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, a four-piece lens structure gradually emerges in lens designs. 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 having large apertures.

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 having large apertures.

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: 2.00≤(f1+f3)/f≤2.30; −8.60≤(f2+f4)/f≤−4.80; −2.10≤(R1+R2)/(R1−R2)≤−1.90; −4.00≤(R3+R4)/(R3−R4)≤−1.00; and 2.00≤(R7+R8)/(R7−R8)≤3.40, where f denotes a focal length of the camera optical lens; f1 denotes a focal length of the first lens; f2 denotes a focal length of the second lens; f3 denotes a focal length of the third lens; f4 denotes a focal length of the fourth lens; R1 denotes a curvature radius of an object side surface 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; R7 denotes a curvature radius of an object side surface of the fourth lens; and R8 denotes a curvature radius of the image side surface of the fourth lens.

As an improvement, the camera optical lens further satisfies a following condition: 0.70≤d3/d2≤0.85, where d2 denotes an on-axis distance from the image side surface of the first lens to the object side surface of the second lens; and d3 denotes an on-axis thickness of the second lens.

As an improvement, the camera optical lens further satisfies following conditions: 0.54≤f1/f≤1.74; and 0.06≤d1/TTL≤0.23, where 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: −14.72≤f2/f≤−2.47; and 0.03≤d3/TTL≤0.11, where d3 denotes an on-axis thickness of the second 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: 0.45≤f3/f≤1.76; 1.36≤(R5+R6)/(R5−R6)≤4.51; and 0.07≤d5/TTL≤0.23, where 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 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: −2.58≤f4/f≤−0.65; and 0.04≤d7/TTL≤0.18, where d7 denotes an on-axis thickness of the fourth 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 a following condition: TTL/IH≤1.37, where 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; and IH denotes an image height of the camera optical lens.

As an improvement, the camera optical lens further satisfies a following condition: FOV≥80.00, where FOV denotes a field of view of the camera optical lens.

As an improvement, the camera optical lens further satisfies a following condition: Fno≤2.27, where Fno denotes an F number of the camera optical lens.

As an improvement, the camera optical lens further satisfies a following condition: 0.64≤f12/f≤2.08, 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, is ultra-thin, wide-angle and has large apertures, 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; 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 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 camera optical lens 10 is defined as f, a focal length of the first lens L1 is defined as f1, and a focal length of the third lens L3 is defined as f3. The camera optical lens 10 should satisfy a condition of 2.00≤(f1+f3)/f≤2.30, which specifies a ratio of a sum of the focal length of the first lens L1 and the focal length of the third lens L3 to the focal length of the camera optical lens 10. This can effectively balance spherical aberrations caused by the first lens L1 and a field curvature of the system.

A focal length of the second lens L2 is defined as f2, a 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 −8.60≤(f2+f4)/f≤−4.80, which specifies a ratio of a sum of the focal length of the second lens L2 and the focal length of the fourth lens L4 to the focal length of the camera optical lens 10. 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 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 −2.10≤(R1+R2)/(R1−R2)≤−1.90, which specifies a shape of the first lens L1. This can facilitate correction of an on-axis aberration.

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 −4.00≤(R3+R4)/(R3−R4)≤−1.00, which specifies a shape of the second lens L2. This can facilitate shaping of the second lens L2 and avoiding bad shaping and generation of stress due to the overly large surface curvature.

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 2.00≤(R7+R8)/(R7−R8)≤3.40, which specifies a shape of the fourth lens L4. This can facilitate correction of an off-axis aberration.

An on-axis thickness of the second lens L2 is defined as d3, 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 0.70≤d3/d2≤0.85, which specifies a ratio of the thickness of the second lens to an air gap between the first lens L1 and the second lens L2. When the condition is satisfied, reduction of the total length can be facilitated, thereby achieving ultra-thin lenses.

The 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 0.54≤f1/f≤1.74, which specifies a ratio of the refractive power of the first lens L1 to the focal length of the camera optical lens 10. When the condition is satisfied, the first lens L1 has an appropriate positive refractive power, thereby facilitating reducing aberrations of the system while facilitating development towards ultra-thin, wide-angle lenses.

A total optical length from an 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 0.06≤d1/TTL≤0.23. When the condition is satisfied, ultra-thin lenses can be achieved.

The focal length of the second lens L2 is defined as f2, the focal length of the camera optical lens 10 is defined as f. The camera optical lens 10 should satisfy a condition of −14.72≤f2/f≤−2.47, 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.

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≤0.11. When the condition is satisfied, ultra-thin lenses can be achieved.

The focal length of the third lens L3 is defined as f3. The camera optical lens 10 should satisfy a condition of 0.45≤f3/f≤1.76. The appropriate distribution of the refractive power leads to better imaging quality and a lower sensitivity.

The 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 1.36≤(R5+R6)/(R5−R6)≤4.51, which specifies a shape of the third lens L3. This can alleviate the deflection of light passing through the lens, thereby effectively reducing aberrations.

The on-axis thickness of the third lens L3 is defined as d5. The camera optical lens 10 should satisfy a condition of 0.07≤d5/TTL≤0.23. 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 −2.58≤f4/f≤−0.65. The appropriate distribution of the refractive power leads to better imaging quality, thereby facilitating improving performance of the optical system.

The on-axis thickness of the fourth lens L4 is defined as d7. The camera optical lens 10 should satisfy a condition of 0.04≤d7/TTL≤0.18. 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 10 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≤1.37. When the condition is satisfied, ultra-thin lenses can be achieved.

A field of view along a diagonal direction of the camera optical lens 10 is defined as FOV. The camera optical lens 10 should satisfy a condition of FOV≥80.00. When the condition is satisfied, wide-angle lenses can be achieved.

An F number of the camera optical lens 10 is defined as Fno. The camera optical lens 10 should satisfy a condition of Fno≤2.27. When the condition is satisfied, lenses having large apertures and high imaging performance 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 0.64≤f12/f≤2.08. 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 having large apertures. 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=
−0.170

R1
1.062
d1=
0.449
nd1
1.5444
ν1
55.82

R2
3.029
d2=
0.285

R3
−5.964
d3=
0.232
nd2
1.6610
ν2
20.53

R4
−106.385
d4=
0.140

R5
−2.043
d5=
0.453
nd3
1.5444
ν3
55.82

R6
−0.981
d6=
0.379

R7
1.284
d7=
0.308
nd4
1.5444
ν4
55.82

R8
0.686
d8=
0.498

R9
∞
d9=
0.110
nd5
1.5168
ν5
64.17

R10
∞
d10=
0.294

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
−7.9461E+00
7.8540E−01
−1.3971E+00
1.7221E+00
5.6911E+00
−3.4655E+01
7.3425E+01
−6.1863E+01

R2
6.4600E+00
−7.0205E−02
−3.3203E−01
1.6866E+00
−1.4256E+01
4.7610E+01
−8.3749E+01
5.0389E+01

R3
7.3396E+01
−4.8255E−01
2.4210E−01
−6.8479E+00
3.8148E+01
−1.3596E+02
2.7557E+02
−2.2391E+02

R4
−3.4998E+02
−1.8818E−01
−4.6969E−01
3.2073E+00
−1.4984E+01
3.8529E+01
−4.7019E+01
2.5437E+01

R5
−2.0810E+00
1.0558E−01
−9.6656E−01
6.8868E+00
−2.0854E+01
3.3888E+01
−2.8692E+01
9.8379E+00

R6
−6.8454E−01
−2.4080E−01
1.4342E+00
−4.4039E+00
1.0248E+01
−1.2116E+01
6.7669E+00
−1.4477E+00

R7
−1.5426E+01
−7.5518E−01
9.4451E−01
−7.3073E−01
3.6154E−01
−1.0655E−01
1.6814E−02
−1.0832E−03

R8
−5.2513E+00
−3.9139E−01
4.0458E−01
−2.8943E−01
1.3161E−01
−3.6792E−02
5.5507E−03
−3.2984E−04

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
Inflexion
Inflexion

inflexion
point
point
point

points
position 1
position 2
position 3

P1R1
1
0.635
0
0

P1R2
1
0.405
0
0

P2R1
0
0
0
0

P2R2
1
0.605
0
0

P3R1
3
0.505
0.815
0.855

P3R2
2
0.605
0.945
0

P4R1
2
0.245
1.125
0

P4R2
2
0.375
1.735
0

TABLE 4

Number of
Arrest
Arrest

arrest
point
point

points
position 1
position 2

P1R1
0
0
0

P1R2
1
0.555
0

P2R1
0
0
0

P2R2
1
0.695
0

P3R1
1
0.905
0

P3R2
0
0
0

P4R1
2
0.475
1.665

P4R2
1
0.945
0

FIG. 2 and FIG. 3 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 486 nm, 588 and 656 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 588 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 the respective conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens 10 is 1.243 mm. The image height of the camera optical lens 10 is 2.300 mm. The FOV (field of view) along a diagonal direction is 82.80°. Thus, the camera optical lens 10 can provide an ultra-thin, wide-angle lens with large apertures 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=
−0.150

R1
1.078
d1=
0.470
nd1
1.5444
ν1
55.82

R2
3.192
d2=
0.286

R3
−6.006
d3=
0.226
nd2
1.6610
ν2
20.53

R4
−16.016
d4=
0.139

R5
−2.003
d5=
0.472
nd3
1.5444
ν3
55.82

R6
−0.924
d6=
0.330

R7
1.531
d7=
0.278
nd4
1.5444
ν4
55.82

R8
0.703
d8=
0.507

R9
∞
d9=
0.110
nd5
1.5168
ν5
64.17

R10
∞
d10=
0.307

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
−7.8481E+00
7.8001E−01
−1.4237E+00
1.6585E+00
5.6533E+00
−3.4450E+01
7.3967E+01
−6.2849E+01

R2
6.5977E+00
−6.6046E−02
−3.4297E−01
1.6795E+00
−1.4411E+01
4.7156E+01
−8.3837E+01
5.4591E+01

R3
6.6292E+01
−4.6386E−01
2.2484E−01
−7.0369E+00
3.7612E+01
−1.3644E+02
2.7679E+02
−2.1696E+02

R4
−1.5880E+04
−1.9137E−01
−4.8321E−01
3.1836E+00
−1.5020E+01
3.8493E+01
−4.6973E+01
2.5774E+01

R5
−1.9213E+00
1.0384E−01
−9.5723E−01
6.8998E+00
−2.0852E+01
3.3866E+01
−2.8720E+01
9.8202E+00

R6
−7.3864E−01
−2.2055E−01
1.4369E+00
−4.4031E+00
1.0249E+01
−1.2116E+01
6.7657E+00
−1.4508E+00

R7
−2.3454E+01
−7.5081E−01
9.4582E−01
−7.3063E−01
3.6148E−01
−1.0659E−01
1.6802E−02
−1.0874E−03

R8
−5.8923E+00
−3.9019E−01
4.0378E−01
−2.8941E−01
1.3162E−01
−3.6797E−02
5.5488E−03
−3.3021E−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
Inflexion
Inflexion

inflexion
point
point
point

points
position 1
position 2
position 3

P1R1
1
0.635
0
0

P1R2
1
0.395
0
0

P2R1
0
0
0
0

P2R2
1
0.615
0
0

P3R1
3
0.505
0.775
0.895

P3R2
2
0.595
0.945
0

P4R1
3
0.225
1.095
1.545

P4R2
2
0.355
1.755
0

TABLE 8

Number of
Arrest

arrest
point

points
position 1

P1R1
0
0

P1R2
1
0.545

P2R1
0
0

P2R2
1
0.705

P3R1
1
0.945

P3R2
0
0

P4R1
1
0.425

P4R2
1
0.905

FIG. 6 and FIG. 7 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 486 nm, 588 nm and 656 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 588 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 13 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 1.233 mm. The image height of the camera optical lens 20 is 2.300 mm. The FOV (field of view) along a diagonal direction is 80.00°. Thus, the camera optical lens 20 can provide an ultra-thin, wide-angle lens with large apertures 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=
−0.070

R1
1.043
d1=
0.386
nd1
1.5450
ν1
55.81

R2
3.237
d2=
0.278

R3
−5.011
d3=
0.208
nd2
1.6610
ν2
20.53

R4
−9.194
d4=
0.158

R5
−1.388
d5=
0.452
nd3
1.5450
ν3
55.81

R6
−0.695
d6=
0.176

R7
1.953
d7=
0.359
nd4
1.5346
ν4
55.69

R8
0.695
d8=
0.500

R9
∞
d9=
0.210
nd5
1.5168
ν5
64.17

R10
∞
d10=
0.252

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
−1.6424E+00
1.4349E−01
1.3022E+00
−1.9135E+01
1.4704E+02
−6.3511E+02
1.4343E+03
−1.3483E+03

R2
8.4847E+00
−1.6248E−01
1.1653E−01
−7.3054E+00
4.4225E+01
−1.8365E+02
3.7857E+02
−3.3071E+02

R3
5.6303E+01
−5.8643E−01
7.2294E−01
−2.2334E+01
1.6316E+02
−6.9615E+02
1.5649E+03
−1.3513E+03

R4
−9.8101E+01
−2.3761E−01
1.4745E−01
−4.5327E+00
2.2375E+01
−6.6302E+01
1.2103E+02
−7.8862E+01

R5
−8.6743E+00
−1.6625E−02
−1.1224E−01
4.4573E+00
−2.2365E+01
4.9426E+01
−5.1450E+01
2.0547E+01

R6
−3.6804E+00
−7.2917E−01
2.4956E+00
−6.6722E+00
1.3863E+01
−1.6011E+01
9.1065E+00
−2.0294E+00

R7
−4.7819E+01
−3.4129E−01
2.7620E−01
−2.5786E−01
2.4355E−01
−1.2841E−01
3.3040E−02
−3.3135E−03

R8
−5.6885E+00
−2.7603E−01
2.6227E−01
−2.1995E−01
1.2299E−01
−4.3413E−02
8.6529E−03
−7.2361E−04

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
Inflexion
Inflexion

inflexion
point
point
point

points
position 1
position 2
position 3

P1R1
1
0.535
0
0

P1R2
1
0.325
0
0

P2R1
0
0
0
0

P2R2
1
0.565
0
0

P3R1
1
0.575
0
0

P3R2
2
0.575
0.915
0

P4R1
3
0.255
1.015
1.575

P4R2
3
0.395
1.615
1.765

TABLE 12

Number of
Arrest
Arrest
Arrest

arrest
point
point
point

points
position 1
position 2
position 3

P1R1
0
0
0
0

P1R2
1
0.465
0
0

P2R1
0
0
0
0

P2R2
1
0.655
0
0

P3R1
0
0
0
0

P3R2
0
0
0
0

P4R1
3
0.495
1.465
1.625

P4R2
1
0.965
0
0

FIG. 10 and FIG. 11 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 486 nm, 588 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 588 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 13 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 1.041 mm. The image height of the camera optical lens 20 is 2.297 mm. The FOV (field of view) along a diagonal direction is 88.40°. Thus, the camera optical lens 30 can provide an ultra-thin, wide-angle lens with large apertures 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

f
2.560
2.540
2.290

f1
2.772
2.774
2.649

f2
−9.484
−14.667
−16.853

f3
3.000
2.732
2.066

f4
−3.300
−2.705
−2.237

f12
3.551
3.250
3.043

Fno
2.06
2.06
2.20

(f1 + f3)/f
2.25
2.17
2.06

(f2 + f4)/f
−4.99
−6.84
−8.34

(R1 + R2)/(R1 − R2)
−2.08
−2.02
−1.95

(R3 + R4)/(R3 − R4)
−1.12
−2.20
−3.40

(R7 + R8)/(R7 − R8)
3.29
2.70
2.10

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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