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 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 three-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 sequentially includes, from an object side to an image side: a first lens having a positive refractive power; a second lens having a negative refractive power; and a third lens having a positive refractive power. The camera optical lens satisfies following conditions: 0.80≤f1/f≤1.10; 0.30≤d3/d5≤1.00; −20.00≤(R5+R6)/(R5−R6)≤−10.00; 5.00≤R2/f≤50.00; and −10.00≤(R3+R4)/(R3−R4)≤−4.00, where f denotes a focal length of the camera optical lens; f1 denotes a focal length of the first lens; R2 denotes a curvature radius of an image side surface of the first lens; R3 denotes a curvature radius of an object side surface of the second lens; R4 denotes a curvature radius of an image side surface of the second 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; d3 denotes an on-axis thickness of the second lens; and d5 denotes an on-axis thickness of the third lens.

As an improvement, the camera optical lens further satisfies a following condition: 2.50≤f3/f≤3.50, where f3 denotes a focal length of the third lens.

As an improvement, the camera optical lens further satisfies a following condition: 0.01≤R1/R2≤0.10, where R1 denotes a curvature radius of an object side surface of the first lens.

As an improvement, the camera optical lens further satisfies a following condition: 1.50≤d1/d2≤3.50, where d1 denotes an on-axis thickness of the first lens; and d2 denotes an on-axis distance from the image side surface of the first lens to the object side surface of the second lens.

As an improvement, the camera optical lens further satisfies following conditions: −2.44≤(R1+R2)/(R1−R2)≤−0.68; and 0.08≤d1/TTL≤0.31, where R1 denotes a curvature radius of an object side surface of the first lens; d1 denotes an on-axis thickness 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: −9.71≤f2/f≤−1.16; and 0.03≤d3/TTL≤0.17, where f2 denotes a focal length 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 a following condition: 0.06≤d5/TTL≤0.33, 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.

As an improvement, the camera optical lens further satisfies a following condition: TTL/IH≤1.62, 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: 0.69≤f12/f≤2.34, where 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 and 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;

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

FIG. 21 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 6 of the present invention;

FIG. 22 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 21;

FIG. 23 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 21; and

FIG. 24 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 21.

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 three 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, and a third lens L3 having a positive refractive power. An optical element such as a glass filter (GF) can be arranged between the third lens L3 and an image plane Si.

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 0.80≤f1/f≤1.10, which specifies a ratio of the focal length of the first lens L1 to the focal length of the camera optical lens 10. This can effectively balance spherical aberrations and a field curvature of the system.

An on-axis thickness of the second lens L2 is defined as d3, and an on-axis thickness of the third lens L3 is defined as d5. The camera optical lens 10 should satisfy a condition of 0.30≤d3/d5≤1.00, which specifies a ratio of the on-axis thickness of the second lens L2 to the on-axis thickness of the third lens L3. When the condition is satisfied, ultra-thin lenses can be facilitated.

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 −20.00≤(R5+R6)/(R5−R6)≤−10.00. If it is outside this range, it would be difficult to correct an off-axis aberration with development towards ultra-thin, wide-angle lenses.

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 5.00≤R2/f≤50.00, which specifies a ratio of the curvature radius of the image side surface of the first lens L1 to the focal length of the camera optical lens 10. This can facilitate improving performance of the system.

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 −10.00≤(R3+R4)/(R3−R4)≤−4.00, which specifies a shape of the second lens L2. This can facilitate correction of an on-axis aberration.

A focal length of the third lens L3 is defined as f3. The camera optical lens 10 should satisfy a condition of 2.50≤f3/f≤3.50, which specifies a ratio of the focal length of the third lens L3 to the focal length of the camera optical lens 10. When the condition is satisfied, the appropriate distribution of the focal length leads to better imaging quality and lower sensitivity of the system.

A curvature radius of an object side surface of the first lens L1 is defined as R1. The camera optical lens 10 should satisfy a condition of 0.01≤R1/R2≤0.10, which specifies a shape of the first lens L1. This can facilitate achieving miniaturization at a high luminous flux state at the aperture.

An on-axis thickness of the first lens L1 is defined as d1, and an on-axis distance from the image side surface of the first lens L1 to the object side surface of the second lens L2 is defined as d2. The camera optical lens 10 should satisfy a condition of 1.50≤d1/d2≤3.50, 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. This can facilitate reducing the total length, thereby achieving ultra-thin lenses.

The curvature radius of the object side surface of the first lens L1 is defined as R1. The camera optical lens 10 should satisfy a condition of −2.44≤(R1+R2)/(R1−R2)≤−0.68. By reasonably controlling the shape of the first lens L1, 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 the on-axis thickness of the first lens L1 is defined as d1. The camera optical lens 10 should satisfy a condition of 0.08≤d1/TTL≤0.31. When the condition is satisfied, ultra-thin lenses can be facilitated.

A focal length of the second lens L2 is defined as f2. The camera optical lens 10 should satisfy a condition of −9.71≤f2/f≤−1.16, 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.

The 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≤0.17. When the condition is satisfied, ultra-thin lenses can be facilitated.

The on-axis thickness of the third lens L3 is defined as d5. The camera optical lens 10 should satisfy a condition of 0.06≤d5/TTL≤0.33. When the condition is satisfied, ultra-thin lenses can be facilitated.

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≤1.62. When the condition is satisfied, ultra-thin lenses can be facilitated.

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 0.69≤f12/f≤2.34. 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 =
−0.060

R1
1.150
d1 =
0.462
nd1
1.5446
ν1
56.04

R2
60.597
d2 =
0.262

R3
−0.872
d3 =
0.275
nd2
1.6614
ν2
20.41

R4
−1.317
d4 =
0.378

R5
1.084
d5 =
0.610
nd3
1.5352
ν3
56.12

R6
1.292
d6 =
0.674

R7
∞
d9 =
0.210
ndg
1.5168
νg
64.17

R8
∞
d10 =
0.126

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 an object side surface of the optical filter GF;

R8: 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 optical filter GF;

d7: on-axis thickness of the optical filter GF;

d8: 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;

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;

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
−1.6761E+01
1.6045E+00
−1.3804E+01
1.1118E+02
−6.1263E+02
1.9807E+03
−3.4017E+03
2.3101E+03

R2
1.1360E+02
−8.8585E−01
9.5547E+00
−1.4087E+02
1.1337E+03
−5.3207E+03
1.3348E+04
−1.3743E+04

R3
2.3177E−01
−1.5510E+00
1.9036E+01
−2.2981E+02
1.7763E+03
−7.5054E+03
1.6743E+04
−1.5548E+04

R4
−9.9335E+00
−1.2056E+00
−2.4897E−01
3.2685E+01
−1.7375E+02
4.9791E+02
−6.9349E+02
3.5020E+02

R5
−8.8580E+00
−2.0187E−01
−1.3561E−01
4.3574E−01
−3.4386E−01
1.0088E−01
−1.8201E−03
−2.4415E−03

R6
−8.6872E−01
−3.9344E−01
9.0666E−02
1.7970E−01
−2.6684E−01
1.6407E−01
−4.9303E−02
5.8234E−03

In Table 2, k is a conic coefficient, and A4, A6, A8, A10, A12, A14, A16, A18 and A20 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; and P3R1 and P3R2 represent the object side surface and the image side surface of the third lens L3, 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 points
position 1

P1R1
1
0.465

P1R2
1
0.045

P2R1
1
0.445

P2R2
1
0.445

P3R1
1
0.375

P3R2
1
0.455

TABLE 4

Number of
Arrest point

arrest points
position 1

P1R1
0
0

P1R2
1
0.075

P2R1
0
0

P2R2
1
0.595

P3R1
1
0.825

P3R2
1
0.915

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 25 below further lists various values of Embodiments 1 to 6 and values corresponding to parameters which are specified in the above conditions.

As shown in Table 25, Embodiment 1 satisfies the respective conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 1.043 mm. The image height of the camera optical lens 10 is 1.851 mm. The FOV (field of view) along a diagonal direction is 76.40°. 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 =
−0.060

R1
1.194
d1 =
0.454
nd1
1.5446
ν1
56.04

R2
45.638
d2 =
0.301

R3
−0.862
d3 =
0.179
nd2
1.6614
ν2
20.41

R4
−1.231
d4 =
0.401

R5
1.041
d5 =
0.580
nd3
1.5352
ν3
56.12

R6
1.272
d6 =
0.606

R7
∞
d9 =
0.210
ndg
1.5168
νg
64.17

R8
∞
d10 =
0.176

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
−3.2659E+01
2.0112E+00
−1.6453E+01
1.1427E+02
−5.9054E+02
1.9429E+03
−3.6362E+03
2.9379E+03

R2
−9.9758E+02
−1.0517E+00
1.1436E+01
−1.5109E+02
1.1634E+03
−5.2836E+03
1.2943E+04
−1.3001E+04

R3
4.0639E−01
−1.9336E+00
2.1040E+01
−2.1873E+02
1.7359E+03
−7.5581E+03
1.7233E+04
−1.6263E+04

R4
−3.7765E−01
−1.1947E+00
2.0170E+00
2.7373E+01
−1.6681E+02
5.5161E+02
−8.8690E+02
4.9788E+02

R5
−6.8258E+00
−1.7452E−01
−1.4712E−01
4.3071E−01
−3.4375E−01
1.0324E−01
−1.0289E−03
−3.2882E−03

R6
−8.6872E−01
−3.5402E−01
5.7117E−02
1.8954E−01
−2.6466E−01
1.6292E−01
−4.9783E−02
5.9886E−03

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
0.455
0

P1R2
1
0.045
0

P2R1
1
0.395
0

P2R2
1
0.405
0

P3R1
2
0.405
1.275

P3R2
1
0.485
0

TABLE 8

Number of
Arrest point

arrest points
position 1

P1R1
0
0

P1R2
1
0.075

P2R1
0
0

P2R2
1
0.555

P3R1
1
0.965

P3R2
1
0.965

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 25 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 1.032 mm. The image height of the camera optical lens 20 is 1.851 mm. The FOV (field of view) along a diagonal direction is 77.40°. 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 =
−0.088

R1
1.013
d1 =
0.482
nd1
1.5446
ν1
56.04

R2
92.873
d2 =
0.262

R3
−0.666
d3 =
0.231
nd2
1.6614
ν2
20.41

R4
−1.011
d4 =
0.328

R5
1.338
d5 =
0.638
nd3
1.5352
ν3
56.12

R6
1.629
d6 =
0.574

R7
∞
d9 =
0.210
ndg
1.5168
νg
64.17

R8
∞
d10 =
0.176

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
−1.1160E+01
1.1736E+00
−9.1032E+00
9.1298E+01
−5.9403E+02
2.0419E+03
−3.3938E+03
1.9340E+03

R2
−9.4134E+02
−9.9280E−01
1.0721E+01
−1.6128E+02
1.1794E+03
−4.6900E+03
9.5919E+03
−7.8596E+03

R3
−4.1413E−01
−5.2655E−01
−7.6669E-01
−1.9175E+01
8.0428E+02
−6.1135E+03
2.0197E+04
−2.5684E+04

R4
−1.1665E+00
−9.9525E−01
5.7388E+00
−3.9064E+00
−1.0704E+02
8.1652E+02
−2.1372E+03
1.8929E+03

R5
−1.8332E+01
−1.7052E−01
−9.5777E−02
3.8448E−01
−3.2520E−01
1.0994E−01
−9.2553E−03
−1.4525E−03

R6
−8.6872E−01
−3.3753E−01
9.4467E−02
1.3692E−01
−2.4207E−01
1.6429E−01
−5.3198E−02
6.6624E−03

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 points
position 1
position 2

P1R1
1
0.455
0

P1R2
1
0.035
0

P2R1
2
0.415
0.475

P2R2
1
0.395
0

P3R1
2
0.345
1.225

P3R2
2
0.435
1.555

TABLE 12

Number of
Arrest point
Arrest point

arrest points
position 1
position 2

P1R1
0
0
0

P1R2
1
0.055
0

P2R1
0
0
0

P2R2
1
0.545
0

P3R1
2
0.795
1.365

P3R2
1
0.845
0

FIG. 10 and FIG. 11 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 30 according to Embodiment 3. FIG. 12 illustrates field curvature and distortion of light with a wavelength of 555 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 25 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 1.050 mm. The image height of the camera optical lens 20 is 1.851 mm. The FOV (field of view) along a diagonal direction is 76.40°. 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 =
−0.067

R1
1.293
d1 =
0.464
nd1
1.5446
ν1
56.04

R2
108.454
d2 =
0.305

R3
−0.913
d3 =
0.158
nd2
1.6614
ν2
20.41

R4
−1.121
d4 =
0.435

R5
1.039
d5 =
0.519
nd3
1.5352
ν3
56.12

R6
1.149
d6 =
0.575

R7
∞
d9 =
0.210
ndg
1.5168
νg
64.17

R8
∞
d10 =
0.176

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
−2.0304E+01
1.2839E+00
−1.2545E+01
1.1071E+02
−6.2417E+02
1.9677E+03
−3.2447E+03
2.2371E+03

R2
−9.9536E+02
−1.1468E+00
1.2730E+01
−1.5264E+02
1.1778E+03
−5.3828E+03
1.2672E+04
−1.1223E+04

R3
6.6734E−01
−2.4032E+00
2.6818E+01
−2.4804E+02
1.7990E+03
−7.2938E+03
1.5786E+04
−1.4817E+04

R4
2.8559E−01
−1.1299E+00
2.5647E+00
2.3713E+01
−1.4198E+02
5.6020E+02
−1.1627E+03
8.6455E+02

R5
−4.8153E+00
−2.7754E−01
−5.5230E−02
3.9195E−01
−3.1926E−01
1.0108E−01
−9.0955E−03
−7.5401E−04

R6
−8.6872E−01
−4.1545E−01
6.1278E−02
2.1070E−01
−2.7059E−01
1.5752E−01
−4.5628E−02
5.1870E−03

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 points
position 1
position 2

P1R1
0
0
0

P1R2
1
0.035
0

P2R1
1
0.375
0

P2R2
1
0.385
0

P3R1
2
0.405
1.365

P3R2
2
0.465
1.615

TABLE 16

Number of
Arrest point

arrest points
position 1

P1R1
0
0

P1R2
1
0.045

P2R1
0
0

P2R2
1
0.535

P3R1
1
1.105

P3R2
1
0.935

FIG. 14 and FIG. 15 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 40 according to Embodiment 4. FIG. 16 illustrates field curvature and distortion of light with a wavelength of 555 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 25 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 0.996 mm. The image height of the camera optical lens 20 is 1.851 mm. The FOV (field of view) along a diagonal direction is 79.00°. 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 =
−0.090

R1
1.153
d1 =
0.496
nd1
1.5446
ν1
56.04

R2
11.663
d2 =
0.323

R3
−0.889
d3 =
0.192
nd2
1.6614
ν2
20.41

R4
−1.280
d4 =
0.328

R5
1.084
d5 =
0.638
nd3
1.5352
ν3
56.12

R6
1.323
d6 =
0.584

R7
∞
d9 =
0.210
ndg
1.5168
νg
64.17

R8
∞
d10 =
0.176

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
−1.7453E+00
4.0842E−01
−8.9399E+00
1.0295E+02
−6.4754E+02
2.2604E+03
−4.1784E+03
3.1972E+03

R2
−9.9996E+02
−8.8944E−01
1.2124E+01
−1.5372E+02
1.1126E+03
−4.7841E+03
1.1270E+04
−1.1101E+04

R3
5.4854E−01
−2.7589E+00
3.1901E+01
−2.5834E+02
1.4282E+03
−4.4336E+03
7.3175E+03
−5.2542E+03

R4
−1.6937E−01
−1.8643E+00
9.3025E+00
−1.0826E+01
−1.1677E+02
7.9707E+02
−1.8339E+03
1.4512E+03

R5
−9.1243E+00
−2.7357E−01
4.5155E−02
3.1679E−01
−3.3337E−01
1.1781E−01
−5.5969E−03
−3.0688E−03

R6
−8.6872E−01
−4.0510E−01
1.2962E−01
1.4289E−01
−2.4949E−01
1.6279E−01
−5.1094E−02
6.2502E−03

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 points
position 1
position 2

P1R1
0
0
0

P1R2
1
0.105
0

P2R1
1
0.415
0

P2R2
1
0.425
0

P3R1
2
0.355
1.225

P3R2
2
0.445
1.555

TABLE 20

Number of
Arrest point
Arrest point

arrest points
position 1
position 2

P1R1
0
0
0

P1R2
1
0.195
0

P2R1
0
0
0

P2R2
1
0.575
0

P3R1
2
0.975
1.355

P3R2
1
0.915
0

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 25 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 1.050 mm. The image height of the camera optical lens 20 is 1.851 mm. The FOV (field of view) along a diagonal direction is 76.40°. 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.

Embodiment 6

Embodiment 6 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1. A structure of a camera optical lens 60 in accordance with Embodiment 6 of the present invention is illustrated in FIG. 21, which only describes differences from Embodiment 1.

Table 21 and Table 22 show design data of a camera optical lens 60 in Embodiment 6 of the present invention.

TABLE 21

R
d
nd
νd

S1
∞
d0 =
−0.094

R1
1.052
d1 =
0.611
nd1
1.5446
ν1
56.04

R2
91.521
d2 =
0.176

R3
−0.795
d3 =
0.333
nd2
1.6614
ν2
20.41

R4
−1.316
d4 =
0.346

R5
0.753
d5 =
0.343
nd3
1.5352
ν3
56.12

R6
0.832
d6 =
0.746

R7
∞
d9 =
0.210
ndg
1.5168
νg
64.17

R8
∞
d10 =
0.176

Table 22 shows aspheric surface data of respective lenses in the camera optical lens 60 according to Embodiment 6 of the present invention.

TABLE 22

Conic

coefficient
Aspherical surface coefficients

k
A4
A6
A8
A10
A12
A14
A16

R1
−4.1325E+01
3.0633E+00
−2.2680E+01
1.0269E+02
−1.2737E+02
−9.4541E+02
4.1630E+03
−5.1254E+03

R2
9.5651E+02
−2.0468E+00
3.3345E+01
−4.6814E+02
3.5831E+03
−1.5712E+04
3.6938E+04
−3.5983E+04

R3
−2.2881E+01
−5.8428E+00
4.1439E+01
−2.6990E+02
1.3266E+03
−4.4448E+03
1.0214E+04
−1.2229E+04

R4
6.4452E−01
−9.1174E−01
−5.0463E−01
5.2621E+01
−3.6372E+02
1.2942E+03
−2.2721E+03
1.5489E+03

R5
−4.4191E+00
−5.0911E−01
3.2927E−01
−1.1683E−02
−2.3267E−02
−5.7405E−02
4.4752E−02
−8.6939E−03

R6
−8.6872E−01
−9.3602E−01
8.0503E−01
−4.7687E−01
9.2224E−02
7.4360E−02
−5.1566E−02
9.3848E−03

Table 23 and Table 24 show design data of inflexion points and arrest points of respective lens in the camera optical lens 60 according to Embodiment 6 of the present invention.

TABLE 23

Number of

inflexion
Inflexion point
Inflexion point

points
position 1
position 2

P1R1
1
0.495
0

P1R2
1
0.025
0

P2R1
0
0
0

P2R2
1
0.435
0

P3R1
2
0.355
1.245

P3R2
2
0.395
1.445

TABLE 24

Number of
Arrest point

arrest points
position 1

P1R1
0
0

P1R2
1
0.035

P2R1
0
0

P2R2
1
0.605

P3R1
1
0.815

P3R2
1
0.855

FIG. 22 and FIG. 23 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 60 according to Embodiment 6. FIG. 24 illustrates field curvature and distortion of light with a wavelength of 555 nm after passing the camera optical lens 60 according to Embodiment 6, 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 25 below further lists various values corresponding to the above conditions according to the present embodiment. The camera optical lens 60 according to the present embodiment satisfies the respective conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens 60 is 1.043 mm. The image height of the camera optical lens 20 is 1.851 mm. The FOV (field of view) along a diagonal direction is 76.60°. Thus, the camera optical lens 60 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 25

Parameters and
Embodi-
Embodi-
Embodi-
Embodi-
Embodi-
Embodi-

Conditions
ment 1
ment 2
ment 3
ment 4
ment 5
ment 6

f
2.294
2.271
2.309
2.191
2.310
2.295

f1
2.140
2.236
1.871
2.391
2.303
1.944

f2
−5.138
−5.347
−4.003
−10.638
−5.424
−4.047

f3
6.201
5.688
7.903
7.636
5.790
5.852

f12
3.506
3.516
3.196
3.081
3.601
3.469

f1/f
0.93
0.98
0.81
1.09
1.00
0.85

d3/d5
0.45
0.31
0.36
0.30
0.30
0.97

(R5 + R6)/
−11.42
−10.01
−10.20
−19.89
−10.07
−19.80

(R5 − R6)

R2/f
26.42
20.10
40.22
49.50
5.05
39.88

(R3 + R4)/
−4.92
−5.67
−4.86
−9.78
−5.55
−4.05

(R3 − R4)

Fno
2.20
2.20
2.20
2.20
2.20
2.20

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

Information

Patent Number

Date Filed

Date Issued

Inventors

Original Assignees

Examiners

Agents

CPC

Field of Search

CPC

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Abstract

Description

Claims

Priority Claims (1)

US Referenced Citations (1)

Related Publications (1)