This application is based on and claims priority under 35 USC 119 from Japanese Patent Applications No. 2009-095325 filed on Apr. 9, 2009 and No. 2009-212419 filed on Sep. 14, 2009.
1. Technical Field
The present invention relates to an exposure device and an image forming device.
2. Related Art
An exposure device of the laser ROS (Raster Output Scanner) method, that scans by a polygon mirror light that is emitted from a laser light source, is conventionally used as an exposure device that writes a latent image onto a photoreceptor drum in copiers, printers and the like that form images by the electrophotographic method. Recently, exposure devices of the LED method that utilize light-emitting diodes (LEDs) as the light source are mainly being used instead of exposure devices of the laser ROS method. An exposure device of the LED method is called an LED print head, and is abbreviated as LPH.
An LED print head has an LED array in which numerous LEDs are arrayed on an elongated substrate, and a lens array in which numerous refractive index distribution type rod lenses are arrayed. Note that, here, “array” means a row of elements in which elements such as plural LEDs or plural lenses or the like are arrayed in a one-dimensional form or a two-dimensional form. In an LED array, numerous LEDs are arrayed in correspondence with the number of pixels in the fast scanning direction, for example, 1200 pixels per inch (i.e., 1200 dpi) are arrayed. A cylindrical rod lens exemplified by a SELFOC™ is used as the refractive index distribution type rod lens.
At the LED print head, the lights emitted from the respective LEDs are collected by the rod lenses, and an erect equal magnification image is imaged on a photoreceptor drum. Accordingly, a scanning optical system of the laser ROS method is not needed, and the structure can be made much more compact than a structure in accordance with the laser ROS method. Further, a driving motor that rotates a polygon mirror also in unnecessary, and there is the advantage that mechanical noise does not arise.
Several techniques using a hologram element array instead of rod lenses in LED print heads have been proposed.
LED print heads using LED arrays are generally used as exposure devices of the electrophotographic method, and therefore, this type of exposure method is usually called the “LED method”. However, because there is no need to limit the light-emitting elements to LEDs, hereinafter, the “LED method” will, for convenience, instead be called the “light-emitting element array method”.
According to an aspect of the invention, there is provided an exposure device including:
a light-emitting element array at which plural light-emitting elements, that emit light that passes through an optical path of diffused light, are arrayed one-dimensionally or two-dimensionally on a substrate; and
a hologram element array at which plural hologram elements are formed at positions, that respectively correspond to the plural light-emitting elements, of a hologram recording layer disposed on the substrate, so as to diffract and collect, at an outer side of illumination regions of all of the plural light-emitting elements, respective lights that are emitted from the plural light-emitting elements respectively.
Exemplary embodiments of the present invention will be described in detail based on the following figures, wherein:
Examples of exemplary embodiments of the present invention will be described in detail hereinafter with reference to the drawings.
The image forming process section 10 has four image forming units 11Y, 11M, 11C, 11K that are disposed in parallel at uniform intervals. The image forming units 11Y, 11M, 11C, 11K form toner images of yellow (Y), magenta (M), cyan (C), black (K), respectively. Note that the image forming units 11Y, 11M, 11C, 11K are collectively called the “image forming units 11” as appropriate.
Each of the image forming units 11 has a photoreceptor drum 12 serving as an image carrier on which an electrostatic latent image is formed and that carries a toner image, a charging unit 13 that uniformly charges the surface of the photoreceptor drum 12 at a predetermined potential, an LED print head (LPH) 14 serving as an exposure device that exposes the photoreceptor drum 12 charged by the charging unit 13, a developing unit 15 that develops the electrostatic latent image obtained by the LPH 14, and a cleaner 16 that cleans the surface of the photoreceptor drum 12 after transfer.
The LPH 14 is an elongated print head of a length that is substantially the same as the axial direction length of the photoreceptor drum 12. Plural LEDs are arranged in the form of an array along the lengthwise direction at the LPH 14. The LPH 14 is disposed at the periphery of the photoreceptor drum 12 such that the lengthwise direction of the LPH 14 faces the axial direction of the photoreceptor drum 12. Further, in the present exemplary embodiment, the operation distance of the LPH 14 is long, and the LPH 14 is disposed so as to be separated by several cm from the surface of the photoreceptor drum 12. Therefore, the width that the LPH 14 occupies in the peripheral direction of the photoreceptor drum 12 is small, and crowding at the periphery of the photoreceptor drum 12 is mitigated.
The image forming process section 10 has an intermediate transfer belt 21 onto which toner images of the respective colors, that were formed at the photoreceptor drums 12 of the respective image forming units 11, are multiple-transferred, a primary transfer roller 22 that successively transfers (primarily transfers) the toner images of the respective colors of the respective image forming units 11 onto the intermediate transfer belt 21, a secondary transfer roller 23 that collectively transfers (secondarily transfers), onto a sheet P that is a recording medium, the superposed toner image transferred on the intermediate transfer belt 21, and a fixing unit 25 that fixes the secondarily-transferred image on the sheet P.
Next, operation of the above-described image forming device will be described.
First, the image forming process section 10 carries out image formation operation on the basis of control signals such as synchronizing signals and the like that are supplied from the control section 30. At this time, image data, that is inputted from the image reading device 3 or the PC 2, is subjected to image processings by the image processing section 40, and is supplied to the respective image forming units 11 via an interface.
For example, at the yellow image forming unit 11Y, the surface of the photoreceptor drum 12, that has been charged uniformly at a predetermined potential by the charging unit 13, is exposed by the LPH 14 that emits light on the basis of the image data obtained from the image processing section 40, and an electrostatic latent image is formed on the photoreceptor drum 12. Namely, due to the respective LEDs of the LPH 14 emitting light on the basis of the image data, the surface of the photoreceptor drum 12 is fast-scanned, and, due to the photoreceptor drum 12 rotating, the surface is subscanned, and the electrostatic latent image is formed on the photoreceptor drum 12. The formed electrostatic latent image is developed by the developing unit 15 such that a yellow toner image is formed on the photoreceptor drum 12. Similarly, toner images of the respective colors of magenta, cyan, black are formed at the image forming units 11M, 11C, 11K.
The toner images of the respective colors formed at the respective image forming units 11 are successively electrostatically attracted and transferred (primarily transferred) by the primary transfer roller 22 onto the intermediate transfer belt 21 that rotates in the arrow A direction in
Then, due to a transfer electric field that is formed by the secondary transfer roller 23 at the secondary transfer portion, the superposed toner image is electrostatically transferred (secondarily transferred) all at once onto the sheet P that has been conveyed-in. The sheet P, on which the superposed toner image has been electrostatically transferred, is peeled-off from the intermediate transfer belt 21 and is conveyed to the fixing unit 25 by the conveying belt 24. The unfixed toner image on the sheet P that has been conveyed to the fixing unit 25 is subjected to fixing processing by heat and pressure by the fixing unit 25, and is thereby fixed on the sheet P. The sheet P on which the fixed image has been formed is then discharged-out to a sheet discharge tray (not shown) that is provided at a discharging section of the image forming device.
Note that, due to a longer length of the operation distance of the LPH, the periphery of the photoreceptor drum does not become crowded, and the image forming device can be made compact on the whole. In a conventional LPH, the optical path length (operation distance) from the lens array end surface of the rod lens to the imaging point is short at around several mm, and the proportion of the periphery of the photoreceptor drum that the exposure device occupies is large. Further, generally, in an LPH that uses LEDs that emit incoherent light, the coherence is low and spot blurring (so-called color aberration) arises, and it is not easy to form minute spots.
<LED Print Head (LPH)>
(Structure of LPH)
As shown in
Each of the plural LEDs 50 is packaged on an elongated LED substrate 58 together with driving circuits (not shown) that drive the respective LEDs 50. As described above, the LEDs 50 are arrayed along a direction parallel to the axial direction of the photoreceptor drum 12. The arrayed direction of the LEDs 50 is the “fast scanning direction”. Further, the respective LEDs 50 are arrayed such that the interval (light-emitting point pitch) in the fast scanning direction of two LEDS 50 (light-emitting points) that are adjacent to one another is a uniform interval. Note that slow scanning is carried out by rotation of the photoreceptor drum 12, and the direction orthogonal to the “fast scanning direction” is illustrated as the “slow scanning direction”.
The hologram element array 56 is formed within a hologram recording layer 60 that is formed on the LED substrate 58. As will be described later, there is no need for the LED substrate 58 and the hologram recording layer 60 to fit tightly together. In the example shown in
The hologram recording layer 60 is structured from a polymer material that can record and hold a hologram permanently. A so-called photopolymer can be used as this polymer material. A photopolymer records a hologram by utilizing the change in the refractive index due to polymerization of photopolymerizable monomers. In the same way as the LEDs 50, the respective hologram elements 54 are arrayed along the fast scanning direction in respective correspondence with the LEDs 50. Further, the respective hologram elements 54 are arrayed such that the interval in the fast scanning direction of two hologram elements 54 that are adjacent to one another is the same interval as the aforementioned light-emitting point pitch.
As shown in
The respective LEDs 50 are disposed on the LED substrate 58 with the light-emitting surfaces thereof facing the surface side of the hologram recording layer 60, so as to emit light toward the corresponding hologram elements 54. The “light-emission optical axis” of the LED 50 passes through a vicinity of the center of the corresponding hologram element 54 (the axis of symmetry of the truncated cone), and is directed in a direction orthogonal to the LED substrate 58. As described above, the light-emission optical axis is orthogonal to both the fast scanning direction and the slow scanning direction.
It is preferable to use, as the LED array 52, an SLED array that is structured by plural SLED chips (not shown), at which plural self-scanning LEDs (SLEDs) are arrayed, are arrayed in series. An SLED array turns switches on and off by two signal wires, and can make the respective SLEDs emit light selectively. Therefore, data lines can be used in common. By using the SLED array, a smaller number of wires on the LED substrate 58 suffices.
Although not illustrated, the LPH 14 is held by a holding member such as a housing or a holder or the like such that the diffracted lights generated at the hologram elements 54 exit in the direction of the photoreceptor drum 12, and the LPH 14 is mounted to a predetermined position within the image forming unit 11. Note that the LPH 14 is preferably structured so as to be able to move in the optical axis direction of the diffracted lights by an adjusting unit such as adjusting screws (not shown) or the like. The imaging positions (focal plane) of the hologram elements 54 are adjusted by the adjusting unit so as to be positioned on the surface of the photoreceptor drum 12. Further, it is preferable that a protective layer is formed by a covering glass or a transparent resin or the like on the hologram recording surface 60. The adhesion of dust is prevented by the protective layer.
(Operation of LPH)
Next, operation of the above-described LPH 14 will be described briefly.
First, the principles of recording/reconstruction of the hologram element 54 will be briefly described.
As shown in
The signal light and the reference light are illuminated onto the hologram recording layer 60A from the same side (the side at which the LED substrate 58 is disposed). The interference fringes (intensity distribution) obtained by interference between the signal light and the reference light are recorded over the depth direction of the hologram recording layer 60A. Due thereto, the hologram recording layer 60 at which the transmission-type hologram elements 54 are formed is obtained. The hologram element 54 is a volume hologram in which the intensity distribution of the interference fringes is recorded in the surface direction and in the depth direction. The LPH 14 is fabricated by mounting the hologram recording layer 60 on the LED substrate 58 to which the LED array 52 is packaged.
The hologram recording layer 60A may be formed so as to contact the LEDs 50, or may be separated therefrom via an air layer, a transparent resin layer, or the like. If the hologram recording layer 60A contacts the LEDs 50, the hologram elements 54 are formed in cone shapes or oval cone shapes. If the hologram recording layer 60A is separated from the LEDs 50, as shown in
Further, although the surface 12A is illustrated schematically in
As shown in
A volume hologram and a phase-type zone plate that is called a kinoform can obtain a diffraction efficiency of 100% in theory due to the design, with respect to coherent light of a specific wavelength, specific incidence direction. However, even if such a hologram element is used, a decrease in the diffraction efficiency cannot be avoided because spreading of the wavelength distribution and spreading of the exiting angle exist particularly with respect to incoherent light sources. Further, with respect to coherent light sources as well, it is difficult to realize a diffraction efficiency of 100% due to wavelength dispersion of the light source, manufacturing dispersion at the time of fabricating the hologram elements, and the like.
The zero-order diffracted light component that is not diffracted becomes background noise of the collected spot, and impedes the achieving of an imaging performance of high contrast. In the present exemplary embodiment, as shown in
As described above, the light that exits from the LED 50 passes through the optical path of the diffused light that spreads from the light-emitting point to the hologram diameter rH. In the present exemplary embodiment, the angle θ that is formed by the light-emission optical axis and the diffracted light optical axis is set such that the photoreceptor drum 12 is positioned at the outer side of the optical path of this diffused light. Therefore, the transmitted reference light is not illuminated as background noise onto the photoreceptor drum 12 that is positioned at the outer side of the optical path of the diffused light.
In other words, because the hologram element 54 emits diffracted light at the outer side of the illumination region of the transmitted reference light, the diffracted light does not include a zero-order diffracted light component (transmitted reference light). Due thereto, the background noise due to zero-order diffracted light is reduced, and a spot having high contrast is formed. Further, in order to prevent generation of stray light, it is preferable to place a light-blocking film 68 such as a light absorbing film or the like at the diffused light transmitting side of the hologram recording layer 60. The light-blocking film 68 is disposed on the optical path of the diffused light that is transmitted.
Similarly, as shown in
The respective diffracted lights that exit are converged in the direction of the photoreceptor drum 12, and are imaged at the surface of the photoreceptor drum 12 that is disposed at the focal plane that is several cm ahead. Namely, each of the plural hologram elements 54 functions as an optical member that diffracts and collects the light emitted from the corresponding LED 50 and images it on the surface of the photoreceptor drum 12. Minute spots 621 through 626 in accordance with the respective diffracted lights are formed on the surface of the photoreceptor drum 12 so as to be arrayed in one row in the fast scanning direction. In other words, the photoreceptor drum 12 is fast-scanned by the LPH 14. Note that, when there is no need to differentiate therebetween, the spots 621 through 626 are collectively called the “spots 62”.
(Sizes of Respective Elements of LPH)
An example in which the six LEDs 501 through 506 are arrayed in one row is shown schematically in
When forming a spot by collecting light by a collective lens, the limit of making the spots minute is derived and determined from the diffraction phenomenon of light. A spot formed by a collective lens is called an Airy disk from the following relational expressions. A diameter φ of the Airy disk (spot size) is expressed as φ=1.22λ/NA (=2.44 λF), by using wavelength λ, and numerical aperture NA of the collective lens. Accordingly, given that the operation distance, which substantially corresponds to the focal length, is f, f=rHφ/2.44λ.
NA=sin θ=rH/2f
F (F number)=f/rH
f: focal length
f=rHφ/2.44λ
At an LPH that uses a conventional hologram element array, each of the plural hologram elements is fabricated at a diameter that is less than or equal to the pitch interval of the LEDs (the light-emitting point pitch) so that the hologram elements do not overlap one another, similarly to a case in which plural lenses are arrayed in respective correspondence with LEDs. The light-emitting point pitch is substantially the same length as the interval between the minute spots formed on the photoreceptor drum (the pixel pitch), and is several tens of μm. At a hologram element of a diameter of several tens of μm, due to the spreading (diffraction limit) of the beam due to diffraction, only an operation distance of the order of several mm can be obtained in the same way as a rod lens. In contrast, in the present exemplary embodiment, by making the diameter of the hologram element larger than the light-emitting point pitch, an operation distance of the cm order is realized.
For example, conventionally, when the diameter of a hologram element is made to be less than or equal to the light-emitting point pitch, at a resolution of 1200 dpi, the hologram size rH must be made to be less than or equal to around 20 μm. At this time, if the wavelength is made to be 780 nm, 420 μm at the highest is the limit of the operation distance, even if the spot size φ is permitted to around 40 μm. In this way, in the conventional art, the operation distance cannot made to be long to the cm order.
On the other hand, if the diameter of the hologram element is made to be larger than the light-emitting point pitch as in the present exemplary embodiment, the operation distance becomes long to the cm order. For example, by making the diameter (hologram diameter rH) of the hologram element 54, that functions as a collective lens, be greater than or equal to 1 mm, the operation distance becomes greater than or equal to 1 cm. For example, as will be described later, if the hologram diameter rH=2 mm and the hologram thickness hH=250 μm, a spot size φ of around 40 μm (around 30 μm at half value width) is realized at an operation distance of 4 cm.
As described above, the diameter of the hologram element may be made to be greater than or equal to 1 mm. Further, if the diameter of the hologram element exceeds 10 mm, the multiplicity of the hologram elements becomes very high. Therefore, the problem arises that the diffraction efficiency, that is limited by the dynamic range of the material, decreases. Accordingly, the diameter of the hologram element may be made to be less than or equal to 10 mm.
(Method of Manufacturing LPH)
Next, the method of manufacturing the LPH 14 will be described.
First, as shown in
Next, as shown in
Next, as shown in
First, the signal light and the reference light, such as the illumination positions of the laser lights, the illumination angles, the spread angles, the converging angles and the like, are designed from the measurement data obtained by the aforementioned chip alignment inspection and the design values of the hologram element 54 (the hologram diameter rH, the hologram thickness hH). Here, the signal light is designed so as to exit in a direction in which the optical axis of the diffracted light generated at the hologram element 54 (the reconstructed signal light) forms the angle θ with the light-emission optical axis, and so as to be collected in the direction of the photoreceptor drum 12. Then, the writing optical systems for illuminating the designed signal light and reference light are placed.
With the writing optical systems placed and fixed, spherical waves that converge are used as the reference light, and the LED substrate 58 on which the hologram recording layer 60A is formed is moved with respect to the signal light and the reference light. The LED substrate 58 is moved at the light-emitting point pitch such that the reference light is successively converged at each of the plural LEDs 50. The plural hologram elements 54 are multiplex-recorded at the hologram recording layer 60A by spherical wave shift multiplexing.
Next, as shown in
Next, the entire surface is exposed, the photopolymerizable monomer remaining at the dark portions is polymerized such that the polymerization reaction is completed, and there is a state in which writing and deletion cannot be carried out. Note that methods based on various recording mechanisms are proposed as the hologram recording material. A material may be used as the hologram recording material in the present invention provided that it is a material at which refractive index modulation corresponding to a light intensity distribution can be recorded.
Finally, as shown in
Note that the above exemplary embodiment describes an example in which the LEDs 50 and the hologram recording layer 60A are contacting. However, the hologram recording layer 60A may be formed so as to be separated from the LEDs 50 via an air layer or a transparent resin layer or the like. At this time, a sheet, that is formed from a hologram recording layer sandwiched by protective layers, may be fabricated separately and may be placed on the light-emitting element array.
As shown in
The plural LEDs 50 are arrayed in a staggered form along the fast scanning direction. In this example, three of the LEDs that are the LED 501, the LED 503 and the LED 505 are arrayed on a first straight line that is parallel to the fast scanning direction, and three of the LEDs that are the LED 502, the LED 504 and the LED 506 are arrayed on a second straight line that is parallel to the fast scanning direction. The first straight line and the second straight line are set apart by a uniform interval in the slow scanning direction. The interval between the first straight line and the second straight line is an interval that is substantially the same as the light-emitting point pitch. In other words, all of the LEDs 50 that structure the LED array 52 (the six LEDS 501 through 506) are disposed so as to be offset in the slow scanning direction so as to not be positioned on a single straight line.
Further, the respective LEDs 50 are arrayed such that the interval (the light-emitting point pitch) in the fast scanning direction of two of the LEDs 50 (light-emitting points) that are adjacent to one another is a uniform interval. For example, the interval in the fast scanning direction between the LED 501 and the LED 502, and the interval in the fast scanning direction between the LED 502 and the LED 503 are equal. By arranging the plural LEDs 50 in a staggered form, the light-emitting point pitch is narrowed.
The respective hologram elements 54 are disposed in a staggered form along the fast scanning direction in correspondence with the respective LEDs 50 and in the same way as the LEDs 50. Further, the respective hologram elements 54 are arrayed such that the interval in the fast scanning direction between two of the hologram elements 54 that are adjacent to one another is the same interval as the aforementioned light-emitting point pitch.
Note that, in the example shown in
The second straight line is apart from the first straight line by a uniform interval in the slow scanning direction. As shown in
Note that, in
The respective diffracted lights that exit are converged in the direction of the photoreceptor drum 12, and are imaged at the surface of the photoreceptor drum 12 that is disposed at the focal plane that is several cm ahead. Spot 621, spot 623, spot 625 are formed on the surface 12A of the photoreceptor drum 12 by the hologram element 541, the hologram element 543, the hologram element 545. Further, spot 622, spot 624, spot 626 are formed by the hologram element 542, the hologram element 544, the hologram element 546.
As shown in
In other words, all of the LEDs 501 through 506 that structure the LED array 52 are disposed so as to be offset in the slow scanning direction so as to not be positioned on a single straight line. For example, the three LEDs that are the LED 501, the LED 502, the LED 503 are not positioned on a single straight line. Note that, if the LED array 52 only includes two of the LEDs 50 in total, the two LEDs 50 will be positioned on a single straight line. Therefore, the LED array 52 of the present exemplary embodiment is a structure that includes three or more LEDs 50.
On the other hand, the six hologram elements 541 through 546 are provided so as to correspond to the LEDs 501 through 506, respectively. The spots 621 through 626, that are diffracted and collected by these six hologram elements 541 through 546 and are formed on the surface 12A of the photoreceptor drum 12, are positioned substantially on a single straight line.
Note that, here, “positioned substantially on a single straight line” includes cases in which the spots are positioned on a single straight line within a range of errors in design. Further, the above describes an example in which the plural LEDs 50 are arrayed in a staggered form. However, even if the plural LEDs 50 are arrayed randomly, it suffices to appropriately design the corresponding hologram elements 54 such that the spots 62 are positioned substantially on a single straight line.
As mentioned above, an SLED array, that is structured by plural SLED chips at which plural SLEDs are arrayed being arrayed in series, can be used as the LED array 52. In this way, if a plurality of chips at which plural LEDs are arrayed are arranged, the plural LEDs can be arrayed in a staggered form in chip units.
As shown in
Even when allotted between the LED chip 581 and the LED chip 582, the respective LEDs 50 are arrayed such that the interval (light-emitting point pitch) in the fast scanning direction of two LEDs 50 (light-emitting points) that are adjacent to one another is a uniform interval. For example, the interval in the fast scanning direction between the LED 502 and the LED 503 is equal to the interval in the fast scanning direction between the LED 503 and the LED 504.
The three LEDs 50 that are the LED 501, the LED 502 and the LED 503 are arrayed on a first straight line that runs along the fast scanning direction, such that an LED array 521 is structured. Further, the three LEDs 50 that are the LED 504, the LED 505 and the LED 506 are arrayed on a second straight line that runs along the fast scanning direction, such that an LED array 522 is structured. The first straight line and the second straight line are separated at a uniform interval in the slow scanning direction. The interval between the first straight line and the second straight line is substantially the same interval as the light-emitting point pitch.
The hologram recording layer 60 is formed on the LED chip 581 and the LED chip 582 so as to cover the LED chip 581 and the LED chip 582. The plural hologram elements 54 are formed at the hologram recording layer 60 along the fast scanning direction in respective correspondence with the plural LEDs 50. The respective hologram elements 54 are arrayed such that the interval in the fast scanning direction between the two hologram elements 54 that are adjacent to one another is the same interval as the aforementioned light-emitting point pitch.
Specifically, the three hologram elements that are the hologram element 541, the hologram element 542 and the hologram element 543 are formed in respective correspondence with the three LEDs 50 of the LED chip 581. Further, the three hologram elements that are the hologram element 541, the hologram element 542 and the hologram element 543 are formed in respective correspondence with the three LEDs 50 of the LED chip 582. Note that, in the example shown in
In the same way as in the example shown in
In the present exemplary embodiment, each light, that exits from the three LEDs that are the LED 501, the LED 502, the LED 503 that are arrayed on the first straight line, is diffracted in a direction that forms the angle θ1 with the light-emission optical axis, by the corresponding hologram element 541, hologram element 542, hologram element 543. Further, each light, that exits from the three LEDs that are the LED 504, the LED 505, the LED 506 that are arrayed on the second straight line, is diffracted in a direction that forms the angle θ2 with the light-emission optical axis, by the corresponding hologram element 544, hologram element 545, hologram element 546.
As shown in
Note that, in the example shown in
As shown in
A light-blocking body 70, that is elongated and extends in the fast scanning direction, is provided at the obverse of the hologram recording layer 60. The elongated light-blocking body 70 is disposed so as to be adjacent, at the photoreceptor drum 12 side, to a plane in which the optical paths of the diffracted lights that are diffracted by the hologram elements 54 (the reconstructed signal lights) and the obverse of the hologram recording layer 60 intersect. Namely, the light-blocking body 70 is disposed so as to avoid the optical paths of the diffused lights (reference lights) that spread from the light-emitting points to the hologram diameters rH, and the optical paths of the diffracted lights (signal lights) that are diffracted by the hologram elements 54.
Note that, in the same way as in the first exemplary embodiment, the LED array 52 has the six LEDs 501 through 506. The six LEDs 501 through 506 are arrayed in a row at a uniform interval (light-emitting point pitch) along the fast scanning direction. Further, in the same way as in the in the first exemplary embodiment, the hologram element array 56 has the six hologram elements 541 through 546. The six hologram elements 541 through 546 are arrayed in a row at a uniform interval (the same pitch as the light-emitting point pitch) along the fast scanning direction.
It is known that emitted light 72, that exits from the LED 50 that is an incoherent light source, diverges and spreads as shown in
As shown in
As shown in
The light-blocking body 70, that is elongated and extends in the fast scanning direction, is provided at the obverse of the hologram recording layer 60. The LED chip 581 and the LED chip 582 are disposed so as to be offset at a uniform interval in the slow scanning direction. The diffracted lights corresponding to the LED chip 581, and the diffracted lights corresponding to the LED chip 582, exit at different angles from different positions. Accordingly, the elongated light-blocking body 70 is formed at a narrow width at the portion corresponding to the LED chip 581 and at a wide width at the portion corresponding to the LED chip 582. The light-blocking body 70 blocks the light other than the diffracted light diffracted by the hologram element array 56, and prevents stray light from being illuminated onto the photoreceptor drum 12.
Note that the fourth exemplary embodiment describes an example in which the light-blocking body 70 is provided on the obverse of the hologram recording layer 60, but the shape and the placement of the light-blocking body 70 are not limited to this. Various modified examples can be supposed, provided that the light-blocking body 70 exhibits the functions of blocking the light other than the diffracted light diffracted by the hologram element array 56, and preventing the other emitted light 72, that is diffused as stray light, from being illuminated onto the photoreceptor drum 12.
As shown in
Further, as shown in
Moreover, as shown in
As shown in
Further, as shown in
Note that the above exemplary embodiments describe an LED print head that is equipped with plural LEDs, but other light-emitting elements, such as ELs or the like, may be used instead of the LEDs. By designing the hologram elements in accordance with the characteristics of the light-emitting elements and by preventing unnecessary exposure by incoherent light, minute spots having distinct outlines are formed in the same way as in cases in which LDs that emit coherent light are used as the light-emitting elements, even when LEDs or ELs that emit incoherent light are used as the light-emitting elements.
Further, the above exemplary embodiments describe examples of multiplex-recording plural hologram elements by spherical wave shift multiplexing. However, the plural hologram elements may be multiplex-recorded by another multiplexing method, provided that it is a multiplexing method by which the desired diffracted lights can be obtained. Further, plural types of multiplexing methods may be used in combination. Examples of other multiplexing methods include angle multiplex recording that records while changing the angle of incidence of the reference light, wavelength multiplex recording that records while changing the wavelength of the reference light, phase multiplex recording that records while changing the phase of the reference light, and the like. If multiplex recording is possible, separate diffracted lights are reconstructed without crosstalk from the plural holograms that are multiplex-recorded.
Further, the above exemplary embodiments describe a digital color printer of the type in which the image forming devices are in tandem, and an LED print head that serves an exposure device that exposes the photoreceptor drums of the respective image forming units. However, it suffices for there to be an image forming device that forms an image by image-wise exposing a photosensitive image recording medium by an exposure device, and the present invention is not limited to the example of the above exemplary embodiments. For example, the image forming device is not limited to a digital color printer of the electrophotographic method. The exposure device of the present invention may also be incorporated in an image forming device of the silver salt method, a writing device such as optical writing type electronic paper or the like, or the like. Further, the photosensitive image recording medium is not limited to a photoreceptor drum. The exposure device of the present invention can also be applied to the exposure of sheet-like photoreceptors or photographic photosensitive materials, photoresists, photopolymers, or the like.
Number | Date | Country | Kind |
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2009-095325 | Apr 2009 | JP | national |
2009-212419 | Sep 2009 | JP | national |
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Apr. 4, 2012 Office Action issued in U.S. Appl. No. 12/614,799. |
Office Action dated Oct. 10, 2013 issued in Chinese Patent Application No. 200910265268.7 (with translation). |
Number | Date | Country | |
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20100259739 A1 | Oct 2010 | US |