CN115128769A - Optical lens - Google Patents
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- CN115128769A CN115128769A CN202211060184.1A CN202211060184A CN115128769A CN 115128769 A CN115128769 A CN 115128769A CN 202211060184 A CN202211060184 A CN 202211060184A CN 115128769 A CN115128769 A CN 115128769A
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/001—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
- G02B13/0015—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design
- G02B13/002—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface
- G02B13/0045—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface having five or more lenses
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/001—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
- G02B13/0055—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras employing a special optical element
- G02B13/006—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras employing a special optical element at least one element being a compound optical element, e.g. cemented elements
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Abstract
The invention provides an optical lens, which comprises seven lenses in total, wherein the seven lenses are sequentially arranged from an object side to an imaging surface along an optical axis: a first lens having a negative optical power; a diaphragm; a second lens having a positive optical power; a third lens having a positive refractive power, an object-side surface of which is convex; a fourth lens having a negative refractive power, an image-side surface of which is concave; a fifth lens element with negative refractive power having a convex object-side surface and a concave image-side surface; a sixth lens element having a positive refractive power, wherein both the object-side surface and the image-side surface are convex; a seventh lens having a negative optical power; the effective focal length f of the optical lens and the real image height IH corresponding to the maximum field angle satisfy that: IH/f is more than 0.6 and less than 0.8. The optical lens has the advantages of long focus, miniaturization, low cost, high resolution and capability of being used in weak light and severe environment.
Description
Technical Field
The invention relates to the technical field of imaging lenses, in particular to an optical lens.
Background
With the rapid development of Advanced Driving Assistance Systems (ADAS), optical lenses have been more widely applied and developed. The method comprises a vehicle data recorder, automatic parking, front vehicle collision early warning (FCW), lane departure early warning (LDW), pedestrian detection early warning (PCW) and the like.
The focal length of the lens required in the long-distance imaging is longer, but the longer focal length causes the total length of the lens to be longer, which is not beneficial to the miniaturization of the lens. Meanwhile, the lens needs a larger aperture, so that the lens has good imaging quality at night or in an environment with weak illumination conditions. Therefore, it is necessary to develop an optical lens that has a long focus, is small in size, has a low cost, has high resolution, and can be used in a low-light and severe environment.
Disclosure of Invention
In view of the above problems, an object of the present invention is to provide an optical lens having advantages of a long focal length, a small size, a low cost, a high resolution, and a capability of being used in a low light and a severe environment.
In order to achieve the purpose, the technical scheme of the invention is as follows:
an optical lens comprises seven lenses, in order from an object side to an image plane along an optical axis:
a first lens having a negative optical power;
a diaphragm;
a second lens having positive optical power;
a third lens having a positive refractive power, an object-side surface of which is convex;
a fourth lens having a negative refractive power, an image-side surface of which is concave;
a fifth lens element with negative refractive power having a convex object-side surface and a concave image-side surface;
a sixth lens element having a positive refractive power, wherein both the object-side surface and the image-side surface are convex;
a seventh lens having a negative optical power;
the effective focal length f of the optical lens and the real image height IH corresponding to the maximum field angle satisfy that: IH/f is more than 0.6 and less than 0.8.
Preferably, the total optical length TTL and the effective focal length f of the optical lens satisfy: TTL/f is less than 2.0.
Preferably, the entrance pupil diameter EPD of the optical lens and the real image height IH corresponding to the maximum field angle satisfy: IH/EPD is more than 1.0 and less than 1.3.
Preferably, the optical back focus BFL and the effective focal length f of the optical lens satisfy: 0.15 is less than BFL/f.
Preferably, the effective focal length f of the optical lens and the focal length f of the first lens are equal 1 Satisfies the following conditions: -25.0 < f 1 /f＜0。
Preferably, the effective focal length f of the optical lensFocal length f of the fifth lens 5 Satisfies the following conditions: -25.0 < f 5 /f＜0。
Preferably, the image-side surface of the fourth lens has a radius of curvature R 8 And the object side curvature radius R of the fifth lens 9 Satisfies the following conditions: r is more than 0.4 8 /R 9 ＜1.7。
Preferably, a real image height IH corresponding to a maximum field angle of the optical lens and an object-side aperture diameter D of the first lens element 1 Satisfies the following conditions: 1.0 < D 1 /IH＜1.3。
Preferably, sago of sagittal height of object side of the seventh lens 13 And the light-transmitting semi-aperture d of the object side surface of the seventh lens 13 Satisfies the following conditions: -0.4 < SAG 13 /d 13 ＜0。
Preferably, the total optical length TTL of the optical lens and the sum Σ CT of the central thicknesses of the first lens element to the seventh lens element along the optical axis satisfy: 0.5 <. sigma CT/TTL < 0.6.
Compared with the prior art, the invention has the beneficial effects that: the optical lens disclosed by the application combines the lens shape and the focal power between the lenses through reasonable collocation, realizes the effects of long focus, miniaturization, low cost, high resolution and capability of being used under weak light and severe environment.
Additional aspects and advantages of the invention will be set forth in part in the description which follows and, in part, will be obvious from the description, or may be learned by practice of the invention.
Drawings
The above and/or additional aspects and advantages of the present invention will become apparent and readily appreciated from the following description of the embodiments, taken in conjunction with the accompanying drawings of which:
fig. 1 is a schematic structural diagram of an optical lens system according to embodiment 1 of the present invention;
fig. 2 is a field curvature graph of the optical lens in embodiment 1 of the present invention;
FIG. 3 is a graph showing F-tan θ distortion of an optical lens in example 1 of the present invention;
fig. 4 is a graph showing a relative illumination of an optical lens in embodiment 1 of the present invention;
fig. 5 is a MTF graph of the optical lens in embodiment 1 of the present invention;
fig. 6 is a graph showing axial aberration of the optical lens in embodiment 1 of the present invention;
fig. 7 is a vertical axis chromatic aberration curve diagram of the optical lens in embodiment 1 of the present invention;
fig. 8 is a schematic structural diagram of an optical lens system according to embodiment 2 of the present invention;
fig. 9 is a graph of curvature of field of the optical lens in embodiment 2 of the present invention;
FIG. 10 is a graph showing F-tan θ distortion of an optical lens in example 2 of the present invention;
fig. 11 is a graph showing a relative illumination of an optical lens in embodiment 2 of the present invention;
fig. 12 is a MTF graph of an optical lens in embodiment 2 of the present invention;
fig. 13 is a graph showing axial aberration of the optical lens in embodiment 2 of the present invention;
fig. 14 is a vertical axis chromatic aberration curve diagram of the optical lens in embodiment 2 of the present invention;
fig. 15 is a schematic structural view of an optical lens system according to embodiment 3 of the present invention;
fig. 16 is a graph of curvature of field of the optical lens in embodiment 3 of the present invention;
FIG. 17 is a graph showing F-tan θ distortion of an optical lens in embodiment 3 of the present invention;
fig. 18 is a graph showing a relative illuminance curve of the optical lens in embodiment 3 of the present invention;
fig. 19 is a MTF graph of an optical lens in embodiment 3 of the present invention;
FIG. 20 is a graph showing axial aberrations of an optical lens according to embodiment 3 of the present invention;
FIG. 21 is a vertical axis chromatic aberration diagram of an optical lens in embodiment 3 of the present invention;
fig. 22 is a schematic structural diagram of an optical lens system according to embodiment 4 of the present invention;
FIG. 23 is a graph of curvature of field of an optical lens in embodiment 4 of the present invention;
FIG. 24 is a graph showing F-tan θ distortion of an optical lens in embodiment 4 of the present invention;
fig. 25 is a graph showing the relative illuminance of the optical lens in embodiment 4 of the present invention;
fig. 26 is a MTF graph of the optical lens in embodiment 4 of the present invention;
fig. 27 is a graph showing axial aberration of the optical lens in embodiment 4 of the present invention;
fig. 28 is a vertical axis chromatic aberration diagram of the optical lens in embodiment 4 of the present invention.
The following detailed description will further illustrate the invention in conjunction with the above-described figures.
Detailed Description
For a better understanding of the present application, various aspects of the present application will be described in more detail with reference to the accompanying drawings. It should be understood that the detailed description is merely illustrative of embodiments of the application and does not 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 this specification, the expressions first, second, third, etc. are used only to distinguish one feature from another, and do not represent any limitation on the features. Thus, the first lens discussed below may also be referred to as the second lens or the third lens without departing from the teachings of the present invention.
In the drawings, the thickness, size and shape of the lens have been slightly exaggerated for convenience of explanation. In particular, the shapes of the spherical or aspherical surfaces shown in the drawings are shown by way of example. That is, the shape of the spherical surface or the aspherical surface is not limited to the shape of the spherical surface or the aspherical surface shown in the drawings. The figures are purely diagrammatic and not drawn to scale.
Herein, the paraxial region refers to a region near the optical axis. If the lens surface is convex and the convex position is not defined, it means that the lens surface is convex at least in the paraxial region; if the lens surface is concave and the concave position is not defined, it means that the lens surface is concave at least in the paraxial region. The surface of each lens closest to the object is called the object side surface of the lens, and the surface of each lens closest to the imaging surface is called the image side surface of the lens.
It will be further understood that the terms "comprises," "comprising," "has," "having," "includes" 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. Moreover, when a statement such as "at least one of" appears after a list of listed features, the entirety of the listed features is modified rather than modifying individual elements in the list. Furthermore, the use of "may" mean "one or more embodiments of the application" when describing 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 the embodiments and features of the embodiments in the present application may be combined with each other without conflict. The present application will be described in detail below with reference to the accompanying drawings in conjunction with embodiments.
The optical lens according to the embodiment of the present invention includes, in order from an object side to an image side: the lens comprises a first lens, a diaphragm, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens and a seventh lens.
In some embodiments, the first lens element may have a negative refractive power, so as to avoid excessive divergence of the object-side light rays, which is beneficial for controlling the aperture of the rear lens element.
In some embodiments, the second lens may have a positive focal power, which is beneficial to reduce the working aperture of the optical lens while converging light rays, thereby being beneficial to miniaturization of the optical lens.
In some embodiments, the third lens element may have a positive focal power, which is advantageous for converging light rays and reducing the deflection angle of the light rays, so that the light rays are smoothly transitioned. The object side surface of the third lens is a convex surface, and light rays with marginal field of view can be converged, so that the converged light rays smoothly enter the rear end of the optical lens, and the imaging quality of the optical lens is improved.
In some embodiments, the fourth lens element may have a negative focal power, which is beneficial to increase an imaging area of the optical lens and improve the imaging quality of the optical lens. The image side surface of the fourth lens is a concave surface, so that light rays of the marginal field of view can be collected, various high-order aberrations caused by excessive divergence of the light rays are avoided, and the imaging quality of the optical lens is improved.
In some embodiments, the fifth lens element may have a negative focal power, which is beneficial to increase of the imaging area of the optical lens, and thus, the phenomenon of too large light deflection caused by too concentrated negative focal power of the fourth lens element is avoided, the difficulty of aberration correction of the optical lens is reduced, and the imaging quality of the optical lens is improved. The fifth lens element has a convex object-side surface and a concave image-side surface, so that more light rays can be transmitted to the rear end of the optical lens element, and the generation of various aberrations can be reduced, thereby increasing the imaging area of the optical lens element and improving the imaging quality of the optical lens element.
In some embodiments, the sixth lens element may have positive refractive power, which is favorable for converging light rays and reducing the deflection angle of the light rays, so that the light rays are in smooth transition. The object side surface and the image side surface of the sixth lens are convex surfaces, so that light rays can be converged, and the illumination of the optical lens can be improved, so that the brightness of the optical lens at the image surface can be improved, and the dark corner can be avoided.
In some embodiments, the seventh lens element may have a negative refractive power, which is beneficial to increase an imaging area of the optical lens and improve the imaging quality of the optical lens.
In some embodiments, the third lens and the fourth lens can be cemented to form a cemented lens, which can effectively correct chromatic aberration of the optical lens, reduce eccentricity sensitivity of the optical lens, balance aberration of the optical lens, and improve imaging quality of the optical lens; the assembly sensitivity of the optical lens can be reduced, the processing difficulty of the optical lens is further reduced, and the assembly yield of the optical lens is improved.
In some embodiments, a diaphragm for limiting the light beam may be disposed between the first lens and the second lens, and the diaphragm may be disposed near an object-side surface of the second lens, so as to reduce generation of ghost of the optical lens, and to facilitate converging light entering the optical system and reduce a rear aperture of the optical lens.
In some embodiments, the aperture value FNO of the optical lens satisfies: FNO is less than or equal to 1.6. The range is satisfied, the large aperture characteristic is favorably realized, and the image definition can be ensured in a low-light environment or at night.
In some embodiments, the maximum field angle FOV of the optical lens satisfies: FOV < 40 deg. The long-focus characteristic is favorably realized by meeting the range, so that the far scene information can be acquired, and the requirement of the optical lens on the detection of the far scene is met.
In some embodiments, the incident angle CRA of the maximum field angle chief ray of the optical lens on the image plane satisfies: CRA < 25 deg. Satisfying the above range, the allowable error value between the CRA of the optical lens and the CRA of the chip photosensitive element can be made larger, and the adaptability of the optical lens to the image sensor can be improved.
In some embodiments, the total optical length TTL and the effective focal length f of the optical lens satisfy: TTL/f is less than 2.0. The optical lens can effectively limit the length of the lens and is beneficial to realizing the miniaturization of the optical lens.
In some embodiments, the real image height IH corresponding to the maximum field angle and the effective focal length f of the optical lens satisfy: IH/f is more than 0.6 and less than 0.8. Satisfying the above range can make the optical lens not only give consideration to the large image plane characteristics, but also have good imaging quality.
In some embodiments, the optical back focus BFL and the effective focal length f of the optical lens satisfy: BFL/f is not less than 0.15. The method meets the range, is favorable for obtaining balance between good imaging quality and easy-to-assemble optical back focal length, and reduces the difficulty of the camera module assembly process while ensuring the imaging quality of the optical lens.
In some embodiments, the real image height IH of the optical lens corresponding to the maximum field angle and the entrance pupil diameter EPD satisfy: IH/EPD is more than 1.0 and less than 1.3. The width of the light ray bundle entering the optical lens can be increased, so that the brightness of the optical lens at the image surface is improved, and the dark corner is avoided.
In some embodiments, the effective focal length f of the optical lens and the focal length f of the first lens are different 1 Satisfies the following conditions: -25.0 < f 1 The/f is less than 0. Satisfying the above range, the first lens element can have a suitable negative focal power, and the object-side light can be prevented from being too much diverged, which is beneficial to controlling the aperture of the rear lens element.
In some embodiments, the effective focal length f of the optical lens and the focal length f of the second lens are different 2 Satisfies the following conditions: f is more than 0 2 The/f is less than 2.0. The second lens has appropriate positive focal power, so that the working aperture of the optical lens is reduced by converging light rays, the spherical aberration of the optical lens is 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 third lens are different 3 Satisfies the following conditions: f is more than 0 3 The/f is less than 2.0. The third lens has appropriate positive focal power, so that light can be smoothly transited, various aberrations of the optical lens are corrected, 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 are 4 Satisfies the following conditions: -1.5 < f 4 The/f is less than 0. Satisfying above-mentioned scope, can making the fourth lens have appropriate negative power, be favorable to increasing optical lens's image area, correct optical lens's coma and astigmatism simultaneously, promote optical lens's image quality.
In some embodiments, the effective focal length f of the optical lens and the focal length f of the fifth lens 5 Satisfies the following conditions: -25.0 < f 5 The/f is less than 0. The fifth lens has appropriate negative focal power, light can be smoothly transited, spherical aberration and field curvature of the optical lens are corrected, and 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 sixth lens 6 Satisfies the following conditions: f is more than 0 6 /fIs less than 1.0. Satisfy above-mentioned scope, can make the sixth lens have appropriate positive focal power, be favorable to the smooth transition of light, correct optical lens's coma and field curvature simultaneously, promote optical lens's imaging quality.
In some embodiments, the effective focal length f of the optical lens and the focal length f of the seventh lens 7 Satisfies the following conditions: -1.0 < f 7 The/f is less than 0. The seventh lens has appropriate negative focal power, the imaging area of the optical lens can be increased, various aberrations of the optical lens can be corrected, and the imaging quality of the optical lens can be improved.
In some embodiments, the effective focal length f of the optical lens and the radius of curvature R of the object-side surface of the first lens element 1 Radius of curvature R of image-side surface 2 Respectively satisfy: | R 1 /f|＜16.0；|R 2 The/| is less than 9.0. The method meets the range, can reduce the caliber of the front end of the optical lens, can moderately increase the distortion, and is suitable for the condition that a front small-range picture needs to be mainly observed in an enlarged mode.
In some embodiments, the fourth lens has a radius of curvature of image side R 8 And the object side radius of curvature R of the fifth lens 9 Satisfies the following conditions: r is more than 0.4 8 /R 9 Is less than 1.7. The optical lens system has the advantages that the image side surface of the fourth lens and the object side surface of the fifth lens can obtain similar surface types, the influence of field curvature on the optical lens is favorably reduced, and the imaging quality of the optical lens is improved.
In some embodiments, the fifth lens has a radius of curvature of the object side R 9 Radius of curvature R of image side surface 10 Satisfies the following conditions: r is more than 1.0 9 /R 10 Is less than 1.3. The optical lens has the advantages that the range is met, the image side surface and the object side surface of the fifth lens can be in a similar surface type, the influence of field curvature on the optical lens is favorably reduced, and the imaging quality of the optical lens is improved.
In some embodiments, the fifth lens has a radius of curvature of image side R 10 And the object side curvature radius R of the sixth lens 11 Satisfies the following conditions: r is more than 0.4 10 /R 11 Is less than 1.3. The optical lens meets the range, can ensure that the image side surface of the fifth lens and the object side surface of the sixth lens have similar surface types, and is favorable for reducing the field curvature to the optical lensThe influence of the head improves the imaging quality of the optical lens.
In some embodiments, the real image height IH corresponding to the maximum field angle of the optical lens and the object-side aperture D of the first lens 1 Satisfies the following conditions: 1.0 < D 1 IH is less than 1.3. The range is satisfied, balance between a large image surface at the imaging end and a small aperture at the object side is obtained, the imaging quality of the optical lens is ensured, and the aperture at the front end is reduced.
In some embodiments, SAGs of the seventh lens object side 13 And the light-transmitting semi-aperture d of the object side surface of the seventh lens 13 Satisfies the following conditions: -0.4 < SAG 13 /d 13 Is less than 0. Satisfy above-mentioned scope, can effectively retrain the face type of seventh lens object side off-axis visual field, guarantee that marginal visual field light has sufficient deflection angle when passing through the seventh lens, guarantee that the incident angle when light incides to the image forming surface is less to ensure that optical lens has great relative illuminance, promote optical lens's imaging quality.
In some embodiments, the total optical length TTL of the optical lens and the sum Σ CT of the central thicknesses of the first lens to the seventh lens along the optical axis, respectively, satisfy: 0.5 <. sigma CT/TTL < 0.6. The optical lens structure meets the range, can effectively compress the total length of the optical lens, and is beneficial to the structural design and the production process of the optical lens.
In order to make the system have better optical performance, a plurality of aspheric lenses are adopted in the lens, and the surface shapes of the aspheric surfaces of the optical lens satisfy the following equation:
wherein z is the distance between the curved surface and the vertex of the curved surface in the direction of the optical axis, h is the distance between the optical axis and the curved surface, c is the curvature of the vertex of the curved surface, K is the coefficient of the quadric surface, and A, B, C, D, E, F are the coefficients of the second order, the fourth order, the sixth order, the eighth order, the tenth order, and the twelfth order.
The invention is further illustrated below in the following examples. In various embodiments, the thickness, the curvature radius, and the material selection of each lens in the optical lens are different, and the specific differences can be referred to in the parameter tables of the various embodiments. The following examples are only preferred embodiments of the present invention, but the embodiments of the present invention are not limited only by the following examples, and any other changes, substitutions, combinations or simplifications which do not depart from the innovative points of the present invention should be construed as being equivalent substitutions and shall be included within the scope of the present invention.
Example 1
Referring to fig. 1, a schematic structural diagram of an optical lens system according to embodiment 1 of the present invention is shown, the optical lens system sequentially includes, from an object side to an image plane along an optical axis: a first lens L1, a diaphragm ST, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6, a seventh lens L7, a filter G1, and a protection glass G2.
The first lens L1 has negative power, and both the object-side surface S1 and the image-side surface S2 are concave;
a diaphragm ST;
the second lens L2 has positive power, and both the object-side surface S3 and the image-side surface S4 are convex;
the third lens L3 has positive power, and both the object-side surface S5 and the image-side surface S6 are convex;
the fourth lens L4 has negative power, and both the object-side surface S7 and the image-side surface S8 are concave;
the fifth lens element L5 has negative power, and has a convex object-side surface S9 and a concave image-side surface S10;
the sixth lens L6 has positive power, and both the object-side surface S11 and the image-side surface S12 are convex;
the seventh lens element L7 has negative power, and has a concave object-side surface S13 and a convex image-side surface S14;
the third lens L3 and the fourth lens L4 can be cemented to form a cemented lens;
the object-side surface S15 and the image-side surface S16 of the filter G1 are both flat surfaces;
the object side S17 and the image side S18 of the protective glass G2 are both flat;
the image forming surface S19 is a plane.
The relevant parameters of each lens in the optical lens in example 1 are shown in table 1-1.
TABLE 1-1
The surface shape parameters of the aspherical lens of the optical lens in example 1 are shown in table 1-2.
Tables 1 to 2
In the present embodiment, a field curvature graph, an F-tan θ distortion graph, a relative illumination graph, an MTF graph, an axial aberration graph, and a vertical axis chromatic aberration graph of the optical lens are respectively shown in fig. 2, fig. 3, fig. 4, fig. 5, fig. 6, and fig. 7.
Fig. 2 shows a field curvature 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, with the horizontal axis indicating a shift amount (unit: mm) and the vertical axis indicating a half field angle (unit: °). As can be seen from the figure, the field curvature of the meridional image plane and the sagittal image plane is controlled within +/-0.09 mm, which shows that the optical lens can well correct the field curvature.
Fig. 3 shows an F-tan θ distortion curve of example 1, which shows the F-tan θ distortion of light rays of different wavelengths at different image heights on an image forming plane, with the horizontal axis showing the F-tan θ distortion (unit:%) and the vertical axis showing the half field angle (unit:%). As can be seen from the figure, the F-tan theta distortion of the optical lens is controlled within +/-3%, which shows that the optical lens can excellently correct the F-tan theta distortion.
Fig. 4 shows a relative illuminance curve of example 1, which represents relative illuminance values at different angles of field of view on the imaging plane, with the horizontal axis representing the half field angle (unit: °) and the vertical axis representing the relative illuminance (unit:%). As can be seen from the figure, the relative illuminance value of the optical lens is still greater than 90% at the maximum half field angle, indicating that the optical lens has excellent relative illuminance.
Fig. 5 shows MTF (modulation transfer function) graphs of embodiment 1, which represent the degree of modulation of lens imaging at different spatial frequencies for each field of view, with the horizontal axis representing the spatial frequency (unit: lp/mm) and the vertical axis representing the MTF value. As can be seen from the figure, the MTF value of the embodiment is more than 0.3 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 has good imaging quality and good detail resolution capability under the conditions of low frequency and high frequency.
Fig. 6 shows an axial aberration curve of example 1, which represents the aberration on the optical axis at the imaging plane for each wavelength, with the horizontal axis representing the axial aberration value (unit: μm) and the vertical axis representing the normalized pupil radius. As can be seen from the figure, the shift amount of the axial aberration is controlled within ± 30 μm, which indicates that the optical lens can correct the axial aberration well.
Fig. 7 shows a vertical axis chromatic aberration curve of example 1, which shows chromatic aberration at different image heights on an image forming plane for each wavelength with respect to a center wavelength (0.55 μm), the horizontal axis shows a vertical axis chromatic aberration value (unit: μm) for each wavelength with respect to the center wavelength, and the vertical axis shows a normalized angle of view. As can be seen from the figure, the vertical axis chromatic aberration of the longest wavelength and the shortest wavelength is controlled within +/-4 mu m, which shows that the optical lens can effectively correct the chromatic aberration of the marginal field of view and the secondary spectrum of the whole image plane.
Example 2
Referring to fig. 8, a schematic structural diagram of an optical lens system according to embodiment 2 of the present invention is shown, the optical lens system sequentially includes, from an object side to an image plane along an optical axis: a first lens L1, a stop ST, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6, a seventh lens L7, a filter G1, and a cover glass G2.
The first lens L1 has negative power, and both the object-side surface S1 and the image-side surface S2 are concave;
a diaphragm ST;
the second lens L2 has positive power, and has a concave object-side surface S3 and a convex image-side surface S4;
the third lens element L3 has positive power, and has a convex object-side surface S5 and a concave image-side surface S6;
the fourth lens element L4 has negative power, and has a convex object-side surface S7 and a concave image-side surface S8;
the fifth lens element L5 has negative power, and has a convex object-side surface S9 and a concave image-side surface S10;
the sixth lens L6 has positive power, and both the object-side surface S11 and the image-side surface S12 are convex;
the seventh lens element L7 has negative power, and has a convex object-side surface S13 and a concave image-side surface S14;
the third lens L3 and the fourth lens L4 may be cemented to form a cemented lens.
The relevant parameters of each lens in the optical lens in embodiment 2 are shown in table 2-1.
TABLE 2-1
The surface shape parameters of the aspherical lens of the optical lens in example 2 are shown in table 2-2.
Tables 2 to 2
In the present embodiment, a field curvature graph, an F-tan θ distortion curve, a relative illumination graph, an MTF graph, an axial aberration graph, and a vertical axis chromatic aberration graph of the optical lens are respectively shown in fig. 9, fig. 10, fig. 11, fig. 12, fig. 13, and fig. 14.
Fig. 9 shows a field curvature curve of example 2, which shows the degree of curvature of light rays of different wavelengths on a meridional image plane and a sagittal image plane, with the horizontal axis representing the amount of displacement (unit: mm) and the vertical axis representing the half field angle (unit: °). As can be seen from the figure, the field curvature of the meridional image plane and the sagittal image plane is controlled within ± 0.04mm, which indicates that the optical lens can correct the field curvature well.
Fig. 10 shows an F-tan θ distortion curve of example 2, which shows F-tan θ distortions at different image heights on an image forming plane for light rays of different wavelengths, with the abscissa representing the F-tan θ distortion (unit:%) and the ordinate representing the half field angle (unit: °). As can be seen from the figure, the F-tan theta distortion of the optical lens is controlled within + -3%, which shows that the optical lens can excellently correct the F-tan theta distortion.
Fig. 11 shows a relative illuminance curve of example 2, which represents relative illuminance values at different angles of field of view on an imaging plane, with the horizontal axis representing a half field angle (unit: °) and the vertical axis representing the relative illuminance (unit:%). As can be seen from the figure, the relative illuminance value of the optical lens is still greater than 90% at the maximum half field angle, indicating that the optical lens has excellent relative illuminance.
Fig. 12 shows MTF (modulation transfer function) graphs of embodiment 2, which represent the degree of modulation of lens imaging at different spatial frequencies for each field of view, with the horizontal axis representing the spatial frequency (unit: lp/mm) and the vertical axis representing the MTF value. As can be seen from the figure, the MTF value of the embodiment is 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 from the center to the edge field of view, and the image quality and the detail resolution capability are excellent under the conditions of low frequency and high frequency.
Fig. 13 shows an axial aberration curve of example 2, which represents the aberration on the optical axis at the imaging plane for each wavelength, with the horizontal axis representing the axial aberration value (unit: μm) and the vertical axis representing the normalized pupil radius. As can be seen from the figure, the amount of shift of the axial aberration is controlled within ± 14 μm, indicating that the optical lens can correct the axial aberration well.
Fig. 14 shows a vertical axis chromatic aberration curve of example 2, which shows chromatic aberration at different image heights on an image forming plane for each wavelength with respect to a center wavelength (0.55 μm), the horizontal axis shows a vertical axis chromatic aberration value (unit: μm) for each wavelength with respect to the center wavelength, and the vertical axis shows a normalized angle of view. As can be seen from the figure, the vertical axis chromatic aberration of the longest wavelength and the shortest wavelength is controlled within +/-3 mu m, which shows that the optical lens can effectively correct the chromatic aberration of the marginal field of view and the secondary spectrum of the whole image plane.
Example 3
Referring to fig. 15, a schematic structural diagram of an optical lens system according to embodiment 3 of the present invention is shown, the optical lens system sequentially includes, from an object side to an image plane along an optical axis: a first lens L1, a stop ST, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6, a seventh lens L7, a filter G1, and a cover glass G2.
The first lens element L1 has negative power, and has a convex object-side surface S1 and a concave image-side surface S2;
a diaphragm ST;
the second lens L2 has positive power, and has a convex object-side surface S3 and a concave image-side surface S4;
the third lens L3 has positive power, and both the object-side surface S5 and the image-side surface S6 are convex;
the fourth lens L4 has negative power, and both the object-side surface S7 and the image-side surface S8 are concave;
the fifth lens element L5 has negative power, and has a convex object-side surface S9 and a concave image-side surface S10;
the sixth lens L6 has positive power, and both the object-side surface S11 and the image-side surface S12 are convex;
the seventh lens element L7 has negative power, and has a concave object-side surface S13 and a convex image-side surface S14;
the third lens L3 and the fourth lens L4 may be cemented to form a cemented lens.
The relevant parameters of each lens in the optical lens in example 3 are shown in table 3-1.
TABLE 3-1
The surface shape parameters of the aspherical lens of the optical lens in example 3 are shown in table 3-2.
TABLE 3-2
In the present embodiment, a field curvature graph, an F-tan θ distortion curve, a relative illuminance graph, an MTF graph, an axial aberration graph, and a vertical axis chromatic aberration graph 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 shows the degree of curvature of light rays of different wavelengths on a meridional image plane and a sagittal image plane, with the horizontal axis representing the amount of displacement (unit: mm) and the vertical axis representing the half field angle (unit: °). As can be seen from the figure, the field curvature of the meridional image plane and the sagittal image plane is controlled within +/-0.06 mm, 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 shows F-tan θ distortions at different image heights on an image forming plane for light rays of different wavelengths, with the abscissa representing the F-tan θ distortion (unit:%) and the ordinate representing the half field angle (unit: °). As can be seen from the figure, the F-tan theta distortion of the optical lens is controlled within +/-0.6%, which shows that the optical lens can excellently correct the F-tan theta distortion.
Fig. 18 shows a relative illuminance curve of example 3, which represents relative illuminance values at different angles of field of view on the imaging plane, with the horizontal axis representing the half field angle (unit: °) and the vertical axis representing the relative illuminance (unit:%). As can be seen from the figure, the relative luminance value of the optical lens is still greater than 80% at the maximum half field angle, indicating that the optical lens has excellent relative luminance.
Fig. 19 shows MTF (modulation transfer function) graphs of embodiment 3, which represent the degree of modulation of lens imaging at different spatial frequencies for each field of view, with the horizontal axis representing the spatial frequency (unit: lp/mm) and the vertical axis representing the MTF value. As can be seen from the figure, the MTF value of the embodiment is 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 from the center to the edge field of view, and the MTF has good imaging quality and good detail resolution capability under the conditions of low frequency and high frequency.
Fig. 20 shows an axial aberration curve of example 3, which represents the aberration on the optical axis at the imaging plane for each wavelength, with the horizontal axis representing the axial aberration value (unit: μm) and the vertical axis representing the normalized pupil radius. As can be seen from the figure, the shift amount of the axial aberration is controlled within ± 21 μm, which indicates that the optical lens can correct the axial aberration well.
Fig. 21 shows a vertical axis chromatic aberration curve of example 3, which shows chromatic aberration at different image heights on an image forming plane for each wavelength with respect to a center wavelength (0.55 μm), the horizontal axis shows a vertical axis chromatic aberration value (unit: μm) for each wavelength with respect to the center wavelength, and the vertical axis shows a normalized angle of view. As can be seen from the figure, the vertical axis chromatic aberration of the longest wavelength and the shortest wavelength is controlled within +/-3 mu m, which shows that the optical lens can effectively correct the chromatic aberration of the marginal field of view and the secondary spectrum of the whole image plane.
Example 4
Referring to fig. 22, a schematic structural diagram of an optical lens system according to embodiment 4 of the present invention is shown, the optical lens system sequentially includes, from an object side to an image plane along an optical axis: a first lens L1, a stop ST, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6, a seventh lens L7, a filter G1, and a cover glass G2.
The first lens element L1 has negative power, and has a concave object-side surface S1 and a convex image-side surface S2;
a diaphragm ST;
the second lens L2 has positive power, and both the object-side surface S3 and the image-side surface S4 are convex;
the third lens L3 has positive power, and both the object-side surface S5 and the image-side surface S6 are convex;
the fourth lens L4 has negative power, and both the object-side surface S7 and the image-side surface S8 are concave;
the fifth lens element L5 has negative power, and has a convex object-side surface S9 and a concave image-side surface S10;
the sixth lens L6 has positive power, and both the object-side surface S11 and the image-side surface S12 are convex;
the seventh lens element L7 has negative power, and has a concave object-side surface S13 and a convex image-side surface S14;
the third lens L3 and the fourth lens L4 may be cemented to form a cemented lens.
The relevant parameters of each lens in the optical lens in example 4 are shown in table 4-1.
TABLE 4-1
The surface shape parameters of the aspherical lens of the optical lens in example 4 are shown in table 4-2.
TABLE 4-2
In the present embodiment, the curvature of field curve, F-tan θ distortion curve, relative illumination curve, MTF curve, axial aberration curve, and vertical axis chromatic aberration curve of the optical lens are respectively shown in fig. 23, 24, 25, 26, 27, and 28.
Fig. 23 shows a field curvature curve of example 4, which shows the degree of curvature of light rays of different wavelengths on a meridional image plane and a sagittal image plane, with the horizontal axis representing the amount of displacement (unit: mm) and the vertical axis representing the half field angle (unit: °). As can be seen from the figure, the field curvature of the meridional image plane and the sagittal image plane is controlled within +/-0.15 mm, which indicates that the optical lens can better correct the field curvature.
Fig. 24 shows an F-tan θ distortion curve of example 4, which shows F-tan θ distortions at different image heights on an image forming plane for light rays of different wavelengths, with the abscissa showing the F-tan θ distortion (unit:%) and the ordinate showing the half field angle (unit: °). As can be seen from the figure, the F-tan theta distortion of the optical lens is controlled within +/-3.6%, which shows that the optical lens can excellently correct the F-tan theta distortion.
Fig. 25 shows a relative illuminance curve of example 4, which represents relative illuminance values at different angles of field of view on the imaging plane, with the horizontal axis representing the half field angle (unit: °) and the vertical axis representing the relative illuminance (unit:%). As can be seen from the figure, the relative illuminance value of the optical lens is still greater than 90% at the maximum half field angle, indicating that the optical lens has excellent relative illuminance.
Fig. 26 shows MTF (modulation transfer function) graphs of embodiment 4, which represent the degree of modulation of lens imaging at different spatial frequencies for each field of view, with the horizontal axis representing the spatial frequency (unit: lp/mm) and the vertical axis representing the MTF value. As can be seen from the figure, the MTF value of the embodiment is more than 0.3 in the whole field of view, and in the range of 0-160 lp/mm, the MTF curve uniformly and smoothly drops in the process of the field of view from the center to the edge, and the MTF has better imaging quality and better detail resolution capability under the conditions of low frequency and high frequency.
Fig. 27 shows an axial aberration curve of example 4, which represents the aberration on the optical axis at the imaging plane for each wavelength, with the horizontal axis representing the axial aberration value (unit: μm) and the vertical axis representing the normalized pupil radius. As can be seen from the figure, the shift amount of the axial aberration is controlled within ± 30 μm, which indicates that the optical lens can correct the axial aberration well.
Fig. 28 shows a vertical axis chromatic aberration curve of example 4, which shows chromatic aberration at different image heights on an image forming plane for each wavelength with respect to a center wavelength (0.55 μm), the horizontal axis shows a vertical axis chromatic aberration value (unit: μm) for each wavelength with respect to the center wavelength, and the vertical axis shows a normalized angle of view. As can be seen from the figure, the vertical axis chromatic aberration of the longest wavelength and the shortest wavelength is controlled within +/-3 mu m, which shows that the optical lens can excellently correct the chromatic aberration of the marginal field of view and the secondary spectrum of the whole image surface.
Please refer to table 5, which shows the corresponding optical characteristics of the above embodiments, including the effective focal length f, the total optical length TTL, the aperture FNO, the real image height IH, and the maximum field angle FOV of the optical lens, and the corresponding values of each conditional expression in the embodiments.
TABLE 5
In summary, the optical lens according to the embodiments of the present invention, by reasonably matching the combination of the lens shape and the focal power between the lenses, achieves the effects of both miniaturization and high resolution at a low cost, and can be used in low light and severe environments.
In the description herein, references to the description of the term "one embodiment," "some embodiments," "an example," "a specific example," or "some examples," etc., mean 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 invention. In this specification, the schematic representations of the terms used above do not necessarily refer to the same embodiment or example. 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 are merely illustrative of several embodiments of the present invention, and the description thereof is more specific and detailed, but not to be construed as limiting the scope of the invention. It should be noted that, for those skilled in the art, various changes and modifications can be made without departing from the spirit of the invention, and these changes and modifications are all within the scope of the invention. Therefore, the protection scope of the present invention should be subject to the appended claims.
Claims (10)
1. An optical lens system comprising seven lens elements, in order from an object side to an image plane along an optical axis:
a first lens having a negative optical power;
a diaphragm;
a second lens having a positive optical power;
a third lens having a positive refractive power, an object-side surface of which is convex;
a fourth lens with negative focal power, wherein the image side surface of the fourth lens is a concave surface;
a fifth lens element with negative refractive power having a convex object-side surface and a concave image-side surface;
a sixth lens element having a positive refractive power, wherein both the object-side surface and the image-side surface are convex;
a seventh lens having a negative optical power;
the effective focal length f of the optical lens and the real image height IH corresponding to the maximum field angle satisfy that: IH/f is more than 0.6 and less than 0.8.
2. An optical lens according to claim 1, wherein the total optical length TTL and the effective focal length f satisfy: TTL/f is less than 2.0.
3. The optical lens of claim 1, wherein an entrance pupil diameter EPD of the optical lens satisfies a real image height IH corresponding to a maximum field angle: IH/EPD is more than 1.0 and less than 1.3.
4. An optical lens according to claim 1, characterized in that the optical back focus BFL of the optical lens and the effective focal length f satisfy: 0.15 is less than BFL/f.
5. An optical lens according to claim 1, characterized in that the effective focal length f of the optical lens and the focal length f of the first lens are 1 Satisfies the following conditions: -25.0 < f 1 /f＜0。
6. An optical lens according to claim 1, characterized in that the effective focal length f of the optical lens and the focal length f of the fifth lens 5 Satisfies the following conditions: -25.0 < f 5 /f＜0。
7. An optical lens barrel according to claim 1, wherein the fourth lens has an image side surface curvature radius R 8 And the object side curvature radius R of the fifth lens 9 Satisfies the following conditions: r is more than 0.4 8 /R 9 ＜1.7。
8. The optical lens barrel according to claim 1, wherein a real image height IH corresponding to a maximum field angle of the optical lens barrel and an object-side light-passing aperture D of the first lens element 1 Satisfies the following conditions: 1.0 < D 1 /IH＜1.3。
9. The optical lens of claim 1, wherein a sagittal height SAG of an object-side surface of the seventh lens 13 A light-passing semi-aperture d with the object side surface of the seventh lens 13 Satisfies the following conditions: -0.4 < SAG 13 /d 13 ＜0。
10. An optical lens according to claim 1, wherein a total optical length TTL of the optical lens and a sum Σ CT of central thicknesses of the first lens to the seventh lens along an optical axis, respectively, satisfy: 0.5 <. sigma CT/TTL < 0.6.
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Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN116643388A (en) * | 2023-07-24 | 2023-08-25 | 江西联益光学有限公司 | optical lens |
| CN117406398A (en) * | 2023-12-14 | 2024-01-16 | 江西联创电子有限公司 | Optical lens |
| WO2024046456A1 (en) * | 2022-09-01 | 2024-03-07 | 江西联创电子有限公司 | Optical lens |
Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN106990510A (en) * | 2017-06-02 | 2017-07-28 | 浙江舜宇光学有限公司 | Optical imaging system |
| CN110908093A (en) * | 2019-12-30 | 2020-03-24 | 浙江舜宇光学有限公司 | Optical imaging lens |
| CN112346208A (en) * | 2019-08-09 | 2021-02-09 | 华为技术有限公司 | Large-aperture lens and terminal equipment |
| CN112731630A (en) * | 2021-03-31 | 2021-04-30 | 江西联创电子有限公司 | Optical imaging lens |
| US20210255429A1 (en) * | 2020-02-14 | 2021-08-19 | Largan Precision Co., Ltd. | Imaging optical lens assembly, image capturing unit and electronic device |
| WO2022082512A1 (en) * | 2020-10-21 | 2022-04-28 | 欧菲光集团股份有限公司 | Optical imaging system, imaging module, and electronic apparatus |
-
2022
- 2022-09-01 CN CN202211060184.1A patent/CN115128769B/en active Active
Patent Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN106990510A (en) * | 2017-06-02 | 2017-07-28 | 浙江舜宇光学有限公司 | Optical imaging system |
| CN112346208A (en) * | 2019-08-09 | 2021-02-09 | 华为技术有限公司 | Large-aperture lens and terminal equipment |
| CN110908093A (en) * | 2019-12-30 | 2020-03-24 | 浙江舜宇光学有限公司 | Optical imaging lens |
| US20210255429A1 (en) * | 2020-02-14 | 2021-08-19 | Largan Precision Co., Ltd. | Imaging optical lens assembly, image capturing unit and electronic device |
| WO2022082512A1 (en) * | 2020-10-21 | 2022-04-28 | 欧菲光集团股份有限公司 | Optical imaging system, imaging module, and electronic apparatus |
| CN112731630A (en) * | 2021-03-31 | 2021-04-30 | 江西联创电子有限公司 | Optical imaging lens |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2024046456A1 (en) * | 2022-09-01 | 2024-03-07 | 江西联创电子有限公司 | Optical lens |
| CN116643388A (en) * | 2023-07-24 | 2023-08-25 | 江西联益光学有限公司 | optical lens |
| CN116643388B (en) * | 2023-07-24 | 2023-11-14 | 江西联益光学有限公司 | optical lens |
| CN117406398A (en) * | 2023-12-14 | 2024-01-16 | 江西联创电子有限公司 | Optical lens |
| CN117406398B (en) * | 2023-12-14 | 2024-03-08 | 江西联创电子有限公司 | Optical lens |
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