Patent application title:

Camera optical lens

Publication number:

US20190121074A1

Publication date:
Application number:

15/840,020

Filed date:

2017-12-13

βœ… Patent granted

Patent number:

US 10,268,022 B1

Grant date:

2019-04-23

PCT filing:

-

PCT publication:

-

Examiner:

Evan P Dzierzynski | Mitchell T Oestreich

Agent:

Na Xu | IPro, PLLC

Adjusted expiration:

2037-12-13

Abstract:

The present disclosure discloses a camera optical lens. The camera optical lens including, in an order from an object side to an image side, a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens and a seventh lens. The camera optical lens further satisfies specific conditions.

Inventors:

Assignee:

Applicant:

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Classification:

G02B13/0045 »  CPC main

Optical objectives specially designed for the purposes specified below; Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface having five or more lenses

G02B13/00 IPC

Optical objectives specially designed for the purposes specified below

G02B9/64 »  CPC further

Optical objectives characterised both by the number of the components and their arrangements according to their sign, i.e. + or - having more than six components

Description

FIELD OF THE PRESENT DISCLOSURE

The present disclosure relates to optical lens, in particular to a camera optical lens suitable for handheld devices such as smart phones and digital cameras and imaging devices.

DESCRIPTION OF RELATED ART

With the emergence of smart phones in recent years, the demand for miniature camera lens is increasing day by day, but the photosensitive devices of general camera lens are no other than Charge Coupled Device (CCD) or Complementary metal-Oxide Semiconductor Sensor (CMOS sensor), and as the progress of the semiconductor manufacturing technology makes the pixel size of the photosensitive devices shrink, coupled with the current development trend of electronic products being that their functions should be better and their shape should be thin and small, miniature camera lens with good imaging quality therefor has become a mainstream in the market. In order to obtain better imaging quality, the lens that is traditionally equipped in mobile phone cameras adopts a three-piece or four-piece lens structure. And, with the development of technology and the increase of the diverse demands of users, and under this circumstances that the pixel area of photosensitive devices is shrinking steadily and the requirement of the system for the imaging quality is improving constantly, the five-piece, six-piece and seven-piece lens structure gradually appear in lens design. There is an urgent need for ultra-thin wide-angle camera lenses which have good optical characteristics and the chromatic aberration of which is fully corrected.

BRIEF DESCRIPTION OF THE DRAWINGS

Many aspects of the exemplary embodiments can be better understood with reference to the following drawings. The components in the drawing are not necessarily drawn to scale, the emphasis instead being placed upon clearly illustrating the principles of the present disclosure.

FIG. 1 is a schematic diagram of a camera optical lens in accordance with a first embodiment of the present invention;

FIG. 2 shows the longitudinal aberration of the camera optical lens shown in FIG. 1;

FIG. 3 shows the lateral color of the camera optical lens shown in FIG. 1;

FIG. 4 presents a schematic diagram of the field curvature and distortion of the camera optical lens shown in FIG. 1;

FIG. 5 is a schematic diagram of a camera optical lens in accordance with a second embodiment of the present invention;

FIG. 6 presents the longitudinal aberration of the camera optical lens shown in FIG. 5;

FIG. 7 presents the lateral color of the camera optical lens shown in FIG. 5;

FIG. 8 presents the field curvature and distortion of the camera optical lens shown in FIG. 5;

FIG. 9 is a schematic diagram of the camera optical lens in the third embodiment of the present invention;

FIG. 10 is a schematic diagram of the longitudinal aberration of the camera optical lens shown in FIG. 9;

FIG. 11 is a schematic diagram of the lateral color of the camera optical lens shown in FIG. 9;

FIG. 12 is a schematic diagram of the field curvature and distortion of the camera optical lens shown in FIG. 9

DETAILED DESCRIPTION OF THE EXEMPLARY EMBODIMENTS

The present disclosure will hereinafter be described in detail with reference to several exemplary embodiments. To make the technical problems to be solved, technical solutions and beneficial effects of the present disclosure more apparent, the present disclosure is described in further detail together with the figure and the embodiments. It should be understood the specific embodiments described hereby is only to explain the disclosure, not intended to limit the disclosure.

Embodiment 1

As referring to FIG. 1, the present invention provides a camera optical lens 10. FIG. 1 shows the camera optical lens 10 of embodiment 1 of the present invention, the camera optical lens 10 comprises 7 lenses. Specifically, from the object side to the image side, the camera optical lens 10 comprises in sequence: an aperture S1, a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6 and a seventh lens L7. Optical element like optical filter GF can be arranged between the seventh lens L7 and the image surface Si. The first lens L1 is made of plastic material, the second lens L2 is made of plastic material, the third lens L3 is made of plastic material, the fourth lens L4 is made of glass material, the fifth lens L5 is made of plastic material, the sixth lens L6 is made of plastic material, the seventh lens L7 is made of plastic material;

Here, the focal length of the whole camera optical lens 10 is defined as f, the focal length of the first lens L1 is defined as f1, the curvature radius of the object side surface of the first lens L1 is defined as R1, the curvature radius of the image side surface of the first lens L1 is defined as R2, the refractive power of the fourth lens L4 is defined as n4, the thickness on axis of the fourth lens L4 is defined as d7, the focal length of the sixth lens is L6 defined as f6, the focal length of the seventh lens L7 is defined as f7, the total optical length of the camera optical lens 10 is defined as TLL. The camera optical lens 10 satisfies the following conditions: βˆ’3≀f1/fβ‰€βˆ’1, 1.7≀n4≀2.2, 1≀f6/f7≀10; 1.2≀(R1+R2)/(R1βˆ’R2)≀10; 0.01≀d7/TTL≀0.2.

Condition βˆ’3≀f1/f≀2.2 fixes the negative refractive power of the first lens L1. If the upper limit of the set value is exceeded, although it benefits the ultra-thin development of lenses, but the negative refractive power of the first lens L1 will be too strong, problem like aberration is difficult to be corrected, and it is also unfavorable for wide-angle development of lens. On the contrary, if the lower limit of the set value is exceeded, the negative refractive power of the first lens L1 becomes too weak, it is then difficult to develop ultra-thin lenses. Preferably, the following condition shall be satisfied, βˆ’3≀f1/fβ‰€βˆ’1.5.

Condition 1.7≀n4≀2.2 fixes the refractive power of the fourth lens L4, refractive power within this range benefits the ultra-thin development of lenses, and it also benefits the correction of aberration. Preferably, the following condition shall be satisfied, 1.7≀n4≀2.0.

Condition 1≀f6/f7≀10 fixes the ratio between the focal length f6 of the sixth lens L6 and the focal length f7 of the seventh lens L7, a ratio within this range can effectively reduce the sensitivity of lens group used in camera and further enhance the imaging quality. Preferably, the following condition shall be satisfied, 2≀f6/f7≀10.

Condition 1.2≀(R1+R2)/(R1βˆ’R2)≀10 fixes the shape of the first lens L1, when the value is beyond this range, with the development into the direction of ultra-thin and wide-angle lenses, problem like aberration of the off-axis picture angle is difficult to be corrected. Preferably, the condition 1.2≀(R1+R2)/(R1βˆ’R2)≀8 shall be satisfied.

Condition 0.01≀d7/TTL≀0.2 fixes the ratio between the thickness on-axis of the fourth lens L4 and the total optical length TTL of the camera optical lens 10, a ratio within this range benefits ultra-thin development of lenses. Preferably, the following condition shall be satisfied, 0.01≀d7/TTL≀0.15.

When the focal length of the camera optical lens 10 of the present invention, the focal length of each lens, the refractive power of the related lens, and the total optical length, the thickness on-axis and the curvature radius of the camera optical lens satisfy the above conditions, the camera optical lens 10 has the advantage of high performance and satisfies the design requirement of low TTL.

In this embodiment, the object side surface of the first lens L1 is a convex surface relative to the proximal axis, its image side surface is a concave surface relative to the proximal axis, and it has negative refractive power; the thickness on axis of the first lens L1 is d1, they satisfy the following condition: 0.09≀d1≀0.27, it is beneficial for ultra-thin development. Preferably, the condition 0.14≀d1≀0.22 shall be satisfied.

In this embodiment, the object side surface of the second lens L2 is a convex surface relative to the proximal axis, its image side surface is a convex surface relative to the proximal axis, and it has positive refractive power; the focal length of the whole camera optical lens 10 is f, the focal length of the second lens L2 is f2, the curvature radius of the object side surface of the second lens L2 is R3, the curvature radius of image side surface of the second lens L2 is R4 and the thickness on-axis of the second lens L2 is d3, they satisfy the following condition: 0.51≀f2/f≀2.35, when the condition is met, the positive refractive power of the second lens L2 is controlled within reasonable scope, the spherical aberration caused by the first lens L1 which has negative refractive power and the field curvature of the system then can be reasonably and effectively balanced; the condition βˆ’2.18≀(R3+R4)/(R3βˆ’R4)β‰€βˆ’0.40 fixes the shape of the second lens L2, when value is beyond this range, with the development into the direction of ultra-thin and wide-angle lenses, problem like on-axis chromatic aberration is difficult to be corrected; if the condition 0.27≀d3≀0.95 is met, it is beneficial for the realization of ultra-thin lenses. Preferably, the following conditions shall be satisfied, 0.81≀f2/f≀1.88; βˆ’1.36≀(R3+R4)/(R3βˆ’R4)β‰€βˆ’0.50; 0.43≀d3≀0.76.

In this embodiment, the image side surface of the third lens L3 is a concave surface relative to the proximal axis, and it has refractive power; the focal length of the whole camera optical lens 10 is f, the focal length of the third lens L3 is f3, the curvature radius of the object side surface of the third lens L3 is R5, the curvature radius of the image side surface of the third lens L3 is R6 and the thickness on-axis of the third lens L3 is d5, they satisfy the condition: βˆ’12.37≀f3/f≀30.72, by meeting this condition, it is helpful for the system to obtain good ability in balancing the field curvature, so that the image quality can be effectively improved; by meeting the condition βˆ’126.42≀(R5+R6)/(R5βˆ’R6)≀1.48 the shape of the third lens L3 can be effectively controlled, it is beneficial for the shaping of the third lens L3 and bad shaping and stress generation due to extra large curvature of surface of the third lens L3 can be avoided; when the condition 0.15≀d5≀0.46 is met, it is beneficial for the realization of ultra-thin lenses. Preferably, the following conditions shall be satisfied, βˆ’7.73≀f3/f≀24.51; βˆ’79.01≀(R5+R6)/(R5βˆ’R6) 1.18; 0.24≀d5≀0.37.

In this embodiment, the object side surface of the fourth lens L4 is a convex surface relative to the proximal axis, its image side surface is a concave surface relative to the proximal axis, and it has refractive power; the focal length of the whole camera optical lens 10 is f, the focal length of the fourth lens L4 is f4, the curvature radius of the object side surface of the fourth lens L4 is R7, the curvature radius of the image side surface of the fourth lens L4 is R8 and the thickness on-axis of the fourth lens L4 is d7, they satisfy the condition: βˆ’10.68≀f4/f≀35.71, the appropriate distribution of refractive power makes it possible that the system has better imaging quality and lower sensitivity; the condition βˆ’276.57≀(R7+R8)/(R7βˆ’R8)≀8.2 fixes the shape of the fourth lens L4, when beyond this range, with the development into the direction of ultra-thin and wide-angle lens, the problem like chromatic aberration is difficult to be corrected; when the condition 0.14≀d7≀0.77 is met, it is beneficial for realization of ultra-thin lenses. Preferably, the following conditions shall be satisfied, βˆ’6.68≀f4/f≀28.57; βˆ’172.86≀(R7+R8)/(R7βˆ’R8)≀6.56; 0.23≀d7≀0.62.

In this embodiment, the object side surface of the fifth lens L5 is a concave surface relative to the proximal axis, its image side surface is a convex surface relative to the proximal axis, and it has positive refractive power; the focal length of the whole camera optical lens 10 is f, the focal length of the fifth lens L5 is f5, the curvature radius of the object side surface of the fifth lens L5 is R9, the curvature radius of the image side surface of the fifth lens L5 is R10 and the thickness on-axis of the fifth lens L5 is d9, they satisfy the condition: 0.25≀f5/f≀0.87, the limitation on the fifth lens L5 can effectively make the light angle of the camera lens flat and the tolerance sensitivity reduces; the condition 0.55≀(R9+R10)/(R9βˆ’R10)≀2.08 fixes the shape of the fifth lens L5, when beyond this range, with the development into the direction of ultra-thin and wide-angle lens, the problem like off-axis chromatic aberration is difficult to be corrected; when the condition 0.52≀d9≀1.57 is met, it is beneficial for the realization of ultra-thin lens. Preferably, the following conditions shall be satisfied, 0.40≀f5/f≀0.69; 0.88≀(R9+R10)/(R9βˆ’R10)≀1.66; 0.84≀d9≀1.26.

In this embodiment, the object side surface of the sixth lens L6 is a convex surface relative to the proximal axis, its image side surface is a concave surface relative to the proximal axis, and it has negative refractive power; the focal length of the whole camera optical lens 10 is f, the focal length of the sixth lens L6 is f6, the curvature radius of the object side surface of the sixth lens L6 is R11, the curvature radius of the image side surface of the sixth lens L6 is R12 and the thickness on-axis of the sixth lens L6 is d11, they satisfy the condition: βˆ’13.76≀f6/fβ‰€βˆ’2.37, the appropriate distribution of refractive power makes it possible that the system has better imaging quality and lower sensitivity; the condition 1.38≀(R11+R12)/(R11βˆ’R12)≀7.31 fixes the shape of the sixth lens L6, when beyond this range, with the development into the direction of ultra-thin and wide-angle lenses, the problem like off-axis chromatic aberration is difficult to be corrected; when the condition 0.11≀d11≀0.77, is met, it is beneficial for the realization of ultra-thin lens. Preferably, the following conditions shall be satisfied, βˆ’8.60≀f6/fβ‰€βˆ’2.97; 2.20≀(R11+R12)/(R11βˆ’R12)≀5.85; 0.16≀d11≀0.62.

In this embodiment, the object side surface of the seventh lens L7 is a convex surface relative to the proximal axis, its image side surface is a concave surface relative to the proximal axis, and it has negative refractive power; the focal length of the whole camera optical lens 10 is f, the curvature radius of the object side surface of the seventh lens L7 is R13, the curvature radius of the image side surface of the seventh lens L7 is R14, the focal length of the seventh lens L7 is f7, and the thickness on-axis of the seventh lens L7 is d13, they satisfy the condition: 0.79≀(R13+R14)/(R13βˆ’R14)≀2.72, which fixes the shape of the seventh lens L7, when beyond this range, with the development into the direction of ultra-thin and wide-angle lenses, the problem like off-axis chromatic aberration is difficult to be corrected; βˆ’1.78≀f7/fβ‰€βˆ’0.46, the appropriate distribution of refractive power makes it possible that the system has better imaging quality and lower sensitivity; when the condition 0.19≀d11≀0.85 is met, it is beneficial for the realization of ultra-thin lens. Preferably, the following conditions shall be satisfied, βˆ’1.11≀f7/fβ‰€βˆ’0.57; 0.30≀d13≀0.68; 1.26≀(R13+R14)/(R13βˆ’R14)≀2.17.

In this embodiment, the total optical length TTL of the camera optical lens 10 is less than or equal to 6.32 mm, it is beneficial for the realization of ultra-thin lenses. Preferably, the total optical length TTL of the camera optical lens 10 is less than or equal to 6.03.

In this embodiment, the aperture F number of the camera optical lens 10 is less than or equal to 2.14. A large aperture has better imaging performance. Preferably, the aperture F number of the camera optical lens 10 is less than or equal to 2.09.

With such design, the total optical length TTL of the whole camera optical lens 10 can be made as short as possible, thus the miniaturization characteristics can be maintained.

In the following, an example will be used to describe the camera optical lens 10 of the present invention. The symbols recorded in each example are as follows. The unit of distance, radius and center thickness is mm.

TTL: Optical length (the distance on-axis from the object side surface to the image surface of the first lens L1).

Preferably, inflexion points and/or arrest points can also be arranged on the object side surface and/or image side surface of the lens, so that the demand for high quality imaging can be satisfied, the description below can be referred for specific implementable scheme.

The design information of the camera optical lens 10 in the first embodiment of the present invention is shown in the following, the unit of the focal length, distance, radius and center thickness is mm.

The design information of the camera optical lens 10 in the first embodiment of the present invention is shown in the tables 1 and 2.

TABLE 1
R d nd Ξ½ d
S1 ∞ d0= βˆ’0.076
R1 1.517 d1= 0.180 nd1 1.6713 Ξ½ 1 19.24
R2 1.158 d2= 0.350
R3 4.055 d3= 0.636 nd2 1.5445 Ξ½ 2 55.99
R4 βˆ’25.640 d4= 0.030
R5 βˆ’2710.177 d5= 0.304 nd3 1.6713 Ξ½ 3 19.24
R6 17.380 d6= 0.219
R7 4.454 d7= 0.516 nd4 1.7225 Ξ½ 4 29.23
R8 4.519 d8= 0.351
R9 βˆ’21.305 d9= 1.049 nd5 1.5352 Ξ½ 5 56.12
R10 βˆ’1.062 d10= 0.020
R11 7.382 d11= 0.444 nd6 1.5352 Ξ½ 6 56.12
R12 4.867 d12= 0.100
R13 4.031 d13= 0.393 nd7 1.5352 Ξ½ 7 56.12
R14 1.068 d14= 1.154
R15 ∞ d15= 0.210 ndg 1.5168 ν g 64.17
R16 ∞ d16= 1.094

In which, the meaning of the various symbols is as follows.

S1: Aperture;

R: The curvature radius of the optical surface, the central curvature radius in case of lens;

R1: The curvature radius of the object side surface of the first lens L1;

R2: The curvature radius of the image side surface of the first lens L1;

R3: The curvature radius of the object side surface of the second lens L2;

R4: The curvature radius of the image side surface of the second lens L2;

R5: The curvature radius of the object side surface of the third lens L3;

R6: The curvature radius of the image side surface of the third lens L3;

R7: The curvature radius of the object side surface of the fourth lens L4;

R8: The curvature radius of the image side surface of the fourth lens L4;

R9: The curvature radius of the object side surface of the fifth lens L5;

R10: The curvature radius of the image side surface of the fifth lens L5;

R11: The curvature radius of the object side surface of the sixth lens L6;

R12: The curvature radius of the image side surface of the sixth lens L6;

R13: The curvature radius of the object side surface of the seventh lens L7;

R14: The curvature radius of the image side surface of the seventh lens L7;

R15: The curvature radius of the object side surface of the optical filter GF;

R16: The curvature radius of the image side surface of the optical filter GF;

d: The thickness on-axis of the lens and the distance on-axis between the lens;

d0: The distance on-axis from aperture S1 to the object side surface of the first lens L1;

d1: The thickness on-axis of the first lens 11;

d2: The distance on-axis from the image side surface of the first lens L1 to the object side surface of the second lens L2;

d3: The thickness on-axis of the second lens L2;

d4: The distance on-axis from the image side surface of the second lens L2 to the object side surface of the third lens L3;

d5: The thickness on-axis of the third lens L3;

d6: The distance on-axis from the image side surface of the third lens L3 to the object side surface of the fourth lens L4;

d7: The thickness on-axis of the fourth lens L4;

d8: The distance on-axis from the image side surface of the fourth lens L4 to the object side surface of the fifth lens L5;

d9: The thickness on-axis of the fifth lens L5;

d10: The distance on-axis from the image side surface of the fifth lens L5 to the object side surface of the sixth lens L6;

d11: The thickness on-axis of the sixth lens L6;

d12: The distance on-axis from the image side surface of the sixth lens L6 to the object side surface of the seventh lens L7;

d13: The thickness on-axis of the seventh lens L7;

d14: The distance on-axis from the image side surface of the seventh lens L7 to the object side surface of the optical filter GF;

d15: The thickness on-axis of the optical filter GF;

d16: The distance on-axis from the image side surface to the image surface of the optical filter GF;

nd: The refractive power of the d line;

nd1: The refractive power of the d line of the first lens L1;

nd2: The refractive power of the d line of the second lens L2;

nd3: The refractive power of the d line of the third lens L3;

nd4: The refractive power of the d line of the fourth lens L4;

nd5: The refractive power of the d line of the fifth lens L5;

nd6: The refractive power of the d line of the sixth lens L6;

nd7: The refractive power of the d line of the seventh lens L7;

ndg: The refractive power of the d line of the optical filter GF;

vd: The abbe number;

v1: The abbe number of the first lens L1;

v2: The abbe number of the second lens L2;

v3: The abbe number of the third lens L3;

v4: The abbe number of the fourth lens L4;

v5: The abbe number of the fifth lens L5;

v6: The abbe number of the sixth lens L6;

v7: The abbe number of the seventh lens L7;

vg: The abbe number of the optical filter GF;

Table 2 shows the aspherical surface data of the camera optical lens 10 in the embodiment 1 of the present invention.

TABLE 2
Conic Index Aspherical Surface Index
k A4 A6 A8 A10 A12 A14 A16
R1 βˆ’3.0115E+00 βˆ’3.6662Eβˆ’02 βˆ’1.2144Eβˆ’02  1.8859Eβˆ’02  7.9201Eβˆ’03 βˆ’1.0995Eβˆ’02  6.0507Eβˆ’03
R2 βˆ’2.4525E+00 βˆ’2.1603Eβˆ’02 βˆ’1.7132Eβˆ’03  2.3790Eβˆ’03  3.9128Eβˆ’03 βˆ’4.0477Eβˆ’03  6.9205Eβˆ’03
R3 βˆ’2.3123E+01 βˆ’3.0310Eβˆ’02 βˆ’2.9729Eβˆ’02 βˆ’3.5745Eβˆ’02 βˆ’7.4248Eβˆ’03 9.4980Eβˆ’03 βˆ’2.1026Eβˆ’02 
R4  3.7931E+02 βˆ’1.0309Eβˆ’01 βˆ’3.3532Eβˆ’02 βˆ’8.7527Eβˆ’03  2.6046Eβˆ’03 2.9984Eβˆ’03 βˆ’3.2301Eβˆ’03  βˆ’1.5950Eβˆ’04
R5  0.0000E+00 βˆ’1.8712Eβˆ’03 βˆ’2.8701Eβˆ’03 βˆ’4.2720Eβˆ’03 βˆ’5.6109Eβˆ’03 3.2986Eβˆ’03 1.9965Eβˆ’03 βˆ’2.4381Eβˆ’03
R6  0.0000E+00 βˆ’1.6512Eβˆ’02  1.0057Eβˆ’02  4.1843Eβˆ’03 βˆ’8.2499Eβˆ’04 βˆ’4.0696Eβˆ’03  1.6427Eβˆ’04 βˆ’2.0726Eβˆ’04
R7 βˆ’2.7655E+00 βˆ’1.0962Eβˆ’01 βˆ’1.3875Eβˆ’02 βˆ’3.5138Eβˆ’03  7.1845Eβˆ’03 3.8842Eβˆ’03 βˆ’1.3310Eβˆ’04  βˆ’1.6879Eβˆ’03
R8  5.3482E+00 βˆ’6.2397Eβˆ’02 βˆ’8.8464Eβˆ’03 βˆ’2.9626Eβˆ’04 βˆ’4.7198Eβˆ’04 βˆ’9.1074Eβˆ’05 
R9  6.3733E+01 βˆ’3.0525Eβˆ’03  1.6544Eβˆ’02 βˆ’7.7245Eβˆ’03 βˆ’2.3096Eβˆ’04 3.7475Eβˆ’04
R10 βˆ’3.0812E+00 βˆ’6.2927Eβˆ’02  1.7469Eβˆ’02 βˆ’2.1724Eβˆ’03  8.0568Eβˆ’04
R11  7.8478E+00 βˆ’1.6933Eβˆ’02  2.1172Eβˆ’03  3.1284Eβˆ’04 βˆ’8.9858Eβˆ’05
R12 βˆ’5.1357Eβˆ’01 βˆ’1.2144Eβˆ’03 βˆ’1.0034Eβˆ’04 βˆ’1.2978Eβˆ’04  1.0245Eβˆ’05
R13 βˆ’2.6744E+00 βˆ’2.3557Eβˆ’03 βˆ’4.8836Eβˆ’04  1.6054Eβˆ’06 βˆ’2.6250Eβˆ’05
R14 βˆ’4.4070E+00 βˆ’5.7214Eβˆ’03  2.1492Eβˆ’03 βˆ’2.5986Eβˆ’04  3.6474Eβˆ’09

Among them, K is a conic index, A4, A6, A8, A10, A12, A14, A16 are aspheric surface indexes.

IH: Image height


y=(x2/R)/[1+{1βˆ’(k+1)(x2/R2)}1/2]+A4x4+A6x6+A8x8+A10x12+A12x12+A14x14+A16x16  (1)

For convenience, the aspheric surface of each lens surface uses the aspheric surfaces shown in the above condition (1). However, the present invention is not limited to the aspherical polynomials form shown in the condition (1).

Table 3 and table 4 show the inflexion points and the arrest point design data of the camera optical lens 10 lens in embodiment 1 of the present invention. In which, R1 and R2 represent respectively the object side surface and image side surface of the first lens L1, R3 and R4 represent respectively the object side surface and image side surface of the second lens L2, R5 and R6 represent respectively the object side surface and image side surface of the third lens L3, R7 and R8 represent respectively the object side surface and image side surface of the fourth lens L4, R9 and R10 represent respectively the object side surface and image side surface of the fifth lens L5, R11 and R12 represent respectively the object side surface and image side surface of the sixth lens L6, R13 and R14 represent respectively the object side surface and image side surface of the seventh lens L7. The data in the column named β€œinflexion point position” are the vertical distances from the inflexion points arranged on each lens surface to the optic axis of the camera optical lens 10. The data in the column named β€œarrest point position” are the vertical distances from the arrest points arranged on each lens surface to the optic axis of the camera optical lens 10.

TABLE 3
Inflexion point number Inflexion point position 1
R1 0
R2 0
R3 1 0.495
R4 0
R5 0
R6 1 0.905
R7 1 0.405
R8 1 0.565
R9 1 1.275
R10 0
R11 1 1.815
R12 1 1.485
R13 1 1.775
R14 0

TABLE 4
Arrest point number Arrest point position 1
R1
R2
R3 1 0.755
R4
R5
R6 1 1.065
R7 1 0.685
R8 1 0.925
R9
R10
R11
R12
R13
R14

FIG. 2 and FIG. 3 show the longitudinal aberration and lateral color schematic diagrams after light with a wavelength of 470 nm, 555 nm and 650 nm passes the camera optical lens 10 in the first embodiment. FIG. 4 shows the field curvature and distortion schematic diagrams after light with a wavelength of 555 nm passes the camera optical lens 10 in the first embodiment, the field curvature S in FIG. 4 is a field curvature in the sagittal direction, T is a field curvature in the meridian direction.

Table 13 shows the various values of the examples 1, 2, 3 and the values corresponding with the parameters which are already specified in the conditions.

As shown in Table 13, the first embodiment satisfies the various conditions.

In this embodiment, the pupil entering diameter of the camera optical lens is 1.988 m, the full vision field image height is 2.9935 mm, the vision field angle in the diagonal direction is 74.99Β°, it has wide-angle and is ultra-thin, its on-axis and off-axis chromatic aberrations are fully corrected, and it has excellent optical characteristics.

Embodiment 2

Embodiment 2 is basically the same as embodiment 1, the meaning of its symbols is the same as that of embodiment 1, in the following, only the differences are described.

Table 5 and table 6 show the design data of the camera optical lens 20 in embodiment 2 of the present invention.

TABLE 5
R d nd Ξ½d
S1 ∞ d0= βˆ’0.076
R1 3.814 d1= 0.180 nd1 1.6713 Ξ½1 19.24
R2 2.548 d2= 0.102
R3 3.231 d3= 0.575 nd2 1.5445 Ξ½2 55.99
R4 βˆ’13.125 d4= 0.030
R5 3.547 d5= 0.304 nd3 1.6713 Ξ½3 19.24
R6 3.661 d6= 0.492
R7 10.141 d7= 0.480 nd4 1.8211 Ξ½4 24.06
R8 4.782 d8= 0.351
R9 βˆ’9.873 d9= 1.049 nd5 1.5352 Ξ½5 56.12
R10 βˆ’1.039 d10= 0.020
R11 7.670 d11= 0.516 nd6 1.5352 Ξ½6 56.12
R12 4.852 d12= 0.100
R13 4.967 d13= 0.374 nd7 1.5352 Ξ½7 56.12
R14 1.113 d14= 1.154
R15 ∞ d15= 0.210 ndg 1.5168 νg 64.17
R16 ∞ d16= 0.366

Table 6 shows the aspherical surface data of each lens of the camera optical lens 20 in embodiment 2 of the present invention.

TABLE 6
Conic Index Aspherical Surface Index
k A4 A6 A8 A10 A12 A14 A16
R1 βˆ’1.3838Eβˆ’01 βˆ’2.4334Eβˆ’02 βˆ’1.0112Eβˆ’02  6.5882Eβˆ’03  5.1170Eβˆ’03 βˆ’7.1469Eβˆ’03  3.1132Eβˆ’03
R2 βˆ’1.4308E+00 βˆ’1.1193Eβˆ’02 βˆ’2.6884Eβˆ’03  3.2625Eβˆ’03  1.1245Eβˆ’03 βˆ’2.7368Eβˆ’03  6.5571Eβˆ’03
R3 βˆ’4.5519E+00 βˆ’1.2242Eβˆ’02 βˆ’1.6413Eβˆ’02 βˆ’1.9836Eβˆ’02 βˆ’4.9202Eβˆ’03 6.3946Eβˆ’03 βˆ’6.7241Eβˆ’03 
R4  1.3436E+02 βˆ’6.1214Eβˆ’02 βˆ’1.8112Eβˆ’02 βˆ’5.6247Eβˆ’03 βˆ’1.2121Eβˆ’03 8.8777Eβˆ’04 βˆ’2.5403Eβˆ’03  βˆ’6.9736Eβˆ’05
R5  0.0000E+00 βˆ’6.7295Eβˆ’04  7.7707Eβˆ’03  3.2124Eβˆ’03 βˆ’4.8276Eβˆ’03 1.7701Eβˆ’05 1.7295Eβˆ’04 βˆ’3.6178Eβˆ’04
R6  0.0000E+00 βˆ’2.5531Eβˆ’04  1.3829Eβˆ’02  3.8320Eβˆ’03 βˆ’1.9903Eβˆ’03 βˆ’3.9229Eβˆ’03  3.0958Eβˆ’04 βˆ’7.4762Eβˆ’04
R7  1.8510E+01 βˆ’1.0623Eβˆ’01 βˆ’9.8341Eβˆ’03 βˆ’1.0104Eβˆ’02  5.7514Eβˆ’03 5.7401Eβˆ’03 8.0081Eβˆ’04 βˆ’2.4575Eβˆ’03
R8  8.3725E+00 βˆ’7.1548Eβˆ’02 βˆ’6.3801Eβˆ’03  2.3486Eβˆ’04 βˆ’6.5661Eβˆ’04 βˆ’1.0261Eβˆ’04 
R9 βˆ’9.7497E+00  2.5138Eβˆ’03  1.5547Eβˆ’02 βˆ’8.0683Eβˆ’03 βˆ’2.7868Eβˆ’04 4.1459Eβˆ’04
R10 βˆ’2.9260E+00 βˆ’6.8875Eβˆ’02  1.9016Eβˆ’02 βˆ’1.6612Eβˆ’03  6.1005Eβˆ’04
R11  8.4763E+00 βˆ’2.2947Eβˆ’02  1.4749Eβˆ’03  7.4614Eβˆ’05 βˆ’1.5525Eβˆ’05
R12 βˆ’7.4109Eβˆ’01 βˆ’1.4252Eβˆ’03 βˆ’4.5696Eβˆ’05 βˆ’1.0021Eβˆ’05 βˆ’1.4600Eβˆ’06
R13 βˆ’6.5181Eβˆ’01  2.7737Eβˆ’04 βˆ’2.0086Eβˆ’04 βˆ’1.2266Eβˆ’05  8.8248Eβˆ’07
R14 βˆ’4.7637E+00 βˆ’9.8315Eβˆ’03  1.9717Eβˆ’03 βˆ’2.1111Eβˆ’04  7.7554Eβˆ’06

Table 7 and table 8 show the inflexion points and the arrest point design data of the camera optical lens 20 lens in embodiment 2 of the present invention.

TABLE 7
Inflexion point Inflexion point Inflexion point
number position 1 position 2
R1 0
R2 0
R3 1 0.665
R4 0
R5 1 1.075
R6 1 1.025
R7 1 0.285
R8 2 0.525 1.455
R9 3 0.805 0.955
R10 1 1.275
R11 2 0.795 1.875
R12 1 2.155
R13 1 2.415
R14 1 1.165

TABLE 8
Arrest point number Arrest point position 1
R1
R2
R3 1 0.945
R4
R5
R6 1 1.215
R7 1 0.475
R8 1 0.895
R9
R10 1 1.745
R11 2 1.555
R12
R13
R14

FIG. 6 and FIG. 7 show the longitudinal aberration and lateral color schematic diagrams after light with a wavelength of 470 nm, 555 nm and 650 nm passes the camera optical lens 20 in the second embodiment. FIG. 8 shows the field curvature and distortion schematic diagrams after light with a wavelength of 555 nm passes the camera optical lens 20 in the second embodiment.

As shown in Table 13, the second embodiment satisfies the various conditions.

In this embodiment, the pupil entering diameter of the camera optical lens is 1.927 mm, the full vision field image height is 2.9935 mm, the vision field angle in the diagonal direction is 74.99Β°, it has wide-angle and is ultra-thin, its on-axis and off-axis chromatic aberrations are fully corrected, and it has excellent optical characteristics.

Embodiment 3

Embodiment 3 is basically the same as embodiment 1, the meaning of its symbols is the same as that of embodiment 1, in the following, only the differences are described.

The design information of the camera optical lens 30 in the third embodiment of the present invention is shown in the tables 9 and 10.

TABLE 9
R d nd Ξ½ d
S1 ∞ d0= 0.010
R1 40.038 d1= 0.180 nd1 1.6713 Ξ½ 1 19.24
R2 3.640 d2= 0.130
R3 2.131 d3= 0.532 nd2 1.5445 Ξ½ 2 55.99
R4 50.391 d4= 0.080
R5 1.820 d5= 0.304 nd3 1.6713 Ξ½ 3 19.24
R6 2.081 d6= 0.763
R7 6.535 d7= 0.289 nd4 1.7225 Ξ½ 4 29.23
R8 4.514 d8= 0.128
R9 βˆ’6.821 d9= 1.049 nd5 1.5352 Ξ½ 5 56.12
R10 βˆ’1.105 d10= 0.020
R11 8.589 d11= 0.220 nd6 1.5352 Ξ½ 6 56.12
R12 4.009 d12= 0.100
R13 4.42E+00 d13= 0.567 nd7 1.5352 Ξ½ 7 56.12
R14 1.27E+00 d14= 1.000
R15 ∞ d15= 0.210 ndg 1.5168 ν g 64.17
R16 ∞ d16= 0.516

Table 10 shows the aspherical surface data of each lens of the camera optical lens 30 in embodiment 3 of the present invention.

TABLE 10
Conic Index Aspherical Surface Index
k A4 A6 A8 A10 A12 A14 A16
R1  0.0000E+00 βˆ’1.3281Eβˆ’02  3.4807Eβˆ’03  6.1650Eβˆ’03 5.9690Eβˆ’03 βˆ’7.6902Eβˆ’03  1.2037Eβˆ’03
R2 βˆ’7.8639E+00 βˆ’1.8161Eβˆ’02  1.9201Eβˆ’02  1.3742Eβˆ’02 1.9499Eβˆ’03 βˆ’8.6581Eβˆ’03  1.6845Eβˆ’03
R3 βˆ’1.8561E+00 βˆ’1.8692Eβˆ’03 βˆ’6.8987Eβˆ’03 βˆ’6.4127Eβˆ’03 2.5137Eβˆ’03 8.4057Eβˆ’03 βˆ’8.4857Eβˆ’03 
R4  0.0000E+00 βˆ’4.1300Eβˆ’02 βˆ’1.3342Eβˆ’02 βˆ’4.8715Eβˆ’03 βˆ’2.2059Eβˆ’03  7.5707Eβˆ’03 βˆ’1.1926Eβˆ’03  βˆ’2.6979Eβˆ’03
R5  0.0000E+00 βˆ’1.7438Eβˆ’02  5.3765Eβˆ’03 βˆ’5.4502Eβˆ’03 βˆ’2.3269Eβˆ’03  6.4797Eβˆ’03 2.6975Eβˆ’03 βˆ’1.6643Eβˆ’03
R6  0.0000E+00  2.8590Eβˆ’02 βˆ’2.0293Eβˆ’03 βˆ’2.2436Eβˆ’04 3.1307Eβˆ’03 βˆ’9.9425Eβˆ’05  4.5890Eβˆ’03  1.5677Eβˆ’03
R7  1.2847E+01 βˆ’1.0794Eβˆ’01 βˆ’8.0017Eβˆ’04 βˆ’2.2412Eβˆ’02 1.2554Eβˆ’02 6.3529Eβˆ’03 βˆ’2.3332Eβˆ’03   3.1032Eβˆ’05
R8  6.6934E+00 βˆ’7.3472Eβˆ’02 βˆ’4.5483Eβˆ’03  3.1123Eβˆ’03 6.0188Eβˆ’04 βˆ’1.0933Eβˆ’04 
R9 βˆ’1.1229E+01  1.1009Eβˆ’02  1.6927Eβˆ’02 βˆ’9.2068Eβˆ’03 βˆ’4.5921Eβˆ’04  6.6563Eβˆ’04
R10 βˆ’3.3717E+00 βˆ’6.4659Eβˆ’02  1.6487Eβˆ’02 βˆ’2.2915Eβˆ’03 5.1930Eβˆ’04
R11  8.3651E+00 βˆ’2.4249Eβˆ’02  1.6927Eβˆ’03  1.2439Eβˆ’04 βˆ’3.4710Eβˆ’06 
R12 βˆ’1.3905E+00 βˆ’2.5302Eβˆ’03 βˆ’2.4332Eβˆ’04 βˆ’2.7257Eβˆ’05 βˆ’3.1891Eβˆ’06 
R13 βˆ’7.7661Eβˆ’01 βˆ’8.6474Eβˆ’04 βˆ’1.8554Eβˆ’04 βˆ’1.3259Eβˆ’05 βˆ’3.4809Eβˆ’07 
R14 βˆ’6.1580E+00 βˆ’1.0126Eβˆ’02  1.9233Eβˆ’03 βˆ’2.0221Eβˆ’04 9.2814Eβˆ’06

Table 11 and table 12 show the inflexion points and the arrest point design data of the camera optical lens 30 lens in embodiment 3 of the present invention.

TABLE 11
Inflexion point Inflexion point Inflexion point
number position 1 position 2
R1 2 0.465 0.595
R2 0
R3 1 0.935
R4 1 0.205
R5 0
R6 0
R7 2 0.355 1.125
R8 2 0.545 1.255
R9 3 0.705 1.155
R10 1 1.395
R11 0.705 1.755
R12 1 1.745
R13 1 2.135
R14 2 1.075 2.475

TABLE 12
Arrest point number Arrest point position 1
R1
R2
R3
R4 1 0.335
R5
R6
R7 1 0.605
R8 2 0.965
R9
R10
R11 1.305
R12
R13
R14

FIG. 10 and FIG. 11 show the longitudinal aberration and lateral color schematic diagrams after light with a wavelength of 470 nm, 555 nm and 650 nm passes the camera optical lens 30 in the third embodiment. FIG. 12 shows the field curvature and distortion schematic diagrams after light with a wavelength of 555 nm passes the camera optical lens 30 in the third embodiment.

The following table 13, in accordance with the above conditions, lists the values in this embodiment corresponding with each condition expression. Apparently, the camera optical system of this embodiment satisfies the above conditions.

In this embodiment, the pupil entering diameter of the camera optical lens is 1.9511 mm, the full vision field image height is 2.9935 mm, the vision field angle in the diagonal direction is 75.00Β°, it has wide-angle and is ultra-thin, its on-axis and off-axis chromatic aberrations are fully corrected, and it has excellent optical characteristics.

TABLE 13
Embodiment 1 Embodiment 2 Embodiment 3
f 4.121 3.950 4.000
f1 βˆ’9.066 βˆ’12.014 βˆ’5.921
f2 6.458 4.806 4.058
f3 βˆ’25.486 80.900 14.562
f4 98.099 βˆ’11.402 βˆ’21.364
f5 2.044 2.076 2.308
f6 βˆ’28.358 βˆ’26.278 βˆ’14.237
f7 βˆ’2.836 βˆ’2.766 βˆ’3.562
f6/f7 10.000 9.500 3.997
(R1 + R2)/(R1 βˆ’ R2) 7.458 5.024 1.200
(R3 + R4)/(R3 βˆ’ R4) βˆ’0.727 βˆ’0.605 βˆ’1.088
(R5 + R6)/(R5 βˆ’ R6) 0.987 βˆ’63.208 βˆ’14.944
(R7 + R8)/(R7 βˆ’ R8) βˆ’138.285 2.785 5.466
(R9 + R10)/(R9 βˆ’ R10) 1.105 1.235 1.387
(R11 + R12)/(R11 βˆ’ R12) 4.871 4.444 2.750
(R13 + R14)/(R13 βˆ’ R14) 1.721 1.578 1.812
f1/f βˆ’2.200 βˆ’3.041 βˆ’1.480
f2/f 1.567 1.217 1.015
f3/f βˆ’6.184 20.479 3.641
f4/f 23.804 βˆ’2.886 βˆ’5.342
f5/f 0.496 0.525 0.577
f6/f βˆ’6.881 βˆ’6.652 βˆ’3.560
f7/f βˆ’0.688 βˆ’0.700 βˆ’0.891
d1 0.180 0.180 0.180
d3 0.636 0.575 0.532
d5 0.304 0.304 0.304
d7 0.516 0.480 0.289
d9 1.049 1.049 1.049
d11 0.444 0.516 0.220
d13 0.393 0.374 0.567
Fno 2.073 2.050 2.050
TTL 5.747 5.727 5.363
d7/TTL 0.090 0.084 0.054
n1 1.6713 1.6713 1.6713
n2 1.5445 1.5445 1.5445
n3 1.6713 1.6713 1.6713
n4 1.7225 1.8211 1.7225
n5 1.5352 1.5352 1.5352
n6 1.5352 1.5352 1.5352
n7 1.5352 1.5352 1.5352

It is to be understood, however, that even though numerous characteristics and advantages of the present exemplary embodiments have been set forth in the foregoing description, together with details of the structures and functions of the embodiments, the disclosure is illustrative only, and changes may be made in detail, especially in matters of shape, size, and arrangement of parts within the principles of the invention to the full extent indicated by the broad general meaning of the terms where the appended claims are expressed.

Claims

What is claimed is:

1. A camera optical lens comprising, from an object side to an image side in sequence: a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens and a seventh lens; the camera optical lens further satisfies the following conditions:


βˆ’3≀f1/fβ‰€βˆ’1;


1.7≀n4≀2.2;


1≀f6/f7≀10;


1.2≀(R1+R2)/(R1βˆ’R2)≀10;


0.01≀d7/TTL≀0.2; where

f: the focal length of the camera optical lens;

f1: the focal length of the first lens;

f6: the focal length of the sixth lens;

f7: the focal length of the seventh lens;

n4: the refractive power of the fourth lens;

R1: curvature radius of object side surface of the first lens;

R2: the curvature radius of image side surface of the first lens;

d7: the thickness on-axis of the fourth lens;

TTL: the total optical length of the camera optical lens.

2. The camera optical lens as described in claim 1, wherein the first lens is made of plastic material, the second lens is made of plastic material, the third lens is made of plastic material, the fourth lens is made of glass material, the fifth lens is made of plastic material, the sixth lens is made of plastic material, the seventh lens is made of plastic material.

3. The camera optical lens as described in claim 1, wherein first lens has a negative refractive power with a convex object side surface and a concave image side surface; the camera optical lens further satisfies the following conditions:


0.09≀d1≀0.27; where

d1: the thickness on-axis of the first lens.

4. The camera optical lens as described in claim 1, wherein the second lens has a positive refractive power with a convex object side surface and a convex image side surface; the camera optical lens further satisfies the following conditions:


0.51≀f2/f≀2.35;


βˆ’2.18≀(R3+R4)/(R3βˆ’R4)β‰€βˆ’0.40;


0.27≀d3≀0.95; where

f: the focal length of the camera optical lens;

f2: the focal length of the second lens;

R3: the curvature radius of the object side surface of the second lens;

R4: the curvature radius of the image side surface of the second lens;

d3: the thickness on-axis of the second lens.

5. The camera optical lens as described in claim 1, wherein the third lens has a concave image side surface; wherein the camera optical lens further satisfies the following conditions:


βˆ’12.37≀f3/f≀30.72;


βˆ’126.42≀(R5+R6)/(R5βˆ’R6)≀1.48;


0.15≀d5≀0.46; where

f: the focal length of the camera optical lens;

f3: the focal length of the third lens;

R5: the curvature radius of the object side surface of the third lens;

R6: the curvature radius of the image side surface of the third lens;

d5: the thickness on-axis of the third lens.

6. The camera optical lens as described in claim 1, wherein the fourth lens has a convex object side surface and a concave image side surface; the camera optical lens further satisfies the following conditions:


βˆ’10.68≀f4/f≀35.71;


βˆ’276.57≀(R7+R8)/(R7βˆ’R8)≀8.2;


0.14≀d7≀0.77; where

f: the focal length of the camera optical lens;

f4: the focal length of the fourth lens;

R7: the curvature radius of the object side surface of the fourth lens;

R8: the curvature radius of the image side surface of the fourth lens;

d7: the thickness on-axis of the fourth lens.

7. The camera optical lens as described in claim 1, wherein the fifth lens has a positive refractive power with a concave object side surface and a convex image side surface; the camera optical lens further satisfies the following conditions:


0.25≀f5/f≀0.87;


0.55≀(R9+R10)/(R9βˆ’R10)≀2.08;


0.52≀d9≀1.57; where

f: the focal length of the camera optical lens;

f5: the focal length of the fifth lens;

R9: the curvature radius of the object side surface of the fifth lens;

R10: the curvature radius of the image side surface of the fifth lens;

d9: the thickness on-axis of the fifth lens.

8. The camera optical lens as described in claim 1, wherein the sixth lens has a negative refractive power with a convex object side surface and a concave image side surface; the camera optical lens further satisfies the following conditions:


βˆ’13.76≀f6/f≀2.37;


1.38≀(R11+R12)/(R11βˆ’R12)≀7.31;


0.11≀d11≀0.77; where

f: the focal length of the camera optical lens;

f6: the focal length of the sixth lens;

R11: the curvature radius of the object side surface of the sixth lens;

R12: the curvature radius of the image side surface of the sixth lens;

d11: the thickness on-axis of the sixth lens.

9. The camera optical lens as described in claim 1, wherein the seventh lens has a negative refractive power with a convex object side surface and a concave image side surface; the camera optical lens further satisfies the following conditions:


0.79≀(R13+R14)/(R13βˆ’R14)≀2.72;


βˆ’1.78≀f7/fβ‰€βˆ’0.46;


0.19≀d13≀0.85; where

f: the focal length of the camera optical lens;

f7: the focal length of the seventh lens;

d13: the thickness on-axis of the seventh lens;

R13: the curvature radius of the object side surface of the seventh lens;

R14: the curvature radius of the image side surface of the seventh lens.

10. The camera optical lens as described in claim 1, wherein the total optical length TTL of the camera optical lens is less than or equal to 6.32 mm.

11. The camera optical lens as described in claim 1, wherein the aperture F number of the camera optical lens is less than or equal to 2.14.

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