CAMERA OPTICAL LENS

TECHNICAL FIELD

The present invention 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 optical lens is increasingly higher, but in general the photosensitive devices of camera optical lens are nothing more than Charge Coupled Devices (CCDs) or Complementary Metal-Oxide Semiconductor Sensors (CMOS sensors). 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 optical lenses with good imaging quality 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. 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 becoming increasingly higher. Although the common four-piece lens has good optical performance, its refractive power, lens spacing and lens shape settings still have some irrationality, such that the lens structure cannot achieve high optical performance while satisfying design requirements for ultra-thin, wide-angle lenses.

SUMMARY

In view of the problems, the present invention aims to provide a camera optical lens, which can achieve high optical performance while satisfying requirements for ultra-thin, wide-angle lenses.

In an embodiment, the present invention provides a camera optical lens. The camera optical lens includes, sequentially from an object side to an image side: a first lens having a positive refractive power; a second lens having a negative refractive power; a third lens having a positive refractive power; and a fourth lens having a negative refractive power. The camera optical lens satisfies following conditions: −0.75≤f1/f2≤−0.67; 0.32≤f4/f2≤0.40; 5.00≤R7/R8≤6.00; and 1.40≤d1/d2≤3.20, where f1 denotes a focal length of the first lens; f2 denotes a focal length of the second lens; f4 denotes a focal length of the fourth lens; R7 denotes a curvature radius of an object side surface of the fourth lens; R8 denotes a curvature radius of an image side surface of the fourth lens; d1 denotes an on-axis thickness of the first lens; and d2 denotes an on-axis distance from an image side surface of the first lens to an object side surface of the second lens.

As an improvement, the camera optical lens further satisfies a following condition: −0.60≤R3/R4≤0.20, where R3 denotes a curvature radius of the object side surface of the second lens; and R4 denotes a curvature radius of an image side surface of the second lens.

As an improvement, the camera optical lens further satisfies following conditions: 0.46≤f1/f≤1.78; −3.21≤(R1+R2)/(R1−R2)≤−0.53; and 0.07≤d1/TTL≤0.32, where f denotes a focal length of the camera optical lens; R1 denotes a curvature radius of an object side surface of the first lens; R2 denotes a curvature radius of the image side surface of the first lens; and TTL denotes a total optical length from the object side surface of the first lens to an image plane of the camera optical lens along an optic axis.

As an improvement, the camera optical lens further satisfies following conditions: −3.45≤f2/f≤−0.88; −2.95≤(R3+R4)/(R3−R4)≤−0.17; and 0.03≤d3/TTL≤0.15, where f denotes a focal length of the camera optical lens; R3 denotes a curvature radius of the object side surface of the second lens; R4 denotes a curvature radius of an image side surface of the second lens; d3 denotes an on-axis thickness of the second lens; and TTL denotes 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.

As an improvement, the camera optical lens further satisfies following conditions: 0.23≤f3/f≤0.76; 0.39≤(R5+R6)/(R5−R6)≤1.76; and 0.09≤d5/TTL≤0.33, where f denotes a focal length of the camera optical lens; f3 denotes a focal length of the third lens; R5 denotes a curvature radius of an object side surface of the third lens; R6 denotes a curvature radius of an image side surface of the third lens; d5 denotes an on-axis thickness of the third lens; and TTL denotes 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.

As an improvement, the camera optical lens further satisfies following conditions: −1.25≤f4/f≤−0.32; 0.70≤(R7+R8)/(R7−R8)≤2.25; and 0.04≤d7/TTL≤0.19, where f denotes a focal length of the camera optical lens; d7 denotes an on-axis thickness of the fourth lens; and TTL denotes 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.

As an improvement, the camera optical lens further satisfies a following condition: TTL/IH≤1.68, where TTL denotes 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; and IH denotes an image height of the camera optical lens.

As an improvement, the camera optical lens further satisfies a following condition: 0.91≤f12/f≤3.71, where f denotes a focal length of the camera optical lens; and f12 denotes a combined focal length of the first lens and the second lens.

The present invention has advantageous effects in that the camera optical lens according to the present invention has excellent optical performance, and is ultra-thin, wide-angle, making it especially suitable for high-pixel camera optical lens assembly of mobile phones and WEB camera optical lenses formed by camera elements such as CCD and CMOS.

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 invention. 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 invention;

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 invention;

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 invention;

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;

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

FIG. 13 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 4 of the present invention;

FIG. 14 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 13;

FIG. 15 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 13;

FIG. 16 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 13;

FIG. 17 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 5 of the present invention;

FIG. 18 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 17;

FIG. 19 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 17; and

FIG. 20 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 17.

DESCRIPTION OF EMBODIMENTS

The present invention 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 invention more apparent, the present invention 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 invention provides a camera optical lens 10. FIG. 1 shows the camera optical lens 10 according to Embodiment 1 of the present invention. The camera optical lens 10 includes four lenses. Specifically, the camera optical lens 10 includes, sequentially from an object side to an image side, an aperture S1, a first lens L1 having a positive refractive power, a second lens L2 having a negative refractive power, a third lens L3 having a positive refractive power, and a fourth lens L4 having a negative refractive power. An optical element such as a glass filter (GF) can be arranged between the fourth lens L4 and an image plane Si.

A focal length of the first lens L1 is defined as f1, and a focal length of the second lens L2 is defined as f2. The camera optical lens 10 should satisfy a condition of −0.75≤f1/f2≤−0.67, which specifies a ratio of the focal length of the first lens L1 to the focal length of the second lens L2. This can effectively balance spherical aberrations and a field curvature of the system.

A focal length of the fourth lens L4 is defined as f4. The camera optical lens 10 should satisfy a condition of 0.32≤f4/f2≤0.40, which specifies a ratio of the focal length of the fourth lens L4 to the focal length of the second lens L2. The appropriate distribution of the focal lengths leads to better imaging quality and a lower sensitivity.

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 5.00≤R7/R8≤6.00, which specifies a shape of the fourth lens L4. This can facilitate correction of an off-axis aberration with development towards ultra-thin, wide-angle lenses.

An on-axis thickness of the first lens L1 is defined as d1, and an on-axis distance from an image side surface of the first lens L1 to an object side surface of the second lens L2 is defined as d2. The camera optical lens 10 should satisfy a condition of 1.40≤d1/d2≤3.20, which specifies a ratio of the on-axis thickness of the first lens L1 to the on-axis distance from the image side surface of the first lens L1 to the object side surface of the second lens L2. When the condition is satisfied, reduction of the total length can be facilitated, thereby achieving ultra-thin lenses.

A curvature radius of the 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 −0.60≤R3/R4≤0.20, which specifies a shape of the second lens L2. This can facilitate correction of an on-axis aberration.

A focal length of the camera optical lens 10 is defined as f, and the focal length of the first lens L1 is defined as f1. The camera optical lens 10 should satisfy a condition of 0.46≤f1/f≤1.78, which specifies a ratio of the focal length of the first lens L1 to the focal length of the camera optical lens 10. When the condition is satisfied, the first lens L1 can have an appropriate positive refractive power, thereby facilitate correction of aberrations with development towards ultra-thin, wide-angle lenses.

The curvature radius of an object side surface of the first lens L1 is defined as R1, and a curvature radius of the image side surface of the first lens L1 is defined as R2. The camera optical lens 10 should satisfy a condition of −3.21≤(R1+R2)/(R1−R2)≤−0.53. When the condition is satisfied, a shape of the first lens L1 can be reasonably controlled, so that the first lens L1 can effectively correct spherical aberrations of the system.

A total optical length from the object side surface of the first lens L1 to an image plane of the camera optical lens 10 along an optic axis is defined as TTL, and an on-axis thickness of the first lens is defined as d1. The camera optical lens 10 should satisfy a condition of 0.07≤d1/TTL≤0.32. When the condition is satisfied, ultra-thin lenses can be achieved.

The focal length of the second lens L2 is defined as f2, and the focal length of the camera optical lens 10 is defined as f. The camera optical lens 10 should satisfy a condition of −3.45≤f2/f≤−0.88, which specifies a ratio of the focal length of the second lens L2 to the focal length of the camera optical lens 10. By controlling the negative refractive power of the second lens L2 within the reasonable range, correction of aberrations of the optical system can be facilitated.

A curvature radius of the 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 −2.95≤(R3+R4)/(R3−R4)≤−0.17, which specifies a shape of the second lens L2. This can facilitate correction of an on-axis aberration with development towards ultra-thin, wide-angle lenses.

An on-axis thickness of the second lens L2 is defined as d3, and the total optical length from the object side surface of the first lens L1 to the image plane of the camera optical lens 10 along the optic axis is defined as TTL. The camera optical lens 10 should satisfy a condition of 0.03≤d3/TTL≤0.15. When the condition is satisfied, ultra-thin lenses can be achieved.

The focal length of the third lens L3 is defined as f3, and the focal length of the camera optical lens 10 is defined as f. The camera optical lens 10 should satisfy a condition of 0.23≤f3/f≤0.76. The appropriate distribution of the refractive power leads to better imaging quality and a lower sensitivity.

The curvature radius of the 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 0.39≤(R5+R6)/(R5−R6)≤1.76. This can effectively control a shape of the third lens L3, thereby facilitating shaping of the third lens L3 and avoiding bad shaping and generation of stress due to the overly large surface curvature of the third lens L3.

The on-axis thickness of the third lens L3 is defined as d5, and the total optical length from the object side surface of the first lens L1 to the image plane of the camera optical lens 10 along the optic axis is defined as TTL. The camera optical lens 10 should satisfy a condition of 0.09≤d5/TTL≤0.33. When the condition is satisfied, ultra-thin lenses can be achieved.

The focal length of the fourth lens L4 is defined as f4, and the focal length of the camera optical lens 10 is defined as f. The camera optical lens 10 should satisfy a condition of −1.25≤f4/f≤−0.32. The appropriate distribution of the refractive power leads to better imaging quality and a lower sensitivity.

A curvature radius of the object side surface of the fourth lens L4 is defined as R7, and a curvature radius of the image side surface of the fourth lens L4 is defined as R8. The camera optical lens 10 should satisfy a condition of 0.70≤(R7+R8)/(R7−R8)≤2.25, which specifies a shape of the fourth lens L4. This can facilitate correction of an off-axis aberration with development towards ultra-thin, wide-angle lenses.

The on-axis thickness of the fourth lens L4 is defined as d7, and the total optical length from the object side surface of the first lens L1 to the image plane of the camera optical lens 10 along the optic axis is defined as TTL. The camera optical lens 10 should satisfy a condition of 0.04≤d7/TTL≤0.19. When the condition is satisfied, ultra-thin lenses can be achieved.

Further, the total optical length from the object side surface of the first lens to the image plane of the camera optical lens along the optic axis is defined as TTL, and 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≤1.68. When the condition is satisfied, ultra-thin lenses can be achieved.

A combined focal length of the first lens L1 and the second lens L2 is defined as f12. The camera optical lens 10 should satisfy a condition of 0.91≤f12/f≤3.71. This can eliminate aberration and distortion of the camera optical lens 10, suppress the back focal length of the camera optical lens 10, and maintain miniaturization of the camera lens system group.

When the above conditions are satisfied, the camera optical lens 10 will have high optical imaging performance while satisfying design requirements for ultra-thin, wide-angle lenses. With these characteristics, the camera optical lens 10 is especially suitable for high-pixel camera optical lens assembly of mobile phones and WEB camera optical lenses formed by imaging elements such as CCD and CMOS.

In the following, examples will be used to describe the camera optical lens 10 of the present invention. 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 Si 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 invention.

TABLE 1

R
d
nd
νd

S1
∞
d0=
−0.135

R1
1.502
d1=
0.547
nd1
1.5444
ν1
55.82

R2
10.851
d2=
0.334

R3
−4.440
d3=
0.381
nd2
1.6610
ν2
20.53

R4
8.928
d4=
0.145

R5
−8.961
d5=
0.755
nd3
1.5444
ν3
55.82

R6
−0.664
d6=
0.042

R7
3.165
d7=
0.412
nd4
1.5346
ν4
55.69

R8
0.600
d8=
0.500

R9
∞
d9=
0.210
ndg
1.5168
νg
64.17

R10
∞
d10=
0.524

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

S1: aperture;

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

R10: 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 optical filter GF;

d9: on-axis thickness of the optical filter GF;

d10: 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;

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;

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 invention.

TABLE 2

Conic coefficient
Aspherical surface coefficients

k
A4
A6
A8
A10
A12
A14
A16

R1
−3.6594E+00
9.5143E−02
1.2954E−01
−1.5598E+00
7.1079E+00
−2.0198E+01
3.0342E+01
−1.8976E+01

R2
−2.8056E+01
−1.4988E−01
1.8271E−01
−2.4549E+00
9.1704E+00
−2.1198E+01
2.6958E+01
−1.4557E+01

R3
2.7852E+01
−3.9007E−01
4.3337E−01
−3.2543E+00
1.1956E+01
−2.9063E+01
4.3445E+01
−2.5698E+01

R4
−1.0403E+02
−2.2130E−01
2.9877E−01
−8.2603E−01
1.6890E+00
−2.6098E+00
2.6008E+00
−1.0074E+00

R5
1.2675E+01
4.4841E−02
−1.0559E−01
5.1989E−01
−1.0670E+00
1.1297E+00
−5.8503E−01
1.1444E−01

R6
−4.0220E+00
−4.2490E−01
1.0083E+00
−1.9183E+00
2.4925E+00
−1.7054E+00
5.6881E−01
−7.4331E−02

R7
−1.0677E+02
−1.6480E−01
−1.2214E−02
9.4858E−02
−5.5035E−02
1.5801E−02
−2.5123E−03
1.4274E−04

R8
−4.9594E+00
−1.7531E−01
1.2556E−01
−7.4367E−02
3.0343E−02
−7.8928E−03
1.1667E−03
−7.5298E−05

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

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 invention is not limited to the aspherical polynomial 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 invention. 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; and P4R1 and P4R2 represent the object side surface and the image side surface of the fourth lens L4, respectively. The data in the column “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 “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 point
Inflexion point
Inflexion point

inflexion points
position 1
position 2
position 3

P1R1
1
0.645
0
0

P1R2
1
0.235
0
0

P2R1
0
0
0
0

P2R2
2
0.215
0.785
0

P3R1
2
0.475
1.045
0

P3R2
2
0.725
1.185
0

P4R1
3
0.265
1.115
1.385

P4R2
1
0.445
0
0

TABLE 4

Number of
Arrest point
Arrest point

arrest points
position 1
position 2

P1R1
0
0
0

P1R2
1
0.375
0

P2R1
0
0
0

P2R2
2
0.375
0.905

P3R1
1
0.775
0

P3R2
2
1.145
1.215

P4R1
1
0.505
0

P4R2
1
1.255
0

FIG. 2 and FIG. 3 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 470 nm, 510 nm, 555 nm, 610 nm and 650 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 555 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 21 below further lists various values of Embodiments 1, 2, 3, 4 and 5 and values corresponding to parameters which are specified in the above conditions.

As shown in Table 21, Embodiment 1 satisfies the respective conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 1.349 mm. The image height IH of the camera optical lens is 2.297 mm. The FOV (field of view) along a diagonal direction is 79.30°. Thus, the camera optical lens 10 can provide an ultra-thin, wide-angle lens 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. A structure of a camera optical lens 20 in accordance with Embodiment 2 of the present invention is illustrated in FIG. 5, which only describes differences from Embodiment 1.

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

TABLE 5

R
d
nd
νd

S1
∞
d0=
−0.140

R1
1.528
d1=
0.759
nd1
1.5444
ν1
55.82

R2
−13.487
d2=
0.267

R3
−1.969
d3=
0.373
nd2
1.6359
ν2
23.82

R4
−12.614
d4=
0.246

R5
6.448
d5=
0.657
nd3
1.5444
ν3
55.82

R6
−0.813
d6=
0.076

R7
3.024
d7=
0.315
nd4
1.5438
ν4
56.03

R8
0.563
d8=
0.500

R9
∞
d9=
0.210
ndg
1.5168
νg
64.17

R10
∞
d10=
0.367

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

TABLE 6

Conic coefficient
Aspherical surface coefficients

k
A4
A6
A8
A10
A12
A14
A16

R1
−5.4508E+00
1.1170E−01
7.1354E−01
−7.6533E+00
3.5458E+01
−8.9505E+01
1.1602E+02
−6.0915E+01

R2
−3.8983E+02
−2.5161E−01
−1.0676E−01
4.0786E−02
−9.0888E−01
2.4631E+00
−1.6716E−01
−3.0983E+00

R3
−1.2922E+01
−6.8273E−01
7.0158E−01
−2.5226E+00
1.0592E+01
−2.1453E+01
2.5675E+01
−1.5112E+01

R4
−1.3701E+01
−1.8750E−01
−8.3992E−01
5.4376E+00
−1.4614E+01
2.2458E+01
−1.7874E+01
5.7001E+00

R5
−1.8063E+02
1.8975E−01
−6.3765E−01
1.1639E+00
−1.2050E+00
7.0137E−01
−2.0992E−01
2.1982E−02

R6
−1.1361E+00
8.5652E−01
−1.6825E+00
2.2251E+00
−1.6522E+00
6.9144E−01
−1.5692E−01
1.5261E−02

R7
−2.0074E+02
−3.2423E−01
−8.3737E−02
4.4959E−01
−3.5549E−01
1.3231E−01
−2.4639E−02
1.8588E−03

R8
−4.9106E+00
−3.0067E−01
2.9931E−01
−2.1557E−01
1.0291E−01
−3.0400E−02
4.8959E−03
−3.2404E−04

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 invention.

TABLE 7

Number of
Inflexion point
Inflexion point

inflexion points
position 1
position 2

P1R1
1
0.645
0

P1R2
0
0
0

P2R1
0
0
0

P2R2
1
0.625
0

P3R1
1
0.885
0

P3R2
2
0.665
1.165

P4R1
2
0.195
0.955

P4R2
1
0.395
0

TABLE 8

Number of
Arrest point
Arrest point

arrest points
position 1
position 2

P1R1
0
0
0

P1R2
0
0
0

P2R1
0
0
0

P2R2
1
0.795
0

P3R1
1
1.095
0

P3R2
0
0
0

P4R1
2
0.355
1.605

P4R2
1
1.135
0

FIG. 6 and FIG. 7 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 470 nm, 510 nm, 555 nm, 610 nm and 650 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 555 nm after passing the camera optical lens 20 according to Embodiment 2, 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 21 below further lists various values corresponding to the above conditions according to the present embodiment. The camera optical lens 20 according to the present embodiment satisfies the respective conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens 20 is 1.376 mm. The image height of the camera optical lens 20 is 2.297 mm. The FOV (field of view) along a diagonal direction is 77.00°. Thus, the camera optical lens 20 can provide an ultra-thin, wide-angle lens 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. A structure of a camera optical lens 30 in accordance with Embodiment 3 of the present invention is illustrated in FIG. 9, which only describes differences from Embodiment 1.

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

TABLE 9

R
d
nd
νd

S1
∞
d0=
−0.135

R1
1.367
d1=
0.554
nd1
1.5444
ν1
55.82

R2
5.877
d2=
0.395

R3
−4.972
d3=
0.329
nd2
1.6610
ν2
20.53

R4
8.427
d4=
0.100

R5
−8.509
d5=
0.811
nd3
1.5444
ν3
55.82

R6
−0.688
d6=
0.060

R7
3.088
d7=
0.413
nd4
1.5346
ν4
55.69

R8
0.615
d8=
0.375

R9
∞
d9=
0.210
ndg
1.5168
νg
64.17

R10
∞
d10=
0.523

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

TABLE 10

Conic coefficient
Aspherical surface coefficients

k
A4
A6
A8
A10
A12
A14
A16

R1
−3.0409E+00
9.6256E−02
3.0749E−01
−1.6900E+00
6.1703E+00
−1.9161E+01
3.5489E+01
−2.6619E+01

R2
3.7713E+01
−1.4642E−01
3.6009E−01
−2.7363E+00
9.3108E+00
−2.1217E+01
2.6666E+01
−1.4389E+01

R3
3.9850E+01
−3.6081E−01
1.0537E−01
−1.7065E+00
1.0564E+01
−3.1648E+01
4.4795E+01
−2.2502E+01

R4
−2.5892E+02
−2.8975E−01
3.9285E−01
−7.2105E−01
1.5405E+00
−2.8428E+00
2.9720E+00
−1.1036E+00

R5
4.4701E+01
−2.2829E−02
−2.4956E−02
5.1726E−01
−1.0965E+00
1.0999E+00
−5.7376E−01
1.2778E−01

R6
−3.9488E+00
−4.1008E−01
1.0060E+00
−1.9422E+00
2.4824E+00
−1.7017E+00
5.7335E−01
−7.5131E−02

R7
−1.4122E+02
−1.3736E−01
−7.6177E−03
9.1477E−02
−5.6685E−02
1.6041E−02
−2.2030E−03
1.1183E−04

R8
−4.9791E+00
−1.6565E−01

1.242IE−01
−7.4134E−02
3.0432E−02
−7.9012E−03
1.1581E−03
−7.2234E−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 invention.

TABLE 11

Number of
Inflexion point
Inflexion point
Inflexion point

inflexion points
position 1
position 2
position 3

P1R1
1
0.675
0
0

P1R2
1
0.355
0
0

P2R1
0
0
0
0

P2R2
2
0.185
0.775
0

P3R1
3
0.605
0.915
0.945

P3R2
2
0.755
1.155
0

P4R1
3
0.265
1.045
1.665

P4R2
1
0.465
0
0

TABLE 12

Number of
Arrest point
Arrest point

arrest points
position 1
position 2

P1R1
0
0
0

P1R2
1
0.545
0

P2R1
0
0
0

P2R2
2
0.325
0.885

P3R1
0
0
0

P3R2
0
0
0

P4R1
2
0.525
1.465

P4R2
1
1.365
0

FIG. 10 and FIG. 11 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 436 nm, 486 nm, 546 nm, 587 nm and 656 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, 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 21 below further lists various values corresponding to the above conditions according to the present embodiment. The camera optical lens 30 according to the present embodiment satisfies the respective conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens 30 is 1.335 mm. The image height of the camera optical lens 30 is 2.297 mm. The FOV (field of view) along a diagonal direction is 79.80°. Thus, the camera optical lens 30 can provide an ultra-thin, wide-angle lens while having on-axis and off-axis aberrations sufficiently corrected, thereby leading to better optical characteristics.

Embodiment 4

Embodiment 4 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1. A structure of a camera optical lens 40 in accordance with Embodiment 4 of the present invention is illustrated in FIG. 13, which only describes differences from Embodiment 1.

Table 13 and Table 14 show design data of a camera optical lens 40 in Embodiment 4 of the present invention.

TABLE 13

R
d
nd
νd

S1
∞
d0=
−0.135

R1
1.426
d1=
0.644
nd1
1.5444
ν1
55.82

R2
6.474
d2=
0.403

R3
−4.394
d3=
0.230
nd2
1.6610
ν2
20.53

R4
8.490
d4=
0.056

R5
−8.906
d5=
0.858
nd3
1.5444
ν3
55.82

R6
−0.716
d6=
0.050

R7
4.271
d7=
0.493
nd4
1.5346
ν4
55.69

R8
0.717
d8=
0.382

R9
∞
d9=
0.210
ndg
1.5168
νg
64.17

R10
∞
d10=
0.523

Table 14 shows aspheric surface data of respective lenses in the camera optical lens 40 according to Embodiment 4 of the present invention.

TABLE 14

Conic coefficient
Aspherical surface coefficients

k
A4
A6
A8
A10
A12
A14
A16

R1
−8.1596E+00
2.6195E−01
1.3491E−01
−2.1258E+00
8.0486E+00
−1.9286E+01
2.7780E+01
−1.7616E+01

R2
7.1537E+01
−1.9032E−01
5.5613E−01
−2.6670E+00
7.3471E+00
−1.9676E+01
3.4999E+01
−2.6211E+01

R3
2.4538E+01
−5.0011E−01
3.9754E−01
−2.4278E+00
1.1056E+01
−2.9632E+01
4.4850E+01
−2.6771E+01

R4
−9.3594E+02
−3.9242E−01
3.9976E−01
−6.1644E−01
1.7112E+00
−2.8370E+00
2.7179E+00
−1.0530E+00

R5
6.5394E+01
−1.1846E−01
1.0404E−01
5.8618E−01
−1.1836E+00
1.0437E+00
−4.9840E−01
1.1056E−01

R6
−3.7112E+00
−4.3583E−01
1.0276E+00
−1.9491E+00
2.4773E+00
−1.6979E+00
5.7736E−01
−7.7499E−02

R7
−2.6721E+02
−1.1706E−01
−9.5612E−03
8.9382E−02
−5.7659E−02
1.6046E−02
−1.8574E−03
3.4521E−05

R8
−5.1768E+00
−1.5379E−01
1.1955E−01
−7.3702E−02
3.0717E−02
−7.9318E−03
1.1286E−03
−6.7516E−05

Table 15 and Table 16 show design data of inflexion points and arrest points of respective lens in the camera optical lens 40 according to Embodiment 4 of the present invention.

TABLE 15

Number of
Inflexion point
Inflexion point
Inflexion point

inflexion points
position 1
position 2
position 3

P1R1
0
0
0
0

P1R2
1
0.365
0
0

P2R1
0
0
0
0

P2R2
2
0.145
0.715
0

P3R1
2
0.565
0.995
0

P3R2
2
0.765
1.175
0

P4R1
3
0.255
1.055
1.525

P4R2
1
0.485
0
0

TABLE 16

Number of
Arrest point
Arrest point

arrest points
position 1
position 2

P1R1
0
0
0

P1R2
1
0.555
0

P2R1
0
0
0

P2R2
2
0.245
0.875

P3R1
2
0.845
1.055

P3R2
0
0
0

P4R1
1
0.495
0

P4R2
1
1.415
0

FIG. 14 and FIG. 15 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 436 nm, 486 nm, 546 nm, 587 nm and 656 nm after passing the camera optical lens 40 according to Embodiment 4. FIG. 16 illustrates field curvature and distortion of light with a wavelength of 546 nm after passing the camera optical lens 40 according to Embodiment 4, 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 21 below further lists various values corresponding to the above conditions according to the present embodiment. The camera optical lens 40 according to the present embodiment satisfies the respective conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens 40 is 1.345 mm. The image height of the camera optical lens 40 is 2.297 mm. The FOV (field of view) along a diagonal direction is 79.50°. Thus, the camera optical lens 40 can provide an ultra-thin, wide-angle lens while having on-axis and off-axis aberrations sufficiently corrected, thereby leading to better optical characteristics.

Embodiment 5

Embodiment 5 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1. A structure of a camera optical lens 50 in accordance with Embodiment 5 of the present invention is illustrated in FIG. 17, which only describes differences from Embodiment 1.

Table 17 and Table 18 show design data of a camera optical lens 50 in Embodiment 5 of the present invention.

TABLE 17

R
d
nd
νd

S1
∞
d0=
−0.140

R1
1.403
d1=
0.802
nd1
1.5444
ν1
55.82

R2
156.843
d2=
0.251

R3
−1.917
d3=
0.291
nd2
1.6359
ν2
23.82

R4
−9.986
d4=
0.234

R5
21.102
d5=
0.668
nd3
1.5444
ν3
55.82

R6
−0.762
d6=
0.048

R7
2.828
d7=
0.350
nd4
1.5438
ν4
56.03

R8
0.563
d8=
0.506

R9
∞
d9=
0.210
ndg
1.5168
νg
64.17

R10
∞
d10=
0.367

Table 18 shows aspheric surface data of respective lenses in the camera optical lens 50 according to Embodiment 5 of the present invention.

TABLE 18

Conic coefficient
Aspherical surface coefficients

k
A4
A6
A8
A10
A12
A14
A16

R1
−7.4593E+00
2.0878E−01
7.4588E−01
−7.8961E+00
3.5555E+01
−8.8912E+01
1.1603E+02
−6.1859E+01

R2
9.9771E+02
−2.7407E−01
−1.5490E−02
−1.5315E−01
−1.3824E+00
2.9653E+00
1.5325E+00
−4.3968E+00

R3
−4.6752E+01
−1.1380E+00
1.3838E+00
−2.3102E+00
8.9457E+00
−2.1246E+01
3.0210E+01
−1.9240E+01

R4
5.0186E+01
−2.5708E−01
−7.3865E−01
5.3829E+00
−1.4297E+01
2.2599E+01
−1.8661E+01
6.1077E+00

R5
−1.0236E+01
1.6693E−01
−6.5662E−01
1.1850E+00
−1.2115E+00
6.9651E−01
−2.1019E−01
1.9958E−02

R6
−1.1545E+00
8.5232E−01
−1.6828E+00
2.2238E+00
−1.6534E+00
6.9132E−01
−1.5661E−01
1.5138E−02

R7
−2.1781E+02
−3.0640E−01
−8.3950E−02
4.4942E−01
−3.5547E−01
1.3226E−01
−2.4666E−02
1.8588E−03

R8
−5.2225E+00
−3.0017E−01
2.9812E−01
−2.1625E−01
1.0328E−01
−3.0315E−02
4.8819E−03
−3.2744E−04

Table 19 and Table 20 show design data of inflexion points and arrest points of respective lens in the camera optical lens 50 according to Embodiment 5 of the present invention.

TABLE 19

Number of
Inflexion point
Inflexion point
Inflexion point

inflexion points
position 1
position 2
position 3

P1R1
1
0.685
0
0

P1R2
1
0.045
0
0

P2R1
2
0.665
0.705
0

P2R2
1
0.585
0
0

P3R1
1
0.515
0
0

P3R2
2
0.685
1.125
0

P4R1
3
0.195
0.925
1.555

P4R2
1
0.385
0
0

TABLE 20

Number of arrest points
Arrest point position 1

P1R1
0
0

P1R2
1
0.075

P2R1
0
0

P2R2
1
0.755

P3R1
1
0.865

P3R2
0
0

P4R1
1
0.365

P4R2
1
1.095

FIG. 18 and FIG. 19 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 470 nm, 510 nm, 555 nm, 610 nm and 650 nm after passing the camera optical lens 50 according to Embodiment 5. FIG. 20 illustrates field curvature and distortion of light with a wavelength of 555 nm after passing the camera optical lens 50 according to Embodiment 5, 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 21 below further lists various values corresponding to the above conditions according to the present embodiment. The camera optical lens 50 according to the present embodiment satisfies the respective conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens 50 is 1.383 mm. The image height of the camera optical lens 50 is 2.297 mm. The FOV (field of view) along a diagonal direction is 77.00°. Thus, the camera optical lens 50 can provide an ultra-thin, wide-angle lens while having on-axis and off-axis aberrations sufficiently corrected, thereby leading to better optical characteristics.

TABLE 21

Parameters

and
Embodi-
Embodi-
Embodi-
Embodi-
Embodi-

Conditions
ment 1
ment 2
ment 3
ment 4
ment 5

f
2.712
2.808
2.683
2.703
2.822

f1
3.127
2.559
3.121
3.200
2.587

f2
−4.397
−3.693
−4.632
−4.300
−3.756

f3
1.273
1.365
1.321
1.373
1.362

f4
−1.462
−1.329
−1.519
−1.686
−1.364

f12
6.604
5.227
5.960
6.677
5.116

f1/f2
−0.71
−0.69
−0.67
−0.74
−0.69

f4/f2
0.33
0.36
0.33
0.39
0.36

R7/R8
5.28
5.37
5.02
5.96
5.02

d1/d2
1.64
2.84
1.40
1.60
3.20

Fno
2.01
2.04
2.01
2.01
2.04

where 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 invention. 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 invention.

CAMERA OPTICAL LENS

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Inventors

Original Assignees

CPC

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Abstract

Description

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Priority Claims (1)