JP4708785B2 - Image exposure method and apparatus - Google Patents

Description

  BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an image exposure apparatus, and more particularly, an image in which light modulated by a spatial light modulation element is passed through an imaging optical system and an image formed by the light is formed on a photosensitive material to expose the photosensitive material. The present invention relates to an exposure apparatus.

  The present invention also relates to an exposure method using the image exposure apparatus as described above.

  2. Description of the Related Art Conventionally, there has been known an image exposure apparatus that passes light modulated by a spatial light modulation element through an imaging optical system, forms an image of this light on a predetermined photosensitive material, and exposes the photosensitive material. This type of image exposure apparatus basically includes a spatial light modulation element in which a large number of pixel units that modulate irradiated light according to a control signal are two-dimensionally arranged, and the spatial light modulation element. A light source for irradiating light and an imaging optical system for forming an image of light modulated by the spatial light modulation element on a photosensitive material are provided. Note that Non-Patent Document 1 and Japanese Patent Application No. 2002-149886 by the applicant of the present application show an example of an image exposure apparatus having the above basic configuration.

  In this type of image exposure apparatus, for example, an LCD (liquid crystal display element), a DMD (digital micromirror device), or the like can be suitably used as the spatial light modulation element. The DMD is a mirror device in which a number of micromirrors that change the angle of the reflecting surface in accordance with a control signal are two-dimensionally arranged on a semiconductor substrate such as silicon.

  In the image exposure apparatus as described above, there is often a demand for enlarging an image projected on a photosensitive material, and in that case, an enlarged imaging optical system is used as an imaging optical system. In doing so, simply passing the light that has passed through the spatial light modulation element through the magnification imaging optical system expands the luminous flux from each pixel portion of the spatial light modulation element, and the pixel size in the projected image is reduced. The image becomes larger and the sharpness of the image decreases.

  Therefore, as shown in the specification of Japanese Patent Application No. 2002-149886, a first imaging optical system is disposed in the optical path of the light modulated by the spatial light modulation element, and an imaging surface formed by this imaging optical system. Includes a microlens array in which microlenses corresponding to the respective pixel portions of the spatial light modulator are arranged in an array, and the optical path of the light that has passed through the microlens array depends on the modulated light. It has been considered that a second imaging optical system that forms an image on a photosensitive material or a screen is disposed, and the image is enlarged and projected by the first and second imaging optical systems. In this configuration, the size of the image projected on the photosensitive material and the screen is enlarged, while the light from each pixel portion of the spatial light modulator is condensed by each microlens of the microlens array. Since the pixel size (spot size) in the image is reduced and kept small, the sharpness of the image can be kept high.

Patent Document 1 shows an example of an image exposure apparatus using DMD as a spatial light modulation element and combining it with a microlens array.
JP 2001-305663 A Akihito Ishikawa "Development shortening and mass production application by maskless exposure", "Electrotronics packaging technology", Technical Research Committee, Vol.18, No.6, 2002, p.74-79

  By the way, in the conventional image exposure apparatus in which the spatial light modulator and the microlens array are combined as described above, the shape of the beam condensed by each microlens of the microlens array is distorted. The problem is recognized. This problem is particularly noticeable when the above-described DMD is used as a spatial light modulator.

  The present invention has been made in view of the above circumstances, and an object of the present invention is to prevent distortion of a beam condensed by a microlens in an image exposure apparatus in which a spatial light modulation element and a microlens array are combined. To do.

  Another object of the present invention is to provide an image exposure method capable of preventing the beam distortion.

A first image exposure apparatus according to the present invention includes:
As described above, a spatial light modulation element in which a large number of pixel portions each modulating the irradiated light are arranged in a two-dimensional manner,
A light source for irradiating light to the spatial light modulator;
Including a microlens array in which microlenses for condensing light from each pixel portion of the spatial light modulator are arranged in an array, and an image formed by the light modulated by the spatial light modulator is formed on a photosensitive material. In an image exposure apparatus comprising an imaging optical system for forming an image,
Each microlens of the microlens array has an aspherical shape that corrects aberration due to distortion of the surface of the pixel portion.

  As the aspheric surface, for example, a toric surface can be preferably used.

  A second image exposure apparatus according to the present invention is an image exposure apparatus including a spatial light modulation element, a light source, and an imaging optical system similar to those in the first image exposure apparatus. Each microlens of the included microlens array has a refractive index distribution for correcting aberration due to distortion of the surface of the pixel portion.

The third image exposure apparatus according to the present invention is
A spatial light modulation element in which a large number of rectangular pixel portions each modulating the irradiated light are arranged two-dimensionally;
A light source for irradiating light to the spatial light modulator;
Including a microlens array in which microlenses for condensing light from each pixel portion of the spatial light modulator are arranged in an array, and an image formed by the light modulated by the spatial light modulator is formed on a photosensitive material. In an image exposure apparatus comprising an imaging optical system for forming an image,
Each microlens of the microlens array included in the imaging optical system has a lens opening shape that does not allow light from the peripheral portion of the pixel portion of the spatial light modulation element to enter. .

  The third image exposure apparatus also has a characteristic part of the first image exposure apparatus, and each microlens of the microlens array corrects aberration due to distortion of the surface of the pixel portion of the spatial light modulator. It is particularly desirable to have an aspheric shape. In that case, the aspherical surface is preferably a toric surface.

  The third image exposure apparatus also has a characteristic part of the second image exposure apparatus, and each microlens of the microlens array corrects an aberration caused by distortion of the surface of the pixel portion of the spatial light modulator. It is particularly desirable to have a rate distribution.

  In the third image exposure apparatus, each microlens of the microlens array preferably has a circular lens opening.

  In the third image exposure apparatus, it is preferable that the opening shape of the microlens is defined by providing a light shielding portion on a part of the lens surface.

  In the first to third image exposure apparatuses according to the present invention described above, the imaging optical system includes a part of the optical system that forms an image of light modulated by the spatial light modulation element on the microlens array. In the case of having the optical system, it is desirable that the imaging position of a part of the optical system is set on the lens surface of the microlens array.

  Furthermore, in the first to third image exposure apparatuses according to the present invention described above, the imaging optical system includes a first imaging optical system and a second imaging optical system similar to those described above. In this case, an aperture array having a large number of apertures arranged in an array to individually squeeze light emitted from the microlens is disposed between the microlens array and the second imaging optical system. Is desirable. In that case, it is desirable that the aperture array is disposed at the focal position of the microlens.

  Further, each of the first to third image exposure apparatuses according to the present invention uses a DMD (digital micromirror device) in which micromirrors as pixel portions are two-dimensionally arranged as a spatial light modulation element. It is desirable to be configured based on

  On the other hand, an image exposure method according to the present invention is characterized in that a predetermined pattern is exposed onto a photosensitive material using the image exposure apparatus according to the present invention described above.

  According to the inventor's research, the above-mentioned problem that the shape of the beam condensed by the microlens is distorted is caused by distortion of the surface of the pixel portion of the spatial light modulator. found. In particular, in DMD, it has been considered that the reflection surface of a micromirror serving as a pixel portion is formed with high precision and flatness, but according to the analysis of the present inventors, this reflection surface is considerably distorted. When the image exposure apparatus is configured using the DMD as a spatial light modulation element, the above problem is likely to occur.

  In view of the above knowledge, in the first image exposure apparatus according to the present invention, each microlens of the microlens array has an aspherical shape that corrects aberration due to distortion of the surface of the pixel portion of the spatial light modulator. Is. Therefore, according to the first image exposure apparatus of the present invention, it is possible to prevent the problem caused by the distortion of the surface of the pixel portion, that is, the problem that the shape of the condensed beam at the condensing position is distorted. Become.

  In the second image exposure apparatus according to the present invention, in view of the above knowledge, each microlens of the microlens array has a refractive index distribution that corrects aberration due to distortion of the surface of the pixel portion. . Therefore, also in the second image exposure apparatus according to the present invention, it is possible to prevent the above problem, that is, the problem that the shape of the condensed beam at the condensing position is distorted.

  As described above, if it is possible to prevent the shape of the beam collected by each microlens of the microlens array from being distorted, a higher-definition image without distortion can be exposed.

  Further, according to the research of the present inventor, especially in DMD, the amount of change in distortion of a rectangular micromirror serving as a pixel portion tends to increase from the center of the pixel portion to the periphery. When the image exposure apparatus is configured by using it as a modulation element, the above problem is likely to occur.

  In view of the above knowledge, in the third image exposure apparatus according to the present invention, each microlens of the microlens array has a lens opening shape that does not allow light from the periphery of the rectangular pixel portion of the spatial light modulator to enter. It is supposed to have. Therefore, according to the third image exposure apparatus, the light that has passed through the periphery of the pixel unit having a large amount of change in distortion is not collected by the microlens, and the shape of the collected beam at the condensing position is distorted. It is possible to prevent problems that occur.

  As described above, if it is possible to prevent the shape of the beam collected by each microlens of the microlens array from being distorted, a higher-definition image without distortion can be exposed.

  In the third image exposure apparatus, in particular, when each microlens of the microlens array has an aspherical shape that corrects aberration due to distortion of the surface of the pixel portion of the spatial light modulator, it is as described above. Since the effect by the aspherical shape (the effect in the first image exposure apparatus) can be obtained synergistically, it is possible to expose a higher definition image without further distortion.

  In the third image exposure apparatus, in particular, when each microlens of the microlens array has a refractive index distribution that corrects aberration due to distortion of the surface of the pixel portion of the spatial light modulator, Since the effect (the effect in the second image exposure apparatus) obtained by providing such a refractive index distribution can also be obtained synergistically, a higher-definition image without further distortion can be exposed.

  Further, in the third image exposure apparatus, when the opening shape of the microlens is defined by providing a light shielding portion on a part of the lens surface, the microlens opening shape passes through the peripheral portion of the pixel portion of the spatial light modulation element. Since the light is blocked by the light shielding portion, the problem that the shape of the condensed beam at the condensing position is distorted can be prevented more reliably.

  In the first to third image exposure apparatuses according to the present invention described above, in particular, the imaging optical system is a part of the optical system that forms an image of light modulated by the spatial light modulation element on the microlens array. When the image forming position of a part of the optical system is set on the lens surface of the microlens array, the image of the pixel portion connected by the part of the optical system is It becomes the smallest state on the surface. If so, the beam can be narrowed down to the minimum on the photosensitive material, so that a higher definition image can be exposed. In general, a pixel portion such as a DMD micromirror is generally less distorted near the center. Therefore, if the image of the pixel portion is the smallest on the lens surface as described above, the pixel portion starts from the vicinity of the center. It is also possible to improve the focusing performance of the microlens by allowing only light with less aberration to pass through the microlens.

  And when the imaging position of the first imaging optical system is set on the lens surface of the microlens array as described above, in particular, the microlens is provided with a light shielding portion on a part of the lens surface, It is assumed that the light from the peripheral portion of the rectangular pixel portion of the spatial light modulator is made into a lens opening shape that does not enter and has an aspheric shape or a refractive index distribution that corrects aberration due to distortion of the surface of the pixel portion. In particular, the light utilization efficiency is increased, and the photosensitive material can be exposed with higher intensity light. That is, in this case, the first imaging optical system refracts the light so that the stray light due to the distortion of the surface of the pixel portion is focused at one point at the imaging position of the optical system, but the aperture is limited to this position. If the light shielding part is formed, light other than stray light is not shielded, and light utilization efficiency is improved.

  Further, in the first to third image exposure apparatuses according to the present invention described above, in particular, the imaging optical system forms a first image formed by the light modulated by the spatial light modulator on the microlens array. An optical system and a second imaging optical system that forms an image of light collected by the microlens array on the photosensitive material, the microlens array and the second imaging optical system; In the case where an aperture array in which a large number of apertures for individually narrowing the light emitted from the microlens are arranged in an array is arranged between each adjacent microlens that does not correspond to each aperture Is prevented from entering, and the extinction ratio is increased. This effect can be obtained particularly remarkably when the aperture array is arranged at the focal position of the microlens.

  The first to third image exposure apparatuses according to the present invention are configured on the assumption that the image exposure apparatus uses a DMD (digital micromirror device) in which micromirrors are arranged two-dimensionally as a spatial light modulation element. In this case, it can be said that it is particularly preferable because the above-mentioned problem that is particularly likely to occur can be prevented.

  On the other hand, since the image exposure method according to the present invention exposes a predetermined pattern onto a photosensitive material using the image exposure apparatus according to the present invention described above, the shape of the condensed beam at the condensing position is distorted. This makes it possible to expose a high-definition pattern.

  An image exposure apparatus according to an embodiment of the present invention will be described below with reference to the drawings.

[Configuration of image exposure apparatus]
As shown in FIG. 1, the image exposure apparatus includes a flat plate-shaped moving stage 152 that holds a sheet-like photosensitive material 150 on the surface thereof. Two guides 158 extending along the stage moving direction are installed on the upper surface of the thick plate-shaped installation table 156 supported by the four legs 154. The stage 152 is disposed so that the longitudinal direction thereof faces the stage moving direction, and is supported by a guide 158 so as to be reciprocally movable. The image exposure apparatus is provided with a stage drive unit 304 (see FIG. 15), which will be described later, that drives a stage 152 as sub-scanning means along a guide 158.

  A U-shaped gate 160 is provided at the center of the installation table 156 so as to straddle the movement path of the stage 152. Each of the end portions of the U-shaped gate 160 is fixed to both side surfaces of the installation table 156. A scanner 162 is provided on one side of the gate 160, and a plurality of (for example, two) sensors 164 for detecting the front and rear ends of the photosensitive material 150 are provided on the other side. The scanner 162 and the sensor 164 are respectively attached to the gate 160 and fixedly arranged above the moving path of the stage 152. The scanner 162 and the sensor 164 are connected to a controller (not shown) that controls them.

As shown in FIGS. 2 and 3B, the scanner 162 includes a plurality of (for example, 14) exposure heads 166 arranged in an approximately matrix of m rows and n columns (for example, 3 rows and 5 columns). . In this example, four exposure heads 166 are arranged in the third row in relation to the width of the photosensitive material 150. In addition, when showing each exposure head arranged in the mth row and the nth column, it is expressed as an exposure head 166 _mn .

An exposure area 168 by the exposure head 166 has a rectangular shape with the short side in the sub-scanning direction. Therefore, as the stage 152 moves, a strip-shaped exposed area 170 is formed on the photosensitive material 150 for each exposure head 166. In addition, when showing the exposure area by each exposure head arranged in the m-th row and the n-th column, it is expressed as an exposure area 168 _mn .

Further, as shown in FIGS. 3A and 3B, each of the exposure heads in each row arranged in a line so that the strip-shaped exposed regions 170 are arranged in the direction orthogonal to the sub-scanning direction without gaps. These are arranged with a predetermined interval (natural number times the long side of the exposure area, twice in this example) in the arrangement direction. Therefore, can not be exposed portion between the exposure area 168 ₁₁ in the first row and the exposure area 168 _12, it can be exposed by the second row of the exposure area 168 ₂₁ and the exposure area 168 ₃₁ in the third row.

As shown in FIGS. 4 and 5, each of the exposure heads 166 _{11 to} 166 _mn is manufactured by Texas Instruments, Inc. as a spatial light modulation element that modulates an incident light beam for each pixel according to image data. Digital micromirror device (DMD) 50. The DMD 50 is connected to a controller 302 (see FIG. 15), which will be described later, provided with a data processing unit and a mirror drive control unit. The data processing unit of the controller 302 generates a control signal for driving and controlling each micromirror in the region to be controlled by the DMD 50 for each exposure head 166 based on the input image data. The area to be controlled will be described later. The mirror drive control unit controls the angle of the reflection surface of each micromirror of the DMD 50 for each exposure head 166 based on the control signal generated by the image data processing unit. The control of the angle of the reflecting surface will be described later.

  On the light incident side of the DMD 50, a fiber array light source 66 including a laser emitting portion in which an emitting end portion (light emitting point) of an optical fiber is arranged in a line along a direction corresponding to the long side direction of the exposure area 168, a fiber A lens system 67 that corrects the laser light emitted from the array light source 66 and collects it on the DMD, and a mirror 69 that reflects the laser light transmitted through the lens system 67 toward the DMD 50 are arranged in this order. In FIG. 4, the lens system 67 is schematically shown.

  As shown in detail in FIG. 5, the lens system 67 includes a condenser lens 71 that condenses the laser light B as illumination light emitted from the fiber array light source 66, and is inserted into the optical path of the light that has passed through the condenser lens 71. The rod-shaped optical integrator 72 (hereinafter referred to as a rod integrator) 72 and an imaging lens 74 disposed in front of the rod integrator 72, that is, on the mirror 69 side. The condenser lens 71, the rod integrator 72, and the imaging lens 74 cause the laser light emitted from the fiber array light source 66 to enter the DMD 50 as a light beam that is close to parallel light and has a uniform beam cross-sectional intensity. The shape and action of this rod integrator 72 will be described in detail later.

  The laser beam B emitted from the lens system 67 is reflected by a mirror 69 and irradiated to the DMD 50 via a TIR (total reflection) prism 70. In FIG. 4, the TIR prism 70 is omitted.

  On the light reflection side of the DMD 50, an imaging optical system 51 that images the laser light B reflected by the DMD 50 on the photosensitive material 150 is disposed. The imaging optical system 51 is schematically shown in FIG. 4, but as shown in detail in FIG. 5, a first imaging optical system comprising lens systems 52 and 54 and a first imaging system comprising lens systems 57 and 58 are shown. The image forming optical system includes two image forming optical systems, a microlens array 55 inserted between these image forming optical systems, and an aperture array 59.

  The microlens array 55 is formed by two-dimensionally arranging a number of microlenses 55a corresponding to each pixel of the DMD 50. In this example, as will be described later, only 1024 × 256 rows of the 1024 × 768 rows of micromirrors of DMD 50 are driven, and accordingly, 1024 × 256 rows of microlenses 55a are arranged. The arrangement pitch of the micro lenses 55a is 41 μm in both the vertical and horizontal directions. As an example, the micro lens 55a has a focal length of 0.19 mm, an NA (numerical aperture) of 0.11, and is formed of the optical glass BK7. The shape of the micro lens 55a will be described in detail later. The beam diameter of the laser beam B at the position of each micro lens 55a is 41 μm.

  The aperture array 59 is formed by forming a large number of apertures (openings) 59a corresponding to the respective microlenses 55a of the microlens array 55. In the present embodiment, the diameter of the aperture 59a is 10 μm.

  The first image-forming optical system forms an image on the microlens array 55 by enlarging the image by the DMD 50 three times. The second imaging optical system enlarges the image passing through the microlens array 55 by 1.6 times, and forms and projects the image on the photosensitive material 150. Therefore, as a whole, the image formed by the DMD 50 is enlarged and enlarged by 4.8 times on the photosensitive material 150 and projected.

  In this example, a prism pair 73 is disposed between the second imaging optical system and the photosensitive material 150, and the prism pair 73 is moved in the vertical direction in FIG. The focus can be adjusted. In the figure, the photosensitive material 150 is sub-scanned in the direction of arrow F.

  As shown in FIG. 6, in the DMD 50, a large number (for example, 1024 × 768) of micromirrors (micromirrors) 62 constituting pixels (pixels) are arranged on a SRAM cell (memory cell) 60 in a lattice pattern. This is a mirror device. In each pixel, a micromirror 62 supported by a support column is provided at the top, and a material having high reflectivity such as aluminum is deposited on the surface of the micromirror 62. The reflectance of the micromirror 62 is 90% or more, and the arrangement pitch is 13.7 μm as an example in both the vertical and horizontal directions. Directly below the micromirror 62, a silicon gate CMOS SRAM cell 60 manufactured on a normal semiconductor memory manufacturing line is disposed via a support including a hinge and a yoke, and the entire structure is monolithic. ing.

  When a digital signal is written to the SRAM cell 60 of the DMD 50, the micromirror 62 supported by the support is tilted within a range of ± α degrees (eg, ± 12 degrees) with respect to the substrate side on which the DMD 50 is disposed with the diagonal line as the center. It is done. 7A shows a state where the micromirror 62 is tilted to + α degrees when the micromirror 62 is in the on state, and FIG. 7B shows a state where the micromirror 62 is tilted to −α degrees when the micromirror 62 is in the off state. Therefore, by controlling the tilt of the micromirror 62 in each pixel of the DMD 50 according to the image signal as shown in FIG. 6, the laser light B incident on the DMD 50 is reflected in the tilt direction of each micromirror 62. The

  FIG. 6 shows an example of a state in which a part of the DMD 50 is enlarged and the micromirror 62 is controlled to + α degrees or −α degrees. The on / off control of each micromirror 62 is performed by the controller 302 connected to the DMD 50. Further, a light absorber (not shown) is arranged in the direction in which the laser beam B reflected by the micromirror 62 in the off state travels.

  Further, it is preferable that the DMD 50 is disposed with a slight inclination so that the short side forms a predetermined angle θ (for example, 0.1 ° to 5 °) with the sub-scanning direction. 8A shows the scanning trajectory of the reflected light image (exposure beam) 53 by each micromirror when the DMD 50 is not tilted, and FIG. 8B shows the scanning trajectory of the exposure beam 53 when the DMD 50 is tilted. Show.

In the DMD 50, a number of micromirror arrays in which a large number (for example, 1024) of micromirrors are arranged in the longitudinal direction are arranged in a short direction (for example, 756 sets). As shown in FIG. Further, by tilting the DMD 50, the pitch P ₁ of the scanning trajectory (scan line) of the exposure beam 53 by each micromirror becomes narrower than the pitch P ₂ of the scanning line when the DMD 50 is not tilted, and the resolution is greatly improved. Can be made. On the other hand, since the inclination angle of the DMD 50 is very small, the scanning width W ₂ when the DMD 50 is inclined and the scanning width W ₁ when the DMD 50 is not inclined are substantially the same.

  Further, the same scanning line is overlapped and exposed (multiple exposure) by different micromirror rows. Thus, by performing multiple exposure, it is possible to control a minute amount of the exposure position with respect to the alignment mark, and to realize high-definition exposure. Further, joints between a plurality of exposure heads arranged in the main scanning direction can be connected without a step by controlling a very small amount of exposure position.

  Note that the same effect can be obtained by arranging the micromirror rows in a staggered manner by shifting the micromirror rows by a predetermined interval in the direction orthogonal to the sub-scanning direction instead of inclining the DMD 50.

  As shown in FIG. 9 a, the fiber array light source 66 includes a plurality of (for example, 14) laser modules 64, and one end of a multimode optical fiber 30 is coupled to each laser module 64. The other end of the multimode optical fiber 30 is coupled with an optical fiber 31 having the same core diameter as the multimode optical fiber 30 and a cladding diameter smaller than the multimode optical fiber 30. As shown in detail in FIG. 9b, seven end portions of the multi-mode optical fiber 31 opposite to the optical fiber 30 are arranged along the main scanning direction orthogonal to the sub-scanning direction, and are arranged in two rows to form a laser. An emission unit 68 is configured.

  As shown in FIG. 9B, the laser emitting portion 68 constituted by the end portion of the multimode optical fiber 31 is sandwiched and fixed between two support plates 65 having a flat surface. Further, it is desirable that a transparent protective plate such as glass is disposed on the light emitting end face of the multimode optical fiber 31 for protection. The light exit end face of the multimode optical fiber 31 is easily collected and easily deteriorated due to its high light density.However, the protective plate as described above prevents the dust from adhering to the end face. Can be delayed.

  In this example, as shown in FIG. 10, an optical fiber 31 having a small cladding diameter of about 1 to 30 cm is coaxially coupled to a tip portion on the laser light emission side of a multimode optical fiber 30 having a large cladding diameter. Yes. The optical fibers 30 and 31 are coupled by fusing the incident end face of the optical fiber 31 to the outgoing end face of the optical fiber 30 in a state where the respective core axes coincide. As described above, the diameter of the core 31a of the optical fiber 31 is the same as the diameter of the core 30a of the multimode optical fiber 30.

  As the multimode optical fiber 30 and the optical fiber 31, any of a step index type optical fiber, a graded index type optical fiber, and a composite type optical fiber can be applied. For example, a step index type optical fiber manufactured by Mitsubishi Cable Industries, Ltd. can be used. In this example, the multimode optical fiber 30 and the optical fiber 31 are step index type optical fibers. The multimode optical fiber 30 has a cladding diameter = 125 μm, a core diameter = 50 μm, NA = 0.2, and transmission of the incident end face coating. The ratio is 99.5% or more, and the optical fiber 31 has a cladding diameter = 60 μm, a core diameter = 50 μm, and NA = 0.2.

  However, the cladding diameter of the optical fiber 31 is not limited to 60 μm. The clad diameter of many optical fibers used in conventional fiber light sources is 125 μm. However, the smaller the clad diameter, the deeper the depth of focus. Therefore, the clad diameter of the multimode optical fiber is preferably 80 μm or less, preferably 60 μm or less. Is more preferable. On the other hand, in the case of a single mode optical fiber, the core diameter needs to be at least 3 to 4 μm, and therefore the cladding diameter of the optical fiber 31 is preferably 10 μm or more. Further, it is preferable from the viewpoint of coupling efficiency that the core diameter of the optical fiber 30 and the core diameter of the optical fiber 31 are matched.

  The laser module 64 is configured by a combined laser light source (fiber light source) shown in FIG. The combined laser light source includes a plurality of (for example, seven) chip-like lateral multimode or single mode GaN-based semiconductor lasers LD1, LD2, LD3, LD4, LD5, LD6, and the like arranged and fixed on the heat block 10. LD 7, collimator lenses 11, 12, 13, 14, 15, 16, and 17 provided corresponding to each of GaN-based semiconductor lasers LD 1 to LD 7, one condenser lens 20, and one multimode light And fiber 30. The number of semiconductor lasers is not limited to seven, and other numbers may be adopted. Further, instead of the seven collimator lenses 11 to 17 as described above, a collimator lens array in which these lenses are integrated can be used.

  The GaN-based semiconductor lasers LD1 to LD7 all have a common oscillation wavelength (for example, 405 nm), and the maximum output is also all common (for example, about 100 mW for a multimode laser and about 50 mW for a single mode laser). As the GaN-based semiconductor lasers LD1 to LD7, lasers that oscillate at wavelengths other than 405 nm in the wavelength range of 350 nm to 450 nm may be used.

  As shown in FIGS. 12 and 13, the above combined laser light source is housed in a box-shaped package 40 having an upper opening together with other optical elements. The package 40 includes a package lid 41 created so as to close the opening, and is formed by introducing a sealing gas after the deaeration process and closing the opening of the package 40 with the package lid 41. The combined laser light source is hermetically sealed in a closed space (sealed space).

  A base plate 42 is fixed to the bottom surface of the package 40. On the top surface of the base plate 42, the heat block 10, a condensing lens holder 45 for holding the condensing lens 20, and a multimode optical fiber 30 are provided. A fiber holder 46 that holds the incident end is attached. The exit end of the multimode optical fiber 30 is drawn out of the package through an opening formed in the wall surface of the package 40.

  A collimator lens holder 44 is attached to the side surface of the heat block 10, and the collimator lenses 11 to 17 are held there. An opening is formed in the lateral wall surface of the package 40, and wiring 47 for supplying a driving current to the GaN-based semiconductor lasers LD1 to LD7 is drawn out of the package through the opening.

  In FIG. 13, in order to avoid complication of the drawing, only the GaN semiconductor laser LD7 is numbered among the plurality of GaN semiconductor lasers, and only the collimator lens 17 is numbered among the plurality of collimator lenses. is doing.

  FIG. 14 shows the front shape of the attachment part of the collimator lenses 11-17. Each of the collimator lenses 11 to 17 is formed in a shape in which a region including the optical axis of a circular lens having an aspherical surface is cut out in a parallel plane. This elongated collimator lens can be formed, for example, by molding resin or optical glass. The collimator lenses 11 to 17 are closely arranged in the arrangement direction of the light emitting points so that the length direction is orthogonal to the arrangement direction of the light emitting points of the GaN-based semiconductor lasers LD1 to LD7 (left and right direction in FIG. 14).

  On the other hand, each of the GaN-based semiconductor lasers LD1 to LD7 includes an active layer having a light emission width of 2 μm, and the laser beams B1 to A laser emitting B7 is used. These GaN-based semiconductor lasers LD1 to LD7 are arranged so that the light emitting points are arranged in a line in a direction parallel to the active layer.

Accordingly, in the laser beams B1 to B7 emitted from the respective light emitting points, the direction in which the divergence angle is large coincides with the length direction and the divergence angle is small with respect to the elongated collimator lenses 11 to 17 as described above. Incident light is incident in a state where the direction coincides with the width direction (direction perpendicular to the length direction). That is, the collimator lenses 11 to 17 have a width of 1.1 mm and a length of 4.6 mm, and the horizontal and vertical beam diameters of the laser beams B1 to B7 incident thereon are 0.9 mm and 2. 6 mm. Each of the collimator lenses 11 to 17 has a focal length f ₁ = 3 mm, NA = 0.6, and a lens arrangement pitch = 1.25 mm.

The condensing lens 20 is formed by cutting a region including the optical axis of a circular lens having an aspheric surface into a long and narrow shape in parallel planes, and is long in the arrangement direction of the collimator lenses 11 to 17, that is, in the horizontal direction and short in the direction perpendicular thereto Is formed. The condenser lens 20 has a focal length f ₂ = 23 mm and NA = 0.2. The condensing lens 20 is also formed by molding resin or optical glass, for example.

  Next, the electrical configuration of the image exposure apparatus of this example will be described with reference to FIG. As shown here, a modulation circuit 301 is connected to the overall control unit 300, and a controller 302 for controlling the DMD 50 is connected to the modulation circuit 301. The overall control unit 300 is connected to an LD drive circuit 303 that drives the laser module 64. Further, a stage driving device 304 that drives the stage 152 is connected to the overall control unit 300.

[Operation of image exposure apparatus]
Next, the operation of the image exposure apparatus will be described. In each exposure head 166 of the scanner 162, laser light B1, B2, B3 emitted in a divergent light state from each of the GaN-based semiconductor lasers LD1 to LD7 (see FIG. 11) constituting the combined laser light source of the fiber array light source 66. Each of B4, B5, B6, and B7 is collimated by the corresponding collimator lenses 11-17. The collimated laser beams B <b> 1 to B <b> 7 are collected by the condenser lens 20 and converge on the incident end face of the core 30 a of the multimode optical fiber 30.

  In this example, the collimator lenses 11 to 17 and the condenser lens 20 constitute a condensing optical system, and the condensing optical system and the multimode optical fiber 30 constitute a multiplexing optical system. That is, the laser beams B1 to B7 collected as described above by the condenser lens 20 enter the core 30a of the multimode optical fiber 30, propagate through the optical fiber, and merge with one laser beam B. The light is emitted from the optical fiber 31 coupled to the output end of the multimode optical fiber 30.

  In each laser module, when the coupling efficiency of the laser beams B1 to B7 to the multimode optical fiber 30 is 0.9 and each output of the GaN-based semiconductor lasers LD1 to LD7 is 50 mW, the light arranged in an array For each of the fibers 31, a combined laser beam B having an output of 315 mW (= 50 mW × 0.9 × 7) can be obtained. Therefore, the entire 14 multi-mode optical fibers 31 can provide a laser beam B with an output of 4.4 W (= 0.315 W × 14).

  At the time of image exposure, image data corresponding to the exposure pattern is input from the modulation circuit 301 shown in FIG. 15 to the controller 302 of the DMD 50 and temporarily stored in the frame memory. This image data is data representing the density of each pixel constituting the image by binary values (whether or not dots are recorded).

  The stage 152 having the photosensitive material 150 adsorbed on the surface is moved at a constant speed from the upstream side to the downstream side of the gate 160 along the guide 158 by the stage driving device 304 shown in FIG. When the leading edge of the photosensitive material 150 is detected by the sensor 164 attached to the gate 160 when the stage 152 passes under the gate 160, the image data stored in the frame memory is sequentially read out for each of a plurality of lines. A control signal is generated for each exposure head 166 based on the image data read by the data processing unit. Then, each of the micromirrors of the DMD 50 is controlled on and off for each exposure head 166 based on the generated control signal by the mirror drive control unit. In the case of this example, the size of the micromirror serving as one pixel portion is 14 μm × 14 μm.

  When the DMD 50 is irradiated with the laser beam B from the fiber array light source 66, the laser beam reflected when the micromirror of the DMD 50 is in an on state is imaged on the photosensitive material 150 by the lens systems 54 and 58. In this manner, the laser light emitted from the fiber array light source 66 is turned on and off for each pixel, and the photosensitive material 150 is exposed in a pixel unit (exposure area 168) that is approximately the same number as the number of used pixels of the DMD 50. Further, when the photosensitive material 150 is moved at a constant speed together with the stage 152, the photosensitive material 150 is sub-scanned in the direction opposite to the stage moving direction by the scanner 162, and a strip-shaped exposed region 170 is formed for each exposure head 166. It is formed.

  In this example, as shown in FIGS. 16A and 16B, the DMD 50 has 768 pairs of micromirror arrays in which 1024 micromirrors are arranged in the main scanning direction. In this example, the controller 302 performs control so that only a part of micromirror rows (eg, 1024 × 256 rows) are driven.

  In this case, a micromirror array arranged at the center of the DMD 50 as shown in FIG. 16A may be used, and the micromirror arranged at the end of the DMD 50 as shown in FIG. A column may be used. In addition, when a defect occurs in some of the micromirrors, the micromirror array to be used may be appropriately changed depending on the situation, such as using a micromirror array in which no defect has occurred.

  Since the data processing speed of the DMD 50 is limited and the modulation speed per line is determined in proportion to the number of pixels used, the modulation speed per line can be increased by using only a part of the micromirror rows. Get faster. On the other hand, in the case of an exposure method in which the exposure head is continuously moved relative to the exposure surface, it is not necessary to use all the pixels in the sub-scanning direction.

  When the sub-scanning of the photosensitive material 150 by the scanner 162 is completed and the rear end of the photosensitive material 150 is detected by the sensor 164, the stage 152 is moved to the most upstream side of the gate 160 along the guide 158 by the stage driving device 304. It returns to a certain origin and is moved again along the guide 158 from the upstream side to the downstream side of the gate 160 at a constant speed.

  Next, the illumination comprising the fiber array light source 66, the condensing lens 71, the rod integrator 72, the imaging lens 74, the mirror 69 and the TIR prism 70 shown in FIG. 5 and irradiating the DMD 50 with the laser light B as the illumination light. The optical system will be described. The rod integrator 72 is a translucent rod formed in, for example, a rectangular column shape, and the intensity distribution in the beam cross section of the laser beam B is made uniform while the laser beam B travels while totally reflecting inside the rod integrator 72. The entrance end face and exit end face of the rod integrator 72 are coated with an antireflection film to increase the transmittance. As described above, if the intensity distribution in the beam cross section of the laser beam B as illumination light can be made highly uniform, non-uniform illumination light intensity can be eliminated and a high-definition image can be exposed on the photosensitive material 150.

  FIG. 17 shows the result of measuring the flatness of the reflecting surface of the micromirror 62 constituting the DMD 50. In the figure, the same height positions of the reflecting surfaces are shown connected by contour lines, and the pitch of the contour lines is 5 nm. Note that the x direction and the y direction shown in the figure are two diagonal directions of the micromirror 62, and the micromirror 62 rotates around the rotation axis extending in the y direction as described above. 18A and 18B show the height position displacement of the reflecting surface of the micromirror 62 along the x direction and the y direction, respectively.

  As shown in FIGS. 17 and 18, there is distortion on the reflection surface of the micromirror 62, and when attention is paid particularly to the center of the mirror, distortion in one diagonal direction (y direction) It is larger than the distortion in the diagonal direction (x direction). Therefore, there may be a problem that the shape of the laser beam B collected by the microlens 55a of the microlens array 55 is distorted.

  In the image exposure apparatus of the present embodiment, the microlens 55a of the microlens array 55 has a special shape different from the conventional one in order to prevent the above-described problem. Hereinafter, this point will be described in detail.

  FIGS. 19A and 19B respectively show the front and side shapes of the entire microlens array 55 in detail. These drawings also show the dimensions of each part of the microlens array 55, and the unit thereof is mm. In this embodiment, as described above with reference to FIG. 16, the 1024 × 256 micromirrors 62 of the DMD 50 are driven. Correspondingly, the microlens array 55 is 1024 in the lateral direction. The microlenses 55a arranged in parallel are arranged in 256 rows in the vertical direction. In FIG. 9A, the arrangement order of the microlens array 55 is indicated by j in the horizontal direction and k in the vertical direction.

  20A and 20B show the front shape and the side shape of one microlens 55a in the microlens array 55, respectively. In FIG. 9A, the contour lines of the micro lens 55a are also shown. The end surface of each microlens 55a on the light emission side has an aspherical shape that corrects the aberration caused by the distortion of the reflection surface of the micromirror 62 described above. More specifically, in the present embodiment, the microlens 55a is a toric lens, and has a radius of curvature Rx = −0.125 mm in a direction optically corresponding to the x direction and a radius of curvature in a direction corresponding to the y direction. Ry = −0.1 mm.

  Therefore, the condensing state of the laser beam B in the cross section parallel to the x direction and the y direction is roughly as shown in FIGS. 21A and 21B, respectively. That is, comparing the cross section parallel to the x direction and the cross section parallel to the y direction, the radius of curvature of the microlens 55a is smaller and the focal length is shorter in the latter cross section. .

  FIGS. 22A, 22B, 22C, and 22D show the results of simulating the beam diameter in the vicinity of the condensing position (focal position) of the microlens 55a when the microlens 55a has the above shape by a computer. For comparison, FIGS. 23A, 23B, 23C, and 23D show the same simulation results for the case where the microlens 55a has a spherical shape with a radius of curvature Rx = Ry = −0.1 mm. Note that the value of z in each figure indicates the evaluation position in the focus direction of the micro lens 55a by the distance from the beam exit surface of the micro lens 55a.

The surface shape of the microlens 55a used in the simulation is

It is. In the above equation, Cx: curvature in the x direction (= 1 / Rx), Cy: curvature in the y direction (= 1 / Ry), X: distance from the lens optical axis O in the x direction, Y: lens in the y direction. The distance from the optical axis O.

  22A to 22D and FIGS. 23A to 23D, in the present embodiment, the microlens 55a has a focal length in a cross section parallel to the y direction that is greater than a focal length in a cross section parallel to the x direction. Since the toric lens is also small, distortion of the beam shape in the vicinity of the condensing position is suppressed. If so, the photosensitive material 150 can be exposed to a higher-definition image without distortion. It can also be seen that the present embodiment shown in FIGS. 22a to 22d has a wider region with a smaller beam diameter, that is, a greater depth of focus.

  In the case where the magnitude relationship between the strains at the center of the micromirror 62 in the x direction and the y direction is opposite to the above, the focal length in the cross section parallel to the x direction is within the cross section parallel to the y direction. If the microlens is composed of a toric lens smaller than the focal length, similarly, a higher-definition image without distortion can be exposed on the photosensitive material 150.

  In addition, the aperture array 59 disposed in the vicinity of the light collection position of the microlens array 55 is disposed such that only light having passed through the corresponding microlens 55a is incident on each aperture 59a. That is, by providing this aperture array 59, it is possible to prevent light from adjacent microlenses 55a not corresponding to each aperture 59a from entering, and to increase the extinction ratio. The aperture array 59 is preferably arranged at the focal position of the microlens array 55. By doing so, it is possible to more reliably prevent light from the adjacent microlens 55a not corresponding to each aperture 59a from entering.

  Originally, if the diameter of the aperture 59a of the aperture array 59 installed for the above purpose is reduced to some extent, an effect of suppressing the distortion of the beam shape at the condensing position of the microlens 55a can be obtained. However, in such a case, the amount of light blocked by the aperture array 59 is increased, and the light use efficiency is reduced. On the other hand, when the microlens 55a has an aspherical shape, the light utilization efficiency is kept high because the light is not blocked.

  In the present embodiment, the microlens 55a which is a toric lens having different curvatures in the x and y directions optically corresponding to the two diagonal directions of the micromirror 62 is applied. Accordingly, the curvatures in the xx and yy directions optically corresponding to the two side directions of the rectangular micromirror 62 are shown in FIGS. A micro lens 55a ′ made of different toric lenses may be applied.

  In this embodiment, the microlens 55a has a secondary aspherical shape. However, by adopting a higher order (4th, 6th,...) Aspherical shape, the beam shape can be further improved. Can be Furthermore, it is possible to adopt a lens shape in which the curvatures in the x direction and the y direction described above coincide with each other in accordance with the distortion of the reflection surface of the micromirror 62. Hereinafter, examples of such lens shapes will be described in detail.

27A and 27B, the microlens 55a ″ showing a front shape and a side shape with contour lines, respectively, has the same curvature in the x direction and the y direction, and the curvature is the same as the curvature Cy of the spherical lens. This is corrected according to the distance h from the center. That is, the spherical lens shape that is the basis of the lens shape of the microlens 55a ″ is, for example, the lens height (the surface of the lens curved surface) by the following equation (Equation 2). An optical axis direction position) z is used.

  FIG. 28 is a graph showing the relationship between the lens height z and the distance h when the curvature Cy = (1 / 0.1 mm).

Then, the curvature Cy of the spherical lens shape is corrected as shown in the following equation (Equation 3) according to the distance h from the lens center to obtain the lens shape of the microlens 55a ″.

In this (Equation 3), the meaning of z is the same as that in (Equation 2). Here, the curvature Cy is corrected using the fourth-order coefficient a and the sixth-order coefficient b. The lens height z and the distance h when the curvature Cy = (1 / 0.1 mm), the fourth-order coefficient a = 1.2 × 10 ³ , and the sixth-order coefficient a = 5.5 × 10 ⁷ are given. The relationship is shown in a graph in FIG.

  In the embodiment described above, the end surface on the light emission side of the micro lens 55a is an aspheric surface (toric surface). However, one of the two light passing end surfaces is a spherical surface and the other is a cylindrical surface. Thus, the microlens array can be configured to obtain the same effect as the above embodiment.

  Further, in the embodiment described above, the microlens 55a of the microlens array 55 has an aspherical shape that corrects aberration due to distortion of the reflecting surface of the micromirror 62. Such an aspherical shape is adopted. Instead, the same effect can be obtained even if each microlens constituting the microlens array has a refractive index distribution that corrects aberration due to distortion of the reflection surface of the micromirror 62.

  An example of such a microlens 155a is shown in FIG. (A) and (B) of the same figure respectively show the front shape and the side shape of the micro lens 155a, and the outer shape of the micro lens 155a is a parallel plate shape as shown in the figure. The x and y directions in the figure are as described above.

  25A and 25B schematically show the condensing state of the laser beam B in the cross section parallel to the x direction and the y direction by the micro lens 155a. The microlens 155a has a refractive index distribution that gradually increases outward from the optical axis O, and the broken line shown in the microlens 155a in FIG. The position changed with the pitch is shown. As shown in the drawing, when the cross section parallel to the x direction and the cross section parallel to the y direction are compared, the ratio of the refractive index change of the microlens 155a is larger in the latter cross section, and the focal length is larger. It is shorter. Even when a microlens array composed of such a gradient index lens is used, it is possible to obtain the same effect as when the microlens array 55 is used.

  In addition, in the microlens whose surface shape is aspherical like the microlens 55a previously shown in FIG. 20 and FIG. 21, a refractive index distribution as described above is given together, and both by the surface shape and the refractive index distribution. The aberration due to the distortion of the reflection surface of the micromirror 62 may be corrected.

  Next, an image exposure apparatus according to still another embodiment of the present invention will be described. Compared with the image exposure apparatus described above with reference to FIGS. 1 to 15, the image exposure apparatus of this embodiment uses a microlens array 255 shown in FIG. 30 instead of the microlens array 55 shown in FIG. 5. However, the other points are basically formed in the same manner. Hereinafter, the microlens array 255 will be described in detail.

  As described above with reference to FIGS. 17 and 18, there is distortion on the reflection surface of the micromirror 62 of the DMD 50, but the amount of change in the distortion gradually increases from the center of the micromirror 62 to the periphery. Has a trend. The amount of change in the peripheral portion distortion in one diagonal direction (y direction) of the micromirror 62 is larger than the amount of change in the peripheral portion distortion in another diagonal direction (x direction), and the above-described tendency is more remarkable. .

  The image exposure apparatus of the present embodiment is one in which a microlens array 255 shown in FIG. 30 is applied in order to cope with the above problem. In the microlens array 255, microlenses 255a arranged in an array have a circular lens opening. Therefore, as described above, the laser beam B reflected at the peripheral portion of the reflecting surface of the micromirror 62 having a large distortion, particularly at the four corners, is not collected by the microlens 255a, and the condensed laser beam B is collected at the condensing position. It is possible to prevent the shape from being distorted. If so, the photosensitive material 150 can be exposed to a higher-definition image without distortion.

  In the present embodiment, as shown in the figure, the back surface of the transparent member 255b (which is usually formed integrally with the microlens 255a) holding the microlens 255a of the microlens array 255, that is, A light-shielding mask 255c is formed on the surface opposite to the surface on which the microlenses 255a are formed so as to fill the outer regions of the lens openings of the plurality of microlenses 255a that are separated from each other. By providing such a mask 255c, the laser beam B reflected at the periphery of the reflecting surface of the micromirror 62, particularly at the four corners, is absorbed and blocked there, so that the shape of the focused laser beam B is Is more reliably prevented from being distorted.

  In the present invention, the opening shape of the microlens is not limited to the circular shape described above. For example, as shown in FIG. 31, a microlens array 455 formed by arranging a plurality of microlenses 455a having elliptical openings. As shown in FIG. 32, a microlens array 555 or the like in which a plurality of microlenses 555a having polygonal (here, quadrangular) openings are arranged in parallel can also be applied. The microlenses 455a and 555a are formed by cutting out a part of a normal axisymmetric spherical lens into a circular shape or a polygonal shape, and have the same light collecting function as that of a normal axisymmetric spherical lens.

  Further, in the present invention, a microlens array as shown in FIGS. 33A, 33B, and 33C can be applied. In the microlens array 655 shown in FIG. 6A, a plurality of microlenses 655a similar to the microlenses 55a, 455a, and 555a are in close contact with the surface of the transparent member 655b on the side where the laser beam B is emitted. A mask 655c similar to the mask 255c is formed on the side where the laser beam B is incident side by side. Note that the mask 255c in FIG. 30 is formed in the outer portion of the lens opening, whereas the mask 655c is provided in the lens opening. In the microlens array 755 shown in FIG. 2B, a plurality of microlenses 755a are arranged in parallel on the surface of the transparent member 755b on the side where the laser beam B is emitted, and the microlens 755a is arranged between the microlenses 755a. And a mask 755c is formed. In the microlens array 855 shown in FIG. 6C, a plurality of microlenses 855a are arranged in parallel with each other on the surface of the transparent member 855b on the side where the laser beam B is emitted, and the periphery of each microlens 855a is arranged. A mask 855c is formed on the part.

  Note that the masks 655c, 755c, and 855c all have circular openings like the above-described mask 255c, whereby the opening of the microlens is defined to be circular.

  As in the microlenses 255a, 455a, 555a, 655a, and 755a described above, a configuration in which a lens opening shape that does not allow light from the periphery of the micromirror 62 of the DMD 50 to enter is provided by providing a mask or the like. An aspherical lens that corrects aberration due to distortion of the surface of the micromirror 62 as in the lens 55a (see FIG. 20), or a refractive index distribution that corrects the aberration as in the microlens 155a (see FIG. 24). It can also be used in combination with a lens. By doing so, the effect of preventing the distortion of the exposure image due to the distortion of the reflection surface of the micromirror 62 is synergistically enhanced.

  In particular, in the configuration in which the mask 855c is formed on the lens surface of the microlens 855a as shown in FIG. 33C, the microlens 855a has the above-described aspherical shape and refractive index distribution. In the case where the imaging position of the first imaging optical system (for example, the lens systems 52 and 54 shown in FIG. 5) is set on the lens surface of the microlens 855a, the light utilization efficiency is particularly high and higher. The photosensitive material 150 can be exposed with intense light. That is, in this case, the first imaging optical system refracts the light so that stray light due to distortion of the reflection surface of the micromirror 62 is focused at one point at the imaging position of the optical system. If it is formed, light other than stray light will not be blocked, and light utilization efficiency will be improved.

  In the above-described embodiment, a laser light source is used as a light source for irradiating light to the spatial light modulation element. However, the present invention is not limited to this, and a lamp light source such as a mercury lamp can also be used.

  In the above embodiment, the aberration due to the distortion of the reflection surface of the micromirror 62 constituting the DMD 50 is corrected. However, even in an image exposure apparatus using a spatial light modulation element other than the DMD, the pixel of the spatial light modulation element is used. When there is distortion on the surface of the part, it is possible to apply the present invention to correct the aberration due to the distortion and to prevent the beam shape from being distorted.

The perspective view which shows the external appearance of the image exposure apparatus which is one Embodiment of this invention 1 is a perspective view showing a configuration of a scanner of the image exposure apparatus in FIG. (A) is a plan view showing an exposed area formed on a photosensitive material, and (B) is a view showing an arrangement of exposure areas by each exposure head. 1 is a perspective view showing a schematic configuration of an exposure head of the image exposure apparatus of FIG. Cross section of the above exposure head Partial enlarged view showing the configuration of a digital micromirror device (DMD) (A) And (B) is explanatory drawing for demonstrating operation | movement of DMD. (A) and (B) are plan views showing the arrangement of the exposure beam and the scanning line in a case where the DMD is not inclined and in a case where the DMD is inclined. The perspective view which shows the structure of a fiber array light source Front view showing arrangement of light emitting points in laser emitting section of fiber array light source Diagram showing the configuration of a multimode optical fiber Plan view showing the configuration of the combined laser light source Plan view showing the configuration of the laser module Side view showing the configuration of the laser module shown in FIG. The partial front view which shows the structure of the laser module shown in FIG. Block diagram showing the electrical configuration of the image exposure apparatus (A) And (B) is a figure which shows the example of the use area | region of DMD. The figure which shows the distortion of the reflective surface of the micromirror which comprises DMD with a contour line The graph which shows distortion of the reflective surface of the said micromirror about two diagonal directions of this mirror Front view (A) and side view (B) of the microlens array used in the image exposure apparatus Front view (A) and side view (B) of the microlens constituting the microlens array Schematic showing the condensing state by the micro lens in one cross section (A) and another cross section (B) The figure which shows the result of having simulated the beam diameter in the condensing position vicinity of a micro lens in the image exposure apparatus of this invention. The figure which shows the simulation result similar to FIG. 22a about another position The figure which shows the simulation result similar to FIG. 22a about another position The figure which shows the simulation result similar to FIG. 22a about another position The figure which shows the result of having simulated the beam diameter in the condensing position vicinity of a micro lens in the conventional image exposure apparatus. The figure which shows the simulation result similar to FIG. 23a about another position The figure which shows the simulation result similar to FIG. 23a about another position The figure which shows the simulation result similar to FIG. 23a about another position The front view (A) and side view (B) of the microlens which comprise the microlens array used for another image exposure apparatus of this invention FIG. 24 is a schematic view showing a light collection state by the microlens of FIG. 24 in one cross section (A) and another cross section (B). Front view (A) and side view (B) showing still another example of a microlens Front view (A) and side view (B) showing still another example of a microlens Graph showing examples of spherical lens shapes The graph which shows another lens surface shape example of the micro lens used for this invention A perspective view showing another example of a microlens array The top view which shows another example of a micro lens array The top view which shows another example of a micro lens array The top view which shows another example of a micro lens array

Explanation of symbols

LD1-LD7 GaN semiconductor laser
30, 31 Multimode optical fiber
50 Digital micromirror device (DMD)
51 Magnification optical system
53, 54 Lens of the first imaging optical system
55, 255, 455, 555, 655, 755, 855 Micro lens array
55a, 55a ', 55a ", 155a, 255a, 455a, 555a, 655a, 755a, 855a Microlens
57, 58 Second imaging optical system lens
59 Aperture array
66 Laser module
66 Fiber array light source
68 Laser emission part
72 Rod integrator
150 photosensitive material
152 stages
162 Scanner
166 Exposure head
168 Exposure area
170 Exposed area

Claims (11)

A spatial light modulation element in which a large number of pixel portions each modulating the irradiated light are two-dimensionally arranged;
A light source for irradiating light to the spatial light modulator;
Including a microlens array in which microlenses for condensing light from each pixel portion of the spatial light modulator are arranged in an array, and an image formed by the light modulated by the spatial light modulator is formed on a photosensitive material. In an image exposure apparatus comprising an imaging optical system for forming an image,
An image exposure apparatus, wherein each microlens of the microlens array has an aspherical shape that corrects an aberration due to distortion of a surface of the pixel portion.   2. The image exposure apparatus according to claim 1, wherein the aspherical surface is a toric surface. A spatial light modulation element in which a large number of pixel portions each modulating the irradiated light are two-dimensionally arranged;
A light source for irradiating light to the spatial light modulator;
Including a microlens array in which microlenses for condensing light from each pixel portion of the spatial light modulator are arranged in an array, and an image formed by the light modulated by the spatial light modulator is formed on a photosensitive material. In an image exposure apparatus comprising an imaging optical system for forming an image,
An image exposure apparatus, wherein each microlens of the microlens array has a refractive index distribution that corrects an aberration due to distortion of a surface of the pixel portion. 4. The image exposure according to claim 1 , wherein each microlens of the microlens array has a lens opening shape that does not allow light from a peripheral portion of the pixel portion to enter. 5. apparatus. The image exposure apparatus according to claim 4, wherein the microlens has a circular lens opening shape. The opening shape of the microlenses, the image exposure apparatus according to claim 4 or 5, wherein that it is defined by providing a light shielding portion in a part of the lens surface. The imaging optical system has at least a part of an optical system that forms an image of light modulated by the spatial light modulation element on the microlens array;
The imaging position of the part of the optical system is an image exposing apparatus that features to claims 1 to 6 any one of claims to, which is set on the lens surface of the microlens array. The imaging optical system includes a first imaging optical system that forms an image of light modulated by the spatial light modulator on the microlens array, and an image of light condensed by the microlens array. A second imaging optical system that forms an image on the photosensitive material;
Between the microlens array and the second imaging optical system, an aperture array having a large number of apertures for individually focusing the light emitted from the microlens is arranged. image exposure apparatus according to claim 1 to 7 or 1, wherein said. The image exposure apparatus according to claim 8 , wherein the aperture array is disposed at a focal position of the microlens. The spatial light modulator, of micromirrors are two-dimensionally arranged consisting DMD according to claims 1, characterized in that the (digital micromirror device) 9 any one as the pixel portion Image exposure device. Image exposure method comprising exposing a predetermined pattern on a photosensitive material using an image exposure apparatus according to claim 1 to 10 any one of claims.