JP2017142509A - Image forming apparatus, and vehicle having image forming apparatus mounted thereon - Google Patents

Image forming apparatus, and vehicle having image forming apparatus mounted thereon Download PDF

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Publication number
JP2017142509A
JP2017142509A JP2017044501A JP2017044501A JP2017142509A JP 2017142509 A JP2017142509 A JP 2017142509A JP 2017044501 A JP2017044501 A JP 2017044501A JP 2017044501 A JP2017044501 A JP 2017044501A JP 2017142509 A JP2017142509 A JP 2017142509A
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surface
mirror
forming apparatus
image forming
light
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JP2017044501A
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Japanese (ja)
Inventor
賢一郎 齊所
Kenichiro Saisho
賢一郎 齊所
佐藤 裕之
Hiroyuki Sato
裕之 佐藤
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株式会社リコー
Ricoh Co Ltd
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Abstract

To provide an image forming apparatus capable of downsizing without sacrificing high brightness and large screen.
The image forming apparatus includes: an optical scanning device configured to two-dimensionally deflect a light beam emitted from a light source element by an optical deflector to form a two-dimensional image on a scanned surface having transparency; A projection optical system for enlarging and projecting a dimensional image onto the projection surface, and the projection surface is a reflective surface of a transflective mirror that is provided outside and transmits part of visible light and reflects part of it The surface to be scanned is a diffusion plate that diffuses incident light toward the traveling direction, and the cross-sectional shape of the light diffused by the diffusion plate is an ellipse.
[Selection] Figure 7

Description

  The present invention relates to an image forming apparatus including an optical scanning device that scans a light beam emitted from a light source element to form a two-dimensional image, and a vehicle equipped with the image forming device.

  2. Description of the Related Art In recent years, there have been widely proposed optical scanning devices that obtain a color two-dimensional image by causing multicolor light beams to enter a mirror that performs two-dimensional scanning. In particular, in an optical scanning device using a semiconductor laser as a light source, high light utilization efficiency is obtained due to the high directivity of the light beam emitted from the semiconductor laser. In addition, an optical scanning device using a semiconductor laser can emit strong light in a device without providing a huge radiator such as a xenon lamp, and in a small optical system because of its high directivity. Can also form bright images.

  An image forming apparatus such as a head-up display can be realized by using an optical scanning device using a semiconductor laser. Since such an image forming apparatus is incorporated in, for example, a passenger car, downsizing is inevitably required.

  However, when a reduction in the size of the image forming apparatus is pursued, there arises a problem that high brightness and a large screen are sacrificed.

  The present invention has been made in view of the above, and an object of the present invention is to provide an image forming apparatus that can be reduced in size without sacrificing higher luminance or larger screen.

  The image forming apparatus includes: an optical scanning device that two-dimensionally deflects a light beam emitted from a light source element by an optical deflector to form a two-dimensional image on a scan target surface having transparency; A projection optical system for enlarging and projecting onto a projection surface, and the projection surface is a reflection surface of a semi-transparent mirror that is provided outside and transmits a part of visible light and reflects a part thereof, The surface to be scanned is a diffusion plate that diffuses incident light toward the traveling direction, and the cross-sectional shape of the light diffused by the diffusion plate is an ellipse.

  According to the disclosed technology, it is possible to provide an image forming apparatus that can realize downsizing without sacrificing high brightness or large screen.

1 is a diagram illustrating an image forming apparatus according to a first embodiment. FIG. 3 is a diagram (part 1) illustrating an optical path of the optical scanning device according to the first embodiment; FIG. 6 is a second diagram illustrating an optical path of the optical scanning device according to the first embodiment; It is a figure for demonstrating the lens. It is a figure for demonstrating arrangement | positioning of an optical deflector and a concave mirror. It is a figure for demonstrating the positional relationship of a to-be-scanned surface and a semi-transmission mirror. It is a figure for demonstrating the cross-sectional shape of each light beam which permeate | transmitted the to-be-scanned surface. It is a figure which illustrates the optical path of the optical scanning device concerning modification 1 of a 1st embodiment. 1 is a diagram illustrating an optical system according to Example 1. FIG. 6 is a diagram illustrating an optical system according to Example 2. FIG. 6 is a diagram illustrating a transflective mirror according to a second embodiment. FIG. 6 is a diagram illustrating an optical system according to Example 3. FIG.

  Hereinafter, embodiments for carrying out the invention will be described with reference to the drawings. In the drawings, the same components are denoted by the same reference numerals, and redundant description may be omitted.

<First Embodiment>
FIG. 1 is a diagram illustrating an image forming apparatus according to the first embodiment. Referring to FIG. 1, the image forming apparatus 20 generally includes an optical scanning device 10, a first mirror 21, a second mirror 22, and a semi-transmissive mirror 23. However, as will be described later, the semi-transmissive mirror 23 is not an essential component of the image forming apparatus 20. In FIG. 1, reference numeral 24 denotes an observer's eyeball (hereinafter referred to as eyeball 24), and 25 denotes a virtual image (hereinafter referred to as virtual image 25).

  First, the optical scanning device 10 will be described. FIG. 2 is a diagram (part 1) illustrating an optical path of the optical scanning device according to the first embodiment. FIG. 3 is a second diagram illustrating an optical path of the optical scanning device according to the first embodiment. 2 and 3 are views of the optical scanning device 10 as seen from different directions. However, in FIG. 3, the optical deflector 16, the concave mirror 17, and the scanned surface 18 shown in FIG. 2 are not shown.

  Referring to FIGS. 2 and 3, the optical scanning device 10 generally includes light source elements 11R, 11G, and 11B, coupling lenses 12R, 12G, and 12B, and apertures 13R, 13G, and 13B. It has an element 14, a lens 15, an optical deflector 16, a concave mirror 17, and a scanned surface 18.

  The light source elements 11R, 11G, and 11B, the coupling lenses 12R, 12G, and 12B, the apertures 13R, 13G, and 13B, the combining element 14, and the lens 15 may be collectively referred to as an incident optical system. is there. Further, the optical deflector 16, the concave mirror 17, and the scanned surface 18 may be referred to as a scanning optical system.

  In the optical scanning device 10, the light source elements 11R, 11G, and 11B can emit light beams having different wavelengths λR, λG, and λB, respectively. The wavelengths λR, λG, and λB can be set to, for example, 640 nm, 530 nm, and 445 nm, respectively. As the light source elements 11R, 11G, and 11B, for example, a laser, an LED (Light Emitting Diode), an SHG (Second Harmonic Generation) element, or the like can be used.

  From the viewpoint of realizing miniaturization while ensuring brightness and high image quality, it is preferable to use semiconductor lasers as the light source elements 11R, 11G, and 11B, respectively. The light source elements 11R, 11G, and 11B are controlled in emission power, emission timing, and the like by a control means (not shown). Note that the control means (not shown) may be provided inside the optical scanning device 10 or may be provided outside.

  Each light beam (diverging light) emitted from the light source elements 11R, 11G, and 11B according to the content of the image signal is converted into substantially parallel light or convergent light by the coupling lenses 12R, 12G, and 12B, respectively, and the aperture 13R. , 13G, and 13B. As the coupling lenses 12R, 12G, and 12B, for example, convex glass lenses, plastic lenses, and the like can be used.

  The apertures 13R, 13G, and 13B have a function of shaping a light beam incident thereon. The apertures 13R, 13G, and 13B can have various shapes such as a circle, an ellipse, a rectangle, and a square according to the divergence angle of the incident light beam.

  In addition, it is good also as a structure which provides one common coupling lens and one common aperture with respect to the light source elements 11R, 11G, and 11B. However, by providing coupling lenses 12R, 12G, and 12B and apertures 13R, 13G, and 13B to the light source elements 11R, 11G, and 11B, respectively, each of the light source elements 11R, 11G, and 11B is provided. Regardless of the difference in divergence angle, there is an advantage that the beam spot diameter on the scanned surface 18 can be adjusted to a desired value while ensuring the light use efficiency.

  The light beams shaped by the apertures 13R, 13G, and 13B are incident on the combining element 14 and are optically combined. The synthesizing element 14 is, for example, a plate-like or prism-like dichroic mirror, and has a function of reflecting or transmitting each light beam according to the wavelength and synthesizing it into one optical path.

  Each light beam combined in the optical path by the combining element 14 is guided by the lens 15 toward the reflecting surface of the optical deflector 16. As the lens 15, for example, a single meniscus lens arranged with the concave surface facing the optical deflector 16 can be used. Here, the lens 15 will be described in more detail with reference to FIG.

  FIG. 4 is a diagram for explaining the lens 15. In FIG. 4, 15 </ b> R and 15 </ b> B indicate two light beams having different wavelengths incident on the lens 15. It is preferable that the light beams 15 </ b> R and 15 </ b> B emitted from the second surface 15 b of the lens 15 are emitted in a size that fits on the reflection surface of the optical deflector 16. Since the lens 15 needs to send the light beams 15R and 15B captured by the apertures 13R and 13B as small as possible to the optical deflector 16, the first surface 15a of the lens 15 focuses the respective light beam diameters of the light beams 15R and 15B. Therefore, it is preferable that the surface is convex.

  Here, if the light beam 15R is a long wavelength light beam and the light beam 15B is a short wavelength light beam, the condensing state on the first surface 15a is different (dispersed) between the light beam 15R and the light beam 15B as shown in FIG. . If the lens 15 has another form (such as a biconvex lens or a plano-convex lens) other than the meniscus lens, the divergence angles of the emitted light beams 15R and 15B vary depending on the wavelength.

  By using a meniscus lens having the second surface 15b as a concave surface as the lens 15, the light beams 15R and 15B dispersed on the first surface 15a are refracted in the direction in which the degree of divergence is returned again on the second surface 15b. As a result, in the lens 15 into which the light beams 15R and 15B having different wavelengths are incident, the variation in the divergence degree of the emitted light beams 15R and 15B can be converged and sent to the optical deflector 16. It is possible to improve the luminance of the image without loss of image quality.

  2 and 3, the light beam emitted from the incident optical system and guided to the reflection surface of the optical deflector 16 is deflected two-dimensionally by the optical deflector 16. As the optical deflector 16, for example, one minute mirror that swings with respect to two orthogonal axes, two minute mirrors that swing or rotate with respect to one axis, and the like can be used. The optical deflector 16 can be, for example, a MEMS manufactured by a semiconductor process or the like. The optical deflector 16 can be driven by, for example, an actuator that uses the deformation force of the piezoelectric element as a driving force.

  The light beam deflected two-dimensionally by the optical deflector 16 enters the concave mirror 17 and is folded by the concave mirror 17 to draw a two-dimensional image on the scanned surface 18. It is preferable that the light beam incident on the scanned surface 18 has a close angle to the traveling direction of the light beam incident on the optical deflector 16. With such an arrangement, the distortion of the two-dimensional image on the scanned surface 18 can be reduced. Further, since the light beam enters the surface to be scanned 18 in a state of being nearly perpendicular, the transmission efficiency can be increased over a wide area in the two-dimensional image.

  By using the concave mirror 17 in the optical scanning device 10, the following effects can be obtained. First, since the concave mirror 17 does not have wavelength dispersion, color misregistration of the image on the scanned surface 18 can be reduced. Second, since the concave mirror 17 reduces the scanning angle of the light beam, the color shift of the image on the scanned surface 18 can be reduced. Third, the incident angle of the scanned surface 18 can be reduced at all scanning angles, and the luminance of the scanned surface 18 can be increased. Here, the color misregistration refers to the misregistration of a plurality of spots formed on the scanned surface 18 by the light source elements 11R, 11G, and 11B having different wavelengths. Fourth, the optical scanning device 10 can be miniaturized by turning back the optical path with the concave mirror 17.

  The concave mirror 17 has a non-arc surface shape in at least one direction, so that the speed characteristic on the scanned surface 18 can be corrected. That is, the light beam deflected by the optical deflector 16 can be given constant velocity, and the pixel pitch on the scanned surface 18 can be made uniform.

  Although a Fresnel lens or a refractive lens can be provided immediately before the scanned surface 18 instead of the concave mirror 17, when a Fresnel lens is provided, a shadow is generated in the sawtooth-shaped backcut portion of the Fresnel lens, and the amount of light is reduced. It is not preferable in that a loss occurs. In addition, when a refractive lens is provided, dispersion occurs in a plurality of light fluxes, and the plurality of light fluxes are shifted according to the wavelength, which is not preferable in terms of color shift.

  The scanned surface 18 is a surface having transparency that allows a light beam reflected by the concave mirror 17 to enter and form a two-dimensional image. As the scanned surface 18, for example, a diffusion plate can be used. The diffuser plate has a function of diffusing incident light toward the traveling direction. Although a microlens array can be used in place of the diffuser plate, the microlens array is not preferable in that a shadow is generated between the lenses, resulting in a large light loss and a reduction in light utilization efficiency.

  On the other hand, the diffusion plate is preferable in that it can select the diffusion angle of the transmitted light by the design of the surface shape, and therefore can reduce the light amount loss of the light beam sent to the subsequent optical system. For example, by forming random minute irregularities on the surface of the diffuser plate at or below the wavelength used, or by forming line-shaped irregularities, light is diffused only to the required range while maintaining high transmittance. Therefore, it is possible to reduce the light loss of the light beam sent to the subsequent optical system.

  Here, the arrangement of the optical deflector 16 and the concave mirror 17 will be described in more detail with reference to FIG. FIG. 5 is a diagram for explaining the arrangement of the optical deflector and the concave mirror. Referring to FIG. 5, the optical deflector 16 and the concave mirror 17 are arranged so that the signs of the declination angles (angles formed by the incident light beam and the outgoing light beam) are opposite to each other with respect to the total light beam. When the optical deflector 16 and the concave mirror 17 are viewed from a direction perpendicular to the YZ plane (X direction), the optical path of the light beam incident on the optical deflector 16, deflected by the optical deflector 16, and reflected by the concave mirror 17 is “Z”. "Draw the letter.

  In the YZ plane of FIG. 5, when the counterclockwise angle counted from the traveling direction of the incident light beam is defined as a positive deflection angle, the deflection angle 16d is negative in the optical deflector 16, and the deflection angle 17d in the concave mirror 17 is Is positive. Thus, the optical deflector 16 and the concave mirror 17 are arranged so that the signs of their declination are opposite to each other. By adopting such an arrangement, the optical path difference between the light beams reaching the upper end and the lower end of the scanned surface 18 is reduced, so that trapezoidal distortion and bending of the image on the scanned surface 18 can be reduced.

  In addition, when trapezoidal distortion or bending occurs in an image without adopting such an arrangement, it is possible to electrically correct the image, but there is a problem that an image becomes dark because invalid pixels are generated. In this embodiment mode, trapezoidal distortion and curvature of an image can be reduced without electrical correction, so that brightness and high image quality can be ensured.

  Thus, in the optical scanning device 10, the light scanning devices 10 that two-dimensionally scan the light beams having different wavelengths emitted from the light source elements 11 R, 11 G, and 11 B to form a multicolor image on the scanned surface 18. , The optical deflector 16 and the concave mirror 17 are arranged in the optical path so that the signs of their declination are opposite to each other. Thereby, the following effects are produced.

  That is, by using the concave mirror 17, the color shift of the image on the scanned surface 18 can be reduced. Further, by using the concave mirror 17, the incident angle of the scanned surface 18 can be reduced in all scanning angles, and the luminance of the scanned surface 18 can be increased. Further, by arranging the optical deflector 16 and the concave mirror 17 so that the signs of their declination are opposite to each other, the optical path difference of the light beam reaching the upper end and the lower end of the scanned surface 18 is reduced. The trapezoidal distortion and bending of the image on the surface 18 can be reduced. Further, by using the concave mirror 17, the optical scanning device 10 can be miniaturized. That is, it is possible to reduce the size of the optical scanning device 10 while ensuring the brightness and image quality of the image.

  Next, returning to FIG. 1, the first mirror 21, the second mirror 22, and the semi-transmissive mirror 23 will be described. In the first embodiment, a convex mirror is used as the first mirror 21, a concave mirror is used as the second mirror 22, and a semi-transmissive mirror having a flat reflecting surface is used as the semi-transmissive mirror 23. However, as shown in the examples described later, at least one of the first mirror 21 and the second mirror 22 may be a convex mirror. The first mirror 21 and the second mirror 22 may be referred to as a projection optical system.

  In the image forming apparatus 20, each light beam that has passed through the surface to be scanned 18 of the optical scanning device 10 is folded (reflected) by the first mirror 21 and enters the second mirror 22. Each light beam incident on the second mirror 22 is folded (reflected) by the second mirror 22 and enters the semi-transmissive mirror 23.

  In the image forming apparatus 20, the first mirror 21, which is a convex mirror, is disposed immediately after the scanned surface 18, so that sunlight entering the optical system of the image forming apparatus 20 is diffused by the first mirror 21, which is a convex mirror. Is done. Therefore, it is possible to prevent sunlight entering the optical system of the image forming apparatus 20 from being concentrated on the scanned surface 18. In addition, the convex mirror can make the intermediate image having a finite divergence angle a wider angle of view and shorten the optical path length, and is suitable for miniaturization. The convex mirror also has an advantage that chromatic aberration does not occur with respect to the lens.

  The semi-transmissive mirror 23 is a mirror having a transmittance in the visible range of 10 to 70%. For example, a dielectric multilayer film or a wire grid is formed on the side where the light flux reflected by the second mirror 22 is incident. Having a reflective surface. The reflecting surface of the semi-transmissive mirror 23 can selectively reflect the wavelength band of the light beam emitted from the light source element. That is, it can have a reflection peak or reflection band including wavelengths λR, λG, and λB, or can be formed so as to increase the reflectance with respect to a specific deflection direction.

  In the present embodiment, as described above, the reflective surface of the semi-transmissive mirror 23 is a flat surface, but the surface opposite to the reflective surface is substantially parallel to the reflective surface. That is, the thickness of the semi-transmissive mirror 23 is substantially constant.

  That is, the semi-transmissive mirror 23 selectively reflects the wavelength band of the light beam emitted from the light source elements 11R, 11G, and 11B of the optical scanning device 10. Therefore, it is possible to increase the brightness due to the plurality of image lights having specific wavelengths emitted from the optical scanning device 10.

  The reflective surface of the first mirror 21 can be anamorphic. That is, the reflection surface of the first mirror 21 can be a reflection surface having a curvature in a predetermined direction and a curvature in a direction orthogonal to the predetermined direction. By making the reflecting surface of the first mirror 21 anamorphic, the curved surface shape of the reflecting surface can be adjusted, and the aberration correction performance can be improved.

  FIG. 6 is a diagram for explaining the positional relationship between the scanned surface and the semi-transmissive mirror. As shown in FIG. 6, in the image forming apparatus 20, the scanned surface 18 and the semi-transmissive mirror 23 are arranged so that the normal line 18 h of the scanned surface 18 does not intersect the semi-transmissive mirror 23. By arranging in this way, stray light emitted from the scanned surface 18 is not reflected on the semi-transmissive mirror 23, and thus it is possible to prevent the generation of a ghost image.

  Although only three normal lines 18h are shown in FIG. 6, the scanned surface 18 and the semi-transmissive mirror 23 are all normal lines of the scanned surface 18 (the three methods shown in FIG. 6). (Including the line 18h) is arranged so as not to intersect the semi-transmissive mirror 23.

  Here, a cross-sectional shape (shape in a direction perpendicular to the light traveling direction) of each light beam transmitted through the scanning surface 18 of the optical scanning device 10 will be described. FIG. 7 is a diagram for explaining a cross-sectional shape of each light beam transmitted through the scanned surface. However, in FIG. 7, for the sake of convenience, the optical path from the optical deflector 16 to the virtual image 25 is shown in a straight line.

  As shown in FIG. 7, the cross-sectional shape 18d of each light beam transmitted through the scanning surface 18 of the optical scanning device 10 can be an ellipse. That is, a diffusing plate can be used as the surface to be scanned 18, and the cross-sectional shape of each light beam diffused by the diffusing plate can be an ellipse. For example, when the aspect ratio (vertical (Y direction): horizontal (X direction)) of the virtual image 25 is 1: 4, the cross-sectional shape 18d of each light beam is preferably an ellipse having an aspect ratio of approximately 1: 4. .

  In this way, a diffusing plate is used as the scanned surface 18, the cross-sectional shape 18 d of each light beam diffused by the diffusing plate is an ellipse, and the major axis direction of the ellipse is made coincident with the longitudinal direction of the virtual image 25. An optical system in which almost all of the light rays emitted from 18 contribute to image formation can be realized.

  In the case where the scanned surface 18 that is long in the X direction is formed into a virtual image 25 that is also long in the X direction, for example, if the cross-sectional shape 18d of each light beam is circular, the light utilization efficiency in the Y direction decreases, and a high-luminance image Can't get. On the other hand, in the optical scanning device 10, since the cross-sectional shape 18d of the light beam is an ellipse whose aspect ratio corresponds to the aspect ratio of the virtual image 25, the light utilization efficiency in the Y direction can be improved and a high brightness image can be obtained. it can.

  The image forming apparatus 20 can be mounted on a vehicle such as a passenger car. At that time, the semi-transmissive mirror 23 may be integrated with a front window of the vehicle. By disposing the image forming apparatus 20 in front of the driver in a vehicle such as a passenger car, the light flux reflected by the reflecting surface of the semi-transmissive mirror 23 (which may be integrated with the front window or the like) The two-dimensional image of the scanned surface 18 enters a predetermined position ahead of the reflecting surface of the translucent mirror 23 (which may be integrated with the front window or the like). It is visually recognized as an enlarged virtual image 25.

  That is, the image forming apparatus 20 can realize a so-called head-up display. In this case, examples of the two-dimensional image of the scanned surface 18 include vehicle instrument information and map information. Since the virtual image 25 is in a predetermined position in front of the reflecting surface of the transflective mirror 23 (which may be integrated with the front window or the like), the driver focuses on the foreground while driving. The vehicle instrument information, map information, etc. can be viewed without moving greatly.

  As described above, in the image forming apparatus 20, the virtual image 25 obtained by enlarging the two-dimensional image formed on the scanned surface 18 of the optical scanning device 10 by the first mirror 21, the second mirror 22, and the semi-transmissive mirror 23. And a so-called head-up display can be realized.

  As is clear from the above description, there are cases where the translucent mirror 23 is included as a component of the image forming apparatus 20 and where the translucent mirror 23 is not included. When the semi-transmissive mirror 23 is not included as a component of the image forming apparatus 20, the function of the semi-transmissive mirror 23 can be provided to the front window of the vehicle.

  As described above, the image forming apparatus according to the first embodiment uses the light deflector to two-dimensionally deflect the light beam emitted from the light source element and to form a two-dimensional image on the scanned surface having transparency. A scanning device and a projection optical system including a convex mirror;

  Equipped with an optical scanning device, it is possible to set the divergence angle after the intermediate image (it is easy to control the divergence angle of the intermediate image), and highly efficient optical with little light loss in the optical system after the optical deflector A system can be realized. As a result of realizing a highly efficient optical system, a high brightness image can be obtained without using a large light source element. That is, by setting the divergence angle of the surface to be scanned to an appropriate value, it is possible to reduce the light loss and obtain a high brightness image.

  In addition, by providing a projection optical system including a convex mirror, for example, an intermediate image with a narrow divergence angle by laser scanning when a semiconductor laser is used as a light source element can be widened by a convex mirror. Therefore, it is possible to realize a large screen and a small size of the image forming apparatus.

  That is, by providing the optical scanning device and the projection optical system including the convex mirror, it is possible to simultaneously realize high brightness, large screen, and small size of the image forming apparatus.

  Note that it is difficult to achieve high brightness, large screen, and miniaturization at the same time in a panel type image forming apparatus that does not perform optical scanning (non-scanning type such as a liquid crystal panel and digital light processing). . This is because it is difficult to control the light divergence angle from the intermediate image so that no light loss occurs. In addition, in order to increase the brightness of a panel type image forming apparatus, a powerful light source that illuminates one screen in a comprehensive manner is necessary, and heat dissipation means such as a heat sink are practically used, which hinders downsizing. .

<Variation 1 of the first embodiment>
The first modification of the first embodiment shows an example of an optical scanning device in which the arrangement of optical elements is different from that of the first embodiment. In the first modification of the first embodiment, the description of the same components as those of the already described embodiment is omitted.

  FIG. 8 is a diagram illustrating an optical path of the optical scanning device according to the first modification of the first embodiment. FIG. 8 is a view of the optical scanning device 10A viewed from the same direction as FIG. However, in FIG. 8, the optical deflector 16, the concave mirror 17, and the scanned surface 18 are not shown in the same manner as in FIG. In the optical scanning device 10 </ b> A, the arrangement of the optical deflector 16, the concave mirror 17, and the scanned surface 18 is the same as that of the optical scanning device 10.

  Referring to FIG. 8, in the optical scanning device 10A, the light source element 11R, the coupling lens 12R, and the aperture 13R, the light source element 11G, the coupling lens 12G, and the aperture 13G, the light source element 11B, the coupling lens 12B, And the aperture 13B are juxtaposed so that the traveling directions of the respective light beams are substantially parallel.

  The points where the light beams shaped by the apertures 13R, 13G, and 13B are incident on the combining element 14 to be optically combined and the optical system after the combining element 14 are the same as those of the optical scanning device 10.

  As described above, the arrangement of the light source element, the coupling lens, the aperture, the synthesis element, and the like can be determined as appropriate. In the image forming apparatus 20, the optical scanning device 10 </ b> A can be used instead of the optical scanning device 10.

  Examples will be described below. Each embodiment is a design example of the first mirror 21, the second mirror 22, and the semi-transmissive mirror 23.

<Example 1>
FIG. 9 is a diagram illustrating an optical system according to the first embodiment. As shown in FIG. 9, the first embodiment is an example in which a convex mirror is used as the first mirror 21, a concave mirror is used as the second mirror 22, and a semi-transmissive mirror having a flat reflecting surface is used as the semi-transmissive mirror 23.

  In the first embodiment, the light beam emitted from the scanned surface 18 is incident on the first mirror 21 which is a convex mirror. The first mirror 21 which is a convex mirror enlarges the radiation angle, and the entire image forming apparatus 20 is enlarged. It has the effect of shortening the optical path length.

  In order for the driver to observe the magnified virtual image 25, the final power surface must have the power to focus the luminous flux. In the first embodiment, since the semi-transmissive mirror 23 is a flat surface, the second mirror 22 is a concave mirror, and the projection optical system as a whole has a positive power. According to the configuration of the first embodiment, the depth of the projection optical system (horizontal direction in FIG. 9) can be made close to the effective diameter of the semi-transmissive mirror 23.

  Tables 1 to 3 below show the optical data of Example 1.

Note that the image plane position of the virtual image 25 is 2 m away from the driver's eyeball 24. Further, the field angle of view of the virtual image 25 was 12 × 3 deg.

<Example 2>
FIG. 10 is a diagram illustrating an optical system according to the second embodiment. As shown in FIG. 10, the second embodiment is an example in which a convex mirror is used as the first mirror 21, a plane mirror is used as the second mirror 22, and a semi-transmissive mirror having a concave reflecting surface is used as the semi-transmissive mirror 23. In the present embodiment, the reflective surface of the semi-transmissive mirror 23 is a concave surface, but the surface opposite to the reflective surface is substantially parallel to the reflective surface. That is, the thickness of the semi-transmissive mirror 23 is substantially constant.

  In Example 2, the convex surface of the first mirror 21 is an anamorphic surface having a curvature in a predetermined direction and a curvature in a direction orthogonal to the curvature. By making the convex surface of the first mirror 21 an anamorphic surface, the curved surface shape of the convex surface can be adjusted, and the aberration correction performance can be improved.

  FIG. 11 is a diagram illustrating a transflective mirror according to the second embodiment. As shown in FIG. 11, in the semi-transparent mirror 23, the position of the deepest point 23c of the concave surface is shifted by about several tens of mm toward the projection optical system side with respect to the position of the optical center 23b of the concave surface. Here, the optical center 23 b is the center of gravity of the entire region 23 a that enters the viewer's field of view of the semi-transmissive mirror 23. The deepest point 23c is the most recessed portion in the entire region 23a that enters the observer's field of view of the semi-transmissive mirror 23.

  Thus, in Example 2, the observer side surface of the semi-transmissive mirror 23 is an eccentric surface. By making the surface on the observer side of the semi-transmissive mirror 23 an eccentric surface, light rays incident on the side of the semi-transmissive mirror 23 closer to the second mirror 22 and the second mirror 22 to the semi-transmissive mirror 23 are arranged. It is possible to balance the optical path with the light beam incident on the side far from the second mirror 22. As a result, distortion generated in the image forming apparatus 20 can be reduced.

  In the second embodiment, the first mirror 21, the second mirror 22, and the semi-transmissive mirror 23 as a whole are given positive power.

  Tables 4 to 6 below show optical data of Example 2.

Note that the image plane position of the virtual image 25 is 2 m away from the driver's eyeball 24. Further, the field angle of view of the virtual image 25 was 6 × 2 deg.

<Example 3>
FIG. 12 is a diagram illustrating an optical system according to the third embodiment. As shown in FIG. 12, the third embodiment is an example in which a concave mirror is used as the first mirror 21, a convex mirror is used as the second mirror 22, and a semi-transmissive mirror having a concave reflecting surface is used as the semi-transmissive mirror 23. In the present embodiment, the reflective surface of the semi-transmissive mirror 23 is a concave surface, but the surface opposite to the reflective surface is substantially parallel to the reflective surface. That is, the thickness of the semi-transmissive mirror 23 is substantially constant.

  In the third embodiment, the scanning surface 18 has a radiation angle of 10.5 degrees in the X direction and 3.5 degrees in the Y direction, and the scanning optical system is designed so as to coincide with it. The concave surface of the first mirror 21 is an anamorphic surface having a curvature in a predetermined direction and a curvature in a direction orthogonal to the curvature. By making the concave surface of the first mirror 21 an anamorphic surface, the curved surface shape of the concave surface can be adjusted, and the aberration correction performance can be improved.

  In the third embodiment, compared with the first and second embodiments, the radiation angle of the scanned surface 18 is designed wider. As a result, the optical path length from the scanned surface 18 to the semi-transmissive mirror 23 is shortened, and the height (longitudinal direction in FIG. 12) and depth (lateral direction in FIG. 12) are reduced from the scanned surface 18 to the semi-transmissive mirror 23. Can be stored below the size of the semi-transparent mirror 23.

  In the third embodiment, the first mirror 21, the second mirror 22, and the semi-transmissive mirror 23 as a whole are given positive power.

  Tables 7 to 9 below show the optical data of Example 3.

Note that the image plane position of the virtual image 25 is 2 m away from the driver's eyeball 24. Further, the field angle of view of the virtual image 25 was 6 × 2 deg.

  The preferred embodiment and its modifications and examples have been described in detail above, but the present invention is not limited to the above-described embodiment and its modifications and examples, and departs from the scope described in the claims. Without departing from the above, various modifications and substitutions can be made to the above-described embodiment and its modifications and examples.

  For example, in each of the embodiments and modifications thereof, an example in which the three light source elements 11R, 11G, and 11B are used in the optical scanning device 10 has been described. However, a single color image is formed using a single light source element. It is good also as a structure. In this case, the synthesis element 14 can be omitted.

  Moreover, although the passenger car was mentioned as an example of a vehicle, this invention is applicable also to other vehicles, such as an aircraft and a train.

10, 10A Optical scanning device 11R, 11G, 11B Light source element 12R, 12G, 12B Coupling lens 13R, 13G, 13B Aperture 14 Combining element 15 Lens 15a First surface 15 of lens 15b Second surface 15B, 15R of lens 15 16 Optical deflector 16d, 17d Deflection angle 17 Concave mirror 18 Scanned surface 18d Cross section of light beam 18h Normal line of scanned surface 20 Image forming device 21 First mirror 22 Second mirror 23 Transflective mirror 23a Region 23b Optical center 23c Deepest point 24 Driver's eyeball 25 Virtual image

JP 2010-145745 A JP 2010-145746 A

Claims (8)

  1. An optical scanning device that two-dimensionally deflects a light beam emitted from a light source element with an optical deflector and forms a two-dimensional image on a scanned surface having transparency;
    A projection optical system for enlarging and projecting the two-dimensional image on a projection surface;
    The projected surface is a reflecting surface of a semi-transmissive mirror that is provided outside and transmits a part of visible light and reflects a part thereof.
    The scanned surface is a diffusing plate that diffuses incident light toward its traveling direction side,
    An image forming apparatus in which a cross-sectional shape of light diffused by the diffusion plate is an ellipse.
  2. An optical scanning device that two-dimensionally deflects a light beam emitted from a light source element with an optical deflector and forms a two-dimensional image on a scanned surface having transparency;
    A transflective mirror that transmits part of visible light and reflects part of it,
    A projection optical system for enlarging and projecting the two-dimensional image onto the reflecting surface of the semi-transmissive mirror,
    The scanned surface is a diffusing plate that diffuses incident light toward its traveling direction side,
    An image forming apparatus in which a cross-sectional shape of light diffused by the diffusion plate is an ellipse.
  3.   The image forming apparatus according to claim 1, wherein a reflection surface of the semi-transmissive mirror is a concave surface, and a position of a deepest point of the concave surface is on the projection optical system side with respect to a position of an optical center of the concave surface.
  4. An enlarged virtual image of the two-dimensional image is formed at a predetermined position on the opposite surface side of the reflecting surface of the semi-transmissive mirror,
    4. The image forming apparatus according to claim 1, wherein a major axis direction of an ellipse of light diffused by the diffusion plate coincides with a longitudinal direction of the virtual image.
  5.   The image forming apparatus according to claim 1, wherein the projection optical system includes a convex mirror.
  6.   The image forming apparatus according to claim 5, wherein the convex mirror is disposed immediately after the surface to be scanned.
  7.   The image forming apparatus according to claim 1, wherein the surface to be scanned is disposed at a position where a normal line of the surface to be scanned does not intersect the semi-transparent mirror.
  8. An image forming apparatus according to claim 1 is mounted,
    The semi-transparent mirror is integrated with the front window,
    A vehicle in which a driver can visually recognize an enlarged virtual image of the two-dimensional image at a predetermined position ahead of the reflecting surface of the semi-transmissive mirror.
JP2017044501A 2017-03-09 2017-03-09 Image forming apparatus, and vehicle having image forming apparatus mounted thereon Pending JP2017142509A (en)

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JPH06270716A (en) * 1993-03-18 1994-09-27 Kansei Corp Head-up display device for vehicle
JPH09133887A (en) * 1995-11-08 1997-05-20 Toppan Printing Co Ltd Light beam deflecting optical device
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WO2019116730A1 (en) * 2017-12-11 2019-06-20 パナソニックIpマネジメント株式会社 Head-up display and moving body with head-up display mounted thereon

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