A SCANNER SYSTEM FOR SUCCESSIVE IRRADIATION OF A WORKING SURFACE, PARTICULARLY FOR ULTRA-VIOLET EXPOSURE OF A PHOTO EMULSION ON A SERIGRAPHIC PRINTING FRAME

Abstract: For producing fine printing patterns on large serigraphical printing frames it is possible to apply an exposure through correspondingly large film areas, but it is cheaper to make use of a successive line-by-line exposure with the use of a modulated light or laser beam, which is caused to sweep across an emulsion coated printing frame surface from an oscillating deflection mirror. The beam (20), in its outermost positions, will be directed obliquely towards the surface (14), and if the latter changes its distance from the oscillating mirror (48) the exposure lines (16) will thus be correspondingly shorter or longer, whereby the printing pattern may be distorted. According to the invention this can be counteracted by the light ray being brought to pass a lense beam (56) mounted just in front of the line of exposure and adapted so as to deflect, all along the line, the light beam such that it will hit the surface perpendicularly, whereby the length of the lines will be independent of occurring distance variations. The width of the lense beam (56) should be at least twice the line width, as the invention also provides for a transverse displacement of the light beam for achieving that the latter may be delivered from a resonancewise oscillating goniometer mirror (48) with a high operational speed without overlappings occurring between the consecutive lines of exposure.

Description: A scanner system for successive irradiation of a working surface, particularly for ultra-violet exposure of a pnoto emulsion on a serigraphic printing frame. The present invention relates to a method of pre¬ paring graphical printing elements of the serigraphical printing frame type with a view to the production of a printing surface, which in accordance with a model pat¬ tern is formed with areas which are permeable and non-permeable respectively to dye. In this field it is common practice to lay out a photographic emulsion on the permeable fabric layer of a serigraphic printing frame and to cover said emulsion with a photographic film indicating the desired print picture in full size, after which the assembly is irra¬ diated with powerful ultra violet light for exposing the emulsion on the fabric layer through a contact print of the film picture, so that afterwards it is possible to treat the emulsion in such a manner that it becomes selectively permeable to dye in accordance with the desired pattern. However, this is a troublesome and expensive pro¬ cess, a.o. because it may be expensive to produce the required films in the relatively very large sizes which may occur, e.g. with edge dimensions essentially exceed¬ ing 1 metre both lengthwise and crosswise. The invention is based on the acknowledgment that it is possible to affect the photographic emulsion in a more direct manner, i.e. by irradiating it with a con¬ centrated light beam, which is controlled so as to de¬ scribe the desired print picture on the print surface. Typically a laser beam may be applied which from a transmission head is caused to sweep over the surface of the emulsion by a scanning process which by an asso- ciated computer control produces just the desired print¬ ing pattern, without the latter having to be present in full size * It has been found, however, that such a scanning cannot easily cover a lane area with a width of more than 50-60 cm, which is far too little in the perform¬ ance of many relevant tasks of printing, for which reason it has been necessary to operate with said con¬ tact prints in case of broader subjects. The width limi¬ tation in question is due to certain basic limitations of a modulated scanning; in connection with the inven¬ tion it has not been found possible to alter said limi¬ tations. On this background the invention proposes to carry out the preparation of an extended emulsion coated print surface by successively, irradiating said area from a beam head in parallel, adjoining lanes of limited width, provision being made to control the operation in such a manner that the individual lane portions are coherent as to the motif. In order to obtain a reasonably good result, i.e. without essential visible distortions of the print pat¬ tern in the border line areas between the various scan¬ ning lanes, it is not sufficient to carry out an accu¬ rate mechanical guiding of a scanner head with relation to the print element, as more problems in connection with the scanning process are associated with the pro¬ duction of such an accurate side bounding of the scan¬ ning lane, that this lane can fulfil the requirement of accurate merging with the adjacent lane or lanes. In case of a single lane edge displacements of the order of 1 mm will normally be insignificant, whereas such dis¬ placement will be quite unacceptable in case of for example a vertical border line inside a print pattern surface, where the aim should be to keep possible dis¬ placement below 0.1 mm, as otherwise visually noticeable border lines may be formed even in coarse print pat¬ terns, though it may be difficult to concretely show the presence of such border lines. Therefore the present invention also deals thor¬ oughly with the scanner itself, as an improved version thereof is almost a condition of making the invention broadly applicable, which, of course is the result aimed at. Therefore this important aspect of the invention will be discussed in detail below. The invention will be explained in more detail in the following with reference to the drawings, in which Fig. 1 is a schematic, perspective view illustrat¬ ing the principal invention. Fig. 2 is a perspective view of a system for execu¬ tion of a scanning in accordance with the invention, Fig. 3 is a perspective detail view of a scanner unit used in said system, Fig. 4 is a detail view of the output end of the scanner opposite the working surface, Fig. 5 is a detail view for further explanation of Fig. 4, Fig. 6 are graphical curves illustrating movements of an oscillating mirror used in the system, and Fig. 7 is a graphical picture of the light spot path on the working surface. Fig. 1 illustrates schematically a serigraphical frame 1 placed below a laser scanner 2, which sweeps across the print surface of the frame along a transverse line 3 which is considerably shorter than the width of the print surface. The print surface is coated with a photographic emulsion which is meant to be irradiated for the production of the print pattern indicated by outlines; of course said pattern may assume any other form. The scanner 2 is so mounted with relation to the frame as to be displaceable both lengthwise and trans- versely across the print surface of the frame, but con¬ trolled to move very accurately parallel therewith, so that the length of the scanner line 3 will be the same everywhere at the occuring angular oscillation of the laser beam from the scanner. The ideal situation would be one, in which the scanner can be moved a single time across the middle of the frame and all the way produce the line 3 with a length that is sufficient to cover the whole width of the printing surface, whereby the desired printing pat¬ tern can be produced by a suitable computer controlled modulation of the light beam. Only it appears in prac¬ tice that the obtainable length of line is so limited that it cannot be extended to the entire width of only fairly large printing surfaces. In the light of this the invention provides for controlling the scanner to move in such a manner, rela¬ tively, that it can work the printing surface along parallel partial zones or lanes shown in the drawing separated by stippled lines a. With a suitable program¬ ming of the control computer it can be obtained that the scanner is moved successively along the respective zones to irradiate these zones for producing the partial pic¬ tures of the print motif associated with said zones. Hereby it is insignificant whether the absolute length of the line 3 is somewhat larger than the width of the zones, if only it is secured that the laser beam is extinguished in the areas where it is potentially di¬ rected towards adjacent zone areas which should not be irradiated in the cycle of operation in question. Referring to Fig. 2 it is shown how a system for the execution of the method may be arranged. The system comprises a wall mounted frame 4 with vertical guide members 5, between which is mounted a vertically dis- placeable cross rail 6 provided with sliding sleeves 8 which embrace the guide members 5, means not shown being provided for causing a downward movement of the cross member 6, 8 along the guide members 5 with a smooth, relatively low speed and an upward movement with sub¬ stantially higher speed. A horizontally displaceable carrier 10 for a scan¬ ning device 12 is mounted on the cross rail 6. The car¬ rier 10 is in a manner not shown provided with a motor part for controlled movement of said part and hence the scanner 12 along the cross rail 6. A working subject 14 in the form of a serigraphic frame with a photo emulsion coating to be treated by irradiation from the scanner 12 may be placed on the wall surface within the frame 4, it being shown that the scanner 12 can work said surface by irradiating it in horizontal lines 16 downwards along a vertical lane field 18, as a light beam 20 oscillating backwards and forwards is supplied from the scanner 12 during the moving down of the scanner on the cross rail 6. The speed of moving down is so adjusted that the lines 16 of irradiation will be drawn edge to edge as seen in relation to the oscillating frequency of the beam 20. On a lower, fixed support 22 on the frame 4 a UV-laser 24 is mounted which is provided with a power supply line 26 and has a modulator 25 connected through a line 28 to a control unit 30 for switching the laser beam designated 32 on and off, the control unit being connected to a computer 34, in which the desired print pattern can be recovered. Further in a manner not shown the computer 34 or the control unit is connected to the means for moving the carrier 10 of the scanner and for vertically moving the cross rail 6. The laser beam 32 hits a fixed deflecting mirror 36, which directs the beam vertically upwards along the right side of the frame 4, where it hits a second mirror 38 placed on the right sliding sleeve 8, from which it is transmitted to the scanner 12 through an opening 40 in the side thereof. Within the scanner the beam passes various lens and mirror systems as described below with the result that it finally appears an an oscillating beam directed towards the subject 14. It will be under¬ stood that by means of a very accurate construction of the mechanical system it is secured that the laser beam all the time is introduced into the scanner on the same place and with the same direction, no matter how the scanner is moved vertically and horizontally. In a system as described above it would in prin¬ ciple be possible to use a scanner 12 of a previously known construction, but in most cases for the result would be highly useless for two reasons, i.e. partly because the prior art scanners operate either far too slow to be practically usable for the present applica¬ tion, or much too inaccurate to produce sharply linearly limited working zones, which can be joined to adjacent zones without clearly visible transitions. Therefore, according to the invention it has been considered necessary to make use of a further developed scanner; the problems presenting themselves in connec¬ tion therewith shall be explained in more detail in the following:- In the scanning process several essential problems occur when an ultra violet laser beam is used and when print patterns of high quality, i.e. high degree of resolution of the pattern, are desired. The production of ultra violet light is rather costly wherefore reduc¬ tion of the losses to the least possible should be aimed at, and the demand for a high degree of resolution in¬ volves the need of working with a rather accurate focus¬ ing of the laser beam on the print element. This demand is difficult to meet in the desirable extremes, as cer¬ tain basic problems in relation to an accurate focusing occur as a consequence of 1) that the laser beam is subjected to changes of direction between a point of deflection and a line segment sweeped by the beam on the receiving surface, whereby the length of the beam and hence the focal point will change all the time as seen from the planar receiving surface, 2) that the focal point of the beam may be outside a larger or smaller part of the receiving surface, unless this is placed at a very accurate prescribed distance from the scanner, 3) that during their runs back and forth the scanner lines will overlap each other in the reversing areas making it difficult to produce unambiguous print patterns in these areas, 4) that the same overlap gives rise to a notice¬ able power problem, because double power is dissipated in said overlap areas, and 5) that the prior art scan¬ ners are rather slow in operation. An associated further purpose of the invention is to provide measures for- extensive remedy of these ad¬ verse conditions, i.e. to provide a scanner, which is able to operate fast and with an accurate focusing while maintaining an almost maximum and extremely well defined working width. Generally, for various reasons it is difficult to operate with an accurate scanning, when the effective working width exceeds about 40 cm; though the invention involves aspects that might contribute to improvement also of this condition, this is not to be further discussed here. Light scanning is most frequently performed by using a rotating polygon mirror hit by a light or laser beam, which beforehand has passed a focusing lens and by the successive passings of the rotating mirror facets is caused to sweep across the surface to be treated. The surface is moved relatively to the scanner in the trans¬ verse direction of the lines, which the scanner hereby "draws" on the surface, whereby ' a larger area can be treated successively. When the beam is modulated, while the light spot is running through the individual lines, i.e. is switched on and off or intensity controlled from an associated control unit, the desired pattern of treatment can be produced with more or less accuracy according to the quality of the scanner. The beam length between the focusing lens and the working surface will be shortest for the beam which in the center position of the mirror facets impinges on the surface at right angles, whereas the length increases towards both sides. If the focusing is sharp in the center area, it may in case of a fairly large working width be difficult or impossible to obtain sharp focus¬ ing in the outer areas, unless the working surface is curved on a cylinder face with the axis going through the focusing lens. However, this problem, also mentioned under 1) above, has already been solved in principle, i.e. by the application of a correcting optics, which is passed by the oscillating beam and varies its focal length, i.e. the distance to the focal point, according to the swing angle, just so that the focal point can be held on a planar surface fairly uniformly all over the line. In return the working surface must then be posi¬ tioned at the distance in question from the lens or from the device as such. A certain slight variation of the distance may be tolerated, which also is needed in prac¬ tice, but this immediately entails another problem, i.e. that a slight increase in the distance will mean that the increase in length of the outermost swung out beams in the angle position in question will be larger than the increase in length of the center beam. This has two adverse effects, i.e. partly that the possible range of variation of the position of the working surface is limited by the fact that it must be within the depth definition of the outer beams, and partly that a change of position of the working surface will means not only a relatively larger change of length of the outer beams, but also a corresponding change of the effective length of the working line on the surface; when the distance is increased, the outer beams will reach farther out on the surface, and if during the movement of the scanner rela¬ tive to the surface the distance variations in question occur, the result will be that the working width will vary so that straight lines, which in the outer areas of the working lane extend in the longitudinal direction thereof, will be correspondingly distorted or wavy. This presents a problem in itself, but particularly so when entire working lanes shall be caused to join each other very accurately, as in case of the technique which is the primary aspect of the invention. A genuine¬ ly accurate print will require a practically- unrealistic accurate set-up of the working surface relatively to the scanner and to the applied moving means. According to the invention the beam is caused to pass an optical system at a short distance outside the working surface, preferably a lens bar which is adapted to deflect the beam everywhere in such a manner that all over the length of the working line it impinges perpen¬ dicularly on the working surface. Thus the lens will be a convex lens with its focal point positioned in the area such as said polygonal mirror, from which the beam is oscillated. Thus, this lens must extend throughout the working line, i.e. it is a fairly large optical element, but apart from the length dimension the element may be of a rather moderate size, as it is to operate exclusively with a beam which is oscillated in a fixed plane rela¬ tively to the scanner, i.e. the lens bar may have a thickness of e.g. only a few millimetres. When the beam all the time is delivered perpendicularly onto the working surface, a possible slight deviation of the distance of the working surface from the scanner as seen along the said working lane will not cause any distortion of the print pattern; in case of such a deviation the outer beams will not hit the working surface correspondingly farther out or in, and the length of the working line will remain constant. In addition an improvement with relation to the other problem is obtained in that the length of the outer beams are not shortened, as they are now sent from the lens directly, not obliquely towards the surface. Though this shortening is not very large, it still means that the depth definition range can be utilized better when not limited by a slanting of the outer beams. Thus the result is that hereafter it will be pos¬ sible to perform the work extremely accurately, e.g. with degrees of resolution of less than 1/10 mm, without the need of overwhelming accuracies with respect to the positioning of the working surface; the distance of this surface from the scanner may vary several millimetres or even a few centimetres. The demand for the high degree of resolution in¬ volves another aspect, viz. that very thin focusing beams must be used, e.g. with a thickness of 25 microns, and as the working lines should be closely adjoining in order to ensure full continuity of the print, the speed of operation understood as the speed of displacement along said working lane will be determined by the velo¬ city with which the working lines can be terminated successively for yielding their respective contribution of e.g. 25 microns to the displacement. It goes without saying that the working lines must be produced with a quite high frequency in order to enable operation with a fairly realistic velocity. Obviously quite high line frequencies can be obtained by application of a rotating polygonal mirror, though centrifugal forces set certain limits to the speed of rotation, but in the use of rota¬ ting mirror facets considerable losses occur, which are unacceptable when, as in the present invention, ultra violet light is primarily applied which is expensive to produce. The explanation of these losses is that at each passage of a corner between two mirror facets past the incident laser beam having a certain thickness, which considerably exceeds the 25 microns mentioned by way of example, a splitting up of the beam between the two facets takes place, and while this is going on, neither of the beam parts will be usable for effective opera¬ tion, i.e. the beam should be switched off in this tran¬ sitional phase, which according to the circumstances may occupy a considerable percentage of the operating time. Thereby the switching off will not bring about any es¬ sential saving, as the laser device in itself has to operate with full power in the meantime. As an alternative to the rotating polygonal mirror it is known to use an oscillating goniometer mirror, which is in permanent contact with the incident beam and can be vibrated in a controlled manner to produce a back and forth swing of the light beam without the occurrence of said ineffective operating phases. Within certain limitations these single mirrors can be controlled to perform a backward and forward turning with constant angular velocity, whereby there will be a linear relation between the turning and the travel of the light spot along the working line, so that there is no unlinear function to be paid regard to in the pro¬ gramming of the print pattern. However, it is signifi¬ cant to the speed of operation of such mirrors that a short ineffective period must necessarily occur each time the mirror is turned to an extreme position and thereafter is to be turned back. Even this condition sets a noticeable limit to the speed of operation, and it must be realized that the line frequency obtainable in this manner is much too low to permit operation with a practically acceptable velocity. It is already known that the oscillating frequency of goniometer mirrors can be increased quite essentially by the application of a resonance system, whereby the mirror oscillates with a sinusoidal characteristic. Mirror oscillations with such a high frequency would be desirable in connection with the invention, but then the problem arises that due to the non-constant angular velocity of the sine function a non-linear speed of movement of the light spot on the working surface will occur, and it appears to be difficult to program a com¬ puter to take this non-linear relation into account, though this would be a possibility according to the invention. The invention provides a quite different possibility, i.e. the application of an optical correc¬ tion, the swinging beam from the oscillating mirror being passed via at least one fixed mirror, the mirror face of which is so shaped that the beam reflected therefrom will swing with a uniform angular velocity, when the incident beam oscillates with an angular velo¬ city according to a sine curve, whereby the desired alteration of the characteristic of the movement will be obtained. Another and more essential problem in the appli¬ cation of a beam oscillating with a non-uniform angular velocity is the fact that the light spot will be moved with uneven velocity along the working line, the veloci¬ ty in connection with a sinusoidal oscillation being maximum at the center of the line and quite low at the outermost end or turning areas. If the relative movement between the scanner and the working surface takes place with a uniform velocity in order that the successive working lines shall adjoin each other edge to edge over a fairly broad center area, then the lower travelling velocity of the light spot at the outer areas will cause an overexposure in these areas. This can be remedied in that the outer areas are made ineffective by switching off the beam, but as mentioned above such switching off will imply a appreciable loss of efficiency, if it ex- tends over a considerable time, as the laser device is operating continuously. Thus the uniform speed of move¬ ment and an only slight lateral overtravel are a primary condition of avoidance of such losses. However, by using oscillating mirrors, which in some way produces a light spot travel with uniform velo¬ city along the working line, a still larger problem may occur, viz. a possible overlapping of the paths of move¬ ment of the light spot in connection with each turning of the light spot movement some distance before and some distance after the turning, as these paths having a certain width are entirely coincident in the very turn¬ ing points. If or when- the paths, i.e. the working lines, are to adjoin each other edge to edge at the center of the field, viz. by displacing the scanner relative to the working- surface with a velocity of one line width per half oscillation of the beam, these over¬ lap areas will extend nearly throughout the length of the working lines, varying between full overlapping at the ends and no overlapping exactly at the center of the field. This presents almost impossible control condi¬ tions, wherefore it may be more appropriate to prefer the solution allowing the working lines to be completely parallel with each other by the application of a rota¬ ting polygonal mirror. To solve this problem it will be in any case a theoretical possibility to make provision for holding the oscillating mirror still for a very short period in each of its outer positions and for utilizing this short period to advance the scanner/working surface a distance just corresponding to a line width, whereas that advance is suspended during each line passage of the light spot. However, for several reasons this will presumably be totally unrealistic? hence this solution will not be further discussed. However, the present invention provides an extreme- ly simple solution of the problem in question, viz. the provision of such a control of the light beam in a plane perpendicular to its plane of oscillation that the light spot at the termination of each swing is displaced one line width transversely of the working line, while the beam and hence the light spot during the tracing of the subsequent working line is corrected in the transverse direction to a position edge to edge relatively to the preceding working line. With the simplest kind of con¬ trol this will be reflected in the working lines being perpendicular to the direction of displacement between the scanner and the working surface, that is irrespec¬ tive of the fact that this displacement is maintained with uniform velocity during the entire process; an overexposure will occur only in the turning points, where the light spot stays at the transition from the end point of the working line to the short transverse movement to the start point of the succeeding working line. For a perfect operation the beam should be switched off just in this transition area, but in view of the fact that the extension thereof is of the order of 20-30 microns unlike an essential part of the total length of the working line, this necessary switching off will not mean any considerable loss of energy or any significant narrowing of the effective working width. The transverse displacement in question of the beam or light spot is of such a small size that it can be produced by means of an almost microscopically small movement of a mirror in the beam path, and in a pre¬ ferred embodiment a mirror mounted on a piezoelectric crystal in front of the goniometer mirror, i.e. at a fairly long distance from the working surface, is used for this deflection. It will be understood that a micro¬ scopic movement will suffice here, when the beam spot is to be swung 20-30 microns from a distance of maybe half a metre. The same transverse displacement mirror can by suitable control of said crystal be caused to bring about such corrections of the beam direction which might be desirable to correct irregularities in the remainder of the optical system with a view to bringing about a working line which is rectilinear in an almost absolute sense. Summarizing the transverse control of the oscilla¬ ting beam makes it practically possible to utilize a back and forth swinging deflecting mirror with negli¬ gible losses, and by means of the optical transformation of a sinusoidally oscillating light or laser beam to a working beam, which is parallel displaced with a uniform velocity all along the working line, several advan¬ tageous effects are obtained, viz. partly a very high capacity of work by the application of a resonance oscillating deflecting mirror, partly a very high effi¬ ciency of the system, because an operative switching off of the beam may be limited to extremely short time in¬ tervals, partly an accurate focusing of the beam all over the length of the working line, and partly a well defined and exactly linear merging of the side edges of the individual working lanes, when these are set up edge to edge for forming broad working faces. Within the scanner, Fig. 3, the laser beam 32 pas¬ ses first a focusing lens 42 and thereafter hits a mir¬ ror 44, which is firmly mounted on a piezoelectric crystal in a housing 46, from which the beam is directed towards a vibrating mirror 48 connected to a goniometer. This mirror oscillates laterally as a resonance oscilla¬ ting goniometer mirror thereby transmitting the now oscillating beam designated 20. This beam is directed towards a primary mirror 52, from which the beam is reflected to a secondary mirror 54 and thereupon re¬ flected forwardly through a bar lens 56 for incidence on the print frame 14. The focal length of the focusing lens 42 is so adapted that the beam 20 will be maximum focused, e.g. down to a width of 25 microns, at the incidence on the print frame 14. Thus, during a vertical movement of the scanner 12 the lane field 18 on the print frame will be exposed by the back and forth swinging beam 20 which by means of the control unit 30 will be switched on and off for the production of desired differentiated pattern details. After the exposure of the lane field 18 the scanner 12 is moved to an adjacent position on the cross rail 6, so that thereafter another lane field 18 adjoining the previous one can be exposed. In this way the entire print frame can be exposed by use of the required number of horizontal shiftings of the scanner 12, hereby it only is very important that the respective side edge areas of the lane fields are exactly coincident. As previously mentioned a first problem hereby is that the working surface or print frame 14 hardly can be placed at an entirely accurate and uniform distance from the scanner, so that problems with respect to varying length of lines 16 may arise. This problem is met by the application of the bar lens 56, this lens as shown in Fig. 4 being so arranged that at every place it deflects the oscillating beam 20 in such a manner that said beam everywhere is directed perpendicularly onto the working surface, whereby the length of line will be independent of, whether the working surface is spaced more or less from the scanner. Fig. 5 shows in more detail that the beam 20 will pass perpendicularly on to the working surface also at the outer ends as indicated by 20', and it will further¬ more be seen that the point of incidence of the beam 20' on the working surface 14 will be the same whether this surface is spaced a little more or less from the scan¬ ner. The outer oblique beam 20 would in the absence of the bar lens 56 continue as shown by 20" with a point of incidence A on the surface 14; if the surface is with¬ drawn to the position shown in a stippled line, this point would obviously be displaced outwardly to the point B, whereby the previously mentioned drawbacks would arise. Furthermore it will be seen that the beam 20" is slightly longer than the beam 20', so that by the use of the lens 56 a more uniform focusing on the work¬ ing surface all along the working line is obtained. The goniometer mirror 48 performs rapid resonance oscillations, i.e. with an angular velocity varying in accordance with a sine curve as shown at the top of Fig. 6. The frequency of oscillation may be very high, e.g. 2-3 kHz, which is conditional of a usable capacity of the whole device, e.g. with a treatment time of about 5 minutes for a surface area of 1 m 2 . The sinusoidal oscillation is reflected only in a non-uniform velocity of movement of the light spot along the working line. However, the secondary mirror 54 is made with such a shape that it purely optically corrects for said non-uniformity, so that the oscillating beam leaves the mirror with a uniform angular velocity. The same correc¬ tion could be made at the primary mirror, but due to its narrower range of operation this mirror would be more difficult to form with exactly the required shape, which, of course, would be still more pronounced as regards the goniometer mirror. The correcting shape has not been further illustrated, but will be defined by the established conditions. The center curve in Fig. 6 represents the uniform and also rectilinear displacement of the picture point along the working line, i.e. the sine curve after the performed optical correction. The maxima and minima of the curve designate the opposite ends of the working line, at which points the curve has a locally rounded shape, as the turning of swinging direction of the beam cannot be carried out absolutely momentaneously. Thus distortions of the print may occur in the very narrow turning areas in question, but in a preferred embodiment these areas are eliminated from the working field by causing the control unit 24 to switch off the beam in said areas, which gives rise to a negligible loss only. As mentioned above there is another condition which might give rise to much higher losses or make the use of the resonance oscillating mirror 48 completely impos¬ sible, viz. the fact that at each turning the beam will produce a new working line, which will overlap the pre¬ vious line largely. The invention proposes to remedy this by controlling the piezoelectric crystal in the housing 46 to produce during the formation of each whole working line a slight progressive deflection of the beam 20 in a direction perpendicular to the swinging plane of the beam, i.e. in the direction of the axis of oscilla¬ tion of the goniometer mirror 48 with a rapid return to the start position at each turning of the beam. The associated pivotal movement of the mirror 44 is shown by the lowermost curve in Fig. 6. When the scanner is ope¬ rating with a downward movement, each working line 16 will from the beginning get to slope slightly downwards, but said control of the crystal to produce a slight upward deflection of the beam results in the lines 16 being drawn exactly horizontally, the total displacement in a vertical upward direction amounting to just a line width, i.e. the diameter of the focused ultraviolet beam. The quite abrupt return of the mirror to its start position will cause an almost entirely vertical and very nearly momentaneous swinging down of the beam, which is thereby displaced a line width downwardly, and during the immediately succeeding return swing of the beam the light spot will draw a new horizontal working line which in an ideal manner will be placed edge to edge with the preceding line entirely without overlapping or spacing between the lines, i.e. with a line drawing as ideal as in the use of a rotating polygonal mirror. The drawing of lines described here is illustrated in Fig. 7 in which said vertical and or turning move¬ ments of the lines 16 are designated 17. It is indicated that very small irregularities may occur in the swings of the beam 20, but particularly by using a resonance oscillating mirror it is possible to keep the irregular¬ ities so small as to be of no practical significance, even if a high degree of accuracy of the edge limita¬ tions of the working lanes 18 is required, when these lanes are to be joined as parts of one and the same print surface. Furthermore it has been shown in stippled lines a. that these lines between them delimit an irra¬ diated face of considerable width, on which a completely regular pattern of parallel, edge to edge adjoining lines 16 occurs; so it is sufficient to keep the beam switched off in quite narrow areas outside said lines a, which incidentally, of course, will follow the small irregularities of the position of the line ends. These very small, permanent switching off areas are condi¬ tional of working with very low losses, this being one of the very important advantages of the invention rela¬ tively to the use of polygonal mirrors. There will hardly be anything to prevent the pro¬ duction of a mirror goniometer, the mirror of which is able to swing in both one plane and the other for inte¬ grating the functions of the mirrors 48 and 44, just as the vertical deflection of the beam could be brought about elsewhere in the system, but just the application of a crystal controlled mirror must be assumed to be the simplest arrangement for the attainment of the desired result. Incidentally it should be remarked that an ex¬ tremely exact production or fine working up of the opti¬ cal elements is required to obtain an exactly recti¬ linear course of the working lines 16; just the use of the crystal controlled mirror 44 makes it possible to electrically introduce corrections of adverse bulges on the lines, which can be much easier than to correct the error in question in the optical system. It should be noted that it may be desirable to guide the scanner unit along laser beams in order that a perfect result shall be obtained.

Claims: C L I M S : 1. A method of preparing graphical printing ele¬ ments of the serigraphy frame type with a view to form¬ ing a printing surface, which in accordance with a model pattern is formed with areas, which are permeable and non-permeable respectively to dye, which forming is made by scanning with a light beam, preferably ultraviolet laser light, modulated from a control unit and directed towards a photographic emulsion placed on the printing surface, after which the printing surface is treated for development and fixation of the printing pattern, char¬ acterized in that a printing surface with a width ex¬ ceeding 20 cm and an arbitrary length is prepared for forming a continuous printing pattern by scanning along parallel lanes with respective accurately coincident side limitations, provision being made to control the operation in such a manner that the printing pattern is reproduced coherently across said side limitations. 2. A method according to claim 1, characterized in that said scanning along the individual lanes is per¬ formed successively by means of one and the same scan¬ ner, which is displaced longitudinally and transversely relatively to the printing element. 3. A scanning device for the execution of the method according to claim 1 or 2, characterized in that the scanning unit of the device or a plurality of such units are movable along parallel lanes, the side limita¬ tion lines of which are exactly coincident, and that an associated control equipment is adapted to ensure that a desired printing pattern is hereby reproduced correctly across said side limitation lines. 4. A scanning device according to claim 3, charac¬ terized in that at a short distance from the working surface the scanning unit is provided with a lens bar, which is placed in the plane of movement of the oεcil- lating light or laser beam, and which has the form of a convex lens with its focal point located in the rotating or oscillating mirror so as to direct the beam towards the working surface perpendicularly thereto all along the length of the working line. 5. A scanning device according to claim 4, charac¬ terized in that the width of the lens bar corresponds to at least twice the width of the working line, and that the scanning unit comprises a deflecting mirror of a forth and back swinging type and a controlled optical element, preferably a mirror element, for displacing the beam by a line width transversely of the plane of oscil¬ lation during each half period of the oscillation and for displacing the beam correspondingly, but abruptly and with an opposite sign at each end of the successive working lines. 6. A scanning device according to claim 4, charac¬ terized in that the oscillating mirror is of the gonio¬ meter controlled resonance swinging type, and that the optical system comprises means for producing from a beam deflection according to a sine function a final beam travel along each working line with constant velocity. 7. A scanning device according to claim 5, charac¬ terized in that the controlled optical element is a mirror mounted on a piezoelectric crystal. 8. A scanning device according to claim 7, charac¬ terized in that a control unit associated with the crystal is adapted to be programmed to correct the or¬ thogonal deflection in the optical system.

Inventors: ANDERSEN ALLAN VINCENT, ANDERSEN, ALLAN, VINCENT
Applicants: ANDERSEN ALLAN V, ANDERSEN, ALLAN, VINCENT
Application year: 1989
Main classification: G03F7
IPC codes: B41C1, G03F7, H04N1