JP4886254B2 - Optical system and image projection apparatus - Google Patents

Description

  The present invention relates to an optical system that is used in an image projection apparatus or the like and guides a light beam from a light source to a light separation surface.

  The image projection apparatus projects a light beam modulated by an image forming element such as a liquid crystal panel on a projection surface such as a screen by using a projection lens. In such an image projection apparatus, it is important that the image projected on the projection surface has substantially uniform brightness throughout.

  In a conventional image projection apparatus (see, for example, Patent Document 1), an illumination optical system that guides illumination light to an image forming element includes a light source and a paraboloid reflector that reflects a light beam emitted from the light source into a substantially parallel light beam. And have. The parallel light beam is divided and condensed by a first fly-eye lens in which a plurality of minute spherical lenses are two-dimensionally arranged.

  The plurality of divided light beams form a plurality of secondary light source images in the vicinity of the second fly-eye lens provided with a plurality of lenses corresponding to the plurality of lenses constituting the first fly-eye lens. The lenses constituting the first and second fly-eye lenses have a rectangular shape similar to the liquid crystal panel that is the illuminated surface.

Further, the plurality of split light beams emitted from the second fly-eye lens are collected by a condenser lens and illuminate the liquid crystal panel in a superimposed manner through a color separation optical system. In the color separation optical system, an optical film such as a dichroic film or a polarization separation film is used as a color separation surface arranged to be inclined with respect to the optical axis.
JP 2004-126696 A

  In such an image projection apparatus, in order to increase the utilization efficiency of the light emitted from the light source, an optical system that condenses the light beam from the light source at a large angle is often used. In this case, the angular distribution of the light beam incident on the optical film is increased.

  However, as described above, when an optical film whose characteristics are likely to change depending on the incident angle of the light beam is used in the color separation optical system, so-called leakage light (for example, light that should originally be reflected by the light separation surface). However, light that passes through the light separation surface is generated. As a result, color unevenness and brightness unevenness occur in the projected image, and the contrast of the image decreases. That is, image quality deterioration occurs.

  The present invention provides an optical system capable of increasing the light use efficiency from the light source while minimizing the generation of light leakage on the light separation surface when guiding the light flux from the light source to the light separation surface. One of the purposes is to do.

An optical system according to an aspect of the present invention is an optical system that guides a light beam from a light source to a light separation surface inclined with respect to a central axis of the optical system, and a part of the light beam reaches the light separation surface. A light flux restricting member for restricting the light beam, and the light flux restricting member includes a central axis and a second surface orthogonal to the first surface including the central axis and a normal line of the light separation surface. A region having an asymmetric shape with respect to the light beam separation surface from the light flux limiting member, and a region on the side where the central axis and the light separation surface with the central axis as a boundary form an obtuse angle; When the first region is set, the center of the light passage opening formed in the light flux limiting member is displaced in the first region with respect to the central axis, and the optical system is located on the first surface. A first lens array for dividing a light beam from the light source into a plurality of light beams in a parallel direction; And a second lens array having a plurality of lenses corresponding to the plurality of lenses constituting the Zuarei, and satisfies the following condition. p / 30 ≦ t ≦ p / 5. Where t is the amount of deviation of the center of the light passage aperture with respect to the central axis, and p is the lens pitch of the second lens array.

  According to the present invention, since the light beam limiting member has an asymmetric shape with respect to the surface including the central axis of the optical system, the angle component that is likely to leak light on the light separation surface among the light beams in one region sandwiching the central axis. Can be blocked, and the light flux in the other region can sufficiently reach the light separation surface. Therefore, it is possible to increase the light use efficiency from the light source while minimizing the occurrence of leakage light on the light separation surface.

  By using such an optical system as an optical system for illuminating the image forming element for image projection, the image forming element can be illuminated with uniform brightness, and there is little color unevenness and brightness unevenness and high contrast. A projected image can be obtained.

  Embodiments of the present invention will be described below with reference to the drawings.

  FIG. 1 shows a schematic configuration of an illumination optical system that is Embodiment 1 of the present invention. In FIG. 1, 1 is an arc tube, and 2 is a reflector that reflects a light beam emitted from the arc tube 1 and converts it into a substantially parallel light beam. Hereinafter, the arc tube 1 and the reflector 2 are collectively referred to as a light source.

  A polarization conversion element 13 converts a non-polarized illumination light beam from the light source (reflector 2) into linearly polarized light having a predetermined polarization direction S. Reference numeral 12 denotes a stop as a light beam limiting member that blocks a part of the illumination light beam emitted from the polarization conversion element 13.

  Reference numeral 10 denotes a polarization beam splitter having a polarization separation surface 14 formed of a multilayer film. The polarization separation surface 14 reflects the polarized light having the polarization direction S in the illumination light flux that has passed through the diaphragm 12 and transmits the polarized light having the polarization direction P orthogonal to the polarization direction S. Reference numeral 11 denotes a reflective liquid crystal panel as an image forming element illuminated by the illumination light beam reflected by the polarization separation surface 14. The reflection direction of the illumination light beam on the polarization separation surface 14 is the short side direction of the liquid crystal panel 11.

  The reflective liquid crystal panel 11 reflects the incident illumination light beam, modulates the image, and emits an image light beam having a polarization direction 23. The image light flux passes through the polarization separation surface 14 and is guided in a direction 24 of a projection lens (not shown).

  C indicates the central axis of the illumination optical system, and in this embodiment, coincides with the optical axis AXL of the illumination optical system. The center axis C will be described later. n is a normal line of the polarization separation surface 14.

  2A and 2B show a more detailed configuration of the illumination optical system. 2A and 2B show a cross-section of the illumination optical system shown in FIG. 1 developed along the central axis C of the illumination optical system.

  Here, in this embodiment, the direction in which the central axis C extends, that is, the traveling direction of the light flux is defined as the z direction, and the cross section including the normal axis n of the central axis C and the polarization separation surface 14 is the xz cross section (first surface). And The x direction (second direction) is a direction parallel to the xz section and perpendicular to the central axis C, and corresponds to the short side direction of the liquid crystal panel 11. FIG. 2B shows an xz section of the illumination optical system.

  In this embodiment, the direction perpendicular to the xz cross section and the central axis C is the y direction (first direction). The yz section (second surface) is a section that includes the central axis C and is orthogonal to the xz section. FIG. 2A shows a yz section of the illumination optical system.

  2A and 2B, the polarization conversion element 13 shown in FIG. 1 is omitted.

  In the xz cross section shown in FIG. 2B, the incident angle distribution of the illumination light beam on the polarization separation surface 14 and the liquid crystal panel 11 is narrower than that in the yz cross section shown in FIG. 2A.

  The light beam emitted radially from the arc tube 1 is converted into a substantially parallel light beam by the reflector 2 having a parabolic reflection surface. As shown in FIG. 2A, the substantially parallel light beam is divided into a plurality of light beams by the a-cylindrical lens array 3 in the yz section (y direction). A schematic shape of the a-cylindrical lens array 3 is shown in FIG. Each cylindrical lens 3 a of the a-cylindrical lens array 3 condenses each divided light beam and forms a first light source image in the vicinity of the b-cylindrical lens array 4. In the b-cylindrical lens array 4, a plurality of cylindrical lenses corresponding to each of the plurality of cylindrical lenses formed in the a-cylindrical lens array 3 are formed. The a-cylindrical lens array 3 forms a plurality of first light source images at positions corresponding to the plurality of cylindrical lenses constituting the b-cylindrical lens array 4.

  FIG. 5A shows a plurality of first light source images formed by the action of the a-cylindrical lens array 3 in this embodiment. FIG. 5A shows the state of the first light source image when viewed from the z direction. In FIG. 5A, a yz cross section (y direction) is indicated by a one-dot chain line. Further, the width of the region where the first light source image is formed in the y direction is W1. Note that W1 indicates the maximum width of the widths of the first light source images obtained when the illumination optical system is cut along various cross sections parallel to the yz cross section.

  Since the a, b-cylindrical lens arrays 3 and 4 have refractive power only in the yz section, the light flux is not substantially affected in the xz section orthogonal to the yz section.

  The illumination light beam emitted from the b-cylindrical lens array 4 enters an afocal optical system 5 as a compression optical system. The afocal optical system 5 is an optical system that emits a parallel light beam from the b-cylindrical lens array 4 as a parallel light beam while narrowing the light beam diameter in the xz cross section (x direction).

  The illumination light beam emitted from the afocal optical system 5 enters the c-cylindrical lens array (first cylindrical lens array) 6. The c-cylindrical lens array 6 divides the illumination light beam into a plurality of light beams in the xz cross section (x direction). Each cylindrical lens of the c-cylindrical lens array 6 condenses each divided light beam and forms a second light source image near the d-cylindrical lens array (second cylindrical lens array) 7. In the d-cylindrical lens array 7, a plurality of cylindrical lenses corresponding to each of the plurality of cylindrical lenses formed in the c-cylindrical lens array 6 are formed. The c-cylindrical lens array 6 forms a plurality of second light source images at positions corresponding to the plurality of cylindrical lenses constituting the d-cylindrical lens array 7.

  FIG. 5B shows a plurality of second light source images formed by the action of the c-cylindrical lens array 6 in this embodiment. FIG. 5B shows a state of the second light source image when viewed from the z direction. In FIG. 5B, the xz cross section (x direction) is indicated by a one-dot chain line. Further, the width of the region where the second light source image is formed in the x direction is W2. W2 indicates the maximum width of the width of the second light source image obtained when the illumination optical system is cut along various cross sections parallel to the xz cross section.

  Reference numeral 8 denotes a condenser lens having the same refractive power in the xz cross section and the yz cross section. Reference numeral 9 denotes a cylindrical lens having a refractive power only in the xz section.

  The afocal optical system 5, the c, d-cylindrical lens arrays 6 and 7, and the cylindrical lens 9 do not have refractive power in the yz section. Accordingly, the plurality of split light beams emitted from the b-cylindrical lens array 4 are not influenced by these optical elements in the yz section, but are collected by the condenser lens 8, pass through the polarization beam splitter 10, and then reflected by the reflective liquid crystal panel 11. Are illuminated in a superimposed manner.

  On the other hand, the plurality of split light beams emitted from the d-cylindrical lens array 7 are subjected to the condensing action of the condenser lens 8 and the cylindrical lens 9 in the xz cross section, and pass through the polarizing beam splitter 10 to superimpose the reflective liquid crystal panel 11. Illuminate.

  In the present embodiment, the ad lens cylindrical arrays 3, 4, 6, and 7 have an odd number of cylindrical lenses. For this reason, the illumination light flux passes through the cylindrical lens in the center of the ad cylindrical lenses arrays 6 and 7 and further passes through the center (optical axis) of the condenser lens 8 to the center of the effective image forming area of the liquid crystal panel 11. There are rays that are incident perpendicularly. The optical path followed by the central ray coincides with the central axis C of the illumination optical system and is also the optical axis AXL of the illumination optical system.

  Further, when the a, b-cylindrical lens arrays 3 and 4 or the c, d-cylindrical lens arrays 6 and 7 have an even number of cylindrical lenses, the central ray does not exist. That is, there is a boundary between the cylindrical lenses on the optical path through which the central ray should pass. In this case, a virtual line perpendicular to the center (optical axis) of the condenser lens 8 and the center of the effective image forming area of the liquid crystal panel 11 becomes the central axis C of the illumination optical system.

  The x direction is a direction in which the generatrix of the cylindrical lenses constituting the a, b-cylindrical lens arrays 3 and 4 extends, and the xz section includes a central axis C and is a plane parallel to the generatrix direction of the cylindrical lenses. It can be said that there is.

  Further, the y direction is a direction in which the generatrix of the cylindrical lenses constituting the c, d-cylindrical lens arrays 6 and 7 extends, and the yz section includes a central axis C and is a plane parallel to the generatrix direction of the cylindrical lenses. It can be said that there is.

In the present embodiment, in the region from the light source in the xz cross section shown in FIG. 2B to the polarization separation surface 14 through the stop 12, the central axis C and the polarization separation surface 14 are obtuse angles α ( A region on the side forming 135 ° is generally referred to as a first region A. In addition, a region on the side where the central axis C and the polarization separation surface 14 form an acute angle (generally 45 °) is referred to as a second region B. In this embodiment, between the c, d-cylindrical lens arrays 6 and 7. In addition, a diaphragm 12 is arranged.

  Next, the shape of the diaphragm 12 in the present embodiment will be described with reference to FIG. FIG. 3 shows a state in which the diaphragm 12 is viewed from the z direction. The aperture (diaphragm aperture) 12a of the aperture 12 is formed in a hexagonal shape in which the aperture width in the x direction is narrower than the aperture width in the y direction. That is, in the x direction and the y direction, the area ratio of the light shielding portion with respect to the diaphragm opening 12a in the diaphragm 12 increases as the distance from the central axis C increases.

Further, in the x direction, the center AC of the stop aperture 12a is shifted toward the first region A described above with respect to the central axis C of the illumination optical system (the shift amount is indicated by t). In other words, the diaphragm 12 has an asymmetric shape with respect to the yz section in the x direction. More specifically, in FIG. 3, the distance a from the inner end of the stop aperture 12a on the first region A side to the central axis C of the illumination optical system, and the inner side of the stop aperture 12a on the second region B side. Between the distance b from the end to the central axis C,
a> b
There is a relationship.

  For this reason, the angular distribution of rays incident on the polarization separation surface 14 is asymmetric with respect to the x direction. As a result, as shown in FIG. 4, the center P2C of the pupil P2 of the illumination optical system provided with the stop 12 is shifted by the shift amount t with respect to the center P1C of the pupil P1 of the illumination optical system not provided with the stop 12. .

  In other words, when there is no stop 12, the light beam that goes to the polarization separation surface 14 at a large angle with respect to the central axis C in the second region B is blocked by the stop 12. On the other hand, a light beam having the same angle as the light beam blocked in the first region A passes through the aperture 12a and reaches the polarization separation surface 14. In the second light source image shown in FIG. 5B, the outermost (upper) hatched portion D on the second region B side is cut off.

  For this reason, if the shift amount t is set so as to block only the components that are likely to be leaked light on the polarization separation surface 14 out of the light flux passing through the second region B, the generation of leakage light on the polarization separation surface 14 is reduced. However, the amount of illumination light of the liquid crystal panel 11 can be hardly reduced. Therefore, a bright projected image with high contrast can be obtained.

  Here, the shift amount t desirably satisfies the following conditions.

p / 30 ≦ t ≦ p / 5 (1)
Here, p is the lens pitch of the d-cylindrical lens array (second cylindrical lens array) 7.

  If the shift amount t is less than the lower limit value of the expression (1), the light flux component that tends to be leaked light on the polarization separation surface 14 cannot be sufficiently blocked. On the other hand, if the shift amount t exceeds the upper limit value of the equation (1), the light beam component that is not easily leaked by the polarization splitting surface 14 is blocked, and the light use efficiency is lowered. The lower limit is more preferably p / 25, and even more preferably p / 20. The upper limit is more preferably p / 8, and even more preferably p / 10.

In this embodiment, p = 3.0 mm (desirably within a range of 2.5 to 3.5 mm), and t is within a range of 0.2 mm (0.16 mm to 0.25 mm). Is desirable).
Further, in this embodiment, as can be seen by comparing FIG. 5A and FIG. 5B, the width W2 of the second light source image in the xz section is larger than the width W1 of the first light source image in the yz section. narrow. The magnitude relationship (ratio) between W1 and W2 is the magnitude relationship of the angular distribution of the light beam incident on the polarization beam splitter 10 (polarization separation surface 14) as it is. For this reason,
W1> W2
Relationship, more preferably,
0.1 <W2 / W1 <0.8
It is desirable that

  In this embodiment, the case where the diaphragm 12 is arranged between the c, d-cylindrical lens arrays 6 and 7 has been described, but it may be arranged at another position. For example, the diaphragm 12 may be disposed closer to the polarizing beam splitter 10 than the d-cylindrical lens array 7. It is desirable to dispose the stop at a position closer to the second light source image formed by the c-cylindrical lens array 6 than at least the first light source image formed by the a-cylindrical lens array 3. Thereby, it is possible to reliably block the light flux that tends to be leaked light on the polarization separation surface 14.

  In addition, the central axis C of the illumination optical system is actually an optical system part closer to the polarization beam splitter 10 than the polarization conversion element 13 with respect to the central axis of the light source side optical system part from the light source to the polarization conversion element 13. The center axis of is shifted in the y direction. This is because inside the polarization conversion element 13, a part of the light beam is reflected in the y direction by the polarization separation film, and further reflected by the reflecting surface in the z direction and emitted.

In this case, the aperture center C of the diaphragm 12 is shifted by t with respect to the beam splitter side center axis in the same direction as the beam splitter side center axis with respect to the light source side center axis, that is, the optical axis shift direction of the condenser lens 8. Good. Thereby, the relationship between the original pupil P1 of the illumination optical system (the optical system portion on the beam splitter 10 side) and the pupil P2 formed by providing the stop 12 is the same as in FIG.
The central axis is an optical path of a light beam passing through the optical axis of the lens when a lens having rotational symmetry or refractive power in the x direction and y direction is arranged downstream of the polarization conversion element 13. Moreover, it is good also as an optical path of the light ray which passes along the central axis of the reflector 2 of a light source. Further, it may be an optical path of a light beam incident perpendicular to the center of the liquid crystal panel. Although these rays may not actually exist, they can be considered as an optical path followed by the rays when such rays are present.

  FIG. 6 shows the shape of the diaphragm 22 in the illumination optical system according to the second embodiment of the present invention. In this embodiment, the shape is a combination of an isosceles triangle having a base that is long in the y direction and a trapezoid having a base that is long in the y direction, with the yz section including the central axis C of the illumination optical system as a boundary.

  Also in the present embodiment, in the x direction and the y direction, the area ratio of the light shielding portion with respect to the diaphragm opening 22a in the diaphragm 22 increases as the distance from the central axis C increases.

In the x direction, the center AC of the aperture 22a is shifted to the first region A side described in the first embodiment with respect to the central axis C of the illumination optical system (shift amount t). In other words, the diaphragm 22 has an asymmetric shape with respect to the yz section in the x direction. And like Example 1,
a> b
There is a relationship. Even when the diaphragm 22 of this embodiment is used in place of the diaphragm 12 of the first embodiment, the same effects as those of the first embodiment can be obtained.

FIG. 7 shows the shape of the diaphragm 32 in the illumination optical system according to the third embodiment of the present invention. The diaphragm 32 of the present embodiment is similar to the first and second embodiments,
a> b
And the aperture opening end on the first region A side is open (that is, there is no aperture opening end). Further, the aperture opening end in the y direction is formed in an uneven shape. In the present embodiment, in the x direction, the area ratio of the light shielding portion with respect to the stop aperture 32a increases as the distance from the central axis C increases.

  Depending on the optical characteristics of the illumination optical system, the illumination of the liquid crystal panel 11 can be optimized by providing the diaphragm 32 having such a complicated shape. Of course, the same effect as that of the first embodiment can be obtained with the diaphragm 32 of the present embodiment.

  FIG. 8 shows the shape of the stop 42 in the illumination optical system of Example 4 of the present invention. The diaphragm 42 of the present embodiment has a shape in which the diaphragm opening end on the first region A side in the diaphragm 32 of the third embodiment is closed.

In this example,
a> b
Have the relationship. Further, in the x direction, the area ratio of the light shielding portion to the aperture opening 42a increases as the distance from the central axis C increases. The diaphragm 42 of the present embodiment can obtain the same effect as that of the first embodiment.

  FIG. 9 shows a configuration around a stop in an illumination optical system that is Embodiment 5 of the present invention. In this embodiment, the diaphragm 12 (which may be the diaphragms 22, 32, and 41 of Embodiments 2 to 4) is provided integrally with the optical filter 15 and is disposed between the cylindrical lens arrays 6 and 7. Furthermore, in this embodiment, the optical filter 15 and the stop 12 can be moved in the x direction in and out of the optical path of the illumination light beam. This movement is performed using the driving force of an actuator that operates in response to a switch operation (not shown).

  The optical filter 15 reduces light in a predetermined wavelength region (for example, orange light of about 570 to 590 nm) out of the illumination light flux from the light source, and improves the color reproducibility of the projected image. It is often used for image projection in so-called cinema mode.

  By setting it as such a structure, the user can select arbitrarily the projection mode which uses the optical filter 15 and the aperture_diaphragm | restriction 12, and the projection mode which does not use these. Of course, the optical filter 15 and the diaphragm 12 may be provided as separate bodies, and each may be independently movable in and out of the optical path.

  As shown in FIG. 10, the diaphragm 12 'may be formed so as to be divided in the y direction, and both divided parts may move to both sides in the y direction. Thereby, when it is necessary to move the stop 12 'in the y direction to move in and out of the optical path of the illumination light beam, the driving amount can be reduced.

  In the above embodiments, the polarization separation surface that separates the light according to the polarization direction is described as an example of the light separation surface. However, the present invention is not limited to other light such as a dichroic surface (film) that separates the light according to the wavelength. The present invention can also be applied to an optical system that leads to a surface (film) having a separation function.

  Further, in each of the above embodiments, the illumination optical system for illuminating the reflective liquid crystal panel has been described. However, the present invention can also be applied to the case of illuminating other image forming elements such as a transmissive liquid crystal panel.

  Next, an overall configuration example of an image projection optical system and an image projection apparatus to which the illumination optical system described in Embodiments 1 to 5 is applied will be described with reference to FIG. In addition, the code | symbol shown with the parenthesis to the component demonstrated below is a code | symbol attached | subjected to the component demonstrated in Example 1. FIG. FIG. 12 shows an xz cross section in each of the above embodiments. For this reason, the optical elements that do not have an optical action in the xz section among the optical elements described in the first embodiment are not shown.

  The image projection apparatus of the present embodiment includes a light source unit 100, an illumination optical system α, a color separation / synthesis optical system β, reflective liquid crystal display elements (liquid crystal panel 11) 111r, 111g, and 111b as image forming elements, And a projection lens 113. The light source unit 100, the illumination optical system α, the color separation / synthesis optical system β, the reflective liquid crystal display elements 111r, 111g, 111b, and the projection lens 113 constitute an image projection system.

  101 is an arc tube (1) that emits white light in a continuous spectrum, and 102 is a reflector (2) that collects light from the arc tube 101 in a predetermined direction. A light source unit 100 is configured by the arc tube 101 and the reflector 102.

  AXL is the optical axis (that is, the central axis C) of the illumination optical system α, the color separation / synthesis optical system β, and the projection lens 150, and indicates the traveling direction of light from the light source unit 100.

  Reference numeral 103 denotes a first cylindrical lens array (3) configured by a plurality of cylindrical lenses having refractive power in a direction parallel to the paper surface of FIG. 1, and 104 corresponds to each lens of the first cylindrical lens array 103. This is a second cylindrical lens array (4) having a plurality of cylindrical lenses.

  Reference numeral 12 denotes the diaphragm described in the first embodiment, and the diaphragms 12, 12 'and 22 to 42 described in the second to fifth embodiments can also be used.

  Reference numeral 105 denotes a polarization conversion element (13) for aligning non-polarized light with predetermined polarized light, 115 is a mirror, and 116 is a condenser lens (8) (the cylindrical lens 9 is not shown).

  A dichroic mirror 106 reflects blue (B: 430 to 495 nm) and red (R: 590 to 650 nm) light, and reflects green (G: 505 to 580 nm) light. Reference numeral 107 denotes a color filter that partially cuts light in the intermediate wavelength region between G light and R light. Reference numerals 108a and 108b denote a first color selective phase difference plate and a second color selective phase difference plate that convert the polarization direction of the B light by 90 degrees and do not convert the polarization direction of the R light.

  109a and 109b are a first half-wave plate and a second half-wave plate. Reference numerals 110a, 110b, and 110c denote a first polarization beam splitter, a second polarization beam splitter, and a third polarization beam splitter (10) that transmit P-polarized light and reflect S-polarized light. Each polarization beam splitter has a polarization separation surface (14).

  Reference numerals 111r, 111g, and 111b denote a red reflective liquid crystal panel, a green reflective liquid crystal panel, and a blue reflective liquid crystal panel that form an original image, reflect incident light, and modulate the image. Here, a drive circuit 120 is connected to the liquid crystal panels 111r, 111g, and 111b, and an image from an image information supply device 130 such as a personal computer, a camera, a DVD player, a video deck, or a broadcast receiver is connected to the drive circuit 120. Information is supplied. The drive circuit 120 drives the liquid crystal panels 111r, 111g, and 111b based on the input image information, and forms an original image for each color corresponding to the image information.

  112r, 112g, and 112b are a quarter wavelength plate for red, a quarter wavelength plate for green, and a quarter wavelength plate for blue, respectively. The optical system constituting the optical path from the dichroic mirror 106 to the third polarizing beam splitter 110c is a color separation / synthesis optical system β that performs color separation and color synthesis of light. Reference numeral 113 denotes a projection lens.

  Next, the optical action will be described. Light emitted from the arc tube 101 is collected in a predetermined direction by the reflector 102. The reflector 102 has a paraboloid shape, and light from the focal position of the paraboloid becomes a light beam parallel to the symmetry axis of the paraboloid. This parallel light beam is divided into a plurality of light beams by the first cylindrical lens array 103 and condensed, and a plurality of light source images are formed in the vicinity of the second cylindrical lens array 104 to reach the polarization conversion element 105.

  A part of the light beam emitted from the first cylindrical lens array 103 is blocked by the diaphragm 12.

  The polarization conversion element 105 includes a polarization separation surface, a reflection surface, and a half-wave plate in order from the incident side. The condensed light flux of each column of the matrix that has entered the polarization conversion element 105 is incident on the polarization separation surface of the column corresponding to that column, and is divided into a P-polarized component that transmits this and a S-polarized component that reflects. The reflected S-polarized component is reflected by the reflecting surface and is emitted in the same direction as the P-polarized component. On the other hand, the transmitted P-polarized light component is converted to the same polarized light component as the S-polarized light component when passing through the half-wave plate, and is emitted as light having the same polarization direction (here, S-polarized light). The plurality of light beams that have undergone polarization conversion are condensed in the vicinity of the polarization conversion element, and then reach the condenser lens 116 via the mirror 115 as divergent light beams.

  Due to the condensing action of the condenser lens 116, the plurality of light beams overlap at positions where images corresponding to the shapes of the individual cylindrical lenses in the first and second cylindrical lens arrays 103 and 104 are formed, and a rectangular uniform illumination area. Form. The light beam emitted from the condenser lens 116 enters the dichroic mirror 106. The dichroic mirror 106 transmits B and R light and reflects G light.

  In FIG. 1, S-polarized light emitted from the polarization conversion element 104 is also S-polarized light with respect to the dichroic mirror 106.

  In the optical path of G light, the light reflected from the dichroic mirror 106 enters the color filter 107. The color filter 107 is a dichroic filter that reflects yellow light in an intermediate wavelength region between G and R, thereby removing yellow light. If there are many yellow components in green, it will become yellowish green, so it is desirable for color reproduction to remove the yellow components by the color filter 107. The color filter 107 may have a characteristic of absorbing yellow light.

  The G light whose color has been adjusted in this way enters the first polarization beam splitter 110a as S-polarized light, is reflected by the polarization separation surface, and reaches the G-use reflective liquid crystal panel 111g. In the G reflective liquid crystal panel 111g, the G light is image-modulated and reflected. Of the modulated and reflected G light, the S polarization component is reflected again by the polarization separation surface of the first polarization beam splitter 110a, returned to the light source side, and removed from the projection light.

  On the other hand, the P-polarized component of the modulated and reflected G light is transmitted through the polarization separation surface of the first polarization beam splitter 110a to become projection light. At this time, in a state where all the polarization components are converted to S-polarized light (in a state where black is displayed), the quarter-wave plate 112g provided between the first polarizing beam splitter 110a and the G-use reflective liquid crystal panel 111g A slow axis that is one of the birefringent main axes is adjusted in a predetermined direction. Thereby, the influence of the disturbance of the polarization state generated in the first polarizing beam splitter 110a and the G-use reflective liquid crystal panel 111g can be reduced.

  The G light as P-polarized light that has passed through the first polarizing beam splitter 110a is rotated by 90 degrees in the polarization direction by the first half-wave plate 109a and is incident on the third polarizing beam splitter 110c as S-polarized light. . Thus, the G light incident on the third polarization beam splitter 110 c is reflected by the polarization separation surface and reaches the projection lens 113.

  On the other hand, the R and B lights transmitted through the dichroic mirror 106 are incident on the first color-selective phase difference plate 108a. The first color-selective retardation plate 108a has an action of rotating the polarization direction by 90 degrees only for B light. Thus, the B light is incident on the second polarization beam splitter 110b as P-polarized light and the R light is incident on S-polarized light. Then, the B light passes through the polarization separation surface of the second polarization beam splitter 110b, and reaches the B reflection type liquid crystal panel 111b via the quarter wavelength plate 112b. The R light is reflected by the polarization splitting surface and reaches the R reflective liquid crystal panel 111r via the quarter-wave plate 112r.

  In the reflective liquid crystal panel 111b for B, the B light is image-modulated and reflected. Of the modulated B light, the P-polarized light component is again transmitted through the polarization separation surface, returned to the light source side, and removed from the projection light. Of the modulated B light, the S-polarized light component is reflected by the polarization separation surface and becomes projection light.

  Similarly, R light is image-modulated and reflected by the R reflective liquid crystal panel 111r. Of the modulated R light, the S polarization component is reflected again by the polarization separation surface, returned to the light source side, and removed from the projection light. In addition, the P-polarized component of the modulated R light is transmitted through the polarization separation surface and becomes projection light. Thereby, the projection light of B and R is combined into one light beam.

  The combined B and R projection light is incident on the second color selective phase difference plate 108b. The second color selective phase difference plate 108b is the same as the first color selective phase difference plate 108a and rotates only the polarization direction of the B light by 90 degrees. As a result, both the R light and the B light are incident on the third polarization beam splitter 110c as P-polarized light, pass through the polarization separation surface, and are combined with the G projection light to reach the projection lens 113. Then, the light is projected onto a projection surface such as a screen by the projection lens 113.

1 is a perspective view showing a schematic configuration of an illumination optical system that is Embodiment 1 of the present invention. FIG. FIG. 2 is a yz sectional view of the illumination optical system according to the first embodiment. FIG. 2 is an xz sectional view of the illumination optical system of Example 1. FIG. 3 is a front view of a diaphragm used in the illumination optical system of Example 1. FIG. 3 is a diagram illustrating a pupil of the illumination optical system according to the first embodiment. FIG. 3 is a diagram showing a first light source image formed by the illumination optical system of Example 1. FIG. 6 is a diagram illustrating a second light source image formed by the illumination optical system according to the first embodiment. FIG. 6 is a front view of a diaphragm used in an illumination optical system that is Embodiment 2 of the present invention. FIG. 6 is a front view of a diaphragm used in an illumination optical system that is Embodiment 3 of the present invention. FIG. 6 is a front view of a diaphragm used in an illumination optical system that is Embodiment 4 of the present invention. FIG. 10 is a front view of a diaphragm used in an illumination optical system that is Embodiment 5 of the present invention. FIG. 10 is a front view showing a modification of the diaphragm of the fifth embodiment. FIG. 3 is a perspective view showing a cylindrical lens array used in the illumination optical system of Example 1. FIG. 10 is a diagram illustrating a configuration of an image projection apparatus that is Embodiment 6 of the present invention.

Explanation of symbols

DESCRIPTION OF SYMBOLS 1 Light emission tube 2 Reflector 3,4,6,7 Cylindrical lens array 8 Condenser lens 9 Cylindrical lens 10 Polarizing beam splitter 11 Liquid crystal panel 12,12 ', 22,32,42 Diaphragm 14 Polarization separation surface AC Center of iris aperture C Illumination Central axis of optical system

Claims (10)

The light beam from the light source, an optical system for guiding the light separation surface inclined with respect to the center axis of the optical science system,
A light flux limiting member for limiting a part of the light flux from reaching the light separation surface;
The light beam limiting member includes said central axis, have a asymmetrical shape with respect to a second plane perpendicular to the first plane including the normal line of the light separation surface and the central axis,
When the first region is a region from the light flux limiting member to the light separation surface, and the region on the side where the central axis and the light separation surface with the central axis as a boundary forms an obtuse angle,
The center of the light passage opening formed in the light flux restricting member is shifted in the first region with respect to the central axis,
The optical system includes: a first lens array that divides a light beam from the light source into a plurality of light beams in a direction parallel to the first surface;
A second lens array having a plurality of lenses corresponding to the plurality of lenses constituting the first lens array;
An optical system characterized by satisfying the following conditions .
p / 30 ≦ t ≦ p / 5
Where t is the amount of deviation of the center of the light passage aperture with respect to the central axis, and p is the lens pitch of the second lens array. The optical system of claim 1, the ratio of the light shielding portion with respect to the light passage openings in the light beam limiting member, characterized in that it increases with increasing distance from said central axis. The light beam limiting member, the optical system according to claim 1 or 2, characterized in that it is movable in and out of the optical path of the light beam from the light source. The optical system has an optical filter,
The light beam limiting member, the optical system according to any one of claims 1 to 3, characterized in that is provided integrally with the optical filter. The optical system is
Forming a first light source image of the light beam, each of the first cross-section and is divided into a plurality of light beams in a first direction perpendicular to a direction parallel to said central axis, said plurality of split light beams from the light source A first optical system,
Forming a second light source image of the light beam, each of the first direction and divided into a plurality of light beams in a second direction perpendicular to a direction parallel to said central axis, said plurality of split light beams from the light source A second optical system,
A condensing optical system that condenses light beams from the plurality of second light source images,
According to the width of the first light source image in the first direction, that any one of claims 1 4, characterized in wider than the width of the second light source images in the second direction Optical system. The optical system according to claim 5 , wherein the light flux limiting member is disposed at a position closer to the second light source image than to the first light source image. The second optical system includes a first cylindrical lens array including a plurality of cylindrical lenses;
A second cylindrical lens array having a plurality of cylindrical lenses corresponding to the respective cylindrical lenses of the first cylindrical lens array;
Between the second cylindrical lens array from the light source, the compression optical system is disposed to compress the width of the light beam from the light source in the second direction to claim 5 or 6, wherein The optical system described. An optical system according to any one of claims 1 to 7 ,
An image forming device which is illuminated by the light beam from the optical system,
An image projection optical system comprising: an optical system that projects a light beam from the image forming element onto a projection surface. An image projection apparatus comprising the image projection optical system according to claim 8 . An image projection device according to claim 9 ,
The image display system characterized by having an image supply apparatus for supplying image information to the image projection apparatus.