CN110703412B - Optical imaging system - Google Patents

Optical imaging system Download PDF

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CN110703412B
CN110703412B CN201910847937.5A CN201910847937A CN110703412B CN 110703412 B CN110703412 B CN 110703412B CN 201910847937 A CN201910847937 A CN 201910847937A CN 110703412 B CN110703412 B CN 110703412B
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lens
imaging system
optical imaging
optical
image
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CN110703412A (en
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张凯元
游兴海
黄林
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Zhejiang Sunny Optics Co Ltd
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Zhejiang Sunny Optics Co Ltd
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • G02B13/001Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
    • G02B13/0015Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design
    • G02B13/002Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface
    • G02B13/0045Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface having five or more lenses
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • G02B13/18Optical objectives specially designed for the purposes specified below with lenses having one or more non-spherical faces, e.g. for reducing geometrical aberration

Abstract

The application discloses an optical imaging system, this optical imaging system includes from the object side to the image side along the optical axis in order: the lens includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens. The first lens has positive focal power, the object side surface of the first lens is a convex surface, and the image side surface of the first lens is a concave surface; the second lens has negative focal power, the object side surface of the second lens is a convex surface, and the image side surface of the second lens is a concave surface; the third lens has focal power, and the object side surface of the third lens is a convex surface, and the image side surface of the third lens is a concave surface; the fourth lens has positive focal power; the fifth lens has focal power; the sixth lens has focal power; the seventh lens element has a negative focal power, and has a convex object-side surface and a concave image-side surface. The effective focal length f4 of the fourth lens and the total effective focal length f of the optical imaging system satisfy 2.5 ≤ f4/f < 6.

Description

Optical imaging system
Divisional application
The application is a divisional application of a Chinese patent application with the invention name of 'optical imaging system' and the application number of 201810746763.9 filed on 2018, 07 and 09.
Technical Field
The present application relates to an optical imaging system, and more particularly, to an optical imaging system including seven lenses.
Background
With the development of science and technology, portable electronic products are gradually emerging, and portable electronic products with a camera shooting function are more popular, so that the market demand for camera lenses suitable for portable electronic products is gradually increased. On one hand, since portable electronic products such as smart phones tend to be miniaturized, the total length of the lens is limited, thereby increasing the design difficulty of the lens. On the other hand, with the improvement of performance and the reduction of size of a common photosensitive element such as a photosensitive coupling element (CCD) or a Complementary Metal Oxide Semiconductor (CMOS), the number of pixels of the photosensitive element is increased and the size of the pixels is reduced, so that higher requirements are placed on high imaging quality and miniaturization of a matched imaging lens.
In order to meet the requirement of miniaturization, the F-number (F-number) of the conventional lens is usually set to 2.0 or more than 2.0, so as to achieve both miniaturization and good optical performance. However, with the continuous development of portable electronic products such as smart phones, higher requirements are put forward on the camera lenses used in cooperation, and particularly, under the conditions of insufficient light (such as rainy days, dusk, and the like) and shaking hands, the lenses with F number of 2.0 or more than 2.0 cannot meet higher-order imaging requirements.
Disclosure of Invention
The present application provides an optical imaging system, such as a large aperture imaging lens, that may be applicable to portable electronic products and that may address at least one of the above-identified shortcomings in the prior art.
An aspect of the present application provides an optical imaging system, in order from an object side to an image side along an optical axis, comprising: the lens includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens. The first lens can have positive focal power, and the object side surface of the first lens can be a convex surface, and the image side surface of the first lens can be a concave surface; the second lens can have negative focal power, and the object side surface of the second lens can be a convex surface, and the image side surface of the second lens can be a concave surface; the third lens has focal power, and the object side surface of the third lens can be a convex surface, and the image side surface of the third lens can be a concave surface; the fourth lens may have a positive optical power; the fifth lens has focal power; the sixth lens has focal power; the seventh lens element can have a negative power, and can have a convex object-side surface and a concave image-side surface. The effective focal length f4 of the fourth lens and the total effective focal length f of the optical imaging system can satisfy f4/f < 6 > which is more than or equal to 2.5.
In one embodiment, the total effective focal length f of the optical imaging system and the maximum half field angle HFOV of the optical system may satisfy 3.8mm < f tau (HFOV) < 4.5 mm.
In one embodiment, the fourth lens and the fifth lens are separated by a distance T45 on the optical axisThe total effective focal length f of the imaging system and the maximum half field angle HFOV of the optical system can meet 0.85mm2≤T45*f*TAN(HFOV)≤3.1mm2
In one embodiment, the effective focal length f1 of the first lens, the effective focal length f2 of the second lens and the total effective focal length f of the optical imaging system can satisfy-2 < f1/f + f2/f < -0.5.
In one embodiment, the effective focal length f4 of the fourth lens and the total effective focal length f of the optical imaging system can satisfy 2.5 ≦ f4/f < 6.
In one embodiment, the effective focal length f7 of the seventh lens and the total effective focal length f of the optical imaging system can satisfy-2.5 < f7/f < -1.
In one embodiment, the radius of curvature R1 of the object-side surface of the first lens and the radius of curvature R2 of the image-side surface of the first lens may satisfy 0.1 < R1/R2 < 0.3.
In one embodiment, the radius of curvature R3 of the object-side surface of the second lens and the radius of curvature R4 of the image-side surface of the second lens may satisfy 0.2 < R4/R3 < 0.5.
In one embodiment, the radius of curvature of the object-side surface of the third lens, R5, R6, R13, and R14 may satisfy 1 < (R5+ R6)/(R13+ R14) < 2.
In one embodiment, the central thickness CT1 of the first lens on the optical axis, the central thickness CT2 of the second lens on the optical axis, and the central thickness CT3 of the third lens on the optical axis may satisfy 1.5 < CT1/(CT2+ CT3) < 2.
In one embodiment, the central thickness CT4 of the fourth lens on the optical axis, the central thickness CT5 of the fifth lens on the optical axis, the central thickness CT6 of the sixth lens on the optical axis and the central thickness CT7 of the seventh lens on the optical axis may satisfy 1 ≦ (CT7+ CT6)/(CT5+ CT4) < 2.
In one embodiment, a combined focal length f1234 of the first, second, third, and fourth lenses and a combined focal length f567 of the fifth, sixth, and seventh lenses may satisfy 1 < | f567/f1234| < 2.5.
In one embodiment, a sum Σ AT of a maximum effective radius DT31 of the object-side surface of the third lens and a separation distance on the optical axis of any adjacent two lenses of the first lens to the seventh lens may satisfy 0.5 < DT31/∑ AT < 1.
In one embodiment, the total effective focal length f of the optical imaging system and the entrance pupil diameter EPD of the optical imaging system may satisfy f/EPD ≦ 1.8.
In one embodiment, a distance TTL between an object side surface of the first lens element and an imaging surface of the optical imaging system on an optical axis and a half ImgH of a diagonal length of an effective pixel area on the imaging surface of the optical imaging system may satisfy TTL/ImgH < 1.5.
The optical imaging system adopts a plurality of lenses (for example, seven lenses), and has at least one beneficial effect of ultra-thinness, miniaturization, large aperture, high imaging quality and the like by reasonably distributing the focal power, the surface type, the central thickness of each lens, the on-axis distance between each lens and the like.
Drawings
Other features, objects, and advantages of the present application will become more apparent from the following detailed description of non-limiting embodiments when taken in conjunction with the accompanying drawings. In the drawings:
fig. 1 shows a schematic configuration diagram of an optical imaging system according to embodiment 1 of the present application;
fig. 2A to 2D show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a magnification chromatic aberration curve, respectively, of the optical imaging system of embodiment 1;
fig. 3 shows a schematic configuration diagram of an optical imaging system according to embodiment 2 of the present application;
fig. 4A to 4D show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a chromatic aberration of magnification curve, respectively, of the optical imaging system of embodiment 2;
fig. 5 shows a schematic configuration diagram of an optical imaging system according to embodiment 3 of the present application;
fig. 6A to 6D show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a chromatic aberration of magnification curve, respectively, of the optical imaging system of embodiment 3;
fig. 7 shows a schematic configuration diagram of an optical imaging system according to embodiment 4 of the present application;
fig. 8A to 8D show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a chromatic aberration of magnification curve, respectively, of the optical imaging system of embodiment 4;
fig. 9 shows a schematic configuration diagram of an optical imaging system according to embodiment 5 of the present application;
fig. 10A to 10D show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a chromatic aberration of magnification curve, respectively, of the optical imaging system of embodiment 5;
fig. 11 shows a schematic configuration diagram of an optical imaging system according to embodiment 6 of the present application;
fig. 12A to 12D show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a chromatic aberration of magnification curve, respectively, of the optical imaging system of embodiment 6;
fig. 13 is a schematic structural view showing an optical imaging system according to embodiment 7 of the present application;
fig. 14A to 14D show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a chromatic aberration of magnification curve, respectively, of the optical imaging system of embodiment 7;
fig. 15 shows a schematic configuration diagram of an optical imaging system according to embodiment 8 of the present application;
fig. 16A to 16D show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a chromatic aberration of magnification curve, respectively, of the optical imaging system of embodiment 8;
fig. 17 is a schematic structural view showing an optical imaging system according to embodiment 9 of the present application;
fig. 18A to 18D show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a chromatic aberration of magnification curve, respectively, of an optical imaging system of example 9;
fig. 19 is a schematic configuration diagram showing an optical imaging system according to embodiment 10 of the present application;
fig. 20A to 20D show an on-axis chromatic aberration curve, an astigmatism curve, a distortion curve, and a chromatic aberration of magnification curve, respectively, of the optical imaging system of embodiment 10.
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 exemplary embodiments of the present application and does not limit the scope of the present 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 application.
In the drawings, the thickness, size, and shape of the lens have been slightly exaggerated for convenience of explanation. In particular, the shapes of the spherical or aspherical surfaces shown in the drawings are shown by way of example. That is, the shape of the spherical surface or the aspherical surface is not limited to the shape of the spherical surface or the aspherical surface shown in the drawings. The figures are purely diagrammatic and not drawn to scale.
Herein, the paraxial region refers to a region near the optical axis. If the lens surface is convex and the convex position is not defined, it means that the lens surface is convex at least in the paraxial region; if the lens surface is concave and the concave position is not defined, it means that the lens surface is concave at least in the paraxial region. In each lens, the surface closest to the object side is referred to as the object side surface of the lens; in each lens, the surface closest to the image side is referred to as 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, when describing embodiments of the present application, the use of "may" mean "one or more embodiments of the present 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 embodiments with reference to the attached drawings. The features, principles, and other aspects of the present application are described in detail below.
The optical imaging system according to the exemplary embodiment of the present application may include, for example, seven lenses having optical powers, i.e., a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens. The seven lenses are arranged in sequence from an object side to an image side along an optical axis, and an air space can be formed between any two adjacent lenses.
In an exemplary embodiment, the first lens may have a positive optical power, and the object side surface thereof may be convex and the image side surface thereof may be concave; the second lens can have negative focal power, and the object side surface of the second lens can be a convex surface, and the image side surface of the second lens can be a concave surface; the third lens has positive focal power or negative focal power, the object side surface of the third lens can be a convex surface, and the image side surface of the third lens can be a concave surface; the fourth lens may have a positive optical power; the fifth lens has positive focal power or negative focal power; the sixth lens has positive focal power or negative focal power; and the seventh lens element can have a negative power, and the object-side surface can be convex and the image-side surface can be concave. The optical imaging system has good imaging quality by reasonably limiting the surface type and the focal power of each lens.
In an exemplary embodiment, the image-side surface of the fourth lens may be convex.
In an exemplary embodiment, the object-side surface of the sixth lens element may be convex, and the image-side surface may be concave.
In an exemplary embodiment, the optical imaging system of the present application may satisfy the conditional expression f/EPD ≦ 1.8, where f is the total effective focal length of the optical imaging system and EPD is the entrance pupil diameter of the optical imaging system. More specifically, f and EPD further satisfy 1.64 ≦ f/EPD ≦ 1.79. By properly adjusting the ratio of the total effective focal length to the entrance pupil diameter of the optical imaging system, the optical imaging system is beneficial to having the characteristics of ultra-thin and large aperture.
In an exemplary embodiment, the optical imaging system of the present application may satisfy the conditional expression of 0.85mm2≤T45*f*TAN(HFOV)≤3.1mm2Where T45 is the separation distance between the fourth lens and the fifth lens on the optical axis, f is the total effective focal length of the optical imaging system, and HFOV is the maximum half field angle of the optical imaging system. More specifically, T45, f and HFOV may further satisfy 0.85mm2≤T45*f*TAN(HFOV)≤3.08mm2. Through the optimization of the spacing distance between the fourth lens and the fifth lens on the optical axis and the limitation of the image height, the imaging system can be well matched with a large image plane chip, so that the imaging system has the characteristics of high pixel, low sensitivity, easiness in processing and the like.
In an exemplary embodiment, the optical imaging system of the present application may satisfy a conditional expression TTL/ImgH < 1.5, where TTL is a distance on an optical axis from an object side surface of the first lens to an imaging surface of the optical imaging system, and ImgH is a half of a diagonal length of an effective pixel area on the imaging surface of the optical imaging system. More specifically, TTL and ImgH can further satisfy 1.40 ≦ TTL/ImgH ≦ 1.42. The characteristics of ultra-thinness and high pixel of the optical imaging system are realized by restricting the ratio of the on-axis distance from the object side surface of the first lens to the imaging surface to half of the diagonal length of the effective pixel area on the imaging surface.
In an exemplary embodiment, the optical imaging system of the present application may satisfy the conditional expression 3.8mm < f tan (HFOV) < 4.5mm, where f is the total effective focal length of the optical imaging system and HFOV is the maximum half field angle of the optical imaging system. More specifically, f and HFOV may further satisfy 3.8mm < f TAN (HFOV) < 4.0mm, for example, 3.85mm ≦ f TAN (HFOV) ≦ 3.96 mm. By reasonably distributing the total effective focal length of the optical imaging system and the maximum half field angle of the optical imaging system, the size of the system can be effectively compressed, so that the light has a smaller deflection angle, and the characteristics of large image surface, easiness in injection molding and the like are favorably realized.
In an exemplary embodiment, the optical imaging system of the present application may satisfy the conditional expression 2.5 ≦ f4/f < 6, where f4 is an effective focal length of the fourth lens, and f is a total effective focal length of the optical imaging system. More specifically, f4 and f can further satisfy 2.90. ltoreq. f 4/f. ltoreq.5.67. By reasonably controlling the ratio of the effective focal length of the fourth lens to the total effective focal length of the optical imaging system, the contribution range of the focal power of the fourth lens can be reasonably controlled, and meanwhile, the negative spherical aberration contribution rate of the fourth lens is reasonably controlled, so that the positive spherical aberration generated by each negative lens in the system can be reasonably balanced.
In an exemplary embodiment, the optical imaging system of the present application may satisfy the conditional expression-2.5 < f7/f < -1, where f7 is an effective focal length of the seventh lens, and f is a total effective focal length of the optical imaging system. More specifically, f7 and f can further satisfy-2.49. ltoreq. f 7/f. ltoreq-1.15. Through the ratio of the effective focal length of the seventh lens to the total effective focal length of the optical imaging system, the seventh lens can effectively balance spherical aberration generated by the front six lenses, further fine adjustment and control are carried out on the spherical aberration of the system, accurate control of the aberration of an on-axis field of view region is strengthened, and imaging quality is improved.
In an exemplary embodiment, the optical imaging system of the present application may satisfy the conditional expression-2 < f1/f + f2/f < -0.5, where f1 is an effective focal length of the first lens, f2 is an effective focal length of the second lens, and f is a total effective focal length of the optical imaging system. More specifically, f1, f2 and f further satisfy-1.83. ltoreq. f1/f + f 2/f. ltoreq. 0.61. The optical lens meets the conditional expression of-2 < f1/f + f2/f < -0.5, and can effectively balance negative third-order spherical aberration and positive fifth-order spherical aberration generated by the first lens and the second lens, so that the system has smaller spherical aberration, and the good imaging quality of an on-axis field area is ensured.
In an exemplary embodiment, the optical imaging system of the present application may satisfy the conditional expression 0.1 < R1/R2 < 0.3, where R1 is a radius of curvature of an object-side surface of the first lens and R2 is a radius of curvature of an image-side surface of the first lens. More specifically, R1 and R2 may further satisfy 0.16. ltoreq. R1/R2. ltoreq.0.26. By controlling the curvature radius of the object side surface and the image side surface of the first lens, the total deflection angle of light rays at the marginal field of view of the object side surface and the image side surface of the first lens can be reasonably controlled, so that the sensitivity of the system is effectively reduced.
In an exemplary embodiment, the optical imaging system of the present application may satisfy the conditional expression 0.2 < R4/R3 < 0.5, where R3 is a radius of curvature of an object-side surface of the second lens and R4 is a radius of curvature of an image-side surface of the second lens. More specifically, R3 and R4 may further satisfy 0.21. ltoreq. R4/R3. ltoreq.0.46. By limiting the ratio range of the curvature radius of the object side surface of the second lens and the curvature radius of the image side surface of the second lens, the shape of the second lens can be effectively constrained, and then the aberration contribution rate of the object side surface and the image side surface of the second lens can be effectively controlled, so that the aberration related to the aperture diaphragm in the system can be effectively balanced, and the imaging quality of the system can be effectively improved.
In an exemplary embodiment, the optical imaging system of the present application may satisfy the conditional expression 1 < (R5+ R6)/(R13+ R14) < 2, where R5 is a radius of curvature of an object-side surface of the third lens, R6 is a radius of curvature of an image-side surface of the third lens, R13 is a radius of curvature of an object-side surface of the seventh lens, and R14 is a radius of curvature of an image-side surface of the seventh lens. More specifically, R5, R6, R13 and R14 may further satisfy 1.31. ltoreq. (R5+ R6)/(R13+ R14). ltoreq.1.81. By reasonably controlling the curvature radius of the object-side surface and the image-side surface of the third lens and the curvature radius of the object-side surface and the image-side surface of the seventh lens, the incident angle of the chief ray of each field of view on the image surface can be reasonably controlled, so that the requirement on the incident angle of the chief ray in the design of an optical system is met.
In an exemplary embodiment, the optical imaging system of the present application may satisfy the conditional expression 1.5 < CT1/(CT2+ CT3) < 2, where CT1 is a central thickness of the first lens on the optical axis, CT2 is a central thickness of the second lens on the optical axis, and CT3 is a central thickness of the third lens on the optical axis. More specifically, CT1, CT2 and CT3 further satisfy 1.65. ltoreq. CT1/(CT2+ CT 3). ltoreq.1.83. The central thicknesses of the first lens, the second lens and the third lens are reasonably controlled, so that the distortion contribution amounts of the three lenses are in a reasonable range, the distortion amount of each field of view of the imaging system is controlled to be below 2%, a good imaging effect is achieved, and the requirement of later debugging is avoided.
In an exemplary embodiment, the optical imaging system of the present application may satisfy the conditional expression 1 ≦ (CT7+ CT6)/(CT5+ CT4) < 2, where CT4 is a central thickness of the fourth lens on the optical axis, CT5 is a central thickness of the fifth lens on the optical axis, CT6 is a central thickness of the sixth lens on the optical axis, and CT7 is a central thickness of the seventh lens on the optical axis. More specifically, CT4, CT5, CT6 and CT7 further satisfy 1.07 ≦ (CT7+ CT6)/(CT5+ CT4) ≦ 1.75. The center thicknesses of the fourth lens, the fifth lens, the sixth lens and the seventh lens are reasonably controlled, so that the processing performance of the imaging system is favorably ensured, and the ultrathin characteristic of the imaging system is favorably realized.
In an exemplary embodiment, the optical imaging system of the present application may satisfy the conditional expression 1 < | f567/f1234| < 2.5, where f1234 is a combined focal length of the first, second, third, and fourth lenses, and f567 is a combined focal length of the fifth, sixth, and seventh lenses. More specifically, f1234 and f567 further satisfy 1.34. ltoreq. f567/f 1234. ltoreq.2.47. By reasonably limiting the ratio range of the combined focal length of the first lens, the second lens, the third lens and the fourth lens and the combined focal length of the fifth lens, the sixth lens and the seventh lens, the excellent image quality of the optical system is ensured, and meanwhile, the good processing performance of the optical system is ensured.
In an exemplary embodiment, the optical imaging system of the present application may satisfy the conditional expression 0.5 < DT31/∑ AT < 1, where DT31 is a maximum effective radius of an object-side surface of the third lens, and Σ AT is a sum of separation distances on an optical axis of any adjacent two lenses of the first lens to the seventh lens. More specifically, DT31 and Σ AT may further satisfy 0.66 ≦ DT31/∑ AT ≦ 0.90. The ratio of the maximum effective radius of the object side surface of the third lens to the sum of the air intervals of any two adjacent lenses from the first lens to the seventh lens on the optical axis is reasonably controlled, so that the size of the lens is favorably reduced, and the miniaturization requirement is met; meanwhile, the resolution of the lens is improved.
In an exemplary embodiment, the optical imaging system may further include a diaphragm to improve the imaging quality of the imaging system. The stop may be disposed at any position between the object side and the image side as needed, for example, the stop may be disposed between the object side and the first lens.
Optionally, the optical imaging system may further include a filter for correcting color deviation and/or a protective glass for protecting the photosensitive element on the imaging surface.
The optical imaging system according to the above-described embodiment of the present application may employ a plurality of lenses, such as the seven lenses described above. By reasonably distributing the focal power, the surface type, the central thickness of each lens, the on-axis distance between each lens and the like, the volume of the system can be effectively reduced, the sensitivity of the system can be reduced, and the processability of the system can be improved, so that the optical imaging system is more favorable for production and processing and can be suitable for portable electronic products. In addition, with the optical imaging system configured as described above, there can also be advantageous effects such as ultra-thinness, miniaturization, large aperture, high imaging quality, and the like.
In the embodiment of the present application, at least one of the mirror surfaces of each lens is an aspherical mirror surface. The aspheric lens is characterized in that: the curvature varies continuously from the center of the lens to the periphery of the lens. Unlike a spherical lens having a constant curvature from the center of the lens to the periphery of the lens, an aspherical lens has better curvature radius characteristics, and has advantages of improving distortion aberration and improving astigmatic aberration. After the aspheric lens is adopted, the aberration generated during imaging can be eliminated as much as possible, thereby improving the imaging quality.
However, it will be appreciated by those skilled in the art that the number of lenses constituting the optical imaging system may be varied to achieve the various results and advantages described in the present specification without departing from the claimed subject matter. For example, although seven lenses are exemplified in the embodiment, the optical imaging system is not limited to include seven lenses. The optical imaging system may also include other numbers of lenses, if desired.
Specific examples of the optical imaging system that can be applied to the above-described embodiments are further described below with reference to the drawings.
Example 1
An optical imaging system according to embodiment 1 of the present application is described below with reference to fig. 1 to 2D. Fig. 1 shows a schematic configuration diagram of an optical imaging system according to embodiment 1 of the present application.
As shown in fig. 1, an optical imaging system according to an exemplary embodiment of the present application includes, in order from an object side to an image side along an optical axis: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, a filter E8, and an image forming surface S17.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2. The second lens element E2 has negative power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has positive power, and has a convex object-side surface S5 and a concave image-side surface S6. The fourth lens element E4 has positive power, and has a convex object-side surface S7 and a convex image-side surface S8. The fifth lens element E5 has negative power, and has a convex object-side surface S9 and a concave image-side surface S10. The sixth lens element E6 has positive power, and has a convex object-side surface S11 and a concave image-side surface S12. The seventh lens element E7 has negative power, and has a convex object-side surface S13 and a concave image-side surface S14. Filter E8 has an object side S15 and an image side S16. The light from the object sequentially passes through the respective surfaces S1 to S16 and is finally imaged on the imaging surface S17.
Table 1 shows the surface type, radius of curvature, thickness, material, and conic coefficient of each lens of the optical imaging system of example 1, wherein the unit of the radius of curvature and the thickness are both millimeters (mm).
Figure BDA0002195892910000091
TABLE 1
As can be seen from table 1, the object-side surface and the image-side surface of any one of the first lens element E1 through the seventh lens element E7 are aspheric. In the present embodiment, the profile x of each aspheric lens can be defined using, but not limited to, the following aspheric formula:
Figure BDA0002195892910000092
wherein x is the rise of the distance from the aspheric surface vertex to the aspheric surface vertex when the aspheric surface is at the position with the height of h along the optical axis direction; c is the paraxial curvature of the aspheric surface, c being 1/R (i.e., paraxial curvature c is the inverse of radius of curvature R in table 1 above); k is the conic coefficient (given in table 1); ai is the correction coefficient of the i-th order of the aspherical surface. Table 2 below shows the high-order coefficient A of each of the aspherical mirror surfaces S1 to S14 used in example 14、A6、A8、A10、A12、A14、A16、A18And A20
Figure BDA0002195892910000093
Figure BDA0002195892910000101
TABLE 2
Table 3 gives the effective focal lengths f1 to f7 of the respective lenses, the total effective focal length f of the optical imaging system, the distance TTL on the optical axis from the object side surface S1 to the imaging surface S17 of the first lens E1, half ImgH of the diagonal length of the effective pixel region on the imaging surface S17, and the maximum half field angle HFOV of the optical imaging system in embodiment 1.
f1(mm) 4.13 f7(mm) -10.54
f2(mm) -10.52 f(mm) 4.74
f3(mm) 1500.00 TTL(mm) 5.55
f4(mm) 17.32 ImgH(mm) 3.96
f5(mm) -83.42 HFOV(°) 39.7
f6(mm) 2806.57
TABLE 3
Fig. 2A shows an on-axis chromatic aberration curve of the optical imaging system of embodiment 1, which represents the deviation of the convergent focal points of light rays of different wavelengths after passing through the system. Fig. 2B shows an astigmatism curve representing meridional field curvature and sagittal field curvature of the optical imaging system of embodiment 1. Fig. 2C shows a distortion curve of the optical imaging system of embodiment 1, which represents corresponding distortion magnitude values at different image heights. Fig. 2D shows a chromatic aberration of magnification curve of the optical imaging system of embodiment 1, which represents the deviation of different image heights on the imaging plane after the light passes through the system. As can be seen from fig. 2A to 2D, the optical imaging system according to embodiment 1 can achieve good imaging quality.
Example 2
An optical imaging system according to embodiment 2 of the present application is described below with reference to fig. 3 to 4D. In this embodiment and the following embodiments, descriptions of parts similar to those of embodiment 1 will be omitted for the sake of brevity. Fig. 3 shows a schematic structural diagram of an optical imaging system according to embodiment 2 of the present application.
As shown in fig. 3, the optical imaging system according to the exemplary embodiment of the present application, in order from an object side to an image side along an optical axis, includes: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, a filter E8, and an image forming surface S17.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2. The second lens element E2 has negative power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has positive power, and has a convex object-side surface S5 and a concave image-side surface S6. The fourth lens element E4 has positive power, and has a convex object-side surface S7 and a convex image-side surface S8. The fifth lens element E5 has negative power, and has a concave object-side surface S9 and a concave image-side surface S10. The sixth lens element E6 has negative power, and has a convex object-side surface S11 and a concave image-side surface S12. The seventh lens element E7 has negative power, and has a convex object-side surface S13 and a concave image-side surface S14. Filter E8 has an object side S15 and an image side S16. The light from the object sequentially passes through the respective surfaces S1 to S16 and is finally imaged on the imaging surface S17.
Table 4 shows the surface type, radius of curvature, thickness, material, and conic coefficient of each lens of the optical imaging system of example 2, wherein the unit of the radius of curvature and the thickness are both millimeters (mm).
Figure BDA0002195892910000111
TABLE 4
As is clear from table 4, in example 2, both the object-side surface and the image-side surface of any one of the first lens element E1 through the seventh lens element E7 are aspheric. Table 5 shows high-order term coefficients that can be used for each aspherical mirror surface in example 2, wherein each aspherical mirror surface type can be defined by formula (1) given in example 1 above.
Flour mark A4 A6 A8 A10 A12 A14 A16 A18 A20
S1 1.0311E-03 -1.6364E-02 5.4797E-02 -1.0903E-01 1.3110E-01 -9.8279E-02 4.4722E-02 -1.1356E-02 1.2299E-03
S2 -2.0023E-02 5.4102E-04 -2.9465E-03 2.9770E-02 -4.8519E-02 3.7886E-02 -1.5710E-02 3.0886E-03 -1.6291E-04
S3 -1.2130E-02 5.6233E-04 3.3490E-02 -5.7428E-02 8.5260E-02 -9.4394E-02 6.5438E-02 -2.4717E-02 3.9333E-03
S4 -6.0923E-03 1.5622E-03 -7.5029E-03 4.5539E-02 -1.0989E-01 1.2172E-01 -7.7743E-02 2.6419E-02 -3.8086E-03
S5 -5.2034E-02 -2.3336E-02 6.4104E-02 -2.4305E-01 5.3104E-01 -6.9202E-01 5.3202E-01 -2.2188E-01 3.8345E-02
S6 -3.9379E-02 3.1508E-02 -2.0232E-01 7.0261E-01 -1.4530E+00 1.8811E+00 -1.4624E+00 6.2684E-01 -1.1326E-01
S7 -2.9275E-02 7.8460E-03 -5.5023E-02 9.1324E-02 -6.7049E-02 -4.4559E-02 1.2220E-01 -8.6636E-02 2.2134E-02
S8 -3.4680E-02 -5.5399E-03 -5.3232E-03 -5.7970E-03 2.3711E-02 -3.9258E-02 3.2837E-02 -1.4143E-02 2.5769E-03
S9 -3.2453E-02 4.0878E-03 -1.1833E-01 2.9157E-01 -3.7734E-01 2.8044E-01 -1.2123E-01 2.8239E-02 -2.7199E-03
S10 5.1178E-03 -1.2685E-01 1.4315E-01 -9.3869E-02 3.3074E-02 -4.0180E-03 -8.2086E-04 2.9141E-04 -2.4034E-05
S11 5.4295E-02 -1.2794E-01 9.8460E-02 -5.4215E-02 1.8268E-02 -3.3816E-03 2.9667E-04 -4.8649E-06 -6.1430E-07
S12 -1.2134E-02 -8.7445E-03 -1.1153E-03 1.6991E-03 -6.6863E-04 1.5013E-04 -1.8381E-05 1.0237E-06 -1.3407E-08
S13 -2.3222E-01 8.2142E-02 -1.7419E-02 2.7291E-03 -3.3962E-04 3.2366E-05 -2.1275E-06 8.3007E-08 -1.4241E-09
S14 -1.9478E-01 8.3440E-02 -2.9937E-02 7.6215E-03 -1.2693E-03 1.3357E-04 -8.5142E-06 2.9936E-07 -4.4481E-09
TABLE 5
Table 6 gives the effective focal lengths f1 to f7 of the respective lenses, the total effective focal length f of the optical imaging system, the distance TTL on the optical axis from the object side surface S1 to the imaging surface S17 of the first lens E1, half ImgH of the diagonal length of the effective pixel region on the imaging surface S17, and the maximum half field angle HFOV of the optical imaging system in embodiment 2.
f1(mm) 4.13 f7(mm) -10.93
f2(mm) -10.29 f(mm) 4.75
f3(mm) 1999.86 TTL(mm) 5.55
f4(mm) 16.87 ImgH(mm) 3.96
f5(mm) -146.03 HFOV(°) 39.6
f6(mm) -65.60
TABLE 6
Fig. 4A shows an on-axis chromatic aberration curve of the optical imaging system of embodiment 2, which represents the convergent focus deviation of light rays of different wavelengths after passing through the system. Fig. 4B shows an astigmatism curve representing meridional field curvature and sagittal field curvature of the optical imaging system of embodiment 2. Fig. 4C shows a distortion curve of the optical imaging system of embodiment 2, which represents corresponding distortion magnitude values at different image heights. Fig. 4D shows a chromatic aberration of magnification curve of the optical imaging system of embodiment 2, which represents the deviation of different image heights on the imaging plane after the light passes through the system. As can be seen from fig. 4A to 4D, the optical imaging system according to embodiment 2 can achieve good imaging quality.
Example 3
An optical imaging system according to embodiment 3 of the present application is described below with reference to fig. 5 to 6D. Fig. 5 shows a schematic structural diagram of an optical imaging system according to embodiment 3 of the present application.
As shown in fig. 5, the optical imaging system according to the exemplary embodiment of the present application, in order from an object side to an image side along an optical axis, includes: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, a filter E8, and an image forming surface S17.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2. The second lens element E2 has negative power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has positive power, and has a convex object-side surface S5 and a concave image-side surface S6. The fourth lens element E4 has positive power, and has a convex object-side surface S7 and a convex image-side surface S8. The fifth lens element E5 has positive power, and has a convex object-side surface S9 and a concave image-side surface S10. The sixth lens element E6 has negative power, and has a convex object-side surface S11 and a concave image-side surface S12. The seventh lens element E7 has negative power, and has a convex object-side surface S13 and a concave image-side surface S14. Filter E8 has an object side S15 and an image side S16. The light from the object sequentially passes through the respective surfaces S1 to S16 and is finally imaged on the imaging surface S17.
Table 7 shows the surface type, radius of curvature, thickness, material, and conic coefficient of each lens of the optical imaging system of example 3, wherein the unit of the radius of curvature and the thickness are both millimeters (mm).
Figure BDA0002195892910000131
TABLE 7
As is clear from table 7, in example 3, both the object-side surface and the image-side surface of any one of the first lens E1 through the seventh lens E7 are aspheric. Table 8 shows high-order term coefficients that can be used for each aspherical mirror surface in example 3, wherein each aspherical mirror surface type can be defined by formula (1) given in example 1 above.
Flour mark A4 A6 A8 A10 A12 A14 A16 A18 A20
S1 1.0348E-03 -1.6452E-02 5.5190E-02 -1.1001E-01 1.3252E-01 -9.9517E-02 4.5366E-02 -1.1541E-02 1.2521E-03
S2 -2.0089E-02 5.4367E-04 -2.9657E-03 3.0014E-02 -4.8995E-02 3.8320E-02 -1.5916E-02 3.1341E-03 -1.6558E-04
S3 -1.2355E-02 5.7803E-04 3.4742E-02 -6.0126E-02 9.0088E-02 -1.0066E-01 7.0425E-02 -2.6846E-02 4.3115E-03
S4 -6.1509E-03 1.5848E-03 -7.6481E-03 4.6643E-02 -1.1310E-01 1.2588E-01 -8.0781E-02 2.7583E-02 -3.9955E-03
S5 -5.2431E-02 -2.3603E-02 6.5086E-02 -2.4771E-01 5.4328E-01 -7.1067E-01 5.4844E-01 -2.2960E-01 3.9829E-02
S6 -3.9904E-02 3.2140E-02 -2.0774E-01 7.2626E-01 -1.5119E+00 1.9704E+00 -1.5420E+00 6.6533E-01 -1.2101E-01
S7 -2.9801E-02 8.0581E-03 -5.7016E-02 9.5476E-02 -7.0723E-02 -4.7420E-02 1.3121E-01 -9.3855E-02 2.4193E-02
S8 -3.5226E-02 -5.6713E-03 -5.4921E-03 -6.0277E-03 2.4848E-02 -4.1463E-02 3.4953E-02 -1.5173E-02 2.7862E-03
S9 -3.2492E-02 4.0951E-03 -1.1861E-01 2.9244E-01 -3.7868E-01 2.8160E-01 -1.2181E-01 2.8390E-02 -2.7360E-03
S10 5.0415E-03 -1.2403E-01 1.3891E-01 -9.0410E-02 3.1616E-02 -3.8122E-03 -7.7299E-04 2.7237E-04 -2.2295E-05
S11 5.5574E-02 -1.3249E-01 1.0315E-01 -5.7464E-02 1.9590E-02 -3.6688E-03 3.2563E-04 -5.4023E-06 -6.9015E-07
S12 -1.2674E-02 -9.3352E-03 -1.2169E-03 1.8947E-03 -7.6201E-04 1.7486E-04 -2.1882E-05 1.2455E-06 -1.6671E-08
S13 -2.3959E-01 8.6085E-02 -1.8543E-02 2.9509E-03 -3.7300E-04 3.6108E-05 -2.4108E-06 9.5541E-08 -1.6650E-09
S14 -2.0547E-01 9.0399E-02 -3.3312E-02 8.7102E-03 -1.4899E-03 1.6102E-04 -1.0542E-05 3.8068E-07 -5.8096E-09
TABLE 8
Table 9 gives the effective focal lengths f1 to f7 of the respective lenses, the total effective focal length f of the optical imaging system, the distance TTL on the optical axis from the object side surface S1 to the imaging surface S17 of the first lens E1, half ImgH of the diagonal length of the effective pixel region on the imaging surface S17, and the maximum half field angle HFOV of the optical imaging system in embodiment 3.
f1(mm) 4.15 f7(mm) -10.34
f2(mm) -10.39 f(mm) 4.74
f3(mm) 431.04 TTL(mm) 5.55
f4(mm) 18.10 ImgH(mm) 3.96
f5(mm) 1600.00 HFOV(°) 39.7
f6(mm) -134.38
TABLE 9
Fig. 6A shows an on-axis chromatic aberration curve of the optical imaging system of embodiment 3, which represents the convergent focus deviation of light rays of different wavelengths after passing through the system. Fig. 6B shows an astigmatism curve representing meridional field curvature and sagittal field curvature of the optical imaging system of embodiment 3. Fig. 6C shows a distortion curve of the optical imaging system of embodiment 3, which represents corresponding distortion magnitude values at different image heights. Fig. 6D shows a chromatic aberration of magnification curve of the optical imaging system of embodiment 3, which represents the deviation of different image heights on the imaging plane after the light passes through the system. As can be seen from fig. 6A to 6D, the optical imaging system according to embodiment 3 can achieve good imaging quality.
Example 4
An optical imaging system according to embodiment 4 of the present application is described below with reference to fig. 7 to 8D. Fig. 7 shows a schematic structural diagram of an optical imaging system according to embodiment 4 of the present application.
As shown in fig. 7, the optical imaging system according to the exemplary embodiment of the present application, in order from an object side to an image side along an optical axis, includes: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, a filter E8, and an image forming surface S17.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2. The second lens element E2 has negative power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has positive power, and has a convex object-side surface S5 and a concave image-side surface S6. The fourth lens element E4 has positive power, and has a convex object-side surface S7 and a convex image-side surface S8. The fifth lens element E5 has positive power, and has a concave object-side surface S9 and a convex image-side surface S10. The sixth lens element E6 has positive power, and has a convex object-side surface S11 and a concave image-side surface S12. The seventh lens element E7 has negative power, and has a convex object-side surface S13 and a concave image-side surface S14. Filter E8 has an object side S15 and an image side S16. The light from the object sequentially passes through the respective surfaces S1 to S16 and is finally imaged on the imaging surface S17.
Table 10 shows the surface type, radius of curvature, thickness, material, and conic coefficient of each lens of the optical imaging system of example 4, wherein the unit of the radius of curvature and the thickness are both millimeters (mm).
Figure BDA0002195892910000141
Figure BDA0002195892910000151
Watch 10
As can be seen from table 10, in example 4, both the object-side surface and the image-side surface of any one of the first lens element E1 through the seventh lens element E7 are aspheric. Table 11 shows high-order term coefficients that can be used for each aspherical mirror surface in embodiment 4, wherein each aspherical mirror surface type can be defined by the formula (1) given in embodiment 1 above.
Flour mark A4 A6 A8 A10 A12 A14 A16 A18 A20
S1 1.0215E-03 -1.6136E-02 5.3784E-02 -1.0652E-01 1.2749E-01 -9.5122E-02 4.3084E-02 -1.0890E-02 1.1739E-03
S2 -1.9533E-02 5.2127E-04 -2.8040E-03 2.7981E-02 -4.5042E-02 3.4737E-02 -1.4227E-02 2.7625E-03 -1.4392E-04
S3 -1.1991E-02 5.5264E-04 3.2722E-02 -5.5789E-02 8.2347E-02 -9.0642E-02 6.2474E-02 -2.3461E-02 3.7119E-03
S4 -6.1269E-03 1.5755E-03 -7.5885E-03 4.6189E-02 -1.1178E-01 1.2416E-01 -7.9525E-02 2.7101E-02 -3.9180E-03
S5 -5.1497E-02 -2.2975E-02 6.2788E-02 -2.3683E-01 5.1477E-01 -6.6735E-01 5.1040E-01 -2.1176E-01 3.6407E-02
S6 -3.9591E-02 3.1763E-02 -2.0450E-01 7.1212E-01 -1.4766E+00 1.9169E+00 -1.4942E+00 6.4219E-01 -1.1635E-01
S7 -2.9832E-02 8.0709E-03 -5.7136E-02 9.5729E-02 -7.0948E-02 -4.7596E-02 1.3177E-01 -9.4302E-02 2.4321E-02
S8 -3.4924E-02 -5.5984E-03 -5.3982E-03 -5.8993E-03 2.4214E-02 -4.0231E-02 3.3769E-02 -1.4595E-02 2.6687E-03
S9 -3.2254E-02 4.0501E-03 -1.1688E-01 2.8711E-01 -3.7042E-01 2.7444E-01 -1.1828E-01 2.7466E-02 -2.6372E-03
S10 5.1101E-03 -1.2657E-01 1.4272E-01 -9.3517E-02 3.2925E-02 -3.9969E-03 -8.1594E-04 2.8945E-04 -2.3854E-05
S11 5.5322E-02 -1.3159E-01 1.0222E-01 -5.6815E-02 1.9325E-02 -3.6109E-03 3.1977E-04 -5.2929E-06 -6.7465E-07
S12 -1.2608E-02 -9.2625E-03 -1.2042E-03 1.8702E-03 -7.5020E-04 1.7170E-04 -2.1430E-05 1.2166E-06 -1.6243E-08
S13 -2.4537E-01 8.9216E-02 -1.9448E-02 3.1319E-03 -4.0063E-04 3.9247E-05 -2.6518E-06 1.0635E-07 -1.8756E-09
S14 -2.1444E-01 9.6383E-02 -3.6284E-02 9.6920E-03 -1.6936E-03 1.8699E-04 -1.2507E-05 4.6138E-07 -7.1932E-09
TABLE 11
Table 12 gives the effective focal lengths f1 to f7 of the respective lenses, the total effective focal length f of the optical imaging system, the distance TTL on the optical axis from the object side surface S1 to the imaging surface S17 of the first lens E1, half ImgH of the diagonal length of the effective pixel region on the imaging surface S17, and the maximum half field angle HFOV of the optical imaging system in embodiment 4.
f1(mm) 4.10 f7(mm) -9.66
f2(mm) -9.29 f(mm) 4.74
f3(mm) 111.82 TTL(mm) 5.55
f4(mm) 18.13 ImgH(mm) 3.96
f5(mm) 298.74 HFOV(°) 39.6
f6(mm) 600.03
TABLE 12
Fig. 8A shows an on-axis chromatic aberration curve of the optical imaging system of embodiment 4, which represents the convergent focus deviation of light rays of different wavelengths after passing through the system. Fig. 8B shows an astigmatism curve representing meridional field curvature and sagittal field curvature of the optical imaging system of embodiment 4. Fig. 8C shows a distortion curve of the optical imaging system of embodiment 4, which represents the corresponding distortion magnitude values at different image heights. Fig. 8D shows a chromatic aberration of magnification curve of the optical imaging system of embodiment 4, which represents the deviation of different image heights on the imaging plane after the light passes through the system. As can be seen from fig. 8A to 8D, the optical imaging system according to embodiment 4 can achieve good imaging quality.
Example 5
An optical imaging system according to embodiment 5 of the present application is described below with reference to fig. 9 to 10D. Fig. 9 shows a schematic structural diagram of an optical imaging system according to embodiment 5 of the present application.
As shown in fig. 9, the optical imaging system according to the exemplary embodiment of the present application, in order from an object side to an image side along an optical axis, includes: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, a filter E8, and an image forming surface S17.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2. The second lens element E2 has negative power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has negative power, and has a convex object-side surface S5 and a concave image-side surface S6. The fourth lens element E4 has positive power, and has a convex object-side surface S7 and a convex image-side surface S8. The fifth lens element E5 has positive power, and has a concave object-side surface S9 and a convex image-side surface S10. The sixth lens element E6 has positive power, and has a convex object-side surface S11 and a concave image-side surface S12. The seventh lens element E7 has negative power, and has a convex object-side surface S13 and a concave image-side surface S14. Filter E8 has an object side S15 and an image side S16. The light from the object sequentially passes through the respective surfaces S1 to S16 and is finally imaged on the imaging surface S17.
Table 13 shows the surface type, radius of curvature, thickness, material, and conic coefficient of each lens of the optical imaging system of example 5, wherein the unit of the radius of curvature and the thickness are both millimeters (mm).
Figure BDA0002195892910000161
Figure BDA0002195892910000171
Watch 13
As is clear from table 13, in example 5, both the object-side surface and the image-side surface of any one of the first lens element E1 through the seventh lens element E7 are aspheric. Table 14 shows high-order term coefficients that can be used for each aspherical mirror surface in example 5, wherein each aspherical mirror surface type can be defined by formula (1) given in example 1 above.
Flour mark A4 A6 A8 A10 A12 A14 A16 A18 A20
S1 1.0241E-03 -1.6197E-02 5.4054E-02 -1.0718E-01 1.2844E-01 -9.5958E-02 4.3516E-02 -1.1013E-02 1.1886E-03
S2 -1.8958E-02 4.9840E-04 -2.6411E-03 2.5965E-02 -4.1176E-02 3.1284E-02 -1.2623E-02 2.4146E-03 -1.2393E-04
S3 -1.2581E-02 5.9397E-04 3.6025E-02 -6.2914E-02 9.5125E-02 -1.0725E-01 7.5723E-02 -2.9128E-02 4.7206E-03
S4 -5.9508E-03 1.5081E-03 -7.1586E-03 4.2942E-02 -1.0241E-01 1.1212E-01 -7.0771E-02 2.3769E-02 -3.3865E-03
S5 -5.1001E-02 -2.2644E-02 6.1584E-02 -2.3116E-01 5.0003E-01 -6.4511E-01 4.9101E-01 -2.0273E-01 3.4686E-02
S6 -3.8683E-02 3.0677E-02 -1.9523E-01 6.7200E-01 -1.3774E+00 1.7674E+00 -1.3618E+00 5.7854E-01 -1.0361E-01
S7 -2.9953E-02 8.1200E-03 -5.7600E-02 9.6701E-02 -7.1814E-02 -4.8274E-02 1.3391E-01 -9.6033E-02 2.4818E-02
S8 -3.6076E-02 -5.8777E-03 -5.7603E-03 -6.3980E-03 2.6691E-02 -4.5072E-02 3.8451E-02 -1.6891E-02 3.1389E-03
S9 -3.1289E-02 3.8697E-03 -1.0999E-01 2.6611E-01 -3.3815E-01 2.4676E-01 -1.0475E-01 2.3956E-02 -2.2656E-03
S10 5.2381E-03 -1.3135E-01 1.4996E-01 -9.9485E-02 3.5462E-02 -4.3585E-03 -9.0083E-04 3.2354E-04 -2.6996E-05
S11 5.4403E-02 -1.2832E-01 9.8852E-02 -5.4484E-02 1.8377E-02 -3.4052E-03 2.9904E-04 -4.9085E-06 -6.2043E-07
S12 -1.2086E-02 -8.6926E-03 -1.1065E-03 1.6824E-03 -6.6072E-04 1.4806E-04 -1.8092E-05 1.0056E-06 -1.3144E-08
S13 -2.4071E-01 8.6688E-02 -1.8716E-02 2.9854E-03 -3.7825E-04 3.6701E-05 -2.4561E-06 9.7564E-08 -1.7042E-09
S14 -2.1441E-01 9.6365E-02 -3.6275E-02 9.6890E-03 -1.6930E-03 1.8691E-04 -1.2500E-05 4.6113E-07 -7.1888E-09
TABLE 14
Table 15 gives the effective focal lengths f1 to f7 of the respective lenses, the total effective focal length f of the optical imaging system, the distance TTL on the optical axis from the object side surface S1 to the imaging surface S17 of the first lens E1, half ImgH of the diagonal length of the effective pixel region on the imaging surface S17, and the maximum half field angle HFOV of the optical imaging system in example 5.
Figure BDA0002195892910000172
Figure BDA0002195892910000181
Watch 15
Fig. 10A shows an on-axis chromatic aberration curve of the optical imaging system of embodiment 5, which represents the convergent focus deviation of light rays of different wavelengths after passing through the system. Fig. 10B shows an astigmatism curve representing meridional field curvature and sagittal field curvature of the optical imaging system of example 5. Fig. 10C shows a distortion curve of the optical imaging system of example 5, which represents the distortion magnitude values in the case of different viewing angles. Fig. 10D shows a chromatic aberration of magnification curve of the optical imaging system of embodiment 5, which represents the deviation of different image heights on the imaging plane after the light passes through the system. As can be seen from fig. 10A to 10D, the optical imaging system according to embodiment 5 can achieve good imaging quality.
Example 6
An optical imaging system according to embodiment 6 of the present application is described below with reference to fig. 11 to 12D. Fig. 11 shows a schematic configuration diagram of an optical imaging system according to embodiment 6 of the present application.
As shown in fig. 11, the optical imaging system according to the exemplary embodiment of the present application, in order from an object side to an image side along an optical axis, includes: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, a filter E8, and an image forming surface S17.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2. The second lens element E2 has negative power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has negative power, and has a convex object-side surface S5 and a concave image-side surface S6. The fourth lens element E4 has positive power, and has a convex object-side surface S7 and a convex image-side surface S8. The fifth lens element E5 has negative power, and has a concave object-side surface S9 and a convex image-side surface S10. The sixth lens element E6 has positive power, and has a convex object-side surface S11 and a concave image-side surface S12. The seventh lens element E7 has negative power, and has a convex object-side surface S13 and a concave image-side surface S14. Filter E8 has an object side S15 and an image side S16. The light from the object sequentially passes through the respective surfaces S1 to S16 and is finally imaged on the imaging surface S17.
Table 16 shows the surface type, radius of curvature, thickness, material, and conic coefficient of each lens of the optical imaging system of example 6, wherein the unit of the radius of curvature and the thickness are both millimeters (mm).
Figure BDA0002195892910000182
Figure BDA0002195892910000191
TABLE 16
As is clear from table 16, in example 6, both the object-side surface and the image-side surface of any one of the first lens E1 to the seventh lens E7 are aspheric. Table 17 shows high-order term coefficients that can be used for each aspherical mirror surface in example 6, wherein each aspherical mirror surface type can be defined by formula (1) given in example 1 above.
Flour mark A4 A6 A8 A10 A12 A14 A16 A18 A20
S1 1.0284E-03 -1.6299E-02 5.4511E-02 -1.0832E-01 1.3008E-01 -9.7382E-02 4.4256E-02 -1.1223E-02 1.2139E-03
S2 -1.9666E-02 5.2658E-04 -2.8421E-03 2.8458E-02 -4.5964E-02 3.5568E-02 -1.4617E-02 2.8478E-03 -1.4886E-04
S3 -1.2079E-02 5.5879E-04 3.3208E-02 -5.6826E-02 8.4189E-02 -9.3011E-02 6.4344E-02 -2.4253E-02 3.8513E-03
S4 -5.9518E-03 1.5085E-03 -7.1610E-03 4.2960E-02 -1.0247E-01 1.1218E-01 -7.0819E-02 2.3787E-02 -3.3894E-03
S5 -5.1341E-02 -2.2871E-02 6.2408E-02 -2.3504E-01 5.1011E-01 -6.6030E-01 5.0424E-01 -2.0889E-01 3.5859E-02
S6 -3.8184E-02 3.0085E-02 -1.9022E-01 6.5051E-01 -1.3247E+00 1.6888E+00 -1.2928E+00 5.4567E-01 -9.7088E-02
S7 -2.8701E-02 7.6163E-03 -5.2886E-02 8.6911E-02 -6.3180E-02 -4.1574E-02 1.1289E-01 -7.9246E-02 2.0047E-02
S8 -3.2553E-02 -5.0381E-03 -4.6901E-03 -4.9484E-03 1.9609E-02 -3.1455E-02 2.5491E-02 -1.0637E-02 1.8777E-03
S9 -2.7618E-02 3.2091E-03 -8.5692E-02 1.9479E-01 -2.3255E-01 1.5943E-01 -6.3581E-02 1.3662E-02 -1.2139E-03
S10 5.6562E-03 -1.4739E-01 1.7486E-01 -1.2054E-01 4.4650E-02 -5.7026E-03 -1.2248E-03 4.5711E-04 -3.9634E-05
S11 5.7699E-02 -1.4016E-01 1.1119E-01 -6.3116E-02 2.1924E-02 -4.1837E-03 3.7837E-04 -6.3961E-06 -8.3259E-07
S12 -1.2651E-02 -9.3098E-03 -1.2124E-03 1.8861E-03 -7.5788E-04 1.7376E-04 -2.1723E-05 1.2353E-06 -1.6521E-08
S13 -2.5532E-01 9.4698E-02 -2.1057E-02 3.4592E-03 -4.5137E-04 4.5106E-05 -3.1089E-06 1.2718E-07 -2.2881E-09
S14 -2.2233E-01 1.0175E-01 -3.9005E-02 1.0609E-02 -1.8877E-03 2.1222E-04 -1.4453E-05 5.4291E-07 -8.6187E-09
TABLE 17
Table 18 gives the effective focal lengths f1 to f7 of the respective lenses, the total effective focal length f of the optical imaging system, the distance TTL on the optical axis from the object side surface S1 to the imaging surface S17 of the first lens E1, half ImgH of the diagonal length of the effective pixel region on the imaging surface S17, and the maximum half field angle HFOV of the optical imaging system in example 6.
f1(mm) 4.31 f7(mm) -11.40
f2(mm) -11.91 f(mm) 4.73
f3(mm) -800.00 TTL(mm) 5.55
f4(mm) 17.74 ImgH(mm) 3.90
f5(mm) -800.00 HFOV(°) 39.4
f6(mm) 1240.00
Watch 18
Fig. 12A shows an on-axis chromatic aberration curve of the optical imaging system of example 6, which represents the convergent focus deviation of light rays of different wavelengths after passing through the system. Fig. 12B shows an astigmatism curve representing meridional field curvature and sagittal field curvature of the optical imaging system of example 6. Fig. 12C shows a distortion curve of the optical imaging system of embodiment 6, which represents the corresponding distortion magnitude values at different image heights. Fig. 12D shows a chromatic aberration of magnification curve of the optical imaging system of example 6, which represents the deviation of different image heights on the imaging plane after the light passes through the system. As can be seen from fig. 12A to 12D, the optical imaging system according to embodiment 6 can achieve good imaging quality.
Example 7
An optical imaging system according to embodiment 7 of the present application is described below with reference to fig. 13 to 14D. Fig. 13 shows a schematic configuration diagram of an optical imaging system according to embodiment 7 of the present application.
As shown in fig. 13, the optical imaging system according to the exemplary embodiment of the present application, in order from an object side to an image side along an optical axis, includes: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, a filter E8, and an image forming surface S17.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2. The second lens element E2 has negative power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has negative power, and has a convex object-side surface S5 and a concave image-side surface S6. The fourth lens element E4 has positive power, and has a concave object-side surface S7 and a convex image-side surface S8. The fifth lens element E5 has negative power, and has a concave object-side surface S9 and a convex image-side surface S10. The sixth lens element E6 has negative power, and has a convex object-side surface S11 and a concave image-side surface S12. The seventh lens element E7 has negative power, and has a convex object-side surface S13 and a concave image-side surface S14. Filter E8 has an object side S15 and an image side S16. The light from the object sequentially passes through the respective surfaces S1 to S16 and is finally imaged on the imaging surface S17.
Table 19 shows the surface type, radius of curvature, thickness, material, and conic coefficient of each lens of the optical imaging system of example 7, wherein the unit of the radius of curvature and the thickness are both millimeters (mm).
Figure BDA0002195892910000201
Figure BDA0002195892910000211
Watch 19
As is clear from table 19, in example 7, both the object-side surface and the image-side surface of any one of the first lens element E1 through the seventh lens element E7 are aspheric. Table 20 shows high-order term coefficients that can be used for each aspherical mirror surface in example 7, wherein each aspherical mirror surface type can be defined by formula (1) given in example 1 above.
Flour mark A4 A6 A8 A10 A12 A14 A16 A18 A20
S1 1.0046E-03 -1.5738E-02 5.2020E-02 -1.0217E-01 1.2126E-01 -8.9729E-02 4.0304E-02 -1.0102E-02 1.0800E-03
S2 -1.9071E-02 5.0290E-04 -2.6730E-03 2.6357E-02 -4.1922E-02 3.1947E-02 -1.2928E-02 2.4806E-03 -1.2769E-04
S3 -1.1925E-02 5.4808E-04 3.2363E-02 -5.5023E-02 8.0993E-02 -8.8905E-02 6.1108E-02 -2.2885E-02 3.6107E-03
S4 -6.0815E-03 1.5580E-03 -7.4765E-03 4.5338E-02 -1.0931E-01 1.2097E-01 -7.7196E-02 2.6210E-02 -3.7751E-03
S5 -5.1541E-02 -2.3005E-02 6.2895E-02 -2.3733E-01 5.1608E-01 -6.6934E-01 5.1214E-01 -2.1257E-01 3.6562E-02
S6 -3.8835E-02 3.0858E-02 -1.9677E-01 6.7860E-01 -1.3937E+00 1.7918E+00 -1.3833E+00 5.8881E-01 -1.0565E-01
S7 -2.8820E-02 7.6637E-03 -5.3325E-02 8.7814E-02 -6.3969E-02 -4.2180E-02 1.1477E-01 -8.0735E-02 2.0466E-02
S8 -3.1825E-02 -4.8700E-03 -4.4826E-03 -4.6763E-03 1.8323E-02 -2.9061E-02 2.3285E-02 -9.6073E-03 1.6769E-03
S9 -2.6832E-02 3.0731E-03 -8.0885E-02 1.8122E-01 -2.1325E-01 1.4411E-01 -5.6648E-02 1.1998E-02 -1.0507E-03
S10 5.4307E-03 -1.3867E-01 1.6119E-01 -1.0889E-01 3.9520E-02 -4.9458E-03 -1.0408E-03 3.8064E-04 -3.2339E-05
S11 5.7709E-02 -1.4020E-01 1.1123E-01 -6.3143E-02 2.1935E-02 -4.1861E-03 3.7862E-04 -6.4009E-06 -8.3328E-07
S12 -1.2584E-02 -9.2361E-03 -1.1997E-03 1.8613E-03 -7.4592E-04 1.7056E-04 -2.1268E-05 1.2062E-06 -1.6089E-08
S13 -2.5398E-01 9.3955E-02 -2.0837E-02 3.4141E-03 -4.4432E-04 4.4285E-05 -3.0443E-06 1.2422E-07 -2.2288E-09
S14 -2.2273E-01 1.0203E-01 -3.9146E-02 1.0657E-02 -1.8979E-03 2.1356E-04 -1.4558E-05 5.4734E-07 -8.6969E-09
Watch 20
Table 21 gives effective focal lengths f1 to f7 of the respective lenses, a total effective focal length f of the optical imaging system, a distance TTL on the optical axis from the object side surface S1 to the imaging surface S17 of the first lens E1, a half ImgH of the diagonal length of the effective pixel region on the imaging surface S17, and a maximum half field angle HFOV of the optical imaging system in embodiment 7.
f1(mm) 4.26 f7(mm) -12.19
f2(mm) -11.08 f(mm) 4.89
f3(mm) -933.76 TTL(mm) 5.57
f4(mm) 19.23 ImgH(mm) 3.98
f5(mm) -814.94 HFOV(°) 39.0
f6(mm) -753.04
TABLE 21
Fig. 14A shows an on-axis chromatic aberration curve of the optical imaging system of example 7, which represents the convergent focus deviation of light rays of different wavelengths after passing through the system. Fig. 14B shows an astigmatism curve representing meridional field curvature and sagittal field curvature of the optical imaging system of embodiment 7. Fig. 14C shows a distortion curve of the optical imaging system of embodiment 7, which represents the corresponding distortion magnitude values at different image heights. Fig. 14D shows a chromatic aberration of magnification curve of the optical imaging system of example 7, which represents the deviation of different image heights on the imaging plane after the light passes through the system. As can be seen from fig. 14A to 14D, the optical imaging system according to embodiment 7 can achieve good imaging quality.
Example 8
An optical imaging system according to embodiment 8 of the present application is described below with reference to fig. 15 to 16D. Fig. 15 shows a schematic structural view of an optical imaging system according to embodiment 8 of the present application.
As shown in fig. 15, the optical imaging system according to the exemplary embodiment of the present application, in order from an object side to an image side along an optical axis, includes: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, a filter E8, and an image forming surface S17.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2. The second lens element E2 has negative power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has negative power, and has a convex object-side surface S5 and a concave image-side surface S6. The fourth lens element E4 has positive power, and has a convex object-side surface S7 and a convex image-side surface S8. The fifth lens element E5 has positive power, and has a convex object-side surface S9 and a concave image-side surface S10. The sixth lens element E6 has negative power, and has a convex object-side surface S11 and a concave image-side surface S12. The seventh lens element E7 has negative power, and has a convex object-side surface S13 and a concave image-side surface S14. Filter E8 has an object side S15 and an image side S16. The light from the object sequentially passes through the respective surfaces S1 to S16 and is finally imaged on the imaging surface S17.
Table 22 shows the surface type, radius of curvature, thickness, material, and conic coefficient of each lens of the optical imaging system of example 8, wherein the unit of the radius of curvature and the thickness are both millimeters (mm).
Figure BDA0002195892910000221
Figure BDA0002195892910000231
TABLE 22
As can be seen from table 22, in example 8, both the object-side surface and the image-side surface of any one of the first lens element E1 through the seventh lens element E7 are aspheric. Table 23 shows high-order term coefficients that can be used for each aspherical mirror surface in embodiment 8, wherein each aspherical mirror surface type can be defined by the formula (1) given in embodiment 1 above.
Flour mark A4 A6 A8 A10 A12 A14 A16 A18 A20
S1 1.1018E-03 -1.8076E-02 6.2572E-02 -1.2870E-01 1.5997E-01 -1.2397E-01 5.8313E-02 -1.5307E-02 1.7137E-03
S2 -2.1590E-02 6.0573E-04 -3.4256E-03 3.5939E-02 -6.0821E-02 4.9314E-02 -2.1234E-02 4.3348E-03 -2.3742E-04
S3 -1.3426E-02 6.5477E-04 4.1024E-02 -7.4010E-02 1.1560E-01 -1.3464E-01 9.8196E-02 -3.9021E-02 6.5326E-03
S4 -6.6773E-03 1.7925E-03 -9.0132E-03 5.7272E-02 -1.4469E-01 1.6779E-01 -1.1219E-01 3.9914E-02 -6.0239E-03
S5 -5.5673E-02 -2.5826E-02 7.3384E-02 -2.8780E-01 6.5042E-01 -8.7674E-01 6.9720E-01 -3.0076E-01 5.3764E-02
S6 -4.2722E-02 3.5604E-02 -2.3813E-01 8.6136E-01 -1.8554E+00 2.5020E+00 -2.0259E+00 9.0449E-01 -1.7023E-01
S7 -3.0828E-02 8.4784E-03 -6.1015E-02 1.0392E-01 -7.8293E-02 -5.3393E-02 1.5026E-01 -1.0932E-01 2.8661E-02
S8 -3.6240E-02 -5.9178E-03 -5.8127E-03 -6.4708E-03 2.7056E-02 -4.5792E-02 3.9154E-02 -1.7239E-02 3.2108E-03
S9 -3.4381E-02 4.4574E-03 -1.3280E-01 3.3682E-01 -4.4865E-01 3.4319E-01 -1.5271E-01 3.6611E-02 -3.6295E-03
S10 5.4387E-03 -1.3897E-01 1.6166E-01 -1.0928E-01 3.9693E-02 -4.9711E-03 -1.0469E-03 3.8314E-04 -3.2575E-05
S11 6.0162E-02 -1.4923E-01 1.2089E-01 -7.0070E-02 2.4853E-02 -4.8429E-03 4.4724E-04 -7.7199E-06 -1.0261E-06
S12 -1.4090E-02 -1.0943E-02 -1.5040E-03 2.4691E-03 -1.0470E-03 2.5333E-04 -3.3426E-05 2.0060E-06 -2.8312E-08
S13 -2.7890E-01 1.0811E-01 -2.5126E-02 4.3139E-03 -5.8832E-04 6.1446E-05 -4.4263E-06 1.8926E-07 -3.5585E-09
S14 -2.3539E-01 1.1085E-01 -4.3720E-02 1.2235E-02 -2.2401E-03 2.5912E-04 -1.8158E-05 7.0183E-07 -1.1464E-08
TABLE 23
Table 24 gives the effective focal lengths f1 to f7 of the respective lenses, the total effective focal length f of the optical imaging system, the distance TTL on the optical axis from the object side surface S1 to the imaging surface S17 of the first lens E1, half ImgH of the diagonal length of the effective pixel region on the imaging surface S17, and the maximum half field angle HFOV of the optical imaging system in embodiment 8.
f1(mm) 4.13 f7(mm) -9.85
f2(mm) -10.92 f(mm) 4.73
f3(mm) -2168.21 TTL(mm) 5.50
f4(mm) 19.41 ImgH(mm) 3.93
f5(mm) 2811.51 HFOV(°) 39.3
f6(mm) -2919.15
Watch 24
Fig. 16A shows an on-axis chromatic aberration curve of the optical imaging system of embodiment 8, which represents the convergent focus deviation of light rays of different wavelengths after passing through the system. Fig. 16B shows an astigmatism curve representing meridional field curvature and sagittal field curvature of the optical imaging system of example 8. Fig. 16C shows a distortion curve of the optical imaging system of embodiment 8, which represents the corresponding distortion magnitude values at different image heights. Fig. 16D shows a chromatic aberration of magnification curve of the optical imaging system of example 8, which represents the deviation of different image heights on the imaging plane after the light passes through the system. As can be seen from fig. 16A to 16D, the optical imaging system according to embodiment 8 can achieve good imaging quality.
Example 9
An optical imaging system according to embodiment 9 of the present application is described below with reference to fig. 17 to 18D. Fig. 17 shows a schematic configuration diagram of an optical imaging system according to embodiment 9 of the present application.
As shown in fig. 17, the optical imaging system according to the exemplary embodiment of the present application, in order from an object side to an image side along an optical axis, includes: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, a filter E8, and an image forming surface S17.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2. The second lens element E2 has negative power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has positive power, and has a convex object-side surface S5 and a concave image-side surface S6. The fourth lens element E4 has positive power, and has a convex object-side surface S7 and a convex image-side surface S8. The fifth lens element E5 has positive power, and has a convex object-side surface S9 and a concave image-side surface S10. The sixth lens element E6 has negative power, and has a convex object-side surface S11 and a concave image-side surface S12. The seventh lens element E7 has negative power, and has a convex object-side surface S13 and a concave image-side surface S14. Filter E8 has an object side S15 and an image side S16. The light from the object sequentially passes through the respective surfaces S1 to S16 and is finally imaged on the imaging surface S17.
Table 25 shows the surface type, radius of curvature, thickness, material, and conic coefficient of each lens of the optical imaging system of example 9, wherein the unit of the radius of curvature and the thickness are both millimeters (mm).
Figure BDA0002195892910000241
TABLE 25
As is clear from table 25, in example 9, both the object-side surface and the image-side surface of any one of the first lens element E1 through the seventh lens element E7 are aspheric. Table 26 shows high-order term coefficients that can be used for each aspherical mirror surface in example 9, wherein each aspherical mirror surface type can be defined by formula (1) given in example 1 above.
Flour mark A4 A6 A8 A10 A12 A14 A16 A18 A20
S1 -2.8068E-03 7.5248E-03 -1.6147E-02 1.3142E-02 -1.3955E-03 -7.0941E-03 5.9394E-03 -2.1178E-03 2.9329E-04
S2 -1.8610E-02 -6.6367E-02 1.9966E-01 -2.8511E-01 2.6322E-01 -1.6768E-01 7.2354E-02 -1.9026E-02 2.2892E-03
S3 8.1130E-04 -1.1473E-01 3.9744E-01 -6.7525E-01 7.5065E-01 -5.6537E-01 2.8140E-01 -8.3345E-02 1.1088E-02
S4 6.4243E-03 -9.0213E-02 3.2255E-01 -6.7759E-01 9.4292E-01 -9.6870E-01 6.9445E-01 -3.0277E-01 5.8330E-02
S5 -6.4632E-02 1.2073E-03 -2.8315E-02 1.3005E-01 -3.0589E-01 3.0594E-01 -1.0325E-01 -2.4836E-02 1.6851E-02
S6 -6.1707E-02 5.4952E-02 -1.7500E-01 4.6778E-01 -7.3426E-01 6.8590E-01 -3.3742E-01 6.9546E-02 1.2539E-04
S7 -2.7092E-02 -3.2222E-01 1.5854E+00 -4.7218E+00 8.7711E+00 -1.0276E+01 7.3825E+00 -2.9725E+00 5.1456E-01
S8 -7.7301E-02 1.2666E-01 -5.0398E-01 1.1211E+00 -1.5215E+00 1.2806E+00 -6.5188E-01 1.8343E-01 -2.1807E-02
S9 -6.2409E-03 -3.6601E-02 -4.2790E-03 4.9658E-02 -7.1684E-02 5.0485E-02 -1.9415E-02 3.9118E-03 -3.2158E-04
S10 3.8416E-02 -1.4035E-01 1.4490E-01 -9.7589E-02 3.7964E-02 -7.6146E-03 5.8018E-04 2.6593E-05 -4.7642E-06
S11 4.8442E-02 -2.0475E-01 2.2051E-01 -1.4445E-01 5.7081E-02 -1.3456E-02 1.8480E-03 -1.3597E-04 4.1152E-06
S12 1.1030E-02 -1.0341E-01 9.4638E-02 -5.0814E-02 1.6966E-02 -3.5905E-03 4.7468E-04 -3.6132E-05 1.2169E-06
S13 -2.8020E-01 1.0875E-01 -2.5504E-02 4.5034E-03 -6.5680E-04 7.6867E-05 -6.3856E-06 3.1803E-07 -6.9792E-09
S14 -3.1008E-01 1.6751E-01 -6.9035E-02 2.0116E-02 -3.9157E-03 4.9094E-04 -3.7907E-05 1.6392E-06 -3.0398E-08
Watch 26
Table 27 gives the effective focal lengths f1 to f7 of the respective lenses, the total effective focal length f of the optical imaging system, the distance TTL on the optical axis from the object side surface S1 to the imaging surface S17 of the first lens E1, half ImgH of the diagonal length of the effective pixel region on the imaging surface S17, and the maximum half field angle HFOV of the optical imaging system in example 9.
f1(mm) 3.75 f7(mm) -5.77
f2(mm) -6.80 f(mm) 5.02
f3(mm) 72.64 TTL(mm) 5.50
f4(mm) 14.57 ImgH(mm) 3.93
f5(mm) 91.95 HFOV(°) 37.8
f6(mm) -412.30
Watch 27
Fig. 18A shows an on-axis chromatic aberration curve of the optical imaging system of example 9, which represents the convergent focus deviation of light rays of different wavelengths after passing through the system. Fig. 18B shows an astigmatism curve representing meridional field curvature and sagittal field curvature of the optical imaging system of example 9. Fig. 18C shows a distortion curve of the optical imaging system of embodiment 9, which represents the corresponding distortion magnitude values at different image heights. Fig. 18D shows a chromatic aberration of magnification curve of the optical imaging system of example 9, which represents the deviation of different image heights on the imaging plane after the light passes through the system. As can be seen from fig. 18A to 18D, the optical imaging system according to embodiment 9 can achieve good imaging quality.
Example 10
An optical imaging system according to embodiment 10 of the present application is described below with reference to fig. 19 to 20D. Fig. 19 shows a schematic structural view of an optical imaging system according to embodiment 10 of the present application.
As shown in fig. 19, the optical imaging system according to the exemplary embodiment of the present application, in order from an object side to an image side along an optical axis, comprises: a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a sixth lens E6, a seventh lens E7, a filter E8, and an image forming surface S17.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2. The second lens element E2 has negative power, and has a convex object-side surface S3 and a concave image-side surface S4. The third lens element E3 has positive power, and has a convex object-side surface S5 and a concave image-side surface S6. The fourth lens element E4 has positive power, and has a convex object-side surface S7 and a convex image-side surface S8. The fifth lens element E5 has positive power, and has a convex object-side surface S9 and a concave image-side surface S10. The sixth lens element E6 has negative power, and has a convex object-side surface S11 and a concave image-side surface S12. The seventh lens element E7 has negative power, and has a convex object-side surface S13 and a concave image-side surface S14. Filter E8 has an object side S15 and an image side S16. The light from the object sequentially passes through the respective surfaces S1 to S16 and is finally imaged on the imaging surface S17.
Table 28 shows the surface type, radius of curvature, thickness, material, and conic coefficient of each lens of the optical imaging system of example 10, wherein the unit of the radius of curvature and the thickness are both millimeters (mm).
Figure BDA0002195892910000261
Watch 28
As can be seen from table 28, in example 10, both the object-side surface and the image-side surface of any one of the first lens element E1 through the seventh lens element E7 are aspheric. Table 29 shows high-order term coefficients that can be used for each aspherical mirror surface in example 10, wherein each aspherical mirror surface type can be defined by formula (1) given in example 1 above.
Flour mark A4 A6 A8 A10 A12 A14 A16 A18 A20
S1 -5.3425E-03 1.7512E-02 -3.6915E-02 4.2809E-02 -2.6666E-02 4.4795E-03 4.1227E-03 -2.5128E-03 4.1215E-04
S2 -1.3884E-02 -1.5941E-02 3.0456E-03 7.0547E-02 -1.4259E-01 1.3727E-01 -7.4265E-02 2.1636E-02 -2.6308E-03
S3 -8.0012E-03 -1.5312E-02 4.0908E-02 -2.1783E-02 1.9175E-02 -4.8369E-02 5.6962E-02 -2.9696E-02 5.9448E-03
S4 4.2149E-03 -7.4112E-02 2.0069E-01 -3.3088E-01 3.3173E-01 -2.0350E-01 7.7888E-02 -2.8536E-02 8.0494E-03
S5 -5.7006E-02 4.2076E-02 -3.4714E-01 1.0046E+00 -1.7561E+00 1.9397E+00 -1.3049E+00 4.8041E-01 -7.3382E-02
S6 -3.9055E-02 5.7255E-02 -3.0872E-01 9.6107E-01 -1.9128E+00 2.4870E+00 -1.9811E+00 8.7411E-01 -1.6243E-01
S7 -4.3094E-02 1.4642E-01 -4.5066E-01 6.6149E-01 -4.1678E-01 -1.1509E-01 3.4629E-01 -2.0233E-01 4.1539E-02
S8 -3.7901E-02 3.0069E-02 -1.5557E-01 3.6382E-01 -5.3612E-01 4.7676E-01 -2.4827E-01 6.8580E-02 -7.5247E-03
S9 -2.7527E-02 -8.4112E-02 9.4274E-02 -1.0916E-02 -1.2211E-01 1.5340E-01 -8.6041E-02 2.3574E-02 -2.5205E-03
S10 2.4219E-02 -2.1181E-01 3.0099E-01 -2.5846E-01 1.3635E-01 -4.2887E-02 7.6846E-03 -6.9985E-04 2.3171E-05
S11 5.7888E-02 -1.4108E-01 1.1494E-01 -6.5908E-02 2.3348E-02 -4.7421E-03 5.1823E-04 -2.5380E-05 2.3492E-07
S12 -9.8426E-03 -1.7093E-02 2.1781E-03 2.9001E-03 -2.1761E-03 7.4625E-04 -1.3921E-04 1.3501E-05 -5.3043E-07
S13 -2.5498E-01 8.6414E-02 -1.2425E-02 -2.6859E-04 4.1418E-04 -7.2450E-05 6.2807E-06 -2.8255E-07 5.2614E-09
S14 -2.2240E-01 9.8726E-02 -3.6956E-02 9.9606E-03 -1.7932E-03 2.0829E-04 -1.4922E-05 5.9886E-07 -1.0302E-08
Watch 29
Table 30 gives the effective focal lengths f1 to f7 of the respective lenses, the total effective focal length f of the optical imaging system, the distance TTL on the optical axis from the object side surface S1 to the imaging surface S17 of the first lens E1, half ImgH of the diagonal length of the effective pixel region on the imaging surface S17, and the maximum half field angle HFOV of the optical imaging system in example 10.
f1(mm) 4.16 f7(mm) -9.47
f2(mm) -12.55 f(mm) 4.58
f3(mm) 502.00 TTL(mm) 5.50
f4(mm) 25.95 ImgH(mm) 3.93
f5(mm) 231.90 HFOV(°) 40.1
f6(mm) -401.60
Watch 30
Fig. 20A shows an on-axis chromatic aberration curve of the optical imaging system of example 10, which represents the convergent focus deviation of light rays of different wavelengths after passing through the system. Fig. 20B shows an astigmatism curve representing meridional field curvature and sagittal field curvature of the optical imaging system of example 10. Fig. 20C shows a distortion curve of the optical imaging system of embodiment 10, which represents the corresponding distortion magnitude values at different image heights. Fig. 20D shows a chromatic aberration of magnification curve of the optical imaging system of example 10, which represents the deviation of different image heights on the imaging plane after the light passes through the system. As can be seen from fig. 20A to 20D, the optical imaging system according to embodiment 10 can achieve good imaging quality.
In summary, examples 1 to 10 each satisfy the relationship shown in table 31.
Figure BDA0002195892910000271
Figure BDA0002195892910000281
Watch 31
The present application also provides an imaging device whose electron photosensitive element may be a photo-coupled device (CCD) or a complementary metal oxide semiconductor device (CMOS). The imaging device may be a stand-alone imaging device such as a digital camera, or may be an imaging module integrated on a mobile electronic device such as a mobile phone. The imaging device is equipped with the optical imaging system described above.
The above description is only a preferred embodiment of the application and is illustrative of the principles of the technology employed. It will be appreciated by a person skilled in the art that the scope of the invention as referred to in the present application is not limited to the embodiments with a specific combination of the above-mentioned features, but also covers other embodiments with any combination of the above-mentioned features or their equivalents without departing from the inventive concept. For example, the above features may be replaced with (but not limited to) features having similar functions disclosed in the present application.

Claims (13)

1. The optical imaging system comprises, in order from an object side to an image side along an optical axis: a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens,
it is characterized in that the preparation method is characterized in that,
the first lens has positive focal power, the object side surface of the first lens is a convex surface, and the image side surface of the first lens is a concave surface;
the second lens has negative focal power, the object side surface of the second lens is a convex surface, and the image side surface of the second lens is a concave surface;
the third lens has focal power, and the object side surface of the third lens is a convex surface, and the image side surface of the third lens is a concave surface;
the fourth lens has positive optical power;
the fifth lens has optical power;
the sixth lens has optical power;
the seventh lens has negative focal power, the object side surface of the seventh lens is a convex surface, and the image side surface of the seventh lens is a concave surface;
at least one mirror surface of the object side surface of the first lens to the image side surface of the seventh lens is an aspherical mirror surface,
an effective focal length f4 of the fourth lens and a total effective focal length f of the optical imaging system satisfy 2.5 ≤ f4/f < 6, an
The total effective focal length f of the optical imaging system and the entrance pupil diameter EPD of the optical imaging system satisfy f/EPD is less than or equal to 1.8.
2. The optical imaging system of claim 1, wherein the effective focal length f1 of the first lens, the effective focal length f2 of the second lens and the total effective focal length f of the optical imaging system satisfy-2 < f1/f + f2/f < -0.5.
3. The optical imaging system of claim 2, wherein a radius of curvature R1 of the object-side surface of the first lens and a radius of curvature R2 of the image-side surface of the first lens satisfy 0.1 < R1/R2 < 0.3.
4. The optical imaging system of claim 2, wherein a radius of curvature R3 of the object-side surface of the second lens and a radius of curvature R4 of the image-side surface of the second lens satisfy 0.2 < R4/R3 < 0.5.
5. The optical imaging system of claim 1, wherein the radius of curvature of the object-side surface of the third lens, R5, R6, R13, and R14 satisfy 1 < (R5+ R6)/(R13+ R14) < 2.
6. The optical imaging system of claim 5, wherein the effective focal length f7 of the seventh lens and the total effective focal length f of the optical imaging system satisfy-2.5 < f7/f < -1.
7. The optical imaging system according to claim 1, wherein a sum Σ AT of a maximum effective radius DT31 of an object side surface of the third lens and a separation distance on the optical axis of any adjacent two lenses of the first lens to the seventh lens satisfies 0.5 < DT31/∑ AT < 1.
8. The optical imaging system according to claim 7, wherein a center thickness CT1 of the first lens on the optical axis, a center thickness CT2 of the second lens on the optical axis, and a center thickness CT3 of the third lens on the optical axis satisfy 1.5 < CT1/(CT2+ CT3) < 2.
9. The optical imaging system of claim 7, wherein a center thickness CT4 of the fourth lens on the optical axis, a center thickness CT5 of the fifth lens on the optical axis, a center thickness CT6 of the sixth lens on the optical axis and a center thickness CT7 of the seventh lens on the optical axis satisfy 1 ≦ (CT7+ CT6)/(CT5+ CT4) < 2.
10. The optical imaging system according to claim 1, characterized in that a combined focal length f1234 of the first lens, the second lens, the third lens and the fourth lens and a combined focal length f567 of the fifth lens, the sixth lens and the seventh lens satisfy 1 < | f567/f1234| < 2.5.
11. The optical imaging system of claim 1, wherein the fourth lens and the fifth lens are spaced on the optical axisThe distance T45, the total effective focal length f of the optical imaging system and the maximum half field angle HFOV of the optical imaging system satisfy 0.85mm2≤T45*f*TAN(HFOV)≤3.1mm2
12. The optical imaging system according to claim 11, characterized in that the total effective focal length f of the optical imaging system and the maximum half field angle HFOV of the optical imaging system satisfy 3.8mm < f tan (HFOV) < 4.5 mm.
13. The optical imaging system according to any one of claims 1 to 12, wherein a distance TTL between an object side surface of the first lens element and an imaging surface of the optical imaging system on the optical axis and a half ImgH of a diagonal length of an effective pixel area on the imaging surface of the optical imaging system satisfy TTL/ImgH < 1.5.
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