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 portable terminal devices such as smart phones and digital cameras and camera devices such as monitors or PC lenses.

BACKGROUND

In recent years, with the popularity of smart phones, the demand for a miniaturized camera lens has increased. The photosensitive devices of a conventional camera lens are nothing more than charge coupled devices (CCD) or complementary metal-oxide semiconductor devices (CMOS Sensor). With the advancement of semiconductor manufacturing technology, the pixel size of the photosensitive device has become smaller and smaller, and nowadays electronic products are developing with good functions and thin and small appearance. Therefore, the miniaturized camera lens with good imaging quality has become the mainstream in the current market.

In order to obtain better imaging quality, and with the development of technology and the increase of the diverse demands of users, and as the pixel area of photosensitive devices is becoming smaller and smaller and the requirement of the system on the imaging quality is improving constantly, a three-lens structure gradually appears in lens designs. Although the common three-lens structure already has good optical performance, its settings on refractive power, lens spacing and lens shape still have some irrationality, which results in that the lens structure cannot achieve a high optical performance while satisfying design requirements for ultra-thinness and a wide angle.

SUMMARY

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

In an embodiment, the present invention provides a camera optical lens. The camera optical lens includes a total of three lenses, and the three lenses are 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; and a third lens having a positive refractive power, wherein the camera optical lens satisfies following conditions: 0.65≤f1/f≤0.85; −0.90≤f2/f≤−0.60; 1.00≤f3/f≤1.20; −8.00≤(R5+R6)/(R5−R6)≤−2.50; 2.50≤d5/d4≤4.50; and 1.55≤n2≤1.70, 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; R5 denotes a central curvature radius of an object side surface of the third lens; R6 denotes a central curvature radius of an image side surface of the third lens; d4 denotes an on-axis distance from an image side surface of the second lens to the object side surface of the third lens; d5 denotes an on-axis thickness of the third lens; and n2 denotes a refractive index of the second lens.

In an improved embodiment, 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 an image side surface of the first lens to an object side surface of the second lens.

In an improved embodiment, the camera optical lens further satisfies a following condition: −3.00≤(R3+R4)/(R3−R4)≤−1.50, where R3 denotes a central curvature radius of an object side surface of the second lens, and R4 denotes a central curvature radius of the image side surface of the second lens.

In an improved embodiment, the camera optical lens further satisfies following conditions: −1.72≤(R1+R2)/(R1−R2)≤−0.21; and 0.08≤d1/TTL≤0.44, where R1 denotes a central curvature radius of an object side surface of the first lens, R2 denotes a central curvature radius of an image 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.

In an improved embodiment, the camera optical lens further satisfies a following condition: 0.03≤d3/TTL≤0.19, where 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.

In an improved embodiment, the camera optical lens further satisfies a following condition: 0.07≤d5/TTL≤0.46, 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.

In an improved embodiment, the camera optical lens further satisfies a following condition: TTL/IH≤1.65, IH denotes an image height of the camera optical 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.

In an improved embodiment, a field of view of the camera optical lens is greater than or equal to 70°.

In an improved embodiment, an F number of the camera optical lens is smaller than or equal to 2.51.

In an improved embodiment, the camera optical lens further satisfies a following condition: 1.10≤f12/f≤4.37, where f12 denotes a combined focal length of the first lens and the second lens.

The present invention has at least the following beneficial effects. The cameral optical lens of the present invention has excellent optical performance while having the characteristics of ultra-thinness and a wide angle, and is especially suitable for camera lens assembly of mobile phones and WEB camera lenses formed by imaging elements such as CCD and CMOS for high pixels.

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 structural diagram of a camera optical lens according to 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 structural diagram of a camera optical lens according to 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 structural diagram of a camera optical lens according to 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 structural diagram of a camera optical lens according to 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 structural diagram of a camera optical lens according to 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 structural diagram of a camera optical lens according to 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;

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

FIG. 25 is a schematic structural diagram of a camera optical lens according to Embodiment 7 of the present invention;

FIG. 26 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 25;

FIG. 27 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 25;

FIG. 28 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 25;

FIG. 29 is a schematic structural diagram of a camera optical lens according to Embodiment 8 of the present invention;

FIG. 30 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 29;

FIG. 31 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 29;

FIG. 32 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 29;

FIG. 33 is a schematic structural diagram of a camera optical lens according to Embodiment 9 of the present invention;

FIG. 34 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 33;

FIG. 35 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 33; and

FIG. 36 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 33.

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 figures and the embodiments. It should be understood the specific embodiments described hereby is only to explain the invention, not intended to limit the invention.

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, from an object side to an image side, an aperture S1, a first lens L1, a second lens L2, and a third lens L3. An optical element such as an optical filter (GF) can be arranged between the third lens L3 and an image plane Si.

In this embodiment, the first lens L1 has a positive refractive power, the second lens L2 has a negative refractive power, and the third lens L3 has a positive refractive power.

In this embodiment, the first lens L1 is made of a plastic material, the second lens L2 is made of a plastic material, and the third lens L3 is made of a plastic material. In other embodiments, the lenses can also be made of other materials.

In this embodiment, 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 satisfies a condition of 0.65≤f1/f≤0.85, which specifics a ratio between the focal length of the first lens and the focal length of the camera optical lens. When the condition is satisfied, a spherical aberration and the field curvature of the system can be effectively balanced.

The focal length of the camera optical lens 10 is defined as f, and a focal length of the second lens L2 is defined as f2. The camera optical lens 10 further satisfies a condition: −0.90≤f2/f≤−0.60, which satisfies a ratio of the focal length of the second lens L2 to the focal length of the system. This leads to the more appropriate allocation of the focal length, thereby achieving a better imaging quality and a lower sensitivity of the system.

The focal length of the camera optical lens 10 is defined as f, and a focal length of the third lens L3 is defined as f3. The camera optical lens 10 further satisfies a condition: 1.00≤f3/f≤1.20, which satisfies a ratio of the focal length f3 of the third lens L3 to the focal length f of the system. The appropriate allocation of the refractive power leads to better imaging quality and a lower sensitivity of the system.

A central curvature radius of an object side surface of the third lens L3 is defined as R5, and a central curvature radius of an image side surface of the third lens L3 is defined as R6. The camera optical lens 10 further satisfies a condition: −8.00≤(R5+R6)/(R5−R6)≤−2.50, which specifies a shape of the third lens L3. This condition can facilitate correction of an off-axis aberration.

An on-axis distance from the image side surface of the second lens L2 to the object side surface of the third lens L3 is defined as d4, and an on-axis thickness of the third lens L3 is defined as d5. The camera optical lens 10 further satisfies a condition: 2.50≤d5/d4≤4.50, which specifies a ratio of a thickness of the third lens L3 to an air gap between the second and third lenses. This condition facilitates to compress a total length of the optical system and achieve ultra-thinness.

A refractive index of the second lens L2 is defined as n2. The camera optical lens 10 further satisfies a condition: 1.55≤n2≤1.70, which specifies the refractive index of the second lens L2. This condition facilitates to improve the performance of the optical system.

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 further satisfies a condition: 1.50≤d1/d2≤3.50, which specifies a ratio of a thickness of the first lens L1 to an air gap between the first and second lenses. This condition facilitates to compress the total length of the optical system and achieve ultra-thinness.

A central curvature radius of an object side surface of the second lens L2 is defined as R3, and a central curvature radius of an image side surface of the second lens L2 is defined as R4. The camera optical lens 10 further satisfies a condition: −3.00≤(R3+R4)/(R3−R4)≤−1.50, which specifies a shape of the second lens L2. This can facilitate correction of an on-axis aberration.

In this embodiment, the object side surface of the first lens L1 is convex at a paraxial position, and an image side surface of the first lens L1 is convex at a paraxial position.

A central curvature radius of the object side surface of the first lens L1 is defined as R1, and a central curvature radius of the image side surface of the first lens L1 is defined as R2. The camera optical lens 10 further satisfies a condition: −1.72≤(R1+R2)/(R1−R2)≤−0.21. This condition can reasonably control a shape of the first lens L1 in such a manner that the first lens L1 can effectively correct spherical aberrations of the system. As an example, the camera optical lens further satisfies a condition: −1.08≤(R1+R2)/(R1−R2)≤−0.26.

An on-axis thickness of the first lens L1 is defined as d1, and a total optical length from the object side surface of the first lens L1 to an image plane of the camera optical lens along an optic axis is defined as TTL. The camera optical lens 10 further satisfies a condition: 0.08≤d1/TTL≤0.44. This condition can facilitate achieving ultra-thin lenses. As an example, the camera optical lens further satisfies a condition: 0.13≤d1/TTL≤0.35.

The object side surface of the second lens L2 is concave at a paraxial position and the image side surface of the second lens L2 is convex at a paraxial position.

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 an optic axis is defined as TTL. The camera optical lens 10 further satisfies a condition: 0.03≤d3/TTL≤0.19. This can facilitate achieving ultra-thinness. As an example, the camera optical lens further satisfies a condition: 0.04≤d3/TTL≤0.15.

The object side surface of the third lens L3 is convex at a paraxial position and an image side surface being concave at a paraxial position.

An 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 an optic axis is defined as TTL. The camera optical lens 10 further satisfies a condition: 0.07≤d5/TTL≤0.46. This condition can facilitate achieving ultra-thin lenses. As an example, the camera optical lens further satisfies a condition: 0.12≤d5/TTL≤0.37.

In this embodiment, an image height of the camera optical lens 10 is defined as IH, 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 an optic axis is defined as TTL. The camera optical lens 10 further satisfies a condition: TTL/IH≤1.65. This condition can facilitate achieving ultra-thinness.

In this embodiment, a field of view (FOV) of the camera optical lens 10 is greater than or equal to 70°, thereby achieving a wide angle.

In this embodiment, an F number (FNO) of the camera optical lens 10 is smaller than or equal to 2.51. The camera optical lens 10 has a large aperture and better imaging performance. As an example, the F number (FNO) of the camera optical lens 10 is smaller than or equal to 2.47.

In this embodiment, the focal length of the camera optical lens 10 is defined as f, and a combined focal length of the first lens L1 and the second lens L2 is defined as f12. The camera optical lens 10 further satisfies a condition: 1.10≤f12/f≤4.37. This can eliminate aberration and distortion of the camera optical lens 10, reduce the back focal length of the camera optical lens 10, and maintain miniaturization of the camera lens system group. As an example, the camera optical lens further satisfies a condition: 1.77≤f12/f≤3.50.

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

In the following, examples will be used to describe the camera optical lens 10 of the present invention. The symbols in each example will be described as follows. The focal length, on-axis distance, central curvature radius, on-axis thickness, inflection point position, and stagnation point position are all expressed in unit of mm.

TTL: Total optical length (on-axis distance from the object side surface of the first lens L1 to the image plane of the camera optical lens along the optic axis) in unit of mm.

F number (FNO): a ratio of an effective focal length of the camera optical lens to an entrance pupil diameter of the camera optical lens.

In an example, an inflection point and/or a stagnation point may 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. Specifically, please refer to the following description.

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
vd

S1
∞
d0=
−0.044

R1
1.196
d1=
0.491
nd1
1.5444
v1
55.82

R2
−3.235
d2=
0.261

R3
−0.665
d3=
0.231
nd2
1.6449
v2
22.54

R4
−1.920
d4=
0.210

R5
0.823
d5=
0.793
nd3
1.5444
v3
55.82

R6
1.373
d6=
0.300

R7
∞
d7=
0.210
ndg
1.5168
vg
64.17

R8
∞
d8=
0.372

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

S1: aperture;

R: central curvature radius of an optical surface;

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

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

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

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

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

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

R7: central curvature radius of the object side surface of the optical filter GF;

R8: central curvature radius of the image side surface of the optical filter GF;

d: on-axis thickness of a lens, 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 lenses in the camera optical lens 10 according to Embodiment 1 of the present invention.

TABLE 2

Cone coefficient
Aspherical coefficient

k
A4
A6
A8
A10
A12

R1
4.1202E−01
−5.6227E−02
−1.1051E+01
3.0868E+02
−5.0421E+03
4.8672E+04

R2
−8.1263E−01
−1.0048E+00
−3.6961E+00
1.5157E+02
−2.5252E+03
2.2595E+04

R3
2.4300E−01
−3.3547E+00
3.2317E+01
−7.3646E+01
−1.9985E+03
3.3393E+04

R4
5.1650E+00
−4.3506E+00
3.7175E+01
−2.4653E+02
1.4382E+03
−6.1533E+03

R5
−8.2064E+00
−1.3527E+00
5.2548E+00
−1.5728E+01
3.4951E+01
−5.4439E+01

R6
−5.8478E−01
−6.6133E−01
7.2546E−01
−6.0733E−01
2.0276E−01
1.6103E−01

Cone coefficient
Aspherical coefficient

k
A14
A16
A18
A20

R1
4.1202E−01
−2.8888E+05
1.0400E+06
−2.1030E+06
1.8518E+06

R2
−8.1263E−01
−1.2045E+05
3.8885E+05
−7.0764E+05
5.5780E+05

R3
2.4300E−01
−2.4104E+05
9.4445E+05
−1.9697E+06
1.7240E+06

R4
5.1650E+00
1.8931E+04
−3.9438E+04
4.8373E+04
−2.5831E+04

R5
−8.2064E+00
5.6748E+01
−3.7431E+01
1.4064E+01
−2.2861E+00

R6
−5.8478E−01
−2.3901E−01
1.3050E−01
−3.5193E−02
3.8776E−03

In Table 2, k represents a cone coefficient, and A4, A6, A8, A10, A12, A14, A16, A18 and A20 represent aspherical coefficients.

y=(x²/R)/{1+[1−(k+1)(x²/R²)]^1/2}+A4x⁴+A6x⁶+A8x⁸+A10x¹⁰+A12x¹²+A14x¹⁴+A16x¹⁶+A18x¹⁸+A20x²⁰ (1)

In the equation (1), x represents a vertical distance between a point on an aspherical curve and the optic axis, and y represents an aspherical depth (a vertical distance between a point on an aspherical surface, having a distance of x from the optic axis, and a surface tangent to a vertex of the aspherical surface on the optic axis).

For convenience, an aspheric surface of each lens surface uses the aspheric surfaces shown in the above equation (1). However, the present invention is not limited to the aspherical polynomial form shown in the equation (1).

Table 3 and Table 4 show design data of inflection points and stagnation points of respective lenses 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 named “inflection point position” refers to a vertical distance from an inflection point arranged on each lens surface to the optic axis of the camera optical lens 10. The data in the column named “stagnation point position” refers to a vertical distance from a stagnation point arranged on each lens surface to the optic axis of the camera optical lens 10. The data in the column named “number of inflection points” refers to the number of inflection points set on the surface of each lens. The data in the column named “number of stagnation points” refers to the number of stagnation points set on the surface of each lens.

TABLE 3

Number of
Inflection
Inflection
Inflection

inflection
point
point
point

points
position 1
position 2
position 3

P1R1
2
0.375
0.475
/

P1R2
0
/
/
/

P2R1
1
0.375
/
/

P2R2
1
0.385
/
/

P3R1
3
0.255
1.025
1.095

P3R2
2
0.375
1.485
/

TABLE 4

Number of stagnation points
Stagnation point position 1

P1R1
0
/

P1R2
0
/

P2R1
0
/

P2R2
1
0.535

P3R1
1
0.705

P3R2
1
0.795

FIG. 2 and FIG. 3 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 650 nm, 610 nm, 555 nm, 510 nm, and 470 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 meridian direction.

Table 37 below lists various values and values corresponding to parameters specified in the above conditions for each of Embodiments 1-9.

As shown in Table 37, Embodiment 1 satisfies respective conditions.

In this embodiment, the entrance pupil diameter ENPD of the camera optical lens is 0.886 mm. The full field of view image height IH is 1.750 mm. The field of view (FOV) is 78.00°. Thus, the camera optical lens 10 can achieve ultra-thinness and a wide angle lenses while having on-axis and off-axis aberrations sufficiently corrected, thereby leading to better optical characteristics.

Embodiment 2

Embodiment 2 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences from Embodiment 1 will be described in the following. FIG. 5 shows a camera optical lens 20 according to Embodiment 2 of the present invention.

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

TABLE 5

R
d
nd
vd

S1
∞
d0=
0.049

R1
1.249
d1=
0.434
nd1
1.5444
v1
55.82

R2
−2.382
d2=
0.285

R3
−0.827
d3=
0.291
nd2
1.6449
v2
22.54

R4
−4.008
d4=
0.227

R5
0.661
d5=
0.606
nd3
1.5444
v3
55.82

R6
0.965
d6=
0.300

R7
∞
d7=
0.210
ndg
1.5168
vg
64.17

R8
∞
d8=
0.236

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

Cone coefficient
Aspherical coefficient

k
A4
A6
A8
A10
A12

R1
−5.4441E−01
−2.7306E−01
−6.7196E−01
−3.5562E+00
−1.2227E+02
3.3734E+03

R2
6.4037E−01
−8.2094E−01
−3.1659E+00
8.6780E+01
−1.5487E+03
1.6029E+04

R3
4.2371E−01
−2.0914E+00
2.3161E+01
−2.1530E+02
1.5941E+03
−6.2987E+03

R4
1.5441E+01
−3.4527E+00
2.7527E+01
−1.8527E+02
1.0463E+03
−4.2118E+03

R5
−6.4038E+00
−3.6110E−01
−3.2388E−01
1.6094E+00
−1.4654E+00
−8.6233E−01

R6
−1.0336E+00
−5.5215E−01
1.5216E−01
4.4984E−01
−7.7647E−01
6.4409E−01

Cone coefficient
Aspherical coefficient

k
A14
A16
A18
A20

R1
−5.4441E−01
−4.1472E+04
2.6566E+05
−8.7331E+05
1.1452E+06

R2
6.4037E−01
−1.0045E+05
3.7533E+05
−7.7015E+05
6.6620E+05

R3
4.2371E−01
9.8218E+03
1.1054E+04
−5.8199E+04
5.5822E+04

R4
1.5441E+01
1.1911E+04
−2.2529E+04
2.5261E+04
−1.2566E+04

R5
−6.4038E+00
2.7518E+00
−2.2627E+00
8.4542E−01
−1.2332E−01

R6
−1.0336E+00
−3.2129E−01
9.6717E−02
−1.6020E−02
1.1036E−03

Table 7 and Table 8 show design data of inflection points and stagnation points of respective lenses in the camera optical lens 20 according to Embodiment 2 of the present invention.

TABLE 7

Number of
Inflection
Inflection
Inflection

inflection
point
point
point

points
position 1
position 2
position 3

P1R1
1
0.325
/
/

P1R2
0
/
/
/

P2R1
1
0.405
/
/

P2R2
1
0.405
/
/

P3R1
3
0.325
0.995
1.135

P3R2
1
0.455
/
/

TABLE 8

Number of stagnation points
Stagnation point position 1

P1R1
0
/

P1R2
0
/

P2R1
0
/

P2R2
1
0.555

P3R1
1
0.865

P3R2
1
1.125

FIG. 6 and FIG. 7 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 650 nm, 610 nm, 555 nm, 510 nm, and 470 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.

As shown in Table 37, Embodiment 2 satisfies respective conditions.

In this embodiment, the entrance pupil diameter ENPD of the camera optical lens is 0.775 mm. The full field of view image height IH is 1.750 mm. The field of view (FOV) is 77.00°. Thus, the camera optical lens 20 can achieve ultra-thinness and a wide angle while having on-axis and off-axis aberrations sufficiently corrected, thereby leading to better optical characteristics.

Embodiment 3

Embodiment 3 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences from Embodiment 1 will be described in the following. FIG. 9 shows a camera optical lens 30 according to Embodiment 3 of the present invention.

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

TABLE 9

R
d
nd
vd

S1
∞
d0=
0.026

R1
1.040
d1=
0.482
nd1
1.5444
v1
55.82

R2
−2.083
d2=
0.267

R3
−0.590
d3=
0.229
nd2
1.6860
v2
31.05

R4
−2.071
d4=
0.186

R5
0.656
d5=
0.592
nd3
1.5444
v3
55.82

R6
1.502
d6=
0.300

R7
∞
d7=
0.210
ndg
1.5168
vg
64.17

R8
∞
d8=
0.138

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

Cone coefficient
Aspherical coefficient

k
A4
A6
A8
A10
A12

R1
2.5924E−02
−3.2266E−01
2.1458E−01
−3.3839E+01
2.4403E+02
2.9359E+03

R2
9.7986E+00
−6.7624E−01
−1.7857E+01
4.5551E+02
−7.6121E+03
8.0986E+04

R3
1.1468E−01
−2.7591E+00
3.2334E+01
−4.2309E+02
4.6840E+03
−2.3478E+04

R4
−2.2679E+00
−4.2336E+00
4.0254E+01
−3.8836E+02
3.1806E+03
−1.7750E+04

R5
−9.7471E+00
5.4517E−01
−6.6939E+00
2.5968E+01
−5.8484E+01
8.4467E+01

R6
−6.5132E−01
3.8043E−01
−3.1079E+00
7.0375E+00
−9.0677E+00
7.3174E+00

Cone coefficient
Aspherical coefficient

k
A14
A16
A18
A20

R1
2.5924E−02
−8.3092E+04
7.4057E+05
−3.0745E+06
4.9146E+06

R2
9.7986E+00
−5.4591E+05
2.2567E+06
−5.2224E+06
5.1742E+06

R3
1.1468E−01
2.8920E+04
1.8685E+05
−7.4816E+05
8.0920E+05

R4
−2.2679E+00
6.7647E+04
−1.6897E+05
2.4590E+05
−1.5627E+05

R5
−9.7471E+00
−7.9164E+01
4.6442E+01
−1.5443E+01
2.2137E+00

R6
−6.5132E−01
−3.7438E+00
1.1742E+00
−2.0506E−01
1.5194E−02

Table 11 and Table 12 show design data of inflection points and stagnation points of respective lenses in the camera optical lens 30 according to Embodiment 3 of the present invention.

TABLE 11

Number of
Inflection
Inflection
Inflection

inflection
point
point
point

points
position 1
position 2
position 3

P1R1
1
0.325
/
/

P1R2
0
/
/
/

P2R1
1
0.385
/
/

P2R2
1
0.375
/
/

P3R1
3
0.315
1.025
1.055

P3R2
1
0.455
/
/

TABLE 12

Number of stagnation points
Stagnation point position 1

P1R1
0
/

P1R2
0
/

P2R1
0
/

P2R2
1
0.515

P3R1
1
0.835

P3R2
1
1.035

FIG. 10 and FIG. 11 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 650 nm, 610 nm, 555 nm, 510 nm, and 470 nm after passing the camera optical lens 30 according to Embodiment 3. FIG. 12 illustrates a field curvature and a distortion of light with a wavelength of 555 nm after passing the camera optical lens 30 according to Embodiment 3.

Table 37 below further lists values corresponding to various conditions in the present embodiment according to the above conditions. It can be seen that the camera optical lens according to this embodiment satisfies the above conditions.

In this embodiment, the entrance pupil diameter ENPD of the camera optical lens is 0.693 mm. The full field of view image height IH is 1.750 mm. The field of view (FOV) in a diagonal direction is 76.20°. Thus, the camera optical lens 30 can achieve ultra-thinness and a wide angle 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, and only differences from Embodiment 1 will be described in the following. FIG. 13 shows a camera optical lens 40 according to Embodiment 4 of the present invention.

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

TABLE 13

R
d
nd
vd

S1
∞
d0=
0.009

R1
1.096
d1 =
0.622
nd1
1.5444
v1
55.82

R2
−2.094
d2=
0.248

R3
−0.636
d3=
0.283
nd2
1.6859
v2
31.06

R4
−2.502
d4=
0.223

R5
0.831
d5=
0.812
nd3
1.5444
v3
55.82

R6
1.374
d6=
0.300

R7
∞
d7=
0.210
ndg
1.5168
vg
64.17

R8
∞
d8=
0.159

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

Cone coefficient
Aspherical coefficient

k
A4
A6
A8
A10
A12

R1
2.3019E−01
−1.9026E−01
6.9812E−01
−4.3673E+01
8.4303E+02
−1.0024E+04

R2
7.9269E+00
−7.5905E−01
−2.8194E+00
5.7298E+01
−7.0285E+02
5.3669E+03

R3
1.1935E−01
−2.3124E+00
2.8194E+01
−3.1053E+02
3.0888E+03
−1.8513E+04

R4
3.7735E+00
−3.0086E+00
2.3921E+01
−1.5145E+02
8.1572E+02
−3.0021E+03

R5
−9.5221E+00
−5.1544E−01
6.5558E−01
−4.7479E−01
1.2654E+00
−3.6099E+00

R6
−5.3171E−01
−3.6992E−01
1.1548E−01
8.6571E−02
−8.6016E−02
−2.6646E−03

Cone coefficient
Aspherical coefficient

k
A14
A16
A18
A20

R1
2.3019E−01
7.2745E+04
−3.1772E+05
7.6567E+05
−7.8759E+05

R2
7.9269E+00
−2.5485E+04
7.3251E+04
−1.1716E+05
8.0038E+04

R3
1.1935E−01
6.4927E+04
−1.2733E+05
1.1898E+05
−2.7812E+04

R4
3.7735E+00
7.4243E+03
−1.2231E+04
1.2341E+04
−5.7708E+03

R5
−9.5221E+00
5.0579E+00
−3.7006E+00
1.3822E+00
−2.0927E−01

R6
−5.3171E−01
3.3551E−02
−1.8284E−02
4.2734E−03
−3.8892E−04

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

TABLE 15

Number of
Inflection
Inflection
Inflection

inflection
point
point
point

points
position 1
position 2
position 3

P1R1
1
0.395
/
/

P1R2
0
/
/
/

P2R1
0
/
/
/

P2R2
1
0.395
/
/

P3R1
3
0.305
0.935
1.155

P3R2
1
0.485
/
/

TABLE 16

Number of stagnation points
Stagnation point position 1

P1R1
0
/

P1R2
0
/

P2R1
0
/

P2R2
1
0.555

P3R1
1
1.225

P3R2
1
1.275

FIG. 14 and FIG. 15 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 650 nm, 610 nm, 555 nm, 510 nm, and 470 nm after passing the camera optical lens 40 according to Embodiment 4. FIG. 16 illustrates a field curvature and a distortion of light with a wavelength of 555 nm after passing the camera optical lens 40 according to Embodiment 4.

In this embodiment, the entrance pupil diameter ENPD of the camera optical lens is 0.871 mm. The full field of view image height IH is 1.750 mm. The field of view (FOV) is 70.00°. Thus, the camera optical lens 40 can achieve ultra-thinness and a wide angle 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, and only differences from Embodiment 1 will be described in the following. FIG. 17 shows a camera optical lens 50 according to Embodiment 5 of the present invention.

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

TABLE 17

R
d
nd
vd

S1
∞
d0=
0.002

R1
0.999
d1=
0.417
nd1
1.5444
v1
55.82

R2
−3.800
d2=
0.264

R3
−0.672
d3=
0.162
nd2
1.6860
v2
31.05

R4
−1.984
d4=
0.209

R5
0.757
d5=
0.737
nd3
1.5444
v3
55.82

R6
1.515
d6=
0.300

R7
∞
d7=
0.210
ndg
1.5168
vg
64.17

R8
∞
d8=
0.149

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

Cone coefficient
Aspherical coefficient

k
A4
A6
A8
A10
A12

R1
2.4341E−02
−3.0300E−01
−1.2291E−01
−1.5410E+01
−1.7898E+02
7.5341E+03

R2
4.4637E+01
−7.7321E−01
−1.3284E+01
3.2249E+02
−5.5719E+03
6.0848E+04

R3
4.6652E−01
−1.8986E+00
−3.9518E+01
1.4506E+03
−2.4204E+04
2.5733E+05

R4
−4.7862E+00
−3.3279E+00
−3.9897E+00
4.0355E+02
−5.0006E+03
3.5851E+04

R5
−8.9399E+00
−1.4508E−01
−4.3986E+00
2.6669E+01
−8.6380E+01
1.7683E+02

R6
−4.3118E−01
8.5454E−02
−2.2368E+00
5.8520E+00
−8.6285E+00
7.9180E+00

Cone coefficient
Aspherical coefficient

k
A14
A16
A18
A20

R1
2.4341E−02
−1.0218E+05
6.9448E+05
−2.4292E+06
3.4561E+06

R2
4.4637E+01
−4.1700E+05
1.7448E+06
−4.0799E+06
4.0806E+06

R3
4.6652E−01
−1.6877E+06
6.5879E+06
−1.4071E+07
1.2697E+07

R4
−4.7862E+00
−1.5297E+05
3.7998E+05
−5.0711E+05
2.8006E+05

R5
−8.9399E+00
−2.3185E+02
1.8764E+02
−8.5083E+01
1.6496E+01

R6
−4.3118E−01
−4.5611E+00
1.5960E+00
−3.0902E−01
2.5293E−02

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

TABLE 19

Number of inflection points
Inflection point position 1

P1R1
1
0.335

P1R2
0
/

P2R1
1
0.355

P2R2
1
0.355

P3R1
1
0.285

P3R2
1
0.425

TABLE 20

Number of stagnation points
Stagnation point position 1

P1R1
0
/

P1R2
0
/

P2R1
0
/

P2R2
1
0.475

P3R1
1
0.675

P3R2
1
0.825

FIG. 18 and FIG. 19 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 650 nm, 610 nm, 555 nm, 510 nm, and 470 nm after passing the camera optical lens 50 according to Embodiment 5. FIG. 20 illustrates a field curvature and a distortion of light with a wavelength of 555 nm after passing the camera optical lens 50 according to Embodiment 5.

In this embodiment, the entrance pupil diameter ENPD of the camera optical lens is 0.738 mm. The full field of view image height IH is 1.750 mm. The field of view (FOV) is 78.40°. Thus, the camera optical lens 50 can achieve ultra-thinness and a wide angle 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, and only differences from Embodiment 1 will be described in the following. FIG. 21 shows a camera optical lens 60 according to Embodiment 6 of the present invention.

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

TABLE 21

R
d
nd
vd

S1
∞
d0=
−0.042

R1
1.029
d1=
0.569
nd1
1.5397
v1
55.85

R2
−13.850
d2=
0.318

R3
−0.606
d3=
0.150
nd2
1.6860
v2
31.05

R4
−1.252
d4=
0.308

R5
0.997
d5=
0.818
nd3
1.6634
v3
53.17

R6
1.605
d6=
0.300

R7
∞
d7=
0.210
ndg
1.5168
vg
64.17

R8
∞
d8=
0.206

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

TABLE 22

Cone coefficient
Aspherical coefficient

k
A4
A6
A8
A10
A12

R1
5.8043E−01
1.8396E−01
−1.7481E+01
4.8475E+02
−8.1761E+03
8.5502E+04

R2
8.7483E+01
−7.3970E−01
1.7548E+00
−5.1417E+01
5.1310E+02
−2.6722E+03

R3
7.8665E−02
−1.8913E+00
−3.0111E+01
1.1063E+03
−1.6517E+04
1.5370E+05

R4
1.4949E+00
−1.9798E+00
−2.1215E+01
6.7773E+02
−7.9997E+03
5.6382E+04

R5
−9.7389E+00
−2.2267E−01
−9.3801E−02
1.6564E+00
−3.9078E+00
4.8465E+00

R6
−1.6515E+00
−2.7938E−01
−1.0503E−01
7.8603E−01
−1.2014E+00
1.0283E+00

Cone coefficient
Aspherical coefficient

k
A14
A16
A18
A20

R1
5.8043E−01
−5.6129E+05
2.2485E+06
−5.0211E+06
4.7855E+06

R2
8.7483E+01
4.8903E+03
1.7066E+04
−9.7073E+04
1.3185E+05

R3
7.8665E−02
−8.9186E+05
3.1269E+06
−6.0761E+06
5.0381E+06

R4
1.4949E+00
−2.4502E+05
6.4370E+05
−9.4049E+05
5.8812E+05

R5
−9.7389E+00
−3.6015E+00
1.6105E+00
−4.0003E−01
4.2398E−02

R6
−1.6515E+00
−5.4849E−01
1.7992E−01
−3.3060E−02
2.5911E−03

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

TABLE 23

Number of
Inflection
Inflection
Inflection

inflection
point
point
point

points
position 1
position 2
position 3

P1R1
1
0.445
/
/

P1R2
0
/
/
/

P2R1
1
0.395
/
/

P2R2
1
0.375
/
/

P3R1
3
0.395
0.815
1.265

P3R2
1
0.455
/
/

TABLE 24

Number of stagnation points
Stagnation point position 1

P1R1
0
/

P1R2
0
/

P2R1
0
/

P2R2
1
0.535

P3R1
0
/

P3R2
1
1.245

FIG. 22 and FIG. 23 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 650 nm, 610 nm, 555 nm, 510 nm, and 470 nm after passing the camera optical lens 60 according to Embodiment 6. FIG. 24 illustrates a field curvature and a distortion of light with a wavelength of 555 nm after passing the camera optical lens 60 according to Embodiment 6.

In this embodiment, the entrance pupil diameter ENPD of the camera optical lens is 0.885 mm. The full field of view image height IH is 1.750 mm. The field of view (FOV) is 71.48°. Thus, the camera optical lens 60 can achieve ultra-thinness and a wide angle while having on-axis and off-axis aberrations sufficiently corrected, thereby leading to better optical characteristics.

Embodiment 7

Embodiment 7 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences from Embodiment 1 will be described in the following. FIG. 25 shows a camera optical lens 70 according to Embodiment 7 of the present invention.

Table 25 and Table 26 show design data of the camera optical lens 70 in Embodiment 7 of the present invention.

TABLE 25

R
d
nd
vd

S1
∞
d0=
0.291

R1
1.054
d1=
0.719
nd1
1.5444
v1
55.82

R2
−2.618
d2=
0.207

R3
−0.751
d3=
0.312
nd2
1.6449
v2
22.54

R4
−3.639
d4=
0.147

R5
0.498
d5=
0.369
nd3
1.5444
v3
55.82

R6
0.640
d6=
0.300

R7
∞
d7=
0.210
ndg
1.5168
vg
64.17

R8
∞
d8=
0.205

Table 26 shows aspherical surface data of respective lenses in the camera optical lens 70 according to Embodiment 7 of the present invention.

TABLE 26

Cone coefficient
Aspherical coefficient

k
A4
A6
A8
A10
A12

R1
1.6492E−03
−7.2865E−02
−1.0388E+00
2.3108E+01
−3.2246E+02
2.2955E+03

R2
1.0520E+01
−2.6278E−01
2.5394E−01
−6.4896E+01
1.0850E+03
−9.7168E+03

R3
−7.0612E−02
1.2435E−01
−2.9227E+00
7.4115E+00
2.1787E+02
−2.1975E+03

R4
8.6105E−01
−3.2608E+00
2.7396E+01
−1.9670E+02
1.1164E+03
−4.3927E+03

R5
−5.3717E+00
1.9916E−02
−4.0185E+00
8.1233E+00
1.7151E+01
−1.5591E+02

R6
−1.5681E+00
−7.1261E−01
−7.2927E−01
4.7470E+00
−9.1942E+00
1.0099E+01

Cone coefficient
Aspherical coefficient

k
A14
A16
A18
A20

R1
1.6492E−03
−7.0914E+03
−5.7547E+03
8.9650E+04
−1.5710E+05

R2
1.0520E+01
5.2514E+04
−1.7217E+05
3.1565E+05
−2.4838E+05

R3
−7.0612E−02
1.1733E+04
−4.1050E+04
8.4503E+04
−7.4911E+04

R4
8.6105E−01
1.1675E+04
−2.0034E+04
1.9966E+04
−8.7339E+03

R5
−5.3717E+00
4.8648E+02
−8.4505E+02
7.9277E+02
−3.1269E+02

R6
−1.5681E+00
−6.8943E+00
2.9035E+00
−6.9374E−01
7.2092E−02

Table 27 and Table 28 show design data of inflection points and stagnation points of respective lenses in the camera optical lens 70 according to Embodiment 7 of the present invention.

TABLE 27

Number of inflection points
Inflection point position 1

P1R1
1
0.455

P1R2
0
/

P2R1
0
/

P2R2
1
0.435

P3R1
1
0.295

P3R2
1
0.385

TABLE 28

Number of stagnation points
Stagnation point position 1

P1R1
0
/

P1R2
0
/

P2R1
0
/

P2R2
1
0.605

P3R1
1
0.565

P3R2
1
0.915

FIG. 26 and FIG. 27 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 650 nm, 610 nm, 555 nm, 510 nm, and 470 nm after passing the camera optical lens 70 according to Embodiment 7. FIG. 28 illustrates a field curvature and a distortion of light with a wavelength of 555 nm after passing the camera optical lens 70 according to Embodiment 7.

In this embodiment, the entrance pupil diameter ENPD of the camera optical lens is 0.736 mm. The full field of view image height IH is 1.750 mm. The field of view (FOV) is 71.20°. Thus, the camera optical lens 70 can achieve ultra-thinness and a wide angle while having on-axis and off-axis aberrations sufficiently corrected, thereby leading to better optical characteristics.

Embodiment 8

Embodiment 8 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences from Embodiment 1 will be described in the following. FIG. 29 shows a camera optical lens 80 according to Embodiment 8 of the present invention.

Table 29 and Table 30 show design data of the camera optical lens 80 in Embodiment 8 of the present invention.

TABLE 29

R
d
nd
vd

S1
∞
d0=
−0.050

R1
1.097
d1=
0.632
nd1
1.5405
v1
55.85

R2
−3.420
d2=
0.288

R3
−0.661
d3=
0.184
nd2
1.5603
v2
44.86

R4
−2.457
d4=
0.233

R5
0.778
d5=
0.586
nd3
1.6134
v3
55.86

R6
1.224
d6=
0.300

R7
∞
d7=
0.210
ndg
1.5168
vg
64.17

R8
∞
d8=
0.181

Table 30 shows aspherical surface data of respective lenses in the camera optical lens 80 according to Embodiment 8 of the present invention.

TABLE 30

Cone coefficient
Aspherical coefficient

k
A4
A6
A8
A10
A12

R1
4.6995E−01
−1.8816E−01
6.4441E−01
−4.2098E+01
9.7533E+02
−1.4155E+04

R2
−2.1931E+01
−6.6373E−01
−6.3987E+00
1.3667E+02
−1.9286E+03
1.7193E+04

R3
2.4486E−01
−3.0568E+00
3.4422E+01
−3.0149E+02
1.9846E+03
−2.6038E+03

R4
5.8746E+00
−4.3456E+00
3.7355E+01
−2.4896E+02
1.3390E+03
−4.3658E+03

R5
−8.7446E+00
−2.0035E−01
−5.8822E−01
2.3349E+00
−3.3212E+00
2.0621E+00

R6
−5.2082E−01
−3.9666E−01
−4.8802E−02
5.1212E−01
−5.9032E−01
3.3093E−01

Cone coefficient
Aspherical coefficient

k
A14
A16
A18
A20

R1
4.6995E−01
1.2842E+05
−7.1133E+05
2.1978E+06
−2.9041E+06

R2
−2.1931E+01
−9.6301E+04
3.2862E+05
−6.2504E+05
5.0758E+05

R3
2.4486E−01
−4.5699E+04
2.8843E+05
−6.9726E+05
6.3106E+05

R4
5.8746E+00
7.7474E+03
−6.0372E+03
−3.4781E+02
2.1935E+03

R5
−8.7446E+00
−6.2455E−02
−6.3280E−01
3.2388E−01
−5.2529E−02

R6
−5.2082E−01
−9.5561E−02
9.7262E−03
1.4177E−03
−3.2532E−04

Table 31 and Table 32 show design data of inflection points and stagnation points of respective lenses in the camera optical lens 80 according to Embodiment 8 of the present invention.

TABLE 31

Number of
Inflection
Inflection
Inflection

inflection
point
point
point

points
position 1
position 2
position 3

P1R1
0
/
/
/

P1R2
0
/
/
/

P2R1
0
/
/
/

P2R2
1
0.365
/
/

P3R1
3
0.335
1.025
1.235

P3R2
1
0.475
/
/

TABLE 32

Number of stagnation points
Stagnation point position 1

P1R1
0
/

P1R2
0
/

P2R1
0
/

P2R2
1
0.515

P3R1
1
1.285

P3R2
1
1.255

FIG. 30 and FIG. 31 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 650 nm, 610 nm, 555 nm, 510 nm, and 470 nm after passing the camera optical lens 80 according to Embodiment 8. FIG. 32 illustrates a field curvature and a distortion of light with a wavelength of 555 nm after passing the camera optical lens 80 according to Embodiment 8.

In this embodiment, the entrance pupil diameter ENPD of the camera optical lens is 0.795 mm. The full field of view image height IH is 1.750 mm. The field of view (FOV) is 70.80°. Thus, the camera optical lens 80 can achieve ultra-thinness and a wide angle while having on-axis and off-axis aberrations sufficiently corrected, thereby leading to better optical characteristics.

Embodiment 9

Embodiment 9 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences from Embodiment 1 will be described in the following. FIG. 33 shows a camera optical lens 90 according to Embodiment 9 of the present invention.

Table 33 and Table 34 show design data of the camera optical lens 90 in Embodiment 9 of the present invention.

TABLE 33

R
d
nd
vd

S1
∞
d0=
0.032

R1
1.142
d1=
0.462
nd1
1.5444
v1
55.82

R2
−3.277
d2=
0.304

R3
−0.722
d3=
0.257
nd2
1.6449
v2
22.54

R4
−2.515
d4=
0.184

R5
0.769
d5=
0.822
nd3
1.5444
v3
55.82

R6
1.195
d6=
0.300

R7
∞
d7=
0.210
ndg
1.5168
vg
64.17

R8
∞
d8=
0.149

Table 34 shows aspherical surface data of respective lenses in the camera optical lens 90 according to Embodiment 9 of the present invention.

TABLE 34

Cone coefficient
Aspherical coefficient

k
A4
A6
A8
A10
A12

R1
−3.1035E−03
−1.9625E−01
−1.6911E+00
3.1075E+01
−6.4128E+02
7.7405E+03

R2
1.2177E+01
−7.3386E−01
−6.3273E−01
6.1439E+00
−1.9727E+02
2.4209E+03

R3
3.1473E−01
−2.0873E+00
2.2366E+01
−2.0744E+02
1.5417E+03
−5.2233E+03

R4
7.9415E+00
−3.6511E+00
2.7135E+01
−1.6139E+02
8.0562E+02
−2.7955E+03

R5
−9.1341E+00
−7.6838E−01
1.4834E+00
−1.6973E+00
1.6964E+00
−1.9810E+00

R6
−1.0371E+00
−4.4861E−01
1.1245E−01
4.5393E−01
−8.4913E−01
7.8323E−01

Cone coefficient
Aspherical coefficient

k
A14
A16
A18
A20

R1
−3.1035E−03
−5.8438E+04
2.6480E+05
−6.6051E+05
6.8673E+05

R2
1.2177E+01
−1.6585E+04
6.6328E+04
−1.4550E+05
1.3409E+05

R3
3.1473E−01
6.3392E+02
4.7028E+04
−1.2465E+05
1.0237E+05

R4
7.9415E+00
7.0700E+03
−1.3195E+04
1.5928E+04
−8.8820E+03

R5
−9.1341E+00
2.0021E+00
−1.2565E+00
4.1574E−01
−5.5562E−02

R6
−1.0371E+00
−4.3075E−01
1.4116E−01
−2.5305E−02
1.9023E−03

Table 35 and Table 36 show design data of inflection points and stagnation points of respective lenses in the camera optical lens 90 according to Embodiment 9 of the present invention.

TABLE 35

Number of
Inflection
Inflection
Inflection
Inflection
Inflection

inflection
point
point
point
point
point

points
position 1
position 2
position 3
position 4
position 5

P1R1
1
0.365
/
/
/
/

P1R2
0
/
/
/
/
/

P2R1
1
0.425
/
/
/
/

P2R2
1
0.405
/
/
/
/

P3R1
5
0.275
0.835
1.145
1.275
1.305

P3R2
1
0.455
/
/
/
/

TABLE 36

Number of stagnation points
Stagnation point position 1

P1R1
0
/

P1R2
0
/

P2R1
0
/

P2R2
1
0.555

P3R1
0
/

P3R2
1
1.155

FIG. 34 and FIG. 35 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 650 nm, 610 nm, 555 nm, 510 nm, and 470 nm after passing the camera optical lens 90 according to Embodiment 9. FIG. 36 illustrates a field curvature and a distortion of light with a wavelength of 555 nm after passing the camera optical lens 90 according to Embodiment 9.

In this embodiment, the entrance pupil diameter ENPD of the camera optical lens is 0.810 mm. The full field of view image height IH is 1.750 mm. The field of view (FOV) is 76.40°. Thus, the camera optical lens 90 can achieve ultra-thinness and a wide angle while having on-axis and off-axis aberrations sufficiently corrected, thereby leading to better optical characteristics.

TABLE 37

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

Conditions
ment 1
ment 2
ment 3
ment 4
ment 5
ment 6
ment 7
ment 8
ment 9

f1/f
0.77
0.83
0.79
0.67
0.83
0.83
0.82
0.83
0.82

f2/f
−0.78
−0.88
−0.76
−0.62
−0.86
−0.87
−0.85
−0.86
−0.84

f3/f
1.15
1.19
1.01
1.19
1.15
1.19
1.19
1.19
1.19

(R5 + R6)/
−3.99
−5.35
−2.55
−4.06
−3.00
−4.28
−7.97
−4.49
−4.61

(R5 − R6)

d5/d4
3.78
2.67
3.18
3.64
3.53
2.66
2.51
2.52
4.47

n2
1.65
1.65
1.69
1.69
1.69
1.69
1.65
1.56
1.65

f
2.162
1.892
1.692
2.125
1.800
2.160
1.796
1.941
1.976

f1
1.664
1.566
1.343
1.415
1.494
1.793
1.478
1.611
1.610

f2
−1.687
−1.664
−1.277
−1.319
−1.552
−1.882
−1.520
−1.668
−1.651

f3
2.491
2.251
1.709
2.521
2.061
2.570
2.137
2.309
2.351

f12
6.301
4.938
4.728
4.981
4.729
5.089
4.062
4.289
5.217

FNO
2.44
2.44
2.44
2.44
2.44
2.44
2.44
2.44
2.44

TTL
2.868
2.589
2.404
2.857
2.448
2.879
2.469
2.614
2.688

IH
1.750
1.750
1.750
1.750
1.750
1.750
1.750
1.750
1.750

FOV
78.00°
77.00°
76.20°
70.00°
78.40°
71.48°
71.20°
70.80°
76.40°

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 scope of the present invention.

CAMERA OPTICAL LENS

Information

Publication Number

Date Filed

Date Published

Inventors

Original Assignees

CPC

International Classifications

Abstract

Description

Claims

Priority Claims (1)