USPatent applicationPatented

Optical lens assembly, image capturing module, and mobile terminal

Granted 24 Dec 2024 · 1 office action

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Abstract

An optical lens assembly, sequentially comprising from an object side to an image side: a first lens; a second lens having positive refractive power, the object side surface of the second lens being concave at the circumference, and the image side surface of the second lens being convex at the circumference; a third lens; and a fourth lens having positive refractive power, the image side surface of the fourth lens being concave at the optical axis, the object side surface and the image side surface of the fourth lens being aspherical, and at least one of the object side surface and the image side surface of the fourth lens having an inflection point. The optical lens assembly satisfies relationship: TT/f<1.3, TT is the distance on the optical axis from the object side surface of the first lens to the image side surface of the fourth lens, and f is effective focal length.

Description

14 parts
›CROSS REFERENCE TO RELATED APPLICATION

This application is a national stage application, filed under 35 U.S.C. § 371, of International Patent Application No. PCT/CN2019/091801, filed 19 Jun. 2019, which claims priority to Chinese Patent Application No. 2019103646988, filed on Apr. 30, 2019.

›TECHNICAL FIELD

The present disclosure relates to the field of optical imaging, in particular to an optical lens assembly, an image capturing module, and a mobile terminal.

›BACKGROUND

With the rapid development of recognition technology (structured light and Time of flight (TOF)), as well as the mass production of photosensitive elements that support the recognition technology, the application fields of the recognition technology will become very extensive, such as face unlocking on mobile phones, automatic drive on cars, human-machine interfaces and games, industrial machine vision and measurement, security monitoring, and the like.

A lens assembly used to collect light, which is indispensable in the recognition technology, is also particularly important. For electronic devices that pursue high screen-to-body ratio and small thickness, how to make the size of the recognition lens assembly smaller to reduce the space occupied by the lens assembly in the electronic device is also a matter of great concern.

›SUMMARY

According to various embodiments of the present disclosure, an optical lens assembly, an image capturing module, and a mobile terminal are provided.

An optical lens assembly sequentially includes from an object side to an image side:

a first lens with a refractive power;

a second lens with a positive refractive power, an object side surface of the second lens is concave at a circumference thereof, and an image side surface of the second lens being convex at a circumference thereof;

a third lens with a refractive power;

a fourth lens with a positive refractive power, an image side surface of the fourth lens is concave at an optical axis, an object side surface and the image side surface of the fourth lens are aspherical, and at least one of the object side surface and the image side surface of the fourth lens has an inflection point;

the optical lens assembly satisfies the following relationship:

TT/f< 1.3;

where, TT is a distance on the optical axis from an object side surface of the first lens to the image side surface of the fourth lens, and f is an effective focal length of the optical lens assembly.

An image capturing module includes a photosensitive element and the optical lens assembly of any one of the above embodiments, the photosensitive element is disposed on an image side of the optical lens assembly.

A mobile terminal includes an emitting module and the image capturing module of the above embodiment. The emitting module is capable of emitting modulated light to a measured object, the modulated light is reflected on a surface of the measured object to form an information light carrying information of the surface of the measured object, and the image capturing module is capable of receiving the information light reflected from the measured object.

The details of one or more embodiments of the present disclosure are set forth in the accompanying drawings and the description below. Other features, objects and advantages of the present disclosure will become apparent from the description, the accompanying drawings, and the claims.

›BRIEF DESCRIPTION OF THE DRAWINGS

To better describe and illustrate embodiments and/or examples of the disclosure disclosed herein, reference can be made to one or more accompanying drawings. The additional details or examples used to describe the accompanying drawings should not be construed as limiting the scope of any of the disclosed disclosure, the presently described embodiments and/or examples, and the presently understood preferred mode of the disclosure.

FIG. 1 is a schematic view of an optical lens assembly provided by a first embodiment of the present disclosure.

FIG. 2 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly in the first embodiment.

FIG. 3 is a schematic view of an optical lens assembly provided by a second embodiment of the present disclosure.

FIG. 4 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly in the second embodiment.

FIG. 5 is a schematic view of an optical lens assembly provided by a third embodiment of the present disclosure.

FIG. 6 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly in the third embodiment.

FIG. 7 is a schematic view of an optical lens assembly provided by a fourth embodiment of the present disclosure.

FIG. 8 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly in the fourth embodiment.

FIG. 9 is a schematic view of an optical lens assembly provided by a fifth embodiment of the present disclosure.

FIG. 10 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly in the fifth embodiment.

FIG. 11 is a schematic view of an optical lens assembly provided by a sixth embodiment of the present disclosure.

FIG. 12 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly in the sixth embodiment.

FIG. 13 is a schematic view of an optical lens assembly provided by a seventh embodiment of the present disclosure.

FIG. 14 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly in the seventh embodiment.

FIG. 15 is a schematic view of an image capturing module provided by an embodiment of the present disclosure.

FIG. 16 is a schematic view of a mobile terminal provided by an embodiment of the present disclosure.

›DETAILED DESCRIPTION OF THE EMBODIMENTS · 1 of 9

In order to facilitate the understanding of the present disclosure, the present disclosure will be described more fully hereinafter with reference to the related accompanying drawings. Preferable embodiments of the present disclosure are presented in the accompanying drawings. However, the present disclosure may be embodied in many different forms and is not limited to the embodiments described herein. Rather, the purpose of providing these embodiments is to make the content of the present disclosure more thorough and comprehensive.

It should be noted that when an element is referred to as being “fixed to” another element, it can be directly fixed to another element or indirectly connected to another element with a mediating element. When an element is considered to be “connected to” another element, it can be directly connected to another element or indirectly connected to another element with a mediating element. The terms “in”, “outer”, “left””, “right”, and the like used herein are for illustrative purposes only and are not intended to be the only embodiments.

The optical lens assembly with miniaturization characteristics provided by the present disclosure can be applied to face unlocking on mobile phones, automatic drive on cars, human-machine interfaces and games, industrial machine vision and measurement, security monitoring, and the like.

Referring to FIG. 1 , an optical lens assembly 110 in an embodiment of the present disclosure includes, sequentially arranged from an object side to an image side, a first lens L 1 with a refractive power, a second lens L 2 with a positive refractive power, a third lens L 3 with a refractive power, and a fourth lens L 4 with a positive refractive power.

The first lens L 1 includes an object side surface S 1 and an image side surface S 2 ; the second lens L 2 includes an object side surface S 3 and an image side surface S 4 ; the third lens L 3 includes an object side surface S 5 and an image side surface S 6 ; and the fourth lens L 4 includes an object side surface S 7 and an image side surface S 8 . In addition, the optical lens assembly 110 includes an imaging plane S 11 located on the image side of the fourth lens L 4 . The imaging plane S 11 may be a photosensitive surface of a photosensitive element. A light ray carrying information of captured object is imaged on the imaging plane S 11 after being adjusted by all the lenses.

The object side surface S 3 of the second lens L 2 is concave at the circumference thereof, and the image side surface S 4 of the second lens L 2 is convex at the circumference thereof. The image side surface S 8 of the fourth lens L 4 is concave at an optical axis, and the object side surface S 7 and the image side surface S 8 of the fourth lens L 4 are both aspherical. At least one of the object side surface S 7 and the image side surface S 8 of the fourth lens L 4 has at least one inflection point, that is, at least one of the object side surface S 7 and the image side surface S 8 of the fourth lens L 4 has an inflection point.

It should be noted that, when describing that a side surface of a lens is convex at the optical axis (a central area of the side surface), it can be understood as that an area of the side surface of the lens near the optical axis is convex, and thus it can also be considered as that the side surface is convex at a paraxial position thereof. When describing that a side surface of a lens is concave at the circumference thereof, it can be understood that an area of the side surface near the maximum effective radius is concave. For example, when the side surface is convex at the optical axis and also convex at the circumference thereof, the shape of the side surface in a direction from the center (the optical axis) to the edge may be completely convex, or the side surface may be firstly transited from a convex shape at the center to a concave shape, and then become a convex surface at a position close to its maximum effective radius. This is only an example to illustrate the relationship between the optical axis and the circumference. The various shapes and structures (concave-convex relationship) of the side surface are not fully described, but other situations can be derived from the above examples.

In some embodiments, the first lens L 1 and the third lens L 3 each have positive refractive power, so as to facilitate shortening the total length of the system. In some embodiments, the first lens L 1 and the third lens L 3 each have negative refractive power, so as to facilitate enlarging the field of view of the system. In some other embodiments, the first lens L 1 has a positive refractive power, and the third lens L 3 has a negative refractive power, so that the system can achieve a balance between a short total length and a large field of view.

In addition, it should be noted that, the system or optical system described in the present disclosure may be composed of optical elements such as an optical lens assembly 110 , a prism, and a filter.

In some embodiments, the first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are made of plastic. In this case, the plastic lens can reduce the weight of the optical lens assembly 110 and reduce the production cost. In some embodiments, the first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are made of glass. In this case, the optical lens assembly 110 can withstand higher temperatures and has better optical performance In some other embodiments, it is also can be that only the first lens L 1 is made of glass and the other lenses are made of plastic. In this case, the first lens L 1 , which is closest to the object side, can well withstand the influence of the ambient temperature on the object side, and since the other lenses are made of plastic, the optical lens assembly 110 can also maintain a relatively low production cost. It should be noted that, according to actual requirements, the first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 may be made of any one of plastic or glass, which is not limited here.

›DETAILED DESCRIPTION OF THE EMBODIMENTS · 2 of 9

In some embodiments, the optical lens assembly 110 is further provided with an optical stop STO therein. In some embodiments, the optical stop STO is arranged on the object side of the first lens L 1 . In some other embodiments, the optical stop STO may be arranged between the first lens L 1 and the fourth lens L 4 , and specifically may be between the first lens L 1 and the second lens L 2 .

In some embodiments, an infrared band pass filter L 5 is arranged at the image side of the fourth lens L 4 . The infrared band pass filter L 5 is arranged between the fourth lens L 4 and the imaging plane S 11 . The infrared band pass filter L 5 can allow infrared light at a specific wavelength band to pass through, and block interference light at other wavelength bands, so as to prevent the interference light from being received by the photosensitive element and affecting normal imaging, thereby improving the imaging quality (such as recognition accuracy) of the optical lens assembly 110 . It should be noted that, in some other embodiments, the infrared band pass filter L 5 is not arranged in the optical lens assembly 110 , but is assembled at the image side of the optical lens assembly 110 along with the photosensitive element when the optical lens assembly 110 is assembled with the photosensitive element.

When the optical lens assembly 110 is used to receive infrared light at a specific wavelength, an antireflection film may be arranged on the surface of each lens or on the surface of infrared band pass filter L 5 to increase the transmittance of infrared light at the corresponding wavelength.

In some embodiments, the object side surfaces and the image side surfaces of the first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are aspherical surfaces. The aspherical surface has a surface shape equation as follows:

Where, Z is a distance from a corresponding point on the aspherical surface to a plane tangent to a vertex of the surface, r is a distance from the corresponding point on the aspherical surface to the optical axis, c is a curvature of the aspherical surface vertex, k is a conic constant, and Ai is a coefficient corresponding to a high-order term of the i-th term in the surface shape equation of the aspherical surface.

In some embodiments, the optical lens assembly 110 satisfies the following relationships:

TT/f< 1.3;

Where, TT is a distance on the optical axis from the object side surface S 1 of the first lens L 1 to the image side surface S 8 of the fourth lens L 4 , and f is an effective focal length of the optical lens assembly 110 . Specifically, TT/f may be 0.920, 0.930, 0.950, 0.970, 0.990, 1.000, or 1.100. Further, in some embodiments, TT/f≤1.10. When the optical lens assembly 110 satisfies the above relationship, the focal length of the optical lens assembly 110 and a length on the optical axis from the first lens L 1 to the fourth lens L 4 can be reasonably controlled, so that not only the miniaturization of the optical lens assembly 110 can be achieved, but also the light ray can be better converged on the imaging plane S 11 .

0.35 mm< T 12+ T 23+ T 34<0.85 mm;

Where, T12 is an air gap on the optical axis between the first lens L 1 and the second lens L 2 , T23 is an air gap on the optical axis between the second lens L 2 and the third lens L 3 , and T34 is an air gap on the optical axis between the third lens L 3 and the fourth lens L 4 . Specifically, T12+T23+T34 may be 0.430, 0.470, 0.520, 0.570, 0.610, 0.650, 0.680, 0.710, or 0.730, in numerical units of mm. When the configuration of the spacings between adjacent lenses satisfies the above relationship, it will be conducive to the assembly of the lenses and can further shorten the total length of the system. When T12+T23+T34<0.35 mm, space allowance for distributing the spacings between the lenses is too small, so that the sensitivity of the optical system is increased and the assembly of the lenses is not facilitated. When T12+T23+T34≥0.85 mm, it is not conducive to the miniaturization design of the optical lens assembly 110 .

1.0< f 2/ f 4<2.5;

Where, f2 is a focal length of the second lens L 2 , and f4 is a focal length of the fourth lens L 4 . Specifically, f2/f4 may be 1.20, 1.40, 1.60, 1.80, 1.90, or 2.00. When the above relationship is satisfied, positive refractive powers can be reasonably distributed among the second lens L 2 and the fourth lens L 4 , so as to balance the spherical aberration generated by the third lens L 3 , reduce the tolerance sensitivity of the system, and improve the imaging quality of the system. When f2/f4≤1.0, the fourth lens L 4 needs to provide most of the positive refractive power, which may cause the object side surface S 7 of the fourth lens L 4 to be excessively curved and poor molded, and thereby affecting the manufacturing yield. When f2/f4≥2.5, the distribution of the refractive powers among the second lens L 2 and the fourth lens L 4 is unbalanced, resulting in excessive aberration of the optical system that is difficult to be corrected.

FNO≤ 1.3;

Where, FNO is an f-number of the optical lens assembly 110 . Specifically, the FNO may be 1.13, 1.17, 1.21, 1.23, 1.25, 1.27, or 1.29. When the above relationship is satisfied, the amount of light passing through the optical lens assembly 110 can be increased, and the optical lens assembly 110 can also obtain clear and detailed information of the measured object in a dark environment or under the condition of insufficient light, thereby improving the imaging quality.

In some embodiments, the optical lens assembly 110 includes an optical stop, and the optical stop STO is arranged at the object side of the first lens L 1 or between the first lens L 1 to the fourth lens L 4 , and the optical lens assembly 110 satisfies the following relationships:

0.8< SL/TTL< 1.1;

Where, SL is a distance on the optical axis from the optical stop STO to the imaging plane S 11 of the optical lens assembly 110 , and TTL is a distance on the optical axis from the object side surface S 1 of the first lens L 1 to the imaging plane S 11 of the optical lens assembly 110 . Specifically, the SL/TTL may be 0.830, 0.850, 0.870, 0.890, 0.910, 0.930, 0.950, or 0.970. When the position of the optical stop STO satisfies the above configuration relationship, the system can achieve a better balance between the characteristics of short total length and large field of view.

›DETAILED DESCRIPTION OF THE EMBODIMENTS · 3 of 9

FFL> 0.7 mm;

Where, FFL is a closest distance from the image side surface S 8 of the fourth lens L 4 to the imaging plane S 11 of the optical lens assembly 110 in a direction of the optical axis. Specifically, FFL may be 0.75, 0.78, 0.81, 0.84, 0.87, or 0.90, in numerical units of mm. When the fourth lens L 4 satisfies the above relationship, it can be ensured that the optical lens assembly 110 has sufficient focusing space during the installation of the module, thereby improving the assembly yield of the module, and in addition, the depth of focus of the optical lens assembly 110 can be widened to obtain more depth information on the object side.

R 8/ R 9<1.0;

Where, R8 is a radius of curvature of the object side surface S 7 of the fourth lens L 4 at the paraxial position, and R9 is a radius of curvature of the image side surface S 8 of the fourth lens L 4 at the paraxial position. Specifically, R8/ R9 may be 0.680, 0.690, 0.730, 0.760, 0.780, 0.810, 0.830, 0.860, or 0.890. When the above relationship is satisfied, the radiuses of curvature of the object side surface S 7 and the image side surface S 8 of the fourth lens L 4 at the paraxial position can be appropriately configured, thereby increasing the workability of the shape of the fourth lens L 4 , and in addition, improving the coma of the optical lens assembly 110 and avoiding other aberrations from being too large.

0.2< R 4/ f 2<0.6;

Where, R4 is a radius of curvature of the object side surface S 3 of the second lens L 2 at the paraxial position, and f2 is a focal length of the second lens L 2 . Specifically, R4/f2 may be 0.240, 0.270, 0.300, 0.330, 0.360, 0.390, 0.420, 0.450, 0.510, or 0.520. When the above relationship is satisfied, the object side surface S 3 of the second lens L 2 has an appropriate radius of curvature on the optical axis, which is beneficial to correct the aberrations. When R2/f2≤0.2, the positive refractive power provided by the second lens L 2 is insufficient, resulting in excessive spherical aberration of the system. When R4/f2≥0.6, the edge of the lens aperture of the second lens L 2 will be excessively recurved, resulting in an increase in stray light of the optical lens assembly 110 and affecting the imaging quality.

First Embodiment

In the first embodiment as shown FIG. 1 , an optical lens assembly 110 includes, sequentially arranged from an object side to an image side, a first lens L 1 with a positive refractive power, an optical stop STO, a second lens L 2 with a positive refractive power, a third lens L 3 with a negative refractive power, and a fourth lens L 4 with a positive refractive power. FIG. 2 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly 110 in the first embodiment, where the astigmatism diagram and the distortion diagram are data diagrams at a reference wavelength.

The object side surface S 1 of the first lens L 1 is convex at the optical axis, the image side surface S 2 of the first lens L 1 is concave at the optical axis; the object side surface S 1 of the first lens L 1 is convex at the circumference thereof, and the image side surface S 2 of the first lens L 1 is convex at the circumference thereof. The object side surface S 3 of the second lens L 2 is convex at the optical axis, the image side surface S 4 of the second lens L 2 is concave at the optical axis; the object side surface S 3 of the second lens L 2 is concave at the circumference thereof, and the image side surface S 4 of the second lens L 2 is convex at the circumference thereof. The object side surface S 5 of the third lens L 3 is concave at the optical axis, the image side surface S 6 of the third lens L 3 is concave at the optical axis; the object side surface S 5 of the third lens L 3 is concave at the circumference thereof, and the image side surface S 6 of the third lens L 3 is concave at the circumference thereof. The object side surface S 7 of the fourth lens L 4 is convex at the optical axis, the image side surface S 8 of the fourth lens L 4 is concave at the optical axis; the object side surface S 7 of the fourth lens L 4 is concave at the circumference thereof, and the image side surface S 8 of the fourth lens L 4 is convex at the circumference thereof.

The object side surfaces and the image side surfaces of the first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are aspherical. The aspherical design can solve the problem of distortion of the field of view, and can also enable the lenses to be smaller, thinner, and flatter while achieving good optical effects, thereby enabling the optical lens assembly 110 to have a smaller volume.

The first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are made of plastic. The plastic lens can reduce the weight of the optical lens assembly 110 and reduce the production cost.

In addition, an infrared band pass filter L 5 is further disposed on the image side of the fourth lens L 4 . The infrared band pass filter L 5 can allow infrared light at a specific wavelength band to pass through, and block interference light at other wavelength bands, so as to prevent the interference light from being received by the photosensitive element and affecting normal imaging, thereby improving the imaging quality of the optical lens assembly 110 .

The optical lens assembly 110 in the first embodiment satisfies the following relationships:

TT/f=0.998; Where, TT is a distance on the optical axis from the object side surface S 1 of the first lens L 1 to the image side surface S 8 of the fourth lens L 4 , and f is an effective focal length of the optical lens assembly 110 . When the above relationship is satisfied, the effective focal length of the optical lens assembly 110 and the total length on the optical axis between the first lens L 1 and the fourth lens L 4 can be reasonably controlled, which can not only realize the miniaturization of the optical lens assembly 110 , but also ensure that the light ray is better converged on the imaging plane S 11 .

›DETAILED DESCRIPTION OF THE EMBODIMENTS · 4 of 9

T12+T23+T34=0.739; Where, T12 is an air gap on the optical axis between the first lens L 1 and the second lens L 2 , T23 is an air gap on the optical axis between the second lens L 2 and the third lens L 3 , and T34 is an air gap on the optical axis between the third lens L 3 and the fourth lens L 4 . When the configuration of the spacings between the lenses satisfies the above relationship, it will be conducive to the assembly of the lenses and can further shorten the total length of the system. When T12+T23+T34≤0.35, space allowance for distributing the spacings between the lenses is too small, so that the sensitivity of the optical system is increased and the assembly of the lenses is not facilitated. When T12+T23+T34≥0.85, it is not conducive to the miniaturization of the optical lens assembly 110 .

f2/f4=1.37; Where, f2 is a focal length of the second lens L 2 , and f4 is a focal length of the fourth lens L 4 . When the above relationship is satisfied, positive refractive powers can be reasonably distributed among the second lens L 2 and the fourth lens L 4 , so as to balance the spherical aberration generated by the third lens L 3 , reduce the tolerance sensitivity of the system, and improve the imaging quality of the system. When f2/f4≤1.0, the fourth lens L 4 needs to provide most of the positive refractive power, which may cause the object side surface S 7 of the fourth lens L 4 to be excessively curved and poor molded, and thereby affecting the manufacturing yield. When f2/f4≥2.5, the distribution of the refractive powers among the second lens L 2 and the fourth lens L 4 is unbalanced, resulting in excessive aberration of the optical system that is difficult to be corrected.

FNO=1.3; Where, FNO is an f-number of the optical lens assembly 110 . When the above relationship is satisfied, the amount of light passing through the optical lens assembly 110 can be increased, and the optical lens assembly 110 can also obtain clear and detailed information of the measured object in a dark environment or under the condition of insufficient light, thereby improving the imaging quality.

SL/TTL=0.823; Where, SL is a distance on the optical axis from the optical stop STO to the imaging plane S 11 , and TTL is a distance on the optical axis from the object side surface S 1 of the first lens L 1 to the imaging plane S 11 . When the position of the optical stop STO satisfies the above configuration relationship, the system can achieve a better balance between the characteristics of short total length and large field of view.

FFL=0.74; where FFL is a closest distance from the image side surface S 8 of the fourth lens L 4 to the imaging plane S 11 in the direction of the optical axis, and the unit of FFL is mm. When the fourth lens L 4 satisfies the above relationship, it can be ensured that the optical lens assembly 110 has sufficient focusing space during the installation of the module, thereby improving the assembly yield of the module, and in addition, the depth of focus of the optical lens assembly 110 can be widened, so as to obtain more depth information on the object side.

R8/ R9=0.821; Where, R8 is a radius of curvature of the object side surface S 7 of the fourth lens L 4 at the paraxial position, and R9 is a radius of curvature of the image side surface S 8 of the fourth lens L 4 at the paraxial position. When the above relationship is satisfied, the radiuses of curvature of the object side surface S 7 and the image side surface S 8 of the fourth lens L 4 at the paraxial position can be appropriately configured, thereby increasing the workability of the shape of the fourth lens L 4 , and in addition, improving the coma of the optical lens assembly 110 and avoiding other aberrations from being too large.

R4/f2=0.233; Where, R4 is a radius of curvature of the object side surface S 3 of the second lens L 2 at the paraxial position, and f2 is a focal length of the second lens L 2 . When the above relationship is satisfied, the object side surface S 3 of the second lens L 2 has an appropriate radius of curvature on the optical axis, which is beneficial to correct the aberrations.

In addition, various parameters of the optical lens assembly 110 are given in Table 1 and Table 2. The elements from the object plane to the imaging plane S 11 are arranged in the order of the elements from top to bottom in Table 1. The surface numbers 2 and 3 in Table 1 are the object side surface S 1 and the image side surface S 2 of the first lens L 1 , respectively. That is, in one same lens, a surface with a smaller surface number is an object side surface, and a surface with a larger surface number is an image side surface. The Y radius is a radius of curvature of an object side surface or an image side surface of a corresponding surface number at the paraxial position. The first value in the “thickness” parameter column of the first lens L 1 is a thickness on the optical axis of the lens, and the second value therein is a distance on the optical axis from the image side surface of the lens to the object side surface of the subsequent lens. The value corresponding to the surface number 11 of the infrared band pass filter L 5 in the “thickness” parameter is a distance from the image side surface S 10 of the infrared band pass filter L 5 to the imaging plane S 11 . K in Table 2 is a conic constant, and Ai is a coefficient corresponding to a high-order term of the i-th term in the surface shape equation of the aspherical surface.

In addition, the refractive index, Abbe number, and focal length of each lens are values at the reference wavelength. The calculation of the relational expression is based on the lens parameters (such as the data in Table 1) and the surface shape parameters (such as the data in Table 2).

In the first embodiment, the effective focal length of the optical lens assembly 110 is f=2.09 mm, the f-number FNO=1.30, the maximum field of view FOV=75.4 degrees (deg.), and the distance on the optical axis from the object side surface S 1 of the first lens L 1 to the imaging plane S 11 TTL=3.0 mm.

›DETAILED DESCRIPTION OF THE EMBODIMENTS · 5 of 9

Second Embodiment

In the second embodiment as shown FIG. 3 , an optical lens assembly 110 sequentially includes, from an object side to an image side, a first lens L 1 with a positive refractive power, an optical stop STO, a second lens L 2 with a positive refractive power, a third lens L 3 with a negative refractive power, and a fourth lens L 4 with a positive refractive power. In addition, an infrared band pass filter L 5 is further disposed on the image side of the fourth lens L 4 . FIG. 4 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly 110 in the second embodiment, where the astigmatism diagram and the distortion diagram are data diagrams at a reference wavelength.

The object side surface S 1 of the first lens L 1 is convex at the optical axis, the image side surface S 2 of the first lens L 1 is concave at the optical axis; the object side surface S 1 of the first lens L 1 is convex at the circumference thereof, and the image side surface S 2 of the first lens L 1 is convex at the circumference thereof. The object side surface S 3 of the second lens L 2 is convex at the optical axis, the image side surface S 4 of the second lens L 2 is concave at the optical axis; the object side surface S 3 of the second lens L 2 is concave at the circumference thereof, and the image side surface S 4 of the second lens L 2 is convex at the circumference thereof. The object side surface S 5 of the third lens L 3 is concave at the optical axis, the image side surface S 6 of the third lens L 3 is convex at the optical axis; the object side surface S 5 of the third lens L 3 is convex at the circumference thereof, and the image side surface S 6 of the third lens L 3 is concave at the circumference thereof. The object side surface S 7 of the fourth lens L 4 is convex at the optical axis, the image side surface S 8 of the fourth lens L 4 is concave at the optical axis; the object side surface S 7 of the fourth lens L 4 is concave at the circumference thereof, and the image side surface S 8 of the fourth lens L 4 is convex at the circumference thereof.

The object side surfaces and the image side surfaces of the first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are aspherical surfaces.

The first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are made of plastic.

In the second embodiment, the effective focal length of the optical lens assembly 110 is f=1.85 mm, the f-number FNO=1.30, the maximum field of view FOV=81.7 degrees (deg.), and the distance on the optical axis from the object side surface S 1 of the first lens L 1 to the imaging plane S 11 TTL=3.0 mm.

The various parameters of the optical lens assembly 110 are given in Table 3 and Table 4, and the definition of each parameter can be obtained from the first embodiment, which will not be repeated here.

According to the parameter information provided above, the following data can be derived:

Third Embodiment

In the third embodiment as shown FIG. 5 , an optical lens assembly 110 sequentially includes, from an object side to an image side, a first lens L 1 with a positive refractive power, an optical stop STO, a second lens L 2 with a positive refractive power, a third lens L 3 with a positive refractive power, and a fourth lens L 4 with a positive refractive power. In addition, an infrared band pass filter L 5 is further disposed on the image side of the fourth lens L 4 . FIG. 6 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly 110 in the third embodiment, where the astigmatism diagram and the distortion diagram are data diagrams at a reference wavelength.

The object side surface S 1 of the first lens L 1 is convex at the optical axis, the image side surface S 2 of the first lens L 1 is concave at the optical axis; the object side surface S 1 of the first lens L 1 is convex at the circumference thereof, and the image side surface S 2 of the first lens L 1 is convex at the circumference thereof. The object side surface S 3 of the second lens L 2 is convex at the optical axis, the image side surface S 4 of the second lens L 2 is concave at the optical axis; the object side surface S 3 of the second lens L 2 is concave at the circumference thereof, and the image side surface S 4 of the second lens L 2 is convex at the circumference thereof. The object side surface S 5 of the third lens L 3 is convex at the optical axis, the image side surface S 6 of the third lens L 3 is concave at the optical axis; the object side surface S 5 of the third lens L 3 is concave at the circumference thereof, and the image side surface S 6 of the third lens L 3 is convex at the circumference thereof. The object side surface S 7 of the fourth lens L 4 is convex at the optical axis, the image side surface S 8 of the fourth lens L 4 is concave at the optical axis; the object side surface S 7 of the fourth lens L 4 is concave at the circumference thereof, and the image side surface S 8 of the fourth lens L 4 is convex at the circumference thereof.

The object side surfaces and the image side surfaces of the first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are aspherical surfaces.

The first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are made of plastic.

In the third embodiment, the effective focal length of the optical lens assembly 110 is f=1.98 mm, the f-number FNO=1.30, the maximum field of view FOV=74 degrees (deg.), and the distance on the optical axis from the object side surface S 1 of the first lens L 1 to the imaging plane S 11 TTL=3.1 mm.

The various parameters of the optical lens assembly 110 are given in Table 5 and Table 6, and the definition of each parameter can be obtained from the first embodiment, which will not be repeated here.

According to the parameter information provided above, the following data can be derived:

›DETAILED DESCRIPTION OF THE EMBODIMENTS · 6 of 9

Fourth Embodiment

In the fourth embodiment as shown FIG. 7 , an optical lens assembly 110 sequentially includes, from an object side to an image side, a first lens L 1 with a positive refractive power, an optical stop STO, a second lens L 2 with a positive refractive power, a third lens L 3 with a negative refractive power, and a fourth lens L 4 with a positive refractive power. In addition, an infrared band pass filter L 5 is further disposed on the image side of the fourth lens L 4 . FIG. 8 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly 110 in the fourth embodiment, where the astigmatism diagram and the distortion diagram are data diagrams at a reference wavelength.

The object side surface S 1 of the first lens L 1 is convex at the optical axis, the image side surface S 2 of the first lens L 1 is concave at the optical axis; the object side surface S 1 of the first lens L 1 is convex at the circumference thereof, and the image side surface S 2 of the first lens L 1 is convex at the circumference thereof. The object side surface S 3 of the second lens L 2 is convex at the optical axis, the image side surface S 4 of the second lens L 2 is concave at the optical axis; the object side surface S 3 of the second lens L 2 is concave at the circumference thereof, and the image side surface S 4 of the second lens L 2 is convex at the circumference thereof. The object side surface S 5 of the third lens L 3 is concave at the optical axis, the image side surface S 6 of the third lens L 3 is convex at the optical axis; the object side surface S 5 of the third lens L 3 is concave at the circumference thereof, and the image side surface S 6 of the third lens L 3 is concave at the circumference thereof. The object side surface S 7 of the fourth lens L 4 is convex at the optical axis, the image side surface S 8 of the fourth lens L 4 is concave at the optical axis; the object side surface S 7 of the fourth lens L 4 is concave at the circumference thereof, and the image side surface S 8 of the fourth lens L 4 is convex at the circumference thereof.

The object side surfaces and the image side surfaces of the first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are aspherical surfaces.

The first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are made of plastic.

In the fourth embodiment, the effective focal length of the optical lens assembly 110 is f=1.8 mm, the f-number FNO=1.20, the maximum field of view FOV=85.3 degrees (deg.), and the distance on the optical axis from the object side surface S 1 of the first lens L 1 to the imaging plane S 11 TTL=2.91 mm.

The various parameters of the optical lens assembly 110 are given in Table 7 and Table 8, and the definition of each parameter can be obtained from the first embodiment, which will not be repeated here.

According to the parameter information provided above, the following data can be derived:

Fifth Embodiment

In the fifth embodiment as shown in FIG. 9 , an optical lens assembly 110 sequentially includes, from an object side to an image side, an optical stop STO, a first lens L 1 with a negative refractive power, a second lens L 2 with a positive refractive power, a third lens L 3 with a negative refractive power, and a fourth lens L 4 with a positive refractive power. In addition, an infrared band pass filter L 5 is further disposed on the image side of the fourth lens L 4 . FIG. 10 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly 110 in the fifth embodiment, where the astigmatism diagram and the distortion diagram are data diagrams at a reference wavelength.

The object side surface S 1 of the first lens L 1 is convex at the optical axis, the image side surface S 2 of the first lens L 1 is concave at the optical axis; the object side surface S 1 of the first lens L 1 is convex at the circumference thereof, and the image side surface S 2 of the first lens L 1 is convex at the circumference thereof. The object side surface S 3 of the second lens L 2 is convex at the optical axis, the image side surface S 4 of the second lens L 2 is concave at the optical axis; the object side surface S 3 of the second lens L 2 is concave at the circumference thereof, and the image side surface S 4 of the second lens L 2 is convex at the circumference thereof. The object side surface S 5 of the third lens L 3 is concave at the optical axis, the image side surface S 6 of the third lens L 3 is convex at the optical axis; the object side surface S 5 of the third lens L 3 is convex at the circumference thereof, and the image side surface S 6 of the third lens L 3 is concave at the circumference thereof. The object side surface S 7 of the fourth lens L 4 is convex at the optical axis, the image side surface S 8 of the fourth lens L 4 is concave at the optical axis; the object side surface S 7 of the fourth lens L 4 is concave at the circumference thereof, and the image side surface S 8 of the fourth lens L 4 is convex at the circumference thereof.

The object side surfaces and the image side surfaces of the first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are aspherical surfaces.

The first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are made of plastic.

In the fifth embodiment, the effective focal length of the optical lens assembly 110 is f=1.81 mm, the f-number FNO=1.10, the maximum field of view FOV=85.5 degrees (deg.), and the distance on the optical axis from the object side surface S 1 of the first lens L 1 to the imaging plane S 11 TTL=2.99 mm.

The various parameters of the optical lens assembly 110 are given in Table 9 and Table 10, and the definition of each parameter can be obtained from the first embodiment, which will not be repeated here.

According to the parameter information provided above, the following data can be derived:

›DETAILED DESCRIPTION OF THE EMBODIMENTS · 7 of 9

Sixth Embodiment

In the sixth embodiment as shown FIG. 11 , an optical lens assembly 110 sequentially includes, from an object side to an image side, an optical stop STO, a first lens L 1 with a positive refractive power, a second lens L 2 with a positive refractive power, a third lens L 3 with a negative refractive power, and a fourth lens L 4 with a positive refractive power. In addition, an infrared band pass filter L 5 is further disposed on the image side of the fourth lens L 4 . FIG. 12 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly 110 in the sixth embodiment, where the astigmatism diagram and the distortion diagram are data diagrams at a reference wavelength.

The object side surface S 1 of the first lens L 1 is convex at the optical axis, the image side surface S 2 of the first lens L 1 is concave at the optical axis; the object side surface S 1 of the first lens L 1 is convex at the circumference thereof, and the image side surface S 2 of the first lens L 1 is convex at the circumference thereof. The object side surface S 3 of the second lens L 2 is convex at the optical axis, the image side surface S 4 of the second lens L 2 is concave at the optical axis; the object side surface S 3 of the second lens L 2 is concave at the circumference thereof, and the image side surface S 4 of the second lens L 2 is convex at the circumference thereof. The object side surface S 5 of the third lens L 3 is concave at the optical axis, the image side surface S 6 of the third lens L 3 is convex at the optical axis; the object side surface S 5 of the third lens L 3 is convex at the circumference thereof, and the image side surface S 6 of the third lens L 3 is concave at the circumference thereof. The object side surface S 7 of the fourth lens L 4 is convex at the optical axis, the image side surface S 8 of the fourth lens L 4 is concave at the optical axis; the object side surface S 7 of the fourth lens L 4 is concave at the circumference thereof, and the image side surface S 8 of the fourth lens L 4 is convex at the circumference thereof.

The object side surfaces and the image side surfaces of the first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are aspherical surfaces.

The first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are made of plastic.

In the sixth embodiment, the effective focal length of the optical lens assembly 110 is f=1.81 mm, the f-number FNO=1.18, the maximum field of view FOV=85.5 degrees (deg.), and the distance on the optical axis from the object side surface S 1 of the first lens L 1 to the imaging plane S 11 TTL=2.99 mm.

The various parameters of the optical lens assembly 110 are given in Table 11 and Table 12, and the definition of each parameter can be obtained from the first embodiment, which will not be repeated here.

According to the parameter information provided above, the following data can be derived:

Seventh Embodiment

In the seventh embodiment as shown FIG. 13 , an optical lens assembly 110 sequentially includes, from an object side to an image side, an optical stop STO, a first lens L 1 with a positive refractive power, a second lens L 2 with a positive refractive power, a third lens L 3 with a negative refractive power, and a fourth lens L 4 with a positive refractive power. In addition, an infrared band pass filter L 5 is further disposed on the image side of the fourth lens L 4 . FIG. 14 is a spherochromatic aberration diagram (mm), an astigmatism diagram (mm), and a distortion diagram (%) of the optical lens assembly 110 in the seventh embodiment, where the astigmatism diagram and the distortion diagram are data diagrams at a reference wavelength.

The object side surface S 1 of the first lens L 1 is convex at the optical axis, the image side surface S 2 of the first lens L 1 is concave at the optical axis; the object side surface S 1 of the first lens L 1 is convex at the circumference thereof, and the image side surface S 2 of the first lens L 1 is convex at the circumference thereof. The object side surface S 3 of the second lens L 2 is convex at the optical axis, the image side surface S 4 of the second lens L 2 is concave at the optical axis; the object side surface S 3 of the second lens L 2 is concave at the circumference thereof, and the image side surface S 4 of the second lens L 2 is convex at the circumference thereof. The object side surface S 5 of the third lens L 3 is concave at the optical axis, the image side surface S 6 of the third lens L 3 is concave at the optical axis; the object side surface S 5 of the third lens L 3 is concave at the circumference thereof, and the image side surface S 6 of the third lens L 3 is concave at the circumference thereof. The object side surface S 7 of the fourth lens L 4 is convex at the optical axis, the image side surface S 8 of the fourth lens L 4 is concave at the optical axis; the object side surface S 7 of the fourth lens L 4 is concave at the circumference thereof, and the image side surface S 8 of the fourth lens L 4 is convex at the circumference thereof.

The object side surfaces and the image side surfaces of the first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are aspherical surfaces.

The first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 are made of plastic.

In the seventh embodiment, the effective focal length of the optical lens assembly 110 is f=2.05 mm, the f-number FNO=1.15, the maximum field of view FOV=78.7 degrees (deg.), and the distance on the optical axis from the object side surface S 1 of the first lens L 1 to the imaging plane S 11 TTL=3.03 mm.

The various parameters of the optical lens assembly 110 are given in Table 13 and Table 14, and the definition of each parameter can be obtained from the first embodiment, which will not be repeated here.

According to the parameter information provided above, the following data can be derived:

›DETAILED DESCRIPTION OF THE EMBODIMENTS · 8 of 9

Referring to FIGS. 13 and 15 , the optical lens assembly 110 and the photosensitive element 120 are assembled together to form an image capturing module 100 , and the photosensitive element 120 is disposed on the image side of the optical lens assembly 110 . The photosensitive element 120 is disposed on the imaging plane S 11 of the optical lens assembly 110 . The photosensitive element 120 may be a CCD (Charge Coupled Device) or a CMOS (Complementary Metal Oxide Semiconductor).

In some embodiments, the photosensitive element 120 is relatively fixedly disposed at the imaging plane S 11 of the optical lens assembly 110 , and in this case the image capturing module 100 is a fixed focus module.

In some other embodiments, a voice coil motor is arranged on the photosensitive element 120 to enable the photosensitive element 120 to relatively move relative to the lens in the optical lens assembly 110 . Alternatively, a fixing member can also be disposed to relatively fix the optical stop STO, the first lens L 1 , the second lens L 2 , the third lens L 3 , and the fourth lens L 4 , and in addition, a voice coil motor is arranged on the fixing member to drive the above lens and the optical stop STO to move relative to the photosensitive element 120 , so that the image capturing module 100 has a focusing function.

The image capturing module 100 can meet the needs of electronic devices for optical recognition functions, such as face unlocking on mobile phones, automatic drive on cars, human-machine interfaces and games, industrial machine vision and measurement, security monitoring, and the like.

Referring to FIG. 16 , when the recognition function is implemented, the image capturing module 100 also needs the cooperation with an emitting module 200 . In some embodiments, the image capturing module 100 and the emitting module 200 are assembled together to form a recognition device. The emitting module 200 emits modulated infrared light to the measured object. The infrared light can be continuous light or pulsed light. After the modulated light reaches the surface of the measured object, the modulated light is reflected and carries the depth information of the surface of the measured object to form information light. The image capturing module 100 can receive the information light reflected by the measured object. Specifically, the modulated light emitted by the emitting module 200 may be 3D (three dimensional) structured light or modulated pulsed light in TOF technology. The infrared band pass filter in the image capturing module 100 can allow the infrared light at a specific wavelength band emitted by the emitting module 200 to pass through, while filtering out light at other wavelength bands to prevent interference light from being received by the photosensitive element, and thus the image capturing module 100 can perfectly cooperate with the emitting module 200 .

The recognition device can be applied to a mobile terminal 10 , the mobile terminal 10 may be a smart phone, a smart watch, a tablet computer, a personal digital assistant, a game console, a PC (Personal Computer), and other devices. By adopting the optical lens assembly of the present disclosure, the mobile terminal 10 can be designed to be thinner and smaller.

The “electronic devices” used in the embodiments of the present disclosure may include, but are not limited to, devices that are configured to be connected via a wired line (such as via a public switched telephone network (PSTN), a digital subscriber line (DSL), a digital cable, a direct cable connection, and/or another data connection/network), and/or receive/transmit communication signals via a wireless interface (for example, for a cellular network, a wireless local area network (WLAN), a digital television network such as a digital video broadcasting handheld (DVB-H) network, a satellite network, an amplitude modulation-frequency modulation (AM-FM) broadcast transmitter, and/or another communication terminal). Electronic devices configured to communicate through a wireless interface may be referred to as “wireless communication terminals”, “wireless terminals”, and/or “mobile terminals”. Examples of the mobile terminal include, but are not limited to, a satellite or cellular phone; a personal communication system (PCS) terminal that can combine a cellular radio telephone with data processing, fax, and data communication capabilities; a personal digital assistant (PDA) that can include a radio telephone, a pager, an Internet/Intranet access, a Web browser, a notepad, a calendar, and/or a global positioning system (GPS) receiver; and a conventional laptop and/or handheld receiver or other electronic device including a radio telephone transceiver.

In the description of the present disclosure, it should be understood that orientation or positional relationship indicated by the terms “center”, “longitudinal”, “transverse”, “length”, “width”, “thickness”, “upper”, “lower”, “front”, “rear”, “left”, “right”, “vertical”, “horizontal”, “top”, “bottom”, “inner”, “outer”, “clockwise”, “counterclockwise”, “axial”, “radial”, “circumferential”, and the like are the orientation or positional relationship shown based on the drawings, which are only to facilitate the description of the present disclosure and simplify the description, rather than indicating or implying the device or elements referred to must have a specific orientation or be constructed and operated in a specific orientation, therefore they cannot be construed as limiting the present disclosure.

In addition, the terms “first” and “second” are used for purposes of description only, and cannot be understood to indicate or imply relative importance or implicitly indicate the number of technical features indicated. Therefore, the features defined “first” and “second” may explicitly or implicitly include at least one of the features. In the description of the present disclosure, the meaning of “plurality” is at least two, such as two, three, or more, unless otherwise clearly and specifically defined.

›DETAILED DESCRIPTION OF THE EMBODIMENTS · 9 of 9

In the present disclosure, unless otherwise clearly specified and limited, the terms “installed”, “connected with each other”, “connected”, “fixed” and other terms should be understood in a broad sense, for example, it may be fixedly connected or detachably connected, or integrated as one; it may be mechanically connected or electrically connected; it may be directly connected, or may be indirectly connected through an intermediate, it may be the communication between two components or the interaction between two components, unless otherwise clearly defined. Those of ordinary skill in the art can understand the specific meanings of the above terms in the present disclosure according to specific situations.

In the present disclosure, unless otherwise clearly specified and defined, a first feature is “on” or “below” a second feature may be that the first and second features are in direct contact, or the first and second features are indirectly contact through an intermediate. The first feature is “at the top of”, “above”, and “over” the second feature may indicate that the first feature is directly or obliquely above the second feature, or only indicate that a level height of the first feature is higher than that of the second feature. The first feature is “at the bottom of”, “below”, and “under” the second feature may be that the first feature is directly or obliquely below the second feature, or only indicate that the level height of the first feature is less than that of the second feature.

In the descriptions of this specification, the descriptions with reference to the terms “an embodiment”, “some embodiments”, “example”, “specific example”, or “some examples”, or the like means that the specific features, structures, materials or characteristics described with reference to the embodiments or examples are included in at least one embodiment or example of the present disclosure. In this specification, the schematic representations of the above terms do not necessarily refer to a same embodiment or example. Moreover, the described specific features, structures, materials or characteristics can be combined in an appropriate manner in any one or more embodiments or examples. In addition, those skilled in the art can combine and assemble the different embodiments or examples and the features of the different embodiments or examples described in this specification without contradicting each other.

The technical features of the above described embodiments can be combined arbitrarily. To simplify the description, not all possible combinations of the technical features in the above embodiments are described. However, all of the combinations of these technical features should be considered as within the scope of the present disclosure, as long as such combinations do not contradict with each other.

The above described embodiments are merely illustrate several embodiments of the present disclosure, which are described more specifically and in detail, but they cannot be understood as limiting the scope of the present disclosure. It should be noted that, for those ordinary skilled in the art, several variations and improvements may be made without departing from the concept of the present disclosure, and all of which are within the protection scope of the present disclosure. Therefore, the protection scope of the present disclosure shall be defined by the appended claims.

›Tables in the description — 21
Z=
c⁢
r2
1+
1-(k+1)⁢c2⁢r2
+
∑i
Ai⁢
ri
TABLE 1 — First Embodiment f = 2.09 mm, FNO = 1.30, FOV = 75.4 degree, TTL = 3.0 mm Focal
SurfaceSurfaceSurfaceY radiusThicknessRefractiveAbbelength
numbernametype(mm)(mm)Materialindexnumber(mm)
0ObjectSphericalInfiniteInfinite
plane
1First lensAspherical1.3620.418Plastic1.54555.9314.616
2Aspherical1.4720.114
3Optical stopSphericalInfinite0.052
4Second lensAspherical0.9260.290Plastic1.66120.3733.971
5Aspherical1.2870.411
6Third lensAspherical−13.5710.317Plastic1.54555.93−13.458
7Aspherical15.4850.162
8Fourth lensAspherical0.6270.320Plastic1.66120.3732.893
9Aspherical0.7640.225
10InfraredSphericalInfinite0.210Glass1.51764.17
11band passSphericalInfinite0.480
filter
12ImagingSphericalInfinite0.000
plane
Note:
The reference wavelength is 940 nm
TABLE 2 — First Embodiment Aspheric coefficient Surface
number12456789
K−0.869−13.336−0.7210.91729.60629.455−4.506−1.477
A4−0.101−0.085−0.518−0.091−0.573−2.542−0.443−0.777
A60.064−1.6731.372−0.7394.69810.911−0.2880.553
A80.0549.506−11.217−0.531−27.192−34.1251.328−0.104
A10−0.278−28.79142.3450.84090.76371.696−1.738−0.164
A12−0.08048.365−89.7384.490−179.476−96.3461.2700.116
A140.532−42.016102.833−10.722194.99476.594−0.495−0.022
A16−0.32014.674−49.4685.771−89.307−26.9010.079−0.001
A180.0000.0000.0000.0000.0000.0000.0000.000
A200.0000.0000.0000.0000.0000.0000.0000.000
TABLE 3 — Second Embodiment f = 1.85 mm, FNO = 1.30, FOV = 81.7 degree, TTL = 3.0 mm Focal
SurfaceSurfaceSurfaceY radiusThicknessRefractiveAbbelength
numbernametype(mm)(mm)Materialindexnumber(mm)
0ObjectSphericalInfiniteInfinite
plane
1First lensAspherical1.4490.280Plastic1.54555.9346.041
2Aspherical1.4350.106
3Optical stopSphericalInfinite0.030
4Second lensAspherical0.9260.281Plastic1.66120.3733.784
5Aspherical1.3300.305
6Third lensAspherical−3.3700.496Plastic1.54555.93−6.836
7Aspherical−44.8170.160
8Fourth lensAspherical0.5810.360Plastic1.66120.3731.863
9Aspherical0.8680.293
10InfraredSphericalInfinite0.210Glass1.51764.17
11band passSphericalInfinite0.478
filter
12ImagingSphericalInfinite0.000
plane
Note:
The reference wavelength is 940 nm
TABLE 4 — Second Embodiment Aspheric coefficient Surface
number12456789
K−1.373−15.789−1.0460.978−50.00030.000−5.206−1.190
A4−0.160−0.218−0.575−0.065−0.427−2.5730.294−0.228
A60.426−0.6791.377−1.5021.36310.497−1.661−0.653
A8−0.4056.303−10.2336.536−3.604−33.5112.9281.330
A10−1.293−26.73438.429−31.593−2.17774.843−2.862−1.190
A123.85061.064−88.55185.89836.475−107.9811.6140.551
A14−3.877−73.838113.650−111.807−62.32490.959−0.483−0.124
A160.74536.447−64.75653.76731.483−32.9450.0590.010
A180.0000.0000.0000.0000.0000.0000.0000.000
A200.0000.0000.0000.0000.0000.0000.0000.000
Second Embodiment
f (mm)1.85
FNO1.30
FOV (degree)81.7
TTL (mm)3.0
TT/f1.091
T12 + T23 + T34 (mm)0.601
f2/f42.03
SL/TTL0.871
FFL (mm)0.74
R8/R90.669
R4/f20.245
TABLE 5 — Third Embodiment f = 1.98 mm, FNO = 1.30, FOV = 74 degree, TTL = 3.1 mm Focal
SurfaceSurfaceSurfaceY radiusThicknessRefractiveAbbelength
numbernametype(mm)(mm)Materialindexnumber(mm)
0ObjectSphericalInfiniteInfinite
plane
1First lensAspherical1.3970.473Plastic1.54555.9312.060
2Aspherical1.5730.087
3Optical stopSphericalInfinite0.050
4Second lensAspherical1.1670.364Plastic1.66120.3734.501
5Aspherical1.7360.348
6Third lensAspherical5.6090.453Plastic1.54555.9318.064
7Aspherical12.9780.094
8Fourth lensAspherical0.6790.322Plastic1.66120.3733.970
9Aspherical0.7580.198
10InfraredSphericalInfinite0.210Glass1.51764.17
11band passSphericalInfinite0.502
filter
12ImagingSphericalInfinite0.000
plane
Note:
The reference wavelength is 940 nm
TABLE 6 — Third Embodiment Aspheric coefficient Surface
number12456789
K−0.847−12.471−0.9720.889−5.14197.137−5.629−1.624
A4−0.2070.213−0.9110.151−0.453−2.718−1.058−0.816
A61.769−11.7388.522−7.2648.98013.3811.163−0.375
A8−12.205131.864−110.77069.908−80.243−45.291−0.6034.978
A1050.024−844.045866.169−430.763420.073102.741−2.074−12.417
A12−125.2203310.068−4277.1281650.495−1392.237−150.7966.15516.913
A14192.617−8086.07013399.590−3937.7462939.555134.085−7.139−13.955
A16−177.53912013.014−25739.6915696.108−3832.436−61.5594.2426.942
A1889.923−9941.33527592.715−4577.9392811.5427.411−1.274−1.919
A20−19.2593516.664−12620.5571569.663−888.3472.4580.1520.227
Third Embodiment
f (mm)1.98
FNO1.30
FOV (degree)74
TTL (mm)3.1
TT/f1.106
T12 + T23 + T34 (mm)0.579
f2/f41.13
SL/TTL0.82
FFL (mm)0.76
R8/R90.896
R4/f20.259
TABLE 7 — Fourth Embodiment f = 1.8 mm, FNO = 1.20, FOV = 85.3 degree, TTL = 2.91 mm Focal
SurfaceSurfaceSurfaceY radiusThicknessRefractiveAbbelength
numbernametype(mm)(mm)Materialindexnumber(mm)
0ObjectSphericalInfiniteInfinite
plane
1First lensAspherical1.2470.410Plastic1.54555.935.621
2Aspherical1.8850.050
3Optical stopSphericalInfinite0.153
4Second lensAspherical1.4370.261Plastic1.66120.3735.038
5Aspherical2.4280.226
6Third lensAspherical−1.6940.478Plastic1.54555.93−16.938
7Aspherical−2.2880.059
8Fourth lensAspherical0.5800.299Plastic1.63923.2612.810
9Aspherical0.7010.285
10InfraredSphericalInfinite0.210Glass1.51764.17
11band passSphericalInfinite0.480
filter
12ImagingSphericalInfinite0.000
plane
Note:
The reference wavelength is 940 nm
TABLE 8 — Fourth Embodiment Aspheric coefficient Surface
number12456789
K−0.723−8.7411.4183.4523.5482.795−9.230−4.087
A4−0.3270.125−0.3780.3100.383−3.987−0.489−0.351
A64.380−5.6732.709−6.055−1.27928.8283.0260.839
A8−36.76361.932−43.38163.1154.501−127.390−12.646−2.280
A10179.159−414.250316.653−451.576−37.854339.13331.0654.361
A12−536.4701696.378−1425.7192005.537303.620−491.076−47.050−5.327
A14993.484−4318.4923978.494−5603.435−1306.586218.64544.3703.997
A16−1109.5336667.155−6748.0139527.7782951.481372.184−25.300−1.767
A18684.256−5709.4016454.968−8888.124−3268.481−554.6437.9620.418
A20−179.0162078.838−2700.0743447.2891390.482219.917−1.059−0.040
Fourth Embodiment
f (mm)1.8
FNO1.20
FOV (degree)85.3
TTL (mm)2.91
TT/f1.07
T12 + T23 + T34 (mm)0.488
f2/f41.79
SL/TTL0.842
FFL (mm)0.74
R8/R90.827
R4/f20.285
TABLE 9 — Fifth Embodiment f = 1.81 mm, FNO = 1.10, FOV = 85.5 degree, TTL = 2.99 mm Focal
SurfaceSurfaceSurfaceY radiusThicknessRefractiveAbbelength
numbernametype(mm)(mm)Materialindexnumber(mm)
0ObjectSphericalInfinite800.000
plane
1Optical stopSphericalInfinite−0.079
2First lensAspherical1.6030.340Plastic1.53555.779−18.010
3Aspherical1.2700.111
4Second lensAspherical1.2210.392Plastic1.66120.3732.328
5Aspherical6.1730.240
6Third lensAspherical−1.6640.488Plastic1.53555.779−4.862
7Aspherical−5.2380.081
8Fourth lensAspherical0.5320.327Plastic1.66120.3732.057
9Aspherical0.6850.331
10InfraredSphericalInfinite0.210Glass1.51764.17
11band passSphericalInfinite0.471
filter
12ImagingSphericalInfinite0.000
plane
Note:
The reference wavelength is 940 nm
TABLE 10 — Fifth Embodiment Aspheric coefficient Surface
number23456789
K−15.908−21.679−22.762−99.000−13.23511.843−5.778−1.867
A40.2760.5761.1090.2810.179−3.706−0.024−0.308
A6−1.757−6.255−6.945−1.192−2.51822.646−0.283−1.190
A86.73532.23227.7316.97714.001−97.186−2.4465.533
A10−9.410−132.203−81.250−38.012−45.198287.68414.919−11.330
A12−44.392375.189120.57799.57877.999−577.440−37.69513.508
A14241.029−690.683−14.777−141.800−68.329766.24452.259−9.884
A16−491.733787.100−208.211112.93125.058−639.396−41.3434.365
A18478.342−505.749266.827−46.1121.012302.99417.482−1.068
A20−183.496140.948−107.2327.013−2.167−62.045−3.0630.111
Fifth Embodiment
f (mm)1.81
FNO1.10
FOV (degree)85.5
TTL (mm)2.99
TT/f1.093
T12 +T23 +T34 (mm)0.432
f2/f41.13
SL/TTL0.974
FFL (mm)0.73
R8/R90.777
R4/f20.524
TABLE 11 — Sixth Embodiment f = 1.81 mm, FNO = 1.18, FOV = 85.5 degree, TTL = 2.99 mm Focal
SurfaceSurfaceSurfaceY radiusThicknessRefractiveAbbelength
numbernametype(mm)(mm)Materialindexnumber(mm)
0ObjectSphericalInfinite800.000
plane
1Optical stopSphericalInfinite-0.101
2First lensAspherical1.6020.397Plastic1.54555.9330.795
3Aspherical1.6210.097
4Second lensAspherical1.4960.372Plastic1.66120.3733.436
5Aspherical4.3160.278
6Third lensAspherical−1.6820.425Plastic1.54555.93−5.041
7Aspherical−4.8550.050
8Fourth lensAspherical0.4900.305Plastic1.66120.3731.853
9Aspherical0.6380.386
10InfraredSphericalInfinite0.210Glass1.51764.17
11band passSphericalInfinite0.471
filter
12ImagingSphericalInfinite0.000
plane
Note:
The reference wavelength is 940 nm
TABLE 12 — Sixth Embodiment Aspheric coefficient Surface
number23456789
K−11.162−26.177−65.223−98.372−24.09910.426−5.267−1.850
A4−0.0280.5461.8240.3500.162−4.088−0.014−0.267
A64.752−7.506−18.347−1.854−1.67826.8990.812−0.785
A8−58.41151.670120.3468.8416.985−119.535−6.9943.269
A10378.488−266.559−576.356−45.027−14.291358.07622.240−5.993
A12−1476.747903.5531837.238131.626−0.271−717.494−39.4126.465
A143552.420−1954.539−3819.294−222.01049.701942.39141.840−4.338
A16−5155.4602609.4994998.524217.707−81.629−775.423−26.3481.786
A184137.505−1962.412−3742.524−116.09455.103362.5369.050−0.416
A20−1410.521635.8561220.13026.190−14.063−73.520−1.3030.042
Sixth Embodiment
f (mm)1.81
FNO1.18
FOV (degree)85.5
TTL (mm)2.99
TT/f1.062
T12 + T23 + T34 (mm)0.425
f2/f41.85
SL/TTL0.966
FFL (mm)0.73
R8/R90.768
R4/f20.435
TABLE 13 — Seventh Embodiment f = 2.05 mm, FNO = 1.15, FOV = 78.7 degree, TTL = 3.03 mm Focal
SurfaceSurfaceSurfaceY radiusThicknessRefractiveAbbelength
numbernametype(mm)(mm)Materialindexnumber(mm)
0ObjectSphericalInfinite742.991
plane
1Optical stopSphericalInfinite−0.225
2First lensAspherical1.1370.341Plastic1.54555.9362.040
3Aspherical1.0540.167
4Second lensAspherical1.3610.401Plastic1.66120.3733.429
5Aspherical3.2250.216
6Third lensAspherical−4.5290.357Plastic1.54555.93−5.722
7Aspherical9.7260.106
8Fourth lensAspherical0.5420.274Plastic1.66120.3732.136
9Aspherical0.7260.328
10InfraredSphericalInfinite0.210Glass1.51764.17
11band passSphericalInfinite0.626
filter
12ImagingSphericalInfinite0.000
plane
Note:
The reference wavelength is 940 nm
TABLE 14 — Seventh Embodiment Aspheric coefficient Surface
number23456789
K−5.062−4.853−23.514−32.209−9.5167.353−3.741−2.233
A40.1180.4330.8720.013−0.216−3.390−0.4910.085
A62.308−5.433−4.6180.2481.96818.8721.904−2.934
A8−25.19345.34720.331−4.939−13.813−79.699−11.9199.667
A10135.900−239.565−86.69425.25956.810244.72742.554−17.548
A12−439.081779.100285.209−84.712−148.626−523.155−89.29319.722
A14873.090−1582.552−639.378169.920251.956750.902113.949−13.960
A16−1046.5341948.013868.180−192.549−258.096−677.032−87.0316.021
A18692.573−1326.475−631.043113.763141.166340.79236.479−1.438
A20−194.121383.876187.831−27.277−31.145−72.112−6.4320.145
Seventh Embodiment
f (mm)2.05
FNO1.15
FOV (degree)78.7
TTL (mm)3.03
TT/f0.908
T12 + T23 + T34 (mm)0.489
f2/f41.61
SL/TTL0.924
FFL (mm)0.915
R8/R90.747
R4/f20.397

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IPC · International Patent Classification
Section G — Physics
  • G02B13/00
  • G02B9/34

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