Technical Field
The present invention relates to a scanning projector transmissive screen.
Related Art
A scanning projector combines laser beams of R, G and B colors subjected to brightness modulation into one beam, and makes them scan on a screen in synchronization with the brightness modulation to form a two-dimensional image on the screen. The scanning projector has a characteristic feature that it is easy to provide high resolution, downsizing and low power consumption compared to a method of projecting two-dimensional images.
By virtue of these characteristic features, the scanning projector is used in practice in an in-vehicle head-up display. Here, the head-up display is a device which displays information such that the information is superposed on a background ahead of a line of sight.
The transmissive screen 300 is a transparent or semitransparent member formed into a rectangular shape, and is provided with microlens arrays 301 composed of multiple microlenses formed on a surface of the transmissive screen 300 at a side of the scanning projector 400. This is to widen a viewing angle by widening a beam transmitting through the transmissive screen 300.
An image (i.e., an intermediate image) projected on the transmissive screen 300 by the scanning pro jector 400 is entered into a magnifying glass 320 via the field lens 310. Further, the image is reflected on the magnifying glass 320, and is projected onto the windshield 330 and recognized by driver's eyes located in an eye box. Here, in place of the windshield 330, a transmissive screen mechanism which is referred to as a combiner, may be provided separately to project images.
As shown in
A diffusion range of the light can be adjusted by changing a curvature of the microlens; however, inhomogeneity of the brightness at the center portion and the end portion cannot be resolved. Hence, to address this problem, the field lens 310 is positioned near the light emission side of the transmissive screen 300 to change the traveling direction of the diffused light at the end portion to be inward, as illustrated in
Patent Literature 1: JP 2010-145924 A
Since a display device using the scanning projector, in particular the head-up display, is configured to project images on the windshield, a projecting unit for performing the projection needs to be housed in a dashboard and such of a vehicle. Meanwhile, a driving mechanism such as a handle and display mechanisms such as a meter and a warning light are arranged inside the dashboard, and thus an installation space for the projector unit is very limited. Consequently, it is preferable that the number of components included in the display device using the scanning projector is small.
As described above, by disposing the field lens 310 near the transmissive screen 300 on which the microlens arrays are formed, it is possible to obtain the images which are entirely clear. However, this results in an increase in the number of components, which is not preferable in view of a size of a housing and an increase in the cost.
It is therefore an object of the present invention to provide a display device using a scanning projector which can obtain images which are entirely clear without increasing the number of components.
To solve the above problem, a scanning projector transmissive screen according to the present invention includes a first surface on which a microlens array is formed, and a second surface formed into a single lens shape. Light that has emitted from the scanning projector and then entered to the transmissive screen for the scanning projector is diffused inside the transmissive screen in a traveling direction corresponding to an incident angle due to the microlens arrays formed on an incident surface. That is, for the light perpendicularly entering to a central portion of the transmissive screen, the light is diffused around the perpendicular direction, but as it gets closer to an end portion of the transmissive screen, the traveling direction of the diffused light spreads outward. The traveling direction of the diffused light is changed to more inward as it gets closer to the end portion by a function of a single lens formed on an emission surface when the diffused light is emitted from the transmissive screen. That is, the transmissive screen for the scanning projector according to the present invention has functions of both of the conventional transmissive screen and a lens arranged near the conventional transmissive screen. Consequently, there is no need to provide a separate lens, thereby reducing the number of components. The single lens shape may form a convex lens. Consequently, the traveling direction of the diffused light can be changed to inward as it gets closer to the end portion. In this case, the single lens shape may form a Fresnel lens. Consequently, thickness of the transmissive screen can be reduced. The single lens shape may forma concave lens. Consequently, the traveling direction of the diffused light can be changed to outward as it gets closer to the end portion.
According to the present invention, there is provided a display device using a scanning projector which can obtain images which are entirely clear without increasing the number of components.
An embodiment of the present invention will be described in detail with reference to the drawings.
The scanning projector 100 includes a red laser light source 110R, a green laser light source 110G and a blue laser light source 110B as light sources, and each light source (110R, 110G and 110B) is subjected to an intensity homogenization and collimation as needed and performs and emits laser light. is subjected to an intensity homogenization and collimation as needed and performs and emits laser light.
The respective emitted lights pass through collective lenses (112R, 112G and 112B) arranged on optical axes near the light sources (110R, 110G and 110B), and thereby providing a convergent light. The convergent lights of three R, G and B colors are combined into one convergent light within the scanning projector 100.
In the example shown in
The synthetic light is bent by a mirror 120 for downsizing, and then an irradiation direction thereof is controlled by a high-speed two-dimensional scanning element 130 to scan the synthetic light in two-dimension. The high-speed two-dimensional scanning element 130 may include a two-dimensional scanning MEMS mirror; however, a vertical scanning MEMS mirror and a horizontal scanning MEMS mirror may be combined and used. Alternatively, a galvanometer mirror may be used as the high-speed two-dimensional scanning element 130.
The MEMS mirror is an optical scanning device produced using a MEMS (Micro Electro Mechanical System) technology, and a movable mirror 130a performs the optical scanning by making reciprocating rotation movement at a predetermined angle around a predetermined rotation axis 130b in a scanning direction. The rotation axis 130b may be defined by a mechanical shaft or may be defined virtually without providing a definite shaft. As the MEMS mirrors, various methods may be employed such as an electromagnetic type moving coil type, an electromagnetic type moving magnet type, an electrostatic type and a piezo type which have been proposed.
The transmissive screen 200 having a rectangular shape is arranged on a light-focusing surface of the synthetic light. The R, G and B synthetic light subjected to brightness modulation per pixel is scanned through the screen 200 at a high speed, thus the two-dimensional image is perceived as a result of an afterimage effect of eyes.
In the present embodiment, the transmissive screen 200 is provided with a microlens array 201 formed on a surface thereof on the side of the scanning projector 100. The microlens array 201 is composed of multiple microlenses . A single lens 202 is formed on an opposite side of the transmissive screen 200. In the shown example, a convex lens is formed as the single lens 202.
According to this configuration, the light entered to the transmissive screen 200 is diffused inside the transmissive screen 200 in a traveling direction corresponding to an incident angle due to the microlens arrays 201 formed on an incident surface. That is, for the light perpendicularly entering to a central portion of the transmissive screen 200, the light is diffused around the perpendicular direction, but as it gets closer to an end portion of the transmissive screen 200, the traveling direction of the diffused light spreads outward.
The traveling direction of the diffused light is changed to more inward as it gets closer to the end portion by a function of the convex lens of the single lens 202 formed on an emission surface when the diffused light is emitted from the transmissive screen 200, thereby an irradiation range is narrowed. That is, the transmissive screen 200 according to this embodiment has functions of both of the conventional transmissive screen 300 and the field lens 310 arranged near the conventional transmissive screen 300. Consequently, there is no need to provide the field lens 310, and the number of components can be reduced.
As described above, in this embodiment, the traveling direction of the diffused light is changed at the end portion in a long-side direction, thus the screen 200 is formed into a cylinder shape having the convex surface in the long-side direction. This is because the scan range is wider in the long-side direction than in the short-side direction, and thus the incident angle of the light is greater at the end portion.
To change the traveling direction of the diffused light in the short-side direction, a cylinder shape having the convex surface in the short-side direction is provided. To change the traveling direction of the diffused light in both of the long-side and short-side directions, a toroidal shape having the convex surfaces in the long-side direction and the short-side direction is provided.
An image (i.e., an intermediate image) projected on the transmissive screen 200 in such manner enters a magnifying glass 220, is projected on a windshield 230, and is recognized by driver's eyes located in an eye box.
Light from the end portion of the transmissive screen 200 sufficiently enters the magnifying glass 220, thus the images which are entirely clear can be recognized in the eye box. In this case, a field lens which was conventionally required is no longer required. Consequently, the images which are entirely clear can be obtained without increasing the number of components.
In addition, the single lens formed on the transmissive screen may be a Fresnel lens. By using the Fresnel lens, the thickness can be thinner, thereby providing further space saving.
In this case, to prevent a defect in display caused by vertical walls of the Fresnel, it is preberable that a group of beams entered from a given one microlens is emitted from one Fresnel surface. For example, as shown in
Here, if a horizontal distance between the light source P0 and the microlens 261a is D0, a thickness of the transmissive screen 260 is D1, a boundary of the microlens 261a to which the beam 1 enters is P1, a boundary of the Fresnel surface 262a from which the beam 1 is emitted is P2, an emission angle of the beam is θ0, and an incident angle and an emission angle of the beam onto the microlens 261a are θ1 (which is known based on a lens radius and a lens pitch) and θ2, respectively, then, a vertical direction distance S0 between P0 and P1, a vertical direction distance S1between P1 and P2, and a vertical direction distance S2 between P0 and P2 can be calculated as follows:
S0=D0 tan θ0
S
1
=D
1 tan θ2, where θ2=sin−1(n1/n0) sin θ1)
S
2
=S
0
−S
1.
Where, n0 is a refractive index of air, and n1 is a refractive index of a material of the transmissive screen 260.
Positions of P3 and P4 can also be calculated in the same manner. Thus, based on the respective positions of P1, P2, P3 and P4, it is possible to determine a positional relationship between one microlens 261a and the corresponding Fresnel surface 262a.
The embodiments of the present invention have been described above. However, the transmissive screen according to the present invention is not limited to the above embodiments, and can be modified in various ways within the scope of the present invention. For example, in the examples shown herein, the convex lens is formed as the single lens at the opposite side of the microlens arrays formation surface. However, as illustrated in
Number | Date | Country | Kind |
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2015-207891 | Oct 2015 | JP | national |