Camera optical lens

TECHNICAL FIELD

The present disclosure relates to the field of optical lens, and more particularly, to a camera optical lens suitable for handheld terminal devices such as smart phones or digital cameras and camera devices such as monitors or PC lenses.

BACKGROUND

With the emergence of smart phones in recent years, the demand for miniature camera lens is increasing day by day, but in general the photosensitive devices of camera lens are nothing more 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 become smaller, plus the current development trend of electronic products towards better functions and thinner and smaller dimensions, miniature camera lenses with good imaging quality therefore have 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, or even a five-piece or six-piece structure. Also, with the development of technology and the increase of the diverse demands of users, and as the pixel area of photosensitive devices is becoming smaller and smaller and the requirement of the system on the imaging quality is improving constantly, an eight-piece lens structure gradually appears in lens designs. Although the common eight-piece lens has good optical performance, its settings on refractive power, lens spacing and lens shape still have some irrationality, which results in that the lens structure cannot achieve a high optical performance while satisfying design requirements for ultra-thin, wide-angle lenses having a big aperture.

BRIEF DESCRIPTION OF DRAWINGS

Many aspects of the exemplary embodiment can be better understood with reference to the following drawings. The components in the drawings are not necessarily drawn to scale, the emphasis instead being placed upon clearly illustrating the principles of the present disclosure. Moreover, in the drawings, like reference numerals designate corresponding parts throughout the several views.

FIG. 1 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 1 of the present disclosure;

FIG. 2 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 1;

FIG. 3 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 1;

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

FIG. 5 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 2 of the present disclosure;

FIG. 6 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 5;

FIG. 7 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 5;

FIG. 8 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 5;

FIG. 9 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 3 of the present disclosure;

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

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

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

DESCRIPTION OF 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

Referring to FIG. 1, the present disclosure provides a camera optical lens 10. FIG. 1 shows the camera optical lens 10 according to Embodiment 1 of the present disclosure. The camera optical lens 10 includes 8 lenses. Specifically, the camera optical lens 10 includes, from an object side to an image side, 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, a seventh lens L7, and an eighth lens L8. An optical element such as a glass filter (GF) can be arranged between the eighth lens L8 and an image plane Si.

The first lens L1 has a positive refractive power, the second lens L2 has a negative refractive power, the third lens L3 has a positive refractive power, the fourth lens L4 has a positive refractive power, the fifth lens L5 has a positive refractive power, the sixth lens L6 has a negative refractive power, the seventh lens L7 has a positive refractive power, and the eighth lens L8 has a negative refractive power.

Here, a focal length of the camera optical lens 10 is defined as f, and a focal length of the first lens L1 is defined as f1. The camera optical lens 10 should satisfy a condition of 1.92≤f1/f≤3.20. When the condition is satisfied, a spherical aberration and the field curvature of the system can be effectively balanced. As an example, 1.93≤f1/f≤3.197.

A focal length of the second lens L2 is defined as f2, which satisfies a condition of f2≤0.00. This leads to the more appropriate distribution of the focal length, thereby achieving a better imaging quality and a lower sensitivity. As an example, f2≤−2.01.

A refractive index of the fourth lens L4 is defined as n4, which satisfies a condition of 1.55≤n4≤1.70. This condition facilitates improving the optical performance of the system. As an example, 1.56≤n4≤1.69.

In this embodiment, with the above configurations of the lenses, the camera optical lens 10 can achieve high performance while satisfying design requirements for a low TTL, which is defined as a total optical length from an object side surface of the first lens to an image plane of the camera optical lens along an optic axis.

An on-axis distance from an image side surface of the sixth lens L6 to an object side surface of the seventh lens L7 is defined as d12, and an on-axis thickness of the seventh lens L7 is defined as d13. The camera optical lens 10 should satisfy a condition of 0.04≤d12/d13≤0.35. This facilitates reducing a total length of the optical system while achieving the ultra-thin effect. As an example, 0.04≤d12/d13≤0.33.

A curvature radius of an object side surface of the second lens L2 is defined as R3, and a curvature radius of an image side surface of the second lens L2 is defined as R4. The camera optical lens 10 should satisfy a condition of 2.00≤(R3+R4)/(R3-R4)≤23.00, which specifies a shape of the second lens. This condition can alleviate the deflection of light passing through the lens while effectively reducing aberrations. As an example, 2.22≤(R3+R4)/(R3−R4)≤22.75.

A curvature radius of the object side surface of the first lens L1 is defined as R1, and a curvature radius of an image side surface of the first lens L1 is defined as R2. The camera optical lens 10 should satisfy a condition of −7.01≤(R1+R2)/(R1-R2)≤−1.25. This condition can reasonably control a shape of the first lens L1 in such a manner that the first lens L1 can effectively correct aberrations of the system. As an example, −4.38≤(R1+R2)/(R1−R2)≤−1.56.

An on-axis thickness of the first lens L1 is defined as d1, and a total optical length from an object side surface of the first lens to an image plane of the camera optical lens along an optic axis is defined as TTL. The camera optical lens 10 should satisfy a condition of 0.04≤d1/TTL≤0.14. This condition can facilitate achieving ultra-thin lenses. As an example, 0.06≤d1/TTL≤0.11.

The focal length of the camera optical lens 10 is defined as f, and the focal length of the second lens L2 is defined as f2. The camera optical lens 10 should satisfy a condition of −190.75≤f2/f≤−1.88. This condition can facilitate correction aberrations of the optical system by controlling a negative refractive power of the second lens L2 within a reasonable range. As an example, −119.22≤f2/f≤−2.34.

An on-axis thickness of the second lens L2 is defined as d3. The camera optical lens 10 should satisfy a condition of 0.03≤d3/TTL≤0.13. This condition can facilitate achieving ultra-thin lenses. As an example, 0.05≤d3/TTL≤0.10.

The focal length of the camera optical lens 10 is defined as f, and the focal length of the third lens L3 is defined as f3. The camera optical lens 10 should satisfy a condition of 1.20≤f3/f≤6.98. This condition can lead to the more appropriate distribution of the refractive power, thereby achieving a better imaging quality and a lower sensitivity. As an example, 1.92≤f3/f≤5.59.

A curvature radius of an object side surface of the third lens L3 is defined as R5, and a curvature radius of an image side surface of the third lens L3 is defined as R6. The camera optical lens 10 should satisfy a condition of −0.56≤(R5+R6)/(R5−R6)≤−0.05, which specifies a shape of the third lens. This condition can alleviate the deflection of light passing through the lens while effectively reducing aberrations. As an example, −0.35≤(R5+R6)/(R5−R6)≤−0.07.

An on-axis thickness of the third lens L3 is defined as d5. The camera optical lens 10 should satisfy a condition of 0.03≤d5/TTL≤0.12. This condition can facilitate achieving ultra-thin lenses. As an example, 0.05≤d5/TTL≤0.09.

The focal length of the camera optical lens 10 is defined as f, and the focal length of the fourth lens L4 is defined as f4. The camera optical lens 10 should satisfy a condition of 0.59≤f4/f≤45.57. This condition can lead to the more appropriate distribution of the refractive power, thereby achieving a better imaging quality and a lower sensitivity. As an example, 0.94≤f4/f≤36.46.

A curvature radius of an object side surface of the fourth lens L4 is defined as R7, and a curvature radius of an image side surface of the fourth lens L4 is defined as R8. The camera optical lens 10 should satisfy a condition of −1.63≤(R7+R8)/(R7−R8)≤9.23, which specifies a shape of the fourth lens L4. This can facilitate correction of an off-axis aberration with development towards ultra-thin lenses. As an example, −1.02≤(R7+R8)/(R7−R8)≤7.38.

An on-axis thickness of the fourth lens L4 is defined as d7. The camera optical lens 10 should satisfy a condition of 0.02≤d7/TTL≤0.06. This condition can facilitate achieving ultra-thin lenses. As an example, 0.03≤d7/TTL≤0.05.

The focal length of the camera optical lens 10 is defined as f, and the focal length of the fifth lens L5 is defined as f5. The camera optical lens 10 should satisfy a condition of 3.95≤f5/f≤85.01. This condition can effectively make a light angle of the camera lens gentle and reduce the tolerance sensitivity. As an example, 6.32≤f5/f≤68.01.

A curvature radius of an object side surface of the fifth lens L5 is defined as R9, and a curvature radius of an image side surface of the fifth lens L5 is defined as R10. The camera optical lens 10 should satisfy a condition of 0.87≤(R9+R10)/(R9-R10)≤15.84, which specifies a shape of the fifth lens L5. This can facilitate correction of an off-axis aberration with development towards ultra-thin lenses. As an example, 1.40≤(R9+R10)/(R9-R10)≤12.68.

An on-axis thickness of the fifth lens L5 is defined as d9. The camera optical lens 10 should satisfy a condition of 0.01≤d9/TTL≤0.07. This condition can facilitate achieving ultra-thin lenses. As an example, 0.02≤d9/TTL≤0.06.

The focal length of the camera optical lens 10 is defined as f, and the focal length of the sixth lens L6 is defined as f6. The camera optical lens 10 should satisfy a condition of −10.41≤f6/f≤−2.06. This condition can lead to the more appropriate distribution of the refractive power, thereby achieving a better imaging quality and a lower sensitivity. As an example, −6.51≤f6/f≤−2.58.

A curvature radius of an object side surface of the sixth lens L6 is defined as R11, and a curvature radius of an image side surface of the sixth lens L6 is defined as R12. The camera optical lens 10 should satisfy a condition of −11.31≤(R11+R12)/(R11−R12)≤−1.79, which specifies a shape of the sixth lens L6. This can facilitate correction of an off-axis aberration with development towards ultra-thin lenses. As an example, −7.07≤(R11+R12)/(R11-R12)≤−2.24.

An on-axis thickness of the sixth lens L6 is defined as d11. The camera optical lens 10 should satisfy a condition of 0.02≤d11/TTL≤0.17. This condition can facilitate achieving ultra-thin lenses. As an example, 0.03≤d11/TTL≤0.14.

The focal length of the camera optical lens 10 is defined as f, and the focal length of the seventh lens L7 is defined as P. The camera optical lens 10 should satisfy a condition of 0.57≤f7/f≤4.61. This condition can lead to the more appropriate distribution of the refractive power, thereby achieving a better imaging quality and a lower sensitivity. As an example, 0.92≤f7/f≤3.69.

A curvature radius of an object side surface of the seventh lens L7 is defined as R13, and a curvature radius of an image side surface of the seventh lens L7 is defined as R14. The camera optical lens 10 should satisfy a condition of −1.72≤(R13+R14)/(R13−R14)≤−0.21, which specifies a shape of the seventh lens L7. This can facilitate correction of an off-axis aberration with development towards ultra-thin lenses. As an example, −1.08≤(R13+R14)/(R13-R14)≤−0.26.

An on-axis thickness of the seventh lens L7 is defined as d13. The camera optical lens 10 should satisfy a condition of 0.05≤d13/TTL≤0.27. This condition can facilitate achieving ultra-thin lenses. As an example, 0.09≤d13/TTL≤0.22.

The focal length of the camera optical lens 10 is defined as f, and the focal length of the eighth lens L8 is defined as f8. The camera optical lens 10 should satisfy a condition of −5.03≤f8/f≤−0.54. This condition can lead to the more appropriate distribution of the refractive power, thereby achieving a better imaging quality and a lower sensitivity. As an example, −3.14≤f8/f≤−0.67.

A curvature radius of an object side surface of the eighth lens L8 is defined as R15, and a curvature radius of an image side surface of the eighth lens L8 is defined as R16. The camera optical lens 10 should satisfy a condition of 0.53≤(R15+R16)/(R15−R16)≤2.10, which specifies a shape of the eighth lens L8. This can facilitate correction of an off-axis aberration with development towards ultra-thin lenses. As an example, 0.85≤(R15+R16)/(R15−R16)≤1.68.

An on-axis thickness of the eighth lens L8 is defined as d15. The camera optical lens 10 should satisfy a condition of 0.02≤d15/TTL≤0.11. This condition can facilitate achieving ultra-thin lenses. As an example, 0.04≤d15/TTL≤0.09.

In this embodiment, an image height of the camera optical lens 10 is defined as IH. The camera optical lens 10 should satisfy a condition of TTL/IH≤1.92. This condition can facilitate achieving ultra-thin lenses.

In this embodiment, an F number of the camera optical lens 10 is defined as Fno. The camera optical lens 10 should satisfy Fno≤1.91, thereby leading to a big aperture.

When the focal length of the camera optical lens 10, the focal lengths of respective lenses, the refractive index of the seventh lens, the on-axis thicknesses of respective lenses, the TTL, and the curvature radius of object side surfaces and image side surfaces of respective lenses satisfy the above conditions, the camera optical lens 10 will have high optical performance while achieving ultra-thin, wide-angle lenses having a big aperture. The camera optical lens 10 is especially suitable for camera lens assembly of mobile phones and WEB camera lenses formed by CCD, CMOS and other imaging elements for high pixels.

With such design, the TTL of the camera optical lens 10 can be as small as possible, thereby maintaining the characteristic of miniaturization.

In the following, examples will be used to describe the camera optical lens 10 of the present disclosure. The symbols recorded in each example will be described as follows. The focal length, on-axis distance, curvature radius, on-axis thickness, inflexion point position, and arrest point position are all in units of mm.

TTL: Optical length (the total optical length from the object side surface of the first lens L1 to the image plane of the camera optical lens along the optic axis) in mm.

In an example, inflexion points and/or arrest points can be arranged on the object side surface and/or image side surface of the lens, so as to satisfy the demand for the high quality imaging. The description below can be referred to for specific implementations.

Table 1 and Table 2 show design data of the camera optical lens 10 according to Embodiment 1 of the present disclosure.

TABLE 1

R
d
nd
νd

S1
∞
d0=
−0.200

R1
1.717
d1=
0.384
nd1
1.5439
ν1
55.95

R2
3.254
d2=
0.024

R3
1.950
d3=
0.348
nd2
1.6400
ν2
23.54

R4
1.784
d4=
0.208

R5
6.431
d5=
0.289
nd3
1.5439
ν3
55.95

R6
−11.419
d6=
0.051

R7
−21.369
d7=
0.158
nd4
1.5661
ν4
37.71

R8
−15.395
d8=
0.068

R9
−36.456
d9=
0.175
nd5
1.5439
ν5
55.95

R10
−9.922
d10=
0.110

R11
−2.116
d11=
0.156
nd6
1.6400
ν6
23.54

R12
−3.025
d12=
0.240

R13
2.908
d13=
0.764
nd7
1.5439
ν7
55.95

R14
−5.578
d14=
0.345

R15
46.705
d15=
0.264
nd8
1.5346
ν8
55.69

R16
1.326
d16=
0.212

R17
∞
d17=
0.210
ndg
1.5170
νg
64.20

R18
∞
d18=
0.206

In the table, meanings of various symbols will be described as follows.

S1: aperture;

R: curvature radius of an optical surface, a central curvature radius for a lens;

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

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

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

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

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

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

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

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

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

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

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

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

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

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

R15: curvature radius of the object side surface of the eighth lens L8;

R16: curvature radius of the image side surface of the eighth lens L8;

R17: curvature radius of an object side surface of the optical filter GF;

R18: curvature radius of an image side surface of the optical filter GF;

d: on-axis thickness of a lens and an on-axis distance between lenses;

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

d1: on-axis thickness of the first lens L1;

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

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

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

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

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

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

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

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

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

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

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

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

d14: on-axis distance from the image side surface of the seventh lens L7 to the object side surface of the eighth lens L8;

d15: on-axis thickness of the eighth lens L8;

d16: on-axis distance from the image side surface of the eighth lens L8 to the object side surface of the optical filter GF;

d17: on-axis thickness of the optical filter GF;

d18: on-axis distance from the image side surface of the optical filter GF to the image plane;

nd: refractive index of d line;

nd1: refractive index of d line of the first lens L1;

nd2: refractive index of d line of the second lens L2;

nd3: refractive index of d line of the third lens L3;

nd4: refractive index of d line of the fourth lens L4;

nd5: refractive index of d line of the fifth lens L5;

nd6: refractive index of d line of the sixth lens L6;

nd7: refractive index of d line of the seventh lens L7;

nd8: refractive index of d line of the eighth lens L8;

ndg: refractive index of d line of the optical filter GF;

vd: abbe number;

v1: abbe number of the first lens L1;

v2: abbe number of the second lens L2;

v3: abbe number of the third lens L3;

v4: abbe number of the fourth lens L4;

v5: abbe number of the fifth lens L5;

v6: abbe number of the sixth lens L6;

v7: abbe number of the seventh lens L7;

v8: abbe number of the eighth lens L8;

vg: abbe number of the optical filter GF.

Table 2 shows aspheric surface data of respective lens in the camera optical lens 10 according to Embodiment 1 of the present disclosure.

TABLE 2

Conic

coefficient
Aspherical surface coefficients

k
A4
A6
A8
A10
A12
A14
A16

R1
7.6732E−02
5.0124E−03
1.2612E−02
2.9449E−02
−4.1630E−02
7.2610E−02
−5.8502E−02
6.5080E−02

R2
−1.3323E+02
−1.7673E−01
4.5108E−01
−3.7090E−01
3.6202E−01
−4.3758E−01
−2.5334E−01
6.7087E−01

R3
−3.2307E+01
−1.3823E−01
3.6790E−01
−4.8130E−01
4.6492E−01
−2.6979E−01
−4.6523E−01
5.7140E−01

R4
−1.1634E+01
1.3411E−01
−2.3517E−01
4.7884E−01
−5.8440E−01
3.1738E−01
−2.6658E−02
−4.0240E−02

R5
−1.2228E+01
−3.4063E−03
−3.7275E−03
1.1664E−02
−3.7523E−02
5.5405E−02
7.6007E−02
−6.3203E−02

R6
1.1296E+02
−4.8457E−03
−3.3308E−02
1.4273E−03
−1.5155E−03
−1.0607E−02
−6.7469E−03
6.0096E−02

R7
4.3423E+02
−3.2026E−02
1.0666E−02
−9.6027E−03
−6.3972E−03
3.3356E−03
8.1947E−03
−5.8170E−03

R8
5.5271E+01
−2.0813E−02
−3.6372E−02
−1.4288E−03
−4.1850E−03
−1.1159E−03
−2.8532E−03
6.7118E−05

R9
1.1447E+03
−5.9513E−02
−3.1455E−02
−2.3466E−02
4.4388E−03
1.0877E−03
4.7242E−04
−8.4964E−04

R10
6.7901E+01
−1.7538E−01
1.1455E−01
−1.0701E−01
−1.1694E−01
3.0803E−01
−2.0752E−01
4.5363E−02

R11
1.1860E+00
−4.5472E−02
2.3191E−01
−4.2921E−01
3.9873E−01
−1.7441E−01
2.2992E−02
−1.0882E−03

R12
−1.7143E+01
−1.4871E−01
2.6588E−01
−3.0280E−01
2.1805E−01
−8.0312E−02
1.1906E−02
1.7897E−04

R13
−1.7044E+01
−4.2712E−02
5.2091E−02
−8.7170E−02
5.2159E−02
−1.7321E−02
2.6097E−03
−5.4587E−05

R14
−8.6067E+01
3.0340E−03
1.0022E−02
−2.6892E−02
1.1151E−02
−1.7264E−03
8.0044E−05
−3.9441E−06

R15
3.3994E+02
−3.4403E−01
1.8795E−01
−5.8711E−02
1.3497E−02
−2.2780E−03
2.3159E−04
−1.0021E−05

R16
−3.4462E+00
−2.3369E−01
1.6113E−01
−7.5278E−02
2.2776E−02
−4.1773E−03
4.1478E−04
−1.7017E−05

In Table 2, k is a conic coefficient, and A4, A6, A8, A10, A12, A14, and A16 are aspheric surface coefficients.

IH: Image Height

y=(x²/R)/[1+{1−(k+1)(x²/R²)}^1/2]+A4x⁴+A6x⁶+A8x⁸+A10x¹⁰+A12x¹²+A14x¹⁴+A16x¹⁶ (1)

In the present embodiment, an aspheric surface of each lens surface uses the aspheric surfaces shown in the above condition (1). However, the present disclosure is not limited to the aspherical polynomials form shown in the condition (1).

Table 3 and Table 4 show design data of inflexion points and arrest points of respective lens in the camera optical lens 10 according to Embodiment 1 of the present disclosure. P1R1 and P1R2 represent the object side surface and the image side surface of the first lens L1, respectively, P2R1 and P2R2 represent the object side surface and the image side surface of the second lens L2, respectively, P3R1 and P3R2 represent the object side surface and the image side surface of the third lens L3, respectively, P4R1 and P4R2 represent the object side surface and the image side surface of the fourth lens L4, respectively, P5R1 and P5R2 represent the object side surface and the image side surface of the fifth lens L5, respectively, P6R1 and P6R2 represent the object side surface and the image side surface of the sixth lens L6, respectively, P7R1 and P7R2 represent the object side surface and the image side surface of the seventh lens L7, respectively, and P8R1 and P8R2 represent the object side surface and the image side surface of the eighth lens L8, respectively. The data in the column named “inflexion point position” refers to vertical distances from 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” refers to vertical distances from arrest points arranged on each lens surface to the optic axis of the camera optical lens 10.

TABLE 3

Number of
Inflexion
Inflexion
Inflexion

inflexion
point
point
point

points
position 1
position 2
position 3

P1R1
0

P1R2
2
0.315
0.415

P2R1
2
0.655
0.825

P2R2
1
0.845

P3R1
0

P3R2
1
0.845

P4R1
0

P4R2
0

P5R1
0

P5R2
0

P6R1
0

P6R2
1
0.875

P7R1
1
0.615

P7R2
0

P8R1
3
0.075
1.325
1.905

P8R2
1
0.515

TABLE 4

Number of
Arrest point

arrest points
position 1

P1R1
0

P1R2
0

P2R1
0

P2R2
0

P3R1
0

P3R2
1
0.955

P4R1
0

P4R2
0

P5R1
0

P5R2
0

P6R1
0

P6R2
1
1.215

P7R1
1
0.995

P7R2
0

P8R1
1
0.125

P8R2
1
1.235

FIG. 2 and FIG. 3 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 656 nm, 587 nm, 546 nm, 486 nm and 436 nm after passing the camera optical lens 10 according to Embodiment 1. FIG. 4 illustrates a field curvature and a distortion of light with a wavelength of 546 nm after passing the camera optical lens 10 according to Embodiment 1, in which a field curvature S is a field curvature in a sagittal direction and T is a field curvature in a tangential direction.

Table 13 below further lists various values of Embodiments 1, 2, and 3 and values corresponding to parameters which are specified in the above conditions.

As shown in Table 13, Embodiment 1 satisfies respective conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 1.659 mm. The image height of 1.0H is 2.90 mm. The FOV (field of view) is 84.40°. Thus, the camera optical lens can achieve ultra-thin, wide-angle lenses while having on-axis and off-axis aberrations sufficiently corrected, thereby leading to better optical characteristics.

Embodiment 2

Embodiment 2 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences therebetween will be described in the following.

Table 5 and Table 6 show design data of a camera optical lens 20 in Embodiment 2 of the present disclosure.

TABLE 5

R
d
nd
νd

S1
∞
d0=
−0.030

R1
1.697
d1=
0.493
nd1
1.5439
ν1
55.95

R2
5.590
d2=
0.025

R3
3.345
d3=
0.357
nd2
1.6400
ν2
23.54

R4
1.402
d4=
0.133

R5
5.962
d5=
0.377
nd3
1.5439
ν3
55.95

R6
−9.120
d6=
0.160

R7
1.371
d7=
0.172
nd4
1.6700
ν4
19.39

R8
−6.519
d8=
0.339

R9
−11.295
d9=
0.254
nd5
1.5439
ν5
55.95

R10
−9.071
d10=
0.276

R11
−2.149
d11=
0.227
nd6
1.6400
ν6
23.54

R12
−4.042
d12=
0.118

R13
2.514
d13=
0.587
nd7
1.5439
ν7
55.95

R14
−13.117
d14=
0.414

R15
10.136
d15=
0.252
nd8
1.5346
ν8
55.69

R16
1.608
d16=
0.804

R17
∞
d17=
0.210
ndg
1.5170
νg
64.20

R18
∞
d18=
0.206

Table 6 shows aspheric surface data of respective lenses in the camera optical lens 20 according to Embodiment 2 of the present disclosure.

TABLE 6

Conic

coefficient
Aspherical surface coefficients

k
A4
A6
A8
A10
A12
A14
A16

R1
9.6297E−01
2.7079E−02
−5.0083E−03
2.9603E−02
4.8505E−01
4.0338E+00
8.2588E+00
−1.7227E+02

R2
−3.5708E+01
−8.2240E−02
8.5700E−01
−1.9548E−01
1.7579E+00
1.4229E+00
−1.9089E+01
−1.4912E+02

R3
−6.9593E+01
−8.7210E−02
3.5371E−01
−1.0454E−01
1.9099E+00
4.3499E+00
2.3642E+00
−1.9309E+02

R4
−7.2088E+00
1.3990E−01
−2.0092E−01
5.2147E−01
−6.4730E−01
4.0248E−01
−2.3776E−01
−2.1999E+00

R5
−3.1174E−01
−1.9611E−02
−6.7386E−03
3.8727E−02
−4.3789E−02
4.1428E−02
−1.2049E−01
−6.3972E−01

R6
1.0620E+02
−5.4201E−02
−3.9466E−02
−7.8800E−03
−5.0159E−03
−3.1451E−03
−3.2659E−03
4.9092E−02

R7
−3.0908E−02
−3.0810E−03
−1.3625E−02
−1.9308E−03
8.0317E−03
7.2103E−03
4.4481E−03
0.0000E+00

R8
2.6402E+01
−1.6681E−02
−1.7755E−02
1.1471E−03
1.7705E−03
−3.6468E−03
−6.6641E−03
3.4419E−03

R9
1.1531E+02
−6.2206E−02
−3.9771E−02
−2.4671E−02
1.1732E−02
1.0369E−02
8.8322E−03
−8.4572E−03

R10
6.5274E+01
−1.7328E−01
8.6852E−02
−1.1551E−01
−8.8177E−02
3.0415E−01
−2.2518E−01
5.3465E−02

R11
2.1048E+00
−5.5815E−02
2.1650E−01
−4.2943E−01
4.2353E−01
−1.7753E−01
2.6735E−02
−1.3174E−03

R12
−2.7031E+01
−1.3211E−01
2.0341E−01
−2.7479E−01
2.0771E−01
−7.7652E−02
1.2009E−02
−2.1440E−04

R13
−1.5797E+01
−1.8420E−02
4.4084E−02
−8.5732E−02
5.0842E−02
−1.5374E−02
2.5858E−03
−1.8455E−04

R14
−3.8423E+02
7.8171E−03
1.3353E−02
−2.3837E−02
1.0151E−02
−1.6942E−03
8.2823E−05
2.8345E−06

R15
1.3749E+01
−3.1556E−01
1.7657E−01
−5.7470E−02
1.3717E−02
−2.3441E−03
2.4070E−04
−1.0768E−05

R16
−6.0612E+00
−2.2055E−01
1.5236E−01
−7.3177E−02
2.2545E−02
−4.1413E−03
4.0816E−04
−1.6421E−05

Table 7 and Table 8 show design data of inflexion points and arrest points of respective lens in the camera optical lens 20 according to Embodiment 2 of the present disclosure.

TABLE 7

Number of
Inflexion point
Inflexion point

inflexion points
position 1
position 2

P1R1
0

P1R2
1
0.485

P2R1
1
0.465

P2R2
1
0.625

P3R1
1
0.595

P3R2
0

P4R1
1
0.885

P4R2
0

P5R1
0

P5R2
0

P6R1
0

P6R2
1
1.165

P7R1
2
0.695
1.515

P7R2
2
0.555
0.745

P8R1
2
0.165
1.275

P8R2
2
0.455
2.105

TABLE 8

Number of
Arrest point

arrest points
position 1

P1R1
0

P1R2
0

P2R1
0

P2R2
0

P3R1
0

P3R2
0

P4R1
0

P4R2
0

P5R1
0

P5R2
0

P6R1
0

P6R2
0

P7R1
1
1.095

P7R2
0

P8R1
1
0.295

P8R2
1
0.975

FIG. 6 and FIG. 7 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 656 nm, 587 nm, 546 nm, 486 nm and 436 nm after passing the camera optical lens 20 according to Embodiment 2. FIG. 8 illustrates a field curvature and a distortion of light with a wavelength of 546 nm after passing the camera optical lens 20 according to Embodiment 2.

As shown in Table 13, Embodiment 2 satisfies respective conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 0.753 mm. The image height of 1.0H is 2.90 mm. The FOV (field of view) is 64.52°. Thus, the camera optical lens can achieve ultra-thin, wide-angle lenses while having on-axis and off-axis aberrations sufficiently corrected, thereby leading to better optical characteristics.

Embodiment 3

Embodiment 3 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences therebetween will be described in the following.

Table 9 and Table 10 show design data of a camera optical lens 30 in Embodiment 3 of the present disclosure.

TABLE 9

R
d
nd
νd

S1
∞
d0=
−0.070

R1
1.794
d1=
0.425
nd1
1.5439
ν1
55.95

R2
3.226
d2=
0.046

R3
1.889
d3=
0.483
nd2
1.6400
ν2
23.54

R4
1.675
d4=
0.254

R5
8.327
d5=
0.427
nd3
1.5439
ν3
55.95

R6
−9.758
d6=
0.200

R7
2.188
d7=
0.237
nd4
1.6700
ν4
19.39

R8
−21.408
d8=
0.168

R9
−11.274
d9=
0.160
nd5
1.5439
ν5
55.95

R10
−9.324
d10=
0.110

R11
−2.034
d11=
0.647
nd6
1.6400
ν6
23.54

R12
−4.443
d12=
0.036

R13
3.764
d13=
0.733
nd7
1.5439
ν7
55.95

R14
−50.334
d14=
0.413

R15
9.948
d15=
0.396
nd8
1.5346
ν8
55.69

R16
1.657
d16=
0.410

R15
∞
d15=
0.210
ndg
1.5170
νg
64.20

R16
∞
d16=
0.206

Table 10 shows aspheric surface data of respective lenses in the camera optical lens 30 according to Embodiment 3 of the present disclosure.

TABLE 10

Conic

coefficient
Aspherical surface coefficients

k
A4
A6
A8
A10
A12
A14
A16

R1
1.0245E−01
−1.3804E−03
5.7510E−02
9.6304E−02
−1.0515E−01
−4.0930E−01
−9.1724E−01
4.4166E+00

R2
−1.8105E+02
−1.6562E−01
6.5959E−01
−6.4402E−01
4.3165E−01
7.1649E−01
−4.0895E+00
4.3769E+00

R3
−3.9452E+01
−5.0402E−02
2.9189E−01
−4.4351E−01
4.3770E−01
1.3331E−01
8.0948E−01
−3.6739E+00

R4
−9.9238E+00
1.2433E−01
−2.1007E−01
5.3598E−01
−7.1284E−01
1.6180E−01
−3.1084E−01
5.2205E−01

R5
3.1299E+01
−3.5006E−03
−1.0393E−02
8.2202E−03
−8.7597E−02
2.3288E−02
−2.5467E−02
−3.4629E−01

R6
1.0648E+02
−3.7555E−02
−2.8198E−02
1.1673E−03
−3.7919E−03
−1.4497E−02
−3.2942E−02
−1.8467E−03

R7
−5.7296E−02
−1.4222E−02
−1.9615E−02
−5.0760E−03
7.0911E−03
6.9474E−03
3.3236E−03
0.0000E+00

R8
4.7095E+01
−2.5960E−03
−1.4505E−02
2.0516E−03
2.5224E−03
−3.5257E−03
−7.5167E−03
1.2748E−03

R9
1.1044E+02
−6.9624E−02
−3.7077E−02
−1.6470E−02
1.8008E−02
1.2184E−02
7.4266E−03
−1.1823E−02

R10
7.0613E+01
−1.7489E−01
9.2794E−02
−1.1659E−01
−9.0168E−02
3.0435E−01
−2.2269E−01
5.7544E−02

R11
2.0760E+00
−3.3605E−02
2.2509E−01
−4.2148E−01
4.2718E−01
−1.7866E−01
2.2321E−02
−6.8769E−03

R12
−9.3419E+01
−1.3953E−01
2.0071E−01
−2.7572E−01
2.0747E−01
−7.7685E−02
1.1992E−02
−2.4123E−04

R13
−9.7918E+00
−4.2735E−02
3.7004E−02
−8.6080E−02
5.0991E−02
−1.5329E−02
2.5857E−03
−1.8775E−04

R14
8.3522E+01
9.9801E−04
1.3363E−02
−2.3743E−02
1.0176E−02
−1.6900E−03
8.3020E−05
2.8051E−06

R15
1.3470E+01
−3.1576E−01
1.7656E−01
−5.7472E−02
1.3717E−02
−2.3427E−03
2.4097E−04
−1.0724E−05

R16
−7.0835E+00
−2.2304E−01
1.5218E−01
−7.3206E−02
2.2541E−02
−4.1418E−03
4.0809E−04
−1.6436E−05

Table 11 and Table 12 show design data of inflexion points and arrest points of respective lens in the camera optical lens 30 according to Embodiment 3 of the present disclosure.

TABLE 11

Number of
Inflexion
Inflexion

inflexion
point
point

points
position 1
position 2

P1R1
0

P1R2
0

P2R1
1
0.635

P2R2
1
0.685

P3R1
1
0.575

P3R2
0

P4R1
1
0.985

P4R2
0

P5R1
0

P5R2
0

P6R1
0

P6R2
1
1.415

P7R1
1
0.605

P7R2
1
1.655

P8R1
2
0.175
1.275

P8R2
2
0.435
2.235

TABLE 12

Number of
Arrest point
Arrest point

arrest points
position 1
position 2

P1R1
0

P1R2
0

P2R1
0

P2R2
0

P3R1
1
0.725

P3R2
0

P4R1
0

P4R2
0

P5R1
0

P5R2
0

P6R1
0

P6R2
0

P7R1
1
0.925

P7R2
0

P8R1
2
0.295
2.085

P8R2
1
0.915

FIG. 10 and FIG. 11 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 656 nm, 587 nm, 546 nm, 486 nm and 436 nm after passing the camera optical lens 30 according to Embodiment 3. FIG. 12 illustrates field curvature and distortion of light with a wavelength of 546 nm after passing the camera optical lens 30 according to Embodiment 3.

Table 13 below further lists various values of the present embodiment and values corresponding to parameters which are specified in the above conditions. Obviously, the camera optical lens according to this embodiment satisfies the above conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 1.102 mm. The image height of 1.0H is 2.90 mm. The FOV (field of view) is 60.00°. Thus, the camera optical lens can achieve ultra-thin, wide-angle lenses while having on-axis and off-axis aberrations sufficiently corrected, thereby leading to better optical characteristics.

TABLE 13

Parameters and

Conditions
Embodiment 1
Embodiment 2
Embodiment 3

f1/f
1.94
2.99
3.19

f2
−180.93
−4.02
−199.81

n4
1.57
1.67
1.67

f
3.152
1.430
2.095

f1
6.116
4.271
6.692

f3
7.575
6.659
8.295

f4
95.757
1.685
2.939

f5
24.898
81.046
95.908

f6
−11.687
−7.445
−6.486

f7
3.614
3.914
6.442

f8
−2.548
−3.597
−3.766

f12
5.850
27.870
6.181

Fno
1.900
1.899
1.901

Fno denotes an F number of the camera optical lens.

It can be appreciated by one having ordinary skill in the art that the description above is only embodiments of the present disclosure. In practice, one having ordinary skill in the art can make various modifications to these embodiments in forms and details without departing from the spirit and scope of the present disclosure.

Number	Name	Date	Kind
20200355891	Ye	Nov 2020	A1
20210181473	Guo	Jun 2021	A1
20210181476	Sun	Jun 2021	A1
20210181479	Lin	Jun 2021	A1
20210181482	Wang	Jun 2021	A1

Camera optical lens

Information

Patent Number

Date Filed

Date Issued

Inventors

Original Assignees

Examiners

Agents

CPC

Field of Search

CPC

International Classifications

Term Extension

Abstract

Description

Claims

Priority Claims (1)

US Referenced Citations (5)

Related Publications (1)