Lighting device transformed in the direction of polarization and projection type image display device using the same

Abstract: In a projection type image display device of light valve type, a lighting device suitable for a device in a constitution making use of polarization in particular is presented. A lighting device transformed in the direction of polarization comprising a light source, an elliptical mirror, polarized light selecting means disposed at a second focal point position of the elliptical mirror, collimating means for transforming the light from the second focal point of the elliptical mirror into nearly parallel light while reflecting, polarization transforming means provided in the collimating means, and optical path transforming means having an aperture in the central part, wherein light is separated into first and second directions of polarization by the polarized light selecting means, the light in the second direction of polarization is set to enter the collimating means, and the direction of polarization is transformed in the same direction as the light of the first direction of polarization, and it is reflected on the same optical axis as the light in the first direction of polarization by the optical path transforming means having its aperture disposed so as to correspond to the position of the polarized light selecting means.

Description: BACKGROUND OF THE INVENTION Technical Field of the Invention The present invention relates to a lighting device transformed in the direction of polarization for controlling the state of polarization of light from a light source in one direction and illuminating, and a projection type image display device of light valve type using the same. Prior Art Instead of the conventional projection type image display device using cathode-ray tube (CRT), the projection type image display device using liquid crystal panel as light valve is being accepted in the market from the viewpoints of small size, light weight, ease of installation, and low price. This projection type image display device comprises an incident side polarizer for preliminarily limiting the direction of polarization of incident light, a liquid crystal panel for controlling the angle of polarization of incident light, and an exit side polarizer for transmitting only light in a specific direction of polarization. In the conventional constitution, only half of the light emitted from the light source can be utilized at maximum, and the brightness of the projected image is insufficient. Besides, the energy of the remaining light not being used generates heat in the device, and hence the reliability of the projection type image display device is lowered. To solve such problems, as the lighting device of projection type image display device, there is proposed a lighting device for inputting on the light valve surface from two optical paths, by separating the light from the light source by polarization selecting means, and then transforming the polarization of the half of the polarized component. In such constitution, however, as seen from the irradiating surface side, the apparent size of the light source is about twice as long as the actual length in one direction. Therefore, to take in the light efficiently by the projection optical system, it is necessary to increase the intake angle. As a result, the projection lens becomes very large, and expensive. Moreover, because the image of the light source is extended in one direction to be long as mentioned above, increase of brightness is not expected in spite of the increased size of the projection lens. If the device of which characteristic varies significantly depending on the incident angle of light as in the conventional transmission type liquid crystal panel is used as the light valve in the constitution, since the incident angle of light is large, the picture quality deteriorates. When transforming the direction of polarization, the transformation efficiency may vary depending on the wavelength. At this time, in comparison between transformed light and non-transformed light, since the angle of incident into the light valve is different, the contribution factor of light in the central part of the projected image is different from the contribution factor of light in the peripheral part. Therefore, the color of the central part of the projected image is different from the color of the peripheral part. As a result, in the projection type image display device using the conventional lighting device, a color difference occurs due to difference in angle of incident angle of light. Various arrangements for optically combining the two polarized light beans in an illumination device are disclosed in FR-A-2 693 561, US-A- 4 913 529, US-A-5 381 278, JP-A-04 245 210, JP-A-02 039 084, JP-A-04 127 120 and JP-A-07 135 145. The preamble of claims 1 and 6 is based on the conventional arrangements. SUMMARY OF THE INVENTION The lighting device of the invention is set out in claims 1, 6. A projection type image display device using a lighting device of the invention is set out in claim 14. In one embodiment, the two directions of polarization are same from the time the optical path is divided by the direction of polarization by the polarization selecting means until the time combined again. Therefore, the light from the light source can be utilized at high efficiency. In another embodiment, the parallel light is divided into optical paths by the polarization selecting means, the direction of polarization of one divided portion of the light is transformed, and the luminous flux of the light magnified from the luminous flux is combined with the other divided portion of the light divided by the polarization selecting means. Therefore, the light from the light source can be utilized at high efficiency. In another embodiment, the aperture of the optical path transforming means is positioned on the optical path of the other divided portion of the light from the polarization selecting means, and the other divided portion of the light passes through this aperture, and is hence combined with the light from the luminous flux magnifying means without being affected by the optical path transforming means. Therefore, the light from the light source can be utilized at high efficiency. The projection type image display device of the invention is constituted by disposing an image display device for displaying an image using polarization in the illuminated position, by utilizing the light combined in the lighting device transformed in the direction of polarization of the invention, and comprising a projection lens for magnifying and projecting the image. In this constitution, the light utilization rate is enhanced, and generation of heat by absorption of light in the image display device and its periphery can be suppressed. As a result, the projection type image display device realizing an image of high luminance at high efficiency can be presented. In the embodiments, rays of light in two different directions of polarization of the light source can be transformed into light of one direction of polarization, and the transformed rays of light are superposed on one optical axis. Therefore, the utilization efficiency of light is greatly enhanced. As a result, the brightness is about twice as much as in the prior art. Alternatively, to obtain the lighting device of the same brightness as in the prior art, the power consumption is saved to half. The light source and driving circuit can be reduced in size and lowered in price. The projection type image display device using the lighting device transformed in the direction of polarization of the invention prevents incident of light in unnecessary direction of polarization in the light control unit of the image display means such as liquid crystal panel, and therefore degreases in the heat generation, so that the projection type image display device of excellent reliability and high luminance may be obtained. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a diagram of an embodiment of a lighting device transformed in the direction of polarization of the invention; Fig. 2 is a diagram of other embodiment of a lighting device transformed in the direction of polarization of the invention; Fig.3 is a diagram of a different embodiment of a lighting device transformed in the direction of polarization of the invention; Fig. 4 is a diagram of the different embodiment of a lighting device transformed in the direction of polarization of the invention; Fig. 5 is a diagram of the different embodiment of a lighting device transformed in the direction of polarization of the invention; Fig. 6 is a diagram of an embodiment of a projection type image display device of the invention; Fig. 7 is a diagram of a further embodiment of a lighting device transformed in the direction of polarization of the invention; Fig. 8 is a diagram of the further embodiment of a lighting device transformed in the direction of polarization of the invention; Fig. 9 is a diagram of the further embodiment of a lighting device transformed in the direction of polarization of the invention; Fig. 10 is a diagram of a further different embodiment of a lighting device transformed in the direction of polarization of the invention; Fig. 11 is a diagram of the further different embodiment of a lighting device transformed in the direction of polarization of the invention; Fig. 12 is a diagram of the further different embodiment of a lighting device transformed in the direction of polarization of the invention; Fig. 13 is a diagram of the further different embodiment of a lighting device transformed in the direction of polarization of the invention; Fig. 14 is a diagram of the further different embodiment of a lighting device transformed in the direction of polarization of the invention; Fig. 15 is a diagram of the further different embodiment of a lighting device transformed in the direction of polarization of the invention: Fig. 16 is a diagram of the further different embodiment of a lighting device transformed in the direction of polarization of the invention; Fig. 17 is a diagram of an illustrative example of a lighting device transformed in the direction of polarization of the invention; Fig. 18 is a perspective view of a further different illustrative example of a lighting device transformed in the direction of polarization of the invention; Fig. 19 is a diagram of the further different embodiment of a lighting device transformed in the direction of polarization of the invention: Fig. 20 is a diagram of other embodiment of a projection type image display device of the invention: and Fig. 21 is a diagram of a different embodiment of a projection type image display device of the invention. REFERENCE NUMERALS 1, 101 Light sources 2, 32, 102 First focal point positions 3, 33, 103 First optical axes 4, 19, 34 Elliptical mirrors 5, 35 Second focal point positions 6, 27, 37, 105, 122 Polarizing beam splitters 7, 106, 123 Second optical axes 8, 15, 20, 36 Collimator lenses 9, 40, 42, 110, 112, 121, 137 Reflectors 10, 29 Quarter-wave plate 11, 30, 43 Apertures of combined reflectors 12 Reflection surface of combined reflector 13, 44, 47, 134 Combined reflectors 14, 31 Concave mirrors 16, 104 Parabolic reflectors 17, 28, 48 Supporting glass plates 18, 39 Half-wave plates 21 Plane polarization beam splitter 22, 128 Incident side polarizers 23, 129 Liquid crystal panels 24, 130 Exit side polarizers 25, 120, 131 Projection lenses 26, 132 Screens 31 Concave mirror 38, 106 Second optical axes 41, 49 Luminous flux magnifying lenses 45, 46, 133 Condenser lenses 100, 200, 300 Lighting devices transformed in the direction of polarization 107, 136 First integrator arrays 108, 138 Second integrator arrays 109 Irradiated surface 111, 133 Condenser lenses 113 Phase difference plate 114, 118, 119, 125 Small reflectors 115 Aperture 116, 117 Luminous flux width transforming lens 124 Third optical axis 126 Field lens 127 Liquid crystal surface 128 Incident side polarizer 129 Liquid crystal panel 130 Exit side polarizer 132 Screen 135 Small aperture 301, 302, 304, 305, 401 Parallel rays of light 303 Convexo-concave combined collimator lens 306 Concave lens DETAILED DESCRIPTION OF THE INVENTION Referring now to the drawings, preferred embodiments of lighting device transformed in the direction of polarization and projection type image display device of the invention are described in detail below. (Embodiment 1) Fig. 1 is a structural diagram of a lighting device transformed in the direction of polarization for explaining a first embodiment of the invention. A light source 1 is disposed at the position of a first focal point 2 of an elliptical mirror 4. In Fig. 1, the light emitted from the light source 1 is condensed in a second focal point position 5 by the elliptical mirror 4 formed to be rotationally symmetrical to the major axis of a first optical axis 3. A polarization beam splitter 6 is provided as polarization selecting means at the second focal point position 5 of the elliptical mirror 4. This polarization beam splitter 6 reflects the S-poiarized light, and the reflected S-polarized light travels onto a second optical axis 7. On the other hand, the P-polarized light passes through the polarization beam splitter 6, and passes through a collimator lens 8 disposed on the first optical axis 3, then passes through a quarter-wave plate 10 which is polarization transforming means disposed at the light exit side of the collimator lens 8, and is reflected by a reflector 9 disposed at the back side of the quarter-wave 10. The polarized light reflected by the reflector 9 passes again through the quarter-wave plate 10 and the collimator lens 8 to be parallel light 301. In order that the light passing through the collimator lens 8 second time may be parallel light, the shape of the collimator lens 8 is designed. The quarter-wave plate 10 as the polarization transforming means acts to transform the entering P-polarized light into a circular polarized light. Therefore, the light becoming a circular polarized light by passing through the quarter-wave plate 10 enters the reflector 9 and is transformed into a circular polarized light of reverse rotation. Later, passing again through the quarter-wave plate 10, the light becoming a circular polarized light of reverse rotation returns to the first optical axis 3 as 90-degree twisted polarized light (that is, S-polarized light) from the direction of polarization of the first entering light. The returnedlight enters a combined reflector 13 as optical path transforming means. The combined reflector 13 forms an aperture 11 in the central part, and the polarization beam splitter 6 is disposed in the aperture 11. The peripheral part of the combined reflector 13 is a reflection plane 12, and on this reflection plane 12, the light entering from the collimator lens 8 is reflected on the second optical axis 7. In this way, according to the embodiment, almost all light emitted from the light source is sent out in one direction as light in one direction of polarization. In this embodiment, the light source 1 is close to a spot light source, and its elliptical mirror 4 is preferred to be large. In this constitution, the light is condensed efficiently on the polarization beam splitter 6. Besides, when the solid angle of the light entering the polarization beam splitter 6 is small, splitting by polarization can be done efficiently, and hence the distance between two focal points of the elliptical mirror 4 is preferred to be longer. The thickness of the luminous flux transformed into parallel light by the collimator lens 8 and reflection plane 12 is preferred to be as large as possible, and it contributes to reduction of loss due to defect in the central part of the reflector 13. The angle of parallel light is not strictly required, but it is preferred to be optimized by combination with 'the system. The collimator lens 8 is not absolutely necessary. In this embodiment, the quarter-wave plate 10 is used as means for transforming the direction of polarization, but the means for transforming may be also realized by disposing a half-wave plate on or near the polarization beam splitter 6 to pass through after splitting the optical path by the direction of polarization by the polarization beam splitter 6. Fig. 2 shows a modified example of the first embodiment. In the lighting device transformed in the direction of polarization in Fig. 2, the reflector 9 in the lighting device transformed in the direction of polarization in Fig. 1 is replaced by a concave mirror 14. By using the concave mirror 14 as the reflecting means in Fig. 2, the light from the quarter-wave plate 10 can be transformed and reflected as parallel light, which eliminates the necessity of collimator lens. Therefore, the device size can be reduced, the loss of light is decreased, and the utilization efficiency of light is enhanced. It is also possible to dispose a condenser lens 15 as condensing means on the second optical axis 7. In this constitution, the structure may be optimized depending on the size of the illuminated surface and the distance to the illuminating position. (Embodiment 2) The constitution of the lighting device transformed in the direction of polarization for realizing a second embodiment of the invention is described while referring to Fig. 3 and Fig. 4. Fig. 3 is a structural diagram showing the constitution of the lighting device transformed in the direction of polarization in the second embodiment of the invention, and Fig. 4 is a structural diagram showing a constitution of a modified example of the lighting device transformed in the direction of polarization shown in Fig. 3. In Fig. 3 and Fig. 4, the light emitted from the light source 1 is reflected by a parabolic reflector 16 formed to be rotationally symmetrical to the major axis of the first optical axis 3, and is transformed into parallel light 302. In the lighting device transformed in the direction of polarization shown in Fig. 1 and Fig. 2, the light control means was the elliptical mirror 4 having the second focal point at the position of the polarization beam splitter 6, and instead, as shown in Fig. 3, in the constitution of using the parabolic reflector 16 as the parallel light transforming means for transforming 302 into parallel light, by entering the parallel light 302, the polarization selectivity of the polarization beam splitter 6 can be used advantageously, so that the efficiency of effective utilization of light may be enhanced. On the other hand, as the parallel light transforming means, by combining the elliptical mirror 19 and collimator lens 20 as shown in Fig. 4, it may be also constituted so that the parallel light 302 may enter the polarization beam splitter 6. In this constitution, the same effects as above can be obtained. The parallel light 302 enters the polarization beam splitter 6 as polarization selecting means, and the polarization beam splitter 6 reflects the S-polarized light, which is caused to travel on the second optical axis 7. On the other hand, the P-polarized light passes through the reflection surface of the polarization beam splitter 6, and further passes through a convexo-concave combined collimator lens 303 as luminous flux magnifying means disposed on the first optical axis 3, and is reflected by the reflector 9, and passes again through the convexo-concave combined collimator lens 303, and is reflected by a combined reflector 13 as parallel light 304. In Fig. 3, as the means for magnifying the luminous flux, the convexo-concave combined collimator lens 303 is used, and a modified example is shown in Fig. 4. In Fig. 4, the parallel light 305 coming from the polarization beam splitter 6 is magnified in the luminous flux by the concave lens 306, and then enters the collimator lens 8. The subsequent traveling path of light is same as in embodiment 1. The P-polarized light reflected by the combined reflector 13 passes through a half-wave plate 18 which is polarization transforming means, and is transformed into S-polarized light. The half-wave plate 18 is supported by a support glass plate 17. The half-wave plate 18 has an aperture near the second optical axis 7, and the S-polarized light reflected by the polarization beam splitter 6 passes through this aperture. Therefore, the light passing through the aperture and the polarized light passing through the half-wave plate 18 are both S-polarized lights, and their tips are combined. Thus, in the embodiment shown in Fig. 3 and Fig. 4, the light is utilized effectively, and the optical path splitting efficiency by the direction of polarization in the polarization beam splitter 6 is enhanced by the utilization of parallel light. As a result, the light in the direction of polarization finally required can be efficiently obtained. (Embodiment 3) Other embodiment of the lighting device transformed in the direction of polarization of the invention is described below by reference to Fig. 5. In Fig. 5, characteristically, a plane type polarization beam splitter 21 is composed as polarization selecting means at the aperture of the combined reflector 13. The other constitution is same as in embodiment 1 explained in Fig. 1. In this constitution, the incident angle is larger. Hence, it is possible to split by polarization at lower cost. (Embodiment 4) An embodiment of a projection type image display device of the invention is described below while referring to Fig. 6. Fig. 6 is an example of the projection type image display device using the lighting device transformed in the direction of polarization explained in Fig. 2. In Fig. 6, the light emitted from a lighting device transformed in the direction of polarization 100 passes through an incident side polarizer 22 provided so that the passing direction of polarization may coincide with the direction of polarization (S-polarization in Fig. 2) from the lighting device transformed in the direction of polarization 100, and enters a liquid crystal panel 23 as image display means. The liquid crystal panel 23 is composed of multiple picture elements which can be independently controlled by external signals. The light entering the picture elements of the liquid crystal panel 23 of the portion to be displayed in white of the image display area passes through the incident side polarizer 22, and, as the direction of polarization is twisted by 90 degrees by the liquid crystal layer of the liquid crystal panel 23, passes through the incident side polarizer 22 and an exit side polarizer 24 orthogonal to the passing direction of polarization. On the other hand, the light entering the picture elements of the liquid crystal panel 23 of the portion to be displayed in black of the image display area passes through the incident side polarizer 22, without being twisted of the direction of polarization by the liquid crystal layer of the liquid crystal panel 23, and enters the exit side polarizer 24 and is absorbed. The light passing through the exit side polarizer 24 is guided onto a screen 26 by a projection lens 25. In this way, the picture elements in the display area of the liquid crystal panel 23 is magnified and projected by the projection lens 25. As a result, a large picture is obtained on the screen 26. Hitherto, the liquid crystal panel could use light in one direction of polarization only, and hence about 50% of the light from the light source was absorbed in the incident side polarizer. Hence, the light utilization rate was poor. Still worse, since the incident side polarizer absorbs the light, heat generation is significant, and it was hard to obtain a high luminance. By contrast, in the constitution of this embodiment, all the light from the light source can be utilized effectively. As a result, the light utilization efficiency is enhanced, and the heat generation is small, and the luminance can be improved. The constitution of the lighting device transformed in the direction of polarization 100 shown in Fig. 6 represents the embodiment in Fig. 2, but the projection type image display device can be realized also by using the lighting device transformed in the direction of polarization shown in embodiment 1 through embodiment 4, and the same effects are obtained. In this embodiment, too, instead of the transmission type liquid crystal panel as the image display means, it is also possible to compose a reflection type liquid crystal panel. (Embodiment 5) A different embodiment of the lighting device transformed in the direction of polarization of the invention is described by referring to Fig. 7. In Fig. 7, the light emitted from the light source 1 is condensed in the second focal point position 5 by the elliptical mirror 4 formed to be rotationally symmetrical to the major axis of the first optical axis 3 so that the light source 1 may be positioned at the first focal point position 2. Near the second focal point position 5, a polarization beam splitter 27 is provided as polarization selecting means, and this polarization beam splitter 27 transmits the P-polarized light, but reflects the S-polarized light as shown in the diagram to reflect to the light source side along the first optical axis 7. This polarization beam splitter 27 is formed by combination of two planes composed symmetrically to the first optical axis 3. The S-polarized light reflected by the polarization beam splitter 27 passes through a quarter-wave plate 29 which is polarization transforming means provided in a support glass plate 28, and is transformed into a circular polarized light. Afterwards, the circular polarized light is reflected by a concave mirror 31 (optical path transforming means) having an aperture 30 for passing light from the light source 1 to the polarization beam splitter 27 in its central part, being formed to be rotationally symmetrical to the first optical axis 3, and is transformed nearly into parallel light 401. In this way, the light entering the quarter-wave plate 29 again is a circular polarized light in reverse direction of the incident light, and is hence emitted as S-polarized light after passing through the quarter-wave plate 29. The light passing through the quarter-wave plate 29 and the light passing through the polarization beam splitter 27 are both S-polarized lights, and these S-polarized lights are combined, and then sent out from the lighting device transformed in the direction of polarization. Thus, also in this embodiment, most of the light emitted from the light source is emitted in one direction as light in one direction of polarization. Therefore, the light utilization efficiency is notably improved. At the same time, the reliability is extremely improved. Moreover, by the use of the concave mirror 31, the device is reduced in scale. The polarization beam splitter 27, instead of being composed of two planes disposed symmetrically on the first optical axis 3, may be formed as a polarization beam splitter of prism type or in a conical form having the center of rotation on the first optical axis. In this embodiment, by the using of the concave mirror 31, the scale of the device can be reduced. Instead of the concave mirror 31, by combination of the plane mirror and lens as shown in embodiment 1 to embodiment 3, the same effects are obtained. (Embodiment 6) A different embodiment of the lighting device transformed in the direction of polarization of the invention is described in Fig. 8. In Fig. 8, the light emitted from the light source 1 is condensed in a second focal point position 35 by an elliptical mirror 34 formed to be rotationally symmetrical to the major axis of a first optical axis 33 so that the light source 1 may be positioned at a first focal point position 32. The light passing through the second focal point position 35 is transformed into nearly parallel light by a collimator lens 36 as parallel light transforming means, and enters a polarization beam splitter 37 as polarization selecting means. In the polarization beam splitter 37, of the incident parallel light, the S-polarized light is reflected and travels on a second optical axis 38. On the other hand, the P-polarized light passes through the reflection plane of the polarization beam splitter 37, and passes through a half-wave plate 39 (polarization transforming means) on the first optical axis 33. On the half-wave plate 39, the P-polarized light is transformed into S-polarized light. It is then reflected by a reflector 40, and enters a luminous flux magnifying lens 41 as luminous flux magnifying means. This luminous flux magnifying lens 41 is designed to magnify the luminous flux of the entering nearly parallel light as it is nearly parallel light. The light passing through the luminous flux magnifying lens 41 is reflected by a reflector 42, and enters a combined reflector 44 as optical path transforming means having an aperture 43 in the center. On the other hand, the S-polarized light traveling up to the second optical axis 38 passes through a condenser lens 45, and is condensed in the aperture 43 of the reflector 44 or its vicinity. Therefore, the S-polarized light traveling on the second optical axis 38 continues to travel on the second optical axis 38 without being affected by the reflector 44. The light reflected by the reflector 42 and entering the combined reflector 44 is reflected by the combined reflector 44, and is reflected to travel on the second optical axis 38. The light entering from the reflector 42 passes through an intermediate half-wave plate 39, and the P-polarized light is transformed into S-polarized light, and finally the light emitted from this lighting device transformed in the direction of polarization is entirely S-polarized light. According to this constitution, by keeping the position of the polarization selecting means away from the optical path transforming means, the structure is complicated more than in the foregoing embodiments, but the luminous flux entering the polarization beam splitter 37 is closer to parallel light, and hence the efficiency of splitting of optical path by the direction of polarization is extremely enhanced. Moreover, since the polarization selecting means is not disposed at the position of the aperture 43, the size of the aperture may be reduced. Therefore, the reflection loss of the light entering from the reflector 42 may be kept to a minimum limit. In this constitution, if the luminous flux diameter after passing through the collimator lens 36 is sufficiently smaller than the luminous flux after passing through the luminous flux magnifying lens 41, the condenser lens 45 may not be always necessary. If the luminous flux condensed in the condense lens 45 is sufficiently smaller than the luminous flux after passing through the collimator lens 36, the luminous flux magnifying lens 41 may not be always necessary. Besides, by setting the lens of the collimator lens 36 so as to focus on the position of the aperture 43 or its vicinity, the condenser lens 45 can be omitted. The constitution and location of the half-wave plate 39 as polarization transforming means are not limited to the above means. That is, instead of the half-wave plate 39, a quarter-wave plate may be used as phase difference plate. In Fig. 8, the elliptical mirror 34 is used, but a parabolic reflector such as the one shown in Fig. 3 may be also used. If the aperture of the parabolic reflector is wide, a condenser lens may be also disposed at the exit side. A same projection type image display device can be constituted by using the lighting device transformed in the direction of polarization of the embodiment as the lighting device transformed in the direction of polarization 100 explained in embodiment 14. In this constitution, too, the same effects as in embodiment 4 are obtained. (Embodiment 7) A further different embodiment of the lighting device transformed in the direction of polarization of the invention is described by reference to Fig. 9. In Fig. 9, the light emitted from the light source 1 is condensed in a second focal point position 35 by an elliptical mirror 34 formed to be rotationally symmetrical to the major axis of a first optical axis 33 so that the light source 1 may be positioned at a first focal point position 32. The light passing through the second focal point position 35 is transformed into nearly parallel light by a collimator lens 36 as parallel light transforming means, and enters a polarization beam splitter 37 as polarization selecting means. The polarization beam splitter 37 reflects the S-polarized light, and allows it to travel onto the second optical axis 38. On the other hand, the P-polarized light passes through the reflection plane of the polarization beam splitter 37, and runs through the condenser lens 46 on the first optical axis 33, half-wave plate 39, reflector 40 and reflector 42, and is condensed on a combined reflector 47 as optical path transforming means. The combined reflector 47 is provided on a support glass plate 48 for transmitting the visible light, disposed obliquely on the second optical axis 38. On the other hand, the S-polarized light traveling up to the second optical axis 38 is sufficiently larger in the luminous flux width than the combined reflector 47, and hence continues to travel on the second optical axis 38 without being affected by the combined reflector 47. The light entering the reflector 47 through the reflector 42 is reflected by the combined reflector 47 so as to travel on the second optical axis 38. The light entering the combined reflector 47 from the reflector 42 passes an intermediate half-wave plate 39, and is twisted of the direction of polarization, and hence the P-polarized light is transformed into S-polarized light. Therefore, finally, all the light emitted from the lighting device transformed in the direction of polarization is S-polarized light only. In this constitution, since the light entering the polarization beam splitter 37 is closer to parallel light, the efficiency of optical path splitting by the direction of polarization may be enhanced. At the same time, the combined reflector 47 as optical path transforming means may be reduced in size. It further provides an effect of minimizing the defect of the light entering from above the second optical axis 38. In the embodiment, the polarization transforming means and its location are not limited to the above constitution, but, instead of the half-wave plate, a quarter-wave plate may be used as phase difference plate. (Embodiment 8) A different embodiment of lighting device transformed in the direction of polarization of the invention is described by referring to Fig. 10. In Fig. 10, same as in the example in Fig. 9, the P-polarized light split by the polarization beam splitter 37 which is polarization selecting means passes through the reflection plane, and enters the combined reflector 47 which is the optical path transforming means, by way of the half-wave plate 39 on the first optical axis 33, reflector 40 and reflector 42. The combined reflector 47 is provided on the support glass plate 48 for transmitting visible light, disposed obliquely on the second optical axis 38. On the other hand, the S-polarized light traveling up to the second optical axis 38 is transformed by the luminous flux magnifying lens 49 so that the luminous flux width may be sufficiently larger than the combined reflector 47, and continues to travel on the second optical axis 38 without being affected by the combined reflector 47. The first light entering the combined reflector 47 through the reflector 42 is reflected by the combined reflector 47 so as to travel on the second optical axis 38. The light entering from the reflector 42 passes through an intermediate half-wave plate 39, and is twisted of the direction of polarization, and the first P-polarized light is transformed into S-polarized light. Therefore, finally, all the light emitted from this lighting device is the S-polarized light only. In this constitution, the same effects as in embodiment 1 can be obtained. In the embodiment, the polarization transforming means and its location are not limited to the half-wave plate 39, but, instead, a quarter-wave plate may be used as phase difference plate. Moreover, in the constitution in Fig. 9 and Fig. 10 of the embodiment, instead of the elliptical mirror 34, a parabolic reflector for emitting parallel light may be used to compose the same lighting device transformed in the direction of polarization. A same projection type image display device can be constituted by using the lighting device transformed in the direction of polarization of the embodiment as the lighting device transformed in the direction of polarization 100 explained in embodiment 14. In this constitution, too, the same effects as in . embodiment 14 are obtained. (Embodiment 9) A different embodiment of the lighting device transformed in the direction of polarization is described in Fig. 11. In Fig. 11, the light emitted from a light source 101 is reflected by a parabolic reflector 104, and enters a polarization beam splitter 105 as polarization selecting means. The parabolic reflector 104 is disposed in rotational symmetricity to a first optical axis 103 so that the light source 101 may be positioned at a focal point position 102. The polarization beam splitter 105 reflects the S-polarized light, and causes the S-polarized light to travel on a second optical axis 106. On the other hand, the P-polarized light passes through the reflection plane of the polarization beam splitter 105, and enters a first integrator lens array 107 which is integrator means on the first optical axis 103. The incident light is split into a plurality of rays of light by each lens of the first integrator lens array 107. Each split light forms a secondary light source image on each corresponding lens of a second integrator lens array 108 which is integrator means. Each light emitted from the second integrator lens array 108 forms a magnified image superposed on each irradiation surface 109. The light traveling up to the second optical axis 106 enters a condenser lens 111 as being guided by a reflector 110 disposed obliquely to the optical axis, and is condensed on a reflector 112 disposed obliquely to the optical axis, and on a small reflector 114 as optical path transforming means through a phase difference plate 113. At this time, the phase difference plate 113 which is polarization transforming means is set so that the direction of polarization may be same as the direction of polarization of the light traveling on the first optical axis 103. The small reflector 114 is disposed obliquely to the first optical axis. This small reflector 114 is set so that the light traveling on the optical axis being guided by the reflector 112 may illuminate the region on the same irradiation surface 109 as the position illuminated by the light emitted from the second integrator lens array 108. According to the constitution, most of the light emitted from the light source 101 may be emitted to illuminate as light in one direction of polarization only. In this embodiment, the light source 101 is preferred to be closer to a spot light source. In this constitution, the image may be formed small on the small reflector 114. Therefore, of the light transmitted through the integrators 107 and 108, the rate of the light cut off by the small reflector 114 is small, so that the effective utilization efficiency of light is enhanced. Likewise, it is also effective to use a large condenser lens 111 to reduce the light source image so as to reduce the size of the small reflector 114, and dispose a relay lens at the exit side of the small reflector 114 so as to illuminate the necessary region on the irradiation surface 109. The light traveling on the first optical axis 103 and passing through the polarization beam splitter 105 can illuminate uniformly by the integrators 107 and 108. However, the light traveling on the second optical axis 106 and reflected by the polarization beam splitter 105 may possibly cause uneven colors somewhat on the irradiation surface 109 if the luminous portion of the light source is uneven in color. In the event of such color unevenness, by disposing a rod type integrator near the small reflector 114, the color uniformity may be enhanced also in the light reaching up to the irradiation surface 109 through the small reflector 114. In the embodiment, as the transforming means of direction of polarization, the phase difference plate of polarization transforming means is used, but not limited to this, it is also possible to use means disposed on the surface of the polarization beam splitter 105 passing after the optical path is split in the direction of polarization by the polarization beam splitter 105, on the reflectors 110, 112, or on the condenser lens 111. The transforming means of the direction of polarization is provided on the optical path of the second optical axis 106 side, being reflected by the polarization beam splitter 105, but instead of this constitution, it may be also disposed on the optical path of the light traveling onto the first optical axis 103 after passing through the polarization beam splitter 105. The same characteristics are obtained if disposed on either side. The invention is not limited by the transforming means of direction of polarization. In the embodiment, the parabolic reflector 104 is used as the means for controlling the light of the light source 101, but this is not limitative. For example, it may be replaced by an elliptical mirror, the light source may be set at its first focal point position, and the small reflector 114 may be set at the second focal point position. In this constitution, the condenser lens 111 is not required. If, however, the parallelism of the light entering the polarization beam splitter 105 is poor, the degree of splitting by the direction of polarization drops, and therefore a constitution short in the distance between focal points is not preferred. It is also possible to compose by comprising means for transforming into parallel light. The position of the small reflector 114 is preferred to be on the first optical axis 103 or on the central line symmetrically dividing the irradiation surface 109, but it is not particularly limited as far as it is within a practically permitted range. (Embodiment 10) A different embodiment of the lighting device transformed in the direction of polarization of the invention is described in Fig. 12. In embodiment 9, the small reflector 114 is disposed at the exit side of the second integrator array 108, whereas in this embodiment, as shown in Fig. 12, the small reflector 114 is disposed between the first integrator array 107 and second integrator array 108. In this constitution, the same effect as in embodiment 9 is obtained. Furthermore, in the direction of the first optical axis 103, the lighting device transformed in the direction of polarization can be constituted in a smaller scale. In Fig. 12, an aperture 115 of the second integrator lens array 108 is disposed in the passing area of the light through the small reflector 114, but instead of this constitution, it is also possible to compose a parallel flat plate in the passing area of the light through the small reflector 114, and in this constitution, as the light through the small reflector 114 passes through the second integrator lens array 108, it reaches the target of the irradiation surface 109. It is further possible to constitute by comprising a lens for illuminating the irradiation surface 109 most efficiently by the light through the small reflector 114 positively, and the degree of freedom of design is enhanced by this constitution. In the case of a rectangular shape of the illuminated surface 109, it is preferred to dispose a lens in a shape asymmetrical in vertical and lateral directions. (Embodiment 11) A different embodiment of the lighting device transformed in the direction of polarization of the invention is described in Fig. 13. In Fig. 13, the light reflected by the polarization beam splitter 105 as the polarization selecting means is transformed into nearly parallel light reduced in the luminous flux by luminous flux width transforming lenses 116 and 117 as luminous flux transforming means, and then enters a small reflector 118 which is optical path transforming means. This small reflector 118 is formed in a curvature so that the light reflected by it may be superposed in the range illuminated by the second integrator lens array 108. In this constitution, the regulation of the condensing position is not strict, and the degree of freedom of design of the condenser lens is larger. Or, as shown in Fig. 14, it is also possible to install a projector lens 120 at the exit side of the small reflector 119. In this constitution, the same effects as in the embodiment in Fig. 13 are obtained. Embodiment 9 through embodiment 11 relate to examples of using the polarization beam splitter 105 as the polarization selecting means for splitting the optical path by the direction of polarization. Generally, however, the transmitted light and reflected light of the polarization beam splitter 105 are mutually different in characteristics. Therefore, to obtain the optimum characteristic, it is preferred to select the light of either optical path to be transformed in polarization. Fig. 15 shows an example of disposing integrator means at the reflected light side of the polarization beam splitter 105. In this constitution, further excellent characteristics may be obtained. (Embodiment 12) A different embodiment of the lighting device transformed in the direction of polarization of the invention is described in Fig. 16. In Fig. 16, a polarization beam splitter 22 having a half incident area as compared with the polarization beam splitter described in the foregoing embodiments is divided into two pieces, and two polarization beam splitters 122 divided into two pieces each are constituted. In this way, by comprising a plurality of polarization selecting means, the incident light is split into a second optical axis 123 and a third optical axis 124, and the irradiation surface 109 is illuminated by a small reflector 125. At this time, the volume of two polarization beam splitters 122 is half that of the polarization beam splitter 105, and the cost is lowered, and hence the size and weight are reduced. In this embodiment, two polarization beam splitters are arranged parallel, but instead the same effects are obtained by one polarization beam splitter having a similar reflection plane. Fig. 17 shows an illustrative example of a lighting device transformed in the direction of polarization using the polarization beam splitter 122. In this example, the small reflector 125 which is the optical path transforming means is disposed at the outside or near the second integrator array 108. In this example, the projection lens is required to have such a brightness as to take in up to the position of the small reflector 125, but since the small reflector 125 is very small as compared with the second integrator array 108, significant change is not required. When the position of the small reflector 125 is located at the exit side of the effective aperture on the second integrator array 108, it is not always required to be located in its center as described so far, and it is preferred to dispose the small reflector 125 at position of weak distribution of illumination. In this case, it is preferred to locate the irradiation surface at a position corresponding to the central line to be split symmetrically. Or in the case of disposing plural small reflectors 125, they are preferred to be disposed symmetrically on both sides of the central line. The shape of the irradiation surface 109 and the shape of the light source image coming out through the polarization beam splitter 122 are similar, and the constituent elements are disposed so as to adjust the magnifying power of these shapes, so that the greatest brightness may be obtained. As a result, the polarization transforming efficiency is enhanced. In the further illustrative example of Fig. 18, a condenser lens 111 is provided on the exit plane of the polarization beam splitter 122, and the exit light is split optically. In this constitution, each shape of the exit light is similar to the shape of the irradiation surface 109 and is superposed on the irradiation surface 109. By thus constituting, the utilization efficiency of light is extremely heightened. Moreover, by splitting the output of the polarization selecting means 122 into plural rays of light and superposing on the irradiation surface 109 in this way, color unevenness in the light source is made less obvious by superposing, and the uniformity of color can be enhanced. In this embodiment, to adjust the magnifying factor, the small reflector 125 is disposed so that the polarized and transformed light may travel across the front surface of the second integrator array 108. Besides, since the condenser lens 111 is set at a position having the center of curvature deviated to the incident light as required, each split image is superposed at the same position on the irradiation surface 109. (Embodiment 13) Other embodiment of the lighting device transformed in the direction of polarization of the invention is described by reference to Fig. 19. In Fig. 19, the light emitted from a light source 101 is reflected by a parabolic reflector 104, and enters a polarization beam splitter 105. The parabolic reflector 104 is disposed in rotational symmetricity to a first optical axis 103 so that the light source 101 may be positioned at a focal point position 102. The polarization beam splitter 105 reflects the S-polarized light, and causes the S-polarized light to travel onto a second optical axis 106. The P-polarized light passes through the reflection plane of the polarization beam splitter 105, and is further condensed on a small aperture 135 provided in a combined reflector 134 disposed obliquely to the optical axis 103 by a condenser lens 133, and passes through it and illuminates on the irradiation surface 109. On the other hand, the light traveling up to the second optical axis 106 passes through a phase difference plate 113 as polarization transforming means, and the direction of polarization is transformed. The phase difference plate 113 is set so as to be same in the direction of polarization as the direction of polarization of the light traveling on the first optical axis 103. Afterwards, the light is reflected by the reflector 110 disposed obliquely to the optical axis, and is put into the first integrator array 136 of the integrator means. The incident light is divided by each lens of the first integrator array 136. The split light is guided by a reflector 137, and a secondary light source image is formed on the lens of the second integrator lens array 138 of each corresponding integrator means. The light emitted therefrom is reflected by the combined reflector 134 of the optical path transforming means, and then magnified views are superposed and formed on the irradiation surface 109. In this embodiment, too, most of the light emitted from the light source 101 is emitted as light in one direction of polarization only to illuminate. In the embodiment, the light source 101 is preferred to be close to a spot light source. This is because the image on the aperture is formed small, and the rate of escaping through the small aperture 135 is small in the light passing through the integrator means. Similarly, using a large condenser lens 133 for reducing the light source image so as to decrease the size of the small aperture 135, it is effective to dispose a relay lens at the exit side of the small aperture 135 for illuminating the necessary region on the irradiation surface 109. Such constitution is also possible. The light traveling on the second optical axis 106 and reflected by the polarization beam splitter 105 can illuminate uniformly through integrator means 136 and 138. However, the light traveling on the first optical axis 103 and passing through the polarization beam splitter 105 may possibly cause uneven colors on the irradiation surface 109 somewhat if there is color unevenness in the luminous portion of the light source. In the event of such color unevenness, by disposing a rod type integrator in the small aperture 135 (or its vicinity), the color uniformity may be enhanced also in the light reaching up to the irradiation surface 109 through the small aperture 135. The position of the small aperture 135 is preferably on the first optical axis 103 or on the central line in the symmetrical position of the irradiation surface 109, but this is not particularly limited as far as it is within a practically permissible range. In this embodiment, too, same as in embodiment 1, the optical path reflected by the polarization beam splitter may be constituted in two divided sections. (Embodiment 14) An embodiment of projection type image display device of the invention is described while referring to Fig. 20. Fig. 20 is a structural diagram of the projection type image display device using the lighting device transformed in the direction of polarization of embodiment 9 described in Fig. 11. The light from a light source 101 enters a field lens 126 as combined light of same polarized light as explained in embodiment 9 in Fig. 11 is emitted from a lighting device transformed in the direction of polarization 200. At this time, it is arranged so that the position of the irradiation surface 109 may correspond to a liquid crystal surface 127. The telecentric property is realized as the light entering the field lens 126 may be same in incident angle regardless of the height of ray of the principal ray of light relative to the liquid crystal surface 127. The light passing through the field lens 126 is limited to polarized light in one direction only by an incident side polarizer 128. The direction of polarization is limited by the lighting device transformed in the direction of polarization 200 before entering the incident side polarizer 128. If, however, the degree of polarization is insufficient due to performance of the polarization beam splitter 105 and random reflection on the interface, and projected image having a sufficient contrast cannot be obtained, it is preferred to install a polarizer 128. Depending on the necessity, however, it is also possible to constitute without polarizer 128. The light passing through the incident side polarizer 128 gets into a liquid crystal panel 129. The liquid crystal panel 129 is composed of multiple picture elements controllable independently from external signal, and the light entering the picture elements of the portion to be displayed in white of the image display portion of the liquid crystal panel passes through the incident side polarizer 128 and is twisted 90 degrees in the direction of polarization by the liquid crystal surface 127, and hence passes through an exit side polarizer 130 orthogonal to the direction of polarization passing through the incident side polarizer 128. On the other hand, the light entering the picture elements in the portion to be displayed in black of the image display portion of the liquid crystal panel 129 passes through the incident side polarizer 128, and passes through the liquid crystal surface 127 without being twisted of direction of polarization, and gets into the exit side polarizer 130 and is absorbed. The image display means is composed of the liquid crystal panel 129, incident side polarizer 128 and exit side polarizer 130. The light passing-through the exit side polarizer 130 is guided onto the screen 132 by projection lens 131. In this way, by magnifying and projecting the picture elements in the display area of the liquid crystal panel 129 by projection lens 131, a large image is obtained on the screen 132. In the conventional liquid crystal panel, only light in one direction of polarization can be utilized, and hence only about 50% of the light from the light source can be absorbed in the incident side polarizer. It was hence difficult to heighten the luminance due to low utilization rate of light, large heat generation by absorption of light by the incident side polarizer, and deterioration of parts by heat generation. By contrast, according to the embodiment, the light from the light source is fully utilized, and the light utilization efficiency is heightened, and the projection type image display device having high luminance and excellent reliability may be obtained. In the embodiment, the transmission type liquid crystal panel 129 is used as the light valve, but it is also possible to use a device for displaying by using polarization instead, and, for example, a reflection type liquid crystal panel can be also used. (Embodiment 15) Other embodiment of the projection type image display device of the invention is described by referring to Fig. 21. Fig. 21 is a structural diagram of a projection type image display device using the lighting device transformed in the direction of polarization 300 of embodiment 13 explained in Fig. 19. The light from the light source 101 is emitted from the lighting device transformed in the direction of polarization 300 of embodiment 13 shown in Fig. 19, and gets into the field lens 126. At this time, it is arranged so that the position of an irradiation surface 132 may correspond to the liquid crystal surface 127. The telecentric property is realized as the light entering the field lens 126 may be same in incident angle regardless of the height of ray of the principal ray of light relative to the liquid crystal surface 127. The light passing through the field lens 126 is limited to polarized light in one direction only by an incident side polarizer 128. The direction of polarization is limited by the lighting device transformed in the direction of polarization 300 before entering the incident side polarizer 128. If, however, the degree of polarization is insufficient due to performance of the polarization beam splitter 105 and random reflection on the interface, and projected image having a sufficient contrast cannot be obtained, it is preferred to install a polarizer in this manner. The light passing through the incident side polarizer 128 gets into a liquid crystal panel 129. The liquid crystal panel 129 is composed of multiple picture elements controllable independently from external signal, and the light entering the picture elements of the portion to be displayed in white of the image display portion of the liquid crystal panel passes through the incident side polarizer 128 and is twisted 90 degrees in the direction of polarization by the liquid crystal surface 127, and hence passes through an exit side polarizer 130 orthogonal to the direction of polarization passing through the incident side polarizer 128. On the other hand, the light entering the picture elements in the portion to be displayed in black of the image display portion of the liquid crystal panel 129 passes through the incident side polarizer 128, and passes through the liquid crystal surface 127 without being twisted of direction of polarization, and gets into the exit side polarizer 130 and is absorbed. The light passing through the exit side polarizer 130 is guided onto the screen 132 by projection lens 131. In this way, by magnifying and projecting the picture elements in the display area of the liquid crystal panel 129 by projection lens 131, a large image is obtained on the screen 132. In the conventional liquid crystal panel, only light in one direction of polarization can be utilized, and hence only about 50% of the light from the light source can be absorbed in the incident side polarizer. It was hence difficult to heighten the luminance due to low utilization rate of light, large heat generation by absorption of light by the incident side polarizer, and deterioration of parts by heat generation. By contrast, according to the embodiment, the light from the light source is fully utilized, and the light utilization efficiency is heightened, and the projection type image display device having high luminance and excellent reliability may be obtained. In the embodiment, the transmission type liquid crystal panel is used as the light valve, but it is also possible to use a device for displaying by using polarization instead, and, for nexample, a reflection type liquid crystal panel can be also used. In embodiment 1 through embodiment 15, the types of transmitted light and reflected light in the polarization selecting means (that is, S-polarized light and P-polarized light) are not particularly limited to the specified forms, but if the S-polarized light and P-polarized light are reverse, the same effects as in the embodiments are obtained. Thus, in the device for controlling the output by utilizing polarization using liquid crystal panel or the like as light valve, the conventional lighting device transformed in the direction of polarization could make use of light only in one direction of polarization, whereas the lighting device transformed in the direction of polarization of the invention can transform both P- and S-polarized light into one direction of polarization, and superpose the exit light on one optical axis. Therefore, the utilization efficiency of light is extremely heightened. As a result, the brightness is about twice as large as in the prior art. Therefore, to obtain the lighting device of same brightness, the power consumption is saved to half. Moreover, the light source and driving circuit are reduced in size and lowered in price. The projection type image display device using the lighting device transformed in the direction of polarization can prevent entry of light in undesired direction of polarization in the light control unit of image display means such as liquid crystal panel, and heat generation decreases, so that the projection type image display device of excellent reliability and high luminance is obtained.

Claims: A lighting device for supplying light transformed in the direction of polarization comprising: a light source (1), polarization selecting means (6) for separating a light from the light source into a first polarized light and a second polarized light, polarization transforming means (10) for transforming the first polarized light into a transformed second polarized light, and optical path transforming means (13) for reflecting the transformed second polarized light, and the transformed second polarized light reflected by the optical path transforming means and the second polarized light separated by the polarization selecting means are combined mutually in the same direction, characterized in that the optical path transforming means has an aperture (11) in its central region, and the polarization selecting means (6) is positioned at the aperture. A device according to claim 1, and comprising luminous flux transforming means (116,117) for changing the width of luminous flux to transform the second polarized light into a luminous flux transformed second polarized light, and wherein the transformed second polarized light reflected by the optical path transforming means and the luminous flux transformed second polarized light transformed in luminous flux by the luminous flux transforming means are combined mutually in a same direction. A lighting device according to claim 1 or 2 and comprising reflecting means for reflecting the transformed second polarized light emitted from the polarization transforming means, and feeding it again into the polarization transforming means, wherein the transformed second polarized light reflected by the reflecting means and passing again through the polarization transforming means is reflected by the optical path transforming means, and the reflected transformed second polarized light and the second polarized light separated by the polarization selecting means are combined mutually in a same direction. A lighting device according to claim 3, further comprising: parallel light transforming means disposed between the polarization transforming means and optical path transforming means, wherein the parallel light transforming means transforms the transformed second polarized light from the polarization transforming means into second polarized light having parallel light. A lighting device according to claim 3, wherein the polarization selecting means is a plane type polarization beam splitter. A lighting device for supplying light transformed in the direction of polarization comprising: a light source (1), polarization selecting means (6) for separating a light from the light source into a first polarized light and a second polarized light, reflecting means (16) for reflecting the first polarized light emitted from the polarization selecting means, optical path transforming means for reflecting the first polarized light from the reflecting means, and polarization transforming means for transforming the first polarized light reflected by the optical path transforming means into a transformed second polarized light, and the transformed second polarized light and the second polarized light separated by the polarization selecting means are combined mutually in the same direction, characterised in that the optical path transforming means has an aperture in its central region, and the polarization selecting means is positioned at the aperture. A lighting device according to claim 6, wherein the polarization transforming means has an aperture in its central region, and the second polarized light separated by the polarization selecting means passes through the aperture. A lighting device according to claim 6, wherein the light source means emits a parallel light, and the device further comprises luminous flux transforming means for transforming the first polarized light into a luminous flux transformed first polarized light having a luminous flux different from the luminous flux of the second polarized light, optical path transforming means being arranged to reflect the luminous flux transformed first polarized light, and polarization transforming means being arranged to transform the luminous flux transformed first polarized light into a transformed second polarized light. A lighting device according to claim 6 or 7, and comprising luminous flux magnifying means for magnifying the luminous flux width to transform the first polarized light into a magnified first polarized light having a magnified luminous flux, wherein the magnified second polarized light reflected by the optical path transforming means, and the transformed second polarized light separated by the polarization selecting means are combined mutually in a same direction. A lighting device according to any one of the preceding claims wherein the polarization transforming means has an aperture in its central region, and the light from the light source passes through the aperture in the optical path transforming means and the aperture, in the polarization transforming means. A lighting device according to claim 2, wherein the luminous flux transforming means is arranged to reduce the luminous flux width to transform the transformed second polarized light into a narrow luminous flux width second polarized light. A lighting device according to any one of the preceding claims and comprising integrator means for separating the first polarized light into a plurality of first polarized lights, and wherein the polarization transforming means is arranged to transform the plurality of first polarized lights into a transformed second polarized light. A lighting device according to claim 12, wherein the integrator means is composed of a plurality of micro lenses. A projection type image display device comprising: (a) a lighting device according to any one of the preceding claims, (b) image display means for transforming the combined light combined by the lighting device transformed in the direction of polarization into an image light; and (c) projection means for projecting the image light transformed by the image display means.

Inventors: YAMAGISHI SHIGEKAZU, YAMAGISHI, SHIGEKAZU
Applicants: MATSUSHITA ELECTRIC IND CO LTD, MATSUSHITA ELECTRIC INDUSTRIAL CO., LTD.
Application year: 1996
Main classification: H04N9
IPC codes: G03B21, G02F1, H04N5, G02B27, H04N9