Optical Imaging Lens

CROSS-REFERENCE TO RELATED APPLICATIONS

The disclosure claims priority to and the benefit of Chinese Patent Application No. 201910231446.8, filed in the China National Intellectual Property Administration (CHIPA) on Mar. 26, 2019, which is incorporated herein by reference in its entirety.

TECHNICAL FIELD

The disclosure relates to an optical imaging lens, and more particularly to an optical imaging lens including seven lenses.

BACKGROUND

Recently, with the booming of the field of smart phones, various major smart phone producers have made more new requirements on mobile phone lenses, and particularly for main cameras of high-end flagship phones, imaging lenses of mobile phones have been increasingly developed to large image surfaces, wide angles, large apertures and ultrathin designs, which poses greater challenges to design of optical systems.

Changes of these principal value parameters of a conventional mobile phone lens greatly improve imaging capabilities and competitive advantages of the mobile phone lens. A large image surface means a higher resolution. A wide angle means a larger field of view. A large aperture represents a higher effective luminous flux and a higher signal-to-noise ratio. An ultrathin design may achieve higher compatibility with a smart phone and make the smart phone convenient to carry. Based on these requirement challenges posed by mobile phone suppliers, a conventional five- or six-element lens structure cannot effectively meet these challenges, and seven lenses optical imaging lens systems may gradually become a mainstream.

SUMMARY

Some embodiments of the disclosure provide an optical imaging lens applicable to a portable electronic product and capable of at least overcoming or partially overcoming at least one shortcoming in a related art.

The disclosure provides an optical imaging lens, which may sequentially include, from an object side to an image side along an optical axis: a first lens with refractive power; a second lens with positive refractive power; a third lens with positive refractive power, wherein an image-side surface thereof is a convex surface; a fourth lens with refractive power, wherein an object-side surface thereof is a concave surface; a fifth lens with positive refractive power, wherein an object-side surface thereof is a concave surface; a sixth lens with refractive power; and a seventh lens with refractive power.

In an implementation mode, a total effective focal length f of the optical imaging lens and a curvature radius R4 of an image-side surface of the second lens may meet 0.6<R4/f<1.5.

In an implementation mode, a maximum field of view (FOV) of the optical imaging lens may meet FOV>90°.

In an implementation mode, TTL is a distance from an object-side surface of the first lens to an imaging surface of the optical imaging lens on the optical axis, and ImgH is a half of a diagonal length of an effective pixel region on the imaging surface of the optical imaging lens, TTL and ImgH meet 0.55<TTL/(ImgH×2)<0.75.

In an implementation mode, the total effective focal length f of the optical imaging lens and an effective focal length f2 of the second lens may meet 0<f/f2<0.8.

In an implementation mode, the total effective focal length f of the optical imaging lens and an effective focal length f3 of the third lens may meet 0.2<f/f3<0.7.

In an implementation mode, a maximum effective radius DT11 of the object-side surface of the first lens and a maximum effective radius DT71 of an object-side surface of the seventh lens may meet 0.2<DT11/DT71<0.7.

In an implementation mode, a center thickness CT3 of the third lens on the optical axis and an air space T23 of the second lens and the third lens on the optical axis may meet 0.1<T23/CT3<0.9.

In an implementation mode, an air space T12 of the first lens and the second lens on the optical axis and an air space T34 of the third lens and the fourth lens on the optical axis may meet 0<T12/T34<0.4.

In an implementation mode, an effective focal length f5 of the fifth lens and a curvature radius R9 of the object-side surface of the fifth lens may meet −1<f5/R9<0.

In an implementation mode, a curvature radius R7 of the object-side surface of the fourth lens and a curvature radius R8 of an image-side surface of the fourth lens may meet 0<|R8−R7|/|R8+R7|≤0.5.

In an implementation mode, the total effective focal length f of the optical imaging lens and a curvature radius R6 of an image-side surface of the third lens may meet −1<f/R6<−0.5.

In an implementation mode, the total effective focal length f of the optical imaging lens and an entrance pupil diameter (EPD) of the optical imaging lens may meet f/EPD<2.

In an implementation mode, a curvature radius R13 of an object-side surface of the seventh lens and a curvature radius R14 of an image-side surface of the seventh lens may meet 0.4<R14/R13<0.9.

According to the disclosure, the seven lenses are adopted, and the refractive power and surface types of each lens, the center thickness of each lens, on-axis distances between the lenses and the like are reasonably configured to achieve at least one beneficial effect of large image surface, wide angle, large aperture, ultrathin design and the like of the optical imaging lens.

BRIEF DESCRIPTION OF THE DRAWINGS

Detailed descriptions are made to unrestrictive implementation modes below in combination with the drawings to make the other characteristics, purposes and advantages of the disclosure more apparent. In the drawings:

FIG. 1 shows a structure diagram of an optical imaging lens according to embodiment 1 of the disclosure;

FIG. 2A to FIG. 2D show a longitudinal aberration curve, an astigmatism curve, a distortion curve and a lateral color curve of an optical imaging lens according to embodiment 1 respectively;

FIG. 3 shows a structure diagram of an optical imaging lens according to embodiment 2 of the disclosure;

FIG. 4A to FIG. 4D show a longitudinal aberration curve, an astigmatism curve, a distortion curve and a lateral color curve of an optical imaging lens according to embodiment 2 respectively;

FIG. 5 shows a structure diagram of an optical imaging lens according to embodiment 3 of the disclosure;

FIG. 6A to FIG. 6D show a longitudinal aberration curve, an astigmatism curve, a distortion curve and a lateral color curve of an optical imaging lens according to embodiment 3 respectively;

FIG. 7 shows a structure diagram of an optical imaging lens according to embodiment 4 of the disclosure;

FIG. 8A to FIG. 8D show a longitudinal aberration curve, an astigmatism curve, a distortion curve and a lateral color curve of an optical imaging lens according to embodiment 4 respectively;

FIG. 9 shows a structure diagram of an optical imaging lens according to embodiment 5 of the disclosure;

FIG. 10A to FIG. 10D show a longitudinal aberration curve, an astigmatism curve, a distortion curve and a lateral color curve of an optical imaging lens according to embodiment 5 respectively;

FIG. 11 shows a structure diagram of an optical imaging lens according to embodiment 6 of the disclosure;

FIG. 12A to FIG. 12D show a longitudinal aberration curve, an astigmatism curve, a distortion curve and a lateral color curve of an optical imaging lens according to embodiment 6 respectively;

FIG. 13 shows a structure diagram of an optical imaging lens according to embodiment 7 of the disclosure;

FIG. 14A to FIG. 14D show a longitudinal aberration curve, an astigmatism curve, a distortion curve and a lateral color curve of an optical imaging lens according to embodiment 7 respectively;

FIG. 15 shows a structure diagram of an optical imaging lens according to embodiment 8 of the disclosure;

FIG. 16A to FIG. 16D show a longitudinal aberration curve, an astigmatism curve, a distortion curve and a lateral color curve of an optical imaging lens according to embodiment 8 respectively;

FIG. 17 shows a structure diagram of an optical imaging lens according to embodiment 9 of the disclosure;

FIG. 18A to FIG. 18D show a longitudinal aberration curve, an astigmatism curve, a distortion curve and a lateral color curve of an optical imaging lens according to embodiment 9 respectively;

FIG. 19 shows a structure diagram of an optical imaging lens according to embodiment 10 of the disclosure;

FIG. 20A to FIG. 20D show a longitudinal aberration curve, an astigmatism curve, a distortion curve and a lateral color curve of an optical imaging lens according to embodiment 10 respectively;

FIG. 21 shows a structure diagram of an optical imaging lens according to embodiment 11 of the disclosure;

FIG. 22A to FIG. 22D show a longitudinal aberration curve, an astigmatism curve, a distortion curve and a lateral color curve of an optical imaging lens according to embodiment 11 respectively;

FIG. 23 shows a structure diagram of an optical imaging lens according to embodiment 12 of the disclosure;

FIG. 24A to FIG. 24D show a longitudinal aberration curve, an astigmatism curve, a distortion curve and a lateral color curve of an optical imaging lens according to embodiment 12 respectively.

DETAILED DESCRIPTION OF THE EMBODIMENTS

For understanding the disclosure better, more detailed descriptions will be made to each aspect of the disclosure with reference to the drawings. It is to be understood that these detailed descriptions are only descriptions about the exemplary implementation modes of the disclosure and not intended to limit the scope of the disclosure in any manner. In the whole specification, the same reference sign numbers represent the same components. Expression “and/or” includes any or all combinations of one or more in associated items that are listed.

It should be noted that, in this description, the expressions of first, second, third, etc. are only used to distinguish one feature from another feature, and do not represent any limitation to the feature. Thus, a first lens discussed below could also be referred to as a second lens or a third lens without departing from the teachings of the disclosure.

In the drawings, the thickness, size and shape of the lens have been slightly exaggerated for ease illustration. In particular, a spherical shape or an aspherical shape shown in the drawings is shown by some embodiments. That is, the spherical shape or the aspherical shape is not limited to the spherical shape or the aspherical shape shown in the drawings. The drawings are by way of example only and not strictly to scale.

Herein, a paraxial region refers to a region nearby an optical axis. If a lens surface is a convex surface and a position of the convex surface is not defined, it indicates that the lens surface is a convex surface at least in the paraxial region; and if the lens surface is a concave surface and a position of the concave surface is not defined, it indicates that the lens surface is a concave surface at least in the paraxial region. A surface of each lens closest to an object-side is called an object-side surface of the lens, and a surface of each lens closest to an imaging surface is called an image-side surface of the lens.

It should also be understood that terms “include”, “including”, “have”, “contain” and/or “containing”, used in the specification, represent existence of a stated characteristic, component and/or part but do not exclude existence or addition of one or more other characteristics, components and parts and/or combinations thereof. In addition, expressions like “at least one in . . . ” may appear after a list of listed characteristics not to modify an individual component in the list but to modify the listed characteristics. Moreover, when the implementation modes of the disclosure are described, “may” is used to represent “one or more implementation modes of the disclosure”. Furthermore, term “exemplary” refers to an example or exemplary description.

Unless otherwise defined, all terms (including technical terms and scientific terms) used in the disclosure have the same meanings usually understood by those of ordinary skill in the art of the disclosure. It should also be understood that the terms (for example, terms defined in a common dictionary) should be explained to have meanings consistent with the meanings in the context of a related art and may not be explained with ideal or excessively formal meanings, unless clearly defined like this in the disclosure.

It should be noted that the embodiments in the disclosure and features in the embodiments can be combined without conflicts. The disclosure will be described below with reference to the drawings and in combination with the embodiments in detail.

The features, principles and other aspects of the disclosure will be described below in detail.

An optical imaging lens according to an exemplary implementation mode of the disclosure may include, for example, seven lenses with refractive power, i.e., a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens and a seventh lens. The seven lenses are sequentially arranged from an object side to an image side along an optical axis. In the first lens to the seventh lens, there may be an air space between any two adjacent lenses.

In an exemplary implementation mode, the first lens has positive refractive power or negative refractive power; the second lens may have positive refractive power; the third lens may have positive refractive power, and an image-side surface thereof may be a convex surface; the fourth lens has positive refractive power or negative refractive power, and an object-side surface thereof may be a concave surface; the fifth lens may have positive refractive power, and an object-side surface thereof may be a concave surface; the sixth lens has positive refractive power or negative refractive power; and the seventh lens has positive refractive power or negative refractive power. Surface types and refractive power of each lens in the first lens to the seventh lens are reasonably configured, so that the performance of an optical system may be ensured, meanwhile, the tolerance sensitivity is reduced, and relatively high mass productivity is achieved.

In the exemplary implementation mode, an object-side surface of the second lens may be a convex surface, while an image-side surface may be a concave surface.

In the exemplary implementation mode, an object-side surface of the third lens may be a convex surface.

In the exemplary implementation mode, the fourth lens may have negative refractive power, and an image-side surface may be a convex surface.

In the exemplary implementation mode, an image-side surface of the fifth lens may be a convex surface.

In the exemplary implementation mode, an image-side surface of the sixth lens may be a concave surface.

In the exemplary implementation mode, the seventh lens may have negative refractive power, an object-side surface thereof may be a convex surface, while an image-side surface may be a concave surface.

In the exemplary implementation mode, the optical imaging lens of the disclosure may meet a conditional expression 0.6<R4/f<1.5, wherein f is a total effective focal length of the optical imaging lens, and R4 is a curvature radius of the image-side surface of the second lens. More specifically, R4 and f may further meet 0.82≤R4/f≤1.21. Meeting the conditional expression 0.6<R4/f<1.5 is met is favorable for obtaining a larger aperture angle and also favorable for correcting a spherical aberration.

In the exemplary implementation mode, the optical imaging lens of the disclosure may meet a conditional expression FOV>90°, wherein FOV is a maximum field of view of the optical imaging lens. More specifically, FOV may further meet 90°<FOV<120°, for example, 97.3°≤FOV≤112.3°. When the conditional expression FOV>90°, a larger field of view may be obtained, and the object information collection capability may be improved.

In the exemplary implementation mode, the optical imaging lens of the disclosure may meet a conditional expression 0.55<TTL/(ImgH×2)<0.75, wherein TTL is a distance from an object-side surface of the first lens to an imaging surface on the optical axis, and ImgH is a half of a diagonal length of an effective pixel region on the imaging surface of the optical imaging lens. More specifically, TTL and ImgH may further meet 0.60≤TTL/(ImgH×2)≤0.68. When the conditional expression 0.55<TTL/(ImgH×2)<0.75 is met, requirements on a large image surface and an ultrathin design may be met at the same time.

In the exemplary implementation mode, the optical imaging lens of the disclosure may meet a conditional expression 0<f/f2<0.8, wherein f is the total effective focal length of the optical imaging lens, and f2 is an effective focal length of the second lens. More specifically, f and f2 may further meet 0.13≤f/f2≤0.52. Reasonably configuring the refractive power of the second lens is favorable for improving the field of view of the optical imaging lens and improving the object information collection capability.

In the exemplary implementation mode, the optical imaging lens of the disclosure may meet a conditional expression 0.2<f/f3<0.7, wherein f is the total effective focal length of the optical imaging lens, and f3 is an effective focal length of the third lens. More specifically, f and f3 may further meet 0.4<f/f3<0.7, for example, 0.53≤f/f3≤0.59. Reasonably configuring the refractive power of the third lens is favorable for correcting a chromatic dispersion of the optical imaging lens and also favorable for ensuring a compact structure of the optical imaging lens.

In the exemplary implementation mode, the optical imaging lens of the disclosure may meet a conditional expression 0.2<DT11/DT71<0.7, wherein DT11 is a maximum effective radius of the object-side surface of the first lens, and DT71 is a maximum effective radius of the object-side surface of the seventh lens. More specifically, DT11 and DT71 may further meet 0.3<DT11/DT71<0.6, for example, 0.44≤DT11/DT71≤0.52. The maximum effective radii of the first lens and the seventh lens may be reasonably configured to meet a machinability requirement.

In the exemplary implementation mode, the optical imaging lens of the disclosure may meet a conditional expression 0.1<T23/CT3<0.9, wherein CT3 is a center thickness of the third lens on the optical axis, and T23 is an air space of the second lens and the third lens on the optical axis. More specifically, T23 and CT3 may further meet 0.3<T23/CT3<0.8, for example, 0.48≤T23/CT3≤0.64. Meeting the conditional expression 0.1<T23/CT3<0.9 is favorable for ensuring the compact structure of the optical imaging lens and also favorable for reducing the sensitivity of T23 and CT3 to a field curvature.

In the exemplary implementation mode, the optical imaging lens of the disclosure may meet a conditional expression 0<T12/T34<0.4, wherein T12 is an air space of the first lens and the second lens on the optical axis, and T34 is an air space of the third lens and the fourth lens on the optical axis. More specifically, T12 and T34 may further meet 0.09≤T12/T34≤0.26. Meeting the conditional expression 0<T12/T34<0.4 is favorable for ensuring the compact structure of the optical imaging lens and meeting the requirement on the ultrathin design.

In the exemplary implementation mode, the optical imaging lens of the disclosure may meet a conditional expression f/EPD<2, wherein f is the total effective focal length of the optical imaging lens, and EPD is an entrance pupil diameter of the optical imaging lens. More specifically, f and EPD may further meet 1.5<f/EPD<2, for example, 1.80≤f/EPD≤1.95Meeting the conditional expression f/EPD<2 is favorable for enlarging a relative aperture of the optical imaging lens, improving chip responsivity and achieving a higher imaging definition.

In the exemplary implementation mode, the optical imaging lens of the disclosure may meet a conditional expression −1<f5/R9<0, wherein f5 is an effective focal length of the fifth lens, and R9 is a curvature radius of the object-side surface of the fifth lens. More specifically, f5 and R9 may further meet −0.86≤f5/R9≤−0.33. Reasonably configuring the refractive power of the fifth lens and the curvature radius of the object-side surface thereof is favorable for correcting the spherical aberration of the optical imaging lens and improving the imaging performance.

In the exemplary implementation mode, the optical imaging lens of the disclosure may meet a conditional expression 0<|R8−R7|/|R8+R7|≤0.5, wherein R7 is a curvature radius of the object-side surface of the fourth lens, and R8 is a curvature radius of the image-side surface of the fourth lens. More specifically, R8 and R7 may further meet 0.26≤|R8−R7|/|R8+R7|≤0.50. Configuring the curvature radii of the object-side surface and the image-side surface of the fourth lens is favorable for correcting an off-axis aberration of the optical imaging lens and also favorable for achieving the performance of large image surface and ultrathin design.

In the exemplary implementation mode, the optical imaging lens of the disclosure may meet a conditional expression −1<f/R6<−0.5, wherein f is the total effective focal length of the optical imaging lens, and R6 is a curvature radius of the image-side surface of the third lens. More specifically, f and R6 may further meet −0.89≤f/R6≤−0.73. Meeting the conditional expression −1<f/R6<−0.5 is favorable for correcting the spherical aberration and axial chromatic aberration of the optical imaging lens and improving the imaging quality.

In the exemplary implementation mode, the optical imaging lens of the disclosure may meet a conditional expression 0.4<R14/R13<0.9, wherein R13 is a curvature radius of the object-side surface of the seventh lens, and R14 is a curvature radius of the image-side surface of the seventh lens. More specifically, R13 and R14 may further meet 0.61≤R14/R13≤0.76. The curvature radii of the object-side surface and the image-side surface of the seventh lens may be reasonably configured to meet machinability and processability requirements of the seventh lens.

In the exemplary implementation mode, the optical imaging lens may further include at least one diaphragm. The diaphragm may be arranged at a proper position as required, for example, arranged between the second lens and the third lens. Optionally, the optical imaging lens may further include an optical filter configured to correct a chromatic aberration and/or protective glass configured to protect a photosensitive element on the imaging surface.

The optical imaging lens according to the implementation mode of the disclosure may adopt seven lenses, for example, the abovementioned seven lenses. The refractive power and surface types of each lens, a center thickness of each lens, on-axis distances between the lenses and the like are reasonably configured to effectively reduce the size of the imaging lens, reduce the sensitivity of the imaging lens, improve the machinability of the imaging lens and ensure that the optical imaging lens is more favorable for production and machining and applicable to a portable electronic product. The disclosure discloses a solution to a seven lenses. The lenses have the characteristics of large image surface, wide angle, large aperture, ultrathin design and the like and may be matched with a higher-resolution sensor and a stronger image processing technology.

In the implementation mode of the disclosure, at least one of mirror surfaces of each lens is an aspherical mirror surface, namely at least one of the object-side surface and the image-side surface of each lens in the first lens, the second lens, the third lens, the fourth lens, the fifth lens, the sixth lens and the seventh lens is an aspherical mirror surface. An aspherical lens has a characteristic that a curvature keeps changing from a center of the lens to a periphery of the lens. Unlike a spherical lens with a constant curvature from a center of the lens to a periphery of the lens, the aspherical lens has a better curvature radius characteristic and the advantages of improving distortions and improving astigmatic aberrations. With adoption of the aspherical lens, the astigmatic aberrations during imaging may be eliminated as much as possible, thereby improving the imaging quality. Optionally, both the object-side surface and the image-side surface of each lens in the first lens, the second lens, the third lens, the fourth lens, the fifth lens, the sixth lens and the seventh lens are aspherical mirror surfaces.

However, those skilled in the art should know that the number of the lenses forming the optical imaging lens may be changed without departing from the technical solutions claimed in the disclosure to achieve each result and advantage described in the specification. For example, although descriptions are made in the implementation with seven lenses as an example, the optical imaging lens is not limited to seven lenses. If necessary, the optical imaging lens may further include another number of lenses.

Specific embodiments of the optical imaging lens applied to the abovementioned implementation mode will further be described below with reference to the drawings.

Embodiment 1

An optical imaging lens according to embodiment 1 of the disclosure will be described below with reference to FIG. 1 to FIG. 2D. FIG. 1 shows a structure diagram of an optical imaging lens according to embodiment 1 of the disclosure.

As shown in FIG. 1, the optical imaging lens sequentially includes, from an object side to an image side along an optical axis, a first lens E1, a second lens E2, a diaphragm STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, an optical filter E8 and an imaging surface S17.

The first lens E1 has positive refractive power, an object-side surface S1 thereof is a concave surface, while an image-side surface S2 is a convex surface. The second lens E2 has positive refractive power, an object-side surface S3 thereof is a convex surface, while an image-side surface S4 is a concave surface. The third lens E3 has positive refractive power, an object-side surface S5 thereof is a convex surface, while an image-side surface S6 is a convex surface. The fourth lens E4 has negative refractive power, an object-side surface S7 thereof is a concave surface, while an image-side surface S8 is a convex surface. The fifth lens E5 has positive refractive power, an object-side surface S9 thereof is a concave surface, while an image-side surface S10 is a convex surface. The sixth lens E6 has negative refractive power, an object-side surface S11 thereof is a convex surface, while an image-side surface S12 is a concave surface. The seventh lens E7 has negative refractive power, an object-side surface S13 thereof is a convex surface, while an image-side surface S14 is a concave surface. The optical filter E8 has an object-side surface S15 and an image-side surface S16. Light from an object sequentially penetrates through each of the surfaces S1 to S16 and is finally imaged on the imaging surface S17.

Table 1 is a basic parameter table of the optical imaging lens of embodiment 1, and units of the curvature radius, the thickness and the focal length are all millimeter (mm).

TABLE 1

Embodiment 1: f = 4.40 mm, TTL = 6.87 mm, ImgH = 5.35 mm

Material

Surface

Refractive
Abbe
Focal
Conic

number
Surface type
Curvature radius
Thickness
index
number
length
coefficient

OBJ
Spherical
Infinite
Infinite

S1
Aspherical
−13.3669
0.3502
1.65
23.53
49.45
−95.0000

S2
Aspherical
−9.5140
0.0400

−95.0000

S3
Aspherical
2.6868
0.5109
1.55
56.11
12.13
−1.2831

S4
Aspherical
4.2168
0.1567

−52.3298

STO
Spherical
Infinite
0.2202

S5
Aspherical
15.5893
0.5891
1.55
56.11
8.05
−93.5821

S6
Aspherical
−6.0343
0.3909

16.6054

S7
Aspherical
−4.2473
0.4399
1.68
19.25
−9.57
6.2168

S8
Aspherical
−12.8183
0.3628

26.0596

S9
Aspherical
−7.1132
0.7936
1.55
56.11
4.05
11.2594

S10
Aspherical
−1.7523
0.0100

−2.9333

S11
Aspherical
111.2178
0.6000
1.67
20.37
−15.03
95.0000

S12
Aspherical
9.1714
0.3897

0.5962

S13
Aspherical
1.7882
0.5600
1.53
55.87
−7.30
−7.8730

S14
Aspherical
1.0934
0.8099

−3.5656

S15
Aspherical
Infinite
0.2100
1.52
64.17

S16
Aspherical
Infinite
0.4013

S17
Spherical
Infinite
Infinite

f is a total effective focal length, of the optical imaging system, TTL is a distance from a center of the object-side surface S1 of the first lens E1 to the imaging surface S17 on the optical axis, and ImgH is a half of a diagonal length of an effective pixel region on the imaging surface S17.

In embodiment 1, both the object-side surface and the image-side surface of any lens in the first lens E1 to the seventh lens E7 are aspherical surfaces, and a surface type x of each aspherical lens may be defined through, but not limited to, the following aspherical surface formula:

$\begin{matrix} x = \frac{{ch}^{2}}{1 + \sqrt{1 - (k + 1) c^{2} h^{2}}} + \sum A ? h ?, & (1) \end{matrix}$

$? indicates text missing or illegible when filed$

wherein x is the distance vector height from a vertex of the aspherical surface when the aspherical surface is at a height of h along the optical axis direction; c is a paraxial curvature of the aspherical surface, c=1/R (namely, the paraxial curvature c is a reciprocal of the curvature radius R in Table 1); k is a conic coefficient; and Ai is the correction coefficient of the i-th order of the aspherical surface. Table 2 shows higher-order coefficients A₄, A₆, A₈, A₁₀,A₁₂, A₁₄, A₁₆, A₁₈and A₂₀that can be used for each of aspherical mirror surfaces S1 and S14 in embodiment 1.

TABLE 2

Surface

number
A4
A6
A8
A10
A12

S1
1.9050E−02
2.7201E−04
−9.8131E−04
4.3070E−04
−7.4331E−05

S2
2.8303E−02
−1.1794E−03
−5.0756E−04
7.5537E−04
−1.7796E−04

S3
2.7064E−03
−1.7680E−02
3.8132E−02
−5.4951E−02
4.3550E−02

S4
3.6584E−02
−9.1771E−02
1.1953E−01
−1.2835E−01
9.7366E−02

S5
−2.4924E−02
3.4395E−03
−4.7643E−02
9.9075E−02
−1.2016E−01

S6
−3.8125E−02
5.8806E−03
−5.1176E−02
9.9500E−02
−1.1000E−01

S7
−8.9961E−02
5.8110E−02
−1.5929E−01
2.5728E−01
−2.7062E−01

S8
−7.5962E−02
7.3692E−02
−9.0669E−02
7.0023E−02
−3.3597E−02

S9
−8.8807E−02
1.7029E−01
−1.4507E−01
7.3092E−02
−2.2318E−02

S10
−2.7462E−02
4.8371E−02
−4.3015E−02
2.2157E−02
−6.4095E−03

S11
1.2183E−01
−8.0709E−02
2.5750E−02
−4.9618E−03
5.7384E−04

S12
9.5135E−02
−6.9531E−02
2.4069E−02
−5.3251E−03
7.8592E−04

S13
−2.7673E−02
−1.8679E−02
8.3315E−03
−1.5247E−03
1.5926E−04

S14
−4.0948E−02
4.6734E−03
2.2449E−05
−6.4986E−05
7.2317E−06

Surface

number
A14
A16
A18
A20

S1
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S2
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S3
−1.8077E−02
3.1657E−03
0.0000E+00
0.0000E+00

S4
−4.3384E−02
8.9052E−03
0.0000E+00
0.0000E+00

S5
8.4775E−02
−3.1738E−02
4.9355E−03
0.0000E+00

S6
7.1963E−02
−2.5573E−02
3.7982E−03
0.0000E+00

S7
1.9684E−01
−9.2037E−02
2.4328E−02
−2.7134E−03

S8
1.0110E−02
−1.7669E−03
1.3526E−04
2.0521E−06

S9
3.6937E−03
−1.7331E−04
−3.6689E−05
4.5046E−06

S10
9.1906E−04
−2.6559E−05
−7.9555E−06
6.7279E−07

S11
−4.2180E−05
2.5507E−06
−1.4435E−07
4.3934E−09

S12
−7.7085E−05
4.8209E−06
−1.7337E−07
2.7167E−09

S13
−1.0180E−05
3.9441E−07
−8.5158E−09
7.8626E−11

S14
−3.4139E−07
4.9822E−09
1.2912E−10
−3.8108E−12

FIG. 2A shows a longitudinal aberration curve of the optical imaging lens according to embodiment 1 to represent deviation of a convergence focal point after light with different wavelengths passes through the lens. FIG. 2B shows an astigmatism curve of the optical imaging lens according to embodiment 1 to represent a meridian image surface curvature and a sagittal image surface curvature. FIG. 2C shows a distortion curve of the optical imaging lens according to embodiment 1 to represent distortion values corresponding to different fields of view. FIG. 2D shows a lateral color curve of the optical imaging lens according to embodiment 1 to represent deviation of different image heights on the imaging surface after the light passes through the lens. According to FIG. 2A to FIG. 2D, it can be seen that the optical imaging lens provided in embodiment 1 may achieve high imaging quality.

Embodiment 2

An optical imaging lens according to embodiment 2 of the disclosure will be described below with reference to FIG. 3 to FIG. 4D. In the embodiment and the following embodiments, parts of descriptions similar to those about embodiment are omitted for simplicity. FIG. 3 shows a structure diagram of an optical imaging lens according to embodiment 2 of the disclosure.

As shown in FIG. 3, the optical imaging lens sequentially includes, from an object side to an image side along an optical axis, a first lens E1, a second lens E2, a diaphragm STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, an optical filter E8 and an imaging surface S17.

Table 3 is a basic parameter table of the optical imaging lens of embodiment 2, and units of the curvature radius, the thickness and the focal length are all millimeter (mm). Table 4 shows high-order coefficients applied to each aspherical mirror surface in embodiment 2. A surface type of each aspherical surface may be defined by formula (1) given in embodiment 1.

TABLE 3

Embodiment 2: f = 4.28 mm, TTL = 6.81 mm, ImgH = 5.35 mm

Material

Surface

Refractive
Abbe
Focal
Conic

number
Surface type
Curvature radius
Thickness
index
number
length
coefficient

OBJ
Spherical
Infinite
Infinite

S1
Aspherical
−102.8605
0.3937
1.65
23.53
58.67
−99.0000

S2
Aspherical
−28.7179
0.0400

−94.1064

S3
Aspherical
2.7137
0.4979
1.55
56.11
10.81
−0.5199

S4
Aspherical
4.6971
0.1214

−52.8602

STO
Spherical
Infinite
0.2201

S5
Aspherical
24.9836
0.5920
1.55
56.11
7.78
−82.8902

S6
Aspherical
−5.0763
0.4112

11.6555

S7
Aspherical
−3.2150
0.4633
1.68
19.25
−7.93
2.6158

S8
Aspherical
−8.4742
0.3148

7.0606

S9
Aspherical
−9.8847
0.8395
1.55
56.11
4.29
19.5116

S10
Aspherical
−1.9519
0.0400

−2.0973

S11
Aspherical
11.9048
0.5889
1.67
20.37
−18.67
−73.6082

S12
Aspherical
5.9631
0.3597

−0.0912

S13
Aspherical
1.4051
0.4943
1.53
55.87
−8.81
−6.4847

S14
Aspherical
0.9502
0.8258

−3.4468

S15
Aspherical
Infinite
0.2100
1.52
64.17

S16
Aspherical
Infinite
0.3984

S17
Spherical
Infinite
Infinite

TABLE 4

Surface

number
A4
A6
A8
A10
A12

S1
1.1767E−02
1.8967E−03
−1.1916E−03
3.7415E−04
−6.3162E−05

S2
2.8078E−02
−4.9000E−03
3.1846E−03
−9.1557E−04
8.1337E−05

S3
4.2608E−03
−1.3238E−02
1.9875E−02
−2.7443E−02
2.3575E−02

S4
2.9007E−02
−6.9232E−02
7.6777E−02
−7.0526E−02
4.3145E−02

S5
−2.4769E−02
−2.3248E−02
3.6446E−02
−7.0457E−02
8.3199E−02

S6
−3.1222E−02
2.2347E−03
−3.6789E−02
7.1607E−02
−8.2510E−02

S7
−8.0242E−02
1.1048E−01
−3.5447E−01
6.7408E−01
−8.1722E−01

S8
−9.1257E−02
1.5983E−01
−2.5209E−01
2.5312E−01
−1.6583E−01

S9
−1.1551E−01
2.4490E−01
−2.6571E−01
1.8132E−01
−8.1803E−02

S10
−3.4474E−02
7.3160E−02
−7.3349E−02
4.1370E−02
−1.4117E−02

S11
1.0948E−01
−7.8288E−02
2.7982E−02
−7.2839E−03
1.5490E−03

S12
8.1866E−02
−6.5942E−02
2.3441E−02
−5.4260E−03
8.5716E−04

S13
−4.2696E−02
−1.9011E−02
1.0363E−02
−2.1091E−03
2.4012E−04

S14
−4.8571E−02
5.7973E−03
2.4215E−04
−1.4006E−04
1.6630E−05

Surface

number
A14
A16
A18
A20

S1
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S2
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S3
−1.1580E−02
2.4672E−03
0.0000E+00
0.0000E+00

S4
−1.4971E−02
2.7781E−03
0.0000E+00
0.0000E+00

S5
−6.0346E−02
2.4899E−02
−4.3722E−03
0.0000E+00

S6
5.7219E−02
−2.1722E−02
3.4401E−03
0.0000E+00

S7
6.3944E−01
−3.0983E−01
8.3931E−02
−9.6350E−03

S8
7.0948E−02
−1.9092E−02
2.9203E−03
−1.9089E−04

S9
2.4351E−02
−4.6033E−03
4.9939E−04
−2.3544E−05

S10
2.9979E−03
−3.8781E−04
2.7936E−05
−8.5872E−07

S11
−2.7176E−04
3.4044E−05
−2.4826E−06
7.6630E−08

S12
−9.1432E−05
6.2758E−06
−2.4870E−07
4.2975E−09

S13
−1.6579E−05
6.9055E−07
−1.5998E−08
1.5859E−10

S14
−1.0114E−06
3.3840E−08
−5.7078E−10
3.4922E−12

FIG. 4A shows a longitudinal aberration curve of the optical imaging lens according to embodiment 2 to represent deviation of a convergence focal point after light with different wavelengths passes through the lens. FIG. 4B shows an astigmatism curve of the optical imaging lens according to embodiment 2 to represent a meridian image surface curvature and a sagittal image surface curvature. FIG. 4C shows a distortion curve of the optical imaging lens according to embodiment 2 to represent distortion values corresponding to different fields of view. FIG. 4D shows a lateral color curve of the optical imaging lens according to embodiment 2 to represent deviation of different image heights on the imaging surface after the light passes through the lens. According to FIG. 4A to FIG. 4D, it can be seen that the optical imaging lens provided in embodiment 2 may achieve high imaging quality.

Embodiment 3

An optical imaging lens according to embodiment 3 of the disclosure is described below with reference to FIG. 5 to FIG. 6D. FIG. 5 shows a structure diagram of an optical imaging lens according to embodiment 3 of the disclosure.

As shown in FIG. 5, the optical imaging lens sequentially includes, from an object side to an image side along an optical axis, a first lens E1, a second lens E2, a diaphragm STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, an optical filter E8 and an imaging surface S17.

Table 5 is a basic parameter table of the optical imaging lens of embodiment 3, and units of the curvature radius, the thickness and the focal length are all millimeter (mm). Table 6 shows high-order coefficients applied to each aspherical mirror surface in embodiment 3. A surface type of each aspherical surface may be defined by formula (1) given in embodiment 1.

TABLE 5

Embodiment 3: f = 4.32 mm, TTL = 6.45 mm, ImgH = 5.35 mm

Material

Surface

Refractive
Abbe
Focal
Conic

number
Surface type
Curvature radius
Thickness
index
number
length
coefficient

OBJ
Spherical
Infinite
Infinite

S1
Aspherical
−197.7834
0.2623
1.65
23.53
40.83
−99.0000

S2
Aspherical
−24.2856
0.0400

−87.9609

S3
Aspherical
2.7569
0.4989
1.55
56.11
10.81
−0.4662

S4
Aspherical
4.8422
0.1224

−51.1813

STO
Spherical
Infinite
0.2201

S5
Aspherical
34.1445
0.5636
1.55
56.11
8.14
−99.0000

S6
Aspherical
−5.0782
0.4318

11.8201

S7
Aspherical
−3.2219
0.4060
1.68
19.25
−8.20
2.4686

S8
Aspherical
−8.0582
0.2974

6.4245

S9
Aspherical
−9.3512
0.7202
1.55
56.11
4.61
19.3572

S10
Aspherical
−2.0357
0.0656

−2.4058

S11
Aspherical
9.7953
0.5190
1.67
20.37
−32.86
−74.5173

S12
Aspherical
6.6247
0.4795

0.0760

S13
Aspherical
1.4640
0.4504
1.53
55.87
−6.95
−7.9545

S14
Aspherical
0.9384
0.7941

−3.6513

S15
Aspherical
Infinite
0.2100
1.52
64.17

S16
Aspherical
Infinite
0.3673

S17
Spherical
Infinite
Infinite

TABLE 6

Surface

number
A4
A6
A8
A10
A12

S1
6.8895E−03
8.3236E−03
−3.9403E−03
9.7288E−04
−1.2932E−04

S2
2.4088E−02
6.4550E−04
8.9430E−04
−8.4803E−04
1.6603E−04

S3
8.0448E−03
−1.5217E−02
2.0660E−02
−2.7236E−02
2.1442E−02

S4
2.8167E−02
−6.6379E−02
7.6572E−02
−7.1036E−02
3.8855E−02

S5
−2.5704E−02
−2.2422E−02
2.3850E−02
−3.1176E−02
1.9984E−02

S6
−2.7884E−02
−1.0398E−02
−2.8969E−03
1.8812E−02
−3.1412E−02

S7
−7.6978E−02
8.8793E−02
−2.9208E−01
5.6109E−01
−6.7109E−01

S8
−9.7063E−02
1.7082E−01
−2.8463E−01
2.9916E−01
−2.0266E−01

S9
−1.2912E−01
2.9650E−01
−3.4518E−01
2.4868E−01
−1.1700E−01

S10
−4.4101E−02
9.8443E−02
−1.0087E−01
5.7391E−02
−1.9473E−02

S11
1.1848E−01
−8.6004E−02
2.8621E−02
−5.5671E−03
5.7350E−04

S12
8.8266E−02
−7.5017E−02
2.8220E−02
−6.8249E−03
1.1088E−03

S13
−5.8573E−02
−2.2844E−02
1.5067E−02
−3.5212E−03
4.5986E−04

S14
−5.8072E−02
8.8376E−03
−2.1773E−04
−1.0790E−04
1.6661E−05

Surface

number
A14
A16
A18
A20

S1
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S2
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S3
−1.0162E−02
2.2252E−03
0.0000E+00
0.0000E+00

S4
−1.0374E−02
1.5386E−03
0.0000E+00
0.0000E+00

S5
−4.7465E−03
−8.3373E−04
5.6374E−04
0.0000E+00

S6
2.6811E−02
−1.1605E−02
1.9923E−03
0.0000E+00

S7
5.1636E−01
−2.4735E−01
6.6651E−02
−7.6452E−03

S8
8.9209E−02
−2.4721E−02
3.9085E−03
−2.6492E−04

S9
3.6074E−02
−7.0427E−03
7.8837E−04
−3.8357E−05

S10
4.0549E−03
−5.0607E−04
3.4306E−05
−9.4881E−07

S11
−2.0445E−05
−9.6260E−07
6.9980E−08
1.6908E−10

S12
−1.2010E−04
8.2999E−06
−3.2953E−07
5.6905E−09

S13
−3.6572E−05
1.7635E−06
−4.7519E−08
5.5006E−10

S14
−1.1967E−06
4.8143E−08
−1.0460E−09
9.5882E−12

FIG. 6A shows a longitudinal aberration curve of the optical imaging lens according to embodiment 3 to represent deviation of a convergence focal point after light with different wavelengths passes through the lens. FIG. 6B shows an astigmatism curve of the optical imaging lens according to embodiment 3 to represent a meridian image surface curvature and a sagittal image surface curvature. FIG. 6C shows a distortion curve of the optical imaging lens according to embodiment 3 to represent distortion values corresponding to different fields of view. FIG. 6D shows a lateral color curve of the optical imaging lens according to embodiment 3 to represent deviation of different image heights on the imaging surface after the light passes through the lens. According to FIG. 6A to FIG. 6D, it can be seen that the optical imaging lens provided in embodiment 3 may achieve high imaging quality.

Embodiment 4

An optical imaging lens according to embodiment 4 of the disclosure is described below with reference to FIG. 7 to FIG. 8D. FIG. 7 shows a structure diagram of an optical imaging lens according to embodiment 4 of the disclosure.

As shown in FIG. 7, the optical imaging lens sequentially includes, from an object side to an image side along an optical axis, a first lens E1, a second lens E2, a diaphragm STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, an optical filter E8 and an imaging surface S17.

The first lens E1 has positive refractive power, an object-side surface S1 thereof is a convex surface, while an image-side surface S2 is a convex surface. The second lens E2 has positive refractive power, an object-side surface S3 thereof is a convex surface, while an image-side surface S4 is a concave surface. The third lens E3 has positive refractive power, an object-side surface S5 thereof is a convex surface, while an image-side surface S6 is a convex surface. The fourth lens E4 has negative refractive power, an object-side surface S7 thereof is a concave surface, while an image-side surface S8 is a convex surface. The fifth lens E5 has positive refractive power, an object-side surface S9 thereof is a concave surface, while an image-side surface S10 is a convex surface. The sixth lens E6 has negative refractive power, an object-side surface S11 thereof is a convex surface, while an image-side surface S12 is a concave surface. The seventh lens E7 has negative refractive power, an object-side surface S13 thereof is a convex surface, while an image-side surface S14 is a concave surface. The optical filter E8 has an object-side surface S15 and an image-side surface S16. Light from an object sequentially penetrates through each of the surfaces S1 to S16 and is finally imaged on the imaging surface S17.

Table 7 is a basic parameter table of the optical imaging lens of embodiment 4, and units of the curvature radius, the thickness and the focal length are all millimeter (mm). Table 8 shows high-order coefficients applied to each aspherical mirror surface in embodiment 4. A surface type of each aspherical surface may be defined by formula (1) given in embodiment 1.

TABLE 7

Embodiment 4: f = 4.48 mm, TTL = 7.28 mm, ImgH = 5.35 mm

Material

Surface

Refractive
Abbe
Focal
Conic

number
Surface type
Curvature radius
Thickness
index
number
length
coefficient

OBJ
Spherical
Infinite
Infinite

S1
Aspherical
96.5476
0.4302
1.65
23.53
71.77
98.9029

S2
Aspherical
−97.8179
0.1040

90.0000

S3
Aspherical
2.6980
0.5276
1.55
56.11
10.70
−0.4081

S4
Aspherical
4.6688
0.1084

−50.0236

STO
Spherical
Infinite
0.2401

S5
Aspherical
21.9064
0.5762
1.55
56.11
7.58
−70.0000

S6
Aspherical
−5.0565
0.4011

11.3762

S7
Aspherical
−3.1537
0.4849
1.68
19.25
−7.85
2.6661

S8
Aspherical
−8.2301
0.3513

10.1240

S9
Aspherical
−9.5153
0.9262
1.55
56.11
4.18
19.2402

S10
Aspherical
−1.9051
0.0994

−2.3451

S11
Aspherical
19.3213
0.6261
1.67
20.37
−15.40
−92.1230

S12
Aspherical
6.6148
0.4088

0.5042

S13
Aspherical
1.8451
0.5583
1.53
55.87
−8.26
−7.1303

S14
Aspherical
1.1652
0.8274

−3.4193

S15
Aspherical
Infinite
0.2100
1.52
64.17

S16
Aspherical
Infinite
0.3999

S17
Spherical
Infinite
Infinite

TABLE 8

Surface

number
A4
A6
A8
A10
A12

S1
1.2906E−02
1.8395E−03
−1.8792E−03
6.6905E−04
−9.7309E−05

S2
2.6948E−02
−1.5342E−03
−1.1896E−03
1.1656E−03
−2.5216E−04

S3
−2.0791E−03
6.1975E−03
−8.3412E−03
−8.4080E−03
2.0252E−02

S4
3.4350E−02
−1.0647E−01
1.9373E−01
−2.6778E−01
2.2802E−01

S5
−3.2346E−02
1.3633E−02
−7.8506E−02
1.2553E−01
−1.1033E−01

S6
−2.5174E−02
−2.7151E−02
3.6834E−02
−4.3066E−02
2.8304E−02

S7
−1.1247E−01
2.6899E−01
−7.7602E−01
1.3808E+00
−1.5975E+00

S8
−8.9136E−02
1.3169E−01
−1.6676E−01
1.3019E−01
−6.5336E−02

S9
−1.0008E−01
1.8513E−01
−1.7468E−01
1.0457E−01
−4.2182E−02

S10
−1.1716E−02
1.9740E−02
−1.5878E−02
6.7035E−03
−1.2490E−03

S11
9.7988E−02
−6.6446E−02
2.1146E−02
−4.3078E−03
6.2746E−04

S12
7.7513E−02
−6.0625E−02
2.0522E−02
−4.3778E−03
6.2079E−04

S13
−3.9746E−02
−1.3054E−02
6.9298E−03
−1.2948E−03
1.3343E−04

S14
−4.6246E−02
5.8872E−03
1.3354E−04
−1.3981E−04
2.0022E−05

Surface

number
A14
A16
A18
A20

S1
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S2
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S3
−1.3310E−02
3.0784E−03
0.0000E+00
0.0000E+00

S4
−1.0541E−01
2.0938E−02
0.0000E+00
0.0000E+00

S5
5.0760E−02
−9.2482E−03
7.3662E−05
0.0000E+00

S6
−7.0789E−03
−1.0240E−03
6.1003E−04
0.0000E+00

S7
1.2027E+00
−5.6438E−01
1.4913E−01
−1.6847E−02

S8
2.1214E−02
−4.2828E−03
4.7520E−04
−1.8961E−05

S9
1.1451E−02
−2.0106E−03
2.0569E−04
−9.2283E−06

S10
−3.5475E−05
5.7726E−05
−9.4091E−06
5.1035E−07

S11
−7.9832E−05
8.9792E−06
−6.5808E−07
2.0714E−08

S12
−5.8504E−05
3.5262E−06
−1.2277E−07
1.8709E−09

S13
−8.2449E−06
3.0309E−07
−6.0758E−09
5.0571E−11

S14
−1.4967E−06
6.4390E−08
−1.5097E−09
1.4989E−11

FIG. 8A shows a longitudinal aberration curve of the optical imaging lens according to embodiment 4 to represent deviation of a convergence focal point after light with different wavelengths passes through the lens. FIG. 8B shows an astigmatism curve of the optical imaging lens according to embodiment 4 to represent a meridian image surface curvature and a sagittal image surface curvature. FIG. 8C shows a distortion curve of the optical imaging lens according to embodiment 4 to represent distortion values corresponding to different fields of view. FIG. 8D shows a lateral color curve of the optical imaging lens according to embodiment 4 to represent deviation of different image heights on the imaging surface after the light passes through the lens. According to FIG. 8A to FIG. 8D, it can be seen that the optical imaging lens provided in embodiment 4 may achieve high imaging quality.

Embodiment 5

An optical imaging lens according to embodiment 5 of the disclosure is described below with reference to FIG. 9 to FIG. 10D. FIG. 9 shows a structure diagram of an optical imaging lens according to embodiment 5 of the disclosure.

As shown in FIG. 9, the optical imaging lens sequentially includes, from an object side to an image side along an optical axis, a first lens E1, a second lens E2, a diaphragm STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, an optical filter E8 and an imaging surface S17.

Table 9 is a basic parameter table of the optical imaging lens of embodiment 5, and units of the curvature radius, the thickness and the focal length are all millimeter (mm). Table 10 shows high-order coefficients applied to each aspherical mirror surface in embodiment 5. A surface type of each aspherical surface may be defined by formula (1) given in embodiment 1.

TABLE 9

Embodiment 5: f = 4.50 mm, TTL = 7.03 mm, ImgH = 5.35 mm

Material

Surface

Refractive
Abbe
Focal
Conic

number
Surface type
Curvature radius
Thickness
index
number
length
coefficient

OBJ
Spherical
Infinite
Infinite

S1
Aspherical
−444.0164
0.4176
1.65
23.53
56.50
15.4050

S2
Aspherical
−35.2605
0.0400

−99.0000

S3
Aspherical
2.7102
0.5059
1.55
56.11
11.30
−0.5853

S4
Aspherical
4.5138
0.1317

−49.7550

STO
Spherical
Infinite
0.2176

S5
Aspherical
13.9312
0.6026
1.55
56.11
7.71
96.9150

S6
Aspherical
−5.9351
0.4122

11.3060

S7
Aspherical
−3.2266
0.4588
1.68
19.25
−8.19
2.8677

S8
Aspherical
−8.1452
0.3377

7.5707

S9
Aspherical
−9.4265
0.8907
1.55
56.11
4.39
19.3921

S10
Aspherical
−1.9760
0.0451

−2.1973

S11
Aspherical
14.6429
0.6227
1.67
20.37
−18.78
−90.0189

S12
Aspherical
6.6327
0.4186

0.1754

S13
Aspherical
1.6533
0.5247
1.53
55.87
−7.67
−7.4227

S14
Aspherical
1.0487
0.8095

−3.5304

S15
Aspherical
Infinite
0.2100
1.52
64.17

S16
Aspherical
Infinite
0.3820

S17
Spherical
Infinite
Infinite

TABLE 10

Surface

number
A4
A6
A8
A10
A12

S1
1.1267E−02
2.6339E−03
−1.7291E−03
5.4264E−04
−8.3368E−05

S2
2.6779E−02
−4.2676E−04
−7.8903E−04
7.2044E−04
−1.7429E−04

S3
2.8001E−03
−1.6317E−02
3.7675E−02
−5.7770E−02
4.7642E−02

S4
2.3270E−02
9.0950E−03
−2.5328E−01
5.8449E−01
−6.3029E−01

S5
−2.5231E−02
−7.3120E−03
−1.0935E−02
2.3958E−02
−2.4242E−02

S6
−2.8187E−02
−3.3463E−03
−2.5422E−02
5.3773E−02
−6.7521E−02

S7
−8.0623E−02
1.2022E−01
−3.7542E−01
6.7998E−01
−7.8750E−01

S8
−8.9818E−02
1.5455E−01
−2.3895E−01
2.3345E−01
−1.4857E−01

S9
−1.1079E−01
2.2360E−01
−2.2923E−01
1.4673E−01
−6.1558E−02

S10
−2.8782E−02
6.2264E−02
−6.0079E−02
3.1620E−02
−9.7751E−03

S11
9.7554E−02
−6.1292E−02
1.5311E−02
−1.2991E−03
−2.6379E−04

S12
7.7029E−02
−6.0247E−02
2.0317E−02
−4.3010E−03
6.0148E−04

S13
−4.1884E−02
−1.9429E−02
1.0629E−02
−2.2023E−03
2.5751E−04

S14
−4.7823E−02
5.6053E−03
3.6418E−04
−1.9042E−04
2.6321E−05

Surface

number
A14
A16
A18
A20

S1
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S2
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S3
−2.0733E−02
3.8239E−03
0.0000E+00
0.0000E+00

S4
3.3213E−01
−6.8003E−02
0.0000E+00
0.0000E+00

S5
1.2087E−02
−1.4040E−03
−2.5370E−04
0.0000E+00

S6
5.0948E−02
−2.0796E−02
3.5522E−03
0.0000E+00

S7
5.8874E−01
−2.7203E−01
7.0056E−02
−7.6151E−03

S8
6.1758E−02
−1.6119E−02
2.3793E−03
−1.4855E−04

S9
1.6867E−02
−2.8967E−03
2.7999E−04
−1.1382E−05

S10
1.8103E−03
−1.9306E−04
1.0401E−05
−1.9185E−07

S11
7.9604E−05
−8.0323E−06
3.4263E−07
−4.4012E−09

S12
−5.5585E−05
3.2760E−06
−1.1160E−07
1.6690E−09

S13
−1.8400E−05
7.9909E−07
−1.9442E−08
2.0385E−10

S14
−1.9942E−06
8.8646E−08
−2.1636E−09
2.2362E−11

FIG. 10A shows a longitudinal aberration curve of the optical imaging lens according to embodiment 5 to represent deviation of a convergence focal point after light with different wavelengths passes through the lens. FIG. 10B shows an astigmatism curve of the optical imaging lens according to embodiment 5 to represent a meridian image surface curvature and a sagittal image surface curvature. FIG. 10C shows a distortion curve of the optical imaging lens according to embodiment 5 to represent distortion values corresponding to different fields of view. FIG. 10D shows a lateral color curve of the optical imaging lens according to embodiment 5 to represent deviation of different image heights on the imaging surface after the light passes through the lens. According to FIG. 10A to FIG. 10D, it can be seen that the optical imaging lens provided in embodiment 5 may achieve high imaging quality.

Embodiment 6

An optical imaging lens according to embodiment 6 of the disclosure is described below with reference to FIG. 11 to FIG. 12D. FIG. 11 shows a structure diagram of an optical imaging lens according to embodiment 6 of the disclosure.

As shown in FIG. 11, the optical imaging lens sequentially includes, from an object side to an image side along an optical axis, a first lens E1, a second lens E2, a diaphragm STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, an optical filter E8 and an imaging surface S17.

Table 11 is a basic parameter table of the optical imaging lens of embodiment 6, and units of the curvature radius, the thickness and the focal length are all millimeter (mm). Table 12 shows high-order coefficients applied to each aspherical mirror surface in embodiment 6. A surface type of each aspherical surface may be defined by formula (1) given in embodiment 1.

TABLE 11

Embodiment 6: f = 4.48 mm, TTL = 7.01 mm, ImgH = 5.35 mm

Material

Surface

Refractive
Abbe
Focal
Conic

number
Surface type
Curvature radius
Thickness
index
number
length
coefficient

OBJ
Spherical
Infinite
Infinite

S1
Aspherical
778.8930
0.3952
1.65
23.53
69.21
−99.0000

S2
Aspherical
−49.8871
0.0503

−76.7481

S3
Aspherical
2.7089
0.5137
1.55
56.11
10.45
−0.4778

S4
Aspherical
4.8107
0.1235

−52.4486

STO
Spherical
Infinite
0.2380

S5
Aspherical
25.4197
0.6156
1.55
56.11
7.81
−21.4033

S6
Aspherical
−5.0825
0.4187

11.4640

S7
Aspherical
−3.1844
0.4608
1.68
19.25
−8.01
2.6488

S8
Aspherical
−8.1501
0.3240

9.5003

S9
Aspherical
−9.5154
0.8627
1.55
56.11
4.35
19.0239

S10
Aspherical
−1.9630
0.0499

−2.2466

S11
Aspherical
13.9206
0.6252
1.67
20.37
−19.09
−83.0612

S12
Aspherical
6.5284
0.4130

0.4070

S13
Aspherical
1.6149
0.5079
1.53
55.87
−7.60
−6.9149

S14
Aspherical
1.0300
0.8126

−3.5656

S15
Aspherical
Infinite
0.2100
1.52
64.17

S16
Aspherical
Infinite
0.3855

S17
Spherical
Infinite
Infinite

TABLE 12

Surface

number
A4
A6
A8
A10
A12

S1
1.2018E−02
1.7075E−03
−1.2070E−03
4.0985E−04
−6.8162E−05

S2
2.7146E−02
−3.7195E−03
2.0881E−03
−3.7556E−04
−1.7825E−05

S3
4.1928E−03
−1.4870E−02
2.7543E−02
−3.9373E−02
3.2963E−02

S4
2.6439E−02
−6.0522E−02
6.1124E−02
−5.0284E−02
2.8436E−02

S5
−2.6441E−02
−1.5380E−02
1.3460E−02
−2.6562E−02
3.3868E−02

S6
−3.0398E−02
−8.8967E−03
9.5403E−05
4.0424E−03
−6.3175E−03

S7
−8.2610E−02
1.1117E−01
−3.3893E−01
6.2269E−01
−7.3336E−01

S8
−9.0908E−02
1.5368E−01
−2.3694E−01
2.3441E−01
−1.5195E−01

S9
−1.0844E−01
2.2209E−01
−2.3387E−01
1.5511E−01
−6.8038E−02

S10
−2.4314E−02
5.5645E−02
−5.6929E−02
3.1578E−02
−1.0226E−02

S11
1.0004E−01
−6.6054E−02
1.8418E−02
−2.3322E−03
−6.6646E−05

S12
7.8622E−02
−6.2561E−02
2.1750E−02
−4.7893E−03
7.0171E−04

S13
−4.2571E−02
−2.1337E−02
1.1833E−02
−2.5153E−03
3.0251E−04

S14
−5.0312E−02
6.1758E−03
2.6071E−04
−1.6896E−04
2.3094E−05

Surface

number
A14
A16
A18
A20

S1
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S2
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S3
−1.5067E−02
2.9121E−03
0.0000E+00
0.0000E+00

S4
−9.9517E−03
2.1561E−03
0.0000E+00
0.0000E+00

S5
−2.6991E−02
1.2222E−02
−2.3016E−03
0.0000E+00

S6
6.1495E−03
−3.0576E−03
5.8465E−04
0.0000E+00

S7
5.6055E−01
−2.6644E−01
7.0981E−02
−8.0270E−03

S8
6.4503E−02
−1.7269E−02
2.6337E−03
−1.7194E−04

S9
1.9685E−02
−3.6160E−03
3.8077E−04
−1.7349E−05

S10
1.9715E−03
−2.1614E−04
1.1550E−05
−1.8049E−07

S11
5.6276E−05
−6.0516E−06
2.0997E−07
4.7334E−10

S12
−6.8410E−05
4.2800E−06
−1.5555E−07
2.4911E−09

S13
−2.2266E−05
9.9713E−07
−2.5045E−08
2.7139E−10

S14
−1.6994E−06
7.2965E−08
−1.7153E−09
1.7031E−11

FIG. 12A shows a longitudinal aberration curve of the optical imaging lens according to embodiment 6 to represent deviation of a convergence focal point after light with different wavelengths passes through the lens. FIG. 12B shows an astigmatism curve of the optical imaging lens according to embodiment 6 to represent a meridian image surface curvature and a sagittal image surface curvature. FIG. 12C shows a distortion curve of the optical imaging lens according to embodiment 6 to represent distortion values corresponding to different fields of view. FIG. 12D shows a lateral color curve of the optical imaging lens according to embodiment 6 to represent deviation of different image heights on the imaging surface after the light passes through the lens. According to FIG. 12A to FIG. 12D, it can be seen that the optical imaging lens provided in embodiment 6 may achieve high imaging quality.

Embodiment 7

An optical imaging lens according to embodiment 7 of the disclosure is described below with reference to FIG. 13 to FIG. 14D. FIG. 13 shows a structure diagram of an optical imaging lens according to embodiment 7 of the disclosure.

As shown in FIG. 13, the optical imaging lens sequentially includes, from an object side to an image side along an optical axis, a first lens E1, a second lens E2, a diaphragm STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, an optical filter E8 and an imaging surface S17.

The first lens E1 has positive refractive power, an object-side surface S1 thereof is a concave surface, while an image-side surface S2 is a convex surface. The second lens E2 has positive refractive power, an object-side surface S3 thereof is a convex surface, while an image-side surface S4 is a concave surface. The third lens E3 has positive refractive power, an object-side surface S5 thereof is a convex surface, while an image-side surface S6 is a convex surface. The fourth lens E4 has negative refractive power, an object-side surface S7 thereof is a concave surface, while an image-side surface S8 is a convex surface. The fifth lens E5 has positive refractive power, an object-side surface S9 thereof is a concave surface, while an image-side surface S10 is a convex surface. The sixth lens E6 has negative refractive power, an object-side surface S11 thereof is a concave surface, while an image-side surface S12 is a concave surface. The seventh lens E7 has negative refractive power, an object-side surface S13 thereof is a convex surface, while an image-side surface S14 is a concave surface. The optical filter E8 has an object-side surface S15 and an image-side surface S16. Light from an object sequentially penetrates through each of the surfaces S1 to S16 and is finally imaged on the imaging surface S17.

Table 13 is a basic parameter table of the optical imaging lens of embodiment 7, and units of the curvature radius, the thickness and the focal length are all millimeter (mm). Table 14 shows high-order coefficients applied to each aspherical mirror surface in embodiment 7. A surface type of each aspherical surface may be defined by formula (1) given in embodiment 1.

TABLE 13

Embodiment 7: f = 4.45 mm, TTL = 6.99 mm, ImgH = 5.35 mm

Material

Surface

Refractive
Abbe
Focal
Conic

number
Surface type
Curvature radius
Thickness
index
number
length
coefficient

OBJ
Spherical
Infinite
Infinite

S1
Aspherical
−715.5514
0.3975
1.65
23.53
57.94
98.1010

S2
Aspherical
−37.2247
0.0400

−98.1564

S3
Aspherical
2.7141
0.5126
1.55
56.11
10.76
−0.4531

S4
Aspherical
4.7071
0.1258

−51.8357

STO
Spherical
Infinite
0.2317

S5
Aspherical
24.7795
0.5966
1.55
56.11
7.75
−23.1466

S6
Aspherical
−5.0608
0.4254

11.5560

S7
Aspherical
−3.1770
0.4735
1.68
19.25
−7.76
2.6732

S8
Aspherical
−8.5087
0.3324

9.6063

S9
Aspherical
−9.8753
0.9050
1.55
56.11
3.23
19.1112

S10
Aspherical
−1.5455
0.0510

−2.4378

S11
Aspherical
−47.1921
0.6241
1.67
20.37
−8.47
73.9504

S12
Aspherical
6.4497
0.3587

−0.0087

S13
Aspherical
1.7542
0.5081
1.53
55.87
−6.78
−7.3627

S14
Aspherical
1.0637
0.8123

−3.4997

S15
Aspherical
Infinite
0.2100
1.52
64.17

S16
Aspherical
Infinite
0.3848

S17
Spherical
Infinite
Infinite

TABLE 14

Surface

number
A4
A6
A8
A10
A12

S1
1.2063E−02
2.0476E−03
−1.5965E−03
5.5889E−04
−8.9715E−05

S2
2.7714E−02
−3.4572E−03
1.2893E−03
6.6993E−05
−9.0553E−05

S3
3.3348E−03
−1.3662E−02
2.6028E−02
−3.9866E−02
3.5096E−02

S4
2.7996E−02
−6.7856E−02
8.0037E−02
−8.1854E−02
5.8855E−02

S5
−2.5919E−02
−1.6294E−02
1.5143E−02
−3.2473E−02
4.5499E−02

S6
−2.9674E−02
−2.9358E−03
−1.8330E−02
3.2897E−02
−3.4786E−02

S7
−7.7419E−02
8.5639E−02
−2.5633E−01
4.5873E−01
−5.3729E−01

S8
−8.0304E−02
1.1155E−01
−1.5086E−01
1.3190E−01
−7.6824E−02

S9
−9.5694E−02
1.5599E−01
−1.2859E−01
6.4979E−02
−2.0864E−02

S10
−2.1981E−03
3.3007E−03
1.1838E−03
−5.4673E−03
4.5416E−03

S11
1.0786E−01
−7.0077E−02
2.2766E−02
−5.1698E−03
9.4828E−04

S12
7.0185E−02
−5.6600E−02
1.9899E−02
−4.5410E−03
6.9967E−04

S13
−3.7231E−02
−1.5811E−02
8.0772E−03
−1.5507E−03
1.6724E−04

S14
−4.7276E−02
6.5981E−03
−3.5499E−04
3.8565E−06
−1.3905E−06

Surface

number
A14
A16
A18
A20

S1
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S2
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S3
−1.6481E−02
3.2493E−03
0.0000E+00
0.0000E+00

S4
−2.5123E−02
5.3075E−03
0.0000E+00
0.0000E+00

S5
−4.0256E−02
2.0106E−02
−4.1576E−03
0.0000E+00

S6
2.2959E−02
−8.3499E−03
1.2484E−03
0.0000E+00

S7
4.1327E−01
−1.9769E−01
5.2792E−02
−5.9535E−03

S8
2.9676E−02
−7.2388E−03
9.9280E−04
−5.5648E−05

S9
4.0670E−03
−4.1391E−04
9.5485E−06
1.2246E−06

S10
−1.8058E−03
3.8912E−04
−4.3878E−05
2.0341E−06

S11
−1.5618E−04
2.0078E−05
−1.5435E−06
5.0095E−08

S12
−7.1877E−05
4.7052E−06
−1.7690E−07
2.8965E−09

S13
−1.0979E−05
4.3621E−07
−9.6652E−09
9.1816E−11

S14
2.9717E−07
−2.1790E−08
7.1514E−10
−8.9888E−12

FIG. 14A shows a longitudinal aberration curve of the optical imaging lens according to embodiment 7 to represent deviation of a convergence focal point after light with different wavelengths passes through the lens. FIG. 14B shows an astigmatism curve of the optical imaging lens according to embodiment 7 to represent a meridian image surface curvature and a sagittal image surface curvature. FIG. 14C shows a distortion curve of the optical imaging lens according to embodiment 7 to represent distortion values corresponding to different fields of view. FIG. 14D shows a lateral color curve of the optical imaging lens according to embodiment 7 to represent deviation of different image heights on the imaging surface after the light passes through the lens. According to FIG. 14A to FIG. 14D, it can be seen that the optical imaging lens provided in embodiment 7 may achieve high imaging quality.

Embodiment 8

An optical imaging lens according to embodiment 8 of the disclosure is described below with reference to FIG. 15 to FIG. 16D. FIG. 15 shows a structure diagram of an optical imaging lens according to embodiment 8 of the disclosure.

As shown in FIG. 15, the optical imaging lens sequentially includes, from an object side to an image side along an optical axis, a first lens E1, a second lens E2, a diaphragm STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, an optical filter E8 and an imaging surface S17.

The first lens E1 has negative refractive power, an object-side surface S1 thereof is a convex surface, while an image-side surface S2 is a concave surface. The second lens E2 has positive refractive power, an object-side surface S3 thereof is a convex surface, while an image-side surface S4 is a concave surface. The third lens E3 has positive refractive power, an object-side surface S5 thereof is a convex surface, while an image-side surface S6 is a convex surface. The fourth lens E4 has negative refractive power, an object-side surface S7 thereof is a concave surface, while an image-side surface S8 is a convex surface. The fifth lens E5 has positive refractive power, an object-side surface S9 thereof is a concave surface, and an image-side surface S10 is a convex surface. The sixth lens E6 has negative refractive power, an object-side surface S11 thereof is a convex surface, while an image-side surface S12 is a concave surface. The seventh lens E7 has negative refractive power, an object-side surface S13 thereof is a convex surface, while an image-side surface S14 is a concave surface. The optical filter E8 has an object-side surface S15 and an image-side surface S16. Light from an object sequentially penetrates through each of the surfaces S1 to S16 and is finally imaged on the imaging surface S17.

Table 15 is a basic parameter table of the optical imaging lens of embodiment 8, and units of the curvature radius, the thickness and the focal length are all millimeter (mm). Table 16 shows high-order coefficients applied to each aspherical mirror surface in embodiment 8. A surface type of each aspherical surface may be defined by formula (1) given in embodiment 1.

TABLE 15

Embodiment 8: f = 4.39 mm, TTL = 6.97 mm, ImgH = 5.35 mm

Material

Surface

Refractive
Abbe
Focal
Conic

number
Surface type
Curvature radius
Thickness
index
number
length
coefficient

OBJ
Spherical
Infinite
Infinite

S1
Aspherical
82.1409
0.3925
1.65
23.53
−278.13
95.0000

S2
Aspherical
57.0963
0.0996

−74.9493

S3
Aspherical
2.5189
0.5319
1.551
56.1
8.48
−0.3828

S4
Aspherical
5.1120
0.1070

−51.7999

STO
Spherical
Infinite
0.2289

S5
Aspherical
36.9870
0.5502
1.55
56.11
8.15
−82.5731

S6
Aspherical
−5.0315
0.4225

11.3977

S7
Aspherical
−3.1501
0.4650
1.68
19.25
−7.83
2.7367

S8
Aspherical
−8.2103
0.3431

9.0430

S9
Aspherical
−9.5221
0.8229
1.55
56.11
3.97
19.0131

S10
Aspherical
−1.8191
0.1046

−2.2705

S11
Aspherical
26.9997
0.5833
1.67
20.37
−12.51
−42.1798

S12
Aspherical
6.3147
0.4118

0.4583

S13
Aspherical
1.5817
0.5328
1.53
55.87
−8.94
−6.8526

S14
Aspherical
1.0497
0.7975

−3.4140

S15
Aspherical
Infinite
0.2100
1.52
64.17

S16
Aspherical
Infinite
0.3700

S17
Spherical
Infinite
Infinite

TABLE 16

Surface

number
A4
A6
A8
A10
A12

S1
1.4577E−02
3.5118E−04
−8.4412E−04
3.3634E−04
−6.1384E−05

S2
2.4506E−02
−1.8597E−03
1.0706E−03
−1.1419E−04
−3.8174E−05

S3
3.8605E−03
−2.5758E−02
6.4249E−02
−9.5380E−02
7.9396E−02

S4
2.3939E−02
−5.8543E−02
7.8883E−02
−9.9561E−02
8.5959E−02

S5
−2.6313E−02
−2.3848E−02
3.9884E−02
−8.2556E−02
9.9080E−02

S6
−3.5021E−02
3.0173E−02
−1.1675E−01
2.0601E−01
−2.1891E−01

S7
−9.2919E−02
1.5118E−01
−4.1381E−01
7.2682E−01
−8.5852E−01

S8
−9.4919E−02
1.6013E−01
−2.3822E−01
2.2823E−01
−1.4575E−01

S9
−9.5568E−02
1.7536E−01
−1.6154E−01
9.3204E−02
−3.5933E−02

S10
−1.9619E−02
3.1781E−02
−2.2075E−02
6.6800E−03
8.1504E−05

S11
9.8297E−02
−6.6715E−02
2.3333E−02
−6.2866E−03
1.4103E−03

S12
6.9843E−02
−5.2780E−02
1.7385E−02
−3.6878E−03
5.2943E−04

S13
−3.8274E−02
−1.5375E−02
8.0006E−03
−1.5451E−03
1.6765E−04

S14
−4.3394E−02
4.8813E−03
9.5792E−05
−8.6559E−05
1.0657E−05

Surface

number
A14
A16
A18
A20

S1
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S2
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S3
−3.5198E−02
6.5096E−03
0.0000E+00
0.0000E+00

S4
−4.2783E−02
9.8080E−03
0.0000E+00
0.0000E+00

S5
−6.7478E−02
2.4333E−02
−3.3944E−03
0.0000E+00

S6
1.3984E−01
−4.9203E−02
7.3058E−03
0.0000E+00

S7
6.7332E−01
−3.3102E−01
9.1233E−02
−1.0644E−02

S8
6.1756E−02
−1.6582E−02
2.5292E−03
−1.6320E−04

S9
9.2949E−03
−1.5576E−03
1.5226E−04
−6.4877E−06

S10
−6.3597E−04
1.8256E−04
−2.2375E−05
1.0547E−06

S11
−2.4858E−04
2.9680E−05
−2.0181E−06
5.7890E−08

S12
−5.1074E−05
3.1661E−06
−1.1340E−07
1.7738E−09

S13
−1.1101E−05
4.4660E−07
−1.0071E−08
9.7963E−11

S14
−6.8833E−07
2.5700E−08
−5.2296E−10
4.4855E−12

FIG. 16A shows a longitudinal aberration curve of the optical imaging lens according to embodiment 8 to represent deviation of a convergence focal point after light with different wavelengths passes through the lens. FIG. 16B shows an astigmatism curve of the optical imaging lens according to embodiment 8 to represent a meridian image surface curvature and a sagittal image surface curvature. FIG. 16C shows a distortion curve of the optical imaging lens according to embodiment 8 to represent distortion values corresponding to different fields of view. FIG. 16D shows a lateral color curve of the optical imaging lens according to embodiment 8 to represent deviation of different image heights on the imaging surface after the light passes through the lens. According to FIG. 16A to FIG. 16D, it can be seen that the optical imaging lens provided in embodiment 8 may achieve high imaging quality.

Embodiment 9

An optical imaging lens according to embodiment 9 of the disclosure is described below with reference to FIG. 17 to FIG. 18D. FIG. 17 shows a structure diagram of an optical imaging lens according to embodiment 9 of the disclosure.

As shown in FIG. 17, the optical imaging lens sequentially includes, from an object side to an image side along an optical axis, a first lens E1, a second lens E2, a diaphragm STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, an optical filter E8 and an imaging surface S17.

The first lens E1 has positive refractive power, an object-side surface S1 thereof is a convex surface, and an image-side surface S2 is a convex surface. The second lens E2 has positive refractive power, an object-side surface S3 thereof is a convex surface, while an image-side surface S4 is a concave surface. The third lens E3 has positive refractive power, an object-side surface S5 thereof is a convex surface, while an image-side surface S6 is a convex surface. The fourth lens E4 has negative refractive power, an object-side surface S7 thereof is a concave surface, while an image-side surface S8 is a convex surface. The fifth lens E5 has positive refractive power, an object-side surface S9 thereof is a concave surface, while an image-side surface S10 is a convex surface. The sixth lens E6 has positive refractive power, an object-side surface S11 thereof is a convex surface, while an image-side surface S12 is a concave surface. The seventh lens E7 has negative refractive power, an object-side surface S13 thereof is a convex surface, while an image-side surface S14 is a concave surface. The optical filter E8 has an object-side surface S15 and an image-side surface S16. Light from an object sequentially penetrates through each of the surfaces S1 to S16 and is finally imaged on the imaging surface S17.

Table 17 is a basic parameter table of the optical imaging lens of embodiment 9, and units of the curvature radius, the thickness and the focal length are all millimeter (mm). Table 18 shows high-order coefficients applied to each aspherical mirror surface in embodiment 9. A surface type of each aspherical surface may be defined by formula (1) given in embodiment 1.

TABLE 17

Embodiments f = 4.31 mm, TTL = 6.85 mm, ImgH = 5.35 mm

Material

Surface

Refractive
Abbe
Focal
Conic

number
Surface type
Curvature radius
Thickness
index
number
length
coefficient

OBJ
Spherical
Infinite
Infinite

S1
Aspherical
150.1798
0.3751
1.65
23.53
57.49
95.0350

S2
Aspherical
−52.5409
0.0999

24.7632

S3
Aspherical
2.7266
0.5200
1.55
56.11
10.94
−0.3963

S4
Aspherical
4.6781
0.1014

−49.8403

STO
Spherical
Infinite
0.2297

S5
Aspherical
22.6030
0.5676
1.55
56.11
7.63
−94.5536

S6
Aspherical
−5.0573
0.4125

11.4075

S7
Aspherical
−3.1625
0.4763
1.68
19.25
−8.15
2.6175

S8
Aspherical
−7.8449
0.3633

10.5883

S9
Aspherical
−9.0524
0.7051
1.55
56.11
6.00
19.1808

S10
Aspherical
−2.4712
0.1000

−1.9665

S11
Aspherical
5.9693
0.6231
1.67
20.37
85.36
−72.3990

S12
Aspherical
6.3906
0.4438

0.4960

S13
Aspherical
1.7129
0.5130
1.53
55.87
−8.24
−6.9354

S14
Aspherical
1.1056
0.7683

−3.3552

S15
Aspherical
Infinite
0.2100
1.52
64.17

S16
Aspherical
Infinite
0.3408

S17
Spherical
Infinite
Infinite

TABLE 18

Surface

number
A4
A6
A8
A10
A12

S1
1.2197E−02
2.0517E−03
−1.5752E−03
5.3334E−04
−8.4586E−05

S2
2.6914E−02
−2.9048E−03
1.1206E−03
−7.2077E−05
−3.4459E−05

S3
3.6980E−03
−1.3400E−02
2.6830E−02
−4.3613E−02
3.9798E−02

S4
2.9694E−02
−7.6384E−02
1.1148E−01
−1.4824E−01
1.3284E−01

S5
−2.5113E−02
−3.1290E−02
7.1023E−02
−1.6963E−01
2.3949E−01

S6
−3.4110E−02
2.0134E−02
−9.0228E−02
1.6163E−01
−1.7342E−01

S7
−9.9155E−02
1.9234E−01
−5.4320E−01
9.7083E−01
−1.1368E+00

S8
−9.7667E−02
1.6804E−01
−2.5814E−01
2.5377E−01
−1.6376E−01

S9
−9.7834E−02
2.1332E−01
−2.2881E−01
1.5202E−01
−6.6416E−02

S10
−3.9352E−02
6.5297E−02
−5.3607E−02
2.3714E−02
−5.1576E−03

S11
1.0529E−01
−7.5966E−02
2.8191E−02
−7.6601E−03
1.6269E−03

S12
7.6968E−02
−5.9235E−02
1.9961E−02
−4.3146E−03
6.3028E−04

S13
−4.2575E−02
−1.7611E−02
9.6727E−03
−1.9577E−03
2.2172E−04

S14
−4.7491E−02
6.6876E−03
−2.4623E−04
−4.3834E−05
6.7508E−06

Surface

number
A14
A16
A18
A20

S1
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S2
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S3
−1.9247E−02
3.9036E−03
0.0000E+00
0.0000E+00

S4
−6.7063E−02
1.5076E−02
0.0000E+00
0.0000E+00

S5
−1.9477E−01
8.4969E−02
−1.5129E−02
0.0000E+00

S6
1.1177E−01
−3.9478E−02
5.8563E−03
0.0000E+00

S7
8.6811E−01
−4.1280E−01
1.1007E−01
−1.2469E−02

S8
6.9171E−02
−1.8347E−02
2.7483E−03
−1.7343E−04

S9
1.9126E−02
−3.5055E−03
3.7024E−04
−1.7058E−05

S10
2.1787E−04
1.3128E−04
−2.5451E−05
1.4611E−06

S11
−2.6443E−04
2.9464E−05
−1.9072E−06
5.2847E−08

S12
−6.1899E−05
3.9099E−06
−1.4279E−07
2.2784E−09

S13
−1.5253E−05
6.3408E−07
−1.4680E−08
1.4546E−10

S14
−4.3549E−07
1.5166E−08
−2.7575E−10
2.0290E−12

FIG. 18A shows a longitudinal aberration curve of the optical imaging lens according to embodiment 9 to represent deviation of a convergence focal point after light with different wavelengths passes through the lens. FIG. 18B shows an astigmatism curve of the optical imaging lens according to embodiment 9 to represent a meridian image surface curvature and a sagittal image surface curvature. FIG. 18C shows a distortion curve of the optical imaging lens according to embodiment 9 to represent distortion values corresponding to different fields of view. FIG. 18D shows a lateral color curve of the optical imaging lens according to embodiment 9 to represent deviation of different image heights on the imaging surface after the light passes through the lens. According to FIG. 18A to FIG. 18D, it can be seen that the optical imaging lens provided in embodiment 9 may achieve high imaging quality.

Embodiment 10

An optical imaging lens according to embodiment 10 of the disclosure is described below with reference to FIG. 19 to FIG. 20D. FIG. 19 shows a structure diagram of an optical imaging lens according to embodiment 10 of the disclosure.

As shown in FIG. 19, the optical imaging lens sequentially includes, from an object side to an image side along an optical axis, a first lens E1, a second lens E2, a diaphragm STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, an optical filter E8 and an imaging surface S17.

Table 19 is a basic parameter table of the optical imaging lens of embodiment 10, and units of the curvature radius, the thickness and the focal length are all millimeter (mm). Table 20 shows high-order coefficients applied to each aspherical mirror surface in embodiment 10. A surface type of each aspherical surface may be defined by formula (1) given in embodiment 1.

TABLE 19

Embodiment 10: f = 4.20 mm, TTL = 6.82 mm, ImgH = 5.35 mm

Material

Surface

Refractive
Abbe
Focal
Conic

number
Surface type
Curvature radius
Thickness
index
number
length
coefficient

OBJ
Spherical
Infinite
Infinite

S1
Aspherical
−126.9925
0.3708
1.65
23.53
64.54
−95.0000

S2
Aspherical
−32.5677
0.0404

−95.0000

S3
Aspherical
2.7323
0.5202
1.55
56.11
11.01
−0.4187

S4
Aspherical
4.6719
0.1053

−49.0743

STO
Spherical
Infinite
0.2227

S5
Aspherical
22.2799
0.5758
1.55
56.11
7.60
−95.0000

S6
Aspherical
−5.0507
0.4154

11.4856

S7
Aspherical
−3.1887
0.4692
1.68
19.25
−7.91
2.7012

S8
Aspherical
−8.3470
0.3184

9.3493

S9
Aspherical
−9.7875
0.8325
1.55
56.11
4.40
18.9984

S10
Aspherical
−1.9853
0.0400

−2.1528

S11
Aspherical
13.1721
0.6103
1.67
20.37
−21.33
−55.0598

S12
Aspherical
6.7096
0.4130

0.5094

S13
Aspherical
1.5954
0.5668
1.53
55.87
−9.22
−6.7674

S14
Aspherical
1.0569
0.7734

−3.3736

S15
Aspherical
Infinite
0.2100
1.52
64.17

S16
Aspherical
Infinite
0.3390

S17
Spherical
Infinite
Infinite

TABLE 20

Surface

number
A4
A6
A8
A10
A12

S1
1.1458E−02
2.4070E−03
−1.8031E−03
6.0773E−04
−9.3329E−05

S2
2.7028E−02
−3.9474E−03
1.7409E−03
−2.1868E−04
−1.7164E−05

S3
4.8782E−03
−1.5870E−02
2.8501E−02
−4.1587E−02
3.5463E−02

S4
2.6831E−02
−5.5686E−02
4.6307E−02
−2.8231E−02
7.1290E−03

S5
−2.3912E−02
−1.5407E−02
−4.434 0E−03
2.3235E−02
−3.4039E−02

S6
−3.1038E−02
7.3963E−03
−4.7669E−02
8.0612E−02
−8.2968E−02

S7
−8.2954E−02
1.2487E−01
−4.0376E−01
7.8104E−01
−9.6225E−01

S8
−9.0460E−02
1.5403E−01
−2.3677E−01
2.3081E−01
−1.4630E−01

S9
−1.0962E−01
2.2462E−01
−2.3448E−01
1.5404E−01
−6.6957E−02

S10
−2.4018E−02
4.5829E−02
−4.0429E−02
1.8828E−02
−4.6418E−03

S11
9.9492E−02
−6.9584E−02
2.5276E−02
−6.6925E−03
1.3689E−03

S12
6.9021E−02
−5.1507E−02
1.7143E−02
−3.6973E−03
5.3867E−04

S13
−3.9646E−02
−1.2927E−02
6.7973E−03
−1.2590E−03
1.2867E−04

S14
−4.4824E−02
8.4771E−03
−1.2651E−03
1.7466E−04
−1.9230E−05

Surface

number
A14
A16
A18
A20

S1
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S2
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S3
−1.6427E−02
3.2393E−03
0.0000E+00
0.0000E+00

S4
1.9209E−03
−3.8576E−04
0.0000E+00
0.0000E+00

S5
2.1426E−02
−4.8239E−03
1.2867E−04
0.0000E+00

S6
5.3082E−02
−1.9177E−02
2.9781E−03
0.0000E+00

S7
7.5831E−01
−3.6632E−01
9.8043E−02
−1.1042E−02

S8
6.0227E−02
−1.5465E−02
2.2282E−03
−1.3424E−04

S9
1.9217E−02
−3.5041E−03
3.6670E−04
−1.6661E−05

S10
4.9974E−04
1.4764E−05
−8.2657E−06
5.3338E−07

S11
−2.1456E−04
2.3333E−05
−1.4891E−06
4.0882E−08

S12
−5.2453E−05
3.2637E−06
−1.1688E−07
1.8247E−09

S13
−7.8940E−06
2.8881E−07
−5.7884E−09
4.8601E−11

S14
1.4193E−06
−6.3961E−08
1.5825E−09
−1.6429E−11

FIG. 20A shows a longitudinal aberration curve of the optical imaging lens according to embodiment 10 to represent deviation of a convergence focal point after light with different wavelengths passes through the lens. FIG. 20B shows an astigmatism curve of the optical imaging lens according to embodiment 10 to represent a meridian image surface curvature and a sagittal image surface curvature. FIG. 20C shows a distortion curve of the optical imaging lens according to embodiment 10 to represent distortion values corresponding to different fields of view. FIG. 20D illustrates a lateral color curve of the optical imaging lens according to embodiment 10 to represent deviation of different image heights on the imaging surface after the light passes through the lens. According to FIG. 20A to FIG. 20D, it can be seen that the optical imaging lens provided in embodiment 10 may achieve high imaging quality.

Embodiment 11

An optical imaging lens according to embodiment 11 of the disclosure is described below with reference to FIG. 21 to FIG. 22D. FIG. 21 shows a structure diagram of an optical imaging lens according to embodiment 11 of the disclosure.

As shown in FIG. 21, the optical imaging lens sequentially includes, from an object side to an image side along an optical axis, a first lens E1, a second lens E2, a diaphragm STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, an optical filter E8 and an imaging surface S17.

Table 21 is a basic parameter table of the optical imaging lens of embodiment 11, and units of the curvature radius, the thickness and the focal length are all millimeter (mm). Table 22 shows high-order coefficients applied to each aspherical mirror surface in embodiment 11. A surface type of each aspherical surface may be defined by formula (1) given in embodiment 1.

TABLE 21

Embodiment 11: f = 4.05 mm, TTL = 6.92 mm, ImgH = 5.30 mm

Material

Surface

Refractive
Abbe
Focal
Conic

number
Surface type
Curvature radius
Thickness
index
number
length
coefficient

OBJ
Spherical
Infinite
Infinite

S1
Aspherical
−73.0758
0.3691
1.65
23.53
67.52
67.8536

S2
Aspherical
−28.1926
0.0494

−93.8081

S3
Aspherical
2.8412
0.5278
1.55
56.11
11.35
−0.4239

S4
Aspherical
4.9023
0.1072

−49.2569

STO
Spherical
Infinite
0.2271

S5
Aspherical
22.0632
0.5859
1.55
56.11
7.72
70.3955

S6
Aspherical
−5.1635
0.4148

11.5023

S7
Aspherical
−3.2334
0.4781
1.68
19.25
−8.10
2.7458

S8
Aspherical
−8.3374
0.3246

9.5645

S9
Aspherical
−9.7420
0.8506
1.55
56.11
4.48
18.5171

S10
Aspherical
−2.0154
0.0410

−2.1286

S11
Aspherical
13.4366
0.6224
1.67
20.37
−21.80
−55.8230

S12
Aspherical
6.8514
0.3934

0.3394

S13
Aspherical
1.4160
0.5778
1.53
55.87
−12.08
−6.7548

S14
Aspherical
0.9966
0.7808

−3.3086

S15
Aspherical
Infinite
0.2100
1.52
64.17

S16
Aspherical
Infinite
0.3564

S17
Spherical
Infinite
Infinite

TABLE 22

Surface

number
A4
A6
A8
A10
A12

S1
1.0605E−02
2.4878E−03
−1.7284E−03
5.4213E−04
−7.7498E−05

S2
2.5964E−02
−4.5165E−03
2.1859E−03
−4.2016E−04
1.6082E−05

S3
−1.4813E−03
1.3777E−02
−3.3821E−02
3.2805E−02
−1.5273E−02

S4
2.2075E−02
−4.6358E−02
6.2102E−02
−9.2211E−02
8.7506E−02

S5
−1.4040E−02
−8.4641E−02
2.5938E−01
−5.1508E−01
6.1377E−01

S6
−3.6909E−02
3.6288E−02
−9.5138E−02
1.1308E−01
−7.1197E−02

S7
−7.8584E−02
1.0846E−01
−3.1857E−01
5.6203E−01
−6.4954E−01

S8
−9.0836E−02
1.6007E−01
−2.6255E−01
2.7748E−01
−1.9250E−01

S9
−1.0605E−01
2.1312E−01
−2.2361E−01
1.4889E−01
−6.5572E−02

S10
−1.5233E−02
2.1261E−02
−1.4496E−02
4.6325E−03
−3.3820E−04

S11
9.4444E−02
−6.4400E−02
2.2478E−02
−5.3320E−03
8.7400E−04

S12
6.4346E−02
−4.7323E−02
1.6089E−02
−3.6374E−03
5.5800E−04

S13
−3.4362E−02
−9.9279E−03
4.8224E−03
−8.1607E−04
7.5837E−05

S14
−4.3484E−02
9.6153E−03
−1.8084E−03
2.7662E−04
−2.9227E−05

Surface

number
A14
A16
A18
A20

S1
9.5988E−08
5.6123E−08
1.2601E−08
−4.6831E−09

S2
1.0586E−07
1.2104E−08
4.6078E−08
−3.4816E−09

S3
2.2668E−03
2.8417E−04
0.0000E+00
0.0000E+00

S4
−4.3439E−02
9.0644E−03
0.0000E+00
0.0000E+00

S5
−4.3655E−01
1.7058E−01
−2.7973E−02
0.0000E+00

S6
2.1295E−02
−1.6691E−03
−2.5744E−04
0.0000E+00

S7
4.9371E−01
−2.3424E−01
6.2165E−02
−6.9706E−03

S8
8.6998E−02
−2.4518E−02
3.8862E−03
−2.6198E−04

S9
1.8975E−02
−3.4633E−03
3.6025E−04
−1.6196E−05

S10
−1.9185E−04
5.8161E−05
−6.5046E−06
2.6693E−07

S11
−1.0119E−04
8.2053E−06
−4.1863E−07
9.8697E−09

S12
−5.6613E−05
3.6090E−06
−1.3020E−07
2.0196E−09

S13
−4.2081E−06
1.3834E−07
−2.4712E−09
1.8305E−11

S14
1.9436E−06
−7.6743E−08
1.6302E−09
−1.4218E−11

FIG. 22A shows a longitudinal aberration curve of the optical imaging lens according to embodiment 11 to represent deviation of a convergence focal point after light with different wavelengths passes through the lens. FIG. 22B shows an astigmatism curve of the optical imaging lens according to embodiment 11 to represent a meridian image surface curvature and a sagittal image surface curvature. FIG. 22C shows a distortion curve of the optical imaging lens according to embodiment 11 to represent distortion values corresponding to different fields of view. FIG. 22D illustrates a lateral color curve of the optical imaging lens according to embodiment 11 to represent deviation of different image heights on the imaging surface after the light passes through the lens. According to FIG. 22A to FIG. 22D, it can be seen that the optical imaging lens provided in embodiment 11 may achieve high imaging quality.

Embodiment 12

An optical imaging lens according to embodiment 12 of the disclosure is described below with reference to FIG. 23 to FIG. 24D. FIG. 23 shows a structure diagram of an optical imaging lens according to embodiment 12 of the disclosure.

As shown in FIG. 23, the optical imaging lens sequentially includes, from an object side to an image side along an optical axis, a first lens E1, a second lens E2, a diaphragm STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, an optical filter E8 and an imaging surface S17.

The first lens E1 has positive refractive power, an object-side surface S1 thereof is a concave surface, while an image-side surface S2 is a convex surface. The second lens E2 has positive refractive power, an object-side surface S3 thereof is a convex surface, while an image-side surface S4 is a concave surface. The third lens E3 has positive refractive power, an object-side surface S5 thereof is a convex surface, while an image-side surface S6 is a convex surface. The fourth lens E4 has negative refractive power, an object-side surface S7 thereof is a concave surface, while an image-side surface S8 is a convex surface. The fifth lens E5 has positive refractive power, an object-side surface S9 thereof is a concave surface, while an image-side surface S10 is a convex surface. The sixth lens E6 has negative refractive power, an object-side surface S11 thereof is a concave surface, while an image-side surface S12 is a concave surface. The seventh lens E7 has negative refractive power, an object-side surface S13 thereof is a convex surface, while an image-side surface S14 is a concave surface. The optical filter E8 has an object-side surface S15 and an image-side surface S16. Light from an object sequentially penetrates through each of the surfaces S1 to S16 and is finally imaged on the imaging surface S17.

Table 23 is a basic parameter table of the optical imaging lens of embodiment 12, and units of the curvature radius, the thickness and the focal length are all millimeter (mm). Table 24 shows high-order coefficients applied to each aspherical mirror surface in embodiment 12. A surface type of each aspherical surface may be defined by formula (1) given in embodiment 1.

TABLE 23

Embodiment 12: f = 4.20 mm, TTL = 7.10 mm, ImgH = 5.35 mm

Material

Surface

Refractive
Abbe
Focal
Conic

number
Surface type
Curvature radius
Thickness
index
number
length
coefficient

OBJ
Spherical
Infinite
Infinite

S1
Aspherical
−7.9917
0.3808
1.65
23.53
30.58
−95.0000

S2
Aspherical
−5.7925
0.0400

−95.0000

S3
Aspherical
2.9811
0.3781
1.55
56.11
31.42
−8.0562

S4
Aspherical
3.4466
0.1617

−44.4213

STO
Spherical
Infinite
0.1813

S5
Aspherical
14.7796
0.7161
1.55
56.11
7.21
−53.3742

S6
Aspherical
−5.2749
0.2863

11.0532

S7
Aspherical
−4.8131
0.4249
1.68
19.25
−17.99
8.6447

S8
Aspherical
−8.2375
0.4587

14.6573

S9
Aspherical
−5.2141
0.8702
1.55
56.11
4.48
5.1693

S10
Aspherical
−1.7636
0.0400

−1.6598

S11
Aspherical
−34.2607
0.5999
1.67
20.37
−9.06
94.6282

S12
Aspherical
7.3830
0.3177

−1.8964

S13
Aspherical
1.3991
0.6081
1.53
55.87
−23.73
−4.8943

S14
Aspherical
1.0692
0.9921

−3.1052

S15
Aspherical
Infinite
0.2100
1.52
64.17

S16
Aspherical
Infinite
0.4341

S17
Spherical
Infinite
Infinite

TABLE 24

Surface

number
A4
A6
A8
A10
A12

S1
3.4073E−03
3.3166E−03
−1.3323E−03
2.2225E−04
−1.3541E−05

S2
1.6780E−03
7.3124E−03
−3.4163E−03
6.5839E−04
−3.9773E−05

S3
3.4071E−02
−5.0845E−02
3.8493E−02
−1.8174E−02
−1.4516E−03

S4
7.2671E−02
−1.6636E−01
2.2019E−01
−2.0988E−01
1.1844E−01

S5
−1.4600E−02
9.0589E−04
−2.0912E−02
2.4897E−02
−1.0930E−02

S6
−3.3988E−02
1.1187E−02
−4.7054E−02
7.2106E−02
−6.5136E−02

S7
−6.244 IE−02
3.3339E−02
−6.9648E−02
8.2885E−02
−7.3130E−02

S8
−4.3146E−02
3.5159E−02
−1.9858E−02
−2.8014E−03
1.1496E−02

S9
−7.4825E−02
5.4658E−02
1.4089E−02
−3.8704E−02
2.445 IE−02

S10
−6.0907E−02
7.4980E−02
−5.7864E−02
2.9192E−02
−9.4831E−03

S11
7.3656E−02
−2.1707E−02
−2.2765E−03
2.9997E−03
−9.4849E−04

S12
5.6259E−02
−2.6889E−02
6.0398E−03
−8.5666E−04
7.7786E−05

S13
−6.3423E−03
−1.3318E−02
4.4198E−03
−7.7048E−04
8.5913E−05

S14
−2.0386E−02
−9.3972E−04
1.0326E−03
−2.3810E−04
2.9326E−05

Surface

number
A14
A16
A18
A20

S1
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S2
0.0000E+00
0.0000E+00
0.0000E+00
0.0000E+00

S3
4.0307E−03
−8.5502E−04
0.0000E+00
0.0000E+00

S4
−3.3762E−02
3.8361E−03
0.0000E+00
0.0000E+00

S5
−5.7271E−03
7.3943E−03
−1.8467E−03
0.0000E+00

S6
3.5631E−02
−1.0908E−02
1.4599E−03
0.0000E+00

S7
4.8969E−02
−2.1358E−02
4.9698E−03
−4.2350E−04

S8
−7.8199E−03
2.6812E−03
−4.9025E−04
3.9070E−05

S9
−8.1773E−03
1.5614E−03
−1.5893E−04
6.5809E−06

S10
1.7871E−03
−1.3907E−04
−5.3019E−06
1.0628E−06

S11
1.6424E−04
−1.6633E−05
9.2152E−07
−2.1525E−08

S12
−4.3655E−06
1.4199E−07
−2.3502E−09
1.4272E−11

S13
−6.1772E−06
2.7442E−07
−6.8261E−09
7.2628E−11

S14
−2.1000E−06
8.6754E−08
−1.9062E−09
1.7139E−11

FIG. 24A shows a longitudinal aberration curve of the optical imaging lens according to embodiment 12 to represent deviation of a convergence focal point after light with different wavelengths passes through the lens. FIG. 24B shows an astigmatism curve of the optical imaging lens according to embodiment 12 to represent a meridian image surface curvature and a sagittal image surface curvature. FIG. 24C shows a distortion curve of the optical imaging lens according to embodiment 12 to represent distortion values corresponding to different fields of view. FIG. 24D illustrates a lateral color curve of the optical imaging lens according to embodiment 12 to represent deviation of different image heights on the imaging surface after the light passes through the lens. According to FIG. 24A to FIG. 24D, it can be seen that the optical imaging lens provided in embodiment 12 may achieve high imaging quality.

From the above, embodiment 1 to embodiment 12 meet a relationship shown in Table 25 respectively.

TABLE 25

Conditional expression/

embodiment
1
2
3
4
5
6
7
8
9
10
11
12

R4/f
0.96
1.10
1.12
1.04
1.00
1.07
1.06
1.16
1.08
1.11
1.21
0.82

FOV (°)
102.4
103.2
102.1
97.3
99.8
100.0
100.3
99.1
98.4
104.3
107.6
112.3

TTL/(ImgH × 2)
0.64
0.64
0.60
0.68
0.66
0.65
0.65
0.65
0.64
0.64
0.65
0.66

f/f2
0.36
0.40
0.40
0.42
0.40
0.43
0.41
0.52
0.39
0.38
0.36
0.13

f/f3
0.55
0.55
0.53
0.59
0.58
0.57
0.57
0.54
0.57
0.55
0.53
0.58

f5/R9
−0.57
−0.43
−0.49
−0.44
−0.47
−0.46
−0.33
−0.42
−0.66
−0.45
−0.46
−0.86

|R8 − R7|/|R8 + R7|
0.50
0.45
0.43
0.45
0.43
0.44
0.46
0.45
0.43
0.45
0.44
0.26

f/R6
−0.73
−0.84
−0.85
−0.89
−0.76
−0.88
−0.88
−0.87
−0.85
−0.83
−0.79
−0.80

T23/CT3
0.64
0.58
0.61
0.60
0.58
0.59
0.60
0.61
0.58
0.57
0.57
0.48

DT11/DT71
0.45
0.46
0.47
0.48
0.47
0.48
0.47
0.47
0.47
0.45
0.44
0.52

T12/T34
0.10
0.10
0.09
0.26
0.10
0.12
0.09
0.24
0.24
0.10
0.12
0.14

f/EPD
1.88
1.88
1.88
1.91
1.80
1.87
1.87
1.88
1.89
1.88
1.95
1.87

R14/R13
0.61
0.68
0.64
0.63
0.63
0.64
0.61
0.66
0.65
0.66
0.70
0.76

The disclosure also provides an imaging device, of which an electronic photosensitive element may be a Charge-Coupled Device (CCD) or a Complementary Metal Oxide Semiconductor (CMOS). The imaging device may be an independent imaging device such as a digital camera, and may also be an imaging module integrated into a mobile electronic device such as a mobile phone. The imaging device is provided with the abovementioned optical imaging lens.

The above description is only description about the preferred embodiments of the disclosure and adopted technical principles. It is understood by those skilled in the art that the scope of the disclosure involved in the disclosure is not limited to the technical solutions formed by specifically combining the technical characteristics and should also cover other technical solutions formed by freely combining the technical characteristics or equivalent characteristics thereof without departing from the inventive concept, for example, technical solutions formed by mutually replacing the characteristics and (but not limited to) the technical characteristics with similar functions disclosed in the disclosure.

Optical Imaging Lens

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