CN113625434A - Optical imaging lens - Google Patents

Optical imaging lens Download PDF

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Publication number
CN113625434A
CN113625434A CN202111114079.7A CN202111114079A CN113625434A CN 113625434 A CN113625434 A CN 113625434A CN 202111114079 A CN202111114079 A CN 202111114079A CN 113625434 A CN113625434 A CN 113625434A
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China
Prior art keywords
lens
optical imaging
imaging lens
image
optical
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CN202111114079.7A
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CN113625434B (en
Inventor
张爽
张晓彬
闻人建科
戴付建
赵烈烽
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Zhejiang Sunny Optics Co Ltd
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Zhejiang Sunny Optics Co Ltd
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • G02B13/001Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
    • G02B13/0015Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design
    • G02B13/002Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface
    • G02B13/0045Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface having five or more lenses
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • G02B13/18Optical objectives specially designed for the purposes specified below with lenses having one or more non-spherical faces, e.g. for reducing geometrical aberration
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03BAPPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
    • G03B30/00Camera modules comprising integrated lens units and imaging units, specially adapted for being embedded in other devices, e.g. mobile phones or vehicles

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Lenses (AREA)

Abstract

The invention provides an optical imaging lens. The imaging lens sequentially comprises from the object side to the image side of the imaging lens: the first lens has positive focal power, and the object side surface of the first lens is a convex surface; the second lens has negative focal power, and the image side surface of the second lens is a concave surface; the third lens has negative focal power, the object side surface of the third lens is a convex surface, and the image side surface of the third lens is a concave surface; a fourth lens having a positive refractive power; a fifth lens having optical power; the sixth lens has negative focal power, the object side surface of the sixth lens is a concave surface, and the image side surface of the sixth lens is a concave surface; wherein, satisfy between the effective focal length f of optical imaging lens and the entrance pupil diameter EPD of optical imaging lens: f/EPD < 1.9; the maximum field angle FOV of the optical imaging lens satisfies the following conditions: 0.5< tan (fov) < 1.5. The invention solves the problem of poor imaging quality of the optical imaging lens in the prior art.

Description

Optical imaging lens
Technical Field
The invention relates to the technical field of optical imaging equipment, in particular to an optical imaging lens.
Background
With the development of mobile phone photography technology, mobile phone photography products are ubiquitous; the vast mobile phone photography enthusiasts can shoot shared pictures and video works through mobile phones every day to share in the social circle of the enthusiasts; good shooting works can be widely spread and shared in social circles; whether pictures with rich layering can be shot or not becomes one of the important reference standards for vast mobile phone users to pay attention to the mobile phones; therefore, in the process of designing the mobile phone, all large mobile phone manufacturers perform key planning and design on the mobile phone shooting function. The existing optical imaging lens has poor imaging quality at present, and the quality of a shot picture is low.
That is to say, the optical imaging lens in the prior art has the problem of poor imaging quality.
Disclosure of Invention
The invention mainly aims to provide an optical imaging lens to solve the problem of poor imaging quality of the optical imaging lens in the prior art.
In order to achieve the above object, the present invention provides an optical imaging lens, comprising in order from an object side to an image side of the optical imaging lens: the first lens has positive focal power, and the object side surface of the first lens is a convex surface; the second lens has negative focal power, and the image side surface of the second lens is a concave surface; the third lens has negative focal power, the object side surface of the third lens is a convex surface, and the image side surface of the third lens is a concave surface; a fourth lens having a positive refractive power; a fifth lens having optical power; the sixth lens has negative focal power, the object side surface of the sixth lens is a concave surface, and the image side surface of the sixth lens is a concave surface; wherein, satisfy between the effective focal length f of optical imaging lens and the entrance pupil diameter EPD of optical imaging lens: f/EPD < 1.9; the maximum field angle FOV of the optical imaging lens satisfies the following conditions: 0.5< tan (fov) < 1.5.
Further, the effective focal length f2 of the second lens and the effective focal length f3 of the third lens satisfy: 0< f2/f3< 1.5.
Further, the effective focal length f of the optical imaging lens and the effective focal length f1 of the first lens satisfy: 1.5< f/f1< 2.5.
Further, the radius of curvature R4 of the image-side surface of the second lens and the radius of curvature R1 of the object-side surface of the first lens satisfy: 1.3< R4/R1< 3.3.
Further, a radius of curvature R6 of the image-side surface of the third lens and a radius of curvature R5 of the object-side surface of the third lens satisfy: 1.1< R5/R6< 1.6.
Further, the curvature radius R12 of the image side surface of the sixth lens, the curvature radius R11 of the object side surface of the sixth lens and the effective focal length f of the optical imaging lens satisfy: 1.7< (R12-R11)/f < 2.7.
Further, the effective half aperture DT11 of the object side surface of the first lens, the effective half aperture DT12 of the image side surface of the first lens and the effective half aperture DT62 of the image side surface of the sixth lens satisfy: 1.3< (DT11+ DT12)/DT62< 1.8.
Further, the combined focal length f12 of the first lens and the second lens, the combined focal length f56 of the fifth lens and the sixth lens, and the effective focal length f of the optical imaging lens satisfy: 1.4< (f12-f56)/f < 2.5.
Further, an air interval T34 between the third lens and the fourth lens on the optical axis of the optical imaging lens, an air interval T45 between the fourth lens and the fifth lens on the optical axis, and an air interval T56 between the fifth lens and the sixth lens on the optical axis satisfy: 0.5< (T34+ T45)/T56< 1.6.
Further, an on-axis distance SAG21 between an intersection point of an object-side surface of the second lens and an optical axis of the optical imaging lens to an effective radius vertex of the object-side surface of the second lens, an on-axis distance SAG22 between an intersection point of an image-side surface of the second lens and the optical axis to an effective radius vertex of the image-side surface of the second lens, an on-axis distance SAG51 between an intersection point of an object-side surface of the fifth lens and the optical axis to an effective radius vertex of an object-side surface of the fifth lens, and an on-axis distance SAG52 between an intersection point of an image-side surface of the fifth lens and the optical axis to an effective radius vertex of an image-side surface of the fifth lens satisfy: -1.2< (SAG21+ SAG22)/(SAG51+ SAG52) < -0.4.
Further, an on-axis distance SAG61 from an intersection point of an object-side surface of the sixth lens and the optical axis of the optical imaging lens to an effective radius vertex of the object-side surface of the sixth lens, and an on-axis distance SAG62 from an intersection point of an image-side surface of the sixth lens and the optical axis to an effective radius vertex of the image-side surface of the sixth lens satisfy: 0.8< SAG62/SAG61< 1.5.
Further, the edge thickness ET2 of the second lens, the edge thickness ET3 of the third lens, the center thickness CT2 of the second lens and the center thickness CT3 of the third lens satisfy: 1.1< (ET2+ ET3)/(CT2+ CT3) < 1.9.
Further, the edge thickness ET5 of the fifth lens and the center thickness CT5 of the fifth lens satisfy: 1.1< ET5/CT5< 2.3.
With the technical solution of the present invention, the method sequentially includes, from an object side of the optical imaging lens to an image side of the optical imaging lens: the lens comprises a first lens, a second lens, a third lens, a fourth lens, a fifth lens and a sixth lens, wherein the first lens has positive focal power, and the object side surface of the first lens is a convex surface; the second lens has negative focal power, and the image side surface of the second lens is a concave surface; the third lens has negative focal power, the object side surface of the third lens is a convex surface, and the image side surface of the third lens is a concave surface; the fourth lens has positive focal power; the fifth lens has focal power; the sixth lens has negative focal power, the object side surface of the sixth lens is a concave surface, and the image side surface of the sixth lens is a concave surface; wherein, satisfy between the effective focal length f of optical imaging lens and the entrance pupil diameter EPD of optical imaging lens: f/EPD < 1.9; the maximum field angle FOV of the optical imaging lens satisfies the following conditions: 0.5< tan (fov) < 1.5.
The first lens with positive focal power and the convex object side surface and the second lens with negative focal power and the concave image side surface are combined, so that the aperture of the optical imaging lens can be enlarged, and meanwhile, the spherical aberration is reduced under the condition of a large aperture; and the lens is matched with a third lens with negative focal power, so that light rays can be transmitted smoothly, and coma, astigmatism and distortion can be reduced. The fourth lens with positive focal power is mainly used for balancing and distributing focal power, and is beneficial to reducing the aberration of the optical imaging lens; the sixth lens with the concave object side and the concave image side and the negative focal power can synchronously balance the distortion of the optical imaging lens while reducing the on-axis chromatic aberration, the coma aberration and the astigmatism. By limiting the f/EPD within a reasonable range, the aperture of the optical imaging lens can be increased, and the light flux entering the optical imaging lens is increased. The tan (FOV) is limited within a reasonable range, mainly in order to increase the focal length of the system, the magnification of the object image is changed by increasing the focal length, and further the image compression is realized, so that the shot meeting the condition range is more layered and stereoscopic in close-up shooting of the person.
Drawings
The accompanying drawings, which are incorporated in and constitute a part of this application, illustrate embodiments of the invention and, together with the description, serve to explain the invention and not to limit the invention. In the drawings:
fig. 1 is a schematic structural diagram of an optical imaging lens according to a first embodiment of the present invention;
fig. 2 to 5 respectively show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a magnification chromatic aberration curve of the optical imaging lens in fig. 1;
fig. 6 is a schematic structural diagram of an optical imaging lens according to a second embodiment of the present invention;
fig. 7 to 10 respectively show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a magnification chromatic aberration curve of the optical imaging lens in fig. 6;
fig. 11 is a schematic structural diagram showing an optical imaging lens according to a third embodiment of the present invention;
fig. 12 to 15 show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a chromatic aberration of magnification curve, respectively, of the optical imaging lens in fig. 11;
fig. 16 is a schematic structural diagram showing an optical imaging lens according to a fourth embodiment of the present invention;
fig. 17 to 20 show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a chromatic aberration of magnification curve, respectively, of the optical imaging lens in fig. 16;
fig. 21 is a schematic structural view showing an optical imaging lens according to embodiment five of the present invention;
fig. 22 to 25 show an on-axis chromatic aberration curve, an astigmatic curve, a distortion curve, and a chromatic aberration of magnification curve, respectively, of the optical imaging lens in fig. 21;
fig. 26 is a schematic structural view showing an optical imaging lens according to a sixth embodiment of the present invention;
fig. 27 to 30 show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a chromatic aberration of magnification curve, respectively, of the optical imaging lens in fig. 26.
Wherein the figures include the following reference numerals:
STO, stop; e1, first lens; s1, the object side surface of the first lens; s2, an image side surface of the first lens; e2, second lens; s3, the object side surface of the second lens; s4, an image side surface of the second lens; e3, third lens; s5, the object side surface of the third lens; s6, an image side surface of the third lens; e4, fourth lens; s7, the object side surface of the fourth lens; s8, an image side surface of the fourth lens element; e5, fifth lens; s9, the object side surface of the fifth lens; s10, an image side surface of the fifth lens element; e6, sixth lens; s11, the object-side surface of the sixth lens element; s12, an image side surface of the sixth lens element; e7, a filter plate; s13, the object side surface of the filter plate; s14, the image side surface of the filter plate; and S15, imaging surface.
Detailed Description
It should be noted that the embodiments and features of the embodiments in the present application may be combined with each other without conflict. The present invention will be described in detail below with reference to the embodiments with reference to the attached drawings.
It is noted that, unless otherwise indicated, all technical and scientific terms used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this application belongs.
In the present invention, unless specified to the contrary, use of the terms of orientation such as "upper, lower, top, bottom" or the like, generally refer to the orientation as shown in the drawings, or to the component itself in a vertical, perpendicular, or gravitational orientation; likewise, for ease of understanding and description, "inner and outer" refer to the inner and outer relative to the profile of the components themselves, but the above directional words are not intended to limit the invention.
It should be noted that in this specification, the expressions first, second, third, etc. are used only to distinguish one feature from another, and do not represent any limitation on the features. Thus, the first lens discussed below may also be referred to as the second lens or the third lens without departing from the teachings of the present application.
In the drawings, the thickness, size, and shape of the lens have been slightly exaggerated for convenience of explanation. In particular, the shapes of the spherical or aspherical surfaces shown in the drawings are shown by way of example. That is, the shape of the spherical surface or the aspherical surface is not limited to the shape of the spherical surface or the aspherical surface shown in the drawings. The figures are purely diagrammatic and not drawn to scale.
Herein, the paraxial region refers to a region near the optical axis. If the lens surface is convex and the convex position 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 concave position is not defined, it means that the lens surface is concave at least in the paraxial region. The surface of each lens close to the object side becomes the object side surface of the lens, and the surface of each lens close to the image side is called the image side surface of the lens. The determination of the surface shape in the paraxial region can be performed by determining whether or not the surface shape is concave or convex, based on the R value (R denotes the radius of curvature of the paraxial region, and usually denotes the R value in a lens database (lens data) in optical software) in accordance with the determination method of a person ordinarily skilled in the art. For the object side surface, when the R value is positive, the object side surface is judged to be convex, and when the R value is negative, the object side surface is judged to be concave; in the case of the image side surface, the image side surface is determined to be concave when the R value is positive, and is determined to be convex when the R value is negative.
The invention provides an optical imaging lens, aiming at solving the problem of poor imaging quality of the optical imaging lens in the prior art.
As shown in fig. 1 to 30, the imaging lens system sequentially includes, from an object side to an image side of the imaging lens system: the lens comprises a first lens, a second lens, a third lens, a fourth lens, a fifth lens and a sixth lens, wherein the first lens has positive focal power, and the object side surface of the first lens is a convex surface; the second lens has negative focal power, and the image side surface of the second lens is a concave surface; the third lens has negative focal power, the object side surface of the third lens is a convex surface, and the image side surface of the third lens is a concave surface; the fourth lens has positive focal power; the fifth lens has focal power; the sixth lens has negative focal power, the object side surface of the sixth lens is a concave surface, and the image side surface of the sixth lens is a concave surface; wherein, satisfy between the effective focal length f of optical imaging lens and the entrance pupil diameter EPD of optical imaging lens: f/EPD < 1.9; the maximum field angle FOV of the optical imaging lens satisfies the following conditions: 0.5< tan (fov) < 1.5.
The first lens with positive focal power and the convex object side surface and the second lens with negative focal power and the concave image side surface are combined, so that the aperture of the optical imaging lens can be enlarged, and meanwhile, the spherical aberration is reduced under the condition of a large aperture; and the lens is matched with a third lens with negative focal power, so that light rays can be transmitted smoothly, and coma, astigmatism and distortion can be reduced. The fourth lens with positive focal power is mainly used for balancing and distributing focal power, and is beneficial to reducing the aberration of the optical imaging lens; the sixth lens with the concave object side and the concave image side and the negative focal power can synchronously balance the distortion of the optical imaging lens while reducing the on-axis chromatic aberration, the coma aberration and the astigmatism. By limiting the f/EPD within a reasonable range, the aperture of the optical imaging lens can be increased, and the light flux entering the optical imaging lens is increased. The tan (FOV) is limited within a reasonable range, mainly in order to increase the focal length of the system, the magnification of the object image is changed by increasing the focal length, and further the image compression is realized, so that the shot meeting the condition range is more layered and stereoscopic in close-up shooting of the person.
Preferably, the effective focal length f of the optical imaging lens and the entrance pupil diameter EPD of the optical imaging lens satisfy: 1.6< f/EPD < 1.88; the maximum field angle FOV of the optical imaging lens satisfies the following conditions: 1.0< tan (fov) < 1.3.
In the present embodiment, the effective focal length f2 of the second lens and the effective focal length f3 of the third lens satisfy: 0< f2/f3< 1.5. The optical power of the second lens and the third lens is distributed to improve the MTF (modulation Transfer function) performance of the optical system and balance the aberrations such as coma, chromatic aberration, astigmatism and the like of the optical imaging lens, so that the imaging quality of the optical imaging lens is improved. Preferably 0.05< f2/f3< 1.2.
In the present embodiment, the effective focal length f of the optical imaging lens and the effective focal length f1 of the first lens satisfy: 1.5< f/f1< 2.5. The proportion of the focal length of the first lens in the focal length of the whole light imaging lens is distributed to reduce the spherical aberration, the coma aberration, the astigmatism, the field curvature and the distortion of the optical imaging lens, and the imaging quality of the optical imaging lens is improved. Preferably 1.6< f/f1< 2.2.
In the present embodiment, the radius of curvature R4 of the image-side surface of the second lens and the radius of curvature R1 of the object-side surface of the first lens satisfy: 1.3< R4/R1< 3.3. By limiting R4/R1 in a reasonable range, the focal power of the first lens and the focal power of the second lens can be restricted, the aberration of the optical imaging lens can be reduced, the ring ghost generated by the reflection of the glass cover plate and the lenses can be improved, and the imaging quality of the optical imaging lens can be ensured. Preferably, 1.4< R4/R1< 3.2.
In the present embodiment, a radius of curvature R6 of the image-side surface of the third lens and a radius of curvature R5 of the object-side surface of the third lens satisfy: 1.1< R5/R6< 1.6. The focal power of the third lens is distributed by restricting the curvature radius of the object side surface of the third lens and the curvature radius of the image side surface of the third lens, so that the shape of the third lens is changed, the optical performance of the optical imaging lens is improved, the manufacturability of lens processing is improved, and the processing of the lens is facilitated. Preferably, 1.12< R5/R6< 1.5.
In the present embodiment, the radius of curvature R12 of the image-side surface of the sixth lens, the radius of curvature R11 of the object-side surface of the sixth lens, and the effective focal length f of the optical imaging lens satisfy: 1.7< (R12-R11)/f < 2.7. By limiting (R12-R11)/f in a reasonable range, the curvature radius of the sixth lens can be restricted, the focal power of the sixth lens in the optical imaging lens is distributed, the optical performance of the optical imaging lens is improved, the field curvature and the distortion are optimized, meanwhile, the ghost image generated by the internal reflection of the sixth lens can be improved, and the imaging quality of the optical imaging lens is improved. Preferably, 1.8< (R12-R11)/f < 2.6.
In the present embodiment, the effective half aperture DT11 of the object-side surface of the first lens, the effective half aperture DT12 of the image-side surface of the first lens, and the effective half aperture DT62 of the image-side surface of the sixth lens satisfy: 1.3< (DT11+ DT12)/DT62< 1.8. By limiting (DT11+ DT12)/DT62 within a reasonable range, the aperture size of the sixth lens is reduced, stray light at the tail end of the optical imaging lens is improved, and the imaging quality of the optical imaging lens is improved. Preferably, 1.4< (DT11+ DT12)/DT62< 1.7.
In the present embodiment, the combined focal length f12 of the first lens and the second lens, the combined focal length f56 of the fifth lens and the sixth lens, and the effective focal length f of the optical imaging lens satisfy: 1.4< (f12-f56)/f < 2.5. The relationship among the focal powers of the first lens, the second lens, the fifth lens and the sixth lens is reasonably distributed, so that the optical performance of the optical imaging lens can be improved, and the aberration of the optical imaging lens is reduced. Preferably, 1.5< (f12-f56)/f < 2.45.
In the present embodiment, an air interval T34 between the third lens and the fourth lens on the optical axis of the optical imaging lens, an air interval T45 between the fourth lens and the fifth lens on the optical axis, and an air interval T56 between the fifth lens and the sixth lens on the optical axis satisfy: 0.5< (T34+ T45)/T56< 1.6. By limiting (T34+ T45)/T56 within a reasonable range, the aberration of the optical imaging lens can be balanced, the field curvature of the optical imaging lens is reduced, and the performance of the optical imaging lens is improved. Preferably, 0.55< (T34+ T45)/T56< 1.55.
In the present embodiment, an on-axis distance SAG21 between an intersection point of an object-side surface of the second lens and an optical axis of the optical imaging lens to an effective radius vertex of the object-side surface of the second lens, an on-axis distance SAG22 between an intersection point of an image-side surface of the second lens and the optical axis to an effective radius vertex of the image-side surface of the second lens, an on-axis distance SAG51 between an intersection point of an object-side surface of the fifth lens and the optical axis to an effective radius vertex of an object-side surface of the fifth lens, and an on-axis distance SAG52 between an intersection point of an image-side surface of the fifth lens and the optical axis to an effective radius vertex of an image-side surface of the fifth lens satisfy: -1.2< (SAG21+ SAG22)/(SAG51+ SAG52) < -0.4. The shapes of the second lens and the fifth lens are controlled by restraining the rise of the lenses, so that the ghost state of the optical imaging lens is optimized, the manufacturability of lens processing is enhanced, and the yield of the optical imaging lens is improved. Preferably, -1.1< (SAG21+ SAG22)/(SAG51+ SAG52) < -0.5.
In this embodiment, an on-axis distance SAG61 between an intersection point of an object-side surface of the sixth lens and an optical axis of the optical imaging lens and an effective radius vertex of the object-side surface of the sixth lens, and an on-axis distance SAG62 between an intersection point of an image-side surface of the sixth lens and the optical axis and an effective radius vertex of the image-side surface of the sixth lens satisfy: 0.8< SAG62/SAG61< 1.5. The shape of the sixth lens is improved by controlling the rise of the sixth lens, the processing manufacturability of the sixth lens is improved, meanwhile, the ghost image generated by the internal reflection of the sixth lens can be optimized, and the imaging quality of the optical imaging lens is improved. Preferably 0.9< SAG62/SAG61< 1.4.
In the present embodiment, the edge thickness ET2 of the second lens, the edge thickness ET3 of the third lens, the center thickness CT2 of the second lens, and the center thickness CT3 of the third lens satisfy: 1.1< (ET2+ ET3)/(CT2+ CT3) < 1.9. The relationship between the edge thickness and the center thickness of the second lens and the third lens is restrained, so that the optimization and improvement of aberrations such as spherical aberration, coma, astigmatism, curvature of field and the like generated by the second lens and the third lens are facilitated, the aberrations are corrected to a certain extent, and meanwhile, the relationship between the edge thickness and the center thickness of the lens is restrained by the condition, so that the processing manufacturability of the lens is improved, the sensitivity of the lens is reduced, and the yield of the optical imaging lens is improved. Preferably, 1.2< (ET2+ ET3)/(CT2+ CT3) < 1.85.
In the present embodiment, the edge thickness ET5 of the fifth lens and the center thickness CT5 of the fifth lens satisfy: 1.1< ET5/CT5< 2.3. The relationship between the edge thickness and the center thickness of the fifth lens is controlled, so that the manufacturability of the fifth lens is improved, the constraint on the conditional expression is favorable for reducing the optical distortion and the field curvature astigmatism of the optical imaging lens, and the shape of the fifth lens is controlled, so that the ghost intensity generated by the reflection of the fifth lens and the sixth lens is reduced. Preferably, 1.2< ET5/CT5< 2.2.
Optionally, the optical imaging lens may further include a filter for correcting color deviation and/or a protective glass for protecting a photosensitive element on the imaging surface.
The optical imaging lens in the present application may employ a plurality of lenses, for example, the above-mentioned six lenses. By reasonably distributing the focal power, the surface shape, the central thickness of each lens, the axial distance between each lens and the like, the aperture of the optical imaging lens can be effectively increased, the sensitivity of the lens can be reduced, and the machinability of the lens can be improved, so that the optical imaging lens is more beneficial to production and processing and can be suitable for portable electronic equipment such as smart phones. The optical imaging lens also has large aperture and large field angle. The advantages of ultra-thin and good imaging quality can meet the miniaturization requirement of intelligent electronic products.
In the present application, at least one of the mirror surfaces of each lens is an aspherical mirror surface. The aspheric lens is characterized in that: the curvature varies 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 better curvature radius characteristics, and has advantages of improving distortion aberration and improving astigmatic aberration. After the aspheric lens is adopted, the aberration generated during imaging can be eliminated as much as possible, thereby improving the imaging quality.
However, it will be appreciated by those skilled in the art that the number of lenses constituting an optical imaging lens may be varied to achieve the various results and advantages described in the present specification without departing from the claimed subject matter. For example, although six lenses are exemplified in the embodiment, the optical imaging lens is not limited to include six lenses. The optical imaging lens may also include other numbers of lenses, as desired.
Examples of specific surface types and parameters applicable to the optical imaging lens of the above-described embodiment are further described below with reference to the drawings.
Example one
As shown in fig. 1 to 5, an optical imaging lens according to a first embodiment of the present application is described. Fig. 1 is a schematic diagram illustrating a structure of an optical imaging lens according to a first embodiment.
As shown in fig. 1, the optical imaging lens includes, in order from an object side to an image side: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a filter E7, and an image forming surface S15.
The first lens element E1 has positive refractive power, and the object-side surface S1 and the image-side surface S2 of the first lens element are convex. The second lens element E2 has negative power, and the object-side surface S3 of the second lens element is convex and the image-side surface S4 of the second lens element is concave. The third lens element E3 has negative power, and the object-side surface S5 of the third lens element is convex and the image-side surface S6 of the third lens element is concave. The fourth lens element E4 has positive refractive power, and the object-side surface S7 of the fourth lens element is concave, and the image-side surface S8 of the fourth lens element is convex. The fifth lens element E5 has positive refractive power, and the object-side surface S9 of the fifth lens element is concave, and the image-side surface S10 of the fifth lens element is convex. The sixth lens element E6 has negative refractive power, and has a concave object-side surface S11 and a concave image-side surface S12. Filter E7 has an object side S13 and an image side S14 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S14 and is finally imaged on the imaging surface S15.
In the present embodiment, the total effective focal length f of the optical imaging lens is 7.07mm, the maximum field angle FOV of the optical imaging lens is 50.3 °, the total length TTL of the optical imaging lens is 6.83mm, and the image height ImgH is 3.36 mm.
Table 1 shows a basic structural parameter table of the optical imaging lens of the first embodiment, in which the units of the radius of curvature, the thickness/distance, the focal length, and the effective radius are all millimeters (mm).
Figure BDA0003271231790000071
Figure BDA0003271231790000081
TABLE 1
In the first embodiment, the object-side surface and the image-side surface of any one of the first lens element E1 through the sixth lens element E6 are aspheric, and the surface shape of each aspheric lens can be defined by, but is not limited to, the following aspheric formula:
Figure BDA0003271231790000082
wherein x is the rise of the distance from the aspheric surface vertex to the aspheric surface vertex when the aspheric surface is at the position with the height of h along the optical axis direction; c is the paraxial curvature of the aspheric surface, c being 1/R (i.e., paraxial curvature c is the inverse of radius of curvature R in table 1 above); k is a conic coefficient; ai is the correction coefficient of the i-th order of the aspherical surface. Table 2 below shows the high-order coefficient A4, A6, A8, A10, A12, A14, A16, A18, A20, A22, A24, A26, A28, A30 which can be used for each of the aspherical mirrors S1-S12 in example one.
Figure BDA0003271231790000083
Figure BDA0003271231790000091
TABLE 2
Fig. 2 shows an axial chromatic aberration curve of the optical imaging lens according to the first embodiment, which indicates that light rays with different wavelengths are deviated from a convergent focus after passing through the optical imaging lens. Fig. 3 shows astigmatism curves of the optical imaging lens according to the first embodiment, which represent meridional field curvature and sagittal field curvature. Fig. 4 shows distortion curves of the optical imaging lens according to the first embodiment, which indicate values of distortion magnitudes corresponding to different angles of view. Fig. 5 shows a chromatic aberration of magnification curve of the optical imaging lens according to the first embodiment, which shows the deviation of different image heights on the imaging surface after the light passes through the lens.
As can be seen from fig. 2 to 5, the optical imaging lens according to the first embodiment can achieve good imaging quality.
Example two
As shown in fig. 6 to 10, an optical imaging lens according to a second embodiment of the present application is described. In this embodiment and the following embodiments, for the sake of brevity, descriptions of parts similar to those of the first embodiment will be omitted. Fig. 6 is a schematic diagram showing a structure of an optical imaging lens according to a second embodiment.
As shown in fig. 6, the optical imaging lens includes, in order from an object side to an image side: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a filter E7, and an image forming surface S15.
The first lens element E1 has positive refractive power, and the object-side surface S1 of the first lens element is convex, and the image-side surface S2 of the first lens element is concave. The second lens element E2 has negative power, and the object-side surface S3 of the second lens element is convex and the image-side surface S4 of the second lens element is concave. The third lens element E3 has negative power, and the object-side surface S5 of the third lens element is convex and the image-side surface S6 of the third lens element is concave. The fourth lens element E4 has positive refractive power, and the object-side surface S7 of the fourth lens element is concave, and the image-side surface S8 of the fourth lens element is convex. The fifth lens element E5 has negative power, and the object-side surface S9 of the fifth lens element is concave, and the image-side surface S10 of the fifth lens element is convex. The sixth lens element E6 has negative refractive power, and has a concave object-side surface S11 and a concave image-side surface S12. Filter E7 has an object side S13 and an image side S14 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S14 and is finally imaged on the imaging surface S15.
In the present embodiment, the total effective focal length f of the optical imaging lens is 7.07mm, the maximum field angle FOV of the optical imaging lens is 50.4 °, the total length TTL of the optical imaging lens is 6.83mm, and the image height ImgH is 3.37 mm.
Table 3 shows a basic structural parameter table of the optical imaging lens of the second embodiment, in which the units of the radius of curvature, the thickness/distance, the focal length, and the effective radius are all millimeters (mm).
Figure BDA0003271231790000092
Figure BDA0003271231790000101
TABLE 3
Table 4 shows the high-order term coefficients that can be used for each aspherical mirror surface in example two, wherein each aspherical mirror surface type can be defined by formula (1) given in example one above.
Flour mark A4 A6 A8 A10 A12 A14 A16
S1 -7.5629E-04 -4.3213E-03 7.7446E-03 -8.6886E-03 5.6686E-03 -2.0260E-03 2.0849E-04
S2 1.4815E-02 -3.2651E-02 3.2029E-02 -2.2906E-02 1.3969E-02 -6.9729E-03 2.5775E-03
S3 5.7955E-02 -7.6053E-02 1.6319E-01 -3.1359E-01 4.0199E-01 -3.4456E-01 2.0032E-01
S4 3.9427E-02 6.2238E-04 -1.9866E-02 2.3458E-01 -8.5680E-01 1.6175E+00 -1.8730E+00
S5 -1.3579E-01 8.9391E-03 2.7245E-01 -7.2339E-01 1.1370E+00 -1.1933E+00 8.4673E-01
S6 -1.4060E-01 7.5562E-02 -1.5422E-01 7.9521E-01 -2.2936E+00 3.9393E+00 -4.2901E+00
S7 4.7481E-03 4.5976E-02 -2.8790E-01 8.9414E-01 -1.7562E+00 2.2654E+00 -1.9421E+00
S8 2.8966E-03 1.7725E-02 -9.9792E-02 1.9613E-01 -2.2889E-01 1.5146E-01 -4.0408E-02
S9 -1.1075E-02 -6.7476E-02 1.1346E-01 -2.5351E-01 3.7164E-01 -3.5148E-01 2.1676E-01
S10 -3.5502E-03 -3.6586E-02 2.4091E-02 -4.0193E-02 5.5303E-02 -4.6565E-02 2.4645E-02
S11 -1.3467E-01 1.2013E-01 -1.0885E-01 9.0750E-02 -6.1419E-02 3.1457E-02 -1.1792E-02
S12 -1.5701E-01 1.1988E-01 -9.3300E-02 6.0381E-02 -2.9920E-02 1.0822E-02 -2.7531E-03
Flour mark A18 A20 A22 A24 A26 A28 A30
S1 1.3148E-04 -6.3170E-05 1.2455E-05 -1.2009E-06 4.5239E-08 0.0000E+00 0.0000E+00
S2 -6.5304E-04 1.0569E-04 -9.7785E-06 3.9220E-07 0.0000E+00 0.0000E+00 0.0000E+00
S3 -7.8109E-02 1.9547E-02 -2.8345E-03 1.8092E-04 0.0000E+00 0.0000E+00 0.0000E+00
S4 1.4094E+00 -6.9301E-01 2.1494E-01 -3.8173E-02 2.9600E-03 0.0000E+00 0.0000E+00
S5 -3.9761E-01 1.1723E-01 -1.9436E-02 1.3631E-03 0.0000E+00 0.0000E+00 0.0000E+00
S6 3.0022E+00 -1.3101E+00 3.2468E-01 -3.4886E-02 0.0000E+00 0.0000E+00 0.0000E+00
S7 1.0945E+00 -3.8911E-01 7.9019E-02 -6.9751E-03 0.0000E+00 0.0000E+00 0.0000E+00
S8 -1.4543E-02 1.5151E-02 -4.6295E-03 5.1688E-04 0.0000E+00 0.0000E+00 0.0000E+00
S9 -8.6537E-02 2.1583E-02 -3.0566E-03 1.8744E-04 0.0000E+00 0.0000E+00 0.0000E+00
S10 -8.2089E-03 1.6697E-03 -1.8963E-04 9.2207E-06 0.0000E+00 0.0000E+00 0.0000E+00
S11 3.1873E-03 -6.1237E-04 8.1432E-05 -7.1159E-06 3.6716E-07 -8.4679E-09 0.0000E+00
S12 4.7118E-04 -4.9580E-05 2.3359E-06 8.5359E-08 -1.5913E-08 5.6856E-10 0.0000E+00
TABLE 4
Fig. 7 shows an on-axis chromatic aberration curve of the optical imaging lens of the second embodiment, which represents the deviation of the convergent focal points of the light rays of different wavelengths after passing through the optical imaging lens. Fig. 8 shows astigmatism curves representing meridional field curvature and sagittal field curvature of the optical imaging lens of the second embodiment. Fig. 9 shows distortion curves of the optical imaging lens of the second embodiment, which represent distortion magnitude values corresponding to different angles of view. Fig. 10 shows a chromatic aberration of magnification curve of the optical imaging lens according to the second embodiment, which shows the deviation of different image heights on the imaging surface after the light passes through the lens.
As can be seen from fig. 7 to 10, the optical imaging lens according to the second embodiment can achieve good imaging quality.
EXAMPLE III
As shown in fig. 11 to 15, an optical imaging lens of a third embodiment of the present application is described. Fig. 11 is a schematic diagram showing a structure of an optical imaging lens according to a third embodiment.
As shown in fig. 11, the optical imaging lens includes, in order from an object side to an image side: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a filter E7, and an image forming surface S15.
The first lens element E1 has positive refractive power, and the object-side surface S1 and the image-side surface S2 of the first lens element are convex. The second lens element E2 has negative power, and the object-side surface S3 of the second lens element is convex and the image-side surface S4 of the second lens element is concave. The third lens element E3 has negative power, and the object-side surface S5 of the third lens element is convex and the image-side surface S6 of the third lens element is concave. The fourth lens element E4 has positive refractive power, and the object-side surface S7 of the fourth lens element is concave, and the image-side surface S8 of the fourth lens element is convex. The fifth lens element E5 has negative power, and the object-side surface S9 of the fifth lens element is convex and the image-side surface S10 of the fifth lens element is concave. The sixth lens element E6 has negative refractive power, and has a concave object-side surface S11 and a concave image-side surface S12. Filter E7 has an object side S13 and an image side S14 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S14 and is finally imaged on the imaging surface S15.
In the present embodiment, the total effective focal length f of the optical imaging lens is 7.13mm, the maximum field angle FOV of the optical imaging lens is 49.9 °, the total length TTL of the optical imaging lens is 6.80mm, and the image height ImgH is 3.36 mm.
Table 5 shows a basic structural parameter table of the optical imaging lens of the third embodiment, in which the units of the radius of curvature, the thickness/distance, the focal length, and the effective radius are all millimeters (mm).
Figure BDA0003271231790000111
Figure BDA0003271231790000121
TABLE 5
Table 6 shows the high-order term coefficients that can be used for each aspherical mirror surface in the third embodiment, wherein each aspherical mirror surface type can be defined by the formula (1) given in the first embodiment.
Flour mark A4 A6 A8 A10 A12 A14 A16
S1 -5.8819E-04 -4.7441E-03 8.6205E-03 -8.4988E-03 2.5786E-03 3.0263E-03 -4.0376E-03
S2 1.1695E-02 -4.1803E-02 1.0095E-01 -1.4557E-01 1.3423E-01 -8.2302E-02 3.4025E-02
S3 7.2572E-03 -5.4272E-02 1.3281E-01 -1.6264E-01 1.0289E-01 -1.3820E-02 -2.7340E-02
S4 -6.6390E-03 -2.1786E-02 7.5286E-02 -1.8451E-01 5.1937E-01 -1.0904E+00 1.4973E+00
S5 -9.2967E-02 -1.6101E-01 9.5179E-01 -3.5657E+00 9.3582E+00 -1.7005E+01 2.1683E+01
S6 -9.5257E-02 7.8133E-02 -1.0159E+00 6.3785E+00 -2.3475E+01 5.7072E+01 -9.5316E+01
S7 4.1491E-02 -1.3647E-01 6.6999E-01 -2.5190E+00 6.2396E+00 -1.0453E+01 1.2040E+01
S8 4.1517E-02 -1.5408E-01 8.2030E-01 -3.4196E+00 9.6537E+00 -1.9002E+01 2.6674E+01
S9 -3.3244E-02 -1.5162E-01 3.9318E-01 -7.9355E-01 1.0149E+00 -7.8093E-01 2.8964E-01
S10 -3.5844E-02 -1.2882E-01 3.6632E-01 -7.5191E-01 1.0632E+00 -1.0534E+00 7.4833E-01
S11 -7.0964E-02 1.6830E-02 8.6937E-05 1.0112E-02 -2.0420E-02 1.7986E-02 -9.4910E-03
S12 -9.1287E-02 3.2033E-02 -1.0911E-02 2.4012E-03 1.1168E-03 -1.9679E-03 1.3702E-03
Flour mark A18 A20 A22 A24 A26 A28 A30
S1 2.2794E-03 -7.4121E-04 1.4317E-04 -1.5260E-05 6.8882E-07 0.0000E+00 0.0000E+00
S2 -9.3900E-03 1.6597E-03 -1.7005E-04 7.6855E-06 0.0000E+00 0.0000E+00 0.0000E+00
S3 2.1790E-02 -7.6801E-03 1.3706E-03 -1.0037E-04 0.0000E+00 0.0000E+00 0.0000E+00
S4 -1.3294E+00 7.5879E-01 -2.6888E-01 5.3770E-02 -4.6291E-03 0.0000E+00 0.0000E+00
S5 -1.9538E+01 1.2370E+01 -5.3786E+00 1.5284E+00 -2.5548E-01 1.9041E-02 0.0000E+00
S6 1.1098E+02 -8.9927E+01 4.9692E+01 -1.7849E+01 3.7552E+00 -3.5102E-01 0.0000E+00
S7 -9.5379E+00 5.1014E+00 -1.7586E+00 3.5250E-01 -3.1192E-02 0.0000E+00 0.0000E+00
S8 -2.7022E+01 1.9781E+01 -1.0356E+01 3.7766E+00 -9.1042E-01 1.3028E-01 -8.3726E-03
S9 4.8342E-02 -1.1303E-01 5.9015E-02 -1.5961E-02 2.2779E-03 -1.3562E-04 0.0000E+00
S10 -3.8586E-01 1.4476E-01 -3.9174E-02 7.4626E-03 -9.5098E-04 7.2858E-05 -2.5390E-06
S11 3.3394E-03 -8.1769E-04 1.4054E-04 -1.6647E-05 1.2929E-06 -5.9128E-08 1.2035E-09
S12 -5.7909E-04 1.6076E-04 -2.9964E-05 3.7159E-06 -2.9376E-07 1.3368E-08 -2.6573E-10
TABLE 6
Fig. 12 shows an on-axis chromatic aberration curve of the optical imaging lens of the third embodiment, which represents the deviation of the convergent focal points of the light rays of different wavelengths after passing through the optical imaging lens. Fig. 13 shows astigmatism curves representing meridional field curvature and sagittal field curvature of the optical imaging lens of the third embodiment. Fig. 14 shows distortion curves of the optical imaging lens of the third embodiment, which represent distortion magnitude values corresponding to different angles of view. Fig. 15 shows a chromatic aberration of magnification curve of the optical imaging lens according to the third embodiment, which shows the deviation of different image heights on the imaging surface after the light passes through the lens.
As can be seen from fig. 12 to 15, the optical imaging lens according to the third embodiment can achieve good imaging quality.
Example four
As shown in fig. 16 to 20, an optical imaging lens according to a fourth embodiment of the present application is described. Fig. 16 is a schematic diagram showing a configuration of an optical imaging lens according to a fourth embodiment.
As shown in fig. 16, the optical imaging lens includes, in order from an object side to an image side: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a filter E7, and an image forming surface S15.
The first lens element E1 has positive refractive power, and the object-side surface S1 and the image-side surface S2 of the first lens element are convex. The second lens E2 has negative power, and the object-side surface S3 of the second lens is concave, and the image-side surface S4 of the second lens is concave. The third lens element E3 has negative power, and the object-side surface S5 of the third lens element is convex and the image-side surface S6 of the third lens element is concave. The fourth lens element E4 has positive refractive power, and the object-side surface S7 of the fourth lens element is convex and the image-side surface S8 of the fourth lens element is concave. The fifth lens element E5 has positive refractive power, and the object-side surface S9 of the fifth lens element is convex and the image-side surface S10 of the fifth lens element is concave. The sixth lens element E6 has negative refractive power, and has a concave object-side surface S11 and a concave image-side surface S12. Filter E7 has an object side S13 and an image side S14 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S14 and is finally imaged on the imaging surface S15.
In the present embodiment, the total effective focal length f of the optical imaging lens is 7.15mm, the maximum field angle FOV of the optical imaging lens is 49.7 °, the total length TTL of the optical imaging lens is 7.20mm, and the image height ImgH is 3.35 mm.
Table 7 shows a basic structural parameter table of the optical imaging lens of the fourth embodiment, in which the units of the radius of curvature, the thickness/distance, the focal length, and the effective radius are all millimeters (mm).
Figure BDA0003271231790000131
TABLE 7
Table 8 shows the high-order term coefficients that can be used for each aspherical mirror surface in the fourth embodiment, wherein each aspherical mirror surface type can be defined by the formula (1) given in the first embodiment described above.
Flour mark A4 A6 A8 A10 A12 A14 A16
S1 7.5598E-02 -5.4382E-02 7.4630E-02 -1.1391E-01 1.4121E-01 -1.2900E-01 8.5470E-02
S2 -1.1106E-02 1.0623E-01 -3.3767E-01 5.8569E-01 -6.4776E-01 4.9533E-01 -2.7337E-01
S3 1.3237E-03 1.1343E-01 -3.6427E-01 6.7129E-01 -8.2537E-01 7.3319E-01 -4.8927E-01
S4 -7.1997E-03 8.2749E-02 -3.2089E-01 1.0018E+00 -2.1882E+00 3.3727E+00 -3.7202E+00
S5 -4.7661E-02 -8.0973E-03 2.0608E-01 -7.2825E-01 1.6357E+00 -2.5375E+00 2.8138E+00
S6 -5.0725E-02 6.5050E-02 -2.9775E-01 1.1154E+00 -2.8138E+00 4.9176E+00 -6.1045E+00
S7 -4.5116E-02 2.3289E-02 -1.1095E-01 4.5393E-01 -1.3626E+00 2.8156E+00 -4.0584E+00
S8 -7.0303E-02 -7.0216E-04 1.9377E-01 -9.6104E-01 2.7289E+00 -5.1537E+00 6.7828E+00
S9 -8.1688E-02 -7.0431E-02 3.8475E-01 -1.4309E+00 3.4400E+00 -5.6521E+00 6.5496E+00
S10 -5.9810E-02 -6.7196E-03 4.6006E-02 -1.8384E-01 4.2983E-01 -6.4198E-01 6.5422E-01
S11 -1.4034E-01 9.9397E-02 -8.8706E-02 8.0968E-02 -6.0656E-02 3.4233E-02 -1.4027E-02
S12 -1.2343E-01 8.0360E-02 -6.0890E-02 4.3885E-02 -2.7540E-02 1.4388E-02 -6.0366E-03
Flour mark A18 A20 A22 A24 A26 A28 A30
S1 -4.1079E-02 1.4288E-02 -3.5553E-03 6.1648E-04 -7.0703E-05 4.8183E-06 -1.4767E-07
S2 1.1134E-01 -3.3748E-02 7.5710E-03 -1.2287E-03 1.3701E-04 -9.4141E-06 3.0039E-07
S3 2.4861E-01 -9.5709E-02 2.7354E-02 -5.5973E-03 7.7148E-04 -6.3909E-05 2.3963E-06
S4 2.9636E+00 -1.7053E+00 7.0101E-01 -2.0048E-01 3.7840E-02 -4.2320E-03 2.1213E-04
S5 -2.2632E+00 1.3229E+00 -5.5601E-01 1.6360E-01 -3.1967E-02 3.7236E-03 -1.9558E-04
S6 5.4552E+00 -3.5169E+00 1.6193E+00 -5.1881E-01 1.0978E-01 -1.3778E-02 7.7609E-04
S7 4.1433E+00 -3.0132E+00 1.5497E+00 -5.5020E-01 1.2809E-01 -1.7567E-02 1.0738E-03
S8 -6.3478E+00 4.2480E+00 -2.0171E+00 6.6337E-01 -1.4361E-01 1.8402E-02 -1.0571E-03
S9 -5.4333E+00 3.2358E+00 -1.3702E+00 4.0197E-01 -7.7512E-02 8.8215E-03 -4.4815E-04
S10 -4.6811E-01 2.3756E-01 -8.5083E-02 2.1025E-02 -3.4098E-03 3.2644E-04 -1.3974E-05
S11 4.0614E-03 -7.9625E-04 9.5265E-05 -4.4765E-06 -4.1630E-07 7.0298E-08 -2.9715E-09
S12 1.9692E-03 -4.8511E-04 8.7606E-05 -1.1168E-05 9.4734E-07 -4.7842E-08 1.0860E-09
TABLE 8
Fig. 17 shows an on-axis chromatic aberration curve of the optical imaging lens of the fourth embodiment, which represents the deviation of the convergent focal points of light rays of different wavelengths after passing through the optical imaging lens. Fig. 18 shows astigmatism curves representing meridional field curvature and sagittal field curvature of the optical imaging lens of the fourth embodiment. Fig. 19 shows distortion curves of the optical imaging lens of the fourth embodiment, which represent distortion magnitude values corresponding to different angles of view. Fig. 20 shows a chromatic aberration of magnification curve of the optical imaging lens according to the fourth embodiment, which represents the deviation of different image heights on the imaging surface after the light passes through the lens.
As can be seen from fig. 17 to 20, the optical imaging lens according to the fourth embodiment can achieve good imaging quality.
EXAMPLE five
As shown in fig. 21 to 25, an optical imaging lens of fifth embodiment of the present application is described. Fig. 21 is a schematic diagram showing a configuration of an optical imaging lens of embodiment five.
As shown in fig. 21, the optical imaging lens includes, in order from an object side to an image side: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a filter E7, and an image forming surface S15.
The first lens element E1 has positive refractive power, and the object-side surface S1 and the image-side surface S2 of the first lens element are convex. The second lens E2 has negative power, and the object-side surface S3 of the second lens is concave, and the image-side surface S4 of the second lens is concave. The third lens element E3 has negative power, and the object-side surface S5 of the third lens element is convex and the image-side surface S6 of the third lens element is concave. The fourth lens element E4 has positive refractive power, and the object-side surface S7 of the fourth lens element is convex and the image-side surface S8 of the fourth lens element is concave. The fifth lens element E5 has positive refractive power, and the object-side surface S9 of the fifth lens element is convex and the image-side surface S10 of the fifth lens element is concave. The sixth lens element E6 has negative refractive power, and has a concave object-side surface S11 and a concave image-side surface S12. Filter E7 has an object side S13 and an image side S14 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S14 and is finally imaged on the imaging surface S15.
In the present embodiment, the total effective focal length f of the optical imaging lens is 7.13mm, the maximum field angle FOV of the optical imaging lens is 50.0 °, the total length TTL of the optical imaging lens is 7.10mm, and the image height ImgH is 3.35 mm.
Table 9 shows a basic structural parameter table of the optical imaging lens of example five, in which the units of the radius of curvature, thickness/distance, focal length, and effective radius are all millimeters (mm).
Figure BDA0003271231790000151
TABLE 9
Table 10 shows the high-order term coefficients that can be used for each aspherical mirror surface in example five, wherein each aspherical mirror surface type can be defined by formula (1) given in example one above.
Figure BDA0003271231790000152
Figure BDA0003271231790000161
Watch 10
Fig. 22 shows an on-axis chromatic aberration curve of the optical imaging lens of the fifth embodiment, which represents the deviation of the convergent focal points of light rays of different wavelengths after passing through the optical imaging lens. Fig. 23 shows astigmatism curves representing meridional field curvature and sagittal field curvature of the optical imaging lens of example five. Fig. 24 shows distortion curves of the optical imaging lens of embodiment five, which represent distortion magnitude values corresponding to different angles of view. Fig. 25 shows a chromatic aberration of magnification curve of the optical imaging lens of the fifth embodiment, which represents a deviation of different image heights on the imaging surface after light passes through the lens.
As can be seen from fig. 22 to 25, the optical imaging lens according to the fifth embodiment can achieve good imaging quality.
EXAMPLE six
As shown in fig. 26 to 30, an optical imaging lens according to a sixth embodiment of the present application is described. Fig. 26 is a schematic diagram showing a configuration of an optical imaging lens of embodiment six.
As shown in fig. 26, the optical imaging lens, in order from an object side to an image side, comprises: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a filter E7, and an image forming surface S15.
The first lens element E1 has positive refractive power, and the object-side surface S1 and the image-side surface S2 of the first lens element are convex. The second lens E2 has negative power, and the object-side surface S3 of the second lens is concave, and the image-side surface S4 of the second lens is concave. The third lens element E3 has negative power, and the object-side surface S5 of the third lens element is convex and the image-side surface S6 of the third lens element is concave. The fourth lens element E4 has positive refractive power, and the object-side surface S7 of the fourth lens element is convex and the image-side surface S8 of the fourth lens element is concave. The fifth lens element E5 has positive refractive power, and the object-side surface S9 of the fifth lens element is convex and the image-side surface S10 of the fifth lens element is concave. The sixth lens element E6 has negative refractive power, and has a concave object-side surface S11 and a concave image-side surface S12. Filter E7 has an object side S13 and an image side S14 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S14 and is finally imaged on the imaging surface S15.
In the present embodiment, the total effective focal length f of the optical imaging lens is 7.11mm, the maximum field angle FOV of the optical imaging lens is 49.9 °, the total length TTL of the optical imaging lens is 6.80mm, and the image height ImgH is 3.35 mm.
Table 11 shows a basic structural parameter table of the optical imaging lens of example six, in which the units of the radius of curvature, thickness/distance, focal length, and effective radius are all millimeters (mm).
Figure BDA0003271231790000171
TABLE 11
Table 12 shows the high-order term coefficients that can be used for each aspherical mirror surface in example six, wherein each aspherical mirror surface type can be defined by formula (1) given in example one above.
Figure BDA0003271231790000172
Figure BDA0003271231790000181
TABLE 12
Fig. 27 shows an on-axis chromatic aberration curve of the optical imaging lens of the sixth embodiment, which represents the deviation of the convergent focal points of light rays of different wavelengths after passing through the optical imaging lens. Fig. 28 shows astigmatism curves representing meridional field curvature and sagittal field curvature of the optical imaging lens of example six. Fig. 29 shows distortion curves of the optical imaging lens of the sixth embodiment, which represent distortion magnitude values corresponding to different angles of view. Fig. 30 shows a chromatic aberration of magnification curve of the optical imaging lens of the sixth embodiment, which represents the deviation of different image heights on the imaging surface after the light passes through the lens.
As can be seen from fig. 27 to 30, the optical imaging lens according to the sixth embodiment can achieve good imaging quality.
In summary, the first to sixth embodiments satisfy the relationships shown in table 13, respectively.
Conditions/examples 1 2 3 4 5 6
f/EPD 1.81 1.81 1.83 1.71 1.76 1.87
tan(FOV) 1.21 1.21 1.19 1.18 1.19 1.19
f2/f3 1.12 0.92 0.58 0.09 0.22 0.34
f/f1 1.75 1.77 1.89 1.89 1.93 2.08
R4/R1 1.49 1.74 1.50 2.92 3.07 2.59
R5/R6 1.39 1.39 1.38 1.16 1.33 1.44
(R12-R11)/f 2.35 2.36 2.54 1.99 2.07 1.97
(DT11+DT12)/DT62 1.42 1.43 1.43 1.61 1.59 1.52
(f12-f56)/f 2.17 1.60 1.59 2.40 2.39 1.91
(T34+T45)/T56 0.99 1.31 1.06 0.81 0.72 0.60
(SAG21+SAG22)/(SAG51+SAG52) -0.88 -0.60 -0.80 -0.62 -0.75 -1.00
SAG62/SAG61 1.08 1.05 1.31 0.99 1.05 1.23
(ET2+ET3)/(CT2+CT3) 1.74 1.76 1.82 1.27 1.29 1.33
ET5/CT5 1.27 1.86 2.16 1.58 1.73 1.98
Watch 13
Table 14 shows the effective focal lengths f of the optical imaging lenses of the first to sixth embodiments, and the effective focal lengths f1 to f6 of the respective lenses.
Figure BDA0003271231790000182
Figure BDA0003271231790000191
TABLE 14
The present application also provides an imaging device whose electron photosensitive element may be a photo-coupled device (CCD) or a complementary metal oxide semiconductor device (CMOS). The imaging device may be a stand-alone imaging device such as a digital camera, or may be an imaging module integrated on a mobile electronic device such as a mobile phone. The imaging device is equipped with the optical imaging lens described above.
It is to be understood that the above-described embodiments are only a few, but not all, embodiments of the present invention. All other embodiments, which can be derived by a person skilled in the art from the embodiments given herein without making any creative effort, shall fall within the protection scope of the present invention.
It is noted that the terminology used herein is for the purpose of describing particular embodiments only and is not intended to be limiting of example embodiments according to the present application. As used herein, the singular is intended to include the plural unless the context clearly dictates otherwise, and it should be further understood that the terms "comprises" and/or "comprising," when used in this specification, specify the presence of features, steps, operations, devices, components, and/or combinations thereof.
It should be noted that the terms "first," "second," and the like in the description and claims of this application and in the drawings described above are used for distinguishing between similar elements and not necessarily for describing a particular sequential or chronological order. It is to be understood that the data so used is interchangeable under appropriate circumstances such that the embodiments of the application described herein are capable of operation in sequences other than those illustrated or described herein.
The above description is only a preferred embodiment of the present invention and is not intended to limit the present invention, and various modifications and changes may be made by those skilled in the art. Any modification, equivalent replacement, or improvement made within the spirit and principle of the present invention should be included in the protection scope of the present invention.

Claims (10)

1. An optical imaging lens, comprising, in order from an object side to an image side of the optical imaging lens:
a first lens having a positive focal power, an object side surface of the first lens being a convex surface;
the second lens has negative focal power, and the image side surface of the second lens is a concave surface;
the third lens has negative focal power, the object side surface of the third lens is a convex surface, and the image side surface of the third lens is a concave surface;
a fourth lens having a positive optical power;
a fifth lens having an optical power;
the sixth lens has negative focal power, the object side surface of the sixth lens is a concave surface, and the image side surface of the sixth lens is a concave surface;
wherein the effective focal length f of the optical imaging lens and the entrance pupil diameter EPD of the optical imaging lens satisfy: f/EPD < 1.9;
the maximum field angle FOV of the optical imaging lens satisfies the following conditions: 0.5< tan (fov) < 1.5.
2. The optical imaging lens of claim 1, wherein an effective focal length f2 of the second lens and an effective focal length f3 of the third lens satisfy: 0< f2/f3< 1.5.
3. The optical imaging lens of claim 1, wherein the effective focal length f of the optical imaging lens and the effective focal length f1 of the first lens satisfy: 1.5< f/f1< 2.5.
4. The optical imaging lens of claim 1, wherein a radius of curvature R4 of the image side surface of the second lens and a radius of curvature R1 of the object side surface of the first lens satisfy: 1.3< R4/R1< 3.3.
5. The optical imaging lens of claim 1, wherein a radius of curvature R6 of the image side surface of the third lens and a radius of curvature R5 of the object side surface of the third lens satisfy: 1.1< R5/R6< 1.6.
6. The optical imaging lens of claim 1, wherein a radius of curvature R12 of an image side surface of the sixth lens, a radius of curvature R11 of an object side surface of the sixth lens, and an effective focal length f of the optical imaging lens satisfy: 1.7< (R12-R11)/f < 2.7.
7. The optical imaging lens according to claim 1, wherein an effective half aperture DT11 of the object side surface of the first lens, an effective half aperture DT12 of the image side surface of the first lens, and an effective half aperture DT62 of the image side surface of the sixth lens satisfy: 1.3< (DT11+ DT12)/DT62< 1.8.
8. The optical imaging lens of claim 1, wherein a combined focal length f12 of the first and second lenses, a combined focal length f56 of the fifth and sixth lenses, and an effective focal length f of the optical imaging lens satisfy: 1.4< (f12-f56)/f < 2.5.
9. The optical imaging lens of claim 1, wherein an air interval T34 of the third lens and the fourth lens on an optical axis of the optical imaging lens, an air interval T45 of the fourth lens and the fifth lens on the optical axis, and an air interval T56 of the fifth lens and the sixth lens on the optical axis satisfy: 0.5< (T34+ T45)/T56< 1.6.
10. The optical imaging lens of claim 1, wherein an on-axis distance SAG21 between an intersection point of an object-side surface of the second lens and an optical axis of the optical imaging lens and an effective radius vertex of the object-side surface of the second lens, an on-axis distance SAG22 between an intersection point of an image-side surface of the second lens and the optical axis and an effective radius vertex of an image-side surface of the second lens, an on-axis distance SAG51 between an intersection point of an object-side surface of the fifth lens and the optical axis and an effective radius vertex of an object-side surface of the fifth lens, and an on-axis distance SAG52 between an intersection point of an image-side surface of the fifth lens and the optical axis and an effective radius vertex of an image-side surface of the fifth lens satisfy: -1.2< (SAG21+ SAG22)/(SAG51+ SAG52) < -0.4.
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