Optical imaging lens

By designing a reasonable combination of six lenses and aspherical mirrors, optical parameters are optimized, and the problem of limited field of view when shooting vast scenes is solved, miniaturized, high-resolution and large field of view optical imaging lenses are realized. on smartphones and other devices.

CN113484974BActive Publication Date: 2024-12-20ZHEJIANG SUNNY OPTICAL CO LTD
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Patent Information

Application Number
CN202010430750.8
Authority / Receiving Office
CN · China
Patent Type
Patents(China)
Current Assignee / Owner
Filing Date
2020-05-20
Publication Date
2024-12-20
Estimated Expiration
2040-05-20

AI Technical Summary

Technical Problem

When shooting vast scenes such as tall buildings or mountains, standard lenses cannot effectively express the grandeur and majestic momentum of the scenery, and have limited vision, which cannot meet users' needs for wide angles and high resolution.

Method used

An optical imaging lens was designed, and by reasonably allocating the power and optimizing the optical parameters, a combination of six lenses, including a lens with positive and negative power, and an aspherical mirror is set between the lenses to meet the specific curvature. Radius, thickness and focal length relationships to achieve large field of view and high resolution imaging.

Benefits of technology

It achieves miniaturization, high resolution and good imaging quality, is suitable for lightweight electronic products, can capture wide-angle scenes and maintain high imaging quality, and is suitable for portable devices such as smartphones.

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Abstract

The present application discloses an optical imaging lens, which includes, in order from the object side to the image side along the optical axis: a first lens with optical power; a second lens with optical power; a third lens with optical power, whose object side surface is concave; a fourth lens with negative optical power; a fifth lens with optical power; and a sixth lens with optical power. Half of the maximum field of view angle Semi-FOV of the optical imaging lens satisfies: Semi-FOV ≥ 60°; the curvature radius R5 of the object side surface of the third lens and the curvature radius R9 of the object side surface of the fifth lens satisfy: 3.5<R5 / R9<11.5; and the curvature radius R9 of the object side surface of the fifth lens and the effective focal length f5 of the fifth lens satisfy: ‑4.0<R9 / f5≤‑1.5.
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Description

Technical Field

[0001] The present application relates to the field of optical elements, and in particular, to an optical imaging lens. Background Art

[0002] Nowadays, portable electronic products such as smartphones are not only a communication device, but also a kind of entertainment for people. Among them, the camera capability of portable electronic products such as smartphones is one of the important functions that people pay attention to.

[0003] With the development of science and technology, the professionalism of photography in portable electronic products such as smartphones is gradually improving. Although ordinary standard lenses can produce clear images in most cases, when shooting vast scenes such as tall buildings or mountains, standard lenses can only capture part of the scenery and cannot show the grandeur and majesty of the scenery. Summary of the invention

[0004] On one hand, the present application provides such an optical imaging lens, which includes, in order from the object side to the image side along the optical axis: a first lens with optical power; a second lens with optical power; a third lens with optical power, whose object side surface is concave; a fourth lens with negative optical power; a fifth lens with optical power; and a sixth lens with optical power. Half of the maximum field of view angle Semi-FOV of the optical imaging lens can satisfy: Semi-FOV ≥ 60°; the curvature radius R5 of the object side surface of the third lens and the curvature radius R9 of the object side surface of the fifth lens can satisfy: 3.5<R5 / R9<11.5; and the curvature radius R9 of the object side surface of the fifth lens and the effective focal length f5 of the fifth lens can satisfy: -4.0<R9 / f5≤-1.5.

[0005] In one embodiment, there is at least one aspherical mirror surface from the object side surface of the first lens to the image side surface of the sixth lens.

[0006] In one embodiment, a center thickness CT3 of the third lens on the optical axis and a spacing distance T12 between the first lens and the second lens on the optical axis may satisfy: 3.0<CT3 / T12<9.5.

[0007] In one embodiment, a center thickness CT5 of the fifth lens on the optical axis and a center thickness CT2 of the second lens on the optical axis may satisfy: 3.5<CT5 / CT2<6.0.

[0008] In one embodiment, a center thickness CT6 of the sixth lens on the optical axis and a spacing distance T56 between the fifth lens and the sixth lens on the optical axis may satisfy: 1.5≤CT6 / T56≤6.5.

[0009] In one embodiment, the interval T23 between the second lens and the third lens on the optical axis and the center thickness CT2 of the second lens on the optical axis may satisfy: 1.0<T23 / CT2<2.5.

[0010] In one embodiment, a curvature radius R11 of the object-side surface of the sixth lens and an effective focal length f6 of the sixth lens may satisfy: -1.0<R11 / f6<2.

[0011] In one embodiment, the effective focal length f3 of the third lens and the effective focal length f4 of the fourth lens may satisfy: -3.0≤f4 / f3≤-1.9.

[0012] In one embodiment, the distance TTL from the object side of the first lens to the imaging plane of the optical imaging lens on the optical axis and half the diagonal length of the effective pixel area on the imaging plane of the optical imaging lens ImgH may satisfy: 1.5<TTL / ImgH<2.0.

[0013] In one embodiment, a spacing distance T23 between the second lens and the third lens on the optical axis, a spacing distance T34 between the third lens and the fourth lens on the optical axis, and a spacing distance T56 between the fifth lens and the sixth lens on the optical axis may satisfy: 1.0<T23 / (T34+T56)<2.0.

[0014] In one embodiment, the sum ΣCT of the center thicknesses of the first lens to the sixth lens on the optical axis and the sum ΣAT of the spacing distances between any two adjacent lenses of the first lens to the sixth lens on the optical axis may satisfy: 2.5<ΣCT / ΣAT<3.5.

[0015] In one embodiment, the first lens, the second lens, and the third lens may have the same refractive index.

[0016] On the other hand, the present application provides an optical imaging lens, which includes, in order from the object side to the image side along the optical axis: a first lens with optical power; a second lens with optical power; a third lens with optical power, whose object side surface is concave; a fourth lens with negative optical power; a fifth lens with optical power; and a sixth lens with optical power. The effective focal length f3 of the third lens and the effective focal length f4 of the fourth lens satisfy: -3.0≤f4 / f3≤-1.9.

[0017] The present application provides an optical imaging lens which can be applied to lightweight electronic products and has miniaturization, high resolution and good imaging quality by reasonably allocating optical focal length and optimizing optical parameters. BRIEF DESCRIPTION OF THE DRAWINGS

[0018] Other features, objects and advantages of the present application will become more apparent by reading the detailed description of non-limiting embodiments made with reference to the following drawings:

[0019] Figure 1 A schematic structural diagram of an optical imaging lens according to Embodiment 1 of the present application is shown;

[0020] FIG. 2A to FIG. 2D The axial chromatic aberration curve, astigmatism curve, distortion curve and magnification chromatic aberration curve of the optical imaging lens of Example 1 are respectively shown;

[0021] Figure 3 A schematic structural diagram of an optical imaging lens according to Embodiment 2 of the present application is shown;

[0022] FIG. 4A to FIG. 4D The axial chromatic aberration curve, astigmatism curve, distortion curve and magnification chromatic aberration curve of the optical imaging lens of Example 2 are respectively shown;

[0023] Figure 5 A schematic structural diagram of an optical imaging lens according to Embodiment 3 of the present application is shown;

[0024] FIG. 6A to FIG. 6D The axial chromatic aberration curve, astigmatism curve, distortion curve and magnification chromatic aberration curve of the optical imaging lens of Example 3 are respectively shown;

[0025] Figure 7 A schematic structural diagram of an optical imaging lens according to Embodiment 4 of the present application is shown;

[0026] FIG. 8A to FIG. 8D The axial chromatic aberration curve, astigmatism curve, distortion curve and magnification chromatic aberration curve of the optical imaging lens of Example 4 are respectively shown;

[0027] Fig. 9 A schematic structural diagram of an optical imaging lens according to Embodiment 5 of the present application is shown;

[0028] FIG. 10A to FIG. 10D The axial chromatic aberration curve, astigmatism curve, distortion curve and magnification chromatic aberration curve of the optical imaging lens of Example 5 are respectively shown;

[0029] Fig.11 A schematic structural diagram of an optical imaging lens according to Embodiment 6 of the present application is shown; and

[0030] FIG. 12A to FIG. 12D The axial chromatic aberration curve, astigmatism curve, distortion curve and magnification chromatic aberration curve of the optical imaging lens of Example 6 are respectively shown. DETAILED DESCRIPTION

[0031] In order to better understand the present application, a more detailed description will be made of various aspects of the present application with reference to the accompanying drawings. It should be understood that these detailed descriptions are only descriptions of exemplary embodiments of the present application, and are not intended to limit the scope of the present application in any way. Throughout the specification, the same reference numerals refer to the same elements. The expression "and / or" includes any and all combinations of one or more of the associated listed items.

[0032] It should be noted that in this specification, the expressions of first, second, third, etc. are only used to distinguish one feature from another feature, and do not represent any limitation on the features. Therefore, without departing from the teaching of the present application, the first lens discussed below may also be referred to as the second lens or the third lens.

[0033] In the drawings, the thickness, size and shape of the lenses have been slightly exaggerated for ease of explanation. Specifically, the shapes of the spherical or aspherical surfaces shown in the drawings are shown by way of example. That is, the shapes of the spherical or aspherical surfaces are not limited to the shapes of the spherical or aspherical surfaces shown in the drawings. The drawings are only examples and are not drawn strictly to scale.

[0034] In this article, the paraxial region refers to the region near the optical axis. If the lens surface is convex and the position of the convex surface is not defined, it means that the lens surface is convex at least in the paraxial region; if the lens surface is concave and the position of the concave surface is not defined, it means that the lens surface is concave at least in the paraxial region. The surface of each lens closest to the object is called the object side of the lens, and the surface of each lens closest to the imaging plane is called the image side of the lens.

[0035] It should also be understood that the terms "comprises", "including", "having", "includes" and / or "comprising", when used in this specification, indicate the presence of the stated features, elements and / or components, but do not exclude the presence or addition of one or more other features, elements, components and / or combinations thereof. In addition, when expressions such as "at least one of..." appear after a list of listed features, they modify the entire listed features rather than modifying the individual elements in the list. In addition, when describing embodiments of the present application, "may" is used to mean "one or more embodiments of the present application". And, the term "exemplary" is intended to refer to an example or illustration.

[0036] Unless otherwise defined, all terms (including technical terms and scientific terms) used in this article have the same meaning as commonly understood by ordinary technicians in the field to which this application belongs. It should also be understood that terms (such as terms defined in commonly used dictionaries) should be interpreted as having the same meaning as their meaning in the context of the relevant technology, and will not be interpreted in an idealized or overly formal sense unless explicitly defined in this article.

[0037] It should be noted that, in the absence of conflict, the embodiments and features in the embodiments of the present application can be combined with each other. The present application will be described in detail below with reference to the accompanying drawings and in combination with the embodiments.

[0038] The features, principles and other aspects of the present application are described in detail below.

[0039] The optical imaging lens according to the exemplary embodiment of the present application may include six lenses with optical power, namely a first lens, a second lens, a third lens, a fourth lens, a fifth lens and a sixth lens. The six lenses are arranged in sequence from the object side to the image side along the optical axis. Any two adjacent lenses from the first lens to the sixth lens may have a spacing distance between them.

[0040] In an exemplary embodiment, the first lens may have positive or negative optical power; the second lens may have positive or negative optical power; the third lens may have positive or negative optical power, and its object side surface may be concave; the fourth lens may have negative optical power; the fifth lens may have positive or negative optical power; and the sixth lens may have positive or negative optical power.

[0041] In an exemplary embodiment, the optical imaging lens according to the present application may satisfy: Semi-FOV ≥ 60°, where Semi-FOV is half of the maximum field of view of the optical imaging lens. More specifically, Semi-FOV may further satisfy: Semi-FOV ≥ 61°. Satisfying Semi-FOV ≥ 60° is conducive to a wide field of view and can have a considerable clear range.

[0042] In an exemplary embodiment, the optical imaging lens according to the present application may satisfy: 3.5<R5 / R9<11.5, where R5 is the radius of curvature of the object side of the third lens, and R9 is the radius of curvature of the object side of the fifth lens. Satisfying 3.5<R5 / R9<11.5 is conducive to reducing the sensitivity of the system, achieving the characteristics of a large field of view and high resolution, and ensuring good processability.

[0043] In an exemplary embodiment, the optical imaging lens according to the present application may satisfy: 3.0<CT3 / T12<9.5, wherein CT3 is the center thickness of the third lens on the optical axis, and T12 is the spacing distance between the first lens and the second lens on the optical axis. More specifically, CT3 and T12 may further satisfy: 3.0<CT3 / T12<9.3. Satisfying 3.0<CT3 / T12<9.5 can effectively reduce the size of the optical imaging lens, avoid the optical imaging lens from being too large, and at the same time reduce the difficulty of assembling the lens, and achieve a higher space utilization rate.

[0044] In an exemplary embodiment, the optical imaging lens according to the present application may satisfy: 3.5<CT5 / CT2<6.0, wherein CT5 is the center thickness of the fifth lens on the optical axis, and CT2 is the center thickness of the second lens on the optical axis. More specifically, CT5 and CT2 may further satisfy: 3.6<CT5 / CT2<5.9. Satisfying 3.5<CT5 / CT2<6.0 can make the lens easy to injection mold, improve the processability of the imaging system, and at the same time ensure good imaging quality.

[0045] In an exemplary embodiment, the optical imaging lens according to the present application may satisfy: 1.5≤CT6 / T56≤6.5, wherein CT6 is the center thickness of the sixth lens on the optical axis, and T56 is the spacing distance between the fifth lens and the sixth lens on the optical axis. Satisfying 1.5≤CT6 / T56≤6.5 can effectively reduce the size of the optical imaging lens, avoid the optical imaging lens from being too large, and at the same time reduce the difficulty of lens assembly, achieving a higher space utilization rate.

[0046] In an exemplary embodiment, the optical imaging lens according to the present application may satisfy: 1.0<T23 / CT2<2.5, wherein T23 is the spacing distance between the second lens and the third lens on the optical axis, and CT2 is the center thickness of the second lens on the optical axis. More specifically, T23 and CT2 may further satisfy: 1.2<T23 / CT2<2.1. Satisfying 1.0<T23 / CT2<2.5 can ensure processing and assembly characteristics, and avoid problems such as interference between front and rear lenses during the assembly process due to too small a gap. At the same time, it is beneficial to slow down the deflection of light, adjust the field curvature of the optical imaging lens, reduce the sensitivity, and thus obtain better imaging quality.

[0047] In an exemplary embodiment, the optical imaging lens according to the present application may satisfy: -4.0<R9 / f5≤-1.5, where R9 is the radius of curvature of the object side of the fifth lens, and f5 is the effective focal length of the fifth lens. More specifically, R9 and f5 may further satisfy: -3.7<R9 / f5≤-1.9. Satisfying -4.0<R9 / f5≤-1.5 can improve the field curvature and distortion of the optical imaging lens, while controlling the difficulty of processing the fifth lens.

[0048] In an exemplary embodiment, the optical imaging lens according to the present application may satisfy: -1.0<R11 / f6<2, where R11 is the radius of curvature of the object side of the sixth lens, and f6 is the effective focal length of the sixth lens. More specifically, R11 and f6 may further satisfy: -0.6<R11 / f6<-0.3. Satisfying -1.0<R11 / f6<2 can improve the field curvature and distortion of the optical imaging lens, and at the same time can control the difficulty of processing the sixth lens.

[0049] In an exemplary embodiment, the optical imaging lens according to the present application may satisfy: -3.0≤f4 / f3≤-1.9, wherein f3 is the effective focal length of the third lens, and f4 is the effective focal length of the fourth lens. More specifically, f4 and f3 may further satisfy: -2.7≤f4 / f3≤-1.9. Satisfying -3.0≤f4 / f3≤-1.9 is beneficial for the optical imaging lens to better balance aberrations and improve the resolution of the system.

[0050] In an exemplary embodiment, the optical imaging lens according to the present application may satisfy: 1.5<TTL / ImgH<2.0, wherein TTL is the distance from the object side of the first lens to the imaging plane of the optical imaging lens on the optical axis, and ImgH is half the diagonal length of the effective pixel area on the imaging plane of the optical imaging lens. More specifically, TTL and ImgH may further satisfy 1.5<TTL / ImgH<1.9. Satisfying 1.5<TTL / ImgH<2.0 is conducive to achieving a shorter total optical length while achieving a larger imaging height, is conducive to miniaturization of the lens, and is conducive to improving imaging quality.

[0051] In an exemplary embodiment, the optical imaging lens according to the present application may satisfy: 1.0<T23 / (T34+T56)<2.0, wherein T23 is the spacing distance between the second lens and the third lens on the optical axis, T34 is the spacing distance between the third lens and the fourth lens on the optical axis, and T56 is the spacing distance between the fifth lens and the sixth lens on the optical axis. More specifically, T23, T34, and T56 may further satisfy: 1.1<T23 / (T34+T56)<2.0. Satisfying 1.0<T23 / (T34+T56)<2.0 is conducive to reducing the difficulty of lens assembly.

[0052] In an exemplary embodiment, the optical imaging lens according to the present application may satisfy: 2.5<∑CT / ∑AT<3.5, wherein ∑CT is the sum of the center thicknesses of the first lens to the sixth lens on the optical axis, and ∑AT is the sum of the spacing distances between any two adjacent lenses of the first lens to the sixth lens on the optical axis. More specifically, ∑CT and ∑AT may further satisfy: 2.5<∑CT / ∑AT<3.4. Satisfying 2.5<∑CT / ∑AT<3.5 can effectively reduce the size of the optical imaging lens, avoid the optical imaging lens from being too large, and at the same time reduce the difficulty of assembling the lens, achieving a higher space utilization rate.

[0053] In example embodiments, the first lens, the second lens, and the third lens may have the same refractive index.

[0054] In an exemplary embodiment, the optical imaging lens according to the present application further includes an aperture arranged between the second lens and the third lens. Optionally, the above-mentioned optical imaging lens may further include a filter for correcting color deviation and / or a protective glass for protecting the photosensitive element located on the imaging surface. The present application proposes an optical imaging lens with the characteristics of miniaturization, large field of view, long depth of field and high imaging quality. The optical imaging lens according to the above-mentioned embodiment of the present application may adopt multiple lenses, such as the six lenses mentioned above. By reasonably allocating the optical focal length, surface shape, center thickness of each lens and axial spacing between each lens, etc., the incident light can be effectively converged, the total optical length of the imaging lens can be reduced, and the processability of the imaging lens can be improved, so that the optical imaging lens is more conducive to production and processing.

[0055] In the embodiment of the present application, at least one of the mirror surfaces of each lens is an aspherical mirror surface, that is, at least one of the mirror surfaces from the object side of the first lens to the image side of the sixth lens is an aspherical mirror surface. The characteristic of the aspherical lens is that the curvature changes continuously from the center of the lens to the periphery of the lens. Unlike a spherical lens with a constant curvature from the center of the lens to the periphery of the lens, an aspherical lens has a better curvature radius characteristic, and has the advantages of improving distortion aberration and improving astigmatism aberration. After adopting an aspherical lens, the aberration occurring during imaging can be eliminated as much as possible, thereby improving the imaging quality. Optionally, at least one of the object side and image side of each lens in the first lens, the second lens, the third lens, the fourth lens, the fifth lens and the sixth lens is an aspherical mirror surface. Optionally, the object side and image side of each lens in the first lens, the second lens, the third lens, the fourth lens, the fifth lens and the sixth lens are all aspherical mirror surfaces.

[0056] However, those skilled in the art should understand that, without departing from the technical solution claimed in the present application, the number of lenses constituting the optical imaging lens can be changed to obtain the various results and advantages described in this specification. For example, although six lenses are described as an example in the embodiments, the optical imaging lens is not limited to including six lenses. If necessary, the optical imaging lens may also include other numbers of lenses.

[0057] Specific embodiments of the optical imaging lens applicable to the above-mentioned embodiments are further described below with reference to the accompanying drawings.

[0058] Example 1

[0059] The following reference Figures 1 to 2D An optical imaging lens according to Embodiment 1 of the present application is described. Figure 1 A schematic structural diagram of an optical imaging lens according to Embodiment 1 of the present application is shown.

[0060] like Figure 1As shown, the optical imaging lens includes, from the object side to the image side, a first lens E1, a second lens E2, an aperture STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a filter E7 and an imaging surface S15.

[0061] The first lens E1 has positive focal power, and its object side surface S1 is convex, and its image side surface S2 is concave. The second lens E2 has negative focal power, and its object side surface S3 is convex, and its image side surface S4 is concave. The third lens E3 has positive focal power, and its object side surface S5 is concave, and its image side surface S6 is convex. The fourth lens E4 has negative focal power, and its object side surface S7 is concave, and its image side surface S8 is concave. The fifth lens E5 has positive focal power, and its object side surface S9 is concave, and its image side surface S10 is convex. The sixth lens E6 has negative focal power, and its object side surface S11 is convex, and its image side surface S12 is concave. The filter E7 has an object side surface S13 and an image side surface S14. The light from the object passes through each surface S1 to S14 in sequence and is finally imaged on the imaging surface S15.

[0062] Table 1 shows the basic parameters of the optical imaging lens of Example 1, wherein the units of the radius of curvature, thickness / distance and focal length are all millimeters (mm).

[0063]

[0064]

[0065] Table 1

[0066] In this example, the total effective focal length f of the optical imaging lens is 2.37 mm, the total length TTL of the optical imaging lens (i.e., the distance from the object-side surface S1 of the first lens E1 to the imaging surface S15 of the optical imaging lens on the optical axis) is 6.08 mm, half of the diagonal length of the effective pixel area on the imaging surface S15 of the optical imaging lens ImgH is 3.63 mm, half of the maximum field of view Semi-FOV of the optical imaging lens is 62.0°, and the aperture value Fno of the optical imaging lens is 2.28.

[0067] In Example 1, the object side surface and the image side surface of any lens among the first lens E1 to the sixth lens E6 are both aspherical surfaces, and the surface shape x of each aspherical lens can be defined by but not limited to the following aspherical surface formula:

[0068]

[0069] Wherein, x is the distance vector height from the vertex of the aspheric surface when the aspheric surface is at a height of h along the optical axis; c is the paraxial curvature of the aspheric surface, c=1 / R (i.e., the paraxial curvature c is the reciprocal of the curvature radius R in Table 1 above); k is the cone coefficient; Ai is the correction coefficient of the i-th order of the aspheric surface. The following Tables 2-1 and 2-2 give the high-order coefficients A that can be used for each aspheric mirror surface S1-S12 in Example 1 4 , A 6 , A 8 , A 10 , A 12 , A 14 , A 16 , A 18 , A 20 , A 22 , A 24 , A 26 , A 28 and A 30 .

[0070]

[0071]

[0072] Table 2-1

[0073] Face number A18 A20 A22 A24 A26 A28 A30 S1 -7.8220E-01 2.8882E-01 -7.5876E-02 1.3790E-02 -1.6418E-03 1.1470E-04 -3.5489E-06 S2 -4.8046E+01 3.0339E+01 -1.3705E+01 4.3236E+00 -9.0528E-01 1.1307E-01 -6.3756E-03 S3 5.5234E+03 -6.4798E+03 5.3734E+03 -3.0859E+03 1.1691E+03 -2.6307E+02 2.6650E+01 S4 2.3882E+06 -5.3203E+06 8.4591E+06 -9.3640E+06 6.8541E+06 -2.9805E+06 5.8266E+05 S5 -4.0248E+07 1.4732E+08 -3.8674E+08 7.0945E+08 -8.6333E+08 6.2615E+08 -2.0487E+08 S6 -1.8503E+05 3.0062E+05 -3.5122E+05 2.8716E+05 -1.5585E+05 5.0416E+04 -7.3547E+03 S7 -5.3809E+02 4.5117E+02 -2.8075E+02 1.2585E+02 -3.8377E+01 7.1126E+00 -6.0354E-01 S8 1.7238E+01 -1.3142E+01 6.8193E+00 -2.3955E+00 5.4698E-01 -7.3424E-02 4.4035E-03 S9 -8.7028E-02 6.2016E-02 -2.5842E-02 6.6960E-03 -1.0626E-03 9.4253E-05 -3.5475E-06 S10 -3.2434E+00 1.3682E+00 -4.1647E-01 8.8812E-02 -1.2567E-02 1.0585E-03 -4.0136E-05 S11 -6.9253E-03 3.2638E-04 1.4203E-04 -3.7761E-05 4.4461E-06 -2.7053E-07 6.8971E-09 S12 -4.2377E-05 1.4999E-06 3.3607E-07 -5.9425E-08 4.4860E-09 -1.7327E-10 2.7924E-12

[0074] Table 2-2

[0075] Figure 2A The axial chromatic aberration curve of the optical imaging lens of Example 1 is shown, which indicates the deviation of light of different wavelengths from the focal point behind the lens. Figure 2B The astigmatism curve of the optical imaging lens of Example 1 is shown, which represents the meridional image curvature and the sagittal image curvature. Figure 2C The distortion curve of the optical imaging lens of Example 1 is shown, which represents the distortion magnitude values ​​corresponding to different field angles. Figure 2D The magnification chromatic aberration curve of the optical imaging lens of Example 1 is shown, which represents the deviation of different image heights on the imaging surface after the light passes through the lens. FIG. 2A to FIG. 2D It can be seen that the optical imaging lens provided in Example 1 can achieve good imaging quality.

[0076] Example 2

[0077] The following reference Figures 3 to 4D The optical imaging lens according to Embodiment 2 of the present application is described. In this embodiment and the following embodiments, for the sake of brevity, some descriptions similar to Embodiment 1 will be omitted. Figure 3 A schematic structural diagram of an optical imaging lens according to Embodiment 2 of the present application is shown.

[0078] like Figure 3 As shown, the optical imaging lens includes, from the object side to the image side, a first lens E1, a second lens E2, an aperture STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a filter E7 and an imaging surface S15.

[0079] The first lens E1 has negative optical power, and its object side surface S1 is concave, and its image side surface S2 is convex. The second lens E2 has positive optical power, and its object side surface S3 is convex, and its image side surface S4 is concave. The third lens E3 has positive optical power, and its object side surface S5 is concave, and its image side surface S6 is convex. The fourth lens E4 has negative optical power, and its object side surface S7 is convex, and its image side surface S8 is concave. The fifth lens E5 has positive optical power, and its object side surface S9 is concave, and its image side surface S10 is convex. The sixth lens E6 has negative optical power, and its object side surface S11 is convex, and its image side surface S12 is concave. The filter E7 has an object side surface S13 and an image side surface S14. The light from the object passes through each surface S1 to S14 in sequence and is finally imaged on the imaging surface S15.

[0080] In this example, the total effective focal length f of the optical imaging lens is 2.26 mm, the total length TTL of the optical imaging lens is 5.95 mm, half of the diagonal length ImgH of the effective pixel area on the imaging surface S15 of the optical imaging lens is 3.63 mm, half of the maximum field of view Semi-FOV of the optical imaging lens is 61.4°, and the aperture value Fno of the optical imaging lens is 2.28.

[0081] Table 3 shows the basic parameters of the optical imaging lens of Example 2, wherein the units of the radius of curvature, thickness / distance and focal length are all in millimeters (mm). Tables 4-1 and 4-2 show the high-order coefficients of each aspherical mirror surface that can be used in Example 2, wherein the surface type of each aspherical surface can be defined by the formula (1) given in the above Example 1.

[0082]

[0083] Table 3

[0084]

[0085]

[0086] Table 4-1

[0087] Face number A18 A20 A22 A24 A26 A28 A30 S1 -4.7846E-03 3.2309E-04 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 S2 -3.9949E+02 3.5724E+02 -2.2435E+02 9.6190E+01 -2.6614E+01 4.2373E+00 -2.8974E-01 S3 2.4084E+03 -2.5723E+03 1.9449E+03 -1.0183E+03 3.5175E+02 -7.2167E+01 6.6657E+00 S4 1.0480E+06 -2.1276E+06 3.0858E+06 -3.1167E+06 2.0815E+06 -8.2583E+05 1.4730E+05 S5 -5.2909E+07 2.0487E+08 -5.6297E+08 1.0713E+09 -1.3417E+09 9.9456E+08 -3.3048E+08 S6 -2.9429E+04 3.5715E+04 -2.8204E+04 1.2391E+04 -1.0966E+03 -1.4242E+03 4.6184E+02 S7 -2.9208E+03 2.9495E+03 -2.1491E+03 1.0977E+03 -3.7217E+02 7.5089E+01 -6.8095E+00 S8 -2.2807E+02 1.7855E+02 -1.0117E+02 4.0322E+01 -1.0711E+01 1.7010E+00 -1.2211E-01 S9 2.5695E+00 -1.2922E+00 4.2528E-01 -8.2761E-02 6.4364E-03 5.6079E-04 -1.0850E-04 S10 -3.9980E+00 1.8454E+00 -6.3466E-01 1.5685E-01 -2.6226E-02 2.6477E-03 -1.2155E-04 S11 -3.3009E-01 8.4752E-02 -1.5694E-02 2.0393E-03 -1.7627E-04 9.0970E-06 -2.1197E-07 S12 3.1695E-03 -3.0241E-04 1.1116E-05 1.0744E-06 -1.6824E-07 9.1229E-09 -1.8918E-10

[0088] Table 4-2

[0089] Figure 4AThe axial chromatic aberration curve of the optical imaging lens of Example 2 is shown, which indicates that light of different wavelengths deviates from the focal point behind the lens. Figure 4B The astigmatism curve of the optical imaging lens of Example 2 is shown, which represents the meridional image curvature and the sagittal image curvature. Figure 4C The distortion curve of the optical imaging lens of Example 2 is shown, which represents the distortion magnitude values ​​corresponding to different field angles. Figure 4D The magnification chromatic aberration curve of the optical imaging lens of Example 2 is shown, which represents the deviation of different image heights on the imaging surface after the light passes through the lens. FIG. 4A to FIG. 4D It can be seen that the optical imaging lens provided in Example 2 can achieve good imaging quality.

[0090] Example 3

[0091] The following reference Figures 5 to 6D An optical imaging lens according to Embodiment 3 of the present application is described. Figure 5 A schematic structural diagram of an optical imaging lens according to Embodiment 3 of the present application is shown.

[0092] like Figure 5 As shown, the optical imaging lens includes, from the object side to the image side, a first lens E1, a second lens E2, an aperture STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a filter E7 and an imaging surface S15.

[0093] The first lens E1 has negative optical power, and its object side surface S1 is concave, and its image side surface S2 is concave. The second lens E2 has negative optical power, and its object side surface S3 is concave, and its image side surface S4 is concave. The third lens E3 has positive optical power, and its object side surface S5 is concave, and its image side surface S6 is convex. The fourth lens E4 has negative optical power, and its object side surface S7 is concave, and its image side surface S8 is concave. The fifth lens E5 has positive optical power, and its object side surface S9 is concave, and its image side surface S10 is convex. The sixth lens E6 has negative optical power, and its object side surface S11 is convex, and its image side surface S12 is concave. The filter E7 has an object side surface S13 and an image side surface S14. The light from the object passes through each surface S1 to S14 in sequence and is finally imaged on the imaging surface S15.

[0094] In this example, the total effective focal length f of the optical imaging lens is 2.19 mm, the total length TTL of the optical imaging lens is 5.77 mm, half of the diagonal length ImgH of the effective pixel area on the imaging surface S15 of the optical imaging lens is 3.63 mm, half of the maximum field of view Semi-FOV of the optical imaging lens is 63.6°, and the aperture value Fno of the optical imaging lens is 2.28.

[0095] Table 5 shows the basic parameters of the optical imaging lens of Example 3, wherein the units of the radius of curvature, thickness / distance and focal length are all in millimeters (mm). Tables 6-1 and 6-2 show the high-order coefficients of each aspherical mirror surface that can be used in Example 3, wherein the surface type of each aspherical surface can be defined by the formula (1) given in the above Example 1.

[0096]

[0097] Table 5

[0098]

[0099]

[0100] Table 6-1

[0101] Face number A18 A20 A22 A24 A26 A28 A30 S1 -3.7011E+00 1.6174E+00 -5.0147E-01 1.0710E-01 -1.4881E-02 1.1999E-03 -4.2045E-05 S2 -1.5006E+01 8.2861E+00 -3.2645E+00 8.9524E-01 -1.6222E-01 1.7430E-02 -8.3861E-04 S3 7.9660E+01 -5.8351E+01 3.0212E+01 -1.0833E+01 2.5625E+00 -3.6004E-01 2.2773E-02 S4 7.5957E+05 -1.4899E+06 2.0857E+06 -2.0329E+06 1.3101E+06 -5.0162E+05 8.6343E+04 S5 2.2041E+07 -7.9512E+07 2.0545E+08 -3.7100E+08 4.4493E+08 -3.1871E+08 1.0332E+08 S6 -2.6563E+05 4.5241E+05 -5.5668E+05 4.8170E+05 -2.7804E+05 9.6105E+04 -1.5047E+04 S7 -2.4641E+02 1.8898E+02 -1.0751E+02 4.4053E+01 -1.2277E+01 2.0794E+00 -1.6125E-01 S8 1.9798E+01 -1.5322E+01 8.0712E+00 -2.8783E+00 6.6717E-01 -9.0913E-02 5.5348E-03 S9 -1.3375E-01 1.0031E-01 -4.3751E-02 1.1818E-02 -1.9459E-03 1.7777E-04 -6.8050E-06 S10 -4.6933E+00 2.0111E+00 -6.1687E-01 1.3083E-01 -1.8044E-02 1.4363E-03 -4.8962E-05 S11 -1.6464E-02 1.1769E-03 2.8357E-04 -9.4220E-05 1.2472E-05 -8.3681E-07 2.3351E-08 S12 -8.4468E-05 3.4404E-06 7.2835E-07 -1.4241E-07 1.1657E-08 -4.8652E-10 8.4616E-12

[0102] Table 6-2

[0103] Fig. 6A The axial chromatic aberration curve of the optical imaging lens of Example 3 is shown, which indicates that light of different wavelengths deviates from the focal point behind the lens. Figure 6B The astigmatism curve of the optical imaging lens of Example 3 is shown, which represents the meridional image curvature and the sagittal image curvature. Figure 6C The distortion curve of the optical imaging lens of Example 3 is shown, which represents the distortion magnitude values ​​corresponding to different field angles. Fig.6D The magnification chromatic aberration curve of the optical imaging lens of Example 3 is shown, which represents the deviation of different image heights on the imaging surface after the light passes through the lens. FIG. 6A to FIG. 6D It can be seen that the optical imaging lens provided in Example 3 can achieve good imaging quality.

[0104] Example 4

[0105] The following reference Figures 7 to 8D An optical imaging lens according to Embodiment 4 of the present application is described. Figure 7 A schematic structural diagram of an optical imaging lens according to Embodiment 4 of the present application is shown.

[0106] like Figure 7 As shown, the optical imaging lens includes, from the object side to the image side, a first lens E1, a second lens E2, an aperture STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a filter E7 and an imaging surface S15.

[0107] The first lens E1 has negative optical power, and its object side surface S1 is concave, and its image side surface S2 is convex. The second lens E2 has negative optical power, and its object side surface S3 is concave, and its image side surface S4 is convex. The third lens E3 has positive optical power, and its object side surface S5 is concave, and its image side surface S6 is convex. The fourth lens E4 has negative optical power, and its object side surface S7 is concave, and its image side surface S8 is concave. The fifth lens E5 has positive optical power, and its object side surface S9 is concave, and its image side surface S10 is convex. The sixth lens E6 has negative optical power, and its object side surface S11 is convex, and its image side surface S12 is concave. The filter E7 has an object side surface S13 and an image side surface S14. The light from the object passes through each surface S1 to S14 in sequence and is finally imaged on the imaging surface S15.

[0108] In this example, the total effective focal length f of the optical imaging lens is 2.31 mm, the total length TTL of the optical imaging lens is 6.54 mm, half of the diagonal length ImgH of the effective pixel area on the imaging surface S15 of the optical imaging lens is 3.63 mm, half of the maximum field of view Semi-FOV of the optical imaging lens is 62.0°, and the aperture value Fno of the optical imaging lens is 2.28.

[0109] Table 7 shows the basic parameters of the optical imaging lens of Example 4, wherein the units of the radius of curvature, thickness / distance and focal length are all in millimeters (mm). Tables 8-1 and 8-2 show the high-order coefficients of each aspherical mirror surface that can be used in Example 4, wherein the surface type of each aspherical surface can be defined by the formula (1) given in the above Example 1.

[0110]

[0111] Table 7

[0112]

[0113]

[0114] Table 8-1

[0115] Face number A18 A20 A22 A24 A26 A28 A30 S1 1.8387E-04 -2.7582E-05 2.2490E-06 -7.6865E-08 0.0000E+00 0.0000E+00 0.0000E+00 S2 -6.2812E-01 2.4017E-01 -6.4332E-02 1.1541E-02 -1.2524E-03 6.2455E-05 0.0000E+00 S3 6.4827E-01 -2.7823E-01 8.4406E-02 -1.7733E-02 2.4577E-03 -2.0232E-04 7.4976E-06 S4 6.2192E+03 -7.1523E+03 5.8706E+03 -3.3548E+03 1.2677E+03 -2.8458E+02 2.8720E+01 S5 -4.5857E+07 1.7184E+08 -4.5808E+08 8.4677E+08 -1.0310E+09 7.4326E+08 -2.4028E+08 S6 3.8142E+03 -5.8165E+03 5.1765E+03 -1.9932E+03 -6.5442E+02 9.6013E+02 -2.8030E+02 S7 -3.6851E+01 2.2842E+01 -1.0494E+01 3.4688E+00 -7.7899E-01 1.0618E-01 -6.6171E-03 S8 2.5540E+00 -1.5736E+00 6.5977E-01 -1.8722E-01 3.4521E-02 -3.7403E-03 1.8096E-04 S9 -2.0262E-02 1.2247E-02 -4.2445E-03 8.7307E-04 -1.0050E-04 5.0311E-06 0.0000E+00 S10 -1.0030E+00 4.0156E-01 -1.1614E-01 2.3601E-02 -3.1989E-03 2.6034E-04 -9.6678E-06 S11 1.5491E-03 -4.2066E-04 7.2782E-05 -8.5070E-06 6.6464E-07 -3.1929E-08 7.2086E-10 S12 1.3368E-03 -2.2059E-04 2.5611E-05 -2.0470E-06 1.0726E-07 -3.3171E-09 4.5901E-11

[0116] Table 8-2

[0117] Fig. 8A The axial chromatic aberration curve of the optical imaging lens of Example 4 is shown, which indicates the deviation of light of different wavelengths from the focal point behind the lens. Figure 8B The astigmatism curve of the optical imaging lens of Example 4 is shown, which represents the meridional image curvature and the sagittal image curvature. Figure 8C The distortion curve of the optical imaging lens of Example 4 is shown, which represents the distortion magnitude values ​​corresponding to different field angles. Fig.8DThe magnification chromatic aberration curve of the optical imaging lens of Example 4 is shown, which represents the deviation of different image heights on the imaging surface after the light passes through the lens. FIG. 8A to FIG. 8D It can be seen that the optical imaging lens provided in Example 4 can achieve good imaging quality.

[0118] Example 5

[0119] The following reference Figures 9 to 10D An optical imaging lens according to Embodiment 5 of the present application is described. Fig. 9 A schematic structural diagram of an optical imaging lens according to Embodiment 5 of the present application is shown.

[0120] like Fig. 9 As shown, the optical imaging lens includes, from the object side to the image side, a first lens E1, a second lens E2, an aperture STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a filter E7 and an imaging surface S15.

[0121] The first lens E1 has positive focal power, and its object side surface S1 is convex, and its image side surface S2 is convex. The second lens E2 has negative focal power, and its object side surface S3 is convex, and its image side surface S4 is concave. The third lens E3 has positive focal power, and its object side surface S5 is concave, and its image side surface S6 is convex. The fourth lens E4 has negative focal power, and its object side surface S7 is convex, and its image side surface S8 is concave. The fifth lens E5 has positive focal power, and its object side surface S9 is concave, and its image side surface S10 is convex. The sixth lens E6 has negative focal power, and its object side surface S11 is convex, and its image side surface S12 is concave. The filter E7 has an object side surface S13 and an image side surface S14. The light from the object passes through each surface S1 to S14 in sequence and is finally imaged on the imaging surface S15.

[0122] In this example, the total effective focal length f of the optical imaging lens is 2.30 mm, the total length TTL of the optical imaging lens is 5.74 mm, half of the diagonal length ImgH of the effective pixel area on the imaging surface S15 of the optical imaging lens is 3.63 mm, half of the maximum field of view Semi-FOV of the optical imaging lens is 61.2°, and the aperture value Fno of the optical imaging lens is 2.28.

[0123] Table 9 shows the basic parameters of the optical imaging lens of Example 5, wherein the units of the radius of curvature, thickness / distance and focal length are all in millimeters (mm). Tables 10-1 and 10-2 show the high-order coefficients of each aspherical mirror surface that can be used in Example 5, wherein the surface shape of each aspherical surface can be defined by the formula (1) given in the above Example 1.

[0124]

[0125] Table 9

[0126]

[0127]

[0128] Table 10-1

[0129] Face number A18 A20 A22 A24 A26 A28 A30 S1 -2.3756E+00 9.8944E-01 -2.9277E-01 5.9809E-02 -7.9801E-03 6.2224E-04 -2.1357E-05 S2 -4.7556E+01 2.9999E+01 -1.3535E+01 4.2646E+00 -8.9173E-01 1.1122E-01 -6.2619E-03 S3 3.6867E+03 -4.1419E+03 3.2884E+03 -1.8078E+03 6.5560E+02 -1.4122E+02 1.3696E+01 S4 2.7863E+06 -6.3231E+06 1.0237E+07 -1.1535E+07 8.5899E+06 -3.7983E+06 7.5461E+05 S5 -5.0432E+07 1.8927E+08 -5.0950E+08 9.5837E+08 -1.1958E+09 8.8932E+08 -2.9836E+08 S6 -1.5332E+05 2.4483E+05 -2.8124E+05 2.2613E+05 -1.2072E+05 3.8413E+04 -5.5126E+03 S7 -2.3241E+02 1.7751E+02 -1.0062E+02 4.1090E+01 -1.1414E+01 1.9270E+00 -1.4895E-01 S8 1.0736E+01 -7.7659E+00 3.8232E+00 -1.2742E+00 2.7604E-01 -3.5155E-02 2.0003E-03 S9 -3.4231E-01 2.8614E-01 -1.3946E-01 4.2224E-02 -7.8274E-03 8.1100E-04 -3.5666E-05 S10 -5.8709E+00 2.6630E+00 -8.7379E-01 2.0104E-01 -3.0681E-02 2.7836E-03 -1.1345E-04 S11 -1.6763E-02 1.3046E-03 2.5126E-04 -8.9069E-05 1.1966E-05 -8.0884E-07 2.2695E-08 S12 -6.9376E-05 2.6489E-06 6.0047E-07 -1.1299E-07 9.0217E-09 -3.6816E-10 6.2661E-12

[0130] Table 10-2

[0131] Fig. 10A The axial chromatic aberration curve of the optical imaging lens of Example 5 is shown, which indicates the deviation of light of different wavelengths from the focal point behind the lens. Fig. 10B The astigmatism curve of the optical imaging lens of Example 5 is shown, which represents the meridional image curvature and the sagittal image curvature. Fig. 10C The distortion curve of the optical imaging lens of Example 5 is shown, which represents the distortion magnitude values ​​corresponding to different field angles. Fig. 10D The magnification chromatic aberration curve of the optical imaging lens of Example 5 is shown, which represents the deviation of different image heights on the imaging surface after the light passes through the lens. FIG. 10A to FIG. 10D It can be seen that the optical imaging lens provided in Example 5 can achieve good imaging quality.

[0132] Example 6

[0133] The following reference Figures 11 to 12D An optical imaging lens according to Embodiment 6 of the present application is described. Fig.11 A schematic structural diagram of an optical imaging lens according to Example 6 of the present application is shown.

[0134] like Fig.11 As shown, the optical imaging lens includes, from the object side to the image side, a first lens E1, a second lens E2, an aperture STO, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a filter E7 and an imaging surface S15.

[0135] The first lens E1 has positive focal power, and its object side surface S1 is convex, and its image side surface S2 is concave. The second lens E2 has negative focal power, and its object side surface S3 is convex, and its image side surface S4 is concave. The third lens E3 has positive focal power, and its object side surface S5 is concave, and its image side surface S6 is convex. The fourth lens E4 has negative focal power, and its object side surface S7 is concave, and its image side surface S8 is convex. The fifth lens E5 has positive focal power, and its object side surface S9 is concave, and its image side surface S10 is convex. The sixth lens E6 has negative focal power, and its object side surface S11 is convex, and its image side surface S12 is concave. The filter E7 has an object side surface S13 and an image side surface S14. The light from the object passes through each surface S1 to S14 in sequence and is finally imaged on the imaging surface S15.

[0136] In this example, the total effective focal length f of the optical imaging lens is 2.34 mm, the total length TTL of the optical imaging lens is 6.00 mm, half of the diagonal length ImgH of the effective pixel area on the imaging surface S15 of the optical imaging lens is 3.63 mm, half of the maximum field of view Semi-FOV of the optical imaging lens is 62.7°, and the aperture value Fno of the optical imaging lens is 2.78.

[0137] Table 11 shows the basic parameters of the optical imaging lens of Example 6, wherein the units of the radius of curvature, thickness / distance and focal length are all in millimeters (mm). Tables 12-1 and 12-2 show the high-order coefficients of each aspherical mirror surface that can be used in Example 6, wherein the surface shape of each aspherical surface can be defined by the formula (1) given in the above Example 1.

[0138]

[0139] Table 11

[0140]

[0141]

[0142] Table 12-1

[0143] Face number A18 A20 A22 A24 A26 A28 A30 S1 -1.4281E+00 5.6313E-01 -1.5789E-01 3.0597E-02 -3.8791E-03 2.8807E-04 -9.4494E-06 S2 -5.3468E+01 3.4185E+01 -1.5634E+01 4.9930E+00 -1.0583E+00 1.3379E-01 -7.6364E-03 S3 4.3511E+03 -4.9815E+03 4.0303E+03 -2.2577E+03 8.3427E+02 -1.8309E+02 1.8090E+01 S4 2.0454E+06 -4.4842E+06 7.0157E+06 -7.6411E+06 5.5024E+06 -2.3537E+06 4.5256E+05 S5 -6.4261E+07 2.4276E+08 -6.5641E+08 1.2376E+09 -1.5441E+09 1.1451E+09 -3.8203E+08 S6 -1.7231E+05 2.7502E+05 -3.1657E+05 2.5588E+05 -1.3780E+05 4.4397E+04 -6.4741E+03 S7 -1.0397E+03 9.3790E+02 -6.2793E+02 3.0286E+02 -9.9364E+01 1.9814E+01 -1.8089E+00 S8 4.8050E+01 -4.1053E+01 2.3872E+01 -9.3978E+00 2.4047E+00 -3.6174E-01 2.4313E-02 S9 -5.4515E-02 3.6993E-02 -1.4652E-02 3.6052E-03 -5.4296E-04 4.5667E-05 -1.6279E-06 S10 -1.9959E+00 8.0548E-01 -2.3509E-01 4.8140E-02 -6.5473E-03 5.3045E-04 -1.9359E-05 S11 -4.6959E-03 1.2195E-04 1.1873E-04 -2.7841E-05 3.0890E-06 -1.7956E-07 4.3957E-09 S12 -3.1100E-05 1.0797E-06 2.2668E-07 -3.8932E-08 2.8425E-09 -1.0610E-10 1.6519E-12

[0144] Table 12-2

[0145] Fig. 12A The axial chromatic aberration curve of the optical imaging lens of Example 6 is shown, which indicates the deviation of light of different wavelengths from the focal point behind the lens. Fig. 12B The astigmatism curve of the optical imaging lens of Example 6 is shown, which represents the meridional image curvature and the sagittal image curvature. Fig. 12C The distortion curve of the optical imaging lens of Example 6 is shown, which represents the distortion magnitude values ​​corresponding to different field angles. Fig.12DThe magnification chromatic aberration curve of the optical imaging lens of Example 6 is shown, which represents the deviation of different image heights on the imaging surface after the light passes through the lens. FIG. 12A to FIG. 12D It can be seen that the optical imaging lens provided in Example 6 can achieve good imaging quality.

[0146] In summary, Examples 1 to 6 respectively satisfy the relationships shown in Table 13.

[0147]

[0148]

[0149] Table 13

[0150] The present application also provides an imaging device, whose electronic photosensitive element can be a photosensitive coupled device (CCD) or a complementary metal oxide semiconductor element (CMOS). The imaging device can be an independent imaging device such as a digital camera, or an imaging module integrated in a mobile electronic device such as a mobile phone. The imaging device is equipped with the optical imaging lens described above.

[0151] The above description is only a preferred embodiment of the present application and an explanation of the technical principles used. Those skilled in the art should understand that the scope of the invention involved in the present application is not limited to the technical solution formed by a specific combination of the above technical features, but should also cover other technical solutions formed by any combination of the above technical features or their equivalent features without departing from the inventive concept. For example, the above features are replaced with the technical features with similar functions disclosed in this application (but not limited to) by each other.

Claims

1. An optical imaging lens, characterized in that: Along the optical axis from the object side to the image side, they include: A first lens having optical power, whose object side surface is convex or concave and whose image side surface is convex or concave; a second lens having optical power, whose object side surface is convex or concave and whose image side surface is convex or concave; The third lens has positive power, its object side surface is concave and its image side surface is convex; a fourth lens having negative power, whose object side surface is convex or concave and whose image side surface is convex or concave; a fifth lens element having positive refractive power, whose object-side surface is concave and whose image-side surface is convex; and a sixth lens having negative optical power, whose object side surface is convex and whose image side surface is concave; Wherein, the number of lenses having optical power in the optical imaging lens is six; The effective focal length f3 of the third lens and the effective focal length f4 of the fourth lens satisfy: -2.60≤f4 / f3≤-1.9; The curvature radius R5 of the object-side surface of the third lens and the curvature radius R9 of the object-side surface of the fifth lens satisfy: 3.52≤R5 / R9≤11.39; and A center thickness CT5 of the fifth lens on the optical axis and a center thickness CT2 of the second lens on the optical axis satisfy: 3.69≤CT5 / CT2≤5.

86.

2. The optical imaging lens according to claim 1, wherein: Half of the maximum field of view Semi-FOV of the optical imaging lens satisfies: 61.2°≤Semi-FOV≤63.6°.

3. The optical imaging lens according to claim 1, wherein: A curvature radius R9 of the object-side surface of the fifth lens and an effective focal length f5 of the fifth lens satisfy: -3.66≤R9 / f5≤-1.

99.

4. The optical imaging lens according to claim 1, wherein: A center thickness CT3 of the third lens on the optical axis and a spacing distance T12 between the first lens and the second lens on the optical axis satisfy: 3.10≤CT3 / T12≤9.

18.

5. The optical imaging lens according to claim 1, wherein: A center thickness CT6 of the sixth lens on the optical axis and a spacing distance T56 between the fifth lens and the sixth lens on the optical axis satisfy: 1.52≤CT6 / T56≤6.

45.

6. The optical imaging lens according to claim 1, wherein: A distance T23 between the second lens and the third lens on the optical axis and a center thickness CT2 of the second lens on the optical axis satisfy: 1.26≤T23 / CT2≤1.

99.

7. The optical imaging lens according to claim 1, wherein: A curvature radius R11 of the object-side surface of the sixth lens and an effective focal length f6 of the sixth lens satisfy: -0.55≤R11 / f6≤-0.

32.

8. The optical imaging lens according to claim 1, wherein: A distance TTL from the object side surface of the first lens to the imaging surface of the optical imaging lens on the optical axis and half of the diagonal length of the effective pixel area on the imaging surface of the optical imaging lens ImgH satisfy: 1.58≤TTL / ImgH≤1.

80.

9. The optical imaging lens according to claim 1, wherein: A distance T23 between the second lens and the third lens on the optical axis, a distance T34 between the third lens and the fourth lens on the optical axis, and a distance T56 between the fifth lens and the sixth lens on the optical axis satisfy: 1.21≤T23 / (T34+T56)≤1.

99.

10. The optical imaging lens according to claim 1, wherein: The sum ΣCT of the center thicknesses of the first lens to the sixth lens on the optical axis and the sum ΣAT of the spacing distances between any two adjacent lenses of the first lens to the sixth lens on the optical axis satisfy: 2.56≤ΣCT / ΣAT≤3.

29.

11. The optical imaging lens according to claim 1, wherein: The first lens, the second lens, and the third lens have the same refractive index.