USPatent applicationPatented

Camera optical lens

Granted 7 May 2019 · no office action yet

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Abstract

The present disclosure discloses a camera optical lens. The camera optical lens includes, 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.

Description

11 parts
›CROSS-REFERENCE TO RELATED APPLICATIONS

This application claims the priority benefit of Chinese Patent Applications Ser. No. 201711151270.2 and Ser. No. 201711151237.X filed on Nov. 18, 2017, the entire content of which is incorporated herein by reference.

›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 a camera optical lens in accordance with a third embodiment of the present invention;

FIG. 10 presents the longitudinal aberration of the camera optical lens shown in FIG. 9 ;

FIG. 11 presents the lateral color of the camera optical lens shown in FIG. 9 ;

FIG. 12 presents 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 · 1 of 4

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 S 1 , a first lens L 1 , a second lens L 2 , a third lens L 3 , a fourth lens L 4 , a fifth lens L 5 , a sixth lens L 6 and a seventh lens L 7 . Optical element like optical filter GF can be arranged between the seventh lens L 7 and the image surface S 1 . The first lens L 1 is made of plastic material, the second lens L 2 is made of plastic material, the third lens L 3 is made of plastic material, the fourth lens L 4 is made of glass material, the fifth lens L 5 is made of plastic material, the sixth lens L 6 is made of plastic material, the seventh lens L 7 is made of glass material;

Here, the focal length of the whole camera optical lens 10 is defined as f, the focal length of the first lens is defined as f 1 , the curvature radius of the object side surface of the first lens is defined as R 1 , the curvature radius of the image side surface of the first lens is defined as R 2 , the refractive power of the fourth lens is n 4 , the refractive power of the seventh lens is n 7 , the focal length of the sixth lens is f 6 , the focal length of the seventh lens is f 7 . The camera optical lens 10 satisfies the following conditions: −3≤f 1 /f≤−1, 1.7≤n 4 ≤2.2, 1≤f 6 /f 7 ≤10; 2≤(R 1 +R 2 )/(R 1 −R 2 )≤10; 1.7≤n 7 ≤2.2.

Condition −≤3≤f 1 /f≤−1 fixes the negative refractive power of the first lens L 1 . 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 L 1 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 becomes too weak, it is then difficult to develop ultra-thin lenses. Preferably, the following condition shall be satisfied, − 2 . 40 ≤f 1 /f≤−1.41.

Condition 1.7≤n 4 ≤2.2 fixes the refractive power of the fourth t lens L 4 , 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, 1.76≤n 4 ≤2.06.

Condition 1≤f 6 /f 7 ≤10 fixes the ratio between the focal length f 6 of the sixth lens L 6 and the focal length f 7 of the seventh lens L 7 , 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, 1.014≤f 6 /f 7 ≤9.75.

Condition 2≤(R 1 +R 2 )/(R 1 −R 2 )≤10 fixes the shape of the first lens L 1 , 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 2.49≤(R 1 +R 2 )/(R 1 −R 2 )≤9.56 shall be satisfied.

Condition 1.7≤n 7 ≤2.2 fixes the refractive power of the seventh lens L 7 , this condition benefits the ultra-thin development of lenses, and it also benefits the correction of aberration. Preferably, the following condition shall be satisfied, 1.76≤n 7 ≤2.1.

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 L 1 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 is f, the focal length of the first lens L 1 is f 1 , the thickness on-axis of the first lens L 1 is d 1 : they satisfy the following condition: 0.11≤d 1 ≤0.37, when the condition is meet, it is beneficial for realization of the ultra-thin lens. Preferably, the condition 0.17≤d 1 ≤0.29 shall be satisfied.

In this embodiment, the object side surface of the second lens L 2 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 positive refractive power; the focal length of the whole camera optical lens 10 is f, the focal length of the second lens L 2 is f 2 , the curvature radius of the object side surface of the second lens L 2 is R 3 , the curvature radius of image side surface of the second lens L 2 is R 4 and the thickness on-axis of the second lens L 2 is d 3 , they satisfy the following condition: 0.48≤f 2 /f≤1.62, when the condition is met, the positive refractive power of the second lens L 2 is controlled within reasonable scope, the spherical aberration caused by the first lens L 1 which has negative refractive power and the field curvature of the system then can be reasonably and effectively balanced; the condition −2.81≤(R 3 +R 4 )/(R 3 −R 4 )≤−0.79 fixes the shape of the second lens L 2 , 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 0.22≤d 3 ≤0.79 is met, it is beneficial for the realization of ultra-thin lenses. Preferably, the following conditions shall be satisfied, 0.77≤f 2 /f≤1.30; −1.76≤(R 3 +R 4 )/(R 3 −R 4 )≤−0.99; 0.35≤d 3 ≤0.64

In this embodiment, the object side surface of the third lens L 3 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 third lens L 3 is f 3 , the curvature radius of the object side surface of the third lens L 3 is R 5 , the curvature radius of the image side surface of the third lens L 3 is R 6 and the thickness on-axis of the third lens L 3 is d 5 , they satisfy the condition: 1.18≤f 3 /f≤4.59, 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 −4.93≤(R 5 +R 6 )/(R 5 −R 6 )≤0.69 the shape of the third lens L 3 can be effectively controlled, it is beneficial for the shaping of the third lens L 3 and bad shaping and stress generation due to extra large curvature of surface of the third lens L 3 can be avoided; when the condition 0.15≤d 5 ≤0.79 is met, it is beneficial for the realization of ultra-thin lenses. Preferably, the following conditions shall be satisfied: 1.89≤f 3 /f≤3.67; −3.08≤(R 5 +R 6 )/(R 5 −R 6 )≤0.55; 0.24≤d 5 ≤0.64.

›Embodiment 1 · 2 of 4

In this embodiment, the focal length of the whole camera optical lens 10 is f, the focal length of the fourth lens L 4 is f 4 , the curvature radius of the object side surface of the fourth lens L 4 is R 7 , the curvature radius of the image side surface of the fourth lens L 4 is R 8 and the thickness on-axis of the fourth lens L 4 is d 7 , they satisfy the condition: −39.14≤f 4 /f≤4.17, the appropriate distribution of refractive power makes it possible that the system has better imaging quality and lower sensitivity; the condition −30.94≤(R 7 +R 8 )/(R 7 −R 8 )≤31.20 fixes the shape of the fourth lens L 4 , 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≤d 7 ≤0.80 is met, it is beneficial for realization of ultra-thin lenses. Preferably, the following conditions shall be satisfied, −24.63≤f 4 /f≤3.34; −19.34≤(R 7 +R 8 )/(R 7 −R 8 )≤24.96; 0.22≤d 7 ≤0.64.

In this embodiment, the object side surface of the fifth lens L 5 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 L 5 is f 5 , the curvature radius of the object side surface of the fifth lens L 5 is R 9 , the curvature radius of the image side surface of the fifth lens L 5 is R 10 and the thickness on-axis of the fifth lens L 5 is d 9 , they satisfy the condition: 0.26≤f 5 /f≤2.26, the limitation on the fifth lens L 5 can effectively make the light angle of the camera lens flat and the tolerance sensitivity reduces; the condition 0.77≤(R 9 +R 10 )/(R 9 −R 10 )≤5.06 fixes the shape of the fifth lens L 5 , 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 0.19≤d 9 ≤0.89 is met, it is beneficial for the realization of ultra-thin lens. Preferably, the following conditions shall be satisfied: 0.42≤f 5 /f≤1.81; 1.24≤(R 9 +R 10 )/(R 9 −R 10 )≤4.05; 0.30≤d 9 ≤0.71.

In this embodiment, the object side surface of the sixth lens L 6 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 L 6 is f 6 , the curvature radius of the object side surface of the sixth lens L 6 is R 11 , the curvature radius of the image side surface of the sixth lens L 6 is R 12 and the thickness on-axis of the sixth lens L 6 is d 11 , they satisfy the condition: −22.14≤f 6 /f≤−0.68, the appropriate distribution of refractive power makes it possible that the system has better imaging quality and lower sensitivity; the condition 0.62≤(R 11 +R 12 )/(R 11 −R 12 )≤8.61 fixes the shape of the sixth lens L 6 , 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 0.14≤d 11 ≤1.33, is met, it is beneficial for the realization of ultra-thin lens. Preferably, the following conditions shall be satisfied, −13.84≤f 6 /f≤−0.85; 0.99≤(R 11 +R 12 )/(R 11 −R 12 )≤6.89; 0.22≤d 11 ≤1.06.

In this embodiment, the object side surface of the seventh lens L 7 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 L 7 is R 13 , the curvature radius of the image side surface of the seventh lens L 7 is R 14 , the focal length of the seventh lens L 7 is f 7 , and the thickness on-axis of the seventh lens L 7 is d 13 , they satisfy the condition: 2.10≤(R 13 +R 14 )/(R 13 −R 14 )≤6.87, which fixes the shape of the seventh lens L 7 , 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 −2.33≤f 7 /f≤−0.61 is met, appropriate distribution of refractive power makes it possible that the system has better imaging quality and lower sensitivity; when the condition 0.13≤d 13 ≤0.48 is met, it is beneficial for the realization of ultra-thin lens. Preferably, the following conditions shall be satisfied, 3.36≤(R 13 +R 14 )/(R 13 −R 14 )≤5.50; −1.46≤f 7 /f≤−0.76; 0.21≤d 13 ≤0.38.

In this embodiment, the total optical length TTL of the camera optical lens 10 is less than or equal to 6.17 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 5.89 mm.

In this embodiment, the aperture F number of the camera optical lens 10 is less than or equal to 2.25. A large aperture has better imaging performance. Preferably, the aperture F number of the camera optical lens 10 is less than or equal to 2.20.

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 L 1 ).

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.

›Embodiment 1 · 3 of 4

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.

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

S 1 : Aperture;

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

R 1 : The curvature radius of the object side surface of the first lens L 1 ;

R 2 : The curvature radius of the image side surface of the first lens L 1 ;

R 3 : The curvature radius of the object side surface of the second lens L 2 ;

R 4 : The curvature radius of the image side surface of the second lens L 2 ;

R 5 : The curvature radius of the object side surface of the third lens L 3 ;

R 6 : The curvature radius of the image side surface of the third lens L 3 ;

R 7 : The curvature radius of the object side surface of the fourth lens L 4 ;

R 8 : The curvature radius of the image side surface of the fourth lens L 4 ;

R 9 : The curvature radius of the object side surface of the fifth lens L 5 ;

R 10 : The curvature radius of the image side surface of the fifth lens L 5 ;

R 11 : The curvature radius of the object side surface of the sixth lens L 6 ;

R 12 : The curvature radius of the image side surface of the sixth lens L 6 ;

R 13 : The curvature radius of the object side surface of the seventh lens L 7 ;

R 14 : The curvature radius of the image side surface of the seventh lens L 7 ;

R 15 : The curvature radius of the object side surface of the optical filter GF;

R 16 : 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;

d 0 : The distance on-axis from aperture S 1 to the object side surface of the first lens L 1 ;

d 1 : The thickness on-axis of the first lens L 1 ;

d 2 : The distance on-axis from the image side surface of the first lens L 1 to the object side surface of the second lens L 2 ;

d 3 : The thickness on-axis of the second lens L 2 ;

d 4 : The distance on-axis from the image side surface of the second lens L 2 to the object side surface of the third lens L 3 ;

d 5 : The thickness on-axis of the third lens L 3 ;

d 6 : The distance on-axis from the image side surface of the third lens L 3 to the object side surface of the fourth lens L 4 ;

d 7 : The thickness on-axis of the fourth lens L 4 ;

d 8 : The distance on-axis from the image side surface of the fourth lens L 4 to the object side surface of the fifth lens L 5 ;

d 9 : The thickness on-axis of the fifth lens L 5 ;

d 10 : The distance on-axis from the image side surface of the fifth lens L 5 to the object side surface of the sixth lens L 6 ;

d 11 : The thickness on-axis of the sixth lens L 6 ;

d 12 : The distance on-axis from the image side surface of the sixth lens L 6 to the object side surface of the seventh lens L 7 ;

d 13 : The thickness on-axis of the seventh lens L 7 ;

d 14 : The distance on-axis from the image side surface of the seventh lens L 7 to the object side surface of the optical filter GF;

d 15 : The thickness on-axis of the optical filter GF;

d 16 : 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;

nd 1 : The refractive power of the d line of the first lens L 1 ;

nd 2 : The refractive power of the d line of the second lens L 2 ;

nd 3 : The refractive power of the d line of the third lens L 3 ;

nd 4 : The refractive power of the d line of the fourth lens L 4 ;

nd 5 : The refractive power of the d line of the fifth lens L 5 ;

nd 6 : The refractive power of the d line of the sixth lens L 6 ;

nd 7 : The refractive power of the d line of the seventh lens L 7 ;

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

vd: The abbe number;

v 1 : The abbe number of the first lens L 1 ;

v 2 : The abbe number of the second lens L 2 ;

v 3 : The abbe number of the third lens L 3 ;

v 4 : The abbe number of the fourth lens L 4 ;

v 5 : The abbe number of the fifth lens L 5 ;

v 6 : The abbe number of the sixth lens L 6 ;

v 7 : The abbe number of the seventh lens L 7 ;

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.

Among them, K is a conic index, A 4 , A 6 , A 8 , A 10 , A 12 , A 14 , A 16 are aspheric surface indexes.

IH: Image height

y =( x 2 /R )/[1+{1−( k+ 1)( x 2 /R 2 )} 1/2 ]+ A 4 x 4 +A 6 x 6 +A 8 x 8 +A 10 x 10 +A 12 x 12 +A 14 x 14 +A 16 x 16   (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, R 1 and R 2 represent respectively the object side surface and image side surface of the first lens L 1 , R 3 and R 4 represent respectively the object side surface and image side surface of the second lens L 2 , R 5 and R 6 represent respectively the object side surface and image side surface of the third lens L 3 , R 7 and R 8 represent respectively the object side surface and image side surface of the fourth lens L 4 , R 9 and R 10 represent respectively the object side surface and image side surface of the fifth lens L 5 , R 11 and R 12 represent respectively the object side surface and image side surface of the sixth lens L 6 , R 13 and R 14 represent respectively the object side surface and image side surface of the seventh lens L 7 . The data in the column named “inflexion 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 “arrest 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 .

›Embodiment 1 · 4 of 4

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 1.808 mm, the full vision field image height is 2.994 mm, the vision field angle in the diagonal direction is 74.66°, 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 6 shows the aspherical surface data of each lens of the camera optical lens 20 in embodiment 2 of the present invention.

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

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 1.797 mm, the full vision field image height is 2.994 mm, the vision field angle in the diagonal direction is 74.80°, 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 10 shows the aspherical surface data of each lens of the camera optical lens 30 in embodiment 3 of the present invention.

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.

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 1.798 mm, the full vision field image height is 2.994 mm, the vision field angle in the diagonal direction is 74.75°, 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.

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.

›Tables in the description — 11
TABLE 1
Rdndνd
S1∞d0 =−0.120
R11.917d1 =0.245nd11.6509ν121.52
R21.338d2 =0.107
R32.080d3 =0.437nd21.5352ν256.09
R424.226d4 =0.060
R55.002d5 =0.455nd31.5352ν356.09
R625.540d6 =0.518
R75.172d7 =0.277nd41.9229ν420.88
R84.698d8 =0.638
R9−4.287d9 =0.590nd51.5352ν556.09
R10−0.917d10 =0.035
R1117.603d11 =0.388nd61.5352ν656.09
R121.878d12 =0.040
R131.606d13 =0.260nd71.8211ν724.06
R140.989d14 =0.690
R15∞d15 =0.210ndg1.5168νg64.17
R16∞d16 =0.500
TABLE 2
Conic IndexAspherical Surface Index
kA4A6A8A10A12A14A16
R1−4.7841E+00−4.8186E−022.8141E−02−8.8242E−03−4.0519E−024.2603E−02−6.5363E−03−1.8110E−03
R2−4.2422E+00−5.7414E−03−9.4047E−03−1.1198E−05−8.6682E−03−1.3327E−021.3182E−021.6088E−03
R3−2.2284E+00−5.0246E−022.3324E−024.1762E−03−1.9110E−02−3.6003E−032.7724E−03−4.6418E−03
R4−1.8520E+02−4.7445E−023.8606E−02−7.9210E−031.9379E−02−4.1401E−03−1.2138E−02−1.4130E−03
R5−5.5280E−01−2.7866E−022.6722E−027.8344E−03−4.3544E−03−1.0576E−036.4263E−04−5.1180E−04
R66.2925E+01−5.0025E−028.2040E−03−1.1229E−024.1567E−031.9499E−033.5552E−041.4204E−04
R7−2.0576E−01−1.1315E−019.8270E−03−7.7712E−031.1095E−02−1.6326E−03−1.1758E−04−1.7901E−06
R83.8637E−02−1.0331E−011.4797E−02−3.0130E−032.0911E−031.3385E−03−4.6922E−04−2.5533E−05
R96.1391E+00−7.1617E−031.9851E−02−5.7460E−034.2132E−045.8230E−059.8584E−05−1.1187E−05
R10−3.6735E+00−5.6374E−023.5554E−02−2.9870E−03−3.3844E−042.4625E−053.4690E−05−1.7386E−06
R110.0000E+00−2.1005E−021.9384E−03−1.3897E−04−1.6261E−05−1.9479E−051.3667E−05−1.7320E−06
R12−1.1836E+01−4.1697E−03−3.2423E−031.7294E−041.3592E−05−7.7888E−062.6030E−071.6922E−08
R13−6.1178E+00−2.9379E−024.8968E−042.9371E−04−4.6052E−06−1.5534E−06−3.4891E−072.3433E−08
R14−4.9584E+00−3.6207E−024.7166E−03−2.7681E−046.6641E−068.9909E−07−1.7226E−07−1.7730E−09
TABLE 3
inflexion pointinflexion pointinflexion pointinflexion point
numberposition 1position 2position 3
R120.7850.915
R210.775
R310.795
R430.2950.6550.895
R511.175
R620.2651.055
R720.3851.155
R820.4351.225
R90
R1010.965
R1110.495
R1210.875
R1310.765
R1410.725
TABLE 5
Rdndνd
S1∞d0 =−0.095
R11.262d1 =0.210nd11.6509ν121.52
R21.013d2 =0.175
R31.724d3 =0.482nd21.5352ν256.09
R410.254d4 =0.243
R53.843d5 =0.529nd31.5352ν356.09
R69.081d6 =0.449
R7−2.758d7 =0.537nd41.8211ν424.06
R8−5.101d8 =0.093
R9−2.867d9 =0.506nd51.5352ν556.09
R10−0.980d10 =0.030
R113.891d11 =0.276nd61.5352ν656.09
R122.736d12 =0.050
R131.470d13 =0.280nd71.9229ν720.88
R140.925d14 =0.914
R15∞d15 =0.210ndg1.5168νg64.17
R16∞d16 =0.500
TABLE 6
Conic IndexAspherical Surface Index
kA4A6A8A10A12A14A16
R1−1.8105E+00−4.0268E−02−4.9434E−02−2.0228E−02−6.7404E−026.6544E−021.6950E−02−3.5289E−02
R2−1.8189E+00−8.5480E−03−1.1076E−015.2372E−03−3.0042E−02−9.4410E−02−1.6341E−038.3691E−02
R3−4.7377E−01−1.8147E−021.8265E−031.3163E−01−1.0334E−02−1.2567E−01−4.8011E−038.7679E−02
R40.0000E+00−1.2220E−011.1533E−01−3.1336E−031.7959E−01−1.6611E−02−3.2389E−029.0882E−02
R5−6.8312E+00−1.1590E−01−4.6314E−021.0616E−01−2.3354E−021.9223E−028.0328E−030.0000E+00
R60.0000E+00−5.4069E−02−7.4353E−023.9084E−02−1.5479E−03−1.1300E−031.7990E−030.0000E+00
R76.9250E−01−4.5171E−02−7.6748E−032.1208E−02−1.0903E−027.0653E−03−4.2521E−040.0000E+00
R82.9749E+00−7.3381E−024.2622E−02−1.3045E−024.7867E−03−1.9028E−05−2.0889E−039.8212E−04
R9−1.2565E+001.8219E−022.2091E−02−4.3238E−03−2.4876E−03−7.1890E−041.2349E−041.9882E−04
R10−3.6474E+00−2.4820E−023.9375E−02−5.7824E−03−6.0622E−04−1.0697E−042.9994E−051.4623E−05
R110.0000E+00−2.6653E−027.3096E−043.0558E−042.0945E−05−8.2808E−06−2.0248E−070.0000E+00
R12−2.0335E+00−1.5272E−02−2.4135E−035.2244E−04−8.5276E−05−6.0505E−076.7265E−079.2080E−08
R13−4.3404E+00−3.7619E−023.7635E−03−3.1939E−048.1459E−063.6300E−06−1.5076E−09−3.8444E−09
R14−4.5676E+00−3.5494E−023.4294E−032.5896E−05−1.3437E−05−4.1819E−07−2.6362E−083.0066E−09
TABLE 7
inflexion pointinflexion pointinflexion pointinflexion point
numberposition 1position 2position 3
R110.645
R210.625
R30
R420.2950.505
R520.4050.755
R610.355
R711.045
R811.145
R930.8451.1051.295
R1010.815
R1111.015
R1211.105
R1320.8052.185
R1410.725
TABLE 8
arrest point numberarrest point position 1
R10
R20
R30
R40
R50
R610.575
R70
R80
R90
R100
R110
R1211.835
R1311.695
R1411.945
TABLE 9
Rdndνd
S1∞d0 =0.000
R12.742d1 =0.240nd11.6355ν123.97
R21.364d2 =0.040
R31.988d3 =0.530nd21.5352ν256.09
R419.761d4 =0.040
R518.230d5 =0.303nd31.5352ν356.09
R6−6.729d6 =0.176
R71.825d7 =0.305nd41.8820ν437.22
R82.077d8 =1.164
R9−2.915d9 =0.377nd51.5352ν556.09
R10−1.582d10 =0.030
R1114.631d11 =0.884nd61.5352ν656.09
R128.767d12 =0.090
R131.977d13 =0.320nd72.0018ν719.32
R141.268d14 =0.398
R15∞d15 =0.210ndg1.5168νg64.17
R16∞d16 =0.500
TABLE 10
Conic IndexAspherical Surface Index
kA4A6A8A10A12A14A16
R1−1.7786E+01−8.5511E−02−1.4302E−032.9456E−02−2.6773E−021.2860E−033.4137E−034.2360E−03
R2−5.5272E+00−7.6288E−02−2.3231E−023.3023E−02−2.8343E−03−8.6837E−032.2383E−031.2268E−02
R32.9842E−01−1.5132E−016.5394E−02−4.9510E−03−1.2596E−022.1237E−035.1754E−037.0053E−03
R40.0000E+00−1.0406E−014.2183E−02−6.4437E−04−1.3077E−02−1.7375E−02−3.8600E−031.2921E−02
R50.0000E+002.8637E−06−4.8569E−03−6.9620E−03−1.7776E−020.0000E+000.0000E+000.0000E+00
R60.0000E+00−3.0545E−035.2658E−02−2.1460E−02−1.3573E−023.5493E−035.5843E−03−4.6292E−03
R74.9009E−01−1.0901E−013.2705E−02−1.6535E−023.2966E−03−2.1163E−031.3950E−03−1.6978E−03
R83.2384E−01−7.9670E−02−2.2892E−032.5621E−032.3113E−03−2.5953E−03−2.2068E−034.1263E−04
R93.1281E+003.3365E−028.5566E−03−3.7992E−03−6.8401E−046.1664E−05−7.3533E−06−3.8542E−05
R10−3.1191E+00−1.3032E−023.2062E−02−5.3220E−03−6.0010E−041.2522E−043.4484E−052.0840E−05
R112.5032E+01−7.2663E−031.9036E−031.5878E−041.6781E−05−3.1290E−054.2339E−06−1.1129E−07
R121.2335E+01−5.0799E−03−6.6846E−033.1739E−041.4786E−061.3905E−06−1.0477E−061.8586E−07
R13−1.2764E+01−4.0389E−024.1087E−048.1364E−051.9337E−07−1.4541E−061.0105E−071.3920E−07
R14−6.0833E+00−4.3567E−025.8361E−03−3.5144E−04−5.9803E−061.1721E−063.3162E−08−2.2473E−09
TABLE 12
arrest point numberarrest point position
R110.865
R20
R30
R410.365
R510.795
R60
R70
R80
R90
R1011.445
R110
R1211.295
R1311.185
R1411.585
TABLE 13
EmbodimentEmbodimentEmbodiment
123
f3.8863.9173.884
f1−8.124−11.732−4.548
f24.2093.7844.074
f311.49411.9839.192
f4−76.586−8.09510.804
f52.0462.5365.865
f6−3.949−18.732−43.007
f7−3.841−3.567−4.527
f6/f71.0285.2519.500
(R1 + R2)/(R1 − R2)5.6309.1292.980
(R3 + R4)/(R3 − R4)−1.188−1.404−1.224
(R5 + R6)/(R5 − R6)−1.487−2.4670.461
(R7 + R8)/(R7 − R8)20.798−3.353−15.468
(R9 + R10)/(R9 − R10)1.5442.0393.374
(R11 + R12)/(R11 − R12)1.2395.7383.990
(R13 + R14)/(R13 − R14)4.2034.3984.580
f1/f−2.090−2.995−1.171
f2/f1.0830.9661.049
f3/f2.9583.0592.366
f4/f−19.707−2.0662.781
f5/f0.5260.6471.510
f6/f−1.016−4.782−11.072
f7/f−0.988−0.911−1.165
d10.2450.2100.240
d30.4370.4820.530
d50.4550.5290.303
d70.2770.5370.305
d90.5900.5060.377
d110.3880.2760.884
d130.2600.2800.320
Fno2.1502.1802.160
TTL5.4515.4845.607
n11.65091.65091.6355
n21.53521.53521.5352
n31.53521.53521.5352
n41.92291.82111.8820
n51.53521.53521.5352
n61.53521.53521.5352
n71.82111.92292.0018

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Classifications

4 codes
IPC · International Patent Classification
Section G — Physics
  • G02B1/04
  • G02B13/00
  • G02B9/64
  • G02B13/18

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