Optical imaging system

Information

  • Patent Grant
  • 11960145
  • Patent Number
    11,960,145
  • Date Filed
    Friday, March 24, 2023
    a year ago
  • Date Issued
    Tuesday, April 16, 2024
    15 days ago
Abstract
An optical imaging system includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens sequentially disposed in numerical order along an optical axis of the optical imaging system from an object side of the optical imaging system toward an imaging plane of the optical imaging system; and a spacer disposed between the sixth and seventh lenses, wherein the optical imaging system satisfies 0.5
Description
BACKGROUND
1. Field

This application relates to an optical imaging system.


2. Description of Related Art

Recently, mobile communications terminals have been provided with camera modules, enabling video calling and image capturing. In addition, as utilization of the camera modules mounted in the mobile communications terminals has increased, camera modules for the mobile communications terminals have gradually been required to have high resolution and performance.


Therefore, the number of lenses included in the camera module has increased. However, since the mobile communications terminal in which the camera module is mounted tends to be miniaturized, it is very difficult to arrange the lenses in the camera module.


Therefore, research into technology capable of performing aberration correction to implement high resolution and arranging a plurality of lenses in a limited space has been ongoing.


SUMMARY

This Summary is provided to introduce a selection of concepts in a simplified form that are further described below in the Detailed Description. This Summary is not intended to identify key features or essential features of the claimed subject matter, nor is it intended to be used as an aid in determining the scope of the claimed subject matter.


In one general aspect, an optical imaging system includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens sequentially disposed in numerical order along an optical axis of the optical imaging system from an object side of the optical imaging system toward an imaging plane of the optical imaging system; and a spacer disposed between the sixth and seventh lenses, wherein the optical imaging system satisfies 0.5<S6d/f<1.4, where S6d is an inner diameter of the spacer, f is an overall focal length of the optical imaging system, and S6d and f are expressed in a same unit of measurement.


The optical imaging system may further satisfy 0.5<S6d/f<1.2.


The optical imaging system may further satisfy 0.1<L1w/L7w<0.3, where L1w is a weight of the first lens, L7w is a weight of the seventh lens, and L1w and L7w are expressed in a same unit of measurement.


The optical imaging system may further satisfy 0.4<L1TR/L7TR<0.7, where L1TR is an overall outer diameter of the first lens, L7TR is an overall outer diameter of the seventh lens, and L1TR and L7TR are expressed in a same unit of measurement.


The optical imaging system may further satisfy 0.5<L1234TRavg/L7TR<0.75, where L1234TRavg is an average value of overall outer diameters of the first to fourth lenses, L7TR is an overall outer diameter of the seventh lens, and L1234TRavg and L7TR are expressed in a same unit of measurement.


The optical imaging system may further satisfy 0.5<L12345TRavg/L7TR<0.76, where L12345TRavg is an average value of overall outer diameters of the first to fifth lenses, L7TR is an overall outer diameter of the seventh lens, and L12345TRavg and L7TR are expressed in a same unit of measurement.


The optical imaging system may further satisfy 0.1<(1/f1+1/f2+1/f3+1/f4+1/f5+1/f6+1/f7)*f<0.8, where f1 is a focal length of the first lens, f2 is a focal length of the second lens, f3 is a focal length of the third lens, f4 is a focal length of the fourth lens, f5 is a focal length of the fifth lens, f6 is a focal length of the sixth lens, f7 is a focal length of the seventh lens, f is an overall focal length of the optical imaging system, and f1, f2, f3, f4, f5, f6, f7, and f are expressed in a same unit of measurement.


The optical imaging system may further satisfy 0.1<(1/f1+1/f2+1/f3+1/f4+1/f5+1/f6+1/f7)*TTL<1.0, where f1 is a focal length of the first lens, f2 is a focal length of the second lens, f3 is a focal length of the third lens, f4 is a focal length of the fourth lens, f5 is a focal length of the fifth lens, f6 is a focal length of the sixth lens, f7 is a focal length of the seventh lens, TTL is a distance along the optical axis from an object-side surface of the first lens to the imaging plane, and f1, f2, f3, f4, f5, f6, f7, and TTL are expressed in a same unit of measurement.


The optical imaging system may further satisfy 0.2<TD1/D67<0.8, where TD1 is a thickness along the optical axis of the first lens, D67 is a distance along the optical axis from an object-side surface of the sixth lens to an image-side surface of the seventh lens, and TD1 and D67 are expressed in a same unit of measurement.


The imaging plane may be an imaging plane of an image sensor, and the optical imaging system may further satisfy TTL 6.00 mm and 0.6<TTL/(2*IMG HT)<0.9, where TTL is a distance along the optical axis from an object-side surface of the first lens to the imaging plane of the image sensor, IMG HT is one-half of a diagonal length of the imaging plane of the image sensor, and TTL and IMG HT are expressed in mm.


The optical imaging system may further satisfy 0.2<ΣSD/ΣTD<0.7, where ΣSD is a sum of air gaps along the optical axis between the first to seventh lenses, ΣTD is a sum of thicknesses along the optical axis of the first to seventh lenses, and ΣSD and ΣTD are expressed in a same unit of measurement.


The optical imaging system may further satisfy 0<min(f1:f3)/max(f4:f7)<0.4, where min(f1:f3) is a minimum value of absolute values of focal lengths of the first to third lenses, max(f4:f7) is a maximum value of absolute values of focal lengths of the fourth to seventh lenses, and min(f1:f3) and max(f4:f7) are expressed in a same unit of measurement.


The optical imaging system may further satisfy 0.4<ΣTD/TTL<0.7, where ΣTD is a sum of thicknesses along the optical axis of the first to seventh lenses, TTL is a distance along the optical axis from an object-side surface of the first lens to the imaging plane, and ΣTD and TTL are expressed in a same unit of measurement.


The optical imaging system may further satisfy 0.81<f12/f123<0.96, where f12 is a composite focal length of the first and second lenses, f123 is a composite focal length of the first to third lenses, and f12 and f123 are expressed in a same unit of measurement.


The optical imaging system may further satisfy 0.6<f12/f1234<0.84, where f12 is a composite focal length of the first and second lenses, f1234 is a composite focal length of the first to fourth lenses, and f12 and f1234 are expressed in a same unit of measurement.


The second lens may have a positive refractive power, and the third lens may have a negative refractive power.


The fifth lens may have a negative refractive power, and a paraxial region of an object-side surface of the fifth lens may be concave or convex.


The fifth lens may have a negative refractive power, and a paraxial region of an image-side surface of the fifth lens may be concave or convex.


A paraxial region of an object-side surface of the sixth lens may be concave or convex.


A paraxial region of an object-side surface of the seventh lens may be concave.


Other features and aspects will be apparent from the following detailed description, the drawings, and the claims.





BRIEF DESCRIPTION OF DRAWINGS


FIG. 1 is a view illustrating a first example of an optical imaging system.



FIG. 2 illustrates aberration curves of the optical imaging system of FIG. 1.



FIG. 3 is a view illustrating a second example of an optical imaging system.



FIG. 4 illustrates aberration curves of the optical imaging system of FIG. 3.



FIG. 5 is a view illustrating a third example of an optical imaging system.



FIG. 6 illustrates aberration curves of the optical imaging system of FIG. 5.



FIG. 7 is a view illustrating a fourth example of an optical imaging system.



FIG. 8 illustrates aberration curves of the optical imaging system of FIG. 7.



FIG. 9 is a view illustrating a fifth example of an optical imaging system.



FIG. 10 illustrates aberration curves of the optical imaging system of FIG. 9.



FIG. 11 is a view illustrating a sixth example of an optical imaging system.



FIG. 12 illustrates aberration curves of the optical imaging system of FIG. 11.



FIG. 13 is a view illustrating a seventh example of an optical imaging system.



FIG. 14 illustrates aberration curves of the optical imaging system of FIG. 13.



FIG. 15 is a view illustrating an eighth example of an optical imaging system.



FIG. 16 illustrates aberration curves of the optical imaging system of FIG. 15.



FIG. 17 is a view illustrating a ninth example of an optical imaging system.



FIG. 18 illustrates aberration curves of the optical imaging system of FIG. 17.



FIG. 19 is a view illustrating a tenth example of an optical imaging system.



FIG. 20 illustrates aberration curves of the optical imaging system of FIG. 19.



FIG. 21 is a view illustrating an eleventh example of an optical imaging system.



FIG. 22 illustrates aberration curves of the optical imaging system of FIG. 21.



FIG. 23 is a view illustrating a twelfth example of an optical imaging system.



FIG. 24 illustrates aberration curves of the optical imaging system of FIG. 23.



FIG. 25 is a view illustrating a thirteenth example of an optical imaging system.



FIG. 26 illustrates aberration curves of the optical imaging system of FIG. 25.



FIG. 27 is a view illustrating a fourteenth example of an optical imaging system.



FIG. 28 illustrates aberration curves of the optical imaging system of FIG. 27.



FIG. 29 is a view illustrating a fifteenth example of an optical imaging system.



FIG. 30 illustrates aberration curves of the optical imaging system of FIG. 29.



FIG. 31 is a view illustrating a sixteenth example of an optical imaging system.



FIG. 32 illustrates aberration curves of the optical imaging system of FIG. 31.



FIG. 33 is a view illustrating a seventeenth example of an optical imaging system.



FIG. 34 illustrates aberration curves of the optical imaging system of FIG. 33.



FIG. 35 is a view illustrating an eighteenth example of an optical imaging system.



FIG. 36 illustrates aberration curves of the optical imaging system of FIG. 35.



FIG. 37 is a view illustrating a nineteenth example of an optical imaging system.



FIG. 38 illustrates aberration curves of the optical imaging system of FIG. 37.



FIG. 39 is a view illustrating a twentieth example of an optical imaging system.



FIG. 40 illustrates aberration curves of the optical imaging system of FIG. 39.



FIG. 41 is a view illustrating a twenty-first example of an optical imaging system.



FIG. 42 illustrates aberration curves of the optical imaging system of FIG. 41.



FIG. 43 is a view illustrating a twenty-second example of an optical imaging system.



FIG. 44 illustrates aberration curves of the optical imaging system of FIG. 43.



FIG. 45 is a view illustrating a twenty-third example of an optical imaging system.



FIG. 46 illustrates aberration curves of the optical imaging system of FIG. 45.



FIG. 47 is a view illustrating a twenty-fourth example of an optical imaging system.



FIG. 48 illustrates aberration curves of the optical imaging system of FIG. 47.



FIG. 49 is a view illustrating a twenty-fifth example of an optical imaging system.



FIG. 50 illustrates aberration curves of the optical imaging system of FIG. 49.



FIG. 51 is a view illustrating a twenty-sixth example of an optical imaging system.



FIG. 52 illustrates aberration curves of the optical imaging system of FIG. 51.



FIG. 53 is a view illustrating a twenty-seventh example of an optical imaging system.



FIG. 54 illustrates aberration curves of the optical imaging system of FIG. 53.



FIGS. 55 and 56 are cross-sectional views illustrating examples of an optical imaging system and a lens barrel coupled to each other.



FIG. 57 is a cross-sectional view illustrating an example of a shape of a rib of a seventh lens.



FIG. 58 is a cross-sectional view illustrating an example of a seventh lens.





Throughout the drawings and the detailed description, the same reference numerals refer to the same elements. The drawings may not be to scale, and the relative size, proportions, and depiction of elements in the drawings may be exaggerated for clarity, illustration, and convenience.


DETAILED DESCRIPTION

The following detailed description is provided to assist the reader in gaining a comprehensive understanding of the methods, apparatuses, and/or systems described herein. However, various changes, modifications, and equivalents of the methods, apparatuses, and/or systems described herein will be apparent after an understanding of the disclosure of this application. For example, the sequences of operations described herein are merely examples, and are not limited to those set forth herein, but may be changed as will be apparent after an understanding of the disclosure of this application, with the exception of operations necessarily occurring in a certain order. Also, descriptions of features that are known in the art may be omitted for increased clarity and conciseness.


The features described herein may be embodied in different forms, and are not to be construed as being limited to the examples described herein. Rather, the examples described herein have been provided merely to illustrate some of the many possible ways of implementing the methods, apparatuses, and/or systems described herein that will be apparent after an understanding of the disclosure of this application.


Throughout the specification, when an element, such as a layer, region, or substrate, is described as being “on,” “connected to,” or “coupled to” another element, it may be directly “on,” “connected to,” or “coupled to” the other element, or there may be one or more other elements intervening therebetween. In contrast, when an element is described as being “directly on,” “directly connected to,” or “directly coupled to” another element, there can be no other elements intervening therebetween.


As used herein, the term “and/or” includes any one and any combination of any two or more of the associated listed items.


Although terms such as “first,” “second,” and “third” may be used herein to describe various members, components, regions, layers, or sections, these members, components, regions, layers, or sections are not to be limited by these terms. Rather, these terms are only used to distinguish one member, component, region, layer, or section from another member, component, region, layer, or section. Thus, a first member, component, region, layer, or section referred to in examples described herein may also be referred to as a second member, component, region, layer, or section without departing from the teachings of the examples.


Spatially relative terms such as “above,” “upper,” “below,” and “lower” may be used herein for ease of description to describe one element's relationship to another element as shown in the figures. Such spatially relative terms are intended to encompass different orientations of the device in use or operation in addition to the orientation depicted in the figures. For example, if the device in the figures is turned over, an element described as being “above” or “upper” relative to another element will then be “below” or “lower” relative to the other element. Thus, the term “above” encompasses both the above and below orientations depending on the spatial orientation of the device. The device may also be oriented in other ways (for example, rotated by 90 degrees or at other orientations), and the spatially relative terms used herein are to be interpreted accordingly.


The terminology used herein is for describing various examples only, and is not to be used to limit the disclosure. The articles “a,” “an,” and “the” are intended to include the plural forms as well, unless the context clearly indicates otherwise. The terms “comprises,” “includes,” and “has” specify the presence of stated features, numbers, operations, members, elements, and/or combinations thereof, but do not preclude the presence or addition of one or more other features, numbers, operations, members, elements, and/or combinations thereof.


Thicknesses, sizes, and shapes of lenses illustrated in the drawings may have been slightly exaggerated for convenience of explanation. In addition, the shapes of spherical surfaces or aspherical surfaces of the lenses described in the detailed description and illustrated in the drawings are merely examples. That is, the shapes of the spherical surfaces or the aspherical surfaces of the lenses are not limited to the examples described herein.


Numerical values of radii of curvature, thicknesses of lenses, distances between elements including lenses or surfaces, effective aperture radii of lenses, focal lengths, and diameters, thicknesses, and lengths of various elements are expressed in millimeters (mm), and angles are expressed in degrees. Thicknesses of lenses and distances between elements including lenses or surfaces are measured along the optical axis of the optical imaging system.


The term “effective aperture radius” as used in this application refers to a radius of a portion of a surface of a lens or other element (an object-side surface or an image-side surface of a lens or other element) through which light actually passes. The effective aperture radius is equal to a distance measured perpendicular to an optical axis of the surface between the optical axis of the surface and the outermost point on the surface through which light actually passes. Therefore, the effective aperture radius may be equal to a radius of an optical portion of a surface, or may be smaller than the radius of the optical portion of the surface if light does not pass through a peripheral portion of the optical portion of the surface. The object-side surface and the image-side surface of a lens or other element may have different effective aperture radii.


In this application, unless stated otherwise, a reference to the shape of a lens surface means the shape of a paraxial region of the lens surface. A paraxial region of a lens surface is a central portion of the lens surface surrounding the optical axis of the lens surface in which light rays incident to the lens surface make a small angle θ to the optical axis and the approximations sin θ≈θ, tan θ≈θ, and cos θ≈1 are valid.


For example, a statement that the object-side surface of a lens is convex means that at least a paraxial region of the object-side surface of the lens is convex, and a statement that the image-side surface of the lens is concave means that at least a paraxial region of the image-side surface of the lens is concave. Therefore, even though the object side-surface of the lens may be described as being convex, the entire object-side surface of the lens may not be convex, and a peripheral region of the object-side surface of the lens may be concave. Also, even though the image-side surface of the lens may be described as being concave, the entire image-side surface of the lens may not be concave, and a peripheral region of the image-side surface of the lens may be convex.



FIGS. 55 and 56 are cross-sectional views illustrating examples of an optical imaging system and a lens barrel coupled to each other.


Referring to FIGS. 55 and 56, an optical imaging system 100 includes a plurality of lenses disposed along an optical axis. In addition, the optical imaging system 100 further includes a lens barrel 200 accommodating the plurality of lenses therein. The plurality of lenses are spaced apart from each other by predetermined distances along the optical axis.


Each lens of the optical imaging system 100 includes an optical portion and a rib. The optical portion of the lens is a portion of the lens that is configured to refract light, and is generally formed in a central portion of the lens. The rib of the lens is an edge portion of the lens that enables the lens to be mounted in the lens barrel 200 and the optical axis of the lens to be aligned with the optical axis of the optical imaging system 100. The rib of the lens extends radially outward from the optical portion, and may be formed integrally with the optical portion. The optical portions of the lenses are generally not in contact with each other. For example, the first to seventh lenses are mounted in the lens barrel 200 so that they are spaced apart from one another by predetermined distances along the optical axis of the optical imaging system 100. The ribs of the lenses may be in selective contact with each other. For example, the ribs of the first to fourth lenses, or the first to fifth lenses, or the second to fourth lenses, may be in contact with each other so that the optical axes of these lenses may be easily aligned with the optical axis of the optical imaging system 100.


The examples of the optical imaging system 100 described in this application may include a self-alignment structure as illustrated in FIGS. 55 and 56.


In one example illustrated in FIG. 55, the optical imaging system 100 includes a self-alignment structure in which optical axes of four consecutive lenses 1000, 2000, 3000, and 4000 are aligned with an optical axis of the optical imaging system 100 by coupling the four lenses 1000, 2000, 3000, and 4000 to one another.


The first lens 1000 disposed closest to an object side of the optical imaging system 100 is disposed in contact with an inner surface of the lens barrel 200 to align the optical axis of the first lens 1000 with the optical axis of the optical imaging system 100, the second lens 2000 is coupled to the first lens 1000 to align the optical axis of the second lens 2000 with the optical axis of the optical imaging system 100, the third lens 3000 is coupled to the second lens 2000 to align the optical axis of the third lens 3000 with the optical axis of the optical imaging system 100, and the fourth lens 4000 is coupled to the third lens 3000 to align the optical axis of the fourth lens 4000 with the optical axis of the optical imaging system 100. The second lens 2000 to the fourth lens 4000 may not be disposed in contact with the inner surface of the lens barrel 200.


Although FIG. 55 illustrates that the first lens 1000 to the fourth lens 4000 are coupled to one another, the four consecutive lenses that are coupled to one another may be changed to the second lens 2000 to a fifth lens 5000, the third lens 3000 to a sixth lens 6000, or the fourth lens 4000 to a seventh lens 7000.


In another example illustrated in FIG. 56, the optical imaging system 100 includes a self-alignment structure in which optical axes of five consecutive lenses 1000, 2000, 3000, 4000, and 5000 are aligned with an optical axis of the optical imaging system 100 by coupling the five lenses 1000, 2000, 3000, 4000, and 5000 to one another.


The first lens 1000 disposed closest to an object side of the optical imaging system 100 is disposed in contact with an inner surface of the lens barrel 200 to align an optical axis of the first lens 1000 with the optical axis of the optical imaging system 100, the second lens 2000 is coupled to the first lens 1000 to align the optical axis of the second lens 2000 with the optical axis of the optical imaging system 100, the third lens 3000 is coupled to the second lens 2000 to align the optical axis of the third lens 3000 with the optical axis of the optical imaging system 100, the fourth lens 4000 is coupled to the third lens 3000 to align the optical axis of the fourth lens 4000 with the optical axis of the optical imaging system 100, and the fifth lens 5000 is coupled to the fourth lens 4000 to align the optical axis of the fifth lens 5000 with the optical axis of the optical imaging system 100. The second lens 2000 to the fifth lens 5000 may not be disposed in contact with the inner surface of the lens barrel 200.


Although FIG. 56 illustrates that the first lens 1000 to the fifth lens 5000 are coupled to one another, the five consecutive lenses that are coupled to one another may be changed to the second lens 2000 to a sixth lens 6000, or the third lens 3000 to a seventh lens 7000.


The first lens 1000 is a lens closest to an object (or a subject) to be imaged by the optical imaging system 100, while the seventh lens 7000 is a lens closest to an image sensor (not shown in FIGS. 55 and 56, but see the image sensor 190 in FIG. 1, for example).


In addition, an object-side surface of a lens is a surface of the lens facing the object, and an image-side surface of a lens is a surface of the lens facing the image sensor.


The examples of the optical imaging system 100 disclosed in this application include seven lenses.


For example, referring to FIGS. 55 and 56, the optical imaging system 100 includes a first lens 1000, a second lens 2000, a third lens 3000, a fourth lens 4000, a fifth lens 5000, a sixth lens 6000, and a seventh lens 7000 sequentially disposed in numerical order along an optical axis of the optical imaging system 100 from an object side of the optical imaging system 100 toward an imaging plane of the optical imaging system 100.


The optical imaging system 100 further includes an image sensor and a filter. The image sensor forms an imaging plane, and converts light refracted by the first to seventh lenses into an electric signal. The filter is disposed between the seventh lens and the imaging plane, and blocks infrared rays in the light refracted by the first to seventh lenses from being incident on the imaging plane.


In addition, the optical imaging system 100 further includes a stop to adjust an amount of light incident on the imaging plane. For example, the stop may be disposed in front of the first lens 1000, or between the first lens 1000 and the second lens 2000, or between the second lens 2000 and the third lens 3000, or at the position of either an object-side surface or an image-side surface of one of the first lens 1000 to the third lens 3000. The stop may be disposed relatively close to the first lens 1000 to reduce a total length (TTL) of the optical imaging system 100. Some examples may include two stops, one of which may be disposed in front of the first lens 1000, or at the position of the object-side surface of the first lens 1000, or between the object-side surface and the image-side surface of the first lens 1000.


In the examples illustrated in FIGS. 55 and 56, a spacer is disposed between each pair of adjacent lenses. At least a portion of the rib of each lens is in contact with one or two of the spacers. The spacers maintain spacings between the lenses, and block stray light from reaching the imaging plane.


The spacers include a first spacer SP1, a second spacer SP2, a third spacer SP3, a fourth spacer SP4, a fifth spacer SP5, and a sixth spacer SP6 disposed from the object side of the optical imaging system 100 toward the image sensor. In some examples, the spacers further include a seventh spacer SP7.


The first spacer SP1 is disposed between the first lens 1000 and the second lens 2000, the second spacer SP2 is disposed between the second lens 2000 and the third lens 3000, the third spacer SP3 is disposed between the third lens 3000 and the fourth lens 4000, the fourth spacer SP4 is disposed between the fourth lens 4000 and the fifth lens 5000, the fifth spacer SP5 is disposed between the fifth lens 5000 and the sixth lens 6000, and the sixth spacer SP6 is disposed between the sixth lens 6000 and the seventh lens 7000. When the seventh spacer SP7 is included, the seventh spacer SP7 is disposed between the sixth lens 6000 and the sixth spacer SP6. A thickness of the seventh spacer SP7 in an optical axis direction may be greater than a thickness of the sixth spacer SP6 in the optical axis direction.


The first lens has a positive refractive power or a negative refractive power. In addition, the first lens may have a meniscus shape of which an object-side surface is convex. In detail, an object-side surface of the first lens may be convex, and an image-side surface thereof may be concave.


At least one of the object-side surface and the image-side surface of the first lens may be aspherical. For example, both surfaces of the first lens may be aspherical.


The second lens has a positive refractive power or a negative refractive power. In addition, the second lens may have a meniscus shape of which an object-side surface is convex. In detail, an object-side surface of the second lens may be convex, and an image-side surface thereof may be concave.


Alternatively, both surfaces of the second lens may be convex. In detail, the object-side surface and the image-side surface of the second lens may be convex.


At least one of the object-side surface and the image-side surface of the second lens may be aspherical. For example, both surfaces of the second lens may be aspherical.


The third lens has a positive refractive power or a negative refractive power. In addition, the third lens may have a meniscus shape of which an object-side surface is convex. In detail, an object-side surface of the third lens may be convex, and an image-side surface thereof may be concave.


Alternatively, both surfaces of the third lens may be convex. In detail, the object-side surface and the image-side surface of the third lens may be convex.


Alternatively, the third lens may have a meniscus shape of which an image-side surface is convex. In detail, an object-side surface of the third lens may be concave, and an image-side surface thereof may be convex.


At least one of the object-side surface and the image-side surface of the third lens may be aspherical. For example, both surfaces of the third lens may be aspherical.


The fourth lens has a positive refractive power or a negative refractive power. In addition, the fourth lens may have a meniscus shape of which an object-side surface is convex. In detail, an object-side surface of the fourth lens may be convex, and an image-side surface thereof may be concave.


Alternatively, both surfaces of the fourth lens may be convex. In detail, the object-side surface and the image-side surface of the fourth lens may be convex.


Alternatively, the fourth lens may have a meniscus shape of which an image-side surface is convex. In detail, an object-side surface of the fourth lens may be concave, and an image-side surface thereof may be convex.


At least one of the object-side surface and the image-side surface of the fourth lens may be aspherical. For example, both surfaces of the fourth lens may be aspherical.


The fifth lens has a positive refractive power or a negative refractive power. In addition, the fifth lens may have a meniscus shape of which an object-side surface is convex. In detail, an object-side surface of the fifth lens may be convex, and an image-side surface thereof may be concave.


Alternatively, the fifth lens may have a meniscus shape of which an image-side surface is convex. In detail, an object-side surface of the fifth lens may be concave, and an image-side surface thereof may be convex.


At least one of the object-side surface and the image-side surface of the fifth lens may be aspherical. For example, both surfaces of the fifth lens may be aspherical.


The sixth lens has a positive refractive power or a negative refractive power. In addition, the sixth lens may have a meniscus shape of which an object-side surface is convex. In detail, an object-side surface of the sixth lens may be convex, and an image-side surface thereof may be concave.


Alternatively, both surfaces of the sixth lens may be convex. In detail, the object-side surface and the image-side surface of the sixth lens may be convex.


Alternatively, the sixth lens may have a meniscus shape of which an image-side surface is convex. In detail, an object-side surface of the sixth lens may be concave, and an image-side surface thereof may be convex.


Alternatively, both surfaces of the sixth lens may be concave. In detail, the object-side surface and the image-side surface of the sixth lens may be concave.


At least one of the object-side surface and the image-side surface of the sixth lens may be aspherical. For example, both surfaces of the sixth lens may be aspherical.


The seventh lens has a positive refractive power or a negative refractive power. In addition, the seventh lens may have a meniscus shape of which an object-side surface is convex. In detail, an object-side surface of the seventh lens may be convex, and an image-side surface thereof may be concave.


Alternatively, both surfaces of the seventh lens may be concave. In detail, the object-side surface and the image-side surface of the seventh lens may be concave.


At least one of the object-side surface and the image-side surface of the seventh lens may be aspherical. For example, both surfaces of the seventh lens may be aspherical.


In addition, at least one inflection point may be formed on at least one of the object-side surface and the image-side surface of the seventh lens. An inflection point is a point where a lens surface changes from convex to concave, or from concave to convex. A number of inflection points is counted from a center of the lens to an outer edge of the optical portion of the lens. For example, the object-side surface of the seventh lens may be convex in a paraxial region, and become concave toward an edge thereof. The image-side surface of the seventh lens may be concave in a paraxial region, and become convex toward an edge thereof.



FIG. 57 is a cross-sectional view illustrating an example of a shape of a rib of a seventh lens.


Light reflected from the object (or the subject) may be refracted by the first to seventh lenses. In this case, an unintended reflection of the light may occur. The unintended reflection of the light, which is light unrelated to formation of an image, may cause a flare phenomenon in a captured image.


The examples of the optical imaging system 100 described in this application may include a structure for preventing a flare phenomenon and reflection.


For example, as illustrated in FIG. 57, a rib of the seventh lens 7000 disposed closest to the image sensor includes a surface-treated area EA. The surface-treated area EA is a portion of a surface of the rib that has been surface-treated to be rougher than other portions of the surface of the rib. For example, the surface-treated area EA may be formed by chemical etching, physical grinding, or any other surface treatment method capable of increasing a roughness of a surface. The surface-treated area EA scatters reflected light.


Therefore, even though the unintended reflection of the light may occur, the reflected light is prevented from being concentrated at one point, and therefore the occurrence of the flare phenomenon may be suppressed.


The surface-treated area EA may be formed in an entire area from an edge of the optical portion of the seventh lens 7000 through which light actually passes to an outer end of the rib. However, as illustrated in FIG. 57, non-treated areas NEA including step portions E11, E21, and E22 may not be surface-treated, or may be surface-treated to have a roughness less than a roughness of the surface-treated area EA. The step portions E11, E21, and E22 are portions where the thickness of the rib abruptly changes. A first non-treated area NEA formed on an object-side surface of the seventh lens 7000 and including a first step portion E1l and a second non-treated area NEA formed on an image-side surface of the seventh lens 7000 and including a second step portion E12 and a third step portion E22 may overlap when viewed in the optical axis direction.


A width G1 of the first non-treated area NEA formed on the object-side surface of the seventh lens 7000 may be different from a width G2 of the second non-treated area NEA formed on the image-side surface of the seventh lens 7000. In the example illustrated in FIG. 57, G1 is greater than G2.


The width G1 of the first non-treated area NEA includes the first step portion E11, the second step portion E21, and the third step portion E22 when viewed in the optical axis direction, and a width of the second non-treated area NEA includes the second step portion E21 and the third step portion E22 but not the first step portion E11 when viewed in the optical axis direction. A distance G4 from the outer end of the rib to the second step portion E21 is smaller than a distance G3 from the outer end of the rib to the first step portion E11. Similarly, a distance G5 from the outer end of the rib to the third step portion E22 is smaller than the distance G3 from the outer end of the rib to the first step portion E11.


The positions at which the non-treated areas NEA and the step portions E11, E21, and E22 are formed as described above and shown in FIG. 57 may be advantageous for measuring a concentricity of the seventh lens 7000.


The lenses of the optical imaging system may be made of a light material having a high light transmittance. For example, the first to seventh lenses may be made of a plastic material. However, a material of the first to seventh lenses is not limited to the plastic material.


In addition, the first to seventh lenses may have at least one aspherical surface. That is, at least one of the object-side surface and the image-side surface of all of the first to seventh lenses may be aspherical. The aspherical surfaces of the first to seventh lenses may be represented by the following Equation 1:









Z
=



cY
2


1
+


1
-


(

1
+
K

)



c
2



Y
2






+

AY
4

+

BY
6

+

CY
8

+

DY
10

+

E


Y

1

2



+

FY

1

4


+

G


Y

1

6



+

HY

1

8


+






(
1
)







In Equation 1, c is a curvature of a lens surface and is equal to an inverse of a radius of curvature of the lens surface at an optical axis of the lens surface, K is a conic constant, Y is a distance from a certain point on an aspherical surface of the lens to an optical axis of the lens in a direction perpendicular to the optical axis, A to H are aspherical constants, Z (or sag) is a distance between the certain point on the aspherical surface of the lens at the distance Y to the optical axis and a tangential plane perpendicular to the optical axis meeting the apex of the aspherical surface of the lens. Some of the examples disclosed in this application include an aspherical constant J. An additional term of JY20 may be added to the right side of Equation 1 to reflect the effect of the aspherical constant J.


The optical imaging system may satisfy one or more of the following Conditional Expressions 1 to 5:

0.1<L1w/L7w<0.4  (Conditional Expression 1)
0.5<S6d/f<1.4  (Conditional Expression 2)
0.4<L1TR/L7TR<1.9  (Conditional Expression 3)
0.5<L1234TRavg/L7TR<0.9  (Conditional Expression 4)
0.5<L12345TRavg/L7TR<0.9  (Conditional Expression 5)


In the above Conditional Expressions, L1w is a weight of the first lens, and L7w is a weight of the seventh lens.


S6d is an inner diameter of the sixth spacer, and f is an overall focal length of the optical imaging system.


L1TR is an overall outer diameter of the first lens, and L7TR is an overall outer diameter of the seventh lens. The overall outer diameter of a lens is an outer diameter of the lens including both the optical portion of the lens and the rib of the lens.


L1234TRavg is an average value of overall outer diameters of the first to fourth lenses, and L12345TRavg is an average value of overall outer diameters of the first to fifth lenses.


Conditional Expression 1 is a conditional expression related to a weight ratio between the first lens and the seventh lens, and when Conditional Expression 1 is satisfied, optical axes may be easily aligned with one another through contact between the respective lenses and contact between the lenses and the lens barrel.


Conditional Expression 2 is a conditional expression related to a ratio between the inner diameter of the sixth spacer disposed between the sixth lens and the seventh lens and the overall focal length of the optical imaging system, and when Conditional Expression 2 is satisfied, the flare phenomenon due to the unintended reflection of the light may be suppressed.


Conditional Expression 3 is a conditional expression related to a ratio between the overall outer diameter of the first lens and the overall outer diameter of the seventh lens, and when Conditional Expression 3 is satisfied, optical axes may be easily aligned with one another through contact between the respective lenses and contact between the lenses and the lens barrel.


Conditional Expression 4 is a conditional expression related to a ratio between the average value of the overall outer diameters of the first to fourth lenses and the overall outer diameter of the seventh lens, and when Conditional Expression 4 is satisfied, aberration may be easily corrected to improve resolution.


Conditional Expression 5 is a conditional expression related to a ratio between the average value of the overall outer diameters of the first to fifth lenses and the overall outer diameter of the seventh lens, and when Conditional Expression 5 is satisfied, aberration may be easily corrected to improve resolution.


The optical imaging system may also satisfy one or more of the following Conditional Expressions 6 to 10:

0.1<L1w/L7w<0.3  (Conditional Expression 6)
0.5<S6d/f<1.2  (Conditional Expression 7)
0.4<L1TR/L7TR<0.7  (Conditional Expression 8)
0.5<L1234TRavg/L7TR<0.75  (Conditional Expression 9)
0.5<L12345TRavg/L7TR<0.76  (Conditional Expression 10)


Conditional Expressions 6 to 10 are the same as Conditional Expressions 1 to 5, except that Conditional Expressions 6 to 10 specify narrower ranges.


The optical imaging system may also satisfy one or more of the following Conditional Expressions 11 to 32:

0.01<R1/R4<1.3  (Conditional Expression 11)
0.1<R1/R5<0.7  (Conditional Expression 12)
0.05<R1/R6<0.9  (Conditional Expression 13)
0.2<R1/R11<1.2  (Conditional Expression 14)
0.8<R1/R14<1.2  (Conditional Expression 15)
0.6<(R11+R14)/(2*R1)<3.0  (Conditional Expression 16)
0.4<D13/D57<1.2  (Conditional Expression 17)
0.1<(1/f1+1/f2+1/f3+1/f4+1/f5+1/f6+1/f7)*f<0.8  (Conditional Expression 18)
0.1<(1/f1+1/f2+1/f3+1/f4+1/f5+1/f6+1/f7)*TTL<1.0   (Conditional Expression 19)
0.2<TD1/D67<0.8  (Conditional Expression 20)
0.1<(R11+R14)/(R5+R6)<1.0  (Conditional Expression 21)
SD12<SD34  (Conditional Expression 22)
SD56<SD67  (Conditional Expression 23)
SD56<SD34  (Conditional Expression 24)
0.6<TTL/(2*IMG HT)<0.9  (Conditional Expression 25)
0.2<ΣSD/ΣTD<0.7  (Conditional Expression 26)
0<min(f1:f3)/max(f4:f7)<0.4  (Conditional Expression 27)
0.4<ΣTD/TTL<0.7  (Conditional Expression 28)
0.7<SL/TTL<1.0  (Conditional Expression 29)
0.81<f12/f123<0.96  (Conditional Expression 30)
0.6<f12/f1234<0.84  (Conditional Expression 31)
TTL≤6.00  (Conditional Expression 32)


In the above Conditional Expressions, R1 is a radius of curvature of an object-side surface of the first lens, R4 is a radius of curvature of an image-side surface of the second lens, 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, R11 is a radius of curvature of an object-side surface of the sixth lens, and R14 is a radius of curvature of an image-side surface of the seventh lens.


D13 is a distance along an optical axis of the optical imaging system from the object-side surface of the first lens to the image-side surface of the third lens, and D57 is a distance along the optical axis from an object-side surface of the fifth lens to the image-side surface of the seventh lens.


f1 is a focal length of the first lens, f2 is a focal length of the second lens, f3 is a focal length of the third lens, f4 is a focal length of the fourth lens, f5 is a focal length of the fifth lens, f6 is a focal length of the sixth lens, f7 is a focal length of the seventh lens, f is an overall focal length of the optical imaging system, and TTL is a distance along the optical axis from the object-side surface of the first lens to an imaging plane of an image sensor of the optical imaging system.


TD1 is a thickness along the optical axis of the first lens, and D67 is a distance along the optical axis from the object-side surface of the sixth lens to the image-side surface of the seventh lens.


SD12 is a distance along the optical axis from an image-side surface of the first lens to an object-side surface of the second lens, SD34 is a distance along the optical axis from the image-side surface of the third lens to an object-side surface of the fourth lens, SD56 is a distance along the optical axis from an image-side surface of the fifth lens to the object-side surface of the sixth lens, and SD67 is a distance along the optical axis from an image-side surface of the sixth lens to an object-side surface of the seventh lens.


IMG HT is one-half of a diagonal length of the imaging plane of the image sensor.


ΣSD is a sum of air gaps along the optical axis between the first to seventh lenses, and ΣTD is a sum of thicknesses along the optical axis of the first to seventh lenses. An air gap is a distance along the optical axis between adjacent ones of the first to seventh lenses.


min(f1:f3) is a minimum value of absolute values of the focal lengths of the first to third lenses, and max(f4:f7) is a maximum value of absolute values of the focal lengths of the fourth to seventh lenses.


SL is a distance along the optical axis from the stop to the imaging plane of the image sensor.


f12 is a composite focal length of the first and second lenses, f123 is a composite focal length of the first to third lenses, and f1234 is a composite focal length of the first to fourth lenses.


When Conditional Expression 11 is satisfied, correction effects of longitudinal spherical aberration and astigmatic field curves may be improved, and resolution may thus be improved.


When Conditional Expression 12 is satisfied, correction effects of longitudinal spherical aberration and astigmatic field curves may be improved, and resolution may thus be improved.


When Conditional Expression 13 is satisfied, correction effects of longitudinal spherical aberration and astigmatic field curves may be improved, and resolution may thus be improved.


When Conditional Expression 14 is satisfied, a correction effect of longitudinal spherical aberration may be improved, and the flare phenomenon may be prevented. Therefore, resolution may be improved.


When Conditional Expression 15 is satisfied, a correction effect of longitudinal spherical aberration may be improved, and an imaging plane curvature phenomenon may be suppressed. Therefore, resolution may be improved.


When Conditional Expression 16 is satisfied, a correction effect of longitudinal spherical aberration may be improved, an imaging plane curvature phenomenon may be suppressed, and the flare phenomenon may be prevented. Therefore, resolution may be improved.


When Conditional Expression 17 is satisfied, a slim optical imaging system may be implemented.


When Conditional Expression 18 is satisfied, sensitivity of each lens may be improved to improve mass productivity.


When Conditional Expression 20 is satisfied, a slim optical imaging system may be implemented.


When Conditional Expression 22 is satisfied, a chromatic aberration correction effect may be improved.


When Conditional Expression 25 is satisfied, a slim optical imaging system may be implemented.


When Conditional Expression 26 is satisfied, mass productivity of each lens may be improved, and a slim optical imaging system may be implemented.


When Conditional Expression 27 is satisfied, a slim optical imaging system may be implemented.


When Conditional Expression 28 is satisfied, mass productivity of each lens may be improved, and a slim optical imaging system may be implemented.


When Conditional Expression 29 is satisfied, a slim optical imaging system may be implemented.


When Conditional Expression 30 is satisfied, a slim optical imaging system may be implemented.


When Conditional Expression 31 is satisfied, a slim optical imaging system may be implemented.


Next, various examples of the optical imaging system will be described. In the tables that appear in the following examples, S1 denotes an object-side surface of a first lens, S2 denotes an image-side surface of the first lens, S3 denotes an object-side surface of a second lens, S4 denotes an image-side surface of the second lens, S5 denotes an object-side surface of a third lens, S6 denotes an image-side surface of the third lens, S7 denotes an object-side surface of a fourth lens, S8 denotes an image-side surface of the fourth lens, S9 denotes an object-side surface of a fifth lens, S10 denotes an image-side surface of the fifth lens, S11 denotes an object-side surface of a sixth lens, S12 denotes an image-side surface of the sixth lens, S13 denotes an object-side surface of a seventh lens, S14 denotes an image-side surface of the seventh lens, S15 denotes an object-side surface of a filter, S16 denotes an image-side surface of the filter, and S17 denotes an imaging plane.


First Example


FIG. 1 is a view illustrating a first example of an optical imaging system, and FIG. 2 illustrates aberration curves of the optical imaging system of FIG. 1.


The first example of the optical imaging system includes a first lens 110, a second lens 120, a third lens 130, a fourth lens 140, a fifth lens 150, a sixth lens 160, a seventh lens 170, a filter 180, an image sensor 190, and a stop (not shown) disposed between the second lens 120 and the third lens 130.


The first lens 110 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 120 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 130 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 140 has a positive refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The fifth lens 150 has a negative refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The sixth lens 160 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 170 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


Two inflection points are formed on the object-side surface of the seventh lens 170. For example, the object-side surface of the seventh lens 170 is convex in the paraxial region, becomes concave in a region outside the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 170. For example, the image-side surface of the seventh lens 170 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 1, the stop is disposed at a distance of 0.657 mm from the object-side surface of the first lens 110 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 1 listed in Table 55 that appears later in this application.


Table 1 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 1, and Table 2 below shows aspherical surface coefficients of the lenses of FIG. 1. Both surfaces of all of the lenses of FIG. 1 are aspherical.















TABLE 1











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.30380276
0.4873118
1.546
56.114
0.90


S2
Lens
4.10661787
0.02


0.86


S3
Second
3.13219869
0.15
1.669
20.353
0.83


S4
Lens
1.99733595
0.1652259


0.76


S5
Third
3.1434573
0.2269519
1.546
56.114
0.77


S6
Lens
5.17017622
0.2383823


0.80


S7
Fourth
−18.619397
0.2512803
1.546
56.114
0.85


S8
Lens
−13.597043
0.242844


1.00


S9
Fifth
−3.8728179
0.23
1.658
21.494
1.06


S10
Lens
−6.4514212
0.1738361


1.35


S11
Sixth
3.37627601
0.3819845
1.658
21.494
1.61


S12
Lens
3.69563051
0.2187456


1.82


S13
Seventh
1.64903762
0.4758711
1.537
55.711
2.42


S14
Lens
1.23703219
0.1960644


2.56


S15
Filter
Infinity
0.11
1.519
64.197
2.91


S16

Infinity
0.6315021


2.94


S17
Imaging
Infinity



3.27



Plane


























TABLE 2







K
A
B
C
D
E
F
G
H

























S1
−0.04855
−0.0104
0.079678
−0.44646
1.099882
−1.60116
1.122811
−0.33899
0


S2
−11.0924
−0.12752
0.167469
0.110923
−1.28207
2.595792
−2.35953
0.804002
0


S3
−1.78612
−0.15851
0.372646
−0.41814
0.573916
−0.88442
1.331314
−0.80599
0


S4
0.5857
−0.06147
0.150875
0.049867
−0.07429
−0.56511
2.092798
−1.36903
0


S5
3.760167
−0.10504
0.175441
−1.2896
5.059804
−10.8279
12.59218
−5.43044
0


S6
0.084295
−0.07194
−0.02894
0.170897
−0.94476
3.211016
−4.65595
3.037354
0


S7
5.45E−09
−0.14415
−0.13498
0.106142
−0.23108
0.696801
−0.58859
0.153297
0


S8
−5.2E−09
−0.10523
−0.05764
−0.27895
0.581635
−0.34032
0.074355
−0.00428
0


S9
−0.32032
−0.09812
0.288941
−1.04554
1.187968
−0.44999
−0.09128
0.062806
0


S10
8.754232
−0.15044
0.20833
−0.46969
0.543726
−0.29268
0.072698
−0.00679
0


S11
−50
0.123875
−0.5262
0.671582
−0.54174
0.252604
−0.06038
0.005742
0


S12
−34.5841
0.046016
−0.26854
0.301454
−0.1998
0.076707
−0.01561
0.001299
0


S13
−0.95155
−0.4722
0.187431
−0.00725
−0.01893
0.007221
−0.00124
0.000106
−3.7E−06


S14
−1.03036
−0.43108
0.275378
−0.13928
0.050665
−0.01212
0.001769
−0.00014
4.72E−06









Second Example


FIG. 3 is a view illustrating a second example of an optical imaging system, and FIG. 4 illustrates aberration curves of the optical imaging system of FIG. 3.


The second example of the optical imaging system includes a first lens 210, a second lens 220, a third lens 230, a fourth lens 240, a fifth lens 250, a sixth lens 260, a seventh lens 270, a filter 280, an image sensor 290, and a stop (not shown) disposed between the first lens 210 and the second lens 220.


The first lens 210 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 220 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 230 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The fourth lens 240 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 250 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 260 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The seventh lens 270 has a negative refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 270. For example, the object-side surface of the seventh lens 270 is concave in the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 270. For example, the image-side surface of the seventh lens 270 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 3, the stop is disposed at a distance of 0.903 mm from the object-side surface of the first lens 210 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 2 listed in Table 55 that appears later in this application.


Table 3 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 3, and Table 4 below shows aspherical surface coefficients of the lenses of FIG. 3. Both surfaces of all of the lenses of FIG. 3 are aspherical except for the object-side surface of the second lens 220, which is spherical.















TABLE 3











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
2.05360683
0.9034685
1.546
56.114
1.57


S2
Lens
8.69896228
0.1210039


1.51


S3
Second
5.79844164
0.23
1.669
20.353
1.41


S4
Lens
3.28223873
0.3719948


1.25


S5
Third
18.2422536
0.5019823
1.546
56.114
1.28


S6
Lens
−30.831764
0.1291516


1.40


S7
Fourth
9.45562649
0.26
1.669
20.353
1.42


S8
Lens
6.85294408
0.2841745


1.59


S9
Fifth
114.717743
0.3398848
1.669
20.353
1.70


S10
Lens
7.75029311
0.2357371


1.96


S11
Sixth
3.82957626
0.8015174
1.546
56.114
2.27


S12
Lens
−2.3157266
0.5095283


2.53


S13
Seventh
−2.7230919
0.38
1.546
56.114
3.25


S14
Lens
2.76379359
0.1236113


3.50


S15
Filter
Infinity
0.11
1.519
64.197
3.79


S16

Infinity
0.697957


3.82


S17
Imaging
Infinity



4.19



Plane


























TABLE 4






K
A
B
C
D
E
F
G
H
J

























S1
−1.06281
0.01395
0.00941
−0.01412
0.016751
−0.01213
0.005246
−0.00125
0.000113
0


S2
10.99365
−0.0496
0.043223
−0.02678
0.01076
−0.00422
0.001531
−0.00036
3.39E−05
0


S3
0
0
0
0
0
0
0
0
0
0


S4
−1.57846
−0.06964
0.064533
0.011426
−0.07261
0.078892
−0.04113
0.010258
−0.00062
0


S5
0
−0.02505
0.012832
−0.06832
0.114397
−0.11363
0.062176
−0.01694
0.001754
0


S6
−95
−0.06124
−0.00208
0.018185
−0.0574
0.078131
−0.05827
0.022909
−0.0037
0


S7
0
−0.13045
0.042894
−0.12127
0.185066
−0.15794
0.079696
−0.02253
0.002763
0


S8
0
−0.10238
0.076048
−0.14731
0.180393
−0.13452
0.060052
−0.01498
0.001622
0


S9
0
−0.12987
0.161036
−0.15532
0.106502
−0.05376
0.017897
−0.00352
0.000315
0


S10
3.618339
−0.19523
0.14843
−0.11064
0.069557
−0.03186
0.009112
−0.00141
8.97E−05
0


S11
−19.5338
−0.02618
−0.01422
0.001668
0.00202
−0.00126
0.0003
−2.8E−05
5.96E−07
0


S12
−0.77737
0.093402
−0.07013
0.024503
−0.00579
0.001227
−0.0002
1.83E−05
−6.9E−07
0


S13
−17.9057
−0.104
0.008741
0.01022
−0.0036
0.000564
−4.8E−05
2.21E−06
−4.2E−08
0


S14
−0.59751
−0.10999
0.036578
−0.00899
0.001629
−0.00023
2.28E−05
−1.5E−06
6.25E−08
−1.1E−09









Third Example


FIG. 5 is a view illustrating a third example of an optical imaging system, and FIG. 6 illustrates aberration curves of the optical imaging system of FIG. 5.


The third example of the optical imaging system includes a first lens 310, a second lens 320, a third lens 330, a fourth lens 340, a fifth lens 350, a sixth lens 360, a seventh lens 370, a filter 380, an image sensor 390, and a stop (not shown) disposed between the first lens 310 and the second lens 320.


The first lens 310 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 320 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 330 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 340 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 350 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 360 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The seventh lens 370 has a negative refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 370. For example, the object-side surface of the seventh lens 370 is concave in the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 370. For example, the image-side surface of the seventh lens 370 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 5, the stop is disposed at a distance of 0.818 mm from the object-side surface of the first lens 310 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 3 listed in Table 55 that appears later in this application.


Table 5 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 5, and Table 6 below shows aspherical surface coefficients of the lenses of FIG. 5. Both surfaces of all of the lenses of FIG. 5 are aspherical except for the object-side surface of the second lens 320, which is spherical.















TABLE 5











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.77268075
0.8181175
1.546
56.114
1.38


S2
Lens
7.43505234
0.0795954


1.33


S3
Second
5.04692927
0.2
1.669
20.353
1.25


S4
Lens
2.94768599
0.3757836


1.10


S5
Third
12.3815508
0.4065563
1.546
56.114
1.13


S6
Lens
25.2118728
0.1314045


1.23


S7
Fourth
5.68409727
0.219
1.669
20.353
1.25


S8
Lens
4.4061916
0.151293


1.41


S9
Fifth
27.7177102
0.3053613
1.644
23.516
1.47


S10
Lens
8.05648759
0.219293


1.71


S11
Sixth
4.76866792
0.6346891
1.546
56.114
1.93


S12
Lens
−1.5557108
0.3548236


2.15


S13
Seventh
−2.2362248
0.373515
1.546
56.114
2.75


S14
Lens
2.35098563
0.1948647


2.96


S15
Filter
Infinity
0.21
1.519
64.197
3.31


S16

Infinity
0.6157031


3.37


S17
Imaging
Infinity



3.70



Plane


























TABLE 6






K
A
B
C
D
E
F
G
H
J

























S1
−1.0302
0.018188
0.032245
−0.07196
0.112928
−0.10738
0.060719
−0.01872
0.002295
0


S2
9.43023
−0.10102
0.141494
−0.11688
0.038896
0.013478
−0.02044
0.008552
−0.00134
0


S3
0
0
0
0
0
0
0
0
0
0


S4
−0.50537
−0.10697
0.153004
0.009755
−0.29683
0.477095
−0.35748
0.129532
−0.01458
0


S5
0
−0.05254
0.023493
−0.1143
0.214047
−0.26482
0.177126
−0.05517
0.005476
0


S6
−99
−0.11144
0.07916
−0.20212
0.267335
−0.18518
0.019544
0.044285
−0.01687
0


S7
0
−0.20077
0.140611
−0.37803
0.453081
−0.18096
−0.09799
0.111673
−0.02809
0


S8
0
−0.20577
0.304963
−0.59986
0.731946
−0.53515
0.225984
−0.05251
0.005575
0


S9
0
−0.28358
0.467356
−0.47172
0.280955
−0.07421
−0.01626
0.014562
−0.00242
0


S10
2.862598
−0.31693
0.301196
−0.21698
0.125203
−0.05589
0.017401
−0.00325
0.000272
0


S11
−19.5338
−0.07211
−0.00681
0.001046
0.009791
−0.00904
0.002973
−0.00036
8.29E−06
0


S12
−1.13682
0.173265
−0.16996
0.078719
−0.01703
0.000973
0.000343
−7.9E−05
 5.3E−06
0


S13
−13.4335
−0.08518
−0.04504
0.056746
−0.02132
0.004215
−0.00048
2.92E−05
−7.6E−07
0


S14
−0.68587
−0.15974
0.072817
−0.02745
0.00783
−0.00164
0.000238
−2.3E−05
1.25E−06
−3E−08









Fourth Example


FIG. 7 is a view illustrating a fourth example of an optical imaging system, and FIG. 8 illustrates aberration curves of the optical imaging system of FIG. 7.


The fourth example of the optical imaging system includes a first lens 410, a second lens 420, a third lens 430, a fourth lens 440, a fifth lens 450, a sixth lens 460, a seventh lens 470, a filter 480, an image sensor 490, and a stop (not shown) disposed between the second lens 420 and the third lens 430.


The first lens 410 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 420 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The third lens 430 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 440 has a positive refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The fifth lens 450 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 460 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 470 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


Two inflection points are formed on the object-side surface of the seventh lens 470. For example, the object-side surface of the seventh lens 470 is convex in the paraxial region, becomes concave in a region outside the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 470. For example, the image-side surface of the seventh lens 470 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 7, the stop is disposed at a distance of 1.160 mm from the object-side surface of the first lens 410 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 4 listed in Table 55 that appears later in this application.


Table 7 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 7, and Table 8 below shows aspherical surface coefficients of the lenses of FIG. 7. Both surfaces of all of the lenses of FIG. 7 are aspherical.















TABLE 7











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.944433
0.44936
1.546
56.114
1.272


S2
Lens
2.977539
0.114456


1.251


S3
Second
2.684097
0.57757
1.546
56.114
1.214


S4
Lens
−14.8551
0.018539


1.179


S5
Third
4.307671
0.185386
1.679
19.236
1.072


S6
Lens
2.138972
0.559077


1.015


S7
Fourth
−1112.32
0.276572
1.679
19.236
1.177


S8
Lens
−1112.32
0.195337


1.351


S9
Fifth
3.11964
0.284764
1.546
56.114
1.590


S10
Lens
3.052659
0.21926


1.857


S11
Sixth
3.020575
0.350029
1.679
19.236
1.993


S12
Lens
2.4858
0.130575


2.317


S13
Seventh
1.44499
0.501569
1.537
53.955
2.663


S14
Lens
1.27E+00
0.243037


2.827


S15
Filter
Infinity
0.11
 1.5187
 64.1664
3.105532


S16

Infinity
0.596879


3.136694


S17
Imaging
Infinity



3.408113



Plane


























TABLE 8






K
A
B
C
D
E
F
G
H
J

























S1
−7.583
0.0888
−0.119
0.0923
−0.0948
0.0482
−0.003
−0.0042
0.0008
0


S2
−20.327
−0.0066
−0.1632
0.1025
0.0438
−0.0722
0.0262
−0.0005
−0.0011
0


S3
−0.2671
−0.0459
−0.0455
−0.027
0.1584
−0.0377
−0.1072
0.0826
−0.0186
0


S4
0
0.0277
−0.1403
0.1228
0.1799
−0.4927
0.4448
−0.186
0.03
0


S5
−4.5253
−0.0875
0.0631
−0.2483
0.8524
−1.3993
1.2015
−0.5193
0.0898
0


S6
0.5431
−0.123
0.1655
−0.2954
0.5449
−0.6999
0.5654
−0.2554
0.0541
0


S7
0
−0.0243
−0.1085
0.1778
−0.2176
0.2407
−0.2382
0.1432
−0.0356
0


S8
0
−0.0162
−0.1425
0.0788
0.0935
−0.1616
0.0885
−0.0169
0
0


S9
−43.017
0.1677
−0.2344
0.1196
−0.0548
0.0387
−0.0269
0.0094
−0.0012
0


S10
−5.2037
−0.0358
0.0999
−0.2203
0.2016
−0.1066
0.0335
−0.0057
0.0004
0


S11
−1.699
0.0343
−0.2737
0.3209
−0.2494
0.1179
−0.0316
0.0045
−0.0003
0


S12
−0.0013
−0.0989
−0.0458
0.0603
−0.0408
0.0165
−0.0038
0.0005
−2E−05 
0


S13
−0.8015
−0.5195
0.2893
−0.1079
0.0311
−0.0069
0.0011
−0.0001
7E−06
−2E−07


S14
−1.2781
−0.3766
0.2432
−0.1184
0.0416
−0.01
0.0016
−0.0002
9E−06
−2E−07









Fifth Example


FIG. 9 is a view illustrating a fifth example of an optical imaging system, and FIG. 10 illustrates aberration curves of the optical imaging system of FIG. 9.


The fifth example of the optical imaging system includes a first lens 510, a second lens 520, a third lens 530, a fourth lens 540, a fifth lens 550, a sixth lens 560, a seventh lens 570, a filter 580, an image sensor 590, and a stop (not shown) disposed between the second lens 520 and the third lens 530.


The first lens 510 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 520 has a positive refractive power, a paraxial region of each of an object-side surface of an image-side surface thereof is convex.


The third lens 530 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 540 has a negative refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The fifth lens 550 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 560 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 570 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


Two inflection points are formed on the object-side surface of the seventh lens 570. For example, the object-side surface of the seventh lens 570 is convex in the paraxial region, becomes concave in a region outside the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 570. For example, the image-side surface of the seventh lens 570 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 9, the stop is disposed at a distance of 1.169 mm from the object-side surface of the first lens 510 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 5 listed in Table 55 that appears later in this application.


Table 9 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 9, and Table 10 below shows aspherical surface coefficients of the lenses of FIG. 9. Both surfaces of all of the lenses of FIG. 9 are aspherical.















TABLE 9











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.951165
0.448752
1.546
56.114
1.307


S2
Lens
3.115162
0.125992


1.253


S3
Second
2.868611
0.575289
1.546
56.114
1.214


S4
Lens
−12.9825
0.018563


1.180


S5
Third
4.506414
0.185629
1.679
19.236
1.074


S6
Lens
2.196855
0.519693


1.016


S7
Fourth
−2108.87
0.279556
1.679
19.236
1.179


S8
Lens
−6755.44
0.171507


1.338


S9
Fifth
3.113522
0.273438
1.546
56.114
1.528


S10
Lens
3.267187
0.241671


1.808


S11
Sixth
3.22281
0.364954
1.679
19.236
1.996


S12
Lens
2.538835
0.143764


2.320


S13
Seventh
1.445077
0.51219
1.537
53.955
2.500


S14
Lens
1.27E+00
0.250094


2.738


S15
Filter
Infinity
0.11
1.5187
 64.1664
2.939872


S16

Infinity
0.597851


2.970893


S17
Imaging
Infinity



3.250775



Plane































TABLE 10






K
A
B
C
D
E
F
G
H
J

























S1
−7.5279
0.0857
−0.105
0.0528
−0.0256
−0.0221
0.0379
−0.0166
0.0023
0


S2
−19.893
−0.0142
−0.1337
0.0682
0.0621
−0.0783
0.0306
−0.0031
−0.0006
0


S3
−0.0142
−0.0449
−0.0418
−0.0147
0.1136
0.012
−0.1333
0.0892
−0.0193
0


S4
0
0.0281
−0.189
0.276
−0.0808
−0.2297
0.2908
−0.1382
0.024
0


S5
−6.2325
−0.0763
−0.0054
−0.0795
0.6054
−1.1875
1.107
−0.5047
0.0912
0


S6
0.4782
−0.115
0.1396
−0.2676
0.5637
−0.7991
0.6898
−0.325
0.0682
0


S7
0
−0.0188
−0.0772
0.0717
0.0184
−0.081
0.0225
0.0277
−0.0139
0


S8
0
−0.0127
−0.1356
0.0837
0.0781
−0.1502
0.0847
−0.0163
0
0


S9
−49.08
0.1815
−0.3205
0.2837
−0.2161
0.1317
−0.0595
0.0158
−0.0017
0


S10
−5.4303
−0.0205
0.025
−0.1003
0.1046
−0.0624
0.0222
−0.0043
0.0003
0


S11
−1.136
0.0314
−0.2615
0.3261
−0.2695
0.133
−0.0369
0.0053
−0.0003
0


S12
0.0272
−0.1293
0.0241
5E−05
−0.0123
0.0085
−0.0024
0.0003
−2E−05 
0


S13
−0.8
−0.5247
0.2994
−0.1227
0.0414
−0.0108
0.002
−0.0002
2E−05
−4E−07


S14
−1.3207
−0.3666
0.2425
−0.1248
0.0468
−0.0121
0.002
−0.0002
1E−05
−3E−07









Sixth Example


FIG. 11 is a view illustrating a sixth example of an optical imaging system, and FIG. 12 illustrates aberration curves of the optical imaging system of FIG. 11.


The sixth example of the optical imaging system includes a first lens 610, a second lens 620, a third lens 630, a fourth lens 640, a fifth lens 650, a sixth lens 660, a seventh lens 670, a filter 680, an image sensor 690, and a stop (not shown) disposed between the first lens 610 and the second lens 620.


The first lens 610 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 620 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 630 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 640 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 650 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 660 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The seventh lens 670 has a negative refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 670. For example, the object-side surface of the seventh lens 670 is concave in the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 670. For example, the image-side surface of the seventh lens 670 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 11, the stop is disposed at a distance of 0.383 mm from the object-side surface of the first lens 610 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 6 listed in Table 55 that appears later in this application.


Table 11 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 11, and Table 12 below shows aspherical surface coefficients of the lenses of FIG. 11. Both surfaces of all of the lenses of FIG. 11 are aspherical.















TABLE 11











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
2.182354
0.332873
1.546
56.114
1.380


S2
Lens
1.943873
0.05


1.369


S3
Second
1.685732
0.732159
1.546
56.114
1.335


S4
Lens
28.37273
0.05


1.264


S5
Third
7.153573
0.22
1.679
19.236
1.185


S6
Lens
2.922347
0.426406


1.050


S7
Fourth
46.9146
0.312126
1.646
23.528
1.112


S8
Lens
17.58601
0.26165


1.268


S9
Fifth
2.265526
0.27
1.646
23.528
1.774


S10
Lens
2.314346
0.373051


1.839


S11
Sixth
8.518581
0.607812
1.546
56.114
2.160


S12
Lens
−1.98711
0.378187


2.308


S13
Seventh
−4.7165
0.36
1.546
56.114
2.780


S14
Lens
1.89E+00
0.145735


2.998


S15
Filter
Infinity
0.11
1.5187
64.1664
3.352752


S16

Infinity
0.67


3.384589


S17
Imaging
Infinity



3.712027



Plane

























TABLE 12






K
A
B
C
D
E
F
G
H
























S1
−3.5715
0.0005
0.0011
−0.0181
0.0025
0.0107
−0.0084
0.0026
−0.0003


S2
−9.1496
−0.0513
−0.0055
0.0116
0.0161
−0.0207
0.0078
−0.001
0


S3
−2.5622
−0.0879
0.1115
−0.1204
0.1625
−0.1325
0.0578
−0.0118
0.0006


S4
−90
−0.078
0.2103
−0.4384
0.6397
−0.6153
0.3736
−0.1288
0.0189


S5
0
−0.1133
0.2975
−0.5447
0.7496
−0.7199
0.4525
−0.1642
0.0257


S6
4.6946
−0.0705
0.1434
−0.2144
0.1998
−0.0956
−0.0142
0.0399
−0.0137


S7
0
−0.0972
0.1221
−0.3303
0.5457
−0.6222
0.4555
−0.1995
0.0405


S8
0
−0.1596
0.2027
−0.3281
0.3412
−0.2472
0.1212
−0.0385
0.0064


S9
−18.27
−0.0564
−0.0069
0.0518
−0.0566
0.0228
−0.0011
−0.0019
0.0004


S10
−15.127
−0.0603
−0.0145
0.0594
−0.0601
0.0318
−0.0096
0.0015
−1E−04


S11
0
0.0027
−0.0398
0.025
−0.0137
0.005
−0.001
1E−04
−4E−06


S12
−1.1693
0.1224
−0.1006
0.0535
−0.0195
0.005
−0.0008
8E−05
−3E−06


S13
−4.4446
−0.097
−0.0137
0.0358
−0.0141
0.0028
−0.0003
2E−05
−5E−07


S14
−8.7431
−0.0906
0.0342
−0.009
0.0017
−0.0002
2E−05
−1E−06 
 3E−08









Seventh Example


FIG. 13 is a view illustrating a seventh example of an optical imaging system, and FIG. 14 illustrates aberration curves of the optical imaging system of FIG. 13.


The seventh example of the optical imaging system includes a first lens 710, a second lens 720, a third lens 730, a fourth lens 740, a fifth lens 750, a sixth lens 760, a seventh lens 770, a filter 780, an image sensor 790, and a stop (not shown) disposed between the first lens 710 and the second lens 720.


The first lens 710 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 720 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 730 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 740 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 750 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 760 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The seventh lens 770 has a negative refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 770. For example, the object-side surface of the seventh lens 770 is concave in the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 770. For example, the image-side surface of the seventh lens 770 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 13, the stop is disposed at a distance of 0.351 mm from the object-side surface of the first lens 710 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 7 listed in Table 55 that appears later in this application.


Table 13 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 13, and Table 14 below shows aspherical surface coefficients of the lenses of FIG. 13. Both surfaces of all of the lenses of FIG. 13 are aspherical.















TABLE 13











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
2.103288
0.300965
1.546
56.114
1.380


S2
Lens
1.828785
0.05


1.362


S3
Second
1.604129
0.748312
1.546
56.114
1.320


S4
Lens
21.76312
0.05


1.249


S5
Third
6.824657
0.22
1.679
19.236
1.185


S6
Lens
2.852069
0.418541


1.050


S7
Fourth
36.70533
0.30841
1.646
23.528
1.104


S8
Lens
23.6439
0.296196


1.268


S9
Fifth
2.423731
0.25
1.646
23.528
1.614


S10
Lens
2.468626
0.362929


1.874


S11
Sixth
8.604153
0.597419
1.546
56.114
2.160


S12
Lens
−1.90679
0.321858


2.300


S13
Seventh
−3.92912
0.36
1.546
56.114
2.780


S14
Lens
1.89E+00
0.135369


2.984


S15
Filter
Infinity
0.11
 1.5187
 64.1664
3.365202


S16

Infinity
0.67


3.39617


S17
Imaging
Infinity



3.709387



Plane

























TABLE 14






K
A
B
C
D
E
F
G
H
























S1
−3.5773
−0.0004
0.0047
−0.0224
0.0032
0.0133
−0.0108
0.0034
−0.0004


S2
−9.0551
−0.045
−0.0042
0.0097
0.0134
−0.0167
0.0059
−0.0008
0


S3
−2.3378
−0.0993
0.1427
−0.1434
0.1477
−0.0828
0.0112
0.0087
−0.003


S4
99.97
−0.0923
0.262
−0.5433
0.7929
−0.7771
0.4878
−0.1745
0.0264


S5
0
−0.1328
0.3622
−0.6631
0.8954
−0.85
0.5347
−0.1961
0.0311


S6
4.6392
−0.08
0.1668
−0.2414
0.2072
−0.0831
−0.0267
0.0433
−0.014


S7
0
−0.1064
0.1429
−0.4185
0.7951
−1.0313
0.8413
−0.3948
0.0819


S8
0
−0.1464
0.1697
−0.3068
0.3901
−0.3663
0.2325
−0.0889
0.0157


S9
−16.976
−0.0598
0.0066
0.0185
−0.0133
−0.0079
0.0105
−0.0041
0.0006


S10
−16.514
−0.0486
−0.0329
0.0697
−0.0576
0.0259
−0.0069
0.001
−7E−05


S11
0
0.0021
−0.0386
0.0152
−0.0049
0.0011
−3E−05
−2E−05
 2E−06


S12
−1.0939
0.1344
−0.1168
0.0671
−0.0277
0.0082
−0.0016
0.0002
−7E−06


S13
−6.2725
−0.1233
0.0218
0.0166
−0.0084
0.0018
−0.0002
1E−05
−3E−07


S14
−9.9341
−0.1059
0.0534
−0.0191
0.0046
−0.0008
8E−05
−4E−06
 1E−07









Eighth Example


FIG. 15 is a view illustrating an eighth example of an optical imaging system, and FIG. 16 illustrates aberration curves of the optical imaging system of FIG. 15.


The eighth example of the optical imaging system includes a first lens 810, a second lens 820, a third lens 830, a fourth lens 840, a fifth lens 850, a sixth lens 860, a seventh lens 870, a filter 880, an image sensor 890, and a stop (not shown) disposed between the first lens 810 and the second lens 820.


The first lens 810 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 820 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 830 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 840 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 850 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 860 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The seventh lens 870 has a negative refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 870. For example, the object-side surface of the seventh lens 870 is concave in the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 870. For example, the image-side surface of the seventh lens 870 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 15, the stop is disposed at a distance of 0.336 mm from the object-side surface of the first lens 810 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 8 listed in Table 55 that appears later in this application.


Table 15 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 15, and Table 16 below shows aspherical surface coefficients of the lenses of FIG. 15. Both surfaces of all of the lenses of FIG. 15 are aspherical.















TABLE 15











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
2.002076
0.290476
1.546
56.114
1.275


S2
Lens
1.735025
0.046207


1.265


S3
Second
1.510849
0.69189
1.546
56.114
1.234


S4
Lens
25.17448
0.050782


1.156


S5
Third
6.622812
0.20331
1.679
19.236
1.088


S6
Lens
2.690882
0.397038


0.970


S7
Fourth
404.2399
0.304853
1.646
23.528
1.031


S8
Lens
26.39909
0.238795


1.192


S9
Fifth
2.030671
0.231034
1.646
23.528
1.495


S10
Lens
2.049104
0.337714


1.721


S11
Sixth
9.000096
0.577572
1.546
56.114
1.996


S12
Lens
−1.67925
0.339723


2.084


S13
Seventh
−3.83664
0.33269
1.546
56.114
2.569


S14
Lens
1.71E+00
0.146102


2.784


S15
Filter
Infinity
0.11
1.5187
64.1664
3.104605


S16

Infinity
0.603297


3.133872


S17
Imaging
Infinity



3.409206



Plane

























TABLE 16






K
A
B
C
D
E
F
G
H
























S1
−3.5658
−0.0001
0.0048
−0.0338
0.0058
0.0258
−0.024
0.0087
−0.0012


S2
−8.9286
−0.0617
−0.0072
0.019
0.0308
−0.0458
0.0196
−0.0029
0


S3
−2.4366
−0.118
0.178
−0.2127
0.3039
−0.2613
0.1138
−0.0182
−0.0012


S4
100
−0.0932
0.2737
−0.6752
1.2227
−1.4655
1.1
−0.4621
0.0813


S5
0
−0.1401
0.3995
−0.8103
1.2941
−1.4787
1.1095
−0.4775
0.0877


S6
4.6754
−0.0913
0.2084
−0.3503
0.3957
−0.2854
0.067
0.0558
−0.0336


S7
0
−0.1191
0.1586
−0.5241
1.0591
−1.4826
1.3333
−0.7155
0.1765


S8
0
−0.2012
0.3026
−0.6033
0.8015
−0.7547
0.4799
−0.1903
0.0367


S9
−18.968
−0.0705
−0.017
0.0854
−0.095
0.0372
0.0031
−0.007
0.0016


S10
−15.615
−0.0761
−0.0114
0.0715
−0.083
0.0509
−0.0182
0.0035
−0.0003


S11
0
−0.0083
−0.0355
0.0253
−0.0245
0.0145
−0.0045
0.0007
−5E−05


S12
−1.1609
0.1552
−0.1513
0.1068
−0.0571
0.0215
−0.005
0.0006
−3E−05


S13
−4.7786
−0.1272
−0.0055
0.0492
−0.0232
0.0053
−0.0007
 4E−05
−1E−06


S14
−8.9618
−0.1184
0.0565
−0.0195
0.0048
−0.0009
1E−04
−6E−06
 2E−07









Ninth Example


FIG. 17 is a view illustrating a ninth example of an optical imaging system, and FIG. 18 illustrates aberration curves of the optical imaging system of FIG. 17.


The ninth example of the optical imaging system includes a first lens 910, a second lens 920, a third lens 930, a fourth lens 940, a fifth lens 950, a sixth lens 960, a seventh lens 970, a filter 980, an image sensor 990, and a stop (not shown) disposed between the first lens 910 and the second lens 920.


The first lens 910 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 920 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 930 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 940 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 950 has a negative refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The sixth lens 960 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The seventh lens 970 has a negative refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 970. For example, the object-side surface of the seventh lens 970 is concave in the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 970. For example, the image-side surface of the seventh lens 970 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 17, the stop is disposed at a distance of 0.731 mm from the object-side surface of the first lens 910 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 9 listed in Table 55 that appears later in this application.


Table 17 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 17, and Table 18 below shows aspherical surface coefficients of the lenses of FIG. 17. Both surfaces of all of the lenses of FIG. 17 are aspherical.















TABLE 17











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.732331
0.731243
1.546
56.114
1.250


S2
Lens
12.53699
0.070023


1.181


S3
Second
5.589296
0.2
1.667
20.353
1.147


S4
Lens
2.573966
0.39715


1.100


S5
Third
8.065523
0.384736
1.546
56.114
1.128


S6
Lens
7.836681
0.192591


1.247


S7
Fourth
6.687158
0.244226
1.546
56.114
1.276


S8
Lens
30.32847
0.271297


1.374


S9
Fifth
−3.28742
0.24968
1.667
20.353
1.481


S10
Lens
−4.51593
0.138845


1.734


S11
Sixth
5.679879
0.519865
1.546
56.114
2.150


S12
Lens
−1.89003
0.316634


2.318


S13
Seventh
−3.93255
0.3
1.546
56.114
2.640


S14
Lens
1.741826
0.193709


2.747


S15
Filter
Infinity
0.11
1.518
64.166
3.146


S16

Infinity
0.78


3.177045639


S17
Imaging
Infinity



3.536356437



Plane



























TABLE 18







K
A
B
C
D
E
F
G
H
J


























S1
−0.7464
0.01386
0.03443
−0.0749
0.10292
−0.0706
0.01727
0.00423
−0.0023
0


S2
36.6688
−0.0823
0.19496
−0.3067
0.36336
−0.323
0.19024
−0.0632
0.00855
0


S3
−1.3559
−0.1603
0.33047
−0.4059
0.33245
−0.1787
0.06728
−0.0166
0.00178
0


S4
−0.4109
−0.0907
0.14443
0.1155
−0.7969
1.50089
−1.4406
0.72187
−0.147
0


S5
0
−0.0739
0.04629
−0.1203
0.11651
−0.0578
−0.0089
0.02328
−0.0057
0


S6
0
−0.0932
0.00341
0.05212
−0.1827
0.24566
−0.2173
0.11261
−0.0241
0


S7
25.1476
−0.1235
−0.1887
0.37626
−0.554
0.67306
−0.5796
0.27819
−0.0538
0


S8
−99
−9E−05
−0.3274
0.35885
−0.3195
0.34506
−0.2608
0.09954
−0.0144
0


S9
−70.894
0.02055
0.04825
−0.5284
0.75832
−0.4915
0.16359
−0.0271
0.00175
0

















S10
2.28319
0.17594
−0.3448
0.22829
−0.0716
0.01095
−0.0007
−4E−06
1.4E−06 
0


S11
−99
0.11875
−0.2169
0.16747
−0.0871
0.02755
−0.0049
0.00045
−2E−05
0


S12
−3.3067
0.16436
−0.1849
0.1159
−0.049
0.01383
−0.0024
0.00023
−9E−06
0


S13
−2.4772
−0.1026
−0.0482
0.07401
−0.0308
0.00666
−0.0008
 5.5E−05
−2E−06
0

















S14
−1.1028
−0.2935
0.20325
−0.1127
0.04574
−0.0129
0.0024
−0.0003
1.8E−05 
−5E−07









Tenth Example


FIG. 19 is a view illustrating a tenth example of an optical imaging system, and FIG. 20 illustrates aberration curves of the optical imaging system of FIG. 19.


The tenth example of the optical imaging system includes a first lens 1010, a second lens 1020, a third lens 1030, a fourth lens 1040, a fifth lens 1050, a sixth lens 1060, a seventh lens 1070, a filter 1080, an image sensor 1090, and a stop (not shown) disposed between the first lens 1010 and the second lens 1020.


The first lens 1010 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 1020 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 1030 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 1040 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 1050 has a negative refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The sixth lens 1060 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The seventh lens 1070 has a negative refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 1070. For example, the object-side surface of the seventh lens 1070 is concave in the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 1070. For example, the image-side surface of the seventh lens 1070 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 19, the stop is disposed at a distance of 0.690 mm from the object-side surface of the first lens 1010 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 10 listed in Table 55 that appears later in this application.


Table 19 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 19, and Table 20 below shows aspherical surface coefficients of the lenses of FIG. 19. Both surfaces of all of the lenses of FIG. 19 are aspherical.















TABLE 19











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.782088
0.689797
1.546
56.114
1.275


S2
Lens
13.89149
0.079047


1.226


S3
Second
6.087772
0.2
1.667
20.353
1.192


S4
Lens
2.729115
0.404069


1.100


S5
Third
8.069534
0.351255
1.546
56.114
1.157


S6
Lens
7.933764
0.173398


1.256


S7
Fourth
6.770708
0.253752
1.546
56.114
1.280


S8
Lens
59.26755
0.221445


1.370


S9
Fifth
−3.04667
0.446166
1.667
20.353
1.423


S10
Lens
−4.61706
0.092345


1.742


S11
Sixth
5.54179
0.885686
1.546
56.114
2.150


S12
Lens
−1.81648
0.263902


2.247


S13
Seventh
−3.72821
0.334926
1.546
56.114
2.609


S14
Lens
1.795292
0.214212


2.895


S15
Filter
Infinity
0.11
1.518
64.166
3.128


S16

Infinity
0.78


3.159505988


S17
Imaging
Infinity



3.5352



Plane



























TABLE 20







K
A
B
C
D
E
F
G
H
J


























S1
−0.7799
0.01197
0.05018
−0.1139
0.15402
−0.1058
0.0277
0.00415
−0.0027
0


S2
47.9347
−0.0683
0.17293
−0.3083
0.40045
−0.3589
0.19954
−0.0605
0.0074
0


S3
1.68169
−0.1465
0.29389
−0.3639
0.28524
−0.0978
−0.0255
0.03457
−0.0087
0


S4
−0.5294
−0.0931
0.17548
−0.0689
−0.2817
0.70925
−0.7504
0.40105
−0.0855
0


S5
0
−0.0692
0.02762
−0.0586
0.02149
0.04226
−0.0786
0.05249
−0.0116
0


S6
0
−0.0923
0.00494
0.02984
−0.1124
0.16118
−0.1632
0.09263
−0.0206
0


S7
25.6946
−0.1416
−0.0429
−0.049
0.12511
0.02541
−0.2058
0.15568
−0.0361
0


S8
−99
0.00488
−0.296
0.32057
−0.3817
0.48577
−0.3607
0.13074
−0.0181
0


S9
−70.539
−0.0878
0.24262
−0.6812
0.81506
−0.4953
0.1593
−0.0257
0.00163
0


S10
1.48962
0.12295
−0.2057
0.12659
−0.0423
0.00892
−0.0013
0.00012
−5E−06
0


S11
−99
0.113
−0.1689
0.11533
−0.0542
0.01559
−0.0025
0.00021
−7E−06
0


S12
−2.8554
0.10708
−0.1088
0.05801
−0.0206
0.0049
−0.0007
5.7E−05
−2E−06
0


S13
−2.6312
−0.0807
−0.0543
0.06724
−0.0264
0.0055
−0.0007
4.3E−05
−1E−06
0


S14
−1.0845
−0.2364
0.13321
−0.0576
0.0184
−0.0041
0.00062
−6E−05 
3.2E−06 
−7E−08









Eleventh Example


FIG. 21 is a view illustrating an eleventh example of an optical imaging system, and FIG. 22 illustrates aberration curves of the optical imaging system of FIG. 21.


The eleventh example of the optical imaging system includes a first lens 1110, a second lens 1120, a third lens 1130, a fourth lens 1140, a fifth lens 1150, a sixth lens 1160, a seventh lens 1170, a filter 1180, an image sensor 1190, and a stop (not shown) disposed between the first lens 1110 and the second lens 1120.


The first lens 1110 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 1120 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 1130 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 1140 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 1150 has a negative refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The sixth lens 1160 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The seventh lens 1170 has a negative refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 1170. For example, the object-side surface of the seventh lens 1170 is concave in the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 1170. For example, the image-side surface of the seventh lens 1170 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 21, the stop is disposed at a distance of 0.726 mm from the object-side surface of the first lens 1110 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 11 listed in Table 55 that appears later in this application.


Table 21 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 21, and Table 22 below shows aspherical surface coefficients of the lenses of FIG. 21. Both surfaces of all of the lenses of FIG. 21 are aspherical.















TABLE 21











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.792301
0.726309
1.546
56.114
1.330


S2
Lens
13.20491
0.090736


1.287


S3
Second
5.976271
0.2
1.667
20.353
1.219


S4
Lens
2.717433
0.392614


1.100


S5
Third
7.924964
0.368939
1.546
56.114
1.160


S6
Lens
7.783378
0.135415


1.266


S7
Fourth
6.732611
0.266976
1.546
56.114
1.283


S8
Lens
34.21537
0.221138


1.379


S9
Fifth
−2.99938
0.446167
1.667
20.353
1.429


S10
Lens
−4.33966
0.050671


1.767


S11
Sixth
5.602517
0.919146
1.546
56.114
2.150


S12
Lens
−1.61634
0.250496


2.124


S13
Seventh
−3.32028
0.3
1.546
56.114
2.555


S14
Lens
1.721575
0.241394


2.854


S15
Filter
Infinity
0.11
1.518
64.166
3.042


S16

Infinity
0.78


3.076461274


S17
Imaging
Infinity



3.539791201



Plane



























TABLE 22







K
A
B
C
D
E
F
G
H
J


























S1
−0.8043
0.01289
0.03726
−0.0816
0.11409
−0.089
0.03652
−0.0062
−0.0001
0


S2
51.3479
−0.0483
0.05093
0.0719
−0.2927
0.39068
−0.2714
0.0975
−0.0144
0


S3
3.11156
−0.1249
0.178
−0.0145
−0.3397
0.56985
−0.443
0.17445
−0.0279
0


S4
−0.6552
−0.0793
0.09873
0.18501
−0.7911
1.31375
−1.1601
0.5393
−0.1015
0


S5
0
−0.066
0.06134
−0.18
0.24321
−0.2015
0.08626
−0.0114
−0.0009
0


S6
0
−0.0855
−0.0306
0.18152
−0.4356
0.54102
−0.4166
0.18221
−0.0336
0


S7
25.5599
−0.1157
−0.2609
0.66152
−1.0774
1.19203
−0.8541
0.34504
−0.0583
0


S8
−99
0.0276
−0.4662
0.78122
−1.0595
1.08297
−0.6699
0.21615
−0.0277
0


S9
−74.927
−0.0825
0.26638
−0.7895
0.98252
−0.6232
0.21113
−0.0363
 0.0025
0


S10
1.48962
0.15316
−0.249
0.16958
−0.0655
0.01574
−0.0024
0.00021
−8E−06
0


S11
−99
0.09288
−0.1748
0.13327
−0.0666
0.02003
−0.0034
0.00029
−1E−05
0


S12
−2.4857
0.11037
−0.1344
0.07896
−0.0304
0.00781
−0.0012
0.00011
−4E−06
0


S13
−2.6312
−0.0289
−0.1097
0.09541
−0.0347
0.00705
−0.0008
5.5E−05
−2E−06
0


S14
−1.0845
−0.2256
0.1217
−0.0516
0.01635
−0.0037
0.00055
−5E−05 
2.8E−06 
−7E−08









Twelfth Example


FIG. 23 is a view illustrating a twelfth example of an optical imaging system, and FIG. 24 illustrates aberration curves of the optical imaging system of FIG. 23.


The twelfth example of the optical imaging system includes a first lens 1210, a second lens 1220, a third lens 1230, a fourth lens 1240, a fifth lens 1250, a sixth lens 1260, a seventh lens 1270, a filter 1280, an image sensor 1290, and a stop (not shown) disposed between the second lens 1220 and the third lens 1230.


The first lens 1210 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 1220 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The third lens 1230 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 1240 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 1250 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 1260 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 1270 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


Two inflection points are formed on the object-side surface of the seventh lens 1270. For example, the object-side surface of the seventh lens 1270 is convex in the paraxial region, becomes concave in a region outside the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 1270. For example, the image-side surface of the seventh lens 1270 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 23, the stop is disposed at a distance of 1.158 mm from the object-side surface of the first lens 1210 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 12 listed in Table 55 that appears later in this application.


Table 23 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 23, and Table 24 below shows aspherical surface coefficients of the lenses of FIG. 23. Both surfaces of all of the lenses of FIG. 23 are aspherical.















TABLE 23











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
2.141
0.481
1.546
56.114
1.450


S2
Lens
3.251
0.110


1.350


S3
Second
3.253
0.542
1.546
56.114
1.285


S4
Lens
−15.773
0.025


1.232


S5
Third
8.425
0.230
1.679
19.236
1.157


S6
Lens
3.514
0.625


1.095


S7
Fourth
25.986
0.296
1.679
19.236
1.265


S8
Lens
15.894
0.230


1.452


S9
Fifth
3.048
0.400
1.546
56.114
1.675


S10
Lens
3.616
0.290


2.092


S11
Sixth
3.762
0.400
1.679
19.236
2.153


S12
Lens
2.792
0.204


2.476


S13
Seventh
1.614
0.510
1.537
53.955
2.938


S14
Lens
1.326
0.196


3.102


S15
Filter
Infinity
0.110
1.518
64.197
3.420


S16

Infinity
0.65


3.450


S17
Imaging
Infinity



3.730



Plane



























TABLE 24







K
A
B
C
D
E
F
G
H
J


























S1
−8.038
0.07067
−0.0797
0.03339
0.00722
−0.0491
0.04654
−0.0186
0.00318
−0.0002


S2
−20.594
−0.0019
−0.1494
0.20409
−0.2922
0.37549
−0.3085
0.14861
−0.0387
0.0042


S3
−0.0908
−0.0339
−0.0641
0.13679
−0.2821
0.49215
−0.4815
0.26054
−0.0746
0.00881


S4
−0.4822
−0.0436
0.17605
−0.3256
0.19989
0.1916
−0.4291
0.32034
−0.1141
0.01622


S5
−1.1841
−0.1073
0.25445
−0.4683
0.49912
−0.2863
0.05651
0.03245
−0.0229
0.00442


S6
0.87331
−0.0693
0.03569
0.20478
−0.8833
1.73278
−1.9742
1.34645
−0.5106
0.08302


S7
−0.4999
−0.0314
0.01347
−0.2894
0.97164
−1.7181
1.79234
−1.1152
0.38365
−0.0563


S8
−1E−06
−0.0273
−0.1177
0.21199
−0.2544
0.21565
−0.1264
0.04694
−0.0093
0.0007


S9
−41.843
0.16235
−0.3487
0.40163
−0.3105
0.13962
−0.027
−0.0038
0.00264
−0.0003


S10
−5.1424
0.03971
−0.1364
0.15688
−0.1229
0.06333
−0.0212
0.0044
−0.0005
2.6E−05 


S11
−2.1666
0.03558
−0.1809
0.19853
−0.1438
0.06411
−0.0173
0.00275
−0.0002
 9E−06


S12
−0.0207
−0.1043
0.02386
−0.0063
−0.0007
0.00066
−3E−06
−4E−05
7.3E−06
−4E−07


S13
−0.7948
−0.4128
0.18634
−0.0516
0.01005
−0.0015
0.00016
−1E−05
6.2E−07
−1E−08


S14
−1.3226
−0.3105
0.17125
−0.0712
0.02129
−0.0043
0.00058
−5E−05
2.3E−06
−5E−08









Thirteenth Example


FIG. 25 is a view illustrating a thirteenth example of an optical imaging system, and FIG. 26 illustrates aberration curves of the optical imaging system of FIG. 25.


The thirteenth example of the optical imaging system includes a first lens 1310, a second lens 1320, a third lens 1330, a fourth lens 1340, a fifth lens 1350, a sixth lens 1360, a seventh lens 1370, a filter 1380, an image sensor 1390, and a stop (not shown) disposed between the second lens 1320 and the third lens 1330.


The first lens 1310 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 1320 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The third lens 1330 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 1340 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 1350 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 1360 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 1370 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


Two inflection points are formed on the object-side surface of the seventh lens 1370. For example, the object-side surface of the seventh lens 1370 is convex in the paraxial region, becomes concave in a region outside the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 1370. For example, the image-side surface of the seventh lens 1370 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 25, the stop is disposed at a distance of 1.199 mm from the object-side surface of the first lens 1310 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 13 listed in Table 55 that appears later in this application.


Table 25 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 25, and Table 26 below shows aspherical surface coefficients of the lenses of FIG. 25. Both surfaces of all of the lenses of FIG. 25 are aspherical.















TABLE 25











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
2.073751483
0.544876
1.546
56.114
1.340


S2
Lens
3.134870736
0.137569


1.302


S3
Second
3.128441404
0.491088
1.546
56.114
1.257


S4
Lens
−25.66530563
0.025843


1.217


S5
Third
12.4369312
0.23
1.679
19.236
1.160


S6
Lens
3.763271555
0.507804


1.182


S7
Fourth
10.7268766
0.360036
1.546
56.114
1.275


S8
Lens
12.82165572
0.348743


1.388


S9
Fifth
4.81387139
0.35
1.546
56.114
1.576


S10
Lens
5.615039352
0.232774


2.010


S11
Sixth
4.324850125
0.438387
1.679
19.236
2.018


S12
Lens
3.02702576
0.173942


2.323


S13
Seventh
1.616003022
0.58366
1.546
56.114
2.710


S14
Lens
1.373602569
0.214276


2.996


S15
Filter
Infinity
0.21
1.518
64.197
3.338


S16

Infinity
0.649998


3.403


S17
Imaging
Infinity



3.729



Plane



























TABLE 26







K
A
B
C
D
E
F
G
H
J


























S1
−1
−0.0025
−0.0098
0.01527
−0.0556
0.09254
−0.0925
0.05356
−0.0163
0.00201


S2
−12.778
−0.0004
−0.1137
0.24524
−0.5515
0.82945
−0.7417
0.38903
−0.1114
0.01344


S3
−1.5504
−0.0322
−0.0682
0.18501
−0.5146
0.9207
−0.9127
0.51588
−0.1579
0.02023


S4
−7.0537
−0.0404
0.29676
−1.2693
2.88262
−3.9202
3.31284
−1.6974
0.47955
−0.0571


S5
13.4217
−0.1043
0.54877
−2.1153
4.90531
−7.1106
6.4814
−3.6045
1.11764
−0.1481


S6
0.76614
−0.0811
0.31536
−1.241
3.19858
−5.2874
5.51634
−3.5023
1.23595
−0.1856


S7
−8.3969
−0.0517
−0.0407
0.14681
−0.3147
0.35116
−0.1879
0.00842
0.03459
−0.0102


S8
6.05573
−0.0665
−0.0069
0.01518
−0.01
−0.044
0.09308
−0.0777
0.03087
−0.0047


S9
−43.417
0.02293
−0.0192
−0.0479
0.09183
−0.0953
0.05836
−0.0215
0.00436
−0.0004

















S10
−1.2708
0.04581
−0.1581
0.19889
−0.1589
0.08059
−0.0262
0.0053
−0.0006
 3E−05


S11
−16.611
0.11516
−0.2515
0.23819
−0.1502
0.06085
−0.0155
0.00238
−0.0002
7.4E−06 

















S12
0.08869
−0.0573
−0.0313
0.03451
−0.02
0.00672
−0.0013
0.00014
 −7E−06
7.4E−08 


S13
−0.815
−0.3784
0.16737
−0.0506
0.01278
−0.0027
0.00044
−5E−05
2.7E−06
−7E−08


S14
−1.3724
−0.2775
0.15305
−0.0638
0.01949
−0.0041
0.00058
−5E−05
2.6E−06
−6E−08









Fourteenth Example


FIG. 27 is a view illustrating a fourteenth example of an optical imaging system, and FIG. 28 illustrates aberration curves of the optical imaging system of FIG. 27.


The fourteenth example of the optical imaging system includes a first lens 1410, a second lens 1420, a third lens 1430, a fourth lens 1440, a fifth lens 1450, a sixth lens 1460, a seventh lens 1470, a filter 1480, an image sensor 1490, and a stop (not shown) disposed between the second lens 1420 and the third lens 1430.


The first lens 1410 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 1420 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 1430 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 1440 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 1450 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 1460 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 1470 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


Two inflection points are formed on the object-side surface of the seventh lens 1470. For example, the object-side surface of the seventh lens 1470 is convex in the paraxial region, becomes concave in a region outside the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 1470. For example, the image-side surface of the seventh lens 1470 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 27, the stop is disposed at a distance of 1.077 mm from the object-side surface of the first lens 1410 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 14 listed in Table 55 that appears later in this application.


Table 27 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 27, and Table 28 below shows aspherical surface coefficients of the lenses of FIG. 27. Both surfaces of all of the lenses of FIG. 27 are aspherical.















TABLE 27











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
2.118305139
0.467301
1.546
56.114
1.360


S2
Lens
2.746507151
0.088291


1.343


S3
Second
2.805315991
0.495083
1.546
56.114
1.313


S4
Lens
29.97218136
0.026058


1.266


S5
Third
5.620498788
0.273577
1.679
19.236
1.212


S6
Lens
2.858933317
0.365293


1.199


S7
Fourth
6.085110345
0.415715
1.546
56.114
1.285


S8
Lens
19.14383505
0.530007


1.350


S9
Fifth
5.783090879
0.4
1.679
19.236
1.600


S10
Lens
4.564410244
0.188701


2.100


S11
Sixth
2.807723971
0.444625
1.546
56.114
1.903


S12
Lens
3.20115397
0.276382


2.470


S13
Seventh
1.650083939
0.458527
1.546
56.114
2.646


S14
Lens
1.194405383
0.21044


2.806


S15
Filter
Infinity
0.21
1.518
64.197
3.241


S16

Infinity
0.649999


3.319


S17
Imaging
Infinity



3.729



Plane



























TABLE 28







K
A
B
C
D
E
F
G
H
J


























S1
−1
−0.0103
0.00782
−0.0588
0.09254
−0.0904
0.0486
−0.0119
0.00038
0.00021


S2
−13.05
0.02575
−0.1274
0.03504
0.06172
−0.0405
0.00034
0.0049
−0.0007
−0.0001


S3
−1.2154
−0.0166
−0.0602
−0.0171
0.06247
0.04814
−0.1007
0.05111
−0.0092
0.00015


S4
−7.0515
−0.047
0.26813
−0.8387
1.45463
−1.5426
1.02637
−0.4201
0.09736
−0.0099


S5
8.8287
−0.0982
0.31064
−0.8268
1.45377
−1.7174
1.3464
−0.6715
0.1944
−0.025


S6
1.72172
−0.0695
0.09394
−0.1196
0.14214
−0.2108
0.2773
−0.2257
0.09968
−0.0182


S7
−1.4309
−0.0448
−0.0056
0.02993
−0.0484
−0.0039
0.08562
−0.1013
0.05106
−0.0095


S8
5.85918
−0.0455
−0.0133
0.03368
−0.0729
0.09223
−0.0766
0.04111
−0.0128
0.00184


S9
−43.521
0.00081
−0.0239
0.02218
−0.0173
0.00514
−0.0002
−0.0003
5.4E−05
4.8E−06


S10
−11.855
−0.0163
−0.0578
0.08324
−0.067
0.0334
−0.0109
0.00227
−0.0003
1.4E−05


S11
−16.199
0.10244
−0.1959
0.19307
−0.1564
0.07971
−0.0243
0.00436
−0.0004
1.8E−05


S12
0.16678
−0.0913
0.11002
−0.1075
0.05366
−0.0157
0.00287
−0.0003
2.1E−05
 −6E−07


S13
−0.8022
−0.4375
0.2118
−0.049
0.00155
0.00209
−0.0006
7E−05
−4E−06 
1.1E−07


S14
−1.407
−0.3709
0.24995
−0.1268
0.04606
−0.0114
0.00184
−0.0002
1.1E−05
 −3E−07









Fifteenth Example


FIG. 29 is a view illustrating a fifteenth example of an optical imaging system, and FIG. 30 illustrates aberration curves of the optical imaging system of FIG. 29.


The fifteenth example of the optical imaging system includes a first lens 1510, a second lens 1520, a third lens 1530, a fourth lens 1540, a fifth lens 1550, a sixth lens 1560, a seventh lens 1570, a filter 1580, an image sensor 1590, and a stop (not shown) disposed between the second lens 1520 and the third lens 1530.


The first lens 1510 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 1520 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 1530 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 1540 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 1550 has a negative refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The sixth lens 1560 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 1570 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


Two inflection points are formed on the object-side surface of the seventh lens 1570. For example, the object-side surface of the seventh lens 1570 is convex in the paraxial region, becomes concave in a region outside the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 1570. For example, the image-side surface of the seventh lens 1570 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 29, the stop is disposed at a distance of 1.093 mm from the object-side surface of the first lens 1510 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 15 listed in Table 55 that appears later in this application.


Table 29 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 29, and Table 30 below shows aspherical surface coefficients of the lenses of FIG. 29. Both surfaces of all of the lenses of FIG. 29 are aspherical.















TABLE 29











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.942384
0.793197
1.5441
56.1138
1.444


S2
Lens
9.934274
0.1


1.402


S3
Second
4.267935
0.2
1.6612
20.3532
1.333


S4
Lens
2.440295
0.233353


1.244


S5
Third
3.840803
0.337213
1.5441
56.1138
1.192


S6
Lens
7.222946
0.29511


1.184


S7
Fourth
10.23439
0.319724
1.5441
56.1138
1.207


S8
Lens
26.51645
0.281354


1.283


S9
Fifth
−5.15487
0.401781
1.651
21.4942
1.301


S10
Lens
−9.64405
0.147362


1.573


S11
Sixth
3.891237
0.810422
1.5441
56.1138
1.674


S12
Lens
4.075702
0.213783


2.386


S13
Seventh
3.034895
0.604963
1.5348
55.7115
2.823


S14
Lens
1.86E+00
0.14844


3.015


S15
Filter
Infinity
0.104878
1.5182
64.1973
3.181842592


S16

Infinity
0.645122


3.2137538


S17
Imaging
Infinity



3.531597426



Plane


























TABLE 30







K
A
B
C
D
E
F
G
H

























S1
0.1119
−0.0077
0.0183
−0.0487
0.065
−0.0521
0.0239
−0.0059
0.0006


S2
−26.097
−0.0447
0.0639
−0.0885
0.0802
−0.0469
0.017
−0.0035
0.0003


S3
−57.375
−0.0493
0.0357
−0.0459
0.0544
−0.0363
0.0155
−0.0043
0.0006


S4
−8.3441
−0.0492
0.0929
−0.1764
0.2477
−0.2307
0.1429
−0.0507
0.0075


S5
1.5878
−0.035
0.0435
−0.1062
0.1611
−0.1672
0.1224
−0.0475
0.0073


S6
−0.0241
−0.0418
−0.0007
0.0745
−0.1984
0.2528
−0.1625
0.0529
−0.0057


S7
−66.305
−0.0937
0.0545
−0.2
0.3691
−0.4471
0.3394
−0.1416
0.0248


S8
19.549
−0.0871
0.0483
−0.1552
0.2353
−0.2493
0.1709
−0.0651
0.0103


S9
7.2773
−0.0493
0.0331
−0.0549
0.0336
−0.0223
0.0129
−0.0036
0


S10
28.608
−0.1159
0.0778
−0.0525
0.0237
−0.0054
0.0001
0.0002
0


S11
−51.379
−0.0153
−0.0854
0.093
−0.0763
0.0386
−0.011
0.0013
0


S12
−31.504
−0.0086
0.0015
−0.0075
0.0041
−0.0012
0.0002
−1E−05
0


S13
−0.4733
−0.2404
0.1187
−0.0378
0.0079
−0.0011
8E−05
−4E−06
7E−08


S14
−0.7879
−0.2013
0.0915
−0.0345
0.009
−0.0015
0.0001
−7E−06
2E−07









Sixteenth Example


FIG. 31 is a view illustrating a sixteenth example of an optical imaging system, and FIG. 32 illustrates aberration curves of the optical imaging system of FIG. 31.


The sixteenth example of the optical imaging system includes a first lens 1610, a second lens 1620, a third lens 1630, a fourth lens 1640, a fifth lens 1650, a sixth lens 1660, a seventh lens 1670, a filter 1680, an image sensor 1690, and a stop (not shown) disposed between the second lens 1620 and the third lens 1630.


The first lens 1610 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 1620 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 1630 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 1640 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 1650 has a negative refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The sixth lens 1660 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 1670 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


Two inflection points are formed on the object-side surface of the seventh lens 1670. For example, the object-side surface of the seventh lens 1670 is convex in the paraxial region, becomes concave in a region outside the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 1670. For example, the image-side surface of the seventh lens 1670 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 31, the stop is disposed at a distance of 0.919 mm from the object-side surface of the first lens 1610 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 16 listed in Table 55 that appears later in this application.


Table 31 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 31, and Table 32 below shows aspherical surface coefficients of the lenses of FIG. 31. Both surfaces of all of the lenses of FIG. 31 are aspherical.















TABLE 31











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.739587
0.598921
1.5441
56.1138
1.100


S2
Lens
11.74576
0.1


1.087


S3
Second
4.594781
0.22
1.6612
20.3532
1.063


S4
Lens
2.200821
0.196896


1.082


S5
Third
3.001538
0.333024
1.5441
56.1138
1.036


S6
Lens
4.949957
0.220769


1.050


S7
Fourth
12.04233
0.308386
1.5441
56.1138
1.051


S8
Lens
17.11235
0.265994


1.143


S9
Fifth
−7.00397
0.297417
1.5441
56.1138
1.199


S10
Lens
−7.82081
0.110621


1.343


S11
Sixth
2.821263
0.520889
1.5441
56.1138
1.400


S12
Lens
3.003035
0.211839


2.055


S13
Seventh
2.369754
0.578763
1.5348
55.7115
2.394


S14
Lens
1.48E+00
0.136479


2.614


S15
Filter
Infinity
0.21
1.5182
64.1973
2.875305214


S16

Infinity
0.59


2.94119348


S17
Imaging
Infinity



3.261482111



Plane


























TABLE 32







K
A
B
C
D
E
F
G
H

























S1
0.1283
−0.0055
0.0045
−0.018
0.0078
0.0301
−0.063
0.046
−0.013


S2
−30.976
−0.0561
0.0444
0.0388
−0.2372
0.4368
−0.4385
0.2311
−0.0505


S3
−55.147
−0.0853
0.0161
0.2247
−0.6095
0.9607
−0.9142
0.4783
−0.1042


S4
−6.2418
−0.0492
0.0165
0.1209
−0.3038
0.4429
−0.3247
0.1012
0.0018


S5
1.4715
−0.0198
0.0181
−0.2874
0.8872
−1.6138
1.7719
−1.012
0.234


S6
−2.9758
−0.0369
0.0559
−0.2665
0.6033
−0.9754
0.967
−0.4745
0.0967


S7
−55.862
−0.1542
0.1102
−0.4806
1.1073
−1.6589
1.3653
−0.5002
0.0586


S8
−87.891
−0.144
0.1419
−0.5705
1.2436
−1.7221
1.4048
−0.6059
0.1078


S9
5.6449
−0.0669
0.1168
−0.4406
0.758
−0.7688
0.403
−0.0844
0


S10
28.194
−0.1694
0.0795
−0.1626
0.3248
−0.3223
0.1516
−0.0266
0


S11
−29.003
0.0237
−0.2637
0.2396
−0.1608
0.0735
−0.0259
0.0049
0


S12
−43.551
0.0645
−0.1366
0.0918
−0.0389
0.0101
−0.0014
 8E−05
0


S13
−0.6727
−0.4248
0.2545
−0.086
0.0183
−0.0024
0.0002
−9E−06
2E−07


S14
−0.8377
−0.3391
0.2016
−0.0975
0.0328
−0.0071
0.0009
−6E−05
2E−06









Seventeenth Example


FIG. 33 is a view illustrating a seventeenth example of an optical imaging system, and FIG. 34 illustrates aberration curves of the optical imaging system of FIG. 33.


The sixteenth example of the optical imaging system includes a first lens 1710, a second lens 1720, a third lens 1730, a fourth lens 1740, a fifth lens 1750, a sixth lens 1760, a seventh lens 1770, a filter 1780, an image sensor 1790, and a stop (not shown) disposed in front of the first lens 1710.


The first lens 1710 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 1720 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 1730 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 1740 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 1750 has a negative refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The sixth lens 1760 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 1770 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 1770. For example, the object-side surface of the seventh lens 1770 is convex in the paraxial region, and becomes concave toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 1770. For example, the image-side surface of the seventh lens 1770 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 33, the stop is disposed at a distance of 0.250 mm from the object-side surface of the first lens 1710 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 17 listed in Table 55 that appears later in this application.


Table 33 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 33, and Table 34 below shows aspherical surface coefficients of the lenses of FIG. 33. Both surfaces of all of the lenses of FIG. 33 are aspherical.















TABLE 33











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.721083
0.634874
1.5441
56.1138
1.100


S2
Lens
11.45706
0.121172


1.071


S3
Second
119.1721
0.203286
1.6612
20.3532
1.057


S4
Lens
4.475787
0.084345


1.043


S5
Third
4.525763
0.310946
1.5441
56.1138
1.051


S6
Lens
20.60825
0.215768


1.015


S7
Fourth
13.21519
0.236935
1.5441
56.1138
1.019


S8
Lens
16.27332
0.210349


1.070


S9
Fifth
−6.57315
0.41188
1.651
21.4942
1.076


S10
Lens
−10.4553
0.371031


1.320


S11
Sixth
3.477886
0.631775
1.5441
56.1138
1.556


S12
Lens
3.199354
0.267164


2.337


S13
Seventh
2.880384
0.505977
1.5441
56.1138
2.489


S14
Lens
1.71E+00
0.138438


2.666


S15
Filter
Infinity
0.21
1.5182
64.1973
3.102058013


S16

Infinity
0.59


3.177033741


S17
Imaging
Infinity



3.529142415



Plane






























TABLE 34






K
A
B
C
D
E
F
G
H
























S1
0.0432
−0.0088
0.0131
−0.0627
0.1199
−0.1345
0.077
−0.018
−0.0004


S2
−26.097
−0.0562
0.051
−0.0514
0.0595
−0.0683
0.0462
−0.0139
−7E−05 


S3
−99
−0.1283
0.1953
−0.2779
0.5135
−0.8812
0.9662
−0.5723
0.1395


S4
−16.567
−0.0971
0.1552
−0.3608
0.985
−2.059
2.5647
−1.6683
0.4378


S5
−1.6774
−0.0377
0.065
−0.4515
1.687
−3.5163
4.2391
−2.6607
0.6752


S6
57.913
−0.0559
0.0533
−0.341
1.3373
−2.8539
3.4811
−2.2114
0.5781


S7
−66.305
−0.1749
−0.0635
0.0963
−0.2061
0.5819
−0.9
0.6874
−0.1979


S8
19.549
−0.1228
−0.0686
0.0207
0.1647
−0.2695
0.1725
−0.0616
0.0161


S9
29.709
−0.0709
0.0826
−0.3062
0.6009
−0.6459
0.3344
−0.0761
0


S10
−31.338
−0.1255
0.1076
−0.1494
0.1908
−0.1423
0.0506
−0.0065
0


S11
−46.453
0.0038
−0.1455
0.1534
−0.126
0.0705
−0.0225
0.0029
0


S12
−31.504
0.0093
−0.0326
0.0149
−0.0033
0.0003
−1E−05
−7E−07
0


S13
−0.5233
−0.2947
0.1709
−0.0627
0.0154
−0.0025
0.0003
−1E−05
3E−07


S14
−0.8257
−0.2584
0.1353
−0.0565
0.0166
−0.0032
0.0004
−3E−05
7E−07









Eighteenth Example


FIG. 35 is a view illustrating an eighteenth example of an optical imaging system, and FIG. 36 illustrates aberration curves of the optical imaging system of FIG. 35.


The eighteenth example of the optical imaging system includes a first lens 1810, a second lens 1820, a third lens 1830, a fourth lens 1840, a fifth lens 1850, a sixth lens 1860, a seventh lens 1870, a filter 1880, an image sensor 1890, and a stop (not shown) disposed between the first lens 1810 and the second lens 1820.


The first lens 1810 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 1820 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 1830 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 1840 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 1850 has a positive refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The sixth lens 1860 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The seventh lens 1870 has a negative refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 1870. For example, the object-side surface of the seventh lens 1870 is concave in the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 1870. For example, the image-side surface of the seventh lens 1870 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 35, the stop is disposed at a distance of 0.768 mm from the object-side surface of the first lens 1810 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 18 listed in Table 55 that appears later in this application.


Table 35 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 35, and Table 36 below shows aspherical surface coefficients of the lenses of FIG. 35. Both surfaces of all of the lenses of FIG. 35 are aspherical.















TABLE 35











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.954768
0.767754
1.5441
56.1138
1.300


S2
Lens
7.885948
0.100479


1.209


S3
Second
4.828842
0.23659
1.6612
20.3532
1.213


S4
Lens
2.866155
0.449288


1.265


S5
Third
8.865496
0.484453
1.5441
56.1138
1.268


S6
Lens
16.67462
0.275209


1.403


S7
Fourth
10.67145
0.369792
1.5441
56.1138
1.456


S8
Lens
22.44715
0.280107


1.642


S9
Fifth
−4.38165
0.271148
1.6612
20.3532
1.769


S10
Lens
−4.38283
0.104957


2.019


S11
Sixth
7.952227
0.567669
1.5441
56.1138
2.357


S12
Lens
−3.03675
0.464825


2.647


S13
Seventh
−7.50793
0.32
1.5441
56.1138
3.123


S14
Lens
1.80E+00
0.189124


3.381


S15
Filter
Infinity
0.11
1.5183
64.1664
3.605133315


S16

Infinity
0.658604


3.63479604


S17
Imaging
Infinity



3.930447751



Plane


























TABLE 36






K
A
B
C
D
E
F
G
H
J

























S1
−0.8127
0.0142
0.0092
−0.0157
0.0206
−0.0137
0.0037
0.0003
−0.0003
0


S2
5.6538
−0.0472
0.0448
−0.0321
0.0158
−0.0059
0.001
0.0004
−0.0002
0


S3
−10.668
−0.0824
0.0792
−0.0266
−0.0158
0.0274
−0.0153
0.0039
−0.0004
0


S4
−0.1737
−0.0508
0.0303
0.1129
−0.3063
0.4131
−0.3101
0.1243
−0.0205
0


S5
0
−0.0377
0.0156
−0.0597
0.0773
−0.0624
0.0268
−0.0045
3E−05
0


S6
0
−0.0706
0.0482
−0.0575
−0.0009
0.0419
−0.0392
0.0166
−0.0028
0


S7
46.114
−0.1374
0.0451
0.0051
−0.0298
0.0052
0.0076
−0.0027
0.0001
0


S8
99
−0.1096
−0.0451
0.1394
−0.1519
0.0948
−0.0333
0.006
−0.0004
0


S9
−99
−0.0865
0.1152
−0.1605
0.1182
−0.0466
0.0099
−0.0011
5E−05
0


S10
−0.2245
0.0593
−0.0542
0.0004
0.0119
−0.0044
0.0007
−5E−05 
1E−06
0


S11
−99
0.1031
−0.1094
0.0579
−0.0216
0.005
−0.0007
4E−05
−1E−06 
0


S12
−4.7232
0.1521
−0.1221
0.0592
−0.0202
0.0046
−0.0007
5E−05
−2E−06 
0


S13
−1.1986
−0.0323
−0.0724
0.0507
−0.0141
0.0021
−0.0002
8E−06
−2E−07 
0


S14
−1.2644
−0.1675
0.0662
−0.0204
0.0047
−0.0007
8E−05
−5E−06 
2E−07
−2E−09









Nineteenth Example


FIG. 37 is a view illustrating a nineteenth example of an optical imaging system, and FIG. 38 illustrates aberration curves of the optical imaging system of FIG. 37.


The nineteenth example of the optical imaging system includes a first lens 1910, a second lens 1920, a third lens 1930, a fourth lens 1940, a fifth lens 1950, a sixth lens 1960, a seventh lens 1970, a filter 1980, an image sensor 1990, and a stop (not shown) disposed between the first lens 1910 and the second lens 1920.


The first lens 1910 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 1920 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 1930 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 1940 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The fifth lens 1950 has a negative refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The sixth lens 1960 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The seventh lens 1970 has a negative refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 1970. For example, the object-side surface of the seventh lens 1970 is concave in the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 1970. For example, the image-side surface of the seventh lens 1970 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 37, the stop is disposed at a distance of 0.624 mm from the object-side surface of the first lens 1910 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 19 listed in Table 55 that appears later in this application.


Table 37 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 37, and Table 38 below shows aspherical surface coefficients of the lenses of FIG. 37. Both surfaces of all of the lenses of FIG. 37 are aspherical.















TABLE 37











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.777275
0.623828
1.5441
56.1138
1.217


S2
Lens
6.456568
0.1


1.158


S3
Second
4.41033
0.236253
1.6612
20.3532
1.157


S4
Lens
2.658351
0.413785


1.184


S5
Third
6.587882
0.464049
1.5441
56.1138
1.177


S6
Lens
10.52328
0.17773


1.282


S7
Fourth
13.47488
0.362661
1.5441
56.1138
1.306


S8
Lens
−20.23
0.232536


1.444


S9
Fifth
−3.18309
0.2
1.6612
20.3532
1.456


S10
Lens
−4.21505
0.1


1.625


S11
Sixth
6.764633
0.608917
1.5441
56.1138
2.207


S12
Lens
−2.87919
0.421093


2.145


S13
Seventh
−6.99582
0.32
1.5441
56.1138
2.280


S14
Lens
1.69E+00
0.14847


3.165


S15
Filter
Infinity
0.11
1.5183
64.1664
2.850141022


S16

Infinity
0.680678


2.888122651


S17
Imaging
Infinity



3.276451571



Plane


























TABLE 38






K
A
B
C
D
E
F
G
H
J

























S1
−0.5383
0.0108
0.0209
−0.0477
0.0729
−0.06
0.0243
−0.0027
−0.0007
0


S2
5.8135
−0.0459
0.0189
0.0248
−0.0559
0.0486
−0.026
0.0094
−0.0019
0


S3
−10.011
−0.085
0.066
0.02
−0.0808
0.0756
−0.0332
0.0069
−0.0006
0


S4
−0.1875
−0.0544
0.0068
0.26
−0.6655
0.9329
−0.7519
0.3313
−0.061
0


S5
0
−0.0569
0.0063
−0.0275
−0.0046
0.0401
−0.0485
0.0264
−0.0053
0


S6
0
−0.0775
−0.0976
0.271
−0.5329
0.5567
−0.3323
0.1128
−0.0176
0


S7
47.015
−0.0863
−0.1024
0.2298
−0.2721
0.1091
0.0392
−0.0378
0.0065
0


S8
−99
−0.0603
−0.0348
0.057
−0.0468
0.0241
−0.007
0.001
−6E−05
0


S9
−99
−0.2672
0.6153
−0.9745
0.9138
−0.5236
0.1786
−0.0332
0.0026
0


S10
−0.0701
0.0268
−0.0377
−0.0253
0.035
−0.0133
0.0024
−0.0002
 7E−06
0


S11
−97.721
0.1556
−0.2109
0.1424
−0.0678
0.02
−0.0033
0.0003
−1E−05
0


S12
−1.5998
0.2298
−0.1811
0.0905
−0.0342
0.0088
−0.0014
0.0001
−4E−06
0


S13
4.8341
−0.1142
−0.0024
0.0306
−0.013
0.0027
−0.0003
2E−05
−5E−07
0


S14
−1.0993
−0.2618
0.1449
−0.0599
0.0171
−0.0032
0.0004
−3E−05 
 1E−06
−2E−08









Twentieth Example


FIG. 39 is a view illustrating a twentieth example of an optical imaging system, and FIG. 40 illustrates aberration curves of the optical imaging system of FIG. 39.


The twentieth example of the optical imaging system includes a first lens 2010, a second lens 2020, a third lens 2030, a fourth lens 2040, a fifth lens 2050, a sixth lens 2060, a seventh lens 2070, a filter 2080, an image sensor 2090, and a stop (not shown) disposed between the first lens 2010 and the second lens 2020.


The first lens 2010 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 2020 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 2030 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 2040 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 2050 has a positive refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The sixth lens 2060 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The seventh lens 2070 has a negative refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is concave.


No inflection point is formed on the object-side surface of the seventh lens 2070.


In addition, one inflection point is formed on the image-side surface of the seventh lens 2070. For example, the image-side surface of the seventh lens 2070 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 39, the stop is disposed at a distance of 0.641 mm from the object-side surface of the first lens 2010 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 20 listed in Table 55 that appears later in this application.


Table 39 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 39, and Table 40 below shows aspherical surface coefficients of the lenses of FIG. 39. Both surfaces of all of the lenses of FIG. 39 are aspherical.















TABLE 39











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.797739
0.640884
1.5441
56.1138
1.270


S2
Lens
3.742203
0.119077


1.211


S3
Second
3.057321
0.22
1.6612
20.3532
1.190


S4
Lens
2.795092
0.393079


1.130


S5
Third
10.62153
0.464034
1.5441
56.1138
1.153


S6
Lens
9.026562
0.1


1.289


S7
Fourth
7.987624
0.36214
1.5441
56.1138
1.328


S8
Lens
138.7678
0.233384


1.454


S9
Fifth
−4.1765
0.219829
1.6612
20.3532
1.518


S10
Lens
−4.13945
0.1


1.656


S11
Sixth
4.613403
0.608917
1.5441
56.1138
2.000


S12
Lens
−3.59211
0.472598


2.038


S13
Seventh
−7.00157
0.32
1.5441
56.1138
2.049


S14
Lens
1.69E+00
0.110689


2.685


S15
Filter
Infinity
0.21
1.5183
64.1664
2.941536401


S16

Infinity
0.549988


3.008025404


S17
Imaging
Infinity



3.291609937



Plane


























TABLE 40






K
A
B
C
D
E
F
G
H
J

























S1
−0.812
0.0136
0.0311
−0.0769
0.1226
−0.1099
0.0531
−0.0116
0.0005
0


S2
−6.6917
−0.0631
0.0174
0.0714
−0.1648
0.1763
−0.1086
0.0376
−0.0059
0


S3
−14.579
−0.0707
0.0068
0.1319
−0.2129
0.173
−0.0715
0.0127
−0.0005
0


S4
−0.188
−0.0614
−0.0138
0.3338
−0.7392
0.9251
−0.6781
0.276
−0.0477
0


S5
0
−0.0572
0.0435
−0.1733
0.2724
−0.2421
0.0931
−0.0042
−0.0038
0


S6
0
−0.1356
−0.0309
0.2183
−0.5547
0.6931
−0.486
0.1856
−0.0304
0


S7
30.023
−0.2107
0.0007
0.1568
−0.2854
0.2586
−0.1154
0.0236
−0.0019
0


S8
−99
−0.1858
−0.0192
0.2616
−0.4111
0.3392
−0.1538
0.0357
−0.0033
0


S9
−98.995
−0.2935
0.5043
−0.5157
0.2657
−0.0658
0.0056
0.0005
−8E−05
0


S10
−0.0701
−0.0775
0.2223
−0.2703
0.1529
−0.0452
0.0073
−0.0006
 2E−05
0


S11
−97.878
0.1479
−0.1956
0.1288
−0.0598
0.0172
−0.0028
0.0002
−8E−06
0


S12
1.4166
0.1234
−0.1416
0.087
−0.0341
0.0088
−0.0014
0.0001
−4E−06
0


S13
9.5503
−0.2864
0.1096
0.0149
−0.0214
0.0064
−0.0009
 6E−05
−2E−06
0


S14
−1.2786
−0.3076
0.1777
−0.0626
0.0143
−0.0022
0.0002
−1E−05
 5E−07
−7E−09









Twenty-First Example


FIG. 41 is a view illustrating a twenty-first example of an optical imaging system, and FIG. 42 illustrates aberration curves of the optical imaging system of FIG. 41.


The twenty-first example of the optical imaging system includes a first lens 2110, a second lens 2120, a third lens 2130, a fourth lens 2140, a fifth lens 2150, a sixth lens 2160, a seventh lens 2170, a filter 2180, an image sensor 2190, and a stop (not shown) disposed between the second lens 2120 and the third lens 2130.


The first lens 2110 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 2120 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 2130 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 2140 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The fifth lens 2150 has a negative refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The sixth lens 2160 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 2170 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 2170. For example, the object-side surface of the seventh lens 2170 is convex in the paraxial region, and becomes concave toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 2170. For example, the image-side surface of the seventh lens 2170 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 41, the stop is disposed at a distance of 1.070 mm from the object-side surface of the first lens 2110 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 21 listed in Table 55 that appears later in this application.


Table 41 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 41, and Table 42 below shows aspherical surface coefficients of the lenses of FIG. 41. Both surfaces of all of the lenses of FIG. 41 are aspherical.















TABLE 41











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.601328
0.4703
1.55
56.11
1.10


S2
Lens
6.723341
0.02


1.07


S3
Second
1.565428
0.18945
1.66
20.40
1.00


S4
Lens
1.191167
0.385927


0.91


S5
Third
3.880104
0.1
1.66
20.40
0.90


S6
Lens
3.812373
0.220903


0.93


S7
Fourth
8.909025
0.639932
1.55
56.11
1.10


S8
Lens
−75.7282
0.331313


1.28


S9
Fifth
−12.2751
0.14904
1.65
21.49
1.33


S10
Lens
−15.1629
0.079448


1.57


S11
Sixth
4.140002
0.553938
1.65
21.49
1.60


S12
Lens
3.897447
0.243033


2.00


S13
Seventh
1.919931
0.511414
1.54
55.71
2.82


S14
Lens
1.453313
0.182833


2.58


S15
Filter
Infinity
0.11
1.52
64.20
2.89


S16

Infinity
0.532581


2.93


S17
Imaging
Infinity



3.26



Plane


























TABLE 42






K
A
B
C
D
E
F
G
H
J

























S1
−0.1212
0.0104
0.0128
−0.0281
0.0435
−0.0381
0.0173
−0.0033
0
0


S2
29.637
−0.0905
0.3333
−0.7525
0.9665
−0.741
0.3153
−0.0585
0
0


S3
−2.48
−0.117
0.4074
−0.8715
1.1061
−0.8249
0.3423
−0.062
0
0


S4
−0.6581
−0.0925
0.1463
−0.1165
−0.011
0.2266
−0.2114
0.0722
0
0


S5
3.0804
−0.1259
0.1776
−0.2375
0.4049
−0.4425
0.2969
−0.0837
0
0


S6
10.659
−0.1644
0.1692
−0.1502
0.1444
−0.0762
0.0151
−0.0003
0
0


S7
21.918
−0.0617
0.0459
−0.0379
0.0564
−0.0364
0.0097
−0.0009
0
0


S8
25.736
−0.0713
0.0217
−0.0106
0.0072
−0.0023
0.0003
−2E−05
0
0


S9
1.6857
−0.1436
0.2565
−0.4332
0.4184
−0.2461
0.0826
−0.0124
0
0


S10
75.072
−0.1186
0.1217
−0.1545
0.1026
−0.0332
0.005
−0.0003
0
0


S11
−52.836
0.0701
−0.2199
0.2058
−0.1343
0.0526
−0.0106
0.0009
0
0


S12
0
−0.0521
−0.0332
0.0285
−0.0129
0.0028
3E−06
−0.0001
2E−05
−5E−07


S13
−0.9427
−0.3217
0.0977
−0.0029
−0.0058
0.0017
−0.0002
 2E−05
−4E−07 
0


S14
−1.0048
−0.2798
0.1282
−0.0461
0.0122
−0.0022
0.0002
−1E−05
4E−07
0









Twenty-Second Example


FIG. 43 is a view illustrating a twenty-second example of an optical imaging system, and FIG. 44 illustrates aberration curves of the optical imaging system of FIG. 43.


The twenty-second example of the optical imaging system includes a first lens 2210, a second lens 2220, a third lens 2230, a fourth lens 2240, a fifth lens 2250, a sixth lens 2260, a seventh lens 2270, a filter 2280, an image sensor 2290, and a stop (not shown) disposed between the second lens 2220 and the third lens 2230.


The first lens 2210 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 2220 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 2230 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 2240 has a positive refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is convex.


The fifth lens 2250 has a negative refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The sixth lens 2260 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 2270 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 2270. For example, the object-side surface of the seventh lens 2270 is convex in the paraxial region, and becomes concave toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 2270. For example, the image-side surface of the seventh lens 2270 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 43, the stop is disposed at a distance of 1.050 mm from the object-side surface of the first lens 2210 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 22 listed in Table 55 that appears later in this application.


Table 43 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 43, and Table 44 below shows aspherical surface coefficients of the lenses of FIG. 43. Both surfaces of all of the lenses of FIG. 43 are aspherical.















TABLE 43











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.618399
0.481078
1.55
56.11
1.11


S2
Lens
6.899203
0.02


1.08


S3
Second
1.572709
0.21298
1.66
20.40
1.01


S4
Lens
1.198393
0.337014


0.91


S5
Third
3.880395
0.1
1.66
20.40
0.90


S6
Lens
3.81266
0.18744


0.93


S7
Fourth
9.071729
0.55292
1.55
56.11
1.08


S8
Lens
−55.0996
0.304351


1.24


S9
Fifth
−12.1837
0.114265
1.65
21.49
1.30


S10
Lens
−15.0249
0.060547


1.57


S11
Sixth
4.118358
0.587621
1.65
21.49
1.52


S12
Lens
3.854992
0.224328


1.90


S13
Seventh
1.919931
0.553429
1.54
55.71
2.82


S14
Lens
1.453313
0.181552


2.49


S15
Filter
Infinity
0.11
1.52
64.20
2.83


S16

Infinity
0.533801


2.87


S17
Imaging
Infinity



3.27



Plane

























TABLE 44






K
A
B
C
D
E
F
G
H
























S1
−0.2038
0.0111
0.0146
−0.0331
0.0534
−0.0486
0.023
−0.0046
0


S2
30.534
−0.0868
0.313
−0.693
0.872
−0.655
0.273
−0.0496
0


S3
−2.347
−0.114
0.3865
−0.8113
1.0115
−0.741
0.3021
−0.0538
0


S4
−0.7241
−0.0836
0.1372
−0.1055
−0.0097
0.1953
−0.1778
0.0592
0


S5
3.0804
−0.1259
0.1776
−0.2375
0.4049
−0.4425
0.2969
−0.0837
0


S6
10.659
−0.1644
0.1692
−0.1502
0.1444
−0.0762
0.0151
−0.0003
0


S7
21.918
−0.0617
0.0459
−0.0379
0.0564
−0.0364
0.0097
−0.0009
0


S8
25.736
−0.0713
0.0217
−0.0106
0.0072
−0.0023
0.0003
−2E−05
0


S9
1.6857
−0.1436
0.2565
−0.4332
0.4184
−0.2461
0.0826
−0.0124
0


S10
75.072
−0.1186
0.1217
−0.1545
0.1026
−0.0332
0.005
−0.0003
0


S11
−52.836
0.0701
−0.2199
0.2058
−0.1343
0.0526
−0.0106
0.0009
0


S12
−34.09
0.0153
−0.0851
0.0637
−0.0302
0.0086
−0.0013
 8E−05
0


S13
−0.9427
−0.3217
0.0977
−0.0029
−0.0058
0.0017
−0.0002
 2E−05
−4E−07


S14
−1.0048
−0.2798
0.1282
−0.0461
0.0122
−0.0022
0.0002
−1E−05
 4E−07









Twenty-Third Example


FIG. 45 is a view illustrating a twenty-third example of an optical imaging system, and FIG. 46 illustrates aberration curves of the optical imaging system of FIG. 45.


The twenty-second example of the optical imaging system includes a first lens 2310, a second lens 2320, a third lens 2330, a fourth lens 2340, a fifth lens 2350, a sixth lens 2360, a seventh lens 2370, a filter 2380, an image sensor 2390, and a stop (not shown) disposed between the second lens 2320 and the third lens 2330.


The first lens 2310 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 2320 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 2330 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 2340 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 2350 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 2360 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 2370 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


Two inflection points are formed on the object-side surface of the seventh lens 2370. For example, the object-side surface of the seventh lens 2370 is convex in the paraxial region, becomes concave in a region outside the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 2370. For example, the image-side surface of the seventh lens 2370 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 45, the stop is disposed at a distance of 1.082 mm from the object-side surface of the first lens 2310 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 23 listed in Table 55 that appears later in this application.


Table 45 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 45, and Table 46 below shows aspherical surface coefficients of the lenses of FIG. 45. Both surfaces of all of the lenses of FIG. 45 are aspherical.















TABLE 45











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
2.33687036
0.432116
1.546
56.114
1.365


S2
Lens
2.85742179
0.025


1.352


S3
Second
2.542185152
0.6
1.546
56.114
1.326


S4
Lens
36.41699638
0.025


1.254


S5
Third
8.193690072
0.23
1.679
19.236
1.217


S6
Lens
3.333584263
0.3221813


1.227


S7
Fourth
6.342713056
0.57111
1.546
56.114
1.322


S8
Lens
11.23703124
0.4048969


1.372


S9
Fifth
18.96145717
0.5066546
1.546
56.114
1.590


S10
Lens
6.683687757
0.0731741


1.931


S11
Sixth
2.354768418
0.6194256
1.546
56.114
2.023


S12
Lens
2.565132372
0.1492156


2.456


S13
Seventh
1.424653122
0.5400405
1.546
56.114
2.710


S14
Lens
1.282185763
0.3444098


2.982


S15
Filter
Infinity
0.21
1.518
64.197
3.258


S16

Infinity
0.6497077


3.333867296


S17
Imaging
Infinity



3.734065733



Plane


























TABLE 46






K
A
B
C
D
E
F
G
H
J

























S1
−0.9157
−0.0242
0.04834
−0.0925
0.03855
0.05774
−0.0925
0.05787
−0.0178
0.0022


S2
−12.376
0.06268
−0.1415
−0.3392
0.89911
−0.7358
0.18342
0.07554
−0.0533
0.00878


S3
−0.8319
0.03105
−0.03
−0.6522
1.49233
−1.3976
0.63517
−0.1105
−0.0112
0.00479


S4
−7.367
−0.1852
1.71789
−6.8471
14.8214
−19.261
15.4645
−7.5184
2.03069
−0.2341


S5
12.337
−0.2536
1.74889
−6.6898
14.6458
−19.491
16.0712
−8.0307
2.2327
−0.2657


S6
1.14541
−0.0901
0.21678
−0.6218
1.45024
−2.2709
2.26343
−1.3948
0.48954
−0.0747


S7
−12.034
0.04238
−0.6838
2.52889
−5.5859
7.65595
−6.5535
3.38285
−0.9545
0.11242


S8
5.85918
−0.0168
−0.1532
0.44792
−0.9325
1.23635
−1.0356
0.53063
−0.1517
0.01866


S9
−43.521
0.01961
0.0447
−0.1445
0.17405
−0.1293
0.05892
−0.0164
0.00257
−0.0002


S10
−9.9703
−0.0233
−0.0527
0.08206
−0.0601
0.02462
−0.0062
0.00098
 −9E−05
3.5E−06


S11
−16.199
0.13832
−0.3024
0.30558
−0.2185
0.10175
−0.0304
0.00571
−0.0006
2.9E−05


S12
0.01179
−0.0979
0.0662
−0.0617
0.03374
−0.0119
0.00278
−0.0004
3.3E−05
 −1E−06


S13
−0.8414
−0.3646
0.15334
−0.0353
0.00329
0.00039
−0.0001
1.6E−05
 −8E−07
1.3E−08


S14
−1.4251
−0.2584
0.13506
−0.0538
0.01612
−0.0034
0.00047
 −4E−05
1.9E−06
 −4E−08









Twenty-Fourth Example


FIG. 47 is a view illustrating a twenty-fourth example of an optical imaging system, and FIG. 48 illustrates aberration curves of the optical imaging system of FIG. 47.


The twenty-fourth example of the optical imaging system includes a first lens 2410, a second lens 2420, a third lens 2430, a fourth lens 2440, a fifth lens 2450, a sixth lens 2460, a seventh lens 2470, a filter 2480, an image sensor 2490, and a stop (not shown) disposed between the second lens 2420 and the third lens 2430.


The first lens 2410 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 2420 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 2430 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fourth lens 2440 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 2450 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 2460 has a negative refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is concave.


The seventh lens 2470 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


One inflection point is formed on the object-side surface of the seventh lens 2470. For example, the object-side surface of the seventh lens 2470 is convex in the paraxial region, and becomes concave toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 2470. For example, the image-side surface of the seventh lens 2470 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 47, the stop is disposed at a distance of 0.963 mm from the object-side surface of the first lens 2410 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 24 listed in Table 55 that appears later in this application.


Table 47 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 47, and Table 48 below shows aspherical surface coefficients of the lenses of FIG. 47. Both surfaces of all of the lenses of FIG. 47 are aspherical.















TABLE 47











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.749266485
0.7080384
1.546
56.114
1.280


S2
Lens
7.762717699
0.025


1.225


S3
Second
3.688311274
0.23
1.667
20.353
1.160


S4
Lens
2.452435605
0.355115


1.033


S5
Third
39.91400184
0.23
1.667
20.353
1.053


S6
Lens
22.42331799
0.025


1.090


S7
Fourth
6.687663883
0.3582464
1.546
56.114
1.130


S8
Lens
17.14258608
0.393231


1.201


S9
Fifth
10.0342824
0.3524638
1.656
21.525
1.329


S10
Lens
6.555482673
0.2520001


1.664


S11
Sixth
−324.864371
0.6106713
1.656
21.525
1.841


S12
Lens
12.28603941
0.0342286


2.288


S13
Seventh
1.951834481
0.8257306
1.536
55.656
2.578


S14
Lens
1.756651038
0.2187466


2.963


S15
Filter
Infinity
0.21
1.518
64.197
3.258


S16

Infinity
0.6499884


3.334462215


S17
Imaging
Infinity



3.728830434



Plane



























TABLE 48







K
A
B
C
D
E
F
G
H
J


























S1
−0.2398
5.3E−05
0.02249
−0.0553
0.07912
−0.0725
0.04077
−0.0137
0.00194
0


S2
6.04243
−0.0363
0.03435
0.01444
−0.1124
0.16667
−0.1307
0.05398
−0.0092
0


S3
−1.7137
−0.0472
0.04097
0.02639
−0.116
0.18951
−0.1701
0.08267
−0.0161
0


S4
−0.2358
−0.0167
−0.01
0.05643
−0.0195
−0.1069
0.22786
−0.1897
0.06253
0


S5
−0.0716
−0.0169
−0.0047
−0.1892
0.62952
−1.0256
0.96124
−0.4977
0.11269
0


S6
−1.1573
0.01994
−0.1372
0.14441
−0.0555
0.14079
−0.2746
0.2067
−0.0539
0


S7
−28.459
0.02126
−0.1017
0.06112
0.04565
0.01801
−0.1503
0.1307
−0.0346
0


S8
−2.3038
−0.0386
0.03937
−0.1206
0.2443
−0.4112
0.47457
−0.3301
0.12291
−0.0182


S9
−3.3254
−0.1025
0.04401
−0.1067
0.23796
−0.3262
0.24087
−0.0929
0.01464
0


S10
−25.215
−0.0274
−0.1331
0.19086
−0.1562
0.07712
−0.0231
0.00411
−0.0003
0


S11
23.2017
0.16789
−0.2882
0.24139
−0.1422
0.05329
−0.0119
0.00149
 −8E−05
0


S12
−49.948
0.00684
−0.0175
0.00273
0.0001
−0.0001
3.8E−05
−6E−06
3.8E−07
0


S13
−1.9292
−0.2614
0.12601
−0.0405
0.00941
−0.0015
0.00015
−9E−06
2.2E−07
0


S14
−0.8288
−0.1737
0.06522
−0.0206
0.00465
−0.0007
6.3E−05
−3E−06
6.6E−08
0









Twenty-Fifth Example


FIG. 49 is a view illustrating a twenty-fifth example of an optical imaging system, and FIG. 50 illustrates aberration curves of the optical imaging system of FIG. 49.


The twenty-fifth example of the optical imaging system includes a first lens 2510, a second lens 2520, a third lens 2530, a fourth lens 2540, a fifth lens 2550, a sixth lens 2560, a seventh lens 2570, a filter 2580, an image sensor 2590, and a stop (not shown) disposed between the second lens 2520 and the third lens 2530.


The first lens 2510 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 2520 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 2530 has a positive refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The fourth lens 2540 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 2550 has a positive refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The sixth lens 2560 has a positive refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The seventh lens 2570 has a negative refractive power, a paraxial region of each of an object-side surface and an image-side surface thereof is concave.


No inflection point is formed on the object-side surface of the seventh lens 2570.


In addition, one inflection point is formed on the image-side surface of the seventh lens 2570. For example, the image-side surface of the seventh lens 2570 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 49, the stop is disposed at a distance of 0.872 mm from the object-side surface of the first lens 2510 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 25 listed in Table 55 that appears later in this application.


Table 49 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 49, and Table 50 below shows aspherical surface coefficients of the lenses of FIG. 49. Both surfaces of all of the lenses of FIG. 49 are aspherical.















TABLE 49











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.76028791
0.6171815
1.546
56.114
1.100


S2
Lens
14.12333348
0.025


1.040


S3
Second
5.834118934
0.23
1.667
20.353
1.011


S4
Lens
3.122671446
0.3733379


0.919


S5
Third
−49.94173366
0.3798697
1.546
56.114
0.995


S6
Lens
−15.18699611
0.1809039


1.096


S7
Fourth
23.36800299
0.3031664
1.667
20.353
1.124


S8
Lens
12.20982926
0.3354305


1.309


S9
Fifth
−4.394771982
0.4728905
1.546
56.114
1.471


S10
Lens
−1.598299305
0.025


1.698


S11
Sixth
−6.081499124
0.5446656
1.546
56.114
1.822


S12
Lens
−3.014533539
0.2724323


2.192


S13
Seventh
−6.149442968
0.42237
1.546
56.114
2.462


S14
Lens
1.636694252
0.1933361


2.880


S15
Filter
Infinity
0.21
1.518
64.197
3.223


S16

Infinity
0.6544156


3.300


S17
Imaging
Infinity



3.728



Plane



























TABLE 50







K
A
B
C
D
E
F
G
H
J


























S1
−1.0054
0.02246
0.02216
−0.0696
0.16036
−0.2238
0.18065
−0.0791
0.01412
0


S2
−1.5097
−0.1275
0.3975
−0.6982
0.68012
−0.322
0.02875
0.02904
−0.0076
0


S3
6.02943
−0.163
0.45041
−0.8514
1.05249
−0.8203
0.42351
−0.138
0.0213
0


S4
−0.8846
−0.0449
0.03929
0.15739
−0.6934
1.31707
−1.3069
0.67995
−0.143
0


S5
0
−0.0513
−0.0193
−0.016
0.00429
0.00341
−0.0155
0.03192
−0.0128
0


S6
0
−0.1089
−0.0569
0.35761
−0.9255
1.19468
−0.8604
0.33221
−0.0547
0


S7
−7.5
−0.2139
−0.0107
0.17878
−0.1827
−0.1159
0.3046
−0.1897
0.04049
0


S8
−43.341
−0.1402
−0.061
0.2777
−0.4123
0.3523
−0.1857
0.05641
−0.0071
0


S9
−35.081
−0.0602
0.07357
−0.1046
0.10843
−0.0726
0.02553
−0.0041
0.00022
0


S10
−1.5734
0.16205
−0.2197
0.18955
−0.107
0.03959
−0.0091
0.00113
−6E−05
0


S11
0.51533
0.21373
−0.3167
0.23989
−0.1217
0.03837
−0.0069
0.00066
−3E−05
0


S12
−1.1466
0.19671
−0.2565
0.15417
−0.0532
0.01146
−0.0015
0.00012
−4E−06
0


S13
−0.9056
−0.0077
−0.2094
0.18829
−0.0749
0.01671
−0.0022
0.00015
−5E−06
0


S14
−1.2797
−0.2192
0.10065
−0.0338
0.00878
−0.0018
0.00026
−2E−05
1.3E−06 
−3E−08









Twenty-Sixth Example


FIG. 51 is a view illustrating a twenty-sixth example of an optical imaging system, and FIG. 52 illustrates aberration curves of the optical imaging system of FIG. 51.


The twenty-sixth example of the optical imaging system includes a first lens 2610, a second lens 2620, a third lens 2630, a fourth lens 2640, a fifth lens 2650, a sixth lens 2660, a seventh lens 2670, a filter 2680, an image sensor 2690, and a stop (not shown) disposed between the second lens 2620 and the third lens 2630.


The first lens 2610 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 2620 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 2630 has a positive refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The fourth lens 2640 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The fifth lens 2650 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 2660 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 2670 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


Two inflection points are formed on the object-side surface of the seventh lens 2670. For example, the object-side surface of the seventh lens 2670 is convex in the paraxial region, becomes concave in a region outside the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 2670. For example, the image-side surface of the seventh lens 2670 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 51, the stop is disposed at a distance of 0.866 mm from the object-side surface of the first lens 2610 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 26 listed in Table 55 that appears later in this application.


Table 51 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 51, and Table 52 below shows aspherical surface coefficients of the lenses of FIG. 51. Both surfaces of all of the lenses of FIG. 51 are aspherical.















TABLE 51











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.882954913
0.5871918
1.546
56.114
1.050


S2
Lens
18.07331507
0.0491976


0.962


S3
Second
4.599463678
0.23
1.667
20.353
0.934


S4
Lens
2.546377474
0.3929389


0.837


S5
Third
−21.75460448
0.2744632
1.546
56.114
1.100


S6
Lens
−13.51443301
0.0611157


1.106


S7
Fourth
25.33486158
0.2655293
1.546
56.114
1.200


S8
Lens
25.33602848
0.3710469


1.285


S9
Fifth
9.468188048
0.3930453
1.656
21.525
1.500


S10
Lens
5.10288098
0.3790363


1.754


S11
Sixth
6.416223875
0.888499
1.546
56.114
2.041


S12
Lens
6.352062001
0.0460253


2.631


S13
Seventh
1.966539749
0.8854198
1.536
55.656
3.050


S14
Lens
1.769884599
0.3097825


3.456


S15
Filter
Infinity
0.21
1.518
64.197
3.768


S16

Infinity
0.65


3.829


S17
Imaging
Infinity



4.129



Plane



























TABLE 52







K
A
B
C
D
E
F
G
H
J


























S1
−0.1525
0.00346
0.00541
−0.0238
0.05874
−0.0925
0.08078
−0.0376
0.00687
0


S2
−36.188
−0.0554
0.19103
−0.4954
0.90918
−1.1194
0.84898
−0.3546
0.06168
0


S3
−0.1164
−0.0883
0.22642
−0.5273
0.9947
−1.274
1.01042
−0.4343
0.07596
0


S4
0.3326
−0.0462
0.09702
−0.2316
0.5455
−0.848
0.78539
−0.3759
0.07082
0


S5
51.7577
−0.0119
−0.0911
0.36173
−0.9067
1.38454
−1.3014
0.68351
−0.1493
0


S6
42.1637
0.0924
−0.5269
1.35579
−2.2584
2.50931
−1.8107
0.76109
−0.139
0


S7
−4.7579
0.13357
−0.5938
1.26101
−1.8115
1.7924
−1.1666
0.44267
−0.0728
0


S8
−3.4393
0.04714
−0.1842
0.28859
−0.3575
0.32734
−0.1971
0.06695
−0.0093
0


S9
−8.5449
−0.0502
−0.0588
0.15989
−0.2027
0.13981
−0.0542
0.01046
−0.0007
0


S10
−18.064
−0.044
−0.0734
0.14254
−0.1303
0.06906
−0.0217
0.00378
−0.0003
0


S11
−4.6497
0.06328
−0.1193
0.08822
−0.0426
0.01348
−0.0028
0.00037
−2E−05
0


S12
−50
0.03403
−0.0497
0.02457
−0.0072
0.00126
−0.0001
6.9E−06
−2E−07
0


S13
−2.4291
−0.1201
0.01667
0.00224
−0.0009
0.00011
−6E−06
1.3E−07
8.8E−10 
0


S14
−1.0032
−0.1111
0.02485
−0.0032
−0.0001
0.00013
−2E−05
1.9E−06
−8E−08
1.4E−09









Twenty-Seventh Example


FIG. 53 is a view illustrating a twenty-seventh example of an optical imaging system, and FIG. 54 illustrates aberration curves of the optical imaging system of FIG. 53.


The twenty-seventh example of the optical imaging system includes a first lens 2710, a second lens 2720, a third lens 2730, a fourth lens 2740, a fifth lens 2750, a sixth lens 2760, a seventh lens 2770, a filter 2780, an image sensor 2790, and a stop (not shown) disposed between the second lens 2720 and the third lens 2730.


The first lens 2710 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The second lens 2720 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The third lens 2730 has a positive refractive power, a paraxial region of an object-side surface thereof is concave, and a paraxial region of an image-side surface thereof is convex.


The fourth lens 2740 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 2750 has a negative refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The sixth lens 2760 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


The seventh lens 2770 has a positive refractive power, a paraxial region of an object-side surface thereof is convex, and a paraxial region of an image-side surface thereof is concave.


Two inflection points are formed on the object-side surface of the seventh lens 2770. For example, the object-side surface of the seventh lens 2770 is convex in the paraxial region, becomes concave in a region outside the paraxial region, and becomes convex toward an edge thereof.


In addition, one inflection point is formed on the image-side surface of the seventh lens 2770. For example, the image-side surface of the seventh lens 2770 is concave in the paraxial region, and becomes convex toward an edge thereof.


Although not illustrated in FIG. 53, the stop is disposed at a distance of 0.904 mm from the object-side surface of the first lens 2710 toward the imaging plane of the optical imaging system. This distance is equal to TTL-SL and can be calculated from the values of TTL and SL for Example 27 listed in Table 55 that appears later in this application.


Table 53 below shows physical properties of the lenses and other elements of the optical imaging system of FIG. 53, and Table 54 below shows aspherical surface coefficients of the lenses of FIG. 53. Both surfaces of all of the lenses of FIG. 53 are aspherical.















TABLE 53











Effective


Surface

Radius of
Thickness/
Index of
Abbe
Aperture


No.
Element
Curvature
Distance
Refraction
Number
Radius





















S1
First
1.898698558
0.6486367
1.546
56.114
1.260


S2
Lens
7.35678597
0.025


1.216


S3
Second
3.87893073
0.23
1.667
20.353
1.161


S4
Lens
2.762008891
0.3408168


1.053


S5
Third
−50.1241934
0.2818618
1.546
56.114
1.120


S6
Lens
−14.98893663
0.0597334


1.158


S7
Fourth
12.04981408
0.269789
1.546
56.114
1.220


S8
Lens
12.56574443
0.2918619


1.320


S9
Fifth
9.592575983
0.35
1.667
20.353
1.520


S10
Lens
5.27478585
0.3343756


1.762


S11
Sixth
6.87350249
0.8484117
1.546
56.114
2.052


S12
Lens
7.493319886
0.0591105


2.641


S13
Seventh
2.033708385
0.8835732
1.536
55.656
3.070


S14
Lens
1.843638917
0.3047846


3.425


S15
Filter
Infinity
0.21
1.518
64.197
3.764


S16

Infinity
0.6591161


3.825


S17
Imaging
Infinity



4.134



Plane



























TABLE 54







K
A
B
C
D
E
F
G
H
J


























S1
−0.1061
−0.0082
0.0469
−0.0925
0.08107
−0.0129
−0.032
0.02237
−0.0047
0


S2
−36.188
−0.0502
0.16245
−0.4029
0.69307
−0.7643
0.50209
−0.1789
0.02641
0


S3
0.0036
−0.0795
0.20571
−0.548
1.07416
−1.291
0.90975
−0.3412
0.05201
0


S4
0.40382
−0.0325
0.08844
−0.3009
0.70037
−0.9194
0.67381
−0.2424
0.03077
0


S5
51.7577
0.00548
−0.1746
0.50176
−0.9395
1.14417
−0.9144
0.4407
−0.0937
0


S6
42.1637
0.09529
−0.4992
1.03966
−1.2284
0.81694
−0.2802
0.03842
 4E−06
0


S7
−4.7579
0.1185
−0.4938
0.85535
−0.8643
0.51674
−0.185
0.04168
−0.0054
0


S8
−3.4393
0.04916
−0.194
0.31472
−0.3773
0.32494
−0.1878
0.06297
−0.0088
0


S9
−8.5449
−0.0638
0.02895
−0.0884
0.16492
−0.171
0.09832
−0.0306
0.00409
0


S10
−18.064
−0.0543
−0.0172
0.03209
−0.0179
0.00397
4.6E−06
−0.0001
7.7E−06 
0


S11
−4.6497
0.05354
−0.0909
0.06134
−0.0311
0.01102
−0.0026
0.00036
−2E−05
0


S12
−50
0.01031
−0.0176
0.00573
−0.0015
0.0003
 −4E−05
2.4E−06
−6E−08
0


S13
−2.606
−0.1177
0.01922
−0.0004
−1E−04
 −1E−05
4.5E−06
 −4E−07
9.4E−09 
0


S14
−1.0102
−0.0979
0.01866
−0.0024
0.00013
2.1E−05
 −6E−06
5.9E−07
−3E−08
5.6E−10









Table 55 below shows an overall focal length f of the optical imaging system, an overall length TTL of the optical imaging system (a distance along the optical axis from the object-side surface of the first lens to the imaging plane), a distance SL along the optical axis from the stop to the imaging plane, an f-number (F No.) of the optical imaging system (the overall focal length f of the optical imaging system divided by the diameter of an entrance pupil of the optical imaging system, where both f and the diameter of the entrance pupil are expressed in mm), an image height (IMG HT) on the imaging plane (one-half of a diagonal length of the imaging plane), and a field of view (FOV) of the optical imaging system for each of 1-27 described herein. The values of f, TTL, SL, and IMG HT are expressed in mm. The values of F No. are dimensionless values. The values of FOV are expressed in degrees.















TABLE 55





Example
f
TTL
SL
F No.
IMG HT
FOV





















1
3.685
4.200
3.543
2.04
3.261
81.60


2
4.848
6.000
5.097
1.54
4.000
77.80


3
4.315
5.290
4.472
1.56
3.552
77.30


4
3.970
4.812
3.652
1.59
3.400
79.54


5
3.950
4.819
3.650
1.58
3.250
77.47


6
4.350
5.300
4.917
1.58
3.384
79.58


7
4.300
5.200
4.849
1.58
3.700
80.13


8
4.020
4.901
4.565
1.58
3.400
79.28


9
4.280
5.100
4.369
1.71
3.535
77.84


10
4.423
5.500
4.810
1.73
3.535
76.14


11
4.381
5.500
4.774
1.65
3.535
76.54


12
4.401
5.300
4.142
1.69
3.728
79.31


13
4.536
5.499
4.300
1.69
3.728
77.56


14
4.544
5.500
4.423
1.67
3.728
77.54


15
4.751
5.637
4.544
1.64
3.528
72.12


16
4.105
4.900
3.981
1.87
3.261
75.03


17
4.447
5.144
4.894
2.07
3.528
75.63


18
4.700
5.650
4.882
1.81
3.928
78.82


19
4.400
5.200
4.576
1.81
3.261
72.55


20
3.994
5.125
4.484
1.57
3.261
77.38


21
3.900
4.720
3.650
1.77
3.261
78.69


22
3.750
4.560
3.510
1.68
3.261
80.29


23
4.451
5.703
4.621
1.63
3.728
78.60


24
4.592
5.478
4.515
1.79
3.728
76.90


25
4.302
5.240
4.368
1.95
3.728
80.46


26
4.966
5.993
5.127
2.36
4.128
78.45


27
4.667
5.797
4.893
1.85
4.128
81.80









Table 56 below shows in mm a focal length f1 of the first lens, a focal length f2 of the second lens, a focal length f3 of the third lens, a focal length f4 of the fourth lens, a focal length f5 of the fifth lens, a focal length f6 of the sixth lens, and a focal length f7 of the seventh lens for each of 1-27 described herein.
















TABLE 56





Example
f1
f2
f3
f4
f5
f6
f7






















1
3.293
−8.705
14.115
90.636
−15.266
40.265
−15.456


2
4.699
−11.772
21.070
−38.885
−12.922
2.771
−2.453


3
4.057
−11.047
44.073
−31.550
−17.744
2.228
−2.041


4
8.888
4.209
−6.477
16272754.8
517.877
−28.106
1852.192


5
8.409
4.355
−6.520
−4512.292
74.369
−22.452
1842.731


6
−64.233
3.248
−7.428
−43.722
52.425
3.010
−2.424


7
−41.858
3.128
−7.376
−103.801
64.750
2.915
−2.286


8
−38.662
2.911
−6.813
−43.728
59.023
2.640
−2.116


9
3.596
−7.349
−1245.238
15.657
−19.723
2.662
−2.171


10
3.671
−7.598
−10000
13.978
−15.153
2.617
−2.173


11
3.715
−7.660
−10000
15.301
−16.799
2.406
−2.034


12
9.952
4.985
−9.042
−60.959
28.461
−19.130
−36.205


13
9.489
5.133
−8.027
113.261
53.479
−17.195
−112.366


14
13.419
5.627
−8.921
16.142
−36.758
29.873
−12.281


15
4.273
−8.936
14.514
30.320
−17.493
61.723
−10.997


16
3.663
−6.575
13.173
72.886
−140.959
42.434
−9.509


17
3.626
−6.978
10.551
125.381
−28.155
−367.720
−9.031


18
4.553
−11.109
33.932
36.853
268.352
4.100
−2.623


19
4.290
−10.606
30.978
14.871
−21.133
3.784
−2.465


20
5.677
−73.551
−122.716
15.510
207.375
3.799
−2.466


21
3.720
−9.340
−800
14.620
−100
−674
−18.040


22
3.740
−9.750
−800
14.290
−99.5
−800
−19.010


23
18.149
4.970
−8.433
25.591
−19.167
25.748
69.101


24
3.971
−11.857
−77.132
19.846
−30.042
−18.041
68.790


25
3.620
−10.428
39.821
−38.762
4.342
10.303
−2.323


26
3.802
−8.955
64.595
12384.769
−17.503
299.093
57.797


27
4.499
−15.674
39.058
453.779
−18.160
102.612
59.134









Table 57 below shows in mm a thickness (DedgeT) of an edge of the first lens, a thickness (L2edgeT) of the edge of the second lens, a thickness (L3edgeT) of the edge of the third lens, a thickness (L4edgeT) of the edge of the fourth lens, a thickness (L5edgeT) of the edge of the fifth lens, a thickness (L6edgeT) of the edge of the sixth lens, and a thickness (L7edgeT) of the edge of the seventh lens for each of 1-27 described herein.
















TABLE 57





Example
L1edgeT
L2edgeT
L3edgeT
L4edgeT
L5edgeT
L6edgeT
L7edgeT






















1
0.202
0.208
0.199
0.197
0.238
0.204
0.351


2
0.253
0.354
0.255
0.348
0.284
0.256
0.831


3
0.226
0.305
0.232
0.280
0.261
0.225
0.618


4
0.232
0.262
0.334
0.193
0.270
0.288
0.298


5
0.233
0.259
0.333
0.203
0.272
0.330
0.376


6
0.220
0.270
0.348
0.224
0.259
0.269
0.437


7
0.200
0.268
0.356
0.220
0.240
0.240
0.353


8
0.194
0.250
0.328
0.211
0.239
0.222
0.388


9
0.222
0.377
0.235
0.240
0.189
0.260
0.323


10
0.181
0.365
0.201
0.239
0.393
0.361
0.817


11
0.179
0.345
0.206
0.257
0.415
0.262
0.950


12
0.257
0.255
0.340
0.276
0.365
0.307
0.278


13
0.280
0.247
0.375
0.321
0.375
0.279
0.517


14
0.250
0.250
0.440
0.270
0.318
0.652
0.294


15
0.223
0.354
0.233
0.210
0.386
0.654
0.695


16
0.225
0.368
0.245
0.232
0.200
0.615
0.447


17
0.269
0.308
0.190
0.230
0.410
0.714
0.300


18
0.323
0.418
0.258
0.328
0.292
0.401
0.493


19
0.205
0.407
0.201
0.333
0.278
0.348
0.815


20
0.218
0.347
0.211
0.259
0.277
0.251
0.950


21
0.100
0.280
0.100
0.410
0.170
0.410
0.580


22
0.110
0.290
0.100
0.330
0.140
0.420
0.620


23
0.248
0.303
0.393
0.456
0.352
0.835
0.513


24
0.250
0.275
0.277
0.250
0.337
0.479
0.782


25
0.252
0.293
0.238
0.374
0.258
0.415
0.686


26
0.293
0.298
0.252
0.251
0.409
0.715
0.678


27
0.246
0.280
0.254
0.273
0.356
0.630
0.692









Table 58 below shows in mm a sag value (L5S1 sag) at an outer end of the optical portion of the object-side surface of the fifth lens, a sag value (L5S2 sag) at an outer end of the optical portion of the image-side surface of the fifth lens, a thickness (Yc71P1) of the seventh lens at a first inflection point on the object-side surface of the seventh lens, a thickness (Yc71P2) of the seventh lens at a second inflection point on the object-side surface of the seventh lens, and a thickness (Yc72P1) of the seventh lens at a first inflection point on the image-side surface of the seventh lens for each of 1-27 described herein.














TABLE 58





Example
L5S1 sag
L5S2 sag
Yc71P1
Yc71P2
Yc72P1




















1
−0.405
−0.345
0.528
0.455
0.629


2
−0.464
−0.496
1.31

0.99


3
−0.315
−0.357
1.089

0.901


4
0.201
0.235
0.554
0.655
0.9


5
0.200
0.202
0.568
0.67 
0.667


6
0.115
0.139
0.93

0.811


7
0.148
0.172
0.88

0.795


8
0.123
0.129
0.859

0.769


9
−0.466
−0.526
2.933

4.142


10
−0.421
−0.473
3.25

4.55


11
−0.422
−0.453
3.319

4.481


12
0.210
0.245
0.569
0.641
0.67


13
0.210
0.185
0.647
0.751
0.771


14
0.185
0.267
0.527
0.485
0.647


15
−0.415
−0.431
0.604
0.886
0.818


16
−0.340
−0.437
0.658
0.747
0.81


17
−0.261
−0.263
0.473

0.631


18
−0.499
−0.478
0.806

0.771


19
−0.485
−0.407
0.89

0.92


20
−0.479
−0.422


0.781


21
−0.440
−0.430
0.72

0.12


22
−0.380
−0.430
0.72

0.12


23
0.210
0.372
0.61
0.706
0.722


24
0.270
0.286
0.889

1.015


25
0.276
0.509


0.968


26
0.092
0.103
0.955
1.103
1.128


27
0.179
0.173
0.964
1.114
1.13









Table 59 below shows in mm an inner diameter of each of the first to seventh spacers for each of 1-27 described herein. S1d is an inner diameter of the first spacer SP1, S2d is an inner diameter of the second spacer SP2, S3d is an inner diameter of the third spacer SP3, S4d is an inner diameter of the fourth spacer SP4, S5d is an inner diameter of the fifth spacer SP5, S6d is an inner diameter of the sixth spacer SP6, and S7d is an inner diameter of the seventh spacer SP7.
















TABLE 59





Example
S1d
S2d
S3d
S4d
S5d
S6d
S7d






















1
1.69
1.51
1.64
2.09
2.95
4.49



2
2.84
2.53
2.83
3.29
4.34
6.31



3
2.52
2.2
2.47
2.93
3.64
5.33



4
1.33
1.26
0.96
1.44
1.94
2.6



5
1.24
1.15
1.03
1.48
1.9
2.46



6
1.34
1.23
1.03
1.5
1.98
2.66



7
1.33
1.23
1.04
1.58
2.1
2.75



8
1.25
1.14
0.94
1.5
1.86
2.44



9
2.31
2.16
2.54
2.94
4.06
4.84
5.12


10
2.48
2.26
2.56
2.84
3.76
4.78
5.2 


11
2.48
2.23
2.56
2.86
3.69
4.58
5.07


12
2.58
2.4
2.49
2.97
4.16
4.89
5.51


13
2.55
2.4
2.49
2.97
4.02
4.89
5.63


14
2.65
2.46
2.39
2.9
3.8
5.15



15
2.706
2.468
2.446
2.616
3.308
5.582



16
2.176
2.058
2.122
2.39
2.808
4.792



17
2.12
2.1
2.04
2.12
2.81
4.64



18
2.43
2.48
2.89
3.38
4.57
6.18



19
2.32
2.36
2.56
2.93
3.7
4.35



20
2.41
2.3
2.66
3.03
3.76




21
2.06
1.784
2.136
2.632
2.956
4.366



22
2.076
1.784
2.078
2.59
2.85
4.128



23
2.68
2.51
2.54
3
3.96
5.28



24
2.39
2.09
2.24
2.65
3.62
4.78
5.08


25
2.06
1.89
2.15
2.7
3.61
4.56
4.84


26
1.89
1.84
2.33
2.73
3.73
5.43
6.03


27
2.39
2.15
2.4
2.82
3.94
5.68
6.02









Table 60 below shows in mm3 a volume of each of the first to seventh lenses for each of 1-27 described herein. L1v is a volume of the first lens, L2v is a volume of the second lens, L3v is a volume of the third lens, L4v is a volume of the fourth lens, L5v is a volume of the fifth lens, L6v is a volume of the sixth lens, and L7v is a volume of the seventh lens.
















TABLE 60





Example
L1v
L2v
L3v
L4v
L5v
L6v
L7v






















1
2.2524
2.0618
2.2767
2.9806
5.367
7.9203
15.204


2
9.4074
6.0389
7.8806
9.9733
14.2491
18.7217
48.3733


3
6.1771
4.5153
5.2418
5.8649
8.7918
11.0804
30.7452


4
4.9183
5.6902
6.3612
5.0504
8.147
10.2679
16.4786


5
6.3442
6.9494
7.7597
6.2076
6.8959
10.3364
16.5597


6
5.7249
8.0179
8.3774
7.9589
10.3434
11.1031
27.1511


7
7.0609
8.2183
8.3812
8.577
10.4368
10.0819
25.7323


8
5.0799
5.7347
5.8704
6.465
6.7471
7.523
21.0455


9
5.2342
5.0595
5.1455
4.1402
5.9856
8.1378
19.6812


10
4.6012
5.0554
4.4232
3.7935
9.9974
13.3429
31.7191


11
4.8917
4.777
4.399
3.8155
10.2897
11.3167
33.3467


12
5.639
4.858
6.6748
7.1627
11.0369
11.9357
27.1217


13
5.8304
4.8865
6.5128
7.1688
10.887
16.2551
26.8011


14
5.165
5.3015
6.2461
7.0472
12.2503
19.1335
17.9152


15
6.5129
6.0017
5.9544
6.0281
13.8948
30.2962
31.1147


16
3.8214
4.3362
4.4869
5.6551
6.8114
19.8745
20.3749


17
3.8115
4.6714
4.0552
5.0631
11.2844
25.7618
16.5646


18
6.2758
6.5315
7.7526
9.5642
12.5716
16.0772
29.9737


19
4.2347
5.5368
5.5931
7.5471
9.4202
8.9992
27.3258


20
4.6529
4.6572
6.2312
6.7131
10.2673
11.7401
33.5372


21
2.7732
3.7423
2.4001
9.3009
4.1785
16.1001
22.2706


22
2.9525
3.7672
1.9989
7.5203
3.1364
16.7166
21.7591


23
5.1107
5.8654
6.3124
10.0933
12.273
29.3788
26.3671


24
5.1465
4.5089
4.4695
4.8122
8.9386
18.2117
35.9358


25
3.81
3.9751
3.9272
6.1885
7.516
13.0347
31.8586


26
4.7517
4.3655
6.4562
5.0723
9.8674
36.8705
47.4701


27
5.6273
4.949
5.1423
5.0791
9.3624
31.5832
47.9081









Table 61 below shows in mg a weight of each of the first to seventh lenses for each of 1-27 described herein. L1w is a weight of the first lens, L2w is a weight of the second lens, L3w is a weight of the third lens, L4w is a weight of the fourth lens, L5w is a weight of the fifth lens, L6w is a weight of the sixth lens, and L7w is a weight of the seventh lens.
















TABLE 61





Example
L1w
L2w
L3w
L4w
L5w
L6w
L7w






















1
2.342
2.536
2.368
3.100
6.709
9.900
15.356


2
9.784
7.428
8.196
12.267
17.811
19.471
50.308


3
6.424
5.554
5.451
7.214
10.990
11.524
31.975


4
5.115
5.918
7.952
6.313
8.473
12.835
16.643


5
6.598
7.227
9.700
7.760
7.172
12.921
16.725


6
5.954
8.339
10.472
9.710
12.619
11.547
28.237


7
7.343
8.547
10.477
10.464
12.733
10.485
26.762


8
5.283
5.964
7.338
7.887
8.231
7.824
21.887


9
5.444
6.223
5.351
4.306
7.362
8.463
20.468


10
4.785
6.218
4.600
3.945
12.297
13.877
32.988


11
5.087
5.876
4.575
3.968
12.656
11.769
34.681


12
5.865
5.052
8.344
8.953
11.478
14.920
27.393


13
6.064
5.082
8.141
7.456
11.322
20.319
27.873


14
5.372
5.514
7.808
7.329
15.313
19.899
18.632


15
6.773
7.382
7.324
6.269
17.230
37.567
31.426


16
3.974
5.334
5.519
5.881
8.446
24.644
20.579


17
3.964
5.746
4.217
5.266
14.106
26.792
17.227


18
6.527
8.034
8.063
9.947
15.463
16.720
31.173


19
4.404
6.810
5.817
7.849
11.587
9.359
28.419


20
4.839
5.728
6.480
6.982
12.629
12.210
34.879


21
2.884
4.603
2.952
9.673
5.223
20.125
22.493


22
3.071
4.634
2.459
7.821
3.921
20.896
21.977


23
5.315
6.100
7.891
10.497
12.764
30.554
27.422


24
5.352
5.546
5.497
5.005
11.173
22.765
36.295


25
3.962
4.889
4.084
7.612
7.817
13.556
33.133


26
4.942
5.370
6.714
5.275
12.334
38.345
47.945


27
5.852
6.087
5.348
5.282
11.516
32.847
48.387









Table 62 below shows in mm an overall outer diameter (including a rib) of each of the first to seventh lenses for each of 1-27 described herein. L1TR is an overall outer diameter of the first lens, L2TR is an overall outer diameter of the second lens, L3TR is an overall outer diameter of the third lens, L4TR is an overall outer diameter of the fourth lens, LSTR is an overall outer diameter of the fifth lens, L6TR is an overall outer diameter of the sixth lens, and L7TR is an overall outer diameter of the seventh lens.
















TABLE 62





Example
L1TR
L2TR
L3TR
L4TR
L5TR
L6TR
L7TR






















1
3.34
3.54
3.84
4.14
4.82
5.72
5.92


2
4.93
5.13
5.63
6.23
7.2
7.6
7.8


3
4.22
4.42
4.72
5.52
6.24
6.64
6.84


4
3.13
3
2.75
2.49
2.37
2.23
2.15


5
2.29
2.4
2.54
2.63
2.78
2.91
3.04


6
2.46
2.58
2.69
2.8
3.17
3.31
3.47


7
2.48
2.61
2.72
2.82
3.19
3.34
3.5


8
2.19
2.32
2.44
2.57
2.74
3
3.11


9
4.22
4.42
4.54
4.72
5.4
5.74
6.3


10
4.2
4.35
4.49
4.65
5.5
5.84
6.63


11
4.14
4.28
4.42
4.58
5.45
5.79
6.58


12
4.21
4.3
4.44
4.84
5.47
6.12
6.9


13
4.21
4.3
4.44
4.84
5.47
6.12
6.9


14
4.19
4.28
4.41
4.81
5.51
6.16
6.52


15
4.502
4.69
5.164
5.752
6.608
6.996
7.182


16
3.836
3.974
4.536
5.176
6.33
6.458
6.558


17
3.51
3.81
4.39
4.98
5.85
6.15
6.25


18
4.27
4.46
5.04
5.63
6.5
6.9
7.1


19
3.93
4.13
4.71
6.17
5.3
6.57
6.67


20
4.03
4.23
4.81
5.4
6.27
6.67
6.77


21
3.802
4.012
4.126
4.902
5.646
6.086
6.422


22
3.8
3.99
4.068
4.816
5.514
5.92
6.246


23
4.26
4.35
4.49
4.89
5.52
6.75
7.26


24
4.1
4.19
4.32
4.72
5.35
6.17
7.03


25
3.73
3.82
3.96
4.39
4.96
6
6.86


26
3.97
4.06
4.19
4.63
5.2
7.15
8.02


27
4.39
4.48
4.61
5.04
5.61
7.09
7.95









Table 63 below shows in mm a maximum thickness of the rib of each of the first to seventh lenses for each of 1-27 described herein. The maximum thickness of the rib is a thickness of a portion of the rib in contact with a spacer. L1rt is a maximum thickness of the rib of the first lens, L2rt is a maximum thickness of the rib of the second lens, L3rt is a maximum thickness of the rib of the third lens, L4rt is a maximum thickness of the rib of the fourth lens, L5rt is a maximum thickness of the rib of the fifth lens, L6rt is a maximum thickness of the rib of the sixth lens, and L7rt is a maximum thickness of the rib of the seventh lens.
















TABLE 63





Example
L1rt
L2rt
L3rt
L4rt
L5rt
L6rt
L7rt






















1
0.245
0.26
0.25
0.235
0.285
0.265
0.44


2
0.58
0.38
0.33
0.3
0.39
0.475
0.92


3
0.485
0.375
0.31
0.21
0.295
0.335
0.685


4
0.51
0.46
0.48
0.27
0.4
0.32
0.36


5
0.54
0.5
0.52
0.42
0.21
0.39
0.4


6
0.39
0.44
0.47
0.36
0.42
0.38
0.47


7
0.59
0.44
0.47
0.35
0.38
0.3
0.39


8
0.54
0.37
0.41
0.33
0.37
0.27
0.42


9
0.435
0.43
0.36
0.215
0.32
0.33
0.405


10
0.38
0.46
0.35
0.18
0.51
0.47
0.85


11
0.41
0.45
0.34
0.18
0.45
0.37
1.01


12
0.55
0.38
0.58
0.41
0.5
0.32
0.53


13
0.56
0.38
0.56
0.41
0.5
0.32
0.54


14
0.52
0.42
0.52
0.41
0.61
0.7
0.37


15
0.482
0.492
0.369
0.196
0.427
0.615
0.737


16
0.422
0.482
0.258
0.282
0.269
0.558
0.489


17
0.482
0.395
0.316
0.328
0.422
0.885
0.409


18
0.508
0.554
0.444
0.473
0.41
0.438
0.522


19
0.431
0.556
0.361
0.429
0.38
0.38
0.667


20
0.431
0.457
0.361
0.364
0.38
0.334
0.729


21
0.35
0.423
0.276
0.46
0.172
0.525
0.641


22
0.366
0.392
0.239
0.383
0.137
0.605
0.655


23
0.5
0.41
0.51
0.54
0.52
0.97
0.55


24
0.46
0.4
0.39
0.26
0.43
0.54
0.83


25
0.4
0.42
0.37
0.5
0.32
0.46
0.72


26
0.47
0.41
0.45
0.41
0.47
0.93
0.7


27
0.44
0.39
0.4
0.4
0.38
0.74
0.72










FIG. 58 is a cross-sectional view illustrating an example of a seventh lens.



FIG. 58 illustrates the overall outer diameter (L7TR) of the seventh lens, the thickness (L7rt) of the flat portion of the rib of the seventh lens, the thickness (L7edgeT) of the edge of the seventh lens, the thickness (Yc71P1) of the seventh lens at the first inflection point on the object-side surface of the seventh lens, the thickness (Yc71P2) of the seventh lens at the second inflection point on the object-side surface of the seventh lens, and the thickness (Yc72P1) of the seventh lens at the first inflection point on the image-side surface of the seventh lens.


The examples described above enable the optical imaging system to be miniaturized and aberrations to be easily corrected to achieve high resolution.


While this disclosure includes specific examples, it will be apparent after an understanding of the disclosure of this application that various changes in form and details may be made in these examples without departing from the spirit and scope of the claims and their equivalents. The examples described herein are to be considered in a descriptive sense only, and not for purposes of limitation. Descriptions of features or aspects in each example are to be considered as being applicable to similar features or aspects in other examples. Suitable results may be achieved if the described techniques are performed in a different order, and/or if components in a described system, architecture, device, or circuit are combined in a different manner, and/or replaced or supplemented by other components or their equivalents. Therefore, the scope of the disclosure is defined not by the detailed description, but by the claims and their equivalents, and all variations within the scope of the claims and their equivalents are to be construed as being included in the disclosure.

Claims
  • 1. An optical imaging system comprising: a first lens having positive refractive power, a convex object-side surface, and a concave image-side surface;a second lens having negative refractive power, a convex object-side surface, and a concave image-side surface;a third lens having positive refractive power;a fourth lens having negative refractive power, a convex object-side surface, and a concave image-side surface;a fifth lens having refractive power;a sixth lens having refractive power; anda seventh lens having refractive power,wherein the first to seventh lenses are sequentially disposed in numerical order along an optical axis of the optical imaging system from an object side of the optical imaging system toward an imaging plane of the optical imaging system,wherein the optical imaging system has a total of seven lenses, andwherein the optical imaging system satisfies 0.6<TTL/(2*Img HT)<0.9, where TTL is a distance along the optical axis from the object-side surface of the first lens to the imaging plane of the image sensor, and Img HT is one-half of a diagonal length of the imaging plane of the image sensor.
  • 2. The optical imaging system of claim 1, wherein the optical imaging system satisfies 0.01<R1/R4<1.3, where R1 is a radius of curvature of the object-side surface of the first lens, and R4 is a radius of curvature of the image-side surface of the second lens.
  • 3. The optical imaging system of claim 2, wherein the seventh lens has a concave image-side surface, and the optical imaging system satisfies 0.6<(R11+R14)/(2*R1)<3.0, where R11 is a radius of curvature of an object-side surface of the sixth lens, and R14 is a radius of curvature of the image-side surface of the seventh lens.
  • 4. The optical imaging system of claim 1, wherein the optical imaging system further satisfies 0.1<(1/f1+1/f2+1/f3+1/f4+1/f5+1/f6+1/f7)*f<0.8, where f1 is a focal length of the first lens, f2 is a focal length of the second lens, f3 is a focal length of the third lens, f4 is a focal length of the fourth lens, f5 is a focal length of the fifth lens, f6 is a focal length of the sixth lens, f7 is a focal length of the seventh lens, and f is an overall focal length of the optical imaging system.
  • 5. The optical imaging system of claim 4, wherein the optical imaging system further satisfies 0.1<(1/f1+1/f2+1/f3+1/f4+1/f5+1/f6+1/f7)*TTL<1.0.
  • 6. The optical imaging system of claim 1, wherein the optical imaging system further satisfies 0.2<TD1/D67<0.8, where TD1 is a thickness along the optical axis of the first lens, and D67 is a distance along the optical axis from the object-side surface of the sixth lens to an image-side surface of the seventh lens.
  • 7. The optical imaging system of claim 1, wherein the optical imaging system satisfies SD12<SD34, wherein SD12 is a distance along an optical axis from the image-side surface of the first lens to the object-side surface of the second lens, and SD34 is a distance along the optical axis from an image-side surface of the third lens to an object-side surface of the fourth lens.
  • 8. The optical imaging system of claim 7, wherein the optical imaging system satisfies SD56<SD34, wherein SD56 is a distance along an optical axis from an image-side surface of the fifth lens to an object-side surface of the sixth lens.
  • 9. The optical imaging system of claim 8, wherein the optical imaging system satisfies SD56<SD67, wherein SD67 is a distance along the optical axis from an image-side surface of the sixth lens to an object-side surface of the seventh lens.
  • 10. The optical imaging system of claim 1, wherein the optical imaging system further satisfies 0.4<ΣTD/TTL<0.7, where ΣTD is a sum of thicknesses along the optical axis of the first to seventh lenses.
  • 11. The optical imaging system of claim 1, wherein the optical imaging system further satisfies 0.2<ΣSD/ΣTD<0.7, where ΣSD is a sum of air gaps along the optical axis between the first to seventh lenses and ΣTD is a sum of thicknesses along the optical axis of the first to seventh lenses.
  • 12. The optical imaging system of claim 1, wherein sixth lens has positive refractive power, and the seventh lens has negative refractive power.
  • 13. The optical imaging system of claim 12, wherein the sixth lens has a convex object-side surface and the seventh lens has a concave image-side surface.
  • 14. The optical imaging system of claim 1, wherein the third lens has a concave object-side surface and a convex image-side surface.
  • 15. The optical imaging system of claim 14, wherein the fifth lens has positive refractive power.
  • 16. The optical imaging system of claim 15, wherein the fifth lens has a concave object-side surface and a convex image-side surface.
Priority Claims (2)
Number Date Country Kind
10-2018-0061409 May 2018 KR national
10-2018-0106170 Sep 2018 KR national
CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a continuation of U.S. patent application Ser. No. 17/099,021 filed on Nov. 16, 2020, which is a continuation of U.S. patent application Ser. No. 16/424,535 filed on May 29, 2019, now U.S. Pat. No. 11,002,943 issued on May 11, 2021, which claims the benefit under 35 USC 119(a) of Korean Patent Application Nos. 10-2018-0061409 filed on May 29, 2018, and 10-2018-0106170 filed on Sep. 5, 2018, in the Korean Intellectual Property Office, the entire disclosures of which are incorporated herein by reference for all purposes.

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Related Publications (1)
Number Date Country
20230236390 A1 Jul 2023 US
Continuations (2)
Number Date Country
Parent 17099021 Nov 2020 US
Child 18189685 US
Parent 16424535 May 2019 US
Child 17099021 US