CN116908994A - optical lens - Google Patents
optical lens Download PDFInfo
- Publication number
- CN116908994A CN116908994A CN202310537417.0A CN202310537417A CN116908994A CN 116908994 A CN116908994 A CN 116908994A CN 202310537417 A CN202310537417 A CN 202310537417A CN 116908994 A CN116908994 A CN 116908994A
- Authority
- CN
- China
- Prior art keywords
- lens
- optical lens
- optical
- image
- focal length
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 248
- 238000003384 imaging method Methods 0.000 claims abstract description 76
- 238000000034 method Methods 0.000 claims abstract description 32
- 230000004075 alteration Effects 0.000 abstract description 76
- 238000010586 diagram Methods 0.000 description 20
- 230000009286 beneficial effect Effects 0.000 description 6
- 239000011521 glass Substances 0.000 description 6
- 230000001681 protective effect Effects 0.000 description 6
- 230000006835 compression Effects 0.000 description 5
- 238000007906 compression Methods 0.000 description 5
- 239000006059 cover glass Substances 0.000 description 5
- 230000008569 process Effects 0.000 description 5
- 210000001747 pupil Anatomy 0.000 description 5
- 238000001228 spectrum Methods 0.000 description 5
- 238000012546 transfer Methods 0.000 description 5
- 238000012937 correction Methods 0.000 description 4
- 230000014509 gene expression Effects 0.000 description 3
- 239000000463 material Substances 0.000 description 3
- 230000008901 benefit Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- 102100034112 Alkyldihydroxyacetonephosphate synthase, peroxisomal Human genes 0.000 description 1
- 101000799143 Homo sapiens Alkyldihydroxyacetonephosphate synthase, peroxisomal Proteins 0.000 description 1
- 238000000848 angular dependent Auger electron spectroscopy Methods 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
- 238000005286 illumination Methods 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 238000006467 substitution reaction Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/18—Optical objectives specially designed for the purposes specified below with lenses having one or more non-spherical faces, e.g. for reducing geometrical aberration
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Lenses (AREA)
Abstract
The application provides an optical lens, which comprises seven lenses in sequence 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; the object side surface of the second lens is a concave surface, and the image side surface of the second lens is a convex surface; a third lens having positive optical power; a diaphragm; a fourth lens element with positive refractive power having convex object-side and image-side surfaces; a fifth lens element with positive refractive power having convex object-side and image-side surfaces; a sixth lens element with negative refractive power having concave object-side and image-side surfaces; a seventh lens having positive optical power; an effective focal length f of the optical lens and a combined focal length f of the first lens to the third lens 13 The method meets the following conditions: 4.0<f 13 /f<20.0. The optical lens provided by the application improves the resolution of the optical lens, reduces the aberration and improves the imaging quality of the optical lens through reasonable configuration of the surface types of the lenses and reasonable collocation of the focal power.
Description
Technical Field
The application relates to the technical field of imaging lenses, in particular to an optical lens.
Background
Along with the continuous improvement of the requirements of people on driving experience, the vehicle-mounted application optical lens is increasingly used in intelligent driving, and the position of the vehicle-mounted optical lens in the related industries of automobiles is continuously improved.
Advanced Driving Assistance Systems (ADASs) play an important role in intelligent driving, and collect environmental information through various lenses in combination with sensors to ensure driving safety of drivers. In addition to the requirements of the optical lens for the conventional ADAS system, the optical lens is required to have a light, thin, short and small shape, high pixels, high resolution and other characteristics, and the optical lens is required to be capable of clearly imaging under the condition of low illumination, so that the development of an optical lens with good imaging effect is required.
Disclosure of Invention
In view of the foregoing, an object of the present application is to provide an optical lens having an advantage of excellent imaging quality.
The application provides an optical lens, which comprises seven lenses in sequence 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;
the object side surface of the second lens is a concave surface, and the image side surface of the second lens is a convex surface;
a third lens having positive optical power;
a diaphragm;
a fourth lens element with positive refractive power having convex object-side and image-side surfaces;
a fifth lens element with positive refractive power having convex object-side and image-side surfaces;
a sixth lens element with negative refractive power having concave object-side and image-side surfaces;
a seventh lens having positive optical power;
an effective focal length f of the optical lens and a combined focal length f of the first lens to the third lens 13 The method meets the following conditions: 4.0<f 13 /f<20.0；
An effective focal length f of the optical lens and a combined focal length f of the fourth lens to the seventh lens 47 The method meets the following conditions: 1.5<f 47 /f<3.0。
Further preferably, the optical total length TTL and the effective focal length f of the optical lens satisfy: 3.0< TTL/f <10.0.
Further preferably, the effective focal length f of the optical lens and the real image height IH corresponding to the maximum field angle satisfy: 1.0< IH/f <2.3.
Further preferably, the opticsThe maximum field angle FOV of the lens, the real image height IH corresponding to the maximum field angle and the light transmission caliber D of the first lens object side surface 1 The three parts are as follows: d is 0.8 < 1 /IH/tan(FOV/2)＜2.8。
Further preferably, the effective focal length f of the optical lens is equal to the focal length f of the first lens 1 The method meets the following conditions: -2.5<f 1 /f<-1.7。
Further preferably, the effective focal length f of the optical lens and the focal length f of the second lens 2 The method meets the following conditions: -20.0<f 2 /f<-3.0。
Further preferably, the effective focal length f of the optical lens and the focal length f of the third lens 3 The method meets the following conditions: 2.0<f 3 /f<5.0。
Further preferably, the effective focal length f of the optical lens and the focal length f of the fourth lens 4 The method meets the following conditions: 1.0<f 4 /f<2.6。
Further preferably, the effective focal length f of the optical lens and the focal length f of the fifth lens 5 The method meets the following conditions: 0.5<f 5 /f<2.5。
Further preferably, the effective focal length f of the optical lens and the focal length f of the seventh lens 7 The method meets the following conditions: f (f) 7 /f＞9.0。
The optical lens provided by the application improves the resolution of the optical lens, reduces the aberration and improves the imaging quality of the optical lens through reasonable configuration of the surface types of the lenses and reasonable collocation of the focal power.
Drawings
The foregoing and/or additional aspects and advantages of the application will become apparent and may be better understood from the following description of embodiments taken in conjunction with the accompanying drawings in which:
fig. 1 is a schematic structural diagram of an optical lens in embodiment 1 of the present application.
Fig. 2 is a graph showing a field curvature of an optical lens in embodiment 1 of the present application.
FIG. 3 is a graph showing F-Tanθ distortion of an optical lens in example 1 of the present application.
Fig. 4 is a graph showing the relative illuminance of the optical lens in embodiment 1 of the present application.
Fig. 5 is an MTF graph of the optical lens in example 1 of the present application.
Fig. 6 is an axial aberration diagram of the optical lens in embodiment 1 of the present application.
Fig. 7 is a graph showing a vertical axis chromatic aberration of an optical lens in embodiment 1 of the present application.
Fig. 8 is a schematic structural diagram of an optical lens in embodiment 2 of the present application.
Fig. 9 is a graph showing a field curvature of an optical lens in embodiment 2 of the present application.
FIG. 10 is a graph showing F-Tanθ distortion of an optical lens in example 2 of the present application.
Fig. 11 is a graph showing the relative illuminance of the optical lens in embodiment 2 of the present application.
Fig. 12 is an MTF graph of the optical lens in example 2 of the present application.
Fig. 13 is an axial aberration diagram of an optical lens in embodiment 2 of the present application.
Fig. 14 is a vertical axis chromatic aberration chart of the optical lens in embodiment 2 of the present application.
Fig. 15 is a schematic structural diagram of an optical lens in embodiment 3 of the present application.
Fig. 16 is a graph showing the field curvature of an optical lens in embodiment 3 of the present application.
FIG. 17 is a graph showing F-Tanθ distortion of an optical lens in example 3 of the present application.
Fig. 18 is a graph showing the relative illuminance of the optical lens in embodiment 3 of the present application.
Fig. 19 is an MTF graph of the optical lens in example 3 of the present application.
Fig. 20 is an axial aberration diagram of an optical lens in embodiment 3 of the present application.
Fig. 21 is a graph showing a vertical axis chromatic aberration of an optical lens in embodiment 3 of the present application.
Fig. 22 is a schematic structural diagram of an optical lens in embodiment 4 of the present application.
Fig. 23 is a graph showing a field curvature of an optical lens in embodiment 4 of the present application.
FIG. 24 is a graph showing F-Tanθ distortion of an optical lens in example 4 of the present application.
Fig. 25 is a graph showing the relative illuminance of the optical lens in embodiment 4 of the present application.
Fig. 26 is an MTF graph of the optical lens in example 4 of the present application.
Fig. 27 is an axial aberration diagram of an optical lens in embodiment 4 of the present application.
Fig. 28 is a vertical axis chromatic aberration chart of the optical lens in embodiment 4 of the application.
Fig. 29 is a schematic diagram of the structure of an optical lens in embodiment 5 of the present application.
Fig. 30 is a graph showing the field curvature of an optical lens in example 5 of the present application.
FIG. 31 is a graph showing F-Tanθ distortion of an optical lens in example 5 of the present application.
Fig. 32 is a graph showing the relative illuminance of the optical lens in embodiment 5 of the present application.
Fig. 33 is an MTF graph of the optical lens in example 5 of the present application.
Fig. 34 is an axial aberration diagram of the optical lens in embodiment 5 of the present application.
Fig. 35 is a graph showing a vertical axis chromatic aberration of an optical lens in embodiment 5 of the present application.
The application will be further described in the following detailed description in conjunction with the above-described figures.
Detailed Description
For a better understanding of the application, various aspects of the application will be described in more detail with reference to the accompanying drawings. It should be understood that these detailed description are merely illustrative of embodiments of the application and are not intended to limit the scope of the application in any way. Like reference numerals refer to like elements throughout the specification. The expression "and/or" includes any and all combinations of one or more of the associated listed items.
It should be noted that in the present specification, the expressions of first, second, third, etc. are only used to distinguish one feature from another feature, and do not represent any limitation on the feature. Accordingly, a first lens discussed below may also be referred to as a second lens or a third lens without departing from the teachings of the present application.
In the drawings, the thickness, size, and shape of the lenses have been slightly exaggerated for convenience of explanation. In particular, the spherical or aspherical shape shown in the drawings is shown by way of example. That is, the shape of the spherical or aspherical surface is not limited to the shape of the spherical or aspherical surface shown in the drawings. The figures are merely examples and are 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, then 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 closest to the object is referred to as the object side of the lens, and the surface of each lens closest to the imaging plane is referred to as the image side of the lens.
It will be further understood that the terms "comprises," "comprising," "includes," "including," "having," "containing," and/or "including," when used in this specification, specify the presence of stated features, elements, and/or components, but do not preclude the presence or addition of one or more other features, elements, components, and/or groups thereof. Furthermore, when a statement such as "at least one of the following" appears after a list of features that are listed, the entire listed feature is modified instead of modifying a separate element in the list. Furthermore, when describing embodiments of the application, use of "may" means "one or more embodiments of the application. Also, the term "exemplary" is intended to refer to an example or illustration.
Unless otherwise defined, all terms (including 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. It will be further understood that terms, such as those defined in commonly used dictionaries, should be interpreted as having a meaning that is consistent with their meaning in the context of the relevant art and will not be interpreted in an idealized or overly formal sense unless expressly so defined herein.
It should be noted that, without conflict, the embodiments of the present application and features of the embodiments may be combined with each other. The application will be described in detail below with reference to the drawings in connection with embodiments.
The optical lens according to the embodiment of the application includes, in order from an object side to an image side along an optical axis: the optical lens comprises a first lens, a second lens, a third lens, a diaphragm, a fourth lens, a fifth lens, a sixth lens, a seventh lens, an optical filter and protective glass.
In some embodiments, the first lens may have negative optical power, which facilitates reducing the tilt angle of incident light rays, thereby achieving effective sharing of the large field of view of the object. The object side surface of the first lens is a convex surface, and the image side surface is a concave surface, so that the light rays with the edge view fields can be collected as much as possible and enter the rear optical lens, and the collection of the light rays with a large angle can be realized.
In some embodiments, the second lens may have a negative power, which may be effective to share the negative power of the front end of the optical lens. The object side surface of the second lens is a concave surface, and the image side surface is a convex surface, so that overlarge light deflection caused by overlarge focal power of the first lens is avoided, and the difficulty of chromatic aberration correction of the optical lens is reduced.
In some embodiments, the third lens may have positive optical power, which is beneficial to converging light while reducing the light deflection angle, so that the light trend is smoothly transited. Meanwhile, various aberrations generated by the optical lens are balanced, and the imaging quality of the optical lens is improved.
In some embodiments, the fourth lens may have positive optical power, which is beneficial to further converging light and reducing the light deflection angle at the same time, so that the light trend is smoothly transited. The object side surface and the image side surface of the fourth lens are convex, so that various aberrations generated by the optical lens are balanced, and the imaging quality of the optical lens is improved.
In some embodiments, the fifth lens may have positive optical power, which is beneficial to further converging light and reducing the light deflection angle, so that the light trend is smoothly transited. The object side surface and the image side surface of the fifth lens are convex, so that various aberrations generated by the optical lens are balanced, and the imaging quality of the optical lens is improved.
In some embodiments, the sixth lens may have negative optical power, which is beneficial to increasing the imaging area of the optical lens and improving the imaging quality of the optical lens. The object side surface and the image side surface of the sixth lens are concave surfaces, so that the chromatic aberration of the optical lens can be optimized, and the imaging quality of the optical lens can be improved.
In some embodiments, the seventh lens may have positive optical power, which is beneficial to suppressing the angle of incidence of the marginal field of view on the imaging surface, effectively transmitting more light beams to the imaging surface, and improving the imaging quality of the optical lens. Meanwhile, the spherical aberration of the optical lens is optimized, and the imaging quality of the optical lens is improved.
In some embodiments, the effective focal length f of the optical lens and the combined focal lengths f of the first lens to the third lens 13 The method meets the following conditions: 4.0<f 13 /f<20.0. The optical power of the first lens to the optical power of the third lens are reasonably distributed, so that the deflection angle of light rays at the front end of the lens is reduced, and the generation of various off-axis aberrations is reduced.
In some embodiments, the effective focal length f of the optical lens and the combined focal lengths f of the fourth lens to the seventh lens 47 The method meets the following conditions: 1.5<f 47 /f<3.0. The requirements are met, the focal length of the optical lens is balanced by reasonably distributing the focal power of the fourth lens to the seventh lens, the correction capability of various aberrations at the rear end of the lens is improved, and the imaging quality of the optical lens is improved.
In some embodiments, the optical total length TTL and the effective focal length f of the optical lens satisfy: 3.0< TTL/f <10.0. The requirements are met, enough space is ensured to adjust the lens structure, and the imaging effect is optimized.
In some embodiments, the effective focal length f of the optical lens and the real image height IH corresponding to the maximum field angle satisfy: 1.0< IH/f <2.3. The range is satisfied, the characteristic of a large image plane can be realized, and the imaging quality of the optical lens is improved.
In some embodiments, the maximum field angle FOV and the real image height IH corresponding to the maximum field angle of the optical lens and the aperture D of the first lens object side surface 1 The three parts are as follows: d is 0.8 < 1 IH/tan (FOV/2) < 2.8. Meets the above range, and can ensure the size and large field of view of the optical lensBalance between angle and large image plane.
In some embodiments, the effective focal length f of the optical lens is equal to the focal length f of the first lens 1 The method meets the following conditions: -2.5<f 1 /f<-1.7. The requirements are met, the first lens can have proper negative focal power, and the inclination angle of incident light rays is reduced, so that the correction difficulty of various aberrations of the optical lens is reduced.
In some embodiments, the effective focal length f of the optical lens and the focal length f of the second lens 2 The method meets the following conditions: -20.0<f 2 /f<-3.0. The requirements are met, the second lens can have proper negative focal power, and the negative focal power at the front end of the optical lens is shared, so that the excessive deflection of light caused by the excessive concentration of the focal power of the first lens is avoided, and the difficulty of chromatic aberration correction of the optical lens is reduced.
In some embodiments, the effective focal length f of the optical lens and the focal length f of the third lens 3 The method meets the following conditions: 2.0<f 3 /f<5.0. The requirements are met, the third lens has proper positive focal power, the light deflection angle is reduced while converging light, the light trend is stably transited, various aberrations generated by the optical lens are balanced, and the imaging quality of the optical lens is improved.
In some embodiments, the effective focal length f of the optical lens and the focal length f of the fourth lens 4 The method meets the following conditions: 1.0<f 4 /f<2.6. The requirements are met, the fourth lens has proper positive focal power, the light deflection angle is reduced while converging light, the light trend is stably transited, various aberrations generated by the optical lens are balanced, and the imaging quality of the optical lens is improved.
In some embodiments, the effective focal length f of the optical lens and the focal length f of the fifth lens 5 The method meets the following conditions: 0.5<f 5 /f<2.5. The requirements are met, the fifth lens has proper positive focal power, the light deflection angle is reduced while converging light, the light trend is stably transited, various aberrations generated by the optical lens are balanced, and the imaging quality of the optical lens is improved.
In some embodimentsAn effective focal length f of the optical lens and a focal length f of the sixth lens 6 The method meets the following conditions: -1.6<f 6 /f<-0.4. The requirements are met, the sixth lens can have proper negative focal power, and the imaging area of the optical lens can be increased; meanwhile, the chromatic aberration of the optical lens can be optimized, and the imaging quality of the optical lens is improved.
In some embodiments, the effective focal length f of the optical lens and the focal length f of the seventh lens 7 The method meets the following conditions: f (f) 7 And/f > 9.0. The requirements are met, the angle of incidence of the edge view field on the imaging surface is favorably pressed, more light beams are effectively transmitted to the imaging surface, and the imaging quality of the optical lens is improved; meanwhile, the spherical aberration of the optical lens is optimized, and the imaging quality of the optical lens is improved.
In some embodiments, the abbe number Vd of at least one of the fifth lens and the sixth lens satisfies: vd > 80, abbe number Vd of the fifth lens 5 And Abbe number Vd of the sixth lens 6 The method meets the following conditions: vd (Vd) 5 -Vd 6 > 60. Meeting the above range is beneficial to realizing confocal of visible light and infrared light.
In some embodiments, the radius of curvature R of the object-side surface of the seventh lens 13 The effective focal length f with the optical lens satisfies: -2.5<R 13 /f<18. Radius of curvature R of image side of seventh lens 14 The effective focal length f with the optical lens satisfies: -2.0<R 14 /f<18. The requirements are met, various aberrations generated by the seventh lens can be reduced, and the imaging quality of the optical lens is improved.
In some embodiments, the fifth lens and the sixth lens can be glued to form a glued lens, so that chromatic aberration of the optical lens can be effectively corrected, decentered sensitivity of the optical lens can be reduced, aberration of the optical lens can be balanced, and imaging quality of the optical lens can be improved; the assembly sensitivity of the optical lens can be reduced, the processing technology difficulty of the optical lens is further reduced, and the assembly yield of the optical lens is improved.
In some embodiments, the second lens, the fourth lens and the seventh lens may each be a surface type of aspherical lens to improve the resolution quality.
For better optical performance of the system, a plurality of aspheric lenses are adopted in the lens, and the shape of each aspheric surface of the optical lens meets the following equation:
wherein z is the distance between the curved surface and the curved surface vertex in the optical axis direction, h is the distance between the optical axis and the curved surface, c is the curvature of the curved surface vertex, K is the quadric surface coefficient, and A, B, C, D, E, F is the second, fourth, sixth, eighth, tenth and twelfth order surface coefficients respectively.
The application 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 application, but the embodiments of the present application 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 application are intended to be equivalent substitutes within the scope of the present application.
Example 1
Referring to fig. 1, a schematic structural diagram of an optical lens provided in embodiment 1 of the present application is shown, where the optical lens includes, in order from an object side to an imaging plane along an optical axis: the first lens L1, the second lens L2, the third lens L3, the stop ST, the fourth lens L4, the fifth lens L5, the sixth lens L6, the seventh lens L7, the filter G1, and the cover glass G2.
The first lens element L1 has negative refractive power, wherein an object-side surface S1 thereof is convex, and an image-side surface S2 thereof is concave;
the second lens element L2 has negative refractive power, wherein an object-side surface S3 thereof is concave, and an image-side surface S4 thereof is convex;
the third lens element L3 has positive refractive power, wherein an object-side surface S5 thereof is concave, and an image-side surface S6 thereof is convex;
a diaphragm ST;
the fourth lens element L4 has positive refractive power, and both an object-side surface S7 and an image-side surface S8 thereof are convex;
the fifth lens element L5 has positive refractive power, and both an object-side surface S9 and an image-side surface S10 thereof are convex;
the sixth lens element L6 has negative refractive power, and an object-side surface S10 and an image-side surface S11 thereof are concave;
the fifth lens element L5 and the sixth lens element L6 form a cemented lens assembly, i.e., the cemented surface between the image side surface of the fifth lens element L5 and the object side surface of the sixth lens element L6 is S10;
the seventh lens element L7 with positive refractive power has a concave object-side surface S12 and a convex image-side surface S13;
the object side surface S14 and the image side surface S15 of the optical filter G1 are planes;
the object side surface S16 and the image side surface S17 of the protective glass G2 are planes;
the imaging surface S18 is a plane.
The relevant parameters of each lens in the optical lens in example 1 are shown in tables 1-1.
TABLE 1-1
The surface profile parameters of the aspherical lens of the optical lens in example 1 are shown in tables 1 to 2.
TABLE 1-2
| Face number | K | A | B | C | D | E | F |
| S3 | -2.46E+00 | 0.00E+00 | 4.83E-04 | -5.65E-06 | 6.15E-07 | -2.70E-08 | 4.70E-10 |
| S4 | -7.09E+00 | 0.00E+00 | 1.73E-04 | 7.84E-06 | -1.01E-07 | 2.56E-09 | -8.09E-11 |
| S7 | -3.10E+00 | 0.00E+00 | 2.71E-04 | -4.36E-05 | 2.04E-06 | -7.10E-08 | -2.47E-09 |
| S8 | 3.83E-01 | 0.00E+00 | 6.57E-04 | -4.24E-05 | 2.56E-06 | -1.22E-07 | 5.78E-10 |
| S12 | -7.99E-02 | 0.00E+00 | 3.32E-03 | 5.39E-05 | -5.65E-06 | 1.99E-08 | 1.23E-08 |
| S13 | -2.53E+00 | 0.00E+00 | 1.31E-03 | 7.64E-05 | -2.53E-06 | -1.18E-07 | 9.97E-09 |
In this embodiment, the field curvature curve, the F-Tan θ distortion curve, the relative illuminance curve, the MTF curve, the axial aberration curve, and the vertical chromatic aberration curve of the optical lens are shown in fig. 2, 3, 4, 5, 6, and 7, respectively.
Fig. 2 shows a field curve of example 1, which indicates the degree of curvature of light rays of different wavelengths on a meridional image plane and a sagittal image plane, the horizontal axis indicates the amount of shift (unit: mm), and the vertical axis indicates the half angle of view (unit: °). From the graph, the field curvature of the meridian image plane and the sagittal image plane is controlled within-0.02 mm to 0.12mm, which shows that the optical lens can well correct the field curvature.
Fig. 3 shows the F-Tan θ distortion curve of example 1, which represents the F-Tan θ distortion of light rays of different wavelengths at different image heights on the imaging plane, the horizontal axis represents the F-Tan θ distortion (unit:%) and the vertical axis represents the half field angle (unit: °). From the figure, the F-Tanθ distortion of the optical lens is controlled within 0-3%, the image compression of the edge angle area is gentle, and the definition of the unfolded image is effectively improved.
Fig. 4 shows the relative illuminance curve of example 1, which represents the relative illuminance values for different field angles on the imaging plane, the horizontal axis represents the half field angle (in: °), and the vertical axis represents the relative illuminance (in:%). As can be seen from the figure, the relative illuminance value of the optical lens is still greater than 60% at the maximum half field angle, which indicates that the optical lens has better relative illuminance.
Fig. 5 shows an MTF (modulation transfer function) graph of example 1, which represents the lens imaging modulation degree of different spatial frequencies at each view field, the horizontal axis represents the spatial frequency (unit: lp/mm), and the vertical axis represents the MTF value. As can be seen from the graph, the MTF values of the embodiment are above 0.5 in the whole field of view, and in the range of 0-160 lp/mm, the MTF curve is uniformly and smoothly reduced in the process of the field of view from the center to the edge, and the MTF image has better imaging quality and better detail resolution under the conditions of low frequency and high frequency.
Fig. 6 shows an axial aberration diagram of example 1, which represents aberration of each wavelength on the optical axis at the imaging plane, the horizontal axis represents an axial aberration value (unit: μm), and the vertical axis represents a normalized pupil radius. As can be seen from the figure, the axial aberration is controlled within ±20μm, which means that the optical lens can correct axial aberration well.
Fig. 7 shows a vertical axis color difference graph of example 1, which shows color differences at different image heights on an imaging plane for each wavelength with respect to a center wavelength (0.55 μm), with the horizontal axis showing a vertical axis color difference value (unit: μm) for each wavelength with respect to the center wavelength, and the vertical axis showing a normalized field angle. As can be seen from the figure, the vertical axis chromatic aberration of the longest wavelength and the shortest wavelength is controlled within-1 mu m to 4.5 mu m, which shows that the optical lens can excellently correct chromatic aberration of an edge view field and a secondary spectrum of the whole image surface.
Example 2
Referring to fig. 8, a schematic structural diagram of an optical lens provided in embodiment 2 of the present application is shown, where the optical lens includes, in order from an object side to an imaging plane along an optical axis: the first lens L1, the second lens L2, the third lens L3, the stop ST, the fourth lens L4, the fifth lens L5, the sixth lens L6, the seventh lens L7, the filter G1, and the cover glass G2.
The first lens element L1 has negative refractive power, wherein an object-side surface S1 thereof is convex, and an image-side surface S2 thereof is concave;
the second lens element L2 has negative refractive power, wherein an object-side surface S3 thereof is concave, and an image-side surface S4 thereof is convex;
the third lens element L3 has positive refractive power, and both an object-side surface S5 and an image-side surface S6 thereof are convex;
a diaphragm ST;
the fourth lens element L4 has positive refractive power, and both an object-side surface S7 and an image-side surface S8 thereof are convex;
the fifth lens element L5 has positive refractive power, and both an object-side surface S9 and an image-side surface S10 thereof are convex;
the sixth lens element L6 has negative refractive power, and an object-side surface S10 and an image-side surface S11 thereof are concave;
the fifth lens element L5 and the sixth lens element L6 form a cemented lens assembly, i.e., the cemented surface between the image side surface of the fifth lens element L5 and the object side surface of the sixth lens element L6 is S10;
the seventh lens element L7 with positive refractive power has a concave object-side surface S12 and a convex image-side surface S13;
the object side surface S14 and the image side surface S15 of the optical filter G1 are planes;
the object side surface S16 and the image side surface S17 of the protective glass G2 are planes;
the imaging surface S18 is a plane.
The relevant parameters of each lens in the optical lens in example 2 are shown in table 2-1.
TABLE 2-1
The surface profile parameters of the aspherical lens of the optical lens in example 2 are shown in tables 2-2.
TABLE 2-2
| Face number | K | A | B | C | D | E | F |
| S3 | -1.71E+00 | 0.00E+00 | 4.42E-04 | -6.73E-06 | 5.89E-07 | -2.55E-08 | 4.78E-10 |
| S4 | -8.21E+00 | 0.00E+00 | 1.30E-04 | 5.10E-06 | -1.00E-07 | 2.81E-09 | -6.65E-11 |
| S7 | -2.98E+00 | 0.00E+00 | 1.91E-04 | -4.83E-05 | 1.77E-06 | -4.21E-08 | -4.91E-09 |
| S8 | 1.02E+00 | 0.00E+00 | 7.08E-04 | -3.66E-05 | 2.40E-06 | -1.21E-07 | 9.33E-10 |
| S12 | -3.27E-01 | 0.00E+00 | 2.90E-03 | 9.11E-05 | -8.90E-06 | 2.87E-07 | 1.09E-08 |
| S13 | -2.28E+00 | 0.00E+00 | 2.83E-04 | 6.53E-05 | -2.01E-06 | -9.42E-08 | 8.23E-09 |
In this embodiment, the field curvature curve, the F-Tan θ distortion curve, the relative illuminance curve, the MTF curve, the axial aberration curve, and the vertical chromatic aberration curve of the optical lens are shown in fig. 9, 10, 11, 12, 13, and 14, respectively.
Fig. 9 shows a field curvature curve of example 2, which indicates the degree of curvature of light rays of different wavelengths on a meridional image plane and a sagittal image plane, the horizontal axis indicates the amount of shift (unit: mm), and the vertical axis indicates the half angle of view (unit: °). From the figure, the field curvature of the meridian image plane and the sagittal image plane is controlled within 0-0.12 mm, which shows that the optical lens can well correct the field curvature.
Fig. 10 shows an F-Tan θ distortion curve of example 2, which represents F-Tan θ distortion of light rays of different wavelengths at different image heights on an imaging plane, the horizontal axis represents F-Tan θ distortion (unit:%) and the vertical axis represents half field angle (unit: °). From the figure, the F-Tanθ distortion of the optical lens is controlled within 0-1%, the image compression of the edge angle area is gentle, and the definition of the unfolded image is effectively improved.
Fig. 11 shows the relative illuminance curve of example 2, which represents the relative illuminance values for different field angles on the imaging plane, the horizontal axis represents the half field angle (in: °), and the vertical axis represents the relative illuminance (in:%). As can be seen from the figure, the relative illuminance value of the optical lens is still greater than 65% at the maximum half field angle, which indicates that the optical lens has better relative illuminance.
Fig. 12 shows an MTF (modulation transfer function) graph of example 2, which represents the lens imaging modulation degree of different spatial frequencies at each view field, the horizontal axis represents the spatial frequency (unit: lp/mm), and the vertical axis represents the MTF value. As can be seen from the graph, the MTF values of the embodiment are above 0.4 in the whole field of view, and in the range of 0-160 lp/mm, the MTF curve is uniformly and smoothly reduced in the process of the field of view from the center to the edge, and the MTF image has better imaging quality and better detail resolution under the conditions of low frequency and high frequency.
Fig. 13 shows an axial aberration diagram of example 2, which represents aberration of each wavelength on the optical axis at the imaging plane, the horizontal axis represents an axial aberration value (unit: μm), and the vertical axis represents a normalized pupil radius. As can be seen from the figure, the offset of the axial aberration is controlled within-15-25 μm, which shows that the optical lens can better correct the axial aberration.
Fig. 14 shows a vertical axis color difference graph of example 2, which shows color differences at different image heights on an imaging plane for each wavelength with respect to a center wavelength (0.55 μm), with the horizontal axis showing a vertical axis color difference value (unit: μm) for each wavelength with respect to the center wavelength, and the vertical axis showing a normalized field angle. As can be seen from the figure, the vertical axis chromatic aberration of the longest wavelength and the shortest wavelength is controlled within-2 mu m to 5 mu m, which shows that the optical lens can excellently correct chromatic aberration of an edge view field and a secondary spectrum of the whole image surface.
Example 3
Referring to fig. 15, a schematic structural diagram of an optical lens provided in embodiment 3 of the present application is shown, where the optical lens includes, in order from an object side to an imaging plane along an optical axis: the first lens L1, the second lens L2, the third lens L3, the stop ST, the fourth lens L4, the fifth lens L5, the sixth lens L6, the seventh lens L7, the filter G1, and the cover glass G2.
The first lens element L1 has negative refractive power, wherein an object-side surface S1 thereof is convex, and an image-side surface S2 thereof is concave;
the second lens element L2 has negative refractive power, wherein an object-side surface S3 thereof is concave, and an image-side surface S4 thereof is convex;
the third lens element L3 has positive refractive power, wherein an object-side surface S5 thereof is convex, and an image-side surface S6 thereof is concave;
a diaphragm ST;
the fourth lens element L4 has positive refractive power, and both an object-side surface S7 and an image-side surface S8 thereof are convex;
the fifth lens element L5 has positive refractive power, and both an object-side surface S9 and an image-side surface S10 thereof are convex;
the sixth lens element L6 has negative refractive power, and an object-side surface S10 and an image-side surface S11 thereof are concave;
the fifth lens element L5 and the sixth lens element L6 form a cemented lens assembly, i.e., the cemented surface between the image side surface of the fifth lens element L5 and the object side surface of the sixth lens element L6 is S10;
the seventh lens element L7 with positive refractive power has a convex object-side surface S12 and a concave image-side surface S13;
the object side surface S14 and the image side surface S15 of the optical filter G1 are planes;
the object side surface S16 and the image side surface S17 of the protective glass G2 are planes;
the imaging surface S18 is a plane.
The relevant parameters of each lens in the optical lens in example 3 are shown in table 3-1.
TABLE 3-1
The surface profile parameters of the aspherical lens of the optical lens in example 3 are shown in table 3-2.
TABLE 3-2
| Face number | K | A | B | C | D | E | F |
| S3 | -1.88E+00 | 0.00E+00 | 8.63E-04 | 2.84E-05 | -1.83E-07 | 2.78E-10 | 2.79E-10 |
| S4 | -4.50E+01 | 0.00E+00 | 8.84E-04 | 4.63E-05 | -2.54E-07 | 1.30E-08 | 3.35E-09 |
| S7 | -2.59E+00 | 0.00E+00 | -2.74E-04 | -1.75E-05 | -2.76E-06 | 3.67E-07 | -2.55E-08 |
| S8 | -8.61E-01 | 0.00E+00 | -5.45E-05 | -6.55E-05 | 6.69E-06 | -4.26E-07 | 2.25E-09 |
| S12 | 4.37E+01 | 0.00E+00 | -5.07E-03 | -1.20E-04 | 1.79E-05 | -1.39E-06 | 1.43E-07 |
| S13 | -4.50E+01 | 0.00E+00 | -2.56E-03 | 3.53E-05 | 1.03E-05 | 1.08E-07 | 5.27E-09 |
In this embodiment, the field curvature curve, the F-Tan θ distortion curve, the relative illuminance curve, the MTF curve, the axial aberration curve, and the vertical chromatic aberration curve of the optical lens are shown in fig. 16, 17, 18, 19, 20, and 21, respectively.
Fig. 16 shows a field curvature curve of example 3, which indicates the degree of curvature of light rays of different wavelengths on a meridional image plane and a sagittal image plane, the horizontal axis indicates the amount of shift (unit: mm), and the vertical axis indicates the half angle of view (unit: °). From the graph, the field curvature of the meridian image plane and the sagittal image plane is controlled within-0.05 mm to 0.09mm, which indicates that the optical lens can well correct the field curvature.
Fig. 17 shows an F-Tan θ distortion curve of example 3, which represents F-Tan θ distortion of light rays of different wavelengths at different image heights on an imaging plane, the horizontal axis represents F-Tan θ distortion (unit:%) and the vertical axis represents half field angle (unit: °). From the figure, the F-Tanθ distortion of the optical lens is controlled within 0-5%, the image compression of the edge angle area is gentle, and the definition of the unfolded image is effectively improved.
Fig. 18 shows the relative illuminance curve of example 3, which represents the relative illuminance values for different field angles on the imaging plane, the horizontal axis represents the half field angle (unit: °), and the vertical axis represents the relative illuminance (unit:%). As can be seen from the figure, the relative illuminance value of the optical lens is still greater than 50% at the maximum half field angle, which indicates that the optical lens has better relative illuminance.
Fig. 19 shows an MTF (modulation transfer function) graph of example 3, which represents the lens imaging modulation degree of different spatial frequencies at each view field, the horizontal axis represents the spatial frequency (unit: lp/mm), and the vertical axis represents the MTF value. As can be seen from the graph, the MTF values of the embodiment are above 0.4 in the whole field of view, and in the range of 0-160 lp/mm, the MTF curve is uniformly and smoothly reduced in the process of the field of view from the center to the edge, and the MTF image has better imaging quality and better detail resolution under the conditions of low frequency and high frequency.
Fig. 20 shows an axial aberration diagram of example 3, which represents aberration of each wavelength on the optical axis at the imaging plane, the horizontal axis represents an axial aberration value (unit: μm), and the vertical axis represents a normalized pupil radius. As can be seen from the figure, the offset of the axial aberration is controlled within-15-20 μm, which shows that the optical lens can better correct the axial aberration.
Fig. 21 shows a vertical axis color difference graph of example 3, which shows color differences at different image heights on an imaging plane for each wavelength with respect to a center wavelength (0.55 μm), with the horizontal axis showing a vertical axis color difference value (unit: μm) for each wavelength with respect to the center wavelength, and the vertical axis showing a normalized field angle. As can be seen from the figure, the vertical axis chromatic aberration of the longest wavelength and the shortest wavelength is controlled within 0-7 mu m, which shows that the optical lens can excellently correct chromatic aberration of the edge view field and the secondary spectrum of the whole image surface.
Example 4
Referring to fig. 22, a schematic structural diagram of an optical lens provided in embodiment 4 of the present application is shown, where the optical lens includes, in order from an object side to an imaging plane along an optical axis: the first lens L1, the second lens L2, the third lens L3, the stop ST, the fourth lens L4, the fifth lens L5, the sixth lens L6, the seventh lens L7, the filter G1, and the cover glass G2.
The first lens element L1 has negative refractive power, wherein an object-side surface S1 thereof is convex, and an image-side surface S2 thereof is concave;
the second lens element L2 has negative refractive power, wherein an object-side surface S3 thereof is concave, and an image-side surface S4 thereof is convex;
the third lens element L3 has positive refractive power, wherein an object-side surface S5 thereof is concave, and an image-side surface S6 thereof is convex;
a diaphragm ST;
the fourth lens element L4 has positive refractive power, and both an object-side surface S7 and an image-side surface S8 thereof are convex;
the fifth lens element L5 has positive refractive power, and both an object-side surface S9 and an image-side surface S10 thereof are convex;
the sixth lens element L6 has negative refractive power, and an object-side surface S10 and an image-side surface S11 thereof are concave;
the fifth lens element L5 and the sixth lens element L6 form a cemented lens assembly, i.e., the cemented surface between the image side surface of the fifth lens element L5 and the object side surface of the sixth lens element L6 is S10;
the seventh lens element L7 with positive refractive power has a concave object-side surface S12 and a convex image-side surface S13;
the object side surface S14 and the image side surface S15 of the optical filter G1 are planes;
the object side surface S16 and the image side surface S17 of the protective glass G2 are planes;
the imaging surface S18 is a plane.
The relevant parameters of each lens in the optical lens in example 4 are shown in table 4-1.
TABLE 4-1
The surface profile parameters of the aspherical lens of the optical lens in example 4 are shown in table 4-2.
TABLE 4-2
| Face number | K | A | B | C | D | E | F |
| S3 | -9.26E-01 | 0.00E+00 | 1.59E-04 | -6.29E-06 | 3.49E-07 | -1.10E-08 | 1.09E-10 |
| S4 | -6.00E+00 | 0.00E+00 | -4.90E-05 | 3.23E-06 | 2.62E-08 | -1.29E-09 | 8.36E-12 |
| S7 | -1.63E+01 | 0.00E+00 | -5.07E-06 | -5.92E-05 | 1.42E-06 | -7.80E-08 | -1.28E-08 |
| S8 | 1.20E+00 | 0.00E+00 | 6.13E-04 | -2.20E-05 | 4.32E-07 | -4.58E-08 | -1.04E-09 |
| S12 | 1.67E-01 | 0.00E+00 | 2.90E-03 | -2.58E-05 | -6.02E-06 | 2.98E-07 | -2.33E-10 |
| S13 | -4.71E+00 | 0.00E+00 | 1.44E-03 | 3.72E-05 | -4.99E-06 | 9.74E-08 | 4.48E-09 |
In this embodiment, the field curvature curve, the F-Tan θ distortion curve, the relative illuminance curve, the MTF curve, the axial aberration curve, and the vertical chromatic aberration curve of the optical lens are shown in fig. 23, 24, 25, 26, 27, and 28, respectively.
Fig. 23 shows a field curvature curve of example 4, in which the degree of curvature of light rays of different wavelengths on a meridional image plane and a sagittal image plane is shown, the horizontal axis represents the amount of shift (unit: mm), and the vertical axis represents the half angle of view (unit: °). From the graph, the field curvature of the meridian image plane and the sagittal image plane is controlled within-0.03 mm to 0.06mm, which indicates that the optical lens can well correct the field curvature.
Fig. 24 shows an F-Tan θ distortion curve of example 4, which represents F-Tan θ distortion of light rays of different wavelengths at different image heights on an imaging plane, the horizontal axis represents F-Tan θ distortion (unit:%) and the vertical axis represents half field angle (unit: °). As can be seen from the figure, the F-Tanθ distortion of the optical lens is controlled within-40% -0, the image compression of the edge angle area is gentle, and the definition of the unfolded image is effectively improved.
Fig. 25 shows the relative illuminance curve of example 4, which represents the relative illuminance values for different field angles on the imaging plane, the horizontal axis represents the half field angle (in: °), and the vertical axis represents the relative illuminance (in:%). As can be seen from the figure, the relative illuminance value of the optical lens is still greater than 70% at the maximum half field angle, which indicates that the optical lens has better relative illuminance.
Fig. 26 shows an MTF (modulation transfer function) graph of example 4, which represents the lens imaging modulation degree of different spatial frequencies at each view field, the horizontal axis represents the spatial frequency (unit: lp/mm), and the vertical axis represents the MTF value. As can be seen from the graph, the MTF values of the embodiment are above 0.4 in the whole field of view, and in the range of 0-160 lp/mm, the MTF curve is uniformly and smoothly reduced in the process of the field of view from the center to the edge, and the MTF image has better imaging quality and better detail resolution under the conditions of low frequency and high frequency.
Fig. 27 shows an axial aberration diagram of example 4, which represents aberration of each wavelength on the optical axis at the imaging plane, the horizontal axis represents an axial aberration value (unit: μm), and the vertical axis represents a normalized pupil radius. As can be seen from the figure, the offset of the axial aberration is controlled within-10-15 μm, which shows that the optical lens can better correct the axial aberration.
Fig. 28 shows a vertical axis color difference graph of example 4, which shows color differences at different image heights on an imaging plane for each wavelength with respect to a center wavelength (0.55 μm), with the horizontal axis showing a vertical axis color difference value (unit: μm) for each wavelength with respect to the center wavelength, and the vertical axis showing a normalized field angle. As can be seen from the figure, the vertical axis chromatic aberration of the longest wavelength and the shortest wavelength is controlled within-2 mu m to 7 mu m, which shows that the optical lens can excellently correct chromatic aberration of an edge view field and a secondary spectrum of the whole image surface.
Example 5
Referring to fig. 29, a schematic structural diagram of an optical lens provided in embodiment 5 of the present application is shown, where the optical lens includes, in order from an object side to an imaging plane along an optical axis: the first lens L1, the second lens L2, the third lens L3, the stop ST, the fourth lens L4, the fifth lens L5, the sixth lens L6, the seventh lens L7, the filter G1, and the cover glass G2.
The first lens element L1 has negative refractive power, wherein an object-side surface S1 thereof is convex, and an image-side surface S2 thereof is concave;
the second lens element L2 has negative refractive power, wherein an object-side surface S3 thereof is concave, and an image-side surface S4 thereof is convex;
the third lens element L3 has positive refractive power, and both an object-side surface S5 and an image-side surface S6 thereof are convex;
a diaphragm ST;
the fourth lens element L4 has positive refractive power, and both an object-side surface S7 and an image-side surface S8 thereof are convex;
the fifth lens element L5 has positive refractive power, and both an object-side surface S9 and an image-side surface S10 thereof are convex;
the sixth lens element L6 has negative refractive power, and an object-side surface S10 and an image-side surface S11 thereof are concave;
the fifth lens element L5 and the sixth lens element L6 form a cemented lens assembly, i.e., the cemented surface between the image side surface of the fifth lens element L5 and the object side surface of the sixth lens element L6 is S10;
the seventh lens element L7 with positive refractive power has a concave object-side surface S12 and a convex image-side surface S13;
the object side surface S14 and the image side surface S15 of the optical filter G1 are planes;
the object side surface S16 and the image side surface S17 of the protective glass G2 are planes;
the imaging surface S18 is a plane.
The relevant parameters of each lens in the optical lens in example 5 are shown in table 5-1.
TABLE 5-1
The surface profile parameters of the aspherical lens of the optical lens in example 5 are shown in table 5-2.
TABLE 5-2
| Face number | K | A | B | C | D | E | F |
| S3 | -9.93E-01 | 0.00E+00 | 2.62E-04 | -5.95E-06 | 2.54E-07 | -7.51E-09 | 8.31E-11 |
| S4 | -8.62E+00 | 0.00E+00 | 4.35E-05 | 4.03E-06 | -1.22E-08 | -1.22E-10 | 3.39E-13 |
| S7 | -1.52E+01 | 0.00E+00 | -1.34E-05 | -5.66E-05 | 8.95E-08 | 7.73E-08 | -2.06E-08 |
| S8 | 1.60E+00 | 0.00E+00 | 4.82E-04 | -2.51E-05 | 1.56E-06 | -1.27E-07 | 1.72E-09 |
| S12 | -3.89E-01 | 0.00E+00 | 2.42E-03 | -2.31E-05 | -7.82E-06 | 2.40E-07 | 6.02E-09 |
| S13 | -3.02E+00 | 0.00E+00 | 1.43E-03 | 1.68E-05 | -6.30E-06 | 1.50E-07 | 3.49E-09 |
In this embodiment, the field curvature curve, the F-Tan θ distortion curve, the relative illuminance curve, the MTF curve, the axial aberration curve, and the vertical chromatic aberration curve of the optical lens are shown in fig. 30, 31, 32, 33, 34, and 35, respectively.
Fig. 30 shows a field curve of example 5, which shows the degree of curvature of light rays of different wavelengths on a meridional image plane and a sagittal image plane, the horizontal axis shows the amount of shift (unit: mm), and the vertical axis shows the half angle of view (unit: °). From the graph, the field curvature of the meridian image plane and the sagittal image plane is controlled within-0.02 mm to 0.06mm, which indicates that the optical lens can well correct the field curvature.
Fig. 31 shows an F-Tan θ distortion curve of example 5, which represents F-Tan θ distortion of light rays of different wavelengths at different image heights on an imaging plane, the horizontal axis represents F-Tan θ distortion (unit:%) and the vertical axis represents half field angle (unit: °). As can be seen from the figure, the F-Tanθ distortion of the optical lens is controlled within-40% -0, the image compression of the edge angle area is gentle, and the definition of the unfolded image is effectively improved.
Fig. 32 shows the relative illuminance curve of example 5, which represents the relative illuminance values for different field angles on the imaging plane, the horizontal axis represents the half field angle (in: °), and the vertical axis represents the relative illuminance (in:%). As can be seen from the figure, the relative illuminance value of the optical lens is still greater than 70% at the maximum half field angle, which indicates that the optical lens has better relative illuminance.
Fig. 33 shows an MTF (modulation transfer function) graph of example 5, which represents the lens imaging modulation degree of different spatial frequencies at each view field, the horizontal axis represents the spatial frequency (unit: lp/mm), and the vertical axis represents the MTF value. As can be seen from the graph, the MTF values of the embodiment are above 0.4 in the whole field of view, and in the range of 0-160 lp/mm, the MTF curve is uniformly and smoothly reduced in the process of the field of view from the center to the edge, and the MTF image has better imaging quality and better detail resolution under the conditions of low frequency and high frequency.
Fig. 34 shows an axial aberration diagram of example 5, which represents aberration of each wavelength on the optical axis at the imaging plane, the horizontal axis represents an axial aberration value (unit: μm), and the vertical axis represents a normalized pupil radius. As can be seen from the figure, the offset of the axial aberration is controlled within-10-15 μm, which shows that the optical lens can better correct the axial aberration.
Fig. 35 shows a vertical axis color difference graph of example 5, which shows color differences at different image heights on an imaging plane for each wavelength with respect to a center wavelength (0.55 μm), with the horizontal axis showing a vertical axis color difference value (unit: μm) for each wavelength with respect to the center wavelength, and the vertical axis showing a normalized field angle. As can be seen from the figure, the vertical axis chromatic aberration of the longest wavelength and the shortest wavelength is controlled within-2 mu m to 7 mu m, which shows that the optical lens can excellently correct chromatic aberration of an edge view field and a secondary spectrum of the whole image surface.
Referring to table 6, the optical characteristics corresponding to the above embodiments include the effective focal length f, the total optical length TTL, the aperture value FNO, the real image height IH, the maximum field angle FOV and the numerical value corresponding to each conditional expression in the embodiments.
TABLE 6
| Parameters and conditions | Example 1 | Example 2 | Example 3 | Example 4 | Example 5 |
| f(mm) | 7.80 | 7.95 | 7.66 | 4.35 | 4.39 |
| TTL(mm) | 39.95 | 39.13 | 27.94 | 40.00 | 40.00 |
| IH(mm) | 9.25 | 9.25 | 9.25 | 9.25 | 9.25 |
| FOV(°) | 60.00 | 60.00 | 60.00 | 120.00 | 120.00 |
| CRA(°) | 20.38 | 20.49 | 30.15 | 21.03 | 22.51 |
| FNO | 2.00 | 2.00 | 2.00 | 2.00 | 2.00 |
| EPD(mm) | 3.90 | 3.98 | 3.83 | 2.17 | 2.20 |
| TTL/f | 5.12 | 4.92 | 3.65 | 9.20 | 9.11 |
| TTL/IH | 4.32 | 4.23 | 3.02 | 4.32 | 4.32 |
| (IH/2)/(f×tan(FOV/2)) | 1.03 | 1.01 | 1.05 | 0.61 | 0.61 |
| FOV/FNO(°) | 30.00 | 30.00 | 30.00 | 60.00 | 60.00 |
| IH/EPD | 2.37 | 2.33 | 2.41 | 4.26 | 4.21 |
| IH/f | 1.19 | 1.16 | 1.21 | 2.13 | 2.11 |
| BFL/f | 0.62 | 0.45 | 0.51 | 1.11 | 0.82 |
| (FOV/2)/CRA | 1.47 | 1.46 | 0.99 | 2.85 | 2.67 |
| FOV*f/IH | 50.56 | 51.56 | 49.72 | 56.38 | 56.97 |
| TTL/IH/FOV | 0.29 | 0.28 | 0.20 | 0.14 | 0.14 |
| D 1 /IH/tan(FOV/2) | 2.61 | 2.54 | 2.29 | 0.96 | 0.94 |
| f 1 /f | -2.35 | -2.23 | -2.21 | -1.96 | -1.97 |
| f 2 /f | -8.81 | -3.68 | -3.36 | -19.65 | -7.43 |
| f 3 /f | 3.00 | 2.11 | 3.25 | 4.89 | 3.73 |
| f 4 /f | 1.49 | 1.40 | 1.08 | 2.48 | 2.50 |
| f 5 /f | 1.80 | 1.74 | 0.71 | 2.32 | 2.16 |
| f 6 /f | -1.19 | -1.28 | -0.49 | -1.55 | -1.44 |
| f 7 /f | 2.22E+05 | 5.56E+04 | 3.42E+09 | 10.58 | 9.31 |
| f 13 /f | 11.63 | 9.78 | 4.27 | 18.39 | 11.67 |
| f 47 /f | 1.82 | 1.74 | 2.04 | 2.71 | 2.71 |
| R 13 /f | -0.66 | -0.50 | 16.74 | -2.05 | -1.57 |
| R 14 /f | -0.73 | -0.58 | 16.67 | -1.76 | -1.41 |
In summary, the optical lens provided by the application has an infrared confocal function, meets the definition requirement of imaging at day and night, and improves the resolution of the optical lens, reduces aberration and improves the imaging quality of the optical lens through reasonable configuration of the lens surfaces and reasonable collocation of optical power.
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 application. 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 foregoing examples illustrate only a few embodiments of the application and are described in detail herein without thereby limiting the scope of the application. 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 application, which are all within the scope of the application. Accordingly, the scope of protection of the present application is to be determined by the appended claims.
Claims (10)
1. An optical lens, seven lenses altogether, characterized in that, from the object side to the imaging plane along the optical axis, are:
the first lens with negative focal power has a convex object side surface and a concave image side surface;
the object side surface of the second lens is a concave surface, and the image side surface of the second lens is a convex surface;
a third lens having positive optical power;
a diaphragm;
a fourth lens element with positive refractive power having convex object-side and image-side surfaces;
a fifth lens element with positive refractive power having convex object-side and image-side surfaces;
a sixth lens element with negative refractive power having concave object-side and image-side surfaces;
a seventh lens having positive optical power;
an effective focal length f of the optical lens and a combined focal length f of the first lens to the third lens 13 The method meets the following conditions: 4.0<f 13 /f<20.0；
An effective focal length f of the optical lens and a combined focal length f of the fourth lens to the seventh lens 47 The method meets the following conditions: 1.5<f 47 /f<3.0。
2. The optical lens of claim 1, wherein the optical total length TTL and the effective focal length f of the optical lens satisfy: 3.0< TTL/f <10.0.
3. The optical lens according to claim 1, wherein the effective focal length f of the optical lens and the real image height IH corresponding to the maximum field angle satisfy: 1.0< IH/f <2.3.
4. The optical lens as claimed in claim 1, wherein the maximum field angle FOV and the true image height IH corresponding to the maximum field angle of the optical lens and the aperture D of the first lens object side face 1 The three parts are as follows: d is 0.8 < 1 /IH/tan(FOV/2)＜2.8。
5. The optical lens of claim 1, wherein an effective focal length f of the optical lens is equal to a focal length f of the first lens 1 The method meets the following conditions: -2.5<f 1 /f<-1.7。
6. The optical lens of claim 1, wherein an effective focal length f of the optical lens and a focal length f of the second lens 2 The method meets the following conditions: -20.0<f 2 /f<-3.0。
7. The optical lens of claim 1, wherein an effective focal length f of the optical lens and a focal length f of the third lens 3 The method meets the following conditions: 2.0<f 3 /f<5.0。
8. The optical lens of claim 1, wherein an effective focal length f of the optical lens and a focal length f of the fourth lens 4 The method meets the following conditions: 1.0<f 4 /f<2.6。
9. The optical lens of claim 1, wherein an effective focal length f of the optical lens and a focal length f of the fifth lens 5 The method meets the following conditions: 0.5<f 5 /f<2.5。
10. The optical lens of claim 1, wherein an effective focal length f of the optical lens and a focal length f of the seventh lens 7 The method meets the following conditions: f (f) 7 /f＞9.0。
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202310537417.0A CN116908994A (en) | 2023-05-15 | 2023-05-15 | optical lens |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202310537417.0A CN116908994A (en) | 2023-05-15 | 2023-05-15 | optical lens |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CN116908994A true CN116908994A (en) | 2023-10-20 |
Family
ID=88361007
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN202310537417.0A Pending CN116908994A (en) | 2023-05-15 | 2023-05-15 | optical lens |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN116908994A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN117369094A (en) * | 2023-12-07 | 2024-01-09 | 联创电子科技股份有限公司 | Optical lens |
-
2023
- 2023-05-15 CN CN202310537417.0A patent/CN116908994A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN117369094A (en) * | 2023-12-07 | 2024-01-09 | 联创电子科技股份有限公司 | Optical lens |
| CN117369094B (en) * | 2023-12-07 | 2024-03-19 | 联创电子科技股份有限公司 | Optical lens |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN116908994A (en) | optical lens | |
| CN117452607A (en) | Optical lens | |
| CN116841019B (en) | Optical lens | |
| CN116256875B (en) | optical lens | |
| CN117492181A (en) | Optical lens | |
| CN116203705B (en) | optical lens | |
| CN116027518B (en) | Optical lens | |
| CN116859549A (en) | Optical lens | |
| CN116184640B (en) | optical lens | |
| CN117389008B (en) | Optical lens | |
| CN116256874B (en) | optical lens | |
| CN116577915B (en) | optical lens | |
| CN117289437B (en) | Optical lens | |
| CN117471657B (en) | Optical lens | |
| CN117310944B (en) | Optical lens | |
| CN117471656B (en) | Optical lens | |
| CN116577914B (en) | optical lens | |
| CN116520538A (en) | Optical lens | |
| CN117666087A (en) | Optical lens | |
| CN118011603A (en) | Optical lens | |
| CN116520539A (en) | Optical lens | |
| CN118151347A (en) | Optical lens | |
| CN117741917A (en) | Optical lens | |
| CN116974048A (en) | Optical lens | |
| CN117666088A (en) | Optical lens |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PB01 | Publication | ||
| PB01 | Publication | ||
| SE01 | Entry into force of request for substantive examination | ||
| SE01 | Entry into force of request for substantive examination |