Camera optical lens including six lenses of +−−−+− refractive powers

Abstract

The present disclosure relates to the field of optical lenses and provides a camera optical lens. The camera optical lens includes, from an object side to an image side: a first lens; a second lens having a negative refractive power; a third lens having a negative refractive power; a fourth lens; a fifth lens; and a sixth lens. The camera optical lens satisfies following conditions: 1.10≤f1/f≤3.00; and −25.00≤R9/d9≤−10.00. The camera optical lens can achieve a high imaging performance while obtaining a low TTL.

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 imaging 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. 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, the five-piece, six-piece and seven-piece lens structures gradually appear in lens designs. There is an urgent need for ultra-thin, wide-angle camera lenses with good optical characteristics and fully corrected chromatic aberration.

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.

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 6 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, and a sixth lens L6. An optical element such as an optical filter GF can be arranged between the sixth lens L6 and an image plane S1.

The first lens L1 is made of a plastic material, the second lens L2 is made of a plastic material, the third lens L3 is made of a plastic material, the fourth lens L4 is made of a plastic material, the fifth lens L5 is made of a plastic material, and the sixth lens L6 is made of a plastic material.

The second lens L2 has a negative refractive power, and the third lens L3 has a negative refractive power.

Here, a focal length of the camera optical lens 10 is defined as f, and a focal length of the first lens L1 is defined as f1. The camera optical lens 10 should satisfy a condition of 1.10≤f1/f≤3.00, which specifies a ratio of the focal length f1 of the first lens L1 and the focal length f of the camera optical lens 10. If the lower limit of the specified value is exceeded, although it would facilitate development of ultra-thin lenses, the positive refractive power of the first lens L1 will be too strong, and thus it is difficult to correct the problem like an aberration and it is also unfavorable for development of wide-angle lenses. On the contrary, if the upper limit of the specified value is exceeded, the positive refractive power of the first lens L1 would become too weak, and it is then difficult to develop ultra-thin lenses. Preferably, 1.13≤f1/f≤2.84.

A curvature radius of the object side surface of the fifth lens L5 is defined as R9, and an on-axis thickness of the fifth lens L5 is defined as d9. The camera optical lens 10 further satisfies a condition of −25.00≤R9/d9≤−10.00, which specifies a shape of the fifth lens L5. Out of this range, a development towards ultra-thin and wide-angle lenses would make it difficult to correct the problem of the aberration. Preferably, −24.90≤R9/d9≤−10.56.

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. When the focal length of the camera optical lens, the focal length of the first lens, the curvature radius of the object side surface of the fifth lens and the on-axis thickness of the fifth lens satisfy the above conditions, the camera optical lens will have the advantage of high performance and satisfy the design requirement of a low TTL.

In this embodiment, the object side surface of the first lens L1 is convex in a paraxial region, the image side surface of the first lens L1 is concave in the paraxial region, and the first lens L1 has a positive refractive power.

A curvature radius of the object side surface of the first lens L1 is defined as R1, and a curvature radius of the image side surface of the first lens L1 is defined as R2. The camera optical lens 10 further satisfies a condition of −12.27≤(R1+R2)/(R1−R2)≤−1.67. This can reasonably control a shape of the first lens L1 in such a manner that the first lens L1 can effectively correct a spherical aberration of the camera optical lens. Preferably, −7.67≤(R1+R2)/(R1−R2)≤−2.09.

An on-axis thickness of the first lens L1 is defined as d1. The camera optical lens 10 further satisfies a condition of 0.06≤d1/TTL≤0.25. This facilitates achieving ultra-thin lenses. Preferably, 0.10≤d1/TTL≤0.20.

In this embodiment, an object side surface of the second lens L2 is convex in the paraxial region, and an object side surface of the second lens L2 is concave in the paraxial region.

The focal length of the camera optical lens 10 is f, and a focal length of the second lens L2 is f2. The camera optical lens 10 further satisfies a condition of −1.26*10⁷≤f2/f≤−5.15. By controlling the negative refractive power of the second lens L2 within the reasonable range, correction of the aberration of the optical system can be facilitated. Preferably, −7.88*10⁶≤f2/f≤−6.44.

A curvature radius of the object side surface of the second lens L2 is defined as R3, and a curvature radius of the image side surface of the second lens L2 is defined as R4. The camera optical lens 10 further satisfies a condition of 5.25≤(R3+R4)/(R3−R4)≤98.43. This can reasonably control a shape of the second lens L2. Out of this range, a development towards ultra-thin and wide-angle lenses would make it difficult to correct the problem of the aberration. Preferably, 8.40≤(R3+R4)/(R3−R4)≤78.74.

An on-axis thickness of the second lens L2 is defined as d3. The camera optical lens 10 further satisfies a condition of 0.02≤d3/TTL≤0.07. This facilitates achieving ultra-thin lenses. Preferably, 0.03≤d3/TTL≤0.05.

In this embodiment, an object side surface of the third lens L3 is convex in the paraxial region, and an image side surface of the third lens L3 is concave in the paraxial region.

The focal length of the camera optical lens 10 is f, and a focal length of the third lens L3 is f3. The camera optical lens 10 further satisfies a condition of −1.05*10⁷≤f3/f≤−8.36. The appropriate distribution of the refractive power leads to a better imaging quality and a lower sensitivity. Preferably, −6.56*10⁶≤f3/f≤−10.45.

A curvature radius of an 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 1.80≤(R5+R6)/(R5−R6)≤324.75, which specifies a shape of the third lens L3. Out of this range, a development towards ultra-thin and wide-angle lenses would make it difficult to correct the problem like an off-axis aberration. Preferably, 2.89≤(R5+R6)/(R5−R6)≤259.80.

An on-axis thickness of the third lens L3 is defined as d5. The camera optical lens 10 further satisfies a condition of 0.03≤d5/TTL≤0.12. This facilitates achieving ultra-thin lenses. Preferably, 0.05≤d5/TTL≤0.09.

In this embodiment, an object side surface of the fourth lens L4 is convex in the paraxial region, an image side surface of the fourth lens L4 is concave in the paraxial region, and the fourth lens L4 has a negative refractive power.

The focal length of the camera optical lens 10 is f, and a focal length of the fourth lens L4 is f4. The camera optical lens 10 further satisfies a condition of −10.41≤f4/f≤−3.14. The appropriate distribution of the refractive power leads to a better imaging quality and a lower sensitivity. Preferably, −6.51≤f4/f≤−3.93.

A curvature radius of an 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 0.97≤(R7+R8)/(R7−R8)≤3.03, which specifies a shape of the fourth lens L4. Out of this range, a development towards ultra-thin and wide-angle lenses would make it difficult to correct the problem like an off-axis aberration. Preferably, 1.55≤(R7+R8)/(R7−R8)≤2.42.

An on-axis thickness of the fourth lens L4 is defined as d7. The camera optical lens 10 further satisfies a condition of 0.02≤d7/TTL≤0.11. This facilitates achieving ultra-thin lenses. Preferably, 0.04≤d7/TTL≤0.09.

In this embodiment, an object side surface of the fifth lens L5 is concave in the paraxial region, an image side surface of the fifth lens L5 is convex in the paraxial region, and the fifth lens L5 has a positive refractive power.

The focal length of the camera optical lens 10 is f, and a focal length of the fifth lens L5 is f5. The camera optical lens 10 further satisfies a condition of 0.33≤f5/f≤1.15. This can effectively make a light angle of the camera lens gentle and reduce the tolerance sensitivity. Preferably, 0.53≤f5/f≤0.92.

A curvature radius of the object side surface of the fifth lens L5 is defined as R9, and a curvature radius of the image side surface of the fifth lens L5 is defined as R10. The camera optical lens 10 further satisfies a condition of 0.58≤(R9+R10)/(R9−R10)≤2.18, which specifies a shape of the fifth lens L5. Out of this range, a development towards ultra-thin and wide-angle lenses would make it difficult to correct the problem like an off-axis aberration. Preferably, 0.93≤(R9+R10)/(R9−R10)≤1.74.

An on-axis thickness of the fifth lens L5 is defined as d9. The camera optical lens 10 further satisfies a condition of 0.07≤d9/TTL≤0.21. This facilitates achieving ultra-thin lenses. Preferably, 0.11≤d9/TTL≤0.17.

In this embodiment, an object side surface of the sixth lens L6 is concave in the paraxial region, an image side surface of the sixth lens L6 is concave in the paraxial region, and the sixth lens L6 has a negative refractive power.

The focal length of the camera optical lens 10 is f, and a focal length of the sixth lens L6 is f6. The camera optical lens 10 further satisfies a condition of −1.80≤f6/f≤−0.49. The appropriate distribution of the refractive power leads to a better imaging quality and a lower sensitivity. Preferably, −1.12≤f6/f≤−0.62.

A curvature radius of the object side surface of the sixth lens L6 is defined as R11, and a curvature radius of the image side surface of the sixth lens L6 is defined as R12. The camera optical lens 10 further satisfies a condition of 0.34≤(R11+R12)/(R11−R12)≤1.15, which specifies a shape of the sixth lens L6. Out of this range, a development towards ultra-thin and wide-angle lenses would make it difficult to correct the problem like an off-axis aberration. Preferably, 0.55≤(R11+R12)/(R11−R12)≤0.92.

A thickness on-axis of the sixth lens L6 is defined as d11. The camera optical lens 10 further satisfies a condition of 0.02≤d11/TTL≤0.07. This facilitates achieving ultra-thin lenses. Preferably, 0.03≤d11/TTL≤0.05.

In this embodiment, the focal length of the camera optical lens 10 is f, and a combined focal length of the first lens L1 and the second lens L2 is f12. The camera optical lens 10 further satisfies a condition of 0.64≤f12/f≤3.89. This can eliminate the aberration and distortion of the camera optical lens while suppressing a back focal length of the camera optical lens, thereby maintaining miniaturization of the camera lens system. Preferably, 1.03≤f12/f≤3.11.

In this embodiment, the total optical length TTL of the camera optical lens 10 is smaller than or equal to 4.95 mm, which is beneficial for achieving ultra-thin lenses. Preferably, the total optical length TTL of the camera optical lens 10 is smaller than or equal to 4.72 mm.

In this embodiment, the camera optical lens 10 has a large F number, which is smaller than or equal to 1.96. The camera optical lens 10 has a better imaging performance. Preferably, the F number of the camera optical lens 10 is smaller than or equal to 1.92.

With such design, the total optical length TTL of the camera optical lens 10 can be made as short as possible, and thus the miniaturization characteristics can be maintained.

In the following, examples will be used to describe the camera optical lens 10 of the present disclosure. 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 to the image plane of the camera optical lens along the optic axis) in mm.

Preferably, 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 Tables 1 and 2.

TABLE 1
	R	d	nd	νd
S1	∞	d0 =	−0.221
R1	1.730	d1 =	0.565	nd1	1.5457	ν1	55.95
R2	2.405	d2 =	0.039
R3	2.645	d3 =	0.199	nd2	1.6664	ν2	20.40
R4	2.565	d4 =	0.160
R5	11.945	d5 =	0.350	nd3	1.5457	ν3	55.95
R6	11.798	d6 =	0.089
R7	21.279	d7 =	0.219	nd4	1.6664	ν4	20.40
R8	7.178	d8 =	0.107
R9	−14.775	d9 =	0.596	nd5	1.5457	ν5	55.95
R10	−1.113	d10 =	0.984
R11	−12.980	d11 =	0.203	nd6	1.5137	ν6	56.26
R12	1.712	d12 =	0.348
R13	∞	d13 =	0.210	ndg	1.5183	νg	64.17
R14	∞	d14 =	0.431

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 an object side surface of the optical filter GF;

R14: 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 optical filter GF;

d13: on-axis thickness of the optical filter GF;

d14: 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;

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;

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	A12	A14	A16
R1	1.2614E−01	1.6394E−04	4.7775E−02	−1.3474E−01	3.3155E−01	−3.8717E−01	2.2287E−01	−3.2178E−02
R2	−2.1162E+01	−1.7382E−01	4.3380E−01	−4.5212E−01	4.7808E−01	−2.2228E−01	−1.6616E−01	−2.5923E−01
R3	−8.0834E+00	−3.4119E−01	6.8154E−01	−4.2950E−01	−3.1921E−02	3.8611E−02	−2.2083E−01	−8.8260E−02
R4	−1.3939E+00	−1.4083E−01	5.8737E−01	−9.1157E−01	1.4610E+00	−2.2435E+00	1.8046E+00	−4.2331E−01
R5	2.0212E+02	−1.4078E−01	−7.0794E−02	2.5900E−01	−1.0921E+00	1.4966E+00	−1.1906E+00	−2.8440E−01
R6	4.8382E+01	−2.4644E−01	−2.6544E−01	1.2593E+00	−2.8124E+00	2.5904E+00	−1.1133E+00	1.0575E−01
R7	−3.7932E+02	−4.4377E−01	1.2896E−01	1.3267E−01	4.7162E−01	−2.1130E+00	2.0896E+00	−5.6553E−01
R8	2.8435E+01	−2.7982E−01	2.3468E−02	3.1939E−01	−4.2062E−01	1.8024E−01	−2.6259E−02	1.5089E−03
R9	1.1483E+02	−1.6871E−02	−8.3754E−02	−5.3207E−02	3.2511E−01	−3.8424E−01	1.6128E−01	−1.7645E−02
R10	−1.6226E+00	−4.0758E−02	−1.7795E−02	−9.9979E−02	1.5065E−01	−9.2708E−02	1.9945E−02	4.4519E−04
R11	2.8530E+01	−2.8036E−01	1.0833E−01	2.1913E−03	−1.5977E−02	4.4000E−03	−4.6727E−04	1.4613E−05
R12	−7.6483E+00	−1.8036E−01	1.0762E−01	−4.5041E−02	1.3634E−02	−2.6832E−03	2.7417E−04	−9.3092E−06

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  (1)

For convenience, an aspheric surface of each lens surface uses the aspheric surfaces shown in the above formula (1). However, the present disclosure is not limited to the aspherical polynomials form shown in the formula (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 disclosure. P1R1 and P1R2 represent the object side surface and the image side surface of the first lens L1, P2R1 and P2R2 represent the object side surface and the image side surface of the second lens L2, P3R1 and P3R2 represent the object side surface and the image side surface of the third lens L3, P4R1 and P4R2 represent the object side surface and the image side surface of the fourth lens L4, P5R1 and P5R2 represent the object side surface and the image side surface of the fifth lens L5, and P6R1 and P6R2 represent the object side surface and the image side surface of the sixth lens L6. 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	Inflexion	Inflexion	Inflexion
	inflexion	point	point	point	point
	points	position 1	position 2	position 3	position 4
P1R1	0	0	0	0	0
P1R2	0	0	0	0	0
P2R1	0	0	0	0	0
P2R2	0	0	0	0	0
P3R1	1	0.395	0	0	0
P3R2	1	0.285	0	0	0
P4R1	1	0.165	0	0	0
P4R2	1	0.365	0	0	0
P5R1	0	0	0	0	0
P5R2	0	0	0	0	0
P6R1	0	0	0	0	0
P6R2	1	0.985	0	0	0

	TABLE 4
		Number of	Arrest point	Arrest point
		arrest points	position 1	position 2
	P1R1	0	0	0
	P1R2	1	0.705	0
	P2R1	1	0.655	0
	P2R2	0	0	0
	P3R1	1	0.235	0
	P3R2	1	0.175	0
	P4R1	1	0.095	0
	P4R2	1	0.215	0
	P5R1	0	0	0
	P5R2	0	0	0
	P6R1	0	0	0
	P6R2	2	0.455	1.965

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 meridian direction.

Table 13 shows 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 above conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 1.717 mm. The image height of 1.0H is 2.72 mm. The FOV (field of view) is 78.70°. Thus, the camera optical lens has a wide-angle and is ultra-thin. Its on-axis and off-axis chromatic aberrations are fully corrected, thereby achieving excellent 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 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 =	−0.251
R1	1.626	d1 =	0.584	nd1	1.5457	ν1	55.95
R2	2.531	d2 =	0.052
R3	2.591	d3 =	0.181	nd2	1.6664	ν2	20.40
R4	2.494	d4 =	0.171
R5	12.811	d5 =	0.334	nd3	1.5457	ν3	55.95
R6	12.693	d6 =	0.101
R7	21.157	d7 =	0.247	nd4	1.6664	ν4	20.40
R8	6.977	d8 =	0.107
R9	−11.115	d9 =	0.643	nd5	1.5457	ν5	55.95
R10	−1.128	d10 =	0.898
R11	−9.077	d11 =	0.198	nd6	1.5137	ν6	56.26
R12	1.709	d12 =	0.348
R13	∞	d13 =	0.210	ndg	1.5183	νg	64.17
R14	∞	d14 =	0.416

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	A12	A14	A16
R1	1.4671E−01	1.3346E−03	4.7315E−02	−1.3750E−01	3.3177E−01	−3.8213E−01	2.2389E−01	−4.9425E−02
R2	−1.7281E+01	−1.7251E−01	4.3377E−01	−4.5609E−01	4.4620E−01	−2.9046E−01	−2.2141E−01	−1.0484E−01
R3	−7.0262E+00	−3.3753E−01	6.8250E−01	−4.3104E−01	−1.9818E−02	7.5382E−02	−1.9883E−01	−2.6116E−01
R4	−3.2477E+00	−1.5250E−01	5.8429E−01	−8.7615E−01	1.5195E+00	−2.1994E+00	1.7653E+00	−5.7909E−01
R5	1.8474E+02	−1.4310E−01	−7.0152E−02	2.4084E−01	−1.0982E+00	1.5444E+00	−1.0569E+00	−1.4184E−01
R6	6.2483E+01	−2.4447E−01	−2.6299E−01	1.2619E+00	−2.8068E+00	2.5877E+00	−1.0998E+00	1.3262E−01
R7	−7.8999E+02	−4.4465E−01	1.3030E−01	1.3238E−01	4.6806E−01	−2.1157E+00	2.0785E+00	−5.8304E−01
R8	2.9109E+01	−2.7948E−01	2.3218E−02	3.2045E−01	−4.1727E−01	1.8191E−01	−2.6111E−02	9.0659E−04
R9	7.9257E+01	−1.7349E−02	−8.3243E−02	−5.2700E−02	3.2387E−01	−3.8506E−01	1.6120E−01	−1.6299E−02
R10	−1.5803E+00	−4.0208E−02	−1.4807E−02	−9.9822E−02	1.4840E−01	−9.4929E−02	1.8590E−02	1.7086E−04
R11	3.1710E+01	−2.8370E−01	1.0892E−01	2.5165E−03	−1.6007E−02	4.2677E−03	−5.6616E−04	−4.1261E−05
R12	−8.0711E+00	−1.8322E−01	1.0698E−01	−4.5100E−02	1.3613E−02	−2.6813E−03	2.7359E−04	−9.4489E−06

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	Inflexion	Inflexion	Inflexion
	inflexion	point	point	point	point
	points	position 1	position 2	position 3	position 4
P1R1	0	0	0	0	0
P1R2	0	0	0	0	0
P2R1	0	0	0	0	0
P2R2	0	0	0	0	0
P3R1	1	0.375	0	0	0
P3R2	1	0.275	0	0	0
P4R1	1	0.165	0	0	0
P4R2	1	0.375	0	0	0
P5R1	0	0	0	0	0
P5R2	0	0	0	0	0
P6R1	0	0	0	0	0
P6R2	1	0.945	0	0	0

	TABLE 8
		Number of	Arrest point	Arrest point
		arrest points	position 1	position 2
	P1R1	0	0	0
	P1R2	1	0.675	0
	P2R1	1	0.665	0
	P2R2	0	0	0
	P3R1	1	0.225	0
	P3R2	1	0.165	0
	P4R1	1	0.095	0
	P4R2	1	0.215	0
	P5R1	0	0	0
	P5R2	0	0	0
	P6R1	0	0	0
	P6R2	1	0.445	0

FIG. 6 and FIG. 7 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 470 nm, 510 nm, 555 nm, 610 nm and 650 nm after passing the camera optical lens 20 according to Embodiment 2. FIG. 8 illustrates a field curvature and a distortion of light with a wavelength of 555 nm after passing the camera optical lens 20 according to Embodiment 2.

As shown in Table 13, Embodiment 2 satisfies the above conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 1.757 mm. The image height of 1.0H is 2.72 mm. The FOV (field of view) is 77.43°. Thus, the camera optical lens has a wide-angle and is ultra-thin. Its on-axis and off-axis chromatic aberrations are fully corrected, thereby achieving excellent 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 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 =	−0.251
R1	1.369	d1 =	0.687	nd1	1.5457	ν1	55.95
R2	3.186	d2 =	0.048
R3	3.268	d3 =	0.143	nd2	1.6664	ν2	20.40
R4	2.699	d4 =	0.276
R5	17.361	d5 =	0.244	nd3	1.5457	ν3	55.95
R6	9.829	d6 =	0.094
R7	24.765	d7 =	0.307	nd4	1.6664	ν4	20.40
R8	7.868	d8 =	0.131
R9	−6.443	d9 =	0.580	nd5	1.5457	ν5	55.95
R10	−1.187	d10 =	0.794
R11	−9.019	d11 =	0.159	nd6	1.5137	ν6	56.26
R12	1.492	d12 =	0.349
R13	∞	d13 =	0.210	ndg	1.5183	νg	64.17
R14	∞	d14 =	0.162

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	A12	A14	A16
R1	6.4152E−02	−3.6527E−03	4.0893E−02	−1.6181E−01	3.1520E−01	−3.6457E−01	2.3763E−01	−8.5082E−02
R2	−2.0846E+01	−2.1324E−01	3.7849E−01	−4.6162E−01	4.5415E−01	−2.8479E−01	−1.8653E−01	1.8715E−01
R3	−5.0269E+00	−3.2410E−01	7.0396E−01	−4.3644E−01	−3.5153E−02	1.1714E−01	−4.3615E−02	−3.0459E−02
R4	1.4421E+00	−1.1924E−01	5.9760E−01	−8.1330E−01	1.5405E+00	−2.2109E+00	1.6867E+00	−2.4512E−01
R5	4.3799E+02	−1.2694E−01	−6.5602E−02	2.4685E−01	−1.0800E+00	1.5409E+00	−9.6252E−01	3.1922E−03
R6	1.0904E+02	−2.3885E−01	−2.3276E−01	1.2696E+00	−2.7727E+00	2.5554E+00	−1.1204E+00	1.7255E−01
R7	8.5306E+01	−4.3992E−01	1.3860E−01	1.4349E−01	4.6622E−01	−2.0820E+00	2.0627E+00	−6.0612E−01
R8	2.2133E+01	−2.8440E−01	1.4645E−02	3.1620E−01	−4.0556E−01	1.8712E−01	−2.1583E−02	−1.0933E−03
R9	2.8811E+01	−3.3081E−02	−8.5151E−02	−5.0031E−02	3.1809E−01	−3.8396E−01	1.5967E−01	−7.7442E−03
R10	−1.8696E+00	−2.3714E−02	−7.2679E−03	−1.0035E−01	1.4472E−01	−9.3772E−02	1.9815E−02	1.8653E−03
R11	−1.9009E+01	−2.6982E−01	1.1020E−01	2.5548E−03	−1.5804E−02	4.2978E−03	−4.7151E−04	3.1937E−05
R12	−5.7542E+00	−1.8485E−01	1.0574E−01	−4.4686E−02	1.3511E−02	−2.6390E−03	2.6976E−04	−1.0253E−05

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

TABLE 11
	Number of	Inflexion	Inflexion	Inflexion	Inflexion
	inflexion	point	point	point	point
	points	position 1	position 2	position 3	position 4
P1R1	0	0	0	0	0
P1R2	1	0.775	0	0	0
P2R1	0	0	0	0	0
P2R2	0	0	0	0	0
P3R1	1	0.345	0	0	0
P3R2	1	0.325	0	0	0
P4R1	1	0.155	0	0	0
P4R2	1	0.345	0	0	0
P5R1	0	0	0	0	0
P5R2	0	0	0	0	0
P6R1	0	0	0	0	0
P6R2	1	1.045	0	0	0

	TABLE 12
		Number of	Arrest point	Arrest point
		arrest points	position 1	position 2
	P1R1	0	0	0
	P1R2	1	0.415	0
	P2R1	0	0	0
	P2R2	0	0	0
	P3R1	1	0.205	0
	P3R2	1	0.195	0
	P4R1	1	0.095	0
	P4R2	2	0.205	1.075
	P5R1	1	1.075	0
	P5R2	1	1.225	0
	P6R1	0	0	0
	P6R2	1	0.485	0

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

Table 13 in the following lists values corresponding to the respective conditions in this embodiment in order to satisfy the above conditions. The camera optical lens according to this embodiment satisfies the above conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 1.763 mm. The image height of 1.0H is 2.72 mm. The FOV (field of view) is 77.29°. Thus, the camera optical lens has a wide-angle and is ultra-thin. Its on-axis and off-axis chromatic aberrations are fully corrected, thereby achieving excellent optical characteristics.

TABLE 13
Parameters	Embod-	Embod-	Embod-
and	iment	iment	iment
conditions	1	2	3
f	3.262	3.338	3.349
f1	8.728	6.789	3.882
f2	−2.057E+07	−391.163	−25.879
f3	−1.090E+04	−1.752E+07	−41.999
f4	−16.356	−15.732	−17.431
f5	2.173	2.249	2.566
f6	−2.930	−2.783	−2.479
f12	8.466	6.695	4.316
FNO	1.90	1.90	1.90
f1/f	2.68	2.03	1.16
R9/d9	−24.79	−17.29	−11.11

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, substantially consisting of, from an object side to an image side: a first lens;a second lens having a negative refractive power;a third lens having a negative refractive power;a fourth lens;a fifth lens; anda sixth lens,wherein the camera optical lens satisfies following conditions: 1.10≤f1/f≤3.00; and−25.00≤R9/d9≤−10.00,wheref denotes a focal length of the camera optical lens;f1 denotes a focal length of the first lens;R9 denotes a curvature radius of an object side surface of the fifth lens; andd9 denotes an on-axis thickness of the fifth lens.

2. The camera optical lens as described in claim 1, further satisfying following conditions: 1.13≤f1/f≤2.84; and−24.90≤R9/d9≤−10.56.

3. The camera optical lens as described in claim 1, wherein the first lens has a positive refractive power, and comprises an object side surface being convex in a paraxial region and an image side surface being concave in the paraxial region, and the camera optical lens further satisfies following conditions: −12.27≤(R1+R2)/(R1−R2)≤−1.67; and0.06≤d1/TTL≤0.25,whereR1 denotes a curvature radius of the object side surface of the first lens;R2 denotes a curvature radius of the image side surface of the first lens;d1 denotes an on-axis thickness of the first lens; andTTL 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.

4. The camera optical lens as described in claim 3, further satisfying following conditions: −7.67≤(R1+R2)/(R1−R2)≤−2.09; and0.10≤d1/TTL≤0.20.

5. The camera optical lens as described in claim 1, wherein the second lens comprises an object side surface being convex in a paraxial region and an image side surface being concave in the paraxial region, and the camera optical lens further satisfies following conditions: −1.26*107≤f2/f≤−5.15;5.25≤(R3+R4)/(R3−R4)≤98.43; and0.02≤d3/TTL≤0.07,wheref2 denotes a focal length of the second lens;R3 denotes a curvature radius of the object side surface of the second lens;R4 denotes a curvature radius of the image side surface of the second lens;d3 denotes an on-axis thickness of the second 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.

6. The camera optical lens as described in claim 5, further satisfying following conditions: −7.88*106≤f2/f≤−6.44;8.40≤(R3+R4)/(R3−R4)≤78.74; and0.03≤d3/TTL≤0.05.

7. The camera optical lens as described in claim 1, wherein the third lens comprises an object side surface being convex in a paraxial region and an image side surface being concave in the paraxial region, and the camera optical lens further satisfies following conditions: −1.05*107≤f3/f≤−8.36;1.80≤(R5+R6)/(R5−R6)≤324.75; and0.03≤d5/TTL≤0.12,wheref3 denotes a focal length of the third lens;R5 denotes a curvature radius of the object side surface of the third lens;R6 denotes a curvature radius of the image side surface of the third 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.

8. The camera optical lens as described in claim 7, further satisfying following conditions: −6.56*106≤f3/f≤−10.45;2.89≤(R5+R6)/(R5−R6)≤259.80; and0.05≤d5/TTL≤0.09.

9. The camera optical lens as described in claim 1, wherein the fourth lens has a negative refractive power, and comprises an object side surface being convex in a paraxial region and an image side surface being concave in the paraxial region, and the camera optical lens further satisfies following conditions: −10.41≤f4/f≤−3.14;0.97≤(R7+R8)/(R7−R8)≤3.03; and0.02≤d7/TTL≤0.11,wheref4 denotes a focal length of the fourth lens;R7 denotes a curvature radius of the object side surface of the fourth lens;R8 denotes a curvature radius of the image side surface of the fourth lens;d7 denotes an on-axis thickness of the fourth 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.

10. The camera optical lens as described in claim 9, further satisfying following conditions: −6.51≤f4/f≤−3.93;1.55≤(R7+R8)/(R7−R8)≤2.42; and0.04≤d7/TTL≤0.09.

11. The camera optical lens as described in claim 1, wherein the fifth lens has a positive refractive power, the object side surface of the fifth lens is concave in a paraxial region, and an image side surface of the fifth lens is convex in the paraxial region, and the camera optical lens further satisfies following conditions: 0.33≤f5/f≤1.15;0.58≤(R9+R10)/(R9−R10)≤2.18; and0.07≤d9/TTL≤0.21,wheref5 denotes a focal length of the fifth lens;R10 denotes a curvature radius of the image side surface of the fifth 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.

12. The camera optical lens as described in claim 11, further satisfying following conditions: 0.53≤f5/f≤0.92;0.93≤(R9+R10)/(R9−R10)≤1.74; and0.11≤d9/TTL≤0.17.

13. The camera optical lens as described in claim 1, wherein the sixth lens has a negative refractive power, and comprises an object side surface being concave in a paraxial region and an image side surface being concave in the paraxial region, and the camera optical lens further satisfies following conditions: −1.80≤f6/f≤−0.49;0.34≤(R11+R12)/(R11−R12)≤1.15; and0.02≤d11/TTL≤0.07,wheref6 denotes a focal length of the sixth lens;R11 denotes a curvature radius of the object side surface of the sixth lens;R12 denotes a curvature radius of the image side surface of the sixth lens;d11 denotes an on-axis thickness of the sixth 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.

14. The camera optical lens as described in claim 13, further satisfying following conditions: −1.12≤f6/f≤−0.62;0.55≤(R11+R12)/(R11−R12)≤0.92; and0.03≤d11/TTL≤0.05.

15. The camera optical lens as described in claim 1, further satisfying a following condition: 0.64≤f12/f≤3.89,wheref12 denotes a combined focal length of the first lens and the second lens.

16. The camera optical lens as described in claim 15, further satisfying a following condition: 1.03≤f12/f≤3.11.

17. The camera optical lens as described in claim 1, wherein a total optical length TTL from an object side surface of the first lens to an image plane of the camera optical lens along an optic axis is smaller than or equal to 4.95 mm.

18. The camera optical lens as described in claim 17, wherein the total optical length TTL of the camera optical lens is smaller than or equal to 4.72 mm.

19. The camera optical lens as described in claim 1, wherein an F number of the camera optical lens is smaller than or equal to 1.96.

20. The camera optical lens as described in claim 19, wherein the F number of the camera optical lens is smaller than or equal to 1.92.