This application claims priority under 35 U.S.C. Section 119 of Japanese Patent Application No. 2007-110962 filed Apr. 19, 2007, entitled “ILLUMINATION DEVICE AND PROJECTION VIDEO DISPLAY DEVICE”, and Japanese Patent Application No. 2007-292217 filed Nov. 9, 2007, entitled “ILLUMINATION DEVICE AND PROJECTION VIDEO DISPLAY DEVICE”.
1. Field of the Invention
The present invention relates to an illumination device and a projection video display device, and more particularly to an illumination device having a plurality of light sources, and a projection video display device incorporated with the illumination device.
2. Disclosure of the Related Art
As a large-screen display device is spread in recent years, a technology of securing high luminance of illumination light is required in a projection video display device (hereinafter, called as a “projector”). As one approach for securing high luminance, there is proposed a multi-lamp arrangement in an illumination device. For instance, there is known a four-lamp illumination device incorporated with four lamps as an emission light source.
In the four-lamp illumination device, for instance, as shown in
In the above arrangement, as shown in
If, however, the light beams from the lamps are directed in a direction closer to the optical axis direction of the illumination device, a part of the light beams from the lamps, which is not reflected on the corresponding mirror, may be increased, thereby causing a drawback that the light use efficiency may be lowered.
The light amount of illumination light can be increased by increasing the number of lamps i.e. by providing a multi-lamp arrangement. However, as the multi-lamp arrangement is provided by simply arranging a multitude of lamps, the area (illumination area) of light beams to be emitted from the illumination device may be increased, as the number of lamps is increased. As a result, the light use efficiency may be lowered according to Etendue theory as follows.
A value obtained by Etendue theory i.e. an Etendue value is obtained by a product of a spread angle i.e. a stereoscopic angle of light flux, and an effective light flux area. Referring to
E=2nS (1−cos θ) (1)
where 2n(1−cos θ) in the expression (1) is a stereoscopic angle of light flux. The Etendue value (E) is calculated in the similar manner as described above, in the case where light is converged as shown in
In an ideal optical system, the Etendue value is retained. However, in an actual optical system, as light propagates, the Etendue value is increased. In a projector incorporated with a liquid crystal panel, if the Etendue value of an illumination device is smaller than the Etendue value of a panel surface, it is possible to guide all the light beams from the illumination device to the panel surface. However, if the Etendue value of the illumination device is larger than the Etendue value of the panel surface, the light use efficiency of the illumination device is decreased.
In the case where the area of the panel surface, and the light incident angle are fixed, if the area of light flux in the illumination device is increased, the Etendue value of the illumination device is increased, as the light flux area is increased. As a result, the light use efficiency i.e. the light incident amount on the panel surface is decreased. In other words, the above arrangement may make it difficult or impossible for light beams to be incident onto the liquid crystal panel with a dispersion angle larger than the effective dispersion angle with respect to the liquid crystal panel.
As described above, as the light flux area in the illumination device is increased, the light use efficiency of the panel surface may be lowered. Accordingly, even if the multi-lamp arrangement is actively adopted to increase the light amount of illumination light, an increased light amount of illumination light may increase the light flux area. An increased light flux area in the illumination device may obstruct effective incidence of illumination light having an increased light amount onto the panel. As a result, an increase in the luminance of a projection image may not be advantageously obtained.
There rises another drawback in addition to the above drawback on the light use efficiency. Specifically, the contrast of a projection image may be lowered, because a convergence angle of illumination light at the time of light incidence onto the panel is increased, as the area of illumination light flux is increased. In view of the above drawbacks, it is necessary to provide a certain constraint on increasing the area of illumination light flux.
A primary object of the invention is to secure high luminance by a multi-lamp arrangement, while keeping high light use efficiency.
An illumination device according to a first aspect of the invention comprises a first light source unit including a plurality of first light sources, a first reflection unit for guiding light beams emitted respectively from the first light sources in an identical direction, and a second light source unit including at least one second light source. Assuming a plane perpendicular to a propagating direction of the light beams emitted from the first light source unit and reflected on the first reflection unit, a center of an optical axis of the second light source is defined in an area surrounded by centers of optical axes of the first light sources, on the plane. The area is an area where a light amount distribution of the light beams from the first light sources is relatively small. In the above arrangement, by defining the optical axis center of the second light source in the area to compensate for the light amount, the light amount of illumination light can be increased while suppressing an increase in the area of illumination light flux.
An illumination device according to a second aspect of the invention comprises four first light sources, a reflection unit including four mirror surfaces for guiding light beams emitted respectively from the four first light sources in an identical direction, and a second light source. Each of the four mirror surfaces is arranged at such a position that a center of an optical axis of the corresponding first light source is aligned with a position of a vertex of a predetermined rectangle, assuming that the rectangle is defined on a plane perpendicular to a propagating direction of the light beams emitted from the first light sources and reflected on the respective corresponding mirror surfaces. A center of an optical axis of the second light source is aligned with a center position of the rectangle. The center position of the rectangle has a relatively small light amount distribution of the light beams from the first light sources. In the above arrangement, by aligning the optical axis center of the second light source with the center position of the rectangle to compensate for the light amount, the light amount of illumination light can be increased while suppressing an increase in the area of illumination light flux.
A projection video display device according to a third aspect of the invention comprises an illumination device for emitting light beams, and a light modulation unit for modulating the light beams in accordance with an input video signal to generate modulated image light beams. The illumination device includes a first light source unit having a plurality of first light sources, a first reflection unit for guiding light beams emitted respectively from the first light sources in an identical direction, and a second light source unit having at least one second light source. Assuming a plane perpendicular to a propagating direction of the light beams emitted from the first light source unit and reflected on the first reflection unit, a center of an optical axis of the second light source is defined in an area, on the plane, where a light amount distribution of the light beams from the first light sources is relatively small. The area is surrounded by centers of optical axes of the first light sources. Similarly to the illumination device according to the first aspect, the illumination device according to the third aspect enables to increase the light amount of illumination light while suppressing an increase in the area of illumination light flux. Thus, the projection video display device according to the third aspect enables to effectively secure high luminance for a projection image.
The foregoing and other objectives and novel features of the present invention will be more fully understood by reading description of a preferred embodiment in combination with the attached drawings as follows:
The drawings are provided mainly for describing the present invention, and do not limit the scope of the present invention.
In the following, embodiments of the invention are described referring to the drawings.
The first embodiment is directed to a projector as an example of an illumination device embodying the invention.
Light beams from the illumination device 10 are incident onto a PBS (polarized beam splitter) array 12 and a condenser lens 13 via an integrator 11. The integrator 11 includes a first integrator lens and a second integrator lens having fly-eye lenses, and imparts a lens function to the light beams to be incident from the illumination device 10 in such a manner that the light amount distribution of light beams to be incident onto liquid crystal panels 18, 24, and 33 is substantially made uniform. The PBS array 12 is formed by arranging a plurality of polarized beam splitters and half-wavelength plates in an array pattern, and is adapted to align polarization directions of light beams incident from the integrator 11 in an identical direction. The condenser lens 13 imparts a condensing function to light beams incident from the PBS array 12. Light beams transmitted through the condenser lens 13 are incident onto a dichroic mirror 14.
The dichroic mirror 14 transmits solely light beams (hereinafter, called as “R beams”) having a wavelength band corresponding to red, and reflects light beams (hereinafter, called as “B beams”) having a wavelength band corresponding to blue, and light beams (hereinafter, called as “G beams”) having a wavelength band corresponding to green, among the light beams incident from the condenser lens 13. The R beams transmitted through the dichroic mirror 14 are reflected on a mirror 15, and then incident onto a condenser lens 16.
The condenser lens 16 imparts a lens function to the R beams in such a manner that the R beams are incident onto the liquid crystal panel 18 as substantially parallel beams. The R beams transmitted through the condenser lens 16 are incident onto the liquid crystal panel 18 via an incident-side polarizer 17. The liquid crystal panel 18 is driven in accordance with a video signal for red color, and modulates the R beams depending on a driving condition of the liquid crystal panel 18. The R beams modulated by the liquid crystal panel 18 are incident onto a dichroic prism 20 via an output-side polarizer 19.
G beams among the light beams reflected on the dichroic mirror 14 are reflected on a dichroic mirror 21, and then incident onto a condenser lens 22. The condenser lens 22 imparts a lens function to the G beams in such a manner that the G beams are incident onto the liquid crystal panel 24 as substantially parallel beams. The G beams transmitted through the condenser lens 22 are incident onto the liquid crystal panel 24 via an incident-side polarizer 23. The liquid crystal panel 24 is driven in accordance with a video signal for green color, and modulates the G beams depending on a driving condition of the liquid crystal panel 24. The G beams modulated by the liquid crystal panel 24 are incident onto the dichroic prism 20 via an output-side polarizer 25.
B beams transmitted through the dichroic mirror 21 are incident onto a condenser lens 26. The condenser lens 26 imparts a lens function to the B beams in such a manner that the B beams are incident onto the liquid crystal panel 33 as substantially parallel beams. The B beams transmitted through the condenser lens 26 propagate along an optical path defined by relay lenses 27, 29, and 31, and two mirrors 28 and 30 for optical path length adjustment, and then incident onto the liquid crystal panel 33 via an incident-side polarizer 32. The liquid crystal panel 33 is driven in accordance with a video signal for blue color, and modulates the B beams depending on a driving condition of the liquid crystal panel 33. The B beams modulated by the liquid crystal panel 33 are incident onto the dichroic prism 20 via an output-side polarizer 34.
The dichroic prism 20 combines the light beams modulated by the liquid crystal panels 18, 24, and 33 for incidence onto a projection lens 35. Light beams (hereinafter, called as “modulated image light beams”) obtained by combination by the dichroic prism 20 are enlarged and projected on the projection screen by the projection lens 35.
In the following, an arrangement of the illumination device 10 is described referring to
As shown in
Light beams emitted from the lamps 101 through 104 are reflected in an identical direction i.e. Y-axis direction by the mirrors 111 through 114, respectively. The mirror 111, 112, 113, 114 has a pentagonal shape obtained by cutting away one vertex portion of a rectangle. As shown in
The optical axis of the lamp 101, 102, 103, 104 is bent by 90° by the mirror 111, 112, 113, 114, respectively. The bent optical axis (hereinafter, called as “illumination optical axis”) of the lamp 101, 102, 103, 104 is aligned with e.g. a position of a vertex of a rectangle. The lamp 105 is arranged at such a position that the optical axis of the lamp 105 is aligned with the center of the rectangle i.e. the optical axis center of the illumination device 10.
As the illumination optical axis of the lamp 101, 102, 103, 104 approaches the optical axis center of the illumination device 10, the light amount of the vicinity area of the optical axis center is increased, and the incident light amount with respect to the projection lens 35 is increased. Despite the advantage, however, as the illumination optical axis of the lamp 101, 102, 103, 104 approaches the optical axis center of the illumination device 10, the light amount of light beams incident onto the cutaway portion of the mirror 111, 112, 113, 114 among the light beams from the lamp 101, 102, 103, 104 is increased, and the light use efficiency of the lamp 101, 102, 103, 104 is decreased. In other words, there is a trade-off relation between the incident light amount with respect to the projection lens 35, and the light use efficiency of the lamp 101, 102, 103, 104, in the case where the illumination optical axis of the lamp 101, 102, 103, 104 approaches the optical axis center of the illumination device 10. In view of the above, the lamps 101 through 104, and the mirrors 111 through 114 are arranged at respective optimum positions thereof, considering the trade-off relation.
In the modification shown in
In the modification shown in
In the modification shown in
In the following, light emission control operations to be performed by the illumination device 10 are described referring to
As compared with the case where all the five lamps 101 through 105 are turned on (see
In the case where the projector is used in a full-time light-on condition, for instance, only the middle lamp 105 is turned on in a standby mode when the user does not gaze at a projection image (see
Alternatively, the illumination device 10 in the first embodiment may be modified into a hybrid illumination system.
In the modification shown in
In the hybrid illumination system, as shown in
In the modifications shown in
Alternatively, as shown in
As described above, according to the first embodiment, the center of the optical axis of the lamp 105 is defined in an area where the light amount distribution is relatively small on a plane (X-Z plane in
In the first embodiment, light beams from the lamp 105 are guided to a center position of illumination light flux, where a sufficient light amount has not been secured by a four-lamp arrangement constituted of the lamps 101 through 104. The first embodiment is advantageous in effectively increasing the light amount of a central portion of illumination light flux. Accordingly, illumination light can be projected with a lower dispersion angle, and the incident light amount with respect to the projection lens 35 can be increased. Thus, high luminance for a projection image can be effectively obtained.
In the first embodiment, the area of illumination light flux is substantially the same as in the four-lamp arrangement constituted of the lamps 101 through 104. Accordingly, there is no likelihood that the convergence angle of light beams to be incident onto the liquid crystal panel 18, 24, 33 may be unduly increased. Thus, as compared with the four-lamp arrangement constituted of the lamps 101 through 104, there is no likelihood that the contrast of a projection image may be degraded.
As described above, the first embodiment is advantageous in effectively securing high luminance for a projection image by addition of a lamp, while keeping the light use efficiency, and simultaneously suppressing lowering of the contrast in a projection image.
In the first embodiment, the lamps 101 through 105 are arranged at such a position that the optical axis of the lamp 105 perpendicularly intersects with the optical axes of the lamps 101 through 104. In the case where the optical axes of the lamps are not aligned in parallel to each other as described above, the arrangement pattern of the illumination device 10 may be limited, and at the same time, there arises a drawback that the usage pattern of the projector may be limited.
For instance, in the arrangement of the first embodiment, if the illumination device 10 is arranged at such a position that X-Z plane in
In the second embodiment, lamps 101 through 105 are arranged at such a position that the optical axes thereof are aligned in parallel to each other to solve the above drawback.
As shown in
Light beams emitted from the lamps 101 through 105 are reflected in an identical direction i.e. Y-axis direction by the mirrors 111 through 115, respectively. Similarly to the first embodiment, the mirror 111, 112, 113, 114 has a pentagonal shape obtained by cutting away one vertex portion of a rectangle. As shown in
The optical axis of the lamp 101, 102, 103, 104 is bent by 90° by the mirror 111, 112, 113, 114, respectively. Similarly to the first embodiment, the bent optical axis of the lamp 101, 102, 103, 104 is aligned with e.g. a position of a vertex of a rectangle. The mirror 115 is arranged at such a position that the optical axis of the lamp 105 is aligned with the center of the rectangle i.e. the optical axis center of the illumination device 10.
Unlike the arrangement shown in
In the second embodiment, the lamps 101 through 105 are arranged at such a position that the optical axes thereof are aligned in parallel to each other. Accordingly, even if the illumination device 10 is arranged at such a position that X-Z plane (see
In the first and the second embodiments, the lamps 101 and 103 are arranged to have the light emission directions opposite to those of the lamps 102 and 104. In the third embodiment, lamps 101 through 104 are arranged at such a position that the light emission directions thereof are identical to each other.
As shown in
Unlike the arrangement shown in
In the above arrangement, light beams in the vicinity area of the optical axis center of the illumination device 10 among the light beams reflected on the mirror 116 are blocked by a mirror portion 117a of the mirror 117. Light beams emitted from the lamp 105 are reflected on the mirror portion 117a and guided to the vicinity area of the optical axis center of the illumination device 10. The mirror portion 117a is formed in the middle of the mirror 117, and an outer portion of the mirror 117 other than the mirror portion 117a is transparent.
In the third embodiment, the lamps 101 through 104 are arranged on an identical plane i.e. Y-Z plane in such a manner that all of the lamps 101 through 104 are directed in an identical direction i.e. X-axis direction. Accordingly, as compared with the first and the second embodiments, the third embodiment is advantageous in reducing the size of the illumination device 10 in X-axis direction. Also, since the mirror 116 is provided as means for reflecting light from the lamps 101 through 104, the third embodiment is advantageous in simplifying the arrangement of the illumination device 10 and reducing the number of parts constituting the illumination device 10. Also, in the modification shown in
In the fourth embodiment, one or more lenses are arranged on an optical path for transmitting light beams emitted from a lamp 105 to reduce the beam diameter of light from the lamp 105.
As shown in
In the above arrangements, since the beam diameter of light from the lamp 105 is reduced by the convex lens 118a and the concave lens 118b, the size of cutaway portions of mirrors 111 through 114 can be reduced. Thereby, the light use efficiency of lamps 101 through 104 can be enhanced.
In the foregoing embodiments, the five lamps 101 through 105 are provided in the illumination device 10. The number of lamps is not limited to five, but lamps of a certain number other than five may be provided in the illumination device 10. Although an increased number of lamps enables to increase the light amount of illumination light, the increased number of lamps may increase the number of parts and the production cost. Also, a measure on the arrangement pattern of lamps and mirrors should be provided, or a countermeasure for preventing an increase in size of the illumination device should be provided. On the other hand, a reduced number of lamps enables to reduce the number of parts and the production cost, and reduce the size of the illumination device. However, the reduced number of lamps may cause a drawback that the light amount of illumination light may be lowered.
In the following, arrangements (fifth to seventh embodiments) in the case where the number of lamps is changed are described.
In the fifth embodiment, the number of lamps is reduced from five to four.
As shown in
Light beams emitted from the lamps 201 through 203 are reflected in an identical direction i.e. Y-axis direction by the mirrors 211 through 213, respectively. The mirror 211, 212 has a pentagonal shape obtained by cutting away one vertex portion of a rectangle. As shown in
In the fifth embodiment, since the number of lamps is reduced by one, as compared with the first embodiment, the number of parts and the production cost can be reduced, and the size of the illumination device can be reduced. In the fifth embodiment, however, the light amount of illumination light may be lowered, as compared with the first embodiment, as the number of lamps is reduced.
In the arrangement shown in
In the sixth embodiment, the number of lamps is increased from five to seven.
As shown in
Light beams emitted from the lamps 301 through 306 are reflected in an identical direction i.e. Y-axis direction by the mirrors 311 through 316, respectively. The mirror 311, 312, 315, 316 has a pentagonal shape obtained by cutting away one vertex portion of a rectangle. As shown in
In the sixth embodiment, since the number of lamps is increased by two, as compared with the first embodiment, the light amount of illumination light can be increased. However, since the number of lamps and the number of mirrors are increased by two, respectively, the production cost may be increased, and the size of the illumination device may be increased by the increased numbers of lamps and mirrors. The lamp 307 may be arranged at such a position that the light emission direction thereof is aligned in X-axis direction, by providing a mirror, in the similar manner as the lamp 105 described in the second embodiment referring to
In the seventh embodiment, the number of lamps is increased from five to eight.
As shown in
Light beams emitted from the lamps 301 through 308 are reflected in an identical direction i.e. Y-axis direction by the mirrors 311 through 318, respectively. The mirror 311, 312, 315, 316 has a pentagonal shape obtained by cutting away one vertex portion of a rectangle. The mirror 313, 314 has a pentagonal shape obtained by cutting away two vertex portions of a rectangle. As shown in
In the seventh embodiment, since the number of lamps is increased by three, as compared with the first and the second embodiments, the light amount of illumination light can be increased. However, since the number of lamps and the number of mirrors are increased, the production cost may be increased, and the size of the illumination device may be increased by the increased numbers of lamps and mirrors. In the arrangement shown in
In the eighth embodiment, a prism array is provided, in place of a mirror, to guide light beams from lamps to an illumination system. The prism array to be used in the eighth embodiment may be the one recited in WO2004/088413.
Light beams emitted from the lamps 401 through 404 are reflected in an identical direction i.e. Y-axis direction by the corresponding prism array 411, 412. The prism array 411, 412 has a rectangular cutaway portion 411a, 412a, which is formed in the middle of one side of a rectangle. As shown in
As shown in
Light beams emitted from the lamps 401 through 404 are reflected on the corresponding prism array 431, 432 in an identical direction i.e. Y-axis direction, respectively. Also, light beams emitted from the lamps 405 and 406 are reflected on the mirrors 433 and 434 in an identical direction i.e. Y-axis direction, respectively.
As shown in
In the arrangement shown in
As shown in
In the following, configuration examples of an optical system in the case where Ye beams are superimposed on modulated image light beams are described. In the following configuration examples, elements substantially identical or equivalent to those in the foregoing embodiments are indicated with the same reference numerals, and description thereof will be omitted herein.
In the following configuration examples, the five-lamp illumination device shown in
First, an illumination device 10 is described. As described above, in Configuration Example 1, the five-lamp illumination device shown in
The UV cutoff filter 121, 122, 123, 124, 125 is arranged in the vicinity of an exit end of a lamp 101, 102, 103, 104, 105 respectively to cut off ultraviolet rays included in light beams emitted from the lamp 101, 102, 103, 104, 105. The ultraviolet rays are unwanted light which should not be superimposed on modulated image light beams. Because of a short wavelength, the ultraviolet rays may likely adversely affect optical components. In view of the above, in the arrangement of
The aperture 126 is adapted to control the beam shape of light to be emitted from the lamp 105 in such a manner that the light from the lamp 105 may not impinge on the backside surface of a mirror 111, 112, 113, 114. If the aperture 126 is not provided, light from the lamp 105 may be reflected on the backside surface of the mirror 111, 112, 113, 114, and incident onto one of the lamps 101 through 104, which may shorten the life of the corresponding lamp. In view of the above drawback, in the arrangement shown in
In the following, an arrangement from an integrator 11 to a projection lens 35 is described. Configuration Example 1 is different from the arrangement shown in
In Configuration Example 1, the dichroic mirror 43 is modified in such a manner as to reflect G beams and Ye beams, and transmit B beams. The incident-side polarizers 45, 49, and 52, and the output-side polarizers 47, 51, and 54 each has a two-piece construction. Use of the two-piece construction for the polarizers enables to prevent damage of the polarizers.
Specifically, in Configuration Example 1, the light amount of light to be emitted from the illumination device 10 is considerably increased, as described above. As a result, the light amount of light to be incident onto the incident-side polarizer and the output-side polarizer arranged in front of and behind liquid crystal panel 18, 24, 33 may be increased. The increased light amount of light to be incident onto the polarizer may increase the light amount of light to be absorbed by the polarizer at the time light transmits through the polarizer. Consequently, a large exothermic heat may be generated by the light absorption. If the polarizer is constituted of one polarizing piece, the large exothermic heat may damage the polarizer. In particular, a considerably large amount of exothermic heat may be generated in a polarizer for transmitting B beams having a short wavelength, and it is highly likely that the polarizer may be damaged. In order to avoid the drawback, in Configuration Example 1, the incident-side polarizers 45, 49, and 52, and the output-side polarizers 47, 51, and 54 each have a two-piece construction to prevent damage of the polarizer by the exothermic heat.
Specifically, concerning the two polarizing pieces constituting each of the incident-side polarizers 45, 49, and 52, and the output-side polarizers 47, 51, and 54, one of the polarizing pieces away from a dichroic prism 20 is adapted to roughly align the polarization direction, and the other one of the polarizing pieces closer to the dichroic prism 20 is adapted to finely align the polarization direction. This arrangement enables to release the exothermic heat generated in the polarizer, thereby preventing damage of the polarizer.
In addition to the above, half wavelength plates (not shown) for rotating the polarization directions of R beams and B beams by 90 degrees are provided for the incident-side polarizer 45 for R beams, and the incident-side polarizer 52 for B beams, respectively. In the above arrangement, R beams and B beams are incident onto the reflection plane of the dichroic prism 20 as S-polarized beams, thereby enhancing the reflection efficiency of R beams and B beams with respect to the dichroic prism 20. A half wavelength plate is not provided for the incident-side polarizer 49 for G beams (and Ye beams). Accordingly, G beams (and Ye beams) are incident onto the reflection plane of the dichroic prism 20 as P-polarized beams, thereby enhancing the transmission efficiency of G beams (and Ye beams) with respect to the dichroic prism 20.
In the arrangement shown in
The light beams reflected on the dichroic mirror 14 are incident onto the dichroic mirror 43 via the condenser lens 42. The dichroic mirror 43 transmits B beams, and reflects G beams and Ye beams, among the incident light beams. The B beams transmitted through the dichroic mirror 43 are incident onto the dichroic prism 20 via the optical elements from a condenser lens 26 to the output-side polarizer 54. In the process, ultraviolet rays that could not be cut off by the UV cutoff filters 121 through 125 in the illumination device 10 are cut off by the UV cutoff filter 44.
The G beams and the Ye beams reflected on the dichroic mirror 43 are incident onto the Ye superimposing element 48. The Ye superimposing element 48 acts only on the Ye beams among the G beams and the Ye beams, and rotates the polarization direction of Ye beams in accordance with an applied voltage. Thereby, the light amount of Ye beams to be superimposed on modulated image light beams is adjusted. The Ye beam superimposing operation to be performed by the Ye superimposing element 48 is described later referring to
The G beams and the Ye beams transmitted through the Ye superimposing element 48 are incident onto the dichroic prism 20 via the optical elements from a condenser lens 22 to the output-side polarizer 51.
As described above, R beams, G beams, Ye beams and B beams that have been incident onto the dichroic prism 20 are combined into modulated image light beams by the dichroic prism 20. The modulated image light beams are projected on a projection plane i.e. a screen plane via the projection lens 35.
In the following, the Ye beam superimposing operation to be performed by the Ye superimposing element 48 is described referring to
A rotation amount of Ye beams can be flexibly adjusted by adjusting the level of a voltage to be applied to the Ye superimposing element 48.
A notch filter element or an edge filter element may be used as the Ye superimposing element 48, for example.
The notch filter element is operable to adjust only the polarization condition of light beams having a specific wavelength band. For instance, the notch filter element may adjust only the polarization condition of light beams having a wavelength band longer than the wavelength of green and shorter than the wavelength of red, in other words, a wavelength band corresponding to yellow. Use of the notch filter element enables to reduce unwanted light e.g. yellow light components.
The edge filter element is operable to adjust the polarization condition of light beams having a wavelength band other than a specific wavelength band, without adjusting the polarization condition of light beams having the specific wavelength band. For instance, the edge filter element adjusts the polarization conditions of light beams having a wavelength band longer than the wavelength of green, and of light beams having a wavelength band shorter than the wavelength of green, without adjusting the polarization condition of light beams having the wavelength band corresponding to green. Use of the edge filter element enables to enhance the color purity of light beams having a specific wavelength band e.g. green light components.
In Configuration Example 1, the position of the incident-side polarizer 49 is adjusted in such a manner that the orientation of the transmission axis thereof is aligned in parallel to the polarization direction of G beams. Consequently, in the case where a voltage is not applied to the Ye superimposing element 48, as shown in
On the other hand, as shown in
Also, changing a tilt angle of the polarization direction of Ye beams with respect to the orientation of the transmission axis of the incident-side polarizer 49 by adjusting the voltage to be applied to the Ye superimposing element 48 enables to transmit the Ye beams of an intended light amount in accordance with the tilt angle through the incident-side polarizer 49.
In Configuration Example 1, the light amount of Ye beams to be superimposed on modulated image light beams can be controlled by controlling the voltage to be applied to the Ye superimposing element 48. Thereby, the luminance and the tint of a projection image can be adjusted by controlling the voltage to be applied to the Ye superimposing element 48.
It is desirable to adjust dynamically the applied voltage in accordance with a video signal. For instance, the light amount of Ye beams to be superimposed on modulated image light beams can be dynamically changed in accordance with the brightness of an image to be expressed by a video signal. Alternatively, the light amount of Ye beams to be superimposed on modulated image light beams can be dynamically changed by adding a tint to be reproduced.
As described above, in Configuration Example 1, higher luminance for a projection image can be secured, and at the same time, the color reproducible area can be increased by superimposing Ye beams on modulated image light beams. Further, an enhanced visual effect for a projection image can be obtained by dynamically changing the light amount of Ye beams to be superimposed on modulated image light beams in accordance with the modulated image light beams.
In Configuration Example 2, the optical elements from a dichroic mirror 65 to a relay lens 74 are provided as an optical system for modulating Ye beams and superimposing the modulated Ye beams on modulated image light beams. In Configuration Example 1, the optical system is configured in such a manner that R beams are initially separated from the light beams to be emitted from the illumination device 10. In Configuration Example 2, an optical system is configured to initially separate B beams.
Light beams emitted from the illumination device 10 are incident onto a dichroic mirror 61 via an integrator 11, a PBS array 12, and a condenser lens 13. Among the incident light beams, B beams are transmitted through the dichroic mirror 61, and the light beams other than the B beams are reflected on the dichroic mirror 61. The B beams transmitted through the dichroic mirror 61 are incident onto a dichroic prism 20 via the optical elements from a mirror 30 to the output-side polarizer 34.
Among the light beams reflected on the dichroic mirror 61, G beams are reflected on a dichroic mirror 62, and the other beams are transmitted through the dichroic mirror 62. The G beams reflected on the dichroic mirror 62 are incident onto the dichroic prism 20 via the optical elements from a condenser lens 22 to the output-side polarizer 25.
The light beams transmitted through the dichroic mirror 62 are incident onto the dichroic mirror 65 via a condenser lens 63 and a relay lens 64. The dichroic mirror 65 reflects R beams and transmits Ye beams among the incident light beams. The R beams reflected on the dichroic mirror 65 are incident onto the dichroic prism 20 via the optical elements from a relay lens 66 to the output-side polarizer 19.
The Ye beams transmitted through the dichroic mirror 65 are incident onto a Ye superimposing element 71 via mirrors 67 and 69, and relay lenses 68 and 70. Similarly to the Ye superimposing element 48 in Configuration Example 1, the Ye superimposing element 71 is an element for rotating the polarization direction of Ye beams in accordance with an applied voltage. In Configuration Example 2, since only the Ye beams are incident onto the Ye superimposing element 71, a liquid crystal panel may be used as the Ye superimposing element 71.
The Ye beams transmitted through the Ye superimposing element 71 are incident onto the dichroic mirror 62 again via a relay lens 72, the relay lens 74, and a mirror 73, and then transmitted through the dichroic mirror 62. Thereafter, the Ye beams propagate along the same optical path as the G beams.
As described above, R beams, G beams, Ye beams and B beams that have been incident onto the dichroic prism 20 are combined into modulated image light beams by the dichroic prism 20. The modulated image light beams are projected on a projection plane i.e. a screen plane via a projection lens 35.
In Configuration Example 2, in the case where a voltage is not applied to the Ye superimposing element 71, the polarization direction of Ye beams is rotated by 90 degrees. Accordingly, in this case, the polarization direction of Ye beams intersects perpendicularly to the polarization direction of G beams. Similarly to Configuration Example 1, the position of the incident-side polarizer 23 is adjusted in such a manner that the orientation of the transmission axis thereof is aligned in parallel to the polarization direction of G beams. Accordingly, in the case where a voltage is not applied to the Ye superimposing element 71, although G beams are transmitted through the incident-side polarizer 23, Ye beams are blocked by the incident-side polarizer 23.
On the other hand, changing a tilt angle of the polarization direction of Ye beams with respect to the orientation of the transmission axis of the incident-side polarizer 23 by adjusting the voltage to be applied to the Ye superimposing element 71 enables to transmit the Ye beams of an intended light amount in accordance with the tilt angle through the incident-side polarizer 23. Accordingly, the light amount of Ye beams to be superimposed on modulated image light beams can be controlled by controlling the voltage to be applied to the Ye superimposing element 71, and the luminance and the tint of a projection image can be adjusted. Similarly to Configuration Example 1, it is desirable to adjust dynamically the applied voltage in accordance with a video signal.
In Configuration Example 2, similarly to Configuration Example 1, higher luminance for a projection image can be secured, and at the same time, the color reproducible area can be increased by superimposing Ye beams on modulated image light beams. Further, an enhanced visual effect for a projection image can be obtained by dynamically changing the light amount of Ye beams to be superimposed on modulated image light beams in accordance with the modulated image light beams.
The Ye superimposing element 71 may be so constructed as to rotate the polarization direction of Ye beams with respect to each of incident areas of Ye beams. For instance, one modulation area may be defined on the Ye superimposing element 71 in correspondence to a certain number of pixel areas on the liquid crystal panel 24.
As described above, controlling the rotation of the polarization direction of Ye beams with respect to each of the modulation areas enables to properly adjust the light amount of Ye beams to be superimposed on a projection image with respect to each of the modulation areas. The above arrangement enables to vary a luminance increment by the Ye beam superimposing operation with respect to a bright area and a dark area in a projection image, for instance, which is further advantageous in securing an enhanced visual effect for a projection image. Similarly to Configuration Example 2, in Configuration Example 1, controlling the rotation of the polarization direction of Ye beams with respect to each of modulation areas enables to secure an enhanced visual effect for a projection image.
In the arrangement of
In Configuration Example 3, incident-side polarizers 17, 23, and 32, and output-side polarizers 19, 25, and 34 each has a one-piece construction in
In Configuration Example 3, similarly to Configuration Example 2, an optical system is configured to initially separate B beams. In Configuration Example 3, constituent elements substantially identical or equivalent to those in Configuration Example 2 are indicated with the same reference numerals. The illumination device 10 in Configuration Example 3 is substantially the same as the illumination device 10 in Configuration Example 1.
Light beams emitted from the illumination device 10 are incident onto a dichroic mirror 61 via an integrator 11, a PBS array 12, and a condenser lens 13. Among the light beams incident onto the dichroic mirror 61, B beams are transmitted through the dichroic mirror 61, and the light beams other than the B beams are reflected on the dichroic mirror 61. The B beams transmitted through the dichroic mirror 61 are incident onto a dichroic prism 20 via the optical elements from a mirror 30 to the output-side polarizer 34.
Among the light beams reflected on the dichroic mirror 61, G beams are incident onto a dichroic mirror 82 having a polarization dependency via a polarization rotating element 81. Similarly to the Ye light valve in Configuration Examples 1 and 2, the polarization rotating element 81 acts only on Ye beams, and rotates the polarization direction of Ye beams in accordance with an applied voltage.
The dichroic mirror 82 has a transmittance characteristic as shown in
In Configuration Example 3, G beams and R beams are incident onto the dichroic mirror 82 in an S-polarized state. Accordingly, as is obvious from the characteristic Ts shown in
Since the polarization direction of Ye beams is rotated by the polarization rotating element 81, a certain amount of Ye beams is transmitted through the dichroic mirror 82, and a certain amount of Ye beams is reflected on the dichroic mirror 82 with a ratio depending on a rotation amount of the polarization direction of Ye beams.
Specifically, in the case where Ye beams are incident onto the dichroic mirror 82 in a state that the polarization direction of Ye beams is aligned in the polarization directions of G beams and R beams, in other words, in the case where Ye beams are incident onto the dichroic mirror 82 as S-polarized beams, a primary part of the Ye beams is reflected on the dichroic mirror 82, and the reflected Ye beams propagate along the same optical path as the G beams.
On the other hand, in the case where Ye beams are incident onto the dichroic mirror 82 in a state that the polarization direction of Ye beams intersects perpendicularly to the polarization directions of G beams and R beams, in other words, in the case where Ye beams are incident onto the dichroic mirror 82 as P-polarized beams, a primary part of the Ye beams is transmitted through the dichroic mirror 82, and the transmitted Ye beams propagate along the same optical path as the R beams.
In the case where the polarization direction of Ye beams with respect to the dichroic mirror 82 is in an intermediate state between the P-polarized state and the S-polarized state, a certain amount of Ye beams is transmitted through the dichroic mirror 82, and a certain amount of Ye beams is reflected on the dichroic mirror 82 with a ratio depending on a tilt angle of the polarization direction of Ye beams with respect to the polarization direction of P-polarized beams. In other words, in this case, a P-polarized component of Ye beams is transmitted through the dichroic mirror 82, and an S-polarized component of Ye beams is reflected on the dichroic mirror 82. In this case, Ye beams are distributed with a predetermined ratio to the optical path for G beams and the optical path for R beams.
Referring back to
On the other hand, R beams and Ye beams transmitted through the dichroic mirror 82 are incident onto a narrowband phase difference plate (half wavelength plate having a wavelength selectivity) 83 via a condenser lens 63. As described above, since the P-polarized component of Ye beams is transmitted through the dichroic mirror 82, the polarization direction of Ye beams after transmitting through the dichroic mirror 82 intersects perpendicularly to the polarization direction of R beams.
The narrowband phase difference plate 83 acts only on Ye beams, and rotates the polarization direction of Ye beams by 90 degrees. By the operation, the polarization direction of Ye beams is aligned in the polarization direction of R beams. Thereafter, the R beams and the Ye beams are incident onto the dichroic prism 20 via the optical elements from a relay lens 64 to the output-side polarizer 19.
As described above, R beams, G beams, Ye beams, and B beams that have been incident onto the dichroic prism 20 are combined into modulated image light beams by the dichroic prism 20. The modulated image light beams are projected on a projection plane i.e. a screen plane via a projection lens 35.
In Configuration Example 3, since Ye beams are superimposed on modulated image light beams via the optical path for G beams and the optical path for R beams, higher luminance for a projection image can be secured. Also, controlling the voltage to be applied to the polarization rotating element 81 enables to change a distribution amount of Ye beams with respect to the optical path for G beams and the optical path for R beams, thereby enabling to adjust a color reproducible area of a projection image.
The voltage to be applied to the polarization rotating element 81 may be fixedly switched in accordance with a mode, or dynamically adjusted in accordance with a video signal. Use of the latter method enables to adjust the tint of a projection image depending on a status of the video signal to be supplied, which is advantageous in securing an enhanced visual effect for a projection image.
In Configuration Example 3, since Ye beams are distributed to either one of the optical path for G beams and the optical path for R beams as necessity, as is obvious from
In the above arrangement, the polarization rotating element 81 is controlled in such a manner that the polarization direction of Ye beams with respect to the dichroic mirror 82 is aligned with the polarization direction of S-polarized beams, and the polarization rotating element 85 is controlled in such a manner that the polarization direction of Ye beams intersects perpendicularly to the orientation of the transmission axis of the incident-side polarizer 23. By the control, only the R beams are allowed to be incident onto the liquid crystal panel 18 for R beams, and only the G beams are allowed to be incident onto the liquid crystal panel 24 for G beams. Thus, in the above arrangement, a red color and a green color having a high purity can be simultaneously reproduced on a projection image.
In the arrangement shown in
In the foregoing, the polarization rotating element 85 is provided to block Ye beams. Additionally, the gradient of Ye beams to be superimposed on G beams or R beams can be more finely controlled, as compared with the arrangement shown in
If Ye beams are superimposed in the manner described in one of Configuration Examples 1 through 3, a projection image may have less blue light components in some occasion. In view of the disadvantage, the light amount of B beams may be increased by replacing the lamp 105 shown in
In Configuration Example 4, incident-side polarizers 17, 23, and 32, and output-side polarizers 19, 25, and 34 each has a one-piece construction in
Similarly to Configuration Example 1, in Configuration Example 4, an optical system is configured to initially separate R beams. In Configuration Example 4, elements substantially identical or equivalent to those in Configuration Example 1 are indicated with the same reference numerals. The illumination device 10 in Configuration Example 4 is substantially the same as the illumination device 10 in Configuration Example 1.
In Configuration Example 4, R beams (Rt beams and Rr beams), G beams (Gt beams and Gr beams), and B beams (Bt beams and Br beams) are separated by dichroic mirrors 91 and 92, and incident onto a polarization rotating element 93 for R beams, a polarization rotating element 94 for G beams, and a polarization rotating element 95 for B beams, respectively. In Configuration Example 4, the wavelength band of R beams and the wavelength band of G beams are contiguous to each other, and the wavelength band of G beams and the wavelength band of B beams are contiguous to each other. Rr beams are the light beams in a wavelength band (shorter wavelength side) closer to the wavelength band corresponding to yellow than the wavelength band of Rt beams. Br beams are the light beams in a wavelength band (longer wavelength side) closer to the wavelength band corresponding to bluish green than the wavelength band of Bt beams. Gr beams may contain light beams in a wavelength band (longer wavelength side) closer to the wavelength band corresponding to yellow than the wavelength band of Gt beams, and light beams in a wavelength band (shorter wavelength side) closer to the wavelength band corresponding to bluish green than the wavelength band of Gt beams. In Configuration Example 4, Gr beams may contain either one or both of the light beams in the wavelength band corresponding to the longer wavelength side, and the light beams in the wavelength band corresponding to the shorter wavelength side.
The polarization rotating element 93 for R beams acts only on Rr beams among Rt beams and Rr beams, and rotates the polarization direction of Rr beams in accordance with an applied voltage. By the operation, the light amount of Rr beams to be incident onto the liquid crystal panel 18 is adjusted.
In the case where a voltage to be applied to the polarization rotating element 93 for R beams is turned off, the polarization rotating element 93 for R beams acts only on Rr beams among Rt beams and Rr beams incident onto the polarization rotating element 93 for R beams, to rotate the polarization direction of Rr beams by 90 degrees. By the operation, the polarization direction of Rr beams intersects perpendicularly to the orientation of the transmission axis of the incident-side polarizer 17. Thereby, substantially the entire light amount of Rr beams is blocked by the incident-side polarizer 17 to allow only the Rt beams to be incident onto the liquid crystal panel 18.
On the other hand, in the case where a voltage of a predetermined level is applied to the polarization rotating element 93 for R beams, since the polarization rotating element 93 for R beams is inoperable to act on Rr beams to rotate the polarization direction of Rr beams, the Rr beams are incident onto the incident-side polarizer 17 in the same polarization direction as the Rt beams. In this case, both of the polarization directions of Rt beams and Rr beams are aligned in parallel to the orientation of the transmission axis of the incident-side polarizer 17. Thereby, substantially the entire light amount of Rt beams and Rr beams is transmitted through the incident-side polarizer 17, and incident onto the liquid crystal panel 18.
Similarly to the operation of the polarization rotating element 93 for R beams, in the case where a voltage to be applied to the polarization rotating element 94 for G beams is turned off, the polarization rotating element 94 for G beams acts on Cr beams to rotate the polarization direction of Gr beams. Thereby, substantially the entire light amount of Gr beams is cut off by the incident-side polarizer 23. In the case where a voltage of a predetermined level is applied to the polarization rotating element 94 for G beams, the polarization rotating element 94 for G beams is inoperable to act on Gr beams to rotate the polarization direction of Gr beams. Thereby, substantially the entire light amount of both of Gt beams and Gr beams is transmitted through the incident-side polarizer 23, and incident onto the liquid crystal panel 24.
In the case where a voltage to be applied to the polarization rotating element 95 for B beams is turned off, the polarization rotating element 95 for B beams acts on Br beams to rotate the polarization direction of Br beams. Thereby, substantially the entire light amount of Br beams is cut off by the incident-side polarizer 32. In the case where a voltage of a predetermined level is applied to the polarization rotating element 95 for B beams, the polarization rotating element 95 for B beams is inoperable to act on Br beams to rotate the polarization direction of Br beams. Thereby, substantially the entire light amount of both of at beams and Br beams is transmitted through the incident-side polarizer 32, and incident onto the liquid crystal panel 33.
Similarly to the Ye superimposing element in Configuration Example 1, the polarization rotating element 93 for R beams, the polarization rotating element 94 for G beams, and the polarization rotating element 95 for B beams each may be constituted of either one of a notch filter element and an edge filter element. With use of any one of the notch filter element and the edge filter element, the polarization rotating element 93 for R beams, the polarization rotating element 94 for G beams, and the polarization rotating element 95 for B beams are configured to act only on the wavelength band of Rr beams, the wavelength band of Gr beams, and the wavelength band of Br beams, respectively.
When the projector is in the light amount priority mode, since Rr beams, Gr beams, and Br beams are respectively incident onto the liquid crystal panels 18, 24, and 33, the total light amount of a projection image is increased by the incidence of Rr beams, Gr beams, and Br beams. However, the incidence of Rr beams, Gr beams, and Br beams may lower the color purity of red, green, and blue. As a result, the color reproducible area of a projection image may be reduced to an area defined by the dotted line in
On the other hand, when the projector is in the color purity priority mode, Rr beams, Gr beams, and Br beams are not allowed to be incident onto the liquid crystal panels 18, 24, and 33, respectively. As a result, the total light amount of a projection image may be lowered, as compared with a condition that the projector is operated in the light amount priority mode. However, since Rr beams, Gr beams, and Br beams are not incident, the color purities of red, green, and blue are increased. Accordingly, the color reproducible area of a projection image is expanded to an area defined by the solid line in
As described above, in Configuration Example 4, the light amount i.e. the luminance, and the color reproducibility of a projection image can be optimally adjusted by controlling on/off operations of the polarization rotating element 93 for R beams, the polarization rotating element 94 for G beams, and the polarization rotating element 95 for B beams. The above arrangement enables to provide a projector operable to satisfy the requirements on high luminance and color reproducibility.
In Configuration Example 4, the rotation amounts of the polarization directions of Rr beams, Gr beams, and Br beams can be flexibly adjusted by controlling the voltages to be applied to the polarization rotating element 93 for R beams, the polarization rotating element 94 for G beams, and the polarization rotating element 95 for B beams, respectively. Thereby, the light amounts of Rr beams, Gr beams, and Br beams to be superimposed on modulated image light beams can be properly adjusted. For instance, configuring a control circuit in such a manner that the voltages to be applied to the polarization rotating element 93 for R beams, the polarization rotating element 94 for G beams, and the polarization rotating element 95 for B beams are controlled in accordance with a video signal enables to dynamically adjust the light amounts of Rr beams, Gr beams, and Br beams to be superimposed on modulated image light beams depending on a status of a projection image. Thereby, optimum luminance and color reproducibility can be secured depending on occasions.
The embodiments of the present invention are described in the foregoing. The present invention, however, is not limited to the foregoing embodiments. The embodiments of the present invention may be changed or modified in various ways, other than the above.
The modifications on the mirror arrangement shown in
The embodiments of the present invention may be changed or modified in various ways, according to needs, as far as such changes and modifications do not depart from a technical concept defined in the scope of the claims.
Configuration Examples 1 through 3 in the ninth embodiment correspond to the embodiment of the invention defined in claim 9, and Configuration Example 4 corresponds to the embodiment of the invention defined in claim 10.
Number | Date | Country | Kind |
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JP2007-110962 | Apr 2007 | JP | national |
JP2007-292217 | Nov 2007 | JP | national |