Camera optical lens

Abstract

The present disclosure provides a camera optical lens. The camera optical lens includes, from an object side to an image side: an aperture; a first lens having a positive refractive power; a second lens having a negative refractive power; a third lens having a positive refractive power; a fourth lens having a negative refractive power; a fifth lens having a positive refractive power; a sixth lens having a negative refractive power; and a seventh lens having a negative refractive power. The camera optical lens satisfies following conditions: 9.00≤f3/f≤30.00; and 2.90≤v1/v2≤5.00, where f denotes a focal length of the camera optical lens; f3 denotes a focal length of the third lens; v1 denotes an abbe number of the first lens; and v2 denotes an abbe number of the second lens.

Description

TECHNICAL FIELD

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

BACKGROUND

With the emergence of smart phones in recent years, the demand for miniature camera lens is increasing day by day, but in general the photosensitive devices of camera lens are nothing more than Charge Coupled Device (CCD) or Complementary Metal-Oxide Semiconductor Sensor (CMOS sensor), and as the progress of the semiconductor manufacturing technology makes the pixel size of the photosensitive devices become smaller, plus the current development trend of electronic products towards better functions and thinner and smaller dimensions, miniature camera lenses with good imaging quality therefore have become a mainstream in the market.

In order to obtain better imaging quality, the lens that is traditionally equipped in mobile phone cameras adopts a three-piece or four-piece lens structure, or even five-piece or six 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 improving constantly, a seven-piece lens structure gradually appears in lens designs. Although the common seven-piece lens has good optical performance, its settings on refractive power, lens spacing and lens shape still have some irrationality, which results in that the lens structure cannot achieve a high optical performance while satisfying design requirements of ultra-thin lenses having a big aperture.

BRIEF DESCRIPTION OF DRAWINGS

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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; and

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

DESCRIPTION OF EMBODIMENTS

The present disclosure will hereinafter be described in detail with reference to several exemplary embodiments. To make the technical problems to be solved, technical solutions and beneficial effects of the present disclosure more apparent, the present disclosure is described in further detail together with the figure and the embodiments. It should be understood the specific embodiments described hereby is only to explain the disclosure, not intended to limit the disclosure.

Embodiment 1

Referring to FIG. 1, the present disclosure provides a camera optical lens 10. FIG. 1 shows the camera optical lens 10 according to Embodiment 1 of the present disclosure. The camera optical lens 10 includes 7 lenses. Specifically, the camera optical lens 10 includes, from an object side to an image side, an aperture S1, a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6 and a seventh lens L7. In this embodiment, preferably, an optical element such as a glass plate GF can be arranged between the seventh lens L7 and an image plane Si. The glass plate GF can be a glass cover plate or an optical filter. In other embodiments, the glass plate GF can also be arranged at other positions.

In this embodiment, the first lens L1 has a positive refractive power, and has an object side surface being a convex surface and an image side surface being a concave surface; the second lens L2 has a negative refractive power, and has an object side surface being a convex surface and an image side surface being a concave surface; the third lens L3 has a positive refractive power, and has an object side surface being a concave surface and an image side surface being a convex surface; the fourth lens L4 has a negative refractive power, and has an object side surface being a convex surface and an image side surface being a concave surface; the fifth lens L5 has a positive refractive power, and has an object side surface being a concave surface and an image side surface being a convex surface; the sixth lens L6 has a negative refractive power, and has an object side surface being a concave surface and an image side surface being a concave surface; and the seventh lens L7 has a negative refractive power, and has an object side surface being a concave surface and an image side surface being a concave surface.

Here, a focal length of the camera optical lens 10 is defined as f in a unit of millimeter (mm), a focal length of the third lens L3 is defined as f3, an abbe number of the first lens L1 is defined as v1, and an abbe number of the second lens L2 is defined as v2. The camera optical lens 10 should satisfy satisfies following conditions:9.00≤f3/f≤30.00  (1); and2.90≤v1/v2≤5.00  (2).

The condition (1) specifies a ratio of the focal length of the third lens L3 and the focal length of the camera optical lens 10. This leads to the appropriate distribution of the refractive power for the third lens L3, such that the field curvature of the system can be effectively balanced for further improving the imaging quality.

The condition (2) specifies a ratio of the abbe number v1 of the first lens L1 and the abbe number v2 of the second lens L2. This facilitates development towards ultra-thin lenses with a big aperture, and also facilitates correction of aberrations.

In this embodiment, with the above configurations of the lenses, the camera optical lens can achieve a high optical performance while satisfying design requirements for ultra-thin lenses having a big aperture.

In an example, a focal length of the second lens L2 is defined as f2. The camera optical lens 10 further satisfies a condition of:−5.00≤f2/f≤−3.00  (3).

The condition (3) specifies a ratio of the focal length of the second lens L2 and the focal length of the camera optical lens 10. This can effectively balance a spherical aberration caused by the first lens and the field curvature of the system.

In an example, an on-axis thickness of the second lens L2 is defined as d3, an on-axis thickness of the third lens L3 is defined as d5, and a 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 of:0≤(d3+d5)/TTL≤0.10  (4).

The condition (4) specifies a ratio of a sum of the on-axis thicknesses of the second lens L2 and the third lens L3 and the TTL. This can facilitate improving the image quality while achieving ultra-thin lenses.

In an example, a curvature radius of the object side surface of the third lens L3 is defined as R5, and a curvature radius of the image side surface of the third lens L3 is defined as R6. The camera optical lens 10 further satisfies a condition of:4.00≤(R5+R6)/(R5−R6)≤11.00  (5).

The condition (5) specifies a shape of the third lens L3. This can facilitate shaping of the third lens L3 and avoid bad shaping and generation of stress due to the overly large surface curvature of the third lens L3.

In an example, a curvature radius of the object side surface of the fourth lens L4 is defined as R7, and a curvature radius of the image side surface of the fourth lens L4 is defined as R8. The camera optical lens 10 further satisfies a condition of:5.00≤(R7+R8)/(R7−R8)≤20.00  (6).

The condition (6) specifies a shape of the third lens L4. This can facilitate correcting an off-axis aberration.

In this embodiment, the first lens L1 is made of a glass material, and thus the first lens L1 has a good performance in terms of temperature and humidity reliability and has a large Abbe number, thereby effectively correcting a chromatic aberration while improving the optical performance of the camera optical lens. In this embodiment, each of the second lens L2, the third lens L3, the fourth lens L4, the fifth lens L5, the sixth lens L6 and the seventh lens L7 is made of a plastic material. This can effectively reduce production costs.

In addition, a surface of a lens can be set as an aspherical surface. The aspherical surface can be easily formed into a shape other than the spherical surface, so that more control variables can be obtained to reduce the aberration, thereby reducing the number of lenses and thus effectively reducing a total length of the camera optical lens according to the present disclosure. In an embodiment of the present disclosure, both an object side surface and an image side surface of each lens are aspherical surfaces.

It should be noted that the first lens L1, the second lens L2, the third lens L3, the fourth lens L4, the fifth lens L5, the sixth lens L6 and the seventh lens L7 that constitute the camera optical lens 10 of the present embodiment have the structure and parameter relationships as described above, and therefore, the camera optical lens 10 can reasonably distribute the refractive power, the surface shape, the material, the on-axis thickness and the like of each lens, and thus correct various aberrations. The camera optical lens 10 has Fno≤1.45. TTL and an image height (IH) of the camera optical lens 10 satisfy a condition of TTL/IH≤1.48. The field of view (FOV) of the camera optical lens 10 satisfies FOV≥76 degrees. This can achieve a high optical performance while satisfying design requirements for ultra-thin lenses having a big aperture.

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.

The design information of the camera optical lens 10 in Embodiment 1 of the present disclosure is shown in the following. It should be noted that each of the distance, radii and the thickness is in a unit of millimeter (mm).

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

	TABLE 1
	R	d	nd	νd
S1	∞	d0=	−0.634
R1	1.987	d1=	1.158	nd1	1.5378	ν1	74.70
R2	10.351	d2=	0.041
R3	9.233	d3=	0.222	nd2	1.6610	ν2	20.53
R4	4.849	d4=	0.489
R5	−18.701	d5=	0.221	nd3	1.6610	ν3	20.53
R6	−15.332	d6=	0.076
R7	6.169	d7=	0.333	nd4	1.5444	ν4	55.82
R8	5.411	d8=	0.468
R9	−13.995	d9=	0.465	nd5	1.5444	ν5	55.82
R10	−1.774	d10=	0.045
R11	−23.288	d11=	0.313	nd6	1.6610	ν6	20.53
R12	12.810	d12=	0.487
R13	−3.636	d13=	0.296	nd7	1.5444	ν7	55.82
R14	4.461	d14=	0.625
R15	∞	d15=	0.210	ndg	1.5168	νg	64.17
R16	∞	d16=	0.140

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

S1: aperture;

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

R15: curvature radius of an object side surface of the optical filter GF;

R16: curvature radius of an image side surface of the optical filter GF;

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

d14: on-axis distance from the image side surface of the seventh lens L7 to the object side surface of the optical filter GF;

d15: on-axis thickness of the optical filter GF;

d16: on-axis distance from the image side surface of the optical filter GF to the image plane;

nd: refractive index of d line;

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

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

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

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

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

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

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

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

vd: abbe number;

v1: abbe number of the first lens L1;

v2: abbe number of the second lens L2;

v3: abbe number of the third lens L3;

v4: abbe number of the fourth lens L4;

v5: abbe number of the fifth lens L5;

v6: abbe number of the sixth lens L6;

v7: abbe number of the seventh lens L7;

vg: abbe number of the optical filter GF.

Table 2 shows aspherical surface data of the camera optical lens 10 in Embodiment 1 of the present disclosure.

TABLE 2
	Conic
	coefficient	Aspherical surface coefficients
	k	A4	A6	A8	A10
R1	−4.8349E−01	−1.0740E−03	1.3185E−02	−1.6884E−02	1.1653E−02
R2	−5.1855E+00	1.2620E−01	−3.6881E−01	4.3075E−01	−2.8472E−01
R3	3.7046E+01	1.6401E−01	−4.1108E−01	5.1146E−01	−3.7999E−01
R4	1.1691E+01	8.4524E−02	−1.8794E−01	3.4580E−01	−4.4857E−01
R5	1.7926E+02	1.2591E−01	−3.6931E−01	6.1843E−01	−6.6714E−01
R6	1.0664E+02	2.3960E−01	−8.1613E−01	1.5771E+00	−1.9075E+00
R7	0.0000E+00	1.1382E−01	−6.0162E−01	1.0251E+00	−9.6662E−01
R8	0.0000E+00	−2.4482E−02	−8.4377E−02	7.4285E−02	−1.0470E−02
R9	−6.7905E+02	−6.1862E−02	2.1789E−01	−2.8306E−01	1.9366E−01
R10	−8.5294E+00	4.4937E−02	2.8091E−02	−1.2438E−01	1.2797E−01
R11	−2.3737E+03	2.4070E−01	−3.1441E−01	1.7152E−01	−5.2787E−02
R12	−9.2371E+02	1.6834E−01	−2.1225E−01	1.1275E−01	−3.8237E−02
R13	1.2857E−01	−4.7255E−03	−7.1033E−02	5.0947E−02	−1.5839E−02
R14	−7.3541E+00	−8.4277E−02	1.2422E−02	2.2961E−03	−9.3880E−04
	Aspherical surface coefficients
	A12	A14	A16	A18	A20
R1	−4.5904E−03	7.7578E−04	−4.3541E−05	0.0000E+00	0.0000E+00
R2	1.0963E−01	−2.2988E−02	2.0287E−03	0.0000E+00	0.0000E+00
R3	1.8182E−01	−5.1476E−02	6.6397E−03	0.0000E+00	0.0000E+00
R4	3.7940E−01	−1.7749E−01	3.5082E−02	0.0000E+00	0.0000E+00
R5	3.9683E−01	−1.1876E−01	1.4189E−02	0.0000E+00	0.0000E+00
R6	1.4128E+00	−6.3839E−01	1.6628E−01	−1.9357E−02	0.0000E+00
R7	5.0076E−01	−1.3173E−01	1.3722E−02	0.0000E+00	0.0000E+00
R8	−2.9114E−02	2.1203E−02	−5.6135E−03	5.2209E−04	0.0000E+00
R9	−7.7314E−02	1.6351E−02	−1.4021E−03	0.0000E+00	0.0000E+00
R10	−7.0388E−02	2.1671E−02	−3.4839E−03	2.2720E−04	0.0000E+00
R11	5.2522E−03	1.4204E−03	−4.0769E−04	2.8923E−05	0.0000E+00
R12	8.1213E−03	−1.0177E−03	6.9217E−05	−2.0213E−06	0.0000E+00
R13	2.7512E−03	−2.7861E−04	1.5464E−05	−3.6474E−07	0.0000E+00
R14	7.9039E−05	5.1689E−06	−1.1658E−06	5.1389E−08	0.0000E+00

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

IH: Image Heighty=(x²/R)/[1+{1−(k+1)(x²/R²)}^1/2]+A4x⁴+A6x⁶+A8x⁸+A10x¹⁰+A12x¹²+A14x¹⁴+A16x¹⁶+A18x¹⁸+A20x²⁰  (7)

For convenience, an aspheric surface of each lens surface uses the aspheric surfaces shown in the above formula (7). However, the present disclosure is not limited to the aspherical polynomials form shown in the formula (7).

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

	TABLE 3
	Number of	Inflexion point	Inflexion point	Inflexion point	Inflexion point
	inflexion points	position 1	position 2	position 3	position 4
P1R1	1	1.395
P1R2	1	0.585
P2R1
P2R2
P3R1	2	0.245	0.425
P3R2	4	0.175	0.465	1.195	1.355
P4R1	3	0.495	1.225	1.445
P4R2	3	0.525	1.405	1.595
P5R1	2	0.495	0.875
P5R2	1	1.925
P6R1	3	0.125	0.715	1.765
P6R2	3	0.735	2.005	2.335
P7R1	1	1.485
P7R2	2	0.475	2.795

	TABLE 4
	Number of	Arrest point	Arrest point
	arrest points	position 1	position 2
	P1R1
	P1R2	1	1.065
	P2R1
	P2R2
	P3R1
	P3R2	2	0.385	0.525
	P4R1	1	0.875
	P4R2	1	0.875
	P5R1
	P5R2
	P6R1	2	0.215	0.975
	P6R2	1	1.055
	P7R1	1	2.765
	P7R2	1	0.855

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 17 shows various values of Embodiments 1, 2, 3 and 4 and values corresponding to parameters which are specified in the above conditions.

As shown in Table 17, Embodiment 1 satisfies the above conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 3.299 mm. The image height of 1.0 H is 3.852 mm. The FOV (field of view) in the diagonal direction is 76.98°. Thus, the camera optical lens can achieve a high optical performance while satisfying design requirements for ultra-thin lenses having a big aperture.

Embodiment 2

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

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

	TABLE 5
	R	d	nd	νd
S1	∞	d0=	−0.582
R1	2.109	d1=	1.099	nd1	1.5806	ν1	60.08
R2	10.422	d2=	0.038
R3	23.609	d3=	0.220	nd2	1.6610	ν2	20.53
R4	6.419	d4=	0.455
R5	−18.251	d5=	0.292	nd3	1.6610	ν3	20.53
R6	−15.177	d6=	0.068
R7	5.455	d7=	0.419	nd4	1.5444	ν4	55.82
R8	4.934	d8=	0.357
R9	−13.960	d9=	0.503	nd5	1.5444	ν5	55.82
R10	−1.308	d10=	0.044
R11	−10.410	d11=	0.357	nd6	1.6610	ν6	20.53
R12	8.523	d12=	0.427
R13	−3.814	d13=	0.327	nd7	1.5444	ν7	55.82
R14	3.637	d14=	0.625
R15	∞	d15=	0.210	ndg	1.5168	νg	64.17
R16	∞	d16=	0.129

Table 6 shows aspherical surface data of each lens of the camera optical lens 20 in Embodiment 2 of the present disclosure.

TABLE 6
	Conic
	coefficient	Aspherical surface coefficients
	k	A4	A6	A8	A10
R1	−3.9959E−01	3.0848E−03	1.0432E−02	−1.7580E−02	1.2276E−02
R2	−8.2006E+01	1.2984E−01	−3.6397E−01	4.3000E−01	−2.8538E−01
R3	−3.5955E+01	1.7242E−01	−4.0782E−01	5.1063E−01	−3.8127E−01
R4	5.1236E+00	9.9137E−02	−1.8130E−01	3.4465E−01	−4.5968E−01
R5	1.6990E+02	1.1851E−01	−3.7122E−01	6.2389E−01	−6.6672E−01
R6	6.6229E+01	2.5166E−01	−8.6090E−01	1.5327E+00	−1.6248E+00
R7	0.0000E+00	9.7026E−02	−5.9800E−01	1.0297E+00	−9.6540E−01
R8	0.0000E+00	−6.7254E−02	9.2537E−02	−2.7277E−01	3.6424E−01
R9	−1.0001E+03	−3.7941E−02	2.2056E−01	−2.8339E−01	1.9340E−01
R10	−9.1464E+00	−1.3325E−01	4.0348E−01	−5.2669E−01	4.1110E−01
R11	−1.1126E+03	5.8609E−02	2.9880E−03	−8.8264E−02	7.1807E−02
R12	−1.1655E+02	−4.1526E−02	7.5574E−02	−7.9701E−02	3.6946E−02
R13	1.3165E−02	−8.4922E−02	2.4042E−02	5.3707E−03	−4.4435E−03
R14	−4.2969E+00	−1.1274E−01	4.3025E−02	−1.1566E−02	2.4098E−03
	Aspherical surface coefficients
	A12	A14	A16	A18	A20
R1	−4.3987E−03	7.5584E−04	−7.4020E−05	0.0000E+00	0.0000E+00
R2	1.0927E−01	−2.3083E−02	2.1131E−03	0.0000E+00	0.0000E+00
R3	1.8139E−01	−5.1266E−02	6.4433E−03	0.0000E+00	0.0000E+00
R4	3.8552E−01	−1.7108E−01	3.0560E−02	0.0000E+00	0.0000E+00
R5	3.9663E−01	−1.1848E−01	1.4082E−02	0.0000E+00	0.0000E+00
R6	9.8458E−01	−3.1996E−01	4.7705E−02	−1.8687E−03	0.0000E+00
R7	5.0055E−01	−1.3204E−01	1.3646E−02	0.0000E+00	0.0000E+00
R8	−2.7076E−01	1.1359E−01	−2.4767E−02	2.1661E−03	0.0000E+00
R9	−7.7363E−02	1.6352E−02	−1.4036E−03	0.0000E+00	0.0000E+00
R10	−1.9818E−01	5.6399E−02	−8.6387E−03	5.4856E−04	0.0000E+00
R11	−3.1792E−02	8.1915E−03	−1.1030E−03	5.9338E−05	0.0000E+00
R12	−9.4192E−03	1.3526E−03	−9.9242E−05	2.7470E−06	0.0000E+00
R13	1.1820E−03	−1.6515E−04	1.2073E−05	−3.6432E−07	0.0000E+00
R14	−3.7269E−04	3.7281E−05	−2.0514E−06	4.6368E−08	0.0000E+00

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

	TABLE 7
	Number of	Inflexion point	Inflexion point	Inflexion point
	inflexion points	position 1	position 2	position 3
P1R1	1	1.395
P1R2	1	0.585
P2R1
P2R2
P3R1	3	0.295	0.345	1.185
P3R2	3	0.175	0.435	1.185
P4R1	3	0.485	1.185	1.345
P4R2	3	0.545	1.385	1.505
P5R1	2	0.385	1.065
P5R2	3	0.655	1.135	1.875
P6R1	3	0.255	0.745	1.725
P6R2	3	0.665	2.015	2.355
P7R1	2	1.465	2.655
P7R2	3	0.485	2.595	3.015

	TABLE 8
	Number of	Arrest point	Arrest point
	arrest points	position 1	position 2
	P1R1	1	1.675
	P1R2	1	1.075
	P2R1
	P2R2
	P3R1
	P3R2	2	0.365	0.485
	P4R1	1	0.875
	P4R2	1	0.885
	P5R1	2	0.615	1.285
	P5R2
	P6R1	2	0.495	0.895
	P6R2	1	0.985
	P7R1	2	2.505	2.745
	P7R2	1	0.945

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.

As shown in Table 17, Embodiment 2 satisfies the above conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 3.057 mm. The image height of 1.0 H is 3.852 mm. The FOV (field of view) in the diagonal direction is 81.61°. Thus, the camera optical lens can achieve a high optical performance while satisfying design requirements for ultra-thin lenses having a big aperture.

Embodiment 3

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

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

	TABLE 9
	R	d	nd	νd
S1	∞	d0=	−0.644
R1	1.937	d1=	1.278	nd1	1.4342	ν1	94.95
R2	22.857	d2=	0.048
R3	6.856	d3=	0.226	nd2	1.6700	ν2	19.39
R4	4.656	d4=	0.372
R5	−18.158	d5=	0.214	nd3	1.6610	ν3	20.53
R6	−10.901	d6=	0.069
R7	5.740	d7=	0.333	nd4	1.5444	ν4	55.82
R8	5.147	d8=	0.377
R9	−6.843	d9=	0.409	nd5	1.5444	ν5	55.82
R10	−2.119	d10=	0.067
R11	6.259	d11=	0.435	nd6	1.6610	ν6	20.53
R12	5.501	d12=	0.589
R13	−3.562	d13=	0.294	nd7	1.5444	ν7	55.82
R14	4.091	d14=	0.525
R15	∞	d15=	0.210	ndg	1.5168	νg	64.17
R16	∞	d16=	0.103

Table 10 shows aspherical surface data of each lens of the camera optical lens 30 in Embodiment 3 of the present disclosure.

TABLE 10
	Conic
	coefficient	Aspherical surface coefficients
	k	A4	A6	A8	A10
R1	−4.4021E−01	1.4142E−03	1.0279E−02	−1.9388E−02	1.3777E−02
R2	2.2371E+02	1.3773E−01	−3.7850E−01	4.3080E−01	−2.8223E−01
R3	1.8842E+01	1.4868E−01	−4.1047E−01	5.0525E−01	−3.8274E−01
R4	9.2379E+00	7.6352E−02	−2.0747E−01	3.3771E−01	−4.4311E−01
R5	−2.3160E+02	1.4575E−01	−3.7963E−01	6.1044E−01	−6.6998E−01
R6	−2.5341E+01	3.0053E−01	−1.0327E+00	2.0834E+00	−2.6557E+00
R7	0.0000E+00	1.1443E−01	−6.0318E−01	1.0248E+00	−9.6573E−01
R8	0.0000E+00	−4.8990E−02	3.5394E−02	−1.6122E−01	2.4358E−01
R9	−3.3281E+02	−3.2767E−02	2.1687E−01	−2.8412E−01	1.9332E−01
R10	−1.2568E+01	−1.6023E−01	4.3628E−01	−5.2143E−01	3.8058E−01
R11	−3.6238E+02	−5.4745E−03	5.2551E−02	−1.0793E−01	8.6262E−02
R12	−8.4686E+01	−1.1929E−02	6.1263E−03	−4.8317E−03	−2.4977E−03
R13	−1.7407E−01	−1.1079E−01	5.9562E−02	−2.3574E−02	9.2428E−03
R14	−7.2236E+00	−1.1958E−01	5.7196E−02	−2.1480E−02	5.6439E−03
	Aspherical surface coefficients
	A12	A14	A16	A18	A20
R1	−4.2213E−03	3.3743E−04	2.7034E−05	0.0000E+00	0.0000E+00
R2	1.0925E−01	−2.3423E−02	2.1410E−03	0.0000E+00	0.0000E+00
R3	1.8411E−01	−5.0924E−02	6.1229E−03	0.0000E+00	0.0000E+00
R4	3.7956E−01	−1.7743E−01	3.4152E−02	0.0000E+00	0.0000E+00
R5	3.9649E−01	−1.1807E−01	1.5516E−02	0.0000E+00	0.0000E+00
R6	2.0678E+00	−9.8053E−01	2.6638E−01	−3.1829E−02	0.0000E+00
R7	5.0089E−01	−1.3182E−01	1.3605E−02	0.0000E+00	0.0000E+00
R8	−1.9676E−01	8.9223E−02	−2.1333E−02	2.0974E−03	0.0000E+00
R9	−7.7367E−02	1.6357E−02	−1.3931E−03	0.0000E+00	0.0000E+00
R10	−1.7904E−01	5.1454E−02	−8.0894E−03	5.2910E−04	0.0000E+00
R11	−4.1832E−02	1.1622E−02	−1.6364E−03	8.9738E−05	0.0000E+00
R12	2.2059E−03	−6.1667E−04	7.9668E−05	−3.9696E−06	0.0000E+00
R13	−2.4829E−03	3.8690E−04	−3.1751E−05	1.0649E−06	0.0000E+00
R14	−9.2135E−04	8.7018E−05	−4.2880E−06	8.3062E−08	0.0000E+00

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

	TABLE 11
	Number of	Inflexion point	Inflexion point	Inflexion point
	inflexion points	position 1	position 2	position 3
P1R1	1	1.465
P1R2	1	0.555
P2R1
P2R2
P3R1	3	0.205	0.565	1.155
P3R2	3	0.185	0.495	1.155
P4R1	1	0.505
P4R2	1	0.555
P5R1	2	0.405	1.015
P5R2	2	0.665	1.075
P6R1	2	0.645	1.695
P6R2	2	0.665	2.035
P7R1	3	1.415	2.385	2.625
P7R2	1	0.445

	TABLE 12
	Number of	Arrest point	Arrest point	Arrest point
	arrest points	position 1	position 2	position 3
P1R1
P1R2	1	0.895
P2R1
P2R2
P3R1	2	0.415	0.665
P3R2	3	0.435	0.545	1.295
P4R1	1	0.895
P4R2	1	0.895
P5R1	2	0.705	1.195
P5R2
P6R1	1	0.955
P6R2	1	1.125
P7R1
P7R2	1	0.845

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.

As shown in Table 17, Embodiment 1 satisfies the above conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 3.117 mm. The image height of 1.0H is 3.852 mm. The FOV (field of view) in the diagonal direction is 80.50°. Thus, the camera optical lens has a big aperture and is ultra-thin, while achieving a high optical performance.

Embodiment 4

Embodiment 4 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences therebetween will be described in the following.

Table 13 and Table 14 show design data of a camera optical lens 40 in Embodiment 2 of the present disclosure.

	TABLE 13
	R	d	nd	νd
S1	∞	d0=	−0.641
R1	2.035	d1=	1.141	nd1	1.5378	ν1	74.70
R2	12.096	d2=	0.049
R3	11.458	d3=	0.203	nd2	1.6610	ν2	20.53
R4	5.536	d4=	0.418
R5	−28.215	d5=	0.157	nd3	1.6610	ν3	20.53
R6	−17.391	d6=	0.089
R7	22.075	d7=	0.438	nd4	1.5444	ν4	55.82
R8	14.744	d8=	0.417
R9	−39.013	d9=	0.453	nd5	1.5444	ν5	55.82
R10	−2.113	d10=	0.020
R11	−96.605	d11=	0.303	nd6	1.6610	ν6	20.53
R12	26.753	d12=	0.516
R13	−3.414	d13=	0.340	nd7	1.5444	ν7	55.82
R14	4.056	d14=	0.625
R15	∞	d15=	0.210	ndg	1.5168	νg	64.17
R16	∞	d16=	0.138

Table 14 shows aspherical surface data of each lens of the camera optical lens 40 in Embodiment 4 of the present disclosure.

TABLE 14
	Conic
	coefficient	Aspherical surface coefficients
	k	A4	A6	A8	A10
R1	−4.8818E−01	−1.0740E−03	1.3185E−02	−1.6884E−02	1.1653E−02
R2	1.1242E+00	1.2620E−01	−3.6881E−01	4.3075E−01	−2.8472E−01
R3	5.7249E+01	1.6401E−01	−4.1108E−01	5.1146E−01	−3.7999E−01
R4	1.3039E+01	8.4524E−02	−1.8794E−01	3.4580E−01	−4.4857E−01
R5	−1.6613E+02	1.2591E−01	−3.6931E−01	6.1843E−01	−6.6714E−01
R6	9.1686E+01	2.3960E−01	−8.1613E−01	1.5771E+00	−1.9075E+00
R7	0.0000E+00	1.1382E−01	−6.0162E−01	1.0251E+00	−9.6662E−01
R8	0.0000E+00	−2.4482E−02	−8.4377E−02	7.4285E−02	−1.0470E−02
R9	4.7757E+02	−6.1862E−02	2.1789E−01	−2.8306E−01	1.9366E−01
R10	−7.8083E+00	4.4937E−02	2.8091E−02	−1.2438E−01	1.2797E−01
R11	−1.4159E+03	2.4070E−01	−3.1441E−01	1.7152E−01	−5.2787E−02
R12	−9.9474E+01	1.6834E−01	−2.1225E−01	1.1275E−01	−3.8237E−02
R13	−2.0681E−01	−4.7255E−03	−7.1033E−02	5.0947E−02	−1.5839E−02
R14	−8.6290E+00	−8.4277E−02	1.2422E−02	2.2961E−03	−9.3880E−04
	Aspherical surface coefficients
	A12	A14	A16	A18	A20
R1	−4.5904E−03	7.7578E−04	−4.3541E−05	0.0000E+00	0.0000E+00
R2	1.0963E−01	−2.2988E−02	2.0287E−03	0.0000E+00	0.0000E+00
R3	1.8182E−01	−5.1476E−02	6.6397E−03	0.0000E+00	0.0000E+00
R4	3.7940E−01	−1.7749E−01	3.5082E−02	0.0000E+00	0.0000E+00
R5	3.9683E−01	−1.1876E−01	1.4189E−02	0.0000E+00	0.0000E+00
R6	1.4128E+00	−6.3839E−01	1.6628E−01	−1.9357E−02	0.0000E+00
R7	5.0076E−01	−1.3173E−01	1.3722E−02	0.0000E+00	0.0000E+00
R8	−2.9114E−02	2.1203E−02	−5.6135E−03	5.2209E−04	0.0000E+00
R9	−7.7314E−02	1.6351E−02	−1.4021E−03	0.0000E+00	0.0000E+00
R10	−7.0388E−02	2.1671E−02	−3.4839E−03	2.2720E−04	0.0000E+00
R11	5.2522E−03	1.4204E−03	−4.0769E−04	2.8923E−05	0.0000E+00
R12	8.1213E−03	−1.0177E−03	6.9217E−05	−2.0213E−06	0.0000E+00
R13	2.7512E−03	−2.7861E−04	1.5464E−05	−3.6474E−07	0.0000E+00
R14	7.9039E−05	5.1689E−06	−1.1658E−06	5.1389E−08	0.0000E+00

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 disclosure.

	TABLE 15
	Number of	Inflexion point	Inflexion point	Inflexion point
	inflexion points	position 1	position 2	position 3
P1R1	1	1.385
P1R2	1	0.575
P2R1
P2R2
P3R1	3	0.175	0.515	1.235
P3R2	3	0.165	0.485	1.175
P4R1	2	0.395	1.235
P4R2	2	0.355	1.415
P5R1	2	0.495	0.845
P5R2	1	1.925
P6R1	3	0.065	0.715	1.765
P6R2	2	0.745	2.005
P7R1	1	1.485
P7R2	2	0.485	2.795

	TABLE 16
	Number of	Arrest point	Arrest point
	arrest points	position 1	position 2
	P1R1
	P1R2	1	1.005
	P2R1
	P2R2
	P3R1	2	0.335	0.645
	P3R2	2	0.325	0.625
	P4R1	1	0.585
	P4R2	1	0.575
	P5R1
	P5R2
	P6R1	2	0.105	0.985
	P6R2	1	1.065
	P7R1	1	2.695
	P7R2	1	0.885

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 240 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.

As shown in Table 17, Embodiment 4 satisfies the above conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 3.171 mm. The image height of 1.0 H is 3.852 mm. The FOV (field of view) in the diagonal direction is 79.47°. Thus, the camera optical lens can achieve a high optical performance while satisfying design requirements for ultra-thin lenses having a big aperture.

TABLE 17
Conditions	Embodiment 1	Embodiment 2	Embodiment 3	Embodiment 4	Notes
f3/f	26.18	29.58	9.01	14.80	Condition (1)
v1/v2	3.64	2.93	4.90	3.64	Condition (2)
f2/f	−3.29	−3.02	−4.99	−3.57	Condition (3)
(d3 + d5)/TTL	0.08	0.09	0.08	0.07	Condition (4)
(R5 + R6)/(R5 − R6)	10.10	10.87	4.00	4.21	Condition (5)
(R7 + R8)/(R7 − R8)	15.28	19.94	18.36	5.02	Condition (6)
f	4.750	4.402	4.488	4.567
f1	4.351	4.328	4.776	4.366
f2	−15.637	−13.291	−22.377	−16.286
f3	124.354	130.199	40.436	67.595
f4	−95.387	−131.975	−113.889	−83.048
f5	3.671	2.606	5.372	4.073
f6	−12.352	−6.976	−88.444	−31.392
f7	−3.621	−3.357	−3.440	−3.341
f12	5.442	5.746	5.613	5.442
TTL	5.589	5.570	5.549	5.517

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

Claims

1. A camera optical lens, comprising, from an object side to an image side: an aperture;a first lens having a positive refractive power;a second lens having a negative refractive power;a third lens having a positive refractive power;a fourth lens having a negative refractive power;a fifth lens having a positive refractive power;a sixth lens having a negative refractive power; anda seventh lens having a negative refractive power,wherein the camera optical lens satisfies following conditions: 9.00≤f3/f≤30.00; and2.90≤v1/v2≤5.00,wheref denotes a focal length of the camera optical lens;f3 denotes a focal length of the third lens;v1 denotes an abbe number of the first lens; andv2 denotes an abbe number of the second lens.

2. The camera optical lens as described in claim 1, further satisfying a following condition: −5.00≤f2/f≤−3.00,where f2 denotes a focal length of the second lens.

3. The camera optical lens as described in claim 1, further satisfying a following condition: 0≤(d3+d5)/TTL≤0.10,whered3 denotes an on-axis thickness of the second lens;d5 denotes an on-axis thickness of the third lens; andTTL 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.

4. The camera optical lens as described in claim 1, further satisfying a following condition: 4.00≤(R5+R6)/(R5−R6)≤11.00,whereR5 denotes a curvature radius of an object side surface of the third lens; andR6 denotes a curvature radius of an image side surface of the third lens.

5. The camera optical lens as described in claim 1, further satisfying a following condition: 5.00≤(R7+R8)/(R7−R8)≤20.00,whereR7 denotes a curvature radius of an object side surface of the fourth lens; andR8 denotes a curvature radius of an image side surface of the fourth lens.