OPTICAL LENS SYSTEM AND PHOTOGRAPHING MODULE
20220334360 · 2022-10-20
Inventors
Cpc classification
G03B30/00
PHYSICS
G02B5/208
PHYSICS
G03B17/12
PHYSICS
International classification
G02B13/00
PHYSICS
G02B27/00
PHYSICS
Abstract
An optical lens system includes, in order from the object side to the image side: a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, an IR band-pass filter, wherein a stop is disposed before an object-side surface of the first lens or between an image-side surface of the first lens and an object-side surface of the second lens, a distance from the stop to an image plane along the optical axis is TSI, a distance from the object-side surface of the first lens to the image plane along the optical axis is TL, a distance from an image-side surface of the sixth lens to the image plane along the optical axis is BFL, a focal length of the optical lens system is f, following condition is satisfied: 0.25 mm.sup.−1<TL/((TSI−BFL)*f)<0.49 mm.sup.−1.
Claims
1. An optical lens system, in order from an object side to an image side, comprising: a first lens with refractive power, comprising an object-side surface and an image-side surface, the object-side surface of the first lens being convex near an optical axis, and at least one of the object-side surface and the image-side surface of the first lens being aspheric; a second lens with refractive power, comprising an object-side surface and an image-side surface, and at least one of the object-side surface and the image-side surface of the second lens being aspheric; a third lens with refractive power, comprising an object-side surface and an image-side surface, and at least one of the object-side surface and the image-side surface of the third lens being aspheric; a fourth lens with refractive power, comprising an object-side surface and an image-side surface, and at least one of the object-side surface and the image-side surface of the fourth lens being aspheric; a fifth lens with refractive power, comprising an object-side surface and an image-side surface, and at least one of the object-side surface and the image-side surface of the fifth lens being aspheric; a sixth lens with refractive power, comprising an object-side surface and an image-side surface, the object-side surface of the sixth lens being convex near the optical axis and the image-side surface of the sixth lens being concave near the optical axis, and at least one of the object-side surface and the image-side surface of the sixth lens being aspheric and provided with an inflection point; and an IR band-pass filter; wherein a stop is disposed before the object-side surface of the first lens or between the image-side surface of the first lens and the object-side surface of the second lens, a distance from the stop to an image plane along the optical axis is TSI, a distance from the object-side surface of the first lens to the image plane along the optical axis is TL, a distance from the image-side surface of the sixth lens to the image plane along the optical axis is BFL, a focal length of the optical lens system is f, and following condition is satisfied: 0.25 mm.sup.−1<TL/((TSI−BFL)*f)<0.49 mm.sup.−1.
2. The optical lens system as claimed in claim 1, wherein a focal length of the third lens is f3, a focal length of the fourth lens is f4, and following condition is satisfied: −1.93<f3/f4<0.62.
3. The optical lens system as claimed in claim 1, wherein a focal length of the first lens is f1, a radius of curvature of the object-side surface of the first lens is R1, and following condition is satisfied: −10.53<f1/R1<3.62.
4. The optical lens system as claimed in claim 1, wherein a focal length of the first lens is f1, the focal length of the optical lens system is f, and following condition is satisfied: −8.16<f1/f<2.15.
5. The optical lens system as claimed in claim 1, wherein a radius of curvature of the object-side surface of the third lens is R5, a radius of curvature of the image-side surface of the third lens is R6, and following condition is satisfied: −0.66<R5/R6<1.18.
6. The optical lens system as claimed in claim 1, wherein a central thickness of the fifth lens along the optical axis is CT5, a radius of curvature of the object-side surface of the fifth lens is R9, a radius of curvature of the image-side surface of the fifth lens is R10, and following condition is satisfied: −15.9 mm<CT5*(R9/R10)<1.81 mm
7. The optical lens system as claimed in claim 1, wherein the distance from the object-side surface of the first lens to the image plane along the optical axis is TL, the focal length of the optical lens system is f, and following condition is satisfied: 1.11<TL/f<1.88.
8. The optical lens system as claimed in claim 1, wherein the distance from the image-side surface of the sixth lens to the image plane along the optical axis is BFL, the distance from the object-side surface of the first lens to the image plane along the optical axis is TL, and following condition is satisfied: 0.15<BFL/TL<0.33.
9. The optical lens system as claimed in claim 1, wherein the distance from the stop to the image plane along the optical axis is TSI, the distance from the object-side surface of the first lens to the image plane along the optical axis is TL, the distance from the image-side surface of the sixth lens to the image plane along the optical axis is BFL, the focal length of the optical lens system is f, and following condition is satisfied: 0.28 mm.sup.−1<TL/((TSI−BFL)*f)<0.47 mm.sup.−1.
10. The optical lens system as claimed in claim 1, wherein a radius of curvature of the object-side surface of the fourth lens is R7, a radius of curvature of the image-side surface of the fourth lens is R8, and following condition is satisfied: 0.10<R7/R8<1.44.
11. The optical lens system as claimed in claim 1, wherein the focal length of the optical lens system is f, a radius of curvature of the image-side surface of the sixth lens is R12, a central thickness of the third lens along the optical axis is CT3, and following condition is satisfied: 3.88 mm.sup.−1<f/(R12*CT3)<10.89 mm.sup.−1.
12. The optical lens system as claimed in claim 1, wherein a central thickness of the sixth lens along the optical axis is CT6, a radius of curvature of the image-side surface of the sixth lens is R12, and following condition is satisfied: 0.27<CT6/R12<0.74.
13. The optical lens system as claimed in claim 4, wherein the focal length of the first lens is f1, the focal length of the optical lens system is f, and following condition is satisfied: −7.48<f1/f<1.98.
14. A photographing module, comprising: a lens barrel, an optical lens system disposed in the lens barrel, and an image sensor disposed on an image plane of the optical lens system, wherein the optical lens system, in order from an object side to an image side, comprising: a first lens with refractive power, comprising an object-side surface and an image-side surface, the object-side surface of the first lens being convex near an optical axis, and at least one of the object-side surface and the image-side surface of the first lens being aspheric; a second lens with refractive power, comprising an object-side surface and an image-side surface, and at least one of the object-side surface and the image-side surface of the second lens being aspheric; a third lens with refractive power, comprising an object-side surface and an image-side surface, and at least one of the object-side surface and the image-side surface of the third lens being aspheric; a fourth lens with refractive power, comprising an object-side surface and an image-side surface, and at least one of the object-side surface and the image-side surface of the fourth lens being aspheric; a fifth lens with refractive power, comprising an object-side surface and an image-side surface, and at least one of the object-side surface and the image-side surface of the fifth lens being aspheric; a sixth lens with refractive power, comprising an object-side surface and an image-side surface, the object-side surface of the sixth lens being convex near the optical axis and the image-side surface of the sixth lens being concave near the optical axis, and at least one of the object-side surface and the image-side surface of the sixth lens being aspheric and provided with an inflection point; and an IR band-pass filter; wherein a stop is disposed before the object-side surface of the first lens or between the image-side surface of the first lens and the object-side surface of the second lens, a distance from the stop to the image plane along the optical axis is TSI, a distance from the object-side surface of the first lens to the image plane along the optical axis is TL, a distance from the image-side surface of the sixth lens to the image plane along the optical axis is BFL, a focal length of the optical lens system is f, and following condition is satisfied: 0.25 mm.sup.−1<TL/((TSI−BFL)*f)<0.49 mm.sup.−1.
15. The photographing module as claimed in claim 14, wherein a focal length of the third lens is f3, a focal length of the fourth lens is f4, and following condition is satisfied: −1.93<f3/f4<0.62.
16. The photographing module as claimed in claim 14, wherein a focal length of the first lens is f1, the focal length of the optical lens system is f, and following condition is satisfied: −8.16<f1/f<2.15.
17. The photographing module as claimed in claim 14, wherein the distance from the image-side surface of the sixth lens to the image plane along the optical axis is BFL, the distance from the object-side surface of the first lens to the image plane along the optical axis is TL, and following condition is satisfied: 0.15<BFL/TL<0.33.
18. A photographing module, comprising: a lens barrel, an optical lens system disposed in the lens barrel, and an image sensor disposed on an image plane of the optical lens system, wherein the optical lens system, in order from an object side to an image side, comprising: a first lens with refractive power, comprising an object-side surface and an image-side surface, the object-side surface of the first lens being convex near an optical axis, and at least one of the object-side surface and the image-side surface of the first lens being aspheric; a second lens with refractive power, comprising an object-side surface and an image-side surface, and at least one of the object-side surface and the image-side surface of the second lens being aspheric; a third lens with refractive power, comprising an object-side surface and an image-side surface, and at least one of the object-side surface and the image-side surface of the third lens being aspheric; a fourth lens with refractive power, comprising an object-side surface and an image-side surface, and at least one of the object-side surface and the image-side surface of the fourth lens being aspheric; a fifth lens with refractive power, comprising an object-side surface and an image-side surface, and at least one of the object-side surface and the image-side surface of the fifth lens being aspheric; a sixth lens with refractive power, comprising an object-side surface and an image-side surface, the object-side surface of the sixth lens being convex near the optical axis and the image-side surface of the sixth lens being concave near the optical axis, and at least one of the object-side surface and the image-side surface of the sixth lens being aspheric and provided with an inflection point; and an IR band-pass filter; wherein a distance from the object-side surface of the first lens to the image plane along the optical axis is TL, half of an image height that can be captured by the optical lens system on the image plane is IMH, and following condition is satisfied: 1.4<TL/IMH<2.37.
19. The photographing module as claimed in claim 18, wherein a focal length of the first lens is f1, a focal length of the optical lens system is f, and following condition is satisfied: −8.16<f1/f<2.15.
20. The photographing module as claimed in claim 18, wherein a distance from the stop to the image plane along the optical axis is TSI, the distance from the object-side surface of the first lens to the image plane along the optical axis is TL, a distance from the image-side surface of the sixth lens to the image plane along the optical axis is BFL, a focal length of the optical lens system is f, and following condition is satisfied: 0.25 mm.sup.−1<TL/((TSI−BFL)*f)<0.49 mm.sup.−1.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0043]
[0044]
[0045]
[0046]
[0047]
[0048]
[0049]
[0050]
[0051]
[0052]
[0053]
[0054]
[0055]
DETAILED DESCRIPTION
[0056] Referring to
[0057] The first lens 110 with negative refractive power, comprising an object-side surface 111 and an image-side surface 112, the object-side surface 111 of the first lens 110 being convex near the optical axis 190 and the image-side surface 112 of the first lens 110 being concave near the optical axis 190, the object-side surface 111 and the image-side surface 112 of the first lens 110 are aspheric, and the first lens 110 is made of plastic material.
[0058] The second lens 120 with positive refractive power, comprising an object-side surface 121 and an image-side surface 122, the object-side surface 121 of the second lens 120 being convex near the optical axis 190 and the image-side surface 122 of the second lens 120 being convex near the optical axis 190, the object-side surface 121 and the image-side surface 122 of the second lens 120 are aspheric, and the second lens 120 is made of plastic material.
[0059] The third lens 130 with negative refractive power, comprising an object-side surface 131 and an image-side surface 132, the object-side surface 131 of the third lens 130 being concave near the optical axis 190 and the image-side surface 132 of the third lens 130 being convex near the optical axis 190, the object-side surface 131 and the image-side surface 132 of the third lens 130 are aspheric, and the third lens 130 is made of plastic material.
[0060] The fourth lens 140 with positive refractive power, comprising an object-side surface 141 and an image-side surface 142, the object-side surface 141 of the fourth lens 140 being convex near the optical axis 190 and the image-side surface 142 of the fourth lens 140 being concave near the optical axis 190, the object-side surface 141 and the image-side surface 142 of the fourth lens 140 are aspheric, and the fourth lens 140 is made of plastic material.
[0061] The fifth lens 150 with positive refractive power, comprising an object-side surface 151 and an image-side surface 152, the object-side surface 151 of the fifth lens 150 being concave near the optical axis 190 and the image-side surface 152 of the fifth lens 150 being convex near the optical axis 190, the object-side surface 151 and the image-side surface 152 of the fifth lens 150 are aspheric, and the fifth lens 150 is made of plastic material.
[0062] The sixth lens 160 with negative refractive power, comprising an object-side surface 161 and an image-side surface 162, the object-side surface 161 of the sixth lens 160 being convex near the optical axis 190 and the image-side surface 162 of the sixth lens 160 being concave near the optical axis 190, the object-side surface 161 and the image-side surface 162 of the sixth lens 160 are aspheric and are provided with at least one inflection point, and the sixth lens 160 is made of plastic material.
[0063] The IR band-pass filter 170 made of glass is located between the sixth lens 160 and the image plane 181 and has no influence on the focal length of the optical lens system. The present embodiment selects a filter which is available in the light wavelength range of 940 nm±30 nm, but not limited to this.
[0064] The equation for the aspheric surface profiles of the respective lenses of the first embodiment is expressed as follows:
[0065] wherein:
[0066] z represents the value of a reference position with respect to a vertex of the surface of a lens and a position with a height h along the optical axis 190;
[0067] c represents a paraxial curvature equal to 1/R (R: a paraxial radius of curvature);
[0068] h represents a vertical distance from the point on the curve of the aspheric surface to the optical axis 190;
[0069] k represents the conic constant;
[0070] A, B, C, D, E, F, G, . . . represent the high-order aspheric coefficients.
[0071] In the first embodiment of the present optical lens system, a focal length of the optical lens system is f, a f-number of the optical lens system is Fno, the optical lens system has a maximum view angle FOV, and following conditions are satisfied: f=4.16 mm; Fno=1.35; and FOV=76.1 degrees.
[0072] In the first embodiment of the present optical lens system, a distance from the stop 100 to the image plane 181 along the optical axis 190 is TSI, a distance from the object-side surface 111 of the first lens 110 to the image plane 181 along the optical axis 190 is TL, a distance from the image-side surface 162 of the sixth lens 160 to the image plane 181 along the optical axis 190 is BFL, a focal length of the optical lens system is f, and following condition is satisfied: TL/((TSI−BFL)*f)=0.31 mm.sup.−1.
[0073] In the first embodiment of the present optical lens system, a focal length of the third lens 130 is f3, a focal length of the fourth lens 140 is f4, and following condition is satisfied: f3/f4=−1.27.
[0074] In the first embodiment of the present optical lens system, a focal length of the first lens 110 is f1, a radius of curvature of the object-side surface 111 of the first lens 110 is R1, and following condition is satisfied: f1/R1=−3.20.
[0075] In the first embodiment of the present optical lens system, the focal length of the first lens 110 is f1, the focal length of the optical lens system is f, and following condition is satisfied: f1/f=−2.83.
[0076] In the first embodiment of the present optical lens system, a radius of curvature of the object-side surface 131 of the third lens 130 is R5, a radius of curvature of the image-side surface 132 of the third lens 130 is R6, and following condition is satisfied: R5/R6=0.48.
[0077] In the first embodiment of the present optical lens system, a central thickness of the fifth lens 150 along the optical axis 190 is CT5, a radius of curvature of the object-side surface 151 of the fifth lens 150 is R9, a radius of curvature of the image-side surface 152 of the fifth lens 150 is R10, and following condition is satisfied: CT5*(R9/R10)=0.65 mm.
[0078] In the first embodiment of the present optical lens system, the distance from the object-side surface 111 of the first lens 110 to the image plane 181 along the optical axis 190 is TL, the focal length of the optical lens system is f, and following condition is satisfied: TL/f=1.57.
[0079] In the first embodiment of the present optical lens system, the distance from the image-side surface 162 of the sixth lens 160 to the image plane 181 along the optical axis 190 is BFL, the distance from the object-side surface 111 of the first lens 110 to the image plane 181 along the optical axis 190 is TL, and following condition is satisfied: BFL/TL=0.20.
[0080] In the first embodiment of the present optical lens system, a radius of curvature of the object-side surface 141 of the fourth lens 140 is R7, a radius of curvature of the image-side surface 142 of the fourth lens 140 is R8, and following condition is satisfied: R7/R8=0.26.
[0081] In the first embodiment of the present optical lens system, the focal length of the optical lens system is f, a radius of curvature of the image-side surface 162 of the sixth lens 160 is R12, a central thickness of the third lens 130 along the optical axis 190 is CT3, and following condition is satisfied: f/(R12*CT3)=5.46 mm.sup.−1.
[0082] In the first embodiment of the present optical lens system, a central thickness of the sixth lens 160 along the optical axis 190 is CT6, the radius of curvature of the image-side surface 162 of the sixth lens 160 is R12, and following condition is satisfied: CT6/R12=0.62.
[0083] In the first embodiment of the present optical lens system, the distance from the object-side surface 111 of the first lens 110 to the image plane 181 along the optical axis 190 is TL, half of an image height that can be captured by the optical lens system on the image plane 181 is IMH, and following condition is satisfied: TL/IMH=1.98.
[0084] In the first embodiment of the present optical lens system, the focal length of the first lens 110 is f1, a focal length of the second lens, the third lens, the fourth lens, the fifth lens and the sixth lens combined is f23456, and following condition is satisfied: f1/f23456=−4.02.
[0085] In the first embodiment of the present optical lens system, a focal length of the second lens 120 and the third lens 130 combined is f23, a focal length of the fourth lens 140 and the fifth lens 150 combined is f45, and following condition is satisfied: f23/f45=0.88.
[0086] The detailed optical data of the first embodiment is shown in table 1, and the aspheric surface data is shown in table 2.
TABLE-US-00001 TABLE 1 Embodiment 1 f(focal length) = 4.16 mm, Fno = 1.35, FOV = 76.1 deg. Curvature Thickness/ Abbe Focal surface Radius gap Material Index(nd) #(vd) length 0 object infinity 700.000 1 stop infinity −0.125 2 Lens 1 3.680 (ASP) 0.537 plastic 1.64 22.5 −11.78 3 2.312 (ASP) 0.091 4 Lens 2 2.289 (ASP) 0.796 plastic 1.64 22.5 3.26 5 −15.069 (ASP) 0.542 6 Lens 3 −2.520 (ASP) 0.500 plastic 1.64 22.5 −8.33 7 −5.284 (ASP) 0.132 8 Lens 4 3.067 (ASP) 0.477 plastic 1.64 22.5 6.58 9 11.592 (ASP) 0.557 10 Lens 5 −2.023 (ASP) 0.600 plastic 1.64 22.5 15.84 11 −1.869 (ASP) 0.035 12 Lens 6 2.409 (ASP) 0.941 plastic 1.64 22.5 −11.32 13 1.526 (ASP) 0.987 14 IR infinity 0.210 glass 1.52 64.2 band-pass filter 15 infinity 0.118 16 Image plane infinity — Note: reference wavelength is 940 nm
TABLE-US-00002 TABLE 2 Aspheric Coefficients surface 2 3 4 5 6 7 K: −1.0210E+01 −9.5009E+00 −7.6591E+00 2.4860E+01 6.5473E−02 −6.3437E+00 A: −8.1072E−03 −3.3255E−02 −1.4051E−02 −1.3959E−02 1.1973E−02 −2.9985E−02 B: 5.4994E−03 −6.1327E−03 −9.7572E−03 −7.6677E−03 −1.8031E−03 9.9731E−03 C: −6.5812E−03 −3.0071E−04 −1.4033E−03 5.0878E−04 4.6438E−03 8.1398E−04 D: 2.0960E−03 1.5899E−04 9.7934E−05 1.3677E−04 −3.4696E−04 −2.8401E−04 E: −2.9030E−04 1.7817E−04 6.9509E−05 −3.9645E−06 −1.7272E−04 −9.3987E−05 F: −1.3681E−05 −5.3643E−05 6.0460E−06 4.1257E−06 2.8561E−05 1.7151E−05 G: 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 −7.1819E−07 −8.0095E−08 surface 8 9 10 11 12 13 K: −7.4437E+00 2.6036E+01 −9.6040E+00 −4.5252E+00 −5.1778E+00 −4.3112E+00 A: 1.2598E−02 3.4185E−02 −5.6647E−03 −2.4313E−02 −6.3956E−02 −2.7041E−02 B: −1.1899E−02 −1.9032E−02 −5.6107E−03 2.2982E−03 1.1050E−02 4.0055E−03 C: −4.1719E−04 −2.3926E−04 1.5778E−03 −9.5630E−04 −1.3934E−03 −2.0475E−04 D: −1.8948E−05 4.7154E−04 8.8003E−05 4.3442E−04 −5.4623E−05 −7.9400E−05 E: −2.7808E−05 −2.0143E−05 9.4915E−06 8.4869E−06 2.7029E−05 1.7092E−05 F: 1.8417E−05 −1.5678E−06 −1.7085E−06 −7.9485E−06 1.6344E−06 −1.3688E−06 G: −7.2504E−07 −6.6423E−08 −1.1135E−06 5.1897E−07 −3.5580E−07 4.0192E−08
[0087] The units of the radius of curvature, the thickness and the focal length in table 1 are expressed in mm, the surface numbers 0-12 represent the surfaces sequentially arranged from the object-side to the image-side along the optical axis, wherein surface 0 represents a gap between the object and the stop 100 along the optical axis 190, surface 1 represents a gap between the stop 100 and the object-side surface 111 of the first lens 110 along the optical axis 190, the stop 100 is farther away from the object-side than the object-side surface 111 of the first lens 110, so it is expressed as a negative value, surfaces 2, 4, 6, 8, 10, 12, 14 are thicknesses of the first lens 110, the second lens 120, the third lens 130, the fourth lens 140, the fifth lens 150, the sixth lens 160, and the IR band-pass filter 170 along the optical axis 190, respectively, surface 3 represents a gap between the first lens 110 and the second lens 120 along the optical axis 190, surface 5 represents a gap between the second lens 120 and the third lens 130 along the optical axis 190, surface 7 represents a gap between the third lens 130 and the fourth lens 140 along the optical axis 190, surface 9 represents a gap between the fourth lens 140 and the fifth lens 150 along the optical axis 190, surface 11 represents a gap between the fifth lens 150 and the sixth lens 160 along the optical axis 190, surface 13 represents a gap between the sixth lens 160 and the IR band-pass filter 170 along the optical axis 190, surface 15 represents a gap between the IR band-pass filter 170 and the image plane 181 along the optical axis 190.
[0088] In table 2, k represents the conic coefficient of the equation of the aspheric surface profiles, and A, B, C, D, E, F, G . . . : represent the high-order aspheric coefficients. The tables presented below for each embodiment are the corresponding schematic parameter and image plane curves, and the definitions of the tables are the same as Table 1 and Table 2 of the first embodiment. Therefore, an explanation in this regard will not be provided again.
[0089] Referring to
[0090] The first lens 210 with positive refractive power, comprising an object-side surface 211 and an image-side surface 212, the object-side surface 211 of the first lens 210 being convex near the optical axis 290 and the image-side surface 212 of the first lens 210 being concave near the optical axis 290, the object-side surface 211 and the image-side surface 212 of the first lens 210 are aspheric, and the first lens 210 is made of plastic material.
[0091] The second lens 220 with positive refractive power, comprising an object-side surface 221 and an image-side surface 222, the object-side surface 221 of the second lens 220 being convex near the optical axis 290 and the image-side surface 222 of the second lens 220 being concave near the optical axis 290, the object-side surface 221 and the image-side surface 222 of the second lens 220 are aspheric, and the second lens 220 is made of plastic material.
[0092] The third lens 230 with negative refractive power, comprising an object-side surface 231 and an image-side surface 232, the object-side surface 231 of the third lens 230 being concave near the optical axis 290 and the image-side surface 232 of the third lens 230 being convex near the optical axis 290, the object-side surface 231 and the image-side surface 232 of the third lens 230 are aspheric, and the third lens 230 is made of plastic material.
[0093] The fourth lens 240 with positive refractive power, comprising an object-side surface 241 and an image-side surface 242, the object-side surface 241 of the fourth lens 240 being convex near the optical axis 290 and the image-side surface 242 of the fourth lens 240 being concave near the optical axis 290, the object-side surface 241 and the image-side surface 242 of the fourth lens 240 are aspheric, and the fourth lens 240 is made of plastic material.
[0094] The fifth lens 250 with positive refractive power, comprising an object-side surface 251 and an image-side surface 252, the object-side surface 251 of the fifth lens 250 being concave near the optical axis 290 and the image-side surface 252 of the fifth lens 250 being convex near the optical axis 290, the object-side surface 251 and the image-side surface 252 of the fifth lens 250 are aspheric, and the fifth lens 250 is made of plastic material.
[0095] The sixth lens 260 with negative refractive power, comprising an object-side surface 261 and an image-side surface 262, the object-side surface 261 of the sixth lens 260 being convex near the optical axis 290 and the image-side surface 262 of the sixth lens 260 being concave near the optical axis 290, the object-side surface 261 and the image-side surface 262 of the sixth lens 260 are aspheric and are provided with at least one inflection point, and the sixth lens 260 is made of plastic material.
[0096] The IR band-pass filter 270 made of glass is located between the sixth lens 260 and the image plane 281 and has no influence on the focal length of the optical lens system. The present embodiment selects a filter which is available in the light wavelength range of 940 nm±30 nm, but not limited to this.
[0097] The detailed optical data of the second embodiment is shown in table 3, and the aspheric surface data is shown in table 4.
TABLE-US-00003 TABLE 3 Embodiment 2 f(focal length) = 4.18 mm, Fno = 1.20, FOV = 76.7 deg. Curvature Thickness/ Abbe Focal surface Radius gap Material Index(nd) #(vd) length 0 object infinity 1000.000 1 stop infinity −0.264 2 Lens 1 3.511 (ASP) 1.001 plastic 1.64 22.5 7.51 3 12.662 (ASP) 0.491 4 Lens 2 3.537 (ASP) 0.360 plastic 1.64 22.5 39.08 5 3.979 (ASP) 0.425 6 Lens 3 −3.081 (ASP) 0.425 plastic 1.64 22.5 −13.47 7 −5.136 (ASP) 0.034 8 Lens 4 3.363 (ASP) 0.508 plastic 1.64 22.5 8.39 9 8.929 (ASP) 0.383 10 Lens 5 −4.758 (ASP) 0.746 plastic 1.64 22.5 6.70 11 −2.353 (ASP) 0.035 12 Lens 6 2.334 (ASP) 0.804 plastic 1.64 22.5 −7.95 13 1.376 (ASP) 0.887 14 IR infinity 0.210 glass 1.52 64.2 band-pass filter 15 infinity 0.242 16 Image plane infinity — Note: reference wavelength is 940 nm
TABLE-US-00004 TABLE 4 Aspheric Coefficients surface 2 3 4 5 6 7 K: 2.1006E+00 3.9214E+01 7.5124E−01 1.3614E+00 7.3391E−01 −1.4398E+00 A: −1.5056E−02 −2.6675E−02 −4.3750E−02 −3.3590E−02 1.3140E−02 −3.4855E−02 B: −3.9055E−04 −4.5510E−04 −8.1067E−03 −8.0076E−03 −2.5329E−03 9.7669E−03 C: −9.1445E−04 −2.2176E−04 −1.1308E−04 1.0560E−03 4.5118E−03 −1.0726E−04 D: −4.1224E−04 −2.6544E−04 3.2822E−04 1.1283E−04 −2.8914E−04 8.6074E−05 E: 1.8353E−04 1.2898E−04 2.4045E−05 −9.0609E−06 −1.5438E−04 1.1312E−05 F: −3.1186E−05 −2.1083E−05 −3.1316E−06 −3.3096E−06 2.8448E−05 1.9781E−05 G: −1.3699E−06 1.6792E−07 −4.4684E−07 2.1661E−07 −1.2276E−06 −4.6485E−06 surface 8 9 10 11 12 13 K: −7.9608E+00 1.4092E+01 −5.1555E+01 −8.8743E+00 −8.1662E−01 −3.6346E+00 A: 4.4921E−03 3.4682E−02 2.2872E−02 −1.7588E−02 −8.4636E−02 −3.2011E−02 B: −9.9189E−03 −1.9360E−02 −9.0207E−03 1.4342E−03 5.2778E−03 4.6356E−03 C: −9.8463E−05 3.8421E−04 1.0906E−03 −1.2410E−03 6.8389E−04 −4.2730E−04 D: 4.0088E−05 6.0099E−04 −2.4014E−04 3.5846E−04 −6.0417E−05 4.8462E−06 E: 4.9738E−06 −8.0953E−05 1.1310E−06 −8.9910E−06 −9.1248E−07 4.5162E−06 F: 2.2099E−05 −1.4877E−05 6.3495E−06 −6.9895E−06 −3.5846E−08 −5.3319E−07 G: −3.2737E−06 3.1321E−06 −5.8299E−07 8.8840E−07 1.3233E−08 2.0103E−08
[0098] In the second embodiment, the equation of the aspheric surface profiles of the aforementioned lenses is the same as the equation of the first embodiment. Also, the definitions of these parameters shown in the following table are the same as those stated in the first embodiment with corresponding values for the second embodiment, so an explanation in this regard will not be provided again.
[0099] Moreover, these parameters can be calculated from Table 3 and Table 4 as the following values and satisfy the following conditions:
TABLE-US-00005 Embodiment 2 f[mm] 4.18 CT5*(R9/R10) [mm] 1.51 Fno 1.20 f/(R12*CT3) [mm.sup.−1] 7.14 FOV[deg.] 76.7 CT6/R12 0.58 TL/((TSI-BFL)*f) [mm.sup.−1] 0.32 TL/f 1.57 f1/f 1.80 BFL/TL 0.20 f3/f4 −1.60 TL/IMH 1.93 f1/R1 2.14 f1/f23456 0.96 R5/R6 0.60 f23/f45 −5.21 R7/R8 0.38
[0100] Referring to
[0101] The first lens 310 with positive refractive power, comprising an object-side surface 311 and an image-side surface 312, the object-side surface 311 of the first lens 310 being convex near the optical axis 390 and the image-side surface 312 of the first lens 310 being convex near the optical axis 390, the object-side surface 311 and the image-side surface 312 of the first lens 310 are aspheric, and the first lens 310 is made of plastic material.
[0102] The second lens 320 with negative refractive power, comprising an object-side surface 321 and an image-side surface 322, the object-side surface 321 of the second lens 320 being concave near the optical axis 390 and the image-side surface 322 of the second lens 320 being convex near the optical axis 390, the object-side surface 321 and the image-side surface 322 of the second lens 320 are aspheric, and the second lens 320 is made of plastic material.
[0103] The third lens 330 with positive refractive power, comprising an object-side surface 331 and an image-side surface 332, the object-side surface 331 of the third lens 330 being convex near the optical axis 390 and the image-side surface 332 of the third lens 330 being convex near the optical axis 390, the object-side surface 331 and the image-side surface 332 of the third lens 330 are aspheric, and the third lens 330 is made of plastic material.
[0104] The fourth lens 340 with negative refractive power, comprising an object-side surface 341 and an image-side surface 342, the object-side surface 341 of the fourth lens 340 being concave near the optical axis 390 and the image-side surface 342 of the fourth lens 340 being convex near the optical axis 390, the object-side surface 341 and the image-side surface 342 of the fourth lens 340 are aspheric, and the fourth lens 340 is made of plastic material.
[0105] The fifth lens 350 with negative refractive power, comprising an object-side surface 351 and an image-side surface 352, the object-side surface 351 of the fifth lens 350 being concave near the optical axis 390 and the image-side surface 352 of the fifth lens 350 being convex near the optical axis 390, the object-side surface 351 and the image-side surface 352 of the fifth lens 350 are aspheric, and the fifth lens 350 is made of plastic material.
[0106] The sixth lens 360 with positive refractive power, comprising an object-side surface 361 and an image-side surface 362, the object-side surface 361 of the sixth lens 360 being convex near the optical axis 390 and the image-side surface 362 of the sixth lens 360 being concave near the optical axis 390, the object-side surface 361 and the image-side surface 362 of the sixth lens 360 are aspheric and are provided with at least one inflection point, and the sixth lens 360 is made of plastic material.
[0107] The IR band-pass filter 370 made of glass is located between the sixth lens 360 and the image plane 381 and has no influence on the focal length of the optical lens system. The present embodiment selects a filter which is available in the light wavelength range of 940 nm±30 nm, but not limited to this.
[0108] The detailed optical data of the third embodiment is shown in table 5, and the aspheric surface data is shown in table 6.
TABLE-US-00006 TABLE 5 Embodiment 3 f(focal length) = 3.85 mm, Fno = 1.40, FOV = 75.7 deg. Curvature Thickness/ Abbe Focal surface Radius gap Material Index(nd) #(vd) length 0 object infinity 700.000 1 stop infinity −0.135 2 Lens 1 3.372 (ASP) 0.776 plastic 1.64 22.5 5.06 3 −41.992 (ASP) 1.008 4 Lens 2 −1.281 (ASP) 0.383 plastic 1.64 22.5 −12.47 5 −1.710 (ASP) 0.034 6 Lens 3 3.947 (ASP) 0.497 plastic 1.66 20.4 4.07 7 −7.141 (ASP) 0.035 8 Lens 4 −6.464 (ASP) 0.337 plastic 1.64 22.5 −12.02 9 −49.334 (ASP) 0.447 10 Lens 5 −1.403 (ASP) 0.402 plastic 1.64 22.5 −95.36 11 −1.595 (ASP) 0.034 12 Lens 6 1.723 (ASP) 0.592 plastic 1.64 22.5 44.91 13 1.595 (ASP) 0.818 14 IR infinity 0.210 glass 1.52 64.2 band-pass filter 15 infinity 0.380 16 Image plane infinity — Note: reference wavelength is 940 nm
TABLE-US-00007 TABLE 6 Aspheric Coefficients surface 2 3 4 5 6 7 K: −4.7869E−01 −4.9619E+01 −5.8392E−01 −1.1222E+00 1.2562E+00 −7.1753E+01 A: −1.4254E−02 −2.3491E−02 7.8525E−02 2.4828E−02 −3.3494E−02 4.6342E−02 B: 4.7196E−04 −6.9391E−03 1.6406E−03 6.7002E−03 1.0370E−02 −1.6409E−02 C: −7.3515E−03 −1.3149E−03 2.2000E−03 −5.5815E−05 −3.7338E−03 −4.9325E−03 D: 2.7825E−03 7.0090E−04 2.2536E−04 −6.1811E−04 −2.0509E−03 1.4958E−03 E: −8.6255E−04 −1.9918E−04 −8.1439E−05 1.3048E−05 4.9360E−04 −6.3492E−06 F: 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 G: 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 surface 8 9 10 11 12 13 K: −9.7715E+01 −7.2978E+01 −2.0393E+00 −1.5608E+00 −7.3021E−01 −8.8325E−01 A: 6.9112E−02 2.0814E−02 5.4243E−02 4.7352E−02 −5.2881E−02 −5.2611E−02 B: −3.2329E−02 −1.7013E−02 −1.7392E−03 3.6419E−04 −7.8613E−04 6.0350E−05 C: −4.5710E−03 4.7181E−03 −7.0691E−04 −4.5470E−04 6.1671E−04 1.1366E−03 D: 5.8572E−03 −2.6911E−04 −4.8525E−05 −9.7587E−05 −4.9056E−05 −2.5623E−04 E: −1.3296E−03 −2.1095E−04 8.4691E−06 2.3271E−06 2.7961E−06 2.5498E−05 F: 8.5543E−05 3.4657E−05 1.4334E−06 1.6801E−06 −1.4351E−07 −9.2755E−07 G: 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 −1.5196E−09 2.4046E−09
[0109] In the third embodiment, the equation of the aspheric surface profiles of the aforementioned lenses is the same as the equation of the first embodiment. Also, the definitions of these parameters shown in the following table are the same as those stated in the first embodiment with corresponding values for the third embodiment, so an explanation in this regard will not be provided again.
[0110] Moreover, these parameters can be calculated from Table 5 and Table 6 as the following values and satisfy the following conditions:
TABLE-US-00008 Embodiment 3 f[mm] 3.85 CT5*(R9/R10) [mm] 0.35 Fno 1.40 f/(R12*CT3) [mm.sup.−1] 4.86 FOV[deg.] 75.7 CT6/R12 0.37 TL/((TSI-BFL)*f) [mm.sup.−1] 0.35 TL/f 1.55 f1/f 1.31 BFL/TL 0.24 f3/f4 −0.34 TL/IMH 1.93 f1/R1 1.50 f1/f23456 0.62 R5/R6 −0.55 f23/f45 −0.44 R7/R8 0.13
[0111] Referring to
[0112] The first lens 410 with negative refractive power, comprising an object-side surface 411 and an image-side surface 412, the object-side surface 411 of the first lens 410 being convex near the optical axis 490 and the image-side surface 412 of the first lens 410 being concave near the optical axis 490, the object-side surface 411 and the image-side surface 412 of the first lens 410 are aspheric, and the first lens 410 is made of plastic material.
[0113] The second lens 420 with positive refractive power, comprising an object-side surface 421 and an image-side surface 422, the object-side surface 421 of the second lens 420 being convex near the optical axis 490 and the image-side surface 422 of the second lens 420 being concave near the optical axis 490, the object-side surface 421 and the image-side surface 422 of the second lens 420 are aspheric, and the second lens 420 is made of plastic material.
[0114] The third lens 430 with positive refractive power, comprising an object-side surface 431 and an image-side surface 432, the object-side surface 431 of the third lens 430 being convex near the optical axis 490 and the image-side surface 432 of the third lens 430 being concave near the optical axis 490, the object-side surface 431 and the image-side surface 432 of the third lens 430 are aspheric, and the third lens 430 is made of plastic material.
[0115] The fourth lens 440 with positive refractive power, comprising an object-side surface 441 and an image-side surface 442, the object-side surface 441 of the fourth lens 440 being concave near the optical axis 490 and the image-side surface 442 of the fourth lens 440 being convex near the optical axis 490, the object-side surface 441 and the image-side surface 442 of the fourth lens 440 are aspheric, and the fourth lens 440 is made of plastic material.
[0116] The fifth lens 450 with negative refractive power, comprising an object-side surface 451 and an image-side surface 452, the object-side surface 451 of the fifth lens 450 being convex near the optical axis 490 and the image-side surface 452 of the fifth lens 450 being concave near the optical axis 490, the object-side surface 451 and the image-side surface 452 of the fifth lens 450 are aspheric, and the fifth lens 450 is made of plastic material.
[0117] The sixth lens 460 with negative refractive power, comprising an object-side surface 461 and an image-side surface 462, the object-side surface 461 of the sixth lens 460 being convex near the optical axis 490 and the image-side surface 462 of the sixth lens 460 being concave near the optical axis 490, the object-side surface 461 and the image-side surface 462 of the sixth lens 460 are aspheric and are provided with at least one inflection point, and the sixth lens 460 is made of plastic material.
[0118] The IR band-pass filter 470 made of glass is located between the sixth lens 460 and the image plane 481 and has no influence on the focal length of the optical lens system. The present embodiment selects a filter which is available in the light wavelength range of 940 nm±30 nm, but not limited to this.
[0119] The detailed optical data of the fourth embodiment is shown in table 7, and the aspheric surface data is shown in table 8.
TABLE-US-00009 TABLE 7 Embodiment 4 f(focal length) = 3.52 mm, Fno = 1.30, FOV = 79.3 deg. Curvature Thickness/ Abbe Focal surface Radius gap Material Index(nd) #(vd) length 0 object infinity 450.000 1 Lens 1 2.725 (ASP) 0.358 plastic 1.64 22.5 −23.92 2 2.187 (ASP) 0.062 3 stop infinity 0.135 4 Lens 2 2.213 (ASP) 0.633 plastic 1.64 22.5 12.92 5 2.721 (ASP) 0.198 6 Lens 3 1.958 (ASP) 0.393 plastic 1.64 22.5 4.41 7 6.349 (ASP) 0.738 8 Lens 4 −1.876 (ASP) 0.626 plastic 1.64 22.5 8.51 9 −1.561 (ASP) 0.034 10 Lens 5 3.383 (ASP) 0.422 plastic 1.64 22.5 −118.41 11 3.079 (ASP) 0.211 12 Lens 6 1.482 (ASP) 0.400 plastic 1.64 22.5 −19.21 13 1.182 (ASP) 0.704 14 IR infinity 0.210 glass 1.52 64.2 band-pass filter 15 infinity 0.380 16 Image plane infinity — Note: reference wavelength is 940 nm
TABLE-US-00010 TABLE 8 Aspheric Coefficients surface 1 2 4 5 6 7 K: −9.3789E+00 −1.2964E+01 −5.1907E+00 −1.2197E+01 −1.3045E+01 −1.7897E+01 A: −6.3843E−03 −2.4955E−02 −7.8229E−02 −1.1969E−01 9.0876E−02 5.5952E−02 B: −1.2651E−02 1.4301E−02 1.0994E−01 9.4180E−02 −1.6752E−01 −4.1392E−02 C: 3.3942E−03 −7.4521E−02 −1.0669E−01 −6.8968E−02 1.4764E−01 1.4253E−02 D: −1.5572E−02 4.7863E−02 3.0682E−02 2.1008E−02 −9.7386E−02 −4.0771E−03 E: 1.0961E−02 −9.0276E−03 1.2341E−02 3.1332E−03 3.5249E−02 −4.8015E−04 F: −3.0242E−03 −1.1594E−03 −8.7346E−03 −3.4636E−03 −6.0160E−03 3.3301E−04 G: 2.8186E−04 4.2225E−04 1.3187E−03 5.7617E−04 3.8136E−04 −2.3044E−05 surface 8 9 10 11 12 13 K: −8.5037E+00 −8.4970E−01 −1.4057E+00 −5.6624E−01 −4.3008E+00 −2.6379E+00 A: −1.1624E−01 9.0147E−03 1.8899E−02 1.0020E−02 −1.9545E−02 −6.4733E−02 B: 1.4949E−01 1.5947E−02 −3.4780E−02 −3.4379E−02 −3.6515E−02 9.4625E−03 C: −1.5487E−01 −2.2990E−02 1.6207E−02 1.5804E−02 1.8176E−02 5.8872E−04 D: 1.1797E−01 1.5779E−02 −4.3962E−03 −4.0149E−03 −3.8465E−03 −6.4513E−04 E: −4.9823E−02 −4.2645E−03 3.0966E−04 2.9909E−04 2.2636E−04 1.5576E−04 F: 1.0153E−02 2.4423E−04 8.0163E−05 5.2407E−05 4.1618E−05 −1.8786E−05 G: −7.7943E−04 5.2161E−05 −1.1092E−05 −7.0548E−06 −4.9064E−06 9.1408E−07
[0120] In the fourth embodiment, the equation of the aspheric surface profiles of the aforementioned lenses is the same as the equation of the first embodiment. Also, the definitions of these parameters shown in the following table are the same as those stated in the first embodiment with corresponding values for the fourth embodiment, so an explanation in this regard will not be provided again.
[0121] Moreover, these parameters can be calculated from Table 7 and Table 8 as the following values and satisfy the following conditions:
TABLE-US-00011 Embodiment 4 f[mm] 3.52 CT5*(R9/R10) [mm] 0.46 Fno 1.30 f/(R12*CT3) [mm.sup.−1] 7.56 FOV[deg.] 79.3 CT6/R12 0.34 TL/((TSI-BFL)*f) [mm.sup.−1] 0.41 TL/f 1.57 f1/f −6.80 BFL/TL 0.24 f3/f4 0.52 TL/IMH 1.90 f1/R1 −8.78 f1/f23456 −8.05 R5/R6 0.31 f23/f45 0.41 R7/R8 1.20
[0122] Referring to
[0123] The first lens 510 with negative refractive power, comprising an object-side surface 511 and an image-side surface 512, the object-side surface 511 of the first lens 510 being convex near the optical axis 590 and the image-side surface 512 of the first lens 510 being concave near the optical axis 590, the object-side surface 511 and the image-side surface 512 of the first lens 510 are aspheric, and the first lens 510 is made of plastic material.
[0124] The second lens 520 with positive refractive power, comprising an object-side surface 521 and an image-side surface 522, the object-side surface 521 of the second lens 520 being convex near the optical axis 590 and the image-side surface 522 of the second lens 520 being concave near the optical axis 590, the object-side surface 521 and the image-side surface 522 of the second lens 520 are aspheric, and the second lens 520 is made of plastic material.
[0125] The third lens 530 with positive refractive power, comprising an object-side surface 531 and an image-side surface 532, the object-side surface 531 of the third lens 530 being convex near the optical axis 590 and the image-side surface 532 of the third lens 530 being concave near the optical axis 590, the object-side surface 531 and the image-side surface 532 of the third lens 530 are aspheric, and the third lens 530 is made of plastic material.
[0126] The fourth lens 540 with positive refractive power, comprising an object-side surface 541 and an image-side surface 542, the object-side surface 541 of the fourth lens 540 being concave near the optical axis 590 and the image-side surface 542 of the fourth lens 540 being convex near the optical axis 590, the object-side surface 541 and the image-side surface 542 of the fourth lens 540 are aspheric, and the fourth lens 540 is made of plastic material.
[0127] The fifth lens 550 with positive refractive power, comprising an object-side surface 551 and an image-side surface 552, the object-side surface 551 of the fifth lens 550 being convex near the optical axis 590 and the image-side surface 552 of the fifth lens 550 being concave near the optical axis 590, the object-side surface 551 and the image-side surface 552 of the fifth lens 550 are aspheric, and the fifth lens 550 is made of plastic material.
[0128] The sixth lens 560 with negative refractive power, comprising an object-side surface 561 and an image-side surface 562, the object-side surface 561 of the sixth lens 560 being convex near the optical axis 590 and the image-side surface 562 of the sixth lens 560 being concave near the optical axis 590, the object-side surface 561 and the image-side surface 562 of the sixth lens 560 are aspheric and are provided with at least one inflection point, and the sixth lens 560 is made of plastic material.
[0129] The IR band-pass filter 570 made of glass is located between the sixth lens 560 and the image plane 581 and has no influence on the focal length of the optical lens system. The present embodiment selects a filter which is available in the light wavelength range of 940 nm±30 nm, but not limited to this.
[0130] The detailed optical data of the fifth embodiment is shown in table 9, and the aspheric surface data is shown in table 10.
TABLE-US-00012 TABLE 9 Embodiment 5 f(focal length) = 3.47 mm, Fno = 1.26, FOV = 80.6 deg. Curvature Thickness/ Abbe Focal surface Radius gap Material Index(nd) #(vd) length 0 object infinity 450.000 1 Lens 1 2.576 (ASP) 0.365 plastic 1.64 22.5 −12.98 2 1.846 (ASP) 0.088 3 stop infinity 0.092 4 Lens 2 1.853 (ASP) 0.627 plastic 1.64 22.5 8.54 5 2.479 (ASP) 0.178 6 Lens 3 1.993 (ASP) 0.403 plastic 1.64 22.5 4.34 7 7.043 (ASP) 0.735 8 Lens 4 −1.489 (ASP) 0.563 plastic 1.64 22.5 12.34 9 −1.427 (ASP) 0.035 10 Lens 5 5.969 (ASP) 0.400 plastic 1.64 22.5 92.00 11 6.494 (ASP) 0.035 12 Lens 6 1.255 (ASP) 0.436 plastic 1.64 22.5 −78.01 13 1.061 (ASP) 0.893 14 IR infinity 0.210 glass 1.52 64.2 band-pass filter 15 infinity 0.380 16 Image plane infinity — Note: reference wavelength is 940 nm
TABLE-US-00013 TABLE 10 Aspheric Coefficients surface 1 2 4 5 6 7 K: −1.2853E+01 −1.2702E+01 −6.3015E+00 −7.8369E+00 −1.1902E+01 1.3873E+01 A: 3.4430E−03 −1.7119E−02 −6.6460E−02 −1.3797E−01 8.4696E−02 5.6687E−02 B: −7.6851E−03 1.4905E−02 1.0886E−01 9.6668E−02 −1.6687E−01 −3.8576E−02 C: −1.3794E−03 −7.6319E−02 −1.0891E−01 −6.6071E−02 1.4961E−01 1.2587E−02 D: −1.4173E−02 4.8044E−02 3.0255E−02 2.0708E−02 −9.7351E−02 −4.4561E−03 E: 1.1412E−02 −8.8817E−03 1.2688E−02 2.8549E−03 3.5119E−02 −4.1460E−04 F: −3.3908E−03 −1.1385E−03 −8.5782E−03 −3.4977E−03 −6.0349E−03 3.4131E−04 G: 3.4113E−04 4.0484E−04 1.2583E−03 6.0453E−04 3.9026E−04 −2.3616E−05 surface 8 9 10 11 12 13 K: −6.9257E+00 −1.1747E+00 6.2468E+00 4.5838E+00 −3.7697E+00 −2.8746E+00 A: −1.0895E−01 2.0574E−02 3.4915E−02 1.6049E−02 −2.3047E−02 −5.0395E−02 B: 1.5645E−01 1.0278E−02 −3.3877E−02 −2.5998E−02 −3.2271E−02 4.4379E−03 C: −1.5365E−01 −2.0169E−02 1.4767E−02 1.3981E−02 1.6831E−02 1.2881E−03 D: 1.1685E−01 1.5562E−02 −4.0619E−03 −4.1553E−03 −3.9247E−03 −6.8252E−04 E: −5.0121E−02 −4.5214E−03 3.2132E−04 3.1317E−04 2.5948E−04 1.4756E−04 F: 1.0160E−02 2.2955E−04 3.6218E−05 5.8650E−05 4.6622E−05 −1.6775E−05 G: −7.4944E−04 7.1241E−05 −4.3325E−06 −7.2822E−06 −5.7571E−06 7.9132E−07
[0131] In the fifth embodiment, the equation of the aspheric surface profiles of the aforementioned lenses is the same as the equation of the first embodiment. Also, the definitions of these parameters shown in the following table are the same as those stated in the first embodiment with corresponding values for the fifth embodiment, so an explanation in this regard will not be provided again.
[0132] Moreover, these parameters can be calculated from Table 9 and Table 10 as the following values and satisfy the following conditions:
TABLE-US-00014 Embodiment 5 f[mm] 3.47 CT5*(R9/R10) [mm] 0.37 Fno 1.26 f/(R12*CT3) [mm.sup.−1] 8.11 FOV[deg.] 80.6 CT6/R12 0.41 TL/((TSI-BFL)*f) [mm.sup.−1] 0.45 TL/f 1.57 f1/f −3.74 BFL/TL 0.27 f3/f4 0.35 TL/IMH 1.81 f1/R1 −5.04 f1/f23456 −4.78 R5/R6 0.28 f23/f45 0.30 R7/R8 1.04
[0133] Referring to
[0134] The optical lens system is provided with an image sensor 682. The lens group comprises, in order from an object side to an image side along an optical axis 690: a first lens 610, a second lens 620, a third lens 630, a fourth lens 640, a fifth lens 650, a sixth lens 660, an IR band-pass filter 670, and an image plane 681, wherein the optical lens system has a total of six lenses with refractive power, but not limited to this. The stop 600 is disposed between the first lens 610 and the second lens 620. The image sensor 682 is disposed on the image plane 681.
[0135] The first lens 610 with negative refractive power, comprising an object-side surface 611 and an image-side surface 612, the object-side surface 611 of the first lens 610 being convex near the optical axis 690 and the image-side surface 612 of the first lens 610 being concave near the optical axis 690, the object-side surface 611 and the image-side surface 612 of the first lens 610 are aspheric, and the first lens 610 is made of plastic material.
[0136] The second lens 620 with positive refractive power, comprising an object-side surface 621 and an image-side surface 622, the object-side surface 621 of the second lens 620 being convex near the optical axis 690 and the image-side surface 622 of the second lens 620 being concave near the optical axis 690, the object-side surface 621 and the image-side surface 622 of the second lens 620 are aspheric, and the second lens 620 is made of plastic material.
[0137] The third lens 630 with positive refractive power, comprising an object-side surface 631 and an image-side surface 632, the object-side surface 631 of the third lens 630 being convex near the optical axis 690 and the image-side surface 632 of the third lens 630 being concave near the optical axis 690, the object-side surface 631 and the image-side surface 632 of the third lens 630 are aspheric, and the third lens 630 is made of plastic material.
[0138] The fourth lens 640 with positive refractive power, comprising an object-side surface 641 and an image-side surface 642, the object-side surface 641 of the fourth lens 640 being concave near the optical axis 690 and the image-side surface 642 of the fourth lens 640 being convex near the optical axis 690, the object-side surface 641 and the image-side surface 642 of the fourth lens 640 are aspheric, and the fourth lens 640 is made of plastic material.
[0139] The fifth lens 650 with positive refractive power, comprising an object-side surface 651 and an image-side surface 652, the object-side surface 651 of the fifth lens 650 being convex near the optical axis 690 and the image-side surface 652 of the fifth lens 650 being concave near the optical axis 690, the object-side surface 651 and the image-side surface 652 of the fifth lens 650 are aspheric, and the fifth lens 650 is made of plastic material.
[0140] The sixth lens 660 with negative refractive power, comprising an object-side surface 661 and an image-side surface 662, the object-side surface 661 of the sixth lens 660 being convex near the optical axis 690 and the image-side surface 662 of the sixth lens 660 being concave near the optical axis 690, the object-side surface 661 and the image-side surface 662 of the sixth lens 660 are aspheric and are provided with at least one inflection point, and the sixth lens 660 is made of plastic material.
[0141] The IR band-pass filter 670 made of glass is located between the sixth lens 660 and the image plane 681 and has no influence on the focal length of the optical lens system. The present embodiment selects a filter which is available in the light wavelength range of 940 nm±30 nm, but not limited to this.
[0142] The detailed optical data of the sixth embodiment is shown in table 11, and the aspheric surface data is shown in table 12.
TABLE-US-00015 TABLE 11 Embodiment 6 f(focal length) = 3.90 mm, Fno = 1.50, FOV = 75.0 deg. Curvature Thickness/ Abbe Focal surface Radius gap Material Index(nd) #(vd) length 0 object infinity 600.000 1 Lens 1 2.207 (ASP) 0.614 plastic 1.64 22.5 6.66 2 4.230 (ASP) 0.155 3 stop infinity 0.159 4 Lens 2 −6.606 (ASP) 0.351 plastic 1.64 22.5 38.73 5 −5.288 (ASP) 0.035 6 Lens 3 1.720 (ASP) 0.324 plastic 1.64 22.5 31.84 7 1.748 (ASP) 0.604 8 Lens 4 6.993 (ASP) 0.362 plastic 1.64 22.5 −99.48 9 6.157 (ASP) 0.327 10 Lens 5 23.808 (ASP) 0.872 plastic 1.64 22.5 2.40 11 −1.566 (ASP) 0.035 12 Lens 6 111.155 (ASP) 0.542 plastic 1.64 22.5 −2.17 13 1.329 (ASP) 0.347 14 IR infinity 0.300 glass 1.52 64.2 band-pass filter 15 infinity 0.380 16 Image plane infinity — Note: reference wavelength is 940 nm
TABLE-US-00016 TABLE 12 Aspheric Coefficients surface 1 2 4 5 6 7 K: −3.8429E−01 2.2752E+00 −1.8535E−01 4.1528E−02 −2.1421E+00 −2.9705E+00 A: −6.2214E−03 −3.3244E−02 4.0717E−04 −6.6057E−04 −4.3097E−03 4.0339E−02 B: 2.0090E−03 −3.0805E−04 −1.7436E−03 −1.9312E−03 1.9003E−02 −3.0123E−02 C: −6.1471E−03 1.0485E−02 −3.5138E−05 −6.3536E−05 −8.2320E−02 8.1254E−03 D: 6.9738E−03 −1.7496E−02 −2.2480E−05 8.4748E−06 9.0992E−02 −2.3715E−02 E: −5.0363E−03 1.1737E−02 −2.8819E−06 −4.2666E−06 −5.7319E−02 2.4475E−02 F: 1.6561E−03 −4.1469E−03 0.0000E+00 0.0000E+00 1.8692E−02 −1.0755E−02 G: −2.4469E−04 5.8913E−04 0.0000E+00 0.0000E+00 −2.3200E−03 1.7800E−03 surface 8 9 10 11 12 13 K: −9.4235E+01 −5.4166E+01 1.9108E+01 −3.4339E+00 7.3374E+01 −8.1311E+00 A: −2.3854E−02 −4.7991E−02 3.2432E−02 1.3925E−01 −1.0791E−01 −6.9147E−02 B: −4.4770E−02 3.6800E−03 −4.9142E−02 −1.7467E−01 6.5438E−03 2.4311E−02 C: 7.2849E−02 −2.1881E−02 5.4009E−02 1.3846E−01 1.4311E−02 −7.2136E−03 D: −6.0627E−02 2.0060E−02 −5.9171E−02 −6.3408E−02 −4.8286E−03 1.1766E−03 E: 2.3609E−02 −1.0617E−02 3.7053E−02 1.5518E−02 6.8825E−04 −9.1354E−05 F: −3.5793E−03 2.3920E−03 −1.3303E−02 −1.8719E−03 −4.7120E−05 2.8514E−06 G: 0.0000E+00 0.0000E+00 1.9344E−03 8.6051E−05 1.2565E−06 −2.1559E−08
[0143] In the sixth embodiment, the equation of the aspheric surface profiles of the aforementioned lenses is the same as the equation of the first embodiment. Also, the definitions of these parameters shown in the following table are the same as those stated in the first embodiment with corresponding values for the sixth embodiment, so an explanation in this regard will not be provided again.
[0144] Moreover, these parameters can be calculated from Table 11 and Table 12 as the following values and satisfy the following conditions:
TABLE-US-00017 Embodiment 6 f[mm] 3.90 CT5*(R9/R10) [mm] −13.25 Fno 1.50 f/(R12*CT3) [mm.sup.−1] 9.08 FOV[deg.] 75.0 CT6/R12 0.41 TL/((TSI-BFL)*f) [mm.sup.−1] 0.38 TL/f 1.38 f1/f 1.71 BFL/TL 0.19 f3/f4 −0.32 TL/IMH 1.75 f1/R1 3.02 f1/f23456 0.60 R5/R6 0.98 f23/f45 6.74 R7/R8 1.14
[0145] Referring to
[0146] In the present optical lens system, the lenses can be made of plastic or glass. If the lenses are made of plastic, the cost will be effectively reduced. If the lenses are made of glass, there is more freedom in distributing the refractive power of the optical lens system. Plastic lenses can have aspheric surfaces, which allow more design parameter freedom (than spherical surfaces), so as to reduce the aberration and the number of the lenses, as well as the total length of the optical lens system.
[0147] In the present optical lens system, if the object-side or the image-side surface of the lenses with refractive power is convex and the location of the convex surface is not defined, the object-side or the image-side surface of the lenses near the optical axis is convex. If the object-side or the image-side surface of the lenses is concave and the location of the concave surface is not defined, the object-side or the image-side surface of the lenses near the optical axis is concave.
[0148] The optical lens system of the present invention can be used in focusing optical systems and can obtain better image quality. The optical lens system of the present invention can also be used in electronic imaging systems, such as, 3D image capturing, digital camera, mobile device, digital flat panel or vehicle camera.
[0149] While we have shown and described various embodiments in accordance with the present invention, it should be clear to those skilled in the art that further embodiments may be made without departing from the scope of the present invention.