CN117008302B

CN117008302B - Optical lens

Info

Publication number: CN117008302B
Application number: CN202311278112.9A
Authority: CN
Inventors: 张力瑶; 章彬炜
Original assignee: Jiangxi Lianyi Optics Co Ltd
Current assignee: Jiangxi Lianyi Optics Co Ltd
Priority date: 2023-10-07
Filing date: 2023-10-07
Publication date: 2024-02-20
Anticipated expiration: 2043-10-07
Also published as: CN117008302A

Abstract

The present invention provides an optical lens comprising, in order from an object side to an imaging surface along an optical axis: the first lens with negative focal power has a convex object side surface and a concave image side surface; a second lens having negative optical power, the image side surface of which is concave; the object side surface of the third lens is a concave surface, and the image side surface of the third lens is a convex surface; a fourth lens element with positive refractive power having a convex object-side surface and a convex image-side surface; a fifth lens having negative optical power; a sixth lens element with positive refractive power having a convex object-side surface and a convex image-side surface at a paraxial region; wherein the maximum field angle FOV of the optical lens and the f-number FNO of the optical lens satisfy: 150 DEG < FOV/FNO < 180 deg. The optical lens provided by the invention has the advantages of large aperture, small size, large field angle and high resolution.

Description

Optical lens

Technical Field

The invention relates to the technical field of imaging lenses, in particular to an optical lens.

Background

With the rapid development of unmanned aerial vehicle, security protection, automobile, weather, medical treatment, VR, AR and other fields, the field angle of view of the wide-angle lens carried by the lens also provides higher and higher requirements. By introducing barrel distortion, the wide-angle lens can compress marginal view field rays as much as possible, and can obtain an ultra-wide-angle lens with a view field angle exceeding 218 degrees. However, the ultra-wide angle lens still has many problems such as small aperture, large difficulty in aberration correction, oversized head, and the like.

Disclosure of Invention

Based on the above technical problems, an object of the present invention is to provide an optical lens, which has at least the advantages of super-large field angle, large aperture and miniaturization.

To this end, the present invention proposes an optical lens comprising, in order from an object side to an imaging surface along an optical axis: the first lens with negative focal power has a convex object side surface and a concave image side surface; a second lens having negative optical power, the image side surface of which is concave; the object side surface of the third lens is a concave surface, and the image side surface of the third lens is a convex surface; a fourth lens element with positive refractive power having a convex object-side surface and a convex image-side surface; a fifth lens having negative optical power; a sixth lens element with positive refractive power having a convex object-side surface and a convex image-side surface at a paraxial region; wherein the maximum field angle FOV of the optical lens and the f-number FNO of the optical lens satisfy: 150 DEG < FOV/FNO < 180 deg.

Compared with the prior art, the optical lens provided by the invention has reasonable focal power distribution, diaphragm position, lens thickness and lens interval arrangement, so that the optical lens has a compact large aperture structure, and more luminous flux can enter the optical lens, so that the optical lens can be clearly imaged in a dim environment, and the effects of ultra-large field of view, large aperture and miniaturization are realized.

Drawings

Fig. 1 is a schematic structural diagram of an optical lens according to a first embodiment of the present invention.

Fig. 2 is a distortion graph of an optical lens according to a first embodiment of the present invention.

Fig. 3 is a graph showing a field curvature of an optical lens according to a first embodiment of the present invention.

Fig. 4 is a vertical axis chromatic aberration diagram of an optical lens according to a first embodiment of the present invention.

Fig. 5 is an axial chromatic aberration diagram of an optical lens according to a first embodiment of the present invention.

Fig. 6 is a schematic structural diagram of an optical lens according to a second embodiment of the present invention.

Fig. 7 is a distortion graph of an optical lens according to a second embodiment of the present invention.

Fig. 8 is a field curvature chart of an optical lens according to a second embodiment of the present invention.

Fig. 9 is a vertical axis chromatic aberration diagram of an optical lens according to a second embodiment of the present invention.

Fig. 10 is an axial chromatic aberration diagram of an optical lens according to a second embodiment of the present invention.

Fig. 11 is a schematic structural diagram of an optical lens according to a third embodiment of the present invention.

Fig. 12 is a distortion graph of an optical lens according to a third embodiment of the present invention.

Fig. 13 is a field curve diagram of an optical lens according to a third embodiment of the present invention.

Fig. 14 is a vertical axis chromatic aberration diagram of an optical lens according to a third embodiment of the present invention.

Fig. 15 is an axial chromatic aberration diagram of an optical lens according to a third embodiment of the present invention.

Detailed Description

In order that the objects, features and advantages of the invention will be readily understood, a more particular description of the invention will be rendered by reference to specific embodiments thereof which are illustrated in the appended drawings. Several embodiments of the invention are presented in the figures. This invention may, however, be embodied in many different forms and should not be construed as limited to the embodiments set forth herein. Rather, these embodiments are provided so that this disclosure will be thorough and complete.

Unless defined otherwise, 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 invention belongs. The terminology used in the description of the invention herein is for the purpose of describing particular embodiments only and is not intended to be limiting of the invention. Like reference numerals refer to like elements throughout the specification.

The invention provides an optical lens, which sequentially comprises from an object side to an imaging surface along an optical axis: the optical centers of the first lens, the second lens, the third lens, the diaphragm, the fourth lens, the fifth lens, the sixth lens and the optical filter are positioned on the same straight line.

Specifically, the first lens has negative focal power, the object side surface of the first lens is a convex surface, and the image side surface of the first lens is a concave surface; the second lens has negative focal power, the object side surface of the second lens is a concave surface at a paraxial region, and the image side surface of the second lens is a concave surface; the third lens has positive focal power, the object side surface of the third lens is a concave surface, and the image side surface of the third lens is a convex surface; the fourth lens has positive focal power, the object side surface of the fourth lens is a convex surface, and the image side surface of the fourth lens is a convex surface; the fifth lens has negative focal power, the object side surface of the fifth lens is a concave surface, and the image side surface of the fifth lens is a concave surface; the sixth lens element has positive refractive power, wherein an object-side surface of the sixth lens element is convex, and an image-side surface of the sixth lens element is convex at a paraxial region. Wherein the first lens is a glass spherical lens, and the second lens to the sixth lens are plastic aspherical lenses.

In some embodiments, the maximum field angle FOV of the optical lens and the f-number FNO of the optical lens satisfy: 150 DEG < FOV/FNO < 180 deg. The optical lens meets the range, is beneficial to expanding the field angle of the optical lens and enlarging the aperture of the optical lens, and realizes the balance of the ultra-large field angle and the large aperture.

In some embodiments, the image height IH corresponding to the maximum field angle of the optical lens and the pupil diameter EPD of the optical lens satisfy: 4.5 < IH/EPD < 5.5. The method meets the range, is favorable for balancing the relative illumination of the image surface and the edge view field, and realizes the balance of large view field, large aperture and miniaturization.

In some embodiments, the combined focal length f12 of the first lens and the second lens and the effective focal length f3 of the third lens satisfy: -0.2 < f12/f3 < -0.05. The optical system has the advantages that the range is met, the focal lengths of the first lens, the second lens and the third lens are reasonably matched, the incident light rays with the ultra-large angles are converted into light rays with small angles in the optical system, the curvature of field and distortion of the system can be well corrected, and the imaging quality is improved.

In some embodiments, the effective focal length f3 of the third lens and the effective focal length f4 of the fourth lens satisfy: 4.0 < f3/f4 < 10.0. The optical power of the third lens and the optical power of the fourth lens are reasonably matched, so that the vertical axis chromatic aberration of off-axis light can be well corrected, and meanwhile, the coma aberration and the field curvature can be corrected, and the eccentric sensitivity of the lens is reduced.

In some embodiments, the combined focal length f45 of the fourth lens and the fifth lens and the effective focal length f of the optical lens satisfy: -13.0 < f45/f < -8.0.

The optical lens has the advantages that the range is met, the focal length of the fourth lens and the focal length of the fifth lens are reasonably matched, the advanced spherical aberration of the optical lens can be well controlled, the field curvature of the optical lens can be reduced, and the imaging quality of the optical lens can be better improved.

In some embodiments, the effective focal length f3 of the third lens and the effective focal length f6 of the sixth lens satisfy: 4.5 < f3/f6 < 9.0. The lens has the advantages that the lens can be guaranteed in processability by reasonably controlling the focal power of the third lens and the focal power of the sixth lens, meanwhile, the turning trend of incident light can be reduced, the incident light can be made to have a smaller incident angle to the image plane, and the chip receiving efficiency is improved.

In some embodiments, the radius of curvature R21 of the second lens object-side surface and the radius of curvature R22 of the second lens image-side surface satisfy: -11.0 < R21/R22 < -2.0; the radius of curvature R31 of the third lens object-side surface and the radius of curvature R32 of the third lens image-side surface satisfy: R31/R32 is more than 1.0 and less than 2.0. The optical lens can well correct the aberration of the optical lens and improve the imaging quality of the optical lens.

In some embodiments, the air space AT12 on the optical axis of the first lens and the second lens, the air space AT23 on the optical axis of the second lens and the third lens, and the air space AT34 on the optical axis of the third lens and the fourth lens satisfy: 4.8 < (AT12+AT23)/AT 34 < 6.5. The axial spherical aberration correction device meets the requirements of the range, and can better correct axial spherical aberration by reasonably limiting the distance between the second lens, the third lens and the front lens and the rear lens, so that point light sources are prevented from being imaged into large light spots, and the imaging quality is improved.

In some embodiments, a sum Σat of air gaps on the optical axis between adjacent lenses of the first lens to the sixth lens, a sum Σct of lens center thicknesses of the first lens to the sixth lens satisfies: sigma AT/Sigma CT 0.58 < 0.65. The lens has the advantages that the range is met, the interval between lenses and the thickness of the lenses are reasonably controlled, the coma and the spherical aberration of the optical lens can be well balanced while the manufacturability of the lenses is met, and the imaging quality and the miniaturization of the optical lens are guaranteed.

In some embodiments, the radius of curvature R21 of the second lens object-side surface and the effective focal length f of the optical lens satisfy:. The lens meets the range, is favorable for slowing down the shape change of the second lens, reduces the sensitivity of the system, can improve the formability of the lens and improves the manufacturing yield.

In some embodiments, the aperture value FNO of the optical lens satisfies: FNO is more than 1.2 and less than 1.4. The range is satisfied, the large aperture characteristic is realized, and the definition of the image can be ensured in a low-light environment or at night.

In some embodiments, the effective focal length f of the optical lens and the total optical length TTL of the optical lens satisfy: f/TTL is more than 0.05 and less than 0.1. The optical lens meets the above range, is beneficial to controlling the focal length of the optical lens in a shorter range while maintaining the miniaturization of the optical lens, and ensures that the optical lens has a larger depth of field.

In some embodiments, the radius of curvature R51 of the fifth lens object-side surface and the radius of curvature R52 of the fifth lens image-side surface satisfy: 0.5 < (R51+R52)/(R51-R52) < 1.0. The field curvature and distortion of the optical lens can be well modified by meeting the above range, and the field curvature and distortion of the optical lens are ensured to be controlled at a smaller level.

In some embodiments, the optical back focal length BFL of the optical lens and the effective focal length f of the optical lens satisfy: BFL/f is less than 1.5 and less than 2.0. The optical lens has larger optical back focus, thereby being beneficial to reducing interference between the lens and the imaging chip and reducing the correction difficulty of CRA.

In the embodiment of the invention, in order to better reduce the total length of the optical lens and increase the field angle of the optical lens, a combination of one glass lens and five plastic lenses is adopted, and the optical lens at least has the advantages of super-large field angle, good imaging quality, large aperture and miniaturization by reasonably distributing the focal power of each lens and optimizing the aspherical shape.

The invention is further illustrated in the following examples. In various embodiments, the thickness, radius of curvature, and material selection portion of each lens in the optical lens may vary, and for specific differences, reference may be made to the parameter tables of the various embodiments. The following examples are merely preferred embodiments of the present invention, but the embodiments of the present invention are not limited to the following examples, and any other changes, substitutions, combinations or simplifications that do not depart from the gist of the present invention are intended to be equivalent substitutes within the scope of the present invention.

In various embodiments of the present invention, when an aspherical lens is used as the lens, the surface shape of the aspherical lens satisfies the following equation:the method comprises the steps of carrying out a first treatment on the surface of the Where z is the distance sagittal height from the aspherical surface vertex when the aspherical surface is at a position of height h along the optical axis direction, c is the paraxial curvature of the surface, k is the conic coefficient conic, A _2i The aspherical surface profile coefficient of the 2 i-th order.

First embodiment

Referring to fig. 1, a schematic structural diagram of an optical lens 100 according to a first embodiment of the present invention is shown, where the optical lens 100 includes, in order from an object side to an imaging surface S15 along an optical axis: a first lens L1, a second lens L2, a third lens L3, a stop ST, a fourth lens L4, a fifth lens L5, a sixth lens L6, and a filter G1.

The first lens element L1 has a negative refractive power, wherein an object-side surface S1 of the first lens element is convex, and an image-side surface S2 of the first lens element is concave; the second lens element L2 has negative refractive power, wherein an object-side surface S3 of the second lens element is concave at a paraxial region thereof, and an image-side surface S4 of the second lens element is concave; the third lens element L3 with positive refractive power has a concave object-side surface S5 and a convex image-side surface S6; the fourth lens element L4 has positive refractive power, wherein an object-side surface S7 of the fourth lens element is convex, and an image-side surface S8 of the fourth lens element is convex; the fifth lens element L5 has negative refractive power, wherein an object-side surface S9 of the fifth lens element is concave, and an image-side surface S10 of the fifth lens element is concave; the sixth lens element L6 with positive refractive power has a convex object-side surface S11 and a convex image-side surface S12 at a paraxial region; the object side surface of the filter G1 is S13, and the image side surface is S14. The first lens L1 is a glass spherical lens, and the second lens L2, the third lens L3, the fourth lens L4, the fifth lens L5 and the sixth lens L6 are plastic aspherical lenses.

Specifically, the design parameters of the optical lens 100 provided in this embodiment are shown in table 1.

TABLE 1

The aspherical surface profile coefficients of the optical lens 100 in this embodiment are shown in table 2.

TABLE 2

In fig. 2, the curves represent distortions corresponding to different image heights on the image plane, the abscissa represents the distortion magnitude (unit:%) and the ordinate represents the half field angle (unit: °). As can be seen from fig. 2, the distortion of the optical lens is controlled within ±7.5% within the required imaging field of view of the optical lens, which means that the distortion of the optical lens is well corrected.

In fig. 3, the curves represent field curves of meridian and sagittal directions at different image heights of an image plane, the abscissa represents the offset (unit: mm), and the ordinate represents the half field angle (unit: °). As can be seen from fig. 3, the curvature of field offset in both the meridian direction and the sagittal direction at the image plane is controlled within ±0.06mm, which indicates that the curvature of field correction of the optical lens is good.

In fig. 4, the graph shows the vertical chromatic aberration at different image heights on the image plane for each wavelength with respect to the dominant wavelength, the abscissa shows the chromatic aberration value (unit: μm), and the ordinate shows the normalized half field angle. As can be seen from fig. 4, the chromatic aberration of each wavelength with respect to the center wavelength is controlled within ±2.8μm in different fields of view, indicating that the chromatic aberration of the optical lens on the vertical axis is well corrected.

In fig. 5, the graph shows the axial chromatic aberration of each wavelength on the optical axis of the image plane, the abscissa shows the chromatic aberration value (unit: mm), and the ordinate shows the normalized pupil radius. As can be seen from fig. 5, the chromatic aberration offset of the dominant wavelength at the zero pupil position is controlled within ±0.01mm, and the axial chromatic aberration of the shortest wavelength and the maximum wavelength is controlled within ±0.05mm, which indicates that the axial chromatic aberration correction of the optical lens is good.

Second embodiment

Referring to fig. 6, a schematic structural diagram of an optical lens 200 according to a second embodiment of the present invention is shown, and the optical lens 200 according to the present embodiment is substantially the same as the first embodiment described above, and the difference is mainly that the radius of curvature, the aspheric coefficients and the thickness of each lens surface are different.

Specifically, the design parameters of the optical lens 200 provided in this embodiment are shown in table 3.

TABLE 3 Table 3

The aspherical surface profile coefficients of the optical lens 200 in this embodiment are shown in table 4.

TABLE 4 Table 4

In the present embodiment, graphs of distortion, curvature of field, chromatic aberration of homeotropic axis, and chromatic aberration of axial direction of the optical lens 200 are shown in fig. 7, 8, 9, and 10, respectively. As can be seen from fig. 7, the distortion of the optical lens is controlled within ±6.5% within the required imaging field of view of the optical lens, indicating that the distortion of the optical lens is well corrected. As can be seen from fig. 8, the curvature of field offset in both the meridian direction and the sagittal direction at the image plane is controlled within ±0.18mm, indicating that the curvature of field correction of the optical lens is good. As can be seen from fig. 9, the chromatic aberration of each wavelength with respect to the center wavelength is controlled within ±2.0 μm in different fields of view, indicating that the chromatic aberration of the optical lens on the vertical axis is also well corrected. As can be seen from fig. 10, the chromatic aberration offset of the dominant wavelength at the zero pupil position is controlled within ±0.01mm, and the axial chromatic aberration of the shortest wavelength and the maximum wavelength is controlled within ±0.04mm, which indicates that the axial chromatic aberration correction of the optical lens is good.

Third embodiment

Referring to fig. 11, a schematic structural diagram of an optical lens 300 according to a third embodiment of the present invention is shown, and the optical lens 300 of the present embodiment is substantially the same as the first embodiment described above, and the difference is mainly that the radius of curvature, the aspheric coefficients and the thickness of each lens surface are different.

Specifically, the design parameters of the optical lens 300 provided in this embodiment are shown in table 5.

TABLE 5

The aspherical surface profile coefficients of the optical lens 300 in this embodiment are shown in table 6.

TABLE 6

In the present embodiment, graphs of distortion, curvature of field, chromatic aberration of homeotropic axis, and chromatic aberration of axial direction of the optical lens 300 are shown in fig. 12, 13, 14, and 15, respectively. As can be seen from fig. 12, the distortion of the optical lens is controlled within ±7.0% within the required imaging field of view of the optical lens, indicating that the distortion of the optical lens is well corrected. As can be seen from fig. 13, the curvature of field offset in both the meridian direction and the sagittal direction at the image plane is controlled within ±0.2mm, indicating that the curvature of field correction of the optical lens is good. As can be seen from fig. 14, the chromatic aberration of each wavelength with respect to the center wavelength is controlled within ±3.0 μm in different fields of view, indicating that the chromatic aberration of the optical lens on the vertical axis is also well corrected. As can be seen from fig. 15, the chromatic aberration offset of the dominant wavelength at the zero pupil position is controlled within ±0.01mm, and the axial chromatic aberration of the shortest wavelength and the maximum wavelength is controlled within ±0.05mm, which indicates that the axial chromatic aberration correction of the optical lens is good.

Referring to table 7, the optical characteristics of the optical lens provided in the above three embodiments, including the maximum field angle FOV, the total optical length TTL, the image height IH, the effective focal length f and the f-number FNO of the optical lens, and the related values corresponding to each of the above conditions are shown.

TABLE 7

In the description of the present specification, a description referring to terms "one embodiment," "some embodiments," "examples," "specific examples," or "some examples," etc., means that a particular feature, structure, material, or characteristic described in connection with the embodiment or example is included in at least one embodiment or example of the present invention. In this specification, schematic representations of the above terms do not necessarily refer to the same embodiments or examples. Furthermore, the particular features, structures, materials, or characteristics described may be combined in any suitable manner in any one or more embodiments or examples.

The above examples merely represent a few embodiments of the present invention, which are described in more detail and are not to be construed as limiting the scope of the present invention. It should be noted that it will be apparent to those skilled in the art that several variations and modifications can be made without departing from the spirit of the invention, which are all within the scope of the invention. Accordingly, the scope of the invention should be assessed as that of the appended claims.

Claims

1. An optical lens comprising six lenses in order from an object side to an imaging surface along an optical axis, comprising:

a first lens with negative focal power, wherein the object side surface of the first lens is a convex surface, and the image side surface of the first lens is a concave surface;

a second lens having negative optical power, an image side surface of the second lens being a concave surface;

a third lens with positive focal power, wherein the object side surface of the third lens is a concave surface, and the image side surface of the third lens is a convex surface;

a diaphragm;

a fourth lens element with positive refractive power, wherein the object-side surface of the fourth lens element is convex, and the image-side surface of the fourth lens element is convex;

a fifth lens having negative optical power;

a sixth lens element with positive refractive power having a convex object-side surface and a convex image-side surface at a paraxial region;

wherein, the maximum field angle FOV of the optical lens and the f-number FNO of the optical lens satisfy: 150 DEG < FOV/FNO < 180 DEG; the image height IH corresponding to the maximum field angle of the optical lens and the pupil diameter EPD of the optical lens satisfy the following conditions: 4.5 < IH/EPD < 5.5.

2. The optical lens according to claim 1, wherein the optical lens satisfies the following conditional expression:

-0.2＜f12/f3＜-0.05；

wherein f12 represents a combined focal length of the first lens and the second lens, and f3 represents an effective focal length of the third lens.

3. The optical lens according to claim 1, wherein the optical lens satisfies the following conditional expression:

4.0＜f3/f4＜10.0；

wherein f3 represents an effective focal length of the third lens, and f4 represents an effective focal length of the fourth lens.

4. The optical lens according to claim 1, wherein the optical lens satisfies the following conditional expression:

-13.0＜f45/f＜-8.0；

wherein f45 represents a combined focal length of the fourth lens and the fifth lens, and f represents an effective focal length of the optical lens.

5. The optical lens according to claim 1, wherein the optical lens satisfies the following conditional expression:

4.5＜f3/f6＜9.0；

wherein f3 represents an effective focal length of the third lens, and f6 represents an effective focal length of the sixth lens.

6. The optical lens according to claim 1, wherein the optical lens satisfies the following conditional expression:

-11.0＜R21/R22＜-2.0；

1.0＜R31/R32＜2.0；

wherein R21 represents a radius of curvature of the second lens object-side surface, R22 represents a radius of curvature of the second lens image-side surface, R31 represents a radius of curvature of the third lens object-side surface, and R32 represents a radius of curvature of the third lens image-side surface.

7. The optical lens according to claim 1, wherein the optical lens satisfies the following conditional expression:

4.8＜(AT12+AT23)/AT34＜6.5；

wherein AT12 represents an air space between the first lens and the second lens on the optical axis, AT23 represents an air space between the second lens and the third lens on the optical axis, and AT34 represents an air space between the third lens and the fourth lens on the optical axis.

8. The optical lens according to claim 1, wherein the optical lens satisfies the following conditional expression:

0.58＜∑AT/∑CT＜0.65；

wherein Σat represents the sum of air gaps on the optical axis between adjacent lenses of the first lens to the sixth lens, Σct represents the sum of thicknesses of the respective lens centers of the first lens to the sixth lens.

9. The optical lens according to claim 1, wherein the optical lens satisfies the following conditional expression:

8.0＜|R21/f|＜26.0；

wherein R21 represents the radius of curvature of the object side surface of the second lens, and f represents the effective focal length of the optical lens.