JP2007249172A - Pixel forming apparatus, optical scanner, optical scanning method, image forming apparatus, color image forming apparatus, program and recording medium - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To allow a positional correction of pixels in a subscanning direction with high accuracy and to correct the bending of a scanning line at an optical system and a mechanical part with high accuracy in an optical scanner having a plurality of light sources. <P>SOLUTION: One pixel is formed by at least m (n≥m≥2) light sources out of n (n≥2) light sources arranged at different positions in a subscanning direction. <P>COPYRIGHT: (C)2007,JPO&INPIT

Description

  The present invention relates to a pixel forming apparatus, an optical scanning apparatus, an optical scanning method, an image forming apparatus, a color image forming apparatus, a program, and a recording medium.

  FIG. 29 is a diagram showing a configuration example of a general image forming apparatus such as a laser printer or a digital copying machine using an electrophotographic process. Referring to FIG. 29, laser light emitted from a semiconductor laser unit 1001 that is a light source unit is deflected and scanned by a rotating polygon mirror 1002 and is a scanned medium through a scanning lens (fθ lens) 1003. A light spot is formed on the photoconductor 1004, and the photoconductor 1004 is exposed to form an electrostatic latent image. At this time, the phase synchronization circuit 1009 sets the modulation signal generated by the clock generation circuit 1008 to a phase synchronized with the photodetector 1005 that detects the light of the semiconductor laser deflected and scanned by the polygon mirror 1002. That is, the phase synchronization circuit 1009 generates a phase-synchronized image clock (pixel clock) for each line based on the output signal of the photo detector 1005 and supplies it to the image processing unit 1006 and the laser drive circuit 1007. To do. In this way, the semiconductor laser unit 1001 performs the operation of the semiconductor laser via the laser driving circuit 1007 according to the image data generated by the image processing unit 1006 and the image clock whose phase is set for each line by the phase synchronization circuit 1009. By controlling the light emission time, the electrostatic latent image on the scanned medium (photoconductor) 1004 can be controlled.

  However, in recent years, there has been an increasing demand for higher printing speed (image forming speed) and higher image quality. On the other hand, higher polygon motors, which are deflectors, and higher pixel clocks, which serve as reference clocks for laser modulation. However, the speed limit of either method is approaching, and the conventional method cannot cope with it.

  Therefore, the use of a multi-beam using a plurality of light sources is used for speeding up. In the multi-beam optical scanning method, the number of light beams that can be simultaneously scanned by the deflection of the deflector increases, so that the rotational speed of the polygon motor, which is a deflector, and the pixel clock frequency can be reduced, and high-speed and stable optical scanning and Image formation is possible.

  As a light source constituting the multi-beam, a method of combining a single beam laser chip or a method of using an LD array in which a plurality of light emitting elements are incorporated in one laser chip is used.

  A semiconductor laser such as an LD array constituting the multi-beam is extremely small and can be directly modulated at a high speed by a driving current, so that it has been widely used as a light source for a laser printer or the like in recent years. However, since the relationship between the drive current of the semiconductor laser and the optical output has a characteristic that varies depending on the temperature, it becomes a problem when the light intensity of the semiconductor laser is set to a desired value. In particular, in the case of a surface emitting laser in which a plurality of light sources are configured on the same chip, the distance between the light sources is short, so that the effects of temperature change and temperature crosstalk due to light emission and extinction are significant, and the light quantity is likely to change.

  For example, in Patent Document 1, in an optical scanning device that scans a scanned medium by arranging a plurality of light sources in a two-dimensional manner and deflecting a plurality of light beams by a deflector, crosstalk caused by heat generation between light emitting points is disclosed. An example is shown in which the arrangement density of the light emitting points is maximized without causing an influence.

  Further, in Patent Document 2, in an image forming apparatus using a surface emitting laser, an electrostatic latent image of a pixel is obtained by having means for changing the light emission intensity of each chip and means for controlling the light emission time in units of pixels. The way to control is shown.

  Further, Patent Document 3 discloses a method for avoiding the problem of thermal stroke and realizing high density of recorded images by adopting a configuration in which the arrangement of light sources is defined in a scanning device using a surface emitting laser. It is shown.

JP 2001-272615 A JP 2003-72135 A JP 2001-350111 A

  However, in the conventional optical scanning device having a plurality of light sources, since one pixel is generally composed of one light source, there is a problem that the light emission level variation of each light source directly leads to the image density variation. In particular, pixel variations in the sub-scanning direction cannot be corrected by the conventional method. In addition, there is a problem that there is no effective means for correcting optical system and mechanical scanning line bending with high accuracy.

  The present invention can perform pixel position correction in the sub-scanning direction with higher accuracy in an optical scanning device having a plurality of light sources, and can also perform optical system and mechanical scanning line bending with high accuracy. An object of the present invention is to provide a pixel forming apparatus, an optical scanning apparatus, an optical scanning method, an image forming apparatus, a color image forming apparatus, a program, and a recording medium that can be corrected.

  In order to achieve the above object, according to the first aspect of the present invention, m (n ≧ m ≧ 2) light sources among n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction. The pixel forming apparatus is characterized in that one pixel is formed as a whole.

  According to a second aspect of the present invention, one pixel is formed of all m (n ≧ m ≧ 2) light sources out of n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction. An optical scanning device characterized in that light source drive control means for changing the drive state of m light sources is provided to move the center of gravity of one pixel in the sub-scanning direction. .

  According to a third aspect of the present invention, one pixel is formed of all m (n ≧ m ≧ 2) light sources out of n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction. When correction data for moving the center of gravity of one pixel in the sub-scanning direction is given, m for moving the center of gravity of one pixel in the sub-scanning direction by an amount corresponding to the correction data. An optical scanning device characterized in that light source drive control means for changing the drive state of each light source is provided.

  According to a fourth aspect of the present invention, in the optical scanning device according to the third aspect, the sub-scanning pixel position for detecting the sub-scanning pixel position and outputting correction data for correcting the pixel position in the sub-scanning direction. Detection means is further provided, and the light source drive control means includes m light sources for moving the center of gravity of one pixel in the sub-scanning direction by an amount corresponding to the correction data output from the sub-scanning pixel position detection means. It is characterized by changing the driving state of the.

  According to a fifth aspect of the present invention, there is provided the optical scanning device according to any one of the second to fourth aspects, wherein the light source drive control means moves the center of gravity of one pixel in the sub-scanning direction. The light emission time ratio of the m light sources is changed so that the total light emission time or the total exposure area of the m light sources is constant.

  According to a sixth aspect of the present invention, in the optical scanning device according to any one of the second to fourth aspects, the light source drive control means moves the center of gravity of one pixel in the sub-scanning direction. It is characterized in that the exposure energy ratio of the m light sources is changed by changing the light emission level ratio of the m light sources so that the total exposure energy of the m light sources becomes constant.

  According to a seventh aspect of the present invention, one pixel is formed of all m (n ≧ m ≧ 2) light sources out of n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction. It is characterized in that the center of gravity of one pixel is moved in the sub-scanning direction by changing the driving state of m light sources.

  In the invention according to claim 8, one pixel is formed by all m (n ≧ m ≧ 2) light sources among n (n ≧ 2) light sources arranged at least at different positions in the sub-scanning direction. The light-emitting light source is switched so that one pixel moves in a predetermined direction in the sub-scanning direction at a certain image height in the main scanning direction with a movement amount equal to the length of the pitch of one light source. An optical scanning device is provided with light source drive control means.

  According to the ninth aspect of the present invention, one pixel is formed of all m (n ≧ m ≧ 2) light sources out of n (n ≧ 2) light sources arranged at least at different positions in the sub-scanning direction. The light-emitting light source is switched so that one pixel moves in a predetermined direction in the sub-scanning direction at a certain image height in the main scanning direction with a movement amount equal to the length of the pitch of one light source. It is characterized by that.

  According to a tenth aspect of the present invention, of n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction, initially m (n>) up to a certain image height in the main scanning direction. One pixel is formed by the whole light source of m ≧ 2), and one pixel is formed by (m + 1) whole light sources from an image height in the main scanning direction, and one light source at a certain image height in the main scanning direction thereafter. One pixel moves from the original one pixel in a predetermined direction in the sub-scanning direction with a movement amount of the same length as the pitch length of the entire m light sources moved by one light source in the sub-scanning direction compared to the original. The light scanning device is characterized in that light source drive control means for changing the drive state of the light source is provided so that one pixel is formed.

  According to an eleventh aspect of the present invention, of n (n ≧ 2) light sources arranged at least at different positions in the sub-scanning direction, initially m (n>) up to a certain image height in the main scanning direction. Light source drive control for changing the driving state of the light source so that one pixel is formed with the entire light source of m ≧ 2) and one pixel is formed with all the (m + 1) light sources from a certain image height in the main scanning direction. Means is provided.

  According to a twelfth aspect of the present invention, in the optical scanning device according to the tenth or eleventh aspect, the light source drive control means is configured to (m + 1) during a period in which one pixel is formed with all (m + 1) light sources. ) A smoothing process is performed in which the driving state of at least one of the light sources is changed stepwise to smooth the edge of the pixel.

  The invention according to claim 13 is the optical scanning device according to claim 12, characterized in that the light source drive control means uses PWM (pulse width modulation) for the smoothing processing.

  The invention according to claim 14 is characterized in that, in the optical scanning device according to claim 12, the light source drive control means uses PM (power modulation) for the smoothing processing.

  Further, the invention according to claim 15 is the optical scanning device according to claim 12, wherein the light source drive control means uses a combination of PWM (pulse width modulation) and PM (power modulation) for the smoothing processing. It is characterized by.

  According to a sixteenth aspect of the present invention, of n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction, initially m (n>) up to a certain image height in the main scanning direction. One pixel is formed by the whole light source of m ≧ 2), and one pixel is formed by (m + 1) whole light sources from an image height in the main scanning direction, and one light source at a certain image height in the main scanning direction thereafter. One pixel is moved in a predetermined direction from the original one pixel by a movement amount having the same length as the pitch length of one pitch, and one pixel is formed by all the m light sources moved by one light source compared to the original. It is characterized by changing the driving state of the light source.

  According to a seventeenth aspect of the present invention, of n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction, initially m (n>) up to an image height in the main scanning direction. The drive state of the light source is changed so that one pixel is formed with the entire light source of m ≧ 2), and one pixel is formed with all (m + 1) light sources from a certain image height in the main scanning direction. It is said.

  The invention according to claim 18 is the optical scanning device according to any one of claims 2 to 6, 8, 10 to 15, wherein the n light sources include: A surface emitting laser configured on the same chip is used.

  The invention according to claim 19 has the optical scanning device according to any one of claims 2 to 6, 8, 10 to 15, and 18. The image forming apparatus.

  The invention described in claim 20 has the optical scanning device according to any one of claims 2 to 6, 6, 8, 10 to 15, and 18. A color image forming apparatus.

  In the invention according to claim 21, one pixel is formed by all m (n ≧ m ≧ 2) light sources out of n (n ≧ 2) light sources arranged at least in different positions in the sub-scanning direction. When correction data for moving the center of gravity of one pixel in the sub-scanning direction is given, m for moving the center of gravity of one pixel in the sub-scanning direction by an amount corresponding to the correction data. This is a program for causing a computer to realize light source drive control processing for changing the drive state of each light source.

  According to a twenty-second aspect of the present invention, one pixel is formed of all m (n ≧ m ≧ 2) light sources out of n (n ≧ 2) light sources arranged at least at different positions in the sub-scanning direction. When correction data for moving the center of gravity of one pixel in the sub-scanning direction is given, m for moving the center of gravity of one pixel in the sub-scanning direction by an amount corresponding to the correction data. A computer-readable recording medium that records a program for causing a computer to execute a light source driving control process for changing the driving state of each light source.

  According to the inventions of claims 1 to 18, 21 and 22, at least m (n ≧ 2) of n (n ≧ 2) light sources arranged at different positions in the sub-scanning direction. Since one pixel is formed by the whole light source of m ≧ 2), the pixel position correction in the sub-scanning direction can be performed with high accuracy by changing the driving device of m light sources forming one pixel. Can be done.

  In particular, in the inventions of claims 2 to 7, the center of gravity of one pixel can be moved in the sub-scanning direction.

  The inventions of claims 8 and 9 are effective for correcting optical system and mechanical scanning line bending with high accuracy in general images other than line images (line images), for example.

  The inventions according to claims 10 to 17 are, for example, in a line image (line image) in which the value of the outer pixel is “0” and the outer side has no special meaning as an image. This is effective for correcting a scan line bending with high accuracy.

  The invention according to claim 18 is the optical scanning device according to any one of claims 2 to 6, 8, 10 to 15, wherein the n light sources include: Since surface-emitting lasers configured on the same chip are used, power saving and high-precision optical scanning can be performed.

  According to a nineteenth aspect of the present invention, there is provided an image forming apparatus comprising the optical scanning device according to any one of the second to sixth aspect, the eighth aspect, the tenth aspect, the fifteenth aspect, and the eighteenth aspect. Since this is a device, when pixel position variations occur in the sub-scanning direction, highly accurate position correction with reduced variations is possible, and optical system and mechanical scanning line bending can be corrected with high accuracy. And high-quality image formation becomes possible.

According to a twentieth aspect of the invention, a color image having the optical scanning device according to any one of the twentieth to sixth, eighth, tenth to fifteenth, and eighteenth aspects. Since it is a forming device, when pixel position variations occur in the sub-scanning direction, highly accurate position correction with reduced variations is possible, and optical system and mechanical scanning line bending are corrected with high accuracy. Thus, it is possible to correct the color misregistration and to form a high-quality image with a reduced color misregistration amount.

  Hereinafter, the best mode for carrying out the present invention will be described with reference to the drawings. In the present invention, one pixel is a pure pixel (for example, a 1200 dpi pixel means a pixel of about 21 μm square), and a plurality of pixels (for example, 4 × It does not mean one pixel as a result of combining (four pixels).

  Further, in the present invention, the n light sources “arranged at least at different positions in the sub-scanning direction” are not only light source arrangements arranged in a line in the sub-scanning direction but also light source arrangements as shown in FIG. (Light source arrangement inclined at an angle θ with respect to the sub-scanning direction) and the like.

(First embodiment)
The first embodiment of the present invention relates to a pixel forming apparatus, and the pixel forming apparatus of the first embodiment includes at least n (n ≧ 2) light sources arranged at different positions in the sub-scanning direction. One of the m light sources (n ≧ m ≧ 2) is characterized in that one pixel is formed.

  The pixel forming apparatus according to the first embodiment will be specifically described.

  Now, in the general image forming apparatus (writing optical system) of FIG. 29, the light source unit 1001 is a semiconductor laser array in which a plurality of light sources (a plurality of semiconductor lasers) are arranged in a lattice shape as shown in FIG. When a plurality of light sources (surface emitting lasers in which a plurality of surface emitting lasers (VCSELs, surface emitting semiconductor lasers) are arranged in a grid pattern) are formed on the same chip, the arrangement direction of the plurality of light sources is the polygon mirror shown in FIG. The arrangement and angle of the light source unit 1001 are adjusted so as to have a certain angle θ with respect to the rotation axis of the deflector.

  In this case, in FIG. 1, when the vertical arrangement direction of the light sources is a to c and the horizontal arrangement direction is 1 to 4, for example, the upper left light source in the drawing is expressed as a1.

  Consider a case in which the light source unit 1001 is arranged with an angle θ so that different scanning positions of the light source a1 and the light source a2 are exposed and one pixel (one pixel) is configured by the two light sources. That is, in FIG. 1, a case where one pixel is realized with two light sources is considered. For example, if one pixel is composed of two light sources a1 and a2, and one pixel is composed of two light sources a3 and a4, a pixel as shown at the right end of FIG. When the vertical direction in the figure is the sub-scanning direction, it is assumed that the distance between the centers of the pixels constituted by the two light sources is equivalent to 600 dpi. At this time, the center interval between the two light sources constituting one pixel is equivalent to 1200 dpi, and the light source density is twice the pixel density. Therefore, by changing the light amount ratio of the light source constituting one pixel, it becomes possible to shift the barycentric position of the pixel in the sub-scanning direction, thereby realizing highly accurate pixel formation.

(Second Embodiment)
The second embodiment of the present invention relates to an optical scanning device. As shown in FIG. 2, the optical scanning device of the second embodiment is at least n (at least in different positions in the sub-scanning direction). One pixel is formed by all m (n ≧ m ≧ 2) light sources among n ≧ 2), and correction data for moving the center of gravity of one pixel in the sub-scanning direction is provided. When given, light source drive control means 50 for changing the drive state of m light sources is provided in order to move the center of gravity of one pixel in the sub-scanning direction by an amount corresponding to the correction data. .

  More specifically, as shown in FIG. 3, the optical scanning device according to the second embodiment of the present invention detects sub-scanning pixel positions and outputs correction data for performing pixel position correction in the sub-scanning direction. Sub-scanning pixel position detection means 51 is provided, and the light source drive control means 50 moves the center of gravity of one pixel in the sub-scanning direction by an amount corresponding to the correction data output from the sub-scanning pixel position detection means 51. Therefore, the drive state of m light sources is changed.

  Here, for example, the technique described in Japanese Patent No. 3644923 can be used for the sub-scanning pixel position detecting means 51.

  That is, the color image forming apparatus described in Japanese Patent No. 3644923 includes a plurality of image forming units that are arranged along the conveying direction of the conveying belt and form images of different colors by an electrophotographic method, and the conveying belt. And at least three sensors arranged at positions including the center and both ends in the main scanning direction orthogonal to the conveyance direction, and the image formation at positions read by all the sensors on the conveyance belt A toner mark creating means for creating a position detection toner mark for each color by a section, and a position of another color with respect to a reference color for each position of each sensor based on the output of the sensor that has read the position detection toner mark A displacement amount detecting means for detecting the displacement amount, and the position displacement amount detecting means is used as the sub-scanning pixel position of the present invention. It can be used as the detection means 51.

  More precisely, the sub-scanning pixel position detecting means 51 of the present invention is a correction for performing pixel position correction in the sub-scanning direction based on the positional deviation amount detected by the positional deviation amount detecting means of Japanese Patent No. 3644923. Data can be output.

  In the optical scanning device of the second embodiment, as described in the pixel forming device of the first embodiment, m of n light sources (n ≧ 2) arranged in the sub-scanning direction. One pixel is formed by the entire light source (n ≧ m ≧ 2), and the method of changing the driving state of the m light sources is the total light emission time or the total exposure area of the m light sources. M light sources by changing the light emission time ratio of m light sources to be constant, or by changing the light emission level ratio of m light sources so that the total exposure energy of m light sources is constant And changing the exposure energy ratio.

  4 to 8 are diagrams for explaining specific examples of how to change the driving state of the m light sources by the light source driving control means 50. FIG.

  FIG. 4 illustrates a specific example of changing the light emission time ratio of m light sources so that the total light emission time of m light sources is constant in order to move the center of gravity of one pixel in the sub-scanning direction. FIG. FIG. 4 shows a case in which one pixel is realized by two light sources A and B. The light emission signals of the two light sources A and B are shown in the upper part of the drawing, and in FIG. The scanning light amount distribution by the scanned light beam is shown with the right side direction of the figure as the main scanning direction.

  For example, consider the case where the light source a1 in FIG. 1 is the light source A in FIG. In the case of the pixel 1, only the light source B is turned on, and the light emission time of the light source B becomes shorter and the light emission time of the light source A becomes longer as the pixels 1, 2, 3,. For example, in the case of the pixel 4, both the light sources A and B are lit for the same light emission time. When this pixel is used as a reference pixel, the pixels 5, 6 and 7 are displaced in the center of gravity in the sub-scanning direction which is the upward direction in the figure ing. On the contrary, as the pixels 3, 2, and 1 are shifted, the barycentric position of the pixel is shifted in the sub-scanning direction in the lower direction in the figure, and the total light emission time of the two light sources is made substantially constant, and the ratio is changed to change the pixel Can be shifted in the sub-scanning direction. For example, in the pixel 3, when the light emission time of the light source A is Ta3 and the light emission time of the light source B is Tb3, the exposure time ratio is changed so that the sum of the light emission times Tall = Ta3 + Tb3 = Tan + Tbn (n is a natural number) = constant. I will do it. At this time, for example, using the technique of Japanese Patent No. 3644923 described above, the positional deviation of the toner image in the sub-scanning direction is measured by patch measurement, and correction data is given so as to correct the positional deviation amount, and the ratio of the emission time. It is possible to correct the pixel position shift in the sub-scanning direction by changing.

  FIG. 5 illustrates a specific example in which the light emission time ratio of the m light sources is changed so that the total exposure area of the m light sources is constant in order to move the center of gravity of one pixel in the sub-scanning direction. It is a figure for doing. FIG. 5 shows a case where one pixel is realized with two light sources A and B. In FIG. 5, exposure areas Sa and Sb on the photosensitive member when the ratio of the light emission signals of the two light sources A and B is changed. However, the right side direction of the figure is shown as the main scanning direction.

  That is, in FIG. 5, when the light emission time width of the light emission signal is changed between the light source A and the light source B, exposure is performed on the photoconductor in the optical scanning device based on the light emission signals from the light sources A and B. The exposure areas when the light sources A and B are used are exposure areas Sa and Sb, respectively. When the exposure areas of the pixels 3 are Sa3 and Sb3, respectively, the light emission signal is controlled so that the sum of the exposure areas Sall = Sa3 + Sb3 = Sai + Sbi (i is a natural number) = constant, thereby reducing the exposure areas of the two light sources as a whole. Can be constant. At this time, without changing the exposure area per pixel, the center of gravity of the exposure area can be shifted in the sub-scanning direction by changing the light emission time ratio of the light emission signals of the light sources A and B here. . In the case of FIG. 5 as well, it is possible to correct the pixel position deviation in the sub-scanning direction by determining the light emission time ratio of the light emission signal so as to correct the position deviation amount as in FIG.

  FIG. 6 relates to the surface potential on the photosensitive member when the light emission signals of the two light sources are changed.

  FIG. 6 shows the case where the number of light sources m is two light sources A and B. When the light emission time width of the light emission signal is changed between the light sources A and B, the light emission signals from the light sources A and B are used. Exposure is performed on the photosensitive member. At this time, a surface potential sufficient to form a pixel is obtained on the photosensitive member depending on the light emission time and light emission level when the light emission amount exceeds the development threshold. The areas of the light sources A and B that are equal to or smaller than the development threshold at this time are SVa and SVb, respectively. When the area of the pixel 3 is SVa3 and SVb3, respectively, by controlling the light emission signal so that the sum of the area areas SVall = SVa3 + SVb3 = SVai + SVbi (i is a natural number) = constant, it depends on the surface potential of the entire two light sources. The area of the region can be made constant. At this time, without changing the area per pixel, the center of gravity of the area is changed in the sub-scanning direction, and the light emission signals of the light sources A and B (for example, the light emission time ratio in the figure and the light emission level are also possible) are changed. By doing so, the center of gravity of one pixel can be shifted. That is, in the case of FIG. 6, similarly to FIG. 4, by determining the light emission time ratio of the light emission signal so as to correct the positional deviation amount, it is possible to correct the pixel positional deviation in the sub-scanning direction.

  FIG. 7 shows an example in the case of three light sources. 4 and 5, the pixel position shift in the sub-scanning direction is corrected by changing the light emission time ratio of the light emission signals of the two light sources and making the total light emission time and the exposure area of the two light sources substantially constant. However, in the example of FIG. 7, by adding the light source C to the light sources A and B, one pixel is formed by three light sources as shown by the pixel 6 of FIG. Further, when a pixel position shift occurs in the sub-scanning direction with respect to the pixel 6, the center of gravity of one pixel can be obtained by controlling the light emission signals of the light sources A, B, and C as shown in other pixels in FIG. It is possible to shift in the sub-scanning direction, and by determining the light emission time ratio of the light emission signal so as to correct the positional shift amount in the same manner as in FIG. 4, it is possible to correct the pixel position shift in the sub-scanning direction.

  FIG. 8 relates to the exposure energy of the scanning light on the photosensitive member when the light emission level ratio of the light emission signals of a plurality of light sources is changed. That is, FIG. 8 shows that the light source level ratio of the m light sources is changed so that the total exposure energy of the m light sources is constant in order to move the center of gravity of one pixel in the sub-scanning direction. It is a figure for demonstrating the specific example in the case of changing exposure energy ratio.

  In the example of FIG. 8, the ratio of the exposure energy amount is changed by changing the light emission level ratio. For example, in the pixel 3, when the exposure energy of the light source A is Ea3 and the exposure energy of the light source B is Eb3, the light emission level is determined so that the sum of the exposure energy Eall = Ea3 + Eb3 = Eai + Ebi (i is a natural number) = constant. Thus, the exposure energy of the entire two light sources can be made substantially constant. At this time, the center of the exposure energy can be shifted in the sub-scanning direction by changing the ratio of the light emission levels of the light sources A and B without changing the exposure energy per pixel. As described above, in the case of FIG. 7 as well, the pixel position deviation in the sub-scanning direction can be corrected by determining the light emission level ratio so that the amount of positional deviation is corrected similarly to FIG.

  9 and 10 are diagrams for explaining how to change the light emission times of the two light sources A and B in the example of FIG. 4, for example (control operation example of the light source drive control means 50). In FIG. 9, for example, when one dot (for example, pixel 1, pixel 2, pixel 3,... In FIG. 4) is composed of 8 pulses, an example of pulses generated by the light source drive control unit 50 is image data. It is the figure shown with the dot image. FIG. 9 shows an example in which a pulse is formed from the center of one dot. Here, the dot image indicates the width of 1 dot, the image data 1 is a 1/8 width dot, the image data 2 is 2/8 width,..., And the image data 8 is a time width of 8/8 width. It is defined as FIG. 10 is a table showing a pattern for controlling the light emission times of the two light sources A and B as shown in FIG. 4 based on the relationship between the image data of FIG. 9 and the dot image output. The vertical axis of the table represents seven types of control patterns 1 to 7 given to the two light sources A and B, and the numbers of the respective light sources represent the image data of FIG.

  Here, the light source drive control means 50 selects the pattern 1 in FIG. 10 when (000) is given as the correction data, and selects the pattern 2 in FIG. 10 when (001) is given as the correction data. When (010) is given as the correction data, the pattern 3 in FIG. 10 is selected, and when (011) is given as the correction data, the pattern 4 in FIG. 10 is selected, and (100) as the correction data. 10 is selected. When (101) is given as correction data, the pattern 6 in FIG. 10 is selected. When (111) is given as correction data, the pattern shown in FIG. One of seven types of patterns is selected, such as selecting 7. For example, when (000), (001), (010), (011), (100), (101), and (111) are sequentially given as correction data, the light source drive control means 50 uses two light sources A and B. The driving state can be changed as shown in FIG.

  As described above, by changing the control pattern of FIG. 10 according to the sub-scanning dot position shift amount of the pixel, the barycentric position of the pixel can be shifted in the sub-scanning direction as shown in FIG. By selecting the control pattern so as to correct the shift amount, the sub-scanning dot position shift correction can be performed.

  Note that image data as shown in FIG. 9 can be generally generated as a pulse width modulation signal PWM from a pulse modulation signal generation circuit 10 as shown in FIG. The pulse modulation signal generation circuit 10 in FIG. 11 includes a high frequency clock generation circuit 11, a modulation data generation circuit 12, and a serial modulation signal generation circuit 13. Here, the high-frequency clock generation circuit 11 generates a high-frequency clock VCLK that is much faster than a basic cycle that represents one dot, which is generally called a pixel clock required in an image forming apparatus. The modulation data generation circuit 12 generates modulation data representing a desired bit pattern based on image data given from outside such as an image processing unit (not shown). The serial modulation signal generation circuit 13 receives the modulation data output from the modulation data generation circuit 12, converts it into a serial pulse pattern sequence (pulse sequence) based on the high frequency clock VCLK, and outputs the pulse modulation signal PWM. Output as. For example, if modulation data from the outside is directly input to the serial modulation signal generation circuit 13, the modulation data generation circuit 12 can be omitted.

  The greatest feature of such a pulse modulation signal generation circuit 10 is that modulated data is input to the serial modulation signal generation circuit 13, and a pulse train corresponding to the bit pattern of the modulation data is based on a high-frequency clock much faster than the pixel clock. Is generated serially to generate the pulse modulation signal PWM. For example, a shift register may be used for the serial modulation signal generation circuit 13.

  The concept of the pulse modulation signal generation circuit 10 in FIG. 11 is basically used to generate image data as shown in FIG. 9 as the pulse width modulation signal PWM and perform drive control with the control pattern as shown in FIG. A light source modulation signal generation circuit 17 as shown in FIG. 12 can be used.

  That is, in the light source modulation signal generation circuit 17 of FIG. 12, when controlling the two light sources A and B, image data and correction data are used as control data. Here, the image data is a scanner image in a copier, data at the time of printer, or the like. On the other hand, the correction data is data for performing pixel position correction in the sub-scanning direction on the image data, such as pixel position correction data in the sub-scanning direction output from the sub-scanning pixel position detecting unit 51.

  In the light source modulation signal generation circuit 17 of FIG. 12, the image data is converted into modulation data by the modulation data generation circuit 1 (12) and input to the serial modulation signal generation circuit 1 (13). Similarly, the correction data is also converted into modulation data by the modulation data generation circuit 2 (14) and input to the serial modulation signal generations 1, 2 (13, 15), respectively. In the serial modulation signal generation circuits 1 and 2 (13 and 15), a pulse is generated based on the modulation data from the modulation data generation circuits 1 and 2 (12 and 14) and the high-frequency clock output from the high-frequency clock generation circuit 11. Width modulation signals (main light source pulse width modulation signal M-PWM, sub light source pulse width modulation signal S-PWM) are output. This relationship is shown as an image diagram in FIG. 9, and a pulse modulation signal of the illustrated dot image is output based on the input data, which is 4-bit image data here. Here, the main light source pulse width modulation signal M-PWM can be used as the drive control signal for the light source B in FIG. 4, and the sub light source pulse width modulation signal S-PWM can be used as the drive control signal for the light source A in FIG. .

  In this case, any one of the seven types of patterns shown in FIG. 10 can be selected using the correction data. Now, assuming that the pulse width at the time of image data 8 (1000) is the reference lighting time, FIG. 10 shows the relationship between the image data of two light sources and the output pattern. It is set to be 8. At this time, the LUT (look-up table) shown in FIG. 10 is provided, and one of the seven patterns is selected based on the value of the correction data, thereby realizing sub-scanning position shift correction using two light sources. Is possible. Specifically, when the correction data is (000), the pattern 1 in FIG. 10 is selected, the light sources A and B are driven and controlled by the image data 0 and 8 in FIG. 9, respectively, and the correction data is (010). In this case, the pattern 3 in FIG. 10 is selected, and the light sources A and B are driven and controlled by the image data 3 and 5 in FIG. 9, respectively.

  In this way, by using the pulse modulation signal generation circuit 10 of FIG. 11 (more precisely, the light source modulation signal generation circuit 17 of FIG. 12) in the light source drive control means 50, the drive states of the two light sources A and B are illustrated. As shown in FIG.

  In the above-described example, the specific circuit configuration when the light source drive control as shown in FIG. 4 is performed has been described. However, when the light source drive control as shown in FIG. As an alternative, a power modulation signal generation circuit 18 as shown in FIG. 13 can be used instead of the pulse modulation signal generation circuit 10 of FIG. In the power modulation signal generation circuit 18 of FIG. 13, the image data input to the modulation data generation circuit 12 indicates the amount of light emitted from each light source, and the signal intensity-modulated by the modulation data generation circuit 12 generates a high-frequency clock. Based on a high-frequency clock much faster than the pixel clock generated by the circuit 11, a power signal corresponding to the emission intensity of the modulation data can be serially output to generate the power modulation signal PM.

  By configuring a circuit similar to that shown in FIG. 12 based on the circuit shown in FIG. 13, light source drive control as shown in FIG. 8 can be performed.

  Further, when the number of light sources to be controlled is three or more (for example, when the drive control as shown in FIG. 7 is performed), the circuit configuration shown in FIG. it can.

  In the present invention, various forms of light source drive control can be performed in addition to the above-described light source drive control.

(Third embodiment)
The optical scanning device according to the third embodiment of the present invention has basically the same configuration as that shown in FIG. 2 or FIG. 3, and at least n (n ≧ 2) arranged at different positions in the sub-scanning direction. ) Of all the light sources (n.gtoreq.m.gtoreq.2) are formed, and one pixel is formed at a certain image height in the main scanning direction. The light source drive control means 50 which switches a light emission light source is provided so that one pixel may move to the predetermined | prescribed direction of a subscanning direction with the movement amount of this.

  The light source drive control method according to the third embodiment is a general image other than a line image (line image), and has no meaning (0 pixels) in the case of a line image (line image). This applies when all pixels have meaning.

  FIG. 14 is a diagram illustrating a specific example of light source drive control in the third embodiment. In the example of FIG. 14, at first, one pixel is formed in the sub-scanning direction by using two light sources B and C. This example shows the case of writing a line in the main scanning direction of one pixel. The line is assumed to be bent in the sub-scanning direction due to optical variations and mechanical variations. Is assumed to be bent downward in FIG. In this case, in order to correct the bending, if the pixel is arranged so as to move upward in FIG. 14 (if the lighting is switched from the light source C to the light source A), the scanning line bending can be corrected. The downward curve in FIG. 14 is corrected so as not to change the position in the sub-scanning direction. Of course, when it is desired to correct in the reverse direction, it is only necessary to switch the lighting from the light source B to the light source under the light source C, instead of switching the lighting from the light source C to the light source A.

  FIG. 15 shows an example of bending correction when one pixel is formed with one light source in the sub-scanning direction. In this case, one pixel line is written in the main scanning direction by the light source B, and the pixel is moved from the (N + 5) th pixel to the adjacent light source A in the main scanning direction. Thus, by changing the pixel position in the sub-scanning direction, it is possible to correct the scanning line bending. In this case, the correction accuracy is determined by the pixel pitch, and when one pixel writes, for example, at 600 dpi, the scanning line bending correction accuracy is 600 dpi≈42.5 μm. Even in this case, correction is possible if the scanning line bend is sufficiently large, but in general, when the pixel is moved at a 42.5 μm pitch, the positional deviation is a bent line even in view of the visual characteristics of the human eye. It will be recognized.

  On the other hand, if the pixel density is made sufficiently fine, for example, 2400 dpi or 4800 dpi pitch, the pixel position correction accuracy will be about 10 μm and 5 μm, respectively. Scan line bending correction can be performed without being recognized. However, from the viewpoint of making an image rather than from the viewpoint of correction, it can be said that writing of 4800 dpi is excessive quality, and setting all systems to 4800 dpi or more is performed even in view of the enormous amount of data. It is hard to think that things are desirable.

  15 has the above-described problem, in the light source drive control as shown in FIG. 14, the writing light source has a resolution of, for example, 2400 dpi or 4800 dpi, and 600 dpi or 1200 dpi as image data. If data is written, that is, if the writing resolution is different from the image data resolution and the writing resolution is greater than the image data resolution, the image data is ensured to be sufficient and the position correction such as scanning line bending is written. An optical writing system that performs finer resolution can be constructed.

  As described above, in the third embodiment, for example, in a general image other than a line image (line image), an optical system and mechanical scanning line bending can be corrected with high accuracy.

  FIG. 16 is a diagram illustrating another specific example of the light source drive control in the third embodiment. Also in the case of FIG. 16, at first, one pixel is formed in the sub-scanning direction by three light sources B, C, and D, and the N + 5th pixel in the main scanning direction is changed to three light sources A, B, and C. By switching the lighting, as in the case of FIG. 14, for example, in a general image other than a line image (line image), optical system and mechanical scanning line bending can be corrected with high accuracy.

(Fourth embodiment)
The optical scanning device according to the fourth embodiment of the present invention has basically the same configuration as that shown in FIG. 2 or 3 and is arranged as a first pattern at least at a position different in the sub-scanning direction. Among n (n ≧ 2) light sources, up to an image height in the main scanning direction, one pixel is formed with all m (n> m ≧ 2) light sources, and an image height in the main scanning direction. From (m + 1) light sources, one pixel is formed, and at a certain image height in the main scanning direction thereafter, one pixel is subtracted from the initial one pixel with a movement amount equal to the length of the pitch of one light source. Light source drive control means for changing the drive state of the light source so as to move in a predetermined direction in the scanning direction and to form one pixel for all m light sources moved in the sub-scanning direction by one light source compared to the initial direction. 50 is provided.

  Alternatively, as the second pattern, of n (n ≧ 2) light sources arranged at least at different positions in the sub-scanning direction, initially m (n> m ≧) up to a certain image height in the main scanning direction. The light source driving control means 50 for changing the driving state of the light source so that one pixel is formed by the entire light source of 2) and one pixel is formed by all the (m + 1) light sources from a certain image height in the main scanning direction. Is provided.

  Then, in the first pattern or the second pattern, the light source drive control means 50 is configured to at least one of the (m + 1) light sources during a period in which one pixel is formed with the entire (m + 1) light sources. Smoothing processing for smoothing the edge of the pixel is performed by changing the driving state of the light source at the end stepwise.

  Here, PWM (pulse width modulation), PM (power modulation), or PWM (pulse width modulation) and PM (power modulation) can be used for the smoothing process. Can also be used in combination.

  Note that the light source drive control method in the fourth embodiment is such that the image is a line image (line image) and has a meaningless pixel (0 pixel) outside the line image (line image). Applied.

FIG. 17 is a diagram illustrating a specific example of light source drive control in the fourth embodiment (example of the first pattern in the fourth embodiment). In the example of FIG. 17, as in the example of FIG. 14, one pixel is initially formed by two light sources B and C, but in the example of FIG. 17, as in the example of FIG. 14, The pixel edge is smoothed by performing pulse width modulation in conjunction with the light source C and the light source A without suddenly switching from the light source C to the light source A at the pixel N + 5 (that is, pixel position correction finer than the pitch between the light sources) ) Is possible. In the example of FIG. 17, for example, assuming that the pulse width has 12 values,
Before pixel N + 1 Light source C: PWM value 12 Light source A: PWM0 (that is, no light is emitted)
Pixel N + 2 Light source C: PWM value 10 Light source A: PWM2
Pixel N + 3 Light source C: PWM value 8 Light source A: PWM4
Pixel N + 4 Light source C: PWM value 6 Light source A: PWM 6
Pixel N + 5 Light source C: PWM value 4 Light source A: PWM 8
Pixel N + 6 Light source C: PWM value 2 Light source A: PWM 10
Pixel N + 7 Light source C: PWM value 0 Light source A: PWM12
Then, smoother pixel position correction can be performed with respect to scanning line bending or the like. That is, in the example of FIG. 17, the driving state of the light sources A and C at both ends of the (m + 1) (three) light sources A, B, and C is changed stepwise to smooth the edge of the pixel. Can do.

  FIGS. 18 to 21 are diagrams showing another specific example (example of the first pattern in the fourth embodiment) of the light source drive control in the fourth embodiment.

  In FIG. 18, in the fourth embodiment, one pixel is initially composed of three light sources B, C, and D, and then one pixel is composed of four light sources A, B, C, and D, and then one pixel is composed. An example in which three light sources A, B, and C are used is shown. In the case of FIG. 18 as well, the driving state of the light sources A and D at both ends of the (m + 1) (four) light sources A, B, C, and D is changed stepwise in the same manner as in FIG. Thus, the edge of the pixel can be smoothed.

  FIG. 19 shows that in the fourth embodiment, one pixel is initially composed of four light sources B, C, D, and E, and then one pixel is composed of five light sources A, B, C, D, and E. Thereafter, an example in which one pixel is constituted by four light sources A, B, C, and D is shown. In the example of FIG. 19, for example, when one pixel in the sub-scanning direction is 600 dpi, the light source pitch is arranged at 2400 dpi pitch. Therefore, even when the light source is suddenly switched as shown in FIG. 16, the pitch is 2400 dpi. Although a sufficiently fine accuracy can be obtained, the pixel position can be corrected more smoothly by adding PWM (pulse width modulation) as shown in FIG.

  Also, FIG. 20 attempts to perform smooth correction with PM (power modulation), whereas FIG. 19 attempts to perform smooth correction with PWM (pulse width modulation). In the case of PM, if the light source unit has, for example, a DAC unit that sets the drive current to a desired value, correction as shown in FIG. 20 is possible.

  FIG. 21 shows an example of drive control in which both PWM and PM are provided in order to perform smoother pixel position correction, and smoother pixel position correction is possible.

  In the specific examples described above (specific examples in FIGS. 17 to 21), in the first pattern of the fourth embodiment, during the period in which one pixel is formed with all (m + 1) light sources, (m + 1) The driving states of the light sources at both ends of the individual light sources are changed stepwise to smooth the edges of the pixels at both ends.

  On the other hand, FIG. 22 shows a specific example of the second pattern of the fourth embodiment. In the specific example of the second pattern, (m + 1) (three in the example of FIG. 22) light sources A. , B, and C, in a period in which one pixel is formed, only the driving state of the light source A at one end of the (m + 1) (three) light sources A, B, and C is changed stepwise. The pixel edges are smoothed.

  Even in the first pattern of the fourth embodiment, only the driving state of the light source at one end of the (m + 1) light sources can be changed in a stepwise manner. In the case of the first pattern, in order to make the edge of the pixel smoother, the driving states of the light sources at both ends of the (m + 1) light sources are stepwise as in the specific examples of FIGS. It is preferable to smooth the edges of the pixels at both ends by changing.

  Further, as the light source drive control means 50, according to whether the image is a line image (line image) or a general image other than the line image (line image), the drive control of the fourth embodiment, the third embodiment It is also possible to configure so that one of the drive controls is switched and selected.

  In each of the embodiments described above, the n light sources include surface emitting lasers (more preferably, surface emitting laser arrays in which n surface emitting lasers are arranged in an array) configured on the same chip. It is preferably used.

  When a surface emitting laser is used as the light source of the optical scanning device, the surface emitting laser can save power compared with a normal semiconductor laser. Further, since the configuration of the plurality of light sources and the light source arrangement can be arbitrarily set, a light source corresponding to the resolution and speed can be provided. Therefore, power saving and highly accurate optical scanning can be performed.

(Fifth embodiment)
The fifth embodiment of the present invention is an image forming apparatus using the above-described optical scanning device of the present invention.

  FIG. 23 is a diagram showing an example of an image forming apparatus using the optical scanning device of the present invention. Referring to FIG. 23, on the back surface of the light source unit 801, a printed circuit board 802 on which a driving circuit for controlling a semiconductor laser and a pixel clock generation device are formed is mounted. The contact is made, and the inclination is adjusted by the adjusting screw 803 to maintain the posture. The adjusting screw 803 is screwed into a protrusion formed on the wall surface of the housing. Inside the optical housing, a cylinder lens 805, a polygon motor 808 that rotates a polygon mirror, an fθ lens 806, a toroidal lens, and a folding mirror 807 are positioned and supported, respectively, and a printed circuit board 809 on which a synchronization detection sensor is mounted includes: Like the light source unit, it is mounted on the housing wall from the outside. The upper portion of the optical housing is sealed with a cover 811 and fixed to the frame member of the image forming apparatus main body with a plurality of mounting portions 810 protruding from the wall surface.

  At this time, a semiconductor laser array having a plurality of light sources as shown in FIG. 1 (specifically, for example, a surface emitting laser (surface emitting laser array)) can be used as the semiconductor laser. The light emitted from the semiconductor laser is deflected and scanned by the polygon mirror as it rotates through the cylinder lens 805, and the deflected and scanned light beam is shown through the fθ lens 806, the toroidal lens, the folding mirror 807, and the like. Not incident on the photoreceptor drum. Further, the scanning light is detected by the sensor as a region not scanned by the photosensitive member or reflected light from a mirror or the like. As a signal detected by the sensor at this time, a time interval between two points in the main scanning direction, which is the scanning direction associated with the rotation of the polygon mirror, is detected by a synchronous detection sensor, or a direction rotated 90 degrees with respect to the main scanning direction The pixel position can be corrected by measuring the amount of misalignment in the sub-scanning direction with a position detection sensor and performing feedback control of the value to the LD control and the modulation circuit or the preceding modulation data generation unit. .

  Next, a multi-beam scanning device (multi-beam optical system) configured using a plurality of light sources will be described.

  FIG. 24 is a diagram illustrating an example of a multi-beam scanning device. In the example of FIG. 24, two (301, 302) semiconductor laser arrays (four channels) in which two light emitting sources are monolithically arranged at an interval ds = 25 μm are used (eight light sources are used).

  In FIG. 24, the semiconductor laser arrays 301 and 302 have the same optical axis as that of the collimating lenses 303 and 304, have an emission angle symmetrical with respect to the main scanning direction, and the emission axes intersect at the reflection point of the polygon mirror 307. It is laid out. A plurality of beams emitted from the respective semiconductor laser arrays 301 and 302 are collectively scanned by a polygon mirror 307 through a cylinder lens 308 and imaged on a photoconductor 312 by an fθ lens 310 and a toroidal lens 311. Print data for one line is stored in the buffer memory for each light source, read out for each surface of the polygon mirror, and recorded simultaneously for four lines.

  In addition, in order to correct the optical scanning length difference and magnification difference caused by the wavelength error of each LD constituting the multi-beam, the phase difference of the pixel clock is shifted to correct the scanning length difference to the phase accuracy. In addition, variations in scanning light can be reduced.

  FIG. 25 shows an example in which a laser array arranged in the sub-scanning direction is used as a light source unit of an optical scanning device when the vertical direction in the drawing is the sub-scanning direction of the optical system. The example of FIG. 25 uses a laser array having four light emitting sources in the vertical direction.

  FIG. 26 shows an example in which a surface emitting laser array in which a plurality of surface emitting lasers are arranged in an array is used for a light source unit of an optical scanning device. In the example of FIG. 26, a surface emitting laser array having a total of 12 light emitting sources (surface emitting lasers), 3 in the horizontal direction and 4 in the vertical direction, is shown.

  FIG. 27 is a diagram showing a configuration example of the image forming apparatus of the present invention. Referring to FIG. 27, around the photosensitive drum 901 that is the surface to be scanned, a charging charger 902 that charges the photosensitive member to a high voltage and a toner charged to the electrostatic latent image recorded by the optical scanning device 900 are attached. A developing roller 903 that visualizes the toner, a toner cartridge 904 that supplies toner to the developing roller 903, and a cleaning case 905 that scrapes and stores toner remaining on the drum 901 are disposed. As described above, a plurality of lines are simultaneously recorded on the photosensitive drum 901 for each surface. The recording paper is supplied from the paper supply tray 906 by the paper supply roller 907, is sent out by the registration roller pair 908 in accordance with the recording start timing in the sub-scanning direction, and is transferred to the toner by the transfer charger 906 when passing the photosensitive drum 901. Is transferred, fixed by the fixing roller 909, and discharged to the paper discharge tray 910 by the paper discharge roller 912. By applying the optical scanning device of the present invention to the optical scanning device 900 of the image forming apparatus, dot position correction with high accuracy becomes possible, and a high-quality image can be obtained.

  The present invention is also applicable to a color image forming apparatus. FIG. 28 shows an example in which the present invention is mounted on a tandem color machine which is an image forming apparatus having a plurality of photoconductors. The tandem color machine requires separate photoconductors corresponding to cyan, magenta, yellow, and black colors, and the optical scanning optical system forms latent images through different optical paths corresponding to the photoconductors. . Therefore, the main scanning dot position shift generated on each photoconductor often has different characteristics.

  In FIG. 28, 18 is a transfer belt, 19a, 19b, 19c and 19d are photoconductors corresponding to the respective colors, and 20a, 20b, 20c and 20d are optical scanning devices corresponding to the respective colors.

  Here, by using the optical scanning device of the present invention for the optical scanning devices 20a, 20b, 20c, and 20d, it is possible to obtain a high-quality image in which the sub-scanning dot position deviation is well corrected. In particular, in terms of image quality, the present invention is effective for misregistration in the sub-scanning direction, and an image with good color reproducibility can be obtained in which color misregistration between stations is effectively reduced.

  FIG. 30 is a diagram showing a hardware configuration example of the light source drive control means of the optical scanning device of the present invention. In this example, the CPU 101, the ROM 102, the RAM 103, the HDD (hard disk drive) 104, the HD (hard disk) 105, the FDD (flexible disk drive) 106, and the like are connected by the bus 100 as the light source drive control means.

  The CPU 101 controls the entire apparatus. The ROM 102 stores a control program. The RAM 103 is used as a work area for the CPU 101. The HDD 104 controls data read / write with respect to the HD 105 according to the control of the CPU 101. The HD 105 stores data written according to the control of the HDD 104. The FDD 106 performs data read / write control with respect to the FD (flexible disk) 107 in accordance with the control of the CPU 101. The FD 107 is detachable and stores data written according to the control of the FDD 106.

  Note that the processing in the light source drive control means 50 described in the above-described best mode for carrying out the present invention can be provided in the form of a program realized by a computer (for example, the CPU 101).

  A program for causing a computer to execute the processing in the light source drive control means 50 described in the above-described best mode for carrying out the present invention includes a hard disk (105), a floppy (registered trademark) disk, a CD-ROM, The program is recorded on a computer-readable recording medium such as MO and DVD, and is executed by being read from the recording medium by the computer. Further, this program can be distributed via a network such as the Internet through the recording medium.

  In the second, third, and fourth embodiments described above, the light sources A, B, and C in FIGS. 7, 14, 17, and 22 are, for example, the light sources a1, a2, and a3 in FIG. The light sources A, B, C, and D in FIGS. 16 and 18 can be, for example, the light sources a1, a2, a3, and a4 in FIG. 1, respectively, and FIGS. The light sources A, B, C, D, and E can be the light sources a1, a2, a3, a4, and b1 in FIG. In FIG. 1, four light sources are arranged in the horizontal direction as a1 to a4. However, the number of light sources in the horizontal direction is not limited to that in FIG. be able to. That is, the number of light sources in the horizontal direction may be, for example, three a1 to a3 or five a1 to a5.

The present invention can be used in laser printers, digital copying machines, and the like.

It is a figure which shows an example of a light source unit. It is a figure which shows the structural example of the optical scanning device of this invention. It is a figure which shows the structural example of the optical scanning device of this invention. It is a figure for demonstrating the specific example of the method of changing the drive state of m light sources. It is a figure for demonstrating the specific example of the method of changing the drive state of m light sources. It is a figure for demonstrating the specific example of the method of changing the drive state of m light sources. It is a figure for demonstrating the specific example of the method of changing the drive state of m light sources. It is a figure for demonstrating the specific example of the method of changing the drive state of m light sources. It is a figure for demonstrating the control operation example of a light source drive control means. It is a figure for demonstrating the control operation example of a light source drive control means. It is a figure which shows the basic structural example of a pulse modulation signal generation circuit. It is a figure which shows the structural example of the light source modulation signal generation circuit using the basic structural example of the pulse modulation signal generation circuit of FIG. It is a figure which shows the basic structural example of a power modulation signal generation circuit. It is a figure which shows the specific example of the light source drive control in 3rd Embodiment. It is a figure which shows the example of curvature correction in the case of forming one pixel with one light source in the sub-scanning direction. In 3rd Embodiment, it is a figure which shows the specific example of the light source drive control in the case of comprising one pixel by 3 light sources A, B, and C. It is a figure which shows the specific example of the light source drive control in 4th Embodiment. It is a figure which shows the specific example of the light source drive control in 4th Embodiment. It is a figure which shows the specific example of the light source drive control in 4th Embodiment. It is a figure which shows the specific example of the light source drive control in 4th Embodiment. It is a figure which shows the specific example of the light source drive control in 4th Embodiment. It is a figure which shows the specific example of the light source drive control in 4th Embodiment. It is a figure which shows an example of the image forming apparatus using the optical scanning device of this invention. It is a figure which shows an example of a multi-beam scanning apparatus. It is a figure which shows an example of a light source unit. It is a figure which shows an example of a light source unit. 1 is a diagram illustrating a configuration example of an image forming apparatus of the present invention. 1 is a diagram illustrating an example of a color image forming apparatus. 1 is a diagram illustrating a configuration example of a general image forming apparatus. It is a figure which shows the hardware structural example of the light source drive control means of the optical scanning device of this invention.

Explanation of symbols

50 Light source drive control means 51 Sub-scanning pixel position detection means 11 High frequency clock generation circuit 12, 14 Modulation data generation circuit 13, 15 Serial modulation signal generation circuit 801, 802 Light source unit 100 Bus 101 CPU
102 ROM
103 RAM
104 HDD (Hard Disk Drive)
105 HD (hard disk)
106 FDD (flexible disk drive)
107 FD (flexible disc)

Claims (22)

One pixel is formed by all m (n ≧ m ≧ 2) light sources among n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction. A pixel forming apparatus. One pixel is formed by all m (n ≧ m ≧ 2) light sources out of n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction. An optical scanning device comprising light source drive control means for changing the drive state of m light sources in order to move the center of gravity of the light source in the sub-scanning direction. One pixel is formed by all m (n ≧ m ≧ 2) light sources out of n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction. When correction data for moving the center of gravity in the sub-scanning direction is given, a light source that changes the driving state of the m light sources to move the center of gravity of one pixel in the sub-scanning direction by an amount corresponding to the correction data An optical scanning device characterized in that drive control means is provided. 4. The optical scanning device according to claim 3, further comprising sub-scanning pixel position detecting means for detecting sub-scanning pixel positions and outputting correction data for performing pixel position correction in the sub-scanning direction, The light source drive control means is characterized in that the driving state of m light sources is changed in order to move the center of gravity of one pixel in the sub-scanning direction by an amount corresponding to the correction data output from the sub-scanning pixel position detecting means. Optical scanning device. 5. The optical scanning device according to claim 2, wherein the light source drive control unit includes a total light emission time or total of m light sources in order to move the center of gravity of one pixel in the sub-scanning direction. An optical scanning device characterized by changing a light emission time ratio of m light sources so that an exposure area is constant. 5. The optical scanning device according to claim 2, wherein the light source drive control unit has a constant total exposure energy of m light sources in order to move the center of gravity of one pixel in the sub-scanning direction. An optical scanning device characterized by changing the light emission level ratio of m light sources so as to change the exposure energy ratio of m light sources. One pixel is formed of all m (n ≧ m ≧ 2) light sources out of n (n ≧ 2) light sources arranged at least in different positions in the sub-scanning direction. An optical scanning method characterized in that the center of gravity of one pixel is moved in the sub-scanning direction by changing the driving state of the light source. One pixel is formed by all of m (n ≧ m ≧ 2) light sources out of n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction. Light source drive control means for switching the light source is provided so that one pixel moves in a predetermined direction in the sub-scanning direction with a moving amount of the same length as the pitch length of one light source at a certain image height. An optical scanning device characterized by the above. One pixel is formed by all of m (n ≧ m ≧ 2) light sources out of n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction. An optical scanning method characterized by switching light emitting light sources so that one pixel moves in a predetermined direction in the sub-scanning direction with a moving amount having the same length as the pitch length of one light source at a certain image height. Of the n (n ≧ 2) light sources arranged at least at different positions in the sub-scanning direction, at first, up to a certain image height in the main scanning direction, the entire m light sources (n> m ≧ 2) are one pixel. From the image height in the main scanning direction, one pixel is formed by all (m + 1) light sources, and the movement is the same length as the pitch of one light source in the image height in the main scanning direction thereafter. One pixel is moved from the original one pixel in a predetermined direction in the sub-scanning direction by an amount, and one pixel is formed by all m light sources moved in the sub-scanning direction by one light source compared to the original. An optical scanning device comprising a light source drive control means for changing a drive state of a light source. Of the n (n ≧ 2) light sources arranged at least at different positions in the sub-scanning direction, at first, up to a certain image height in the main scanning direction, the entire m light sources (n> m ≧ 2) are one pixel. And a light source driving control means for changing the driving state of the light source is provided so that one pixel is formed from all (m + 1) light sources from an image height in the main scanning direction. Optical scanning device. 12. The optical scanning device according to claim 10, wherein the light source drive control means includes at least one of (m + 1) light sources during a period in which one pixel is formed of all (m + 1) light sources. An optical scanning device characterized in that smoothing processing is performed to smooth the edge of a pixel by changing the driving state of an end light source stepwise. 13. The optical scanning device according to claim 12, wherein the light source drive control means uses PWM (pulse width modulation) for the smoothing process. 13. The optical scanning device according to claim 12, wherein the light source drive control means uses PM (power modulation) for the smoothing process. 13. The optical scanning device according to claim 12, wherein the light source drive control means uses a combination of PWM (pulse width modulation) and PM (power modulation) for the smoothing processing. Of the n (n ≧ 2) light sources arranged at least at different positions in the sub-scanning direction, at first, up to a certain image height in the main scanning direction, the entire m light sources (n> m ≧ 2) are one pixel. From the image height in the main scanning direction, one pixel is formed by all (m + 1) light sources, and the movement is the same length as the pitch of one light source in the image height in the main scanning direction thereafter. The drive state of the light source is changed so that one pixel is moved in a predetermined direction from the original one pixel by a quantity, and one pixel is formed by all m light sources moved by one light source compared to the original. An optical scanning method. Of the n (n ≧ 2) light sources arranged at least at different positions in the sub-scanning direction, at first, up to a certain image height in the main scanning direction, the entire m light sources (n> m ≧ 2) are one pixel. And a driving state of the light source is changed so that one pixel is formed from all (m + 1) light sources from a certain image height in the main scanning direction. 16. The optical scanning device according to claim 2, wherein the n light sources are surface-emitting lasers configured on the same chip. An optical scanning device characterized in that is used. An image forming apparatus comprising the optical scanning device according to any one of claims 2 to 6, 6, 8, 10 to 15, and 18. A color image forming apparatus comprising the optical scanning device according to any one of claims 2 to 6, 6, 8, 10 to 15, and 18. One pixel is formed by all m (n ≧ m ≧ 2) light sources out of n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction. When correction data for moving the center of gravity in the sub-scanning direction is given, a light source that changes the driving state of the m light sources to move the center of gravity of one pixel in the sub-scanning direction by an amount corresponding to the correction data A program for causing a computer to implement drive control processing. One pixel is formed by all m (n ≧ m ≧ 2) light sources out of n (n ≧ 2) light sources arranged at different positions in at least the sub-scanning direction. When correction data for moving the center of gravity in the sub-scanning direction is given, a light source that changes the driving state of the m light sources to move the center of gravity of one pixel in the sub-scanning direction by an amount corresponding to the correction data A computer-readable recording medium on which a program for causing a computer to execute drive control processing is recorded.

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