OPTICAL SYSTEM, LENS MODULE, AND ELECTRONIC DEVICE

Information

  • Patent Application
  • 20210396960
  • Publication Number
    20210396960
  • Date Filed
    August 31, 2021
    3 years ago
  • Date Published
    December 23, 2021
    3 years ago
Abstract
An optical system is provided. The optical system includes a first lens with a positive refractive power, where the first lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis; a second lens with a negative refractive power, where the second lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis; a third lens with a refractive power; a fourth lens with a positive refractive power; a fifth lens with a refractive power; a sixth lens with a refractive power, where the sixth lens has an object-side surface which is concave near the optical axis; and a seventh lens with a negative refractive power, where the seventh lens has an object-side surface which is convex near the optical axis and an image-side surface.
Description
TECHNICAL FIELD

The present disclosure relates to the technical field of optical imaging, and in particular to an optical system, a lens module, and an electronic device.


BACKGROUND

In recent years, with the development of manufacturing technologies for electronic devices such as smart phones and tablets and the emergence of diversified user requirements, the demand for miniaturized camera lenses in the market is gradually increasing. At present, an electronic device is usually equipped with multiple cameras with different characteristics and suitable for different application environments. As the size and thickness of electronic devices are maintained or even reduced, more stringent requirements on the miniaturization of the lenses of the electronic devices have emerged. In addition, with the advancement of semiconductor process technology, the pixel size of photosensitive elements has also been reduced, and miniaturized lenses with good imaging quality have become the mainstream of the market.


In order to provide users with a better imaging experience, imaging devices are usually equipped with large photosensitive elements. In addition, in order to achieve high imaging quality and large aperture, more lenses need to be installed in the imaging device, which makes it difficult to realize the miniaturization of the camera lens of the imaging device. Therefore, the existing lens cannot satisfy the requirements of large aperture, high resolution, and miniaturization at the same time.


SUMMARY

The present disclosure aims to provide an optical system, a lens module, and an electronic device to solve the above technical problems.


An optical system is provided in the present disclosure. The optical system includes, in order from an object side to an image side along an optical axis: a first lens with a positive refractive power, where the first lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis; a second lens with a negative refractive power, where the second lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis; a third lens with a refractive power; a fourth lens with a positive refractive power; a fifth lens with a refractive power; a sixth lens with a refractive power, where the sixth lens has an object-side surface which is concave near the optical axis; and a seventh lens with a negative refractive power, where the seventh lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis. Each of the first lens to the seventh lens has an aspherical object-side surface and an aspherical image-side surface. The optical system satisfies the following expression: TTL/Imgh<1.32, where TTL represents a distance from the object-side surface of the first lens to an imaging surface of the optical system along the optical axis, and Imgh represents half of a length of a diagonal of an effective pixel area of the imaging surface. According to the present disclosure, the first lens to the seventh lens are configured with appropriate surface profiles and refractive powers, so that the optical system can satisfy the requirements of high resolution, large aperture, and good imaging quality as well as maintain a compact structure and miniaturized. When the optical system satisfies the above expression and the imaging surface is fixed, the total length of the optical system can be small, and the miniaturization requirement for the optical system can be realized.


In some implementations, the optical system satisfies the following expression: 2<f/R14<3.5, where f represents an effective focal length of the optical system, and R14 represents a radius of curvature of the image-side surface of the seventh lens at the optical axis. When the optical system satisfies the above expression, R14 is assigned with an appropriate value, and the chief ray angle of the internal field of view of the chip can be better matched.


In some implementations, the optical system satisfies the following expression: FNO≤2, where FNO represents an F-number of the optical system. When the optical system satisfies the above expression and the effective focal length of the optical system is fixed, a large aperture can be ensured with FNO≤2, so that the amount of light entering the optical system can be large enough. Therefore, an image captured can be clearer, and the imaging quality of scenes with low brightness, such as night scenes, starry sky can be improved.


In some implementations, the optical system satisfies the following expression: TTL/f<1.35, where TTL represents the distance from the object-side surface of the first lens to the imaging surface of the optical system along the optical axis, and f represents an effective focal length of the optical system. When the optical system satisfies the above expression and the effective focal length of the optical system is fixed, the miniaturization requirement for the optical system can be satisfied.


In some implementations, the optical system satisfies the following expression: f1/f2>−0.15, where f1 represents an effective focal length of the first lens, and f2 represents an effective focal length of the second lens. When the optical system satisfies the above expression, among the effective focal length of the first lens and the effective focal length of the second lens, one is positive and the other is negative, which effectively helps to balance the chromatic aberration of the optical system. The above focal length ratio can be assigned with an appropriate value, thereby reducing the sensitivity of the optical system to a certain extent.


In some implementations, the optical system satisfies the following expression: sag1/sag2<15, where sag1 represents a saggital depth at an effective aperture of the object-side surface of the first lens, and sag2 represents a saggital depth at an effective aperture of the image-side surface of the first lens. When the optical system satisfies the above expression, the ratio of sag1/sag2 can be assigned with an appropriate value, thereby ensuring the manufacturability of the first lens, which is beneficial to manufacturing. In addition, the sensitivity of the entire optical system can be reduced.


In some implementations, the optical system satisfies the following expression: (R2+R1)/(R2−R1)<5, where R1 represents a radius of curvature of the object-side surface of the first lens, and R2 represents a radius of curvature of the image-side surface of the first lens. When the optical system satisfies the above expression, the ratio of (R2+R1)/(R2−R1) can be assigned with an appropriate value, thereby enhancing the refractive power of the first lens. The chromatic spherical aberration can be well corrected even with a large aperture, and the overall performance can be improved.


In some implementations, the optical system satisfies the following expression: f1234/f567>−0.5, where f1234 represents a combined focal length of the first lens to the fourth lens, and f567 represents a combined focal length of the fifth lens to the seventh lens. The optical system of the present disclosure can be regarded as composed of two groups of lenses. The first group of lenses includes the first lens to the fourth lens and has a positive focal length, and the second group of lenses includes the fifth lens to the seventh lens and has a negative focal length, which helps to correct the chromatic aberration of the entire optical system and improve the performance of the optical system. When the optical system satisfies the above expression, the absolute value of the focal length of the first group of lenses is smaller than the absolute value of the focal length of the second group of lenses, thereby reducing the sensitivity of the second group of lenses and improving the yield rate in the actual production process.


A lens module is provided. The lens includes a lens barrel, an electronic photosensitive element, and the above optical system. The first lens to the seventh lens of the optical system are disposed in the lens barrel, and the electronic photosensitive element is disposed on the image side of the optical system and configured to convert light passing through the first lens to the seventh lens and incident on the electronic photosensitive element into an electrical signal of an image. According to the present disclosure, the first lens to the seventh lens of the optical system are installed in the lens module and are configured with appropriate surface profiles and refractive powers. In this way, the lens module can satisfy the requirements of high resolution, large aperture, and good imaging quality as well as maintain a compact structure, and the miniaturization of the lens module can be achieved.


An electronic device is provided. The electronic device includes a housing and the above lens module received in the housing. According to the present disclosure, the above lens module is disposed in the electronic device, so that the electronic device can satisfy the requirements of high resolution, large aperture, and good imaging quality as well as maintain a compact structure, and the miniaturization of the electronic device can be achieved.





BRIEF DESCRIPTION OF THE DRAWINGS

In order to more clearly describe the technical solutions in the implementations of the present disclosure or the related art, the following will briefly introduce the drawings that need to be used in the description of the implementations or the related art. Obviously, the drawings in the following description illustrate only some implementations of the present disclosure. For those of ordinary skill in the art, other drawings can be obtained based on these drawings without creative work.



FIG. 1a is a schematic structural view of an optical system according to an implementation.



FIG. 1b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 1a.



FIG. 2a is a schematic structural view of an optical system according to an implementation.



FIG. 2b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 2a.



FIG. 3a is a schematic structural view of an optical system according to an implementation.



FIG. 3b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 3a.



FIG. 4a is a schematic structural view of an optical system according to an implementation.



FIG. 4b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 4a.



FIG. 5a is a schematic structural view of an optical system according to an implementation.



FIG. 5b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 5a.



FIG. 6a is a schematic structural view of an optical system according to an implementation.



FIG. 6b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 6a.



FIG. 7a is a schematic structural view of an optical system according to an implementation.



FIG. 7b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 7a.





DETAILED DESCRIPTION

Technical solutions in the implementations of the present disclosure will be described clearly and completely hereinafter with reference to the accompanying drawings in the implementations of the present disclosure. Apparently, the described implementations are merely some rather than all implementations of the present disclosure. All other implementations obtained by those of ordinary skill in the art based on the implementations of the present disclosure without creative efforts shall fall within the protection scope of the present disclosure.


A lens module is provided. The lens includes a lens barrel, an electronic photosensitive element, and an optical system according to some implementations of the present disclosure. The first lens to the seventh lens of the optical system are disposed in the lens barrel, and the electronic photosensitive element is disposed on the image side of the optical system and configured to convert light passing through the first lens to the seventh lens and incident on the electronic photosensitive element into an electrical signal of an image. The electronic photosensitive element may be a complementary metal oxide semiconductor (CMOS) or a charge-coupled device (CCD). The lens module can be an independent lens of a digital camera, or an imaging module integrated on an electronic device such as a smart phone. According to the present disclosure, the first lens to the seventh lens of the optical system are installed in the lens module and are configured with appropriate surface profiles and refractive powers. In this way, the lens module can satisfy the requirements of high resolution, large aperture, and good imaging quality as well as maintain a compact structure, and the miniaturization of the lens module can be achieved.


An electronic device is provided. The electronic device includes a housing and a lens module according to some implementations of the present disclosure received in the housing. The electronic device can be a smart phone, a personal digital assistant (PDA), a tablet computer, a smart watch, a drone, an e-book reader, a driving recorder, a wearable device, or the like. According to the present disclosure, the above lens module is provided in the electronic device, so that the electronic device can satisfy the requirements of high resolution, large aperture, and good imaging quality as well as maintain a compact structure, and the miniaturization of the electronic device can be achieved.


An optical system is provided. The optical system includes, in order from an object side to an image side along an optical axis: a first lens, a second lens, a third lens, a fourth lens, a fifth lens, and a seventh lens. In the first to sixth lenses, there is an air gap between any two adjacent lenses.


The first lens has a positive refractive power and an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis. The second lens has a negative refractive power and an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis. The third lens has a refractive power. The fourth lens has a positive refractive power. The fifth lens has a refractive power. The sixth lens has a refractive power and an object-side surface which is concave near the optical axis. The seventh lens has a negative refractive power and an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis. Each of the first lens to the seventh lens has an aspherical object-side surface and an aspherical image-side surface. The optical system satisfies the following expression: TTL/Imgh<1.32, where TTL represents a distance from the object-side surface of the first lens to an imaging surface of the optical system along the optical axis, and Imgh represents half of a length of a diagonal of an effective pixel area of the imaging surface. According to the present disclosure, the first lens to the seventh lens are configured with appropriate surface profiles and refractive powers, so that the optical system can satisfy the requirements of high resolution, large aperture, and good imaging quality as well as maintain a compact structure and miniaturized. When the optical system satisfies the above expression and the imaging surface is fixed, the total length of the optical system can be small, and the miniaturization requirement for the optical system can be realized.


In some implementations, the optical system satisfies the following expression: 2<f/R14<3.5, where f represents an effective focal length of the optical system, and R14 represents a radius of curvature of the image-side surface of the seventh lens at the optical axis. When the optical system satisfies the above expression, R14 is assigned with an appropriate value, and the chief ray angle of the internal field of view of the chip can be better matched.


In some implementations, the optical system satisfies the following expression: FNO≤2, where FNO represents an F-number of the optical system. When the optical system satisfies the above expression and the effective focal length of the optical system is fixed, a large aperture can be ensured with FNO≤2, so that the amount of light entering the optical system can be large enough. Therefore, an image captured can be clearer, and the imaging quality of scenes with low brightness, such as night scenes, starry sky can be improved.


In some implementations, the optical system satisfies the following expression: TTL/f<1.35, where TTL represents the distance from the object-side surface of the first lens to the imaging surface of the optical system along the optical axis, and f represents an effective focal length of the optical system. When the optical system satisfies the above expression and the effective focal length of the optical system is fixed, the miniaturization requirement for the optical system can be satisfied. An upper limit of TTL can be set, for example, to 7 mm.


In some implementations, the optical system satisfies the following expression: f1/f2>−0.15, where f1 represents an effective focal length of the first lens, and f2 represents an effective focal length of the second lens. When the optical system satisfies the above expression, among the effective focal length of the first lens and the effective focal length of the second lens, one is positive and the other is negative, which effectively helps to balance the chromatic aberration of the optical system. The above focal length ratio can be assigned with an appropriate value, thereby reducing the sensitivity of the optical system to a certain extent.


In some implementations, the optical system satisfies the following expression: sag1/sag2<15, where sag1 represents a saggital depth at an effective aperture of the object-side surface of the first lens, and sag2 represents a saggital depth at an effective aperture of the image-side surface of the first lens. When the optical system satisfies the above expression, the ratio of sag1/sag2 can be assigned with an appropriate value, thereby ensuring the manufacturability of the first lens, which is beneficial to manufacturing. In addition, the sensitivity of the entire optical system can be reduced.


In some implementations, the optical system satisfies the following expression: (R2+R1)/(R2−R1)<5, where R1 represents a radius of curvature of the object-side surface of the first lens, and R2 represents a radius of curvature of the image-side surface of the first lens. When the optical system satisfies the above expression, the ratio of (R2+R1)/(R2−R1) can be assigned with an appropriate value, thereby enhancing the refractive power of the first lens. The chromatic spherical aberration can be well corrected even with a large aperture, and the overall performance can be improved.


In some implementations, the optical system satisfies the following expression: f1234/f567>−0.5, where f1234 represents a combined focal length of the first lens to the fourth lens, and f567 represents a combined focal length of the fifth lens to the seventh lens. The optical system of the present disclosure can be regarded as composed of two groups of lenses. The first group of lenses includes the first lens to the fourth lens and has a positive focal length, and the second group of lenses includes the fifth lens to the seventh lens and has a negative focal length, which helps to correct the chromatic aberration of the entire optical system and improve the performance of the optical system. When the optical system satisfies the above expression, the absolute value of the focal length of the first group of lenses is smaller than the absolute value of the focal length of the second group of lenses, thereby reducing the sensitivity of the second group of lenses and improving the yield rate in the actual production process.


Referring to FIG. 1a and FIG. 1b, the optical system in this implementation includes, in order from an object side to an image side along an optical axis: a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6, and a seventh lens L7.


The first lens L1 has a positive refractive power. The object-side surface S1 of the first lens is convex near the optical axis, and the image-side surface S2 of the first lens is concave near the optical axis. The object-side surface S1 of the first lens is concave at the periphery, and the image-side surface S2 of the first lens is concave at the periphery. The second lens L2 has a negative refractive power. The object-side surface S3 of the second lens is convex near the optical axis, and the image-side surface S4 of the second lens is concave near the optical axis. The object-side surface S3 of the second lens is convex at the periphery, and the image-side surface S4 of the second lens is concave at the periphery. The third lens L3 has a negative refractive power. The object-side surface S5 of the third lens is convex near the optical axis, and the image-side surface S6 of the third lens is concave near the optical axis. The object-side surface S5 of the third lens is concave at the periphery, and the image-side surface S6 of the third lens is concave at the periphery. The fourth lens L4 has a positive refractive power. The object-side surface S7 of the fourth lens is convex near the optical axis, and the image-side surface S8 of the fourth lens is concave near the optical axis. The object-side surface S7 of the fourth lens is convex at the periphery, and the image-side surface S8 is a concave surface at the periphery. The fifth lens L5 has a negative refractive power. The object-side surface S9 of the fifth lens is concave near the optical axis, and the image-side surface S10 of the fifth lens is convex near the optical axis. The object-side surface S9 of the fifth lens is convex at the periphery, and the image-side surface S10 is convex at the periphery. The sixth lens L6 has a positive refractive power. The object-side surface S11 of the sixth lens is convex near the optical axis, and the image-side surface S12 of the sixth lens is concave near the optical axis. The object-side surface S11 of the sixth lens is convex at the periphery, and the image-side surface S12 is concave at the periphery. The seventh lens L7 has a negative refractive power. The object-side surface S13 of the seventh lens is convex near the optical axis, and the image-side surface S14 of the seventh lens is concave near the optical axis. The object-side surface S13 of the seventh lens is concave at the periphery, and the image-side surface S14 is convex at the periphery. The first lens L1 to the seventh lens L7 are all made of plastic.


In addition, the optical system also includes a stop (STO), an infrared filter L8, and an imaging surface S17. The stop is disposed on one side of the first lens L1 away from the second lens L2 for controlling the amount of light entering the optical system. In some implementations, the stop can also be disposed between two adjacent lenses or on other lenses. The infrared filter L8 is disposed on the image side of the seventh lens L7 and includes the object-side surface S15 and the image-side surface S16. The infrared filter L8 is used to filter out infrared light so that the light incident on the imaging surface S17 only contains visible light. The wavelength of the visible light is 380 nm-780 nm. The infrared filter L8 is made of glass and can be coated thereon. The imaging surface S17 is the surface on which an image formed after the light from an object passes through the optical system.


Table 1a shows characteristics of the optical system in this implementation. Data in Table 1a is obtained based on light of a wavelength of 587 nm. Y radius, thickness, and focal length are all in millimeters (mm).









TABLE 1a







Optical system of FIG. 1a


f = 5.91 mm, FNO = 1.75, FOV = 84.99°, TTL = 7.00 mm























Effective


Surface
Surface
Surface
Y


Refractive
Abbe
focal


number
name
type
Radius
Thickness
Material
index
number
length





OBJ
Object-
Spherical
Infinity
Infinity







side










surface









STO
Stop
Spherical
Infinity
−0.7397






S1 
First
Aspherical
2.2555
0.9948
Plastic
1.54
56.11
5.77


S2 
lens
Aspherical
6.7545
0.1653






S3 
Second
Aspherical
14.6558
0.2895
Plastic
1.67
19.24
−22.49


S4 
lens
Aspherical
7.3774
0.3206






S5 
Third
Aspherical
36.3401
0.3002
Plastic
1.67
19.24
−45.42


S6 
lens
Aspherical
16.5257
0.0763






S7 
Fourth
Aspherical
8.2472
0.4910
Plastic
1.52
56.74
19.96


S8 
lens
Aspherical
40.4931
0.4976






S9 
Fifth
Aspherical
−24.3496
0.3632
Plastic
1.59
28.32
−156.22


S10
lens
Aspherical
−33.3253
0.2661






S11
Sixth
Aspherical
4.5595
0.7035
Plastic
1.59
28.32
35.86


S12
lens
Aspherical
5.4867
0.4893






S13
Seventh
Aspherical
4.6352
0.8960
Plastic
1.54
55.75
−9.37


S14
lens
Aspherical
2.2461
0.3910






S15
Infrared
Spherical
Infinity
0.2100
Glass





S16
filter
Spherical
Infinity
0.5456






S17
Imaging
Spherical
Infinity
0.0000







surface





Note:


The reference wavelength = 587 nm.






The effective focal length of the optical system is represented as f, the F-number of the optical system is represented as FNO, the angle of view of the optical system is represented as FOV, and the distance from the object-side surface of the first lens to the imaging surface of the optical system along the optical axis is represented as TTL.


In this implementation, the object-side surface and the image-side surface of any one of the first lens L1 to the seventh lens L5 are aspherical. The surface profile x of each aspherical lens can be defined by but not limited to the following aspherical formula:







x
=



ch
2


1
+


1
-


(

k
+
1

)







c
2



h
2






+

Σ






Aih
i




;




where x represents a distance (saggital depth) along the optical axis from a vertex of the aspherical surface to a position on the aspherical surface at a height h, c represents the paraxial curvature of the aspherical surface, which is the inverse of the Y radius (that is, c=1/R, where R represents the Y radius in the Table 1a), k represents the conic coefficient, Ai represents the i-th order correction coefficient of the aspherical surface. Table 1b shows higher-order coefficients A4, A6, A8, A10, A12, A14, A16, A18, and A20 of each of aspherical lens surfaces S1 to S16 in the optical system of FIG. 1a.














TABLE 1b







Surface number
K
A4
A6
A8
A10





S1
−0.4993
0.0041
0.0081
−0.0154
0.0203


S2
−7.9341
−0.0158
0.0058
−0.0127
0.0240


S3
1.5364
−0.0355
0.0215
−0.0192
0.0356


S4
2.3871
−0.0190
0.0136
0.0023
0.0023


S5
0.0000
−0.0171
−0.0139
0.0275
−0.0451


S6
1.0666
−0.0293
−0.0126
0.0492
−0.0853


S7
−2.4870
−0.0410
−0.0029
0.0230
−0.0344


S8
9.7150
−0.0203
−0.0033
0.0015
−0.0069


S9
2.0000
−0.0076
−0.0045
−0.0112
0.0220


S10
−14.7771
−0.0123
−0.0249
0.0246
−0.0140


S11
−2.9609
−0.0032
−0.0253
0.0193
−0.0111


S12
−6.6950
−0.0106
0.0072
−0.0056
0.0017


S13
−2.5499
−0.1046
0.0323
−0.0075
0.0013


S14
−1.4469
−0.0895
0.0276
−0.0065
0.0010





Surface number
A12
A14
A16
A18
A20





S1
−0.0162
0.0080
−0.0024
0.0004
0.0000


S2
−0.0257
0.0164
−0.0063
0.0013
−0.0001


S3
−0.0394
0.0251
−0.0094
0.0019
−0.0002


S4
−0.0127
0.0153
−0.0097
0.0032
−0.0005


S5
0.0393
−0.0179
0.0023
0.0011
−0.0003


S6
0.0858
−0.0530
0.0196
−0.0039
0.0003


S7
0.0281
−0.0133
0.0032
−0.0003
0.0000


S8
0.0097
−0.0070
0.0028
−0.0006
0.0001


S9
−0.0211
0.0111
−0.0033
0.0005
0.0000


S10
0.0044
−0.0007
0.0000
0.0000
0.0000


S11
0.0040
−0.0009
0.0001
0.0000
0.0000


S12
−0.0003
0.0000
0.0000
0.0000
0.0000


S13
−0.0002
0.0000
0.0000
0.0000
0.0000


S14
−0.0001
0.0000
0.0000
0.0000
0.0000










FIG. 1b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 1a. The longitudinal spherical aberration curve represents the focus deviation of light of different wavelengths after passing through the lenses of the optical system. The astigmatic field curve represents the tangential field curvature and sagittal field curvature. The distortion curve represents the magnitude of distortion corresponding to different angles of view. As illustrated in FIG. 1b, the optical system of FIG. 1a can have good imaging quality.


Referring to FIG. 2a and FIG. 2b, the optical system in this implementation includes, in order from an object side to an image side along an optical axis: a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6, and a seventh lens L7.


The first lens L1 has a positive refractive power. The object-side surface S1 of the first lens is convex near the optical axis, and the image-side surface S2 of the first lens is concave near the optical axis. The object-side surface S1 of the first lens is concave at the periphery, and the image-side surface S2 of the first lens is convex at the periphery. The second lens L2 has a negative refractive power. The object-side surface S3 of the second lens is convex near the optical axis, and the image-side surface S4 of the second lens is concave near the optical axis. The object-side surface S3 of the second lens is convex at the periphery, and the image-side surface S4 of the second lens is convex at the periphery. The third lens L3 has a positive refractive power. The object-side surface S5 of the third lens is concave near the optical axis, and the image-side surface S6 of the third lens is convex near the optical axis. The object-side surface S5 of the third lens is concave at the periphery, and the image-side surface S6 of the third lens is concave at the periphery. The fourth lens L4 has a positive refractive power. The object-side surface S7 of the fourth lens is convex near the optical axis, and the image-side surface S8 of the fourth lens is convex near the optical axis. The object-side surface S7 of the fourth lens is convex at the periphery, and the image-side surface S8 is a concave surface at the periphery. The fifth lens L5 has a negative refractive power. The object-side surface S9 of the fifth lens is concave near the optical axis, and the image-side surface S10 of the fifth lens is convex near the optical axis. The object-side surface S9 of the fifth lens is convex at the periphery, and the image-side surface S10 is concave at the periphery. The sixth lens L6 has a positive refractive power. The object-side surface S11 of the sixth lens is convex near the optical axis, and the image-side surface S12 of the sixth lens is concave near the optical axis. The object-side surface S11 of the sixth lens is convex at the periphery, and the image-side surface S12 is concave at the periphery. The seventh lens L7 has a negative refractive power. The object-side surface S13 of the seventh lens is convex near the optical axis, and the image-side surface S14 of the seventh lens is concave near the optical axis. The object-side surface S13 of the seventh lens is concave at the periphery, and the image-side surface S14 is convex at the periphery.


The other structures of the optical system of FIG. 2a are identical with the optical system of FIG. 1a, reference can be made to the optical system of FIG. 1a.


Table 2a shows characteristics of the optical system in this implementation. Data in Table 2a is obtained based on light of a wavelength of 587 nm. Y radius, thickness, and focal length are all in millimeters (mm).









TABLE 2a







Optical system of FIG. 2a


f = 5.90 mm, FNO = 1.78, FOV = 84.97°, TTL = 7.00 mm























Effective


Surface
Surface
Surface
Y


Refractive
Abbe
focal


number
name
type
Radius
Thickness
Material
index
number
length





OBJ
Object-
Spherical
Infinity
Infinity







side










surface









STO
Stop
Spherical
Infinity
−0.7221






S1 
First
Aspherical
2.2446
0.9837
Plastic
1.54
56.11
5.55


S2 
lens
Aspherical
7.3970
0.1497






S3 
Second
Aspherical
16.3737
0.2560
Plastic
1.67
19.24
−18.18


S4 
lens
Aspherical
6.9488
0.3240






S5 
Third
Aspherical
−42.6470
0.2985
Plastic
1.67
19.24
918.36


S6 
lens
Aspherical
−40.0000
0.0567






S7 
Fourth
Aspherical
12.6162
0.4846
Plastic
1.52
56.74
23.75


S8 
lens
Aspherical
−427.5720
0.6377






S9 
Fifth
Aspherical
−16.0282
0.3500
Plastic
1.59
28.32
−64.82


S10
lens
Aspherical
−27.9003
0.1819






S11
Sixth
Aspherical
4.8786
0.7095
Plastic
1.59
28.32
75.20


S12
lens
Aspherical
5.1890
0.4504






S13
Seventh
Aspherical
4.4476
0.9647
Plastic
1.54
55.75
−10.48


S14
lens
Aspherical
2.2931
0.3969






S15
Infrared
Spherical
Infinity
0.2100
Glass





S16
filter
Spherical
Infinity
0.5456






S17
Imaging
Spherical
Infinity
0.0000







surface
Spherical
Infinity





Note:


The reference wavelength = 587 nm.






Each parameter in Table 2a represents the same meaning as that in the optical system of FIG. 1a.


Table 2b shows higher-order coefficients that can be used for each aspherical lens surface in the optical system of FIG. 2a, where the surface profile of each aspherical lens surface can be defined by the formula given in the optical system of FIG. 1a.














TABLE 2b







Surface number
K
A4
A6
A8
A10





S1
−0.4790
0.0031
0.0120
−0.0224
0.0286


S2
−6.5209
−0.0158
0.0018
−0.0009
0.0086


S3
10.0000
−0.0359
0.0198
−0.0117
0.0308


S4
1.8169
−0.0190
0.0201
−0.0311
0.0893


S5
0.0000
−0.0127
−0.0115
−0.0136
0.0533


S6
−18.0000
−0.0071
−0.0618
0.1233
−0.1714


S7
3.8640
−0.0251
−0.0254
0.0203
0.0115


S8
−10.2850
−0.0215
−0.0020
0.0026
−0.0150


S9
2.0000
−0.0068
−0.0112
0.0029
0.0054


S10
−18.0000
−0.0018
−0.0539
0.0562
−0.0354


S11
−2.1235
0.0070
−0.0524
0.0448
−0.0268


S12
−7.8596
−0.0083
0.0059
−0.0059
0.0022


S13
−2.4290
−0.1016
0.0333
−0.0083
0.0015


S14
−1.4674
−0.0856
0.0271
−0.0067
0.0011





Surface number
A12
A14
A16
A18
A20





S1
−0.0226
0.0112
−0.0034
0.0006
0.0000


S2
−0.0134
0.0106
−0.0048
0.0012
−0.0001


S3
−0.0428
0.0318
−0.0136
0.0031
−0.0003


S4
−0.1406
0.1266
−0.0670
0.0194
−0.0024


S5
−0.0890
0.0864
−0.0497
0.0156
−0.0020


S6
0.1636
−0.0999
0.0370
−0.0075
0.0006


S7
−0.0364
0.0341
−0.0167
0.0042
−0.0004


S8
0.0220
−0.0165
0.0069
−0.0015
0.0001


S9
−0.0089
0.0055
−0.0017
0.0003
0.0000


S10
0.0137
−0.0032
0.0004
0.0000
0.0000


S11
0.0102
−0.0024
0.0003
0.0000
0.0000


S12
−0.0004
0.0001
0.0000
0.0000
0.0000


S13
−0.0002
0.0000
0.0000
0.0000
0.0000


S14
−0.0001
0.0000
0.0000
0.0000
0.0000










FIG. 2b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 2a. As illustrated in FIG. 2b, the optical system of FIG. 2a can have good imaging quality.


Referring to FIG. 3a and FIG. 3b, the optical system in this implementation includes, in order from an object side to an image side along an optical axis: a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6, and a seventh lens L7.


The first lens L1 has a positive refractive power. The object-side surface S1 of the first lens is convex near the optical axis, and the image-side surface S2 of the first lens is concave near the optical axis. The object-side surface S1 of the first lens is concave at the periphery, and the image-side surface S2 of the first lens is convex at the periphery. The second lens L2 has a negative refractive power. The object-side surface S3 of the second lens is convex near the optical axis, and the image-side surface S4 of the second lens is concave near the optical axis. The object-side surface S3 of the second lens is convex at the periphery, and the image-side surface S4 of the second lens is convex at the periphery. The third lens L3 has a negative refractive power. The object-side surface S5 of the third lens is convex near the optical axis, and the image-side surface S6 of the third lens is concave near the optical axis. The object-side surface S5 of the third lens is concave at the periphery, and the image-side surface S6 of the third lens is concave at the periphery. The fourth lens L4 has a positive refractive power. The object-side surface S7 of the fourth lens is convex near the optical axis, and the image-side surface S8 of the fourth lens is concave near the optical axis. The object-side surface S7 of the fourth lens is convex at the periphery, and the image-side surface S8 is a concave surface at the periphery. The fifth lens L5 has a positive refractive power. The object-side surface S9 of the fifth lens is convex near the optical axis, and the image-side surface S10 of the fifth lens is concave near the optical axis. The object-side surface S9 of the fifth lens is convex at the periphery, and the image-side surface S10 is convex at the periphery. The sixth lens L6 has a positive refractive power. The object-side surface S11 of the sixth lens is convex near the optical axis, and the image-side surface S12 of the sixth lens is concave near the optical axis. The object-side surface S11 of the sixth lens is convex at the periphery, and the image-side surface S12 is concave at the periphery. The seventh lens L7 has a negative refractive power. The object-side surface S13 of the seventh lens is convex near the optical axis, and the image-side surface S14 of the seventh lens is concave near the optical axis. The object-side surface S13 of the seventh lens is concave at the periphery, and the image-side surface S14 is convex at the periphery.


The other structures of the optical system of FIG. 3a are identical with the optical system of FIG. 1a, reference can be made to the optical system of FIG. 1a.


Table 3a shows characteristics of the optical system in this implementation. Data in Table 3a is obtained based on light of a wavelength of 587 nm. Y radius, thickness, and focal length are all in millimeters (mm).









TABLE 3a







Optical system of FIG. 3a


f = 5.90 mm, FNO = 1.75, FOV = 84.94°, TTL = 7.00 mm























Effective


Surface
Surface
Surface
Y


Refractive
Abbe
focal


number
name
type
Radius
Thickness
Material
index
number
length





OBJ
Object-
Spherical
Infinity
Infinity







side










surface









STO
Stop
Spherical
Infinity
−0.7389






S1 
First
Aspherical
2.2604
0.9956
Plastic
1.54
56.11
5.70


S2 
lens
Aspherical
7.0529
0.1353






S3 
Second
Aspherical
13.6928
0.3157
Plastic
1.67
19.24
−20.83


S4 
lens
Aspherical
6.8543
0.3212






S5 
Third
Aspherical
64.8948
0.2900
Plastic
1.67
19.24
−42.34


S6 
lens
Aspherical
19.7301
0.0769






S7 
Fourth
Aspherical
8.6064
0.4800
Plastic
1.52
56.74
19.20


S8 
lens
Aspherical
64.2953
0.5334






S9 
Fifth
Aspherical
250.0000
0.3644
Plastic
1.59
28.32
2257.96


S10
lens
Aspherical
307.8892
0.2771






S11
Sixth
Aspherical
5.0757
0.7000
Plastic
1.59
28.32
39.90


S12
lens
Aspherical
6.1476
0.4715






S13
Seventh
Aspherical
4.9301
0.8960
Plastic
1.54
55.75
−8.80


S14
lens
Aspherical
2.2563
0.3874






S15
Infrared
Spherical
Infinity
0.2100
Glass





S16
filter
Spherical
Infinity
0.5456






S17
Imaging
Spherical
Infinity
0.0000







surface












Note:


The reference wavelength = 587 nm.






Each parameter in Table 3a represents the same meaning as that in the optical system of FIG. 1a.


Table 3b shows higher-order coefficients that can be used for each aspherical lens surface in the optical system of FIG. 3a, where the surface profile of each aspherical lens surface can be defined by the formula given in the optical system of FIG. 1a.














TABLE 3b







Surface number
K
A4
A6
A8
A10





S1
−0.4912
0.0033
0.0094
−0.0164
0.0199


S2
−7.1839
−0.0187
0.0061
−0.0071
0.0153


S3
7.8178
−0.0344
0.0202
−0.0117
0.0223


S4
2.2704
−0.0178
0.0229
−0.0335
0.0808


S5
0.0000
−0.0315
0.0276
−0.0713
0.1178


S6
−14.0833
−0.0494
0.0285
−0.0085
−0.0257


S7
−4.4771
−0.0591
0.0431
−0.0595
0.0757


S8
−0.2850
−0.0252
0.0031
−0.0056
−0.0017


S9
−18.0000
−0.0130
0.0002
−0.0161
0.0257


S10
−8.0000
−0.0079
−0.0339
0.0319
−0.0177


S11
−2.3210
0.0068
−0.0365
0.0259
−0.0141


S12
−6.2843
−0.0047
0.0032
−0.0043
0.0015


S13
−2.2037
−0.1037
0.0318
−0.0073
0.0012


S14
−1.4424
−0.0905
0.0285
−0.0069
0.0011





Surface number
A12
A14
A16
A18
A20





S1
−0.0148
0.0069
−0.0019
0.0003
0.0000


S2
−0.0182
0.0125
−0.0051
0.0011
−0.0001


S3
−0.0281
0.0198
−0.0081
0.0018
−0.0002


S4
−0.1214
0.1075
−0.0562
0.0161
−0.0020


S5
−0.1381
0.1082
−0.0540
0.0154
−0.0019


S6
0.0452
−0.0355
0.0149
−0.0032
0.0003


S7
−0.0715
0.0453
−0.0182
0.0041
−0.0004


S8
0.0085
−0.0080
0.0037
−0.0009
0.0001


S9
−0.0217
0.0104
−0.0028
0.0004
0.0000


S10
0.0059
−0.0011
0.0001
0.0000
0.0000


S11
0.0049
−0.0011
0.0001
0.0000
0.0000


S12
−0.0003
0.0000
0.0000
0.0000
0.0000


S13
−0.0001
0.0000
0.0000
0.0000
0.0000


S14
−0.0001
0.0000
0.0000
0.0000
0.0000










FIG. 3b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 3a. As illustrated in FIG. 3b, the optical system of FIG. 3a can have good imaging quality.


Referring to FIG. 4a and FIG. 4b, the optical system in this implementation includes, in order from an object side to an image side along an optical axis: a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6, and a seventh lens L7.


The first lens L1 has a positive refractive power. The object-side surface S1 of the first lens is convex near the optical axis, and the image-side surface S2 of the first lens is concave near the optical axis. The object-side surface S1 of the first lens is concave at the periphery, and the image-side surface S2 of the first lens is convex at the periphery. The second lens L2 has a negative refractive power. The object-side surface S3 of the second lens is convex near the optical axis, and the image-side surface S4 of the second lens is concave near the optical axis. The object-side surface S3 of the second lens is convex at the periphery, and the image-side surface S4 of the second lens is convex at the periphery. The third lens L3 has a negative refractive power. The object-side surface S5 of the third lens is convex near the optical axis, and the image-side surface S6 of the third lens is concave near the optical axis. The object-side surface S5 of the third lens is concave at the periphery, and the image-side surface S6 of the third lens is concave at the periphery. The fourth lens L4 has a positive refractive power. The object-side surface S7 of the fourth lens is convex near the optical axis, and the image-side surface S8 of the fourth lens is concave near the optical axis. The object-side surface S7 of the fourth lens is convex at the periphery, and the image-side surface S8 is a concave surface at the periphery. The fifth lens L5 has a positive refractive power. The object-side surface S9 of the fifth lens is convex near the optical axis, and the image-side surface S10 of the fifth lens is concave near the optical axis. The object-side surface S9 of the fifth lens is concave at the periphery, and the image-side surface S10 is convex at the periphery. The sixth lens L6 has a negative refractive power. The object-side surface S11 of the sixth lens is concave near the optical axis, and the image-side surface S12 of the sixth lens is concave near the optical axis. The object-side surface S11 of the sixth lens is convex at the periphery, and the image-side surface S12 is concave at the periphery. The seventh lens L7 has a negative refractive power. The object-side surface S13 of the seventh lens is convex near the optical axis, and the image-side surface S14 of the seventh lens is concave near the optical axis. The object-side surface S13 of the seventh lens is concave at the periphery, and the image-side surface S14 is convex at the periphery.


The other structures of the optical system of FIG. 4a are identical with the optical system of FIG. 1a, reference can be made to the optical system of FIG. 1a.


Table 4a shows characteristics of the optical system in this implementation. Data in Table 4a is obtained based on light of a wavelength of 587 nm. Y radius, thickness, and focal length are all in millimeters (mm).









TABLE 4a







Optical system of FIG. 4a


f = 5.88 mm, FNO = 1.75, FOV = 84.93°, TTL = 7.00 mm























Effective


Surface
Surface
Surface
Y


Refractive
Abbe
focal


number
name
type
Radius
Thickness
Material
index
number
length





OBJ
Object-
Spherical
Infinity
Infinity







side










surface









STO
Stop
Spherical
Infinity
−0.7364






S1 
First
Aspherical
2.2527
0.9920
Plastic
1.54
56.11
5.74


S2 
lens
Aspherical
6.8366
0.1352






S3 
Second
Aspherical
13.9790
0.3220
Plastic
1.67
19.24
−23.29


S4 
lens
Aspherical
7.3123
0.3012






S5 
Third
Aspherical
47.5774
0.2900
Plastic
1.67
19.24
−46.38


S6 
lens
Aspherical
18.7734
0.1066






S7 
Fourth
Aspherical
7.3168
0.4800
Plastic
1.52
56.74
18.96


S8 
lens
Aspherical
28.3537
0.5684






S9 
Fifth
Aspherical
−26.9211
0.4526
Plastic
1.59
28.32
13.92


S10
lens
Aspherical
−6.3117
0.2686






S11
Sixth
Aspherical
−99.9367
0.7000
Plastic
1.59
28.32
−19.18


S12
lens
Aspherical
12.7317
0.3131






S13
Seventh
Aspherical
4.9077
0.9094
Plastic
1.54
55.75
−8.42


S14
lens
Aspherical
2.1976
0.4052






S15
Infrared
Spherical
Infinity
0.2100
Glass





S16
filter
Spherical
Infinity
0.5456






S17
Imaging
Spherical
Infinity
0.0000







surface





Note:


The reference wavelength = 587 nm.






Each parameter in Table 4a represents the same meaning as that in the optical system of FIG. 1a.


Table 4b shows higher-order coefficients that can be used for each aspherical lens surface in the optical system of FIG. 4a, where the surface profile of each aspherical lens surface can be defined by the formula given in the optical system of FIG. 1a.














TABLE 4b







Surface number
K
A4
A6
A8
A10





S1
−0.4893
0.0019
0.0150
−0.0281
0.0346


S2
−8.0854
−0.0170
0.0046
−0.0089
0.0206


S3
5.8805
−0.0323
0.0194
−0.0209
0.0426


S4
3.7165
−0.0151
0.0186
−0.0305
0.0811


S5
0.0000
−0.0325
0.0380
−0.0801
0.0972


S6
−12.5796
−0.0533
0.0488
−0.0351
−0.0167


S7
−5.6570
−0.0631
0.0453
−0.0398
0.0257


S8
−10.2850
−0.0332
0.0137
−0.0236
0.0241


S9
2.0000
−0.0362
0.0495
−0.0793
0.0774


S10
−18.0000
−0.0222
0.0064
−0.0110
0.0070


S11
−12.8810
0.0317
−0.0470
0.0282
−0.0163


S12
1.6104
0.0154
−0.0090
−0.0004
0.0008


S13
−2.3616
−0.0953
0.0320
−0.0080
0.0014


S14
−1.4139
−0.0918
0.0298
−0.0075
0.0013





Surface number
A12
A14
A16
A18
A20





S1
−0.0262
0.0124
−0.0036
0.0006
0.0000


S2
−0.0246
0.0169
−0.0069
0.0015
−0.0001


S3
−0.0508
0.0351
−0.0142
0.0031
−0.0003


S4
−0.1243
0.1105
−0.0577
0.0164
−0.0020


S5
−0.0838
0.0514
−0.0223
0.0062
−0.0008


S6
0.0563
−0.0509
0.0234
−0.0055
0.0005


S7
−0.0164
0.0108
−0.0055
0.0016
−0.0002


S8
−0.0164
0.0067
−0.0015
0.0001
0.0000


S9
−0.0494
0.0202
−0.0051
0.0007
0.0000


S10
−0.0022
0.0005
−0.0001
0.0000
0.0000


S11
0.0068
−0.0018
0.0003
0.0000
0.0000


S12
−0.0002
0.0000
0.0000
0.0000
0.0000


S13
−0.0002
0.0000
0.0000
0.0000
0.0000


S14
−0.0001
0.0000
0.0000
0.0000
0.0000










FIG. 4b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 4a. As illustrated in FIG. 4b, the optical system of FIG. 4a can have good imaging quality.


Referring to FIG. 5a and FIG. 5b, the optical system in this implementation includes, in order from an object side to an image side along an optical axis: a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6, and a seventh lens L7.


The first lens L1 has a positive refractive power. The object-side surface S1 of the first lens is convex near the optical axis, and the image-side surface S2 of the first lens is concave near the optical axis. The object-side surface S1 of the first lens is concave at the periphery, and the image-side surface S2 of the first lens is convex at the periphery. The second lens L2 has a negative refractive power. The object-side surface S3 of the second lens is convex near the optical axis, and the image-side surface S4 of the second lens is concave near the optical axis. The object-side surface S3 of the second lens is convex at the periphery, and the image-side surface S4 of the second lens is convex at the periphery. The third lens L3 has a negative refractive power. The object-side surface S5 of the third lens is convex near the optical axis, and the image-side surface S6 of the third lens is concave near the optical axis. The object-side surface S5 of the third lens is concave at the periphery, and the image-side surface S6 of the third lens is concave at the periphery. The fourth lens L4 has a positive refractive power. The object-side surface S7 of the fourth lens is convex near the optical axis, and the image-side surface S8 of the fourth lens is convex near the optical axis. The object-side surface S7 of the fourth lens is convex at the periphery, and the image-side surface S8 is a concave surface at the periphery. The fifth lens L5 has a negative refractive power. The object-side surface S9 of the fifth lens is concave near the optical axis, and the image-side surface S10 of the fifth lens is convex near the optical axis. The object-side surface S9 of the fifth lens is convex at the periphery, and the image-side surface S10 is concave at the periphery. The sixth lens L6 has a positive refractive power. The object-side surface S11 of the sixth lens is convex near the optical axis, and the image-side surface S12 of the sixth lens is convex near the optical axis. The object-side surface S11 of the sixth lens is convex at the periphery, and the image-side surface S12 is concave at the periphery. The seventh lens L7 has a negative refractive power. The object-side surface S13 of the seventh lens is convex near the optical axis, and the image-side surface S14 of the seventh lens is concave near the optical axis. The object-side surface S13 of the seventh lens is concave at the periphery, and the image-side surface S14 is convex at the periphery.


The other structures of the optical system of FIG. 5a are identical with the optical system of FIG. 1a, reference can be made to the optical system of FIG. 1a.


Table 5a shows characteristics of the optical system in this implementation. Data in Table 5a is obtained based on light of a wavelength of 587 nm. Y radius, thickness, and focal length are all in millimeters (mm).









TABLE 5a







Optical system of FIG. 5a


f = 5.90 mm, FNO = 1.75, FOV = 84.97°, TTL = 7.00 mm























Effective


Surface
Surface
Surface
Y


Refractive
Abbe
focal


number
name
type
Radius
Thickness
Material
index
number
length





OBJ
Object-
Spherical
Infinity
Infinity







side










surface









STO
Stop
Spherical
Infinity
−0.7471






S1 
First
Aspherical
2.2464
1.0091
Plastic
1.54
56.11
5.54


S2 
lens
Aspherical
7.4300
0.1410






S3 
Second
Aspherical
13.9437
0.3035
Plastic
1.67
19.24
−19.13


S4 
lens
Aspherical
6.6261
0.3047






S5 
Third
Aspherical
80.5962
0.2900
Plastic
1.67
19.24
−26.65


S6 
lens
Aspherical
14.6208
0.0431






S7 
Fourth
Aspherical
6.8944
0.4915
Plastic
1.52
56.74
13.16


S8 
lens
Aspherical
−450.4000
0.5195






S9 
Fifth
Aspherical
−17.6839
0.3519
Plastic
1.59
28.32
−38.72


S10
lens
Aspherical
−80.0072
0.2671






S11
Sixth
Aspherical
7.6040
0.8573
Plastic
1.59
28.32
12.06


S12
lens
Aspherical
−100.0238
0.4661






S13
Seventh
Aspherical
7.3849
0.7967
Plastic
1.54
55.75
−5.95


S14
lens
Aspherical
2.1405
0.4031






S15
Infrared
Spherical
Infinity
0.2100
Glass





S16
filter
Spherical
Infinity
0.5456






S17
Imaging
Spherical
Infinity
0.0000







surface












Note:


The reference wavelength = 587 nm.






Each parameter in Table 5a represents the same meaning as that in the optical system of FIG. 1a.


Table 5b shows higher-order coefficients that can be used for each aspherical lens surface in the optical system of FIG. 5a, where the surface profile of each aspherical lens surface can be defined by the formula given in the optical system of FIG. 1a.














TABLE 5b







Surface number
K
A4
A6
A8
A10





S1
−0.4870
0.0036
0.0090
−0.0148
0.0168


S2
−6.9169
−0.0168
0.0060
−0.0091
0.0188


S3
8.6198
−0.0334
0.0193
−0.0130
0.0264


S4
1.0318
−0.0175
0.0200
−0.0292
0.0746


S5
0.0000
−0.0250
0.0110
−0.0301
0.0458


S6
−18.0035
−0.0624
0.0352
−0.0016
−0.0558


S7
−11.9849
−0.0740
0.0568
−0.0630
0.0556


S8
−10.2850
−0.0179
−0.0088
0.0170
−0.0335


S9
2.0000
−0.0175
−0.0455
0.0590
−0.0423


S10
2.0000
0.0045
−0.0941
0.0975
−0.0614


S11
0.4460
0.0487
−0.0770
0.0516
−0.0256


S12
−17.7960
0.0448
−0.0203
0.0033
−0.0002


S13
−0.8143
−0.0851
0.0245
−0.0058
0.0011


S14
−1.4699
−0.0965
0.0323
−0.0083
0.0014





Surface number
A12
A14
A16
A18
A20





S1
−0.0116
0.0050
−0.0013
0.0002
0.0000


S2
−0.0215
0.0143
−0.0056
0.0012
−0.0001


S3
−0.0328
0.0227
−0.0091
0.0020
−0.0002


S4
−0.1132
0.1005
−0.0527
0.0152
−0.0018


S5
−0.0548
0.0473
−0.0270
0.0088
−0.0012


S6
0.0934
−0.0750
0.0328
−0.0075
0.0007


S7
−0.0321
0.0123
−0.0035
0.0007
−0.0001


S8
0.0373
−0.0246
0.0096
−0.0021
0.0002


S9
0.0154
−0.0016
−0.0006
0.0002
0.0000


S10
0.0247
−0.0062
0.0009
−0.0001
0.0000


S11
0.0086
−0.0019
0.0002
0.0000
0.0000


S12
0.0000
0.0000
0.0000
0.0000
0.0000


S13
−0.0001
0.0000
0.0000
0.0000
0.0000


S14
−0.0002
0.0000
0.0000
0.0000
0.0000










FIG. 5b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 5a. As illustrated in FIG. 5b, the optical system of FIG. 5a can have good imaging quality.


Referring to FIG. 6a and FIG. 6b, the optical system in this implementation includes, in order from an object side to an image side along an optical axis: a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6, and a seventh lens L7.


The first lens L1 has a positive refractive power. The object-side surface S1 of the first lens is convex near the optical axis, and the image-side surface S2 of the first lens is concave near the optical axis. The object-side surface S1 of the first lens is concave at the periphery, and the image-side surface S2 of the first lens is concave at the periphery. The second lens L2 has a negative refractive power. The object-side surface S3 of the second lens is convex near the optical axis, and the image-side surface S4 of the second lens is concave near the optical axis. The object-side surface S3 of the second lens is convex at the periphery, and the image-side surface S4 of the second lens is convex at the periphery. The third lens L3 has a positive refractive power. The object-side surface S5 of the third lens is convex near the optical axis, and the image-side surface S6 of the third lens is concave near the optical axis. The object-side surface S5 of the third lens is concave at the periphery, and the image-side surface S6 of the third lens is concave at the periphery. The fourth lens L4 has a positive refractive power. The object-side surface S7 of the fourth lens is concave near the optical axis, and the image-side surface S8 of the fourth lens is convex near the optical axis. The object-side surface S7 of the fourth lens is convex at the periphery, and the image-side surface S8 is a concave surface at the periphery. The fifth lens L5 has a negative refractive power. The object-side surface S9 of the fifth lens is concave near the optical axis, and the image-side surface S10 of the fifth lens is convex near the optical axis. The object-side surface S9 of the fifth lens is convex at the periphery, and the image-side surface S10 is convex at the periphery. The sixth lens L6 has a positive refractive power. The object-side surface S11 of the sixth lens is convex near the optical axis, and the image-side surface S12 of the sixth lens is concave near the optical axis. The object-side surface S11 of the sixth lens is convex at the periphery, and the image-side surface S12 is concave at the periphery. The seventh lens L7 has a negative refractive power. The object-side surface S13 of the seventh lens is convex near the optical axis, and the image-side surface S14 of the seventh lens is concave near the optical axis. The object-side surface S13 of the seventh lens is concave at the periphery, and the image-side surface S14 is convex at the periphery.


The other structures of the optical system of FIG. 6a are identical with the optical system of FIG. 1a, reference can be made to the optical system of FIG. 1a.


Table 6a shows characteristics of the optical system in this implementation. Data in Table 6a is obtained based on light of a wavelength of 587 nm. Y radius, thickness, and focal length are all in millimeters (mm).









TABLE 6a







Optical system of FIG. 6a


f = 5.90 mm, FNO = 1.75, FOV = 84.90°, TTL = 7.00 mm























Effective


Surface
Surface
Surface
Y


Refractive
Abbe
focal


number
name
type
Radius
Thickness
Material
index
number
length





OBJ
Object-
Spherical
Infinity
Infinity







side










surface









STO
Stop
Spherical
Infinity
−0.7383






S1 
First
Aspherical
2.2615
1.0041
Plastic
1.54
56.11
5.59


S2 
lens
Aspherical
7.4534
0.1038






S3 
Second
Aspherical
13.0069
0.3112
Plastic
1.67
19.24
−19.14


S4 
lens
Aspherical
6.4010
0.3151






S5 
Third
Aspherical
16.8642
0.2900
Plastic
1.67
19.24
422.84


S6 
lens
Aspherical
17.8055
0.1660






S7 
Fourth
Aspherical
−100.0421
0.5079
Plastic
1.52
56.74
26.26


S8 
lens
Aspherical
−11.9580
0.5490






S9 
Fifth
Aspherical
−25.2305
0.3500
Plastic
1.59
28.32
−94.42


S10
lens
Aspherical
−46.5181
0.1824






S11
Sixth
Aspherical
4.4488
0.6568
Plastic
1.59
28.32
61.72


S12
lens
Aspherical
4.7939
0.4922






S13
Seventh
Aspherical
4.7214
0.9234
Plastic
1.54
55.75
−9.74


S14
lens
Aspherical
2.3087
0.3925






S15
Infrared
Spherical
Infinity
0.2100
Glass





S16
filter
Spherical
Infinity
0.5456






S17
Imaging
Spherical
Infinity
0.0000







surface












Note:


The reference wavelength = 587 nm.






Each parameter in Table 6a represents the same meaning as that in the optical system of FIG. 1a.


Table 6b shows higher-order coefficients that can be used for each aspherical lens surface in the optical system of FIG. 6a, where the surface profile of each aspherical lens surface can be defined by the formula given in the optical system of FIG. 1a.














TABLE 6b







Surface number
K
A4
A6
A8
A10





S1
−0.4930
0.0033
0.0084
−0.0130
0.0139


S2
−8.1952
−0.0241
0.0048
0.0073
−0.0063


S3
10.0000
−0.0365
0.0224
−0.0033
0.0062


S4
2.9573
−0.0164
0.0274
−0.0465
0.1119


S5
0.0000
−0.0354
0.0151
−0.0474
0.0842


S6
−2.8665
−0.0267
−0.0143
0.0453
−0.0889


S7
3.8640
−0.0210
−0.0067
0.0005
0.0079


S8
−7.0454
−0.0245
0.0101
−0.0209
0.0157


S9
−18.0000
−0.0111
0.0156
−0.0304
0.0300


S10
2.0000
−0.0115
−0.0138
0.0161
−0.0106


S11
−2.8207
−0.0054
−0.0265
0.0208
−0.0118


S12
−7.3236
−0.0066
0.0024
−0.0032
0.0011


S13
−2.4607
−0.0966
0.0291
−0.0068
0.0012


S14
−1.4448
−0.0842
0.0255
−0.0060
0.0009





Surface number
A12
A14
A16
A18
A20





S1
−0.0090
0.0035
−0.0008
0.0001
0.0000


S2
0.0007
0.0019
−0.0014
0.0004
−0.0001


S3
−0.0142
0.0128
−0.0059
0.0014
−0.0001


S4
−0.1701
0.1520
−0.0798
0.0228
−0.0028


S5
−0.1054
0.0877
−0.0461
0.0138
−0.0018


S6
0.1021
−0.0692
0.0275
−0.0058
0.0005


S7
−0.0179
0.0190
−0.0105
0.0030
−0.0003


S8
−0.0052
−0.0007
0.0013
−0.0004
0.0001


S9
−0.0200
0.0083
−0.0021
0.0003
0.0000


S10
0.0037
−0.0007
0.0001
0.0000
0.0000


S11
0.0041
−0.0009
0.0001
0.0000
0.0000


S12
−0.0002
0.0000
0.0000
0.0000
0.0000


S13
−0.0001
0.0000
0.0000
0.0000
0.0000


S14
−0.0001
0.0000
0.0000
0.0000
0.0000










FIG. 6b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 6a. As illustrated in FIG. 6b, the optical system of FIG. 6a can have good imaging quality.


Referring to FIG. 7a and FIG. 7b, the optical system in this implementation includes, in order from an object side to an image side along an optical axis: a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6, and a seventh lens L7.


The first lens L1 has a positive refractive power. The object-side surface S1 of the first lens is convex near the optical axis, and the image-side surface S2 of the first lens is concave near the optical axis. The object-side surface S1 of the first lens is convex at the periphery, and the image-side surface S2 of the first lens is concave at the periphery. The second lens L2 has a negative refractive power. The object-side surface S3 of the second lens is convex near the optical axis, and the image-side surface S4 of the second lens is concave near the optical axis. The object-side surface S3 of the second lens is convex at the periphery, and the image-side surface S4 of the second lens is convex at the periphery. The third lens L3 has a negative refractive power. The object-side surface S5 of the third lens is concave near the optical axis, and the image-side surface S6 of the third lens is concave near the optical axis. The object-side surface S5 of the third lens is concave at the periphery, and the image-side surface S6 of the third lens is concave at the periphery. The fourth lens L4 has a positive refractive power. The object-side surface S7 of the fourth lens is convex near the optical axis, and the image-side surface S8 of the fourth lens is concave near the optical axis. The object-side surface S7 of the fourth lens is convex at the periphery, and the image-side surface S8 is a concave surface at the periphery. The fifth lens L5 has a negative refractive power. The object-side surface S9 of the fifth lens is concave near the optical axis, and the image-side surface S10 of the fifth lens is concave near the optical axis. The object-side surface S9 of the fifth lens is concave at the periphery, and the image-side surface S10 is convex at the periphery. The sixth lens L6 has a positive refractive power. The object-side surface S11 of the sixth lens is convex near the optical axis, and the image-side surface S12 of the sixth lens is concave near the optical axis. The object-side surface S11 of the sixth lens is convex at the periphery, and the image-side surface S12 is concave at the periphery. The seventh lens L7 has a negative refractive power. The object-side surface S13 of the seventh lens is convex near the optical axis, and the image-side surface S14 of the seventh lens is concave near the optical axis. The object-side surface S13 of the seventh lens is concave at the periphery, and the image-side surface S14 is convex at the periphery.


The other structures of the optical system of FIG. 7a are identical with the optical system of FIG. 1a, reference can be made to the optical system of FIG. 1a.


Table 7a shows characteristics of the optical system in this implementation. Data in Table 7a is obtained based on light of a wavelength of 587 nm. Y radius, thickness, and focal length are all in millimeters (mm).









TABLE 7a







Optical system of FIG. 7a


f = 5.88 mm, FNO = 1.69, FOV = 84.02°, TTL = 7.05 mm























Effective


Surface
Surface
Surface
Y


Refractive
Abbe
focal


number
name
type
Radius
Thickness
Material
index
number
length





OBJ
Object-
Spherical
Infinity
Infinity







side










surface









STO
Stop
Spherical
Infinity
−0.7748






S1 
First
Aspherical
2.3261
1.0151
Plastic
1.54
56.11
5.91


S2 
lens
Aspherical
7.1083
0.1357






S3 
Second
Aspherical
10.2099
0.2643
Plastic
1.67
19.24
−23.39


S4 
lens
Aspherical
6.1232
0.3730






S5 
Third
Aspherical
−61.0685
0.2900
Plastic
1.67
19.24
−21.94


S6 
lens
Aspherical
19.4491
0.0615






S7 
Fourth
Aspherical
7.1298
0.5083
Plastic
1.52
56.74
13.90


S8 
lens
Aspherical
1136.6270
0.6374






S9 
Fifth
Aspherical
−33.4699
0.3577
Plastic
1.59
28.32
−50.20


S10
lens
Aspherical
249.1381
0.1923






S11
Sixth
Aspherical
3.5998
0.7382
Plastic
1.59
28.32
14.52


S12
lens
Aspherical
5.7546
0.6185






S13
Seventh
Aspherical
5.4327
0.7308
Plastic
1.54
55.75
−7.50


S14
lens
Aspherical
2.1998
0.3717






S15
Infrared
Spherical
Infinity
0.2100
Glass





S16
filter
Spherical
Infinity
0.5456






S17
Imaging
Spherical
Infinity
0.0000







surface












Note:


The reference wavelength = 587 nm.






Each parameter in Table 7a represents the same meaning as that in the optical system of FIG. 1a.


Table 7b shows higher-order coefficients that can be used for each aspherical lens surface in the optical system of FIG. 7a, where the surface profile of each aspherical lens surface can be defined by the formula given in the optical system of FIG. 1a.














TABLE 7b







Surface number
K
A4
A6
A8
A10





S1
−0.4776
0.0028
0.0087
−0.0139
0.0154


S2
−6.0407
−0.0214
0.0062
−0.0005
0.0029


S3
−10.0000
−0.0408
0.0232
−0.0075
0.0130


S4
−0.3807
−0.0221
0.0226
−0.0221
0.0494


S5
0.0000
−0.0315
0.0273
−0.0466
0.0444


S6
−18.0000
−0.0771
0.0708
−0.0554
0.0050


S7
−16.1360
−0.0874
0.0751
−0.0726
0.0421


S8
−10.2850
−0.0228
−0.0048
0.0077
−0.0139


S9
2.0000
−0.0050
−0.0146
0.0127
−0.0067


S10
−18.0000
−0.0237
−0.0313
0.0371
−0.0228


S11
−4.0311
−0.0056
−0.0297
0.0232
−0.0129


S12
−5.3966
0.0082
−0.0069
−0.0001
0.0005


S13
−2.1595
−0.1036
0.0295
−0.0060
0.0009


S14
−1.3568
−0.0997
0.0313
−0.0076
0.0012





Surface number
A12
A14
A16
A18
A20





S1
−0.0104
0.0044
−0.0011
0.0002
0.0000


S2
−0.0050
0.0038
−0.0016
0.0004
0.0000


S3
−0.0185
0.0134
−0.0054
0.0011
−0.0001


S4
−0.0718
0.0594
−0.0286
0.0075
−0.0008


S5
−0.0271
0.0105
−0.0028
0.0007
−0.0001


S6
0.0393
−0.0409
0.0197
−0.0047
0.0005


S7
−0.0064
−0.0080
0.0057
−0.0015
0.0002


S8
0.0142
−0.0086
0.0031
−0.0006
0.0001


S9
0.0009
0.0006
−0.0003
0.0001
0.0000


S10
0.0083
−0.0018
0.0002
0.0000
0.0000


S11
0.0045
−0.0009
0.0001
0.0000
0.0000


S12
−0.0001
0.0000
0.0000
0.0000
0.0000


S13
−0.0001
0.0000
0.0000
0.0000
0.0000


S14
−0.0001
0.0000
0.0000
0.0000
0.0000










FIG. 7b illustrates the longitudinal spherical aberration curve, the astigmatic field curve, and the distortion curve of the optical system of FIG. 7a. As illustrated in FIG. 7b, the optical system of FIG. 7a can have good imaging quality.


Table 8 shows values of TTL/Imgh, f/R14, FNO, TTL/f, f1/f2, sag1/sag2, (R2+R1)/(R2−R1), f1234/f567 of the optical systems of FIGS. 1a, 2a, 3a, 4a, 5a, 6a, 7a.













TABLE 8








TTL/Imgh
f/R14
FNO
TTL/f





Optical system of FIG. 1a
1.27
2.63
1.75
1.18


Optical system of FIG. 2a
1.27
2.57
1.78
1.19


Optical system of FIG. 3a
1.27
2.61
1.75
1.19


Optical system of FIG. 4a
1.27
2.67
1.75
1.19


Optical system of FIG. 5a
1.27
2.76
1.75
1.19


Optical system of FIG. 6a
1.27
2.56
1.75
1.19


Optical system of FIG. 7a
1.28
2.67
1.69
1.20








(R2 + R1)/
f1234/



f1/f2
sag1/sag2
(R2 − R1)
f567





Optical system of FIG. 1a
−0.26
7.18
2.00
−0.26


Optical system of FIG. 2a
−0.31
7.61
1.87
−0.31


Optical system of FIG. 3a
−0.27
7.40
1.94
−0.27


Optical system of FIG. 4a
−0.25
7.31
1.98
−0.25


Optical system of FIG. 5a
−0.29
7.90
1.87
−0.29


Optical system of FIG. 6a
−0.29
8.11
1.87
−0.29


Optical system of FIG. 7a
−0.25
7.15
1.97
−0.25









It can be seen from table 8 that each optical systems according to each implementation satisfies the following expressions: TTL/Imgh<1.32, 2<f/R14<3.5, FNO≤2, TTL/f<1.35, f1/f2>−0.15, sag1/sag2<15, (R2+R1)/(R2−R1)<5, f1234/f567>−0.5.


The technical features of the implementations of the present disclosure can be combined. For brief description, not all possible combinations of the various technical features in the implementations of the present disclosure are described herein. However, as long as there is no conflict in the combination of these technical features, such combination should be considered within the scope of the present disclosure.


Only some implementations of the present disclosure are described in detail herein, which should not be understood as a limitation on the scope of the present disclosure. It should be noted that, for those of ordinary skill in the art, without departing from the concept of the present disclosure, modifications and improvements can be made and should be considered within the scope of the present disclosure. Therefore, the scope of the present disclosure should be subject to the appended claims.

Claims
  • 1. An optical system comprising, in order from an object side to an image side along an optical axis: a first lens with a positive refractive power, wherein the first lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis;a second lens with a negative refractive power, wherein the second lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis;a third lens with a refractive power;a fourth lens with a positive refractive power;a fifth lens with a refractive power;a sixth lens with a refractive power, wherein the sixth lens has an object-side surface which is concave near the optical axis; anda seventh lens with a negative refractive power, wherein the seventh lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis;wherein each of the first lens to the seventh lens has an aspherical object-side surface and an aspherical image-side surface, and the optical system satisfies the following expression: TTL/Imgh<1.32;wherein TTL represents a distance from the object-side surface of the first lens to an imaging surface of the optical system along the optical axis, and Imgh represents half of a length of a diagonal of an effective pixel area of the imaging surface.
  • 2. The optical system of claim 1, wherein the optical system satisfies the following expression: 2<f/R14<30.5;wherein f represents an effective focal length of the optical system, and R14 represents a radius of curvature of the image-side surface of the seventh lens at the optical axis.
  • 3. The optical system of claim 1, wherein the optical system satisfies the following expression: FNO≤2;wherein FNO represents an F-number of the optical system.
  • 4. The optical system of claim 1, wherein the optical system satisfies the following expression: TTL/f<1.35;wherein TTL represents the distance from the object-side surface of the first lens to the imaging surface of the optical system along the optical axis, and f represents an effective focal length of the optical system.
  • 5. The optical system of claim 1, wherein the optical system satisfies the following expression: f1/f2>−0.15;wherein f1 represents an effective focal length of the first lens, and f2 represents an effective focal length of the second lens.
  • 6. The optical system of claim 1, wherein the optical system satisfies the following expression: sag1/sag2<15;wherein sag1 represents a saggital depth at an effective aperture of the object-side surface of the first lens, and sag2 represents a saggital depth at an effective aperture of the image-side surface of the first lens.
  • 7. The optical system of claim 1, wherein the optical system satisfies the following expression: (R2+R1)/(R2−R1)<5;wherein R1 represents a radius of curvature of the object-side surface of the first lens, and R2 represents a radius of curvature of the image-side surface of the first lens.
  • 8. The optical system of claim 1, wherein the optical system satisfies the following expression: f1234/f567>−0.5;wherein f1234 represents a combined focal length of the first lens to the fourth lens, and f567 represents a combined focal length of the fifth lens to the seventh lens.
  • 9. A lens module, comprising: a lens barrel;an electronic photosensitive element; andan optical system comprising, in order from an object side to an image side along an optical axis: a first lens with a positive refractive power, wherein the first lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis;a second lens with a negative refractive power, wherein the second lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis;a third lens with a refractive power;a fourth lens with a positive refractive power;a fifth lens with a refractive power;a sixth lens with a refractive power, wherein the sixth lens has an object-side surface which is concave near the optical axis; anda seventh lens with a negative refractive power, wherein the seventh lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis;wherein each of the first lens to the seventh lens has an aspherical object-side surface and an aspherical image-side surface, and the optical system satisfies the following expression: TTL/Imgh<1.32;wherein TTL represents a distance from the object-side surface of the first lens to an imaging surface of the optical system along the optical axis, and Imgh represents half of a length of a diagonal of an effective pixel area of the imaging surface; andwherein the first lens to the seventh lens of the optical system are disposed in the lens barrel, and the electronic photosensitive element is disposed on the image side of the optical system and configured to convert light passing through the first lens to the seventh lens and incident on the electronic photosensitive element into an electrical signal of an image.
  • 10. The lens module of claim 9, wherein the optical system satisfies the following expression: 2<f/R14<3.5;wherein f represents an effective focal length of the optical system, and R14 represents a radius of curvature of the image-side surface of the seventh lens at the optical axis.
  • 11. The lens module of claim 9, wherein the optical system satisfies the following expression: FNO≤2;wherein FNO represents an F-number of the optical system.
  • 12. The lens module of claim 9, wherein the optical system satisfies the following expression: TTL/f<1.35;wherein TTL represents the distance from the object-side surface of the first lens to the imaging surface of the optical system along the optical axis, and f represents an effective focal length of the optical system.
  • 13. The lens module of claim 9, wherein the optical system satisfies the following expression: f1/f2>−0.15;wherein f1 represents an effective focal length of the first lens, and f2 represents an effective focal length of the second lens.
  • 14. The lens module of claim 9, wherein the optical system satisfies the following expression: sag1/sag2<15;wherein sag1 represents a saggital depth at an effective aperture of the object-side surface of the first lens, and sag2 represents a saggital depth at an effective aperture of the image-side surface of the first lens.
  • 15. The lens module of claim 9, wherein the optical system satisfies the following expression: (R2+R1)/(R2−R1)<5;wherein R1 represents a radius of curvature of the object-side surface of the first lens, and R2 represents a radius of curvature of the image-side surface of the first lens.
  • 16. The lens module of claim 9, wherein the optical system satisfies the following expression: f1234/f567>−0.5;wherein f1234 represents a combined focal length of the first lens to the fourth lens, and f567 represents a combined focal length of the fifth lens to the seventh lens.
  • 17. An electronic device, comprising: a housing; anda lens module received in the housing, wherein the lens module comprising: a lens barrel;an electronic photosensitive element; andan optical system comprising, in order from an object side to an image side along an optical axis: a first lens with a positive refractive power, wherein the first lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis;a second lens with a negative refractive power, wherein the second lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis;a third lens with a refractive power;a fourth lens with a positive refractive power;a fifth lens with a refractive power;a sixth lens with a refractive power, wherein the sixth lens has an object-side surface which is concave near the optical axis; anda seventh lens with a negative refractive power, wherein the seventh lens has an object-side surface which is convex near the optical axis and an image-side surface which is concave near the optical axis;wherein each of the first lens to the seventh lens has an aspherical object-side surface and an aspherical image-side surface, and the optical system satisfies the following expression: TTL/Imgh<1.32;wherein TTL represents a distance from the object-side surface of the first lens to an imaging surface of the optical system along the optical axis, and Imgh represents half of a length of a diagonal of an effective pixel area of the imaging surface; andwherein the first lens to the seventh lens of the optical system are disposed in the lens barrel, and the electronic photosensitive element is disposed on the image side of the optical system and configured to convert light passing through the first lens to the seventh lens and incident on the electronic photosensitive element into an electrical signal of an image.
  • 18. The electronic device of claim 17, wherein the optical system satisfies the following expression: 2<f/R14<30.5;wherein f represents an effective focal length of the optical system, and R14 represents a radius of curvature of the image-side surface of the seventh lens at the optical axis.
  • 19. The electronic device of claim 17, wherein the optical system satisfies the following expression: FNO≤2;wherein FNO represents an F-number of the optical system.
  • 20. The electronic device of claim 17, wherein the optical system satisfies the following expression: TTL/f<1.35;wherein TTL represents the distance from the object-side surface of the first lens to the imaging surface of the optical system along the optical axis, and f represents an effective focal length of the optical system.
CROSS-REFERENCE TO RELATED APPLICATIONS

The present application is a continuation of International Application No. PCT/CN2020/088513, filed on Apr. 30, 2020, the disclosure of which is hereby incorporated by reference in its entirety.

Continuations (1)
Number Date Country
Parent PCT/CN2020/088513 Apr 2020 US
Child 17462798 US