Source: https://patents.google.com/patent/EP1901105B1/en
Timestamp: 2020-04-09 14:49:59
Document Index: 691072915

Matched Legal Cases: ['art 1209', 'art 1109', 'art 1108', 'art 1209', 'arts 1208', 'art 1209', 'art\n1206', 'application No. 2006', 'application No. 2007']

EP1901105B1 - Projection optical system and image projecting apparatus - Google Patents
Projection optical system and image projecting apparatus Download PDF
EP1901105B1
EP1901105B1 EP07253643A EP07253643A EP1901105B1 EP 1901105 B1 EP1901105 B1 EP 1901105B1 EP 07253643 A EP07253643 A EP 07253643A EP 07253643 A EP07253643 A EP 07253643A EP 1901105 B1 EP1901105 B1 EP 1901105B1
EP07253643A
EP1901105A1 (en
Abe Issei
2006-09-15 Priority to JP2006251907 priority Critical
2007-09-04 Priority to JP2007229441A priority patent/JP2008096983A/en
2007-09-13 Application filed by Ricoh Co Ltd filed Critical Ricoh Co Ltd
2008-03-19 Publication of EP1901105A1 publication Critical patent/EP1901105A1/en
2010-11-03 Publication of EP1901105B1 publication Critical patent/EP1901105B1/en
239000000562 conjugates Substances 0 claims description 43
In recent years, an enlarging projection system has attracted attention which uses a displaying device (referred to as a light valve, below) in which a transmission-type or reflection-type dot matrix liquid crystal and a DMD (Digital Micro-mirror-Device) is used and which enlarges and projects an image displayed on the light valve onto a screen so as to exhibit it as a large image.
Recently, various kinds of devices for reducing a projection distance with respect to a large screen have been developed increasingly. However, for example, a projection distance of at least about 1 m is required for a front-type one in order to obtain an image with a diagonal size of 50 - 60 inches in a conventional technique, and at such a distance, a problem often occurs such that the shadow of a presenter reflects on a screen.
A common problem to the conventional techniques described above is to use many aspheric surfaces including a free-form surface in order to maintain an imaging performance and realize a wide angle of view, and accordingly, it is necessary to keep a strict precision of the distance between respective surfaces as well as a precision of the surface shape. Particularly, since the influence of an error in regard to the precision of a mirror surface is large in a type including the reflection mirrors in Japanese Patent Application Publication No. 2002-040326 , there is a problem of setting of a comparatively narrower tolerance among these conventional projection-optical systems.
Thus, in regard to the projection optical system, projection-type image displaying device and image displaying system disclosed in Japanese Patent Application Publication No. 2004-061959 , a lens system and plural reflective surfaces having a power are used in the projection optical system. Therefore, it is possible to compensate for a chromatic aberration caused by, for example, the color combining prism, by using the lens system. However, 3 - 5 aspheric mirrors are used in the practical examples and the cost is high. Also, it is necessary to set the surface precision and positional precision of the reflective surfaces to be extremely high similarly to the publicly known case described above, and there is a problem of a strict precision of assembly for the optical system. Furthermore, since light beams emitted from an image forming element is not telecentric, the brightness at an image plane may not be uniform or it may be necessary to make the effective angular range of a film of the color combining prism be wider than the divergence angle of light emitted from the light valve, whereby the separation characteristic may be degraded.
Also, in regard to the projection optical system, enlarging projection optical system, enlarging projection apparatus and image projecting apparatus disclosed in Japanese Patent Application Publication No. 2004-258620 , a lens system and plural reflective surfaces having a power are used in the projection optical system. Since enlargement is attained by using one rotationally aspherical reflective surface, the cost is saved and the precision of assembly is totally lowered compared to the technique disclosed in Japanese Patent Application Publication No. 2004-061959 . However, since the lens system is parallel decentered and tilted with respect to the optical axis in practical examples 1 - 5, it is very difficult to conduct the centering thereof. Also, a lens system is used without decentering in practical example 6, but the diameter of a lens that is closest to a screen is large due to the lens configuration, and therefore, the cost is high. That is, since the lens configuration is positive, negative and negative, the diameter of the last lens is large, which is a factor of cost increase.
In such a situation, the inventor(s) considered to provide a more compact projection optical system.
Also, the inventor(s) considered to provide an image projecting apparatus which includes a more compact projection optical system.
WO 2006/043666 discloses a projection optical system including a first optical system for forming an intermediate image of the primary image surface and a second optical system having a concave reflection surface for forming the secondary image surface by the intermediate image. The second optical system may comprise a convex reflector toward the primary image.
US 2004/0156117 Al discloses a projection optical system including first and second optical systems arranged along an optical path. The first optical system includes at least one dioptric system and has positive power. The second optical system includes at least one reflecting surface having power and has positive power. An intermediate image formed in the optical path is magnified and projected.
According to the present invention, there is provided a projection optical system as specified in claim 1.
According to an aspect of the present invention, there is provided an image projecting apparatus wherein the claimed projection optical system is installed.
The present invention will now be further described by way of example only, with reference to the accompanying drawings, in which:
Fig. 4 is a top view of the system of Fig. 1.
Fig. 5 is a diagram showing the distortion condition of an enlarged image on the last conjugate plane B.
Fig. 6 is a diagram showing the resolution performance with respect to an enlarged image on the last conjugate plane B.
Fig. 7 is a diagram showing practical example 2.
Fig. 8 is an enlarged view of the first optical system of practical example 2.
Fig. 9 is a diagram showing the distortion condition of an enlarged image on the last conjugate plane B.
Fig. 10 is a diagram showing the resolution performance with respect to an enlarged image on the last conjugate plane B.
Fig. 13 is a diagram showing practical example 3.
Fig. 14 is an enlarged view of the first optical system of practical example 3.
Fig. 15 is a diagram showing the distortion condition of an enlarged image on the last conjugate plane B.
Fig. 16 is a diagram showing the resolution performance with respect to an enlarged image on the last conjugate plane B.
The first embodiment of the present invention is a projection optical system in which plural light beams emitted from an image forming element displaying image information on a conjugate plane A are allowed to be obliquely incident on a conjugate plane B so as to form an enlarged image of an image formed by the image forming element on the conjugate plane B, wherein the projection optical system comprises, at least, a first optical system, a second optical system, an intermediate image of the image forming element between the first optical system and the second optical system on which the plural light beams are generally converged, an optical system having a refractive power in the first optical system being composed of only a lens system transmitting the light beams, the intermediate image being formed by only a refractive power of the first optical system, the second optical system being a reflective optical system comprising a reflection mirror having a positive refractive power which reflects the light beams and is directly behind the intermediate image, and the first optical system being composed of lens groups having positive, positive, and negative refractive powers in sequence from the side of conjugate plane A.
According to the first embodiment of the present invention, since the lens groups of the first optical system are positive, positive and negative in sequence from the side of image forming element, the lens diameter of the third group, particularly, the size or diameter of the last lens, may be reduced. Accordingly, a production error may be small and/or a resolution performance may be improved, which may lead to cost reduction.
The second embodiment of the present invention is a projection optical system in which plural light beams emitted from an image forming element displaying image information on a conjugate plane A are allowed to be obliquely incident on a conjugate plane B so as to form an enlarged image of an image formed by the image forming element on the conjugate plane B, wherein the projection optical system comprises, at least, a first optical system, a second optical system, an intermediate image of the image forming element between the first optical system and the second optical system on which the plural light beams are generally converged, an optical system having a refractive power in the first optical system being composed of a lens system transmitting the light beams and a reflection mirror being rotationally symmetric with respect to an optical axis of the first optical system and having a negative refractive power, the intermediate image being formed by only a refractive power of the first optical system, the second optical system being a reflective optical system comprising a reflection mirror having a positive refractive power which reflects the light beams and is directly behind the intermediate image, and the lens system transmitting the light beams in the first optical system being composed of lens groups having positive, positive, and negative refractive powers in sequence from the side of conjugate plane A.
According to the second embodiment of the present invention, since the lens groups of the first optical system are positive, positive and negative in sequence from the side of image forming element, the lens diameter of the third group, particularly, the size or diameter of the last lens, may be reduced. Accordingly, a production error may be small and/or a resolution performance may be improved, which may lead to cost reduction.
According to the third embodiment of the present invention, a distortion aberration of an enlarged image on a screen may be corrected. Accordingly, a resolution performance may be improved.
The fourth embodiment of the present invention is the projection optical system according to the first, second, or third embodiment of the present invention, wherein the mirror having a positive refractive power in the second optical system has an anamorphic and polynomial free-form surface having different powers between a minor axis direction and major axis direction of the image forming element.
The fifth embodiment of the present invention is the projection optical system according to the first, second, or third embodiment of the present invention, wherein the mirror having a positive refractive power in the second optical system has a surface with a rotationally symmetric and aspherical shape.
The sixth embodiment of the present invention is the projection optical system according to the first, second, third, fourth or fifth embodiment of the present invention, wherein a lens of the first optical system has at least one surface with an aspherical shape.
The seventh embodiment of the present invention is the projection optical system according to the sixth embodiment of the present invention, wherein the aspherical surface in the first optical system is positioned in a third group.
According to the eighth embodiment of the present invention, since the lens having a positive power in the third group is also a lens at which the angles of view of the light beams are most separated in the third group, the light beams at respective angles of view may be corrected independently. Accordingly, a resolution performance with respect to an enlarged image may be further improved.
The ninth embodiment of the present invention is the projection optical system according to the first, second, third, fourth, fifth, sixth, seventh, or eighth embodiment of the present invention, wherein the intermediate image is curved and tilted with respect to a surface perpendicular to an optical axis of the first optical system.
According to the ninth embodiment of the present invention, a field curvature at the conjugate plane B may be corrected which may be caused by reducing the curvature of the mirror having a positive power in the second optical system from the optical axis to the perimeter in the third embodiment of the present invention.
The tenth embodiment of the present invention is the projection optical system according to the first, second, third, fourth, fifth, sixth, seventh, eighth, or ninth embodiment of the present invention, wherein the projection optical system is generally telecentric from the image forming element to a first surface of the transmittable refractive optical system.
According to the tenth embodiment of the present invention, since the light beams emitted from the image forming element are introduced into the first optical system at generally the same angle over the entire angle of view, the brightness of an enlarged image on the screen may be generally uniformized. Also, when a film having a certain incident angle characteristic is arranged between the image forming element and the first optical system, it is only necessary to take only the range of introduction angle into consideration. Therefore, the incident angle may be reduced, which may lead to cost reduction.
The eleventh embodiment of the present invention is the projection optical system according to the first, second, third, fourth, fifth, sixth, seventh, eighth, ninth, or tenth embodiment of the present invention, wherein a reflection mirror is arranged between lenses of the first optical system.
According to the eleventh embodiment of the present invention, a folding mirror is arranged between lenses in the first optical system. Accordingly, an optical path from the image forming element to the folding mirror may be folded in empty space, whereby the spatial occupancy of the optical system may be reduced.
The twelfth embodiment of the present invention is an image projecting apparatus wherein the projection optical system according to any of the first to eleventh embodiments of the present invention is installed.
According to the twelfth embodiment of the present invention, a projection apparatus may be realized in which a projection optical system is used whose lens size is not so large even if the magnification thereof is high and the resolution performance is high. Therefore, a projection apparatus may be realized in which a desired magnification may be obtained, short distance projection may be possible, and the cost may be saved. Also, when the projection optical system according to any of the embodiments of the present invention is applied to rear-projection, an apparatus may be realized whose cost may be reduced compared to the conventional one and which may be possible to be thinned.
The thirteenth embodiment of the present invention is a projection optical system comprising a first optical system configured to form a second image conjugate to a first image and a second optical system configured to comprise a reflective optical element which reflects light from the second image and to project a third image conjugate to the second image onto a projection surface, wherein the first optical system comprises a stop and at least one optical element with a positive refractive power and at least one optical element with a negative refractive power which are provided between the stop and the second image, and an optical element with a strongest positive refractive power in the at least one optical element with a positive refractive power is provided between the stop and an optical element with a strongest negative refractive power in the at least one optical element with a negative refractive power.
According to the thirteenth embodiment of the present invention, a more compact projection optical system may be provided.
The fourteenth embodiment of the present invention is an image projecting apparatus wherein the projection optical system according to the thirteenth embodiment of the present invention is installed.
According to the fourteenth embodiment of the present invention, an image projecting apparatus may be provided which includes a more compact projection optical system.
A projection optical system is to project an image formed by an image forming element 011 on a conjugate plane A onto a screen 016 on a conjugate plane B, and is composed of a first optical system 013 that is a coaxial system and includes at least one refractive optical system and a second optical system 015 that includes at least one reflective surface having a positive power, wherein the first optical system 013 and the second optical system 015 are arranged from the image forming element 011, and an intermediate image between the first optical system 013 and the second optical system 015 is once formed from the image formed from on the image forming element 011, while enlarging projection is made as a whole. Additionally, a folding mirror 014 is arranged between the first optical system 013 and the second optical system 015 so as to fold the optical path and to reduce the spatial occupancy in Fig. 1 but practical example 1 of the present invention can be implemented without arranging the folding mirror 014.
Fig. 4 is a top view of Fig. 1, that is, a cross-sectional view of the system in an XZ plane, in which the direction of folding of the optical path by a folding mirror 043 is changed and a folding mirror 045 parallel to a screen 046 is arranged in the second optical system 044, 045. In Fig. 1, the direction of folding of the optical path by the folding mirror 014 is such that the first optical system 013 and the lower part are folded to a Y-direction, but it is obvious that, for example, the first optical system 042 may be folded to an X-direction as shown in Fig. 4, so as to reduce the spatial occupancy of the optical system. Furthermore, in the second optical system 044, 045, a folding mirror 045 parallel to a screen 046 may be arranged behind a reflection mirror 044 having a positive power, and when the optical system is installed in one housing 047 as shown in Fig. 4, the depth of the housing 047 may be reduced.
Additionally, for simplicity, only one image forming element is shown in the figures, but it is obvious that a color image may be projected onto a screen 1211 by using plural elements such as red, green, and blue ones, color-combining light beams modulated by the respective elements using a color combining part 1209 such as a publicly known dichroic prism, and then, introducing them into the first optical system, as shown in Fig. 12.
Also, as shown in Fig. 11, when light beams are generally telecentric from an image forming element 1107 to the first surface of a first optical system (the tenth embodiment of the present invention), the brightness of an enlarged image of the image forming element on a screen 1110 may be uniformized and the angular characteristic of an dichroic film of a color combining part 1109 that may be used for a color image projection using plural elements as described above may be narrow so as to become easy to produce the film itself, since it is only necessary to take only the divergence angle of light emitted from the image forming element 1107 into consideration. Furthermore, in the case of an image forming apparatus using a polarized-light separating part 1108, the angular characteristic of a polarized-light separating film thereof may be preferably narrow. Of course, the embodiment(s) of the present invention is applicable to a non-telecentric optical system.
When the first optical system is divided into three lens groups 023, 024, 025 by a stop 022 and the space where the maximum lens distance is provided in the lens groups 024, 025 at the side of conjugate plane B from the stop 022, the three lens groups 023, 024, 025 has positive, positive and negative powers, respectively, in sequence from the side of conjugate plane A. Light beams emitted from the image forming element 021 are refracted by the first group 023 having a positive power and the maximum of the angles of view of the principal rays of light beams passing through the stop 022 behind the first optical system is determined by the positive power of the first group 023 and the quantity of parallel decentering of the image forming element 021 with respect to the optical axis of the first optical system. The greater the maximum angle of view is, the heights of the rays of the light beam with respect to the optical axis are greater, and therefore, the diameters of the following lenses tend to be greater. However, since the second group 024 arranged behind the stop 022 has a positive power so as to suppress increase of the angle of view, the lens diameter of the third group 025 is prevented from increasing. Particularly, since the third group 025 has a negative power which may increase the angle of view, the lens diameter of the last lens may be prevented from increasing (the first embodiment of the present invention).
Also, as shown in Fig. 2, the freedom of design may be increased by using an aspherical lens for the first optical system, and therefore, the performance of imaging on the screen may be improved (the sixth embodiment of the present invention). Furthermore, since the third group 025 is a group in which the light beams with respective angles of view are most separated, aberration correction may be independently applied with respect to the angles of view by using an aspherical surface in the group (the seventh embodiment of the present invention). In particular, the light beams with the respective angles of view are most separated at a positive lens behind a negative lens as shown in Fig. 2, the capability of the aspherical surface in regard to aberration correction is most effective (the eighth embodiment of the present invention).
The light beams emitted from a first optical system 033, whose optical paths are folded by an folding mirror 034, are incident on a second optical system 035 and are enlarged and projected by a reflection mirror having a positive power in a third optical system. An intermediate image 036 of an image forming element 031, on which image the light beams are generally converged, is formed between the first optical system 033 and the second optical system 035.
The distortion aberration of an image of the image forming element 031 which image is enlarged and projected onto the conjugate plane B by the positive power of the second optical system 035 are generally proportional to the cube of an incident angle of view. That is, when the light rays emitted from object points that are arrayed at equal spaces on the image forming element 031 form into images on the conjugate plane B by the projection optical system, the formed images are not equally spaced and the degree of deviation increases with increasing the distance of the image point from the optical axis.
In the subject optical system, when a curved surface in the third optical system is a spherical surface, the space between the image points on the projected image increases with increasing the angle of view of the light beam, that is, increasing the distance thereof from the optical axis, and the image curves to the side of object points. In order to correct the distortion aberration in an enlarging projection system as described above, the reflection mirror having a positive power in the second optical system 035 has a curved surface having a shape such that the positive power further decreases with increasing the distance from the optical axis 037 (the third embodiment of the present invention). Also, when the reflection mirror having a positive power in the second optical system 035 has a shape of anamorphic and polynomial free-form surface, the freedom of design may increase and the capability of correcting an aberration, including the above distortion aberration, may be improved (the fourth embodiment of the present invention). Additionally, although a concave reflective surface is used in the descriptions, it is not limited to the surface and may be a Fresnel reflection mirror or a hologram reflection mirror as long as it is a reflective optical element having a light-condensing power.
Additionally, "anamorphic and polynomial free-form surface" in the above descriptions is a shape represented by Z = X ⁢ 2 ⋅ x 2 + Y ⁢ 2 ⋅ y 2 + X ⁢ 2 ⁢ Y ⋅ x 2 ⁢ y + Y ⁢ 3 ⋅ y 3 + X ⁢ 4 ⋅ x 4 + X ⁢ 2 ⁢ Y ⁢ 2 ⋅ x 2 ⁢ y 2 + Y ⁢ 4 ⋅ y 4 + X ⁢ 4 ⁢ Y ⋅ x 4 ⁢ y + X ⁢ 2 ⁢ Y ⁢ 3 ⋅ x 2 ⁢ y 3 + Y ⁢ 5 ⋅ y 5 + X ⁢ 6 ⋅ x ⁢ 6 + X ⁢ 4 ⁢ Y ⁢ 2 ⋅ x 4 ⁢ y 2 + X ⁢ 2 ⁢ Y ⁢ 4 ⋅ x 2 ⁢ y 2 + Y ⁢ 6 ⋅ y 6 + .....
wherein the up-and-down directions and left-and-right directions on the projected image as a reference are Y-directions and X-directions, respectively, the depth of the curved surface is Z-directions, and "X2, Y2, X2Y, Y3, X2Y2, etc." are coefficients.
Furthermore, the positive power decreasing with increasing the distance from the optical axis means that the focal length increases with increasing the distance from the optical axis. Then, the intermediate image conjugate to an enlarged image formed by the reflection mirror having a positive power in the second optical system is tilted and curved such that the optical path length to the reflection mirror having a positive power in the second optical system increases with increasing the distance of the light ray from the optical axis, since the focal length increases with increasing the distance from the optical axis (the ninth embodiment of the present invention).
Although 7, 1, and 4 lenses, (totally 12 lenses,) are used for the first group 023, the second group 024, and the third group 025, respectively, in the first optical system in practical example 1 as shown in Fig. 2, the embodiments of the present invention are not limited to the above-mentioned number of lenses. Also, although only the lenses are used for the first optical system, it is obvious that the spatial occupancy of the optical system may be reduced by arranging a reflection mirror between lenses so as to fold the optical path (the eleventh embodiment of the present invention).
In Table 1, "SHIFT" is the quantity of shift-decentering and "TILT" is the quantity of tilt-decentering. The units of the RADIUS OF CURVATURE, the SURFACE DISTANCE, and the quantity of shift-decentering are "mm" and the unit of the quantity of tilt-decentering is "degree(s)". Also, in regard to the signs of the SHIFT and TILT, shifting to the positive direction of the Y-axis directions has a "+" sign and tilting to the direction of the counterclockwise rotation around the X-axis has a "+" sign. These similarly apply to each of the following practical examples. Table 1 SURFACE NUMBER RADIUS OF CURVATURE SURFACE DISTANCE REFRACTIVE INDEX DISPERSION SHIFT TILT SURFACE SHAPE 0 ∞ 0 1 ∞ 43.6 1.517 64.2 2 ∞ 40 3 41 10.35 1.497 81.6 6.087 SPHERICAL SURFACE 4 -450.5 2.50 SPHERICAL SURFACE 5 114.5 1.00 1.786 44.2 SPHERICAL SURFACE 6 36.8 8.34 1.497 81.6 SPHERICAL SURFACE 7 1504.6 1.00 SPHERICAL SURFACE 8 98.0 8.26 1.497 81.6 SPHERICAL SURFACE 9 -48.2 1.00 1.834 37.1 SPHERICAL SURFACE 10 73.7 1.00 SPHERICAL SURFACE 11 48.6 10.28 1.620 36.3 SPHERICAL SURFACE 12 -47.4 1.00 SPHERICAL SURFACE 13 -42.7 10.00 1.492 57.8 SPHERICAL SURFACE 14 -142.7 22.70 ASPHERICAL SURFACE 15 STOP ∞ 117.63 0.652 16 65.6 5.12 1.773 49.6 -0.652 SPHERICAL SURFACE 17 115.0 35.93 SPHERICAL SURFACE 18 -2652.3 10.00 1.497 81.6 SPHERICAL SURFACE 19 123.9 6.15 SPHERICAL SURFACE 20 -201.0 1.00 1.667 48.2 SPHERICAL SURFACE 21 82.8 14.75 SPHERICAL SURFACE 22 -82.4 5.00 1.492 57.8 ASPHERICAL SURFACE 23 -57.9 12.52 ASPHERICAL SURFACE 24 -44.3 5.00 1.717 29.5 SPHERICAL SURFACE 25 -45.4 100.00 SPHERICAL SURFACE 26 ∞ -200.00 REFLECTION -45 SPHERICAL SURFACE 27 ∞ 530.00 REFLECTION -94.593 34 POLYNOMIAL FREE-FORM SURFACE 28 ∞ 0.00
As known well, a rotationally symmetric aspherical surface is represented by a formula of aspherical surface: Z = c ⋅ r 2 / 1 + √ 1 - 1 + k ⁢ c 2 ⁢ r 2 + Ar 4 + Br 6 + Cr 8 ..... ,
wherein Z, c, r, and k are a depth in the directions of the optical axis, a paraxial radius of curvature, a distance from the optical axis in the direction orthogonal to the optical axis, and a conical coefficient, respectively, and A, B, C, ..., etc., are higher-order coefficients of the aspherical surface. Herein, its shape is determined by providing the values of k, A, B, C, ... etc. These similarly apply to other practical examples described below.
The coefficients of the aspherical surfaces in practical example 1 are provided in Table 2. Table 2 COEFFICIENT 14TH SURFACE 22TH SURFACE 23TH SURFACE CONICAL COEFFICIENT: k 0 0 0 4TH ORDER COEFFICIENT:A 4.12088E-06 -3.40765E-07 -7.30853E-08 6TH ORDER COEFFICIENT: B 2.01448E-09 -3.20990E-09 -2.68979E-09 8TH ORDER COEFFICIENT: C 1.44924E-12 1.06467E-12 4.63464E-13
The coefficients of the polynomial free-form surface in practical example 1 are provided in Table 3. The coefficients of the polynomial free-form surface correspond to those of formula (1) described above. Table 3 COEFFICIENT COEFFICIENT VALUE X2 2.97156.E-03 Y2 1.75306.E-03 X2Y 1.03771.E-05 Y3 4.56218.E-06 X4 2.79059.E-09 X2Y2 5.87011.E-08 Y4 2.87829.E-08 X4Y -1.84772.E-11 X2Y3 2.39223.E-10 Y5 1.67000.E-10 X6 1.48824.E-13 X4Y2 -1.57412.E-13 X2Y4 7.39255.E-13 Y6 5.38089.E-13
Fig. 5 shows the distortion condition of an enlarged image on the last conjugate plane B and Fig. 6 shows the resolution performance with respect to the image.
Both of them are the results where a panel with a diagonal size of 0.7 inches and a vertical to horizontal ratio of 3:4 is assumed as an image forming element. The enlargement ratio is approximately 85.7. It can be seen that grid images are formed in generally equal spaces as shown in Fig. 5 and the distortion is corrected well. Also, it can be seen that the MTF value at an evaluation frequency of 0.5 c/mm is 79 % or greater as shown in Fig. 6 and the resolution performance is very high. Additionally, the F number of light emitted from the image forming element is F 2.8 and the thickness in the directions of the depth is 600 mm. Also, the lens having the largest diameter in the first optical system is a lens closest to the screen and the diameter is 80 mm.
Next, practical example 2, which is an unclaimed example, is described below.
Fig. 7 shows practical example 2 and Fig. 8 shows an enlarged view of a first optical system in practical example 2.
The specific data of practical example 2 are shown in Table 4. Table 4 SURFACE NUMBER RADIUS OF CURVATURE SURFACE DISTANCE REFRACTIVE INDEX DISPERSION SHIFT TILT SURFACE SHAPE 0 ∞ 0.00 1 ∞ 43.60 1.517 64.2 2 ∞ 40.00 3 120.4 7.84 1.497 81.6 6.047 SPHERICAL SURFACE 4 -103.1 5.73 SPHERICAL SURFACE 5 146 11.70 1.786 44.2 SPHERICAL SURFACE 6 41.6 9.85 1.497 81.6 SPHERICAL SURFACE 7 150.4 1.65 SPHERICAL SURFACE 8 281.6 6.48 1.497 81.6 SPHERICAL SURFACE 9 -59.9 13.00 1.834 37.1 SPHERICAL SURFACE 10 75.8 1.04 SPHERICAL SURFACE 11 70.9 13.00 1.620 36.3 SPHERICAL SURFACE 12 -65.9 32.83 SPHERICAL SURFACE 13 STOP ∞ 165.75 0.749 14 60.4 12.36 1.591 64.1 -0.749 SPHERICAL SURFACE 15 232.6 39.20 SPHERICAL SURFACE 16 -117.8 12.85 1.748 46.5 SPHERICAL SURFACE 17 617.3 7.21 SPHERICAL SURFACE 18 -134.3 7.37 1.747 51.3 SPHERICAL SURFACE 19 81.2 5.48 SPHERICAL SURFACE 20 100.5 5.33 1.492 57.8 ASPHERICAL SURFACE 21 239.9 17.09 ASPHERICAL SURFACE 22 -66.1 5.00 1.791 26.2 SPHERICAL SURFACE 23 -60.0 190.00 SPHERICAL SURFACE 24 1000.0 -160.00 REFLECTION -45 SPHERICAL SURFACE 25 ∞ 240.00 REFLECTION -115.48 35.9 POLYNOMIAL FREE-FORM SURFACE 26 ∞ -290.00 REFLECTION 27 ∞ 0.00
The coefficients of the aspherical surfaces in practical example 2 are provided in Table 5. Table 5 COEFFICIENT 20TH SURFACE 21TH SURFACE CONICAL COEFFICIENT: k 0 0 4TH ORDER COEFFICIENT:A -3.60680E-06 -2.76455E-06 6TH ORDER COEFFICIENT: B -7.27350E-10 -1.02629E-09 8TH ORDER COEFFICIENT:C 1.00351 E-1 2 9.17691 E-1 3
The coefficients of the polynomial free-form surface in practical example 2 are provided in Table 6. The coefficients of the polynomial free-form surface correspond to those of formula (1) described above. Table 6 COEFFICIENT COEFFICIENT VALUE X2 2.54164.E-03 Y2 1.47203.E-03 X2Y 7.24107.E-06 Y3 2.89309.E-06 X4 2.96578.E-09 X2Y2 3.76036.E-08 Y4 1.43611.E-08 X4Y 9.34107.E-12 X2Y3 1.67235.E-10 Y5 9.46304.E-11 X6 8.80991.E-14 X4Y2 -1.71084.E-14 X2Y4 5.48160.E-13 Y6 3.84113.E-13
Fig. 9 shows the distortion condition of an enlarged image on the last conjugate plane B and Fig. 10 shows the resolution performance with respect to the image.
Both of them are the results where a panel with a diagonal size of 0.7 inches and a vertical to horizontal ratio of 3:4 is assumed as an image forming element. The enlargement ratio is approximately 85.7. It can be seen that grid images are formed in generally equal spaces as shown in Fig. 8 and the distortion is corrected well. Also, it can be seen that the MTF value at an evaluation frequency of 0.5 c/mm is 75 % or greater as shown in Fig. 9 and the resolution performance is good but is lower than that of practical example 1. It is considered that this is because the configuration of practical example 2 is such that one lens (aspherical lens) is removed from practical example 1, as described above, and therefore, the freedom of design is lowered. Additionally, the F number of light emitted from the image forming element is F 2.8 and the thickness in the directions of the depth is 300 mm. Also, the lens having the largest diameter in the first optical system is a lens closest to the screen and the diameter is 80 mm.
[Practical example 3]
Next, practical example 3 for the fifth embodiment of the present invention is described below.
Fig. 13 shows practical example 3 and Fig. 14 shows an enlarged view of a first optical system in practical example 3.
Similarly to practical example 1 of the present invention, a projection optical system is to project an image formed by an image forming element 131 on a conjugate plane A onto a screen 136 on a conjugate plane B, and is composed of a first optical system 133 that is a coaxial system and includes at least one refractive optical system and a second optical system 135 that includes at least one reflective surface having a positive power, wherein the first optical system 133 and the second optical system 135 are arranged from the image forming element 131, and an intermediate image between the first optical system 133 and the second optical system 135 is once formed from the image formed from on the image forming element 131. It is an optical system for enlarging projection as a whole. Herein, the reflective surface having a positive power in the second optical system 135 has a shape of rotationally symmetric aspherical surface.
Also, the optical path is folded by a folding mirror 134, and in regard to the folding direction, the first optical system 133 is folded to the direction of the height of the conjugate plane B, that is, the Y-direction, in Fig. 13 but it is obvious that the first optical system 133 may be folded to, for example, the direction of the depth in the figure, that is, the X-direction, so as to further reduce the spatial occupancy of the optical system.
The specific data of practical example 3 are shown in Table 7. Table 7 SURFACE NUMBER RADIUS OF CURVATURE SURFACE DISTANCE REFRACTIVE INDEX DISPERSION SHIFT TILT SURFACE SHAPE 0 ∞ 1.80 1.519 64.2 1 ∞ 2.00 2 ∞ 0.40 1.549 92.0 3 ∞ 2.00 4 ∞ 16.00 1.591 61.3 5 ∞ 3.25 1.591 61.3 6 ∞ 25.00 1.519 64.2 7 ∞ 0.00 8 ∞ 6.45 9 306.6 6.60 1.489 70.4 0.606 SPHERICAL SURFACE 10 -42.2 6.00 SPHERICAL SURFACE 11 22.5 2.83 1.489 70.4 SPHERICAL SURFACE 12 1951.0 7.00 SPHERICAL SURFACE 13 136.1 0.30 1.794 33.1 SPHERICAL SURFACE 14 16.6 1.80 1.489 70.4 SPHERICAL SURFACE 15 -34.7 10.00 SPHERICAL SURFACE 16 -26.0 1.50 1.825 36.1 SPHERICAL SURFACE 17 37.7 1.80 1.498 81.6 SPHERICAL SURFACE 18 -19.7 8.00 SPHERICAL SURFACE 19 -20.2 0.30 1.742 45.6 SPHERICAL SURFACE 20 43.8 1.70 1.791 25.7 SPHERICAL SURFACE 21 -29.7 7.00 SPHERICAL SURFACE 22 ∞ 86.77 23 46.5 12.78 1.501 80.9 SPHERICAL SURFACE 24 211.3 25.56 SPHERICAL SURFACE 25 109.8 6.06 1.839 43.0 ASPHERICAL SURFACE 26 50.4 13.75 ASPHERICAL SURFACE 27 37.0 12.83 1.532 68.0 SPHERICAL SURFACE 28 -1021.9 12.32 SPHERICAL SURFACE 29 -69.6 10.00 1.839 43.0 SPHERICAL SURFACE 30 42.4 18.06 SPHERICAL SURFACE 31 -14964.0 6.59 1.523 63.9 ASPHERICAL SURFACE 32 -93.7 100.00 ASPHERICAL SURFACE 33 ∞ -123.94 REFLECTION -45 34 82.5 540.00 REFLECTION -0.065 0.072 ASPHERICAL SURFACE 35
The coefficients of the aspherical surfaces in practical example 3 are provided in Table 8. Table 8 SURFACE NUMBER 25 26 31 32 34 CONICAL COEFFICIENT : k 0.00000E+00 -7.02000E+00 0.00000E+00 0.00000E+00 2.24406E+00 4TH ORDER COEFFICIENT : A -1.41265E-05 -9.47818E-06 -3.06324E-06 -2.18744E-06 8.06745E-08 6TH ORDER COEFFICIENT: B 1.40628E-08 1.53629E-08 7.98633E-09 4.59424E-09 1.11257E-13 8TH ORDER COEFFICIENT: C -1.04074E-11 -1.88643E-11 -1.51318E-12 3.04683E-12 -5.92556E-17 10TH ORDER COEFFICIENT: D 1.91167E-14 3.53510E-14 4.27712E-17 -2.09239E-15 -1.78199E-20 12TH ORDER COEFFICIENT: E -3.61156E-17 -5.29456E-17 0.00000E+00 1.92505E-18 2.14275E-24 14TH ORDER COEFFICIENT: F 2.08514E-20 2.77262E-20 0.00000E+00 -1.04171 E-21 -6.49568E-29
Herein, the first group 143 is composed of 8 lenses denoted by surface numbers 9 - 24, wherein the focal length of the lens system of the first group 143 is approximately + 55.3 mm and the lens system of the first group 143 has a positive power of approximately + 0.0181 mm-1. Also, the second group 144 is composed of one lens denoted by surface numbers 25 and 26, wherein the focal length of the lens system of the second group 144 is approximately + 116 mm and the lens system of the second group 144 has a positive power of approximately + 0.00865 mm-1. Similarly, the third group 145 is composed of four lenses denoted by surface numbers 27 - 34, wherein the focal length of the lens system of the third group 145 is approximately - 77.1 mm and the lens system of the third group 145 has a negative power of approximately - 0.0130 mm-1.
Fig. 15 shows the distortion condition of an enlarged image on the last conjugate plane B and Fig. 16 shows the resolution performance with respect to the image.
Both of them are the results where a panel with a diagonal size of 0.6 inches and a vertical to horizontal ratio of 9:16 is assumed as an image forming element. The enlargement ratio is approximately 100 (that is, an image plane with a diagonal size of 60 inches and a vertical to horizontal ratio of 9:16 is obtained). It can be seen that grid images are formed in generally equal spaces as shown in Fig. 15 and the distortion is corrected well (Additionally, a so-called TV-distortion is approximately 0.5 %). Also, it can be seen that the MTF value at an evaluation frequency of 0.72 c/mm is 75 % or greater as shown in Fig. 16 and the resolution performance is good. The F number of light emitted from the image forming element is F 2.45 and the thickness in the directions of the depth is 540 mm.
An image projecting apparatus may be provided by applying the projection optical system according to the embodiment(s) of the present invention to a projection apparatus (the twelfth embodiment of the present invention).
Additionally, as described above, it is obvious that a color image may be projected onto a screen 1211 by using plural image forming elements 1207 such as ones for red, green and blue, applying illumination light transmitting through the respective color filters, and introducing light combined by a color combining part 1209 into the projection optical system 1210.
Then, as shown in Fig. 12, the distance from an image forming element 1207 to the first surface of a first optical system of the projection optical system 1210 has to be a long distance due to the presence of a polarized-light separation parts 1208 on an illumination optical path and a projection optical path and a color combining part 1209 for coloring. In practical examples 1 and 2, a color image may be projected using the above-mentioned coloring part since the air-equivalent length thereof is 68.7 mm.
Thus, according to at least one of the practical examples as described above, a more compact projection optical system may be provided.
Also, according to at least one of the practical examples as described above, an image projecting apparatus which includes a more compact projection optical system may be provided.
011, 021, 031, 041, 071, 081, 131, 141, 1107, 1207: Image Forming Element
012, 022, 032, 082, 132, 142: Stop
013, 033, 042, 072, 133: First Optical
014, 034, 043, 134: Folding Mirror
015, 035, 135: Second Optical System
016, 046, 076, 136, 1110, 1211: Screen
023, 083, 143: First Group
024, 084, 144: Second Group
025, 085, 145: Third Group
044, 074: Second Optical System - 1
045, 075: Second Optical System - 2 (Folding
073: Rotationally Symmetric Reflection
1104, 1204: Polarized-Light Converting
1105, 1205: Illumination Unoformizing Part
1206: Color Separation Part
Typical embodiments (1) to (13) of the present invention are described below.
Embodiment (1) is a projection optical system comprising a first optical system configured to form a second image conjugate to a first image and a second optical system configured to comprise a reflective optical element which reflects light from the second image and to project a third image conjugate to the second image onto a projection surface, characterized in that the first optical system comprises a stop and at least one optical element with a positive refractive power and at least one optical element with a negative refractive power which are provided between the stop and the second image, and an optical element with a strongest positive refractive power in the at least one optical element with a positive refractive power is provided between the stop and an optical element with a strongest negative refractive power in the at least one optical element with a negative refractive power.
Additionally, "an optical element with a strongest positive refractive power in the at least one optical element with a positive refractive power being provided between the stop and an optical element with a strongest negative refractive power in the at least one optical element with a negative refractive power" includes, for example, "the first optical system being composed of lens groups having positive, positive, and negative refractive powers in sequence from the side of conjugate plane A" in the first embodiment of the present invention and "the lens system transmitting the light beams in the first optical system being composed of lens groups having positive, positive, and negative refractive powers in sequence from the side of conjugate plane A" in the second embodiment of the present invention.
Embodiment (3) is the projection optical system as described in embodiment (2) above, characterized in that the at least one optical element with a positive refractive power and the at least one optical element with a negative refractive power are composed of lenses only.
Embodiment (4) is the projection optical system as described in embodiment (2) above, characterized in that the at least one optical element with a negative refractive power comprises a mirror that is rotationally symmetric around the optical axis.
Embodiment (9) is the projection optical system as described in embodiment (8) above, characterized in that the optical element having an aspherical surface is provided between the optical element with a strongest positive refractive power in the at least one optical element with a positive refractive power and the second image.
Embodiment (11) is the projection optical system as described in any of embodiments (2) to (10) above, characterized in that the second image is an image which is tilted with respect to the optical axis and is curved.
Embodiment (12) is the projection optical system as described in any of embodiments (1) to (11) above, characterized in that the first optical system is a generally telecentric optical system with respect to the first image.
Embodiment (13) is the projection optical system as described in any of embodiments (1) to (12) above, characterized in that the first optical system comprises a first lens and a second lens and a mirror provided between the first lens and the second lens.
Embodiment (14) is an image projecting apparatus configured to project an image onto a projection surface, characterized by comprising the projection optical system as described in any of embodiments (1) to (13) above.
Although the embodiment(s) and specific example(s) of the present invention have been described above specifically, the present invention is not limited to the embodiment(s) or specific example(s), and the embodiment(s) and specific example(s) of the present invention can be altered or modified without departing from the scope of the present invention defined by the claims only.
The present application is based on Japanese priority application No. 2006-251907 filed on September 15, 2006 and Japanese priority application No. 2007-229441 filed on September 04, 2007.
A projection optical system in which plural light beams emitted from an image forming element (021, 031) displaying image information on a conjugate plane A are allowed to be obliquely incident on a conjugate plane B so as to form an enlarged image of an image formed by the image forming element (021, 031) on the conjugate plane B, wherein:
the projection optical system comprises, at least a first optical system (033) and a second optical system (035);
an intermediate image (036) of the image forming element (021, 031) is formed between the first optical system (033) and the second optical system (035) on which the plural light beams are generally converged;
the light beams are transmitted in the first optical system (033) by only a lens system;
the intermediate image (036) is formed by only a refractive power of the first optical system (033);
the second optical system (035) is a reflective optical system comprising a reflection mirror (035) having a positive refractive power which reflects the light beams and is directly behind the intermediate image (036); and
the first optical system (033) is divided into three lens groups (023, 024, 025) by a stop (022) and a space where the maximum distance between adjacent lens surfaces is provided in the lens groups (024, 025) at the side of conjugate plane B with respect to the stop (022), the three lens groups (023, 024, 025) having positive, positive, and negative refractive powers in sequence from the side of conjugate plane A;
characterized in that at least one surface with an aspherical shape is positioned on a lens having a positive refractive power in the lens group (025) having negative refractive power.
A projection optical system according to claim 1, wherein a curved surface of the mirror (035) having a positive refractive power in the second optical system (035) has a shape such that a curvature thereof becomes smaller from its intersection point with an optical axis of the first optical system to a perimeter thereof.
A projection optical system according to claim 1 or 2, wherein the mirror (035) having positive refractive power in the second optical system (035) has an anamorphic and polynominal free-form surface having different powers between a minor axis direction and major axis direction of the image forming element (021, 031).
A projection optical system according to claim 1 or 2, wherein the mirror (035) having a positive refractive power in the second optical system (035) has a surface conforming to part of a rotationally symmetric and aspherical shape.
A projection optical system according to any one of claims 1 to 4, wherein the intermediate image (036) is curved and tilted with respect to a surface perpendicular to an optical axis of the first optical system (033).
A projection optical system according to any one of claims 1 to 5, wherein the projection optical system is generally telecentric from the image forming element (021, 031) to a first surface of the transmitting lens system of the first optical system (033).
A projection optical system according to any one of claims 1 to 6, wherein a reflection mirror is arranged between lenses of the first optical system (033).
An image projecting apparatus comprising a projection optical system as claimed in any one of the preceding claims.
EP07253643A 2006-09-15 2007-09-13 Projection optical system and image projecting apparatus Active EP1901105B1 (en)
JP2006251907 2006-09-15
JP2007229441A JP2008096983A (en) 2006-09-15 2007-09-04 Projection optical system and image projection device
EP1901105A1 EP1901105A1 (en) 2008-03-19
EP1901105B1 true EP1901105B1 (en) 2010-11-03
ID=38753540
EP07253643A Active EP1901105B1 (en) 2006-09-15 2007-09-13 Projection optical system and image projecting apparatus
US (1) US8025415B2 (en)
EP (1) EP1901105B1 (en)
JP (1) JP2008096983A (en)
CN (1) CN101221282B (en)
DE (1) DE602007010217D1 (en)
JP2010197495A (en) * 2009-02-23 2010-09-09 Ricoh Co Ltd Projection optical system and image display
KR20180000345A (en) * 2010-07-06 2018-01-02 시리얼 테크놀로지즈 에스.에이. Beam divergence and various collimators for holographic or stereoscopic displays
JP5561087B2 (en) * 2010-10-14 2014-07-30 株式会社リコー Image projection device
EP2560393B1 (en) * 2011-08-16 2018-10-10 Ricoh Company Ltd. Image displaying apparatus
CN105759543A (en) * 2014-12-17 2016-07-13 深圳市亿思达科技集团有限公司 Projection optical system and projection device
CN105158884B (en) * 2015-10-10 2018-03-23 浙江大学 A kind of ultrashort out-of-focus projection's lens system
2007-09-04 JP JP2007229441A patent/JP2008096983A/en active Pending
2007-09-13 DE DE602007010217T patent/DE602007010217D1/en active Active
2007-09-13 US US11/854,920 patent/US8025415B2/en active Active
2007-09-13 EP EP07253643A patent/EP1901105B1/en active Active
2007-09-17 CN CN2007103077819A patent/CN101221282B/en active IP Right Grant
US20080068564A1 (en) 2008-03-20
EP1901105A1 (en) 2008-03-19
JP2008096983A (en) 2008-04-24
DE602007010217D1 (en) 2010-12-16
CN101221282A (en) 2008-07-16
CN101221282B (en) 2012-08-08
US8025415B2 (en) 2011-09-27
EP1512283B1 (en) 2008-05-21 Short throw image projection system and method
US7896504B2 (en) 2011-03-01 Projection module and projector incorporating same
US7885008B2 (en) 2011-02-08 Optical system for digital cinema projection
US7420177B2 (en) 2008-09-02 High-resolution-imaging system for scanned-column projectors
Ref document number: 602007010217