Optical imaging lens

Through the combination of double prism structure and multi-piece lenses, the telephoto lens design is optimized, which solves the problem of lens length becoming longer, and realizes the ultra-large field of view and ultra-thin characteristics, which is suitable for portable electronic products.

CN111399181BActive Publication Date: 2024-12-20ZHEJIANG SUNNY OPTICAL CO LTD
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Patent Information

Application Number
CN202010343329.3
Authority / Receiving Office
CN · China
Patent Type
Patents(China)
Current Assignee / Owner
Filing Date
2020-04-27
Publication Date
2024-12-20
Estimated Expiration
2040-04-27

AI Technical Summary

Technical Problem

The existing telephoto lens design results in the overall optical length of the lens becoming longer, making it difficult to meet the ultra-thin characteristics of the mobile phone, and the conventional coaxial telephoto solution cannot effectively shorten the lateral distance of the lens.

Method used

Using a combination of double prism structure and multi-piece lenses, including lenses with negative and positive power, the combined focal length and curvature radius of the lens are reasonably controlled, and combined with a prism with a 45° angle, the total effective focal length of the optical imaging lens is optimized and The maximum field of view angle relationship shortens the lateral and longitudinal distances of the lens.

Benefits of technology

It achieves the shortening of the lens lateral distance while maintaining a small longitudinal distance, provides a large field of view and good light convergence capability, and is suitable for portable electronic products, expanding the design possibilities of mobile phone camera modules.

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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 negative optical power; a first prism including an incident surface, a reflection surface and an exit surface, wherein the angle between the reflection surface and the optical axis is 45°; an aperture; a second lens with positive optical power; a third lens with optical power; a fourth lens with positive optical power; a fifth lens with negative optical power; and a second prism including an incident surface, a reflection surface and an exit surface, wherein the angle between the reflection surface and the optical axis is 45°; wherein the total effective focal length f of the optical imaging lens and the maximum field of view FOV of the optical imaging lens satisfy: 2.50 mm<f×tan 2 (FOV / 2)<4.00mm.
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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 including five lenses and a double prism structure. Background Art

[0002] Recently, most mobile phones sold on the market have a 3+1 lens configuration including a large image lens, a wide-angle lens, a telephoto lens, and a TOF lens. Among them, most telephoto lenses have 5x, 10x, and 15x optical zoom capabilities. If a conventional coaxial telephoto solution is used, the total optical length (TTL) of the lens will be longer to meet the long focal length of the telephoto lens, which may make the mobile phone unable to meet the ultra-thin requirements. Therefore, an optical imaging lens with prism refraction performance came into being, which can effectively reduce the length of the mobile phone lens in the direction of light incidence.

[0003] Different from a single-prism optical imaging system, the present technical solution is a dual-prism optical imaging system, which can ensure that the incident direction of light is perpendicular to the imaging surface of the optical imaging lens, and can shorten the lateral distance of the optical imaging lens while maintaining a small longitudinal distance of the lens, so that the mobile phone system with the optical imaging lens of the present solution has better application prospects. Summary of the invention

[0004] The present application provides an optical imaging lens applicable to portable electronic products, which can at least solve or partially solve at least one of the above-mentioned shortcomings in the prior art, such as an optical imaging lens with ultra-large field of view and ultra-thin characteristics.

[0005] One aspect of 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 negative optical power; a first prism including an incident surface, a reflection surface and an exit surface, wherein the angle between the reflection surface and the optical axis is 45°; an aperture; a second lens with positive optical power; a third lens with optical power; a fourth lens with positive optical power; a fifth lens with negative optical power; and a second prism including an incident surface, a reflection surface and an exit surface, wherein the angle between the reflection surface and the optical axis is 45°.

[0006] In one embodiment, the total effective focal length f of the optical imaging lens and the maximum field of view FOV of the optical imaging lens may satisfy: 2.50 mm < f × tan 2 (FOV / 2)<4.00mm.

[0007] In one embodiment, the combined focal length f23 of the second lens and the third lens and the combined focal length f34 of the third lens and the fourth lens may satisfy: 1.00<f34 / f23<2.50.

[0008] In one embodiment, the effective focal length f1 of the first lens and the effective focal length f5 of the fifth lens may satisfy: 0.50<f1 / f5<2.00.

[0009] In one embodiment, the combined focal length f345 of the third lens, the fourth lens, and the fifth lens and the effective focal length f5 of the fifth lens may satisfy: -8.00<f345 / f5<-2.00.

[0010] In one embodiment, a curvature radius R1 of the object-side surface of the first lens and a curvature radius R2 of the image-side surface of the first lens may satisfy: 2.50<(R1-R2) / (R1+R2)<4.00.

[0011] In one embodiment, the combined focal length f345 of the third lens, the fourth lens, and the fifth lens and the curvature radius R10 of the image-side surface of the fifth lens may satisfy: 7.00<f345 / R10<12.00.

[0012] In one embodiment, the on-axis distance SAG11 from the intersection of the object side surface of the first lens and the optical axis to the effective radius vertex of the object side surface of the first lens and the on-axis distance SAG12 from the intersection of the image side surface of the first lens and the optical axis to the effective radius vertex of the image side surface of the first lens may satisfy: 4.00<SAG12 / SAG11<5.50.

[0013] In one embodiment, a center thickness CT4 of the fourth lens on the optical axis and an air interval T45 between the fourth lens and the fifth lens on the optical axis may satisfy: 24.00<CT4 / T45<52.00.

[0014] In one embodiment, the on-axis distance SAG22 from the intersection of the image side surface of the second lens and the optical axis to the effective radius vertex of the image side surface of the second lens and the on-axis distance SAG31 from the intersection of the object side surface of the third lens and the optical axis to the effective radius vertex of the object side surface of the third lens may satisfy: 3.00<SAG22 / SAG31<9.00.

[0015] In one embodiment, the maximum effective radius DT21 of the object-side surface of the second lens and the maximum effective radius DT22 of the image-side surface of the second lens may satisfy: 11.00<(DT21+DT22) / (DT22-DT21)<17.00.

[0016] In one embodiment, the maximum field of view FOV of the optical imaging lens may satisfy: FOV>88.0°.

[0017] The optical imaging lens provided in the present application includes a plurality of lenses (for example, the first lens to the fifth lens) and a dual prism structure (for example, the first prism and the second prism). By providing two prisms, it is possible to ensure that the incident direction of light is perpendicular to the imaging surface of the lens, and the lateral and longitudinal distances of the lens can be effectively shortened. At the same time, by reasonably controlling the relationship between the total effective focal length and the maximum field of view of the optical imaging lens, and optimizing the optical focal length and surface shape of each lens, it is beneficial for the optical imaging lens to have good light converging ability and ultra-large field of view, so that more models of mobile phone camera modules can be designed according to the reentrant lens of the present technical solution. BRIEF DESCRIPTION OF THE DRAWINGS

[0018] Other features, purposes and advantages of the present application will become more apparent through the following detailed description of non-limiting embodiments in conjunction with the accompanying drawings. In the accompanying 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. 2C The astigmatism curve, distortion curve and relative illumination 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. 4C The astigmatism curve, distortion curve and relative illumination 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. 6C The astigmatism curve, distortion curve and relative illumination 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. 8C The astigmatism curve, distortion curve and relative illumination 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. 10C The astigmatism curve, distortion curve and relative illumination 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;

[0030] FIG. 12A to FIG. 12C The astigmatism curve, distortion curve and relative illumination 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: a first lens, a first prism, an aperture, a second lens, a third lens, a fourth lens, a fifth lens and a second prism in order from the object side to the image side along the optical axis, wherein the first prism and the second prism are arranged so that the angle between their respective reflection surfaces and the optical axis is 45°. There may be air gaps between adjacent lenses and between prisms and lenses.

[0040] Both the first prism and the second prism can be triangular prisms. The triangular prism includes an incident surface, a reflection surface and an exit surface, and the incident surface and the exit surface are perpendicular, so that the light perpendicularly incident to the incident surface is changed by 90° on the reflection surface and then exits perpendicularly to the exit surface. The double triangular prism structure can ensure that the incident direction of light is perpendicular to the imaging surface of the optical imaging lens, and can effectively shorten the lateral distance (i.e., the distance in the direction perpendicular to the imaging surface) of the optical imaging lens while effectively avoiding the longitudinal distance (i.e., the distance in the direction parallel to the imaging surface) being too long, so that the imaging lens can be applied to more portable devices.

[0041] In an exemplary embodiment, the first lens may have negative optical power; the second lens may have positive optical power; the third lens may have positive optical power or negative optical power; the fourth lens may have positive optical power; and the fifth lens may have negative optical power. The optical power and surface shape of each lens in the optical system are reasonably matched to ensure the rationality of the optical imaging lens structure, thereby effectively widening the maximum field of view of the optical imaging lens and enabling the optical system to have good light convergence ability.

[0042] In example embodiments, the object-side surface of the first lens may be a concave surface, and the image-side surface may be a concave surface.

[0043] In example embodiments, the object-side surface of the second lens may be a convex surface, and the image-side surface may be a convex surface.

[0044] In example embodiments, the object-side surface of the third lens may be a convex surface.

[0045] In example embodiments, the image-side surface of the fourth lens may be a convex surface.

[0046] In example embodiments, the image-side surface of the fifth lens may be a concave surface.

[0047] In an exemplary embodiment, the total effective focal length f of the optical imaging lens and the maximum field of view FOV of the optical imaging lens may satisfy: 2.50 mm < f×tan 2 (FOV / 2)<4.00mm. Reasonable control of the relationship between the total effective focal length of the optical imaging lens and the maximum half field of view angle of the optical imaging lens is conducive to controlling the imaging size and imaging range of the optical system, so that the system has a larger imaging surface.

[0048] In an exemplary embodiment, the combined focal length f23 of the second lens and the third lens and the combined focal length f34 of the third lens and the fourth lens may satisfy: 1.00<f34 / f23<2.50. For example, 1.00<f34 / f23<2.10. By controlling the ratio of the combined focal length of the second lens and the third lens to the combined focal length of the third lens and the fourth lens within a reasonable numerical range, the maximum field of view of the optical imaging lens can be increased while ensuring that the imaging lens has a good light convergence ability, and avoiding the occurrence of problems such as increased sensitivity of the imaging lens and difficulty in processing due to excessive concentration of light focal length.

[0049] In an exemplary embodiment, the effective focal length f1 of the first lens and the effective focal length f5 of the fifth lens may satisfy: 0.50<f1 / f5<2.00. For example, 0.80<f1 / f5<1.70. By satisfying this numerical range, the ratio of the effective focal lengths of the first lens and the fifth lens is controlled within a reasonable numerical range, so that the optical imaging lens has a better light converging ability, and at the same time, it can avoid the risk of difficulty in processing the fifth lens due to excessive concentration of light focal length.

[0050] In an exemplary embodiment, the combined focal length f345 of the third lens, the fourth lens and the fifth lens and the effective focal length f5 of the fifth lens may satisfy: -8.00<f345 / f5<-2.00. By controlling the ratio of the combined focal length of the third lens, the fourth lens and the fifth lens to the effective focal length of the fifth lens within a reasonable numerical range, the optical imaging lens can have a basic light converging ability, while avoiding the risk of increased sensitivity of the imaging lens due to excessive light focal concentration.

[0051] In an exemplary embodiment, the radius of curvature R1 of the object side surface of the first lens and the radius of curvature R2 of the image side surface of the first lens may satisfy: 2.50<(R1-R2) / (R1+R2)<4.00. For example, 2.90<(R1-R2) / (R1+R2)<3.80. Reasonable control of the relationship between the radius of curvature of the object side surface and the image side surface of the first lens can increase the maximum field angle of the optical imaging lens while maintaining a relatively small prism size, thereby facilitating the reduction of the lateral size of the imaging lens.

[0052] In an exemplary embodiment, the combined focal length f345 of the third lens, the fourth lens, and the fifth lens and the curvature radius R10 of the image side surface of the fifth lens may satisfy: 7.00<f345 / R10<12.00. By controlling the ratio of the combined focal length of the third lens, the fourth lens, and the fifth lens to the curvature radius of the image side surface of the fifth lens within a reasonable numerical range, the optical imaging lens can have a basic light convergence capability, avoid the risk of imaging lens processing difficulties caused by the absolute value of the curvature radius of the image side surface of the fifth lens being too small, and at the same time effectively reduce the energy intensity of the ghost image generated by the reflection between the fourth lens and the fifth lens.

[0053] In an exemplary embodiment, the on-axis distance SAG11 from the intersection of the object side surface of the first lens and the optical axis to the vertex of the effective radius of the object side surface of the first lens and the on-axis distance SAG12 from the intersection of the image side surface of the first lens and the optical axis to the vertex of the effective radius of the image side surface of the first lens may satisfy: 4.00<SAG12 / SAG11<5.50. For example, 4.20<SAG12 / SAG11<5.10. By controlling the ratio of the sagitta of the object side surface to the image side surface of the first lens within a reasonable numerical range, it is beneficial to increase the maximum field of view of the optical imaging lens while avoiding the situation that the size of the prism in the optical system is too large due to the excessive sagitta of the object side surface or the image side surface of the first lens, which is not conducive to shortening the lateral distance of the imaging lens; at the same time, it can also avoid the situation that the maximum field of view of the optical imaging lens cannot be effectively increased due to the sagitta of the object side surface or the image side surface of the first lens is too small, and the increase in sensitivity of the first lens makes the imaging lens difficult to process.

[0054] In an exemplary embodiment, the center thickness CT4 of the fourth lens on the optical axis and the air interval T45 between the fourth lens and the fifth lens on the optical axis may satisfy: 24.00<CT4 / T45<52.00. By controlling the ratio of the center thickness of the fourth lens on the optical axis to the air interval between the fourth lens and the fifth lens on the optical axis within a reasonable numerical range, the energy intensity of the ghost image generated by the reflection on the object side and the image side of the fourth lens and the reflection between the fourth lens and the fifth lens can be effectively reduced, and the overall imaging quality of the optical imaging lens can be effectively improved.

[0055] In an exemplary embodiment, the axial distance SAG22 from the intersection of the image side surface of the second lens and the optical axis to the effective radius vertex of the image side surface of the second lens and the axial distance SAG31 from the intersection of the object side surface of the third lens and the optical axis to the effective radius vertex of the object side surface of the third lens can satisfy: 3.00<SAG22 / SAG31<9.00. By controlling the ratio of the sagittal height of the image side surface of the second lens to the object side surface of the third lens within a reasonable numerical range, it is beneficial to increase the maximum field angle of the optical imaging lens and improve the aberration correction ability of the imaging lens while avoiding risks such as processing difficulties caused by excessive bending of the edge of the lens.

[0056] In an exemplary embodiment, the maximum effective radius DT21 of the object side surface of the second lens and the maximum effective radius DT22 of the image side surface of the second lens may satisfy: 11.00<(DT21+DT22) / (DT22-DT21)<17.00. By rationally controlling the relationship between the maximum effective radii of the object side surface and the image side surface of the second lens and cooperating with the first lens, the sensitivity of the decentering and curvature radius of the second lens can be reduced while increasing the maximum field angle of the optical imaging lens, thereby improving the processing performance of the second lens.

[0057] In an exemplary embodiment, the maximum field of view FOV of the optical imaging lens can satisfy: FOV>88.0°. For example, 88.0°<FOV<110.0°. By increasing the maximum field of view of the optical imaging lens, it is possible to configure more models of mobile phone camera modules on mobile phones, greatly expanding the scope of use of the dual-prism optical imaging lens. At the same time, it also provides the possibility of further shortening the size of mobile phones.

[0058] In an exemplary embodiment, the optical imaging lens may further include a diaphragm. The diaphragm may be disposed at an appropriate position as required. For example, the diaphragm may be disposed between the first prism and the second lens. Optionally, the optical imaging lens may further include a filter for correcting color deviation and / or a protective glass for protecting a photosensitive element located on the imaging surface.

[0059] The present application proposes an optical imaging lens with an ultra-large field of view and ultra-thin characteristics. The optical imaging lens according to the above-mentioned embodiment of the present application may adopt multiple lenses, such as the five lenses described above. By reasonably allocating the optical focal length, surface shape, effective focal length and curvature radius of each lens, the incident light can be effectively converged, the maximum field of view of the optical imaging lens can be widened, and the processability of the imaging lens can be effectively improved, making the optical imaging lens more conducive to production and processing. In addition, the optical imaging lens according to the present application adopts a dual prism structure, so that the lateral distance of the lens can be effectively shortened while maintaining a small longitudinal distance of the lens.

[0060] In an exemplary embodiment, 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 fifth lens is an aspherical mirror surface. The characteristic of an aspherical lens is that the curvature changes continuously from the center of the lens to the periphery of the lens. Unlike a spherical lens having 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 and the fifth 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 and the fifth lens are all aspherical mirror surfaces.

[0061] 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.

[0062] 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 five lenses are described as an example in the embodiments, the optical imaging lens is not limited to including five lenses. If necessary, the optical imaging lens may also include other numbers of lenses.

[0063] Specific embodiments of the optical imaging lens applicable to the above-mentioned embodiments are further described below with reference to the accompanying drawings.

[0064] Example 1

[0065] The following reference Figures 1 to 2CAn optical imaging lens according to Embodiment 1 of the present application is described. Figure 1 is a schematic diagram showing the structure of an optical imaging lens according to Example 1 of the present application.

[0066] like Figure 1 As shown, the optical imaging lens includes, in order from the object side to the image side along the optical axis: a first lens E1, a first prism E2, an aperture STO, a second lens E3, a third lens E4, a fourth lens E5, a fifth lens E6, a second prism E7, and a filter E8.

[0067] The first lens E1 has negative focal power, and its object side surface S1 is concave, and the image side surface S2 is concave. The incident surface S3, the reflection surface S4 and the exit surface S5 of the first prism E2 are all spherical surfaces, and the reflection surface S4 forms an angle of 45° with the optical axis, so that the light incident perpendicular to the incident surface S3 of the first prism E2 is deflected 90° by the reflection surface S4 and then exits from the first prism E2 perpendicularly to the exit surface S5. The second lens E3 has positive focal power, and its object side surface S6 is convex, and the image side surface S7 is convex. The third lens E4 has negative focal power, and its object side surface S8 is convex, and the image side surface S9 is concave. The fourth lens E5 has positive focal power, and its object side surface S10 is convex, and the image side surface S11 is convex. The fifth lens E6 has negative focal power, and its object side surface S12 is convex, and the image side surface S13 is concave. The incident surface S14, the reflection surface S15 and the exit surface S16 of the second prism E7 are all spherical surfaces, and the reflection surface S15 forms an angle of 45° with the optical axis, so that the light incident perpendicular to the incident surface S14 of the second prism E7 is deflected 90° by the reflection surface S15 and then exits the second prism E7 perpendicular to the exit surface S16. The filter E8 has an object side surface S17 and an image side surface S18. The light from the object passes through each surface S1 to S18 in sequence and is finally imaged on the imaging surface S19 (not shown).

[0068] Table 1 shows the basic parameters of the optical imaging lens of Example 1, wherein the units of the radius of curvature, thickness and focal length are all millimeters (mm).

[0069]

[0070] Table 1

[0071] In this embodiment, the total effective focal length f of the optical imaging lens is 2.74 mm, half of the diagonal length of the effective pixel area on the imaging surface S19 is ImgH=2.40 mm, the maximum half field of view Semi-FOV of the optical imaging lens is 44.1°, and the aperture value Fno of the optical imaging lens is 2.65.

[0072] In Example 1, the object side surface and the image side surface of any lens among the first lens E1 to the fifth 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:

[0073]

[0074] 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 Table 2 gives the high-order coefficients A4, A6, A8, A9, A10, A11, A12, A13, A14, A15, A16, A17, A18, A19, A20, A21, A22, A23, A24, A25, A26, A27, A28, A29, A30, A31, A32, A33, A34, A35, A36, A37, A38, A39 10 , A 12 , A 14 , A 16 , A 18 and A 20 .

[0075] Face number A4 A6 A8 A10 A12 A14 A16 A18 A20 S1 1.8065E-01 -1.4662E-01 9.0896E-02 -1.7279E-02 -3.4361E-02 4.3180E-02 -2.6809E-02 1.0445E-02 -2.6521E-03 S2 2.1843E-01 -5.1008E-02 -2.9432E-01 9.8930E-01 -1.7838E+00 2.1330E+00 -1.7745E+00 1.0355E+00 -4.1731E-01 S6 3.0060E-02 -1.9436E-01 2.2486E+00 -1.4441E+01 5.9736E+01 -1.6539E+02 3.1294E+02 -4.0574E+02 3.5445E+02 S7 7.7728E-03 -7.8478E-02 9.6899E-01 -4.2961E+00 1.2564E+01 -2.5120E+01 3.4502E+01 -3.2476E+01 2.0574E+01 S8 1.9606E-01 -9.1765E-01 6.8116E+00 -3.1758E+01 9.8168E+01 -2.0534E+02 2.9562E+02 -2.9344E+02 1.9687E+02 S9 1.6665E-01 -1.7922E+00 1.4406E+01 -6.2798E+01 1.7301E+02 -3.2627E+02 4.3682E+02 -4.1681E+02 2.7645E+02 S10 -2.4534E-02 -1.3556E+00 1.3248E+01 -5.5461E+01 1.3574E+02 -2.2123E+02 2.5870E+02 -2.2601E+02 1.4712E+02 S11 -6.8295E-01 4.6156E+00 -2.3695E+01 8.9565E+01 -2.5421E+02 5.3133E+02 -7.9772E+02 8.4022E+02 -6.0237E+02 S12 -1.1963E-02 3.1948E+00 -1.9033E+01 6.9874E+01 -1.8285E+02 3.5222E+02 -4.9517E+02 4.9654E+02 -3.4343E+02 S13 1.4098E-01 7.0696E-02 -1.2147E+00 4.1803E+00 -8.8103E+00 1.3554E+01 -1.5811E+01 1.3626E+01 -8.2444E+00

[0076] Table 2

[0077] Figure 2A 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 2B The distortion curve of the optical imaging lens of Example 1 is shown, which represents the distortion magnitude values ​​corresponding to different image heights. Figure 2C The relative illumination curve of the optical imaging lens of Example 1 is shown, which indicates the relative illumination values ​​corresponding to different image heights. FIG. 2A to FIG. 2C It can be seen that the optical imaging lens provided in Example 1 can achieve good imaging quality.

[0078] Example 2

[0079] The following reference Figures 3 to 4C An optical imaging lens according to Embodiment 2 of the present application is described. Figure 3 is a schematic diagram showing the structure of an optical imaging lens according to Embodiment 2 of the present application.

[0080] like Figure 3 As shown, the optical imaging lens includes, in order from the object side to the image side along the optical axis: a first lens E1, a first prism E2, an aperture STO, a second lens E3, a third lens E4, a fourth lens E5, a fifth lens E6, a second prism E7, and a filter E8.

[0081] The first lens E1 has negative focal power, and its object side surface S1 is concave, and its image side surface S2 is concave. The incident surface S3, the reflection surface S4, and the exit surface S5 of the first prism E2 are all spherical surfaces, and the reflection surface S4 forms an angle of 45° with the optical axis, so that the light incident perpendicular to the incident surface S3 of the first prism E2 is deflected 90° by the reflection surface S4 and then exits the first prism E2 perpendicularly to the exit surface S5. The second lens E3 has positive focal power, and its object side surface S6 is convex, and the image side surface S7 is convex. The third lens E4 has negative focal power, and its object side surface S8 is convex, and the image side surface S9 is concave. The fourth lens E5 has positive focal power, and its object side surface S10 is concave, and the image side surface S11 is convex. The fifth lens E6 has negative focal power, and its object side surface S12 is convex, and the image side surface S13 is concave. The incident surface S14, the reflection surface S15 and the exit surface S16 of the second prism E7 are all spherical surfaces, and the reflection surface S15 forms an angle of 45° with the optical axis, so that the light incident perpendicular to the incident surface S14 of the second prism E7 is deflected 90° by the reflection surface S15 and then exits the second prism E7 perpendicular to the exit surface S16. The filter E8 has an object side surface S17 and an image side surface S18. The light from the object passes through each surface S1 to S18 in sequence and is finally imaged on the imaging surface S19 (not shown).

[0082] In this embodiment, the total effective focal length f of the optical imaging lens is 2.74 mm, half of the diagonal length of the effective pixel area on the imaging surface S19 is ImgH=2.40 mm, the maximum half field of view Semi-FOV of the optical imaging lens is 44.1°, and the aperture value Fno of the optical imaging lens is 2.65.

[0083] Table 3 shows the basic parameters of the optical imaging lens of Example 2, wherein the units of the radius of curvature, thickness and focal length are all millimeters (mm).

[0084]

[0085] Table 3

[0086] In Example 2, the object side surface and the image side surface of any one of the first lens E1 to the fifth lens E6 are aspherical surfaces. The following Table 4 lists the high-order coefficients A4, A6, A8, A9, A10, A11, A12, A13, A14, A15, A16, A17, A18, A19, A20, A21, A22, A23, A24, A25, A26, A27, A28, A29, A30, A31, A32, A33, A34, A35, A36, A37, A38, A39, A40, A41, A42, A43, A44, A45, A46, A47, A48, A49, A50, A51, A52, A53, A54, A55, A56, A57, A58, 10 , A 12 , A 14 , A 16 , A 18 and A 20 , wherein each aspheric surface shape can be defined by the formula (1) given in the above embodiment 1.

[0087] Face number A4 A6 A8 A10 A12 A14 A16 A18 A20 S1 1.8241E-01 -1.3638E-01 6.7667E-02 8.9226E-03 -5.1761E-02 4.9525E-02 -2.7372E-02 9.8657E-03 -2.3560E-03 S2 2.2127E-01 -6.7914E-02 -7.4345E-02 1.8776E-02 6.2129E-01 -1.6681E+00 2.2487E+00 -1.8567E+00 9.7813E-01 S6 2.5879E-02 -1.6526E-01 2.0065E+00 -1.3330E+01 5.6608E+01 -1.5977E+02 3.0638E+02 -4.0077E+02 3.5200E+02 S7 1.1458E-02 2.0157E-02 -8.6361E-02 5.2771E-01 -1.2771E+00 1.7263E+00 -1.4399E+00 7.7228E-01 -2.8988E-01 S8 1.0120E-01 -4.0105E-01 3.9741E+00 -2.3100E+01 8.4342E+01 -2.0026E+02 3.1860E+02 -3.4244E+02 2.4489E+02 S9 1.0023E-01 -1.6231E+00 1.9379E+01 -1.1016E+02 3.7820E+02 -8.5471E+02 1.3157E+03 -1.3885E+03 9.8807E+02 S10 -5.4466E-02 -1.8562E+00 2.5201E+01 -1.4419E+02 4.9050E+02 -1.1010E+03 1.6932E+03 -1.7961E+03 1.2922E+03 S11 -8.5228E-01 7.2545E+00 -4.0956E+01 1.5454E+02 -4.1073E+02 7.8431E+02 -1.0758E+03 1.0444E+03 -6.9692E+02 S12 -1.4315E-01 5.4335E+00 -3.5436E+01 1.3941E+02 -3.7492E+02 7.1852E+02 -9.8942E+02 9.6828E+02 -6.5477E+02 S13 1.5025E-01 1.3339E-02 -1.3622E+00 5.3872E+00 -1.1709E+01 1.6872E+01 -1.7243E+01 1.2807E+01 -6.8584E+00

[0088] Table 4

[0089] Figure 4A 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 4B The distortion curve of the optical imaging lens of Example 2 is shown, which represents the distortion magnitude values ​​corresponding to different image heights. Figure 4C The relative illumination curve of the optical imaging lens of Example 2 is shown, which indicates the relative illumination values ​​corresponding to different image heights. FIG. 4A to FIG. 4C 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 6C An optical imaging lens according to Embodiment 3 of the present application is described. Figure 5 is a schematic diagram showing the structure of an optical imaging lens according to Example 3 of the present application.

[0092] like Figure 5 As shown, the optical imaging lens includes, in order from the object side to the image side along the optical axis: a first lens E1, a first prism E2, an aperture STO, a second lens E3, a third lens E4, a fourth lens E5, a fifth lens E6, a second prism E7, and a filter E8.

[0093] The first lens E1 has negative focal power, and its object side surface S1 is concave, and the image side surface S2 is concave. The incident surface S3, the reflection surface S4 and the exit surface S5 of the first prism E2 are all spherical surfaces, and the reflection surface S4 forms an angle of 45° with the optical axis, so that the light incident perpendicular to the incident surface S3 of the first prism E2 is deflected 90° by the reflection surface S4 and then exits from the first prism E2 perpendicularly to the exit surface S5. The second lens E3 has positive focal power, and its object side surface S6 is convex, and the image side surface S7 is convex. The third lens E4 has positive focal power, and its object side surface S8 is convex, and the image side surface S9 is concave. The fourth lens E5 has positive focal power, and its object side surface S10 is concave, and the image side surface S11 is convex. The fifth lens E6 has negative focal power, and its object side surface S12 is convex, and the image side surface S13 is concave. The incident surface S14, the reflection surface S15 and the exit surface S16 of the second prism E7 are all spherical surfaces, and the reflection surface S15 forms an angle of 45° with the optical axis, so that the light incident perpendicular to the incident surface S14 of the second prism E7 is deflected 90° by the reflection surface S15 and then exits the second prism E7 perpendicular to the exit surface S16. The filter E8 has an object side surface S17 and an image side surface S18. The light from the object passes through each surface S1 to S18 in sequence and is finally imaged on the imaging surface S19 (not shown).

[0094] In this embodiment, the total effective focal length f of the optical imaging lens is 2.75 mm, half of the diagonal length of the effective pixel area on the imaging surface S19 is ImgH=2.40 mm, the maximum half field of view Semi-FOV of the optical imaging lens is 44.6°, and the aperture value Fno of the optical imaging lens is 2.60.

[0095] Table 5 shows the basic parameters of the optical imaging lens of Example 3, wherein the units of the radius of curvature, thickness and focal length are all millimeters (mm).

[0096]

[0097]

[0098] Table 5

[0099] In Example 3, the object side surface and the image side surface of any one of the first lens E1 to the fifth lens E6 are aspherical surfaces. The following Table 6 lists the high-order coefficients A4, A6, A8, A9, A10, A11, A12, A13, A14, A15, A16, A17, A18, A19, A20, A21, A22, A23, A24, A25, A26, A27, A28, A29, A30, A31, A32, A33, A34, A35, A36, A37, A38, A39, A40, A41, A42, A43, A44, A45, A46, A47, A48, A49, A50, A51, A52, A53, A54, A55, A56, A57, A58, 10 , A 12 , A 14 , A 16 , A 18 and A 20 , wherein each aspheric surface shape can be defined by the formula (1) given in the above embodiment 1.

[0100] Face number A4 A6 A8 A10 A12 A14 A16 A18 A20 S1 1.8414E-01 -1.3365E-01 5.4048E-02 3.1475E-02 -7.4351E-02 6.4593E-02 -3.4264E-02 1.2034E-02 -2.8169E-03 S2 2.1974E-01 -1.7385E-02 -3.3658E-01 8.3663E-01 -1.0799E+00 7.6840E-01 -1.8619E-01 -1.6285E-01 1.7468E-01 S6 2.7357E-02 -2.0706E-01 2.3052E+00 -1.4327E+01 5.6956E+01 -1.5062E+02 2.7087E+02 -3.3256E+02 2.7436E+02 S7 2.3269E-02 -3.2665E-02 3.0415E-01 -1.7031E+00 6.0940E+00 -1.3479E+01 1.9222E+01 -1.8097E+01 1.1201E+01 S8 1.0833E-01 -6.7890E-01 6.9174E+00 -3.7948E+01 1.2807E+02 -2.8211E+02 4.1892E+02 -4.2269E+02 2.8531E+02 S9 1.2147E-01 -2.3977E+00 2.5629E+01 -1.3383E+02 4.2348E+02 -8.8221E+02 1.2526E+03 -1.2209E+03 8.0404E+02 S10 -1.1455E-03 -2.7110E+00 3.0879E+01 -1.6286E+02 5.1717E+02 -1.0859E+03 1.5640E+03 -1.5573E+03 1.0548E+03 S11 -8.5655E-01 7.1974E+00 -3.9649E+01 1.4498E+02 -3.7147E+02 6.8225E+02 -9.0048E+02 8.4376E+02 -5.4584E+02 S12 -1.4402E-01 5.5272E+00 -3.5611E+01 1.3681E+02 -3.5706E+02 6.6242E+02 -8.8434E+02 8.4289E+02 -5.5852E+02 S13 1.5788E-01 5.6600E-02 -1.9083E+00 7.6551E+00 -1.7154E+01 2.5120E+01 -2.5214E+01 1.7549E+01 -8.3724E+00

[0101] Table 6

[0102] Fig. 6A 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 6B The distortion curve of the optical imaging lens of Example 3 is shown, which represents the distortion magnitude values ​​corresponding to different image heights. Figure 6C The relative illumination curve of the optical imaging lens of Example 3 is shown, which indicates the relative illumination values ​​corresponding to different image heights. FIG. 6A to FIG. 6C It can be seen that the optical imaging lens provided in Example 3 can achieve good imaging quality.

[0103] Example 4

[0104] The following reference Figures 7 to 8C An optical imaging lens according to Embodiment 4 of the present application is described. Figure 7 is a schematic diagram showing the structure of an optical imaging lens according to Example 4 of the present application.

[0105] like Figure 7As shown, the optical imaging lens includes, in order from the object side to the image side along the optical axis: a first lens E1, a first prism E2, an aperture STO, a second lens E3, a third lens E4, a fourth lens E5, a fifth lens E6, a second prism E7, and a filter E8.

[0106] The first lens E1 has negative focal power, and its object side surface S1 is concave, and the image side surface S2 is concave. The incident surface S3, the reflection surface S4 and the exit surface S5 of the first prism E2 are all spherical surfaces, and the reflection surface S4 forms an angle of 45° with the optical axis, so that the light incident perpendicular to the incident surface S3 of the first prism E2 is deflected 90° by the reflection surface S4 and then exits from the first prism E2 perpendicularly to the exit surface S5. The second lens E3 has positive focal power, and its object side surface S6 is convex, and the image side surface S7 is convex. The third lens E4 has positive focal power, and its object side surface S8 is convex, and the image side surface S9 is concave. The fourth lens E5 has positive focal power, and its object side surface S10 is concave, and the image side surface S11 is convex. The fifth lens E6 has negative focal power, and its object side surface S12 is concave, and the image side surface S13 is concave. The incident surface S14, the reflection surface S15 and the exit surface S16 of the second prism E7 are all spherical surfaces, and the reflection surface S15 forms an angle of 45° with the optical axis, so that the light incident perpendicular to the incident surface S14 of the second prism E7 is deflected 90° by the reflection surface S15 and then exits the second prism E7 perpendicular to the exit surface S16. The filter E8 has an object side surface S17 and an image side surface S18. The light from the object passes through each surface S1 to S18 in sequence and is finally imaged on the imaging surface S19 (not shown).

[0107] In this embodiment, the total effective focal length f of the optical imaging lens is 2.72 mm, half of the diagonal length of the effective pixel area on the imaging surface S19 is ImgH=2.40 mm, the maximum half field of view Semi-FOV of the optical imaging lens is 45.6°, and the aperture value Fno of the optical imaging lens is 2.55.

[0108] Table 7 shows the basic parameters of the optical imaging lens of Example 4, wherein the units of the radius of curvature, thickness and focal length are all millimeters (mm).

[0109]

[0110] Table 7

[0111] In Example 4, the object side surface and the image side surface of any one of the first lens E1 to the fifth lens E6 are aspherical surfaces. The following Table 8 lists the high-order coefficients A4, A6, A8, A9, A10, A11, A12, A13, A14, A15, A16, A17, A18, A19, A20, A21, A22, A23, A24, A25, A26, A27, A28, A29, A30, A31, A32, A33, A34, A35, A36, A37, A38, A39, A40, A41, A42, A43, A44, A45, A46, A47, A48, A49, A50, A51, A52, A53, A54, A55, A56, A57, A58, 10 , A 12 , A 14 , A 16 , A 18 and A 20, wherein each aspheric surface shape can be defined by the formula (1) given in the above embodiment 1.

[0112] Face number A4 A6 A8 A10 A12 A14 A16 A18 A20 S1 1.9431E-01 -1.5682E-01 8.8993E-02 -9.3520E-03 -3.8393E-02 4.1092E-02 -2.3061E-02 8.2228E-03 -1.9210E-03 S2 2.3054E-01 -1.4444E-02 -4.4667E-01 1.2650E+00 -2.0172E+00 2.1069E+00 -1.4960E+00 7.2545E-01 -2.3681E-01 S6 2.4424E-02 -2.0823E-01 2.1382E+00 -1.2249E+01 4.5108E+01 -1.1103E+02 1.8654E+02 -2.1455E+02 1.6612E+02 S7 4.9858E-03 5.0511E-02 8.0895E-01 -6.4464E+00 2.2150E+01 -4.4729E+01 5.8437E+01 -5.1009E+01 2.9637E+01 S8 5.4841E-02 -5.7778E-01 7.9145E+00 -4.1289E+01 1.2323E+02 -2.3742E+02 3.1122E+02 -2.8203E+02 1.7437E+02 S9 5.9369E-02 -1.2535E+00 1.4446E+01 -6.8789E+01 1.8689E+02 -3.2428E+02 3.7842E+02 -3.0288E+02 1.6508E+02 S10 1.0453E-02 -1.2809E+00 1.3802E+01 -6.5577E+01 1.7925E+02 -3.1416E+02 3.7143E+02 -3.0243E+02 1.6879E+02 S11 -6.5597E-01 3.9500E+00 -1.8270E+01 5.8934E+01 -1.3738E+02 2.3651E+02 -3.0145E+02 2.8012E+02 -1.8356E+02 S12 1.5936E-01 1.3824E+00 -9.1590E+00 2.9231E+01 -5.5585E+01 6.3234E+01 -3.5456E+01 -5.3357E+00 2.3574E+01 S13 3.2505E-01 -1.2348E+00 3.8748E+00 -9.7277E+00 1.9073E+01 -2.8495E+01 3.1751E+01 -2.5705E+01 1.4556E+01

[0113] Table 8

[0114] Fig. 8A 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 8B The distortion curve of the optical imaging lens of Example 4 is shown, which represents the distortion magnitude values ​​corresponding to different image heights. Figure 8C The relative illumination curve of the optical imaging lens of Example 4 is shown, which indicates the relative illumination values ​​corresponding to different image heights. FIG. 8A to FIG. 8C It can be seen that the optical imaging lens provided in Example 4 can achieve good imaging quality.

[0115] Example 5

[0116] The following reference Figures 9 to 10C An optical imaging lens according to Embodiment 5 of the present application is described. Fig. 9 is a schematic diagram showing the structure of an optical imaging lens according to Example 5 of the present application.

[0117] like Fig. 9 As shown, the optical imaging lens includes, in order from the object side to the image side along the optical axis: a first lens E1, a first prism E2, an aperture STO, a second lens E3, a third lens E4, a fourth lens E5, a fifth lens E6, a second prism E7, and a filter E8.

[0118] The first lens E1 has negative focal power, and its object side surface S1 is concave, and the image side surface S2 is concave. The incident surface S3, the reflection surface S4 and the exit surface S5 of the first prism E2 are all spherical surfaces, and the reflection surface S4 forms an angle of 45° with the optical axis, so that the light incident perpendicular to the incident surface S3 of the first prism E2 is deflected 90° by the reflection surface S4 and then exits from the first prism E2 perpendicularly to the exit surface S5. The second lens E3 has positive focal power, and its object side surface S6 is convex, and the image side surface S7 is convex. The third lens E4 has positive focal power, and its object side surface S8 is convex, and the image side surface S9 is convex. The fourth lens E5 has positive focal power, and its object side surface S10 is concave, and the image side surface S11 is convex. The fifth lens E6 has negative focal power, and its object side surface S12 is concave, and the image side surface S13 is concave. The incident surface S14, the reflection surface S15 and the exit surface S16 of the second prism E7 are all spherical surfaces, and the reflection surface S15 forms an angle of 45° with the optical axis, so that the light incident perpendicular to the incident surface S14 of the second prism E7 is deflected 90° by the reflection surface S15 and then exits the second prism E7 perpendicular to the exit surface S5. The filter E8 has an object side surface S17 and an image side surface S18. The light from the object passes through each surface S1 to S18 in sequence and is finally imaged on the imaging surface S19 (not shown).

[0119] In this embodiment, the total effective focal length f of the optical imaging lens is 2.60 mm, half of the diagonal length of the effective pixel area on the imaging surface S19 is ImgH=2.40 mm, the maximum half field of view Semi-FOV of the optical imaging lens is 47.6°, and the aperture value Fno of the optical imaging lens is 2.40.

[0120] Table 9 shows the basic parameters of the optical imaging lens of Example 5, wherein the units of the radius of curvature, thickness and focal length are all millimeters (mm).

[0121]

[0122]

[0123] Table 9

[0124] In Example 5, the object side surface and the image side surface of any one of the first lens E1 to the fifth lens E6 are aspherical surfaces. The following Table 10 lists the high-order coefficients A4, A6, A8, A9, A10, A11, A12, A13, A14, A15, A16, A17, A18, A19, A20, A21, A22, A23, A24, A25, A26, A27, A28, A29, A30, A31, A32, A33, A34, A35, A36, A37, A38, A39, A40, A41, A42, A43, A44, A45, A46, A47, A48, A49, A50, A51, A52, A53, A54, A55, A56, A57, A58 10 , A 12 , A 14 , A 16 , A 18 and A 20 , wherein each aspheric surface shape can be defined by the formula (1) given in the above embodiment 1.

[0125] Face number A4 A6 A8 A10 A12 A14 A16 A18 A20 S1 2.0578E-01 -1.7456E-01 1.1361E-01 -3.9774E-02 -9.3510E-03 2.0959E-02 -1.3164E-02 4.8259E-03 -1.1265E-03 S2 2.4814E-01 -7.2595E-02 -1.6763E-01 3.3899E-01 -3.1806E-02 -7.3614E-01 1.2853E+00 -1.1432E+00 6.1249E-01 S6 2.1515E-02 -1.5464E-01 1.4467E+00 -7.5314E+00 2.5337E+01 -5.7080E+01 8.7899E+01 -9.2721E+01 6.5858E+01 S7 1.0823E-01 -6.6115E-01 2.6779E+00 -7.9955E+00 1.7925E+01 -2.9195E+01 3.4014E+01 -2.7921E+01 1.5714E+01 S8 1.3599E-01 -5.6529E-01 3.8799E+00 -1.7807E+01 5.4781E+01 -1.1396E+02 1.6242E+02 -1.5837E+02 1.0356E+02 S9 -1.0829E-02 2.5451E-01 7.5610E-01 -9.1583E+00 3.7006E+01 -8.7593E+01 1.3455E+02 -1.3769E+02 9.3124E+01 S10 -3.3291E-02 2.1167E-01 2.3696E-01 -6.2263E+00 2.8673E+01 -7.3835E+01 1.2129E+02 -1.3153E+02 9.3820E+01 S11 -2.7551E-01 9.0913E-02 2.0985E+00 -1.0625E+01 3.0803E+01 -6.2288E+01 9.0840E+01 -9.4639E+01 6.8341E+01 S12 5.0826E-01 -2.5051E+00 1.0421E+01 -3.0424E+01 6.3333E+01 -9.5379E+01 1.0490E+02 -8.4479E+01 4.9520E+01 S13 3.8397E-01 -1.9413E+00 6.6906E+00 -1.4953E+01 1.9486E+01 -6.9944E+00 -2.3103E+01 4.7657E+01 -4.5417E+01

[0126] Table 10

[0127] Fig. 10A 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. 10B The distortion curve of the optical imaging lens of Example 5 is shown, which represents the distortion magnitude values ​​corresponding to different image heights. Fig. 10C The relative illumination curve of the optical imaging lens of Example 5 is shown, which indicates the relative illumination values ​​corresponding to different image heights. FIG. 10A to FIG. 10C It can be seen that the optical imaging lens provided in Example 5 can achieve good imaging quality.

[0128] Example 6

[0129] The following reference Figures 11 to 12C An optical imaging lens according to Example 6 of the present application is described. Fig.11 is a schematic diagram showing the structure of an optical imaging lens according to Example 6 of the present application.

[0130] like Fig.11 As shown, the optical imaging lens includes, in order from the object side to the image side along the optical axis: a first lens E1, a first prism E2, an aperture STO, a second lens E3, a third lens E4, a fourth lens E5, a fifth lens E6, a second prism E7, and a filter E8.

[0131] The first lens E1 has negative focal power, and its object side surface S1 is concave, and the image side surface S2 is concave. The incident surface S3, the reflection surface S4 and the exit surface S5 of the first prism E2 are all spherical surfaces, and the reflection surface S4 forms an angle of 45° with the optical axis, so that the light incident perpendicular to the incident surface S3 of the first prism E2 is deflected 90° by the reflection surface S4 and then exits from the first prism E2 perpendicularly to the exit surface S5. The second lens E3 has positive focal power, and its object side surface S6 is convex, and the image side surface S7 is convex. The third lens E4 has positive focal power, and its object side surface S8 is convex, and the image side surface S9 is convex. The fourth lens E5 has positive focal power, and its object side surface S10 is concave, and the image side surface S11 is convex. The fifth lens E6 has negative focal power, and its object side surface S12 is convex, and the image side surface S13 is concave. The incident surface S14, the reflection surface S15 and the exit surface S16 of the second prism E7 are all spherical surfaces, and the reflection surface S15 forms an angle of 45° with the optical axis, so that the light incident perpendicular to the incident surface S14 of the second prism E7 is deflected 90° by the reflection surface S15 and then exits the second prism E7 perpendicular to the exit surface S5. The filter E8 has an object side surface S17 and an image side surface S18. The light from the object passes through each surface S1 to S18 in sequence and is finally imaged on the imaging surface S19 (not shown).

[0132] In this embodiment, the total effective focal length f of the optical imaging lens is 2.42 mm, half of the diagonal length of the effective pixel area on the imaging surface S19 is ImgH=2.40 mm, the maximum half field of view Semi-FOV of the optical imaging lens is 51.1°, and the aperture value Fno of the optical imaging lens is 2.80.

[0133] Table 11 shows the basic parameters of the optical imaging lens of Example 6, wherein the units of the radius of curvature, thickness and focal length are all millimeters (mm).

[0134]

[0135] Table 11

[0136] In Example 6, the object side surface and the image side surface of any one of the first lens E1 to the fifth lens E6 are aspherical surfaces. The following Table 12 lists the high-order coefficients A4, A6, A8, A9, A10, A11, A12, A13, A14, A15, A16, A17, A18, A19, A20, A21, A22, A23, A24, A25, A26, A27, A28, A29, A30, A31, A32, A33, A34, A35, A36, A37, A38, A39, A40, A41, A42, A43, A44, A45, A46, A47, A48, A49, A50, A51, A52, A53, A54, A55, A56, A57, A58 10 , A 12 , A 14 , A 16 , A 18 and A 20 , wherein each aspheric surface shape can be defined by the formula (1) given in the above embodiment 1.

[0137] Face number A4 A6 A8 A10 A12 A14 A16 A18 A20 S1 2.0530E-01 -1.5975E-01 7.3069E-02 1.5708E-02 -5.6699E-02 4.7944E-02 -2.3696E-02 7.6466E-03 -1.6351E-03 S2 2.5101E-01 -7.9466E-02 5.1693E-02 -7.6656E-01 2.8075E+00 -5.2271E+00 5.9567E+00 -4.4067E+00 2.1313E+00 S6 1.9321E-02 -8.0612E-02 1.4388E+00 -1.2650E+01 7.0185E+01 -2.5705E+02 6.3754E+02 -1.0765E+03 1.2187E+03 S7 1.2633E-01 -1.2396E+00 8.0099E+00 -3.5967E+01 1.1356E+02 -2.5377E+02 4.0525E+02 -4.6144E+02 3.6654E+02 S8 1.8134E-01 -1.2270E+00 9.2164E+00 -4.5582E+01 1.5441E+02 -3.7422E+02 6.6824E+02 -8.7619E+02 8.1399E+02 S9 2.3532E-02 -3.6418E-03 1.6910E+00 -1.0173E+01 3.1467E+01 -6.5800E+01 1.1314E+02 -1.6785E+02 1.8949E+02 S10 -4.2403E-02 -1.9504E-02 3.4097E+00 -2.6182E+01 1.0864E+02 -3.0136E+02 5.9556E+02 -8.4260E+02 8.2739E+02 S11 -3.8667E-01 1.3650E+00 -1.0044E+00 -2.9666E+01 1.9795E+02 -6.7617E+02 1.4709E+03 -2.1471E+03 2.0988E+03 S12 4.3112E-01 -1.6217E+00 1.1820E+01 -8.5905E+01 4.0998E+02 -1.2782E+03 2.7020E+03 -3.9282E+03 3.8786E+03 S13 3.9811E-01 -2.1252E+00 9.8567E+00 -4.1052E+01 1.3730E+02 -3.3952E+02 6.0324E+02 -7.5877E+02 6.5940E+02

[0138] Table 12

[0139] Fig. 12A 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. 12B The distortion curve of the optical imaging lens of Example 6 is shown, which represents the distortion magnitude values ​​corresponding to different image heights. Fig. 12C The relative illumination curve of the optical imaging lens of Example 6 is shown. FIG. 12A to FIG. 12C It can be seen that the optical imaging lens provided in Example 6 can achieve good imaging quality.

[0140] In summary, Examples 1 to 6 respectively satisfy the relationships shown in Table 13.

[0141] Conditional / Example 1 2 3 4 5 6 <![CDATA[f×tan 2 (FOV / 2)(mm)]]> 2.58 2.58 2.67 2.84 3.12 3.72 f34 / f23 2.03 1.58 1.38 1.11 1.13 1.19 f1 / f5 0.83 1.07 1.29 1.65 1.58 1.42 f345 / f5 -2.53 -3.41 -4.38 -6.40 -7.78 -6.00 (R1-R2) / (R1+R2) 3.70 3.77 3.73 3.57 3.41 2.97 f345 / R10 7.34 7.97 8.56 8.96 11.46 9.02 SAG12 / SAG11 4.61 4.22 4.56 5.04 4.81 4.95 CT4 / T45 24.60 40.96 41.09 47.58 51.23 45.74 SAG22 / SAG31 6.49 7.59 6.99 8.49 4.14 3.39 (DT21+DT22) / (DT22-DT21) 12.93 12.89 11.91 12.47 16.14 16.21 FOV(°) 88.2 88.3 89.3 91.3 95.3 102.2

[0142] Table 13

[0143] The present application also provides an imaging device, which is provided with an electronic photosensitive element for imaging, and the electronic photosensitive element can be a charge coupled device (CCD) or a complementary metal oxide semiconductor (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.

[0144] 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 (but not limited to) technical features with similar functions disclosed in the present application.

Claims

1. An optical imaging lens, It is characterized in that Along the optical axis from the object side to the image side, they include: The first lens has a negative optical power, and its object side surface is concave and its image side surface is concave; A first prism, wherein the first prism comprises an incident surface, a reflecting surface and an exiting surface, wherein the angle between the reflecting surface of the first prism and the optical axis is 45°; Aperture; The second lens has positive power, and its object-side surface is convex and its image-side surface is convex; a third lens having optical power and having a convex object-side surface; a fourth lens element having positive refractive power and a convex image-side surface; a fifth lens element having negative refractive power, the image side surface of which is concave; and a second prism, wherein the second prism comprises an incident surface, a reflecting surface and an emitting surface, wherein the angle between the reflecting surface of the second prism and the optical axis is 45°; Wherein, the number of lenses having optical power in the optical imaging lens is five; The total effective focal length f of the optical imaging lens and the maximum field of view FOV of the optical imaging lens satisfy: 2.58mm≤f×tan 2 (FOV / 2)≤3.72 mm; A center thickness CT4 of the fourth lens on the optical axis and an air interval T45 between the fourth lens and the fifth lens on the optical axis satisfy: 24.60≤CT4 / T45≤51.

23.

2. The optical imaging lens according to claim 1, It is characterized in that The combined focal length f23 of the second lens and the third lens and the combined focal length f34 of the third lens and the fourth lens satisfy: 1.11≤f34 / f23≤2.

03.

3. The optical imaging lens according to claim 1, It is characterized in that The effective focal length f1 of the first lens and the effective focal length f5 of the fifth lens satisfy: 0.83≤f1 / f5≤1.

65.

4. The optical imaging lens according to claim 1, It is characterized in that The combined focal length f345 of the third lens, the fourth lens and the fifth lens and the effective focal length f5 of the fifth lens satisfy: -7.78≤f345 / f5≤-2.

53.

5. The optical imaging lens according to claim 1, It is characterized in that The curvature radius R1 of the object side surface of the first lens and the curvature radius R2 of the image side surface of the first lens satisfy: 2.97≤(R1-R2) / (R1+R2)≤3.

77.

6. The optical imaging lens according to claim 1, It is characterized in that The combined focal length f345 of the third lens, the fourth lens and the fifth lens and the curvature radius R10 of the image side surface of the fifth lens satisfy: 7.34≤f345 / R10≤11.

46.

7. The optical imaging lens according to claim 1, It is characterized in that 4.22≤SAG12 / SAG11≤5.04, Among them, SAG11 is the on-axis distance from the intersection of the object side surface of the first lens and the optical axis to the vertex of the effective radius of the object side surface of the first lens, and SAG12 is the on-axis distance from the intersection of the image side surface of the first lens and the optical axis to the vertex of the effective radius of the image side surface of the first lens.

8. The optical imaging lens according to claim 1, It is characterized in that 3.39≤SAG22 / SAG31≤8.49, Among them, SAG22 is the on-axis distance from the intersection of the image side surface of the second lens and the optical axis to the vertex of the effective radius of the image side surface of the second lens, and SAG31 is the on-axis distance from the intersection of the object side surface of the third lens and the optical axis to the vertex of the effective radius of the object side surface of the third lens.

9. The optical imaging lens according to claim 1, It is characterized in that The maximum effective radius DT21 of the object side surface of the second lens and the maximum effective radius DT22 of the image side surface of the second lens satisfy: 11.91≤(DT21+DT22) / (DT22-DT21)≤16.

21.

10. The optical imaging lens according to claim 1, It is characterized in that The maximum field of view FOV of the optical imaging lens satisfies: 88.2°≤FOV≤102.2°.