the reference scale (14). This generates a faster reference signal (16) (fig. 5b) into the oscillator (17) . The oscillator generates consequently a faster pixel clock (18) (fig. 5c) . This causes the laser driver (19) to write the pixels faster onto the image plane (10) (fig. 5d) . As a result, the pixels are positioned on a perfect distance from each other, regardless of the inaccuracies present .
It is also understood that the reference scale (14) could easily be placed near the image plane (10) so that the
reference (12) and writing beams (2b) do not have to separate before the final mirror (8) .