CN215297805U - Optical imaging lens group - Google Patents

Optical imaging lens group Download PDF

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CN215297805U
CN215297805U CN202120813191.9U CN202120813191U CN215297805U CN 215297805 U CN215297805 U CN 215297805U CN 202120813191 U CN202120813191 U CN 202120813191U CN 215297805 U CN215297805 U CN 215297805U
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lens
optical imaging
lens group
imaging lens
focal length
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陈超
计云兵
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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Abstract

The utility model provides an learn imaging lens group. The optical imaging lens group sequentially comprises from an object side to an image side along an optical axis: a diaphragm; a first lens having a positive refractive power; a second lens; a third lens; a fourth lens having a positive refractive power; wherein the maximum field angle FOV of the optical imaging lens group satisfies: FOV < 20. The utility model provides an among the prior art optical imaging lens group have the poor problem of quality of formation of image.

Description

Optical imaging lens group
Technical Field
The utility model relates to an optical imaging equipment technical field particularly, relates to an optical imaging lens group.
Background
The telephoto lens has a long focal length, a small viewing angle, and a large image on the negative film. Suitable for photographing distant objects. Because the depth of field range of the camera is smaller than that of a standard lens, the camera can more effectively blur the background highlighted focusing main body, the shot main body is generally far away from the camera, the deformation in the perspective aspect of the portrait is smaller, and the photographed portrait is more vivid.
The long-focus shooting is more stable, but the traditional telescopic lens has the problem of unstable shooting. In addition, the use of the telescopic zoom lens affects the thickness and reliability of the body, so the inner zoom is the best way for the mobile phone to realize the optical zoom. In order to realize zooming in an ultrathin fuselage, a telephoto lens gradually adopts a periscopic structure, but the current telephoto lens has a problem of poor imaging quality.
That is, the optical imaging lens group in the prior art has the problem of poor imaging quality.
SUMMERY OF THE UTILITY MODEL
A primary object of the present invention is to provide an optical imaging lens assembly to solve the problem of poor imaging quality of the optical imaging lens assembly in the prior art.
In order to achieve the above object, according to one aspect of the present invention, there is provided an optical imaging lens group, comprising in order from an object side to an image side along an optical axis: a diaphragm; a first lens having a positive refractive power; a second lens; a third lens; a fourth lens having a positive refractive power; wherein the maximum field angle FOV of the optical imaging lens group satisfies: FOV < 20.
Further, the effective focal length f of the optical imaging lens group, the effective focal length f1 of the first lens, and the effective focal length f2 of the second lens satisfy: 4.0 ≦ f/f1| + | f/f2| ≦ 5.0.
Further, the effective focal length f1 of the first lens and the curvature radius R1 of the object side surface of the first lens satisfy: 2.0 ≦ f1/R1 ≦ 3.0.
Further, the effective focal length f2 of the second lens, the radius of curvature R3 of the object-side surface of the second lens, and the radius of curvature R4 of the image-side surface of the second lens satisfy: 0.7 ≦ (R3+ R4)/f2| ≦ 1.6.
Further, the effective focal length f1 of the first lens, the radius of curvature R4 of the image-side surface of the second lens, and the radius of curvature R5 of the object-side surface of the third lens satisfy: 0 ≦ (R4+ R5)/f1 ≦ 2.0.
Further, a center thickness CT1 of the first lens on the optical axis, a center thickness CT2 of the second lens on the optical axis, a center thickness CT3 of the third lens on the optical axis, a center thickness CT4 of the fourth lens on the optical axis, and an air interval T12 of the first lens and the second lens on the optical axis satisfy: 0.5 ≦ (CT1+ CT2+ T12)/(CT3+ CT4) ≦ 1.4.
Further, the combined focal length f234 of the second lens, the third lens and the fourth lens, and the effective focal length f2 of the second lens satisfy: 0.5 ≦ f234/f2 ≦ 2.0.
Further, an on-axis distance TTL from the object side surface of the first lens to the imaging surface of the optical imaging lens group and a distance SD from the diaphragm of the optical imaging lens group to the image side surface of the fourth lens satisfy: 2.0 ≦ TTL/SD ≦ 3.5.
Further, the distance BFL between the image side surface of the fourth lens and the imaging surface of the optical imaging lens group on the optical axis and the sum sigma CT of the central thicknesses of all the lenses on the optical axis satisfy that: 2.0 ≦ BFL/Σ CT ≦ 3.0.
Further, the effective focal length f1 of the first lens and the effective focal length f2 of the second lens satisfy: 0 ≦ f1/f4 ≦ 0.6.
According to another aspect of the present invention, there is provided an optical imaging lens assembly, comprising, in order from an object side to an image side along an optical axis: a diaphragm; a first lens; a second lens having a negative focal power; a third lens; a fourth lens having a positive refractive power; the distance TD on the axis from the object side surface of the first lens to the image side surface of the fourth lens and the distance BFL on the optical axis from the image side surface of the fourth lens to the imaging surface of the optical imaging lens group satisfy that: 0.5 ≦ TD/BFL ≦ 1.0.
Further, the effective focal length f of the optical imaging lens group, the effective focal length f1 of the first lens, and the effective focal length f2 of the second lens satisfy: 4.0 ≦ f/f1| + | f/f2| ≦ 5.0.
Further, the effective focal length f1 of the first lens and the curvature radius R1 of the object side surface of the first lens satisfy: 2.0 ≦ f1/R1 ≦ 3.0.
Further, the effective focal length f2 of the second lens, the radius of curvature R3 of the object-side surface of the second lens, and the radius of curvature R4 of the image-side surface of the second lens satisfy: 0.7 ≦ (R3+ R4)/f2| ≦ 1.6.
Further, the effective focal length f1 of the first lens, the radius of curvature R4 of the image-side surface of the second lens, and the radius of curvature R5 of the object-side surface of the third lens satisfy: 0 ≦ (R4+ R5)/f1 ≦ 2.0.
Further, a center thickness CT1 of the first lens on the optical axis, a center thickness CT2 of the second lens on the optical axis, a center thickness CT3 of the third lens on the optical axis, a center thickness CT4 of the fourth lens on the optical axis/an air interval T12 of the first lens and the second lens on the optical axis satisfy: 0.5 ≦ (CT1+ CT2+ T12)/(CT3+ CT4) ≦ 1.4.
Further, the combined focal length f234 of the second lens, the third lens and the fourth lens, and the effective focal length f2 of the second lens satisfy: 0.5 ≦ f234/f2 ≦ 2.0.
Further, an on-axis distance TTL from the object side surface of the first lens to the imaging surface of the optical imaging lens group and a distance SD from the diaphragm of the optical imaging lens group to the image side surface of the fourth lens satisfy: 2.0 ≦ TTL/SD ≦ 3.5.
Further, the distance BFL between the image side surface of the fourth lens and the imaging surface of the optical imaging lens group on the optical axis and the sum sigma CT of the central thicknesses of all the lenses on the optical axis satisfy that: 2.0 ≦ BFL/Σ CT ≦ 3.0.
Further, an effective focal length f1 of the first lens and an effective focal length f4 of the fourth lens satisfy: 0 ≦ f1/f4 ≦ 0.6.
By applying the technical scheme of the utility model, the optical imaging lens group comprises a diaphragm, a first lens, a second lens, a third lens and a fourth lens from the object side to the image side along the optical axis in sequence, and the first lens has positive focal power; the fourth lens has positive focal power; wherein the maximum field angle FOV of the optical imaging lens group satisfies: FOV < 20.
Through the reasonable distribution of the focal power of each lens, the aberration generated by the optical imaging lens group is favorably balanced, and the imaging quality of the optical imaging lens group is greatly improved. By limiting the maximum field angle of the optical imaging lens group within a reasonable range, the optical system is favorable for having better capability of balancing chromatic aberration and distortion, and the imaging quality is favorably improved.
Drawings
The accompanying drawings, which form a part of the present application, are included to provide a further understanding of the invention, and are incorporated in and constitute a part of this specification, 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 view of an optical imaging lens group according to a first example of the present invention;
fig. 2 to 4 respectively show an on-axis chromatic aberration curve, an astigmatism curve, and a distortion curve of the optical imaging lens group in fig. 1;
fig. 5 is a schematic structural view of an optical imaging lens group according to a second example of the present invention;
fig. 6 to 8 show an on-axis chromatic aberration curve, an astigmatism curve, and a distortion curve of the optical imaging lens group in fig. 5, respectively;
fig. 9 is a schematic structural view of an optical imaging lens group according to a third example of the present invention;
fig. 10 to 12 show an on-axis chromatic aberration curve, an astigmatism curve, and a distortion curve of the optical imaging lens group in fig. 9, respectively;
fig. 13 is a schematic structural view of an optical imaging lens group according to example four of the present invention;
fig. 14 to 16 show an on-axis chromatic aberration curve, an astigmatism curve, and a distortion curve of the optical imaging lens group in fig. 13, respectively;
fig. 17 is a schematic structural view of an optical imaging lens group according to a fifth example of the present invention;
fig. 18 to 20 show an on-axis chromatic aberration curve, an astigmatism curve, and a distortion curve of the optical imaging lens group in fig. 17, respectively;
fig. 21 is a schematic structural view of an optical imaging lens group according to a sixth example of the present invention;
fig. 22 to 24 respectively show an on-axis chromatic aberration curve, an astigmatism curve, and a distortion curve of the optical imaging lens group in fig. 21;
fig. 25 is a schematic structural view of an optical imaging lens group according to a seventh example of the present invention;
fig. 26 to 28 show an on-axis chromatic aberration curve, an astigmatism curve, and a distortion curve of the optical imaging lens group in fig. 25, respectively.
Fig. 29 is a schematic view showing a structure of an optical imaging lens group according to example eight of the present invention;
fig. 30 to 32 show an on-axis chromatic aberration curve, an astigmatism curve, and a distortion curve of the optical imaging lens group in fig. 29, respectively.
Wherein the figures include the following reference numerals:
STO, stop; e1, first lens; s1, the object-side surface of the first lens; s2, the image-side surface of the first lens; e2, second lens; s3, the object-side surface of the second lens; s4, the image-side surface of the second lens; e3, third lens; s5, the object-side surface of the third lens; s6, the image-side surface of the third lens; e4, fourth lens; s7, the object-side surface of the fourth lens; s8, the image-side surface of the fourth lens; e5, filters; s9, the object side surface of the optical filter; s10, the image side of the filter; s11, image forming plane.
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 accompanying drawings in conjunction with embodiments.
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 application, where the contrary is not intended, the use of directional words such as "upper, lower, top and bottom" is generally with respect to the orientation shown in the drawings, or with respect to the component itself in the vertical, perpendicular or gravitational direction; 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.
In order to solve the problem that the optical imaging lens group has the quality of formation of image poor among the prior art, the utility model provides an optical imaging lens group.
Example one
As shown in fig. 1 to 32, the optical imaging lens group includes, in order from an object side to an image side along an optical axis, a diaphragm, a first lens, a second lens, a third lens, and a fourth lens, the first lens having positive power; the fourth lens has positive focal power; wherein the maximum field angle FOV of the optical imaging lens group satisfies: FOV < 20.
Through the reasonable distribution of the focal power of each lens, the aberration generated by the optical imaging lens group is favorably balanced, and the imaging quality of the optical imaging lens group is greatly improved. By limiting the maximum field angle of the optical imaging lens group within a reasonable range, the optical system is favorable for having better capability of balancing chromatic aberration and distortion, and the imaging quality is favorably improved.
In the present embodiment, the effective focal length f of the optical imaging lens group, the effective focal length f1 of the first lens, and the effective focal length f2 of the second lens satisfy: 4.0 ≦ f/f1| + | f/f2| ≦ 5.0. By limiting the ranges of the effective focal length f of the optical imaging lens group, the effective focal length f1 of the first lens and the effective focal length f2 of the second lens, the reasonable distribution of focal power of each lens can be ensured, and the realization of small aberration of an optical system is facilitated. Preferably, 4.05 ≦ f/f1| + | f/f2| ≦ 4.9.
In the present embodiment, the effective focal length f1 of the first lens and the radius of curvature R1 of the object side surface of the first lens satisfy: 2.0 ≦ f1/R1 ≦ 3.0. By limiting the ratio of the effective focal length f1 of the first lens and the curvature radius of the object side surface of the first lens, the imaging lens group can better balance aberration, and the resolution of the optical imaging lens group can be improved. Preferably, 2.05 ≦ f1/R1 ≦ 2.6.
In the present embodiment, the effective focal length f2 of the second lens, the radius of curvature R3 of the object-side surface of the second lens, and the radius of curvature R4 of the image-side surface of the second lens satisfy: 0.7 ≦ (R3+ R4)/f2| ≦ 1.6. The arrangement is favorable for controlling the incident angle of the light rays of the off-axis field of view on the image plane, and the matching performance of the light rays with the photosensitive element and the band-pass filter is improved. Preferably, 0.8 ≦ l (R3+ R4)/f2| ≦ 1.55.
In the present embodiment, the effective focal length f1 of the first lens, the radius of curvature R4 of the image-side surface of the second lens, and the radius of curvature R5 of the object-side surface of the third lens satisfy: 0 ≦ (R4+ R5)/f1 ≦ 2.0. By limiting the relationship among the effective focal length f1 of the first lens, the radius of curvature R4 of the image-side surface of the second lens, and the radius of curvature R5 of the object-side surface of the third lens, optical distortion can be reduced, ensuring better imaging quality. Preferably, 0.6 ≦ (R4+ R5)/f1 ≦ 1.8.
In the present embodiment, the central thickness CT1 of the first lens on the optical axis, the central thickness CT2 of the second lens on the optical axis, the central thickness CT3 of the third lens on the optical axis, the central thickness CT4 of the fourth lens on the optical axis/the air interval T12 of the first lens and the second lens on the optical axis satisfy: 0.5 ≦ (CT1+ CT2+ T12)/(CT3+ CT4) ≦ 1.4. By limiting the relation among the central thickness CT1 of the first lens on the optical axis, the central thickness CT2 of the second lens on the optical axis, the central thickness CT3 of the third lens on the optical axis, the central thickness CT4 of the fourth lens on the optical axis and the air interval T12 of the first lens and the second lens on the optical axis, the optical lens can be ensured to have good processing characteristics, and the processing and manufacturing of each lens are facilitated. Preferably, 0.8 ≦ (CT1+ CT2+ T12)/(CT3+ CT4) ≦ 1.35.
In the present embodiment, the combined focal length f234 of the second lens, the third lens, and the fourth lens, and the effective focal length f2 of the second lens satisfy: 0.5 ≦ f234/f2 ≦ 2.0. By controlling the effective focal length of the second lens and the optical system, chromatic aberration is facilitated to be improved. Preferably, 0.5 ≦ f234/f2 ≦ 1.9.
In this embodiment, an on-axis distance TTL from the object side surface of the first lens to the imaging surface of the optical imaging lens group and a distance SD from the stop of the optical imaging lens group to the image side surface of the fourth lens satisfy: 2.0 ≦ TTL/SD ≦ 3.5. The arrangement can reduce the processing difficulty and simultaneously ensure that the assembly of the optical imaging lens group has higher stability. Preferably, 2.3 ≦ TTL/SD ≦ 3.3.
In this embodiment, a distance BFL on the optical axis from the image-side surface of the fourth lens to the imaging surface of the optical imaging lens group, and a sum Σ CT of center thicknesses of all lenses on the optical axis satisfy: 2.0 ≦ BFL/Σ CT ≦ 3.0. Reasonable size layout ensures that the optical imaging lens group has longer back focus. Preferably, 2.1 ≦ BFL/Σ CT ≦ 3.0.
In the present embodiment, the effective focal length f1 of the first lens and the effective focal length f4 of the fourth lens satisfy: 0 ≦ f1/f4 ≦ 0.6. The focal power of the first lens and the focal power of the fourth lens are reasonably controlled, the optical sensitivity of the first lens and the optical sensitivity of the fourth lens are effectively reduced, and the mass production is more favorably realized. Preferably, 0.2 ≦ f1/f4 ≦ 0.6.
Example two
As shown in fig. 1 to 32, the optical imaging lens group includes, in order from an object side to an image side along an optical axis, a diaphragm, a first lens, a second lens, a third lens, and a fourth lens, the second lens having a negative power; the fourth lens has positive focal power; the distance TD on the axis from the object side surface of the first lens to the image side surface of the fourth lens and the distance BFL on the optical axis from the image side surface of the fourth lens to the imaging surface of the optical imaging lens group satisfy that: 0.5 ≦ TD/BFL ≦ 1.0.
Through the reasonable distribution of the focal power of each lens, the aberration generated by the optical imaging lens group is favorably balanced, and the imaging quality of the optical imaging lens group is greatly improved. The ratio of the distance TD from the object side surface of the first lens to the image side surface of the fourth lens to the distance BFL from the image side surface of the fourth lens to the imaging surface of the optical imaging lens group on the optical axis is limited within a reasonable range, so that the optical imaging lens group is favorably ensured to have longer back focus, and the periscopic structural design can be met.
Preferably, an on-axis distance TD from the object-side surface of the first lens to the image-side surface of the fourth lens and a distance BFL from the image-side surface of the fourth lens to the imaging surface of the optical imaging lens group on the optical axis satisfy: 0.5 ≦ TD/BFL ≦ 0.9.
In the present embodiment, the effective focal length f of the optical imaging lens group, the effective focal length f1 of the first lens, and the effective focal length f2 of the second lens satisfy: 4.0 ≦ f/f1| + | f/f2| ≦ 5.0. By limiting the ranges of the effective focal length f of the optical imaging lens group, the effective focal length f1 of the first lens and the effective focal length f2 of the second lens, the reasonable distribution of focal power of each lens can be ensured, and the realization of small aberration of an optical system is facilitated. Preferably, 4.05 ≦ f/f1| + | f/f2| ≦ 4.9.
In the present embodiment, the effective focal length f1 of the first lens and the radius of curvature R1 of the object side surface of the first lens satisfy: 2.0 ≦ f1/R1 ≦ 3.0. By limiting the ratio of the effective focal length f1 of the first lens and the curvature radius R1 of the object side surface of the first lens, the optical imaging lens group can better balance aberration, and the resolution power of the optical imaging lens group can be improved. Preferably, 2.05 ≦ f1/R1 ≦ 2.6.
In the present embodiment, the effective focal length f2 of the second lens, the radius of curvature R3 of the object-side surface of the second lens, and the radius of curvature R4 of the image-side surface of the second lens satisfy: 0.7 ≦ (R3+ R4)/f2| ≦ 1.6. The arrangement is favorable for controlling the incident angle of the light rays of the off-axis field of view on the image plane, and the matching performance of the light rays with the photosensitive element and the band-pass filter is improved. Preferably, 0.8 ≦ l (R3+ R4)/f2| ≦ 1.55.
In the present embodiment, the effective focal length f1 of the first lens, the radius of curvature R4 of the image-side surface of the second lens, and the radius of curvature R5 of the object-side surface of the third lens satisfy: 0 ≦ (R4+ R5)/f1 ≦ 2.0. By limiting the relationship among the effective focal length f1 of the first lens, the radius of curvature R4 of the image-side surface of the second lens, and the radius of curvature R5 of the object-side surface of the third lens, optical distortion can be reduced, ensuring better imaging quality. Preferably, 0.6 ≦ (R4+ R5)/f1 ≦ 1.8.
In the present embodiment, the central thickness CT1 of the first lens on the optical axis, the central thickness CT2 of the second lens on the optical axis, the central thickness CT3 of the third lens on the optical axis, the central thickness CT4 of the fourth lens on the optical axis, and the air interval T12 of the first lens and the second lens on the optical axis satisfy: 0.5 ≦ (CT1+ CT2+ T12)/(CT3+ CT4) ≦ 1.4. The optical lens has good processing characteristics and is convenient to process and manufacture each lens by limiting the relation among the central thickness CT1 of the first lens on the optical axis, the central thickness CT2 of the second lens on the optical axis, the central thickness CT3 of the third lens on the optical axis, the central thickness CT4 of the fourth lens on the optical axis and the air interval T12 of the first lens and the second lens on the optical axis. Preferably, 0.8 ≦ (CT1+ CT2+ T12)/(CT3+ CT4) ≦ 1.35.
In the present embodiment, the combined focal length f234 of the second lens, the third lens, and the fourth lens, and the effective focal length f2 of the second lens satisfy: 0.5 ≦ f234/f2 ≦ 2.0. By controlling the effective focal length of the second lens and the optical system, chromatic aberration is facilitated to be improved. Preferably, 0.5 ≦ f234/f2 ≦ 1.9.
In this embodiment, an on-axis distance TTL from the object side surface of the first lens to the imaging surface of the optical imaging lens group and a distance SD from the stop of the optical imaging lens group to the image side surface of the fourth lens satisfy: 2.0 ≦ TTL/SD ≦ 3.5. The arrangement can reduce the processing difficulty and simultaneously ensure that the assembly of the optical imaging lens group has higher stability. Preferably, 2.3 ≦ TTL/SD ≦ 3.3.
In this embodiment, a distance BFL on the optical axis from the image-side surface of the fourth lens to the imaging surface of the optical imaging lens group, and a sum Σ CT of center thicknesses of all lenses on the optical axis satisfy: 2.0 ≦ BFL/Σ CT ≦ 3.0. Reasonable size layout ensures that the optical imaging lens group has longer back focus. Preferably, 2.1 ≦ BFL/Σ CT ≦ 3.0.
In the present embodiment, the effective focal length f1 of the first lens and the effective focal length f4 of the fourth lens satisfy: 0 ≦ f1/f4 ≦ 0.6. The focal power of the first lens and the focal power of the fourth lens are reasonably controlled, the optical sensitivity of the first lens and the optical sensitivity of the fourth lens are effectively reduced, and the mass production is more favorably realized. Preferably, 0.2 ≦ f1/f4 ≦ 0.6.
Optionally, the optical imaging lens group may further include a filter for correcting color deviation and/or a protective glass for protecting a photosensitive element on an imaging surface.
The optical imaging lens group in the present application may employ a plurality of lenses, for example, four lenses as described above. 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 group 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 group is more beneficial to production and processing and can be suitable for portable electronic equipment such as smart phones. The optical imaging lens group has large aperture and large angle of view. 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 the optical imaging lens group can be varied to achieve the various results and advantages described in the present specification without departing from the claimed subject matter. For example, although four lenses are exemplified in the embodiment, the optical imaging lens group is not limited to include four lenses. The optical imaging lens group may also include other numbers of lenses, as desired.
Specific surface types, parameters of the optical imaging lens group applicable to the above embodiments are further described below with reference to the drawings.
It should be noted that any one of the following examples one to eight is applicable to all embodiments of the present application.
Example one
As shown in fig. 1 to 4, an optical imaging lens group of a first example of the present application is described, and fig. 1 shows a schematic structural view of the optical imaging lens group of the first example.
As shown in fig. 1, the optical imaging lens assembly, in order from an object side to an image side, comprises: stop STO, first lens E1, second lens E2, third lens E3, fourth lens E4, filter E5, and image plane S11.
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 refractive power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has positive refractive 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. Filter E5 has an object side S9 of the filter and an image side S10 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging plane S11.
In this example, the total effective focal length f of the optical imaging lens group is 26.98mm, and the maximum half field angle FOV of the optical imaging lens group is 6.11 ° and Fno of the optical imaging lens group is 4.15.
Table 1 shows a basic structural parameter table of an optical imaging lens group of example one, in which the units of the radius of curvature, thickness/distance, and focal length are all millimeters (mm).
Figure BDA0003029906630000081
TABLE 1
In example one, the object-side surface and the image-side surface of any one of the first lens element E1 to the fourth lens element E4 are aspheric, and the surface shape of each aspheric lens can be defined by, but is not limited to, the following aspheric formula:
Figure BDA0003029906630000091
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 gives the high-order coefficient A4, A6, A8, A10 that may be used for each of the aspherical mirror surfaces S1-S8 in example one.
Flour mark A4 A6 A8 A10
S5 -1.4320E-03 -8.6831E-05 -2.1663E-05 0.0000E+00
S6 6.3476E-04 -9.5966E-05 -3.1557E-05 0.0000E+00
S7 8.9112E-04 -6.6172E-05 1.0024E-05 1.2424E-07
S8 -2.1448E-04 -6.1490E-05 1.4412E-06 4.9673E-07
TABLE 2
Fig. 2 shows an on-axis chromatic aberration curve of the optical imaging lens group of example one, which represents a convergent focus deviation of light rays of different wavelengths after passing through the optical imaging lens group. Fig. 3 shows astigmatism curves of the optical imaging lens group of the first example, which represent meridional field curvature and sagittal field curvature. Fig. 4 shows distortion curves of the optical imaging lens group of example one, which indicate distortion magnitude values corresponding to different angles of view.
As can be seen from fig. 2 to 4, the optical imaging lens group given in the first example can achieve good imaging quality.
Example two
As shown in fig. 5 to 8, an optical imaging lens group of example two of the present application is described. In this example and the following examples, descriptions of parts similar to example two will be omitted for the sake of brevity. Fig. 5 shows a schematic view of the optical imaging lens group of example two.
As shown in fig. 5, the optical imaging lens assembly, in order from an object side to an image side, comprises: stop STO, first lens E1, second lens E2, third lens E3, fourth lens E4, filter E5, and image plane S11.
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 refractive power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has negative refractive 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 convex. Filter E5 has an object side S9 of the filter and an image side S10 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging plane S11.
In this example, the total effective focal length f of the optical imaging lens group is 26.99mm, and the maximum half field angle FOV of the optical imaging lens group is 6.12 ° and Fno of the optical imaging lens group is 4.15.
Table 3 shows a basic structural parameter table of the optical imaging lens group of example two, in which the units of the radius of curvature, thickness/distance, and focal length are all millimeters (mm).
Figure BDA0003029906630000101
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 two above.
Flour mark A4 A6 A8 A10
S5 -1.7893E-03 -1.1466E-04 -9.2100E-06 0.0000E+00
S6 -2.7058E-03 -3.2368E-04 -4.0632E-05 0.0000E+00
S7 1.6726E-04 1.4995E-04 -6.4341E-05 6.8410E-06
S8 -5.8424E-04 1.5201E-04 -6.5983E-05 6.6284E-06
TABLE 4
Fig. 6 shows an on-axis chromatic aberration curve of the optical imaging lens group of example two, which represents a convergent focus deviation of light rays of different wavelengths after passing through the optical imaging lens group. Fig. 7 shows astigmatism curves of the optical imaging lens group of example two, which represent meridional field curvature and sagittal field curvature. Fig. 8 shows distortion curves of the optical imaging lens group of example two, which indicate values of distortion magnitudes corresponding to different angles of view.
As can be seen from fig. 6 to 8, the optical imaging lens group given in example two can achieve good imaging quality.
Example III
As shown in fig. 9 to 12, an optical imaging lens group of example three of the present application is described. In this example and the following examples, descriptions of parts similar to example three will be omitted for the sake of brevity. Fig. 9 shows a schematic view of the optical imaging lens group of example three.
As shown in fig. 9, the optical imaging lens assembly, in order from an object side to an image side, comprises: stop STO, first lens E1, second lens E2, third lens E3, fourth lens E4, filter E5, and image plane S11.
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 refractive power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has negative refractive 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 convex. Filter E5 has an object side S9 of the filter and an image side S10 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging plane S11.
In this example, the total effective focal length f of the optical imaging lens group is 26.99mm, and the maximum half field angle FOV of the optical imaging lens group is 6.13 ° and Fno of the optical imaging lens group is 3.90.
Table 5 shows a basic structural parameter table of the optical imaging lens group of example three, in which the units of the radius of curvature, thickness/distance, and focal length are all millimeters (mm).
Figure BDA0003029906630000111
TABLE 5
Table 6 shows the high-order term coefficients that can be used for each aspherical mirror surface in example three, wherein each aspherical mirror surface type can be defined by formula (1) given in example three above.
Figure BDA0003029906630000112
Figure BDA0003029906630000121
TABLE 6
Fig. 10 shows on-axis chromatic aberration curves of the optical imaging lens group of example three, which represent the convergent focus deviations of light rays of different wavelengths after passing through the optical imaging lens group. Fig. 11 shows astigmatism curves of the optical imaging lens group of example three, which represent meridional field curvature and sagittal field curvature. Fig. 12 shows distortion curves of the optical imaging lens group of example three, which represent distortion magnitude values corresponding to different angles of view.
As can be seen from fig. 10 to 12, the optical imaging lens group given in example three can achieve good imaging quality.
Example four
As shown in fig. 13 to 16, an optical imaging lens group of example four of the present application is described. In this example and the following examples, descriptions of parts similar to example four will be omitted for the sake of brevity. Fig. 13 shows a schematic view of the optical imaging lens group of example four.
As shown in fig. 13, the optical imaging lens assembly, in order from an object side to an image side, comprises: stop STO, first lens E1, second lens E2, third lens E3, fourth lens E4, filter E5, and image plane S11.
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 convex. The second lens element E2 has negative refractive power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has negative refractive 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 convex. Filter E5 has an object side S9 of the filter and an image side S10 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging plane S11.
In this example, the total effective focal length f of the optical imaging lens group is 27.01mm, and the maximum half field angle FOV of the optical imaging lens group is 6.11 ° and Fno of the optical imaging lens group is 4.16.
Table 7 shows a basic structural parameter table of the optical imaging lens group of example four, in which the units of the radius of curvature, thickness/distance, and focal length are all millimeters (mm).
Figure BDA0003029906630000122
Figure BDA0003029906630000131
TABLE 7
Table 8 shows the high-order term coefficients that can be used for each aspherical mirror surface in example four, wherein each aspherical mirror surface type can be defined by formula (1) given in example four above.
Flour mark A4 A6 A8 A10
S5 -2.5724E-03 -8.4059E-05 1.5908E-06 0.0000E+00
S6 -2.3319E-03 -1.4013E-04 1.4963E-05 0.0000E+00
S7 1.7603E-03 -2.9137E-05 2.8887E-05 2.4601E-07
S8 9.4865E-04 4.7840E-07 1.3992E-05 1.6492E-06
TABLE 8
Fig. 14 shows on-axis chromatic aberration curves of the optical imaging lens group of example four, which represent convergent focus deviations of light rays of different wavelengths after passing through the optical imaging lens group. Fig. 15 shows astigmatism curves of the optical imaging lens group of example four, which represent meridional field curvature and sagittal field curvature. Fig. 16 shows distortion curves of the optical imaging lens group of example four, which represent distortion magnitude values corresponding to different angles of view.
As can be seen from fig. 14 to 16, the optical imaging lens group given in example four can achieve good imaging quality.
Example five
As shown in fig. 17 to 20, an optical imaging lens group of example five of the present application is described. In this example and the following examples, descriptions of parts similar to example five will be omitted for the sake of brevity. Fig. 17 shows a schematic view of the optical imaging lens group structure of example five.
As shown in fig. 17, the optical imaging lens assembly, in order from an object side to an image side, comprises: stop STO, first lens E1, second lens E2, third lens E3, fourth lens E4, filter E5, and image plane S11.
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 convex. The second lens element E2 has negative refractive power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has negative refractive 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. Filter E5 has an object side S9 of the filter and an image side S10 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging plane S11.
In this example, the total effective focal length f of the optical imaging lens group is 27.01mm, and the maximum half field angle FOV of the optical imaging lens group is 6.11 ° and Fno of the optical imaging lens group is 4.16.
Table 9 shows a basic structural parameter table of the optical imaging lens group of example five, in which the units of the radius of curvature, thickness/distance, and focal length are all millimeters (mm).
Figure BDA0003029906630000141
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 five above.
Flour mark A4 A6 A8 A10
S5 -2.1412E-03 -9.8681E-05 4.7163E-08 0.0000E+00
S6 -1.1857E-03 -1.4764E-04 2.4755E-05 0.0000E+00
S7 -5.5697E-04 -3.6139E-05 -4.4463E-07 -2.3778E-07
S8 -1.0841E-03 -4.5632E-05 -4.3826E-06 -2.2404E-07
Watch 10
Fig. 18 shows an on-axis chromatic aberration curve of an optical imaging lens group of example five, which represents a convergent focus deviation of light rays of different wavelengths after passing through the optical imaging lens group. Fig. 19 shows astigmatism curves of the optical imaging lens group of example five, which represent meridional field curvature and sagittal field curvature. Fig. 20 shows distortion curves of the optical imaging lens group of example five, which represent distortion magnitude values corresponding to different angles of view.
As can be seen from fig. 18 to 20, the optical imaging lens group given in example five can achieve good imaging quality.
Example six
As shown in fig. 21 to 24, an optical imaging lens group of example six of the present application is described. In this example and the following examples, descriptions of portions similar to example six will be omitted for the sake of brevity. Fig. 21 shows a schematic view of the optical imaging lens group of example six.
As shown in fig. 21, the optical imaging lens assembly, in order from an object side to an image side, comprises: stop STO, first lens E1, second lens E2, third lens E3, fourth lens E4, filter E5, and image plane S11.
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 refractive power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has negative refractive 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. Filter E5 has an object side S9 of the filter and an image side S10 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging plane S11.
In this example, the total effective focal length f of the optical imaging lens group is 26.99mm, and the maximum half field angle FOV of the optical imaging lens group is 6.12 ° and Fno of the optical imaging lens group is 4.15.
Table 11 shows a basic structural parameter table of the optical imaging lens group of example six, in which the units of the radius of curvature, thickness/distance, and focal length are all millimeters (mm).
Figure BDA0003029906630000151
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 six above.
Flour mark A4 A6 A8 A10
S5 -1.8299E-03 -1.2314E-04 -1.1671E-05 0.0000E+00
S6 -2.4613E-03 -3.3168E-04 -5.1476E-05 0.0000E+00
S7 1.9411E-04 1.1257E-04 -6.0872E-05 5.9296E-06
S8 -7.2208E-04 9.5347E-05 -5.6586E-05 4.9770E-06
TABLE 12
Fig. 22 shows an on-axis chromatic aberration curve of an optical imaging lens group of example six, which represents a convergent focus deviation of light rays of different wavelengths after passing through the optical imaging lens group. Fig. 23 shows astigmatism curves of the optical imaging lens group of example six, which represent meridional field curvature and sagittal field curvature. Fig. 24 shows distortion curves of the optical imaging lens group of example six, which represent distortion magnitude values corresponding to different angles of view.
As can be seen from fig. 22 to 24, the optical imaging lens group given in example six can achieve good imaging quality.
Example seven
As shown in fig. 25 to 28, an optical imaging lens group of example seven of the present application is described. In this example and the following examples, a description of portions similar to example seven will be omitted for the sake of brevity. Fig. 25 shows a schematic view of the optical imaging lens group structure of example seven.
As shown in fig. 25, the optical imaging lens assembly, in order from an object side to an image side, comprises: stop STO, first lens E1, second lens E2, third lens E3, fourth lens E4, filter E5, and image plane S11.
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 refractive power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has negative refractive 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. Filter E5 has an object side S9 of the filter and an image side S10 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging plane S11.
In this example, the total effective focal length f of the optical imaging lens group is 27mm, and the maximum half field angle FOV of the optical imaging lens group is 6.13 ° and Fno of the optical imaging lens group is 4.15.
Table 13 shows a basic structural parameter table of the optical imaging lens group of example seven, in which the units of the radius of curvature, thickness/distance, and focal length are all millimeters (mm).
Figure BDA0003029906630000161
Watch 13
Table 14 shows the high-order term coefficients that can be used for each aspherical mirror surface in example seven, wherein each aspherical mirror surface type can be defined by formula (1) given in example seven above.
Flour mark A4 A6 A8 A10
S5 -2.3818E-03 -1.5882E-04 -4.1301E-06 0.0000E+00
S6 -3.3905E-03 -3.8120E-04 1.1775E-06 0.0000E+00
S7 1.6357E-03 -4.0640E-05 2.2624E-05 1.2024E-07
S8 1.2635E-03 -6.3953E-06 1.3387E-05 1.2619E-06
TABLE 14
Fig. 26 shows an on-axis chromatic aberration curve of an optical imaging lens group of example seven, which represents a convergent focus deviation of light rays of different wavelengths after passing through the optical imaging lens group. Fig. 27 shows astigmatism curves of the optical imaging lens group of example seven, which represent meridional field curvature and sagittal field curvature. Fig. 28 shows distortion curves of the optical imaging lens group of example seven, which represent distortion magnitude values corresponding to different angles of view.
As can be seen from fig. 26 to 28, the optical imaging lens group given in example seven can achieve good imaging quality.
Example eight
As shown in fig. 29 to 32, an optical imaging lens group of example eight of the present application is described. In this example and the following examples, descriptions of portions similar to example eight will be omitted for the sake of brevity. Fig. 29 shows a schematic view of an optical imaging lens group configuration of example eight.
As shown in fig. 29, the optical imaging lens assembly, in order from an object side to an image side, comprises: stop STO, first lens E1, second lens E2, third lens E3, fourth lens E4, filter E5, and image plane S11.
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 refractive power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has negative refractive 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 convex. Filter E5 has an object side S9 of the filter and an image side S10 of the filter. The light from the object sequentially passes through the respective surfaces S1 to S10 and is finally imaged on the imaging plane S11.
In this example, the total effective focal length f of the optical imaging lens group is 26.99mm, and the maximum half field angle FOV of the optical imaging lens group is 6.13 ° and Fno of the optical imaging lens group is 4.15.
Table 15 shows a basic structural parameter table of the optical imaging lens group of example eight, in which the units of the radius of curvature, thickness/distance, and focal length are all millimeters (mm).
Figure BDA0003029906630000171
Figure BDA0003029906630000181
Watch 15
Table 16 shows the high-order term coefficients that can be used for each aspherical mirror surface in example eight, wherein each aspherical mirror surface type can be defined by formula (1) given in example eight above.
Flour mark A4 A6 A8 A10
S5 -2.1453E-03 -1.5272E-04 -1.0499E-05 0.0000E+00
S6 -2.7869E-03 -3.9382E-04 -3.8479E-05 0.0000E+00
S7 1.9312E-04 2.4344E-05 -2.8581E-05 3.5514E-06
S8 -5.6058E-04 3.5177E-05 -3.1522E-05 3.4423E-06
TABLE 16
Fig. 30 shows on-axis chromatic aberration curves of the optical imaging lens group of example eight, which represent convergent focus deviations of light rays of different wavelengths after passing through the optical imaging lens group. Fig. 31 shows astigmatism curves of the optical imaging lens group of example eight, which represent meridional field curvature and sagittal field curvature. Fig. 32 shows distortion curves of the optical imaging lens group of example eight, which represent distortion magnitude values corresponding to different angles of view.
As can be seen from fig. 30 to 32, the optical imaging lens group given in example eight can achieve good imaging quality.
To sum up, examples one to eight satisfy the relationships shown in table 17, respectively.
Figure BDA0003029906630000182
Figure BDA0003029906630000191
TABLE 17
Table 18 gives the effective focal lengths f, f1 to f4, and the maximum half field angle FOV of the optical imaging lens groups of examples one to eight.
Example parameters 1 2 3 4 5 6 7 8
f 26.98 26.99 26.99 27.01 27.01 26.99 27.00 26.99
f1 13.09 11.65 11.38 9.70 9.68 11.24 10.71 11.20
f2 -9.83 -13.90 -13.76 -20.93 -19.15 -13.51 -14.44 -13.28
f3 55.83 -39.02 -37.33 -11.67 -13.40 -38.06 -25.78 -34.97
f4 24.46 25.75 27.76 28.37 33.76 27.17 29.78 26.25
TTL 24.00 24.00 24.00 24.00 24.00 24.00 24.00 24.00
ImgH 2.90 2.90 2.90 2.90 2.90 2.90 2.90 2.90
Semi-FOV 6.11 6.12 6.13 6.11 6.11 6.12 6.13 6.13
Fno 4.15 4.15 3.90 4.16 4.16 4.15 4.15 4.15
Watch 18
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 group described above.
It is obvious that the above described embodiments are only some of the embodiments of the present invention, and not all of them. Based on the embodiments in the present invention, all other embodiments obtained by a person skilled in the art without creative efforts shall belong to 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 assembly, comprising, in order from an object side to an image side along an optical axis:
a diaphragm;
a first lens having a positive optical power;
a second lens;
a third lens;
a fourth lens having a positive optical power;
wherein a maximum field angle FOV of the optical imaging lens group satisfies: FOV < 20.
2. The optical imaging lens group of claim 1, wherein the effective focal length f of the optical imaging lens group, the effective focal length f1 of the first lens, and the effective focal length f2 of the second lens are such that: 4.0 ≦ f/f1| + | f/f2| ≦ 5.0.
3. The optical imaging lens group of claim 1, wherein the effective focal length f1 of the first lens and the radius of curvature of the object-side surface of the first lens satisfy: 2.0 ≦ f1/R1 ≦ 3.0.
4. The optical imaging lens group of claim 1, wherein the effective focal length f2 of the second lens, the radius of curvature R3 of the object side surface of the second lens, and the radius of curvature R4 of the image side surface of the second lens are such that: 0.7 ≦ (R3+ R4)/f2| ≦ 1.6.
5. The optical imaging lens group of claim 1, wherein an effective focal length f1 of the first lens, a radius of curvature R4 of an image-side surface of the second lens, and a radius of curvature R5 of an object-side surface of the third lens are satisfied: 0 ≦ (R4+ R5)/f1 ≦ 2.0.
6. The optical imaging lens group of claim 1, wherein a center thickness CT1 of the first lens on the optical axis, a center thickness CT2 of the second lens on the optical axis, a center thickness CT3 of the third lens on the optical axis, a center thickness CT4 of the fourth lens on the optical axis, and an air space T12 of the first and second lenses on the optical axis satisfy: 0.5 ≦ (CT1+ CT2+ T12)/(CT3+ CT4) ≦ 1.4.
7. The optical imaging lens group of claim 1, wherein a combined focal length f234 of the second lens, the third lens and the fourth lens, an effective focal length f2 of the second lens, satisfies: 0.5 ≦ f234/f2 ≦ 2.0.
8. The optical imaging lens group of claim 1, wherein an on-axis distance TTL from an object side surface of the first lens to an imaging surface of the optical imaging lens group and a distance SD from a stop of the optical imaging lens group to an image side surface of the fourth lens satisfy: 2.0 ≦ TTL/SD ≦ 3.5.
9. The optical imaging lens group of claim 1, wherein a distance BFL on the optical axis from an image side surface of the fourth lens to an image surface of the optical imaging lens group, a sum Σ CT of center thicknesses of all lenses on the optical axis satisfies: 2.0 ≦ BFL/Σ CT ≦ 3.0.
10. The optical imaging lens group of claim 1, wherein an effective focal length f1 of the first lens and an effective focal length f4 of the fourth lens satisfy: 0 ≦ f1/f4 ≦ 0.6.
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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115166943A (en) * 2022-07-18 2022-10-11 歌尔光学科技有限公司 Optical system and augmented reality equipment
WO2023185942A1 (en) * 2022-03-31 2023-10-05 华为技术有限公司 Telephoto lens, camera module and electronic device

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2023185942A1 (en) * 2022-03-31 2023-10-05 华为技术有限公司 Telephoto lens, camera module and electronic device
CN115166943A (en) * 2022-07-18 2022-10-11 歌尔光学科技有限公司 Optical system and augmented reality equipment
CN115166943B (en) * 2022-07-18 2024-03-12 歌尔光学科技有限公司 Optical system and augmented reality device

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