CAMERA OPTICAL LENS

TECHNICAL FIELD

The present disclosure relates to the field of optical lens, particular, to a camera optical lens suitable for handheld devices, such as smart phones and 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 lens 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 lens structure gradually appears in lens designs. There is an urgent need for an ultra-thin camera optical lens having a long focal length and achieving excellent optical characteristics.

SUMMARY

In view of the problems, the present disclosure aims to provide a camera lens, which can achieve a high imaging performance while satisfying design requirements for ultra-thin, long focal length lenses.

In an embodiment, the present disclosure provides a camera optical lens. The camera optical lens includes, from an object side to an image side: a first lens having a positive refractive power; a second lens; a third lens having a positive refractive power; a fourth lens; and a fifth lens having a negative refractive power. The camera optical lens satisfies following conditions: 0.45≤f3/f≤1.00; 2.50≤d4/d3≤4.50; 1.50≤d7/d8≤3.00; and 2.00≤(R3+R4)/(R3−R4); where f denotes a focal length of the camera optical lens; f3 denotes a focal length of the third lens; d3 denotes an on-axis thickness of the second lens; d4 denotes an on-axis distance from the image-side surface of the second lens to the object-side surface of the third lens; d7 denotes an on-axis thickness of the fourth lens; d8 denotes an on-axis distance from the image-side surface of the fourth lens to the object-side surface of the fifth lens; R3 denotes a curvature radius of the object-side surface of the second lens; and R4 denotes a curvature radius of the image-side surface of the second lens.

The present disclosure can achieve ultra-thin, long focal length lenses having high optical performance and a big aperture, which are especially suitable for camera lens assembly of mobile phones and WEB camera lenses formed by CCD, CMOS and other imaging elements for high pixels.

BRIEF DESCRIPTION OF DRAWINGS

To illustrate the technical solutions according to the embodiments of the present disclosure or in the prior art more clearly, the accompanying drawings for describing the embodiments or the prior art are introduced briefly in the following. Apparently, the accompanying drawings in the following description are only some embodiments of the present disclosure, and persons of ordinary skill in the art can derive other drawings from the accompanying drawings without creative efforts.

FIG. 1 is a schematic diagram of a structure of a camera optical lens according to 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 according to 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 according to 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.

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 according to 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.

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

DETAILED DESCRIPTION OF EMBODIMENTS

The present disclosure will be further described with reference to the accompanying drawings and embodiments in the following.

To make the objects, technical solutions, and advantages of the present disclosure clearer, embodiments of the present disclosure are described in detail with reference to accompanying drawings in the following. A person of ordinary skill in the art can understand that, in the embodiments of the present disclosure, many technical details are provided to make readers better understand the present disclosure. However, even without these technical details and any changes and modifications based on the following embodiments, technical solutions required to be protected by the present disclosure can be implemented.

Embodiment 1

Referring to FIGS. 1-4, the present disclosure provides a camera optical lens 10 of Embodiment 1 of the present disclosure. In FIG. 1, the left side is an object side and the right side is an image side. The camera optical lens 10 includes five lenses, and specifically includes, from the object side to the image side: an aperture S1, a first lens L1, a second lens L2, a third lens L3, a fourth lens L4 and a fifth lens L5. A glass plate GF is provided between the fifth lens L5 and an image surface S1. The glass plate GF may be a glass cover plate or an optical filter.

In an embodiment, the first lens L1 has a positive refractive power; the second lens L2 has a negative refractive power; the third lens L3 has a positive refractive power; the fourth lens L4 has a positive refractive power; the fifth lens L5 has a negative refractive power.

Here, a focal length of the entire camera optical lens is defined as f, a focal length of the third lens L3 is defined as f3, an on-axis thickness of the second lens L2 is defines as d3, 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, an on-axis thickness of the fourth lens L4 is defined as d7, an on-axis distance from the image-side surface of the fourth lens L4 to the object-side surface of the fifth lens L5 is defined as d8, a curvature radius of the object-side surface of the second lens L2 is defined as R3, a curvature radius of the image-side surface of the second lens L2 is defined as R4, and the camera optical lens 10 satisfies the following conditions:

0.45≤f3/f≤1.00 (1)

2.50≤d4/d3≤4.50 (2)

1.50≤d7/d8≤3.00 (3)

2.00≤(R3 +R4)/(R3−R4) (4)

The condition (1) specifies a range of a ratio of the focal length of the third lens to the focal length of the entire camera optical lens. Within this range, the aberration can be effectively corrected, and the imaging quality can be improved.

The condition (2) specifies a range of d4/d3, within which the on-axis thickness of the second lens and the on-axis distance of the image-side surface of the second lens to the object-side surface of the third lens can be effectively distributed, and processing and assembly of the lenses can be facilitated.

The condition (3) specifies a range of d7/d8, within which a long focal length of the lenses can be achieved.

The conditional expression (4) specifies a shape of the second lens. Within the range, a deflection degree of the light passing through the lens can be alleviated to effectively reduce the aberration.

A focal length of the first lens L1 is defined as f1, and the camera optical lens 10 further satisfies a condition of 0.65≤f1/f≤1.00, which specifies a range of a ratio of the focal length of the first lens to the focal length of the entire camera optical lens. Within this range, the aberration can be effectively corrected, and the imaging quality can be improved.

In an embodiment, the object-side surface of the first lens L1 is convex in a paraxial region, and the image-side surface of the first lens L1 is concave in the paraxial region.

A curvature radius of an object-side surface of the first lens L1 is defined as R1, a curvature radius of an image-side surface of the first lens L1 is defined as R2, and the camera optical lens 10 further satisfies a condition of −3.80≤(R1+R2)/(R1−R2)≤−0.49. 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, the camera optical lens 10 further satisfies a condition of −2.38≤(R1+R2)/(R1−R2)≤−0.61.

An on-axis thickness of the first lens L1 is defined as d1, a total optical length from the object side surface of the first lens L1 to an image surface S1 of the camera optical lens along an optical axis is defined as TTL, and the camera optical lens 10 further satisfies a condition of 0.07≤d1/TTL≤0.30. This can facilitate achieving ultra-thin lenses. Preferably, the camera optical lens 10 further satisfies a condition of 0.10≤d1/TTL<0.24.

In an embodiment, an object-side surface of the second lens L2 is convex in the proximal region, and an image-side surface of the second lens L2 is concave in the proximal region.

A focal length of the second lens L2 is defined as f2. The camera optical lens 10 further satisfies a condition of −3.67≤f2/f≤34.95. By controlling a negative power of the second lens L2 within a reasonable range, correction of the aberration of the optical system can be facilitated. Preferably, the camera optical lens 10 further satisfies a condition of −2.29≤f2/f≤27.96.

An on-axis thickness of the second lens L2 is defines as d3, and the camera optical lens 10 further satisfies a condition of 0.02≤d3/TTL≤0.11. This can facilitate achieving ultra-thin lenses. Preferably, the camera optical lens 10 further satisfies a condition of 0.03≤d3/TTL<0.09.

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

A curvature radius of the object-side surface of the third lens L3 is defined as R5, a curvature radius of the image-side surface of the third lens L3 is defined as R6, and the camera optical lens 10 further satisfies a condition of 0.17≤(R5+R6)/(R5−R6)≤2.65, which specifies a shape of the third lens L3, thereby facilitating shaping of the third lens L3. Within this range, a deflection degree of the light passing through the lens can be alleviated to effectively reduce the aberration. Preferably, the camera optical lens 10 further satisfies a condition of 0.27≤(R5+R6)/(R5−R6)≤2.12.

An on-axis thickness of the third lens L3 is defined as d5, and the camera optical lens 10 further satisfies a condition of 0.06≤d5/TTL≤0.28. This can facilitate achieving ultra-thin lenses. Preferably, the camera optical lens 10 further satisfies a condition of 0.10≤d5/TTL≤0.22.

In an embodiment, an object-side surface of the fourth lens L4 is convex in the proximal region, and an image-side surface of the fourth lens L4 is convex in the proximal region.

A focal length of the fourth lens L4 is defined as f4, and the camera optical lens 10 further satisfies a condition of −5.37≤f4/f≤9.68. The appropriate distribution of refractive power makes it possible that the system has the better imaging quality and the lower sensitivity. Preferably, the camera optical lens 10 further satisfies a condition of −3.36≤f4/f≤7.74.

A curvature radius of the object-side surface of the fourth lens L4 is defined as R7, a curvature radius of the image-side surface of the fourth lens L4 is defined as R8, and the camera optical lens 10 further satisfies a condition of −7.12≤(R7+R8)/(R7−R8)≤1.69, which specifies a shape of the fourth lens L4. Within this range, a development towards ultra-thin lens would facilitate correcting a problem like an off-axis aberration. Preferably, the camera optical lens 10 further satisfies a condition of −4.45≤(R7+R8)/(R7−R8)<1.35.

An on-axis thickness of the fourth lens L4 is defined as d7, and the camera optical lens 10 further satisfies a condition of 0.04≤d7/TTL≤0.41. This can facilitate achieving ultra-thin lenses. Preferably, the camera optical lens 10 further satisfies a condition of 0.07≤d7/TTL≤0.33.

In an embodiment, an object-side surface of the fifth lens L5 is concave in the proximal region, and an image-side surface of the fifth lens L5 is concave in the proximal region.

A focal length of the fifth lens L5 is defined as f5, and the camera optical lens 10 further satisfies a condition of −1.47≤f5/f≤−0.32, which can effectively make a light angle of the camera lens gentle and reduce a tolerance sensitivity. Preferably, the camera optical lens 10 further satisfies a condition of −0.92≤f5/f<−0.40.

A curvature radius of the object-side surface of the fifth lens L5 is defined as R9, a curvature radius of the image-side surface of the fifth lens L5 is defined as R10, and the camera optical lens 10 further satisfies a condition of −1.96≤(R9+R10)/(R9−R10)≤1.06, which specifies a shape of the fifth lens L5. Within this range, processing of the lenses is facilitated. Preferably, the camera optical lens 10 further satisfies a condition of −1.22≤(R9+R10)/(R9−R10)≤0.84.

An on-axis thickness of the fifth lens L5 is defined as d9, and the camera optical lens 10 further satisfies a condition of 0.02≤d9/TTL≤0.07. This can facilitate achieving ultra-thin lenses. Preferably, the camera optical lens 10 further satisfies a condition of 0.03≤d9/TTL≤0.06.

In an embodiment, the camera optical lens 10 further satisfies a condition of TTL/f≤1.36, so as to achieve ultra-thin lenses.

In an embodiment, an image height of the entire camera optical lens 10 is defined as IH, and the camera optical lens 10 further satisfies a condition of f/IH≥2.00, so as to achieve a long focal length of the lenses.

In an embodiment, an F number Fno of the camera optical lens 10 is less than or equal to 1.57, such that the camera optical lens 10 has a large aperture and a better imaging performance.

In an embodiment, a combined focal length of the first lens L1 and the second lens L2 is defined as f12, and the camera optical lens 10 further satisfies a condition of 0.45≤f12/f≤2.29. Within this range, the aberration and distortion of the camera optical lens 10 can be eliminated, and a back focal length of the camera optical lens 10 can be suppressed to maintain the miniaturization of the image lens system. Preferably, the camera optical lens 10 further satisfies a condition of 0.73≤f12/f≤1.83.

In addition, in the camera optical lens 10 provided in an embodiment, the surface of each lens may be aspherical. The aspherical surface can be easily made into a shape other than a spherical surface, and more control variables can be obtained to reduce aberration and thus to reduce the number of lenses, so that the total length of the camera optical lens 10 can be effectively reduced. In an embodiment, both the object-side surface and the image-side surface of each lens are aspherical.

It should be appreciated that since the first lens L1, the second lens L2, the third lens L3, the fourth lens L4, and the fifth lens L5 have the aforementioned structure and parameter relationships, the optical powers, intervals, and shapes of the respective lenses in the camera optical lens 10 can be reasonably distributed, and thus various types of aberrations are corrected.

In addition, inflexion points and/or arrest points can be arranged on at least one of the object-side surface and the image-side surface of each lens, so as to satisfy the demand for high quality imaging. The description below can be referred for specific implementations.

The design data of the camera optical lens 10 in Embodiment 1 of the present disclosure are shown as follows.

Table 1 shows the curvature radiuses of the object-side surfaces and the image-side surfaces, the on-axis thicknesses, the on-axis distances d between adjacent lenses, the refractive indexes nd and the abbe number vd of the first to fifth lenses (L1 to L5) constituting the camera optical lens 10 in Embodiment 1 of the present disclosure. It should be noted that 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 surface of the camera optical lens along the optical axis) in mm.

TABLE 1

R
d
nd
νd

S1
∞
d0=
−0.689

R1
2.013
d1=
1.087
nd1
1.5450
ν1
55.81

R2
53.837
d2=
0.181

R3
1.447
d3=
0.293
nd2
1.6700
ν2
19.39

R4
0.989
d4=
1.071

R5
−28.298
d5=
1.008
nd3
1.5450
ν3
55.81

R6
−1.557
d6=
0.030

R7
26.429
d7=
0.474
nd4
1.6700
ν4
19.39

R8
−67.710
d8=
0.208

R9
−1.516
d9=
0.230
nd5
1.5450
ν5
55.81

R10
145.993
d10=
0.150

R11
∞
d11=
0.210
ndg
1.5168
νg
64.17

R12
∞
d12=
0.537

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 an object-side surface of the optical filter GF;

R12: 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 lens;

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 optical filter GF;

d11: on-axis thickness of the optical filter GF;

d12: on-axis distance from the image-side surface to the image surface of the optical filter GF;

nd: refractive index of the d line;

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

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

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

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

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

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

νd: abbe number;

ν1: abbe number of the first lens L1;

ν2: abbe number of the second lens L2;

ν3: abbe number of the third lens L3;

ν4: abbe number of the fourth lens L4;

ν5: abbe number of the fifth lens L5;

νg: 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
Aspheric surface coefficients

k
A4
A6
A8
A10

R1
−1.0738E−01
8.9992E−04
6.1127E−03
−1.8070E−02
3.0493E−02

R2
−9.8969E+01
−7.5424E−02
1.8137E−01
−2.7643E−01
2.9852E−01

R3
−6.2266E+00
−7.2506E−03
−5.5290E−02
1.4881E−01
−2.6193E−01

R4
−3.1306E+00
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

R5
−1.9085E+01
−1.6194E−02
1.5514E−02
−4.9330E−02
1.1057E−01

R6
−5.7367E+00
−5.7367E−02
−2.5978E−02
9.7586E−02
−1.3345E−01

R7
1.1749E+00
5.2915E−03
−3.8605E−02
−2.5704E−02
7.9035E−02

R8
7.1678E+01
−6.3461E−02
1.4507E−01
−2.4620E−01
2.0495E−01

R9
−5.5434E+00
5.4923E−02
−2.9628E−02
−3.7180E−02
7.4275E−02

R10
−9.8185E+01
1.2264E−01
−2.0722E−01
1.8484E−01
−9.7280E−02

Aspheric surface coefficients

A12
A14
A16
A18
A20

R1
−3.0969E−02
1.9509E−02
−7.4486E−03
1.5814E−03
−1.4378E−04

R2
−2.2488E−01
1.1448E−01
−3.7393E−02
7.0601E−03
−5.8624E−04

R3
2.9611E−01
−2.1560E−01
9.7171E−02
−2.4631E−02
2.6866E−03

R4
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

R5
−1.4217E−01
1.1229E−01
−5.2652E−02
1.3337E−02
−1.3975E−03

R6
1.1896E−01
−7.0617E−02
2.6913E−02
−5.8933E−03
5.5692E−04

R7
−9.3936E−02
5.9538E−02
−2.0728E−02
3.7690E−03
−2.8058E−04

R8
−1.0365E−01
3.4025E−02
−7.1987E−03
8.9484E−04
−4.9151E−05

R9
−4.9726E−02
1.7440E−02
−3.4542E−03
3.6624E−04
−1.6144E−05

R10
3.1649E−02
−6.4174E−03
7.7878E−04
−5.0891E−05
1.3510E−06

In table 2, K is a conic coefficient, and A4, A6, A8, A10, A12, A14, A16, A18 and A20 are aspheric surface coefficients.

IH: Image height

y=(x²/R)/[1+{1−(k+1)(x²/R²)}^1/2]+A4x⁴+A6x⁶+A8x⁸+A10x¹⁰A12x¹²+A14x¹⁴+A16x¹⁶+A18x¹⁸+A20x²⁰ (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 each lens of the camera optical lens 10 according to the present embodiment. 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. The data in the column named “inflexion point position” refer 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” refer to vertical distances from arrest points arranged on each lens surface to the optical axis of the camera optical lens 10.

TABLE 3

Number(s) of
Inflexion point
Inflexion point
Inflexion point

inflexion points
position 1
position 2
position 3

P1R1
0

P1R2
3
0.155
0.685
1.305

P2R1
1
0.795

P2R2
0

P3R1
1
0.995

P3R2
1
1.265

P4R1
3
0.455
1.605
1.775

P4R2
1
1.785

P5R1
3
0.905
1.645
1.985

P5R2
2
1.365
2.205

TABLE 4

Number(s) of
Arrest point
Arrest point
Arrest point

arrest points
position 1
position 2
position 3

P1R1
0

P1R2
3
0.285
1.005
1.435

P2R1
0

P2R2
0

P3R1
1
1.285

P3R2
1
1.645

P4R1
1
0.665

P4R2
0

P5R1
1
2.095

P5R2
1
1.685

In addition, in the subsequent Table 17, various parameters of Embodiments 1 and values corresponding to the parameters specified in the above conditions are shown.

FIG. 2 and FIG. 3 illustrate a longitudinal aberration and a lateral color with wavelengths of 430 nm, 510 nm, 578 nm, 588 nm, 610 nm and 650 nm after passing the camera optical lens 10, respectively. FIG. 4 illustrates a field curvature and a distortion with a wavelength of 588 nm after passing the camera optical lens 10. A field curvature S in FIG. 4 is a field curvature in a sagittal direction, and T is a field curvature in a tangential direction.

In this Embodiment, an entrance pupil diameter of the camera optical lens 10 is 3.096 mm, an image height of 1.0 H is 2.04 mm, and an FOV (field of view) in a diagonal direction is 49.39°. Thus, the camera optical lens 10 has a large aperture and a long focal length, and is ultra-thin, thereby achieving excellent optical characteristics.

Embodiment 2

FIG. 5 is a schematic diagram of a structure of a camera optical lens 20 according to 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.

An object-side surface of the third lens L3 is convex in the proximal region, and an object-side surface of the fourth lens L4 is concave in the proximal region.

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=
−0.468

R1
2.207
d1=
0.752
nd1
1.5450
ν1
55.81

R2
55.349
d2=
0.489

R3
10.215
d3=
0.421
nd2
1.6700
ν2
19.39

R4
3.419
d4=
1.061

R5
6.601
d5=
1.015
nd3
1.5450
ν3
55.81

R6
−3.310
d6=
0.061

R7
−58.098
d7=
0.708
nd4
1.6700
ν4
19.39

R8
−3.447
d8=
0.238

R9
−7.689
d9=
0.230
nd5
1.5450
ν5
55.81

R10
1.337
d10=
0.350

R11
∞
d11=
0.210
ndg
1.5168
νg
64.17

R12
∞
d12=
0.243

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
Aspheric surface coefficients

k
A4
A6
A8
A10

R1
−1.3808E−02
1.1022E−05
1.3438E−02
−4.0097E−02
7.8845E−02

R2
9.7971E+01
−4.7749E−03
4.3658E−03
−6.1504E−03
1.7159E−02

R3
−5.6730E+01
−6.1408E−02
1.6309E−02
−4.4342E−03
5.7954E−03

R4
−1.1069E+01
−2.8568E−02
2.0155E−02
−3.6293E−02
9.9489E−02

R5
−9.8829E+01
2.1209E−02
−5.8141E−02
8.0592E−02
−1.0078E−01

R6
−8.1459E−01
−1.1470E−01
1.1720E−01
−9.6080E−02
4.5915E−02

R7
8.2966E+01
−6.9805E−02
1.0303E−01
−1.6445E−01
1.8426E−01

R8
−2.4219E+01
1.1984E−01
−1.6193E−01
5.4547E−02
5.5002E−02

R9
8.8594E+00
−4.8325E−02
−2.1097E−01
2.0392E−01
−1.3609E−02

R10
−3.0012E+00
−2.1055E−01
1.0790E−01
−2.6845E−02
1.8391E−03

Aspheric surface coefficients

A12
A14
A16
A18
A20

R1
−9.5902E−02
7.3525E−02
−3.4646E−02
9.1888E−03
−1.0586E−03

R2
−3.1093E−02
3.1609E−02
−1.8497E−02
5.8167E−03
−7.7248E−04

R3
−1.6262E−02
2.2973E−02
−1.7261E−02
6.7850E−03
−1.1058E−03

R4
−1.6431E−01
1.6951E−01
−1.0492E−01
3.5910E−02
−5.1695E−03

R5
8.8708E−02
−5.1769E−02
1.8776E−02
−3.7282E−03
3.0684E−04

R6
−1.1538E−02
−6.4410E−04
1.6892E−03
−5.6649E−04
6.9867E−05

R7
−1.4347E−01
6.9741E−02
−1.9889E−02
2.9205E−03
−1.6209E−04

R8
−6.9259E−02
3.2394E−02
−7.7377E−03
9.3690E−04
−4.5680E−05

R9
−7.1458E−02
4.5772E−02
−1.2915E−02
1.7872E−03
−9.8766E−05

R10
−6.0494E−05
4.0625E−04
−1.5840E−04
2.2604E−05
−1.1468E−06

Table 7 and table 8 show design data of inflexion points and arrest points of each lens of the camera optical lens 20.

TABLE 7

Number(s) of
Inflexion point
Inflexion point
Inflexion point

inflexion points
position 1
position 2
position 3

P1R1
0

P1R2
1
0.945

P2R1
1
0.365

P2R2
0

P3R1
2
0.685
1.345

P3R2
1
1.525

P4R1
0

P4R2
0

P5R1
2
1.285
1.905

P5R2
3
0.545
1.625
1.815

TABLE 8

Number of
Arrest point
Arrest point

arrest points
position 1
position 2

P1R1
0

P1R2
1
1.175

P2R1
1
0.645

P2R2
0

P3R1
2
1.115
1.465

P3R2
0

P4R1
0

P4R2
0

P5R1
0

P5R2
1
1.455

In addition, in the subsequent Table 17, various parameters of Embodiments 2 and values corresponding to the parameters specified in the above conditions are shown.

FIG. 6 and FIG. 7 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 430 nm, 510 nm, 578 nm, 588 nm, 610 nm and 650 nm after passing the camera optical lens 20. FIG. 8 illustrates a field curvature and a distortion of light with a wavelength of 588 nm after passing the camera optical lens 20. A field curvature S in FIG. 8 is a field curvature in a sagittal direction, and T is a field curvature in a tangential direction.

In an embodiment, an entrance pupil diameter of the camera optical lens 20 is 2.735 mm, an image height of 1.0 H is 2.04 mm, and an FOV (field of view) in the diagonal direction is 49.54°. Thus, the camera optical lens 20 has a large aperture and a long focal length, and is ultra-thin, thereby achieving excellent optical characteristics.

Embodiment 3

FIG. 9 is a schematic diagram of a structure of a camera optical lens 30 according to 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.

In an embodiment, the fourth lens L4 has a negative refractive power.

An image-side surface of the first lens L1 is convex in the proximal region, and an object-side surface of the fourth lens L4 is concave in the proximal region.

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=
−0.802

R1
1.950
d1=
1.162
nd1
1.5450
ν1
55.81

R2
−12.616
d2=
0.164

R3
2.520
d3=
0.262
nd2
1.6700
ν2
19.39

R4
1.322
d4=
1.175

R5
−16.504
d5=
0.744
nd3
1.5450
ν3
55.81

R6
−1.144
d6=
0.030

R7
−1.585
d7=
0.749
nd4
1.6700
ν4
19.39

R8
−2.834
d8=
0.493

R9
−2.661
d9=
0.287
nd5
1.5450
ν5
55.81

R10
4.041
d10=
0.250

R11
∞
d11=
0.210
ndg
1.5168
νg
64.17

R12
∞
d12=
0.252

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
Aspheric surface coefficients

k
A4
A6
A8
A10

R1
−1.5570E−01
1.4177E−03
−7.1798E−04
1.1153E−03
−1.1425E−03

R2
−9.9000E+01
−2.7328E−02
8.9462E−02
−1.3857E−01
1.4242E−01

R3
−1.0314E+01
−1.1525E−01
1.8561E−01
−2.1511E−01
1.9000E−01

R4
−3.4326E+00
−3.8714E−02
1.2594E−01
−5.7228E−02
−1.3846E−01

R5
9.9000E+01
−3.0311E−02
5.4002E−02
−1.7115E−01
3.3270E−01

R6
−1.3852E+01
2.6788E−01
−1.0751E+00
1.8764E+00
−2.1093E+00

R7
−2.8671E+01
3.2405E−01
−1.1118E+00
1.8819E+00
−2.1722E+00

R8
−6.4068E+00
5.6447E−02
−1.4291E−01
1.1749E−01
−6.8022E−02

R9
−1.5889E+00
9.4722E−02
−2.5418E−01
2.8687E−01
−1.9084E−01

R10
−1.6547E+01
1.0857E−02
−1.0989E−01
1.2980E−01
−8.4164E−02

Aspheric surface coefficients

A12
A14
A16
A18
A20

R1
7.1047E−04
−2.6474E−04
4.5301E−05
−1.7688E−07
−8.4003E−07

R2
−9.9511E−02
4.6380E−02
−1.3756E−02
2.3436E−03
−1.7437E−04

R3
−1.2185E−01
5.5655E−02
−1.7420E−02
3.4207E−03
−3.1974E−04

R4
4.1880E−01
−5.4323E−01
4.0669E−01
−1.6894E−01
3.0767E−02

R5
−3.9468E−01
2.9166E−01
−1.3036E−01
3.2288E−02
−3.3957E−03

R6
1.6322E+00
−8.7076E−01
3.0675E−01
−6.4080E−02
5.9632E−03

R7
1.7626E+00
−9.9334E−01
3.6892E−01
−8.0803E−02
7.8498E−03

R8
3.1638E−02
−1.2577E−02
3.8726E−03
−7.5813E−04
6.7608E−05

R9
8.4061E−02
−2.5026E−02
4.8419E−03
−5.4440E−04
2.6719E−05

R10
3.4686E−02
−9.3272E−03
1.5830E−03
−1.5368E−04
6.5252E−06

Table 11 and Table 12 show design data inflexion points and arrest points of each lens in the camera optical lens 30.

TABLE 11

Number(s) of
Inflexion point
Inflexion point

inflexion points
position 1
position 2

P1R1
0

P1R2
2
0.795
1.515

P2R1
0

P2R2
0

P3R1
1
1.165

P3R2
0

P4R1
0

P4R2
1
1.645

P5R1
1
1.375

P5R2
2
0.625
1.855

TABLE 12

Number of
Arrest point
Arrest point

arrest points
position 1
position 2

P1R1
0

P1R2
0

P2R1
0

P2R2
0

P3R1
1
1.395

P3R2
0

P4R1
0

P4R2
0

P5R1
1
1.885

P5R2
2
1.405
2.005

In addition, in the subsequent Table 17, various parameters of Embodiments 3 and values corresponding to the parameters specified in the above conditions are shown.

FIG. 10 and FIG. 11 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 430 nm, 510 nm, 578 nm, 588 nm, 610 nm and 650 nm after passing the camera optical lens 30. FIG. 12 illustrates a field curvature and a distortion of light with a wavelength of 588 nm after passing the camera optical lens 30. A field curvature S in FIG. 12 is a field curvature in a sagittal direction, and T is a field curvature in a tangential direction.

In an embodiment, an entrance pupil diameter of the camera optical lens 30 is 3.247 mm, an image height of 1.0 H is 2.04 mm, and an FOV (field of view) in the diagonal direction is 44.00°. Thus, the camera optical lens 30 has a large aperture and a long focal length, and is ultra-thin, thereby achieving excellent optical characteristics.

Embodiment 4

FIG. 13 is a schematic diagram of a structure of a camera optical lens 40 according to 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.

In an embodiment, the fourth lens L4 has a negative refractive power, the second lens L2 has a positive refractive power, and an object-side surface of the fourth lens L4 is concave in the proximal region.

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

TABLE 13

R
d
nd
νd

S1
∞
d0=
−0.738

R1
1.878
d1=
1.010
nd1
1.5450
ν1
55.81

R2
6.047
d2=
0.083

R3
1.993
d3=
0.230
nd2
1.6700
ν2
19.39

R4
1.953
d4=
0.633

R5
−6.409
d5=
0.768
nd3
1.5450
ν3
55.81

R6
−1.778
d6=
0.030

R7
−2.492
d7=
1.595
nd4
1.6700
ν4
19.39

R8
−4.437
d8=
0.535

R9
−4.647
d9=
0.230
nd5
1.5450
ν5
55.81

R10
3.224
d10=
0.300

R11
∞
d11=
0.210
ndg
1.5168
νg
64.17

R12
∞
d12=
0.155

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
Aspheric surface coefficients

k
A4
A6
A8
A10

R1
−5.9529E−02
1.2659E−03
2.6961E−03
−7.5823E−03
1.4055E−02

R2
−9.9000E+01
−6.2761E−02
7.6249E−02
−4.8466E−02
−2.0835E−03

R3
−7.5201E+00
−2.1194E−02
−3.3520E−02
8.9199E−02
−1.5089E−01

R4
−4.0346E+00
3.5950E−02
−8.5609E−02
1.1938E−01
−5.5041E−02

R5
−8.7808E+00
−9.0973E−03
−1.7138E−02
5.1502E−02
−1.6378E−01

R6
−5.6223E+00
1.1526E−01
−6.1855E−01
1.2299E+00
−1.6670E+00

R7
−1.6483E+01
3.4343E−02
−4.2884E−01
8.2772E−01
−1.0377E+00

R8
−4.5100E+01
−4.7934E−02
3.1691E−02
−3.9073E−02
3.8186E−02

R9
1.8045E+00
−9.6021E−02
1.0999E−02
3.1029E−02
−2.6991E−02

R10
−1.5072E+01
−7.6102E−02
1.2461E−02
2.0437E−02
−2.3878E−02

Aspheric surface coefficients

A12
A14
A16
A18
A20

R1
−1.5929E−02
1.1233E−02
−4.8123E−03
1.1439E−03
−1.1612E−04

R2
3.7087E−02
−3.6191E−02
1.7558E−02
−4.4413E−03
4.6446E−04

R3
1.9881E−01
−1.7095E−01
9.0234E−02
−2.6433E−02
3.2365E−03

R4
−7.4336E−02
2.0321E−01
−2.0119E−01
9.8195E−02
−1.8980E−02

R5
3.2751E−01
−3.8704E−01
2.7292E−01
−1.0535E−01
1.7189E−02

R6
1.5798E+00
−1.0150E+00
4.1527E−01
−9.6799E−02
9.6973E−03

R7
8.2393E−01
−3.5976E−01
3.5471E−02
3.2433E−02
−9.5955E−03

R8
−2.5237E−02
1.1308E−02
−3.3186E−03
5.7226E−04
−4.2441E−05

R9
9.6899E−03
2.5595E−05
−1.3553E−03
4.4089E−04
−4.4551E−05

R10
1.3019E−02
−4.2395E−03
8.2210E−04
−8.6969E−05
3.8521E−06

Table 15 and table 16 show design data of inflexion points and arrest points of each lens of the camera optical lens 40.

TABLE 15

Number(s) of
Inflexion point
Inflexion point
Inflexion point

inflexion points
position 1
position 2
position 3

P1R1
0

P1R2
3
0.475
1.035
1.315

P2R1
1
1.285

P2R2
0

P3R1
1
1.005

P3R2
0

P4R1
0

P4R2
1
1.465

P5R1
1
1.595

P5R2
1
0.515

TABLE 16

Number of
Arrest point

arrest points
position 1

P1R1
0

P1R2
0

P2R1
0

P2R2
0

P3R1
1
1.215

P3R2
0

P4R1
0

P4R2
0

P5R1
0

P5R2
1
1.015

In addition, in the subsequent Table 17, various parameters of Embodiments 4 and values corresponding to the parameters specified in the above conditions are shown.

FIG. 14 and FIG. 15 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 430 nm, 510 nm, 578 nm, 588 nm, 610 nm and 650 nm after passing the camera optical lens 40. FIG. 16 illustrates a field curvature and a distortion of light with a wavelength of 588 nm after passing the camera optical lens 40. A field curvature S in FIG. 16 is a field curvature in a sagittal direction, and T is a field curvature in a tangential direction.

In an embodiment, an entrance pupil diameter of the camera optical lens 40 is 3.023 mm, an image height of 1.0 H is 2.04 mm, and an FOV (field of view) in the diagonal direction is 45.80°. Thus, the camera optical lens 40 has a large aperture and a long focal length, and is ultra-thin, thereby achieving excellent optical characteristics.

Table 17 in the following shows values corresponding to the conditions and values of other relevant parameters according to the aforementioned conditions in the Embodiment 1, Embodiment 2, Embodiment 3, and Embodiment 4.

TABLE 17

Parameters and conditions

Embod-
Embod-
Embod-
Embod-

iment 1
iment 2
iment 3
iment 4

f
4.395
4.279
4.887
4.694

f1
3.805
4.193
3.186
4.600

f2
−6.272
−7.844
−4.542
109.365

f3
2.981
4.193
2.215
4.260

f4
28.353
5.426
−7.058
−12.614

f5
−2.749
−2.069
−2.897
−3.454

f12
5.793
6.536
5.669
4.257

Fno
1.42
1.56
1.51
1.55

f3/f
0.68
0.98
0.45
0.91

d4/d3
3.66
2.52
4.49
2.75

d7/d8
2.28
2.98
1.52
2.98

(R3 + R4)/
5.32
2.01
3.21
98.65

(R3 − R4)

Although the disclosure is illustrated and described herein with reference to specific embodiments, the disclosure is not intended to be limited to the details shown. Rather, various modifications may be made in the details within the scope and range of equivalents of the claims and without departing from the disclosure.

CAMERA OPTICAL LENS

Information

Publication Number

Date Filed

Date Published

Inventors

Original Assignees

CPC

International Classifications

Abstract

Description

Claims

Priority Claims (1)