A projection lens

Abstract: An improved projection lens capable of substantially and advantageously implementing a distinct picture by compensating for a chromatic aberration and a residue aberration, which includes a first lens group (100), including a lens element convex to a screen and having a relatively weak optical power, for eliminating a spherical surface aberration; a second lens group (101) having positive optical power and cemented with a two side lens element having a positive optical element and a lens element having a negative optical element, which have a different dispersion from each other; a third lens group (102) having a positive optical power on an optical axis and a radius code of a curvature surface toward an upper surface of which has the same radius code as the radius curvature surface of a cathode ray tube; and a fourth lens group (103) having a high optical power toward an upper surface of the screen for compensating for a field dependent aberration.

Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a projection lens for use in combination with a cathode ray tube, and more particularly to an improved projection lens capable of substantially and advantageously implementing a distinct picture by compensating for a chromatic aberration and a residue aberration. 2. Description of the Conventional Art Conventionally, a preferred form of projection lenses for wide screen television is disclosed in U.S. Pat Nos. 4,300,817, 4, 348, 081, 4,526,442, and 4,770, 513. In these previous patents, the lens units have been referred to as groups which perform specified optical function. Here, the term "lens unit" refers to one or more lens elements or lens components which provide a defined optical function or functions in the design of the overall lens. It is well known that a specified or defined optical function(s) of a lens or group in an overall lens may be accomplished by using one element or component or more than one element or component dependent upon the correction or function desired. A decision as to whether one or more elements is used as a lens unit in an overall lens design may be based on various considerations, including but not limited to, ultimate performance of the lens, ultimate costs of the lens, acceptable size of the lens, etc. Accordingly, in the following specification and appended claims, the terms "lens unit" refers to one or more lens elements or lens components which provide a defined optical function or functions in the design of the overall lens. The lens disclosed in the aforementioned patents generally comprises three lens units: from the image end a first lens unit, having at least one aspheric surface, which serves as an aberration-corrector; a second lens unit including a biconvex element which supplies all or substantially all of the positive power of the lens; and a third lens unit having a concave surface towards the image end of the lens, serving as a field flattener, and essentially correcting for Petzval curvature of the lens. The lens, as disclosed, are designed for use with a surface of a cathode ray tube(CRT). The lenses of U.S. Pat. No. 4,300,817, utilizing a single biconvex element in the second lens unit, all have an equivalent focal length(EFL) of one hundred twenty-seven millimeters or greater, while the lens of U.S. Pat. No. 4,348,081, which utilize a two-element second lens unit, including the biconvex element, may have an EFL reduced to eighty-five millimeters as designed for direct projection for a five inch diagonal CRT. The lens described in U.S. Pat. No. 4,526,442 are designed to have a fold in the optical axis between the first and second lens units and have been designed so that the EFL is as low as one hundred twenty-six millimeters. These EFL's also for CRT screens having a viewing surface with an approximate five inch diagonal. Projection TV sets are rather bulky and have required high volume cabinet. One manner of reducing the cabinet size is to decrease the EFL of the projection lenses. This, of course, increases the field angle of the lens. The EFL of the lens is a function of the total conjugate distance between the CRT and the display screen. This is shown by the relationship OL = EFL(1+1/M)+EFL(1+M) where OL is the overall conjugate distance of the system from object to image, EFL(1+M) is the distance from the image to the first principal point of the lens, EFL(1+1/M) is the distance from the object to the second principal point of the lens and M is the magnification of the system expressed as the ratio of object height to image height. Therefore, in order to decrease the total distance between the CRT and the screen, it is necessary to reduce the EFL, or alternately stated, increase the field angle of the lens. An effect of increasing the angular coverage of the lens as a result of decreasing the EFL is that the aberrations become more difficult to correct. A further consideration is introduced wherein a spacing in provided between the phosphor screen of the CRT and the third lens unit of the projection lens. This spacing may be required for the inclusion of a liquid cooling and/or optical coupling material and a housing necessary to enclose the coolant against the face of the CRT. This additional spacing between the face of the CRT causes the third negative lens unit to contribute more negative power, which must be compensated by increased power in the positive second lens unit. In some cases, the phosphor surface of the CRT is curved convex to increase the convex brightness. This permits a power reduction in the third groupinasmuch as the power requirement for correction of field curvature is reduced. A single biconvex element second lens unit, as shown in the aforementioned patents, does not provide the lens designer adequate degrees of freedom to correct for the resulting astigmatism and distortion. By dividing the optical power of the second lens unit, as disclosed in U.S. Pat. No. 4,348,081, a better control of aberrations can be obtained for a shorter EFL. However, merely splitting the optical power of the second lens unit into two elements to obtain additional degrees of optical design freedom does not provide acceptable contrast and resolution where the angular coverage of the projection lenses is required to be in excess of twenty-seven degrees. Since the advent of lens, as shown in U.S. Pat. No. 4,300,817, which made large screen home projection television sets feasible, there has been continuing efforts to design projection lens with wider field angles which are more compact, and easier to manufacture at the greatest economy. This, of course, is an effort to reduce the cost of the lens and reduce the depth of the housing of the television system while maintaining or increasing the size of the viewing screen. Projection lens of the overall type described have been designed with decreased EFL's by designing a more complex second lens unit split into more than one lens element, as exemplified in the lenses disclosed in U.S. Pat. No. 4,697,892 These designs are currently used on many wide screen projection television sets and may have an equivalent focal length as low as eighty millimeters. It will be understood that the EFL will be greater if there is a fold in the optical axis between the first and second lens units. This approach works very well and leads to high quality optical performance of the lens. However, it requires large diameter positive elements in the second lens unit to accommodate the diverging bundle of light(as traced from the long conjugate). This construction also requires a lens of relatively long front vertex distance(FVD), largely due to a long space between the first negative element and the following power unit, which is necessary to use to achieve an appropriate correction of field curvature and astigmatism. The front vertex distance is the distance from the image side of the first lens unit to the face place of the CRT. The related co-pending application discloses a lens of the type described, which consists of a first lens unit which comprises a single element with two aspheric surface, and an overall positive meniscus shape preferably convex to the image end, a second positive element, and a third lens unit having a storingly negative surface concave to the image end. The first lens element is of positive optical power at the optical axis of the lens, but due to the aspheric power of the surfaces, the positive optical power decreases with distance from the optical axis and may become strongly negative at or closely adjacent the clear aperture of the first lens element, as hereinafter explained. The strong negative power of the third lens unit contributes to correction of the Petzval sum of other lens elements. The strongly concave surface may be made aspheric to also correct for residual astigmatism and field curvature of the lens. The second lens element provides the majority of the positive power of the lens and some correction for astigmatism. The first lens element must then correct the aperture dependent aberrations, particularly, spherical and coma. Lenses as described in the related application are very compact, having the first and second lens unit spaced more closely than heretofore. Lenses as described may have a field angle as great as 73° while comprising only three elements. In lenses of the type described in U.S. Pat. No. 4,300,817, all the elements are made out of acrylic because of simplicity of manufacturing aspherical surface on plastic. However, the refractive index of acrylic varies significantly with temperature. This leads to a change in focal lengths of the acrylic lens elements, which in turn, can lead to defocus or lack of sharp focus of the overall lens. One way of compensating for focus shift with temperature is to design a lens mount and lens barrel using a bi-metallic plate or other means that will shift the position of the lens relative to the CRT as a function of temperature in such a way that the focus of the lens will remain in a constant position. alternatively, the second or power lens unit may be formed of glass, as disclosed in U.S. Pat. No. 4,348,081, which does not exhibit nay substantial change in index of refraction with temperature. however, this restricts the lens designer in that it is very expensive to define an aspheric surface on glass. A further solution is to design a hybrid lens using a glass power unit with an additional acrylic corrector with one or more aspheric surfaces adjacent the power unit. However, this does not necessarily provide a lens with a wider field angle and decreased length. To reduce the cost of manufacturing projection lenses, it is desirable to decrease the size of the elements. In the present invention, a positive first lens unit is utilized to reduce the diameter of the other elements of the lens. This is achieved through the use of a positive first lens unit preferably in the overall form of a meniscus which converges the rays toward the strongly positive second lens unit(as traced from the long conjugate side). The spacing between the first lens unit and the second lens unit it thereby reduced, which results in a reduction in the front vertex distance of the lens. To resolve such problems, there is well disclosed in U.S. Pat. No. 4,776,681. Referring to Fig. 1, the invention of the conventional projection lens will now be explained. As shown therein, projection lens of the overall type described have been designed with a plastic non-aspheric lens and as shown in Fig. 2A to 2C the chromatic aberration is not compensated. The conventional projection lens can not perform optimum result because the lenses are designed in e-line(546.0nm) which is a central wave of a green CRT and then the same lenses are used in the red and blue CRT. A central wavelength of the blue CRT and a d-line(590.0mm) which is a central wavelength of the red CRT are deviated from the e-line(546.0nm) which is a central wavelength of a green CRT, in addition, as shown in Fig. 2B, it is difficult to compensate for a coma aberration and an upper surface concave aberration sue to a sagittal field curve and a tangential field curve from a center of an aberration distance. In addition, as shown in Fig. 2C, a distortion occurs therein. Figs. 3A to 3C show spectrum characteristics which are obtained from the green, blue, and red CRTs. Since all the CRTs have a part of different wavelength band width, respectively, chromatic aberration occurs too. The green lens assembly influences much for the display quality of television. However, the spectrum of the green CRT as shown in Fig. 3A contains the blue and red light besides the central wavelength, so that compensation for the chromatic aberration is adapted therein. Generally, the optical system in which the compensation of the chromatic aberration is not performed degrades the display quality and the contrast, so that compensation for the chromatic aberration is required in the high definition digital television and the high definition video projector. In the drawings, the lens unit are identified by the reference G followed by successive arabic numerals except that a corrector lens unit is designated by the reference CR; lens elements are identified by the reference L followed by successive arabic numerals from the image to the object end. Surfaces of the lens elements are identified by the reference S followed by successive arabic numerals from the image to the object end. The reference Si denotes the phosphor surface of a cathode ray tube. The first lens unit G1 comprises an element of positive power and an overall positive shaped meniscus, and has at least one aspheric surface defined by the equation X = C r 2 1+√1-(1+K)C r 2 +D y 4 +E y 6 +F y 8 +G y 10 +H y 12 +I y 14 where X is the surface sag at a semi-aperture distance y from the axis A of the lens C, is the curvature of a lens surface at the optical axis A equal to the reciprocal of the radius at the optical axis, K is a conic constant, and D, E, F G, H and I; are aspheric coefficients. The second lens unit G2 is biconvex and preferably consists of a single biconvex element having spherical surfaces, and is of a glass material to minimize the variation of refractive index with temperature. The lens unit G3 acts as a field flattener, that is, it corrects Petzval curvature of the first and second lens units. The concave image side surface of the third lens unit G3 may be spherical or aspheric, as hereinafter set forth. AS disclosed in U.S. Pat. No. 4,685,774. The spacing D 12 between the first element of lens unit G1 and lens unit G2 is important in aiding in the correction of field curvature. The spacing D 12 between the first and second lens units should be 0.10<¦D 12 /F 3 ¦<0.48 where F 3 is the equivalent focal length of the third lens unit. If ¦D 12 /F 3 ¦ goes below 0.10, the field curvature becomes over corrected and the image quality becomes unacceptable. If ¦D 12 /F 3 ¦ exceeds 0.48, the field curvature is undercorrected and the image quality is again not acceptable. As one attempt to increase the field angle of the lens, more astigmatism is introduced. This may be corrected at the expense of correction of spherical aberration in the second lens unit G2. The lens unit G1 then corrects for the spherical aberration introduced by lens unit G2 as well as coma and some other off-axis aberration. This is achieved by providing element L1 with two aspheric surfaces S1 and S2, which define element L1 as having positive optical power at the optical axis which decreases with distance from the optical axis and may change to negative optical power, which becomes very strong at the time limit of the clear aperture. There is set forth the aspheric optical power K CA /K A of the first lens element L1 of each prescription at or adjacent the clear aperture from the optical axis to the limit of the clear aperture or just adjacent the limit of the clear aperture. In each case the power at the optical axis is positive and decreases with height y and may become negative and then increase in negative power to an absolute value at least two and one-half times the optical power at the axis with one exception. These relationships exemplify the change in optical power of the lens element L1 from the optical axis to the limit of the clear aperture of the lens. The optical power K y is calculated from the equation K y = (n-1)(C 1y -C 2y ) where n is the index of the refraction of lens element L1, C 1y is the local curvature of the first lens surface at a height y from the optical axis A, and C 2y is the local curvature of the second lens surface at the height y from the optical axis. SUMMARY OF THE INVENTION Accordingly, it is an object of the present invention to provide a projection lens. It is another object of the present invention to provide an improved projection lens capable of substantially and advantageously implementing a distinct picture by compensating for chromatic aberration and a residual aberration. To achieve, these objects, there is provided an improved projection lens according to claim 1 or claim 12. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a side view of showing a projection lens axial and off-axis rays traced from a conventional conjugator. Figs. 2A to 2C are aberration graph/showing the projection shown in Fig. 1. Fig. 3A is a characteristic diagram showing an emission spectrum of a green CRT phosphor surface. Fig. 3B is a characteristic diagram showing an emission spectrum distortion of a blue CRT phosphor surface. Fig. 3C is a characteristic diagram showing an emission spectrum distortion of a red CRT phosphor surface. Fig. 4 is a side view showing a projection lens of a first embodiment according to the present invention. Fig. 5 is a side view showing a projection lens of a second embodiment according to the present invention. Fig. 6 is a side view showing a projection lens of a third embodiment according to the present invention. Fig. 7 is a side view showing a projection lens of a fourth embodiment according to the present invention. Fig. 8 is a side view showing a projection lens of a fifth embodiment according to the present invention. Fig. 9 is a side view showing a projection lens of a sixth embodiment according to the present invention. Fig. 10A is a characteristic diagram showing a spherical aberration of the projection lens shown in Fig. 4. Fig. 10B is a characteristic diagram showing an upper surface aberration (field curvature) of the projection lens shown in Fig. 4. Fig. 10C is a characteristic diagram showing a distortion of the projection lens shown in Fig. 4. Fig. 11A is a characteristic diagram showing aspheric aberration of the projection lens shown in Fig. 5. Fig. 11B is a characteristic diagram showing an upper surface aberration (field curvature) of the projection lens shown in Fig. 5. Fig. 11C is a characteristic diagram showing a distortion of the projection lens shown in Fig. 5. Fig. 12A is a characteristic diagram showing a spheric surface aberration of the projection lens shown in Fig. 6. Fig. 12B is a characteristic diagram showing an upper surface aberration (field curvature) of the projection lens shown in Fig. 6. Fig. 12C is a characteristic diagram showing a distortion of the projection lens shown in Fig. 6. Fig. 13A is a characteristic diagram showing a spheric surface aberration of the projection lens shown in Fig. 7. Fig. 13B is a characteristic diagram showing an upper surface aberration of the projection lens shown in Fig. 7. Fig. 13C is a characteristic diagram showing a distortion of the projection lens shown in Fig. 7. Fig. 14A is a characteristic diagram showing a spheric surface aberration of the projection lens shown in Fig. 8. Fig. 14B is a characteristic diagram showing an upper surface aberration of the projection lens shown in Fig. 8. Fig. 14C is a characteristic diagram showing a distortion of the projection lens shown in Fig. 8. Fig. 15A is a characteristic diagram showing a spheric surface aberration of the projection Lens shown in Fig. 9. Fig. 15B is a characteristic diagram showing an upper surface aberration of the projection lens shown in Fig. 9. Fig. 15C is a characteristic diagram showing modulation transfer function of the projection lens shown in Fig. 9. Fig. 16 is a characteristic diagram showing a resolution of the projection lens shown Fig. 4. Fig. 17 is a characteristic diagram showing a resolution of the projection shown in Fig. 9. DETAILED DESCRIPTION OF THE INVENTION Referring to Figs. 4 through 9, there are shown side views of the projection lens according to the present invention. As shown therein, the projection lens includes a first lens group 100 having a relatively weak positive power to a screen for eliminating spherical surface aberration, a second lens group 101 having a positive power, including a biconvex lens L2 cemented to a concave lens L3, a third lens group 102 in order to compensate the coma aberration, and a fourth lens groups 103 having a high negative optical power in order to compensate field dependent aberrations. The lens elements are provided with serial reference numerals L1 to L5 from the object to the image. The surfaces of the first through fifth lens elements L1 through L5 are indicated by serial reference numerals S1 through S11 and Si. In addition, in the drawings, "Stop" denotes an iris located between the first lens group 100 and the second lens group 101 and "C" denotes a coolant. As described above, the lens system embodying the present invention consists of four groups consisting of 5 lenses, so that the projection lens can secure a good quality performance such as large screen diameter, quality display, shorter focus wider display angle and a thermalisation. For quality display, F/number of lens should be less, so that the diameter of the lens increases. Accordingly, since the spherical aberration increases, the aspherical lens element L1 having a meniscus shaped in the same way as the first lens 100 shown in Fig. 4 is required in order to avoid such spherical aberration. In addition, the projection lens requires a lens having a big magnifying ratio in order to minimize the focus shift in accordance with the temperature changes, so that the lens should be a biconvex lens and made of glass. The projection lens embodying the present invention makes aberration in an upper portion (in an outer portion of the field), including distortion aberration since the size of the high definition set is decreased, so that a lens element L5 concave to the "upper" surface of the screen of the fourth lens group 103, as shown in Fig. 4, is advantageously provided. In addition, it is more effective to provide aspheric surface S9 on the upper screen surface of such lens and to provide a proper curvature on the phosphor surface Si of the CRT. However, since it is still difficult to correct for the coma aberration and residual aberration and to enhance the outer or corner optical illumination using the fourth lens group 103 only, as shown in Fig. 4 the third lens group 102 provided between the second lens group 101 and the fourth lens group 103 is required to correct for such problems. To begin with, it is very effective to minimize the Petzval sum P G3 of the third lens group 102 in order to avoid the "upper" or outer surface aberration (field curvature) which is not substantially corrected at the fourth lens group 103. where P G3 is the Petzval sum of the third lens group 102, K G3 is the power ratio of the third lens group 102, N G3 is the power ratio of the fourth lens element L4 of the third lens group 102, C 7 is the curvature of the "upper" surface of the screen side of the fourth lens element L4 of the third lens group 102, and C 8 is the curvature to the surface of the CRT side of the fourth lens element L4 of the third lens group 102. Accordingly, as shown by formula 2, the curvature of both surfaces S7 and S8 of the fourth lens element L4 should have the same sign value in order to minimize the Petzval sum of the third lens group 102. The sign of the curvature radius at the optical axis should be a minus, so that the concave shape thereof is provided toward the screen. In addition, the shape of the third lens group 102 should be concave at an outer extent or effective diameter(that is, the end portion of the fourth lens element L4) so that rays at the effective diameter are not cut, thereby displaying the image on the end portion (corners) of the phosphor surface Si of the CRT. In addition, plastic lens are not preferably be used as power lens because the changes of the curvature ratio is 10 times those of glass in accordance with the temperature changes. Accordingly, the curvature (and correlatively optical power) of the plastic lens should be small so that the performance of the projection lens can substantially be obtained by adapting the aspheric surface which is good for the aberration correction. Referring to Figs. 4 through 9, the second lens group 101 embodying the present invention is a pair of cemented glass lenses. Here, the reason why the second lens group 101 is formed with cemented lens is as follows. Generally, the display (imaging) quality of the projection TV is affected by the lens elements which are adapted at the green CRT. However, referring to Fig. 3A, showing an inspection of the spectrum characteristic of the green CRT, the red and blue concurrently come out beside the central wavelength which is referred to the green, so that chromatic aberrations occur due to another color of the green CRT (fig.3A) The chromatic aberration acts as a factor of decreasing the resolution of the lens and of reducing the contrast, so that it is not good for the optical system for quality display and high definition television. The present invention provides a biconvex lens cemented with concave lens in the second lens group 101. The cemented lens of the second lens group 101 consists of a second lens element L2 having a convex shape with a low dispersion(a large Abbe number) and a third lens element L3 having a concave shape with a large dispersion(a small Abbe number) and is effective for correcting for the chromatic aberration of the optical system. The spectrum of the phosphor surface Si of the CRT, as shown in Fig. 3C, has a strong color characteristic because the width of the wavelength is narrow, so that chromatic aberration cannot occur. As shown in Fig. 3B, since the spectrum of the blue CRT is provided in the wide region of the wavelength, so that the compensation of the chromatic aberrations is required. The weights for the color emanated from the green CRT and adapted in the lens according to the present invention is as follows. wavelength (nm) weight 590nm 6 544nm 80 450nm 14 Referring to Figs. 10A through 15C, there are shown aberrations of the lens shown in Figs. 4 through 9 according to the present invention designed by adapting such concepts. In addition, examples of the embodiments according to the present invention are shown in the following tables. The first embodiment (Figs. 4 and 10) No Radius Thickness Refr. index Power ratio (Nd) Abbe No. (Vd) OBJ infinite 1148.440 S1: 79.70009 6.000 1.4915 57.9 S2: 100.57599 18.790 S3: infinite 17.000 S4: 71.17807 23.029 1.6031 60.7 S5: -90.82899 4.000 1.7552 27.5 S6: -161.40410 14.365 S7: -960.38209 7.059 1.4915 57.9 S8: -155.87479 34.000 S9: -46.18203 3.300 1.50 52.0 S10: -49.01676 8.000 1.435 S11: infinite 13.000 1.563 IMG -350.00000 -0.000 A spherical surface coefficient for a spherical surface No. K A B C D S1: -1.14278 -0.12928E-06 -0.42533E-09 0.15913E-13 0.22409E-16 S2: 3.03468 -0.22978E-06 -0.52783E-09 0.12357E-12 -0.21059E-16 S7: 0.00000 0.32759E-06 0.43299E-09 0.49903E-12 -0.33180E-15 S8: 12.78419 0.18182E-05 0.21562E-09 0.11299E-11 -0.44354E-15 S9: 0.31670 -0.17305E-05 0.2516E-08 -0.16231E-11 0.54321E-15 The second embodiment (Figs. 4 and 10) No Radius Thickness Ref. index (Nd) Abbe No. (Vd) OBJ infinite 1112.736 S1: 76.41966 6.335 1.4915 57.9 S2: 95.9440 18.090 S3: infinite 15.000 S4: 67.49192 24.342 1.6031 60.7 S5: -87.33557 3620 1.7552 27.5 S6: -163.49488 11.270 S7: -708.77108 6.596 1.4915 57.9 S8: -134.91412 33.000 S9: -46.45925 3.172 1.50 52.0 S10: -47.13150 9.000 1.435 S11: infinite 13.000 1.563 IMG -350.00000 -0.000 A spherical surface coefficients for a spherical surface No. K A B C D S1: -1.11598 -0.13182E-06 -0.49380E-09 0.47255E-13 0.18457E-16 S2: 2.87012 -0.23375E-06 -0.61698E-09 0.18039E-12 -0.34888E-16 S7: 0.00000 0.41461E-06 0.69743E-09 0.11311E-11 -0.66790E-15 S8: 10.98191 0.21471E-05 0.44243E-09 0.18415E-11 -0.66770E-15 S9: 0.48931 -0.27490E-05 0.34343-08 -0.24653E-11 0.87469E-15 The third embodiment (Figs. 6 and 12) No Radius Thickness Refr. index (Nd) Abbe No. (Vd) OBJ infinite 1169.692 S1: 79.18792 6.919 1.4915 57.9 S2: 102.63401 18.003 S3: infinite 9.835 S4: 76.29694 24.710 1.6031 60.7 S5: -95.00000 3.696 1.7552 27.5 S6: -148.79710 11.403 S7: -515.69609 8.000 1.4915 57.9 S8: -135.64498 35.231 S9: -46.00000 3.500 1.50 52.0 S10: -48.00000 8.500 1.435 S11: infinite 13.000 1.563 IMG -350.00000 -0.000 A spherical surface coefficient for a spherical surface No. K A B C D S1: -1.76552 -0.28538E-06 -0.53692E-09 0.50686E-13 0.23590E-16 S2: 3.23072 -0.59592E-06 -0.39291E-09 0.33002E-13 -0.13657E-16 S7: 0.00000 0.81697E-06 0.43593E-09 0.68366E-12 -0.30977E-15 S8: 10.00000 0.19989E-05 0.56185E-09 0.91827E-12 -0.22630E-15 S9: 0.31133 -0.22247E-05 0.26218-08 -0.20841E-11 0.76461E-15 The fourth embodiment (Figs. 7 and 13) No Radius Thickness Refr. index (Nd) Abbe No. (Vd) OBJ infinite 1154.867 S1: 84.71609 6.500 1.4915 47.9 S2: 115.08340 28.394 S3: infinite 0.000 S4: 75.40076 24.667 1.6031 60.7 S5: -95.00000 4.000 1.7552 27.5 S6: -142.250170 10.003 S7: -607.90200 8.000 1.4915 57.9 S8: -140.29061 35.793 S9: -46.00000 3.300 1.50 52.0 S10: -47.00000 8.500 1.435 S11: infinite 13.000 1.563 IMG -350.00000 -0.380 A spherical surface coefficients for a spherical surface No. K A B C D S1: -2.33488 -0.38824E-06 -0.42414E-09 0.92575E-13 0.48685E-17 S2: -2.85528 -0.19524E-06 0.41075E-10 -0.95711E-13 0.68474E-16 S7: 0.00000 0.10641E-05 0.11185E-09 0.12053E-11 -0.49461E-15 S8: 11.57219 0.21441E-05 0.25702E-09 0.11626E-11 -0.30104E-15 S9: 0.37569 -0.28034E-05 0.26936E-08 -0.19955E-11 0.74996E-15 The fifth embodiment (Figs. 8 and 14) No Radius Thickness Refr. index (Nd) Abbe No. (Vd) OBJ infinite 1165.190 S1: 79.55170 6.300 1.4915 57.9 S2: 105.27984 20.172 S3: infinite 0.000 S4: 71.00000 25.888 1.6030 60.7 S5: -95.00000 3.600 1.81965 22.5 S6: -154.15415 11.132 S7: -389.26313 7.422 1.4915 57.9 S8: -129.66159 34.146 S9: -45.00000 3.300 1.500 52.0 S10: -48.00000 8.500 1.435 S11: infinite 13.000 1.563 IMG -350.00000 -0.350 A spherical surface coefficients for a spherical surface No. K A B C D S1: -1.35068 -0.18379E-06 -0.47515E-09 0.64348E-13 0.15099E-16 S2: 3.28379 -0.41059E-06 -0.39179E-09 0.67282E-13 0.46370E-17 S7: -9.75709 0.64591E-06 0.17801E-10 0.11137E-11 -0.54687E-15 S8: 10.06411 0.19537E-05 0.65521E-09 0.84533E-12 -0.22590E-15 S9: 0.31927 -0.19883E-05 0.24170E-08 -0.16435E-11 0.63355E-15 The fifth embodiment(Figs. 9 and 15) No Radius Thickness Refer. index (Nd) Abbe No. (Vd) OBJ infinite 832.730 S1: 78.57000 6.300 1.4915 57.9 S2: 101.79000 20.818 S3: infinite 0.000 S4: 69.13985 24.522 1.6031 60.7 S5: -90.00000 4.000 1.6889 31.2 S6: -174.41387 11.384 S7: -449.98684 7.832 1.4915 57.9 S8: -132.11493 34.736 S9: -46.00000 3.500 1.500 52.0 S10: -48.00000 8.500 1.535 S11: infinite 13.000 1.563 IMG -350.00000 -0.356 A spherical surface coefficients for a spherical surface No. K A B C D S1: -1.35000 -0.18600E-06 -0.48900E-09 0.49600E-13 0.19400E-16 S2: 2.98600 -0.42500E-06 -0.41700E-09 0.59200E-13 0.55800E-17 S7: 0.00000 0.38571E-06 -0.36492E-09 0.12321E-11 -0.54861E-15 38: 10.03041 0.19339E-05 -0.87626E-10 0.13290E-11 -0.37737E-15 S9: 0.36900 -0.24200E-05 0.32500E-08 -0.24400E-11 0.87000E-15 As shown in Figs. 15A through 15C, the spherical aberration, a spherical upper surface aberration and chromatic aberration are relatively corrected in comparison with the conventional art. Referring to Figs. 16 through 17, there are shown MTF characteristics of Fig. 4 (table I) and Fig. 9(table VI). All lenses have enough MTF value at space frequency of 61p/mm. Here, when the space frequency 61p/mm is computed as a horizontal resolution of television, it is about 1200 TV-line. The projection lens according to the present invention have a proper performance as a lens of high definition television. Referring to Figs. 4 through 9, Si refers to the phosphor surface of the CRT. S11 refers to a panel surface of the CRT and C refers to coolant. The projection lens according to the present invention have utmost focusing capacity when the raster size of 12,7 x 13,5 cm (5.0" - 5.3") are displayed on the screen 9 to 15 times the CRT raster size. In addition, the maximum half field angle of the lens embodying the present invention is over 35° and F/number of lens is below 1.05. The distance from the screen to the phosphor surface Si of the fourth lens group 103 is very short, so that a television set with a thin thickness is possible with a full reflection mirror. In particular, the projection lens, data of which are shown in tables 1 through 5 according to the present invention is possible on 15,2 x 17,8 cm (60-70 inches) screen and the table VI shows for the screen of 10,2 x 12,7 cm (40-50 inches) of the projection lens. In addition, the focal length of the lens is 80-85mm. How to refer to the tables I through VI is as follows. For example, the curvature of the screen is flat at infinity and the distance from the screen to the front surface S1 of the first lens elements L1 of the first lens group 100 is 1148.44mm. The space between the screen and the front surface S1 of the first lens element L1 is called an object space OBJ and the refraction index is 1.0 because the space is in air. The curvature of the front surface S1 of the first lens group 100 is 79.70mm and the thickness is 6.0mm and the curvature ratio Nd of the first lens unit L1 is 1.4915 on the d-line and the Abbe number thereof is 57.9. The front surface S1 of the first lens unit L1 is aspheric and K, A, B, C, and D are defined as the following equation. Z = (r 2 /R D )[1+{1-(1+K)r 2 /R D 2 } 1/2 ]+A*r 4 +B*r 6 +C*r 8 +D*r 10 where R D is the curvature radius and is r 2 = x 2 + y 2 . Z-axis in the formula 3 is an optical axis. When the tangential direction of the lens is Y-axis, Z is the element value of each lens. The first to fifth lens elements L1 to L5 of the second to fourth lens group 101 to 103 including the first lens group 100 and the phosphor surface Si of the CRT and the radius, thickness, index, and Abbe number Vd of the panel surface S11 of the CRT is the same as above. The shape of the aspheric surface should preferably be maintained to be smooth for easy manufacturing. In addition, the thickness of the plastic lens should preferably be designed within a range of 3-8mm because the thickness is closely related to the manufacturing net price and the manufacturing time. As a result, the projection lens according to the present invention includes a first lens group 100 having a low curvature ratio and consequently small optical power for compensating for the spherical aberration which is closely related to the lens aperture, a second lens group 101 having a high curvature in order to secure the stable performance to and magnifying ratio when the surrounding temperature changes by cementing the convex second lens element L2 and the concave third lens element L3 having different dispersions, a third lens group 102 having a fourth lens element L4 which has the same sign as the curvature R D of both surfaces in order to compensate for the upper (outer) surface aberration and to enhance the surrounding light amount in the corners, and a fourth lens group 103 including a fifth lens L5 having a high negative power to the "upper" surface of the screen in order to compensate for the "upper" surface aberration and the distortion aberration. The projection lens including aforementioned elements according to the present invention satisfy the following condition as shown in table VII, for example: lenses spacing lens No. f0/f1 f0/f2 f0/f3 f0/f4 f0 1 0.120 0.941 0.223 -0.654 84.99 2 0.119 0.933 0.244 -0.620 81.99 3 0.133 0.928 0.229 -0.654 85.00 4 0.138 0.918 0.229 -0.644 84.00 5 0.139 0.941 0.218 -0.675 85.00 6 0.129 0.930 0.219 -0.635 82.50 0.11<f0/f1<0.14 0.91<f0/f2<0.95 0.21<f0/f3<0.25 -0.68<f0/f4<-0.62 where f0 is the entire focal length of the projection lens, f1 is the focal length of the first lens group, f2 is the focal length of the second lens group, f3 is the focal length of the third lens group, and f4 is the focal length of the fourth lens group. In addition, the following condition shown in table VIII should be satisfied in order to obtain a predetermined performance and a light amount at the screen surrounding or corners lens spacing lens No. D12 D23 D34 D12/f0 D23/f0 D34/f0 1 35.80 14.36 34.00 0.421 0.169 0.400 2 30.75 10.29 34.75 0.366 0.122 0.414 3 27.83 11.40 35.23 0.327 0.134 0.414 4 28.40 10.00 35.79 0.338 0.119 0.426 5 32.20 11.14 34.14 0.379 0.131 0.402 6 33.49 11.39 34.74 0.406 0.138 0.421 where D12 is the distance between the first lens group 100 and the second lens group 101 and f0 is the focal distance of the entire lens. 0.32<D12/f0<0.42 When the distance D23 between the second lens group 101 and the third lens group 102 meets the following condition, the coma aberration compensation is very effective in the extreme field. 1.1<D23/f0<1.7 In addition, the distance D34 between the third lens group 102 and the fourth lens group 103 should meet the following condition. 0.40<D34/f0<0.43 As the distance D34 increases, the light amount ratio or brightness at the screen corners decreases, If on the contrary (field curvature) the distance D34 decreases, upper surface aberration and coma aberration occur, so that the focusing performance of the projection lens decreases. The concave lenses should be provided in the second lens group 101 and the concave lens of the projection lens according to the present invention compensate for the chromatic aberration and the comma aberration. As shown in table IX, for example, in the second lens group 101, the following condition should be met in order to effectively compensate the chromatic aberration. powers of the second lens group lens No. f0/f2a f0/f2b V2a V2b f2a/f2b V2a/V2b 1 1.221 -0.304 60.7 27.5 -0.249 2.207 2 1.227 -0.326 60.7 27.5 -0.266 2.207 3 1.150 -0.239 60.7 27.5 -0.208 2.207 4 1.144 -0.241 60.7 23.8 -0.211 2.55 5 1.192 -0.277 60.7 22.6 -0.232 2.686 6 1.204 -0.302 60.7 31.2 -0.251 1.946 where f 2a is the focal distance of the second lens element L2 toward the screen in the second lens group, V 2a is the dispersion of the material, f 2b is the focal distance of the third lens element L3 toward the CRT in the second lens group 101, and V 2b is the dispersion of the material. Accordingly, the second lens group 101 is required to have a biconvex lens and a concave lens having negative power in order to compensate the chromatic aberration and the coma aberration. -0.62<f 2a V 2a /f 2b V 2b <-0.4 The formula 11 is referred to in the following description. The focal distance changes δf2 due to focal variations of the lens in which the second convex lens element L2 and the third concave lens element L3 have a different dispersion from each other as in the second lens group 101 is as follows. δf2 = 1/(f 2a V 2a )+1/(f 2b V 2b ) Here, in order to maintain a predetermined focal distance for wavelength changes, δf2 should be zero. However the chromatic aberration for the system of the second convex lens element L2 and the third convex lens element L3 exists within a predetermined region since the chromatic aberration occurred due to other lens group is added thereto. In order to asign a proper chromatic aberration of the second lens group 101, it is possible to designate the relative value of f 2a V 2a and f 2b V 2b in the formula 12. If the value of f 2a V 2a /f 2b V 2b is larger than -0.4 in formula 11, the chromatic aberration becomes an under type as the curvature ratio of the second lens element L2 relatively increases; on the contrary if the value of f 2a V 2a /f 2b V 2b is smaller than -0.6 in the formula 11, the chromatic aberration becomes an over type since the power of the third lens element L3 increases, so that the entire chromatic compensation can not be secured. Accordingly, the chromatic compensation is well achieved when the value of f 2a V 2a /f 2b V 2b is between -0.62 and -0.4.

Claims: A projection lens for projection on a screen, comprising: a first lens group (100) including a lens element (L1) convex to a screen and having a relatively weak positive optical power, for eliminating spherical aberrations; a second lens group (101) having a positive optical power, , including a lens element having positive optical power element and a lens element having negative optical power element, which have different dispersions; a third lens group (102) having a positive optical power on an optical axis and a radius sign of a curvature surface toward an upper surface having the same radius code as the radius for compensation of high level coma aberrations; and a fourth lens group having a negative relatively high optical power toward an upper surface of the screen for compensation of field dependent aberrations, wherein said lens satisfies a condition 0.32<D12/f0<0.42 where D12 is the distance between the first lens group and the second lens group and f0 is the focal distance of the entire projection lens, and a condition 0.11<f0/f1<0.14 0.91<f0/f2<0.95 0.21<f0/f3<0.25 -0.68<f0/f4<-0.62 where f0 is the focal distance of the entire projection lens, f1 is the focal distance of the first lens group, f2. is the focal distance of the second lens group, f3 is the focal distance of the third lens group, and f4 is the focal distance of the fourth lens group. The lens of claim 1, wherein said first lens group is formed of a an a spherical single lens element which is positive at the optical axis and changes to a negative optical power adjacent the outer extent of a clear aperture in order to compensate for aperture dependent aberrations. The lens of claim 1 or 2, wherein said second lens group of high optical power includes a bi convex lens elements having an Abbe's dispersion number Vd of more than 60 and a lens concave to the screen having an Abbe's dispersion number Vd less than 35. The lens of claim 1, 2 or 3, wherein said second lens group satisfies a condition -0.62<f 2a V 2a /f 2b V 2b <-0.4 where f 2a is the focal distance of the lens element having a positive optical power in the second lens group, f 2b is the focal distance of the lens element having a negative optical power in the second lens group, V 2a is the Abbe's dispersion number of the positive lens element in the second lens group, and V 2b is the Abbe's dispersion number of the negative lens element in the second lens group. The lens of claim 1, wherein said lens satisfies a condition 0.11<D23/f0<0.17 where D23 is the distance between the second lens group and the third lens group and f0 is the entire focal distance of the projection lens. The lens of claim 1, wherein the distance between said third lens group and said fourth lens group satisfies a condition 0.40<D34/f0<0.43 where D34 is the distance between the third lens group and the fourth lens group and f0 is the entire focal distance of the projection lens. The lens of claim 1, wherein said second lens group satisfies a condition -0.62<f 2a V 2a /f 2b V 2b <-0.4 where f 2a is the focal distance of the lens element which faces toward the screen, V 2a is the dispersion of the material of said lens, f 2b is the focal distance of the lens element which faces toward the CRT, and V 2b is the dispersion of the material of said lens. The lens of claim 7, wherein said focal distance of said second lens group satisfies a condition δf2 = 1/(f 2a V 2a )+1/(f 2b V 2b ) where δf is the focal distance shift in accordance with the wavelength of the cemented lens, f 2a is the focal distance of the lens element which faces toward the screen, V 2a is the dispersion of the material of said lens, f 2b is the focal distance of the lens element which faces toward the CRT, and V 2b is the dispersion of the material of said lens. A projection lens, comprising: a first lens group (100) having a lens (L1) convex to a screen and of weak positive optical power for eliminating a spherical aberration a second lens group having an overall positive optical power and consisting of a positive bi-convex lens element (L2) in contact with a negative lens element (L3), respectively, having different optical dispersions; a third lens group (102); and a fourth lens group having a negative optical power and concave toward the screen for compensating field dependent aberrations, wherein said lens satisfies a condition 0.32<D12/f0<0.42 where D12 is the distance between the first lens group and the second lens group and f0 is the focal length of the entire projection lens, and wherein said lens further satisfies a condition 0.11<D23/f0<0.17 where D23 is the distance between the second lens group and the third lens group and to is the entire focal distance of the projection lens. A projection lens, comprising: a first lens group (100) having a lens (L1) convex to a screen and of weak positive optical power for eliminating a spherical aberration a second lens group having an overall positive optical power and consisting of a positive bi-convex lens element (L2) in contact with a negative lens element (L3), respectively, having different optical dispersions; a third lens group (102) and a fourth lens group having a negative optical power and concave toward the screen for compensating field dependent aberrations, wherein said lens satisfies a condition 0.32<D12/f0<0.42 where D12 is the distance between the first lens group and the second lens group and f0 is the focal length of the entire projection lens, and wherein said lens further satisfies a condition 0.11<D23/f0<0.17 where D23 is the distance between the second lens group and the third lens group and to is the entire focal distance of the projection lens. The lens of claim 10, wherein said first lens group is formed of an aspherical single lens element having a optical power which is positive at an optical axis and changes to negative optical power adjacent the outer extent of a clear aperture for compensation of an aperture dependent aberration. The lens of claim 9, wherein said second lens group satisfies a condition -0.62<f 2a V 2a /f 2b V 2b <-0.4 where f 2a is the focal length of the lens element having positive optical power in the second lens group, f 2b is the focal length of the lens element having negative optical power in the second lens group, V 2a is the Abbe's dispersion number of the lens element having positive optical power in the second lens group and V 2b is the Abbe's dispersion number of the lens element having negative optical power in the second lens group. The lens of any one of claims 9-10 and 12, wherein said third lens group and fourth lens group are spaced by a predetermined distance satisfying a condition 0.40<D34/f0<0.43 where D34 is the distance between the third lens group and the fourth lens group and f0 is the entire focal distance of the projection lens. The lens of any one of claims 9-10 and 12 wherein said lens system satisfies a condition 0.11<f0/f1<0.14 0.91<f0/f2<0.95 0.21<f0/f3<0.25 -0.68<f0/f4<-0.62 where fo is the entire focal distance of the projection lens, f1 is the focal distance of the first lens group, f2 is the focal distance of the second lens group, f3 is the focal distance of the third lens group, and f4 is the focal distance of the fourth lens group. The lens of any one of claims 9-10 and 12, wherein said second lens group satisfies a condition -0.62<f 2a V 2a /f 2b V 2b <-0.4 where f 2a is the focal distance of the lens element which faces toward the screen, V 2a is the dispersion of the material of said lens, f 2b is the focal distance of the lens element which faces toward the CRT, and V 2b is the dispersion of the material of said lens. The lens of claim 15, wherein said second lens group includes a focal distance satisfying a condition δf2 = 1/(f 2a V 2a )+1/(f 2b V 2b ) where δf is the focal distance shift in accordance with the wavelength of the cemented lens, f 2a is the focal distance of the lens element which faces toward the screen, V 2a is the dispersion of the material of said lens, f 2b is the focal distance of the lens element which faces toward the CRT, and V 2b is the dispersion of the material of said lens. The projection lens of any one of claims 9, 10 and 12-15, wherein said second lens group is formed of glass.

Inventors: PARK SUNG CHAN, PARK, SUNG CHAN
Applicants: LG ELECTRONICS INC, LG ELECTRONICS INC.
Application year: 1995
Main classification: G02B13
IPC codes: G02B13, G02B9