A METHOD FOR RECORDING SIGNALS ON BANDS BY MEANS OF LASER BEAMS AND APPARATUS FOR CARRYING OUT THE METHOD

Abstract: A method for recording character or marking signals by multi-beam laser technique, in which the characters are recorded in multi-rastered bands in such a way that the character information is inverted, whereby the recording surface is illuminated by the laser beams at each location that do not comprise characters or marks. In character locations the surface is not illuminated. The gaps between adjacent bands are illuminated by separate band gap illuminating laser beams. By using this method the electrophotographic image recording can be solved by means of conventional inexpensive positive copiers in which image reversal does not take place. The apparatus for carrying out the method comprises a Bragg cell, a control unit for producing several raster scanning laser beams, and oscillators for generating additional band gap illuminating laser beams. An inverting unit is inserted in the path between the information source and the control unit to perform electronic image reversal.

Description: A METHOD FOR RECORDING SIGNALS ON BANDS BY MEANS OF LASER BEAMS AND APPARATUS FOR CARRYING OUT THE METHOD Technical Field The invention relates to a method for recording signals on bands, by means of which signal information transmitted in digital form from a source can be record¬ ed in a suitable recording surface in bands wherein each band comprises a plurality of character raster lines. The main field of application of the invention includes electronically controlled character printers, text writing copiers and electronic film producing techniques. The invention relates also to an apparatus for carrying out the method. Background Art In the DE OS 2 755 575 a laser operated signal recording apparatus is described that comprises an acousto-optical cell utilizing Bragg diffraction for generating a plurality of simultaneously outgoing diffracted laser beams. The outgoing laser beams are projected on a signal recording surface by means of a suitable optical system and the beams are also deflect¬ ed to scan a band-like raster on the signal recording surface. The acousto-optical cell is controlled in accordance with the information defined by of the characters to be recorded, and the scanning beams illuminate the recording surface in locations that correspond to the presence of the characters. The areas that do not comprise characters are not illuminated at all. . This known apparatus provides for a fast information recording, and due to the application of a multi-beam raster the speed of its electronic circuitry does not have to be chosen above normal specification values. - . - There are a large number of conventional multi-beam information recording equipments including the above cited typical example that have- a common drawback which lies in that the recording surface is illuminated in locations corresponding to the position of the characters to be recorded. Usually in the recorded documents the character locations should have a definite shade that distinguishes them from the generally white shade of the carrier (paper). For ensu ing such properties in conventional laser operated recording equipments of the above type an electro¬ photographic image reversal is used, by means of which the recorded document comprises positive (black) sur- faces at the illuminated locations. The moans used for electrophotographic image reversal are substantially complex and expensive compared to the widely used document copying equip¬ ments intended for use in offices. In such equipments positive copies are produced without electrophotograph image reversal, and the copy is black at locations in which the original document is black. In order to eliminate the usage of photographic image reversal in laser operated record¬ ing equipments the image reversal.should be carried out by optoelectronic means,.by the appropriate control of the .laser bc3m used for recording the characters. " In the periodical "Electronics" (No, 5 1979, pp 46 to 48) an apparatus is described, in which a single laser bearn scans a raster on the recording surface, and the " control of the laser beam occurs in accordance with optoelectronic image reversal. This way in- that apparatus there is no need of electro¬ photographic image reversal any more, and positive •copier units can be used for the image recording. . The application of a single laser beam that scans each raster-line of the character separately necessitates a remarkable increase in the scanning • frequency compared to multi-beam recording technique, if the time of the recording remains unchanged. The. required fast deflection of the laser beam cannot be solved by means of the widely used swinging mirror technique, and such fast scanning can be realized by an expensive rotating mirror or by mean's of an v additional acousto-optical cell. Due to the higher speed used in the single beam technique, the speed of controlling the acousto-optical cell should also be increased in a corresponding manner, however, the application- of high speed electronic circuits substan¬ tially contribute to the productional costs. To ensure an undistorted image reconstruction from the raster picture a precise synchronism should be provided bet- ween the movement of the scanning beam and the dis¬ placement of the recording medium. Additionally, a synchronism between subsequent raster lines should be provided for with an accuracy that lies in the order of few nanoseconds* Owing to the above sketched technical diffi¬ culties connected with this technical construction th advantages coming from the elimination of the usage of an electrophotographic image reversal will at S least in great part be compensated by the problems connected with the optoelectronic image reversal when a single raster beam is used. Object of the invention The object of the invention is to provide a method and an apparatus for laser operated signal -.- recording, that eliminates the usage of an electro¬ photographic image reversal and provides for characte recording in discrete bands by the. application of multi-beam technique. - Disclosure of Invention According to the invention the above object solved by a method, in which a plurality of laser bea propagating in a common plane are projected onto a recording surface and the projected beams are deflect ed to scan discrete bands, wherein the character reco ing laser beams define a plurality of raster lines in which characters or marks are imaged- and in each reco ing location of the band the generation of all charac recording laser beams associated with this band is achieved simultaneously in accordance with the shape of the character or mark in the same location, and according to the invention the improvement lies in th the character recording laser beams are used to illum nate locations of the recording surface that do not comprise any character or mark, and the laser beams a -extinguished in the locations of the characters or ma and in addition to the generation of the character recording laser beams at least one band gap illumina,ι laser beam. is generated that propagates together with' and in the plane of the character recording laser beams to illuminate the band gaps of the recording surface. In the method according to the invention the multi-beam character recording technique has been improved to. be able for optoelectronic image reversal by means of ensuring the correct illumination of the band gaps in addition to the inverting of the character signals, whereby the complete recording surface is illuminated with the exception of the positions of the characters. In the apparatus for carrying out the method the control unit of the beam generating acousto-optical cell comprises oscillators of constant frequency associated with the generation of character recording laser beams, and gating circuits for coupling the oscillators to the acousto-optical cell, and an in¬ verter connected between the gating input of the gat- ing circuit and an information receiving unit to per¬ form an electronic image reversal, whereby the gating circuit- inhibits the passage of the oscillator output therethrough in the moments of existing character contents, while enables said passage in any other moment, and the control unit comprises at least one additional oscillator for generating band-gap illuminat¬ ing laser beams to illuminate band gaps between the bands of characters. Brief Description of Drawings Fig. 1 shows an optical arrangement used for the method according to the invention, Fig. 2 shows the block diagram of the first embodi- - 6 ^ ment of the apparatus according to the invention, Fig. 3 shows the voltage curves in characteristica points of the circuit of Fig.2, 5. Fig. 4 shows an enlarged detail of two tracks re¬ corded by the apparatus shown in Fig. 2 with a scanning occurring in line direction Fig. 5 is an enlarged view similar to Fig. 4 in case of a scanning in column direction, 10. Fig. 6 is the block diagram of a second embodiment of the invention that enables the matching of the lines in a direction normal to the deflection plane, and ' Fig. 7 shows a view similar to. Fig. 5 illustrating 15 a character band plotted by two neighbourin recording bands when ' the scanning occurs in .column direction. Best Mode of Carrying Out the Invention . ' Fig. 1 shows, the arrangement of the optical 20 units of the apparatus according to the invention and this arrangement is similar to Fig. 1 of the DE OS 2755 575. The arrangement comprises a laser source 1 and an acousto-optical cell 3 receiving the outgoing laser beam 2 of the laser source. A number of ultra- 5 sonic transducers 4 are arranged behind each other on a surface of the acousto-optical cell 3 and each of them comprises a terminal 5. In the acousto-optical cell 3 the Bragg diffraction is utilized, and in respo to appropriate control signals the cell 3 generates an 30 undeflected laser beam 6 and a plurality of diffracted laser beams 7. The outgoing laser beams 5 and 7.propa¬ gate in a common plane. The design of the acousto-op¬ tical cell 3 can be identical with the cell described . in the DE OS 2755 575 referred to above. The specific way of control of ' the cell 3 will be described later in connection with Figs. 2 and 6. In the path of the undeflected and iffracted laser beams 6 and 7 an optics 8 (preferably a lens) and a swinging mirror 9 are arranged. The swinging mirror ' 9 • is turned periodically around a rotational axis 10 to perform a swinging movement, whereby the direction of the laser beams 6 and 7 projected through the optics 8 varies periodically. In Fig. 1 the two extreme positions of the undeflected laser beam 6 is illustrated by heavy lines. The so deflected laser beams 7 scan discrete bands defined on a recording surface. In the exemplary embodiment shown in Fig. 1 the recording surface is a mantle surface of an electrophotographic copying drum 12 which performs a rotation with constant speed around its axis 11. In each swinging period of the swinging mirror 9 the laser beams scan different bands on the recording surface. It should be noted that the swinging mirror 9 can be replaced by any appropriate means which is capable of deflecting the laser beams in the required manner. In response to the scanning movement of the laser beams 7 and the rotation of the drum 12, raster bands are formed on the surface of the drum 12. The raster bands illustrated in Fig. 1 extend horizontally in line directions. The laser beams 7 can be graeped in laser beams 7a for scanning character lines in which characters can be recorded and in laser beams 7b used for illuminating the band gaps defined between the discrete character bands. The recording sur¬ face does not need to be a cylindrical one and it can have any appropriate shape e.g. it can well be. a planar surface. In the latter case the rotation of th cylinder should be replaced by a suitable linear move ment. In the exemplary embodiment shown in Fig. 1 the undeflected laser beam 6 impinges a knife edge 13 arranged in front of the copying drum 12. The upper contour line of the knife edge 13 falls below the hor zontal raster band scanned by the diffracted laser beams 7. There are arranged in front of the copying drum 12 a first photodetector 14, a light guiding rod 15 and a second photodetector 17. The photodetector 1 is adapted to sense the extreme positions of the lase beam 6 and to generate a signal to a control unit (no shown in Fig. 1) when the laser beams commence scanni a horizontal character band but they still do not reach the useful recording surface. The length of the light guiding rod 15 equals to the width. of the usefu recording surface i.e. to the length 16 of the charac bands. The light guiding rod 15 is made preferably of an optically transparent material, and in response to the laser beam 6 falling on any point of its surface delivers a light pulse to the photodetector 17 by utilizing a multiplicity of internal light reflection The .so illuminated active condition of the photodetec 17 means that the deflected laser beams fall within the useful recording range. The rotational speed of the copying drum 12 should be adjusted in accordance with the movement of the swinging mirror 9. For the purpose of adjusting and holding the appropriate rotational speed, a coded disc 18 is mounted at one end to the copying drum 12 an angular position detector 19 is used for sensing t speed of the coded disc 18. Referring now to Fig. 2 in which the units used for controlling the apparatus according to the invention is illustrated, the terminals 5 of the ultra¬ sonic transducers 4 of the acousto-optical cell 3 are driven by a control unit 20. The structural design of the control unit 20 is substantially identical with the control unit described in our copending European application having the publication number 00 181 50 used for controlling a similar acousto-optical cell. The control unit 20 comprises linear summing networks 47 and the number of these networks corresponds to the number of the terminals 5. The first inputs of the first two linear summing networks 47 are coupled through res¬ pective AND gates 42 to outputs of VHF or UHF osciila- tors 21 having fixed frequencies. The frequencies of - the oscillators 21 are chosen in such a way that each frequency defines the diffraction angle of a corres¬ ponding laser beam 7a when leaving the acousto-optical cell 3. The amplitudes of the oscillators 21 -determine the intensities of the associated laser beams. In the example shown in Fig. 2 seven oscillators 21 have been illustrated that can be used for a seven-line or seven- -column character recording. Of course, the number of the oscillators can be greater than seven, and in that case the resolution of the recording will be better. The third linear summing network 47 comprises a pair of inputs which are coupled through respective AND gates 45 and 46 to 1 outputs of oscillators 22 and 23 with variable frequency. The oscillators 22 and 23 comprise respective frequency determining control in¬ puts 25 and 26. Later it will be explained that the frequency bands of the oscillators 22 and 23 do not comprise the discrete frequencies of the oscillators 21, and these bands are adjusted in such a way that the associated laser beams 7b should illuminate the line gaps or column gaps defined between the characte bands. The second inputs of the AND gates form control inputs 24 for the control unit 20. Similarly, the second inputs of the AND gates 45 and 46 form control inputs 27 and 28 for the control unit 20. The operation of the apparatus is controlled by the pulses of a raster clock 35. The raster clock generates respective raster pulses which in case of scanning in line direction define the duration of elementary raster columns of the characters, and in case of scanning in column direction define the. duration- of elementary raster lines of the characters The swinging frequency of the swinging mirror 9 shown in Fig. 1 is defined through a drive for line deflect 40 also by means of the raster clock 35. The drive ' 40 provides for a correspondence between a complete deflection period of the swinging mirror 9 and the full time of the raster pulses occurring during this deflection. The photodetector 17 shown in Fig. 1 that de.livers pulses during the useful recording range is coupled through a discriminator 41 to an AND gate 37. The AND gate 37 comprises a second input coupled to t output of the raster clock 35. s a result of this connection the output of the AND ' gate 37 comprises- th raster pulses during the useful recording range only. The output of the AND gate 37 is coupled to the enabl input of a memory and decoder unit 30 which receives through its information inputs 29 the information de¬ fining the character or mark to be recorded. The memo and decoder unit 30 has respective outputs 31 in whic " during each raster pulse the simultaneously existing picture information of the respective character record¬ ing laser beams will be present. Under the term ."si ul- taneously existing" it is understood that the res- pective outputs 31 provide digital signals during each raster pulse and said signals carry the information of points located vertically under each other in a charac¬ ter band in the moment of the raster pulse, when the scanning is horizontal, and said signals carry the information of horizontal points of a character column when the scanning is vertical, The outputs 31 are coupled to an inverter unit 32, in which respective inverters are arranged for each of the outputs 31. The inverter unit 32 comprises out- puts 33 providing the inverted values of the. digits present at the outputs 31. This means that in the points of the image to be recorded that do not carry any picture information, the logical value of the associat- - ed output 33 will be M l", and in the points that carry picture information, the logical value will be M 0 H . The outputs 33 are coupled to the first in¬ puts of AND gates 34. The second inputs of the AND • gates 34 are interconnected and coupled to the output of a pulse generator 44 which is activated during the complete line duration (column duration). The outputs of the AND gates 34 are coupled to the control inputs 24 of the control unit 20 to define those time periods, in which the outputs of the oscillators 21 can pass to the acousto-optical cell 3. -The pulse generator 44 generates the pulse of the complete line duration (or column duration) from the output signal of the photodetector 14 by means of a discriminator 43. Additionally, the output ' pulse generator 44 controls through the ' control in¬ puts 27 and 28 the open condition of the AND gates 45 and 46. The output of the raster clock 35 is coupled ' 5 to control inputs of triangle or sawtooth signal gene rators 38. and 39. The triangle signal generators 38 and 39 control the frequency determining control in¬ puts 2. and 26 of the variable frequency oscillators ,22 and 23 by a frequency signal which is equal to or 0 higher than the frequency of the raster pulses. In response to such control the output frequency of the oscillators 22 and 23 varies between lower and upper limit frequency values in accordance with the triangular or sawtooth control signal. 5 The operation of the apparatus according to the invention and the examples for carrying out the method will be described in connection with.Figs, 4 and 5, in which reference will be made to the time curves of Fig. 3, 0 Fig. 4 shows an enlarged detail of an image recorded by means of the arrangement shown in Fig, 1, that illustrates respective parts of a pair of neighbouring character bands C--, and C g2 . . The seven .character recording laser beams 7a 5 and the two band gap illuminating laser beams 7b gene rated by the acousto-optical cell 3 take a position i the moment t, , in which the undeflected laser beam 6 illuminates the photodetector 14, and the pulses of the photodetector 14 are shown in Fig. 3, diagram g. 0 The operation of the control unit shown in Fig. 2 is enabled by a line duration signal derived from the pulse of the photodetector 14, and the line duration signal (Fig. 3 diagram h) is provided in the output of the pulse generator 44 and it enables the open condition of the AND gates 34 and of the AND gates 45, 46. Now, the generation of the band gap illuminat¬ ing laser beam 7b will be described. After the moment t, the outputs of the variable frequency oscillators 22 and 23 are coupled to a segment of the acousto-op¬ tical cell 3 and provide diffracted laser beams 7b according to their actual frequencies. In the example shown in Fig. 4 two laser beams 7b have been provided, and the first of these beams falls on the recording surface just above the band of the character recording laser beams 7a, while the other beam 7b falls just below this band. The upper band gap illuminating laser beam should illuminate a band gap which has a height of four raster lines. If this illumination is provided by a single laser beam 7b, the intensity of this laser beam should be four times higher than the intensity any of the character recording laser beams 7a. By periodically changing the frequency of the oscillator 22 in accordance with the triangular control signal (shown in diagram d. in Fig, 3), the laser beam 7b associated with the upper band gap will be diffracted vertically to perform an alternating up-down movement in a band gap having a height of four raster lines, and the deflection provided by the movement of the swinging mirror 9 in the horizontal direction results in that the laser beam 7b will completely illuminate the upper band gap. The focal diameter of the laser beam 7b corresponds preferably to the size of a- raster line, which has been indicated in Fig. 4 by respective circles. If the frequency of the triangular signal is at least equal to the frequency of the raster pulses^ - 14 - then the condition required for the complete illumin¬ ation of the band gap is satisfied. In a similar way the lower one of the laser beams 7b illuminates a part of the lower band gap. In the exemplary case the height of the lower illuminated gap corresponds to that of three raster lines, and the frequency of the associated oscillator 23 is changed within a correspondingly narrower band. It is also sufficient for the appropriat gap illumination if the lower laser beam 7b has three times as high intensity as the character recording lase beam 7a has. It can be seen from the ' two adjacent character bands shown in Fig. 4 that an overlapping range with a height of two raster lines have been provided between the illuminated neighbouring band gaps, i.e. the upper two hypothetical band gap raster lines of the lower band coincides with the two lower hypothetical band gap' raster lines of the upper band. The so obtained over¬ lapping between the band gaps is advantageous because the fluctuations of the speed of rotation of the copying drum 12 can not cause recording errors and the need for an expensive and precise synchronism between the speed of the drum 12 and the control of the swinging move- - ent of the mirror 9 will this way be eliminated. It should be noted that the application of laser beams 7b deflected in accordance with a triangular control signal is preferable, however, the illumination of the band gaps can also be provided by the application of undeflected laser beams generated by constant frequency oscillators if such beams scan each of the raster lines falling in the band gaps. The recording of the characters can be s^ante after the moment t , whereafter the laser beams fall in the useful recording range. The useful recording period is shown in diagram b. of Fig, 3. During this period the photodetector 17 is continuously illu inat- - ed by the light guiding rod 15. Diagram c. in Fig. 3 shows the ' gated raster pulses present at the output of the AND gate 37. Each raster pulse provides for the reading of the seven information bits associated with the seven raster lines of the character to be recorded, whereby the corresponding information will occur in the respective outputs 31. In the exemplary case the character to be recorded consists of seven. raster lines and each of these lines is associated with a respective one of the oscillators 21 used for generating the laser beam illuminating the particular raster line. When e.g. the letter "I" shown in Fig. 4 is recorded, each of the seven outputs 31 comprises logical "1" level, while each of the inverted outputs 33 comprises logical "0" level. During the useful recording period the.AND gates 34 receive enable signals from the pulse generator 44 through their second inputs, whereby the condition of the AND gates 4-2 will be determined only by the conditions of the respective inverted outputs 33. Diagram e. in Fig. 3 shows the logical state of one of the outputs 31 throughout several raster periods, while diagram f, shows the condition of the associated inverted out¬ puts 33. Due to the inversion the output 33 comprises a logical "1" level when the associated laser beam has already scanned the useful recording section between the moments t ? and t.,. This can be seen in diagram i-« of .Fig. 3' illustrating the condition of the output of the associated AND gate 42, As a result of the above described recording . - 16 - technique the ppsitive image of the character to be recorded will be imaged on the recording surface i.e. the surface will not be illuminated in positions in which a character exists, and all other areas of the surface will be illuminated. This positive illumin¬ ation is preferable because in that case any con¬ ventional positive recording technique can be used. In order to exclude any recording during the returning movement of the swinging mirror 9, the out- . put of the pulse generator 44 is used for switching off all laser beams between the moment t. and the starting moment t, of the next period by means of inhibiting the passage of signals through the AND gates 34, 45 and 46. Fig. 5 corresponds substantially to Fig. 4, however, the recording occurs here in a normal direction (turned by 90 ) relative to the recording in Fig. 4 i.e. in the recorded document the directions X * and X 2 will be mutually interchanged. " The character bands in Fig. 4 will be character columns in Fig. 5, while the band gaps will be column gap?.-. The recording technique re¬ mains substantially unchanged, however, the memory and decoder unit 30 should comprise now the horizontal information of the characters in common addresses. Fig.5 shows three column bands extending beside each other, in which each column band comprises five raster columns, a left column gap having a width corresponding to that of two raster columns and a right column gap with an iden¬ tical width. The overlapping between neighbouring column gaps takes the width of two raster columns. If the number of the character recording laser beams 7a remains unchanged when vertical scanning is . used, the resolution of the characters will be finer because the heigh-t of the characters is greater than their width, and the number of the recording laser beams can not influence the vertical resolution during ver¬ tical scanning. -Fig. 6 shows a further embodiment of the apparatus according to the invention by which all of the outgoing laser beams can be deflected simultaneous ¬ ly in their common plane, whereby the exact position ad¬ justment of the bands can be carried out normal to the scanning direction. The control unit 20 of Fig. 6 is similar to the corresponding unit described in our copending European application having the publication number 00 181 50, that can be u&ed for ' the simulta¬ neous deflection of all outgoing laser beams. The control unit 20 of Fig. 6 differs from the control unit of Fig. 2 in that it uses an auxiliary oscillator 49 which is coupled to first inputs of mixers 48. The second inputs of the mixers 48 are connected with the outputs of the linear summing networks 47, and the out- puts of the mixers 48 a re coupled through respective band-pass filters 50 to the terminals 5 of the acousto- -optical cell 3, The relative frequences of the oscillators 21, 22 and 23 should be set in the same way as in the embo- diment of Fig. 2, and the only difference lies in that in the present case the differences between the frequencies of the auxiliary oscillator 49 and that of the oscillators 21, 22 and 23 should be adjusted to the same VHF or UHF values that ensures the appropriate operation. The band-pass filters 50 are tuned to these VHF or UHF frequency bands. The frequency of the auxiliary oscillator 49 can be changed by a voltage signal coupled to its frequency determining control input 51, and the position of all diffracted laser 18 - • beams 7 that leave the cell 3 will change accordingly. The control input 51 is controlled by means of the angular position detector .19 (shown in Fig, 1) through an' error signal forming unit 52 and a regulat- 5 ing unit 53. By simultaneously shifting the position • of the laser beams 7, the respective recording bands ' can be positioned exactly side by side even if the speed of the recording surface (the speed of the drum 12) is fluctuating or slightly changing. 0 Fig. 7 shows the enlarged view of a part of a recording made in this way. The possibility -of adjust ment of the position of the laser beams in a direction normal to the scanning direction .provides for attaining a finer resolution even if the number of the character 5 recording laser beams is unchanged. In that case the , recording of a complete character band takes two. scann ing periods of the swinging mirror 9. " " In the first of these periods from the two band gap illuminating laser beams 7b only the upper one is enabled and.from the 0 memory and decoder unit 30 the information of the uppe seven raster lines of the character is read out. In th second period the upper band gap illuminating laser- beam 7b will be blocked and the lower one enabled, and the information read out from the unit 30 will corres- ' 5 pond to the seven lower raster lines of the same cha¬ racter. By using this method the character recording " will have a resoltuion of fourteen raster lines by means of seven oscillators and associated recording 0 laser beams. It can be seen from the above described examples that the essence of the present invention e " in. the recording by the inverted signals of the characters and in the illumination of the full record-' ing surface in positions other than that comprise •characters. In this way the conventional inexpensive positive electrophotographic recording techniques can be used. An additional advantage is connected with the application of overlapping between the band gaps or column gaps because in that case the speed of the recording surface does not have to be kept in a pre- cisely constant value. The actual way of generation of the character recording laser beams, the actual type of the scanning and the type ' of image recording are indifferent in view of the essence of the present invention. The swing- ing mirror 9 can e.g. be replaced by a scanning obtain¬ ed by means of an additional acousto-optical cell o a rotating mirror. Similarly,, the cylindrical recording surface can be replaced by a planar surface. Also, the inverter 32 can be spared if the inverted character values are written in the memory and decoder unit 30. In order to visualize the parameters of the recording that can be made by the present invention, the following table comprises characteristic data in case of character recordings by seven and sixteen raster lines, respectively if the recorded document is an A4 form paper (210 x 297 mm). - 20 - ■ Table I.

Claims: Claims t 1. A method for recording signals on bands by means of laser beams, comprising the steps of pro¬ jecting a plurality of character recording laser beams propagating in a common plane onto a recording 5 surface, deflecting said beams to scan respective raster lines on discrete recording bands of said-sur- face, generating said character recording laser beams simultaneously in each recording point of each band in accordance with the shape of the signal or cha- 0 racter falling in the corresponding points, c h a¬ r a c t e r i z e d in, that comprising additionally the steps of illuminating said recording surface by -.. means of the character recording laser beams (7a) in -. ' locations that do not comprise any character or signal, 5 blocking the passage of said character recording laser beams (7a) towards locations of said recording surface that comprise characters or signals, generating at least one band gap illuminating laser beam (7b) in addition to the recording laser beams (7a) to propagate 0 together and in a common plane therewith, and illuminat¬ ing the band gaps of the recording surface. 2. The method as claimed in claim 1, c h a¬ r a c t e r i z e d in, that adjusting the intensity of said at least one band gap illuminating laser beam 5 (7b) to be higher than the intensity any of the cha¬ racter recording laser beams (7a), and deflecting said band gap illuminating laser beam (7b) normal to the scanning direction to perform an alternating movement within a predetermined band gap height with a speed 0 substantially higher than the speed of scanning move- - 22 - ment, whereby the band gaps will be evenly illumina 3. ' The method as claimed in claim 1, c h / r a c t e r i z e d in, that defining respective b gaps at both sides of said recording bands, and ill 5 minating said band gaps by means of one of more ban • gap illuminating laser beams (7b). 4. The method as claimed in claim 1, c h r a c t e r i z e d in, that adjusting the heights the band gaps of neighbouring bands so as to overla 0 each other. -.. ' 5. The method as claimed in claim 1,- c h- a r a c t e r i z e d in> that recording each of said discrete bands by means of two full scanning period said laser beams in such a way that in the first per 5 illuminating one " of the band gaps associated with sa band and a part of the character recording band,.and the other period illuminating the second part of sai character recording band and the other associated ba gap*. 0 6. The method as claimed in any of claims 1 5, c h a r a c t e r i z e d in, that sensing the of the relativ movement between said laser beams and said recording surface in a direction normal to the scanning direction, forming the difference between t 5 sensed speed and a predetermined nominal speed,, and simultaneously adjusting the positions of all laser beams in their common plane on the basis of said / / difference to precisely arrange neighbouring.bands in side by side positions. 7. Apparatus for carrying out ' the method of ■ claim 1, comprising a laser source, an acousto-optical cell arranged in the path of the laser beam of said source, a control unit coupled to the acousto-optical cell for generating a plurality of outgoing diffracted laser beams in the cell by means of Bragg diffraction, in which each of said laser beams lie in a common plane, an optical system for deflecting all laser beams coming out from the cell to scan bands on a recording surface, actuating means for establishing a relative movement between the laser beams and the recording surface in a- direction normal to the scanning, and an information receiving means for receiving the information to be re¬ corded and forwarding the same in the form of digital - signals to said control unit, c h a r a c t e r i z e d in, that said control unit (2θ) comprises a predetermin¬ ed number of oscillators (21) with fixed frequency for generating character recording laser beams (7a), gate circuits (42) for coupling the outputs of said oscilla¬ tors (21) to the acousto-optical cell (3), inverter means (32) coupled between the outputs of said information receiving means and the gating inputs of said gate cir- cuits (42) in moments when characters or signals exist and to enable .said signal passage in any other moment, and at least one additional oscillator (22 and/or 23) for generating band gap illuminating laser beams (7b) to illuminate to band gaps between said bands. 8. The apparatus as claimed in claim 7, c h a ¬ r a c t e r i z e d in, that it comprises a raster clock ' (35) coupled to driving unit (4θ) of said deflecting sys- - 24 - tern (9) to provide synchronism between the scanning movement and the relative movement of said recording surface, said information receiving means comprising a memory and decoder unit (30) with an enable input coupled through a gating circuit (37) to the output of the raster clock (35). 9. The apparatus as claimed in claim 8, c h a r a c t e r i z e d in, that it comprises a full line duration determining unit (44) having an output coupled to appropriate enable inputs of said control unit (20) for blocking the generation of laser beams in moments of the scanning period other than the duration of full line scanning. 10. The apparatus as claimed in claim 9, c h a r a c t e r i z e d in, that it comprises a useful lin duration determining unit (41), and an AND gate (37) enabled by the output of said useful line duration de¬ termining unit (4l), said AND gate (37) being coupled between the output of the raster clock (35) and the en- able input of said memory and decoder unit (30) to en-, able information recording during the scanning of the useful line duration only. 11, The apparatus as claimed in claim 8, c h a r a c t e r i z e d in, that the oscillators (22,23) for generating the laser beams (7b) for illuminating the band gaps are variable frequency oscillators, havin respective frequency determining control inputs ' (25,26) said control inputs (25,26) are connected with outputs of triangle or sawtooth signal generators (38,39) hav- ing operating frequencies being at least equal to the frequency of the raster clock pulses. 12. The apparatus as claimed in claim 9, c h a - r a c t e r i z e d in, that the control unit (20) comprises an auxiliary oscillator with variable frequency (49) to enable simultaneous changing the de¬ flection of all outgoing laser beams (7), in their common plane, a sensing means (19) for sensing the' speed of movement of said recording surface, an error signal form- ing unit (52) and a regulating unit (53), the output of said sensing means (19) is coupled through said error signal forming unit (52) and regulating unit (53) to the frequency determining control input (5l) of said auxiliary oscillator (49) for tjhe exact positioning of - said bands on the recording surface.

Inventors: MARKUS L, PODMANICZKY A, TOKES S
Applicants: MAGYAR TUDOMANYOS AKADEMIA, MARKUS L, PODMANICZKY A, TOKES S
Application year: 1980
Main classification: G11B7
IPC codes: B41J2, G02F1, G03B27, G03G15, G06K15, G11B7, H04N1